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Note: This page contains sample records for the topic "q4 q1 q1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
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1

Q2 Q3 Q4 Q4 Q3 Q2 Q1 Q1 Q2 Q3 Q4 Q3 Q2 Q1 Q1 Q2 Q3 Q4 Q4 Q3 Q2 Q1  

E-Print Network [OSTI]

. and Solar Energy Industries Association. All Rights Reserved 2 Key Findings Photovoltaics (PV) PV.S. solar market was the growth of utility-scale solar. Utility PV installations in the U.S. grew 670% over Q2 Q3 Q4 Q4 Q3 Q2 Q1 Q1 Q2 Q3 Q4 A Greentech Media Company U.S. SOLAR MARKET INSIGHT REPORT | Q1

2

Better Buildings EECBG Q1 Reporting Webinar  

Broader source: Energy.gov [DOE]

Better Buildings EECBG Q1 Reporting Webinar, from the U.S. Department of Energy's Better Buildings program.

3

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

4

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. 2009; Biggs et al. 2010), as well as a variety of shallower surface processes. These include previously thought to be quiescent (e.g. on the East African Rift: Biggs et al. 2009) and at locations

Biggs, Juliet

5

Quarterly SSP Experiment Summary-FY13-1Q 1  

National Nuclear Security Administration (NNSA)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "ofEarlyEnergyDepartmentNational Nuclearhas 'Natitude' |Requests | National Nuclearenvironment |1-4Q3-1Q 1

6

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.

7

2014_Q1.indd  

Energy Savers [EERE]

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious RankCombustionImprovement3 Beryllium-Associated Worker2014 HouseCoveredAir ConditionersLamps;40901W We We We

8

Q1 1998 STEO Docs  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9,0,InformationU.S.Feet) Year Weekly DownloadData8

9

nl403402q 1..7  

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

the Li ions into the electrode, which may change the kinetics and phase behaviors of solid-state electrode lithiation. Third, the use of the ionic liquid or Li 2 O electrolyte...

10

am501650q 1..8  

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

energy density is proportional to the square of the voltage, increasing the voltage window quadratically increases the energy density. It has further been shown that MnO 2...

11

jp404990q 1..9  

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

as components of energy storage devices such as batteries, capacitors, fuel cells , and solar cells, and as electrochemical sensors, biosensors, and drug release systems. 1,2 In...

12

FOIA Quarterly Reports (Q1 2013)  

Broader source: Energy.gov [DOE]

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...

13

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.

14

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.

15

Dish Sterling High Performance Thermal Storage- FY13 Q1  

Broader source: Energy.gov [DOE]

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

16

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.

17

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....

18

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.

19

Bloo Solar formerly Q1 Nanosystems | Open Energy Information  

Open Energy Info (EERE)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Office of InspectorConcentrating SolarElectricEnergyCTBarre BiomassTHIS PAGE ISJump to:Blackfeet Nation

20

Quarterly SSP Experiment Summary-Q1FY14 1  

National Nuclear Security Administration (NNSA)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "ofEarlyEnergyDepartmentNational Nuclearhas 'Natitude' |Requests | National Nuclearenvironment

Note: This page contains sample records for the topic "q4 q1 q1" 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

Domestic Coal Distribution 2009 Q1 by Destination State: Alabama  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecemberSteam Coal Import96 4.87CBECS Public Use Data0 0(BTUFeet)(Dollars per604

22

Domestic Coal Distribution 2009 Q1 by Origin State: Alabama  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecemberSteam Coal Import96 4.87CBECS Public Use Data0 0(BTUFeet)(Dollars

23

Significant Cost Improvement of Li-Ion Cells Through Non-NMP...  

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

Q3 Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 Approach 5 Dry coated electrode Electrode design optimization Binder and electrolyte development Process and equipment optimization...

24

Significant Cost Improvement of Li-Ion Cells Through Non-NMP...  

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

Q3 Q4 Q1 Q2 Q3 Q4 Q1 Q2 Q3 Q4 Approach 5 Dry coated electrode Electrode design optimization Binder and electrolyte development Process and equipment optimization Water...

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data CenterFranconia, Virginia:FAQ <Information Administration (EIA) 103. Relative Standard Errors for Table N8.3;" "3

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data CenterFranconia, Virginia:FAQ <Information Administration (EIA) 103. Relative Standard Errors for Table N8.3;" "34

27

"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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data CenterFranconia, Virginia:FAQ <Information Administration (EIA) 103. Relative Standard Errors for Table N8.3;"

28

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

SciTech Connect (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 Q2, the square of the four-momentum transfer, is related to the distribution of charge and magnetization within the nucleon. High precision measurements of the nucleon form factors are essential for stringent tests of our current theoretical understanding of confinement within the nucleon. Measurements of the neutron form factors, in particular, those of the neutron electric form factor, have been notoriously difficult due to the lack of a free neutron target and the vanishing integral charge of the neutron. Indeed, a precise measurement of the neutron electric form factor has eluded experimentalists for decades; however, with the advent of high duty-factor polarized electron beam facilities, experiments employing polarization degrees of freedom have finally yielded the first precise measurements of this fundamental quantity. Following a general overview of the experimental and theoretical status of the nucleon form factors, a detailed description of an experiment designed to extract the neutron electric form factor from measurements of the neutron's recoil polarization in quasielastic 2H(e, e')1H scattering is presented. The experiment described here employed the Thomas Jefferson National Accelerator Facility's longitudinally polarized electron beam, a magnetic spectrometer for detection of the scattered electron, and a neutron polarimeter designed specifically for this experiment. Measurements were conducted at three Q2 values of 0.45, 1.13, and 1.45 (GeV/c)2, and the final results extracted from an analysis of the data acquired in this experiment are reported and compared with recent theoretical predictions for the nucleon form factors.

Bradley Plaster

2004-02-01T23:59:59.000Z

29

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

30

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.

31

Conservative Flux Recovery from the Q1 Conforming Finite Element Method on  

E-Print Network [OSTI]

University, Bowling Green, Ohio 43403-0221 2 Department of Mathematics and Statistics, Bowling Green State State University, Bowling Green, OH 43403-0221 (e-mail: chou@bgnet.bgsu.edu) Contract grant sponsor-Hsiang Chou,1 Songnian He,2 Wen-Wei Lin3 1 Department of Mathematics and Statistics, Bowling Green State

Lin, Wen-Wei

32

Conservative Flux Recovery from the Q1 Conforming Finite Element Method on  

E-Print Network [OSTI]

--Hsiang Chou Department of Mathematics and Statistics Bowling Green State University Bowling Green, OH 43403­0221, email:chou@bgnet.bgsu.edu 1 Songnian He Department of Mathematics and Statistics Bowling Green State University Bowling Green, OH 43403­0221 Wen­Wei Lin Department of Mathematics National Tsing­Hua University

Chou, So-Hsiang

33

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.

34

Direct s-CO2 Receiver Development- 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.

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

Observation of nuclear fusion driven by a pyroelectric crystalQ1  

E-Print Network [OSTI]

in a room temperature solid-state setting, including `cold' fusion5 and `bubble' fusion6 , have met.............................................................. Observation of nuclear fusion driven ............................................................................................................................................................................. While progress in fusion research continues with magnetic1 and inertial2 confinement, alternative

Gimzewski, James

37

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.

38

Self-Cleaning CSP Optics with EDS- FY13 Q1  

Broader source: Energy.gov [DOE]

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

39

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.

40

High-Temperature Solar Selective Coating Development for Power Tower Receivers- FY13 Q1  

Broader source: Energy.gov [DOE]

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

Note: This page contains sample records for the topic "q4 q1 q1" 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

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.

42

Microsoft Word - MDA FINAL FY14 Q1_1_31_14.doc  

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

utility based in the Pacific Northwest within the Department of Energy. BPA markets wholesale electrical power from 31 federal hydroelectric projects owned and operated by the...

43

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

44

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....

45

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.

