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1

Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4  

U.S. Energy Information Administration (EIA) Indexed Site

Current Forecast: December 10, 2013; Previous Forecast: November 13, 2013 Current Forecast: December 10, 2013; Previous Forecast: November 13, 2013 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 2011 2012 2013 2014 2011-2012 2012-2013 2013-2014 U.S. Energy Supply U.S. Crude Oil Production (million barrels per day) Current 6.22 6.29 6.42 7.02 7.11 7.29 7.61 7.97 8.26 8.45 8.57 8.86 5.65 6.49 7.50 8.54 14.8% 15.6% 13.8% Previous 6.22 6.30 6.43 7.04 7.13 7.30 7.60 7.91 8.22 8.40 8.52 8.80 5.65 6.50 7.49 8.49 15.0% 15.2% 13.3% Percent Change 0.0% -0.1% -0.2% -0.2% -0.3% -0.1% 0.1% 0.7% 0.5% 0.5% 0.6% 0.6% 0.0% -0.1% 0.1% 0.6% U.S. Dry Natural Gas Production (billion cubic feet per day) Current 65.40 65.49 65.76 66.34 65.78 66.50 67.11 67.88 67.99 67.74 67.37 67.70 62.74 65.75 66.82 67.70 4.8% 1.6% 1.3% Previous 65.40 65.49 65.76 66.34 65.78 66.50 67.11 67.30 67.47 67.41 67.04 67.37 62.74 65.75 66.68 67.32

2

Bloo Solar formerly Q1 Nanosystems | Open Energy Information  

Open Energy Info (EERE)

Solar formerly Q1 Nanosystems Jump to: navigation, search Name: Bloo Solar (formerly Q1 Nanosystems) Place: West Sacramento, California Zip: 95691 Sector: Solar Product: String...

3

Domestic Coal Distribution 2009 Q1 by Origin State: Alabama  

U.S. Energy Information Administration (EIA) Indexed Site

Q1 by Origin State: Alabama Q1 by Origin State: Alabama (1000 Short Tons) 1 / 58 Domestic Coal Distribution 2009 Q1 by Origin State: Alabama (1000 Short Tons) Destination State Transportation Mode Electricity Generation Coke Plants Industrial Plants Excluding Coke Commercial & Institutional Total Alabama Railroad 950 4 84 - 1,038 Alabama River 1,110 - - - 1,110 Alabama Truck 37 170 249 - 456 Alabama Total 2,096 174 333 - 2,603 Florida Railroad - - 22 - 22 Georgia Railroad 45 - - - 45 Georgia Truck s - 20 - 21 Georgia Total 45 - 20 - 65 Hawaii Ocean Vessel s - - - s Indiana Railroad - 78 - - 78 Indiana Truck - 32 - - 32 Indiana Total - 110 - - 110 South Carolina Truck - - 2 - 2 Tennessee Truck - - 1 - 1 Texas Railroad 72 - - - 72 Origin State Total 2,213 284 378 - 2,875 Ocean Vessel s - - - s Railroad 1,066 82 106 - 1,255 River 1,110 - - - 1,110 Truck 37 202 272 - 511 2 / 58

4

FOIA Quarterly Reports (Q1 2013) | Department of Energy  

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

Q1 2013) Q1 2013) FOIA Quarterly Reports (Q1 2013) The DOE's mission is to advance the national, economic, and energy security of the United States; to promote scientific and technological innovation in support of that mission; and to ensure the environmental cleanup of the national nuclear weapons complex. The records maintained by the DOE often involve proprietary matters, classified matters, innovation matters, and environmental matters. The DOE invokes several of the FOIA's exemptions to protect information that is: classified as restricted data or formerly restricted data; proprietary; personal; and pre-decisional and deliberative. These types of information may not be granted under the FOIA to protect national security, proprietary interests of submitters; personal privacy of

5

Domestic Coal Distribution 2009 Q1 by Destination State: Alabama  

U.S. Energy Information Administration (EIA) Indexed Site

4 4 Domestic Coal Distribution 2009 Q1 by Destination State: Alabama (1000 Short Tons) 1 / 64 Domestic Coal Distribution 2009 Q1 by Destination State: Alabama (1000 Short Tons) Origin State Transportation Mode Electricity Generation Coke Plants Industrial Plants Excluding Coke Commercial & Institutional Total Alabama Railroad 950 4 84 - 1,038 Alabama River 1,110 - - - 1,110 Alabama Truck 37 170 249 - 456 Alabama Total 2,096 174 333 - 2,603 Arkansas Railroad - 6 - - 6 Colorado Railroad 279 - - - 279 Illinois Railroad 11 - - - 11 Illinois River 109 - - - 109 Illinois Total 119 - - - 119 Indiana River 197 - - - 197 Kentucky Railroad 442 - 28 - 471 Kentucky Truck - - 2 - 2 Kentucky Total 442 - 31 - 473 Kentucky (East) Railroad 357 - 28 - 385 Kentucky (East) Truck - - 2 - 2 Kentucky (East)

6

Next Generation Solar Collectors for CSP - FY13 Q1 | Department...  

Office of Environmental Management (EM)

Next Generation Solar Collectors for CSP - FY13 Q1 Next Generation Solar Collectors for CSP - FY13 Q1 This document summarizes the progress of this 3M project, funded by SunShot,...

7

Electric Field How does a charge, q1, exert a force on  

E-Print Network [OSTI]

Electric Field How does a charge, q1, exert a force on another charge, q2, when the charges don't touch? The charge, q1, sets up an electric field in its surrounding space This electric field has both magnitude and direction which determine the magnitude and direction of the force acting on q2 #12;Electric

Bertulani, Carlos A. - Department of Physics and Astronomy, Texas A&M University

8

Applicability of InSAR to tropical volcanoes: insights from Central AmericaQ1  

E-Print Network [OSTI]

volcanoes: insights from Central AmericaQ1 S. K. EBMEIER1*, J. BIGGS2,3, T. A. MATHER1 & F. AMELUNG3 1 COMET+, Department of Earth Sciences, University of Oxford, South Parks Road, Oxford OX1 3AN, UK 2 COMET+, Department rapid in southern Central America where Evergreen broad- leaf vegetation dominates. Land

Biggs, Juliet

9

Quarterly SSP Experiment Summary-FY13-1Q 1  

National Nuclear Security Administration (NNSA)

3-1Q 1 3-1Q 1 Summary of Experiments Conducted in Support of Stockpile Stewardship January 2013 The U.S. Stockpile Stewardship Program is a robust program of scientific inquiry used to sustain and assess the nuclear weapons stockpile without the use of underground nuclear tests. The experiments carried out within the program are used in combination with Advanced Simulation and Computing (ASC) to continually assess the stockpile to ensure it is safe, secure, and effective. (For links to the ASC program, see: http://nnsa.energy.gov/asc) For a link to the Nuclear Posture Review 2010, see: http://www.defense.gov/npr/docs/2010%20nuclear%20posture%20review%20report.pdf . An extraordinary set of science, technology, and engineering (ST&E) facilities have been established and are active everyday in support of the

10

2012-12-06 Quarterly SSP Experiment Summary-FY12-4Q 1  

National Nuclear Security Administration (NNSA)

2-12-06 Quarterly SSP Experiment Summary-FY12-4Q 1 2-12-06 Quarterly SSP Experiment Summary-FY12-4Q 1 Summary of Experiments Conducted in Support of Stockpile Stewardship October 2012 The U.S. Stockpile Stewardship Program is a robust program of scientific inquiry used to sustain and assess the nuclear weapons stockpile without the use of underground nuclear tests. The experiments carried out within the program are used in combination with Advanced Simulation and Computing (ASC) to continually assess the stockpile to ensure it is safe, secure, and effective. (For links to the ASC program, see: http://nnsa.energy.gov/asc) For a link to the Nuclear Posture Review 2010, see: http://www.defense.gov/npr/docs/2010%20nuclear%20posture%20review%20report.pdf . An extraordinary set of science, technology, and engineering (ST&E) facilities have been established and are active everyday in support of the

11

BPS M2-branes in AdS4Q1,1,1 and their dual loop operators  

Science Journals Connector (OSTI)

In this paper, we first compute the Killing spinors of AdS4Q1,1,1 and its certain orbifolds. Based on this, two classes of M2-brane solutions are found. The first class of solutions includes M2-branes dual to Wilson loops in the fundamental representation as a special case. The second class includes the candidates of the holographic description of vortex loops in the dual field theories.

Jun-Bao Wu and Meng-Qi Zhu

2014-06-05T23:59:59.000Z

12

"State","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Sep","Q3 Total","Oct","Nov","Dec","Q4 Total","2002 Total"  

U.S. Energy Information Administration (EIA) Indexed Site

Jun","Q2 Total","Jul","Aug","Sep","Q3 Total","Oct","Nov","Dec","Q4 Total","2002 Total" Jun","Q2 Total","Jul","Aug","Sep","Q3 Total","Oct","Nov","Dec","Q4 Total","2002 Total" "Alabama",1595069,1422595,1446039,4463703,1651900,1673270,1619686,4944856,1609758,1743418,1702481,5055657,1618031,1459125,1520148,4597304,19061520 "Alaska",132989,119164,123742,375895,111713,113169,109538,334420,76798,83175,78226,238199,80312,66775,50123,197210,1145724 "Arizona",1158076,1038925,1084980,3281981,1017804,1030975,974342,3023121,988049,1095624,1063939,3147612,1183635,1062729,1104980,3351344,12804058 "Arkansas",978,1085,2107,4170,1565,1582,1524,4671,636,689,971,2296,935,843,871,2649,13786 "Colorado",3163974,2824806,2885394,8874174,2997782,3036576,2869817,8904175,2629615,2915930,3075236,8620781,3004721,2814415,2884793,8703929,35103059

13

Chemical Engineering Science, Vol. 45, No. 7, pp. 1719-1731.1990. ooo9-2509/90 53.00 + 0.00 Printed in Grca~ Britain. Q 1wo Pergamon Press plc  

E-Print Network [OSTI]

in Grca~ Britain. Q 1wo Pergamon Press plc SIMULTANEOUS MOMENTUM, HEAT AND MASS TRANSFER WITH CHEMICAL

Aksay, Ilhan A.

14

2014_Q1.indd  

Energy Savers [EERE]

environmental analyses; complying with regulatory orders; responding to dangers to public health, safety, and the environment; and maintaining the lease tracts and their existing...

15

Fusion Rules of the Lowest Weight Representations of osp_q(1|2) at Roots of Unity: Polynomial Realization and Degeneration at Roots of Unity  

E-Print Network [OSTI]

The degeneracy of the lowest weight representations of the quantum superalgebra $osp_q(1|2)$ and their tensor products at exceptional values of %when deformation parameter $q$ takes exceptional values is studied. The main features of the structures of the finite dimensional lowest weight representations and their fusion rules are illustrated using realization of group generators as finite-difference operators acting in the space of the polynomials. The complete fusion rules for the decompositions of the tensor products at roots of unity are presented. The appearance of indecomposable representations in the fusions is described using Clebsh-Gordan coefficients derived for general values of $q$ and at roots of unity.

D. Karakhanyan; Sh. Khachatryan

2006-02-08T23:59:59.000Z

16

Q1 1998 STEO Docs  

Gasoline and Diesel Fuel Update (EIA)

8 (Released January 12, 1998) 8 (Released January 12, 1998) Energy Information Administration DOE/EIA-0202(98/1Q) Distribution Category UC-950 Short-Term Energy Outlook Quarterly Projections First Quarter 1998 Energy Information Administration Office of Energy Markets and End Use U.S. Department of Energy Washington, DC 20585 This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the U.S. Department of Energy. The information contained herein should be attributed to the Energy Information Administration and should not be construed as advocating or reflecting any policy position of the Department of Energy or any other organization. Energy Information Administration/Short-Term Energy Outlook --January 1998

17

FOIA Quarterly Reports (Q1-2014)  

Broader source: Energy.gov [DOE]

Report that captures quarterly FOIA data at the DOE level. Through the use of an Applied Programming Interface (or API), the information will display on www.FOIA.gov.

18

Microsoft Word - Issue FY2010 Q1 Draft 20091228.doc  

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

On October 5, 2009, On October 5, 2009, President Obama signed Executive Order (EO) 13514, Federal Leadership in Environmental, Energy, and Economic Performance. 1 This order represents a transformative shift in the way the government will operate by establishing greenhouse gas emissions (GHGs) as the integrating metric for tracking progress toward federal sustainability. The new order does not replace EO 13423, Strengthening Federal Environmental, Energy, and Transportation Management. Like previous orders, the new order relies heavily on effective real property asset management practices to achieve its goals. It provides new direction in these areas: * Stormwater, potable, industrial and landscaping water * Waste including recycling and composting * Integrated planning

19

9 Science Service FeaturQ 1 IHY THE FIEATHER ?  

E-Print Network [OSTI]

increases the wind velocity indoors; Systems of re- frigeration lover the temperature of cars Or buildings n moisture, Air driers o r moisteners i n operation night and day are not Cotton mills prefer, "condition11 t h e i r air and keep the windows shut, Modern mills now Lsather, too, may be injured by lack

20

System Advisor Model Enhancements for CSP- FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


21

Q1 Review Session Complex system fails for complex reasons!  

E-Print Network [OSTI]

interlocks -- protective circuits · Therac-25 · software shared code with Therac-20 · software interlock that, in practice, hardware interlocks are necessary for safety. · True. The authors discuss the need of radiation, contributed to the accidents. · True. Some of the accidents occurred when one part of the machine

22

NBB Enclosed Particle Receiver- FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

23

Advanced Manufacture of Reflectors- FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this University of Arizona project, funded by SunShot, for the first quarter of fiscal year 2013.

24

Quarterly SSP Experiment Summary-Q1FY14 1  

National Nuclear Security Administration (NNSA)

fundamental properties of material, plasma, radiation, fusion ignition, and thermonuclear burn at temperatures and pressures relevant to those obtained in a nuclear weapon....

25

"State","Jan","Feb","Mar","Q1 Total","Apr","May","Jun ","Q2 Total","Jul","Aug","Sep","Q3 Total","Oct","Nov","Dec","Q4 Total","2003 Total"  

U.S. Energy Information Administration (EIA) Indexed Site

3 Total" 3 Total" "Alabama",1771113,1510892,1622954,4904959,1863504,1845388,1776824,5485716,1600128,1565897,1672632,4838657,1763889,1479114,1734574,4977577,20206909 "Alaska",87443,76405,79754,243602,62928,62232,69581,194741,67907,66760,67789,202456,156990,131143,152391,440524,1081323 "Arizona",1073559,941887,1030496,3045942,943093,932681,884672,2760446,1040168,1016416,1058519,3115103,1107584,941831,1088188,3137603,12059094 "Arkansas",829,426,1561,2816,484,478,264,1226,442,432,494,1368,769,439,946,2154,7564 "Colorado",2846715,2541328,2830992,8219035,2865526,2903720,2827776,8597022,3131374,3268010,3269638,9669022,3014173,2950843,3381090,9346106,35831185 "Illinois",2961000,2440349,2876040,8277389,2706876,2702220,3169886,8578982,2373950,2388551,2344648,7107149,2993442,2346572,2456095,7796109,31759629

26

"State","Jan","Feb","Mar","Q1 Total","Apr","May","Jun ","Q2 Total","Jul","Aug","Sep","Q3 Total","Oct","Nov","Dec","Q4 Total","2004 Total"  

U.S. Energy Information Administration (EIA) Indexed Site

4 Total" 4 Total" "Alabama",1725998,1581616,2004066,5311680,1926051,1739300,2099141,5764492,1605125,1654151,1850943,5110219,1976865,2078720,2086665,6142250,22328641 "Alaska",140314,131982,185547,457843,61887,55405,120646,237938,131114,130814,96529,358457,149748,156396,151405,457549,1511787 "Arizona",977250,897698,1100939,2975887,1049375,950831,1069753,3069959,1098199,1113785,977716,3189700,1129140,1195127,1171016,3495283,12730829 "Arkansas",1133,1013,845,2991,679,692,1274,2645,411,400,432,1243,170,166,113,449,7328 "Colorado",3527103,3179582,3398625,10105310,3407363,3451070,3468743,10327176,3293260,3357952,3258228,9909440,3172777,3167266,3188128,9528171,39870097 "Illinois",2888652,2695556,3272892,8857100,2664839,2497528,2930733,8093100,2657588,2695324,2480874,7833786,2322429,2411032,2394081,7127542,31911528

27

Low-Cost Metal Hydride TES Systems- FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress for this Savannah Reiver National Laboratory project, funded by SunShot, for the first quarter of fiscal year 2013.

28

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total...  

U.S. Energy Information Administration (EIA) Indexed Site

"Arkansas",218,114,136,468,174,172,167,513,253,283,245,781,341,303,157,801,2563 "Colorado",3339797,3246183,3644547,10230527,3101948,3095295,3141507,9338750,3284972,3442912...

29

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total...  

U.S. Energy Information Administration (EIA) Indexed Site

901,5222,5790,16913,6096,6383,6653,19132,8430,9527,8169,26126,5636,7084,7786,20506,82677 "Colorado",2732284,2480711,2775220,7988215,3264406,3408511,3417513,10090430,2999471,3278170...

30

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total...  

U.S. Energy Information Administration (EIA) Indexed Site

7135,7446,22132,3555,3697,3686,10938,9304,10021,8613,27938,12782,12327,12004,37113,98121 "Colorado",2551829,2353617,2123193,7028639,2286316,2208508,2390122,6884946,2544298,2770090,...

31

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total...  

U.S. Energy Information Administration (EIA) Indexed Site

611611,596681,1843797,3813909 "Arkansas",5862,5366,5865,17093,8039,7743,7457,23239,40332 "Colorado",1750313,1873107,1653903,5277323,2284260,1942356,2289442,6516058,11793381...

32

Table 1. Questions Q1, gender 1 = male, 2 = female. (3 occurences of "Not  

E-Print Network [OSTI]

on AoC compared to exercises in other courses" Likert scale where 1 = Strongly Agree, 2 = Somewhat Agree value 3). Q7, "AoC is more motivating than a traditional set of exercises" Likert scale as for Q5. Q9, "I perceive the learning effect by using AoC as good compared to traditional exercises Likert scale

Natvig, Lasse

33

Microsoft Word - fy09_annualtarget_climatemodeling1_Q1 _2_.doc  

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

WD, Bitz CM, Blackmon ML, Bonan GB, Bretherton CS, Carton JA, Chang P, Doney SC, Hack JJ,Henderson TB (2006) The Community Climate System Model Version 3 (CCSM3). Journal of...

34

Q1Report for CADWR Project: Desalination Using Carbon NAnotube Membranes  

SciTech Connect (OSTI)

In this research and development project, LLNL will leverage the process for fabrication of the membranes developed by our internally funded effort (LLNL Laboratory Directed Research and Development). LLNL will then employ chemical manipulations to modify charge at the ends of the nanotubes and make the membranes more selective to either positive or negative ions through a combination of size and charge selectivity. LLNL's goal is to demonstrate ion exclusion while preserving high permeabilities and low energy use. Success of this research and development project may warrant further developments in the fabrication of membranes.

Bakajin, O

2008-05-14T23:59:59.000Z

35

FY14-Q1 1.2.1.3.ML.1 INL Biomass Feeding Survey Report  

SciTech Connect (OSTI)

Approximately 20 institutions were contacted by telephone and/or electronic mail and requested to provide responses to a survey on feeding biomass feedstock materials. Fourteen individuals responded. Responses from the participants, including information that was offered in addition to answers to the survey questions are summarized in this report, which fully meets the requirements of the milestone.

Tyler L. Westover

2014-04-01T23:59:59.000Z

36

High Efficiency Thermal Energy Storage System for CSP- FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress for this Argonne National Laboratory project, funded by SunShot, for the first quarter of fiscal year 2013.

37

High Operating Temperature Heat Transfer Fluids for Solar Thermal Power Generation FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this UCLA project, funded by the SunShot CSP Multidisciplinary University Research Initiative, for the first quarter of fiscal year 2013.

38

Low-Cost Heliostat for Modular Systems- FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

39

Corrosion Studies in High-Temperature Molten Salt Systems for CSP Applications- FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this Savannah River National Laboratory project, funded by SunShot, for the first quarter of fiscal year 2013.

40

High-Temperature Thermal Array for Next Generation Solar Thermal Power Production- FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this Los Alamos National Laboratory project, funded by SunShot, for the first quarter of fiscal year 2013.

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


41

Low-Cost, Lightweight Solar Concentrators - FY13 Q1 | Department...  

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

More Documents & Publications Low-Cost, Lightweight Solar Concentrators FY13 Q2 Low-Cost, Lightweight Solar Concentrator Low-Cost Light Weigh Thin Film Solar Concentrators...

42

Baseload CSP Generation Integrated with Sulfur-Based Thermochemical Heat Storage- FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this General Atomics project, funded by SunShot, for the first quarter of fiscal year 2013.

43

1Q1 Mathematics for Engineers and Scientists Lecturer: Professor Paul Glendinning  

E-Print Network [OSTI]

this as understood. #12;3.8 Integration by parts Stroud P15 Integrate the product formula of dierentiation: (uv)H = uHv + uvH to get Z (uv)Hdx = Z uHv dx + Z uvHdx Now, by the Fundamental Theorem of Calculus the left hand side is just [uv] so [uv] = Z uHv dx + Z uvHdx or Z uvHdx = [uv] Z uHv dx This is the formula

Glendinning, Paul

44

The neutron electric form factor to Q = 1.45 (GeV/c)  

E-Print Network [OSTI]

The nucleon elastic electromagnetic form factors are fundamental quantities needed for an understanding of nucleon and nuclear electromagnetic structure. The evolution of the Sachs electric and magnetic form factors with ...

Plaster, Bradley R. (Bradley Robert), 1976-

2004-01-01T23:59:59.000Z

45

FY14 Q1 Progress Report for SECA Core Technology Program  

SciTech Connect (OSTI)

This quarterly progress report was prepared under field work proposal (FWP) 40552 and covers technical work performed during the period October 1 through December 31, 2013 (FY14 1st quarter). The report highlights and documents technical progress and milestone status in tasks related to advanced cell and stack component materials development and computational design and simulation. Technical highlights related to cell and stack materials development and characterization include: Surface modified, Ce-modified MC spinel-coated AISI 441 exhibited improved spallation resistance (compared to coated mill reference 441) after 30,000 hours of oxidation at 800C in air. Similar beneficial results from surface modification were observed after 26,000 hours of oxidation at 850C. MnCo spinel coatings prepared from metallic powder precursors exhibited low area-specific resistance after 12,000 hours of testing at 800C. Long-term validation tests (6,000 hours of operation followed by 10 deep thermal cycles) of surface-blasted, spinel-coated AISI 441 interconnects were completed using PNNLs SECA CTP stack test fixture. Results of post-test results will be reported in the next quarterly progress report. Long-term evaluation of compliant glass seals (SCN-1 glass with YSZ fibers) was in progress using PNNLs SECA CTP stack test fixture. Baseline testing of LSCF-based cells from Fuel Cell Materials was performed in PNNLs SECA CTP stack test fixture. Overall performance was similar to that previously obtained with similar cells from H.C. Starck. A study on pore coarsening of compliant glass seals with and without inert fillers (ZrO2 short fibers or ZrO2 crushed hollow balls) has reached 2,000 hours of testing; results to date indicate that the addition of the fillers was partially effective in hindering the pore coalescence process. Cell tests attempting to correlate effects of fuel water content on anode performance with previously observed changes in Ni/YSZ anode microstructure were initiated. Technical highlights in the computational modeling area include: A method to interface the 3D SOFC-MP modeling tool with commercial FEA codes ABAQUS and ANSYS was developed to facilitate model construction and output of the predicted temperature field for structural stress analyses of stacks. The error estimation and verification tools of the reduced order modeling (ROM) framework was improved to facilitate error handling for a large number of cases and perform user-specified test cases for error analysis of the generated ROM. Mechanical behavior and damage characteristics of the compliant glass seal was investigated for a large planar cell design under different realistic electrochemical operating conditions (as predicted using SOFC-MP 3D) and thermal cycling events. The methodology for lifetime prediction of the interconnect was improved to include the mechanical influence of the spinel protection coating on the prediction of critical scale thickness. 3 Experimental characterization of the crack healing rate was performed for compliant glass SCN-1 with various amounts of fiber reinforcement. This information is needed for modeling evaluations of compliant seal healing during stack operations.

Stevenson, Jeffry W.; Koeppel, Brian J.

2014-01-31T23:59:59.000Z

46

DOE/EIA-0202|83/2Q)-1 Short-Term Energy Outlook  

Gasoline and Diesel Fuel Update (EIA)

ministration (EIA), Office of Energy Markets and End Use, under the direc tion "of Wray Smith (202252-1617). General supervision is provided by W. Calvin Kilgore (202252-1130),...

47

Quarterly SSP Experiment Summary-FY13-1Q 1  

National Nuclear Security Administration (NNSA)

fundamental properties of material, plasma, radiation, fusion ignition, and thermonuclear burn at temperatures and pressures relevant to those obtained in a nuclear weapon....

48

Microsoft Word - DE-FE0010160 Q1 report.doc  

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

Oil & Natural Gas Technology Oil & Natural Gas Technology DOE Award No.: DE-FE0010160 Quarterly Research Performance Progress Report (Period ending 12/31/2012) Advanced Hydrate Reservoir Modeling Using Rock Physics Techniques 10/1/2012 - 9/30/2013 Submitted by: Principal Investigator: Dan McConnell Fugro GeoConsulting, Inc. DUNS #: 118972301 6100 Hillcroft Ave., 3 rd Floor Houston, TX 77081 e-mail: dmcconnell@fugro.com Phone number: (713) 778-6801 Prepared for: United States Department of Energy National Energy Technology Laboratory January 31, 2013 Executive Summary This research effort will focus on developing and refining techniques that integrate rock physics modeling, amplitude analysis, and spectral decomposition to characterize complex gas hydrate reservoirs. The

49

acs_cm_cm-2009-03769q 1..3  

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

pubs.acs.org/cm pubs.acs.org/cm Published on Web 02/16/2010 r 2010 American Chemical Society Chem. Mater. 2010, 22, 1943-1945 1943 DOI:10.1021/cm903769q Universal and Solution-Processable Precursor to Bismuth Chalcogenide Thermoelectrics Robert Y. Wang, † Joseph P. Feser, ‡ Xun Gu, § Kin Man Yu, † Rachel A. Segalman, †,§ Arun Majumdar, †,‡ Delia J. Milliron,* ,† and Jeffrey J. Urban* ,† † Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, ‡ Department of Mechanical Engineering, and § Department of Chemical Engineering, University of California, Berkeley, California 94720 Received December 15, 2009 Revised Manuscript Received February 7, 2010 Thermoelectric materials convert thermal power into electrical power and vice versa. In practice, thermoelectric coolers and power generators are made by alternately

50

MSSV FAQ 2013-14 Q1 How close is Murano to the University?  

E-Print Network [OSTI]

a kitchen with a cooker, fridge/freezer, microwave, toaster and kettle. Each large flat (10/12 persons) has a #12;kitchen with 2 cookers, 2 fridges and freezers, microwave, kettle, toaster. Ironing equipment

Glasgow, University of

51

Berechenbarkeitstheorie Ralf Schindler  

E-Print Network [OSTI]

Tafel (eine Matrix) der Gr¨o?e n · m wiedergegeben werden, wobei n die Zahl der Element von Q und m die ¨Ubergangsfunktion : Q ? Q durch folgende Tafel gegeben sein. 0 1 q0 q1 q2 q1 q2 q3 q2 q3 q3 q3 q3 q3 Die

Schindler, Ralf

52

Berechenbarkeitstheorie Ralf Schindler  

E-Print Network [OSTI]

endlicher Automat, A = (Q, #, #, q 0 , F ). Dann kann # auch durch eine Tafel (eine Matrix) der Gr? o?e n ? Ubergangsfunktion # : Q? # # Q durch folgende Tafel gegeben sein. 0 1 q 0 q 1 q 2 q 1 q 2 q 3 q 2 q 3 q 3 q 3 q 3 q

Schindler, Ralf

53

Microsoft PowerPoint - DOE Supplemental Instructions for OMB Section 1512 Reporting Contractors Q1 2010 [Compatibility Mode]  

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

Contractors Contractors 1 For Contractors Quarterly reporting through FederalReporting.gov April 2010 April 2010 Reporting Timeline Date Action Ongoing Registration open for FederalReporting.gov. Early registration is encouraged. April 1, 2010 Reporting Period Begins April 16, 2010 Reporting Period Ends - No new reports can be entered after 11:59 PM PDT on this date. NOTE: Reporting deadline was extended. April 17, 2010 Prime Recipient Review begins- Only corrections to existing reports can be made. April 19, 2010 Prime Recipient Review ends- No updates may be made after 11:59 PM PDT on this date without DOE Reviewer action. April 20, 2010 Federal review of data begins -Recipients may be contacted to answer 2 April 20, 2010 Federal review of data begins -Recipients may be contacted to answer

54

Microsoft PowerPoint - DOE Supplemental Instructions for OMB Section 1512 Reporting Grant and Loan Recipients Q1 2010 [Compati  

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

Grant and Loan Recipients Grant and Loan Recipients | 1 For Grant and Loan Recipients Quarterly reporting through FederalReporting.gov April 2010 April 2010 Reporting Timeline Date Action Ongoing Registration open for FederalReporting.gov. Early registration is encouraged. April 1, 2010 Reporting Period Begins April 16, 2010 Reporting Period Ends - No new reports can be entered after 11:59 PM PDT on this date. NOTE: Reporting deadline was extended. April 17, 2010 Prime Recipient Review begins- Only corrections to existing reports can be made. April 19, 2010 Prime Recipient Review ends- No updates may be made after 11:59 PM PDT on this date without DOE Reviewer action. For more information, contact DOE at: https://recoveryclearinghouse.energy.gov or 1-888-363-7289 or go to: http://www.FederalReporting.gov

55

Q1. Who is Healthyroads? Healthyroads is our wellness program provider. The university selected Healthyroads from a  

E-Print Network [OSTI]

.com to sign up. Q6. What's this about a wellness rebate? A. To encourage employees and their spouses're making it worth your time with a rebate of up to $600 for you, and $600 for your spouse, for a total of up to $1,200. #12;Q7. What does earning a rebate "up to $600" mean? How is it paid to us? The rebate

Pantaleone, Jim

56

Chemical Communications c2cc30957b Q1Hypergolic ionic liquids to mill, suspend, and ignite  

E-Print Network [OSTI]

of nanoscale additives to improve EIL properties, such as energetic density and heat of combustion, while to their practical use such as low density5 and relatively low heats of combustion6 when compared to the current

Anderson, Scott L.

57

Q1, gender 1 = male, 2 = female. (1 occurence of "Not answered" (0) changed to median value 1).  

E-Print Network [OSTI]

, average time per week used on AoC 1 = less than 1 hour, 2 = 1-3 hours, 3 = 3-5 hours, 4 = 5-7 hours, 5 = more than 7 hours Q4, "Compared with an average student in the course I used ... on AoC" 1 = much less would definitely benefit from using a system like AoC" followed Likert scale where 1 = strongly disagree

Natvig, Lasse

58

2 Photosystem II and the unique role of bicarbonate: A historical perspective 3 DmitriyQ1 Shevela a,  

E-Print Network [OSTI]

of Illinois at Urbana-Champaign, 265 Morrill Hall, 505 South Goodwin Avenue, Urbana, IL 61801, USA 10 g Center). We end this review by discussing the uniqueness of bi- 44carbonate's role in oxygenic photosynthesis and its role in the evolutionary development of O2-evolving PSII. This 45article is part of a Special

Govindjee

59

Degradation Mechanisms and Development of Protective Coatings for TES and HTF Containment Materials- F13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this NREL project, funded by SunShot, for the first quarter of fiscal year 2013.

60

Prova Scritta di Robotica I 4 Dicembre 2006  

E-Print Network [OSTI]

cartesiane ammesse sono pari a Vmax = 1 m/s e, rispettivamente, Amax = 4 m/s2 . Determinare la legge oraria A4(q3, q4) = 2 R4(q3, q4) 0 Nc4 q3 + Ns4 0T 1 1 A4(q2, q3, q4) = 1 R4(q2, q3, q4) s2(q3 + Ns4) -c2(q3 + Ns4) Nc4 0T 1 0 A4(q1, q2, q3, q4) = 0 R4(q1, q2, q3, q4) Mc1 + c1s2(q3

De Luca, Alessandro

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


61

J. theor. Biol. (1997) 189, 171174 00225193/97/220171 + 04 $25.00/0/jt970503 7 1997 Academic Press Limited  

E-Print Network [OSTI]

with regard to their statistical #12;p1 5' -- 3' -- C( ) q3 p2 -- -- C( ) q2 p3 -- -- C( ) q1 -- -- 3' 5' A

Michel, Christian

62

FOIA Quarterly Reports (Q3 2013) | Department of Energy  

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

Q3 2013) Q3 2013) FOIA Quarterly Reports (Q3 2013) The DOE's mission is to advance the national, economic, and energy security of the United States; to promote scientific and technological innovation in support of that mission; and to ensure the environmental cleanup of the national nuclear weapons complex. The records maintained by the DOE often involve proprietary matters, classified matters, innovation matters, and environmental matters. The DOE invokes several of the FOIA's exemptions to protect information that is: classified as restricted data or formerly restricted data; proprietary; personal; and pre-decisional and deliberative. These types of information may not be granted under the FOIA to protect national security, proprietary interests of submitters; personal privacy of

63

Lone Star I (Q3) Wind Farm | Open Energy Information  

Open Energy Info (EERE)

I (Q3) Wind Farm I (Q3) Wind Farm Jump to: navigation, search Name Lone Star I (Q3) Wind Farm Facility Lone Star I (Q3) Sector Wind energy Facility Type Commercial Scale Wind Facility Status In Service Owner Horizon Developer RES/Horizon Energy Purchaser Direct Energy Location Callahan and Shackelford counties TX Coordinates 32.594885°, -99.506464° Loading map... {"minzoom":false,"mappingservice":"googlemaps3","type":"ROADMAP","zoom":14,"types":["ROADMAP","SATELLITE","HYBRID","TERRAIN"],"geoservice":"google","maxzoom":false,"width":"600px","height":"350px","centre":false,"title":"","label":"","icon":"","visitedicon":"","lines":[],"polygons":[],"circles":[],"rectangles":[],"copycoords":false,"static":false,"wmsoverlay":"","layers":[],"controls":["pan","zoom","type","scale","streetview"],"zoomstyle":"DEFAULT","typestyle":"DEFAULT","autoinfowindows":false,"kml":[],"gkml":[],"fusiontables":[],"resizable":false,"tilt":0,"kmlrezoom":false,"poi":true,"imageoverlays":[],"markercluster":false,"searchmarkers":"","locations":[{"text":"","title":"","link":null,"lat":32.594885,"lon":-99.506464,"alt":0,"address":"","icon":"","group":"","inlineLabel":"","visitedicon":""}]}

64

FY 2014 Metric Summary | Department of Energy  

Office of Environmental Management (EM)

4 Metric Summary FY 2014 Metric Summary FY 2014 Q1 Metric Summary.pdf FY 2014 Q2 Metric Summary.pdf FY 2014 Q3 Metric Summary.pdf More Documents & Publications FY 2014 Q3 Metric...

65

High-Efficiency Low-Cost Solar Receiver for Use in a Supercritical CO2 Recompression Cycle- FY13 Q1  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this Brayton Energy project, funded by SunShot, for the fist quarter of fiscal year 2013.

66

OFFICE OF THE CHIEF INFORMATION OFFICER (OCIO)  

Office of Environmental Management (EM)

Security. (FY 12 Q4 - FY 13 Q3) One GS-13 employee is participating in the NDU 14-week Advanced Management Program. (FY 12 Q4 - FY 13 Q1) The OCIO strives to ensure supervisors,...

67

Domestic Uranium Production Report - Quarterly - Energy Information  

U.S. Energy Information Administration (EIA) Indexed Site

All Nuclear Reports All Nuclear Reports Domestic Uranium Production Report - Quarterly Data for 3rd Quarter 2013 | Release Date: October 31, 2013 | Next Release Date: February 2014 | full report Previous Issues Year: 2013-Q2 2013-Q1 2012-Q4 2012-Q3 2012-Q2 2012-Q1 2011-Q4 2011-Q3 2011-Q2 2011-Q1 2010-Q4 2010-Q3 2010-Q2 2010-Q1 2009-Q4 2009-Q3 2009-Q2 2009-Q1 2008-Q4 2008-Q3 2008-Q2 2008-Q1 Go 3rd Quarter 2013 U.S. production of uranium concentrate in the third quarter 2013 was 1,171,278 pounds U3O8, down 16 percent from the previous quarter and up 12 percent from the third quarter 2012. Third quarter 2013 uranium production is at its highest level since 1999. During the third quarter 2013, U.S. uranium was produced at six U.S. uranium facilities. U.S. Uranium Mill in Production (State)

68

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Year total  

U.S. Energy Information Administration (EIA) Indexed Site

Year total" Year total" "Alabama",1562473,1400113,1447708,4410294,1592661,1584520,1474279,4651460,9061754 "Alaska",102639,95553,102206,300398,151343,155955,134279,441577,741975 "Arizona",626131,579206,619554,1824891,748419,751109,684147,2183675,4008566 "Arkansas",1344,1241,1331,3916,572,572,538,1682,5598 "Colorado",2049961,1815249,1916126,5781336,1708460,1651160,1937762,5297382,11078718 "Illinois",4897036,4449010,4664902,14010948,4596761,4692289,4224673,13513723,27524671 "Indiana",3304230,2985013,3132637,9421880,3242977,3260643,3012840,9516460,18938340 "Kansas",1589,1462,1564,4615,1627,1605,1527,4759,9374 "Kentucky Total",7194068,6511926,6926423,20632417,7065146,7169716,6488303,20723165,41355582

69

The Mathieu group M12 and the M13 game  

E-Print Network [OSTI]

). The permutation induced by the entire path is (0 8)(7 12) (1 8)(4 9) (1 12)(5 10) (6 12)(3 9) (0 6)(4 5) = (1 7 12 6 8)(3 4 10 5 9). Two paths are called equivalent if they induce the same permutation. We readily check that if p, q, r are collinear..., the points q1, q2, q3, q4 form an oval. Thus we may adopt the labelling (2.1), with q5 = q1q2 ? q3q4 = r1, q6 = q1q3 ? q2q4 = r2, y = s12. If s12 = 0, then the paths [s12, r2, s23] and [s12, r3, r1, s14] induce the permuta- tions ? = (s12 s23 r2)(r3 s34)(r1 s...

Conway, John H.; Elkies, Noam D.; Martin, Jeremy L.

2006-01-01T23:59:59.000Z

70

Shielded Payload Containers Will Enhance the Safety and  

E-Print Network [OSTI]

Drop Test #12;End Drop Test Results · Pre- and post-drop position of SCAs and radial shock absorber configuration in HalfPACT under current design and licensing bases: - 7,600 lb max payload - 30 watts max decay Q-2 Q-3 Q-4 Q-1 Q-2 Q-3 Q-4 2007 2008 2009 Engineering and testing Stakeholder meeting 11/29/07 EPA

71

Joint Top-K Spatial Keyword Query Processing Dingming Wu, Man Lung Yiu, Gao Cong, and Christian S. Jensen, Fellow, IEEE  

E-Print Network [OSTI]

-8200 Aarhus, Denmark. E-mail: csj@cs.au.dk p1 q3 q1 {pizza, grill} {curry, sushi}{curry, seafood} Q p3 p2 q2 {sushi, soup, curry} {seafood, grill, sushi} {seafood, sushi} p4 {soup, steak} Q Fig. 1. Top1 prefers `curry' and `sushi,' user q2 prefers `seafood' and `sushi,' and user q3 prefers `curry

Yiu, Man Lung

72

Warm water occupancy by North Sea cod  

Science Journals Connector (OSTI)

...Southern Bight), 963, 861 (German Bight), 3443 (Flamborough), 10401 (Eastern...the year (Q) for cod from the Southern Bight and west Shetland. region Q1 Q2 Q3 Q4...Gillibrand1996Hydrography of the East Shetland Basin in relation to decadal North Sea variability...

2007-01-01T23:59:59.000Z

73

After starting with a 12,000-job bang in 2010-Q2, Connecticut's  

E-Print Network [OSTI]

Sales -0.1% State Exports -2.9% Personal Income (est.) +3.2% Coincident GDI +0.6% Indicators of Future GDI +4.1% TAKING STOCK 'TIS THE SEASON? -10 -8 -6 -4 -2 0 2 4 6 8 Retail Construction Q4Q3Q2Q1 CT JOBS

Holsinger, Kent

74

Download Full-text PDF  

Science Journals Connector (OSTI)

tracer of terrigenous dissolved organic carbon in river-influenced ocean margins ..... values: M 5 median, Q1 5 first quartile, Q3 5 third quartile, and whiskers are set at 6 1.53 ..... Leanne Powers and the crews of the R/V Cape Hatteras and the.

2012-08-06T23:59:59.000Z

75

2014_Q3.indd  

Energy Savers [EERE]

continue monitoring the region very closely." LM is currently assessing the best way to repair the damage that occurred to the mud pit caps and is scheduled to conduct biological...

76

Effect of unsteady wake passing frequency on boundary layer transition on the concave surface of a curved plate  

E-Print Network [OSTI]

for Q= 0. 0 (O-rods), 1. 033 (3-rods), 1. 725 (5-rods), 3A43 (10-rods), 5. 166 (15-rods). . 82 Figure 23. Ensemble-averaged velocity traces for Q = 1. 003 at different s/s. with t/r as parameter Figure 24. Ensemble-averaged velocity traces for Q = 1.... 725 at different s/s, with t/r as parameter Figure 25. Ensemble-averaged velocity traces for Q = 3. 443 at different s/s, with t/~ Page 83 89 as parameter Figure 26. Ensemble-averaged velocity traces for Q = 5. 166 at different s/s, with t/r...

Read, Robert Kevin

2012-06-07T23:59:59.000Z

77

Slide 1  

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

Kassianov Kassianov Aerosol remote sensing under partly cloudy conditions: How well are we doing? Background Ground-based/airborne lidar observations: Raman Lidar (RL), Micropulse Lidar (MPL) High Spectral Resolution Lidar (HSRL) Can they be extended by other observations? Outline Q1: Why it is important? Q2: What issues do we have? Q3: How can we address them? Q1: IAE and Aerosol RF Simultaneous and coincident measurements of aerosol and cloud properties are desirable: Indirect Aerosol Effects (IAEs) Aerosol Radiative Forcing (RF) Ghan and Schwartz, BAMS, 2007 Myhre et al., ACP, 2009 Q1: Occurrence Partly cloudy sky: 30% (SGP), 40-80% (TWP) Credit: C. Long Q2: 3D Problem Examples of 3D Cloud Impacts: Positive Cloud Radiative Forcing (RF) Reflectance Enhancement Cloud Screening Q2: Positive Cloud RF

78

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Se  

U.S. Energy Information Administration (EIA) Indexed Site

89641,1665248,1813673,5268562,1605603,1418925,1574797,4599325,1560226,1520979,1548087,4629292,1595758,1512352,1566079,4674189,19171368 89641,1665248,1813673,5268562,1605603,1418925,1574797,4599325,1560226,1520979,1548087,4629292,1595758,1512352,1566079,4674189,19171368 "Alaska",157348,149707,163004,470059,165229,146865,163558,475652,126370,123922,126533,376825,179973,172560,185294,537827,1860363 "Arizona",615155,578338,629726,1823219,607331,529736,589913,1726980,684161,661439,675382,2020982,662176,605888,634784,1902848,7474029 "Arkansas",1368,1265,1373,4006,44,42,49,135,75,63,73,211,100,84,102,286,4638 "Colorado",2598599,2398691,2624231,7621521,2480199,2301680,2410596,7192475,2455799,2551386,2458359,7465544,2080422,1958496,1948749,5987667,28267207 "Illinois",2808999,2634005,2873292,8316296,3159879,2871581,3122311,9153771,2831358,2822706,2817902,8471966,2751380,2615582,2712181,8079143,34021176

79

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Se  

U.S. Energy Information Administration (EIA) Indexed Site

590156,1549121,1890240,5029517,1837008,1612832,1817764,5267604,1748827,1836260,1829250,5414337,1492063,1580746,1611253,4684062,20395520 590156,1549121,1890240,5029517,1837008,1612832,1817764,5267604,1748827,1836260,1829250,5414337,1492063,1580746,1611253,4684062,20395520 "Alaska",169145,171367,209428,549940,173925,153851,175804,503580,157110,166999,164746,488855,199224,205990,203505,608719,2151094 "Arizona",570518,563089,688183,1821790,656991,574518,646273,1877782,632198,671964,662911,1967073,683134,705482,697016,2085632,7752277 "Arkansas",61,21,38,120,21,20,42,83,2070,2222,2243,6535,8094,8775,8694,25563,32301 "Colorado",2322065,2187158,2595450,7104673,2124653,2012449,1834574,5971676,1808658,1912885,2451386,6172929,2126637,1895802,1890809,5913248,25162526 "Illinois",2562464,2507353,3029909,8099726,2908053,2654999,2859539,8422591,2736555,2873367,2839818,8449740,2744642,2850172,2897794,8492608,33464665

80

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Se  

U.S. Energy Information Administration (EIA) Indexed Site

55341,1681343,1892574,5329258,1658658,1670531,1742534,5071723,1410575,1654603,1555258,4620436,1414541,1475429,1469622,4359592,19381009 55341,1681343,1892574,5329258,1658658,1670531,1742534,5071723,1410575,1654603,1555258,4620436,1414541,1475429,1469622,4359592,19381009 "Alaska",192973,186567,214662,594202,157877,160560,166491,484928,147331,177894,166088,491313,191081,196389,191013,578483,2148926 "Arizona",642124,620818,714289,1977231,669838,675081,709437,2054356,609976,734758,686039,2030773,676671,695481,676430,2048582,8110942 "Arkansas",11974,11580,13334,36888,13213,13591,14398,41202,7961,9719,9086,26766,9411,9673,9407,28491,133347 "Colorado",1929471,1900070,2298696,6128237,2283478,1810220,2149953,6243651,2060280,2721721,2820414,7602415,2775211,1986851,2153267,6915329,26889632 "Illinois",2989525,2827862,3153966,8971353,2967621,3035216,3035405,9038242,3187769,3653573,3443141,10284483,3162324,3233725,3247382,9643431,37937509

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


81

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Se  

U.S. Energy Information Administration (EIA) Indexed Site

72722,1652685,1998911,5524318,1471117,1597213,1449134,4517464,1423501,1603213,1457981,4484695,1605882,1508880,1380680,4495442,19021919 72722,1652685,1998911,5524318,1471117,1597213,1449134,4517464,1423501,1603213,1457981,4484695,1605882,1508880,1380680,4495442,19021919 "Alaska",114843,99176,120137,334156,121810,134985,129878,386673,99616,112621,101599,313836,138523,130333,121502,390358,1425023 "Arizona",716328,607106,761870,2085304,550294,596655,802028,1948977,665397,763415,690796,2119608,735514,692009,634843,2062366,8216255 "Arkansas",1133,1091,1358,3582,363,400,3739,4502,1808,2040,1864,5712,2692,2525,3739,8956,22752 "Colorado",2387855,2081513,2450873,6920241,3801879,3949839,2602952,10354670,3080487,3253632,3429159,9763278,3286901,3017466,2979227,9283594,36321783 "Illinois",2785216,2462110,2950202,8197528,2491704,2687396,2573207,7752307,2694833,2967093,2729343,8391269,2968605,2766731,2652360,8387696,32728800

82

state","Jan","Feb","Mar","Q1 Total","Apr","May","Jun","Q2 Total","Jul","Aug","Se  

U.S. Energy Information Administration (EIA) Indexed Site

37013,1847191,1852958,5637162,1679453,1697484,1543327,4920264,1696796,1671906,1699481,5068183,1984467,1700253,1847148,5531868,21157477 37013,1847191,1852958,5637162,1679453,1697484,1543327,4920264,1696796,1671906,1699481,5068183,1984467,1700253,1847148,5531868,21157477 "Alaska",129329,125265,125952,380546,108802,109831,102313,320946,107919,106795,108897,323611,161955,136692,153265,451912,1477015 "Arizona",666141,615518,614586,1896245,554503,559721,651658,1765882,787471,774751,790062,2352284,723180,613209,674173,2010562,8024973 "Arkansas",4995,4715,4674,14384,5556,5604,3913,15073,5154,5056,5144,15354,8839,7448,8083,24370,69181 "Colorado",2775379,2662914,2807565,8245858,2749564,2843044,2837128,8429736,2646860,2778764,2672384,8098008,2586749,2325481,2342628,7254858,32028460 "Illinois",2630380,2533189,2580968,7744537,2648952,2698785,2302695,7650432,2901260,2937658,2923435,8762353,3168268,2775871,2973000,8917139,33074461

83

Applications of the LM392 Comparator Op Amp IC  

E-Print Network [OSTI]

Applications of the LM392 Comparator Op Amp IC The LM339 quad comparator and the LM324 op amp operation and ease of use has contributed to the wide range of applications for these devices. The LM392 FIGURE 1. 00749302 Q1, Q2, Q3 = 2N2369 Q4 = 2N2907 C1, A1 = LM392 amplifier-comparator dual *1% metal

Lanterman, Aaron

84

Second Quarter 2014 Volume 7, number 2  

E-Print Network [OSTI]

.5% in Q2, 4.1% in Q3, and 2.6% in Q4. March projections for annual average real GDP provided. The Bureau of Economic Analysis (BEA) reports U.S. real GDP expanded at an annual rate of 1.1% in Q1 2013, 2 coincides with positive signals from the market--accelerating GDP growth, employment gains, and rebounding

85

LLQR-2012-Q3.pdf  

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

2 2 September 5, 2012; Issue no. 72 NEPA Lessons Learned September 2012 1 Secretary Chu: Integrate Project Management with NEPA To Improve Decision Making "I cannot overstate the importance of integrating the NEPA compliance process with program and project management and of applying best management practices to NEPA compliance in DOE," said Secretary of Energy Steven Chu in a June 12, 2012, memorandum on Improved Decision Making through the Integration of Program and Project Management with National Environmental Policy Act Compliance. He reminded DOE officials that NEPA compliance is a "pre-requisite to successful implementation of DOE programs and projects" and that "the NEPA process is a valuable planning tool and provides an opportunity to improve the quality of DOE's

86

Q3 1997 STEO, Final  

Gasoline and Diesel Fuel Update (EIA)

7 (Released July 8, 1997) 7 (Released July 8, 1997) Energy Information Administration DOE/EIA-0202(97/3Q) Distribution Category UC-950 Short-Term Energy Outlook Quarterly Projections Third Quarter 1997 Energy Information Administration Office of Energy Markets and End Use U.S. Department of Energy Washington, DC 20585 This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the Department of Energy. The information contained herein should not be construed as advocating or reflecting any policy position of the Department of Energy or any other organization. Contacts The Short-Term Energy Outlook is prepared by the Energy Information Administration (EIA), Office of Energy Markets and End Use (EMEU). General questions concerning the content of the report may be referred to W. Calvin Kilgore (202-586-1617), Director

87

b4.pdf  

U.S. Energy Information Administration (EIA) Indexed Site

........... ........... 4,657 208 479 782 406 748 396 618 315 705 Building Floorspace (Square Feet) 1,001 to 5,000 .............................................. 2,348 99 206 390 230 368 189 360 155 351 5,001 to 10,000 ............................................ 1,110 41 128 200 72 194 80 139 80 175 10,001 to 25,000 .......................................... 708 38 92 122 66 105 87 69 39 91 25,001 to 50,000 .......................................... 257 14 25 32 17 43 25 25 25 52 50,001 to 100,000 ........................................ 145 10 16 22 13 24 9 16 12 23 100,001 to 200,000 ...................................... 59 3 7 11 5 11 4 6 4 8 200,001 to 500,000 ...................................... 23 1 4 5 2 4 1 2 Q 3 Over 500,000 ............................................... 7 Q 2 1 1 1 Q 1 Q 1 Principal Building Activity Education ....................................................

