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  1. Perrin Ranch | Open Energy Information

    Open Energy Info (EERE)

    Perrin Ranch Jump to: navigation, search Name Perrin Ranch Facility Perrin Ranch Sector Wind energy Facility Type Commercial Scale Wind Facility Status In Service Owner NextEra...

  2. West Perrine, Florida: Energy Resources | Open Energy Information

    Open Energy Info (EERE)

    Hide Map This article is a stub. You can help OpenEI by expanding it. West Perrine is a census-designated place in Miami-Dade County, Florida.1 References ...

  3. DOE Tour of Zero Floorplans: Row Homes at Perrin's Row by New Town Builders

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    | Department of Energy Row Homes at Perrin's Row by New Town Builders DOE Tour of Zero Floorplans: Row Homes at Perrin's Row by New Town Builders DOE Tour of Zero Floorplans: Row Homes at Perrin's Row by New Town Builders DOE Tour of Zero Floorplans: Row Homes at Perrin's Row by New Town Builders DOE Tour of Zero Floorplans: Row Homes at Perrin's Row by New Town Builders DOE Tour of Zero Floorplans: Row Homes at Perrin's Row by New Town Builders DOE Tour of Zero Floorplans: Row Homes at

  4. DOE Tour of Zero: Row Homes at Perrin's Row by New Town Builders |

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Department of Energy Row Homes at Perrin's Row by New Town Builders DOE Tour of Zero: Row Homes at Perrin's Row by New Town Builders Addthis 1 of 14 New Town Builders, now known as Thrive, built 26 units at the Row Homes at Perrin's Row in Denver, Colorado, to the performance criteria of the U.S. Department of Energy Zero Energy Ready Home (ZERH) program. 2 of 14 Homeowners in the three-story row homes are projected to save $682 in annual energy costs thanks to the homes' efficient

  5. HIA 2015 DOE Zero Energy Ready Home Case Study: New Town Builders, Town Homes at Perrin's Row, Wheat Ridge, CO

    Energy Savers [EERE]

    Town Homes at Perrin's Row Wheat Ridge, CO DOE ZERO ENERGY READY HOME(tm) The U.S. Department of Energy invites home builders across the country to meet the extraordinary levels of excellence and quality specified in DOE's Zero Energy Ready Home program (formerly known as Challenge Home). Every DOE Zero Energy Ready Home starts with ENERGY STAR Certified Homes Version 3.0 for an energy-efficient home built on a solid foundation of building science research. Advanced technologies are designed in

  6. Molecular Mimicry Regulates ABA Signaling by SnRK2 Kinases and PP2C Phosphatases

    SciTech Connect (OSTI)

    Soon, Fen-Fen; Ng, Ley-Moy; Zhou, X. Edward; West, Graham M.; Kovach, Amanda; Tan, M.H. Eileen; Suino-Powell, Kelly M.; He, Yuanzheng; Xu, Yong; Chalmers, Michael J.; Brunzelle, Joseph S.; Zhang, Huiming; Yang, Huaiyu; Jiang, Hualiang; Li, Jun; Yong, Eu-Leong; Cutler, Sean; Zhu, Jian-Kang; Griffin, Patrick R.; Melcher, Karsten; Xu, H. Eric

    2014-10-02

    Abscisic acid (ABA) is an essential hormone for plants to survive environmental stresses. At the center of the ABA signaling network is a subfamily of type 2C protein phosphatases (PP2Cs), which form exclusive interactions with ABA receptors and subfamily 2 Snfl-related kinase (SnRK2s). Here, we report a SnRK2-PP2C complex structure, which reveals marked similarity in PP2C recognition by SnRK2 and ABA receptors. In the complex, the kinase activation loop docks into the active site of PP2C, while the conserved ABA-sensing tryptophan of PP2C inserts into the kinase catalytic cleft, thus mimicking receptor-PP2C interactions. These structural results provide a simple mechanism that directly couples ABA binding to SnRK2 kinase activation and highlight a new paradigm of kinase-phosphatase regulation through mutual packing of their catalytic sites.

  7. Hadlock, R.K.; Abbey, O.B. 22 GENERAL STUDIES OF NUCLEAR REACTORS...

    Office of Scientific and Technical Information (OSTI)

    on ultimate heat sinks--cooling ponds Hadlock, R.K.; Abbey, O.B. 22 GENERAL STUDIES OF NUCLEAR REACTORS; 20 FOSSIL-FUELED POWER PLANTS; COOLING PONDS; PERFORMANCE TESTING; NUCLEAR...

  8. Structural basis for basal activity and autoactivation of abscisic acid (ABA) signaling SnRK2 kinases

    SciTech Connect (OSTI)

    Ng, Ley-Moy; Soon, Fen-Fen; Zhou, X. Edward; West, Graham M.; Kovach, Amanda; Suino-Powell, Kelly M.; Chalmers, Michael J.; Li, Jun; Yong, Eu-Leong; Zhu, Jian-Kang; Griffin, Patrick R.; Melcher, Karsten; Xu, H. Eric

    2014-10-02

    Abscisic acid (ABA) is an essential hormone that controls plant growth, development, and responses to abiotic stresses. Central for ABA signaling is the ABA-mediated autoactivation of three monomeric Snf1-related kinases (SnRK2.2, -2.3, and -2.6). In the absence of ABA, SnRK2s are kept in an inactive state by forming physical complexes with type 2C protein phosphatases (PP2Cs). Upon relief of this inhibition, SnRK2 kinases can autoactivate through unknown mechanisms. Here, we report the crystal structures of full-length Arabidopsis thaliana SnRK2.3 and SnRK2.6 at 1.9- and 2.3-{angstrom} resolution, respectively. The structures, in combination with biochemical studies, reveal a two-step mechanism of intramolecular kinase activation that resembles the intermolecular activation of cyclin-dependent kinases. First, release of inhibition by PP2C allows the SnRK2s to become partially active because of an intramolecular stabilization of the catalytic domain by a conserved helix in the kinase regulatory domain. This stabilization enables SnRK2s to gain full activity by activation loop autophosphorylation. Autophosphorylation is more efficient in SnRK2.6, which has higher stability than SnRK2.3 and has well-structured activation loop phosphate acceptor sites that are positioned next to the catalytic site. Together, these data provide a structural framework that links ABA-mediated release of PP2C inhibition to activation of SnRK2 kinases.

  9. NREL: Photovoltaics Research - Greg Perrin

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    maintenance, and repair; machining and other lab support. Printable Version Photovoltaics Research Home Silicon Polycrystalline Thin Films Multijunctions New Materials,...

  10. Magnetic dipole sequences in {sup 83}Rb

    SciTech Connect (OSTI)

    Schwengner, R.; Schnare, H.; Wagner, A.; Doenau, F.; Rainovski, G.; Frauendorf, S.; Jungclaus, A.; Hausmann, M.; Lieb, K. P.; Yordanov, O.; Napoli, D. R.; De Angelis, G.; Axiotis, M.; Marginean, N.; Brandolini, F.; Alvarez, C. Rossi

    2009-10-15

    High-spin states in {sup 83}Rb were populated in the reaction {sup 11}B+{sup 76}Ge at beam energies of 45 and 50 MeV. {gamma} rays were detected with the spectrometer GASP. The level scheme of {sup 83}Rb was extended up to 13.9 MeV. Mean lifetimes of 23 levels were determined using the Doppler-shift-attenuation method. Among the bands newly established is a sequence comprising intense M1 transitions and crossover E2 transitions. This sequence turns out to be irregular and thus shows that magnetic rotation as observed in the neighboring odd-odd isotopes is not realized in this odd-even nuclide. Excited states in {sup 83}Rb were interpreted in terms of the shell model using the model space {pi}(0f{sub 5/2},1p{sub 3/2},1p{sub 1/2},0g{sub 9/2}) {nu}(1p{sub 1/2},0g{sub 9/2}). The configurations predicted for the negative-parity M1 sequence reproduce the M1 transition strengths fairly well.

  11. Rb-Sr Geochronologic Investigation Of Precambrian Samples From...

    Open Energy Info (EERE)

    Rb-Sr Geochronologic Investigation Of Precambrian Samples From Deep Geothermal Drill Holes, Fenton Hill, New Mexico Jump to: navigation, search OpenEI Reference LibraryAdd to...

  12. R.K. Owen

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    interests are in hiking, trail building through V.O.Cal, geocaching, LINUX, and code hacking. Currently, he is the key maintainer of the environment modules package, a...

  13. Microporous titanosilicate AM-2: Rb-exchange and thermal behaviour

    SciTech Connect (OSTI)

    Doebelin, Nicola . E-mail: nicola@doebelin.org; Armbruster, Thomas

    2007-01-18

    Rb-exchange and thermal stability of the microporous titanosilicate AM-2 were analysed by powder X-ray diffraction, thermo-gravimetric analysis, and chemical analysis of the mother liquid after exchange. The dehydration and thermal stability of the exchanged structure were monitored with in situ high temperature powder X-ray diffraction. Crystal structures were refined with Rietveld methods at 25 and 400 deg. C. The AM-2 structure was found to incorporate Rb{sup +} by replacing K{sup +}. After four exchange cycles and 166 h reaction time at 90 deg. C, the chemical composition was refined to K{sub 0.18}Rb{sub 1.82}TiSi{sub 3}O{sub 9}.H{sub 2}O. Extrapolation suggests that higher exchange ratios may be obtained after further cycles. H{sub 2}O was expelled by heating, leading to a dehydrated structure at 360 deg. C. Dehydration was associated with a change of space group symmetry from orthorhombic P2{sub 1}2{sub 1}2{sub 1} to monoclinic P2{sub 1}, which proved to be reversible after rehydration. This change of symmetry leaves the AM-2 characteristic structural topology uninfluenced and causes only minor distortions. The monoclinic AM-2 structure breaks down above 600 deg. C to become X-ray amorphous, and at 750 deg. C a wadeite-type phase (K {sub x}Rb{sub 2-x}TiSi{sub 3}O{sub 9}) crystallises. This transformation is irreversible and leads to immobilisation of Rb{sup +}.

  14. Short-lived isomers in {sup 94}Rb

    SciTech Connect (OSTI)

    Tsekhanovich, I.; Dare, J. A.; Smith, A. G.; Varley, B. J.; Simpson, G. S.; Urban, W.; Soldner, T.; Jolie, J.; Linnemann, A.; Orlandi, R.; Smith, J. F.; Scherillo, A.; Rzaca-Urban, T.; Zlomaniec, A.; Dorvaux, O.; Gall, B. J. P.; Roux, B.

    2008-07-15

    The medium-spin structure of the neutron-rich, odd-odd nucleus {sup 94}Rb was studied by means of {gamma}-ray spectroscopy. Excited levels were populated in the neutron-induced fission of {sup 235}U and in the spontaneous fission of {sup 252}Cf and {sup 248}Cm. Two isomeric states were found at 1485.2 and 2074.8 keV with half-lives of 18 and 107 ns, respectively. The probable structures of the two isomers involve the fully aligned, proton-neutron configurations [{pi}(g{sub 9/2}) x {nu}(g{sub 7/2})]{sub 8{sup +}} and [{pi}(g{sub 9/2}) x {nu}(h{sub 11/2})]{sub 10{sup -}}, respectively. These new data give information on the single-particle energies in the region.

  15. The electrical transport properties of liquid Rb using pseudopotential theory

    SciTech Connect (OSTI)

    Patel, A. B. Bhatt, N. K. Thakore, B. Y. Jani, A. R.; Vyas, P. R.

    2014-04-24

    Certain electric transport properties of liquid Rb are reported. The electrical resistivity is calculated by using the self-consistent approximation as suggested by Ferraz and March. The pseudopotential due to Hasegawa et al for full electron-ion interaction, which is valid for all electrons and contains the repulsive delta function due to achieve the necessary s-pseudisation was used for the calculation. Temperature dependence of structure factor is considered through temperature dependent potential parameter in the pair potential. Finally, thermo-electric power and thermal conductivity are obtained. The outcome of the present study is discussed in light of other such results, and confirms the applicability of pseudopotential at very high temperature via temperature dependent pair potential.

  16. Electron transport in carbon nanotube/RbAg{sub 4}I{sub 5} film...

    Office of Scientific and Technical Information (OSTI)

    We explore the transport properties of mixed ionic-electronic conductors made of carbon nanotubeRbAgsub 4Isub 5 film composite nanostructures in the presence of optical ...

  17. Ba2+-inhibitable /sup 86/Rb+ fluxes across membranes of vesicles from toad urinary bladder

    SciTech Connect (OSTI)

    Garty, H.; Civan, M.M.

    1987-01-01

    /sup 86/Rb+ fluxes have been measured in suspensions of vesicles prepared from the epithelium of toad urinary bladder. A readily measurable barium-sensitive, ouabain-insensitive component has been identified; the concentration of external Ba2+ required for half-maximal inhibition was 0.6 mM. The effects of externally added cations on /sup 86/Rb+ influx and efflux have established that this pathway is conductive, with a selectivity for K+, Rb+ and Cs+ over Na+ and Li+. The Rb+ uptake is inversely dependent on external pH, but not significantly affected by internal Ca2+ or external amiloride, quinine, quinidine or lidocaine. It is likely, albeit not yet certain, that the conductive Rb+ pathway is incorporated in basolateral vesicles oriented right-side-out. It is also not yet clear whether this pathway comprises the principle basolateral K+ channel in vivo, and that its properties have been unchanged during the preparative procedures. Subject to these caveats, the data suggest that the inhibition by quinidine of Na+ transport across toad bladder does not arise primarily from membrane depolarization produced by a direct blockage of the basolateral channels. It now seems more likely that the quinidine-induced elevation of intracellular Ca2+ activity directly blocks apical Na+ entry.

  18. High-spin states and level structure in {sup 84}Rb

    SciTech Connect (OSTI)

    Shen Shuifa; Han Guangbing; Wen Shuxian; Gu Jianzhong; Wu Xiaoguang; Zhu Lihua; He Chuangye; Li Guangsheng; Yu Beibei; Pan Feng; Zhu Jianyu; Draayer, J. P.; Wen Tingdun; Yan, Yupeng

    2010-07-15

    High-spin states in {sup 84}Rb have been studied by using the {sup 70}Zn({sup 18}O,p3n){sup 84}Rb reaction at beam energy of 75 MeV. The gamma-gamma coincidence, excitation function, and ratios for directional correlation of oriented states were determined. A new level scheme was established in which the positive- and negative-parity bands have been extended up to 17{sup +} and 17{sup -} with an excitation energy of about 7 MeV. The signature splitting and signature inversion of the positive-parity yrast band were observed. To understand the microscopic origin of the signature inversion in the yrast positive-parity bands of doubly odd Rb nuclei, as an example, we performed calculations using the projected shell model to describe the energy spectra in {sup 84}Rb. It can be seen that the main features are reproduced in the calculations. This analysis shows that the signature splitting, especially its inversion, can be reproduced by varying only the gamma deformation with increasing spin. To research the deformation of {sup 84}Rb carefully, we calculate the total Routhian surfaces of positive-parity yrast states by the cranking shell model formalism. In addition, the results of theoretical calculations about the negative-parity yrast band in {sup 84}Rb with configuration pi(p{sub 3/2},f{sub 5/2}) x nug{sub 9/2} are compared with experimental data, and a band diagram calculated for this band is also shown to extract physics from the numerical results.

  19. Electron transport in carbon nanotube/RbAg{sub 4}I{sub 5} film composite

    Office of Scientific and Technical Information (OSTI)

    nanostructures modulated by optical field (Journal Article) | SciTech Connect SciTech Connect Search Results Journal Article: Electron transport in carbon nanotube/RbAg{sub 4}I{sub 5} film composite nanostructures modulated by optical field Citation Details In-Document Search Title: Electron transport in carbon nanotube/RbAg{sub 4}I{sub 5} film composite nanostructures modulated by optical field We explore the transport properties of mixed ionic-electronic conductors made of carbon

  20. Bandwidth and Electron Correlation-Tuned Superconductivity in Rb 0.8 Fe 2 (

    Office of Scientific and Technical Information (OSTI)

    Se 1 - z S z ) 2 (Journal Article) | SciTech Connect Bandwidth and Electron Correlation-Tuned Superconductivity in Rb 0.8 Fe 2 ( Se 1 - z S z ) 2 Citation Details In-Document Search This content will become publicly available on December 14, 2016 Title: Bandwidth and Electron Correlation-Tuned Superconductivity in Rb 0.8 Fe 2 ( Se 1 - z S z ) 2 Authors: Yi, M. ; Wang, Meng ; Kemper, A. F. ; Mo, S.-K. ; Hussain, Z. ; Bourret-Courchesne, E. ; Lanzara, A. ; Hashimoto, M. ; Lu, D. H. ; Shen,

  1. Half metallic ferromagnetism in alkali metal nitrides MN (M = Rb, Cs): A first principles study

    SciTech Connect (OSTI)

    Murugan, A. Rajeswarapalanichamy, R. Santhosh, M. Sudhapriyanga, G.; Kanagaprabha, S.

    2014-04-24

    The structural, electronic and elastic properties of two alkali metal nitrides (MN: M= Rb, Cs) are investigated by the first principles calculations based on density functional theory using the Vienna ab-initio simulation package. At ambient pressure the two nitrides are stable in ferromagnetic state with CsCl structure. The calculated lattice parameters are in good agreement with the available results. The electronic structure reveals that these materials are half metallic in nature. A pressure-induced structural phase transition from CsCl to ZB phase is observed in RbN and CsN.

  2. Total absorption spectroscopy study of ?Rb decay: A major contributor to reactor antineutrino spectrum shape [Total absorption spectroscopy study of ?Rb: A major contributor to reactor antineutrino flux

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Sonzogni, A.; Zakari-Issoufou, A. -A.; Fallot, M.; Porta, A.; Algora, A.; Tain, J. L.; Valencia, E.; Rice, S.; Bui, V. M.; Cormon, S.; et al

    2015-03-09

    The accurate determination of the emitted reactor antineutrino flux is still a major challenge for actual and future neutrino experiments at reactors, especially after the evidence of a disagreement between the measured antineutrino energy spectrum by Double Chooz, Daya Bay, and Reno and calculated antineutrino spectra obtained from the conversion of the unique integral beta spectra measured at the ILL reactor. Using nuclear data to compute reactor antineutrino spectra may help understanding this bias, with the study of the underlying nuclear physics. Summation calculations allow identifying a list of nuclei that contribute importantly to the antineutrino energy spectra emitted aftermorethe fission of ?,?Pu and ?,?U, and whose beta decay properties might deserve new measurements. Among these nuclei, ?Rb exhausts by itself about 16% of of the antineutrino energy spectrum emitted by Pressurized Water Reactors in the 5 to 8 MeV range. In this Letter, we report new Total Absorption Spectroscopy (TAS) results for this important contributor. The obtained beta feeding from ?Rb shows beta intensity unobserved before in the 4.5 to 5.5 MeV energy region and gives a ground state to ground state branch of 87.5 % 3%. These new data induce a dramatic change in recent summation calculations where a 51% GS to GS branch was considered for ?Rb, increasing the summation antineutrino spectrum in the region nearby the observed bias.The new data still have an important impact on other summation calculations in which more recent data were consideredless

  3. Total absorption spectroscopy study of ?Rb decay: A major contributor to reactor antineutrino spectrum shape [Total absorption spectroscopy study of ?Rb: A major contributor to reactor antineutrino flux

    SciTech Connect (OSTI)

    Sonzogni, A.; Zakari-Issoufou, A. -A.; Fallot, M.; Porta, A.; Algora, A.; Tain, J. L.; Valencia, E.; Rice, S.; Bui, V. M.; Cormon, S.; Estienne, M.; Agramunt, J.; Aysto, J.; Bowry, M.; Briz Monago, J. A.; Caballero-Folch, R.; Cano-Ott, D.; Cucoanes, A.; Eloma, V.; Estvez, E.; Farrelly, G. F.; Garcia, A.; Gelletly, W.; Gomez-Hornillos, M. B.; Gorlychev, V.; Hakala, J.; Jokinen, A.; Jordan, M. D.; Kankainen, A.; Kondev, F. G.; Martinez, T.; Mendoza, E.; Molina, F.; Moore, I.; Perez, A.; Podolyak, Zs.; Penttil, H.; Regan, P. H.; Shiba, T.; Rissanen, J.; Rubio, B.; Weber, C.

    2015-03-09

    The accurate determination of the emitted reactor antineutrino flux is still a major challenge for actual and future neutrino experiments at reactors, especially after the evidence of a disagreement between the measured antineutrino energy spectrum by Double Chooz, Daya Bay, and Reno and calculated antineutrino spectra obtained from the conversion of the unique integral beta spectra measured at the ILL reactor. Using nuclear data to compute reactor antineutrino spectra may help understanding this bias, with the study of the underlying nuclear physics. Summation calculations allow identifying a list of nuclei that contribute importantly to the antineutrino energy spectra emitted after the fission of ?,?Pu and ?,?U, and whose beta decay properties might deserve new measurements. Among these nuclei, ?Rb exhausts by itself about 16% of of the antineutrino energy spectrum emitted by Pressurized Water Reactors in the 5 to 8 MeV range. In this Letter, we report new Total Absorption Spectroscopy (TAS) results for this important contributor. The obtained beta feeding from ?Rb shows beta intensity unobserved before in the 4.5 to 5.5 MeV energy region and gives a ground state to ground state branch of 87.5 % 3%. These new data induce a dramatic change in recent summation calculations where a 51% GS to GS branch was considered for ?Rb, increasing the summation antineutrino spectrum in the region nearby the observed bias.The new data still have an important impact on other summation calculations in which more recent data were considered

  4. Precise Measurement of Strontium-82 Radioactivity in the Sr-Rb PET

    Office of Science (SC) Website

    Generator | U.S. DOE Office of Science (SC) Precise Measurement of Strontium-82 Radioactivity in the Sr-Rb PET Generator Nuclear Physics (NP) NP Home About Research Facilities Science Highlights Benefits of NP Applications of Nuclear Science Applications of Nuclear Science Archives Small Business Innovation / Technology Transfer Funding Opportunities Nuclear Science Advisory Committee (NSAC) Community Resources Contact Information Nuclear Physics U.S. Department of Energy SC-26/Germantown

  5. Two spatially separated phases in semiconducting Rb0.8Fe1.5S2

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Wang, Meng; Tian, Wei; Valdivia, P.; Chi, Songxue; Bourret-Courchesne, E. D.; Dai, Pengcheng; Birgeneau, R. J.

    2014-01-01

    We report neutron scattering and transport measurements on semiconducting Rb0.8Fe1.5S2, a compound isostructural and isoelectronic to the well-studied A0.8FeySe2(A = K, Rb, Cs, Tl/K) superconducting systems. Both resistivity and dc susceptibility measurements reveal a magnetic phase transition at T = 275 K. Neutron diffraction studies show that the 275 K transition originates from a phase with rhombic iron vacancy order which exhibits an in-plane stripe antiferromagnetic ordering below 275 K. In addition, the stripe antiferromagnetic phase interdigitates mesoscopically with an ubiquitous phase with 5 5 iron vacancy order. This phase has a magnetic transition at TN = 425 K andmore » an iron vacancy order-disorder transition at TS = 600 K. These two different structural phases are closely similar to those observed in the isomorphous Se materials. Based on the close similarities of the in-plane antiferromagnetic structures, moments sizes, and ordering temperatures in semiconducting Rb0.8Fe1.5S2 and K0.81Fe1.58Se2, we argue that the in-plane antiferromagnetic order arises from strong coupling between local moments. Superconductivity, previously observed in the A0.8FeySe2 zSz system, is absent in Rb0.8Fe1.5S2, which has a semiconducting ground state. The implied relationship between stripe and block antiferromagnetism and superconductivity in these materials as well as a strategy for further investigation is discussed in this paper.« less

  6. Differential Light-Shift Cancellation in a Magnetic-Field-Insensitive Transition of {sup 87}Rb

    SciTech Connect (OSTI)

    Chicireanu, R.; Nelson, K. D.; Olmschenk, S.; Porto, J. V.; Lundblad, N.; Derevianko, A.

    2011-02-11

    The precise measurement of transition frequencies of trapped atomic samples is susceptible to inaccuracy arising from the inhomogeneous differential shift of the relevant energy levels in the presence of the trapping fields. We demonstrate near-complete cancellation of the differential ac Stark shift (''light shift'') of a two-photon magnetic-field-insensitive microwave hyperfine (clock) transition in {sup 87}Rb atoms trapped in an optical lattice. Up to 95(2)% of the differential light shift is cancelled while maintaining magnetic-field insensitivity. This technique should have applications in quantum information and frequency metrology.

  7. Structure of the SPRY domain of human Ash2L and its interactions with RbBP5

    Office of Scientific and Technical Information (OSTI)

    and DPY30 (Journal Article) | SciTech Connect Structure of the SPRY domain of human Ash2L and its interactions with RbBP5 and DPY30 Citation Details In-Document Search Title: Structure of the SPRY domain of human Ash2L and its interactions with RbBP5 and DPY30 Authors: Chen, Yong ; Cao, Fang ; Wan, Bingbing ; Dou, Yali ; Lei, Ming [1] + Show Author Affiliations (Michigan-Med) Publication Date: 2013-10-07 OSTI Identifier: 1093479 Resource Type: Journal Article Resource Relation: Journal Name:

  8. Structure and optical properties of a noncentrosymmetric borate RbSr{sub 4}(BO{sub 3}){sub 3}

    SciTech Connect (OSTI)

    Xia, M.J.; Li, R.K.

    2013-01-15

    A new noncentrosymmetric borate, RbSr{sub 4}(BO{sub 3}){sub 3} (abbreviated as RSBO), has been grown from Rb{sub 2}O--B{sub 2}O{sub 3}--RbF flux and its crystal structure was determined by single crystal x-ray diffraction. It crystallizes in space group Ama2 with cell parameters of a=11.128(10) A, b=12.155(15) A, c=6.952(7) A, Z=4. The basic structural units are isolated planar BO{sub 3} groups. Second harmonic generation (SHG) test of the title compound by the Kurtz-Perry method shows that RSBO can be phase matchable with an effective SHG coefficient about two-thirds as large as that of KH{sub 2}PO{sub 4} (KDP). Finally, based on the anionic group approximation, the optical properties of the title compound are compared with those of the structure-related apatite-like compounds with the formula 'A{sub 5}(TO{sub n}){sub 3}X'. - Graphical abstract: RbSr{sub 4}(BO{sub 3}){sub 3} and some other borate NLO compounds, namely Ca{sub 5}(BO{sub 3}){sub 3}F RCa{sub 4}(BO{sub 3}){sub 3}O (R=Y or Gd) and Na{sub 3}La{sub 2}(BO{sub 3}){sub 3} can be viewed as the derivatives of apatite. They have similar formula composed of five cations and three anion groups (we call them 5/3 structures). The detailed SHG coefficients and optical properties of the apatite-like NLO crystals were compared and summarized. Highlights: Black-Right-Pointing-Pointer A new noncentrosymmetric borate RbSr{sub 4}(BO{sub 3}){sub 3} was grown from flux. Black-Right-Pointing-Pointer The RbSr{sub 4}(BO{sub 3}){sub 3} can be viewed as a derivative of the apatite-like structure. Black-Right-Pointing-Pointer The structure and its relationship to the optical properties of RbSr{sub 4}(BO{sub 3}){sub 3} are compared with other NLO crystals with apatite-like structures. Black-Right-Pointing-Pointer The basic structural units are the planar BO{sub 3} groups in the structure. Black-Right-Pointing-Pointer Second harmonic generation (SHG) test shows that RbSr{sub 4}(BO{sub 3}){sub 3} can be phase matchable with an effective SHG coefficient about two-thirds as large as that of KH{sub 2}PO{sub 4}.

  9. Two spatially separated phases in semiconducting Rb 0.8 Fe 1.5 S 2 (Journal

    Office of Scientific and Technical Information (OSTI)

    Article) | DOE PAGES Two spatially separated phases in semiconducting Rb 0.8 Fe 1.5 S 2 « Prev Next » Title: Two spatially separated phases in semiconducting Rb 0.8 Fe 1.5 S 2 Authors: Wang, Meng ; Tian, Wei ; Valdivia, P. ; Chi, Songxue ; Bourret-Courchesne, E. ; Dai, Pengcheng ; Birgeneau, R. J. Publication Date: 2014-09-26 OSTI Identifier: 1180514 Grant/Contract Number: AC02-05CH11231; AC03-76SF008 Type: Publisher's Accepted Manuscript Journal Name: Physical Review B Additional Journal

  10. Experimental observation of magic-wavelength behavior of {sup 87}Rb atoms in an optical lattice

    SciTech Connect (OSTI)

    Lundblad, N.; Schlosser, M.; Porto, J. V.

    2010-03-15

    We demonstrate the cancellation of the differential ac Stark shift of the microwave hyperfine clock transition in trapped {sup 87}Rb atoms. Recent progress in metrology exploits so-called magic wavelengths, whereby an atomic ensemble can be trapped with laser light whose wavelength is chosen so that both levels of an optical atomic transition experience identical ac Stark shifts. Similar magic-wavelength techniques are not possible for the microwave hyperfine transitions in the alkali metals due to their simple electronic structure. We show, however, that ac Stark shift cancellation is indeed achievable for certain values of wavelength, polarization, and magnetic field. The cancellation comes at the expense of a small magnetic-field sensitivity. The technique demonstrated here has implications for experiments involving the precise control of optically trapped neutral atoms.

  11. Dipole-dipole broadening of Rb ns-np microwave transitions

    SciTech Connect (OSTI)

    Park, Hyunwook; Tanner, P. J.; Claessens, B. J.; Shuman, E. S.; Gallagher, T. F.

    2011-08-15

    The dipole-dipole broadening of ns-np microwave transitions of cold Rb Rydberg atoms in a magneto-optical trap has been recorded for 28{<=}n{<=}51. Since the electric dipole transition matrix elements scale as n{sup 2}, a broadening rate scaling as n{sup 4} is expected and a broadening rate of 8.2x10{sup -15}n{sup 4} MHz cm{sup 3} is observed. The observed broadening is smaller than expected from a classical picture due to the spin-orbit interaction in the np atoms. The broadened resonances are asymmetric and cusp shaped, and their line shapes can be reproduced by a diatomic model which takes into account the dipole-dipole interaction, including the spin-orbit interaction, the strengths of the allowed microwave transitions, and the distribution of the atomic spacings in the trap.

  12. Ionization of Rb Rydberg atoms in the attractive nsnp dipole-dipole potential

    SciTech Connect (OSTI)

    Park, Hyunwook; Shuman, E. S.; Gallagher, T. F.

    2011-11-15

    We have observed the ionization of a cold gas of Rb Rydberg atoms which occurs when nsns van der Waals pairs of ns atoms of n{approx_equal} 40 on a weakly repulsive potential are transferred to an attractive dipole-dipole nsnp potential by a microwave transition. Comparing the measurements to a simple model shows that the initial 300-{mu}K thermal velocity of the atoms plays an important role. Excitation to a repulsive dipole-dipole potential does not lead to more ionization on a 15-{mu}s time scale than leaving the atoms in the weakly repulsive nsns state. This observation is slightly surprising since a radiative transition must occur to allow ionization in the latter case. Finally, by power broadening of the microwave transition, to allow transitions from the initial nsns state to the nsnp state over a broad range of internuclear spacings, it is possible to accelerate markedly the evolution to a plasma.

  13. Cation ordering and effect of biaxial strain in double perovskite CsRbCaZnCl6

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Pilania, G.; Uberuaga, B. P.

    2015-03-19

    Here, we investigate the electronic structure, energetics of cation ordering, and effect of biaxial strain on double perovskite CsRbCaZnCl6 using first-principles calculations based on density functional theory. The two constituents (i.e., CsCaCl3 and RbZnCl3) forming the double perovskite exhibit a stark contrast. While CsCaCl3 is known to exist in a cubic perovskite structure and does not show any epitaxial strain induced phase transitions within an experimentally accessible range of compressive strains, RbZnCl3 is thermodynamically unstable in the perovskite phase and exhibits ultra-sensitive response at small epitaxial strains if constrained in the perovskite phase. We show that combining the two compositionsmore » in a double perovskite structure not only improves overall stability but also the strain-polarization coupling of the material. Our calculations predict a ground state with P4/nmm space group for the double perovskite, where A-site cations (i.e., Cs and Rb) are layer-ordered and B-site cations (i.e., Ca and Zn) prefer a rocksalt type ordering. The electronic structure and bandgap in this system are shown to be quite sensitive to the B-site cation ordering and is minimally affected by the ordering of A-site cations. We find that at experimentally accessible compressive strains CsRbCaZnCl6 can be phase transformed from its paraelectric ground state to an antiferroelectric state, where Zn atoms contribute predominantly to the polarization. Furthermore, both energy difference and activation barrier for a transformation between this antiferroelectric state and the corresponding ferroelectric configuration are predicted to be small. As a result, the computational approach presented here opens a new pathway towards a rational design of novel double perovskites with improved strain response and functionalities.« less

  14. Spectroscopy and applications of the 3?{sup 3}?{sup +} electronic state of {sup 39}K{sup 85}Rb

    SciTech Connect (OSTI)

    Banerjee, Jayita Rahmlow, David; Carollo, Ryan; Bellos, Michael; Eyler, Edward E.; Gould, Phillip L.; Stwalley, William C.

    2013-11-07

    We report new results on the spectroscopy of the 3?{sup 3}?{sup +} electronic state of {sup 39}K{sup 85}Rb. The observations are based on resonance-enhanced multiphoton ionization of ultracold KRb molecules starting in vibrational levels v?? = 1823 of the a?{sup 3}?{sup +} state and ionized via the intermediate 3?{sup 3}?{sup +} state. The a-state ultracold molecules are formed by photoassociation of ultracold {sup 39}K and {sup 85}Rb atoms to the 3(0{sup +}) state of KRb followed by spontaneous emission. We discuss the potential applications of this state to future experiments, as a pathway for populating the lowest vibrational levels of the a state as well as the X state.

  15. Charging Properties of Cassiterite (alpha-SnO2) surfaces in NaCl and RbCl Ionic Media.

    SciTech Connect (OSTI)

    Rosenqvist, Jorgen K; Machesky, Michael L.; Vlcek, Lukas; Wesolowski, David J

    2009-09-01

    The acid-base properties of cassiterite (alpha-SnO2) surfaces at 10-50 degrees C were studied using potentiometric titrations of powder suspensions in aqueous NaCl and RbCl media. The proton sorption isotherms exhibited common intersection points in the pH range of 4.0-4.5 under all conditions, and the magnitude of charging was similar but not identical in NaCl and RbCl. The hydrogen bonding configuration at the oxide-water interface, obtained from classical molecular dynamics (MD) simulations, was analyzed in detail, and the results were explicitly incorporated in calculations of protonation constants for the reactive surface sites using the revised MUSIC model. The calculations indicated that the terminal SnOH2 group is more acidic than the bridging Sn2OH group, with protonation constants (log KH) of 3.60 and 5.13 at 25 degrees C, respectively. This is contrary to the situation on the isostructural alpha-TiO2 (rutile), apparently because of the difference in electronegativity between Ti and Sn. MD simulations and speciation calculations indicated considerable differences in the speciation of Na+ and Rb+, despite the similarities in overall charging. Adsorbed sodium ions are almost exclusively found in bidentate surface complexes, whereas adsorbed rubidium ions form comparable numbers of bidentate and tetradentate complexes. Also, the distribution of adsorbed Na+ between the different complexes shows a considerable dependence on the surface charge density (pH), whereas the distribution of adsorbed Rb+ is almost independent of pH. A surface complexation model (SCM) capable of accurately describing both the measured surface charge and the MD-predicted speciation of adsorbed Na+/Rb+ was formulated. According to the SCM, the deprotonated terminal group (SnOH(-0.40)) and the protonated bridging group (Sn2OH+0.36) dominate the surface speciation over the entire pH range of this study (2.7-10). The complexation of medium cations increases significantly with increasing negative surface charge, and at pH 10, roughly 40% of the terminal sites are predicted to form cation complexes, whereas anion complexation is minor throughout the studied pH range.

  16. Charging Properties of Cassiterite (alpha-SnO2) Surfaces in NaCl and RbCl Ionic Media.

    SciTech Connect (OSTI)

    Rosenqvist, Jorgen K; Machesky, Michael L.; Vlcek, Lukas; Wesolowski, David J

    2009-09-01

    The acid-base properties of cassiterite ({alpha}-SnO{sub 2}) surfaces at 10-50 C were studied using potentiometric titrations of powder suspensions in aqueous NaCl and RbCl media. The proton sorption isotherms exhibited common intersection points in the pH range of 4.0-4.5 under all conditions, and the magnitude of charging was similar but not identical in NaCl and RbCl. The hydrogen bonding configuration at the oxide-water interface, obtained from classical molecular dynamics (MD) simulations, was analyzed in detail, and the results were explicitly incorporated in calculations of protonation constants for the reactive surface sites using the revised MUSIC model. The calculations indicated that the terminal SnOH{sub 2} group is more acidic than the bridging Sn{sub 2}OH group, with protonation constants (log K{sub H}) of 3.60 and 5.13 at 25 C, respectively. This is contrary to the situation on the isostructural {alpha}-TiO{sub 2} (rutile), apparently because of the difference in electronegativity between Ti and Sn. MD simulations and speciation calculations indicated considerable differences in the speciation of Na{sup +} and Rb{sup +}, despite the similarities in overall charging. Adsorbed sodium ions are almost exclusively found in bidentate surface complexes, whereas adsorbed rubidium ions form comparable numbers of bidentate and tetradentate complexes. Also, the distribution of adsorbed Na{sup +} between the different complexes shows a considerable dependence on the surface charge density (pH), whereas the distribution of adsorbed Rb{sup +} is almost independent of pH. A surface complexation model (SCM) capable of accurately describing both the measured surface charge and the MD-predicted speciation of adsorbed Na{sup +}/Rb{sup +} was formulated. According to the SCM, the deprotonated terminal group (SnOH{sup -0.40}) and the protonated bridging group (Sn{sub 2}OH{sup +0.36}) dominate the surface speciation over the entire pH range of this study (2.7-10). The complexation of medium cations increases significantly with increasing negative surface charge, and at pH 10, roughly 40% of the terminal sites are predicted to form cation complexes, whereas anion complexation is minor throughout the studied pH range.

  17. Total Absorption Spectroscopy Study of ⁹²Rb Decay: A Major Contributor to Reactor Antineutrino Spectrum Shape

    SciTech Connect (OSTI)

    Sonzogni, A.; Zakari-Issoufou, A. -A.; Fallot, M.; Porta, A.; Algora, A.; Tain, J. L.; Valencia, E.; Rice, S.; Bui, V. M.; Cormon, S.; Estienne, M.; Agramunt, J.; Aysto, J.; Bowry, M.; Briz Monago, J. A.; Caballero-Folch, R.; Cano-Ott, D.; Cucoanes, A.; Eloma, V.; Estvez, E.; Farrelly, G. F.; Garcia, A.; Gelletly, W.; Gomez-Hornillos, M. B.; Gorlychev, V.; Hakala, J.; Jokinen, A.; Jordan, M. D.; Kankainen, A.; Kondev, F. G.; Martinez, T.; Mendoza, E.; Molina, F.; Moore, I.; Perez, A.; Podolyak, Zs.; Penttil, H.; Regan, P. H.; Shiba, T.; Rissanen, J.; Rubio, B.; Weber, C.

    2015-03-09

    The accurate determination of the emitted reactor antineutrino flux is still a major challenge for actual and future neutrino experiments at reactors, especially after the evidence of a disagreement between the measured antineutrino energy spectrum by Double Chooz, Daya Bay, and Reno and calculated antineutrino spectra obtained from the conversion of the unique integral beta spectra measured at the ILL reactor. Using nuclear data to compute reactor antineutrino spectra may help understanding this bias, with the study of the underlying nuclear physics. Summation calculations allow identifying a list of nuclei that contribute importantly to the antineutrino energy spectra emitted after the fission of ²³⁹,²⁴¹Pu and ²³⁵,²³⁸U, and whose beta decay properties might deserve new measurements. Among these nuclei, ⁹²Rb exhausts by itself about 16% of of the antineutrino energy spectrum emitted by Pressurized Water Reactors in the 5 to 8 MeV range. In this Letter, we report new Total Absorption Spectroscopy (TAS) results for this important contributor. The obtained beta feeding from ⁹²Rb shows beta intensity unobserved before in the 4.5 to 5.5 MeV energy region and gives a ground state to ground state branch of 87.5 % ± 3%. These new data induce a dramatic change in recent summation calculations where a 51% GS to GS branch was considered for ⁹²Rb, increasing the summation antineutrino spectrum in the region nearby the observed bias.The new data still have an important impact on other summation calculations in which more recent data were considered

  18. Total Absorption Spectroscopy Study of ⁹²Rb Decay: A Major Contributor to Reactor Antineutrino Spectrum Shape

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Sonzogni, A.; Zakari-Issoufou, A. -A.; Fallot, M.; Porta, A.; Algora, A.; Tain, J. L.; Valencia, E.; Rice, S.; Bui, V. M.; Cormon, S.; et al

    2015-03-09

    The accurate determination of the emitted reactor antineutrino flux is still a major challenge for actual and future neutrino experiments at reactors, especially after the evidence of a disagreement between the measured antineutrino energy spectrum by Double Chooz, Daya Bay, and Reno and calculated antineutrino spectra obtained from the conversion of the unique integral beta spectra measured at the ILL reactor. Using nuclear data to compute reactor antineutrino spectra may help understanding this bias, with the study of the underlying nuclear physics. Summation calculations allow identifying a list of nuclei that contribute importantly to the antineutrino energy spectra emitted aftermore » the fission of ²³⁹,²⁴¹Pu and ²³⁵,²³⁸U, and whose beta decay properties might deserve new measurements. Among these nuclei, ⁹²Rb exhausts by itself about 16% of of the antineutrino energy spectrum emitted by Pressurized Water Reactors in the 5 to 8 MeV range. In this Letter, we report new Total Absorption Spectroscopy (TAS) results for this important contributor. The obtained beta feeding from ⁹²Rb shows beta intensity unobserved before in the 4.5 to 5.5 MeV energy region and gives a ground state to ground state branch of 87.5 % ± 3%. These new data induce a dramatic change in recent summation calculations where a 51% GS to GS branch was considered for ⁹²Rb, increasing the summation antineutrino spectrum in the region nearby the observed bias.The new data still have an important impact on other summation calculations in which more recent data were considered« less

  19. Crystal structural study of ternary molybdate LiRbBi{sub 2}(MoO{sub 4}){sub 4}

    SciTech Connect (OSTI)

    Klevtsova, R.F.; Glinskaya, L.A.; Alekseev, V.I.

    1994-03-01

    Single crystals of the title compound have been synthesized and its crystal structure has been determined. The compound crystallizes in the monoclinic system, space group C2/c, Z = 2 (a = 5.3056, b = 12.976, c = 19.578 {angstrom}, {beta} = 92.583{degrees}, R = 0.029). A distinctive feature of the structure is lacy layers of eight-vertex Bi polyhedra and Mo tetrahedra connected to them via common vertices. The adjacent layers are linked together by ten-vertex Rb polyhedra and Li octahedra.

  20. PRODUCTIOR"OF TRORI~JW~IETALIWES PROCESS F6R RB)IJCIRO T&Old 2 ':

    Office of Legacy Management (LM)

    PRODUCTIOR"OF TRORI~JW~IETALIWES PROCESS F6R RB)IJCIRO T&Old 2 ': am wm ..,. :I.::. ? ; \: :.:, .,, : ,. / 1. ..ri:,:,.:, :/ I 8yblBOLa PPaJPT i: >. ,,;.;~:,,; ,;.. !,., ,ip; ,,,:. ;., -. , ^ , . . 3 '>) ! .,:<;:,,..,. ; : :..,, ,,.+ -../ ,:,; I,:;?: ..: : ,, ,,: ; !. (' '; ::, Durine,~~~v%eit'to Amae &8Htate~Coliegd on Mar6h 4 and 2 to dl&ni& prinalpally~~asl~~prd~ess~~~1 also r&&&d wltlvDii 8. Wilhelm and Dr. D. Peterson of An~?e Iowa State College

  1. Calcium accumulated by sickle cell anemia red cells does not affect their potassium (86Rb+) flux components

    SciTech Connect (OSTI)

    Ortiz, O.E.; Lew, V.L.; Bookchin, R.M.

    1986-03-01

    We investigate here the hypothesis that the high Ca content of sickle cell anemia (SS) red cells may produce a sustained activation of the Ca2+-dependent K+ permeability (Gardos effect) and that the particularly high Ca levels in the dense SS cell fraction rich in irreversibly sickled cells (ISCs) might account for the Na pump inhibition observed in these cells. We measured active and passive 86Rb+ influx (as a marker for K+) in density-fractionated SS cells before and after extraction of their excess Ca by exposure to the Ca ionophore (A23187) and ethylene glycol tetra-acetic acid and with or without adenosine triphosphate depletion or addition of quinine. None of these maneuvers revealed any evidence of a Ca2+-dependent K leak in SS discocytes or dense cells. Na pump inhibition in the dense SS cells was associated with normal activation by external K+ and a low Vmax that persisted after Ca extraction from the cells. These results are consistent with our recent findings that the excess Ca in these cells is compartmentalized in intracellular inside-out vesicles and unavailable as free Ca2+ to the inner membrane surface. Although the steady-state free cytoplasmic Ca2+ in oxygenated SS cells must be below the levels needed to activate the K+ channel, possible brief activation of the channels of some SS cells resulting from transient elevations of cell Ca2+ during deoxygenation-induced sickling cannot be excluded. The dense, ISC-rich SS cell fraction showed a Ca2+-independent increase in the ouabain-resistant, nonsaturable component of 86Rb+ influx that, if uncompensated by Na+ gain, could contribute to the dehydration of these cells.

  2. DOE ZERH Case Study: New Town Builders, Town Homes at Perrin's Row, Wheat Ridge, CO

    SciTech Connect (OSTI)

    none,

    2015-09-01

    Case study of a DOE 2015 Housing Innovation Award winning multifamily project with 26 units in the cold climate that got a HERS 54 without PV, or HERS 28 with PV, with 2x6 24” on center walls with R-23 blown fiberglass; slab foundation with R-10 rigid at slab edge; plus R-10 rigid exterior; R-22 ICF basement walls; vented attic with R-50 blown fiberglass; 92 AFUE furnace, 13 SEER AC.

  3. DOE Tour of Zero: Row Homes at Perrin's Row by New Town Builders...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Water-saving EPA WaterSense-rated fixtures and a "smart" hot water recirculation loop reduce wasted water down the drain waiting for hot water inside. Drought-tolerant, ...

  4. Shape resonances in ground-state diatomic molecules: General trends and the example of RbCs

    SciTech Connect (OSTI)

    Londono, B. E.; Mahecha, J. E.; Luc-Koenig, E.; Crubellier, A.

    2010-07-15

    The presence of shape resonances due to tunneling through the centrifugal barrier modifies strongly the dynamics of cold atom scattering. As shown on the example of the ground and lowest triplet electronic states of the {sup 85}Rb{sup 133}Cs molecule, the crucial parameter is, as usual for cold collisions, the scattering length. A general description of shape resonances of diatomic molecules is given from three simple single channel asymptotic models, whose respective performances are discussed. The first model, which consists of a R{sup -6} potential limited at short range by a repulsive wall, positioned to reproduce the s-wave scattering length, accounts satisfactorily for the main system-independent properties of shape resonances. Introduction in the model of energy- and angular-momentum-dependent nodal lines specific to the inner part of the potential greatly improves its efficiency. When the energy and angular momentum dependence of the nodal lines cannot be deduced from full potential calculations or from experiment, a rough, but universal, estimate of these properties is obtained by extending the R{sup -6} behavior of the potential up to the origin.

  5. Synthesis and structural characterization of a new rubidium borosulfate, Rb{sub 5}BS{sub 4}O{sub 16}

    SciTech Connect (OSTI)

    Dong, Lingyun; Pan, Shilie; Wang, Ying; Yu, Hongwei; Lin, Xiaoxia; Han, Shujuan

    2015-03-15

    Highlights: • Rb{sub 5}BS{sub 4}O{sub 16} has been synthesized using (NH{sub 4}){sub 2}SO{sub 4} as a source of sulfate ions for the first time. • Zero-dimensional anion groups, [B(SO{sub 4}){sub 4}]{sup 5−}, exist in the title compound. • Spectral properties and thermal analysis of Rb{sub 5}BS{sub 4}O{sub 16} were reported. - Abstract: A new rubidium borosulfate, Rb{sub 5}BS{sub 4}O{sub 16}, has been synthesized using (NH{sub 4}){sub 2}SO{sub 4} as a source of sulfate ions for the first time. The compound crystallizes in the space group P4{sub 3}2{sub 1}2 (No. 96) of the tetragonal system with a = 10.148(4) Å, c = 16.689(14) Å, V = 1718.8(17) Å{sup 3}, and Z = 4. Zero-dimensional anion groups, [B(SO{sub 4}){sub 4}]{sup 5−}, a central BO{sub 4} tetrahedron sharing all its four vertices with neighboring sulfate tetrahedra, exist in the title compound, and then the rubidium atoms are situated in the voids of the resulting structure. The IR spectrum confirms the presence of BO{sub 4} and SO{sub 4} units. The UV–vis-NIR diffuse reflectance spectrum exhibits a band gap of about 3.99 eV. The TG-DSC analysis suggests that Rb{sub 5}BS{sub 4}O{sub 16} is an incongruent melting compound.

  6. X-ray absorption studies of mixed salt polymer electrolytes: ZnBr{sub 2}/CaBr{sub 2}-PEO, ZnBr{sub 2}/LiBr-PEO, and ZnBr{sub 2}/RbBr-PEO complexes

    SciTech Connect (OSTI)

    McBreen, J.; Yang, X.Q.; Lee, H.S.; Okamoto, Y.

    1995-02-01

    Polyethylene oxide (PEO)-salt systems are an important new class of electrolytes that are being considered for many uses. X-ray absorption (XAS) studies of ZnBr{sub 2}-PEO complexes, at the Zn K edge, at temperatures between 25 and 120 C, indicate that additions of bromide salts of Li, Rb, or Ca result in the formation of ZnBr{sub 4}{sup {minus} 2} complexes with a Zn-Br bond length of 2.42 {angstrom}. XAS, at the Rb K edge, in mixed RbBr/ZnBr{sub 2}-PEO complexes with an excess of ZnBr{sub 2}, shows that the ZnBr{sub 2} causes the RbBr to dissolve in the polymer. The Rb{sup +} ions are weakly complexed with the PEO with an Rb-O bond distance of 2.93 {angstrom}.

  7. Observation of cold Rb{sub 2} molecules trapped in an optical dipole trap using a laser-pulse-train technique

    SciTech Connect (OSTI)

    Menegatti, Carlos R.; Marangoni, Bruno S.; Marcassa, Luis G.

    2011-11-15

    In this work, we have developed and characterized a laser-pulse-train technique to observe cold Rb{sub 2} molecules trapped in an optical dipole trap. The molecules are produced in a magneto-optical trap, and then loaded into a crossed optical dipole trap. The time evolution of the molecular population is obtained by applying a laser pulse train, which photoionizes the ground-state molecules through intermediate molecular bands. Our results show that this technique allows us to obtain a faster data acquisition rate of the time evolution of the molecule population than other techniques.

  8. Proceedings of the wellbore sampling workshop Traeger, R.K. ...

    Office of Scientific and Technical Information (OSTI)

    Harding, B.W. 58 GEOSCIENCES; 15 GEOTHERMAL ENERGY; 02 PETROLEUM; 03 NATURAL GAS; 04 OIL SHALES AND TAR SANDS; 11 NUCLEAR FUEL CYCLE AND FUEL MATERIALS; BOREHOLES; SAMPLING;...

  9. Test report : Raytheon / KTech RK30 energy storage system.

    SciTech Connect (OSTI)

    Rose, David Martin; Schenkman, Benjamin L.; Borneo, Daniel R.

    2013-10-01

    The Department of Energy Office of Electricity (DOE/OE), Sandia National Laboratories (SNL) and the Base Camp Integration Lab (BCIL) partnered together to incorporate an energy storage system into a microgrid configured Forward Operating Base to reduce the fossil fuel consumption and to ultimately save lives. Energy storage vendors will be sending their systems to SNL Energy Storage Test Pad (ESTP) for functional testing and then to the BCIL for performance evaluation. The technologies that will be tested are electro-chemical energy storage systems comprising of lead acid, lithium-ion or zinc-bromide. Raytheon/KTech has developed an energy storage system that utilizes zinc-bromide flow batteries to save fuel on a military microgrid. This report contains the testing results and some limited analysis of performance of the Raytheon/KTech Zinc-Bromide Energy Storage System.

  10. A combined Sm-Nd, Rb-Sr, and U-Pb isotopic study of Mg-suite norite 78238: Further evidence for early differentiation of the Moon

    SciTech Connect (OSTI)

    Edmunson, J; E.Borg, L; Nyquist, L E; Asmerom, Y

    2008-11-17

    Lunar Mg-suite norite 78238 was dated using the Sm-Nd, Rb-Sr, and U-Pb isotopic systems in order to constrain the age of lunar magma ocean solidification and the beginning of Mg-suite magmatism, as well as to provide a direct comparison between the three isotopic systems. The Sm-Nd isotopic system yields a crystallization age for 78238 of 4334 {+-} 37 Ma and an initial {var_epsilon}{sub Nd}{sup 143} value of -0.27 {+-} 0.74. The age-initial {var_epsilon}{sub Nd}{sup 143} (T-I) systematics of a variety of KREEP-rich samples, including 78238 and other Mg-suite rocks, KREEP basalts, and olivine cumulate NWA 773, suggest that lunar differentiation was completed by 4492 {+-} 61 Ma assuming a Chondritic Uniform Reservoir bulk composition for the Moon. The Rb-Sr isotopic systematics of 78238 were disturbed by post-crystallization processes. Nevertheless, selected data points yield two Rb-Sr isochrons. One is concordant with the Sm-Nd crystallization age, 4366 {+-} 53 Ma. The other is 4003 {+-} 95 Ma and is concordant with an Ar-Ar age for 78236. The {sup 207}Pb-{sup 206}Pb age of 4333 {+-} 59 Ma is concordant with the Sm-Nd age. The U-Pb isotopic systematics of 78238 yield linear arrays equivalent to younger ages than the Pb-Pb system, and may reflect fractionation of U and Pb during sample handling. Despite the disturbed nature of the U-Pb systems, a time-averaged {mu} ({sup 238}U/{sup 204}Pb) value of the source can be estimated at 27 {+-} 30 from the Pb-Pb isotopic systematics. Because KREEP-rich samples are likely to be derived from source regions with the highest U/Pb ratios, the relatively low {mu} value calculated for the 78238 source suggests the bulk Moon does not have an exceedingly high {mu} value.

  11. Luminescent properties of phosphor converted LED using an orange-emitting Rb{sub 2}CaP{sub 2}O{sub 7}:Eu{sup 2+} phosphor

    SciTech Connect (OSTI)

    Song, Hee Jo; Yim, Dong Kyun; Cho, In-Sun; Roh, Hee-Suk; Kim, Ju Seong; Kim, Dong-Wan; Hong, Kug Sun

    2012-12-15

    Graphical abstract: Display Omitted Highlights: ► Phase-pure Rb{sub 2}CaP{sub 2}O{sub 7}:Eu{sup 2+} powders were synthesized by a solid state reaction process. ► The optimum emission intensity was observed at the Eu{sup 2+} ion concentration of 0.006. ► The dipole–dipole interaction was the major concentration quenching mechanism. ► The pc-LED coated with Rb{sub 2}CaP{sub 2}O{sub 7}:Eu{sup 2+} had higher CRI than commercial red phosphor. -- Abstract: A series of orange-emitting Rb{sub 2}CaP{sub 2}O{sub 7}:Eu{sup 2+} phosphors were synthesized by a conventional solid-state reaction method. The as-prepared phosphors were characterized by X-ray powder diffraction (XRD), fluorescence spectroscopy, and spectroradiometry. XRD showed that all prepared samples exhibited a monoclinic Rb{sub 2}CaP{sub 2}O{sub 7} phase. Fluorescence spectroscopy showed that the photoluminescence efficiency of Rb{sub 2}Ca{sub 1−x}P{sub 2}O{sub 7}:Eu{sub x}{sup 2+} phosphors increased with increasing Eu{sup 2+} concentration until x = 0.006, then decreased at higher concentrations, due to a concentration quenching effect. The thermal activation energy was also measured to be 0.40 eV. Furthermore, a phosphor-converted LED (pc-LED) coated with Rb{sub 2}Ca{sub 0.994}P{sub 2}O{sub 7}:Eu{sub 0.006}{sup 2+} was fabricated, which exhibited bright orange emission under a forward bias, from 200 to 300 mA. The color rendering index (CRI) of pc-LED coated with Rb{sub 2}Ca{sub 0.994}P{sub 2}O{sub 7}:Eu{sub 0.006}{sup 2+} was higher than the CRI of pc-LED coated with commercial red phosphor, due to the broad emission band of Rb{sub 2}CaP{sub 2}O{sub 7}:Eu{sup 2+} phosphor. In applying with three-band pc-LEDs, moreover, white pc-LED using Rb{sub 2}CaP{sub 2}O{sub 7}:Eu{sup 2+} phosphor had a higher CRI, than using commercial phosphor. These results indicated that Rb{sub 2}CaP{sub 2}O{sub 7}:Eu{sup 2+} phosphor could be a good candidate for a near-UV based w-LED.

  12. Direct evidence for a pressure-induced nodal superconducting gap in the Ba0.65Rb0.35Fe2As2 superconductor

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Guguchia, Z.; Amato, A.; Kang, J.; Luetkens, H.; Biswas, P. K.; Prando, G.; von Rohr, F.; Bukowski, Z.; Shengelaya, A.; Keller, H.; et al

    2015-11-09

    The superconducting gap structure in iron-based high-temperature superconductors (Fe-HTSs) is non-universal. Contrasting with other unconventional superconductors, in the Fe-HTSs both d-wave and extended s-wave pairing symmetries are close in energy. Probing the proximity between these very different superconducting states and identifying experimental parameters that can tune them is of central interest. Here we report high-pressure muon spin rotation experiments on the temperature-dependent magnetic penetration depth in the optimally doped nodeless s-wave Fe-HTS Ba0.65Rb0.35Fe2As2. Upon pressure, a strong decrease of the penetration depth in the zero-temperature limit is observed, while the superconducting transition temperature remains nearly constant. More importantly, the low-temperaturemore » behaviour of the inverse-squared magnetic penetration depth, which is a direct measure of the superfluid density, changes qualitatively from an exponential saturation at zero pressure to a linear-in-temperature behaviour at higher pressures, indicating that hydrostatic pressure promotes the appearance of nodes in the superconducting gap.« less

  13. Identification of a genetic interaction between the tumor suppressor EAF2 and the retinoblastoma protein (Rb) signaling pathway in C. elegans and prostate cancer cells

    SciTech Connect (OSTI)

    Cai, Liquan; Wang, Dan; Fisher, Alfred L.; Wang, Zhou

    2014-05-02

    Highlights: RNAi screen identified genetic enhancers for the C. elegans homolog of EAF2. EAF2 and RBBP4 proteins physically bind to each other and alter transcription. Overexpression of EAF2 and RBBP4 induces the cell death in prostate cancer cells. - Abstract: The tumor suppressor EAF2 is regulated by androgen signaling and associated with prostate cancer. While EAF2 and its partner ELL have been shown to be members of protein complexes involved in RNA polymerase II transcriptional elongation, the biologic roles for EAF2 especially with regards to the development of cancer remains poorly understood. We have previously identified the eaf-1 gene in Caenorhabditiselegans as the ortholog of EAF2, and shown that eaf-1 interacts with the ELL ortholog ell-1 to control development and fertility in worms. To identify genetic pathways that interact with eaf-1, we screened RNAi libraries consisting of transcription factors, phosphatases, and chromatin-modifying factors to identify genes which enhance the effects of eaf-1(tm3976) on fertility. From this screen, we identified lin-53, hmg-1.2, pha-4, ruvb-2 and set-6 as hits. LIN-53 is the C. elegans ortholog of human retinoblastoma binding protein 4/7 (RBBP 4/7), which binds to the retinoblastoma protein and inhibits the Ras signaling pathway. We find that lin-53 showed a synthetic interaction with eaf-1(tm3976) where knockdown of lin-53 in an eaf-1(tm3976) mutant resulted in sterile worms. This phenotype may be due to cell death as the treated worms contain degenerated embryos with increased expression of the ced-1:GFP cell death marker. Further we find that the interaction between eaf-1 and lin-53/RBBP4/7 also exists in vertebrates, which is reflected by the formation of a protein complex between EAF2 and RBBP4/7. Finally, overexpression of either human EAF2 or RBBP4 in LNCaP cells induced the cell death while knockdown of EAF2 in LNCaP enhanced cell proliferation, indicating an important role of EAF2 in controlling the growth and survival of prostate cancer cells. Together these findings identify a novel physical and functional interaction between EAF2 and the Rb pathway.

  14. Milestone Report - M4FT-15OR03120218 - A Literature Search on the Effects of the Decay of 85Kr to 85Rb on Long-term Storage Options

    SciTech Connect (OSTI)

    Bruffey, Stephanie H.; Strachan, Denis M.; Jubin, Robert Thomas; Spencer, Barry B.

    2015-10-01

    Reprocessing of UNF that has been out of the reactor for less than about 50 y requires the removal of 85Kr from the process off-gas streams. This is needed despite the relatively small amount of that isotope in the combined Xe and Kr inventory (Table 1). The decay of 85Kr to 85Rb presents challenges to the materials that will potentially be used to remove and store the Kr recovered from the off-gas. To address some of these problems, a thorough literature survey was completed, and the results of that analysis are summarized in this document.

  15. Binding energies of the ground triplet state a{sup 3}?{sub u}{sup +} of Rb{sub 2} and Cs{sub 2} in terms of the generalized Le RoyBernstein near-dissociation expansion

    SciTech Connect (OSTI)

    Sovkov, V. B.; Ivanov, V. S. [V.A. Fock Institute of Physics and Department of Physics of St. Petersburg State University, Ulyanovskaya Street 1, Petrodvoretz, St. Petersburg 198504 (Russian Federation)] [V.A. Fock Institute of Physics and Department of Physics of St. Petersburg State University, Ulyanovskaya Street 1, Petrodvoretz, St. Petersburg 198504 (Russian Federation)

    2014-04-07

    Formulae of Le RoyBernstein near-dissociation theory are derived in a general isotopeinvariant form, applicable to any term in the rotational expansion of a diatomic ro-vibrational term value. It is proposed to use the generalized Le RoyBernstein expansion to describe the binding energies (ro-vibrational term values) of the ground triplet state a{sup 3}?{sub u}{sup +} of alkali metal dimers. The parameters of this description are determined for Rb{sub 2} and Cs{sub 2} molecules. This approach gives a recipe to calculate the whole variety of the binding energies with characteristic accuracies from ?1 10{sup ?3} to 1 10{sup ?2} cm{sup ?1} using a relatively simple algebraic equation.

  16. Direct evidence for a pressure-induced nodal superconducting gap in the Ba0.65Rb0.35Fe2As2 superconductor

    SciTech Connect (OSTI)

    Guguchia, Z.; Amato, A.; Kang, J.; Luetkens, H.; Biswas, P. K.; Prando, G.; von Rohr, F.; Bukowski, Z.; Shengelaya, A.; Keller, H.; Morenzoni, E.; Fernandes, Rafael M.; Khasanov, R.

    2015-11-09

    The superconducting gap structure in iron-based high-temperature superconductors (Fe-HTSs) is non-universal. Contrasting with other unconventional superconductors, in the Fe-HTSs both d-wave and extended s-wave pairing symmetries are close in energy. Probing the proximity between these very different superconducting states and identifying experimental parameters that can tune them is of central interest. Here we report high-pressure muon spin rotation experiments on the temperature-dependent magnetic penetration depth in the optimally doped nodeless s-wave Fe-HTS Ba0.65Rb0.35Fe2As2. Upon pressure, a strong decrease of the penetration depth in the zero-temperature limit is observed, while the superconducting transition temperature remains nearly constant. More importantly, the low-temperature behaviour of the inverse-squared magnetic penetration depth, which is a direct measure of the superfluid density, changes qualitatively from an exponential saturation at zero pressure to a linear-in-temperature behaviour at higher pressures, indicating that hydrostatic pressure promotes the appearance of nodes in the superconducting gap.

  17. A9RB1B5.tmp

    Gasoline and Diesel Fuel Update (EIA)

    November 2014 1 November 2014 Short-Term Energy Outlook (STEO) Highlights  North Sea Brent crude oil spot prices fell from $95/barrel (bbl) on October 1 to $84/bbl at the end of the month. The causes included weakening outlooks for global economic and oil demand growth, the return to the market of previously disrupted Libyan crude oil production, and continued growth in U.S. tight oil production. Brent crude oil spot prices averaged $87/bbl in October, the first month Brent prices have

  18. DOE Zero Energy Ready Home Case Study: New Town Builders, Town...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Town Homes at Perrin's Row, Wheat Ridge, CO DOE Zero Energy Ready Home Case Study: New Town Builders, Town Homes at Perrin's Row, Wheat Ridge, CO Case study of a DOE 2015 Housing ...

  19. File:EIA-Appalach7-TN-KY-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  20. File:EIA-Ventura-E-liquids.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  1. File:EIA-BlackWarrior-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  2. File:EIA-Appalach4-southOH-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  3. File:EIA-Ventura-E-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  4. File:EIA-Appalach7-TN-KY-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  5. File:EIA-Williston-S-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  6. File:EIA-PSJ-SE-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  7. File:EIA-Denver-N-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  8. File:EIA-Denver-Mid-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  9. File:EIA-MTB-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  10. File:EIA-Denver-S-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  11. File:EIA-AK-NorthSlope-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  12. File:EIA-PSJ-SE-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  13. File:EIA-UP-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  14. File:EIA-FL-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  15. File:EIA-Appalach6-WV-VA-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  16. File:EIA-shaleusa1.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Natural Gas Creation Date 2008-10-01 Extent Regional Countries...

  17. File:EIA-Appalach5-eastWV-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  18. File:EIA-PSJ-NW-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  19. File:EIA-Appalach2-OH-PA-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  20. File:EIA-PRB-N-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  1. File:EIA-AK-CookInlet-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  2. File:EIA-Appalach3-eastPA-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  3. File:EIA-PRB-S-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  4. File:EIA-PRB-S-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  5. File:EIA-WTB-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  6. File:EIA-Ventura-W-Cent-liquids.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  7. File:EIA-Denver-N-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  8. File:EIA-GGR-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  9. File:EIA-Appalach6-WV-VA-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  10. File:EIA-Eastern-GreatBasin-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  11. File:EIA-Appalach4-southOH-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  12. File:EIA-PSJ-NW-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  13. File:EIA-AK-NPRA-ANWR-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  14. File:EIA-UP-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  15. File:EIA-Denver-S-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  16. File:EIA-MTB-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  17. File:EIA-AK-NorthSlope-liquids.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  18. File:EIA-Denver-Mid-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  19. File:EIA-Williston-NE-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  20. File:EIA-Williston-NW-Liquids.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  1. File:EIA-Appalach3-eastPA-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  2. File:EIA-WTB-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  3. File:EIA-Eastern-OR-WA-liquids.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  4. File:EIA-AK-NPRA-ANWR-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  5. File:EIA-FL-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  6. File:EIA-Williston-NW-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  7. File:EIA-shaleusa3.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Natural Gas Creation Date 2008-12-01 Extent Regional Countries...

  8. File:EIA-BlackWarrior-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  9. File:EIA-AK-CookInlet-Liquids.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  10. File:EIA-Eastern-OR-WA-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  11. File:EIA-Appalach5-eastWV-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  12. File:EIA-PRB-N-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  13. File:EIA-Appalach2-OH-PA-LIQ.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  14. File:EIA-Ventura-W-Cent-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  15. File:EIA-Williston-NE-Liquids.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  16. File:EIA-Williston-S-Liquids.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  17. File:EIA-Eastern-GreatBasin-liquids.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  18. File:EIA-GGR-BOE.pdf | Open Energy Information

    Open Energy Info (EERE)

    Samuel H. Limerick; Lucy Luo; Gary Long; David F. Morehouse; Jack Perrin; Robert F. King Related Technologies Oil, Natural Gas Creation Date 2005-09-01 Extent Regional...

  19. EA-1853: Finding of No Significant Impact | Department of Energy

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    of No Significant Impact EA-1853: Finding of No Significant Impact Perrin Ranch Wind Energy Interconnection Project, Coconino County, Arizona Based on findings and analysis in...

  20. International Linear Collider-A Technical Progress Report (Technical...

    Office of Scientific and Technical Information (OSTI)

    Authors: Elsen, Eckhard ; DESY ; Harrison, Mike ; Brookhaven ; Hesla, Leah ; Fermilab ; Ross, Marc ; Fermilab ; Royole-Degieux, Perrine ; Paris, IN2P3 ; Takahashi, Rika ; ...

  1. Materials Data on Rb(WO3)6 (SG:71) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  2. Materials Data on Rb(TeO3)2 (SG:227) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2015-04-15

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  3. Materials Data on Rb6Te2O9 (SG:15) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  4. Materials Data on RbPaF6 (SG:67) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  5. Materials Data on Rb4Sn2Au7 (SG:166) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  6. Materials Data on RbBr (SG:221) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  7. Materials Data on RbAu (SG:221) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  8. Materials Data on RbScBP2HO9 (SG:2) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  9. Materials Data on RbGaBP2HO9 (SG:14) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  10. Materials Data on RbZn2P2HO8 (SG:2) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  11. Materials Data on RbP(HO)2 (SG:62) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  12. Materials Data on RbP(HO2)2 (SG:43) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  13. Materials Data on RbMnP3HO10 (SG:15) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  14. Materials Data on Rb3Cu2Cl7 (SG:68) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2015-03-25

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  15. Materials Data on RbInI4 (SG:161) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  16. Materials Data on Rb2PtI6 (SG:225) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  17. Materials Data on RbTiI3 (SG:185) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2015-03-25

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  18. Materials Data on Rb2ZnI3 (SG:11) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2015-04-15

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  19. Materials Data on Rb2TeI6 (SG:128) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  20. Materials Data on RbI3 (SG:62) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  1. Materials Data on Rb2PdSe16 (SG:117) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  2. Materials Data on RbAg7S4 (SG:85) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  3. Materials Data on Rb4(BS)9 (SG:2) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  4. Materials Data on RbAl(H2N)4 (SG:85) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2015-04-29

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  5. Materials Data on RbBO2 (SG:167) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  6. Materials Data on RbAg2SbS4 (SG:154) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  7. Precise Measurement of Strontium-82 Radioactivity in the Sr-Rb...

    Office of Science (SC) Website

    Nuclear Physics (NP) NP Home About Research Facilities Science Highlights Benefits of NP Applications of Nuclear Science Applications of Nuclear Science Archives Small Business ...

  8. (References: Klein SA, RB McCoy, H Morrison, AS Ackerman, A

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    YC Sud, DD Turner, DE Veron, K von Salzen, GK Walker, Z Wang, AB Wolf, S Xie, KM Xu, F Yang, and G Zhang. 2009. "Intercomparison of model simulations of mixed- phase clouds...

  9. Materials Data on Rb2Hg7 (SG:164) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2015-02-09

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  10. Materials Data on RbHg11 (SG:221) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  11. Materials Data on Rb5Hg19 (SG:87) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  12. Materials Data on RbSO3 (SG:150) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  13. Materials Data on Rb2SO4 (SG:62) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  14. Materials Data on RbSF5 (SG:62) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  15. Materials Data on RbInTe2 (SG:140) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  16. Materials Data on RbCd(NO2)3 (SG:200) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  17. Materials Data on RbCaF3 (SG:221) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  18. Materials Data on RbAuF4 (SG:140) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  19. Materials Data on RbB(CN)4 (SG:88) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  20. Materials Data on Rb4P21I (SG:63) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  1. Materials Data on Rb6C5 (SG:189) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2015-04-10

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  2. Materials Data on RbCO3 (SG:14) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  3. Materials Data on RbLi2(IO3)3 (SG:14) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  4. Materials Data on RbCr3O8 (SG:12) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  5. Materials Data on Rb2Te5 (SG:12) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2015-02-09

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  6. Materials Data on Rb2Si2O5 (SG:15) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  7. Materials Data on RbSbS2 (SG:2) by Materials Project

    SciTech Connect (OSTI)

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  8. Materials Data on Rb(WO3)3 (SG:10) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  9. DOE Zero Energy Ready Home Case Study: New Town Builders, Town Homes at

    Energy Savers [EERE]

    Perrin's Row, Wheat Ridge, CO | Department of Energy Town Homes at Perrin's Row, Wheat Ridge, CO DOE Zero Energy Ready Home Case Study: New Town Builders, Town Homes at Perrin's Row, Wheat Ridge, CO Case study of a DOE 2015 Housing Innovation Award winning multifamily project with 26 units in the cold climate that got a HERS 54 without PV, or HERS 28 with PV, with 2x6 24" on center walls with R-23 blown fiberglass; slab foundation with R-10 rigid at slab edge; plus R-10 rigid exterior;

  10. I I THE AEROSPACE CORPORATION I I,W. I

    Office of Legacy Management (LM)

    CT Perrine Field, FL Bloomington, IN Layfayette, IN Note I South Bend, IN Note 2 Cambridge, MA Medford, MA Baltimore, MD 1 NAME (Continued) University of Michigan St. Louis...

  11. E&nr Ph. S. W.. Wahhgt~n. D.C. 200242174, TIkpbnc (202) 48a60uo

    Office of Legacy Management (LM)

    CT Perrine Field, FL Bloomington, IN Layfayette, IN Note 1 South Bend, IN Note 2 Cambridge, MA Medford, MA Baltimore, MD . 1 NAME (Continued) University of Michigan St. Louis...

  12. EA-1853: Final Environmental Assessment | Department of Energy

    Broader source: Energy.gov (indexed) [DOE]

    Perrin Ranch Wind submitted an interconnection request to Western in 2010 to interconnect the proposed project to the existing Moenkopi-Yavapai 500-kV transmission line. Western is...

  13. DOE Zero Energy Ready Home Case Study: New Town Builders, Denver...

    Energy Savers [EERE]

    Energy Ready Home Case Study: New Town Builders, Town Homes at Perrin's Row, Wheat Ridge, CO DOE Zero Energy Ready Home Case Study: Palo Duro Homes, Via del Cielo, Santa Fe, NM...

  14. William & Mary Undergrad Receives JSA Research Assistantship | Jefferson

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Lab William & Mary Undergrad Receives JSA Research Assistantship Alice Perrin, a senior physics major at The College of William and Mary Alice Perrin, a senior physics major at The College of William and Mary is the recipient of the 2014-15 Jefferson Science Associates Minority/Female Undergraduate Research Assistantship (JSA MFURA) at Jefferson Lab. Her assistantship project involves setting up a testing facility to measure the performance of 3D printed scintillators to be used in a

  15. Materials Data on RbGa2P2H5O11 (SG:14) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  16. Materials Data on Rb2Ti(Si2O5)3 (SG:9) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  17. Colloid formation study of U, Th, Ra, Pb, Po, Sr, Rb, and Cs in briny (high ionic strength) groundwaters

    SciTech Connect (OSTI)

    Maiti, T.C.; Smith, M.R.; Laul, J.C.

    1989-01-01

    Colloid formation of uranium, thorium, radium, lead, polonium, strontium, rubidium, and cesium in briny (high ionic strength) groundwaters is studied to predict their capability as vectors for transporting radionuclides. This knowledge is essential in developing models to infer the transport of radionuclides from the source region to the surrounding environment. Except polonium, based on the experimental results, colloid formation of uranium, thorium, radium, lead, strontium, rubidium, and cesium is unlikely in brines with compositions similar to the synthetic Palo Duro Basin brine. This observation of no colloid formation is explained by electrokinetic theory and inorganic solution chemistry.

  18. Materials Data on Rb2Ni2(MoO4)3 (SG:14) by Materials Project

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Kristin Persson

    2014-11-02

    Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

  19. Innogrow BV | Open Energy Information

    Open Energy Info (EERE)

    Jump to: navigation, search Name: Innogrow BV Place: Utrecht, Netherlands Zip: 3503 RK Product: Innogrow has developed a greenhouse product for gardening and thermal energy source....

  20. A restated conceptual model for the Humboldt House-Rye Patch...

    Open Energy Info (EERE)

    within the subbasin are anticipated as exploration and development proceeds. Author R.K. Ellis Published Journal Geothermal Resources Council Transactions, 2011 DOI Not Provided...

  1. The Humboldt House-Rye Patch geothermal district: an interim...

    Open Energy Info (EERE)

    completed gathering and reinjection piping network. Authors A. Waibel, D.D. Blackwell and R.K. Ellis Conference GRC Annual Meeting; Morelia, Mexico; 20031015 Published Geothermal...

  2. Rachna Khurana > > Center Alumni > The Energy Materials Center at Cornell

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Rachna Khurana rk455@cornell.edu Formerly a member of the Coates Group, Rachna received her PhD in Summer 2014

  3. mom_sc99

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    between NERSC and GFDL R. Pacanowski, V. Balaji, S. Griffles, J. Shelton, B. Ross Geophyisical Fluid Dynamics Laboratory R.K Owen, H. Anand, S. Luzmoor, H. Simon...

  4. Slide 1

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    - case study Sandia National Laboratories (SNL) Knowledge Preservation for Nuclear Weapons - case study NEA-OECD Sponsored Records, Knowledge and Memory (RK&M) Project ...

  5. Ecofys Subsidiary of Econcern | Open Energy Information

    Open Energy Info (EERE)

    of Econcern Jump to: navigation, search Name: Ecofys Subsidiary of Econcern Address: PO Box 8408 Place: Utrecht Zip: 3503 RK Region: Netherlands Sector: Marine and Hydrokinetic...

  6. Characterizing Photometric Flicker

    Energy Savers [EERE]

    Characterizing Photometric Flicker February 2016 Prepared for: Solid-State Lighting Program Building Technologies Office Office of Energy Efficiency and Renewable Energy U.S. Department of Energy Prepared by: Pacific Northwest National Laboratory Characterizing Photometric Flicker Prepared in support of the DOE Solid-State Lighting Program Study Participants: Pacific Northwest National Laboratory U.S. Department of Energy TE Perrin CC Brown ME Poplawski NJ Miller February 2016 Prepared for:

  7. Generating Bioenergy Solutions for the Clean Energy Economy of Tomorrow |

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Department of Energy Generating Bioenergy Solutions for the Clean Energy Economy of Tomorrow Generating Bioenergy Solutions for the Clean Energy Economy of Tomorrow June 10, 2014 - 2:50pm Addthis Imagine Tomorrow participants Pavan Kumar (from left), Isaak Nanneman, Ethan Perrin, Andrew Wang and Oisin Doherty were selected by the Bioenergy Technologies Office to present their idea at the Biomass 2014 conference next month. The student team from Redmond, Washington, was chosen for their idea

  8. Microsoft Word - DOE-ID-INL-15-049.docx

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    9 SECTION A. Project Title: RB-21 and RB-22 Evacuation Siren Relocation SECTION B. Project Description and Purpose: The proposed action would relocate evacuation sirens RB-21 and RB-22. The power to siren RB-21 is being fed through building Test Reactor Area (TRA)-673 which is being prepared for decommissioning and demolition. Siren RB-21 would be relocated from a wooden pole north of TRA-673 to a new wooden pole to be installed just north of TRA-625. Siren RB-22 is fed from an overhead power

  9. User Science Images

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    mp111 marcdayhydrogenflame.jpg ASCR: Lab-scale Flame Simulation September 1, 2009 | Author(s): M.S.Day, J.B. Bell, R.K. Cheng, S. Tachibana, V.E. Beckner and M.J. Lijewski...

  10. One West Third Street Tulsa, Oklahoma

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    ... City Water and Light Plant of the City of Jonesboro, ... its new program, the Hydropower Modernization Initiative, which, ... an update on the ozaRk majoR RehaBilitation pRoject. ...

  11. Assessing the Rye Patch geothermal field, a classic Basin-and...

    Open Energy Info (EERE)

    if one or two additional wells are drilled for injection. Authors Sanyal, S.K., McNitt, J.R., Butler, S.J., Klein, C.W., and Ellis and R.K. Conference GRC Annual Meeting;...

  12. Siantar, C.L.; Bergstrom, P.M.; Chandler, W.P.; Cox, L.J.; Daly...

    Office of Scientific and Technical Information (OSTI)

    Fast Monte Carlo for radiation therapy: the PEREGRINE Project Hartmann Siantar, C.L.; Bergstrom, P.M.; Chandler, W.P.; Cox, L.J.; Daly, T.P.; Garrett, D.; House, R.K.; Moses, E.I.;...

  13. "Title","Creator/Author","Publication Date","OSTI Identifier...

    Office of Scientific and Technical Information (OSTI)

    Fast Monte Carlo for radiation therapy: the PEREGRINE Project","Hartmann Siantar, C.L.; Bergstrom, P.M.; Chandler, W.P.; Cox, L.J.; Daly, T.P.; Garrett, D.; House, R.K.; Moses,...

  14. June 2015 Most Viewed Documents for Engineering | OSTI, US Dept...

    Office of Scientific and Technical Information (OSTI)

    results on five materials and NIST verification specimens using instrumented 2-mm and 8-mm strikers Nanstad, R.K.; Sokolov, M.A. (1995) 247 Stress analysis and evaluation of a ...

  15. SAND2005-2638

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Co., 1995. 5 Paul, Clayton R., "Introduction to Electromagnetic Compatibility," John Wiley and Sons, Inc., 1992. 6 Schneider, Larry X, Dinallo, M.A., Howard, R.K., Glover,...

  16. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Introducing WEBMADS Dedecker, R.G., Quinn, G.M., Garcia, R.K., and Revercomb, H.E., ... WEB-MADS is a Web based prototype version of MADS that allows remote access to the same ...

  17. Section 63

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    R.K. Garcia, P. van Delst, and W.L. Smith University of Wisconsin - Madison Madison, ... problem (which grew to about 4% and W.L. Smith, 1996: Atmospheric Emitted Radiance in the ...

  18. Performance of wells in solution-gas-drive reservoirs

    SciTech Connect (OSTI)

    Camacho-V, R.G. ); Raghavan, R. )

    1989-12-01

    The authors examine buildup responses in solution-gas-drive reservoirs. The development presented here parallels the development for single-phase liquid flow. Analogs from pseudopressures and time transformations are presented and gas-drive-solutions are correlated with appropriate liquid-flow solutions. The influence of the skin region is documented. The basis for the success of the producing GOR method to compute the saturation distribution at shut-in is presented. The consequences of using the Perrine-Martin analog to analyze buildup data are discussed.

  19. DISCLAIMER

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    ARM-TR-101 Doppler Lidar (DL) Handbook RK Newsom February 2012 Work supported by the U.S. Department of Energy, Office of Science, Office of Biological and Environmental Research RK Newsom, February 2012, DOE/SC-ARM-TR-101 iii Acronyms and Abbreviations AGL above ground level AMF ARM Mobile Facility AMFDL AMF Doppler Lidar ARM Atmospheric Radiation Measurement DL Doppler Lidar DMF Data Management Facility DOE U.S. Department of Energy DQO Data Quality Office GVAX Ganges Valley Aerosol Experiment

  20. Relativistic-Klystron two-beam accelerator as a power source for future linear colliders

    SciTech Connect (OSTI)

    Lidia, S. M.; Anderson, D. E.; Eylon, S.; Henestroza, E.; Vanecek, D. L.; Yu, S. S. [Lawrence Berkeley National Laboratory, Berkeley, California 94720 (United States); Houck, T. L.; Westenskow, G. A. [Lawrence Livermore National Laboratory, Livermore, California 94550 (United States)

    1999-05-07

    The technical challenge for making two-beam accelerators into realizable power sources for high-energy colliders lies in the creation of the drive beam and in its propagation over long distances through multiple extraction sections. This year we have been constructing a 1.2-kA, 1-MeV, induction gun for a prototype relativistic klystron two-beam accelerator (RK-TBA). The electron source will be a 8.9 cm diameter, thermionic, flat-surface cathode with a maximum shroud field stress of approximately 165 kV/cm. Additional design parameters for the injector include a pulse length of over 150-ns flat top (1% energy variation), and a normalized edge emittance of less than 300 pi-mm-mr. The prototype accelerator will be used to study, physics, engineering, and costing issues involved in the application of the RK-TBA concept to linear colliders. We have also been studying optimization parameters, such as frequency, for the application of the RK-TBA concept to multi-TeV linear colliders. As an rf power source the RK-TBA scales favorably up to frequencies around 35 GHz. An overview of this work with details of the design and performance of the prototype injector, beam line, and diagnostics will be presented.

  1. Relativistic-Klystron two-beam accelerator as a power source for future linear colliders

    SciTech Connect (OSTI)

    Lidia, S.M.; Anderson, D.E.; Eylon, S.; Henestroza, E.; Vanecek, D.L.; Yu, S.S. [Lawrence Berkeley National Laboratory, Berkeley, California 94720 (United States); Westenskow, G.A. [Lawrence Livermore National Laboratory, Livermore, California 94550 (United States)

    1999-05-01

    The technical challenge for making two-beam accelerators into realizable power sources for high-energy colliders lies in the creation of the drive beam and in its propagation over long distances through multiple extraction sections. This year we have been constructing a 1.2-kA, 1-MeV, induction gun for a prototype relativistic klystron two-beam accelerator (RK-TBA). The electron source will be a 8.9 cm diameter, thermionic, flat-surface cathode with a maximum shroud field stress of approximately 165 kV/cm. Additional design parameters for the injector include a pulse length of over 150-ns flat top (1{percent} energy variation), and a normalized edge emittance of less than 300 pi-mm-mr. The prototype accelerator will be used to study, physics, engineering, and costing issues involved in the application of the RK-TBA concept to linear colliders. We have also been studying optimization parameters, such as frequency, for the application of the RK-TBA concept to multi-TeV linear colliders. As an rf power source the RK-TBA scales favorably up to frequencies around 35 GHz. An overview of this work with details of the design and performance of the prototype injector, beam line, and diagnostics will be presented. {copyright} {ital 1999 American Institute of Physics.}

  2. Relativistic-klystron two-beam accelerator as a power source for future linear colliders

    SciTech Connect (OSTI)

    Anderson, D E; Eylon, S; Henestroza, E; Houck, T L; Lidia, M; Vanecek, D L; Westenskow, G A; Yu, S S

    1998-10-05

    The technical challenge for making two-beam accelerators into realizable power sources for high-energy colliders lies in the creation of the drive beam and in its propagation over long distances through multiple extraction sections. This year we have been constructing a 1.2&A, l-MeV, induction gun for a prototype relativistic klystron two-beam accelerator (RK-TBA). The electron source will be a 8.9 cm diameter, thermionic, flat-surface cathode with a maximum shroud field stress of approximately 165 kV/cm. Additional design parameters for the injector include a pulse length of over 150-ns flat top (1% energy variation), and a normalized edge emittance of less than 300 pi-mm-n-n. The prototype accelerator will be used to study physics, engineering, and costing issues involved in the application of the RK-TBA concept to linear colliders. We have also been studying optimization parameters, such as frequency, for the application of the RK-TBA concept to multi-TeV linear colliders. As an rf power source the RK-TBA scales favorably up to frequencies around 35 GHz. An overview of this work with details of the design and performance of the prototype injector, beam line, and diagnostics will be presented.

  3. Slide 1

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    no t re fle ct all wo rk IU Iso lat ed Un it RO D Re co rd of De cis ion TS D Tre atm en t, Sto rag e, Dis po sa l K A re a K Ea st Ba sin De mo lish ed Int eri m Sa...

  4. LBL--29472 DE91

    Office of Scientific and Technical Information (OSTI)

    ... In the Ini(tdle of each cell, at z L2 and cos kz 0, all h)ur va,nes a,re spa, ce(1 ... When atmRFQ is first, operated, it will spa.rk and multipa.ctor at lower fields. ...

  5. Zahirul Islam

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Revealed by X-Ray Diffraction in Pulsed Magnetic Fields," J.P.C. Ruff, J.-H. Chu, H.-H. Kuo, R.K. Das, H. Nojiri, I.R. Fisher, Z. Islam, Phys. Rev. Lett. 109, 027004 (2012)....

  6. Mo{sub 6}Se{sub 8}-cluster-based superconducting compounds Cs{sub 2}Mo{sub 12}Se{sub 14} and Rb{sub 4}Mo{sub 18}Se{sub 20}: Evidence for a strongly correlated and anisotropic electron system

    SciTech Connect (OSTI)

    Brusetti, R.; Laborde, O.; Sulpice, A.; Calemczuk, R.; Potel, M.; Gougeon, P.

    1995-08-01

    We studied the normal and superconducting states of the title compounds by measuring the conductivity and magnetization of single crystals and powder samples. From the upper and lower critical fields we deduced the characteristic lengths and thermodynamical fields. These results are borne out by our specific-heat measurements. We recognize in these compounds many features of the Chevrel-phase superconductors, including very small coherence lengths and strong-coupling-like effects. However, we show that the electron system is much more anisotropic and still less delocalized in these materials where the Mo{sub 6}Se{sub 8} clusters have condensed in Mo{sub 6{ital n}}Se{sub 6{ital n}+2} finite chains. This condensation is accompanied by an enhancement of the magnetic response whereas the lengthening of the chains leads to a counteracting reduction of the density of carriers. This indicates that superconductivity is built upon highly correlated molecular states. Reviewing the available data on the other Chevrel-cluster-based superconductors confirms this picture and suggests that the small coherence lengths reflect the local character of the electron pairing. This comparison also shows that forming finite chains of Mo{sub 6}Se{sub 8} clusters makes the electron correlations more repulsive and pushes the electron system near the borderline between superconductivity and magnetism. In this respect these compounds could provide valuable complementary information on issues which are at the center of the research upon high-{ital Y}{sub {ital c}} superconductivity.

  7. Expression of eukaryotic polypeptides in chloroplasts

    DOE Patents [OSTI]

    Mayfield, Stephen P.

    2013-06-04

    The present invention relates to a gene expression system in eukaryotic and prokaryotic cells, preferably plant cells and intact plants. In particular, the invention relates to an expression system having a RB47 binding site upstream of a translation initiation site for regulation of translation mediated by binding of RB47 protein, a member of the poly(A) binding protein family. Regulation is further effected by RB60, a protein disulfide isomerase. The expression system is capable of functioning in the nuclear/cytoplasm of cells and in the chloroplast of plants. Translation regulation of a desired molecule is enhanced approximately 100 fold over that obtained without RB47 binding site activation.

  8. RNA binding protein and binding site useful for expression of recombinant molecules

    DOE Patents [OSTI]

    Mayfield, Stephen

    2000-01-01

    The present invention relates to a gene expression system in eukaryotic and prokaryotic cells, preferably plant cells and intact plants. In particular, the invention relates to an expression system having a RB47 binding site upstream of a translation initiation site for regulation of translation mediated by binding of RB47 protein, a member of the poly(A) binding protein family. Regulation is further effected by RB60, a protein disulfide isomerase. The expression system is capable of functioning in the nuclear/cytoplasm of cells and in the chloroplast of plants. Translation regulation of a desired molecule is enhanced approximately 100 fold over that obtained without RB47 binding site activation.

  9. RNA binding protein and binding site useful for expression of recombinant molecules

    DOE Patents [OSTI]

    Mayfield, Stephen P.

    2006-10-17

    The present invention relates to a gene expression system in eukaryotic and prokaryotic cells, preferably plant cells and intact plants. In particular, the invention relates to an expression system having a RB47 binding site upstream of a translation initiation site for regulation of translation mediated by binding of RB47 protein, a member of the poly(A) binding protein family. Regulation is further effected by RB60, a protein disulfide isomerase. The expression system is capable of functioning in the nuclear/cytoplasm of cells and in the chloroplast of plants. Translation regulation of a desired molecule is enhanced approximately 100 fold over that obtained without RB47 binding site activation.

  10. March 2015 Most Viewed Documents for Environmental Sciences ...

    Office of Scientific and Technical Information (OSTI)

    Statistical methods for environmental pollution monitoring Gilbert, R.O. (1987) 131 ... Study of using oxygen-enriched combustion air for locomotive diesel engines Poola, R.B.; ...

  11. Compound and Elemental Analysis At Fenton Hill HDR Geothermal...

    Open Energy Info (EERE)

    Analysis Activity Date - 1983 Usefulness useful DOE-funding Unknown Notes See linked abstract for a synopsis of chemical analyses and Rb-Sr age determinations for gneissic...

  12. Search for: All records | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    ... All rights reserved. less August 2013 , Elsevier Three Alkali-Metal-Gold-Gallium ... have been characterized in the alkali metal (A Na, Rb, Cs)-gold-gallium systems. ...

  13. Preservation of Records, Knowledge and Memory Across Generations. An emerging Multidisciplinary Work Area and an NEA Project - 12218

    SciTech Connect (OSTI)

    Schroeder, Jantine; Pescatore, Claudio

    2012-07-01

    Disposal in engineered facilities built in stable, deep geological formations is the reference means for permanently isolating long-lived radioactive waste from the human biosphere. This management method is designed to be intrinsically safe and final, i.e. not dependent on human presence and intervention in order to fulfil its safety goal. There is however no intention to forgo, at any time, knowledge and awareness either of the repository or of the waste that it contains. The preservation of Records, Knowledge and Memory (RK and M) is seen as an integral part of radioactive waste management, supporting lengthy and complex socio-technical processes across pre-operational, operational and post-operational lifetimes. Long-term preservation of RK and M is an emerging multidisciplinary work area in which much learning is expected over the coming years. Novel methods are being sought that are least vulnerable to both natural degradation and to changes in socio-economic conditions. Progress has been made in individual countries, but there is a need to internationalise the thinking, compare approaches, investigate potential solutions and share decisions. This is the task of the NEA RK and M project. A major outcome of the project will be a 'menu-driven document' that will allow people to identify the main elements of a strategic action plan for RK and M preservation. In sum, the preservation of RK and M is a unprecedented task in which technical, scientific and social information is interwoven and needs to be developed and preserved across generations and across specialist boundaries. Important studies have been undertaken in the past decades to explore a variety of approaches to preserving RK and M across different timescales, including archives and markers. The work of the past in this area is useful, but innovative thinking is also needed. Seen from today's perspective, very little work is available on for example the contextualization of data for later use; on the systematic identification of mechanisms for RK and M transfer; on implementing a culture of RK and M-keeping in organisations; and on creating cultural links between the waste disposals and the siting communities. Moreover, international cooperation is recognised as being crucial in providing shared means and meanings for memory transmission over longer timescales. International cooperation has also been identified as a catalyst to ensure that a wide range of approaches and experiences is considered, thus potentially reducing uncertainty related to variations in approach. Overall, multiple approaches, requiring active and less active care, need to be considered from the start of the radioactive waste management programme and refined in the course of time. The RK and M project members want to further investigate and deliver support to fulfil this task. (authors)

  14. Measurement of K/sup +/ conductance in gastric vesicles from secreting stomach

    SciTech Connect (OSTI)

    Rabon, E.; Gunther, R.D.

    1986-05-01

    Specific inhibitors were used to identify two components of /sup 86/Rb/sup +/ uptake in vesicles obtained from secreting rabbit stomachs. Rb/sup +/ transport was measured in vesicles as trace /sup 86/Rb/sup +/ uptake following removal of external K/sup +/ from vesicles equilibrated in potassium gluconate. /sup 86/Rb)2= uptake mediated by the gastric H/sup +/K/sup +/-ATPase was identified by sensitivity to vanadate, ATP and pyridyl (1,2a) imidazole (SCH28080). In contrast, /sup 86/Rb/sup +/ influx through a K/sup +/ conductance mechanism was inhibited by the protonophore (TCS) induced collapse of the K/sup +/ diffusion potential. K/sup +/ conductance sensitivity to quinine and the K/sup +/ channel blocker bis-Guanidinium (bis G-8) were demonstrated by inhibition of a K/sup +/ induced chase of intravesicular /sup 86/Rb/sup +/ previously loaded by /sup 86/Rb/sup +//K/sup +/ exchange in the presence of 2 ..mu..M SCH28080. The K/sup +/ conductance is Ba/sup 2 +/ and apamine insensitive and exhibits a monovalent cation specificity of Rb > Kapprox. = Cs >> Na, Li. KCl dependent H/sup +/ transport exhibited complete sensitivity to the H/sup +/, K/sup +/-ATPase inhibitors SCH28080 and vanadate. The measurements of Rb/sup +/ pathways distinctive for the H/sup +/, K/sup +/-ATPase and a K/sup +/ conductance support previous suggestions of a functional linkage between the H/sup +/, K/sup +/-ATPase and a K/sup +/ conductance in vesicles, obtained from stimulated stomach. The experimental discrimination between the two Rb/sup +/ pathways suggests that a separate mechanism is utilized for each transport pathway.

  15. Final Report, IUT - B291527, January 1996 - March 1997

    SciTech Connect (OSTI)

    Henestroza, E.

    1996-04-23

    The following note investigates scaling the 11.4-GHz TBNLC design of a relativistic klystron two-beam accelerator for a 30-GHz, 50-bunch accelerator design. We will refer to this point design as the RK-CLIC. We do not expect that the design will be optimal, but offer it as a starting point for discussions. In this memo, we begin with a general description of the RK-CLIC and drive beam dynamics, discuss required changes to major components, estimate the efficiency of wall plug to microwave power, and estimate costs. To be of interest the design must be such that it: (1) Can be installed at modest cost, (2) Operate with high wall plug to reconversion efficiency, and (3) Have acceptable drive beam dynamics.

  16. Subcooled Flow Boiling Heat Transfer to Water and Ethylene Glycol/Water

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Mixtures in a Bottom-Heated Tube | Argonne National Laboratory Subcooled Flow Boiling Heat Transfer to Water and Ethylene Glycol/Water Mixtures in a Bottom-Heated Tube Title Subcooled Flow Boiling Heat Transfer to Water and Ethylene Glycol/Water Mixtures in a Bottom-Heated Tube Publication Type Journal Article Year of Publication 2015 Authors Yu, W, France, DM, Zhao, W, Singh, D, Smith, RK Journal Experimental Heat Transfer: A Journal of Thermal Energy Generation, Transport, Storage, and

  17. Research Highlight

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Retrieving Cloud and Aerosol Properties from the ARM Raman Lidar Download a printable PDF Submitter: Thorsen, T., NASA - Langley Research Center Fu, Q., University of Washington Area of Research: Cloud Distributions/Characterizations Working Group(s): Aerosol Life Cycle, Cloud Life Cycle Journal Reference: Thorsen TJ, Q Fu, RK Newsom, DD Turner, and JM Comstock. 2015. "Automated retrieval of cloud and aerosol properties from the ARM Raman lidar, Part I: Feature detection." Journal of

  18. Evaluation of the Life History of Native Salmonids in the Malheur River Basin; Cooperative Bull Trout/Redband Trout Research Project, 1999-2000 Annual Report.

    SciTech Connect (OSTI)

    Schwabe, Lawrence; Tiley, Mark; Perkins, Raymond R.

    2000-11-01

    The purpose of this study is to document the seasonal distribution of adult/sub-adult bull trout (Salvelinus confluentus) in the Malheur River basin. Due to the decline of bull trout in the Columbia Basin, the United States Fish and Wildlife Service listed bull trout as a threatened species in June 1998. Past land management activities; construction of dams; and fish eradication projects in the North Fork and Middle Fork Malheur River by poisoning have worked in concert to cumulatively impact native species in the Malheur Basin (Bowers et. al. 1993). Survival of the remaining bull trout populations is severely threatened (Buchanan 1997). 1999 Research Objects are: (1) Document the migratory patterns of adult/sub-adult bull trout in the North Fork Malheur River; (2) Determine the seasonal bull trout use of Beulah Reservoir and bull trout entrainment; and (3) Timing and location of bull trout spawning in the North Fork Malheur River basin. The study area includes the Malheur basin from the mouth of the Malheur River located near Ontario, Oregon to the headwaters of the North Fork Malheur River (Map 1). All fish collected and most of the telemetry effort was done on the North Fork Malheur River subbasin (Map 2). Fish collection was conducted on the North Fork Malheur River at the tailwaters of Beulah Reservoir (RK 29), Beulah Reservoir (RK 29-RK 33), and in the North Fork Malheur River at Crane Crossing (RK 69) to the headwaters of the North Fork Malheur. Radio telemetry was done from the mouth of the Malheur River in Ontario, Oregon to the headwaters of the North Fork Malheur. This report will reflect all migration data collected from 3/1/99 to 12/31/99.

  19. September 2013 Most Viewed Documents for Engineering | OSTI, US Dept of

    Office of Scientific and Technical Information (OSTI)

    Energy, Office of Scientific and Technical Information September 2013 Most Viewed Documents for Engineering Science Subject Feed Conduction heat transfer solutions VanSant, J.H. (1980) 190 /> Charpy impact test results on five materials and NIST verification specimens using instrumented 2-mm and 8-mm strikers Nanstad, R.K.; Sokolov, M.A. (1995) 117 /> Stress analysis and evaluation of a rectangular pressure vessel. [For equipment for sampling Hanford tank radwaste] Rezvani, M.A.;

  20. September 2013 Most Viewed Documents for Materials | OSTI, US Dept of

    Office of Scientific and Technical Information (OSTI)

    Energy, Office of Scientific and Technical Information September 2013 Most Viewed Documents for Materials Science Subject Feed The influence of grain size on the mechanical properties ofsteel Morris Jr., J.W. (2001) 119 /> Charpy impact test results on five materials and NIST verification specimens using instrumented 2-mm and 8-mm strikers Nanstad, R.K.; Sokolov, M.A. (1995) 117 /> Mechanical properties and energy absorption characteristics of a polyurethane foam Goods, S.H.;

  1. DOE/SC-ARM-14-034 Lower Atmospheric Boundary Layer Experiment

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    4 Lower Atmospheric Boundary Layer Experiment (LABLE) Final Campaign Report P Klein WG Blumberg TA Bonin S Mishra JF Newman M Carney DD Turner EP Jacobsen PB Chilson S Wharton CE Wainwright RK Newsom November 2014 DISCLAIMER This report was prepared as an account of work sponsored by the U.S. Government. Neither the United States nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy,

  2. DOE/SC-ARM/TR-120 Raman Lidar Profiles-Temperature

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    0 Raman Lidar Profiles-Temperature (RLPROFTEMP) Value-Added Product RK Newsom C Sivaraman SA McFarlane October 2012 DISCLAIMER This report was prepared as an account of work sponsored by the U.S. Government. Neither the United States nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents

  3. April 2013 Most Viewed Documents for Engineering | OSTI, US Dept of Energy,

    Office of Scientific and Technical Information (OSTI)

    Office of Scientific and Technical Information April 2013 Most Viewed Documents for Engineering Science Subject Feed Charpy impact test results on five materials and NIST verification specimens using instrumented 2-mm and 8-mm strikers Nanstad, R.K.; Sokolov, M.A. (1995) 534 /> Heat Treatment Procedure Qualification -- Final Technical Report Robert C. Voigt (2004) 488 /> Conduction heat transfer solutions VanSant, J.H. (1980) 364 /> Damage identification and health monitoring of

  4. Doppler Lidar Vertical Velocity Statistics Value-Added Product

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    49 Doppler Lidar Vertical Velocity Statistics Value-Added Product RK Newsom C Sivaraman TR Shippert LD Riihimaki July 2015 DISCLAIMER This report was prepared as an account of work sponsored by the U.S. Government. Neither the United States nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or

  5. Doppler Lidar Wind Value-Added Product

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    8 Doppler Lidar Wind Value-Added Product RK Newsom C Sivaraman TR Shippert LD Riihimaki July 2015 DISCLAIMER This report was prepared as an account of work sponsored by the U.S. Government. Neither the United States nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would

  6. July 2013 Most Viewed Documents for Engineering | OSTI, US Dept of Energy,

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Office of Scientific and Technical Information July 2013 Most Viewed Documents for Engineering Science Subject Feed Heat Treatment Procedure Qualification -- Final Technical Report Robert C. Voigt (2004) 513 /> Charpy impact test results on five materials and NIST verification specimens using instrumented 2-mm and 8-mm strikers Nanstad, R.K.; Sokolov, M.A. (1995) 241 /> Conduction heat transfer solutions VanSant, J.H. (1980) 194 /> Damage identification and health monitoring of

  7. July 2013 Most Viewed Documents for Materials | OSTI, US Dept of Energy,

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Office of Scientific and Technical Information July 2013 Most Viewed Documents for Materials Science Subject Feed Heat Treatment Procedure Qualification -- Final Technical Report Robert C. Voigt (2004) 513 /> Fatigue design curves for 6061-T6 aluminum Yahr, G.T. (1993) 346 /> Charpy impact test results on five materials and NIST verification specimens using instrumented 2-mm and 8-mm strikers Nanstad, R.K.; Sokolov, M.A. (1995) 241 /> Enhancing thermal conductivity of fluids with

  8. Microsoft Word - Wind Industry Work Order Information Flow Survey__WithSNLMarkings_Final.docx

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    In Mui ind nfor ir Data S Ind rma a Syste Sandia Jame MUIR DAT dust ation ems / W a Natio es Parle, Jona 1 TA SYSTEMS try W n Flo Wind E onal La athan Gibson 10/4/2013 S, INC. Wor ow Energy aborato n, Chad Reese rk O Sur y Techn ories e Orde rvey nologie er y es 1 Contents: 1.0 Executive Summary ................................................................................................................................. 3 2.0 Introduction

  9. Most Viewed Documents - Engineering | OSTI, US Dept of Energy, Office of

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Scientific and Technical Information - Engineering Conduction heat transfer solutions VanSant, J.H. (1980) Lunar Wireless Power Transfer Feasibility Study Sheldon Freid, et al. (2008) Charpy impact test results on five materials and NIST verification specimens using instrumented 2-mm and 8-mm strikers Nanstad, R.K.; Sokolov, M.A. (1995) Heat transfer model of above and underground insulated piping systems Kwon, K.C. (1998) Stress analysis and evaluation of a rectangular pressure vessel. [For

  10. The Business Case for Fuel Cells 2013: Reliability, Resiliency & Savings

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    The Business Case for Fuel Cells 2013 Reliability, Resiliency & Savings i Authors and Acknowledgements This report was written and compiled by Sandra Curtin and Jennifer Gangi of Fuel Cells 2000, an activity of the Breakthrough Technologies Institute in Washington, D.C. Special thanks to Peter Callowhill of NetGain Energy Advisors for contributing the PPA section and to Matthew Crescimanno and Eirik Mørk for assisting in research. Support was provided by the U.S. Department of Energy's

  11. Summary of On-Board Storage Models and Analyses | Department of Energy

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    On-Board Storage Models and Analyses Summary of On-Board Storage Models and Analyses Presentation by R.K. Ahluwalia at the Joint Meeting on Hydrogen Delivery Modeling and Analysis, May 8-9, 2007 PDF icon deliv_analysis_ahluwalia.pdf More Documents & Publications Potential Carriers and Approaches for Hydrogen Delivery Analyses of Hydrogen Storage Materials and On-Board Systems Technical Assessment of Organic Liquid Carrier Hydrogen Storage Systems for Automotive Applications

  12. Measurements of branching fraction ratios and CP-asymmetries in suppressed B-→ D(→ K+π-)K- and B-→ D(→ K+π-)π- decays

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aaltonen, T.

    2011-08-01

    We report the first reconstruction in hadron collisions of the suppressed decays B-→ D(→ K+π-)K- and B-→ D(→ K+π-)π- decays, sensitive to the CKM phase {gamma}, using data from 7 fb-1 of integrated luminosity collected by the CDF II detector at the Tevatron collider. We reconstruct a signal for the B-→ D(→ K+π-)K- suppressed mode with a significance of 3.2 standard deviations, and measure the ratios of the suppressed to favored branching fractions R(K) = [22.0 ± 8.6(stat) ± 2.6(syst)] x 10-3, R+(K) = [42.6 ± 13.7(stat) ± 2.8(syst)] x 10-3, R-(K) = [3.8 ± 10.3(stat) ± 2.7(syst)] x 10-3more » as well as the direct CP-violating asymmetry A(K) = -0.82±0.44(stat)±0.09(syst) of this mode. Corresponding quantities for B- → D(→ K+π-)π- decay are also reported.« less

  13. Measurements of branching fraction ratios and CP-asymmetries in suppressed B-→ D(→ K+π-)K- and B-→ D(→ K+π-)π- decays

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aaltonen, T.

    2011-08-01

    We report the first reconstruction in hadron collisions of the suppressed decays B-→ D(→ K+π-)K- and B-→ D(→ K+π-)π- decays, sensitive to the CKM phase {gamma}, using data from 7 fb-1 of integrated luminosity collected by the CDF II detector at the Tevatron collider. We reconstruct a signal for the B-→ D(→ K+π-)K- suppressed mode with a significance of 3.2 standard deviations, and measure the ratios of the suppressed to favored branching fractions R(K) = [22.0 ± 8.6(stat) ± 2.6(syst)] x 10-3, R+(K) = [42.6 ± 13.7(stat) ± 2.8(syst)] x 10-3, R-(K) = [3.8 ± 10.3(stat) ± 2.7(syst)] x 10-3more »as well as the direct CP-violating asymmetry A(K) = -0.82±0.44(stat)±0.09(syst) of this mode. Corresponding quantities for B- → D(→ K+π-)π- decay are also reported.« less

  14. Breakdown of ionic character of molecular alkali bromides in inner-valence photoionization

    SciTech Connect (OSTI)

    Karpenko, A. Iablonskyi, D.; Kettunen, J. A.; Cao, W.; Huttula, M.; Aksela, H.; Urpelainen, S.

    2014-05-28

    The inner-valence region of alkali bromide XBr (X=Li, Na, K, Rb) vapours has been studied experimentally by means of synchrotron radiation excited photoelectron spectroscopy. Experimental spectra were analyzed by comparing them with available theoretical results and previous experiments. Ionic character of alkali bromides is seen to change in the inner-valence region with increasing atomic number of the alkali atom. A mechanism involving mixing between Br 4s and Rb 4p orbitals has been suggested to account for the fine structure observed in inner-valence ionization region of RbBr.

  15. Ion-modulated nonlinear electronic transport in carbon nanotube

    Office of Scientific and Technical Information (OSTI)

    bundle/RbAg{sub 4}I{sub 5} thin film composite nanostructures (Journal Article) | SciTech Connect Ion-modulated nonlinear electronic transport in carbon nanotube bundle/RbAg{sub 4}I{sub 5} thin film composite nanostructures Citation Details In-Document Search Title: Ion-modulated nonlinear electronic transport in carbon nanotube bundle/RbAg{sub 4}I{sub 5} thin film composite nanostructures We have explored the ion-modulated electronic transport properties of mixed ionic-electronic conductor

  16. Chemical migration by contact metamorphism between pegmatite/country rocks: natural analogs for radionuclides migration. [Black Hills, South Dakota

    SciTech Connect (OSTI)

    Laul, J.C.; Walker, R.J.; Shearer, C.K.; Papike, J.J.; Simon, S.B.

    1983-10-01

    Comparison of trace element signatures of country rocks as a function of distance from the contact with two pegmatites, Tin Mountain and Etta, in the Black Hills of South Dakota, suggests that some elements such as K, Li, Rb, Cs, As, Sb, Zn and Pb, have migrated to distances of 4 to 40 meters during contact metamorphism. The relative degree of migration varies depending on the element. On the other hand, there is virtually no migration of rare earth elements (REE), Al, Sc, Cr, Hf, U, and Th. Biotite and muscovite are effective trace element traps for Li, Rb and Cs. Biotite has a greater affinity for Rb, Cs and Li than muscovite.

  17. Search for: All records | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    ... explore the transport properties of mixed ionic-electronic conductors made of carbon nanotubeRbAgsub 4Isub 5 film composite nanostructures in the presence of optical fields. ...

  18. Search for: All records | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    explore the transport properties of mixed ionic-electronic conductors made of carbon nanotubeRbAgsub 4Isub 5 film composite nanostructures in the presence of optical fields. ...

  19. CHRISTIAN SEIGNEUR

    Broader source: All U.S. Department of Energy (DOE) Office 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...

  20. Isotopes Products

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    are saving lives, advancing cutting-edge research and keeping the U.S. safe. Products stress and rest Stress and rest Rb-82 PET images in a patient with dipyridamole...

  1. FY 2009 Overall Contract and Project Management Improvement Performanc...

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    Improvement Performance Metrics and Targets PDF icon FY2009 1st Quarter RCAGAOOMB Attachment 2009-02-18 (2)(RB).pdf PDF icon FY2009 2nd Quarter RCAGAOOMB Attachment...

  2. Observation of Temperature-Induced Crossover to an Orbital-Selective...

    Office of Scientific and Technical Information (OSTI)

    Temperature-Induced Crossover to an Orbital-Selective Mott Phase in AxFe2-ySe2 (AK, Rb) Superconductors Citation Details In-Document Search Title: Observation of Temperature-Induc...

  3. Cesium iodide alloys

    DOE Patents [OSTI]

    Kim, Hyoun-Ee (Oak Ridge, TN); Moorhead, Arthur J. (Knoxville, TN)

    1992-01-01

    A transparent, strong CsI alloy havign additions of monovalent iodides. Although the perferred iodide is AgI, RbI and CuI additions also contribute to an improved polycrystalline CsI alloy.

  4. Core Analysis At Fenton Hill HDR Geothermal Area (Brookins &...

    Open Energy Info (EERE)

    Core Analysis Activity Date - 1983 Usefulness useful DOE-funding Unknown Notes See linked abstract for a synopsis of chemical analyses and Rb-Sr age determinations for gneissic...

  5. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Spectral Irradiance During CRYSTAL-FACE Pilewskie, P.(a), Guan, H.(b), Platnick, S.(c), Yang, P.(d), Bergstrom, R.(b), Wendisch, M.(e), Howard, S.(b), and Pommier, J.(b), Ames...

  6. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    ARM Aerosol IOP May 2003 Schwartz, S.E.(a), Ferrare R.(b), Ogren, J.E.(c), Daum, P.H.(a), Schmid, B.(d), and Ghan, S.(e), Brookhaven National Laboratory (a), NASA Langley Research...

  7. Consortium for Advanced Simulation of Light Water Reactors (CASL...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    in Drekar, CASL Technical Report: CASL-U-2012-0080-000, June 30, 2012. Bakosi, J., N. Barnett, M.A. Christon, M.M. Francois, R.B. Lowrie and R. Sankaran, Integration of Hydra-TH...

  8. The U.S. DOE Methane Hydrate R&D Program Publications and Presentation...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    ... Ecol., 77: 518-532. Hamdan, L.J., Coffin, R.B., Sikaroodi, M., Greinert, J., Treude, T., and Gillevet, P.M., 2012. Ocean currents shape the microbiome of Arctic marine sediments. ...

  9. Structure of the SPRY domain of human Ash2L and its interactions...

    Office of Scientific and Technical Information (OSTI)

    Structure of the SPRY domain of human Ash2L and its interactions with RbBP5 and DPY30 Citation Details In-Document Search Title: Structure of the SPRY domain of human Ash2L and its ...

  10. Complex States, Emergent Phenomena & Superconductivity in Intermetalli...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    expansion and lattice dynamics of RB66 compounds at low temperatures. Physics of the Solid State. 2014. 56, 2069-2076. Abstract Cho K ; Tanatar M A ; Ni N ; Prozorov R....

  11. Retinoblastoma protein co-purifies with proteasomal insulin-degrading enzyme: Implications for cell proliferation control

    SciTech Connect (OSTI)

    Radulescu, Razvan T., E-mail: ratura@gmx.net [Molecular Concepts Research (MCR), Muenster (Germany); Duckworth, William C. [Department of Medicine, Phoenix VA Health Care System, Phoenix, AZ (United States)] [Department of Medicine, Phoenix VA Health Care System, Phoenix, AZ (United States); Levy, Jennifer L. [Research Service, Phoenix VA Health Care System, Phoenix, AZ (United States)] [Research Service, Phoenix VA Health Care System, Phoenix, AZ (United States); Fawcett, Janet, E-mail: janet.fawcett@va.gov [Research Service, Phoenix VA Health Care System, Phoenix, AZ (United States)] [Research Service, Phoenix VA Health Care System, Phoenix, AZ (United States)

    2010-04-30

    Previous investigations on proteasomal preparations containing insulin-degrading enzyme (IDE; EC 3.4.24.56) have invariably yielded a co-purifying protein with a molecular weight of about 110 kDa. We have now found both in MCF-7 breast cancer and HepG2 hepatoma cells that this associated molecule is the retinoblastoma tumor suppressor protein (RB). Interestingly, the amount of RB in this protein complex seemed to be lower in HepG2 vs. MCF-7 cells, indicating a higher (cytoplasmic) protein turnover in the former vs. the latter cells. Moreover, immunofluorescence showed increased nuclear localization of RB in HepG2 vs. MCF-7 cells. Beyond these subtle differences between these distinct tumor cell types, our present study more generally suggests an interplay between RB and IDE within the proteasome that may have important growth-regulatory consequences.

  12. Celt Power Ltd | Open Energy Information

    Open Energy Info (EERE)

    United Kingdom Zip: SY16 1RB Sector: Wind energy Product: JV between Euros Energy Europe and ScottishPower to develop UK wind farms. References: Celt Power Ltd1 This article...

  13. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Implementing Flexible Cloud Vertical Structure in GFDL's AM-2 Large-Scale Model Using Stochastic Clouds Pincus, R.(a), Klein, S.A.(b), and Hemmler, R.(b), NOAA-CIRES Climate...

  14. Publications and Presentations at Scientific Meetings | Stanford

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Synchrotron Radiation Lightsource Publications and Presentations at Scientific Meetings Calendar Year 2014: †Denotes papers on which a university or other collaborator was the lead author. Alessi D.S., J.S. Lezama-Pacheco, J.E. Stubbs, M. Janousch, J.R. Bargar, P. Persson, and R. Bernier-Latmani (2014) The product of microbial uranium reduction includes multiple species with U(IV)-phosphate coordination, Geochim. Cosmochim. Acta, in press. †Qafoku, N.P., B.N. Gartman, R.K. Kukkadapu,

  15. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    AERI Observations in the Arctic: Monthly-Average Radiance Spectra and Longwave Cloud Radiative Forcing Walden, V.P., Revercomb, H.E., Knuteson, R.O., Best, F.A., Ciganovich, N., Dedecker, R.G., Dirkx, T., Garcia, R.K., Herbsleb, R., Howell, H.B., McRae, D., Short, J., and Tobin, D., Cooperative Institute of Mesoscale Meteorological Studies/Space Science and Engineering Center/University of Wisconsin Ninth Atmospheric Radiation Measurement (ARM) Science Team Meeting Atmospheric Emitted Radiance

  16. Laser Ionized Preformed Plasma at FACET (Conference) | SciTech Connect

    Office of Scientific and Technical Information (OSTI)

    Conference: Laser Ionized Preformed Plasma at FACET Citation Details In-Document Search Title: Laser Ionized Preformed Plasma at FACET Authors: Li, S.Z. ; /SLAC ; Adli, E. ; /SLAC /U. Oslo ; Clarke, C.I. ; Corde, S. ; Edstrom, S.A. ; Fisher, A.S. ; Frederico, J. ; Frisch, J.C. ; Gessner, S. ; Gilevich, S. ; Hering, P. ; Hogan, M.J. ; Jobe, R.K. ; Litos, M. ; May, J.E. ; Walz, D.R. ; Yakimenko ; /SLAC more »; Clayton, C.E. ; Joshi, C. ; Marsh, K.A. ; Vafaei-Najafabadi, N. ; /UCLA /Munich, Max

  17. R. K. Owen

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    R. K. Owen R. K. Owen Profile4x5 R.K.Owen R. K. Owen Ph.D. Sr Computer Systems Engineer Infrastructure Services National Energy Research Scientific Computing Center rkowen@lbl.gov Phone: (510) 486-7556 Fax: (510) 486-4340 Web: http://owen.sj.ca.us/rkowen/ Lawrence Berkeley National Laboratory 1 Cyclotron Road Mailstop 59R4010A Berkeley, CA 94720 US Biographical Sketch R.K. Owen received his Ph.D. in physics from UC Berkeley, specializing in atomic and molecular physics. His dissertation topic

  18. December 2015 Most Viewed Documents for Engineering | OSTI, US Dept of

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Energy, Office of Scientific and Technical Information Engineering Heat Treatment Procedure Qualification -- Final Technical Report Robert C. Voigt (2004) 776 Charpy impact test results on five materials and NIST verification specimens using instrumented 2-mm and 8-mm strikers Nanstad, R.K.; Sokolov, M.A. (1995) 546 Conduction heat transfer solutions VanSant, J.H. (1980) 527 Automotive vehicle sensors Sheen, S.H.; Raptis, A.C.; Moscynski, M.J. (1995) 373 Pressure and flow characteristics of

  19. December 2015 Most Viewed Documents for Materials | OSTI, US Dept of

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Energy, Office of Scientific and Technical Information Materials The influence of grain size on the mechanical properties ofsteel Morris Jr., J.W. (2001) 859 Heat Treatment Procedure Qualification -- Final Technical Report Robert C. Voigt (2004) 776 Fatigue design curves for 6061-T6 aluminum Yahr, G.T. (1993) 749 Charpy impact test results on five materials and NIST verification specimens using instrumented 2-mm and 8-mm strikers Nanstad, R.K.; Sokolov, M.A. (1995) 546 Mechanical properties

  20. April 2013 Most Viewed Documents for Materials | OSTI, US Dept of Energy,

    Office of Scientific and Technical Information (OSTI)

    Office of Scientific and Technical Information April 2013 Most Viewed Documents for Materials Science Subject Feed Fatigue design curves for 6061-T6 aluminum Yahr, G.T. (1993) 554 /> Charpy impact test results on five materials and NIST verification specimens using instrumented 2-mm and 8-mm strikers Nanstad, R.K.; Sokolov, M.A. (1995) 534 /> Heat Treatment Procedure Qualification -- Final Technical Report Robert C. Voigt (2004) 488 /> The influence of grain size on the mechanical

  1. Results From Plasma Wakefield Acceleration Experiments at FACET

    Office of Scientific and Technical Information (OSTI)

    (Conference) | SciTech Connect Results From Plasma Wakefield Acceleration Experiments at FACET Citation Details In-Document Search Title: Results From Plasma Wakefield Acceleration Experiments at FACET Authors: Li, S.Z. ; Clarke, C.I. ; England, R.J. ; Frederico, J. ; Gessner, S.J. ; Hogan, M.J. ; Jobe, R.K. ; Litos, M.D. ; Walz, D.R. ; /SLAC ; Muggli, P. ; /Munich, Max Planck Inst. ; An, W. ; Clayton, C.E. ; Joshi, C. ; Lu, W. ; Marsh, K.A. ; Mori, W. ; Tochitsky, S. ; /UCLA more »; Adli,

  2. PNWD

    Office of Legacy Management (LM)

    - - - - - -- - - - -- -- -- - - - - - - - - - - -- - - - - - - -- - - -- - --, PNWD -3802 Battelle 71u! Business a/Innovation Monticello Mill Ta:i.lings Site Macroinvertebrate Sampling for 2006 A.L. Bunn R.P. Mueller CA. Duberstein J.M. Brandenberger February 2007 Prepared for the U.S. Department of Ene rgy under Con tract DE-AC13-02GJ79491 DI SCLAIM ER This report was prepared as an account of wo rk spo nso red by an agency of th e United States Go vernment. N either th e United States G

  3. Richard King | Department of Energy

    Energy Savers [EERE]

    Richard King About Us Richard King - Director, Solar Decathlon RK Madrid3.jpg The Solar Decathlon is an award-winning competition that challenges teams to design, build, and demonstrate high-performance net zero energy homes. The two-year program culminates with a competition at a single site where the houses are on public display in a Solar Village. Mr. King created the inspiring collegiate competition in 2000 and has been its director for the past 15 years. Starting with the Solar Decathlon

  4. TO: FILE FROM: I SUBJECT:

    Office of Legacy Management (LM)

    TO: FILE FROM: I .- SUBJECT: 9EEEW Pos$:&&~ rk/ErvlK& @orzb Current: Lov?r_ &%2J*l&o3?fi; Owner contacted 0 yes &no; if yes, date contacted . TYPE OF OPERATION ----------------- q Research & Development @ Facility Type 0 Production scale testing 0 Pilot Scale & rlanuf acturing 0 Bench Scale Process 0 University 0 Theoretical Studies 0 Research Organizatil 0 Sample SC Analysis 0 Government Sponsarec 0 Other -------------_ q Production 0 Disposal /Storage TYPE CIF

  5. I

    Office of Legacy Management (LM)

    3S 3 I if 4 ; RADIOLOGICAL SURVEY OF THE LIQUID EFFLUENT DISPOSAL PATHWAYS FORMERLY USED BY LINDE AIR PRODUCTS DIVISION (Union Carbide Corporation) Tonawanda, New York P.W . Frame, J.D. Berger, C.F. Riemke, L.A. Young W .O. Helton, R.D. Condra, C.F. Weaver October 8, 1981 W o rk performed by Radiological Site Assessment Program Manpower Education, Research, and Training Division Oak Ridge Associated Universities Oak Ridge, Tennessee 37830 under Contract DE ACOS-76OROOO33 with the U.S. Department

  6. IO6490

    Office of Legacy Management (LM)

    1 ' f. (5 4 . . i/ IO6490 ~-~~ -Landfill, ' cleanup plan' is. expected by August peruneat OfEnergy tiy they hope mlxa~~amfari~cclcanupplan for four radioactive oitcs m the puwn of Tonawanda by early e- naidE.%rk,DOEsitcman- ~a,saidalltkrexarchandtech- fucd data cdkted at ctkc four 6ilc5 ha3 been forwarded ti his suptx.iors In WashingronJC. ' when it still awaits We' re still wal r .f$, co* liar iEP-+-* 6adMr. Wehmdaiinourd0cum8nu in February .bur unfommuely them' s a group in Wnshington we.

  7. IVASI I-

    Office of Legacy Management (LM)

    IVASI I- /& 1 -i /' / . /' A 1:' *' , tui POR-I RAI)IOI,OGICAI, sLlRvt:Y 01: 1' IlE SIblO?!DS s,w c STEEL Co!4'~Is'l R. W . Leggctt , J . Burden, bl. T. Ryan, D. L. Anderson, B. S. Ellis, and D. 3. Christian W o rk performed Health Physics Divisidn OAK RIDGE NATIOI\TAL LABOR4TORY Oak Ridge, Tennessee FEBRUARY 1977 for U. S. ENERGY RESEARCH AND DEVELOPblENT ADFIINISTRATION as part of The Radiological Surveys of Former Manhattan Engineering District/ Atomic Energy Commission Sites By .cc.ptmc.

  8. Mr. Carl Schafer Director of Environmental Policy

    Office of Legacy Management (LM)

    oi Energy rk rA$i Washington. DC 20545 .-~~~ ~ MY 2 9 1987 Mr. Carl Schafer Director of Environmental Policy Office of the Deputy Assistant Secretary of Defense for Installations Pentagon Washington, D.C. 20301 Dear Mr. Schafer: As you know, the Department of Energy (DOE) is implementing a program to identify sites that may. be radiologically contaminated as a result of DOE predecessor operations and to correct any problems associated with this contamination if there is DOE authority to do so.

  9. GABA/sub B/ receptor activation inhibits Ca/sup 2 +/-activated potassium channels in synaptosomes: involvement of G-proteins

    SciTech Connect (OSTI)

    Ticku, M.K.; Delgado, A.

    1989-01-01

    /sup 86/Rb-efflux assay from preloaded synaptosomes of rat cerebral cortex was developed to study the effect of GABA/sub B/ receptor agonist baclofen on Ca/sup 2 +/-activated K/sup +/-channels. Depolarization of /sup 86/Rb-loaded synaptosomes in physiological buffer increased Ca/sup 2 +/-activated /sup 86/Rb-efflux by 400%. The /sup 86/Rb-efflux was blocked by quinine sulfate, tetraethylammonium, and La/sup 3 +/ indicating the involvement of Ca/sup 2 +/-activated K/sup +/-channels. (-)Baclofen inhibited Ca/sup 2 +/-activated /sup 86/Rb-efflux in a stereospecific manner. The inhibitory effect of (-)baclofen was mediated by GABA/sub B/ receptor activation, since it was blocked by GABA/sub B/ antagonist phaclofen, but not by bicuculline. Further, pertussis toxin also blocked the ability of baclofen or depolarizing action to affect Ca/sup 2 +/-activated K/sup +/-channels. These results suggest that baclofen inhibits Ca/sup 2 +/-activated K/sup +/-channels in synaptosomes and these channels are regulated by G-proteins. This assay may provide an ideal in vitro model to study GABA/sub B/ receptor pharmacology.

  10. Effect of angiotensin II, ATP, and ionophore A23187 on potassium efflux in adrenal glomerulosa cells

    SciTech Connect (OSTI)

    Lobo, M.V.; Marusic, E.T.

    1986-02-01

    Angiotensin II stimulus on perifused bovine adrenal glomerulosa cells elicited an increase in 86Rb efflux from cells previously equilibrated with the radioisotope. When 45Ca fluxes were measured under similar conditions, it was observed that Ca and Rb effluxes occurred within the first 30 s of the addition of the hormone and were independent of the presence of external Ca. The 86Rb efflux due to angiotensin II was inhibited by quinine and apamin. The hypothesis that the angiotensin II response is a consequence of an increase in the K permeability of the glomerulosa cell membrane triggered by an increase in cytosolic Ca is supported by the finding that the divalent cation ionophore A23187 also initiated 86Rb or K loss (as measured by an external K electrode). This increased K conductance was also seen with 10(-4) M ATP. Quinine and apamin greatly reduced the effect of ATP or A23187 on 86Rb or K release in adrenal glomerulosa cells. The results suggest that Ca-dependent K channels or carriers are present in the membranes of bovine adrenal glomerulosa cells and are sensitive to hormonal stimulus.

  11. Chemical migration by contact metamorphism between pegmatite and country rocks: natural analogs for radionuclide migration

    SciTech Connect (OSTI)

    Laul, J.C.; Walker, R.J.; Shearer, C.K.; Papike, J.J.; Simon, S.B.

    1984-01-01

    Comparison of trace element signatures of country rocks as a function of distance from the contact with two pegmatites, Tin Mountain and Etta, in the Black Hills of South Dakota, suggests that some elements such as K, Li, Rb, Cs, As, Sb, Zn and Pb, have migrated to distances of 4 to 40 meters during contact metamorphism. The relative degree of migration varies depending on the element. On the other hand, there is virtually no migration of rare earth elements (REE), Al, Sc, Cr, Hf, U, and Th. Biotite and muscovite are effective trace element traps for Li, Rb, and Cs. Biotite has a greater affinity for Rb, Cs and Li than muscovite. 9 references, 5 figures, 1 table.

  12. Strong Second Harmonic Generation from the Tantalum Thioarsenates

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    A3Ta2AsS11 (A = K and Rb) | Energy Frontier Research Centers Strong Second Harmonic Generation from the Tantalum Thioarsenates A3Ta2AsS11 (A = K and Rb) Home Author: T.K. Bera, J.I. Jang, J.B. Ketterson, M.G. Kanatzidis Year: 2009 Abstract: The strongly anisotropic thioarsenates A(3)Ta(2)AsS(11) are stabilized in a polysulfide flux. All compounds contain the same parallel (1)/(infinity)[Ta(2)AsS(11)(3-)] polymeric anionic chains, but the size of the alkali-metals has a profound effect on the

  13. Synergistic extraction of some univalent cations into nitrobenzene by using cesium dicarbollylcobaltate and calix[4]arene-...

    SciTech Connect (OSTI)

    Makrlik, Emanuel; Selucky, P.; Vanura, Petr; Moyer, Bruce A

    2013-01-01

    From extraction experiments and c-activity measurements, the exchange extraction constants corresponding to the general equilibrium M+ (aq) + CsL+ (nb) , ML+ (nb) + Cs+ (aq) taking place in the two-phase water nitrobenzene system (M+ = K+, Rb+, NH+4,Ag+, Tl+; L = calix[4]arene-bis(t-octylbenzo-18-crown-6); aq = aqueous phase, nb = nitrobenzene phase) were evaluated. Furthermore, the stability constants of the ML+ complexes in nitrobenzene saturated with water were calculated; they were found to increase in the following cation order: NH+4 < K+ < Ag+ < Rb+ < Tl+.

  14. Isotopes Products

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Isotopes Products Isotopes Products Isotopes produced at Los Alamos National Laboratory are saving lives, advancing cutting-edge research and keeping the U.S. safe. Products stress and rest Stress and rest Rb-82 PET images in a patient with dipyridamole stress-inducible lateral wall and apical ischemia. (http://www.fac.org.ar/scvc/llave/image/machac/machaci.htm#f2,3,4) Strontium-82 is supplied to our customers for use in Sr-82/Rb-82 generator technologies. The generators in turn are supplied to

  15. Roof bolting equipment & technology

    SciTech Connect (OSTI)

    Fiscor, S.

    2009-04-15

    Technology provides an evaluator path to improvement for roof bolting machines. Bucyrus offers three different roof bolts models for various mining conditions. The LRB-15 AR is a single-arm boiler recommended for ranges of 32 inches and above; the dual-arm RB2-52A for ranges of 42 inches and above; and the dual-arm RB2-88A for ranges of 54 inches and above. Design features are discussed in the article. Developments in roof bolting technology by Joy Mining Machinery are reported. 4 photos.

  16. Cask weeping mitigation

    DOE Patents [OSTI]

    Krumhansl, James L. (Albuquerque, NM); Brady, Patrick V. (Albuquerque, NM); Teter, David M. (Edgewood, NM); McConnell, Paul (Albuquerque, NM)

    2007-09-18

    A method (and concomitant kit) for treating a surface to reduce subsequent .sup.137Cs nuclide desorption comprising contacting the surface with a first cation-containing solution, the cation being one or more of Cs.sup.+, Rb.sup.+, Ag.sup.+, Tl.sup.+, K.sup.+, and NH.sub.4.sup.+, and contacting the surface with a second cation-containing solution, the cation being one or more of Cs.sup.+, Rb.sup.+, Ag.sup.+, Tl.sup.+, K.sup.+, and NH.sub.4.sup.+, thereby reducing amounts of radioactive cesium embedded in clays found on the surface.

  17. Cesium iodide alloys

    DOE Patents [OSTI]

    Kim, H.E.; Moorhead, A.J.

    1992-12-15

    A transparent, strong CsI alloy is described having additions of monovalent iodides. Although the preferred iodide is AgI, RbI and CuI additions also contribute to an improved polycrystalline CsI alloy with outstanding multispectral infrared transmittance properties. 6 figs.

  18. Observation of ground-state Ramsey fringes

    SciTech Connect (OSTI)

    Weel, M.; Kumarakrishnan, A. [Department of Physics and Astronomy, York University, Toronto, Ontario, M3J 1P3 (Canada)

    2003-06-01

    We have used trapped {sup 85}Rb atoms to demonstrate an atom interferometric measurement of atomic recoil in the frequency domain. The measurement uses echo techniques to generate a Ramsey fringe pattern. The pattern exhibits recoil components consistent with theoretical predictions. We find the measurement to be insensitive to magnetic field gradients and discuss the prospects for a precision measurement of the recoil frequency.

  19. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Jr., W.L.(a), Doelling, D.R.(b), Heck, P.W.(c), Khaiyer, M.M.(b), Palikonda, R.(b), Young, D.F.(a), Spangenberg, D.A.(b), Chakrapani, V.(b), Walter, B.J.(b), and Nowicki,...

  20. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    the ARMNSA Site Brower, W.S.(a), Jensen, A.M.(a), Ivanoff, J. Sr.(a), Whiteman, D.(a), Wong, M.(a), Storvold, R.(b), Zak, B.D.(c), and Zirzow, J.(c), Ukpeagvik Iupiat Corporation...

  1. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    The Second ARM Diffuse Horizontal Irradiance Comparison Fall 2003 Michalsky, J.J.(a), Dolce, R.(b), Dutton, E.G.(c), Long, C.N.(d), Jeffries, W.Q.(e), McArthur, L.J.B.(f),...

  2. PAPERS PUBLISHED / 2005-2006 Progress in Research / Cyclotron...

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    C. Boudreau, F. Buchinger, J.E. Crawford, J.P. Greene, S. Gulick, J.C. Hardy, A.A. Hecht, A. Heinz, J.K.P. Lee, A.F. Levand, B.F. Lundgren, R.B. Moore, G. Savard, N.D....

  3. Observation

    Office of Scientific and Technical Information (OSTI)

    to an Orbital-Selective Mott Phase in A x Fe 2-y Se 2 (AK, Rb) Superconductors M. Yi, 1, 2 D. H. Lu, 3 R. Yu, 4 S. C. Riggs, 1, 2 J.-H. Chu, 1, 2 B. Lv, 5 Z. Liu, 1, 2 M. Lu,...

  4. 2004 ORAU/ORISE Bibliography

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Program At Rocky Flats. 2004. Aldrich, J.M., N.M. Daugherty, D.L. Cragle, E.D. Ellis, R.B. Falk, J. Follmer, F.J. Furman, D.J. Girardi, D. Hilmas, J.P. Watkins, and S.M....

  5. Nissan's new in-line DOHC six cylinder engine and its development

    SciTech Connect (OSTI)

    Ishida, Y.; Ito, K.; Kita, Y.; Kadowaki, S.

    1986-01-01

    The new RB20 engine series comprises in-line, 6-cylinder, 2-liter gasoline engines with an all-new design that succeed the L20 engine (1), whose performance has been upgraded numerous times since it was first released 20 years ago. The RB20 engine series includes a single-overhead-cam (SOHC) engine and a double-overhead-cam (DOHC) engine, each of which also has a turbocharged version, making a total of four different engine variations. This range of variations is intended to meet the broad, diversified needs of today's market. The main development theme set for the new engine family was to achieve ''improved performance that would appeal to the senses.'' Thus emphasis was not merely put on obtaining high performance figures, but on making real improvements in engine response and quietness that the driver could actually feel. This paper focuses on two of the four engine variations - the DOHC engine with and without a turbocharger. It discusses the basic engine construction, principal component parts and major development objectives. In the discussion that follows the DOHC engine without a turbocharger is referred to as RB20DE and the turbocharged DOHC engine is referred to as RB20DET.

  6. UCRL-JC-l20677 PREPRINT Detailed and Global Chemical Kinetics...

    Office of Scientific and Technical Information (OSTI)

    ... Kin., 26, 389, 1994. 4. Sutherland, J.W.; Patterson, P.M.; and Klemm, R.B.: J. Phys. ... Albuquerque, N.M., SAND87-8215B, 1987. 12. Wong, W.; and Davis, D.D.: Int. J. Chem. ...

  7. C. SIrENET

    Office of Legacy Management (LM)

    m. 61 12!?1/37 C. SIrENET PR jwnlrn RB-JUTA,000LffiBe kw4LV ID TM Ca#lsSION KSII~ ELECTRIC CL@'. VlTiiuFsf MRCS PL#il CMWIE-IELLa CYcLOTml FK

  8. Rapid quantification of mutant fitness in diverse bacteria by sequencing randomly bar-coded transposons

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Wetmore, Kelly M.; Price, Morgan N.; Waters, Robert J.; Lamson, Jacob S.; He, Jennifer; Hoover, Cindi A.; Blow, Matthew J.; Bristow, James; Butland, Gareth; Arkin, Adam P.; et al

    2015-05-12

    Transposon mutagenesis with next-generation sequencing (TnSeq) is a powerful approach to annotate gene function in bacteria, but existing protocols for TnSeq require laborious preparation of every sample before sequencing. Thus, the existing protocols are not amenable to the throughput necessary to identify phenotypes and functions for the majority of genes in diverse bacteria. Here, we present a method, random bar code transposon-site sequencing (RB-TnSeq), which increases the throughput of mutant fitness profiling by incorporating random DNA bar codes into Tn5 and mariner transposons and by using bar code sequencing (BarSeq) to assay mutant fitness. RB-TnSeq can be used with anymore » transposon, and TnSeq is performed once per organism instead of once per sample. Each BarSeq assay requires only a simple PCR, and 48 to 96 samples can be sequenced on one lane of an Illumina HiSeq system. We demonstrate the reproducibility and biological significance of RB-TnSeq with Escherichia coli, Phaeobacter inhibens, Pseudomonas stutzeri, Shewanella amazonensis, and Shewanella oneidensis. To demonstrate the increased throughput of RB-TnSeq, we performed 387 successful genome-wide mutant fitness assays representing 130 different bacterium-carbon source combinations and identified 5,196 genes with significant phenotypes across the five bacteria. In P. inhibens, we used our mutant fitness data to identify genes important for the utilization of diverse carbon substrates, including a putative D-mannose isomerase that is required for mannitol catabolism. RB-TnSeq will enable the cost-effective functional annotation of diverse bacteria using mutant fitness profiling. A large challenge in microbiology is the functional assessment of the millions of uncharacterized genes identified by genome sequencing. Transposon mutagenesis coupled to next-generation sequencing (TnSeq) is a powerful approach to assign phenotypes and functions to genes. However, the current strategies for TnSeq are too laborious to be applied to hundreds of experimental conditions across multiple bacteria. Here, we describe an approach, random bar code transposon-site sequencing (RB-TnSeq), which greatly simplifies the measurement of gene fitness by using bar code sequencing (BarSeq) to monitor the abundance of mutants. We performed 387 genome-wide fitness assays across five bacteria and identified phenotypes for over 5,000 genes. RB-TnSeq can be applied to diverse bacteria and is a powerful tool to annotate uncharacterized genes using phenotype data.« less

  9. Volume regulation by human lymphocytes. Role of calcium

    SciTech Connect (OSTI)

    Grinstein, S.; Dupre, A.; Rothstein, A.

    1982-05-01

    Human peripheral blood lymphocytes regulate their volumes in hypotonic solutions. In hypotonic media in which Na+ is the predominant cation, an initial swelling phase is followed by a regulatory volume decrease (RVD) associated with a net loss of cellular K+. In media in which K+ is the predominant cation, the rapid initial swelling is followed by a slower second swelling phase. /sup 86/Rb+ fluxes increased during RVD and returned to normal when the original volume was approximately regained. Effects similar to those induced by hypotonic stress could also be produced by raising the intracellular Ca++ level. In isotonic, Ca++-containing media cells were found to shrink upon addition of the Ca++ ionophore A23187 in K+-free media, but to swell in K+-rich media. Exposure to Ca++ plus A23187 also increased /sup 86/Rb+ fluxes. Quinine (75 microM), an inhibitor of the Ca++-activated K+ pathway in other systems blocked RVD, the associated K+ loss, and the increase in /sup 86/Rb+ efflux. Quinine also inhibited the volume changes and the increased /sup 86/Rb fluxes induced by Ca++ plus ionophore. The calmodulin inhibitors trifluoperazine, pimozide and chlorpromazine blocked RVD as well as Ca++ plus A23187-induced volume changes. Trifluoperazine also prevented the increase in /sup 86/Rb+ fluxes and K+ loss induced by hypotonicity. Chlorpromazine sulfoxide, a relatively ineffective calmodulin antagonist, was considerably less potent as an inhibitor of RVD than chlorpromazine. It is suggested than an elevation in cytoplasmic (Ca++), triggered by cell swelling, increases the plasma membrane permeability to K+, the ensuing increased efflux of K+, associated anions, and osmotically obliged water, leading to cell shrinking (RVD).

  10. GV DTit

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    £c £iV£d GV DTit «0- i3?0 ■ Comparison of 3D Classical Trajectory and Transition-State Theory Reaction Cross Sections t . ' G. W. Koeppl and M. Karplus Department of Chemistry, Harvard University Cambridge, Massachusetts 02138 -------------------------- L E G A L N O T I C E --------------------------- T h is r e p o r t was p re p a re d as an a c c o u n t o f w o rk sp onsored b y th e U n ite d S tates G o v e rn m e n t. N e ith e r th e U n ite d States n o r th e U n ite d S tates A

  11. Oak Ridge Site Specific Advisory Board * P.O. Box 2001, EM-91, Oak Ridge, TN 37831

    Office of Environmental Management (EM)

    Ridge Site Specific Advisory Board * P.O. Box 2001, EM-91, Oak Ridge, TN 37831 Phone: 865-241-4583, 865-241-4584, 1-800-382-6938 * Fax: 865-241-6932 * Internet: www.oakridge.doe.gov/em/ssab M Ma an ny y V Vo oi ic ce es s W Wo or rk ki in ng g f fo or r t th he e C Co om mm mu un ni it ty y O O a a k k R R i i d d g g e e S S i i t t e e S S p p e e c c i i f f i i c c A A d d v v i i s s o o r r y y B B o o a a r r d d September 11, 2014 Susan Cange Acting Manager Oak Ridge Office of

  12. I

    Office of Legacy Management (LM)

    v 6 ; , rg ;I x2.s I F$Z - ' i<G q 7322 : 5;" .f r? r, r; i 2, m it zp i 5 2' TX KP $2 3 2 -I - - ! 1. 3 : P 3 > : : + !, 3 a. n E 3 ; - - - = - - - 21 4 r g n E P- . i! P, rf P* 0 3 0 ch 2 4 1 0 . ' 9 2 s t r w * e I E . a -- l cn . r w cu . 2 P r . s 5 b2 2 8 t= "0 $ : cn ' 1 l ; 6 1 4 : ; co W. : a & . j* w ' t+ P i z c1. , 5 & i p tf -- ' is P ; $ r % tz % - - - = - -- 2 2 F s * ; 7 $ n s 2 K 3 a E rk Pa ml - - - 3 - -. - - - b ;: ; 5 r+ f f t 4. 3 5: n !, 9 : + - - -

  13. I M E M O R A N D U M T O

    Office of Legacy Management (LM)

    M E M O R A N D U M T O : FILE D A T E -------w----m-- F R O M :: /M1, L A U ------------e-e- S W J E C T : g/r'm n 'h a + ~ 'o n f l e c o w w n d a + t '~ ~ S ITE N A M E : /A C ios ?ith~fiC A L T E R N A T E ---w-------- ------------------_------- N A M E : ---------------------- CITY: 4 7 F u lfw S t N e b )/4rk -------------L------,,,,,_ S T A T E : N. 1: e - m -- O W N E R ( S ) .---me--- Past: ------------------------ Current: O w n e r contacted 0 yes a no; _-----------------------a- if

  14. Bonded Radii and the Contraction of the Electron Density of the Oxygen Atom by Bonded Interactions

    SciTech Connect (OSTI)

    Gibbs, Gerald V.; Ross, Nancy L.; Cox, David F.; Rosso, Kevin M.; Iversen, Bo B.; Spackman, M. A.

    2013-02-21

    The bonded radii for more than 550 bonded pairs of atoms, comprising more than 50 crystals, determined from experimental and theoretical electron density distributions, are compared with the effective ionic, ri(M), and crystal radii, rc(M), for metal atoms, M, bonded to O atoms. At odds with the fixed ionic radius of 1.40 , assumed for the O atom in the compilation of the ionic radii, the bonded radius for the atom, rb(O), is not fixed but displays a relatively wide range of values as the O atom is progressively polarized by the M-O bonded interactions: as such, rb(O) decreases systematically from 1.40 (the Pauling radius of the oxide anion) as bond lengths decrease when bonded to an electropositive atom like sodium, to 0.64 (Braggs atomic radius of the O atom) when bonded to an electronegative atom like nitrogen. Both rb(M) and rb(O) increase in tandum with the increasing coordination number of the M atom. The bonded radii of the M atoms are highly correlated with both ri(M) and rc(M), but they both depart systematically from rb(M) and become smaller as the electronegativity of the M atom increases and the M-O bond length decreases. The well-developed correlations between both sets of radii and rb(M) testifies to the relative precision of both sets of radii and the fact that both sets are highly correlated the M-O bond 1 lengths. On the other hand, the progressive departure of rb(O) from the fixed ionic radius of the O atom with the increasing electronegativity of the bonded M atom indicates that any compilation of sets of ionic radii, assuming that the radius for the oxygen atom is fixed in value, is problematical and impacts on the accuracy of the resulting sets of ionic and crystal radii thus compiled. The assumption of a fixed O atom radius not only results in a negative ionic radii for several atoms, but it also results in values of rb(M) that are much as ~ 0.6 larger than the ri(M) and rc(M) values, respectively, particularly for the more electronegative M atoms. On the other hand, the ionic radii are in closer agreement with rb(M) for the more electropositive atoms. Notwithstanding that ionic radii are typically smaller than bonded radii, particularly for the more electronegative atoms, they have been used with considerable success in understanding and rationalizing problems and properties in crystal chemistry primarily because both ionic and crystal radii are highly correlated on a one-to-one basis with both the bonded radii and the associated M-O bond lengths. The lack of agreement between the effective ionic and crystal radii and the bonded radii for the more shared bonded interactions is ascribed to the progressive increase in the polarization of the O atom by the bonded atoms with a concomitant decrease in its radius, a factor that was neglected in the compilation of ionic and crystal radii for fluorides, oxides, sulfides and nitrides. This accounts for ionic radii for these materials being smaller than the bonded radii for the more electronegative atoms.

  15. Identifying and Mitigating Potential Nutrient and Sediment Hot Spots under a Future Scenario in the Missouri River Basin

    SciTech Connect (OSTI)

    Wu, May; Zhang, Zhonglong

    2015-09-01

    Using the Soil and Water Assessment Tool (SWAT) for large-scale watershed modeling could be useful for evaluating the quality of the water in regions that are dominated by nonpoint sources in order to identify potential “hot spots” for which mitigating strategies could be further developed. An analysis of water quality under future scenarios in which changes in land use would be made to accommodate increased biofuel production was developed for the Missouri River Basin (MoRB) based on a SWAT model application. The analysis covered major agricultural crops and biofuel feedstock in the MoRB, including pasture land, hay, corn, soybeans, wheat, and switchgrass. The analysis examined, at multiple temporal and spatial scales, how nitrate, organic nitrogen, and total nitrogen; phosphorus, organic phosphorus, inorganic phosphorus, and total phosphorus; suspended sediments; and water flow (water yield) would respond to the shifts in land use that would occur under proposed future scenarios. The analysis was conducted at three geospatial scales: (1) large tributary basin scale (two: Upper MoRB and Lower MoRB); (2) regional watershed scale (seven: Upper Missouri River, Middle Missouri River, Middle Lower Missouri River, Lower Missouri River, Yellowstone River, Platte River, and Kansas River); and (3) eight-digit hydrologic unit (HUC-8) subbasin scale (307 subbasins). Results showed that subbasin-level variations were substantial. Nitrogen loadings decreased across the entire Upper MoRB, and they increased in several subbasins in the Lower MoRB. Most nitrate reductions occurred in lateral flow. Also at the subbasin level, phosphorus in organic, sediment, and soluble forms was reduced by 35%, 45%, and 65%, respectively. Suspended sediments increased in 68% of the subbasins. The water yield decreased in 62% of the subbasins. In the Kansas River watershed, the water quality improved significantly with regard to every nitrogen and phosphorus compound. The improvement was clearly attributable to the conversion of a large amount of land to switchgrass. The Middle Lower Missouri River and Lower Missouri River were identified as hot regions. Further analysis identified four subbasins (10240002, 10230007, 10290402, and 10300200) as being the most vulnerable in terms of sediment, nitrogen, and phosphorus loadings. Overall, results suggest that increasing the amount of switchgrass acreage in the hot spots should be considered to mitigate the nutrient loads. The study provides an analytical method to support stakeholders in making informed decisions that balance biofuel production and water sustainability.

  16. Spallation production of neutron deficient radioisotopes in North America

    SciTech Connect (OSTI)

    Jamriska, D.J.; Peterson, E.J.; Carty, J.

    1997-12-31

    The US Department of Energy produces a number of neutron deficient radioisotopes by high energy proton induced spallation reactions in accelerators at Los Alamos National Laboratory in New Mexico and Brookhaven National Laboratory in New York. Research isotopes are also recovered from targets irradiated at TRIUMF in British Columbia, Canada. The radioisotopes recovered are distributed for use in nuclear medicine, environmental research, physics research, and industry worldwide. In addition to the main product line of Sr-82 from either Mo or Rb targets, Cu-67 from ZnO targets, and Ge-68 and RbBr targets, these irradiation facilities also produce some unique isotopes in quantities not available from any other source such as Al-26, Mg-28, Si-32, Ti-44, Fe-52, Gd-148, and Hg-194. The authors will describe the accelerator irradiation facilities at the Los Alamos and Brookhaven National Laboratories. The high level radiochemical processing facilities at Los Alamos and brief chemical processes will be described.

  17. X-ray studies of concentrated aqueous solutions

    SciTech Connect (OSTI)

    Ludwig, K.F. Jr.; Warburton, W.K.; Fontaine, A.

    1987-07-01

    Concentrated aqueous solutions of three transition metal bromides (ZnBr/sub 2/, CuBr/sub 2/, and NiBr/sub 2/) and an alkali bromide (RbBr) have been studied with differential anomalous scattering (DAS) and extended x-ray absorption fine structure (EXAFS). The aq-ZnBr/sub 2/ solutions exhibit considerable inner-shell ion complexing with the formation of tetrahedral complexes about the Zn/sup 2 +/. In aq-CuBr/sub 2/, the Cu/sup 2 +/ has an octahedral coordination shell. Most of the anions are bound directly to the cations in both solutions. In contrast, there are only a few Ni--Br nearest neighbors in aq-NiBr/sub 2/. Instead, cations and anions share hydrating water molecules. Preliminary data show that any ion complexing in aq-RbBr must be weak. These results are in good agreement with published thermodynamic studies.

  18. Atom chip apparatus for experiments with ultracold rubidium and potassium gases

    SciTech Connect (OSTI)

    Ivory, M. K.; Ziltz, A. R.; Fancher, C. T.; Pyle, A. J.; Sensharma, A.; Chase, B.; Field, J. P.; Garcia, A.; Aubin, S.; Jervis, D.

    2014-04-15

    We present a dual chamber atom chip apparatus for generating ultracold {sup 87}Rb and {sup 39}K atomic gases. The apparatus produces quasi-pure Bose-Einstein condensates of 10{sup 4} {sup 87}Rb atoms in an atom chip trap that features a dimple and good optical access. We have also demonstrated production of ultracold {sup 39}K and subsequent loading into the chip trap. We describe the details of the dual chamber vacuum system, the cooling lasers, the magnetic trap, the multicoil magnetic transport system, the atom chip, and two optical dipole traps. Due in part to the use of light-induced atom desorption, the laser cooling chamber features a sufficiently good vacuum to also support optical dipole trap-based experiments. The apparatus is well suited for studies of atom-surface forces, quantum pumping and transport experiments, atom interferometry, novel chip-based traps, and studies of one-dimensional many-body systems.

  19. First Use of High Charge States for Mass Measurements of Short-Lived Nuclides in a Penning Trap

    SciTech Connect (OSTI)

    Ettenauer, S.; Gallant, A. T.; Dilling, J.; Simon, M. C.; Chaudhuri, A.; Mane, E.; Delheij, P.; Pearson, M. R.; Brunner, T.; Chowdhury, U.; Simon, V. V.; Brodeur, M.; Andreoiu, C.; Audi, G.; Lopez-Urrutia, J. R. Crespo; Ullrich, J.; Gwinner, G.; Lapierre, A.; Lunney, D.; Ringle, R.

    2011-12-30

    Penning trap mass measurements of short-lived nuclides have been performed for the first time with highly charged ions, using the TITAN facility at TRIUMF. Compared to singly charged ions, this provides an improvement in experimental precision that scales with the charge state q. Neutron-deficient Rb isotopes have been charge bred in an electron beam ion trap to q=8-12+ prior to injection into the Penning trap. In combination with the Ramsey excitation scheme, this unique setup creating low energy, highly charged ions at a radioactive beam facility opens the door to unrivaled precision with gains of 1-2 orders of magnitude. The method is particularly suited for short-lived nuclides such as the superallowed {beta} emitter {sup 74}Rb (T{sub 1/2}=65 ms). The determination of its atomic mass and an improved Q{sub EC} value are presented.

  20. Reply to “Comment on ‘Optically pumped spin-exchange polarized-electron source’ ”

    SciTech Connect (OSTI)

    Pirbhai, M.; Knepper, J.; Litaker, E. T.; Tupa, D.; Gay, T. J.

    2015-05-26

    In the proceeding Comment [1] on our recent report of a Rb spin-exchange polarized-electron source [2], Williams et al. contend: (a) that our source is poorly characterized compared with modern GaAs sources, (b) that we have overstated the difficulties of using GaAs photoemission sources, and (c) that our explanation of various physics issues related to the source's operating principles are not cogent.

  1. Improved ambient-pressure organic superconductor. [Bis(ethylenedithio)TTF-MX/sub 2/

    DOE Patents [OSTI]

    Williams, J.M.; Wang, Hsien-Hau; Beno, M.A.

    1985-05-29

    Disclosed is a new class of organic superconductors having the formula (ET)/sub 2/MX/sub 2/ wherein ET represents bis(ethylenedithio)-tetrathiafulvalene, M is a metal such as Au, Ag, In, Tl, Rb, Pd and the like and X is a halide. The superconductor (ET)/sub 2/AuI/sub 2/ exhibits a transition temperature of 5/sup 0/K which is high for organic superconductors.

  2. Reply to “Comment on ‘Optically pumped spin-exchange polarized-electron source’ ”

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Pirbhai, M.; Knepper, J.; Litaker, E. T.; Tupa, D.; Gay, T. J.

    2015-05-26

    In the proceeding Comment [1] on our recent report of a Rb spin-exchange polarized-electron source [2], Williams et al. contend: (a) that our source is poorly characterized compared with modern GaAs sources, (b) that we have overstated the difficulties of using GaAs photoemission sources, and (c) that our explanation of various physics issues related to the source's operating principles are not cogent.

  3. OFF-SITE SURVEILLANCE ACTIVITIES bF TFE

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    bF TFE \ !":! iri SOUTHWESTERN RbIOLQGICAL HEALTH LABORATORY \/ from July throtigh December 1969 Environmental-Surveillance Southwestern Radiological Health Laboratory ENVIROh'MENTAL PROTECTION AGEKCY February 1971 This surveillance pe.rfonned under a Memorandum of Understanding (No. SF 54 373) for the U. S. ATOMIC EKERGY COMXISSION SWRHL-98r OFF-SITE SURVEILLANCE ACTIVITIES OF THE SOUTHWESTERN RADIOLOGICAL HEALTH LABORATORY from July through December 1969 by Environmental Surveillance

  4. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Comparisons Between Measured and Modeled Longwave Irradiances During Arctic Winter: Results from the Second International Pyrgeometer and Absolute Sky-Scanning Radiometer Comparison (IPARSC-II) Marty, Ch.(a), Storvold, R.(a), Philipona, R.(b), Delamere, J.(c), Dutton, E.(d), Michalsky, J.(e), Stamnes, K.(f), Eide, H.(f), and Stoffel, T.(g), Geophysical Institute, University of Alaska Fairbanks (a), World Radiation Center, Davos, Switzerland (b), Atmospheric and Environmental Research, Boston

  5. Hospital Triage in the First 24 Hours after a Nuclear or Radiological Disaster

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Hospital Triage in the First 24 Hours after a Nuclear or Radiological Disaster Berger, ME; Leonard, RB; Ricks, RC; Wiley, AL; Lowry, PC; Flynn, DF Abstract: This article addresses the problems emergency physicians would face in the event of a nuclear or radiological catastrophe. It presents information about what needs to be done so that useful information will be gathered and reasonable decisions made in the all important triage period. A brief introductory explanation of radiation injury is

  6. Photoionization of optically trapped ultracold atoms with a high-power light-emitting diode

    SciTech Connect (OSTI)

    Goetz, Simone; Hoeltkemeier, Bastian; Amthor, Thomas; Weidemueller, Matthias [Physikalisches Institut, Universitaet Heidelberg, Im Neuenheimer Feld 226, 69120 Heidelberg (Germany)

    2013-04-15

    Photoionization of laser-cooled atoms using short pulses of a high-power light-emitting diode (LED) is demonstrated. Light pulses as short as 30 ns have been realized with the simple LED driver circuit. We measure the ionization cross section of {sup 85}Rb atoms in the first excited state, and show how this technique can be used for calibrating efficiencies of ion detector assemblies.

  7. September 2015 Most Viewed Documents for Environmental Sciences | OSTI, US

    Office of Scientific and Technical Information (OSTI)

    Dept of Energy, Office of Scientific and Technical Information September 2015 Most Viewed Documents for Environmental Sciences Separation of heavy metals: Removal from industrial wastewaters and contaminated soil Peters, R.W.; Shem, L. (1993) 285 Statistical methods for environmental pollution monitoring Gilbert, R.O. (1987) 126 Building a secondary containment system Broder, M.F. (1994) 121 Study of using oxygen-enriched combustion air for locomotive diesel engines Poola, R.B.; Sekar, R.

  8. FY2005 SSRLUO Executive Committee

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    5 Executive Committee corner corner Environmental Sciences Graduate Student LCLS Macromolecular Crystallography Materials Chemistry SSRL Liaison Structural Molecular Biology corner corner Juana Acrivos CSU San Jose, Chemistry, 1 Washington Square, SanJose, CA 95192-0101 Juana Acrivos has done experiments at SSRL since 1978. She is a chemist at SJSU (Professor). Her students first work at SSRL (Alan Robertson, Kevin Hathaway) showed how metal (Rb and Ba) in ammonia solutions change valence from 0

  9. FY2006 SSRLUO Executive Committee

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    6 Executive Committee corner corner Environmental Sciences Graduate Student LCLS Macromolecular Crystallography Materials Chemistry SSRL Liaison Biospectroscopy corner corner Juana Acrivos CSU San Jose, Chemistry, 1 Washington Square, SanJose, CA 95192-0101 Juana Acrivos has done experiments at SSRL since 1978. She is a chemist at SJSU (Professor). Her students first work at SSRL (Alan Robertson, Kevin Hathaway) showed how metal (Rb and Ba) in ammonia solutions change valence from 0 (in metallic

  10. Final Environmental Impact Statement

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    ... S o i l s cont a i n i ng h i gh amoun t s o f o rg an i c mat t e r and c l ay have a h i gh c apa c i ty t o a d s o rb ( i . e . , t ak e up and h o l d ) organ i c h e r b i c ...

  11. Ambient-pressure organic superconductor

    DOE Patents [OSTI]

    Williams, Jack M. (Downers Grove, IL); Wang, Hsien-Hau (Willowbrook, IL); Beno, Mark A. (Woodridge, IL)

    1986-01-01

    A new class of organic superconductors having the formula (ET).sub.2 MX.sub.2 wherein ET represents bis(ethylenedithio)-tetrathiafulvalene, M is a metal such as Au, Ag, In, Tl, Rb, Pd and the like and X is a halide. The superconductor (ET).sub.2 AuI.sub.2 exhibits a transition temperature of 5 K which is high for organic superconductors.

  12. Ambient-temperature superconductor symetrical metal-dihalide bis-(ethylenedithio)-tetrathiafulvalene compounds

    DOE Patents [OSTI]

    Williams, Jack M. (Downers Grove, IL); Wang, Hsien-Hau (Willowbrook, IL); Beno, Mark A. (Woodridge, IL)

    1987-01-01

    A new class of organic superconductors having the formula (ET).sub.2 MX.sub.2 wherein ET represents bis(ethylenedithio)-tetrathiafulvalene, M is a metal such as Au, Ag, In, Tl, Rb, Pd and the like and X is a halide. The superconductor (ET).sub.2 AuI.sub.2 exhibits a transition temperature of 5 K. which is high for organic superconductors.

  13. Microsoft PowerPoint - Garcia-Diaz - LiT Electrolysis Projects Summary V3

    Office of Environmental Management (EM)

    * Maroni is the Baseline for LiT Electrolysis * LLNL LDRD tries to improve molten salt liquid-liquid extraction and SRNL is contributing by investigating RbCl containing salts * SRNL LDRD tries process intensification to eliminate molten salt liquid-liquid extraction using advanced solid state electrolytes 2 3 * Upper Process shows generalized process flow diagram for Maroni Process * Lower right shows the simplification in the process flow diagram through the elimination of the liquid-liquid

  14. Process for the production of .sup.18 F-2-deoxy-2-fluoro-D-glucose

    DOE Patents [OSTI]

    Elmaleh, David R.; Levy, Shlomo; Shiue, Chyng-Yann; Wolf, Alfred P.

    1986-01-01

    Process for the production of 2-deoxy-2-fluoro-D-glucose and the corresponding .sup.18 F-compound in which methyl 4,6-O-benzylidine-3-O-methyl-2-O-trifluoromethanesulfonyl-.beta.-D-mannopy ranoside is reacted with a triflating reagent, the resulting compound reacted with CsHF.sub.2, RbF or the corresponding .sup.18 F-compounds, and thereafter the alkyl groups removed by hydrolysis.

  15. Investigation of refractory black carbon-containing particle morphologies using the single-particle soot photometer (SP2)

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Sedlacek, III, Arthur J.; Lewis, Ernie R.; Onasch, Timothy B.; Lambe, Andrew T.; Davidovits, Paul

    2015-07-24

    An important source of uncertainty in radiative forcing by absorbing aerosol particles is the uncertainty in their morphologies (i.e., the location of the absorbing substance on/in the particles). To examine the effects of particle morphology on the response of an individual black carbon-containing particle in a Single-Particle Soot Photometer (SP2), a series of experiments was conducted to investigate black carbon-containing particles of known morphology using Regal black (RB), a proxy for collapsed soot, as the light-absorbing substance. Particles were formed by coagulation of RB with either a solid substance (sodium chloride or ammonium sulfate) or a liquid substance (dioctyl sebacate),more » and by condensation with dioctyl sebacate, the latter experiment forming particles in a core-shell configuration. Each particle type experienced fragmentation (observed as negative lagtimes), and each yielded similar lagtime responses in some instances, confounding attempts to differentiate particle morphology using current SP2 lagtime analysis. SP2 operating conditions, specifically laser power and sample flow rate, which in turn affect the particle heating and dissipation rates, play an important role in the behavior of particles in the SP2, including probability of fragmentation. This behavior also depended on the morphology of the particles and on the thermo-chemical properties of the non-RB substance. Although these influences cannot currently be unambiguously separated, the SP2 analysis may still provide useful information on particle mixing states and black carbon particle sources.« less

  16. Investigation of refractory black carbon-containing particle morphologies using the single-particle soot photometer (SP2)

    SciTech Connect (OSTI)

    Sedlacek, III, Arthur J.; Lewis, Ernie R.; Onasch, Timothy B.; Lambe, Andrew T.; Davidovits, Paul

    2015-07-24

    An important source of uncertainty in radiative forcing by absorbing aerosol particles is the uncertainty in their morphologies (i.e., the location of the absorbing substance on/in the particles). To examine the effects of particle morphology on the response of an individual black carbon-containing particle in a Single-Particle Soot Photometer (SP2), a series of experiments was conducted to investigate black carbon-containing particles of known morphology using Regal black (RB), a proxy for collapsed soot, as the light-absorbing substance. Particles were formed by coagulation of RB with either a solid substance (sodium chloride or ammonium sulfate) or a liquid substance (dioctyl sebacate), and by condensation with dioctyl sebacate, the latter experiment forming particles in a core-shell configuration. Each particle type experienced fragmentation (observed as negative lagtimes), and each yielded similar lagtime responses in some instances, confounding attempts to differentiate particle morphology using current SP2 lagtime analysis. SP2 operating conditions, specifically laser power and sample flow rate, which in turn affect the particle heating and dissipation rates, play an important role in the behavior of particles in the SP2, including probability of fragmentation. This behavior also depended on the morphology of the particles and on the thermo-chemical properties of the non-RB substance. Although these influences cannot currently be unambiguously separated, the SP2 analysis may still provide useful information on particle mixing states and black carbon particle sources.

  17. Elementary excitations and universal interaction in Bose-Einstein condensates at large scattering lengths

    SciTech Connect (OSTI)

    Sarjonen, R.; Saarela, M.; Mazzanti, F.

    2011-10-15

    We present a theoretical analysis of excitation modes in Bose-Einstein condensates of ultracold alkali-metal gases for large scattering lengths, showing clear deviations from the Bogoliubov prediction as seen by Papp et al.[Phys. Rev. Lett. 101, 135301 (2008)]. We construct the atom-atom interaction by deriving the T matrix of such systems from two coupled (open and closed) channels assuming that the Feshbach resonance dominates the latter. We calculate molecular bound-state energies as a function of the magnetic field and compare with available experiments. The s-wave phase shifts determine the local effective interaction with long-ranged repulsion and short-ranged attraction. We show that it becomes a universal function at large scattering lengths. Finally, we use this interaction to characterize the ground-state and elementary excitations of {sup 85}Rb, {sup 87}Rb, and {sup 23}Na gases. Good agreement with line shift experiments in {sup 85}Rb is achieved. We find that, at large scattering lengths, Bragg scattering experiments could directly measure the momentum dependence of the effective two-body potential.

  18. Fabrication of nano Delafossite LiCo{sub 0.5}Fe{sub 0.5}O{sub 2} as the new adsorbent in efficient removal of reactive blue 5 from aqueous solutions

    SciTech Connect (OSTI)

    Khosravi, Iman; Yazdanbakhsh, Mohammad; Eftekhar, Melika; Haddadi, Zohreh

    2013-06-01

    Highlights: ? Fabrication of nano Delafossite LiCo{sub 0.5}Fe{sub 0.5}O{sub 2} by solgel method. ? Kinetic study of the adsorption properties. ? Removal of reactive blue 5 (RB5) as a reactive dye by the prepared new nanocatalyst. - Abstract: In this paper, nanoparticles of delafossite-type LiCo{sub 0.5}Fe{sub 0.5}O{sub 2} were prepared by solgel method in the presence of maleic acid as a chelating agent. The nanoparticles were characterized using differential thermal analysis, X-ray powder diffraction, Fourier infrared spectroscopy, transmission electron microscope, scanning electron microscopy and scanning tunneling microscopy. The nanoparticles showed the excellent adsorption properties towards reactive dye, reactive blue 5 (RB5). The adsorption studies were carried out at different pH values, various adsorbent dosages and contact time in a batch experiments. The kinetic studies indicate that the removal process obeys the second-order kinetic equation. Also, the isotherm evaluations reveal that the adsorption of RB5 by the nanoparticles follows the Freundlich model.

  19. Charging properties of cassiterite (alfa-SnO2) surfaces

    SciTech Connect (OSTI)

    Rosenqvist, Jorgen K; Machesky, Michael L.; Vlcek, L.; Cummings, Peter T; Wesolowski, David J

    2009-01-01

    The acid-base properties of cassiterite (alfa-SnO2) surfaces at 10 50 C were studied using potentiometric titrations of powder suspensions in aqueous NaCl and RbCl media. The proton sorption isotherms exhibited common intersection points in the pH-range 4.0 to 4.5 at all conditions and the magnitude of charging was similar but not identical in NaCl and RbCl. The hydrogen bonding configuration at the oxide-water interface, obtained from classical Molecular Dynamics (MD) simulations, was analyzed in detail and the results were explicitly incorporated in calculations of protonation constants for the reactive surface sites using the revised MUSIC model. The calculations indicated that the terminal SnOH2 group is more acidic than the bridging Sn2OH group, with protonation constants (log KH) of 3.60 and 5.13 at 25 C, respectively. This is contrary to the situation on the isostructural alfa-TiO2 (rutile), apparently due to the difference in electronegativity between Ti and Sn. MD simulations and speciation calculations indicated considerable differences in the speciation of Na+ and Rb+, despite the similarities in overall charging. Adsorbed sodium ions are almost exclusively found in bidentate surface complexes, while adsorbed rubidium ions form comparable amounts of bidentate and tetradentate complexes. Also, the distribution of adsorbed Na+ between the different complexes shows a considerable dependence on surface charge density (pH), while the distribution of adsorbed Rb+ is almost independent of pH. A Surface Complexation Model (SCM) capable of accurately describing both the measured surface charge and the MD predicted speciation of adsorbed Na+/Rb+ was formulated. According to the SCM, the deprotonated terminal group (SnOH-0.40) and the protonated bridging group (Sn2OH+0.36) dominate the surface speciation over the entire pH-range (2.7 10), illustrating the ability of positively and negatively charged surface groups to coexist. Complexation of the medium cations increases significantly with increasing negative surface charge and at pH 10 roughly 40 percent of the terminal sites are predicted to form cation complexes, while anion complexation is minor throughout the studied pH-range.

  20. HGSYSTEMUF6. Model for Simulating Dispersion due to Atmospheric Release of UF6

    SciTech Connect (OSTI)

    Hanna, G; Chang, J.C.; Zhang, J.X.; Bloom, S.G.; Goode, W.D. Jr; Lombardi, D.A.; Yambert, M.W.

    1998-08-01

    HGSYSTEMUF6 is a suite of models designed for use in estimating consequences associated with accidental, atmospheric release of Uranium Hexafluoride (UF6) and its reaction products, namely Hydrogen Fluoride (HF), and other non-reactive contaminants which are either negatively, neutrally, or positively buoyant. It is based on HGSYSTEM Version 3.0 of Shell Research LTD., and contains specific algorithms for the treatment of UF6 chemistry and thermodynamics. HGSYSTEMUF6 contains algorithms for the treatment of dense gases, dry and wet deposition, effects due to the presence of buildings (canyon and wake), plume lift-off, and the effects of complex terrain. The models components of the suite include (1) AEROPLUME/RK, used to model near-field dispersion from pressurized two-phase jet releases of UF6 and its reaction products, (2) HEGADAS/UF6 for simulating dense, ground based release of UF6, (3) PGPLUME for simulation of passive, neutrally buoyant plumes (4) UF6Mixer for modeling warm, potentially reactive, ground-level releases of UF6 from buildings, and (5) WAKE, used to model elevated and ground-level releases into building wake cavities of non-reactive plumes that are either neutrally or positively buoyant.

  1. Conference report on the 3rd international symposium on lithium application for fusion devices

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Mazzitelli, G.; Hirooka, Y.; Hu, J. S.; Mirnov, S. V.; Nygren, R.; Shimada, M.; Ono, M.; Tabares, F. L.

    2015-01-14

    The third International Symposium on Lithium Application for Fusion Device (ISLA-2013) was held on 9–11 October 2013 at ENEA Frascati Centre with growing participation and interest from the community working on more general aspect of liquid metal research for fusion energy development. ISLA-2013 has been confirmed to be the largest and the most important meeting dedicated to liquid metal application for the magnetic fusion research. Overall, 45 presentation plus 5 posters were given, representing 28 institutions from 11 countries. The latest experimental results from nine magnetic fusion devices were presented in 16 presentations from NSTX (PPPL, USA), FTU (ENEA, Italy),more » T-11M (Trinity, RF), T-10 (Kurchatov Institute, RF), TJ-II (CIEMAT, Spain), EAST(ASIPP, China), HT-7 (ASIPP, China), RFX (Padova, Italy), KTM (NNC RK, Kazakhstan). Sessions were devoted to the following: (I) lithium in magnetic confinement experiments (facility overviews), (II) lithium in magnetic confinement experiments (topical issues), (III) special session on liquid lithium technology, (IV) lithium laboratory test stands, (V) Lithium theory/modelling/comments, (VI) innovative lithium applications and (VII) special Session on lithium-safety and lithium handling. There was a wide participation from the fusion technology communities, including IFMIF and TBM communities providing productive exchange with the physics oriented magnetic confinement liquid metal research groups. This international workshop will continue on a biennial basis (alternating with the Plasma–Surface Interactions (PSI) Conference) and the next workshop will be held at CIEMAT, Madrid, Spain, in 2015.« less

  2. Conference report on the 3rd international symposium on lithium application for fusion devices

    SciTech Connect (OSTI)

    Mazzitelli, G.; Hirooka, Y.; Hu, J. S.; Mirnov, S. V.; Nygren, R.; Shimada, M.; Ono, M.; Tabares, F. L.

    2015-01-14

    The third International Symposium on Lithium Application for Fusion Device (ISLA-2013) was held on 9–11 October 2013 at ENEA Frascati Centre with growing participation and interest from the community working on more general aspect of liquid metal research for fusion energy development. ISLA-2013 has been confirmed to be the largest and the most important meeting dedicated to liquid metal application for the magnetic fusion research. Overall, 45 presentation plus 5 posters were given, representing 28 institutions from 11 countries. The latest experimental results from nine magnetic fusion devices were presented in 16 presentations from NSTX (PPPL, USA), FTU (ENEA, Italy), T-11M (Trinity, RF), T-10 (Kurchatov Institute, RF), TJ-II (CIEMAT, Spain), EAST(ASIPP, China), HT-7 (ASIPP, China), RFX (Padova, Italy), KTM (NNC RK, Kazakhstan). Sessions were devoted to the following: (I) lithium in magnetic confinement experiments (facility overviews), (II) lithium in magnetic confinement experiments (topical issues), (III) special session on liquid lithium technology, (IV) lithium laboratory test stands, (V) Lithium theory/modelling/comments, (VI) innovative lithium applications and (VII) special Session on lithium-safety and lithium handling. There was a wide participation from the fusion technology communities, including IFMIF and TBM communities providing productive exchange with the physics oriented magnetic confinement liquid metal research groups. This international workshop will continue on a biennial basis (alternating with the Plasma–Surface Interactions (PSI) Conference) and the next workshop will be held at CIEMAT, Madrid, Spain, in 2015.

  3. Model for Simulating Dispersion due to Atmospheric Release of UF6

    Energy Science and Technology Software Center (OSTI)

    1997-01-01

    HGSYSTEMUF6 is a suite of models designed for use in estimating consequences associated with accidental, atmospheric release of Uranium Hexafluoride (UF6) and its reaction products, namely Hydrogen Fluoride (HF), and other non-reactive contaminants which are either negatively, neutrally, or positively buoyant. It is based on HGSYSTEM Version 3.0 of Shell Research LTD., and contains specific algorithms for the treatment of UF6 chemistry and thermodynamics. HGSYSTEMUF6 contains algorithms for the treatment of dense gases, dry andmore » wet deposition, effects due to the presence of buildings (canyon and wake), plume lift-off, and the effects of complex terrain. The models components of the suite include (1) AEROPLUME/RK, used to model near-field dispersion from pressurized two-phase jet releases of UF6 and its reaction products, (2) HEGADAS/UF6 for simulating dense, ground based release of UF6, (3) PGPLUME for simulation of passive, neutrally buoyant plumes (4) UF6Mixer for modeling warm, potentially reactive, ground-level releases of UF6 from buildings, and (5) WAKE, used to model elevated and ground-level releases into building wake cavities of non-reactive plumes that are either neutrally or positively buoyant.« less

  4. The FIRST-2MASS Red Quasar Survey

    SciTech Connect (OSTI)

    Glikman, E; Helfand, D J; White, R L; Becker, R H; Gregg, M D; Lacy, M

    2007-06-28

    Combining radio observations with optical and infrared color selection--demonstrated in our pilot study to be an efficient selection algorithm for finding red quasars--we have obtained optical and infrared spectroscopy for 120 objects in a complete sample of 156 candidates from a sky area of 2716 square degrees. Consistent with our initial results, we find our selection criteria--J-K > 1.7,R-K > 4.0--yield a {approx} 50% success rate for discovering quasars substantially redder than those found in optical surveys. Comparison with UVX- and optical color-selected samples shows that {approx}> 10% of the quasars are missed in a magnitude-limited survey. Simultaneous two-frequency radio observations for part of the sample indicate that a synchrotron continuum component is ruled out as a significant contributor to reddening the quasars spectra. We go on to estimate extinctions for our objects assuming their red colors are caused by dust. Continuum fits and Balmer decrements suggest E(B-V) values ranging from near zero to 2.5 magnitudes. Correcting the K-band magnitudes for these extinctions, we find that for K {le} 14.0, red quasars make up between 25% and 60% of the underlying quasar population; owing to the incompleteness of the 2MASS survey at fainter K-band magnitudes, we can only set a lower limit to the radio-detected red quasar population of > 20-30%.

  5. NYO-7593 LECTIJHES ON DISPERSION THEORY

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    7593 LECTIJHES ON DISPERSION THEORY by Abduss S a lm Departiaent o f Physics U n iv e rsity o f R ochester R o ch ester, New York L E G A L N O T I C E T h is r e p o r t w as p r e p a r e d a s a n a c c o u n t o f G o v e m m e n t s p o n s o r e d w o rk . N e ith e r the U nited S ta te s , n o r th e C o m m is s io n , n o r any p e r s o n a c tin g on b e h a lf of th e C o m m issio n : A . M a k es any w a r r a n ty o r re p r e s e n ta tio n , e x p r e s s e d o r im p lie d , w

  6. Application of EPA wetland research program approach to a floodplain wetland restoration assessment.

    SciTech Connect (OSTI)

    Kolka, R., K.; Trettin, C., C.; Nelson, E., A.; Barton, C., D.; Fletcher, D., E.

    2002-01-01

    Kolka, R.K., C.C. Trettin, E.A. Nelson, C.D. Barton, and D.E. Fletcher. 2002. Application of the EPA Wetland Research Program Approach to a floodplain wetland restoration assessment. J. Env. Monitoring & Restoration 1(1):37-51. Forested wetland restoration assessment is difficult because of the timeframe necessary for the development of a forest ecosystem. The development of a forested wetland ecosystem includes the recovery of hydrology, soils, vegetation, and faunal communities. To assess forested wetland restoration projects, measures need to be developed that are sensitive to early changes in community development and are predictive of future conditions. In this study we apply the EPS's Wetland Research Program's (WRP) approach to assess the recovery of two thermally altered riparian wetland systems in South Carolina. In one of the altered wetland systems, approximately 75% of the wetland was planted with bottomland tree seedlings in an effort to hasten recovery. Individual studies addressing hydrology, soils, vegetation, and faunal communities indicate variable recovery responses.

  7. Harrods commissions new CHP station

    SciTech Connect (OSTI)

    Mullins, P.

    1994-04-01

    Three new combined heat and power (CHP) sets have recently been commissioned at Harrods, the world-famous department store in the heart of London's fashionable Knightsbridge district. The sets provide all the electricity needed by the store for lighting, heating and air-conditioning and are powered by Ruston 6RK270 turbocharged, charge-air-cooled diesel engines each producing 1392 kW at 750 r/min. These high power-to-weight ratio units were chosen in view of severe engine room space limitations. Low-grade waste heat is extracted from the engine jacket water to preheat water for three new boilers supplying some 1600 kg/h of steam for process heat to the store. The engines drive Brush BJS HW 10 100/8 alternators and are fully automatic in operation through a Regulateurs Europa control system. Some 600 sensors feed data into a Satchwell Building Management System (BMS). In the event of a breakdown, the engine control system can be switched to manual. 5 figs.

  8. Correlating sampling and intensity statistics in nanoparticle diffraction experiments

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Öztürk, Hande; Yan, Hanfei; Hill, John P.; Noyan, I. Cevdet

    2015-07-28

    It is shown in a previous article [Öztürk, Yan, Hill & Noyan (2014).J. Appl. Cryst.47, 1016–1025] that the sampling statistics of diffracting particle populations within a polycrystalline ensemble depended on the size of the constituent crystallites: broad X-ray peak breadths enabled some nano-sized particles to contribute more than one diffraction spot to Debye–Scherrer rings. Here it is shown that the equations proposed by Alexander, Klug & Kummer [J. Appl. Phys.(1948),19, 742–753] (AKK) to link diffracting particle and diffracted intensity statistics are not applicable if the constituent crystallites of the powder are below 10 nm. In this size range, (i) themore » one-to-one correspondence between diffracting particles and Laue spots assumed in the AKK analysis is not satisfied, and (ii) the crystallographic correlation between Laue spots originating from the same grain invalidates the assumption that all diffracting plane normals are randomly oriented and uncorrelated. Such correlation produces unexpected results in the selection of diffracting grains. For example, three or more Laue spots from a given grain for a particular reflection can only be observed at certain wavelengths. In addition, correcting the diffracted intensity values by the traditional Lorentz term, 1/cos θ, to compensate for the variation of particles sampled within a reflection band does not maintain fidelity to the number of poles contributing to the diffracted signal. A new term, cos θB/cos θ, corrects this problem.« less

  9. FORMERLY U T I L I Z E D MED/AEC S I T E S REMEDIAL ACTION PROGRAM

    Office of Legacy Management (LM)

    U T I L I Z E D MED/AEC S I T E S REMEDIAL ACTION PROGRAM RADIOLOGICAL SURVEY KENT CHEMICAL LAI3OMTORY U N I V E R S I T Y OF CHICAGO CHICAGO, I L L I N O I S September 7 - 1 3 , 1 9 7 7 Conducted by: Argonne N a t i o n a l L a b o r a t o r y . >IED/AEC Resurvey Group H e a l t h P h y s i c s S e c t i o n O c c u p a t i o n a l H e a l t h & S a f e t y D i v i s i o n f o r t h e : U . S . Department of Energy under Budget A c t i v i t y ERDA RK-01-05-02-3 and ANL 73706 C o n t r a

  10. DAx

    Office of Legacy Management (LM)

    r .*, J ".t , hj rk - DAx Jtdp -I 0 ' ,, i$i? m ;, ;. ESE p L, 21, ).,.G,,YlZ -w F M M c, !. ?Z-=S i%Df J,- :. ?i2& . ti. _ xri ?M SE t.' C z 39-&i stz-eet Fe-rbc;t.e L s;zewr A YI *- co2;$r-:-c' ,;c=;, & the 3ybb SFe& T&*-ehczfc Lnc!E:8ks 502 s*y-,"r=c rte2 ~2 i=GJwe ;ieAL*c--e ih ' ,be =a- ,y,z-t -._ **c -4 Qd"& F-5 Cs??lS' ,e' L XT 7, 3949. CCP L' s.S bt-""d -c, f oaf 22 ' ,be ba.a, tjg ,e$, cn$ op e-;_uf ~r:,t re>. >iz cs kriLcLt.ti on

  11. I

    Office of Legacy Management (LM)

    I , l ' I *; g j q / q / p - ; a _ . . . .o . P R E L IM I N A R Y S U R V E Y O F T H E F O R M E R G R A S S E L L I - R E S E A R C H L A B O R A T O R Y O F E .I. D U P O N T D E N E M O U R S A N D C O M P A N Y Cleveland, O h io W o rk p e r f o r m e d b y th e Health a n d S a fe ty R e s e a r c h Division O a k R i d g e N a tio n a l L a b o r a tory O a k R i d g e , T e n n e s s e e 3 7 8 3 0 M a r c h 1 9 8 0 O A K R I D G E N A T IO N A L L A B O R A T O R Y o p e r a te d b y U

  12. The mechanism of patulin's cytotoxicity and the antioxidant activity of indole tetramic acids

    SciTech Connect (OSTI)

    Riley, R.T.; Showker, J.L. )

    1991-06-01

    In LLC-PK1 cells exposed to patulin (50 microM), lipid peroxidation, abrupt calcium influx, extensive blebbing, and total LDH release appeared to be serially connected events with each representing a step in the loss of structural integrity of the plasma membrane. The aforementioned patulin-induced events were prevented by concurrent incubation with butylated hydroxytoluene, deferoxamine, and cyclopiazonic acid, a fungal metabolite. Patulin also caused depletion of nonprotein sulfhydryls, increased 86Rb+ efflux, dome collapse, and eventually the loss of cell viability. These events were not prevented by antioxidants, results consistent with the hypothesis that they were also serially connected but occurring parallel to those previously mentioned. The earliest events observed in patulin-treated cells were the decrease in nonprotein sulfhydryls and increase in 86Rb+ efflux (5 min) which occurred before statistically significant alterations in protein-bound sulfhydryls. The increased potassium efflux (86Rb+ efflux) occurred via a pathway distinct from BaCl2, quinine, or tetraethylammonium sensitive potassium channels. This is the first published report of the antioxidant activity of indole tetramic acids (cyclopiazonic acid and cyclopiazonic acid imine). The protective effect of tetramic acids in LLC-PK1 cells was restricted to indole tetramic acids, and their prevention of lipid peroxidation did not involve iron chelation. The results of this study demonstrate that cyclopiazonic acid is a potent inhibitor of azide-insensitive, ATP-dependent, a23187-sensitive calcium uptake by the lysate of LLC-PK1 cells. This result is consistent with the hypothesis that the endoplasmic reticulum calcium transport ATPase is a sensitive target for cyclopiazonic acid in LLC-PK1 cells.

  13. Validity of ELTB Equation for Suitable Description of BEC

    SciTech Connect (OSTI)

    Kim, Dooyoung; Kim, Jinguanghao; Yoon, Jin-Hee

    2005-10-17

    The Bose-Einstein condensation (BEC) has been found for various alkali-metal gases such as 7Li, 87Rb, Na, and H. For the description of atoms in this condensate state, the Gross-Pitaevskii (GP) equation has been widely used. However, the GP equation contains the nonlinear term, which makes this equation hard to solve. Therefore, physical quantities are usually obtained numerically, and sometimes it is difficult to extract a physical meaning from the calculated results. The nuclear theory group at Purdue University in the U.S. developed a new simple equation, the equivalent linear two-body (ELTB) equation, using the hyper-radius coordinates and tested it for one-dimensional BEC system. Their results are consistent with the numerical values from the GP equation within 4.5%.We test the validity of the ELTB equation for three-dimensional BEC system by calculating the energies per particle and the wave functions for 87Rb gas and for 7Li gas. We use the quantum-mechanical variational method for the BEC energy. Our result for 87Rb gas agrees with a numerical calculation based on the GP equation, with a relative error of 12% over a wide range of N from 100 to 10,000. The relative distances between particles for 7Li gas are consistent within a relative error of 17% for N {<=} 1300. The relatively simple form of the ELTB equation, compared with the GP equation, enables us to treat the N-body system easily and efficiently. We conclude that the ELTB equation is a powerful equation for describing BEC system because it is easy to treat.

  14. Nuclear Data Sheets for A = 75

    SciTech Connect (OSTI)

    Negret, Alexandru; Singh, Balraj

    2013-08-15

    The experimental nuclear spectroscopic data for known nuclides of mass number 75 (Fe, Co, Ni, Cu, Zn, Ga, Ge, As, Se, Br, Kr, Rb, Sr) have been evaluated and presented together with Adopted properties for levels and ? rays. New high-spin data are available for {sup 75}Ga, and {sup 75}Rb; and lifetime data for high-spin states in {sup 75}Br and {sup 75}Kr. For ?J =1, M1+E2 transitions in two rotational bands in {sup 75}Kr, several B(E2)(W.u.) values are anomalously high, deviating by 23 ? values from currently accepted RUL(E2) = 300. In the opinion of the evaluators, there is need to remeasure level lifetimes and multipole mixing ratios in {sup 75}Kr to resolve this serious discrepancy. New precise single-particle transfer cross section data are available for {sup 75}Ga, {sup 75}Ge, {sup 75}As and {sup 75}Se from several different reactions (2009Ka06,2008Sc03); these data give information for occupancy of valence neutron orbitals in the ground states of target nuclides: {sup 76}Ge, {sup 76}Se and {sup 78}Se. No significant new data since the 1999 NDS for A = 75 have been reported for {sup 75}As and {sup 75}Se. No data are yet available for excited states in {sup 75}Co, {sup 75}Ni and {sup 75}Sr. For {sup 75}Fe, only the isotopic identification is made with one observed event. The radioactive decay schemes of {sup 75}Co and {sup 75}Ni are unknown while those for {sup 75}Rb and {sup 75}Sr are incomplete. This work supersedes the data presented in the previous NDS evaluation of A = 75 published by 1999Fa05.

  15. The influence of pairing correlations on the isospin symmetry breaking corrections of superallowed Fermi beta decays

    SciTech Connect (OSTI)

    Cal Latin-Small-Letter-Dotless-I k, A. E.; Gerceklioglu, M.; Selam, C.

    2013-05-15

    Within the framework of quasi-particle random phase approximation, the isospin breaking correction of superallowed 0{sup +} {yields} 0{sup +} beta decay and unitarity of Cabibbo-Kobayashi-Maskawa mixing matrix have been investigated. The broken isotopic symmetry of nuclear part of Hamiltonian has been restored by Pyatov's method. The isospin symmetry breaking correction with pairing correlations has been compared with the previous results without pairing. The effect of pairing interactions has been examined for nine superallowed Fermi beta decays; their parent nuclei are {sup 26}Al, {sup 34}Cl, {sup 38}K, {sup 42}Sc, {sup 46}V, {sup 50}Mn, {sup 54}Co, {sup 62}Ga, {sup 74}Rb.

  16. Mixtures of Strongly Interacting Bosons in Optical Lattices

    SciTech Connect (OSTI)

    Buonsante, P.; Penna, V.; Giampaolo, S. M.; Illuminati, F.; Vezzani, A.

    2008-06-20

    We investigate the properties of strongly interacting heteronuclear boson-boson mixtures loaded in realistic optical lattices, with particular emphasis on the physics of interfaces. In particular, we numerically reproduce the recent experimental observation that the addition of a small fraction of {sup 41}K induces a significant loss of coherence in {sup 87}Rb, providing a simple explanation. We then investigate the robustness against the inhomogeneity typical of realistic experimental realizations of the glassy quantum emulsions recently predicted to occur in strongly interacting boson-boson mixtures on ideal homogeneous lattices.

  17. Conversion method of powder inelastic scattering data for one-dimensional systems

    SciTech Connect (OSTI)

    Tomiyasu, Dr. Keisuke; Fujita, Prof. Masaki; Kolesnikov, Alexander I; Bewley, Robert I.; Bull, Dr. Martyn J.; Bennington, Dr. Stephen M.

    2009-01-01

    Extracting dispersive magnetic excitations from inelastic neutron scattering data usually requires large single crystals. We present a simple yet powerful method for extracting such information from polycrystalline or powder data for one-dimensional systems. We demonstrate the effectiveness of this data treatment by extracting dispersion curves from powder inelastic neutron scattering data on the one-dimensional spin-half systems: CuGeO3 and Rb2Cu2Mo3O12. For many such materials it is not possible to grow sufficiently large crystals and this method offers a quick and efficient way to study their magnetic excitations.

  18. SSRLUO 2005 Executive Committee Members | Stanford Synchrotron Radiation

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Lightsource 5 Executive Committee Members Juana Acrivos CSU San Jose, Chemistry, 1 Washington Square, SanJose, CA 95192-0101 Juana Acrivos has done experiments at SSRL since 1978. She is a chemist at SJSU (Professor). Her students first work at SSRL (Alan Robertson, Kevin Hathaway) showed how metal (Rb and Ba) in ammonia solutions change valence from 0 (in metallic solutions) to ionic values as the dilution is increased. The dynamics of intercalation chemistry was investigated in the '80s

  19. SSRLUO 2006 Executive Committee Members | Stanford Synchrotron Radiation

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Lightsource 6 Executive Committee Members Juana Acrivos CSU San Jose, Chemistry, 1 Washington Square, SanJose, CA 95192-0101 Juana Acrivos has done experiments at SSRL since 1978. She is a chemist at SJSU (Professor). Her students first work at SSRL (Alan Robertson, Kevin Hathaway) showed how metal (Rb and Ba) in ammonia solutions change valence from 0 (in metallic solutions) to ionic values as the dilution is increased. The dynamics of intercalation chemistry was investigated in the '80s

  20. Shot-noise-limited magnetometer with sub-picotesla sensitivity at room temperature

    SciTech Connect (OSTI)

    Lucivero, Vito Giovanni; Anielski, Pawel; Gawlik, Wojciech; Mitchell, Morgan W.

    2014-11-15

    We report a photon shot-noise-limited (SNL) optical magnetometer based on amplitude modulated optical rotation using a room-temperature {sup 85}Rb vapor in a cell with anti-relaxation coating. The instrument achieves a room-temperature sensitivity of 70 fT/?(Hz) at 7.6 ?T. Experimental scaling of noise with optical power, in agreement with theoretical predictions, confirms the SNL behaviour from 5 ?T to 75??T. The combination of best-in-class sensitivity and SNL operation makes the system a promising candidate for application of squeezed light to a state-of-the-art atomic sensor.

  1. Spin Self-Rephasing and Very Long Coherence Times in a Trapped Atomic Ensemble

    SciTech Connect (OSTI)

    Deutsch, C.; Reinhard, F.; Schneider, T.; Laloee, F.; Reichel, J. [Laboratoire Kastler Brossel, ENS, UPMC, CNRS, 24 rue Lhomond, 75005 Paris (France); Ramirez-Martinez, F.; Lacroute, C.; Rosenbusch, P. [LNE-SYRTE, Observatoire de Paris, UPMC, CNRS, 61 av de l'Observatoire, 75014 Paris (France); Fuchs, J. N.; Piechon, F. [Laboratoire de Physique des Solides, CNRS UMR 8502, Univ. Paris-Sud, 91405 Orsay (France)

    2010-07-09

    We perform Ramsey spectroscopy on the ground state of ultracold {sup 87}Rb atoms magnetically trapped on a chip in the Knudsen regime. Field inhomogeneities over the sample should limit the 1/e contrast decay time to about 3 s, while decay times of 58{+-}12 s are actually observed. We explain this surprising result by a spin self-rephasing mechanism induced by the identical spin rotation effect originating from particle indistinguishability. We propose a theory of this synchronization mechanism and obtain good agreement with the experimental observations. The effect is general and may appear in other physical systems.

  2. Observation of a Topological and Parity-Dependent Phase of m=0 Spin States

    SciTech Connect (OSTI)

    Usami, Koji [PRESTO, Japan Science and Technology Agency, 3-5, Sanbancho, Chiyodaku, Tokyo 332-0012 (Japan); Department of Physics, Tokyo Institute of Technology, 2-12-1 O-okayama, Meguro-ku, Tokyo 152-8550 (Japan); Kozuma, Mikio [Department of Physics, Tokyo Institute of Technology, 2-12-1 O-okayama, Meguro-ku, Tokyo 152-8550 (Japan); CREST, Japan Science and Technology Agency, 3-5, Sanbancho, Chiyodaku, Tokyo 332-0012 (Japan)

    2007-10-05

    A Ramsey interrogation scheme was used to measure the phase shift of laser-cooled {sup 87}Rb clock-transition pseudospins arising as a result of a reversal of a bias-magnetic field, i.e., B{yields}-B, during the interrogation. While no phase shift occurred when the reversal was sudden, the Ramsey fringes were shifted by a factor of {pi} when the reversal was adiabatic. We thus verified the prediction that the spin states |F,m=0> acquire a purely topological and parity-dependent phase factor of (-1){sup F} as a result of B{yields}-B.

  3. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    The Use of Performance Metrics to Enhance Meteorological Operations Jakob, C.(a), Pincus, R.(b), Hannay, C.(b), and Xu, K.-M.(c), BMRC (a), NOAA/CIRES CDC (b), NASA Langley (c) Thirteenth Atmospheric Radiation Measurement (ARM) Science Team Meeting It is highly desirable to use cloud radar data in the evaluation of model simulations of clouds at various scales. Unfortunately there is an inherent mismatch between the spatial and temporal scales of the models and the observations. Usually this

  4. ARM - Publications: Science Team Meeting Documents

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    The Site and Computer Access Request System Doty, K.J.(a), Eagan, R.(b), Sisterson, D.L.(b), and Wagener, R.(a), Brookhaven National Laboratory (a), Argonne National Laboratory (b) The implementation and use of a collection of web-based tools for a Site and Computer Access Request system is presented. The system is used by ARM to provide advance notice of on-site visits to site managers in order to coordinate support as well as to provide a mechanism for managing remote and on-site access to ARM

  5. Recipient: Colorado State University

    Office of Scientific and Technical Information (OSTI)

    of work under Grant DE-FG02-96ER14647 Recipient: Colorado State University Office of Sponsored Programs Fort Collins, CO 80523 Grant Period: Sept. 1, 1996 - May 31, 2015 Principal Investigator: Stephen R. Lundeen This project originated with the desire to apply the dense CW Rb Rydberg target, developed by the PI under previous NSF support, to the study of collisions between highly-charged ions (HCI) and Rydberg atoms. The feasibility of such studies was demonstrated in initial unfunded studies

  6. Local surface plasmon mediated extraordinary optical transmission of multi-spatial-mode quantum noise reduction

    SciTech Connect (OSTI)

    Lawrie, Benjamin J; Evans, Philip G; Pooser, Raphael C

    2013-01-01

    We demonstrate the coherent transduction of quantum noise reduction, or squeezed light, by Ag localized surface plasmons (LSPs). Squeezed light, generated through four-wave-mixing in Rb vapor, is coupled to a Ag nanohole array designed to exhibit LSP mediated extraordinary-optical transmission (EOT) spectrally coincident with the squeezed light source at 795 nm. We demonstrate that quantum noise reduction as a function of transmission is found to match closely with linear attenuation models, thus demonstrating that the photon-LSP-photon transduction process is coherent near the LSP resonance.

  7. Hydra-TH: A Thermal-Hydraulics Code for Nuclear Reactor Applications

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Hydra-TH: A Thermal-Hydraulics Code for Nuclear Reactor Applications Idaho National Laboratory and Los Alamos National Laboratory R.R. Nourgaliev, M.A. Christon, J. Bakosi, R.B. Lowrie, L.A. Pritchett- Sheats May 12-17, 2013: CASL-U-2013-0100-000 Fifteenth International Topical Meeting on Nuclear Reactor Thermal Hydraulics (NURETH-15) NURETH15-636 Pisa, Italy, May 12 - 17, 2013. Hydra-TH: A Thermal-Hydraulics Code for Nuclear Reactor Applications R.R. Nourgaliev Nuclear Science & Technology,

  8. Café Systems Express Access Form

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    Café Systems Express Access Form Job Aid 7/18/12 - rb Café Systems Express Access Form - Job Aid NEED HELP? Call 847-491-HELP consultant@northwestern.edu © 2012 Northwestern University Page 1 of 3 Follow these steps to complete the Café Systems Express Access Form. For access not indicated by the roles below, use the General Security Access Form instead. 1. Select Applicant Information checkboxes (as applicable).  Enter Date, NetID, Name, EMPLID (employee ID number), title, department

  9. Nuclear Data Sheets for A = 91

    SciTech Connect (OSTI)

    Baglin, Coral M.

    2013-10-15

    Experimental nuclear structure and decay data for all known A=91 nuclides (As, Se, Br, Kr, Rb, Sr, Y, Zr, Nb, Mo, Tc, Ru, Rh, Pd) have been evaluated. This evaluation, covering data received by 1 September 2013, supersedes the 1998 evaluation by C. M. Baglin published in Nuclear Data Sheets86, 1 (1999) (15 December 1998 literature cutoff), and subsequent evaluations by C. M. Baglin added to the ENSDF database for Kr, Sr and Zr (29 December 2000 literature cutoff) and by B. Singh for {sup 91}Tc (6 November 2000 literature cutoff)

  10. Nuclear Data Sheets for A=85

    SciTech Connect (OSTI)

    Singh, Balraj; Chen, Jun

    2014-02-01

    Evaluated experimental data are presented for 13 known nuclides of mass 85 (Zn, Ga, Ge, As, Se, Br, Kr, Rb, Sr, Y, Zr, Nb, Mo). Since the previous 1990 evaluation of A=85, {sup 85}Zn, {sup 85}Ga, {sup 85}Ge and {sup 85}nuclides are newly added here. Excited state data for {sup 85}Se, {sup 85}Zr have become available from radioactive decay and inbeam ?ray studies. New and improved highspin data are available for {sup 85}Br, {sup 85}Kr, {sup 85}Rb, {sup 85}Y, {sup 85}Nb and {sup 85}Mo. New direct and precise measurement of atomic masses of {sup 85}Ge, {sup 85}As, {sup 85}Se, {sup 85}Br, {sup 85}Rb, {sup 85}Zr, {sup 85}Nb and {sup 85}Mo have greatly improved the landscape of ? decayQ values and separation energies in this mass region. In spite of extensive experimental work on the isobaric nuclei of this mass chain several deficiencies remain. No excited states are known in {sup 85}Zn, {sup 85}Ga, {sup 85}As. Only a few excited state are assigned in {sup 85}Ge from {sup 85}Ga ? decay. From radioactivity studies, the decay schemes of {sup 85}Zn and {sup 85}Mo are not known, and those for {sup 85}Ga, {sup 85}Ge, {sup 85}As and 10.9s isomer of {sup 85}Zr are incomplete. Level lifetimes are not known for excited states in {sup 85}Se, {sup 85}Br, {sup 85}Nb and {sup 85}Mo. The {sup 85}Tc nuclide has not been detected in fragmentation experiments at GANIL, alluding to its unbound nature for proton emission. The {sup 85}Kr, {sup 85}Rb, {sup 85}Sr, and {sup 85}Y nuclides remain the most extensively studied from many different reactions and decays. The evaluation of A=85 nuclides has been done after a span of 23 years, thus includes an extensive amount of new data for almost each nuclide. This work supersedes the data for A=85 nuclides presented in earlier full NDS publication by J. Tepel in 1980Te04 and a later one published in an update mode by H. Sievers in 1991Si01.

  11. Nuclear Data Sheets for A = 92

    SciTech Connect (OSTI)

    Baglin, Coral M.

    2012-10-15

    Nuclear structure and decay data pertaining to all nuclides with mass number A = 92 (As, Se, Br, Kr, Rb, Sr, Y, Zr, Nb, Mo, Tc, Ru, Rh, Pd) have been compiled and evaluated, and incorporated into the ENSDF data file. All literature available by 15 September 2012 has been considered. This evaluation supersedes the previous publication for this mass chain (Coral M. Baglin, Nuclear Data Sheets 91, 423 (2000) (November 2000 cutoff date)), and subsequent unpublished reevaluations by C.M. Baglin for {sup 92}Kr (January 2004 literature cut-off) and {sup 92}Sr (August 2003 literature cut-off).

  12. A clip-on Zeeman slower using toroidal permanent magnets

    SciTech Connect (OSTI)

    Krzyzewski, S. P.; Akin, T. G.; Dahal, Parshuram; Abraham, E. R. I.

    2014-10-15

    We present the design of a zero-crossing Zeeman slower for {sup 85}Rb using rings of flexible permanent magnets. The design is inexpensive, requires no power or cooling, and can be easily attached and removed for vacuum maintenance. We show theoretically that such a design can reproduce a magnetic field profile of a standard zero-crossing Zeeman slower. Experimental measurements of a prototype and comparisons to theoretical simulations demonstrate the feasibility of the design and point toward future improvements. Simulations show an atom flux similar to other Zeeman slowers.

  13. A new method for measurement of safety rod drop times

    SciTech Connect (OSTI)

    Pesic, M.; Stefanovic, D. ); Marinkovic, P. )

    1992-10-01

    In this paper, a new method for the accurate measurement of safety rod drop times is proposed. It is based on a fast electromagnetic transducer and an analog-to-digital converter (ADC) conected to a computer system. Evaluation of recorded data is conducted by a developed computer code. The first measurements performed at the HERBE fast-thermal RB reactor show that a relative uncertainty (confidence level 95%) of less than 6% can be achieved in determination of rod drop time (with time intervals ranging from 0.4-10.0 s). Further improvements in accuracy are possible.

  14. TRIPlDpl

    Office of Legacy Management (LM)

    TRIPlDpl f??Wld~. It.D. .nme a, 19% w-0 E. n. camBmult OBJECTIVE OP TRIP: this trip eaa -de to observe the operetion and to mke reoom- mendatioaa from a health and sefety standpoint during the process of compauting emall pleues of thorium metal into an eleotrode* to aonduat a health and safety survey, and to advice on the p&per decontamlmation mthoda after the oapaotlng oper&lOn ~88 completed. COXCLUSIONS AND RB~TIONSr During the compacting operation full protective alothingj JRmt- ',I'

  15. The Secretary of Energy'

    Office of Legacy Management (LM)

    ? >g*+. , . dc*rb&.+ :c-r.3-b. g ;.i' 8 . I. ' . . 3 @ g. -- Q ' \ 4,: 6 L;Is)zLTEsdi# ' -. . ! h -. The Secretary of Energy' Washington, bC 20585 u , October 10, 1997 ' The .Honorabie William S . Cohen Secretary ofDefense Washington, D.C. 20301 -' &arMr. Secietary: !I " .,.. *- . = . . # ' The Congress recently se@ to the President for signature the Energy and Water ,, Development Appropriations Act, 1998. Among other provisions, this bill would immediately transfer

  16. T PamI J. I(. u!borekl

    Office of Legacy Management (LM)

    mr a. L. khbert - mchn:aal Director T PamI J. I(. u!borekl r&&r r.B.0. Produotlon Order Eo. 304 Sat' ional Lead Ia to furnieh Brld&eporf- Braem Company In Adrian, Ulchlmm, aachlned hollow &rtmelon bllleto for uev.;;: in prodaoing extruded hollow urenlum rod etodb , The extrwlon program oos ' . aleta of two parts; one, fabrloetion of nowal uranium hollow extrusion billet8 iroa WOW lqote and, two. fkbrlcatlon of both $10~ urenlm and n0ma.l ?reninm hollow extrusion billet8 from

  17. A C-terminal Hydrophobic, Solvent-protected Core and a Flexible N-terminus are Potentially Required for Human Papillomavirus 18 E7 Protein Functionality

    SciTech Connect (OSTI)

    Liu, S.; Tian, Y; Greenaway, F; Sun, M

    2010-01-01

    The oncogenic potential of the high-risk human papillomavirus (HPV) relies on the expression of genes specifying the E7 and E6 proteins. To investigate further the variation in oligomeric structure that has been reported for different E7 proteins, an HPV-18 E7 cloned from a Hispanic woman with cervical intraepithelial neoplasia was purified to homogeneity most probably as a stable monomeric protein in aqueous solution. We determined that one zinc ion is present per HPV-18 E7 monomer by amino acid and inductively coupled plasma-atomic emission spectroscopy analysis. Intrinsic fluorescence and circular dichroism spectroscopic results indicate that the zinc ion is important for the correct folding and thermal stability of HPV-18 E7. Hydroxyl radical mediated protein footprinting coupled to mass spectrometry and other biochemical and biophysical data indicate that near the C-terminus, the four cysteines of the two Cys-X{sub 2}-Cys motifs that are coordinated to the zinc ion form a solvent inaccessible core. The N-terminal LXCXE pRb binding motif region is hydroxyl radical accessible and conformationally flexible. Both factors, the relative flexibility of the pRb binding motif at the N-terminus and the C-terminal metal-binding hydrophobic solvent-protected core, combine together and facilitate the biological functions of HPV-18 E7.

  18. Optical polarizer material

    DOE Patents [OSTI]

    Ebbers, C.A.

    1999-08-31

    Several crystals have been identified which can be grown using standard single crystals growth techniques and which have a high birefringence. The identified crystals include Li.sub.2 CO.sub.3, LiNaCO.sub.3, LiKCO.sub.3, LiRbCO.sub.3 and LiCsCO.sub.3. The condition of high birefringence leads to their application as optical polarizer materials. In one embodiment of the invention, the crystal has the chemical formula LiK.sub.(1-w-x-y) Na.sub.(1-w-x-z) Rb.sub.(1-w-y-z) Cs.sub.(1-x-y-z) CO.sub.3, where w+x+y+z=1. In another embodiment, the crystalline material may be selected from a an alkali metal carbonate and a double salt of alkali metal carbonates, where the polarizer has a Wollaston configuration, a Glan-Thompson configuration or a Glan-Taylor configuration. A method of making an LiNaCO.sub.3 optical polarizer is described. A similar method is shown for making an LiKCO.sub.3 optical polarizer.

  19. Optical polarizer material

    DOE Patents [OSTI]

    Ebbers, Christopher A. (Livermore, CA)

    1999-01-01

    Several crystals have been identified which can be grown using standard single crystals growth techniques and which have a high birefringence. The identified crystals include Li.sub.2 CO.sub.3, LiNaCO.sub.3, LiKCO.sub.3, LiRbCO.sub.3 and LiCsCO.sub.3. The condition of high birefringence leads to their application as optical polarizer materials. In one embodiment of the invention, the crystal has the chemical formula LiK.sub.(1-w-x-y) Na.sub.(1-w-x-z) Rb.sub.(1-w-y-z) Cs.sub.(1-x-y-z) CO.sub.3, where w+x+y+z=1. In another embodiment, the crystalline material may be selected from a an alkali metal carbonate and a double salt of alkali metal carbonates, where the polarizer has a Wollaston configuration, a Glan-Thompson configuration or a Glan-Taylor configuration. A method of making an LiNaCO.sub.3 optical polarizer is described. A similar method is shown for making an LiKCO.sub.3 optical polarizer.

  20. Cation Uptake and Allocation by Red Pine Seedlings under Cation-Nutrient Stress in a Column Growth Experiment

    SciTech Connect (OSTI)

    Shi, Zhenqing; Balogh-Brunstad, Zsuzsanna; Grant, Michael R.; Harsh, James B.; Gill, Richard; Thomashow, Linda; Dohnalkova, Alice; Stacks, Daryl; Letourneau, Melissa; Keller, Chester K.

    2014-01-10

    Background and Aims Plant nutrient uptake is affected by environmental stress, but how plants respond to cation-nutrient stress is poorly understood. We assessed the impact of varying degrees of cation-nutrient limitation on cation uptake in an experimental plant-mineral system. Methods Column experiments, with red pine (Pinus resinosa Ait.) seedlings growing in sand/mineral mixtures, were conducted for up to nine months under a range of Ca- and K-limited conditions. The Ca and K were supplied from both minerals and nutrient solutions with varying Ca and K concentrations. Results Cation nutrient stress had little impact on carbon allocation after nine months of plant growth and K was the limiting nutrient for biomass production. The Ca/Sr and K/Rb ratio results allowed independent estimation of dissolution incongruency and discrimination against Sr and Rb during cation uptake processes. The fraction of K in biomass from biotite increased with decreasing K supply from nutrient solutions. The mineral anorthite was consistently the major source of Ca, regardless of nutrient treatment. Conclusions Red pine seedlings exploited more mineral K in response to more severe K deficiency. This did not occur for Ca. Plant discrimination factors must be carefully considered to accurately identify nutrient sources using cation tracers.

  1. Precision polarization measurements of atoms in a far-off-resonance optical dipole trap

    SciTech Connect (OSTI)

    Fang, F.; Vieira, D. J.; Zhao, X.

    2011-01-15

    Precision measurement of atomic and nuclear polarization is an essential step for beta-asymmetry measurement of radioactive atoms. In this paper, we report the polarization measurement of Rb atoms in an yttrium-aluminum-garnet (YAG) far-off-resonance optical dipole trap. We have prepared a cold cloud of polarized Rb atoms in the YAG dipole trap by optical pumping and achieved an initial nuclear polarization of up to 97.2(5)%. The initial atom distribution in different Zeeman levels is measured by using a combination of microwave excitation, laser pushing, and atomic retrap techniques. The nuclear-spin polarization is further purified to 99.2(2)% in 10 s and maintained above 99% because the two-body collision loss rate between atoms in mixed spin states is greater than the one-body trap loss rate. Systematic effects on the nuclear polarization, including the off-resonance Raman scattering, magnetic field gradient, and background gas collisions, are discussed.

  2. Search for b→u transitions in B±→[K∓π±π⁰]DK± decays

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Lees, J. P.; Poireau, V.; Tisserand, V.; Garra Tico, J.; Grauges, E.; Martinelli, M.; Milanes, D. A.; Palano, A.; Pappagallo, M.; Eigen, G.; et al

    2011-07-06

    We present a study of the decays B±→DK± with D mesons reconstructed in the K⁺π⁻π⁰ or K⁻π⁺π⁰ final states, where D indicates a D⁰ or a D¯¯¯0 meson. Using a sample of 474×10⁶ BB¯¯¯ pairs collected with the BABAR detector at the PEP-II asymmetric-energy e⁺e⁻ collider at SLAC, we measure the ratios R±≡((Γ(B±→[K∓π±π⁰]DK±))/((Γ(B±→[K±π∓π⁰]DK±)). We obtain R⁺=(5⁺12⁻10(stat)⁺2⁻4(syst))×10⁻³ and R⁻=(12⁺12⁻10(stat)⁺3⁻5(syst))×10⁻³, from which we extract the upper limits at 90% probability: R⁺<23×10⁻³ and R⁻<29×10⁻³. Using these measurements, we obtain an upper limit for the ratio rB of the magnitudes of the b→u and b→c amplitudes rB<0.13 at 90% probability.

  3. ?-Fe{sub 2}O{sub 3} nanoparticles: An easily recoverable effective photo-catalyst for the degradation of rose bengal and methylene blue dyes in the waste-water treatment plant

    SciTech Connect (OSTI)

    Dutta, Amit Kumar; Maji, Swarup Kumar; Adhikary, Bibhutosh

    2014-01-01

    Graphical abstract: - Highlights: ?-Fe{sub 2}O{sub 3} NPs from a single-source precursor and characterized by XRD, TEM, UVvis spectra. The NPs were tested as effective photocatalyst toward degradation of RB and MB dyes. The possible pathway of the photocatalytic decomposition process has been discussed. The active species, OH, was detected by TA photoluminescence probing techniques. - Abstract: ?-Fe{sub 2}O{sub 3} nanoparticles (NPs) were synthesized from a single-source precursor complex [Fe{sub 3}O(C{sub 6}H{sub 5}COO){sub 6}(H{sub 2}O){sub 3}]NO{sub 3} by a simple thermal decomposition process and have been characterized by X-ray diffraction analysis (XRD), transmission electron microscopy (TEM) and UVvis spectroscopic techniques. The NPs were highly pure and well crystallized having hexagonal morphology with an average particle size of 35 nm. The prepared ?-Fe{sub 2}O{sub 3} (maghemite) NPs show effective photo-catalytic activity toward the degradation of rose bengal (RB) and methylene blue (MB) dyes under visible light irradiation and can easily be recoverable in the presence of magnetic field for successive re-uses. The possible photo-catalytic decomposition mechanism is discussed through the detection of hydroxyl radical (OH) by terephthalic acid photo-luminescence probing technique.

  4. Enhanced γ -Ray Emission from Neutron Unbound States Populated in β Decay

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Tain, J. L.; Valencia, E.; Algora, A.; Agramunt, J.; Rubio, B.; Rice, S.; Gelletly, W.; Regan, P.; Zakari-Issoufou, A. -A.; Fallot, M.; et al

    2015-08-01

    Total absorption spectroscopy was used to investigate the β -decay intensity to states above the neutron separation energy followed by γ -ray emission in 87,88Br and 94Rb. Accurate results were obtained thanks to the careful control of systematic errors. An unexpectedly large γ intensity was observed in all three cases extending well beyond the excitation energy region where neutron penetration is hindered by low neutron energy. The γ branching as a function of excitation energy was compared to Hauser-Feshbach model calculations. For 87Br and 88Br the branching reaches 57% and 20% respectively, and could be explained as a nuclear structuremore » effect. Some of the states populated in the daughter can only decay through the emission of a large orbital angular momentum neutron with a strongly reduced barrier penetrability. In the case of neutron-rich 94Rb the observed 4.5% branching is much larger than the calculations performed with standard nuclear statistical model parameters, even after proper correction for fluctuation effects on individual transition widths. The difference can be reconciled introducing an enhancement of one order-of-magnitude in the photon strength to neutron strength ratio. An increase in the photon strength function of such magnitude for very neutron-rich nuclei, if it proved to be correct, leads to a similar increase in the (n, γ) cross section that would have an impact on r process abundance calculations.« less

  5. Estrogen inhibits cell cycle progression and retinoblastoma phosphorylation in rhesus ovarian surface epithelial cell culture

    SciTech Connect (OSTI)

    Wright, Jay W.; Stouffer, Richard L.; Rodland, Karin D.

    2003-10-31

    Estrogen promotes the growth of some ovarian cancer cells at nanomolar concentrations, but has been shown to inhibit growth of normal ovarian surface epithelial (OSE) cells at micromolar concentrations (1?g/ml). OSE cells express the estrogen receptor (ER)-?, and are the source of 90% of various cancers. The potential sensitivity of OSE cells to estrogen stresses the importance of understanding the estrogen-dependent mechanisms at play in OSE proliferation and transformation, as well as in anticancer treatment. We investigated the effects of estradiol on cell proliferation in vitro, and demonstrate an intracellular locus of action of estradiol in cultured rhesus ovarian surface epithelial (RhOSE) cells. We show that ovarian and breast cells are growth-inhibited by micromolar concentration of estradiol and that this inhibition correlates with estrogen receptor expression. We further show that normal rhesus OSE cells do not activate ERK or Akt in response to estradiol nor does estradiol block the ability of serum to stimulate ERK or induce cyclin D expression. Contrarily, estradiol inhibits serum-dependent retinoblastoma protein (Rb) phosphorylation and blocks DNA synthesis. This inhibition does not formally arrest cells and is reversible within hours of estrogen withdrawal. Our data are consistent with growth inhibition by activation of Rb and indicate that sensitivity to hormone therapy in anticancer treatment can be modulated by cell cycle regulators downstream of the estrogen receptor.

  6. Uranium Bioreduction Rates across Scales: Biogeochemical Hot Moments and Hot Spots during a Biostimulation Experiment at Rifle, Colorado

    SciTech Connect (OSTI)

    Bao, Chen; Wu, Hongfei; Li, Li; Newcomer, Darrell R.; Long, Philip E.; Williams, Kenneth H.

    2014-09-02

    We aim to understand the scale-dependent evolution of uranium bioreduction during a field experiment at a former uranium mill site near Rifle, Colorado. Acetate was injected to stimulate Fe-reducing bacteria (FeRB) and to immobilize aqueous U(VI) to insoluble U(IV). Bicarbonate was coinjected in half of the domain to mobilize sorbed U(VI). We used reactive transport modeling to integrate hydraulic and geochemical data and to quantify rates at the grid block (0.25 m) and experimental field scale (tens of meters). Although local rates varied by orders of magnitude in conjunction with biostimulation fronts propagating downstream, field-scale rates were dominated by those orders of magnitude higher rates at a few selected hot spots where Fe(III), U(VI), and FeRB were at their maxima in the vicinity of the injection wells. At particular locations, the hot moments with maximum rates negatively corresponded to their distance from the injection wells. Although bicarbonate injection enhanced local rates near the injection wells by a maximum of 39.4%, its effect at the field scale was limited to a maximum of 10.0%. We propose a rate-versus-measurement-length relationship (log R' = -0.63

  7. Microfabricated alkali vapor cell with anti-relaxation wall coating

    SciTech Connect (OSTI)

    Straessle, R.; Ptremand, Y.; Briand, D.; Rooij, N. F. de; Pellaton, M.; Affolderbach, C.; Mileti, G.

    2014-07-28

    We present a microfabricated alkali vapor cell equipped with an anti-relaxation wall coating. The anti-relaxation coating used is octadecyltrichlorosilane and the cell was sealed by thin-film indium-bonding at a low temperature of 140?C. The cell body is made of silicon and Pyrex and features a double-chamber design. Depolarizing properties due to liquid Rb droplets are avoided by confining the Rb droplets to one chamber only. Optical and microwave spectroscopy performed on this wall-coated cell are used to evaluate the cell's relaxation properties and a potential gas contamination. Double-resonance signals obtained from the cell show an intrinsic linewidth that is significantly lower than the linewidth that would be expected in case the cell had no wall coating but only contained a buffer-gas contamination on the level measured by optical spectroscopy. Combined with further experimental evidence this proves the presence of a working anti-relaxation wall coating in the cell. Such cells are of interest for applications in miniature atomic clocks, magnetometers, and other quantum sensors.

  8. AGR-2 AND AGR-3/4 RELEASE-TO-BIRTH RATIO DATA ANALYSIS

    SciTech Connect (OSTI)

    Pham, Binh T; Einerson, Jeffrey J; Scates, Dawn M; Maki, John T; Petti, David A

    2014-09-01

    A series of Advanced Gas Reactor (AGR) irradiation tests is being conducted in the Advanced Test Reactor at Idaho National Laboratory in support of development and qualification of tristructural isotropic (TRISO) low enriched fuel used in the High Temperature Gas-cooled Reactor (HTGR). Each AGR test consists of multiple independently controlled and monitored capsules containing fuel compacts placed in a graphite cylinder shrouded by a steel shell. These capsules are instrumented with thermocouples embedded in the graphite enabling temperature control. AGR configuration and irradiation conditions are based on prismatic HTGR technology distinguished primarily by the use of helium coolant, a low-power-density ceramic core capable of withstanding very high temperatures, and TRISO coated particle fuel. Thus, these tests provide valuable irradiation performance data to support fuel process development, qualify fuel for normal operating conditions, and support development and validation of fuel performance and fission product transport models and codes. The release-rate-to-birth-rate ratio (R/B) for each of fission product isotopes (i.e., krypton and xenon) is calculated from release rates in the sweep gas flow measured by the germanium detectors used in the AGR Fission Product Monitoring (FPM) System installed downstream from each irradiated capsule. Birth rates are calculated based on the fission power in the experiment and fission product generation models. Thus, this R/B is a measure of the ability of fuel kernel, particle coating layers, and compact matrix to retain fission gas atoms preventing their release into the sweep gas flow, especially in the event of particle coating failures that occurred during AGR-2 and AGR-3/4 irradiations. The major factors that govern gaseous radioactive decay, diffusion, and release processes are found to be material diffusion coefficient, temperature, and isotopic decay constant. For each of all AGR capsules, ABAQUS-based three-dimensional finite-element thermal models are created to predict daily averages of fuel compact temperatures for the entire irradiation period, which are used in establishing the R/B correlation with temperature and decay constant. This correlation can be used by reactor designers to estimate fission gas release from postulated failed fuel particles in HTGR cores, which is the key safety factor for fuel performance assessment.

  9. Quadruple-layered perovskite (CuCl)Ca{sub 2}NaNb{sub 4}O{sub 13}

    SciTech Connect (OSTI)

    Kitada, A.; Tsujimoto, Y.; Yamamoto, T. [Department of Energy and Hydrocarbon Chemistry, Faculty of Engineering, Kyoto University, Nishikyo, Kyoto 615-8510 (Japan); Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502 (Japan); Kobayashi, Y. [Department of Energy and Hydrocarbon Chemistry, Faculty of Engineering, Kyoto University, Nishikyo, Kyoto 615-8510 (Japan); Narumi, Y. [Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581 (Japan); Institute for Materials Research, Tohoku University, Katahira 2-1-1, Sendai 980-8577 (Japan); Kindo, K. [Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581 (Japan); Aczel, A.A.; Luke, G.M. [Department of Physics and Astronomy, McMaster University, Hamilton, Ontario, L8S 4M1 (Canada); Uemura, Y.J. [Department of Physics, Columbia University, New York, NY 10027 (United States); Kiuchi, Y.; Ueda, Y. [Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581 (Japan); Yoshimura, K. [Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502 (Japan); Ajiro, Y. [Department of Energy and Hydrocarbon Chemistry, Faculty of Engineering, Kyoto University, Nishikyo, Kyoto 615-8510 (Japan); Kageyama, H., E-mail: kage@scl.kyoto-u.ac.jp [Department of Energy and Hydrocarbon Chemistry, Faculty of Engineering, Kyoto University, Nishikyo, Kyoto 615-8510 (Japan); Department of Chemistry, Graduate School of Science, Kyoto University, Kyoto 606-8502 (Japan); Institute for Integrated Cell-Material Sciences, Kyoto University, Sakyo, Kyoto 606-8501 (Japan); CREST, Japan Science and Technology Agency, Kawaguchi 332-0012 (Japan)

    2012-01-15

    We will present the synthesis, structure and magnetic properties of a new quadruple-layered perovskite (CuCl)Ca{sub 2}NaNb{sub 4}O{sub 13}. Through a topotactic ion-exchange reaction with CuCl{sub 2}, the precursor RbCa{sub 2}NaNb{sub 4}O{sub 13} presumably having an incoherent octahederal tliting changes into (CuCl)Ca{sub 2}NaNb{sub 4}O{sub 13} with a 2a{sub p} Multiplication-Sign 2a{sub p} Multiplication-Sign 2c{sub p} superstructure (tetragonal; a=7.73232(5) A, c=39.2156(4) A). The well-defined superstructure for the ion-exchanged product should be stabilized by the inserted CuCl{sub 4}O{sub 2} octahedral layers that firmly connect with neighboring perovskite layers. Magnetic studies show the absence of long-range magnetic ordering down to 2 K despite strong in-plane interactions. Aleksandrov Prime s group theory and Rietveld refinement of synchrotron X-ray diffraction data suggest the structure to be of I4/mmm space group with in-phase tilting along the a and b axes, a two-tilt system (++0). - Graphical Abstract: We present a quadruple-layered copper oxyhalide (CuCl)Ca{sub 2}NaNb{sub 4}O{sub 13} synthesized through a topotactic ion-exchange reaction of RbCa{sub 2}NaNb{sub 4}O{sub 13} with CuCl{sub 2}. The compound has a well-defined superstructure. Magnetic studies suggest the absence of magnetic order even at 2 K. Highlights: Black-Right-Pointing-Pointer (CuCl)Ca{sub 2}NaNb{sub 4}O{sub 13} was prepared by ion-exchange reaction of RbCa{sub 2}NaNb{sub 4}O{sub 13} with CuCl{sub 2}. Black-Right-Pointing-Pointer Compound has a 2a{sub p} Multiplication-Sign 2a{sub p} Multiplication-Sign 2c{sub p} superstructure (tetragonal; a=7.73 A, c=39.21 A). Black-Right-Pointing-Pointer Such a well-defined superstructure was not observed in the precursor compound. Black-Right-Pointing-Pointer Aleksandrov Prime s theory and Rietveld study suggest a (++0) octahedral tilting (I4/mmm). Black-Right-Pointing-Pointer Magnetic studies revealed the absence of magnetic order down to 2 K.

  10. Systematic study of doping dependence on linear magnetoresistance in p-PbTe

    SciTech Connect (OSTI)

    Schneider, J. M.; Chitta, V. A.; Oliveira, N. F.; Peres, M. L. Castro, S. de; Soares, D. A. W.; Wiedmann, S.; Zeitler, U.; Abramof, E.; Rappl, P. H. O.; Mengui, U. A.

    2014-10-20

    We report on a large linear magnetoresistance effect observed in doped p-PbTe films. While undoped p-PbTe reveals a sublinear magnetoresistance, p-PbTe films doped with BaF{sub 2} exhibit a transition to a nearly perfect linear magnetoresistance behaviour that is persistent up to 30?T. The linear magnetoresistance slope ?R/?B is to a good approximation, independent of temperature. This is in agreement with the theory of Quantum Linear Magnetoresistance. We also performed magnetoresistance simulations using a classical model of linear magnetoresistance. We found that this model fails to explain the experimental data. A systematic study of the doping dependence reveals that the linear magnetoresistance response has a maximum for small BaF{sub 2} doping levels and diminishes rapidly for increasing doping levels. Exploiting the huge impact of doping on the linear magnetoresistance signal could lead to new classes of devices with giant magnetoresistance behavior.

  11. Influence of mobile ion concentrations on the chemical composition of geothermal waters in granitic areas; Example of hot springs form Piemonte Italy

    SciTech Connect (OSTI)

    Michard, G.; Grimaud, D. ); D'Amore, F.; Fancelli, R. )

    1989-01-01

    The six hot springs from Vinadio and the springs from Valdieri (Piemonte, Italy) have similar emergence temperatures ({approximately}50{degrees} C), similar deep temperatures ({approximately}115{degrees} C) and their chloride content varies from 0.9 to 30 mmol/kg. Major elements and some trace elements concentrations (Li, Rb, Cs, Sr, Ba, Mn) correlate closely with Na concentrations. The correlations in a log-log diagram are linear with a slope close to the electric charge of the ion. This is explained, for major elements, by an equilibrium between a complete assemblage of minerals and a water containing varying amounts of chloride. It is suggested, from the Cl/Br ratio, that chloride originates by halite dissolution during the descent of the water.

  12. Energy Division annual progress report for period ending September 30, 1981

    SciTech Connect (OSTI)

    Not Available

    1982-05-01

    This eighth annual report of the Division covers work done during FY 1981 (October 1, 1980, through September 30, 1981). As with these documents in the past, the format follows approximately the organizational structure of the Energy Division. Chapters 2 through 6 summarize the activities of the sections of the Division: Environmental Impact Section, headed by H.E. Zittel; Regional and Urban Studies Section, R.M. Davis; Economic Analysis Section, R.B. Shelton; Data and Analysis Section, A.S. Loebl; and Efficiency and Renewables Research Section, J.W. Michel. In addition, work on a variety of projects which cut across section lines is reported in Chapter 7, Integrated Programs. These activities are under the supervision of T.J. Wilbanks, Associate Director for the Division. Separate abstracts are included for individual projects.

  13. Reducing collective quantum state rotation errors with reversible dephasing

    SciTech Connect (OSTI)

    Cox, Kevin C.; Norcia, Matthew A.; Weiner, Joshua M.; Bohnet, Justin G.; Thompson, James K.

    2014-12-29

    We demonstrate that reversible dephasing via inhomogeneous broadening can greatly reduce collective quantum state rotation errors, and observe the suppression of rotation errors by more than 21?dB in the context of collective population measurements of the spin states of an ensemble of 2.110{sup 5} laser cooled and trapped {sup 87}Rb atoms. The large reduction in rotation noise enables direct resolution of spin state populations 13(1) dB below the fundamental quantum projection noise limit. Further, the spin state measurement projects the system into an entangled state with 9.5(5) dB of directly observed spectroscopic enhancement (squeezing) relative to the standard quantum limit, whereas no enhancement would have been obtained without the suppression of rotation errors.

  14. Localized collapse and revival of coherence in an ultracold Bose gas

    SciTech Connect (OSTI)

    McGuirk, J. M.; Zajiczek, L. F. [Department of Physics, Simon Fraser University, Burnaby, British Columbia V5A 1S6 (Canada)

    2011-01-15

    We study the collapse and revival of coherence induced by dipolar spin waves in a trapped gas of {sup 87}Rb atoms. In particular, we observe spatially localized collapse and revival of Ramsey fringe contrast and show how the pattern of coherence depends on the strength of the spin-wave excitation. We find that the spatial character of the coherence dynamics is incompatible with a simple model based only on position-space overlap of wave functions. We show that this phenomenon requires a full phase-space description of the atomic spin using a quantum Boltzmann transport equation, which highlights spin-wave-induced coherent spin currents and the ensuing dynamics they drive.

  15. Ternary alkali-metal and transition metal or metalloid acetylides as alkali-metal intercalation electrodes for batteries

    DOE Patents [OSTI]

    Nemeth, Karoly; Srajer, George; Harkay, Katherine C; Terdik, Joseph Z

    2015-02-10

    Novel intercalation electrode materials including ternary acetylides of chemical formula: A.sub.nMC.sub.2 where A is alkali or alkaline-earth element; M is transition metal or metalloid element; C.sub.2 is reference to the acetylide ion; n is an integer that is 0, 1, 2, 3 or 4 when A is alkali element and 0, 1, or 2 when A is alkaline-earth element. The alkali elements are Lithium (Li), Sodium (Na), Potassium (K), Rubidium (Rb), Cesium (Cs) and Francium (Fr). The alkaline-earth elements are Berilium (Be), Magnesium (Mg), Calcium (Ca), Strontium (Sr), Barium (Ba), and Radium (Ra). M is a transition metal that is any element in groups 3 through 12 inclusive on the Periodic Table of Elements (elements 21 (Sc) to element 30 (Zn)). In another exemplary embodiment, M is a metalloid element.

  16. West Maui Groundwater Flow Model

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Nicole Lautze

    2015-01-01

    Groundwater flow model for West Maui. Data is from the following sources: Whittier, R. and A.I. El-Kadi. 2014. Human and Environmental Risk Ranking of Onsite Sewage Disposal Systems For the Hawaiian Islands of Kauai, Molokai, Maui, and Hawaii – Final. Prepared by the University of Hawaii, Dept. of Geology and Geophysics for the State of Hawaii Dept. of Health, Safe Drinking Water Branch. September 2014; and Whittier, R.B., K. Rotzoll, S. Dhal, A.I. El-Kadi, C. Ray, G. Chen, and D. Chang. 2004. Hawaii Source Water Assessment Program Report – Volume V – Island of Maui Source Water Assessment Program Report. Prepared for the Hawaii Department of Health, Safe Drinking Water Branch. University of Hawaii, Water Resources Research Center. Updated 2008.

  17. Kauai Groundwater Flow Model

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Nicole Lautze

    2015-01-01

    Groundwater flow model for Kauai. Data is from the following sources: Whittier, R. and A.I. El-Kadi. 2014. Human and Environmental Risk Ranking of Onsite Sewage Disposal Systems For the Hawaiian Islands of Kauai, Molokai, Maui, and Hawaii – Final. Prepared by the University of Hawaii, Dept. of Geology and Geophysics for the State of Hawaii Dept. of Health, Safe Drinking Water Branch. September 2014.; and Whittier, R.B., K. Rotzoll, S. Dhal, A.I. El-Kadi, C. Ray, G. Chen, and D. Chang. 2004. Hawaii Source Water Assessment Program Report – Volume IV – Island of Kauai Source Water Assessment Program Report. Prepared for the Hawaii Department of Health, Safe Drinking Water Branch. University of Hawaii, Water Resources Research Center. Updated 2015.

  18. Kauai Groundwater Flow Model

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Nicole Lautze

    2015-01-01

    Groundwater flow model for Kauai. Data is from the following sources: Whittier, R. and A.I. El-Kadi. 2014. Human and Environmental Risk Ranking of Onsite Sewage Disposal Systems For the Hawaiian Islands of Kauai, Molokai, Maui, and Hawaii Final. Prepared by the University of Hawaii, Dept. of Geology and Geophysics for the State of Hawaii Dept. of Health, Safe Drinking Water Branch. September 2014.; and Whittier, R.B., K. Rotzoll, S. Dhal, A.I. El-Kadi, C. Ray, G. Chen, and D. Chang. 2004. Hawaii Source Water Assessment Program Report Volume IV Island of Kauai Source Water Assessment Program Report. Prepared for the Hawaii Department of Health, Safe Drinking Water Branch. University of Hawaii, Water Resources Research Center. Updated 2015.

  19. West Maui Groundwater Flow Model

    DOE Data Explorer [Office of Scientific and Technical Information (OSTI)]

    Nicole Lautze

    2015-01-01

    Groundwater flow model for West Maui. Data is from the following sources: Whittier, R. and A.I. El-Kadi. 2014. Human and Environmental Risk Ranking of Onsite Sewage Disposal Systems For the Hawaiian Islands of Kauai, Molokai, Maui, and Hawaii Final. Prepared by the University of Hawaii, Dept. of Geology and Geophysics for the State of Hawaii Dept. of Health, Safe Drinking Water Branch. September 2014; and Whittier, R.B., K. Rotzoll, S. Dhal, A.I. El-Kadi, C. Ray, G. Chen, and D. Chang. 2004. Hawaii Source Water Assessment Program Report Volume V Island of Maui Source Water Assessment Program Report. Prepared for the Hawaii Department of Health, Safe Drinking Water Branch. University of Hawaii, Water Resources Research Center. Updated 2008.

  20. FY 2008 Annual Performance Report

    Energy Savers [EERE]

    Hyd rog en Tan k Res earc h, LLN L PH EN IX Ex pe rim en t, BN L Fu el Ce ll Re sea rch , AN L Ca rb on Se qu es tra tio n Re se ar ch , PN NL Hi gh Ex pl os iv es Ap pl ic at io ns Fa ci lit y, LL NL Com put er Sim ulat ion The ater , LAN L Al ga e Re se ar ch , NR EL Ad va nc ed Bio fue ls Re se arc h, LB NL T ra in in g Nuc lear Mat eria ls Sto rag e, SRS C o a l G a s if ic a ti o n R e s e a rc h , P N N L Cli ma te Mo de lin g, OR NL AnnuAl PerformAnce rePort fY 2008 Table of Contents

  1. Remote NMR/MRI detection of laser polarized gases

    DOE Patents [OSTI]

    Pines, Alexander; Saxena, Sunil; Moule, Adam; Spence, Megan; Seeley, Juliette A.; Pierce, Kimberly L.; Han, Song-I; Granwehr, Josef

    2006-06-13

    An apparatus and method for remote NMR/MRI spectroscopy having an encoding coil with a sample chamber, a supply of signal carriers, preferably hyperpolarized xenon and a detector allowing the spatial and temporal separation of signal preparation and signal detection steps. This separation allows the physical conditions and methods of the encoding and detection steps to be optimized independently. The encoding of the carrier molecules may take place in a high or a low magnetic field and conventional NMR pulse sequences can be split between encoding and detection steps. In one embodiment, the detector is a high magnetic field NMR apparatus. In another embodiment, the detector is a superconducting quantum interference device. A further embodiment uses optical detection of Rb--Xe spin exchange. Another embodiment uses an optical magnetometer using non-linear Faraday rotation. Concentration of the signal carriers in the detector can greatly improve the signal to noise ratio.

  2. Ran GTPase protein promotes human pancreatic cancer proliferation by deregulating the expression of Survivin and cell cycle proteins

    SciTech Connect (OSTI)

    Deng, Lin; Department of Oncology, Tangdu Hospital, Fourth Military Medical University, Xian, Shaanxi 710038 ; Lu, Yuanyuan; Zhao, Xiaodi; Sun, Yi; Shi, Yongquan; Fan, Hongwei; Liu, Changhao; Zhou, Jinfeng; Nie, Yongzhan; Wu, Kaichun; Fan, Daiming; Guo, Xuegang

    2013-10-18

    Highlights: Overexpression of Ran in pancreatic cancer was correlated with histological grade. Downregulation of Ran could induce cell apoptosis and inhibit cell proliferation. The effects were mediated by cell cycle proteins, Survivin and cleaved Caspase-3. -- Abstract: Ran, a member of the Ras GTPase family, has important roles in nucleocytoplasmic transport. Herein, we detected Ran expression in pancreatic cancer and explored its potential role on tumour progression. Overexpressed Ran in pancreatic cancer tissues was found highly correlated with the histological grade. Downregulation of Ran led to significant suppression of cell proliferation, cell cycle arrest at the G1/S phase and induction of apoptosis. In vivo studies also validated that result. Further studies revealed that those effects were at least partly mediated by the downregulation of Cyclin A, Cyclin D1, Cyclin E, CDK2, CDK4, phospho-Rb and Survivin proteins and up regulation of cleaved Caspase-3.

  3. AGR-2 IRRADIATION TEST FINAL AS-RUN REPORT

    SciTech Connect (OSTI)

    Blaise, Collin

    2014-07-01

    This document presents the as-run analysis of the AGR-2 irradiation experiment. AGR-2 is the second of the planned irradiations for the Advanced Gas Reactor (AGR) Fuel Development and Qualification Program. Funding for this program is provided by the U.S. Department of Energy as part of the Very High Temperature Reactor (VHTR) Technical Development Office (TDO) program. The objectives of the AGR-2 experiment are to: (a) Irradiate UCO (uranium oxycarbide) and UO2 (uranium dioxide) fuel produced in a large coater. Fuel attributes are based on results obtained from the AGR-1 test and other project activities. (b) Provide irradiated fuel samples for post-irradiation experiment (PIE) and safety testing. (c) Support the development of an understanding of the relationship between fuel fabrication processes, fuel product properties, and irradiation performance. The primary objective of the test was to irradiate both UCO and UO2 TRISO (tri-structural isotropic) fuel produced from prototypic scale equipment to obtain normal operation and accident condition fuel performance data. The UCO compacts were subjected to a range of burnups and temperatures typical of anticipated prismatic reactor service conditions in three capsules. The test train also includes compacts containing UO2 particles produced independently by the United States, South Africa, and France in three separate capsules. The range of burnups and temperatures in these capsules were typical of anticipated pebble bed reactor service conditions. The results discussed in this report pertain only to U.S. produced fuel. In order to achieve the test objectives, the AGR-2 experiment was irradiated in the B-12 position of the Advanced Test Reactor (ATR) at Idaho National Laboratory (INL) for a total irradiation duration of 559.2 effective full power days (EFPD). Irradiation began on June 22, 2010, and ended on October 16, 2013, spanning 12 ATR power cycles and approximately three and a half calendar years. The test contained six independently controlled and monitored capsules. Each U.S. capsule contained 12 compacts of either UCO or UO2 AGR coated fuel. No fuel particles failed during the AGR-2 irradiation. Final burnup values on a per compact basis ranged from 7.26 to 13.15% FIMA (fissions per initial heavy-metal atom) for UCO fuel, and 9.01 to 10.69% FIMA for UO2 fuel, while fast fluence values ranged from 1.94 to 3.471025 n/m2 (E >0.18 MeV) for UCO fuel, and from 3.05 to 3.531025 n/m2 (E >0.18 MeV) for UO2 fuel. Time-average volume-average (TAVA) temperatures on a capsule basis at the end of irradiation ranged from 987C in Capsule 6 to 1296C in Capsule 2 for UCO, and from 996 to 1062C in UO2-fueled Capsule 3. By the end of the irradiation, all of the installed thermocouples (TCs) had failed. Fission product release-to-birth (R/B) ratios were quite low. In the UCO capsules, R/B values during the first three cycles were below 10-6 with the exception of the hotter Capsule 2, in which the R/Bs reached 210-6. In the UO2 capsule (Capsule 3), the R/B values during the first three cycles were below 10-7. R/B values for all following cycles are not reliable due to gas flow and cross talk issues.

  4. AGR-2 irradiation test final as-run report, Rev. 1

    SciTech Connect (OSTI)

    Collin, Blaise

    2014-08-01

    This document presents the as-run analysis of the AGR-2 irradiation experiment. AGR-2 is the second of the planned irradiations for the Advanced Gas Reactor (AGR) Fuel Development and Qualification Program. Funding for this program is provided by the U.S. Department of Energy as part of the Very High Temperature Reactor (VHTR) Technical Development Office (TDO) program. The objectives of the AGR-2 experiment are to: (a) Irradiate UCO (uranium oxycarbide) and UO2 (uranium dioxide) fuel produced in a large coater. Fuel attributes are based on results obtained from the AGR-1 test and other project activities; (b) Provide irradiated fuel samples for post-irradiation experiment (PIE) and safety testing; and, (c) Support the development of an understanding of the relationship between fuel fabrication processes, fuel product properties, and irradiation performance. The primary objective of the test was to irradiate both UCO and UO2 TRISO (tri-structural isotropic) fuel produced from prototypic scale equipment to obtain normal operation and accident condition fuel performance data. The UCO compacts were subjected to a range of burnups and temperatures typical of anticipated prismatic reactor service conditions in three capsules. The test train also includes compacts containing UO2 particles produced independently by the United States, South Africa, and France in three separate capsules. The range of burnups and temperatures in these capsules were typical of anticipated pebble bed reactor service conditions. The results discussed in this report pertain only to U.S. produced fuel. In order to achieve the test objectives, the AGR-2 experiment was irradiated in the B-12 position of the Advanced Test Reactor (ATR) at Idaho National Laboratory (INL) for a total irradiation duration of 559.2 effective full power days (EFPD). Irradiation began on June 22, 2010, and ended on October 16, 2013, spanning 12 ATR power cycles and approximately three and a half calendar years. The test contained six independently controlled and monitored capsules. Each U.S. capsule contained 12 compacts of either UCO or UO2 AGR coated fuel. No fuel particles failed during the AGR-2 irradiation. Final burnup values on a per compact basis ranged from 7.26 to 13.15% FIMA (fissions per initial heavy-metal atom) for UCO fuel, and 9.01 to 10.69% FIMA for UO2 fuel, while fast fluence values ranged from 1.94 to 3.471025 n/m2 (E >0.18 MeV) for UCO fuel, and from 3.05 to 3.531025 n/m2 (E >0.18 MeV) for UO2 fuel. Time-average volume-average (TAVA) temperatures on a capsule basis at the end of irradiation ranged from 987C in Capsule 6 to 1296C in Capsule 2 for UCO, and from 996 to 1062C in UO2-fueled Capsule 3. By the end of the irradiation, all of the installed thermocouples (TCs) had failed. Fission product release-to-birth (R/B) ratios were quite low. In the UCO capsules, R/B values during the first three cycles were below 10-6 with the exception of the hotter Capsule 2, in which the R/Bs reached 210-6. In the UO2 capsule (Capsule 3), the R/B values during the first three cycles were below 10-7. R/B values for all following cycles are not reliable due to gas flow and cross talk issues.

  5. AGR-2 Irradiation Test Final As-Run Report, Rev 2

    SciTech Connect (OSTI)

    Blaise Collin

    2014-08-01

    This document presents the as-run analysis of the AGR-2 irradiation experiment. AGR-2 is the second of the planned irradiations for the Advanced Gas Reactor (AGR) Fuel Development and Qualification Program. Funding for this program is provided by the U.S. Department of Energy as part of the Very High Temperature Reactor (VHTR) Technical Development Office (TDO) program. The objectives of the AGR-2 experiment are to: (a) Irradiate UCO (uranium oxycarbide) and UO2 (uranium dioxide) fuel produced in a large coater. Fuel attributes are based on results obtained from the AGR-1 test and other project activities. (b) Provide irradiated fuel samples for post-irradiation experiment (PIE) and safety testing. (c) Support the development of an understanding of the relationship between fuel fabrication processes, fuel product properties, and irradiation performance. The primary objective of the test was to irradiate both UCO and UO2 TRISO (tri-structural isotropic) fuel produced from prototypic scale equipment to obtain normal operation and accident condition fuel performance data. The UCO compacts were subjected to a range of burnups and temperatures typical of anticipated prismatic reactor service conditions in three capsules. The test train also includes compacts containing UO2 particles produced independently by the United States, South Africa, and France in three separate capsules. The range of burnups and temperatures in these capsules were typical of anticipated pebble bed reactor service conditions. The results discussed in this report pertain only to U.S. produced fuel. In order to achieve the test objectives, the AGR-2 experiment was irradiated in the B-12 position of the Advanced Test Reactor (ATR) at Idaho National Laboratory (INL) for a total irradiation duration of 559.2 effective full power days (EFPD). Irradiation began on June 22, 2010, and ended on October 16, 2013, spanning 12 ATR power cycles and approximately three and a half calendar years. The test contained six independently controlled and monitored capsules. Each U.S. capsule contained 12 compacts of either UCO or UO2 AGR coated fuel. No fuel particles failed during the AGR-2 irradiation. Final burnup values on a per compact basis ranged from 7.26 to 13.15% FIMA (fissions per initial heavy-metal atom) for UCO fuel, and 9.01 to 10.69% FIMA for UO2 fuel, while fast fluence values ranged from 1.94 to 3.471025 n/m2 (E >0.18 MeV) for UCO fuel, and from 3.05 to 3.531025 n/m2 (E >0.18 MeV) for UO2 fuel. Time-average volume-average (TAVA) temperatures on a capsule basis at the end of irradiation ranged from 987C in Capsule 6 to 1296C in Capsule 2 for UCO, and from 996 to 1062C in UO2-fueled Capsule 3. By the end of the irradiation, all of the installed thermocouples (TCs) had failed. Fission product release-to-birth (R/B) ratios were quite low. In the UCO capsules, R/B values during the first three cycles were below 10-6 with the exception of the hotter Capsule 2, in which the R/Bs reached 210-6. In the UO2 capsule (Capsule 3), the R/B values during the first three cycles were below 10-7. R/B values for all following cycles are not reliable due to gas flow and cross talk issues.

  6. Bose-Einstein condensate in a light-induced vector gauge potential using 1064-nm optical-dipole-trap lasers

    SciTech Connect (OSTI)

    Fu Zhengkun; Wang Pengjun; Chai Shijie; Huang Lianghui; Zhang Jing

    2011-10-15

    Using two crossed 1064-nm optical-dipole-trap lasers to be the Raman beams, an effective vector gauge potential for Bose-Einstein condensed {sup 87}Rb in the F=2 hyperfine ground state is experimentally created. The moderate strength of the Raman coupling still can be achieved when the detuning from atomic resonance is larger than the excited-state fine structure, since rubidium has 15 nm energy-level spitting. The atoms at the far detuning of the Raman coupling are loaded adiabatically into the dressed states by ramping the homogeneous bias magnetic field with different paths and the dressed states with different energies are studied experimentally. The experimental scheme can be easily extended to produce the synthetic magnetic or electric field by means of a spatial or time dependence of the effective vector potential.

  7. Magnetic phase diagram of a spin-1 condensate in two dimensions with dipole interaction

    SciTech Connect (OSTI)

    Kjaell, Jonas A.; Essin, Andrew M.; Moore, Joel E.

    2009-12-01

    Several new features arise in the ground-state phase diagram of a spin-1 condensate trapped in an optical trap when the magnetic-dipole interaction between the atoms is taken into account along with confinement and spin precession. The boundaries between the regions of ferromagnetic and polar phases move as the dipole strength is varied and the ferromagnetic phases can be modulated. The magnetization of the ferromagnetic phase perpendicular to the field becomes modulated as a helix winding around the magnetic field direction with a wavelength inversely proportional to the dipole strength. This modulation should be observable for current experimental parameters in {sup 87}Rb. Hence the much-sought supersolid state with broken continuous translation invariance in one direction and broken global U(1) invariance, occurs generically as a metastable state in this system as a result of dipole interaction. The ferromagnetic state parallel to the applied magnetic field becomes striped in a finite system at strong dipolar coupling.

  8. Optimized Bose-Einstein-condensate production in a dipole trap based on a 1070-nm multifrequency laser: Influence of enhanced two-body loss on the evaporation process

    SciTech Connect (OSTI)

    Lauber, T.; Kueber, J.; Wille, O.; Birkl, G.

    2011-10-15

    We present an optimized strategy for the production of tightly confined Bose-Einstein condensates (BEC) of {sup 87}Rb in a crossed dipole trap with direct loading from a magneto-optical trap. The dipole trap is created with light of a multifrequency fiber laser with a center wavelength of 1070 nm. Evaporative cooling is performed by ramping down the laser power only. A comparison of the resulting atom number in an almost pure BEC to the initial atom number and the value for the gain in phase space density per atom lost confirm that this straightforward strategy is very efficient. We observe that the temporal characteristics of evaporation sequence are strongly influenced by power-dependent two-body losses resulting from enhanced optical pumping to the higher-energy hyperfine state. We characterize these losses and compare them to results obtained with a single-frequency laser at 1030 nm.

  9. Millimeter wave detection via Autler-Townes splitting in rubidium Rydberg atoms

    SciTech Connect (OSTI)

    Gordon, Joshua A. Holloway, Christopher L.; Schwarzkopf, Andrew; Anderson, Dave A.; Miller, Stephanie; Thaicharoen, Nithiwadee; Raithel, Georg

    2014-07-14

    In this paper, we demonstrate the detection of millimeter waves via Autler-Townes splitting in {sup 85}Rb Rydberg atoms. This method may provide an independent, atom-based, SI-traceable method for measuring mm-wave electric fields, which addresses a gap in current calibration techniques in the mm-wave regime. The electric-field amplitude within a rubidium vapor cell in the WR-10 wave guide band is measured for frequencies of 93.71 GHz and 104.77?GHz. Relevant aspects of Autler-Townes splitting originating from a four-level electromagnetically induced transparency scheme are discussed. We measured the E-field generated by an open-ended waveguide using this technique. Experimental results are compared to a full-wave finite element simulation.

  10. inner-sphere complexation of cations at the rutile-water interface: A concise surface structural interpretation with the CD and MUSIC model

    SciTech Connect (OSTI)

    Ridley, Mora K.; Hiemstra, T; Van Riemsdijk, Willem H.; Machesky, Michael L.

    2009-01-01

    Acid base reactivity and ion-interaction between mineral surfaces and aqueous solutions is most frequently investigated at the macroscopic scale as a function of pH. Experimental data are then rationalized by a variety of surface complexation models. These models are thermodynamically based which in principle does not require a molecular picture. The models are typically calibrated to relatively simple solid-electrolyte solution pairs and may provide poor descriptions of complex multicomponent mineral aqueous solutions, including those found in natural environments. Surface complexation models may be improved by incorporating molecular-scale surface structural information to constrain the modeling efforts. Here, we apply a concise, molecularly-constrained surface complexation model to a diverse suite of surface titration data for rutile and thereby begin to address the complexity of multi-component systems. Primary surface charging curves in NaCl, KCl, and RbCl electrolyte media were fit simultaneously using a charge distribution (CD) and multisite complexation (MUSIC) model [Hiemstra T. and Van Riemsdijk W. H. (1996) A surface structural approach to ion adsorption: the charge distribution (CD) model. J. Colloid Interf. Sci. 179, 488 508], coupled with a Basic Stern layer description of the electric double layer. In addition, data for the specific interaction of Ca2+ and Sr2+ with rutile, in NaCl and RbCl media, were modeled. In recent developments, spectroscopy, quantum calculations, and molecular simulations have shown that electrolyte and divalent cations are principally adsorbed in various inner-sphere configurations on the rutile 110 surface [Zhang Z., Fenter P., Cheng L., Sturchio N. C., Bedzyk M. J., Pr edota M., Bandura A., Kubicki J., Lvov S. N., Cummings P. T., Chialvo A. A., Ridley M. K., Be ne zeth P., Anovitz L., Palmer D. A., Machesky M. L. and Wesolowski D. J. (2004) Ion adsorption at the rutile water interface: linking molecular and macroscopic properties. Langmuir 20, 4954 4969]. Our CD modeling results are consistent with these adsorbed configurations provided adsorbed cation charge is allowed to be distributed between the surface (0-plane) and Stern plane (1-plane). Additionally, a complete description of our titration data required inclusion of outer-sphere binding, principally for Cl which was common to all solutions, but also for Rb+ and K+. These outer-sphere species were treated as point charges positioned at the Stern layer, and hence determined the Stern layer capacitance value. The modeling results demonstrate that a multi-component suite of experimental data can be successfully rationalized within a CD and MUSIC model using a Stern-based description of the EDL. Furthermore, the fitted CD values of the various inner-sphere complexes of the mono- and divalent ions can be linked to the microscopic structure of the surface complexes and other data found by spectroscopy as well as molecular dynamics (MD). For the Na+ ion, the fitted CD value points to the presence of bidenate inner-sphere complexation as suggested by a recent MD study. Moreover, its MD dominance quantitatively agrees with the CD model prediction. For Rb+, the presence of a tetradentate complex, as found by spectroscopy, agreed well with the fitted CD and its predicted presence was quantitatively in very good agreement with the amount found by spectroscopy.

  11. Neutron activation analysis of NBS oyster tissue (SRM 1566) and IAEA animal bone (H-5)

    SciTech Connect (OSTI)

    Lepel, E.A.; Laul, J.C.

    1983-10-01

    Data have been presented for 35 elements determined by INAA for NBS oyster tissue (SRM 1566) and for 38 elements determined by INAA and RNAA for IAEA animal bone (H-5). The experimental data showed excellent agreement with published values wherever the comparison exists. Additional trace-element data in the ppb range have been presented for the elements Sc, Sb, Cs, La, Ce, Nd, Sm, Eu, Tb, Dy, Ho, Yb, Lu, Hf, Ta, W and Th in NBS oyster tissue. Also, additional trace-element data for IAEA animal bone (H-5) in the ppb range for the elements Al, Sc, Co, Rb, Cs, La, Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, Tm, Yb, lu, Hf, Ta and Th have been presented.

  12. CSTEC Working Groups

    Broader source: All U.S. Department of Energy (DOE) Office Webpages (Extended Search)

    January 2 010 --- A ugust 2 010 Transport ( merged i nto o ther T hin F ilms, T E, a nd A bsorption a fter s ummer 2 010) February 1 Discussion a bout f ormat o f m eetings February 2 2 PC K u p resented h is r esearch June 11 Sung J oo K im p resenting July 3 0 Discussion o f O rtmann 2 009 P RB p aper o n c harge t ransport Theory ( merged i nto o ther w orking g roups) February 1 9 Discussion o n f ormat o f m eetings Thin F ilms February 9 Discussion o f f ormat o f m eetings March 2 Steve F

  13. DOE/EIS-0132-F United States Department of Energy

    Office of Energy Efficiency and Renewable Energy (EERE) Indexed Site

    132-F United States Department of Energy Final Environmental Impact Statement REMEDIAL ACTIONS AT THE FORMER UNION CARBIDE CORPORATION U RANIUM MILL SITES RIFLE, GARFIELD COUNTY, COLORADO VOLUME I: TEXT MARCH 1990 U.S. DEPARTMENT OF ENERGY R emed i a l A c t i o n s a t t h e Fo rme r U n i on C a rb i d e C o rporat i on U ra n i um M i l l S i t e s R i f l e , Ga r f i e l d C o u n t y , C o l o ra d o F i n a l Ma rch 1 9 9 0 U . s . Depa rtmen t o f E n e rgy UMTRA P roj e c t O f f i c e

  14. Enhancement of ultracold molecule formation by local control in the nanosecond regime

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Carini, J. L.; Kallush, S.; Kosloff, R.; Gould, P. L.

    2015-02-01

    We describe quantum simulations of ultracold 87Rb2 molecule formation using photoassociation (PA) with nanosecond-time-scale pulses of frequency chirped light. In particular, we compare the case of a linear chirp to one where the frequency evolution is optimized by local control (LC) of the phase, and find that LC can provide a significant enhancement. The resulting optimal frequency evolution corresponds to a rapid jump from the PA absorption resonance to a downward transition to a bound level of the lowest triplet state. We also consider the case of two frequencies and investigate interference effects. The assumed chirp parameters should be achievablemore »with nanosecond pulse shaping techniques and are predicted to provide a significant enhancement over recent experiments with linear chirps.« less

  15. Frequency mixing crystal

    DOE Patents [OSTI]

    Ebbers, Christopher A.; Davis, Laura E.; Webb, Mark

    1992-01-01

    In a laser system for converting infrared laser light waves to visible light comprising a source of infrared laser light waves and means of harmoic generation associated therewith for production of light waves at integral multiples of the frequency of the original wave, the improvement of said means of harmonic generation comprising a crystal having the chemical formula X.sub.2 Y(NO.sub.3).sub.5 .multidot.2 nZ.sub.2 o wherein X is selected from the group consisting of Li, Na, K, Rb, Cs, and Tl; Y is selected from the group consisting of Sc, Y, La, Ce, Nd, Pr, Sm, Eu, Gd, Tb, Dy, Ho, Er, Tm, Yb, Lu, Al, Ga, and In; Z is selected from the group consisting of H and D; and n ranges from 0 to 4.

  16. Ternary oxide nanostructures and methods of making same

    DOE Patents [OSTI]

    Wong, Stanislaus S.; Park, Tae-Jin

    2009-09-08

    A single crystalline ternary nanostructure having the formula A.sub.xB.sub.yO.sub.z, wherein x ranges from 0.25 to 24, and y ranges from 1.5 to 40, and wherein A and B are independently selected from the group consisting of Ag, Al, As, Au, B, Ba, Br, Ca, Cd, Ce, Cl, Cm, Co, Cr, Cs, Cu, Dy, Er, Eu, F, Fe, Ga, Gd, Ge, Hf, Ho, I, In, Ir, K, La, Li, Lu, Mg, Mn, Mo, Na, Nb, Nd, Ni, Os, P, Pb, Pd, Pr, Pt, Rb, Re, Rh, Ru, S, Sb, Sc, Se, Si, Sm, Sn, Sr, Ta, Tb, Tc, Te, Ti, Tl, Tm, U, V, W, Y, Yb, and Zn, wherein the nanostructure is at least 95% free of defects and/or dislocations.

  17. Systems and methods for treating material

    DOE Patents [OSTI]

    Scheele, Randall D; McNamara, Bruce K

    2014-10-21

    Systems for treating material are provided that can include a vessel defining a volume, at least one conduit coupled to the vessel and in fluid communication with the vessel, material within the vessel, and NF.sub.3 material within the conduit. Methods for fluorinating material are provided that can include exposing the material to NF.sub.3 to fluorinate at least a portion of the material. Methods for separating components of material are also provided that can include exposing the material to NF.sub.3 to at least partially fluorinate a portion of the material, and separating at least one fluorinated component of the fluorinated portion from the material. The materials exposed to the NF.sub.3 material can include but are not limited to one or more of U, Ru, Rh, Mo, Tc, Np, Pu, Sb, Ag, Am, Sn, Zr, Cs, Th, and/or Rb.

  18. Evaluation of a commercially available passively Q-switched Nd:YAG laser with LiF:F-2 saturable absorber for laser-induced breakdown spectroscopy

    SciTech Connect (OSTI)

    Carson, Cantwell; Goueguel, Christian; Sanghapi, Herve; Jinesh, Jain; McIntyre, Dustin

    2015-12-11

    Interest in passively Q-switched microchip lasers as a means for miniaturization of laser-induced breakdown spectroscopy (LIBS) apparatus has rapidly grown in the last years. To explore the possibility of using a comparatively UV–vis transparent absorber, we herein present the first report on the evaluation of a commercially available flash lamp-pumped passively Q-switched Nd:YAG laser with LiF: saturable absorber as an excitation source in LIBS. Quantitative measurements of barium, strontium, rubidium and lithium in granite, rhyolite, basalt and syenite whole-rock glass samples were performed. Using a gated intensified benchtop spectrometer, limits of detection of 0.97, 23, 37, and 144 ppm were obtained for Li, Sr, Rb, and Ba, respectively. Finally, we discuss the advantages of using such a laser unit for LIBS applications in terms of ablation efficiency, analytical performances, output energy, and standoff capabilities.

  19. Nuclear shape transitions in neutron-rich medium-mass nuclei

    SciTech Connect (OSTI)

    Sarriguren, P.; Rodriguez-Guzman, R.; Robledo, L. M.

    2012-10-20

    We study the isotopic evolution of the ground-state nuclear shapes in neutron-rich Kr, Rb, Sr, Y, Zr, Nb, and Mo isotopic chains. Both even-even and odd-A nuclei are included in the analysis. For the latter we also study the systematics of their one-quasiparticle low-lying configurations. The theoretical approach is based on a selfconsistent Hartree-Fock-Bogoliubov formalism with finite range Gogny energy density functionals. Neutron separation energies, charge radii, and the spin-parity of the ground states are calculated and compared with available data. Shape-transition signatures are identified around N= 60 isotones as discontinuities in both charge radii isotopic shifts and spin-parities of the ground states. The nuclear deformation including triaxiality is shown to play a relevant role in the understanding of the bulk and spectroscopic features of the ground and low-lying one-quasiparticle states.

  20. STATE YJ#wIY STbNs

    Office of Legacy Management (LM)

    Pap lb. 26 12121167 6EmcFi 3, 1987 STATE YJ#wIY STbNs SlTEN4E . TLFrS CMEEE FfCoP~ MY IWICATE TMT THIS SITE DID ESEMUX TIE WE WILL HOT BE INULWJ IN Flmw. SITE IS uiwl LIENSE. SITE w ItMSTIGMED As R NJTRiTIk FWW SITE, Ho RRDI&iZTCV!N FOUWD. ELIHlNMION PWH w DWLETES 111 CYIWb, hu ww REEDM XTIW IS REWIW. tEVRE?ENT OF EXTRKTIOH OF UuwIUn t-KW Lx ANP bt&LYSIS a cm FM TtE bfc / N.E. RbD!ccoGIC.@L EQLTNLb6 k?T!W. LEbD U.S. PUBLIC KALTH mvrE nom LRNDFILL

  1. X-ray area backlighter development at the National Ignition Facility (invited)

    SciTech Connect (OSTI)

    Barrios, M. A. Fournier, K. B.; Smith, R.; Lazicki, A.; Rygg, R.; Fratanduono, D. E.; Eggert, J.; Park, H.-S.; Huntington, C.; Bradley, D. K.; Landen, O. L.; Collins, G. W.; Regan, S. P.; Epstein, R.

    2014-11-15

    1D spectral imaging was used to characterize the K-shell emission of Z ? 3035 and Z ? 4042 laser-irradiated foils at the National Ignition Facility. Foils were driven with up to 60 kJ of 3? light, reaching laser irradiances on target between 0.5 and 20 10{sup 15} W/cm{sup 2}. Laser-to-X-ray conversion efficiency (CE) into the He{sub ?} line (plus satellite emission) of 1.0%1.5% and 0.15%0.2% was measured for Z ? 3032 and Z ? 4042, respectively. Measured CE into He{sub ?} (plus satellite emission) of Br (Z = 35) compound foils (either KBr or RbBr) ranged between 0.16% and 0.29%. Measured spectra are compared with 1D non-local thermodynamic equilibrium atomic kinetic and radiation transport simulations, providing a fast and accurate predictive capability.

  2. AGR-2 Data Qualification Report for ATR Cycles 149B, 150A, 150B, 151A, and 151B

    SciTech Connect (OSTI)

    Michael L. Abbott; Binh T. Pham

    2012-06-01

    This report provides the data qualification status of AGR-2 fuel irradiation experimental data from Advanced Test Reactor (ATR) cycles 149B, 150A, 150B, 151A, and 151B), as recorded in the Nuclear Data Management and Analysis System (NDMAS). The AGR-2 data streams addressed include thermocouple temperatures, sweep gas data (flow rate, pressure, and moisture content), and fission product monitoring system (FPMS) data for each of the six capsules in the experiment. A total of 3,307,500 5-minute thermocouple and sweep gas data records were received and processed by NDMAS for this period. There are no AGR-2 data for cycle 150A because the experiment was removed from the reactor. Of these data, 82.2% were determined to be Qualified based on NDMAS accuracy testing and data validity assessment. There were 450,557 Failed temperature records due to thermocouple failures, and 138,528 Failed gas flow records due to gas flow cross-talk and leakage problems that occurred in the capsules after cycle 150A. For FPMS data, NDMAS received and processed preliminary release rate and release-to-birth rate ratio (R/B) data for the first three reactor cycles (cycles 149B, 150B, and 151B). This data consists of 45,983 release rate records and 45,235 R/B records for the 12 radionuclides reported. The qualification status of these FPMS data has been set to In Process until receipt of QA-approved data generator reports. All of the above data have been processed and tested using a SAS-based enterprise application software system, stored in a secure Structured Query Language database, and made available on the NDMAS Web portal (http://ndmas.inl.gov) for both internal and external VHTR project participants.

  3. Structure of the unique SEFIR domain from human interleukin 17 receptor A reveals a composite ligand-binding site containing a conserved ?-helix for Act1 binding and IL-17 signaling

    SciTech Connect (OSTI)

    Zhang, Bing [Oklahoma State University, Stillwater, OK 74078 (United States); Liu, Caini; Qian, Wen [Lerner Research Institute, Cleveland Clinic, 9500 Euclid Avenue, Cleveland, OH 44195 (United States); Han, Yue [Oklahoma State University, Stillwater, OK 74078 (United States); Li, Xiaoxia, E-mail: lix@ccf.org [Lerner Research Institute, Cleveland Clinic, 9500 Euclid Avenue, Cleveland, OH 44195 (United States); Deng, Junpeng, E-mail: lix@ccf.org [Oklahoma State University, Stillwater, OK 74078 (United States)

    2014-05-01

    Crystal structure of the SEFIR domain from human IL-17 receptor A provides new insights into IL-17 signaling. Interleukin 17 (IL-17) cytokines play a crucial role in mediating inflammatory and autoimmune diseases. A unique intracellular signaling domain termed SEFIR is found within all IL-17 receptors (IL-17Rs) as well as the key adaptor protein Act1. SEFIR-mediated proteinprotein interaction is a crucial step in IL-17 cytokine signaling. Here, the 2.3 resolution crystal structure of the SEFIR domain of IL-17RA, the most commonly shared receptor for IL-17 cytokine signaling, is reported. The structure includes the complete SEFIR domain and an additional ?-helical C-terminal extension, which pack tightly together to form a compact unit. Structural comparison between the SEFIR domains of IL-17RA and IL-17RB reveals substantial differences in protein topology and folding. The uniquely long insertion between strand ?C and helix ?C in IL-17RA SEFIR is mostly well ordered, displaying a helix (?CC?{sub ins}) and a flexible loop (CC?). The DD? loop in the IL-17RA SEFIR structure is much shorter; it rotates nearly 90 with respect to the counterpart in the IL-17RB SEFIR structure and shifts about 12 to accommodate the ?CC?{sub ins} helix without forming any knots. Helix ?C was identified as critical for its interaction with Act1 and IL-17-stimulated gene expression. The data suggest that the heterotypic SEFIRSEFIR association via helix ?C is a conserved and signature mechanism specific for IL-17 signaling. The structure also suggests that the downstream motif of IL-17RA SEFIR together with helix ?C could provide a composite ligand-binding surface for recruiting Act1 during IL-17 signaling.

  4. Analysis of three sets of SWIW tracer-test data using a two-population complex fracture model for matrix diffusion and sorption

    SciTech Connect (OSTI)

    Doughty, C.; Tsang, C.F.

    2009-08-01

    A complex fracture model employing two populations for diffusion and sorption is proposed to analyze three representative single-well injection-withdrawal (SWIW) tracer tests from Forsmark and Laxemar, the two sites under investigation by the Swedish Nuclear Fuel and Waste Management Company (SKB). One population represents the semi-infinite rock matrix and the other represents finite blocks that can become saturated, thereafter accepting no further diffusion or sorption. The diffusion and sorption parameters of the models are inferred by matching tracer breakthrough curves (BTCs). Three tracers are simultaneously injected, uranine (Ur), which is conservative, and rubidium (Rb) and cesium (Cs), which are non-conservative. For non-sorbing tracer uranine, the finite blocks become saturated with test duration of the order of 10 hours, and both the finite and the semi-infinite populations play a distinct role in controlling BTCs. For sorbing tracers Rb and Cs, finite blocks do not saturate, but act essentially as semi-infinite, and thus BTC behavior is comparable to that obtained for a model containing only a semi-infinite rock matrix. The ability to obtain good matches to BTCs for both sorbing and non-sorbing tracers for these three different SWIW data sets demonstrates that the two-population complex fracture model may be a useful conceptual model to analyze all SWIW tracer tests in fractured rock, and perhaps also usual multiwell tracer tests. One of the two populations should be semi-infinite rock matrix and the other finite blocks that can saturate. The latter can represent either rock blocks or gouge within the fracture, a fracture skin zone, or stagnation zones.

  5. Accurate potential energy, dipole moment curves, and lifetimes of vibrational states of heteronuclear alkali dimers

    SciTech Connect (OSTI)

    Fedorov, Dmitry A.; Varganov, Sergey A.; Derevianko, Andrei

    2014-05-14

    We calculate the potential energy curves, the permanent dipole moment curves, and the lifetimes of the ground and excited vibrational states of the heteronuclear alkali dimers XY (X, Y = Li, Na, K, Rb, Cs) in the X{sup 1}?{sup +} electronic state using the coupled cluster with singles doubles and triples method. All-electron quadruple-? basis sets with additional core functions are used for Li and Na, and small-core relativistic effective core potentials with quadruple-? quality basis sets are used for K, Rb, and Cs. The inclusion of the coupled cluster non-perturbative triple excitations is shown to be crucial for obtaining the accurate potential energy curves. A large one-electron basis set with additional core functions is needed for the accurate prediction of permanent dipole moments. The dissociation energies are overestimated by only 14 cm{sup ?1} for LiNa and by no more than 114 cm{sup ?1} for the other molecules. The discrepancies between the experimental and calculated harmonic vibrational frequencies are less than 1.7 cm{sup ?1}, and the discrepancies for the anharmonic correction are less than 0.1 cm{sup ?1}. We show that correlation between atomic electronegativity differences and permanent dipole moment of heteronuclear alkali dimers is not perfect. To obtain the vibrational energies and wave functions the vibrational Schrdinger equation is solved with the B-spline basis set method. The transition dipole moments between all vibrational states, the Einstein coefficients, and the lifetimes of the vibrational states are calculated. We analyze the decay rates of the vibrational states in terms of spontaneous emission, and stimulated emission and absorption induced by black body radiation. In all studied heteronuclear alkali dimers the ground vibrational states have much longer lifetimes than any excited states.

  6. Fluidized Bed Steam Reforming (FBSR) Mineralization for High Organic and Nitrate Waste Streams for the Global Nuclear Energy Partnership (GNEP)

    SciTech Connect (OSTI)

    Jantzen, C.M.; Williams, M.R. [Savannah River National Laboratory, Aiken, SC (United States)

    2008-07-01

    Waste streams that may be generated by the Global Nuclear Energy Partnership (GNEP) Advanced Energy Initiative may contain significant quantities of organics (0-53 wt%) and/or nitrates (0-56 wt%). Decomposition of high nitrate streams requires reducing conditions, e.g. organic additives such as sugar or coal, to reduce the NOx in the off-gas to N{sub 2} to meet the Clean Air Act (CAA) standards during processing. Thus, organics will be present during waste form stabilization regardless of which GNEP processes are chosen, e.g. organics in the feed or organics for nitrate destruction. High organic containing wastes cannot be stabilized with the existing HLW Best Developed Available Technology (BDAT) which is HLW vitrification (HLVIT) unless the organics are removed by preprocessing. Alternative waste stabilization processes such as Fluidized Bed Steam Reforming (FBSR) operate at moderate temperatures (650-750 deg. C) compared to vitrification (1150-1300 deg. C). FBSR converts organics to CAA compliant gases, creates no secondary liquid waste streams, and creates a stable mineral waste form that is as durable as glass. For application to the high Cs-137 and Sr-90 containing GNEP waste streams a single phase mineralized Cs-mica phase was made by co-reacting illite clay and GNEP simulated waste. The Cs-mica accommodates up to 30% wt% Cs{sub 2}O and all the GNEP waste species, Ba, Sr, Rb including the Cs-137 transmutation to Ba-137. For reference, the cesium mineral pollucite (CsAlSi{sub 2}O{sub 6}), currently being studied for GNEP applications, can only be fabricated at {>=}1000 deg. C. Pollucite mineralization creates secondary aqueous waste streams and NOx. Pollucite is not tolerant of high concentrations of Ba, Sr or Rb and forces the divalent species into different mineral host phases. The pollucite can accommodate up to 33% wt% Cs{sub 2}O. (authors)

  7. FLUIDIZED BED STEAM REFORMING MINERALIZATION FOR HIGH ORGANIC AND NITRATE WASTE STREAMS FOR THE GLOBAL NUCLEAR ENERGY PARTNERSHIP

    SciTech Connect (OSTI)

    Jantzen, C; Michael Williams, M

    2008-01-11

    Waste streams that may be generated by the Global Nuclear Energy Partnership (GNEP) Advanced Energy Initiative may contain significant quantities of organics (0-53 wt%) and/or nitrates (0-56 wt%). Decomposition of high nitrate streams requires reducing conditions, e.g. organic additives such as sugar or coal, to reduce the NO{sub x} in the off-gas to N{sub 2} to meet the Clean Air Act (CAA) standards during processing. Thus, organics will be present during waste form stabilization regardless of which GNEP processes are chosen, e.g. organics in the feed or organics for nitrate destruction. High organic containing wastes cannot be stabilized with the existing HLW Best Developed Available Technology (BDAT) which is HLW vitrification (HLVIT) unless the organics are removed by preprocessing. Alternative waste stabilization processes such as Fluidized Bed Steam Reforming (FBSR) operate at moderate temperatures (650-750 C) compared to vitrification (1150-1300 C). FBSR converts organics to CAA compliant gases, creates no secondary liquid waste streams, and creates a stable mineral waste form that is as durable as glass. For application to the high Cs-137 and Sr-90 containing GNEP waste streams a single phase mineralized Cs-mica phase was made by co-reacting illite clay and GNEP simulated waste. The Cs-mica accommodates up to 30% wt% Cs{sub 2}O and all the GNEP waste species, Ba, Sr, Rb including the Cs-137 transmutation to Ba-137. For reference, the cesium mineral pollucite (CsAlSi{sub 2}O{sub 6}), currently being studied for GNEP applications, can only be fabricated at {ge} 1000 C. Pollucite mineralization creates secondary aqueous waste streams and NO{sub x}. Pollucite is not tolerant of high concentrations of Ba, Sr or Rb and forces the divalent species into different mineral host phases. The pollucite can accommodate up to 33% wt% Cs{sub 2}O.

  8. Synthesis and characterization of F-N-W-codoped TiO{sub 2} photocatalyst with enhanced visible light response

    SciTech Connect (OSTI)

    Shi, Xiaoliang; School of Materials Science and Engineering, Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070 ; Qin, Haibo; Yang, Xingyong; Zhang, Qiaoxin; School of Materials Science and Engineering, Wuhan University of Technology, 122 Luoshi Road, Wuhan 430070

    2012-12-15

    Graphical abstract: Display Omitted Highlights: ? Anatase F-N-W-codoped TiO{sub 2} was prepared by a solgel-hydrothermal method. ? Under visible illumination, carbon removal rate of RB reached 94% using F-7NW-TiO{sub 2}. ? F, N and W dopants narrowed band gap and lowed charge pairs recombination rate. ? There were W{sub x}Ti{sub 1?x}O{sub 2}, O-Ti-N and valence variation of W ions existing. -- Abstract: Anatase F-N-W-codoped TiO{sub 2} photocatalyst was successfully prepared by a method combining solgel with hydrothermal treatment. Effects of F, N and W ion dosage concentration on the crystallinity, morphology, grain size and chemical status of the photocatalyst were investigated. The results showed that the F-7NW-TiO{sub 2} photocatalyst composed of uniform ellipsoidal particles around 20 nm in length and 10 nm in width, and the photocatalyst displayed enhanced visible-light absorption and photocatalytic activities. Using the photocatalyst and under visible irradiation for 1.5 h, the decoloration percent of RB and carbon removal rate were about 98% and 94% respectively, which were much higher than that of commercial P25, TiO{sub 2}, N-W-TiO{sub 2} and F-TiO{sub 2}. The high visible-light photocatalytic activity of F-7NW-TiO{sub 2} might result from narrowing the band gap and lowing charge pairs recombination rate for the W{sub x}Ti{sub 1?x}O{sub 2}, O-Ti-N and valence variation of W ions existing.

  9. Phosphate glass useful in high energy lasers

    DOE Patents [OSTI]

    Hayden, Yuiko T. (Clarks Summit, PA); Payne, Stephen A. (Castro Valley, CA); Hayden, Joseph S. (Clarks Summit, PA); Campbell, John H. (Livermore, CA); Aston, Mary Kay (Moscow, PA); Elder, Melanie L. (Dublin, CA)

    1996-01-01

    In a high energy laser system utilizing phosphate laser glass components to amplify the laser beam, the laser system requires a generated laser beam having an emission bandwidth of less than 26 nm and the laser glass components consist essentially of (on an oxide composition basis) in mole percent: P{sub 2}O{sub 5}, 50--75; Al{sub 2}O{sub 3}, {gt}0--10; K{sub 2}O, {gt}0--30; MgO, 0--30; CaO, 0--30; Li{sub 2}O, 0--20; Na{sub 2}O, 0--20; Rb{sub 2}O, 0--20; Cs{sub 2}O, 0--20; BeO, 0--20; SrO, 0--20; BaO, 0--20; ZnO, 0--20; PbO, 0--20; B{sub 2}O{sub 3}, 0--10; Y{sub 2}O{sub 3}, 0--10; La{sub 2}O{sub 3}, 0--8; Ln{sub 2}O{sub 3}, 0.01--8; wherein the sum of MgO and CaO is >0--30; the sum of Li{sub 2}O, Na{sub 2}O, Rb{sub 2}O, and Cs{sub 2}O is 0--20; the sum of BeO, SrO, BaO, ZnO, and PbO is 0--20; the sum of B{sub 2}O{sub 3} and Y{sub 2}O{sub 3} is 0--10; and Ln{sub 2}O{sub 3} represents the sum of the oxides of active lasing lanthanides of atomic number 58--71. 21 figs.

  10. Phosphate glass useful in high energy lasers

    DOE Patents [OSTI]

    Hayden, Y.T.; Payne, S.A.; Hayden, J.S.; Campbell, J.H.; Aston, M.K.; Elder, M.L.

    1996-06-11

    In a high energy laser system utilizing phosphate laser glass components to amplify the laser beam, the laser system requires a generated laser beam having an emission bandwidth of less than 26 nm and the laser glass components consist essentially of (on an oxide composition basis) in mole percent: P{sub 2}O{sub 5}, 50--75; Al{sub 2}O{sub 3}, {gt}0--10; K{sub 2}O, {gt}0--30; MgO, 0--30; CaO, 0--30; Li{sub 2}O, 0--20; Na{sub 2}O, 0--20; Rb{sub 2}O, 0--20; Cs{sub 2}O, 0--20; BeO, 0--20; SrO, 0--20; BaO, 0--20; ZnO, 0--20; PbO, 0--20; B{sub 2}O{sub 3}, 0--10; Y{sub 2}O{sub 3}, 0--10; La{sub 2}O{sub 3}, 0--8; Ln{sub 2}O{sub 3}, 0.01--8; wherein the sum of MgO and CaO is >0--30; the sum of Li{sub 2}O, Na{sub 2}O, Rb{sub 2}O, and Cs{sub 2}O is 0--20; the sum of BeO, SrO, BaO, ZnO, and PbO is 0--20; the sum of B{sub 2}O{sub 3} and Y{sub 2}O{sub 3} is 0--10; and Ln{sub 2}O{sub 3} represents the sum of the oxides of active lasing lanthanides of atomic number 58--71. 21 figs.

  11. A behaviorally-explicit approach for delivering vaccine baits to mesopredators to control epizootics in fragmented landscapes

    SciTech Connect (OSTI)

    Beasley, James C.; Atwood, Todd C.; Byrne, Michael E.; Vercauteren, Kurt C.; Johnson, Shylo R.; Olin E. Rhodes, Jr.; Schnell, Matthias Johannes

    2015-01-14

    Despite the widespread use of aerial baiting to manage epizootics among free-ranging populations,particularly in rabies management, bait acceptance and seroconversion rates often are lower than required to eliminate spread of disease. Our objectives in this study, therefore, were to evaluate the performance of stratified bait distribution models derived from resource selection functions (RSF) on uptake of placebo rabies baits by raccoons (Procyon lotor) and Virginia opossums (Didelphis virginiana), as well as the probability of bait uptake as a function of proximity to bait distribution areas in fragmented agricultural ecosystems. Among 478 raccoons and 108 opossums evaluated for presence of Rhodamine B (RB) across 8 sites, only 26% of raccoons and 20% of opossums exhibited marking consistent with bait consumption 1424 days post-baiting. The effective area treated, based on 90% kernel density estimators of marked individuals, ranged from 99240 ha larger than bait distribution zones, with RB marked individuals captured up to 753m beyond the bait zone. Despite incorporation of RSF data into bait distribution models, no differences in uptake rates were observed between treatment and control sites. These data likely reflect the underlying constraints imposed by the loss and fragmentation of habitat on animal movement in heterogeneous landscapes, forcing individuals to optimize movements at coarse (i.e., patch-level) rather than fine spatial scales in highly fragmented environments. Our data also confirm that the probability of bait acceptance decreases with increasing distance from bait zone interiors, even within the zone itself. Thus, although bait acceptance was confirmed beyond bait zone boundaries, the proportion of vaccinated individuals may comprise a small minority of the population at increasing distances from baiting interiors. These data suggest focal baiting creates a buffered area of treated individuals around bait zones or bait stations, but repeated treatments may be needed to achieve sufficient uptake to eradicate disease.

  12. Radiation Doses to Members of the U.S. Population from Ubiquitous Radionuclides in the Body: Part 1, Autopsy and In Vivo Data

    SciTech Connect (OSTI)

    Watson, David J.; Strom, Daniel J.

    2011-02-25

    This paper is part one of a three-part series investigating annual effective doses to residents of the United States from intakes of ubiquitous radionuclides, including radionuclides occurring naturally, radionuclides whose concentrations are technologically enhanced, and anthropogenic radionuclides. This series of papers explicitly excludes intakes from inhaling 222Rn, 220Rn, and their short-lived decay products; it also excludes intakes of radionuclides in occupational and medical settings. The goal of part one of this work was to review, summarize, and characterize all published and some unpublished data for U.S. residents on ubiquitous radionuclide concentrations in tissues and organs. Forty-five papers and reports were obtained and their data reviewed, and three data sets were obtained via private communication. The 45 radionuclides of interest are the 238U series (14 nuclides), the actinium series (headed by 235U; 11 nuclides), and the 232Th series (11 nuclides); primordial radionuclides 87Rb and 40 K; cosmogenic and fallout radionuclides 14C and 3H; and purely anthropogenic radionuclides 137Cs-137mBa, 129I, and 90Sr-90Y. Measurements judged to be relevant were available for only 15 of these radionuclides: 238U, 235U, 234U, 232Th, 230Th, 228Th, 228Ra, 226Ra, 210Pb, 210Po, 137Cs, 87Rb, 40K, 14C, and 3H. Recent and relevant measurements were not available for 129I and 90Sr-90Y. A total of 11,714 radionuclide concentration measurements were found in one or more tissues or organs from 14 States. Data on age, sex, geographic locations, height, and weight of subjects were available only sporadically. Too often authors did not provide meaningful values of uncertainty of measurements so that variability in data sets is confounded with measurement uncertainty. The following papers detail how these shortcomings are overcome to achieve the goals of the three-part series.

  13. Nuclear Data Sheets for A=77

    SciTech Connect (OSTI)

    Singh B.; Nica N.; Singh,B.; Nica,N.

    2012-05-01

    The experimental nuclear spectroscopic data for known nuclides of mass number 77 (Ni, Cu, Zn, Ga, Ge, As, Se, Br, Kr, Rb, Sr, Y) have been evaluated and presented together with adopted properties for levels and {gamma} rays. New high-spin data are available for {sup 77}Ga, {sup 77}Br and {sup 77}Kr. New precise single-particle transfer cross section data are available for {sup 77}Ge, {sup 77}As, {sup 77}Se and {sup 77}Br from eight different reactions (2009Ka06,2008Sc03); these data give information for occupancy of valence neutron orbitals in the ground states of target nuclides: {sup 76}Ge, {sup 76}Se and {sup 78}Se. No significant new data since the 1997 NDS for A = 77 (1997Fa12) have been reported for {sup 77}Rb and {sup 77}Sr. No data are yet available for excited states in {sup 77}Ni, {sup 77}Cu and {sup 77}Y. Level schemes from the radioactive decays of {sup 77}Ni to {sup 77}Cu and {sup 77}Y to {sup 77}Sr are unknown, while those for the decays of {sup 77}Cu to {sup 77}Zn and {sup 77}Ga to {sup 77}Ge are incomplete. Detailed gamma-ray data for {sup 77}Ge from thermal-neutron capture in {sup 76}Ge, together with extensive gamma-ray data from {sup 77}Ge decay to {sup 77}As have become available from 2012Me04. This work benefited from earlier evaluations (1997Fa12,1989Fa07,1980Si05,1973Ur02) of A = 77 nuclides, however, the data presented here supersede those in above evaluations.

  14. A behaviorally-explicit approach for delivering vaccine baits to mesopredators to control epizootics in fragmented landscapes

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Beasley, James C.; Atwood, Todd C.; Byrne, Michael E.; Vercauteren, Kurt C.; Johnson, Shylo R.; Olin E. Rhodes, Jr.; Schnell, Matthias Johannes

    2015-01-14

    Despite the widespread use of aerial baiting to manage epizootics among free-ranging populations,particularly in rabies management, bait acceptance and seroconversion rates often are lower than required to eliminate spread of disease. Our objectives in this study, therefore, were to evaluate the performance of stratified bait distribution models derived from resource selection functions (RSF) on uptake of placebo rabies baits by raccoons (Procyon lotor) and Virginia opossums (Didelphis virginiana), as well as the probability of bait uptake as a function of proximity to bait distribution areas in fragmented agricultural ecosystems. Among 478 raccoons and 108 opossums evaluated for presence of Rhodaminemore » B (RB) across 8 sites, only 26% of raccoons and 20% of opossums exhibited marking consistent with bait consumption 14–24 days post-baiting. The effective area treated, based on 90% kernel density estimators of marked individuals, ranged from 99–240 ha larger than bait distribution zones, with RB marked individuals captured up to 753m beyond the bait zone. Despite incorporation of RSF data into bait distribution models, no differences in uptake rates were observed between treatment and control sites. These data likely reflect the underlying constraints imposed by the loss and fragmentation of habitat on animal movement in heterogeneous landscapes, forcing individuals to optimize movements at coarse (i.e., patch-level) rather than fine spatial scales in highly fragmented environments. Our data also confirm that the probability of bait acceptance decreases with increasing distance from bait zone interiors, even within the zone itself. Thus, although bait acceptance was confirmed beyond bait zone boundaries, the proportion of vaccinated individuals may comprise a small minority of the population at increasing distances from baiting interiors. These data suggest focal baiting creates a buffered area of treated individuals around bait zones or bait stations, but repeated treatments may be needed to achieve sufficient uptake to eradicate disease.« less

  15. Studies of beam dynamics in relativistic klystron two-beam accelerators

    SciTech Connect (OSTI)

    Lidia, Steven M.

    1999-11-01

    Two-beam accelerators (TBAs) based upon free-electron lasers (FELs) or relativistic klystrons (RK-TBAs) have been proposed as efficient power sources for next generation high-energy linear colliders. Studies have demonstrated the possibility of building TBAs from X-band ({approximately}8-12 GHz) through Ka band ({approximately} 30-35 GHz) frequency regions. Provided that further prototyping shows stable beam propagation with minimal current loss and production of good quality, high-power rf fields, this technology is compatible with current schemes for electron-positron colliders in the multi-TeV center-of-mass scale. A new method of simulating the beam dynamics in accelerators of this type has been developed in this dissertation. There are three main components to this simulation. The first is a tracking algorithm to generate nonlinear transfer maps for pushing noninteracting particles through the external fields. The second component is a 3D Particle-In-Cell (PIC) algorithm that solves a set of Helmholtz equations for the self-fields, including the conducting boundary condition, and generates impulses that are interleaved with the nonlinear maps by means of a split-operation algorithm. The Helmholtz equations are solved by a multi-grid algorithm. The third component is an equivalent circuit equation solver that advances the modal rf cavity fields in time due to excitation by the modulated beam. The RTA project is described, and the simulation code is used to design the latter portions of the experiment. Detailed calculations of the beam dynamics and of the rf cavity output are presented and discussed. A beamline design is presented that will generate nearly 1.2 GW of power from 40 input, gain, and output rv cavities over a 10 m distance. The simulations show that beam current losses are acceptable, and that longitudinal and transverse focusing techniques are sufficient capable of maintaining a high degree of beam quality along the entire beamline. Additional experimental efforts are also described.

  16. Deformation Behavior of Sub-micron and Micron Sized Alumina Particles in Compression.

    SciTech Connect (OSTI)

    Sarobol, Pylin; Chandross, Michael E.; Carroll, Jay; Mook, William; Boyce, Brad; Kotula, Paul G.; McKenzie, Bonnie B.; Bufford, Daniel Charles; Hall, Aaron Christopher.

    2014-09-01

    The ability to integrate ceramics with other materials has been limited due to high temperature (>800degC) ceramic processing. Recently, researchers demonstrated a novel process , aerosol deposition (AD), to fabricate ceramic films at room temperature (RT). In this process, sub - micro n sized ceramic particles are accelerated by pressurized gas, impacted on the substrate, plastically deformed, and form a dense film under vacuum. This AD process eliminates high temperature processing thereby enabling new coatings and device integration, in which ceramics can be deposited on metals, plastics, and glass. However, k nowledge in fundamental mechanisms for ceramic particle s to deform and form a dense ceramic film is still needed and is essential in advancing this novel RT technology. In this wo rk, a combination of experimentation and atomistic simulation was used to determine the deformation behavior of sub - micron sized ceramic particle s ; this is the first fundamental step needed to explain coating formation in the AD process . High purity, singl e crystal, alpha alumina particles with nominal size s of 0.3 um and 3.0 um were examined. Particle characterization, using transmission electron microscopy (TEM ), showed that the 0.3 u m particles were relatively defect - free single crystals whereas 3.0 u m p articles were highly defective single crystals or particles contained low angle grain boundaries. Sub - micron sized Al 2 O 3 particles exhibited ductile failure in compression. In situ compression experiments showed 0.3um particles deformed plastically, fractured, and became polycrystalline. Moreover, dislocation activit y was observed within the se particles during compression . These sub - micron sized Al 2 O 3 particles exhibited large accum ulated strain (2 - 3 times those of micron - sized particles) before first fracture. I n agreement with the findings from experimentation , a tomistic simulation s of nano - Al 2 O 3 particles showed dislocation slip and significant plastic deformation during compressi on . On the other hand, the micron sized Al 2 O 3 particles exhibited brittle f racture in compression. In situ compression experiments showed 3um Al 2 O 3 particles fractured into pieces without observable plastic deformation in compression. Particle deformation behaviors will be used to inform Al 2 O 3 coating deposition parameters and particle - particle bonding in the consolidated Al 2 O 3 coatings.

  17. AGR-1 Irradiation Test Final As-Run Report

    SciTech Connect (OSTI)

    Blaise P. Collin

    2012-06-01

    This document presents the as-run analysis of the AGR-1 irradiation experiment. AGR-1 is the first of eight planned irradiations for the Advanced Gas Reactor (AGR) Fuel Development and Qualification Program. Funding for this program is provided by the US Department of Energy (DOE) as part of the Next-Generation Nuclear Plant (NGNP) project. The objectives of the AGR-1 experiment are: 1. To gain experience with multi-capsule test train design, fabrication, and operation with the intent to reduce the probability of capsule or test train failure in subsequent irradiation tests. 2. To irradiate fuel produced in conjunction with the AGR fuel process development effort. 3. To provide data that will support the development of an understanding of the relationship between fuel fabrication processes, fuel product properties, and irradiation performance. In order to achieve the test objectives, the AGR-1 experiment was irradiated in the B-10 position of the Advanced Test Reactor (ATR) at the Idaho National Laboratory (INL) for a total duration of 620 effective full power days of irradiation. Irradiation began on December 24, 2006 and ended on November 6, 2009 spanning 13 ATR cycles and approximately three calendar years. The test contained six independently controlled and monitored capsules. Each capsule contained 12 compacts of a single type, or variant, of the AGR coated fuel. No fuel particles failed during the AGR-1 irradiation. Final burnup values on a per compact basis ranged from 11.5 to 19.6 %FIMA, while fast fluence values ranged from 2.21 to 4.39 ?1025 n/m2 (E >0.18 MeV). Well say something here about temperatures once thermal recalc is done. Thermocouples performed well, failing at a lower rate than expected. At the end of the irradiation, nine of the originally-planned 19 TCs were considered functional. Fission product release-to-birth (R/B) ratios were quite low. In most capsules, R/B values at the end of the irradiation were at or below 10-7 with only one capsule significantly exceeding this value. A maximum R/B of around 2?10-7 was reached at the end of the irradiation in Capsule 5. Several shakedown issues were encountered and resolved during the first three cycles. These include the repair of minor gas line leaks; repair of faulty gas line valves; the need to position moisture monitors in regions of low radiation fields for proper functioning; the enforcement of proper on-line data storage and backup, the need to monitor thermocouple performance, correcting for detector spectral gain shift, and a change in the mass flow rate range of the neon flow controllers.

  18. DEVELOPMENT OF CRYSTALLINE CERAMICS FOR IMMOBILIZATION OF ADVANCED FUEL CYCLE REPROCESSING WASTES

    SciTech Connect (OSTI)

    Fox, K.; Brinkman, K.

    2011-09-22

    The Savannah River National Laboratory (SRNL) is developing crystalline ceramic waste forms to incorporate CS/LN/TM high Mo waste streams consisting of perovskite, hollandite, pyrochlore, zirconolite, and powellite phase assemblages. Simple raw materials, including Al{sub 2}O{sub 3}, CaO, and TiO{sub 2} were combined with simulated waste components to produce multiphase crystalline ceramics. Fiscal Year 2011 (FY11) activities included (i) expanding the compositional range by varying waste loading and fabrication of compositions rich in TiO{sub 2}, (ii) exploring the processing parameters of ceramics produced by the melt and crystallize process, (iii) synthesis and characterization of select individual phases of powellite and hollandite that are the target hosts for radionuclides of Mo, Cs, and Rb, and (iv) evaluating the durability and radiation stability of single and multi-phase ceramic waste forms. Two fabrication methods, including melting and crystallizing, and pressing and sintering, were used with the intent of studying phase evolution under various sintering conditions. An analysis of the XRD and SEM/EDS results indicates that the targeted crystalline phases of the FY11 compositions consisting of pyrochlore, perovskite, hollandite, zirconolite, and powellite were formed by both press and sinter and melt and crystallize processing methods. An evaluation of crystalline phase formation versus melt processing conditions revealed that hollandite, perovskite, zirconolite, and residual TiO{sub 2} phases formed regardless of cooling rate, demonstrating the robust nature of this process for crystalline phase development. The multiphase ceramic composition CSLNTM-06 demonstrated good resistance to proton beam irradiation. Electron irradiation studies on the single phase CaMoO{sub 4} (a component of the multiphase waste form) suggested that this material exhibits stability to 1000 years at anticipated self-irradiation doses (2 x 10{sup 10}-2 x 10{sup 11} Gy), but that its stability may be rate dependent, therefore limiting the activity of the waste for which it can be employed. Overall, these preliminary results indicate good radiation damage tolerance for the crystalline ceramic materials. The PCT results showed that, for all of the waste forms tested, the normalized release values for most of the elements measured, including all of the lanthanides and noble metals, were either very small or below the instrument detection limits. Elevated normalized release values were measured only for Cs, Mo, and Rb. It is difficult to draw further conclusions from these data until a benchmark material is developed for the PCT with this type of waste form. Calcined, simulated CS/LN/TM High Mo waste without additives had relatively low normalized release values for Cs, Mo, and Rb. A review of the chemical composition data for this sample showed that these elements were well retained after the calcination. Therefore, it will be useful to further characterize the calcined material to determine what form these elements are in after calcining. This, along with single phase studies on Cs containing crystal structures such as hollandite, should provide insight into the most ideal phases to incorporate these elements to produce a durable waste form.

  19. AGR-1 Irradiation Test Final As-Run Report, Rev. 3

    SciTech Connect (OSTI)

    Collin, Blaise P.

    2015-01-01

    This document presents the as-run analysis of the AGR-1 irradiation experiment. AGR-1 is the first of eight planned irradiations for the Advanced Gas Reactor (AGR) Fuel Development and Qualification Program. Funding for this program is provided by the US Department of Energy (DOE) as part of the Next-Generation Nuclear Plant (NGNP) project. The objectives of the AGR-1 experiment are: 1. To gain experience with multi-capsule test train design, fabrication, and operation with the intent to reduce the probability of capsule or test train failure in subsequent irradiation tests. 2. To irradiate fuel produced in conjunction with the AGR fuel process development effort. 3. To provide data that will support the development of an understanding of the relationship between fuel fabrication processes, fuel product properties, and irradiation performance. In order to achieve the test objectives, the AGR-1 experiment was irradiated in the B-10 position of the Advanced Test Reactor (ATR) at the Idaho National Laboratory (INL) for a total duration of 620 effective full power days of irradiation. Irradiation began on December 24, 2006 and ended on November 6, 2009 spanning 13 ATR cycles and approximately three calendar years. The test contained six independently controlled and monitored capsules. Each capsule contained 12 compacts of a single type, or variant, of the AGR coated fuel. No fuel particles failed during the AGR-1 irradiation. Final burnup values on a per compact basis ranged from 11.5 to 19.6 %FIMA, while fast fluence values ranged from 2.21 to 4.39 x 1025 n/m2 (E >0.18 MeV). Well say something here about temperatures once thermal recalc is done. Thermocouples performed well, failing at a lower rate than expected. At the end of the irradiation, nine of the originally-planned 19 TCs were considered functional. Fission product release-to-birth (R/B) ratios were quite low. In most capsules, R/B values at the end of the irradiation were at or below 10-7 with only one capsule significantly exceeding this value. A maximum R/B of around 2 x 10-7 was reached at the end of the irradiation in Capsule 5. Several shakedown issues were encountered and resolved during the first three cycles. These include the repair of minor gas line leaks; repair of faulty gas line valves; the need to position moisture monitors in regions of low radiation fields for proper functioning; the enforcement of proper on-line data storage and backup, the need to monitor thermocouple performance, correcting for detector spectral gain shift, and a change in the mass flow rate range of the neon flow controllers.

  20. Phosphate glass useful in high energy lasers

    DOE Patents [OSTI]

    Hayden, Y.T.; Guesto-Barnak, D.

    1992-12-22

    Disclosed is a low-or no-silica, low- or no-alkali phosphate glass useful as a laser amplifier in a multiple pass, high energy laser system having a high thermal conductivity, K[sub 90 C] >0.85 W/mK, a low coefficient of thermal expansion, [alpha][sub 20-300 C] <80[times]10[sup [minus]7]/C, low emission cross section, [sigma]<2.5[times]10[sup [minus]20] cm[sup 2], and a high fluorescence lifetime, [tau]>325 [mu]secs at 3 wt. % Nd doping, consisting essentially of (on an oxide composition basis): (Mole %) P[sub 2]O[sub 5], (52-72); Al[sub 2]O[sub 3], (0-<20); B[sub 2]O[sub 3], (>0-25); ZnO, (0-31); Li[sub 2]O, (0-5); K[sub 2]O, (0-5); Na[sub 2]O, (0-5); Cs[sub 2]O, (0-5); Rb[sub 2]O, (0-5); MgO, (>0-<30); CaO, (0-20); BaO, (0-20); SrO, (0-<20); Sb[sub 2]O[sub 3], (0-<1); As[sub 2]O[sub 3], (0-<1); Nb[sub 2]O[sub 5], (0-<1); Ln[sub 2]O[sub 3], (up to 6.5); PbO, (0-<5); and SiO[sub 2], (0-3); wherein Ln[sub 2]O[sub 3] is the sum of lanthanide oxides; [Sigma]R[sub 2]O is <5, R being Li, Na, K, Cs, and Rb; the sum of Al[sub 2]O[sub 3] and MgO is <24 unless [Sigma]R[sub 2]O is 0, then the sum of Al[sub 2]O[sub 3] and MgO is <42; and the ratio of MgO to B[sub 2]O[sub 3] is 0.48-4.20. 7 figs.

  1. Strontium Isotopic Composition of Paleozoic Carbonate Rocks in the Nevada Test Site Vicinity, Clark, Lincoln, and Nye Counties, Nevada and Inyo County, California.

    SciTech Connect (OSTI)

    James B. Paces; Zell E. Peterman; Kiyoto Futa; Thomas A. Oliver; and Brian D. Marshall.

    2007-08-07

    Ground water moving through permeable Paleozoic carbonate rocks represents the most likely pathway for migration of radioactive contaminants from nuclear weapons testing at the Nevada Test Site, Nye County, Nevada. The strontium isotopic composition (87Sr/86Sr) of ground water offers a useful means of testing hydrochemical models of regional flow involving advection and reaction. However, reaction models require knowledge of 87Sr/86Sr data for carbonate rock in the Nevada Test Site vicinity, which is scarce. To fill this data gap, samples of core or cuttings were selected from 22 boreholes at depth intervals from which water samples had been obtained previously around the Nevada Test Site at Yucca Flat, Frenchman Flat, Rainier Mesa, and Mercury Valley. Dilute acid leachates of these samples were analyzed for a suite of major- and trace-element concentrations (MgO, CaO, SiO2, Al2O3, MnO, Rb, Sr, Th, and U) as well as for 87Sr/86Sr. Also presented are unpublished analyses of 114 Paleozoic carbonate samples from outcrops, road cuts, or underground sites in the Funeral Mountains, Bare Mountain, Striped Hills, Specter Range, Spring Mountains, and ranges east of the Nevada Test Site measured in the early 1990's. These data originally were collected to evaluate the potential for economic mineral deposition at the potential high-level radioactive waste repository site at Yucca Mountain and adjacent areas (Peterman and others, 1994). Samples were analyzed for a suite of trace elements (Rb, Sr, Zr, Ba, La, and Ce) in bulk-rock powders, and 87Sr/86Sr in partial digestions of carbonate rock using dilute acid or total digestions of silicate-rich rocks. Pre-Tertiary core samples from two boreholes in the central or western part of the Nevada Test Site also were analyzed. Data are presented in tables and summarized in graphs; however, no attempt is made to interpret results with respect to ground-water flow paths in this report. Present-day 87Sr/86Sr values are compared to values for Paleozoic seawater present at the time of deposition. Many of the samples have 87Sr/86Sr compositions that remain relatively unmodified from expected seawater values. However, rocks underlying the northern Nevada Test Site as well as rocks exposed at Bare Mountain commonly have elevated 87Sr/86Sr values derived from post-depositional addition of radiogenic Sr most likely from fluids circulating through rubidium-rich Paleozoic strata or Precambrian basement rocks.

  2. AGR-2 Data Qualification Report for ATR Cycles 151B-2, 152A, 152B, 153A, 153B and 154A

    SciTech Connect (OSTI)

    Binh T. Pham; Jeffrey J. Einerson

    2013-09-01

    This report documents the data qualification status of AGR-2 fuel irradiation experimental data from Advanced Test Reactor (ATR) Cycles 152A, 152B, 153A, 153B, and 154A, as recorded in the Nuclear Data Management and Analysis System (NDMAS). The AGR-2 data streams addressed include thermocouple (TC) temperatures, sweep gas data (flow rate, pressure, and moisture content), and fission product monitoring system (FPMS) data for each of the six capsules in the experiment. A total of 13,400,520 every minute instantaneous TC and sweep gas data records were received and processed by NDMAS for this period. Of these data, 8,911,791 records (66.5% of the total) were determined to be Qualified based on NDMAS accuracy testing and data validity assessment. For temperature, there were 4,266,081 records (74% of the total TC data) that were Failed due to TC instrument failures. For sweep gas flows, there were 222,648 gas flow records (2.91% of the flow data) that were Failed. The inlet gas flow failures due to gas flow cross-talk and leakage problems that occurred after Cycle 150A were corrected by using the same gas mixture in all six capsules and the Leadout. For FPMS data, NDMAS received and processed preliminary release rate and release-to-birth rate ratio (R/B) data for three reactor cycles (Cycles 149B, 150B, and 151A) . This data consists of 45,983 release rate records and 45,235 R/B records for the 12 radionuclides reported. The qualification status of these FPMS data has been set to In Process until receipt of Quality Assurance-approved data generator reports. All of the above data have been processed and tested using a SAS-based enterprise application software system, stored in a secure Structured Query Language database, made available on the NDMAS Web portal (http://ndmas.inl.gov), and approved by the INL STIM for release to both internal and appropriate external Very High Temperature Reactor Program participants.

  3. Semi-automated lab-on-a-chip for dispensing GA-68 radiotracers

    SciTech Connect (OSTI)

    Weinberg, Irving

    2014-03-12

    We solved a technical problem that is hindering American progress in molecular medicine, and restricting US citizens from receiving optimal diagnostic care. Specifically, the project deals with a mother/daughter generator of positron-emitting radiotracers (Ge-68/Ga-68). These generator systems are approved in Europe but cannot be used in the USA, because of safety issues related to possible breakthrough of long-lived Ge-68 (mother) atoms. Europeans have demonstrated abilities of Ga-68-labeled radiotracers to image cancer foci with high sensitivity and specificity, and to use such methods to effectively plan therapy.The USA Food and Drug Administration (FDA) and Nuclear Regulatory Commission (NRC) have taken the position that every patient administration of Ga-68 should be preceded by an assay demonstrated that Ge-68 breakthrough is within acceptable limits. Breakthrough of parent elements is a sensitive subject at the FDA, as evidenced by the recent recall of Rb-82 generators due to inadvertent administrations of Sr-82. Commercially, there is no acceptable rapid method for assaying breakthrough of Ge-68 prior to each human administration. The gamma emissions of daughter Ga-68 have higher energies than the parent Ge-68, so that the shielding assays typically employed for Mo-99/Tc-99m generators cannot be applied to Ga-68 generators. The half-life of Ga-68 is 68 minutes, so that the standard 10-half-life delay (used to assess breakthrough in Sr-82/Rb-82 generators) cannot be applied to Ga-68 generators. As a result of the aforementioned regulatory requirements, Ga-68 generators are sold in the USA for animal use only.The American clinical communitys inability to utilize Ga-68 generators impairs abilities to treat patients domestically, and puts the USA at a disadvantage in developing exportable products. The proposed DOE project aimed to take advantage of recent technological advances developed for lab-on-a-chip (LOC) applications. Based on our experiences constructing such devices, the proposed microfluidics-based approach could provide cost-effective validation of breakthrough compliance in minutes.

  4. Prenatal cadmium exposure produces persistent changes to thymus and spleen cell phenotypic repertoire as well as the acquired immune response

    SciTech Connect (OSTI)

    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 females had changed percentages of numerous splenic cell populations. ? The antibody response of a streptococcal vaccine showed numerous changes.

  5. Quality Quantification of Evaluated Cross Section Covariances

    SciTech Connect (OSTI)

    Varet, S.; Dossantos-Uzarralde, P.

    2015-01-15

    Presently, several methods are used to estimate the covariance matrix of evaluated nuclear cross sections. Because the resulting covariance matrices can be different according to the method used and according to the assumptions of the method, we propose a general and objective approach to quantify the quality of the covariance estimation for evaluated cross sections. The first step consists in defining an objective criterion. The second step is computation of the criterion. In this paper the Kullback-Leibler distance is proposed for the quality quantification of a covariance matrix estimation and its inverse. It is based on the distance to the true covariance matrix. A method based on the bootstrap is presented for the estimation of this criterion, which can be applied with most methods for covariance matrix estimation and without the knowledge of the true covariance matrix. The full approach is illustrated on the {sup 85}Rb nucleus evaluations and the results are then used for a discussion on scoring and Monte Carlo approaches for covariance matrix estimation of the cross section evaluations.

  6. Determination of the direct double- β -decay Q value of Zr 96 and atomic masses of Zr 90 - 92 , 94 , 96 and Mo 92 , 94 - 98 , 100

    SciTech Connect (OSTI)

    Gulyuz, K.; Ariche, J.; Bollen, G.; Bustabad, S.; Eibach, M.; Izzo, C.; Novario, S. J.; Redshaw, M.; Ringle, R.; Sandler, R.; Schwarz, S.; Valverde, A. A.

    2015-05-06

    Experimental searches for neutrinoless double-β decay offer one of the best opportunities to look for physics beyond the standard model. Detecting this decay would confirm the Majorana nature of the neutrino, and a measurement of its half-life can be used to determine the absolute neutrino mass scale. Important to both tasks is an accurate knowledge of the Q value of the double-β decay. The LEBIT Penning trap mass spectrometer was used for the first direct experimental determination of the ⁹⁶Zr double-β decay Q value: Qββ=3355.85(15) keV. This value is nearly 7 keV larger than the 2012 Atomic Mass Evaluation [M. Wang et al., Chin. Phys. C 36, 1603 (2012)] value and one order of magnitude more precise. The 3-σ shift is primarily due to a more accurate measurement of the ⁹⁶Zr atomic mass: m(⁹⁶Zr)=95.90827735(17) u. Using the new Q value, the 2νββ-decay matrix element, |M|, is calculated. Improved determinations of the atomic masses of all other zirconium (90-92,94,96Zr) and molybdenum (92,94-98,100Mo) isotopes using both ¹²C₈ and ⁸⁷Rb as references are also reported.

  7. Determination of the direct double- β -decay Q value of Zr 96 and atomic masses of Zr 90 - 92 , 94 , 96 and Mo 92 , 94 - 98 , 100

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Gulyuz, K.; Ariche, J.; Bollen, G.; Bustabad, S.; Eibach, M.; Izzo, C.; Novario, S. J.; Redshaw, M.; Ringle, R.; Sandler, R.; et al

    2015-05-06

    Experimental searches for neutrinoless double-β decay offer one of the best opportunities to look for physics beyond the standard model. Detecting this decay would confirm the Majorana nature of the neutrino, and a measurement of its half-life can be used to determine the absolute neutrino mass scale. Important to both tasks is an accurate knowledge of the Q value of the double-β decay. The LEBIT Penning trap mass spectrometer was used for the first direct experimental determination of the ⁹⁶Zr double-β decay Q value: Qββ=3355.85(15) keV. This value is nearly 7 keV larger than the 2012 Atomic Mass Evaluation [M.more » Wang et al., Chin. Phys. C 36, 1603 (2012)] value and one order of magnitude more precise. The 3-σ shift is primarily due to a more accurate measurement of the ⁹⁶Zr atomic mass: m(⁹⁶Zr)=95.90827735(17) u. Using the new Q value, the 2νββ-decay matrix element, |M2ν|, is calculated. Improved determinations of the atomic masses of all other zirconium (90-92,94,96Zr) and molybdenum (92,94-98,100Mo) isotopes using both ¹²C₈ and ⁸⁷Rb as references are also reported.« less

  8. Baseline Glass Development for Combined Fission Products Waste Streams

    SciTech Connect (OSTI)

    Crum, Jarrod V.; Billings, Amanda Y.; Lang, Jesse B.; Marra, James C.; Rodriguez, Carmen P.; Ryan, Joseph V.; Vienna, John D.

    2009-06-29

    Borosilicate glass was selected as the baseline technology for immobilization of the Cs/Sr/Ba/Rb (Cs), lanthanide (Ln) and transition metal fission product (TM) waste steams as part of a cost benefit analysis study.[1] Vitrification of the combined waste streams have several advantages, minimization of the number of waste forms, a proven technology, and similarity to waste forms currently accepted for repository disposal. A joint study was undertaken by Pacific Northwest National Laboratory (PNNL) and Savannah River National Laboratory (SRNL) to develop acceptable glasses for the combined Cs + Ln + TM waste streams (Option 1) and Cs + Ln combined waste streams (Option 2) generated by the AFCI UREX+ set of processes. This study is aimed to develop baseline glasses for both combined waste stream options and identify key waste components and their impact on waste loading. The elemental compositions of the four-corners study were used along with the available separations data to determine the effect of burnup, decay, and separations variability on estimated waste stream compositions.[2-5] Two different components/scenarios were identified that could limit waste loading of the combined Cs + LN + TM waste streams, where as the combined Cs + LN waste stream has no single component that is perceived to limit waste loading. Combined Cs + LN waste stream in a glass waste form will most likely be limited by heat due to the high activity of Cs and Sr isotopes.

  9. Thermoelectric materials ternary penta telluride and selenide compounds

    DOE Patents [OSTI]

    Sharp, Jeffrey W.

    2001-01-01

    Ternary tellurium compounds and ternary selenium compounds may be used in fabricating thermoelectric devices with a thermoelectric figure of merit (ZT) of 1.5 or greater. Examples of such compounds include Tl.sub.2 SnTe.sub.5, Tl.sub.2 GeTe.sub.5, K.sub.2 SnTe.sub.5 and Rb.sub.2 SnTe.sub.5. These compounds have similar types of crystal lattice structures which include a first substructure with a (Sn, Ge) Te.sub.5 composition and a second substructure with chains of selected cation atoms. The second substructure includes selected cation atoms which interact with selected anion atoms to maintain a desired separation between the chains of the first substructure. The cation atoms which maintain the desired separation between the chains occupy relatively large electropositive sites in the resulting crystal lattice structure which results in a relatively low value for the lattice component of thermal conductivity (.kappa..sub.g). The first substructure of anion chains indicates significant anisotropy in the thermoelectric characteristics of the resulting semiconductor materials.

  10. Thermoelectric materials: ternary penta telluride and selenide compounds

    DOE Patents [OSTI]

    Sharp, Jeffrey W.

    2002-06-04

    Ternary tellurium compounds and ternary selenium compounds may be used in fabricating thermoelectric devices with a thermoelectric figure of merit (ZT) of 1.5 or greater. Examples of such compounds include Tl.sub.2 SnTe.sub.5, Tl.sub.2 GeTe.sub.5, K.sub.2 SnTe.sub.5 and Rb.sub.2 SnTe.sub.5. These compounds have similar types of crystal lattice structures which include a first substructure with a (Sn, Ge) Te.sub.5 composition and a second substructure with chains of selected cation atoms. The second substructure includes selected cation atoms which interact with selected anion atoms to maintain a desired separation between the chains of the first substructure. The cation atoms which maintain the desired separation between the chains occupy relatively large electropositive sites in the resulting crystal lattice structure which results in a relatively low value for the lattice component of thermal conductivity (.kappa..sub.g). The first substructure of anion chains indicates significant anisotropy in the thermoelectric characteristics of the resulting semiconductor materials.

  11. Cross-correlation spin noise spectroscopy of heterogeneous interacting spin systems

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Roy, Dibyendu; Yang, Luyi; Crooker, Scott A.; Sinitsyn, Nikolai A.

    2015-04-30

    Interacting multi-component spin systems are ubiquitous in nature and in the laboratory. As such, investigations of inter-species spin interactions are of vital importance. Traditionally, they are studied by experimental methods that are necessarily perturbative: e.g., by intentionally polarizing or depolarizing one spin species while detecting the response of the other(s). Here, we describe and demonstrate an alternative approach based on multi-probe spin noise spectroscopy, which can reveal inter-species spin interactions - under conditions of strict thermal equilibrium - by detecting and cross-correlating the stochastic fluctuation signals exhibited by each of the constituent spin species. Specifically, we consider a two-component spinmore » ensemble that interacts via exchange coupling, and we determine cross-correlations between their intrinsic spin fluctuations. The model is experimentally confirmed using “two-color” optical spin noise spectroscopy on a mixture of interacting Rb and Cs vapors. Noise correlations directly reveal the presence of inter-species spin exchange, without ever perturbing the system away from thermal equilibrium. These non-invasive and noise-based techniques should be generally applicable to any heterogeneous spin system in which the fluctuations of the constituent components are detectable.« less

  12. The structural diversity of ABS{sub 3} compounds with d{sup 0} electronic configuration for the B-cation

    SciTech Connect (OSTI)

    Brehm, John A. Bennett, Joseph W.; Schoenberg, Michael Rutenberg; Grinberg, Ilya; Rappe, Andrew M.

    2014-06-14

    We use first-principles density functional theory within the local density approximation to ascertain the ground state structure of real and theoretical compounds with the formula ABS{sub 3} (A = K, Rb, Cs, Ca, Sr, Ba, Tl, Sn, Pb, and Bi; and B = Sc, Y, Ti, Zr, V, and Nb) under the constraint that B must have a d{sup 0} electronic configuration. Our findings indicate that none of these AB combinations prefer a perovskite ground state with corner-sharing BS{sub 6} octahedra, but that they prefer phases with either edge- or face-sharing motifs. Further, a simple two-dimensional structure field map created from A and B ionic radii provides a neat demarcation between combinations preferring face-sharing versus edge-sharing phases for most of these combinations. We then show that by modifying the common Goldschmidt tolerance factor with a multiplicative term based on the electronegativity difference between A and S, the demarcation between predicted edge-sharing and face-sharing ground state phases is enhanced. We also demonstrate that, by calculating the free energy contribution of phonons, some of these compounds may assume multiple phases as synthesis temperatures are altered, or as ambient temperatures rise or fall.

  13. CHARACTERIZATION OF SALT PARTICLE INDUCED CORROSION PROCESSES BY SYNCHROTRON GENERATED X-RAY FLUORESCENCE AND COMPLEMENTARY SURFACE ANALYSIS TOOLS.

    SciTech Connect (OSTI)

    NEUFELD, A.K.; COLE, I.S.; BOND, A.M.; ISAACS, H.S.; FURMAN, S.A.

    2001-03-25

    The benefits of using synchrotron-generated X-rays and X-ray fluorescence analysis in combination with other surface analysis techniques have been demonstrated. In studies of salt-induced corrosion, for example, the detection of Rb ions in the area of secondary spreading when salt-containing micro-droplets are placed on zinc surfaces, further supports a mechanism involving cation transport during the corrosion and spreading of corrosive salt on exposed metal surfaces. Specifically, the new analytical data shows that: (a) cations are transported radially from a primary drop formed from a salt deposit in a thin film of secondary spreading around the drop; (b) subsequently, micro-pools are formed in the area of secondary spreading, and it is likely that cations transported within the thin film accumulate in these micro-pools until the area is dehydrated; (c) the mechanism of cation transport into the area of secondary spreading does not include transport of the anions; and (d) hydroxide is the counter ion formed from oxygen reduction at the metal surface within the spreading layer. Data relevant to iron corrosion is also presented and the distinct differences relative to the zinc situation are discussed.

  14. Trapping ultracold gases near cryogenic materials with rapid reconfigurability

    SciTech Connect (OSTI)

    Naides, Matthew A.; Turner, Richard W.; Lai, Ruby A.; DiSciacca, Jack M.; Lev, Benjamin L.

    2013-12-16

    We demonstrate an atom chip trapping system that allows the placement and high-resolution imaging of ultracold atoms within microns from any ?100??m-thin, UHV-compatible material, while also allowing sample exchange with minimal experimental downtime. The sample is not connected to the atom chip, allowing rapid exchange without perturbing the atom chip or laser cooling apparatus. Exchange of the sample and retrapping of atoms has been performed within a week turnaround, limited only by chamber baking. Moreover, the decoupling of sample and atom chip provides the ability to independently tune the sample temperature and its position with respect to the trapped ultracold gas, which itself may remain in the focus of a high-resolution imaging system. As a first demonstration of this system, we have confined a 700-nK cloud of 8??10{sup 4} {sup 87}Rb atoms within 100??m of a gold-mirrored 100-?m-thick silicon substrate. The substrate was cooled to 35?K without use of a heat shield, while the atom chip, 120??m away, remained at room temperature. Atoms may be imaged and retrapped every 16?s, allowing rapid data collection.

  15. First measurement of Φ₃ with a model-independent Dalitz plot analysis of B±→DK±, D→KS⁰π⁺π⁻ decay

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Aihara, H.; Arinstein, K.; Asner, D. M.; Aulchenko, V.; Aushev, T.; Bakich, A. M.; Belous, K.; Bhuyan, B.; Bischofberger, M.; Bondar, A.; et al

    2012-06-26

    We present the first measurement of the angle Φ₃ of the unitarity triangle using a model-independent Dalitz plot analysis of B±→DK±, D→KS⁰π⁺π⁻ decays. The method uses, as input, measurements of the strong phase of the D→K⁰Sπ⁺π⁻ amplitude from the CLEO Collaboration. The result is based on the full data set of 772×106 BB¯¯¯ pairs collected by the Belle experiment at the Υ(4S) resonance. We obtain Φ₃=(77.3+15.1–14.9±4.1±4.3)° and the suppressed amplitude ratio rB=0.145±0.030±0.010±0.011. Here the first error is statistical, the second is the experimental systematic uncertainty, and the third is the error due to the precision of the strong-phase parameters obtainedmore » by CLEO.« less

  16. Performance of Low Smeared Density Sodium-cooled Fast Reactor Metal Fuel

    SciTech Connect (OSTI)

    D. L. Porter; H. J. M. Chichester; P. G. Medvedev; S. L. Hayes; M. C. Teague

    2015-10-01

    An experiment was performed in the Experimental Breeder Rector-II (EBR-II) in the 1990s to show that metallic fast reactor fuel could be used in reactors with a single, once-through core. To prove the long duration, high burnup, high neutron exposure capability an experiment where the fuel pin was designed with a very large fission gas plenum and very low fuel smeared density (SD). The experiment, X496, operated to only 8.3 at. % burnup because the EBR-II reactor was scheduled for shut-down at that time. Many of the examinations of the fuel pins only funded recently with the resurgence of reactor designs using very high-burnup fuel. The results showed that, despite the low smeared density of 59% the fuel swelled radially to contact the cladding, fission gas release appeared to be slightly higher than demonstrated in conventional 75%SD fuel tests and axial growth was about the same as 75% SD fuel. There were axial positions in some of the fuel pins which showed evidence of fuel restructuring and an absence of fission products with low metaling points and gaseous precursors (Cs and Rb). A model to investigate whether these areas may have overheated due to a loss of bond sodium indicates that it is a possible explanation for the fuel restructuring and something to be considered for fuel performance modeling of low SD fuel.

  17. THE INFLUENCE OF INTERMITTENCY ON THE SPECTRAL ANISOTROPY OF SOLAR WIND TURBULENCE

    SciTech Connect (OSTI)

    Wang, Xin; Tu, Chuanyi; He, Jiansen; Wang, Linghua; Marsch, Eckart

    2014-03-01

    The relation between the intermittency and the anisotropy of the power spectrum in the solar wind turbulence is studied by applying the wavelet technique to the magnetic field and flow velocity data measured by the WIND spacecraft. It is found that when the intermittency is removed from the turbulence, the spectral indices of the power spectra of the field and velocity turn out to be independent of the angle ?{sub RB} between the direction of the local scale-dependent background magnetic field and the heliocentric direction. The spectral index becomes 1.63 0.02 for magnetic field fluctuations and 1.56 0.02 for velocity fluctuations. These results may suggest that the recently found spectral anisotropy of solar wind power spectra in the inertial range could result from turbulence intermittency. As a consequence, a new concept is here proposed of an intermittency-associated sub-range of the inertial domain adjacent to the dissipation range. Since spectral anisotropy was previously explained as evidence for the presence of a ''critical balance'' type turbulent cascade, and also for the existence of kinetic Alfvn waves, this new finding may stimulate fresh thoughts on how to analyze and interpret solar wind turbulence and the associated heating.

  18. Color stable manganese-doped phosphors

    DOE Patents [OSTI]

    Lyons, Robert Joseph; Setlur, Anant Achyut; Deshpande, Anirundha Rajendra; Grigorov, Ljudmil Slavchev

    2014-04-29

    A lighting apparatus capable of emitting white light includes a semiconductor light source; and a phosphor material radiationally coupled to the light source. The phosphor material includes a color-stable Mn.sup.+4 doped phosphor prepared by a process including providing a phosphor of formula I; A.sub.x[MF.sub.y]:Mn.sup.+4 I and contacting the phosphor in particulate form with a saturated solution of a composition of formula II in aqueous hydrofluoric acid; A.sub.x[MF.sub.y]; II wherein A is Li, Na, K, Rb, Cs, NR.sub.4 or a combination thereof; M is Si, Ge, Sn, Ti, Zr, Al, Ga, In, Sc, Y, La, Nb, Ta, Bi, Gd, or a combination thereof; R is H, lower alkyl, or a combination thereof; x is the absolute value of the charge of the [MF.sub.y] ion; and y is 5, 6 or 7. In particular embodiments, M is Si, Ge, Sn, Ti, Zr, or a combination thereof.

  19. Color stable manganese-doped phosphors

    DOE Patents [OSTI]

    Lyons, Robert Joseph; Setlur, Anant Achyut; Deshpande, Anirudha Rajendra; Grigorov, Ljudmil Slavchev

    2012-08-28

    A process for preparing color stable Mn.sup.+4 doped phosphors includes providing a phosphor of formula I; A.sub.x[MF.sub.y]:Mn.sup.+4 I and contacting the phosphor in particulate form with a saturated solution of a composition of formula II in aqueous hydrofluoric acid; A.sub.x[MF.sub.y]; II wherein A is Li, Na, K, Rb, Cs, NR.sub.4 or a combination thereof; M is Si, Ge, Sn, Ti, Zr, Al, Ga, In, Sc, Y, La, Nb, Ta, Bi, Gd, or a combination thereof; R is H, lower alkyl, or a combination thereof; x is the absolute value of the charge of the [MF.sub.y] ion; and y is 5, 6 or 7. In particular embodiments, M is Si, Ge, Sn, Ti, Zr, or a combination thereof. A lighting apparatus capable of emitting white light includes a semiconductor light source; and a phosphor composition radiationally coupled to the light source, and which includes a color stable Mn.sup.+4 doped phosphor.

  20. Blue-green and green phosphors for lighting applications

    DOE Patents [OSTI]

    Setlur, Anant Achyut; Chandran, Ramachandran Gopi; Henderson, Claire Susan; Nammalwar, Pransanth Kumar; Radkov, Emil

    2012-12-11

    Embodiments of the present techniques provide a related family of phosphors that may be used in lighting systems to generate blue or blue-green light. The phosphors include systems having a general formula of: ((Sr.sub.1-zM.sub.z).sub.1-(x+w)A.sub.wCe.sub.x).sub.3(Al.sub.1-ySi.s- ub.y)O.sub.4+y+3(x-w)F.sub.1-y-3(x-w) (I), wherein 0Rb, or Ag or any combinations thereof, and M is Ca, Ba, Mg, Zn, or Sn or any combinations thereof. Advantageously, phosphors made accordingly to these formulations maintain emission intensity across a wide range of temperatures. The phosphors may be used in lighting systems, such as LEDs and fluorescent tubes, among others, to produce blue and blue/green light. Further, the phosphors may be used in blends with other phosphors, or in combined lighting systems, to produce white light suitable for illumination.

  1. Toward tailorable surfaces: A combined theoretical and experimental study of lanthanum niobate layered perovskites

    SciTech Connect (OSTI)

    Di Tommaso, Stefania E-mail: frederic.labat@chimie-paristech.fr; Giannici, Francesco; Mossuto Marculescu, Adriana; Martorana, Antonino; Adamo, Carlo; Labat, Frdric E-mail: frederic.labat@chimie-paristech.fr

    2014-07-14

    A comprehensive theoretical investigation of the MLaNb{sub 2}O{sub 7} (M = H, Li, Na, K, Rb, and Cs) series of ion-exchangeable layered perovskite is presented. These perovskites are in particular interesting in view of their potential applications as inorganic supports for the design of new hybrid inorganic-organic proton conductors. In particular, their structural and electronic properties have been investigated by periodic calculations in the framework of Density Functional Theory, using different exchange-correlation functionals. A general very good agreement with the available experimental (XRD, NPD, and EXAFS) data has been found. The structure of the protonated HLaNb{sub 2}O{sub 7} form has also been further clarified and a new tetragonal space group is proposed for this compound, better reproducing the experimental cell parameters and yielding to a more realistic picture of the system. The electronic investigation highlighted that all the compounds considered are very similar to each other and that the interaction between interlayer cations and perovskite slabs is purely ionic, except for the proton that is, instead, covalently bound.

  2. Phosphate glass useful in high energy lasers

    DOE Patents [OSTI]

    Hayden, Yuiko T. (Clarks Summit, PA); Guesto-Barnak, Donna (Dupont, PA)

    1992-01-01

    A low-or no-silica, low- or no-alkali phosphate glass useful as a laser amplifier in a multiple pass, high energy laser system having a high thermal conductivity, K.sub.90.degree. C. >0.85 W/mK, a low coefficient of thermal expansion, .alpha..sub.20.degree.-300.degree. C. <80.times.10.sup.-7 /.degree.C., low emission cross section, .sigma.<2.5.times.10.sup.-20 cm.sup.2, and a high fluorescence lifetime, .tau.>325 .mu.secs at 3 wt. % Nd doping, consisting essentially of (on an oxide composition basis): wherein Ln.sub.2 O.sub.3 is the sum of lanthanide oxides; .SIGMA.R.sub.2 O is <5, R being Li, Na, K, Cs, and Rb; the sum of Al.sub.2 O.sub.3 and MgO is <24 unless .SIGMA.R.sub.2 O is 0, then the sum of Al.sub.2 O.sub.3 and MgO is <42; and the ratio of MgO to B.sub.2 O.sub.3 is 0.48-4.20.

  3. Color stable phosphors for LED lamps and methods for preparing them

    SciTech Connect (OSTI)

    Murphy, James Edward; Setlur, Anant Achyut; Camardello, Samuel Joseph

    2013-11-26

    An LED lamp includes a light source configured to emit radiation with a peak intensity at a wavelength between about 250 nm and about 550 nm; and a phosphor composition configured to be radiationally coupled to the light source. The phosphor composition includes particles of a phosphor of formula I, said particles having a coating composition disposed on surfaces thereof; ((Sr.sub.1-zM.sub.z).sub.1-(x+w)A.sub.wCe.sub.x).sub.3(Al.sub.1-ySi.sub.y-)O.sub.4+y+3(x-w)F.sub.1-y-3(x-w) I wherein the coating composition comprises a material selected from aluminum oxide, magnesium oxide, calcium oxide, barium oxide, strontium oxide, zinc oxide, aluminum hydroxide, magnesium hydroxide, calcium hydroxide, barium hydroxide, strontium hydroxide, zinc hydroxide, aluminum phosphate, magnesium phosphate, calcium phosphate, barium phosphate, strontium phosphate, and combinations thereof; and A is Li, NA, K, or Rb, or a combination thereof; M is Ca, Ba, Mg, Zn, or a combination thereof; and 0

  4. Radiant barrier testing to assess effects of dust accumulation, attic ventilation, and other key variables

    SciTech Connect (OSTI)

    Hall, J.A.

    1988-07-01

    This report summarized the work accomplished during the fifth season of testing at TVA's EUTF. Previously, tests were conducted at the EUTF during the 1985/1986 summer and winter and the 1986/1987 summer and winter. This previous work at TVA, and work at the University of Mississippi, the FSEC, Texas A and M, and ORNL, have shown that in the summer: all RB installation locations provide large reductions in ceiling heat flux when used with R11 and R19 fiberglass, cellulose, or rock wool; reductions in ceiling heat flux from RBs when used with R30 are not nearly as large as from RBs when used with R19; the RBR and RBT provide sizable reductions in whole-house cooling loads; and the RBT provides the largest reduction in ceiling heat flux in most cases. Previous work has shown that in the winter: the RBT provides moderate ceiling heat flux reductions and whole-house heating load saving with R11 and R19 fiberglass, cellulose, or rock wool; the RBR shows very little reduction in ceiling heat flux in most cases; and reductions in ceiling heat flux with R30 are usually much less than with R11 or R19 insulation. 12 refs., 14 figs., 11 tabs.

  5. Data summary report for fission product release test HI-1. [PWR; BWR

    SciTech Connect (OSTI)

    Osborne, M.F.; lorenz, R.A.; Travis, J.R.; Webster, C.S.

    1982-12-01

    This first in a series of high-temperature fission product release tests was conducted for 30 min at 1400/sup 0/C, with the release taking place into flowing steam. The fuel specimen was a 20-cm-long section of H.B. Robinson fuel rod, irradiated to 28,000 MWd per metric ton (t). After the test, the Zircaloy cladding of the specimen was almost completely oxidized and was quite fragile. The fission product collection system included a thermal gradient tube (700-150/sup 0/C), filters, heated charcoal, and cooled charcoal. Gamma ray analysis of apparatus components and collectors showed that about 2.83% of the /sup 85/Kr and 1.75% of the /sup 137/Cs were released from the fuel. Activation analysis of leach solutions from these components indicated that 2.04% of the /sup 129/I was released. Other analyses revealed small but significant releases of the radionuclides /sup 125/Sb and /sup 106/Ru, and of the elements Br, Rb, Sr, Zr, Ag, Sn, Te, Ba, and La.

  6. The Bholghati (howardite) consortium: An overview

    SciTech Connect (OSTI)

    Laul, J.C. )

    1990-08-01

    The Bholghati (howardite) has had a complex history. The consortium studies indicate that eucrite clasts show evidence of rapid crystallization followed by prolonged subsolidus annealing. Dark clasts are carbonaceous CM2 type. Bholghati bulk composition can be modeled by 55% eucritic, 45% diogenitic, and 3% dark clast components. The eucritic clasts show a LREE depleted pattern relative to HREEs, which is not typical of a normal eucrite. The LREE depletion requires two-stage melting from a chondritic source. The volatile/mobile trace element patterns in dark and eucritic clasts are highly variable, probably due to volatile redistribution. The eucritic clast shows excess fission Xe, which is attributed to in situ decay of Pu-244. The cosmic-ray exposure age is 10-17 Ma. The Rb-Sr, Sm-Nd, and K-Ar ages of Bholghati bulk and eucritic clasts indicate 4.53 Ga as crystallization age, 2-3 Ga as metamorphic event, and probably a minor thermal event < 1 Ga. The Bholghati evolution scenario is (1) early multiple magmatic events (4.53 Ga ago), producing eucrites and diogenites; (2) a metamorphic event (2-3 Ga ago) and prolonged subsolidus annealing; (3) Fragmentation and low-temperature mixing of eucrites and diogenites; (4) low-velocity impact (<1 Ga. ago) and admixing of carbonaceous material; (5) disruption of regolith and ejection of Bholghati 10-17 Ma ago; and (6) Bholghati fell on the Earth in 1905.

  7. Degradation characteristic of monoazo, diazo and anthraquinone dye by UV/H{sub 2}O{sub 2} process

    SciTech Connect (OSTI)

    Abidin, Che Zulzikrami Azner E-mail: drfahmi@unimap.edu.my E-mail: fatinnadhirah89@gmail.com; Fahmi, Muhammad Ridwan E-mail: drfahmi@unimap.edu.my E-mail: fatinnadhirah89@gmail.com; Fazara, Md Ali Umi E-mail: drfahmi@unimap.edu.my E-mail: fatinnadhirah89@gmail.com; Nadhirah, Siti Nurfatin E-mail: drfahmi@unimap.edu.my E-mail: fatinnadhirah89@gmail.com

    2014-10-24

    In this study, the degradation characteristic of monoazo, diazo and anthraquinone dye by UV/H{sub 2}O{sub 2} process was evaluated based on the trend of color, chemical oxygen demand (COD) and total organic carbon (TOC) removal. Three types of dyes consist of monoazo, diazo and anthraquinone dyes were used to compare the degradation mechanism of the dyes. The UV/H{sub 2}O{sub 2} experiments were conducted in a laboratory scale cylindrical glass reactor operated in semi-batch mode. The UV/Vis characterization of monoazo, diazo and anthraquinone dye indicated that the rapid degradation of the dyes by UV/H{sub 2}O{sub 2} process is meaningful with respect to decolourization, as a result of the azo bonds and substitute antraquinone chromophore degradation. However, this process is not efficient for aromatic amines removal. The monoazo MO was difficult to be decolorized than diazo RR120 dye, which imply that number of sulphonic groups in the dye molecules determines the reactivity with hydroxyl radical. The increased in COD removal is the evidence for oxidation and decreased in carbon content of dye molecules. TOC removal analysis shows that low TOC removal of monoazo MO and diazo RR120, as compared to anthraquinone RB19 may indicate an accumulation of by-products that are resistant to the H{sub 2}O{sub 2} photolysis.

  8. Chloride, bromide and iodide scintillators with europium doping

    DOE Patents [OSTI]

    Zhuravleva, Mariya; Yang, Kan

    2014-08-26

    A halide scintillator material is disclosed where the halide may comprise chloride, bromide or iodide. The material is single-crystalline and has a composition of the general formula ABX.sub.3 where A is an alkali, B is an alkali earth and X is a halide which general composition was investigated. In particular, crystals of the formula ACa.sub.1-yEu.sub.yI.sub.3 where A=K, Rb and Cs were formed as well as crystals of the formula CsA.sub.1-yEu.sub.yX.sub.3 (where A=Ca, Sr, Ba, or a combination thereof and X=Cl, Br or I or a combination thereof) with divalent Europium doping where 0.ltoreq.y.ltoreq.1, and more particularly Eu doping has been studied at one to ten mol %. The disclosed scintillator materials are suitable for making scintillation detectors used in applications such as medical imaging and homeland security.

  9. Quasichemical analysis of the cluster-pair approximation for the thermodynamics of proton hydration

    SciTech Connect (OSTI)

    Pollard, Travis; Beck, Thomas L.

    2014-06-14

    A theoretical analysis of the cluster-pair approximation (CPA) is presented based on the quasichemical theory of solutions. The sought single-ion hydration free energy of the proton includes an interfacial potential contribution by definition. It is shown, however, that the CPA involves an extra-thermodynamic assumption that does not guarantee uniform convergence to a bulk free energy value with increasing cluster size. A numerical test of the CPA is performed using the classical polarizable AMOEBA force field and supporting quantum chemical calculations. The enthalpy and free energy differences are computed for the kosmotropic Na{sup +}/F{sup −} ion pair in water clusters of size n = 5, 25, 105. Additional calculations are performed for the chaotropic Rb{sup +}/I{sup −} ion pair. A small shift in the proton hydration free energy and a larger shift in the hydration enthalpy, relative to the CPA values, are predicted based on the n = 105 simulations. The shifts arise from a combination of sequential hydration and interfacial potential effects. The AMOEBA and quantum chemical results suggest an electrochemical surface potential of water in the range −0.4 to −0.5 V. The physical content of single-ion free energies and implications for ion-water force field development are also discussed.

  10. Method for ultra-trace cesium isotope ratio measurements from environmental samples using thermal ionization mass spectrometry

    SciTech Connect (OSTI)

    Snow, Mathew S.; Snyder, Darin C.; Mann, Nick R.; White, Byron M.

    2015-05-01

    135Cs/137Cs isotope ratios can provide the age, origin and history of environmental Cs contamination. Relatively high precision 135Cs/137Cs isotope ratio measurements from samples containing femtogram quantities of 137Cs are needed to accurately track contamination resuspension and redistribution following environmental 137Cs releases; however, mass spectrometric analyses of environmental samples are limited by the large quantities of ionization inhibitors and isobaric interferences which are present at relatively high concentrations in the environment. We report a new approach for Cs purification from environmental samples. An initial ammonium molybdophosphate-polyacrylonitrile (AMP-PAN) column provides a robust method for extracting Cs under a wide variety of sample matrices and mass loads. Cation exchange separations using a second AMP-PAN column result in more than two orders of magnitude greater Cs/Rb separation factors than commercially available strong cation exchangers. Coupling an AMP-PAN cation exchanging step to a microcation column (AG50W resin) enables consistent 2-4% (2?) measurement errors for samples containing 3-6,000 fg 137Cs, representing the highest precision 135Cs/137Cs ratio measurements currently reported for soil samples at the femtogram level.

  11. Equilibrium pressure measurements in the beta region of palladium protide and palladium deuteride

    SciTech Connect (OSTI)

    Carstens, D.H.W.; David, W.R.

    1989-03-01

    We have measured the pressure-composition isotherms of the palladium-deuterium and palladium-protium systems in the beta region of both and the plateau region of the protide. For these two systems, data were measured at pressures up to about 3.5 MPa (500 psi) and at temperatures from 173 to 473 K. This study extends to a greater pressure and temperature regime the work on palladium hydrides reported previously by other authors. We also report results of an empirical analytical fit to the data for these two isotope systems. For completeness, we have applied our analysis to previously reported data for the tritide. The data were fit to an equation of the form P = exp/A + 2ln(R/(1 - R))-(B - CR)/T/ + exp(D + E/T), where R is the hydrogen-to-metal atomic ratio, P is the pressure, and T is the temperature. A, B, C, D, and E are empirically determined parameters and differ for absorbing and desorbing systems of each isotope. This equation gives a good fit to the data in the beta region of the absorption curves but a poorer fit in the alpha plus beta (plateau) region. 15 refs., 6 figs.

  12. Alleghanian development of the Goat Rock fault zone, southernmost Appalachians: Temporal compatibility with the master decollement

    SciTech Connect (OSTI)

    Steltenpohl, M.G. (Auburn Univ., AL (United States)); Goldberg, S.A. (Univ. of North Carolina, Chapel Hill (United States)); Hanley, T.B. (Columbus College, GA (United States)); Kunk, M.J. (Geological Survey, Reston, VA (United States))

    1992-09-01

    The Goat Rock and associated Bartletts Ferry fault zones, which mark the eastern margin of the Pine Mountain Grenville basement massif, are controversial due to the suggestion that they are rare exposed segments of the late Paleozoic southern Appalachian master decollement. The controversy in part stems from reported middle Paleozoic (Acadian) radiometric dates postulated as the time of movement along these fault zones. Ultramylonite samples from the type area at Goat Rock Dam yield a 287 [plus minus] 15 Ma Rb-Sr isochron interpreted as the time of Sr isotopic rehomgenization during mylonitization. This date is corroborated by Late Pennsylvanian-Early Permian [sup 40]Ar/[sup 39]Ar mineral ages on hornblende (297-288 Ma) and muscovite (285-278 Ma) from neomineralized and dynamically recrystallized rocks within and straddling the fault zone. These Late Pennsylvanian-Early Permian dates indicate the time of right-slip movement (Alleghenian) along the Goat Rock fault zone, which is compatible with the timing suggested by COCORP for thrusting along the southern Appalachian master decollement.

  13. Tensor to scalar ratio and large scale power suppression from pre-slow roll initial conditions

    SciTech Connect (OSTI)

    Lello, Louis; Boyanovsky, Daniel, E-mail: lal81@pitt.edu, E-mail: boyan@pitt.edu [Department of Physics and Astronomy, University of Pittsburgh, 3941 O'Hara St, Pittsburgh, PA 15260 (United States)

    2014-05-01

    We study the corrections to the power spectra of curvature and tensor perturbations and the tensor-to-scalar ratio r in single field slow roll inflation with standard kinetic term due to initial conditions imprinted by a ''fast-roll'' stage prior to slow roll. For a wide range of initial inflaton kinetic energy, this stage lasts only a few e-folds and merges smoothly with slow-roll thereby leading to non-Bunch-Davies initial conditions for modes that exit the Hubble radius during slow roll. We describe a program that yields the dynamics in the fast-roll stage while matching to the slow roll stage in a manner that is independent of the inflationary potentials. Corrections to the power spectra are encoded in a ''transfer function'' for initial conditions T{sub ?}(k), P{sub ?}(k) = P{sup BD}{sub ?}(k)T{sub ?}(k), implying a modification of the ''consistency condition'' for the tensor to scalar ratio at a pivot scale k{sub 0}: r(k{sub 0}) = ?8n{sub T}(k{sub 0})[T{sub T}(k{sub 0})/T{sub R}(k{sub 0})]. We obtain T{sub ?}(k) to leading order in a Born approximation valid for modes of observational relevance today. A fit yields T{sub ?}(k) = 1+A{sub ?}k{sup ?p}cos [2??k/H{sub sr}+?{sub ?}], with 1.5?R}(k) and r(k{sub 0}) with a period of the order of the Hubble scale during slow roll inflation. The results are quite general and independent of the specific inflationary potentials, depending solely on the ratio of kinetic to potential energy ? and the slow roll parameters ?{sub V}, ?{sub V} to leading order in slow roll. For a wide range of ? and the values of ?{sub V};?{sub V} corresponding to the upper bounds from Planck, we find that the low quadrupole is consistent with the results from Planck, and the oscillations in r(k{sub 0}) as a function of k{sub 0} could be observable if the modes corresponding to the quadrupole and the pivot scale crossed the Hubble radius very few (23) e-folds after the onset of slow roll. We comment on possible impact on the recent BICEP2 results.

  14. Alternate Funding Sources for the International Atomic Energy Agency

    SciTech Connect (OSTI)

    Toomey, Christopher; Wyse, Evan T.; Kurzrok, Andrew J.; Swarthout, Jordan M.

    2012-09-04

    Since 1957, the International Atomic Energy Agency (IAEA) has worked to ensure the safe and responsible promotion of nuclear technology throughout the world. The IAEA operates at the intersection of the Nuclear Nonproliferation Treatys (NPT) fourth and third articles, which guarantee Parties to the Treaty the right to peaceful uses of nuclear technology, provided those activities are placed under safeguards verified by the IAEA. However, while the IAEA has enjoyed substantial success and prestige in the international community, there is a concern that its resources are being stretched to a point where it may no longer be possible to execute its multifaceted mission in its entirety. As noted by the Director General (DG) in 2008, demographics suggest that every aspect of the IAEAs operations will be in higher demand due to increasing reliance on non-carbon-based energy and the concomitant nonproliferation, safety, and security risks that growth entails. In addition to these nuclear energy concerns, the demand for technical developmental assistance in the fields of food security, resource conservation, and human health is also predicted to increase as the rest of the world develops. Even with a 100% value-for-money rating by the U.S. Office of Management and Budget (OMB) and being described as an extraordinary bargain by the United Nations Secretary-Generals High-level Panel on Threats, Challenges and Change, real budget growth at the Agency has been limited to zero-real growth for a better part of the last two decades. Although the 2012 regular budget (RB) received a small increase for most programs, the 2013 RB has been set at zero-real growth. As a result, the IAEA has had to defer infrastructure investments, which has hindered its ability to provide the public goods its Members seek, decreased global security and development opportunities, and functionally transformed the IAEA into a charity, dependent on extrabudgetary (EB) contributions to sustain its mission and capabilities. To resolve these resource constraints, we recommend the creation of an endowment, funded entirely through private contributions. Our initial estimates for the endowment are that a 2B principal. This level of capitalization could provide significant support to all aspects of the IAEAs mission, including Capital Investment and Innovation; Technical Cooperation; as well as incentivizing the policy and technology entrepreneurship that will be necessary for the future health of the nonproliferation regime. Given this potential, our future efforts will focus on a more rigorous assessment of the financial requirements, while simultaneously creating the beginnings of a functional organization. These include: organizational structure, metrics for grant-making and performance evaluation, and outreach and fundraising strategies. At the end of this process, there should be sufficient information and engagement to begin to operationalize the endowment through external funding sources.

  15. RECONSTRUCTING PALEO-SMT POSITIONS ON THE CASCADIA MARGIN USING MAGNETIC SUSCEPTIBILITY

    SciTech Connect (OSTI)

    Johnson, Joel; Phillips, Stephen

    2014-09-30

    Magnetic susceptibility (κ) is a mixed signal in marine sediments, representing primary depositional and secondary diagenetic processes. Production of hydrogen sulfide via anaerobic oxidation of methane (AOM) at the sulfate-methane transition (SMT) and organoclastic sulfate reduction above the SMT can result in the dissolution of iron oxides, altering κ in sediments in methane gas and gas hydrate bearing regions. We investigated records of κ on the Cascadia margin (ODP Sites 1249 and 1252; IODP Site 1325) using a Zr/Rb heavy mineral proxy from XRF core scanning to identify intervals of primary detrital magnetic susceptibility and intervals and predict intervals affected by magnetite dissolutions. We also measured total sulfur content, grain size distributions, total organic carbon (TOC) content, and magnetic mineral assemblage. The upper 100 m of Site 1252 contains a short interval of κ driven by primary magnetite, with multiple intervals (> 90 m total) of decreased κ correlated with elevated sulfur content, consistent with dissolution of magnetite and re-precipitation of pyrite. In the upper 90 m of Site 1249, κ is almost entirely altered by diagenetic processes, with much of the low κ explained by a high degree of pyritization, and some intervals affected by the precipitation of magnetic iron sulfides. At Site 1325, κ between 0-20 and 51-73 mbsf represents primary mineralogy, and in the interval 24-51 mbsf, κ may be reduced due to pyritization. This integrated approach allows for a prediction of primary κ and the amount of κ loss at each site when compared to actual κ measurements. In the case of magnetite dissolution and full pyritization, these drawdowns in κ are supported by sulfur measurements, and the exposure times of magnetite to hydrogen sulfide can be modeled. The presence of methane and methane hydrates at these sites, as well as large variations in TOC content, suggest that the past migration rates of the SMT and variation in sulfate reduction rates may influence κ alteration along the Cascadia margin.

  16. Martensitic transformation behaviors of rapidly solidified TiNiMo powders

    SciTech Connect (OSTI)

    Kim, Yeon-wook

    2012-10-15

    For the fabrication of bulk near-net-shape shape memory alloys and porous metallic biomaterials, consolidation of TiNiMo alloy powders is more useful than that of elemental powders of Ti, Ni and Mo. Ti{sub 50}Ni{sub 49.9}Mo{sub 0.1} shape memory alloy powders were prepared by gas atomization, and transformation temperatures and microstructures of those powders were investigated as a function of powder size. XRD analysis showed that the B2RB19 martensitic transformation occurred in powders smaller than 150 ?m. According to DSC analysis of the as-atomized powders, the B2R transformation temperature (T{sub R}) of the 2550 ?m powders was 18.4 C. The T{sub R} decreased with increasing powder size, however, the difference in T{sub R} between 2550 ?m powders and 100150 ?m powders is only 1 C. Evaluation of powder microstructures was based on SEM examination of the surface and the polished and etched powder cross sections and the typical images of the rapidly solidified powders showed cellular morphology. Porous cylindrical foams of 10 mm diameter and 1.5 mm length were fabricated by spark plasma sintering (SPS) at 800 C and 5 MPa. Finally these porous TiNi alloy samples are heat-treated for 1 h at 850 C, and then quenched in ice water. The bulk samples have 23% porosity and 4.6 g/cm{sup 3} density and their T{sub R} is 17.8 C.

  17. Zn2+ and Sr2+ Adsorption at the TiO2 (110)-Electrolyte Interface: Influence of Ionic Strength, Coverage, and Anions

    SciTech Connect (OSTI)

    Zhang,Z.; Fenter, P.; Cheng, L.; Sturchio, N.; Bedzyk, M.; Machesky, M.; Anovitz, L.; Wesolowski, D.

    2006-01-01

    The X-ray standing wave technique was used to probe the sensitivity of Zn{sup 2+} and Sr{sup 2+} ion adsorption to changes in both the adsorbed ion coverage and the background electrolyte species and concentrations at the rutile ({alpha}-TiO{sub 2}) (110)-aqueous interface. Measurements were made with various background electrolytes (NaCl, NaTr, RbCl, NaBr) at concentrations as high as 1 m. The results demonstrate that Zn{sub 2+} and Sr{sub 2+} reside primarily in the condensed layer and that the ion heights above the Ti-O surface plane are insensitive to ionic strength and the choice of background electrolyte (with <0.1 Angstroms changes over the full compositional range). The lack of any specific anion coadsorption upon probing with Br{sup -}, coupled with the insensitivity of Zn{sup 2+} and Sr{sup 2+} cation heights to changes in the background electrolyte, implies that anions do not play a significant role in the adsorption of these divalent metal ions to the rutile (110) surface. Absolute ion coverage measurements for Zn{sup 2+} and Sr{sup 2+} show a maximum Stern-layer coverage of {approx}0.5 monolayer, with no significant variation in height as a function of Stern-layer coverage. These observations are discussed in the context of Gouy-Chapman-Stern models of the electrical double layer developed from macroscopic sorption and pH-titration studies of rutile powder suspensions. Direct comparison between these experimental observations and the MUltiSIte Complexation (MUSIC) model predictions of cation surface coverage as a function of ionic strength revealed good agreement between measured and predicted surface coverages with no adjustable parameters.

  18. Solvent Refined Coal (SRC) process: trace elements. Research and development report No. 53, interim report No. 30. Volume III. Pilot plant development work. Part 6. The fate of trace elements in the SRC process. [111 references

    SciTech Connect (OSTI)

    Khalil, S. R.

    1980-02-01

    Instrumental neutron activation analysis was used to study the distribution and fate of up to 36 elements in the Solvent Refined Coal Process Pilot Plant located at Fort Lewis, Washington. The elements Ti, V, Mg, Ca, Al, Cl, Mn, As, Br, Na, K, Sm, La, Ga, Cu, Sb, Se, Hg, Ni, Co, Cr, Fe, Rb, Cs, Sc, Tb, Eu, Ce, Sr, Ba, Th, U, Hf, Ta, Zr and Zn were measured in feed coal, insoluble residues, process solvent, process and effluent waters, by-product sulfur, SRC-I solid product, liquid-liquid separator oils and SRC-II liquid products. The material balance was calculated for each element from the concentration data and yields of each process fraction for both the SRC-I and SRC-II processes. Except for Ti, Cl and Br in the SRC-I mode and Hg in the SRC-II mode, each element was substantially lower in the SRC products than in the original feed coal. Residues from the process contained more than 80% of the trace element content found in the coal, except for Hg. More than 98.5% of the total contents of K and Fe in coal were retained in the insoluble residues. Elements such as Hg, Se, As and Sb can form volatile compounds (such as Hg/sup 0/, H/sub 2/Se, AsH/sub 3/ and SbH/sub 3/) stable under the process conditions. The high enhancement factors of Se (957), As (202) and Sb (27.4) in the aqueous phase of the separator water compared to that of the oil are evidence for the formation of volatile species which are more soluble in water than in the oil phase.

  19. Selective oxidation of alkanes and/or alkenes to valuable oxygenates

    DOE Patents [OSTI]

    Lin, Manhua (Maple Glen, PA); Pillai, Krishnan S. (North Brunwick, NJ)

    2011-02-15

    A catalyst, its method of preparation and its use for producing at least one of methacrolein and methacrylic acid, for example, by subjecting isobutane or isobutylene or a mixture thereof to a vapor phase catalytic oxidation in the presence of air or oxygen. In the case where isobutane alone is subjected to a vapor phase catalytic oxidation in the presence of air or oxygen, the product is at least one of isobutylene, methacrolein and methacrylic acid. The catalyst comprises a compound having the formula A.sub.aB.sub.bX.sub.xY.sub.yZ.sub.zO.sub.o wherein A is one or more elements selected from the group of Mo, W and Zr, B is one or more elements selected from the group of Bi, Sb, Se, and Te, X is one or more elements selected from the group of Al, Bi, Ca, Ce, Co, Fe, Ga, Mg, Ni, Nb, Sn, W and Zn, Y is one or more elements selected from the group of Ag, Au, B, Cr, Cs, Cu, K, La, Li, Mg, Mn, Na, Nb, Ni, P, Pb, Rb, Re, Ru, Sn, Te, Ti, V and Zr, and Z is one or more element from the X or Y groups or from the following: As, Ba, Pd, Pt, Sr, or mixtures thereof, and wherein a=1, 0.05

  20. Synthesis, structure, and bonding in K12Au21Sn4. A polar intermetallic compound with dense Au20 and open AuSn4 layers

    SciTech Connect (OSTI)

    Li, Bin; Kim, Sung-Jin; Miller, Gordon J.; and Corbett, John D.

    2009-10-29

    The new phase K{sub 12}Au{sub 21}Sn{sub 4} has been synthesized by direct reaction of the elements at elevated temperatures. Single crystal X-ray diffraction established its orthorhombic structure, space group Pmmn (No. 59), a = 12.162(2); b = 18.058(4); c = 8.657(2) {angstrom}, V = 1901.3(7) {angstrom}{sup 3}, and Z = 2. The structure consists of infinite puckered sheets of vertex-sharing gold tetrahedra (Au{sub 20}) that are tied together by thin layers of alternating four-bonded-Sn and -Au atoms (AuSn{sub 4}). Remarkably, the dense but electron-poorer blocks of Au tetrahedra coexist with more open and saturated Au-Sn layers, which are fragments of a zinc blende type structure that maximize tetrahedral heteroatomic bonding outside of the network of gold tetrahedra. LMTO band structure calculations reveal metallic properties and a pseudogap at 256 valence electrons per formula unit, only three electrons fewer than in the title compound and at a point at which strong Au-Sn bonding is optimized. Additionally, the tight coordination of the Au framework atoms by K plays an important bonding role: each Au tetrahedra has 10 K neighbors and each K atom has 8-12 Au contacts. The appreciably different role of the p element Sn in this structure from that in the triel members in K{sub 3}Au{sub 5}In and Rb{sub 2}Au{sub 3}Tl appears to arise from its higher electron count which leads to better p-bonding (valence electron concentrations = 1.32 versus 1.22).

  1. The development of explosions in axisymmetric ab initio core-collapse supernova simulations of 12–25 M⊙ stars

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Bruenn, Stephen W.; Lentz, Eric J.; Hix, William Raphael; Mezzacappa, Anthony; Harris, James Austin; Messer, O. E. Bronson; Endeve, Eirik; Blondin, John M.; Chertkow, Merek Austin; Lingerfelt, Eric J.; et al

    2016-02-16

    We present four ab initio axisymmetric core-collapse supernova simulations initiated from 12, 15, 20, and 25 M⊙ zero-age main sequence progenitors. All of the simulations yield explosions and have been evolved for at least 1.2 s after core bounce and 1 s after material first becomes unbound. These simulations were computed with our Chimera code employing RbR spectral neutrino transport, special and general relativistic transport effects, and state-of-the-art neutrino interactions. Continuing the evolution beyond 1 s after core bounce allows the explosions to develop more fully and the processes involved in powering the explosions to become more clearly evident. Wemore » compute explosion energy estimates, including the negative gravitational binding energy of the stellar envelope outside the expanding shock, of 0.34, 0.88, 0.38, and 0.70 Bethe (B ≡ 1051 erg) and increasing at 0.03, 0.15, 0.19, and 0.52 BS–1, respectively, for the 12, 15, 20, and 25 M⊙ models at the endpoint of this report. We examine the growth of the explosion energy in our models through detailed analyses of the energy sources and flows. We discuss how the explosion energies may be subject to stochastic variations as exemplfied by the effect of the explosion geometry of the 20 M⊙ model in reducing its explosion energy. We compute the proto-neutron star masses and kick velocities. We compare our results for the explosion energies and ejected 56Ni masses against some observational standards despite the large error bars in both models and observations.« less

  2. PARFUME Theory and Model basis Report

    SciTech Connect (OSTI)

    Darrell L. Knudson; Gregory K Miller; G.K. Miller; D.A. Petti; J.T. Maki; D.L. Knudson

    2009-09-01

    The success of gas reactors depends upon the safety and quality of the coated particle fuel. The fuel performance modeling code PARFUME simulates the mechanical, thermal and physico-chemical behavior of fuel particles during irradiation. This report documents the theory and material properties behind various capabilities of the code, which include: 1) various options for calculating CO production and fission product gas release, 2) an analytical solution for stresses in the coating layers that accounts for irradiation-induced creep and swelling of the pyrocarbon layers, 3) a thermal model that calculates a time-dependent temperature profile through a pebble bed sphere or a prismatic block core, as well as through the layers of each analyzed particle, 4) simulation of multi-dimensional particle behavior associated with cracking in the IPyC layer, partial debonding of the IPyC from the SiC, particle asphericity, and kernel migration (or amoeba effect), 5) two independent methods for determining particle failure probabilities, 6) a model for calculating release-to-birth (R/B) ratios of gaseous fission products that accounts for particle failures and uranium contamination in the fuel matrix, and 7) the evaluation of an accident condition, where a particle experiences a sudden change in temperature following a period of normal irradiation. The accident condition entails diffusion of fission products through the particle coating layers and through the fuel matrix to the coolant boundary. This document represents the initial version of the PARFUME Theory and Model Basis Report. More detailed descriptions will be provided in future revisions.

  3. Fission Product Monitoring and Release Data for the Advanced Gas Reactor -1 Experiment

    SciTech Connect (OSTI)

    Dawn M. Scates; John B. Walter; Jason M. Harp; Mark W. Drigert; Edward L. Reber

    2010-10-01

    The AGR-1 experiment is a fueled multiple-capsule irradiation experiment that was irradiated in the Advanced Test Reactor (ATR) from December 26, 2006 until November 6, 2009 in support of the Very High Temperature Reactor (VHTR) Technology Development Office (TDO) Fuel Development and Qualification program. An important measure of the fuel performance is the quantification of the fission product releases over the duration of the experiment. To provide this data for the inert fission gasses(Kr and Xe), a fission product monitoring system (FPMS) was developed and implemented to monitor the individual capsule effluents for the radioactive species. The FPMS continuously measured the concentrations of various krypton and xenon isotopes in the sweep gas from each AGR-1 capsule to provide an indicator of fuel irradiation performance. Spectrometer systems quantified the concentrations of Kr-85m, Kr-87, Kr-88, Kr-89, Kr-90, Xe-131m, Xe-133, Xe 135, Xe 135m, Xe-137, Xe-138, and Xe-139 accumulated over repeated eight hour counting intervals.-. To determine initial fuel quality and fuel performance, release activity for each isotope of interest was derived from FPMS measurements and paired with a calculation of the corresponding isotopic production or birthrate. The release activities and birthrates were combined to determine Release-to-Birth ratios for the selected nuclides. R/B values provide indicators of initial fuel quality and fuel performance during irradiation. This paper presents a brief summary of the FPMS, the release to birth ratio data for the AGR-1 experiment and preliminary comparisons of AGR-1 experimental fuels data to fission gas release models.

  4. Surface Complexation of Neodymium at the Rutile-Water Interface: A Potentiometric and Modeling Study in NaCl Media to 250C

    SciTech Connect (OSTI)

    Ridley, Mora K.; Machesky, Michael L.; Wesolowski, David J; Palmer, Donald

    2005-01-01

    The adsorption of Nd{sup 3+} onto rutile surfaces was examined by potentiometric titration from 25 to 250 C, in 0.03 and 0.30m NaCl background electrolyte. Experimental results show that Nd{sup 3+} sorbs strongly, even at low temperature, with adsorption commencing below the pHznpc of rutile. In addition, there is a systematic increase in Nd{sup 3+} adsorption with increasing temperature. The experimental results were rationalized and described using surface oxygen proton affinities computed from the MUlti SIte Complexation or MUSIC model, coupled with a Stern-based three-layer description of the oxide/water interface. Moreover, molecular-scale information was incorporated successfully into the surface complexation model, providing a unique geometry for the adsorption of Nd{sup 3+} on rutile. The primary mode of Nd{sup 3+} adsorption was assumed to be the tetradentate configuration found for Y{sup 3+} adsorption on the rutile (110) surface from previously described in situ X-ray standing wave experiments, wherein the sorbing cations bond directly with two adjacent ''terminal'' and two adjacent ''bridging'' surface oxygen atoms. Similarly, the adsorption of Na{sup +} counterions was also assumed to be tetradentate, as supported by MD simulations of Na{sup +} interactions with the rutile (110) surface, and by analogous X-ray standing wave results for Rb{sup +} adsorption on rutile. Fitting parameters for Nd{sup 3+} adsorption included binding constants for the tetradentate adsorption complex and capacitance values for the inner-sphere binding plane. In addition, hydrolysis of the tetradentate adsorption complex was permitted and resulted in significantly improved model fits at higher temperature and pH values. The modeling results indicate that the Stern-based MUSIC surface-complexation model adequately accommodates molecular-scale information to uniquely rationalize and describe multivalent ion adsorption systematically into the hydrothermal regime.

  5. Natural-analog studies for partial validation of conceptual models of radionuclide retardation at the Waste Isolation Pilot Plant (WIPP)

    SciTech Connect (OSTI)

    Ward, D.B.; Brookins, D.G. . Dept. of Geology); Siegel, M.D.; Lambert, S.J. )

    1990-01-01

    Transport by groundwater within the Culebra Dolomite, an aquifer above the Waste Isolation Pilot Plant (WIPP), is the most probable mechanism for long-term release of radionuclides to the accessible environment. Radionuclides could be retarded by sorption if the groundwater is exposed to sufficient amounts of fracture-lining clays. In this natural-analog study, distributions of U and trace metals have been examined to constrain the strength of clay/solute interactions within the Culebra. Uranium solid/liquid distribution ratios, calculated from U concentrations of groundwaters and consanguineous fracture-filling clays, range from {approximately}80 to 800 m{ell}/g and imply retardation factors of 60 to 500 using a fracture-flow model. Retardation factors inferred from uranium-series disequilibria and {sup 14}C ages in Culebra groundwaters alone are much lower ({approximately}10), implying that clays may contain a significant unreactive component of U. Such a possibility is corroborated by Rb/Sr ages; these imply long-term stability of the clays,with resetting occurring more than 250 Ma ago. Factor analysis and mass-balance calculations suggest, however, that Mg-rich clays are dissolving in Pleistocene-age groundwaters and/or are converting to Na-rich smectites, and that B and Li are taken up from the water by the clays. Apparently, the solution chemistry reflects gradual equilibration of clays with groundwater, but thus far the bulk of the clays remain structurally intact. Measurements of the distribution of U in the Culebra will be more meaningful if the inert and exchangeable components of the U content of the clays can be quantified. 26 refs., 3 figs., 2 tabs.

  6. Mass transfer during wall-rock alteration: An example from a quartz-graphite vein, Black Hills, South Dakota

    SciTech Connect (OSTI)

    Galbreath, K.C.; Duke, E.F.; Papike, J.J. ); Laul, J.C. )

    1988-07-01

    Mass transfer and fluid-rock interaction have been evaluated along two sample traverses in low-sillimanite grade quartz-mica schist adjacent to a synmetamorphic quartz-graphite vein in the southern Black Hills, South Dakota. In an {approximately}17 cm halo between apparently unaltered schist and the vein contact is an outer zone of cryptic alteration and three inner zones of visible alteration. The cryptic zone consists of the original prograde metamorphic mineral assemblage plus anomalously high amounts of tourmaline. The outermost visible zone contains abundant graphite. The second visible zone is defined by intensive bleaching of the schist. The innermost visible zone, immediately adjacent to the vein, is tourmaline + quartz + plagioclase + limonite + graphite. The vein is composed almost entirely of quartz, but also contains trace amounts of graphite. Mass balance calculations indicate that Al was essentially inert. The predominant chemical changes during wall-rock alteration were addition of B and C from the vein-forming fluid along with loss of K from the wall rocks, corresponding to precipitation of tourmaline and graphite, and the progressive destruction of microcline, biotite, and muscovite toward the vein. In addition, the elements V, Cr, Cu, Zn, Pb, As, Sb, W, and Au were introduced into the country rock, whereas Si, Rb, Ba, and Cs were removed. Fluid-rock interaction modeling suggests that between one and four equivalent masses of fluid interacted chemically with the most altered mineral assemblages. In addition, greater than one equivalent mass of reactive fluid penetrated to distances of at least 5 cm from the vein contact.

  7. Solvent Refined Coal (SRC) process: trace elements. Research and development report No. 53, interim report No. 31, August 1976-July 1977. Volume III. Pilot plant development work. Part 6. [Fate of 36 trace elements

    SciTech Connect (OSTI)

    1980-03-01

    Results are presented on a study of the distribution and fate of 34 trace elements in the Solvent Refined Coal Process at the pilot plant located at Fort Lewis, Washington, and operated by The Pittsburg and Midway Coal Mining Co. under contract with the US Department of Energy. Neutron activation analysis was used to determine Ti, V, Ca, Mg, Al, Cl, Mn, As, Sb, Se, Hg, Br, Co, Ni, Cr, Fe, Na, Rb, Cs, K, Sc, Tb, Eu, Sm, Ce, La, Sr, Ba, Th, Hf, Ta, Ga, Zr, and Cu in feed coals, process solvent, Solvent Refined Coal (SRC), mineral residues, wet filter cake, by-product solvents, process and effluent waters and by-product sulfur. The sample points were chosen such that the major process streams were adequately described and that the major input and output materials were included. Atomic absorption spectrophotometry was used to measure the toxic elements Pb, Cd, Be in plant-derived solvents, effluent water and Hamer Marsh water. Specific methods were developed for analysis of a wide range of material compositions. The neutron activation analysis procedures were divided into short and long irradiation procedures for elements with short half lives (less than 3 hours) and intermediate to long half lives ( 8 hours to 5.2 years). Data are presented for a third equilibrium set of samples from the SRC-I process and compared to two similar sets analyzed previously. A material balance (or budget) was calculated for each element from the concentration data and the yields of each process fraction. Data are also presented on a study of carbon monoxide addition to the hydrogen stream and its effect on trace elements, and trace element data on a study of thirty-six plant effluent water samples taken during an SRC-I production run.

  8. Insulin like growth factor 2 regulation of aryl hydrocarbon receptor in MCF-7 breast cancer cells

    SciTech Connect (OSTI)

    Tomblin, Justin K.; Salisbury, Travis B.

    2014-01-17

    Highlights: IGF-2 stimulates concurrent increases in AHR and CCND1 expression. IGF-2 promotes the binding of AHR to the endogenous cyclin D1 promoter. AHR knockdown inhibits IGF-2 stimulated increases in CCND1 mRNA and protein. AHR knockdown inhibits IGF-2 stimulated increases in MCF-7 proliferation. -- Abstract: Insulin like growth factor (IGF)-1 and IGF-2 stimulate normal growth, development and breast cancer cell proliferation. Cyclin D1 (CCND1) promotes cell cycle by inhibiting retinoblastoma protein (RB1). The aryl hydrocarbon receptor (AHR) is a major xenobiotic receptor that also regulates cell cycle. The purpose of this study was to investigate whether IGF-2 promotes MCF-7 breast cancer proliferation by inducing AHR. Western blot and quantitative real time PCR (Q-PCR) analysis revealed that IGF-2 induced an approximately 2-fold increase (P < .001) in the expression of AHR and CCND1. Chromatin immunoprecipitation (ChIP), followed by Q-PCR indicated that IGF-2 promoted (P < .001) a 7-fold increase in AHR binding on the CCND1 promoter. AHR knockdown significantly (P < .001) inhibited IGF-2 stimulated increases in CCND1 mRNA and protein. AHR knockdown cells were less (P < .001) responsive to the proliferative effects of IGF-2 than control cells. Collectively, our findings have revealed a new regulatory mechanism by which IGF-2 induction of AHR promotes the expression of CCND1 and the proliferation of MCF-7 cells. This previously uncharacterized pathway could be important for the proliferation of IGF responsive cancer cells that also express AHR.

  9. The composition of peridotite tectonites from the Ivrea Complex, northern Italy: Residues from melt extraction

    SciTech Connect (OSTI)

    Hartmann, G.; Wedepohl, K.H. )

    1993-04-01

    Peridotite tectonites have been analyzed for major elements, forty minor elements, mineral composition, and a subset a samples have been investigated for [delta]D, [delta][sup 18]O, [delta][sup 34]S, and [sup 87]Sr/[sup 86]Sr ratios. The spinel lherzolites from Balmuccia and Baldissero contain on average 56% olivine, 28% orthopyroxene, 14% clinopyroxene, and 1.5% spinel. They have a neodymium and strontium isotopic signature similar to MORB (oceanic ridge basalt). These peridotites were moderately depleted in Al and Ca and highly depleted in incompatible elements by the separation of 4.5% P-MORB. The MORB in excess to the formation and subduction of the oceanic crust fractionated into a tonalitic continental crust and a pyroxenitic residue which was recycled into the mantle. The crustal mass fraction of the upper mantle-crust system is 2.8%. A primitive mantle composition can be calculated from 97.2% Balmuccia model peridotite plus 2.8% bulk crust. The new set of primitive mantle concentrations is in accordance, within about 10%, with the data from fertile peridotite xenoliths and primitive meteorites for the elements Li, Mg, Si, Ca, Sc, V, Mn, Fe, Co, Ni, Zn, Ga, Y, Zr, La, Ce, Nd, Eu, Tb, Dy, Yb, Lu and Hf. Larger differences occur for the elements F, Na, P, Ti, Cr, and Cu. The bulk crust concentrations of the highly incompatible and mobile elements K, Rb, Ba, Th, and U exceed those being supplied from a primitive upper mantle reservoir of 660 km depth. An additional lower mantle source is required for about half of the crustal accumulation of these elements. Moderately depleted peridotite bodies with a cross section of 3 km can be sufficiently well homogenized in compatible and moderately incompatible elements to represent MORB producing upper mantle. Concentrations of Na, Sc, Ti, V, Ga, Y, Zr, and Yb are well correlated with the Al abundance so that primitive mantle values can also be estimated using the cosmically derived primordial Al concentration.

  10. Synthesis, characterization and optical properties of NH{sub 4}Dy(PO{sub 3}){sub 4}

    SciTech Connect (OSTI)

    Chemingui, S.; Ferhi, M. Horchani-Naifer, K.; Férid, M.

    2014-09-15

    Polycrystalline powders of NH{sub 4}Dy(PO{sub 3}){sub 4} polyphosphate have been grown by the flux method. This compound was found to be isotopic with NH{sub 4}Ce(PO{sub 3}){sub 4} and RbHo(PO{sub 3}){sub 4}. It crystallizes in the monoclinic space group P2{sub 1/n} with unit cell parameters a=10.474(6) Å, b=9.011(4) Å, c=10.947(7) Å and β=106.64(3)°. The title compound has been transformed to triphosphate Dy(PO{sub 3}){sub 3} after calcination at 800 °C. Powder X-ray diffraction, infrared and Raman spectroscopies and the differential thermal analysis have been used to identify these materials. The spectroscopic properties have been investigated through absorption, excitation, emission spectra and decay curves of Dy{sup 3+} ion in both compounds at room temperature. The emission spectra show the characteristic emission bands of Dy{sup 3+} in the two compounds, before and after calcination. The integrated emission intensity ratios of the yellow to blue (I{sub Y}/I{sub B}) transitions and the chromaticity properties have been determined from emission spectra. The decay curves are found to be double-exponential. The non-exponential behavior of the decay rates was related to the resonant energy transfer as well as cross-relaxation between the donor and acceptor Dy{sup 3+} ions. The determined properties have been discussed as function of crystal structure of both compounds. They reveal that NH{sub 4}Dy(PO{sub 3}){sub 4} is promising for white light generation but Dy(PO{sub 3}){sub 3} is potential candidates in field emission display (FED) and plasma display panel (PDP) devices. - Graphical abstract: The CIE color coordinate diagrams showing the chromatic coordinates of Dy{sup 3+} luminescence in NH{sub 4}Dy(PO{sub 3}){sub 4} and Dy(PO{sub 3}){sub 3}. - Highlights: • The polycrystalline powders of NH{sub 4}Dy(PO{sub 3}){sub 4} and Dy(PO{sub 3}){sub 3} are synthesized. • The obtained powders are characterized. • The spectroscopic properties of Dy{sup 3+} ion are investigated. • Results are discussed as function of crystal structure and chemical composition. • The usefulness of NH{sub 4}Dy(PO{sub 3}){sub 4} and Dy(PO{sub 3}){sub 3} in optical devices is revealed.

  11. Transient inhibition of cell proliferation does not compromise self-renewal of mouse embryonic stem cells

    SciTech Connect (OSTI)

    Wang, Ruoxing; Guo, Yan-Lin

    2012-10-01

    Embryonic stem cells (ESCs) have unlimited capacity for self-renewal and can differentiate into various cell types when induced. They also have an unusual cell cycle control mechanism driven by constitutively active cyclin dependent kinases (Cdks). In mouse ESCs (mESCs). It is proposed that the rapid cell proliferation could be a necessary part of mechanisms that maintain mESC self-renewal and pluripotency, but this hypothesis is not in line with the finding in human ESCs (hESCs) that the length of the cell cycle is similar to differentiated cells. Therefore, whether rapid cell proliferation is essential for the maintenance of mESC state remains unclear. We provide insight into this uncertainty through chemical intervention of mESC cell cycle. We report here that inhibition of Cdks with olomoucine II can dramatically slow down cell proliferation of mESCs with concurrent down-regulation of cyclin A, B and E, and the activation of the Rb pathway. However, mESCs display can recover upon the removal of olomoucine II and are able to resume normal cell proliferation without losing self-renewal and pluripotency, as demonstrated by the expression of ESC markers, colony formation, embryoid body formation, and induced differentiation. We provide a mechanistic explanation for these observations by demonstrating that Oct4 and Nanog, two major transcription factors that play critical roles in the maintenance of ESC properties, are up-regulated via de novo protein synthesis when the cells are exposed to olomoucine II. Together, our data suggest that short-term inhibition of cell proliferation does not compromise the basic properties of mESCs. -- Highlights: Black-Right-Pointing-Pointer Inhibition of Cdks slows down mESCs proliferation. Black-Right-Pointing-Pointer mESCs display remarkable recovery capacity from short-term cell cycle interruption. Black-Right-Pointing-Pointer Short-term cell cycle interruption does not compromise mESC self-renewal. Black-Right-Pointing-Pointer Oct4 and Nanog are up-regulated via de novo synthesis by cell cycle interruption.

  12. Genetic Factors Affecting Susceptibility to Low Dose & Low Dose-Rate Radiation

    SciTech Connect (OSTI)

    Bedford, Joel

    2014-04-18

    Our laboratory has, among other things, developed and used the gamma H2AX focus assay and other chromosomal and cell killing assays to show that differences in this DNA double strand break (dsb) related response can be clearly and distinctly demonstrated for cells which are mildly hyper-radiosensitive such as those associated with A-T heterozygosity. We have found this level of mild hypersensitivity for cells from some 20 to 30 % of apparently normal individuals and from apparently normal parents of Retinoblastoma patients. We found significant differences in gene expression in somatic cells from unaffected parents of Rb patients as compared with normal controls, suggesting that these parents may harbor some as yet unidentified genetic abnormality. In other experiments we sought to determine the extent of differences in normal human cellular reaponses to radiation depending on their irradiation in 2D monolayer vs 3D organized acinar growth conditions. We exmined cell reproductive death, chromosomal aberration induction, and the levels of ?-H2AX foci in cells after single acute gamma-ray doses and immediately after 20 hours of irradiation at a dose rate of 0.0017 Gy/min. We found no significant differences in the dose-responses of these cells under the 2D or 3D growth conditions. While this does not mean such differences cannot occur in other situations, it does mean that they do not generally or necessarily occur. In another series of studies in collaboration with Dr Chuan Li, with supprt from this current grant. We reported a role for apoptotic cell death in promoting wound healing and tissue regeneration in mice. Apoptotic cells released growth signals that stimulated the proliferation of progenitor or stem cells. In yet another collaboration with Dr, B. Chen with funds from this grant, the relative radiosensitivity to cell killing as well as chromosomal instability of 13 DNA-PKcs site-directed mutant cell lines (defective at phosphorylation sites or kinase activity) were examined after exposure of synchronized G1 cells to 137Cs c rays. DNA-PKcs mutant cells defective in phosphorylation at multiple sites withinthe T2609 cluster or within the PI3K domain displayed extreme radiosensitivity. Cells defective at the S2056 cluster or T2609 single site alone were only mildly radiosensitive, but cells defective at even one site in both the S2056 and T2609 clusters were maximally radiosensitive. Thus a synergism between the capacity for phosphorylation at the S2056 and T2609 clusterswas found to be critical for induction of radiosensitivity.

  13. Structural and Crystal Chemical Properties of Alkali Rare-earth Double Phosphates

    SciTech Connect (OSTI)

    Farmer, James Matthew; Boatner, Lynn A.; Chakoumakos, Bryan C.; Rawn, Claudia J.; Richardson, Jim

    2015-09-16

    When appropriately activated, alkali rare-earth double phosphates of the form: M3RE(PO4)2 (where M denotes an alkali metal and RE represents either a rare-earth element or Y or Sc) are of interest for use as inorganic scintillators for radiation detection at relatively long optical emission wavelengths. These compounds exhibit layered crystal structures whose symmetry properties depend on the relative sizes of the rare-earth and alkali-metal cations. Single-crystal X-ray and powder neutron diffraction methods were used here to refine the structures of the series of rare-earth double phosphate compounds: K3RE(PO4)2 with RE = Lu, Er, Ho, Dy, Gd, Nd, Ce, plus Y and Sc - as well as the compounds: A3Lu(PO4)2, with A = Rb, and Cs. The double phosphate K3Lu(PO4)2 was reported and structurally refined previously. This material had a hexagonal unit cell at room temperature with the Lu ion six-fold coordinated with oxygen atoms of the surrounding phosphate groups. Additionally two lower-temperature phases were observed for K3Lu(PO4)2. The first phase transition to a monoclinic P21/m phase occurred at ~230 K, and the Lu ion retained its six-fold coordination. The second K3Lu(PO4)2 phase transition occurred at ~130 K. The P21/m space group symmetry was retained, however, one of the phosphate groups rotated to increase the oxygen coordination number of Lu from six to seven. This structure then became isostructural with the room-temperature form of the compound K3Yb(PO4)2 reported here that also exhibits an additional high-temperature phase which occurs at T = 120 C with a transformation to hexagonal P-3 space group symmetry and a Yb-ion coordination number reduction from seven to six. This latter result was confirmed using EXAFS. The single-crystal growth methods structural systematics, and thermal expansion properties of the present series of alkali rare-earth double phosphates, as determined by X-ray and neutron diffraction methods, are treated here.

  14. Nuclear Data Sheets for A = 84

    SciTech Connect (OSTI)

    Abriola, Daniel; Bostan, Melih; Erturk, Sefa; Fadil, Manssour; Galan, Monica; Juutinen, Sakari; Kibedi, Tibor; Kondev, Filip; Luca, Aurelian; Negret, Alexandru; Nica, Ninel; Pfeiffer, Bernd; Singh, Balraj; Sonzogni, Alejandro; Timar, Janos; Tuli, Jagdish; Venkova, Tsanka; Zuber, Kazimierz

    2009-11-15

    The evaluated spectroscopic data are presented for 12 known nuclides of mass 84 (Ga, Ge, As, Se, Br, Kr, Rb, Sr, Y, Zr, Nb, Mo). Except for the stable nuclides {sup 84}Sr and {sup 84}Kr, extensive new data are available for all the other nuclides since the 1997 evaluation by J.K. Tuli (1997Tu02) of A = 84 nuclides. Many precise Penning-trap mass measurements since AME-2003 for A = 84 nuclides (2009Re03,2008Ha23,2008We10,2007Ke09,2006Ka48,2006De36,2006Ri15) have resulted in improved Q values and separation energies. However, many deficiencies still remain. Some examples are given below. Excited-state data for {sup 84}Ga and {sup 84}As are nonexistent, and those for {sup 84}Ge are scarce. The radioactive decay schemes of {sup 84}Ga, {sup 84}Ge, {sup 84}Se, {sup 84}Y (39.5 min), {sup 84}Y (4.6 s), {sup 84}Zr and {sup 84}Nb suffer from incompleteness and that for {sup 84}Mo decay is not known at all. The energy ordering of the two activities (39.5 min and and 4.6 s) of {sup 84}Y is not well established, although, high-spin with tentative spin-parity of (6+) is adopted here as the ground state of {sup 84}Y based on weak arguments. From a conference report published in 2000, it is clear that extensive experiments were done to investigate decays of {sup 84}Zr and {sup 84}Y, but details of these studies never appeared in literature and none were made available to the evaluators when requested from original authors. This evaluation was carried out as part of ENSDF workshop for Nuclear Structure and Decay Data Evaluators, organized and hosted by the 'Horia Hulubei' National Institute for Physics and Nuclear Engineering, Bucharest, Romania during March 30, 2009 - April 3, 2009. Names of the evaluators principally responsible for evaluation of individual nuclides are given under the respective Adopted data sets.

  15. Science based stockpile stewardship, uncertainty quantification, and fission fragment beams

    SciTech Connect (OSTI)

    Stoyer, M A; McNabb, D; Burke, J; Bernstein, L A; Wu, C Y

    2009-09-14

    Stewardship of this nation's nuclear weapons is predicated on developing a fundamental scientific understanding of the physics and chemistry required to describe weapon performance without the need to resort to underground nuclear testing and to predict expected future performance as a result of intended or unintended modifications. In order to construct more reliable models, underground nuclear test data is being reanalyzed in novel ways. The extent to which underground experimental data can be matched with simulations is one measure of the credibility of our capability to predict weapon performance. To improve the interpretation of these experiments with quantified uncertainties, improved nuclear data is required. As an example, the fission yield of a device was often determined by measuring fission products. Conversion of the measured fission products to yield was accomplished through explosion code calculations (models) and a good set of nuclear reaction cross-sections. Because of the unique high-fluence environment of an exploding nuclear weapon, many reactions occurred on radioactive nuclides, for which only theoretically calculated cross-sections are available. Inverse kinematics reactions at CARIBU offer the opportunity to measure cross-sections on unstable neutron-rich fission fragments and thus improve the quality of the nuclear reaction cross-section sets. One of the fission products measured was {sup 95}Zr, the accumulation of all mass 95 fission products of Y, Sr, Rb and Kr (see Fig. 1). Subsequent neutron-induced reactions on these short lived fission products were assumed to cancel out - in other words, the destruction of mass 95 nuclides was more or less equal to the production of mass 95 nuclides. If a {sup 95}Sr was destroyed by an (n,2n) reaction it was also produced by (n,2n) reactions on {sup 96}Sr, for example. However, since these nuclides all have fairly short half-lives (seconds to minutes or even less), no experimental nuclear reaction cross-sections exist, and only theoretically modeled cross-sections are available. Inverse kinematics reactions at CARIBU offer the opportunity, should the beam intensity be sufficient, to measure cross-sections on a few important nuclides in order to benchmark the theoretical calculations and significantly improve the nuclear data. The nuclides in Fig. 1 are prioritized by importance factor and displayed in stoplight colors, green the highest and red the lowest priority.

  16. Nuclear data sheets for A=84.

    SciTech Connect (OSTI)

    Abriola, D.; Bostan, M.; Erturk, S.; Fadil, M.; Galan, M; Juutinen, S.; Luca, A.; Negret, A.; Nica, N.; Pfeiffer, B.; Singh, B.; Sonzogni, A.; Timar, J.; Tuli, J.; Venkova, T.; Zuber, K.; Kondev, F.; Nuclear Engineering Division; IAEA, Austria; Istanbul Univ.; Nigde Univ.; GANIL, France; CIEMAT, Spain; Univ. Jyvaskyla; ANU, Austrialia; IFIN-HH, Romania; Texas A&M; GSI, Germany; McMaster,Canada; NNDC; ATOMKI, Hungary; INRNE, Bulgaria; IFJ-PAN, Poland

    2009-01-01

    The evaluated spectroscopic data are presented for 12 known nuclides of mass 84 (Ga, Ge, As, Se, Br, Kr, Rb, Sr, Y, Zr, Nb, Mo). Except for the stable nuclides {sup 84}Sr and {sup 84}Kr, extensive new data are available for all the other nuclides since the 1997 evaluation by J.K. Tuli (1997Tu02) of A = 84 nuclides. Many precise Penning-trap mass measurements since AME-2003 for A = 84 nuclides (2009Re03,2008Ha23,2008We10,2007Ke09,2006Ka48,2006De36,2006Ri15) have resulted in improved Q values and separation energies. However, many deficiencies still remain. Some examples are given below. Excited-state data for {sup 84}Ga and {sup 84}As are nonexistent, and those for {sup 84}Ge are scarce. The radioactive decay schemes of {sup 84}Ga, {sup 84}Ge, {sup 84}Se, {sup 84}Y (39.5 min), {sup 84}Y (4.6 s), {sup 84}Zr and {sup 84}Nb suffer from incompleteness and that for {sup 84}Mo decay is not known at all. The energy ordering of the two activities (39.5 min and 4.6 s) of {sup 84}Y is not well established, although, high-spin with tentative spin-parity of (6+) is adopted here as the ground state of {sup 84}Y based on weak arguments. From a conference report published in 2000, it is clear that extensive experiments were done to investigate decays of {sup 84}Zr and {sup 84}Y, but details of these studies never appeared in literature and none were made available to the evaluators when requested from original authors. This evaluation was carried out as part of ENSDF workshop for Nuclear Structure and Decay Data Evaluators, organized and hosted by the 'Horia Hulubei' National Institute for Physics and Nuclear Engineering, Bucharest, Romania during March 30, 2009 - April 3, 2009. Names of the evaluators principally responsible for evaluation of individual nuclides are given under the respective Adopted data sets.

  17. Nuclear Data Sheets A = 84

    SciTech Connect (OSTI)

    Abriola, D.; Sonzogni, A.; Bostan,M. Erturk,S.; Fadi,M.; Galan,M.; Juutinen,S.; Kibed,T.; Kondev,F.; Luca,A.; Negret,A.; Nica,N.; Pfeiffer,B.; Singh.B.; Sonzogni,A.; Timar,J.; Tuli,J.; Venkova,T.; Zuber,K.

    2009-11-01

    The evaluated spectroscopic data are presented for 12 known nuclides of mass 84 (Ga, Ge, As, Se, Br, Kr, Rb, Sr, Y, Zr, Nb, Mo). Except for the stable nuclides {sup 84}Sr and {sup 84}Kr, extensive new data are available for all the other nuclides since the 1997 evaluation by J.K. Tuli (1997Tu02) of A = 84 nuclides. Many precise Penning-trap mass measurements since AME-2003 for A = 84 nuclides (2009Re03,2008Ha23,2008We10,2007Ke09,2006Ka48,2006De36,2006Ri15) have resulted in improved Q values and separation energies. However, many deficiencies still remain. Some examples are given below. Excited-state data for {sup 84}Ga and {sup 84}As are nonexistent, and those for {sup 84}Ge are scarce. The radioactive decay schemes of {sup 84}Ga, {sup 84}Ge, {sup 84}Se, {sup 84}Y (39.5 min), {sup 84}Y (4.6 s), {sup 84}Zr and {sup 84}Nb suffer from incompleteness and that for {sup 84}Mo decay is not known at all. The energy ordering of the two activities (39.5 min and and 4.6 s) of {sup 84}Y is not well established, although, high-spin with tentative spin-parity of (6+) is adopted here as the ground state of {sup 84}Y based on weak arguments. From a conference report published in 2000, it is clear that extensive experiments were done to investigate decays of {sup 84}Zr and {sup 84}Y, but details of these studies never appeared in literature and none were made available to the evaluators when requested from original authors. This evaluation was carried out as part of ENSDF workshop for Nuclear Structure and Decay Data Evaluators, organized and hosted by the 'Horia Hulubei' National Institute for Physics and Nuclear Engineering, Bucharest, Romania during March 30, 2009 - April 3, 2009. Names of the evaluators principally responsible for evaluation of individual nuclides are given under the respective Adopted data sets.

  18. Radiation Doses to Members of the U.S. Population from Ubiquitous Radionuclides in the Body: Part 3, Results, Variability, and Uncertainty

    SciTech Connect (OSTI)

    Watson, David J.; Strom, Daniel J.

    2011-02-25

    This paper is part three of a three-part series investigating annual effective doses to residents of the United States from intakes of ubiquitous radionuclides, including radionuclides occurring naturally, radionuclides whose concentrations are technologically enhanced, and anthropogenic radionuclides. The radionuclides of interest are the 238U series (14 nuclides), the actinium series (headed by 235U; 11 nuclides), and the 232Th series (11 nuclides); primordial radionuclides 87Rb and 40K; cosmogenic and fallout radionuclides 14C and 3H; and purely anthropogenic radionuclides 137Cs-137mBa, 129I and 90Sr-90Y. This series of papers explicitly excludes intakes from inhaling 222Rn, 220Rn, and their short-lived decay products; it also excludes intakes of radionuclides in occupational and medical settings. Part one reviewed, summarized, characterized, and grouped all published and some unpublished data for U.S. residents on ubiquitous radionuclide concentrations in tissues and organs. Part two described the methods used to organize the data collected in part one and segregate it into the ages and genders defined by the study, imputed missing values from the existing data, apportioned activity in bone, and imputed activity in hollow organ contents and the remainder of the body. This paper estimates equivalent doses to target tissues from source regions and maps target tissues to lists of tissues with International Commission on Radiation Protection (ICRP) tissue-weighting factors or to surrogate tissue regions when there is no direct match. Effective doses, using ICRP tissue-weighting factors recommended in 1977, 1990, and 2007, are then calculated, and an upper bound of variability of the effective dose is estimated by calculating the average coefficients of variation (CV), assuming all variance is due to variability. Most of the data were for adult males, whose average annual effective dose is estimated to be 337 ?Sv (CV = 0.65, geometric mean = 283 ?Sv, geometric standard deviation sG = 1.81) using 2007 ICRP tissue-weighting factors. This result is between the National Council on Radiation Protection & Measurements 1987 estimate of 390 ?Sv (using 1977 wTs) and its 2009 estimate of 285 ?Sv (using 2007 wTs) and is higher than the United Nations Scientific Committee on the Effects of Atomic Radiations 2000 estimate of 310 ?Sv (using 1990 wTs). The methods and software developed for this project are sufficiently detailed and sufficiently general to be usable with autopsy data from any or all countries.

  19. Structural and Crystal Chemical Properties of Alkali Rare-earth Double Phosphates

    DOE Public Access Gateway for Energy & Science Beta (PAGES Beta)

    Farmer, James Matthew; Boatner, Lynn A.; Chakoumakos, Bryan C.; Rawn, Claudia J.; Richardson, Jim

    2015-09-16

    When appropriately activated, alkali rare-earth double phosphates of the form: M3RE(PO4)2 (where M denotes an alkali metal and RE represents either a rare-earth element or Y or Sc) are of interest for use as inorganic scintillators for radiation detection at relatively long optical emission wavelengths. These compounds exhibit layered crystal structures whose symmetry properties depend on the relative sizes of the rare-earth and alkali-metal cations. Single-crystal X-ray and powder neutron diffraction methods were used here to refine the structures of the series of rare-earth double phosphate compounds: K3RE(PO4)2 with RE = Lu, Er, Ho, Dy, Gd, Nd, Ce, plus Ymore » and Sc - as well as the compounds: A3Lu(PO4)2, with A = Rb, and Cs. The double phosphate K3Lu(PO4)2 was reported and structurally refined previously. This material had a hexagonal unit cell at room temperature with the Lu ion six-fold coordinated with oxygen atoms of the surrounding phosphate groups. Additionally two lower-temperature phases were observed for K3Lu(PO4)2. The first phase transition to a monoclinic P21/m phase occurred at ~230 K, and the Lu ion retained its six-fold coordination. The second K3Lu(PO4)2 phase transition occurred at ~130 K. The P21/m space group symmetry was retained, however, one of the phosphate groups rotated to increase the oxygen coordination number of Lu from six to seven. This structure then became isostructural with the room-temperature form of the compound K3Yb(PO4)2 reported here that also exhibits an additional high-temperature phase which occurs at T = 120 °C with a transformation to hexagonal P-3 space group symmetry and a Yb-ion coordination number reduction from seven to six. This latter result was confirmed using EXAFS. The single-crystal growth methods structural systematics, and thermal expansion properties of the present series of alkali rare-earth double phosphates, as determined by X-ray and neutron diffraction methods, are treated here.« less

  20. Evaporation a key mechanism for the thaumasite form of sulfate attack

    SciTech Connect (OSTI)

    Mittermayr, Florian; Baldermann, Andre; Kurta, Christoph; Observatoire Midi-Pyrnes, Laboratoire Gosciences Environnement Toulouse, 14, avenue Edouard Belin, 31400 TOULOUSE ; Klammer, Dietmar; Leis, Albrecht; Dietzel, Martin

    2013-07-15

    Understanding the mechanisms leading to chemical attack on concrete is crucial in order to prevent damage of concrete structures. To date, most studies on sulfate attack and thaumasite formation are based on empirical approaches, as the identification of associated reaction mechanisms and paths is known to be highly complex. In this study, sulfate damaged concrete from Austrian tunnels was investigated by mineralogical, chemical and isotope methods to identify the reactions which caused intense concrete alteration. Major, minor and trace elemental contents as well as isotope ratios of local ground water (GW), drainage water (DW) and interstitial solutions (IS), extracted from damaged concrete material, were analyzed. Locally occurring GW contained 3 to 545 mg L{sup ?1} of SO{sub 4} and is thus regarded as slightly aggressive to concrete in accordance to standard specifications (e.g. DIN EN 206-1). The concrete linings and drainage systems of the studied tunnels, however, have partly suffered from intensive sulfate attack. Heavily damaged concrete consisted mainly of thaumasite, secondary calcite, gypsum, and relicts of aggregates. Surprisingly, the concentrations of dissolved ions were extremely enriched in the IS with up to 30,000 and 12,000 mg L{sup ?1} of SO{sub 4} and Cl, respectively. Analyses of aqueous ions with a highly conservative behavior, e.g. K, Rb and Li, as well as {sup 2}H/H and {sup 18}O/{sup 16}O isotope ratios of H{sub 2}O of the IS showed an intensive accumulation of ions and discrimination of the light isotopes vs. the GW. These isotope signals of the IS clearly revealed evaporation at distinct relative humidities. From ion accumulation and isotope fractionation individual total and current evaporation degrees were estimated. Our combined elemental and isotopic approach verified wettingdrying cycles within a highly dynamic concrete-solution-atmosphere system. Based on these boundary conditions, key factors controlling thaumasite formation are discussed regarding the development of more sulfate-resistant concrete and concrete structures.

  1. The new barium zinc mercurides Ba{sub 3}ZnHg{sub 10} and BaZn{sub 0.6}Hg{sub 3.4} - Synthesis, crystal and electronic structure

    SciTech Connect (OSTI)

    Schwarz, Michael; Wendorff, Marco; Roehr, Caroline

    2012-12-15

    The title compounds Ba{sub 3}ZnHg{sub 10} and BaZn{sub 0.6}Hg{sub 3.4} were synthesized from stoichiometric ratios of the elements in Ta crucibles. Their crystal structures, which both represent new structure types, have been determined using single crystal X-ray data. The structure of Ba{sub 3}ZnHg{sub 10} (orthorhombic, oP28, space group Pmmn, a=701.2(3), b=1706.9(8), c=627.3(3)pm, Z=2, R1=0.0657) contains folded 4{sup 4} Hg nets, where the meshes form the bases of flat rectangular pyramids resembling the structure of BaAl{sub 4}. The flat pyramids are connected via Hg-Zn/Hg bonds, leaving large channels at the folds, in which Ba(1) and Hg(2) atoms alternate. Whereas the remaining Hg/Zn atoms form a covalent 3D network of three- to five-bonded atoms with short M-M distances (273-301 pm; CN 9-11), the Hg(2) atoms in the channels adopt a comparatively large coordination number of 12 and increased distances (317-348 pm) to their Zn/Hg neighbours. In the structure of BaZn{sub 0.6}Hg{sub 3.4} (cubic, cI320, space group I4{sup Macron }3d, a=2025.50(7) pm, Z=64, R1=0.0440), with a chemical composition not much different from that of Ba{sub 3}ZnHg{sub 10}, the Zn/Hg atoms of the mixed positions M(1/2) are arranged in an slightly distorted primitive cubic lattice with a 4 Multiplication-Sign 4 Multiplication-Sign 4 subcell relation to the unit cell. The 24 of the originating 64 cubes contain planar cis tetramers Hg(5,6){sub 4} with Hg in a nearly trigonal planar or tetrahedral coordination. In another 24 of the small cubes, two opposing faces are decorated by Hg(3,4){sub 2} dumbbells, two by Ba(2) atoms respectively. The third type of small cubes are centered by Ba(1) atoms only. The complex 3D polyanionic Hg/Zn network thus formed is compared with the Hg partial structure in Rb{sub 3}Hg{sub 20} applying a group-subgroup relation. Despite their different overall structures, the connectivity of the negatively charged Hg atoms, the rather metallic Zn bonding characteristic (as obtained from FP-LAPW band structure calculations) and the coordination number of 16 for all Ba cations relate the two title compounds. - Graphical abstract: Six of the 64 small sub-cubes of three types (A, B, C) forming the unit cell of the Hg-rich mercuride BaZn{sub 0.6}Hg{sub 3.4}. Highlights: Black-Right-Pointing-Pointer Two new Hg-rich Ba mercurides, both synthesized from the elements in pure phase. Black-Right-Pointing-Pointer BaZn{sub 0.6}HgG{sub 3.4} and Ba{sub 3}ZnHg{sub 10} with new complex structure types. Black-Right-Pointing-Pointer Structure relation to other complex cubic intermetallics. Black-Right-Pointing-Pointer Discussion of covalent and metallic bonding aspects, as found by the structure features and band structure calculations.

  2. Geo-Chemo-Mechanical Studies for Permanent CO{sub 2} Storage in Geologic Reservoirs

    SciTech Connect (OSTI)

    Kelemen, Peter; Park, Ah-hyung; Matter, Jurg; Gadikota, Greeshma; Lisabeth, Harrison; Zhu, Wenlu

    2013-09-30

    This two-pronged study investigated the rates and mechanisms of formation of Ca and Mg carbonate minerals via reaction of aqueous fluids with silicate minerals and rocks, and the geomechanical effects of such reactions. The kinetic studies focused on the separation of variables, following from previous studies demonstrating rapid formation of carbonates via reaction of the mineral olivine with aqueous fluids rich in NaHCO{sub 3} (plus KHCO{sub 3} and RbHCO{sub 3}) and NaCl at a high partial pressure of CO{sub 2}. We wished to separate and quantify the effects of NaHCO{sub 3} and NaCl, and to investigate whether bicarbonate-rich, aqueous fluids would also cause rapid formation of carbonates via reaction with other minerals and rocks. Further, we wished to improve upon previous work by adding precise characterization of grain size distributions and surface area, and their changes as a result of reaction. We confirmed previous reports of very rapid olivine carbonation. We found that at a given temperature and CO{sub 2} partial pressure the previously observed rate enhancement in olivine carbonation is due mainly to NaHCO{sub 3}, and not to dissolved NaCl. Further, though reaction of the mineral plagioclase, and two rock compositions, were all faster in the presence of NaHCO{sub 3}-rich fluids, compared with saline and de-ionized water, they were all much slower than reaction of olivine. In the experiments showing the fastest reaction rate, average grain size tended to increase during experiments, presumably due to dissolution of small reactant grains plus growth of product phases on reactant surfaces. Porosity/surface area of grains tended to change with reaction progress, due to the formation of dissolution pits and irregular growth of product phases on reactant grain surfaces. Development of a passivating phase (e.g., a layer of silica) due to incongruent dissolution of solid reactants and/or precipitation of solid products was detected, but was relatively minor and did not have a discernable effect on reaction progress. Geomechanical experiments did not identify pressure-temperature-composition conditions under which porous olivine aggregates undergo reaction driven cracking. Little carbonate formed in these experiments. Though we fulfilled the milestones for this project, a variety of reasons for this remain to be investigated in the future. Reaction of porous olivine aggregates with brines rich in NaHCO{sub 3} caused substantial weakening of samples in compression, due to formation of dissolution pits along olivine-olivine grain boundaries, reducing the solid-solid surface area. A preliminary modeling study funded in part by this grant emphasized potential rate enhancements due to reaction-driven cracking. In related research, not funded by this grant, several additional experimental and modeling studies of reaction-driven cracking are underway.

  3. AGR-2 Final Data Qualification Report for U.S. Capsules - ATR Cycles 147A Through 154B

    SciTech Connect (OSTI)

    Pham, Binh T; Einerson, Jeffrey J

    2014-07-01

    This report provides the data qualification status of AGR-2 fuel irradiation experimental data in four U.S. capsules from all 15 Advanced Test Reactor (ATR) Cycles 147A, 148A, 148B, 149A, 149B, 150A, 150B, 151A, 151B, 152A, 152B, 153A, 153B, 154A, and 154B, as recorded in the Nuclear Data Management and Analysis System (NDMAS). Thus, this report covers data qualification status for the entire AGR-2 irradiation and will replace four previously issued AGR-2 data qualification reports (e.g., INL/EXT-11-22798, INL/EXT-12-26184, INL/EXT-13-29701, and INL/EXT-13-30750). During AGR-2 irradiation, two cycles, 152A and 153A, occurred when the ATR core was briefly at low power, so AGR-2 irradiation data are not used for physics and thermal calculations. Also, two cycles, 150A and 153B, are Power Axial Locator Mechanism (PALM) cycles when the ATR power is higher than during normal cycles. During the first PALM cycle, 150A, the experiment was temporarily moved from the B-12 location to the ATR water canal and during the second PALM cycle, 153B, the experiment was temporarily moved from the B-12 location to the I-24 location to avoid being overheated. During the Outage cycle, 153A, seven flow meters were installed downstream from seven Fission Product Monitoring System (FPMS) monitors to measure flows from the monitors and these data are included in the NDMAS database. The AGR-2 data streams addressed in this report include thermocouple (TC) temperatures, sweep gas data (flow rates including new FPM downstream flows, pressure, and moisture content), and FPMS data (release rates and release-to-birth rate ratios [R/Bs]) for each of the four U.S. capsules in the AGR-2 experiment (Capsules 2, 3, 5, and 6). The final data qualification status for these data streams is determined by a Data Review Committee comprised of AGR technical leads, Very High Temperature Reactor (VHTR) Program Quality Assurance (QA), and NDMAS analysts. The Data Review Committee, which convened just before each data qualification report was issued, reviewed the data acquisition process, considered whether the data met the requirements for data collection as specified in QA-approved VHTR data collection plans, examined the results of NDMAS data testing and statistical analyses, and confirmed the qualification status of the data as given in each report. This report performs the following tasks: (1) combine existing qualification status of all AGR-2 data, (2) provide FPMS data qualification update and new release-to-birth ratio (R/B) data calculated using daily calculated birthrates, and (3) revise data qualification status of TC readings for some TCs in Capsule 6 based on their differences relative to calculated temperatures at TC locations. A total of 17,001,695 TC temperature and sweep gas data records were received and processed by NDMAS for four U.S. capsules during AGR-2 irradiation. Of these records, 9,655,474 (56.8% of the total) were determined to be Qualified; 5,792,052 (34.1% of the total) were determined to be Failed; and 1,554,169 (9.1% of the total) were determined to be Trend. For the first nice cycles, from ATR Cycle 147A to 151B, data records are 5- minute or 10-minute averaged values provided on weekly basis in EXCEL spreadsheets. For the last six cycles, ATR Cycle 152A through 154B, data records are instantaneous measurements recorded every minute and provided by .csv text files automatically every 2 hours. Therefore, the number of processed irradiation data was increased substantially from ATR Cycle 152A. For TC temperature data, there were 6,857,675 records and of these data 5,288,249 records (77.1% of the total TC data) were Failed due to TC instrument failures and 418,569 records (6.1% of the total TC data) were Trend due to large differences between TC readings and calculated values. By the end of Cycle 154A, all TCs in the AGR-2 test train failed. The overall percentage of Failed TC records is high, to some extent, because TCs failed toward the end of irradiation when the recording frequency was higher. For sweep gas data, there were 10,1

  4. 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"

    U.S. 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,,100,95,122495,69041,120326,93234,54624,109729,118689,69742,107396,119799,68307,78398,7077,4459,86216,111744,65001,89393,128830,75618,81101,97034,56642,114450,105402,58755,119892,1050