46

Next Generation Solar Collectors for CSP - FY13 Q1 | Department of Energy  

Office of Environmental Management (EM)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "of EnergyEnergyENERGY TAXBalanced Scorecard Federal2EnergyDepartment ofNews News RecentNextNext

47

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

Gasoline and Diesel Fuel Update (EIA)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"Click worksheet9,1,50022,3,,,,6,1,,781Title:DOBEIA-0202(83/4Q) Short-Term2Q) Energy1Q) 1992 1

48

Microsoft Word - MDA FINAL FY14 Q1_1_31_14.doc  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr MayAtmospheric Optical Depth7-1D: VegetationEquipment Surfaces andMappingENVIRONMENTALHYDROPOWERFebruarySave the October 30,74

49

Microsoft Word - fy09_annualtarget_climatemodeling1_Q1 _2_.doc  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr MayAtmospheric Optical Depth7-1D: VegetationEquipment SurfacesResource Program Preliminary Needs535:UFC5,Overview ofLanceBTARGET: FY09:

50

FY 2015 Q1 Metrics Supporting Documentation 2015-02-09.xls  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "of EnergyEnergyENERGYWomentheATLANTA, GA5 &of EnergyOrganizationtotal FYNuclear Research FOA5 EM5

51

PowerPoint Presentation - FY13 Q1 | Department of Energy  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious RankCombustion | Department ofT ib l L d FNEPA/309 Reviewers |of Excellence BuildingESPCPCS

52

Low-Cost, Lightweight Solar Concentrators - FY13 Q1 | Department of Energy  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "ofEarly Career Scientists'Montana.ProgramJulietipDepartmentJuneWhenJulyBadges atEnergyVehicles |ORNLdocument

53

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

National Nuclear Security Administration (NNSA)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "ofEarlyEnergyDepartment ofDepartmentStewardshipAdministration helps more than 600 kidspeople |1G U

54

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 800şC in air. Similar beneficial results from surface modification were observed after 26,000 hours of oxidation at 850şC. • MnCo spinel coatings prepared from metallic powder precursors exhibited low area-specific resistance after 12,000 hours of testing at 800°C. • 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 PNNL’s 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 PNNL’s SECA CTP stack test fixture. • Baseline testing of LSCF-based cells from Fuel Cell Materials was performed in PNNL’s 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

55

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

56

Observations from The EV Project in Q4 2013  

SciTech Connect (OSTI)

This is a summary report for The EV Project 4th quarter 2013 reports. It describes electric vehicle driver driving and charging behavior observed in Q4. It is the same report as the previously approved/published Q3 2013 report, only the numbers have been updated. It is for public release and does not have limited distribution.

John Smart

2014-02-01T23:59:59.000Z

57

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.

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

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.

60

RPS Status Report Q1 & Q2 2012 Page 2 I. ABOUT THE RPS AND THIS REPORT  

E-Print Network [OSTI]

-scale renewable energy development in California, there are other programs that stimulate development of customer- side renewable generation. The California Solar Initiative (CSI) and Self-Generation Incentive Program (SGIP) provide incentives for customers to install renewable distributed generation technologies

Note: This page contains sample records for the topic "q4 q1 q1" 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

Roles of poloidal rotation in the q = 1 high-order harmonic tearing modes in a tokamak plasma  

SciTech Connect (OSTI)

Roles of poloidal rotation in stabilizing the m/n=1/1 kink-tearing mode and exciting its high-order harmonic tearing modes are numerically investigated by using a reduced magnetohydrodynamic model. It is found that the high-order harmonic tearing modes, such as m/n=2/2, m/n=3/3, or even much higher-m harmonics, can be destabilized so significantly by rotation shear as to be more unstable than or comparable to the m/n=1/1 mode. Moreover, the short wave-length Kelvin- Helmholtz (KH) instabilities can be excited in the large rotation shear regime. The scaling power laws of the linear growth rate for each harmonic mode in different rotation shear regimes are verified by the previous relevant theoretical results based on the non-constant-{psi} and constant-{psi} behavior categories in tearing modes. During the nonlinear evolution, the m/n=2/2 mode dominated phase first appears and then is followed by the m/n=1/1 mode dominated nonlinear phase instead. Afterward, some smaller sub-islands due to the high-order harmonics are produced in the large irregular m=1 crescent-shaped island, and then a coalescence process of turbulent island chains occurs before the decay phase.

Wei Lai; Wang Zhengxiong [Key Laboratory of Materials Modification by Beams of the Ministry of Education, School of Physics and Optoelectronic Technology, Dalian University of Technology, Dalian 116024 (China)

2013-01-15T23:59:59.000Z

62

A Small-Particle Solar Receiver for High-Temperature Brayton Power Cycles- FY13 Q1  

Broader source: Energy.gov [DOE]

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

63

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

64

Notes on MATH39522 Q1 A few people didn't attempt this at all. Of those that did, most got the first part. For the second  

E-Print Network [OSTI]

people coped with (a) & (b), many getting full marks. However, I was a bit surprised at how many ­ many writing down incorrect formulae. Q6 Most people did well on this relatively straightforward question. Q7 A wide range of marks, some people scoring very highly. Many who scored middle-range marks did

Sidorov, Nikita

65

State","Jan 2015","Feb 2015","Mar 2015","Q1 2015","Apr 2015  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data CenterFranconia,(Million Barrels) Crude Oil Reserves in NonproducingAdditions to Capacity5","Feb 2015","Mar

66

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)...

67

Minimally non-local nucleon-nucleon potentials in $?$EFT at order $Q^4$  

E-Print Network [OSTI]

We construct a coordinate-space chiral potential, including $\\Delta$-isobar intermediate states in its two-pion-exchange component. The contact interactions entering at next-to-leading and next-to-next-to-next-to-leading orders ($Q^2$ and $Q^4$, respectively, $Q$ denoting generically the low momentum scale) are rearranged by Fierz transformations to yield terms at most quadratic in the relative momentum operator of the two nucleons. The low-energy constants multiplying these contact interactions are fitted to the 2013 Granada database, consisting of 2309 $pp$ and 2982 $np$ data (including, respectively, 148 and 218 normalizations) in the laboratory-energy range 0--300 MeV. For the total 5291 $pp$ and $np$ data in this range, we obtain a $\\chi^2$/datum of roughly 1.3 for a set of three models characterized by long- and short-range cutoffs, $R_{\\rm L}$ and $R_{\\rm S}$ respectively, ranging from $(R_{\\rm L},R_{\\rm S})=(1.2,0.8)$ fm down to $(0.8,0.6)$ fm. The long-range (short-range) cutoff regularizes the one- and two-pion exchange (contact) part of the potential.

M. Piarulli; L. Girlanda; R. Schiavilla; R. Navarro Pérez; J. E. Amaro; E. Ruiz Arriola

2014-12-19T23:59:59.000Z

68

"!#$%'&()$021436587 9A@BC5D9EBGFH@7I@P$Q1SRTUV WYX`$a'14RTbcRTde1SfGgihqprs%412tvuuw xyy Hd$yefygyTxheiHd$yecjqkl#mn$xhopyqn  

E-Print Network [OSTI]

Ł¦ŁˇGgihqprs%412tvu¨u¨w xyy Hd$yefygyTxheiHd$yecjqkl#mn$xhopyqn ersqrtTuTv¦w)w)xTy{z|tuf}r~r¨SxTw)xTyv yvC'nvYD8Sv chromospheric conditions is plotted in Fig. 1. "!Tv¦w Ë : # E$±%$YC'ĹC·ÉcA}{8Ć|'Y¦S®iÇ (¦ ˙& Ł˘ ę ćÁç2č ĺ' ó ă ( For instance, in regions of sufficiently strong vertical mag- netic field, a series of shocks may lift

Kosovichev, Alexander G.

69

Q1: What is the birth date of the employees whose first name is `Franklin'? Q2: Retrieve the names of all employees who work for the `Research' department.  

E-Print Network [OSTI]

of all employees who work for the `Research' department. Q3: Retrieve names of departments who have in `Chicago', and also list the name of projects; Q5: Retrieve the salary of every employee; Q6: Retrieve all distinct salary values; Q7: Make a list of all projects that involve an employee whose last name

Li, Yanjun "Lisa"

70

State","Jan 2013","Feb 2013","Mar 2013","Q1 2013","Apr 2013","May 2013","Jun 201  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data CenterFranconia,(Million Barrels) Crude Oil Reserves in NonproducingAdditions to Capacity onF.Sample andDecade,"2014Jan

71

State","Jan 2014","Feb 2014","Mar 2014","Q1 2014","Apr 2014","May 2014","Jun 201  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data CenterFranconia,(Million Barrels) Crude Oil Reserves in NonproducingAdditions to Capacity onF.Sample

72

State","Jan 2014","Feb 2014","Mar 2014","Q1 2014","Apr 2014","May 2014","Jun 201  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data CenterFranconia,(Million Barrels) Crude Oil Reserves in NonproducingAdditions to Capacity

73

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

74

2013_Q4.indd  

Energy Savers [EERE]

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious RankCombustionImprovement3 Beryllium-Associated Worker Registry Summary 2013Evaluation32013

75

2012_Q4  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:YearRound-Up from theDepartment( SampleEnergyof Environmental| Department2012 MarketSTART2 -

76

Professional Worker Career Experience Survey (PWCES) Data and Metadata  

E-Print Network [OSTI]

qname,question,QPage,type,DataType,value,answer,Measuring,Source Q1,My current job title is,1,text,text,,,Work History,ITWF Q2,How long have you been in your current position?,1,text,numeric,,,,ITWF Q3,How long have you been with your current... employer?,1,text,numeric,,,Work History,ITWF Q4,My current career field is classified as,1,select,numeric,99,Select One,,ITWF Q4,,1,select,numeric,1,Management/Financial/Professional ,, Q4,,1,select,numeric,2,Computer/Mathematical ,, Q4,,1,select,numeric,3...

Rosenbloom, Joshua L.; Ash, Ronald A.

2009-10-06T23:59:59.000Z

77

U.S. Residential Photovoltaic (PV) System Prices, Q4 2013 Benchmarks: Cash Purchase, Fair Market Value, and Prepaid Lease Transaction Prices  

SciTech Connect (OSTI)

The price of photovoltaic (PV) systems in the United States (i.e., the cost to the system owner) has dropped precipitously in recent years, led by substantial reductions in global PV module prices. This report provides a Q4 2013 update for residential PV systems, based on an objective methodology that closely approximates the book value of a PV system. Several cases are benchmarked to represent common variation in business models, labor rates, and module choice. We estimate a weighted-average cash purchase price of $3.29/W for modeled standard-efficiency, polycrystalline-silicon residential PV systems installed in the United States. This is a 46% decline from the 2013-dollar-adjusted price reported in the Q4 2010 benchmark report. In addition, this report frames the cash purchase price in the context of key price metrics relevant to the continually evolving landscape of third-party-owned PV systems by benchmarking the minimum sustainable lease price and the fair market value of residential PV systems.

Davidson, C.; James, T. L.; Margolis, R.; Fu, R.; Feldman, D.

2014-10-01T23:59:59.000Z

78

BeamlineEXP1&EXP3 88030.491660  

E-Print Network [OSTI]

.4 87310.4 88030.491660 92115 BPM3 Spectrometer DipoleB1 94075 96220 97340 2145 1120 455.2 93000 (94062.5) (96207.5)(97327.5) 85830.4 14801030 700 Q5 (Q1EXP3) BPM1BPM2Q4Q1 + H1 Q2Q3 + H2W W 418ToroidT7 Toroid T8 Matrix If the bpm's are calibrated and the resolution known, then the rms energy resolution yields: 1

79

COBIOT-836; NO. OF PAGES 6 Please cite this article in press as: Chew YH, Halliday KJ. A Q1stress-free walk from Arabidopsis to crops, Curr Opin Biotechnol (2010), doi:10.1016/j.copbio.2010.11.011  

E-Print Network [OSTI]

are threatened by global warming and increas- ingCO2 levels[2].Toensurefoodsupplieskeeppacewitha growing Halliday1,2 Global concerns such as food security and climate change have highlighted an urgent need

Millar, Andrew J.

2010-01-01T23:59:59.000Z

80

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

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative FuelsTotal" (Percent) Type: SulfurBase4,"Ames City of",6,1,"OmahaThousand Cubic Feet)

Note: This page contains sample records for the topic "q4 q1 q1" 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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative FuelsTotal" (Percent) Type: SulfurBase4,"Ames City of",6,1,"OmahaThousand Cubic

82

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

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative FuelsTotal" (Percent) Type: SulfurBase4,"Ames City of",6,1,"OmahaThousand

83

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

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative FuelsTotal" (Percent) Type: SulfurBase4,"Ames City

84

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

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative FuelsTotal" (Percent) Type: SulfurBase4,"Ames

85

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

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative FuelsTotal" (Percent) Type:

86

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

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative FuelsTotal" (Percent)

87

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

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative FuelsTotal"

88

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

89

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

90

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

91

Microchannel Receiver Development- FY12 Q4  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this Oregon State University project, funded by SunShot, for the fourth quarter of fiscal year 2012.

92

A disease of swine caused by a chromobacterium species  

E-Print Network [OSTI]

?Pa(y.?h.b.PO< TABLE OF CONTENTS x? pPOTa?mrOpaP O9, 1gs,'s, w'us,1 VS r9Q6M6V'w4, Q?uM ?g6?'w,uM 9's 864 V,,8 1,swQgV,1 JQ,?g6us?S g8 sAg8,? p4 A's w68sg1,Q,1 65 su55gwg'84 gM? J6Q4'8w, 56Q ' 1gss,Q4'4g68 JQ6V?,M 56Q 49, 56??6Ag8C Q,'s68s7 ?'? p4 'JJ,'Qs 's '8... 'wu4, 6Q w9Q68gw J8,uM68g'? ls 49gs CQ6uJ 6 5 1gs,'s,s gs Q,?'4g? ,?S J66Q?S u81,Qs4661 g8 sAg8, _T g4 A's w68sg1,Q,1 1,sgQ'V?, 46 g8?,s4gC'4, 49, w681g4g68? ?V? O9, 1gs,'s, '?s6 6wwuQs g8 9uM'8s '81 49,Q,56Q, 9's J 6ssgV?, JuV?gw 9,'?49 'sJ,w4s...

Sippel, William Lawrence

1955-01-01T23:59:59.000Z

93

Optimisations for quadrature representations of finite element tensors through automated code generation  

E-Print Network [OSTI]

= 1, q = 2 608 13.77 3084 6.62 12412 1.69 52124 0.81 p = 1, q = 3 2660 29.11 12432 12.26 46528 3.30 205424 1.30 p = 1, q = 4 7955 57.90 38007 20.99 155751 5.14 622679 2.04 p = 2, q = 1 314 6.02 3336 1.75 34984 0.40 359984 0.08 p = 2, q = 2 1838 11...

Oelgaard, Kristian B; Wells, G N

2009-07-20T23:59:59.000Z

94

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...

95

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

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

High-Temperature Solar Selective Coating Development for Power Tower Receivers - FY13 Q1 High-Temperature Solar Selective Coating Development for Power Tower Receivers - FY13 Q1...

96

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

97

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...

98

Kronecker-Jacobi symbol and Quadratic Reciprocity Let Q be the ...  

E-Print Network [OSTI]

Proof. Since d(2) = 8, the Theorem (with b = 2) reduces the problem to the simple cases a = 1,3,5,7. Corollary 3. If q is an odd prime, q? = (?1) q?1. 2 q, and a = 0 ...

2012-11-29T23:59:59.000Z

99

c17a.xls  

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

... Q 26 19 Q 1,451 1,192 Q 17.9 16.3 Principal Building Activity Education ... Q 12 16 Q 1,384 1,990 Q 8.4 7.9 Food...

100

General Physics II Exam 1 -Chs. 16,17,18 -Electric Fields, Potential, Current Feb. 11, 2013 Name Rec. Instr. Rec. Time  

E-Print Network [OSTI]

General Physics II Exam 1 - Chs. 16,17,18 - Electric Fields, Potential, Current Feb. 11, 2013 Name charge can experience an electric force. 4. (2) T F The smallest magnitude (non-zero) net charge of the electric force on Q1 due to Q2. b) (3) The direction of the electric force acting on Q1 is a. pushing Q1

Wysin, Gary

Note: This page contains sample records for the topic "q4 q1 q1" 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

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

102

Interpretation of searches for supersymmetry with simplified models  

E-Print Network [OSTI]

~g ! q #1;q~#6;LSP All-hadronic [12–14,16] T2 ~q~q#6; ~q ! q~#6;LSP All-hadronic [12,13,16] T5zz ~g ~g ~g ! q #1;q~#6;02, ~#6;02 ! Z~#6;LSP All-hadronic [13,14] Opposite-sign dileptons [25] Multileptons [23] T3w ~g ~g ~g ! q #1;q~#6;LSP Single leptonţ... jets [17] ~g ! q #1;q~#6;#4;1 , ~#6;#4;1 ! W#4; ~#6;LSP T5lnu ~g ~g ~g ! q #1;q~#6;#4;1 , ~#6;#4;1 ! ‘#7;~#6;LSP Same-sign dileptons [19] T3lh ~g ~g ~g ! q #1;q~#6;LSP Opposite-sign dileptons [21,22] ~g ! q #1;q~#6;02, ~#6;02 ! ‘ţ‘#1; ~#6;LSP T1bbbb ~g...

Baringer, Philip S.; Bean, Alice; Benelli, Gabriele; Kenny, R. P. III; Murray, Michael J.; Noonan, Danny; Sanders, Stephen J.; Stringer, Robert W.; Tinti, Gemma; Wood, Jeffrey Scott; Chatrchyan, S.; Khachatryan, V.; Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Aguilo, E.

2013-09-23T23:59:59.000Z

103

CSP Tower Air Brayton Combustor- FY12 Q4  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this SWRI project, funded by SunShot, for the fourth quarter of fiscal year 2012.

104

Supercritical Carbon Dioxide Turbo-Expander- FY12 Q4  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this SWRI project, funded by SunShot, for the fourth quarter of fiscal year 2012.

105

Next Generation Solar Collectors for CSP- FY12 Q4  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this 3M project, funded by SunShot, for the fourth quarter of fiscal year 2012.

106

Advanced Manufacture of Reflectors- FY12 Q4  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this University of Arizona project, funded by SunShot, for the fourth quarter of fiscal year 2012.

107

Scattering Solar Thermal Concentrators- FY12 Q4  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this Penn State project, funded by SunShot, for the fourth quarter of fiscal year 2012.

108

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 Connecticut’s existing residential energy efficiency programs that are overseen by the ratepayer fund board and administered by CT utilities. N2N’s 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 N2N’s and DOE’s short-term program goals, as well as the State of Connecticut’s 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

109

Greedy Strategies for Convex Minimization  

E-Print Network [OSTI]

?ig satis es the following inequality e1 E(0) E( x); (4.6) and ek ek 1 1 Aj Sj q 2(q 1) e (p 1)q (q 1)p k 1 ; k 2; (4.7) where A = (p 1) q(p 1) p(q 1) (q 1) qq q=ppq 1 q 1 : Proof. Clearly e1 = E(x1) E( x) E(0) E( x) since... := inff X ? jc?( x)j : x = X ? c?( x)?g: We prove the following lemma. Lemma 4.2.6. Let the objective function E satisfy Condition 0 and Condition 1 with M0 < qM q 1. Let problem (1.1) have a solution x = P ? c?( x)? 2 , where f?g = D is a...

Nguyen, Hao Thanh

2013-08-22T23:59:59.000Z

110

PERMUTATION POLYNOMIALS AND GROUP PERMUTATION POLYNOMIALS  

E-Print Network [OSTI]

of polynomi- als of the form xrf(xs), where s | q - 1. This class originated from the work of Rogers. These are called monomials. The permutation polynomials of the form h(x) = xrf(xs) over Fq are closely related to polynomials h(x) such that (r, s) = 1 and s | q - 1. Let d = (q - 1)=s. Suppose that h(x) = xrf

Park, Young Ho

111

Why Was Short-Time Work Unattractive During the Crisis?  

E-Print Network [OSTI]

Metal products (11%),metallurgy (10%), Rubber and Plastics (Rubber and Plastics Metallurgy Fabricated Metal productscrisis. In 2009Q1, the metallurgy and the equipment sectors

Gonthier, Pauline

2012-01-01T23:59:59.000Z

112

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...

113

University of California Response to DOE Questions Regarding...  

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

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:...

114

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...

115

Stretch Efficiency for Combustion Engines: Exploiting New Combustion...  

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

II experiments address the main irreversibilities in unrestrained combustion * 'Internal' heat transfer - Products to reactants heat transfer over large Ts - dS Q Q(1T C -...

116

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

117

E-Print Network 3.0 - analysis program eeap Sample Search Results  

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

DAC 16 Master CANS (Cont.) Assig. Q1 Q2 EEAP Gil Gmez, Marisa Martorell Bofill, Xavier Navarro... Informaci (Master MINT) APDA: Advanced Programming and Distributed...

118

Stretch Efficiency for Combustion Engines: Exploiting New Combustion...  

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

and Modeling Modified Bajulasz 2-Chamber Architecture (SAE 860534) Q 1 st stage * Air & reformate compressed in inner chamber * Ignition occurs * Fuel injection & reforming...

119

Making a difference for minorities: Evaluation of an educational enrichment program  

E-Print Network [OSTI]

matriculated in educational programs toward higher degrees,EVALUATION OF AN EDUCATIONAL ENRICHMENT PROGRAM Q1 Studentevaluation of an educational intervention program designed

Barlow, AEL; Villarejo, Merna R

2004-01-01T23:59:59.000Z

120

--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...

Note: This page contains sample records for the topic "q4 q1 q1" 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

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...

122

c36a.xls  

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

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...

123

c36.xls  

Gasoline and Diesel Fuel Update (EIA)

... 302 Q Q Q 1.09 1.12 1.16 1.03 0.23 Q 0.04 Q HVAC Equipment Upgrade ... 223 13 37 Q 1.14 1.10 1.13 1.04 0.15 Q 0.04 0.01...

124

c35.xls  

Gasoline and Diesel Fuel Update (EIA)

Re-Configuration ... 277 Q Q Q 1,305 651 740 392 0.21 Q 0.03 Q HVAC Equipment Upgrade ... 197 Q 33 Q 1,482 709 909 405 0.13 Q 0.04 Q Lighting...

125

Z .Atmospheric Research 57 2001 5180 www.elsevier.comrlocateratmos  

E-Print Network [OSTI]

2 , depending on the ice habit. It is also shown that mixed-phase clouds are more sensitive; Radiation budget; Ice optical properties; Mixed phase ) Corresponding author. Tel.: q1-814-863-1584; fax: q1 for the parameterization of cloud optical properties in bulk and bin microphysical models. Implications for arctic cloudy

Harrington, Jerry Y.

126

Final Exam/Fall 1998 Math 351 Name (10) 1. Find a 2 × 2 matrix A ...  

E-Print Network [OSTI]

... be a 2 × 2 matrix, Q1 = [1, -1]t and Q2 = [3, -2]t. Assume that. AQ1 = 4Q1 , AQ2 = 9Q2. (i) Find an invertible matrix Q and a diagonal matrix D such that A = QDQ.

1910-10-62T23:59:59.000Z

127

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...

128

--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...

129

Introduction to Measurement with Theory  

E-Print Network [OSTI]

principle. Bennet (1920) and Montgomery (1937) pursued the branch of index number theory where differences replaced the ratios in (12). Thus, they looked for two functions of 4N variables, ?P(p0,p1,q0,q1) and ?Q(p0,p1,q0,q1), which added up...1,q0,q1). However, the basic idea can be traced back to the early accounting and industrial engineering literature; see Harrison (1918; 275). 20 started by Marshall (1890) and Bennet (1920) and continued by Hotelling( 1938; 253- 254), Hicks...

Barnett, William A.; Diewert, W. Erwin; Zellner, Arnold

2009-09-01T23:59:59.000Z

130

IFT3355: Infographie Sujet 5: shading 2  

E-Print Network [OSTI]

partir de l'objet · Cette visibilité est simplefiée: il faut seulement identifier si un objet bloque la cossin qq ii NMT 22 1 11 cossin sin )cos( qq q q i ii i N VN T Ti Ni(cosq1 cosq2)Vi1 Ti 1 2 (Ni cosq1 Vi1) Ni cosq2 1sin2 q2 12 sin2 q1 12 1cos2 q1 1q 2q 1sinq 2sinqM 1iV 1cosqiN 1 11

Montréal, Université de

131

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

132

A Simple Mixture Theory for ? Newtonian and Generalized Newtonian Constituents  

E-Print Network [OSTI]

] based on the following notations L(?) = gradv?(x, t) D(?) = 1 2 ( L(?) + L T (?) ) q = ?? ?=1 q? Q = 1 ?m ?? ?=1 ??Q? ? = 1 ?m ?? ?=1 ????(x, t) pi = ?pi1 = pi2 (2.39) 13 In which q is heat flux, Q is heat supply, ? and ?? are entropy densities... of the mixture and the constituents. We begin with the entropy inequality ?m D? Dt + div (q ? ) ? ? Q ? ? 0 (2.40) We have assumed that entropy due to heat flux q? is q? ? where ? is the common temperature of the constituents and the entropy due to heat supply Q?...

Powell, Michael Joseph

2012-08-31T23:59:59.000Z

133

U.S. Residential Photovoltaic (PV) System Prices, Q4 2013 Benchmarks...  

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

by the top 10 installers in terms of installed capacity, based on data from the California Solar Initiative (CSI 2013). Focusing our analysis on large installers represents a...

134

http://www.eh.doe.gov/nepa/process/ll/95q4.htm  

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

Amarillo, Texas High Explosive Waste Water Treatment Facility at LANL, Los Alamos, New Mexico Decontamination and Dismantlement of the Pinellas Plant, Pinellas, Florida...

135

Self-Cleaning CSP Optics with EDS- FY12 Q4  

Broader source: Energy.gov [DOE]

This document summarizes the progress of this Boston University project, funded by SunShot, for the fourth quarter of fiscal year 2012.

136

FY 2014 Q4 Metrics Report 2014-11-06.xlsx  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "of EnergyEnergyENERGYWomentheATLANTA, GA5 &of EnergyOrganizationtotal FY 20106EnergyFY

137

High-Efficiency Receivers for Supercritical Carbon Dioxide Cycles - FY12 Q4  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Delicious Rank EERE:YearRound-UpHeatMulti-Dimensional Subject:Ground Hawaii HIGHBrayton Energy's supercritical carbon|

138

Microsoft PowerPoint - SRS Headcount by County of Residence Q4 FY 2013.pptx  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May JunDatastreamsmmcrcalgovInstrumentsrucLas Conchas recovery challenge fundProject QuarterlyDepartment ofEvaluationRequest

139

On the physics of the $so_q(4)$ hydrogen atom  

E-Print Network [OSTI]

In this work we investigate the $q$-deformation of the $so(4)$ dynamical symmetry of the hydrogen atom using the theory of the quantum group $su_q(2)$. We derive the energy spectrum in a physically consistent manner and find a degeneracy breaking as well as a smaller Hilbert space. We point out that using the deformed Casimir as was done before leads to inconsistencies in the physical interpretation of the theory.

P. G. Castro; R. Kullock

2015-03-05T23:59:59.000Z

140

active-learning laboratory session: Topics by E-print Network  

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

Ac.Yr. 201112, 1e Sem. Q1 - Exercise Session 5 - sc4026 1 12 Abate, Alessandro 190 1999 Special Session CiteSeer Summary: This report was prepared under the auspicies of the...

Note: This page contains sample records for the topic "q4 q1 q1" 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

E-Print Network 3.0 - aff aulacosterna stal Sample Search Results  

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

Aff(1, K) die affine Gruppe. Sie ist definiert als die Gruppe der affinen... , b K GL(2, K) Ist K ein endlicher Korper mit q |K|, so ist | Aff(1, K)| q(q - 1). Aufgabe...

142

Postgraduate Diploma in Social Work/MSW Frequently Asked Questions  

E-Print Network [OSTI]

Postgraduate Diploma in Social Work/MSW Frequently Asked Questions Educational Qualifications Q 1 I months full-time equivalent relevant experience always required of applicants to the MSW at the point

Mottram, Nigel

143

Competing Types of Order in Two-Dimensional Bose-Fermi Mixtures  

E-Print Network [OSTI]

PRL 97, 030601 (2006) PHYSICAL REVIEW LETTERS week ending 21The American Physical Society PRL 97, 030601 (2006) PHYSICAL0 minf‘ p ; ‘ q 1 g, , k k 1 PRL 97, 030601 (2006) PHYSICAL

Mathey, Ludwig; Tsai, Shan-Wen; Castro Neto, Antonio H.

2006-01-01T23:59:59.000Z

144

1493.ps - Optimization Online  

E-Print Network [OSTI]

Q1 = fx : a kx g k;alx g lg; Q2 = fy : c ky h k;cly h lg: 9 .... Electronic Colloquium on Computational Complexity Report TR03-012 (2003). [16] J. Kraj cek, Lower ...

145

How Generic is Burning Plasma Physics? S.C. Prager  

E-Print Network [OSTI]

bound zero transferability = zero utility An upper bound A tokamak BP expt will NOT pre-empt a non electrons · ...... #12;Sample List of Configurations · q > 1 axisymmetric: tokamak family AT, ST · q

146

High-Efficiency Receivers for Supercritical Carbon Dioxide Cycles...  

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

More Documents & Publications High-Efficiency Low-Cost Solar Receiver for Use in a Supercritical CO2 Recompression Cycle - FY13 Q1 High-Efficiency Receivers for Supercritical...

147

High-Efficiency Low-Cost Solar Receiver for Use in a Supercritical...  

Office of Environmental Management (EM)

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

148

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

149

Degradation Mechanisms and Development of Protective Coatings...  

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

and Development of Protective Coatings for TES and HTF Containment Materials - F13 Q1 Corrosion in Very High-Temperature Molten Salt for Next Generation CSP Systems Direct s-CO2...

150

Stochastic Nash Equilibrium Problems - Optimization Online  

E-Print Network [OSTI]

marginal cost is 5+2?1q1 and it increases as parameter ?1 increases. We list details of other .... locational prices, Operations Research, Vol. 55, pp. 809-827 ...

2010-01-22T23:59:59.000Z

151

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

E-Print Network [OSTI]

Aizhu Chen. “China’s 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

152

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

E-Print Network [OSTI]

China View. 2009. China’s energy intensity down 2.9% in Q1:demand at constant energy intensity, 1980–2006. Source: NBS,percent reduction in energy intensity (defined as energy use

Zhou, Nan

2010-01-01T23:59:59.000Z

153

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

154

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,...

155

The Tate conjecture over finite fields (AIM talk) These are my notes for a talk at the The Tate Conjecture workshop at the American Institute  

E-Print Network [OSTI]

. For example, for a model X1 Pn over Fq, acts as .a1W a2W : : :/ 7! .a q 1W a q 2W : : :/W X1.F/ ! X1.F/; X1.F

Milne, Jim

156

Pless Power Moments 2-weight Projective Codes  

E-Print Network [OSTI]

, (2) w1A1 + w2A2 = n(q - 1)qk-1 , (3) w2 1A1 + w2 2A2 = n(q - 1){n(q - 1) + 1}qk-2 (4) a0 a1 a0 = w1w2, a1 = -(w1 + w2) (x - w1)(x - w2) = a0 + a1x + x2 (5) x a0(2) + a1(3) + (4) a0(A1 + A2) + a1(w1A1 + w2A2) + w2 1A1 + w2 2A2 = A1(a0 + a1w1 + w2 1) + A2(a0 + a1w2 + w2 2) (6) = a0(qk - 1) + a1n(q - 1)qk

Yoshii, Yoji

157

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

158

MTH221, LINEAR ALGEBRA, FINAL EXAM FALL 2006 Question 1 ...  

E-Print Network [OSTI]

If A = (. 1 1. 0 3 ) a) (4 points) Find all eigenvalues A b) (6 points)Find a nonsingular matrix Q and a diagonal matrix D such that. Q?1AQ = D (that it is A = QDQ?1) ...

John L Casti (Santa Fe) 1377 2003 Feb 12 15:14:22

2008-12-02T23:59:59.000Z

159

x  

E-Print Network [OSTI]

Dec 18, 2004 ... components A B and Q and a StructuredVector component ?. § ?P ˇ ?D¨ in the form. §Ą Q Ą ? 1. P. BT. A. ?D ¨. An AugSysMatrix can either be ...

2004-12-18T23:59:59.000Z

160

--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...

Note: This page contains sample records for the topic "q4 q1 q1" 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

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 ...

162

c18a.xls  

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

... 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...

163

c19a.xls  

Gasoline and Diesel Fuel Update (EIA)

... 21 Q 16 Q Q 1,119 21.2 Q 14.5 Principal Building Activity Education ... 15 6 11 1,198 640 1,027 12.8 9.4 10.7...

164

Europaisches Patentamt European Patent Office  

E-Print Network [OSTI]

Europaisches Patentamt European Patent Office Office europeen des brevets ® Publication number: o 303 459 A2 @ EUROPEAN PATENT APPLICATION ® Application number: 88307391.8 @ Int. C1.4: C 12 Q 1

Church, George M.

165

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

166

A complete characterization of termination of Hans ZANTEMA  

E-Print Network [OSTI]

A complete characterization of termination of 0 p 1 q ! 1 r 0 s Hans ZANTEMA Universiteit Utrecht@fmi.uni­passau.de Abstract We completely characterize termination of one­rule string rewriting systems of the form 0 p 1 q ! 1 r 0 s for every choice of positive integers p, q, r, and s. For the simply terminating cases, we

Utrecht, Universiteit

167

A note on the Lyapunov Equation Alessandro Abate  

E-Print Network [OSTI]

A note on the Lyapunov Equation Alessandro Abate a.abate@tudelft.nl Delft Center for Systems and Control, TU Delft October 27, 2011 ­ Ac.Yr. 2011/12, 1e Sem. Q1 ­ Note ­ sc4026 #12;A. Abate Consider/12, 1e Sem. Q1 ­ Note ­ sc4026 1 #12;A. Abate Consider the following operations: AX + XAT = -Q2 AXX-1

Abate, Alessandro

168

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.

169

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

170

Bose Einstein condensation in a gas of the Fibonacci oscillators  

E-Print Network [OSTI]

We consider a system of the two-parameter deformed boson oscillators whose spectrum is given by a generalized Fibonacci sequence. In order to obtain the role of the deformation parameters (q1,q2) on the thermostatistics of the system, we calculate several thermostatistical functions in the thermodynamical limit and investigate the low-temperature behavior of the system. In this framework, we show that the thermostatistics of the (q1,q2)-bosons can be studied by the formalism of Fibonacci calculus which generalizes the recently proposed formalism of q-calculus. We also discuss the conditions under which the Bose-Einstein condensation would occur in the present two-parameter generalized boson gas. However, the ordinary boson gas results can be obtained by applying the limit q1=q2=1.

Abdullah Algin

2008-10-10T23:59:59.000Z

171

Approximate String Joins in a Database (Almost) for Free Luis Gravano Panagiotis G. Ipeirotis H. V. Jagadish  

E-Print Network [OSTI]

1AiQ.Pos - R2AjQ.Pos k AND R2AjQ.Pos - R1AiQ.Pos k AND LEN(R1.Ai) - LEN(R2.Aj) k AND LEN(R2.Aj) - LEN(R1.Ai) k GROUP BY R1.A0, R2.A0, R1.Ai, R2.Aj HAVING COUNT(*) LEN(R1.Ai)+q-1 - k*q AND COUNT(*) LEN(R2.Aj)+q-1 - k*q AND edit distance(R1.A

Gravano, Luis

172

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

173

Collinearity in Linear Structural Models of Market Power Jeffrey M. Perloff*  

E-Print Network [OSTI]

if the marginal cost and demand equations are linear. Key Words: collinearity, estimation, market power. JEL that the marginal cost curve is cMC = + w+ r + Q + , (1) where w is the wage, r is the rental rate on capital, Q The well-known structural model used to estimate market power suffers from a severe collinearity problem

Perloff, Jeffrey M.

174

2/25/2014 Page 1 of 4 PON-13-610 Questions, Answers, and Clarifications  

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Statistics on the remaining amount of funding available through PON-13-610 can be found at: http://energy to Buydownincentives@energy.state.ca.us. Available Funding Q.1 Will the Energy Commission add additional funding from to this program. The Energy Commission, at its sole discretion, reserves the right to increase or decrease funding

175

--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...

176

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...

177

--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...

178

--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...

179

--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...

180

--No Title--  

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

13 45 34 742 2,638 1,695 17.9 17.2 20.1 Heating Equipment (more than one may apply) Heat Pumps ... Q 21 12 Q 1,019 719 Q 20.5 16.3 Packaged...

Note: This page contains sample records for the topic "q4 q1 q1" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
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We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


181

Abstract--In the context of the ongoing deregulation of the electricity industry, we revisit the commonly held assumption that,  

E-Print Network [OSTI]

to current debates in the context of deregulation by supporting the following two points: First in the following two sections. II. CENTRALIZED VERSUS DECENTRALIZED UNIT COMMITMENT In the following expressions ( ) = n i i Q i C Q (1) such that total generation equals total load. 1= = n i D i Q Q (2) This basic

Ilic, Marija D.

182

Bio-Char Soil Management on Highly Weathered Soils in the Humid Tropics  

E-Print Network [OSTI]

therefore have to be applied each year to sustain soil productivity. Management of black carbon (C36 Bio-Char Soil Management on Highly Weathered Soils in the Humid Tropics Johannes Lehmann1), ColombiaQ1 CONTENTS 36.1 Bio-Char Management and Soil Nutrient Availability

Lehmann, Johannes

183

MATH 360: Project 5, Modeling of a single species population This project is due Friday 5th December.  

E-Print Network [OSTI]

December. Background: In this project, we will study a fish population in a lake. By setting up of protection of this population, we will set up a scheme for fishing. Question 1: Denote by P(t) the fish and M using the relations in Q1. Suppose an epidemic disease attacked the fish in the lake

Fletcher, Alastair

184

General Physics II Exam 1 -Chs. 16,17 -Electric Fields & Potential Feb. 2, 2009 Name Rec. Instr. Rec. Time  

E-Print Network [OSTI]

General Physics II Exam 1 - Chs. 16,17 - Electric Fields & Potential Feb. 2, 2009 Name Rec. Instr produce an electric field in the surrounding region. a) (6) Find the electric field that Q1 produces at point A. Draw and label it it as an arrow E1 on the diagram. b) (6) Find the electric field that Q2

Wysin, Gary

185

A Combinatorial Model for the Macdonald Polynomials Department of Mathematics  

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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

186

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

187

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"

188

Atom microscopy via two-photon spontaneous emission spectroscopy RID A-5077-2009  

E-Print Network [OSTI]

#1;e?i#1;#7;k?#6;2#2;t#3;e?i#6;1tC1#1;t#2; ? ei#6;1tC2#1;t#2;#4; + 1 2#8;q gqe i#1;#7;q+#6;2#2;tCe k,q#1;t#2; , #1;6c#2; C? 4 k#1;t#2; = 1 2 gk #1;e?i#1;#7;k+#6;2#2;t#3;e?i#6;1tC1#1;t#2; ? ei#6;1tC2#1;t#2;#4; ? 1 2#8;q gqe i#1;#7;q?#6...;2#2;tCe k,q#1;t#2; , #1;6d#2; C? e k,q#1;t#2; = 1 2gq #1;e?i#7;qt#3;e?i#6;2tC3k#1;t#2; ? C4k#1;t#2;ei#6;2t#4; . #1;6e#2; In the long-time limit, #5;#12;#1;t ? #14;#2;#6; = #8; k,q Ce k,q#1;#14;#2;#5;e,1k,1q#6; . #1;7#2; The final...

Qamar, Sajid; Evers, Joerg; Zubairy, M. Suhail

2009-01-01T23:59:59.000Z

189

Mathematics 136 Calculus 2 Lab Day 3: Environmental Modeling (Tropical Forests Forever?)  

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, 2014 Goals The logistic differential equation (1) dQ dt = kQ 1 - Q M can be used to model any quantity the greatest amount of plant material per unit area. This is often referred to as the plant biomass. Biomass, to simplify, plant biomass will be measured by the carbon content of the plants. The mean plant biomass on 1

Little, John B.

190

Micromachining technologies for miniaturized communication devices Clark T.-C. Nguyen  

E-Print Network [OSTI]

beams, to high-Q inductors and tunable capacitors, to switches and antennas. Environmental parasites, inductor, capacitor, switch, communications, Q 1. INTRODUCTION Due in large part to regulatory bodies than their super-heterodyne counterparts, the former are still preferred over the latter because

Nguyen, Clark T.-C.

191

Contents lists available at ScienceDirect journal homepage: www.elsevier.com/locate/enpol  

E-Print Network [OSTI]

2011 Keywords: Wind power Offshore wind power Levelized cost of energy Breakeven priceQ1 a b s t r a c that drive these costs, we develop a pro-forma cash flow model to calculate two results: the levelized cost other new renewable energy technologies, though it is more costly than land-based wind power and most

Firestone, Jeremy

192

BIOCHEMISTRY OF SNAKE VENOM NEUROTOXINS AND THEIR APPLICATION TO THE STUDY OF THE SYNAPSE  

E-Print Network [OSTI]

Bgt s-Bgt BSA CD Q.1 OviF Ddt D! viS d- TC DTT GABA HNB 3H-Labeling of a-Bgt and Ddt. Iodinated derivatives of the twodendra- toxin ([125r]-ddt) was the only product isolated (

Hanley, M.R.

2011-01-01T23:59:59.000Z

193

1 SOFE, Chicago, IL, June 27, 2011 Design of the ITER First Wall and  

E-Print Network [OSTI]

First Wall (FW) panel and a Shield Block (SB). It covers ~600 m2 Cooling water (3 MPa and 70°C) is supplied to the BM by manifolds supported off the vacuum vessel behind or to the side of the SB. #12 Pipes Be ?les Be ?les Normal Heat Flux Finger: · q'' = ~ 1-2 MW/m2 · Steel Cooling Pipes · HIP

Raffray, A. René

194

CONTROL ISSUES IN THE DESIGN OF A GAS TURBINE CYCLE FOR CO2 CAPTURE  

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CONTROL ISSUES IN THE DESIGN OF A GAS TURBINE CYCLE FOR CO2 CAPTURE Query Sheet Q1: AU: short title OF A GAS TURBINE CYCLE FOR CO2 CAPTURE Lars Imsland, Dagfinn Snarheim, and Bjarne A. Foss Department-closed / gas turbine cycle for capture. Some control strategies and their interaction with the process design

Foss, Bjarne A.

195

Evidence of universality in the dynamical response of nanomechanical ultra-nanocrystalline diamond resonators at millikelvin temperatures  

E-Print Network [OSTI]

independent theory. In particular, polycrystalline diamond is an exciting material for nanomechanical devicesEvidence of universality in the dynamical response of nanomechanical ultra-nanocrystalline diamond fabricated from ultra-nanocrystalline diamond. Frequency shift f/f0 and dissipa- tion Q-1 demonstrate

196

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.

197

On the Fermat-Weber Center of a Convex Object Sariel Har-Peled  

E-Print Network [OSTI]

On the Fermat-Weber Center of a Convex Object Paz Carmi Sariel Har-Peled Matthew J. Katz May 23, 2004 Abstract We show that for any convex object Q in the plane, the average distance from the Fermat-Weber scheme for finding an approximate Fermat-Weber center of a convex polygon Q. 1 Introduction For a planar

Har-Peled, Sariel

198

HAZARDOUS MATERIALS EMERGENCY RESPONSE  

E-Print Network [OSTI]

ANNEX Q HAZARDOUS MATERIALS EMERGENCY RESPONSE #12;ANNEX Q - HAZARDOUS MATERIALS EMERGENCY RESPONSE 03/10/2014 v.2.0 Page Q-1 PROMULGATION STATEMENT Annex Q: Hazardous Materials Emergency Response, and contents within, is a guide to how the University conducts a response specific to a hazardous materials

199

Exercise Session 6 (with solutions) Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 6 (with solutions) Alessandro Abate a.abate@tudelft.nl Marco Forgione m Session 6 ­ sc4026 #12;A. Abate, M. Forgione Linear Quadratic Regulator, in Theory Consider an object ­ Ac.Yr. 2012/13, 1e Sem. Q1 ­ Exercise Session 6 ­ sc4026 1 #12;A. Abate, M. Forgione it can be easily

Abate, Alessandro

200

Exercise Session 4 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 4 Alessandro Abate a.abate@tudelft.nl Solomon Zegeye s Session 4­ sc4026 #12;A. Abate, S.K. Zegeye Controllability and Observability of Feedback Interconnection. The input of the ­ Ac.Yr. 2009/10, 1e Sem. Q1 ­ Exercise Session 4­ sc4026 1 #12;A. Abate, S.K. Zegeye

Abate, Alessandro

Note: This page contains sample records for the topic "q4 q1 q1" 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

Exercise Session 2 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 2 Alessandro Abate a.abate@tudelft.nl Pawel Stano p ­ Exercise Session 2 ­ sc4026 #12;A. Abate, P. Stano Review of Eigenvalues and Eigenvectors Computation Find with the aid of MATLAB. ­ Ac.Yr. 2011/12, 1e Sem. Q1 ­ Exercise Session 2 ­ sc4026 1 #12;A. Abate, P. Stano

Abate, Alessandro

202

Exercise Session 6 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 6 Alessandro Abate a.abate@tudelft.nl Marco Forgione m Session 6 ­ sc4026 #12;A. Abate, M. Forgione Linear Quadratic Regulator, in Theory Consider an object Sem. Q1 ­ Exercise Session 6 ­ sc4026 1 #12;A. Abate, M. Forgione Integral Control Consider the simple

Abate, Alessandro

203

Exercise Session 3 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 3 Alessandro Abate a.abate@tudelft.nl Marco Forgione m ­ Exercise Session 3 ­ sc4026 #12;A. Abate, M. Forgione Linearization Example In the following diagram, we.Yr. 2012/13, 1e Sem. Q1 ­ Exercise Session 3 ­ sc4026 1 #12;A. Abate, M. Forgione · x, horizontal position

Abate, Alessandro

204

Exercise Session 7 (with solutions) Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 7 (with solutions) Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a Session 7 ­ sc4026 #12;A. Abate, A. Haber Solution to state space models Find the output response Sem. Q1 ­ Exercise Session 7 ­ sc4026 1 #12;A. Abate, A. Haber The output is Y (t) = CX(t) + DU

Abate, Alessandro

205

Exercise Session 7 (with solutions) Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 7 (with solutions) Alessandro Abate a.abate@tudelft.nl Marco Forgione m Session 7 ­ sc4026 #12;A. Abate, M. Forgione Solution to state space models Find the output response Sem. Q1 ­ Exercise Session 7 ­ sc4026 1 #12;A. Abate, M. Forgione The output is Y (t) = CX(t) + DU

Abate, Alessandro

206

Bonus Point Exercise 1 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Bonus Point Exercise 1 Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a ­ Exercise Session 1 ­ sc4026 #12;A. Abate, A. Haber Linearization Example In the following diagram, we have.Yr. 2009/10, 1e Sem. Q1 ­ Exercise Session 1 ­ sc4026 1 #12;A. Abate, A. Haber · x, horizontal position

Abate, Alessandro

207

Exercise Session 3 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 3 Alessandro Abate a.abate@tudelft.nl Pawel Stano p ­ Exercise Session 3 ­ sc4026 #12;A. Abate, P. Stano Linearization Example In the following diagram, we have.Yr. 2011/12, 1e Sem. Q1 ­ Exercise Session 3 ­ sc4026 1 #12;A. Abate, P. Stano · x, horizontal position

Abate, Alessandro

208

Exercise Session 3 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 3 Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a ­ Exercise Session 3­ sc4026 #12;A. Abate, A. Haber Linearization Example In the following diagram, we have.Yr. 2010/11, 1e Sem. Q1 ­ Exercise Session 3­ sc4026 1 #12;A. Abate, A. Haber · x, horizontal position

Abate, Alessandro

209

Bonus Point Exercise 2 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Bonus Point Exercise 2 Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a ­ Exercise Session 2 ­ sc4026 #12;A. Abate, A. Haber Solution to state space models Find the output response Sem. Q1 ­ Exercise Session 2 ­ sc4026 1 #12;A. Abate, A. Haber Equilibria and Phase Portrait Determine

Abate, Alessandro

210

Exercise Session 6 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 6 Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a Session 6 ­ sc4026 #12;A. Abate, A. Haber Linear Quadratic Regulator, in Theory Consider an object of mass Sem. Q1 ­ Exercise Session 6 ­ sc4026 1 #12;A. Abate, A. Haber Integral Control Consider the simple

Abate, Alessandro

211

Exercise Session 2 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 2 Alessandro Abate a.abate@tudelft.nl Jacopo Antonello j ­ Exercise Session 2 ­ sc4026 #12;A. Abate, J. Antonello Review of Eigenvalues and Eigenvectors Computation with the aid of MATLAB. ­ Ac.Yr. 2012/13, 1e Sem. Q1 ­ Exercise Session 2 ­ sc4026 1 #12;A. Abate, J. Antonello

Abate, Alessandro

212

Exercise Session 3 (with solutions) Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 3 (with solutions) Alessandro Abate a.abate@tudelft.nl Marco Forgione m ­ Exercise Session 3 ­ sc4026 #12;A. Abate, M. Forgione Linearization Example In the following diagram, we.Yr. 2012/13, 1e Sem. Q1 ­ Exercise Session 3 ­ sc4026 1 #12;A. Abate, M. Forgione · x, horizontal position

Abate, Alessandro

213

Exercise Session 1 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 1 Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a ­ Exercise Session 1 ­ sc4026 #12;A. Abate, A. Haber 1. Properties of the matrix exponential Show, by using/10, 1e Sem. Q1 ­ Exercise Session 1 ­ sc4026 1 #12;A. Abate, A. Haber 2. Elaboration of the Predator

Abate, Alessandro

214

Exercise Session 3 (with solutions) Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 3 (with solutions) Alessandro Abate a.abate@tudelft.nl Pawel Stano p ­ Exercise Session 3 ­ sc4026 #12;A. Abate, P. Stano Linearization Example In the following diagram, we have.Yr. 2011/12, 1e Sem. Q1 ­ Exercise Session 3 ­ sc4026 1 #12;A. Abate, P. Stano · x, horizontal position

Abate, Alessandro

215

Exercise Session 4 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 4 Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a ­ Exercise Session 4­ sc4026 #12;A. Abate, A. Haber Nonlinear System, Linearization, Stability Consider. ­ Ac.Yr. 2010/11, 1e Sem. Q1 ­ Exercise Session 4­ sc4026 1 #12;A. Abate, A. Haber Controllability Show

Abate, Alessandro

216

Exercise Session 2 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 2 Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a ­ Exercise Session 2 ­ sc4026 #12;A. Abate, A. Haber Properties of the matrix exponential Show, by using/11, 1e Sem. Q1 ­ Exercise Session 2 ­ sc4026 1 #12;A. Abate, A. Haber Review of Eigenvalues

Abate, Alessandro

217

Effects of municipal effluent on algal growth  

E-Print Network [OSTI]

a method to re- 13 move phosphorus to O. 01 ppm by using ferric chloride Alum has also been used for phosphate removal in both the secondary and tertiary processes. It has reduced *he phosphorus concentration of the ef'fluent *o O. q- 1. 0 mg...

Sung, Yeh-Min

1975-01-01T23:59:59.000Z

218

SANDIA REPORT SAND2007-1423  

E-Print Network [OSTI]

SANDIA REPORT SAND2007-1423 Unlimited Release Printed March 2007 A Multi-Scale Q1/P0 Approach for the United States Department of Energy by Sandia Corporation. NOTICE: This report was prepared as an account Department of Energy's National Nuclear Security Administration under Contract DE-AC04-94AL85000. Approved

Shashkov, Mikhail

219

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

220

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

Note: This page contains sample records for the topic "q4 q1 q1" 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

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

222

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

223

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

224

Geology of the Hilda-Northwest Area, Mason County, Texas  

E-Print Network [OSTI]

of the Wilberns formation, was named by Barnes (1944, p. 37) for the Welge land surveys in northern Gillespie County. Neaatite 004Q1es Oa sn enposnse of the Ikon lhnuatein sandstone amber, Shush hesatite cygoles oa a weethere4 L4on Mowntain sendsteno slaps...

Fisher, Neil E

1960-01-01T23:59:59.000Z

225

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...

226

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

227

Iteration Bounds for Finding the ?-Stationary Points for Structured ...  

E-Print Network [OSTI]

Oct 15, 2014 ... where ? = p/q with 1/p + 1/q = 1, then we prove that the new algorithms have an overall iteration complexity bound of O(1/?q) in finding an ?-stationary ...... + Mr,. (35) which means that if the perturbation is small, then the ...

2014-10-15T23:59:59.000Z

228

Page 1 of 10 PON-13-606 Q&A Questions, Answers and Clarifications  

E-Print Network [OSTI]

Infrastructure Solicitation PON-13-606 Alternative and Renewable Fuel and Vehicle Technology Program California Energy Commission December 18, 2013 General Questions Q.1 Under each category requirement still have to layer on the expense of a credit card reader? A.2 The Solicitation has been amended

229

(a) p contact p-lnGaAs --p-lnP cladding  

E-Print Network [OSTI]

of different dimensions and/or materials have to be aligned to sub- micron precision to enable efficient (PL:1545 nm) Spacer Super lattice Bonding layer 1 .7Q-AI0055Ga0292In0653As (8x) nP 1.1 Q-1n085Ga0 5As

Bowers, John

230

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

231

ccsd-00000736(version2):22Oct2003 Electron correlation effects on the dielectric function of liquid metals  

E-Print Network [OSTI]

of a system of interacting electrons is to study the acoustic excitations of liquid metals, since the speed, the speed of sound, c, can be expressed as: c = pi Q (Q) . (1) Here Q is the wave number, (Q) is the total response of the liquid is to- tally elastic and one measures the infinite-frequency value of the sound

Paris-Sud XI, Université de

232

ccsd00000736 Electron correlation e ects on the dielectric function of liquid metals  

E-Print Network [OSTI]

metals, since the speed of sound in these systems is related to the screening action of the electrons between the ions, the speed of sound, c, can be expressed as: c = pi Q p #15;(Q) : (1) Here Q is the wave of liquid metals P. Giura 1 , R. Angelini 1 , C. A. Burns 2 , G. Monaco 1 and F. Sette 1 . 1 European

233

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

234

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

235

Nonlinear Landau damping and formation of Bernstein-Greene-Kruskal structures for plasmas with q-nonextensive velocity distributions  

SciTech Connect (OSTI)

In the past, long-time evolution of an initial perturbation in collisionless Maxwellian plasma (q = 1) has been simulated numerically. The controversy over the nonlinear fate of such electrostatic perturbations was resolved by Manfredi [Phys. Rev. Lett. 79, 2815-2818 (1997)] using long-time simulations up to t=1600{omega}{sub p}{sup -1}. The oscillations were found to continue indefinitely leading to Bernstein-Greene-Kruskal (BGK)-like phase-space vortices (from here on referred as 'BGK structures'). Using a newly developed, high resolution 1D Vlasov-Poisson solver based on piecewise-parabolic method (PPM) advection scheme, we investigate the nonlinear Landau damping in 1D plasma described by toy q-distributions for long times, up to t=3000{omega}{sub p}{sup -1}. We show that BGK structures are found only for a certain range of q-values around q = 1. Beyond this window, for the generic parameters, no BGK structures were observed. We observe that for values of q<1 where velocity distributions have long tails, strong Landau damping inhibits the formation of BGK structures. On the other hand, for q>1 where distribution has a sharp fall in velocity, the formation of BGK structures is rendered difficult due to high wave number damping imposed by the steep velocity profile, which had not been previously reported. Wherever relevant, we compare our results with past work.

Raghunathan, M. [Indian Institute of Science Education and Research (IISER), Pune 411021 (India); Ganesh, R. [Institute for Plasma Research, Gandhinagar 382428 (India)

2013-03-15T23:59:59.000Z

236

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

237

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

238

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

239

Compactness of the ? ? -Neumann Operator on the Intersection Domains in ?^(N)  

E-Print Network [OSTI]

) domains satisfies McNeal's property ( P ?). More precisely, let ?_(1) and ?_(2) be bounded (not necessarily smooth) pseudoconvex domains in ?^(n) which intersect each other in a domain ?. If the ? ?-Neumann operators N_(q)^(?_(1)) and N_(q)^(?_(2...

Ayyuru, Mustafa

2014-07-10T23:59:59.000Z

240

Baryonic torii: Toroidal baryons in a generalized Skyrme model  

E-Print Network [OSTI]

We study a Skyrme-type model with a potential term motivated by Bose-Einstein condensates (BECs), which we call the BEC Skyrme model. We consider two flavors of the model, the first is the Skyrme model and the second has a sixth-order derivative term instead of the Skyrme term; both with the added BEC-motivated potential. The model contains toroidally shaped Skyrmions and they are characterized by two integers P and Q, representing the winding numbers of two complex scalar fields along the toroidal and poloidal cycles of the torus, respectively. The baryon number is B=PQ. We find stable Skyrmion solutions for P=1,2,3,4,5 with Q=1, while for P=6 and Q=1 it is only metastable. We further find that configurations with higher Q>1 are all unstable and split into Q configurations with Q=1. Finally we discover a phase transition, possibly of first order, in the mass parameter of the potential under study.

Sven Bjarke Gudnason; Muneto Nitta

2015-02-10T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q1" 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

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

242

Constant power speed range extension of surface mounted PM motors  

DOE Patents [OSTI]

A circuit and method for controlling a rotating machine (11) in the constant horsepower range above base speed uses an inverter (15) having SCR's (T1-T6) connected in series with the primary commutation switches (Q1-Q6) to control turn off of the primary commutation switches and to protect the primary commutation switches from faults. The primary commutation switches (Q1-Q6) are controlled by a controller (14), to fire in advance or after a time when the back emf equals the applied voltage, and then to turn off after a precise dwell time, such that suitable power is developed at speeds up to at least six times base speed.

Lawler, Jack Steward (Knoxville, TN); Bailey, John Milton (Knoxville, TN)

2001-01-01T23:59:59.000Z

243

Downstream hydraulic geometry relations: 2. Calibration and testing  

E-Print Network [OSTI]

, whereas h h is dependent on r. The three parameters, h B , h h , and h n , are defined, respectively, as: h B ? 0:5 S 0:069 Q 0:138 ?33? h n ? 0:5 S 0:269 Q 0:538 ?34? h h ? 0:5 S 1 21?r?? C00:231 Q 1 1?r C00:462 ?35? If h B * ? h B Q 0:138 S 0:069 ?36? h... n * ? h n Q 0:538 S 0:269 ?37? h h * ? h h Q 1 1?r C00:462 S 1 21?r?? C00:231 ?38? then h B* , h h* , and h n* assume a constant value of 0.5. A comparison between equations (36) to (38) and the database A consisting of 277 sets of data is shown...

Singh, Vijay P.; Yang, Chih Ted; Deng, Zhi-Qiang

2003-12-04T23:59:59.000Z

244

Impacts of Openness  

E-Print Network [OSTI]

Q1 100W – 90W N=34 Q2 90W – 80W N=50 Q3 80W – 70W N=35 40N – 48N Lat N=weather stations • Four Periods P1: 1-10 May P2 : 11-20 May P3 : 21-30 May P4 : 31 May -9 June Regions for first monarch sightings analysis Q1 Q2 Q3 First sightings and # 70...Authorities ID person of interest as Saudi national in marathon bombings, under guard at Boston hospital • By Post Staff Report • April 15, 2013 | 8:28pm • Photo: AP • Police clear the area at the finish line of the 2013 Boston Marathon. Balanced...

Peterson, A. Townsend; Lee, Steven W.; Keel, William; DeSarle, Matthew; Witczak, Andi; Taylor, Orley R.; Dandridge, Deborah; Thiel, Sarah Goodwin; Shulenburger, David E.

2013-10-25T23:59:59.000Z

245

A New Blackbody Radiation Law Based on Fractional Calculus and its Application to NASA COBE Data  

E-Print Network [OSTI]

By applying fractional calculus to the equation proposed by M. Planck in 1900, we obtain a new blackbody radiation law described by a Mittag-Leffler (ML) function. We have analyzed NASA COBE data by means of a non-extensive formula with a parameter $(q-1)$, a formula proposed by Ertik et al. with a fractional parameter $(\\alpha-1)$, and our new formula including a parameter $(p-1)$, as well as the Bose-Einstein distribution with a dimensionless chemical potential $\\mu$. It can be said that one role of the fractional parameter $(p-1)$ is almost the same as that of chemical potential $(\\mu)$ as well as that of the parameter $(q-1)$ in the non-extensive approach.

Biyajima, Minoru; Suzuki, Naomichi

2015-01-01T23:59:59.000Z

246

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

247

Time series analysis, 2013, PC 8 | ARCH and GARCH processes 9 8 ARCH and GARCH processes  

E-Print Network [OSTI]

Time series analysis, 2013, PC 8 | ARCH and GARCH processes 9 8 ARCH and GARCH processes A GARCH(q) process. Exercise 8.2 (Computation of the kurtosis of a conditionally Gaussian GARCH(1, 1) pro- cess that = 3 + 3 Var(E[X2 t | Gt 1]) (E[X2 t ])2 . 3. For a GARCH(1,1) process, with p = q = 1 and a, b = b1, c

Gaïffas, Stéphane

248

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

249

Revista Brasileira de Ensino de Fisica, v. 27, n. 1, p. 103 -107, (2005) www.sbfisica.org.br  

E-Print Network [OSTI]

fun¸c~ao energia1 . Seja ainda J(t, q1 . . . ql, 1 . . . l) uma integral completa da equa~ao Carlos, SP, Brasil. Revis~ao t´ecnica de Marcus A.M. de Aguiar. Instituto de F´isica "Gleb Wataghin", Universidade Estadual de Campinas, Campinas, SP, Brasil. 1Pois tem-se neste caso dH dt = i H qi . qi + i H pi

de Aguiar, Marcus A. M.

250

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

251

Physical Constants k = 1/4 0 = 8.988 GNm2  

E-Print Network [OSTI]

/second 1 = 1 V/A = 1 ohm = 1 J·s/C2 1 T = 1 N/A·m = 1 tesla = 1 newton/ampere·meter 1 G = 10-4 T = 1 gauss = 10-4 tesla Chapter 16 Equations Charges: Q = ±Ne, Q1 + Q2 = 0, e = 1.602 � 10-19 C. Electric Force: F generator) V - E = IR (motor's counter-emf) E1 = -M I2 t (mutua

Wysin, Gary

252

On-Bill Repayment: A Proposal to Increase Investment in Texas  

E-Print Network [OSTI]

be adequately compensated for services - Fees from lenders/investors for REPs - Credit for energy savings for TDUs 3 OBR OFFERS FLEXIBILITY ? Retrofits ? Renewables / CHP ? Energy Star Appliances A well-designed OBR program maximizes... for public comment on October 2, 2012 ? Expected to be operational Q1 2013 ? EDF will pursue legislation in 2013 to create OBR programs for residential and commercial properties in Texas, Ohio and North Carolina ? Potential Pilot Projects...

Copithorne, B.

2012-01-01T23:59:59.000Z

253

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

254

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. Biró; G. G. Barnaföldi; P. Ván; K. Ürmössy

2014-04-04T23:59:59.000Z

255

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

256

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

257

On the FermatWeber Center of a Convex Object Paz Carmi # Sariel HarPeled + Matthew J. Katz #  

E-Print Network [OSTI]

On the Fermat­Weber Center of a Convex Object Paz Carmi # Sariel Har­Peled + Matthew J. