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  1. Emerging Edge Capital EEC | Open Energy Information

    OpenEI (Open Energy Information) [EERE & EIA]

    Edge Capital EEC Jump to: navigation, search Name: Emerging Edge Capital (EEC) Place: London, United Kingdom Zip: SW1Y 4RS Sector: Renewable Energy Product: London-based company...

  2. UC Davis Energy Efficiency Center EEC | Open Energy Information

    OpenEI (Open Energy Information) [EERE & EIA]

    UC Davis Energy Efficiency Center EEC Jump to: navigation, search Name: UC Davis Energy Efficiency Center (EEC) Place: California Sector: Efficiency Product: With a leadership...

  3. Edge Equilibrium Code (EEC) For Tokamaks

    SciTech Connect

    Li, Xujling

    2014-02-24

    The edge equilibrium code (EEC) described in this paper is developed for simulations of the near edge plasma using the finite element method. It solves the Grad-Shafranov equation in toroidal coordinate and uses adaptive grids aligned with magnetic field lines. Hermite finite elements are chosen for the numerical scheme. A fast Newton scheme which is the same as implemented in the equilibrium and stability code (ESC) is applied here to adjust the grids

  4. Runoff simulations from the Greenland ice sheet at Kangerlussuaq from 2006-2007 to 2007/08. West Greenland

    SciTech Connect

    Mernild, Sebastian Haugard [Los Alamos National Laboratory; Hasholt, Bent [UNIV OF COPENHAGEN; Van Den Broeke, Michiel [UTRECHT UNIV; Liston, Glen [COLORADO STATE UNIV

    2009-01-01

    This study focuses on runoff from a large sector of the Greenland Ice Sheet (GrIS) - the Kangerlussuaq drainage area, West Greenland - for the runoff observation period 2006/07 to 2007/08. SnowModel, a state-of-the-art snow-evolution modeling system, was used to simulate winter accumulation and summer ablation processes, including runoff. Independent in situ end-of-winter snow depth and high-resolution runoff observations were used for validation of simulated accumulation and ablation processes. Runoff was modeled on both daily and hourly time steps, filling a data gap of runoff exiting part of the GrIS. Using hourly meteorological driving data instead of smoothed daily-averaged data produced more realistic meteorological conditions in relation to snow and melt threshold surface processes, and produced 6-17% higher annual cumulative runoff. The simulated runoff series yielded useful insights into the present conditions of inter-seasonal and inter-annual variability of Kangerlussuaq runoff, and provided an acceptable degree of agreement between simulated and observed runoff. The simulated spatial runoff distributions, in some areas of the GrIS terminus, were as high as 2,750 mm w.eq. of runoff for 2006/07, while only 900 mm w.eq was simulated for 2007/08. The simulated total runoff from Kangerlussuaq was 1.9 km{sup 3} for 2006/07 and 1.2 km{sup 3} for 2007/08, indicating a reduction of 35-40% caused by the climate conditions and changes in the GrIS freshwater storage. The reduction in runoff from 2006/07 to 2007/08 occurred simultaneously with the reduction in the overall pattern of satellite-derived GrIS surface melt from 2007 to 2008.

  5. Team advances understanding of the Greenland Ice Sheet's meltwater

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    channels Greenland Ice Sheet's meltwater channels Team advances understanding of the Greenland Ice Sheet's meltwater channels An international research team's field work is showing that, well, things are more complicated than we thought. October 1, 2014 An international team of researchers deployed to western Greenland to study the melt rates of the Greenland Ice Sheet. An international team of researchers deployed to western Greenland to study the melt rates of the Greenland Ice Sheet.

  6. Greenland Ice Sheet Modeling Update (Conference) | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    Greenland Ice Sheet Modeling Update Citation Details In-Document Search Title: Greenland Ice Sheet Modeling Update You are accessing a document from the Department of Energy's...

  7. Complex systems influence melting of Greenland ice sheet

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    melting of Greenland ice sheet Complex systems influence melting of Greenland ice sheet International research team's field work shows that, well, things are more complicated...

  8. ARM - Field Campaign - Lidar support for ICECAPS at Summit, Greenland

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    govCampaignsLidar support for ICECAPS at Summit, Greenland Campaign Links ICECAPS Campaign Summary (PDF) Summit Station Research Highlight New Data from Greenland for Arctic...

  9. Greenland: Energy Resources | Open Energy Information

    OpenEI (Open Energy Information) [EERE & EIA]

    Country Profile Name Greenland Population 56,968 GDP Unavailable Energy Consumption 0.01 Quadrillion Btu 2-letter ISO code GL 3-letter ISO code GRL Numeric ISO...

  10. Greenland ice sheet surface mass-balance modeling in a 131-year perspective, 1950-2080

    SciTech Connect

    Mernild, Sebastian Haugard; Liston, Glen; Hiemstra, Christopher; Christensen, Jens

    2009-01-01

    Fluctuations in the Greenland Ice Sheet (GrIS) surface mass-balance (SMB) and freshwater influx to the surrounding oceans closely follow climate fluctuations and are of considerable importance to the global eustatic sea level rise. SnowModel, a state-of-the-art snow-evolution modeling system, was used to simulate variations in the GrIS melt extent, surface water balance components, changes in SMB, and freshwater influx to the ocean. The simulations are based on the IPCC scenario AlB modeled by the HIRHAM4 RCM (using boundary conditions from ECHAM5 AOGCM) from 1950 through 2080. In-situ meteorological station (GC-Net and WMO DMI) observations from inside and outside the GrIS were used to validate and correct RCM output data before it was used as input for SnowModel. Satellite observations and independent SMB studies were used to validate the SnowModel output and confirm the model's robustness. We simulated a {approx}90% increase in end-of-summer surface melt extent (0.483 x 10{sup 6} km{sup 2}) from 1950 to 2080, and a melt index (above 2,000-m elevation) increase of 138% (1.96 x 10{sup 6} km{sup 2} x days). The greatest difference in melt extent occured in the southern part of the GrIS, and the greatest changes in the number of melt days was seen in the eastern part of the GrIS ({approx}50-70%) and was lowest in the west ({approx}20-30%). The rate of SMB loss, largely tied to changes in ablation processes, lead to an enhanced average loss of 331 km{sup 3} from 1950 to 2080, an average 5MB level of -99 km{sup 3} for the period 2070-2080. GrIS surface freshwater runoff yielded an eustatic rise in sea level from 0.8 {+-} 0.1 (1950-1959) to 1.9 {+-} 0.1 mm (2070-2080) sea level equivalent (SLE) y{sup -1}. The accumulated GrIS freshwater runoff contribution from surface melting equaled 160 mm SLE from 1950 through 2080.

  11. Microsoft Word - Gr91-CREEP-RUPTURE-rev.doc

    Office of Scientific and Technical Information (OSTI)

    to the Generation IV Nuclear Energy Systems Program 1. ... Gr 91. IDENTIFICATION OF MATERIALS Grade 91 steel is one of ... (ORNL) assumed the management of the technology program. ...

  12. Hainan Greenland Microalgae Biotechnology Co Ltd | Open Energy...

    OpenEI (Open Energy Information) [EERE & EIA]

    Microalgae Biotechnology Co Ltd Jump to: navigation, search Name: Hainan Greenland Microalgae Biotechnology Co Ltd Place: Hainan Province, China Product: Chinese biotechnology firm...

  13. New climate model predicts likelihood of Greenland ice melt,...

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    A new computer model of accumulated carbon emissions predicts the likelihood of crossing several dangerous climate change thresholds. November 20, 2015 Greenland ice loss. ...

  14. Greenland, New Hampshire: Energy Resources | Open Energy Information

    OpenEI (Open Energy Information) [EERE & EIA]

    Greenland, New Hampshire: Energy Resources Jump to: navigation, search Equivalent URI DBpedia Coordinates 43.0361995, -70.8328322 Show Map Loading map... "minzoom":false,"mapp...

  15. Meltwater effects on flow of Greenland's ice sheet less severe...

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    (University of Texas). Location: west coast of the Greenland Ice Sheet. Photo by Matt Hoffman, Los Alamos National Laboratory Contact Nancy Ambrosiano Communications Office (505)...

  16. Greenland in RASM (Conference) | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    Citation Details In-Document Search Title: Greenland in RASM Authors: Lipscomb, William Henry 1 + Show Author Affiliations Los Alamos National Laboratory Publication Date: ...

  17. Complex systems influence melting of Greenland ice sheet

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Complex systems influence melting of Greenland ice sheet Complex systems influence melting of Greenland ice sheet International research team's field work shows that, well, things are more complicated than we thought December 22, 2014 The newly discovered rolling movement shown in (A) three-dimensional cryo-electron microscopy image of ribosome, and (B) computer-generated atomic-resolution model of the human ribosome consistent with microscopy. An international team of researchers deployed to

  18. Sandia's ice sheet modeling of Greenland, Antarctica helps predict

    National Nuclear Security Administration (NNSA)

    sea-level rise | National Nuclear Security Administration | (NNSA) Sandia's ice sheet modeling of Greenland, Antarctica helps predict sea-level rise Wednesday, March 2, 2016 - 12:00am Sandia California researchers Irina Tezaur and Ray Tuminaro analyze a model of Antarctica. They are part of a Sandia team working to improve the reliability and efficiency of computational models that describe ice sheet behavior and dynamics. The Greenland and Antarctic ice sheets will make a dominant

  19. Meltwater flux and runoff modeling in the abalation area of jakobshavn Isbrae, West Greenland

    SciTech Connect

    Mernild, Sebastian Haugard [Los Alamos National Laboratory; Chylek, Petr [Los Alamos National Laboratory; Liston, Glen [COLORADO STATE UNIV.; Steffen, Konrad [UNIV OF COLORADO

    2009-01-01

    The temporal variability in surface snow and glacier melt flux and runoff were investigated for the ablation area of lakobshavn Isbrae, West Greenland. High-resolution meteorological observations both on and outside the Greenland Ice Sheet (GrIS) were used as model input. Realistic descriptions of snow accumulation, snow and glacier-ice melt, and runoff are essential to understand trends in ice sheet surface properties and processes. SnowModel, a physically based, spatially distributed meteorological and snow-evolution modeling system was used to simulate the temporal variability of lakobshavn Isbrre accumulation and ablation processes for 2000/01-2006/07. Winter snow-depth observations and MODIS satellite-derived summer melt observations were used for model validation of accumulation and ablation. Simulations agreed well with observed values. Simulated annual surface melt varied from as low as 3.83 x 10{sup 9} m{sup 3} (2001/02) to as high as 8.64 x 10{sup 9} m{sup 3} (2004/05). Modeled surface melt occurred at elevations reaching 1,870 m a.s.l. for 2004/05, while the equilibrium line altitude (ELA) fluctuated from 990 to 1,210 m a.s.l. during the simulation period. The SnowModel meltwater retention and refreezing routines considerably reduce the amount of meltwater available as ice sheet runoff; without these routines the lakobshavn surface runoff would be overestimated by an average of 80%. From September/October through May/June no runoff events were simulated. The modeled interannual runoff variability varied from 1.81 x 10{sup 9} m{sup 3} (2001/02) to 5.21 x 10{sup 9} m{sup 3} (2004/05), yielding a cumulative runoff at the Jakobshavn glacier terminus of {approx}2.25 m w.eq. to {approx}4.5 m w.eq., respectively. The average modeled lakobshavn runoff of {approx}3.4 km{sup 3} y{sup -1} was merged with previous estimates of Jakobshavn ice discharge to quantify the freshwater flux to Illulissat Icefiord. For both runoff and ice discharge the average trends are

  20. Update on Greenland Ice Sheet Simulations In CISM and CESM (Conference...

    Office of Scientific and Technical Information (OSTI)

    Title: Update on Greenland Ice Sheet Simulations In CISM and CESM Authors: Lipscomb, William Henry 1 + Show Author Affiliations Los Alamos National Laboratory Publication Date: ...

  1. Optical observations of the type Ic supernova 2007gr in NGC 1058

    SciTech Connect

    Chen, Juncheng; Wang, Xiaofeng; Li, Junzheng; Ganeshalingam, Mohan; Silverman, Jeffrey M.; Filippenko, Alexei V.; Li, Weidong; Chornock, Ryan; Steele, Thea E-mail: wang_xf@mail.tsinghua.edu.cn

    2014-08-01

    We present extensive optical observations of the normal Type Ic supernova (SN) 2007gr, spanning from about one week before maximum light to more than one year thereafter. The optical light and color curves of SN 2007gr are very similar to those of the broad-lined Type Ic SN 2002ap, but the spectra show remarkable differences. The optical spectra of SN 2007gr are characterized by unusually narrow lines, prominent carbon lines, and slow evolution of the line velocity after maximum light. The earliest spectrum (taken at t = –8 days) shows a possible signature of helium (He I λ5876 at a velocity of ∼19,000 km s{sup –1}). Moreover, the larger intensity ratio of the [O I] λ6300 and λ6364 lines inferred from the early nebular spectra implies a lower opacity of the ejecta shortly after the explosion. These results indicate that SN 2007gr perhaps underwent a less energetic explosion of a smaller-mass Wolf-Rayet star (∼8-9 M{sub ☉}) in a binary system, as favored by an analysis of the progenitor environment through pre-explosion and post-explosion Hubble Space Telescope images. In the nebular spectra, asymmetric double-peaked profiles can be seen in the [O I] λ6300 and Mg I] λ4571 lines. We suggest that the two peaks are contributed by the blueshifted and rest-frame components. The similarity in velocity structure and the different evolution of the strength of the two components favor an aspherical explosion with the ejecta distributed in a torus or disk-like geometry, but inside the ejecta the O and Mg have different distributions.

  2. Meltwater effects on flow of Greenland's ice sheet less severe for sea

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    level rise than earlier feared, scientists say Stories » Side effects of increasing meltwater less severe than feared Meltwater effects on flow of Greenland's ice sheet less severe for sea level rise than earlier feared, scientists say The team found that accelerating ice sheet movement from increasing meltwater lubrication is likely to have only a minor role in future sea-level rise. August 19, 2013 A stream of meltwater on the surface of the Greenland Ice Sheet enters a moulin connecting

  3. Evaluation of Irradiation Embrittlement of A508 Gr 4N and Comparison to Other Low-Alloy Steels

    SciTech Connect

    G.L. Wire, W. J. Beggs and T.R. Leax

    2002-06-17

    A508 Gr 4N has improved fracture toughness because of the addition of 3% nickel, compared to typical low alloy steels which have less than 1% nickel. However, there is an expectation in much of the recent literature, based mostly on low-alloy steels with nickel below 1%, that irradiation embrittlement will increase with increasing nickel (Ni) content. In contrast, the raw irradiation test data show that ASTM A508 Grade 4N containing up to 3.7% nickel, 0.1% Cu and 0.01% P does not show enhanced irradiation embrittlement. A simple statistical fit to irradiation dose and irradiation temperature was developed to make direct comparisons to other low-alloy steels. Since the A508 Gr 4N data showed little discernible effect of Cu in the raw data, the damage may be classified as 'matrix' damage. The peak irradiation embrittlement of A508 Gr 4N is no greater than that of A508 Gr 2, a 0.7% Ni forging material tested under similar conditions with similar limits on Cu and P. At high dose (80 mdpa) the average embrittlement of A508 Gr 4N is slightly higher (33%) than the lower nickel materials. This trend also occurs for low copper A533B and A302B plate material. The irradiation temperature dependence of embrittlement in A508 Gr 4N is nearly the same as other low copper low-alloy steels tested over a wide range of temperatures. The increase in Charpy transition temperature in A508 Gr 4N is due to radiation hardening, and the ratio of TTS to yield strength increase in 3 Ni steels is nearly identical to that observed for conventional low-alloy steels with lower nickel. A very detailed statistical fit was made to the overall data on A508 Gr 4N to evaluate the sensitivity of embrittlement to minor elements and to compare to results from the US surveillance test data, which is at low flux. The fit includes the effect of dose, irradiation temperature, flux, and composition. The embrittlement increases lightly at high flux, consistent with unstable matrix defects (UMD). Cu and P each

  4. Mr. G. !4, :iundGr, :?l.ang l4.xqpr

    Office of Legacy Management (LM)

    Mr. G. !4, :iundGr, :?l.ang l4.xqpr - - K~*ti.Cranl &&tad cclqmy of mu 2. 0. Tkxs 158; 45%. Mealthy R~ticrn Cix3 Armti 31, ohlo ' WP i%r, gLtsx.hst * .- 3.sfzrcnEe ira made 9x8 your 3.&&w ddafi ihmmbdr %1, 3-956, pergarding thtr rEfrrp&d. of ttm ti~orim rna:irfuw WC the Eurwa CS 1Mfnaia, dixqyJ orr!pl. Thio of.mJs Rim earreagwndrd wfth th3 tmakb fJp4waBisrasr O flica the ~tsr5.n~ of' +.&~":a rrs&iuerg at "chair site, 1X0 iar D ctccayt thtl :K' ta:.E:il aril

  5. Changes in the firn structure of the western Greenland Ice Sheet caused by recent warming

    DOE PAGES [OSTI]

    de la Peña, S.; Howat, I. M.; Nienow, P. W.; van den Broeke, M. R.; Mosley-Thompson, E.; Price, S. F.; Mair, D.; Noël, B.; Sole, A. J.

    2015-06-11

    Atmospheric warming over the Greenland Ice Sheet during the last 2 decades has increased the amount of surface meltwater production, resulting in the migration of melt and percolation regimes to higher altitudes and an increase in the amount of ice content from refrozen meltwater found in the firn above the superimposed ice zone. Here we present field and airborne radar observations of buried ice layers within the near-surface (0–20 m) firn in western Greenland, obtained from campaigns between 1998 and 2014. We find a sharp increase in firn-ice content in the form of thick widespread layers in the percolation zone,more » which decreases the capacity of the firn to store meltwater. The estimated total annual ice content retained in the near-surface firn in areas with positive surface mass balance west of the ice divide in Greenland reached a maximum of 74 ± 25 Gt in 2012, compared to the 1958–1999 average of 13 ± 2 Gt, while the percolation zone area more than doubled between 2003 and 2012. Increased melt and column densification resulted in surface lowering averaging –0.80 ± 0.39 m yr⁻¹ between 1800 and 2800 m in the accumulation zone of western Greenland. Since 2007, modeled annual melt and refreezing rates in the percolation zone at elevations below 2100 m surpass the annual snowfall from the previous year, implying that mass gain in the region is retained after melt in the form of refrozen meltwater. If current melt trends over high elevation regions continue, subsequent changes in firn structure will have implications for the hydrology of the ice sheet and related abrupt seasonal densification could become increasingly significant for altimetry-derived ice sheet mass balance estimates.« less

  6. Greenland Ice Sheet "Sliding" a Small Contributor to Future Sea-Level

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Rise | U.S. DOE Office of Science (SC) Greenland Ice Sheet "Sliding" a Small Contributor to Future Sea-Level Rise Advanced Scientific Computing Research (ASCR) ASCR Home About Research Facilities Science Highlights Benefits of ASCR Funding Opportunities Advanced Scientific Computing Advisory Committee (ASCAC) Community Resources Contact Information Advanced Scientific Computing Research U.S. Department of Energy SC-21/Germantown Building 1000 Independence Ave., SW Washington, DC

  7. Leak before break evaluation for main steam piping system made of SA106 Gr.C

    SciTech Connect

    Yang, Kyoung Mo; Jee, Kye Kwang; Pyo, Chang Ryul; Ra, In Sik

    1997-04-01

    The basis of the leak before break (LBB) concept is to demonstrate that piping will leak significantly before a double ended guillotine break (DEGB) occurs. This is demonstrated by quantifying and evaluating the leak process and prescribing safe shutdown of the plant on the basis of the monitored leak rate. The application of LBB for power plant design has reduced plant cost while improving plant integrity. Several evaluations employing LBB analysis on system piping based on DEGB design have been completed. However, the application of LBB on main steam (MS) piping, which is LBB applicable piping, has not been performed due to several uncertainties associated with occurrence of steam hammer and dynamic strain aging (DSA). The objective of this paper is to demonstrate the applicability of the LBB design concept to main steam lines manufactured with SA106 Gr.C carbon steel. Based on the material properties, including fracture toughness and tensile properties obtained from the comprehensive material tests for base and weld metals, a parametric study was performed as described in this paper. The PICEP code was used to determine leak size crack (LSC) and the FLET code was used to perform the stability assessment of MS piping. The effects of material properties obtained from tests were evaluated to determine the LBB applicability for the MS piping. It can be shown from this parametric study that the MS piping has a high possibility of design using LBB analysis.

  8. History of ancient copper smelting pollution during Roman and Medieval times recorded in Greenland ice

    SciTech Connect

    Hong, Sungmin; Candelone, J.P.; Patterson, C.C.; Boultron, C.F.

    1996-04-12

    Determination of copper concentrations in Greenland ice dated from seven millennia ago to the present showed values exceeding natural levels, beginning about 2500 years ago. This early large-scale pollution of the atmosphere of the Northern Hemisphere is attributed to emissions from the crude, highly polluting smelting technologies used for copper production during Roman and medieval times, especially in Europe and China. This study opens the way to a quantitative assessment of the history of early metal production, which was instrumental in the development of human cultures during ancient eras. 27 refs., 1 fig., 2 tabs.

  9. Study of the Phototransference in GR-200 Dosimetric Material and its Convenience for Dose Re-estimation

    SciTech Connect

    Baly, L.; Otazo, M. R.; Molina, D.; Pernas, R.

    2006-09-08

    A study of the phototransference of charges from deep to dosimetric traps in GR-200 material is presented and its convenience for dose re-estimation in the dose range between 2 and 100mSv is also analyzed. The recovering coefficient (RC) defined as the ratio between the phototransferred thermoluminescence (PTTL) and the original thermoluminescence (TL) of the dosimetric trap was used to evaluate the ratio of phototransferred charges from deep traps and the original charges in the dosimetric traps. The results show the convenience of this method for dose re-estimation for this material in the selected range of doses.

  10. Microstructural Aspects of Irradiation Damage in A508 Gr 4N Forging Steel: Composition and Flux Effects

    SciTech Connect

    M.G. Burke; R.J. Stofanak; J.M. Hyde; C.A. English; W.L. Server

    2002-10-09

    Neutron irradiation can promote significant changes in the microstructure and associated mechanical properties of low alloy steels. In particular, irradiation can induce the formation of non-equilibrium phases and segregation, which may lead to a degradation in toughness. In this study, the microstructural changes caused by neutron irradiation have been characterized in A508 Grade (Gr) 4N-type steels ({approx}3.5% Ni) using a variety of state-of-the-art analytical techniques including 3D-Atom Probe Field-Ion Microscopy and Small Angle Neutron Scattering, along with post-irradiation annealing studies combining Positron Annihilation Lineshape Analysis and hardness measurements. Important differences between conventional and ''superclean'' A508 Gr 4N steel have been identified in this investigation. The data indicate that Ni is not the controlling factor in the irradiation damage behavior of these materials; rather, the Mn content of the steel is a dominant factor in the irradiation-induced microstructural development of solute-related hardening features.

  11. Heat sources within the Greenland Ice Sheet: dissipation, temperate paleo-firn and cryo-hydrologic warming

    SciTech Connect

    Lthi, M. P.; Ryser, C.; Andrews, L. C.; Catania, G. A.; Funk, M.; Hawley, R. L.; Hoffman, M. J.; Neumann, T. A.

    2015-01-01

    Ice temperature profiles from the Greenland Ice Sheet contain information on the deformation history, past climates and recent warming. We present full-depth temperature profiles from two drill sites on a flow line passing through Swiss Camp, West Greenland. Numerical modeling reveals that ice temperatures are considerably higher than would be expected from heat diffusion and dissipation alone. The possible causes for this extra heat are evaluated using a Lagrangian heat flow model. The model results reveal that the observations can be explained with a combination of different processes: enhanced dissipation (strain heating) in ice-age ice, temperate paleo-firn, and cryo-hydrologic warming in deep crevasses.

  12. Heat sources within the Greenland Ice Sheet: dissipation, temperate paleo-firn and cryo-hydrologic warming

    DOE PAGES [OSTI]

    Lüthi, M. P.; Ryser, C.; Andrews, L. C.; Catania, G. A.; Funk, M.; Hawley, R. L.; Hoffman, M. J.; Neumann, T. A.

    2015-01-01

    Ice temperature profiles from the Greenland Ice Sheet contain information on the deformation history, past climates and recent warming. We present full-depth temperature profiles from two drill sites on a flow line passing through Swiss Camp, West Greenland. Numerical modeling reveals that ice temperatures are considerably higher than would be expected from heat diffusion and dissipation alone. The possible causes for this extra heat are evaluated using a Lagrangian heat flow model. The model results reveal that the observations can be explained with a combination of different processes: enhanced dissipation (strain heating) in ice-age ice, temperate paleo-firn, and cryo-hydrologic warmingmore » in deep crevasses.« less

  13. Seismicity on the western Greenland Ice Sheet: Surface fracture in the vicinity of active moulins

    SciTech Connect

    Carmichael, Joshua D.; Joughin, Ian; Behn, Mark D.; Das, Sarah; King, Matt A.; Stevens, Laura; Lizarralde, Dan

    2015-06-25

    We analyzed geophone and GPS measurements collected within the ablation zone of the western Greenland Ice Sheet during a ~35 day period of the 2011 melt season to study changes in ice deformation before, during, and after a supraglacial lake drainage event. During rapid lake drainage, ice flow speeds increased to ~400% of winter values, and icequake activity peaked. At times >7 days after drainage, this seismicity developed variability over both diurnal and longer periods (~10 days), while coincident ice speeds fell to ~150% of winter values and showed nightly peaks in spatial variability. Approximately 95% of all detected seismicity in the lake basin and its immediate vicinity was triggered by fracture propagation within near-surface ice (<330 m deep) that generated Rayleigh waves. Icequakes occurring before and during drainage frequently were collocated with the down flow (west) end of the primary hydrofracture through which the lake drained but shifted farther west and outside the lake basin after the drainage. We interpret these results to reveal vertical hydrofracture opening and local uplift during the drainage, followed by enhanced seismicity and ice flow on the downstream side of the lake basin. This region collocates with interferometric synthetic aperture radar-measured speedup in previous years and could reflect the migration path of the meltwater supplied to the bed by the lake. The diurnal seismic signal can be associated with nightly reductions in surface melt input that increase effective basal pressure and traction, thereby promoting elevated strain in the surficial ice.

  14. Seismicity on the western Greenland Ice Sheet: Surface fracture in the vicinity of active moulins

    DOE PAGES [OSTI]

    Carmichael, Joshua D.; Joughin, Ian; Behn, Mark D.; Das, Sarah; King, Matt A.; Stevens, Laura; Lizarralde, Dan

    2015-06-25

    We analyzed geophone and GPS measurements collected within the ablation zone of the western Greenland Ice Sheet during a ~35 day period of the 2011 melt season to study changes in ice deformation before, during, and after a supraglacial lake drainage event. During rapid lake drainage, ice flow speeds increased to ~400% of winter values, and icequake activity peaked. At times >7 days after drainage, this seismicity developed variability over both diurnal and longer periods (~10 days), while coincident ice speeds fell to ~150% of winter values and showed nightly peaks in spatial variability. Approximately 95% of all detected seismicitymore » in the lake basin and its immediate vicinity was triggered by fracture propagation within near-surface ice (<330 m deep) that generated Rayleigh waves. Icequakes occurring before and during drainage frequently were collocated with the down flow (west) end of the primary hydrofracture through which the lake drained but shifted farther west and outside the lake basin after the drainage. We interpret these results to reveal vertical hydrofracture opening and local uplift during the drainage, followed by enhanced seismicity and ice flow on the downstream side of the lake basin. This region collocates with interferometric synthetic aperture radar-measured speedup in previous years and could reflect the migration path of the meltwater supplied to the bed by the lake. The diurnal seismic signal can be associated with nightly reductions in surface melt input that increase effective basal pressure and traction, thereby promoting elevated strain in the surficial ice.« less

  15. Microwave signatures of ice hydrometeors from ground-based observations above Summit, Greenland

    DOE PAGES [OSTI]

    Pettersen, Claire; Bennartz, Ralf; Kulie, Mark S.; Merrelli, Aronne J.; Shupe, Matthew D.; Turner, David D.

    2016-04-15

    Multi-instrument, ground-based measurements provide unique and comprehensive data sets of the atmosphere for a specific location over long periods of time and resulting data compliment past and existing global satellite observations. This paper explores the effect of ice hydrometeors on ground-based, high-frequency passive microwave measurements and attempts to isolate an ice signature for summer seasons at Summit, Greenland, from 2010 to 2013. Data from a combination of passive microwave, cloud radar, radiosonde, and ceilometer were examined to isolate the ice signature at microwave wavelengths. By limiting the study to a cloud liquid water path of 40 gm–2 or less, themore » cloud radar can identify cases where the precipitation was dominated by ice. These cases were examined using liquid water and gas microwave absorption models, and brightness temperatures were calculated for the high-frequency microwave channels: 90, 150, and 225 GHz. By comparing the measured brightness temperatures from the microwave radiometers and the calculated brightness temperature using only gas and liquid contributions, any residual brightness temperature difference is due to emission and scattering of microwave radiation from the ice hydrometeors in the column. The ice signature in the 90, 150, and 225 GHz channels for the Summit Station summer months was isolated. As a result, this measured ice signature was then compared to an equivalent brightness temperature difference calculated with a radiative transfer model including microwave single-scattering properties for several ice habits. Initial model results compare well against the 4 years of summer season isolated ice signature in the high-frequency microwave channels.« less

  16. Diagenesis and porosity development associated with major sea level fluctuations, Upper Permian, Jameson land, east Greenland

    SciTech Connect

    Scholle, P.A.; Ulmer, D.S. ); Stemmerik, L. )

    1990-05-01

    The Upper Permian of Jameson Land includes two major carbonate sequences, represented by the Karstryggen and Wegener Halvoe formations. The initial Karstryggen transgression led to the development of a shallow marine platform with structurally controlled evaporite basins (salinas) separated by stromatolitic, peloidal, or micritic carbonate depositional areas. The Wegener Havloe sequence reflects more rapid and extensive transgression with the deposition of three subcycles of fully marine, platform, or biohermal carbonates containing minor evaporites near the basin margins. Bioherms (bryozoan-brachiopod-marine cement mounds) show > 100 m of relief, indicating that large relative sea level changes were involved. Both the Karstryggen and Wgener Havloe cycles were terminated by major regressions, which led to karstic and/or fluvial incision of the underlying sequences. Not surprisingly, carbonate and evaporite diagenesis was greatly affected by these regional or eustatic sea level fluctuations. Evaporites dissolved or were replaced by calcite and celestite under the influence of meteoric waters. Limestones show collapse brecciation, grain leaching, soil development, and characteristic vadose and phreatic cements. Most significantly meteoric flushing led to massive dissolution of botryoidal marine cements (aragonite and probable high-Mg calcite) within biohermal facies on the Wegener Peninsula. This early porosity resurrection led to the preservation of porous bioherm core zones until hydrocarbon migration. Only late (posthydrocarbon), probably hydrothermal fluid flow led to cementation of the bioherm cores while expelling most of the reservoired hydrocarbons. If the sea level changes affecting the Greenlandic Permian are eustatic, then this study may provide significant clues to porosity development throughout the largely unexplored northern Zechstein basin.

  17. Depositional environment and organic geochemistry of the Upper Permian Ravenfjeld Formation source rock in East Greenland

    SciTech Connect

    Christiansen, F.G.; Piasecki, S.; Stemmerik, L. ); Telnaes, N. )

    1993-09-01

    The Upper Permian Ravnefjeld Formation in East Greenland is composed of shales that laterally pass into carbonate buildups and platforms of the Wegener Halvo Formation. The Ravnefjeld Formation is subdivided into five units that can be traced throughout the Upper Permian depositional basin. Two of the units are laminated and organic rich and were deposited under anoxic conditions. They are considered good to excellent source rocks for liquid hydrocarbons with initial average TOC (total organic carbon) values between 4 and 5% and HI (hydrogen index) between 300 and 400. The cumulative source rocks are separated and enclosed by three units of bioturbated siltstone with a TOC of less than 0.5% and an HI of less than 100. These siltstones were deposited under relatively oxic conditions. The organic geochemistry of the source rocks is typical for marine source rocks with some features normally associated with carbonate/evaporite environments [low Pr/Ph (pristane/phytane), low CPI (carbon preference index), distribution of tricyclic and pentacyclic terpanes]. The establishment of anoxic conditions and subsequent source rock deposition was controlled by eustatic sea level changes. The subenvironment (paleogeographic setting, influx of carbonate material, water depth, salinity) has some influence on a number of bulk parameters [TOC-HI relations, TOC-TS (total sulfur) relations] and, in particular, biomarker parameters such as Pr/Ph and terpane ratios. All the basal shales or shales in the vicinity of carbonate buildups of platforms are characterized by low Pr/Ph, high C[sub 23] tricyclic terpanes, and high C[sub 35] and C[sub 33] hopanes. 52 refs., 20 figs., 3 tabs.

  18. G-r

    Office of Legacy Management (LM)

    ... AppnximntaLy 265 tons hwe beu shipprd to .Si-sondr this month. 1 UC: mrtelti cc one UCE coLosd haTo been rrcelved. car ml11 be doll.r+C .' uuery 2s. Tba d&C XI;: ba Cellvcrad ...

  19. Greenland and Antarctic mass balances for present and doubled atmospheric CO{sub 2} from the GENESIS version-2 global climate model

    SciTech Connect

    Thompson, S.L.; Pollard, D.

    1997-05-01

    As anthropogenic greenhouse warming occurs in the next century, changes in the mass balances of Greenland and Antarctica will probably accelerate and may have significant effects on global sea level. Recent trends and possible future changes in these mass balances have received considerable attention in the glaciological literature, but until recently relatively few general circulation modeling (GCM) studies have focused on the problem. However, there are two significant problems in using GCMs to predict mass balance distributions on ice sheets: (i) the relatively coarse GCM horizontal resolution truncates the topography of the ice-sheet flanks and smaller ice sheets such as Greenland, and (ii) the snow and ice physics in most GCMs does not include ice-sheet-specific processes such as the refreezing of meltwater. Two techniques are described that attack these problems, involving (i) an elevation-based correction to the surface meteorology and (ii) a simple a posteriori correction for the refreezing of meltwater following Pfeiffer et al. Using these techniques in a new version 2 of the Global Environmental and Ecological Simulation of Interactive Systems global climate model, the authors present global climate and ice-sheet mass-balance results from two equilibrated runs for present and doubled atmospheric CO{sub 2}. This GCM is well suited for ice-sheet mass-balance studies because (a) the surface can be represented at a finer resolution (2{degrees} lat x 2{degrees} long) than the atmospheric GCM, (b) the two correction techniques are included as part of the model, and the model`s mass balances for present-day Greenland and Antarctica are realistic. 131 refs., 23 figs., 2 tabs.

  20. Diagenetic history and hydrocarbon potential of Upper Permian carbonate buildups, Wegener Halvoe area, Jameson Land basin, east Greenland

    SciTech Connect

    Scholle, P.A.; Ulmer, D.S. ); Stemmerik, L. )

    1991-04-01

    The Upper Permian of Jameson Land includes two carbonate sequences, the Karstryggen and Wegener Halvoe formations. The Karstryggen Formation contains hypersaline carbonates and localized evaporites that were heavily weathered and dissected prior to deposition of the overlying strata. The overlying Wegener Halvoe Formation represents an abrupt and extensive marine inundation over the underlying karstified Karstryggen surface. Bryozoan-brachiopod-algal-cement buildups of the Wegener Halvoe Formation are localized on karstic highs, and show up to 150 m of depositional relief. The diagenetic histories of the core and flank facies are very different. Core facies porosity was initially obliterated by marine cements, but repeated meteoric exposure altered unstable core facies constituents. This alteration produced extensive secondary porosity through grain and cement leaching with local collapse brecciation. Flank strata, however, underwent little sea-floor diagenesis, and low permeability and mineralogically stable grain composition protected these strata from meteoric alteration. Subsequent fracturing and hydrothermal fluid flow, however, flushed hydrocarbons and filled pores with ferroan calcite, barite, fluorite, galena, and baroque dolomite. This heating and flushing is thought to have been especially intense in the Wegener Halvoe region; thus, more basinal areas may still have reservoirs containing significant oil in equivalent Upper Permian limestones. If, as is likely, the sea level changes affecting the Greenland Permian were eustatic, then this study may provide significant clues to porosity development throughout the largely unexplored northern Zechstein basin and the Arctic basin of the Barent Sea. This study also provides some important connections to the probably time-equivalent Guadalupian carbonate reservoir rocks of west Texas-New Mexico and Wyoming.

  1. On the scalability of the Albany/FELIX first-order Stokes approximation ice sheet solver for large-scale simulations of the Greenland and Antarctic ice sheets

    DOE PAGES [OSTI]

    Tezaur, Irina K.; Tuminaro, Raymond S.; Perego, Mauro; Salinger, Andrew G.; Price, Stephen F.

    2015-01-01

    We examine the scalability of the recently developed Albany/FELIX finite-element based code for the first-order Stokes momentum balance equations for ice flow. We focus our analysis on the performance of two possible preconditioners for the iterative solution of the sparse linear systems that arise from the discretization of the governing equations: (1) a preconditioner based on the incomplete LU (ILU) factorization, and (2) a recently-developed algebraic multigrid (AMG) preconditioner, constructed using the idea of semi-coarsening. A strong scalability study on a realistic, high resolution Greenland ice sheet problem reveals that, for a given number of processor cores, the AMG preconditionermore » results in faster linear solve times but the ILU preconditioner exhibits better scalability. A weak scalability study is performed on a realistic, moderate resolution Antarctic ice sheet problem, a substantial fraction of which contains floating ice shelves, making it fundamentally different from the Greenland ice sheet problem. Here, we show that as the problem size increases, the performance of the ILU preconditioner deteriorates whereas the AMG preconditioner maintains scalability. This is because the linear systems are extremely ill-conditioned in the presence of floating ice shelves, and the ill-conditioning has a greater negative effect on the ILU preconditioner than on the AMG preconditioner.« less

  2. The influence of air temperature inversions on snowmelt and glacier mass-balance simulations, Ammassalik island, SE Greenland

    SciTech Connect

    Mernild, Sebastian Haugard [Los Alamos National Laboratory; Liston, Glen [COLORADO STATE UNIV.

    2009-01-01

    In many applications, a realistic description of air temperature inversions is essential for accurate snow and glacier ice melt, and glacier mass-balance simulations. A physically based snow-evolution modeling system (SnowModel) was used to simulate eight years (1998/99 to 2005/06) of snow accumulation and snow and glacier ice ablation from numerous small coastal marginal glaciers on the SW-part of Ammassalik Island in SE Greenland. These glaciers are regularly influenced by inversions and sea breezes associated with the adjacent relatively low temperature and frequently ice-choked fjords and ocean. To account for the influence of these inversions on the spatiotemporal variation of air temperature and snow and glacier melt rates, temperature inversion routines were added to MircoMet, the meteorological distribution sub-model used in SnowModel. The inversions were observed and modeled to occur during 84% of the simulation period. Modeled inversions were defined not to occur during days with strong winds and high precipitation rates due to the potential of inversion break-up. Field observations showed inversions to extend from sea level to approximately 300 m a.s.l., and this inversion level was prescribed in the model simulations. Simulations with and without the inversion routines were compared. The inversion model produced air temperature distributions with warmer lower elevation areas and cooler higher elevation areas than without inversion routines due to the use of cold sea-breeze base temperature data from underneath the inversion. This yielded an up to 2 weeks earlier snowmelt in the lower areas and up to 1 to 3 weeks later snowmelt in the higher elevation areas of the simulation domain. Averaged mean annual modeled surface mass-balance for all glaciers (mainly located above the inversion layer) was -720 {+-} 620 mm w.eq. y{sup -1} for inversion simulations, and -880 {+-} 620 mm w.eq. y{sup -1} without the inversion routines, a difference of 160 mm w.eq. y

  3. Evaluation of the use of common sculpin (Myoxocephalus scorpius) organ histology as bioindicator for element exposure in the fjord of the mining area Maarmorilik, West Greenland

    SciTech Connect

    Sonne, Christian; Bach, Lis; Søndergaard, Jens; Rigét, Frank F.; Dietz, Rune; Mosbech, Anders; Leifsson, Pall S.; Gustavson, Kim

    2014-08-15

    The former Black Angel lead–zinc mine in Maarmorilik, West Greenland, is a historic example of how mining activity may result in a significant impact on the surrounding fjord system in terms of elevated concentrations of especially lead (Pb) and zinc (Zn) in seawater, sediments and surrounding biota. In order to shed light on the present contamination and possible effects in the fjord we initiated a range of studies including a pilot study on gill and liver morphology of common sculpins (Myoxocephalus scorpius) around Maarmorilik. Sculpins were caught and sampled at five different stations known to represent a gradient of Pb concentrations. Fish livers from all specimens were analyzed for relevant elements in the area: Fe, Zn, As, Cu, Se, Cd, Pb, Ag, Hg, Co and Ni. Lead, As and Hg showed significant differences among the five stations. For 20% of the sculpins, Hg concentrations were in the range of lowest observed effect dose (LOED) of 0.1–0.5 μg/g ww for toxic threshold on reproduction and subclinical endpoints. Likewise LOEDs for tissue lesions, LOEDs for biochemistry, growth, survival and reproduction were exceeded for Cd (0.42–1.8 μg/g ww) and for As (11.6 μg/g ww) in 28% and 85% of the sculpins, respectively. Similar to this, the no observed effect dose (NOED) for biochemistry was exceeded for Pb (0.32 μg/g ww) and for growth, mortality and reproduction for Zn (60–68 μg/g ww) in 33% and 24% of the sculpins, respectively. For all sculpins, females were significantly larger than males and for five of the elements (Fe, Co, Ni, Cu, Se) females had higher concentrations. The chronic lesions observed in liver (mononuclear cell infiltrates, necrosis, vacuolar hepatocytes, portal fibrosis, bile duct hyperplasia, active melanomacrophage centers) and gills (fusion and edema of secondary lamellae, laminar telangiectasis, mononuclear cell infiltrates, blebs) were similar to those in the literature studies for both wild and laboratory exposed sculpins and

  4. Greenland New Energy | Open Energy Information

    OpenEI (Open Energy Information) [EERE & EIA]

    China Sector: Solar Product: China-based firm involved in silicon thin film solar cell technology. Coordinates: 31.966261, 119.472687 Show Map Loading map......

  5. Microsoft Word - Gr-hBN boundary state (050214)

    Office of Scientific and Technical Information (OSTI)

    ... B atoms are specified in blue, N atoms are green, carbons are black, and Cu atoms are ... The boundary states are located around 0.1 eV above the Fermi energy. The calculations ...

  6. Sandia's ice sheet modeling of Greenland, Antarctica helps predict...

    National Nuclear Security Administration (NNSA)

    Institute of Technology, Florida State University, the University of Bristol, the University of Texas at Austin, the University of South Carolina and New York University. ...

  7. Greenland Ice Sheet Modeling Update (Conference) | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    Resource Relation: Conference: Regional Arctic System Model workshop ; 2014-06-04 - ... Sponsoring Org: DOELANL Country of Publication: United States Language: English Subject: ...

  8. Greenland Ice Sheet "Sliding" a Small Contributor to Future Sea...

    Office of Science (SC)

    ... by DOE's Office of Science under contract DE-AC02-05CH11231) and at Oak Ridge National Laboratory (supported by DOE's Office of Science under contract DE-AC05-00OR22725). ...

  9. Meltwater effects on flow of Greenland's ice sheet less severe...

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    more to future sea-level rise than when considering the increases in melting alone," said co-author Stephen Price of the Los Alamos National Laboratory Climate Ocean and Sea...

  10. New Method Relates Greenland Ice Sheet Changes to Sea-Level Rise...

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... Research from Edwards et al. 2014a was funded by the ice2sea programme from the European Union (EU) 7th Framework Programme (grant number 226375; ice2sea contribution number 120). ...

  11. Update on Greenland Ice Sheet Simulations In CISM and CESM (Conference...

    Office of Scientific and Technical Information (OSTI)

    Authors: Lipscomb, William Henry 1 + Show Author Affiliations Los Alamos National Laboratory Publication Date: 2016-02-12 OSTI Identifier: 1238137 Report Number(s): ...

  12. EM Press Releases | Department of Energy

    Office of Energy Efficiency and Renewable Energy (EERE) (indexed site)

    is awarding two separate grants together totaling about 7 million to the Commonwealth of Kentucky, Energy and Environment Cabinet (EEC) for regulatory oversight of the Paducah...

  13. Management Council - Center for Solar and Thermal Energy Conversion

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Organization  MANAGEMENT COUNCIL Peter Green, Dir. MSE Rachel Goldman MSE Ctirad Uher Physics Jamie Phillips EECS Max Shtein MSE Roy Clarke Physics Ted Goodson III Chemistry ...

  14. Assessment of Negligible Creep, Off-Normal Welding and Heat Treatment of Gr91 Steel for Nuclear Reactor Pressure Vessel Application

    SciTech Connect

    Ren, Weiju; Terry, Totemeier

    2006-10-01

    Two different topics of Grade 91 steel are investigated for Gen IV nuclear reactor pressure vessel application. On the first topic, negligible creep of Grade 91 is investigated with the motivation to design the reactor pressure vessel in negligible creep regime and eliminate costly surveillance programs during the reactor operation. Available negligible creep criteria and creep strain laws are reviewed, and new data needs are evaluated. It is concluded that modifications of the existing criteria and laws, together with their associated parameters, are needed before they can be reliably applied to Grade 91 for negligible creep prediction and reactor pressure vessel design. On the second topic, effects of off-normal welding and heat treatment on creep behavior of Grade 91 are studied with the motivation to better define the control over the parameters in welding and heat treatment procedures. The study is focused on off-normal austenitizing temperatures and improper cooling after welding but prior to post-weld heat treatment.

  15. Investigators - Center for Solar and Thermal Energy Conversion

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Investigators Director Name Department Email Peter Green MSE/ChemE pfgreen@umich.edu Principal Investigators Name Department Email Akram Boukai MSE boukai@umich.edu Roy Clarke Physics royc@umich.edu Barry Dunietz Chemistry bdunietz@umich.edu Steve Forrest EECS/Phys/MSE stevefor@umich.edu Eitan Geva Chemistry eitan@umich.edu Rachel Goldman MSE/EECS/Phys rsgold@umich.edu Ted Goodson Chemistry tgoodson@umich.edu L (Jay) Guo EECS guo@umich.edu Massoud Kaviany ME kaviany@umich.edu John Kieffer MSE

  16. Fall 2013 Working Groups

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    September 27 EECS 3427 Adam Barito Joe Furgal Heidi Phillips October 25 1504 GGBrown Dan Wilcox David Bilby Shu-Hao Chang November 22 1504 GGBrown Bing Huan Anton Li Anurag Panda...

  17. # Energy Measuremenfs Group

    Office of Legacy Management (LM)

    ri EECE Energy Measuremenfs Group SUMMARY REPORT . AiRIAL R4DIOLOGICAL SURVEY - NIAGARA ... Herbirt F. Hahn, Department of Energy PERFDRflED BY EGtf, INC. UNDER CONTRACT NO. ...

  18. INSL5 may be a unique marker of colorectal endocrine cells and neuroendocrine tumors

    SciTech Connect

    Mashima, Hirosato; Ohno, Hideki; Yamada, Yumi; Sakai, Toshitaka; Ohnishi, Hirohide

    2013-03-22

    Highlights: ► INSL5 is expressed in enteroendocrine cells along the colorectum. ► INSL5 is expressed increasingly from proximal colon to rectum. ► INSL5 co-localizes rarely with chromogranin A. ► All rectal neuroendocrine tumors examined expressed INSL5. -- Abstract: Insulin-like peptide 5 (INSL5) is a member of the insulin superfamily, and is a potent agonist for RXFP4. We have shown that INSL5 is expressed in enteroendocrine cells (EECs) along the colorectum with a gradient increase toward the rectum. RXFP4 is ubiquitously expressed along the digestive tract. INSL5-positive EECs have little immunoreactivity to chromogranin A (CgA) and might be a unique marker of colorectal EECs. CgA-positive EECs were distributed normally along the colorectum in INSL5 null mice, suggesting that INSL5 is not required for the development of CgA-positive EECs. Exogenous INSL5 did not affect the proliferation of human colon cancer cell lines, and chemically-induced colitis in INSL5 null mice did not show any significant changes in inflammation or mucosal healing compared to wild-type mice. In contrast, all of the rectal neuroendocrine tumors examined co-expressed INSL5 and RXFP4. INSL5 may be a unique marker of colorectal EECs, and INSL5–RXFP4 signaling might play a role in an autocrine/paracrine fashion in the colorectal epithelium and rectal neuroendocrine tumors.

  19. November

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    National Laboratory, won an R&D 100 Award. - 112015 Greenland ice loss. New climate model predicts likelihood of Greenland ice melt, sea level rise and dangerous temperatures A...

  20. Influence of long-time stress relief treatments on the dynamic fracture toughness properties of ASME SA508 C1 2a and ASME SA533 GR B C12 pressure vessel steels

    SciTech Connect

    Logsdon, W.A.

    1982-03-01

    Dynamic fracture toughness tests were performed on materials which had been subjected to one of three long-time post weld type stress relief heat treatments: 48 hours at 1000/degree/F (538/degree/C), 24 hours at 1125/degree/F (607/degree/C), and 48 hours at 1125/degree/F (607/degree/C). Linear elastic K/sub Id/ results were obtained at low temperatures while J-integral techniques were utilized to evaluate dynamic fracture toughness over the transition and upper shelf temperature ranges. Tensile, Charpy impact, and drop weight nil-ductility transition tests as well as room temperature, air environment fatigue crack growth rate tests (SA508 Cl 2a only) were also performed. The fracture toughness of both materials exceeded the ASME specified minimum reference toughness K/sub IR/ curve. 17 refs.

  1. ARM - Facility News Article

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    8, 2012 [Data Announcements, Facility News] New Data from Greenland for Arctic Climate Research Bookmark and Share Instruments for ICECAPS operate on top and inside of the Mobile Science Facility at Summit Station in Greenland. Instruments for ICECAPS operate on top and inside of the Mobile Science Facility at Summit Station in Greenland. In 2010, researchers installed a powerful suite of climate and weather instruments at Greenland's frozen research outpost, Summit Station, for a long-term

  2. Washington County, Arkansas: Energy Resources | Open Energy Informatio...

    OpenEI (Open Energy Information) [EERE & EIA]

    Farmington, Arkansas Fayetteville, Arkansas Goshen, Arkansas Greenland, Arkansas Johnson, Arkansas Lincoln, Arkansas Prairie Grove, Arkansas Springdale, Arkansas Tontitown,...

  3. First increment of second specimen results to performance assessment-long term corrosion

    SciTech Connect

    Wang, F.

    1998-01-01

    In this correspondence, we report the 6 month corrosion data of corrosion resistant alloys (alloys 825, C22 & C4, and Ti Gr 12 & Ti Gr 16, and Inconel 625) and one year data of corrosion-allowance materials (A387 Gr22, A516 Gr55 and A27 Gr70-40), intermediate resistance alloys (Monel 400 and CDA 715) and corrosion resistant materials (alloys C22 and 625 only).

  4. CX-003582: Categorical Exclusion Determination

    Energy.gov [DOE]

    Energy Efficiency and Conservation Strategy (EECS) and Air Conditioning Unity Replacement-Police StationCX(s) Applied: A11, B1.4, B2.5, B5.1Date: 08/23/2010Location(s): Wauwatosa, WisconsinOffice(s): Energy Efficiency and Renewable Energy

  5. CX-001547: Categorical Exclusion Determination

    Energy.gov [DOE]

    St. Tammany Parish, Louisiana American Recovery and Reinvestment Act Energy Efficiency and Conservation Block Grant - Energy Efficiency and Conservation Summary (EECS) (S)CX(s) Applied: A9, A11, B5.1Date: 03/31/2010Location(s): LouisianaOffice(s): Energy Efficiency and Renewable Energy, Golden Field Office

  6. 1

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    drainage system are lacking and its evolution over the melt season is poorly understood. "Everyone wants to know what's happening under Greenland as it experiences more and...

  7. Rockingham County, New Hampshire: Energy Resources | Open Energy...

    OpenEI (Open Energy Information) [EERE & EIA]

    New Hampshire Derry, New Hampshire East Kingston, New Hampshire Epping, New Hampshire Exeter, New Hampshire Fremont, New Hampshire Greenland, New Hampshire Hampstead, New...

  8. EC Publications

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... French Polynesia Gabon Gambia Georgia Germany Ghana Greece Greenland Grenada Guam Guatemala Guinea Guinea-Bissau Guyana Haiti Honduras Hong Kong Hungary Iceland India Indonesia ...

  9. MELCOR / CSARP / MCAP / IMUG / MACCS Meetings 2016

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... French Polynesia Gabon Gambia Georgia Germany Ghana Greece Greenland Grenada Guam Guatemala Guinea Guinea-Bissau Guyana Haiti Honduras Hong Kong Hungary Iceland India Indonesia ...

  10. SNL-ESSC (Sandia National Laboratories - Extreme Sea State Contour...

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... French Polynesia Gabon Gambia Georgia Germany Ghana Greece Greenland Grenada Guam Guatemala Guinea Guinea-Bissau Guyana Haiti Honduras Hong Kong Hungary Iceland India Indonesia ...

  11. Workbook Contents

    Energy Information Administration (EIA) (indexed site)

    ... Exports to Greenland of Petroleum Coke (Thousand Barrels)","U.S. Exports to Guatemala of Petroleum Coke (Thousand Barrels)","U.S. Exports to Honduras of Petroleum Coke ...

  12. SNL-Delft3D-CEC

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... French Polynesia Gabon Gambia Georgia Germany Ghana Greece Greenland Grenada Guam Guatemala Guinea Guinea-Bissau Guyana Haiti Honduras Hong Kong Hungary Iceland India Indonesia ...

  13. Offshore Wind RD&D: Large Offshore Rotor Development

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... French Polynesia Gabon Gambia Georgia Germany Ghana Greece Greenland Grenada Guam Guatemala Guinea Guinea-Bissau Guyana Haiti Honduras Hong Kong Hungary Iceland India Indonesia ...

  14. December

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Laboratory depicts sea surface temperatures around Greenland from October 2010. Effect of ocean temperature on southwestern U.S. climate analyzed Researchers concluded...

  15. NERSC Supercomputers Help Explain the Last Big Freeze

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Atlantic (near Greenland), allowing it to disrupt the ocean's heat engine. "With 18 kilometers between each grid-point, we have the highest resolution ocean model in paleoclimate....

  16. Effect of ocean temperature on southwestern U.S. climate analyzed

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    depicts sea surface temperatures around Greenland from October 2010. Assuming that the past is a good indicator of the future, the scientists conclude that there should be...

  17. The use of electrical impedance spectroscopy for monitoring the hydration products of Portland cement mortars with high percentage of pozzolans

    SciTech Connect

    Cruz, J.M.; Fita, I.C.; Soriano, L.; Pay, J.; Borrachero, M.V.

    2013-08-15

    In this paper, mortars and pastes containing large replacement of pozzolan were studied by mechanical strength, thermogravimetric analysis (TGA), scanning electronic microscopy (SEM), mercury intrusion porosimetry (MIP) and electrical impedance spectroscopy (EIS). The effect of metakaolin (35%) and fly ash (60%) was evaluated and compared with an inert mineral addition (andalusite). The portlandite content was measured, finding that the pozzolanic reaction produced cementing systems with all portlandite fixed. The EIS measurements were analyzed by the equivalent electrical circuit (EEC) method. An EEC with three branches in parallel was applied. The dc resistance was related to the degree of hydration and allowed us to characterize plain and blended mortars. A constant phase element (CPE) quantified the electrical properties of the hydration products located in the solidsolution interface and was useful to distinguish the role of inert and pozzolanic admixtures present in the cement matrix.

  18. Risk Group and Biosafety Level Definitions

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Group and Biosafety Level Definitions European Economic Community (DIRECTIVE 93/88/EEC, Oct. 1993) (1) Group 1 biological agent means one that is unlikely to cause human disease; (2) Group 2 biological agent means one that can cause human disease and might be a hazard to workers; it is unlikely to spread to the community; there is usually effective prophylaxis or treatment available; (3) Group 3 biological agent means one that can cause severe human disease and present a serious hazard to

  19. Research Program - Center for Solar and Thermal Energy Conversion

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    In the Inorganic PV thrust, we develop nanostructured materials architectures for solar energy conversion by engineering absorption and transport properties not available in the bulk. In particular, we aim to exploit unique quantum effects at the nanoscale which are promising for the realization of new paradigms in solar energy conversion such as intermediate band or hot carrier solar cells. Thrust Leaders: Prof. Rachel Goldman (MSE)&nbspand Prof. Jamie Phillips (EECS) Recent Publications -

  20. Software-Defined Solutions for Managing Energy Use in Small Commercial

    Office of Energy Efficiency and Renewable Energy (EERE) (indexed site)

    Buildings | Department of Energy Software-Defined Solutions for Managing Energy Use in Small Commercial Buildings Software-Defined Solutions for Managing Energy Use in Small Commercial Buildings Lead Performer: University of California, Berkeley Project Partners: -- California Institute for Energy & Enviornment - Berkeley, CA -- Software Defined Buildings/EECS/UC Berkeley - Berkeley, CA -- Western Regional Cooling Center/UC Davis - Davis, CA -- Lawrence Berkeley National Laboratory -

  1. Edge equilibrium code for tokamaks

    SciTech Connect

    Li, Xujing; Drozdov, Vladimir V.

    2014-01-15

    The edge equilibrium code (EEC) described in this paper is developed for simulations of the near edge plasma using the finite element method. It solves the Grad-Shafranov equation in toroidal coordinate and uses adaptive grids aligned with magnetic field lines. Hermite finite elements are chosen for the numerical scheme. A fast Newton scheme which is the same as implemented in the equilibrium and stability code (ESC) is applied here to adjust the grids.

  2. Analyzing

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Analyzing the Effect of Different Programming Models Upon Performance and Memory Usage on Cray XT5 Platforms Hongzhang Shan Future Technology Group, Computational Research Division, Lawrence Berkeley National Laboratory, Berkeley, CA 94720 Haoqiang Jin NAS Division, NASA Arms Research Center, Moffett Field, CA 94035-1000 Karl Fuerlinger University of California at Berkeley, EECS Department, Computer Science Division Berkeley, CA 94720 Alice Koniges, Nicholas J. Wright NERSC, Lawrence Berkeley

  3. ARM - Publications: Science Team Meeting Documents

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Inferring Optical Depth of Broken Clouds above Green Vegetation. Part I:Methodology for Surface- and Aircraft-based Observations Barker, H.W. (a), Marshak, A. (b), Pavloski C.F. (c), and Clothiaux E.E.(c), Environment Canada (a), UMBC/JCET (b), The Pennsylvania State University (c) Eleventh Atmospheric Radiation Measurement (ARM) Science Team Meeting A method for inferring cloud optical depth is introduced and assessed using simulated radiometric measurements produced by a 3D Monte Carlo

  4. ARM - Different Climates

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Some places near the North and South Poles, such as Antarctica and Greenland, are extremely cold and dry. Amount of Solar Radiation The main cause of the variation of temperature ...

  5. 1

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    The Greenland and Antarctic ice sheets will make a dominant contribution to twenty-first century sea-level rise if current climate trends continue, studied in a five-year project ...

  6. LMS-AMC-S01980-0-0.cdr

    Office of Legacy Management (LM)

    1965-2005 Year Pollock Pacific Cod Sable Fish Yellow Fin Sole Greenland Turbot Arrow Tooth Flounder a Rock Sole c Other Flat Fish Alaska Plaice Pacific Ocean Complex b Pacific ...

  7. Women @ Energy: Shannon Goodwin | Department of Energy

    Office of Environmental Management (EM)

    ... jungles, mountains and beaches of Borneo, spent weeks camping on an island off the coast of Belize, trekked the Inca Trail in Peru, and adventure travel in Iceland and Greenland. ...

  8. ARM - Facility News Article

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    10, 2010 [Facility News] Supporting Science at Summit Station, Greenland Bookmark and Share This month, an ARM micropulse lidar and ceilometer began collecting data from Summit Station in Greenland as part of the ICECAPS field campaign that runs through October 2014. Scientist Matthew Shupe joined colleagues on location to install the ICECAPS mobile laboratory, documenting their progress through his field blog. Great job, Matt! Visit the campaign website for more information

  9. Sandia National Laboratories:

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    05, 2016 Articles Nondestructive Testing Nondestructive Testing: Sandia looks inside composites Sandia takes home three national tech transfer awards Decon, bombs, and above and beyond Sandians win Black Engineer of the Year awards Sandians win Black Engineer of the Year awards Ice sheet modeling of Greenland, Antarctica helps predict sea-level rise Ice sheet modeling of Greenland, Antarctica helps predict sea-level rise Making waves Making waves Grid modernization Grid modernization New Mexico

  10. Oak Ridge National Laboratory | National Nuclear Security Administration

    National Nuclear Security Administration (NNSA)

    Oak Ridge National Laboratory A snapshot of NNSA's counterterrorism mission NNSA's mission of counterterrorism and counterproliferation is supported through innovative science and technology. Recently, Associate Administrator and Deputy Undersecretary for Counterterrorism and Counterproliferation Jay Tilden visited Oak Ridge National Laboratory (ORNL) and met with... Sandia's ice sheet modeling of Greenland, Antarctica helps predict sea-level rise The Greenland and Antarctic ice sheets will make

  11. climate | National Nuclear Security Administration

    National Nuclear Security Administration (NNSA)

    climate NNSA labs fight fire with simulation Fire season is in full swing in the driest parts of the United States, and capabilities of NNSA's labs are helping equip firefighters in the heated battle to save property and environment. NNSA's labs are perfectly suited to support emergency response related to fire. A long history of... Sandia's ice sheet modeling of Greenland, Antarctica helps predict sea-level rise The Greenland and Antarctic ice sheets will make a dominant contribution to 21st

  12. ornl | National Nuclear Security Administration

    National Nuclear Security Administration (NNSA)

    ornl A snapshot of NNSA's counterterrorism mission NNSA's mission of counterterrorism and counterproliferation is supported through innovative science and technology. Recently, Associate Administrator and Deputy Undersecretary for Counterterrorism and Counterproliferation Jay Tilden visited Oak Ridge National Laboratory (ORNL) and met with... Sandia's ice sheet modeling of Greenland, Antarctica helps predict sea-level rise The Greenland and Antarctic ice sheets will make a dominant contribution

  13. Gabriel Rodriguez-Calero > Postdoc - Abrua Group > Researchers...

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Gabriel Rodriguez-Calero Postdoc - Abrua Group gr235@cornell.edu Gabriel received his PhD in Summer 2014...

  14. Thermal Gradient Holes At Breitenbush Hot Springs Area (Ingebritsen...

    OpenEI (Open Energy Information) [EERE & EIA]

    (1993) Heat Flow From Four New Research Drill Holes In The Western Cascades, Oregon, Usa Additional References Retrieved from "http:en.openei.orgwindex.php?titleThermalGr...

  15. Selecting The Optimal Logging Suite For Geothermal Reservoir...

    OpenEI (Open Energy Information) [EERE & EIA]

    and tensile wall fractures, and were adequate to detect stratigraphic features. Density, photo-electric factor (PEF), neutron, and gamma ray (GR) logs provided sufficient...

  16. Neutron Log At Alum Area (Moos & Ronne, 2010) | Open Energy Informatio...

    OpenEI (Open Energy Information) [EERE & EIA]

    Technique Neutron Log Activity Date Usefulness useful DOE-funding Unknown Notes Density, photo-electric factor (PEF), neutron, and gamma ray (GR) logs provided sufficient...

  17. Gamma Log At Alum Area (Moos & Ronne, 2010) | Open Energy Information

    OpenEI (Open Energy Information) [EERE & EIA]

    Technique Gamma Log Activity Date Usefulness useful DOE-funding Unknown Notes Density, photo-electric factor (PEF), neutron, and gamma ray (GR) logs provided sufficient...

  18. Micro-Earthquake At Coso Geothermal Area (2007) | Open Energy...

    OpenEI (Open Energy Information) [EERE & EIA]

    area Julian, B.R.; Foulger, G.R. (1 January 2010) IMPROVED METHODS FOR MAPPING PERMEABILITY AND HEAT SOURCES IN GEOTHERMAL AREAS USING MICROEARTHQUAKE DATA Additional...

  19. Lion Energy SA | Open Energy Information

    OpenEI (Open Energy Information) [EERE & EIA]

    search Name: Lion Energy SA Place: Athens, Greece Zip: GR 152 35 Sector: Hydro, Hydrogen, Solar Product: Lion Energy owns proprietary technologies for conversion of waste...

  20. A Cloud Data Sharing Platform for Real-time PMU Data

    Office of Energy Efficiency and Renewable Energy (EERE) (indexed site)

    A Cloud Data Sharing Platform for Real-time PMU Data Carl Hauser Clinical Associate Professor School of Electrical Engineering and Computer Science Washington State University hauser@eecs.wsu.edu PSERC Public Webinar September 13, 2016 2:00-3:00 p.m. Eastern Time (11:00-12:00 p.m. Pacific) Description: We present the results of a study conducted by WSU, Cornell and ISO-NE aimed at understanding the practical challenges associated with using cloud computing infrastructures to monitor PMU devices

  1. Meeting PMU Data Quality Requirements for Mission Critical Applications

    Office of Energy Efficiency and Renewable Energy (EERE) (indexed site)

    Meeting PMU Data Quality Requirements for Mission Critical Applications Anurag Srivastava School of Electrical Engineering and Computer Science Washington State University asrivast@eecs.wsu.edu PSERC Public Webinar Tuesday, November 17, 2015 2:00-3:00 p.m. Eastern Time (11:00-12:00 p.m. Pacific) If you plan to use the phone bridge, use the NEW number: 877-820-7831 (passcode: 965722#). Description: Phasor Measurement Units (PMU's) provide synchronized measurements at high rates for wide area

  2. Control system and method for a hybrid electric vehicle

    DOEpatents

    Tamor, Michael Alan

    2001-03-06

    Several control methods are presented for application in a hybrid electric vehicle powertrain including in various embodiments an engine, a motor/generator, a transmission coupled at an input thereof to receive torque from the engine and the motor generator coupled to augment torque provided by the engine, an energy storage device coupled to receive energy from and provide energy to the motor/generator, an engine controller (EEC) coupled to control the engine, a transmission controller (TCM) coupled to control the transmission and a vehicle system controller (VSC) adapted to control the powertrain.

  3. ARM - Publications: Science Team Meeting Documents

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Numerical Tests of the Cloud-Surface Interaction Based Broken-Cloud Field Optical Depth Retrieval: Sensitivity to Surface Albedo, Droplet Phase Function, Aerosol, and Instrument Noise Beaulne, A.(a), Barker, H.W.(b), Blanchet, J.P.(a), Pavloski, C.F.(c), Clothiaux, E.E.(c), and Marshak, A.(d), Universite du Quebec a Montreal (a), Environment Canada (b), The Pennsylvania State University (c), NASA-GSFC (d) Twelfth Atmospheric Radiation Measurement (ARM) Science Team Meeting The algorithm proposed

  4. DOE HQ Special Needs in an Emergency

    Office of Energy Efficiency and Renewable Energy (EERE) (indexed site)

    T he in fo rm at io n m ay be ag gr eg at ed in to li st s, ch ar ts , an d or gr ap hs . In fo rm at io n pr ov id ed ne ed on ly de sc ri be th e ki nd of as si st an ce re qu ...

  5. Influence of emission threshold of explosive emission cathodes on current waveform in foilless diodes

    SciTech Connect

    Wu, P.; Liu, G. Z.; Huo, S. F.; Sun, J.; Chen, C. H.

    2015-08-15

    The emission threshold of explosive emission cathodes (EECs) is an important factor for beam quality. It can affect the explosive emission delay time, the plasma expansion process on the cathode surface, and even the current amplitude when the current is not fully space-charge-limited. This paper researches the influence of the emission threshold of an annular EEC on the current waveform in a foilless diode when the current is measured by a Rogowski coil. The particle-in-cell simulation which is performed under some tolerable and necessary simplifications shows that the long explosive emission delay time of high-threshold cathodes may leave an apparent peak of displacement current on the rise edge of the current waveform, and this will occur only when the electron emission starts after this peak. The experimental researches, which are performed under a diode voltage of 1 MV and a repetitive frequency of 20 Hz, demonstrate that the graphite cathode has a lower emission threshold and a longer lifetime than the stainless steel cathode according to the variation of the peak of displacement current on the rise edge of the current waveform.

  6. Efficient H{sub 2} production over Au/graphene/TiO{sub 2} induced by surface plasmon resonance of Au and band-gap excitation of TiO{sub 2}

    SciTech Connect

    Liu, Yang; Yu, Hongtao; Wang, Hua; Chen, Shuo; Quan, Xie

    2014-11-15

    Highlights: Both surface plasmon resonance and band-gap excitation were used for H{sub 2} production. Au/Gr/TiO{sub 2} composite photocatalyst was synthesized. Au/Gr/TiO{sub 2} exhibited enhancement of light absorption and charge separation. H{sub 2} production rate of Au/Gr/TiO{sub 2} was about 2 times as high as that of Au/TiO{sub 2}. - Abstract: H{sub 2} production over Au/Gr/TiO{sub 2} composite photocatalyst induced by surface plasmon resonance of Au and band-gap excitation of TiO{sub 2} using graphene (Gr) as an electron acceptor has been investigated. Electron paramagnetic resonance study indicated that, in this composite, Gr collected electrons not only from Au with surface plasmon resonance but also from TiO{sub 2} with band-gap excitation. Surface photovoltage and UVvis absorption measurements revealed that compared with Au/TiO{sub 2}, Au/Gr/TiO{sub 2} displayed more effective photogenerated charge separation and higher optical absorption. Benefiting from these advantages, the H{sub 2} production rate of Au/Gr/TiO{sub 2} composite with Gr content of 1.0 wt% and Au content of 2.0 wt% was about 2 times as high as that of Au/TiO{sub 2}. This work represents an important step toward the efficient application of both surface plasmon resonance and band-gap excitation on the way to converting solar light into chemical energy.

  7. ARM - Feature Stories and Releases Article

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    3, 2013 [Facility News, Feature Stories and Releases] Cloud Cocktail Melts Greenland Ice Sheet Bookmark and Share Like the partygoer that just won't leave, low-level clouds hang around and cause temperatures to rise Not all clouds are created equal-especially in the Arctic. New research published in the journal Nature shows that low-level clouds in Greenland that contain just the right amount of water are thick enough to block heat from escaping to space, but thin enough to allow sunlight to

  8. 1

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Meltwater effects on flow of Greenland's ice sheet less severe for sea level rise than earlier feared, scientists say August 19, 2013 LOS ALAMOS, N.M., Aug. 19, 2013-The effects of increased melting on the future motion of and sea-level contribution from Greenland's massive ice sheet are not quite as dire as previously thought, according to a new study from an international team of researchers. In a paper published this month in Proceedings of the National Academy of Sciences (PNAS), the team

  9. Enhanced efficiency of graphene-silicon Schottky junction solar cells by doping with Au nanoparticles

    SciTech Connect

    Liu, X.; Zhang, X. W. Yin, Z. G.; Meng, J. H.; Gao, H. L.; Zhang, L. Q.; Zhao, Y. J.; Wang, H. L.

    2014-11-03

    We have reported a method to enhance the performance of graphene-Si (Gr/Si) Schottky junction solar cells by introducing Au nanoparticles (NPs) onto the monolayer graphene and few-layer graphene. The electron transfer between Au NPs and graphene leads to the increased work function and enhanced electrical conductivity of graphene, resulting in a remarkable improvement of device efficiency. By optimizing the initial thickness of Au layers, the power conversion efficiency of Gr/Si solar cells can be increased by more than three times, with a maximum value of 7.34%. These results show a route for fabricating efficient and stable Gr/Si solar cells.

  10. Search for: All records | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    Hogg, D.W. (2) Ichikawa, S.-I. (2) Inada, Naohisa (2) Ivezic, Z. (2) Kayo, Issha (2) Kent, S. (2) Knapp, G.R. (2) Morokuma, Tomoki (2) Save Results Save this search to My...

  11. Press Pass - Press Releases

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Tufts University: Cindy Pollard, 617-627-3175, cynthia.pollard@tufts.edu Greece: University of Athens: Elias Marselos, 1-36 89 772, elmars@interel.uoa.gr Korea:...

  12. Rolls Royce Fuel Cell Systems Ltd RRFCS | Open Energy Information

    OpenEI (Open Energy Information) [EERE & EIA]

    Rolls Royce Fuel Cell Systems Ltd RRFCS Jump to: navigation, search Name: Rolls-Royce Fuel Cell Systems Ltd (RRFCS) Place: Leicestershire, England, United Kingdom Zip: LE11 3GR...

  13. CHRISTIAN SEIGNEUR

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Huang, M., G.R. Carmichael, S. Kulkarni, D.G. Streets, Z. Lu, Q. Zhang, R.B. Pierce, Y. Kondo, J.L. Jimenez, M.J. Cubison, B. Anderson, and A. Wisthaler, Sectoral and Geographical...

  14. A=19O (1983AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    83AJ01) (See Energy Level Diagrams for 19O) GENERAL: See (1978AJ03) and Table 19.1 [Table of Energy Levels] (in PDF or PS). Shell model: (1977GR16, 1979DA15, 1980KU05, 1982KI02). Electromagnetic transitions: (1976MC1G, 1978KR19, 1980KU05). Special states: (1977GR16, 1977SH18, 1979DA15, 1982KI02). Astrophysical questions: (1978WO1E). Complex reactions involving 19O: (1978KO01, 1979AL22, 1981GR08). Other topics: (1977GR16, 1977SH18, 1979BE1H, 1979CO09, 1980SH1H, 1982KI02). Ground-state properties

  15. A=6B (2002TI10)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    2002TI10) (Not illustrated) Not observed: see ( 1984AJ01, 1989GR06 [6Li(π+, π-) at Eπ+ = 180, 240 MeV], 1993PO11 [properties of exotic light nuclei]) (1998SU18

  16. A=6C (2002TI10)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    2002TI10) (Not illustrated) Not observed: see (1979AJ01, 1984AJ01, 1989GR06 [6Li(π+, π-) at Eπ+ = 180, 240 MeV], 1993PO11 [properties of exotic light nuclei]) (1998SU18

  17. Glossary Glossary

    Energy Information Administration (EIA) (indexed site)

    calculated in terms of the following for- mula: Deg API 141.5 sp gr60degF 60degF - 131.5 The higher the API gravity, the lighter the compound. Light crudes generally exceed...

  18. ARM XDC Datastreams

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... GR HAIL RA RAIN DZ DRIZZLE SN SNOW SG SNOW GRAINS GS SMALL HAIL &OR SNOW PELLETS PE ICE PELLETS IC CRYSTALS FG+ HEAVY FOG (FG & LE.25 MILES) FG FOG BR MIST UP UNKNOWN ...

  19. Directory

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    order Object Created Object Last Modified Assessment of Negligible Creep Off-Normal Welding and Heat Treatment of GR91 Steel for Nuclear Reactor Pressure Vessel Application.pdf...

  20. Microsoft Word - chapter FeNiCrMo_ver4.doc

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... OH, 1990, pp. 140-194. 2. MR Louthan, RG Derrick, JA Donovan, and GR Caskey, "Hydrogen Transport in Iron and Steel", in Effect of Hydrogen on Behavior of Materials, AW Thompson ...

  1. Microsoft Word - TP22135.doc

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... Park Ridge NJ: Noyes Publications (1985) p. 822-862. 4. MR Louthan and RG Derrick. Hydrogen Transport in Austenitic Stainless Steel. Corrosion Science 15 (1975) 565-577. 5. GR ...

  2. Microsoft Word - TPHP9420.doc

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... Metall Trans 8A (1977) 265-272. 7. MR Louthan, RG Derrick, JA Donovan and GR Caskey. Hydrogen Transport in Iron and Steel. in: AW Thompson and IM Bernstein, editor. Effect of ...

  3. What will the Smart Grid Look Like?

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ... consistent market operation across regions. reVISIon date: 32009 For more InFormatIon Go to: www.themodernGrId.orG Fourth, it will provide power quality for the digital economy. ...

  4. CX-002557: Categorical Exclusion Determination

    Energy.gov [DOE]

    G.R. SilicateCX(s) Applied: B5.1Date: 05/26/2010Location(s): Hoquiam, WashingtonOffice(s): Energy Efficiency and Renewable Energy, Golden Field Office

  5. Presentations

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    March 19, 2013 | Author(s): Alex Friedman, LLNL | Download File: ndcx40g.r6000res1280ipstep5faster.mov | mov | 26 MB Kinetic Modelling in ICF March 19, 2013 | Author(s): Chuang ...

  6. BABAR-PUB-14/002 SLAC-PUB-15979

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    ab , 55 G. Piredda a , 55 C. B unger, 56 S. Dittrich, 56 O. Gr unberg, 56 T. Hartmann, 56 M. Hess, 56 T. Leddig, 56 C. Vo, 56 R. Waldi, 56 T. Adye, 57 E. O. Olaiya, 57...

  7. General and localized corrosion of carbon and low-alloy steels in oxygenated high-temperature water. Final report. [BWR

    SciTech Connect

    Macdonald, D.D.; Smialowska, S.; Pednekar, S.

    1983-02-01

    The susceptibilities to stress corrosion cracking (SCC) of two carbon steels, SA106-grB and SA333-gr6, which are used in seamless BWR piping, and a low-alloy pressure vessel steel, A508-C12, were studied in high purity water as a function of oxygen concentration (0.16 to 8 ppM) and temperature (50 to 288/sup 0/C) . The susceptibility to SCC was measured using the slow strain rate technique. The fracture surfaces of the test specimens were also examined using SEM to determine the mode of failure. In water containing 1 and 8 ppM oxygen and at temperatures above 135/sup 0/C, transgranular stress corrosion cracking (TGSCC) was observed to occur in A508-C12, SA333-gr6 and SA106grB steels at very high stresses. The susceptibility to SCC increased with temperature.

  8. Technical Sessions J. C. Doran Pacific; Northwest Laboratory

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    a site, we hoped to see a clear signature of the effElcts of surface inhomogeneities, test one or more par;metric schemes relating turbulent fluxes to vertical gr;dients of...

  9. G R Inc formerly known as Jawon Medical Co Ltd | Open Energy...

    OpenEI (Open Energy Information) [EERE & EIA]

    R Inc formerly known as Jawon Medical Co Ltd Jump to: navigation, search Name: G&R Inc (formerly known as Jawon Medical Co Ltd) Place: Gwangju, Gwangju, Korea (Republic) Zip:...

  10. The role of intrahepatic CD3 +/CD4 −/CD8 − double negative T (DN T) cells in enhanced acetaminophen toxicity

    SciTech Connect

    Getachew, Yonas; Cusimano, Frank A.; James, Laura P.; Thiele, Dwain L.

    2014-10-15

    The role of the immune system, specifically NK, NKT and CD3 cells, in acetaminophen (APAP) induced liver injury remains inconsistently defined. In the present study, wild type (C57BL/6J) mice and granzyme B deficient (GrB −/−) mice were treated with acetaminophen to assess the role of the immune system in acute liver injury. Doses of acetaminophen that induced sub lethal liver injury in wild type mice unexpectedly produced fatal hepatotoxicity in granzyme B deficient (GrB −/−) mice. Analysis revealed that GrB −/− mice had an increased population of intrahepatic CD3 (+), CD4 (−), and CD8 (−) lymphocytes expressing the CD69 activation marker and Fas ligand. Depletion of these cells in the GrB −/− and wild type mice made them less susceptible to APAP injury, while depletion of NK1.1 (+) cells or both CD4 (+) and CD8 (+) T cells failed to provide the same hepatoprotection. Transfer of the GrB −/− IHLs further exacerbated liver injury and increased mortality in wild type mice but not in LRP/LPR mice, lacking fas expression. Conclusions: Acetaminophen toxicity is enhanced by the presence of activated, FasL expressing intrahepatic CD3 (+), CD4 (−), CD8 (−), NK1.1 (−) T cells. Depletion of these cells from GrB −/− mice and wild type mice greatly reduces mortality and improves the course of liver injury recovery. - Highlights: • Intrahepatic lymphocytes (IHLs) from GrB −/− mice harbor activated DNT cells. • IHLs from GrB −/− mice exhibit enhanced Fas ligand expression. • Acetaminophen toxicity is enhanced by activated, FasL expressing DNT cells.

  11. Rectal Toxicity After Proton Therapy For Prostate Cancer: An Analysis of Outcomes of Prospective Studies Conducted at the University of Florida Proton Therapy Institute

    SciTech Connect

    Colaco, Rovel J.; Hoppe, Bradford S.; Flampouri, Stella; McKibben, Brian T.; Henderson, Randal H.; Bryant, Curtis; Nichols, Romaine C.; Mendenhall, William M.; Li, Zuofeng; Su, Zhong; Morris, Christopher G.; Mendenhall, Nancy P.

    2015-01-01

    Purpose: Study goals were to characterize gastrointestinal effects of proton therapy (PT) in a large cohort of patients treated for prostate cancer, identify factors associated with rectal bleeding (RB), and compare RB between patients receiving investigational protocols versus those in outcome-tracking protocols. Methods and Materials: A total of 1285 consecutive patients were treated with PT between August 2006 and May 2010. Potential pre-existing clinical and treatment-related risk factors for rectal toxicity were recorded. Common Terminology Criteria for Adverse Events version 3.0 was used to score toxicity. Results: Transient RB was the predominant grade 2 or higher (GR2+) toxicity after PT, accounting for 95% of gastrointestinal events. GR1 RB occurred in 217 patients (16.9%), GR2 RB in 187 patients (14.5%), and GR3 in 11 (0.9%) patients. There were no GR4 or GR5 events. Univariate analyses showed correlations between GR2+ RB and anticoagulation therapy (P=.008) and rectal and rectal wall dose-volume histogram (DVH) parameters (P<.001). On multivariate analysis, anticoagulation therapy (P=.0034), relative volume of rectum receiving 75 Gy (V75; P=.0102), and relative rectal wall V75 (P=.0017) were significant predictors for G2+ RB. Patients treated with investigational protocols had toxicity rates similar to those receiving outcome-tracking protocols. Conclusions: PT was associated with a low rate of GR2+ gastrointestinal toxicity, predominantly transient RB, which was highly correlated with anticoagulation and rectal DVH parameters. Techniques that limit rectal exposure should be used when possible.

  12. Desk study of production energy savings control systems feasibility study. (Russia). Volume 1. Export trade information

    SciTech Connect

    Not Available

    1992-07-17

    The objective of the feasibility study is to determine the marketability of heating/ventilating energy conserving control systems in the major city markets of eastern Russia. The second part of the objective is to determine if the existing military based Zelenograd micro-electronic manufacturing and research facility can be utilized to produce Direct Digital Control systems for use within Russia as well as for export to the European Economic Community (EEC) and other countries. Because significant exports of U.S. products and services to support the joint venture are questionable, it is suggested that, potential markets for U.S. products be identified. Sources of capital to finance the joint venture should be identified.

  13. Progress in passive solar energy systems. Volume 8. Part 1

    SciTech Connect

    Hayes, J.; Andrejko, D.A.

    1983-01-01

    This book presents the papers given at a conference sponsored by the US DOE, the Solar Energy Research Institute, SolarVision, Inc., and the Southern California Solar Energy Society. The topics considered at the conference included sizing solar energy systems for agricultural applications, a farm scale ethanol production plant, the EEC wind energy RandD program, the passive solar performance assessment of an earth-sheltered house, the ARCO 1 MW photovoltaic power plant, the performance of a dendritic web photovoltaic module, second generation point focused concentrators, linear fresnel lens concentrating photovoltaic collectors, photovoltaic conversion efficiency, amorphous silicon thin film solar cells, a photovoltaic system for a shopping center, photovoltaic power generation for the utility industry, spectral solar radiation, and the analysis of insolation data.

  14. Extracting the three- and four-graviton vertices from binary pulsars and coalescing binaries

    SciTech Connect

    Cannella, Umberto; Foffa, Stefano; Maggiore, Michele; Sanctuary, Hillary; Sturani, Riccardo

    2009-12-15

    Using a formulation of the post-Newtonian expansion in terms of Feynman graphs, we discuss how various tests of general relativity (GR) can be translated into measurement of the three- and four-graviton vertices. In problems involving only the conservative dynamics of a system, a deviation of the three-graviton vertex from the GR prediction is equivalent, to lowest order, to the introduction of the parameter {beta}{sub PPN} in the parametrized post-Newtonian formalism, and its strongest bound comes from lunar laser ranging, which measures it at the 0.02% level. Deviation of the three-graviton vertex from the GR prediction, however, also affects the radiative sector of the theory. We show that the timing of the Hulse-Taylor binary pulsar provides a bound on the deviation of the three-graviton vertex from the GR prediction at the 0.1% level. For coalescing binaries at interferometers we find that, because of degeneracies with other parameters in the template such as mass and spin, the effects of modified three- and four-graviton vertices is just to induce an error in the determination of these parameters and, at least in the restricted PN approximation, it is not possible to use coalescing binaries for constraining deviations of the vertices from the GR prediction.

  15. Raman scattering from superhard rhenium diboride under high pressure

    SciTech Connect

    Xie, Miao; Winkler, Björn; Mao, Zhu; Kaner, Richard B.; Tolbert, Sarah H. E-mail: tolbert@chem.ucla.edu; Kavner, Abby E-mail: tolbert@chem.ucla.edu

    2014-01-06

    Lattice vibrational properties of superhard rhenium diboride (ReB{sub 2}) were examined up to 8 GPa in a diamond anvil cell using Raman spectroscopy techniques. Linear pressure coefficients and mode Grüneisen parameters are obtained. Good agreement is found between the experimental and theoretical calculated Grüneisen parameters. Examination of the calculated mode Grüneisen parameters reveals that both B-B and Re-B covalent bonds play a dominant role in supporting the applied load under pressure. A comparison of vibrations parallel and perpendicular to the c-axis indicates that bonds along the c-axis tend to take greater loads. Our results agree with observations of elastic lattice anisotropy obtained from both in situ X-ray diffraction measurements and ultrasonic resonance spectra.

  16. A=20O (1983AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    3AJ01) (See Energy Level Diagrams for 20O) GENERAL: See also (1978AJ03) and Table 20.1 [Table of Energy Levels] (in PDF or PS). Model calculations: (1977GR16). Special states: (1977GR16). Astrophysical questions: (1978WO1E). Other topics: (1977GR16, 1978RA1J, 1979BE1H). 1. 20O(β-)20F Qm = 3.816 20O decays to 20F*(1.06) [Jπ = 1+] with a half-life of 13.51 ± 0.05 sec (weighted mean of (1970MA42, 1974AL09)), log ft = 3.75 ± 0.01. Upper limits for the branching to other states of 20F are shown

  17. Geoengineering: Plan B Remedy for Global Warming Andrew A. Lacis

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Plan B Remedy for Global Warming Andrew A. Lacis NASA Goddard Institute for Space Studies Accelerated melting of Greenland ice is a clear indication that consequences of global warming are real and impending. The underlying causes of global warming are well enough understood, but the necessary reduction of greenhouse gases to prevent irreversible climate change is unlikely to happen before the point of no return is reached. To reverse the impending sea level rise, geoengineering counter-

  18. Microsoft PowerPoint - 06_ARM_AWG_Lacis_2007.ppt [Compatibility Mode]

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Geoengineering: Plan B Remedy for Global Warming y g Andy Lacis Aerosol Working Group 26 March 2007 Some Radiative Aspects of Proposed Geoengineering Countermeasures to Global Warming (submitted to PNAS) g ( ) Andrew A. Lacis, Jennifer L. Alltop, Solomon M. Hsiang, Kirk D. Knobelspiesse, Jing Li, Cindy B. Pearl Accelerated melting of Greenland ice due to global warming . . . How can aerosols be used to counteract global warming? * Injection of sulfur into the lower stratosphere * Injection of

  19. Science Briefs - 2013

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Science Briefs - 2013 Read in detail about specific Los Alamos science achievements, and the honors our scientists are accruing. Image from National Oceanic and Atmospheric Administration's Environmental Visualization Laboratory depicts sea surface temperatures around Greenland from October 2010. Effect of ocean temperature on southwestern U.S. climate analyzed Researchers concluded that only part of the recent temperature rise in the Southwest could be attributed to greenhouse gases. -

  20. Industry`s turnaround looks real

    SciTech Connect

    1997-08-01

    The paper discusses the industry outlook for North American gas and oil industries. In a robust Canada, land sales are setting records, drilling is up, and output is rising beyond last year`s 21% growth. A perception among US operators that wellhead prices will remain stable is translating to increased spending. The USA, Canada, Mexico, Cuba are evaluated separately, with brief evaluations of Greenland, Guatemala, Belize, and Costa Rico. Data are presented on drilling activities.

  1. PISCEES for prediction

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    PISCEES for prediction PISCEES for prediction The Greenland and Antarctic ice sheets will make a dominant contribution to twenty-first century sea-level rise if current climate trends continue, studied in a five-year project called Predicting Ice Sheet and Climate Evolution at Extreme Scales (PISCEES) February 19, 2016 Human-gorilla divergence may have occurred two million years earlier than thought (Photo : Flickr: Rod Waddington) Antarctica "The data we get from climate scientists are

  2. News Stories

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    News Stories News Stories Featured articles about DOE Office of Science programs and people at Los Alamos. Advanced Scientific Computing Los Alamos projects help set path to next-generation supercomputers Greenland Ice Sheet "Sliding" a Small Contributor to Future Sea-Level Rise Awards David L. Clark selected for 2017 Glenn T. Seaborg Award for Nuclear Chemistry Ten Los Alamos scientists, including four sponsored by the DOE Office of Science, honored by American Physical Society Los

  3. Effect of ocean temperature on southwestern U.S. climate analyzed

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Effect of ocean temperature on southwestern climate Effect of ocean temperature on southwestern U.S. climate analyzed Researchers concluded that only part of the recent temperature rise in the Southwest could be attributed to greenhouse gases. December 19, 2013 Image from National Oceanic and Atmospheric Administration's Environmental Visualization Laboratory depicts sea surface temperatures around Greenland from October 2010. Image from National Oceanic and Atmospheric Administration's

  4. Effect of ocean temperature on southwestern U.S. climate analyzed

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    December » Effect of ocean temperature on southwestern climate Effect of ocean temperature on southwestern U.S. climate analyzed Researchers concluded that only part of the recent temperature rise in the Southwest could be attributed to greenhouse gases. December 19, 2013 Image from National Oceanic and Atmospheric Administration's Environmental Visualization Laboratory depicts sea surface temperatures around Greenland from October 2010. Image from National Oceanic and Atmospheric

  5. Development of integraded mechanistically-based degradation-mode models for performance assessment of high-level waste containers

    SciTech Connect

    Farmer, J. C., LLNL

    1998-06-01

    A key component of the Engineered Barrier System (EBS) being designed for containment of spent-fuel and high-level waste at the proposed geological repository at Yucca Mountain, Nevada is a two-tayer canister. In this particular design, the inner barrier is made of a corrosion resistant material (CRM) such as Alloy 825, 625 or C-22, while the outer barrier is made of a corrosion-allowance material (CAM) such as A516 Gr 55 or Monel 400. At the present time, Alloy C- 22 and A516 Gr 55 are favored.

  6. Import Manipulate Plot RELAP5/MOD3 Data

    SciTech Connect

    Jones, K. R.

    1999-10-05

    XMGR5 was derived from an XY plotting tool called ACE/gr, which is copyrighted by Paul J. Turner and in the public domain. The interactive version of ACE/GR is xmgr, and includes a graphical interface to the X-windows system. Enhancements to xmgr have been developed which import, manipualate, and plot data from RELAP/MOD3, MELCOR, FRAPCON, and SINDA codes, and NRC databank files. capabilities, include two-phase property table lookup functions, an equation interpreter, arithmetic library functions, and units conversion. Plot titles, labels, legends, and narrative can be displayed using Latin or Cyrillic alphabets.

  7. Molecular Solid EOS based on Quasi-Harmonic Oscillator approximation for phonons

    SciTech Connect

    Menikoff, Ralph

    2014-09-02

    A complete equation of state (EOS) for a molecular solid is derived utilizing a Helmholtz free energy. Assuming that the solid is nonconducting, phonon excitations dominate the specific heat. Phonons are approximated as independent quasi-harmonic oscillators with vibrational frequencies depending on the specific volume. The model is suitable for calibrating an EOS based on isothermal compression data and infrared/Raman spectroscopy data from high pressure measurements utilizing a diamond anvil cell. In contrast to a Mie-Gr ̈uneisen EOS developed for an atomic solid, the specific heat and Gr ̈uneisen coefficient depend on both density and temperature.

  8. Import Manipulate Plot RELAP5/MOD3 Data

    Energy Science and Technology Software Center

    1999-10-05

    XMGR5 was derived from an XY plotting tool called ACE/gr, which is copyrighted by Paul J. Turner and in the public domain. The interactive version of ACE/GR is xmgr, and includes a graphical interface to the X-windows system. Enhancements to xmgr have been developed which import, manipualate, and plot data from RELAP/MOD3, MELCOR, FRAPCON, and SINDA codes, and NRC databank files. capabilities, include two-phase property table lookup functions, an equation interpreter, arithmetic library functions, andmore » units conversion. Plot titles, labels, legends, and narrative can be displayed using Latin or Cyrillic alphabets.« less

  9. Papers Published - April 1, 1999 - March 31, 2000

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    P.W. Stankus, T.N. Thompson, R.S. Towell, R.E. Tribble, M.A. Vasiliev, Y.C. Wang, Z.F. Wang, J.C. Webb, J.L. Willis, D.K. Wise and G.R. Young (FNAL E866NuSea Collaboration)...

  10. Globular and Open Clusters Observed by SDSS/SEGUE: the Giant Stars

    DOE PAGES [OSTI]

    Morrison, Heather L.; Ma, Zhibo; Clem, James L.; An, Deokkeun; Connor, Thomas; Schechtman-Rook, Andrew; Casagrande, Luca; Rockosi, Constance; Yanny, Brian; Harding, Paul; et al

    2015-12-18

    We present griz observations for the clusters M92, M13 and NGC 6791 and gr photometry for M71, Be 29 and NGC 7789. In addition we present new membership identifications for all these clusters, which have been observed spectroscopically as calibrators for the SDSS/SEGUE survey; this paper focuses in particular on the red giant branch stars in the clusters. In a number of cases, these giants were too bright to be observed in the normal SDSS survey operations, and we describe the procedure used to obtain spectra for these stars. For M71, also present a new variable reddening map and amore » new fiducial for the gr giant branch. For NGC 7789, we derived a transformation from Teff to g-r for giants of near solar abundance, using IRFM Teff measures of stars with good ugriz and 2MASS photometry and SEGUE spectra. The result of our analysis is a robust list of known cluster members with correctly dereddened and (if needed) transformed gr photometry for crucial calibration efforts for SDSS and SEGUE.« less

  11. Testing universal relations of neutron stars with a nonlinear matter-gravity coupling theory

    SciTech Connect

    Sham, Y.-H.; Lin, L.-M.; Leung, P. T. E-mail: lmlin@phy.cuhk.edu.hk

    2014-02-01

    Due to our ignorance of the equation of state (EOS) beyond nuclear density, there is still no unique theoretical model for neutron stars (NSs). It is therefore surprising that universal EOS-independent relations connecting different physical quantities of NSs can exist. Lau et al. found that the frequency of the f-mode oscillation, the mass, and the moment of inertia are connected by universal relations. More recently, Yagi and Yunes discovered the I-Love-Q universal relations among the mass, the moment of inertia, the Love number, and the quadrupole moment. In this paper, we study these universal relations in the Eddington-inspired Born-Infeld (EiBI) gravity. This theory differs from general relativity (GR) significantly only at high densities due to the nonlinear coupling between matter and gravity. It thus provides us an ideal case to test how robust the universal relations of NSs are with respect to the change of the gravity theory. Due to the apparent EOS formulation of EiBI gravity developed recently by Delsate and Steinhoff, we are able to study the universal relations in EiBI gravity using the same techniques as those in GR. We find that the universal relations in EiBI gravity are essentially the same as those in GR. Our work shows that, within the currently viable coupling constant, there exists at least one modified gravity theory that is indistinguishable from GR in view of the unexpected universal relations.

  12. A=17F (71AJ02)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Electromagnetic transitions: (BA59M, FA59E, RA60B, BA64AA, GR65E, KA65F, MA66BB, KA67J, ... The decay is to the ground state of 17O. The spectrum has the allowed shape down to 150 ...

  13. U.S. Geological Survey Open-File Report 99-310

    National Nuclear Security Administration (NNSA)

    r e d fr om Gr a v i t y D a ta , Ne va da Test Si te , N e va da by G.A. Phelps 1 , V.E. ... Figure 1. Map showing simplified geology of the Nevada Test Site region. White, Cenozoic ...

  14. Transforming PV Installations Toward Dispatchable, Schedulable...

    Office of Energy Efficiency and Renewable Energy (EERE) (indexed site)

    Toward disPaTchable, schedulable energy soluTions MIChAEl MIllS-PrICE, SEGIS-AC ProGrAM MAnAGEr, AE SolAr EnErGy A B C N SATCON518kw1 B2+2 Cap Bank 7825S PHC870 6896 Aout Ain ...

  15. APPOLLO 9

    ScienceCinema

    None

    2011-04-25

    le DG B.Grégory prend la parole et introduit le cosmonaute américain Russell Schweickart, qui fait un exposé sur la mission APPOLLO 9 et l'avenir de l'exploration spatiale avec présentation d'un film avec musique, mais sans parole, après commentaires et questions

  16. Globular and Open Clusters Observed by SDSS/SEGUE: the Giant Stars

    SciTech Connect

    Morrison, Heather L.; Ma, Zhibo; Clem, James L.; An, Deokkeun; Connor, Thomas; Schechtman-Rook, Andrew; Casagrande, Luca; Rockosi, Constance; Yanny, Brian; Harding, Paul; Beers, Timothy C.; Johnson, Jennifer A.; Schneider, Donald P.

    2015-12-18

    We present griz observations for the clusters M92, M13 and NGC 6791 and gr photometry for M71, Be 29 and NGC 7789. In addition we present new membership identifications for all these clusters, which have been observed spectroscopically as calibrators for the SDSS/SEGUE survey; this paper focuses in particular on the red giant branch stars in the clusters. In a number of cases, these giants were too bright to be observed in the normal SDSS survey operations, and we describe the procedure used to obtain spectra for these stars. For M71, also present a new variable reddening map and a new fiducial for the gr giant branch. For NGC 7789, we derived a transformation from Teff to g-r for giants of near solar abundance, using IRFM Teff measures of stars with good ugriz and 2MASS photometry and SEGUE spectra. The result of our analysis is a robust list of known cluster members with correctly dereddened and (if needed) transformed gr photometry for crucial calibration efforts for SDSS and SEGUE.

  17. Enhancing the use of coals by gas reburning-sorbent injection: Volume 4 -- Gas reburning-sorbent injection at Lakeside Unit 7, City Water, Light and Power, Springfield, Illinois. Final report

    SciTech Connect

    1996-03-01

    A demonstration of Gas Reburning-Sorbent Injection (GR-SI) has been completed at a cyclone-fired utility boiler. The Energy and Environmental Research Corporation (EER) has designed, retrofitted and tested a GR-SI system at City Water Light and Power`s 33 MWe Lakeside Station Unit 7. The program goals of 60% NO{sub x} emissions reduction and 50% SO{sub 2} emissions reduction were exceeded over the long-term testing period; the NO{sub x} reduction averaged 63% and the SO{sub 2} reduction averaged 58%. These were achieved with an average gas heat input of 22% and a calcium (sorbent) to sulfur (coal) molar ratio of 1.8. GR-SI resulted in a reduction in thermal efficiency of approximately 1% at full load due to firing natural gas which forms more moisture in flue gas than coal and also results in a slight increase in air heater exit gas temperature. Minor impacts on other areas of unit performance were measured and are detailed in this report. The project at Lakeside was carried out in three phases, in which EER designed the GR-SI system (Phase 1), completed construction and start-up activities (Phase 2), and evaluated its performance with both short parametric tests and a long-term demonstration (Phase 3). This report contains design and technical performance data; the economics data for all sites are presented in Volume 5.

  18. BPA-2012-01869-FOIA Response

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    information because it does not shed any light on how BPA has performed its statutory duties. N*me Ed*c*den Oe'.S.ries Gr*dc Cannell,KevinG Ex 0193 12 Schmidt,Sunshine R Ex 6...

  19. Fatigue and environmentally assisted cracking in light water reactors

    SciTech Connect

    Kassner, T.F.; Ruther, W.E.; Chung, H.M.; Hicks, P.D.; Hins, A.G.; Park, J.Y.; Shack, W.J.

    1992-03-01

    Fatigue and stress corrosion cracking (SCC) for low-alloy steel used in piping and in steam generator and reactor pressure vessels have been investigated. Fatigue data were obtained on medium-sulfur-content A533-Gr B and A106-Gr B steels in high-purity (HP) deoxygenated water, in simulated pressurized water reactor water, and in air. Analytical studies focused on the behavior of carbon steels in boiling water reactor (BWR) environments. Crack-growth rates of composite fracture-mechanics specimens of A533-Gr B/Inconel-182/Inconel-600 (plated with nickel) and homogeneous specimens of A533-Gr B steel were determined under small-amplitude cyclic loading in HP water with {approx}300 pbb dissolved oxygen. Radiation-induced segregation and irradiation-assisted SCC of Type 304 SS after accumulation of relatively high fluence also have been investigated. Microchemical and microstructural changes in HP and commercial-purity Type 304 SS specimens from control-blade absorber tubes used in two operating BWRs were studied by Auger electron spectroscopy and scanning electron microscopy, and slow-strain-rate tensile tests were conducted on tubular specimens in air and in simulated BWR water at 289{degrees}C.

  20. American Associatio

    Office of Scientific and Technical Information (OSTI)

    ... that transfers in the case of planarians, it seems ... cm around the foodcup was white and constituted the "food ... RNA ige cte d gr ou p. , i n j e c t 0 n 8 40 09 g 'e Kl 0 ...

  1. A=20Ne (1987AJ02)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    1986VA18, 1986VA23, 1986WE1C, 1987FA09, 1987KO15, 1987NI04, 1987RI03, 1987RO10). Muon and neutrino capture and reactions: (1983RO1E, 1984EL1D, 1984GR03, 1985MI1D,...

  2. A=20F (1959AJ76)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    are listed in Table 20.4 Resonances in 19F(n, )16N (in PDF or PS) (BO55A, MA55L: see graph in (HU58)). See also (WI37E, BO55D, GR55D, KO58A). 15. 19F(d, p)20F Qm 4.379 Q0 ...

  3. A=9Be (1979AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    PDF or PS). Shell model: (1975KU27, 1975SC1K, 1977CA08, 1977JA14, 1978BO31). and cluster models: (1974CH19, 1974GR42, 1974PA1B, 1975AB1E, 1975CH28, 1975KR1D, 1975RO1B,...

  4. A=19F (1983AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    1978DA1N, 1978MA2H, 1979DA15, 1980KU05, 1980MC1L, 1981ER03, 1981GR06, 1982KI02). Cluster, collective and rotational models: (1977BU22, 1977FO1E, 1978BR21, 1978CH26,...

  5. Scaling of volume to surface ratio and doubling time in growing unicellular organisms: Do cells appear quantum-mechanical systems?

    SciTech Connect

    Atanasov, Atanas Todorov

    2014-10-06

    The scaling of physical and biological characteristics of the living organisms is a basic method for searching of new biophysical laws. In series of previous studies the author showed that in Poikilotherms, Mammals and Aves, the volume to surface ratio VS{sup ?1} (m) of organisms is proportional to their generation time T{sub gt}(s) via growth rate v (m s{sup ?1}): VS{sup ?1}?=?v{sub gr}T{sup r}. The power and the correlation coefficients are near to 1.0. Aim of this study is: i) to prove with experimental data the validity of the above equation for Unicellular organisms and ii) to show that perhaps, the cells are quantum-mechanical systems. The data for body mass M (kg), density ? (kg/m{sup 3}), minimum and maximum doubling time T{sub dt} (s) for 50 unicellular organisms are assembled from scientific sources, and the computer program Statistics is used for calculations. In result i) the analytical relationship from type: VS{sup ?1}?=?4.46?10{sup ?11}T{sub dt} was found, where v{sub gr}?=?4.4610{sup ?11} m/s and ii) it is shown that the products between cell mass M, cell length expressed by V/S ratio and growth rate v{sub gr} satisfied the Heisenberg uncertainty principle i.e. the inequalities V/SMv{sub gr}>h/2? and T{sub dt}Mv{sub gr}{sup 2}>h/2? are valid, where h= 6.62610{sup ?34} J?s is the Planck constant. This rise the question: do cells appear quantum-mechanical systems?.

  6. Processing and modeling issues for thin-film solar cell devices: Annual subcontract report, January 16, 1995 -- January 15, 1996

    SciTech Connect

    Birkmire, R.W.; Phillips, J.E.; Buchanan, W.A.; Eser, E.; Hegedus, S.S.; McCandless, B.E.; Meyers, P.V.; Shafarman, W.N.

    1996-08-01

    The overall mission of the Institute of Energy Conversion is the development of thin film photovoltaic cells, modules, and related manufacturing technology and the education of students and professionals in photovoltaic technology. The objectives of this four-year NREL subcontract are to advance the state of the art and the acceptance of thin film PV modules in the areas of improved technology for thin film deposition, device fabrication, and material and device characterization and modeling, relating to solar cells based on CuInSe{sub 2} and its alloys, on a-Si and its alloys, and on CdTe. In the area of CuInSe{sub 2} and its alloys, EEC researchers have produced CuIn{sub 1-x}GaxSe{sub 2} films by selenization of elemental and alloyed films with H{sub 2}Se and Se vapor and by a wide variety of process variations employing co-evaporation of the elements. Careful design, execution and analysis of these experiments has led to an improved understanding of the reaction chemistry involved, including estimations of the reaction rate constants. Investigation of device fabrication has also included studies of the processing of the Mo, US and ZnO deposition parameters and their influence on device properties. An indication of the success of these procedures was the fabrication of a 15% efficiency CuIn{sub 1-x}GaxSe{sub 2} solar cell.

  7. Field installation proves coiled tubing ESP completions successful

    SciTech Connect

    Tovar, J.J.; Head, P.; Jordan, R.

    1995-06-01

    Coiled tubing (CT) technology has contributed new and innovative solutions for wells using electrical submersible pumps (ESP). A CT-ESP deployment system was developed as part of a joint industry project to take advantage of this new technology. Ten oil and service companies and the EEC, under the Thermie program, participated in its development. Two main areas were identified to introduce these innovations. The first was deployment and well control. This area has a great impact on the safety and operational aspects of installing and servicing ESPs. The second is cost. As ESPs are considered for new field developments and recompletion of old fields, installation and workover costs play a major role in the selection of completion alternatives. One of the main limitations of ESPs in the past has been the economics of installation and uncertainty about pump life. With focus in these two major areas, a system was successfully produced that offers considerable advantages over existing technologies. The reduction in rig time and equipment cost makes this alternative very attractive for areas where technical and economic obstacles such as live well deployment and high operating cost limit the use of ESP technology. Two field tests have been carried successfully during the development of this system.

  8. Biogas end-use in the European community

    SciTech Connect

    Constant, M.; Naveau, H.; Nyns, E.J. ); Ferrero, G.L.

    1989-01-01

    In Europe over the past few years the generation of biogas for energy and environmental purposes has been gaining in importance. Industrial wastewaters, cattle manure, sewage sludges, urban wastes, crop residues, algae and aquatic biomass are all typical of the materials being utilized. In contrast to the extensive inventory of biomethanation processes which has been carried out within the EEC, until recently a detailed, up-to-date investigation of the end-sues of biogas had not been undertaken. To supply the necessary information, the Commission of the European Communities and the Belgian Science Policy Office jointly entrusted a study to the Unit of Bioengineering at the Catholic University of Louvain, Belgium. This book is record of the study and has the following key features: it gives a broad overview of the ongoing use of biogas in Europe; it summarizes available data on storage, purification and engines using biogas; it draws several conclusions concerning the technical and economic viability of the processes; it discusses the problems of using biogas; and it outlines recommendations and future R and D and demonstration projects in the field.

  9. Lung Cancer Survival Prediction using Ensemble Data Mining on Seer Data

    DOE PAGES [OSTI]

    Agrawal, Ankit; Misra, Sanchit; Narayanan, Ramanathan; Polepeddi, Lalith; Choudhary, Alok

    2012-01-01

    We analyze the lung cancer data available from the SEER program with the aim of developing accurate survival prediction models for lung cancer. Carefully designed preprocessing steps resulted in removal/modification/splitting of several attributes, and 2 of the 11 derived attributes were found to have significant predictive power. Several supervised classification methods were used on the preprocessed data along with various data mining optimizations and validations. In our experiments, ensemble voting of five decision tree based classifiers and meta-classifiers was found to result in the best prediction performance in terms of accuracy and area under the ROC curve. We have developedmore » an on-line lung cancer outcome calculator for estimating the risk of mortality after 6 months, 9 months, 1 year, 2 year and 5 years of diagnosis, for which a smaller non-redundant subset of 13 attributes was carefully selected using attribute selection techniques, while trying to retain the predictive power of the original set of attributes. Further, ensemble voting models were also created for predicting conditional survival outcome for lung cancer (estimating risk of mortality after 5 years of diagnosis, given that the patient has already survived for a period of time), and included in the calculator. The on-line lung cancer outcome calculator developed as a result of this study is available at http://info.eecs.northwestern.edu:8080/LungCancerOutcomeCalculator/.« less

  10. Push or Pull? Proton Responsive Ligand Effects in Rhenium Tricarbonyl CO 2 Reduction Catalysts

    SciTech Connect

    Manbeck, Gerald F.; Muckerman, James T.; Szalda, David J.; Himeda, Yuichiro; Fujita, Etsuko

    2015-02-19

    Proton responsive ligands offer control of catalytic reactions through modulation of pH-dependent properties, second coordination sphere stabilization of transition states, or by providing a local proton source for multi-proton, multi-electron reactions. Two fac-[ReI(?-diimine)(CO)?Cl] complexes with ?-diimine = 4,4'- (or 6,6'-) dihydroxy-2,2'-bipyridine (4DHBP and 6DHBP) have been prepared and analyzed as electrocatalysts for reduction of carbon dioxide. Consecutive electrochemical reduction of these complexes yields species identical to those obtained by chemical deprotonation. An energetically feasible mechanism for reductive deprotonation is proposed in which the bpy anion is protonated followed by loss of H? and 2H?. Cyclic voltammetry reveals a two-electron, three-wave system owing to competing EEC and ECE pathways. The chemical step of the ECE pathway might be attributed to the reductive deprotonation. but cannot be distinguished from chloride dissociation. The rate obtained by digital simulation is approximately 8 s?. Under CO?, these competing reactions generate a two-slope catalytic waveform with onset potential of 1.65 V vs Ag/AgCl. Reduction of CO? to CO by the [ReI (4DHBP2H?)(CO)?]? suggests the interaction of CO? with the deprotonated species or a third reduction followed by catalysis. Conversely, the reduced form of [Re(6DHBP)(CO)?Cl] converts CO? to CO with a single turnover.

  11. Minerals yearbook: Mineral industries of Europe and the USSR. Volume 3. 1990 international review

    SciTech Connect

    Not Available

    1990-01-01

    The section of the Minerals Yearbook reviews the minerals industries of 29 countries: the 12 nations of the European Community (Belgium, France, the Federal Republic of Germany (FRG), Italy, Greece, the Netherlands, Denmark/Greenland, Spain, Portugal, Luxembourg, The United Kingdom, and Ireland); 6 of the 7 nations of the European Free Trade Association (Sweden, Norway, Finland, Iceland, Austria, and Switzerland); Malta; the 8 Centrally Planned Economies of Eastern Europe (the German Democratic Republic (GDR), Poland, Yugoslavia, Albania, Hungary, Czechoslovakia, Romania, and Bulgaria); and the USSR.

  12. TESTING GRAVITY WITH QUASI-PERIODIC OSCILLATIONS FROM ACCRETING BLACK HOLES: THE CASE OF THE EINSTEIN–DILATON–GAUSS–BONNET THEORY

    SciTech Connect

    Maselli, Andrea; Gualtieri, Leonardo; Ferrari, Valeria; Pani, Paolo; Stella, Luigi

    2015-03-10

    Quasi-periodic oscillations (QPOs) observed in the X-ray flux emitted by accreting black holes are associated with phenomena occurring near the horizon. Future very large area X-ray instruments will be able to measure QPO frequencies with very high precision, thus probing this strong-field region. Using the relativistic precession model, we show the way in which QPO frequencies could be used to test general relativity (GR) against those alternative theories of gravity which predict deviations from the classical theory in the strong-field and high-curvature regimes. We consider one of the best-motivated high-curvature corrections to GR, namely, the Einstein–Dilaton–Gauss–Bonnet theory, and show that a detection of QPOs with the expected sensitivity of the proposed ESA M-class mission LOFT would set the most stringent constraints on the parameter space of this theory.

  13. Phonon anharmonicity of monoclinic zirconia and yttrium-stabilized zirconia

    DOE PAGES [OSTI]

    Li, Chen W.; Smith, Hillary L.; Lan, Tian; Niedziela, Jennifer L.; Munoz, Jorge A.; Keith, J. Brian; Mauger, L.; Abernathy, Douglas L; Fultz, B.

    2015-04-13

    Inelastic neutron scattering measurements on monoclinic zirconia (ZrO2) and 8 mol% yttrium-stabilized zirconia were performed at temperatures from 300 to 1373 ωK. We reported temperature-dependent phonon densities of states (DOS) and Raman spectra obtained at elevated temperatures. First-principles lattice dynamics calculations with density functional theory gave total and partial phonon DOS curves and mode Grüneisen parameters. These mode Grüneisen parameters were used to predict the experimental temperature dependence of the phonon DOS with partial success. However, substantial anharmonicity was found at elevated temperatures, especially for phonon modes dominated by the motions of oxygen atoms. Yttrium-stabilized zirconia (YSZ) was somewhat moremore » anharmonic and had a broader phonon spectrum at low temperatures, owing in part to defects in its structure. YSZ also has a larger vibrational entropy than monoclinic zirconia.« less

  14. Phonon anharmonicity of monoclinic zirconia and yttrium-stabilized zirconia

    SciTech Connect

    Li, Chen W.; Smith, Hillary L.; Lan, Tian; Niedziela, Jennifer L.; Munoz, Jorge A.; Keith, J. Brian; Mauger, L.; Abernathy, Douglas L; Fultz, B.

    2015-04-13

    Inelastic neutron scattering measurements on monoclinic zirconia (ZrO2) and 8 mol% yttrium-stabilized zirconia were performed at temperatures from 300 to 1373 ωK. We reported temperature-dependent phonon densities of states (DOS) and Raman spectra obtained at elevated temperatures. First-principles lattice dynamics calculations with density functional theory gave total and partial phonon DOS curves and mode Grüneisen parameters. These mode Grüneisen parameters were used to predict the experimental temperature dependence of the phonon DOS with partial success. However, substantial anharmonicity was found at elevated temperatures, especially for phonon modes dominated by the motions of oxygen atoms. Yttrium-stabilized zirconia (YSZ) was somewhat more anharmonic and had a broader phonon spectrum at low temperatures, owing in part to defects in its structure. YSZ also has a larger vibrational entropy than monoclinic zirconia.

  15. A=11C (1985AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    5AJ01) (See Energy Level Diagrams for 11C) GENERAL: See also (1980AJ01) and Table 11.17 [Table of Energy Levels] (in PDF or PS). Model calculations:(1981RA06, 1983SH38). Special states:(1981RA06). Complex reactions involving 11C:(1979BO22, 1980GR10, 1980WI1K, 1980WI1L, 1981MO20, 1982GE05, 1982LY1A, 1982RA31, 1983FR1A, 1983OL1A, 1983WI1A, 1984GR08, 1984HI1A). Electromagnetic transitions:(1978KR19). Applied work:(1979DE1H, 1982BO1N, 1982HI1H, 1982KA1R, 1982ME1C, 1982NE1D, 1982PI1H, 1982YA1C,

  16. A=18F (1983AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    83AJ01) (See Energy Level Diagrams for 18F) GENERAL: See also (1978AJ03) and Table 18.11 [Table of Energy Levels] (in PDF or PS). Shell model: (1977AN1P, 1977GR16, 1977SO1C, 1978CO08, 1978DA1N, 1978MA2H, 1979BU12, 1979DA15, 1980GO01, 1980KU05, 1980MA18, 1981EL1D, 1981ER03, 1981GR06, 1982KI02). Cluster, collective and deformed models: (1977BU22, 1978BU03, 1978PI1E, 1978SA15, 1978TA1A, 1979BU12, 1979SA31, 1980RO19, 1981CH24). Electromagnetic transitions: (1976MC1G, 1977BU22, 1977HA1Z, 1977HE1L,

  17. A=19Ne (1987AJ02)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    7AJ02) (See Energy Level Diagrams for 19Ne) GENERAL: See (1983AJ01) and Table 19.21 [Table of Energy Levels] (in PDF or PS). Nuclear models:(1983BR29, 1983PO02). Special states: (1983BI1C, 1983BR29, 1983PO02, 1986AN07). Electromagnetic transitions: (1982BR24, 1983BR29, 1985AL21). Astrophysical questions: (1981WA1Q, 1982WI1B, 1986LA07). Applications:(1982BO1N). Complex reactions involving 19Ne:(1981DE1P, 1983JA05, 1984GR08, 1985BE40, 1986GR1A, 1986HA1B, 1987RI03). Pion capture and reactions (See

  18. A=6Li (1979AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    79AJ01) (See Energy Level Diagrams for 6Li) GENERAL: See also (1974AJ01) and Table 6.2 [Table of Energy Levels] (in PDF or PS) here. Shell model: (1974KA11, 1975DI04, 1975GO1B, 1975VE01, 1976CE03, 1976GH1A). Collective, rotational and deformed models: (1974BO25). Cluster and α-particle models: (1972KR1A, 1973DO09, 1973LI23, 1974BA30, 1974GR24, 1974JA1K, 1974KA11, 1974NO03, 1974PA1B, 1974SH08, 1974WO1B, 1975BL1C, 1975GO08, 1975GR26, 1975HA48, 1975KR1A, 1975LE1A, 1975LI1C, 1975MI09, 1975NO03,

  19. Strangeness production with massive'' gluons

    SciTech Connect

    Biro, T.S. Institut fuer Theoretische Physik, Justus-Liebig-Universitaet, Giessen ); Levai, P.; Mueller, B. )

    1990-11-01

    We present a perturbative calculation of strange-quark production by the processes {ital g}{r arrow}{ital s}+{ital {bar s}}, {ital g}+{ital g}{r arrow}{ital s}+{ital {bar s}}, and {ital q}+{ital {bar q}}{r arrow}{ital s}+{ital {bar s}} in a quark-gluon plasma containing gluons that are effectively massive'' due to medium effects. We consider only transverse polarizations of the gluons. We find that for a gluon mass beyond 300 MeV the one-gluon decay dominates, and that there is an {ital enhancement} of {ital s{bar s}} production from massive gluons compared with the massless case.

  20. Imaging an event horizon: mitigation of scattering toward Sagittarius A*

    SciTech Connect

    Fish, Vincent L.; Lu, Ru-Sen; Doeleman, Sheperd S.; Pankratius, Victor; Johnson, Michael D.; Narayan, Ramesh; Vertatschitsch, Laura E.; Bouman, Katherine L.; Zoran, Daniel; Freeman, William T.; Psaltis, Dimitrios; Broderick, Avery E.; Gwinn, Carl R.

    2014-11-10

    The image of the emission surrounding the black hole in the center of the Milky Way is predicted to exhibit the imprint of general relativistic (GR) effects, including the existence of a shadow feature and a photon ring of diameter ∼50 μas. Structure on these scales can be resolved by millimeter-wavelength very long baseline interferometry. However, strong-field GR features of interest will be blurred at λ ≥ 1.3 mm due to scattering by interstellar electrons. The scattering properties are well understood over most of the relevant range of baseline lengths, suggesting that the scattering may be (mostly) invertible. We simulate observations of a model image of Sgr A* and demonstrate that the effects of scattering can indeed be mitigated by correcting the visibilities before reconstructing the image. This technique is also applicable to Sgr A* at longer wavelengths.

  1. GALEX DIFFUSE OBSERVATIONS OF THE SKY: THE DATA

    SciTech Connect

    Murthy, Jayant

    2014-08-01

    I present tabulations of the diffuse observations made by the GALEX spacecraft in two UV bands (FUV: 1539 and NUV: 2316 ) from the (almost) final data release of the GALEX spacecraft (GR6/GR7). This data release includes all the FUV observations and the majority of the NUV observations. I discuss overall trends in the data but the primary purpose of this paper is to make the data available to the public. The data files described in this paper are hosted by the Mikulski Archive for Space Telescopes at the Space Telescope Science Insitute from whence they may be downloaded. For ease of use, I have also created maps of the diffuse radiation in both bands over the entire observed sky at 6' resolution.

  2. Experimental determination of the radial dose function of {sup 90}Sr/{sup 90}Y IVBT sources

    SciTech Connect

    Holmes, Shannon M.; DeWerd, Larry A.; Micka, John A.

    2006-09-15

    A series of measurements were undertaken using both high sensitivity radiochromic film and new lithium fluoride thermoluminescent dosimeters in a liquid water medium to define the radial dose function of {sup 90}Sr/{sup 90}Y beta emitting intravascular brachytherapy sources more accurately. These measurements of a single 5 French source pellet served to verify current Monte Carlo transport models and extrapolation chamber measurements of the radial dose function, thus providing the recommended independent published measurements for g(r) of these sources. A slight deviation in the published radial dose function at depth leads the authors to recommend that treatment planning be performed using updated g(r) values from current Monte Carlo transport models verified by measurements such as those shown in this investigation.

  3. Evaluation of Gas Reburning and Low N0x Burners on a Wall Fired Boiler

    SciTech Connect

    1998-09-01

    Under the U.S. Department of Energy's Clean Coal Technology Program (Round 3), a project was completed to demonstrate control of boiler emissions that comprise acid rain precursors, especially NOX. The project involved operating gas reburning technology combined with low NO, burner technology (GR-LNB) on a coal-fired utility boiler. Low NOX burners are designed to create less NOX than conventional burners. However, the NO, control achieved is in the range of 30-60-40, and typically 50%. At the higher NO, reduction levels, CO emissions tend to be higher than acceptable standards. Gas Reburning (GR) is designed to reduce the level of NO. in the flue gas by staged fuel combustion. When combined, GR and LNBs work in harmony to both minimize NOX emissions and maintain an acceptable level of CO emissions. The demonstration was performed at Public Service Company of Colorado's (PSCO) Cherokee Unit 3, located in Denver, Colorado. This unit is a 172 MW. wall-fired boiler that uses Colorado bituminous, low-sulfur coal and had a pre GR-LNB baseline NOX emission of 0.73 lb/1 Oe Btu. The target for the project was a reduction of 70 percent in NOX emissions. Project sponsors included the U.S. Department of Energy, the Gas Research Institute, Public Service Company of Colorado, Colorado Interstate Gas, Electric Power Research Institute, and the Energy and Environmental Research Corporation (EER). EER conducted a comprehensive test demonstration program over a wide range of boiler conditions. Over 4,000 hours of operation were achieved. Intensive measurements were taken to quantify the reductions in NOX emissions, the impact on boiler equipment and operability, and all factors influencing costs. The results showed that GR-LNB technology achieved excellent emission reductions. Although the performance of the low NOX burners (supplied by others) was somewhat less than expected, a NOX reduction of 65% was achieved at an average gas heat input of 180A. The performance goal of 70

  4. Synthesis, crystal structure and DFT studies of N-(4-acetyl-5,5-dimethyl-4,5-dihydro-1,3,4-thiadiazol-2-yl)acetamide

    SciTech Connect

    Gautam, P.; Gautam, D.; Chaudhary, R. P.

    2013-12-15

    The title compound N-(4-acetyl-5,5-dimethyl-4,5-dihydro-1,3,4-thiadiazol-2-yl)acetamide (III) was obtained from the reaction of 2-(propan-2-ylidene)hydrazinecarbothioamide (II) with acetic anhydride instead of formation of the desired thiosemcarbazide derivative of Meldrum acid. The structures of II and III were established by elemental analysis, IR, NMR, Mass and X-ray crystallographic studies. II crystallizes in triclinic system, sp. gr. P-bar1 Z = 2; III crystallizes in the monoclinic system, sp. gr. P2{sub 1}/c, Z = 8. Density functional theory (DFT) calculations have been carried out for III. {sup 1}H and {sup 13}C NMR of III has been calculated and correlated with experimental results.

  5. Synthesis and structure of triphenylbismuth bis(3-phenylprop-2-enoate)

    SciTech Connect

    Andreev, P. V. Somov, N. V.; Kalistratova, O. S.; Gushchin, A. V.; Chuprunov, E. V.

    2015-07-15

    The newly synthesized triphenylbismuth bis(3-phenylprop-2-enoate) was studied by X-ray diffraction and by IR, UV, and NMR spectroscopy. The crystals are monoclinic, sp. gr. C2/c, Z = 4, a = 13.2820(4) Å, b = 21.3750(2) Å, c = 12.2407(2) Å, β = 119.936(1)°. The coordination polyhedron of the bismuth atom can be described as a distorted pentagonal bipyramid.

  6. Slide 1

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    in the Blackbody Calibration of Pyrgeometers By Ibrahim Reda, Julian Gröbner * , Tom Stoffel, Daryl Myers, and Bruce Forgan ** Eighteenth Atmospheric Radiation Measurement (ARM) Program Science Team Meeting *Physikalisch-Meteorologisches Observatorium Davos, World Radiation Center (PMOD/WRC) ** Bureau of Meteorology, Australia Abstract Pyrgeometers are used to measure the atmospheric longwave irradiance through out the ARM program sites. Previous calibrations of pyrgeometers using

  7. Research Highlight

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Cloud Cover Homogenizes Arctic Vegetation Submitter: Street, L., University of Edinburgh Area of Research: Surface Properties Working Group(s): Cloud-Aerosol-Precipitation Interactions Journal Reference: Street LE, GR Shaver, EB Rastetter, MT van Wijk, BA Kaye, and M Williams. 2012. "Incident radiation and the allocation of nitrogen within Arctic plant canopies: implications for predicting gross primary productivity." Global Change Biology, 18(9), doi:10.1111/j.1365-2486.2012.02754.x.

  8. Research Highlight

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Light Absorption of Primary Organic Aerosol Paper Named ACS Editors' Choice Download a printable PDF Submitter: Lu, Z., Argonne National Laboratory Streets, D. ., Argonne National Laboratory Area of Research: Aerosol Properties Working Group(s): Aerosol Life Cycle Journal Reference: Lu Z, DG Streets, E Winijkul, F Yan, Y Chen, TC Bond, Y Feng, MK Dubey, S Liu, JP Pinto, and GR Carmichael. 2015. "Light absorption properties and radiative effects of primary organic aerosol emissions."

  9. Research Highlight

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    From Fire to Ice Download a printable PDF Submitter: Kulkarni, G., Pacific Northwest National Laboratory Area of Research: Aerosol Properties Working Group(s): Aerosol Life Cycle Journal Reference: Kulkarni GR, M Nandasiri, A Zelenyuk, J Beranek, N Madaan, A Devaraj, V Shutthanandan, S Thevuthasan, and T Varga. 2015. "Effects of crystallographic properties on the ice nucleation properties of volcanic ash particles." Geophysical Research Letters, 42(8), doi:10.1002/2015GL063270. Tons of

  10. Research Highlight

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Pollution Changes Clouds' Ice Crystal Genesis Download a printable PDF Submitter: Kulkarni, G., Pacific Northwest National Laboratory Area of Research: Cloud Processes Working Group(s): Cloud Life Cycle Journal Reference: Kulkarni GR, K Zhang, C Zhao, M Nandasiri, V Shutthanandan, X Liu, L Berg, and J Fast. 2015. "Ice formation on nitric acid-coated dust particles: Laboratory and modeling studies." Journal of Geophysical Research - Atmospheres, 120(15), doi:10.1002/2014JD022637.

  11. SASW Measurements at Hanford

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    H - Spectral Analysis of Surface Waves Hanford Site-Wide Probabilistic Seismic Hazard Analysis (PSHA): Seismic Shear Wave Velocity Profiling at Hanford, WA SASW Testing and Analysis Procedures, V s Profiles, Sensitivity Studies and Responses to Technical Integration Team Questions for Pacific Northwest National Laboratory Richland, WA by Kenneth H. Stokoe, II Yin-Cheng Lin Sungmoon Hwang, and Julia Roberts May 7, 2014 Geotechnical Engineering Report GR14-1 Geotechnical Engineering Center Civil

  12. Aluminoborosilicate glasses codoped with rare-earth elements as radiation-protective covers for solar cells

    SciTech Connect

    Malchukova, E. V. Abramov, A. S.; Nepomnyashchikh, A. I.; Terukov, E. I.

    2015-06-15

    The radiation hardness of aluminoborosilicate glasses codoped with rare-earth ions of Sm, Gd or Sm, Eu in various ratios is studied. The effect of codoping and β irradiation at a dose of 10{sup 9} Gr on the optical transmission and electron paramagnetic resonance spectra is examined. It is found that the introduction of Sm and Gd codopants in a 1 : 1 ratio reduces the number of radiation defects and raises the transmission of irradiated glasses in the visible spectral range.

  13. Is Electromagnetic Gravity Control Possible?

    SciTech Connect

    Vargas, Jose G.; Torr, Douglas G.

    2004-02-04

    We study the interplay of Einstein's Gravitation (GR) and Maxwell's Electromagnetism, where the distribution of energy-momentum is not presently known (The Feynman Lectures, Vol 2, Chapter 27, section 4). As Feynman himself stated, one might in principle use Einstein's equations of GR to find such a distribution. GR (born in 1915) presently uses the Levi-Civita connection, LCC (the LCC was born two years after GR as a new concept, and not just as the pre-existing Christoffel symbols that represent it). Around 1927, Einstein proposed for physics an alternative to the LCC that constitutes a far more sensible and powerful affine enrichment of metric Riemannian geometry. It is called teleparallelism (TP). Its Finslerian version (i.e. in the space-time-velocity arena) permits an unequivocal identification of the EM field as a geometric quantity. This in turn permits one to identify a completely geometric set of Einstein equations from curvature equations. From their right hand side, one may obtain the actual distribution of EM energy-momentum. It is consistent with Maxwell's equations, since these also are implied by the equations of structure of TP. We find that the so-far-unknown terms in this distribution amount to a total differential and do not, therefore, alter the value of the total EM energy-momentum. And yet these extra terms are at macroscopic distances enormously larger than the standard quadratic terms. This allows for the generation of measurable gravitational fields by EM fields. We thus answer affirmatively the question of the title.

  14. History of Cern

    ScienceCinema

    None

    2016-07-12

    Cérémonie à l'occasion de l'apparition du premier volume du livre sur l'histoire du Cern, avec plusieurs personnes présentes qui jouaient un rôle important dans cette organisation européenne couronnée de succès grâce à l'esprit des membres fondateurs qui est et restera essentiel

  15. How does pressure gravitate? Cosmological constant problem confronts observational cosmology

    SciTech Connect

    Narimani, Ali; Scott, Douglas; Afshordi, Niayesh E-mail: nafshordi@pitp.ca

    2014-08-01

    An important and long-standing puzzle in the history of modern physics is the gross inconsistency between theoretical expectations and cosmological observations of the vacuum energy density, by at least 60 orders of magnitude, otherwise known as the cosmological constant problem. A characteristic feature of vacuum energy is that it has a pressure with the same amplitude, but opposite sign to its energy density, while all the precision tests of General Relativity are either in vacuum, or for media with negligible pressure. Therefore, one may wonder whether an anomalous coupling to pressure might be responsible for decoupling vacuum from gravity. We test this possibility in the context of the Gravitational Aether proposal, using current cosmological observations, which probe the gravity of relativistic pressure in the radiation era. Interestingly, we find that the best fit for anomalous pressure coupling is about half-way between General Relativity (GR), and Gravitational Aether (GA), if we include Planck together with WMAP and BICEP2 polarization cosmic microwave background (CMB) observations. Taken at face value, this data combination excludes both GR and GA at around the 3 σ level. However, including higher resolution CMB observations (''highL'') or baryonic acoustic oscillations (BAO) pushes the best fit closer to GR, excluding the Gravitational Aether solution to the cosmological constant problem at the 4- 5 σ level. This constraint effectively places a limit on the anomalous coupling to pressure in the parametrized post-Newtonian (PPN) expansion, ζ{sub 4} = 0.105 ± 0.049 (+highL CMB), or ζ{sub 4} = 0.066 ± 0.039 (+BAO). These represent the most precise measurement of this parameter to date, indicating a mild tension with GR (for ΛCDM including tensors, with 0ζ{sub 4}=), and also among different data sets.

  16. Switchable Ionic Liquids: An Environmentally-friendly Medium to Synthesize

    Office of Scientific and Technical Information (OSTI)

    Nanoparticulate Green Rust (Journal Article) | SciTech Connect Switchable Ionic Liquids: An Environmentally-friendly Medium to Synthesize Nanoparticulate Green Rust Citation Details In-Document Search Title: Switchable Ionic Liquids: An Environmentally-friendly Medium to Synthesize Nanoparticulate Green Rust Under anoxic conditions, a novel nanoparticulate green rust with carbonate (nano GR) was synthesized by addition of methanol to degassed switchable ionic liquid (SWIL) solution comprised

  17. Creep behavior of a nuclear pressure vessel under severe accident conditions

    SciTech Connect

    Beghini, M.; Bertini, L.; Vitale, E.

    1996-12-31

    The results of a study on the creep behavior of the vessel lower head under severe accident conditions are reported. An experimental program aimed at the evaluation of the creep properties of A533grB steel at high temperature (800--1,100 C) and under biaxial loading is summarized and the main results reported. A Finite Element simulation of the lower head under severe accident conditions allows to show the effect of the main parameters affecting the time to rupture.

  18. Microsoft Word - NiGdNi_multilayers bh

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    A Comprehensive Study of a Rare-earth Ferromagnet/Transition Metal Ferromagnet Interface Using X-ray Magnetic Circular Dichroism The manipulation of thin-film magnetic multilayers has been an active and technologically relevant area of research since the discovery of giant magnetoresistance in magnetic multilayers by Fert and Grünberg in 1988 [1, 2]. The design of such devices is made simpler by utilizing the intrinsic properties of the materials from which they are made. In this study

  19. June 2014 Most Viewed Documents for Biology And Medicine | OSTI, US Dept of

    Office of Scientific and Technical Information (OSTI)

    Energy Office of Scientific and Technical Information June 2014 Most Viewed Documents for Biology And Medicine Modification to the Monte Carlo N-Particle (MCNP) Visual Editor (MCNPVised) to Read in Computer Aided Design (CAD) Files Randolph Schwarz; Leland L. Carter; Alysia Schwarz (2005) 37 Geothermal demonstration: Zunil food dehydration facility Maldonado, O. (Consultecnia, Guatemala City (Guatemala)); Altseimer, J.; Thayer, G.R. (Los Alamos National Lab., NM (United States)); Cooper, L.

  20. March 2014 Most Viewed Documents for Biology And Medicine | OSTI, US Dept

    Office of Scientific and Technical Information (OSTI)

    of Energy Office of Scientific and Technical Information March 2014 Most Viewed Documents for Biology And Medicine Carbon Dioxide Sequestering Using Microalgal Systems Daniel J. Stepan; Richard E. Shockey; Thomas A. Moe; Ryan Dorn (2002) 30 Dose and volume specification for reporting interstitial therapy NONE (1997) 29 Geothermal demonstration: Zunil food dehydration facility Maldonado, O. (Consultecnia, Guatemala City (Guatemala)); Altseimer, J.; Thayer, G.R. (Los Alamos National Lab., NM

  1. A Comprehensive Study of a Rare-earth Ferromagnet/Transition Metal

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Ferromagnet Interface Using X-ray Magnetic Circular Dichroism | Stanford Synchrotron Radiation Lightsource A Comprehensive Study of a Rare-earth Ferromagnet/Transition Metal Ferromagnet Interface Using X-ray Magnetic Circular Dichroism Wednesday, August 31, 2016 The manipulation of thin-film magnetic multilayers has been an active and technologically relevant area of research since the discovery of giant magnetoresistance in magnetic multilayers by Fert and Grünberg in 1988 [1, 2]. The

  2. Environmentally assisted cracking in light water reactors. Semiannual report, April--September 1991: Volume 13

    SciTech Connect

    Kassner, T F; Ruther, W E; Chung, H M; Hicks, P D; Hins, A G; Park, J Y; Soppet, W K; Shack, W J

    1992-03-01

    This report summarizes work performed by Argonne National Laboratory on fatigue and environmentally assisted cracking in high water reactors during the six months from April 1991 through September 1991. Topics that have been investigated during this period include (1) fatigue and stress corrosion cracking (SCC) of low-alloy steel used in piping and in steam generator and reactor pressure vessels; (2) role of chromate and sulfate in simulated boiling water reactor (BWR) water on SCC of sensitized Type 304 SS; and (3) radiation-induced segregation (RIS) and irradiation-assisted SCC of Type 304 SS after accumulation of relatively high fluence. Fatigue data were obtained on medium-S-content A533-Gr B and A106-Gr B steels in high-purity (HP) deoxygenated water, in simulated pressurized water reactor (PWR) water, and in air. Crack-growth-rates (CGRs) of composite specimens of A533-Gr B/Inconel-182/Inconel-600 (plated with nickel) and homogeneous specimens of A533-Gr B were determined under small- amplitude cyclic loading in HP water with {approx} 300 ppb dissolved oxygen. CGR tests on sensitized Type 304 SS indicate that low chromate concentrations in BWR water (25--35 ppb) may actually have a beneficial effect on SCC if the sulfate concentration is below a critical level. Microchemical and microstructural changes in HP and commercial-purity Type 304 SS specimens from control-blade absorber tubes used in two operating BWRs were studied by Auger electron spectroscopy and scanning electron microscopy, and slow-strain,rate- tensile tests were conducts on tubular specimens in air and in simulated BWR water at 289{degrees}C.

  3. USDA Rural Development: Sustaining Relationships in Indian Country

    Office of Energy Efficiency and Renewable Energy (EERE) (indexed site)

    Sustaining Relationships in Indian Country USDA Rural Development Organizational Structure National Office State Directors Program Directors Specialists Architects Engineers Technicians Area Directors Native American Coordinators General Field Representatives Rur al Utilities Ser vice Rur al Housing & Community Facilities Rur al Business Cooper ative Ser vice Rural Development Program Areas Progr am Areas Business & Industr y Guar anteed Loans Rur al Business Enter pr ise Gr ants Rur al

  4. Degradation mode survey of titanium-base alloys

    SciTech Connect

    Gdowski, G.E.; Ahluwalia, H.S.

    1995-01-30

    Of the materials reviewed, commercially pure titanium, Ti Gr 2, is the most susceptible to crevice corrosion. Ti Gr 7, 12, and 16 are likely to be resistant to crevice corrosion under the current expected Yucca Mountain repository conditions. Although Grade 7 has the greatest resistance to crevice corrosion it is also the most expensive. Although the possibility of sustained loads cracking exists, it has not yet been observed in a Ti alloys. For hydride precipitation to occur 100{degrees}C, the hydrogen concentration would need to be relatively high, much higher than the maximum amount of hydrogen allowed during the manufacture of ({alpha} Ti alloys (0.0 15 wt%). A large amount of (SCC) stress corrosion cracking data accumulated at SNL and BNL for the WIPP program and by the Canadian Waste Management Program on titanium grades 2 and 12 indicates that there is no SCC at naturally occurring potentials in various brines. Hydride-induced cracking of titanium is a possibility and therefore, further investigation of this phenomenon under credible repository conditions is warranted. One disadvantage of titanium and its alloys is that their strengths decrease rather rapidly with temperature. This is due to the strong temperature dependence of interstitial solute strengthening mechanisms. Ti Gr 12 and 16 are recommended for further consideration as candidate materials for high level nuclear waste containers.

  5. Theory of gyroresonance and free-free emissions from non-Maxwellian quasi-steady-state electron distributions

    SciTech Connect

    Fleishman, Gregory D.; Kuznetsov, Alexey A.

    2014-02-01

    Currently there is a concern about the ability of the classical thermal (Maxwellian) distribution to describe quasi-steady-state plasma in the solar atmosphere, including active regions. In particular, other distributions have been proposed to better fit observations, for example, kappa- and n-distributions. If present, these distributions will generate radio emissions with different observable properties compared with the classical gyroresonance (GR) or free-free emission, which implies a way of remotely detecting these non-Maxwellian distributions in the radio observations. Here we present analytically derived GR and free-free emissivities and absorption coefficients for the kappa- and n-distributions, and discuss their properties, which are in fact remarkably different from each other and from the classical Maxwellian plasma. In particular, the radio brightness temperature from a gyrolayer increases with the optical depth τ for kappa-distribution, but decreases with τ for n-distribution. This property has a remarkable consequence allowing a straightforward observational test: the GR radio emission from the non-Maxwellian distributions is supposed to be noticeably polarized even in the optically thick case, where the emission would have strictly zero polarization in the case of Maxwellian plasma. This offers a way of remote probing the plasma distribution in astrophysical sources, including solar active regions as a vivid example.

  6. Massive gravity wrapped in the cosmic web

    SciTech Connect

    Shim, Junsup; Lee, Jounghun; Li, Baojiu E-mail: jounghun@astro.snu.ac.kr

    2014-03-20

    We study how the filamentary pattern of the cosmic web changes if the true gravity deviates from general relativity (GR) on a large scale. The f(R) gravity, whose strength is controlled to satisfy the current observational constraints on the cluster scale, is adopted as our fiducial model and a large, high-resolution N-body simulation is utilized for this study. By applying the minimal spanning tree algorithm to the halo catalogs from the simulation at various epochs, we identify the main stems of the rich superclusters located in the most prominent filamentary section of the cosmic web and determine their spatial extents per member cluster to be the degree of their straightness. It is found that the f(R) gravity has the effect of significantly bending the superclusters and that the effect becomes stronger as the universe evolves. Even in the case where the deviation from GR is too small to be detectable by any other observables, the degree of the supercluster straightness exhibits a conspicuous difference between the f(R) and the GR models. Our results also imply that the supercluster straightness could be a useful discriminator of f(R) gravity from the coupled dark energy since it is shown to evolve differently between the two models. As a final conclusion, the degree of the straightness of the rich superclusters should provide a powerful cosmological test of large scale gravity.

  7. Xyce Parallel Electronic Simulator Reference Guide Version 6.4

    SciTech Connect

    Keiter, Eric R.; Mei, Ting; Russo, Thomas V.; Schiek, Richard; Sholander, Peter E.; Thornquist, Heidi K.; Verley, Jason; Baur, David Gregory

    2015-12-01

    This document is a reference guide to the Xyce Parallel Electronic Simulator, and is a companion document to the Xyce Users' Guide [1] . The focus of this document is (to the extent possible) exhaustively list device parameters, solver options, parser options, and other usage details of Xyce . This document is not intended to be a tutorial. Users who are new to circuit simulation are better served by the Xyce Users' Guide [1] . Trademarks The information herein is subject to change without notice. Copyright c 2002-2015 Sandia Corporation. All rights reserved. Xyce TM Electronic Simulator and Xyce TM are trademarks of Sandia Corporation. Portions of the Xyce TM code are: Copyright c 2002, The Regents of the University of California. Produced at the Lawrence Livermore National Laboratory. Written by Alan Hindmarsh, Allan Taylor, Radu Serban. UCRL-CODE-2002-59 All rights reserved. Orcad, Orcad Capture, PSpice and Probe are registered trademarks of Cadence Design Systems, Inc. Microsoft, Windows and Windows 7 are registered trademarks of Microsoft Corporation. Medici, DaVinci and Taurus are registered trademarks of Synopsys Corporation. Amtec and TecPlot are trademarks of Amtec Engineering, Inc. Xyce 's expression library is based on that inside Spice 3F5 developed by the EECS Department at the University of California. The EKV3 MOSFET model was developed by the EKV Team of the Electronics Laboratory-TUC of the Technical University of Crete. All other trademarks are property of their respective owners. Contacts Bug Reports (Sandia only) http://joseki.sandia.gov/bugzilla http://charleston.sandia.gov/bugzilla World Wide Web http://xyce.sandia.gov http://charleston.sandia.gov/xyce (Sandia only) Email xyce@sandia.gov (outside Sandia) xyce-sandia@sandia.gov (Sandia only)

  8. The anti-esophageal cancer cell activity by a novel tyrosine/phosphoinositide kinase inhibitor PP121

    SciTech Connect

    Peng, Yi; Zhou, Yajuan; Cheng, Long; Hu, Desheng; Zhou, Xiaoyi; Wang, Zhaohua; Xie, Conghua; Zhou, Fuxiang

    2015-09-11

    Here we explored the potential effect of PP121, a novel dual inhibitor of tyrosine and phosphoinositide kinases, against human esophageal cancer cells. We showed that PP121 exerted potent cytotoxic effect in primary (patient-derived) and established (Eca-109, TE-1 and TE-3 lines) esophageal cancer cells, possibly through activating caspase-3-dependnent apoptosis. PP121 was, however, non-cytotoxic to the normal human esophageal epithelial cells (EECs). At the molecular level, we showed that PP121 blocked Akt-mTOR (mammalian target of rapamycin) activation in esophageal cancer cells, which was restored by introducing a constitutively-active Akt (CA-Akt). Yet, CA-Akt only partly inhibited cytotoxicity by PP121 in Eca-109 cells. Importantly, we showed that PP121 inhibited nuclear factor kappa B (NFκB) signaling activation in esophageal cancer cells, which appeared independent of Akt-mTOR blockage. In vivo, oral administration of PP121 remarkably inhibited Eca-109 xenograft growth in nude mice, and significantly improved mice survival. Further, the immunohistochemistry (IHC) and Western blot assays analyzing xenografted tumors showed that PP121 inhibited Akt-mTOR and NFκB activations in vivo. Together, we demonstrate that PP121 potently inhibits esophageal cancer cells in vitro and in vivo, possibly through concurrently inhibiting Akt-mTOR and NFκB signalings. - Highlights: • PP121 is cytotoxic against primary and established esophageal cancer cells. • PP121 induces caspase-3-dependnent apoptosis in esophageal cancer cells. • PP121 blocks Akt-mTOR activation in esophageal cancer cells. • PP121 inhibits NFκB activation, independent of Akt-mTOR blockage. • PP121 inhibits Eca-109 xenograft growth and Akt-mTOR/NFκB activation in vivo.

  9. Human health safety evaluation of cosmetics in the EU: A legally imposed challenge to science

    SciTech Connect

    Pauwels, M.; Rogiers, V.

    2010-03-01

    As stated in the European legislation, cosmetic products present on the European market must be safe for the consumer. Safety evaluation of the products is carried out by a qualified safety assessor who needs to consider potential exposure scenarios next to the physicochemical and toxicological profiles of all composing ingredients. Whereas, until recently, the tools to determine the toxicological profile of cosmetic ingredients mainly consisted of animal experiments, they have now been narrowed down substantially by the legally imposed animal testing ban on cosmetic ingredients, taken up in the Cosmetic Products Directive (76/768/EEC). This Directive, however, is not a stand-alone piece of European legislation, since as well directly as indirectly it is influenced by a complex web of related legislations. Vertical legislations deal with different categories of chemicals, including dangerous substances, biocides, plant protection products, food additives, medicinal products, and of course also cosmetics. Horizontal legislative texts, on the contrary, cover more general fields such as protection of experimental animals, consumer product safety, misleading of consumers, specific provisions for aerosols, and others. Experience has learnt that having a general overview of these related legislations is necessary to understand their impact on the cosmetic world in general terms and on cosmetic safety evaluation in particular. This goes for a variety of concerned parties, including national and European regulators/agencies, contract laboratories, raw material suppliers, cosmetic companies, research and educational centers. They all deal with a number of aspects important for the quality and toxicity of cosmetics and their ingredients. This review summarises the most relevant points of the legislative texts of different types of product categories and emphasises their impact on the safety evaluation of cosmetics.

  10. Push or Pull? Proton Responsive Ligand Effects in Rhenium Tricarbonyl CO 2 Reduction Catalysts

    DOE PAGES [OSTI]

    Manbeck, Gerald F.; Muckerman, James T.; Szalda, David J.; Himeda, Yuichiro; Fujita, Etsuko

    2015-02-19

    Proton responsive ligands offer control of catalytic reactions through modulation of pH-dependent properties, second coordination sphere stabilization of transition states, or by providing a local proton source for multi-proton, multi-electron reactions. Two fac-[ReI(α-diimine)(CO)₃Cl] complexes with α-diimine = 4,4'- (or 6,6'-) dihydroxy-2,2'-bipyridine (4DHBP and 6DHBP) have been prepared and analyzed as electrocatalysts for reduction of carbon dioxide. Consecutive electrochemical reduction of these complexes yields species identical to those obtained by chemical deprotonation. An energetically feasible mechanism for reductive deprotonation is proposed in which the bpy anion is protonated followed by loss of H₂ and 2H⁺. Cyclic voltammetry reveals a two-electron, three-wavemore » system owing to competing EEC and ECE pathways. The chemical step of the ECE pathway might be attributed to the reductive deprotonation. but cannot be distinguished from chloride dissociation. The rate obtained by digital simulation is approximately 8 s⁻¹. Under CO₂, these competing reactions generate a two-slope catalytic waveform with onset potential of –1.65 V vs Ag/AgCl. Reduction of CO₂ to CO by the [ReI (4DHBP–2H⁺)(CO)₃]⁻ suggests the interaction of CO₂ with the deprotonated species or a third reduction followed by catalysis. Conversely, the reduced form of [Re(6DHBP)(CO)₃Cl] converts CO₂ to CO with a single turnover.« less

  11. Push or Pull? Proton Responsive Ligand Effects in Rhenium Tricarbonyl CO 2 Reduction Catalysts

    SciTech Connect

    Manbeck, Gerald F.; Muckerman, James T.; Szalda, David J.; Himeda, Yuichiro; Fujita, Etsuko

    2015-02-19

    Proton responsive ligands offer control of catalytic reactions through modulation of pH-dependent properties, second coordination sphere stabilization of transition states, or by providing a local proton source for multi-proton, multi-electron reactions. Two fac-[ReI(α-diimine)(CO)₃Cl] complexes with α-diimine = 4,4'- (or 6,6'-) dihydroxy-2,2'-bipyridine (4DHBP and 6DHBP) have been prepared and analyzed as electrocatalysts for reduction of carbon dioxide. Consecutive electrochemical reduction of these complexes yields species identical to those obtained by chemical deprotonation. An energetically feasible mechanism for reductive deprotonation is proposed in which the bpy anion is protonated followed by loss of H₂ and 2H⁺. Cyclic voltammetry reveals a two-electron, three-wave system owing to competing EEC and ECE pathways. The chemical step of the ECE pathway might be attributed to the reductive deprotonation. but cannot be distinguished from chloride dissociation. The rate obtained by digital simulation is approximately 8 s⁻¹. Under CO₂, these competing reactions generate a two-slope catalytic waveform with onset potential of –1.65 V vs Ag/AgCl. Reduction of CO₂ to CO by the [ReI (4DHBP–2H⁺)(CO)₃]⁻ suggests the interaction of CO₂ with the deprotonated species or a third reduction followed by catalysis. Conversely, the reduced form of [Re(6DHBP)(CO)₃Cl] converts CO₂ to CO with a single turnover.

  12. SU-E-I-07: An Improved Technique for Scatter Correction in PET

    SciTech Connect

    Lin, S; Wang, Y; Lue, K; Lin, H; Chuang, K

    2014-06-01

    Purpose: In positron emission tomography (PET), the single scatter simulation (SSS) algorithm is widely used for scatter estimation in clinical scans. However, bias usually occurs at the essential steps of scaling the computed SSS distribution to real scatter amounts by employing the scatter-only projection tail. The bias can be amplified when the scatter-only projection tail is too small, resulting in incorrect scatter correction. To this end, we propose a novel scatter calibration technique to accurately estimate the amount of scatter using pre-determined scatter fraction (SF) function instead of the employment of scatter-only tail information. Methods: As the SF depends on the radioactivity distribution and the attenuating material of the patient, an accurate theoretical relation cannot be devised. Instead, we constructed an empirical transformation function between SFs and average attenuation coefficients based on a serious of phantom studies with different sizes and materials. From the average attenuation coefficient, the predicted SFs were calculated using empirical transformation function. Hence, real scatter amount can be obtained by scaling the SSS distribution with the predicted SFs. The simulation was conducted using the SimSET. The Siemens Biograph 6 PET scanner was modeled in this study. The Software for Tomographic Image Reconstruction (STIR) was employed to estimate the scatter and reconstruct images. The EEC phantom was adopted to evaluate the performance of our proposed technique. Results: The scatter-corrected image of our method demonstrated improved image contrast over that of SSS. For our technique and SSS of the reconstructed images, the normalized standard deviation were 0.053 and 0.182, respectively; the root mean squared errors were 11.852 and 13.767, respectively. Conclusion: We have proposed an alternative method to calibrate SSS (C-SSS) to the absolute scatter amounts using SF. This method can avoid the bias caused by the insufficient

  13. Evaluation of Gas Reburning and Low N0x Burners on a Wall Fired Boiler

    SciTech Connect

    1998-07-01

    Under the U.S. Department of Energy's Clean Coal Technology Program (Round 3), a project was completed to demonstrate control of boiler NOX emissions and to a lesser degree, due to coal replacement, SO2 emissions. The project involved combining Gas Reburning with Low NOX Burners (GR-LNB) on a coal-fired electric utility boiler to determine if high levels of NO, reduction (70VO) could be achieved. Sponsors of the project included the U.S. Depatiment of Energy, the Gas Research Institute, Public Service Company of Colorado, Colorado Interstate Gas, Electric Power Research Institute, and the Energy and Environmental Research Corporation. The GR-LNB demonstration was petformed on Public Service Company of Colorado's (PSCO) Cherokee Unit #3, located in Denver, Colorado. This unit is a 172 MW~ wall-fired boiler that uses Colorado bituminous, low-sulfur coal. It had a baseline NO, emission level of 0.73 lb/1 OG Btu using conventional burners. Low NOX burners are designed to yield lower NOX emissions than conventional burners. However, the NOX control achieved with this technique is limited to 30-50Y0. Also, with LNBs, CO emissions can increase to above acceptable standards. Gas Reburning (GR) is designed to reduce NO, in the flue gas by staged fuel combustion. This technology involves the introduction of' natural gas into the hot furnace flue gas stream. When combined, GR and LNBs minimize NOX emissions and maintain acceptable levels of CO emissions. A comprehensive test program was completed, operating over a wide range of boiler conditions. Over 4,000 hours of operation were achieved, providing substantial data. Measurements were taken to quantify reductions in NOX emissions, the impact on boiler equipment and operability and factors influencing costs. The GR-LNB technology achieved good NO, emission reductions and the goals of the project were achieved. Although the performance of the low NOX burners (supplied by others) was less than expected, a NOX reduction of 65

  14. Biochemical characterization of nuclear receptors for vitamin D{sub 3} and glucocorticoids in prostate stroma cell microenvironment

    SciTech Connect

    Hidalgo, Alejandro A.; Montecinos, Viviana P.; Paredes, Roberto; Godoy, Alejandro S.; McNerney, Eileen M.; Tovar, Heribelt; Pantoja, Diego; Johnson, Candace; Trump, Donald; Onate, Sergio A.

    2011-08-19

    Highlights: {yields} Fibroblasts from benign and carcinoma-associated stroma were biochemically characterized for VDR and GR function as transcription factors in prostate stroma cell microenvironment. {yields} Decreased SRC-1/CBP coactivators recruitment to VDR and GR may result in hormone resistance to 1,25D{sub 3} in stromal cell microenvironment prostate cancer. {yields} 1a,25-Dyhidroxyvitamin D{sub 3} (1,25D{sub 3}) and glucocorticoids, either alone or in combination, may not be an alternative for 'some' advanced prostate cancers that fails androgen therapies. -- Abstract: The disruption of stromal cell signals in prostate tissue microenvironment influences the development of prostate cancer to androgen independence. 1{alpha},25-Dihydroxyvitamin D{sub 3} (1,25D{sub 3}) and glucocorticoids, either alone or in combination, have been investigated as alternatives for the treatment of advanced prostate cancers that fails androgen therapies. The effects of glucocorticoids are mediated by the intracellular glucocorticoid receptor (GR). Similarly, the effect of 1,25D{sub 3} is mediated by the 1,25D{sub 3} nuclear receptor (VDR). In this study, fibroblasts from benign- (BAS) and carcinoma-associated stroma (CAS) were isolated from human prostates to characterize VDR and GR function as transcription factors in prostate stroma. The VDR-mediated transcriptional activity assessed using the CYP24-luciferase reporter was limited to 3-fold induction by 1,25D{sub 3} in 9 out of 13 CAS (70%), as compared to >10-fold induction in the BAS clinical sample pair. Expression of His-tagged VDR (Ad-his-VDR) failed to recover the low transcriptional activity of the luciferase reporter in 7 out of 9 CAS. Interestingly, expression of Ad-his-VDR successfully recovered receptor-mediated induction in 2 out of the 9 CAS analyzed, suggesting that changes in the receptor protein itself was responsible for decreased response and resistance to 1,25D{sub 3} action. Conversely, VDR

  15. Switchgrass (Panicum virgatum L.) Intraspecific Variation and Thermotolerance Classification Using in Vitro Seed Germination Assay

    DOE PAGES [OSTI]

    Seepaul, Ramdeo; Macoon, Bisoondat; Reddy, K. Raja; Baldwin, Brian

    2011-06-01

    Cardinal temperatures for plant processes have been used for thermotolerance screening of genotypes, geoclimatic adaptability determination and phenological prediction. Current simulation models for switchgrass (Panicum virgatum L.) utilize single cardinal temperatures across genotypes for both vegetative and reproductive processes although in-tra-specific variation exists among genotypes. An experiment was conducted to estimate the cardinal temperatures for seed germination of 14 diverse switchgrass genotypes and to classify genotypes for temperature tolerance. Stratified seeds of each genotype were germinated at eight constant temperatures from 10 °C to 45 °C under a constant light intensity of 35 μmol m-2s-1 for 12 hd-1. Germination wasmore » recorded at 6-h intervals in all treatments. Maximum seed germination (MSG) and germination rate (GR), estimated by fitting Sigmoidal function to germination-time series data, varied among genotypes. Quadratic and bilinear models best described the MSG and GR responses to temperature, respectively. The mean cardinal temperatures, Tmin, Topt, and Tmax, were 8.1, 26.6, and 45.1 °C for MSG and 11.1, 33.1, and 46.0 °C for GR, respectively. Cardinal temperatures for MSG and GR; however, varied significantly among genotypes. Genotypes were classified as sensitive (Cave-in-Rock, Dacotah, Expresso, Forestburg˜, Kanlow, ˜Sunburst, Trailblazer, and ˜Tusca™), intermediate (˜Alamo, Blackwell, Carthage, ˜Shawnee™, and Shelter™) and tolerant (˜Summer) to high temperature based on cumulative temperature response index (CTRI) estimated by summing individual response indices estimated from the MSG and GR cardinal temperatures. Similarly, genotypes were also classified as sensitive (Alamo, Blackwell, Carthage, Dacotah, Shawnee, Shelter and Summer), moderately sensitive (Cave-in-rock, Forestburg, Kanlow, Sunburst, and Tusca), moderately tolerant (Trailblazer), and tolerant (Expresso) to low temperatures. The cardinal

  16. Time varying arctic climate change amplification

    SciTech Connect

    Chylek, Petr; Dubey, Manvendra K; Lesins, Glen; Wang, Muyin

    2009-01-01

    During the past 130 years the global mean surface air temperature has risen by about 0.75 K. Due to feedbacks -- including the snow/ice albedo feedback -- the warming in the Arctic is expected to proceed at a faster rate than the global average. Climate model simulations suggest that this Arctic amplification produces warming that is two to three times larger than the global mean. Understanding the Arctic amplification is essential for projections of future Arctic climate including sea ice extent and melting of the Greenland ice sheet. We use the temperature records from the Arctic stations to show that (a) the Arctic amplification is larger at latitudes above 700 N compared to those within 64-70oN belt, and that, surprisingly; (b) the ratio of the Arctic to global rate of temperature change is not constant but varies on the decadal timescale. This time dependence will affect future projections of climate changes in the Arctic.

  17. Latitudinal distribution of the recent Arctic warming

    SciTech Connect

    Chylek, Petr; Lesins, Glen K; Wang, Muyin

    2010-12-08

    Increasing Arctic temperature, disappearance of Arctic sea ice, melting of the Greenland ice sheet, sea level rise, increasing strength of Atlantic hurricanes are these impending climate catastrophes supported by observations? Are the recent data really unprecedented during the observational records? Our analysis of Arctic temperature records shows that the Arctic and temperatures in the 1930s and 1940s were almost as high as they are today. We argue that the current warming of the Arctic region is affected more by the multi-decadal climate variability than by an increasing concentration of carbon dioxide. Unfortunately, none of the existing coupled Atmosphere-Ocean General Circulation Models used in the IPCC 2007 cIimate change assessment is able to reproduce neither the observed 20th century Arctic cIimate variability nor the latitudinal distribution of the warming.

  18. Laurentide Ice Sheet meltwater and abrupt climate change during the last glaciation

    SciTech Connect

    Hill, H W; Flower, B P; Quinn, T M; Hollander, D J; Guilderson, T P

    2005-10-02

    A leading hypothesis to explain abrupt climate change during the last glacial cycle calls on fluctuations in the margin of the North American Laurentide Ice Sheet (LIS), which may have routed freshwater between the Gulf of Mexico (GOM) and North Atlantic, affecting North Atlantic Deep Water (NADW) variability and regional climate. Paired measurements of {delta}O and Mg/Ca of foraminiferal calcite from GOM sediments reveal five episodes of LIS meltwater input from 28-45 thousand years ago (ka) that do not match the millennial-scale Dansgaard-Oeschger (D/O) warmings recorded in Greenland ice. We suggest that summer melting of the LIS may occur during Antarctic warming and likely contributed to sea-level variability during Marine Isotope Stage 3 (MIS 3).

  19. Evaluation of Gas Reburning & Low NOx Burners on a Wall Fired Boiler Performance and Economics Report Gas Reburning-Low NOx Burner System Cherokee Station Unit 3 Public Service Company of Colorado

    SciTech Connect

    1998-07-01

    Under the U.S. Department of Energy's Clean Coal Technology Program (Round 3), a project was completed to demonstrate control of boiler NOX emissions and to a lesser degree, due to coal replacement, SO2 emissions. The project involved combining Gas Reburning with Low NOX Burners (GR-LNB) on a coal-fired electric utility boiler to determine if high levels of NOX reduction (70%) could be achieved. Sponsors of the project included the U.S. Department of Energy, the Gas Research Institute, Public Service Company of Colorado, Colorado Interstate Gas, Electric Power Research Institute, and the Energy and Environmental Research Corporation. The GR-LNB demonstration was performed on Public Service Company of Colorado's (PSCO) Cherokee Unit #3, located in Denver, Colorado. This unit is a 172 MW~ wall-fired boiler that uses Colorado Bituminous, low-sulfur coal. It had a baseline NOX emission level of 0.73 lb/106 Btu using conventional burners. Low NOX burners are designed to yield lower NOX emissions than conventional burners. However, the NOX control achieved with this technique is limited to 30-50%. Also, with LNBs, CO emissions can increase to above acceptable standards. Gas Reburning (GR) is designed to reduce NOX in the flue gas by staged fuel combustion. This technology involves the introduction of natural gas into the hot furnace flue gas stream. When combined, GR and LNBs minimize NOX emissions and maintain acceptable levels of CO emissions. A comprehensive test program was completed, operating over a wide range of boiler conditions. Over 4,000 hours of operation were achieved, providing substantial data. Measurements were taken to quantify reductions in NOX emissions, the impact on boiler equipment and operability and factors influencing costs. The GR-LNB technology achieved good NOX emission reductions and the goals of the project were achieved. Although the performance of the low NOX burners (supplied by others) was less than expected, a NOX reduction of 65% was

  20. A multi-model assessment of pollution transport to the Arctic

    SciTech Connect

    Shindell, D T; Chin, M; Dentener, F; Doherty, R M; Faluvegi, G; Fiore, A M; Hess, P; Koch, D M; MacKenzie, I A; Sanderson, M G; Schultz, M G; Schulz, M; Stevenson, D S; Teich, H; Textor, C; Wild, O; Bergmann, D J; Bey, I; Bian, H; Cuvelier, C; Duncan, B N; Folberth, G; Horowitz, L W; Jonson, J; Kaminski, J W; Marmer, E; Park, R; Pringle, K J; Schroeder, S; Szopa, S; Takemura, T; Zeng, G; Keating, T J; Zuber, A

    2008-03-13

    We examine the response of Arctic gas and aerosol concentrations to perturbations in pollutant emissions from Europe, East and South Asia, and North America using results from a coordinated model intercomparison. These sensitivities to regional emissions (mixing ratio change per unit emission) vary widely across models and species. Intermodel differences are systematic, however, so that the relative importance of different regions is robust. North America contributes the most to Arctic ozone pollution. For aerosols and CO, European emissions dominate at the Arctic surface but East Asian emissions become progressively more important with altitude, and are dominant in the upper troposphere. Sensitivities show strong seasonality: surface sensitivities typically maximize during boreal winter for European and during spring for East Asian and North American emissions. Mid-tropospheric sensitivities, however, nearly always maximize during spring or summer for all regions. Deposition of black carbon (BC) onto Greenland is most sensitive to North American emissions. North America and Europe each contribute {approx}40% of total BC deposition to Greenland, with {approx}20% from East Asia. Elsewhere in the Arctic, both sensitivity and total BC deposition are dominated by European emissions. Model diversity for aerosols is especially large, resulting primarily from differences in aerosol physical and chemical processing (including removal). Comparison of modeled aerosol concentrations with observations indicates problems in the models, and perhaps, interpretation of the measurements. For gas phase pollutants such as CO and O{sub 3}, which are relatively well-simulated, the processes contributing most to uncertainties depend on the source region and altitude examined. Uncertainties in the Arctic surface CO response to emissions perturbations are dominated by emissions for East Asian sources, while uncertainties in transport, emissions, and oxidation are comparable for European

  1. Van der Waals epitaxial growth of two-dimensional single-crystalline GaSe domains on graphene

    DOE PAGES [OSTI]

    Li, Xufan; Basile, Leonardo; Huang, Bing; Ma, Cheng; Lee, Jaekwang; Vlassiouk, Ivan V.; Puretzky, Alexander A.; Lin, Ming -Wei; Chi, Miaofang; Idrobo Tapia, Juan Carlos; et al

    2015-07-22

    Two-dimensional (2D) van der Waals (vdW) heterostructures are a family of artificially-structured materials that promise tunable optoelectronic properties for devices with enhanced functionalities. Compared to stamping, direct epitaxy of vdW heterostructures is ideal for clean interlayer interfaces and scalable device fabrication. Here, we explore the synthesis and preferred orientations of 2D GaSe atomic layers on graphene (Gr) by vdW epitaxy. Guided by the wrinkles on graphene, GaSe nuclei form that share a predominant lattice orientation. Due to vdW epitaxial growth many nuclei grow as perfectly aligned crystals and coalesce to form large (tens of microns), single-crystal flakes. Through theoretical investigationsmore » of interlayer energetics, and measurements of preferred orientations by atomic-resolution STEM and electron diffraction, a 10.9 interlayer rotation of the GaSe lattice with respect to the underlying graphene is found to be the most energetically preferred vdW heterostructure with the largest binding energy and the longest-range ordering. These GaSe/Gr vdW heterostructures exhibit an enhanced Raman E21g band of monolayer GaSe along with highly-quenched photoluminescence due to strong charge transfer. Despite the very large lattice mismatch of GaSe/Gr through vdW epitaxy, the predominant orientation control and convergent formation of large single-crystal flakes demonstrated here is promising for the scalable synthesis of large-area vdW heterostructures for the development of new optical and optoelectronic devices.« less

  2. Van der Waals epitaxial growth of two-dimensional single-crystalline GaSe domains on graphene

    SciTech Connect

    Li, Xufan; Basile, Leonardo; Huang, Bing; Ma, Cheng; Lee, Jaekwang; Vlassiouk, Ivan V.; Puretzky, Alexander A.; Lin, Ming -Wei; Chi, Miaofang; Idrobo Tapia, Juan Carlos; Rouleau, Christopher M.; Sumpter, Bobby G.; Yoon, Mina; Geohegan, David B.; Xiao, Kai

    2015-07-22

    Two-dimensional (2D) van der Waals (vdW) heterostructures are a family of artificially-structured materials that promise tunable optoelectronic properties for devices with enhanced functionalities. Compared to stamping, direct epitaxy of vdW heterostructures is ideal for clean interlayer interfaces and scalable device fabrication. Here, we explore the synthesis and preferred orientations of 2D GaSe atomic layers on graphene (Gr) by vdW epitaxy. Guided by the wrinkles on graphene, GaSe nuclei form that share a predominant lattice orientation. Due to vdW epitaxial growth many nuclei grow as perfectly aligned crystals and coalesce to form large (tens of microns), single-crystal flakes. Through theoretical investigations of interlayer energetics, and measurements of preferred orientations by atomic-resolution STEM and electron diffraction, a 10.9 interlayer rotation of the GaSe lattice with respect to the underlying graphene is found to be the most energetically preferred vdW heterostructure with the largest binding energy and the longest-range ordering. These GaSe/Gr vdW heterostructures exhibit an enhanced Raman E21g band of monolayer GaSe along with highly-quenched photoluminescence due to strong charge transfer. Despite the very large lattice mismatch of GaSe/Gr through vdW epitaxy, the predominant orientation control and convergent formation of large single-crystal flakes demonstrated here is promising for the scalable synthesis of large-area vdW heterostructures for the development of new optical and optoelectronic devices.

  3. Van der Waals Epitaxial Growth of Single-Crystal Two-Dimensional GaSe on Graphene

    DOE PAGES [OSTI]

    Li, Xufan; Basile, Leonardo; Huang, Bing; Ma, Cheng; Lee, Jaekwang; Vlassiouk, Ivan V.; Puretzky, Alexander A.; Lin, Ming-Wei; Chi, Miaofang; Idrobo Tapia, Juan Carlos; et al

    2015-07-22

    Two-dimensional (2D) van der Waals (vdW) heterostructures are a family of artificially-structured materials that promise tunable optoelectronic properties for devices with enhanced functionalities. Compared to stamping, direct epitaxy of vdW heterostructures is ideal for clean interlayer interfaces and scalable device fabrication. Here, we explore the synthesis and preferred orientations of 2D GaSe atomic layers on graphene (Gr) by vdW epitaxy. Guided by the wrinkles on graphene, GaSe nuclei form that share a predominant lattice orientation. Due to vdW epitaxial growth many nuclei grow as perfectly aligned crystals and coalesce to form large (tens of microns), single-crystal flakes. Through theoretical investigationsmoreof interlayer energetics, and measurements of preferred orientations by atomic-resolution STEM and electron diffraction, a 10.9 interlayer rotation of the GaSe lattice with respect to the underlying graphene is found to be the most energetically preferred vdW heterostructure with the largest binding energy and the longest-range ordering. These GaSe/Gr vdW heterostructures exhibit an enhanced Raman E21g band of monolayer GaSe along with highly-quenched photoluminescence due to strong charge transfer. Despite the very large lattice mismatch of GaSe/Gr through vdW epitaxy, the predominant orientation control and convergent formation of large single-crystal flakes demonstrated here is promising for the scalable synthesis of large-area vdW heterostructures for the development of new optical and optoelectronic devices.less

  4. Environmentally assisted cracking in Light Water Reactors. Volume 16: Semiannual report, October 1992--March 1993

    SciTech Connect

    Chung, H.M.; Chopra, O.K.; Ruther, W.E.; Kassner, T.F.; Michaud, W.F.; Park, J.Y.; Sanecki, J.E.; Shack, W.J.

    1993-09-01

    This report summarizes work performed by Argonne National Laboratory on fatigue and environmentally assisted cracking (EAC) in light water reactors (LWRs) during the six months from October 1992 to March 1993. Fatigue and EAC of piping, pressure vessels, and core components in LWRs are important concerns as extended reactor lifetimes are envisaged. Topics that have been investigated include (1) fatigue of low-alloy steel used in piping, steam generators, and reactor pressure vessels. (2) EAC of cast stainless steels (SSs), (3) radiation-induced segregation and irradiation-assisted stress corrosion cracking of Type 304 SS after accumulation of relatively high fluence, and (4) EAC of low-alloy steels. Fatigue tests were conducted on medium-sulfur-content A106-Gr B piping and A533-Gr B pressure vessel steels in simulated PWR water and in air. Additional crack growth data were obtained on fracture-mechanics specimens of cast austenitic SSs in the as-received and thermally aged conditions and chromium-nickel-plated A533-Gr B steel in simulated boiling-water reactor (BWR) water at 289{degrees}C. The data were compared with predictions based on crack growth correlations for ferritic steels in oxygenated water and correlations for wrought austenitic SS in oxygenated water developed at ANL and rates in air from Section XI of the ASME Code. Microchemical and microstructural changes in high- and commercial-purity Type 304 SS specimens from control-blade absorber tubes and a control-blade sheath from operating BWRs were studied by Auger electron spectroscopy and scanning electron microscopy.

  5. The dark side of galaxy colour: evidence from new SDSS measurements of galaxy clustering and lensing

    SciTech Connect

    Hearin, Andrew P.; Watson, Douglas F.; Becker, Matthew R.; Reyes, Reinabelle; Berlind, Andreas A.; Zentner, Andrew R.

    2014-08-12

    The age matching model has recently been shown to predict correctly the luminosity L and g-r color of galaxies residing within dark matter halos. The central tenet of the model is intuitive: older halos tend to host galaxies with older stellar populations. In this paper, we demonstrate that age matching also correctly predicts the g-r color trends exhibited in a wide variety of statistics of the galaxy distribution for stellar mass M* threshold samples. In particular, we present new measurements of the galaxy two-point correlation function and the galaxy-galaxy lensing signal as a function of M* and g-r color from the Sloan Digital Sky Survey, and show that age matching exhibits remarkable agreement with these and other statistics of low-redshift galaxies. In so doing, we also demonstrate good agreement between the galaxy-galaxy lensing observed by SDSS and the signal predicted by abundance matching, a new success of this model. We describe how age matching is a specific example of a larger class of Conditional Abundance Matching models (CAM), a theoretical framework we introduce here for the first time. CAM provides a general formalism to study correlations at fixed mass between any galaxy property and any halo property. The striking success of our simple implementation of CAM provides compelling evidence that this technique has the potential to describe the same set of data as alternative models, but with a dramatic reduction in the required number of parameters. CAM achieves this reduction by exploiting the capability of contemporary N-body simulations to determine dark matter halo properties other than mass alone, which distinguishes our model from conventional approaches to the galaxy-halo connection.

  6. Crystallization and preliminary X-ray diffraction study of porcine carboxypeptidase B

    SciTech Connect

    Akparov, V. Kh.; Timofeev, V. I. Kuranova, I. P.

    2015-05-15

    Crystals of porcine pancreatic carboxypeptidase B have been grown in microgravity by the capillary counter-diffusion method through a gel layer. The X-ray diffraction study showed that the crystals belong to sp. gr. P4{sub 1}2{sub 1}2 and have the following unit-cell parameters: a = b = 79.58 Å, c = 100.51 Å; α = β = γ = 90.00°. The X-ray diffraction data set suitable for the determination of the three-dimensional structure at atomic resolution was collected from one of the grown crystals at the SPring 8 synchrotron facility to 0.98 Å resolution.

  7. Research & patents generated by Nobel Laureate discovery highlighted at

    Office of Scientific and Technical Information (OSTI)

    OSTI | OSTI, US Dept of Energy Office of Scientific and Technical Information & patents generated by Nobel Laureate discovery highlighted at OSTI Back to the OSTI News Listing for 2007 A discovery in 1988 has yielded not only the 2007 Nobel Prize in Physics, but a birthing of subsequent DOE research and patents now at OSTI. GMR, or Giant Magnetoresistance, is considered an early application in the growing field of nanotechnology. In 1988, Dr. Peter Grünberg of Forschungszentrum Jülich

  8. Evaluation of In-Situ Tritium Transport Parameters for Type 316 Stainless Steel during Irradiation

    Office of Environmental Management (EM)

    In-Situ Tritium Transport Parameters for Type 316 Stainless Steel during Irradiation D.J. Senor, W.G. Luscher K.K. Clayton, G.R. Longhurst Tritium Focus Group Meeting Savannah River National Laboratory Aiken, SC 23 April 2014 PNNL-SA-102143 Motivation and Scope TMIST-2 Experiment Measured in-reactor steady state tritium permeation through Type 316 stainless steel as a function of tritium partial pressure and temperature Tritium permeation irradiation enhancement of ~3X was observed relative to

  9. A=8B (1988AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    8AJ01) (See Energy Level Diagrams for 8B) GENERAL: See also (1984AJ01) and Table 8.9 [Table of Energy Levels] (in PDF or PS) here. Model calculations: (1983SH38). Special states: (1982PO12, 1988KH03). Complex reactions involving 8B: (1982AL08, 1983OL1A, 1984GR08, 1986HA1B, 1987TAZU, 1988AR05, 1988KI05). Astrophysical questions: (1984HA1B, 1985BO1E, 1985GI1C, 1985KL1A, 1985LA1C, 1988BA86). Reactions involving pions: (1983SP06). Hypernuclei: (1983SH38). Other topics: (1985AN28). Ground state of

  10. Raymond Murphy | Inventors | GE Global Research

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    Raymond Murphy Raymond Murphy Water Technical Manager GR Oil & Gas Technology Center Click to email this to a friend (Opens in new window) Share on Facebook (Opens in new window) Click to share (Opens in new window) Click to share on LinkedIn (Opens in new window) Click to share on Tumblr (Opens in new window) "The oil & gas industry is in constant search of water treatment products that promise smarter, cheaper and more environmentally friendly operation. We invent those

  11. High pressure melting curves of silver, gold and copper

    SciTech Connect

    Hieu, Ho Khac

    2013-11-15

    In this work, based on the Lindemann's formula of melting and the pressure-dependent Grüneisen parameter, we have investigated the pressure effect on melting temperature of silver, gold and copper metals. The analytical expression of melting temperature as a function of volume compression has been derived. Our results are compared with available experimental data as well as with previous theoretical studies and the good and reasonable agreements are found. We also proposed the potential of this approach on predicting melting of copper at very high pressure.

  12. Development of integrated mechanistically-based degradation-mode models for performance assessment of high-level waste containers

    SciTech Connect

    Bedrossian, P; Estill, J; Farmer, J; Hopper, R; Horn, J; Huang, J S; McCright, D; Roy, A; Wang, F; Wilfinger, K

    1999-02-08

    A key component of the Engineered Barrier System (EBS) being designed for containment of spent-fuel and high-level waste at the proposed geological repository at Yucca Mountain, Nevada is a two-layer canister. In this particular design, the inner barrier is made of a corrosion resistant material (CRM) such as Alloy 825, 625 or C-22, while the outer barrier is made of a corrosion-allowance material (CAM) such as A516 Gr 55, a carbon steel, or Monel 400. At the present time, Alloy C-22 and A516 G4 55 are favored.

  13. Experimental Validation Data for Computational Fluid Dynamics of Forced Convection on a Vertical Flat Plate

    DOE PAGES [OSTI]

    Harris, Jeff R.; Lance, Blake W.; Smith, Barton L.

    2015-08-10

    We present computational fluid dynamics (CFD) validation dataset for turbulent forced convection on a vertical plate. The design of the apparatus is based on recent validation literature and provides a means to simultaneously measure boundary conditions (BCs) and system response quantities (SRQs). Important inflow quantities for Reynolds-Averaged Navier-Stokes (RANS). CFD are also measured. Data are acquired at two heating conditions and cover the range 40,000 < Rex < 300,000, 357 < Reδ2 < 813, and 0.02 < Gr/Re2 < 0.232.

  14. Experimental Validation Data for Computational Fluid Dynamics of Forced Convection on a Vertical Flat Plate

    SciTech Connect

    Harris, Jeff R.; Lance, Blake W.; Smith, Barton L.

    2015-08-10

    We present computational fluid dynamics (CFD) validation dataset for turbulent forced convection on a vertical plate. The design of the apparatus is based on recent validation literature and provides a means to simultaneously measure boundary conditions (BCs) and system response quantities (SRQs). Important inflow quantities for Reynolds-Averaged Navier-Stokes (RANS). CFD are also measured. Data are acquired at two heating conditions and cover the range 40,000 < Rex < 300,000, 357 < Reδ2 < 813, and 0.02 < Gr/Re2 < 0.232.

  15. Shear viscosity coefficient of liquid lanthanides

    SciTech Connect

    Patel, H. P. Thakor, P. B. Prajapati, A. V.; Sonvane, Y. A.

    2015-05-15

    Present paper deals with the computation of shear viscosity coefficient (η) of liquid lanthanides. The effective pair potential v(r) is calculated through our newly constructed model potential. The Pair distribution function g(r) is calculated from PYHS reference system. To see the influence of local field correction function, Hartree (H), Tailor (T) and Sarkar et al (S) local field correction function are used. Present results are compared with available experimental as well as theoretical data. Lastly, we found that our newly constructed model potential successfully explains the shear viscosity coefficient (η) of liquid lanthanides.

  16. Scapolite as a potential sensor of fluid composition in calc-silicates and granulites

    SciTech Connect

    Moecher, D.P.; Essene, E.J.

    1985-01-01

    Scapolite has been proposed as reservoir for CO/sub 2/ in the lower crust (Goldsmith 1976) and as a sensor of fluid composition in scapolite-bearing calc-silicates and granulites. The scapolite decarbonation reaction 2Meionite(Me)+Quartz(Qz)=5Anorthite(An)+Grossular(Gr)+2CO/sub 2/, obtained by addition of the reaction 3An+Cc=Me and An+2Cc+Qz=Gr+2CO/sub 2/, is a potential equilibrium applicable to a variety of lithologies and grades by which CO/sub 2/ activities could theoretically be calculated. Assuming partial ordering in natural scapolite, and S/sub 298//sup 0/ (Me)=728.6J/mol x K, the scapolite decarbonation reaction has a virtually flat slope in the range 700-1000/sup 0/C and 2.2+/-0.1kb with 2Me+Qz on the high P side of the reaction. Values of logK for the reaction were determined at elevated P, and aCO/sub 2/ calculated for scapolite-bearing calc-silicate assemblages (Sc+Pg+Gt+Q+Di+/-Cc) from Perry Sound (PS), Ontario and the Furua Complex (FC), Tanzania (Coolen 1980), for which X(Gr)approx. =0.8, X(An)approx. =0.6-0.8, and X(Me)greater than or equal to0.7. The a-X relations used were Perkins (1979) for garnet, Newton and Perkins (1982) for plagioclase, and Oterdoom and Gunter (1983) for scapolite. However application of the scapolite decarbonation reaction to garnet-bearing granulites with X(Gr)less than or equal to0.20 yields erroneous estimates of aCO/sub 2/(greater than or equal to1.0) suggesting incorrect assumptions used to determine S/sub 298//sup 0/ for stably ordered meionite or the a-X relations of Oterdoom and Gunter. Further refinement of the thermodynamic data base and evaluation of the degree and effect of order-disorder in natural scapolites must be performed in order to use scapolite to calculate fluid composition in high grade metamorphites.

  17. Diquat induces renal proximal tubule injury in glutathione reductase-deficient mice

    SciTech Connect

    Rogers, Lynette K. . E-mail: rogersl@ccri.net; Bates, Carlton M.; Welty, Stephen E.; Smith, Charles V.

    2006-12-15

    Reactive oxygen species (ROS) have been associated with many human diseases, and glutathione (GSH)-dependent processes are pivotal in limiting tissue damage. To test the hypothesis that Gr1{sup a1Neu} (Neu) mice, which do not express glutathione reductase (GR), would be more susceptible than are wild-type mice to ROS-mediated injury, we studied the effects of diquat, a redox cycling toxicant. Neu mice exhibited modest, dose- and time-dependent elevations in plasma alanine aminotransferase (ALT) activities, 126 {+-} 36 U/l at 2 h after 5 {mu}mol/kg of diquat, but no ALT elevations were observed in diquat-treated C3H/HeN mice for up to 6 h after 50 {mu}mol/kg of diquat. Histology indicated little or no hepatic necrosis in diquat-treated mice of either strain, but substantial renal injury was observed in diquat-treated Neu mice, characterized by brush border sloughing in the proximal tubules by 1 h and tubular necrosis by 2 h after doses of 7.5 {mu}mol/kg. Decreases in renal GSH levels were observed in the Neu mice by 2 h post dose (3.4 {+-} 0.4 vs 0.2 {+-} 0.0 {mu}mol/g tissue at 0 and 50 {mu}mol/kg, respectively), and increases in renal GSSG levels were observed in the Neu mice as early as 0.5 h after 7.5 {mu}mol/kg (105.5 {+-} 44.1 vs 27.9 {+-} 4.8 nmol/g tissue). Blood urea nitrogen levels were elevated by 2 h in Neu mice after doses of 7.5 {mu}mol/kg (Neu vs C3H, 32.8 {+-} 4.1 vs 17.9 {+-} 0.3 mg/dl). Diquat-induced renal injury in the GR-deficient Neu mice offers a useful model for studies of ROS-induced renal necrosis and of the contributions of GR in defense against oxidant-mediated injuries in vivo.

  18. Table Definitions, Sources, and Explanatory Notes

    Gasoline and Diesel Fuel Update

    API Gravity Definitions Key Terms Definition API Gravity An arbitrary scale expressing the gravity or density of liquid petroleum products. The measuring scale is calibrated in terms of degrees API; it is calculated as follows: Degrees API = (141.5 / (sp. gr. 60ºF / 60ºF)) - 131.5 The higher the API gravity, the lighter the compound. Light crudes generally exceed 38 degrees API and heavy crudes are commonly labeled as all crudes with an API gravity of 22 degrees or below. Intermediate crudes

  19. LA--12O48-MS DE91

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    -12O48-MS DE91 010299 I ~ I i Tm Thou.mwl Yews of Solitude? 0)1 llzfuhwh!lll Illfrlwiml i)ffo fhc Wmtefsolfltiwl Pilot Project Rqwsitory GrL~gor!/B L')/fo)"(i* Craig W. Kirhood** HmwjOfwf7y Marfit~/. Pmquak!!i+ ~~~~n~~~~L..Al...s.Me. M.xico 87541 L A N L % D I O T D I U E Table of Contents Preface . . . . . . . . . . . . . . . . . . . . . . . . . . .. .. .. .. .. .. .. D O . . . . . . . . . . . ...ooOO.OO..OOOOO"OO".OO """"."" 'ti 1. Introduction . .

  20. Grande Ronde Basin Chinook Salmon Captive Brood and Conventional Supplementation Program, 2000 Annual Report.

    SciTech Connect

    Carmichael, Richard W.

    2003-03-01

    Endangered Species Permit Number 1011 (formerly Permit No. 973) authorizes ODFW to take listed spring chinook salmon juveniles from Catherine Creek (CC), Lostine River (LR) and Grande Ronde River (GR) for research and enhancement purposes. Modification 2 of this permit authorizes ODFW to take adults for spawning and the production and release of smolts for the Captive and Conventional broodstock programs. This report satisfies the requirement that an annual report be submitted. Herein we report on activities conducted and provide cursory data analyses for the Grande Ronde spring chinook salmon Captive and Conventional broodstock projects from 1 January-31 December 2000.

  1. Xyce Parallel Electronic Simulator Users Guide Version 6.2.

    SciTech Connect

    Keiter, Eric R.; Mei, Ting; Russo, Thomas V.; Schiek, Richard Louis; Sholander, Peter E.; Thornquist, Heidi K.; Verley, Jason C.; Baur, David Gregory

    2014-09-01

    registered trademarks of Cadence Design Systems, Inc. Microsoft, Windows and Windows 7 are registered trademarks of Microsoft Corporation. Medici, DaVinci and Taurus are registered trademarks of Synopsys Corporation. Amtec and TecPlot are trademarks of Amtec Engineering, Inc. Xyce 's expression library is based on that inside Spice 3F5 developed by the EECS Department at the University of California. The EKV3 MOSFET model was developed by the EKV Team of the Electronics Laboratory-TUC of the Technical University of Crete. All other trademarks are property of their respective owners. Contacts Bug Reports (Sandia only) http://joseki.sandia.gov/bugzilla http://charleston.sandia.gov/bugzilla World Wide Web http://xyce.sandia.gov http://charleston.sandia.gov/xyce (Sandia only) Email xyce@sandia.gov (outside Sandia) xyce-sandia@sandia.gov (Sandia only)

  2. Orthorhombic YBaCo{sub 4}O{sub 8.4} crystals as a result of saturation of hexagonal YBaCo{sub 4}O{sub 7} crystals with oxygen

    SciTech Connect

    Podberezskaya, N. V.; Bolotina, N. B.; Komarov, V. Yu. Kameneva, M. Yu.; Kozeeva, L. P.; Lavrov, A. N.; Smolentsev, A. I.

    2015-07-15

    Hexagonal YBaCo{sub 4}O{sub 7} crystals (sp. gr. P6{sub 3}mc, a{sub h} = 6.3058(4) Å, c{sub h} = 10.2442(7) Å, Z = 2) are saturated with oxygen to the YBaCo{sub 4}O{sub 8.4} composition and studied by X-ray diffraction (XRD) analysis. The saturation is completed by a structural first-order phase transition to orthorhombic crystals (sp. gr. Pbc2{sub 1}, a{sub o} = 31.8419(2) Å, b{sub o} = 10.9239(5) Å, c{sub o} = 10.0960(5) Å, Z = 20). The connection of two lattices is expressed in terms of the action of matrix (500/120/001) on the hexagonal basis. Five structural fragments of the same type but with different degrees of order alternate along the long axis of the oxygen-saturated orthorhombic structure. The XRD data on single crystals differ from the results obtained by other researchers on ceramic samples; possible causes of these differences are discussed.

  3. Gravitational mass of positron from LEP synchrotron losses

    DOE PAGES [OSTI]

    Kalaydzhyan, Tigran

    2016-07-27

    General relativity(GR) is the current description of gravity in modern physics. One of the cornerstones of GR, as well as Newton’s theory of gravity, is the weak equivalence principle (WEP), stating that the trajectory of a freely falling test body is independent of its internal structure and composition. WEP is known to be valid for the normal matter with a high precision. However, due to the rarity of antimatter and weakness of the gravitational forces, the WEP has never been confirmed for antimatter. The current direct bounds on the ratio between the gravitational and inertial masses of the antihydrogen domore » not rule out a repulsive nature for the antimatter gravity. Here we establish an indirect bound of 0.13% on the difference between the gravitational and inertial masses of the positron (antielectron) from the analysis of synchrotron losses at the Large Electron-Positron collider (LEP). As a result, this serves as a confirmation of the conventional gravitational properties of antimatter without common assumptions such as, e.g., coupling of gravity to virtual particles, dynamics of distant astrophysical sources and the nature of absolute gravitational potentials.« less

  4. Crystalline and spin chiralities in multiferroics with langasite-type structure and Fe{sub 1–x}Co{sub x}Si crystals

    SciTech Connect

    Pikin, S. A. Lyubutin, I. S.; Dudka, A. P.

    2015-09-15

    It is shown that, when magnetic ordering occurs in layered iron-containing langasites (sp. gr. P321), one of the reasons for spin chiralities of different signs is the presence of structural chirality (the existence of inversion twins), which, in turn, is due to the nonsymmetricity of these crystals. Spin helicoids arise in these multiferroics at split sites of Fe{sup 3+} ions below the Néel point. The direction of electric polarization vectors coincides with the direction of the magnetic helicoid axes because of the piezoelectric properties of these materials. Due to the magnetostriction effects, structural chirality wave vector k{sub z} exceeds the magnetic helicoid wave vector by a factor of 2: k{sub z} = 2q{sub z}. The temperatures of transitions to the chiral structural and chiral magnetic states may differ. In particular, if the structural transition initial temperature exceeds the magnetic transition temperature (Τ{sub U}> Τ{sub M}), structural displacements may arise in the absence of magnetism at Τ{sub M} < Τ < Τ{sub U}. In noncentrosymmetric Fe{sub 1–x}Co{sub x}Si crystals (sp. gr. P2{sub 1}3), which are not multiferroics, magnetic chirality is due to the Dzyaloshinski–Moriya interaction. The dependence of the moduli of incommensurate wave number of the corresponding helicoid on the atomic composition of the crystals under consideration is nonmonotonic.

  5. Particle image velocimetry measurements for opposing flow in a vertical channel with a differential and asymmetric heating condition

    SciTech Connect

    Martinez-Suastegui, L. [Graduate Student, Facultad de Ingenieria, Universidad Nacional Autonoma de Mexico, C.U., Mexico 04510 D.F. (Mexico); Trevino, C. [Facultad de Ciencias, Universidad Nacional Autonoma de Mexico, C.U., Mexico 04510 D.F. (Mexico)

    2007-10-15

    Particle image velocimetry (PIV) measurements were carried out in an experimental investigation of laminar mixed convection in a vertical duct with a square cross-section. The main downward water-flow is driven by gravity while a portion of a lateral side is heated, and buoyancy forces produce non-stationary vortex structures close to the heated region. Various ranges of the Grashof number, Gr are studied in combination with the Reynolds number, Re varying from 300 to 700. The values of the generalized buoyancy parameter or Richardson number, Ri = Gr/Re{sup 2} parallel to the Grashof number are included in the results. The influence of these nondimensional parameters and how they affect the fluid flow structure and vortex sizes and locations are reported. The flow patterns are nonsymmetric, periodic, and exhibit increasing complexity and frequency for increasing buoyancy. For the averaged values of the resulting vortex dimensions, it was found that a better and more congruent representation occurs when employing the Grashof and Reynolds numbers as independent parameters. (author)

  6. Photocatalytic and antibacterial properties of Au-TiO{sub 2} nanocomposite on monolayer graphene: From experiment to theory

    SciTech Connect

    He, Wangxiao; Huang, Hongen; Yan, Jin; Zhu, Jian

    2013-11-28

    The formation of the Au-TiO{sub 2} nanocomposite on monolayer Graphene (GTA) by sequentially depositing titanium dioxide particles and gold nanoparticles on graphene sheet was synthesized and analyzed in our work. The structural, morphological, and physicochemical properties of samples were thoroughly investigated by UV-Vis spectrophotometer, Raman spectroscopy, Fourier transform infrared spectroscopy, atomic force microscopy, scanning electron microscope, and transmission electron microscope. Photocatalytic performance of GTA, graphene (GR), TiO{sub 2,} and TiO{sub 2} -graphene nanocomposite (GT) were comparatively studied for degradation of methyl orange, and it was found that GTA had highest performance among all samples. More importantly, antibacterial performance of this novel composite against Gram-positive bacteria, Gram-negative bacteria, and fungus was predominant compared to GR, TiO{sub 2}, and GT. And the result of biomolecules oxidation tests suggested that antimicrobial actions were contributed by oxidation stress on both membrane and antioxidant systems. Besides, the rate of two decisive processes during photocatalytic reaction, the rate of the charge transfer (k{sub CT}) and the rate of the electron-hole recombination (k{sub R}) have been studied by Perturbation theory, Radiation theory, and Schottky barrier theory. Calculation and derivation results show that GTA possesses superior charge separation and transfer rate, which gives an explanation for the excellent oxidation properties of GTA.

  7. Large-scale structure in brane-induced gravity. I. Perturbation theory

    SciTech Connect

    Scoccimarro, Roman

    2009-11-15

    We study the growth of subhorizon perturbations in brane-induced gravity using perturbation theory. We solve for the linear evolution of perturbations taking advantage of the symmetry under gauge transformations along the extra-dimension to decouple the bulk equations in the quasistatic approximation, which we argue may be a better approximation at large scales than thought before. We then study the nonlinearities in the bulk and brane equations, concentrating on the workings of the Vainshtein mechanism by which the theory becomes general relativity (GR) at small scales. We show that at the level of the power spectrum, to a good approximation, the effect of nonlinearities in the modified gravity sector may be absorbed into a renormalization of the gravitational constant. Since the relation between the lensing potential and density perturbations is entirely unaffected by the extra physics in these theories, the modified gravity can be described in this approximation by a single function, an effective gravitational constant for nonrelativistic motion that depends on space and time. We develop a resummation scheme to calculate it, and provide predictions for the nonlinear power spectrum. At the level of the large-scale bispectrum, the leading order corrections are obtained by standard perturbation theory techniques, and show that the suppression of the brane-bending mode leads to characteristic signatures in the non-Gaussianity generated by gravity, generic to models that become GR at small scales through second-derivative interactions. We compare the predictions in this work to numerical simulations in a companion paper.

  8. Film condensation of saturated and superheated vapors along isothermal vertical surfaces in mixed convection

    SciTech Connect

    Winkler, C.M.; Chen, T.S.; Minkowycz, W.J.

    1999-09-01

    An analysis for condensation from an isothermal vertical flat plate in mixed convection is reported. The entire mixed convection regime is divided into two regions. One region covers the forced-convection-dominated regime, and the other covers the free-convection-dominated regime. The governing system of equations is first transformed into a dimensionless form by the nonsimilar transformation, separately for each regime, and then solved using the local nonsimilarity method along with a finite difference scheme. Two nonsimilarity parameters are introduced. The parameter {xi}{sub f} = Gr{sub x}/Re{sub x}{sup 2} characterizes the effect of buoyancy force on forced convection, while the parameter {xi}{sub n} = Re{sub x}/Gr{sub x}{sup 1/2} characterizes the effect of forced flow on free convection. Numerical results for pure steam and refrigerant R-134a are presented for both saturated and superheated cases. It is found that the buoyancy force significantly increases the wall shear stress and condensate mass flux. To a lesser degree, the buoyancy force also increases the wall heat flux. Superheating is found to have an insignificant effect on wall heat flux for a pure vapor.

  9. PAMAM dendrimers and graphene: Materials for removing aromatic contaminants from water

    SciTech Connect

    DeFever, Ryan S.; Geitner, Nicholas K.; Bhattacharya, Priyanka; Ding, Feng; Ke, Pu Chun; Sarupria, Sapna

    2015-04-07

    We present results from experiments and atomistic molecular dynamics simulations on the association of naphthalene with polyamidoamine (PAMAM) dendrimers and graphene oxide (GrO). Specifically, we investigate 3rd-6th generation (G3-G6) PAMAM dendrimers and GrO with different levels of oxidation. The work is motivated by the potential applications of these materials in removing polycyclic aromatic hydrocarbon contaminants from water. Our experimental results indicate that graphene oxide outperforms dendrimers in removing naphthalene from water. Molecular dynamics simulations suggest that the prominent factors driving naphthalene association to these seemingly disparate materials are similar. Interestingly, we find that cooperative interactions between the naphthalene molecules play a significant role in enhancing their association to the dendrimers and graphene oxide. Our findings highlight that while selection of appropriate materials is important, the interactions between the contaminants themselves can also be important in governing the effectiveness of a given material. The combined use of experiments and molecular dynamics simulations allows us to comment on the possible factors resulting in better performance of graphene oxide in removing naphthalene from water.

  10. Emergent cosmology revisited

    SciTech Connect

    Bag, Satadru; Sahni, Varun; Shtanov, Yuri; Unnikrishnan, Sanil E-mail: varun@iucaa.ernet.in E-mail: sanil@lnmiit.ac.in

    2014-07-01

    We explore the possibility of emergent cosmology using the effective potential formalism. We discover new models of emergent cosmology which satisfy the constraints posed by the cosmic microwave background (CMB). We demonstrate that, within the framework of modified gravity, the emergent scenario can arise in a universe which is spatially open/closed. By contrast, in general relativity (GR) emergent cosmology arises from a spatially closed past-eternal Einstein Static Universe (ESU). In GR the ESU is unstable, which creates fine tuning problems for emergent cosmology. However, modified gravity models including Braneworld models, Loop Quantum Cosmology (LQC) and Asymptotically Free Gravity result in a stable ESU. Consequently, in these models emergent cosmology arises from a larger class of initial conditions including those in which the universe eternally oscillates about the ESU fixed point. We demonstrate that such an oscillating universe is necessarily accompanied by graviton production. For a large region in parameter space graviton production is enhanced through a parametric resonance, casting serious doubts as to whether this emergent scenario can be past-eternal.

  11. Light hadron spectra in the constituent quark model with the Kobayashi-Kondo-Maskawa-'t Hooft effective U {sub A} (1) symmetry breaking interaction

    SciTech Connect

    Dmitrasinovic, V. . E-mail: dmitrasin@yahoo.com; Toki, H.

    2006-02-15

    We make a critical comparison of several versions of instanton-induced interactions present in the literature, all based on ITEP group's extension to three colours and flavours of 't Hooft's effective lagrangian, with the predictions of the phenomenological Kobayashi-Kondo-Maskawa (KKM) chiral quark lagrangian. We analyze the effects of all versions of the effective U {sub A} (1) symmetry breaking interactions on light hadron spectra in the non-relativistic constituent quark model. We show that the KKMT force, when used as a residual hyperfine interaction reproduces the correct ordering of pseudoscalar and vector mesons even without explicitly taking chiral symmetry into account. Moreover, the nucleon spectra are also correctly reproduced, only the Roper resonance remains too high, albeit lower than usual, at 1660 MeV. The latter's lower than expected mass is not due to a small excitation energy, as in the Glozman-Riska (GR) model, but to a combination of colour, flavour, and spatial wave function properties that enhance the relevant matrix elements. The KKMT interaction explicitly depends on flavour and spin of the quarks, but unlike the GR flavour-spin one it has a firm footing in QCD. In the process we provide several technical advances, in particular we show the first explicit derivation of the three-body Fierz transformation and apply it to the KKM interaction. We also discuss the ambiguities associated with the colour degree of freedom.

  12. Buoyant instabilities in downward flow in a symmetrically heated vertical channel

    SciTech Connect

    Evans, G.; Greif, R.

    1996-07-01

    This study of the downward flow of nitrogen in a tall, partially heated vertical channel (upstream isothermal at T{sub in}*, heated region isothermal at T{sub s}* downstream adiabatic) shows the strong effects of buoyancy even for small temperature differences. Time-dependent oscillations including periodic flow reversals occur along the channel walls. Although the flow and heat transfer are asymmetric, the temperature and axial component of velocity show symmetric reflections at two times that are half a period apart and the lateral component of velocity shows antisymmetric reflections at the two times. There is strong interaction between the downward flow in the central region of the channel and the upward flow along the heated channel walls. At the top of the heated region, the upward buoyant flow turns toward the center of the channel and is incorporated into the downward flow. Along the channel centerline there are nonmonotonic variations of the axial component of velocity and temperature and a large lateral component of velocity that reverses direction periodically. Results are presented for Re = 219.7 and Gr/Re{sup 2} = 1.83, 8.0, and 13.7. The heat transfer and the frequency of the oscillations increases and the flow and temperature fields become more complex as Gr/Re{sup 2} increases. The results have applications to fiber drying, food processing, crystal growth, solar energy collection, cooling of electronic circuits, ventilation, etc.

  13. Structure of complexes of nitrilo tris methylene phosphonic acid with copper, [CuN(CH{sub 2}PO{sub 3}){sub 3}(H{sub 2}O){sub 3}] and Na{sub 4}[CuN(CH{sub 2}PO{sub 3}){sub 3}]{sub 2} · 19H{sub 2}O, as bactericides and inhibitors of scaling and corrosion

    SciTech Connect

    Somov, N. V.; Chausov, F. F.

    2015-03-15

    Nitrilotris methylene phosphonate triaqua copper and octasodium bis(nitrilotris methylene phosphonate cuprate(II)) nonadecahydrate have been synthesized and investigated. [CuN(CH{sub 2}PO{sub 3}){sub 3}(H{sub 2}O){sub 3}] is crystallized in the sp. gr. P2{sub 1}/c, Z = 4, a = 9.2506(2) Å, b = 15.9815(2) Å, c = 9.5474(2) Å, β = 113.697(2)°. The copper atom is coordinated by oxygen atoms in the configuration of elongated octahedron; the ligand (of bridge type) links neighboring copper atoms. Na{sub 8}[CuN(CH{sub 2}PO{sub 3}){sub 3}]{sub 2} · 19H{sub 2}O is crystallized in the sp. gr. P2{sub 1}/c, Z = 2, a = 11.24550(10) Å, b = 17.38980(10) Å, c = 13.5852(2) Å, β = 127.8120(10)°. This complex is chelating; the copper atom closes three five-membered N-C-P-O-Cu cycles with a shared Cu-N bond. Copper is coordinated in a distorted trigonal-bipyramidal configuration.

  14. The MGGB equation-of-state for multifield applications: a numerical recipe for analytic expression of sesame EOS data

    SciTech Connect

    Kashiwa, B. A.

    2010-12-01

    Abstract A thermodynamically consistent and fully general equationof state (EOS) for multifield applications is described. EOS functions are derived from a Helmholtz free energy expressed as the sum of thermal (fluctuational) and collisional (condensedphase) contributions; thus the free energy is of the MieGruneisen1 form. The phasecoexistence region is defined using a parameterized saturation curve by extending the form introduced by Guggenheim,2 which scales the curve relative to conditions at the critical point. We use the zerotemperature condensedphase contribution developed by Barnes,3 which extends the ThomasFermiDirac equation to zero pressure. Thus, the functional form of the EOS could be called MGGB (for Mie GruneisenGuggenheimBarnes). Substancespecific parameters are obtained by fitting the lowdensity energy to data from the Sesame4 library; fitting the zerotemperature pressure to the Sesame cold curve; and fitting the saturation curve and latent heat to laboratory data,5 if available. When suitable coexistence data, or Sesame data, are not available, then we apply the Principle of Corresponding States.2 Thus MGGB can be thought of as a numerical recipe for rendering the tabular Sesame EOS data in an analytic form that includes a proper coexistence region, and which permits the accurate calculation of derivatives associated with compressibility, expansivity, Joule coefficient, and specific heat, all of which are required for multifield applications. 1

  15. Degradation mode survey candidate titanium-base alloys for Yucca Mountain project waste package materials. Revision 1

    SciTech Connect

    Gdowski, G.E.

    1997-12-01

    The Yucca Mountain Site Characterization Project (YMP) is evaluating materials from which to fabricate high-level nuclear waste containers (hereafter called waste packages) for the potential repository at Yucca Mountain, Nevada. Because of their very good corrosion resistance in aqueous environments titanium alloys are considered for container materials. Consideration of titanium alloys is understandable since about one-third (in 1978) of all titanium produced is used in applications where corrosion resistance is of primary importance. Consequently, there is a considerable amount of data which demonstrates that titanium alloys, in general, but particularly the commercial purity and dilute {alpha} grades, are highly corrosion resistant. This report will discuss the corrosion characteristics of Ti Gr 2, 7, 12, and 16. The more highly alloyed titanium alloys which were developed by adding a small Pd content to higher strength Ti alloys in order to give them better corrosion resistance will not be considered in this report. These alloys are all two phase ({alpha} and {beta}) alloys. The palladium addition while making these alloys more corrosion resistant does not give them the corrosion resistance of the single phase {alpha} and near-{alpha} (Ti Gr 12) alloys.

  16. Li-Ion polymer cells thermal property changes as a function of cycle-life

    SciTech Connect

    Maleki, Hossein; Wang, Hsin; Porter, Wallace D; Hallmark, Jerry

    2014-01-01

    The impact of elevated temperature chargeedischarge cycling on thermal conductivity (K-value) of Lithium Ion Polymer (LIP) cells of various chemistries from three different manufacturers was investigated. These included high voltage (Graphite/LiCoO2:3.0e4.35 V), wide voltage (Si:C/LiCoO2:2.7e4.35 V) and conventional (Graphite/LiCoO2:3.0e4.2 V) chemistries. Investigation results show limited variability within the in-plane and through-plane K-values for the fresh cells with graphite-based anodes from all three suppliers. After 500 cycles at 45 C, in-plane and through-plane K-values of the high voltage cells reduced less vs. those for the wide voltage cells. Such results suggest that high temperature cycling could have a greater impact on thermal properties of Si:C cells than on the LIP cells with graphite (Gr) anode cells we tested. This difference is due to the excess swelling of Si:C-anode based cells vs. Gr-anode cells during cycling, especially at elevated temperatures. Thermal modeling is used to evaluate the impact of K-value changes, due to cycles at 45 C, on the cells internal heat propagation under internal short circuit condition that leads to localized meltdown of the separator.

  17. Enhancing the use of coals by gas reburning-sorbent injection

    SciTech Connect

    Not Available

    1988-12-22

    The objective of this project is to evaluate and demonstrate a cost effective emission control technology for acid rain precursors, oxides of nitrogen (NO{sub x}) and sulfur (SO{sub x}), on three coal fired utility boilers in Illinois. The units selected are representative of pre-NSPS design practices; tangential, wall, and cyclone fired. The specific objectives are to demonstrate reductions of 60 percent in NO{sub x} and 50 percent in SO{sub x} emissions, by a combination of two developed technologies, gas reburning (GR) and sorbent injection (SI). With GR, about 80--85 percent of the coal fuel is fired in the primary combustion zone. The balance of the fuel is added downstream as natural gas to create a slightly fuel rich environment in which NO{sub x} is converted to N{sub 2}. The combustion process is completed by overfire air addition. SO{sub x} emissions are reduced by injecting dry sorbents (usually calcium based) into the upper furnace, at the superheater exit or into the ducting following the air heater. The sorbents trap SO{sub x} as solid sulfates and sulfites, which are collected in the particulate control device.

  18. Neutrophils and monocytes transport tumor cell antigens from the peritoneal cavity to secondary lymphoid tissues

    SciTech Connect

    Terasawa, Masao; Nagata, Kisaburo [Division of Molecular Medicine, Department of Biomolecular Science, Faculty of Science, Toho University, 2-2-1, Miyama, Funabashi (Japan); Kobayashi, Yoshiro [Division of Molecular Medicine, Department of Biomolecular Science, Faculty of Science, Toho University, 2-2-1, Miyama, Funabashi (Japan)], E-mail: yoshiro@biomol.sci.toho-u.ac.jp

    2008-12-12

    Antigen-transporting cells take up pathogens, and then migrate from sites of inflammation to secondary lymphoid tissues to induce an immune response. Among antigen-transporting cells, dendritic cells (DCs) are believed to be the most potent and professional antigen-presenting cells that can stimulate naive T cells. However, the cells that transport antigens, tumor cell antigens in particular, have not been clearly identified. In this study we have analyzed what types of cells transport tumor cell antigens to secondary lymphoid tissues. We show that neutrophils, monocytes and macrophages but not DCs engulf X-irradiated P388 leukemic cells after their injection into the peritoneal cavity, and that neutrophils and monocytes but not macrophages migrate to the parathymic lymph nodes (pLN), the blood, and then the spleen. The monocytes in the pLN comprise Gr-1{sup -} and Gr-1{sup +} ones, and some of these cells express CD11c. Overall, this study demonstrates that neutrophils and monocytes transport tumor cell antigens from the peritoneal cavity to secondary lymphoid tissues.

  19. Monte Carlo calculations and experimental measurements of dosimetric parameters of the IRA-{sup 103}Pd brachytherapy source

    SciTech Connect

    Sadeghi, Mahdi; Raisali, Gholamreza; Hosseini, S. Hamed; Shavar, Arzhang

    2008-04-15

    This article presents a brachytherapy source having {sup 103}Pd adsorbed onto a cylindrical silver rod that has been developed by the Agricultural, Medical, and Industrial Research School for permanent implant applications. Dosimetric characteristics (radial dose function, anisotropy function, and anisotropy factor) of this source were experimentally and theoretically determined in terms of the updated AAPM Task group 43 (TG-43U1) recommendations. Monte Carlo simulations were used to calculate the dose rate constant. Measurements were performed using TLD-GR200A circular chip dosimeters using standard methods employing thermoluminescent dosimeters in a Perspex phantom. Precision machined bores in the phantom located the dosimeters and the source in a reproducible fixed geometry, providing for transverse-axis and angular dose profiles over a range of distances from 0.5 to 5 cm. The Monte Carlo N-particle (MCNP) code, version 4C simulation techniques have been used to evaluate the dose-rate distributions around this model {sup 103}Pd source in water and Perspex phantoms. The Monte Carlo calculated dose rate constant of the IRA-{sup 103}Pd source in water was found to be 0.678 cGy h{sup -1} U{sup -1} with an approximate uncertainty of {+-}0.1%. The anisotropy function, F(r,{theta}), and the radial dose function, g(r), of the IRA-{sup 103}Pd source were also measured in a Perspex phantom and calculated in both Perspex and liquid water phantoms.

  20. Spherically symmetric analysis on open FLRW solution in non-linear massive gravity

    SciTech Connect

    Chiang, Chien-I; Izumi, Keisuke; Chen, Pisin E-mail: izumi@phys.ntu.edu.tw

    2012-12-01

    We study non-linear massive gravity in the spherically symmetric context. Our main motivation is to investigate the effect of helicity-0 mode which remains elusive after analysis of cosmological perturbation around an open Friedmann-Lemaitre-Robertson-Walker (FLRW) universe. The non-linear form of the effective energy-momentum tensor stemming from the mass term is derived for the spherically symmetric case. Only in the special case where the area of the two sphere is not deviated away from the FLRW universe, the effective energy momentum tensor becomes completely the same as that of cosmological constant. This opens a window for discriminating the non-linear massive gravity from general relativity (GR). Indeed, by further solving these spherically symmetric gravitational equations of motion in vacuum to the linear order, we obtain a solution which has an arbitrary time-dependent parameter. In GR, this parameter is a constant and corresponds to the mass of a star. Our result means that Birkhoff's theorem no longer holds in the non-linear massive gravity and suggests that energy can probably be emitted superluminously (with infinite speed) on the self-accelerating background by the helicity-0 mode, which could be a potential plague of this theory.

  1. Cutting-edge issues of core-collapse supernova theory

    SciTech Connect

    Kotake, Kei; Nakamura, Ko; Kuroda, Takami; Takiwaki, Tomoya

    2014-05-02

    Based on multi-dimensional neutrino-radiation hydrodynamic simulations, we report several cutting-edge issues about the long-veiled explosion mechanism of core-collapse supernovae (CCSNe). In this contribution, we pay particular attention to whether three-dimensional (3D) hydrodynamics and/or general relativity (GR) would or would not help the onset of explosions. By performing 3D simulations with spectral neutrino transport, we show that it is more difficult to obtain an explosion in 3D than in 2D. In addition, our results from the first generation of full general relativistic 3D simulations including approximate neutrino transport indicate that GR can foster the onset of neutrino-driven explosions. Based on our recent parametric studies using a light-bulb scheme, we discuss impacts of nuclear energy deposition behind the supernova shock and stellar rotation on the neutrino-driven mechanism, both of which have yet to be included in the self-consistent 3D supernova models. Finally we give an outlook with a summary of the most urgent tasks to extract the information about the explosion mechanisms from multi-messenger CCSN observables.

  2. Environmentally assisted cracking in light water reactors. Semiannual report, April 1994--September 1994, Volume 19

    SciTech Connect

    Chopra, O.K.; Chung, H.M.; Gavenda, D.J.

    1995-09-01

    This report summarizes work performed by Argonne National Laboratory (ANL) on fatigue and environmentally assisted cracking (EAC) in light water reactors from April to September 1994. Topics that have been investigated include (a) fatigue of carbon and low-alloy steel used in piping and reactor pressure vessels, (b) EAC of austenitic stainless steels (SSs) and Alloy 600, and (c) irradiation-assisted stress corrosion cracking (IASCC) of Type 304 SS. Fatigue tests have been conducted on A106-Gr B and A533-Gr B steels in oxygenated water to determine whether a slow strain rate applied during different portions of a tensile-loading cycle are equally effective in decreasing fatigue life. Crack growth data were obtained on fracture-mechanics specimens of SSs and Alloy 600 to investigate EAC in simulated boiling water reactor (BWR) and pressurized water reactor environments at 289{degrees}C. The data were compared with predictions from crack growth correlations developed at ANL for SSs in water and from rates in air from Section XI of the ASME Code. Microchemical changes in high- and commercial-purity Type 304 SS specimens from control-blade absorber tubes and a control-blade sheath from operating BWRs were studied by Auger electron spectroscopy and scanning electron microscopy to determine whether trace impurity elements may contribute to IASCC of these materials.

  3. Ground-state and dynamical properties of two-dimensional dipolar Fermi liquids

    SciTech Connect

    Abedinpour, Saeed H.; Asgari, Reza; Tanatar, B.; Polini, Marco

    2014-01-15

    We study the ground-state properties of a two-dimensional spin-polarized fluid of dipolar fermions within the EulerLagrange Fermi-hypernetted-chain approximation. Our method is based on the solution of a scattering Schrdinger equation for the pair amplitude ?(g(r)), where g(r) is the pair distribution function. A key ingredient in our theory is the effective pair potential, which includes a bosonic term from JastrowFeenberg correlations and a fermionic contribution from kinetic energy and exchange, which is tailored to reproduce the HartreeFock limit at weak coupling. Very good agreement with recent results based on quantum Monte Carlo simulations is achieved over a wide range of coupling constants up to the liquid-to-crystal quantum phase transition. Using the fluctuationdissipation theorem and a static approximation for the effective inter-particle interactions, we calculate the dynamical densitydensity response function, and furthermore demonstrate that an undamped zero-sound mode exists for any value of the interaction strength, down to infinitesimally weak couplings. -- Highlights: We have studied the ground state properties of a strongly correlated two-dimensional fluid of dipolar fermions. We have calculated the effective inter-particle interaction and the dynamical densitydensity response function. We have shown that an undamped zero sound mode exists at any value of the interaction strength.

  4. Single-well experimental design for studying residual trapping of superciritcal carbon dioxide

    SciTech Connect

    Zhang, Y.; Freifeld, B.; Finsterle, S.; Leahy, M.; Ennis-King, J.; Paterson, L.; Dance, T.

    2010-06-15

    The objective of our research is to design a single-well injection-withdrawal test to evaluate residual phase trapping at potential CO{sub 2} geological storage sites. Given the significant depths targeted for CO{sub 2} storage and the resulting high costs associated with drilling to those depths, it is attractive to develop a single-well test that can provide data to assess reservoir properties and reduce uncertainties in the appraisal phase of site investigation. The main challenges in a single-well test design include (1) difficulty in quantifying the amount of CO{sub 2} that has dissolved into brine or migrated away from the borehole; (2) non-uniqueness and uncertainty in the estimate of the residual gas saturation (S{sub gr}) due to correlations among various parameters; and (3) the potential biased S{sub gr} estimate due to unaccounted heterogeneity of the geological medium. To address each of these challenges, we propose (1) to use a physical-based model to simulation test sequence and inverse modeling to analyze data information content and to quantify uncertainty; (2) to jointly use multiple data types generated from different kinds of tests to constrain the Sgr estimate; and (3) to reduce the sensitivity of the designed tests to geological heterogeneity by conducting the same test sequence in both a water-saturated system and a system with residual gas saturation. To perform the design calculation, we build a synthetic model and conduct a formal analysis for sensitivity and uncertain quantification. Both parametric uncertainty and geological uncertainty are considered in the analysis. Results show (1) uncertainty in the estimation of Sgr can be reduced by jointly using multiple data types and repeated tests; and (2) geological uncertainty is essential and needs to be accounted for in the estimation of S{sub gr} and its uncertainty. The proposed methodology is applied to the design of a CO{sub 2} injection test at CO2CRC's Otway Project Site, Victoria

  5. Arsenic Sequestration By Sorption Processes in High-Iron Sediments

    SciTech Connect

    Root, R.A.; Dixit, S.; Campbell, K.M.; Jew, A.D.; Hering, J.G.; O'Day, P.A.

    2009-06-04

    High-iron sediments in North Haiwee Reservoir (Olancha, CA), resulting from water treatment for removal of elevated dissolved arsenic in the Los Angeles Aqueduct system, were studied to examine arsenic partitioning between solid phases and porewaters undergoing shallow burial. To reduce arsenic in drinking water supplies, ferric chloride and a cationic polymer coagulant are added to the aqueduct upstream of Haiwee Reservoir, forming an iron-rich floc that scavenges arsenic from the water. Analysis by synchrotron X-ray absorption spectroscopy (XAS) showed that the aqueduct precipitate is an amorphous hydrous ferric oxide (HFO) similar to ferrihydrite, and that arsenic is associated with the floc as adsorbed and/or coprecipitated As(V). Arsenic-rich floc and sediments are deposited along the inlet channel as aqueduct waters enter the reservoir. Sediment core samples were collected in two consecutive years from the edge of the reservoir along the inlet channel using 30- or 90-cm push cores. Cores were analyzed for total and extractable arsenic and iron concentrations. Arsenic and iron speciation and mineralogy in sediments were examined at selected depths by synchrotron XAS and X-ray diffraction (XRD). Sediment-porewater measurements were made adjacent to the core sample sites using polyacrylamide gel probe samplers. Results showed that sediment As(V) is reduced to As(III) in all cores at or near the sediment-water interface (0--4 cm), and only As(III) was observed in deeper sediments. Analyses of EXAFS spectra indicated that arsenic is present in the sediments mostly as a bidentate-binuclear, inner-sphere sorption complex with local atomic geometries similar to those found in laboratory studies. Below about 10 cm depth, XAS indicated that the HFO floc had been reduced to a mixed Fe(II, III) solid with a local structure similar to that of synthetic green rust (GR) but with a slightly contracted average interatomic Fe-Fe distance in the hydroxide layer. There was no

  6. Probing the nature of electron transfer in metalloproteins on graphene-family materials as nanobiocatalytic scaffold using electrochemistry

    SciTech Connect

    Gupta, Sanju; Irihamye, Aline

    2015-03-15

    Graphene-based nanomaterials have shown great promise not only in nanoelectronics due to ultrahigh electron mobility but also as biocatalytic scaffolds owing to irreversible protein surface adsorption and facilitating direct electron transfer. In this work, we synthesized stable dispersions of graphene using liquid-phase exfoliation approach based on non-covalent interactions between graphene and 1-pyrenesulfonic acid sodium salt (Py–1SO{sub 3}), 1-pyrenemethylamine salt (Py − Me-NH{sub 2}) and Pluronic{sup ®} P-123 surfactant using only water as solvent compatible with biomolecules. The resulting graphene nanoplatelets (Gr-LPE) are characterized by a combination of analytical (microscopy and spectroscopy) techniques revealing mono- to few-layer graphene displaying that the exfoliation efficiency strongly depends upon the type of pyrene-based salts and organic surfactants. Moreover being completely water-based approach, we build robust nanoscaffolds of graphene-family nanomaterials (GFNs) namely, monolayer graphene, Gr-LPE (the one prepared with Pluronic{sup ®} P-123), graphene oxide (GO) and its reduced form (rGO) on glassy carbon electrode surface with three important metalloproteins include cytochrome c (Cyt c) [for electron transfer], myoglobin (Mb) [for oxygen storage] and horseradish peroxidase (HRP) [for catalyzing the biochemical reaction]. In order to demonstrate the nanobiocatalytical activity of these proteins, we used electrochemical interfacial direct electron transfer (DET) kinetics and attempt to determine the rate constant (k{sub ET}) using two different analytical approaches namely, linear sweep voltammetry and Laviron’s theory. We elucidated that all of the metalloproteins retain their structural integrity (secondary structure) upon forming mixtures with GFNs confirmed through optical and vibrational spectroscopy and biological activity using electrochemistry. Among the GFNs studied, Gr-LPE, GO and rGO support the efficient electrical

  7. Enahancing the Use of Coals by Gas Reburning - Sorbent Injection Volume 5 - Guideline Manual

    SciTech Connect

    1998-09-01

    The purpose of the Guideline Manual is to provide recommendations for the application of combined gas reburning-sorbent injection (GR-SI) technologies to pre-NSPS boilers. The manual includes design recommendations, performance predictions, economic projections and comparisons with competing technologies. The report also includes an assessment of boiler impacts. Two full-scale demonstrations of gas reburning-sorbent injection form the basis of the Guideline Manual. Under the U.S. Department of Energy's Clean Coal Technology Program (Round 1), a project was completed to demonstrate control of boiler emissions that comprise acid rain precursors, specifically oxides of nitrogen (NOX) and sulfur dioxide (S02). Other project sponsors were the Gas Research Institute and the Illinois State Department of Commerce and Community Affairs. The project involved demonstrating the combined use of Gas Reburning and Sorbent Injection (GR-SI) to assess the air emissions reduction potential of these technologies.. Three potential coal-fired utility boiler host sites were evaluated: Illinois Power's tangentially-fired 71 MWe (net) Hennepin Unit W, City Water Light and Power's cyclone- fired 33 MWe (gross) Lakeside Unit #7, and Central Illinois Light Company's wall-fired 117 MWe (net) Edwards Unit #1. Commercial demonstrations were completed on the Hennepin and Lakeside Units. The Edwards Unit was removed from consideration for a site demonstration due to retrofit cost considerations. Gas Reburning (GR) controls air emissions of NOX. Natural gas is introduced into the furnace hot flue gas creating a reducing reburning zone to convert NOX to diatomic nitrogen (N,). Overfire air is injected into the furnace above the reburning zone to complete the combustion of the reducing (fuel) gases created in the reburning zone. Sorbent Injection (S1) consists of the injection of dry, calcium-based sorbents into furnace hot flue gas to achieve S02 capture. At each site where the techno!o@es were to

  8. Enhancing the Use of Coals by Gas Reburning - Sorbent Injection Volume 5 - Guideline Manual

    SciTech Connect

    1998-06-01

    The purpose of the Guideline Manual is to provide recommendations for the application of combined gas reburning-sorbent injection (GR-SI) technologies to pre-NSPS boilers. The manual includes design recommendations, performance predictions, economic projections and comparisons with competing technologies. The report also includes an assessment of boiler impacts. Two full-scale demonstrations of gas reburning-sorbent injection form the basis of the Guideline Manual. Under the U.S. Department of Energy's Clean Coal Technology Program (Round 1), a project was completed to demonstrate control of boiler emissions that comprise acid rain precursors, specifically oxides of nitrogen (NOX) and sulfur dioxide (S02). Other project sponsors were the Gas Research Institute and the Illinois State Department of Commerce and Community Affairs. The project involved d,emonstrating the combined use of Gas Reburning and Sorbent Injection (GR-SI) to assess the air emissions reduction potential of these technologies.. Three potential coal-fired utility boiler host sites were evaluated: Illinois Power's tangentially-fired 71 MWe (net) Hennepin Unit #1, City Water Light and Power's cyclone- fired 33 MWe (gross) Lakeside Unit #7, and Central Illinois Light Company's wall-fired 117 MWe (net) Edwards Unit #1. Commercial demonstrations were completed on the Hennepin and Lakeside Units. The Edwards Unit was removed from consideration for a site demonstration due to retrofit cost considerations. Gas Reburning (GR) controls air emissions of NOX. Natural gas is introduced into the furnace hot flue gas creating a reducing reburning zone to convert NOX to diatomic nitrogen (N,). Overfire air is injected into the furnace above the reburning zone to complete the combustion of the reducing (fuel) gases created in the reburning zone. Sorbent Injection (S1) consists of the injection of dry, calcium-based sorbents into furnace hot flue gas to achieve S02 capture. `At each site where the technologies were

  9. Crystallization and preliminary X-ray diffraction study of phosphopantetheine adenylyltransferase from M. tuberculosis crystallizing in space group P3{sub 2}

    SciTech Connect

    Timofeev, V. I.; Chupova, L. A.; Esipov, R. S.; Kuranova, I. P.

    2015-09-15

    Crystals of M. tuberculosis phosphopantetheine adenylyltransferase were grown in microgravity by the capillary counter-diffusion method through a gel layer. The X-ray diffraction data set suitable for the determination of the three-dimensional structure at atomic resolution was collected from one crystal at the Spring-8 synchrotron facility to 2.00-Å resolution. The crystals belong to sp. gr. P3{sub 2} and have the following unit-cell parameters: a = b = 106.47 Å, c = 71.32 Å, α = γ = 90°, β = 120°. The structure was solved by the molecular-replacement method. There are six subunits of the enzyme comprising a hexamer per asymmetric unit. The hexamer is a biologically active form of phosphopantetheine adenylyltransferase from M. tuberculosis.

  10. Purification, crystallization, and preliminary X-ray diffraction study of purine nucleoside phosphorylase from E. coli

    SciTech Connect

    Abramchik, Yu. A. Timofeev, V. I. Zhukhlistova, N. E.; Muravieva, T. I.; Esipov, R. S.; Kuranova, I. P.

    2015-07-15

    Crystals of E. coli purine nucleoside phosphorylase were grown in microgravity by the capillary counter-diffusion method through a gel layer. The X-ray diffraction data set suitable for the determination of the three-dimensional structure at atomic resolution was collected from one crystal at the Spring-8 synchrotron facility to 0.99 Å resolution. The crystals belong to sp. gr. P2{sub 1} and have the following unit-cell parameters: a = 74.1 Å, b = 110.2 Å, c = 88.2 Å, α = γ = 90°, β = 111.08°. The crystal contains six subunits of the enzyme comprising a hexamer per asymmetric unit. The hexamer is the biological active form of E. coli. purine nucleoside phosphorylase.

  11. Size-tunable strain engineering in Ge nanocrystals embedded within SiO{sub 2} and Si{sub 3}N{sub 4}

    SciTech Connect

    Liao, P. H.; Hsu, T. C.; Chen, K. H.; Wang, C. C.; Li, P. W.; Cheng, T. H.; Hsu, T. M.; George, T.

    2014-10-27

    We report a unique ability to control the sign and size of the stress within Ge nanocrystals or nanodots fabricated using a complementary metal-oxide-semiconductor-compatible process within SiO{sub 2} and Si{sub 3}N{sub 4} layers. Very large (as much as 4.5%), size-dependent compressive and tensile strains can be generated depending on whether the dot is embedded within either a Si{sub 3}N{sub 4} or a SiO{sub 2} layer. Raman measurements reveal significant anharmonicity for smaller Ge dots and possible distortions of the diamond cubic lattice as evidenced by the measured Grünesien parameters and confirmed by their transmission electron diffraction patterns. Two completely different mechanisms are proposed to explain the formation of the tensile and compressive strain states, respectively.

  12. Microscopic picture of non-relativistic classicalons

    SciTech Connect

    Berkhahn, Felix; Mller, Sophia; Niedermann, Florian; Schneider, Robert E-mail: sophia.x.mueller@physik.uni-muenchen.de E-mail: robert.bob.schneider@physik.uni-muenchen.de

    2013-08-01

    A theory of a non-relativistic, complex scalar field with derivatively coupled interaction terms is investigated. This toy model is considered as a prototype of a classicalizing theory and in particular of general relativity, for which the black hole constitutes a prominent example of a classicalon. Accordingly, the theory allows for a non-trivial solution of the stationary Gross-Pitaevskii equation corresponding to a black hole in the case of GR. Quantum fluctuations on this classical background are investigated within the Bogoliubov approximation. It turns out that the perturbative approach is invalidated by a high occupation of the Bogoliubov modes. Recently, it was proposed that a black hole is a Bose-Einstein condensate of gravitons that dynamically ensures to stay at the verge of a quantum phase transition. Our result is understood as an indication for that claim. Furthermore, it motivates a non-linear numerical analysis of the model.

  13. Solvation of fluoro-acetonitrile in water by 2D-IR spectroscopy: A combined experimental-computational study

    SciTech Connect

    Cazade, Pierre-André; Das, Akshaya K.; Tran, Halina; Kläsi, Felix; Hamm, Peter; Bereau, Tristan; Meuwly, Markus

    2015-06-07

    The solvent dynamics around fluorinated acetonitrile is characterized by 2-dimensional infrared spectroscopy and atomistic simulations. The lineshape of the linear infrared spectrum is better captured by semiempirical (density functional tight binding) mixed quantum mechanical/molecular mechanics simulations, whereas force field simulations with multipolar interactions yield lineshapes that are significantly too narrow. For the solvent dynamics, a relatively slow time scale of 2 ps is found from the experiments and supported by the mixed quantum mechanical/molecular mechanics simulations. With multipolar force fields fitted to the available thermodynamical data, the time scale is considerably faster—on the 0.5 ps time scale. The simulations provide evidence for a well established CF–HOH hydrogen bond (population of 25%) which is found from the radial distribution function g(r) from both, force field and quantum mechanics/molecular mechanics simulations.

  14. Structural phase transition of ternary dielectric SmGdO{sub 3}: Evidence from angle dispersive x-ray diffraction and Raman spectroscopic studies

    SciTech Connect

    Sharma, Yogesh E-mail: satya504@gmail.com Sahoo, Satyaprakash E-mail: satya504@gmail.com Misra, Pankaj; Pavunny, Shojan P.; Katiyar, Ram S. E-mail: satya504@gmail.com; Mishra, A. K.; Dwivedi, Abhilash; Sharma, S. M.

    2015-03-07

    High-pressure synchrotron based angle dispersive x-ray diffraction (ADXRD) studies were carried out on SmGdO{sub 3} (SGO) up to 25.7 GPa at room temperature. ADXRD results indicated a reversible pressure-induced phase transition from ambient monoclinic to hexagonal phase at ∼8.9 GPa. The observed pressure-volume data were fitted with the third order Birch-Murnaghan equation of state yielding zero pressure bulk modulus B{sub 0} = 132(22) and 177(9) GPa for monoclinic (B-type) and hexagonal (A-type) phases, respectively. Pressure dependent micro-Raman spectroscopy further confirmed the monoclinic to hexagonal phase transition at about 5.24 GPa. The mode Grüneisen parameters and pressure coefficients for different Raman modes corresponding to each individual phases of SGO were calculated using pressure dependent Raman mode analysis.

  15. Phonon anharmonicity in silicon from 100 to 1500 K

    DOE PAGES [OSTI]

    Kim, D. S.; Smith, Hillary L.; Niedziela, Jennifer L.; Li, Chen W.; Abernathy, Douglas L.; Fultz, B.

    2015-01-21

    Inelastic neutron scattering was performed on silicon powder to measure the phonon density of states (DOS) from 100 to 1500 K. The mean fractional energy shifts with temperature of the modes weremore » $$\\langle$$Δεi/εiΔT$$\\rangle$$=₋0.07, giving a mean isobaric Grüneisen parameter of +6.95±0.67, which is significantly different from the isothermal parameter of +0.98. These large effects are beyond the predictions from quasiharmonic models using density functional theory or experimental data, demonstrating large effects from phonon anharmonicity. At 1500 K the anharmonicity contributes 0.15kB/atom to the vibrational entropy, compared to 0.03kB/atom from quasiharmonicity. Lastly, excellent agreement was found between the entropy from phonon DOS measurements and the reference NIST-JANAF thermodynamic entropy from calorimetric measurements.« less

  16. Phonon anharmonicity in silicon from 100 to 1500 K

    SciTech Connect

    Kim, D. S.; Smith, Hillary L.; Niedziela, Jennifer L.; Li, Chen W.; Abernathy, Douglas L.; Fultz, B.

    2015-01-21

    Inelastic neutron scattering was performed on silicon powder to measure the phonon density of states (DOS) from 100 to 1500 K. The mean fractional energy shifts with temperature of the modes were $\\langle$ΔεiiΔT$\\rangle$=₋0.07, giving a mean isobaric Grüneisen parameter of +6.95±0.67, which is significantly different from the isothermal parameter of +0.98. These large effects are beyond the predictions from quasiharmonic models using density functional theory or experimental data, demonstrating large effects from phonon anharmonicity. At 1500 K the anharmonicity contributes 0.15kB/atom to the vibrational entropy, compared to 0.03kB/atom from quasiharmonicity. Lastly, excellent agreement was found between the entropy from phonon DOS measurements and the reference NIST-JANAF thermodynamic entropy from calorimetric measurements.

  17. Definition of energy-calibrated spectra for national reachback

    SciTech Connect

    Kunz, Christopher L.; Hertz, Kristin L.

    2014-01-01

    Accurate energy calibration is critical for the timeliness and accuracy of analysis results of spectra submitted to National Reachback, particularly for the detection of threat items. Many spectra submitted for analysis include either a calibration spectrum using 137Cs or no calibration spectrum at all. The single line provided by 137Cs is insufficient to adequately calibrate nonlinear spectra. A calibration source that provides several lines that are well-spaced, from the low energy cutoff to the full energy range of the detector, is needed for a satisfactory energy calibration. This paper defines the requirements of an energy calibration for the purposes of National Reachback, outlines a method to validate whether a given spectrum meets that definition, discusses general source considerations, and provides a specific operating procedure for calibrating the GR-135.

  18. Quantization of systems with temporally varying discretization. II. Local evolution moves

    SciTech Connect

    Hhn, Philipp A.

    2014-10-15

    Several quantum gravity approaches and field theory on an evolving lattice involve a discretization changing dynamics generated by evolution moves. Local evolution moves in variational discrete systems (1) are a generalization of the Pachner evolution moves of simplicial gravity models, (2) update only a small subset of the dynamical data, (3) change the number of kinematical and physical degrees of freedom, and (4) generate a dynamical (or canonical) coarse graining or refining of the underlying discretization. To systematically explore such local moves and their implications in the quantum theory, this article suitably expands the quantum formalism for global evolution moves, constructed in Paper I [P. A. Hhn, Quantization of systems with temporally varying discretization. I. Evolving Hilbert spaces, J. Math. Phys. 55, 083508 (2014); e-print http://arxiv.org/abs/arXiv:1401.6062 [gr-qc

  19. A=10B (59AJ76)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    59AJ76) (See the Energy Level Diagram for 10B) GENERAL: See also Table 10.4 [Table of Energy Levels] (in PDF or PS). Theory: See (FR55H, KU56, FR57, GR57D, KU57A, FR58B, KU58A, WA59). 1. 6Li(α, γ)10B Qm = 4.459 Five resonances are observed in the range Eα = 0.5 to 2.6 MeV, corresponding to 10B*(4.76 - 6.06 MeV): see Table 10.5 (in PDF or PS). No other resonances appear for Eα < 3.8 MeV (10B*(6.74)) (ME57D). The 4.76-MeV state decays mainly to 10B*(0.7). The angular distribution of γ-rays

  20. A=10B (66LA04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 10B) GENERAL: See (BA59F, BR59M, TA60L, TR61, IN62, BU63D, KU63B, ME63A, MO63C, OL63B, VL63A, WA63C, AM64, BA64V, FR64D, GR64C, MA64HH, NE64C, OL64A, ST64, VA64F, FA65C, NE65). See also Table 10.6 [Table of Energy Levels] (in PDF or PS). Ground State: μ = +1.8007 nm (FU65E). Q = +0.08 b (FU65E). 1. 6Li(α, γ)10B Qm = 4.461 Six resonances are observed in the range Eα = 0.5 to 2.6 MeV, corresponding to 10B*(4.76 - 6.06 MeV): see Table 10.8 (in PDF or PS).

  1. A=10C (66LA04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 10C) GENERAL: See (TA60L, IN62, GR64C, VO64C). See also Table 10.24 [Table of Energy Levels] (in PDF or PS). Mass of 10C: From the Q-value of the 10B(p, n)10C reaction (TA61E: Q0 = -4.393 ± 0.025 MeV) and the β+ end-point energy (BA63R: Eβ+(max) = 1.865 ± 0.015 MeV), the mass excess of 10C is 15.658 ± 0.013 MeV, based on 12C ≡ 0 (MA65A). 1. 10C(β+)10B Qm = 3.606 The decay is complex. See 10B. 2. 10B(p, n)10C Qm = -4.388 The ground state threshold

  2. A=11Be (1985AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    85AJ01) (See Energy Level Diagrams for 11Be) GENERAL: See also (1980AJ01) and Table 11.3 [Table of Energy Levels] (in PDF or PS). Model calculations:(1981RA06, 1981SE06, 1983MI1E, 1984VA06). Electromagnetic transitions:(1980MI1G). Complex reactions involving 11Be:(1979BO22, 1980WI1L, 1983EN04, 1983WI1A, 1984GR08, 1984HI1A). Hypernuclei:(1979BU1C, 1982IK1A, 1982KA1D, 1982KO11, 1983FE07, 1983KO1D, 1983MI1E). Other topics:(1981SE06, 1982NG01). Ground-state properties of 11Be:(1981AV02, 1982NG01,

  3. A=12C (1980AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    0AJ01) (See Energy Level Diagrams for 12C) GENERAL: See also (1975AJ02) and Table 12.7 [Table of Energy Levels] (in PDF or PS). Shell model: (1974BO1P, 1975BI05, 1975BO27, 1975FR06, 1975GI1C, 1975MU13, 1975WA30, 1976BA24, 1977CA02, 1977CA08, 1977GR02, 1977JA14, 1978FU13, 1978MU04, 1978SV01, 1979LO1F). Collective and deformed models: (1974BO1P, 1975BO27, 1975KI21, 1975LE14, 1975MC15, 1975SO07, 1976GL1C, 1976PA25, 1977CA08, 1977TH03, 1977UE01, 1977VI03, 1979MA1J). Cluster and alpha particle

  4. A=13O (1976AJ04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    76AJ04) (See the Isobar Diagram for 13O) GENERAL: See also (1970AJ04) and Table 13.29 [Table of Energy Levels] (in PDF or PS). Theoretical papers: (1973HA49, 1973RO1R, 1973SP1A, 1975GR03, 1975BE31, 1975HU14). Review papers: (1972CE1A, 1972WA07, 1973HA77). Mass of 13O: From the Q-value of the 16O(3He, 6He)13O reaction [Q0 = -30.508 ± 0.010 MeV] the atomic mass excess of 13O is determined to be 23.105 ± 0.010 MeV (1971TR03). 13O is then bound with respect to 12N + p and 11C + 2p by 1.528 and

  5. A=15C (1986AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    6AJ01) (See Energy Level Diagrams for 15C) GENERAL: See also (1981AJ01) and Table 15.1 [Table of Energy Levels] (in PDF or PS) here. Model calculations:(1983ANZQ, 1984VA06). Electromagnetic transitions:(1980RI06). Complex reactions involving 15C:(1981GR08, 1983BE02, 1983EN04, 1983FR1A, 1983HO08, 1983MA06, 1983OL1A, 1983WI1A, 1984HI1A, 1984HO23). Pion capture and reactions:(1981OS04). Hypernuclei:(1981WA1J, 1982KA1D, 1983DO1B, 1983FE07, 1983KO1V, 1984AS1D). Other topics:(1984PO11). Ground state

  6. A=15N (1970AJ04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    0AJ04) (See Energy Level Diagrams for 15N) GENERAL: See Table 15.4 [Table of Energy Levels] (in PDF or PS) here. Model calculations: (1957HA1E, 1959BR1E, 1959FE1B, 1960TA1C, 1961BA1E, 1963BU1C, 1963KU1B, 1964MA1G, 1965CO25, 1965FA1B, 1965GR1H, 1965GU1A, 1965ZA1B, 1966EL08, 1966SO05, 1967CO32, 1967EL03, 1967PA05, 1968EL1A, 1968HO1H, 1968MA2B, 1968SH08, 1968WA04, 1968ZH05, 1969CH1R, 1969EL1B). General calculations and reviews: (1964EV1A, 1965BE1B, 1966OL1C, 1966WI1E, 1967FA1A, 1967LO03, 1968BI1C,

  7. A=16N (1977AJ02)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    7AJ02) (See Energy Level Diagrams for 16N) GENERAL: See also (1971AJ02) and Table 16.3 [Table of Energy Levels] (in PDF or PS). Model calculations: (1971AR1R, 1973RE17, 1973SI1G, 1975RA1T). Reactions involving muons: (1971GR1U, 1971LA17, 1973JO17, 1973KA30, 1973NA28, 1975FU1F, 1975PA01). Reactions involving pions: (1970AL22, 1971EI01, 1971GU13, 1971SR03, 1973CA25, 1973KA1D, 1973LA1G, 1973LA1H, 1973RE10, 1973SR02, 1974LI15, 1974SZ04, 1975RA1R, 1976TR1A). Other topics: (1971AR02, 1971SR03,

  8. A=16N (1986AJ04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    6AJ04) (See Energy Level Diagrams for 16N) GENERAL: See also (1982AJ01) and Table 16.3 [Table of Energy Levels] (in PDF or PS) here. Model calculations: (1984BA24, 1984KA1H, 1984VA06). Complex reactions involving 16N: (1981ME13, 1981OL1C, 1983EN04, 1983FR1A, 1983MA06, 1983OL1A, 1983PL1A, 1983SA06, 1983WI1A, 1984GR08, 1984HI1A, 1984HO23, 1984KA1H, 1985BE40, 1985PO11, 1986HA1P). Reactions involving muons nad neutrinos (See also reaction 14.): (1981GM02, 1981TO16, 1983EG03, 1983JA10, 1984JA06,

  9. A=16O (1959AJ76)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    59AJ76) (See the Energy Level Diagram for 16O) GENERAL: See also Table 16.3 [Table of Energy Levels] (in PDF or PS). Theory: See (DE54C, FL54A, HE55F, JA55A, MA55F, MA55O, SC55A, WI55F, EL56, FE56B, JA56C, KA56A, MO56, PE56A, RE56B, WI56C, EL57B, FE57D, GR57C, HE57B, RE57, TA57A, TO57A, CA58C, DA58A, DA58D, FE58A, FE58B, HA58B, MO58, RA58F, UM58, WI58G). 1. 12C(α, γ)16O Qm = 7.148 Resonant capture radiation to 16Og.s. is observed at Eα ~ 3.24 MeV, corresponding to the known J = 1- state at

  10. A=17F (1986AJ04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    6AJ04) (See Energy Level Diagrams for 17F) GENERAL: See (1982AJ01) and Table 17.17 [Table of Energy Levels] (in PDF or PS). Nuclear models: (1982ZH01, 1983BR29, 1984ZI04, 1985ME06). Special states: (1981WI1K, 1983AU1B, 1983BR29, 1983WI15, 1984ANZV, 1985ME06, 1985SH24). Electromagnetic transitions: (1982BR24, 1983BR29, 1983TO08, 1984SAZW, 1985AL21). Astrophysical questions: (1981WA1Q, 1981WE1F, 1982WI1B). Complex reactions involving 17F: (1984GR08, 1984HI1A, 1984HO23). Pion reactions: (1980CR03).

  11. A=17Ne (1982AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    82AJ01) (See the Isobar Diagram for 17Ne) GENERAL: See (1977AJ02) and Table 17.22 [Table of Energy Levels] (in PDF or PS). Theory and reviews:(1975BE56, 1977CE05, 1978GU10, 1978WO1E, 1979BE1H). Other topics:(1981GR08). Mass of 17Ne: The mass excess adopted by (1977WA08) is 16.478 ± 0.026 MeV, based on unpublished data. We retain the mass excess 16.48 ± 0.05 MeV based on the evidence reviewed in (1977AJ02). 1. (a) 17Ne(β+)17F* → 16O + p Qm = 13.93 (b) 17Ne(β+)17F Qm = 14.53 The half-life of

  12. A=18F (1959AJ76)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    59AJ76) (See Energy Level Diagram for 18F) GENERAL: See also Table 18.4 [Table of Energy Levels] (in PDF or PS). Theory: See (RE54C, EL55, EL55A, NE56D, GR57D, WA59). 1. 18F(β+)18O Qm = 1.677 The positron end point is 635 ± 15 (BL49A), 649 ± 9 keV (RU51). The spectrum is simple (see (DR56A)). The half-life is 112 ± 1 min (BL49A), 111 ± 1 min (JA55), 110 ± 1 min (BE58G): log ft = 3.62. The fact that the β transition to the ground state of 18O is allowed indicates J = 1+ for 18F (assumed T

  13. A=19O (1987AJ02)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    7AJ02) (See Energy Level Diagrams for 19O) GENERAL: See (1983AJ01) and Table 19.1 [Table of Energy Levels] (in PDF or PS). Nuclear models: (1978WI1B, 1983BR29, 1983PO02, 1983SH44, 1984BA24, 1984CH1V, 1984RA13, 1986WA1R). Special states: (1978WI1B, 1983BR29, 1983HU1J, 1983PO02, 1983SH44, 1984BA24, 1984CH1V, 1984RA13, 1984WI17, 1985LE1L, 1986AN07). Electromagnetic transitions: (1983BR29, 1985LE1L). Complex reactions involving 19O: (1983FR1A, 1983WI1A, 1984GR08, 1984HI1A, 1984HO23, 1985PO11,

  14. A=20F (1983AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    3AJ01) (See Energy Level Diagrams for 20F) GENERAL: See also (1978AJ03) and Table 20.3 [Table of Energy Levels] (in PDF or PS). Shell model: (1978MA2H, 1981EL1D, 1982KI02). Electromagnetic transitions: (1976MC1G). Special states: (1978MA2H, 1981EL1D, 1982KI02). Complex reactions involving 20F: (1978SH18, 1982FR03). Astrophysical questions: (1978WO1E). Muon and pion capture and reactions: (1979KN1G, 1980TR1A). Other topics: (1977GR16, 1978MA2H, 1978RA1J, 1979BE1H, 1981EL1D, 1982KI02, 1982QUZY).

  15. A=20F (1987AJ02)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    7AJ02) (See Energy Level Diagrams for 20F) GENERAL: See (1983AJ01) and Table 20.2 [Table of Energy Levels] (in PDF or PS). Model calculations:(1978WI1B, 1982HA43, 1983BR29, 1984FO16, 1984RA13, 1986CA27, 1986COZZ, 1986VO05, 1986WA1R, 1987HA08, 1987IA1B). Complex reactions involving 20F:(1983BE02, 1983DE26, 1983WI1A, 1984GR08, 1984HO23, 1984KO25, 1985BE40, 1985HA1N, 1985PO11, 1986GA1I, 1986HA1B, 1986ME06, 1986PO06, 1987RI03, 1987RO10). Hypernuclei:(1984AS1D). Other topics:(1978WI1B, 1983AR1J,

  16. A=5Li (66LA04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 5Li) GENERAL: See Table 5.4 [Table of Energy Levels] (in PDF or PS). See also (BA59N, MI59B, PE60C, PH60A, VA61K, DI62B, IN62, KU63I, BA64HH, GR64C, SA64G, ST64). 1. 3He(d, γ)5Li Qm = 16.388 The excitation curve measured from Ed = 0.2 to 2.85 MeV shows a broad maximum at Ed = 0.45 ± 0.04 MeV (Eγ = 16.6 ± 0.2 MeV, σ = 50 ± 10 μb, Γγ = 11 ± 2 eV). Above this maximum, non-resonant capture is indicated by a slow rise of the cross section. The

  17. A=6He (66LA04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 6He) GENERAL: See (PH60A, TA60L, AH61, BA61N, IN62, IN62B, BO63B, MO63C, VL63A, GR64C, WA64F, BO65B, LO65A). See also Table 6.1 [Table of Energy Levels] (in PDF or PS). Ground state: J = 0 (CO58H). 1. 6He(β-)6Li Qm = 3.510 The decay proceeds to the ground state of 6Li(1+) and is a super-allowed Gamow-Teller transition. Recently reported end points are: Eβ = 3.50 ± 0.05 (WU52), 3.50 ± 0.02 (SC56I), 3.508 ± 0.015 (VI63), 3.508 ± 0.004 MeV (JO63). The

  18. A=7H (2002TI10)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    2002TI10) (Not illustrated) 7H has not been observed. Attempts have been made to detect it in the spontaneous fission of 252Cf (1982AL33) and in the 7Li(π-, π+) reaction [see (1984AJ01)]. A study of 9Be(π-, 2p) (1987GO25) found no evidence for 7H. See also the review of (1989OG1B) and the 7Li(π-, π+) investigation reported in (1989GR06). The ground state is calculated to have Jπ = 1/2+ and to be unstable with respect to 1n, 2n, 3n and 4n emission. Excited states are predicted at 4.84, 5.00

  19. A=8B (1984AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    4AJ01) (See Energy Level Diagrams for 8B) GENERAL: See also (1979AJ01) and Table 8.11 [Table of Energy Levels] (in PDF or PS). Special states: (1980OK01). Complex reactions involving 8B (The reactions 6Li(6Li, 4H)8B, 12C(6Li, 10Be)8B, 9Be(7Li, 8He)8B and 12C(7Li, 11Be)8B have been studied at E(6Li) = 72 MeV and E(7Li) = 83 MeV (1982AL08): see 8He, 10Be, as well as 11Be in (1985AJ01).): (1979BO22, 1980GR10, 1981MO20). Astrophysical questions: (1981BA17, 1983LI01). Reactions involving pions: (

  20. A=8B (66LA04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    8B (66LA04) (See Energy Level Diagrams for 8B) GENERAL: See (FO58D, TA60L, IN62, NA63E, BA64I, BA64GG, GR64C, ST64). See also Table 8.18 [Table of Energy Levels] (in PDF or PS). 1. 8B(β+)8Be Qm = 17.979 The beta decay leads mainly to 8Be*(2.9). Reported half lives are listed in Table 8.19 (in PDF or PS); taking τ1/2 = 0.774 sec and Q = 17.979 - 2.90, ft = 4.41 x 105 (BA65K). There is also observed a branch to a 8Be state at ~ 16.6 MeV; log ft = 2.9 (MA64D). See also (BA64GG) and 8Be. 2.

  1. A=8Be (1984AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    4AJ01) (See Energy Level Diagrams for 8Be) GENERAL: See also (1979AJ01) and Table 8.4 [Table of Energy Levels] (in PDF or PS). Shell model: (1978RA1B, 1979EL04, 1981BO1Y, 1981RA06, 1981ST22, 1982FI13). Collective, rotational and deformed models: (1978CA1D, 1979EL04, 1979MA1J, 1980FI09, 1981RA06, 1981ST22, 1982FI13). Cluster and α-particle models: (1977WU1A, 1979GO24, 1979GR1F, 1979PA22, 1979ZH1C, 1980FU1G, 1980HA1M, 1980IK1B, 1981GA1J, 1981KA1P, 1981KN12, 1981KR1J, 1981ST22, 1982HA1M, 1982TS1A,

  2. A=8Li (1988AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    8AJ01) (See Energy Level Diagrams for 8Li) GENERAL: See also (1984AJ01) and Table 8.2 [Table of Energy Levels] (in PDF or PS) here. Nuclear models: (1983KU17, 1983SH38, 1984MO1H, 1984REZZ, 1984VA06, 1988WO04). Special states: (1982PO12, 1983KU17, 1984REZZ, 1984VA06, 1986XU02). Electromagnetic transitions: (1983KU17). Astrophysics: (1987MA2C). Complex reactions involving 8Li: (1983FR1A, 1983GU1A, 1983OL1A, 1983WI1A, 1984GR08, 1984HI1A, 1984LA27, 1985JA1B, 1985MA02, 1985MA13, 1985MO17, 1986AV1B,

  3. A=9C (66LA04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    66LA04) (See the Isobar Diagram for 9C) GENERAL: See (55AJ61, SW56A, GR64C, WI64E, JA65C, WO65). Mass of 9C: The atomic mass excess of 9C is 28.99 ± 0.07 MeV: see 12C(3He, 6He)9C (CE65). 1. 9C(β+)9B → 8Be + p Qm = 16.76 Two groups of delayed protons are observed, indicating a component of the β+ decay to a level of 9B at 12.05 ± 0.2 MeV with Γ = 800 ± 100 keV which then decays to p + 8Be(0) and 8Be*(2.9). The half-life is 127 ± 3 msec. The allowed character of the decay suggests Jπ =

  4. A=9Li (1988AJ01)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    8AJ01) (See Energy Level Diagrams for 9Li) GENERAL: See also (1984AJ01) and Table 9.1 [Table of Energy Levels] (in PDF or PS). Model calculations: (1983KU17, 1984CH24, 1984VA06). Special states: (1983KU17, 1984VA06). Electromagnetic interactions: (1983KU17). Astrophysical questions: (1987MA2C). Complex reactions involving 9Li: (1983OL1A, 1983WI1A, 1984GR08, 1985JA1B, 1985MA02, 1985MO17, 1986CS1A, 1986HA1B, 1986SA30, 1986WE1C, 1987BA38, 1987CH26, 1987JA06, 1987KO1Z, 1987SH1K, 1987TAZU, 1987WA09,

  5. A=9Li (66LA04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 9Li) GENERAL: See (GR64C). See also Table 9.1 [Table of Energy Levels] (in PDF or PS). Mass of 9Li: From the Q-value for 7Li(t, p)9Li: Q = -2.397 ± 0.020 MeV, the mass excess of 9Li is 24.965 ± 0.020 MeV (MI64E, MA65A). 1. 9Li(β-)9Be Qm = 13.615 9Li decays to the ground state (25 ± 15 %) and to the 2.43 MeV, neutron-unstable state of 9Be (75 ± 15 %). The β-endpoints are 13.5 ± 0.3 MeV and 11.0 ± 0.4 MeV; log ft = 5.5 ± 0.2 and 4.7 ± 0.2,

  6. Symmetry restored in dibosons at the LHC?

    DOE PAGES [OSTI]

    Brehmer, Johann; Hewett, JoAnne; Kopp, Joachim; Rizzo, Thomas; Tattersall, Jamie

    2015-10-28

    A number of LHC resonance search channels display an excess in the invariant mass region of 1.8–2.0 TeV. Among them is a 3.4σ excess in the fully hadronic decay of a pair of Standard Model electroweak gauge bosons, in addition to potential signals in the HW and dijet final states. We perform a model-independent cross-section fit to the results of all ATLAS and CMS searches sensitive to these final states. We then interpret these results in the context of the Left-Right Symmetric Model, based on the extended gauge group SU(2)L × SU(2)R × U(1)', and show that a heavy right-handedmore » gauge boson WR can naturally explain the current measurements with just a single coupling gR ~ 0.4. Thus, we discuss a possible connection to dark matter.« less

  7. Advanced steel reheat furnace

    SciTech Connect

    Moyeda, D.; Sheldon, M.; Koppang, R.; Lanyi, M.; Li, X.; Eleazer, B.

    1997-10-01

    Energy and Environmental Research Corp. (EER) under a contract from the Department of Energy is pursuing the development and demonstration of an Advanced Steel Reheating Furnace. This paper reports the results of Phase 1, Research, which has evaluated an advanced furnace concept incorporating two proven and commercialized technologies previously applied to other high temperature combustion applications: EER`s gas reburn technology (GR) for post combustion NOx control; and Air Product`s oxy-fuel enrichment air (OEA) for improved flame heat transfer in the heating zones of the furnace. The combined technologies feature greater production throughput with associated furnace efficiency improvements; lowered NOx emissions; and better control over the furnace atmosphere, whether oxidizing or reducing, leading to better control over surface finish.

  8. Cosmology of bigravity with doubly coupled matter

    SciTech Connect

    Comelli, D.; Crisostomi, M.; Koyama, K.; Pilo, L.; Tasinato, G.

    2015-04-20

    We study cosmology in the bigravity formulation of the dRGT model where matter couples to both metrics. At linear order in perturbation theory two mass scales emerge: an hard one from the dRGT potential, and an environmental dependent one from the coupling of bigravity with matter. At early time, the dynamics is dictated by the second mass scale which is of order of the Hubble scale. The set of gauge invariant perturbations that couples to matter follow closely the same behaviour as in GR. The remaining perturbations show no issue in the scalar sector, while problems arise in the tensor and vector sectors. During radiation domination, a tensor mode grows power-like at super-horizon scales. More dangerously, the only propagating vector mode features an exponential instability on sub-horizon scales. We discuss the consequences of such instabilities and speculate on possible ways to deal with them.

  9. Turbulent natural and mixed convection along a vertical plate

    SciTech Connect

    Abu-Mulaweh, H.I.; Armaly, B.F.; Chen, T.S.; Zhao, J.Z.

    1997-07-01

    Measurements of turbulent boundary-layer air flow in natural and mixed convection adjacent to an isothermal vertical flat plate are reported. Laser-Doppler velocimeter and cold wire anemometer were used, respectively, to measure simultaneously the mean turbulent velocity and temperature distributions were measured for a temperature difference, {Delta}T, of 30 C between the heated wall and the free stream air at a fixed location x = 3 m (with a corresponding Grashof number Gr{sub x} = 8.55 x 10{sup 10}), and for a range of free stream velocities 0 m/s {le} U{sub {infinity} } {le} 0.41 m/s. The effect of small free stream velocity on the turbulent natural convection is examined. These results reveal that the introduction of small free stream velocity on turbulent natural convection flow suppresses turbulence and decreases the heat transfer rate from the heated wall.

  10. Synthesis, characterization, and crystal structure of 2-amino-7-methyl-5-oxo-4-phenyl-4,5-dihydropyrano[3,2-c] pyran-3-carbonitrile

    SciTech Connect

    Sharma, S.; Banerjee, B.; Brahmachari, G.; Kant, Rajni; Gupta, V. K.

    2015-12-15

    2-Amino-7-methyl-5-oxo-4-phenyl-4,5-dihydropyrano[3,2-c] pyran-3-carbonitrile, C{sub 16}H{sub 12}N{sub 2}O{sub 3} is synthesized via one-pot multi-component reaction at room temperature using commercially available urea as inexpensive and environmentally benign organo-catalyst. Its structure is determined by single-crystal X-ray diffraction technique The crystals are monoclinic, a = 10.7357(12), b = 8.7774(8), c = 15.0759(16) Å, β = 103.575(11)°, Z = 4, sp. gr. P2{sub 1}/n, R = 0.0551 for 1696 observed reflections. The crystal structure is stabilized by N–H···N, C–H···O, and C–H···π interactions.

  11. Java XMGR

    SciTech Connect

    Dr. George L. Mesina; Steven P. Miller

    2004-08-01

    The XMGR5 graphing package [1] for drawing RELAP5 [2] plots is being re-written in Java [3]. Java is a robust programming language that is available at no cost for most computer platforms from Sun Microsystems, Inc. XMGR5 is an extension of an XY plotting tool called ACE/gr extended to plot data from several US Nuclear Regulatory Commission (NRC) applications. It is also the most popular graphing package worldwide for making RELAP5 plots. In Section 1, a short review of XMGR5 is given, followed by a brief overview of Java. In Section 2, shortcomings of both tkXMGR [4] and XMGR5 are discussed and the value of converting to Java is given. Details of the conversion to Java are given in Section 3. The progress to date, some conclusions and future work are given in Section 4. Some screen shots of the Java version are shown.

  12. L'Aventure du LHC

    ScienceCinema

    None

    2016-07-12

    Cette présentation s’adressera principalement aux personnes qui ont construit le LHC. La construction du LHC fut longue et difficile. De nombreux problèmes sont apparus en cours de route. Tous ont été résolus grâce au dévouement et à l’engagement du personnel et des collaborateurs. Je reviendrai sur les coups durs et les réussites qui ont marqués ces 15 dernières années et je vous montrerai combien cette machine, le fruit de vos efforts, est extraordinaire.

  13. Fort Bliss Geothermal Area Data: Temperature profile, logs, schematic model and cross section

    SciTech Connect

    Adam Brandt

    2015-11-15

    This dataset contains a variety of data about the Fort Bliss geothermal area, part of the southern portion of the Tularosa Basin, New Mexico. The dataset contains schematic models for the McGregor Geothermal System, a shallow temperature survey of the Fort Bliss geothermal area. The dataset also contains Century OH logs, a full temperature profile, and complete logs from well RMI 56-5, including resistivity and porosity data, drill logs with drill rate, depth, lithology, mineralogy, fractures, temperature, pit total, gases, and descriptions among other measurements as well as CDL, CNL, DIL, GR Caliper and Temperature files. A shallow (2 meter depth) temperature survey of the Fort Bliss geothermal area with 63 data points is also included. Two cross sections through the Fort Bliss area, also included, show well position and depth. The surface map included shows faults and well spatial distribution. Inferred and observed fault distributions from gravity surveys around the Fort Bliss geothermal area.

  14. Spin(1)spin(2) effects in the motion of inspiralling compact binaries at third order in the post-Newtonian expansion

    SciTech Connect

    Porto, Rafael A.; Rothstein, Ira Z.

    2008-08-15

    We use effective field theory techniques to compute the potentials due to spin-spin and spin-orbit effects, from which the O(S{sub 1}S{sub 2}) contribution to the motion of spinning compact binaries to third Post-Newtonian (PN) order follow. We use a formalism which allows us to impose the spin supplementary condition (SSC) in a canonical framework to all orders in the PN expansion. We explicitly show the equivalence with our previous results, obtained using the Newton-Wigner SSC at the level of the action for spin-spin and spin-orbit potentials reported in arXiv:gr-qc/0604099 and arXiv:0712.2032 , respectively.

  15. F-1

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    E B R U A R Y 2 0 1 2 Executive Office of the President President's Council of Advisors on Science and Technology R E P OR T T O T H E PR E SI DEN T ENGAGE TO E XCEL: PRODUCI NG ONE M ILLION A DDI T IONA L COLLEGE GR A DUAT ES W I T H DEGR EES I N SCIENCE , T ECH NOLOGY, ENGI NEER I NG, A N D M AT HEM AT ICS F E B R U A R Y 2 0 1 2 Executive Office of the President President's Council of Advisors on Science and Technology R E P OR T T O T H E PR E SI DEN T ENGAGE TO E XCEL: PRODUCI NG ONE M

  16. F E B R U A R

    Office of Energy Efficiency and Renewable Energy (EERE) (indexed site)

    E B R U A R Y 2 0 1 2 Executive Office of the President President's Council of Advisors on Science and Technology R E P OR T T O T H E PR E SI DEN T ENGAGE TO E XCEL: PRODUCI NG ONE M ILLION A DDI T IONA L COLLEGE GR A DUAT ES W I T H DEGR EES I N SCIENCE , T ECH NOLOGY, ENGI NEER I NG, A N D M AT HEM AT ICS F E B R U A R Y 2 0 1 2 Executive Office of the President President's Council of Advisors on Science and Technology R E P OR T T O T H E PR E SI DEN T ENGAGE TO E XCEL: PRODUCI NG ONE M

  17. Crystal structure of 1-methyl-3-([2,2-dimethyl-4,6-dioxo-1,3-dioxane-5-ylidene]methyl)urea

    SciTech Connect

    Habibi, A. Ghorbani, H. S.; Bruno, G.; Rudbari, H. A.; Valizadeh, Y.

    2013-12-15

    The crystal structure of 1-Methyl-3-([2,2-dimethyl-4,6-dioxo-1,3-dioxane-5-ylidene]methyl)urea (C{sub 9}H{sub 12}N{sub 2}O{sub 5}) has been determined by single crystal X-ray diffraction analysis. The crystals are monoclinic, a = 5.3179(2), b = 18.6394(6), c =10.8124(3) , ? = 100.015(2), Z = 4, sp. gr. P2{sub 1}/c, R = 0.0381 for 2537 reflections with I > 2?(I). Except for C(CH{sub 3}){sub 2} group, the molecule is planar. The structure is stabilized by inter- and intramolecular N-H...O hydrogen bonds and weak C-H...O interactions.

  18. Inflationary scenarios in Starobinsky model with higher order corrections

    SciTech Connect

    Artymowski, Michał; Lalak, Zygmunt; Lewicki, Marek

    2015-06-17

    We consider the Starobinsky inflation with a set of higher order corrections parametrised by two real coefficients λ{sub 1} ,λ{sub 2}. In the Einstein frame we have found a potential with the Starobinsky plateau, steep slope and possibly with an additional minimum, local maximum or a saddle point. We have identified three types of inflationary behaviour that may be generated in this model: i) inflation on the plateau, ii) at the local maximum (topological inflation), iii) at the saddle point. We have found limits on parameters λ{sub i} and initial conditions at the Planck scale which enable successful inflation and disable eternal inflation at the plateau. We have checked that the local minimum away from the GR vacuum is stable and that the field cannot leave it neither via quantum tunnelling nor via thermal corrections.

  19. Effect of initial temperature and concentration of catalyst in polyeugenol production

    SciTech Connect

    Widayat

    2015-12-29

    Objective of this research to study influencing of sulfuric acid concentration and initials temperature on polymerization of eugenol. Eugenol is the largest compound in the clove oil that used as raw material. Eugenol was polymerized laboratory scale. Polymerization processing conducted in reactor at 30 minutes. Polyeugenol was obtained in polymerization was conducted at temperature 40°C and ratio eugenol to sulfuric acid 1:15 mole. This research was pbtained the highest yield 81.49%. However, the weight would be increase in according with increasing of initial temperature. The polymerization in temperature 50°C with 1:1.5 mole ratio has the heaviest molecule weight; 47,530.76 gr/mole.

  20. X-ray diffraction, spectroscopic and DFT studies of 1-(4-bromophenyl)-3,5-diphenylformazan

    SciTech Connect

    Tezcan, H.; Tokay, N.; Alpaslan, G.; Erdnmez, A.

    2013-12-15

    The crystal structure of 1-(4-bromophenyl)-3,5-diphenylformazan was determined by X-ray single crystal diffraction technique. The crystals are orthorhombic, a = 23.0788(9), b = 7.9606(3), c = 18.6340(12) , Z = 8, sp. gr. Pbca, R{sub 1} = 0.074. The structure was also examined using the density-functional theory. Its structure stability, and frontier molecular orbital components were discussed and the results were compared with X-ray and spectral results. The maximum absorbtion peaks of the UV-vis spectrum of the compound have been calculated using the time-dependent density-functional theory. It was found a good agreement between the calculated and experimental maximum absorption wavelength.

  1. 13N

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    N β+-Decay Evaluated Data Measurements 1950HO01: 13N. 1953CH34: 13N. 1954GR66: 13N. 1955WI43: 13N. 1957DA08: 13N. 1957DE22: 13N. 1957NO17: 13N. 1958AR15: 13N. 1958DA09: 13N. 1960JA12: 13N; measured not abstracted; deduced nuclear properties. 1960KI02: 13N; measured not abstracted; deduced nuclear properties. 1965BO42: 13N; measured T1/2. 1965EB01: 13N; measured T1/2. 1968RI15: 13N; measured not abstracted; deduced nuclear properties. 1971GO40: 13N. 1973SIYS: 13N; measured T1/2. 1977AZ01: 13N;

  2. 16C

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    C β--Decay Evaluated Data Measurements 1961HI01: 16C; measured not abstracted; deduced nuclear properties. 1976AL02: 16C; measured Eγ, Iγ, γ(t), T1/2, delayed neutrons log ft. 16N deduced levels. 1976FI03: 16C; measured T1/2, delayed γ, delayed neutrons. 1983GA03: 16C(β-), (β-n); measured β(t), γ(t), βγ-coin; deduced log ft. 16N levels deduced β-branching ratio. 2000BU33, 2001GR06: 16C(β-n); measured β-delayed neutron spectra. 16N deduced level, J, π. Comparison with shell model

  3. 16F

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    F Ground-State Decay Evaluated Data Measured Ground-State Γcm for 16F Adopted value: 40 ± 20 keV (1993TI07) Measured Mass Excess for 16F Adopted value: 10680 ± 8 keV (2003AU02) Measurements 1965GR15: 16O(p, n)16F, E = 30.50 MeV; measured σ(En). 16F deduced levels. 1968AD03: 14N(3He, n), E = 3 MeV; measured Q, σ(En). 16F deduced levels. 1971ADZZ: 14N(3He, n), E = 1.73 - 3.6 MeV; measured σ(E; En, θ), Q. 16F deduced levels, mass excess. 1971MO34: 16O(p, n), E = 23 MeV; measured En. 16F

  4. 16N

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    β--Decay Evaluated Data Measurements 1959EL41: 16N; measured T1/2. 1962MA38: 16N; measured not abstracted; deduced nuclear properties. 1964BI02: 16N; measured not abstracted; deduced nuclear properties. 1965GR21: 16N; measured T1/2. 1966SC05: 16N; measured T1/2. 1969HA42: 16N; measured Eα, Iα; deduced Iβ, log ft. 16O levels deduced α-width. 1970AL21: 16N; measured T1/2. 1970JO25: 16N; measured β-delayed α-spectrum. 16O level deduced no parity-forbidden α-decay. 1974NE10: 16N; measured

  5. Reverse Monte Carlo simulation of Se{sub 80}Te{sub 20} and Se{sub 80}Te{sub 15}Sb{sub 5} glasses

    SciTech Connect

    Abdel-Baset, A. M.; Rashad, M.; Moharram, A. H.

    2013-12-16

    Two-dimensional Monte Carlo of the total pair distribution functions g(r) is determined for Se{sub 80}Te{sub 20} and Se{sub 80}Te{sub 15}Sb{sub 5} alloys, and then it used to assemble the three-dimensional atomic configurations using the reverse Monte Carlo simulation. The partial pair distribution functions g{sub ij}(r) indicate that the basic structure unit in the Se{sub 80}Te{sub 15}Sb{sub 5} glass is di-antimony tri-selenide units connected together through Se-Se and Se-Te chain. The structure of Se{sub 80}Te{sub 20} alloys is a chain of Se-Te and Se-Se in addition to some rings of Se atoms.

  6. Synthesis and structures of new uranyl malonate complexes with carbamide derivatives

    SciTech Connect

    Serezhkina, L. B.; Grigor’ev, M. S.; Medvedkov, Ya. A.; Serezhkin, V. N.

    2015-09-15

    Crystals of new malonate-containing uranyl complexes [UO{sub 2}(C{sub 3}H{sub 2}O{sub 4})(Imon)(H{sub 2}O)] (I) and [UO{sub 2}(C{sub 3}H{sub 2}O4)(Meur){sub 3}] (II), where Imon is imidazolidin-2-one (ethylenecarbamide) and Meur is methyl-carbamide, have been synthesized and studied by X-ray diffraction. Both compounds crystallize in the monoclinic system with the following unit-cell parameters (at 100 K): a = 11.1147(10) Å, b = 6.9900(6) Å, c = 14.4934(12) Å, β = 92.042(2)°, V = 1125.30(17) Å{sup 3}, sp. gr. P2{sub 1}/n, Z = 4, R{sub 1} = 0.0398 (I); a = 16.6613(5) Å, b = 9.5635(3) Å, c = 22.9773(6) Å, β = 103.669(2)°, V = 3557.51(18) Å{sup 3}, sp. gr. C2/c, Z = 8, R{sub 1} = 0.0207 (II). The crystals are composed of electroneutral chains [UO{sub 2}(C{sub 3}H{sub 2}O{sub 4})(Imon)(H{sub 2}O)] and mononuclear groups [UO{sub 2}(C{sub 3}H{sub 2}O{sub 4})(Meur){sub 3}] as the structural units belonging to the crystal-chemical groups AT{sup 11}M{sub 2}{sup 1} and AB{sup 01}M{sub 3}{sup 1} (A =UO{sub 2}{sup 2+}, T{sup 11} and B{sup 01} = C{sub 3}H{sub 2}, M{sup 1} = Imon, H{sub 2}O, or Meur), respectively, of uranyl complexes. The packing modes of the uranyl-containing complexes were analyzed by the method of molecular Voronoi—Dirichlet polyhedra.

  7. Anisotropic lattice thermal expansion of PbFeBO{sub 4}: A study by X-ray and neutron diffraction, Raman spectroscopy and DFT calculations

    SciTech Connect

    Murshed, M. Mangir; Mendive, Cecilia B.; Curti, Mariano; Nénert, Gwilherm; Kalita, Patricia E.; Lipinska, Kris; Cornelius, Andrew L.; Huq, Ashfia; Gesing, Thorsten M.

    2014-11-15

    Highlights: • Mullite-type PbFeBO{sub 4} shows uni-axial negative coefficient of thermal expansion. • Anisotropic thermal expansion of the metric parameters was modeled using modified Grüneisen approximation. • The model includes harmonic, quasi-harmonic and intrinsic anharmonic contributions to the internal energy. • DFT calculation, temperature- and pressure-dependent Raman spectra help understand the phonon decay and associated anharmonicity. - Abstract: The lattice thermal expansion of mullite-type PbFeBO{sub 4} is presented in this study. The thermal expansion coefficients of the metric parameters were obtained from composite data collected from temperature-dependent neutron and X-ray powder diffraction between 10 K and 700 K. The volume thermal expansion was modeled using extended Grüneisen first-order approximation to the zero-pressure equation of state. The additive frame of the model includes harmonic, quasi-harmonic and intrinsic anharmonic potentials to describe the change of the internal energy as a function of temperature. The unit-cell volume at zero-pressure and 0 K was optimized during the DFT simulations. Harmonic frequencies of the optical Raman modes at the Γ-point of the Brillouin zone at 0 K were also calculated by DFT, which help to assign and crosscheck the experimental frequencies. The low-temperature Raman spectra showed significant anomaly in the antiferromagnetic regions, leading to softening or hardening of some phonons. Selected modes were analyzed using a modified Klemens model. The shift of the frequencies and the broadening of the line-widths helped to understand the anharmonic vibrational behaviors of the PbO{sub 4}, FeO{sub 6} and BO{sub 3} polyhedra as a function of temperature.

  8. Increased reserves through horizontal drilling in a mature waterflood, Long Beach unit, Wilmington Oil Field, California

    SciTech Connect

    Berman, B.H.

    1996-12-31

    Ranger Zone development started in 1965. A waterflood was initiated from the start using a staggered line-drive pattern. Infill drilling in the early 1980s and again in the 1990s revealed bypassed oil in the upper Ranger Fo sand. Detailed studies of the aerial extent of the remaining oil resulted in drilling 17 horizontal wells to recover these reserves. The Fo target sand thickness is 20 to 50 feet. Well courses are between 10 and 15 feet below the top of the Fo with lengths varying from 800 to 1,000 feet. The success of the Fo drilling program has prompted expansion of horizontal drilling into thin-bedded sand units. Well lengths have increased to between 1,500 and 1,800 feet with structural trend used to advantage. Where needed, probes are designed to penetrate the target sand before setting intermediate casing. The drilling program has been extended into bilateral horizontal completions. Geosteering with MWD/GR and a 2 MHz dual propagation resistivity tool is used to the casing point. In the completion interval, only the MWD/GR tool is used and a drillpipe conveyed E-log is run afterward to confirm expected resistivities. Despite the many well penetrations in the Ranger Zone, structural control is only fair. Accuracy of MWD data is generally low and geosteering is done by TVD log correlation. With a recovery factor of over 30 percent in Ranger West, from approximately 800 wells drilled in the last 30 years, the horizontal drilling program targeting bypassed reserves has brought new life to this mature reservoir.

  9. Increased reserves through horizontal drilling in a mature waterflood, Long Beach unit, Wilmington Oil Field, California

    SciTech Connect

    Berman, B.H. )

    1996-01-01

    Ranger Zone development started in 1965. A waterflood was initiated from the start using a staggered line-drive pattern. Infill drilling in the early 1980s and again in the 1990s revealed bypassed oil in the upper Ranger Fo sand. Detailed studies of the aerial extent of the remaining oil resulted in drilling 17 horizontal wells to recover these reserves. The Fo target sand thickness is 20 to 50 feet. Well courses are between 10 and 15 feet below the top of the Fo with lengths varying from 800 to 1,000 feet. The success of the Fo drilling program has prompted expansion of horizontal drilling into thin-bedded sand units. Well lengths have increased to between 1,500 and 1,800 feet with structural trend used to advantage. Where needed, probes are designed to penetrate the target sand before setting intermediate casing. The drilling program has been extended into bilateral horizontal completions. Geosteering with MWD/GR and a 2 MHz dual propagation resistivity tool is used to the casing point. In the completion interval, only the MWD/GR tool is used and a drillpipe conveyed E-log is run afterward to confirm expected resistivities. Despite the many well penetrations in the Ranger Zone, structural control is only fair. Accuracy of MWD data is generally low and geosteering is done by TVD log correlation. With a recovery factor of over 30 percent in Ranger West, from approximately 800 wells drilled in the last 30 years, the horizontal drilling program targeting bypassed reserves has brought new life to this mature reservoir.

  10. Chronic nandrolone administration promotes oxidative stress, induction of pro-inflammatory cytokine and TNF-α mediated apoptosis in the kidneys of CD1 treated mice

    SciTech Connect

    Riezzo, Irene; Turillazzi, Emanuela; Bello, Stefania; Cantatore, Santina; Cerretani, Daniela; Di Paolo, Marco; Fiaschi, Anna Ida; Frati, Paola; Neri, Margherita; Pedretti, Monica; Fineschi, Vittorio

    2014-10-01

    Nandrolone decanoate administration and strenuous exercise increase the extent of renal damage in response to renal toxic injury. We studied the role played by oxidative stress in the apoptotic response caused by nandrolone decanoate in the kidneys of strength-trained male CD1 mice. To measure cytosolic enzyme activity, glutathione peroxidase (GPx), glutathione reductase (GR) and malondialdehyde (MDA) were determined after nandrolone treatment. An immunohistochemical study and Western blot analysis were performed to evaluate cell apoptosis and to measure the effects of renal expression of inflammatory mediators (IL-1β, TNF-α) on the induction of apoptosis (HSP90, TUNEL). Dose-related oxidative damage in the kidneys of treated mice is shown by an increase in MDA levels and by a reduction of antioxidant enzyme GR and GPx activities, resulting in the kidney's reduced radical scavenging ability. Renal specimens of the treated group showed relevant glomeruli alterations and increased immunostaining and protein expressions, which manifested significant focal segmental glomerulosclerosis. The induction of proinflammatory cytokine expression levels was confirmed by Western blot analysis. Long-term administration of nandrolone promotes oxidative injury in the mouse kidneys. TNF-α mediated injury due to nandrolone in renal cells appears to play a role in the activation of both the intrinsic and extrinsic apoptosis pathways. - Highlights: • We analyze abuse of nandrolone decanoate in strength-trained male CD1 mice. • Nandrolone decanoate administration increases oxidative stress. • Increased cytokine expressions were observed. • Renal apoptosis was described. • Long-term administration of nandrolone promotes oxidative injury in mice kidney.

  11. PROBING SHOCK BREAKOUT AND PROGENITORS OF STRIPPED-ENVELOPE SUPERNOVAE THROUGH THEIR EARLY RADIO EMISSIONS

    SciTech Connect

    Maeda, Keiichi

    2013-01-01

    We study properties of early radio emission from stripped-envelope supernovae (SNe; those of Type IIb/Ib/Ic). We suggest there is a sub-class of stripped-envelope SNe based on their radio properties, including the optically well-studied Type Ic SNe (SNe Ic) 2002ap and 2007gr, showing a rapid rise to a radio peak within {approx}10 days and reaching a low luminosity (at least an order of magnitude fainter than a majority of SNe IIb/Ib/Ic). They show a decline after the peak that is shallower than that of other stripped-envelope SNe while their spectral index is similar. We show that all these properties are naturally explained if the circumstellar material (CSM) density is low and therefore the forward shock is expanding into the CSM without deceleration. Since the forward shock velocity in this situation, as estimated from the radio properties, still records the maximum velocity of the SN ejecta following the shock breakout, observing these SNe in radio wavelengths provides new diagnostics on the nature of both the breakout and the progenitor which otherwise require a quite rapid follow-up in other wavelengths. The inferred post-shock breakout velocities of SNe Ic 2002ap and 2007gr are sub-relativistic, {approx}0.3c. These are higher than that inferred for SN II 1987A, in line with suggested compact progenitors. However, these are lower than expected for a Wolf-Rayet (W-R) progenitor. It may reflect an as yet unresolved nature of the progenitors just before the explosion, and we suggest that the W-R progenitor envelopes might have been inflated which could quickly reduce the maximum ejecta velocity from the initial shock breakout velocity.

  12. Epitaxial growth of AlN films via plasma-assisted atomic layer epitaxy

    SciTech Connect

    Nepal, N.; Qadri, S. B.; Hite, J. K.; Mahadik, N. A.; Mastro, M. A.; Eddy, C. R. Jr.

    2013-08-19

    Thin AlN layers were grown at 200650 C by plasma assisted atomic layer epitaxy (PA-ALE) simultaneously on Si(111), sapphire (1120), and GaN/sapphire substrates. The AlN growth on Si(111) is self-limited for trimethyaluminum (TMA) pulse of length > 0.04 s, using a 10 s purge. However, the AlN nucleation on GaN/sapphire is non-uniform and has a bimodal island size distribution for TMA pulse of ?0.03 s. The growth rate (GR) remains almost constant for T{sub g} between 300 and 400 C indicating ALE mode at those temperatures. The GR is increased by 20% at T{sub g} = 500 C. Spectroscopic ellipsometry (SE) measurement shows that the ALE AlN layers grown at T{sub g} ? 400 C have no clear band edge related features, however, the theoretically estimated band gap of 6.2 eV was measured for AlN grown at T{sub g} ? 500 C. X-ray diffraction measurements on 37 nm thick AlN films grown at optimized growth conditions (T{sub g} = 500 C, 10 s purge, 0.06 s TMA pulse) reveal that the ALE AlN on GaN/sapphire is (0002) oriented with rocking curve full width at the half maximum (FWHM) of 670 arc sec. Epitaxial growth of crystalline AlN layers by PA-ALE at low temperatures broadens application of the material in the technologies that require large area conformal growth at low temperatures with thickness control at the atomic scale.

  13. Synthesis and structure of R{sub 2}[UO{sub 2}(NO{sub 3}){sub 2}(NCS){sub 2}] (R = Rb or Cs)

    SciTech Connect

    Serezhkin, V. N.; Peresypkina, E. V.; Grigor’eva, V. A.; Virovets, A. V.; Serezhkina, L. B.

    2015-01-15

    Crystals Rb{sub 2}[UO{sub 2}(NO{sub 3}){sub 2}(NCS){sub 2}] (I) and Cs{sub 2}[UO{sub 2}(NO{sub 3}){sub 2}(NCS){sub 2}] (II) have been synthesized and studied by IR spectroscopy and X-ray diffraction. Crystals I are monoclinic, with the following parameters: a = 12.2118(5) Å, b = 10.2545(3) Å, c = 11.8754(4) Å, β = 110.287(1)°, sp. gr. C2/c, Z = 4, and R = 0.0523. Crystals II are orthorhombic, with a = 13.7309(3) Å, b = 10.5749(2) Å, c = 10.1891(2) Å, sp. gr. Pnma, Z = 4, and R = 0.0411. The basic structural units of crystals I and II are one-core complexes [UO{sub 2}(NO{sub 3}){sub 2}(NCS){sub 2}]{sup 2−}, which belong to the crystallochemical group cis-AB{sub 2}{sup 01}M{sub 2}{sup 1} (A = UO{sub 2}{sup 2+}, B{sup 01} = NO{sub 3}{sup −}, M{sup 1} = NCS{sup −}), which are combined into a framework via electrostatic interactions with ions of alkaline metals R (R = Rb or Cs). The structural features of crystals I and II, which condition the formation of [UO{sub 2}(NO{sub 3}){sub 2}(NCS){sub 2}]{sup 2−} complexes with a cis rather than a trans position of isothiocyanate ions in the coordination sphere of uranyl ions, are discussed.

  14. Dark matter relic density in Gauss-Bonnet braneworld cosmology

    SciTech Connect

    Meehan, Michael T.; Whittingham, Ian B., E-mail: Michael.Meehan@my.jcu.edu.au, E-mail: Ian.Whittingham@jcu.edu.au [College of Science, Technology and Engineering, James Cook University, 1 James Cook Dr., Townsville 4811 (Australia)

    2014-12-01

    The relic density of symmetric and asymmetric dark matter in a Gauss-Bonnet (GB) modified Randall-Sundrum (RS) type II braneworld cosmology is investigated. The existing study of symmetric dark matter in a GB braneworld (Okada and Okada, 2009) found that the expansion rate was reduced compared to that in standard General Relativity (GR), thereby delaying particle freeze-out and resulting in relic abundances which are suppressed by up to O(10{sup ?2}). This is in direct contrast to the behaviour observed in RS braneworlds where the expansion rate is enhanced and the final relic abundance boosted. However, this finding that relic abundances are suppressed in a GB braneworld is based upon a highly contrived situation in which the GB era evolves directly into a standard GR era, rather than passing through a RS era as is the general situation. This collapse of the RS era requires equating the mass scale m{sub ?} of the GB modification and the mass scale m{sub ?} of the brane tension. However, if the GB contribution is to be considered as the lowest order correction from string theory to the RS action, we would expect m{sub ?} > m{sub ?}. We investigate the effect upon the relic abundance of choosing more realistic values for the ratio R{sub m} ? m{sub ?}/m{sub ?} and find that the relic abundance can be either enhanced or suppressed by more than two orders of magnitude. However, suppression only occurs for a small range of parameter choices and, overwhelmingly, the predominant situation is that of enhancement as we recover the usual Randall-Sundrum type behaviour in the limit R{sub m} >> 1. We use the latest observational bound ?{sub DM}h{sup 2}=0.11870.0017 to constrain the various model parameters and briefly discuss the implications for direct/indirect dark matter detection experiments as well as dark matter particle models.

  15. ELM PARTICLE AND ENERGY TRANSPORT IN THE SOL AND DIVERTOR OF DIII-D

    SciTech Connect

    FENSTERMACHER,ME; LEONARD,AW; SNYDER,PB; BOEDO,JA; COLCHIN,RJ; GROEBNER,RJ; GRAY,DS; GROTH,M; HOLLMANN,E; LASNIER,CJ; OSBORNE,TH; PETRIE,TW; RUDAKOV,DL; TAKAHASHI,H; WATKINS,JG; ZENG,L

    2003-04-01

    A271 ELM PARTICLE AND ENERGY TRANSPORT IN THE SOL AND DIVERTOR OF DIII-D. Results from a series of dedicated experiments measuring the effect of particle and energy pulses from Type-I Edge Localized Modes (ELMs) in the DIII-D scrape-off layer (SOL) and divertor are compared with a simple model of ELM propagation in the boundary plasma. The simple model asserts that the propagation of ELM particle and energy perturbations is dominated by ion parallel convection along SOL fields lines and the recovery from the ELM perturbation is determined by recycling physics. Time scales associated with the initial changes of boundary plasma parameters are expected to be on the order of the ion transit time from the outer midplane, where the ELM instability is initiated, to the divertor targets. To test the model, the ion convection velocity is changed in the experiment by varying the plasma density. At moderate to high density, n{sub e}/n{sub Gr} = 0.5-0.8, the delays in the response of the boundary plasma to the midplane ELM pulses, the density dependence of those delays and other observations are consistent with the model. However, at the lowest densities, n{sub e}/n{sub Gr} {approx} 0.35, small delays between the response sin the two divertors, and changes in the response of the pedestal thermal energy to ELM events, indicate that additional factors including electron conduction in the SOL, the pre-ELM condition of the divertor plasma, and the ratio of ELM instability duration to SOL transit time, may be playing a role. The results show that understanding the response of the SOL and divertor plasmas to ELMs, for various pre-ELM conditions, is just as important to predicting the effect of ELM pulses on the target surfaces of future devices as is predicting the characteristics of the ELM perturbation of the core plasma.

  16. Albany/FELIX: A parallel, scalable and robust, finite element, first-order Stokes approximation ice sheet solver built for advanced analysis

    SciTech Connect

    Tezaur, I. K.; Perego, M.; Salinger, A. G.; Tuminaro, R. S.; Price, S. F.

    2015-04-27

    This paper describes a new parallel, scalable and robust finite element based solver for the first-order Stokes momentum balance equations for ice flow. The solver, known as Albany/FELIX, is constructed using the component-based approach to building application codes, in which mature, modular libraries developed as a part of the Trilinos project are combined using abstract interfaces and template-based generic programming, resulting in a final code with access to dozens of algorithmic and advanced analysis capabilities. Following an overview of the relevant partial differential equations and boundary conditions, the numerical methods chosen to discretize the ice flow equations are described, along with their implementation. The results of several verification studies of the model accuracy are presented using (1) new test cases for simplified two-dimensional (2-D) versions of the governing equations derived using the method of manufactured solutions, and (2) canonical ice sheet modeling benchmarks. Model accuracy and convergence with respect to mesh resolution are then studied on problems involving a realistic Greenland ice sheet geometry discretized using hexahedral and tetrahedral meshes. Also explored as a part of this study is the effect of vertical mesh resolution on the solution accuracy and solver performance. The robustness and scalability of our solver on these problems is demonstrated. Lastly, we show that good scalability can be achieved by preconditioning the iterative linear solver using a new algebraic multilevel preconditioner, constructed based on the idea of semi-coarsening.

  17. A Scalable and Extensible Earth System Model for Climate Change Science

    SciTech Connect

    Gent, Peter; Lamarque, Jean-Francois; Conley, Andrew; Vertenstein, Mariana; Craig, Anthony

    2013-02-13

    The objective of this award was to build a scalable and extensible Earth System Model that can be used to study climate change science. That objective has been achieved with the public release of the Community Earth System Model, version 1 (CESM1). In particular, the development of the CESM1 atmospheric chemistry component was substantially funded by this award, as was the development of the significantly improved coupler component. The CESM1 allows new climate change science in areas such as future air quality in very large cities, the effects of recovery of the southern hemisphere ozone hole, and effects of runoff from ice melt in the Greenland and Antarctic ice sheets. Results from a whole series of future climate projections using the CESM1 are also freely available via the web from the CMIP5 archive at the Lawrence Livermore National Laboratory. Many research papers using these results have now been published, and will form part of the 5th Assessment Report of the United Nations Intergovernmental Panel on Climate Change, which is to be published late in 2013.

  18. High-altitude chemical-release systems for Project BIME (Brazilian Ionospheric Modification Experiments) Project IMS (Ionospheric Modification Studies) Project PIIE (Polar Ionospheric Irregularities Experiment) Project Polar Arcs. Final report, 30 September 1981-30 June 1987

    SciTech Connect

    Stokes, C.S.; Murphy, W.J.

    1987-07-31

    Project BIME, a Spread-F observation program involved the launching of two Nike-Black Brant rockets each containing a payload containing Ammonium Nitrate Fuel Oil (ANFO). The rockets were launched from Barriera Do Inferno Launch Site in Natal, Brazil in August of 1982. Project IMS, an F-layer modification experiment involved three launch vehicles. A Nike-Tomahawk and two Sonda III rockets. The Nike-Tomahawk carried a sulfur hexafluoride (SF/sub 6/) payload. One of the Sonda III rockets carried a payload that consisted of an SF/sub 6/ canister and a samarium/strontium thermite canister. The remaining Sonda III carried a payload that consisted of a trifluorobromo methane (CF/sub 3/Br) canister and a samarium thermite canister. The rockets were launched from Wallops Island Launch Facility, Virginia in November of 1984. Project PIIE and Polar Arcs, a program to investigate polar ionospheric irregularities, involved the launch of a Nike-Black Brant rocket which housed one samarium thermite canister and six barium canisters. An attempted launch of the payload was returned in March of 1985, however, launch criteria could not be met and the payload was returned to FRC for storage and refurbishment for launch in 1987. The rocket was launched successfully from Sondrestrom Air Base, Greenland in March of 1987.

  19. Non-stationary Return Levels of CMIP5 Multi-model Temperature Extremes

    SciTech Connect

    Cheng, L.; Phillips, T. J.; AghaKouchak, A.

    2015-05-01

    The objective of this study is to evaluate to what extent the CMIP5 climate model simulations of the climate of the twentieth century can represent observed warm monthly temperature extremes under a changing environment. The biases and spatial patterns of 2-, 10-, 25-, 50- and 100-year return levels of the annual maxima of monthly mean temperature (hereafter, annual temperature maxima) from CMIP5 simulations are compared with those of Climatic Research Unit (CRU) observational data considered under a non-stationary assumption. The results show that CMIP5 climate models collectively underestimate the mean annual maxima over arid and semi-arid regions that are most subject to severe heat waves and droughts. Furthermore, the results indicate that most climate models tend to underestimate the historical annual temperature maxima over the United States and Greenland, while generally disagreeing in their simulations over cold regions. Return level analysis shows that with respect to the spatial patterns of the annual temperature maxima, there are good agreements between the CRU observations and most CMIP5 simulations. However, the magnitudes of the simulated annual temperature maxima differ substantially across individual models. Discrepancies are generally larger over higher latitudes and cold regions.

  20. Abrupt Climate Change and the Atlantic Meridional Overturning Circulation: sensitivity and non-linear response to Arctic/sub-Arctic freshwater pulses. Collaborative research. Final report

    SciTech Connect

    Hill, Christopher

    2015-06-15

    This project investigated possible mechanisms by which melt-water pulses can induce abrupt change in the Atlantic Meridional Overturning Circulation (AMOC) magnitude. AMOC magnitude is an important ingredient in present day climate. Previous studies have hypothesized abrupt reduction in AMOC magnitude in response to influxes of glacial melt water into the North Atlantic. Notable fresh-water influxes are associated with the terminus of the last ice age. During this period large volumes of melt water accumulated behind retreating ice sheets and subsequently drained rapidly when the ice weakened sufficiently. Rapid draining of glacial lakes into the North Atlantic is a possible origin of a number of paleo-record abrupt climate shifts. These include the Younger-Dryas cooling event and the 8,200 year cooling event. The studies undertaken focused on whether the mechanistic sequence by which glacial melt-water impacts AMOC, which then impacts Northern Hemisphere global mean surface temperature, is dynamically plausible. The work has implications for better understanding past climate stability. The work also has relevance for today’s environment, in which high-latitude ice melting in Greenland appears to be driving fresh water outflows at an accelerating pace.

  1. From Thule to Huli`s: Use of Magnetotellurics in difficult acquisition areas

    SciTech Connect

    Christopherson, K.R.

    1996-12-31

    Recent applications of Magnetotellurics have produced results superior to those of earlier years by many improvements in the technology, the application and, the interpretation of the method. MT continues to be useful in those areas where seismic acquisition is either difficult or expensive, where the surface inhibits effective seismic penetration, or where the use of MT is cost-effective as a predecessor to seismic. Improvements made to MT within the last few years include: multi-site acquisition with varied station spacings and omni-directional, low frequency antennae; smaller, higher storage field computers, sensor-box modifications for filtering unwanted signal (such as lightning); post-acquisition re-processing of the data via robust schemes; and faster, larger 2-D and 3-D modeling capabilities. Within the last two years, MT has been used world-wide for a variety of exploration targets. These include the continued use of MT for mapping subcarbonate plays in Papua New Guinea with on-going drilling. Here, use of seismic is precluded due to thick, high-velocity surface limestone. MT has been used as a precursor to seismic in overthrust regimes in Nevada and Colorado where MT is used to highgrade areas as prospects before seismic programs are acquired. In Greenland, MT has been used for reconnaissance mapping in large basin environments sub-basalt. On-going system modifications are being made to provide larger channel systems and future marine acquisition of MT.

  2. From Thule to Huli's: Use of Magnetotellurics in difficult acquisition areas

    SciTech Connect

    Christopherson, K.R. )

    1996-01-01

    Recent applications of Magnetotellurics have produced results superior to those of earlier years by many improvements in the technology, the application and, the interpretation of the method. MT continues to be useful in those areas where seismic acquisition is either difficult or expensive, where the surface inhibits effective seismic penetration, or where the use of MT is cost-effective as a predecessor to seismic. Improvements made to MT within the last few years include: multi-site acquisition with varied station spacings and omni-directional, low frequency antennae; smaller, higher storage field computers, sensor-box modifications for filtering unwanted signal (such as lightning); post-acquisition re-processing of the data via robust schemes; and faster, larger 2-D and 3-D modeling capabilities. Within the last two years, MT has been used world-wide for a variety of exploration targets. These include the continued use of MT for mapping subcarbonate plays in Papua New Guinea with on-going drilling. Here, use of seismic is precluded due to thick, high-velocity surface limestone. MT has been used as a precursor to seismic in overthrust regimes in Nevada and Colorado where MT is used to highgrade areas as prospects before seismic programs are acquired. In Greenland, MT has been used for reconnaissance mapping in large basin environments sub-basalt. On-going system modifications are being made to provide larger channel systems and future marine acquisition of MT.

  3. A subtropical fate awaited freshwater discharged from glacial Lake Agassiz

    SciTech Connect

    Condron, Alan; Winsor, Peter

    2011-02-01

    The 8.2 kyr event is the largest abrupt climatic change recorded in the last 10,000 years, and is widely hypothesized to have been triggered by the release of thousands of kilometers cubed of freshwater into the North Atlantic Ocean. Using a high-resolution (1/6) global, ocean-ice circulation model we present an alternative view that freshwater discharged from glacial Lake Agassiz would have remained on the continental shelf as a narrow, buoyant, coastal current, and would have been transported south into the subtropical North Atlantic. The pathway we describe is in contrast to the conceptual idea that freshwater from this lake outburst spread over most of the sub-polar North Atlantic, and covered the deep, open-ocean, convection regions. This coastally confined freshwater pathway is consistent with the present-day routing of freshwater from Hudson Bay, as well as paleoceanographic evidence of this event. Using a coarse-resolution (2.6) version of the same model, we demonstrate that the previously reported spreading of freshwater across the sub-polar North Atlantic results from the inability of numerical models of this resolution to accurately resolve narrow coastal flows, producing instead a diffuse circulation that advects freshwater away from the boundaries. To understand the climatic impact of freshwater released in the past or future (e.g. Greenland and Antarctica), the ocean needs to be modeled at a resolution sufficient to resolve the dynamics of narrow, coastal buoyant flows.

  4. Black carbon contribution to global warming

    SciTech Connect

    Chylek, P.; Johnson, B.; Kou, L.; Wong, J.

    1996-12-31

    Before the onset of industrial revolution the only important source of black carbon in the atmosphere was biomass burning. Today, black carbon production is divided between the biomass and fossil fuel burning. Black carbon is a major agent responsible for absorption of solar radiation by atmospheric aerosols. Thus black carbon makes other aerosols less efficient in their role of reflecting solar radiation and cooling the earth-atmosphere system. Black carbon also contributes to the absorption of solar radiation by clouds and snow cover. The authors present the results of black carbon concentrations measurements in the atmosphere, in cloud water, in rain and snow melt water collected during the 1992--1996 time period over the southern Nova Scotia. Their results are put into the global and historical perspective by comparing them with the compilation of past measurements at diverse locations and with their measurements of black carbon concentrations in the Greenland and Antarctic ice cores. Black carbon contribution to the global warming is estimated, and compared to the carbon dioxide warming, using the radiative forcing caused by the black carbon at the top of the atmosphere.

  5. The Characterization of Psychrophilic Microorganisms and their potentially useful Cold-Active Glycosidases Final Progress Report

    SciTech Connect

    Brenchly, Jean E.

    2008-06-30

    Our studies of novel, cold-loving microorganisms have focused on two distinct extreme environments. The first is an ice core sample from a 120,000 year old Greenland glacier. The results of this study are particularly exciting and have been highlighted with press releases and additional coverage. The first press release in 2004 was based on our presentation at the General Meeting of the American Society for Microbiology and was augmented by coverage of our publication (Appl. Environ. Microbiol. 2005. Vol. 71:7806) in the Current Topics section of the ASM news journal, “Microbe.” Of special interest for this report was the isolation of numerous, phylogenetically distinct and potentially novel ultrasmall microorganisms. The detection and isolation of members of the ultrasmall population is significant because these cells pass through 0.2 micron pore filters that are generally used to trap microorganisms from environmental samples. Thus, analyses by other investigators that examined only cells captured on the filters would have missed a significant portion of this population. Only a few ultrasmall isolates had been obtained prior to our examination of the ice core samples. Our development of a filtration enrichment and subsequent cultivation of these organisms has added extensively to the collection of, and knowledge about, this important population in the microbial world.

  6. Comparison of optically measured and radar-derived horizontal neutral winds. Master's thesis

    SciTech Connect

    Christie, M.S.

    1990-01-01

    Nighttime thermospheric winds for Sondrestrom, Greenland from 11 nights between 1983 and 1988, have been compared to learn about the O(+)-O collision cross section and the high-latitude atomic oxygen density. The horizontal winds in the magnetic meridian were derived indirectly from incoherent-scatter radar (ISR) measurements on ion velocities antiparallel to the magnetic field and directly from Fabry-Perot interferometer (FPI) measurements of Doppler shifts of the (6300-A) emission of atomic oxygen. In deriving the radar winds, the O(+)-O collision cross section, was scaled by a factor of f what was varied from 0.5 to 5.1. On the basis of several arguments the altitude of the 6300-A emission was assumed to be 230 km. The best agreement between the ISR and FPI winds was obtained when f was increased substantially, to between 1.7 and 3.4. If the average peak emission altitude were higher, these factors would be larger; if it were lower, they would be somewhat smaller. However, if the average altitude were substantially lower it would have been more difficult to have obtained agreement between the two techniques.

  7. How much of the world’s land has been urbanized, really? A hierarchical framework for evading confusion

    SciTech Connect

    Liu, zhifeng; He, Chunyang; Zhou, Yuyu; Wu, jianguo

    2014-05-01

    Urbanization has transformed the world’s landscapes, resulting in a series of ecological and environmental problems. To assess urbanization impacts and improve sustainability, one of the first questions that we must address is: how much of the world’s land has been urbanized? Unfortunately, the estimates of the global urban land reported in the literature vary widely from less than 1% to 3% primarily because different definitions of urban land were used. To evade confusion, here we propose a hierarchical framework for representing and communicating the spatial extent of the world’s urbanized land at the global, regional, and more local levels. The hierarchical framework consists of three spatially nested definitions: “urban area” that is delineated by administrative boundaries, “built-up area” that is dominated by artificial surfaces, and “impervious surface area” that is devoid of life. These are really three different measures of urbanization. In 2010, the global urban land was close to 3%, the global built-up area was 0.65%, and the global impervious surface area was 0.45%, of the word’s total land area (excluding Antarctica and Greenland). We argue that this hierarchy of urban land measures, in particular the ratios between them, can also facilitate better understanding the biophysical and socioeconomic processes and impacts of urbanization.

  8. Albany/FELIX: A parallel, scalable and robust, finite element, first-order Stokes approximation ice sheet solver built for advanced analysis

    DOE PAGES [OSTI]

    Tezaur, I. K.; Perego, M.; Salinger, A. G.; Tuminaro, R. S.; Price, S. F.

    2015-04-27

    This paper describes a new parallel, scalable and robust finite element based solver for the first-order Stokes momentum balance equations for ice flow. The solver, known as Albany/FELIX, is constructed using the component-based approach to building application codes, in which mature, modular libraries developed as a part of the Trilinos project are combined using abstract interfaces and template-based generic programming, resulting in a final code with access to dozens of algorithmic and advanced analysis capabilities. Following an overview of the relevant partial differential equations and boundary conditions, the numerical methods chosen to discretize the ice flow equations are described, alongmore » with their implementation. The results of several verification studies of the model accuracy are presented using (1) new test cases for simplified two-dimensional (2-D) versions of the governing equations derived using the method of manufactured solutions, and (2) canonical ice sheet modeling benchmarks. Model accuracy and convergence with respect to mesh resolution are then studied on problems involving a realistic Greenland ice sheet geometry discretized using hexahedral and tetrahedral meshes. Also explored as a part of this study is the effect of vertical mesh resolution on the solution accuracy and solver performance. The robustness and scalability of our solver on these problems is demonstrated. Lastly, we show that good scalability can be achieved by preconditioning the iterative linear solver using a new algebraic multilevel preconditioner, constructed based on the idea of semi-coarsening.« less

  9. The microbial fate of carbon in high-latitude seas: Impact of the microbial loop on oceanic uptake of CO{sub 2}

    SciTech Connect

    Yager, P.L.

    1996-12-31

    This dissertation examines pelagic microbial processes in high-latitude seas, how they affect regional and global carbon cycling, and how they might respond to hypothesized changes in climate. Critical to these interests is the effect of cold temperature on bacterial activity. Also important is the extent to which marine biological processes in general impact the inorganic carbon cycle. The study area is the Northeast Water (NEW) Polynya, a seasonally-recurrent opening in the permanent ice situated over the northeastern Greenland continental shelf. This work was part of an international, multi-disciplinary research project studying carbon cycling in the coastal Arctic. The first chapter describes a simple model which links a complex marine food web to a simplified ocean and atmosphere. The second chapter investigates the inorganic carbon inventory of the summertime NEW Polynya surface waters to establish the effect of biological processes on the air-sea pCO{sub 2} gradient. The third and fourth chapters use a kinetic approach to examine microbial activities in the NEW Polynya as a function of temperature and dissolved organic substrate concentration, testing the so-called Pomeroy hypothesis that microbial activity is disproportionately reduced at low environmental temperatures owing to increased organic substrate requirements. Together, the suite of data collected on microbial activities, cell size, and grazing pressure suggest how unique survival strategies adopted by an active population of high-latitude bacteria may contribute to, rather than detract from, an efficient biological carbon pump.

  10. On the origin of Laurentia

    SciTech Connect

    Dalziel, I.W.D. . Inst. for Geophysics)

    1992-01-01

    Laurentia, the Precambrian core of the North American continent, is surrounded by late Precambrian rift systems and therefore constitutes a suspect terrane''. A geometric and geological fit can be achieved between the Atlantic margin of Laurentia and the Pacific margin of the Gondwana craton. The enigmatic Arequipa massif along the southern Peruvian coast, that yields ca. 2.0 Ga radiometric ages, is juxtaposed with the Makkovik-Ketilidian province of the same age range in Labrador and southern Greenland. The Greenville belt continues beneath the ensialic Andes of the present day to join up with the 1.3--1.0 Ga San Ignacio and Sonsas-Aguapei orogens of the Transamazonian craton. Together with the recent identification of possible continuations of the Greenville orogen in East Antarctica and of the Taconic Appalachians in southern South America, the fit supports suggestions that Laurentia originated between East Antarctica-Australia and embryonic South America prior to the opening of the Pacific Ocean basin and amalgamation of the Gondwana Cordilleran and Appalachian margins, this implies that there may have been two supercontinents during the Neoproterozoic, before and after opening of the Pacific Ocean. As Laurentia and Gondwana appear to have collided on at least two occasions during the Paleozoic, this scenario therefore calls to question the existence of so-called supercontinental cycles. The Arica bight of the present day may reflect a primary reentrant in the South American continental margin that controlled subduction processes along the Andean margin and eventually led to uplift of the Altiplano.

  11. Iridium geochemistry of volcanic ash layers from the early Eocene rifting of the northeastern North Atlantic and some other Phanerozoic events

    SciTech Connect

    Schmitz, B.; Asaro, F. |

    1996-04-01

    This study shows that some types of explosive volcanism can result in significant Ir anomalies (up to 750 ppt); however, these are readily discerned from impact-related, extraterrestrial Ir amomalies by other chemical and mineralogical criteria. Iridium and major and trace elements were analyzed in 34 of the >180 volcanic ash layers in the Fur Formation of early Eocene age in Denmark. These ashes originate from explosive volcanism during rifting of the Greenland-Eurasia continent and subsequent sea-floor spreading in the young northeastern North Atlantic. In addition, 15 older Phanerozoic ashes, associated with other dramatic global events, have been analyzed for Ir. The Fur Formation ashes are unusually well preserved and have a wide compositional range - for example, rhyolitic, dacitic, tholeiitic and alkaline basaltic, mafic alkaline, and different salic alkaline ashes, and ashes with intermediate or unknown magma origin. Iridium shows a bimodal distribution, where all types of salic (alkaline as well as subalkaline) ashes have very low Ir concentrations (<50 ppt), similar to values for average continental crust, whereas all types of basaltic ashes show higher concentrations, generally in the range 70-450 ppt. A strongly alkaline, mafic (nephelinitic) ash holds 102{+-}29 ppt Ir. 97 refs., 5 figs., 8 tabs.

  12. Non-stationary Return Levels of CMIP5 Multi-model Temperature Extremes

    DOE PAGES [OSTI]

    Cheng, L.; Phillips, T. J.; AghaKouchak, A.

    2015-05-01

    The objective of this study is to evaluate to what extent the CMIP5 climate model simulations of the climate of the twentieth century can represent observed warm monthly temperature extremes under a changing environment. The biases and spatial patterns of 2-, 10-, 25-, 50- and 100-year return levels of the annual maxima of monthly mean temperature (hereafter, annual temperature maxima) from CMIP5 simulations are compared with those of Climatic Research Unit (CRU) observational data considered under a non-stationary assumption. The results show that CMIP5 climate models collectively underestimate the mean annual maxima over arid and semi-arid regions that are mostmore » subject to severe heat waves and droughts. Furthermore, the results indicate that most climate models tend to underestimate the historical annual temperature maxima over the United States and Greenland, while generally disagreeing in their simulations over cold regions. Return level analysis shows that with respect to the spatial patterns of the annual temperature maxima, there are good agreements between the CRU observations and most CMIP5 simulations. However, the magnitudes of the simulated annual temperature maxima differ substantially across individual models. Discrepancies are generally larger over higher latitudes and cold regions.« less

  13. Xyce Parallel Electronic Simulator - Users' Guide Version 2.1.

    SciTech Connect

    Hutchinson, Scott A; Hoekstra, Robert J.; Russo, Thomas V.; Rankin, Eric; Pawlowski, Roger P.; Fixel, Deborah A; Schiek, Richard; Bogdan, Carolyn W.; Shirley, David N.; Campbell, Phillip M.; Keiter, Eric R.

    2005-06-01

    meet the unique needs of the laboratory.4 XyceTMUsers' GuideAcknowledgementsThe authors would like to acknowledge the entire Sandia National Laboratories HPEMS(High Performance Electrical Modeling and Simulation) team, including Steve Wix, CarolynBogdan, Regina Schells, Ken Marx, Steve Brandon and Bill Ballard, for their support onthis project. We also appreciate very much the work of Jim Emery, Becky Arnold and MikeWilliamson for the help in reviewing this document.Lastly, a very special thanks to Hue Lai for typesetting this document with LATEX.TrademarksThe information herein is subject to change without notice.Copyrightc 2002-2003 Sandia Corporation. All rights reserved.XyceTMElectronic Simulator andXyceTMtrademarks of Sandia Corporation.Orcad, Orcad Capture, PSpice and Probe are registered trademarks of Cadence DesignSystems, Inc.Silicon Graphics, the Silicon Graphics logo and IRIX are registered trademarks of SiliconGraphics, Inc.Microsoft, Windows and Windows 2000 are registered trademark of Microsoft Corporation.Solaris and UltraSPARC are registered trademarks of Sun Microsystems Corporation.Medici, DaVinci and Taurus are registered trademarks of Synopsys Corporation.HP and Alpha are registered trademarks of Hewlett-Packard company.Amtec and TecPlot are trademarks of Amtec Engineering, Inc.Xyce's expression library is based on that inside Spice 3F5 developed by the EECS De-partment at the University of California.All other trademarks are property of their respective owners.ContactsBug Reportshttp://tvrusso.sandia.gov/bugzillaEmailxyce-support%40sandia.govWorld Wide Webhttp://www.cs.sandia.gov/xyce5 XyceTMUsers' GuideThis page is left intentionally blank6

  14. Xyce Parallel Electronic Simulator Users Guide Version 6.4

    SciTech Connect

    Keiter, Eric R.; Mei, Ting; Russo, Thomas V.; Schiek, Richard; Sholander, Peter E.; Thornquist, Heidi K.; Verley, Jason; Baur, David Gregory

    2015-12-01

    registered trademarks of Cadence Design Systems, Inc. Microsoft, Windows and Windows 7 are registered trademarks of Microsoft Corporation. Medici, DaVinci and Taurus are registered trademarks of Synopsys Corporation. Amtec and TecPlot are trademarks of Amtec Engineering, Inc. Xyce 's expression library is based on that inside Spice 3F5 developed by the EECS Department at the University of California. The EKV3 MOSFET model was developed by the EKV Team of the Electronics Laboratory-TUC of the Technical University of Crete. All other trademarks are property of their respective owners. Contacts Bug Reports (Sandia only) http://joseki.sandia.gov/bugzilla http://charleston.sandia.gov/bugzilla World Wide Web http://xyce.sandia.gov http://charleston.sandia.gov/xyce (Sandia only) Email xyce@sandia.gov (outside Sandia) xyce-sandia@sandia.gov (Sandia only)

  15. A subtropical fate awaited freshwater discharged from glacial Lake Agassiz

    DOE PAGES [OSTI]

    Condron, Alan; Winsor, Peter

    2011-02-10

    The 8.2 kyr event is the largest abrupt climatic change recorded in the last 10,000 years, and is widely hypothesized to have been triggered by the release of thousands of kilometers cubed of freshwater into the North Atlantic Ocean. Using a high-resolution (1/6°) global, ocean-ice circulation model we present an alternative view that freshwater discharged from glacial Lake Agassiz would have remained on the continental shelf as a narrow, buoyant, coastal current, and would have been transported south into the subtropical North Atlantic. The pathway we describe is in contrast to the conceptual idea that freshwater from this lake outburstmore » spread over most of the sub-polar North Atlantic, and covered the deep, open-ocean, convection regions. This coastally confined freshwater pathway is consistent with the present-day routing of freshwater from Hudson Bay, as well as paleoceanographic evidence of this event. In this study, using a coarse-resolution (2.6°) version of the same model, we demonstrate that the previously reported spreading of freshwater across the sub-polar North Atlantic results from the inability of numerical models of this resolution to accurately resolve narrow coastal flows, producing instead a diffuse circulation that advects freshwater away from the boundaries. To understand the climatic impact of freshwater released in the past or future (e.g. Greenland and Antarctica), the ocean needs to be modeled at a resolution sufficient to resolve the dynamics of narrow, coastal buoyant flows.« less

  16. Collaborative research on the Northeast Water Polynya: NEWP92 hydrographic data report. USCGC Polar Sea cruise, July 15--August 15, 1992

    SciTech Connect

    Wallace, D.W.R.; Behrens, W.J.; Hopkins, T.S.; Kinder, C.; Deming, J.; Smith, W.O.; Top, Z.; Walsh, I.D.

    1995-06-01

    The Northeast Water Polynya (NEW) off the northeast coast of Greenland was the focus of two cruises aboard the USCGC Polar Sea during the summers of 1992 and 1993. The cruises were supported by the National Science Foundation Arctic Systems Science (ARCSS) program and were part of the Arctic Ocean Science Board`s International Arctic Polynya Program. The Polar Sea cruises were designed as multidisciplinary studies to test hypotheses about the mechanisms of heat, water and carbon flow within and beyond the boundaries of the polynya. Preliminary results of the 1992 study have been described elsewhere. A collection of papers arising from the 1992 cruise have been published in a Special Section of the Journal of Geophysical Research. This data report presents the hydrographic and basic chemical observations made from CTD/Rosette casts during the 1992 cruise. The station positions cruise are plotted in Figure 1. Also included in the report are selected section plots and vertical profiles. A total of 130 CTD casts were made during the cruise, measuring pressure, temperature, conductivity, dissolved oxygen, fluorescence and light transmission. Discrete samples were collected in 10-liter, rosette-mounted, Niskin bottles and analyzed, from most casts, for: salinity, dissolved nutrients, dissolved oxygen, anthropogenic halocarbons (e.g., Freon gases), pigments, particulate organic carbon and nitrogen. Suspended particulate matter was analyzed at selected stations and these data were used to calibrate the CTD-transmissometer. Samples were collected from selected stations and depths for tritium and helium analyses, carbonate chemistry, as well as for measurements of bacterial abundance.

  17. Multi-model Mean Nitrogen and Sulfur Deposition from the Atmospheric Chemistry and Climate Model Intercomparison Project (ACCMIP): Evaluation of Historical and Projected Future Changes

    SciTech Connect

    Lamarque, Jean-Francois; Dentener, Frank; McConnell, J.R.; Ro, C-U; Shaw, Mark; Vet, Robert; Bergmann, D.; Cameron-Smith, Philip; Dalsoren, S.; Doherty, R.; Faluvegi, G.; Ghan, Steven J.; Josse, B.; Lee, Y. H.; MacKenzie, I. A.; Plummer, David; Shindell, Drew; Skeie, R. B.; Stevenson, D. S.; Strode, S.; Zeng, G.; Curran, M.; Dahl-Jensen, D.; Das, S.; Fritzsche, D.; Nolan, M.

    2013-08-20

    We present multi-model global datasets of nitrogen and sulfate deposition covering time periods from 1850 to 2100, calculated within the Atmospheric Chemistry and Climate Model Intercomparison Project (ACCMIP). The computed deposition fluxes are compared to surface wet deposition and ice-core measurements. We use a new dataset of wet deposition for 2000-2002 based on critical assessment of the quality of existing regional network data. We show that for present-day (year 2000 ACCMIP time-slice), the ACCMIP results perform similarly to previously published multi-model assessments. The analysis of changes between 1980 and 2000 indicates significant differences between model and measurements over the United States, but less so over Europe. This difference points towards misrepresentation of 1980 NH3 emissions over North America. Based on ice-core records, the 1850 deposition fluxes agree well with Greenland ice cores but the change between 1850 and 2000 seems to be overestimated in the Northern Hemisphere for both nitrogen and sulfur species. Using the Representative Concentration Pathways to define the projected climate and atmospheric chemistry related emissions and concentrations, we find large regional nitrogen deposition increases in 2100 in Latin America, Africa and parts of Asia under some of the scenarios considered. Increases in South Asia are especially large, and are seen in all scenarios, with 2100 values more than double 2000 in some scenarios and reaching >1300 mgN/m2/yr averaged over regional to continental scale regions in RCP 2.6 and 8.5, ~30-50% larger than the values in any region currently (2000). Despite known issues, the new ACCMIP deposition dataset provides novel, consistent and evaluated global gridded deposition fields for use in a wide range of climate and ecological studies.

  18. Early Proterozoic transcontinental orogenic belts in the United States

    SciTech Connect

    Van Schmus, W.R. . Dept. of Geology); Bickford, M.E. . Dept. of Geology); Condie, K.C. . Dept. Geoscience)

    1993-02-01

    It has been recognized for many years that Early Proterozoic orogenic rocks in the western US range from 1.8 to 1.6 Ga, with a general distribution such that 1.8 to 1.7 Ga rocks underlie Colorado, northern Arizona, and northern New Mexico and 1.7 to 1.6 Ga rocks underlie southern Arizona and southern New Mexico. Recent U-Pb geochronologic and Sm-Nd isotopic studies by a variety of research groups have refined crustal history in the western region and have extended knowledge eastward into the buried midcontinent basement. As a result, the authors propose that 1.8 Ga to 1.6 Ga crust of the US by divided into two distinct, but overlapping, orogenic belts: a 1.8 to 1.7 Ga Inner Accretionary Belt and a 1.7 to 1.6 Ga Outer Tectonic Belt. The Inner Accretionary Belt (IAB) comprises rock suites with compositions and isotopic signatures compatible with origin as juvenile crustal terranes formed as oceanic or off-shore and related terranes that were accreted to southern Laurentia between 1.8 and 1.6 Ga. The IAB includes the Yavapai Province of Arizona, Early Proterozoic basement of Colorado and southern Wyoming, and the basement of Nebraska. The Mojave Province of California may be part of this belt, although it also includes components derived from older Proterozoic or Archean crust. Extension of the IAB eastward from Nebraska is uncertain at present, although coeval rocks that may be eastern manifestations of this 1.8 to 1.7 Ga orogenesis occur in Wisconsin (1.76 Ga granite-rhyolite suite), Ontario (Killarney granite), Labrador (Makkovic Province) and southern Greenland (Ketilidian orogen). The Outer Tectonic Belt (OTB) comprises rock suites which have compositions, structures, and isotopic signature compatible with origin in continental margin tectonic settings between 1.7 and 1.6 Ga.

  19. Evaluation of Preindustrial to Present-day Black Carbon and its Albedo Forcing from Atmospheric Chemistry and Climate Model Intercomparison Project (ACCMIP)

    SciTech Connect

    Lee, Y. H.; Lamarque, J.-F.; Flanner, M. G.; Jiao, C.; Shindell, Drew; Berntsen, T.; Bisiauxs, M.; Cao, J.; Collins, W. J.; Curran, M.; Edwards, R.; Faluvegi, G.; Ghan, Steven J.; Horowitz, L.; McConnell, J.R.; Ming, J.; Myhre, G.; Nagashima, T.; Naik, Vaishali; Rumbold, S.; Skeie, R. B.; Sudo, K.; Takemura, T.; Thevenon, F.; Xu, B.; Yoon, Jin-Ho

    2013-03-05

    As a part of the Atmospheric Chemistry and Climate Model Intercomparison Project (ACCMIP), we evaluate the historical black carbon (BC) aerosols simulated by 8 ACCMIP models against the observations including 12 ice core records, a long-term surface mass concentrations and recent Arctic BC snowpack measurements. We also estimate BC albedo forcing by performing additional simulations using the NCAR Community Land and Sea-Ice model 4 with prescribed meteorology from 1996-2000, which includes the SNICAR BC-snow model. We evaluated the vertical profile of BC snow concentrations from these offline simulations to using recent BC snowpack measurements. Despite using the same BC emissions, global BC burden differs by approximately a factor of 3 among models due to the differences in aerosol removal parameterizations and simulated meteorology among models; 34 Gg to 103 Gg in 1850 and 82 Gg to 315 Gg in 2000. However,models agree well on 2.5~3 times increase in the global BC burden from preindustrial to present-day, which matches with the 2.5 times increase in BC emissions. We find a large model diversity at both NH and SH high latitude regions for BC burden and at SH high latitude regions for deposition fluxes. The ACCMIP simulations match the observed BC mass concentrations well in Europe and North America except at Jungfrauch and Ispra. However, the models fail to capture the Arctic BC seasonality due tosevere underestimations during winter and spring. Compared to recent snowpack measurements, the simulated vertically resolved BC snow concentrations are, on average, within a factor of 2-3 of observations except for Greenland and Arctic Ocean. However, model and observation differ widely due to missing interannual variations in emissions and possibly due to the choice of the prescribed meteorology period (i.e., 1996-2000).

  20. A CHRONOLOGICAL FRAMEWORK FOR THE HOLOCENE VEGETATIONAL HISTORY OF CENTRAL MINNESOTA: THE STEEL LAKE POLLEN RECORD

    SciTech Connect

    Wright, H E; Stefanova, I; Tian, J; Brown, T A; Hu, F S

    2003-11-10

    Paleorecords from Minnesota and adjacent areas have often been used to evaluate large-scale climatic processes in the mid-continent of North America. However, most of these records are compromised by chronological flaws, making problematic any comparisons with climatic interpretations based on other records (e.g., GISP2 in Greenland). We report here a high-resolution pollen record with a secure chronology constrained by 26 {sup 14}C dates on terrestrial macrofossils from Steel Lake, central Minnesota. About 11,200 years ago (calibrated yr BP) the late-glacial Picea forest near Steel Lake was succeeded abruptly by Pinus banksiana and/or resinosa. The Pinus forest began to open 9.4 ka cal BP with the expansion of prairie taxa, and a pine parkland or savanna prevailed until about 8 ka cal BP, when Quercus replaced Pinus to become the dominant tree in the prairie areas for 4500 years. The close chronological control permits the correlation of key vegetational changes with those at other reliably dated sites in the eastern Dakotas and in Minnesota, suggesting that the abrupt decline of the spruce forest was time-transgressive from southwest to northeast during 2000 years, and that the development of prairie was time-transgressive in the same direction over 2600 years. Correlation of key pollen horizons at Steel Lake with those in the high-resolution pollen profiles of Elk Lake, ca. 50 km northwest of Steel Lake, suggests that the well-known Elk Lake varve chronology for the early Holocene is about 1000 years too young.

  1. The ARIES Advanced And Conservative Tokamak (ACT) Power Plant Study

    SciTech Connect

    Kessel, C. E.; Poli, F. M.; Ghantous, K.; Gorelenkov, N.; Tillack, M. S.; Najmabadi, F.; Wang, X. R.; Navaei, D.; Toudeshki, H. H.; Koehly, C.; El-Guebaly, L.; Blanchard, J. P.; Martin, C. J.; Mynsburge, L.; Humrickhouse, P.; Rensink, M. E.; Rognlien, T. D.; Yoda, M.; Abdel-Khalik, S. I.; Hageman, M. D.; Mills, B. H.; Radar, J. D.; Sadowski, D. L.; Snyder, P. B.; St. John, H.; Turnbull, A. D.; Waganer, L. M.; Malang, S.; Rowcliffe, A. F.

    2014-03-05

    Tokamak power plants are studied with advanced and conservative design philosophies in order to identify the impacts on the resulting designs and to provide guidance to critical research needs. Incorporating updated physics understanding, and using more sophisticated engineering and physics analysis, the tokamak configurations have developed a more credible basis compared to older studies. The advanced configuration assumes a self-cooled lead lithium (SCLL) blanket concept with SiC composite structural material with 58% thermal conversion efficiency. This plasma has a major radius of 6.25 m, a toroidal field of 6.0 T, a q95 of 4.5, a {beta}N{sup total} of 5.75, H{sub 98} of 1.65, n/nGr of 1.0, and peak divertor heat flux of 13.7 MW/m{sup 2}. The conservative configuration assumes a dual coolant lead lithium (DCLL) blanket concept with ferritic steel structural material and helium coolant, achieving a thermal conversion efficiency of 45%. The plasma major radius is 9.75 m, a toroidal field of 8.75 T, a q95 of 8.0, a {beta}N{sup total} of 2.5, H{sub 98} of 1.25, n/n{sub Gr} of 1.3, and peak divertor heat flux of 10 MW/m{sup 2}. The divertor heat flux treatment with a narrow power scrape-off width has driven the plasmas to larger major radius. Edge and divertor plasma simulations are targeting a basis for high radiated power fraction in the divertor, which is necessary for solutions to keep the peak heat flux in the range of 10-15 MW/m{sup 2}. Combinations of the advanced and conservative approaches show intermediate sizes. A new systems code using a database approach has been used and shows that the operating point is really an operating zone with some range of plasma and engineering parameters and very similar costs of electricity. Papers in this issue provide more detailed discussion of the work summarized here.

  2. Lineage-related cytotoxicity and clonogenic profile of 1,4-benzoquinone-exposed hematopoietic stem and progenitor cells

    SciTech Connect

    Chow, Paik Wah; Abdul Hamid, Zariyantey; Chan, Kok Meng; Inayat-Hussain, Salmaan Hussain; Rajab, Nor Fadilah

    2015-04-01

    Hematopoietic stem cells (HSCs) and hematopoietic progenitor cells (HPCs) are sensitive targets for benzene-induced hematotoxicity and leukemogenesis. The impact of benzene exposure on the complex microenvironment of HSCs and HPCs remains elusive. This study aims to investigate the mechanism linking benzene exposure to targeting HSCs and HPCs using phenotypic and clonogenic analyses. Mouse bone marrow (BM) cells were exposed ex vivo to the benzene metabolite, 1,4-benzoquinone (1,4-BQ), for 24 h. Expression of cellular surface antigens for HSC (Sca-1), myeloid (Gr-1, CD11b), and lymphoid (CD45, CD3e) populations were confirmed by flow cytometry. The clonogenicity of cells was studied using the colony-forming unit (CFU) assay for multilineage (CFU-GM and CFU-GEMM) and single-lineage (CFU-E, BFU-E, CFU-G, and CFU-M) progenitors. 1,4-BQ demonstrated concentration-dependent cytotoxicity in mouse BM cells. The percentage of apoptotic cells increased (p < 0.05) following 1,4-BQ exposure. Exposure to 1,4-BQ showed no significant effect on CD3e{sup +} cells but reduced the total counts of Sca-1{sup +}, CD11b{sup +}, Gr-1{sup +}, and CD45{sup +} cells at 7 and 12 μM (p < 0.05). Furthermore, the CFU assay showed reduced (p < 0.05) clonogenicity in 1,4-BQ-treated cells. 1,4-BQ induced CFU-dependent cytotoxicity by significantly inhibiting colony growth for CFU-E, BFU-E, CFU-G, and CFU-M starting at a low concentration of exposure (5 μM); whereas for the CFU-GM and CFU-GEMM, the inhibition of colony growth was remarkable only at 7 and 12 μM of 1,4-BQ, respectively. Taken together, 1,4-BQ caused lineage-related cytotoxicity in mouse HPCs, demonstrating greater toxicity in single-lineage progenitors than in those of multi-lineage. - Highlights: • We examine 1,4-BQ toxicity targeting mouse hematopoietic cell lineages. • 1,4-BQ induces concentration-dependent cytotoxicity in bone marrow (BM) cells. • 1,4-BQ shows lineage-related toxicity on hematopoietic stem and

  3. The ARIES Advanced and Conservative Tokamak Power Plant Study

    SciTech Connect

    Kessel, C. E; Tillak, M. S; Najmabadi, F.; Poli, F. M.; Ghantous, K.; Gorelenkov, N.; Wang, X. R.; Navaei, D.; Toudeshki, H. H.; Koehly, C.; EL-Guebaly, L.; Blanchard, J. P.; Martin, C. J.; Mynsburge, L.; Humrickhouse, P.; Rensink, M. E.; Rognlien, T. D.; Yoda, M.; Abdel-Khalik, S. I.; Hageman, M. D.; Mills, B. H.; Rader, J. D.; Sadowski, D. L.; Snyder, P. B.; St. John, H.; Turnbull, A. D.; Waganer, L. M.; Malang, S.; Rowcliffe, A. F.

    2015-12-22

    Tokamak power plants are studied with advanced and conservative design philosophies to identify the impacts on the resulting designs and to provide guidance to critical research needs. Incorporating updated physics understanding and using more sophisticated engineering and physics analysis, the tokamak configurations have developed a more credible basis compared with older studies. The advanced configuration assumes a self-cooled lead lithium blanket concept with SiC composite structural material with 58% thermal conversion efficiency. This plasma has a major radius of 6.25 m, a toroidal field of 6.0 T, a q₉₅ of 4.5, aᵦtotal N of 5.75, an H98 of 1.65, an n/nGr of 1.0, and a peak divertor heat flux of 13.7 MW/m² . The conservative configuration assumes a dual-coolant lead lithium blanket concept with reduced activation ferritic martensitic steel structural material and helium coolant, achieving a thermal conversion efficiency of 45%. The plasma has a major radius of 9.75 m, a toroidal field of 8.75 T, a q₉₅ of 8.0, aᵦtotalN of 2.5, an H₉₈ of 1.25, an n/nGr of 1.3, and a peak divertor heat flux of 10 MW/m² . The divertor heat flux treatment with a narrow power scrape off width has driven the plasmas to larger major radius. Edge and divertor plasma simulations are targeting a basis for high radiated power fraction in the divertor, which is necessary for solutions to keep the peak heat flux in the range 10 to 15 MW/m² . Combinations of the advanced and conservative approaches show intermediate sizes. A new systems code using a database approach has been used and shows that the operating point is really an operating zone with some range of plasma and engineering parameters and very similar costs of electricity. Other papers in this issue provide more detailed discussion of the work summarized here.

  4. Exogenous contrast agents for thermoacoustic imaging: An investigation into the underlying sources of contrast

    SciTech Connect

    Ogunlade, Olumide Beard, Paul

    2015-01-15

    Purpose: Thermoacoustic imaging at microwave excitation frequencies is limited by the low differential contrast exhibited by high water content tissues. To overcome this, exogenous thermoacoustic contrast agents based on gadolinium compounds, iron oxide, and single wall carbon nanotubes have previously been suggested and investigated. However, these previous studies did not fully characterize the electric, magnetic, and thermodynamic properties of these agents thus precluding identification of the underlying sources of contrast. To address this, measurements of the complex permittivity, complex permeability, DC conductivity, and Grüneisen parameter have been made. These measurements allowed the origins of the contrast provided by each substance to be identified. Methods: The electric and magnetic properties of the contrast agents were characterized at 3 GHz using two rectangular waveguide cavities. The DC conductivity was measured separately using a conductivity meter. Thermoacoustic signals were then acquired and compared to those generated in water. Finally, 3D electromagnetic simulations were used to decouple the different contributions to the absorbed power density. Results: It was found that the gadolinium compounds provided appreciable electric contrast but not originating from the gadolinium itself. The contrast was either due to dissociation of the gadolinium salt which increased ionic conductivity or its nondissociated polar fraction which increased dielectric polarization loss or a combination of both. In addition, very high concentrations were required to achieve appreciable contrast, to the extent that the Grüneisen parameter increased significantly and became a source of contrast. Iron oxide particles were found to produce low but measurable dielectric contrast due to dielectric polarization loss, but this is attributed to the coating of the particles not the iron oxide. Single wall carbon nanotubes did not provide measurable contrast of any type

  5. The ARIES Advanced and Conservative Tokamak Power Plant Study

    DOE PAGES [OSTI]

    Kessel, C. E; Tillak, M. S; Najmabadi, F.; Poli, F. M.; Ghantous, K.; Gorelenkov, N.; Wang, X. R.; Navaei, D.; Toudeshki, H. H.; Koehly, C.; et al

    2015-12-22

    Tokamak power plants are studied with advanced and conservative design philosophies to identify the impacts on the resulting designs and to provide guidance to critical research needs. Incorporating updated physics understanding and using more sophisticated engineering and physics analysis, the tokamak configurations have developed a more credible basis compared with older studies. The advanced configuration assumes a self-cooled lead lithium blanket concept with SiC composite structural material with 58% thermal conversion efficiency. This plasma has a major radius of 6.25 m, a toroidal field of 6.0 T, a q₉₅ of 4.5, aᵦtotal N of 5.75, an H98 of 1.65, anmore » n/nGr of 1.0, and a peak divertor heat flux of 13.7 MW/m² . The conservative configuration assumes a dual-coolant lead lithium blanket concept with reduced activation ferritic martensitic steel structural material and helium coolant, achieving a thermal conversion efficiency of 45%. The plasma has a major radius of 9.75 m, a toroidal field of 8.75 T, a q₉₅ of 8.0, aᵦtotalN of 2.5, an H₉₈ of 1.25, an n/nGr of 1.3, and a peak divertor heat flux of 10 MW/m² . The divertor heat flux treatment with a narrow power scrape off width has driven the plasmas to larger major radius. Edge and divertor plasma simulations are targeting a basis for high radiated power fraction in the divertor, which is necessary for solutions to keep the peak heat flux in the range 10 to 15 MW/m² . Combinations of the advanced and conservative approaches show intermediate sizes. A new systems code using a database approach has been used and shows that the operating point is really an operating zone with some range of plasma and engineering parameters and very similar costs of electricity. Other papers in this issue provide more detailed discussion of the work summarized here.« less

  6. Structural, thermal, magnetic, and electronic transport properties of the LaNi₂(Ge1-xPx)₂ system

    DOE PAGES [OSTI]

    Goetsch, R. J.; Anand, V. K.; Pandey, Abhishek; Johnston, D. C.

    2012-02-29

    Polycrystalline samples of LaNi₂(Ge1-xPx)₂ (x=0,0.25,0.50,0.75,1) were synthesized and their properties investigated by x-ray diffraction (XRD) measurements at room temperature and by heat capacity Cp, magnetic susceptibility χ, and electrical resistivity ρ measurements versus temperature T from 1.8 to 350 K. Rietveld refinements of powder XRD patterns confirm that these compounds crystallize in the body-centered-tetragonal ThCr₂Si₂-type structure (space group I4/mmm) with composition-dependent lattice parameters that slightly deviate from Vegard's law. The ρ(T) measurements showed a positive temperature coefficient for all samples from 1.8 to 300 K, indicating that all compositions in this system are metallic. The low-T Cp measurements yield amore » rather large Sommerfeld electronic specific heat coefficient γ=12.4(2) mJ/mol K² for x=0, reflecting a large density of states at the Fermi energy that is comparable with the largest values found for the AFe₂As₂ class of materials with the same crystal structure. The γ decreases approximately linearly with x to 7.4(1) mJ/mol K² for x=1. The χ measurements show nearly temperature-independent paramagnetic behavior across the entire range of compositions except for LaNi₂Ge₂, where a broad peak is observed at ≈300 K from χ(T) measurements up to 1000 K that may arise from short-range antiferromagnetic correlations in a quasi-two-dimensional magnetic system. High-accuracy Padé approximants representing the Debye lattice heat capacity and Bloch-Grüneisen electron-phonon resistivity functions versus T are presented and are used to analyze our experimental Cp(T) and ρ(T) data, respectively, for 1.8K≤T≤300 K. The T dependences of ρ for all samples are well-described over this T range by the Bloch-Grüneisen model, although the observed ρ(300 K) values are larger than calculated from this model. A significant T dependence of the Debye temperature determined from the Cp(T) data was observed

  7. Imaging individual lanthanum atoms in zeolite Y by scanning transmission electron microscopy: evidence of lanthanum pair sites

    SciTech Connect

    Xu, Pinghong; Lu, Jing; Aydin, C.; Debefve, Louise M.; Browning, Nigel D.; Chen, Cong-Yan; Gates, Bruce C.

    2015-09-01

    Images of La-exchanged NaY zeolite obtained with aberration-corrected scanning transmission electron microscopy (STEM) show that about 80% of the La cations were present as site-isolated species, with the remainder in pair sites. The distance between La cations in the pair sites ranged from 1.44 to 3.84 Å, consistent with the presence of pairs of cations tilted at various angles with respect to the support surface. The actual distance between La cations in the pair sites is inferred to be approximately 3.84 Å, which is shorter than the distance between the nearest Al sites in the zeolite (4.31 Å). The results therefore suggest the presence of dimeric structures of La cations bridged with OH groups, and the presence of such species has been inferred previously on the basis of X-ray photoelectron spectroscopy (W. Grünert, U. Sauerlandt, R. Schlögl, H.G. Karge, J. Phys. Chem., 97 (1993) 1413).

  8. Anisotropic lattice thermal expansion of PbFeBO4: A study by X-ray and neutron diffraction, Raman spectroscopy and DFT calculations

    DOE PAGES [OSTI]

    Murshed, M. Mangir; Mendive, Cecilia B.; Curti, Mariano; Nénert, Gwilherm; Kalita, Patricia E.; Lipinska, Kris; Cornelius, Andrew L.; Huq, Ashfia; Gesing, Thorsten M.

    2014-11-01

    We present the lattice thermal expansion of mullite-type PbFeBO4 in this study. The thermal expansion coefficients of the metric parameters were obtained from composite data collected from temperature-dependent neutron and X-ray powder diffraction between 10 K and 700 K. The volume thermal expansion was modeled using extended Grüneisen first-order approximation to the zero-pressure equation of state. The additive frame of the model includes harmonic, quasi-harmonic and intrinsic anharmonic potentials to describe the change of the internal energy as a function of temperature. Moreover, the unit-cell volume at zero-pressure and 0 K was optimized during the DFT simulations. Harmonic frequencies ofmore » the optical Raman modes at the Γ-point of the Brillouin zone at 0 K were also calculated by DFT, which help to assign and crosscheck the experimental frequencies. The low-temperature Raman spectra showed significant anomaly in the antiferromagnetic regions, leading to softening or hardening of some phonons. Selected modes were analyzed using a modified Klemens model. The shift of the frequencies and the broadening of the line-widths helped to understand the anharmonic vibrational behaviors of the PbO4, FeO6 and BO3 polyhedra as a function of temperature.« less

  9. Anisotropic lattice thermal expansion of PbFeBO4: A study by X-ray and neutron diffraction, Raman spectroscopy and DFT calculations

    SciTech Connect

    Murshed, M. Mangir; Mendive, Cecilia B.; Curti, Mariano; Nénert, Gwilherm; Kalita, Patricia E.; Lipinska, Kris; Cornelius, Andrew L.; Huq, Ashfia; Gesing, Thorsten M.

    2014-11-01

    We present the lattice thermal expansion of mullite-type PbFeBO4 in this study. The thermal expansion coefficients of the metric parameters were obtained from composite data collected from temperature-dependent neutron and X-ray powder diffraction between 10 K and 700 K. The volume thermal expansion was modeled using extended Grüneisen first-order approximation to the zero-pressure equation of state. The additive frame of the model includes harmonic, quasi-harmonic and intrinsic anharmonic potentials to describe the change of the internal energy as a function of temperature. Moreover, the unit-cell volume at zero-pressure and 0 K was optimized during the DFT simulations. Harmonic frequencies of the optical Raman modes at the Γ-point of the Brillouin zone at 0 K were also calculated by DFT, which help to assign and crosscheck the experimental frequencies. The low-temperature Raman spectra showed significant anomaly in the antiferromagnetic regions, leading to softening or hardening of some phonons. Selected modes were analyzed using a modified Klemens model. The shift of the frequencies and the broadening of the line-widths helped to understand the anharmonic vibrational behaviors of the PbO4, FeO6 and BO3 polyhedra as a function of temperature.

  10. The Physics of Basis For A Conservative Physics And Conservative Technology Tokamak Power Plant, ARIES-ACT2

    SciTech Connect

    Kessel, C. E.

    2014-03-04

    The conservative physics and conservative technology tokamak power plant ARIES-ACT2 has a major radius of 9.75 m at aspect ratio of 4.0, strong shaping with elongation of 2.2 and triangularity of 0.63. The no wall {beta}N reaches {approximately} 2.4, limited by n=1 external kink mode, and can be extended to 3.2 with a stabilizing shell behind the ring structure shield. The bootstrap current fraction is 77% with a q95 of 8.0, requiring about {approximately} 4.0 MA of external current drive. This current is supplied with 30 MW of ICRF/FW and 80 MW of negative ion NB. Up to 1.0 MA can be driven with LH with no wall, and 1.5 or more MA can be driven with a stabilizing shell. EC was examined and is most effective for safety factor control over {rho} {approximately} 0.2-0.6 with 20 MW. The pedestal density is {approximately} 0.65x10{sup 20}/m{sup 3} and the temperature is {approximately} 9.0 keV. The H98 factor is 1.25, n/n{sub Gr} = 1.3, and the net power to LH threshold power is 1.3-1.4 in the flattop. Due to the high toroidal field and high central temperature the cyclotron radiation loss was found to be high depending on the first wall reflectivity.

  11. Quantization of systems with temporally varying discretization. I. Evolving Hilbert spaces

    SciTech Connect

    Hhn, Philipp A.

    2014-08-15

    A temporally varying discretization often features in discrete gravitational systems and appears in lattice field theory models subject to a coarse graining or refining dynamics. To better understand such discretization changing dynamics in the quantum theory, an according formalism for constrained variational discrete systems is constructed. While this paper focuses on global evolution moves and, for simplicity, restricts to flat configuration spaces R{sup N}, a Paper II [P. A. Hhn, Quantization of systems with temporally varying discretization. II. Local evolution moves, J. Math. Phys., e-print http://arxiv.org/abs/arXiv:1401.7731 [gr-qc].] discusses local evolution moves. In order to link the covariant and canonical picture, the dynamics of the quantum states is generated by propagators which satisfy the canonical constraints and are constructed using the action and group averaging projectors. This projector formalism offers a systematic method for tracing and regularizing divergences in the resulting state sums. Non-trivial coarse graining evolution moves lead to non-unitary, and thus irreversible, projections of physical Hilbert spaces and Dirac observables such that these concepts become evolution move dependent on temporally varying discretizations. The formalism is illustrated in a toy model mimicking a creation from nothing. Subtleties arising when applying such a formalism to quantum gravity models are discussed.

  12. Properties of gravitationally equilibrated Yukawa systemsA molecular dynamics study

    SciTech Connect

    Charan, Harish; Ganesh, Rajaraman Joy, Ashwin

    2014-04-15

    Using 2D Molecular Dynamics simulation, the equilibrium and dynamical properties of a gravitationally equilibrated Yukawa liquid are investigated. We observe that due to asymmetry introduced in one direction by gravity, several interesting features arise. For example, for a given value of coupling parameter ?, screening parameter ?, and according to a chosen value of gravitational force g (say in y-direction), the system is seen to exhibit super-, sub- or normal diffusion. Interestingly, x-averaged density profiles, unlike a barotropic fluid, acquires sharp, free surface with scale free linear y-dependence. As can be expected for a system with macroscopic gradients, self-diffusion calculated from Green-Kubos formalism does not agree with that obtained from Einstein-Smoluchowski diffusion. A 2D angular-radial pair correlation function g(r, ?) clearly indicates asymmetric features induced by gravity. We observe that due to compression in y-direction, though in liquid state for all values of gravity considered, the transverse mode is found to predominant as compared to the longitudinal mode, leading to a novel Anisotropic Solid-like Yukawa liquid.

  13. A=07Be (66LA04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 7Be) GENERAL: See (FR57, PH60A, SH60C, TA60L, KU61E, TA61G, TO61B, GL62A, IN62, AR64D, BA64I, GR64C, HO64D, LI64G, MO64F, NE64D, PA64N, PH64, RA64, SA64G, ST64). See also Table 7.9 [Table of Energy Levels] (in PDF or PS). 1. 7Be(ε)7Li Qm = 0.862 The decay is complex: see 7Li. 2. 4He(3He, γ)7Be Qm = 1.587 In the range Eα = 0.42 to 5.80 MeV the cross section rises from 0.02 to 4 μb. The branching ratio γ0 (to g.s.)/γ1 (to 0.4 MeV state) remains at 73/27

  14. A=07Li (66LA04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 7Li) GENERAL: See (HU57D, BA59K, BA59N, BR59M, FE59E, MA59E, MA59H, KU60A, PE60E, PH60A, SH60C, TA60L, BA61H, BA61N, BL61C, CL61D, KH61, TA61G, TO61B, CL62E, CR62A, IN62, CH63, CL63C, KL63, SC63I, BE64H, GR64C, MA64HH, NE64C, OL64A, SA64G, BE65F, FA65A, JA65H, NE65, PR65). See also Table 7.1 [Table of Energy Levels] (in PDF or PS). Ground state: Q = -45 ± 5 mb (KA61F, VA63F, WH64); μ = +3.2564 nm (FU65E). 1. 4He(t, γ)7Li Qm = 2.467 Excitation functions

  15. A=14C (1970AJ04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    0AJ04) (See Energy Level Diagrams for 14C) GENERAL: See Table 14.1 [Table of Energy Levels] (in PDF or PS). See (1954JA1A, 1956EL1B, 1957VI1A, 1958BA1A, 1959OT1A, 1959SK1A, 1960TA1C, 1960WA12, 1961BA1F, 1961FR1C, 1962TA1E, 1963BL1B, 1963NA04, 1963SO04, 1963VL1A, 1964LI1B, 1964LO1B, 1965BA1X, 1965KO1D, 1965WA1J, 1965ZA1B, 1966BA42, 1966BO1R, 1966GU08, 1966MI1G, 1966ZA03, 1967GR1D, 1967HA10, 1967IN1B, 1967KO1N, 1967KO1F, 1968EI1C, 1968FA1B, 1968FR03, 1968NE1C, 1968RO1C, 1969AR13, 1969AT1A,

  16. A=6Li (66LA04)

    U.S. Department of Energy (DOE) - all webpages (Extended Search)

    66LA04) (See Energy Level Diagrams for 6Li) GENERAL: See Table 6.4 [Table of Energy Levels] (in PDF or PS). See also (AU55, LA55, ME56, FR57, HU57D, LE57F, PI58, BA59K, BR59M, FE59E, SK59, UB59, AN60, JA60G, KO60E, PH60A, TA60L, WA60F, BA61N, KO61A, SH61B, TA61G, VA61, CO62B, CR62A, DI62B, FO62E, GA62C, IN62, IN62A, IN62B, JA62, ME62A, NA62C, SA62C, ST62B, WA62H, BO63B, BU63D, DA63D, EL63D, HA63K, JA63C, JO63B, KL63, KU63B, KU63I, MO63C, OL63B, SA63K, SC63E, SC63I, VL63A, WA63, GR64C, JI64,

  17. Interfacial microstructure and properties of copper clad steel produced using friction stir welding versus gas metal arc welding

    SciTech Connect

    Shen, Z.; Chen, Y.; Haghshenas, M.; Nguyen, T.; Galloway, J.; Gerlich, A.P.

    2015-06-15

    A preliminary study compares the feasibility and microstructures of pure copper claddings produced on a pressure vessel A516 Gr. 70 steel plate, using friction stir welding versus gas metal arc welding. A combination of optical and scanning electron microscopy is used to characterize the grain structures in both the copper cladding and heat affected zone in the steel near the fusion line. The friction stir welding technique produces copper cladding with a grain size of around 25 μm, and no evidence of liquid copper penetration into the steel. The gas metal arc welding of copper cladding exhibits grain sizes over 1 mm, and with surface microcracks as well as penetration of liquid copper up to 50 μm into the steel substrate. Transmission electron microscopy reveals that metallurgical bonding is produced in both processes. Increased diffusion of Mn and Si into the copper cladding occurs when using gas metal arc welding, although some nano-pores were detected in the FSW joint interface. - Highlights: • Cladding of steel with pure copper is possible using either FSW or GMAW. • The FSW yielded a finer grain structure in the copper, with no evidence of cracking. • The FSW joint contains some evidence of nano-pores at the interface of the steel/copper. • Copper cladding by GMAW contained surface cracks attributed to high thermal stresses. • The steel adjacent to the fusion line maintained a hardness value below 248 HV.

  18. Crystallization and preliminary X-ray diffraction study of phosphoribosyl pyrophosphate synthetase from E. Coli

    SciTech Connect

    Timofeev, V. I. Abramchik, Yu. A. Zhukhlistova, N. E. Kuranova, I. P.

    2015-09-15

    Enzymes of the phosphoribosyl pyrophosphate synthetase family (PRPPS, EC 2.7.6.1) catalyze the formation of 5-phosphoribosyl pyrophosphate (5-PRPP) from adenosine triphosphate and ribose 5-phosphate. 5-Phosphoribosyl pyrophosphate is an important intermediate in the synthesis of purine, pyrimidine, and pyridine nucleotides, as well as of the amino acids histidine and tryptophan. The crystallization conditions for E. coli PRPPS were found by the vapor-diffusion technique and were optimized to apply the capillary counter-diffusion technique. The X-ray diffraction data set was collected from the crystals grown by the counter-diffusion technique using a synchrotron radiation source to 3.1-Å resolution. The crystals of PRPPS belong to sp. gr. P6{sub 3}22 and have the following unit-cell parameters: a = b = 104.44 Å, c = 124.98 Å, α = β = 90°, γ = 120°. The collected X-ray diffraction data set is suitable for the solution of the three-dimensional structure of PRPPS at 3.1-Å resolution.

  19. Advanced steel reheat furnaces: Research and development. Final report

    SciTech Connect

    Nguyen, Q.; Koppang, R.; Maly, P.; Moyeda, D.; Li, X.

    1999-01-14

    The purpose of this report is to present the results of two phases of a three-phase project to develop and evaluate an Advanced Steel Reheat Furnace (SSRF) concept which incorporates two proven and commercialized technologies, oxy-fuel enriched air (OEA) combustion and gas reburning (GR). The combined technologies aim to improve furnace productivity with higher flame radiant heat transfer in the heating zones of a steel reheat furnace while controlling potentially higher NOx emissions from these zones. The project was conducted under a contract sponsored by the Department of Energy (DOE). Specifically, this report summarizes the results of a modeling study and an experimental study to define and evaluate the issues which affect the integration and performance of the combined technologies. Section 2.0 of the report describes the technical approach uses in the development and evaluation of the advanced steel reheat furnace. Section 3.0 presents results of the modeling study applied to a model steel furnace. Experimental validation of the modeling results obtained from EER`s Fuel Evaluation Facility (FEF) pilot-scale furnace discussed in Section 4.0. Section 5.0 provides an economic evaluation on the cost effectiveness of the advanced reheat furnace concept. Section 6.0 concludes the report with recommendations on the applicability of the combined technologies of steel reheat furnaces.

  20. MAPPING THE LOCAL HALO: STATISTICAL PARALLAX ANALYSIS OF SDSS LOW-MASS SUBDWARFS

    SciTech Connect

    Bochanski, John J.; Savcheva, Antonia; West, Andrew A.; Hawley, Suzanne L.

    2013-02-01

    We present a statistical parallax study of nearly 2000 M subdwarfs with photometry and spectroscopy from the Sloan Digital Sky Survey (SDSS). Statistical parallax analysis yields the mean absolute magnitudes, mean velocities, and velocity ellipsoids for homogenous samples of stars. We selected homogeneous groups of subdwarfs based on their photometric colors and spectral appearance. We examined the color-magnitude relations of low-mass subdwarfs and quantified their dependence on the newly refined metallicity parameter, {zeta}. We also developed a photometric metallicity parameter, {delta}{sub (g-r)}, based on the g - r and r - z colors of low-mass stars and used it to select stars with similar metallicities. The kinematics of low-mass subdwarfs as a function of color and metallicity were also examined and compared to main-sequence M dwarfs. We find that the SDSS subdwarfs share similar kinematics to the inner halo and thick disk. The color-magnitude relations derived in this analysis will be a powerful tool for identifying and characterizing low-mass metal-poor subdwarfs in future surveys such as Gaia and LSST, making them important and plentiful tracers of the stellar halo.

  1. Precision grid and hand motion for accurate needle insertion in brachytherapy

    SciTech Connect

    McGill, Carl S.; Schwartz, Jonathon A.; Moore, Jason Z.; McLaughlin, Patrick W.; Shih, Albert J.

    2011-08-15

    Purpose: In prostate brachytherapy, a grid is used to guide a needle tip toward a preplanned location within the tissue. During insertion, the needle deflects en route resulting in target misplacement. In this paper, 18-gauge needle insertion experiments into phantom were performed to test effects of three parameters, which include the clearance between the grid hole and needle, the thickness of the grid, and the needle insertion speed. Measurement apparatus that consisted of two datum surfaces and digital depth gauge was developed to quantify needle deflections. Methods: The gauge repeatability and reproducibility (GR and R) test was performed on the measurement apparatus, and it proved to be capable of measuring a 2 mm tolerance from the target. Replicated experiments were performed on a 2{sup 3} factorial design (three parameters at two levels) and analysis included averages and standard deviation along with an analysis of variance (ANOVA) to find significant single and two-way interaction factors. Results: Results showed that grid with tight clearance hole and slow needle speed increased precision and accuracy of needle insertion. The tight grid was vital to enhance precision and accuracy of needle insertion for both slow and fast insertion speed; additionally, at slow speed the tight, thick grid improved needle precision and accuracy. Conclusions: In summary, the tight grid is important, regardless of speed. The grid design, which shows the capability to reduce the needle deflection in brachytherapy procedures, can potentially be implemented in the brachytherapy procedure.

  2. Preferred frame parameters in the tensor-vector-scalar theory of gravity and its generalization

    SciTech Connect

    Sagi, Eva

    2009-08-15

    The tensor-vector-scalar theory of gravity, which was designed as a relativistic implementation to the modified dynamics paradigm, has fared quite well as an alternative to dark matter, on both galactic and cosmological scales. However, its performance in the Solar System, as embodied in the post-Newtonian formalism, has not yet been fully investigated. We calculate the post-Newtonian parameters for TeVeS with the cosmological value of the scalar field taken into account, and show that in this situation the cosmological value of the scalar field is tightly linked to the vector field coupling constant K, preventing the former from evolving as predicted by its equation of motion. We show that generalizing TeVeS to have an Aether-type vector action, as suggested by Skordis, removes the aforesaid link, and this generalized version of TeVes has its {beta}, {gamma}, and {xi} parameterized post-Newtonian parameters identical to those in GR, while solar system constraints on the preferred frame parameters {alpha}{sub 1} and {alpha}{sub 2} can be satisfied within a modest range of small values of the scalar and vector fields coupling parameters, and for cosmological values of the scalar field consistent with evolution within the framework of existing cosmological models.

  3. Influence of piezoelectric strain on the Raman spectra of BiFeO3 films deposited on PMN-PT substrates

    DOE PAGES [OSTI]

    Himcinschi, Cameliu; Guo, Er -Jia; Talkenberger, Andreas; Dorr, Kathrin; Kortus, Jens

    2016-01-27

    In this study, BiFeO3 epitaxial thin films were deposited on piezoelectric 0.72Pb(Mg1/3Nb2/3)O3-0.28PbTiO3 (PMN-PT) substrates with a conductive buffer layer (La0.7Sr0.3MnO3 or SrRuO3) using pulsed laser deposition. The calibration of the strain values induced by the electric field applied on the piezoelectric PMN-PT substrates was realised using X-Ray diffraction measurements. The method of piezoelectrically induced strain allows to obtain a quantitative correlation between strain and the shift of the Raman-active phonons, ruling out the influence of extrinsic factors, such as growth conditions, crystalline quality of substrates, or film thickness. Using the Poisson number for BiFeO3 one can determine the volume changemore » induced by strain, and therefore the Gr neisen parameters for specific phonon modes.« less

  4. Extracellular Matrix-Regulated Gene Expression RequiresCooperation of SWI/SNF and Transcription Factors

    SciTech Connect

    Xu, Ren; Spencer, Virginia A.; Bissell, Mina J.

    2006-05-25

    Extracellular cues play crucial roles in the transcriptional regulation of tissue-specific genes, but whether and how these signals lead to chromatin remodeling is not understood and subject to debate. Using chromatin immunoprecipitation (ChIP) assays and mammary-specific genes as models, we show here that extracellular matrix (ECM) molecules and prolactin cooperate to induce histone acetylation and binding of transcription factors and the SWI/SNF complex to the {beta}- and ?-casein promoters. Introduction of a dominant negative Brg1, an ATPase subunit of SWI/SNF complex, significantly reduced both {beta}- and ?-casein expression, suggesting that SWI/SNF-dependent chromatin remodeling is required for transcription of mammary-specific genes. ChIP analyses demonstrated that the ATPase activity of SWI/SNF is necessary for recruitment of RNA transcriptional machinery, but not for binding of transcription factors or for histone acetylation. Coimmunoprecipitation analyses showed that the SWI/SNF complex is associated with STAT5, C/EBP{beta}, and glucocorticoid receptor (GR). Thus, ECM- and prolactin-regulated transcription of the mammary-specific casein genes requires the concerted action of chromatin remodeling enzymes and transcription factors.

  5. Luminescence characteristics of cerium-containing glass phases and ceramics based on them

    SciTech Connect

    Alimov, R.; Gulamova, R.R.; Muminov, M.I.; Khotamov, M.D.

    1987-12-01

    The authors considered the results obtained in investigations of the optical characteristics, namely the gamma luminescence and the thermoluminescence, in gamma-irradiated glasses selected as the glass phases and in ceramics synthetized on the basis of those glasses. An investigation of the gamma luminescence of the cerium glasses has shown that the gamma luminescence spectra of magnesium-containing glasses in which the cerium concentration varies between 1.5 and 9% are composed of a single band with the maximum at 410-420, 440, and 460 nm. An increase in the CeO/sub 2/ concentration shifts the maximum of the bands toward longer wavelengths and reduces the luminescence intensity, probably by concentration quenching. The thermoluminescence of the cerium-containing glasses was studied in the temperature range 0-450/sup 0/C and at absorbed doses of 10/sup 2/-2 x 10/sup 8/ Gr. On the thermoluminescence curves of the irradiated samples there appears a peak whose T/sub max/ and intensity depend upon the cerium concentration i the glass and upon the absorbed energy of the gamma radiation

  6. An emergent universe from a loop

    SciTech Connect

    Mulryne, David J.; Tavakol, Reza; Lidsey, James E.; Ellis, George F. R.

    2005-06-15

    Closed, singularity-free, inflationary cosmological models have recently been studied in the context of general relativity. Despite their appeal, these so called emergent models suffer from a number of limitations. These include the fact that they rely on an initial Einstein static state to describe the past-eternal phase of the universe. Given the instability of such a state within the context of general relativity, this amounts to a very severe fine tuning. Also in order to be able to study the dynamics of the universe within the context of general relativity, they set the initial conditions for the universe in the classical phase. Here we study the existence and stability of such models in the context of Loop Quantum Cosmology and show that both these limitations can be partially remedied, once semiclassical effects are taken into account. An important consequence of these effects is to give rise to a static solution (not present in GR), which dynamically is a center equilibrium point and located in the more natural semiclassical regime. This allows the construction of emergent models in which the universe oscillates indefinitely about such an initial static state. We construct an explicit emergent model of this type, in which a nonsingular past-eternal oscillating universe enters a phase where the symmetry of the oscillations is broken, leading to an emergent inflationary epoch, while satisfying all observational and semiclassical constraints. We also discuss emergent models in which the universe possesses both early- and late-time accelerating phases.

  7. Effects of constraint on upper shelf fracture toughness

    SciTech Connect

    Joyce, J.A.; Link, R.E.

    1995-12-31

    The upper shelf fracture toughness and tearing resistance of two structural steels, HY-100 and ASTM A533, Gr. B, were determined over a wide range of applied constraint. The constraint conditions were varied by changes in specimen geometry and loading mode. Bend specimens with shallow and deep cracks, compact specimens, and single and double edge notched tension specimens were used in this study. A rotation correction was developed for the single edge notch tension specimen which greatly improved the behavior of the J-R curves determined using this specimen. The experimental results were used to investigate the applicability of the Q and T stress parameters to the correlation of upper shelf initiation toughness, J{sub Ic}, and tearing resistance, T{sub mat}. The J-Q and J-T stress loci, and corresponding plots of material tearing resistance plotted against Q and T, were developed and compared with the expectations of the O`Dowd and Shih and the Betegon and Hancock analyses. The principle conclusions of this work are that J{sub Ic} does not appear to be dependent on T stress or Q while the material tearing resistance, T{sub mat}, is dependent on T stress and Q, with the tearing modulus increasing as constraint decreases.

  8. Study of runaway electrons using dosimetry of hard x-ray radiations in Damavand tokamak

    SciTech Connect

    Rasouli, C.; Pourshahab, B.; Rasouli, H.; Hosseini Pooya, S. M.; Orouji, T.

    2014-05-15

    In this work several studies have been conducted on hard x-ray emissions of Damavand tokamak based on radiation dosimetry using the Thermoluminescence method. The goal was to understand interactions of runaway electrons with plasma particles, vessel wall, and plasma facing components. Total of 354 GR-200 (LiF:Mg,Cu,P) thermoluminescence dosimeter (TLD) crystals have been placed on 118 points – three TLDs per point – to map hard x-ray radiation doses on the exterior of the vacuum vessel. Results show two distinctive levels of x-ray radiations doses on the exterior of the vessel. The low-dose area on which measured dose is about 0.5 mSv/shot. In the low-dose area there is no particular component inside the vessel. On the contrary, on high-dose area of the vessel, x-ray radiations dose exceeds 30 mSv/shot. The high-dose area coincides with the position of limiters, magnetic probe ducts, and vacuum vessel intersections. Among the high-dose areas, the highest level of dose is measured in the position of the limiter, which could be due to its direct contact with the plasma column and with runaway electrons. Direct collisions of runaway electrons with the vessel wall and plasma facing components make a major contribution for production of hard x-ray photons in Damavand tokamak.

  9. Measurement of the W boson helicity in events with a single reconstructed top quark in pp collisions at $ \\sqrt{s}=8 $ TeV

    SciTech Connect

    Khachatryan, V.

    2015-01-12

    A measurement of the W boson helicity is presented, where the W boson originates from the decay of a top quark produced in pp collisions. The event selection, optimized for reconstructing a single top quark in the final state, requires exactly one isolated lepton (muon or electron) and exactly two jets, one of which is likely to originate from the hadronization of a bottom quark. The analysis is performed using data recorded at a center-of-mass energy of 8 TeV with the CMS detector at the CERN LHC in 2012. The data sample corresponds to an integrated luminosity of 19.7 fb$^{-1}$. The measured helicity fractions are F$_{L}$ = 0.298 0.028 (stat) 0.032(syst), F$_{0}$ = 0.720 0.039 (stat) 0.037(syst), and F$_{R}$ = -0.018 0.019 (stat) 0.011(syst). These results are used to set limits on the real part of the tWb anomalous couplings, g$_{L}$ and g$_{R}$.

  10. Synthesis and crystal structure of the coordination compound of pyridoxine with manganese sulfate

    SciTech Connect

    Furmanova, N. G. Verin, I. A.; Shyityeva, N.; Sulaimankulov, K. S.; Berdalieva, Zh.; Resnyanskii, V. F.; Duishenbaeva, A. T.

    2011-11-15

    The reaction of pyridoxine with manganese sulfate in an aqueous solution gave the coordination compound MnSO{sub 4} {center_dot} 2C{sub 8}H{sub 11}O{sub 3}N {center_dot} 2H{sub 2}O (I). The structure of I was determined from single-crystal X-ray diffraction data. In the centrosymmetric complex (sp. gr. P1-bar, Z = 1), the Mn atom is coordinated by two pyridoxine molecules and two water molecules, thus adopting an octahedral coordination. The sulfate anion is also at a center of symmetry and, consequently, is disordered. The pyridoxine molecules are coordinated to the metal atom through the oxygen atoms of the deprotonated hydroxyl group and the CH{sub 2}OH group that retains the hydrogen atom. The nitrogen atom is protonated in such a way that the heterocycle assumes a pyridinium character. The crystal structure also contains six water molecules of crystallization. A thermogravimetric study showed that the decomposition of I occurs in several successive steps, such as dehydration, the combustion of organic ligands, and the formation of an inorganic residue.

  11. Dosimetric comparison of four new design {sup 103}Pd brachytherapy sources: Optimal design using silver and copper rod cores

    SciTech Connect

    Hosseini, S. Hamed; Sadeghi, Mahdi; Ataeinia, Vahideh

    2009-07-15

    Four new brachytherapy sources, IRA1-{sup 103}Pd, IRA2-{sup 103}Pd, IRA3-{sup 103}Pd, and IRA4-{sup 103}Pd, have been developed at Agricultural, Medical, and Industrial Research School and are designed for permanent implant application. With the goal of determining an optimal design for a {sup 103}Pd source, this article compares the dosimetric properties of these sources with reference to the authors' earlier IRA-{sup 103}Pd source. The four new sources differ in end cap configuration and thickness and in the core material, silver or copper, that carries the adsorbed {sup 103}Pd. Dosimetric data derived from the authors' Monte Carlo simulation results are reported in accordance with the updated AAPM Task Group No. 43 report (TG-43U1). For each source, the authors obtained detailed results for the dose rate constant {Lambda}, the radial dose function g(r), the anisotropy function F(r,{theta}), and the anisotropy factor {phi}{sub an}(r). In this study, the optimal source IRA3-{sup 103}Pd provides the most isotropic dose distribution in water with the dose rate constant of 0.678({+-}0.1%) cGy h{sup -1} U{sup -1}. The IRA3-{sup 103}Pd design has a silver rod core combined with thin-wall, concave end caps. Finally, the authors compared the results for their optimal source with published results for those of other source manufacturers.

  12. Preparation of the Crystal Complex of Phosphopantetheine Adenylyltransferase from Mycobacterium tuberculosis with Coenzyme A and Investigation of Its Three-Dimensional Structure at 2.1-A Resolution

    SciTech Connect

    Timofeev, V. I.; Smirnova, E. A.; Chupova, L. A.; Esipov, R. S.; Kuranova, I. P.

    2010-11-15

    Recombinant phosphopantetheine adenylyltransferase from Mycobacterium tuberculosis (PPAT Mt), which was produced by a high-producing strain and purified to 99%, was used for the crystal growth of the complex of the enzyme with coenzyme A (CoA). Crystals suitable for X-ray diffraction study were obtained by cocrystallization. The crystals belong to sp. gr. R32 and have the unit-cell parameters a = b = 98.840 A, c = 112.880 A, {alpha} = {beta} = 90.00{sup o}, and {gamma} = 120.00{sup o}. The three-dimensional structure of the complex was determined based on X-ray diffraction data collected from the crystals to 2.1 A resolution and refined to Rf = 22.7% and Rfree = 25.93%. Active-site bound coenzyme A was found, and its nearest environment was described. The conformational changes of the enzyme due to ligand binding were revealed. The binding of CoA by tuberculosis phosphopantetheine adenylyltransferase was characterized by comparing the structures of the title complex to a similar complex of PPAT from E. coli (PPAT Ec).

  13. Structural characterization of Green River oil-shale at high-pressure using pair distribution function analysis and small angle x-ray scattering.

    SciTech Connect

    Locke, D. R.; Chupas, P. J.; Chapman, K. W.; Pugmire, R. J.; Winans, R. E.; Univ. of Utah

    2008-01-01

    The compression behavior of a silicate-rich oil shale from the Green River formation in the pressure range 0.0-2.4 GPa was studied using in situ high pressure X-ray pair distribution function (PDF) measurements for the sample contained within a Paris-Edinburgh cell. The real-space local structural information in the PDF, G(r), was used to evaluate the compressibility of the oil shale. Specifically, the pressure-induced reduction in the medium- to long-range atom distances (6-20 {angstrom}) yielded an average sample compressibility corresponding to a bulk modulus of ca. 61-67 GPa. A structural model consisting of a three phase mixture of the principal crystalline oil shale components (quartz, albite and Illite) provided a good fit to the ambient pressure PDF data (R 30.7%). Indeed the features in the PDF beyond 6 {angstrom}, were similarly well fit by a single phase model of the highest symmetry, highly crystalline quartz component.

  14. High pressure pair distribution function studies of Green River oil shale.

    SciTech Connect

    Chapman, K. W.; Chupas, P. J.; Locke, D. R.; Winans, R. E.; Pugmire, R. J.; Univ. of Utah

    2008-01-01

    The compression behavior of a silicate-rich oil shale from the Green River formation in the pressure range 0.0-2.4 GPa was studied using in situ high pressure X-ray pair distribution function (PDF) measurements for the sample contained within a Paris-Edinburgh cell. The real-space local structural information in the PDF, G(r), was used to evaluate the compressibility of the oil shale. Specifically, the pressure-induced reduction in the medium- to long-range atom distances ({approx}6-20 {angstrom}) yielded an average sample compressibility corresponding to a bulk modulus of ca. 61-67 GPa. A structural model consisting of a three phase mixture of the principal crystalline oil shale components (quartz, albite and Illite) provided a good fit to the ambient pressure PDF data (R {approx} 30.7%). Indeed the features in the PDF beyond {approx} {angstrom}, were similarly well fit by a single phase model of the highest symmetry, highly crystalline quartz component. The factors influencing the observed compression behavior are discussed.

  15. One-dimensional modeling of radial heat removal during depressurized heatup transients in modular pebble-bed and prismatic high temperature gas-cooled reactors

    SciTech Connect

    Savage, M.G.

    1984-07-01

    A one-dimensional computational model was developed to evaluate the heat removal capabilities of both prismatic-core and pebble-bed modular HTGRs during depressurized heatup transients. A correlation was incorporated to calculate the temperature- and neutron-fluence-dependent thermal conductivity of graphite. The modified Zehner-Schluender model was used to determine the effective thermal conductivity of a pebble bed, accounting for both conduction and radiation. Studies were performed for prismatic-core and pebble-bed modular HTGRs, and the results were compared to analyses performed by GA and GR, respectively. For the particular modular reactor design studied, the prismatic HTGR peak temperature was 2152.2/sup 0/C at 38 hours following the transient initiation, and the pebble-bed peak temperature was 1647.8/sup 0/C at 26 hours. These results compared favorably with those of GA and GE, with only slight differences caused by neglecting axial heat transfer in a one-dimensional radial model. This study found that the magnitude of the initial power density had a greater effect on the temperature excursion than did the initial temperature.

  16. Linear temperature behavior of thermopower and strong electron-electron scattering in thick F-doped SnO{sub 2} films

    SciTech Connect

    Lang, Wen-Jing; Li, Zhi-Qing

    2014-07-28

    Both the semi-classical and quantum transport properties of F-doped SnO{sub 2} thick films (∼1 μm) were investigated experimentally. We found that the resistivity caused by the thermal phonons obeys Bloch-Grüneisen law from ∼90 to 300 K, while only the diffusive thermopower, which varies linearly with temperature from 300 down to 10 K, can be observed. The phonon-drag thermopower is completely suppressed due to the long electron-phonon relaxation time in the compound. These observations, together with the fact that the carrier concentration has negligible temperature dependence, indicate that the conduction electrons in F-doped SnO{sub 2} films possess free-electron-like characteristics. At low temperatures, the electron-electron scattering dominates over the electron-phonon scattering and governs the inelastic scattering process. The theoretical predications of scattering rates of large- and small-energy-transfer electron-electron scattering processes, which are negligibly weak in three-dimensional disordered conventional conductors, are quantitatively tested in this lower carrier concentration and free-electron-like highly degenerate semiconductor.

  17. Synthesis, characterization, crystal structure, and thermal analysis of 2-chloro-N-(1,5-dimethyl-3-oxo-2-phenyl-2,3-dihydro-1H-pyrazol-4-yl) acetamide

    SciTech Connect

    Sharma, R.; Nayak, P. S.; Narayana, B.; Kant, R.

    2015-12-15

    The title compound, C{sub 13}H{sub 14}O{sub 2}N{sub 3}Cl, has been synthesized by the reaction of chloroacetyl chloride with 4-aminoantipyrine in basic media and characterized by FT-IR, CHN elemental analysis, UV-Vis, TGA, DTA, DSC and single crystal X-ray diffraction. crystals are monoclinic, sp. gr. P2{sub 1}/c, a = 6.9994(6), b = 12.4035(13), c = 15.836(2) Å, β = 100.367(9)°, Z = 4. The crystal structure is stabilized by N–H···O and C–H···O interactions, the former interactions result in the formation of dimers corresponding to R{sub 2}{sup 2} (10) graphset motif and the dimers are further connected by C–H···O hydrogen bonding forming chains. In addition, the thermal stability of the compound was determined by TGA, DTA, DSC analysis, and absorption at λ{sub max} = 298 nm was determined by UV-Vis spectrophotometer.

  18. Study of hypervelocity projectile impact on thick metal plates

    DOE PAGES [OSTI]

    Roy, Shawoon K.; Trabia, Mohamed; O’Toole, Brendan; Hixson, Robert S.; Becker, Steven; Pena, Michael T.; Jennings, Richard; Somasoundaram, Deepak; Matthes, Melissa; Daykin, Edward P.; et al

    2016-01-01

    Hypervelocity impacts generate extreme pressure and shock waves in impacted targets that undergo severe localized deformation within a few microseconds. These impact experiments pose unique challenges in terms of obtaining accurate measurements. Similarly, simulating these experiments is not straightforward. This paper proposed an approach to experimentally measure the velocity of the back surface of an A36 steel plate impacted by a projectile. All experiments used a combination of a two-stage light-gas gun and the photonic Doppler velocimetry (PDV) technique. The experimental data were used to benchmark and verify computational studies. Two different finite-element methods were used to simulate the experiments:more » Lagrangian-based smooth particle hydrodynamics (SPH) and Eulerian-based hydrocode. Both codes used the Johnson-Cook material model and the Mie-Grüneisen equation of state. Experiments and simulations were compared based on the physical damage area and the back surface velocity. Finally, the results of this study showed that the proposed simulation approaches could be used to reduce the need for expensive experiments.« less

  19. Study of hypervelocity projectile impact on thick metal plates

    SciTech Connect

    Roy, Shawoon K.; Trabia, Mohamed; O’Toole, Brendan; Hixson, Robert S.; Becker, Steven; Pena, Michael T.; Jennings, Richard; Somasoundaram, Deepak; Matthes, Melissa; Daykin, Edward P.; Machorro, Eric

    2016-01-01

    Hypervelocity impacts generate extreme pressure and shock waves in impacted targets that undergo severe localized deformation within a few microseconds. These impact experiments pose unique challenges in terms of obtaining accurate measurements. Similarly, simulating these experiments is not straightforward. This paper proposed an approach to experimentally measure the velocity of the back surface of an A36 steel plate impacted by a projectile. All experiments used a combination of a two-stage light-gas gun and the photonic Doppler velocimetry (PDV) technique. The experimental data were used to benchmark and verify computational studies. Two different finite-element methods were used to simulate the experiments: Lagrangian-based smooth particle hydrodynamics (SPH) and Eulerian-based hydrocode. Both codes used the Johnson-Cook material model and the Mie-Grüneisen equation of state. Experiments and simulations were compared based on the physical damage area and the back surface velocity. Finally, the results of this study showed that the proposed simulation approaches could be used to reduce the need for expensive experiments.

  20. Elastic-plastic and phase transition of zinc oxide single crystal under shock compression

    SciTech Connect

    Liu, Xun; Mashimo, Tsutomu Li, Wei; Zhou, Xianming; Sekine, Toshimori

    2015-03-07

    The Hugoniot data for zinc oxide (ZnO) single crystals were measured up to 80 GPa along both the 〈112{sup ¯}0〉 (a-axis) and 〈0001〉 (c-axis) directions using a velocity interferometer system for any reflector and inclined-mirror method combined with a powder gun and two-stage light gas gun. The Hugoniot-elastic limits of ZnO were determined to be 10.5 and 11.5 GPa along the a- and c-axes, respectively. The wurtzite (B4) to rocksalt (B1) phase transition pressures along the a- and c-axes are 12.3 and 14.4 GPa, respectively. Shock velocity (U{sub s}) versus particle velocity (U{sub p}) relation of the final phase is given by the following relationship: U{sub s} (km/s) = 2.76 + 1.51U{sub p} (km/s). Based on the Debye-Grüneisen model and Birch-Murnaghan equation of state (EOS), we discuss the EOS of the B1 phase ZnO. The bulk modulus (K{sub 0}) and its pressure derivative (K{sub 0}′) are estimated to be K{sub 0} = 174 GPa and K{sub 0}′ = 3.9, respectively.

  1. Climate data, analysis and models for the study of natural variability and anthropogenic change

    SciTech Connect

    Jones, Philip D.

    2014-07-31

    grid resolution is coarse (5° by 5° lat/long) the changes in storm activity are similar to those developed from the pressure triangle approach with station data. Analyses of humidity and pressure data In Simmons et al. (2010) we showed a reduction in relative humidity over low-latitude and mid-latitude land areas for the 10 years to 2008, based on monthly anomalies of surface air temperature and humidity from ECMWF reanalyses (ERA-40 and ERA-Interim) and our earlier land-only dataset (CRUTEM3) and synoptic humidity observations (HadCRUH). Updates of this station-based humidity dataset (now called HadISDH) extend the record, showing continued reductions (Willett et al., 2013). Analyses of Proxy Temperature Data In Vinther et al. (2010), relationships between the seasonal stable isotope data from Greenland Ice Cores and Greenland and Icelandic instrumental temperatures were investigated for the past 150-200 years. The winter season stable isotope data are found to be influenced by the North Atlantic Oscillation (NAO) and very closely related to SW Greenland temperatures. The summer season stable isotope data display higher correlations with Icelandic summer temperatures and North Atlantic SST conditions than with local SW Greenland temperatures. In Jones et al. (2014) we use these winter isotope reconstructions to show the expected inverse correlation (due to the NAO) with winter-season documentary reconstructions from the Netherlands and Sweden over the last 800 years. Finally, in this section Jones et al. (2013) shows the agreement between tree-ring width measurements from Northern Sweden and Finland and an assessment of the link to explosive volcanic eruptions. An instrumental record for the region in the early 19th century indicates that the summer of 1816 was only slightly below normal, explaining why this year has normal growth for both ring width and density. GCM/RCM/Reanalysis Evaluation In this section we have intercompared daily temperature extremes across

  2. The Milky Way Tomography with SDSS. 2. Stellar Metallicity

    SciTech Connect

    Ivezic, Zeljko; Sesar, Branimir; Juric, Mario; Bond, Nicholas; Dalcanton, Julianne; Rockosi, Constance M.; Yanny, Brian; Newberg, Heidi J.; Beers, Timothy C.; Prieto, Carlos Allende; Wilhelm, Ron; /Texas Tech. /Michigan State U.

    2008-04-01

    In addition to optical photometry of unprecedented quality, the Sloan Digital Sky Survey (SDSS) is producing a massive spectroscopic database which already contains over 280,000 stellar spectra. Using effective temperature and metallicity derived from SDSS spectra for {approx}60,000 F and G type main sequence stars (0.2 < g-r < 0.6), we develop polynomial models, reminiscent of traditional methods based on the UBV photometry, for estimating these parameters from the SDSS u-g and g-r colors. These estimators reproduce SDSS spectroscopic parameters with a root-mean-square scatter of 100 K for effective temperature, and 0.2 dex for metallicity (limited by photometric errors), which are similar to random and systematic uncertainties in spectroscopic determinations. We apply this method to a photometric catalog of coadded SDSS observations and study the photometric metallicity distribution of {approx}200,000 F and G type stars observed in 300 deg{sup 2} of high Galactic latitude sky. These deeper (g < 20.5) and photometrically precise ({approx}0.01 mag) coadded data enable an accurate measurement of the unbiased metallicity distribution for a complete volume-limited sample of stars at distances between 500 pc and 8 kpc. The metallicity distribution can be exquisitely modeled using two components with a spatially varying number ratio, that correspond to disk and halo. The best-fit number ratio of the two components is consistent with that implied by the decomposition of stellar counts profiles into exponential disk and power-law halo components by Juric et al. (2008). The two components also possess the kinematics expected for disk and halo stars. The metallicity of the halo component can be modeled as a spatially invariant Gaussian distribution with a mean of [Fe/H] = -1.46 and a standard deviation of {approx}0.3 dex. The disk metallicity distribution is non-Gaussian, with a remarkably small scatter (rms {approx}0.16 dex) and the median smoothly decreasing with distance

  3. X-ray-selected galaxy groups in Boötes

    SciTech Connect

    Vajgel, Bruna; Lopes, Paulo A. A.; Jones, Christine; Forman, William R.; Murray, Stephen S.; Goulding, Andrew; Andrade-Santos, Felipe

    2014-10-10

    We present the X-ray and optical properties of the galaxy groups selected in the Chandra X-Boötes survey. We used follow-up Chandra observations to better define the group sample and their X-ray properties. Group redshifts were measured from the AGN and Galaxy Evolution Survey spectroscopic data. We used photometric data from the NOAO Deep Wide Field Survey to estimate the group richness (N {sub gals}) and the optical luminosity (L {sub opt}). Our final sample comprises 32 systems at z < 1.75 with 14 below z = 0.35. For these 14 systems, we estimate velocity dispersions (σ {sub gr}) and perform a virial analysis to obtain the radii (R {sub 200} and R {sub 500}) and total masses (M {sub 200} and M {sub 500}) for groups with at least 5 galaxy members. We use the Chandra X-ray observations to derive the X-ray luminosity (L{sub X} ). We examine the performance of the group properties σ{sub gr}, L {sub opt}, and L{sub X} , as proxies for the group mass. Understanding how well these observables measure the total mass is important to estimate how precisely the cluster/group mass function is determined. Exploring the scaling relations built with the X-Boötes sample and comparing these with samples from the literature, we find a break in the L{sub X} -M {sub 500} relation at approximately M {sub 500} = 5 × 10{sup 13} M {sub ☉} (for M {sub 500} > 5 × 10{sup 13} M {sub ☉}, M{sub 500}∝L{sub X}{sup 0.61±0.02}, while for M {sub 500} ≤ 5 × 10{sup 13} M {sub ☉}, M{sub 500}∝L{sub X}{sup 0.44±0.05}). Thus, the mass-luminosity relation for galaxy groups cannot be described by the same power law as galaxy clusters. A possible explanation for this break is the dynamical friction, tidal interactions, and projection effects that reduce the velocity dispersion values of the galaxy groups. By extending the cluster luminosity function to the group regime, we predict the number of groups that new X-ray surveys, particularly eROSITA, will detect. Based on our cluster

  4. Mixed convection heat transfer to and from a horizontal cylinder in cross-flow with heating from below.

    SciTech Connect

    Greif, Ralph (University of California, Berkeley, CA); Evans, Gregory Herbert; Kearney, Sean Patrick (Sandia National Laboratories, Albuquerque, NM); Laskowski, Gregory Michael

    2006-02-01

    Heat transfer to and from a circular cylinder in a cross-flow of water at low Reynolds number was studied both experimentally and numerically. The experiments were carried out in a high aspect ratio water channel. The test section inflow temperature and velocity, channel lower surface temperature and cylinder surface temperature were controlled to yield either laminar or turbulent flow for a desired Richardson number. When the lower surface was unheated, the temperatures of the lower surface and water upstream of the cylinder were maintained approximately equal and the flow was laminar. When the lower surface was heated, turbulence intensities as high as 20% were measured several cylinder diameters upstream of the cylinder due to turbulent thermal plumes produced by heating the lower surface. Variable property, two-dimensional simulations were undertaken using a variant of the u{sup 2}-f turbulence model with buoyancy production of turbulence accounted for by a simple gradient diffusion model. Predicted and measured heat flux distributions around the cylinder are compared for values of the Richardson number, Gr{sub d}/Re{sub d}{sup 2} from 0.3 to 9.3. For laminar flow, the predicted and measured heat flux results agreed to within the experimental uncertainty. When the lower surface was heated, and the flow was turbulent, there was qualitative agreement between predicted and measured heat flux distributions around the cylinder. However the predicted spatially averaged Nusselt number was from 37% to 53% larger than the measured spatially averaged Nusselt number. Additionally, spatially averaged Nusselt numbers are compared to correlations in the literature for mixed convection heat transfer to/from cylinders in cross-flow. The results presented here are larger than the correlation values. This is believed to be due to the effects of buoyancy-induced turbulence resulting from heating the lower surface and the proximity of the cylinder to that surface.

  5. Measurement of the scattering cross section of slow neutrons on liquid parahydrogen from neutron transmission

    SciTech Connect

    Grammer, K. B.; Alarcon, R.; Barrn-Palos, L.; Blyth, D.; Bowman, J. D.; Calarco, J.; Crawford, C.; Craycraft, K.; Evans, D.; Fomin, N.; Fry, J.; Gericke, M.; Gillis, R. C.; Greene, G. L.; Hamblen, J.; Hayes, C.; Kucuker, S.; Mahurin, R.; Maldonado-Velzquez, M.; Martin, E.; McCrea, M.; Mueller, P. E.; Musgrave, M.; Nann, H.; Penttil, S. I.; Snow, W. M.; Tang, Z.; Wilburn, W. S.

    2015-05-08

    Liquid hydrogen is a dense Bose fluid whose equilibrium properties are both calculable from first principles using various theoretical approaches and of interest for the understanding of a wide range of questions in many-body physics. Unfortunately, the pair correlation function g(r) inferred from neutron scattering measurements of the differential cross section d?/d? from different measurements reported in the literature are inconsistent. We have measured the energy dependence of the total cross section and the scattering cross section for slow neutrons with energies between 0.43 and 16.1 meV on liquid hydrogen at 15.6 K (which is dominated by the parahydrogen component) using neutron transmission measurements on the hydrogen target of the NPDGamma collaboration at the Spallation Neutron Source at Oak Ridge National Laboratory. The relationship between the neutron transmission measurement we perform and the total cross section is unambiguous, and the energy range accesses length scales where the pair correlation function is rapidly varying. At 1 meV our measurement is a factor of 3 below the data from previous work. We present evidence that these previous measurements of the hydrogen cross section, which assumed that the equilibrium value for the ratio of orthohydrogen and parahydrogen has been reached in the target liquid, were in fact contaminated with an extra nonequilibrium component of orthohydrogen. Liquid parahydrogen is also a widely used neutron moderator medium, and an accurate knowledge of its slow neutron cross section is essential for the design and optimization of intense slow neutron sources. Furthermore, we describe our measurements and compare them with previous work.

  6. A MAGELLAN MIKE AND SPITZER MIPS STUDY OF 1.5-1.0 M{sub sun} STARS IN SCORPIUS-CENTAURUS

    SciTech Connect

    Chen, Christine H.; Bitner, Martin A.; Mamajek, Eric E.; Pecaut, Mark; Su, Kate Y. L.; Weinberger, Alycia J.

    2011-09-10

    We obtained Spitzer Space Telescope Multiband Imaging Photometer for Spitzer (MIPS) 24 {mu}m and 70 {mu}m observations of 182 nearby, Hipparcos F- and G-type common proper motion single and binary systems in the nearest OB association, Scorpius-Centaurus. We also obtained Magellan/MIKE R {approx} 50,000 visual spectra at 3500-10500 A for 181 candidate ScoCen stars in single and binary systems. Combining our MIPS observations with those of other ScoCen stars in the literature, we estimate 24 {mu}m F+G-type disk fractions of 9/27 (33% {+-} 11%), 21/67 (31% {+-} 7%), and 25/71 (35% {+-} 7%) for Upper Scorpius ({approx}10 Myr), Upper Centaurus Lupus ({approx}15 Myr), and Lower Centaurus Crux ({approx}17 Myr), respectively. We confirm previous IRAS and MIPS excess detections and present new discoveries of 41 protoplanetary and debris disk systems, with fractional infrared luminosities ranging from L{sub IR}/L{sub *} = 10{sup -5} to 10{sup -2} and grain temperatures ranging from T{sub gr} = 40-300 K. We searched for an increase in 24 {mu}m excess at an age of 15-20 Myr, consistent with the onset of debris production predicted by coagulation N-body simulations of outer planetary systems. We found such an increase around 1.5 M{sub sun} stars but discovered a decrease in the 24 {mu}m excess around 1.0 M{sub sun} stars. We additionally discovered that the 24 {mu}m excess around 1.0 M{sub sun} stars is larger than predicted by self-stirred models. Finally, we found a weak anti-correlation between fractional infrared luminosity (L{sub IR}/L{sub *}) and chromospheric activity (R'{sub HK}), that may be the result of differences in stellar properties, such as mass, luminosity, and/or winds.

  7. A SPITZER MIPS STUDY OF 2.5-2.0 M{sub Sun} STARS IN SCORPIUS-CENTAURUS

    SciTech Connect

    Chen, Christine H.; Bitner, Martin; Pecaut, Mark; Mamajek, Eric E.; Su, Kate Y. L.

    2012-09-10

    We have obtained Spitzer Space Telescope Multiband Imaging Photometer for Spitzer (MIPS) 24 {mu}m and 70 {mu}m observations of 215 nearby, Hipparcos B- and A-type common proper-motion single and binary systems in the nearest OB association, Scorpius-Centaurus. Combining our MIPS observations with those of other ScoCen stars in the literature, we estimate 24 {mu}m B+A-type disk fractions of 17/67 (25{sup +6}{sub -5}%), 36/131 (27{sup +4}{sub -4}%), and 23/95 (24{sup +5}{sub -4}%) for Upper Scorpius ({approx}11 Myr), Upper Centaurus Lupus ({approx}15 Myr), and Lower Centaurus Crux ({approx}17 Myr), respectively, somewhat smaller disk fractions than previously obtained for F- and G-type members. We confirm previous IRAS excess detections and present new discoveries of 51 protoplanetary and debris disk systems, with fractional infrared luminosities ranging from L{sub IR}/L{sub *} = 10{sup -6} to 10{sup -2} and grain temperatures ranging from T{sub gr} = 40 to 300 K. In addition, we confirm that the 24 {mu}m and 70 {mu}m excesses (or fractional infrared luminosities) around B+A-type stars are smaller than those measured toward F+G-type stars and hypothesize that the observed disk property dependence on stellar mass may be the result of a higher stellar companion fraction around B- and A-type stars at 10-200 AU. Finally, we note that the majority of the ScoCen 24 {mu}m excess sources also possess 12 {mu}m excess, indicating that Earth-like planets may be forming via collisions in the terrestrial planet zone at {approx}10-100 Myr.

  8. Photochemical solar cells based on dye-sensitization of nanocrystalline TiO{sub 2}

    SciTech Connect

    Deb, S.K.; Ellingson, R.; Ferrere, S.; Frank, A.J.; Gregg, B.A.; Nozik, A.J.; Park, N.; Schlichthoerl, G.; Zaban, A.

    1999-03-01

    A photoelectrochemical solar cell that is based on the dye-sensitization of thin nanocrystalline films of TiO{sub 2} (anatase) nanoparticles in contact with a non-aqueous liquid electrolyte is described. The cell, fabricated at NREL, shows a conversion efficiency of {approximately}9.2{percent} at AM1.5, which approaches the best reported value of 10{percent}-11{percent} by Gr{umlt a}tzel at EPFL in Lausanne, Switzerland. Femtosecond (fs) pump-probe spectroscopy has been used to time resolve the injection of electrons into the conduction band of nanocrystalline TiO{sub 2} films under ambient conditions following photoexcitation of the adsorbed Ru(II)-complex dye. The measurement indicates an instrument-limited {minus}50 fs upper limit on the electron injection time. We also report the sensitization of nanocrystalline TiO{sub 2} by a novel iron-based dye. cis-[Fe{sup II}(2,2{sup {prime}}-bipyridine-4,4{sup {prime}}-dicarboxylic&hthinsp;acid){sub 2}(CN){sub 2}], a chromophore with an extremely short-lived, nonemissive excited state. The dye also exhibits a unique {open_quotes}band selective{close_quotes} sensitization through one of its two absorption bands. The operational principle of the device has been studied through the measurement of electric field distribution within the device structure and studies on the pH dependence of dye-redox potential. The incorporation of a WO{sub 3}-based electrochromic layer into this device has led to a novel photoelectrochromic device structure for {open_quotes}smart window{close_quotes} applications. {copyright} {ital 1999 American Institute of Physics.}

  9. The Physics Basis For An Advanced Physics And Advanced Technology Tokamak Power Plant Configuration, ARIES-ACT1

    SciTech Connect

    Charles Kessel, et al

    2014-03-05

    The advanced physics and advanced technology tokamak power plant ARIES-ACT1 has a major radius of 6.25 m at aspect ratio of 4.0, toroidal field of 6.0 T, strong shaping with elongation of 2.2 and triangularity of 0.63. The broadest pressure cases reached wall stabilized βN ~ 5.75, limited by n=3 external kink mode requiring a conducting shell at b/a = 0.3, and requiring plasma rotation, feedback, and or kinetic stabilization. The medium pressure peaking case reached βN = 5.28 with BT = 6.75, while the peaked pressure case reaches βN < 5.15. Fast particle MHD stability shows that the alpha particles are unstable, but this leads to redistribution to larger minor radius rather than loss from the plasma. Edge and divertor plasma modeling show that about 75% of the power to the divertor can be radiated with an ITER-like divertor geometry, while over 95% can be radiated in a stable detached mode with an orthogonal target and wide slot geometry. The bootstrap current fraction is 91% with a q95 of 4.5, requiring about ~ 1.1 MA of external current drive. This current is supplied with 5 MW of ICRF/FW and 40 MW of LHCD. EC was examined and is most effective for safety factor control over ρ ~ 0.2-0.6 with 20 MW. The pedestal density is ~ 0.9x1020 /m3 and the temperature is ~ 4.4 keV. The H98 factor is 1.65, n/nGr = 1.0, and the net power to LH threshold power is 2.8- 3.0 in the flattop.

  10. Measurement of the scattering cross section of slow neutrons on liquid parahydrogen from neutron transmission

    DOE PAGES [OSTI]

    Grammer, K. B.; Alarcon, R.; Barrón-Palos, L.; Blyth, D.; Bowman, J. D.; Calarco, J.; Crawford, C.; Craycraft, K.; Evans, D.; Fomin, N.; et al

    2015-05-08

    Liquid hydrogen is a dense Bose fluid whose equilibrium properties are both calculable from first principles using various theoretical approaches and of interest for the understanding of a wide range of questions in many-body physics. Unfortunately, the pair correlation function g(r) inferred from neutron scattering measurements of the differential cross section dσ/dΩ from different measurements reported in the literature are inconsistent. We have measured the energy dependence of the total cross section and the scattering cross section for slow neutrons with energies between 0.43 and 16.1 meV on liquid hydrogen at 15.6 K (which is dominated by the parahydrogen component)more » using neutron transmission measurements on the hydrogen target of the NPDGamma collaboration at the Spallation Neutron Source at Oak Ridge National Laboratory. The relationship between the neutron transmission measurement we perform and the total cross section is unambiguous, and the energy range accesses length scales where the pair correlation function is rapidly varying. At 1 meV our measurement is a factor of 3 below the data from previous work. We present evidence that these previous measurements of the hydrogen cross section, which assumed that the equilibrium value for the ratio of orthohydrogen and parahydrogen has been reached in the target liquid, were in fact contaminated with an extra nonequilibrium component of orthohydrogen. Liquid parahydrogen is also a widely used neutron moderator medium, and an accurate knowledge of its slow neutron cross section is essential for the design and optimization of intense slow neutron sources. Furthermore, we describe our measurements and compare them with previous work.« less

  11. Physics basis for an advanced physics and advanced technology tokamak power plant configuration: ARIES-ACT1

    DOE PAGES [OSTI]

    Kessel, C. E.; Poli, F. M.; Ghantous, K.; Gorelenkov, N. N.; Rensink, M. E.; Rognlien, T. D.; Snyder, P. B.; St. John, H.; Turnbull, A. D.

    2015-01-01

    Here, the advanced physics and advanced technology tokamak power plant ARIES-ACT1 has a major radius of 6.25 m at an aspect ratio of 4.0, toroidal field of 6.0 T, strong shaping with elongation of 2.2, and triangularity of 0.63. The broadest pressure cases reached wall-stabilized βN ~ 5.75, limited by n = 3 external kink mode requiring a conducting shell at b/a = 0.3, requiring plasma rotation, feedback, and/or kinetic stabilization. The medium pressure peaking case reaches βN = 5.28 with BT = 6.75, while the peaked pressure case reaches βN < 5.15. Fast particle magnetohydrodynamic stability shows that themore » alpha particles are unstable, but this leads to redistribution to larger minor radius rather than loss from the plasma. Edge and divertor plasma modeling shows that 75% of the power to the divertor can be radiated with an ITER-like divertor geometry, while >95% can be radiated in a stable detached mode with an orthogonal target and wide slot geometry. The bootstrap current fraction is 91% with a q95 of 4.5, requiring ~1.1 MA of external current drive. This current is supplied with 5 MW of ion cyclotron radio frequency/fast wave and 40 MW of lower hybrid current drive. Electron cyclotron is most effective for safety factor control over ρ~0.2 to 0.6 with 20 MW. The pedestal density is ~0.9×1020/m3, and the temperature is ~4.4 keV. The H98 factor is 1.65, n/nGr = 1.0, and the ratio of net power to threshold power is 2.8 to 3.0 in the flattop.« less

  12. The relationship between constraint and ductile fracture initiation as defined by micromechanical analyses

    SciTech Connect

    Panontin, T.L.; Sheppard, S.D.

    1995-12-31

    The overall objective of this study is to provide a proven methodology to allow the transfer of ductile fracture initiation properties measured in standard laboratory specimens to large, complex, flawed structures. A significant part of this work involved specifically addressing the effects of constrain on transferability under large scale yielding conditions. The approach taken was to quantify constrain effects through micromechanical fracture models coupled with finite element generated crack tip stress-strain fields to identify the local condition corresponding to fracture initiation. Detailed finite element models predicted the influence of specimen geometry, loading mode, and material flow properties on the crack tip fields. The ability of two local, ductile fracture models (the Rice and Tracey void growth model (VGM) and the stress-modified, critical strain (SMCS) criterion of Mackenzie et al. and Hancock and Cowling) to predict fracture initiation were investigated. Predictions were made using experimentally verified, two- and three-dimensional, finite strain, large deformation, finite element analyses. Two, high toughness pressure vessel steels were investigated: A516 Gr70, a ferritic, carbon-manganese mild steel demonstrating high hardening behavior, and HY-80, a martensitic, high strength low alloy (HSLA) steel possessing medium hardening ability. Experimental verification of the ductile fracture initiation predictions was performed in a variety of crack geometries possessing a range of a/w ratios from 0.15 to 0.70 and experiencing a range of load conditions from three point bending to nearly pure tension. The predicted constrain dependence of global ductile fracture parameters in the two materials is shown.

  13. 6-Thioguanine-loaded polymeric micelles deplete myeloid-derived suppressor cells and enhance the efficacy of T cell immunotherapy in tumor-bearing mice

    DOE PAGES [OSTI]

    Jeanbart, Laura; Kourtis, Iraklis C.; van der Vlies, André J.; Swartz, Melody A.; Hubbell, Jeffrey A.

    2015-05-16

    Myeloid-derived suppressor cells (MDSCs) are a heterogeneous population of immature myeloid cells that suppress effector T cell responses and can reduce the efficacy of cancer immunotherapies. We previously showed that ultra-small polymer nanoparticles efficiently drain to the lymphatics after intradermal injection and target antigen-presenting cells, including Ly6chi Ly6g₋monocytic MDSCs (Mo-MDSCs), in skin-draining lymph nodes (LNs) and spleen. Here, we developed ultra-small polymer micelles loaded with 6-thioguanine (MC-TG), a cytotoxic drug used in the treatment of myelogenous leukemia, with the aim of killing Mo-MDSCs in tumor-bearing mice and thus enhancing T cell-mediated anti-tumor responses. We found that 2 days post-injection inmore » tumor-bearing mice (B16-F10 melanoma or E.G7-OVA thymoma), MC-TG depleted Mo-MDSCs in the spleen, Ly6clo Ly6g+ granulocytic MDSCs (G-MDSCs) in the draining LNs, and Gr1int Mo-MDSCs in the tumor. In both tumor models, MC-TG decreased the numbers of circulating Mo- and G-MDSCs, as well as of Ly6chi macrophages, for up to 7 days following a single administration. MDSC depletion was dose dependent and more effective with MC-TG than with equal doses of free TG. Finally, we tested whether this MDSC-depleting strategy might enhance cancer immunotherapies in the B16-F10 melanoma model. We found that MC-TG significantly improved the efficacy of adoptively transferred, OVA-specific CD8+ T cells in melanoma cells expressing OVA. Ultimately, these findings highlight the capacity of MC-TG in depleting MDSCs in the tumor microenvironment and show promise in promoting anti-tumor immunity when used in combination with T cell immunotherapies.« less

  14. Effect of dynamic monotonic and cyclic loading on fracture behavior for Japanese carbon steel pipe STS410

    SciTech Connect

    Kinoshita, Kanji; Murayama, Kouichi; Ogata, Hiroyuki

    1997-04-01

    The fracture behavior for Japanese carbon steel pipe STS410 was examined under dynamic monotonic and cyclic loading through a research program of International Piping Integrity Research Group (EPIRG-2), in order to evaluate the strength of pipe during the seismic event The tensile test and the fracture toughness test were conducted for base metal and TIG weld metal. Three base metal pipe specimens, 1,500mm in length and 6-inch diameter sch.120, were employed for a quasi-static monotonic, a dynamic monotonic and a dynamic cyclic loading pipe fracture tests. One weld joint pipe specimen was also employed for a dynamic cyclic loading test In the dynamic cyclic loading test, the displacement was controlled as applying the fully reversed load (R=-1). The pipe specimens with a circumferential through-wall crack were subjected four point bending load at 300C in air. Japanese STS410 carbon steel pipe material was found to have high toughness under dynamic loading condition through the CT fracture toughness test. As the results of pipe fracture tests, the maximum moment to pipe fracture under dynamic monotonic and cyclic loading condition, could be estimated by plastic collapse criterion and the effect of dynamic monotonic loading and cyclic loading was a little on the maximum moment to pipe fracture of the STS410 carbon steel pipe. The STS410 carbon steel pipe seemed to be less sensitive to dynamic and cyclic loading effects than the A106Gr.B carbon steel pipe evaluated in IPIRG-1 program.

  15. Verification of Allowable Stresses In ASME Section III Subsection NH For Grade 91 Steel & Alloy 800H

    SciTech Connect

    R. W. Swindeman; M. J. Swindeman; B. W. Roberts; B. E. Thurgood; D. L. Marriott

    2007-11-30

    The database for the creep-rupture of 9Cr-1Mo-V (Grade 91) steel was collected and reviewed to determine if it met the needs for recommending time-dependent strength values, S{sub t}, for coverage in ASME Section III Subsection NH (ASME III-NH) to 650 C (1200 F) and 600,000 hours. The accumulated database included over 300 tests for 1% total strain, nearly 400 tests for tertiary creep, and nearly 1700 tests to rupture. Procedures for analyzing creep and rupture data for ASME III-NH were reviewed and compared to the procedures used to develop the current allowable stress values for Gr 91 for ASME II-D. The criteria in ASME III-NH for estimating S{sub t} included the average strength for 1% total strain for times to 600,000 hours, 80% of the minimum strength for tertiary creep for times to 600,000 hours, and 67% of the minimum rupture strength values for times to 600,000 hours. Time-temperature-stress parametric formulations were selected to correlate the data and make predictions of the long-time strength. It was found that the stress corresponding to 1% total strain and the initiation of tertiary creep were not the controlling criteria over the temperature-time range of concern. It was found that small adjustments to the current values in III-NH could be introduced but that the existing values were conservative and could be retained. The existing database was found to be adequate to extend the coverage to 600,000 hours for temperatures below 650 C (1200 F).

  16. Measurement of the scattering cross section of slow neutrons on liquid parahydrogen from neutron transmission

    SciTech Connect

    Grammer, K. B.; Alarcon, R.; Barrón-Palos, L.; Blyth, D.; Bowman, J. D.; Calarco, J.; Crawford, C.; Craycraft, K.; Evans, D.; Fomin, N.; Fry, J.; Gericke, M.; Gillis, R. C.; Greene, G. L.; Hamblen, J.; Hayes, C.; Kucuker, S.; Mahurin, R.; Maldonado-Velázquez, M.; Martin, E.; McCrea, M.; Mueller, P. E.; Musgrave, M.; Nann, H.; Penttilä, S. I.; Snow, W. M.; Tang, Z.; Wilburn, W. S.

    2015-05-08

    Liquid hydrogen is a dense Bose fluid whose equilibrium properties are both calculable from first principles using various theoretical approaches and of interest for the understanding of a wide range of questions in many-body physics. Unfortunately, the pair correlation function g(r) inferred from neutron scattering measurements of the differential cross section dσ/dΩ from different measurements reported in the literature are inconsistent. We have measured the energy dependence of the total cross section and the scattering cross section for slow neutrons with energies between 0.43 and 16.1 meV on liquid hydrogen at 15.6 K (which is dominated by the parahydrogen component) using neutron transmission measurements on the hydrogen target of the NPDGamma collaboration at the Spallation Neutron Source at Oak Ridge National Laboratory. The relationship between the neutron transmission measurement we perform and the total cross section is unambiguous, and the energy range accesses length scales where the pair correlation function is rapidly varying. At 1 meV our measurement is a factor of 3 below the data from previous work. We present evidence that these previous measurements of the hydrogen cross section, which assumed that the equilibrium value for the ratio of orthohydrogen and parahydrogen has been reached in the target liquid, were in fact contaminated with an extra nonequilibrium component of orthohydrogen. Liquid parahydrogen is also a widely used neutron moderator medium, and an accurate knowledge of its slow neutron cross section is essential for the design and optimization of intense slow neutron sources. Furthermore, we describe our measurements and compare them with previous work.

  17. The Arctic as a test case for an assessment of climate impacts on national security.

    SciTech Connect

    Taylor, Mark A.; Zak, Bernard Daniel; Backus, George A.; Ivey, Mark D.; Boslough, Mark Bruce Elrick

    2008-11-01

    organizations. Because changes in the Arctic environment are happening so rapidly, a successful program will be one that can adapt very quickly to new information as it becomes available, and can provide decision makers with projections on the 1-5 year time scale over which the most disruptive, high-consequence changes are likely to occur. The greatest short-term impact would be to initiate exploratory simulations to discover new emergent and robust phenomena associated with one or more of the following changing systems: Arctic hydrological cycle, sea ice extent, ocean and atmospheric circulation, permafrost deterioration, carbon mobilization, Greenland ice sheet stability, and coastal erosion. Sandia can also contribute to new technology solutions for improved observations in the Arctic, which is currently a data-sparse region. Sensitivity analyses have the potential to identify thresholds which would enable the collaborative development of 'early warning' sensor systems to seek predicted phenomena that might be precursory to major, high-consequence changes. Much of this work will require improved regional climate models and advanced computing capabilities. Socio-economic modeling tools can help define human and national security consequences. Formal uncertainty quantification must be an integral part of any results that emerge from this work.

  18. Phase 1A Final Report for the AREVA Team Enhanced Accident Tolerant Fuels Concepts

    SciTech Connect

    Morrell, Mike E.

    2015-03-19

    plants large scale investment by the fuel vendors is difficult to justify. Specific EATF enhancements considered by the AREVA team were; Improved performance in DB and BDB conditions; Reduced release to the environment in a catastrophic accident; Improved performance during normal operating conditions; Improved performance if US reactors start to load follow; Equal or improved economics of the fuel; and Improvements to the fuel behavior to support future transportation and storage of the used nuclear fuel (UNF). In pursuit of the above enhancements, EATF technology concepts that our team considered were; Additives to the fuel pellets which included; Chromia doping to increase fission gas retention. Chromia doping has the potential to improve load following characteristics, improve performance of the fuel pellet during clad failure, and potentially lock up cesium into the fuel matrix; Silicon Carbide (SiC) Fibers to improve thermal heat transfer in normal operating conditions which also improves margin in accident conditions and the potential to lock up iodine into the fuel matrix; Nano-diamond particles to enhance thermal conductivity; Coatings on the fuel cladding; and Nine coatings on the existing Zircaloy cladding to increase coping time and reduce clad oxidation and hydrogen generation during accident conditions, as well as reduce hydrogen pickup and mitigate hydride reorientation in the cladding. To facilitate the development process AREVA adopted a formal “Gate Review Process” (GR) that was used to review results and focus resources onto promising technologies to reduce costs and identify the technologies that would potentially be carried forward to LFAs within a 10 year period. During the initial discovery phase of the project AREVA took the decision to be relatively hands off and allow our university and National Laboratory partners to be free thinking and consider options that would not be constrained by preconceived ideas from the fuel vendor. To counter

  19. A first class constraint generates not a gauge transformation, but a bad physical change: The case of electromagnetism

    SciTech Connect

    Pitts, J. Brian

    2014-12-15

    . Clarity about Hamiltonian electromagnetism will be useful for an analogous treatment of GR. - Highlights: A first-class constraint changes the electric field E, spoiling Gausss law. A first-class constraint does not leave the action invariant or preserve q,0?dH/dp. The gauge generator preserves E,q,0?dH/dp, and the canonical action. The error in proofs that first-class primaries generating gauge is shown. Diracs conjecture about secondary first-class constraints is blocked.

  20. Single-Step Ironmaking from Ore to Improve Energy Efficiency

    SciTech Connect

    S.K. Kawatra; B. Anamerie; T.C. Eisele

    2005-10-01

    production of pig iron nuggets was determined. It was determined that pig iron nuggets produced had a high apparent density (6.7-7.2 gr/cm3), highly metallized, slag free structure, high iron content (95-97%), high microhardness values (> 325 HVN) and microstructure similar to white cast iron. These properties made them a competitive alternative to blast furnace pig iron.

  1. Signals from the Noise: Image Stacking for Quasars in the FIRST Survey

    SciTech Connect

    White, R L; Helfand, D J; Becker, R H; Glikman, E; deVries, W

    2006-05-05

    We present a technique to explore the radio sky into the nanoJansky regime by employing image stacking using the FIRST radio sky survey. We begin with a discussion of the non-intuitive relationship between the mean and median values of a non-Gaussian distribution in which measurements of the members of the distribution are dominated by noise. Following a detailed examination of the systematic effects present in the 20 cm VLA snapshot images that comprise FIRST, we demonstrate that image stacking allows us to recover the average properties of source populations with flux densities a factor of 30 or more below the rms noise level. With the calibration described herein, mean estimates of radio flux density, luminosity, radio loudness, etc. are derivable for any undetected source class having arcsecond positional accuracy. We demonstrate the utility of this technique by exploring the radio properties of quasars found in the Sloan Digital Sky Survey. We compute the mean luminosities and radio-loudness parameters for 41,295 quasars in the SDSS DR3 catalog. There is a tight correlation between optical and radio luminosity, with the radio luminosity increasing as the 0.72 power of optical luminosity. This implies declining radio-loudness with optical luminosity, with the most luminous objects (M{sub UV} = -30) having on average ten times lower radio-to-optical ratios than the least luminous objects (M{sub UV} = -21). There is also a striking correlation between optical color and radio loudness: quasars that are either redder or bluer than the norm are brighter radio sources. Quasars having g-r {approx} 0.8 magnitudes redder than the SDSS composite spectrum are found to have radio-loudness ratios that are higher by a factor of 8. We examine the radio properties of the subsample of quasars with broad absorption lines, finding, surprisingly, that BAL quasars have higher mean radio flux densities at all redshifts, with the greatest disparity arising in the rare low

  2. Crystal structures and luminescence properties of novel compounds K{sub 4}M{sub 2}[Al{sub 2}Si{sub 8}O{sub 24}] (M = Ce, Gd)

    SciTech Connect

    Aksenov, S. M., E-mail: aks.crys@gmail.com [Russian Academy of Sciences, Shubnikov Institute of Crystallography (Russian Federation); Rassulov, V. A. [Russian Academy of Sciences, Fedorovsky All-Russian Research Institute of Mineral Resources (Russian Federation)] [Russian Academy of Sciences, Fedorovsky All-Russian Research Institute of Mineral Resources (Russian Federation); Rastsvetaeva, R. K. [Russian Academy of Sciences, Shubnikov Institute of Crystallography (Russian Federation)] [Russian Academy of Sciences, Shubnikov Institute of Crystallography (Russian Federation); Taroev, V. K. [Russian Academy of Sciences, Institute of Geochemistry, Siberian Branch (Russian Federation)] [Russian Academy of Sciences, Institute of Geochemistry, Siberian Branch (Russian Federation)

    2013-11-15

    Two novel potassium rare earth silicates, obtained by hydrothermal synthesis, have been investigated by X-ray diffraction and described by the general formula K{sub 4}M{sub 2}[Al{sub 2}Si{sub 8}O{sub 24}] (M = Ce, Gd). The parameters of the monoclinic K{sub 4}Ce{sub 2}[Al{sub 2}Si{sub 8}O{sub 24}] and K{sub 4}Gd{sub 2}[Al{sub 2}Si{sub 8}O{sub 24}] cells are, respectively, as follows: a = 26.867(1), 26.6520(2) A; b = 7.4150(2), 7.2854(1) A; c = 14.910(1), 14.8182(1) A; {beta} = 123.52(1) Degree-Sign , 123.46(1) Degree-Sign ; and sp. gr. P2{sub 1}/n. The structures are solved by the charge flipping method and refined in the anisotropic approximation of thermal vibrations for atoms to R = 5.2 and 2.5%, respectively. The compounds under study are crystallized into a new structural type, which is based on two-level [Al{sub 2}Si{sub 8}O{sub 24}] layers, combined into a three-dimensional framework by columns of edge-sharing seven-vertex REE polyhedra. Potassium atoms are located in the framework channels. The spectral luminescence characteristics are determined. The luminescence bands are typical of Gd{sup 3+} and Ce{sup 3+} ions. Upon excitation by light with {lambda}{sub exc} = 246 nm, a band due to the {sup 2}D {yields} {sup 8}F{sub 5/2} transition with {lambda}{sub max} = 430 nm is observed in the spectrum of K{sub 4}Ce{sub 2}[Al{sub 2}Si{sub 8}O{sub 24}] and a band related to the {sup 6}P{sub 7/2} {yields} {sup 8}S{sub 7/2} transition with {lambda}{sub max} = 311 nm is observed in the spectrum of K{sub 4}Gd{sub 2}[Al{sub 2}Si{sub 8}O{sub 24}].

  3. 6-Thioguanine-loaded polymeric micelles deplete myeloid-derived suppressor cells and enhance the efficacy of T cell immunotherapy in tumor-bearing mice

    SciTech Connect

    Jeanbart, Laura; Kourtis, Iraklis C.; van der Vlies, André J.; Swartz, Melody A.; Hubbell, Jeffrey A.

    2015-05-16

    Myeloid-derived suppressor cells (MDSCs) are a heterogeneous population of immature myeloid cells that suppress effector T cell responses and can reduce the efficacy of cancer immunotherapies. We previously showed that ultra-small polymer nanoparticles efficiently drain to the lymphatics after intradermal injection and target antigen-presenting cells, including Ly6chi Ly6gmonocytic MDSCs (Mo-MDSCs), in skin-draining lymph nodes (LNs) and spleen. Here, we developed ultra-small polymer micelles loaded with 6-thioguanine (MC-TG), a cytotoxic drug used in the treatment of myelogenous leukemia, with the aim of killing Mo-MDSCs in tumor-bearing mice and thus enhancing T cell-mediated anti-tumor responses. We found that 2 days post-injection in tumor-bearing mice (B16-F10 melanoma or E.G7-OVA thymoma), MC-TG depleted Mo-MDSCs in the spleen, Ly6clo Ly6g+ granulocytic MDSCs (G-MDSCs) in the draining LNs, and Gr1int Mo-MDSCs in the tumor. In both tumor models, MC-TG decreased the numbers of circulating Mo- and G-MDSCs, as well as of Ly6chi macrophages, for up to 7 days following a single administration. MDSC depletion was dose dependent and more effective with MC-TG than with equal doses of free TG. Finally, we tested whether this MDSC-depleting strategy might enhance cancer immunotherapies in the B16-F10 melanoma model. We found that MC-TG significantly improved the efficacy of adoptively transferred, OVA-specific CD8+ T cells in melanoma cells expressing OVA. Ultimately, these findings highlight the capacity of MC-TG in depleting MDSCs in the tumor microenvironment and show promise in promoting anti-tumor immunity when used in combination with T cell immunotherapies.

  4. Prenatal cadmium exposure produces persistent changes to thymus and spleen cell phenotypic repertoire as well as the acquired immune response

    SciTech Connect

    Holskov, Ida; Elliott, Meenal; Hanson, Miranda L.; Schafer, Rosana [Department of Microbiology, Immunology and Cell Biology, West Virginia University School of Medicine, Morgantown, WV 26506 (United States)] [Department of Microbiology, Immunology and Cell Biology, West Virginia University School of Medicine, Morgantown, WV 26506 (United States); Barnett, John B., E-mail: jbarnett@hsc.wvu.edu [Department of Microbiology, Immunology and Cell Biology, West Virginia University School of Medicine, Morgantown, WV 26506 (United States); Mary Babb Randolph Cancer Center, West Virginia University School of Medicine, Morgantown, WV 26506 (United States)

    2012-12-01

    Cadmium (Cd) is a common environmental contaminant. Adult exposure to Cd alters the immune system, however, there are limited studies on the effects of prenatal exposure to Cd. Pregnant C57Bl/6 mice were exposed to an environmentally relevant dose of CdCl{sub 2} (10 ppm) and the effects on the immune system of the offspring were assessed at 20 weeks of age. Prenatal Cd exposure caused an increase in the percent of CD4{sup ?}CD8{sup ?}CD44{sup +}CD25{sup ?} (DN1) thymocytes in both sexes and a decrease in the percent of CD4{sup ?}CD8{sup ?}CD44{sup ?}CD25{sup +} (DN3) thymocytes in females. Females had an increase in the percent of splenic CD4{sup +} T cells, CD8{sup +} T cells, and CD45R/B220{sup +} B cells and a decrease in the percent of NK cells and granulocytes (Gr-1{sup +}). Males had an increase in the percent of splenic CD4{sup +} T cells and CD45R/B220{sup +} B cells and a decrease in the percent of CD8{sup +} T cells, NK cells, and granulocytes. The percentage of neutrophils and myeloid-derived suppressor cells were reduced in both sexes. The percent of splenic nTreg cells was decreased in all Cd-exposed offspring. Cd-exposed offspring were immunized with a streptococcal vaccine and the antibody response was determined. PC-specific serum antibody titers were decreased in Cd exposed female offspring but increased in the males. PspA-specific serum IgG titers were increased in both females and males compared to control animals. Females had a decrease in PspA-specific serum IgM antibody titers. Females and males had a decrease in the number of splenic anti-PspA antibody-secreting cells when standardized to the number of B cells. These findings demonstrate that very low levels of Cd exposure during gestation can result in long term sex-specific alterations on the immune system of the offspring. -- Highlights: ? Prenatal exposure to cadmium alters the immune system of 20 week old offspring. ? The percentage of DN1 and DN3 thymocytes was changed. ? Males and

  5. Engineered Nano-scale Ceramic Supports for PEM Fuel Cells. Tech Team Meeting Presentaion

    SciTech Connect

    Brosha, Eric L.; Elbaz Alon, Lior; Henson, Neil J.; Rockward, Tommy; Roy, Aaron; Serov, Alexey; Ward, Timothy

    2012-08-13

    Catalyst support durability is currently a technical barrier for commercialization of polymer electrolyte membrane (PEM) fuel cells, especially for transportation applications. Degradation and corrosion of the conventional carbon supports leads to losses in active catalyst surface area and, consequently, reduced performance. As a result, the goal of this work is to develop support materials that interact strongly with Pt, yet sustain bulk-like catalytic activities with very highly dispersed particles. Ceramic materials that are prepared using conventional solid-state methods have large grain sizes and low surface areas that can only be minimally ameliorated through grinding and ball milling. Other synthesis routes to produce ceramic materials must be investigated and utilized in order to obtain desired surface areas. In this work, several different synthesis methods are being utilized to prepare electronically conductive ceramic boride, nitride, and oxide materials with high surface areas and have the potential for use as PEMFC catalyst supports. Polymer-assisted deposition (PAD) and aerosol-through plasma (A-T-P) torch are among several methods used to obtain ceramic materials with surface areas that are equal to, or exceed Vulcan XC-72R supports. Cubic Mo-based ceramic phases have been prepared with average XRD-determined crystallite sizes as low as 1.6 nm (from full profile, XRD fitting) and a BET surface area exceeding 200 m{sup 2}/g. Additionally, black, sub-stoichiometric TiO{sub 2-x}, have been prepared with an average crystallite size in the 4 nm range and surface areas exceeding 250 m{sup 2}/gr. Pt disposition using an incipient wetness approach produced materials with activity for hydrogen redox reactions and ORR. Cyclic voltammetry data will be shown for a variety of potential Pt/ceramic catalysts. Initial experiments indicate enhanced Pt metal-support interactions as well. Plane wave periodic density functional calculations (VASP) are being used to

  6. Metformin suppresses CYP1A1 and CYP1B1 expression in breast cancer cells by down-regulating aryl hydrocarbon receptor expression

    SciTech Connect

    Do, Minh Truong; Kim, Hyung Gyun; Tran, Thi Thu Phuong; Khanal, Tilak; Choi, Jae Ho; Chung, Young Chul; Jeong, Tae Cheon; Jeong, Hye Gwang

    2014-10-01

    Induction of cytochrome P450 (CYP) 1A1 and CYP1B1 by environmental xenobiotic chemicals or endogenous ligands through the activation of the aryl hydrocarbon receptor (AhR) has been implicated in a variety of cellular processes related to cancer, such as transformation and tumorigenesis. Here, we investigated the effects of the anti-diabetes drug metformin on expression of CYP1A1 and CYP1B1 in breast cancer cells under constitutive and inducible conditions. Our results indicated that metformin down-regulated the expression of CYP1A1 and CYP1B1 in breast cancer cells under constitutive and 2,3,7,8-tetrachlorodibenzo-p-dioxin (TCDD)-induced conditions. Down-regulation of AhR expression was required for metformin-mediated decreases in CYP1A1 and CYP1B1 expression, and the metformin-mediated CYP1A1 and CYP1B1 reduction is irrelevant to estrogen receptor α (ERα) signaling. Furthermore, we found that metformin markedly down-regulated Sp1 protein levels in breast cancer cells. The use of genetic and pharmacological tools revealed that metformin-mediated down-regulation of AhR expression was mediated through the reduction of Sp1 protein. Metformin inhibited endogenous AhR ligand-induced CYP1A1 and CYP1B1 expression by suppressing tryptophan-2,3-dioxygenase (TDO) expression in MCF-7 cells. Finally, metformin inhibits TDO expression through a down-regulation of Sp1 and glucocorticoid receptor (GR) protein levels. Our findings demonstrate that metformin reduces CYP1A1 and CYP1B1 expression in breast cancer cells by down-regulating AhR signaling. Metformin would be able to act as a potential chemopreventive agent against CYP1A1 and CYP1B1-mediated carcinogenesis and development of cancer. - Graphical abstract: Schematic of the CYP1A1 and CYP1B1 gene regulation by metformin. - Highlights: • Metformin inhibits CYP1A1 and CYP1B1 expression. • Metformin down-regulates the AhR signaling. • Metformin reduces Sp1 protein expression. • Metformin suppresses TDO expression.

  7. ADVANCED GASIFICATION MERCURY/TRACE METAL CONTROL WITH MONOLITH TRAPS

    SciTech Connect

    Mark A. Musich; Michael L. Swanson; Grant E. Dunham; Joshua J. Stanislowski

    2010-07-31

    Two Corning monoliths and a non-carbon-based material have been identified as potential additives for mercury capture in syngas at temperatures above 400F and pressure of 600 psig. A new Corning monolith formulation, GR-F1-2189, described as an active sample appeared to be the best monolith tested to date. The Corning SR Liquid monolith concept continues to be a strong candidate for mercury capture. Both monolith types allowed mercury reduction to below 5-?g/m3 (~5 ppb), a current U.S. Department of Energy (DOE) goal for trace metal control. Preparation methods for formulating the SR Liquid monolith impacted the ability of the monolith to capture mercury. The Energy & Environmental Research Center (EERC)-prepared Noncarbon Sorbents 1 and 2 appeared to offer potential for sustained and significant reduction of mercury concentration in the simulated fuel gas. The Noncarbon Sorbent 1 allowed sustained mercury reduction to below 5-?g/m3 (~5 ppb). The non-carbon-based sorbent appeared to offer the potential for regeneration, that is, desorption of mercury by temperature swing (using nitrogen and steam at temperatures above where adsorption takes place). A Corning cordierite monolith treated with a Group IB metal offered limited potential as a mercury sorbent. However, a Corning carbon-based monolith containing prereduced metallic species similar to those found on the noncarbon sorbents did not exhibit significant or sustained mercury reduction. EERC sorbents prepared with Group IB and IIB selenide appeared to have some promise for mercury capture. Unfortunately, these sorbents also released Se, as was evidenced by the measurement of H2Se in the effluent gas. All sorbents tested with arsine or hydrogen selenide, including Corning monoliths and the Group IB and IIB metal-based materials, showed an ability to capture arsine or hydrogen selenide at 400F and 600 psig. Based on current testing, the noncarbon metal-based sorbents appear to be the most effective arsine and

  8. IMPLEMENTING A NOVEL CYCLIC CO2 FLOOD IN PALEOZOIC REEFS

    SciTech Connect

    James R. Wood; W. quinlan; A. Wylie

    2006-06-01

    heterogeneity and compartmentalization in these reservoirs associated with the original depositional fabric and pore types of the carbonate reservoir rocks. Accumulated pressure data supports the hypothesis of extreme heterogeneity in the Dover 35. Some intervals now have pressure readings over 2345 psig (April 29, 2005) in the A-1 Carbonate while nearby Niagaran Brown intervals only show 1030 psig (March 7, 2005). This is a pressure differential over 1300 psig and suggests significant vertical barriers in the reef, consistent with the GR tomography modeling. Digital and hard copy data have been compiled for the Niagaran reefs in the Michigan Basin, including a detailed summary of 20 fields in the vicinity of the demonstration well. Technology transfer took place through technical presentations regarding visualization of the reservoir heterogeneity in these Niagaran reefs. Oral presentations were given at two Petroleum Technology Transfer Council workshops, a Michigan Oil and Gas Association Conference, a Michigan Basin Geological Society meeting, and the Eastern American Association of Petroleum Geologist's Annual meeting. In addition, we met with our industry partners several times during the first half of 2005 to communicate and discuss the reservoir characterization and field site aspects of the demonstration project. A technical paper was published in the April 2005 issue of the AAPG Bulletin on the characterization of the Belle River Mills Field.

  9. Implementing A Novel Cyclic CO2 Flood In Paleozoic Reefs

    SciTech Connect

    James R. Wood; W. Quinlan; A. Wylie

    2005-03-31

    heterogeneity and compartmentalization in these reservoirs associated with the original depositional fabric and pore types of the carbonate reservoir rocks. Accumulated pressure data supports the hypothesis of extreme heterogeneity in the Dover 35. Some intervals now have pressure readings over 2345 psig (April 29, 2005) in the A-1 Carbonate while nearby Niagaran Brown intervals only show 1030 psig (March 7, 2005). This is a pressure differential over 1300 psig and suggests significant vertical barriers in the reef, consistent with the GR tomography modeling Digital and hard copy data continue to be compiled for the Niagaran reefs in the Michigan Basin. Technology transfer took place through technical presentations regarding visualization of the reservoir heterogeneity in these Niagaran reefs. Oral presentations were given at two Petroleum Technology Transfer Council workshops, a Michigan Oil and Gas Association Conference, a Michigan Basin Geological Society meeting, and the Eastern American Association of Petroleum Geologist's Annual meeting. In addition, we met with our industry partners several times during the first half of 2005 to communicate and discuss the reservoir characterization and field site aspects of the demonstration project. A technical paper was published in the April 2005 issue of the AAPG Bulletin on the characterization of the Belle River Mills Field.

  10. Liquid Salts as Media for Process Heat Transfer from VHTR's: Forced Convective Channel Flow Thermal Hydraulics, Materials, and Coating

    SciTech Connect

    Sridharan, Kumar; Anderson, Mark; Allen, Todd; Corradini, Michael

    2012-01-30

    .083 channel, the experimental heat transfer coefficient was shown to agree with values obtained from heat transfer correlations used for water. In the 0.370 D channel, the experimental heat transfer coefficient data was predictable by either a correlation for mixed convection, or forced convection depending on the value of Gr*/Re. These experiments provided new insights into the construction and operation of molten salt flow systems. The selection of multi-component salts for molten salt flow systems requires knowledge of properties such as melting point, heat capacity, density, and viscosity of these salts. Theoretical models have been developed for the prediction of these properties of multi-component salts.

  11. INTEGRATED GENOME-BASED STUDIES OF SHEWANELLA ECOPHYSIOLOGY

    SciTech Connect

    NEALSON, KENNETH H.

    2013-10-15

    products of dissimilatory iron reduction. Geochim. Cosmochim. Acta. 74:574-583. 10. Karpinets, T.V., A.Y Obraztsova, Y. Wang, D.D. Schmoyer, G.H. Kora, B.H. Park, M.H. Serres, M.F. Ropmine, M.L. Land, T.B. Kothe, J.K. Fredrickson, K.H. Nealson, and E.C. Uberbacher 2010. Conserved synteny at the protein family level reveals genes underlying Shewanella species? cold tolerance and predicts their novel phenotypes. Funct. Integr. Genomics 10: 97 ? 110. (DOI 10.1007/s10143-009-0142-y) 11. Bretschger, O., A.C.M. Cheung, F. Mansfeld, and K.H. Nealson. 2010. Comparative microbial fuel cell evaluations of Shewanella spp. Electroanalysis 22: 883-894. 12. McLean, J.S., G. Wanger, Y.A. Gorby, M. Wainstein, J. McQuaid, Shun?ichi Ishii, O. Bretschger, H. Beyanal, K.H. Nealson. 2010. Quantification of electron transfer rates to a solid phase electron acceptor through the stages of biofilm formation from single cells to multicellular communities. Env. Sci. Technol. 44:2721-2717. 13. El-Naggar, M., G. Wanger, K.M. Leung, T.D. Yuzvinsky, G. Southam, J. Yang, W.M. Lau, K.H. Nealson, and Y.A. Gorby. 2010. Electrical Transport Along Bacterial Nanowires from Shewanella oneidensis MR-1 Proc. Nat. Acad. Sci. USA 107:18127-18131. 14. Biffinger, J.C., L.A. Fitzgerald, R. Ray, B.J. Little, S.E. Lizewski, E.R. Petersen, B.R. Ringeisen, W.C. Sanders, P.E. Sheehan, J.J. Pietron, J.W. Baldwin, L.J. Nadeau, G.R. Johnson, M. Ribbens, S.E. Finkel, K.H. Nealson. 2010. The utility of Shewanella japonica for microbial fuel cells. Bioresource Technol. 102:290-297. 15. Rodionov, D. , C. Yang, X. Li, I. Rodionova, Y. Wang, A.Y. Obraztsova, O. P. Zagnitko, R. Overbeek, M. F. Romine, S. Reed, J.K. Fredrickson, K.H. Nealson, A.L. Osterman. 2010. Genomic encyclopedia of sugar utilization pathways in the Shewanella genus. BMC Genomics 2010, 11:494 16. Kan, J., L. Hsu, A.C.M. Cheung, M. Pirbazari, and K.H. Nealson. 2011. Current production by bacterial communities in microbial fuel cells enriched from wastewater sludge

  12. 11,23,1,1,,19,10,"BANGOR HYDRO ELECTRIC CO","ELLSWORTH",0,,1179,"0A",1294,,,95,2941,0,0,3518,0,0,4870,0,0,1732,0,0,3252,0,0,2193,0,0,134,0,0,447,0,0,465,0,0,538,0,0,4295,0,0,3601,0,0,1469,6,50159,"WAT","HY"

    Energy Information Administration (EIA) (indexed site)

    NAD_UTIL","FILLER","EFFDATE","STATUS","MULTIST","YEAR","GEN01","CON01","STK01","GEN02","CON02","STK02","GEN03","CON03","STK03","GEN04","CON04","STK04","GEN05","CON05","STK05","GEN06","CON06","STK06","GEN07","CON07","STK07","GEN08","CON08","STK08","GEN09","CON09","STK09","GEN10","CON10","STK10","GEN11","CON11","STK11","GEN12","CON12","STK12","PCODE","NERC","UTILCODE","FUELDESC","PMDESC" 11,23,1,1,,19,10,"BANGOR HYDRO ELECTRIC CO","ELLSWORTH",0,,1179,"0A",1294,,,95,2941,0,0,3518,0,0,4870,0,0,1732,0,0,3252,0,0,2193,0,0,134,0,0,447,0,0,465,0,0,538,0,0,4295,0,0,3601,0,0,1469,6,50159,"WAT","HY" 11,23,1,1,,19,15,"BANGOR HYDRO ELECTRIC CO","HOWLAND",0,,1179,"0A",1294,,,95,772,0,0,858,0,0,1012,0,0,727,0,0,1061,0,0,917,0,0,385,0,0,118,0,0,0,0,0,657,0,0,905,0,0,820,0,0,1472,6,50159,"WAT","HY" 11,23,1,1,,19,30,"BANGOR HYDRO ELECTRIC CO","MEDWAY",0,,1179,"0A",1294,,,95,2116,0,0,1715,0,0,1459,0,0,1821,0,0,1946,0,0,2134,0,0,2157,0,0,1797,0,0,1745,0,0,1829,0,0,2224,0,0,2386,0,0,1474,6,50159,"WAT","HY" 11,23,1,3,2,19,30,"BANGOR HYDRO ELECTRIC CO","MEDWAY",0,"LIGHT OIL",1179,"0A",1294,,,95,0,0,553,181,307,419,0,0,593,31,55,538,66,120,418,219,399,383,324,598,481,313,579,614,97,178,575,1,2,573,0,0,608,98,171,611,1474,6,50159,"FO2","IC" 11,23,1,1,,19,35,"BANGOR HYDRO ELECTRIC CO","MILFORD",0,,1179,"0A",1294,,,95,3843,0,0,3348,0,0,4177,0,0,3759,0,0,4855,0,0,4740,0,0,2971,0,0,2432,0,0,1786,0,0,1561,0,0,3510,0,0,4606,0,0,1475,6,50159,"WAT","HY" 11,23,1,1,,19,45,"BANGOR HYDRO ELECTRIC CO","ORONO",0,,1179,"0A",1294,,,95,895,0,0,836,0,0,966,0,0,576,0,0,624,0,0,736,0,0,684,0,0,464,0,0,408,0,0,616,0,0,849,0,0,896,0,0,1476,6,50159,"WAT","HY" 11,23,1,1,,19,55,"BANGOR HYDRO ELECTRIC CO","STILLWATER",0,,1179,"0A",1294,,,95,1191,0,0,844,0,0,939,0,0,1021,0,0,1114,0,0,1181,0,0,1170,0,0,878,0,0,818,0,0,880,0,0,923,0,0,950,0,0,1478,6,50159,"WAT","HY" 11,23,1,1,,19,60,"BANGOR HYDRO ELECTRIC CO","VEAZIE A",0,,1179,"0A",1294,,,95,4314,0,0,3855,0,0,5043,0,0,5153,0,0,6053,0,0,5342,0,0,3542,0,0,2651,0,0,2281,0,0,3932,0,0,5128,0,0,3842,0,0,1479,6,50159,"WAT","HY" 11,23,1,1,,19,62,"BANGOR HYDRO ELECTRIC CO","VEAZIE B",0,,1179,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,7199,6,50159,"WAT","HY" 11,23,1,3,2,19,68,"BANGOR HYDRO ELECTRIC CO","BAR HARBOR",0,"LIGHT OIL",1179,"0A",1294,,,95,42,73,538,379,659,574,0,0,574,73,128,446,69,125,512,225,420,440,312,579,556,449,813,455,32,60,586,49,89,497,6,10,487,152,264,571,1466,6,50159,"FO2","IC" 11,23,1,3,2,19,75,"BANGOR HYDRO ELECTRIC CO","EASTPORT",0,"LIGHT OIL",1179,"0A",1294,,,95,39,70,576,80,139,412,0,0,586,10,18,557,32,58,494,111,204,464,172,317,495,182,334,509,19,36,472,0,0,470,15,29,429,67,117,460,1468,6,50159,"FO2","IC" 11,23,1,1,,37,5,"CENTRAL MAINE POWER CO","ANDROSCOG 3",0,,3266,"0M",1294,,,95,2536,0,0,2573,0,0,2732,0,0,2703,0,0,2639,0,0,2235,0,0,2379,0,0,2201,0,0,1657,0,0,2352,0,0,2282,0,0,2805,0,0,1480,6,50491,"WAT","HY" 11,23,1,1,,37,10,"CENTRAL MAINE POWER CO","BAR MILLS",0,,3266,"0M",1294,,,95,2420,0,0,1389,0,0,2414,0,0,2364,0,0,2584,0,0,1195,0,0,623,0,0,586,0,0,293,0,0,1310,0,0,2401,0,0,2056,0,0,1481,6,50491,"WAT","HY" 11,23,1,1,,37,20,"CENTRAL MAINE POWER CO","BONNY EAGLE",0,,3266,"0M",1294,,,95,6041,0,0,3654,0,0,5858,0,0,5255,0,0,4575,0,0,2217,0,0,1233,0,0,1084,0,0,592,0,0,3323,0,0,7098,0,0,4100,0,0,1482,6,50491,"WAT","HY" 11,23,1,1,,37,40,"CENTRAL MAINE POWER CO","CATARACT",0,,3266,"0M",1294,,,95,5330,0,0,4194,0,0,4953,0,0,4656,0,0,4888,0,0,5331,0,0,818,0,0,662,0,0,102,0,0,2232,0,0,5064,0,0,4090,0,0,1486,6,50491,"WAT","HY" 11,23,1,1,,37,42,"CENTRAL MAINE POWER CO","CONTINENTAL",0,,3266,"0M",1294,,,95,-14,0,0,-15,0,0,322,0,0,72,0,0,147,0,0,12,0,0,3,0,0,13,0,0,15,0,0,109,0,0,555,0,0,-18,0,0,1487,6,50491,"WAT","HY" 11,23,1,1,,37,50,"CENTRAL MAINE POWER CO","DEER RIP 1",0,,3266,"0M",1294,,,95,2694,0,0,2434,0,0,4080,0,0,3776,0,0,4034,0,0,2023,0,0,686,0,0,215,0,0,83,0,0,1916,0,0,3984,0,0,3453,0,0,1488,6,50491,"WAT","HY" 11,23,1,1,,37,60,"CENTRAL MAINE POWER CO","FT HALIFAX",0,,3266,"0M",1294,,,95,959,0,0,424,0,0,1026,0,0,961,0,0,925,0,0,526,0,0,51,0,0,5,0,0,155,0,0,380,0,0,977,0,0,659,0,0,1490,6,50491,"WAT","HY" 11,23,1,1,,37,75,"CENTRAL MAINE POWER CO","GULF ISLAND",0,,3266,"0M",1294,,,95,10764,0,0,9131,0,0,13512,0,0,13282,0,0,13485,0,0,8299,0,0,5537,0,0,4070,0,0,2892,0,0,9130,0,0,15549,0,0,11464,0,0,1491,6,50491,"WAT","HY" 11,23,1,1,,37,80,"CENTRAL MAINE POWER CO","HARRIS",0,,3266,"0M",1294,,,95,14325,0,0,24479,0,0,22937,0,0,6538,0,0,5448,0,0,21283,0,0,13285,0,0,11928,0,0,12813,0,0,10770,0,0,19708,0,0,26783,0,0,1492,6,50491,"WAT","HY" 11,23,1,1,,37,85,"CENTRAL MAINE POWER CO","HIRAM",0,,3266,"0M",1294,,,95,5791,0,0,3447,0,0,5873,0,0,6762,0,0,6516,0,0,2778,0,0,1397,0,0,1182,0,0,155,0,0,2992,0,0,7160,0,0,4285,0,0,1493,6,50491,"WAT","HY" 11,23,1,1,,37,90,"CENTRAL MAINE POWER CO","MESALONSK 2",0,,3266,"0M",1294,,,95,1280,0,0,585,0,0,1625,0,0,606,0,0,869,0,0,350,0,0,2,0,0,-1,0,0,9,0,0,710,0,0,1668,0,0,745,0,0,1497,6,50491,"WAT","HY" 11,23,1,1,,37,95,"CENTRAL MAINE POWER CO","MESALONSK 3",0,,3266,"0M",1294,,,95,753,0,0,330,0,0,977,0,0,349,0,0,507,0,0,180,0,0,0,0,0,-6,0,0,0,0,0,414,0,0,1038,0,0,416,0,0,1498,6,50491,"WAT","HY" 11,23,1,1,,37,100,"CENTRAL MAINE POWER CO","MESALONSK 4",0,,3266,"0M",1294,,,95,405,0,0,183,0,0,451,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1499,6,50491,"WAT","HY" 11,23,1,1,,37,105,"CENTRAL MAINE POWER CO","MESALONSK 5",0,,3266,"0M",1294,,,95,699,0,0,292,0,0,0,0,0,378,0,0,0,0,0,203,0,0,13,0,0,9,0,0,4,0,0,408,0,0,923,0,0,390,0,0,1500,6,50491,"WAT","HY" 11,23,1,1,,37,110,"CENTRAL MAINE POWER CO","NO GORHAM",0,,3266,"0M",1294,,,95,1215,0,0,963,0,0,842,0,0,520,0,0,455,0,0,503,0,0,595,0,0,604,0,0,413,0,0,340,0,0,740,0,0,1180,0,0,1501,6,50491,"WAT","HY" 11,23,1,1,,37,125,"CENTRAL MAINE POWER CO","SHAWMUT",0,,3266,"0M",1294,,,95,5226,0,0,5495,0,0,6547,0,0,5776,0,0,5295,0,0,4910,0,0,3475,0,0,2346,0,0,2571,0,0,3529,0,0,4803,0,0,6066,0,0,1504,6,50491,"WAT","HY" 11,23,1,1,,37,130,"CENTRAL MAINE POWER CO","SKELTON",0,,3266,"0M",1294,,,95,13276,0,0,8614,0,0,12134,0,0,11304,0,0,11550,0,0,5199,0,0,2833,0,0,2610,0,0,687,0,0,6731,0,0,13037,0,0,9456,0,0,1505,6,50491,"WAT","HY" 11,23,1,1,,37,145,"CENTRAL MAINE POWER CO","WEST BUXTON",0,,3266,"0M",1294,,,95,4424,0,0,2556,0,0,4381,0,0,3723,0,0,3292,0,0,1602,0,0,798,0,0,745,0,0,418,0,0,1944,0,0,4334,0,0,3045,0,0,1508,6,50491,"WAT","HY" 11,23,1,1,,37,150,"CENTRAL MAINE POWER CO","WESTON",0,,3266,"0M",1294,,,95,8095,0,0,8443,0,0,9513,0,0,8520,0,0,7843,0,0,7850,0,0,5819,0,0,4618,0,0,4257,0,0,5361,0,0,7925,0,0,9347,0,0,1509,6,50491,"WAT","HY" 11,23,1,1,,37,155,"CENTRAL MAINE POWER CO","WILLIAMS",0,,3266,"0M",1294,,,95,9171,0,0,9162,0,0,10255,0,0,6585,0,0,7543,0,0,8658,0,0,6098,0,0,5593,0,0,5308,0,0,5891,0,0,8857,0,0,10646,0,0,1510,6,50491,"WAT","HY" 11,23,1,1,,37,160,"CENTRAL MAINE POWER CO","WYMAN HYDRO",0,,3266,"0M",1294,,,95,30298,0,0,37016,0,0,38382,0,0,18735,0,0,24745,0,0,31774,0,0,20433,0,0,17564,0,0,16353,0,0,19735,0,0,40234,0,0,38504,0,0,1511,6,50491,"WAT","HY" 11,23,1,4,2,37,175,"CENTRAL MAINE POWER CO","CAPE",0,"LIGHT OIL",3266,"0M",1294,,,95,40,282,7937,40,336,7601,-57,44,7557,-40,24,7533,5,162,7371,38,208,7316,611,1872,6581,497,1571,5887,-24,32,5855,-32,27,5828,-45,25,5803,-25,145,5552,1484,6,50491,"FO2","GT" 11,23,1,2,2,37,200,"CENTRAL MAINE POWER CO","WYMAN STEAM",0,"LIGHT OIL",3266,"0M",1294,,,95,707,1587,1149,810,1542,1579,117,264,1534,980,1825,1680,366,883,1468,854,1640,1807,783,1460,2327,653,1307,1677,115,266,1410,20,76,1335,486,1282,2039,604,1177,2212,1507,6,50491,"FO2","ST" 11,23,1,2,3,37,200,"CENTRAL MAINE POWER CO","WYMAN STEAM",0,"HEAVY OIL",3266,"0M",1294,,,95,47051,97029,319010,122493,214459,275338,22777,47240,228098,127804,222606,207728,22560,50003,278752,79660,140051,253816,153893,263859,173676,74046,134076,202289,16596,35140,288543,3258,10955,197963,18538,44437,353526,107031,192190,308382,1507,6,50491,"FO6","ST" 11,23,1,3,2,37,204,"CENTRAL MAINE POWER CO","ISLESBORO",0,"LIGHT OIL",3266,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1494,6,50491,"FO2","IC" 11,23,1,3,2,37,206,"CENTRAL MAINE POWER CO","PEAK IS",0,"LIGHT OIL",3266,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1502,6,50491,"FO2","IC" 11,23,1,1,,37,210,"CENTRAL MAINE POWER CO","BRUNSWICK",0,,3266,"0M",1294,,,95,7964,0,0,6898,0,0,11266,0,0,10237,0,0,10095,0,0,6009,0,0,3698,0,0,2974,0,0,2429,0,0,6541,0,0,12216,0,0,8541,0,0,1483,6,50491,"WAT","HY" 11,23,1,1,,37,215,"CENTRAL MAINE POWER CO","W CHANNEL",0,,3266,"0M",1294,,,95,0,0,0,-33,0,0,-20,0,0,-22,0,0,-1,0,0,-1,0,0,-1,0,0,-21,0,0,-1,0,0,19,0,0,-11,0,0,-22,0,0,695,6,50491,"WAT","HY" 11,23,1,1,,37,220,"CENTRAL MAINE POWER CO","BATES UPPER",0,,3266,"0M",1294,,,95,-41,0,0,-34,0,0,610,0,0,144,0,0,273,0,0,15,0,0,1,0,0,15,0,0,18,0,0,217,0,0,4223,0,0,-30,0,0,7044,6,50491,"WAT","HY" 11,23,1,1,,37,225,"CENTRAL MAINE POWER CO","BATES LOWER",0,,3266,"0M",1294,"S",,95,-17,0,0,-16,0,0,-8,0,0,-2,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,-1,0,0,-3,0,0,-17,0,0,7045,6,50491,"WAT","HY" 11,23,1,1,,37,235,"CENTRAL MAINE POWER CO","ANDRO LOWER",0,,3266,"0M",1294,,,95,23,0,0,-11,0,0,21,0,0,-2,0,0,12,0,0,0,0,0,-1,0,0,0,0,0,0,0,0,5,0,0,38,0,0,-14,0,0,7047,6,50491,"WAT","HY" 11,23,1,1,,37,240,"CENTRAL MAINE POWER CO","HILL MILL",0,,3266,"0M",1294,,,95,-3,0,0,-2,0,0,183,0,0,-6,0,0,60,0,0,2,0,0,1,0,0,0,0,0,1,0,0,105,0,0,467,0,0,-6,0,0,7048,6,50491,"WAT","HY" 11,23,1,1,,37,245,"CENTRAL MAINE POWER CO","C E MONTY",0,,3266,"0M",1294,,,95,11840,0,0,10124,0,0,14280,0,0,13297,0,0,13808,0,0,8324,0,0,5496,0,0,4271,0,0,3199,0,0,9333,0,0,15686,0,0,12247,0,0,805,6,50491,"WAT","HY" 11,23,1,1,,37,250,"CENTRAL MAINE POWER CO","SMELT HILL",0,,3266,"0M",294,"A",,95,0,0,0,400,0,0,352,0,0,239,0,0,180,0,0,162,0,0,191,0,0,178,0,0,-608,0,0,766,0,0,224,0,0,283,0,0,7514,6,50491,"WAT","HY" 11,23,1,2,"B",37,255,"CENTRAL MAINE POWER CO","AROOSTOOK V",0,"WOOD",3266,"0M",294,"A",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,165,0,0,134,0,0,0,0,0,0,0,0,7513,6,50491,"WD","ST" 11,23,1,1,,94,5,"MAINE PUBLIC SERVICE CO","CARIBOU",0,,11522,"0M",1294,,,95,454,0,0,469,0,0,519,0,0,451,0,0,454,0,0,410,0,0,48,0,0,1,0,0,-2,0,0,178,0,0,536,0,0,504,0,0,1513,6,51747,"WAT","HY" 11,23,1,2,3,94,5,"MAINE PUBLIC SERVICE CO","CARIBOU",0,"HEAVY OIL",11522,"0M",1294,,,95,343,903,9375,592,1410,7984,-32,0,8005,-29,0,7995,-26,6,8015,-27,4,8057,-26,0,8067,222,644,7448,-28,0,7396,-29,0,7390,857,1841,5557,2237,4973,2370,1513,6,51747,"FO6","ST" 11,23,1,3,2,94,5,"MAINE PUBLIC SERVICE CO","CARIBOU",0,"LIGHT OIL",11522,"0M",1294,,,95,50,251,1746,5,143,1693,-65,0,1583,78,225,1932,-18,17,1865,-9,6,1829,38,115,1683,233,500,1802,86,210,1776,-6,65,2071,-56,28,1948,244,599,2098,1513,6,51747,"FO2","IC" 11,23,1,1,,94,10,"MAINE PUBLIC SERVICE CO","SQUA PAN",0,,11522,"0M",1294,,,95,115,0,0,363,0,0,152,0,0,-10,0,0,-7,0,0,-3,0,0,-3,0,0,-4,0,0,-6,0,0,-7,0,0,3,0,0,223,0,0,1516,6,51747,"WAT","HY" 11,23,1,3,2,94,23,"MAINE PUBLIC SERVICE CO","FLOS INN",0,"LIGHT OIL",11522,"0M",1294,,,95,27,115,314,19,82,232,-29,0,232,19,79,373,-23,2,371,-16,0,371,13,80,290,124,284,232,74,135,323,-3,51,272,-25,8,264,217,451,388,1514,6,51747,"FO2","IC" 11,23,1,3,2,94,25,"MAINE PUBLIC SERVICE CO","HOULTON",0,"LIGHT OIL",11522,"0M",1294,,,95,6,28,13,-8,1,12,-8,2,10,-8,0,10,-6,0,10,-3,0,10,-2,0,10,-3,0,10,-3,0,10,-4,0,11,-4,2,8,14,34,6,1515,6,51747,"FO2","IC" 11,23,1,2,1,97,1,"MAINE YANKEE ATOMIC PWR C","MAIN YANKEE",0,"NUCLEAR",11525,"0M",1294,,,95,197577,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1517,6,51748,"UR","ST" 11,23,1,3,2,116,10,"PUB SERV CO OF NEW HAMP","SWANS FALLS",0,"LIGHT OIL",15472,"0M",1294,"R",180,95,-7,0,2,-7,0,2,-6,0,2,-3,0,2,-2,0,2,-1,0,2,-1,0,2,-1,0,2,-1,0,2,-1,0,2,-3,0,2,0,0,0,1518,6,52411,"FO2","IC" 11,23,5,1,,525,1,"LEWISTON (CITY OF)","ANDRO UPPER",0,,10963,"0A",1294,,,95,296,0,0,378,0,0,310,0,0,424,0,0,264,0,0,390,0,0,256,0,0,258,0,0,304,0,0,270,0,0,342,0,0,324,0,0,7046,6,54168,"WAT","HY" 11,23,5,1,,566,1,"MADISON (CITY OF)","NORRIDGEWCK",0,,11477,"0A",1294,,,95,306,0,0,241,0,0,261,0,0,291,0,0,379,0,0,277,0,0,75,0,0,0,0,0,26,0,0,121,0,0,197,0,0,224,0,0,6701,6,51737,"WAT","HY" 11,23,8,3,2,835,5,"EASTERN MAINE ELEC COOP","PORTABLE",0,"LIGHT OIL",5609,"0A",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,6366,6,50848,"FO2","IC" 11,23,8,3,2,940,1,"SWANS ISLAND ELEC COOP","MINTURN",0,"LIGHT OIL",18368,"0A",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1550,6,52863,"FO2","IC" 12,33,1,1,,106,5,"NEW ENGLAND POWER CO","COMERFORD",0,,13433,"0M",1294,,90,95,34273,0,0,19125,0,0,43429,0,0,11874,0,0,22700,0,0,13853,0,0,5565,0,0,11061,0,0,5412,0,0,30636,0,0,45527,0,0,18948,0,0,2349,6,52007,"WAT","HY" 12,33,1,1,,106,10,"NEW ENGLAND POWER CO","MCINDOES",0,,13433,"0M",1294,,90,95,4420,0,0,3434,0,0,6350,0,0,3330,0,0,4648,0,0,2664,0,0,1453,0,0,2497,0,0,1353,0,0,4755,0,0,7050,0,0,3740,0,0,6483,6,52007,"WAT","HY" 12,33,1,1,,106,13,"NEW ENGLAND POWER CO","S C MOORE",0,,13433,"0M",1294,,90,95,29434,0,0,15866,0,0,34014,0,0,9521,0,0,19359,0,0,12124,0,0,4787,0,0,9805,0,0,4357,0,0,27013,0,0,40020,0,0,16551,0,0,2351,6,52007,"WAT","HY" 12,33,1,1,,106,15,"NEW ENGLAND POWER CO","VERNON",0,,13433,"0M",1294,,90,95,7120,0,0,5523,0,0,9186,0,0,7993,0,0,7582,0,0,3197,0,0,1355,0,0,2525,0,0,19,0,0,5912,0,0,9702,0,0,7342,0,0,2352,6,52007,"WAT","HY" 12,33,1,1,,106,20,"NEW ENGLAND POWER CO","WILDER",0,,13433,"0M",1294,,90,95,1974,0,0,3326,0,0,18722,0,0,7773,0,0,8911,0,0,4713,0,0,4047,0,0,5176,0,0,2849,0,0,9330,0,0,12667,0,0,7471,0,0,2353,6,52007,"WAT","HY" 12,33,1,2,1,123,1,"PUB SERV CO OF NEW HAMP","SEABROOK",0,"NUCLEAR",15472,"0M",1294,,180,95,857441,0,0,778373,0,0,863021,0,0,832472,0,0,865152,0,0,495425,0,0,690261,0,0,805711,0,0,800410,0,0,828658,0,0,60958,0,0,501494,0,0,6115,6,52411,"UR","ST" 12,33,1,1,,123,4,"PUB SERV CO OF NEW HAMP","AMOSKEAG",0,,15472,"0M",1294,,180,95,10690,0,0,7028,0,0,11425,0,0,749,0,0,15769,0,0,4245,0,0,2251,0,0,3257,0,0,434,0,0,5760,0,0,11044,0,0,6264,0,0,2354,6,52411,"WAT","HY" 12,33,1,1,,123,6,"PUB SERV CO OF NEW HAMP","AYERS IS",0,,15472,"0M",1294,,180,95,3909,0,0,2249,0,0,4743,0,0,3555,0,0,4487,0,0,1520,0,0,1448,0,0,1727,0,0,380,0,0,3303,0,0,5711,0,0,2632,0,0,2355,6,52411,"WAT","HY" 12,33,1,1,,123,16,"PUB SERV CO OF NEW HAMP","EASTMAN FLS",0,,15472,"0M",1294,,180,95,2843,0,0,1293,0,0,2781,0,0,2587,0,0,2725,0,0,1214,0,0,1763,0,0,10079,0,0,-9794,0,0,1729,0,0,3266,0,0,1701,0,0,2356,6,52411,"WAT","HY" 12,33,1,1,,123,20,"PUB SERV CO OF NEW HAMP","GARVIN FLS",0,,15472,"0M",1294,,180,95,5209,0,0,3143,0,0,5693,0,0,4388,0,0,3956,0,0,2019,0,0,755,0,0,1667,0,0,350,0,0,3233,0,0,6336,0,0,3913,0,0,2357,6,52411,"WAT","HY" 12,33,1,1,,123,22,"PUB SERV CO OF NEW HAMP","GORHAM",0,,15472,"0M",1294,,180,95,989,0,0,1031,0,0,1249,0,0,885,0,0,1193,0,0,756,0,0,568,0,0,530,0,0,580,0,0,864,0,0,1116,0,0,1202,0,0,2358,6,52411,"WAT","HY" 12,33,1,1,,123,28,"PUB SERV CO OF NEW HAMP","HOOKSETT",0,,15472,"0M",1294,,180,95,787,0,0,865,0,0,912,0,0,1164,0,0,1141,0,0,791,0,0,156,0,0,317,0,0,43,0,0,751,0,0,952,0,0,776,0,0,2359,6,52411,"WAT","HY" 12,33,1,1,,123,30,"PUB SERV CO OF NEW HAMP","JACKMAN",0,,15472,"0M",1294,,180,95,1997,0,0,535,0,0,1239,0,0,236,0,0,557,0,0,305,0,0,191,0,0,722,0,0,-8,0,0,1339,0,0,2326,0,0,864,0,0,2360,6,52411,"WAT","HY" 12,33,1,1,,123,50,"PUB SERV CO OF NEW HAMP","SMITH STA",0,,15472,"0M",1294,,180,95,8143,0,0,9737,0,0,11648,0,0,6108,0,0,8349,0,0,6172,0,0,4454,0,0,4871,0,0,3742,0,0,6861,0,0,10860,0,0,10308,0,0,2368,6,52411,"WAT","HY" 12,33,1,4,2,123,57,"PUB SERV CO OF NEW HAMP","LOST NATION",0,"LIGHT OIL",15472,"0M",1294,,180,95,-15,0,2159,79,306,1853,-15,0,1853,-12,0,1853,42,125,1728,50,140,1587,209,595,1527,275,828,1235,-11,0,1235,-11,0,1235,-10,0,1235,111,338,1076,2362,6,52411,"FO2","GT" 12,33,1,2,2,123,59,"PUB SERV CO OF NEW HAMP","MERRIMACK",0,"LIGHT OIL",15472,"0M",1294,,180,95,27,45,275,16,29,156,22,38,180,23,38,218,0,0,0,29,52,151,6,14,205,30,55,180,52,96,222,62,108,185,57,96,176,20,35,176,2364,6,52411,"FO2","ST" 12,33,1,2,6,123,59,"PUB SERV CO OF NEW HAMP","MERRIMACK",0,"BIT COAL",15472,"0M",1294,,180,95,266403,101539,253077,274308,103830,266334,256612,98157,263978,216443,80934,278945,76504,17154,315133,246563,95683,297713,281671,111493,247571,263463,95839,235114,181335,71786,264069,207269,81066,275589,253852,96425,269715,287608,108204,247069,2364,6,52411,"BIT","ST" 12,33,1,4,2,123,59,"PUB SERV CO OF NEW HAMP","MERRIMACK",0,"LIGHT OIL",15472,"0M",1294,,180,95,-47,0,3032,411,1048,3032,-21,0,1984,-18,0,1984,112,282,1702,122,334,1367,613,1576,1494,582,1554,2033,-14,0,2033,-11,20,2013,-20,0,2013,242,603,1411,2364,6,52411,"FO2","GT" 12,33,1,2,3,123,63,"PUB SERV CO OF NEW HAMP","SCHILLER",0,"HEAVY OIL",15472,"0M",1294,,180,95,1350,2702,31413,820,1554,92325,2073,4352,187620,1454,2823,184796,1826,3479,189663,2478,4626,184835,4062,7903,176932,2011,4193,53637,1321,2911,170000,1885,4329,165671,5233,10859,154812,3538,6785,118334,2367,6,52411,"FO6","ST" 12,33,1,2,6,123,63,"PUB SERV CO OF NEW HAMP","SCHILLER",0,"BIT COAL",15472,"0M",1294,,180,95,53534,27148,87087,68779,32692,50318,47008,24972,52027,65230,33724,53967,55312,27020,32185,49976,24400,75043,55074,26887,62380,30313,18396,42154,18241,9931,51974,16092,9642,54786,30357,16856,90418,65541,32424,72200,2367,6,52411,"BIT","ST" 12,33,1,4,2,123,63,"PUB SERV CO OF NEW HAMP","SCHILLER",0,"LIGHT OIL",15472,"0M",1294,,180,95,-13,0,804,95,260,723,-12,0,723,-9,0,723,57,118,604,-7,0,604,90,262,723,242,963,714,-7,0,714,0,0,714,-9,0,714,120,301,794,2367,6,52411,"FO2","GT" 12,33,1,4,9,123,63,"PUB SERV CO OF NEW HAMP","SCHILLER",0,"NAT GAS",15472,"0M",1294,,180,95,19,240,0,12,140,0,24,310,0,25,300,0,22,264,0,17,210,0,219,2700,0,121,2803,0,14,190,0,15,220,0,24,320,0,22,260,0,2367,6,52411,"NG","GT" 12,33,1,4,2,123,70,"PUB SERV CO OF NEW HAMP","WHITE LAKE",0,"LIGHT OIL",15472,"0M",1294,,180,95,-17,0,2383,97,350,2033,-14,4,2029,-7,0,2029,48,94,1935,136,341,1595,147,405,1763,357,924,1410,-3,0,1410,-3,0,1410,-13,0,1410,-6,129,1281,2369,6,52411,"FO2","GT" 12,33,1,2,2,123,72,"PUB SERV CO OF NEW HAMP","NEWINGTON",0,"LIGHT OIL",15472,"0M",1294,,180,95,2141,4247,1577,1729,3274,1766,1111,2327,1824,1584,4149,1209,1580,3072,1209,1589,3168,1640,1162,2239,1856,1703,3313,1598,1134,2258,1388,173,817,1751,1894,3703,1630,507,3096,1651,8002,6,52411,"FO2","ST" 12,33,1,2,3,123,72,"PUB SERV CO OF NEW HAMP","NEWINGTON",0,"HEAVY OIL",15472,"0M",1294,,180,95,73391,138116,328850,119485,206586,321529,32827,62816,434361,89003,159420,245596,100291,177704,321055,73382,134661,317462,125529,216497,100965,57182,118647,2305699,45699,82009,405756,1560,6611,399144,100544,177099,222046,136392,231245,388270,8002,6,52411,"FO6","ST" 12,33,1,2,9,123,72,"PUB SERV CO OF NEW HAMP","NEWINGTON",0,"NAT GAS",15472,"0M",1294,,180,95,1463,17053,0,0,0,0,0,0,0,0,0,0,35353,394385,0,45744,527451,0,57696,624462,0,48968,544320,0,10747,122302,0,57,1545,0,742,8312,0,0,0,0,8002,6,52411,"NG","ST" 13,50,1,1,,22,2,"CENTRAL VT PUB SERV CORP","ARNOLD FLS",0,,3292,"0A",1294,,350,95,112,0,0,27,0,0,168,0,0,290,0,0,100,0,0,18,0,0,33,0,0,37,0,0,17,0,0,172,0,0,245,0,0,135,0,0,3707,6,50503,"WAT","HY" 13,50,1,1,,22,10,"CENTRAL VT PUB SERV CORP","CAVENDISH",0,,3292,"0A",1294,,350,95,534,0,0,309,0,0,847,0,0,607,0,0,267,0,0,83,0,0,0,0,0,134,0,0,-3,0,0,391,0,0,928,0,0,383,0,0,3710,6,50503,"WAT","HY" 13,50,1,1,,22,11,"CENTRAL VT PUB SERV CORP","CLARKS FLS",0,,3292,"0A",1294,,350,95,1404,0,0,1026,0,0,1689,0,0,1865,0,0,1729,0,0,855,0,0,596,0,0,1076,0,0,567,0,0,1648,0,0,1970,0,0,1412,0,0,3711,6,50503,"WAT","HY" 13,50,1,1,,22,15,"CENTRAL VT PUB SERV CORP","FAIRFAX",0,,3292,"0A",1294,,350,95,1873,0,0,1589,0,0,2321,0,0,2516,0,0,2499,0,0,1241,0,0,878,0,0,1432,0,0,744,0,0,2114,0,0,2573,0,0,2233,0,0,3712,6,50503,"WAT","HY" 13,50,1,1,,22,16,"CENTRAL VT PUB SERV CORP","GAGE",0,,3292,"0A",1294,,350,95,221,0,0,24,0,0,244,0,0,307,0,0,290,0,0,73,0,0,85,0,0,38,0,0,48,0,0,305,0,0,523,0,0,226,0,0,3713,6,50503,"WAT","HY" 13,50,1,1,,22,18,"CENTRAL VT PUB SERV CORP","GLEN",0,,3292,"0A",1294,,350,95,1041,0,0,605,0,0,731,0,0,367,0,0,238,0,0,98,0,0,83,0,0,323,0,0,183,0,0,629,0,0,1307,0,0,401,0,0,3714,6,50503,"WAT","HY" 13,50,1,1,,22,22,"CENTRAL VT PUB SERV CORP","LW MIDLEBRY",0,,3292,"0A",1294,,350,95,725,0,0,534,0,0,1054,0,0,920,0,0,550,0,0,286,0,0,79,0,0,150,0,0,104,0,0,524,0,0,1220,0,0,492,0,0,3716,6,50503,"WAT","HY" 13,50,1,1,,22,26,"CENTRAL VT PUB SERV CORP","MILTON",0,,3292,"0A",1294,,350,95,3538,0,0,2446,0,0,4215,0,0,4336,0,0,3864,0,0,1806,0,0,1204,0,0,2514,0,0,1210,0,0,4046,0,0,4879,0,0,3192,0,0,3717,6,50503,"WAT","HY" 13,50,1,1,,22,28,"CENTRAL VT PUB SERV CORP","PASSUMPSIC",0,,3292,"0A",1294,,350,95,315,0,0,97,0,0,378,0,0,435,0,0,415,0,0,90,0,0,51,0,0,150,0,0,94,0,0,370,0,0,434,0,0,44,0,0,3718,6,50503,"WAT","HY" 13,50,1,1,,22,30,"CENTRAL VT PUB SERV CORP","PATCH",0,,3292,"0A",1294,,350,95,107,0,0,58,0,0,59,0,0,21,0,0,7,0,0,5,0,0,5,0,0,28,0,0,7,0,0,42,0,0,158,0,0,30,0,0,3719,6,50503,"WAT","HY" 13,50,1,1,,22,34,"CENTRAL VT PUB SERV CORP","PIERCE MLS",0,,3292,"0A",1294,,350,95,113,0,0,81,0,0,121,0,0,180,0,0,161,0,0,59,0,0,47,0,0,47,0,0,17,0,0,102,0,0,181,0,0,116,0,0,3721,6,50503,"WAT","HY" 13,50,1,1,,22,36,"CENTRAL VT PUB SERV CORP","PITTSFORD",0,,3292,"0A",1294,,350,95,1275,0,0,941,0,0,158,0,0,47,0,0,-2,0,0,9,0,0,0,0,0,489,0,0,354,0,0,726,0,0,1999,0,0,679,0,0,3722,6,50503,"WAT","HY" 13,50,1,1,,22,38,"CENTRAL VT PUB SERV CORP","SALISBURY",0,,3292,"0A",1294,,350,95,325,0,0,210,0,0,191,0,0,62,0,0,141,0,0,65,0,0,25,0,0,72,0,0,111,0,0,88,0,0,-6,0,0,303,0,0,3724,6,50503,"WAT","HY" 13,50,1,1,,22,40,"CENTRAL VT PUB SERV CORP","SILVER LAKE",0,,3292,"0A",1294,,350,95,800,0,0,508,0,0,722,0,0,405,0,0,402,0,0,227,0,0,103,0,0,275,0,0,84,0,0,500,0,0,973,0,0,535,0,0,3725,6,50503,"WAT","HY" 13,50,1,1,,22,41,"CENTRAL VT PUB SERV CORP","TAFTSVILLE",0,,3292,"0A",1294,,350,95,150,0,0,135,0,0,208,0,0,200,0,0,119,0,0,12,0,0,0,0,0,17,0,0,-1,0,0,55,0,0,175,0,0,162,0,0,3727,6,50503,"WAT","HY" 13,50,1,1,,22,44,"CENTRAL VT PUB SERV CORP","WEYBRIDGE",0,,3292,"0A",1294,,350,95,1391,0,0,616,0,0,1819,0,0,1459,0,0,991,0,0,370,0,0,156,0,0,354,0,0,167,0,0,1042,0,0,2031,0,0,856,0,0,3728,6,50503,"WAT","HY" 13,50,1,1,,22,45,"CENTRAL VT PUB SERV CORP","PETERSON",0,,3292,"0A",1294,,350,95,2522,0,0,1281,0,0,3601,0,0,3092,0,0,2335,0,0,1090,0,0,702,0,0,1605,0,0,681,0,0,2814,0,0,4021,0,0,1742,0,0,3720,6,50503,"WAT","HY" 13,50,1,4,2,22,48,"CENTRAL VT PUB SERV CORP","RUTLAND",0,"LIGHT OIL",3292,"0A",1294,,350,95,13,125,4525,45,327,4198,40,218,3979,19,143,3836,20,127,3709,101,381,3328,272,898,2430,277,932,1498,34,167,3475,-8,46,3429,32,195,3234,152,651,2583,3723,6,50503,"FO2","GT" 13,50,1,4,2,22,49,"CENTRAL VT PUB SERV CORP","ASCUTNEY",0,"LIGHT OIL",3292,"0A",1294,,350,95,27,136,2572,77,326,2246,69,300,1946,18,96,1851,8,65,1786,41,144,1641,268,895,2175,226,765,1409,-1,38,3277,-15,0,3277,-3,71,3206,88,353,2853,3708,6,50503,"FO2","GT" 13,50,1,3,2,22,60,"CENTRAL VT PUB SERV CORP","ST ALBANS",0,"LIGHT OIL",3292,"0A",1294,,350,95,-14,0,89,5,38,214,-11,4,210,-10,5,205,7,17,188,21,40,148,72,149,234,59,123,111,-1,2,110,-3,0,110,-6,0,108,9,42,236,3726,6,50503,"FO2","IC" 13,50,1,1,,22,65,"CENTRAL VT PUB SERV CORP","SMITH",0,,3292,"0A",1294,,350,95,361,0,0,154,0,0,495,0,0,658,0,0,519,0,0,163,0,0,121,0,0,123,0,0,72,0,0,258,0,0,692,0,0,170,0,0,3709,6,50503,"WAT","HY" 13,50,1,1,,22,70,"CENTRAL VT PUB SERV CORP","EAST BARNET",0,,3292,"0A",1294,,350,95,595,0,0,399,0,0,900,0,0,1046,0,0,922,0,0,325,0,0,322,0,0,358,0,0,203,0,0,790,0,0,1148,0,0,702,0,0,788,6,50503,"WAT","HY" 13,50,1,1,,24,5,"CITIZENS UTILITIES CO","CHARLESTON",0,,3611,"0A",1294,,,95,339,0,0,244,0,0,393,0,0,445,0,0,409,0,0,252,0,0,154,0,0,192,0,0,90,0,0,382,0,0,461,0,0,314,0,0,3729,6,50560,"WAT","HY" 13,50,1,1,,24,10,"CITIZENS UTILITIES CO","NEWPORT",0,,3611,"0A",1294,,,95,1625,0,0,946,0,0,1961,0,0,1655,0,0,1645,0,0,917,0,0,474,0,0,1107,0,0,331,0,0,1614,0,0,2652,0,0,1235,0,0,3731,6,50560,"WAT","HY" 13,50,1,3,2,24,15,"CITIZENS UTILITIES CO","NEWPORT DSL",0,"LIGHT OIL",3611,"0A",1294,,,95,0,0,377,16,33,290,0,0,259,0,0,229,0,0,206,0,0,206,0,0,206,7,12,194,8,16,177,0,0,177,0,0,137,0,0,85,3730,6,50560,"FO2","IC" 13,50,1,1,,24,20,"CITIZENS UTILITIES CO","TROY",0,,3611,"0A",1294,,,95,150,0,0,72,0,0,150,0,0,267,0,0,209,0,0,71,0,0,28,0,0,30,0,0,3,0,0,74,0,0,244,0,0,128,0,0,3733,6,50560,"WAT","HY" 13,50,1,1,,47,10,"GREEN MOUNTAIN POWER CORP","ESSEX 19",0,,7601,"0M",1294,,,95,2888,0,0,2870,0,0,4338,0,0,3931,0,0,3261,0,0,980,0,0,333,0,0,1531,0,0,936,0,0,2161,0,0,3540,0,0,2964,0,0,3737,6,51169,"WAT","HY" 13,50,1,3,2,47,10,"GREEN MOUNTAIN POWER CORP","ESSEX 19",0,"LIGHT OIL",7601,"0M",1294,,,95,0,0,311,11,27,284,1,1,283,0,0,283,7,16,267,28,61,385,45,85,300,33,65,235,9,19,394,0,0,394,0,0,394,12,25,369,3737,6,51169,"FO2","IC" 13,50,1,1,,47,15,"GREEN MOUNTAIN POWER CORP","GORGE NO 18",0,,7601,"0M",1294,,,95,901,0,0,986,0,0,1573,0,0,1661,0,0,1125,0,0,122,0,0,113,0,0,692,0,0,0,0,0,0,0,0,0,0,0,0,0,0,6475,6,51169,"WAT","HY" 13,50,1,1,,47,20,"GREEN MOUNTAIN POWER CORP","MARSHFIELD6",0,,7601,"0M",1294,,,95,891,0,0,1188,0,0,245,0,0,107,0,0,0,0,0,3,0,0,2,0,0,54,0,0,53,0,0,604,0,0,1300,0,0,430,0,0,3739,6,51169,"WAT","HY" 13,50,1,1,,47,25,"GREEN MOUNTAIN POWER CORP","MIDDLESEX 2",0,,7601,"0M",1294,,,95,1134,0,0,848,0,0,1580,0,0,1697,0,0,1156,0,0,150,0,0,111,0,0,717,0,0,45,0,0,1158,0,0,2061,0,0,1133,0,0,3740,6,51169,"WAT","HY" 13,50,1,1,,47,40,"GREEN MOUNTAIN POWER CORP","VERGENNES 9",0,,7601,"0M",1294,,,95,972,0,0,799,0,0,1171,0,0,1224,0,0,968,0,0,441,0,0,247,0,0,499,0,0,318,0,0,590,0,0,1307,0,0,899,0,0,6519,6,51169,"WAT","HY" 13,50,1,3,2,47,40,"GREEN MOUNTAIN POWER CORP","VERGENNES 9",0,"LIGHT OIL",7601,"0M",1294,,,95,15,27,282,68,118,164,15,24,319,5,8,311,4,25,465,108,264,200,174,319,417,163,302,294,20,35,437,3,2,436,2,4,432,35,62,370,6519,6,51169,"FO2","IC" 13,50,1,1,,47,53,"GREEN MOUNTAIN POWER CORP","WATRBRY 22",0,,7601,"0M",1294,,,95,2101,0,0,2029,0,0,1441,0,0,318,0,0,823,0,0,444,0,0,464,0,0,1190,0,0,485,0,0,2251,0,0,2609,0,0,1566,0,0,6520,6,51169,"WAT","HY" 13,50,1,1,,47,55,"GREEN MOUNTAIN POWER CORP","W DANVIL 15",0,,7601,"0M",1294,,,95,445,0,0,146,0,0,507,0,0,509,0,0,301,0,0,77,0,0,87,0,0,220,0,0,103,0,0,544,0,0,661,0,0,151,0,0,3743,6,51169,"WAT","HY" 13,50,1,4,2,47,58,"GREEN MOUNTAIN POWER CORP","BERLIN NO 5",0,"LIGHT OIL",7601,"0M",1294,,,95,32,270,10962,606,1501,9460,21,72,9388,0,0,9338,254,677,8711,731,1834,7632,1214,3039,11011,1354,3377,12369,189,463,14376,681,1521,12855,79,209,12646,389,879,11767,3734,6,51169,"FO2","GT" 13,50,1,4,2,47,60,"GREEN MOUNTAIN POWER CORP","COLCHSTR 16",0,"LIGHT OIL",7601,"0M",1294,,,95,7,28,1071,86,296,775,5,25,750,0,0,750,9,33,717,6,26,1583,117,472,1112,76,320,791,0,0,1506,0,0,1506,0,0,1507,0,0,1506,3735,6,51169,"FO2","GT" 13,50,1,1,,47,65,"GREEN MOUNTAIN POWER CORP","BOLTON FALL",0,,7601,"0M",1294,,,95,3020,0,0,2253,0,0,3823,0,0,2884,0,0,2258,0,0,636,0,0,502,0,0,1603,0,0,428,0,0,2596,0,0,4478,0,0,2430,0,0,7056,6,51169,"WAT","HY" 13,50,1,7,"D",47,70,"GREEN MOUNTAIN POWER CORP","CARTHUSIANS",0,"N/A",7601,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,7260,6,51169,"WI","WI" 13,50,1,1,,73,5,"NEW ENGLAND POWER CO","BELLOWS FLS",0,,13433,"0M",1294,,90,95,22299,0,0,16448,0,0,28735,0,0,22260,0,0,21635,0,0,10244,0,0,6175,0,0,10541,0,0,3991,0,0,19464,0,0,30239,0,0,18843,0,0,3745,6,52007,"WAT","HY" 13,50,1,1,,73,10,"NEW ENGLAND POWER CO","HARRIMAN",0,,13433,"0M",1294,,90,95,14391,0,0,13610,0,0,13092,0,0,2630,0,0,807,0,0,1394,0,0,2040,0,0,2968,0,0,2416,0,0,10136,0,0,16468,0,0,11713,0,0,3746,6,52007,"WAT","HY" 13,50,1,1,,73,15,"NEW ENGLAND POWER CO","SEARSBURG",0,,13433,"0M",1294,,90,95,3120,0,0,2878,0,0,3094,0,0,1942,0,0,1012,0,0,853,0,0,152,0,0,1319,0,0,954,0,0,2077,0,0,3042,0,0,2675,0,0,6529,6,52007,"WAT","HY" 13,50,1,1,,73,18,"NEW ENGLAND POWER CO","VERNON",0,,13433,"0M",1294,,90,95,4592,0,0,4182,0,0,5197,0,0,4922,0,0,4427,0,0,2397,0,0,1604,0,0,3525,0,0,1667,0,0,3876,0,0,4946,0,0,3693,0,0,8904,6,52007,"WAT","HY" 13,50,1,1,,73,20,"NEW ENGLAND POWER CO","WILDER",0,,13433,"0M",1294,,90,95,9053,0,0,5888,0,0,8525,0,0,1765,0,0,2559,0,0,1204,0,0,21,0,0,1756,0,0,407,0,0,4556,0,0,8802,0,0,2669,0,0,8905,6,52007,"WAT","HY" 13,50,1,1,,98,5,"PUB SERV CO OF NEW HAMP","CANAAN",0,,15472,"0M",1294,,180,95,729,0,0,718,0,0,805,0,0,483,0,0,569,0,0,345,0,0,252,0,0,190,0,0,195,0,0,728,0,0,765,0,0,738,0,0,3750,6,52411,"WAT","HY" 13,50,1,2,1,135,1,"VT YANKEE NUCLEAR PR CORP","VT YANKEE",0,"NUCLEAR",19796,"0M",1294,,,95,384928,0,0,346136,0,0,192519,0,0,0,0,0,335965,0,0,365673,0,0,371198,0,0,375476,0,0,363210,0,0,389313,0,0,379730,0,0,354361,0,0,3751,6,53128,"UR","ST" 13,50,1,1,,304,1,"VERMONT MARBLE CO","PROCTOR",0,,19794,"0A",1294,,,95,3213,0,0,2009,0,0,3559,0,0,3058,0,0,2032,0,0,1143,0,0,395,0,0,893,0,0,294,0,0,1839,0,0,3796,0,0,1853,0,0,6450,6,53127,"WAT","HY" 13,50,1,1,,304,5,"VERMONT MARBLE CO","CTR RUTLAND",0,,19794,"0A",1294,,,95,161,0,0,164,0,0,188,0,0,211,0,0,211,0,0,121,0,0,26,0,0,62,0,0,19,0,0,85,0,0,190,0,0,184,0,0,6453,6,53127,"WAT","HY" 13,50,1,1,,304,10,"VERMONT MARBLE CO","BELDENS",0,,19794,"0A",1294,,,95,2174,0,0,1009,0,0,2729,0,0,1624,0,0,972,0,0,405,0,0,95,0,0,369,0,0,149,0,0,1679,0,0,2997,0,0,1013,0,0,6451,6,53127,"WAT","HY" 13,50,1,4,2,304,15,"VERMONT MARBLE CO","FLORENCE",0,"LIGHT OIL",19794,"0A",1294,,,95,-2,95,12708,118,200,12076,184,475,11934,674,1762,7457,74,191,4607,157,358,9260,354,1040,6925,210,559,6363,167,435,4707,-11,3,10761,-13,60,8428,167,550,7887,7337,6,53127,"FO2","GT" 13,50,5,1,,520,1,"BARTON (VILLAGE OF)","W CHARLESTN",0,,1299,"0A",1294,,,95,477,0,0,231,0,0,556,0,0,533,0,0,570,0,0,256,0,0,132,0,0,351,0,0,83,0,0,382,0,0,680,0,0,196,0,0,3753,6,50178,"WAT","HY" 13,50,5,3,2,520,1,"BARTON (VILLAGE OF)","W CHARLESTN",0,"LIGHT OIL",1299,"0A",1294,,,95,0,0,206,14,34,172,0,0,172,0,0,172,1,3,169,19,51,118,39,103,190,42,112,78,7,19,59,0,0,59,0,0,118,10,86,32,3753,6,50178,"FO2","IC" 13,50,5,4,2,536,1,"BURLINGTON (CITY OF)","GAS TURB",0,"LIGHT OIL",2548,"0M",1294,,,95,0,1,1628,248,707,868,0,4,2022,0,0,2015,19,66,1949,459,1365,1742,608,1830,1698,485,1472,1476,56,189,1287,0,0,1285,84,242,1001,165,472,1772,3754,6,50375,"FO2","GT" 13,50,5,2,"B",536,10,"BURLINGTON (CITY OF)","J C MC NEIL",0,"WOD CHIPS",2548,"0M",1294,,,95,7742,0,0,12138,0,0,4790,0,0,12108,0,0,15618,0,0,11949,0,0,14425,0,0,8887,0,0,5359,0,0,3746,0,0,10817,0,0,19589,0,0,589,6,50375,"WOD","ST" 13,50,5,2,2,536,10,"BURLINGTON (CITY OF)","J C MC NEIL",0,"LIGHT OIL",2548,"0M",1294,,,95,136,326,2416,132,350,1989,41,99,1826,0,216,1559,0,39,1448,0,22,1351,4,23,1264,0,81,1183,0,52,1021,0,40,945,19,99,3170,24,98,2994,589,6,50375,"FO2","ST" 13,50,5,2,9,536,10,"BURLINGTON (CITY OF)","J C MC NEIL",0,"NAT GAS",2548,"0M",1294,,,95,1750,24386,0,816,12632,0,1337,18689,0,0,2252,0,0,3244,0,0,3721,0,177,4800,0,0,2471,0,0,2396,0,0,2708,0,449,13380,0,2064,47618,0,589,6,50375,"NG","ST" 13,50,5,1,,551,5,"ENOSBURG FALLS (VILLAGE)","KENDALL",0,,5915,"0A",1294,,,95,52,0,0,126,0,0,145,0,0,160,0,0,164,0,0,130,0,0,102,0,0,121,0,0,68,0,0,109,0,0,147,0,0,64,0,0,3757,6,50910,"WAT","HY" 13,50,5,3,2,551,10,"ENOSBURG FALLS (VILLAGE)","DIESEL PLT",0,"LIGHT OIL",5915,"0A",1294,,,95,1,5,320,14,24,296,0,1,296,1,3,293,4,13,280,16,34,246,20,37,351,23,44,307,2,6,301,0,0,301,0,0,0,12,21,279,4247,6,50910,"FO2","IC" 13,50,5,1,,551,15,"ENOSBURG FALLS (VILLAGE)","VILLAGE PLT",0,,5915,"0A",1294,,,95,370,0,0,204,0,0,298,0,0,433,0,0,408,0,0,218,0,0,87,0,0,140,0,0,45,0,0,324,0,0,364,0,0,395,0,0,4246,6,50910,"WAT","HY" 13,50,5,1,,567,1,"HARDWICK (VILLAGE OF)","WOLCOTT",0,,8104,"0A",1294,,,95,228,0,0,139,0,0,381,0,0,480,0,0,332,0,0,55,0,0,41,0,0,20,0,0,22,0,0,331,0,0,526,0,0,262,0,0,6477,6,51238,"WAT","HY" 13,50,5,3,2,567,5,"HARDWICK (VILLAGE OF)","HARDWICK",0,"LIGHT OIL",8104,"0A",1294,,,95,0,0,451,0,0,451,0,0,451,0,0,451,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,6476,6,51238,"FO2","IC" 13,50,5,1,,644,5,"LYNDONVILLE (CITY OF)","GREAT FALLS",0,,11359,"0A",1294,,,95,160,0,0,115,0,0,308,0,0,489,0,0,746,0,0,350,0,0,273,0,0,122,0,0,171,0,0,457,0,0,558,0,0,437,0,0,3762,6,51721,"WAT","HY" 13,50,5,1,,644,10,"LYNDONVILLE (CITY OF)","VAIL",0,,11359,"0A",1294,,,95,100,0,0,71,0,0,99,0,0,123,0,0,225,0,0,93,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,107,0,0,3763,6,51721,"WAT","HY" 13,50,5,1,,659,5,"MORRISVILLE (VILLAGE OF)","CADYS FALLS",0,,12989,"0A",1294,,,95,396,0,0,268,0,0,387,0,0,226,0,0,403,0,0,133,0,0,101,0,0,2,0,0,71,0,0,356,0,0,337,0,0,160,0,0,3765,6,51943,"WAT","HY" 13,50,5,1,,659,10,"MORRISVILLE (VILLAGE OF)","MORRISVILLE",0,,12989,"0A",1294,,,95,250,0,0,312,0,0,619,0,0,801,0,0,581,0,0,131,0,0,-1,0,0,-1,0,0,-1,0,0,-1,0,0,-2,0,0,227,0,0,3764,6,51943,"WAT","HY" 13,50,5,1,,659,15,"MORRISVILLE (VILLAGE OF)","W K SANDERS",0,,12989,"0A",1294,,,95,-5,0,0,114,0,0,24,0,0,13,0,0,33,0,0,10,0,0,-1,0,0,38,0,0,-2,0,0,83,0,0,177,0,0,7,0,0,678,6,51943,"WAT","HY" 13,50,5,1,,737,5,"SWANTON (VILLAGE OF)","HIGHGATE FL",0,,18371,"0A",1294,,,95,3846,0,0,2084,0,0,5329,0,0,5012,0,0,4484,0,0,2556,0,0,711,0,0,1431,0,0,444,0,0,4486,0,0,6056,0,0,2920,0,0,6618,6,52864,"WAT","HY" 13,50,8,1,,800,5,"VERMONT ELECTRIC COOP","N HARTLAND",0,,19791,"0A",1294,,,95,1260,0,0,415,0,0,212,0,0,990,0,0,623,0,0,190,0,0,90,0,0,4,0,0,8,0,0,484,0,0,1466,0,0,734,0,0,590,6,53125,"WAT","HY" 13,50,8,1,,810,5,"WASHINGTON ELECTRIC COOP","WRIGHTSVILE",0,,20151,"0A",1294,,,95,270,0,0,88,0,0,334,0,0,327,0,0,246,0,0,50,0,0,54,0,0,128,0,0,47,0,0,3224,0,0,418,0,0,153,0,0,7051,6,58100,"WAT","HY" 14,25,1,2,1,23,1,"BOSTON EDISON CO","PILGRIM",0,"NUCLEAR",1998,"0M",1294,,,95,494219,0,0,433548,0,0,370903,0,0,0,0,0,0,0,0,313826,0,0,476983,0,0,486906,0,0,466384,0,0,470820,0,0,479805,0,0,492451,0,0,1590,6,50300,"UR","ST" 14,25,1,4,2,23,15,"BOSTON EDISON CO","EDGAR",0,"LIGHT OIL",1998,"0M",1294,,,95,43,139,1048,160,393,893,25,79,1053,64,124,929,28,74,855,110,379,953,323,950,955,245,760,910,38,108,1040,37,107,933,56,139,1032,134,337,934,1585,6,50300,"FO2","GT" 14,25,1,4,2,23,17,"BOSTON EDISON CO","FRAMINGHAM",0,"LIGHT OIL",1998,"0M",1294,,,95,141,378,1770,276,681,1804,67,203,1601,44,165,1674,70,215,1698,449,1329,1559,788,2383,1819,766,2306,1658,95,258,1630,53,142,1734,74,277,1695,278,761,1649,1586,6,50300,"FO2","GT" 14,25,1,4,2,23,20,"BOSTON EDISON CO","L STREET",0,"LIGHT OIL",1998,"0M",1294,,,95,18,71,606,223,524,481,31,74,586,101,254,571,64,181,628,302,790,611,232,657,597,450,1241,537,70,195,581,33,121,579,41,95,603,202,478,601,1587,6,50300,"FO2","GT" 14,25,1,2,2,23,25,"BOSTON EDISON CO","MYSTIC",0,"LIGHT OIL",1998,"0M",1294,,,95,251,519,1723,2082,3518,560,0,0,2480,874,1565,1748,1508,2858,1987,1285,2470,2852,2284,4277,1789,1325,2537,1992,119,230,1762,111,219,2019,220,439,1580,238,420,1327,1588,6,50300,"FO2","ST" 14,25,1,2,3,23,25,"BOSTON EDISON CO","MYSTIC",0,"HEAVY OIL",1998,"0M",1294,,,95,112692,212897,634701,250006,389639,396000,28170,35809,578539,46219,75659,622498,47350,81843,540595,74633,131731,529651,114158,195470,453259,65504,114254,339850,9543,16899,623019,18574,33314,589243,137777,234264,549412,333744,539006,466193,1588,6,50300,"FO6","ST" 14,25,1,2,9,23,25,"BOSTON EDISON CO","MYSTIC",0,"NAT GAS",1998,"0M",1294,,,95,54301,611365,0,41760,387451,0,199825,2260608,0,223483,2242300,0,121095,1295784,0,76698,835115,0,229079,2424349,0,221936,2420968,0,166749,1844575,0,138588,1545200,0,1185,12271,0,4690,47014,0,1588,6,50300,"NG","ST" 14,25,1,4,2,23,25,"BOSTON EDISON CO","MYSTIC",0,"LIGHT OIL",1998,"0M",1294,,,95,27,56,491,103,175,435,20,57,497,61,110,506,37,71,435,192,369,532,279,524,365,264,506,455,27,53,523,26,52,471,36,92,498,52,92,444,1588,6,50300,"FO2","GT" 14,25,1,2,2,23,30,"BOSTON EDISON CO","NEW BOSTON",0,"LIGHT OIL",1998,"0M",1294,,,95,0,0,60,0,0,60,0,0,60,0,0,60,0,0,60,0,0,60,0,0,60,0,0,60,0,0,60,0,0,60,0,0,60,0,0,60,1589,6,50300,"FO2","ST" 14,25,1,2,3,23,30,"BOSTON EDISON CO","NEW BOSTON",0,"HEAVY OIL",1998,"0M",1294,,,95,215120,320592,70394,155709,225131,71506,167349,258313,38374,0,0,38374,0,0,38374,0,0,38374,0,0,38403,0,0,38403,0,0,38403,0,0,38808,0,0,73197,633,1026,94600,1589,6,50300,"FO6","ST" 14,25,1,2,9,23,30,"BOSTON EDISON CO","NEW BOSTON",0,"NAT GAS",1998,"0M",1294,,,95,0,0,0,151,1334,0,2301,23751,0,201560,2042478,0,231080,2303282,0,366745,3613841,0,376840,3697457,0,381210,3746576,0,337660,3311625,0,328300,3254233,0,343010,3322669,0,159417,1573389,0,1589,6,50300,"NG","ST" 14,25,1,4,2,23,40,"BOSTON EDISON CO","WEST MEDWAY",0,"LIGHT OIL",1998,"0M",1294,,,95,532,1305,6724,2615,5858,6588,305,882,6659,441,1064,6548,648,1783,6907,1922,5806,5619,2304,7193,6789,2376,1139,6841,43,153,6688,33,101,6587,199,636,6665,2492,6199,6929,1592,6,50300,"FO2","GT" 14,25,1,4,9,23,40,"BOSTON EDISON CO","WEST MEDWAY",0,"NAT GAS",1998,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,963,16262,0,363,42170,0,305,906,0,134,2149,0,0,0,0,0,0,0,1592,6,50300,"NG","GT" 14,25,1,2,3,25,5,"COMMONWEALTH ENERGY SYS","BLACKSTONE",0,"HEAVY OIL",4120,"0M",1294,,80,95,12,9,1622,622,891,254,0,0,0,12,11,3277,4,9,3067,8,31,3303,19,66,3122,71,286,2313,8,25,2707,0,0,2900,388,267,2375,216,151,3016,1594,6,50412,"FO6","ST" 14,25,1,2,9,25,5,"COMMONWEALTH ENERGY SYS","BLACKSTONE",0,"NAT GAS",4120,"0M",1294,,80,95,643,3052,0,809,7234,0,0,0,0,329,1924,0,176,2782,0,306,7064,0,840,18553,0,641,16359,0,98,2009,0,0,0,0,26,113,0,3,12,0,1594,6,50412,"NG","ST" 14,25,1,2,3,25,10,"COMMONWEALTH ENERGY SYS","KENDALL SQ",0,"HEAVY OIL",4120,"0M",1294,,80,95,1966,3331,44639,4440,7426,46357,571,1025,43350,551,1184,40895,279,518,39729,76,146,39422,226,384,45928,178,367,45253,473,969,43288,91,206,42859,6937,10643,43043,10035,14044,33074,1595,6,50412,"FO6","ST" 14,25,1,2,9,25,10,"COMMONWEALTH ENERGY SYS","KENDALL SQ",0,"NAT GAS",4120,"0M",1294,,80,95,8305,87563,0,5498,57215,0,7487,85115,0,6963,94695,0,6096,81153,0,7445,90078,0,8638,93009,0,7941,103714,0,6154,79756,0,5898,84299,0,580,5629,0,447,3954,0,1595,6,50412,"NG","ST" 14,25,1,4,2,25,10,"COMMONWEALTH ENERGY SYS","KENDALL SQ",0,"LIGHT OIL",4120,"0M",1294,,80,95,0,0,1889,173,442,1930,0,0,1930,10,26,1904,381,951,1671,340,886,1969,587,1240,1863,822,2088,2078,160,754,1323,0,0,1561,0,0,1561,183,453,1925,1595,6,50412,"FO2","GT" 14,25,1,2,3,25,15,"COMMONWEALTH ENERGY SYS","CANAL",0,"HEAVY OIL",4120,"0M",1294,,80,95,162391,279085,64428,147412,254620,37606,178077,310890,35916,210807,342420,34150,172965,296386,68134,149960,274442,64297,204907,357210,66759,386648,623547,65078,202416,316252,66152,59087,109907,66707,307766,492512,64272,421791,645524,63446,1599,6,50412,"FO6","ST" 14,25,1,3,2,25,25,"COMMONWEALTH ENERGY SYS","OAK BLUFFS",0,"LIGHT OIL",4120,"0M",1294,,80,95,0,0,1131,70,125,1006,0,0,1006,3,6,1000,58,98,1011,55,97,1035,183,321,1005,196,350,1036,1,4,1032,0,0,1159,6,15,1144,63,118,1026,1597,6,50412,"FO2","IC" 14,25,1,3,2,25,30,"COMMONWEALTH ENERGY SYS","W TISBURY",0,"LIGHT OIL",4120,"0M",1294,,80,95,0,0,2023,42,87,1936,0,0,1936,2,4,1932,38,68,1918,40,70,1848,243,439,1711,204,373,1827,0,0,1827,0,0,2044,5,18,2026,47,98,1928,6049,6,50412,"FO2","IC" 14,25,1,3,2,25,35,"COMMONWEALTH ENERGY SYS","AIRPORT DIE",0,"LIGHT OIL",4120,"0M",1294,,80,95,2,4,65,20,32,57,6,9,48,14,26,23,3,17,6,0,6,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,7184,6,50412,"FO2","IC" 14,25,1,4,2,46,1,"FITCHBURG GAS & ELEC LGT","FITCHBURG",0,"LIGHT OIL",6374,"0M",1294,,,95,113,320,1233,544,1372,812,0,0,1289,68,210,1079,120,416,1139,539,1444,1109,663,1798,2154,708,1974,1126,70,191,2125,49,166,1960,0,0,1960,461,1173,2216,1601,6,50990,"FO2","GT" 14,25,1,1,,59,5,"HOLYOKE WTR PWR CO","BB HOLBROOK",0,,8779,"0M",1294,,554,95,215,0,0,12,0,0,439,0,0,48,0,0,0,0,0,-4,0,0,-2,0,0,111,0,0,7,0,0,88,0,0,177,0,0,95,0,0,1602,6,51327,"WAT","HY" 14,25,1,1,,59,7,"HOLYOKE WTR PWR CO","CHEMICAL",0,,8779,"0M",1294,,554,95,390,0,0,65,0,0,264,0,0,560,0,0,1378,0,0,-3,0,0,-2,0,0,33,0,0,-2,0,0,199,0,0,228,0,0,152,0,0,1604,6,51327,"WAT","HY" 14,25,1,1,,59,10,"HOLYOKE WTR PWR CO","HADLEY FLLS",0,,8779,"0M",1294,,554,95,19318,0,0,16252,0,0,20835,0,0,17997,0,0,1047,0,0,10005,0,0,4815,0,0,8945,0,0,1536,0,0,13795,0,0,19251,0,0,19209,0,0,1605,6,51327,"WAT","HY" 14,25,1,1,,59,15,"HOLYOKE WTR PWR CO","RIVERSIDE",0,,8779,"0M",1294,,554,95,2283,0,0,798,0,0,2407,0,0,2806,0,0,1058,0,0,-32,0,0,-28,0,0,236,0,0,-31,0,0,991,0,0,1475,0,0,1658,0,0,1607,6,51327,"WAT","HY" 14,25,1,1,,59,20,"HOLYOKE WTR PWR CO","BOATLOCK",0,,8779,"0M",1294,,554,95,1401,0,0,440,0,0,1465,0,0,1749,0,0,-1985,0,0,-45,0,0,34,0,0,364,0,0,188,0,0,1015,0,0,1030,0,0,1719,0,0,1603,6,51327,"WAT","HY" 14,25,1,1,,59,21,"HOLYOKE WTR PWR CO","SKINNER",0,,8779,"0M",1294,,554,95,1087,0,0,-990,0,0,135,0,0,122,0,0,0,0,0,-3,0,0,-3,0,0,10,0,0,-5,0,0,48,0,0,88,0,0,144,0,0,1608,6,51327,"WAT","HY" 14,25,1,2,2,59,23,"HOLYOKE WTR PWR CO","MT TOM",0,"LIGHT OIL",8779,"0M",1294,,554,95,253,312,334,85,74,223,86,144,363,96,161,0,210,338,471,128,216,400,63,106,0,319,575,0,148,244,0,283,596,339,311,528,442,268,461,289,1606,6,51327,"FO2","ST" 14,25,1,2,6,59,23,"HOLYOKE WTR PWR CO","MT TOM",0,"BIT COAL",8779,"0M",1294,,554,95,83436,31625,65901,94304,36568,48767,100316,38568,48417,92219,34981,57613,86828,32256,68520,89522,33641,55040,96838,37232,50903,67013,26869,64337,58083,21428,72102,20300,9635,85211,75120,28714,96373,83498,33548,87268,1606,6,51327,"BIT","ST" 14,25,1,2,3,85,1,"MONTAUP ELECTRIC COMPANY","SOMERSET",0,"HEAVY OIL",12833,"0M",1294,,,95,5362,8778,70647,3605,6271,64376,3682,6389,57987,572,894,57093,4068,7388,49705,3861,6474,101371,1808,3090,98281,1729,8455,89825,4071,6826,83000,7484,12748,70251,8762,14647,55605,1259,3587,97942,1613,6,56511,"FO6","ST" 14,25,1,2,6,85,1,"MONTAUP ELECTRIC COMPANY","SOMERSET",0,"BIT COAL",12833,"0M",1294,,,95,57318,21462,76767,61443,26125,64290,61730,25219,52529,14739,5125,47404,25607,10149,50811,58410,21998,42203,65563,26654,42553,52228,21241,48670,53057,20314,65856,44642,17190,76089,48433,18499,83931,70559,26084,98563,1613,6,56511,"BIT","ST" 14,25,1,4,2,85,1,"MONTAUP ELECTRIC COMPANY","SOMERSET",0,"LIGHT OIL",12833,"0M",1294,,,95,143,374,5116,433,1118,3998,115,229,3769,65,186,3583,285,740,4510,629,1593,4110,1349,3410,5229,1777,4429,5348,136,348,5000,0,0,4999,5,26,5687,653,1369,4318,1613,6,56511,"FO2","GT" 14,25,1,3,2,90,15,"NANTUCKET ELEC CO","NANTUCKET",0,"LIGHT OIL",13206,"0M",1294,,,95,7539,12658,2602,7625,13184,8503,7218,12056,5494,6969,12757,2261,7465,13354,7937,7820,14759,9687,10453,19444,7486,10644,19689,5848,7894,13523,10626,6823,12246,7898,7832,14492,3042,9557,16800,2912,1615,6,51977,"FO2","IC" 14,25,1,1,,96,5,"NEW ENGLAND POWER CO","DEERFIELD 2",0,,13433,"0M",1294,,90,95,3908,0,0,2952,0,0,3971,0,0,2045,0,0,1064,0,0,520,0,0,442,0,0,617,0,0,404,0,0,2016,0,0,3583,0,0,2747,0,0,6047,6,52007,"WAT","HY" 14,25,1,1,,96,10,"NEW ENGLAND POWER CO","DEERFIELD 3",0,,13433,"0M",1294,,90,95,4040,0,0,3243,0,0,4233,0,0,2293,0,0,1182,0,0,848,0,0,445,0,0,722,0,0,460,0,0,1885,0,0,3570,0,0,3116,0,0,6083,6,52007,"WAT","HY" 14,25,1,1,,96,15,"NEW ENGLAND POWER CO","DEERFIELD 4",0,,13433,"0M",1294,,90,95,3691,0,0,2835,0,0,3555,0,0,1674,0,0,865,0,0,673,0,0,414,0,0,621,0,0,420,0,0,1920,0,0,3135,0,0,2638,0,0,6119,6,52007,"WAT","HY" 14,25,1,1,,96,20,"NEW ENGLAND POWER CO","DEERFIELD 5",0,,13433,"0M",1294,,90,95,8684,0,0,6946,0,0,8699,0,0,2314,0,0,807,0,0,564,0,0,515,0,0,177,0,0,0,0,0,0,0,0,3382,0,0,5810,0,0,1620,6,52007,"WAT","HY" 14,25,1,1,,96,25,"NEW ENGLAND POWER CO","SHERMAN",0,,13433,"0M",1294,,90,95,4117,0,0,3467,0,0,4264,0,0,1151,0,0,407,0,0,439,0,0,377,0,0,602,0,0,527,0,0,2183,0,0,3889,0,0,2917,0,0,6012,6,52007,"WAT","HY" 14,25,1,2,3,96,27,"NEW ENGLAND POWER CO","BRAYTON PT",0,"HEAVY OIL",13433,"0M",1294,,90,95,40093,74054,435541,65951,116563,318656,49098,75749,438283,41100,69916,368366,2212,5326,519600,0,0,519442,0,0,519401,488,4266,515767,0,0,516617,0,0,516584,7553,10954,505630,71672,125949,379784,1619,6,52007,"FO6","ST" 14,25,1,2,6,96,27,"NEW ENGLAND POWER CO","BRAYTON PT",0,"BIT COAL",13433,"0M",1294,,90,95,657136,245754,255528,538158,200282,277893,335153,130042,379361,336389,128159,523785,552184,203304,520224,709319,259373,461575,714608,267126,390587,681408,256270,431828,600517,222478,518312,676108,250140,322224,643066,226804,159986,692743,256541,166201,1619,6,52007,"BIT","ST" 14,25,1,2,9,96,27,"NEW ENGLAND POWER CO","BRAYTON PT",0,"NAT GAS",13433,"0M",1294,,90,95,2475,65992,0,19895,234494,0,87264,1046891,0,115149,1305242,0,165738,1925331,0,192541,2159965,0,121121,1465806,0,138514,1578722,0,90677,1067560,0,7950,208839,0,642,50267,0,499,65467,0,1619,6,52007,"NG","ST" 14,25,1,3,2,96,27,"NEW ENGLAND POWER CO","BRAYTON PT",0,"LIGHT OIL",13433,"0M",1294,,90,95,48,91,0,168,321,0,49,91,0,66,120,0,149,212,0,229,427,0,434,803,0,429,813,0,49,97,0,17,33,0,0,0,0,122,221,0,1619,6,52007,"FO2","IC" 14,25,1,2,3,96,33,"NEW ENGLAND POWER CO","SALEM HABR",0,"HEAVY OIL",13433,"0M",1294,,90,95,4216,6811,427550,19621,51462,372000,43825,80929,296042,52176,100975,196885,88546,157427,294207,74155,134469,405510,143472,245061,157683,78033,135040,315193,15952,29894,481681,10242,22800,451257,31856,63264,446411,130138,177251,300301,1626,6,52007,"FO6","ST" 14,25,1,2,6,96,33,"NEW ENGLAND POWER CO","SALEM HABR",0,"BIT COAL",13433,"0M",1294,,90,95,170230,67910,116594,174526,68827,87604,182421,75469,107334,180983,73494,87888,123760,53441,145441,149482,64633,132065,157915,67184,148469,169338,69504,116124,140768,59871,93091,133365,56779,72780,147538,65216,99054,158287,70574,72828,1626,6,52007,"BIT","ST" 14,25,1,3,2,96,40,"NEW ENGLAND POWER CO","GLOUCESTER",0,"LIGHT OIL",13433,"0M",1294,,90,95,180,400,1027,365,1056,1255,495,500,1183,191,320,863,798,1430,1148,331,615,1333,398,757,1219,767,1957,1197,100,165,1033,0,0,1031,2,3,1465,491,918,1190,1624,6,52007,"FO2","IC" 14,25,1,3,2,96,50,"NEW ENGLAND POWER CO","NEWBURYPORT",0,"LIGHT OIL",13433,"0M",1294,,90,95,23,31,898,242,431,942,1,0,943,124,222,720,79,135,986,279,516,828,384,714,746,466,834,770,24,47,723,5,10,715,0,0,929,200,360,998,1625,6,52007,"FO2","IC" 14,25,1,1,,96,55,"NEW ENGLAND POWER CO","FIFE BROOK",0,,13433,"0M",1294,,90,95,4107,0,0,3775,0,0,4880,0,0,1321,0,0,312,0,0,338,0,0,198,0,0,494,0,0,291,0,0,2274,0,0,4150,0,0,3161,0,0,8004,6,52007,"WAT","HY" 14,25,1,1,,96,60,"NEW ENGLAND POWER CO","BEAR SWAMP",0,"P-PUMPSTG",13433,"0M",1294,,90,95,-17861,61325,0,-15324,57381,0,-16082,58258,0,-15241,53916,0,-14630,56226,0,-16812,61971,0,-18159,63682,0,-15902,62948,0,-16995,61404,0,-17477,62001,0,-15650,58713,0,-16215,58454,0,8005,6,52007,"WAT","HY" 14,25,1,1,,145,5,"W MASSACHUSETTS ELEC CO","CABOT",0,,20455,"0M",1294,,555,95,27350,0,0,20962,0,0,33562,0,0,28813,0,0,2450,0,0,11373,0,0,5730,0,0,10888,0,0,1060,0,0,21360,0,0,32264,0,0,23532,0,0,1629,6,53266,"WAT","HY" 14,25,1,1,,145,10,"W MASSACHUSETTS ELEC CO","COBBLE MT",0,,20455,"0M",1294,,555,95,2687,0,0,2401,0,0,3134,0,0,1490,0,0,613,0,0,1371,0,0,1579,0,0,2606,0,0,404,0,0,934,0,0,679,0,0,2257,0,0,1630,6,53266,"WAT","HY" 14,25,1,1,,145,12,"W MASSACHUSETTS ELEC CO","DWIGHT",0,,20455,"0M",1294,,555,95,541,0,0,520,0,0,744,0,0,709,0,0,972,0,0,422,0,0,241,0,0,219,0,0,137,0,0,316,0,0,187,0,0,450,0,0,6378,6,53266,"WAT","HY" 14,25,1,1,,145,20,"W MASSACHUSETTS ELEC CO","GARDER FLS",0,,20455,"0M",1294,,555,95,1535,0,0,1501,0,0,2140,0,0,1273,0,0,591,0,0,393,0,0,159,0,0,373,0,0,244,0,0,740,0,0,1394,0,0,1292,0,0,1634,6,53266,"WAT","HY" 14,25,1,1,,145,30,"W MASSACHUSETTS ELEC CO","IND ORCHARD",0,,20455,"0M",1294,,555,95,1913,0,0,854,0,0,1614,0,0,786,0,0,661,0,0,177,0,0,8,0,0,59,0,0,4,0,0,434,0,0,1375,0,0,741,0,0,6379,6,53266,"WAT","HY" 14,25,1,1,,145,32,"W MASSACHUSETTS ELEC CO","PUTTS BRDGE",0,,20455,"0M",1294,,555,95,224,0,0,252,0,0,1368,0,0,249,0,0,550,0,0,741,0,0,249,0,0,393,0,0,186,0,0,1233,0,0,1150,0,0,251,0,0,1637,6,53266,"WAT","HY" 14,25,1,1,,145,33,"W MASSACHUSETTS ELEC CO","RED BRIDGE",0,,20455,"0M",1294,,555,95,2265,0,0,1259,0,0,1699,0,0,1592,0,0,1025,0,0,689,0,0,212,0,0,256,0,0,150,0,0,1248,0,0,7724,0,0,1271,0,0,1638,6,53266,"WAT","HY" 14,25,1,1,,145,35,"W MASSACHUSETTS ELEC CO","TURNERS FL",0,,20455,"0M",1294,,555,95,1180,0,0,-9,0,0,2580,0,0,457,0,0,2357,0,0,3,0,0,320,0,0,753,0,0,1529,0,0,1437,0,0,3487,0,0,96,0,0,6388,6,53266,"WAT","HY" 14,25,1,1,,145,37,"W MASSACHUSETTS ELEC CO","NORTHFLD MT",0,"P-PUMPSTG",20455,"0M",1294,,555,95,-40582,142177,0,-33131,122422,0,-34507,127754,0,-38191,123876,0,-53574,130653,0,-54650,139615,0,-65287,149806,0,-58299,150495,0,-60095,144418,0,-65178,152081,0,-51403,135668,0,-54958,140849,0,547,6,53266,"WAT","HY" 14,25,1,4,2,145,38,"W MASSACHUSETTS ELEC CO","DOREEN",0,"LIGHT OIL",20455,"0M",1294,,555,95,50,156,956,319,789,738,14,84,997,11,135,1029,31,63,967,166,460,863,117,360,1099,422,1231,1099,69,204,1073,-10,0,1073,34,122,951,162,418,771,1631,6,53266,"FO2","GT" 14,25,1,2,2,145,55,"W MASSACHUSETTS ELEC CO","W SPRINGFLD",0,"LIGHT OIL",20455,"0M",1294,,555,95,0,0,533,101,224,458,0,0,458,19,36,411,0,0,411,0,0,411,0,0,411,0,0,411,0,0,411,0,0,411,0,0,411,0,0,379,1642,6,53266,"FO2","ST" 14,25,1,2,3,145,55,"W MASSACHUSETTS ELEC CO","W SPRINGFLD",0,"HEAVY OIL",20455,"0M",1294,,555,95,3033,6175,75421,4119,8425,75374,344,607,80604,1867,3252,77352,19,33,77318,750,1321,75997,1456,2596,73401,758,1343,72058,0,0,72058,0,0,72923,2320,5181,76520,13739,24402,55074,1642,6,53266,"FO6","ST" 14,25,1,2,9,145,55,"W MASSACHUSETTS ELEC CO","W SPRINGFLD",0,"NAT GAS",20455,"0M",1294,,555,95,2167,27681,0,81,1046,0,24872,278755,0,28674,316564,0,33801,372726,0,33691,376470,0,34950,395433,0,39329,440670,0,21443,242289,0,3420,45099,0,110,1547,0,158,1773,0,1642,6,53266,"NG","ST" 14,25,1,4,2,145,55,"W MASSACHUSETTS ELEC CO","W SPRINGFLD",0,"LIGHT OIL",20455,"0M",1294,,555,95,45,159,682,84,220,801,-17,0,801,-12,0,801,-3,12,789,108,297,6777,282,717,1096,319,633,977,0,0,977,0,0,977,0,0,977,0,0,977,1642,6,53266,"FO2","GT" 14,25,1,4,2,145,60,"W MASSACHUSETTS ELEC CO","WOODLAND RD",0,"LIGHT OIL",20455,"0M",1294,,555,95,38,127,1027,218,623,814,3,20,1144,11,96,1048,22,56,992,219,604,924,341,963,1130,373,1030,1017,32,105,1090,-7,0,1090,5,59,1032,156,398,534,1643,6,53266,"FO2","GT" 14,25,5,3,2,532,5,"BRAINTREE (CITY OF)","POTTER",0,"LIGHT OIL",2144,"0M",1294,,,95,1,3,0,40,86,0,2,4,0,8,15,0,18,33,0,0,0,0,66,37,0,90,173,0,8,15,0,16,29,0,0,0,0,47,86,0,1660,6,50315,"FO2","IC" 14,25,5,5,9,532,5,"BRAINTREE (CITY OF)","POTTER",0,"WASTE HT",2144,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1660,6,50315,"NG","CC" 14,25,5,6,2,532,5,"BRAINTREE (CITY OF)","POTTER",0,"LIGHT OIL",2144,"0M",1294,,,95,597,1163,3860,1950,3916,4922,529,946,3897,722,1243,2632,0,0,2595,0,0,2595,0,0,0,0,0,0,0,0,0,418,803,0,0,0,0,563,1271,0,1660,6,50315,"FO2","CT" 14,25,5,6,9,532,5,"BRAINTREE (CITY OF)","POTTER",0,"NAT GAS",2144,"0M",1294,,,95,6985,76876,0,16116,164048,0,4161,42418,0,25648,268544,0,6647,61554,0,0,0,0,6439,68107,0,22225,231091,0,11633,125960,0,2826,30097,0,605,6473,0,2795,30378,0,1660,6,50315,"NG","CT" 14,25,5,1,,597,5,"HOLYOKE (CITY OF)","HOLYOKE",0,,8776,"0M",1294,,,95,1039,0,0,94,0,0,1200,0,0,538,0,0,244,0,0,216,0,0,169,0,0,308,0,0,243,0,0,308,0,0,843,0,0,63,0,0,9864,6,51325,"WAT","HY" 14,25,5,2,3,597,5,"HOLYOKE (CITY OF)","HOLYOKE",0,"HEAVY OIL",8776,"0M",1294,,,95,-34,8,21223,-7,161,18597,-32,0,17335,-149,242,9944,-157,0,11105,-26,144,12014,197,918,10400,173,751,10383,0,0,21744,-26,2,23445,-45,21,21407,48,571,24539,9864,6,51325,"FO6","ST" 14,25,5,2,9,597,5,"HOLYOKE (CITY OF)","HOLYOKE",0,"NAT GAS",8776,"0M",1294,,,95,-406,548,0,-47,7095,0,-432,0,0,-151,1508,0,-180,0,0,-82,2775,0,358,10343,0,495,13260,0,-282,0,0,-300,136,0,-310,907,0,116,8617,0,9864,6,51325,"NG","ST" 14,25,5,3,2,602,1,"HUDSON (CITY OF)","CHERRY ST",0,"LIGHT OIL",8973,"0A",1294,,,95,126,216,6535,468,801,5733,24,47,5687,49,79,5608,60,99,5509,136,242,5267,334,576,4687,237,442,10028,21,36,9992,0,0,9992,0,0,9992,0,613,9379,9038,6,51362,"FO2","IC" 14,25,5,3,9,602,1,"HUDSON (CITY OF)","CHERRY ST",0,"NAT GAS",8973,"0A",1294,,,95,16,177,0,0,0,0,0,0,0,27,276,0,223,2327,0,514,5353,0,813,8555,0,1067,10973,0,248,2679,0,0,0,0,0,0,0,0,0,0,9038,6,51362,"NG","IC" 14,25,5,3,2,613,1,"IPSWICH (CITY OF)","IPSWICH",0,"LIGHT OIL",9442,"0A",1294,,,95,3,144,1524,185,504,1020,-44,84,928,26,97,839,45,81,751,112,229,1817,221,430,1388,171,335,1053,42,71,981,0,0,1991,0,13,1901,70,285,1616,1670,6,51411,"FO2","IC" 14,25,5,3,9,613,1,"IPSWICH (CITY OF)","IPSWICH",0,"NAT GAS",9442,"0A",1294,,,95,0,0,0,0,0,0,-7,91,0,26,564,0,193,2049,0,356,4180,0,540,6225,0,488,5467,0,218,2149,0,0,0,0,0,164,0,0,0,0,1670,6,51411,"NG","IC" 14,25,5,3,2,630,20,"MARBLEHEAD (CITY OF)","COMM ST 2",0,"LIGHT OIL",11624,"0A",1294,,,95,0,0,134,30,54,153,0,0,124,1,4,109,8,23,86,22,43,163,30,67,96,40,77,139,3,3,134,0,0,129,0,0,107,16,31,153,6585,6,51769,"FO2","IC" 14,25,5,3,2,630,25,"MARBLEHEAD (CITY OF)","WILKINS STA",0,"LIGHT OIL",11624,"0A",1294,,,95,24,42,422,242,404,495,3,4,490,17,25,466,41,67,398,140,249,387,184,331,532,214,384,390,17,34,833,0,0,831,0,0,833,105,187,646,6586,6,51769,"FO2","IC" 14,25,5,4,2,640,5,"MASS MUN WHOLESALE ELEC","STONY BROOK",0,"LIGHT OIL",11806,"0M",1294,,,95,868,1812,0,3250,6760,0,1070,2159,0,1016,2152,0,1531,3641,0,3583,7206,0,6923,15010,0,5440,12228,0,1296,2825,0,251,525,0,0,0,0,2081,4355,0,6081,6,56516,"FO2","GT" 14,25,5,5,2,640,5,"MASS MUN WHOLESALE ELEC","STONY BROOK",0,"LIGHT OIL",11806,"0M",1294,,,95,4867,0,0,4882,0,0,1895,0,0,0,0,0,1645,0,0,1298,0,0,2909,0,0,2231,0,0,542,0,0,137,0,0,778,0,0,7866,0,0,6081,6,56516,"FO2","CC" 14,25,5,5,9,640,5,"MASS MUN WHOLESALE ELEC","STONY BROOK",0,"WASTE HT",11806,"0M",1294,,,95,667,6409,0,33,225,0,713,7903,0,38860,226425,0,32080,282829,0,30410,271547,0,30355,268417,0,22281,199679,0,16911,152536,0,13731,126250,0,649,6336,0,0,0,0,6081,6,56516,"NG","CC" 14,25,5,6,2,640,5,"MASS MUN WHOLESALE ELEC","STONY BROOK",0,"LIGHT OIL",11806,"0M",1294,,,95,16765,34499,275954,17076,35625,171066,1732,3145,164811,15194,31318,130811,4458,10049,117055,3259,6474,203614,7129,14689,223923,5719,12097,199458,1427,2966,193410,406,852,191674,2974,6318,192851,24527,50346,140778,6081,6,56516,"FO2","CT" 14,25,5,6,9,640,5,"MASS MUN WHOLESALE ELEC","STONY BROOK",0,"NAT GAS",11806,"0M",1294,,,95,2298,22081,0,33,225,0,7123,78947,0,38860,226425,0,85133,750563,0,75927,677993,0,74156,655728,0,57044,511219,0,44278,399380,0,38588,354794,0,2475,24166,0,0,0,0,6081,6,56516,"NG","CT" 14,25,5,4,2,668,10,"PEABODY (CITY OF)","WATERS RIVR",0,"LIGHT OIL",14605,"0M",1294,,,95,4,11,7009,461,990,6019,3,13,6006,114,218,5789,218,411,5378,259,572,4806,1447,3081,5724,79,204,5787,0,0,5770,0,0,5770,0,0,5770,751,1304,4214,1678,6,52270,"FO2","GT" 14,25,5,4,9,668,10,"PEABODY (CITY OF)","WATERS RIVR",0,"NAT GAS",14605,"0M",1294,,,95,71,948,0,818,8676,0,0,0,0,298,3898,0,500,6079,0,1161,14052,0,735,10563,0,2810,34245,0,871,10971,0,16,244,0,0,0,0,136,1612,0,1678,6,52270,"NG","GT" 14,25,5,3,2,695,1,"SHREWSBURY (CITY OF)","SHREWSBURY",0,"LIGHT OIL",17127,"0A",1294,,,95,-48,53,1717,-20,96,1621,-72,0,1621,-59,0,1621,-27,43,1577,28,133,1444,206,450,994,393,793,1630,-12,58,1571,-52,4,1568,-66,0,1568,5,146,1421,6125,6,52653,"FO2","IC" 14,25,5,2,3,711,10,"TAUNTON (CITY OF)","CLRY FLOOD",0,"HEAVY OIL",18488,"0M",1294,,,95,707,1487,45484,117,274,41056,124,1171,40232,227,881,38944,154,338,18232,1782,3821,13122,1997,4404,13146,1671,3714,26632,1017,1981,30701,285,1042,41468,209,665,43572,1269,2308,3691,1682,6,52885,"FO6","ST" 14,25,5,5,3,711,10,"TAUNTON (CITY OF)","CLRY FLOOD",0,"HEAVY OIL",18488,"0M",1294,,,95,2588,4259,0,3074,4987,0,7,71,0,264,1016,0,10569,21610,0,5376,8750,0,7132,10296,0,7761,11325,0,6430,8473,0,269,1218,0,135,435,0,7563,7563,0,1682,6,52885,"FO6","CC" 14,25,5,5,9,711,10,"TAUNTON (CITY OF)","CLRY FLOOD",0,"NAT GAS",18488,"0M",1294,,,95,0,0,0,88,2162,0,0,0,0,0,7,0,70,898,0,11828,118101,0,7953,72245,0,11517,102477,0,3409,38796,0,275,3743,0,0,0,0,0,0,0,1682,6,52885,"NG","CC" 14,25,5,6,2,711,10,"TAUNTON (CITY OF)","CLRY FLOOD",0,"LIGHT OIL",18488,"0M",1294,,,95,600,1721,500,1175,3321,414,0,10,405,0,0,405,23,155,250,230,719,0,424,1426,393,75,247,983,20,69,920,0,0,922,172,601,798,1596,4611,881,1682,6,52885,"FO2","CT" 14,25,5,6,3,711,10,"TAUNTON (CITY OF)","CLRY FLOOD",0,"HEAVY OIL",18488,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1682,6,52885,"FO6","CT" 14,25,5,6,9,711,10,"TAUNTON (CITY OF)","CLRY FLOOD",0,"NAT GAS",18488,"0M",1294,,,95,215,3547,0,0,0,0,0,0,0,9,220,0,91,2523,0,3269,55134,0,3573,59309,0,4974,79500,0,4776,58796,0,188,2751,0,2,41,0,0,0,0,1682,6,52885,"NG","CT" 15,44,1,3,2,59,1,"BLOCK ISLAND POWER CO","BLOCK ISL",0,"LIGHT OIL",1857,"0A",1294,,,95,640,929,1894,560,757,1368,454,801,1953,666,926,2412,871,1183,2384,728,1492,1815,1748,2173,1258,1686,2317,1251,852,1532,1104,890,1214,1044,683,904,1044,537,1042,1378,6567,6,50270,"FO2","IC" 15,44,1,2,3,60,5,"NEW ENGLAND POWER CO","MANCHSTR ST",0,"HEAVY OIL",13433,"0M",1294,,90,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,6954,6984,12805,21121,8031,15471,21089,11950,17787,9381,10642,17134,20900,3236,6,52007,"FO6","ST" 15,44,1,2,6,60,5,"NEW ENGLAND POWER CO","MANCHSTR ST",0,"BIT COAL",13433,"0M",1294,,90,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,3236,6,52007,"BIT","ST" 15,44,1,2,9,60,5,"NEW ENGLAND POWER CO","MANCHSTR ST",0,"NAT GAS",13433,"0M",1294,,90,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,185,6790,0,5496,108488,0,22180,283931,0,57696,544903,0,43911,426261,0,200212,1571059,0,273062,2060878,0,3236,6,52007,"NG","ST" 15,44,1,3,2,71,5,"NEWPORT ELECTRIC CORP","ELDRED",0,"LIGHT OIL",13549,"0A",1294,,,95,0,0,912,146,241,919,0,0,916,14,24,893,280,476,872,38,285,806,254,445,603,431,759,765,53,97,884,0,0,884,30,55,818,186,311,942,3240,6,52046,"FO2","IC" 15,44,1,3,2,71,15,"NEWPORT ELECTRIC CORP","JEPSON",0,"LIGHT OIL",13549,"0A",1294,,,95,10,19,1047,104,179,864,0,0,1112,13,24,1094,58,103,998,35,303,926,228,421,966,339,620,1037,31,56,977,0,0,977,0,0,977,162,273,920,3241,6,52046,"FO2","IC" 15,44,5,1,,600,1,"PROVIDENCE (CITY OF)","PROVIDENCE",0,,15440,"0A",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,3245,6,52404,"WAT","HY" 16,9,1,1,,21,1,"GILMAN BROTHERS CO","GILMAN",0,,6885,"0A",1294,"R",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,536,6,50309,"WAT","HY" 16,9,1,1,,37,5,"CONNECTICUT LGT & PWR CO","BULLS BRDGE",0,,4176,"0M",1294,,550,95,4542,0,0,3859,0,0,4535,0,0,4526,0,0,711,0,0,1545,0,0,596,0,0,576,0,0,83,0,0,3291,0,0,5258,0,0,4512,0,0,541,6,50651,"WAT","HY" 16,9,1,1,,37,15,"CONNECTICUT LGT & PWR CO","ROBERTSVLE",0,,4176,"0M",1294,,550,95,228,0,0,144,0,0,74,0,0,117,0,0,0,0,0,23,0,0,4,0,0,14,0,0,1,0,0,58,0,0,0,0,0,7,0,0,549,6,50651,"WAT","HY" 16,9,1,1,,37,20,"CONNECTICUT LGT & PWR CO","ROCKY RIVER",0,"C-PUMPSTG",4176,"0M",1294,,550,95,-532,573,0,-108,831,0,-5011,4942,0,-3890,3881,0,-2483,2464,0,-30,0,0,-50,160,0,-45,941,0,-34,0,0,-295,262,0,3242,0,0,3543,0,0,539,6,50651,"WAT","HY" 16,9,1,1,,37,25,"CONNECTICUT LGT & PWR CO","SCOTLAND DM",0,,4176,"0M",1294,,550,95,1196,0,0,762,0,0,1285,0,0,753,0,0,65,0,0,169,0,0,32,0,0,83,0,0,9,0,0,401,0,0,43,0,0,524,0,0,551,6,50651,"WAT","HY" 16,9,1,1,,37,28,"CONNECTICUT LGT & PWR CO","SHEPAUG",0,,4176,"0M",1294,,550,95,19987,0,0,8510,0,0,16746,0,0,8668,0,0,479,0,0,3113,0,0,1323,0,0,1665,0,0,561,0,0,4280,0,0,17593,0,0,9586,0,0,552,6,50651,"WAT","HY" 16,9,1,1,,37,30,"CONNECTICUT LGT & PWR CO","STEVENSON",0,,4176,"0M",1294,,550,95,14594,0,0,6873,0,0,12878,0,0,7022,0,0,5946,0,0,2333,0,0,1155,0,0,1565,0,0,585,0,0,7574,0,0,15018,0,0,7269,0,0,553,6,50651,"WAT","HY" 16,9,1,1,,37,33,"CONNECTICUT LGT & PWR CO","TAFTVILLE",0,,4176,"0M",1294,,550,95,1047,0,0,773,0,0,1181,0,0,662,0,0,0,0,0,286,0,0,106,0,0,168,0,0,58,0,0,376,0,0,802,0,0,539,0,0,554,6,50651,"WAT","HY" 16,9,1,1,,37,35,"CONNECTICUT LGT & PWR CO","TUNNEL",0,,4176,"0M",1294,,550,95,1344,0,0,790,0,0,1127,0,0,808,0,0,808,0,0,130,0,0,51,0,0,62,0,0,13,0,0,528,0,0,1238,0,0,756,0,0,557,6,50651,"WAT","HY" 16,9,1,4,2,37,35,"CONNECTICUT LGT & PWR CO","TUNNEL",0,"LIGHT OIL",4176,"0M",1294,,550,95,92,241,1121,148,413,1052,-10,0,1052,8,34,1017,-9,0,1017,174,492,1054,399,1075,1028,391,1123,1060,-10,0,1060,-9,0,1060,-8,0,1060,247,642,1013,557,6,50651,"FO2","GT" 16,9,1,4,2,37,37,"CONNECTICUT LGT & PWR CO","COS COB",0,"LIGHT OIL",4176,"0M",1294,,550,95,338,879,6366,1004,2550,5530,-6,0,6730,61,328,6402,100,252,6836,1043,2766,6164,1606,4183,6744,1574,4512,6417,89,372,6045,10,115,5931,-7,47,5884,478,1250,6205,542,6,50651,"FO2","GT" 16,9,1,2,2,37,40,"CONNECTICUT LGT & PWR CO","DEVON",0,"LIGHT OIL",4176,"0M",1294,,550,95,4,7,607,26,48,738,10,19,719,8,14,705,6,12,693,5,10,683,12,21,662,5,10,652,35,67,586,12,21,564,10,19,545,126,250,652,544,6,50651,"FO2","ST" 16,9,1,2,3,37,40,"CONNECTICUT LGT & PWR CO","DEVON",0,"HEAVY OIL",4176,"0M",1294,,550,95,1691,2896,140820,5317,8938,131882,6310,10503,160145,2309,3909,156236,1040,1748,154488,1026,1746,152742,366,624,152118,0,0,152118,0,0,152118,1119,1895,186866,0,0,223227,52715,95704,164704,544,6,50651,"FO6","ST" 16,9,1,2,9,37,40,"CONNECTICUT LGT & PWR CO","DEVON",0,"NAT GAS",4176,"0M",1294,,550,95,139882,1480772,0,125833,1333372,0,140034,1484076,0,74718,805341,0,129292,1364215,0,113222,1209824,0,134347,1440396,0,141005,1520883,0,84240,919763,0,92690,988325,0,85651,910220,0,1027,11734,0,544,6,50651,"NG","ST" 16,9,1,4,2,37,40,"CONNECTICUT LGT & PWR CO","DEVON",0,"LIGHT OIL",4176,"0M",1294,,550,95,-8,0,826,52,143,1016,-6,0,1016,11,41,975,15,50,924,93,252,873,213,464,899,323,840,1155,12,42,1113,14,46,864,-8,0,864,126,312,755,544,6,50651,"FO2","GT" 16,9,1,2,2,37,45,"CONNECTICUT LGT & PWR CO","MONTVILLE",0,"LIGHT OIL",4176,"0M",1294,,550,95,79,187,224,71,184,282,0,0,277,35,81,316,26,52,254,126,275,254,225,460,205,169,342,281,13,78,193,-9,27,344,11,35,57,248,530,404,546,6,50651,"FO2","ST" 16,9,1,2,3,37,45,"CONNECTICUT LGT & PWR CO","MONTVILLE",0,"HEAVY OIL",4176,"0M",1294,,550,95,19404,42123,179930,11903,28403,229734,496,984,267130,8852,18669,287361,73,131,287230,16090,31789,255441,33046,60820,194621,29759,54794,250449,448,2452,286041,-459,1261,284780,4782,14127,272628,50192,96782,219079,546,6,50651,"FO6","ST" 16,9,1,2,9,37,45,"CONNECTICUT LGT & PWR CO","MONTVILLE",0,"NAT GAS",4176,"0M",1294,,550,95,2644,35575,0,1337,19886,0,14239,177907,0,15760,209674,0,26332,300080,0,15321,191070,0,33080,384304,0,29657,341116,0,660,22744,0,-410,7132,0,948,17617,0,2622,31910,0,546,6,50651,"NG","ST" 16,9,1,3,2,37,45,"CONNECTICUT LGT & PWR CO","MONTVILLE",0,"LIGHT OIL",4176,"0M",1294,,550,95,5,11,429,51,91,429,3,5,429,21,47,429,5,10,429,32,60,429,47,88,429,44,82,429,5,10,429,0,0,429,7,15,429,14,27,429,546,6,50651,"FO2","IC" 16,9,1,2,2,37,46,"CONNECTICUT LGT & PWR CO","NORWALK HAR",0,"LIGHT OIL",4176,"0M",1294,,550,95,1942,3751,1166,1049,1831,1166,1411,2570,1166,801,1409,746,830,1566,1275,1306,2393,1275,1212,2164,1208,1005,1793,1129,448,996,1090,743,1549,1201,1863,3623,816,1573,2830,1073,548,6,50651,"FO2","ST" 16,9,1,2,3,37,46,"CONNECTICUT LGT & PWR CO","NORWALK HAR",0,"HEAVY OIL",4176,"0M",1294,,550,95,61485,109340,281515,116317,186438,251428,53269,89422,277523,112195,177490,244461,49615,86635,387526,72024,117143,423659,87276,142042,395624,69104,110519,365065,12764,26032,444868,12966,24423,458286,56112,97835,437824,98414,160154,343905,548,6,50651,"FO6","ST" 16,9,1,4,2,37,46,"CONNECTICUT LGT & PWR CO","NORWALK HAR",0,"LIGHT OIL",4176,"0M",1294,"R",550,95,0,0,0,0,0,0,-12,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,548,6,50651,"FO2","GT" 16,9,1,1,,37,60,"CONNECTICUT LGT & PWR CO","BANTAM",0,,4176,"0M",1294,,550,95,166,0,0,122,0,0,177,0,0,99,0,0,0,0,0,24,0,0,2,0,0,9,0,0,0,0,0,66,0,0,182,0,0,126,0,0,6457,6,50651,"WAT","HY" 16,9,1,1,,37,65,"CONNECTICUT LGT & PWR CO","FLS VILLAGE",0,,4176,"0M",1294,,550,95,6485,0,0,3067,0,0,6148,0,0,4269,0,0,57,0,0,1043,0,0,359,0,0,386,0,0,86,0,0,3283,0,0,6134,0,0,3241,0,0,560,6,50651,"WAT","HY" 16,9,1,4,2,37,70,"CONNECTICUT LGT & PWR CO","FRANKLIN DR",0,"LIGHT OIL",4176,"0M",1294,,550,95,87,251,1073,112,303,770,-21,0,770,6,41,429,9,45,1229,156,508,1033,386,937,931,385,1480,880,-11,0,808,-12,0,808,-14,0,0,109,306,1000,561,6,50651,"FO2","GT" 16,9,1,2,2,37,75,"CONNECTICUT LGT & PWR CO","MIDDLETOWN",0,"LIGHT OIL",4176,"0M",1294,,550,95,52,116,72,106,200,205,37,72,134,69,119,181,93,171,177,62,115,62,142,274,121,143,283,195,159,331,184,25,61,123,89,174,116,58,124,159,562,6,50651,"FO2","ST" 16,9,1,2,3,37,75,"CONNECTICUT LGT & PWR CO","MIDDLETOWN",0,"HEAVY OIL",4176,"0M",1294,,550,95,28156,57773,619646,82338,144562,470965,28954,52136,494722,112799,180932,367774,91771,154447,321716,103385,178821,285273,180564,315539,192342,120265,219668,308678,14240,27382,395204,9172,20697,432521,29631,53865,465010,116423,197687,379501,562,6,50651,"FO6","ST" 16,9,1,4,2,37,75,"CONNECTICUT LGT & PWR CO","MIDDLETOWN",0,"LIGHT OIL",4176,"0M",1294,,550,95,0,0,986,60,155,998,2,12,986,0,0,986,18,56,1096,133,235,803,220,518,962,326,864,969,6,21,948,0,0,946,0,0,936,0,0,936,562,6,50651,"FO2","GT" 16,9,1,2,"C",37,80,"CONNECTICUT LGT & PWR CO","S MEADOW",0,"REFUSE",4176,"0M",1294,,550,95,36668,0,0,31584,0,0,30750,0,0,36558,0,0,4988,0,0,38064,0,0,35273,0,0,35840,0,0,37803,0,0,39379,0,0,36583,0,0,40236,0,0,563,6,50651,"GEO","ST" 16,9,1,4,2,37,80,"CONNECTICUT LGT & PWR CO","S MEADOW",0,"LIGHT OIL",4176,"0M",1294,,550,95,547,1286,33605,2263,5797,27807,-4,195,27613,257,794,4952,465,1373,43574,2527,6621,35953,4081,8784,28189,3486,11650,34410,234,1143,29931,-49,0,29931,56,271,29660,2479,6072,23588,563,6,50651,"FO2","GT" 16,9,1,4,2,37,85,"CONNECTICUT LGT & PWR CO","TORRINGTN T",0,"LIGHT OIL",4176,"0M",1294,,550,95,80,183,802,-19,0,802,9,49,753,4,24,729,-6,0,1062,163,373,867,4081,6864,28189,583,1059,947,4,16,931,-7,0,931,-8,0,931,173,446,1006,565,6,50651,"FO2","GT" 16,9,1,4,2,37,90,"CONNECTICUT LGT & PWR CO","BRANFORD",0,"LIGHT OIL",4176,"0M",1294,,550,95,-23,0,993,-11,0,993,-12,0,983,-9,0,993,-12,0,993,-15,0,963,303,888,1170,580,1248,981,112,115,1073,-7,12,1061,12,62,999,103,312,1042,540,6,50651,"FO2","GT" 16,9,1,2,1,45,1,"CONN YANKEE ATOMIC PWR CO","HADDAM NECK",0,"NUCLEAR",4187,"0M",1294,,551,95,349804,0,0,-2724,0,0,-2714,0,0,80321,0,0,411060,0,0,385019,0,0,346822,0,0,397229,0,0,404771,0,0,427136,0,0,421633,0,0,435253,0,0,558,6,50652,"UR","ST" 16,9,1,1,,70,1,"FARMINGTON RIVER POWER CO","RAINBOW",0,,6207,"0A",1294,,,95,4465,0,0,2602,0,0,3654,0,0,2574,0,0,1712,0,0,1108,0,0,787,0,0,842,0,0,700,0,0,2530,0,0,4222,0,0,2756,0,0,559,6,50970,"WAT","HY" 16,9,1,2,1,85,1,"NORTHEAST NUCL ENERGY CO","MILLSTONE",0,"NUCLEAR",21687,"0M",1294,,553,95,474794,0,0,424364,0,0,479164,0,0,452923,0,0,470915,0,0,397551,0,0,307242,0,0,369216,0,0,459416,0,0,478184,0,0,46176,0,0,-2630,0,0,566,6,50005,"UR","ST" 16,9,1,2,1,85,2,"NORTHEAST NUCL ENERGY CO","MILLSTONE",0,"NUCLEAR",21687,"0M",1294,,553,95,-2968,0,0,-3117,0,0,-2841,0,0,12840,0,0,0,0,0,0,0,0,-8427,0,0,340333,0,0,625348,0,0,645987,0,0,618792,0,0,511064,0,0,566,6,50005,"UR","ST" 16,9,1,2,1,85,3,"NORTHEAST NUCL ENERGY CO","MILLSTONE",0,"NUCLEAR",21687,"0M",1294,,553,95,853882,0,0,758672,0,0,851613,0,0,328284,0,0,0,0,0,594786,0,0,853005,0,0,844847,0,0,822134,0,0,852985,0,0,817800,0,0,422956,0,0,566,6,50005,"UR","ST" 16,9,1,2,2,159,3,"UNITED ILLUMINATING CO","BRDGEPT HBR",0,"LIGHT OIL",19497,"0M",1294,,,95,289,498,533,83,144,555,103,183,538,278,575,297,94,164,466,159,276,523,127,224,632,239,436,363,60,105,591,207,368,557,52,92,465,58,101,530,568,6,53003,"FO2","ST" 16,9,1,2,3,159,3,"UNITED ILLUMINATING CO","BRDGEPT HBR",0,"HEAVY OIL",19497,"0M",1294,,,95,12678,20036,157706,31465,49414,142873,1716,2749,140124,28015,51807,143380,11615,18496,124884,34707,55499,150609,43253,69685,122107,18699,30642,149294,6814,10677,163242,4908,7842,155400,4195,6665,148735,54634,86347,0,568,6,53003,"FO6","ST" 16,9,1,2,6,159,3,"UNITED ILLUMINATING CO","BRDGEPT HBR",0,"BIT COAL",19497,"0M",1294,,,95,193441,73716,182983,223214,85285,166858,221070,86802,148636,4755,2176,201542,224862,86475,170775,217578,84500,168741,225684,88542,121774,166492,67303,123827,199715,77070,157924,143992,56780,199095,198867,77375,176894,249682,95223,163986,568,6,53003,"BIT","ST" 16,9,1,4,2,159,3,"UNITED ILLUMINATING CO","BRDGEPT HBR",0,"LIGHT OIL",19497,"0M",1294,,,95,4,8,549,151,259,469,0,0,647,5,12,635,10,18,617,12,22,595,145,256,696,308,560,493,63,111,560,0,0,560,9,16,545,75,130,594,568,6,53003,"FO2","GT" 16,9,1,2,2,159,5,"UNITED ILLUMINATING CO","ENGLISH",0,"LIGHT OIL",19497,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,569,6,53003,"FO2","ST" 16,9,1,2,3,159,5,"UNITED ILLUMINATING CO","ENGLISH",0,"HEAVY OIL",19497,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,569,6,53003,"FO6","ST" 16,9,1,2,2,159,12,"UNITED ILLUMINATING CO","N HAVEN HBR",0,"LIGHT OIL",19497,"0M",1294,,,95,876,1540,484,437,731,468,424,737,445,327,564,583,511,892,406,254,441,667,361,632,570,401,702,762,359,651,646,23,502,680,959,1741,546,779,1314,482,6156,6,53003,"FO2","ST" 16,9,1,2,3,159,12,"UNITED ILLUMINATING CO","N HAVEN HBR",0,"HEAVY OIL",19497,"0M",1294,,,95,104071,166097,286634,171042,260046,151260,95848,151028,241794,147390,227183,379543,69013,110799,306351,74009,117219,286218,97251,153426,333078,88533,139665,374595,39346,64393,310202,163,3184,307018,72476,120773,186245,162959,252660,0,6156,6,53003,"FO6","ST" 16,9,1,2,9,159,12,"UNITED ILLUMINATING CO","N HAVEN HBR",0,"NAT GAS",19497,"0M",1294,,,95,0,0,0,0,0,0,31250,307224,0,64504,630374,0,76077,749979,0,81590,800742,0,99404,985733,0,49501,489902,0,13044,134068,0,34,4180,0,0,0,0,0,0,0,6156,6,53003,"NG","ST" 16,9,5,1,,556,5,"NORWICH (CITY OF)","SECOND ST",0,,13831,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,5,0,0,174,0,0,101,0,0,67,0,0,17,0,0,180,0,0,272,0,0,324,0,0,580,6,52123,"WAT","HY" 16,9,5,1,,556,10,"NORWICH (CITY OF)","OCCUM",0,,13831,"0A",1294,,,95,516,0,0,356,0,0,529,0,0,370,0,0,225,0,0,257,0,0,63,0,0,95,0,0,42,0,0,215,0,0,420,0,0,292,0,0,582,6,52123,"WAT","HY" 16,9,5,1,,556,13,"NORWICH (CITY OF)","TENTH ST",0,,13831,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,83,0,0,0,0,0,113,0,0,54,0,0,255,0,0,534,0,0,636,0,0,583,6,52123,"WAT","HY" 16,9,5,4,2,556,20,"NORWICH (CITY OF)","N MAIN ST",0,"LIGHT OIL",13831,"0A",1294,,,95,0,0,1935,53,168,1767,0,0,1767,0,0,1767,23,56,1711,62,161,1550,402,1007,1693,531,1325,1518,0,0,1518,0,0,1518,0,0,1518,117,296,2388,581,6,52123,"FO2","GT" 16,9,5,3,2,560,1,"SOUTH NORWALK (CITY OF)","SO NORWALK",0,"LIGHT OIL",17569,"0A",1294,,,95,50,90,1114,84,147,1614,27,49,1523,27,45,1455,71,123,1331,70,125,1235,242,444,819,209,351,1604,20,34,1570,2,4,1736,9,13,1671,98,158,1418,6598,6,52704,"FO2","IC" 16,9,5,2,3,567,1,"WALLINGFORD (CITY OF)","PIERCE",0,"HEAVY OIL",20038,"0A",1294,,,95,0,15,1540,368,1067,2318,0,0,2318,0,0,2318,0,0,2318,0,0,2318,0,0,2318,0,0,2318,146,445,1873,0,0,1873,0,0,1873,0,0,1873,6635,6,53175,"FO6","ST" 21,36,1,1,,35,10,"CENTRAL HUDSON GAS & ELEC","DASHVILLE",0,,3249,"0M",1294,,,95,2381,0,0,502,0,0,1130,0,0,814,0,0,844,0,0,273,0,0,156,0,0,52,0,0,6,0,0,1173,0,0,1735,0,0,901,0,0,2481,6,50484,"WAT","HY" 21,36,1,1,,35,18,"CENTRAL HUDSON GAS & ELEC","NEVERSINK",0,,3249,"0M",1294,,,95,4408,0,0,4221,0,0,4645,0,0,2716,0,0,2618,0,0,2849,0,0,10968,0,0,9289,0,0,3298,0,0,2724,0,0,2482,0,0,4970,0,0,2483,6,50484,"WAT","HY" 21,36,1,1,,35,20,"CENTRAL HUDSON GAS & ELEC","STURGEON PL",0,,3249,"0M",1294,,,95,9300,0,0,4140,0,0,8251,0,0,4665,0,0,3127,0,0,1123,0,0,872,0,0,359,0,0,111,0,0,5834,0,0,7954,0,0,3663,0,0,2486,6,50484,"WAT","HY" 21,36,1,2,3,35,25,"CENTRAL HUDSON GAS & ELEC","DANSKAMMER",0,"HEAVY OIL",3249,"0M",1294,,,95,0,0,10567,2887,4585,13091,0,0,13091,0,0,13091,377,619,12472,1176,2123,10349,198,406,9943,0,0,9943,0,0,9943,0,0,9943,16,30,9913,0,0,9913,2480,6,50484,"FO6","ST" 21,36,1,2,6,35,25,"CENTRAL HUDSON GAS & ELEC","DANSKAMMER",0,"BIT COAL",3249,"0M",1294,,,95,180547,67912,176943,208851,77841,149786,144579,54893,173619,180437,67955,164986,58267,23110,161831,149627,57630,163884,131893,51114,152154,127793,49654,170960,144488,55872,134561,60315,24424,150152,137406,60589,138420,208309,77898,129136,2480,6,50484,"BIT","ST" 21,36,1,2,9,35,25,"CENTRAL HUDSON GAS & ELEC","DANSKAMMER",0,"NAT GAS",3249,"0M",1294,,,95,12788,136338,0,5348,58875,0,52133,554622,0,1003,12881,0,26410,269381,0,9355,110458,0,50047,563362,0,64005,727957,0,42268,475832,0,72329,806049,0,21208,238996,0,526,5007,0,2480,6,50484,"NG","ST" 21,36,1,3,2,35,25,"CENTRAL HUDSON GAS & ELEC","DANSKAMMER",0,"LIGHT OIL",3249,"0M",1294,,,95,38,70,119,10,15,278,29,38,240,10,9,231,5,9,222,30,55,167,29,60,281,48,81,200,48,99,274,48,83,191,38,76,289,9,16,273,2480,6,50484,"FO2","IC" 21,36,1,4,2,35,35,"CENTRAL HUDSON GAS & ELEC","SOUTH CAIRO",0,"LIGHT OIL",3249,"0M",1294,,,95,74,178,2486,0,0,2486,0,0,2486,0,0,2486,13,31,2455,198,577,1878,16,34,1844,70,197,1647,0,0,2719,0,0,2719,39,93,2626,18,49,2577,2485,6,50484,"FO2","GT" 21,36,1,4,2,35,40,"CENTRAL HUDSON GAS & ELEC","W COXSACKIE",0,"LIGHT OIL",3249,"0M",1294,,,95,0,0,2176,0,0,2176,0,0,2176,0,0,2176,0,0,2176,0,0,2176,0,0,2176,0,0,2176,0,0,2176,0,0,2176,0,0,2176,0,0,2176,2487,6,50484,"FO2","GT" 21,36,1,4,9,35,40,"CENTRAL HUDSON GAS & ELEC","W COXSACKIE",0,"NAT GAS",3249,"0M",1294,,,95,90,1181,0,32,427,0,0,0,0,45,632,0,59,962,0,631,9351,0,109,1557,0,530,7243,0,0,0,0,52,789,0,180,2430,0,69,1043,0,2487,6,50484,"NG","GT" 21,36,1,2,2,35,45,"CENTRAL HUDSON GAS & ELEC","ROSETON JO",0,"LIGHT OIL",3249,"0M",1294,,,95,1744,3069,2289,782,1361,3014,1071,2036,2369,0,0,2542,0,0,2542,0,0,2542,0,0,2542,0,0,2542,0,0,2542,0,17,2525,654,2512,1229,581,1004,2137,8006,6,50484,"FO2","ST" 21,36,1,2,3,35,45,"CENTRAL HUDSON GAS & ELEC","ROSETON JO",0,"HEAVY OIL",3249,"0M",1294,,,95,49649,80148,781308,157108,249990,495225,13890,23984,478029,0,0,478029,0,0,478029,0,0,604069,0,0,604069,0,0,604069,0,0,604069,0,0,589640,1356,4755,599314,189513,299562,451927,8006,6,50484,"FO6","ST" 21,36,1,2,9,35,45,"CENTRAL HUDSON GAS & ELEC","ROSETON JO",0,"NAT GAS",3249,"0M",1294,,,95,33526,336575,0,69660,692555,0,24026,260204,0,0,0,0,177930,1880760,0,186946,1950511,0,310122,3310810,0,247281,2627847,0,0,0,0,0,0,0,2849,61824,0,7068,69278,0,8006,6,50484,"NG","ST" 21,36,1,1,,35,50,"CENTRAL HUDSON GAS & ELEC","HIGH FALLS",0,,3249,"0M",1294,,,95,1184,0,0,92,0,0,1122,0,0,69,0,0,143,0,0,23,0,0,26,0,0,0,0,0,0,0,0,340,0,0,1057,0,0,170,0,0,579,6,50484,"WAT","HY" 21,36,1,1,,37,5,"CENTRAL VT PUB SERV CORP","CARVERS FLS",0,,3292,"0A",1294,,350,95,921,0,0,597,0,0,1182,0,0,1121,0,0,691,0,0,250,0,0,18,0,0,58,0,0,0,0,0,391,0,0,1196,0,0,502,0,0,6456,6,50503,"WAT","HY" 21,36,1,2,3,40,1,"CONSOL EDISON CO N Y INC","ARTHUR KILL",0,"HEAVY OIL",4226,"0M",1294,,,95,0,0,5711,0,0,5711,0,0,5711,0,0,5711,0,0,5711,0,0,5711,0,0,5711,7328,11940,18519,0,0,18519,0,0,18519,0,0,18513,0,0,18513,2490,6,50653,"FO6","ST" 21,36,1,2,9,40,1,"CONSOL EDISON CO N Y INC","ARTHUR KILL",0,"NAT GAS",4226,"0M",1294,,,95,-1408,17220,0,-1393,16473,0,-1276,5546,0,42517,495291,0,55216,582417,0,194234,1938196,0,301093,2957985,0,278373,2754690,0,147636,1480827,0,-1783,3561,0,-1398,5,0,-1433,5,0,2490,6,50653,"NG","ST" 21,36,1,4,2,40,1,"CONSOL EDISON CO N Y INC","ARTHUR KILL",0,"LIGHT OIL",4226,"0M",1294,,,95,13,44,1913,67,194,1823,0,0,1823,36,79,1744,215,635,1882,298,918,2083,566,1739,2154,371,1201,1884,0,0,0,0,0,0,0,0,0,0,0,0,2490,6,50653,"FO2","GT" 21,36,1,2,1,40,2,"CONSOL EDISON CO N Y INC","INDIAN PT",0,"NUCLEAR",4226,"0M",1294,,,95,562851,0,0,52711,0,0,-6970,0,0,-3790,0,0,-13730,0,0,241777,0,0,674078,0,0,678357,0,0,681364,0,0,661697,0,0,694091,0,0,636105,0,0,2497,6,50653,"UR","ST" 21,36,1,2,3,40,3,"CONSOL EDISON CO N Y INC","ASTORIA",0,"HEAVY OIL",4226,"0M",1294,,,95,44284,69523,204071,87234,136417,162405,51168,80603,150832,37361,58624,135192,36339,59441,192317,36196,59149,130130,89762,143025,106180,87335,138221,98117,59995,93814,117887,54037,87216,125085,64568,101738,117638,289554,461968,161157,8906,6,50653,"FO6","ST" 21,36,1,2,9,40,3,"CONSOL EDISON CO N Y INC","ASTORIA",0,"NAT GAS",4226,"0M",1294,,,95,270672,2666431,0,244705,2376465,0,354262,3528212,0,241575,2383868,0,275033,2732177,0,466083,4630924,0,417404,4132582,0,422777,4216725,0,331846,3235732,0,333120,3377003,0,267480,2653281,0,78615,787377,0,8906,6,50653,"NG","ST" 21,36,1,4,2,40,3,"CONSOL EDISON CO N Y INC","ASTORIA",0,"LIGHT OIL",4226,"0M",1294,,,95,1484,3523,70541,935,2176,68112,695,1314,66869,1270,3125,63744,1033,2385,61076,1517,3666,57410,5121,12698,44790,1655,4191,48468,794,1989,67296,758,1842,65454,651,1541,63965,4785,11328,52945,8906,6,50653,"FO2","GT" 21,36,1,4,9,40,3,"CONSOL EDISON CO N Y INC","ASTORIA",0,"NAT GAS",4226,"0M",1294,,,95,1238,16825,0,4723,63317,0,9436,102713,0,19761,279920,0,13199,175023,0,14602,203072,0,50641,721027,0,30754,443611,0,22755,324431,0,10683,150198,0,29807,410036,0,1300,17862,0,8906,6,50653,"NG","GT" 21,36,1,2,3,40,5,"CONSOL EDISON CO N Y INC","EAST RIVER",0,"HEAVY OIL",4226,"0M",1294,,,95,48411,100447,260377,52328,112594,251467,22577,46041,196293,14368,29471,111609,10915,20599,75923,9443,18148,129321,17347,33410,143239,17145,35799,154704,57,119,208820,391,883,155405,24581,53489,125358,26299,56899,135819,2493,6,50653,"FO6","ST" 21,36,1,2,9,40,5,"CONSOL EDISON CO N Y INC","EAST RIVER",0,"NAT GAS",4226,"0M",1294,,,95,22936,297706,0,16423,222129,0,33740,432005,0,32894,424765,0,83114,976015,0,52018,626673,0,74759,901280,0,43540,571392,0,62070,814818,0,38780,549257,0,26334,362630,0,4079,55677,0,2493,6,50653,"NG","ST" 21,36,1,2,3,40,8,"CONSOL EDISON CO N Y INC","59TH STREET",0,"HEAVY OIL",4226,"0M",1294,,,95,134,711,28019,-168,0,13932,-186,0,17029,-180,0,14663,-186,0,16921,-180,0,14962,-186,0,34238,-186,0,28013,0,0,18655,-186,0,24175,-180,0,21506,-186,0,15408,2503,6,50653,"FO6","ST" 21,36,1,2,9,40,8,"CONSOL EDISON CO N Y INC","59TH STREET",0,"NAT GAS",4226,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,-180,0,0,0,0,0,0,0,0,0,0,0,2503,6,50653,"NG","ST" 21,36,1,4,2,40,8,"CONSOL EDISON CO N Y INC","59TH STREET",0,"LIGHT OIL",4226,"0M",1294,,,95,0,0,2421,12,43,2379,0,0,2379,34,63,2315,382,920,2169,220,532,2101,517,1422,2132,154,399,2018,0,0,2018,0,0,2018,0,0,2019,0,0,2019,2503,6,50653,"FO2","GT" 21,36,1,4,2,40,10,"CONSOL EDISON CO N Y INC","GOWANUS",0,"LIGHT OIL",4226,"0M",1294,,,95,3431,10187,54995,3032,8863,61517,3332,9885,51514,5596,16946,54888,9656,30399,58173,10867,35156,51183,35078,112111,54362,18095,69179,54055,9925,32320,51120,3062,9091,61678,11850,35551,63660,11082,31386,52408,2494,6,50653,"FO2","GT" 21,36,1,4,2,40,17,"CONSOL EDISON CO N Y INC","INDIAN PT",0,"LIGHT OIL",4226,"0M",1294,,,95,10,470,1357,110,334,1476,0,0,1438,10,26,1387,190,648,1553,120,502,1367,618,1994,1429,339,1276,1561,10,65,1518,10,49,1466,70,568,1361,10,79,1524,2497,6,50653,"FO2","GT" 21,36,1,2,3,40,18,"CONSOL EDISON CO N Y INC","HUDSON AVE",0,"HEAVY OIL",4226,"0M",1294,,,95,13942,16640,116475,22892,27677,121761,19571,25683,88715,5881,7513,112117,13579,17821,145862,8960,11221,121321,17004,23012,156902,16358,21789,184711,8488,11589,233738,9039,12876,207818,15377,22058,190563,21649,30797,210122,2496,6,50653,"FO6","ST" 21,36,1,4,2,40,18,"CONSOL EDISON CO N Y INC","HUDSON AVE",0,"LIGHT OIL",4226,"0M",1294,,,95,32,106,3790,262,520,3270,24,63,4088,0,0,4088,318,932,4131,366,1254,4363,1154,3982,3948,684,2253,4361,44,148,4212,7,28,4185,255,954,4157,0,0,4471,2496,6,50653,"FO2","GT" 21,36,1,4,2,40,23,"CONSOL EDISON CO N Y INC","NARROWS BAY",0,"LIGHT OIL",4226,"0M",1294,,,95,1815,5002,70995,2374,6488,64363,3121,8503,70742,4829,13085,57595,4696,13259,61188,7112,20641,70359,14360,43802,86922,0,0,86754,113,310,61193,358,1046,60146,2527,7040,53007,5977,17365,64411,2499,6,50653,"FO2","GT" 21,36,1,4,9,40,23,"CONSOL EDISON CO N Y INC","NARROWS BAY",0,"NAT GAS",4226,"0M",1294,,,95,160,2545,0,0,0,0,1437,23105,0,3151,50378,0,5478,91177,0,7841,132409,0,26727,472807,0,23321,410674,0,8725,137237,0,6684,112244,0,14121,266734,0,726,12168,0,2499,6,50653,"NG","GT" 21,36,1,2,3,40,25,"CONSOL EDISON CO N Y INC","RAVENSWOOD",0,"HEAVY OIL",4226,"0M",1294,,,95,56562,96769,43835,156038,248776,28947,15866,27428,34677,22910,42845,42500,30055,54093,37926,31922,55970,39660,31596,55334,44269,54612,90412,42941,11656,19796,32055,4144,7555,26939,45172,77641,44297,97823,181018,43354,2500,6,50653,"FO6","ST" 21,36,1,2,9,40,25,"CONSOL EDISON CO N Y INC","RAVENSWOOD",0,"NAT GAS",4226,"0M",1294,,,95,209768,2234824,0,193780,1928735,0,161992,1747544,0,161776,1895581,0,200509,2260799,0,241862,2659354,0,377330,4132582,0,492580,5112387,0,269868,2872681,0,121326,1378858,0,190022,2065045,0,34903,408143,0,2500,6,50653,"NG","ST" 21,36,1,4,2,40,25,"CONSOL EDISON CO N Y INC","RAVENSWOOD",0,"LIGHT OIL",4226,"0M",1294,,,95,317,1144,40469,1114,3166,37304,412,1109,36195,1364,3752,32443,0,0,32613,292,765,31848,1020,2785,39004,707,2001,37003,43,116,38759,232,819,37940,91,256,37684,3105,8078,40525,2500,6,50653,"FO2","GT" 21,36,1,4,9,40,25,"CONSOL EDISON CO N Y INC","RAVENSWOOD",0,"NAT GAS",4226,"0M",1294,,,95,699,14506,0,461,7543,0,1614,25061,0,3849,61087,0,2639,36379,0,6191,93115,0,11215,178768,0,7292,120354,0,2766,43431,0,1873,38571,0,2782,45521,0,533,8123,0,2500,6,50653,"NG","GT" 21,36,1,2,3,40,30,"CONSOL EDISON CO N Y INC","74TH STREET",0,"HEAVY OIL",4226,"0M",1294,,,95,4001,11849,37330,7337,16422,1428,4042,7539,1190,6302,7774,1190,11192,14181,1190,8567,12004,1190,7521,9483,1190,3846,5472,1365,3937,4892,1428,-949,0,1429,3253,6242,1429,3602,5677,1429,2504,6,50653,"FO6","ST" 21,36,1,4,2,40,30,"CONSOL EDISON CO N Y INC","74TH STREET",0,"LIGHT OIL",4226,"0M",1294,,,95,-13,0,1690,-11,0,2143,-12,0,2083,-12,0,1952,-3,12,1881,-12,0,1762,-12,24,1738,-13,0,1747,-12,0,1548,-12,0,1524,-12,0,1595,-12,0,2202,2504,6,50653,"FO2","GT" 21,36,1,2,3,40,40,"CONSOL EDISON CO N Y INC","WATERSIDE",0,"HEAVY OIL",4226,"0M",1294,,,95,3119,5797,0,25178,41438,0,1003,1798,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,146,266,0,2502,6,50653,"FO6","ST" 21,36,1,2,9,40,40,"CONSOL EDISON CO N Y INC","WATERSIDE",0,"NAT GAS",4226,"0M",1294,,,95,59934,697096,0,47441,490868,0,53623,603408,0,39082,449151,0,37250,448243,0,36423,288224,0,55999,633276,0,55829,627391,0,38346,480259,0,35286,396996,0,48220,540897,0,63071,723341,0,2502,6,50653,"NG","ST" 21,36,1,2,3,40,50,"CONSOL EDISON CO N Y INC","OIL STORAGE",0,"HEAVY OIL",4226,"0M",1294,,,95,0,0,2766499,0,0,2324286,0,0,2545579,0,0,2254272,0,0,1899927,0,0,1649376,0,0,1484314,0,0,1332860,0,0,1420463,0,0,1532278,0,0,1814997,0,0,1473629,8801,6,50653,"FO6","ST" 21,36,1,4,2,40,60,"CONSOL EDISON CO N Y INC","OIL STORAGE",0,"LIGHT OIL",4226,"0M",1294,,,95,0,0,204071,0,0,265070,0,0,259969,0,0,242953,0,0,247234,0,0,245330,0,0,259288,0,0,251578,0,0,241219,0,0,257945,0,0,250930,0,0,243796,8802,6,50653,"FO2","GT" 21,36,1,4,2,40,65,"CONSOL EDISON CO N Y INC","BUCHANAN",0,"LIGHT OIL",4226,"0M",1294,,,95,55,213,3746,295,599,4326,12,22,4481,20,42,4440,199,586,4211,634,1857,4497,979,2573,4452,907,2783,4475,35,172,4303,63,247,4282,398,1093,4230,56,191,4039,4233,6,50653,"FO2","GT" 21,36,1,1,,49,5,"HYDRO DEV GROUP INC","DEXTER",0,,9145,"0A",1294,,,95,2082,0,0,1260,0,0,2412,0,0,1860,0,0,1134,0,0,690,0,0,834,0,0,558,0,0,666,0,0,1998,0,0,2619,0,0,1908,0,0,2505,6,50785,"WAT","HY" 21,36,1,1,,49,10,"HYDRO DEV GROUP INC","PYRITES #1",0,,9145,"0A",1294,,,95,228,0,0,53,0,0,337,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2506,6,50785,"WAT","HY" 21,36,1,1,,49,12,"HYDRO DEV GROUP INC","PYRITES #2",0,,9145,"0A",1294,,,95,2658,0,0,1453,0,0,3335,0,0,2856,0,0,2370,0,0,1044,0,0,630,0,0,678,0,0,606,0,0,2458,0,0,3186,0,0,2166,0,0,7031,6,50785,"WAT","HY" 21,36,1,1,,49,15,"HYDRO DEV GROUP INC","HAILESBORO",0,,9145,"0A",1294,,,95,1037,0,0,706,0,0,1087,0,0,1097,0,0,854,0,0,509,0,0,415,0,0,624,0,0,389,0,0,982,0,0,1159,0,0,780,0,0,6573,6,50785,"WAT","HY" 21,36,1,1,,49,20,"HYDRO DEV GROUP INC","FOWLER",0,,9145,"0A",1294,,,95,426,0,0,394,0,0,515,0,0,491,0,0,515,0,0,316,0,0,245,0,0,349,0,0,250,0,0,398,0,0,507,0,0,434,0,0,6572,6,50785,"WAT","HY" 21,36,1,1,,49,25,"HYDRO DEV GROUP INC","#6 MILL",0,,9145,"0A",1294,,,95,471,0,0,407,0,0,463,0,0,491,0,0,394,0,0,231,0,0,201,0,0,313,0,0,208,0,0,384,0,0,494,0,0,499,0,0,453,6,50785,"WAT","HY" 21,36,1,1,,49,50,"HYDRO DEV GROUP INC","COPENHAGEN",0,,9145,"0A",1294,,,95,1176,0,0,560,0,0,1460,0,0,1532,0,0,460,0,0,108,0,0,360,0,0,112,0,0,312,0,0,1396,0,0,1884,0,0,924,0,0,742,6,50785,"WAT","HY" 21,36,1,1,,49,55,"HYDRO DEV GROUP INC","DIAMOND IS",0,,9145,"0A",1294,,,95,665,0,0,468,0,0,733,0,0,702,0,0,504,0,0,251,0,0,228,0,0,190,0,0,239,0,0,583,0,0,773,0,0,616,0,0,2553,6,50785,"WAT","HY" 21,36,1,1,,49,60,"HYDRO DEV GROUP INC","THERESA",0,,9145,"0A",1294,,,95,752,0,0,606,0,0,800,0,0,836,0,0,556,0,0,150,0,0,78,0,0,202,0,0,34,0,0,710,0,0,842,0,0,794,0,0,2618,6,50785,"WAT","HY" 21,36,1,1,,49,70,"HYDRO DEV GROUP INC","#3 MILL",0,,9145,"0A",1294,,,95,456,0,0,350,0,0,485,0,0,483,0,0,398,0,0,240,0,0,157,0,0,294,0,0,180,0,0,283,0,0,456,0,0,346,0,0,743,6,50785,"WAT","HY" 21,36,1,1,,49,75,"HYDRO DEV GROUP INC","GOODYEAR LK",0,,9145,"0A",1294,,,95,640,0,0,400,0,0,757,0,0,542,0,0,315,0,0,166,0,0,49,0,0,25,0,0,19,0,0,171,0,0,575,0,0,550,0,0,7358,6,50785,"WAT","HY" 21,36,1,3,2,59,1,"FISHERS IS ELEC CORP (THE","FISHERS ISL",0,"LIGHT OIL",6369,"0A",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,6575,6,50989,"FO2","IC" 21,36,1,4,2,87,1,"LONG ISLAND LIGHTING CO","W BABYLON",0,"LIGHT OIL",11172,"0M",1294,,,95,-9,0,10978,184,398,10580,-10,0,10580,-8,0,10580,-10,0,10580,-10,0,10580,1589,3799,6781,1012,2525,9994,-8,0,9994,23,63,9931,12,52,9878,-6,0,9878,2521,6,51685,"FO2","GT" 21,36,1,2,2,87,2,"LONG ISLAND LIGHTING CO","E F BARRETT",0,"LIGHT OIL",11172,"0M",1294,,,95,0,0,382,0,0,382,0,0,382,0,0,382,0,0,382,0,0,382,0,0,382,0,0,382,189,351,31,0,0,31,0,0,0,0,0,0,2511,6,51685,"FO2","ST" 21,36,1,2,3,87,2,"LONG ISLAND LIGHTING CO","E F BARRETT",0,"HEAVY OIL",11172,"0M",1294,,,95,7679,13204,183912,19277,32691,151221,6888,12026,167809,7622,13054,154755,21364,35883,118872,5001,8521,110351,0,0,100351,0,0,150055,0,0,176621,0,0,176621,4499,7876,168745,30931,52133,130983,2511,6,51685,"FO6","ST" 21,36,1,2,9,87,2,"LONG ISLAND LIGHTING CO","E F BARRETT",0,"NAT GAS",11172,"0M",1294,,,95,88641,923891,0,72376,743992,0,119516,1265049,0,108791,1129535,0,161464,1644681,0,176300,1817157,0,201713,2124759,0,207176,2182914,0,194067,2023621,0,176719,1855067,0,152642,1622397,0,111293,1143313,0,2511,6,51685,"NG","ST" 21,36,1,4,2,87,2,"LONG ISLAND LIGHTING CO","E F BARRETT",0,"LIGHT OIL",11172,"0M",1294,,,95,0,0,21322,0,0,21322,0,0,21322,0,0,21322,0,0,21322,0,0,21322,0,0,21322,0,0,21322,0,0,21322,0,0,21322,0,0,21322,89,272,21050,2511,6,51685,"FO2","GT" 21,36,1,4,9,87,2,"LONG ISLAND LIGHTING CO","E F BARRETT",0,"NAT GAS",11172,"0M",1294,,,95,2584,48858,0,2455,39578,0,396,9580,0,7540,115964,0,15423,241318,0,13024,203027,0,13183,202506,0,13611,214090,0,2215,41056,0,3367,60239,0,3070,49795,0,1324,23100,0,2511,6,51685,"NG","GT" 21,36,1,2,3,87,5,"LONG ISLAND LIGHTING CO","FAR ROCKWAY",0,"HEAVY OIL",11172,"0M",1294,,,95,0,0,630,0,0,630,0,0,630,0,0,630,0,0,630,0,0,630,0,0,630,0,0,630,0,0,630,0,0,630,0,0,630,0,0,630,2513,6,51685,"FO6","ST" 21,36,1,2,9,87,5,"LONG ISLAND LIGHTING CO","FAR ROCKWAY",0,"NAT GAS",11172,"0M",1294,,,95,35652,370173,0,-382,0,0,37901,413154,0,47344,499677,0,39814,418408,0,43785,454694,0,44918,522402,0,46370,490439,0,46043,485717,0,32114,356625,0,40424,437203,0,48243,507731,0,2513,6,51685,"NG","ST" 21,36,1,2,3,87,15,"LONG ISLAND LIGHTING CO","GLENWOOD",0,"HEAVY OIL",11172,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2514,6,51685,"FO6","ST" 21,36,1,2,9,87,15,"LONG ISLAND LIGHTING CO","GLENWOOD",0,"NAT GAS",11172,"0M",1294,,,95,57152,656357,0,88875,989013,0,43090,513102,0,64609,758501,0,65972,764067,0,85437,987225,0,91585,1053103,0,91614,1044546,0,87436,984844,0,70615,831640,0,65930,771090,0,72860,814525,0,2514,6,51685,"NG","ST" 21,36,1,4,2,87,15,"LONG ISLAND LIGHTING CO","GLENWOOD",0,"LIGHT OIL",11172,"0M",1294,,,95,-13,0,28987,348,833,28155,-2,113,28042,-10,0,28042,-15,0,28042,308,112,27929,1020,3353,24576,1330,3635,20941,-16,0,20941,52,122,20819,-18,0,20787,-15,0,20787,2514,6,51685,"FO2","GT" 21,36,1,3,2,87,17,"LONG ISLAND LIGHTING CO","E HAMPTON",0,"LIGHT OIL",11172,"0M",1294,,,95,-6,0,971,33,69,902,-4,4,898,-6,0,898,-1,8,890,2,12,878,464,935,369,527,862,816,51,112,705,-6,0,705,-1,4,915,0,3,911,2512,6,51685,"FO2","IC" 21,36,1,4,2,87,17,"LONG ISLAND LIGHTING CO","E HAMPTON",0,"LIGHT OIL",11172,"0M",1294,,,95,-17,0,2876,-11,17,2859,-15,0,2859,-9,0,2859,-4,25,2834,34,116,2718,2330,5851,265,2246,5851,2259,76,212,2471,-10,0,2471,27,113,2789,-12,0,2789,2512,6,51685,"FO2","GT" 21,36,1,4,2,87,18,"LONG ISLAND LIGHTING CO","SOUTHOLD",0,"LIGHT OIL",11172,"0M",1294,,,95,-8,0,2716,-15,0,2716,-15,0,2716,-11,0,2716,-9,0,2716,14,79,2637,79,316,2534,39,174,2784,-8,0,2784,-8,0,2784,33,160,2624,-15,0,2624,2520,6,51685,"FO2","GT" 21,36,1,2,2,87,21,"LONG ISLAND LIGHTING CO","NORTHPORT",0,"LIGHT OIL",11172,"0M",1294,,,95,393,703,2446,1919,3360,10568,787,1448,10918,244,438,10694,0,0,10694,1255,2346,10708,543,987,10787,859,1604,10653,1224,1286,10857,0,0,11070,42,78,10992,866,1558,10948,2516,6,51685,"FO2","ST" 21,36,1,2,3,87,21,"LONG ISLAND LIGHTING CO","NORTHPORT",0,"HEAVY OIL",11172,"0M",1294,,,95,251839,410183,917940,419721,669714,545119,137170,230153,627264,93546,156459,751601,4614,7948,743653,138528,235371,730114,232571,387065,831393,198326,339587,780654,65679,111985,948390,0,0,1048629,13006,22156,1026473,263245,435054,787488,2516,6,51685,"FO6","ST" 21,36,1,2,9,87,21,"LONG ISLAND LIGHTING CO","NORTHPORT",0,"NAT GAS",11172,"0M",1294,,,95,161173,1656185,0,109357,1099738,0,179917,1902183,0,179876,1858552,0,249772,2620522,0,277680,2980882,0,392501,4094975,0,395601,4243388,0,332956,3533654,0,339896,3613412,0,310631,3313635,0,259449,2673147,0,2516,6,51685,"NG","ST" 21,36,1,4,2,87,21,"LONG ISLAND LIGHTING CO","NORTHPORT",0,"LIGHT OIL",11172,"0M",1294,,,95,-16,0,2030,-16,0,2030,11,87,1943,-13,0,1943,-12,0,1943,-8,15,1928,10,25,1904,24,175,1729,-2,17,1712,-7,0,0,-15,0,1290,-10,0,1506,2516,6,51685,"FO2","GT" 21,36,1,3,2,87,23,"LONG ISLAND LIGHTING CO","SHOREHAM",0,"LIGHT OIL",11172,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2518,6,51685,"FO2","IC" 21,36,1,4,2,87,23,"LONG ISLAND LIGHTING CO","SHOREHAM",0,"LIGHT OIL",11172,"0M",1294,,,95,-4,0,10375,81,259,11414,11,38,11377,-7,0,11377,340,528,10848,91,128,10720,441,1417,9303,551,846,15679,5,41,15638,18,32,15605,-4,0,15605,-7,3,15602,2518,6,51685,"FO2","GT" 21,36,1,2,2,87,24,"LONG ISLAND LIGHTING CO","P JEFFERSON",0,"LIGHT OIL",11172,"0M",1294,,,95,505,940,248,368,651,173,451,865,267,430,769,71,340,624,210,273,507,271,308,573,265,205,379,265,120,230,224,260,511,310,181,337,162,173,317,229,2517,6,51685,"FO2","ST" 21,36,1,2,3,87,24,"LONG ISLAND LIGHTING CO","P JEFFERSON",0,"HEAVY OIL",11172,"0M",1294,,,95,83231,142447,374658,116002,187180,292517,84682,149701,363973,88134,146337,217636,86246,147673,240914,86540,147162,367784,119762,202643,388397,116504,197519,283029,62653,110443,267311,37059,67418,404544,57551,98596,305948,73017,122780,291514,2517,6,51685,"FO6","ST" 21,36,1,4,2,87,24,"LONG ISLAND LIGHTING CO","P JEFFERSON",0,"LIGHT OIL",11172,"0M",1294,,,95,14,70,2055,36,150,1905,-16,0,1905,-11,0,1905,30,100,1805,15,79,1726,94,282,1444,49,175,2118,-8,0,2118,2,49,2069,-12,0,2069,-14,0,2069,2517,6,51685,"FO2","GT" 21,36,1,4,2,87,26,"LONG ISLAND LIGHTING CO","SOUTHAMPTON",0,"LIGHT OIL",11172,"0M",1294,,,95,-16,0,2575,22,137,2438,-17,0,2438,-9,0,2438,-4,9,2430,36,153,2277,200,649,2266,170,698,2628,-11,0,2628,-8,0,2628,-2,0,2628,-18,0,2628,2519,6,51685,"FO2","GT" 21,36,1,3,2,87,29,"LONG ISLAND LIGHTING CO","MONTAUK",0,"LIGHT OIL",11172,"0M",1294,,,95,-6,0,685,34,66,619,-6,0,619,-6,0,619,0,0,619,2,46,572,274,574,424,184,319,529,57,109,420,-6,0,420,0,23,611,-6,0,611,2515,6,51685,"FO2","IC" 21,36,1,4,2,87,30,"LONG ISLAND LIGHTING CO","HOLTSVILLE",0,"LIGHT OIL",11172,"0M",1294,,,95,3418,7966,65483,2730,6945,98989,1349,3183,95807,3573,8991,86815,1220,3009,83806,4957,12317,71489,13538,28073,71475,15481,41712,89159,785,2396,86763,-94,234,86529,427,1487,85042,2296,5778,79264,8007,6,51685,"FO2","GT" 21,36,1,4,2,87,35,"LONG ISLAND LIGHTING CO","BROOKHAVEN",0,"LIGHT OIL",11172,"0M",1294,,,95,2290,4982,38416,2652,6010,38901,226,279,38622,3165,6704,37310,6210,13571,28376,6235,12488,40846,9816,21210,30472,9736,19194,39142,-52,0,39142,113,688,40071,528,1470,40751,2660,5996,37572,7146,6,51685,"FO2","GT" 21,36,1,1,,100,1,"N Y STATE ELEC & GAS CORP","CADYVILLE",0,,13511,"0M",1294,,,95,2289,0,0,1760,0,0,2697,0,0,2249,0,0,2033,0,0,1277,0,0,1043,0,0,1271,0,0,873,0,0,1835,0,0,2411,0,0,1256,0,0,2522,6,52036,"WAT","HY" 21,36,1,1,,100,3,"N Y STATE ELEC & GAS CORP","MILL 'C'",0,,13511,"0M",1294,,,95,1082,0,0,1120,0,0,1325,0,0,1217,0,0,1424,0,0,918,2,0,782,0,0,1153,0,0,591,0,0,1982,0,0,2696,0,0,728,0,0,6486,6,52036,"WAT","HY" 21,36,1,1,,100,8,"N Y STATE ELEC & GAS CORP","HIGH FALLS",0,,13511,"0M",1294,,,95,8036,0,0,6467,0,0,9348,0,0,7548,0,0,6945,0,0,4111,0,0,3127,0,0,4402,0,0,2270,0,0,1885,0,0,8998,0,0,6023,0,0,2530,6,52036,"WAT","HY" 21,36,1,1,,100,9,"N Y STATE ELEC & GAS CORP","KENT FALLS",0,,13511,"0M",1294,,,95,4267,0,0,3614,0,0,5729,0,0,4500,0,0,4403,0,0,2459,0,0,1821,0,0,2011,0,0,1112,0,0,2429,0,0,0,0,0,2462,0,0,2532,6,52036,"WAT","HY" 21,36,1,1,,100,11,"N Y STATE ELEC & GAS CORP","KEUKA",0,,13511,"0M",1294,,,95,479,0,0,618,0,0,1104,0,0,424,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,246,0,0,368,0,0,87,0,0,2533,6,52036,"WAT","HY" 21,36,1,1,,100,18,"N Y STATE ELEC & GAS CORP","RAINBOW FLS",0,,13511,"0M",1294,,,95,844,0,0,484,0,0,1136,0,0,1424,0,0,2008,0,0,1044,0,0,972,0,0,828,0,0,572,0,0,920,0,0,1432,0,0,800,0,0,6526,6,52036,"WAT","HY" 21,36,1,1,,100,20,"N Y STATE ELEC & GAS CORP","SENECA FLS",0,,13511,"0M",1294,,,95,929,0,0,0,0,0,237,0,0,418,0,0,57,0,0,12,0,0,35,0,0,0,0,0,0,0,0,144,0,0,1097,0,0,1515,0,0,6525,6,52036,"WAT","HY" 21,36,1,1,,100,26,"N Y STATE ELEC & GAS CORP","WATERLOO",0,,13511,"0M",1294,,,95,218,0,0,0,0,0,91,0,0,167,0,0,47,0,0,38,0,0,63,0,0,15,0,0,0,0,0,28,0,0,273,0,0,435,0,0,2538,6,52036,"WAT","HY" 21,36,1,2,2,100,28,"N Y STATE ELEC & GAS CORP","GOUDEY",0,"LIGHT OIL",13511,"0M",1294,,,95,4,6,902,7,12,922,38,860,816,166,1093,889,115,412,787,23,40,755,14,25,726,19,34,1012,88,159,674,17,29,652,15,27,781,57,99,755,2526,6,52036,"FO2","ST" 21,36,1,2,6,100,28,"N Y STATE ELEC & GAS CORP","GOUDEY",0,"BIT COAL",13511,"0M",1294,,,95,49140,18404,38386,47957,17309,33487,38535,14154,31196,29944,11570,19706,47570,19243,17396,46082,17833,16951,48114,18609,8401,48907,19270,14458,47509,18547,11816,46734,17563,21803,47743,17962,29205,49938,18814,16951,2526,6,52036,"BIT","ST" 21,36,1,2,2,100,30,"N Y STATE ELEC & GAS CORP","GREENIDGE",0,"LIGHT OIL",13511,"0M",1294,,,95,49,84,1482,143,249,1673,49,85,1663,69,118,1503,97,194,1276,101,268,963,140,255,1024,312,565,929,134,232,1184,28,65,1082,27,47,1003,135,254,963,2527,6,52036,"FO2","ST" 21,36,1,2,6,100,30,"N Y STATE ELEC & GAS CORP","GREENIDGE",0,"BIT COAL",13511,"0M",1294,,,95,59064,22369,46139,64896,24628,34337,56536,21560,33567,61588,23327,27754,60141,23147,16512,44718,17812,44179,56844,23346,35975,63282,25535,39483,33115,12718,51031,52461,19935,48906,51733,19814,48981,79778,32545,44179,2527,6,52036,"BIT","ST" 21,36,1,2,6,100,32,"N Y STATE ELEC & GAS CORP","HICKLING",0,"BIT COAL",13511,"0M",1294,,,95,29937,25353,59845,37278,28317,42388,31428,24287,26231,36848,29367,9739,25540,20965,7417,26619,21486,11619,19927,15033,13417,19292,17747,12211,16109,14260,19398,15799,13125,25995,15584,11444,38506,16518,14020,11619,2529,6,52036,"BIT","ST" 21,36,1,2,"B",100,34,"N Y STATE ELEC & GAS CORP","JENNISON",0,"WOOD CHIP",13511,"0M",1294,,,95,1937,0,0,2506,0,0,1706,0,0,446,0,0,510,0,0,631,0,0,0,0,0,966,0,0,1443,0,0,1357,0,0,215,0,0,517,0,0,2531,6,52036,"WOD","ST" 21,36,1,2,6,100,34,"N Y STATE ELEC & GAS CORP","JENNISON",0,"BIT COAL",13511,"0M",1294,,,95,18813,12027,31771,27918,18374,13300,18598,13682,9272,12405,9568,1166,10568,8258,1035,8066,6810,737,10639,7167,2889,9803,7780,5121,7664,6371,9926,7104,5362,9933,11173,7198,8195,18436,12369,737,2531,6,52036,"BIT","ST" 21,36,1,2,2,100,35,"N Y STATE ELEC & GAS CORP","MILLIKEN",0,"LIGHT OIL",13511,"0M",1294,,,95,206,337,1812,188,320,1856,273,465,1873,142,244,1879,53,94,1978,249,452,1841,116,209,1815,158,288,1863,211,385,1831,258,462,1670,59,105,1738,26,47,1841,2535,6,52036,"FO2","ST" 21,36,1,2,6,100,35,"N Y STATE ELEC & GAS CORP","MILLIKEN",0,"BIT COAL",13511,"0M",1294,,,95,192258,68792,79141,180255,67185,80127,183681,68408,89806,153861,58397,69230,98273,37927,98714,132074,52498,118633,185234,73165,90889,184163,73756,101056,131693,53020,97110,185372,73940,102961,167135,65625,99048,191784,76075,118633,2535,6,52036,"BIT","ST" 21,36,1,3,2,100,35,"N Y STATE ELEC & GAS CORP","MILLIKEN",0,"LIGHT OIL",13511,"0M",1294,,,95,0,1,0,20,38,0,3,84,0,104,107,0,54,144,0,1,38,0,-64,39,0,10,20,0,0,1,0,12,39,0,11,44,0,17,32,0,2535,6,52036,"FO2","IC" 21,36,1,3,2,100,40,"N Y STATE ELEC & GAS CORP","HARRIS LAKE",0,"LIGHT OIL",13511,"0M",1294,,,95,-11,0,405,0,0,349,0,0,0,-4,0,313,0,0,260,0,0,242,64,122,269,12,25,244,2,0,436,0,0,357,0,0,290,-13,0,242,2528,6,52036,"FO2","IC" 21,36,1,1,,100,43,"N Y STATE ELEC & GAS CORP","MECHANICVLE",0,,13511,"0M",1294,,,95,9072,0,0,6867,0,0,9702,0,0,6867,0,0,4347,0,0,2961,0,0,1134,0,0,2331,0,0,1953,0,0,5670,0,0,12663,0,0,8946,0,0,625,6,52036,"WAT","HY" 21,36,1,2,2,100,50,"N Y STATE ELEC & GAS CORP","KINTIGH",0,"LIGHT OIL",13511,"0M",1294,,,95,219,378,4169,770,1322,2904,474,811,3335,953,1656,3113,165,283,2839,314,543,2288,879,1523,3426,394,685,2738,627,1087,4124,1183,2162,2118,626,1094,4657,509,873,2288,6082,6,52036,"FO2","ST" 21,36,1,2,6,100,50,"N Y STATE ELEC & GAS CORP","KINTIGH",0,"BIT COAL",13511,"0M",1294,,,95,429496,166336,132032,393694,148405,142690,419527,160683,178911,416807,160659,178855,418612,159916,174957,381565,146069,162034,348178,133246,124345,413546,158604,73112,376458,141570,75380,181079,73253,130474,363691,142233,133771,423315,159637,162034,6082,6,52036,"BIT","ST" 21,36,1,2,1,105,1,"NIAGARA MOHAWK POWER CORP","NINE MILE P",0,"NUCLEAR",13573,"0M",1294,,190,95,368414,0,0,58742,0,0,0,0,0,332154,0,0,459193,0,0,439571,0,0,434942,0,0,437261,0,0,420930,0,0,452099,0,0,441551,0,0,459844,0,0,2589,6,52053,"UR","ST" 21,36,1,2,1,105,2,"NIAGARA MOHAWK POWER CORP","NINE MILE P",0,"NUCLEAR",13573,"0M",1294,,190,95,694823,0,0,533574,0,0,742888,0,0,149501,0,0,0,0,0,575400,0,0,821880,0,0,766368,0,0,443850,0,0,845303,0,0,824493,0,0,841323,0,0,2589,6,52053,"UR","ST" 21,36,1,1,,105,5,"NIAGARA MOHAWK POWER CORP","ALLENS FLS",0,,13573,"0M",1294,,190,95,2087,0,0,1758,0,0,2479,0,0,2662,0,0,2344,0,0,1289,0,0,1268,0,0,1240,0,0,1099,0,0,2308,0,0,2305,0,0,2092,0,0,2540,6,52053,"WAT","HY" 21,36,1,1,,105,10,"NIAGARA MOHAWK POWER CORP","BALDWINSVLE",0,,13573,"0M",1294,,190,95,205,0,0,112,0,0,221,0,0,171,0,0,60,0,0,7,0,0,-3,0,0,16,0,0,1,0,0,57,0,0,217,0,0,140,0,0,2542,6,52053,"WAT","HY" 21,36,1,1,,105,15,"NIAGARA MOHAWK POWER CORP","BELFORT",0,,13573,"0M",1294,,190,95,861,0,0,751,0,0,805,0,0,464,0,0,550,0,0,561,0,0,714,0,0,764,0,0,730,0,0,557,0,0,1171,0,0,1354,0,0,2544,6,52053,"WAT","HY" 21,36,1,1,,105,20,"NIAGARA MOHAWK POWER CORP","BENNETTS B",0,,13573,"0M",1294,,190,95,10231,0,0,5759,0,0,9838,0,0,5346,0,0,4404,0,0,1938,0,0,-33,0,0,313,0,0,5443,0,0,9001,0,0,13335,0,0,6313,0,0,2545,6,52053,"WAT","HY" 21,36,1,1,,105,25,"NIAGARA MOHAWK POWER CORP","BLACK RIVER",0,,13573,"0M",1294,,190,95,3477,0,0,2422,0,0,3823,0,0,3907,0,0,2562,0,0,1270,0,0,1501,0,0,948,0,0,1559,0,0,3563,0,0,4456,0,0,3477,0,0,2546,6,52053,"WAT","HY" 21,36,1,1,,105,30,"NIAGARA MOHAWK POWER CORP","BLAKE",0,,13573,"0M",1294,,190,95,6604,0,0,6486,0,0,5072,0,0,2962,0,0,3721,0,0,3715,0,0,672,0,0,2828,0,0,1682,0,0,3534,0,0,9144,0,0,6300,0,0,2547,6,52053,"WAT","HY" 21,36,1,1,,105,35,"NIAGARA MOHAWK POWER CORP","BROWNS FLS",0,,13573,"0M",1294,,190,95,6785,0,0,3738,0,0,4510,0,0,1724,0,0,1746,0,0,1866,0,0,545,0,0,2901,0,0,1160,0,0,4896,0,0,7492,0,0,3767,0,0,2548,6,52053,"WAT","HY" 21,36,1,1,,105,40,"NIAGARA MOHAWK POWER CORP","CHASM",0,,13573,"0M",1294,,190,95,1902,0,0,1138,0,0,1426,0,0,1777,0,0,1751,0,0,1323,0,0,994,0,0,1236,0,0,1014,0,0,1752,0,0,1795,0,0,1489,0,0,2550,6,52053,"WAT","HY" 21,36,1,1,,105,45,"NIAGARA MOHAWK POWER CORP","COLTON",0,,13573,"0M",1294,,190,95,20600,0,0,18761,0,0,20043,0,0,13701,0,0,15937,0,0,15548,0,0,9456,0,0,14510,0,0,7469,0,0,15049,0,0,2073,0,0,19935,0,0,2551,6,52053,"WAT","HY" 21,36,1,1,,105,50,"NIAGARA MOHAWK POWER CORP","DEFERIET",0,,13573,"0M",1294,,190,95,4478,0,0,3495,0,0,5869,0,0,5234,0,0,3642,0,0,1740,0,0,1638,0,0,1204,0,0,1248,0,0,5355,0,0,7027,0,0,4656,0,0,2552,6,52053,"WAT","HY" 21,36,1,1,,105,65,"NIAGARA MOHAWK POWER CORP","EAGLE",0,,13573,"0M",1294,,190,95,2653,0,0,2021,0,0,2505,0,0,1200,0,0,1421,0,0,1737,0,0,2331,0,0,1979,0,0,2045,0,0,1398,0,0,3203,0,0,3777,0,0,2555,6,52053,"WAT","HY" 21,36,1,1,,105,70,"NIAGARA MOHAWK POWER CORP","EEL WEIR",0,,13573,"0M",1294,,190,95,866,0,0,622,0,0,964,0,0,803,0,0,524,0,0,203,0,0,115,0,0,125,0,0,7,0,0,655,0,0,1332,0,0,994,0,0,2556,6,52053,"WAT","HY" 21,36,1,1,,105,75,"NIAGARA MOHAWK POWER CORP","EFFLEY",0,,13573,"0M",1294,,190,95,1093,0,0,986,0,0,1153,0,0,580,0,0,694,0,0,845,0,0,905,0,0,982,0,0,900,0,0,740,0,0,1558,0,0,1767,0,0,2557,6,52053,"WAT","HY" 21,36,1,1,,105,80,"NIAGARA MOHAWK POWER CORP","ELMER",0,,13573,"0M",1294,,190,95,812,0,0,575,0,0,796,0,0,380,0,0,439,0,0,552,0,0,441,0,0,640,0,0,593,0,0,496,0,0,1010,0,0,1135,0,0,2559,6,52053,"WAT","HY" 21,36,1,1,,105,85,"NIAGARA MOHAWK POWER CORP","ET NORFOLK",0,,13573,"0M",1294,,190,95,2479,0,0,1995,0,0,2559,0,0,1703,0,0,1975,0,0,1859,0,0,1059,0,0,1731,0,0,851,0,0,1883,0,0,2471,0,0,2519,0,0,2561,6,52053,"WAT","HY" 21,36,1,1,,105,90,"NIAGARA MOHAWK POWER CORP","FIVE FALLS",0,,13573,"0M",1294,,190,95,10795,0,0,10405,0,0,8347,0,0,4782,0,0,5926,0,0,5896,0,0,3396,0,0,5619,0,0,2631,0,0,5807,0,0,14654,0,0,10198,0,0,2562,6,52053,"WAT","HY" 21,36,1,1,,105,95,"NIAGARA MOHAWK POWER CORP","FLAT ROCK",0,,13573,"0M",1294,,190,95,1503,0,0,871,0,0,1489,0,0,592,0,0,450,0,0,401,0,0,136,0,0,528,0,0,169,0,0,1414,0,0,1912,0,0,876,0,0,2563,6,52053,"WAT","HY" 21,36,1,1,,105,98,"NIAGARA MOHAWK POWER CORP","FRANKLIN F",0,,13573,"0M",1294,,190,95,775,0,0,767,0,0,1052,0,0,613,0,0,385,0,0,496,0,0,336,0,0,352,0,0,-1,0,0,-1,0,0,-1,0,0,-1,0,0,2564,6,52053,"WAT","HY" 21,36,1,1,,105,100,"NIAGARA MOHAWK POWER CORP","FULTON",0,,13573,"0M",1294,,190,95,464,0,0,333,0,0,608,0,0,437,0,0,459,0,0,300,0,0,406,0,0,363,0,0,304,0,0,474,0,0,653,0,0,625,0,0,2566,6,52053,"WAT","HY" 21,36,1,1,,105,105,"NIAGARA MOHAWK POWER CORP","GRANBY",0,,13573,"0M",1294,,190,95,5845,0,0,3502,0,0,6558,0,0,1324,0,0,640,0,0,477,0,0,-38,0,0,491,0,0,-42,0,0,3025,0,0,5404,0,0,5157,0,0,2569,6,52053,"WAT","HY" 21,36,1,1,,105,110,"NIAGARA MOHAWK POWER CORP","HANNAWA",0,,13573,"0M",1294,,190,95,5253,0,0,4772,0,0,5248,0,0,3332,0,0,4051,0,0,3941,0,0,2329,0,0,3797,0,0,1747,0,0,1086,0,0,2696,0,0,5321,0,0,2571,6,52053,"WAT","HY" 21,36,1,1,,105,115,"NIAGARA MOHAWK POWER CORP","HERRINGS",0,,13573,"0M",1294,,190,95,1980,0,0,1586,0,0,2151,0,0,2116,0,0,1509,0,0,629,0,0,705,0,0,371,0,0,337,0,0,1747,0,0,2341,0,0,2187,0,0,2572,6,52053,"WAT","HY" 21,36,1,1,,105,120,"NIAGARA MOHAWK POWER CORP","HEUVELTON",0,,13573,"0M",1294,,190,95,458,0,0,468,0,0,484,0,0,556,0,0,455,0,0,254,0,0,195,0,0,277,0,0,149,0,0,433,0,0,506,0,0,588,0,0,2573,6,52053,"WAT","HY" 21,36,1,1,,105,125,"NIAGARA MOHAWK POWER CORP","HIGH DAM 6",0,,13573,"0M",1294,,190,95,0,0,0,0,0,0,1863,0,0,2023,0,0,1494,0,0,922,0,0,725,0,0,989,0,0,179,0,0,2024,0,0,2607,0,0,3766,0,0,2574,6,52053,"WAT","HY" 21,36,1,1,,105,126,"NIAGARA MOHAWK POWER CORP","HIGH FALLS",0,,13573,"0M",1294,,190,95,2622,0,0,1900,0,0,2648,0,0,1268,0,0,1439,0,0,1814,0,0,2106,0,0,1998,0,0,1847,0,0,1571,0,0,3045,0,0,3527,0,0,2575,6,52053,"WAT","HY" 21,36,1,1,,105,130,"NIAGARA MOHAWK POWER CORP","HIGLEY",0,,13573,"0M",1294,,190,95,3414,0,0,2999,0,0,3075,0,0,1774,0,0,2177,0,0,2037,0,0,1416,0,0,2086,0,0,1120,0,0,2315,0,0,3556,0,0,3242,0,0,2576,6,52053,"WAT","HY" 21,36,1,1,,105,135,"NIAGARA MOHAWK POWER CORP","HOGANSBURG",0,,13573,"0M",1294,,190,95,98,0,0,143,0,0,192,0,0,192,0,0,148,0,0,129,0,0,87,0,0,146,0,0,79,0,0,113,0,0,186,0,0,218,0,0,2577,6,52053,"WAT","HY" 21,36,1,1,,105,140,"NIAGARA MOHAWK POWER CORP","KAMARGO",0,,13573,"0M",1294,,190,95,2374,0,0,1857,0,0,2750,0,0,2638,0,0,1924,0,0,960,0,0,1034,0,0,398,0,0,612,0,0,2497,0,0,3433,0,0,1788,0,0,2581,6,52053,"WAT","HY" 21,36,1,1,,105,145,"NIAGARA MOHAWK POWER CORP","LIGHTHOUSE",0,,13573,"0M",1294,,190,95,2431,0,0,1342,0,0,2514,0,0,1178,0,0,925,0,0,399,0,0,-14,0,0,-14,0,0,1080,0,0,1999,0,0,3282,0,0,1507,0,0,2582,6,52053,"WAT","HY" 21,36,1,1,,105,155,"NIAGARA MOHAWK POWER CORP","MACOMB",0,,13573,"0M",1294,,190,95,434,0,0,398,0,0,641,0,0,569,0,0,481,0,0,319,0,0,-4,0,0,-4,0,0,132,0,0,534,0,0,627,0,0,520,0,0,2583,6,52053,"WAT","HY" 21,36,1,1,,105,160,"NIAGARA MOHAWK POWER CORP","MINETTO",0,,13573,"0M",1294,,190,95,3847,0,0,2604,0,0,4467,0,0,2022,0,0,1607,0,0,940,0,0,602,0,0,800,0,0,427,0,0,1690,0,0,4151,0,0,4554,0,0,2586,6,52053,"WAT","HY" 21,36,1,1,,105,165,"NIAGARA MOHAWK POWER CORP","MOSHIER",0,,13573,"0M",1294,,190,95,2698,0,0,2561,0,0,2447,0,0,1064,0,0,1751,0,0,2554,0,0,2993,0,0,2896,0,0,2791,0,0,736,0,0,3994,0,0,5506,0,0,2588,6,52053,"WAT","HY" 21,36,1,1,,105,170,"NIAGARA MOHAWK POWER CORP","NORFOLK",0,,13573,"0M",1294,,190,95,2391,0,0,2156,0,0,2979,0,0,1872,0,0,2207,0,0,2139,0,0,1223,0,0,2018,0,0,958,0,0,2054,0,0,3088,0,0,2630,0,0,2590,6,52053,"WAT","HY" 21,36,1,1,,105,175,"NIAGARA MOHAWK POWER CORP","NORWOOD",0,,13573,"0M",1294,,190,95,1536,0,0,1408,0,0,1536,0,0,938,0,0,1146,0,0,1136,0,0,605,0,0,1104,0,0,480,0,0,1072,0,0,1232,0,0,1488,0,0,2591,6,52053,"WAT","HY" 21,36,1,1,,105,180,"NIAGARA MOHAWK POWER CORP","OSWEGATCHIE",0,,13573,"0M",1294,,190,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2593,6,52053,"WAT","HY" 21,36,1,1,,105,182,"NIAGARA MOHAWK POWER CORP","OSWEGO FL E",0,,13573,"0M",1294,,190,95,2890,0,0,2449,0,0,2510,0,0,1688,0,0,1604,0,0,996,0,0,637,0,0,679,0,0,550,0,0,1991,0,0,2836,0,0,2816,0,0,2595,6,52053,"WAT","HY" 21,36,1,1,,105,183,"NIAGARA MOHAWK POWER CORP","OSWEGO FL W",0,,13573,"0M",1294,,190,95,1223,0,0,423,0,0,1212,0,0,176,0,0,-1,0,0,28,0,0,-2,0,0,47,0,0,14,0,0,385,0,0,730,0,0,1172,0,0,2596,6,52053,"WAT","HY" 21,36,1,1,,105,185,"NIAGARA MOHAWK POWER CORP","PARISHVILLE",0,,13573,"0M",1294,,190,95,0,0,0,690,0,0,1562,0,0,1603,0,0,1516,0,0,848,0,0,849,0,0,763,0,0,749,0,0,1395,0,0,1488,0,0,1298,0,0,2597,6,52053,"WAT","HY" 21,36,1,1,,105,187,"NIAGARA MOHAWK POWER CORP","PIERCEFIELD",0,,13573,"0M",1294,,190,95,1488,0,0,1283,0,0,1529,0,0,1482,0,0,1341,0,0,627,0,0,429,0,0,881,0,0,370,0,0,1195,0,0,1783,0,0,1527,0,0,2598,6,52053,"WAT","HY" 21,36,1,1,,105,192,"NIAGARA MOHAWK POWER CORP","PROSPECT",0,,13573,"0M",1294,,190,95,1704,0,0,0,0,0,4257,0,0,5788,0,0,3672,0,0,2881,0,0,2386,0,0,1689,0,0,184,0,0,6691,0,0,11309,0,0,6904,0,0,2599,6,52053,"WAT","HY" 21,36,1,1,,105,195,"NIAGARA MOHAWK POWER CORP","RAINBOW",0,,13573,"0M",1294,,190,95,10771,0,0,10270,0,0,8298,0,0,4779,0,0,5959,0,0,5843,0,0,3452,0,0,5583,0,0,2641,0,0,5774,0,0,14120,0,0,9950,0,0,2600,6,52053,"WAT","HY" 21,36,1,1,,105,200,"NIAGARA MOHAWK POWER CORP","RAYMONDVLE",0,,13573,"0M",1294,,190,95,932,0,0,816,0,0,1452,0,0,926,0,0,670,0,0,1102,0,0,674,0,0,1036,0,0,530,0,0,1056,0,0,1404,0,0,1120,0,0,2601,6,52053,"WAT","HY" 21,36,1,1,,105,210,"NIAGARA MOHAWK POWER CORP","S EDWARDS",0,,13573,"0M",1294,,190,95,1404,0,0,1076,0,0,1387,0,0,973,0,0,1018,0,0,736,0,0,427,0,0,1020,0,0,558,0,0,1359,0,0,1919,0,0,1392,0,0,2604,6,52053,"WAT","HY" 21,36,1,1,,105,215,"NIAGARA MOHAWK POWER CORP","SEWALLS",0,,13573,"0M",1294,,190,95,1372,0,0,889,0,0,1518,0,0,1486,0,0,1205,0,0,544,0,0,246,0,0,320,0,0,319,0,0,1211,0,0,1489,0,0,1514,0,0,2608,6,52053,"WAT","HY" 21,36,1,1,,105,220,"NIAGARA MOHAWK POWER CORP","SOFT MAPLE",0,,13573,"0M",1294,,190,95,2633,0,0,1616,0,0,2359,0,0,882,0,0,1236,0,0,1714,0,0,2341,0,0,1918,0,0,1850,0,0,1760,0,0,3432,0,0,4125,0,0,2610,6,52053,"WAT","HY" 21,36,1,1,,105,225,"NIAGARA MOHAWK POWER CORP","SOTH COLTON",0,,13573,"0M",1294,,190,95,8860,0,0,8292,0,0,6906,0,0,3510,0,0,4607,0,0,4842,0,0,2861,0,0,4595,0,0,2211,0,0,4731,0,0,12247,0,0,8305,0,0,2611,6,52053,"WAT","HY" 21,36,1,1,,105,230,"NIAGARA MOHAWK POWER CORP","STARK",0,,13573,"0M",1294,,190,95,10035,0,0,10162,0,0,7531,0,0,4401,0,0,5629,0,0,5788,0,0,3281,0,0,5363,0,0,2475,0,0,5187,0,0,14852,0,0,9960,0,0,2613,6,52053,"WAT","HY" 21,36,1,1,,105,235,"NIAGARA MOHAWK POWER CORP","SUGAR IS",0,,13573,"0M",1294,,190,95,2908,0,0,2519,0,0,2995,0,0,2818,0,0,2884,0,0,2757,0,0,1893,0,0,2754,0,0,1376,0,0,2667,0,0,2781,0,0,2983,0,0,2616,6,52053,"WAT","HY" 21,36,1,1,,105,240,"NIAGARA MOHAWK POWER CORP","TAYLORVILLE",0,,13573,"0M",1294,,190,95,2219,0,0,1663,0,0,2176,0,0,1051,0,0,1247,0,0,1560,0,0,1566,0,0,1692,0,0,1630,0,0,1392,0,0,2700,0,0,3109,0,0,2617,6,52053,"WAT","HY" 21,36,1,1,,105,250,"NIAGARA MOHAWK POWER CORP","TRENTON",0,,13573,"0M",1294,,190,95,12363,0,0,10763,0,0,12685,0,0,10309,0,0,6711,0,0,6004,0,0,5262,0,0,4565,0,0,3995,0,0,8295,0,0,14603,0,0,11617,0,0,2619,6,52053,"WAT","HY" 21,36,1,1,,105,255,"NIAGARA MOHAWK POWER CORP","VARICK",0,,13573,"0M",1294,,190,95,3510,0,0,2348,0,0,3552,0,0,1467,0,0,836,0,0,546,0,0,363,0,0,629,0,0,211,0,0,2344,0,0,3490,0,0,3553,0,0,2621,6,52053,"WAT","HY" 21,36,1,1,,105,265,"NIAGARA MOHAWK POWER CORP","YALEVILLE",0,,13573,"0M",1294,,190,95,293,0,0,255,0,0,406,0,0,320,0,0,373,0,0,341,0,0,243,0,0,407,0,0,242,0,0,346,0,0,275,0,0,248,0,0,2624,6,52053,"WAT","HY" 21,36,1,3,2,105,270,"NIAGARA MOHAWK POWER CORP","NINE MILE P",0,"LIGHT OIL",13573,"0M",1294,,190,95,6,136,4435,3,121,4470,11,87,4380,0,100,4256,13,323,4316,10,36,4349,6,164,4288,7,218,4320,6,11,535,6,12,573,6,13,557,6,12,543,2589,6,52053,"FO2","IC" 21,36,1,2,3,105,275,"NIAGARA MOHAWK POWER CORP","OSWEGO",0,"HEAVY OIL",13573,"0M",1294,,190,95,0,0,632933,120407,215553,417380,0,0,417380,26504,46741,370639,0,0,370639,1371,4130,366508,44092,30232,330715,13690,33269,298197,9883,21973,276183,0,0,276183,0,0,542213,0,0,542213,2594,6,52053,"FO6","ST" 21,36,1,2,9,105,275,"NIAGARA MOHAWK POWER CORP","OSWEGO",0,"NAT GAS",13573,"0M",1294,,190,95,999,22854,0,10635,117884,0,0,0,0,0,0,0,0,0,0,0,0,0,108,461,0,38513,570000,0,15497,213000,0,0,0,0,0,0,0,0,0,0,2594,6,52053,"NG","ST" 21,36,1,3,2,105,275,"NIAGARA MOHAWK POWER CORP","OSWEGO",0,"LIGHT OIL",13573,"0M",1294,,190,95,0,0,2149,0,0,2149,0,0,2149,0,0,2149,0,0,2149,0,0,2149,0,0,2149,0,0,2149,4,11,2138,0,0,2138,0,0,2138,0,0,2138,2594,6,52053,"FO2","IC" 21,36,1,1,,105,285,"NIAGARA MOHAWK POWER CORP","BEARDSLEE F",0,,13573,"0M",1294,,190,95,5266,0,0,1946,0,0,6556,0,0,4417,0,0,2463,0,0,1946,0,0,895,0,0,759,0,0,741,0,0,5400,0,0,6369,0,0,2631,0,0,2543,6,52053,"WAT","HY" 21,36,1,1,,105,290,"NIAGARA MOHAWK POWER CORP","BAKER FALLS",0,,13573,"0M",1294,"R",190,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2541,6,52053,"WAT","HY" 21,36,1,1,,105,300,"NIAGARA MOHAWK POWER CORP","EL J WEST",0,,13573,"0M",1294,,190,95,5989,0,0,5250,0,0,1580,0,0,972,0,0,1241,0,0,3218,0,0,3059,0,0,2326,0,0,4257,0,0,1425,0,0,10684,0,0,8834,0,0,6527,6,52053,"WAT","HY" 21,36,1,1,,105,305,"NIAGARA MOHAWK POWER CORP","EPHRATAH",0,,13573,"0M",1294,,190,95,2045,0,0,902,0,0,1493,0,0,780,0,0,337,0,0,463,0,0,97,0,0,147,0,0,127,0,0,1599,0,0,1298,0,0,1198,0,0,2560,6,52053,"WAT","HY" 21,36,1,1,,105,315,"NIAGARA MOHAWK POWER CORP","GLEN FALLS",0,,13573,"0M",1294,,190,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2567,6,52053,"WAT","HY" 21,36,1,1,,105,317,"NIAGARA MOHAWK POWER CORP","GREEN ISL",0,,13573,"0M",1294,,190,95,3672,0,0,3067,0,0,3470,0,0,3478,0,0,2678,0,0,2110,0,0,1303,0,0,1440,0,0,1476,0,0,2837,0,0,2513,0,0,3722,0,0,6528,6,52053,"WAT","HY" 21,36,1,1,,105,320,"NIAGARA MOHAWK POWER CORP","INGHAMS",0,,13573,"0M",1294,,190,95,2951,0,0,1446,0,0,3570,0,0,3006,0,0,1806,0,0,1403,0,0,605,0,0,518,0,0,480,0,0,2716,0,0,3695,0,0,1829,0,0,2579,6,52053,"WAT","HY" 21,36,1,1,,105,325,"NIAGARA MOHAWK POWER CORP","JOHNSONVLE",0,,13573,"0M",1294,,190,95,783,0,0,709,0,0,698,0,0,730,0,0,706,0,0,415,0,0,84,0,0,196,0,0,71,0,0,754,0,0,1347,0,0,777,0,0,2580,6,52053,"WAT","HY" 21,36,1,1,,105,340,"NIAGARA MOHAWK POWER CORP","MOREAU",0,,13573,"0M",1294,"R",190,95,0,0,0,2501,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2587,6,52053,"WAT","HY" 21,36,1,1,,105,350,"NIAGARA MOHAWK POWER CORP","SCH ST COHS",0,,13573,"0M",1294,,190,95,17365,0,0,13801,0,0,18549,0,0,16246,0,0,8330,0,0,6836,0,0,4087,0,0,3410,0,0,3303,0,0,14028,0,0,23804,0,0,15352,0,0,2605,6,52053,"WAT","HY" 21,36,1,1,,105,355,"NIAGARA MOHAWK POWER CORP","SCHAGHTICKE",0,,13573,"0M",1294,,190,95,6959,0,0,4628,0,0,1779,0,0,7008,0,0,3998,0,0,2703,0,0,925,0,0,1694,0,0,513,0,0,4157,0,0,7065,0,0,4122,0,0,2606,6,52053,"WAT","HY" 21,36,1,1,,105,360,"NIAGARA MOHAWK POWER CORP","SCHUYLERVLE",0,,13573,"0M",1294,,190,95,766,0,0,454,0,0,951,0,0,408,0,0,291,0,0,185,0,0,26,0,0,77,0,0,-5,0,0,527,0,0,1089,0,0,771,0,0,2607,6,52053,"WAT","HY" 21,36,1,1,,105,365,"NIAGARA MOHAWK POWER CORP","SHERMAN",0,,13573,"0M",1294,,190,95,14937,0,0,11480,0,0,11483,0,0,9158,0,0,6495,0,0,5892,0,0,5453,0,0,6179,0,0,6999,0,0,9121,0,0,7996,0,0,9198,0,0,2609,6,52053,"WAT","HY" 21,36,1,1,,105,370,"NIAGARA MOHAWK POWER CORP","SPIER FALLS",0,,13573,"0M",1294,,190,95,22054,0,0,16130,0,0,18521,0,0,13202,0,0,8844,0,0,7373,0,0,6467,0,0,7246,0,0,8844,0,0,15741,0,0,12177,0,0,20353,0,0,2612,6,52053,"WAT","HY" 21,36,1,1,,105,380,"NIAGARA MOHAWK POWER CORP","STEWARTS BR",0,,13573,"0M",1294,,190,95,10770,0,0,11203,0,0,3959,0,0,1818,0,0,5172,0,0,2348,0,0,5366,0,0,4271,0,0,7737,0,0,2666,0,0,19084,0,0,17328,0,0,2614,6,52053,"WAT","HY" 21,36,1,1,,105,385,"NIAGARA MOHAWK POWER CORP","STUYVESANT",0,,13573,"0M",1294,,190,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2615,6,52053,"WAT","HY" 21,36,1,2,2,105,395,"NIAGARA MOHAWK POWER CORP","ALBANY",0,"LIGHT OIL",13573,"0M",1294,,190,95,0,0,220,0,0,220,0,0,220,0,0,220,0,0,220,0,0,220,0,0,201,0,0,201,0,0,195,0,0,192,0,0,189,0,0,185,2539,6,52053,"FO2","ST" 21,36,1,2,3,105,395,"NIAGARA MOHAWK POWER CORP","ALBANY",0,"HEAVY OIL",13573,"0M",1294,,190,95,58267,97691,332532,62750,94595,237938,5641,8097,184840,0,0,184840,0,0,184840,1711,4230,180610,0,0,180610,0,0,180610,0,0,180610,0,0,180610,18591,30657,149952,25930,42050,107902,2539,6,52053,"FO6","ST" 21,36,1,2,9,105,395,"NIAGARA MOHAWK POWER CORP","ALBANY",0,"NAT GAS",13573,"0M",1294,,190,95,57789,665226,0,58253,669709,0,144263,1550322,0,53054,571524,0,31237,333909,0,47841,524896,0,130139,1434248,0,147338,1604315,0,50979,541649,0,49257,521886,0,6001,121469,0,5994,104410,0,2539,6,52053,"NG","ST" 21,36,1,3,2,105,395,"NIAGARA MOHAWK POWER CORP","ALBANY",0,"LIGHT OIL",13573,"0M",1294,,190,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2539,6,52053,"FO2","IC" 21,36,1,4,2,105,395,"NIAGARA MOHAWK POWER CORP","ALBANY",0,"LIGHT OIL",13573,"0M",1294,,190,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2539,6,52053,"FO2","GT" 21,36,1,4,9,105,395,"NIAGARA MOHAWK POWER CORP","ALBANY",0,"NAT GAS",13573,"0M",1294,,190,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2539,6,52053,"NG","GT" 21,36,1,1,,105,420,"NIAGARA MOHAWK POWER CORP","GLENWOOD",0,,13573,"0M",1294,,190,95,584,0,0,584,0,0,712,0,0,35,0,0,602,0,0,501,0,0,510,0,0,499,0,0,459,0,0,493,0,0,412,0,0,213,0,0,2568,6,52053,"WAT","HY" 21,36,1,1,,105,425,"NIAGARA MOHAWK POWER CORP","HYDRAULIC R",0,,13573,"0M",1294,,190,95,0,0,0,0,0,0,0,0,0,247,0,0,1980,0,0,1737,0,0,1757,0,0,1761,0,0,1655,0,0,1715,0,0,209,0,0,0,0,0,2578,6,52053,"WAT","HY" 21,36,1,1,,105,440,"NIAGARA MOHAWK POWER CORP","WATERPORT",0,,13573,"0M",1294,,190,95,1372,0,0,1372,0,0,1447,0,0,69,0,0,924,0,0,779,0,0,723,0,0,727,0,0,684,0,0,922,0,0,936,0,0,428,0,0,2623,6,52053,"WAT","HY" 21,36,1,2,2,105,445,"NIAGARA MOHAWK POWER CORP","DUNKIRK",0,"LIGHT OIL",13573,"0M",1294,,190,95,1601,2790,0,653,1081,0,675,1178,0,599,1017,0,1403,2417,0,539,896,0,638,1090,0,1031,1725,0,723,1216,0,997,1731,0,914,1625,0,396,651,0,2554,6,52053,"FO2","ST" 21,36,1,2,6,105,445,"NIAGARA MOHAWK POWER CORP","DUNKIRK",0,"BIT COAL",13573,"0M",1294,,190,95,254022,99455,112963,311173,114689,97723,298538,114582,80138,317020,119632,52831,259603,99967,52456,255038,95545,74556,311521,120965,80149,307244,117398,77577,307482,116339,76599,257442,99939,138351,253614,100750,153571,354614,131876,151153,2554,6,52053,"BIT","ST" 21,36,1,3,2,105,445,"NIAGARA MOHAWK POWER CORP","DUNKIRK",0,"LIGHT OIL",13573,"0M",1294,,190,95,0,0,1079,0,0,1334,0,0,1300,0,0,1323,0,0,635,0,0,1174,0,0,1343,0,0,1234,0,0,1317,0,0,1090,0,0,1325,0,0,1484,2554,6,52053,"FO2","IC" 21,36,1,2,2,105,450,"NIAGARA MOHAWK POWER CORP","C R HUNTLEY",0,"LIGHT OIL",13573,"0M",1294,,190,95,681,1256,1160,349,688,1247,690,1294,1076,1705,3207,1221,704,1326,1175,1004,1818,1727,1072,1981,1452,554,1037,1301,324,570,1193,1215,2237,1180,832,1567,1213,253,461,1135,2549,6,52053,"FO2","ST" 21,36,1,2,6,105,450,"NIAGARA MOHAWK POWER CORP","C R HUNTLEY",0,"BIT COAL",13573,"0M",1294,,190,95,272246,110975,103175,276497,121255,106086,220640,91915,179212,270614,112094,162277,265384,109603,157439,267756,107734,190733,286378,118727,131748,337035,139658,120591,316597,122391,136393,245260,100618,129570,236599,99435,197282,339259,137453,168549,2549,6,52053,"BIT","ST" 21,36,1,3,2,105,450,"NIAGARA MOHAWK POWER CORP","C R HUNTLEY",0,"LIGHT OIL",13573,"0M",1294,,190,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2549,6,52053,"FO2","IC" 21,36,1,1,,105,460,"NIAGARA MOHAWK POWER CORP","OAK ORCHARD",0,,13573,"0M",1294,,190,95,0,0,0,0,0,0,0,0,0,0,0,0,178,0,0,186,0,0,185,0,0,187,0,0,174,0,0,176,0,0,46,0,0,0,0,0,2592,6,52053,"WAT","HY" 21,36,1,1,,105,465,"NIAGARA MOHAWK POWER CORP","BEEBEE IS",0,,13573,"0M",1294,,190,95,3633,0,0,2768,0,0,5208,0,0,4383,0,0,3010,0,0,1959,0,0,2292,0,0,1754,0,0,2115,0,0,4754,0,0,5881,0,0,3959,0,0,6434,6,52053,"WAT","HY" 21,36,1,1,,105,470,"NIAGARA MOHAWK POWER CORP","FEEDER DAM",0,,13573,"0M",1294,,190,95,3058,0,0,0,0,0,2491,0,0,1680,0,0,1085,0,0,869,0,0,595,0,0,648,0,0,1046,0,0,1795,0,0,3058,0,0,2885,0,0,2666,6,52053,"WAT","HY" 21,36,1,1,,115,3,"ORANGE & ROCKLAND UTL INC","GRAHAMSVILE",0,,14154,"0M",1294,,,95,7995,0,0,10213,0,0,10828,0,0,5471,0,0,3765,0,0,6843,0,0,11715,0,0,11385,0,0,6049,0,0,6915,0,0,5017,0,0,7158,0,0,2627,6,52181,"WAT","HY" 21,36,1,1,,115,5,"ORANGE & ROCKLAND UTL INC","MONGAUP FLS",0,,14154,"0M",1294,,,95,1849,0,0,830,0,0,1994,0,0,1152,0,0,218,0,0,502,0,0,749,0,0,605,0,0,91,0,0,475,0,0,1859,0,0,1637,0,0,2630,6,52181,"WAT","HY" 21,36,1,1,,115,10,"ORANGE & ROCKLAND UTL INC","RIO",0,,14154,"0M",1294,,,95,4380,0,0,1792,0,0,4911,0,0,2578,0,0,759,0,0,986,0,0,1125,0,0,978,0,0,116,0,0,1041,0,0,4467,0,0,3352,0,0,2631,6,52181,"WAT","HY" 21,36,1,1,,115,15,"ORANGE & ROCKLAND UTL INC","SWING BR 1",0,,14154,"0M",1294,,,95,1041,0,0,442,0,0,1445,0,0,608,0,0,266,0,0,374,0,0,391,0,0,409,0,0,76,0,0,299,0,0,1316,0,0,873,0,0,2633,6,52181,"WAT","HY" 21,36,1,1,,115,20,"ORANGE & ROCKLAND UTL INC","SWING BR 2",0,,14154,"0M",1294,,,95,687,0,0,340,0,0,661,0,0,428,0,0,16,0,0,-84,0,0,164,0,0,42,0,0,-68,0,0,68,0,0,889,0,0,593,0,0,2634,6,52181,"WAT","HY" 21,36,1,2,3,115,25,"ORANGE & ROCKLAND UTL INC","BOWLINE PT",0,"HEAVY OIL",14154,"0M",1294,,,95,43906,73730,656595,138605,222519,509921,36874,60431,690856,47123,77864,612992,171664,281797,399693,132603,218077,395393,121658,204130,412273,93622,159538,457749,16475,28676,564249,22772,39554,562775,23802,41159,590697,87447,145316,516559,2625,6,52181,"FO6","ST" 21,36,1,2,9,115,25,"ORANGE & ROCKLAND UTL INC","BOWLINE PT",0,"NAT GAS",14154,"0M",1294,,,95,168974,1723560,0,82272,1239913,0,246716,2463200,0,218627,2199380,0,99656,966090,0,197607,1984380,0,277722,2939140,0,259468,2692570,0,188365,2000250,0,195838,2071510,0,142378,1499610,0,41983,424600,0,2625,6,52181,"NG","ST" 21,36,1,2,3,115,30,"ORANGE & ROCKLAND UTL INC","LOVETT",0,"HEAVY OIL",14154,"0M",1294,,,95,8,15,100319,1955,3363,96956,1,1,96927,0,0,96968,162,289,96714,7,13,96701,10,18,96682,5,10,96706,6,11,96717,0,0,96732,0,0,96732,5,10,96723,2629,6,52181,"FO6","ST" 21,36,1,2,6,115,30,"ORANGE & ROCKLAND UTL INC","LOVETT",0,"BIT COAL",14154,"0M",1294,,,95,111799,49067,63359,155251,65603,75519,116513,50062,70545,69873,29960,67950,67316,29174,75567,80224,36666,84715,138923,58882,82515,118307,52178,76055,140703,61690,59229,113469,49704,60388,125569,51656,62679,132749,58514,56774,2629,6,52181,"BIT","ST" 21,36,1,2,9,115,30,"ORANGE & ROCKLAND UTL INC","LOVETT",0,"NAT GAS",14154,"0M",1294,,,95,29773,323525,0,26698,280445,0,15824,169812,0,33214,357965,0,35392,384353,0,65900,754578,0,47901,513697,0,42001,470557,0,20369,222754,0,24743,268834,0,21096,220661,0,31665,346005,0,2629,6,52181,"NG","ST" 21,36,1,4,2,115,35,"ORANGE & ROCKLAND UTL INC","HILLBURN",0,"LIGHT OIL",14154,"0M",1294,,,95,0,0,4238,0,0,4238,0,0,4238,0,0,4238,0,9,4229,0,0,4229,52,164,4065,108,334,3731,0,0,3731,0,0,3731,0,0,3731,0,0,3731,2628,6,52181,"FO2","GT" 21,36,1,4,9,115,35,"ORANGE & ROCKLAND UTL INC","HILLBURN",0,"NATURAL G",14154,"0M",1294,,,95,44,1217,0,0,0,0,37,1143,0,565,8996,0,-13,1208,0,256,5250,0,276,4745,0,945,15862,0,444,6906,0,-18,82,0,-27,456,0,24,430,0,2628,6,52181,"NG","GT" 21,36,1,4,2,115,40,"ORANGE & ROCKLAND UTL INC","SHOEMAKER",0,"LIGHT OIL",14154,"0M",1294,,,95,0,0,4599,73,30,4569,29,103,4466,-1,30,4485,1,2,4463,45,124,4068,0,0,4068,1,3,4065,0,0,4065,22,81,3984,84,247,3738,0,0,3738,2632,6,52181,"FO2","GT" 21,36,1,4,9,115,40,"ORANGE & ROCKLAND UTL INC","SHOEMAKER",0,"NAT GAS",14154,"0M",1294,,,95,217,4023,0,342,7789,0,599,11559,0,-31,207,0,1856,30143,0,3256,49008,0,4402,75566,0,4597,74746,0,2492,42150,0,713,14586,0,45,456,0,53,1654,0,2632,6,52181,"NG","GT" 21,36,1,2,1,135,1,"ROCHESTER GAS & ELEC CORP","GINNA",0,"NUCLEAR",16183,"0M",1294,,,95,351805,0,0,321771,0,0,293087,0,0,-2750,0,0,299117,0,0,334397,0,0,342637,0,0,305248,0,0,336763,0,0,353447,0,0,342871,0,0,354889,0,0,6122,6,52501,"UR","ST" 21,36,1,1,,135,5,"ROCHESTER GAS & ELEC CORP","MILLS M 172",0,,16183,"0M",1294,,,95,68,0,0,0,0,0,79,0,0,31,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2636,6,52501,"WAT","HY" 21,36,1,1,,135,10,"ROCHESTER GAS & ELEC CORP","MT MORR 160",0,,16183,"0M",1294,,,95,0,0,0,75,0,0,0,0,0,0,0,0,49,0,0,121,0,0,87,0,0,44,0,0,16,0,0,124,0,0,132,0,0,67,0,0,2637,6,52501,"WAT","HY" 21,36,1,1,,135,15,"ROCHESTER GAS & ELEC CORP","ROCHESTER 2",0,,16183,"0M",1294,,,95,3983,0,0,3890,0,0,4861,0,0,4119,0,0,4073,0,0,2681,0,0,1898,0,0,1483,0,0,708,0,0,3228,0,0,4230,0,0,3509,0,0,2639,6,52501,"WAT","HY" 21,36,1,1,,135,25,"ROCHESTER GAS & ELEC CORP","ROCHESTER 5",0,,16183,"0M",1294,,,95,18727,0,0,8869,0,0,21670,0,0,13445,0,0,7303,0,0,4173,0,0,5885,0,0,2422,0,0,1347,0,0,9730,0,0,15462,0,0,12738,0,0,2641,6,52501,"WAT","HY" 21,36,1,1,,135,28,"ROCHESTER GAS & ELEC CORP","RCHESTER 26",0,,16183,"0M",1294,,,95,596,0,0,1040,0,0,1215,0,0,1302,0,0,1083,0,0,420,0,0,405,0,0,282,0,0,135,0,0,726,0,0,1174,0,0,1054,0,0,2638,6,52501,"WAT","HY" 21,36,1,1,,135,35,"ROCHESTER GAS & ELEC CORP","WISCOY 170",0,,16183,"0M",1294,,,95,517,0,0,408,0,0,590,0,0,391,0,0,204,0,0,97,0,0,121,0,0,83,0,0,55,0,0,240,0,0,470,0,0,462,0,0,2646,6,52501,"WAT","HY" 21,36,1,2,2,135,45,"ROCHESTER GAS & ELEC CORP","ROCHESTER 3",0,"LIGHT OIL",16183,"0M",394,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,102,143,2305,77,143,2008,122,214,1718,91,167,1882,68,119,1700,27,58,1645,2640,6,52501,"FO2","ST" 21,36,1,2,3,135,45,"ROCHESTER GAS & ELEC CORP","ROCHESTER 3",0,"HEAVY OIL",16183,"0M",1294,"R",,95,27,48,2860,14,24,2809,14,24,2745,14,24,2703,0,0,2703,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2640,6,52501,"FO6","ST" 21,36,1,2,6,135,45,"ROCHESTER GAS & ELEC CORP","ROCHESTER 3",0,"BIT COAL",16183,"0M",1294,,,95,36334,13900,770,42264,15300,1458,40715,15300,1556,45572,16900,817,17481,6500,1591,36715,14100,1438,41179,15700,936,37637,15017,1800,37010,13802,1800,27740,10832,1630,33466,12558,1431,34731,13210,1105,2640,6,52501,"BIT","ST" 21,36,1,4,2,135,45,"ROCHESTER GAS & ELEC CORP","ROCHESTER 3",0,"LIGHT OIL",16183,"0M",1294,,,95,26,81,0,4,27,0,13,41,0,3,18,0,0,0,0,6,34,0,4,6,0,46,154,0,25,76,0,8,26,0,13,63,0,1,7,0,2640,6,52501,"FO2","GT" 21,36,1,2,2,135,50,"ROCHESTER GAS & ELEC CORP","ROCHESTER 7",0,"LIGHT OIL",16183,"0M",1294,,,95,299,571,1111,90,167,1127,375,690,1162,173,310,1211,249,452,1299,566,1071,1121,331,643,1190,434,833,1065,37,71,1065,373,738,1065,345,643,958,311,571,1102,2642,6,52501,"FO2","ST" 21,36,1,2,6,135,50,"ROCHESTER GAS & ELEC CORP","ROCHESTER 7",0,"BIT COAL",16183,"0M",1294,,,95,66357,27700,114902,86515,35300,90431,90609,36600,83204,137634,53400,75835,121093,47500,85250,104898,43000,113923,112687,47700,112973,116634,48507,127749,110993,45157,153399,77990,33362,173353,81051,33064,173047,90029,35948,150667,2642,6,52501,"BIT","ST" 21,36,1,4,2,135,60,"ROCHESTER GAS & ELEC CORP","ROCHESTER 9",0,"LIGHT OIL",16183,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2644,6,52501,"FO2","GT" 21,36,1,4,9,135,60,"ROCHESTER GAS & ELEC CORP","ROCHESTER 9",0,"NAT GAS",16183,"0M",1294,,,95,26,383,0,2,74,0,14,216,0,4,174,0,0,0,0,8,290,0,17,280,0,3,89,0,24,381,0,0,0,0,3,98,0,8,143,0,2644,6,52501,"NG","GT" 21,36,5,3,2,578,5,"FREEPORT (VILLAGE OF)","PLANT NO 2",0,"LIGHT OIL",6775,"0M",1294,,,95,1463,3067,3172,1434,3271,2622,413,1557,2551,-162,121,3525,-118,217,5782,984,2264,6164,3712,7100,3595,3729,7301,5720,584,1625,6684,895,1423,5789,787,2037,3752,1869,3903,3213,2679,6,51057,"FO2","IC" 21,36,5,4,2,578,5,"FREEPORT (VILLAGE OF)","PLANT NO 2",0,"LIGHT OIL",6775,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2,12,0,13,58,0,18,95,0,0,0,0,0,0,0,0,0,0,0,0,0,2679,6,51057,"FO2","GT" 21,36,5,3,2,578,10,"FREEPORT (VILLAGE OF)","PLANT NO 1",0,"LIGHT OIL",6775,"0M",1294,,,95,182,658,1479,376,1032,1630,468,1254,1391,320,920,1697,251,803,1542,452,1093,1119,571,1281,1220,740,1757,1321,639,1551,1424,175,575,1295,402,1078,1704,465,1231,1436,2678,6,51057,"FO2","IC" 21,36,5,1,,586,1,"GOUVERNEUR (CITY OF)","GOUVERNEUR",0,,7422,"0A",1294,,,95,46,0,0,92,0,0,47,0,0,50,0,0,50,0,0,38,0,0,13,0,0,45,0,0,29,0,0,20,0,0,26,0,0,41,0,0,2680,6,51137,"WAT","HY" 21,36,5,3,2,599,1,"GREENPORT (CITY OF)","GREENPORT",0,"LIGHT OIL",7630,"0A",1294,,,95,-32,0,183,-32,0,183,-27,0,183,0,2,181,0,0,0,0,1,180,-20,0,180,-4,28,152,-10,14,182,-19,0,182,0,0,182,-1,26,181,2681,6,51177,"FO2","IC" 21,36,5,2,2,624,1,"JAMESTOWN (CITY OF)","S A CARLSON",0,"LIGHT OIL",9645,"0M",1294,,,95,105,273,377,41,102,275,21,59,394,24,59,335,20,54,281,26,64,394,57,144,250,59,144,281,26,66,215,26,69,323,44,114,209,51,136,250,2682,6,51437,"FO2","ST" 21,36,5,2,6,624,1,"JAMESTOWN (CITY OF)","S A CARLSON",0,"BIT COAL",9645,"0M",1294,,,95,17974,10638,3526,17648,10013,3826,11794,7305,3597,9844,5439,3428,9879,6006,2629,11487,6255,2811,13511,7717,2530,13208,7291,3578,9538,5398,3370,10505,6096,2827,12704,7245,3946,16956,10165,3924,2682,6,51437,"BIT","ST" 21,36,5,3,2,675,1,"ROCKVILLE CTR(VILLAGE OF)","ROCKVILLE C",0,"LIGHT OIL",16217,"0M",1294,,,95,105,294,2332,321,741,2091,43,283,1808,-60,82,1726,-18,114,2338,244,637,2368,957,2138,1919,2160,4073,1884,560,1129,2277,20,216,2061,38,213,2151,101,381,1770,2695,6,52509,"FO2","IC" 21,36,5,3,9,675,1,"ROCKVILLE CTR(VILLAGE OF)","ROCKVILLE C",0,"NAT GAS",16217,"0M",1294,,,95,642,7257,0,510,5912,0,15,471,0,0,325,0,-11,282,0,1931,20033,0,4455,46010,0,2523,26516,0,352,4031,0,47,1369,0,46,1025,0,450,5750,0,2695,6,52509,"NG","IC" 21,36,5,3,2,700,5,"SKANEATELES VILLAGE OF","SKANEATELES",0,"LIGHT OIL",17280,"0A",1294,"R",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2697,6,52670,"FO2","IC" 21,36,5,1,,712,1,"SPRINGVILLE (CITY OF)","SPRINGVILLE",0,,17846,"0A",1294,,,95,145,0,0,118,0,0,104,0,0,166,0,0,172,0,0,129,0,0,84,0,0,63,0,0,12,0,0,39,0,0,110,0,0,124,0,0,2698,6,52772,"WAT","HY" 21,36,5,1,,725,1,"WATERTOWN (CITY OF)","WATERTOWN",0,,20188,"0A",1294,,,95,2508,0,0,1826,0,0,2861,0,0,2520,0,0,2042,0,0,715,0,0,684,0,0,252,0,0,458,0,0,1925,0,0,2671,0,0,2141,0,0,2700,6,53199,"WAT","HY" 21,36,9,1,,668,1,"POWER AUTHY OF ST OF N Y","LEWISTON PG",0,"C-PUMPSTG",15296,"0M",1294,,,95,-23392,48481,0,-16321,48107,0,-18062,52914,0,-34170,75041,0,-32754,81523,0,-35246,84639,0,-35971,80543,0,-31970,78905,0,-33926,76500,0,-34404,82531,0,-25619,66689,0,-26848,63831,0,2692,6,52375,"WAT","HY" 21,36,9,2,1,668,1,"POWER AUTHY OF ST OF N Y","FITZPATRICK",0,"NUCLEAR",15296,"0M",1294,,,95,0,0,0,0,0,0,34055,0,0,544665,0,0,562170,0,0,384520,0,0,579310,0,0,577530,0,0,402855,0,0,590100,0,0,572680,0,0,580835,0,0,6110,6,52375,"UR","ST" 21,36,9,1,,668,3,"POWER AUTHY OF ST OF N Y","MOSES NIAG",0,,15296,"0M",1294,,,95,1463973,0,0,1230590,0,0,1418230,0,0,1163933,0,0,1279083,0,0,1132981,0,0,1197133,0,0,1148436,0,0,1021706,0,0,1145560,0,0,1382957,0,0,1354956,0,0,2693,6,52375,"WAT","HY" 21,36,9,2,1,668,3,"POWER AUTHY OF ST OF N Y","INDIAN PT 3",0,"NUCLEAR",15296,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,17,0,0,434533,0,0,716433,0,0,320544,0,0,0,0,0,0,0,0,-2,0,0,8907,6,52375,"UR","ST" 21,36,9,1,,668,5,"POWER AUTHY OF ST OF N Y","MOSES PR DM",0,,15296,"0M",1294,,,95,524759,0,0,481624,0,0,585412,0,0,549618,0,0,532348,0,0,526743,0,0,545520,0,0,559232,0,0,538635,0,0,554432,0,0,576778,0,0,569302,0,0,2694,6,52375,"WAT","HY" 21,36,9,1,,668,8,"POWER AUTHY OF ST OF N Y","BLENHEIM G",0,"P-PUMPSTG",15296,"0M",1294,,,95,-80117,223900,0,-66116,187582,0,-64757,198518,0,-71547,180530,0,-58305,185571,0,-61293,196731,0,-78558,215353,0,-75753,237341,0,-63547,183628,0,-66325,194141,0,-57795,177791,0,-70135,192222,0,2691,6,52375,"WAT","HY" 21,36,9,2,3,668,15,"POWER AUTHY OF ST OF N Y","POLETTI",0,"HEAVY OIL",15296,"0M",1294,,,95,33400,61649,303226,126069,209523,203682,20403,35475,168236,17269,37577,130679,19806,35708,94972,47803,62254,32718,36004,60668,68293,14149,23707,150452,35247,61190,430389,17481,30727,459549,62862,110242,349307,252627,421942,245156,2491,6,52375,"FO6","ST" 21,36,9,2,9,668,15,"POWER AUTHY OF ST OF N Y","POLETTI",0,"NAT GAS",15296,"0M",1294,,,95,99454,1128061,0,99940,1020449,0,202945,2167293,0,211435,2738075,0,258894,2862705,0,324525,2604689,0,262599,2721610,0,310920,3222176,0,205757,2168448,0,224611,2374781,0,128580,1368464,0,2466,25078,0,2491,6,52375,"NG","ST" 21,36,9,1,,668,20,"POWER AUTHY OF ST OF N Y","ASHOKAN",0,,15296,"0M",1294,,,95,1615,0,0,587,0,0,1045,0,0,2214,0,0,2450,0,0,2277,0,0,2117,0,0,2126,0,0,1756,0,0,1286,0,0,1083,0,0,1303,0,0,88,6,52375,"WAT","HY" 21,36,9,1,,668,25,"POWER AUTHY OF ST OF N Y","KENSICO",0,,15296,"0M",1294,,,95,802,0,0,73,0,0,0,0,0,1521,0,0,150,0,0,271,0,0,1411,0,0,1244,0,0,1418,0,0,1191,0,0,880,0,0,0,0,0,650,6,52375,"WAT","HY" 21,36,9,1,,668,30,"POWER AUTHY OF ST OF N Y","JARVIS",0,,15296,"0M",1294,,,95,4048,0,0,2165,0,0,2416,0,0,2485,0,0,1720,0,0,1501,0,0,1162,0,0,1003,0,0,575,0,0,2833,0,0,5091,0,0,2476,0,0,808,6,52375,"WAT","HY" 21,36,9,1,,668,35,"POWER AUTHY OF ST OF N Y","CRESCENT",0,,15296,"0M",1294,,,95,6303,0,0,4034,0,0,7316,0,0,4624,0,0,3019,0,0,2031,0,0,104,0,0,713,0,0,703,0,0,3132,0,0,6120,0,0,4690,0,0,2685,6,52375,"WAT","HY" 21,36,9,1,,668,40,"POWER AUTHY OF ST OF N Y","VISCHER FER",0,,15296,"0M",1294,,,95,5945,0,0,3714,0,0,6024,0,0,4504,0,0,2789,0,0,1833,0,0,986,0,0,123,0,0,654,0,0,2259,0,0,5980,0,0,4591,0,0,2686,6,52375,"WAT","HY" 21,36,9,5,9,668,45,"POWER AUTHY OF ST OF N Y","FLYNN",0,"WASTE HT",15296,"0M",1294,,,95,24819,192100,0,17369,134483,0,27383,211172,0,18948,146928,0,26056,199854,0,24430,188777,0,23492,184084,0,25126,194127,0,24424,188668,0,23749,183457,0,20261,158951,0,19720,154115,0,7314,6,52375,"WH","CC" 21,36,9,6,2,668,45,"POWER AUTHY OF ST OF N Y","FLYNN",0,"LIGHT OIL",15296,"0M",1294,,,95,7722,10369,101959,21462,28859,72145,0,0,72242,14,20,72083,0,0,72104,0,0,72094,0,0,72044,0,0,72052,0,0,72062,157,211,71873,9447,12866,58992,27271,36998,78070,7314,6,52375,"FO2","CT" 21,36,9,6,9,668,45,"POWER AUTHY OF ST OF N Y","FLYNN",0,"NAT GAS",15296,"0M",1294,,,95,74458,576302,0,52111,403450,0,82153,633518,0,56849,440785,0,78170,599562,0,73293,566331,0,71470,552251,0,75381,582382,0,73276,566005,0,71251,550371,0,60784,476853,0,59162,462344,0,7314,6,52375,"NG","CT" 22,34,1,2,2,24,1,"ATLANTIC CITY ELEC CO","DEEPWATER",0,"LIGHT OIL",963,"0M",1294,,181,95,0,0,123,81,130,93,0,0,131,0,0,138,14,28,165,67,129,202,80,160,147,5,10,137,40,91,189,0,29,160,0,29,131,4,8,123,2384,3,56513,"FO2","ST" 22,34,1,2,3,24,1,"ATLANTIC CITY ELEC CO","DEEPWATER",0,"HEAVY OIL",963,"0M",1294,,181,95,1345,2425,95467,4563,6516,88951,0,0,88951,0,0,88261,0,0,88261,1177,2026,86235,3361,5958,80277,5273,9351,70926,5555,8624,62302,0,0,62302,0,0,62302,0,0,62302,2384,3,56513,"FO6","ST" 22,34,1,2,6,24,1,"ATLANTIC CITY ELEC CO","DEEPWATER",0,"BIT COAL",963,"0M",1294,,181,95,29945,12519,39313,35838,15203,23710,8276,3561,20149,0,0,34389,5810,3059,52665,34469,14723,52014,42129,18253,40567,44451,19515,27979,11926,4625,44084,33654,13941,51248,53859,21346,70836,57721,22974,63900,2384,3,56513,"BIT","ST" 22,34,1,2,9,24,1,"ATLANTIC CITY ELEC CO","DEEPWATER",0,"NAT GAS",963,"0M",1294,,181,95,1491,16310,0,0,0,0,944,9940,0,1878,22040,0,11307,122240,0,11062,117040,0,27862,302860,0,29442,321050,0,12534,120040,0,807,8090,0,1552,15370,0,0,0,0,2384,3,56513,"NG","ST" 22,34,1,4,2,24,1,"ATLANTIC CITY ELEC CO","DEEPWATER",0,"LIGHT OIL",963,"0M",1294,,181,95,-8,0,770,27,44,729,14,39,690,20,103,587,0,0,587,0,0,587,0,0,587,0,0,587,0,0,587,0,0,587,0,0,587,0,0,0,2384,3,56513,"FO2","GT" 22,34,1,4,9,24,1,"ATLANTIC CITY ELEC CO","DEEPWATER",0,"NAT GAS",963,"0M",1294,,181,95,-8,0,0,0,0,0,0,0,0,0,0,0,0,0,0,629,6657,0,3831,41649,0,3649,39793,0,1027,14649,0,628,9167,0,1061,10505,0,694,6875,0,2384,3,56513,"NG","GT" 22,34,1,4,2,24,2,"ATLANTIC CITY ELEC CO","MISSOURI AV",0,"LIGHT OIL",963,"0M",1294,,181,95,-4,100,9869,278,791,9635,3,53,9582,-21,5,9576,-17,8,9568,177,455,9113,2101,5546,7361,1882,5382,8451,605,2439,10201,-18,16,10185,-16,19,10167,2,70,10097,2383,3,56513,"FO2","GT" 22,34,1,2,2,24,5,"ATLANTIC CITY ELEC CO","B L ENGLAND",0,"LIGHT OIL",963,"0M",1294,,181,95,510,999,1734,317,596,1818,213,395,1756,107,200,1734,125,224,1843,424,778,1734,424,814,1508,552,1027,1647,500,1086,1588,450,958,1654,643,1122,1377,242,442,1435,2378,3,56513,"FO2","ST" 22,34,1,2,3,24,5,"ATLANTIC CITY ELEC CO","B L ENGLAND",0,"HEAVY OIL",963,"0M",1294,,181,95,4583,8307,99579,7833,13643,103560,0,0,103560,0,0,103560,0,0,103560,8731,14731,88829,37756,66914,51324,29729,50813,69931,850,2842,113855,18800,33751,80103,0,0,80103,15770,26499,87607,2378,3,56513,"FO6","ST" 22,34,1,2,6,24,5,"ATLANTIC CITY ELEC CO","B L ENGLAND",0,"BIT COAL",963,"0M",1294,,181,95,68381,30282,165387,127521,54088,125492,123787,53379,95025,85963,36061,88754,176115,72435,61413,155554,64926,62658,185411,80134,49009,173888,73305,41509,130330,53650,71904,83030,32962,118367,145947,62033,109160,196038,81549,81843,2378,3,56513,"BIT","ST" 22,34,1,3,2,24,5,"ATLANTIC CITY ELEC CO","B L ENGLAND",0,"LIGHT OIL",963,"0M",1294,,181,95,0,0,0,5,11,0,0,0,0,0,0,0,0,0,0,12,23,0,133,257,0,321,597,0,5,10,0,0,0,0,0,0,0,0,0,0,2378,3,56513,"FO2","IC" 22,34,1,4,2,24,20,"ATLANTIC CITY ELEC CO","MIDDLE STA",0,"LIGHT OIL",963,"0M",1294,,181,95,-834,144,15410,-227,1590,15128,-1342,459,14669,-815,159,14510,-333,16,14494,-558,315,9113,2009,5421,12193,2243,7786,14637,-670,677,15327,-729,232,15284,-745,423,15069,-730,254,14814,2382,3,56513,"FO2","GT" 22,34,1,4,2,24,25,"ATLANTIC CITY ELEC CO","CEDAR STA",0,"LIGHT OIL",963,"0M",1294,,181,95,-474,179,21675,-321,918,21875,-42,70,21804,-546,56,21748,-110,38,21710,62,61,21650,3843,9672,14702,3756,10444,18151,-253,1075,20407,-631,431,21246,-535,219,21027,-679,322,20705,2380,3,56513,"FO2","GT" 22,34,1,4,2,24,30,"ATLANTIC CITY ELEC CO","CARLL CORNR",0,"LIGHT OIL",963,"0M",1294,,181,95,-28,8,13554,78,379,13175,-43,0,13175,-20,0,13175,-965,8,13167,-121,166,13002,1394,2899,10102,1615,4499,9171,-32,0,13713,-16,0,14849,-44,0,14849,49,332,14517,2379,3,56513,"FO2","GT" 22,34,1,4,9,24,30,"ATLANTIC CITY ELEC CO","CARLL CORNR",0,"NAT GAS",963,"0M",1294,,181,95,35,1120,0,452,8170,0,-76,50,0,-19,1010,0,73,2450,0,835,15970,0,6072,93380,0,5324,82370,0,-117,28460,0,861,14250,0,-44,7170,0,172,150,0,2379,3,56513,"NG","GT" 22,34,1,4,2,24,32,"ATLANTIC CITY ELEC CO","MICKETON ST",0,"LIGHT OIL",963,"0M",1294,,181,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,8008,3,56513,"FO2","GT" 22,34,1,4,9,24,32,"ATLANTIC CITY ELEC CO","MICKETON ST",0,"NAT GAS",963,"0M",1294,,181,95,665,11020,0,1084,16250,0,714,11030,0,1017,15170,0,334,6070,0,2355,35610,0,9801,143090,0,8665,129480,0,2856,42750,0,30,1480,0,2277,33340,0,276,5380,0,8008,3,56513,"NG","GT" 22,34,1,4,2,24,33,"ATLANTIC CITY ELEC CO","CUMBERLAND",0,"LIGHT OIL",963,"0M",1294,,181,95,-76,0,18141,-10,0,18141,-38,0,18141,-31,0,18141,-30,0,18141,0,0,18141,5894,12888,17367,7323,16647,12470,3,249,14661,0,0,17077,-158,198,17249,60,412,16838,5083,3,56513,"FO2","GT" 22,34,1,4,9,24,33,"ATLANTIC CITY ELEC CO","CUMBERLAND",0,"NAT GAS",963,"0M",1294,,181,95,-76,0,0,-10,0,0,-38,0,0,-31,0,0,0,0,0,-27,130,0,342,4020,0,16,200,0,1,380,0,-93,0,0,0,0,0,101,3810,0,5083,3,56513,"NG","GT" 22,34,1,4,2,24,35,"ATLANTIC CITY ELEC CO","MANTU DEPOT",0,"LIGHT OIL",963,"0M",1294,,181,95,0,0,53843,0,0,50861,0,0,80853,0,0,80853,0,0,80853,0,0,80853,0,0,58245,0,0,12871,0,0,12871,0,0,52645,0,0,52645,0,0,82122,8803,3,56513,"FO2","GT" 22,34,1,4,3,24,40,"ATLANTIC CITY ELEC CO","MANTU DEPOT",0,"HEAVY OIL",963,"0M",1294,,181,95,0,0,128847,0,0,111223,0,0,111223,0,0,111223,0,0,111223,0,0,111223,0,0,81814,0,0,111865,0,0,111865,0,0,115694,0,0,115694,0,0,131074,8804,3,56513,"FO6","GT" 22,34,1,4,2,24,45,"ATLANTIC CITY ELEC CO","SHERMAN AVE",0,"LIGHT OIL",963,"0M",1294,,181,95,70,186,14708,-45,0,14708,-30,0,14708,0,0,14708,-11,0,14708,0,0,14708,0,0,14708,-190,0,14708,0,0,14708,0,0,14708,76,193,14515,232,590,14513,7288,3,56513,"FO2","GT" 22,34,1,4,9,24,45,"ATLANTIC CITY ELEC CO","SHERMAN AVE",0,"NAT GAS",963,"0M",1294,,181,95,1386,19950,0,-45,0,0,-30,0,0,0,0,0,0,0,0,0,0,0,0,0,0,-190,0,0,0,0,0,0,0,0,1704,23780,0,2984,41500,0,7288,3,56513,"NG","GT" 22,34,1,2,1,50,1,"GPU NUCLEAR CORP","OYSTER CRK",0,"NUCLEAR",7423,"0M",1294,,,95,471880,0,0,400185,0,0,466040,0,0,457427,0,0,440064,0,0,447364,0,0,438119,0,0,420825,0,0,447572,0,0,468215,0,0,428423,0,0,307964,0,0,2388,3,58850,"UR","ST" 22,34,1,1,,78,5,"JERSEY CENTRAL PWR & LGT","YARDS CR JO",0,"P-PUMPSTG",9726,"0M",1294,,,95,-9476,31075,0,-6121,19602,0,-8606,30644,0,-9596,30043,0,-9800,36086,0,-15417,52655,0,-13938,46076,0,-11848,42668,0,-7525,27636,0,0,0,0,0,0,0,-2205,5358,0,6522,3,56512,"WAT","HY" 22,34,1,4,2,78,7,"JERSEY CENTRAL PWR & LGT","GLEN GARDNR",0,"LIGHT OIL",9726,"0M",1294,,,95,357,1074,17830,457,1242,16588,29,247,16340,30,141,16199,0,0,16199,360,1062,15138,0,0,15138,0,0,15138,149,445,14693,21,60,14633,69,223,14409,10,63,16838,8227,3,56512,"FO2","GT" 22,34,1,4,9,78,7,"JERSEY CENTRAL PWR & LGT","GLEN GARDNR",0,"NAT GAS",9726,"0M",1294,,,95,1,10,0,31,485,0,2,90,0,0,0,0,0,0,0,698,11690,0,15562,248730,0,18982,309960,0,4246,71580,0,3046,50662,0,1111,20594,0,10,377,0,8227,3,56512,"NG","GT" 22,34,1,2,3,78,9,"JERSEY CENTRAL PWR & LGT","GILBERT",0,"HEAVY OIL",9726,"0M",1294,,,95,268,611,153901,2150,4403,149484,0,0,149488,0,0,149544,0,0,149379,0,0,150080,0,0,150051,0,0,149974,0,0,150075,0,0,149949,0,0,149926,8990,12417,137518,2393,3,56512,"FO6","ST" 22,34,1,2,9,78,9,"JERSEY CENTRAL PWR & LGT","GILBERT",0,"NAT GAS",9726,"0M",1294,,,95,1658,32084,0,198,3865,0,-452,0,0,-364,0,0,-363,0,0,6011,80854,0,28213,364986,0,24888,306021,0,915,14545,0,340,8670,0,825,13717,0,331,2840,0,2393,3,56512,"NG","ST" 22,34,1,4,2,78,9,"JERSEY CENTRAL PWR & LGT","GILBERT",0,"LIGHT OIL",9726,"0M",1294,,,95,150,431,0,803,2747,0,39,127,0,0,0,0,0,0,0,1,8,0,1,3,0,791,2604,0,31,88,0,0,0,0,0,0,0,0,0,0,2393,3,56512,"FO2","GT" 22,34,1,4,9,78,9,"JERSEY CENTRAL PWR & LGT","GILBERT",0,"NAT GAS",9726,"0M",1294,,,95,1,16,0,0,0,0,1,15,0,0,0,0,0,0,0,3,79,0,2862,50800,0,6493,121452,0,911,15880,0,4,174,0,979,364,0,29,249,0,2393,3,56512,"NG","GT" 22,34,1,5,2,78,9,"JERSEY CENTRAL PWR & LGT","GILBERT",0,"LIGHT OIL",9726,"0M",1294,,,95,728,0,0,3136,0,0,1259,0,0,1612,0,0,-587,0,0,5741,0,0,26058,0,0,28272,0,0,20554,0,0,8047,0,0,19296,0,0,18926,0,0,2393,3,56512,"FO2","CC" 22,34,1,5,9,78,9,"JERSEY CENTRAL PWR & LGT","GILBERT",0,"WASTE HT",9726,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2393,3,56512,"NG","CC" 22,34,1,6,2,78,9,"JERSEY CENTRAL PWR & LGT","GILBERT",0,"LIGHT OIL",9726,"0M",1294,,,95,1147,2566,252704,5572,11989,236313,1136,2545,232067,367,826,230086,0,0,229824,2660,6112,221348,82,189,219853,2038,4709,211204,942,1977,207539,163,373,205587,83,183,203671,5739,8660,193069,2393,3,56512,"FO2","CT" 22,34,1,6,9,78,9,"JERSEY CENTRAL PWR & LGT","GILBERT",0,"NAT GAS",9726,"0M",1294,,,95,5385,68331,0,8729,106467,0,6306,80671,0,7352,94029,0,-100,0,0,15594,203104,0,61026,877903,0,70864,931070,0,54572,701754,0,24094,329931,0,60664,796524,0,81101,693848,0,2393,3,56512,"NG","CT" 22,34,1,2,3,78,10,"JERSEY CENTRAL PWR & LGT","SAYREVILLE",0,"HEAVY OIL",9726,"0M",1294,,,95,4224,7914,90214,19448,37587,72103,7,16,72200,0,0,72163,792,1710,90373,6448,15362,75189,42812,86857,27305,24793,50118,55888,1650,3646,52242,0,0,71301,7,18,90540,10844,23847,66865,2390,3,56512,"FO6","ST" 22,34,1,2,9,78,10,"JERSEY CENTRAL PWR & LGT","SAYREVILLE",0,"NAT GAS",9726,"0M",1294,,,95,20137,245800,0,2651,32100,0,6917,89800,0,-727,100,0,-407,2800,0,141,2100,0,224,4900,0,16338,199000,0,1429,25400,0,-704,0,0,2904,47900,0,306,4100,0,2390,3,56512,"NG","ST" 22,34,1,4,2,78,10,"JERSEY CENTRAL PWR & LGT","SAYREVILLE",0,"LIGHT OIL",9726,"0M",1294,,,95,93,224,31996,752,2238,29758,0,0,29758,0,0,29758,139,640,29118,0,0,29118,0,0,29118,0,0,29118,0,0,29118,0,0,29118,0,0,29118,0,0,29118,2390,3,56512,"FO2","GT" 22,34,1,4,9,78,10,"JERSEY CENTRAL PWR & LGT","SAYREVILLE",0,"NAT GAS",9726,"0M",1294,,,95,1500,19800,0,1294,21300,0,831,12100,0,898,13300,0,187,4800,0,2507,37100,0,16534,266200,0,24165,379300,0,3245,51100,0,2451,37300,0,265,3800,0,22,300,0,2390,3,56512,"NG","GT" 22,34,1,2,3,78,15,"JERSEY CENTRAL PWR & LGT","WERNER",0,"HEAVY OIL",9726,"0M",1294,,,95,259,628,28845,5405,11437,18060,1926,4703,13792,-265,311,13764,-275,69,13780,1352,3366,28845,10346,20351,28459,7922,15595,12784,55,70,13159,-271,197,32022,-298,546,32144,3509,7954,24818,2385,3,56512,"FO6","ST" 22,34,1,4,2,78,15,"JERSEY CENTRAL PWR & LGT","WERNER",0,"LIGHT OIL",9726,"0M",1294,,,95,44,115,40240,398,1664,37864,88,236,37615,0,0,37379,13,702,36473,348,618,35855,2640,8238,27453,4764,13326,33888,215,290,33598,10,269,33202,0,25,42792,3,278,41910,2385,3,56512,"FO2","GT" 22,34,1,4,2,78,20,"JERSEY CENTRAL PWR & LGT","FORKED RVR",0,"LIGHT OIL",9726,"0M",1294,,,95,0,0,16388,1066,2219,17602,713,1618,15984,0,0,15971,0,0,15989,0,0,15969,0,0,15974,0,0,15980,0,0,15980,5,12,15970,0,0,15994,221,489,15505,7138,3,56512,"FO2","GT" 22,34,1,4,9,78,20,"JERSEY CENTRAL PWR & LGT","FORKED RVR",0,"NAT GAS",9726,"0M",1294,,,95,364,4569,0,160,1908,0,1306,15609,0,1647,20147,0,1120,14174,0,2225,28309,0,12875,162923,0,11844,149957,0,4227,53220,0,1880,23454,0,1759,25611,0,749,9475,0,7138,3,56512,"NG","GT" 22,34,1,2,1,131,1,"PUBLIC SERV ELEC & GAS CO","SALEM",0,"NUCLEAR",15477,"0M",1294,,,95,818199,0,0,47631,0,0,687443,0,0,753981,0,0,247176,0,0,-8310,0,0,-7985,0,0,-5500,0,0,-3133,0,0,-2112,0,0,-2002,0,0,-2639,0,0,2410,3,52414,"UR","ST" 22,34,1,2,1,131,1,"PUBLIC SERV ELEC & GAS CO","HOPE CREEK",0,"NUCLEAR",15477,"0M",1294,,,95,778188,0,0,711976,0,0,566874,0,0,750262,0,0,767051,0,0,742345,0,0,309223,0,0,760021,0,0,742281,0,0,733449,0,0,210606,0,0,-8357,0,0,6118,3,52414,"UR","ST" 22,34,1,2,1,131,2,"PUBLIC SERV ELEC & GAS CO","SALEM",0,"NUCLEAR",15477,"0M",1294,,,95,-17867,0,0,12090,0,0,369001,0,0,767911,0,0,765246,0,0,157494,0,0,-5523,0,0,-7400,0,0,-4042,0,0,-4499,0,0,-4002,0,0,-3638,0,0,2410,3,52414,"UR","ST" 22,34,1,4,2,131,2,"PUBLIC SERV ELEC & GAS CO","BAYONNE 1",0,"LIGHT OIL",15477,"0M",1294,,,95,-19,40,3837,74,282,453,-9,0,453,-44,0,1097,-18,0,3930,-2,0,3930,252,805,3125,134,585,2744,-24,0,3373,-42,0,3744,0,26,3744,-33,25,3898,2397,3,52414,"FO2","GT" 22,34,1,2,9,131,3,"PUBLIC SERV ELEC & GAS CO","BERGEN",0,"NAT GAS",15477,"0M",1294,,,95,-2112,0,0,-2514,3702,0,8759,159907,0,3706,93882,0,82739,754972,0,167861,1271630,0,281448,2131152,0,334990,2488678,0,184434,1379778,0,154884,1248547,0,151551,1232638,0,151368,1176288,0,2398,3,52414,"NG","ST" 22,34,1,4,2,131,3,"PUBLIC SERV ELEC & GAS CO","BERGEN",0,"LIGHT OIL",15477,"0M",1294,,,95,0,0,0,0,0,21622,0,0,21622,0,0,38592,0,0,38592,0,0,61623,2310,3197,102565,0,0,118429,0,0,118396,3765,5367,113029,4832,7091,116664,465,652,117805,2398,3,52414,"FO2","GT" 22,34,1,4,9,131,3,"PUBLIC SERV ELEC & GAS CO","BERGEN",0,"NAT GAS",15477,"0M",1294,,,95,-13,0,0,0,0,0,-6,664,0,-6,644,0,-9,0,0,0,0,0,347,35845,0,505,5090,0,0,0,0,-7,0,0,-7,0,0,-8,0,0,2398,3,52414,"NG","GT" 22,34,1,2,2,131,5,"PUBLIC SERV ELEC & GAS CO","BURLINGTON",0,"LIGHT OIL",15477,"0M",1294,,,95,922,1740,0,1014,1683,0,707,1131,0,668,1366,0,0,0,0,911,1528,0,1631,2761,0,200,501,0,0,0,0,0,0,0,0,0,0,0,0,0,2399,3,52414,"FO2","ST" 22,34,1,2,3,131,5,"PUBLIC SERV ELEC & GAS CO","BURLINGTON",0,"HEAVY OIL",15477,"0M",1294,,,95,9046,15688,55522,11250,17153,88452,0,0,88452,0,0,88452,-534,0,88437,2949,4515,83916,25958,40320,43596,1803,5025,88868,-545,0,88868,-541,0,88868,-541,0,88868,-573,0,88868,2399,3,52414,"FO6","ST" 22,34,1,4,2,131,5,"PUBLIC SERV ELEC & GAS CO","BURLINGTON",0,"LIGHT OIL",15477,"0M",1294,,,95,1176,2221,83444,10436,17314,64340,158,253,93381,55,114,91811,-75,14,91811,57,96,90581,102,173,81026,4040,11276,88868,-82,16,87601,-75,58,86367,29,348,84382,4578,8912,83631,2399,3,52414,"FO2","GT" 22,34,1,4,9,131,5,"PUBLIC SERV ELEC & GAS CO","BURLINGTON",0,"NAT GAS",15477,"0M",1294,,,95,60222,642634,0,62039,580691,0,60695,548854,0,9404,108237,0,42361,363894,0,31693,299006,0,63357,605299,0,60174,537745,0,21155,187254,0,17575,158420,0,24156,217635,0,18363,172905,0,2399,3,52414,"NG","GT" 22,34,1,6,2,131,5,"PUBLIC SERV ELEC & GAS CO","BURLINGTON",0,"LIGHT OIL",15477,"0M",894,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,144,235,0,0,0,0,0,0,0,0,0,0,0,0,0,2399,3,52414,"FO2","CT" 22,34,1,4,2,131,7,"PUBLIC SERV ELEC & GAS CO","EDISON",0,"LIGHT OIL",15477,"0M",1294,,,95,152,366,106308,281,513,105795,252,403,105392,7,135,105257,0,0,105257,88,644,104610,675,1783,102827,687,1976,100851,0,0,110803,0,0,110803,126,444,110359,742,2206,108153,2400,3,52414,"FO2","GT" 22,34,1,4,9,131,7,"PUBLIC SERV ELEC & GAS CO","EDISON",0,"NAT GAS",15477,"0M",1294,,,95,-33,582,0,70,992,0,-80,345,0,0,0,0,-162,750,0,0,0,0,3046,44211,0,2441,36716,0,-100,537,0,120,3310,0,89,2079,0,28,428,0,2400,3,52414,"NG","GT" 22,34,1,4,2,131,8,"PUBLIC SERV ELEC & GAS CO","ESSEX",0,"LIGHT OIL",15477,"0M",1294,,,95,0,0,112211,4598,10660,104446,0,0,104446,0,0,103802,0,0,96326,4,10,91990,0,0,91990,0,0,91990,0,0,112914,2,185,112914,234,400,112327,894,2118,110210,2401,3,52414,"FO2","GT" 22,34,1,4,9,131,8,"PUBLIC SERV ELEC & GAS CO","ESSEX",0,"NAT GAS",15477,"0M",1294,,,95,20171,250330,0,38746,466002,0,28312,330527,0,6195,75506,0,7086,87770,0,17745,236062,0,65291,864255,0,62756,803138,0,18682,243317,0,3599,40505,0,3163,40505,0,1420,2118,0,2401,3,52414,"NG","GT" 22,34,1,2,2,131,13,"PUBLIC SERV ELEC & GAS CO","HUDSON",0,"LIGHT OIL",15477,"0M",1294,,,95,119,251,0,0,0,0,0,0,0,0,0,0,0,0,0,3,6,0,4,9,0,4,9,0,0,0,0,0,0,0,0,0,0,0,0,0,2403,3,52414,"FO2","ST" 22,34,1,2,3,131,13,"PUBLIC SERV ELEC & GAS CO","HUDSON",0,"HEAVY OIL",15477,"0M",1294,,,95,11188,21576,147242,40039,87268,59974,0,0,59974,158,379,13064,0,0,13064,0,0,13064,0,0,13064,0,0,0,0,0,0,0,0,0,0,0,0,-2401,3164,109182,2403,3,52414,"FO6","ST" 22,34,1,2,6,131,13,"PUBLIC SERV ELEC & GAS CO","HUDSON",0,"BIT COAL",15477,"0M",1294,,,95,0,0,239403,0,0,239403,46093,19713,219690,82549,35226,208484,158939,68702,225010,141427,62425,162585,235608,99546,193639,263396,110928,173063,10310,4383,258904,0,0,349753,57703,21908,369380,339660,132744,293504,2403,3,52414,"BIT","ST" 22,34,1,2,9,131,13,"PUBLIC SERV ELEC & GAS CO","HUDSON",0,"NAT GAS",15477,"0M",1294,,,95,30599,362930,0,7194,97478,0,122788,1378604,0,43966,500739,0,16188,203737,0,20750,232325,0,137870,1458255,0,96187,1102638,0,1254,45160,0,-3375,2793,0,356,3383,0,1493,16683,0,2403,3,52414,"NG","ST" 22,34,1,4,2,131,13,"PUBLIC SERV ELEC & GAS CO","HUDSON",0,"LIGHT OIL",15477,"0M",1294,,,95,119,251,352215,256,609,34606,-63,0,34606,-54,0,34597,-48,0,34597,0,0,34597,1239,2320,32262,396,2283,29962,-50,0,29962,-46,0,29962,-55,0,29962,-71,0,29959,2403,3,52414,"FO2","GT" 22,34,1,4,9,131,13,"PUBLIC SERV ELEC & GAS CO","HUDSON",0,"NAT GAS",15477,"0M",1294,,,95,0,0,0,7,103,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,3,38,0,0,0,0,0,0,0,0,0,0,0,0,0,2403,3,52414,"NG","GT" 22,34,1,2,2,131,16,"PUBLIC SERV ELEC & GAS CO","KEARNY",0,"LIGHT OIL",15477,"0M",1294,,,95,0,0,0,47,160,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2404,3,52414,"FO2","ST" 22,34,1,2,3,131,16,"PUBLIC SERV ELEC & GAS CO","KEARNY",0,"HEAVY OIL",15477,"0M",1294,,,95,-1419,0,47358,3162,9747,46218,-1264,0,46218,-811,0,43218,-763,0,46218,2322,7151,47602,25660,53229,45133,22324,46979,41775,-837,0,41775,-758,0,41755,-1135,0,41775,-1308,0,46698,2404,3,52414,"FO6","ST" 22,34,1,4,2,131,16,"PUBLIC SERV ELEC & GAS CO","KEARNY",0,"LIGHT OIL",15477,"0M",1294,,,95,375,941,65441,656,2205,61502,0,175,60444,-48,459,59831,-54,459,66419,-11,40,64109,2241,5425,58552,1592,6227,53502,-37,0,73227,-117,0,73054,-84,226,71810,-19,331,69761,2404,3,52414,"FO2","GT" 22,34,1,4,9,131,16,"PUBLIC SERV ELEC & GAS CO","KEARNY",0,"NAT GAS",15477,"0M",1294,,,95,778,10891,0,531,10070,0,-183,586,0,-132,928,0,-131,324,0,1324,24641,0,4064,67350,0,6293,99804,0,-119,0,0,-6,0,0,-8,139,0,-23,0,0,2404,3,52414,"NG","GT" 22,34,1,2,3,131,18,"PUBLIC SERV ELEC & GAS CO","LINDEN",0,"HEAVY OIL",15477,"0M",1294,,,95,-2975,0,169370,18699,47791,121579,1724,8149,41900,-1941,0,88431,-2550,0,88431,1771,15138,11078,59268,130643,95281,51534,115049,125814,-2711,0,128815,-1641,0,126134,-2551,10434,115700,-1747,0,115700,2406,3,52414,"FO6","ST" 22,34,1,4,2,131,18,"PUBLIC SERV ELEC & GAS CO","LINDEN",0,"LIGHT OIL",15477,"0M",1294,,,95,26,253,53370,313,1361,52009,448,1157,50882,3498,6627,44255,6478,14170,30085,0,0,30085,0,0,30085,564,1160,28925,0,0,49924,-37,195,49604,202,372,49037,451,1756,51571,2406,3,52414,"FO2","GT" 22,34,1,4,9,131,18,"PUBLIC SERV ELEC & GAS CO","LINDEN",0,"NAT GAS",15477,"0M",1294,,,95,-96,0,0,43,2616,0,3961,49847,0,1854,18696,0,15141,180135,0,13553,160573,0,33255,393680,0,32192,409006,0,8666,121819,0,8374,103539,0,3980,41596,0,1468,15561,0,2406,3,52414,"NG","GT" 22,34,1,2,6,131,22,"PUBLIC SERV ELEC & GAS CO","MERCER",0,"BIT COAL",15477,"0M",1294,,,95,260338,90961,263541,283481,98338,252219,105820,38401,312566,69927,25278,364038,58034,23857,399943,121372,47152,419711,144178,55677,392291,111773,44297,360087,169493,64917,301841,40666,17201,334307,135703,47712,346850,209008,71876,359245,2408,3,52414,"BIT","ST" 22,34,1,2,9,131,22,"PUBLIC SERV ELEC & GAS CO","MERCER",0,"NAT GAS",15477,"0M",1294,,,95,15072,160572,0,10698,100608,0,12860,134613,0,17393,171693,0,23606,242604,0,33578,373796,0,130882,1357300,0,110572,1186167,0,12727,142016,0,7184,77196,0,1387,12188,0,362,30224,0,2408,3,52414,"NG","ST" 22,34,1,4,2,131,22,"PUBLIC SERV ELEC & GAS CO","MERCER",0,"LIGHT OIL",15477,"0M",1294,,,95,58,452,0,99,166,0,-80,45,0,-80,22,0,-90,0,0,-84,0,0,174,1003,0,1250,2375,0,-74,0,0,-89,0,0,-86,0,0,65,504,0,2408,3,52414,"FO2","GT" 22,34,1,4,9,131,22,"PUBLIC SERV ELEC & GAS CO","MERCER",0,"NAT GAS",15477,"0M",1294,,,95,0,0,0,11,107,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,23,252,0,0,0,0,0,0,0,0,0,0,0,0,0,2408,3,52414,"NG","GT" 22,34,1,4,2,131,24,"PUBLIC SERV ELEC & GAS CO","NATIONAL PK",0,"LIGHT OIL",15477,"0M",1294,,,95,-7,0,2850,-5,0,2850,-6,0,168,-6,0,167,-7,0,1390,-6,0,3548,-6,0,3548,33,67,3481,-6,0,3481,3,25,3456,2,22,3434,-6,0,3434,2409,3,52414,"FO2","GT" 22,34,1,2,3,131,25,"PUBLIC SERV ELEC & GAS CO","SEWAREN",0,"HEAVY OIL",15477,"0M",1294,,,95,915,2021,98313,16425,33366,104241,341,778,103613,0,0,103613,1016,2372,101241,0,0,101241,128,279,100962,2211,4787,96175,4969,9343,86832,2764,7861,78971,2025,6536,72435,11423,30324,105394,2411,3,52414,"FO6","ST" 22,34,1,2,9,131,25,"PUBLIC SERV ELEC & GAS CO","SEWAREN",0,"NAT GAS",15477,"0M",1294,,,95,30968,435199,0,63113,771440,0,13222,183529,0,3478,58360,0,10032,124996,0,30077,426413,0,86401,1129748,0,69754,958979,0,7865,101861,0,-868,15021,0,1354,26896,0,943,15389,0,2411,3,52414,"NG","ST" 22,34,1,4,2,131,25,"PUBLIC SERV ELEC & GAS CO","SEWAREN",0,"LIGHT OIL",15477,"0M",1294,,,95,51,704,34543,121,263,34280,-71,0,34280,-133,0,34280,-130,0,34280,-22,30,38575,438,1523,37052,831,2943,34109,-123,0,34109,-124,0,34109,23,82,34027,80,208,33819,2411,3,52414,"FO2","GT" 22,34,1,4,9,131,25,"PUBLIC SERV ELEC & GAS CO","SEWAREN",0,"NAT GAS",15477,"0M",1294,,,95,0,0,0,2,31,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,16,0,0,0,0,2411,3,52414,"NG","GT" 22,34,1,4,2,131,27,"PUBLIC SERV ELEC & GAS CO","SALEM JO",0,"LIGHT OIL",15477,"0M",1294,,,95,-18,3,16640,85,264,16528,-5,49,16528,-14,28,17721,-15,0,17581,0,0,17581,398,125,32262,152,455,31807,-6,0,16295,2764,7861,78971,-14,0,14970,54,170,12261,2410,3,52414,"FO2","GT" 22,34,5,2,3,645,1,"VINELAND (CITY OF)","HOWARD DOWN",0,"HEAVY OIL",19856,"0M",1294,,,95,0,0,24261,803,2139,23900,486,1664,22238,294,1029,21209,2656,6649,16338,890,2102,21318,4629,11673,9645,3246,7549,10200,0,0,10347,0,0,10397,0,0,10320,2429,6628,6595,2434,3,53140,"FO6","ST" 22,34,5,2,6,645,1,"VINELAND (CITY OF)","HOWARD DOWN",0,"BIT COAL",19856,"0M",1294,,,95,7844,4284,7953,7472,4143,6788,3415,1988,9938,0,0,9849,2186,1111,8737,7260,3928,6843,6950,3861,9709,3584,3042,7673,388,209,9251,1581,798,8709,5259,2954,5755,3724,2035,5931,2434,3,53140,"BIT","ST" 22,34,5,4,2,645,10,"VINELAND (CITY OF)","WEST",0,"LIGHT OIL",19856,"0M",1294,,,95,74,199,9430,353,887,8543,45,128,8417,0,0,8417,0,0,8417,315,901,7389,2079,6227,5808,2543,5808,3568,151,900,3206,36,73,3061,6,80,2981,129,339,2818,6776,3,53140,"FO2","GT" 23,42,1,2,1,52,1,"DUQUESNE LGT CO","B VALLEY",0,"NUCLEAR",5487,"0M",1294,,,95,17240,0,0,-6300,0,0,367420,0,0,596300,0,0,615700,0,0,589500,0,0,604900,0,0,561482,0,0,591490,0,0,614130,0,0,582150,0,0,452460,0,0,6040,1,50827,"UR","ST" 23,42,1,2,1,52,2,"DUQUESNE LGT CO","B VALLEY",0,"NUCLEAR",5487,"0M",1294,,,95,610052,0,0,558397,0,0,377306,0,0,-2502,0,0,358108,0,0,592883,0,0,609130,0,0,296500,0,0,598381,0,0,622939,0,0,557126,0,0,601216,0,0,6040,1,50827,"UR","ST" 23,42,1,2,6,52,5,"DUQUESNE LGT CO","CHESWICK",0,"BIT COAL",5487,"0M",1294,,,95,355392,137291,317861,331090,126419,307477,249582,96410,291500,17430,8507,318494,299247,119774,288017,339756,132948,261655,256633,102182,276100,296500,118467,263069,297357,118900,201464,311698,126308,186349,351416,139379,173501,306740,121467,188856,8226,1,50827,"BIT","ST" 23,42,1,2,9,52,5,"DUQUESNE LGT CO","CHESWICK",0,"NAT GAS",5487,"0M",1294,,,95,1427,13928,0,331,3531,0,1002,9220,0,1172,14418,0,1806,18532,0,1364,13508,0,1549,14158,0,2639,26716,0,2701,26104,0,1881,19412,0,1411,14459,0,1232,12044,0,8226,1,50827,"NG","ST" 23,42,1,2,2,52,13,"DUQUESNE LGT CO","ELRAMA",0,"LIGHT OIL",5487,"0M",1294,,,95,1941,3768,1508,1330,2779,1204,1589,3262,979,1253,2681,1633,1006,2112,1445,803,1634,1382,1389,3062,1487,1368,2719,1591,1136,2443,1644,986,1991,1570,898,1981,1539,1195,2526,782,3098,1,50827,"FO2","ST" 23,42,1,2,6,52,13,"DUQUESNE LGT CO","ELRAMA",0,"BIT COAL",5487,"0M",1294,,,95,240736,111790,172599,220356,101044,171860,197080,90684,191628,207597,94541,190808,200161,89633,171686,159939,73949,169611,197010,95313,150545,226664,107371,139013,188236,90982,151708,97661,45101,189092,223530,101521,181601,237771,106889,154459,3098,1,50827,"BIT","ST" 23,42,1,2,2,52,15,"DUQUESNE LGT CO","F PHILLIPS",0,"LIGHT OIL",5487,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,3099,1,50827,"FO2","ST" 23,42,1,2,6,52,15,"DUQUESNE LGT CO","F PHILLIPS",0,"BIT COAL",5487,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,3099,1,50827,"BIT","ST" 23,42,1,4,2,52,27,"DUQUESNE LGT CO","BRUNOT ILND",0,"LIGHT OIL",5487,"0M",1294,,,95,-733,567,24237,-801,692,23545,-848,9,23536,-662,220,23316,-662,0,23316,-579,460,22856,1005,4706,18150,5198,15710,17539,-587,0,19993,-604,0,19993,-808,0,19993,-777,582,20583,3096,1,50827,"FO2","GT" 23,42,1,5,2,52,27,"DUQUESNE LGT CO","BRUNOT ILND",0,"LIGHT OIL",5487,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,3096,1,50827,"FO2","CC" 23,42,1,6,2,52,27,"DUQUESNE LGT CO","BRUNOT ILND",0,"LIGHT OIL",5487,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,3096,1,50827,"FO2","CT" 23,42,1,2,1,100,1,"GPU NUCLEAR CORP","3 MI ISLAND",0,"NUCLEAR",7423,"0M",1294,,,95,611412,0,0,552321,0,0,609022,0,0,586279,0,0,599986,0,0,573186,0,0,584601,0,0,586748,0,0,144888,0,0,338797,0,0,590553,0,0,610193,0,0,8011,3,58850,"UR","ST" 23,42,1,1,,114,15,"METROPOLITAN EDISON CO","YORK HAVEN",0,,12390,"0M",1294,,,95,8890,0,0,9724,0,0,12867,0,0,10005,0,0,12383,0,0,12781,0,0,10950,0,0,1654,0,0,3141,0,0,8336,0,0,12409,0,0,9435,0,0,3117,3,54020,"WAT","HY" 23,42,1,4,2,114,24,"METROPOLITAN EDISON CO","HAMILTON",0,"LIGHT OIL",12390,"0M",1294,,,95,0,44,4643,342,858,4499,38,102,4397,28,68,4330,-2,0,4330,0,0,4330,432,1398,2932,1179,2884,2369,143,356,3085,0,0,3085,47,129,3491,190,511,4606,3109,3,54020,"FO2","GT" 23,42,1,4,2,114,25,"METROPOLITAN EDISON CO","HUNTERSTOWN",0,"LIGHT OIL",12390,"0M",1294,,,95,44,117,8244,904,2365,9808,139,361,9448,53,150,8583,0,1,8583,0,0,8582,1,3,8579,16,42,8895,2,7,9067,19,50,9017,7,22,8995,281,706,8304,3110,3,54020,"FO2","GT" 23,42,1,4,9,114,25,"METROPOLITAN EDISON CO","HUNTERSTOWN",0,"NAT GAS",12390,"0M",1294,,,95,1133,17680,0,1048,17830,0,7,180,0,729,13320,0,504,8500,0,1339,19320,0,3546,41940,0,6556,84500,0,3434,53290,0,1503,23470,0,1262,20430,0,1780,27282,0,3110,3,54020,"NG","GT" 23,42,1,4,2,114,27,"METROPOLITAN EDISON CO","MOUNTAIN",0,"LIGHT OIL",12390,"0M",1294,,,95,71,188,6429,964,2523,5157,48,126,5031,4,12,5912,0,0,5912,0,1,5911,0,2,5910,0,0,5910,36,175,5913,0,0,6270,0,2,6804,367,1234,6575,3111,3,54020,"FO2","GT" 23,42,1,4,9,114,27,"METROPOLITAN EDISON CO","MOUNTAIN",0,"NATURAL G",12390,"0M",1294,,,95,297,5940,0,476,8360,0,443,6390,0,469,7770,0,208,3710,0,328,5630,0,1743,26610,0,3541,53620,0,894,14500,0,170,2840,0,572,8810,0,1301,18260,0,3111,3,54020,"NG","GT" 23,42,1,4,2,114,31,"METROPOLITAN EDISON CO","ORRTANNA",0,"LIGHT OIL",12390,"0M",1294,,,95,48,116,4401,346,875,4418,88,218,4200,26,66,4135,0,0,4135,0,0,4135,593,1575,2917,1316,3402,1824,159,409,2667,26,65,3674,0,7,5453,229,581,4898,3112,3,54020,"FO2","GT" 23,42,1,2,2,114,32,"METROPOLITAN EDISON CO","PORTLAND",0,"LIGHT OIL",12390,"0M",1294,,,95,1210,2219,56721,612,1085,51313,671,1307,49944,1587,3013,45429,432,812,42830,190,349,41500,955,1701,39591,434,783,37499,499,951,35882,161,335,60358,2066,4127,57233,222,397,56872,3113,3,54020,"FO2","ST" 23,42,1,2,6,114,32,"METROPOLITAN EDISON CO","PORTLAND",0,"BIT COAL",12390,"0M",1294,,,95,132808,53399,109521,182821,71489,66961,66747,28478,108572,54477,22914,130642,57698,23989,150827,144768,58703,134821,179344,71804,85267,178789,70856,51093,83228,35019,46481,11852,5425,93489,58689,25583,120272,183470,71507,85462,3113,3,54020,"BIT","ST" 23,42,1,4,2,114,32,"METROPOLITAN EDISON CO","PORTLAND",0,"LIGHT OIL",12390,"0M",1294,,,95,77,142,2671,1704,3020,3973,50,98,3938,790,1501,3938,951,1787,3938,662,1215,3705,281,501,3412,727,1310,3410,2125,4049,3409,1,3,3407,122,245,3406,1839,3288,3291,3113,3,54020,"FO2","GT" 23,42,1,4,9,114,32,"METROPOLITAN EDISON CO","PORTLAND",0,"NAT GAS",12390,"0M",1294,,,95,7,72,0,1596,15661,0,2973,32178,0,2051,22130,0,3978,42351,0,12035,125176,0,33248,336088,0,28922,295790,0,5224,56353,0,750,8818,0,2029,22553,0,597,5955,0,3113,3,54020,"NG","GT" 23,42,1,4,2,114,34,"METROPOLITAN EDISON CO","SHAWNEE",0,"LIGHT OIL",12390,"0M",1294,,,95,73,171,6099,265,687,6483,16,27,6472,20,60,6412,44,112,6301,35,90,6211,135,371,5839,869,2245,3594,68,177,3417,0,0,4845,68,117,5622,0,0,5679,3114,3,54020,"FO2","GT" 23,42,1,2,2,114,35,"METROPOLITAN EDISON CO","TITUS",0,"LIGHT OIL",12390,"0M",1294,,,95,102,198,885,73,138,926,387,772,869,487,933,1186,472,874,1205,168,334,1228,294,559,1026,220,409,617,291,530,803,369,699,998,321,614,560,227,431,880,3115,3,54020,"FO2","ST" 23,42,1,2,6,114,35,"METROPOLITAN EDISON CO","TITUS",0,"BIT COAL",12390,"0M",1294,,,95,73788,31030,99475,51570,21149,100003,47245,20126,101173,38103,15904,107895,66063,26455,103387,95872,40846,84743,118659,48529,57453,118052,46687,37871,105060,41177,26170,83805,34936,50826,103029,42373,57757,128752,52966,41217,3115,3,54020,"BIT","ST" 23,42,1,4,2,114,35,"METROPOLITAN EDISON CO","TITUS",0,"LIGHT OIL",12390,"0M",1294,,,95,58,114,4000,793,1492,4117,0,0,4117,1,2,4115,0,0,4115,4,8,4106,65,124,3983,133,248,3983,0,0,3983,131,248,3734,20,39,3695,0,0,3755,3115,3,54020,"FO2","GT" 23,42,1,4,9,114,35,"METROPOLITAN EDISON CO","TITUS",0,"NAT GAS",12390,"0M",1294,,,95,53,575,0,23,240,0,80,890,0,60,640,0,52,541,0,22,250,0,1587,16770,0,2936,30250,0,319,3230,0,110,1190,0,149,1590,0,5,60,0,3115,3,54020,"NG","GT" 23,42,1,4,2,114,38,"METROPOLITAN EDISON CO","TOLNA",0,"LIGHT OIL",12390,"0M",1294,,,95,68,175,6400,563,1516,6278,90,224,6054,0,1,6053,0,0,6053,0,0,6053,759,2033,4020,2323,6134,2677,164,447,5438,64,349,6339,62,101,6238,114,281,6229,3116,3,54020,"FO2","GT" 23,42,1,2,2,133,1,"PENNSYLVANIA ELEC CO","CONMAUGH JO",0,"LIGHT OIL",14711,"0M",1294,,250,95,514,827,5361,559,930,4122,454,736,6813,810,1319,5181,459,747,4344,78,121,4153,878,1456,2385,538,892,3017,74,121,5479,0,0,5356,3148,5217,7748,383,627,6559,3118,3,54025,"FO2","ST" 23,42,1,2,6,133,1,"PENNSYLVANIA ELEC CO","CONMAUGH JO",0,"BIT COAL",14711,"0M",1294,,250,95,1122156,419851,722958,925303,359096,640938,1076935,406220,574117,992331,375372,600365,1073542,404411,660222,1082614,409954,586984,1087889,419782,543363,1144736,439047,524854,727433,274855,587632,579871,221827,735222,799742,308937,733868,1107177,421853,608881,3118,3,54025,"BIT","ST" 23,42,1,2,9,133,1,"PENNSYLVANIA ELEC CO","CONMAUGH JO",0,"NAT GAS",14711,"0M",1294,,250,95,1516,13798,0,1026,9654,0,566,5184,0,1707,15719,0,1710,15719,0,264,2319,0,2347,22035,0,3446,32313,0,452,4120,0,258,2408,0,2434,22766,0,571,5283,0,3118,3,54025,"NG","ST" 23,42,1,3,2,133,1,"PENNSYLVANIA ELEC CO","CONMAUGH JO",0,"LIGHT OIL",14711,"0M",1294,,250,95,59,96,0,34,57,0,59,97,0,181,295,0,54,89,0,45,71,0,187,311,0,146,243,0,46,75,0,31,52,0,78,130,0,46,76,0,3118,3,54025,"FO2","IC" 23,42,1,1,,133,5,"PENNSYLVANIA ELEC CO","PINEY",0,,14711,"0M",1294,,250,95,7087,0,0,2980,0,0,8315,0,0,7025,0,0,7405,0,0,7866,0,0,1807,0,0,900,0,0,618,0,0,1506,0,0,5259,0,0,4760,0,0,3124,3,54025,"WAT","HY" 23,42,1,1,,133,13,"PENNSYLVANIA ELEC CO","SENECA JO",0,"C-PUMPSTG",14711,"0M",1294,,250,95,-18038,60718,0,-12762,44459,0,-13759,53339,0,-14476,46086,0,-10189,43886,0,-20535,71955,0,-32632,124316,0,-31819,130160,0,-23462,98242,0,-26851,110227,0,-17180,96885,0,-19235,101307,0,8225,3,54025,"WAT","HY" 23,42,1,4,9,133,17,"PENNSYLVANIA ELEC CO","BLOSSBURG",0,"NAT GAS",14711,"0M",1294,,250,95,-5,0,0,248,3769,0,-4,0,0,0,0,0,0,0,0,0,0,0,502,7485,0,846,9556,0,243,7354,0,-5,0,0,-4,0,0,-4,0,0,3120,3,54025,"NG","GT" 23,42,1,2,2,133,25,"PENNSYLVANIA ELEC CO","HOMER CTYJO",0,"LIGHT OIL",14711,"0M",1294,,250,95,724,1106,10724,239,368,10825,1397,2089,8613,678,1026,8717,2469,3709,5517,3227,5084,7324,1158,1765,5736,474,737,6933,1569,3909,7274,769,1187,8528,7523,12170,9104,4070,6343,6965,3122,3,54025,"FO2","ST" 23,42,1,2,6,133,25,"PENNSYLVANIA ELEC CO","HOMER CTYJO",0,"BIT COAL",14711,"0M",1294,,250,95,1185616,454082,568142,1188794,455176,479305,1210546,457862,391125,1087359,409749,340123,685495,258590,520058,1050104,414471,562956,1147586,445483,356766,1213094,474606,228657,448257,271599,331273,758425,290978,460056,823682,334855,431770,991225,388795,409243,3122,3,54025,"BIT","ST" 23,42,1,2,2,133,45,"PENNSYLVANIA ELEC CO","SEWARD",0,"LIGHT OIL",14711,"0M",1294,,250,95,662,1281,675,306,595,618,281,535,616,145,261,535,122,305,409,432,940,535,285,552,414,274,531,585,416,789,657,463,878,671,432,834,724,340,657,600,3130,3,54025,"FO2","ST" 23,42,1,2,6,133,45,"PENNSYLVANIA ELEC CO","SEWARD",0,"BIT COAL",14711,"0M",1294,,250,95,101596,46820,104963,110101,50567,86392,110470,50520,76721,54307,23628,78208,29270,17347,91227,52721,27510,83682,115539,53769,77789,119322,55517,67991,102723,46904,73094,107866,49063,74467,105367,48397,85472,116951,53923,61526,3130,3,54025,"BIT","ST" 23,42,1,2,2,133,48,"PENNSYLVANIA ELEC CO","SHAWVILLE",0,"LIGHT OIL",14711,"0M",1294,,250,95,1123,1920,8833,2602,4605,6882,3250,5700,8490,1312,2317,8459,872,1542,9545,917,1633,7965,912,1584,7411,1122,2141,8065,1665,3195,7890,1607,2973,8086,2444,4275,8035,3504,6399,6379,3131,3,54025,"FO2","ST" 23,42,1,2,6,133,48,"PENNSYLVANIA ELEC CO","SHAWVILLE",0,"BIT COAL",14711,"0M",1294,,250,95,269348,109338,102763,256827,107901,105884,326710,136132,96046,350160,145852,80632,328883,137262,84982,336010,141689,79617,350851,144610,79435,304942,138068,76369,248206,112475,83476,317261,138069,65107,346273,142913,61290,323453,141293,48123,3131,3,54025,"BIT","ST" 23,42,1,3,2,133,48,"PENNSYLVANIA ELEC CO","SHAWVILLE",0,"LIGHT OIL",14711,"0M",1294,,250,95,31,54,764,42,75,689,26,47,797,22,39,757,20,37,721,29,52,669,42,74,740,203,388,705,22,43,662,24,46,763,18,32,731,24,44,819,3131,3,54025,"FO2","IC" 23,42,1,2,2,133,60,"PENNSYLVANIA ELEC CO","WARREN",0,"LIGHT OIL",14711,"0M",1294,,250,95,101,246,375,38,94,281,58,147,313,65,158,336,29,123,391,38,93,297,45,104,725,30,76,657,8,20,637,47,126,511,41,109,402,38,97,482,3132,3,54025,"FO2","ST" 23,42,1,2,6,133,60,"PENNSYLVANIA ELEC CO","WARREN",0,"BIT COAL",14711,"0M",1294,,250,95,23223,13460,34201,30943,18008,26672,17000,10379,34033,20947,11998,35372,16865,16419,30837,28698,16502,23133,35556,19496,14235,32084,18799,17943,18322,10742,21117,17556,10786,25392,16779,10295,31120,32207,19202,23049,3132,3,54025,"BIT","ST" 23,42,1,4,2,133,60,"PENNSYLVANIA ELEC CO","WARREN",0,"LIGHT OIL",14711,"0M",1294,,250,95,2,7,9205,924,2260,9835,124,314,9521,0,1,9519,94,389,9130,154,374,8757,2078,4788,7154,3447,8693,6033,514,1272,7934,0,0,7934,105,276,7658,393,986,9466,3132,3,54025,"FO2","GT" 23,42,1,4,9,133,60,"PENNSYLVANIA ELEC CO","WARREN",0,"NAT GAS",14711,"0M",1294,,250,95,0,10,0,0,10,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,3132,3,54025,"NG","GT" 23,42,1,3,2,133,75,"PENNSYLVANIA ELEC CO","BENTON",0,"LIGHT OIL",14711,"0M",1294,"R",250,95,-3,0,0,-2,0,0,-3,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,3119,3,54025,"FO2","IC" 23,42,1,4,2,133,87,"PENNSYLVANIA ELEC CO","WAYNE",0,"LIGHT OIL",14711,"0M",1294,,250,95,-99,18,20263,508,1505,18758,-92,0,18758,-86,0,18758,-70,1,18757,-54,0,18757,1349,3469,15288,3798,9355,11397,490,1027,13199,-52,0,13199,141,1098,14037,154,691,18031,3134,3,54025,"FO2","GT" 23,42,1,2,2,133,90,"PENNSYLVANIA ELEC CO","KEYSTONE JO",0,"LIGHT OIL",14711,"0M",1294,,250,95,2244,3690,6503,1272,2084,8137,0,0,8969,4533,7554,9207,714,1204,9434,965,1623,9346,2145,3684,9013,3083,5243,9005,923,1553,9324,753,1254,8496,1264,2066,8810,0,0,8724,3136,3,54025,"FO2","ST" 23,42,1,2,6,133,90,"PENNSYLVANIA ELEC CO","KEYSTONE JO",0,"BIT COAL",14711,"0M",1294,,250,95,1102214,423987,311858,582793,225211,453587,563417,222247,605342,809149,315890,648804,1078337,426399,648546,1084349,429852,601163,1034268,420581,454702,938657,378854,582342,1033031,410618,649687,1088547,426659,795799,1058746,408591,711979,1180880,456067,560683,3136,3,54025,"BIT","ST" 23,42,1,3,2,133,90,"PENNSYLVANIA ELEC CO","KEYSTONE JO",0,"LIGHT OIL",14711,"0M",1294,,250,95,349,575,0,349,573,0,34,59,0,204,341,0,100,170,0,35,60,0,207,356,0,870,1480,0,155,262,0,66,110,0,178,291,0,46,86,0,3136,3,54025,"FO2","IC" 23,42,1,2,2,135,1,"PENNSYLVANIA POWER CO","NEW CASTLE",0,"LIGHT OIL",14716,"0M",1294,,,95,157,295,104,61,118,158,276,532,107,184,352,158,327,657,138,250,493,138,176,344,140,152,297,106,171,327,131,192,372,116,117,218,145,156,288,161,3138,1,52289,"FO2","ST" 23,42,1,2,6,135,1,"PENNSYLVANIA POWER CO","NEW CASTLE",0,"BIT COAL",14716,"0M",1294,,,95,167856,72057,99647,154279,67443,98213,130534,58811,77871,125682,55847,86191,67772,31976,90113,98557,45757,95531,118202,53998,90022,140629,64008,74786,116270,52148,73949,88872,40250,91385,140709,61724,82726,150687,61716,63171,3138,1,52289,"BIT","ST" 23,42,1,3,2,135,1,"PENNSYLVANIA POWER CO","NEW CASTLE",0,"LIGHT OIL",14716,"0M",1294,,,95,22,56,1012,6,7,1012,7,22,863,1,3,991,4,9,875,1,7,1095,68,120,980,348,650,769,21,48,895,12,25,914,9,4,978,1,5,846,3138,1,52289,"FO2","IC" 23,42,1,2,2,135,12,"PENNSYLVANIA POWER CO","MANSFLD JO",0,"LIGHT OIL",14716,"0M",1294,,,95,1007,1692,29171,723,1155,27861,1506,2563,20232,2103,3540,37005,3377,5991,30895,1363,2382,49447,1396,2364,47084,1578,2757,44327,1128,2011,40209,852,1442,3868,625,1076,37528,5978,10675,26852,6094,1,52289,"FO2","ST" 23,42,1,2,6,135,12,"PENNSYLVANIA POWER CO","MANSFLD JO",0,"BIT COAL",14716,"0M",1294,,,95,1000025,404047,691181,900788,348267,715644,764097,314521,842427,1018498,413184,894368,1102944,466816,876286,1268001,530524,794307,1358940,556273,756092,1346419,567300,719388,816664,349651,802659,889136,365870,922037,897824,373667,888666,766127,330985,1035343,6094,1,52289,"BIT","ST" 23,42,1,2,1,137,1,"PENNSYLVANIA PWR & LGT CO","SUSQUEHANNA",0,"NUCLEAR",14715,"0M",1294,,,95,784581,0,0,707744,0,0,597267,0,0,-6623,0,0,455272,0,0,764570,0,0,800626,0,0,807866,0,0,781516,0,0,816456,0,0,256044,0,0,663200,0,0,6103,3,52288,"UR","ST" 23,42,1,2,1,137,2,"PENNSYLVANIA PWR & LGT CO","SUSQUEHANNA",0,"NUCLEAR",14715,"0M",1294,,,95,819260,0,0,744537,0,0,809836,0,0,572523,0,0,800757,0,0,763767,0,0,784244,0,0,790491,0,0,327567,0,0,158303,0,0,801099,0,0,820399,0,0,6103,3,52288,"UR","ST" 23,42,1,1,,137,8,"PENNSYLVANIA PWR & LGT CO","HOLTWOOD",0,,14715,"0M",1294,,,95,63368,0,0,44815,0,0,66767,0,0,61784,0,0,47914,0,0,44060,0,0,38745,0,0,15029,0,0,8892,0,0,3395,0,0,54454,0,0,52183,0,0,3145,3,52288,"WAT","HY" 23,42,1,2,2,137,8,"PENNSYLVANIA PWR & LGT CO","HOLTWOOD",0,"LIGHT OIL",14715,"0M",1294,,,95,2,293,307,92,564,453,76,299,502,6,12,486,9,103,375,64,316,412,48,185,402,32,69,513,156,340,542,105,324,374,44,96,457,71,158,639,3145,3,52288,"FO2","ST" 23,42,1,2,4,137,8,"PENNSYLVANIA PWR & LGT CO","HOLTWOOD",0,"ANTH COAL",14715,"0M",1294,,,95,16657,10967,92177,28295,20094,81874,38352,28374,83310,37995,26901,93553,28887,20504,97262,21957,15483,110941,27038,19535,107719,38254,26848,105902,36692,25935,106839,27783,20333,110563,38411,27438,93901,40473,29360,79473,3145,3,52288,"ANT","ST" 23,42,1,2,5,137,8,"PENNSYLVANIA PWR & LGT CO","HOLTWOOD",0,"COKE",14715,"0M",1294,,,95,5600,3687,7954,10386,7347,6463,12376,9136,6569,13390,9479,6750,10455,7419,8863,7778,5469,5689,9256,6676,3115,13170,9235,2168,11989,8438,3400,7495,5464,2289,8623,7102,1550,11704,5956,0,3145,3,52288,"PC","ST" 23,42,1,1,,137,14,"PENNSYLVANIA PWR & LGT CO","WALLENPAUPK",0,,14715,"0M",1294,,,95,12278,0,0,38773,0,0,4171,0,0,-24207,0,0,735,0,0,560,0,0,5204,0,0,2717,0,0,244,0,0,24,0,0,11908,0,0,11545,0,0,3153,3,52288,"WAT","HY" 23,42,1,4,2,137,15,"PENNSYLVANIA PWR & LGT CO","ALLENTOWN",0,"LIGHT OIL",14715,"0M",1294,,,95,64,195,4597,200,523,4444,0,0,4446,40,90,4355,0,0,4356,122,333,4024,199,561,4006,2797,7611,4017,44,168,4389,12,34,4355,0,0,4351,134,369,4531,3139,3,52288,"FO2","GT" 23,42,1,2,2,137,20,"PENNSYLVANIA PWR & LGT CO","BRUNNER ISL",0,"LIGHT OIL",14715,"0M",1294,,,95,5215,9667,5220,2811,6985,2945,2623,7457,4341,1006,3274,4688,1673,5855,4747,623,3511,4635,1145,3027,3800,192,491,4638,1850,4455,1752,956,1998,4421,1497,3195,3955,6348,15226,4765,3140,3,52288,"FO2","ST" 23,42,1,2,6,137,20,"PENNSYLVANIA PWR & LGT CO","BRUNNER ISL",0,"BIT COAL",14715,"0M",1294,,,95,726861,278333,624176,797416,299207,615563,638681,243796,659948,618218,235042,726562,483331,182515,843219,636052,246917,774595,729927,280541,565746,770922,293672,454478,661164,258193,418744,632910,240757,448356,500569,201629,451028,542332,211139,476821,3140,3,52288,"BIT","ST" 23,42,1,3,2,137,20,"PENNSYLVANIA PWR & LGT CO","BRUNNER ISL",0,"LIGHT OIL",14715,"0M",1294,,,95,43,75,0,27,35,0,29,50,0,11,33,0,29,50,0,27,47,0,38,66,0,41,123,0,30,52,0,27,47,0,21,37,0,28,47,0,3140,3,52288,"FO2","IC" 23,42,1,4,2,137,26,"PENNSYLVANIA PWR & LGT CO","FISHBACH",0,"LIGHT OIL",14715,"0M",1294,,,95,0,0,2203,37,115,2088,0,0,2076,11,33,2043,0,0,2039,16,52,1987,102,265,2080,1274,3289,1978,63,218,2105,0,0,2095,0,0,2105,13,33,2071,3142,3,52288,"FO2","GT" 23,42,1,4,2,137,28,"PENNSYLVANIA PWR & LGT CO","HARWOOD",0,"LIGHT OIL",14715,"0M",1294,,,95,0,0,2216,83,240,2157,0,0,2152,44,152,2171,0,0,2171,13,61,2272,289,883,2098,1064,3093,1958,134,415,2230,60,205,2217,0,0,2217,0,0,2208,3144,3,52288,"FO2","GT" 23,42,1,4,2,137,29,"PENNSYLVANIA PWR & LGT CO","HARRISBURG",0,"LIGHT OIL",14715,"0M",1294,,,95,0,0,4184,328,916,4530,0,0,4528,34,103,4425,7,31,4394,111,326,4426,221,659,4486,3286,9229,3610,329,960,4424,0,0,4424,8,0,4410,101,283,4486,3143,3,52288,"FO2","GT" 23,42,1,2,2,137,32,"PENNSYLVANIA PWR & LGT CO","MARTINS CRK",0,"LIGHT OIL",14715,"0M",1294,,,95,1397,3966,1367,1654,3961,905,487,1818,1153,845,3118,1197,886,4111,1282,1222,4052,1400,1679,4825,803,2026,5349,775,303,753,1408,633,2680,1365,1511,3919,1485,2510,5735,1078,3148,3,52288,"FO2","ST" 23,42,1,2,3,137,32,"PENNSYLVANIA PWR & LGT CO","MARTINS CRK",0,"HEAVY OIL",14715,"0M",1294,,,95,3313,20105,1792976,137098,246817,1537637,4594,16136,1518993,7837,26024,1486208,0,0,1482804,46574,94076,1387076,225007,410380,970823,241933,469387,1094662,32635,57250,1132457,11373,23775,1505839,59422,125764,1590347,265457,506756,1125474,3148,3,52288,"FO6","ST" 23,42,1,2,6,137,32,"PENNSYLVANIA PWR & LGT CO","MARTINS CRK",0,"BIT COAL",14715,"0M",1294,,,95,77736,33553,94127,107453,45145,78631,33245,15373,94972,56476,25532,79013,56350,25210,63411,56558,24356,57931,77903,34985,45157,72539,34251,53601,19134,10553,62015,28384,12765,56271,68305,31511,46146,107135,53235,34362,3148,3,52288,"BIT","ST" 23,42,1,3,2,137,32,"PENNSYLVANIA PWR & LGT CO","MARTINS CRK",0,"LIGHT OIL",14715,"0M",1294,,,95,19,33,0,53,92,0,70,124,0,63,90,0,15,57,0,18,30,0,7,12,0,39,74,0,10,20,0,7,13,0,4,7,0,20,9,0,3148,3,52288,"FO2","IC" 23,42,1,4,2,137,32,"PENNSYLVANIA PWR & LGT CO","MARTINS CRK",0,"LIGHT OIL",14715,"0M",1294,,,95,0,0,5154,253,713,4491,0,0,4487,23,66,4408,0,0,4408,97,271,4056,301,924,3141,2928,8451,3433,332,1023,4044,0,0,4797,34,92,6619,47,134,6156,3148,3,52288,"FO2","GT" 23,42,1,4,2,137,34,"PENNSYLVANIA PWR & LGT CO","JENKINS",0,"LIGHT OIL",14715,"0M",1294,,,95,0,0,2287,49,143,2325,0,0,2326,12,59,2267,0,0,2265,0,0,2261,285,831,1773,1377,3617,2093,62,169,2280,17,50,2230,0,0,2177,0,0,2170,3146,3,52288,"FO2","GT" 23,42,1,4,2,137,36,"PENNSYLVANIA PWR & LGT CO","LOCK HAVEN",0,"LIGHT OIL",14715,"0M",1294,,,95,2,17,2072,0,0,2072,0,0,2071,0,0,2072,0,0,2231,19,50,2181,47,187,2160,309,776,1940,29,62,2234,0,0,2233,0,0,2229,0,0,2223,3147,3,52288,"FO2","GT" 23,42,1,2,2,137,38,"PENNSYLVANIA PWR & LGT CO","MONTOUR",0,"LIGHT OIL",14715,"0M",1294,,,95,5284,3061,15269,1120,9829,7128,603,1538,7267,606,3951,8198,13,2000,6913,5227,30521,8337,1368,7253,4923,878,2071,5843,1573,7626,7055,7633,17598,7723,1969,8730,7062,7059,10859,7500,3149,3,52288,"FO2","ST" 23,42,1,2,6,137,38,"PENNSYLVANIA PWR & LGT CO","MONTOUR",0,"BIT COAL",14715,"0M",1294,,,95,847074,335924,519372,875346,340631,445625,780698,304571,380887,372505,141113,452083,435583,162563,503087,625764,248102,531404,836431,328954,481373,911902,352540,306054,690630,264412,407406,817637,314073,299288,838531,328858,291789,880367,352324,220532,3149,3,52288,"BIT","ST" 23,42,1,2,2,137,40,"PENNSYLVANIA PWR & LGT CO","SUNBURY",0,"LIGHT OIL",14715,"0M",1294,,,95,120,1018,953,89,415,868,270,1417,1025,212,1169,913,362,1349,784,121,240,1084,94,305,938,95,427,967,167,1398,1038,316,896,961,315,1038,893,516,1056,864,3152,3,52288,"FO2","ST" 23,42,1,2,4,137,40,"PENNSYLVANIA PWR & LGT CO","SUNBURY",0,"ANTH COAL",14715,"0M",1294,,,95,59791,48178,418732,52800,43904,407593,42379,34783,387855,56229,44534,380823,54876,44151,401119,43071,35250,457310,34960,27900,513983,38518,30044,586494,54062,41683,635399,58158,44699,652259,58144,45249,613424,56311,42856,591156,3152,3,52288,"ANT","ST" 23,42,1,2,5,137,40,"PENNSYLVANIA PWR & LGT CO","SUNBURY",0,"COKE",14715,"0M",1294,,,95,32080,14266,18014,37875,17579,8930,34489,14591,2989,39190,17032,15602,35966,15206,24516,28052,11818,24368,21736,9175,21882,27009,11174,25559,37827,15339,20820,35544,14870,22116,40820,17176,11347,43815,18422,22426,3152,3,52288,"PC","ST" 23,42,1,2,6,137,40,"PENNSYLVANIA PWR & LGT CO","SUNBURY",0,"BIT COAL",14715,"0M",1294,,,95,38602,20937,145827,50229,27422,136935,127350,62833,126363,110076,53702,131074,110470,54187,128876,117078,56381,126273,137002,67568,99984,129986,64144,93470,121920,58717,95585,117436,55949,93435,118781,56941,78649,145641,68789,57848,3152,3,52288,"BIT","ST" 23,42,1,3,2,137,40,"PENNSYLVANIA PWR & LGT CO","SUNBURY",0,"LIGHT OIL",14715,"0M",1294,,,95,29,54,0,17,32,0,22,41,0,12,22,0,18,33,0,15,28,0,10,19,0,41,76,0,14,26,0,21,39,0,16,30,0,15,28,0,3152,3,52288,"FO2","IC" 23,42,1,4,2,137,40,"PENNSYLVANIA PWR & LGT CO","SUNBURY",0,"LIGHT OIL",14715,"0M",1294,,,95,0,0,4196,0,0,4357,0,0,4367,0,0,4367,0,0,4367,12,34,4284,56,161,4122,1269,3772,3896,136,375,4425,0,0,4425,0,0,4304,59,188,4116,3152,3,52288,"FO2","GT" 23,42,1,4,2,137,41,"PENNSYLVANIA PWR & LGT CO","WEST SHORE",0,"LIGHT OIL",14715,"0M",1294,,,95,0,0,1981,146,397,2124,0,0,2125,23,63,2063,0,0,2063,27,85,2157,93,275,2060,1581,3944,1664,97,247,1948,0,0,1948,0,0,1943,0,0,1936,3154,3,52288,"FO2","GT" 23,42,1,4,2,137,42,"PENNSYLVANIA PWR & LGT CO","WILLIAMPORT",0,"LIGHT OIL",14715,"0M",1294,,,95,11,25,2095,108,303,2299,33,89,2120,24,80,2130,0,0,1062,31,83,2085,166,469,2282,1685,4637,1796,229,615,2348,0,1,2347,0,0,2347,47,129,2218,3155,3,52288,"FO2","GT" 23,42,1,2,4,137,44,"PENNSYLVANIA PWR & LGT CO","COAL STORAG",0,"ANTH COAL",14715,"0M",1294,,,95,0,0,4326102,0,0,4287048,0,0,4250306,0,0,4192077,0,0,4116068,0,0,4024607,0,0,3949307,0,0,3858966,0,0,3770991,0,0,3712178,0,0,3655315,0,0,3627389,8805,3,52288,"ANT","ST" 23,42,1,2,1,144,1,"PECO ENERGY CO","LIMERICK",0,"NUCLEAR",14940,"0M",1294,,260,95,758738,0,0,649503,0,0,788638,0,0,741991,0,0,644273,0,0,749037,0,0,735331,0,0,472319,0,0,293869,0,0,781359,0,0,758883,0,0,774008,0,0,6105,3,52304,"UR","ST" 23,42,1,2,1,144,2,"PECO ENERGY CO","LIMERICK",0,"NUCLEAR",14940,"0M",1294,,260,95,305997,0,0,145495,0,0,841460,0,0,792169,0,0,828631,0,0,759339,0,0,812705,0,0,648469,0,0,793584,0,0,839715,0,0,794719,0,0,838665,0,0,6105,3,52304,"UR","ST" 23,42,1,2,1,144,2,"PECO ENERGY CO","PEACHBOTTOM",0,"NUCLEAR",14940,"0M",1294,,260,95,835865,0,0,758077,0,0,833805,0,0,783656,0,0,813085,0,0,767048,0,0,814131,0,0,781700,0,0,787889,0,0,812587,0,0,755502,0,0,620649,0,0,3166,3,52304,"UR","ST" 23,42,1,1,,144,3,"PECO ENERGY CO","MUDDY RUN",0,"P-PUMPSTG",14940,"0M",1294,,260,95,-58588,197635,0,-48050,161907,0,-57936,201052,0,-62063,184331,0,-54454,193555,0,-64502,219733,0,-77254,238571,0,-71435,248510,0,-71632,228867,0,-151911,225998,0,-140643,200522,0,-140747,207063,0,3164,3,52304,"WAT","HY" 23,42,1,2,1,144,3,"PECO ENERGY CO","PEACHBOTTOM",0,"NUCLEAR",14940,"0M",1294,,260,95,777483,0,0,711496,0,0,640321,0,0,740258,0,0,699846,0,0,588449,0,0,497410,0,0,423621,0,0,284823,0,0,314451,0,0,800042,0,0,695148,0,0,3166,3,52304,"UR","ST" 23,42,1,4,2,144,10,"PECO ENERGY CO","CHESTER",0,"LIGHT OIL",14940,"0M",1294,,260,95,40,143,6303,283,871,5973,4,13,5960,0,0,5960,0,0,5960,134,251,5709,1965,3097,5088,2547,9094,4622,135,622,5417,6,46,5371,9,117,5615,0,0,5615,3157,3,52304,"FO2","GT" 23,42,1,2,2,144,18,"PECO ENERGY CO","CROMBY",0,"LIGHT OIL",14940,"0M",1294,,260,95,552,1065,739,136,247,742,559,972,675,596,1108,639,800,1555,694,542,1023,717,107,204,786,442,846,656,532,1027,700,390,751,648,1349,2625,514,669,1263,679,3159,3,52304,"FO2","ST" 23,42,1,2,3,144,18,"PECO ENERGY CO","CROMBY",0,"HEAVY OIL",14940,"0M",1294,,260,95,2359,4204,37192,40300,66566,38230,6132,9753,28477,2439,4170,38531,1755,3147,35384,2326,3992,31392,2427,4219,27173,2684,4698,32767,5362,9562,23250,2962,5168,40075,2887,5164,35070,3164,5422,36172,3159,3,52304,"FO6","ST" 23,42,1,2,6,144,18,"PECO ENERGY CO","CROMBY",0,"BIT COAL",14940,"0M",1294,,260,95,74489,31603,37801,84553,33984,30569,59404,28393,32942,68130,28446,39783,56042,24391,55616,62095,25757,51736,68743,28828,37015,81385,34554,29542,73288,31653,35675,82081,34906,31898,75734,32689,34891,88164,36436,31030,3159,3,52304,"BIT","ST" 23,42,1,2,9,144,18,"PECO ENERGY CO","CROMBY",0,"NAT GAS",14940,"0M",1294,,260,95,71643,785884,0,61834,634083,0,79727,785913,0,51172,541950,0,54177,597370,0,81502,865110,0,111181,1192120,0,110008,1192120,0,68568,752990,0,0,0,0,0,0,0,69,740,0,3159,3,52304,"NG","ST" 23,42,1,3,2,144,18,"PECO ENERGY CO","CROMBY",0,"LIGHT OIL",14940,"0M",1294,,260,95,0,0,425,2,5,382,1,2,380,1,3,377,0,0,377,0,1,376,6,13,363,0,0,363,2,5,358,0,0,358,3,6,352,0,0,352,3159,3,52304,"FO2","IC" 23,42,1,2,2,144,20,"PECO ENERGY CO","DELAWARE",0,"LIGHT OIL",14940,"0M",1294,,260,95,83,167,285,230,443,159,379,1037,262,0,1258,270,63,112,285,407,948,313,503,939,296,248,512,251,125,311,303,0,535,306,0,1886,292,1548,3097,274,3160,3,52304,"FO2","ST" 23,42,1,2,3,144,20,"PECO ENERGY CO","DELAWARE",0,"HEAVY OIL",14940,"0M",1294,,260,95,7566,13842,54536,40968,72617,57755,6149,15501,61363,-988,853,60510,1023,1674,58836,10372,22370,60784,73226,125872,59240,61586,116298,48551,3817,8670,64382,-880,0,64382,-848,109,64273,42071,77005,46160,3160,3,52304,"FO6","ST" 23,42,1,3,2,144,20,"PECO ENERGY CO","DELAWARE",0,"LIGHT OIL",14940,"0M",1294,,260,95,4,8,0,6,12,0,0,0,0,8,4,0,0,0,0,0,0,0,0,0,0,5,12,0,0,0,0,0,0,0,3,6,0,0,0,0,3160,3,52304,"FO2","IC" 23,42,1,4,2,144,20,"PECO ENERGY CO","DELAWARE",0,"LIGHT OIL",14940,"0M",1294,,260,95,14,29,4606,471,908,4510,16,46,5120,42,103,4834,0,0,5221,137,321,4998,1693,3157,5919,4022,8277,4823,175,434,5097,11,64,4495,0,0,4139,3,6,3960,3160,3,52304,"FO2","GT" 23,42,1,2,2,144,23,"PECO ENERGY CO","EDDYSTONE",0,"LIGHT OIL",14940,"0M",1294,,260,95,2860,5785,8309,7265,14150,6730,691,1392,5338,656,1353,6842,1090,2439,5446,1497,2992,3502,265,545,7647,1122,2234,5367,200,403,4943,1397,2645,5855,940,1740,11279,4634,8834,12016,3161,3,52304,"FO2","ST" 23,42,1,2,3,144,23,"PECO ENERGY CO","EDDYSTONE",0,"HEAVY OIL",14940,"0M",1294,,260,95,28189,52308,219884,149450,269038,232369,3289,6168,226201,212,405,225796,779,1602,224194,12605,22920,225716,34139,63954,190796,58828,107390,228949,6004,24353,228406,13370,23208,205198,25814,43623,161575,159697,281810,186014,3161,3,52304,"FO6","ST" 23,42,1,2,6,144,23,"PECO ENERGY CO","EDDYSTONE",0,"BIT COAL",14940,"0M",1294,,260,95,230611,102377,114701,145600,63304,115351,142036,63132,95986,141196,64796,114142,75987,37394,136129,72749,31969,156190,38241,17251,161746,115645,50809,196139,101095,70609,237844,255413,106924,214128,279475,114586,204428,343647,144382,154263,3161,3,52304,"BIT","ST" 23,42,1,2,9,144,23,"PECO ENERGY CO","EDDYSTONE",0,"NAT GAS",14940,"0M",1294,,260,95,44577,509816,0,75572,836629,0,64058,732536,0,42770,502085,0,37425,473140,0,199205,2238826,0,248894,2876189,0,290649,3273871,0,116178,2028607,0,136486,1466691,0,26917,282787,0,17773,193338,0,3161,3,52304,"NG","ST" 23,42,1,4,2,144,23,"PECO ENERGY CO","EDDYSTONE",0,"LIGHT OIL",14940,"0M",1294,,260,95,88,179,7824,301,588,7236,23,47,7189,0,0,7189,59,133,7056,38,77,6979,2082,4276,7703,5802,11553,9393,213,2838,8159,40,77,8082,74,138,7944,162,310,8951,3161,3,52304,"FO2","GT" 23,42,1,2,3,144,25,"PECO ENERGY CO","OIL STORAGE",0,"HEAVY OIL",14940,"0M",1294,,260,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,8806,3,52304,"FO6","ST" 23,42,1,4,2,144,26,"PECO ENERGY CO","FALLS",0,"LIGHT OIL",14940,"0M",1294,,260,95,6,16,10772,174,460,10312,0,0,10312,0,0,10312,0,0,10312,323,626,9686,1716,2316,9307,2167,6952,8374,53,261,8289,8,112,8177,0,0,8503,0,0,8503,3162,3,52304,"FO2","GT" 23,42,1,4,2,144,27,"PECO ENERGY CO","MOSER",0,"LIGHT OIL",14940,"0M",1294,,260,95,62,154,10920,416,1304,10329,2,7,10322,0,0,10322,0,0,10322,174,159,10163,2401,3681,8582,3033,9617,8076,165,385,7691,0,0,7691,49,1948,8854,0,0,8854,3163,3,52304,"FO2","GT" 23,42,1,4,2,144,30,"PECO ENERGY CO","RICHMOND",0,"LIGHT OIL",14940,"0M",1294,,260,95,73,705,25225,1538,2518,24154,176,209,23945,0,0,23945,0,0,23945,546,1092,22853,7883,15050,19654,8358,22812,19604,1489,4282,16208,573,1391,19605,1780,4530,22192,2646,5558,20232,3168,3,52304,"FO2","GT" 23,42,1,2,2,144,35,"PECO ENERGY CO","SCHUYLKILL",0,"LIGHT OIL",14940,"0M",1294,,260,95,10,31,177,29,55,282,0,13,330,0,0,58,5,32,173,21,41,260,32,63,204,31,64,224,0,0,285,0,0,204,0,13,117,174,366,292,3169,3,52304,"FO2","ST" 23,42,1,2,3,144,35,"PECO ENERGY CO","SCHUYLKILL",0,"HEAVY OIL",14940,"0M",1294,,260,95,2569,7049,0,27433,47982,0,-514,221,0,-442,0,0,787,4441,0,7540,12988,0,45149,79435,0,40737,74952,0,2171,4408,0,-450,0,0,-487,0,0,33696,64594,0,3169,3,52304,"FO6","ST" 23,42,1,3,2,144,35,"PECO ENERGY CO","SCHUYLKILL",0,"LIGHT OIL",14940,"0M",1294,,260,95,0,0,0,11,21,0,1,6,0,0,0,0,0,0,0,0,0,0,0,0,0,4,9,0,2,8,0,0,0,0,0,0,0,0,0,0,3169,3,52304,"FO2","IC" 23,42,1,4,2,144,35,"PECO ENERGY CO","SCHUYLKILL",0,"LIGHT OIL",14940,"0M",1294,,260,95,0,0,4077,183,347,4272,0,0,4454,0,0,4454,16,102,4352,25,48,4304,1060,2033,4025,3086,6214,3655,57,113,3542,0,0,3542,0,0,4435,0,0,4435,3169,3,52304,"FO2","GT" 23,42,1,4,2,144,39,"PECO ENERGY CO","SOUTHWARK",0,"LIGHT OIL",14940,"0M",1294,,260,95,7,10,6164,245,786,6101,28,123,5978,0,0,5978,0,0,5978,21,33,5945,2299,3702,5765,2572,9427,4876,120,646,4593,9,18,4592,0,0,5461,12,32,5429,3170,3,52304,"FO2","GT" 23,42,1,4,2,144,62,"PECO ENERGY CO","CROYDON",0,"LIGHT OIL",14940,"0M",1294,,260,95,908,1378,96105,5368,13129,82976,1206,2774,80202,185,1674,78528,-30,449,78079,2904,7166,70913,28748,58359,102954,34047,90855,75978,5816,17011,58967,4006,14190,124677,9344,33758,90919,20108,59103,81811,8012,3,52304,"FO2","GT" 23,42,1,1,,166,1,"SAFE HARBOR WATERPOWER CO","SAFE HARBOR",0,,16537,"0M",1294,,,95,143384,0,0,59393,0,0,126476,0,0,89759,0,0,63828,0,0,55553,0,0,43077,0,0,14256,0,0,7655,0,0,60191,0,0,112079,0,0,82918,0,0,3175,3,52553,"WAT","HY" 23,42,1,2,2,182,5,"UNITED GAS IMP CO (THE)","HUNLOCK CRK",0,"LIGHT OIL",19390,"0M",1294,,,95,513,820,149,94,161,167,202,328,185,435,618,244,11,18,226,1,2,224,140,230,170,0,0,170,514,892,135,73,127,175,21,35,140,24,41,99,3176,3,52988,"FO2","ST" 23,42,1,2,4,182,5,"UNITED GAS IMP CO (THE)","HUNLOCK CRK",0,"ANTH COAL",19390,"0M",1294,,,95,22922,15408,12384,27213,18489,14764,29884,19399,26578,8930,5383,44202,31976,21379,41110,31087,20919,40663,28632,19193,37106,32217,21657,39145,28079,19274,38194,32138,21308,38517,32139,20464,33331,30924,20327,26649,3176,3,52988,"ANT","ST" 23,42,1,2,2,187,1,"WEST PENN POWER CO","ARMSTRONG",0,"LIGHT OIL",20387,"0M",1294,,71,95,1137,2044,435,250,438,461,208,349,465,208,340,516,357,602,494,249,434,577,87,154,405,77,134,448,175,297,469,719,1212,478,755,1324,33,100,171,531,3178,1,54030,"FO2","ST" 23,42,1,2,6,187,1,"WEST PENN POWER CO","ARMSTRONG",0,"BIT COAL",20387,"0M",1294,,71,95,116602,48997,133134,169087,69152,118235,94695,37329,143043,106738,41224,154005,90547,35992,160453,93589,37605,145126,109058,44341,133889,108429,43934,141795,50453,20094,155423,132983,52637,143306,163282,66595,118118,227115,90923,97838,3178,1,54030,"BIT","ST" 23,42,1,2,2,187,5,"WEST PENN POWER CO","HATFIELD",0,"LIGHT OIL",20387,"0M",1294,,71,95,431,715,4466,429,677,4860,16,26,4860,109,176,5175,295,498,4642,232,393,4202,112,193,4003,116,200,3858,440,729,3846,625,1001,3653,200,324,4266,345,551,4530,3179,1,54030,"FO2","ST" 23,42,1,2,6,187,5,"WEST PENN POWER CO","HATFIELD",0,"BIT COAL",20387,"0M",1294,,71,95,924993,349235,573422,796344,286253,580468,654622,239981,562743,652050,240234,569141,751057,287421,561772,807472,310567,503117,873489,338429,425399,814220,315517,429242,611272,228129,438816,665375,244419,472140,717809,264457,471668,976850,352523,470255,3179,1,54030,"BIT","ST" 23,42,1,2,2,187,15,"WEST PENN POWER CO","MITCHELL",0,"LIGHT OIL",20387,"0M",1294,,71,95,1099,1660,62781,14264,26130,36652,9573,16358,20294,0,0,95,0,0,20294,0,0,20294,2975,5533,14761,9534,17307,37248,0,0,37248,370,623,36693,0,0,102,0,0,36712,3181,1,54030,"FO2","ST" 23,42,1,2,6,187,15,"WEST PENN POWER CO","MITCHELL",0,"BIT COAL",20387,"0M",1294,,71,95,133543,54702,81824,96423,41467,82859,153555,62524,77796,125039,49503,90740,49588,20363,93045,53622,23986,82955,92131,39751,72392,131370,55646,87997,44218,20045,99480,112797,45127,97501,86006,35430,95483,91125,37261,96203,3181,1,54030,"BIT","ST" 23,42,1,2,9,187,15,"WEST PENN POWER CO","MITCHELL",0,"NAT GAS",20387,"0M",1294,,71,95,997,8782,0,512,5468,0,649,6574,0,362,3518,0,98,1012,0,493,5639,0,384,4175,0,352,3732,0,608,6884,0,229,2287,0,632,6538,0,411,4215,0,3181,1,54030,"NG","ST" 23,42,1,2,3,187,25,"WEST PENN POWER CO","SPRINGDALE",0,"HEAVY OIL",20387,"0M",1294,"S",71,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,3182,1,54030,"FO6","ST" 23,42,8,1,,800,5,"ALLEGHENY ELECTRIC COOP","RAYSTOWN",0,,332,"0A",1294,,,95,10581,0,0,4872,0,0,10420,0,0,7145,0,0,9214,0,0,7292,0,0,7823,0,0,1871,0,0,1862,0,0,6232,0,0,13092,0,0,11263,0,0,7128,1,58500,"WAT","HY" 31,39,1,2,2,30,5,"CARDINAL OPERATING CO","CARDINAL",0,"LIGHT OIL",3006,"0M",1294,,365,95,1506,2512,16004,1987,3269,21891,793,1326,20561,810,1358,18998,750,1207,17783,5623,9537,7493,587,994,18460,1462,2531,15746,996,1682,14054,1293,2176,11850,586,984,10858,3751,6207,17605,2828,1,50359,"FO2","ST" 31,39,1,2,6,30,5,"CARDINAL OPERATING CO","CARDINAL",0,"BIT COAL",3006,"0M",1294,,365,95,964403,385031,651565,952635,371878,631820,970861,386058,589923,907026,357640,591393,523077,201759,670651,745173,300966,631446,1013299,410501,467099,1010121,415926,370224,984185,397240,345127,996339,400914,397108,987234,392815,487317,940659,377797,434608,2828,1,50359,"BIT","ST" 31,39,1,4,2,43,1,"CINCINNATI GAS ELEC CO","DICKS CREEK",0,"LIGHT OIL",3542,"0M",1294,,210,95,20,1175,6144,23,332,5811,9,35,5776,18,399,5377,0,0,5377,10,47,5330,233,987,4343,377,1342,3001,3,41,5373,8,49,5325,18,65,5260,1,7,5253,2831,1,50556,"FO2","GT" 31,39,1,4,9,43,1,"CINCINNATI GAS ELEC CO","DICKS CREEK",0,"NAT GAS",3542,"0M",1294,,210,95,74,4943,0,-217,0,0,17,13,0,-138,563,0,-109,0,0,227,871,0,3843,78877,0,4803,89226,0,-34,0,0,-101,1423,0,240,6693,0,672,17724,0,2831,1,50556,"NG","GT" 31,39,1,2,2,43,2,"CINCINNATI GAS ELEC CO","WC BECKJORD",0,"LIGHT OIL",3542,"0M",1294,,210,95,1063,1868,0,520,909,0,1246,2193,0,616,1040,0,909,1575,0,1694,2920,0,83,148,0,648,1175,0,673,1200,0,1185,2032,0,1335,2313,0,1124,2076,0,2830,1,50556,"FO2","ST" 31,39,1,2,6,43,2,"CINCINNATI GAS ELEC CO","WC BECKJORD",0,"BIT COAL",3542,"0M",1294,,210,95,376000,158991,137317,393834,167236,139827,297378,127194,171002,437582,181317,177440,274678,116442,192793,481664,200911,197721,528583,228082,195580,602321,260506,195850,213081,91113,206835,487454,202145,200676,427365,176777,196004,493746,218176,193234,2830,1,50556,"BIT","ST" 31,39,1,4,2,43,2,"CINCINNATI GAS ELEC CO","WC BECKJORD",0,"LIGHT OIL",3542,"0M",1294,,210,95,904,1589,30711,253,443,29179,30,54,26769,24,41,25499,30,53,23746,206,356,41971,10845,19305,22349,18056,32731,31385,523,933,29084,23,40,26796,38,67,23956,1551,2863,41821,2830,1,50556,"FO2","GT" 31,39,1,2,2,43,5,"CINCINNATI GAS ELEC CO","MIAMI FORT",0,"LIGHT OIL",3542,"0M",1294,,210,95,1008,1795,0,465,820,0,830,1457,0,436,757,0,862,1538,0,1665,3001,0,1804,3164,0,3368,6051,0,1292,2324,0,260,450,0,548,956,0,3202,5528,0,2832,1,50556,"FO2","ST" 31,39,1,2,6,43,5,"CINCINNATI GAS ELEC CO","MIAMI FORT",0,"BIT COAL",3542,"0M",1294,,210,95,637745,262491,294369,502865,207419,302760,559242,231277,318869,305741,124954,357678,414341,174583,369622,502174,211728,359534,599203,248510,325680,672906,285623,264937,557339,235511,249465,607306,250021,246891,553335,226505,248836,594845,241403,260437,2832,1,50556,"BIT","ST" 31,39,1,4,2,43,5,"CINCINNATI GAS ELEC CO","MIAMI FORT",0,"LIGHT OIL",3542,"0M",1294,,210,95,184,328,29994,104,184,28839,51,90,27190,104,182,26060,90,161,23971,260,470,20424,2604,4567,34307,5930,10654,29284,0,0,26912,56,98,26221,132,231,25022,4,7,19483,2832,1,50556,"FO2","GT" 31,39,1,2,2,43,10,"CINCINNATI GAS ELEC CO","W H ZIMMER",0,"LIGHT OIL",3542,"0M",1294,,210,95,387,627,43117,405,662,42455,266,437,42018,446,721,41297,544,908,40390,5437,9067,40610,3869,6259,34351,2406,3947,30404,654,1074,29331,0,0,28641,10375,17945,31644,228,326,31318,6019,1,50556,"FO2","ST" 31,39,1,2,6,43,10,"CINCINNATI GAS ELEC CO","W H ZIMMER",0,"BIT COAL",3542,"0M",1294,,210,95,945287,364436,470303,860575,334587,468422,931671,360276,429932,905494,345488,449089,895923,353208,433131,685071,269191,462164,813824,313887,471999,817013,315668,465279,858265,326707,439814,-6015,0,440306,643755,258809,446427,954218,369625,445092,6019,1,50556,"BIT","ST" 31,39,1,4,2,43,15,"CINCINNATI GAS ELEC CO","WOODSDALE",0,"PROPANE",3542,"0M",1294,,210,95,3264,17257,47281,251,6836,40445,206,1875,39359,655,3378,35981,0,2040,33941,765,1976,31965,599,1450,30515,128,307,30208,2,8,30200,22,122,30078,2291,8079,47000,9027,29590,47410,7158,1,50556,"FO2","GT" 31,39,1,4,9,43,15,"CINCINNATI GAS ELEC CO","WOODSDALE",0,"NAT GAS",3542,"0M",1294,,210,95,150,4500,0,6,900,0,329,16900,0,549,16100,0,-24,5400,0,8444,123700,0,78223,1073891,0,127374,1732000,0,11241,209600,0,798,24900,0,8079,161217,0,5288,98400,0,7158,1,50556,"NG","GT" 31,39,1,2,1,47,1,"CLEVELAND ELEC ILLUM CO","PERRY",0,"NUCLEAR",3755,"0M",1294,,,95,876776,0,0,768903,0,0,819283,0,0,488364,0,0,856246,0,0,825532,0,0,844484,0,0,836109,0,0,563058,0,0,867378,0,0,562127,0,0,802040,0,0,6020,1,50587,"UR","ST" 31,39,1,2,2,47,5,"CLEVELAND ELEC ILLUM CO","ASHTABULA",0,"LIGHT OIL",3755,"0M",1294,,,95,42,104,847,0,0,847,118,290,165,18,45,836,36,88,1105,993,2435,781,1126,2764,920,735,1805,1069,508,1246,1250,554,1359,961,372,912,1126,318,78,1063,2835,1,50587,"FO2","ST" 31,39,1,2,6,47,5,"CLEVELAND ELEC ILLUM CO","ASHTABULA",0,"BIT COAL",3755,"0M",1294,,,95,52796,31491,71024,49964,29829,71024,55761,34212,70589,75864,42918,70589,57256,34078,70589,75393,41494,70589,152351,73482,69602,185535,87655,62911,92554,48842,63273,134786,62671,50375,152108,70363,39853,183631,84228,39391,2835,1,50587,"BIT","ST" 31,39,1,2,2,47,10,"CLEVELAND ELEC ILLUM CO","AVON",0,"LIGHT OIL",3755,"0M",1294,,,95,545,1336,12357,217,533,11823,334,820,11003,71,175,13126,623,1529,11274,103,252,10337,204,501,9328,209,514,12564,219,537,11551,455,1117,10529,439,1076,9330,211,518,8657,2836,1,50587,"FO2","ST" 31,39,1,2,6,47,10,"CLEVELAND ELEC ILLUM CO","AVON",0,"BIT COAL",3755,"0M",1294,,,95,418792,166008,147432,412531,162705,122460,424163,169344,131476,363532,138488,180398,251231,98651,203325,203947,82859,218224,353614,137703,162497,424161,173437,95914,388690,173071,75855,373672,144052,89758,227150,92153,101135,197850,84233,81208,2836,1,50587,"BIT","ST" 31,39,1,4,2,47,10,"CLEVELAND ELEC ILLUM CO","AVON",0,"LIGHT OIL",3755,"0M",1294,,,95,-48,0,1833,46,308,1525,-44,0,1525,16,93,1432,-27,0,1432,51,171,1260,97,283,1453,726,2175,826,-20,0,1302,-23,0,1326,-40,0,1326,-55,0,1861,2836,1,50587,"FO2","GT" 31,39,1,2,2,47,15,"CLEVELAND ELEC ILLUM CO","EASTLAKE",0,"LIGHT OIL",3755,"0M",1294,,,95,1497,3674,9572,911,2234,8964,764,1874,9624,751,1842,8674,1166,2861,7850,1418,3479,8310,853,2092,5787,966,2369,13472,911,2234,13178,758,1860,11437,682,1673,13358,1121,2750,10965,2837,1,50587,"FO2","ST" 31,39,1,2,6,47,15,"CLEVELAND ELEC ILLUM CO","EASTLAKE",0,"BIT COAL",3755,"0M",1294,,,95,563066,214828,125324,531721,201833,127529,552063,214200,127558,603752,229103,113946,476696,183152,148312,528305,201681,134280,545020,211638,133115,580108,227637,126504,418750,164875,155538,237147,95621,161064,619540,234785,116588,554005,216330,121544,2837,1,50587,"BIT","ST" 31,39,1,4,2,47,15,"CLEVELAND ELEC ILLUM CO","EASTLAKE",0,"LIGHT OIL",3755,"0M",1294,,,95,-26,411,1392,-34,64,1328,-7,96,1232,-39,0,1232,-17,48,1184,80,272,913,110,487,2330,416,1227,1642,-21,0,1642,-29,0,1642,-48,0,1642,-62,0,1642,2837,1,50587,"FO2","GT" 31,39,1,2,2,47,20,"CLEVELAND ELEC ILLUM CO","LAKE SHORE",0,"LIGHT OIL",3755,"0M",1294,,,95,1807,4433,0,1095,2687,0,655,1878,10867,822,2016,9030,822,2016,9030,822,2016,9030,822,2016,9030,0,0,9030,0,0,9030,0,0,9030,0,0,9030,0,0,9030,2838,1,50587,"FO2","ST" 31,39,1,2,3,47,20,"CLEVELAND ELEC ILLUM CO","LAKE SHORE",0,"HEAVY OIL",3755,"0M",1294,,,95,-1345,0,0,-1121,0,0,-1101,0,0,-967,0,0,-1013,0,0,-1144,0,0,-1177,0,0,-1109,0,0,-1101,0,0,-886,0,0,-1113,0,0,-1190,0,0,2838,1,50587,"FO6","ST" 31,39,1,2,6,47,20,"CLEVELAND ELEC ILLUM CO","LAKE SHORE",0,"BIT COAL",3755,"0M",1294,,,95,-2869,0,0,-2051,0,0,-8655,0,0,-1765,0,0,-1630,0,0,-1592,0,0,-1511,0,0,-680,0,0,-664,0,0,-785,0,0,-839,0,0,-939,0,0,2838,1,50587,"BIT","ST" 31,39,1,3,2,47,20,"CLEVELAND ELEC ILLUM CO","LAKE SHORE",0,"LIGHT OIL",3755,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2838,1,50587,"FO2","IC" 31,39,1,2,2,50,5,"COLUMBUS SOUTHERN PWR CO","CONESVILLE",0,"LIGHT OIL",4062,"0M",1294,,369,95,781,1346,11167,848,1487,10088,1527,2569,9973,647,1108,10480,1150,1863,10818,808,1412,11137,1992,3195,10638,911,1520,12206,2980,5206,7444,848,1360,7419,1411,2362,6092,1247,2194,6515,2840,1,50633,"FO2","ST" 31,39,1,2,6,50,5,"COLUMBUS SOUTHERN PWR CO","CONESVILLE",0,"BIT COAL",4062,"0M",1294,,369,95,839897,361439,480236,776708,341510,409270,577474,241703,450938,516809,220156,545479,471259,188870,589930,540735,233443,590510,666114,292069,537443,960463,414977,380548,748475,319718,311923,775359,307972,333993,824448,339869,356943,594247,257598,411899,2840,1,50633,"BIT","ST" 31,39,1,2,2,50,15,"COLUMBUS SOUTHERN PWR CO","PICWAY",0,"LIGHT OIL",4062,"0M",1294,,369,95,77,157,318,80,151,162,0,0,158,0,0,163,0,0,150,271,581,410,67,164,258,153,329,279,86,168,293,52,109,355,102,206,330,71,149,354,2843,1,50633,"FO2","ST" 31,39,1,2,6,50,15,"COLUMBUS SOUTHERN PWR CO","PICWAY",0,"BIT COAL",4062,"0M",1294,,369,95,24098,12576,18902,17338,8355,10547,0,0,10547,0,0,10547,0,0,10547,12062,7059,8508,8499,5099,16411,33626,17892,7051,12493,6357,14305,11264,6148,20174,12256,6425,23762,14575,8110,25135,2843,1,50633,"BIT","ST" 31,39,1,3,2,56,15,"DAYTON PWR & LGT CO (THE)","FRANK TAIT",0,"LIGHT OIL",4922,"0M",1294,,,95,10,18,2118,30,55,1880,24,44,4879,67,123,5809,5,9,5601,0,0,8437,59,128,8308,638,1170,6968,8,15,6953,0,0,6953,4,31,12908,0,0,12704,2847,1,50752,"FO2","IC" 31,39,1,4,2,56,15,"DAYTON PWR & LGT CO (THE)","FRANK TAIT",0,"LIGHT OIL",4922,"0M",494,,,95,0,0,0,0,0,0,0,0,0,8,31,0,2615,5585,0,2094,4660,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,87,204,0,2847,1,50752,"FO2","GT" 31,39,1,4,9,56,15,"DAYTON PWR & LGT CO (THE)","FRANK TAIT",0,"NAT GAS",4922,"0M",494,,,95,0,0,0,0,0,0,0,0,0,206,4610,0,2453,30366,0,2250,29020,0,2757,33743,0,5899,80360,0,392,7740,0,65,1370,0,35,1210,0,1279,17010,0,2847,1,50752,"NG","GT" 31,39,1,2,6,56,20,"DAYTON PWR & LGT CO (THE)","HUTCHINGS",0,"BIT COAL",4922,"0M",1294,,,95,1189,1204,103680,11354,5882,97799,-864,0,97799,0,0,97799,-467,0,97799,38657,18515,85185,73119,34885,59277,140943,65371,20520,7427,3975,45638,4351,2521,84275,3553,2065,93826,62576,27616,66210,2848,1,50752,"BIT","ST" 31,39,1,2,9,56,20,"DAYTON PWR & LGT CO (THE)","HUTCHINGS",0,"NAT GAS",4922,"0M",1294,,,95,408,9899,0,595,6448,0,0,0,0,-804,48,0,4,164,0,1487,14801,0,2254,22264,0,5404,59821,0,688,9010,0,440,6133,0,353,5099,0,1464,15898,0,2848,1,50752,"NG","ST" 31,39,1,4,2,56,20,"DAYTON PWR & LGT CO (THE)","HUTCHINGS",0,"LIGHT OIL",4922,"0M",1294,,,95,71,303,1433,82,157,1275,0,1,1275,0,0,1275,0,0,1274,0,0,1274,0,0,1274,0,1,1274,0,0,1274,0,0,1274,58,147,1127,49,94,1395,2848,1,50752,"FO2","GT" 31,39,1,4,9,56,20,"DAYTON PWR & LGT CO (THE)","HUTCHINGS",0,"NAT GAS",4922,"0M",1294,,,95,0,10,0,0,0,0,5,1130,0,16,400,0,8,327,0,0,0,0,140,1384,0,423,4690,0,0,0,0,0,0,0,0,0,0,41,453,0,2848,1,50752,"NG","GT" 31,39,1,2,2,56,23,"DAYTON PWR & LGT CO (THE)","J M STUART",0,"LIGHT OIL",4922,"0M",1294,,,95,1332,2321,1749,646,1073,2134,623,1061,2140,1223,2081,1858,1631,2823,2062,975,1647,2197,223,358,2194,623,1047,2043,1054,1794,2183,2669,4498,2177,1035,1708,1924,2772,4191,2252,2850,1,50752,"FO2","ST" 31,39,1,2,6,56,23,"DAYTON PWR & LGT CO (THE)","J M STUART",0,"BIT COAL",4922,"0M",1294,,,95,1324209,556655,951299,1313535,540148,931841,981133,406226,1101726,963505,397393,1210633,1235488,518718,880851,1223521,506083,868835,1340550,537277,869585,1339861,554937,815555,984147,409972,981044,990034,409244,867049,1361690,549068,888832,1361213,508529,976472,2850,1,50752,"BIT","ST" 31,39,1,3,2,56,23,"DAYTON PWR & LGT CO (THE)","J M STUART",0,"LIGHT OIL",4922,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2850,1,50752,"FO2","IC" 31,39,1,4,2,56,28,"DAYTON PWR & LGT CO (THE)","YANKEE ST",0,"LIGHT OIL",4922,"0M",1294,,,95,392,1042,6368,143,449,7390,1,3,5791,0,0,5791,0,1,5790,0,2,5788,0,0,5788,0,2,6395,2,7,6388,0,1,6388,60,192,6195,298,738,6316,2854,1,50752,"FO2","GT" 31,39,1,4,9,56,28,"DAYTON PWR & LGT CO (THE)","YANKEE ST",0,"NAT GAS",4922,"0M",1294,,,95,10,160,0,62,1100,0,162,1963,0,84,1410,0,82,1499,0,110,1913,0,390,6135,0,2583,45005,0,16,299,0,118,2067,0,15,279,0,1,15,0,2854,1,50752,"NG","GT" 31,39,1,3,2,56,34,"DAYTON PWR & LGT CO (THE)","MONUMENT",0,"LIGHT OIL",4922,"0M",1294,,,95,48,88,666,38,70,596,24,44,749,8,15,735,20,37,698,0,0,698,0,0,698,868,1591,510,12,22,679,8,15,664,3,6,658,23,73,586,2851,1,50752,"FO2","IC" 31,39,1,3,2,56,38,"DAYTON PWR & LGT CO (THE)","SIDNEY",0,"LIGHT OIL",4922,"0M",1294,,,95,36,66,654,39,72,582,19,35,547,12,22,525,27,50,476,38,70,594,200,367,418,928,1701,298,12,22,467,14,26,441,11,20,599,27,50,550,2852,1,50752,"FO2","IC" 31,39,1,2,2,56,40,"DAYTON PWR & LGT CO (THE)","KILLEN",0,"LIGHT OIL",4922,"0M",1294,,,95,1515,2654,38401,2032,3512,34941,568,957,33906,811,1364,32383,2303,3935,28369,2103,3623,24697,1150,1949,22638,3905,6750,39224,3140,5527,33621,140,241,33352,1226,2214,31022,7796,9042,43816,6031,1,50752,"FO2","ST" 31,39,1,2,6,56,40,"DAYTON PWR & LGT CO (THE)","KILLEN",0,"BIT COAL",4922,"0M",1294,,,95,396655,162048,146219,299969,123570,141430,380134,154283,172985,326056,132202,166969,335211,138111,191956,337194,139038,170239,357281,145509,178055,407089,168349,129255,293108,123208,110897,435673,179182,98466,52201,22774,186101,115941,32572,227624,6031,1,50752,"BIT","ST" 31,39,1,2,2,133,10,"OHIO EDISON CO","EDGEWATER",0,"LIGHT OIL",13998,"0M",1294,"A",,95,0,0,0,0,0,0,255,723,33,159,366,33,0,0,0,308,793,33,68,152,33,5,124,33,27,86,33,7,17,33,1286,2860,33,3,6,33,2857,1,52154,"FO2","ST" 31,39,1,2,9,133,10,"OHIO EDISON CO","EDGEWATER",0,"NAT GAS",13998,"0M",394,,,95,0,0,0,0,0,0,7097,98907,0,15050,194824,0,0,0,0,5911,86537,0,13656,173637,0,24053,289252,0,13182,151945,0,7495,97750,0,13698,169535,0,9290,104799,0,2857,1,52154,"NG","ST" 31,39,1,4,2,133,10,"OHIO EDISON CO","EDGEWATER",0,"LIGHT OIL",13998,"0M",1294,,,95,39,51,10875,58,329,9555,-8,73,8938,-14,44,9839,0,0,9464,200,693,10736,984,3224,10487,1718,5378,9687,120,437,8935,-17,0,8918,15,18,8748,20,140,9834,2857,1,52154,"FO2","GT" 31,39,1,2,2,133,15,"OHIO EDISON CO","GORGE STEAM",0,"LIGHT OIL",13998,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2858,1,52154,"FO2","ST" 31,39,1,2,6,133,15,"OHIO EDISON CO","GORGE STEAM",0,"BIT COAL",13998,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2858,1,52154,"BIT","ST" 31,39,1,4,2,133,30,"OHIO EDISON CO","MAD RIVER",0,"LIGHT OIL",13998,"0M",1294,,,95,-78,0,15547,-26,273,15273,-54,0,15273,-54,0,15273,363,2822,15479,99,426,15053,1080,3857,14177,3295,9983,13051,179,602,14577,62,386,15260,60,421,14839,73,357,15562,2860,1,52154,"FO2","GT" 31,39,1,2,2,133,43,"OHIO EDISON CO","NILES",0,"LIGHT OIL",13998,"0M",1294,,,95,5,9,253,86,166,190,142,266,280,33,64,216,17,38,406,275,522,253,67,130,224,50,97,303,45,88,221,63,123,320,28,54,266,27,53,213,2861,1,52154,"FO2","ST" 31,39,1,2,6,133,43,"OHIO EDISON CO","NILES",0,"BIT COAL",13998,"0M",1294,,,95,123871,55965,73387,98573,45856,68795,100911,45527,84171,102317,46469,88241,6938,3797,109930,76341,34497,104722,105408,49207,76769,73326,33732,70283,103996,47562,47231,111221,52359,33613,108872,49872,33134,113766,51273,29923,2861,1,52154,"BIT","ST" 31,39,1,4,2,133,43,"OHIO EDISON CO","NILES",0,"LIGHT OIL",13998,"0M",1294,,,95,55,295,7474,75,333,7682,-36,56,7626,-41,0,7626,-25,30,7596,100,416,7180,647,2274,6851,1403,4579,5630,65,256,6970,-7,118,6852,3,124,6728,61,335,7293,2861,1,52154,"FO2","GT" 31,39,1,2,2,133,45,"OHIO EDISON CO","R E BURGER",0,"LIGHT OIL",13998,"0M",1294,,,95,101,204,570,57,119,629,70,132,675,95,173,502,63,117,562,95,188,374,81,156,558,51,100,633,44,83,549,46,91,458,2,3,632,119,296,336,2864,1,52154,"FO2","ST" 31,39,1,2,6,133,45,"OHIO EDISON CO","R E BURGER",0,"BIT COAL",13998,"0M",1294,,,95,220103,104240,157034,164294,78521,184267,126512,54034,193327,150997,63973,186573,81596,35961,201217,96775,43949,193287,127163,56391,181386,166656,74197,142563,130934,57102,99030,67387,30839,87088,93946,40429,64542,82572,48775,54306,2864,1,52154,"BIT","ST" 31,39,1,3,2,133,45,"OHIO EDISON CO","R E BURGER",0,"LIGHT OIL",13998,"0M",1294,,,95,7,10,1284,23,46,1417,9,11,1407,0,0,1407,0,0,1407,34,84,1323,236,429,1243,566,1044,904,17,35,1224,23,43,1181,0,0,1181,30,77,1647,2864,1,52154,"FO2","IC" 31,39,1,2,2,133,57,"OHIO EDISON CO","W H SAMMIS",0,"LIGHT OIL",13998,"0M",1294,,,95,1482,2546,867,528,903,1046,558,954,844,550,932,638,695,1199,912,544,955,1493,706,1274,1304,451,1354,1217,1142,2017,1181,1316,2293,1036,94,160,983,2104,3601,973,2866,1,52154,"FO2","ST" 31,39,1,2,6,133,57,"OHIO EDISON CO","W H SAMMIS",0,"BIT COAL",13998,"0M",1294,,,95,1276095,514756,525945,1279324,511426,457910,1239563,502275,472374,1278563,515393,459047,1160892,479648,563045,1211972,504994,605054,1203599,510803,549162,1367687,590999,470321,991825,414819,354704,1017793,422778,445492,1052538,422578,399901,1094820,447068,288610,2866,1,52154,"BIT","ST" 31,39,1,3,2,133,57,"OHIO EDISON CO","W H SAMMIS",0,"LIGHT OIL",13998,"0M",1294,,,95,21,47,2208,62,132,2422,24,52,2506,21,51,2619,18,49,2690,84,169,2569,424,916,2504,994,1895,1445,56,115,2687,17,62,1885,61,120,2363,49,78,2264,2866,1,52154,"FO2","IC" 31,39,1,5,2,133,80,"OHIO EDISON CO","W LORAIN JO",0,"LIGHT OIL",13998,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2869,1,52154,"FO2","CC" 31,39,1,6,2,133,80,"OHIO EDISON CO","W LORAIN JO",0,"LIGHT OIL",13998,"0M",1294,"A",,95,0,0,0,0,0,0,18,114,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2869,1,52154,"FO2","CT" 31,39,1,2,2,141,28,"OHIO POWER CO","MUSKINGUM R",0,"LIGHT OIL",14006,"0M",1294,,364,95,3882,6525,18086,2171,3713,17991,1663,2732,19038,2100,3500,20732,2616,4271,21458,2357,4274,22882,1323,2298,23072,3025,5284,24028,1082,2039,25141,1349,2367,24554,1527,2671,21638,6433,9974,10617,2872,1,54028,"FO2","ST" 31,39,1,2,6,141,28,"OHIO POWER CO","MUSKINGUM R",0,"BIT COAL",14006,"0M",1294,,364,95,535201,215186,421884,537048,220375,419768,597967,235236,427281,521184,207858,375208,449068,175136,430680,464394,194776,458208,580017,239178,402984,570215,237224,362814,265479,117802,367772,240284,100504,368567,286463,120853,342833,504050,190482,323803,2872,1,54028,"BIT","ST" 31,39,1,2,2,141,30,"OHIO POWER CO","GAVIN",0,"LIGHT OIL",14006,"0M",1294,,364,95,3763,6775,47403,769,1320,46083,4239,7491,38592,399,722,37870,719,1203,36667,2089,3543,33123,1042,1767,31357,1100,2128,29229,787,1372,39659,1447,2509,37150,1827,3076,34074,190,326,33748,8102,1,54028,"FO2","ST" 31,39,1,2,6,141,30,"OHIO POWER CO","GAVIN",0,"BIT COAL",14006,"0M",1294,,364,95,64858,30038,1931820,651490,284413,2186971,988276,436625,1888556,1196488,552083,1872871,1419448,615414,1838157,1182854,513910,1760692,1417031,613808,1615051,1643009,713610,1363516,1514789,657244,1159863,1269184,559173,1152059,1395530,601427,1176037,1375641,605361,1157372,8102,1,54028,"BIT","ST" 31,39,1,1,,141,35,"OHIO POWER CO","RACINE",0,,14006,"0M",1294,,364,95,18331,0,0,19396,0,0,21002,0,0,26318,0,0,19638,0,0,23776,0,0,16330,0,0,12023,0,0,7551,0,0,14526,0,0,23751,0,0,24817,0,0,6006,1,54028,"WAT","HY" 31,39,1,2,6,141,40,"OHIO POWER CO","TIDD",0,"BIT COAL",14006,"0M",1294,"S",364,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2874,1,54028,"BIT","ST" 31,39,1,2,2,147,1,"OHIO VALLEY ELEC CORP","KYGER CREEK",0,"LIGHT OIL",14015,"0M",1294,,506,95,214,364,1335,346,582,1079,478,772,930,80,131,1631,298,520,1248,203,342,1489,97,168,1464,0,0,1642,55,92,1550,582,973,577,236,390,1258,83,146,1373,2876,1,52156,"FO2","ST" 31,39,1,2,6,147,1,"OHIO VALLEY ELEC CORP","KYGER CREEK",0,"BIT COAL",14015,"0M",1294,,506,95,702913,271965,605907,555922,215202,643003,623778,230327,685798,645615,237897,675827,712862,278407,639864,676683,252935,580389,702720,270228,524058,722985,274975,470824,637930,231881,406765,609383,225508,431319,645928,235364,421426,715380,277692,649924,2876,1,52156,"BIT","ST" 31,39,1,2,1,168,1,"TOLEDO EDISON CO (THE)","DAVIS-BESSE",0,"NUCLEAR",18997,"0M",1294,,,95,658580,0,0,596841,0,0,657111,0,0,620608,0,0,643953,0,0,629968,0,0,645923,0,0,643124,0,0,630210,0,0,652469,0,0,633467,0,0,645496,0,0,6149,1,52927,"UR","ST" 31,39,1,2,2,168,9,"TOLEDO EDISON CO (THE)","ACME",0,"PROPANE",18997,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2877,1,52927,"FO2","ST" 31,39,1,2,6,168,9,"TOLEDO EDISON CO (THE)","ACME",0,"BIT COAL",18997,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2877,1,52927,"BIT","ST" 31,39,1,2,9,168,9,"TOLEDO EDISON CO (THE)","ACME",0,"NAT GAS",18997,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2877,1,52927,"NG","ST" 31,39,1,2,2,168,11,"TOLEDO EDISON CO (THE)","BAY SHORE",0,"LIGHT OIL",18997,"0M",1294,,,95,136,448,525,273,439,445,156,255,550,380,622,464,160,607,393,170,407,521,159,530,700,226,457,598,155,367,588,238,402,364,76,315,588,112,197,572,2878,1,52927,"FO2","ST" 31,39,1,2,6,168,11,"TOLEDO EDISON CO (THE)","BAY SHORE",0,"BIT COAL",18997,"0M",1294,,,95,271495,103216,169716,328463,121979,150035,259418,97335,167411,220548,81660,204738,228937,86543,252579,283830,108691,226673,265296,101256,155041,323077,180415,73781,309205,109740,75119,176674,67648,106761,254611,97258,111939,278242,107020,82847,2878,1,52927,"BIT","ST" 31,39,1,4,2,168,11,"TOLEDO EDISON CO (THE)","BAY SHORE",0,"LIGHT OIL",18997,"0M",1294,,,95,14,64,566,36,59,688,0,0,782,14,24,758,0,0,758,17,30,1086,46,267,997,175,646,886,8,62,825,2,5,820,0,19,979,1,53,926,2878,1,52927,"FO2","GT" 31,39,1,4,2,168,18,"TOLEDO EDISON CO (THE)","RICHLAND",0,"LIGHT OIL",18997,"0M",1294,,,95,0,40,2793,0,0,2793,0,0,2793,0,25,2768,0,3,2764,27,124,2641,49,260,2380,192,729,1652,0,0,1652,0,44,1607,0,0,2325,0,0,2325,2880,1,52927,"FO2","GT" 31,39,1,4,9,168,18,"TOLEDO EDISON CO (THE)","RICHLAND",0,"NAT GAS",18997,"0M",1294,,,95,0,276,0,0,594,0,0,324,0,0,621,0,0,756,0,25,675,0,71,2079,0,345,7385,0,0,215,0,0,3046,0,0,92,0,2,392,0,2880,1,52927,"NG","GT" 31,39,1,4,2,168,19,"TOLEDO EDISON CO (THE)","STRYKER",0,"LIGHT OIL",18997,"0M",1294,,,95,10,159,1191,0,0,1191,0,0,1191,0,0,1191,0,0,1191,0,0,1191,0,0,1191,0,8,1183,0,0,1183,16,41,1142,0,0,92,0,29,1113,2881,1,52927,"FO2","GT" 31,39,5,3,2,522,1,"ARCANUM (CITY OF)","ARCANUM",0,"LIGHT OIL",768,"0A",1294,,,95,27,51,203,49,90,186,15,31,155,4,8,148,3,5,143,17,33,110,14,27,82,52,101,101,4,8,93,3,6,87,4,13,74,8,21,171,2902,1,50096,"FO2","IC" 31,39,5,3,2,552,1,"BRYAN (CITY OF)","BRYAN",0,"LIGHT OIL",2439,"0M",1294,,,95,14,23,355,14,25,329,0,0,329,178,304,378,39,68,310,12,21,289,145,250,215,87,158,235,29,50,179,16,27,153,37,63,268,9,32,237,2903,1,50356,"FO2","IC" 31,39,5,4,2,552,1,"BRYAN (CITY OF)","BRYAN",0,"LIGHT OIL",2439,"0M",1294,,,95,22,50,6950,0,0,6950,2,156,6795,0,0,6790,0,0,6790,0,0,6790,0,0,6790,0,0,6790,0,0,6760,0,0,6720,6,12,6690,1,5,6682,2903,1,50356,"FO2","GT" 31,39,5,4,9,552,1,"BRYAN (CITY OF)","BRYAN",0,"NAT GAS",2439,"0M",1294,,,95,22,566,0,82,2330,0,0,0,0,254,4926,0,3992,62915,0,6018,86797,0,4936,89292,0,8968,190437,0,6094,104355,0,104,2299,0,132,2762,0,420,8161,0,2903,1,50356,"NG","GT" 31,39,5,4,2,561,2,"CLEVELAND (CITY OF)","COLLINWOOD",0,"LIGHT OIL",3762,"0M",1294,,,95,0,1,1070,0,4,1066,83,263,803,0,0,803,4,238,565,0,0,922,0,0,922,50,256,1022,0,0,1022,0,0,1022,0,0,1022,0,0,1022,2906,1,50589,"FO2","GT" 31,39,5,4,9,561,2,"CLEVELAND (CITY OF)","COLLINWOOD",0,"NAT GAS",3762,"0M",1294,,,95,27,729,0,0,0,0,1,32,0,0,33,0,0,0,0,674,8563,0,274,8962,0,32,941,0,17,380,0,0,3,0,0,7,0,0,4,0,2906,1,50589,"NG","GT" 31,39,5,2,2,561,10,"CLEVELAND (CITY OF)","LAKE ROAD",0,"LIGHT OIL",3762,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2908,1,50589,"FO2","ST" 31,39,5,2,6,561,10,"CLEVELAND (CITY OF)","LAKE ROAD",0,"BIT COAL",3762,"0M",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2908,1,50589,"BIT","ST" 31,39,5,4,2,561,20,"CLEVELAND (CITY OF)","W 41ST ST",0,"LIGHT OIL",3762,"0M",1294,,,95,0,1,1995,0,0,1994,0,0,1994,0,0,1993,0,0,1993,0,0,1992,0,1,1992,0,1,1991,0,0,1990,0,0,1990,0,1,1989,0,0,1989,2909,1,50589,"FO2","GT" 31,39,5,4,9,561,20,"CLEVELAND (CITY OF)","W 41ST ST",0,"NAT GAS",3762,"0M",1294,,,95,477,14950,0,526,10745,0,431,12673,0,247,6523,0,221,6443,0,340,8176,0,1197,15109,0,4074,94135,0,593,26459,0,537,13366,0,668,16240,0,628,17345,0,2909,1,50589,"NG","GT" 31,39,5,2,6,579,1,"DOVER (CITY OF)","DOVER",0,"BIT COAL",5336,"0M",1294,,,95,7510,5164,474,5838,3935,612,7700,4900,592,6987,4742,130,0,7,150,0,0,623,5223,3579,213,7330,5046,506,6122,4199,218,2658,1764,200,6852,5320,346,7262,4963,413,2914,1,50806,"BIT","ST" 31,39,5,2,9,579,1,"DOVER (CITY OF)","DOVER",0,"NAT GAS",5336,"0M",794,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,27,403,0,884,12716,0,410,6737,0,110,1163,0,663,9798,0,637,9130,0,2914,1,50806,"NG","ST" 31,39,5,3,2,579,1,"DOVER (CITY OF)","DOVER",0,"LIGHT OIL",5336,"0M",1294,,,95,0,0,66,0,0,66,4,9,61,0,0,66,0,0,57,18,228,79,36,74,109,29,75,101,0,0,101,0,0,101,0,0,101,0,0,101,2914,1,50806,"FO2","IC" 31,39,5,4,9,579,5,"DOVER (CITY OF)","DOVER",0,"NAT GAS",5336,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,65,1022,0,0,0,0,0,0,0,0,0,0,48,698,0,0,0,0,0,0,0,0,0,0,0,0,0,2914,1,50806,"NG","GT" 31,39,5,2,2,605,1,"HAMILTON (CITY OF)","HAM MUN EL",0,"LIGHT OIL",7977,"0M",1294,,,95,5,11,1751,1,3,1749,1,4,1747,1,5,1744,1,4,1743,4,10,1737,3,7,1734,4,9,1730,4,11,1724,1,4,1722,1,6,1719,7,16,1711,2917,1,51225,"FO2","ST" 31,39,5,2,6,605,1,"HAMILTON (CITY OF)","HAM MUN EL",0,"BIT COAL",7977,"0M",1294,,,95,22703,11176,13737,252,146,15989,5474,3315,16142,8640,5428,12982,9803,5101,7881,11553,6584,1297,16363,9478,2000,22973,9375,5688,24478,13592,4621,4956,3752,6715,4870,4046,7024,23079,11772,7422,2917,1,51225,"BIT","ST" 31,39,5,2,9,605,1,"HAMILTON (CITY OF)","HAM MUN EL",0,"NAT GAS",7977,"0M",1294,,,95,157,1874,0,13990,195116,0,5260,76784,0,483,7231,0,4563,57272,0,9310,123945,0,17338,207709,0,14384,141922,0,1816,24404,0,676,12116,0,270,5334,0,784,9339,0,2917,1,51225,"NG","ST" 31,39,5,4,2,605,1,"HAMILTON (CITY OF)","HAM MUN EL",0,"LIGHT OIL",7977,"0M",1294,,,95,0,0,1751,0,0,1749,0,0,1748,0,0,1745,0,0,1742,0,0,1738,0,0,1735,0,0,1730,0,0,1725,0,0,1723,0,0,1719,0,0,1711,2917,1,51225,"FO2","GT" 31,39,5,4,9,605,1,"HAMILTON (CITY OF)","HAM MUN EL",0,"NAT GAS",7977,"0M",1294,,,95,11,142,0,174,2439,0,83,1220,0,26,393,0,18,234,0,55,745,0,1064,12754,0,1170,28673,0,18,250,0,134,2411,0,10,207,0,18,217,0,2917,1,51225,"NG","GT" 31,39,5,1,,605,5,"HAMILTON (CITY OF)","HMLTN HYDRO",0,,7977,"0M",1294,"R",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,7807,1,51225,"WAT","HY" 31,39,5,3,2,629,1,"LEBANON (CITY OF)","LEBANON",0,"LIGHT OIL",10830,"0M",1294,,,95,3,23,1067,0,0,1067,90,268,799,0,0,799,0,0,799,0,0,799,29,63,734,52,106,805,0,0,805,0,0,805,0,0,805,0,0,805,2921,1,51615,"FO2","IC" 31,39,5,4,2,629,1,"LEBANON (CITY OF)","LEBANON",0,"LIGHT OIL",10830,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2921,1,51615,"FO2","GT" 31,39,5,3,2,684,1,"OBERLIN (CITY OF)","OBERLIN",0,"LIGHT OIL",13949,"0A",1294,,,95,5,65,637,21,41,596,0,37,558,8,17,528,0,0,509,33,80,429,17,210,218,239,528,405,11,41,364,8,17,348,194,525,358,145,391,324,2933,1,52140,"FO2","IC" 31,39,5,3,9,684,1,"OBERLIN (CITY OF)","OBERLIN",0,"NAT GAS",13949,"0A",1294,,,95,275,2724,0,260,2802,0,5,1676,0,75,826,0,13,132,0,200,1734,0,339,3535,0,552,5958,0,39,487,0,82,884,0,969,9721,0,63,1533,0,2933,1,52140,"NG","IC" 31,39,5,2,6,689,1,"ORRVILLE (CITY OF)","ORRVILLE",0,"BIT COAL",14194,"0M",1294,,,95,30925,20332,2401,27128,23359,528,19190,7163,1721,22147,13962,524,29670,13038,1437,23583,15893,1741,24259,14697,2641,28372,19561,2485,22121,14691,1281,18235,13105,1557,28993,15643,959,24197,16177,783,2935,1,52192,"BIT","ST" 31,39,5,2,9,689,1,"ORRVILLE (CITY OF)","ORRVILLE",0,"NAT GAS",14194,"0M",1294,,,95,45,744,0,42,811,0,122,1020,0,127,1797,0,112,1116,0,51,780,0,63,856,0,72,1126,0,22,331,0,46,762,0,78,961,0,76,1181,0,2935,1,52192,"NG","ST" 31,39,5,2,2,691,1,"PAINESVILLE (CITY OF)","PAINESVILLE",0,"LIGHT OIL",14381,"0M",1294,,,95,0,0,1518,0,0,1518,0,0,1518,36,100,1776,5,13,1762,0,0,1048,0,0,1762,25,73,1689,25,73,1616,4,14,1602,17,53,1548,10,20,1528,2936,1,52227,"FO2","ST" 31,39,5,2,6,691,1,"PAINESVILLE (CITY OF)","PAINESVILLE",0,"BIT COAL",14381,"0M",1294,,,95,17099,10622,1607,15231,10037,2990,13188,8922,6467,12361,8060,7830,13138,7996,7962,15287,8544,8154,15901,9966,8093,12362,8310,8580,11176,7757,8780,11298,8213,9293,8336,6116,9293,7235,5099,7825,2936,1,52227,"BIT","ST" 31,39,5,2,9,691,1,"PAINESVILLE (CITY OF)","PAINESVILLE",0,"NAT GAS",14381,"0M",1294,,,95,16,258,0,29,464,0,152,2440,0,67,1072,0,27,394,0,18,254,0,42,658,0,113,1904,0,81,1386,0,46,839,0,100,1812,0,97,1715,0,2936,1,52227,"NG","ST" 31,39,5,2,2,700,10,"PIQUA (CITY OF)","PIQUA",0,"LIGHT OIL",15095,"0M",1294,,,95,0,1,33,1,9,24,0,0,35,1,7,27,0,0,32,0,1,31,0,1,30,0,0,30,0,0,30,0,4,26,0,3,23,1,6,36,2937,1,52334,"FO2","ST" 31,39,5,2,6,700,10,"PIQUA (CITY OF)","PIQUA",0,"BIT COAL",15095,"0M",1294,,,95,2963,3832,1560,2779,3526,1061,2427,2994,1038,1970,2648,582,2418,2789,195,1914,2556,734,1374,2211,15,1611,2421,41,1481,2312,382,2468,3140,627,2650,3515,1751,2688,3569,2090,2937,1,52334,"BIT","ST" 31,39,5,4,2,700,10,"PIQUA (CITY OF)","PIQUA",0,"LIGHT OIL",15095,"0M",1294,,,95,24,119,2949,51,239,3071,-37,127,2947,119,588,2896,109,897,3032,277,1359,2730,469,2758,2645,595,2956,2720,-11,101,2619,37,176,2979,59,288,3048,121,591,2992,2937,1,52334,"FO2","GT" 31,39,5,2,6,722,1,"SAINT MARYS (CITY OF)","ST MARYS",0,"BIT COAL",17891,"0M",1294,,,95,1250,698,645,3927,2565,332,4111,3269,140,0,0,150,0,0,150,1641,1050,490,5298,3368,489,222,149,638,1630,1068,419,4646,3274,449,4461,2807,449,4928,3119,495,2942,1,52789,"BIT","ST" 31,39,5,4,2,722,1,"SAINT MARYS (CITY OF)","ST MARYS",0,"LIGHT OIL",17891,"0M",1294,,,95,1,12,318,0,0,307,28,146,352,0,0,352,0,0,352,1,4,348,59,83,428,3,8,420,1,24,396,0,0,520,1,3,518,2,6,512,2942,1,52789,"FO2","GT" 31,39,5,2,6,726,1,"SHELBY (CITY OF)","SHELBY",0,"BIT COAL",17043,"0M",1294,,,95,8039,5710,300,7249,5098,300,7132,4852,300,6141,3985,300,6694,4389,300,8103,4859,300,6796,4831,300,7378,5266,0,6897,3944,300,6844,4580,300,7615,5188,300,8726,5206,300,2943,1,52637,"BIT","ST" 31,39,5,2,9,726,1,"SHELBY (CITY OF)","SHELBY",0,"NAT GAS",17043,"0M",1294,,,95,134,1996,0,47,686,0,36,517,0,9,134,0,0,0,0,30,381,0,96,1415,0,11,164,0,19,230,0,41,576,0,48,685,0,44,555,0,2943,1,52637,"NG","ST" 31,39,5,3,2,726,1,"SHELBY (CITY OF)","SHELBY",0,"LIGHT OIL",17043,"0M",1294,,,95,0,0,73,0,0,73,0,0,73,0,0,103,0,0,103,0,0,103,1,5,93,1,4,83,2,5,78,0,1,77,0,1,76,0,1,45,2943,1,52637,"FO2","IC" 31,39,5,3,9,726,1,"SHELBY (CITY OF)","SHELBY",0,"NAT GAS",17043,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2943,1,52637,"NG","IC" 31,39,5,3,2,774,1,"WOODSFIELD (CITY OF)","WOODSFIELD",0,"LIGHT OIL",20977,"0A",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2945,1,53350,"FO2","IC" 31,39,5,3,9,774,1,"WOODSFIELD (CITY OF)","WOODSFIELD",0,"NAT GAS",20977,"0A",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2945,1,53350,"NG","IC" 31,39,8,2,6,800,1,"AMER MUN POWER-OHIO INC","R GORSUCH",0,"BIT COAL",40577,"0M",1294,,,95,99037,64265,81413,104738,67228,84252,126378,79745,86718,63579,42733,100556,123281,76701,94920,115392,69307,101317,117333,72018,101225,121473,79176,86641,108722,66669,90892,126955,78956,87022,103717,67360,86260,126485,80616,78276,7286,1,58910,"BIT","ST" 31,39,8,2,9,800,1,"AMER MUN POWER-OHIO INC","R GORSUCH",0,"NAT GAS",40577,"0M",1294,,,95,1576,22702,0,1469,21157,0,638,9083,0,541,8226,0,767,10634,0,1094,14686,0,877,12191,0,505,7352,0,810,11188,0,528,7439,0,733,10544,0,821,11624,0,7286,1,58910,"NG","ST" 32,18,1,2,6,25,1,"COMMONWEALTH ED CO IND","STATE LINE",0,"BIT COAL",4111,"0M",1294,,101,95,111368,64033,111935,149730,82697,41943,169301,90886,94463,49952,30907,197006,107334,61118,203229,185763,102059,199201,147171,80912,167481,211732,117972,103696,93902,54629,131796,97942,56647,95060,141995,78255,74660,93050,52182,100094,981,4,54003,"BIT","ST" 32,18,1,2,9,25,1,"COMMONWEALTH ED CO IND","STATE LINE",0,"NAT GAS",4111,"0M",1294,,101,95,6077,64670,0,5326,53012,0,4895,48146,0,1349,14775,0,4538,48258,0,4988,51500,0,4470,45645,0,4498,45907,0,2972,32243,0,3706,39699,0,5098,51893,0,3793,39849,0,981,4,54003,"NG","ST" 32,18,1,2,2,45,1,"INDIANA-KENTUCKY EL CORP","CLIFTY CRK",0,"LIGHT OIL",9269,"0M",1294,,505,95,186,351,3905,152,276,3630,241,444,3700,377,692,3522,263,551,3142,200,360,3468,175,320,4005,93,171,4177,112,189,3988,183,330,3658,234,419,3925,187,321,3947,983,1,54010,"FO2","ST" 32,18,1,2,6,45,1,"INDIANA-KENTUCKY EL CORP","CLIFTY CRK",0,"BIT COAL",9269,"0M",1294,,505,95,680000,340288,711560,681685,332462,794224,771872,377298,719124,715568,349771,768331,774831,394798,790608,706890,347717,739042,846234,432529,698423,836401,439085,664104,841295,424266,608234,755940,378632,751924,859900,416889,759244,867253,423226,804472,983,1,54010,"BIT","ST" 32,18,1,1,,57,5,"INDIANA MICHIGAN POWER CO","ELKHART",0,,9324,"0M",1294,,363,95,1650,0,0,1194,0,0,1755,0,0,1250,0,0,1341,0,0,1179,0,0,1157,0,0,1230,0,0,728,0,0,610,0,0,606,0,0,1138,0,0,986,1,57745,"WAT","HY" 32,18,1,1,,57,15,"INDIANA MICHIGAN POWER CO","TWIN BRANCH",0,,9324,"0M",1294,,363,95,2749,0,0,2559,0,0,3177,0,0,3035,0,0,3169,0,0,2570,0,0,2394,0,0,2550,0,0,1769,0,0,1707,0,0,2868,0,0,2542,0,0,989,1,57745,"WAT","HY" 32,18,1,2,2,57,40,"INDIANA MICHIGAN POWER CO","TANNERS CRK",0,"LIGHT OIL",9324,"0M",1294,,363,95,1203,1922,5959,701,1134,5915,1180,2025,6714,1059,1682,6177,1112,1829,5848,1144,1978,6336,1259,2060,7095,1078,1912,5713,665,1191,4522,206,409,5361,886,1592,4308,1326,2011,4418,988,1,57745,"FO2","ST" 32,18,1,2,6,57,40,"INDIANA MICHIGAN POWER CO","TANNERS CRK",0,"BIT COAL",9324,"0M",1294,,363,95,432338,162155,420217,485332,183170,404434,427268,171172,375261,371083,146417,383926,364601,144830,374644,383224,158993,372917,442272,183537,275408,494886,200826,195877,151186,61682,248353,10073,4559,312659,189477,75997,327350,330050,118848,262047,988,1,57745,"BIT","ST" 32,18,1,4,2,57,55,"INDIANA MICHIGAN POWER CO","FOURTH ST",0,"LIGHT OIL",9324,"0M",1294,,363,95,0,0,90,0,0,90,0,0,90,0,0,90,0,0,90,0,0,90,0,0,90,0,0,90,0,0,90,0,0,90,0,0,90,0,0,90,1025,1,57745,"FO2","GT" 32,18,1,2,2,57,60,"INDIANA MICHIGAN POWER CO","ROCKPORT",0,"LIGHT OIL",9324,"0M",1294,,363,95,1253,2167,36532,1335,2320,34384,3886,6841,48740,4321,7609,41131,3580,6420,34711,5662,10180,45654,3887,6888,38767,4216,7569,31198,1478,2587,28611,1002,1634,26976,690,1194,25782,1723,4126,33355,6166,1,57745,"FO2","ST" 32,18,1,2,6,57,60,"INDIANA MICHIGAN POWER CO","ROCKPORT",0,"BIT COAL",9324,"0M",1294,,363,95,1749008,1032186,1725862,1579775,933220,1565332,1339465,797497,1717887,1321428,787392,1749794,910898,553161,1861348,1507665,916281,1691338,1420244,862282,1685879,1514621,918947,1761783,1599963,954251,1694782,1691163,933949,1738612,1640828,959611,1762887,1464158,854236,1918162,6166,1,57745,"BIT","ST" 32,18,1,2,2,63,5,"INDIANAPOLIS PWR & LGT CO","E W STOUT",0,"LIGHT OIL",9273,"0M",1294,,,95,566,1401,20541,856,1914,17945,116,609,17337,446,1143,15565,419,1038,14023,233,762,13073,334,805,11083,970,3484,18728,223,679,18049,471,1101,16948,1380,2012,14910,618,1456,13138,990,1,51394,"FO2","ST" 32,18,1,2,6,63,5,"INDIANAPOLIS PWR & LGT CO","E W STOUT",0,"BIT COAL",9273,"0M",1294,,,95,194584,90056,252587,180919,84581,279836,140480,66420,317709,160947,73882,318796,235268,109052,299888,217930,103073,287645,259644,122601,267666,349367,162431,221093,272895,126479,196285,244308,112170,197708,270443,125748,220391,253279,116842,274191,990,1,51394,"BIT","ST" 32,18,1,3,2,63,5,"INDIANAPOLIS PWR & LGT CO","E W STOUT",0,"LIGHT OIL",9273,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,990,1,51394,"FO2","IC" 32,18,1,4,2,63,5,"INDIANAPOLIS PWR & LGT CO","E W STOUT",0,"LIGHT OIL",9273,"0M",1294,,,95,1107,4856,0,-42,681,0,-50,0,0,112,628,0,182,504,0,-7,189,0,293,1179,0,349,1894,0,-35,0,0,-43,0,0,-50,26,0,-11,317,0,990,1,51394,"FO2","GT" 32,18,1,4,9,63,5,"INDIANAPOLIS PWR & LGT CO","E W STOUT",0,"NAT GAS",9273,"0M",1294,,,95,1286,11256,0,10,1339,0,-53,1880,0,93,2875,0,1102,18630,0,448,8470,0,4489,66365,0,11695,166046,0,-64,3722,0,-37,1618,0,3205,49273,0,3710,54428,0,990,1,51394,"NG","GT" 32,18,1,2,2,63,15,"INDIANAPOLIS PWR & LGT CO","PERRY K",0,"LIGHT OIL",9273,"0M",1294,,,95,0,0,4682,0,0,4553,0,0,4331,0,0,4301,0,0,4287,0,0,3841,0,0,3636,0,0,5062,0,0,5057,0,0,5051,0,0,5042,0,0,4762,992,1,51394,"FO2","ST" 32,18,1,2,6,63,15,"INDIANAPOLIS PWR & LGT CO","PERRY K",0,"BIT COAL",9273,"0M",1294,,,95,0,0,79574,-1610,0,80083,0,0,75101,0,0,73147,0,0,75348,0,0,76456,766,826,73924,340,352,74885,1152,1362,75776,0,0,74934,0,0,77090,0,0,71176,992,1,51394,"BIT","ST" 32,18,1,2,9,63,15,"INDIANAPOLIS PWR & LGT CO","PERRY K",0,"NAT GAS",9273,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,17,437,0,7,193,0,32,957,0,0,0,0,0,0,0,0,0,0,992,1,51394,"NG","ST" 32,18,1,5,9,63,15,"INDIANAPOLIS PWR & LGT CO","PERRY K",0,"WASTE HT",9273,"0M",1294,,,95,-782,0,0,0,0,0,1330,0,0,1056,0,0,2878,0,0,887,0,0,1971,0,0,1192,0,0,1301,0,0,1055,0,0,-372,0,0,-854,0,0,992,1,51394,"WT","CC" 32,18,1,2,2,63,20,"INDIANAPOLIS PWR & LGT CO","PERRY W",0,"LIGHT OIL",9273,"0M",1294,,,95,-49,0,697,-71,0,697,-71,0,697,-67,0,697,-59,0,697,-46,0,697,-51,0,697,-47,0,697,-42,0,697,-44,0,697,-59,0,697,-65,0,697,993,1,51394,"FO2","ST" 32,18,1,2,9,63,20,"INDIANAPOLIS PWR & LGT CO","PERRY W",0,"NAT GAS",9273,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,993,1,51394,"NG","ST" 32,18,1,5,9,63,20,"INDIANAPOLIS PWR & LGT CO","PERRY W",0,"WASTE HT",9273,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,993,1,51394,"WH","CC" 32,18,1,2,2,63,23,"INDIANAPOLIS PWR & LGT CO","PETERSBURG",0,"LIGHT OIL",9273,"0M",1294,,,95,610,1111,6386,445,819,5517,317,533,4940,401,748,8963,2218,4082,4553,637,1151,5787,377,687,4945,1822,3221,6367,801,1483,4763,545,999,3635,1447,2637,5880,1975,3581,4564,994,1,51394,"FO2","ST" 32,18,1,2,6,63,23,"INDIANAPOLIS PWR & LGT CO","PETERSBURG",0,"BIT COAL",9273,"0M",1294,,,95,1040025,481608,951198,910590,421941,973809,942914,432679,1023657,783657,368727,1096578,667135,315158,1184238,973163,448245,1179213,992610,460767,1051137,936517,439379,945966,722162,339012,925268,812107,376653,886087,794558,370468,820716,931266,431118,719090,994,1,51394,"BIT","ST" 32,18,1,3,2,63,23,"INDIANAPOLIS PWR & LGT CO","PETERSBURG",0,"LIGHT OIL",9273,"0M",1294,,,95,2,5,0,0,0,0,25,44,0,102,178,0,189,328,0,45,76,0,52,90,0,74,131,0,46,80,0,67,116,0,39,43,0,31,78,0,994,1,51394,"FO2","IC" 32,18,1,2,2,63,25,"INDIANAPOLIS PWR & LGT CO","H T PRTCHRD",0,"LIGHT OIL",9273,"0M",1294,,,95,318,680,5661,350,656,4975,104,195,4685,436,902,7879,417,829,7014,283,586,6386,443,914,5445,1802,3787,7417,307,627,7108,203,431,6547,316,654,5835,499,993,4785,991,1,51394,"FO2","ST" 32,18,1,2,6,63,25,"INDIANAPOLIS PWR & LGT CO","H T PRTCHRD",0,"BIT COAL",9273,"0M",1294,,,95,39918,21829,172846,38399,18739,164110,25730,13890,166007,31554,16614,192907,62657,32105,189004,38978,20477,189810,89346,46785,168301,129720,68988,123731,61410,31642,119624,29705,15920,161259,67519,35572,171574,68221,34547,157787,991,1,51394,"BIT","ST" 32,18,1,3,2,63,25,"INDIANAPOLIS PWR & LGT CO","H T PRTCHRD",0,"LIGHT OIL",9273,"0M",1294,,,95,10,18,0,10,18,0,11,19,0,10,19,0,10,19,0,10,18,0,9,18,0,10,18,0,9,18,0,3,5,0,10,11,0,10,16,0,991,1,51394,"FO2","IC" 32,18,1,1,,97,25,"NORTHERN IND PUB SERV CO","NORWAY",0,,13756,"0M",1294,,,95,2951,0,0,1754,0,0,3112,0,0,3813,0,0,3505,0,0,2903,0,0,2206,0,0,1230,0,0,509,0,0,-5,0,0,935,0,0,741,0,0,998,1,52101,"WAT","HY" 32,18,1,1,,97,30,"NORTHERN IND PUB SERV CO","OAKDALE",0,,13756,"0M",1294,,,95,4302,0,0,2658,0,0,4495,0,0,5358,0,0,4552,0,0,4225,0,0,3387,0,0,1840,0,0,1214,0,0,492,0,0,1566,0,0,1435,0,0,999,1,52101,"WAT","HY" 32,18,1,2,5,97,35,"NORTHERN IND PUB SERV CO","BAILLY",0,"COKE",13756,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,995,1,52101,"PC","ST" 32,18,1,2,6,97,35,"NORTHERN IND PUB SERV CO","BAILLY",0,"BIT COAL",13756,"0M",1294,,,95,255092,122559,79738,278804,133215,33213,188964,93227,81145,300874,140721,83750,249838,120767,64124,246937,117749,44162,235477,114020,45186,281196,134308,37119,206770,100042,54350,171878,84048,49037,248313,118863,34340,215434,105042,32995,995,1,52101,"BIT","ST" 32,18,1,2,9,97,35,"NORTHERN IND PUB SERV CO","BAILLY",0,"NAT GAS",13756,"0M",1294,,,95,2509,26046,0,1617,16709,0,6960,74244,0,364,3631,0,132,1380,0,473,4895,0,3976,41921,0,11155,116087,0,295,3099,0,9000,94567,0,731,7651,0,10008,106430,0,995,1,52101,"NG","ST" 32,18,1,4,2,97,35,"NORTHERN IND PUB SERV CO","BAILLY",0,"LIGHT OIL",13756,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,995,1,52101,"FO2","GT" 32,18,1,4,9,97,35,"NORTHERN IND PUB SERV CO","BAILLY",0,"NAT GAS",13756,"0M",1294,,,95,260,4325,0,239,4585,0,197,4652,0,73,729,0,0,0,0,128,2648,0,1309,27718,0,1556,27641,0,86,2797,0,94,990,0,0,0,0,0,0,0,995,1,52101,"NG","GT" 32,18,1,2,6,97,50,"NORTHERN IND PUB SERV CO","MICH CITY",0,"BIT COAL",13756,"0M",1294,,,95,236420,123317,103301,234123,120234,148075,251278,135807,162546,205743,116541,177892,112253,67389,170049,124057,76284,129959,232893,135633,114125,231506,135299,93596,234187,129907,86183,254454,138881,100596,227408,129965,87044,241351,131616,87326,997,1,52101,"BIT","ST" 32,18,1,2,9,97,50,"NORTHERN IND PUB SERV CO","MICH CITY",0,"NAT GAS",13756,"0M",1294,,,95,22888,245981,0,12315,127428,0,7313,77250,0,2223,23885,0,17374,195664,0,14491,167133,0,33790,372448,0,46983,516773,0,57,601,0,277,2894,0,14761,158089,0,7779,81844,0,997,1,52101,"NG","ST" 32,18,1,2,6,97,54,"NORTHERN IND PUB SERV CO","D MITCHELL",0,"BIT COAL",13756,"0M",1294,,,95,145857,82802,116751,116897,65893,113729,119863,69185,152487,141199,84936,154502,149654,87531,159194,148998,85732,121077,153374,92272,109798,153611,89672,90907,105137,61906,133520,134131,77926,126283,118138,72811,149593,119904,77033,120350,996,1,52101,"BIT","ST" 32,18,1,2,9,97,54,"NORTHERN IND PUB SERV CO","D MITCHELL",0,"NAT GAS",13756,"0M",1294,,,95,9050,99836,0,19988,219179,0,4693,51173,0,2044,22775,0,681,7679,0,15253,169699,0,31855,357533,0,49912,561059,0,1836,21192,0,688,7733,0,17585,198980,0,12007,137527,0,996,1,52101,"NG","ST" 32,18,1,4,2,97,54,"NORTHERN IND PUB SERV CO","D MITCHELL",0,"LIGHT OIL",13756,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,996,1,52101,"FO2","GT" 32,18,1,4,9,97,54,"NORTHERN IND PUB SERV CO","D MITCHELL",0,"NAT GAS",13756,"0M",1294,,,95,0,0,0,62,1005,0,19,314,0,61,972,0,59,947,0,23,381,0,1109,18451,0,787,13562,0,0,0,0,17,200,0,19,316,0,40,614,0,996,1,52101,"NG","GT" 32,18,1,2,2,97,60,"NORTHERN IND PUB SERV CO","SCHAHFER",0,"LIGHT OIL",13756,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,6085,1,52101,"FO2","ST" 32,18,1,2,5,97,60,"NORTHERN IND PUB SERV CO","SCHAHFER",0,"COKE",13756,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,5680,2361,3668,16726,6787,383,17831,7291,7,6085,1,52101,"PC","ST" 32,18,1,2,6,97,60,"NORTHERN IND PUB SERV CO","SCHAHFER",0,"BIT COAL",13756,"0M",1294,,,95,535261,312105,335057,389163,229937,440028,546548,302317,415959,448635,246990,395514,597050,350998,454670,756850,452731,337454,682007,398333,335076,754511,435319,290970,649742,383628,258615,683709,390480,291948,637992,357548,247219,681946,380639,238033,6085,1,52101,"BIT","ST" 32,18,1,2,9,97,60,"NORTHERN IND PUB SERV CO","SCHAHFER",0,"NAT GAS",13756,"0M",1294,,,95,3899,42407,0,6373,71396,0,4950,53485,0,5022,55321,0,9160,101163,0,8473,94946,0,11416,127138,0,11318,127241,0,6765,76948,0,5330,59832,0,10465,114654,0,16610,183389,0,6085,1,52101,"NG","ST" 32,18,1,4,2,97,60,"NORTHERN IND PUB SERV CO","SCHAHFER",0,"LIGHT OIL",13756,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,6085,1,52101,"FO2","GT" 32,18,1,4,9,97,60,"NORTHERN IND PUB SERV CO","SCHAHFER",0,"NAT GAS",13756,"0M",1294,,,95,723,10302,0,782,11325,0,1650,23018,0,308,4700,0,805,15657,0,1994,32783,0,15126,225451,0,13726,215839,0,142,2242,0,733,10618,0,280,4262,0,601,10905,0,6085,1,52101,"NG","GT" 32,18,1,1,,115,10,"PSI ENERGY, INC","MARKLAND",0,,15470,"0M",1294,,,95,25874,0,0,30535,0,0,30427,0,0,34190,0,0,21420,0,0,33483,0,0,37429,0,0,31238,0,0,21329,0,0,31723,0,0,32028,0,0,33480,0,0,1005,1,52410,"WAT","HY" 32,18,1,2,2,115,20,"PSI ENERGY, INC","CAYUGA",0,"LIGHT OIL",15470,"0M",1294,,,95,132,235,5513,571,1037,4367,530,968,3231,360,648,6046,1268,2286,3656,1673,3058,5188,191,340,4690,456,897,3714,450,808,2757,116,203,4365,648,1159,3695,1043,1890,4595,1001,1,52410,"FO2","ST" 32,18,1,2,6,115,20,"PSI ENERGY, INC","CAYUGA",0,"BIT COAL",15470,"0M",1294,,,95,560086,260374,595374,436002,205588,619769,507290,241920,579748,458167,216960,558238,273942,132145,579528,461324,222630,594519,529339,250671,586438,553167,264792,531310,481498,229472,498542,556861,260068,435186,538773,254635,379746,560196,264529,360124,1001,1,52410,"BIT","ST" 32,18,1,3,2,115,20,"PSI ENERGY, INC","CAYUGA",0,"LIGHT OIL",15470,"0M",1294,,,95,52,94,835,80,146,689,46,85,604,32,59,546,48,87,793,40,74,719,187,332,719,345,632,893,44,79,814,57,100,714,46,83,810,52,95,715,1001,1,52410,"FO2","IC" 32,18,1,4,2,115,20,"PSI ENERGY, INC","CAYUGA",0,"LIGHT OIL",15470,"0M",1294,,,95,94,169,5321,0,0,5313,0,0,5287,0,0,5295,9,17,5278,0,0,5274,0,0,5261,0,0,5256,0,0,5278,0,0,5291,0,0,5304,0,0,5321,1001,1,52410,"FO2","GT" 32,18,1,4,9,115,20,"PSI ENERGY, INC","CAYUGA",0,"NAT GAS",15470,"0M",1294,,,95,2346,23310,0,1913,19353,0,1506,15557,0,1635,16714,0,1240,12674,0,4044,41468,0,15842,159433,0,18202,212550,0,0,0,0,0,0,0,2097,21202,0,3527,35908,0,1001,1,52410,"NG","GT" 32,18,1,2,2,115,30,"PSI ENERGY, INC","EDWARDSPORT",0,"LIGHT OIL",15470,"0M",1294,,,95,209,496,4820,64,150,4672,155,373,4297,0,0,4295,0,0,4292,97,238,4052,689,1571,2481,2502,5818,2869,342,868,2002,0,0,2002,0,0,1997,147,370,1625,1004,1,52410,"FO2","ST" 32,18,1,2,6,115,30,"PSI ENERGY, INC","EDWARDSPORT",0,"BIT COAL",15470,"0M",1294,,,95,17730,11048,72080,19934,11948,70647,12688,8051,74559,-527,0,75232,-535,0,75232,15454,10259,64973,35050,21901,43072,52741,33340,15650,4173,2912,38766,-602,0,62015,-609,0,63195,16335,10947,52274,1004,1,52410,"BIT","ST" 32,18,1,2,2,115,32,"PSI ENERGY, INC","R GALLAGHER",0,"LIGHT OIL",15470,"0M",1294,,,95,2035,3891,1605,1454,2810,1394,1851,3297,1699,1757,3179,1643,2068,3708,1567,1765,3297,1717,1740,3339,1643,1698,3478,1699,628,1171,1662,1918,3473,1772,1054,1957,1432,2452,4557,1662,1008,1,52410,"FO2","ST" 32,18,1,2,6,115,32,"PSI ENERGY, INC","R GALLAGHER",0,"BIT COAL",15470,"0M",1294,,,95,228795,101724,280677,208492,94433,264483,157312,68908,321856,177541,78622,327010,219815,95103,325222,282888,123689,301473,287606,128632,273012,307948,143686,219622,142108,60394,233330,173570,72509,241738,224846,92953,254240,214410,90070,255848,1008,1,52410,"BIT","ST" 32,18,1,2,2,115,35,"PSI ENERGY, INC","NOBLESVILLE",0,"LIGHT OIL",15470,"0M",1294,,,95,51,112,562,83,160,505,48,112,674,66,152,531,0,0,490,110,229,643,81,169,664,55,117,548,22,64,674,58,167,474,0,43,548,34,71,476,1007,1,52410,"FO2","ST" 32,18,1,2,6,115,35,"PSI ENERGY, INC","NOBLESVILLE",0,"BIT COAL",15470,"0M",1294,,,95,11044,6031,55495,9455,4868,50627,3897,2460,49399,4036,2484,49078,-19,344,48734,11688,6456,42278,26318,14879,27399,34289,19561,18825,965,758,32438,3085,2324,49315,-104,155,61612,12274,6417,55744,1007,1,52410,"BIT","ST" 32,18,1,2,2,115,38,"PSI ENERGY, INC","WABASH RIVR",0,"LIGHT OIL",15470,"0M",1294,,,95,2430,4476,2106,1459,2739,2128,1389,2692,1967,1849,3579,2218,1434,2758,1631,681,1290,2176,1683,3263,2148,2465,4797,2269,945,1807,2338,1000,1900,2380,729,1435,2430,2010,3862,1720,1010,1,52410,"FO2","ST" 32,18,1,2,6,115,38,"PSI ENERGY, INC","WABASH RIVR",0,"BIT COAL",15470,"0M",1294,,,95,269453,126688,229629,237554,115161,230254,111825,56100,288778,84991,42415,325474,75621,37146,348471,305101,147377,290801,239625,122121,244288,280979,141633,160506,165651,82144,169356,117517,58071,210036,143505,72409,218547,185588,91761,206945,1010,1,52410,"BIT","ST" 32,18,1,3,2,115,38,"PSI ENERGY, INC","WABASH RIVR",0,"LIGHT OIL",15470,"0M",1294,,,95,22,41,295,6,12,283,29,57,226,36,71,155,22,43,283,17,33,250,46,91,336,25,50,286,1,2,283,16,31,37,14,29,343,5,10,333,1010,1,52410,"FO2","IC" 32,18,1,3,2,115,40,"PSI ENERGY, INC","MIAMI WBASH",0,"LIGHT OIL",15470,"0M",1294,,,95,-10,953,9190,166,743,8447,-197,894,7552,-39,60,7493,16,281,7212,81,612,6600,891,3627,5277,1034,3669,3913,-3,92,3821,-25,12,3809,-92,165,3644,-114,427,3217,1006,1,52410,"FO2","IC" 32,18,1,4,2,115,43,"PSI ENERGY, INC","CONNERSVILE",0,"LIGHT OIL",15470,"0M",1294,,,95,598,1430,6151,267,338,5812,185,528,5284,-1,88,5196,74,91,5105,363,946,4160,1734,3950,0,1728,5143,7132,123,299,6833,35,74,6797,36,197,6601,68,309,6291,1002,1,52410,"FO2","GT" 32,18,1,2,2,115,47,"PSI ENERGY, INC","GIBSON STA",0,"LIGHT OIL",15470,"0M",1294,,,95,3573,6225,8026,3627,6211,8525,2908,4962,6089,2299,3933,7385,2638,4537,9046,4608,8201,6236,1193,2069,8692,1020,1752,9495,2262,3909,8491,2394,4067,6679,1306,2237,7725,1788,3105,5067,6113,1,52410,"FO2","ST" 32,18,1,2,6,115,47,"PSI ENERGY, INC","GIBSON STA",0,"BIT COAL",15470,"0M",1294,,,95,1411040,662768,2861774,1615449,737476,2742578,1641475,746285,2737505,1326993,600387,2789580,1389674,630387,2844473,1353290,632853,2819275,1781130,810634,2543921,1880261,844888,2374175,1610199,724136,2280260,1401722,620957,2297336,1703790,761235,2101523,1647889,748548,1888232,6113,1,52410,"BIT","ST" 32,18,1,4,2,127,1,"SOUTHERN INDIANA G & E CO","BROADWAY",0,"LIGHT OIL",17633,"0M",1294,,,95,0,0,801,0,0,801,0,0,801,0,0,801,0,0,801,0,0,801,0,0,801,0,0,801,0,0,801,0,0,801,0,0,801,0,0,801,1011,1,52727,"FO2","GT" 32,18,1,4,9,127,1,"SOUTHERN INDIANA G & E CO","BROADWAY",0,"NAT GAS",17633,"0M",1294,,,95,108,1488,0,31,496,0,72,936,0,66,992,0,675,9932,0,358,9922,0,3822,54621,0,11701,173627,0,131,4946,0,181,9912,0,586,4959,0,0,0,0,1011,1,52727,"NG","GT" 32,18,1,2,2,127,3,"SOUTHERN INDIANA G & E CO","CULLEY",0,"LIGHT OIL",17633,"0M",1294,,,95,0,0,350,0,0,350,0,0,350,0,0,350,0,0,350,0,0,250,0,0,250,0,0,250,0,0,250,0,0,250,0,0,250,0,0,250,1012,1,52727,"FO2","ST" 32,18,1,2,6,127,3,"SOUTHERN INDIANA G & E CO","CULLEY",0,"BIT COAL",17633,"0M",1294,,,95,122067,60600,138140,167988,82419,159735,169634,79436,181228,114459,53639,191704,165848,81055,168418,184693,87570,154235,207611,100070,138520,218589,105190,134359,160446,77417,139667,174664,86907,135057,217251,106316,124021,205575,102713,115674,1012,1,52727,"BIT","ST" 32,18,1,2,9,127,3,"SOUTHERN INDIANA G & E CO","CULLEY",0,"NAT GAS",17633,"0M",1294,,,95,285,3090,0,126,1344,0,136,1410,0,300,3116,0,121,1311,0,107,1123,0,101,1082,0,285,3040,0,412,4406,0,312,3443,0,180,1935,0,153,1681,0,1012,1,52727,"NG","ST" 32,18,1,4,9,127,9,"SOUTHERN INDIANA G & E CO","NORTHEAST",0,"NAT GAS",17633,"0M",1294,,,95,24,992,0,48,5399,0,0,0,0,0,0,0,0,0,0,22,2492,0,0,0,0,562,10295,0,0,0,0,0,0,0,23,3023,0,26,4467,0,1013,1,52727,"NG","GT" 32,18,1,2,6,127,20,"SOUTHERN INDIANA G & E CO","WARRICK",0,"BIT COAL",17633,"0M",1294,,,95,95617,41510,100212,86572,39259,87257,96250,42312,89684,93020,40228,97629,96270,44344,83127,82739,38242,69870,89329,39892,44260,100497,44406,41656,97103,42826,35874,28941,12332,66823,92060,41077,55982,99718,45727,57793,6705,1,52727,"BIT","ST" 32,18,1,2,9,127,20,"SOUTHERN INDIANA G & E CO","WARRICK",0,"NAT GAS",17633,"0M",1294,,,95,27,261,0,112,1120,0,11,112,0,29,276,0,5,50,0,0,0,0,136,1318,0,83,796,0,0,0,0,295,2822,0,57,575,0,62,639,0,6705,1,52727,"NG","ST" 32,18,1,2,2,127,25,"SOUTHERN INDIANA G & E CO","BROWN",0,"LIGHT OIL",17633,"0M",1294,,,95,0,0,1712,0,0,1437,0,0,2186,0,0,2151,0,0,1998,0,0,1988,0,0,2336,0,0,2336,0,0,2336,0,0,2336,0,0,2175,0,0,2175,6137,1,52727,"FO2","ST" 32,18,1,2,6,127,25,"SOUTHERN INDIANA G & E CO","BROWN",0,"BIT COAL",17633,"0M",1294,,,95,217766,95613,450544,147685,72927,476200,218223,106171,479883,196964,85661,485255,182235,86959,499237,216954,101195,498135,247301,113099,429991,275892,131703,360852,177911,84026,286413,238026,112468,229493,139223,67172,246596,170321,82481,189492,6137,1,52727,"BIT","ST" 32,18,1,2,9,127,25,"SOUTHERN INDIANA G & E CO","BROWN",0,"NAT GAS",17633,"0M",1294,,,95,728,7231,0,709,7962,0,465,5154,0,1271,12486,0,681,7404,0,869,9196,0,829,8558,0,910,9792,0,91,976,0,1005,9912,0,462,4959,0,1013,10609,0,6137,1,52727,"NG","ST" 32,18,1,4,2,127,25,"SOUTHERN INDIANA G & E CO","BROWN",0,"LIGHT OIL",17633,"0M",1294,,,95,0,0,0,139,275,0,10,21,0,20,35,0,75,144,0,155,289,0,4,9,0,0,0,0,0,0,0,0,0,0,84,161,0,0,0,0,6137,1,52727,"FO2","GT" 32,18,1,4,9,127,25,"SOUTHERN INDIANA G & E CO","BROWN",0,"NAT GAS",17633,"0M",1294,,,95,371,3684,0,237,2668,0,72,799,0,244,2399,0,872,9478,0,725,7671,0,3499,36107,0,8313,89423,0,835,8917,0,0,0,0,0,0,0,115,1208,0,6137,1,52727,"NG","GT" 32,18,5,3,2,529,15,"BLUFFTON (CITY OF)","BLUFFTON",0,"LIGHT OIL",1896,"0A",1294,,,95,1,60,1391,2,67,1322,61,54,1600,8,70,1533,12,90,1444,17,90,1361,5,46,0,16,58,1746,9,46,1693,5,45,1674,1,9,1658,1,20,1637,1023,1,54077,"FO2","IC" 32,18,5,3,9,529,15,"BLUFFTON (CITY OF)","BLUFFTON",0,"NAT GAS",1896,"0A",1294,,,95,252,951,0,283,1047,0,187,936,0,252,888,0,327,1129,0,322,1124,0,21,749,0,165,1201,0,79,956,0,14,141,0,8,282,0,62,1131,0,1023,1,54077,"NG","IC" 32,18,5,2,6,552,1,"CRAWFORDSVILLE (CITY OF)","CRAWFRDVIL",0,"BIT COAL",4508,"M",1294,,,95,2633,2217,2514,2446,2032,2094,1890,1637,1012,0,12,1693,0,9,2211,497,408,1961,0,0,1961,1383,1034,1775,0,0,2801,0,0,2783,0,0,2783,2446,2070,2457,1024,1,50698,"BIT","ST" 32,18,5,2,9,552,1,"CTAWFORDSVILLE (CITY OF)","CRAWFRDVIL",0,"NAT GAS",4508,"M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,11,198,0,0,9,0,25,397,0,0,0,0,0,0,0,0,0,0,0,0,0,1024,1,50698,"NG","ST" 32,18,5,3,2,552,1,"CRAWFORDSVILLE (CITY OF)","CRAWFRDVIL",0,"LIGHT OIL",4508,"M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1024,1,50698,"FO2","IC" 32,18,5,2,6,601,1,"JASPER (CITY OF)","JASPER",0,"BIT COAL",9667,"0A",1294,,,95,5717,4616,631,5399,3895,631,5890,4398,631,2952,2186,631,3065,2373,631,5988,4375,631,5621,4191,631,2798,2138,631,0,0,1075,5001,3514,1051,5782,4146,1096,5466,4050,1096,6225,1,51443,"BIT","ST" 32,18,5,2,9,601,1,"JASPER (CITY OF)","JASPER",0,"NAT GAS",9667,"0A",1294,,,95,20,339,0,0,0,0,0,0,0,0,0,0,16,267,0,0,0,0,0,0,0,0,0,0,0,0,0,14,206,0,0,0,0,0,0,0,6225,1,51443,"NG","ST" 32,18,5,2,6,622,1,"LOGANSPORT (CITY OF)","LOGANSPORT",0,"BIT COAL",11142,"0M",1294,,,95,16294,10401,3093,15182,9658,2825,130,68,5257,0,0,7057,2842,2773,7049,15721,9566,3565,18496,9015,1600,18517,10895,1421,17032,9835,4095,8771,5557,5126,12606,7370,5733,23315,13078,934,1032,1,51681,"BIT","ST" 32,18,5,4,2,622,1,"LOGANSPORT (CITY OF)","LOGANSPORT",0,"LIGHT OIL",11142,"0M",1294,,,95,0,0,1887,0,0,1887,0,0,1887,0,0,1887,0,0,1887,0,0,1887,0,0,1887,0,0,1887,0,0,1887,0,0,1887,0,0,1887,0,0,1887,1032,1,51681,"FO2","GT" 32,18,5,4,9,622,1,"LOGANSPORT (CITY OF)","LOGANSPORT",0,"NAT GAS",11142,"0M",1294,,,95,127,2771,0,0,0,0,0,0,0,0,0,0,0,0,0,75,2842,0,0,0,0,217,5351,0,0,0,0,0,0,0,0,0,0,0,0,0,1032,1,51681,"NG","GT" 32,18,5,2,2,658,1,"PERU UTILITIES","PERU",0,"LIGHT OIL",14839,"0M",1294,,,95,2,7,60,0,0,40,0,0,29,0,0,45,0,0,42,0,0,89,0,0,89,28,62,123,2,6,104,0,0,104,0,0,64,0,0,58,1037,1,52298,"FO2","ST" 32,18,5,2,6,658,1,"PERU UTILITIES","PERU",0,"BIT COAL",14839,"0M",1294,,,95,597,409,462,0,0,462,0,0,462,0,0,462,0,0,462,0,0,664,0,0,664,4138,2475,1193,1602,1122,71,0,0,71,0,0,71,0,0,71,1037,1,52298,"BIT","ST" 32,18,5,3,2,666,1,"RENSSELAER (CITY OF)","RENSSELAER",0,"LIGHT OIL",15860,"0A",1294,,,95,0,5,507,0,4,492,0,0,385,0,0,376,42,89,635,0,0,624,11,22,610,10,24,577,13,25,557,13,33,523,18,34,485,12,25,448,1038,1,52461,"FO2","IC" 32,18,5,3,9,666,1,"RENSSELAER (CITY OF)","RENSSELAER",0,"NAT GAS",15860,"0A",1294,,,95,12,2242,0,5,609,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1038,1,52461,"NG","IC" 32,18,5,2,2,669,10,"RICHMOND (CITY OF)","WHITEWATER",0,"LIGHT OIL",15989,"0M",1294,,,95,66,135,651,4,9,642,11,23,618,36,75,544,43,89,455,36,75,380,33,65,315,24,51,800,38,79,721,40,84,637,125,241,754,33,67,866,1040,1,52479,"FO2","ST" 32,18,5,2,6,669,10,"RICHMOND (CITY OF)","WHITEWATER",0,"BIT COAL",15989,"0M",1294,,,95,52567,26931,66546,54464,27521,59857,50869,26046,61570,37981,19323,61813,34761,18221,70185,50812,25880,63189,54367,27836,58351,55464,28592,56536,47367,24058,57432,31433,16236,61431,49216,24827,57518,55122,27935,65411,1040,1,52479,"BIT","ST" 32,18,8,2,2,849,5,"HOOSIER ENERGY RURAL","RATTS",0,"LIGHT OIL",9267,"0M",1294,,,95,36,63,331,24,42,427,57,99,328,82,143,185,157,271,264,220,383,175,69,123,225,64,116,273,67,119,314,72,130,300,169,298,360,213,374,345,1043,1,51339,"FO2","ST" 32,18,8,2,6,849,5,"HOOSIER ENERGY RURAL","RATTS",0,"BIT COAL",9267,"0M",1294,,,95,152672,68804,12521,138850,61631,20613,120820,54271,33350,149240,67046,34059,138601,62960,37387,104185,47642,37604,152193,70371,29049,149047,69157,33970,133611,61143,30823,84154,38731,32856,131727,59094,30160,146986,66592,32432,1043,1,51339,"BIT","ST" 32,18,8,2,2,849,10,"HOOSIER ENERGY RURAL","MEROM",0,"LIGHT OIL",9267,"0M",1294,,,95,195,354,6014,19,38,10415,677,1227,9188,41,76,9112,1799,3447,5664,1764,3378,7059,771,1387,5672,508,946,4725,1207,2219,7281,584,1062,6218,468,838,10208,592,1063,9145,6213,1,51339,"FO2","ST" 32,18,8,2,6,849,10,"HOOSIER ENERGY RURAL","MEROM",0,"BIT COAL",9267,"0M",1294,,,95,462676,222254,448322,417644,215416,460946,384780,184640,471566,246060,116767,519358,230592,116155,570294,429927,213604,544280,462605,221660,492415,499492,244053,429843,353022,171326,433018,376476,178855,429945,480027,227666,396833,503880,236844,364841,6213,1,51339,"BIT","ST" 32,18,9,4,2,900,5,"INDIANA MUN POWER AGENCY","ANDERSON",0,"LIGHT OIL",9234,"0M",1294,,,95,19,44,5010,33,68,4942,40,82,4860,14,24,4835,7,12,4824,25,62,4762,0,1,4761,1,4,4757,0,0,4757,14,27,4730,3,9,4721,10,13,4708,7336,1,19234,"FO2","GT" 32,18,9,4,9,900,5,"INDIANA MUN POWER AGENCY","ANDERSON",0,"NAT GAS",9234,"0M",1294,,,95,53,772,0,54,717,0,199,2578,0,66,914,0,31,416,0,481,7593,0,2482,36348,0,6354,89340,0,94,1557,0,64,1343,0,36,450,0,47,750,0,7336,1,19234,"NG","GT" 33,17,1,2,2,29,5,"CENTRAL ILLINOIS LIGHT CO","E D EDWARDS",0,"LIGHT OIL",3252,"0M",1294,,,95,580,979,551,369,645,642,581,1050,511,539,979,621,777,1362,571,696,1201,688,793,1392,574,425,792,507,571,980,634,610,991,501,329,558,506,455,759,491,856,4,50485,"FO2","ST" 33,17,1,2,6,29,5,"CENTRAL ILLINOIS LIGHT CO","E D EDWARDS",0,"BIT COAL",3252,"0M",1294,,,95,278723,111505,170727,240983,94522,156151,283715,115017,142278,219332,90164,180893,314512,130292,145461,303524,124741,120263,294912,127410,143742,416665,181855,115286,215994,93604,136103,343831,139588,97044,284797,118784,138306,257830,101322,144327,856,4,50485,"BIT","ST" 33,17,1,4,9,29,12,"CENTRAL ILLINOIS LIGHT CO","STERLING AV",0,"NAT GAS",3252,"0M",1294,,,95,91,1361,0,30,486,0,29,443,0,29,495,0,28,483,0,114,1973,0,236,4614,0,495,8477,0,62,1057,0,60,926,0,32,555,0,79,1259,0,860,4,50485,"NG","GT" 33,17,1,2,2,29,20,"CENTRAL ILLINOIS LIGHT CO","DUCK CREEK",0,"LIGHT OIL",3252,"0M",1294,,,95,464,794,607,155,264,573,38,67,506,39,69,437,368,658,640,47,83,557,76,135,598,252,429,597,203,353,523,461,865,374,191,334,581,221,383,548,6016,4,50485,"FO2","ST" 33,17,1,2,6,29,20,"CENTRAL ILLINOIS LIGHT CO","DUCK CREEK",0,"BIT COAL",3252,"0M",1294,,,95,186107,88236,146013,184996,85972,174445,212342,99989,207941,178133,85191,199728,101736,49494,191824,209741,99840,163763,218825,104416,121412,182815,87426,161492,205874,98086,126656,49432,25199,182072,221479,104789,147984,208001,98018,120664,6016,4,50485,"BIT","ST" 33,17,1,2,9,29,25,"CENTRAL ILLINOIS LIGHT CO","MIDWEST GRN",0,"NAT GAS",3252,"0M",694,"A",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1987,12379,0,4809,36302,0,4873,33446,0,2693,19047,0,0,0,0,3046,22292,0,4051,25863,0,7384,4,50485,"NG","ST" 33,17,1,2,2,32,2,"CENTRAL ILL PUBLIC SER CO","COFFEEN",0,"LIGHT OIL",3253,"0M",1294,,,95,281,528,4129,159,291,4010,394,749,4105,523,1002,3949,771,1637,3876,506,903,4329,271,491,4241,39,71,3944,249,436,4034,521,930,3986,417,729,4572,962,1745,3927,861,4,50486,"FO2","ST" 33,17,1,2,6,32,2,"CENTRAL ILL PUBLIC SER CO","COFFEEN",0,"BIT COAL",3253,"0M",1294,,,95,365821,196265,250663,291393,151752,268915,248792,134522,254062,79012,43562,287270,49602,29698,377234,331239,171527,392358,397070,207104,345747,370867,195382,346249,139189,69530,387149,251535,126615,387760,291764,143554,406398,266300,137380,362886,861,4,50486,"BIT","ST" 33,17,1,2,2,32,5,"CENTRAL ILL PUBLIC SER CO","GRAND TOWER",0,"LIGHT OIL",3253,"0M",1294,,,95,146,294,559,222,423,494,139,267,578,60,171,742,-59,75,667,310,600,753,324,626,481,405,753,769,154,287,834,78,162,672,389,761,607,217,428,533,862,4,50486,"FO2","ST" 33,17,1,2,6,32,5,"CENTRAL ILL PUBLIC SER CO","GRAND TOWER",0,"BIT COAL",3253,"0M",1294,,,95,19817,10029,48685,18173,8634,59296,12650,6089,70908,3933,2772,73473,-503,161,78207,17238,8399,74696,44644,21400,58784,77238,35607,26412,11609,5363,31994,11150,5893,34133,57466,27803,19044,47800,23991,32368,862,4,50486,"BIT","ST" 33,17,1,2,2,32,10,"CENTRAL ILL PUBLIC SER CO","HUTSONVILLE",0,"LIGHT OIL",3253,"0M",1294,,,95,72,148,1592,254,501,1092,252,532,1126,117,284,1556,421,883,1560,398,781,1662,440,832,1760,236,429,1331,196,323,1008,158,382,1338,346,655,1437,140,264,1173,863,4,50486,"FO2","ST" 33,17,1,2,6,32,10,"CENTRAL ILL PUBLIC SER CO","HUTSONVILLE",0,"BIT COAL",3253,"0M",1294,,,95,17493,9580,55605,13103,6803,61393,11330,6319,65444,3457,2220,70186,6929,4012,73260,18641,9997,71065,43752,22295,48771,75386,37255,19363,5801,2524,33120,7107,4480,39773,44924,22754,26665,48938,24435,23714,863,4,50486,"BIT","ST" 33,17,1,3,2,32,10,"CENTRAL ILL PUBLIC SER CO","HUTSONVILLE",0,"LIGHT OIL",3253,"0M",1294,,,95,5,10,124,0,0,126,0,0,130,5,9,121,5,9,106,0,0,106,15,30,72,10,21,233,0,0,229,0,0,228,5,9,225,0,0,227,863,4,50486,"FO2","IC" 33,17,1,2,2,32,15,"CENTRAL ILL PUBLIC SER CO","MEREDOSIA",0,"LIGHT OIL",3253,"0M",1294,,,95,276,524,1245,240,455,1295,109,257,1541,576,1050,1518,264,464,1396,272,471,1722,478,864,1170,665,1188,1390,137,250,1672,104,202,1469,-609,0,1671,636,1140,1388,864,4,50486,"FO2","ST" 33,17,1,2,3,32,15,"CENTRAL ILL PUBLIC SER CO","MEREDOSIA",0,"HEAVY OIL",3253,"0M",1294,,,95,-878,0,41246,-869,0,41246,-953,0,41246,-789,0,41246,-6,0,41246,1105,5986,35342,1753,6017,29342,6547,17169,22153,-808,333,23977,-646,0,42084,996,1890,42084,-711,0,42084,864,4,50486,"FO6","ST" 33,17,1,2,6,32,15,"CENTRAL ILL PUBLIC SER CO","MEREDOSIA",0,"BIT COAL",3253,"0M",1294,,,95,66774,32586,105182,41839,21008,131939,15303,9402,148998,70146,32222,148546,91295,40883,144840,111244,50699,134953,137571,64325,109649,184516,85228,55561,77698,37291,62196,86881,43240,73623,78143,41045,82454,97009,48373,93368,864,4,50486,"BIT","ST" 33,17,1,2,2,32,20,"CENTRAL ILL PUBLIC SER CO","NEWTON",0,"LIGHT OIL",3253,"0M",1294,,,95,844,1577,4500,512,956,5160,1182,2043,4716,553,984,5869,379,679,5723,681,1231,5199,190,328,5578,942,1748,4784,746,1331,5217,282,508,5420,60,105,5315,649,3661,4337,6017,4,50486,"FO2","ST" 33,17,1,2,6,32,20,"CENTRAL ILL PUBLIC SER CO","NEWTON",0,"BIT COAL",3253,"0M",1294,,,95,556271,262272,366063,518547,246265,373901,546762,245831,417351,503402,237591,446819,516641,244361,536330,468640,219703,623301,560024,252360,476964,466441,225593,612105,491641,228921,632582,454181,204761,666122,359030,160358,746315,378431,180592,722338,6017,4,50486,"BIT","ST" 33,17,1,1,,41,1,"COMMONWEALTH EDISON CO","DIXON",0,,4110,"0M",1294,,100,95,1217,0,0,1001,0,0,1400,0,0,1473,0,0,1443,0,0,1109,0,0,1264,0,0,1341,0,0,1211,0,0,1365,0,0,1603,0,0,1067,0,0,868,4,50643,"WAT","HY" 33,17,1,2,1,41,1,"COMMONWEALTH EDISON CO","QUAD CITIES",0,"NUCLEAR",4110,"0M",1294,,100,95,265985,0,0,516483,0,0,563772,0,0,556271,0,0,570166,0,0,541658,0,0,537742,0,0,552522,0,0,533277,0,0,383182,0,0,293985,0,0,571167,0,0,880,4,50643,"UR","ST" 33,17,1,2,1,41,1,"COMMONWEALTH EDISON CO","BRAIDWOOD",0,"NUCLEAR",4110,"0M",1294,,100,95,845089,0,0,487988,0,0,443133,0,0,527594,0,0,838888,0,0,802928,0,0,825056,0,0,825520,0,0,701927,0,0,-9715,0,0,-10027,0,0,307159,0,0,6022,4,50643,"UR","ST" 33,17,1,2,1,41,1,"COMMONWEALTH EDISON CO","BYRON",0,"NUCLEAR",4110,"0M",1294,,100,95,766116,0,0,735235,0,0,817602,0,0,779568,0,0,804172,0,0,742334,0,0,790248,0,0,800198,0,0,786058,0,0,542611,0,0,-9310,0,0,142399,0,0,6023,4,50643,"UR","ST" 33,17,1,2,1,41,1,"COMMONWEALTH EDISON CO","LASALLE CTY",0,"NUCLEAR",4110,"0M",1294,,100,95,813809,0,0,531418,0,0,813835,0,0,788528,0,0,782478,0,0,561931,0,0,750639,0,0,609485,0,0,617973,0,0,773354,0,0,684375,0,0,641459,0,0,6026,4,50643,"UR","ST" 33,17,1,2,1,41,1,"COMMONWEALTH EDISON CO","ZION",0,"NUCLEAR",4110,"0M",1294,,100,95,777628,0,0,706122,0,0,778794,0,0,744367,0,0,679639,0,0,751346,0,0,778214,0,0,771971,0,0,190946,0,0,-8633,0,0,-8349,0,0,290089,0,0,885,4,50643,"UR","ST" 33,17,1,2,1,41,2,"COMMONWEALTH EDISON CO","ZION",0,"NUCLEAR",4110,"0M",1294,,100,95,62829,0,0,-7517,0,0,-8823,0,0,214602,0,0,763695,0,0,707962,0,0,768388,0,0,745403,0,0,742149,0,0,737928,0,0,708434,0,0,471011,0,0,885,4,50643,"UR","ST" 33,17,1,2,1,41,2,"COMMONWEALTH EDISON CO","LASALLE CTY",0,"NUCLEAR",4110,"0M",1294,,100,95,805795,0,0,433271,0,0,-8184,0,0,-8016,0,0,-8927,0,0,375943,0,0,773928,0,0,744199,0,0,446327,0,0,816638,0,0,792434,0,0,804502,0,0,6026,4,50643,"UR","ST" 33,17,1,2,1,41,2,"COMMONWEALTH EDISON CO","BYRON",0,"NUCLEAR",4110,"0M",1294,,100,95,753651,0,0,166639,0,0,50362,0,0,767250,0,0,824285,0,0,786866,0,0,797334,0,0,811901,0,0,764206,0,0,832898,0,0,804540,0,0,823838,0,0,6023,4,50643,"UR","ST" 33,17,1,2,1,41,2,"COMMONWEALTH EDISON CO","BRAIDWOOD",0,"NUCLEAR",4110,"0M",1294,,100,95,839335,0,0,759006,0,0,840028,0,0,777131,0,0,635751,0,0,794146,0,0,802182,0,0,795885,0,0,801537,0,0,846700,0,0,810185,0,0,831152,0,0,6022,4,50643,"UR","ST" 33,17,1,2,1,41,2,"COMMONWEALTH EDISON CO","QUAD CITIES",0,"NUCLEAR",4110,"0M",1294,,100,95,501116,0,0,453211,0,0,58157,0,0,-5752,0,0,-5952,0,0,-5994,0,0,-6618,0,0,93771,0,0,422180,0,0,318808,0,0,77988,0,0,571746,0,0,880,4,50643,"UR","ST" 33,17,1,2,1,41,2,"COMMONWEALTH EDISON CO","DRESDEN",0,"NUCLEAR",4110,"0M",1294,,100,95,535595,0,0,493244,0,0,81638,0,0,302574,0,0,449851,0,0,27639,0,0,-3615,0,0,-4287,0,0,-5566,0,0,-5704,0,0,-5672,0,0,-5963,0,0,869,4,50643,"UR","ST" 33,17,1,2,1,41,3,"COMMONWEALTH EDISON CO","DRESDEN",0,"NUCLEAR",4110,"0M",1294,,100,95,420814,0,0,506779,0,0,533907,0,0,467390,0,0,432429,0,0,-5060,0,0,-3401,0,0,-3807,0,0,41448,0,0,138092,0,0,358426,0,0,577978,0,0,869,4,50643,"UR","ST" 33,17,1,4,2,41,4,"COMMONWEALTH EDISON CO","BLOOM",0,"LIGHT OIL",4110,"0M",1294,,100,95,0,0,15589,0,0,15589,69,87,15502,0,0,15495,0,0,15495,0,0,15475,146,497,14951,792,2784,12167,0,0,15755,0,0,15755,0,0,15755,1,3,15739,865,4,50643,"FO2","GT" 33,17,1,4,2,41,6,"COMMONWEALTH EDISON CO","CALUMET",0,"LIGHT OIL",4110,"0M",1294,,100,95,0,0,16437,0,0,16437,0,0,16437,145,127,16310,0,0,16310,0,0,16310,593,2028,14281,508,1365,12917,0,0,15298,0,0,15298,0,0,15298,0,0,15298,866,4,50643,"FO2","GT" 33,17,1,4,9,41,6,"COMMONWEALTH EDISON CO","CALUMET",0,"NAT GAS",4110,"0M",1294,,100,95,0,0,0,68,1045,0,0,8,0,0,0,0,62,540,0,0,0,0,2902,56071,0,3743,56299,0,1,46,0,106,1474,0,29,760,0,0,0,0,866,4,50643,"NG","GT" 33,17,1,2,6,41,10,"COMMONWEALTH EDISON CO","CRAWFORD",0,"BIT COAL",4110,"0M",1294,,100,95,79127,52566,254284,56492,34236,247898,154770,96060,204338,157819,95401,178999,77964,50034,154295,195593,125311,78949,167051,106642,75986,220876,140947,52693,111791,74002,178401,100936,63677,173394,171688,108863,144620,107184,68961,169485,867,4,50643,"BIT","ST" 33,17,1,2,9,41,10,"COMMONWEALTH EDISON CO","CRAWFORD",0,"NAT GAS",4110,"0M",1294,,100,95,4191,46278,0,3822,41541,0,6151,66002,0,6881,74296,0,3205,34575,0,3676,39819,0,4307,47007,0,11765,128609,0,2943,33297,0,3202,34374,0,2534,27690,0,3684,42386,0,867,4,50643,"NG","ST" 33,17,1,4,2,41,10,"COMMONWEALTH EDISON CO","CRAWFORD",0,"LIGHT OIL",4110,"0M",1294,,100,95,39,239,11718,31,208,15427,7,85,15342,60,196,15146,0,0,15146,145,654,14492,207,1709,12783,90,287,12496,0,0,12495,0,0,12495,5,41,12453,0,0,12451,867,4,50643,"FO2","GT" 33,17,1,4,9,41,10,"COMMONWEALTH EDISON CO","CRAWFORD",0,"NAT GAS",4110,"0M",1294,,100,95,99,3367,0,462,10721,0,90,6128,0,496,8920,0,41,832,0,2338,60078,0,1956,92769,0,6353,117178,0,232,23469,0,130,22477,0,606,26280,0,716,38106,0,867,4,50643,"NG","GT" 33,17,1,2,2,41,16,"COMMONWEALTH EDISON CO","JOLIET",0,"LIGHT OIL",4110,"0M",1294,,100,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,874,4,50643,"FO2","ST" 33,17,1,2,6,41,16,"COMMONWEALTH EDISON CO","JOLIET",0,"BIT COAL",4110,"0M",1294,,100,95,122495,69041,120326,93234,54624,109729,118689,69742,107396,119799,68307,78398,7077,4459,86216,111744,65001,89393,128830,75618,81101,97034,56642,114450,105402,58755,119892,105052,56846,73967,38927,23143,87158,80786,46625,136310,874,4,50643,"BIT","ST" 33,17,1,2,9,41,16,"COMMONWEALTH EDISON CO","JOLIET",0,"NAT GAS",4110,"0M",1294,,100,95,2191,22095,0,1467,15220,0,2310,24340,0,2244,23500,0,166,1970,0,2208,24000,0,2239,22730,0,1106,11930,0,1732,18230,0,1439,14430,0,1402,15430,0,1598,17620,0,874,4,50643,"NG","ST" 33,17,1,3,2,41,16,"COMMONWEALTH EDISON CO","JOLIET",0,"LIGHT OIL",4110,"0M",1294,,100,95,28,24,0,19,36,0,26,24,0,38,121,0,42,65,0,45,88,0,191,342,0,177,323,0,43,60,8,25,36,0,50,114,0,33,48,0,874,4,50643,"FO2","IC" 33,17,1,4,2,41,16,"COMMONWEALTH EDISON CO","JOLIET",0,"LIGHT OIL",4110,"0M",1294,,100,95,0,0,12982,0,0,12946,0,0,13461,0,0,13339,0,0,11260,0,0,11071,56,101,11058,0,0,11182,0,0,11123,0,0,11087,0,0,11349,0,0,11301,874,4,50643,"FO2","GT" 33,17,1,4,9,41,16,"COMMONWEALTH EDISON CO","JOLIET",0,"NAT GAS",4110,"0M",1294,,100,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1395,27871,0,8945,90787,0,8183,223338,0,866,13196,0,229,3746,0,131,5138,0,234,3377,0,874,4,50643,"NG","GT" 33,17,1,2,2,41,17,"COMMONWEALTH EDISON CO","JOLIET 7&8",0,"LIGHT OIL",4110,"0M",1294,,100,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,384,4,50643,"FO2","ST" 33,17,1,2,6,41,17,"COMMONWEALTH EDISON CO","JOLIET 7&8",0,"BIT COAL",4110,"0M",1294,,100,95,520241,284540,251012,441016,243169,314690,475210,271066,278538,286729,169187,274394,417122,253105,368822,380291,234398,349806,434794,265270,338716,502962,304953,251022,375036,226403,245187,274949,166801,229512,204177,119561,295972,195022,118007,392005,384,4,50643,"BIT","ST" 33,17,1,2,9,41,17,"COMMONWEALTH EDISON CO","JOLIET 7&8",0,"NAT GAS",4110,"0M",1294,,100,95,11103,108953,0,8750,87209,0,12754,127880,0,12398,126498,0,15389,159604,0,14468,153070,0,34003,358096,0,38820,399592,0,12449,130392,0,5845,61103,0,9664,99401,0,15109,163833,0,384,4,50643,"NG","ST" 33,17,1,2,2,41,18,"COMMONWEALTH EDISON CO","KINCAID",0,"LIGHT OIL",4110,"0M",1294,,100,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,876,4,50643,"FO2","ST" 33,17,1,2,6,41,18,"COMMONWEALTH EDISON CO","KINCAID",0,"BIT COAL",4110,"0M",1294,,100,95,55770,32758,306574,225554,110119,355485,177700,87847,323621,111716,54633,362527,59730,40786,398523,326434,167542,321546,302831,139901,261736,370353,171207,168914,152028,76179,217203,146493,75067,252142,105685,62572,325669,303394,153078,287687,876,4,50643,"BIT","ST" 33,17,1,2,9,41,18,"COMMONWEALTH EDISON CO","KINCAID",0,"NAT GAS",4110,"0M",1294,,100,95,1202,16174,0,747,8607,0,913,10721,0,996,11458,0,1078,14934,0,450,5024,0,586,6470,0,981,10590,0,742,8548,0,1541,18276,0,2200,30312,0,917,10402,0,876,4,50643,"NG","ST" 33,17,1,4,2,41,19,"COMMONWEALTH EDISON CO","LOMBARD",0,"LIGHT OIL",4110,"0M",1294,,100,95,0,0,16204,0,0,16203,0,2,15828,0,0,15828,0,0,15471,0,0,15471,0,0,15471,0,0,15471,0,0,15471,0,0,15471,0,0,15471,0,0,15471,877,4,50643,"FO2","GT" 33,17,1,4,9,41,19,"COMMONWEALTH EDISON CO","LOMBARD",0,"NAT GAS",4110,"0M",1294,,100,95,0,0,0,0,0,0,216,9440,0,28,3677,0,45,1042,0,1545,52076,0,2695,90228,0,4011,66015,0,277,4570,0,110,2620,0,70,1556,0,6,1352,0,877,4,50643,"NG","GT" 33,17,1,4,2,41,22,"COMMONWEALTH EDISON CO","EL JUNCTION",0,"LIGHT OIL",4110,"0M",1294,,100,95,0,0,16029,0,0,16029,0,0,16029,0,0,16029,0,0,16029,0,0,16029,0,0,16029,0,0,16029,0,0,16029,0,0,16029,0,0,16029,0,0,16029,870,4,50643,"FO2","GT" 33,17,1,4,9,41,22,"COMMONWEALTH EDISON CO","EL JUNCTION",0,"NAT GAS",4110,"0M",1294,,100,95,45,1465,0,255,9385,0,433,17490,0,266,17646,0,201,1306,0,3974,165292,0,3141,117346,0,6577,120875,0,317,6236,0,0,0,0,0,0,0,0,0,0,870,4,50643,"NG","GT" 33,17,1,2,2,41,25,"COMMONWEALTH EDISON CO","POWERTON",0,"LIGHT OIL",4110,"0M",1294,,100,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,879,4,50643,"FO2","ST" 33,17,1,2,6,41,25,"COMMONWEALTH EDISON CO","POWERTON",0,"BIT COAL",4110,"0M",1294,,100,95,295687,209649,423935,447158,294017,440451,348046,239570,435308,212232,137447,636432,150582,105273,808681,358461,251527,710182,600064,381559,542202,449473,321219,483261,473891,314575,379942,711307,426764,426047,347462,223314,654319,369211,237119,790527,879,4,50643,"BIT","ST" 33,17,1,2,9,41,25,"COMMONWEALTH EDISON CO","POWERTON",0,"NAT GAS",4110,"0M",1294,,100,95,2163,27135,0,934,10806,0,1060,12568,0,352,4015,0,411,4960,0,1912,23178,0,1304,14277,0,344,4172,0,2982,34612,0,1175,12623,0,1089,12285,0,860,10186,0,879,4,50643,"NG","ST" 33,17,1,4,2,41,34,"COMMONWEALTH EDISON CO","SABROOKE",0,"LIGHT OIL",4110,"0M",1294,,100,95,0,0,10453,0,0,10453,0,0,10453,0,0,10453,0,0,10453,1060,4114,11113,2120,6610,10937,3819,12030,8749,0,0,10491,0,0,10491,92,332,10159,19,57,10102,882,4,50643,"FO2","GT" 33,17,1,2,6,41,35,"COMMONWEALTH EDISON CO","FISK ST",0,"BIT COAL",4110,"0M",1294,,100,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,1258,2813,0,64730,37523,0,49452,31868,0,82828,51049,0,0,0,0,0,0,0,886,4,50643,"BIT","ST" 33,17,1,2,9,41,35,"COMMONWEALTH EDISON CO","FISK ST",0,"NAT GAS",4110,"0M",1294,,100,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,950,35700,0,6315,65190,0,4278,50522,0,3262,35967,0,0,0,0,0,0,0,886,4,50643,"NG","ST" 33,17,1,3,2,41,35,"COMMONWEALTH EDISON CO","FISK ST",0,"LIGHT OIL",4110,"0M",1294,,100,95,45,155,416,0,0,416,77,84,332,39,37,295,68,30,266,66,86,180,134,219,491,125,84,407,40,16,391,17,100,291,19,95,196,0,0,174,886,4,50643,"FO2","IC" 33,17,1,4,2,41,35,"COMMONWEALTH EDISON CO","FISK ST",0,"LIGHT OIL",4110,"0M",1294,,100,95,1,5,23532,47,93,23145,99,257,23261,297,889,22373,31,91,22630,3411,9368,21922,4887,12963,23223,4869,20375,20364,0,0,20364,0,0,20364,335,1236,19127,365,1339,17788,886,4,50643,"FO2","GT" 33,17,1,2,2,41,40,"COMMONWEALTH EDISON CO","WAUKEGAN",0,"LIGHT OIL",4110,"0M",1294,,100,95,895,1547,2815,3612,6129,2742,4931,8714,2873,777,1407,3668,959,1672,3660,3946,7104,2494,3955,7041,2217,5282,9737,2829,3119,5998,3784,2859,5228,2552,3518,6749,3529,1606,3513,2435,883,4,50643,"FO2","ST" 33,17,1,2,6,41,40,"COMMONWEALTH EDISON CO","WAUKEGAN",0,"BIT COAL",4110,"0M",1294,,100,95,297287,177180,273721,300831,175220,239888,317665,191650,286982,225455,141450,324935,256271,154756,392524,243529,150801,389581,310909,188184,335255,296518,187813,197729,119579,79260,209183,165704,104633,209690,128110,85584,284788,41660,30532,414595,883,4,50643,"BIT","ST" 33,17,1,2,9,41,40,"COMMONWEALTH EDISON CO","WAUKEGAN",0,"NAT GAS",4110,"0M",1294,,100,95,1435,14340,0,1745,16984,0,6345,64552,0,12306,127984,0,2631,26534,0,2700,27935,0,4475,45751,0,8173,86616,0,1604,17712,0,0,0,0,0,0,0,1606,20058,0,883,4,50643,"NG","ST" 33,17,1,4,2,41,40,"COMMONWEALTH EDISON CO","WAUKEGAN",0,"LIGHT OIL",4110,"0M",1294,,100,95,311,627,9084,81,252,8832,0,0,8832,62,220,8612,0,0,8612,2971,8993,7575,4093,8993,10099,3465,12846,8690,217,650,9693,15,46,9832,388,721,9111,455,101,8825,883,4,50643,"FO2","GT" 33,17,1,2,2,41,45,"COMMONWEALTH EDISON CO","WILL COUNTY",0,"LIGHT OIL",4110,"0M",1294,,100,95,1062,18762,3939,7295,13109,3758,10624,18496,3941,8221,14895,3199,9084,16531,4090,8920,16134,4050,10413,17507,4073,8717,15307,3888,6246,11354,3823,8028,14057,4581,13300,23039,4265,11454,20638,3742,884,4,50643,"FO2","ST" 33,17,1,2,6,41,45,"COMMONWEALTH EDISON CO","WILL COUNTY",0,"BIT COAL",4110,"0M",1294,,100,95,339333,214481,728644,276729,163281,493423,436182,242324,418178,363653,209416,394195,307990,182353,450891,397251,238256,419768,378522,212664,447725,475303,276214,354866,276771,166573,326404,319122,188012,314278,367545,210217,297641,236545,145482,315427,884,4,50643,"BIT","ST" 33,17,1,2,2,41,60,"COMMONWEALTH EDISON CO","COLLINS",0,"LIGHT OIL",4110,"0M",1294,,100,95,44,168,8953,149,398,8555,143,315,8240,46,189,8051,8,33,9226,37,94,9132,118,236,8896,161,333,8562,33,186,8376,121,346,8030,407,870,7160,418,907,6253,6025,4,50643,"FO2","ST" 33,17,1,2,3,41,60,"COMMONWEALTH EDISON CO","COLLINS",0,"HEAVY OIL",4110,"0M",1294,,100,95,10708,14958,858168,17136,41575,816594,22453,44431,829903,5094,19291,887973,1621,6324,924611,37801,79457,874073,46886,87834,814064,170809,316836,497228,8876,46988,565732,30191,78409,602644,60143,118667,704727,63549,126751,840744,6025,4,50643,"FO6","ST" 33,17,1,2,9,41,60,"COMMONWEALTH EDISON CO","COLLINS",0,"NAT GAS",4110,"0M",1294,,100,95,39831,890044,0,143526,2177150,0,287955,3565711,0,53575,1269470,0,42336,1034381,0,242662,3192054,0,342245,4012183,0,559661,6496563,0,22424,742913,0,72437,1176239,0,234867,2894481,0,189527,2361026,0,6025,4,50643,"NG","ST" 33,17,1,2,2,59,5,"ELECTRIC ENERGY INC","JOPPA STEAM",0,"LIGHT OIL",5748,"0M",1294,,,95,200,374,1123,39,70,1273,99,185,1072,621,1113,2510,355,632,917,223,421,1063,108,203,1046,324,609,1093,203,369,937,141,253,1041,23,42,874,163,297,1013,887,4,50877,"FO2","ST" 33,17,1,2,6,59,5,"ELECTRIC ENERGY INC","JOPPA STEAM",0,"BIT COAL",5748,"0M",1294,,,95,714619,413405,218343,620332,359921,257338,581511,352021,367649,615267,357331,494389,555217,326921,554836,664604,410139,566371,692201,431949,348896,616065,383985,389108,610216,368490,418929,705090,420489,495502,724030,433000,497231,719491,431637,526478,887,4,50877,"BIT","ST" 33,17,1,2,9,59,5,"ELECTRIC ENERGY INC","JOPPA STEAM",0,"NAT GAS",5748,"0M",1294,,,95,3,39,0,3,32,0,2,31,0,4,42,0,2,29,0,3,39,0,2,28,0,2,25,0,2,30,0,3,33,0,4,43,0,2,27,0,887,4,50877,"NG","ST" 33,17,1,2,1,72,1,"ILLINOIS POWER CO","CLINTON",0,"NUCLEAR",9208,"0M",1294,,,95,606581,0,0,556463,0,0,137066,0,0,-6903,0,0,405888,0,0,658164,0,0,673318,0,0,670862,0,0,558375,0,0,682367,0,0,659454,0,0,500645,0,0,204,4,51385,"UR","ST" 33,17,1,2,"C",72,20,"ILLINOIS POWER CO","BALDWIN",0,"TIRES",9208,"0M",294,"A",,95,0,0,0,1818,0,0,3181,0,0,7099,0,0,6807,0,0,5350,0,0,7244,0,0,3493,0,0,6277,0,0,7534,0,0,10681,0,0,7569,0,0,889,4,51385,"TIR","ST" 33,17,1,2,2,72,20,"ILLINOIS POWER CO","BALDWIN",0,"LIGHT OIL",9208,"0M",1294,,,95,1081,1918,2086,605,1061,2802,687,1177,4303,886,1546,2758,788,1102,2909,1035,1849,3333,1018,1819,2723,194,347,3603,519,926,3761,917,1661,2395,449,802,2830,719,1288,2830,889,4,51385,"FO2","ST" 33,17,1,2,6,72,20,"ILLINOIS POWER CO","BALDWIN",0,"BIT COAL",9208,"0M",1294,,,95,660540,312984,326606,560194,261218,347154,721218,332734,317839,1001149,461485,170294,940043,347817,194365,784737,373003,199111,952571,453263,98640,1114689,528001,10906,767993,364295,81430,684089,329233,150289,880194,419001,132828,809209,388865,132828,889,4,51385,"BIT","ST" 33,17,1,2,2,72,35,"ILLINOIS POWER CO","HAVANA",0,"LIGHT OIL",9208,"0M",1294,,,95,910,1948,1153,666,1365,840,307,580,1330,461,889,1682,716,1472,1237,733,1517,1451,606,1199,1513,905,1843,2122,693,1487,1847,988,1998,879,1035,1991,1192,678,1527,1192,891,4,51385,"FO2","ST" 33,17,1,2,3,72,35,"ILLINOIS POWER CO","HAVANA",0,"HEAVY OIL",9208,"0M",1294,,,95,0,0,11893,0,0,11893,0,0,11893,0,0,11893,0,0,11893,0,0,11893,0,0,11893,0,0,11893,0,0,11893,0,0,11893,0,0,362,0,0,362,891,4,51385,"FO6","ST" 33,17,1,2,6,72,35,"ILLINOIS POWER CO","HAVANA",0,"BIT COAL",9208,"0M",1294,,,95,98112,49256,30789,118979,58411,50159,224224,102634,40379,160060,74936,66818,118264,58880,70245,116146,58574,89918,115561,56674,118529,151230,75783,90549,71688,37378,112421,88892,44663,121996,115087,53793,99387,131730,71564,99387,891,4,51385,"BIT","ST" 33,17,1,2,9,72,35,"ILLINOIS POWER CO","HAVANA",0,"NAT GAS",9208,"0M",1294,,,95,1067,12979,0,440,5089,0,63,677,0,179,1951,0,351,4046,0,300,3543,0,463,5170,0,355,4086,0,402,4873,0,559,6392,0,891,9670,0,763,9698,0,891,4,51385,"NG","ST" 33,17,1,2,2,72,37,"ILLINOIS POWER CO","HENNEPIN",0,"LIGHT OIL",9208,"0M",1294,,,95,0,0,139,0,0,118,0,0,98,0,0,73,0,0,226,0,0,198,0,0,171,0,0,143,0,0,124,0,0,81,0,0,206,0,0,206,892,4,51385,"FO2","ST" 33,17,1,2,6,72,37,"ILLINOIS POWER CO","HENNEPIN",0,"BIT COAL",9208,"0M",1294,,,95,87360,41868,110995,113939,53993,91245,148496,70812,66931,128982,61958,52605,126965,61905,34055,114742,56218,13963,122662,60852,24745,143091,72106,29954,79631,39909,56695,59580,30905,81408,39508,20500,71977,116352,56957,71977,892,4,51385,"BIT","ST" 33,17,1,2,9,72,37,"ILLINOIS POWER CO","HENNEPIN",0,"NAT GAS",9208,"0M",1294,,,95,32318,326516,0,1234,12249,0,1222,12243,0,808,8187,0,416,4252,0,2050,20916,0,733,7579,0,551,5765,0,776,8044,0,87,951,0,169,1816,0,493,5034,0,892,4,51385,"NG","ST" 33,17,1,4,2,72,39,"ILLINOIS POWER CO","OGLESBY",0,"LIGHT OIL",9208,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,8629,0,0,8629,0,0,8629,0,0,8629,0,0,8629,0,0,8629,0,0,8629,0,0,8805,0,0,8805,894,4,51385,"FO2","GT" 33,17,1,4,9,72,39,"ILLINOIS POWER CO","OGLESBY",0,"NAT GAS",9208,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,2951,33996,0,2725,56764,0,0,0,0,110,1650,0,0,0,0,519,7497,0,894,4,51385,"NG","GT" 33,17,1,4,2,72,40,"ILLINOIS POWER CO","STALLINGS",0,"LIGHT OIL",9208,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,895,4,51385,"FO2","GT" 33,17,1,4,9,72,40,"ILLINOIS POWER CO","STALLINGS",0,"NAT GAS",9208,"0M",1294,,,95,-5,0,0,0,0,0,-188,0,0,-57,0,0,-40,0,0,-31,0,0,556,11621,0,1460,27572,0,-38,0,0,-159,0,0,0,0,0,40,1636,0,895,4,51385,"NG","GT" 33,17,1,2,2,72,45,"ILLINOIS POWER CO","VERMILION",0,"LIGHT OIL",9208,"0M",1294,,,95,115,249,624,91,198,602,191,417,364,236,549,361,18,38,279,0,0,257,0,0,333,0,0,327,0,0,327,0,0,284,0,0,284,0,0,284,897,4,51385,"FO2","ST" 33,17,1,2,6,72,45,"ILLINOIS POWER CO","VERMILION",0,"BIT COAL",9208,"0M",1294,,,95,30154,17048,27000,17324,9743,30113,23022,12947,17166,26005,15643,2483,5797,3221,2966,977,640,2326,0,0,2326,0,0,2326,0,0,2326,0,0,2326,-194,0,2326,0,0,2326,897,4,51385,"BIT","ST" 33,17,1,2,9,72,45,"ILLINOIS POWER CO","VERMILION",0,"NAT GAS",9208,"0M",794,"A",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,35157,523154,0,35815,280703,0,5530,63136,0,-181,425,0,0,0,0,0,0,0,897,4,51385,"NG","ST" 33,17,1,4,2,72,45,"ILLINOIS POWER CO","VERMILION",0,"LIGHT OIL",9208,"0M",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,-967,0,0,13,1679,0,0,0,0,0,0,0,897,4,51385,"FO2","GT" 33,17,1,2,"B",72,50,"ILLINOIS POWER CO","WOOD RIVER",0,"WOOD",9208,"0M",294,"A",,95,0,0,0,16,0,0,178,0,0,229,0,0,90,0,0,216,0,0,58,0,0,48,0,0,0,0,0,0,0,0,0,0,0,18,0,0,898,4,51385,"WD","ST" 33,17,1,2,2,72,50,"ILLINOIS POWER CO","WOOD RIVER",0,"LIGHT OIL",9208,"0M",1294,,,95,44,79,5600,23,43,5507,47,83,5347,40,74,5395,21,44,5332,24,48,5204,12,23,5294,49,90,5144,25,46,5028,38,67,5235,0,0,4820,0,0,4820,898,4,51385,"FO2","ST" 33,17,1,2,6,72,50,"ILLINOIS POWER CO","WOOD RIVER",0,"BIT COAL",9208,"0M",1294,,,95,179203,74998,45031,134748,57471,69498,189897,79401,76252,58215,25205,85871,13578,6765,84103,56995,25313,99570,176787,75799,113318,203949,86831,93346,141728,61520,85883,170165,70959,78358,166564,67877,95046,152328,67698,95046,898,4,51385,"BIT","ST" 33,17,1,2,9,72,50,"ILLINOIS POWER CO","WOOD RIVER",0,"NAT GAS",9208,"0M",1294,,,95,2917,29530,0,3161,32758,0,2112,21194,0,620,6474,0,455,5401,0,3940,43447,0,1042,11274,0,7813,79539,0,841,8463,0,2100,20806,0,1416,13732,0,3310,34114,0,898,4,51385,"NG","ST" 33,17,1,1,,76,5,"MIDAMERICAN ENERGY","MOLINE",0,,9438,"0M",1294,,50,95,867,0,0,502,0,0,693,0,0,501,0,0,751,0,0,1306,0,0,1909,0,0,1606,0,0,1628,0,0,1499,0,0,1295,0,0,824,0,0,899,5,51406,"WAT","HY" 33,17,1,4,2,76,5,"MIDAMERICAN ENERGY","MOLINE",0,"LIGHT OIL",9438,"0M",1294,,50,95,-104,1,1972,-89,0,1972,-80,0,1972,0,0,1972,0,0,1972,0,0,1972,0,0,1972,0,0,1972,-1,0,1972,-33,0,1972,-32,0,1972,-41,0,1972,899,5,51406,"FO2","GT" 33,17,1,4,9,76,5,"MIDAMERICAN ENERGY","MOLINE",0,"NAT GAS",9438,"0M",1294,,50,95,0,0,0,0,0,0,0,0,0,0,0,0,-61,2,0,1064,18944,0,1548,27660,0,1838,32171,0,-50,33,0,-34,0,0,-33,0,0,-42,0,0,899,5,51406,"NG","GT" 33,17,1,1,,107,1,"NATIONAL HYDRO","DAYTON",0,,9366,"0A",1294,,,95,1202,0,0,1122,0,0,1638,0,0,1567,0,0,992,0,0,1383,0,0,911,0,0,403,0,0,0,0,0,0,0,0,1259,0,0,1438,0,0,901,4,52081,"WAT","HY" 33,17,1,1,,134,1,"SO BELOIT WTR GAS & ELEC","ROCKTON",0,,17535,"0A",1294,,521,95,467,0,0,390,0,0,678,0,0,788,0,0,728,0,0,505,0,0,154,0,0,655,0,0,616,0,0,694,0,0,698,0,0,536,0,0,903,4,54026,"WAT","HY" 33,17,1,2,2,151,15,"UNION ELECTRIC CO","VENICE",0,"LIGHT OIL",19436,"0M",1294,,150,95,-14,55,40501,-148,624,39877,0,0,39877,0,0,39877,1716,6693,33184,1509,6175,27009,165,558,26451,1421,5295,29829,0,0,33009,0,0,33009,63,822,32186,-598,1970,30216,913,4,52997,"FO2","ST" 33,17,1,2,9,151,15,"UNION ELECTRIC CO","VENICE",0,"NAT GAS",19436,"0M",1294,,150,95,-1037,23078,0,-714,17082,0,745,29759,0,2615,70964,0,3881,85875,0,3694,85747,0,12175,233282,0,18970,400955,0,1254,9297,0,1125,26918,0,146,10894,0,-478,8990,0,913,4,52997,"NG","ST" 33,17,1,4,2,151,15,"UNION ELECTRIC CO","VENICE",0,"LIGHT OIL",19436,"0M",1294,,150,95,-67,27,1614,-28,163,2000,-35,94,1906,-28,27,1879,-20,89,1790,-20,0,1790,170,758,2114,425,1509,1672,-19,2,1670,-26,4,1666,-54,3,1664,-53,1,1663,913,4,52997,"FO2","GT" 33,17,5,2,2,528,1,"BREESE (CITY OF)","BREESE",0,"LIGHT OIL",2188,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,934,4,50322,"FO2","ST" 33,17,5,3,2,528,1,"BREESE (CITY OF)","BREESE",0,"LIGHT OIL",2188,"0A",1294,,,95,0,54,940,18,32,905,18,33,866,22,40,817,30,30,781,17,32,740,176,328,755,261,482,780,19,35,911,19,35,872,19,34,835,13,22,811,934,4,50322,"FO2","IC" 33,17,5,3,9,528,1,"BREESE (CITY OF)","BREESE",0,"NAT GAS",2188,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,934,4,50322,"NG","IC" 33,17,5,3,2,530,1,"BUSHNELL (CITY OF)","BUSHNELL",0,"LIGHT OIL",2634,"0A",1294,,,95,0,1,838,7,14,824,0,0,824,0,0,824,0,0,824,0,0,824,29,58,766,0,0,766,0,0,766,0,0,766,0,0,766,0,0,766,935,4,50383,"FO2","IC" 33,17,5,3,9,530,1,"BUSHNELL (CITY OF)","BUSHNELL",0,"NAT GAS",2634,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,935,4,50383,"NG","IC" 33,17,5,3,2,534,1,"CARLYLE (CITY OF)","CARLYLE",0,"LIGHT OIL",3037,"0A",1294,,,95,12,16,176,0,13,163,9,11,151,9,13,138,12,10,121,51,53,404,141,155,248,144,203,381,11,12,368,10,17,351,11,18,333,0,0,333,936,4,50438,"FO2","IC" 33,17,5,3,9,534,1,"CARLYLE (CITY OF)","CARLYLE",0,"NAT GAS",3037,"0A",1294,,,95,0,3,0,0,2,0,0,2,0,0,3,0,0,3,0,1,11,0,10,64,0,4,38,0,0,6,0,0,6,0,0,0,0,0,0,0,936,4,50438,"NG","IC" 33,17,5,3,2,537,1,"CARMI (CITY OF)","CARMI",0,"LIGHT OIL",3040,"0A",1294,,,95,16,38,765,95,45,720,10,19,700,7,19,681,5,21,660,5,32,627,5,12,616,9,15,600,18,53,722,9,20,702,10,22,702,61,90,590,937,4,50440,"FO2","IC" 33,17,5,3,9,537,1,"CARMI (CITY OF)","CARMI",0,"NAT GAS",3040,"0A",1294,,,95,70,720,0,25,1014,0,15,177,0,17,350,0,16,125,0,26,162,0,15,157,0,11,87,0,40,313,0,11,92,0,8,100,0,83,985,0,937,4,50440,"NG","IC" 33,17,5,2,6,559,1,"FAIRFIELD (CITY OF)","FAIRFIELD",0,"BIT COAL",6141,"0A",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,940,4,50941,"BIT","ST" 33,17,5,3,2,559,1,"FAIRFIELD (CITY OF)","FAIRFIELD",0,"LIGHT OIL",6141,"0A",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,940,4,50941,"FO2","IC" 33,17,5,3,9,559,1,"FAIRFIELD (CITY OF)","FAIRFIELD",0,"NAT GAS",6141,"0A",1294,"S",,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,940,4,50941,"NG","IC" 33,17,5,3,2,562,1,"FARMER (CITY OF)","FARMER CITY",0,"LIGHT OIL",6192,"0A",1294,,,95,1,3,227,0,0,227,0,0,227,0,0,227,1,2,230,10,20,208,7,23,186,38,71,283,4,4,279,0,0,279,0,0,274,0,0,274,941,4,50955,"FO2","IC" 33,17,5,3,9,562,1,"FARMER (CITY OF)","FARMER CITY",0,"NAT GAS",6192,"0A",1294,,,95,3,26,0,0,0,0,0,0,0,0,0,0,6,58,0,46,504,0,0,0,0,163,1723,0,0,0,0,0,0,0,0,0,0,0,0,0,941,4,50955,"NG","IC" 33,17,5,3,2,571,1,"FREEBURG (CITY OF)","FREEBURG",0,"LIGHT OIL",6764,"0A",1294,,,95,1,2,129,17,33,214,173,298,93,12,23,70,12,23,47,13,26,197,81,158,39,110,201,200,13,177,0,8,16,161,8,10,151,8,21,130,943,4,51056,"FO2","IC" 33,17,5,3,9,571,1,"FREEBURG (CITY OF)","FREEBURG",0,"NAT GAS",6764,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,943,4,51056,"NG","IC" 33,17,5,3,2,574,1,"GENESEO (CITY OF)","GENESEO",0,"LIGHT OIL",7095,"0A",1294,,,95,2,16,314,4,11,301,0,13,290,5,13,281,0,0,294,15,26,446,65,111,339,78,133,383,0,0,389,0,0,388,0,0,389,2,4,385,944,4,51093,"FO2","IC" 33,17,5,3,9,574,1,"GENESEO (CITY OF)","GENESEO",0,"NAT GAS",7095,"0A",1294,,,95,7,250,0,2,57,0,7,527,0,2,52,0,0,0,0,93,1716,0,562,6490,0,735,8338,0,0,0,0,0,0,0,0,0,0,0,1,0,944,4,51093,"NG","IC" 33,17,5,3,2,589,1,"HIGHLAND (CITY OF)","HIGHLAND",0,"LIGHT OIL",8573,"0A",1294,,,95,21,37,490,4,5,486,0,0,486,4,9,823,0,0,825,47,78,792,28,140,634,472,536,371,24,46,371,0,0,322,11,21,755,8,15,754,946,4,51298,"FO2","IC" 33,17,5,3,9,589,1,"HIGHLAND (CITY OF)","HIGHLAND",0,"NAT GAS",8573,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,946,4,51298,"NG","IC" 33,17,5,3,2,606,15,"MCLEANSBORO (CITY OF)","MCLEANSBORO",0,"LIGHT OIL",12167,"0A",1294,,,95,19,48,201,15,25,176,12,30,322,14,21,301,14,29,272,11,29,243,22,38,205,14,48,336,43,88,246,25,45,201,27,51,325,20,34,291,948,4,51812,"FO2","IC" 33,17,5,3,2,612,10,"MASCOUTAH (CITY OF)","MASCOUTAH",0,"LIGHT OIL",11790,"0A",1294,,,95,0,0,815,0,0,815,0,0,814,1,12,803,24,59,563,0,0,563,4,56,859,30,64,967,0,0,967,0,0,967,0,0,965,0,0,966,950,4,51789,"FO2","IC" 33,17,5,3,9,612,10,"MASCOUTAH (CITY OF)","MASCOUTAH",0,"NAT GAS",11790,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,10,410,0,0,0,0,0,0,0,74,4890,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,950,4,51789,"NG","IC" 33,17,5,2,9,646,1,"PERU (CITY OF)","PERU",0,"NAT GAS",14840,"0M",1294,,,95,-15,0,0,-11,0,0,4,0,0,-13,0,0,-7,0,0,77,680,0,-9,0,0,-62,0,0,0,0,0,8,0,0,0,0,0,0,0,0,955,4,52299,"NG","ST" 33,17,5,3,2,646,1,"PERU (CITY OF)","PERU",0,"LIGHT OIL",14840,"0M",1294,,,95,-30,12,619,-13,24,595,-13,23,572,-6,24,548,-2,23,525,63,146,560,189,366,550,299,560,533,-14,0,533,-1,23,510,-22,12,498,-33,0,498,955,4,52299,"FO2","IC" 33,17,5,4,2,646,1,"PERU (CITY OF)","PERU",0,"LIGHT OIL",14840,"0M",1294,,,95,-17,5,621,-6,30,547,-28,31,516,-11,19,497,2,45,621,32,120,501,-5,0,501,78,277,563,-5,0,563,2,31,532,-6,34,498,-8,0,498,955,4,52299,"FO2","GT" 33,17,5,3,2,649,15,"PRINCETON (CITY OF)","PRINCETON",0,"LIGHT OIL",15388,"0M",1294,,,95,6,12,977,0,0,976,3,7,975,2,4,971,3,7,975,23,40,932,56,97,838,536,913,802,20,35,768,17,32,720,0,3,712,14,25,688,957,4,52397,"FO2","IC" 33,17,5,3,9,649,15,"PRINCETON (CITY OF)","PRINCETON",0,"NAT GAS",15388,"0M",1294,,,95,21,220,0,0,0,0,27,268,0,15,153,0,24,231,0,137,1308,0,636,6226,0,1790,17269,0,131,1265,0,82,827,0,0,106,0,75,752,0,957,4,52397,"NG","IC" 33,17,5,3,2,652,15,"RANTOUL (CITY OF)","RANTOUL",0,"LIGHT OIL",15686,"0A",1294,,,95,18,21,236,2,5,232,6,12,220,11,25,195,23,32,203,55,112,186,16,31,295,0,0,299,0,0,299,8,15,284,0,0,284,0,0,284,958,4,52436,"FO2","IC" 33,17,5,3,2,655,1,"RED BUD (CITY OF)","RED BUD",0,"LIGHT OIL",15772,"0A",1294,,,95,28,56,1047,2,5,1040,2,3,1034,0,1,1030,4,7,1021,15,26,993,6,9,981,14,25,956,0,0,956,0,0,953,0,0,949,0,0,948,959,4,52447,"FO2","IC" 33,17,5,3,9,655,1,"RED BUD (CITY OF)","RED BUD",0,"NAT GAS",15772,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,959,4,52447,"NG","IC" 33,17,5,3,2,661,5,"ROCHELLE (CITY OF)","N NINTH ST",0,"LIGHT OIL",16179,"0A",1294,,,95,0,0,0,5,15,779,0,0,0,3,0,771,0,0,764,12,23,741,59,110,631,112,214,527,0,0,416,0,0,415,0,24,711,0,25,686,960,4,52498,"FO2","IC" 33,17,5,3,9,661,5,"ROCHELLE (CITY OF)","N NINTH ST",0,"NAT GAS",16179,"0A",1294,,,95,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,9,98,0,490,5142,0,1012,10917,0,0,0,0,0,0,0,0,1171,0,0,705,0,960,4,52498,"NG","IC" 33,17,5,2,6,661,10,"ROCHELLE (CITY OF)","S MAIN ST",0,"BIT COAL",16179,"0A",1294,,,95,182,283,317,0,0,1359,692,1123,1498,0,0,1498,0,0,1498,0,0,1498,0,0,1498,0,0,1498,0,0,1218,0,0,0,256,380,38,0,38,0,961,4,52498,"BIT","ST" 33,17,5,2,9,661,10,"ROCHELLE (CITY OF)","S MAIN ST",0,"NAT GAS",16179,"0A",1294,,,95,2606,84363,0,2941,19198,0,1831,61444,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0,927,28450,0,0,0,0,961,4,52498,"NG","ST" 33,17,5,3,2,661,10,"ROCHELLE (CITY OF)","S MAIN ST",0,"LIGHT OIL",16179,"0A",1294,,,95,0,0,0,0,0,261,0,0,259,7,8,258,0,0,258,0,0,1498,0,0,1498,0,2,252,0,0,251,0,0,252,0,1,249,0,0,216,961,4,52498,"FO2","IC" 33,17,5,3,9,661,10,"ROCHELLE (CITY OF)","S MAIN ST",0,"NAT GAS",16179,"0A",1294,,,95,0,0,0,0,0,0,14,486,0,2,19,0,0,0,0,0,0,0,0,0,0,83,2186,0,0,0,0,0,0,0,10,323,0,0,0,0,961,4,52498,"NG","IC" 33,17,5,2,2,676,1,"SPRINGFIELD (CITY OF)","LAKESIDE",0,"LIGHT OIL",17828,"0M",1294,,,95,18,56,3309,-376,0,3847,35,123,3773,38,88,3309,8,21,2805,159,387,2233,123,292,1856,53,125,1641,42,111,1830,11,54,1641,16,39,2126,38,94,1910,964,4,52766,"FO2","ST" 33,17,5,2,6,676,1,"SPRINGFIELD (CITY OF)","LAKESIDE",0,"BIT COAL",17828,"0M",1294,,,95,1426,1194,2186,0,0,2186,1719,1619,3329,28971,18281,2724,3680,2612,1929,9405,6305,1526,17496,11431,1377,28851,18625,1401,2662,1934,379,394,523,1151,16922,10895,1211,7009,4720,1069,964,4,52766,"