88

JGI - Statistics  

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

Statistics Statistics FY 2014 Overall Sequencing Progress, Updated Quarterly Quarter Total Bases (trillions) Operating Hours Goal Actual Total* Actual % of Goal Goal (hours)** Actual Total Actual % Goal Q1 2014 15,000 18.827 126% 2,164 2208 102% Q2 2014 17,000 2,117 Q3 2014 18,000 2,140 Q4 2014 18,000 2,164 FY 2014 Total 68,000 18.827 28% 8,585 2208 26% * Includes Illumina HiSeq, MiSeq and PacBio sequencing platforms. ** Operating Hour target is based on 98% of the total available hours. FY 2013 Overall Sequencing Progress, Updated Quarterly Quarter Total Bases (Billions) Operating Hours Goal Actual Total* Actual % of Goal Goal (hours)** Actual Total Actual % Goal Q1 2013 15,000 20,004 133% 2,164 2,208 102%

89

Executive Branch Management Scorecard  

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

June 30, 2009 June 30, 2009 CURRENT STATUS (As of June 30,, 2009) PROGRESS Third Quarter FY 2009 COMMENTS REAL PROPERTY Agency Lead: Paul Bosco, Senior Real Property Officer Lead RMO Examiner: Cynthia Vallina Lead OFFM Analyst: Joseph Pika Asset management plan (AMP) X in place by Q1 2005 (Y) X consistent with Federal Real Property Council (FRPC) standards or expected equivalent by Q2 2005 (Y) X OMB-approved by Q2 2005 (Y) X 3 year timeline for meeting plan goals/objectives by Q3 2006 (G) X evidence that plan is being implemented to achieve improved real property mgmt by Q4 2006 (G) Accurate and current inventory X in place by Q3 2004 (Y) X consistent with FRPC standards or expected equivalent by Q3 2004 (Y) X provided to govt.-wide real property

90

Executive Branch Management Scorecard  

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

September 30, 2009 September 30, 2009 CURRENT STATUS (As of September 30, 2009) PROGRESS Fourth Quarter FY 2009 COMMENTS REAL PROPERTY Agency Lead: Paul Bosco, Senior Real Property Officer Lead RMO Examiner: Cynthia Vallina Lead OFFM Analyst: Joseph Pika Asset management plan (AMP) X in place by Q1 2005 (Y) X consistent with Federal Real Property Council (FRPC) standards or expected equivalent by Q2 2005 (Y) X OMB-approved by Q2 2005 (Y) X 3 year timeline for meeting plan goals/objectives by Q3 2006 (G) X evidence that plan is being implemented to achieve improved real property mgmt by Q4 2006 (G) Accurate and current inventory X in place by Q3 2004 (Y) X consistent with FRPC standards or expected equivalent by Q3 2004 (Y) X provided to govt.-wide real property

91

The impact of uncertainty and risk measures  

E-Print Network [OSTI]

papers indicating crude oil price shocks as a contributingdifferent measures of the crude oil price volatility series.of real average crude oil prices from 1957Q1 to 2010Q1

Jo, Soojin; Jo, Soojin

2012-01-01T23:59:59.000Z

92

Corrosion Studies in High-Temperature Molten Salt Systems for...  

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

Corrosion Studies in High-Temperature Molten Salt Systems for CSP Applications - FY13 Q1 Corrosion Studies in High-Temperature Molten Salt Systems for CSP Applications - FY13 Q1...

93

High-Temperature Thermal Array for Next Generation Solar Thermal...  

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

3 Q1 High-Temperature Thermal Array for Next Generation Solar Thermal Power Production - FY13 Q1 This document summarizes the progress of this Los Alamos National Laboratory...

94

Microsoft PowerPoint - Proceedings Cover Sheets  

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

Monitoring, Mitigation, and Verification Monitoring, Mitigation, and Verification Measuring Surface and Shallow Gas Flux and Composition As a Prelude to Geologic Carbon Sequestration in Eastern Kentucky Thomas (Marty) Parris, Mike Solis, and Kathryn Takacs May 8-11, 2006 * Hilton Alexandria Mark Center * Alexandria, Virginia Organization & Schedule Organization & Schedule Phase I Task 1.0 Task 3.0 Task 4.0 Start 2005 2006 2007 End 07/15/05 Q3 Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 01/14/08 Phase II Phase III Task 2.0 Task 5.0 Task 6.0 Task 7.0 Task 8.0 Task 9.0 Task 10.0 Task 11.0 Task 12.0 Task 13.0 Phase II Phase II - - Tasks Tasks Task 5.0- Training, instrumentation, calibration, strategy Task 6.0- Surface & shallow measurements Task 7.0- Laboratory GC & isotope measurements Task 8.0- Evaluate surface data- anomalies & deep wells

95

Q3 1996 STEO TEXT/TABLES  

Gasoline and Diesel Fuel Update (EIA)

202(96/3Q) 202(96/3Q) Distribution Category UC-950 Short-Term Energy Outlook Quarterly Projections Third Quarter 1996 Energy Information Administration Office of Energy Markets and End Use U.S. Department of Energy Washington, DC 20585 This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the Department of Energy. The information contained herein should not be construed as advocating or reflecting any policy position of the Department of Energy or any other organization. Contacts The Short-Term Energy Outlook is prepared by the Energy Information Administration (EIA), Office of Energy Markets and End Use (EMEU). General questions concerning the content of the report may be referred to W. Calvin Kilgore (202-586-1617), Director of EMEU; Mark Rodekohr (202-586-1441), Director of Energy Markets and Contingency

96

Microsoft Word - Q3_Jun_07.doc  

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

Project Title Project Title Seismic Gas Hydrate Quantification by Cumulative Attributes (CATTs) Quarterly Progress Report DE-FC26-06NT42961 Prepared for: DOE/NETL, Morgantown, WV Prepared by: Rock Solid Images 2600 S. Gessner, Suite 650 Houston, TX, 77063 Principal Investigator: Joel Walls Phone: 713-783-5593 Fax: 713-783-5594 j.walls@rocksolidimages.com Date: July 30, 2007 2 Progress Report Award No. DE-FC26-06NT42961 Seismic Gas Hydrate Quantification by Cumulative Attributes (CATTs) Reporting Period: April 1, 2007 to June 30, 2007 Reporting Date: July 30, 2007 Executive Summary During this period, we have narrowed our data selection to the Milne Point area of Prudhoe Bay, Alaska. We feel this data set offers the best combination of known hydrate

97

FOIA Quarterly Reports (Q3 2014)  

Broader source: Energy.gov [DOE]

Report that captures quarterly FOIA data at the DOE level. Through the use of an Applied Programming Interface (or API), the information will display on www.FOIA.gov.

98

On CORI Results Merging Ilya Markov1  

E-Print Network [OSTI]

a source R: snorm(d|q) = 1 + 0.4 · sMinMax (R|q) 1.4 · sMinMax (d|q), (1) P. Serdyukov et al. (Eds.): ECIR. Arampatzis, and F. Crestani where sMinMax (R|q) denotes the relevance of the source R to a query q and rewrite Eq. 1 as follows: snorm(d|q) = 1 + · sMinMax (R|q) 1 + · sMinMax (d|q). (2) Depending on , Eq. 2

Arampatzis, Avi

99

幻灯片 1  

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

Electric-Drive Vehicle Testing Electric-Drive Vehicle Testing at CAERI Hao Zhang China Automotive Engineering Research Institute 1. Overview 2. On-going Work 3. Future Work 4. Conclusion Contents Three-year Plan Full Hybrid BEV Plug-in REEV Mild Hybrid  Three year program in CAERI  Evaluating the performance of the EV, HEV and PHEV  Plan to benchmark more than 12 cars in three years ☆ Milestones 2011-Q2 2011-Q3 2011-Q4 2012-Q1 2012-Q2 2012-Q3 2012-Q4 Test Procedures Research and Preparation for cars Civic Hybrid Test and Analysis Nissan Leaf Test and Analysis MY2010 Prius Test and Analysis Fusion Hybrid Test and Analysis Volt Test and Analysis Plug-in Prius Test and Analysis 2011-2012 works Testing Approach  The vehicle testing activity and analysis approach has been defined:

100

Energy Efficiency and Conservation Block Grant (EECBG): Better Buildings Neighborhood Program Final Report  

SciTech Connect (OSTI)

The Neighbor to Neighbor Energy Challenge (N2N) brought together a consortium of 14 leading clean energy rural, suburban, and low income communities throughout Connecticut. N2N was awarded $4.2 million from the U.S. Department of Energy (DOE) competitive BetterBuildings Neighborhood Program on August 10, 2010 to run a two-year pilot program (plus one year of transition and evaluation) (Award No. EMCBC- 00969-10). N2N tested innovative program models and hypotheses for improving Connecticuts existing residential energy efficiency programs that are overseen by the ratepayer fund board and administered by CT utilities. N2Ns original goal was to engage 10 percent of households in participating communities to reduce their energy usage by 20 percent through energy upgrades and clean energy measures. N2N planned for customers to complete more comprehensive whole-home energy efficiency and clean energy measures and to achieve broader penetration than existing utility-administered regulated programs. Since this was an ARRA award, we report the following figures on job creation in Table 1. Since N2N is not continuing in its current form, we do not provide figures on job retention. Table 1 N2N Job Creation by Quarter Jobs Created 2010 Q4 6.65 2011 Q1 7.13 2011 Q2 4.98 2011 Q3 9.66 2011 Q4 5.43 2012 Q1 11.11 2012 Q2 6.85 2012 Q3 6.29 2012 Q4 6.77 2013 Q1 5.57 2013 Q2 8.35 2013 Q3 6.52 Total 85.31 The N2N team encountered several gaps in the existing efficiency program performance that hindered meeting N2Ns and DOEs short-term program goals, as well as the State of Connecticuts long-term energy, efficiency, and carbon reduction goals. However, despite the slow program start, N2N found evidence of increasing upgrade uptake rates over time, due to delayed customer action of one to two years from N2N introduction to completion of deeper household upgrades. Two main social/behavioral principles have contributed to driving deeper upgrades in CT: 1. Word of mouth, where people share their experience with others, which leads to others to take action; and 2. Self-herding, where people follow past behavior, which leads to deeper and deeper actions within individual households.

Donnelly, Kat A.

2014-01-10T23:59:59.000Z

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


101

A Smoothing SQP Framework for a Class of Composite $L_q ...  

E-Print Network [OSTI]

Jul 28, 2014 ... Abstract: The composite $L_q$ (0<q<1) minimization problem over a general polyhedron has received various applications in machine...

Ya-Feng Liu

2014-07-28T23:59:59.000Z

102

E-Print Network 3.0 - ancillary service rate Sample Search Results  

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

Institute of Technology (MIT) Collection: Engineering ; Geosciences 15 MARCELLUS SHALE APRIL 2011 EDITION Summary: to 2011 Q1): 48,000 new hires within the Marcellus...

103

Analysis of residual spectra and the monopole spectrum for 3 K blackbody radiation by means of non-extensive thermostatistics  

E-Print Network [OSTI]

We analyze residual spectra of 3 K blackbody radiation (CMB) using non-extensive thermostatistics with a parameter q-1. The limits of |q-1|<1.2x10^{-5} and the temperature fluctuation |delta T|<(1.6-4.3)x10^{-5} are smaller than those by Tsallis et al. Moreover, analyzing the monopole spectrum by a formula including the chemical potential mu, we obtain the limits |q-1|<2.3x10^{-5} and |mu|<1.6x10^{-4}. |q-1| is comparable with the Sunyaev-Zeldovich effect y.

Minoru Biyajima; Takuya Mizoguchi

2012-10-22T23:59:59.000Z

104

Materials for Advanced Turbocharger Designs (Agreement ID:17257...  

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

for the U.S. Department of Energy Presentationname Milestones * FY2013, Q1 - complete neutron-scattering residual- stress measurements on wheelshaft assemblies with...

105

E-Print Network 3.0 - achras miller fosberg Sample Search Results  

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

Q WSU FOUNDATION Q 1 CRIMSON BENEFACTORS Summary: Corporation Steven and Janice Boots Cleve and Judith Borth +Louis and +Edythe Bosch +Edythe Miller Boucher... and Kathryn...

106

Fundamental Corrosion Studies in High-Temperature Molten Salt...  

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

Molten Salt Systems for CSP Applications - FY13 Q1 Advanced Ceramic Materials and Packaging Technologies for Realizing Sensors for Concentrating Solar Power Systems...

107

--No Title--  

Gasoline and Diesel Fuel Update (EIA)

226 188 94 68 Q N Food Service ... 297 282 94 149 Q Q Health Care ... 129 124 49 65 Q 1 Inpatient...

108

a7.xls  

U.S. Energy Information Administration (EIA) Indexed Site

Buildings .................................... Buildings .................................... 4,859 3,754 762 117 47 22 157 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,586 2,131 338 Q Q N 100 5,001 to 10,000 ................................. 948 720 182 Q N Q Q 10,001 to 25,000 ............................... 810 590 140 51 13 Q Q 25,001 to 50,000 ............................... 261 163 54 19 12 Q Q 50,001 to 100,000 ............................. 147 87 29 8 13 4 Q 100,001 to 200,000 ........................... 74 43 13 6 5 4 Q 200,001 to 500,000 ........................... 26 15 5 Q 1 3 Q Over 500,000 .................................... 8 3 1 Q Q 3 Q Principal Building Activity Education .......................................... 386 360 21 Q N N N Food Sales ....................................... 226 203 Q N N Q N Food Service .....................................

109

Office of Headquarters Security Operations: Questions and Answers on the  

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

Questions and Answers on the New Access Control System at DOE Headquarters Questions and Answers on the New Access Control System at DOE Headquarters Q1 Why is the current access control system to security areas being changed? Q2 How is the new access control system different from the existing one? Q3 Who is affected? Q4 When will the new proximity card readers be installed? Q5 How will affected personnel at DOE HQ be notified about the installation of the proximity card readers that will affect their access to the HQ facilities and security areas, and the actions they will be required to take to assure their HSPD-12 badge will operate in the new readers? Q6 What will DOE HQ "Q" and "L" badged employees need to do? Q7 Will all DOE HQ security areas be changed out to the new access control system at the same time?

110

USDOE Technology Transfer, Frequently Asked Questions about Agreement for  

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

Frequently Asked Questions about ACT: Frequently Asked Questions about ACT: Q1: What is ACT (Agreement for Commercializing Technology)? A1: ACT is a pilot program under which businesses may partner with participating DOE laboratories for research and development that commercializes technology. Q2: Why is this pilot being introduced? A2: ACT is being piloted to address concerns about difficulties in partnering with the DOE laboratories that were raised in public responses to a DOE Request for Information on improving technology transfer. These concerns include requirements for advance payments, indemnification and government use rights in intellectual property. Q3: Who can partner with the laboratories under ACT? A3: ACT is available to a full range of sponsors, including start-ups, small and large businesses that provide private funding to

111

22680  

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

QUARTERLY PROGRAM REPORT QUARTERLY PROGRAM REPORT State: __________________ Budget period: / / - / / Grant Number: __________________ I. GRANT OUTLAYS - FUNDS SUBJECT TO DOE PROGRAM RULES (rounded to the nearest dollar) DOE F 540.3 (08/05) OMB Control No. 1910-5127 Expiration Date: 6/30/08 A. OUTLAYS BY FUND SOURCE DOE Other funds included in grant budget, section A B. OUTLAYS BY FUNCTION Grantee Administration Subgrantee Administration Grantee T&TA Subgrantee T&TA Program Operations Total Health and Safety Vehicles and Equipment - Acquisition Cost* Liability Insurance Leveraging Financial Audits Vehicles and Equipment - Amortized Cost* Total Grant Outlays Total Grant Outlays Reporting Period Quarter / - / Q1 / - / Q2 / - / Q3 / - / Q4 Total To Date Notes: Total grant outlays must equal outlays reported on the Financial Status Report, line 10.d.

112

Microsoft PowerPoint - compliant sealing glass review 7,27,2010 rev1.pptx [Read-Only]  

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

Compliant glass seal development Compliant glass seal development Y-S Matt Chou, E. Thomsen, E. Mast, J-P Choi, W. Voldrich, and J. W. Stevenson Introduction and objectives Q1: Effect of differential pressure on thermal cycle stability 1 experimental 1. experimental 2. leak rates versus cycling (700-850 o C/1000h) Q2: thermal stability study in a duel environment 1. leak rates versus time (750-800 o C/1000h) 2. microstructure and interface characterization Q3: assess YSZ coating and other mat'l for spacer rings Q g p g Summary Future work Solid-State Energy Conversion Alliance Core Technology Programs Review, July 27-29, 2010, Pittsburgh, PA Compliant versus refractory sealing glass  = E T Compliant sealing glass 1.20E-02 YSO1 glass Refractory sealing glass Data provided by ORNL

113

Phase behavior of colloidal superballs: Shape interpolation from spheres to cubes  

Science Journals Connector (OSTI)

The phase behavior of hard superballs is examined using molecular dynamics within a deformable periodic simulation box. A superballs interior is defined by the inequality |x|2q+|y|2q+|z|2q?1, which provides a versatile family of convex particles (q?0.5) with cubelike and octahedronlike shapes as well as concave particles (q<0.5) with octahedronlike shapes. Here, we consider the convex case with a deformation parameter q between the sphere point (q=1) and the cube (q=?). We find that the asphericity plays a significant role in the extent of cubatic ordering of both the liquid and crystal phases. Calculation of the first few virial coefficients shows that superballs that are visually similar to cubes can have low-density equations of state closer to spheres than to cubes. Dense liquids of superballs display cubatic orientational order that extends over several particle lengths only for large q. Along the ordered, high-density equation of state, superballs with 1<q<3 exhibit clear evidence of a phase transition from a crystal state to a state with reduced long-ranged orientational order upon the reduction of density. For q?3, long-ranged orientational order persists until the melting transition. The width of the apparent coexistence region between the liquid and ordered, high-density phase decreases with q up to q=4.0. The structures of the high-density phases are examined using certain order parameters, distribution functions, and orientational correlation functions. We also find that a fixed simulation cell induces artificial phase transitions that are out of equilibrium. Current fabrication techniques allow for the synthesis of colloidal superballs and thus the phase behavior of such systems can be investigated experimentally.

Robert D. Batten; Frank H. Stillinger; Salvatore Torquato

2010-06-02T23:59:59.000Z

114

Microsoft Word - Q3report_rev.doc  

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

April 2009 to June 2009 April 2009 to June 2009 Heat Flow and Gas Hydrates on the Continental Margin of India: Building on Results from NGHP Expedition 01 Submitted by: College of Oceanic and Atmospheric Science Oregon State University Corvallis, OR 97331 Principal Investigator: Anne M. Trehu Prepared for: United States Department of Energy National Energy Technology Laboratory July 28, 2009 Oil & Natural Gas Technology 1 Progress Report April 2009 to June 2009 Heat flow and gas hydrates on the continental margin of India: Building on results from NGHP expedition 01 DE-NT0005669 Principal Investigator Anne Trehu (PI) Oregon State University July 28, 2009 2 Table of Contents: Executive Summary..................................................................................................

115

Microsoft Word - DOE_ANNUAL_METRICS_2009Q3.docx  

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

14404 14404 Third Quarter 2009 Modeling Program Metric: Coupled model comparison with observations using improved dynamics at coarse resolution Quantifying the impact of a finite volume dynamical core in CCSM3 on simulated precipitation over major catchment areas July 2009 Peter J. Gleckler and Karl E. Taylor Lawrence Livermore National Laboratory Livermore, CA Work supported by the U.S. Department of Energy, Office of Science, Office of Biological and Environmental Research 
 2
 Disclaimer This document was prepared as an account of work sponsored by an agency of the United States government. Neither the United States government nor Lawrence Livermore National Security, LLC, nor any of their employees makes any warranty,

116

Flexible Assembly Solar Technology- FY13 Q3  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this BrightSource Energy project, funded by SunShot, for the second quarter of fiscal year 2013.

117

Observations from The EV Project in Q3 2013  

SciTech Connect (OSTI)

This is a brief report that summarizes results published in numerous other reports. It describes the usage of electric vehicles and charging units in the EV Project over the past 3 months. There is no new data or information provided in this report, only summarizing of information published in other reports (which have all been approved for unlimited distribution publication). This report will be posted to the INL/AVTA website for viewing by the general public.

John Smart

2013-12-01T23:59:59.000Z

118

SUPPLEMENTARY MATERIAL Supplementary Material to "High-Dimensional Structure Learning of Ising Models  

E-Print Network [OSTI]

SUPPLEMENTARY MATERIAL Supplementary Material to "High-Dimensional Structure Learning of Ising) (P, Q) := 1 2 P - Q 1 = 1 2 xX |P(x) - Q(x)|. 1.1. Analysis of Ising Models on Trees. We first derive simple expressions for Ising models Markov on trees. This will be later used upon reduction of general

Anandkumar, Animashree

119

Novel Atomic Coherence and Interference Effects in Quantum Optics and Atomic Physics  

E-Print Network [OSTI]

. . . . . . . . . . . . . . . . . . . . . . . . . 7 1. Probability Amplitude Method . . . . . . . . . . . . . . . 9 2. Density Matrix Approach . . . . . . . . . . . . . . . . . . 12 B. Maxwell-Schrodinger Equation . . . . . . . . . . . . . . . . . 14 C. Three-Level Atom.... . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 27 8 Pulse shapes given by Eq.(3.17). (a) Pulse shapes with varying ? and c = 2, q = ?1, ab = 0. (b) Pulse shapes with varying c and ? = 2, q = ?1, ab = 0. . . . . . . . . . . . . . . . . . . . . . . . . . . 30 xii FIGURE Page 9 Pulse shapes...

Jha, Pankaj

2012-10-19T23:59:59.000Z

120

The effect of airflow cooling on a scramjet: a preliminary assessment  

Science Journals Connector (OSTI)

...4 as affected by the heat loss q1 through an initial...10). Figure 19. Heat added during combustion H as a multiple of h...H. For a typical hydrocarbon fuel, c would be ca...200 (h/H). The heat loss q1 due to the coolant...

1999-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


121

c36a.xls  

Gasoline and Diesel Fuel Update (EIA)

Education ... 293 Q Q Q 1.04 Q Q Q 0.31 Q Q Q Health Care... Q Q 19 8 Q 1.06 1.08 1.16 Q Q 0.02 0.03...

122

Energy Information Administration - Commercial Energy Consumption...  

Annual Energy Outlook 2013 [U.S. Energy Information Administration (EIA)]

Education ... 293 Q Q Q 1.04 Q Q Q 0.31 Q Q Q Health Care... Q Q 19 8 Q 1.06 1.08 1.16 Q Q 0.02 0.03...

123

--No Title--  

Annual Energy Outlook 2013 [U.S. Energy Information Administration (EIA)]

Education ... 293 Q Q Q 1.04 Q Q Q 0.31 Q Q Q Health Care... Q Q 19 8 Q 1.06 1.08 1.16 Q Q 0.02 0.03...

124

c36a.xls  

Gasoline and Diesel Fuel Update (EIA)

,437 ,437 178 130 82 1.10 1.04 1.21 1.28 0.22 0.06 0.03 Q Building Floorspace (Square Feet) 1,001 to 10,000 ................................. 460 Q Q Q 1.21 Q Q Q 0.60 Q Q Q 10,001 to 100,000 ............................. 444 70 Q Q 1.10 1.12 1.29 1.31 0.25 0.11 Q Q Over 100,000 .................................... 533 22 48 Q 1.03 1.06 1.08 1.26 0.14 0.01 0.01 Q Principal Building Activity Education .......................................... 293 Q Q Q 1.04 Q Q Q 0.31 Q Q Q Health Care........................................ Q Q 19 8 Q 1.06 1.08 1.16 Q Q 0.02 0.03 Office ................................................ 122 8 18 Q 1.16 1.32 1.26 1.44 0.09 0.01 0.01 0.00 All Others .......................................... 980 Q 64 50 1.12 1.02 1.34 1.26 0.26 0.10 0.03 Q Year Constructed 1945 or Before .................................. 620 Q Q Q 1.10 Q Q Q 0.29

125

c36.xls  

Gasoline and Diesel Fuel Update (EIA)

,393 ,393 176 125 81 1.10 1.03 1.21 1.28 0.23 0.06 0.03 Q Building Floorspace (Square Feet) 1,001 to 10,000 ................................. 460 Q Q Q 1.21 Q Q Q 0.61 Q Q Q 10,001 to 100,000 ............................. 408 70 Q Q 1.09 1.12 1.29 1.31 0.24 0.11 Q Q Over 100,000 .................................... 524 21 47 Q 1.03 1.05 1.07 1.26 0.14 0.01 0.02 Q Principal Building Activity Education .......................................... 293 Q Q Q 1.04 Q Q Q 0.31 Q Q Q Health Care........................................ Q Q 19 8 Q 1.06 1.08 1.16 Q Q 0.02 0.03 Office ................................................ 122 8 18 Q 1.16 1.32 1.26 1.44 0.09 0.01 0.01 0.00 All Others .......................................... 936 Q 59 50 1.12 1.01 1.34 1.26 0.27 0.11 0.04 Q Year Constructed 1945 or Before .................................. 612 Q Q Q 1.10 Q Q Q 0.29

126

Figure 7.1. Control of an alarm system. Figure 7.2. A simple memory element.  

E-Print Network [OSTI]

-digit BCD counter. Enable Q0 Q1 Q2 D0 D1 D2 Load Clock 1 0 0 0 Clock Q30 D3 Enable Q0 Q1 Q2 D0 D1 D2 Load Clock 0 0 0 Q30 D3 BCD0 BCD1 Clear Figure 7.30. Johnson counter. D Q Q Clock D Q Q D Q Q Q0 Q1 Qn 1 by CAD tools. Data Clock Latch #12;Figure 7.34. Timing simulation of storage elements. Figure 7.35. Code

Kalla, Priyank

127

EXISTENCE OF DICRITICAL DIVISORS Section 1: Introduction. The ...  

E-Print Network [OSTI]

Conversely, for any finite subset U of D(R)?, upon letting. ?R(U) = ? ... gives a bijection W ? W. In turn g ?? Sg gives a bijection W ? Q1(R) where. M(Sg)=(g...

2010-07-30T23:59:59.000Z

128

Agenda Compiled by VP Anna Josephson Page 1 of 3 Senate Meeting  

E-Print Network [OSTI]

://www.purdue.edu/newsroom/purduetoday/releases/2014/Q1/active- learning-center-open-forum-being-held-march-13.html III. Approval of Minutes IV Bruce bruce7@purdue.edu> Treasurer: Yang Liu #12;

Ginzel, Matthew

129

High-Temperature Solar Selective Coating Development for Power...  

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

progress of this Sandia National LaboratoriesNREL project, funded by SunShot, for the first quarter of fiscal year 2013. snlpachecofy13q1.pdf More Documents & Publications...

130

E-Print Network 3.0 - antenatal corticosteroid therapy Sample...  

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

Genetics, National Institutes of Health Collection: Biology and Medicine 50 Uricase for gout treatment Chapter 5.1 Summary: ) + q 4 w (for 3 y) 0.20 mgkg; q 1 w (for 16 m)...

131

PowerPoint Presentation  

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

1, 2013 (NEW PROJECT) Planned end date: September 30, 2014 Key Milestones 1. 200g Dark Red Pigment, End Q1 2. Additional Pigments Identified, End Q2 3. 500g of 2 New Pigments,...

132

Experimental determination of dynamic Young's modulus and mechanical damping, and theoretical prediction of dislocation density for depleted uranium-0.75 wt% titanium using the PUCOT  

Science Journals Connector (OSTI)

Dynamic Young's modulus (E) and mechanical damping (Q ?1) measurements were made for three microstructures (?, ? + ?, and ??) of a depleted uranium-0.75 wt% titanium alloy. The...E and Q ...

K. H. Keene; A. Wolfenden; G. M. Ludtka

1988-08-01T23:59:59.000Z

133

ATF Video Frame Grabber Subsystems - Frequently Asked Questions  

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

III - Re-creating images from captured data (Q1) Using Matlab, how can I recreate an image from captured data (without using the ATF frame grabber program)? (A1) The easiest way is...

134

EV-Smart Grid Research & Interoperability Activities 2014 DOE...  

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

to establish interoperability centers - Q1, FY 2012 Official Argonne launch - Q4, FY 2013 2 Budget* FY2012 - 1180 K FY2013 - 2200 K FY2014 - 1550 K Barriers...

135

E-Print Network 3.0 - arterial pressure difference Sample Search...  

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

Collection: Mathematics 5 Bio390 Atherosclerosis and Resistance thanks to Dr. J.F. Anderson, Summary: the pressure difference required: P R * Q 1.52. In the overall...

136

E-Print Network 3.0 - acholeplasma laidlawii b Sample Search...  

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

Cedex, France. Email... lateral information is lost. b) CCD images are taken (using a Peltier-cooled camera, 12421152 pixels... by Rosenfeld (33, Eq. (6.8)): S-1 hd (q) 1 + 4...

137

What Can China Do? China's Best Alternative Outcome for Energy Efficiency and CO2 Emissions  

E-Print Network [OSTI]

Aizhu Chen. Chinas energy intensity rises 3.2 pct in Q1. Table 1 Energy Use, Energy Intensity, and GDP Data (2005-2 Table 2 Frozen 2005 Energy Intensity Baseline and Reported

G. Fridley, David

2010-01-01T23:59:59.000Z

138

The Greening of the Middle Kingdom: The Story of Energy Efficiency in China  

E-Print Network [OSTI]

China View. 2009. Chinas energy intensity down 2.9% in Q1:demand at constant energy intensity, 19802006. Source: NBS,percent reduction in energy intensity (defined as energy use

Zhou, Nan

2010-01-01T23:59:59.000Z

139

MATH 690 NOTES 1. August 22, 2007, Filtered rings As Paolo and ...  

E-Print Network [OSTI]

Aug 22, 2007 ... ?bi1 = ai1 + ?ci1, where ai1 ? R and ?ci1 ? Q1. ?R1. Then f = s. ? ...... ian local domains (R, m) for which the set G(R) of Goto numbers of...

1910-71-00T23:59:59.000Z

140

E-Print Network 3.0 - asymmetric mass distribution Sample Search...  

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

the potential energy landscape on the fission dynamics K. Mazurek1,2,a Summary: of the fis- sion valley (red dashed lines in the Fig. 1) is presented in Fig. 2 in the plane q1,...

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


141

Low-Cost, Lightweight Solar Concentrator | Department of Energy  

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

Documents & Publications Low-Cost, Lightweight Solar Concentrators - FY13 Q1 Low-Cost Light Weigh Thin Film Solar Concentrators Low-Cost, Lightweight Solar Concentrators FY13...

142

TOUGH+Hydrate v1.0 User's Manual: A Code for the Simulation of System Behavior in Hydrate-Bearing Geologic Media  

E-Print Network [OSTI]

of radiative heat transfer between the two grid blocks is: Q= 1: The heat exchange is activated (for grid blocks thatgrid blocks Optional; provides time-variable conditions at specific boundaries Optional; list of mass or heat

Moridis, George

2008-01-01T23:59:59.000Z

143

--No Title--  

Gasoline and Diesel Fuel Update (EIA)

226 Q N 1,255 Q N Food Service ... 297 27 Q 1,654 264 Q Health Care ... 129 26 4 3,163 1,899 733 Inpatient...

144

A Study of Internal Friction, Electric Resistance and Shape Change in Cu-Zn and Cu-Zn-Al Alloys During Phase Transformation Use Simultaneous Measurement Method  

Science Journals Connector (OSTI)

The internal friction (Q-1), electric resistance (r), shape change (X),...-1...peaks are not due to the phase transformation but due to point defects. The electric resistance during thermoelastic martensite (TEM)...

Yuan-Ti Huang; Tian-Fei Wang; Yin Mei

1990-01-01T23:59:59.000Z

145

IKs channels open slowly because KCNE1 accessory subunits slow the movement of S4 voltage sensors in KCNQ1 pore-forming subunits  

Science Journals Connector (OSTI)

...41). Assuming nine elementary gating charges per Q1...smaller fraction of the electric field...Microelectrodes had a resistance of 0.3 M{omega}. SDF Recordings...fluorometric approach to local electric field measurements in...

Katarina J. Ruscic; Francesco Miceli; Carlos A. Villalba-Galea; Hui Dai; Yukiko Mishina; Francisco Bezanilla; Steve A. N. Goldstein

2013-01-01T23:59:59.000Z

146

264.ps  

E-Print Network [OSTI]

Jan 30, 2001 ... P.O.Box 5031, 2600 GA Delft, The Netherlands. zDepartment of ..... [10, page 4]); by taking = q 1, the de nition coincides. with (15). By using...

147

Differential-und Integralrechnung III Losungen fur Woche 4  

E-Print Network [OSTI]

(i) = xi und g(j) = yj. Dann saft die H¨older-Ungleichung: n i=1 |xiyi| (|xi|p ) 1 p |yj|q () 1 q wo 1/p

Mitchener, Paul

148

DELFT UNIVERSITY OF TECHNOLOGY REPORT 06-05  

E-Print Network [OSTI]

2 - P0), (P2+ - P1) elements and (P2+ - P1) grid 9 3 Taylor Hood family mini elements Q+ 1 - Q1], the incompressible Stokes and Navier Stokes problems are solved in a square and L-shaped domain with a varying grid. Different ordering techniques of the grid points and the unknowns are used to avoid breakdown of the LU de

Vuik, Kees

149

BIG IMPROVEMENTS OF THE WEIL BOUND FOR ARTIN-SCHREIER CURVES  

E-Print Network [OSTI]

gives the estimate |Nr(f) - qr | (d - 1)(q - 1)q r 2 . This bound can be sharp in general, for instance to a somewhat better bound: |Nr(f) - qr | (d - 1)(q - 1) 2 [2q r 2 ], where [x] denotes the integer part the estimate |Nr(f) - qr | Cd,rq r+1 2 , where Cd,r is the constant Cd,r = r a=0 |a - 1| d - 2 + r - a r - a d

Wan, Daqing

150

Physics 182 Equation Sheet for Exams Good Stuff from 181  

E-Print Network [OSTI]

QH = 1 - QC QH Carnot = 1 - TC TH Refrigerator: Win + QC = QH K = QC Win = QC QH -QC KCarnot = TC TH -TC 1 #12;· Chapter 25: Coulomb Law: |Fq1q2 | = K |q1||q2| r2 = 1 40 |q1||q2| r2 Charge in a Field: F = q E Field of a Point Charge q: E = K q r2 ^r = 1 40 q r2 ^r · Chapter 26: Dipole Moment: p = (qs

Alexander, Stephen G.

151

Table 5.8. U.S. Vehicle Fuel Consumption by Family Income, 1994  

U.S. Energy Information Administration (EIA) Indexed Site

17.0 16 or 17 Years ... 9.6 Q Q Q 1.4 1.6 2.4 3.3 Q 1.4 2.1 30.8 Households Without Children ... 50.2 1.1 2.8 3.9 10.1 7.7 10.2 14.5 2.9 4.3 7.9 11.2...

152

Spin waves in a persistent spin-current Fermi liquid  

Science Journals Connector (OSTI)

We report two theoretical results for transverse spin waves, which arise in a system with a persistent spin current. Using Fermi liquid theory, we introduce a spin current in the ground state of a polarized or unpolarized Fermi liquid, and we derive the resultant spin waves using the Landau kinetic equation. The resulting spin waves have a q1 and q1/2 dispersion to leading order for the polarized and unpolarized systems, respectively.

J. D. Feldmann and K. S. Bedell

2010-06-14T23:59:59.000Z

153

c17.xls  

Gasoline and Diesel Fuel Update (EIA)

32 32 116 153 2,942 9,867 11,373 10.8 11.7 13.5 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 4 9 20 345 652 908 12.7 13.8 22.0 5,001 to 10,000 ................................. 3 7 8 350 732 781 7.7 9.6 10.7 10,001 to 25,000 ............................... Q 16 20 Q 1,390 1,934 Q 11.2 10.5 25,001 to 50,000 ............................... Q 8 16 Q 944 1,534 Q 8.5 10.4 50,001 to 100,000 ............................. Q 15 21 Q 1,524 1,618 Q 10.2 12.9 100,001 to 200,000 ........................... Q 17 26 Q 1,703 1,671 Q 10.1 15.5 200,001 to 500,000 ........................... Q 22 24 Q 1,673 1,801 Q 13.1 13.1 Over 500,000 .................................... Q 22 18 Q 1,248 1,126 Q 17.3 16.4 Principal Building Activity Education .......................................... Q 12 16 Q 1,384 1,990 Q 8.4 7.9 Food Sales .......................................

154

LANL Calendar  

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

Calendar Calendar LANL Calendar LANL Public Events. . . Careers» Community» Environment» 70th Anniversary» C Your browser does not appear to support JavaScript, but this page needs to use JavaScript to display correctly. You can visit the HTML-only version of this page at: https://www.google.com/calendar/htmlembed?showTitle=0&showTabs=0&showCalendars=0&height=600&wkst=1&bgcolor=%23FFFFFF&src=19q3q9uc7hhi0n1g26a2lrjtbk@group.calendar.google.com&color=%23875509&src=fgk10mie1loqb2j74p1d31f1p0@group.calendar.google.com&color=%23853104&src=q1tai2uhgddrvti32ntk5c8s0o@group.calendar.google.com&color=%232F6309&src=lanleventscalendar@gmail.com&color=%232952A3&src=2irr2g4nfn589m88hatkpa4v8k@group.calendar.google.com&color=%23253b55&src=2irr2g4nfn589m88hatkpa4v8k@group.calendar.google.com&color=%23182C57&ctz=America%2FDenver

155

Frequently Asked Questions Form EIA-857  

U.S. Energy Information Administration (EIA) Indexed Site

Natural Gas Survey Forms FAQ Natural Gas Survey Forms FAQ EIA-857, "Monthly Report of Natural Gas Purchases and Deliveries to Consumers" You may always call Amy Sweeney for assistance at (202) 586-2627 or e-mail us at OOG.SURVEYS@eia.gov. Q1. How do I get a copy of the form and/or the instructions? Q2. What version of the form should I use? Q3. How do I submit the form? Q4. When is the form due? Q5. My company does not have the information required on the Form EIA-857 within 30 days after the end of the report month. Can we get an extension? Q6. Who should I inform of a change in the contact person in our company for Form EIA-857? Q7. Who should I inform if our company is sold, merged with another company, or buys another natural gas company? Q8. Why does my company always get selected to file Form EIA-857?

156

c35.xls  

Gasoline and Diesel Fuel Update (EIA)

65 65 170 104 63 6,080 2,832 4,122 2,123 0.21 0.06 0.03 Q Building Floorspace (Square Feet) 1,001 to 10,000 ............................... 381 Q Q Q 757 Q 255 Q 0.50 Q 0.10 Q 10,001 to 100,000 ........................... 375 63 Q Q 1,704 643 833 351 0.22 0.10 Q Q Over 100,000 .................................. 509 20 44 Q 3,618 1,983 3,034 1,673 0.14 0.01 0.01 Q Principal Building Activity Education ........................................ 282 Q Q Q 933 Q Q Q 0.30 Q Q Q Health Care...................................... Q Q 17 7 Q 492 786 262 Q Q 0.02 0.03 Office .............................................. 105 6 14 1 1,379 714 1,235 748 0.08 0.01 0.01 0.00 All Others ........................................ 837 Q 44 40 3,426 1,281 1,644 984 0.24 Q 0.03 Q Year Constructed 1945 or Before ................................ 555 Q Q Q 2,126 Q Q Q 0.26 Q Q Q 1946 to 1959 ...................................

157

Embargoed Deletion  

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

PNAS proof PNAS proof Embargoed Deletion of Cel48S Q:1 from Clostridium thermocellum ; 2 Daniel G. Olson a,b,c , Shital A. Tripathi a,c , Richard J. Giannone c,d , Jonathan Lo b,c , Nicky C. Caiazza a,c , David A. Hogsett a,c , Robert Hettich c,d , Adam M. Guss b,c , Genia Dubrovsky b,c , and Lee R. Lynd a,b,c,e,1 a Mascoma Corporation, NH 03766; b Thayer School of Engineering and e Department of Biological Sciences, Dartmouth College, NH 03755; and c BioEnergy Science Center, d Oak Ridge National Laboratory, TN 37830 Q:3 Edited* by Lonnie O'Neal Ingram, University of Florida, Gainesville, FL, and approved August 16, 2010 (received for review April 9, 2010) Clostridium thermocellum is a thermophilic anaerobic bacterium that rapidly solubilizes cellulose with the aid of a multienzyme cel- lulosome complex. Creation of knockout mutants for Cel48S (also known as CelS, S S , and S8), the most abundant cellulosome

158

Energy Information Administration - Commercial Energy Consumption Survey-  

Gasoline and Diesel Fuel Update (EIA)

5A. Fuel Oil Consumption and Conditional Energy Intensity by Census Region for All Buildings, 2003 5A. Fuel Oil Consumption and Conditional Energy Intensity by Census Region for All Buildings, 2003 Total Fuel Oil Consumption (million gallons) Total Floorspace of Buildings Using Fuel Oil (million square feet) Fuel Oil Energy Intensity (gallons/square foot) North- east Mid- west South West North- east Mid- west South West North- east Mid- west South West All Buildings .............................. 1,302 172 107 64 6,464 2,909 4,663 2,230 0.20 0.06 0.02 Q Building Floorspace (Square Feet) 1,001 to 10,000 ............................ 381 Q Q Q 763 Q 274 Q 0.50 Q 0.10 Q 10,001 to 100,000 ........................ 404 63 Q Q 1,806 648 985 351 0.22 0.10 Q Q Over 100,000 ............................... 517 21 45 Q 3,894 2,055 3,404 1,780 0.13 0.01 0.01 Q

159

Mechanism of runaway electron beam formation during plasma disruptions in tokamaks  

E-Print Network [OSTI]

A new physical mechanism of the formation of runaway electron (RE) beams during plasma disruptions in tokamaks is proposed. The plasma disruption is caused by strong stochastic magnetic field formed due to nonlinearly excited low-mode number magnetohydrodynamic (MHD) modes. It is conjectured that the runaway electron beam is formed in the central plasma region confined inside the intact magnetic surface located between $q=1$ and the closest low--order rational magnetic surfaces [$q=3/2$, $q=4/3$, \\dots]. It results in that runaway electron beam current has a helical nature with a predominant $m/n=1/1$ component. The thermal quench and current decay times are estimated using the collisional models for electron diffusion and ambipolar particle transport in a stochastic magnetic field, respectively. Possible mechanisms of the decay of runaway electron current due to an outward drift electron orbits and resonance interaction of high--energy electrons with the $m/n=1/1$ MHD mode are discussed.

Abdullaev, S S; Wongrach, K; Tokar, M; Koslowski, H R; Willi, O; Zeng, L

2015-01-01T23:59:59.000Z

160

Household energy consumption and its demand elasticity in Thailand  

Science Journals Connector (OSTI)

This study concentrates on the analysis of energy consumption, expenditure on oil and LPG use in cars and aims to examine the elasticity effect of various types of oil consumption. By using the Deaton's analysis framework, the cross-sectional data of Thai households economic survey 2009 were used. By defining energy goods in the scope of automobile fuel, the results reflect the low importance of high-quality automobile fuel on all income level households. Thai households tend to vary the quality rather than the quantity of thermal energy. All income groups have a tendency to switch to lower quality fuel. Middle and high-middle households (Q3 and Q4) are the income groups with the greatest tendency to switch to lower-quality fuel when a surge in the price of oil price occurs. The poorest households (Q1) are normally insensitive to a change of energy expenditure in terms of quality and quantity. This finding illustrates the LPG price subsidy policy favours middle and high-middle income households. The price elasticity of energy quantity demand is negative in all income levels. High to middle income families are the most sensitive to changes in the price of energy.

Montchai Pinitjitsamut

2012-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


161

DOE FY10_Svc_Cont_Inv 122910 v2 MAX.xlsx  

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

Fixed Fixed Price Cost T&M/LH Other Competed Not Competed Blank Q1 Q2 Q3 Q4 B505 Cost Benefit Analyses $0 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% R406 Policy Review/Development Services $0 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% 0% R407 Program Evaluation Services $6,598,775 0% 1% 0% 99% 0% 30% 5% 65% 5% 33% 32% 31% R408 Program Management/Support Services $311,028,791 1% 2% 67% 32% 0% 90% 4% 6% 26% 25% 13% 35% R409 Program Review/Development Services $49,991 0% 100% 0% 0% 0% 100% 0% 0% 0% 0% 0% 100% R413 Specifications Development Service $106,958 0% 0% 100% 0% 0% 100% 0% 0% 0% 100% 0% 0% R707 Management Services/Contract & Procurement Support $35,519,976 0% 3% 93% 4% 0% 0% 100% 0% 17% 1% 49% 32% R423 Intelligence Services $10,385,300 0% 2% 0% 98% 0% 57% 0% 43% 7% 39% 26% 29% R425 Engineering and Technical Services $315,519,561 1% 2% 58% 33% 7% 93% 6% 1% 10% 25% 23% 42% R414 Systems Engineering Services

162

c35a.xls  

Gasoline and Diesel Fuel Update (EIA)

02 02 172 107 64 6,464 2,909 4,663 2,230 0.20 0.06 0.02 Q Building Floorspace (Square Feet) 1,001 to 10,000 ............................... 381 Q Q Q 763 Q 274 Q 0.50 Q 0.10 Q 10,001 to 100,000 ........................... 404 63 Q Q 1,806 648 985 351 0.22 0.10 Q Q Over 100,000 .................................. 517 21 45 Q 3,894 2,055 3,404 1,780 0.13 0.01 0.01 Q Principal Building Activity Education ........................................ 282 Q Q Q 933 Q Q Q 0.30 Q Q Q Health Care...................................... Q Q 17 7 Q 492 786 262 Q Q 0.02 0.03 Office .............................................. 105 6 14 1 1,379 714 1,235 748 0.08 0.01 0.01 0.00 All Others ........................................ 873 Q 47 40 3,810 1,358 2,186 1,091 0.23 Q 0.02 Q Year Constructed 1945 or Before ................................ 562 Q Q Q 2,162 Q Q Q 0.26 Q Q Q 1946 to 1959 ...................................

163

a3.xls  

U.S. Energy Information Administration (EIA) Indexed Site

4,859 252 509 728 577 926 360 587 316 603 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,586 134 240 372 356 474 217 294 166 333 5,001 to 10,000 ................................. 948 49 106 128 100 200 59 127 62 117 10,001 to 25,000 ............................... 810 46 92 133 78 151 54 103 61 91 25,001 to 50,000 ............................... 261 10 29 48 27 52 16 28 16 34 50,001 to 100,000 ............................. 147 8 23 25 10 26 11 21 7 15 100,001 to 200,000 ........................... 74 3 12 14 5 18 Q 10 3 7 200,001 to 500,000 ........................... 26 Q 6 6 1 4 Q 3 1 3 Over 500,000 .................................... 8 Q 2 1 Q 2 Q Q Q 1 Principal Building Activity Education .......................................... 386 Q 21 34 29 87 Q 56 39 97 Food Sales .......................................

164

http://www.eh.doe.gov/nepa/process/ll/95q3.htm  

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

3RD 3RD QUARTER FY 1995 Office of NEPA Policy and Assistance U.S. Department of Energy September 1, 1995 INTRODUCTION To foster continuing improvement of the Department's National Environmental Policy Act (NEPA) compliance program, the Secretarial Policy Statement on NEPA, issued June 13, 1994, requires the Office of Environment, Safety and Health to solicit comments on lessons learned in the process of completing NEPA documents from the NEPA Document Manager, the NEPA Compliance Officer, and team members after completing each environmental impact statement (EIS) and environmental assessment (EA), and to distribute a quarterly summary to all NEPA Compliance Officers and NEPA Document Managers. This quarterly report summarizes the lessons learned for documents completed between April 1 and June

165

TOTAL_ARRA_Homes_Weatherized_thru_Q3_2010_11_9_10.pdf | Department...  

Energy Savers [EERE]

TOTALARRAHomesWeatherizedthruQ3201011910.pdf TOTALARRAHomesWeatherizedthruQ3201011910.pdf TOTALARRAHomesWeatherizedthruQ3201011910.pdf More Documents &...

166

High-Efficiency Receivers for Supercritical Carbon Dioxide Cycles- FY13 Q3  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this Brayton Energy project, funded by SunShot, for the third quarter of fiscal year 2013.

167

c27a.xls  

Gasoline and Diesel Fuel Update (EIA)

85 85 364 550 1,861 8,301 10,356 45.4 43.8 53.1 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... Q 42 69 Q 427 741 Q 98.4 92.9 5,001 to 10,000 ................................. Q 32 49 Q 518 743 Q 62.1 65.5 10,001 to 25,000 ............................... Q 47 102 Q 952 1,860 Q 49.7 54.6 25,001 to 50,000 ............................... Q 42 78 Q 900 1,567 Q 47.1 49.6 50,001 to 100,000 ............................. Q 49 77 Q 1,421 1,611 Q 34.4 47.7 100,001 to 200,000 ........................... Q 44 73 Q 1,531 1,454 Q 28.4 50.4 200,001 to 500,000 ........................... Q 55 58 Q 1,484 1,323 Q 37.3 43.5 Over 500,000 .................................... Q 52 45 Q 1,068 1,056 Q 48.6 43.0 Principal Building Activity Education .......................................... Q 49 99 Q 1,247 1,804 Q 39.5 54.6 Food Sales .......................................

168

Determination of mechanical properties of the high temperature ceramic superconductors YBa?Cu?O????x (where x[0.5)  

E-Print Network [OSTI]

). 2. M. K Wu, J. Ashburn, C. J. Torng, P. H. Hor, R. L. Meng, L. Gao, Z. J. Huang, Y. Q. Wang, and C. W. Chu, Phys. Rev. Lett. Vol. 58, p. 908 (1987). 3. S. Jin, T. H. Tiefel, R. C. Sherwood, G. W. Kammlott and S. M. Zahurak, Appl. Phys. Lett... mass of gauge crystal mj mass of component j mq mass of quartz spacer rod ms mass of specimen md+ mg mdgq mdgqs mt nld + nlg + nlq md+ mg+ mq+ms total mass N q -1 ideal transf'ormerratio of quartz mechanical damping of component j q -1...

Rahman, Saifur

2012-06-07T23:59:59.000Z

169

A study of a lime-free calcium arsenate and lime-free calcium arsenate mixed with organic insecticides for cotton insect control  

E-Print Network [OSTI]

between observations and the fitted line: v ( a ) = - s - W - = - E c m r ? -0 2 3 9 - E q ? ( 1 2 ) 18 a n d V ( b ) " [ J ^ " T 7 3 ^ 2 T = * 7 6 5 5 * E q * ( 1 3 ) But if chi-square indicates a significant degree of heterogeneity...) (7.U081;) = 3-5012. The portion of survivors q was substituted in equation (2a) when expected probits were greater than 5o0: y = ( Y / 2 ) - q ( i ) Eq. (2A)a F or y = 6.2812 - oBUYD (2.5700) = 5-2532. A weight value was found for each corrected...

Roussel, John Severin

2013-10-04T23:59:59.000Z

170

Bayesian multiuser detection for CDMA with nonlinear modulation  

E-Print Network [OSTI]

. The probability density Welsh code l Walsh code 2 0 C g, (') ?, (& ck &(1) Spread Walsh code l Spread Welsh code 2 Fig. 1. Result of spreading on Walsh codes for q = 1, z = 4. 'r'n& Cbm. . l W( & x (m) Welsh pnooder In(ra&eever $ Random Spreader 2.... The probability density Welsh code l Walsh code 2 0 C g, (') ?, (& ck &(1) Spread Walsh code l Spread Welsh code 2 Fig. 1. Result of spreading on Walsh codes for q = 1, z = 4. 'r'n& Cbm. . l W( & x (m) Welsh pnooder In(ra&eever $ Random Spreader 2...

Phan, Van Dao

2012-06-07T23:59:59.000Z

171

Application of Fibonacci oscillators in the Debye model  

E-Print Network [OSTI]

In this paper we study the thermodynamics of a crystalline solid by applying q-deformed algebra of Fibonacci oscillators through the generalized Fibonacci sequence of two real and independent deformation parameters q1 and q2. We find a (q1, q2)-deformed Hamiltonian and consequently the q-deformed thermodynamic quantities. The results led us to interpret the deformation parameters acting as disturbance or impurities factors modifying the characteristics of a crystal structure. More specifically, we found the possibility of adjusting the Fibonacci oscillators to describe the change of thermal conductivity of a given element as one inserts impurities.

Marinho, Andre A A; Chesman, C

2014-01-01T23:59:59.000Z

172

SustSciTeam_ProgramSummary_051611.xlsx.5/16/11 1Q 2Q 3Q Summer  

E-Print Network [OSTI]

-month) Orientation and Team Building Year 1 Sustainability Science ESS280A (4units) Independent Research XXX299 (4 units) Independent Research XXX299 (4 units) Summer Salary Sustainability Science Course; Define Team Report; Progress mtgs. Sustainability Science Team - Summary Schedule Apply to Sustainability Science

Rose, Michael R.

173

c27.xls  

Gasoline and Diesel Fuel Update (EIA)

73 73 343 512 1,465 7,716 9,570 49.5 44.4 53.5 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... Q 41 68 Q 417 729 Q 99.5 93.6 5,001 to 10,000 ................................. Q 31 43 Q 482 654 Q 64.8 66.0 10,001 to 25,000 ............................... Q 45 90 Q 931 1,681 Q 47.9 53.6 25,001 to 50,000 ............................... Q 39 70 Q 829 1,422 Q 47.4 49.5 50,001 to 100,000 ............................. Q 43 73 Q 1,263 1,554 Q 34.1 47.2 100,001 to 200,000 ........................... Q 41 67 Q 1,445 1,264 Q 28.3 52.7 200,001 to 500,000 ........................... Q 55 56 Q 1,484 1,277 Q 37.3 44.1 Over 500,000 .................................... Q 47 44 Q 865 989 Q 54.0 44.4 Principal Building Activity Education .......................................... Q 49 99 Q 1,247 1,804 Q 39.5 54.6 Food Sales .......................................

174

SHARP THRESHOLDS FOR THE RANDOM-CLUSTER AND ISING MODELS  

E-Print Network [OSTI]

SHARP THRESHOLDS FOR THE RANDOM-CLUSTER AND ISING MODELS BENJAMIN GRAHAM AND GEOFFREY GRIMMETT. The models in question are the random-cluster model near the self-dual point psd(q) = q/(1 + q), the Ising in statistical physics, namely those of the random-cluster model and the Ising model. In each case, the event

Grimmett, Geoffrey

175

The Optimal Design of Investments in Biodiversity Conservation  

E-Print Network [OSTI]

The Optimal Design of Investments in Biodiversity Conservation q1 p1 Area Price q2 p2 qd qc Paul R to terrestrial biodiversity and financial investment in habitat conservation efforts has become a cornerstone the needs of biodiversity leads to ineffective conservation programmes and may even risk conservation

Gray, Matthew

176

b11.pdf  

U.S. Energy Information Administration (EIA) Indexed Site

11,774 Q Q Q Q 1,100 2,426 8,086 Other Electronic Equipment (more than one may apply) Laser Printers ... 46,567 3,246 3,323 5,128 8,881...

177

Nonextensive effects on the relativistic nuclear equation of state  

E-Print Network [OSTI]

The Walecka many-body field theory is investigated in the context of quantum nonextensive statistical mechanics, characterized by a dimensionless parameter $q$. We consider nuclear matter described statistically by a power-law distribution which generalizes the standard Fermi-Dirac distribution ($q = 1$). We show that the scalar and vector meson fields become more intense due to the nonextensive effects ($q \

F. I. M. Pereira; R. SIlva; J. S. Alcaniz

2007-05-02T23:59:59.000Z

178

On abelian automorphism groups of Mumford curves  

Science Journals Connector (OSTI)

......P1,P2,Q1,Q2 be four distinct points on the boundary of Tk...by . Since the fixed point of in the boundary is...Let v1, v2 be two lifts of v1, v2 on the BruhatTits...have the same fixed points. Hence a lift of the edge e in TN......

Aristides Kontogeorgis; Victor Rotger

2008-06-01T23:59:59.000Z

179

A Mutant Form of the Neisseria gonorrhoeae Pilus Secretin Protein PilQ Allows Increased Entry of Heme and Antimicrobial Compounds  

Science Journals Connector (OSTI)

...grids were used to lift cells directly from...solidified GC agar. Four filter paper disks...of them carried a point mutation in hpuB...precisely the same point mutation in one...FA7186H19. The other four hgbX mutants had the...preservation of the pilQ1 point mutation. The necessity...

Ching-ju Chen; Deborah M. Tobiason; Christopher E. Thomas; William M. Shafer; H. Steven Seifert; P. Frederick Sparling

2004-02-01T23:59:59.000Z

180

Quarter 1, 2012 Page 1 of 2  

E-Print Network [OSTI]

incompatible chemicals? 16. Are incompatible chemicals segregated according to SU storage scheme? 17. Is lab-level contact. (Return roster with completed Q1-12 Self-Inspection checklist to department) 22. Our lab has. Make sure that ALL rooms listed for your PI have been included as part of this quarter's self

Ford, James

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
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to obtain the most current and comprehensive results.


181

Fluctuation theory of connectivities for subcritical random cluster models  

E-Print Network [OSTI]

Fluctuation theory of connectivities for subcritical random cluster models Massimo Campanino subcritical regime; the latter is known to be true, in any dimensions, when q = 1, q = 2, and when q. Campanino et al./Connectivities of subcritical random cluster models 2 variance principle, Ruelle operator

182

rsif.royalsocietypublishing.org Cite this article: Menguc Y, Rohrig M,  

E-Print Network [OSTI]

Institute of Technology (KIT), 76344 Eggenstein-Leopoldshafen, Germany The exceptionally adhesive foot¨lscher H, Sitti M. 2014 Staying sticky: contact self-cleaning of gecko-inspired adhesives. J. R. Soc 2014 Subject Areas: biomimetics Keywords: adhesion, gecko, self-cleaning, contactQ1 , micro

Sitti, Metin

183

Alpha-particle physics in tokamaks  

Science Journals Connector (OSTI)

...achieving ignition or high fusion gain regimes (Q 1) in a tokamak...as an example. Keywords: fusion; tokamak; energetic -particles...Self-sustained ignition of a thermonuclear plasma in a tokamak reactor...4 He ions) produced from fusion reactions. The -particles...

1999-01-01T23:59:59.000Z

184

Z .Journal of Contaminant Hydrology 51 2001 112 www.elsevier.comrlocaterjconhyd  

E-Print Network [OSTI]

in the unsaturated, fractured welded tuff Z .within the Exploratory Studies Facility ESF at Yucca Mountain, NV repository at Yucca Mountain. While fast and localized fracture flow has ) Corresponding author. Fax: q1 continuum model for simulating transient flow and transport at Yucca Mountain. An extensive set

Hu, Qinhong "Max"

185

AN OPTIMAL ITERATIVE METHOD FOR THE TIME-DEPENDENT STOKES PROBLEM  

E-Print Network [OSTI]

well for the Mini element. Numerical experiments indicate that this preconditioner also works for the Q will propose a preconditioner which is uniform in " and h, where h is the grid size parameter. The system (2 at least the Mini element and seemingly the Q 2 Q 1 element possess. We notice that the " parameter only

186

ITC-12/APFA'01 December 10-14, 2001  

E-Print Network [OSTI]

) Electricity Generation Equivalent Q > 1 ~ Advanced Tokamak Study Reactor Technologies Core Program/NIFSUniversities/NIFS STASTA JAERI/Nat. Labs.JAERI/Nat. Labs. MEXTMEXT Ministry of Education,Ministry of Education, CultureMagneto-- electric/Magnetelectric/Magnet System/SafetySystem/Safety ICFICF Structural MaterialsStructural Materials

187

--No Title--  

U.S. Energy Information Administration (EIA) Indexed Site

2,711 1,916 1,197 2,649 942 1,565 973 1,638 Heating Equipment (more than one may apply) Heat Pumps ... 8,814 Q 1,019 719 339 3,677 542 722 333...

188

Energy Information Administration - Commercial Energy Consumption...  

Annual Energy Outlook 2013 [U.S. Energy Information Administration (EIA)]

Q 375 261 764 2,711 1,916 161.3 138.2 136.1 Heating Equipment (more than one may apply) Heat Pumps ... Q 141 68 Q 1,019 719 Q 137.9 94.1 Packaged...

189

--No Title--  

U.S. Energy Information Administration (EIA) Indexed Site

386 276 Q Q 68 3,210 1,767 Q Q 1,068 Heating Equipment (more than one may apply) Heat Pumps ... 476 N 37 61 378 8,814 N 670 1,497 6,647...

190

b34.xls  

Gasoline and Diesel Fuel Update (EIA)

386 276 Q Q 68 3,210 1,767 Q Q 1,068 Heating Equipment (more than one may apply) Heat Pumps ... 476 N 37 61 378 8,814 N 670 1,497 6,647...

191

--No Title--  

Gasoline and Diesel Fuel Update (EIA)

29 24 28 1,177 931 1,401 24.4 26.0 19.8 Heating Equipment (more than one may apply) Heat Pumps ... 12 Q 17 722 Q 1,268 16.2 Q 13.4 Packaged...

192

--No Title--  

Annual Energy Outlook 2013 [U.S. Energy Information Administration (EIA)]

58 134 75 1,284 3,076 1,551 45.5 43.5 48.6 Heating Equipment (more than one may apply) Heat Pumps ... Q 66 17 Q 1,947 373 Q 33.8 45.1 Packaged...

193

Dynamics of plasma formation during quasicontinuous laser irradiation of metals in high-pressure nitrogen atmospheres  

Science Journals Connector (OSTI)

This is a study of target destruction and the dynamics of surface plasma formation during the interaction of quasicontinuous laser...q = 17 MW/cm2..., ? ? 1.5 msec) with D16T duraluminum and bismuth in nitrogen

V. I. Nasonov; Yu. A. Chivel

2009-11-01T23:59:59.000Z

194

Dualities and Topological Field Theories from Twisted Geometries  

E-Print Network [OSTI]

modes on the D2-brane and F1-strings for (a) Sectors 1 anda) A fundamental string (F1) bound to the D2-brane. The D2-12 q 13 ? q 1m SR q 23 F1 q 20 q 21 q 22 q 2m SR F1 q

Markov, Ruza

2012-01-01T23:59:59.000Z

195

Contemporary Mathematics Algebraic Multigrid and Schur Complement Strategies  

E-Print Network [OSTI]

form: ut + g = F(1.1) t + · [(h + )u] = Q(1.2) where u = (u, v) is the velocity vector, is the sea acceleration, h is the resting depth of the fluid, Q is a mass source/sink term. The vector F = (fx , fy, viscous dissipation, and wind forcing. For simplicity, we assume no-slip boundary conditions. The shallow

Douglas, Craig C.

196

A Combinatorial Model for the Macdonald Polynomials Department of Mathematics  

E-Print Network [OSTI]

A Combinatorial Model for the Macdonald Polynomials J. Haglund Department of Mathematics University that ? C µ [Z; q, t] is none other than the modified Macdonald polynomial ? H µ [Z; q, t]. We further partition, set ? K #,µ (q, t) = t #(µ) K #,µ (q, 1/t), where K #,µ (q, t) is Macdonald's q, t

Haglund, Jim

197

A Combinatorial Model for the Macdonald Polynomials Department of Mathematics  

E-Print Network [OSTI]

A Combinatorial Model for the Macdonald Polynomials J. Haglund Department of Mathematics University, t] is none other than the modified Macdonald polynomial ~Hµ[Z; q, t]. We further introduce a general,µ(q, t) = t(µ)K,µ(q, 1/t), where K,µ(q, t) is Macdonald's q, t-Kostka polynomial [Mac95, p.354]. We call

Haglund, Jim

198

ukasiewicz Logic: From Proof Systems To Logic Programming  

Science Journals Connector (OSTI)

......n, n ? n)}, a contradiction. The next step is to show that all valid atomic (and hence also irreducible) queries suc- ceed in GDL. To this end we introduce a translation from irreducible queries containing propositional variables q1, . . . , qn into......

George Metcalfe; Nicola Olivetti; Dov Gabbay

2005-09-01T23:59:59.000Z

199

National Institutes of Health Q&A Transcript  

E-Print Network [OSTI]

how different parts of the brain work! Below is a description of the brain's lobes and their primary functions, followed by 12 questions and answers. The four brain lobes and their primary functions are. It also affects brain functions such as memory and emotion. Q1. Which part of the brain enables you

Baker, Chris I.

200

BY STEVEN P. LANZA Connecticut's 7,000-job addition  

E-Print Network [OSTI]

BY STEVEN P. LANZA Connecticut's 7,000-job addition in 2012-Q1 was opportune, as the Bureau the historical relationship between U.S. GDP and Connecticut job growth, and taking into account the state economy's recent dynamics, Connecticut can expect to add jobs at a rate of about 2,900 quarterly or nearly

Holsinger, Kent

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


201

Solutions to the non-autonomous ABS lattice equations: Casoratians and bilinearization  

E-Print Network [OSTI]

In the paper non-autonomous H1, H2, H3$_\\delta$ and Q1$_\\delta$ equations in the ABS list are bilinearized. Their solutions are derived in Casoratian form. We also list out some Casoratian shift formulae which are used to verify Casoratian solutions.

Ying Shi; Da-jun Zhang; Song-lin Zhao

2012-01-31T23:59:59.000Z

202

Potential Energy Total electric potential energy, U, of a system of  

E-Print Network [OSTI]

Potential Energy Total electric potential energy, U, of a system of charges is obtained from of work done by the field, W*= -W. Bring q1 from , W *= 0 since no electric F yet #12;Potential Energy Total electric potential energy, U, of a system of charges is obtained from the work done by an external

Bertulani, Carlos A. - Department of Physics and Astronomy, Texas A&M University

203

CAT: Correct Answers of Continuous Queries Using Triggers  

E-Print Network [OSTI]

down the speed between 4:30PM and 9:30PM. Tr1 enters that segment after 4:30PM, and its future portion, issued the query Q1, we have to re-evaluate the answer. Research partially supported by NSF grant EIA-000

Scheuermann, Peter

204

Machine Learning as an Objective Approach to Understanding Musical Origin  

E-Print Network [OSTI]

Machine Learning as an Objective Approach to Understanding Musical Origin Claire Q1 and Ross King2 1 Aberystwyth University, UK, ceq08@aber.ac.uk 2 Manchester University, UK, ross of pieces of music. We collected 1,142 pieces of music from 73 countries, and described them using 2

Malerba, Donato

205

BIO321-Lec10 The cell...  

E-Print Network [OSTI]

-lectins #12;Protein export/secretion is essential for life #12;Q1:How do proteins cross lipid bilayers;...composed of phopholipids in out H20 H20 Lipid #12;...that form a dynamic bilayer H2O H2O headgroups headgroups Hydrocarbon chains Lipid bilayer in out H20 H20 Lipid #12;Bird's eye view of a sea of lipids

Economou, Tassos

206

ELEC3028 Digital Transmission Overview & Information Theory S Chen Revision of Lecture 2  

E-Print Network [OSTI]

(symbols/s) information rate: R = Rs · H (bits/s) · Code each symbol by log2 q bits (BCD), then data rate Rs · log2 q > R, unless source is equal probable pi = 1/q, 1 i q · How to code symbols is coded ­ For example, samples of speech waveform are correlated; redundancy in samples is first removed

Chen, Sheng

207

INSTITUTE OF PHYSICS PUBLISHING PLASMA PHYSICS AND CONTROLLED FUSION Plasma Phys. Control. Fusion 47 (2005) 13671377 doi:10.1088/0741-3335/47/9/001  

E-Print Network [OSTI]

. They develop in the presence of a value of the safety factor q = 1: the nested magnetic flux surfaces]. Magnetic islands either accompany sawtooth activity [4] or are in the form of persistent (`snake proved very successful in describing temperature oscillations in several situations [4,14,15], it cannot

Zonca, Fulvio

208

Total Space Heating Water Heating Cook-  

Gasoline and Diesel Fuel Update (EIA)

Q Q Q Q Q Q Q Q Q Q Food Service ... Q Q Q Q Q Q Q Q Q Q Health Care ... 11 6 2 Q 2 5.6 3.3 0.8 Q 1.3 Inpatient...

209

Question and Answers Alternative Fuel Readiness Plans  

E-Print Network [OSTI]

Question and Answers Alternative Fuel Readiness Plans PON-13-603 September 3, 2013 Eligibility Q1 to readiness plans? A1 This solicitation is limited to readiness planning only for alternative fuels. Q2 In regards to PON-13-603 - Alternative Fuel Readiness Plans, is electricity used for transportation

210

SC  

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

ROW * Wastesites 1221 Other Set-Asides r:;c::J Areas B Hydric Soils D Three Rivers Landfill N A o o 660 Meters * CompartQ1enLJJ o 330 o 0 o o "0 ro o a: ..c:: O CO Soil...

211

A Cross-Flow Ceramic Heat Recuperator for Industrial Heat Recovery  

E-Print Network [OSTI]

recuperators currently available suffer from problems of creep, corrosion and oxidation, particularly at high temperatures. The Department of Energy and GTE Products corporation have pursued a jointly funded venture, Contract No. EX-76-C-Q1-2162, to establish...

Gonzalez, J. M.; Cleveland, J. J.; Kohnken, K. H.; Rebello, W. J.

1980-01-01T23:59:59.000Z

212

b14.xls  

U.S. Energy Information Administration (EIA) Indexed Site

64,783 64,783 12,208 3,939 1,090 3,754 4,050 10,078 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 1,382 336 122 416 1,034 895 5,001 to 10,000 ................................. 6,585 938 518 Q 744 722 868 10,001 to 25,000 ............................... 11,535 1,887 1,077 Q 1,235 1,021 2,064 25,001 to 50,000 ............................... 8,668 1,506 301 Q 930 560 1,043 50,001 to 100,000 ............................. 9,057 1,209 474 Q Q Q 1,494 100,001 to 200,000 ........................... 9,064 1,428 868 Q Q Q 1,162 200,001 to 500,000 ........................... 7,176 1,493 Q Q Q Q 1,322 Over 500,000 .................................... 5,908 2,365 Q Q N Q Q Year Constructed Before 1920 ...................................... 3,769 749 323 Q 586 Q 254 1920 to 1945 .....................................

213

An inverse scheme for sensitivity and uncertainty analysis in basin modeling: the resolution limits of Easy%Ro  

E-Print Network [OSTI]

, Mona-1 , Sten-1 and Q-1 wells located in the Danish Central Trough, in the North Sea. A range of geothermal gradients are investigated using the model. As a quantitative measure of mismatch between modeled and measured values, the mean squared residual...

Huvaz, Ozkan

2012-06-07T23:59:59.000Z

214

On bounding the bandwidth of graphs with symmetry - Optimization ...  

E-Print Network [OSTI]

Hamming graph H(2,q) (also known as the lattice graph) has bandwidth equal to. (q+1)q. 2. ?1 .... 59. 10 3 120. 72. 75. 76. 90. Table 9: Bounds on the bandwidth of K(v,2) and K(v,3). v d meig .... Freeman, San Francisco, 1979. [19] Graham, A.

2013-08-08T23:59:59.000Z

215

Page not found | Department of Energy  

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

691 - 31700 of 31,917 results. 691 - 31700 of 31,917 results. Rebate Renewables Portfolio Standard Note: In July 2012 New Jersey enacted S.B. 1925 substantially revising its solar carve-out. The summary below incorporates information on the changes made to the solar carve-out as well as the... http://energy.gov/savings/renewables-portfolio-standard-7 Download FOIA Quarterly Reports (Q1 2013) The DOE's mission is to advance the national, economic, and energy security of the United States; to promote scientific and technological innovation in support of that mission; and to ensure the... http://energy.gov/management/downloads/foia-quarterly-reports-q1-2013 Download Environmental Justice Interagency Collaborative Newsletter Volume 1 The inaugural edition of the Environmental Justice Interagency

216

Page not found | Department of Energy  

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

41 - 18450 of 28,905 results. 41 - 18450 of 28,905 results. Download Develop baseline computational model for proactive welding stress management to suppress helium induced cracking during weld repair There are over 100 nuclear power plants operating in the U.S., which generate approximately 20% of the nation's electricity. These plants range from 15 to 40 years old. Extending the service lives... http://energy.gov/ne/downloads/develop-baseline-computational-model-proactive-welding-stress Download FOIA Quarterly Reports (Q1 2013) The DOE's mission is to advance the national, economic, and energy security of the United States; to promote scientific and technological innovation in support of that mission; and to ensure the... http://energy.gov/management/downloads/foia-quarterly-reports-q1-2013

217

b19.xls  

U.S. Energy Information Administration (EIA) Indexed Site

4,645 4,645 3,754 643 55 23 14 157 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,552 2,131 311 Q Q N 100 5,001 to 10,000 ................................. 889 720 136 Q N Q Q 10,001 to 25,000 ............................... 738 590 104 22 Q Q Q 25,001 to 50,000 ............................... 241 163 50 11 Q Q Q 50,001 to 100,000 ............................. 129 87 25 4 5 Q Q 100,001 to 200,000 ........................... 65 43 11 4 Q Q Q 200,001 to 500,000 ........................... 25 15 5 Q 1 2 Q Over 500,000 .................................... 7 3 1 Q Q 1 Q Principal Building Activity Education .......................................... 386 360 21 Q N N N Food Sales ....................................... 226 203 Q N N Q N Food Service ..................................... 297 270 26 Q N N N Health Care .......................................

218

New Beam Delivery System Optics: BDS9901 Peter Tenenbaum LCC-Note-0020  

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

Beam Beam Delivery System Optics: BDS9901 Peter Tenenbaum LCC-Note-0020 14-July-1999 Abstract We describe in detail the optics and XSIF decks for the NLC Beam Delivery System in its present version, BDS9901. 1 Introduction In this Note, we describe the present optics design of the NLC Beam Delivery System, which has been somewhat revised for 1999. Most important optical changes include: * Organization of BPMs into quad-style (BPMQ), BPMs in feedback loops (BPMFB), BPMs which provide sub-train/multibunch information (BPMMB), and BPMs used to measure beam-beam deflections (BPMIP) * Addition of a number of small quad, skew-quad, sextupole, and skew-sextupole tuning mag- nets * Addition of actuators for the feedbacks * A 6-quadrupole final telescope, which allows all of the linear degrees of freedom to be opti- mized * Replacement of the low-energy final quads Q1A and Q1B with a single

219

high  

Gasoline and Diesel Fuel Update (EIA)

0 0 Summary Our short-term outlook for a wide array of energy prices has been adjusted upward as international and domestic energy supply conditions have tightened. We think that crude oil prices are as likely as not to end the year $2 to $3 per barrel higher than our previous projections. Thus, we think that the probability of West Texas Intermediate costing an average of $30 per barrel or more at midwinter is about 50 percent. On their current track, heating oil prices are likely to be about 30 percent above year-ago levels in the fourth quarter. Prices for Q1 2001 seem more likely now to match or exceed the high level seen in Q1 2000. Tight oil markets this year and an inherent propensity for high gas utilization in incremental power supply have resulted in rising North American natural gas

220

Structural and electronic properties of the quasi-one-dimensional metallic chains of the Au-induced facets on the Si(5 5 12) surface  

Science Journals Connector (OSTI)

We have investigated the atomic arrangements and electronic properties of the quasi-one-dimensional (Q1D) atomic chains of the Au-induced facets formed on the clean Si(5 5 12)-21 surface. The interchain distances of the two well ordered facet structures are estimated to be 30.2 and 22.8 . By utilizing linearly polarized synchrotron photons, we also determine a complete band diagram of the surface bands and their symmetry characteristics along the two high symmetry azimuths (?-M and ?-X) of the surface Brillouin zone. The Q1D nature of the Au-induced atomic chains has been well demonstrated by the extremely anisotropic band dispersions of the Au-induced surface bands in addition to the 21 surface morphology. We find that while the clean reconstructed Si(5 5 12)-21 surface is insulating, the Au-induced chains form a highly anisotropic metallic system.

S. S. Lee; N. D. Kim; C. G. Hwang; H. J. Song; J. W. Chung

2002-09-23T23:59:59.000Z

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


221

Distribution of stresses in a tapered cantilever beam due to a concentrated load at the end  

E-Print Network [OSTI]

- To dctc5$1BS Oy 8$ 2~ 4858idsx' gigugo 14 {c, ) Oy 4P' = Oy Gy Care~n)4. y Fgy (Rc g?) P Zxy (Xg~~)ton OC (g) Other apprcndsmLte methods may be used for the datexminatim of the stresses at any points but they do not lend themselves as wQ1...- To dctc5$1BS Oy 8$ 2~ 4858idsx' gigugo 14 {c, ) Oy 4P' = Oy Gy Care~n)4. y Fgy (Rc g?) P Zxy (Xg~~)ton OC (g) Other apprcndsmLte methods may be used for the datexminatim of the stresses at any points but they do not lend themselves as wQ1...

Wilhoit, James Cammack

2012-06-07T23:59:59.000Z

222

Sawtooth stabilization by localized electron cyclotron heating in a tokamak plasma  

Science Journals Connector (OSTI)

Sawtooth oscillations (STO) in the Ohmically heated WT-3 tokamak are strongly modified or suppressed by localized-electron cyclotron resonance heating (ECH) near the q=1 surface, where q refers to the safety factor. The efect of ECH is much stronger when it is applied on the high-field side as compared to the low-field side. Complete suppression of the STO is achieved for the duration of the ECH, in most cases, when it is applied on the high-field side of a low-density plasma, provided the ECH power exceeds a threshold value. The STO stabilization is attributed to a modification of the current-density profile by hot electrons generated by ECH, which reduces the shear in the q=1 region.

K. Hanada; H. Tanaka; M. Iida; S. Ide; T. Minami; M. Nakamura; T. Maekawa; Y. Terumichi; S. Tanaka; M. Yamada; J. Manickam; R. B. White

1991-04-15T23:59:59.000Z

223

A study of laser annealing effects in boron ion implanted polycrystalline silicon films  

E-Print Network [OSTI]

/cm 15 2 65 Q=1x10 /cm 15 2 Q=5x10 /cm 15 2 65 24 34. 8 25 35 Nethod 1: Ion implanted before Hall pattern was defined. Nethod 2 : Hall pattern was defined before ion implantation. + All ps and pH values are average of 3 readings. Individual... N. M = NOT measurable with Hall effect analyzer STANDARD SAMPLE R = 3. 378 1 R2 = 3. 478 b, V = . 2mV at I = 5. 6mA ~ B = 4. 5 KG d. R pH =? Bx Ps Ps = 15. 536 A/a 45 Orate Q 1KHz 3 KHz eak 225W 161W 10 T. A. at 1000 0 P=-46K n/Q Q...

Suh, Inhak Harry

1982-01-01T23:59:59.000Z

224

Neutron-Spin Resonance in the Optimally Electron-Doped Superconductor Nd{sub 1.85}Ce{sub 0.15}CuO{sub 4-{delta}}  

SciTech Connect (OSTI)

We use inelastic neutron scattering to probe magnetic excitations of an optimally electron-doped superconductor Nd{sub 1.85}Ce{sub 0.15}CuO{sub 4-{delta}} above and below its superconducting transition temperature T{sub c}=25 K. In addition to gradually opening a spin pseudogap at the antiferromagnetic ordering wave vector Q=(1/2,1/2,0), the effect of superconductivity is to form a resonance centered also at Q=(1/2,1/2,0) but at energies above the spin pseudogap. The intensity of the resonance develops like a superconducting order parameter, similar to those for hole-doped superconductors and electron-doped Pr{sub 0.88}LaCe{sub 0.12}CuO{sub 4}. The resonance is therefore a general phenomenon of cuprate superconductors, and must be fundamental to the mechanism of high-T{sub c} superconductivity.

Zhao Jun; Li Shiliang [Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996-1200 (United States); Dai Pengcheng [Department of Physics and Astronomy, University of Tennessee, Knoxville, Tennessee 37996-1200 (United States); Neutron Scattering Sciences Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831-6393 (United States); Freeman, Paul G. [Institut Laue-Langevin, 6, rue Jules Horowitz, BP156-38042 Grenoble Cedex 9 (France); Onose, Y. [Spin Superstructure Project, ERATO, Japan Science and Technology, Tsukuba 305-8562 (Japan); Tokura, Y. [Spin Superstructure Project, ERATO, Japan Science and Technology, Tsukuba 305-8562 (Japan); Department of Applied Physics, University of Tokyo, Tokyo 13-8656 (Japan)

2007-07-06T23:59:59.000Z

225

Resonance in Optimally Electron-Doped Superconductor Nd1.85Ce0.15CuO4??  

SciTech Connect (OSTI)

We use inelastic neutron scattering to probe magnetic excitations of an optimally electron-doped superconductor Nd1.85Ce0.15CuO4? above and below its superconducting transition temperature Tc = 25 K. In addition to gradually opening a spin pseudo gap at the antiferromagnetic ordering wavevector Q = (1/2, 1/2, 0), the effect of superconductivity is to form a resonance centered also at Q = (1/2, 1/2, 0) but at energies above the spin pseudo gap. The intensity of the resonance develops like a superconducting order parameter, similar to those for hole-doped superconductors and electron-doped Pr0.88LaCe0.12CuO4. The resonance is therefore a general phenomenon of cuprate superconductors, and must be fundamental to the mechanism of high-Tc superconductivity.

Zhao, Jun [ORNL; Dai, Pengcheng [ORNL; Li, Shiliang [University of Tennessee, Knoxville (UTK); Freeman, Paul G. [Institut Laue-Langevin (ILL); Onose, Y,. [Spin Superstructure Project, ERATO, Japan Science and Technology, Tsukuba 305-85; Tokura, Y. [University of Tokyo, Tokyo, Japan

2007-01-01T23:59:59.000Z

226

Fuzzy transformations and extremality of Gibbs measures for the Potts model on a Cayley tree  

E-Print Network [OSTI]

We continue our study of the full set of translation-invariant splitting Gibbs measures (TISGMs, translation-invariant tree-indexed Markov chains) for the $q$-state Potts model on the Cayley tree. In our previous work we gave the full description of the TISGMs, and showed in particular that at sufficiently low temperatures their number is $2^{q}-1$. In this paper we find some regions for the temperature parameter ensuring that a given TISGM is (non-)extreme in the set of all Gibbs measures. In particular we show the existence of a temperature interval for which there are at least $2^{q-1} + q$ extremal TISGMs. For the Cayley tree of order two we give explicit formulae and some numerical values.

C. Kuelske; U. A. Rozikov

2014-03-23T23:59:59.000Z

227

Investor Confidence Project  

E-Print Network [OSTI]

projects (under $1MM), Lighter engineering requirements V1 Released September 2013 Targeted Commercial Single Measure or Non-Interactive Retrofits Release Date Dec 2013 Multifamily Release Q1 2014 Quality Assurance Protocol Currently in BETA...Environmental Defense Funds Investor Confidence Project Delivering Investment Quality Energy Efficiency to Market ESL-KT-13-12-38 CATEE 2013: Clean Air Through Energy Efficiency Conference, San Antonio, Texas Dec. 16-18 Investor Confidence Project...

Golden, M.

2013-01-01T23:59:59.000Z

228

INFINITE GENERATION FOR RINGS OF SYMMETRIC TENSORS  

E-Print Network [OSTI]

N.I. Shepherd-Barron DPMMS, 16 Mill Lane, Cambridge CB2 1SB, UK If X.I. SHEPHERD-BARRON Put x = Xe, and let p, q : Xe ! be the two projections; then 1eX~= p* 1 q* 1 as -linearized bundles, so that by descent 1X ~=O(A) O(B) for some divisor classes A, B on X. Lemma 1. h0(O

Shepherd-Barron, Nick

229

May 28-29, 2008/ARR Thermal Effect of Off-Normal Energy  

E-Print Network [OSTI]

#12;May 28-29, 2008/ARR 2 Power Plant FW Under Energy Deposition from Off- Normal Conditions · Thermal for Power Plant with Bare FS FW · Disruption simulation: q''=1.667 x 109 W/m2 over 3 ms (~5 MJ/m2) · 4+1 mm impact of off-normal events on power plant FW presented before for SiC and W · Questions arise

Raffray, A. René

230

Location of ray paths for a known wave normal in biaxial crystals  

Science Journals Connector (OSTI)

...In an arbitrary frarneof reference,the tensorequationthat relatesD andE is: (20) TABLE 1.E)(AMPLE oFTHECAIfUn-IIONS K11K12K13 K2LK,2K23 K31K32K33 whereD, andQ arethe componentsof D andE in the arbitraryframeof reference,andtheQ1arethecompo-nents...

James Nicholls

231

IEIITIEIIT--CNRCNR 1 Introduction to Robustness and  

E-Print Network [OSTI]

of Mini-UAV - wingspan 1000 mm - maximum take-off weight 1500 g - DC motor - remote piloting For the Mini-UAV we set some specifications (system property) ExamplesExamples:: 1. Flight speed in the range Rectangle Q q1 q2 1.2 1.7 1.7 2.2 #12;IEIIT-CNR ©© IEIITIEIIT--CNRCNR 16 Grid Approach Suppose we follow

Tempo, Roberto

232

COEFFICIENTS OF EXPONENTIAL FUNCTIONS ATTACHED TO DRINFELD MODULES OF RANK 2  

E-Print Network [OSTI]

author and supported by Priority Research Centers Program through the NRF funded by the Ministry of Education, Science and Technology(2010-0028298) and by the NRF grant funded by the Korea government formulae for the di's. d0 = 0, d1 = v(a1) q + 1 + d0, di min v(a1) qi + di-1, v(a2) qi + di-2 + 1 for i 2

Chen, Imin

233

HODGE-THEORETIC INVARIANTS FOR ALGEBRAIC CYCLES MARK GREEN AND PHILLIP GRIFFITHS  

E-Print Network [OSTI]

) Spreads; explanation of the idea (3) Construction of the filtration on CHp (X)Q (4) Interpretations, these conjectures would have the following implications for the Chow group CHP (X)Q: (I) There is a filtration CHp (X)Q = F0 CHp (X)Q F1 CHp (X)Q(1.1) · · · Fp CHp (X)Q Fp+1 CHp (X)Q = 0 whose successive

234

Name: Entry: Gp: 1 Indian Institute of Technology, Delhi  

E-Print Network [OSTI]

relation R #18; A#2;A is an equivalence. R = f (a; b) : f(a) = f(b) g Re exivity: for all a 2 S : (a; a) 2 Marks: 80 Q1 [8 Marks] Equivalences. Suppose f : A ! B is a total function. Prove that the following(c). By transitivity of equality, f(a) = f(c), whence (a; c) 2 R. Q2 [8+8 Marks] Partial Orders. In a partial order h

Prasad, Sanjiva

235

The SeventhAsian Congressof Fluid Mechanics Dec8 -12, 1997,Chennai (Madras)  

E-Print Network [OSTI]

S~A~q~M'V"S!duI"Spoq1~wOM1~q1jOf.:)U~1S!stia:,~~qS!lq~1S~ --1u~II~:)x~~qL"~~:)J~!IJv.~~q101p~Jv.dwo:)P~1~:)!ldwo:)001Jv

Mittal, Sanjay

236

Dimensions: Sketching Piotr  

E-Print Network [OSTI]

structures 2 Dimensionality Reduction in HammingMetric Theorem: For any r and eps>0 (small enough: -- If D(p,q)eps/10)t -- If D(p,q)>(1+eps)r then D(G(p), G(q)) >(c+eps/20)t is at least 1­P, as long as t=C*log(2/P)/eps 2 , C large constant. . Given n points, we can reduce

237

Statistical Power-Law Spectra due to Reservoir Fluctuations  

E-Print Network [OSTI]

LHC ALICE data are interpreted in terms of statistical power-law tailed pT spectra. As explanation we derive such statistical distributions for particular particle number fluctuation patterns in a finite heat bath exactly, and for general thermodynamical systems in the subleading canonical expansion approximately. Our general result, $q = 1 - 1/C + \\Delta T^2 / T^2$, demonstrates how the heat capacity and the temperature fluctuation effects compete, and cancel only in the standard Gaussian approximation.

T. S. Bir; G. G. Barnafldi; P. Vn; K. rmssy

2014-04-04T23:59:59.000Z

238

UNCORRECTED 2 Efficient and scalable provisioning of always-on multicast  

E-Print Network [OSTI]

a MPI-SWS, Germany 6 b Rutgers University, USA 7 c AT&T Labs ­ Research, USA 8 d KAIST, KoreaQ1 9 1 1 a r t i c l e i n f o 12 Article history: 13 Received 30 May 2008 14 Received in revised form 24 June Stock 63Exchange now distributes the stock price update ticker over 64an IP network [7]. As a third

Moon, Sue B.

239

McMaster University Libraries library.mcmaster.ca 905.525.9140 x22533 library@mcmaster.ca Sociology 1A06  

E-Print Network [OSTI]

________________________________________________________________________________________________ McMaster University Libraries · library.mcmaster.ca · 905.525.9140 x22533 · library@mcmaster.ca! ________________________________________________________________________________________________ McMaster University Libraries · library.mcmaster.ca · 905.525.9140 x22533 · library@mcmaster.ca Your ________________________________________________________________________________________________ McMaster University Libraries · library.mcmaster.ca · 905.525.9140 x22533 · library@mcmaster.ca Q1

Haykin, Simon

240

Journal ofNon-CrystallineSolids137&138(1991)531-534 North-Holland  

E-Print Network [OSTI]

technique with both 2eV and 4eV photons to generate and probe directly hot carriers with considerable excess discharge reactor. This procedure results in the growth of high quality a-Ge:H films exhibiting improved- % % (los) -3 v Q 1 (a) (b) I I I I 2 3 4 % % (ps) FIGURE 1 Comparison of decays in Ae1 in a-Si:H for 4e

Schiff, Eric A.

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


241

Polynomial Relations between Polynomial Roots Gerd Baron, Michael Drmota, and Mariusz Ska lba 1  

E-Print Network [OSTI]

; : : : ; xn . Suppose that #23; #20; n and that P (X 1 ; : : : ; X #23; ) 2 K[X 1 ; : : : ; X #23; ] is a polynomial in #23; variables such that P (x 1 ; : : : ; x #23; ) = 0: Then P (X 1 ; : : : ; X #23; ) has a representation of the form P (X 1 ; : : : ; X #23; ) = f 1 (X 1 )q 1 (X 1 ; : : : ; X #23; ) + f 2 (X 1 ; X 2 )q

Drmota, Michael

242

Thermal distributions in stellar plasmas, nuclear reactions and solar neutrinos  

E-Print Network [OSTI]

The physics of nuclear reactions in stellar plasma is reviewed with special emphasis on the importance of the velocity distribution of ions. Then the properties (density and temperature) of the weak-coupled solar plasma are analysed, showing that the ion velocities should deviate from the Maxwellian distribution and could be better described by a weakly-nonexstensive (|q-1|solar neutrino fluxes, and on the pp neutrino energy spectrum, and analyse the consequences for the solar neutrino problem.

M. Coraddu; G. Kaniadakis; A. Lavagno; M. Lissia; G. Mezzorani; P. Quarati

1998-11-24T23:59:59.000Z

243

BIO1502/1403 Proteins in the cell  

E-Print Network [OSTI]

! ! ! !-hormones! #12;Protein! export/secretion! is essential ! for life! #12;Q1:How do proteins ! cross! lipid of phopholipids! in! out! H!2!0! H!2!0! Lipid #12;...that form a dynamic bilayer! H2O! H2O! headgroups! headgroups! Hydrocarbon! chains! Lipid bilayer! in! out! H!2!0! H!2!0! Lipid #12;Birds eye view of a sea of lipids

Economou, Tassos

244

Transmission Information  

E-Print Network [OSTI]

(symbols/s) information rate: R = Rs ·H (bits/s) . Code each symbol by log 2 q bits (BCD), then data rate Rs · log 2 q > R, unless source is equal probable pi = 1/q, 1 # i # q . How to code symbols in an e that the signal exhibits some form of redundancy, which should be exploited when the signal is coded

Chen, Sheng

245

The 4000-3400A S02 vibration spectrum with long absorbing paths  

E-Print Network [OSTI]

~ Of the eyeetrngreyh ~rating n oae a+noted te refloat light fxoo tho loxp ~ tbe?ido open slit 8 onto plane sdxror tL?~ N~ nas xn11ostsd to oonter the r?floated bono ca R x and pries Rapzssaed te ebs nearest eea4iaeteri LL ~ prh pg 4 p1~tL Q1wcLnste ths socaen...

Russell, Ralph Keith

1954-01-01T23:59:59.000Z

246

06-02552 Princ. of Progr. Languages (and "Extended") The University of Birmingham Autumn Semester 2014-15 School of Computer Science  

E-Print Network [OSTI]

the quotient q and remainder r of given integers a and b, and prove its correctness using assertion(A = a && B = b && a 0 && b > 0); Q := 0; R := A; invariant(R = a-(b*Q) && 0 R); while (R B) do { Q := Q+1; R := R-B; } assert(R = a-(b*Q) && 0 R R = a-(b*Q) as our main invariant, taken

Reddy, Uday S.

247

Advanced, Low/Zero Emission Boiler Design and Operation  

SciTech Connect (OSTI)

In partnership with the U.S. Department of Energy's National Energy Technology Laboratory, B&W and Air Liquide are developing and optimizing the oxy-combustion process for retrofitting existing boilers as well as new plants. The main objectives of the project is to: (1) demonstrate the feasibility of the oxy-combustion technology with flue gas recycle in a 5-million Btu/hr coal-fired pilot boiler, (2) measure its performances in terms of emissions and boiler efficiency while selecting the right oxygen injection and flue gas recycle strategies, and (3) perform technical and economic feasibility studies for application of the technology in demonstration and commercial scale boilers. This document summarizes the work performed during the period of performance of the project (Oct 2002 to June 2007). Detailed technical results are reported in corresponding topical reports that are attached as an appendix to this report. Task 1 (Site Preparation) has been completed in 2003. The experimental pilot-scale O{sub 2}/CO{sub 2} combustion tests of Task 2 (experimental test performance) has been completed in Q2 2004. Process simulation and cost assessment of Task 3 (Techno-Economic Study) has been completed in Q1 2005. The topical report on Task 3 has been finalized and submitted to DOE in Q3 2005. The calculations of Task 4 (Retrofit Recommendation and Preliminary Design of a New Generation Boiler) has been completed in 2004. In Task 6 (engineering study on retrofit applications), the engineering study on 25MW{sub e} unit has been completed in Q2, 2008 along with the corresponding cost assessment. In Task 7 (evaluation of new oxy-fuel power plants concepts), based on the design basis document prepared in 2005, the design and cost estimate of the Air Separation Units, the boiler islands and the CO{sub 2} compression and trains have been completed, for both super and ultra-supercritical case study. Final report of Task-7 is published by DOE in Oct 2007.

Babcock/Wilcox; Illinois State Geological; Worley Parsons; Parsons Infrastructure/Technology Group

2007-06-30T23:59:59.000Z

248

b4.xls  

U.S. Energy Information Administration (EIA) Indexed Site

East East South Central West South Central Mountain Pacific All Buildings* .................................. 4,645 233 493 696 571 874 348 553 299 580 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,552 127 237 369 356 457 215 294 165 333 5,001 to 10,000 ................................. 889 48 101 117 97 189 56 116 56 110 10,001 to 25,000 ............................... 738 37 90 122 75 139 51 88 54 81 25,001 to 50,000 ............................... 241 10 26 44 27 47 15 26 14 32 50,001 to 100,000 ............................. 129 7 21 24 10 21 10 18 5 13 100,001 to 200,000 ........................... 65 3 12 12 5 16 Q 8 Q 6 200,001 to 500,000 ........................... 25 Q 6 6 1 4 Q 2 1 3 Over 500,000 .................................... 7 Q 1 1 Q 1 Q Q Q 1 Principal Building Activity Education ..........................................

249

Total Space Heating Water Heating Cook-  

Gasoline and Diesel Fuel Update (EIA)

28 28 198 18 Q 10 14.0 12.2 1.1 Q 0.6 Building Floorspace (Square Feet) 1,001 to 5,000 ........................... 34 32 Q (*) Q 56.9 52.2 Q (*) Q 5,001 to 10,000 .......................... 36 33 Q (*) Q 49.4 44.7 Q 0.1 Q 10,001 to 25,000 ........................ 28 25 1 (*) Q 26.7 23.8 1.4 0.1 Q 25,001 to 50,000 ........................ 17 16 Q (*) 1 19.1 17.8 Q (*) 0.6 50,001 to 100,000 ...................... 29 26 1 Q 1 15.6 14.1 0.7 Q 0.5 100,001 to 200,000 .................... 37 35 Q Q 1 12.5 11.5 Q Q 0.5 200,001 to 500,000 .................... 36 25 Q Q 2 10.5 7.4 2.4 Q 0.5 Over 500,000 ............................. 10 Q Q Q 2 2.1 Q Q Q 0.4 Principal Building Activity Education .................................. 47 45 2 Q Q 25.4 23.9 0.8 Q 0.3 Food Sales ................................ Q Q Q Q Q Q Q Q Q Q Food Service ............................. Q Q Q Q Q Q Q Q Q Q

250

Eltron Research & Development  

SciTech Connect (OSTI)

This topical report covers technical work conducted under contract DE-FC26-05NT42469 between FY06 Q1 through FY14 Q2. The project evolved through several budget periods, budget revisions and continuation applications. This report covers work performed under the base program. In 2010 ARRA funding was added to the project. A separate report covering the ARRA portion of the project was submitted to DOE. The original project was focused on research and development for scale-up of hydrogen separation membrane for a FutureGen type power plant. The work included membrane testing and evaluation of metal alloy flat plates vs. tubes and metal membranes vs. cermet membranes. In addition, economic analysis and process modeling was performed. The original project team included CoorsTek, NORAM, and Praxair. In FY10Q2 a continuation application was filed for conducting a scale-up test at Eastman Chemical. In this part of the project a Subscale Engineering Prototype (SEP) membrane skid was designed, fabricated, and operated on a gasified coal slip-stream on Eastmans site in Kingsport, TN. Following operation, the project was reorganized and a second continuation application with a new statement of work was initiated in FY12Q1. Finally, based on DOEs decision not to proceed with a Process Development Unit (PDU) field test, a third continuation application and statement of work was initiated in FY13Q1 to close out the project.

Evenson, Carl; Mackay, Richard; Faull, John

2014-03-01T23:59:59.000Z

251

Power requirements for electron cyclotron current drive and ion cyclotron resonance heating for sawtooth control in ITER  

E-Print Network [OSTI]

13MW of electron cyclotron current drive (ECCD) power deposited inside the q = 1 surface is likely to reduce the sawtooth period in ITER baseline scenario below the level empirically predicted to trigger neo-classical tearing modes (NTMs). However, since the ECCD control scheme is solely predicated upon changing the local magnetic shear, it is prudent to plan to use a complementary scheme which directly decreases the potential energy of the kink mode in order to reduce the sawtooth period. In the event that the natural sawtooth period is longer than expected, due to enhanced alpha particle stabilisation for instance, this ancillary sawtooth control can be provided from > 10MW of ion cyclotron resonance heating (ICRH) power with a resonance just inside the q = 1 surface. Both ECCD and ICRH control schemes would benefit greatly from active feedback of the deposition with respect to the rational surface. If the q = 1 surface can be maintained closer to the magnetic axis, the efficacy of ECCD and ICRH schemes sig...

Chapman, I T; Sauter, O; Zucca, C; Asunta, O; Buttery, R J; Coda, S; Goodman, T; Igochine, V; Johnson, T; Jucker, M; La Haye, R J; Lennholm, M; Contributors, JET-EFDA

2013-01-01T23:59:59.000Z

252

DOE/EIA-0516(85) Energy Information Administration Manufacturing Energy Consumption Survey:  

U.S. Energy Information Administration (EIA) Indexed Site

6(85) 6(85) Energy Information Administration Manufacturing Energy Consumption Survey: Changes in Energy Efficienc y 1980-198 5 0 6 6 T ' L I A n s n u e r b i r p u T J d J T O J u o i j E i a o s s v 1 I Q 3 H O O l O H d s > | i i e } a B B J O j s j o n p c u d j o s e u e s v : o } o n d s e s e - e s z ( 2 0 2 ) O Q ' u o i 6 u m s B M I U 8 L U U I 8 A O O ' S ' H s j u e i u n o o a j o l u e p u e i u u a d n g U J 9 1 S B 3 ' j - ^ ' ' U J ' d g - ' i u ' B g : s j n o H 1 8 1 . 1 - 9 8 9 ( 2 0 2 ) : A | U Q J B 9 Q 9 4 1 J 0 * 3 3 I A 8 Q S U O j l B O ! U n U J U J < X > 8 | 8 1 0 0 8 8 - 9 8 9 ( 2 0 2 ) 9 8 9 0 2 0 0 8 t O - d I L U O O U ' S u j p n n g U O | J B J t S ! U | L U p V U O U B L U J O J U I A B J 8 U 3 I . £ 2 - 1 3 ' J 8 i U 8 0 U O j l B U U J O J U l A 6 J 8 U 3 | B U O I i B N : M O | 8 q J B e d d B s j n o g p u s ' s j s q t u n u s u o i j d s i a j ' s s s s s j p p v ' ( Q Q l ) J Q J s o j A S p s u o ! J B O ! u n i u u u o o 8 | 8 i ' J O 8 u o q d a | 8 i ' H B I U A q Q | 3 N 9 M I 0 1 p s p s j j p s q p i n o i j s S O J I S J I B I S A B u o s u o u s s n o ' ( O I 3 N ) J Q 1 U 8 Q U O U B I U J O ^ U I A B j s u g I B U O J I B N s , v i 3 e g u o O d

253

Microsoft Word - 2011 Aug Report to Congress_080511_GC edits_v2_clean.docx  

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

Table 2. Multi-Year Schedule Table 2 presents DOE's currently scheduled rulemaking activities for energy conservation standards and test procedures. It is noted that the test procedure rulemakings listed below for residential products include revisions to all facets of the test procedure unless otherwise specified as a revision to the active mode or standby/off modes only. Test procedures for commercial and industrial products address active mode only. Appliance Standards Product Categories Driver Approx. Rule Initiation Date Final Action Date Heating Products Rulemakings Residential Water Heaters, Direct Heating Equipment, and Pool Heaters (Standby Mode and Off Mode) Test Procedure EISA 2007 Fiscal Year (FY) 2009, Quarter (Q) 1 Feb. 2012 *

254

Quarterly Coal Report  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Quarterly Coal Report January - March 2008 July 2008 Energy Information Administration Office of Coal, Nuclear, Electric, and Alternate Fuels U.S. Department of Energy Washington, DC 20585 _____________________________________________________________________________ This report is available on the Web at: http://www.eia.doe.gov/cneaf/coal/quarterly/qcr.pdf _____________________________________________ This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the U.S. Department of Energy. The information contained herein should be not be construed as advocating or reflecting any policy position of the U.S. Department of Energy or any other organization.

255

Microsoft Word - 2011 Aug Report to Congress_080511_GC edits_v2_clean.docx  

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

Table 2. Multi-Year Schedule Table 2 presents DOE's currently scheduled rulemaking activities for energy conservation standards and test procedures. It is noted that the test procedure rulemakings listed below for residential products include revisions to all facets of the test procedure unless otherwise specified as a revision to the active mode or standby/off modes only. Test procedures for commercial and industrial products address active mode only. Appliance Standards Product Categories Driver Approx. Rule Initiation Date Final Action Date Heating Products Rulemakings Residential Water Heaters, Direct Heating Equipment, and Pool Heaters (Standby Mode and Off Mode) Test Procedure EISA 2007 Fiscal Year (FY) 2009, Quarter (Q) 1 Feb. 2012 *

256

Help:External searches | Open Energy Information  

Open Energy Info (EERE)

searches searches Jump to: navigation, search 50px Move proposal : It has been suggested that this page be moved to a new name : '(new name to be decided)'. Use the talk page to discuss this action. It is possible to create an external searches of a topic using key words using a template. For example, this is something that would work for Google: [[Image:GoogleIcon.PNG]] [http://www.google.com/search?hl=en&safe=off&q={{{1|Wiki}}}&btnG=Search&meta= {{{1|Google}}}] ==Usage== Allows to establish a link to a search query at the Google search engine: {{Google|Term1+Term2+Term3}}

257

Microsoft Word - QCR012009.doc  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Quarterly Coal Report January - March 2009 June 2009 Energy Information Administration Office of Coal, Nuclear, Electric, and Alternate Fuels U.S. Department of Energy Washington, DC 20585 _____________________________________________________________________________ This report is available on the Web at: http://www.eia.doe.gov/cneaf/coal/quarterly/qcr.pdf _____________________________________________ This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the U.S. Department of Energy. The information contained herein should be not be construed as advocating or reflecting any policy position of the U.S. Department of Energy or any other organization.

258

Microsoft Word - QCR012005.doc  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Quarterly Coal Report January - March 2005 June 2005 Energy Information Administration Office of Coal, Nuclear, Electric, and Alternate Fuels U.S. Department of Energy Washington, DC 20585 _____________________________________________________________________________ This report is available on the Web at: http://www.eia.doe.gov/cneaf/coal/quarterly/qcr.pdf _____________________________________________ This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the U.S. Department of Energy. The information contained herein should be not be construed as advocating or reflecting any policy position of the U.S. Department of Energy or any other organization.

259

A quantum algorithm for the quantum Schur-Weyl transform  

E-Print Network [OSTI]

We construct an efficient quantum algorithm to compute the quantum Schur-Weyl transform for any value of the quantum parameter $q \\in [0,\\infty]$. Our algorithm is a $q$-deformation of the Bacon-Chuang-Harrow algorithm, in the sense that it has the same structure and is identically equal when $q=1$. When $q=0$, our algorithm is the unitary realization of the Robinson-Schensted-Knuth (or RSK) algorithm, while when $q=\\infty$ it is the dual RSK algorithm together with phase signs. Thus, we interpret a well-motivated quantum algorithm as a generalization of a well-known classical algorithm.

Sonya Berg

2012-05-17T23:59:59.000Z

260

On the elastic energy and stress correlation in the contact between elastic solids with randomly rough surfaces  

E-Print Network [OSTI]

When two elastic solids with randomly rough surfaces are brought in contact, a very inhomogeneous stress distribution sigma(x) will occur at the interface. Here I study the elastic energy and the correlation function , where sigma(q) is the Fourier transform of sigma(x) and where stands for ensemble average. I relate to the elastic energy stored at the interface, and I show that for self affine fractal surfaces, quite generally \\sim q^{-(1+H)}, where H is the Hurst exponent of the self-affine fractal surface.

B. N. J. Persson

2008-05-06T23:59:59.000Z

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


261

Analysis and computation of multiple unstable solutions to nonlinear elliptic systems  

E-Print Network [OSTI]

. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 118 23 A radial positive solution to the Lane-Emden system (see Exam- ple V.4) with ? ={x?R2 :|x|< 2}, p = 5,q = 1.5: superlinear case. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 119 24 A radial positive solution... to the biharmonic problem (5.51) with p = 3, ? ={x?R2 :|x|< 3}. Here, u =??v. . . . . . . . . . . . . 120 25 A sign-changing solution to the biharmonic problem (5.51) with p = 3, ? ={x?R2 :|x|< 3}. Here, u =??v. . . . . . . . . . . . . 121 1 CHAPTER I INTRODUCTION...

Chen, Xianjin

2009-05-15T23:59:59.000Z

262

Real-Time Kadanoff-Baym Approach to Nuclear Response Functions  

E-Print Network [OSTI]

Linear response functions are calculated for symmetric nuclear matter of normal density by time-evolving two-time Green's functions with conserving self-energy insertions, thereby satisfying the energy-sum rule. Nucleons are regarded as moving in a mean field defined by an effective mass. A two-body effective (or residual) interaction, represented by a gaussian local interaction, is used to find the effect of correlations in a second order as well as a ring approximation. The response function S(e,q) is calculated for 0.2<q<1.2 fm^{-1}. Comparison is made with the nucleons being un-correlated, "RPA+HF" only.

H. S. Kohler; N. H. Kwong

2013-11-19T23:59:59.000Z

263

Particulate Waste Product Combustion System  

E-Print Network [OSTI]

. The introduction of fuels with high ash or silica content into burn.ers have produced problems of fly ash in the exhaust stream causing extensive darrage to boilers f1red by th gasification process. For exanple, the contlus ioo of the rice hull pre sents a... manner using underfire and overflre air to support fficient gasification of the by product, which results ln he pro:Juction of a c~ bustible gas mixture characteristic of organic sub- stances. Intro:Juction of the fuel stock into t cQ1mustion chamber...

King, D. R.; Chastain, C. E.

1984-01-01T23:59:59.000Z

264

Methods to assess quality of boiled sorghum, gruel and chapaties from sorghums with different kernel characteristics  

E-Print Network [OSTI]

of carotenoids Endosperm color is classified as white, heteroyellow ?nd yellow. Waxy or non-waxy endo- sperm type is determined by the proportion of the types of starch (13, 14) . The types of starch in sorghum are primarily amylose and amylopectin. Both... are polymers of o-d-glucose. Amylose is an o. -1, 4- linked straight chain polymer. Amylopectin is an o. '-1, 6-branched, Q-1, 4-linked polymer. In most sorghums about 25% of the starch is amylose, but in waxy types almost all of the starch is amylopectin...

Waniska, Ralph Dean

2012-06-07T23:59:59.000Z

265

Vrme-och strmningsteknik / Thermal and flow engineering Massverfring & separationsteknik /  

E-Print Network [OSTI]

vätskefas vid kokpunkts-temperaturen (dvs. q = 1). Trycket är p = 1.05+(d/40) bar. ?terflödesförhållandet R(K): Förångningsvärmen för C5 och C6 är hvap = 30 kJ/mol. Kondensorn är en totalkondensor medan återkokaren är partiell och löpande drifts- och underhållskostnader Cv, vilka är relaterade till återflödesförhållandet R för

Zevenhoven, Ron

266

Vrme-och strmningsteknik / Thermal and flow engineering Massverfring & separationsteknik /  

E-Print Network [OSTI]

vätskefas vid kokpunktstemperaturen, dvs. q = 1. Trycket är p = 1.05 + (d/40) bar. ?terflödesförhållandet R(K): Förångningsvärmen för C5 och C6 är hvap = 30 kJ/mol. Kondensorn är en totalkondensor medan återkokaren är partiell och löpande drifts- och underhållskostnader Cv, vilka är relaterade till återflödesförhållandet R för

Zevenhoven, Ron

267

Effect of Trapped Energetic Particles on the Resistive Wall Mode  

SciTech Connect (OSTI)

A stability analysis for the resistive wall mode is studied in the presence of trapped energetic particles (EPs). When the EPs' beta exceeds a critical value, a fishbonelike bursting mode (FLM) with an external kink eigenstructure can exist. This offers the first analytic interpretation of the experimental observations [Phys. Rev. Lett. 103, 045001 (2009)]. The mode-particle resonances for the FLM and the q=1 fishbone occur in different regimes of the precession frequency of EPs. In certain ranges of the plasma rotation speed and the EPs' beta, a mode conversion can occur between the resistive wall mode and FLM.

Hao, G. Z.; Wang, A. K.; Qiu, X. M. [Southwestern Institute of Physics, Post Office Box 432, Chengdu 610041 (China); Liu, Y. Q. [Euratom/CCFE Fusion Association, Culham Science Centre, Abingdon, Oxon OX14 3DB (United Kingdom)

2011-07-01T23:59:59.000Z

268

TD du cours de Theorie de l'Information et Codage 21 fevrier 2011.  

E-Print Network [OSTI]

´e (q1, . . . , qn) est atteint pour qk = pk, 1 k n. 1 #12;2. En d´eduire les th´eor`emes suivants: Th´eor = 1/n. 3. Th´eor`eme 2.2 Si X et Y sont des v.a. (discr`etes) alors H(X, Y ) H(X) + H(Y ), avec) H(X|Y ) = 0 si et seulement si X = g(Y ) pour une fonction g. (3) 2. Montrer le th´eor`eme suivant

Lelarge, Marc

269

Partial Differential Equations/Differential Geometry QUASILINEAR ELLIPTIC HAMILTON-JACOBI EQUATIONS ON  

E-Print Network [OSTI]

(x)| cn,p,qB 1 q+1-p x M. Une des cons´equences est un th´eor`eme de type Liouville. 1. Laboratoire de > 0 et que les hypoth`eses du Th´eor`eme 1 portant sur la courbure sectionnelle soient v´erifi´ees si´esultat du th´eor`eme 1, on en d´eduit Th´eor`eme 3. Supposons que p > 1 et que les hypoth`eses du Th´eor

Boyer, Edmond

270

A method for the determination of dissolved organic carbon in sea water by gas chromatography  

E-Print Network [OSTI]

of organic matter was carried out at elevated temperature and pressure after collection of a large number of samples. The resulting carbon dioxide was flushed through a gas chromatograph with helium as the carrier gas and the signal was recorded on a strip... chart recorder. Chromatographic analysis time was approximately eleven minutes per sample with a precision of + Q. 1 mg C/l. The organic carbon content of the sample was determined by measurement of the peak area using an appropriate carbon dioxide...

Fredericks, Alan D

1965-01-01T23:59:59.000Z

271

State of the campuS April 17, 2012  

E-Print Network [OSTI]

Ree YeaRS · 115 RiSe pRopoSalS fRom facultY StAte oF the CAMpUS 6 UC dAViS iS A ReSeaRch poweRhouSe #12RceNt iN fY 2011-12 StAte oF the CAMpUS 8 2012 Q1-Q2 ReSeaRch awaRdS ($m) UC dAViS iS A ReSeaRch poweRhouSe

California at Davis, University of

272

Non-Extensive Black Hole Thermodynamics Estimate for Power-Law Particle Spectra  

E-Print Network [OSTI]

We point out that by considering the Hawking-Bekenstein entropy of Schwarzschild black hole horizons as a non-extensive Tsallis entropy, its additive formal logarithm, coinciding with the Renyi entropy, generates an equation of state with positive heat capacity above a threshold energy. Based on this, the edge of stability is conjectured to be trans-Planckian, i.e. being in the quantum range. From this conjecture an estimate arises for the q-parameter in the Renyi entropy, (q=2/pi^2), also manifested in the canonical power-law distribution of high energy particles (q ~ 1.2 for quark matter).

Tamas S. Biro

2010-11-15T23:59:59.000Z

273

Potts model with invisible colours: Random-cluster representation and Pirogov-Sinai analysis  

E-Print Network [OSTI]

We study a variant of the ferromagnetic Potts model, recently introduced by Tamura, Tanaka and Kawashima, consisting of a ferromagnetic interaction among $q$ "visible" colours along with the presence of $r$ non-interacting "invisible" colours. We introduce a random-cluster representation for the model, for which we prove the existence of a first-order transition for any $q>0$, as long as $r$ is large enough. When $q>1$, the low-temperature regime displays a $q$-fold symmetry breaking. The proof involves a Pirogov-Sinai analysis applied to this random-cluster representation of the model.

Aernout C. D. van Enter; Giulio Iacobelli; Siamak Taati

2011-09-01T23:59:59.000Z

274

Formation and Stability of Impurity "snakes" in Tokamak Plasmas  

SciTech Connect (OSTI)

New observations of the formation and dynamics of long-lived impurity-induced helical "snake" modes in tokamak plasmas have recently been carried-out on Alcator C-Mod. The snakes form as an asymmetry in the impurity ion density that undergoes a seamless transition from a small helically displaced density to a large crescent-shaped helical structure inside q < 1, with a regularly sawtoothing core. The observations show that the conditions for the formation and persistence of a snake cannot be explained by plasma pressure alone. Instead, many features arise naturally from nonlinear interactions in a 3D MHD model that separately evolves the plasma density and temperature

L. Delgado-Aparicio, et. al.

2013-01-28T23:59:59.000Z

275

Past and Future Blurring at Fundamental Length Scale  

SciTech Connect (OSTI)

We obtain the {kappa}-deformed versions of the retarded and advanced Green functions and show that their causality properties are blurred in a time interval of the order of a length parameter q=1/(2{kappa}). The functions also indicate a smearing of the light cone. These results favor the interpretation of q as a fundamental length scale below which the concept of a point in space-time should be substituted by the concept of a fuzzy region of radius q, as proposed long ago by Heisenberg.

Neves, M. J. [Centro Brasileiro de Pesquisas Fisicas, Rua Dr. Xavier Sigaud 150, Urca, Rio de Janeiro, RJ, 22290-180 (Brazil); Farina, C.; Cougo-Pinto, M. V. [Instituto de Fisica, UFRJ, CP 68528, Rio de Janeiro, RJ, 21941-972 (Brazil)

2010-11-19T23:59:59.000Z

276

An investigation of rainfall variability and distribution in Luzon and a mesoscale study of rainfall of the province of Laguna and adjacent areas, Philippines  

E-Print Network [OSTI]

cover only from 1962 through 1965. r'~OCt 81'IO '-. -4' L ! t Q, Leg en d: 500 &t ----- 1000 tt "-" ~ ~ )1000 ft v'?+ S 121 o MANILA -~ 2~2 )' ~ P. ' )~, o' ) \\ t:. , ~ J, LANrj; ' 3i5)'. v. ', ' wucena 75 Og 122 ~ FIGURE 2. RELIEF... the area 120 90 122 o 124o LUZON P H ILt P PINES 18o / / I I I I I 100 / / 90 Baguio 80 GO Aparri rag LLi C3 O 16 Cabanatuan o LI Q 1 Go Olor a po 80 MANILA 40 14o S. Pablo 4o 'Q Naga ga&pua FIGIJRE 5. COEFFICIENT...

Coligado, Mauro Comendador

1967-01-01T23:59:59.000Z

277

S:\VM3\RX97\TBL_LIST.WPD [PFP#201331587]  

U.S. Energy Information Administration (EIA) Indexed Site

b. Appliances by Four Most Populated States, b. Appliances by Four Most Populated States, Percent of U.S. Households, 1997 Appliance Types and Characteristics RSE Column Factor: Total Four Most Populated States RSE Row Factors New York California Texas Florida 0.4 1.3 1.2 1.2 1.4 Total .............................................................. 100.0 100.0 100.0 100.0 100.0 0.0 Households With Electric Air-Conditioning Equipment ...................... 72.5 62.6 41.4 91.7 96.0 3.5 Central Equipment Not Used ....................... 0.3 Q 1.2 0.5 1.1 29.3 Room Air Conditioners Not Used ................ 0.7 Q Q Q 1.1 36.9 Households Using Electric Air-Conditioning 1 ........................................ 71.6 62.2 39.9 91.2 94.3 3.3 Type of Electric Air-Conditioning Used Central Air-Conditioning 2 ............................

278

c18.xls  

Gasoline and Diesel Fuel Update (EIA)

62 62 210 50 5,328 12,097 3,220 11.7 17.4 15.5 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 10 26 7 821 1,157 472 12.4 22.9 15.5 5,001 to 10,000 ................................. 7 18 4 666 1,308 359 10.7 13.9 12.0 10,001 to 25,000 ............................... 8 27 11 1,164 2,207 791 7.3 12.2 14.2 25,001 to 50,000 ............................... 15 24 5 949 1,672 442 16.1 14.4 10.9 50,001 to 100,000 ............................. 8 25 10 642 1,470 650 12.8 16.7 14.8 100,001 to 200,000 ........................... 8 39 Q 614 2,087 Q 12.3 18.9 Q 200,001 to 500,000 ........................... Q 22 Q Q 1,072 Q Q 20.4 Q Over 500,000 .................................... Q 29 Q Q 1,123 Q Q 25.6 Q Principal Building Activity Education .......................................... 5 39 Q 549 2,445 Q 8.8 16.0 Q Food Sales .......................................

279

c31a.xls  

Gasoline and Diesel Fuel Update (EIA)

Buildings .................................... Buildings .................................... 467 882 688 7,144 21,928 19,401 65.4 40.2 35.5 Principal Building Activity Education .......................................... Q 137 101 419 3,629 2,997 53.9 37.6 33.7 Food Sales ....................................... 16 Q Q 339 Q Q 46.6 Q Q Food Service ..................................... 149 48 N 774 622 N 192.5 77.2 N Health Care ....................................... 12 37 187 233 520 1,792 49.5 70.8 104.4 Inpatient .......................................... N Q 181 N Q 1,662 N Q 109.0 Outpatient ....................................... 12 20 Q 233 377 Q 49.5 52.3 Q Lodging ............................................. Q 83 113 Q 1,750 2,374 Q 47.6 47.4 Mercantile ......................................... 60 134 61 1,094 3,572 3,205 55.2 37.6 19.1 Retail (Other Than Mall) ..................

280

c18a.xls  

Gasoline and Diesel Fuel Update (EIA)

66 66 254 57 5,523 13,837 3,546 12.0 18.3 16.2 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 10 28 7 821 1,233 481 12.4 22.4 15.4 5,001 to 10,000 ................................. 7 20 5 681 1,389 386 10.8 14.4 13.3 10,001 to 25,000 ............................... 9 31 12 1,204 2,411 842 7.8 12.8 14.1 25,001 to 50,000 ............................... 15 29 6 949 1,867 490 16.1 15.5 11.7 50,001 to 100,000 ............................. 9 35 13 664 1,797 749 13.1 19.2 17.0 100,001 to 200,000 ........................... 8 50 Q 614 2,422 Q 12.3 20.6 Q 200,001 to 500,000 ........................... Q 23 Q Q 1,148 Q Q 20.4 Q Over 500,000 .................................... Q 38 Q Q 1,572 Q Q 24.3 Q Principal Building Activity Education .......................................... 5 39 Q 549 2,445 Q 8.8 16.0 Q Food Sales .......................................

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


281

c7.xls  

Gasoline and Diesel Fuel Update (EIA)

294 294 978 1,254 2,964 9,941 11,595 99.0 98.3 108.1 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 33 85 146 360 666 974 91.2 128.1 149.7 5,001 to 10,000 ................................. Q 64 73 359 764 843 Q 83.7 86.8 10,001 to 25,000 ............................... Q 115 163 553 1,419 1,934 Q 81.2 84.3 25,001 to 50,000 ............................... Q 74 140 347 944 1,618 Q 78.7 86.8 50,001 to 100,000 ............................. Q 134 148 516 1,524 1,618 Q 87.8 91.5 100,001 to 200,000 ........................... Q 150 203 414 1,703 1,682 Q 87.9 120.8 200,001 to 500,000 ........................... Q 177 214 Q 1,673 1,801 Q 105.8 118.8 Over 500,000 .................................... Q Q Q Q 1,248 1,126 Q Q Q Principal Building Activity Education .......................................... Q 143

282

c7a.xls  

Gasoline and Diesel Fuel Update (EIA)

345 345 1,052 1,343 3,452 10,543 12,424 99.8 99.7 108.1 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 37 86 147 383 676 986 95.9 127.9 148.9 5,001 to 10,000 ................................. 39 68 83 369 800 939 106.0 85.4 88.2 10,001 to 25,000 ............................... Q 121 187 674 1,448 2,113 Q 83.4 88.4 25,001 to 50,000 ............................... Q 84 155 366 1,022 1,763 Q 82.5 87.6 50,001 to 100,000 ............................. Q 155 160 590 1,682 1,712 Q 92.0 93.3 100,001 to 200,000 ........................... Q 161 224 448 1,790 1,872 Q 90.0 119.6 200,001 to 500,000 ........................... Q 177 218 Q 1,673 1,847 Q 105.8 117.9 Over 500,000 .................................... Q Q Q Q 1,451 1,192 Q Q Q Principal Building Activity Education ..........................................

283

 

Gasoline and Diesel Fuel Update (EIA)

A. Fuel Oil Consumption (Btu) and Energy Intensities by End Use for All A. Fuel Oil Consumption (Btu) and Energy Intensities by End Use for All Buildings, 2003 Total Fuel Oil Consumption (trillion Btu) Fuel Oil Energy Intensity (thousand Btu/square foot) Total Space Heating Water Heating Cook- ing Other Total Space Heating Water Heating Cook- ing Other All Buildings ......................... 228 198 18 Q 10 14.0 12.2 1.1 Q 0.6 Building Floorspace (Square Feet) 1,001 to 5,000 ......................... 34 32 Q (*) Q 56.9 52.2 Q (*) Q 5,001 to 10,000 ....................... 36 33 Q (*) Q 49.4 44.7 Q 0.1 Q 10,001 to 25,000 ..................... 28 25 1 (*) Q 26.7 23.8 1.4 0.1 Q 25,001 to 50,000 ..................... 17 16 Q (*) 1 19.1 17.8 Q (*) 0.6 50,001 to 100,000 ................... 29 26 1 Q 1 15.6 14.1 0.7 Q 0.5

284

c8.xls  

Gasoline and Diesel Fuel Update (EIA)

436 436 1,064 309 5,485 12,258 3,393 79.5 86.8 91.1 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 60 116 36 922 1,207 538 64.9 96.5 67.8 5,001 to 10,000 ................................. 44 103 Q 722 1,387 393 60.5 74.0 Q 10,001 to 25,000 ............................... 65 126 Q 1,164 2,240 810 55.9 56.4 Q 25,001 to 50,000 ............................... 107 112 Q 949 1,672 498 112.5 67.3 Q 50,001 to 100,000 ............................. 64 123 59 642 1,470 650 99.0 83.4 91.3 100,001 to 200,000 ........................... 49 237 Q 614 2,087 Q 79.8 113.5 Q 200,001 to 500,000 ........................... Q 110 Q 395 1,072 Q Q 102.2 Q Over 500,000 .................................... Q 137 Q Q 1,123 Q Q 122.1 Q Principal Building Activity Education .......................................... 45 198 Q 552 2,445

285

Inelastic exchange scattering in electron-energy-loss spectroscopy: Localized excitations in transition-metal and rare-earth systems  

Science Journals Connector (OSTI)

Cross sections for quasiatomic excitation by exchange scattering of electrons are calculated in the Born-Ochkur approximation for 3p-3d and 3d-3d transitions in transition-metal systems, and for 4d-4f and 4f-4f transitions in rare earths. The energy dependence of the spin polarization of 3p-3d and 4d-4f losses in reflection electron-energy-loss spectroscopy from ferromagnetic surfaces involves a balance of small-angle spin-dependent inelastic processes accompanied by a high-angle elastic scattering, and large-angle spin-flip exchange scattering without the need for elastic scattering. Both 3d-3d excitations, e.g., in transition-metal compounds, and 4f-4f excitations in rare earths involve spin-flip transitions whose scattering amplitudes g fall off with momentum transfer q such that the full width at half maximum q1/2 (in a.u.) is given by q1/2?rnl??2, where ?rnl? is the expectation value of r for the 3d or 4f electron. The angular width of the spin-flip differential cross section is then much greater than for dipole transitions, a pattern that helps to account for how these intra-atomic transitions compete with dipole processes for primary energies in excess of 100 eV.

S. J. Porter; J. A. D. Matthew; R. J. Leggott

1994-07-15T23:59:59.000Z

286

Renyi entropy, stationarity, and entanglement of the conformal scalar  

E-Print Network [OSTI]

We extend previous work on the perturbative expansion of the Renyi entropy, $S_q$, around $q=1$ for a spherical entangling surface in a general CFT. Applied to conformal scalar fields in various spacetime dimensions, the results appear to conflict with the known conformal scalar Renyi entropies. On the other hand, the perturbative results agree with known Renyi entropies in a variety of other theories, including theories of free fermions and vector fields and theories with Einstein gravity duals. We propose a resolution stemming from a careful consideration of boundary conditions near the entangling surface. This is equivalent to a proper treatment of total-derivative terms in the definition of the modular Hamiltonian. As a corollary, we are able to resolve an outstanding puzzle in the literature regarding the Renyi entropy of ${\\cal N}=4$ super-Yang-Mills near $q=1$. A related puzzle regards the question of stationarity of the renormalized entanglement entropy (REE) across a circle for a (2+1)-dimensional massive scalar field. We point out that the boundary contributions to the modular Hamiltonian shed light on the previously-observed non-stationarity. Moreover, IR divergences appear in perturbation theory about the massless fixed point that inhibit our ability to reliably calculate the REE at small non-zero mass.

Jeongseog Lee; Aitor Lewkowycz; Eric Perlmutter; Benjamin R. Safdi

2014-07-29T23:59:59.000Z

287

Renyi entropy, stationarity, and entanglement of the conformal scalar  

E-Print Network [OSTI]

We extend previous work on the perturbative expansion of the Renyi entropy, $S_q$, around $q=1$ for a spherical entangling surface in a general CFT. Applied to conformal scalar fields in various spacetime dimensions, the results appear to conflict with the known conformal scalar Renyi entropies. On the other hand, the perturbative results agree with known Renyi entropies in a variety of other theories, including theories of free fermions and vector fields and theories with Einstein gravity duals. We propose a resolution stemming from a careful consideration of boundary conditions near the entangling surface. This is equivalent to a proper treatment of total-derivative terms in the definition of the modular Hamiltonian. As a corollary, we are able to resolve an outstanding puzzle in the literature regarding the Renyi entropy of ${\\cal N}=4$ super-Yang-Mills near $q=1$. A related puzzle regards the question of stationarity of the renormalized entanglement entropy (REE) across a circle for a (2+1)-dimensional ma...

Lee, Jeongseog; Perlmutter, Eric; Safdi, Benjamin R

2014-01-01T23:59:59.000Z

288

Formation of an internal transport barrier and magnetohydrodynamic activity in experiments with the controlled density of rational magnetic surfaces in the T-10 Tokamak  

SciTech Connect (OSTI)

Results are presented from experiments on the formation of an internal electron transport barrier near the q = 1.5 rational surface in the T-10 tokamak. The experiments were carried out in the regime with off-axis electron cyclotron resonance (ECR) heating followed by a fast plasma current ramp-up. After suppressing sawtooth oscillations by off-axis ECR heating, an internal transport barrier began to form near the q = 1.5 rational surface. In the phase of the current ramp-up, the quality of the transport barrier improved; as a result, the plasma energy confinement time increased 22.5 times. The intentionally produced flattening of the profile of the safety factor q(r) insignificantly affected magnetohydrodynamic activity in the plasma column in spite of the theoretical possibility of formation of substantial m/n = 3/2 and 2/1 magnetic islands. Conditions are discussed under which the flattening of the profile of the safety factor q near low-order rational surfaces leads to the formation of either an internal transport barrier or the development of an island magnetic structure induced by tearing modes.

Razumova, K. A., E-mail: razumova@nfi.kiae.ru; Andreev, V. F.; Belbas, I. S.; Gorshkov, A. V.; Dnestrovskij, A. Yu.; Dyabilin, K. S.; Kislov, A. Ya.; Lysenko, S. E.; Notkin, G. E.; Timchenko, N. N.; Chudnovskiy, A. N.; Shelukhin, D. A. [National Research Centre Kurchatov Institute (Russian Federation)] [National Research Centre Kurchatov Institute (Russian Federation)

2013-09-15T23:59:59.000Z

289

b5.xls  

U.S. Energy Information Administration (EIA) Indexed Site

West West South Central Mountain Pacific All Buildings* .................................. 64,783 2,964 9,941 11,595 5,485 12,258 3,393 7,837 3,675 7,635 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 360 666 974 922 1,207 538 788 464 871 5,001 to 10,000 ................................. 6,585 359 764 843 722 1,387 393 879 418 820 10,001 to 25,000 ............................... 11,535 553 1,419 1,934 1,164 2,240 810 1,329 831 1,256 25,001 to 50,000 ............................... 8,668 347 944 1,618 949 1,672 498 998 511 1,132 50,001 to 100,000 ............................. 9,057 516 1,524 1,618 642 1,470 650 1,314 374 948 100,001 to 200,000 ........................... 9,064 414 1,703 1,682 614 2,087 Q 1,131 Q 895 200,001 to 500,000 ........................... 7,176 Q 1,673 1,801 395 1,072

290

 

Gasoline and Diesel Fuel Update (EIA)

. Fuel Oil Consumption (Btu) and Energy Intensities by End Use for . Fuel Oil Consumption (Btu) and Energy Intensities by End Use for Non-Mall Buildings, 2003 Total Fuel Oil Consumption (trillion Btu) Fuel Oil Energy Intensity (thousand Btu/square foot) Total Space Heating Water Heating Cook- ing Other Total Space Heating Water Heating Cook- ing Other All Buildings* ........................ 222 194 17 Q 10 14.7 12.8 1.1 Q 0.6 Building Floorspace (Square Feet) 1,001 to 5,000 ......................... 34 32 Q (*) Q 57.4 52.7 Q (*) Q 5,001 to 10,000 ....................... 36 33 Q (*) Q 50.6 45.8 Q 0.1 Q 10,001 to 25,000 ..................... 27 25 1 (*) Q 28.2 25.4 1.5 0.1 Q 25,001 to 50,000 ..................... 16 15 Q (*) 1 19.7 18.8 Q (*) 0.7 50,001 to 100,000 ................... 26 23 1 Q 1 15.0 13.3 0.8 Q 0.6

291

Trends in U.S. Venture Capital Investments Related to Energy: 1980 through the Second Quarter of 2010  

SciTech Connect (OSTI)

This report documents trends in U.S. venture capital investments over the period 1980 through the second quarter of calendar year 2010 (2010Q1+Q2). Particular attention is given to U.S. venture capital investments in the energy/industrial sector over the period 1980-2010Q1+Q2 as well as in the more recently created cross-cutting category of CleanTech over the period 1995-2010Q1+Q2. During the early 1980s, U.S. venture capital investments in the energy/industrial sector accounted for more than 20% of all venture capital investments. However subsequent periods of low energy prices, the deregulation of large aspects of the energy industry, and the emergence of fast growing new industries like computers (both hardware and software), biotechnology and the Internet quickly reduced the priority accorded to energy/industrial investments. To wit, venture capital investments related to the energy/industrial sector accounted for only 1% of the $119 billion dollars invested in 2000 by the U.S. venture capital community. The significant increase in the real price of oil that began in 2003-2004 correlates with renewed interest and increased investment by the venture capital community in energy/industrial investment opportunities. Venture capital investments for 2009 for the energy/industrial sector accounted for $2.1 billion or slightly more than 13% of all venture capital invested that year. The total venture capital invested in energy/industrial during the first two quarters of 2010 is close to $1.8 billion accounting for 17% of all venture capital investments during the first two quarters of 2010. In 2009, the aggregate amount invested in CleanTech was $1.8 billion (30% of the total US venture capital invested in that lean year) and for the first two quarters of 2010 US venture capital investments in CleanTech have already exceeded $1.9 billion (19% of all US venture capital investments made during the first half of 2010). Between 2004 and 2009, U.S. venture capital investments in energy/industrial as well as CleanTech have more than quadrupled in real terms.

Dooley, James J.

2010-07-29T23:59:59.000Z

292

u.s. DEPARTMENT OF ENERGY EERE PROJECT MAN AG EMENT CENTER NEPA DETERlVIINATION  

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

AG EMENT CENTER AG EMENT CENTER NEPA DETERlVIINATION RECIPIENT:Snohomish County PUD PROJECT TITLE : Development of Post-Installation Monitoring Capabilities Page lof3 STATE: WA Funding Opportunity Announcement Number Procurement Instrument Numbu NEPA Control Number CID Number NlA - CDP DE-EE0000301 GF0-00003Q1'()()2 EE301 Based on my review orlhe information concerning the proposed action, as NEPA Compliance Officer (authori7.ed under DOE Order 451.IA), I have made the following determination: ex, EA, [IS APPENDIX AND NUMBER: Description : AS Informabon gathering (including, but nollimiled 10, literature surveys, inventories, audits), data analYSIS (including computer modeling), document preparation (sud1 as conceptual design or feasibility studies, analytical erJergy supply and

293

Teleseismic-Seismic Monitoring At Coso Geothermal Area (1975-1976) | Open  

Open Energy Info (EERE)

Teleseismic-Seismic Monitoring At Coso Geothermal Area (1975-1976) Teleseismic-Seismic Monitoring At Coso Geothermal Area (1975-1976) Jump to: navigation, search GEOTHERMAL ENERGYGeothermal Home Exploration Activity: Teleseismic-Seismic Monitoring At Coso Geothermal Area (1975-1976) Exploration Activity Details Location Coso Geothermal Area Exploration Technique Teleseismic-Seismic Monitoring Activity Date 1975 - 1976 Usefulness not indicated DOE-funding Unknown Exploration Basis Estimate thermal regime and potential of the system Notes Three-dimensional Q -1 model of the Coso Hot Springs known geothermal resource area was conducted. To complete the model a regional telemetered network of sixteen stations was operated by the U.S. Geological Survey; deployed a portable Centipede array of 26 three-component stations near the

294

University of California Response to DOE Questions Regarding Price-Anderson Renewal  

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

of California Response to DOE Questions of California Response to DOE Questions Regarding Price-Anderson Renewal January 30, 1998 -1- Q 1. Should the DOE Price-Anderson indemnification be continued without modification? Answer: Price-Anderson indemnification should definitely be continued. Shifting responsibility for payment of claims from the United States to contractors would undermine the certainty of compensation and would therefore be inappropriate. Recent experience with large class claims, an example being claims arising from faulty breast implants, shows that the availability of bankruptcy protection can defeat the payment of adequate compensation to all harmed citizens. The United States government must remain the insurer for its people so long as nuclear materials are used in research, medicine, power

295

" Million Housing Units, Final"  

U.S. Energy Information Administration (EIA) Indexed Site

8 Televisions in Homes in Northeast Region, Divisions, and States, 2009" 8 Televisions in Homes in Northeast Region, Divisions, and States, 2009" " Million Housing Units, Final" ,,"Northeast Census Region" ,,,"New England Census Division",,,"Middle Atlantic Census Division" ,"Total U.S.1 (millions)",,"Total New England",,,"Total Middle Atlantic" ,,"Total Northeast",,,"CT, ME, NH, RI, VT" "Televisions",,,,"MA",,,"NY","PA","NJ" "Total Homes",113.6,20.8,5.5,2.5,3,15.3,7.2,4.9,3.2 "Televisions" "Number of Televisions" 0,1.5,0.4,0.1,0.1,"Q",0.2,"Q","Q","Q" 1,24.2,4.6,1.2,0.6,0.6,3.5,2,1,0.4

296

Supplemental Guidance Regarding Compensatory Time Off for Travel  

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

SUPPLEMENTAL GUIDANCE SUPPLEMENTAL GUIDANCE REGARDING COMPENSATORY TIME OFF FOR TRAVEL (Revised October 27, 2008) Following are questions and answers on issues that supplement the final regulations effective this date on compensatory time for travel issued by the Office of Personnel Management on April 17, 2007. In addition, a sample worksheet is attached to assist travelers in determining and documenting their travel time that may be credited for compensatory time for travel. This information will be incorporated in Appendix D of the DOE Handbook on Overtime when the handbook is updated. Q1. Who is eligible for this benefit? A1. All employees are eligible except the following: the Secretary, SESs, employees covered by other forms of overtime compensation, including law enforcement

297

OFFICE OF THE VICE PRESIDENT WASHINGTQO  

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

- * , 2001-023459 10/19 A 10:00 - * , 2001-023459 10/19 A 10:00 OFFICE OF THE VICE PRESIDENT WASHINGTQO 023459 * zJ OCT q1 A 1: 00 September 20, 2001 The Honorable Spencer Abraham ;ecretary of Energy 1000 Independence Avenue, SW Washington, D.C. 20585 Dear Mr. Secretary: Enclosed are numerous unsolicited proposals and idea papers that we received from citizens from all across the country during the development of the National Energy Policy, and in the mlonths to follow. Many of these individuals and companies have already received correspondence and acknowledgement from the NEPDG and/or the Vice President's office. What most of these citizens are looking for, however, is for review and consideration of thcir proposals and ideas by program professionals. In turn, we would appreciate your vetting these

298

Quarterly Coal Report: January-March 2002  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Distribution Category UC-950 Quarterly Coal Report January - March 2002 August 2002 Energy Information Administration Office of Coal, Nuclear, Electric, and Alternate Fuels U.S. Department of Energy Washington, DC 20585 _____________________________________________________________________________ This report is available on the Web at: http://www.eia.doe.gov/cneaf/coal/quarterly/qcr_sum.html _____________________________________________ This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the U.S. Department of Energy. The information contained herein should be not be construed as advocating or reflecting any policy position of the U.S. Department of Energy or any other organization. Energy Information Administration/Quarterly Coal Report January - March 2002 ii Contacts

299

Total U.S. Housing Units........................................  

U.S. Energy Information Administration (EIA) Indexed Site

15.1 15.1 5.5 Do Not Have Heating Equipment........................... 1.2 Q Q Q Have Space Heating Equipment............................ 109.8 20.5 15.1 5.4 Use Space Heating Equipment............................. 109.1 20.5 15.1 5.4 Have But Do Not Use Equipment.......................... 0.8 N N N Space Heating Usage During 2005 Heated Floorspace (Square Feet) None................................................................. 3.6 Q Q Q 1 to 499............................................................. 6.1 1.3 0.9 0.4 500 to 999......................................................... 27.7 5.6 4.2 1.4 1,000 to 1,499................................................... 26.0 4.3 3.3 1.1 1,500 to 1,999................................................... 17.6 3.0 2.3 0.7 2,000 to 2,499...................................................

300

Ayuda:Buscadores externos | Open Energy Information  

Open Energy Info (EERE)

Ayuda:Buscadores externos Ayuda:Buscadores externos Jump to: navigation, search 50px Move proposal : It has been suggested that this page be moved to a new name : '(new name to be decided)'. Use the talk page to discuss this action. Es posible crear búsquedas externas sobre un tema utilizando palabras claves o una plantilla. A continuación un ejemplo que puede funcionar en Google: [[Image:GoogleIcon.PNG]] [http://www.google.com/search?hl=en&safe=off&q={{{1|Wiki}}}&btnG=Search&meta= {{{1|Google}}}] ==Uso== Permite establecer un enlace a una consulta de búsqueda en el motor de búsqueda de Google: {{Google|Term1+Term2+Term3}}

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


301

U.S. Department of Energy Categorical Exclusion Determination Form  

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

Dismantlement and Removal of 321-M Solvent Storage Tank Area Dynamic Underground Stripping (DUS I) Remnants Dismantlement and Removal of 321-M Solvent Storage Tank Area Dynamic Underground Stripping (DUS I) Remnants Savannah River Site Aiken/Aiken/South Carolina Dynamic Underground Stripping (DUS) at SRS was first deployed at the 321-M Solvent Storage Tank Area (west of the former Building 321-M) to remediate solvent source zone contamination in the vadose zone. The deployment was successful and the DUS equipment has been removed. However, the wells associated with the deployment, as well as the operating header of a portable soil vapor extraction unit (SVEU) and assorted debris remain at the site. The purpose of this activity is to abandon the wells per Manual 3Q1 requirements, dismantle and remove for disposal assorted equipment that is no longer required, and to perform general housekeeping at the site of the original DUS deployment.

302

Quarterly Coal Report, January-March 1998  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Distribution Category UC-950 Quarterly Coal Report January-March 1998 Energy Information Administration Office of Coal, Nuclear, Electric and Alternate Fuels U.S. Department of Energy Washington, DC 20585 This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the Department of Energy. The information contained herein should not be construed as advocating or reflecting any policy position of the Department of Energy or any other organization. Contacts This publication was prepared by Paulette Young under the direction of Mary K. Paull, Project Leader, Coal Data Branch, Coal and Electric Data and Renewables Division, Office of Coal, Nuclear, Elec- tric and Alternate Fuels. Questions addressing the

303

DOE/EIA-0202(85/1Q) Short-Term Energy Outlook Quarterly Projections  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Short-Term Energy Outlook Quarterly Projections January 1985 Published: February 1985 Energy Information Administration Washington, D.C. t rt jrt .ort lort lort lort nort lort *.ort ort Tt .m .erm -Term -Term -Term -Term -Term -Term -Term -Term -Term -Term -Term -Term -Term -Term -Term uergy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy Energy ^nergy Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Outlook Short Short Short Short Short Short Short Short Short Short Short Short Short Short Short Short Short Short Short Short Short Short Short Short

304

 

Gasoline and Diesel Fuel Update (EIA)

0. Fuel Oil Consumption (gallons) and Energy Intensities by End Use for 0. Fuel Oil Consumption (gallons) and Energy Intensities by End Use for Non-Mall Buildings, 2003 Total Fuel Oil Consumption (million gallons) Fuel Oil Energy Intensity (gallons/square foot) Total Space Heating Water Heating Cook- ing Other Total Space Heating Water Heating Cook- ing Other All Buildings* ........................ 1,602 1,397 125 Q 69 0.11 0.09 0.01 Q (*) Building Floorspace (Square Feet) 1,001 to 5,000 ......................... 249 228 Q (*) Q 0.41 0.38 Q (*) Q 5,001 to 10,000 ....................... 261 237 Q 1 Q 0.37 0.33 Q (*) Q 10,001 to 25,000 ..................... 196 177 10 (*) Q 0.20 0.18 0.01 (*) Q 25,001 to 50,000 ..................... 117 112 Q (*) 4 0.14 0.14 Q (*) (*)

305

Symmetric Long Straight Section Lattices  

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

Symmetric Symmetric Long Straight Section Lattices for 2, 4, and 8 Sectors formerly AOP-TN-2009-007, Rev. 2 Michael Borland March 23, 2009 Accelerator Systems Division, Advanced Photon Source 1 Introduction Long straight sections [1] (LSS) are anticipated to be one of the significant changes to the accel- erator as part of the APS Renewal. Previously [2], we developed a lattice with eight LSS that, while workable, would have presented some operational challenges. In the present note, we show improved results for 8LSS, along with new solutions for 4LSS and 2LSS. As before, these lattices are developed by removing the Q2 quadrupoles and moving the Q1 back into its place, permitting a 7.7-m-long insertion device (as judged by the increase in face-to-face distance for the innermost powered quadrupoles). Further increases in length (perhaps 10%) might be possible by removing corrector magnets,

306

Accessibility of pores in coal to methane and carbon dioxide  

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

Accessibility Accessibility of pores in coal to methane and carbon dioxide 3 Yuri B. Melnichenko a,b,⇑ , Lilin He a , Richard Sakurovs c,⇑ , Arkady L. Kholodenko d , Tomasz Blach e , 4 Maria Mastalerz f , Andrzej P. Radlin ´ ski e,f , Gang Cheng g,h , David F.R. Mildner i 5 a Neutron Scattering Sciences Division, Oak Ridge National Laboratory, Oak Ridge, TN 37831, USA 6 b Department of Physics and Astronomy, University of Tennessee, Knoxville, TN 37996, USA 7 c CSIRO Energy Technology, 11 Julius Avenue, North Ryde, 2113 NSW, Australia 8 d 375 H.L. Hunter Laboratories, Clemson University, Clemson, SC 29634-0973, USA 9 e Nanoscale Science and Technology Centre, Griffith University, Nathan 4111, Brisbane, Australia 10 f Indiana Geological Survey, Indiana University, Bloomington, IN 47405-2208, USA 11 g Sandia National Laboratories, Q1 Livermore, CA 94551, USA 12 h Sandia National Laboratories, Albuquerque,

307

Table HC11.1 Housing Unit Characteristics by Northeast Census Region, 2005  

U.S. Energy Information Administration (EIA) Indexed Site

1.1 Housing Unit Characteristics by Northeast Census Region, 2005 1.1 Housing Unit Characteristics by Northeast Census Region, 2005 Total......................................................................... 111.1 20.6 15.1 5.5 Urban/Rural Location (as Self-Reported) City....................................................................... 47.1 6.9 4.7 2.2 Town..................................................................... 19.0 6.0 4.2 1.9 Suburbs................................................................ 22.7 4.4 4.0 0.5 Rural..................................................................... 22.3 3.2 2.3 0.9 Climate Zone 1 Less than 2,000 CDD and-- Greater than 7,000 HDD.................................... 10.9 1.9 Q 1.3 5,500 to 7,000 HDD........................................... 26.1 9.8 5.7 4.1 4,000 to 5,499 HDD...........................................

308

Page not found | Department of Energy  

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

11 - 14620 of 28,905 results. 11 - 14620 of 28,905 results. Download CX-009210: Categorical Exclusion Determination Silver Butte Fiber Burial Project CX(s) Applied: B.47 Date: 08/28/2012 Location(s): Montana, Montana Offices(s): Bonneville Power Administration http://energy.gov/nepa/downloads/cx-009210-categorical-exclusion-determination Download Microsoft PowerPoint- DOE Supplemental Instructions for OMB Section 1512 Reporting Contractors Q1 2010 [Compatibility Mode] http://energy.gov/downloads/microsoft-powerpoint-doe-supplemental-instructions-omb-section-1512-reporting-contractors Rebate TVA- Green Power Providers Tennessee Valley Authority (TVA) and participating power distributors of TVA power offer a performance-based incentive program to homeowners and businesses for the installation of renewable...

309

u.s. Dl!PARThIENT OF ENERGY EERE PROJECT MANAGEMENT CENTER NEPA DETERMINATION  

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

PARThIENT OF ENERGY PARThIENT OF ENERGY EERE PROJECT MANAGEMENT CENTER NEPA DETERMINATION Page 1 of2 RECIPIENT: University of Oregon STATE: OR PROJECT TITLE: Vapor Transport Deposition for Thin Film III-V Photovoltaics fo'unding Opportunity Announcement Number Procurement Instrument Number NEPA Control Number CID Number DE-FOA..()()()()654 DE-EEOOO5957 GF0-0005957·0Q1 Based on my review of the information concerning the proposed action, as NI<:PA Compliance Officer (authorized under DOE Order 451.1A), I have made the following determination : ex, EA, EIS APPENDIX AND NUMBER: Description: A9 Information gathering, analysis, and dissemination Information gathering (including, but not limited to, literature surveys, inventories, site visits, and audits). data analysis (including, but not limited to, computer modeling), document preparation

310

Research Highlight  

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

Comparing Global Atmospheric Model Simulations of Tropical Convection Comparing Global Atmospheric Model Simulations of Tropical Convection Download a printable PDF Submitter: Lin, Y., Geophysical Fluid Dynamics Laboratory Area of Research: General Circulation and Single Column Models/Parameterizations Working Group(s): Cloud Life Cycle Journal Reference: N/A Mean profiles of (first column) total precipitation normalized Q1, (second column) convective precipitation normalized convective heating, (third column) stratiform heating, and (fourth column) convective mass flux for the (top) wet, (middle) dry, and (bottom) break period from models and available observational estimates. Dashed lines are fine resolution model results. Note the different x axis scale for the third and fourth columns. An intercomparison of global atmospheric model simulations of tropical

311

DOE Review  

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

Review 2007 Review 2007 AWA Facility Update, High Gradient Wakefield Generation, and Future Upgrades Manoel Conde, Sergey Antipov, Felipe Franchini, Wei Gai, Feng Gao, Chunguang Jing, Richard Konecny, Wanming Liu, Jidong Long, John Power, Haitao Wang, Zikri Yusof Argonne Wakefield Accelerator Group High Energy Physics Division April 25 - 27, 2007 2 Outline Description of AWA Facililty. Wakefield structures built and tested. Measurements and simulations. List of next experiments to be performed. Plans for Facility upgrades. 3 AWA Drive Beamline Drive Gun Linac & Steering Coils Quads Wakefield Structure Experimental Chambers 4.5 m GV GV YAG1 YAG2 Spectrometer YAG5 Dump/ Faraday Cup Slits YAG4 YAG3 ICT1 ICT2 BPM Single bunch operation - Q=1-100 nC - Energy=15 MeV - High Current = 10 kAmp

312

Engineered microbial systems for enhanced conversion of lignocellulosic biomass  

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

752; 752; NO. OF PAGES 6 Please cite this article in press as: Elkins JG, et al. Engineered Q1microbial systems for enhanced conversion of lignocellulosic biomass, Curr Opin Biotechnol (2010), doi:10.1016/ j.copbio.2010.05.008 Available online at www.sciencedirect.com Engineered microbial systems for enhanced conversion of lignocellulosic biomass James G Elkins, Babu Raman and Martin Keller In order for plant biomass to become a viable feedstock for meeting the future demand for liquid fuels, efficient and cost- effective processes must exist to breakdown cellulosic materials into their primary components. A one-pot conversion strategy or, consolidated bioprocessing, of biomass into ethanol would provide the most cost-effective route to renewable fuels and the realization of this technology is being actively pursued by both multi-disciplinary research centers and

313

Mr. James Schaus Vice President  

Office of Legacy Management (LM)

Mr. James Schaus Mr. James Schaus Vice President Finance and Administration Niagara Cold Drawn Corp. 110 Hopkins Street P.O. Box 399 Buffalo, New York 14240 Dear Mr. Schaus: This is to notify you that the U.S. Department of Energy (DOE) has designated the former Bliss & Laughlin Steel Company facility for remedial action as a part of the Formerly Utilized Sites Remedial Action Program. Remedial activities are managed by the DOE Oak Ridge Field Office, and Mr. Ron Kirk (615-576-7477) will be the site manager. As a result of the designation decision, Mr. Kirk will be the appropriate point of contact in the future. If you have any questions, please call me at 301-903-8149. Sincerely, /' /f-j , f-i 4 /fi /C q--1 - ,i/ -' uj %I&//& L' /< 1 i&x.-:,

314

Quarterly Coal Report  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Distribution Category UC-950 Quarterly Coal Report January-March 1999 Energy Information Administration Office of Coal, Nuclear, Electric and Alternate Fuels U.S. Department of Energy Washington, DC 20585 This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the Department of Energy. The information contained herein should not be construed as advocating or reflecting any policy position of the Department of Energy or any other organization. Contacts This publication was prepared by Paulette Young under the direction of B.D. Hong, Leader, Coal Infor- mation Team, Office of Coal, Nuclear, Electric and Alternate Fuels. Questions addressing the Appendix A, U.S. Coal Imports section should be directed

315

DOE/EIA-0202(84/1Q) Short-Term Energy Outlook Quarterly Projections  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Short-Term Energy Outlook Quarterly Projections February 1984 Published: March 1984 Energy Information Administration Washington, D.C. t rt jrt- .ort- iort- iort- .iort- iort- lort-

316

Spot Award Recipient List-complete 11-2013.xlsx  

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

Recipient Recipient Division Date Award For (Pictures) Kurt Ettinger EHS 09/2013 Kurt created Smartsheets for the Fall Protection Permit Inventory and helped develop a digital Fall Protection Matrix which tracks real-time projects that require fall protection systems to protect workers from fall hazards. The effort enabled a scientist complete required training and obtain permit off-site for work near Pemberton, NJ. Kurt's effort also enables EHS to introduce paperless record keeping processes to the Fall Protection Competent Person Group in Q1FY14. David Mustar FA 09/2013 On a Saturday before dawn, David was walking in the B71 area checking on liquid nitrogen tanks when he heard a faint sound. After a considerable time searching for the source of the sound, he came near a trailer and realized

317

Research Highlight  

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

Weather Forecasting in the Tropics with Climate Models Is Feasible Weather Forecasting in the Tropics with Climate Models Is Feasible Submitter: Boyle, J., Lawrence Livermore National Laboratory Area of Research: General Circulation and Single Column Models/Parameterizations Working Group(s): Cloud Modeling Journal Reference: Climate Model Forecast Experiments for TOGA-COARE. J. Boyle,S. Klein,G. Zhang,S. Xie,X. Wei. Accepted by Monthly Weather Review Figure 1. Profiles of the apparent heat source (Q1) at the TOGA-COARE central site for the observations and day-two forecasts of the CAM, CAM with Zhang modification (ZMO), and AM2 averaged over the entire TOGA-COARE period are shown. Units are degrees Kelvin day. The CAM with the Zhang modified deep convection produced the best fit to the observations. Proper simulation of both the magnitude and level of maximum heating were shown to

318

Frequently Asked Questions about the New ISM Manual  

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

FREQUENTLY ASKED QUESTIONS FREQUENTLY ASKED QUESTIONS (ABOUT THE NEW ISM MANUAL) Questions about Attachment 2 Q1: How important is Attachment 2? A: Attachment 2 is very important to obtaining a full understanding of the vision for full ISM implementation, at multiple, interacting levels, from the enterprise-level to the site-level, from the facility-level to the activity-level. The Attachment states: "This Attachment provides the vision for DOE to achieve the essential attributes of a high-performing organization, and further improve the Department's safety record and productivity record. This vision captures the elements needed for DOE to move beyond a compliance-based approach to a performance-based approach, consistent with more mature high-reliability organizations."

319

U.S. DEPARTMENT OF ENERGY EERE PROJECT MANAGEMENT CENTER NEPA DETElUIINATION  

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

DETElUIINATION DETElUIINATION Page 1 of2 RECIPIENT:Emerson Electric Company STATE: GA PROJECT TITLE: Recovery Act: Water Heater Zigbee Open Standard Wireless Controller Funding Opportunity Announcement Number DE-FOA-QOOO119 Procurement Instrument Number DE-EE0004000 NEPA Control Number GFO-OOO4O()(H}Q1 CID Number G04000 Based on my review of the information concerning the proposed action, as NEPA Compliance Officer (authorized under DOE Order451.IA), I have made the following determination: CX, EA, EIS APPENDIX AND NUMBER: Description: 85,1 Actions to (a) Actions to conserve energy or water, demonstrate potential energy or water conservation, and promote conserve energy effiCiency that would not have the potential to cause significant changes in the indoor or outdoor

320

Frequently Asked Questions - DOE O 420.1C  

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

Frequently Asked Questions Regarding DOE Order 420.1C, Facility Safety, and its supporting directives, DOE-STD-1020-2012, Natural Phenomena Hazards Analysis and Design Criteria for DOE Facilities, and DOE-STD-1066-2012, Fire Protection Q-1: For existing facilities how do I determine the list of applicable design codes and standards? A: For existing facilities the code of record (i.e. those codes and standards in effect at the time that the facility was designed) is the list of applicable design codes and standards. In the case of major modifications to existing facilities, the design codes and standards of O 420.1C apply. Q-2: I work at an existing facility. What changes in DOE O 420.1C do I have to be concerned about?

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


321

Total U.S. Housing Units........................................  

U.S. Energy Information Administration (EIA) Indexed Site

5.6 5.6 17.7 7.9 Do Not Have Heating Equipment........................... 1.2 Q Q N Have Space Heating Equipment............................ 109.8 25.6 17.7 7.9 Use Space Heating Equipment............................. 109.1 25.6 17.7 7.9 Have But Do Not Use Equipment.......................... 0.8 N N N Space Heating Usage During 2005 Heated Floorspace (Square Feet) None................................................................. 3.6 0.5 Q Q 1 to 499............................................................. 6.1 0.9 0.6 0.2 500 to 999......................................................... 27.7 5.7 3.6 2.1 1,000 to 1,499................................................... 26.0 5.2 3.9 1.3 1,500 to 1,999................................................... 17.6 3.9 2.7 1.2 2,000 to 2,499...................................................

322

Quarterly Coal Report, January-March 1997  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Distribution Category UC-950 Quarterly Coal Report January-March 1997 Energy Information Administration Office of Coal, Nuclear, Electric and Alternate Fuels U.S. Department of Energy Washington, DC 20585 This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the Department of Energy. The information contained herein should not be construed as advocating or reflecting any policy position of the Department of Energy or any other organization. Contacts This publication was prepared by Paulette Young under the direction of Mary K. Paull, Acting Chief, Coal Data Branch, Coal and Electric Data and Renewables Division, Office of Coal, Nuclear, Elec- tric and Alternate Fuels. Questions addressing the

323

U.S. Department of Energy Categorical Exclusion Determination Form  

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

Dismantlement and Removal of 321-M Solvent Storage Tank Area Dynamic Underground Stripping (DUS I) Remnants Dismantlement and Removal of 321-M Solvent Storage Tank Area Dynamic Underground Stripping (DUS I) Remnants Savannah River Site Aiken/Aiken/South Carolina Dynamic Underground Stripping (DUS) at SRS was first deployed at the 321-M Solvent Storage Tank Area (west of the former Building 321-M) to remediate solvent source zone contamination in the vadose zone. The deployment was successful and the DUS equipment has been removed. However, the wells associated with the deployment, as well as the operating header of a portable soil vapor extraction unit (SVEU) and assorted debris remain at the site. The purpose of this activity is to abandon the wells per Manual 3Q1 requirements, dismantle and remove for disposal assorted equipment that is no longer required, and to perform general housekeeping at the site of the original DUS deployment.

324

ESS 2012 Peer Review - Tehachapi Wind Energy Storage Project Using Li-Ion Batteries - Christopher Clarke, SCE  

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

Tehachapi Storage Project (TSP) Tehachapi Storage Project (TSP) American Recovery and Reinvestment Act Funded Project Christopher R. Clarke - Southern California Edison (SCE) christopher.r.clarke@sce.com Examples of Wind Generation in the Tehachapi Wind Resource Area August 2012 June 2012 May 2012 February 2012 April 2012 Progress To Date * Facility construction expected to complete in September 2012 * First Power Conversion System installed September 13, 2012 * A123 to ship initial battery equipment for delivery week of September 24, 2012 Future Major Milestones * September 2012 - Completion of BESS facility * October 2012 - Initial installation * November 2012 - Installation of second Power Conversion Subsystem * Q1 2013 - Install balance of equipment and commissioning * Q2 2013 - Start of 2 year M&V testing and reporting

325

b25.pdf  

U.S. Energy Information Administration (EIA) Indexed Site

4,657 4,657 3,239 1,546 1,520 110 62 130 Building Floorspace (Square Feet) 1,001 to 5,000 .............................................. 2,348 1,456 795 574 Q Q Q 5,001 to 10,000 ............................................ 1,110 778 317 429 Q Q Q 10,001 to 25,000 .......................................... 708 574 265 274 14 9 31 25,001 to 50,000 .......................................... 257 222 87 127 9 14 Q 50,001 to 100,000 ........................................ 145 127 51 71 5 9 Q 100,001 to 200,000 ...................................... 59 54 21 31 Q 5 Q 200,001 to 500,000 ...................................... 23 21 7 12 2 2 Q Over 500,000 ............................................... 7 7 4 3 Q 1 N Principal Building Activity Education .................................................... 327 240 95 132 9 19 Q Food Sales ..................................................

326

" Million U.S. Housing Units" ,,"2005 Household Income",,,,,"Below Poverty Line","Eligible for Federal Assistance1"  

U.S. Energy Information Administration (EIA) Indexed Site

2 Living Space Characteristics by Household Income, 2005" 2 Living Space Characteristics by Household Income, 2005" " Million U.S. Housing Units" ,,"2005 Household Income",,,,,"Below Poverty Line","Eligible for Federal Assistance1" ,"Housing Units (millions)" ,,"Less than $20,000","$20,000 to $39,999","$40,000 to $59,999","$60,000 to $79,999","$80,000 or More" "Living Space Characteristics" "Total",111.1,26.7,28.8,20.6,13.1,22,16.6,38.6 "Floorspace (Square Feet)" "Total Floorspace1" "Fewer than 500",3.2,1.9,0.9,"Q","Q","Q",1.3,2.3 "500 to 999",23.8,10.5,7.3,3.3,1.4,1.2,6.6,12.9 "1,000 to 1,499",20.8,5.8,7,3.8,2.2,2,3.9,8.9

327

b8.pdf  

U.S. Energy Information Administration (EIA) Indexed Site

4,657 4,657 419 499 763 665 774 846 690 Building Floorspace (Square Feet) 1,001 to 5,000 .............................................. 2,348 227 270 359 321 367 413 390 5,001 to 10,000 ............................................ 1,110 107 102 240 166 193 156 145 10,001 to 25,000 .......................................... 708 63 90 97 84 130 179 65 25,001 to 50,000 .......................................... 257 13 20 39 53 44 43 44 50,001 to 100,000 ........................................ 145 7 9 19 24 26 33 27 100,001 to 200,000 ...................................... 59 Q 5 5 12 8 15 12 200,001 to 500,000 ...................................... 23 Q 2 3 4 4 4 4 Over 500,000 ............................................... 7 Q 1 1 1 2 2 1 Principal Building Activity Education .................................................... 327

328

Lessons Learned Quarterly Report, March 2013 | Department of Energy  

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

March 2013 March 2013 Lessons Learned Quarterly Report, March 2013 In this issue, we highlight the many benefits of NEPA to DOE, including improved planning, and better public involvement and environmental protection. Articles in this issue include: Sharing DOE's NEPA Success Stories Integrating NEPA and Project Planning Works Minimize EIS Printing Costs DOE Cooperating Agency Report Electronic Guidance Compendium Tribal Energy Resource CEQ IT Working Group Conferences DOE-wide NEPA Contracts Update Transitions EAs and EISs Completed This Quarter Questionnaire Results Cost and Time Facts LLQR-2013-Q1.pdf More Documents & Publications Lessons Learned Quarterly Report, December 2012 Lessons Learned Quarterly Report, March 2013 Lessons Learned Quarterly Report, June 2013 Lessons Learned Quarterly Report, September

329

Quarterly Coal Report January-March 1996  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Distribution Category UC-950 Quarterly Coal Report January-March 1996 Energy Information Administration Office of Coal, Nuclear, Electric and Alternate Fuels U.S. Department of Energy Washington, DC 20585 This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the Department of Energy. The information contained herein should not be construed as advocating or reflecting any policy position of the Department of Energy or any other organization. Contacts This publication was prepared by Paulette Young under the direction of Noel C. Balthasar, Chief, Coal Data Branch, Coal and Electric Data and Renewables Division, Office of Coal, Nuclear, Electric and Alter- nate Fuels. Specific information about

330

QUARTER SHORT-TERM ENERGY OUTLOOK QUARTERLY PROJECTIONS ENERGY INFORMATION ADMINISTRATION  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) 1991 1 QUARTER SHORT-TERM ENERGY OUTLOOK QUARTERLY PROJECTIONS ENERGY INFORMATION ADMINISTRATION February 1991 This publication may be purchased from the Superintendent of Documents, U.S. Government Printing Office. Purchasing in formation for this or other Energy Information Administration (EIA) publications may be obtained from the Government Printing Office or ElA's National Energy Information Center. Questions on energy statistics should be directed to the Center by mail, telephone, or telecommunications device for the hearing impaired. Addresses, telephone numbers, and hours are as follows: National Energy Information Center, El-231 Energy Information Administration Forrestal Building, Room 1F-048 Washington, DC 20585 (202) 586-8800 Telecommunications Device for the

331

QCRS  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Distribution Category UC-950 Quarterly Coal Report January-March 2000 Energy Information Administration Office of Coal, Nuclear, Electric and Alternate Fuels U.S. Department of Energy Washington, DC 20585 This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the Department of Energy. The information contained herein should not be construed as advocating or reflecting any policy position of the Department of Energy or any other organization. Contacts This publication was prepared by Paulette Young under the direction of Betsy O'Brien, Director, Coal, Electric and Renewables Division, Office of Coal, Nuclear, Electric and Alternate Fuels. Questions addressing the Appendix A, U.S. Coal Imports section

332

Heating Oil and Propane Update  

Gasoline and Diesel Fuel Update (EIA)

State Energy Offices State Energy Offices Q1: What price should be reported to EIA when submitting weekly data? EIA requests that you collect / report the residential credit price (keep-full prices being preferred) and that all prices exclude taxes for the Monday of each survey week, even if that Monday falls on a holiday. Prices should not include discounts for payment of cash or for payment made within a short period of time. However, if a company deals exclusively in cash, then this price should be reported and noted in the file sent to EIA. Q2: When is this data due to EIA each week? The EIA-877 "Winter Heating Fuels Telephone Survey" will begin the first Monday in October. Data should be submitted to EIA as soon as they are available but no later than noon on Tuesday of each week. Data collection

333

B. S. Wolf, Y.D., Ibed%& '  

Office of Legacy Management (LM)

S. Wolf, Y.D., Ibed%& ' S. Wolf, Y.D., Ibed%& ' Direotor..~ ' .' .. .., ,- : ,, ,. ,~ WEEKLY ACTIVITY REPORT 4JZ!Q$% 1' ti &IL 7 ,. ' . .,;;;,: ., ' is: * A oanferenbe ia& h&of the ti' Produotion, "Seourlty and uediO& Dlvi~lon~ on tho Pormtiiation of plans in the event of dienntora 2: our plants. Itwa.9 ae0id6d to invite oontraotor representatives CO ,.I 6 The klioal Mieota had a oonfe&oc ' jxt tho' ~rgonns IiatiOr& Lnb&toly on problems arising from the dlspoaal of rndioaotiw waste aaterikle. = The Chief, Health and Safety Branoh dellvorecl B paper at tic oonferenoe of the Amerioan Industrial f$giene Aaeoolation at Boston, Mess. on "Rnvlr~montal Studleo in ,Plante and Laboratoriee Uelng B~rylllti". A oonfomnoe wae held with repreeontativss of the Bellex Corporation

334

An Investigation of Coupling of the Internal Kink Mode to Error Field Correction Coils in Tokamaks  

SciTech Connect (OSTI)

The coupling of the internal kink to an external m/=1/1 pertubation if studied for profiles that are known to result in a saturated internal kink in the limit of a cylindrical tokamak. It is found from 3D equilibrium calculations that, for A 30 circular plasmas and A=3 elliptical shapes, this coupling of the boundary perturbation to the internal kink is strong; the amplitude of the m/n=1/1 structure at q=1 is large compared to the amplitude applied at the plasma boundary. It is proposed that this excitation, which could readily be applied with error field correction coils, be explored as a mechanism for controlling sawtooth amplitudes in high performance tokamak discharges. This saturated internal kink, resulting from small field errors in proposed as an explanation for the TEXTOR measurements of q0 and the distinction between sawtooth effects on the q-profile observed in TEXTOR and DIII-D.

Lazarus, Edward Alan [ORNL] [ORNL

2013-01-01T23:59:59.000Z

335

Deformed Statistics Formulation of the Information Bottleneck Method  

E-Print Network [OSTI]

A candidate variational principle for the information bottleneck (IB) method is formulated within the ambit of the generalized nonadditive statistics of Tsallis. Given a nonadditivity parameter $ q $, the role of the \\textit{additive duality} of nonadditive statistics ($ q^*=2-q $) in relating Tsallis entropies for ranges of the nonadditivity parameter $ q 1 $ is described. Defining $ X $, $ \\tilde X $, and $ Y $ to be the source alphabet, the compressed reproduction alphabet, and, the \\textit{relevance variable} respectively, it is demonstrated that minimization of a generalized IB Lagrangian defined in terms of the nonadditivity parameter $ q^* $ self-consistently yields the \\textit{nonadditive effective distortion measure} to be the \\textit{$ q $-deformed} generalized Kullback-Leibler divergence: $ D_{K-L}^{q}[p(Y|X)||p(Y|\\tilde X)] $. This result is achieved without enforcing any \\textit{a-priori} assumptions. Finally, it is proven that the nonadditive free energy of the system in $ q^* $ space is non-ne...

Venkatesan, R C

2008-01-01T23:59:59.000Z

336

Effect of the counterrotating terms on polarizability in atom-field interactions  

E-Print Network [OSTI]

Effect of the counterrotating terms on polarizability in atom-field interactions Da-wei Wang,1 Ai-jun Li,2 Li-gang Wang,1 Shi-yao Zhu,1,3 and M. Suhail Zubairy4 1Center of Optical Sciences and Department of Physics, The Chinese University of Hong...#1;#3;z#1;t#2; #16;#3;#3;+#1;t#1;#2; + #3;#1;t#1;#2;#4;ei#2;q#1;t#1;?t#2; ? H.c.#7; . #1;8#2; WANG et al. PHYSICAL REVIEW A 80, 063826 #1;2009#2; 063826-2 Suppose the initial field state is a coherent state with wave vector q0 and frequency #2;, i...

Wang, Da-wei; Li, Ai-jun; Wang, Li-gang; Zhu, Shi-yao; Zubairy, M. Suhail

2009-01-01T23:59:59.000Z

337

The well ordering of sets and applications to functions  

E-Print Network [OSTI]

) = m(S)~ Also, since S c U and fa~b) c U 20 m(Q. [aJb] + S) & 1(U), On the other hand, we have m(Q. fa Jb] ) + m(S) & v + -Pal(U). These last tge inequalities give 1(U) v + Q 1(U), or 1(U) (1 - + ) & v, or 1(U) ? + & v. Hence ~ 1(U) ? & v, so e... numbers j/)b) and k/ ib( of Hb suoh that J ~ k e 8 and ]/(bl -Ml bI R ~ z'at Zonal, Thus, ] k-br ~ 0 j wbsx'e r is either R or -R. This cozztradicts Theorem 13, however& Hence our assumption is false and m(H) ~ 0 ~ THEOREM 16 ' Zf f is a funct1on...

Pearcy, Carl Mark

2012-06-07T23:59:59.000Z

338

Motion of the guest ion as precursor to the first-order phase transition in the cage system GdB6  

Science Journals Connector (OSTI)

The motion of guest Gd ions in oversized boron cages in GdB6 was investigated from phonon spectra measurements obtained by inelastic x-ray scattering. The measured phonon modes soften by about 10% from 300 K down to TN=16 K, in particular, the longitudinal phonon for the propagation vector q1=(1/2,0,0) that characterizes the distorted structure below TN. Besides, the dispersion relation curves show kinklike anomalies at qk=(0.38,0.38,0). The observed results imply that the motion of the guest Gd ion interplays with the f electrons magnetoelastically and with carriers via Fermi surface nesting. The anomalous properties previously reported for this material far above TN originate from the strong electron-phonon coupling, which causes the motion of guest ions as precursors to the first-order phase transition.

Kazuaki Iwasa; Ryosuke Igarashi; Kotaro Saito; Claire Laulh; Toshihiko Orihara; Satoru Kunii; Keitaro Kuwahara; Hironori Nakao; Youichi Murakami; Fumitoshi Iga; Masafumi Sera; Satoshi Tsutsui; Hiroshi Uchiyama; Alfred Q. R. Baron

2011-12-28T23:59:59.000Z

339

First evidence of Alfven wave activity in KSTAR plasmas  

E-Print Network [OSTI]

We report on first evidence of wave activity during neutral beam heating in KSTAR plasmas: 40 kHz magnetic fluctuations with a toroidal mode number of n=1. Our analysis suggests this a beta-induced Alfven eigenmode resonant with the q=1 surface. A kinetic analysis, when coupled with electron temperature measurements from electron cyclotron emission and ion/electron temperature ratios from crystallography, enables calculation of the frequency evolution, which is in agreement with observations. Complementary detailed MHD modelling of the magnetic configuration and wave modes supports the BAE mode conclusion, by locating an n=1 mode separated from the continuum in the core region. Finally, we have computed the threshold to marginal stability for a range of ion temperature profiles. These suggest the BAE can be driven unstable by energetic ions when the ion temperature radial gradient is sufficiently large. Our findings suggest that mode existence could be used as a form of inference for temperature profile consi...

Hole, M J; Woo, M H; Bak, J G; Sharapov, S E; Fitzgerald, M

2013-01-01T23:59:59.000Z

340

Factorizations of some weighted spanning tree enumerators  

E-Print Network [OSTI]

.08.003, Open Access version: http://kuscholarworks.ku.edu/dspace/ 4 JEREMY L. MARTIN AND VICTOR REINER In particular, setting yi = xi gives X T2Tree(G) xdeg(T) = x1x2 xn n 1Y r=2 0 @ 0rX i=1 xi 1 A: The proof, sketched in Section 6, proceeds by identi... S [n] x S x[n]nS 1 2 degT (S) = Y edges fS;Rg in T xSxR x[n] (6) Theorem 3. X T2Tree(Qn) qdir(T)xwt(T) = q1 qn Y A [n] jAj 2 X i2A qi x 1i + xi : Proof. As before, regard the vertex set of Qn as the power set 2[n]. Denote the symmetric di erence...

Martin, Jeremy L.; Reiner, Victor

2003-11-01T23:59:59.000Z

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341

Shell-Model Analysis for Brueckner Calculations in Light Nuclei  

Science Journals Connector (OSTI)

Brueckner self-consistent calculations are performed for O16, H3, and He4 nuclei with various modern hard-core interactions. Elements of the G matrix are calculated by the reference-spectrum method, while Q-1 corrections are made by matrix inversion in the proper single-particle space. Thus, it is not assumed that Q commutes with the center-of-mass motion. The prescription for selecting the appropriate spectrum of single-particle excited states is investigated by comparing results of the Brueckner method with other calculations. These comparisons indicate that the particle spectrum should be left unperturbed. One then finds that the Hamada-Johnston, Yale, and Reid (hard-core) interactions yield about one half the binding energy of O16. The calculated results are dissected into shell-model components. This analysis indicates that the short-range part of the hard-core interaction is too strongly repulsive.

Ram K. Tripathi and Paul Goldhammer

1972-07-01T23:59:59.000Z

342

Critical behaviors of black holes in the Einstein-Maxwell gravity with conformal anomaly  

E-Print Network [OSTI]

We study $P-V$ critical behavior of 4-dimensional AdS black hole in the Einstein-Maxwell gravity with conformal anomaly by treating the cosmological constant as a variable related to the thermodynamic pressure. It shows that there is no phase transition if taking $k=0$ or -1. When the charge $q_1$ of conformal field and the coefficient $\\alpha$ satisfy a certain relation, the Van der Waal like phase transition for the spherical black hole can occur in case of the temperature is lower than the small critical temperature or higher than the large one. We also evaluate the critical exponents of the phase transitions and find that the thermodynamic exponents associated with this 4-dimensional AdS black hole coincide with those of the van der Waals fluid.

Zhang, Ming; Yang, Zhan-Ying

2014-01-01T23:59:59.000Z

343

Comparison of an exact analytic second born term with its asymptotic approximations  

E-Print Network [OSTI]

) If we use this wave to calculate the scattering amplitude, T ?(Q), for a transition to y we obtain T, ?(Q) = mp & y (r) ~e ' ' Vp(q) + ? dQ"e '( / I l' V (Q/2 ? Q") I 2(H ? e ) + 2k (Q" + Q/2) ? iI, e Vp(Q + Q/2)lxo(r) ) Here ke=vp ~ (6) Q=(Qs Qz... similar to (I+r) '=Q( ? *)' 1=0 Thus equation (19) becomes z &1. (20) 1 ( ? 2(H, ? 6) 2(6' ? e?) y 2k, (Q" y Q/2) ? iI' ~ (2(6 ? s?) + 2k, . (Q" + Q/2) ? fr) where the radius of convergence is not as clearly defined as in the above expansion...

Fitzpatrick, Mathew Jared

2012-06-07T23:59:59.000Z

344

Valuation Network Representation and Solution of Asymmetric Decision Problems  

E-Print Network [OSTI]

are subsets of X, suppose q i is a probability valuation for h, and suppose q j is a probability valuation for g. Then the combination Table 2 Probability valuations in the UCB problem X S r X fS;R 1 g q 1 X fS;R 1 ;R 2 g q 2 p 0.80 p n 1 1 p n 1 n 2 1 l 0.... The marginal of q for h {X}, denoted by q # h fXg , is a probability valuation for h {X} such that q # h X c Rfq c;x jx2W X 3 c;x 2X h g for all c2X h fXg . Suppose q is a probability valuation for r. We say q is a probability distribution for r...

Shenoy, Prakash P.

2000-03-16T23:59:59.000Z

345

Investigation of cracking and leaking of nuclear reactor pools  

E-Print Network [OSTI]

nf Ql ced coal. l 8 te Bnd. 8 5 f t *bi ck out ex' pox't1an Gf 183. nf arced high aensity tlal'3 te. Bggl*egate concx'ete? Tbcx'8 3 8 also 8 O. 2 j xn. BIIUBinUQI liner l Gne 181 ge, slUml num thai lllal cQ1Umn thx'QUgl'I the caner'e*e wall snd. 6... and vertical plane but slope up and down as one portion of cracliing is joined to another (Figure 6b ). fj: V:~N) ~ E P f l: Fignre 6b. Gsl!ch Patherxls on Pood Nail. Gage points have heen located et points. i thxough 6, shovxl on Figare 3q Bhont Kl d...

Cooper, William Bernard

2012-06-07T23:59:59.000Z

346

Equilibrium and Stability of Partial Toroidal Plasma Discharges  

SciTech Connect (OSTI)

The equilibrium and stability of partial toroidal flux ropes are studied in detail in the laboratory, motivated by ubiquitous loop structures on the solar surface. The flux ropes studied here are magnetized arc discharges formed in the Magnetic Reconnection Experiment (MRX). It is found that these loops robustly maintain their equilibrium on time scales much longer than the Alfven time over a wide range of plasma current, guide eld strength, and angle between electrodes, even in the absence of a strapping fi eld. Additionally, the external kink stability of these flux ropes is found to be governed by the Kruskal-Shafranov limit for a flux rope with line-tied boundary conditions at both ends (q > 1).

E. Oz, C. E. Myers, M. Yamada, H. Ji, R. Kulsrud, and J. Xie

2011-01-04T23:59:59.000Z

347

The nexus between electricity consumption and economic growth in Bahrain  

Science Journals Connector (OSTI)

Abstract This paper explores the relationship between electricity consumption, foreign direct investment, capital and economic growth in the case of the Kingdom of Bahrain. The CobbDouglas production is used over the period of 1980Q12010Q4. We have applied the ARDL bounds testing approach and found that cointegration exists among the series. Electricity consumption, foreign direct investment and capital add in economic growth. The VECM Granger causality analysis has exposed the feedback effect between electricity consumption and economic growth and the same is true for foreign direct investment and electricity consumption. This study suggests government authorities to explore new sources of energy to achieve sustainable economic development for the long run.

Helmi Hamdi; Rashid Sbia; Muhammad Shahbaz

2014-01-01T23:59:59.000Z

348

Solution of systems of columns with energy exchange between recycle streams  

E-Print Network [OSTI]

. . t 1, ? l. j+l, i ji ji j-l, i (42) to eliminate one of the flow rate yields, H T'+1 i ( )-)v. ) + (( ( +1) h( ')i)1'') j+1 i j i ji tl) ~ h(T ~ ]). )1 ] 3-1, & (43) After the corrected compositions have been substituted, the result so obtained may... N OB Unit 3: Double-Pipe Heat Exchanger Bl T 02, 0 0 ? 02 Bl T 02 01, 0 Figure 4. A System of Two Columns with Heat Exchange Between Recycle Streams 54 1 gll ~ FX' h (T )' h(T ' ~ b '(h(T h(T ). ) ? d (h(T ), ? h(T ), )) + Q ) ] ? 1 (108...

Haas, Joe Ray

2012-06-07T23:59:59.000Z

349

Inter-ELM Power Decay Length for JET and ASDEX Upgrade: Measurement and Comparison with Heuristic Drift-Based Model  

Science Journals Connector (OSTI)

Experimental measurements of the SOL power decay length (?q) estimated from analysis of fully attached divertor heat load profiles from two tokamaks, JET and ASDEX Upgrade, are presented. Data was measured by means of infrared thermography. An empirical scaling reveals parametric dependency ?q in mm=0.73BT-0.78qcyl1.2PSOL0.1Rgeo0, where BT(T) describes the toroidal magnetic field, qcyl the cylindrical safety factor, PSOL(MW) the power crossing the separatrix and Rgeo(m) the major radius of the device. A comparison of these measurements to a heuristic particle drift-based model shows satisfactory agreement in both absolute magnitude and scaling. Extrapolation to ITER gives ?q?1??mm.

T. Eich; B. Sieglin; A. Scarabosio; W. Fundamenski; R. J. Goldston; A. Herrmann (ASDEX Upgrade Team)

2011-11-14T23:59:59.000Z

350

Numerical solution of the linear least squares problem for splines  

E-Print Network [OSTI]

~ 0 and max a + 0 as k+1 s ss s ss * s knots converge to t , then K -+ ~. Since t' g x for all m, 24 ~t* ? x ~ & 0. Order the x so that x&x&' ~ '&x&t &x?''x 1 2 q q+1 Next suppose that t* lies in the interval [t. , t. ] for j' j+1 some j, 1...=lt J JP1ML = JPI-L VM = VNIKX(L)/{OELTAP(L) + OELTAM{ JP1ML) ) VNIKX(L ) = VM+OELTAP(L ) + VMPREV VMPRFV = VM+DELTAM(JPIML) VNIKX( JP1) = YMPREV J = JPI IF ( J . LT ~ JHIGH) FUNCTION BVALUE ( Te Ae Nt Kw Xt IDERIV ) CALCULATES VALUE AT +X...

Vonderhaar, Thomas Jerome

1975-01-01T23:59:59.000Z

351

Equipment balancing and cost estimating a computer approach  

E-Print Network [OSTI]

Selection(13. 4) REM Selection (13. 4) = Selection (Capacity. Iieneuver, Lode, No. of Dozers) FOR Q=1 TO 13 FOR R=l TO 4 29 READ Selection(Q, R) SolutionScraper (Q, R) = Selection(Q. R) DATA 11, 0. 7, 0. 9, 0, 16, 0. 7, 0. 9. 0, 20. 0. 7. 0. 7. 1. 22... Cos(Scraper(53, 4) FOR I = I T09 READ CostDozer g(l) NEXT I FOR I I T09 FORJ=I T03 READ CostDozer(I J) NEXT J CostDozer(l, 4) = CostDozer(l, 2) NEXT I DATA D38 . D4E . DSB . 06D DATA 07G, 07H, DBL . 09L, D I IN DATA 7, 10, 17, 10, 13. 20...

Cottrell, David Sherman

1987-01-01T23:59:59.000Z

352

A distributed converging overland flow model: 2. Effect of infiltration  

E-Print Network [OSTI]

area; f is dependent on the depth of flow h in the following sense: f(x, t) >0 if h(x, t) >0 f(x, t) = 0 if h(x, t) = 0 We will assume further that q(x, t) > f(x, t) O< t < T 0 < x < L(1 - r) where q is the lateral inflow per unit area..., T is the duration of q, L is the length of the converging section, r is the degree of convergence, and x and t are space and time coordinates. Then the continuity and momentum equations are Oh O(uh) uh q- -- q(x, t) -- ](x, t) q- (1) Ot Ox L -- x Q = uh = a...

Sherman, Bernard; Singh, Vijay P.

353

Computer simulation of the dispersion of carbon monoxide from roadways  

E-Print Network [OSTI]

and that the transport of material in the x-direction is due mainly to the mean wind, one can reduce equation (1) to BB B BV B BB u ? = ? (K ? ) + ? (K ? ) Bx By y By Bz z Bz (4) with the following boundary conditions, 1) I ~ 0 as x -+ 2) V~ asx-+0 (5) 3... are illustrated in Figures 5 and 6. Using equations (24) and (25) with n = 1 and equation (21), the concentration equations (19) and (20) become Q 1 v 21 r&(x, y, z, h) 2rra a u exp P- ? (~) J L2 ~ z z-h) 1 z+h)2 a az 'z (28) t(x, z, h) = exp /2rr a u z...

Maldonado, Cesar

1976-01-01T23:59:59.000Z

354

Nonadditive entropy reconciles the area law in quantum systems with classical thermodynamics  

Science Journals Connector (OSTI)

The BoltzmannGibbsvon Neumann entropy of a large part (of linear size L) of some (much larger) d-dimensional quantum systems follows the so-called area law (as for black holes), i.e., it is proportional to Ld?1. Here we show, for d=1,2, that the (nonadditive) entropy Sq satisfies, for a special value of q?1, the classical thermodynamical prescription for the entropy to be extensive, i.e., Sq?Ld. Therefore, we reconcile with classical thermodynamics the area law widespread in quantum systems. Recently, a similar behavior was exhibited in mathematical models with scale-invariant correlations [C. Tsallis, M. Gell-Mann, and Y. Sato, Proc. Natl. Acad. Sci. U.S.A.102 15377 (2005)]. Finally, we find that the system critical features are marked by a maximum of the special entropic index q.

Filippo Caruso and Constantino Tsallis

2008-08-05T23:59:59.000Z

355

Individual Sawtooth Pacing by Synchronized ECCD in TCV  

SciTech Connect (OSTI)

Previous real-time sawtooth control scenarios using EC actuators have attempted to shorten or lengthen the sawtooth period by optimally positioning the EC absorption near the q = 1 surface. In new experiments we demonstrate for the first time that individual sawtooth crashes can be repetitively induced at predictable times by reducing the stabilizing ECCD power after a predetermined time from the preceding crash. Other stabilizing actuators (e.g. ICRF, NBI) are expected to produce similar effects. Armed with these results, we present a new sawtooth / NTM control paradigm for improved performance in burning plasmas. The potential appearance of neo-classical tearing modes, triggered by long period sawtooth crashes even at low beta, becomes predictable and therefore amenable to preemptive ECCD. The ITER Electron Cyclotron Upper Launcher (EC-UL) design incorporates the needed functionalities for this method to be applied. The methodology and associated TCV experiments will be presented.

Goodman, T. P.; Felici, F.; Canal, G.; Duval, B. P.; Graves, J. P.; Reimerdes, H.; Sauter, O.; Testa, D. [Centre de Recherches en Physique des Plasmas, Ecole Polytechnique Federale de Lausanne (CRPP-EPFL), Lausanne (Switzerland)

2011-12-23T23:59:59.000Z

356

Sawtooth control in ITER using ion cyclotron resonance heating  

SciTech Connect (OSTI)

Numerical modeling of the effects of ion cyclotron resonance heating (ICRH) on the stability of the internal kink mode suggests that ICRH should be considered as an essential sawtooth control tool in ITER. Sawtooth control using ICRH is achieved by directly affecting the energy of the internal kink mode rather than through modification of the magnetic shear by driving localized currents. Consequently, ICRH can be seen as complementary to the planned electron cyclotron current drive actuator, and indeed will improve the efficacy of current drive schemes. Simulations of the ICRH distribution using independent RF codes give confidence in numerical predictions that the stabilizing influence of the fusion-born alphas can be negated by appropriately tailored minority (3)He ICRH heating in ITER. Finally, the effectiveness of all sawtooth actuators is shown to increase as the q = 1 surface moves towards the manetic axis, whilst the passive stabilization arising from the alpha and NBI particles decreases.

Chapman, I. T. [EURATOM CCFE Fus Assoc, Culham Sci Ctr, Abingdon, Oxon, England; Graves, J P [Ecole Polytechnique Federale de Lausanne, Switzerland; Johnson, T. [KTH, EES, EURATOM VR Assoc., Stockholm, Sweden; Asunta, O. [Aalto University, Finland; Bonoli, P. [Massachusetts Institute of Technology (MIT); Choi, M. [General Atomics; Jaeger, E. F. [Oak Ridge National Laboratory (ORNL); Jucker, M. [Ecole Polytechnique Federale de Lausanne, Switzerland; Sauter, O. [Ecole Polytechnique Federale de Lausanne, Switzerland

2011-01-01T23:59:59.000Z

357

Model studies of the effects of certain factors of the marine environment on enzyme activity  

E-Print Network [OSTI]

+jtE6 ]tsji+y i] j=r lt+E6r r6eE+i6lr6j i6 r6C0lr tsjEeEj0 E1 E6j+ib[sjEi6 j?/ l*VKq/ rq?KVTqc/q! j?/ T?/q ./*. ?VT?K?/ * VK?K? /q?KVTqc/q! ?TV !?/KV c^VK*? Kq?*SK!*q!.? j?/ .*)! ?Tq!/q! K. q/*V)^ ?Tq.!*q! *! ??? ?/V ?/q!1 j?/ !/c?/V*!mV/ V*q?/ K.../!*ST)K? ?VT?/../. !T Kq!/Vq*) ??*q?/. SVTm??! *STm! S^ !?/ /q?KVTqc/q!? j?/ Eq!/Vq*) lK)K/m aK?/ *??*V/q!)^ TVK?Kq*!/? Kq !?/ ./*? *q? !?/ ??/cK?*) ?VT? ?/../. T? )K?/ .!K)) !*?/ ?)*?/ Kq * .*)! ?*!/V c/?Kmc ?/q/V*))^ ?K!? * ?= ?/V^ ?)T./ !T !?*! T...

Proctor, Charles Mahan

2013-10-04T23:59:59.000Z

358

Antiferromagnetic spin excitations in single crystals of nonsuperconducting Li$_{1-x}$FeAs  

SciTech Connect (OSTI)

We use neutron scattering to determine spin excitations in single crystals of nonsuperconducting Li1 xFeAs throughout the Brillouin zone. Although angle resolved photoemission experiments and local density approximation calculations suggest poor Fermi surface nesting conditions for antiferromagnetic (AF) order, spin excitations in Li1 xFeAs occur at the AF wave vectors Q = (1,0) at low energies, but move to wave vectors Q = ( 0.5, 0.5) near the zone boundary with a total magnetic bandwidth comparable to that of BaFe2As2. These results reveal that AF spin excitations still dominate the low-energy physics of these materials and suggest both itinerancy and strong electron-electron correlations are essential to understand the measured magnetic excitations.

Wang, Meng [ORNL; Wang, X.C. [Beijing National Laboratory for Condensed Matter Physics/Chinese Academy of Scie; Abernathy, Douglas L [ORNL; Harriger, Leland W [ORNL; Luo, H.Q. [Beijing National Laboratory for Condensed Matter Physics, Institute of Physics; Zhao, Yang [ORNL; Lynn, J. W. [National Institute of Standards and Technology (NIST); Liu, Q.Q. [Beijing National Laboratory for Condensed Matter Physics, Institute of Physics; Jin, C.Q. [Beijing National Laboratory for Condensed Matter Physics, Institute of Physics; Fang, Chen [Purdue University; Hu, Jiangping [Purdue University and Chinese Academy of Sciences; Dai, Pengcheng [University of Tennessee, Knoxville (UTK)

2011-01-01T23:59:59.000Z

359

Low-Lying Energy Levels in Sc41  

Science Journals Connector (OSTI)

The reaction Ca40(d,n)Sc41 was studied at 4.15-Mev bombarding energy using nuclear emulsions as detectors. Four groups of neutrons were observed with Q values of -0.57, -2.43, -2.64, and -2.85 Mev. The observed angular distributions can be fitted with distirbution curves obtained from stripping analysis on the basis of r0=6.0 fermi and lp=3,1,1,1, respectively. Two additional groups of questionable assignment were observed at Q=-1.13and-1.41 Mev. Neutron groups from reactions on C12 and O16 were also observed and served to confirm the beam calibration as well as background and other correction methods.

H. S. Plendl and F. E. Steigert

1959-12-15T23:59:59.000Z

360

Page not found | Department of Energy  

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

21 - 24230 of 26,764 results. 21 - 24230 of 26,764 results. Download Testimony Before the House Energy and Commerce Subcommittee on Energy and Environment Subject: Renewable Portfolio Standards By: Howard Gruenspecht, Acting Administrator, Energy Information Administration http://energy.gov/congressional/downloads/testimony-house-energy-and-commerce-subcommittee-energy-and-environment Download Microsoft PowerPoint- DOE Supplemental Instructions for OMB Section 1512 Reporting Grant and Loan Recipients Q1 2010 [Compati http://energy.gov/downloads/microsoft-powerpoint-doe-supplemental-instructions-omb-section-1512-reporting-grant-and Download Inspection Report: INS-O-10-02 Severance Repayments at the Savannah River Site http://energy.gov/ig/downloads/inspection-report-ins-o-10-02 Download Audit Report: IG-0453

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
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361

QCRS  

Gasoline and Diesel Fuel Update (EIA)

1Q) 1Q) Distribution Category UC-950 Quarterly Coal Report January-March 2001 Energy Information Administration Office of Coal, Nuclear, Electric and Alternate Fuels U.S. Department of Energy Washington, DC 20585 This report was prepared by the Energy Information Administration, the independent statistical and analytical agency within the Department of Energy. The information contained herein should not be construed as advocating or reflecting any policy position of the Department of Energy or any other organization. Energy Information Administration/Quarterly Coal Report January-March 2001 ii Contacts This publication was prepared by Paulette Young under the direction of Betsy O'Brien, Director, Coal, Electric and Renewables Division, Office of Coal, Nuclear, Electric and Alternate Fuels. Questions

362

Microsoft Word - Mar98_report  

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

7 7 MODELING STUDIES ON THE LOW β y LATTICE Annick Ropert, ESRF Introduction The N = 40 low β y lattice (which had not been used since Run 1997-7) was re-commissioned at the beginning of Run 1998-2. The testing of the optics addressed several puzzling questions: - strong discrepancy of the vertical β-function with respect to the model, thus making it necessary to detune Q1 by more than 6% in order to get closer to theoretical β- functions, - very small energy acceptance, which is very likely responsible for the moderate lifetime, - strong dependence of the lifetime on the closed orbit pattern. These pending questions have triggered the work presently reported in this note. The studies were focused on understanding the discrepancies between the real machine and the model and

363

T. Khoe  

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

TK-LS (3/4/85) LS-1S TK-LS (3/4/85) LS-1S T. Khoe March 4, 1985 Chromaticity Correction and Betafunction Distortion The required value of the chromaticity is otained by introducing sextupole magnets in the dispersive straight sections = - ~ f S (K - Sn) d s , Q1fV I dB where K = -- --l is the focusing strength of the lattice Bp dx Z I d By quadrupoles, S = -- -----2- the strength of the correction sextupoles and n is Bp dx the dispersion function. About one half of the quadrupoles are located in dispersion-free straight sections. Furthermore, the natural chromaticity of the low-emittance lattice is large and one will have large harmonic components in the Fourier series expansion of 6(K - Sn). Since the beta functions depend on the focusing strength, these Fourier components will effect the beta

364

Property:Product | Open Energy Information  

Open Energy Info (EERE)

Product Product Jump to: navigation, search This is a property of type String. Subproperties This property has the following 208 subproperties: A AEE AG AFS Trinity Power Corp ANV Partners Advanced Plant Pharmaceuticals Inc Aeronautica Windpower LLC AgRefresh Agrivert Alliance to Save Energy Alternative Energy Consultants Alternative Energy Finance Ambene American Hydrogen Corporation American Superconductor Corporation AMSC Angelantoni Industrie Spa Apollo Solar Energy Inc Ariane Environment Auriga Energy B Bannockburn Capital LTD Baoding Huide Wind Power Engineering Co Ltd Beijing Haohua Rivers International Water Engineering Consulting Co Ltd BiBB Western Region Bloo Solar formerly Q1 Nanosystems Blue Green Capital C C12 Energy Inc CSR Zhuzhou Electric Locomotive Research Institute

365

Microsoft Word - 176 EFS FAQ-2012.docx  

U.S. Energy Information Administration (EIA) Indexed Site

Frequently Asked Questions Frequently Asked Questions on the Form EIA-176, "Annual Report of Natural Gas and Supplemental Gas Supply & Disposition" The following material provides answers to questions that EIA has received about the Form EIA-176, "Annual Report of Natural and Supplemental Gas Supply and Disposition." The survey collects annual data on natural, synthetic, and other supplemental gas supplies, disposition and certain revenues. If you do not find an answer to your specific question, please contact EIA staff, listed at the end of this product. Q1: I cannot file the information requested by the due date. Is it possible to get an extension? How can I obtain a filing extension for my company? A1: If you are unable to meet the March 1st deadline, please send an email to

366

b31.xls  

U.S. Energy Information Administration (EIA) Indexed Site

4,645 4,645 3,472 1,910 1,445 94 27 128 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,552 1,715 1,020 617 41 N 66 5,001 to 10,000 ................................. 889 725 386 307 Q Q 27 10,001 to 25,000 ............................... 738 607 301 285 16 Q 27 25,001 to 50,000 ............................... 241 217 110 114 Q Q Q 50,001 to 100,000 ............................. 129 119 53 70 Q 5 Q 100,001 to 200,000 ........................... 65 60 27 35 Q 5 Q 200,001 to 500,000 ........................... 25 23 9 14 Q 2 Q Over 500,000 .................................... 7 6 3 3 Q 1 N Principal Building Activity Education .......................................... 386 298 144 149 10 6 15 Food Sales ....................................... 226 186 109 68 Q N Q Food Service .....................................

367

The effect of geometry on symbology recognition  

E-Print Network [OSTI]

displays' Of the twenty geometric forms tested it was reported that the best combinations of five symbols each were 1 ) rectangle, circle, zig-zag Z, cross, and semicircle or 2) cross, semicircle, ellipse, triangle, and square. These studies led...AaTA fiue 1e Tte1ap 1sa[[errrs aq1 uJaosrp o1 1o[rd aq1 aJTnbaJ uot1eurJogut go sadfi1 q1oH srUa1sfis fieydstp pue s1uaurnJ1sut 1geJoJre aq1 rrroJQ pa~taoaJ st uo rlerUJogut 1oaJTpuZ '1geJoJ&e aq1 go 1uarUuoJznua TeuJa1xa aq1 rUoJg pawTaoaJ st uoT, 1errr...

Boyless, James Andrus

2012-06-07T23:59:59.000Z

368

I  

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

BAECC: BAECC: I ni*al S ite L ayout AOS Instrument Field, radars, and containers Instrument F ield a nd C ontainers 6 0 m 9 0 m Met Twr T r e e H e i g h t ~ 2 0 M T r e e H e i g h t ~ 2 0 m Tree Height ~5m T r e e H e i g h t ~ 2 0 m K A Z R B S R W P P D M Rad Tables: mfrsr, TSI skyrad, SPN 10 M Scale M W A C R MWR mounted side by side with 1 m in between scan direction indicated by arrows MWR3C p w r P W R D r o p G P R W P A N T E Q 1 9 0 f t 6 4 f t E Q 2 u n d e r s a c r E Q 1 A N T Snow Fence Measurements a re c lose a pproximates. S ite w as l aid o ut D uring A ug S ite V isit Container P ad D etail AMF2 SACR OPS Van GP Van RWP Van 20' 90' 64' PWR 20' 20' mpl 2d VD MAERI BBSS cart WBRG VCEIL Instrument Field 10" 10' 10" 10" 10" SWACR Antenna EQ1 Van AMFX SACR 20' EQ2 under SACR Instrument F ield 1 1 2 3 2 3 Instrument F ield Looking S outh E ast Looking S outh Looking N orth E ast Looking N orth W---Band a nd K a---Band R adar

369

Temperature Tomography of the Soft X-Ray Corona: Measurements  

Science Journals Connector (OSTI)

We analyze long-exposure and off-pointing Yohkoh/SXT data of the solar corona observed on 1992 August 26. We develop a new (temperature) tomography method that is based on a forward-fitting method of a four-parameter model to the observed soft X-ray fluxes F1(h) and F2(h) of two SXT wavelength filters as a function of height h. The model is defined in terms of a differential emission measure (DEM) distribution dEM(h, T)/dT, which includes also a temperature dependence of density scale heights ?n(T) = q??T and allows us to quantify deviations (q? ? 1) from hydrostatic equilibrium (q? = 1). This parametrization facilitates a proper line-of-sight integration and relates the widely used filter ratio temperature TFR to the peak of the DEM distribution. A direct consequence of the multi-scale height atmosphere is that the filter ratio temperature TFR(h) is predicted to increase with height, even if all magnetic field lines are isothermal. Our model fitting reveals that coronal holes and quiet-Sun regions are in perfect hydrostatic equilibrium but that coronal streamers have a scale height that exceeds the hydrostatic scale height by a factor of up to q? 2.3, which underscores the dynamic nature of coronal streamers. Our density measurements in coronal holes are slightly lower than most of the white-light polarized brightness inversions and seem to come closer to the requirements of solar wind models. Our DEM model provides also a physical framework for the semiempirical Baumbach-Allen formula and quantifies the temperature ranges and degree of hydrostaticity of the K, L, and F coronae.

Markus J. Aschwanden; Loren W. Acton

2001-01-01T23:59:59.000Z

370

Nonlinear quantum equations: Classical field theory  

SciTech Connect (OSTI)

An exact classical field theory for nonlinear quantum equations is presented herein. It has been applied recently to a nonlinear Schrdinger equation, and it is shown herein to hold also for a nonlinear generalization of the Klein-Gordon equation. These generalizations were carried by introducing nonlinear terms, characterized by exponents depending on an index q, in such a way that the standard, linear equations, are recovered in the limit q? 1. The main characteristic of this field theory consists on the fact that besides the usual ?(x(vector sign),t), a new field ?(x(vector sign),t) needs to be introduced in the Lagrangian, as well. The field ?(x(vector sign),t), which is defined by means of an additional equation, becomes ?{sup *}(x(vector sign),t) only when q? 1. The solutions for the fields ?(x(vector sign),t) and ?(x(vector sign),t) are found herein, being expressed in terms of a q-plane wave; moreover, both field equations lead to the relation E{sup 2}=p{sup 2}c{sup 2}+m{sup 2}c{sup 4}, for all values of q. The fact that such a classical field theory works well for two very distinct nonlinear quantum equations, namely, the Schrdinger and Klein-Gordon ones, suggests that this procedure should be appropriate for a wider class nonlinear equations. It is shown that the standard global gauge invariance is broken as a consequence of the nonlinearity.

Rego-Monteiro, M. A.; Nobre, F. D. [Centro Brasileiro de Pesquisas Fsicas and National Institute of Science and Technology for Complex Systems, Rua Xavier Sigaud 150, 22290-180 Rio de Janeiro - RJ (Brazil)] [Centro Brasileiro de Pesquisas Fsicas and National Institute of Science and Technology for Complex Systems, Rua Xavier Sigaud 150, 22290-180 Rio de Janeiro - RJ (Brazil)

2013-10-15T23:59:59.000Z

371

q008.dvi  

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

b b ' (4 th Generation) Quark, Searches for NODE=Q008 b ' -quark/hadron mass limits in p p and p p collisions b ' -quark/hadron mass limits in p p and p p collisions b ' -quark/hadron mass limits in p p and p p collisions b ' -quark/hadron mass limits in p p and p p collisions NODE=Q008BPP NODE=Q008BPP VALUE (GeV) CL% DOCUMENT ID TECN COMMENT >685 (CL = 95%) >685 (CL = 95%) >685 (CL = 95%) >685 (CL = 95%) [>128 GeV (CL = 95%) OUR 2012 BEST LIMIT] >480 >480 >480 >480 95 1 AAD 12AT ATLS B(b ' → W t) = 1 >400 >400 >400 >400 95 2 AAD 12AU ATLS B(b ' → Z b) = 1 >350 >350 >350 >350 95 3 AAD 12BC ATLS B(b ' → W q) = 1 (q=u,c) >685 >685 >685 >685 95 4 CHATRCHYAN 12BH CMS m t ' = m b ' >611 >611 >611 >611 95 5 CHATRCHYAN 12X CMS B(b ' → W t) = 1 >190 >190 >190 >190 95 6 ABAZOV 08X D0 cτ = 200mm >190 >190 >190 >190 95 7 ACOSTA 03 CDF quasi-stable

372

 

U.S. Energy Information Administration (EIA) Indexed Site

3. Energy Sources, Floorspace for Non-Mall Buildings, 2003 3. Energy Sources, Floorspace for Non-Mall Buildings, 2003 Total Floorspace (million square feet) All Buildings* Buildings Using Any Energy Source Energy Sources Used (more than one may apply) Elec- tricity Natural Gas Fuel Oil District Heat District Chilled Water Propane Other a All Buildings* ............................... 64,783 63,343 63,307 43,468 15,157 5,443 2,853 7,076 1,401 Building Floorspace (Square Feet) 1,001 to 5,000 ................................ 6,789 6,362 6,346 3,084 600 Q Q 806 199 5,001 to 10,000 .............................. 6,585 6,212 6,197 3,692 716 Q Q 725 Q 10,001 to 25,000 ............................ 11,535 11,370 11,370 7,053 966 289 Q 1,014 Q 25,001 to 50,000 ............................ 8,668 8,385 8,385 6,025 825 369 240 638 Q

373

b16.xls  

U.S. Energy Information Administration (EIA) Indexed Site

64,783 64,783 15,492 6,166 7,803 10,989 7,934 6,871 9,528 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 4,659 1,264 689 155 Q Q N 5,001 to 10,000 ................................. 6,585 3,323 1,373 1,109 689 Q Q N 10,001 to 25,000 ............................... 11,535 4,006 2,075 2,456 2,113 692 Q N 25,001 to 50,000 ............................... 8,668 1,222 836 1,327 2,920 1,648 667 Q 50,001 to 100,000 ............................. 9,057 704 291 1,157 2,865 2,151 1,518 371 100,001 to 200,000 ........................... 9,064 804 Q Q 1,558 2,014 2,455 1,452 200,001 to 500,000 ........................... 7,176 Q Q Q 533 1,077 1,706 2,571 Over 500,000 .................................... 5,908 Q N N Q Q Q 5,087 Principal Building Activity Education ..........................................

374

Total.................................................................  

U.S. Energy Information Administration (EIA) Indexed Site

49.2 49.2 15.1 15.6 11.1 7.0 5.2 8.0 Have Cooling Equipment............................... 93.3 31.3 15.1 15.6 11.1 7.0 5.2 8.0 Use Cooling Equipment................................ 91.4 30.4 14.6 15.4 11.1 6.9 5.2 7.9 Have Equipment But Do Not Use it............... 1.9 1.0 0.5 Q Q Q Q Q Do Not Have Cooling Equipment................... 17.8 17.8 N N N N N N Air-Conditioning Equipment 1, 2 Central System............................................. 65.9 3.9 15.1 15.6 11.1 7.0 5.2 8.0 Without a Heat Pump................................ 53.5 3.5 12.9 12.7 8.6 5.5 4.2 6.2 With a Heat Pump..................................... 12.3 0.4 2.2 2.9 2.5 1.5 1.0 1.8 Window/Wall Units........................................ 28.9 27.5 0.5 Q 0.3 Q Q Q 1 Unit......................................................... 14.5 13.5 0.3 Q Q Q N Q 2 Units.......................................................

375

Table HC1-5a. Housing Unit Characteristics by Type of Owner-Occupied Housing Unit,  

U.S. Energy Information Administration (EIA) Indexed Site

5a. Housing Unit Characteristics by Type of Owner-Occupied Housing Unit, 5a. Housing Unit Characteristics by Type of Owner-Occupied Housing Unit, Million U.S. Households, 2001 Housing Unit Characteristics RSE Column Factor: Total Owner- Occupied Units Type of Owner-Occupied Housing Unit RSE Row Factors Single-Family Apartments in Buildings With Mobile Homes Two to Four Units Five or More Units 0.4 0.4 1.8 2.1 1.4 Total ............................................... 72.7 63.2 2.1 1.8 5.7 6.7 Census Region and Division Northeast ...................................... 13.0 10.8 1.1 0.5 0.6 11.4 New England .............................. 3.5 3.1 0.2 Q 0.1 16.9 Middle Atlantic ............................ 9.5 7.7 0.9 0.4 0.4 13.4 Midwest ......................................... 17.5 16.0 0.3 Q 1.0 10.3 East North Central ......................

376

char_household2001.pdf  

U.S. Energy Information Administration (EIA) Indexed Site

5a. Household Characteristics by Type of Owner-Occupied Housing Unit, 5a. Household Characteristics by Type of Owner-Occupied Housing Unit, Million U.S. Households, 2001 Household Characteristics RSE Column Factor: Total Owner- Occupied Units Type of Owner-Occupied Housing Unit RSE Row Factors Single-Family Apartments in Buildings With Mobile Homes Two to Four Units Five or More Units 0.3 0.4 2.0 2.9 1.3 Total Owner-Occupied Units ....... 72.7 63.2 2.1 1.8 5.7 6.7 Household Size 1 Person ....................................... 15.8 12.5 0.8 0.9 1.6 10.3 2 Persons ...................................... 25.9 23.4 0.5 0.5 1.5 10.1 3 Persons ...................................... 11.6 9.6 0.5 Q 1.3 12.1 4 Persons ...................................... 11.8 10.9 Q Q 0.7 15.7 5 Persons ...................................... 5.1 4.5 Q Q 0.4 24.2 6 or More Persons

377

b23.xls  

U.S. Energy Information Administration (EIA) Indexed Site

64,783 64,783 63,343 63,307 43,468 15,157 5,443 2,853 7,076 1,401 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 6,362 6,346 3,084 600 Q Q 806 199 5,001 to 10,000 ................................. 6,585 6,212 6,197 3,692 716 Q Q 725 Q 10,001 to 25,000 ............................... 11,535 11,370 11,370 7,053 966 289 Q 1,014 Q 25,001 to 50,000 ............................... 8,668 8,385 8,385 6,025 825 369 240 638 Q 50,001 to 100,000 ............................. 9,057 9,031 9,031 6,683 1,740 574 332 925 Q 100,001 to 200,000 ........................... 9,064 9,018 9,018 6,645 2,927 1,399 793 989 Q 200,001 to 500,000 ........................... 7,176 7,056 7,051 5,679 3,400 1,018 495 1,165 Q Over 500,000 .................................... 5,908 5,908 5,908 4,606 3,981 1,693 822 Q Q Principal Building Activity

378

b41.xls  

U.S. Energy Information Administration (EIA) Indexed Site

64,783 64,783 56,940 11,035 9,041 12,558 2,853 11,636 29,969 1,561 1,232 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 5,007 1,568 675 972 Q Q 1,957 179 Q 5,001 to 10,000 ................................. 6,585 5,408 1,523 563 1,012 Q Q 2,741 207 Q 10,001 to 25,000 ............................... 11,535 9,922 2,173 1,441 1,740 Q 456 5,260 378 Q 25,001 to 50,000 ............................... 8,668 7,776 1,683 1,155 2,301 240 729 4,264 Q Q 50,001 to 100,000 ............................. 9,057 8,331 1,388 1,440 1,958 332 1,722 4,732 Q Q 100,001 to 200,000 ........................... 9,064 8,339 993 1,158 2,259 793 2,366 4,504 Q Q 200,001 to 500,000 ........................... 7,176 6,565 1,136 1,273 1,223 495 3,023 3,834 Q Q Over 500,000 .................................... 5,908 5,591 569 1,334 1,095

379

TableHC14.5.xls  

U.S. Energy Information Administration (EIA) Indexed Site

4.2 4.2 7.6 16.6 Do Not Have Heating Equpment............................ 1.2 0.7 Q 0.7 Have Space Heating Equpment............................. 109.8 23.4 7.5 16.0 Use Space Heating Equpment.............................. 109.1 22.9 7.4 15.4 Have But Do Not Use Equipment.......................... 0.8 0.6 Q 0.5 Space Heating Usage During 2005 Heated Floorspace (Square Feet) None................................................................. 3.6 2.1 Q 1.9 1 to 499............................................................. 6.1 2.1 0.4 1.7 500 to 999......................................................... 27.7 6.0 1.6 4.4 1,000 to 1,499................................................... 26.0 5.2 1.8 3.4 1,500 to 1,999................................................... 17.6 3.9 1.7 2.2 2,000 to 2,499...................................................

380

TableHC4.13.xls  

U.S. Energy Information Administration (EIA) Indexed Site

.. .. 111.1 33.0 8.0 3.4 5.9 14.4 1.2 Indoor Lights Turned On During Summer Number of Lights Turned On Between 1 and 4 Hours per Day......................... 91.8 26.8 6.7 2.8 4.8 11.7 0.9 1........................................................................ 28.6 10.7 1.9 1.2 2.0 5.2 0.4 2........................................................................ 29.5 9.0 2.4 0.7 1.8 3.7 0.3 3........................................................................ 14.7 3.6 1.1 0.4 0.5 1.5 Q 4........................................................................ 9.3 2.0 0.7 0.3 Q 0.7 Q 5 or More........................................................... 9.7 1.5 0.5 Q 0.3 0.5 N Energy-Efficient Bulbs Used........................... 31.1 8.2 2.1 0.7 1.6 3.6 Q 1....................................................................

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


381

set7.pdf  

U.S. Energy Information Administration (EIA) Indexed Site

Heat Heat Pumps Furnaces Individual Space Heaters District Heat Boilers Packaged Heating Units Other All Buildings ............................................... 67,338 61,602 8,923 14,449 17,349 5,534 19,522 25,743 4,073 Building Floorspace (Square Feet) 1,001 to 5,000 .............................................. 6,774 5,684 679 2,271 1,183 Q 463 1,779 250 5,001 to 10,000 ............................................ 8,238 7,090 745 2,848 1,350 Q 1,040 2,301 Q 10,001 to 25,000 .......................................... 11,153 9,865 1,288 3,047 3,021 307 2,047 3,994 401 25,001 to 50,000 .......................................... 9,311 8,565 1,376 1,674 2,218 617 2,591 3,695 510 50,001 to 100,000 ........................................ 10,112 9,597 1,493 1,718 2,492 905 3,698 4,262 511 100,001 to 200,000 ......................................

382

CT NC0  

Office of Legacy Management (LM)

x-L* d! x-L* d! CT NC0 - i , ,. i, .' i :.:(e.!' ,A\~, L.,t, - (iI :i' , . y- 2 .L i ._ 1 c\ :- i;! Ii $ 4. Ci:lc:i.nnati. 39, t>:::i.f> (J&l3 q-1 -3 sui3 Jrn T3 FRCM .I iirz 1 ?j ~ 1.3 bL1 T:' IP !REFOI?T TC 5YC?CZCiC~ :EWllIFl;j",tsSS L' I"JIsIc:;. .:;xli3;. iCAN !fA(=;-fL,yg-j L' sc,, E. $.iCLX:i?, -iIJ,x:q()Is. ON hL4X 24 - 25 ) 1.9tic ;i. A. Quiglel;, A.3, 3, M. ChenauEt gpxrIvB OF TP.~ The purpose of t3is trip was tc observe a proposed method for the dchy- dratim of green salt md to determine that all health and safety measures were being xrried out, SurveiU.ance of this nature provided protection against excessi3z personnel exposure, insured compliance with ICC shipping regulaticns, tion of the equ'~ and determined when adequate decontamira-

383

F  

Office of Legacy Management (LM)

7' )J i b' ' -* . * 1 **-p-d ra . - .., -. -. -. ,- ? i. (, . . . . . ..* . s ,' ;. .-, jd .: ,... ',_ .<'t ':<';. ::-,' -. i y,- , . ,,- ., I ..d . c ~~; ZC ANT %C -~j~~~i-: ~~~~~s~~ !~~~,KS b ~' ,cc,!~~,L' ~~~ N,~,' , ?:;c,:g iz c:~~-&y~ 30 .-.;;.z-' ::; ggf~g.piJ\ ,I..? , .7* -26 g z -_ I . f ;' ., :dy~gj-";:, ;:.:1; : -;; ;-+,,: -. 1; .- . . c J " y&=;@ F / tEfW?& FUS ' *Lx5 ms .xm I? ,ziic%*~g~J&a~ yF.n?-m- - - me rsaa.jxig q 1, c P 32 h qpg?~Io2 m ~i.liB-&& ccsy &tw SL SaaP eax@ &mcl I22 p&g& #a a&! Ya;tj,ss imd a? aacctim &wcivta?d. tri3.s w&s %em f&o zatot $vr the sm~2azl.g b8wisec vas ideci ia' da the S&XI @betrkat pfD~% 5x! 9?w 5z%im.~* Rt o;= c?EA u4 cac5 fpzxh esae? t&9 xf.acr

384

Untitled Document  

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

Post-Upgrade Diagram - Beam Optics Post-Upgrade Diagram - Beam Optics \\serv1\d-drive\mike\drawings\Post Upgrade Diagram Beam Optics.doc Page 1 of 2 Michael Wiplich 09/21/05 9:20 AM MP-6 NII = Steerer = Quad = Faraday Cup = Multiwire = Slits = Beam Xformer = Valve 6DH01 Velocity Selector 6VSB/E 6QV1 (QA) 6QH1 (QB) Fast Valve 6VA007 7TDH1 7TDV1 7MW020 7FC020 7QH1 7QV1 7TDH2 7TDV2 5XF.LE 6XF.HE MP-6 Object Foils 7VP019 7VP021 6VP019 6TDH1 6TDV1 7Q1 Not Used 6MW017 6TV2 6TH2 Electrostatic MP-6 HE Cup MP-6 LE Cup MP-6 Dump Cup = Viewer Viewer Rotary Aperture ESAG Lens N = Foil Holder = Beam Stop MP-6 Beam Stops H/V Magnetic Steerer/Wiggler LE Gate Valve MP6 Object Slits HE Gate Valve = ESAG Lens Patch Panel A MP-6 HE Quad 7DH01 A

385

c21.xls  

Gasoline and Diesel Fuel Update (EIA)

Square Square Feet All Buildings* .................................. 190 341 360 12,543 28,786 21,977 15.1 11.8 16.4 Principal Building Activity Education .......................................... 9 55 45 806 5,378 3,687 11.1 10.2 12.2 Food Sales ....................................... 36 24 Q 747 467 Q 48.8 51.1 Q Food Service ..................................... 47 16 Q 986 664 Q 47.8 24.5 Q Health Care ....................................... 6 17 50 445 835 1,883 13.1 20.5 26.3 Inpatient .......................................... N Q 47 N Q 1,723 N Q 27.0 Outpatient ....................................... 6 11 Q 445 652 Q 13.1 17.4 Q Lodging ............................................. 4 31 34 260 2,274 2,563 14.0 13.5 13.5 Retail (Other Than Mall)..................... 17 28 18 1,363 2,133 821 12.2 12.9 21.5 Office ................................................

386

c9a.xls  

Gasoline and Diesel Fuel Update (EIA)

684 684 446 617 9,022 4,207 8,613 75.8 106.1 71.6 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 87 44 64 788 466 871 110.9 94.8 73.0 5,001 to 10,000 ................................. 67 39 84 957 465 878 69.7 84.8 95.1 10,001 to 25,000 ............................... 77 91 89 1,555 933 1,429 49.4 97.2 62.4 25,001 to 50,000 ............................... 70 56 71 1,062 568 1,239 65.8 98.2 57.5 50,001 to 100,000 ............................. 92 49 78 1,514 492 1,092 61.0 100.2 71.2 100,001 to 200,000 ........................... 119 Q 79 1,426 346 1,007 83.4 Q 78.0 200,001 to 500,000 ........................... 60 Q 68 749 339 977 80.4 Q 69.6 Over 500,000 .................................... Q Q Q Q Q 1,119 Q Q Q Principal Building Activity Education .......................................... 74 53 76 1,198

387

TableHC2.3.xls  

U.S. Energy Information Administration (EIA) Indexed Site

Total................................................................... Total................................................................... 111.1 78.1 64.1 4.2 1.8 2.3 5.7 Household Size 1 Person......................................................... 30.0 18.6 13.2 1.4 0.7 1.3 2.1 2 Persons........................................................ 34.8 26.8 22.9 1.3 0.5 0.7 1.4 3 Persons........................................................ 18.4 12.8 10.7 0.5 0.4 Q 1.0 4 Persons........................................................ 15.9 11.5 9.8 0.6 Q Q 0.9 5 Persons........................................................ 7.9 5.9 5.3 0.2 Q Q 0.3 6 or More Persons........................................... 4.1 2.4 2.1 Q Q N Q 2005 Annual Household Income Category Less than $9,999............................................. 9.9 4.7 3.1 0.3 0.3 Q 0.8 $10,000 to $14,999.........................................

388

 

U.S. Energy Information Administration (EIA) Indexed Site

1. Cooling Equipment, Floorspace for Non-Mall Buildings, 2003 1. Cooling Equipment, Floorspace for Non-Mall Buildings, 2003 Total Floorspace (million square feet) All Build- ings* Cooled Build- ings Cooling Equipment (more than one may apply) Resid- ential- Type Central Air Condi- tioners Heat Pumps Indiv- idual Air Condi- tioners District Chilled Water Central Chillers Pack- aged Air Condi- tioning Units Swamp Coolers Other All Buildings* ............................... 64,783 56,940 11,035 9,041 12,558 2,853 11,636 29,969 1,561 1,232 Building Floorspace (Square Feet) 1,001 to 5,000 ................................ 6,789 5,007 1,568 675 972 Q Q 1,957 179 Q 5,001 to 10,000 .............................. 6,585 5,408 1,523 563 1,012 Q Q 2,741 207 Q 10,001 to 25,000 ............................ 11,535 9,922 2,173 1,441 1,740 Q 456 5,260 378 Q

389

m129.dvi  

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

3100) 3100) I G (J PC ) = ? ? (? ?? ) OMITTED FROM SUMMARY TABLE Narrow peak observed in several (Λ p + pions) and (Λ p + pions) states in Σ - Be reactions by BOURQUIN 86 and in n p and n A re- actions by ALEEV 93. Not seen by BOEHNLEIN 91. If due to strong decays, this state has exotic quantum numbers (B=0,Q=+ 1,S=- 1 for Λ p π + π + and I ≥ 3/2 for Λ p π - ). Needs confirmation. K (3100) MASS K (3100) MASS K (3100) MASS K (3100) MASS VALUE (MeV) DOCUMENT ID ≈ 3100 OUR ESTIMATE ≈ 3100 OUR ESTIMATE ≈ 3100 OUR ESTIMATE ≈ 3100 OUR ESTIMATE 3-BODY DECAYS 3-BODY DECAYS 3-BODY DECAYS 3-BODY DECAYS VALUE (MeV) DOCUMENT ID TECN COMMENT 3054± 11 OUR AVERAGE 3054± 11 OUR AVERAGE 3054± 11 OUR AVERAGE 3054± 11 OUR AVERAGE 3060± 7± 20 1 ALEEV 93 BIS2 K (3100) → Λ p π + 3056± 7± 20 1 ALEEV 93 BIS2 K (3100) → Λ p π - 3055± 8± 20 1 ALEEV 93 BIS2 K (3100) → Λ p π - 3045± 8± 20 1 ALEEV 93 BIS2 K (3100) → Λ p π + 4-BODY DECAYS

390

c8a.xls  

Gasoline and Diesel Fuel Update (EIA)

456 456 1,241 340 5,680 13,999 3,719 80.2 88.7 91.4 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 60 123 37 922 1,283 547 64.9 96.2 67.6 5,001 to 10,000 ................................. 45 111 27 738 1,468 420 61.6 75.4 63.2 10,001 to 25,000 ............................... 71 145 74 1,204 2,443 861 59.0 59.3 Q 25,001 to 50,000 ............................... 107 133 Q 949 1,867 545 112.5 71.1 Q 50,001 to 100,000 ............................. 66 163 71 664 1,797 749 99.0 90.4 95.1 100,001 to 200,000 ........................... 49 278 Q 614 2,422 Q 79.8 114.8 Q 200,001 to 500,000 ........................... Q 118 Q 441 1,148 Q Q 102.4 Q Over 500,000 .................................... Q 171 Q Q 1,572 Q Q 109.0 Q Principal Building Activity Education .......................................... 45 198 Q

391

c12a.xls  

Gasoline and Diesel Fuel Update (EIA)

1,522 3,228 1,772 18,031 33,384 20,243 84.4 96.7 87.6 Building Floorspace (Square Feet) 1,001 to 5,000 ................................. 193 300 193 2,168 2,904 1,850 89.0 103.2 104.2 5,001 to 10,000 ............................... 134 263 165 2,032 3,217 1,784 66.0 81.9 92.5 10,001 to 25,000 ............................. 241 432 226 3,273 5,679 3,707 73.6 76.1 60.9 25,001 to 50,000 ............................. 181 370 191 2,517 4,518 2,347 71.8 81.8 81.5 50,001 to 100,000 ............................ 156 473 285 2,095 4,763 3,433 74.3 99.3 82.9 100,001 to 200,000 .......................... 219 523 323 2,161 4,706 3,350 101.1 111.1 96.5 200,001 to 500,000 .......................... 221 371 160 2,179 3,623 1,692 101.4 102.3 94.3 Over 500,000 ................................... 179 497 Q 1,606 3,974 2,080 111.2 125.0 Q Principal Building Activity

392

MODIS Land Products Subsets  

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

methods methods This section describes methods used to generate MODIS Land Subsets for Collection 4 and Collection 5 data products. Methods for Selected Sites (Collections 4 and 5) Methods for North America Tool (Collection 4) Methods for the Global Tool (Collection 5) Methods for Selected Sites (Collection 4 and 5) Source for Selected Site Data: Full MODIS scenes (1200-km x 1200-km) are initially subset to 11-km x 31-km (Collection 4) or 25-km x 25-km (Collection 5) by the MODAPS; these initial subsets contain the field site or flux tower. Reformatting and additional subsetting to 7-km x 7-km containing the field site or flux tower are done by the ORNL DAAC. Tools Used: The ORNL DAAC uses the MODIS Reprojection Tool (MRT) to reformat the MODIS data from HDF-EOS to binary format. A tool developed at ORNL is then used to convert the binary format to ASCII. The MRT is available from the Land Processes DAAC. Whereas the MRT can also be used to reproject data from its native projection to other projections, ORNL chose to forgo the resampling associated with reprojection to minimize data manipulation and distortion. The MOD12Q1 Land Cover Collection 3 data are in I-Sin projection, and the Collection 4 and Collection 5 data are in Sinusoidal projection.

393

b32.xls  

U.S. Energy Information Administration (EIA) Indexed Site

64,783 64,783 56,478 27,490 28,820 1,880 3,088 1,422 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 4,759 2,847 1,699 116 N 169 5,001 to 10,000 ................................. 6,585 5,348 2,821 2,296 Q Q 205 10,001 to 25,000 ............................... 11,535 9,562 4,809 4,470 265 Q 430 25,001 to 50,000 ............................... 8,668 7,734 3,924 4,055 Q Q Q 50,001 to 100,000 ............................. 9,057 8,412 3,659 5,005 Q 303 Q 100,001 to 200,000 ........................... 9,064 8,300 3,884 4,754 Q 822 Q 200,001 to 500,000 ........................... 7,176 6,680 2,722 4,076 Q 621 Q Over 500,000 .................................... 5,908 5,683 2,824 2,467 Q 1,064 N Principal Building Activity Education .......................................... 9,874 9,481 3,829

394

set5.pdf  

U.S. Energy Information Administration (EIA) Indexed Site

Electricity Electricity Natural Gas Fuel Oil District Heat District Chilled Water Propane Other a All Buildings ............................................... 67,338 65,753 65,716 45,525 13,285 5,891 2,750 6,290 2,322 Building Floorspace (Square Feet) 1,001 to 5,000 .............................................. 6,774 6,309 6,280 3,566 620 Q Q 635 292 5,001 to 10,000 ............................................ 8,238 7,721 7,721 5,088 583 Q Q 986 Q 10,001 to 25,000 .......................................... 11,153 10,851 10,843 7,001 983 414 Q 1,203 290 25,001 to 50,000 .......................................... 9,311 9,175 9,175 6,405 983 660 294 568 250 50,001 to 100,000 ........................................ 10,112 10,034 10,034 7,165 1,612 933 525 865 350 100,001 to 200,000 ...................................... 8,271

395

b8.xls  

U.S. Energy Information Administration (EIA) Indexed Site

4,645 4,645 330 527 562 579 731 707 876 334 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 2,552 174 315 331 298 350 438 481 165 5,001 to 10,000 ................................. 889 71 107 90 120 180 98 158 66 10,001 to 25,000 ............................... 738 55 64 90 95 122 103 151 58 25,001 to 50,000 ............................... 241 19 23 26 33 48 32 39 21 50,001 to 100,000 ............................. 129 7 9 14 22 16 20 28 13 100,001 to 200,000 ........................... 65 Q 5 8 8 10 10 15 8 200,001 to 500,000 ........................... 25 Q 4 2 3 4 4 4 2 Over 500,000 .................................... 7 Q 1 1 0 1 2 1 Q Principal Building Activity Education .......................................... 386 12 26 78 60 58 44 75 32 Food Sales ....................................... 226 Q Q Q Q Q 33 56 Q Food Service .....................................

396

a4.xls  

U.S. Energy Information Administration (EIA) Indexed Site

East East South Central West South Central Mountain Pacific All Buildings .................................... 71,658 3,452 10,543 12,424 5,680 13,999 3,719 9,022 4,207 8,613 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,922 383 676 986 922 1,283 547 788 466 871 5,001 to 10,000 ................................. 7,033 369 800 939 738 1,468 420 957 465 878 10,001 to 25,000 ............................... 12,659 674 1,448 2,113 1,204 2,443 861 1,555 933 1,429 25,001 to 50,000 ............................... 9,382 366 1,022 1,763 949 1,867 545 1,062 568 1,239 50,001 to 100,000 ............................. 10,291 590 1,682 1,712 664 1,797 749 1,514 492 1,092 100,001 to 200,000 ........................... 10,217 448 1,790 1,872 614 2,422 Q 1,426 346 1,007 200,001 to 500,000 ...........................

397

table10.6_02.xls  

U.S. Energy Information Administration (EIA) Indexed Site

6 Capability to Switch Electricity to Alternative Energy Sources, 2002; 6 Capability to Switch Electricity to Alternative Energy Sources, 2002; Level: National Data and Regional Totals; Row: NAICS Codes, Value of Shipments and Employment Sizes; Column: Energy Sources; Unit: Million Kilowatthours. Coal Coke RSE NAICS Total Not Natural Distillate Residual and Row Code(a) Subsector and Industry Receipts(c) Switchable Switchable Gas Fuel Oil Fuel Oil Coal LPG Breeze Other(d) Factors Total United States RSE Column Factors: 0.9 1.4 0.9 1.6 1.7 0.6 0.8 1.7 0.5 0.9 311 Food 68,230 2,270 49,890 239 2,125 17 9 72 0 Q 12.2 311221 Wet Corn Milling 7,098 77 6,062 77 0 0 0 0 0 0 0.9 31131 Sugar 733 21 602 * 11 9 9 0 0 * 1 311421 Fruit and Vegetable Canning 1,987 Q 1,764 Q Q 0 0 25

398

doepresentation.dvi  

U.S. Energy Information Administration (EIA) Indexed Site

Oil Oil Shocks and U.S. External Adjustment Martin Bodenstein, Christopher Erceg, Luca Guerrieri Division of International Finance, Federal Reserve Board April 2008 Net Exports of Petroleum and Products and Goods Trade Balance (percent share of GDP, 1970q1-2007q4) 1970 1975 1980 1985 1990 1995 2000 2005 -7 -6 -5 -4 -3 -2 -1 0 1 Persian Gulf War Iran-Iraq War Iranian Revolution Arab- Israeli War Effects of An Oil Demand Shock that Drives the Price of Oil Up by 20% (Linear Estimator) 1 2 3 4 5 6 7 8 0 5 10 15 20 25 30 Real Oil Price Percent Quarters 1 2 3 4 5 6 7 8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 Overall Trade Balance (GDP share) Percentage Point Quarters Effects of An Oil Demand Shock that Drives the Price of Oil Up by 20% (Linear Estimator) 1 2 3 4 5 6 7 8 -0.2 0 0.2 0.4 0.6 0.8 1 1.2 Non-oil Trade Balance (GDP share) Quarters Percentage Point 1 2 3 4 5 6 7 8 -0.8 -0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 Oil Trade Balance (GDP share)

399

Table 11.2 Electricity: Components of Net Demand, 2010;  

U.S. Energy Information Administration (EIA) Indexed Site

2 Electricity: Components of Net Demand, 2010; 2 Electricity: Components of Net Demand, 2010; Level: National and Regional Data; Row: Values of Shipments and Employment Sizes; Column: Electricity Components; Unit: Million Kilowatthours. Sales and Net Demand Economic Total Onsite Transfers for Characteristic(a) Purchases Transfers In(b) Generation(c) Offsite Electricity(d) Total United States Value of Shipments and Receipts (million dollars) Under 20 91,909 Q 1,406 194 93,319 20-49 86,795 81 2,466 282 89,060 50-99 90,115 215 2,593 1,115 91,808 100-249 124,827 347 11,375 5,225 131,324 250-499 116,631 2,402 24,079 5,595 137,516 500 and Over 225,242 6,485 91,741 20,770 302,699 Total 735,520 9,728 133,661 33,181 845,727 Employment Size Under 50

400

b23.pdf  

U.S. Energy Information Administration (EIA) Indexed Site

67,338 67,338 61,602 17,627 32,729 3,719 5,077 Building Floorspace (Square Feet) 1,001 to 5,000 .............................................. 6,774 5,684 1,567 3,080 482 Q 5,001 to 10,000 ............................................ 8,238 7,090 1,496 4,292 557 Q 10,001 to 25,000 .......................................... 11,153 9,865 3,035 5,320 597 232 25,001 to 50,000 .......................................... 9,311 8,565 2,866 4,416 486 577 50,001 to 100,000 ........................................ 10,112 9,597 2,765 5,261 484 836 100,001 to 200,000 ...................................... 8,271 7,893 2,497 4,128 383 853 200,001 to 500,000 ...................................... 6,851 6,445 1,509 3,531 474 894 Over 500,000 ............................................... 6,628 6,465 1,892 2,701 Q 1,554 Principal Building Activity

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401

m129.dvi  

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

29 29 K (3100) I G (J PC ) = ? ? (? ?? ) OMITTED FROM SUMMARY TABLE Narrow peak observed in several (Λ p + pions) and (Λ p + pions) NODE=M129 states in Σ - Be reactions by BOURQUIN 86 and in n p and n A re- actions by ALEEV 93. Not seen by BOEHNLEIN 91. If due to strong decays, this state has exotic quantum numbers (B=0,Q=+1,S=- 1 for Λ p π + π + and I ≥ 3/2 for Λ p π - ). Needs confirmation. K (3100) MASS K (3100) MASS K (3100) MASS K (3100) MASS NODE=M129205 NODE=M129M VALUE (MeV) DOCUMENT ID ≈ 3100 OUR ESTIMATE ≈ 3100 OUR ESTIMATE ≈ 3100 OUR ESTIMATE ≈ 3100 OUR ESTIMATE → UNCHECKED ← 3-BODY DECAYS 3-BODY DECAYS 3-BODY DECAYS 3-BODY DECAYS NODE=M129M1 NODE=M129M1 VALUE (MeV) DOCUMENT ID TECN COMMENT 3054 ± 11 OUR AVERAGE 3054 ± 11 OUR AVERAGE 3054 ± 11 OUR AVERAGE 3054 ± 11 OUR AVERAGE 3060 ± 7 ± 20 1 ALEEV 93 BIS2 K (3100) → Λ p π + OCCUR=2 3056 ± 7 ± 20 1 ALEEV 93 BIS2 K (3100) → Λ p π - OCCUR=3 3055

402

I I  

Office of Legacy Management (LM)

Header Sheet Header Sheet .Doc ID # 7 e) AW-h a""- - 'IN r 1,9- / q 1-1- 31 0 )c // C) SC CCN: FUSRAP COMMUNICATIONS DISTRIBUTION FSRD= COMM. TYPELL-1-1 FORMER SITES RESTORATION DIVISION (EW-93) SAIC SENSITIVE DATE PROCESSED BY PDCC APR 0 3 1997 COMM REF ADMIN RCD SUBJECT .1 lrhnu rn t FROM To r P, COMM DATE ADDR CODE I I CLOSES CNN Wes I - RESPONSE TRACKING INFORMATION AC TION DESCRIPTION: 01: Ioi: OWEOTO- OWED BY: (ORG) I (ORG) TARGETDAT9.A IcLosiNr cco..coaoip. DATE CLOSING REF- 02: 1 02'. OWED M. OWED BY: (ORG) fORG). .TARGET-DATE CLOSING CCN..COMP. DATE CLOSING REF- MESSAGE: FSRD W/A W/0 SITES: W/A W/0 BNI W/A W/o ACTNG DIRECTOR: W S.., las nup 138 MIS PROGRAM MANAGER: k B.. WIA W/O W/A W/O 112 PNV 139 CIS DEPUTY PROGRAM MGR-: W. F.Vell D. AcK., R. Kii* IISSLD 140 His PROGRAM INT. MGk: G. D..,

403

c12.xls  

Gasoline and Diesel Fuel Update (EIA)

1,488 1,488 2,794 1,539 17,685 29,205 17,893 84.1 95.7 86.0 Building Floorspace (Square Feet) 1,001 to 5,000 ................................. 191 290 190 2,146 2,805 1,838 89.1 103.5 103.5 5,001 to 10,000 ............................... 131 231 154 1,972 2,917 1,696 66.2 79.2 91.0 10,001 to 25,000 ............................. 235 351 191 3,213 4,976 3,346 73.1 70.5 57.0 25,001 to 50,000 ............................. 172 328 173 2,449 4,128 2,091 70.4 79.4 82.5 50,001 to 100,000 ............................ 150 380 228 2,060 4,018 2,979 73.0 94.6 76.7 100,001 to 200,000 .......................... 214 438 281 2,124 3,947 2,993 100.7 111.1 94.0 200,001 to 500,000 .......................... 219 354 152 2,155 3,427 1,593 101.7 103.2 95.3 Over 500,000 ................................... 176 421 Q 1,566 2,986 1,357 112.1 141.2 Q Principal Building Activity

404

viv-pmg-2002-02.ppt  

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

February 15, 2002 February 15, 2002 February 15, 2001 Vivian O'Dell, US CMS User Facilities Status 2 Progress Since Last PMG Progress Since Last PMG Schedule Overview Current Status of Hardware R&D Quarterly Summary (Q1 FY02) Summary February 15, 2001 Vivian O'Dell, US CMS User Facilities Status 3 Major Milestones Major Milestones FY2002 FY2003 FY2004 FY2005 FY2006 FY2007 FY2008 1 2 3 4 1 2 3 4 1 2 3 4 1 2 3 4 1 2 3 4 1 2 3 4 1 2 3 4 1-2% Data Challenge 12/1/2001 User Analysis Cluster Commissioned 6/1/2002 FY02 Hardware Upgrade 8/1/2002 DAQ TDR 11/1/2002 Software Baseline: persistency choice 12/1/2002 5 % Data Challenge 1/1/2003 * Design of T1 5% prototype 6/1/2003 Implementation of 5 % prototype 3/1/2004 Software and Computing TDR 12/1/2003 1st Pilot Tier 2 center 1/1/2004 20 % Data Challenge 6/1/2004 Physics TDR 12/1/2004

405

Microsoft PowerPoint - UTSR-Biot, 2010-10-19-Shih.pptx  

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

UTSR Workshop on Heat Transfer UTSR Workshop on Heat Transfer Co-Organized by Penn State University and DoE NETL 19-21 October 2010 The Role of the Biot Number i T bi C li D i d A l i in Turbine-Cooling Design and Analysis Tom Shih, 1,2 Kyle Chi, 1 Prashanth Ramachandran, 1 Robin Ames, 3 and Rich Dennis 3 1 School of Aeronautics and Astronautics, Purdue University 2 Ames National Laboratory U S Dept of Energy Ames National Laboratory, U.S. Dept. of Energy 3 National Energy Technology Laboratory, U.S. Dept. of Energy DoE - NETL & Ames Laboratory What are the issues on Biot numbers? Biot number is a dimensionless parameter that cuts across equations. * gas phase: Re, Pr, Nu, Mach, ... gas phase: Re, Pr, Nu, Mach, ... * solid phase: Fourier number Biot number is easy to define only in 0-D and 1-D. c h L T T q 1 1     If local T

406

c21a.xls  

Gasoline and Diesel Fuel Update (EIA)

Square Square Feet All Buildings .................................... 201 412 431 13,124 31,858 25,200 15.3 12.9 17.1 Principal Building Activity Education .......................................... 9 55 45 806 5,378 3,687 11.1 10.2 12.2 Food Sales ....................................... 36 24 Q 747 467 Q 48.8 51.1 Q Food Service ..................................... 47 16 Q 986 664 Q 47.8 24.5 Q Health Care ....................................... 6 17 50 445 835 1,883 13.1 20.5 26.3 Inpatient .......................................... N Q 47 N Q 1,723 N Q 27.0 Outpatient ....................................... 6 11 Q 445 652 Q 13.1 17.4 Q Lodging ............................................. 4 31 34 260 2,274 2,563 14.0 13.5 13.5 Mercantile ......................................... 28 99 89 1,944 5,204 4,044 14.2 19.0 21.9 Retail (Other Than Mall) ..................

407

GC-62  

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

5/99 WED 13:10 FAX 202a862805 5/99 WED 13:10 FAX 202a862805 GC-62 , OAlKU*D o 0 0 -*, . ,.. ..,"',. The Cotactor agras ihabU ny producta mbodying any wuAi vv orproducd rhmreg the uer a ivfdy wm invenion wiH be namfenred mbs*amiy in the Uni~ud Satg unals thm Conrtor can A*hw to the aifi~tion ofDOE tb*a it is nt com rciafly f~Asibl to do so. la th* eve DOE ages to fixign arnrre e will be a rei en the the Goveramarns Apport of hrb tcnolgy be recognid in some appruopiate t n , g., recoup r aofte Oovraument's invien, etc. Thu Conacutor ftlirra arrsm to mnaktho Oabo *OnQ1 hi CwfM;imy on any Ussi gnra li an r any onky athmawime acquidng rilht to Wny gini g gjgm lwwinn in bsequaeTst **5. n mr Should the Conr=oatrm ar such atityifctinmg rigts in any vaa chne in onr p a chroUllDaginrus tti-tb waivUr, ulicenn or othr asfr of rigis i Wy

408

b12.xls  

U.S. Energy Information Administration (EIA) Indexed Site

64,783 64,783 9,874 1,255 1,654 1,905 1,258 5,096 4,317 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 409 409 544 N 165 99 638 5,001 to 10,000 ................................. 6,585 399 356 442 N 280 160 725 10,001 to 25,000 ............................... 11,535 931 Q 345 Q 312 631 1,284 25,001 to 50,000 ............................... 8,668 1,756 Q Q Q Q 803 578 50,001 to 100,000 ............................. 9,057 2,690 Q Q Q 206 841 Q 100,001 to 200,000 ........................... 9,064 2,167 Q N Q Q 930 524 200,001 to 500,000 ........................... 7,176 1,420 N Q 467 Q 1,185 Q Over 500,000 .................................... 5,908 Q N N 973 N Q Q Year Constructed Before 1920 ...................................... 3,769 410 Q 281 Q Q Q 220 1920 to 1945 .....................................

409

table10.8_02.xls  

U.S. Energy Information Administration (EIA) Indexed Site

8 Capability to Switch Distillate Fuel Oil to Alternative Energy Sources, 2002; 8 Capability to Switch Distillate Fuel Oil to Alternative Energy Sources, 2002; Level: National Data and Regional Totals; Row: NAICS Codes, Value of Shipments and Employment Sizes; Column: Energy Sources; Unit: Thousand Barrels. Coal Coke RSE NAICS Total Not Electricity Natural Residual and Row Code(a) Subsector and Industry Consumed(c) Switchable Switchable Receipts(d) Gas Fuel Oil Coal LPG Breeze Other(e) Factors Total United States RSE Column Factors: 1.7 1.6 1.7 0.9 1.5 0.6 0.7 1.7 0.3 0.8 311 Food 3,177 986 767 Q 297 Q 1 Q 0 Q 10.4 311221 Wet Corn Milling 14 4 10 * 3 0 1 2 0 * 0.8 31131 Sugar 169 W 143 W W 0 0 0 0 0 0.7 311421 Fruit and Vegetable Canning 242 Q 121 0 Q 0 0 0 0 * 27.1 312 Beverage and Tobacco Products

410

q009.dvi  

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

t t ' (4 th Generation) Quark, Searches for NODE=Q009 t ' -quark/hadron mass limits in p p and p p collisions t ' -quark/hadron mass limits in p p and p p collisions t ' -quark/hadron mass limits in p p and p p collisions t ' -quark/hadron mass limits in p p and p p collisions NODE=Q009TPP NODE=Q009TPP;CHECK LIMITS VALUE (GeV) CL% DOCUMENT ID TECN COMMENT >685 (CL = 95%) >685 (CL = 95%) >685 (CL = 95%) >685 (CL = 95%) [>256 GeV (CL = 95%) OUR 2011 BEST LIMIT] >656 >656 >656 >656 95 1 AAD 13F ATLS B(t ' → W b) = 1 >350 >350 >350 >350 95 2 AAD 12BC ATLS B(t ' → W q)=1 (q=d,s,b) >420 >420 >420 >420 95 3 AAD 12C ATLS t ' → X t (m X < 140 GeV) >685 >685 >685 >685 95 4 CHATRCHYAN 12BH CMS m b ' = m t ' >557 >557 >557 >557 95 5 CHATRCHYAN 12P CMS t ' t ' → W + b W - b → b ℓ + ν b ℓ - ν * * * We do not use the following data for averages, fits, limits, etc.

411

Million U.S. Housing Units Total U.S. Housing Units........................................  

U.S. Energy Information Administration (EIA) Indexed Site

Housing Units........................................ Housing Units........................................ 111.1 10.9 26.1 27.3 24.0 22.8 Do Not Have Heating Equipment........................... 1.2 Q Q N 0.3 0.8 Have Space Heating Equipment............................. 109.8 10.9 26.0 27.3 23.7 22.0 Use Space Heating Equipment.............................. 109.1 10.9 26.0 27.3 23.2 21.7 Have But Do Not Use Equipment.......................... 0.8 N N Q 0.5 Q Space Heating Usage During 2005 Heated Floorspace (Square Feet) None.................................................................. 3.6 Q 0.5 Q 1.4 1.4 1 to 499............................................................. 6.1 0.2 1.2 1.5 1.9 1.2 500 to 999.......................................................... 27.7 2.3 6.9 6.5 6.5 5.6 1,000 to 1,499....................................................

412

Total Space Heating Water Heating Cook-  

Gasoline and Diesel Fuel Update (EIA)

Buildings.............................. Buildings.............................. 1,644 1,429 131 Q 72 0.10 0.09 0.01 Q (*) Building Floorspace (Square Feet) 1,001 to 5,000 ........................... 249 228 Q (*) Q 0.41 0.38 Q (*) Q 5,001 to 10,000 .......................... 262 237 Q 1 Q 0.36 0.32 Q (*) Q 10,001 to 25,000 ........................ 201 179 11 (*) Q 0.19 0.17 0.01 (*) Q 25,001 to 50,000 ........................ 124 115 Q (*) 4 0.14 0.13 Q (*) (*) 50,001 to 100,000 ...................... 209 188 10 Q 7 0.11 0.10 0.01 Q (*) 100,001 to 200,000 .................... 270 250 Q Q 10 0.09 0.08 Q Q (*) 200,001 to 500,000 .................... 258 183 Q Q 11 0.08 0.05 0.02 Q (*) Over 500,000 ............................. 72 Q Q Q 15 0.02 Q Q Q (*) Principal Building Activity Education .................................. 342 322 11 Q Q 0.18 0.17 0.01 Q (*) Food Sales ................................

413

b20.xls  

U.S. Energy Information Administration (EIA) Indexed Site

64,783 64,783 45,144 10,960 1,958 1,951 2,609 2,161 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 5,613 916 Q Q N 223 5,001 to 10,000 ................................. 6,585 5,304 1,031 Q N Q Q 10,001 to 25,000 ............................... 11,535 9,098 1,732 383 Q Q Q 25,001 to 50,000 ............................... 8,668 5,807 1,837 355 Q Q Q 50,001 to 100,000 ............................. 9,057 6,218 1,739 273 337 Q Q 100,001 to 200,000 ........................... 9,064 6,102 1,545 539 Q Q Q 200,001 to 500,000 ........................... 7,176 4,246 1,361 Q 389 531 Q Over 500,000 .................................... 5,908 2,756 800 Q Q 1,522 Q Principal Building Activity Education .......................................... 9,874 8,714 946 Q N N N Food Sales .......................................

414

Summary of Prinicpal Building Activities in Commercial Buildings  

U.S. Energy Information Administration (EIA) Indexed Site

Sumary Comparison Table Sumary Comparison Table Return to: A Look at CBECS Building Activities SUMMARY COMPARISON TABLE Number of Buildings (thousand) Total Floorspace (million square feet) Average Square Feet per Building (thousand) Total Workers (thousand) Average Square Feet per Worker All Commercial Buildings 4,579 58,772 12.8 76,767 766 Building Activity Retail and Service 1,289 12,728 9.9 13,464 945 -- Retail 704 9,127 13.0 8,675 1,052 --- Strip Mall 130 2,887 22.3 3,529 818 --- Enclosed Mall 12 1,817 Q 1,814 1,001 --- Other Retail 562 4,423 7.9 3,332 1,328 --Service 585 3,601 6.2 4,788 752 Office 705 10,478 14.9 27,053 387 Warehouse 580 8,481 14.6 4,904 1,730 Public Assembly 326 3,948 12.1 2,997 1,317 Education 309 7,740 25.1 10,096 767

415

A<ACD6B;GAQ=CD4Q  

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

AQ(%,1-Q .WAFTWbe?#Q 9TT@Xe (3* e.AO AW:K e&T[ O"Q- W:OY d  ]L *aA <[YI ^Ae) IWA= YTWe 0T: Oe 4WTF W:M Xe3C >Ae %RS[:Ke2:YITO:Ke+O_IWTONAOY:Ke5TKH=ce %

416

 

Gasoline and Diesel Fuel Update (EIA)

7. Electricity Consumption and Conditional Energy Intensity by Census Division for Non-Mall Buildings, 2003: Part 1 7. Electricity Consumption and Conditional Energy Intensity by Census Division for Non-Mall Buildings, 2003: Part 1 Total Electricity Consumption (billion kWh) Total Floorspace of Buildings Using Electricity (million square feet) Electricity Energy Intensity (kWh/square foot) New England Middle Atlantic East North Central New England Middle Atlantic East North Central New England Middle Atlantic East North Central All Buildings* ............................... 32 116 153 2,942 9,867 11,373 10.8 11.7 13.5 Building Floorspace (Square Feet) 1,001 to 5,000 ................................ 4 9 20 345 652 908 12.7 13.8 22.0 5,001 to 10,000 .............................. 3 7 8 350 732 781 7.7 9.6 10.7 10,001 to 25,000 ............................ Q 16 20 Q 1,390 1,934 Q 11.2 10.5

417

Energy confinement and magnetic field generation in the SSPX spheromaka)  

Science Journals Connector (OSTI)

The Sustained Spheromak Physics Experiment (SSPX) [Hooper et al. Nuclear Fusion39 863 (1999)] explores the physics of efficient magnetic field buildup and energy confinement both essential parts of advancing the spheromak concept. Extending the spheromak formation phase increases the efficiency of magnetic field generation with the maximum edge magnetic field for a given injector current ( B ? I ) from 0.65 T ? MA previously to 0.9 T ? MA . We have achieved the highest electron temperatures ( T e ) recorded for a spheromak with T e > 500 eV toroidalmagnetic field ? 1 T and toroidal current ( ? 1 MA ) [Wood et al. Improved magnetic field generation efficiency and higher temperaturespheromakplasmas Phys. Rev. Lett. (submitted)]. Extending the sustainment phase to > 8 ms extends the period of low magnetic fluctuations ( input power and dominantly collisional majority ion heating. The evolution of electron temperature shows a distinct and robust feature of spheromak formation: A hollow-to-peaked T e ( r ) associated with q ? 1 ? 2 .

B. Hudson; R. D. Wood; H. S. McLean; E. B. Hooper; D. N. Hill; J. Jayakumar; J. Moller; D. Montez; C. A. Romero-Talams; T. A. Casper; J. A. Johnson III; L. L. LoDestro; E. Mezonlin; L. D. Pearlstein

2008-01-01T23:59:59.000Z

418

Diagonal Ising susceptibility: elliptic integrals, modular forms and CalabiYau equations  

Science Journals Connector (OSTI)

We give the exact expressions of the partial susceptibilities ?(3)d and ?(4)d for the diagonal susceptibility of the Ising model in terms of modular forms and CalabiYau ODEs, and more specifically, 3F2([1/3, 2/3, 3/2],?[1, 1];?z) and 4F3([1/2, 1/2, 1/2, 1/2],?[1, 1, 1];?z) hypergeometric functions. By solving the connection problems we analytically compute the behavior at all finite singular points for ?(3)d and ?(4)d. We also give new results for ?(5)d. We see, in particular, the emergence of a remarkable order-6 operator, which is such that its symmetric square has a rational solution. These new exact results indicate that the linear differential operators occurring in the n-fold integrals of the Ising model are not only 'derived from geometry' (globally nilpotent), but actually correspond to 'special geometry' (homomorphic to their formal adjoint). This raises the question of seeing if these 'special geometry' Ising operators are 'special' ones, reducing, in fact systematically, to (selected, k-balanced, ...) q + 1Fq hypergeometric functions, or correspond to the more general solutions of CalabiYau equations.

M Assis; S Boukraa; S Hassani; M van Hoeij; J-M Maillard; B M McCoy

2012-01-01T23:59:59.000Z

419

A detached double degenerate with a 1.4 hr orbital period  

E-Print Network [OSTI]

We have discovered that the detached double degenerate binary WD 0957-666 has an orbital period of 1.46 hours, rather than the 1.15 day orbital period reported earlier. This is the shortest period example of such a system yet discovered. We obtain a unique period, which fits both our and earlier data. At this period the emission of gravitational radiation will cause the binary to merge within approximately 2.0 x 10*8 years. This system represents a population of short orbital period binaries which will merge within a Hubble time, and so could account for type Ia supernovae, although due to the low mass of both stars (0.3 to 0.4 solar masses), it is unlikely to become a supernova itself. We have detected the companion star and have measured a mass ratio of q = 1.15. This is the third double degenerate for which q has been measured and all three have q close to 1, which is in conflict with the predicted mass ratio distribution which peaks at 0.7. This system is viewed close to edge on, and we estimate that the probability of this system undergoing eclipses is 15 %.

C. Moran; T. R. Marsh; A. Bragaglia

1997-04-24T23:59:59.000Z

420

Theoretical study of line and boundary tension in adsorbed colloid-polymer mixtures  

E-Print Network [OSTI]

An extended theoretical study of interface potentials in adsorbed colloid-polymer mixtures is performed. To describe the colloid-polymer mixture near a hard wall, a simple Cahn-Nakanishi-Fisher free-energy functional is used. The bulk phase behavior and the substrate-adsorbate interaction are modelled by the free-volume theory for ideal polymers with polymer-to-colloid size ratios q=0.6 and q=1. The interface potentials are constructed with help from a Fisher-Jin crossing constraint. By manipulating the crossing density, a complete interface potential can be obtained from natural, single-crossing, profiles. The line tension in the partial wetting regime and the boundary tension along prewetting are computed from the interface potentials. The line tensions are of either sign, and descending with increasing contact angle. The line tension takes a positive value of 10^-14 - 10^-12 N near a first-order wetting transition, passes through zero and decreases to minus 10^-14 - 10^-12 N away from the first-order transition. The calculations of the boundary tension along prewetting yield values increasing from zero at the prewetting critical point up to the value of the line tension at first-order wetting.

Jesper Koning; Yves Vandecan; Joseph Indekeu

2014-04-25T23:59:59.000Z

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421

Short- and medium-range order in Zr[subscript 80]Pt[subscript 20] liquids  

SciTech Connect (OSTI)

The atomic structures in equilibrium and supercooled liquids of Zr{sub 80}Pt{sub 20} were determined as a function of temperature by in situ high-energy synchrotron diffraction studies of the levitated liquids (containerless processing) using the beamline electrostatic levitation (BESL) technique. The presence of a pronounced pre-peak at q - 1.7 {angstrom}{sup -1} in the static structure factor indicates medium-range order (MRO) in the liquid. The position and intensity of the pre-peak remain constant with cooling, indicating that the MRO is already present in the liquid above its melting temperature. An analysis of the liquid atomic structures obtained using the Reverse Monte Carlo method utilizing both the structure factor S(q) from x-ray diffraction experiments and the partial pair-correlation functions from ab initio molecular dynamics simulations show that the pre-peak arises from a Pt-Pt correlation that can be identified with icosahedral short-range order around the Pt atoms. The local atomic ordering is dominated by icosahedral-like structures, raising the nucleation barrier between the liquid and these phases, thus assisting glass formation.

Mauro, N.A.; Wessels, V.; Bendert, J.C.; Klein, S.; Gangopadhyay, A.K.; Kramer, M.J.; Hao, S.G.; Rustan, G.E.; Kreyssig, A.; Goldman, A.I.; Kelton, K.F. (WU); (ETH Zurich); (Iowa State); (IMW-Germany)

2011-12-09T23:59:59.000Z

422

PERIOD ERROR ESTIMATION FOR THE KEPLER ECLIPSING BINARY CATALOG  

SciTech Connect (OSTI)

The Kepler Eclipsing Binary Catalog (KEBC) describes 2165 eclipsing binaries identified in the 115 deg{sup 2} Kepler Field based on observations from Kepler quarters Q0, Q1, and Q2. The periods in the KEBC are given in units of days out to six decimal places but no period errors are provided. We present the PEC (Period Error Calculator) algorithm, which can be used to estimate the period errors of strictly periodic variables observed by the Kepler Mission. The PEC algorithm is based on propagation of error theory and assumes that observation of every light curve peak/minimum in a long time-series observation can be unambiguously identified. The PEC algorithm can be efficiently programmed using just a few lines of C computer language code. The PEC algorithm was used to develop a simple model that provides period error estimates for eclipsing binaries in the KEBC with periods less than 62.5 days: log {sigma}{sub P} Almost-Equal-To - 5.8908 + 1.4425(1 + log P), where P is the period of an eclipsing binary in the KEBC in units of days. KEBC systems with periods {>=}62.5 days have KEBC period errors of {approx}0.0144 days. Periods and period errors of seven eclipsing binary systems in the KEBC were measured using the NASA Exoplanet Archive Periodogram Service and compared to period errors estimated using the PEC algorithm.

Mighell, Kenneth J. [National Optical Astronomy Observatory, 950 North Cherry Avenue, Tucson, AZ 85719 (United States); Plavchan, Peter [NASA Exoplanet Science Institute, California Institute of Technology, Pasadena, CA 91125 (United States)

2013-06-15T23:59:59.000Z

423

Effective field theory and integrability in two-dimensional Mott transition  

SciTech Connect (OSTI)

Highlights: > Mott transition in 2d lattice fermion model. > 3D integrability out of 2D. > Effective field theory for Mott transition in 2d. > Double Chern-Simons. > d-Density waves. - Abstract: We study the Mott transition in a two-dimensional lattice spinless fermion model with nearest neighbors density-density interactions. By means of a two-dimensional Jordan-Wigner transformation, the model is mapped onto the lattice XXZ spin model, which is shown to possess a quantum group symmetry as a consequence of a recently found solution of the Zamolodchikov tetrahedron equation. A projection (from three to two space-time dimensions) property of the solution is used to identify the symmetry of the model at the Mott critical point as U{sub q}(sl(2)-circumflex)xU{sub q}(sl(2)-circumflex), with deformation parameter q = -1. Based on this result, the low-energy effective field theory for the model is obtained and shown to be a lattice double Chern-Simons theory with coupling constant k = 1 (with the standard normalization). By further employing the effective filed theory methods, we show that the Mott transition that arises is of topological nature, with vortices in an antiferromagnetic array and matter currents characterized by a d-density wave order parameter. We also analyze the behavior of the system upon weak coupling, and conclude that it undergoes a quantum gas-liquid transition which belongs to the Ising universality class.

Bottesi, Federico L. [Facultad de Ingenieria Pontificia Universidad Catolica Argentina, Av. Alicia Moreau de Justo 1500, 1428 Buenos Aires (Argentina); Physics Department, Comision Nacional de Energia Atomica, Av. Libertador 8250, 1429 Buenos Aires (Argentina); Zemba, Guillermo R., E-mail: zemba@tander.cnea.gov.ar [Facultad de Ingenieria Pontificia Universidad Catolica Argentina, Av. Alicia Moreau de Justo 1500, 1428 Buenos Aires (Argentina); Physics Department, Comision Nacional de Energia Atomica, Av. Libertador 8250, 1429 Buenos Aires (Argentina)

2011-08-15T23:59:59.000Z

424

A disease of swine caused by a chromobacterium species  

E-Print Network [OSTI]

\\j O O lAvO ?A O -tU M A lX S 'v O r -O 'H rC f\\ y5Pml6gQPa66I4jDI?Q?4s6w?QIw?I6I664jDw6I?Iw??I46 CM OJCMCMOJCVOJCVJOJOJOJCMOJCMCNJCVCNJCVCVCMCNJCM Oi O H C*-I?I wQS 0,2 5 M ? ? <,' ? S w u ?4 u Q , P6 Q ,'w 4g 68 0.2 5...library l i b rayy?hyI a? OQItj'Q'1u'4,

Sippel, William Lawrence

2013-10-04T23:59:59.000Z

425

Termination of Safeguards for Accountable Nuclear Materials at the Idaho National Laboratory  

SciTech Connect (OSTI)

Termination of safeguards ends requirements of Nuclear Material Control and Accountability (MC&A) and thereby removes the safeguards basis for applying physical protection requirements for theft and diversion of nuclear material, providing termination requirements are met as described. Department of Energy (DOE) M 470.4 6 (Nuclear Material Control and Accountability [8/26/05]) stipulates: 1. Section A, Chapter I (1)( q) (1): Safeguards can be terminated on nuclear materials provided the following conditions are met: (a) 'If the material is special nuclear material (SNM) or protected as SNM, it must be attractiveness level E and have a measured value.' (b) 'The material has been determined by DOE line management to be of no programmatic value to DOE.' (c) 'The material is transferred to the control of a waste management organization where the material is accounted for and protected in accordance with waste management regulations. The material must not be collocated with other accountable nuclear materials.' Requirements for safeguards termination depend on the safeguards attractiveness levels of the material. For attractiveness level E, approval has been granted from the DOE Idaho Operations Office (DOE ID) to Battelle Energy Alliance, LLC (BEA) Safeguards and Security (S&S). In some cases, it may be necessary to dispose of nuclear materials of attractiveness level D or higher. Termination of safeguards for such materials must be approved by the Departmental Element (this is the DOE Headquarters Office of Nuclear Energy) after consultation with the Office of Security.

Michael Holzemer; Alan Carvo

2012-04-01T23:59:59.000Z

426

Anisotropic inplane spin correlation in the parent and Co-doped BaFe2As2: A neutron scattering study  

Science Journals Connector (OSTI)

Abstract Antiferromagnetic spin fluctuations were investigated in the normal states of the parent (x=0), under-doped (x=0.04) and optimally-doped (x=0.06) Ba ( Fe 1 - x Co x ) 2 As 2 single crystals using inelastic neutron scattering technique. For all the doping levels, quasi-two-dimensional antiferromagnetic fluctuations were observed as a broad peak localized at Q = ( 1 / 2 , 1 / 2 , l ) . At lower energies, the peak shows an apparent anisotropy in the h k 0 plane; longitudinal peak widths are considerably smaller than transverse widths. The anisotropy is larger for the higher doping level. These results are consistent with the random phase approximation (RPA) calculations taking account of the orbital character of the electronic bands, confirming that the anisotropic nature of the spin fluctuations in the normal states is mostly dominated by the nesting of Fermi surfaces. On the other hand, the quasi-two-dimensional spin correlations grow much rapidly for decreasing temperature in the x=0 parent compound, compared to that expected for nearly antiferromagnetic metals. This may be another sign of the unconventional nature of the antiferromagnetic transition in BaFe2As2.

S. Ibuka; Y. Nambu; T. Yamazaki; M.D. Lumsden; T.J. Sato

2014-01-01T23:59:59.000Z

427

Neutrinoless Double Beta Decay with R-parity Violation  

E-Print Network [OSTI]

We consider recently observed neutrinoless double beta decay in the context of the minimal supersymmetric standard model with R-parity violating couplings lambda^{'}. We observe that most of the current experimental bounds on the R-parity violating couplings do not exclude the possibility that the neutrinoless double beta decay is caused by R-parity violation. But if we consider K-bar{K} oscillation, we observe that we have to make the R-parity violating couplings generation-dependent to accomodate with the observed neutrinoless double beta decay. And furthermore, we need some mechanism to cancel the contribution to K-bar{K} mixing from a large R-parity violating coupling. We realized this cancellation by assuming that the first- and the second- generation of quark sector do not couple with the first-generation lepton sector by R-parity violating couplings except the term W=lambda_{111}^{'} L_{1} Q_{1} D_{1}^{c}, which is responsible for the observed neutrinoless double beta decay.

Yosuke Uehara

2002-06-26T23:59:59.000Z

428

Transition from decelerated to accelerated cosmic expansion in braneworld universes  

E-Print Network [OSTI]

Braneworld theory provides a natural setting to treat, at a classical level, the cosmological effects of vacuum energy. Non-static extra dimensions can generally lead to a variable vacuum energy, which in turn may explain the present accelerated cosmic expansion. We concentrate our attention in models where the vacuum energy decreases as an inverse power law of the scale factor. These models agree with the observed accelerating universe, while fitting simultaneously the observational data for the density and deceleration parameter. The redshift at which the vacuum energy can start to dominate depends on the mass density of ordinary matter. For Omega = 0.3, the transition from decelerated to accelerated cosmic expansion occurs at z approx 0.48 +/- 0.20, which is compatible with SNe data. We set a lower bound on the deceleration parameter today, namely q > - 1 + 3 Omega/2, i.e., q > - 0.55 for Omega = 0.3. The future evolution of the universe crucially depends on the time when vacuum starts to dominate over ord...

De Leon, J P

2004-01-01T23:59:59.000Z

429

Neutron scattering and magnetic studies of ferrihydrite nanoparticles  

Science Journals Connector (OSTI)

Magnetic properties of two-line ferrihydrite (FeOOD?nD2O) nanoparticles with an average size ?4 nm are investigated using neutron scattering and magnetometry. Comparison of the neutron scattering and x-ray diffraction patterns identifies the (002) peak at Q=1.3 -1 as predominantly magnetic. The intensity of this peak, measured from 10 to 450 K, decreases almost linearly with temperature until 350 K, becoming temperature independent above 350 K. From this, TN?350 K is identified to be the ordering temperature of the core spins of the nanoparticles. The width of the line is temperature independent, yielding a magnetic coherence length?particle size. The temperature variations (5300 K) of the initial susceptibility ? for the field-cooled (FC) and zero-field-cooled (ZFC) cases yield a peak at Tp(m)?65 K, below which ?(FC)>?(ZFC). For T>Tp(m), the variation of ?-1 vs T is analyzed in terms of the model of El-Hilo et al., involving particle-size distribution and interparticle interactions, and substantial interparticle interactions are inferred. Following the observations in ferritin, the field dependence of the magnetization M for T>Tp(m) is analyzed in terms of the modified Langevin variation: M=MoL(?pH/kT)+?aH, where ?p is the magnetic moment/particle. The fit at 100 K yields ?p?250 ?B, consistent with the theoretical estimates based on uncompensated surface spins of Fe3+.

M. S. Seehra; V. S. Babu; A. Manivannan; J. W. Lynn

2000-02-01T23:59:59.000Z

430

Search milli-charged particles at SLAC  

SciTech Connect (OSTI)

Particles with electric charge q {triple_bond} Qe {le} 10{sup -3} e and masses in the range 1-1000 MeV/c{sup 2} are not excluded by present experiments or by astrophysical or cosmological arguments. A beam dump experiment uniquely suited to the detection of such {open_quotes}milli-charged{close_quotes} particles has been carried out at SLAC, utilizing the short-duration pulses of the SLC electron beam to establish a tight coincidence window for the signal. The detector, a large scintillation counter sensitive to very small energy depositions, provided much greater sensitivity than previous searches. Analysis of the data leads to the exclusion of a substantial portion of the charge-mass plane. In this report, a preliminary mass-dependent upper limit is presented for the charge of milli-charged particles, ranging from Q = 1.7 x 10{sup -5} at milli-charged particle mass 0.1 MeV/c{sup 2} to Q = 9.5 x 10{sup -4} at 100 MeV/c{sup 2}.

Langeveld, W.G.J. [Stanford Univ., CA (United States)

1997-01-01T23:59:59.000Z

431

Modeling Merging Galaxies using MINGA - Improving Restricted N-body by Dynamical Friction  

E-Print Network [OSTI]

Modeling interacting galaxies to reproduce observed systems is still a challenge due to the extended parameter space (among other problems). Orbit and basic galaxy parameters can be tackled by fast simulation techniques like the restricted N-body method, applied in the fundamental work by Toomre & Toomre (1972). This approach allows today for the study of millions of models in a short time. One difficulty for the classical restricted N-body method is the missing orbital decay, not allowing for galaxy mergers. Here we present an extension of the restricted N-body method including dynamical friction. This treatment has been developed by a quantitative comparison with a set of self-consistent merger simulations. By varying the dynamical friction (formalism, strength and direction), we selected the best-fitting parameters for a set of more than 250000 simulations. We show that our treatment reliably reproduces the orbital decay and tidal features of merging disk galaxies for mass ratios up to q=1/3 between host and satellite. We implemented this technique into our genetic algorithm based modeling code MINGA and present first results.

Hanns P. Petsch; Christian Theis

2008-10-03T23:59:59.000Z

432

Micro Computers: An Industrial Energy Conservation Tool  

E-Print Network [OSTI]

8" 8" of dr,. rue' MOISTURE ".00 ETHANE C2 H. ".97 3 ...m HYDROGEN 2 ..... m0 ... 08 "ETHANE CH' 99.43 ~O\\. 40 7:1.64 1.25 PROPANE C3 H8 l.~o\\ 0.~0 CARBON OXYGEN 0.00 li!!I.QUil' N-BUTANE H,a 1.7Gl1 0.~11I C' CARBON DI-OXIDE ca2 L~4 0....00 1iII.01l1 SULFUR 0.1lI0 0.01 CARBON DIOXIDE , .54 SuLFUR DIOXIDE iii. 00 NITROGEN N2 Q'l.82 0.:5Q1 NITROGEN IlI.B'2 l1I.0'lA:H COMeUST[ON CONSTANT K- 89.8:3 HHV- 2:3.14" LHV-20.Q70 eTu/Le H20 1n CO""bustlO,", pRODUCTS? 2.1~ LB/La ,"uel cp...

Harriz, J. T.

1984-01-01T23:59:59.000Z

433

The Super HMS  

SciTech Connect (OSTI)

As a part of physics instrumentation development for TJNAF long range institution upgrade plan, a 12 GeV/c Super High Momentum Spectrometer (the Super HMS) has been proposed for high luminosity and high q2 physics in endstation Hall C. The fundamental configuration of Super HMS is QQDD. Two identical quadrupoles are the superconducting HMS Q1s with maximum gradient 8 Tesla/m. Two identical SLAC B202/B203 dipole magnets are considered for the use of dispersive elements with accumulative bending power 18.7 degree at 12 GeV/c while the central field is set to 2.05 Tesla. A sliding mechanism could guide the whole system, including the magnetic elements and detector house, moving forwards and backwards by +/- 100 cm. Under an assumed magnetic structure, the Super HMS optics performance has been studied by using TRANSPORT, TURTLE, and RAYTRACE codes and related reconstruction methods. The applicable solid angle can be adjusted between 1 msr and 2.3 msr. The maximum central momentum is 12 GeV/c. The reconstructed momentum resolution within full momentum range 20% is better than 10-3. The in-plane angle reconstruction accuracy is about 0.5 mr, mainly determined by the local multiple scattering from detector materials. This report also points out the strategy of super HMS optics adapting low rigidity quadrupoles for the use of high momentum operation, and the potential capability of very forward angle operations.

Chen Yan

1998-06-01T23:59:59.000Z

434

HIGH-INCLINATION ATENS ARE INDEED RARE  

SciTech Connect (OSTI)

A recent publication by the Near-Earth Object (NEOWISE) team (Mainzer et al.) using data from the Wide-field Infrared Survey Explorer compared the spacecraft's detected near-Earth asteroid subpopulation orbital element distributions to those expected from the Bottke et al. NEO orbital model. They found a discrepency between the detected and expected Aten inclination distribution. We show that the more recent NEO orbital distribution model by Greenstreet et al., when biased using the NEOWISE detection biases, gives a better match to the NEOWISE detections for the Aten (a < 1.0 AU, Q > 0.983 AU) population in semimajor axis (a), eccentricity (e), and inclination (i) than the Bottke et al. model. A Kolmogorov-Smirnov test gives the probability of drawing the NEOWISE detections from the biased Bottke et al. model as not rejectable (at >99% confidence) for the Aten semimajor axis distribution, but is rejectable at such a high level of confidence for the Aten eccentricity and inclination distributions. For all three orbital element distributions, the biased Greenstreet et al. model provides an acceptable match to the NEOWISE Aten detections. The deficiency in the previous model is likely due to the numerical integration's accuracy having broken down in the high-speed regime for planetary encounters near the Sun, an effect which the newer model does not suffer, and thus likely is the model of preference for perihelia q < 1.0 AU.

Greenstreet, S.; Gladman, B., E-mail: sarahg@phas.ubc.ca [Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, British Columbia V6T 1Z1 (Canada)

2013-04-10T23:59:59.000Z

435

Million U.S. Housing Units Total....................................................................................  

U.S. Energy Information Administration (EIA) Indexed Site

78.1 78.1 64.1 4.2 1.8 2.3 5.7 Cooking Appliances Frequency of Hot Meals Cooked 3 or More Times A Day................................................. 8.2 4.7 3.8 Q Q Q 0.6 2 Times A Day.............................................................. 24.6 16.0 13.3 0.8 0.4 Q 1.3 Once a Day.................................................................. 42.3 32.1 26.5 1.6 0.7 1.1 2.2 A Few Times Each Week............................................. 27.2 19.3 15.8 1.3 0.4 0.6 1.3 About Once a Week..................................................... 3.9 2.8 2.2 Q N Q 0.3 Less Than Once a Week.............................................. 4.1 2.7 2.3 Q Q Q Q No Hot Meals Cooked.................................................. 0.9 0.4 Q Q Q Q N Conventional Oven Use an Oven................................................................

436

tablehc3.3.xls  

U.S. Energy Information Administration (EIA) Indexed Site

8.1 8.1 64.1 4.2 1.8 2.3 5.7 Household Size 1 Person......................................................... 30.0 18.6 13.2 1.4 0.7 1.3 2.1 2 Persons........................................................ 34.8 26.8 22.9 1.3 0.5 0.7 1.4 3 Persons........................................................ 18.4 12.8 10.7 0.5 0.4 Q 1.0 4 Persons........................................................ 15.9 11.5 9.8 0.6 Q Q 0.9 5 Persons........................................................ 7.9 5.9 5.3 0.2 Q Q 0.3 6 or More Persons........................................... 4.1 2.4 2.1 Q Q N Q 2005 Annual Household Income Category Less than $9,999............................................. 9.9 4.7 3.1 0.3 0.3 Q 0.8 $10,000 to $14,999......................................... 8.5 3.9 2.7 Q Q Q 0.8 $15,000 to $19,999.........................................

437

Total U.S. Housing Units............................................  

U.S. Energy Information Administration (EIA) Indexed Site

.. .. 111.1 7.1 7.0 8.0 12.1 Do Not Have Heating Equipment............................... 1.2 Q Q Q 0.2 Have Space Heating Equipment................................ 109.8 7.1 6.8 7.9 11.9 Use Space Heating Equipment................................. 109.1 7.1 6.6 7.9 11.4 Have But Do Not Use Equipment.............................. 0.8 N Q N 0.5 Space Heating Usage During 2005 Heated Floorspace (Square Feet) None...................................................................... 3.6 Q 0.7 Q 1.3 1 to 499................................................................. 6.1 0.5 0.4 0.5 1.4 500 to 999............................................................. 27.7 2.7 1.4 2.4 3.4 1,000 to 1,499....................................................... 26.0 1.4 2.2 1.6 2.5 1,500 to 1,999.......................................................

438

Million U.S. Housing Units Total....................................................................................  

U.S. Energy Information Administration (EIA) Indexed Site

33.0 33.0 8.0 3.4 5.9 14.4 1.2 Cooking Appliances Frequency of Hot Meals Cooked 3 or More Times A Day................................................. 8.2 3.4 1.0 0.4 0.6 1.2 Q 2 Times A Day.............................................................. 24.6 8.6 2.3 1.0 1.6 3.5 0.2 Once a Day.................................................................. 42.3 10.1 2.3 1.1 2.1 4.3 0.4 A Few Times Each Week............................................. 27.2 7.8 2.0 0.7 1.3 3.6 Q About Once a Week..................................................... 3.9 1.1 Q Q Q 0.6 Q Less Than Once a Week.............................................. 4.1 1.4 Q Q Q 1.0 N No Hot Meals Cooked.................................................. 0.9 0.4 Q N Q 0.3 Q Conventional Oven Use an Oven................................................................

439

Table HC2.9 Home Appliances Characteristics by Type of Housing Unit, 2005  

U.S. Energy Information Administration (EIA) Indexed Site

Million U.S. Housing Units Total U.S............................................................ 111.1 72.1 7.6 7.8 16.7 6.9 Cooking Appliances Conventional Ovens Use an Oven............................................... 109.6 71.3 7.4 7.7 16.4 6.8 1.............................................................. 103.3 66.2 7.2 7.4 15.9 6.7 2 or More................................................. 6.2 5.1 Q 0.3 0.5 Q Do Not Use an Oven................................... 1.5 0.7 Q Q 0.4 Q Most-Used Oven Fuel Electric..................................................... 67.9 45.5 4.4 3.7 10.7 3.7 Natural Gas.............................................. 36.4 22.0 3.0 3.9 5.6 1.8 Propane/LPG........................................... 5.2 3.8 Q Q Q 1.3 Self-Cleaning Oven Use a Self-Cleaning Oven........................

440

b9.xls  

U.S. Energy Information Administration (EIA) Indexed Site

64,783 64,783 3,769 6,871 7,045 8,101 10,772 10,332 12,360 5,533 Building Floorspace (Square Feet) 1,001 to 5,000 ................................... 6,789 490 796 860 690 966 1,149 1,324 515 5,001 to 10,000 ................................. 6,585 502 827 643 865 1,332 721 1,209 486 10,001 to 25,000 ............................... 11,535 804 988 1,421 1,460 1,869 1,647 2,388 958 25,001 to 50,000 ............................... 8,668 677 838 935 1,234 1,720 1,174 1,352 739 50,001 to 100,000 ............................. 9,057 491 641 927 1,483 1,146 1,390 2,058 921 100,001 to 200,000 ........................... 9,064 Q 704 1,148 1,039 1,411 1,496 1,934 1,060 200,001 to 500,000 ........................... 7,176 Q 1,288 569 947 1,243 1,237 984 609 Over 500,000 .................................... 5,908 Q 790 541 382 1,085 1,518 1,111 Q Principal Building Activity

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While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


441

 

Gasoline and Diesel Fuel Update (EIA)

A. Fuel Oil Consumption (gallons) and Energy Intensities by End Use for All Buildings, 2003 A. Fuel Oil Consumption (gallons) and Energy Intensities by End Use for All Buildings, 2003 Total Fuel Oil Consumption (million gallons) Fuel Oil Energy Intensity (gallons/square foot) Total Space Heating Water Heating Cook- ing Other Total Space Heating Water Heating Cook- ing Other All Buildings.......................... 1,644 1,429 131 Q 72 0.10 0.09 0.01 Q (*) Building Floorspace (Square Feet) 1,001 to 5,000 ......................... 249 228 Q (*) Q 0.41 0.38 Q (*) Q 5,001 to 10,000 ....................... 262 237 Q 1 Q 0.36 0.32 Q (*) Q 10,001 to 25,000 ..................... 201 179 11 (*) Q 0.19 0.17 0.01 (*) Q 25,001 to 50,000 ..................... 124 115 Q (*) 4 0.14 0.13 Q (*) (*) 50,001 to 100,000 ................... 209 188 10 Q 7 0.11 0.10 0.01 Q (*)

442

q008.dvi  

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

' ' (4 th Generation) Quark, Searches for b ' -quark/hadron mass limits in p p and p p collisions b ' -quark/hadron mass limits in p p and p p collisions b ' -quark/hadron mass limits in p p and p p collisions b ' -quark/hadron mass limits in p p and p p collisions VALUE (GeV) CL% DOCUMENT ID TECN COMMENT >480 >480 >480 >480 95 1 AAD 12AT ATLS B(b ' → W t) = 1 >400 >400 >400 >400 95 2 AAD 12AU ATLS B(b ' → Z b) = 1 >350 >350 >350 >350 95 3 AAD 12BC ATLS B(b ' → W q) = 1 (q=u,c) >685 >685 >685 >685 95 4 CHATRCHYAN 12BH CMS m t ' = m b ' >611 >611 >611 >611 95 5 CHATRCHYAN 12X CMS B(b ' → W t) = 1 >190 >190 >190 >190 95 6 ABAZOV 08X D0 cτ = 200mm >190 >190 >190 >190 95 7 ACOSTA 03 CDF quasi-stable b ' * * * We do not use the following data for averages, fits, limits, etc. * * * >450 95 8 AAD 12BE ATLS B(b ' → W t) = 1 >372 95 9 AALTONEN 11J CDF b

443

q009.dvi  

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

' ' (4 th Generation) Quark, Searches for t ' -quark/hadron mass limits in p p and p p collisions t ' -quark/hadron mass limits in p p and p p collisions t ' -quark/hadron mass limits in p p and p p collisions t ' -quark/hadron mass limits in p p and p p collisions VALUE (GeV) CL% DOCUMENT ID TECN COMMENT >656 >656 >656 >656 95 1 AAD 13F ATLS B(t ' → W b) = 1 >350 >350 >350 >350 95 2 AAD 12BC ATLS B(t ' → W q)=1 (q=d,s,b) >420 >420 >420 >420 95 3 AAD 12C ATLS t ' → X t (m X < 140 GeV) >685 >685 >685 >685 95 4 CHATRCHYAN 12BH CMS m b ' = m t ' >557 >557 >557 >557 95 5 CHATRCHYAN 12P CMS t ' t ' → W + b W - b → b ℓ + ν b ℓ - ν * * * We do not use the following data for averages, fits, limits, etc. * * * >404 95 6 AAD 12AR ATLS B(t ' → W b) = 1 >570 95 7 CHATRCHYAN 12BC CMS t ' t ' → W + b W - b >400 95 8 AALTONEN 11AH CDF t ' → X t (m X < 70 GeV) >358 95 9 AALTONEN 11AL

444

" Million Housing Units, Final"  

U.S. Energy Information Administration (EIA) Indexed Site

Televisions in U.S. Homes, by Housing Unit Type, 2009" Televisions in U.S. Homes, by Housing Unit Type, 2009" " Million Housing Units, Final" ,,"Housing Unit Type" ,,"Single-Family Units",,"Apartments in Buildings With" ,"Total U.S.1 (millions)" ,," Detached"," Attached"," 2 to 4 Units","5 or More Units","Mobile Homes" "Televisions" "Total Homes",113.6,71.8,6.7,9,19.1,6.9 "Televisions" "Number of Televisions" 0,1.5,0.5,0.1,0.2,0.6,"Q" 1,24.2,11,1.2,3,7.3,1.7 2,37.5,21.4,2.4,3.3,7.7,2.7 3,26.6,18.4,2,1.8,2.8,1.6 4,14.2,11.6,0.7,0.6,0.5,0.7 "5 or More",9.7,8.8,0.4,0.2,"Q",0.2 "Most-Used Television" "Display Size"

445

Effect of storage temperature on the quality of vacuum packed pecans  

E-Print Network [OSTI]

O f F I O I IV 5 g X I &0 Ca (p O (p O CD I I fV Ql O O V I f O 0 Df O O Ol O I O O I I PJ (V O O V O I I (p O O 0 8 IV Ql F O O O O 0 (D 0' 0 O V (D GI (D 0 (D 0 (D GD G 0 DD I-' n- '? ID... 03 I I I Car V I V I I V 0 0 0 V V V ID ID 0 0 0 0 0 0 0 ~ 0' 0 0 0 V. ID V 0 ~o 0 V f0 fV L0 ~ ~ ~ P C 0 lTl &oo 0 V ct 0 IDI 0 t4 ct M 0 V Q1 l~l (D ID 0 ID CD Ql LJl Ul CD ~ ~ 0' c. 0 C) CO C Co C CG +o...

Ahmed, Husain Salem Sayed

2012-06-07T23:59:59.000Z

446

Deformed Matrix Models, Supersymmetric Lattice Twists and N=1/4 Supersymmetry  

SciTech Connect (OSTI)

A manifestly supersymmetric nonperturbative matrix regularization for a twisted version of N = (8, 8) theory on a curved background (a two-sphere) is constructed. Both continuum and the matrix regularization respect four exact scalar supersymmetries under a twisted version of the supersymmetry algebra. We then discuss a succinct Q = 1 deformed matrix model regularization of N = 4 SYM in d = 4, which is equivalent to a non-commutative A*{sub 4} orbifold lattice formulation. Motivated by recent progress in supersymmetric lattices, we also propose a N = 1/4 supersymmetry preserving deformation of N = 4 SYM theory on R{sup 4}. In this class of N = 1/4 theories, both the regularized and continuum theory respect the same set of (scalar) supersymmetry. By using the equivalence of the deformed matrix models with the lattice formulations, we give a very simple physical argument on why the exact lattice supersymmetry must be a subset of scalar subalgebra. This argument disagrees with the recent claims of the link approach, for which we give a new interpretation.

Unsal, Mithat

2008-09-24T23:59:59.000Z

447

Stability Analysis of Continuous-Time Macroeconometic Systems  

E-Print Network [OSTI]

+ 2 flog(Q #3; e y 4 + P #3; e y 11 ) #0; log(Q #3; + P #3; )#0; #12; 2 y 7 + (#12; 2 #0; #12; 3 )Dy 5 #0; y 1 g (2.15) D 2 y 2 = #0; 3 Dy 2 + 4 #26; 1 #12; 6 log " (Q #3; ) #0;#12; 6 #0; #12; 5 (K #3; ) #0;#12; 6 (Q #3; ) #0;#12; 6 e #0;#12; 6 y 4 #0...; #21; 2 ) + #12; 8 ] #27; (2.17) D 2 y 4 = #0; 7 Dy 4 + 8 #26; log " 1#0; #12; 9 (q #3; p #3; =p #3; i ) #12; 10 e #12; 10 (y 5 +y 14 ) 1#0; #12; 9 (q #3; p #3; =p #3; i ) #12; 10 # + log (C #3; e y 1 + g #3; (Q #3; e y 4 + P #3; e y 11 ) +K #3; e y 3...

Barnett, William A.; He, Yijun

1999-01-01T23:59:59.000Z

448

gxxx005-sumtab.dvi  

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

GAUGE GAUGE AND HIGGS BOSONS GAUGE AND HIGGS BOSONS GAUGE AND HIGGS BOSONS GAUGE AND HIGGS BOSONS γ γ γ γ I (J PC ) = 0,1(1 - - ) Mass m < 1 × 10 -18 eV Charge q < 1 × 10 -35 e Mean life τ = Stable g g g g or gluon or gluon or gluon or gluon I (J P ) = 0(1 - ) Mass m = 0 [a] SU(3) color octet graviton graviton graviton graviton J = 2 Mass m < 7 × 10 -32 eV W W W W J = 1 Charge = ± 1 e Mass m = 80.385 ± 0.015 GeV m Z - m W = 10.4 ± 1.6 GeV m W + - m W - = - 0.2 ± 0.6 GeV Full width Γ = 2.085 ± 0.042 GeV N π ± = 15.70 ± 0.35 N K ± = 2.20 ± 0.19 N p = 0.92 ± 0.14 N charged = 19.39 ± 0.08 HTTP://PDG.LBL.GOV Page 1 Created: 7/31/2013 15:19 Citation: J. Beringer et al. (Particle Data Group), PR D86, 010001 (2012) and 2013 partial update for the 2014 edition (URL: http://pdg.lbl.gov) W - modes are charge conjugates of the modes below. p W + DECAY MODES W + DECAY MODES W + DECAY MODES W + DECAY MODES Fraction (Γ i /Γ) Confidence level (MeV /c)

449

1.1-silicon.pptx  

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

Tutorial Tutorial 1 : B asic G W c alcula1ons o n s ilicon David A . S trubbe Department o f M aterials S cience a nd E ngineering, Massachuse8s I ns:tute o f T echnology BerkeleyGW t utorial 22 November 2013 Workflow f or t he t utorial SCF WFN WFNq WFN_inner RHO vxc.dat WFN_fi epsilon sigma inteqp kgrid.x wfn_rho_vxc_info.x Epsilon: s creening a s a f unc1on o f | q| 0 2 4 6 8 10 12 14 16 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 |q| ε 0,0 (q) 1/ε -1 0,0 (q) Sigma: Q P c orrec1ons a s a f unc1on o f L DA e nergy, w ith l inear fi ts -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 -10 -5 0 5 10 15 20 25 QP correction (eV) LDA energy (eV) conduction conduction fit valence valence fit Inteqp: i nterpolated bandstructure http://www.berkeleygw.org/releases/manual_v1.0.6.html Goals Basic g oals: 1. Understand t he b asic w orkflow o f B erkeleyGW, a nd t he r ela1on b etween

450

Total...........................................................  

U.S. Energy Information Administration (EIA) Indexed Site

26.7 26.7 28.8 20.6 13.1 22.0 16.6 38.6 Floorspace (Square Feet) Total Floorspace 1 Fewer than 500................................... 3.2 1.9 0.9 Q Q Q 1.3 2.3 500 to 999........................................... 23.8 10.5 7.3 3.3 1.4 1.2 6.6 12.9 1,000 to 1,499..................................... 20.8 5.8 7.0 3.8 2.2 2.0 3.9 8.9 1,500 to 1,999..................................... 15.4 3.1 4.2 3.4 2.0 2.7 1.9 5.0 2,000 to 2,499..................................... 12.2 1.7 2.7 2.9 1.8 3.2 1.1 2.8 2,500 to 2,999..................................... 10.3 1.2 2.2 2.3 1.7 2.9 0.6 2.0 3,000 to 3,499..................................... 6.7 0.9 1.4 1.5 1.0 1.9 0.4 1.4 3,500 to 3,999..................................... 5.2 0.8 1.2 1.0 0.8 1.5 0.4 1.3 4,000 or More...................................... 13.3 0.9 1.9 2.2 2.0 6.4 0.6 1.9 Heated Floorspace

451

JET and the Prospect for Nuclear Fusion  

Science Journals Connector (OSTI)

This paper describes the Joint European Torus (JET) device which was built as a European collaboration effort, with the aim of testing the scientific feasibility of producing controlled thermonuclear reactions between light nuclei with a net yield of energy. JET is the largest magnetic confinement machine in the world both in physical size and in the magnitude of the plasma current (5 ? 106 Amperes). The machine came into operation in mid-1983 and has followed the first stages of a planned evolution, in which the performance is progressively increased mainly by adding more heating power and which will culminate in eventual operation in a deuterium-tritium mixture. This will permit study of the plasma performance when there is a substantial power input from the ?-particle fusion products. So far operating in deuterium gas with 8 MW of additional heating by neutral beams, a peak ion temperature of 12 keV has been obtained with a corresponding fusion product (density ? confinement time) of 8 ? 1018 m-3 s. If the same conditions were to be achieved in a deuterium-tritium mixture, then the ratio of thermonuclear power output to the heating power input, Q, would be ~ 0.1. It is expected that following further technical improvements to JET, "scientific breakthrough" (namely Q = 1) will be achieved. The next step after JET will be to study a burning or ignited plasma in which no power input is required because energy losses are balanced by ?-particle heating. The requirements for such an experiment will become increasingly clear as more data is obtained from JET. At present it seems likely that a larger apparatus will be needed with a plasma current capability of 12-15 MA. These requirements for the thermonuclear furnace remain broadly consistent with the known technological constraints on an eventual power reactor.

R J Bickerton

1988-01-01T23:59:59.000Z

452

Fluctuation theory of connectivities for subcritical random cluster models  

E-Print Network [OSTI]

We develop a fluctuation theory of connectivities for subcritical random cluster models. The theory is based on a comprehensive nonperturbative probabilistic description of long connected clusters in terms of essentially one-dimensional chains of irreducible objects. Statistics of local observables, for example, displacement, over such chains obey classical limit laws, and our construction leads to an effective random walk representation of percolation clusters. The results include a derivation of a sharp Ornstein--Zernike type asymptotic formula for two point functions, a proof of analyticity and strict convexity of inverse correlation length and a proof of an invariance principle for connected clusters under diffusive scaling. In two dimensions duality considerations enable a reformulation of these results for supercritical nearest-neighbor random cluster measures, in particular, for nearest-neighbor Potts models in the phase transition regime. Accordingly, we prove that in two dimensions Potts equilibrium crystal shapes are always analytic and strictly convex and that the interfaces between different phases are always diffusive. Thus, no roughening transition is possible in the whole regime where our results apply. Our results hold under an assumption of exponential decay of finite volume wired connectivities [assumption (1.2) below] in rectangular domains that is conjectured to hold in the whole subcritical regime; the latter is known to be true, in any dimensions, when $q=1$, $q=2$, and when $q$ is sufficiently large. In two dimensions assumption (1.2) holds whenever there is an exponential decay of connectivities in the infinite volume measure. By duality, this includes all supercritical nearest-neighbor Potts models with positive surface tension between ordered phases.

Massimo Campanino; Dmitry Ioffe; Yvan Velenik

2008-08-26T23:59:59.000Z

453

Quantum Critical Behavior in the Heavy Fermion Single Crystal Ce(Ni0.935Pd0.065)2Ge2  

SciTech Connect (OSTI)

We have performed magnetic susceptibility, specific heat, resistivity, and inelastic neutron scattering measurements on a single crystal of the heavy Fermion compound Ce(Ni{sub 0.935}Pd{sup 0.065}){sub 2}Ge{sub 2}, which is believed to be close to a quantum critical point (QCP) at T = 0. At lowest temperature (1.8--3.5 K), the magnetic susceptibility behaves as {chi}(T)-{chi} (0) {proportional_to} T{sup -1/6} with {chi} (0) = 0.032 x 10{sup -6} m{sup 3}/mole (0.0025 emu/mole). For T < 1 K, the specific heat can be fit to the formula {Delta} C/T = {gamma}{sub 0} - T{sup 1/2} with {gamma}{sub 0} of order 700 mJ/mole-K{sup 2}. The resistivity behaves as {rho} = {rho}{sub 0} + AT{sup 3/2} for temperatures below 2 K. This low temperature behavior for {gamma} (T) and {rho} (T) is in accord with the SCR theory of Moriya and Takimoto. The inelastic neutron scattering spectra show a broad peak near 1.5 meV that appears to be independent of Q; we interpret this as Kondo scattering with T{sub K} = 17 K. In addition, the scattering is enhanced near Q=(1/2, 1/2, 0) with maximum scattering at {Delta} E = 0.45 meV{sup -}; we interpret this as scattering from antiferromagnetic fluctuations near the antiferromagnetic QCP.

Wang, Cuihuan [ORNL; Lawrence, J M [University of California, Irvine; Christianson, Andrew D [ORNL; Chang, S [NIST Center for Neutron Research (NCRN), Gaithersburg, MD; Bauer, E D [Los Alamos National Laboratory (LANL); Gofryk, K [Los Alamos National Laboratory (LANL); Ronning, F [Los Alamos National Laboratory (LANL); Thompson, J D [Los Alamos National Laboratory (LANL); McClellan, K J [Los Alamos National Laboratory (LANL); Rodriguez-Rivera, J A [NCNR and University of Maryland; Lynn, J W [NIST Center for Neutron Research (NCRN), Gaithersburg, MD

2011-01-01T23:59:59.000Z

454

The determination of the void structure of microporous coals by small?angle neutron scattering: Void geometry and structure in Illinois No. 6 bituminous coal  

Science Journals Connector (OSTI)

The access of solvents and reactants to the microvoid volume in porous materials such as coal plays an important role in determining the overall chemistry which takes place during a variety of chemical transformations including oxidation combustion and pyrolysis. The structure and surface composition of these voids were studied using small?angle neutron scattering techniques to examine selectively the subset of the overall void volume distribution which comprises the microvoid volume. Powdered Illinois No. 6 coal containing approximately 20% void volume was slurried in several different aqueous and cyclohexane solutions. The solutions used had various hydrogen?to?deuterium ratios in order to contrast match most of the open pore volume thereby making the microvoid volume visible. The microvoid volume observed is characterized as elongated voids having a fairly well?defined diameter and surface composition. The scattering intensity from the microvoid volume shows a well?defined Porod region indicating that the smallest void dimension is resolved by the instrumental configuration employed. A Guinier region exhibiting Q ? 1 behavior which is characteristic of elongated structures is also observed. The average radius of a circular cross section of these voids is found to be 25.4 . The microvoids are found to be completely filled by aqueous solutions so that the residual neutron scattering which is not eliminated by the contrast?matching aqueous solution is due to the organic matrix structure. Nonaqueous mixtures of cyclohexane cannot fill the entire microvoid volume as effectively as the aqueous mixtures. The scattering differences observed between the aqueous and nonaqueous filled coal indicates that the surface of the microvoids is predominantly aliphatic in character with the principal compositional variation being the presence or absence of acidic functionality on the surface.

Jon S. Gethner

1986-01-01T23:59:59.000Z

455

Search for new particles decaying to diject in 7 TeV proton-proton collisions at CMS  

SciTech Connect (OSTI)

This thesis presents a measurement of the dijet invariant mass spectrum and search for new particles decaying to dijets at CMS in 7 TeV pp collisions using data corresponding to an integrated luminosity of 2.875 pb{sup -1}. The measured dijet mass distribution is compared to QCD prediction from PYTHIA . It is required the pseudorapidity separation of the two jets to satisfy |Dh| < 1.3 with each jet inside the region of |{eta}| < 2.5. The observed dijet mass spectrum is fitted by a smooth function to search for dijet resonances. Since there is no evidence for dijet resonances, the upper limits at 95% Confidence Level (C.L.) on the resonance cross section are set. These generic cross section limits are compared with theoretical predictions for the cross section for several models of new particles: string resonances, axigluons, colorons, excited quarks, E{sub 6} diquarks, Randall-Sundrum gravitons, W' and Z'. It is excluded at 95% C.L. string resonances in the mass range 0.50 < M(S) < 2.50 TeV, excited quarks in the mass range 0.50 < M(q*) < 1.58 TeV, axigluons and colorons in the mass ranges 0.50 < M(A) < 1.17 TeV and 1.47 < M(A) < 1.52 TeV, and E{sub 6} diquarks in the mass ranges 0.50 < M(D) < 0.58 TeV, 0.97 < M(D) < 1.08 TeV, and 1.45 < M(D) < 1.60 TeV. These exclusions extend previously published limits on all models.

Ozturk, Sertac; /Cukurova U.

2011-03-01T23:59:59.000Z

456

Modelling the effect of toroidal plasma rotation on magnetohydrodynamic instabilities in MAST  

SciTech Connect (OSTI)

Present day tokamaks are capable of generating toroidal flows approaching the ion sound speed. Such toroidal rotation is known to have a stabilising effect on resistive wall modes. Here the effects of plasma rotation and diamagnetic drifts on the n = 1 internal kink mode and high-n ballooning modes are presented with specific comparison to experimental data from MAST, Results from MAST concerning the effect of toroidal rotation driven by neutral beam injection (NBI) on sawteeth are presented. The sawteeth period is shown to increase as the co-NBI power, and thus the toroidal plasma rotation, is increased. Conversely, as the counter-NBI is increased, the sawtooth period decreases to some minimum that is shorter than in Ohmically heated plasmas, before lengthening at high toroidal flows. Magnetohydrodynamic stability analyses of the n = 1 internal kink mode with respect to toroidal rotation at finite ion diamagnetic frequency have been performed using a new code, called MISHKA-F. The results indicate that the marginally stable radial location of the q = 1 surface reaches a minimum at approximately the same counter-toroidal rotation as that which minimises the sawtooth period experimentally. It has also been shown that sheared toroidal rotation is able to stabilise the peeling-ballooning modes which are thought to be the likely trigger of Edge Localised Modes (ELMs). A model for ELM triggering in MAST is proposed, such that, initially the rotation shear keeps the edge stabilised until the pressure gradient sufficiently exceeds the stability boundary for static plasmas. When the mode becomes unstable, it grows, ties the flux surfaces together and consequently flattens the rotation profile. This further destabilises the plasma edge, leading to the ELM crash.

Chapman, I. T.; SArelma, S.; Hender, T. C.; Sharapov, S. E.; Meyer, H.; Kirk, A. [UKAEA Fusion Association, Culham Science Centre, Abingdon, Oxfordshire OX14 3DB (United Kingdom); Huysmans, G. T. A. [Association EURATOM-CEA Cadarache, 13108 St. Paul-Lez-Durance (France); Mikhailovskii, A. B. [RRC Kurchatov Institute, Kurchatov Sqr 1, Moscow 123182 (Russian Federation); Wilson, H. R. [University of York, Heslington, York YO10 5DD (United Kingdom)

2006-11-30T23:59:59.000Z

457

Systematic Study of Azimuthal Anisotropy in Cu$+$Cu and Au$+$Au Collisions at $\\sqrt{s_{_{NN}}} = 62.4$ and 200~GeV  

E-Print Network [OSTI]

We have studied the dependence of azimuthal anisotropy $v_2$ for inclusive and identified charged hadrons in Au$+$Au and Cu$+$Cu collisions on collision energy, species, and centrality. The values of $v_2$ as a function of transverse momentum $p_T$ and centrality in Au$+$Au collisions at $\\sqrt{s_{_{NN}}}$=200~GeV and 62.4~GeV are the same within uncertainties. However, in Cu$+$Cu collisions we observe a decrease in $v_2$ values as the collision energy is reduced from 200 to 62.4~GeV. The decrease is larger in the more peripheral collisions. By examining both Au$+$Au and Cu$+$Cu collisions we find that $v_2$ depends both on eccentricity and the number of participants, $N_{\\rm part}$. We observe that $v_2$ divided by eccentricity ($\\varepsilon$) monotonically increases with $N_{\\rm part}$ and scales as ${N_{\\rm part}^{1/3}}$. The Cu$+$Cu data at 62.4 GeV falls below the other scaled $v_{2}$ data. For identified hadrons, $v_2$ divided by the number of constituent quarks $n_q$ is independent of hadron species as a function of transverse kinetic energy $KE_T=m_T-m$ between $0.1q<1$~GeV. Combining all of the above scaling and normalizations, we observe a near-universal scaling, with the exception of the Cu$+$Cu data at 62.4 GeV, of $v_2/(n_q\\cdot\\varepsilon\\cdot N^{1/3}_{\\rm part})$ vs $KE_T/n_q$ for all measured particles.

A. Adare; S. Afanasiev; C. Aidala; N. N. Ajitanand; Y. Akiba; H. Al-Bataineh; A. Al-Jamel; J. Alexander; K. Aoki; L. Aphecetche; R. Armendariz; S. H. Aronson; J. Asai; E. T. Atomssa; R. Averbeck; T. C. Awes; B. Azmoun; V. Babintsev; G. Baksay; L. Baksay; A. Baldisseri; K. N. Barish; P. D. Barnes; B. Bassalleck; S. Bathe; S. Batsouli; V. Baublis; F. Bauer; A. Bazilevsky; S. Belikov; R. Bennett; Y. Berdnikov; A. A. Bickley; M. T. Bjorndal; J. G. Boissevain; H. Borel; K. Boyle; M. L. Brooks; D. S. Brown; D. Bucher; H. Buesching; V. Bumazhnov; G. Bunce; J. M. Burward-Hoy; S. Butsyk; S. Campbell; J. -S. Chai; B. S. Chang; J. -L. Charvet; S. Chernichenko; C. Y. Chi; J. Chiba; M. Chiu; I. J. Choi; T. Chujo; P. Chung; A. Churyn; V. Cianciolo; C. R. Cleven; Y. Cobigo; B. A. Cole; M. P. Comets; P. Constantin; M. Csand; T. Csrg?; T. Dahms; K. Das; G. David; M. B. Deaton; K. Dehmelt; H. Delagrange; A. Denisov; D. d'Enterria; A. Deshpande; E. J. Desmond; O. Dietzsch; A. Dion; M. Donadelli; J. L. Drachenberg; O. Drapier; A. Drees; A. K. Dubey; A. Durum; V. Dzhordzhadze; Y. V. Efremenko; J. Egdemir; F. Ellinghaus; W. S. Emam; A. Enokizono; H. En'yo; B. Espagnon; S. Esumi; K. O. Eyser; D. E. Fields; M. Finger; M. Finger; \\, Jr.; F. Fleuret; S. L. Fokin; B. Forestier; Z. Fraenkel; J. E. Frantz; A. Franz; A. D. Frawley; K. Fujiwara; Y. Fukao; S. -Y. Fung; T. Fusayasu; S. Gadrat; I. Garishvili; F. Gastineau; M. Germain; A. Glenn; H. Gong; M. Gonin; J. Gosset; Y. Goto; R. Granier de Cassagnac; N. Grau; S. V. Greene; M. Grosse Perdekamp; T. Gunji; H. -. Gustafsson; T. Hachiya; A. Hadj Henni; C. Haegemann; J. S. Haggerty; M. N. Hagiwara; H. Hamagaki; R. Han; H. Harada; E. P. Hartouni; K. Haruna; M. Harvey; E. Haslum; K. Hasuko; R. Hayano; X. He; M. Heffner; T. K. Hemmick; T. Hester; J. M. Heuser; H. Hiejima; J. C. Hill; R. Hobbs; M. Hohlmann; M. Holmes; W. Holzmann; K. Homma; B. Hong; T. Horaguchi; D. Hornback; S. Huang; M. G. Hur; T. Ichihara; H. Iinuma; K. Imai; M. Inaba; Y. Inoue; D. Isenhower; L. Isenhower; M. Ishihara; T. Isobe; M. Issah; A. Isupov; B. V. Jacak; J. Jia; J. Jin; O. Jinnouchi; B. M. Johnson; K. S. Joo; D. Jouan; F. Kajihara; S. Kametani; N. Kamihara; J. Kamin; M. Kaneta; J. H. Kang; H. Kanou; T. Kawagishi; D. Kawall; A. V. Kazantsev; S. Kelly; A. Khanzadeev; J. Kikuchi; D. H. Kim; D. J. Kim; E. Kim; Y. -S. Kim; E. Kinney; . Kiss; E. Kistenev; A. Kiyomichi; J. Klay; C. Klein-Boesing; L. Kochenda; V. Kochetkov; B. Komkov; M. Konno; D. Kotchetkov; A. Kozlov; A. Krl; A. Kravitz; P. J. Kroon; J. Kubart; G. J. Kunde; N. Kurihara; K. Kurita; M. J. Kweon; Y. Kwon; G. S. Kyle; R. Lacey; Y. S. Lai; J. G. Lajoie; A. Lebedev; Y. Le Bornec; S. Leckey; D. M. Lee; M. K. Lee; T. Lee; M. J. Leitch; M. A. L. Leite; B. Lenzi; X. Li; X. H. Li; H. Lim; T. Lika; A. Litvinenko; M. X. Liu; B. Love; D. Lynch; C. F. Maguire; Y. I. Makdisi; A. Malakhov; M. D. Malik; V. I. Manko; Y. Mao; L. Maek; H. Masui; F. Matathias; M. C. McCain; M. McCumber; P. L. McGaughey; Y. Miake; P. Mike; K. Miki; T. E. Miller; A. Milov; S. Mioduszewski; G. C. Mishra; M. Mishra; J. T. Mitchell; M. Mitrovski; A. Morreale; D. P. Morrison; J. M. Moss; T. V. Moukhanova; D. Mukhopadhyay; J. Murata; S. Nagamiya; Y. Nagata; J. L. Nagle; M. Naglis; I. Nakagawa; Y. Nakamiya; T. Nakamura; K. Nakano; J. Newby; M. Nguyen; B. E. Norman; R. Nouicer; A. S. Nyanin; J. Nystrand; E. O'Brien; S. X. Oda; C. A. Ogilvie; H. Ohnishi; I. D. Ojha; M. Oka; K. Okada; O. O. Omiwade; A. Oskarsson; I. Otterlund; M. Ouchida; K. Ozawa; R. Pak; D. Pal; A. P. T. Palounek; V. Pantuev; V. Papavassiliou; J. Park; W. J. Park; S. F. Pate; H. Pei; J. -C. Peng; H. Pereira; V. Peresedov; D. Yu. Peressounko; C. Pinkenburg; R. P. Pisani; M. L. Purschke; A. K. Purwar; H. Qu; J. Rak; A. Rakotozafindrabe; I. Ravinovich; K. F. Read; S. Rembeczki; M. Reuter; K. Reygers; V. Riabov; Y. Riabov; G. Roche; A. Romana; M. Rosati; S. S. E. Rosendahl; P. Rosnet; P. Rukoyatkin; V. L. Rykov; S. S. Ryu; B. Sahlmueller; N. Saito; T. Sakaguchi; S. Sakai; H. Sakata; V. Samsonov; H. D. Sato; S. Sato; S. Sawada; J. Seele; R. Seidl; V. Semenov; R. Seto; D. Sharma; T. K. Shea; I. Shein; A. Shevel; T. -A. Shibata; K. Shigaki; M. Shimomura; T. Shohjoh; K. Shoji; A. Sickles; C. L. Silva; D. Silvermyr; C. Silvestre; K. S. Sim; C. P. Singh; V. Singh; S. Skutnik; M. Slune?ka; W. C. Smith; A. Soldatov; R. A. Soltz; W. E. Sondheim; S. P. Sorensen; I. V. Sourikova; F. Staley; P. W. Stankus; E. Stenlund; M. Stepanov; A. Ster; S. P. Stoll; T. Sugitate; C. Suire; J. P. Sullivan; J. Sziklai; T. Tabaru; S. Takagi; E. M. Takagui; A. Taketani; K. H. Tanaka; Y. Tanaka; K. Tanida; M. J. Tannenbaum; A. Taranenko; P. Tarjn; T. L. Thomas; T. Todoroki; M. Togawa; A. Toia; J. Tojo; L. Tomek; H. Torii; R. S. Towell; V-N. Tram; I. Tserruya; Y. Tsuchimoto; S. K. Tuli; H. Tydesj; N. Tyurin; C. Vale; H. Valle

2014-12-02T23:59:59.000Z

458

EXPLORING TRANSITIONS OF SPACE PLASMAS OUT OF EQUILIBRIUM  

SciTech Connect (OSTI)

Space plasmas from the solar wind to planetary magnetospheres and the outer heliosphere are systems in stationary states out of equilibrium. Empirical kappa distributions, which naturally emerge from Tsallis Statistics, successfully describe these space plasmas. The Tsallis formalism offers a solid statistical foundation and provides a set of proven tools for understanding these distributions, including a consistent definition of temperature-the physical temperature, which characterizes the non-equilibrium stationary states. Here, we develop a measure of the 'thermodynamic distance' of stationary states away from equilibrium. The stationary states are labeled by the value of the entropic q-index, lying in a spectrum from q = 1 (equilibrium) to the maximum value of q, which specifies the furthest possible stationary state from equilibrium. We call this the 'q-frozen state', because as a system approaches this state, it behaves analogously to when its temperature approaches absolute zero. We also introduce a novel isothermal procedure that describes a system's transition into different stationary states by varying the q-index, and show how the variation of temperature can be realized using an 'iso-metastability' procedure, in which the system remains in a fixed stationary state. These innovations allow a generalization of the zeroth law of thermodynamics to cover stationary states out of equilibrium. By expressing the entropy in terms of the q-index, we show the detailed paths by which the transition of stationary states evolves toward equilibrium following the dynamics of a characteristic difference equation along the q-indices. This naturally exhibits certain stationary states out of equilibrium that are frequently observed in space plasmas.

Livadiotis, G.; McComas, D. J. [Southwest Research Institute, San Antonio, TX 78238 (United States)

2010-05-01T23:59:59.000Z

459

Switching power pulse system  

DOE Patents [OSTI]

A switching system for delivering pulses of power from a source (10) to a load (20) using a storage capacitor (C3) charged through a rectifier (D1, D2), and maintained charged to a reference voltage level by a transistor switch (Q1) and voltage comparator (12). A thyristor (22) is triggered to discharge the storage capacitor through a saturable reactor (18) and fractional turn saturable transformer (16) having a secondary to primary turn ratio N of n:l/n=n.sup.2. The saturable reactor (18) functions as a "soaker" while the thyristor reaches saturation, and then switches to a low impedance state. The saturable transformer functions as a switching transformer with high impedance while a load coupling capacitor (C4) charges, and then switches to a low impedance state to dump the charge of the storage capacitor (C3) into the load through the coupling capacitor (C4). The transformer is comprised of a multilayer core (26) having two secondary windings (28, 30) tightly wound and connected in parallel to add their output voltage and reduce output inductance, and a number of single turn windings connected in parallel at nodes (32, 34) for the primary winding, each single turn winding linking a different one of the layers of the multilayer core. The load may be comprised of a resistive beampipe (40) for a linear particle accelerator and capacitance of a pulse forming network (42). To hold off discharge of the capacitance until it is fully charged, a saturable core (44) is provided around the resistive beampipe (40) to isolate the beampipe from the capacitance (42) until it is fully charged.

Aaland, Kristian (Livermore, CA)

1983-01-01T23:59:59.000Z

460

Santa Barbara County, California Data Dashboard | Department...  

Energy Savers [EERE]

Program. bbnpbban0003796pmcdashboardy13-q3.xls More Documents & Publications Kansas City Data Dashboard Lowell, Massachusetts Data Dashboard Rutland County Data Dashboard...

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


461

Kansas City Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Kansas City Data Dashboard The data dashboard for Kansas City, a partner in the Better Buildings Neighborhood Program. bbnpbban0003564pmcdashboardy13-q3.xls...

462

Final Meeting Summary Page 1  

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

EIS (TC & WM EIS), Q4 * Draft Land Conveyance Environmental Assessment, Q2 * Natural Gas Pipeline Environmental Impact Statement (EIS), Q3 * 2014 Budget meetings (2015 & 2016...

463

Connecticut Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Connecticut Data Dashboard The Data Dashboard for Connecticut, a partner in the Better Buildings Neighborhood Program. connecticutbban0003806pmcdashboardy13-q3...

464

Indianapolis Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Indianapolis Data Dashboard The data dashboard for Indianapolis, a partner in the Better Buildings Neighborhood Program. bbnpbban0003577pmcdashboardy13-q3.xls...

465

Maryland Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Maryland Data Dashboard The data dashboard for Maryland, a partner in the Better Buildings Neighborhood Program. bbnpbban0003571pmcdashboardy13-q3.xls More...

466

Nevada -- SEP Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Nevada -- SEP Data Dashboard The data dashboard for Nevada -- SEP, a partner in the Better Buildings Neighborhood Program. bbnpbban0004471pmcdashboardy13-q3.xl...

467

Los Angeles Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Los Angeles Data Dashboard The data dashboard for Los Angeles, a partner in the Better Buildings Neighborhood Program. bbnpbban0003562pmcdashboardy13-q3.xls...

468

Seattle Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Seattle Data Dashboard The data dashboard for Seattle, Washington, a partner in the Better Buildings Neighborhood Program. bbnpbban0003573pmcdashboardy13-q3.xl...

469

Cincinnati Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Cincinnati Data Dashboard The data dashboard for Cincinnati, a partner in the Better Buildings Neighborhood Program. bbnpbban0003574pmcdashboardy13-q3.xls More...

470

Greensboro Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Greensboro Data Dashboard The data dashboard for Greensboro, a partner in the Better Buildings Neighborhood Program. bbnpbban0003567pmcdashboardy13-q3.xls More...

471

NYSERDA Data Dashboard | Department of Energy  

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

Data Dashboard NYSERDA Data Dashboard The data dashboard for NYSERDA, a partner in the Better Buildings Neighborhood Program. bbnpbban0003558pmcdashboardy13-q3.xls More...

472

Maine -- SEP Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Maine -- SEP Data Dashboard The data dashboard for Maine -- SEP, a partner in the Better Buildings Neighborhood Program. bbnpbban0004439pmcdashboardy13-q3.xls...

473

New Hampshire Data Dashboard | Department of Energy  

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

Data Dashboard New Hampshire Data Dashboard The data dashboard for New Hampshire, a partner in the Better Buildings Neighborhood Program. bbnpbban0003576pmcdashboardy13-q3.xl...

474

Alabama -- SEP Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Alabama -- SEP Data Dashboard The data dashboard for Alabama -- SEP, a partner in the Better Buildings Neighborhood Program. bbnpbban0004507pmcdashboardy13-q3....

475

Portland Data Dashboard | Department of Energy  

Energy Savers [EERE]

Data Dashboard Portland Data Dashboard The data dashboard for Portland, Oregon, a partner in the Better Buildings Neighborhood Program. bbnpbban0003565pmcdashboardy13-q3.xls...

476

Wisconsin Data Dashboard | Department of Energy  

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

Data Dashboard Wisconsin Data Dashboard The data dashboard for Wisconsin, a partner in the Better Buildings Neighborhood Program. bbnpbban0003579pmcdashboardy13-q3.xls More...

477

Missouri Data Dashboard | Department of Energy  

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

Data Dashboard Missouri Data Dashboard The data dashboard for Missouri, a partner in the Better Buildings Neighborhood Program. bbnpbban0003580pmcdashboardy13-q3.xls More...

478

Michigan Data Dashboard | Department of Energy  

Energy Savers [EERE]

Program. bbnpbban0003559pmcdashboardy13-q3.xls More Documents & Publications Portland Data Dashboard Southeast Energy Efficiency Alliance Data Dashboard Austin Energy...

479

Low-Cost Illumination-Grade LEDs  

SciTech Connect (OSTI)

Solid State Lighting is a cost-effective, energy-conserving technology serving a rapidly expand- ing multi-billion dollar market. This program was designed to accelerate this lighting revolution by reducing the manufacturing cost of Illumination-Grade LEDs. The technical strategy was to investigate growth substrate alternatives to standard planar sapphire, select the most effective and compatible option, and demonstrate a significant increase in Lumen/$ with a marketable LED. The most obvious alternate substrate, silicon, was extensively studied in the first two years of the program. The superior thermal and mechanical properties of Si were expected to improve wavelength uniformity and hence color yield in the manufacture of high-power illumination- grade LEDs. However, improvements in efficiency and epitaxy uniformity on standard c-plane sapphire diminished the advantages of switching to Si. Furthermore, the cost of sapphire decreased significantly and the cost of processing Si devices using our thin film process was higher than expected. We concluded that GaN on Si was a viable technology but not a practical option for Philips Lumileds. Therefore in 2012 and 2013, we sought and received amendments which broadened the scope to include other substrates and extended the time of execution. Proprietary engineered substrates, off-axis (non-c-plane) sapphire, and c-plane patterned sapphire substrates (PSS) were all investigated in the final 18 months of this program. Excellent epitaxy quality was achieved on all three candidates; however we eliminated engineered substrates and non-c-plane sapphire because of their higher combined cost of substrate, device fabrication and packaging. Ultimately, by fabricating a flip-chip (FC) LED based upon c-plane PSS we attained a 42% reduction in LED manufacturing cost relative to our LUXEON Rebel product (Q1-2012). Combined with a flux gain from 85 to 102 Lm, the LUXEON Q delivered a 210% increase in Lm/$ over this time period. The technology was commercialized in our LUXEON Q product in Sept., 2013. Also, the retention of the sapphire increased the robustness of the device, enabling sales of low-cost submount-free chips to lighting manufacturers. Thus, blue LED die sales were initiated in the form of a PSS-FC in February, 2013.

Epler, John

2013-08-31T23:59:59.000Z

480

Development and validation of a HILICMS/MS method for quantification of decitabine in human plasma by using lithium adduct detection  

Science Journals Connector (OSTI)

Abstract A highly sensitive, selective, and rugged quantification method was developed and validated for decitabine (5-aza-2?-deoxycytidine) in human plasma treated with 100?g/mL of tetrahydrouridine (THU). Chromatographic separation was accomplished using hydrophilic interaction liquid chromatography (HILIC) and detection used electrospray ionization (ESI) tandem mass spectrometry (MS/MS) by monitoring lithiated adducts of the analytes as precursor ions. The method involves simple acetonitrile precipitation steps (in an ice bath) followed by injection of the supernatant onto a Thermo Betasil Silica-100, 100נ3.0mm, 5?m LC column. Protonated ([M+H]+), sodiated ([M+Na]+), and lithiated ([M+Li]+) adducts as precursor ions for MS/MS detection were evaluated for best sensitivity and assay performance. During initial method development abundant sodium [M+Na]+ and potassium [M+K]+ adducts were observed while the protonated species [M+H]+ was present at a relative abundance of less than 5% in Q1. The alkali adducts were not be able to be minimized by the usual approach of increasing acid content in mobile phases. Significant analyte/internal standard (IS) co-suppression and inter-lot response differences were observed when using the sodium adduct as the precursor ion for quantification. By adding 2mM lithium acetate in aqueous mobile phase component, the lithium adduct effectively replaced other cationic species and was successfully used as the precursor ion for selected reaction monitoring (SRM) detection. The method demonstrated the separation of anomers and from other endogenous interferences using a 3-min gradient elution. Decitabine stock, working solution stabilities were investigated during method development. Three different peaks, including one from anomerization, were observed in the SRM transition of the analyte when it was in neutral aqueous solution. The assay was validated over a concentration range of 0.5500ng/mL (or 0.44440pg injected on column) in 50?L of human plasma. The accuracy and precision were within 8.6% relative error and 6.3% coefficient of variation, respectively. Decitabine was stable in THU treated human plasma for at least 68 days and after 5 freezethaw cycles when stored at ?70C. Stability of decitabine in THU treated human whole blood, matrix factor and recovery were also evaluated during method validation. The method was successfully used for clinical sample analysis.

Wenyi Hua; Thomas Ierardi; Michael Lesslie; Brian T. Hoffman; Daniel Mulvana

2014-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "q1 q1 q3" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


481

Inflation driven by q-de Sitter in light of Planck 2013 and BICEP2 results  

E-Print Network [OSTI]

We propose a generalised de Sitter scale factor for the cosmology of early and late time universe, including single scalar field is called as inflaton. This form of scale factor has a free parameter $q$ is called as nonextensivity parameter. When $q=1$, the scale factor is de Sitter. This scale factor is an intermediate form between power-law and de Sitter. We study cosmology of such families. We show that both kinds of dark components, dark energy and dark matter simultaneously are described by this family of solutions. As a motivated idea, we investigate inflation in the framework of $q$-de Sitter. We consider three types of scenarios for inflation. In a single inflation scenario, we observe that, inflation ended without any specific ending inflation $\\phi_{end}$, the spectral index and the associated running of the spectral index are %$ n_\\mathrm{s} - 1 \\sim -2\\epsilon, \\quad \\alpha_\\mathrm{s} \\equiv 0 $. To end the inflation: we should have $q=\\frac{3}{4}$. We deduce that the inflation ends when the evolution of the scale factor is $a (t) =e_ {3/4} (t) $. With this scale factor there is no need to specify $\\phi_{end}$. As an alternative to have inflation with ending point, We will study q-inflation model in the context of warm inflation. We propose two forms of damping term $\\Gamma$. In the first case when $\\Gamma=\\Gamma_0$, we show the scale invariant spectrum, (Harrison-Zeldovich spectrum, i.e. $n_s=1$) may be approximately presented by ($q=\\frac{9}{10},~~N=70$). Also there is a range of values of $R$ and $n_s$ which is compatible with the BICEP2 data where $q=\\frac{9}{10}$. In case $\\Gamma=\\Gamma_1V(\\phi)$, it is observed that small values of a number of e-folds are assured for small values of $q$ parameter. For $q=\\frac{9}{10}$ a range of values of $R$ and $n_s$ is compatible with the BICEP2 data.

M. R. Setare; D. Momeni; V. Kamali; R. Myrzakulov

2014-09-09T23:59:59.000Z

482

solar PV | OpenEI  

Open Energy Info (EERE)

PV PV Dataset Summary Description This dataset highlights trends in financing terms for U.S. renewable energy projects that closed financing between Q3 2009 and Q3 2010. Information tracked includes debt interest rates, equity returns, financial structure applied, PPA duration, and other information. NREL's Renewable Energy Finance Tracking Initiative (REFTI) tracks renewable energy project financing terms by technology and project size. The intelligence gathered is intended to reveal industry trends and to inform input assumptions for models. Source NREL Date Released March 27th, 2011 (3 years ago) Date Updated Unknown Keywords biomass financial geothermal project finance solar PV wind onshore Data application/vnd.openxmlformats-officedocument.spreadsheetml.sheet icon RE Project Finance Trends Q3 2009 - Q3 2010 (xlsx, 309.2 KiB)

483

wind onshore | OpenEI  

Open Energy Info (EERE)

onshore onshore Dataset Summary Description This dataset highlights trends in financing terms for U.S. renewable energy projects that closed financing between Q3 2009 and Q3 2010. Information tracked includes debt interest rates, equity returns, financial structure applied, PPA duration, and other information. NREL's Renewable Energy Finance Tracking Initiative (REFTI) tracks renewable energy project financing terms by technology and project size. The intelligence gathered is intended to reveal industry trends and to inform input assumptions for models. Source NREL Date Released March 27th, 2011 (3 years ago) Date Updated Unknown Keywords biomass financial geothermal project finance solar PV wind onshore Data application/vnd.openxmlformats-officedocument.spreadsheetml.sheet icon RE Project Finance Trends Q3 2009 - Q3 2010 (xlsx, 309.2 KiB)

484

Microsoft PowerPoint - C-Mod_quarterly_intro.ppt  

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

Q3 Q3 21 July 2009 Developing the steady state, high-Z wall, high-field tokamak for ITER and beyond FY09 Q3 Status and Plans * Alternator Recertified (April, 2009) - Now in service and operating normally * Disassembly, inspection, TF refurbishment complete - Also improved LN2 systems, vessel heaters, etc. * Lower Hybrid Launcher - Delayed by combination of redeployment of engineering resources to deal with alternator and unexpected technical issues - Installation after end of FY09 campaign * Advanced ICRF antenna - Aimed at strong reduction of RF sheath induced impurity generation - Design progressing well, schedule can be accelerated with ARRA incremental funding FY09 Q3 Status and Plans * Successful Ideas Forum (April, 2009) - >130 presentations, including strong student,

485

project finance | OpenEI  

Open Energy Info (EERE)

project finance project finance Dataset Summary Description This dataset highlights trends in financing terms for U.S. renewable energy projects that closed financing between Q3 2009 and Q3 2010. Information tracked includes debt interest rates, equity returns, financial structure applied, PPA duration, and other information. NREL's Renewable Energy Finance Tracking Initiative (REFTI) tracks renewable energy project financing terms by technology and project size. The intelligence gathered is intended to reveal industry trends and to inform input assumptions for models. Source NREL Date Released March 27th, 2011 (3 years ago) Date Updated Unknown Keywords biomass financial geothermal project finance solar PV wind onshore Data application/vnd.openxmlformats-officedocument.spreadsheetml.sheet icon RE Project Finance Trends Q3 2009 - Q3 2010 (xlsx, 309.2 KiB)

486

TWC-Transcribed Flipcharts  

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

HSEP) o Coordination with WPRS Savannah River Group (Sharon) * Direct Feed LAW Page 1 Safety Culture * Follow-up: Q3 briefing (AprilJune) o Changes actions based on ongoing...

487

Polymer-Ceramic MEMS Bimorphs as Thermal Infrared Sensors  

E-Print Network [OSTI]

bolometer arrays: a review. 2007: SPIE. FLIR SystemsInc, FLIR Q3 Investor Presentation. 2009. Jones, C.D.W. , etYork: Wiley-Interscience. FLIR Systems, Inc. [cited Jan 11,

Warren, Clinton Gregory

2010-01-01T23:59:59.000Z

488

JOURNAL DE PHYSIQUE Colloque C8, Supplement au no 12, Tonie 49, dhcembre 1988  

E-Print Network [OSTI]

, CORRELATION FUNCTIONS AND NEUTRON SCATTERING LAW IN AMORPHOUS MAGNETS K. H. Fischer IFF der, equation (2) leads to the neutron scattering form factor scl(Q) = TXo,(Q) +9, (Q) (3) for T

Boyer, Edmond

489

Three Essays in Business Management, the Natural Environment, and Environmental Policy  

E-Print Network [OSTI]

expenditures, CDP disclosure & GHG emissions .. 63 Table 3.matrix 1. Return on Assets 2. Tobin's Q 3. Direct GHG 4.Supply Chain GHG 0.05 -0.35 0.77 1.00 5. Water Abstraction -

Nairn-Birch, Nicholas Simon

2012-01-01T23:59:59.000Z

490

Homework #1: Critical Reading Describe each of the elements of a System Engineering Design and Analysis (in the table below)  

E-Print Network [OSTI]

(rate equation) 4) Bi-valve reproduction and sustainability (not modeled) 5) Benthic growth/decay (complex biological processes modeled in VIMS) Q2: What is the context of the study? Q3: Who are the major

491

Attachment 1 - PIC Transcribed Flip Chart Notes Final Meeting...  

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

Plan | *** Q2 * 100 D-H Proposed Plan * Draft Land Conveyance EA | Q2 * Natural Gas Pipeline EIS | * Q2 * 2014 Budget Meetings (2015 & 2016 Budgets) | ** Q3 *...

492

Hitchin's Equations and M-Theory Phenomenology  

E-Print Network [OSTI]

Phenomenological compactifications of M-theory involve 7-manifolds with G_2 holonomy and various singularities. Here we study local geometries with such singularities, by thinking of them as compactifications of 7d supersymmetric Yang-Mills theory on a three-manifold Q_3. We give a general discussion of compactifications of 7d Yang-Mills theory in terms of Higgs bundles on Q_3. We show they can be constructed using spectral covers, which are Lagrangian branes with a flat connection in the cotangent bundle T^*Q_3. We explain the dictionary with ALE fibrations over Q_3 and conjecture that these configurations have G_2 holonomy. We further develop tools to study the low energy effective theory of such a model. We show that the naive massless spectrum is corrected by instanton effects. Taking the instanton effects into account, we find that the massless spectrum and many of the interactions can be computed with Morse theoretic methods.

Tony Pantev; Martijn Wijnholt

2009-05-13T23:59:59.000Z

493

"Table B22. Primary Space-Heating Energy Sources, Number of...  

U.S. Energy Information Administration (EIA) Indexed Site

...",174,149,53,77,"Q","Q" "Food Service ...",349,321,87,176,"Q","Q" "Health Care ...",127,127,55,62,"Q",3 " Inpatient ...",11,11,...

494

financial | OpenEI  

Open Energy Info (EERE)

financial financial Dataset Summary Description This dataset highlights trends in financing terms for U.S. renewable energy projects that closed financing between Q3 2009 and Q3 2010. Information tracked includes debt interest rates, equity returns, financial structure applied, PPA duration, and other information. NREL's Renewable Energy Finance Tracking Initiative (REFTI) tracks renewable energy project financing terms by technology and project size. The intelligence gathered is intended to reveal industry trends and to inform input assumptions for models. Source NREL Date Released March 27th, 2011 (3 years ago) Date Updated Unknown Keywords biomass financial geothermal project finance solar PV wind onshore Data application/vnd.openxmlformats-officedocument.spreadsheetml.sheet icon RE Project Finance Trends Q3 2009 - Q3 2010 (xlsx, 309.2 KiB)

495

On the determination of phosphorous via charged particle activation analysis  

E-Print Network [OSTI]

of Cyclotron Terminal . "or Activation Analysis Ql ? WATER INLET Q2 ? BNC CONNECTOR Q3 ? LUCITE Q4 ? CA RBON Figure 3. Four-leaved Carl. on Pea, -. Monitor 1. Ta COLLIMATOR 2. Cu HEAT SINK K MONITOR 4. SAMPLE 5. Cu BASE PLATE 6. WATER COOLING I 2... of Cyclotron Terminal . "or Activation Analysis Ql ? WATER INLET Q2 ? BNC CONNECTOR Q3 ? LUCITE Q4 ? CA RBON Figure 3. Four-leaved Carl. on Pea, -. Monitor 1. Ta COLLIMATOR 2. Cu HEAT SINK K MONITOR 4. SAMPLE 5. Cu BASE PLATE 6. WATER COOLING I 2...

Poland, John Edward

2012-06-07T23:59:59.000Z

496

Deutsche Telekom to offer Microsoft Office on a monthly payment plan Jun 11, 2009  

E-Print Network [OSTI]

Deutsche Telekom to offer Microsoft Office on a monthly payment plan Jun 11, 2009 · Customers able · Offer available first to T-Mobile Austria mobile broadband customers and Deutsche Telekom business customers in Germany from Q3 2009 · Deutsche Telekom is the first telecommunications provider to offer

Deutschmann, Rainer

497

Computational Science Technical Note CSTN-205 Optimising Computations for Evaluating Ising and Potts Model Partition  

E-Print Network [OSTI]

0 Computational Science Technical Note CSTN-205 Optimising Computations for Evaluating Ising and Potts Model Partition Functions by Exact Enumeration K. A. Hawick and D. P. Playne 2013 The Ising computationally feasible for the Q=3,4 state Potts model as well as the 2 state Ising spin model. We report on bit

Hawick, Ken

498

Pinch Effect for Trapped Particles in a Tokamak  

Science Journals Connector (OSTI)

Conservation of canonical angular momentum is shown to require that all trapped particles drift towards the magnetic axis with velocity cE?B? (E? is the toroidal electric field; B? the poloidal magnetic field). This property, plus an amplification process for the number of trapped particles, will explain the relaxation oscillations which occur for q3.

A. A. Ware

1970-07-06T23:59:59.000Z

499

KEY DASHBOARD INDICATORS OF PROGRESS TOWARD Goals Human Resources, FY 09-10  

E-Print Network [OSTI]

in alignment with our service approach, technical Progress Indication capability, and regulatory requirements 2Q 3Q 4Q measuring performance, and increasing transparency · Identify, review, and enhance the top plan to reduce energy costs Supports Strategic Directions 1, 5, & 7 #12;

New Mexico, University of

500

Stable lattice Boltzmann schemes with a dual entropy approach  

E-Print Network [OSTI]

Stable lattice Boltzmann schemes with a dual entropy approach for monodimensional nonlinear waves of a lattice Boltzmann scheme. This method is expressed in terms of the dual of the mathematical entropy with D1Q3 lattice Boltzmann schemes for the Burgers equation. It conducts to the explicitation of three

Boyer, Edmond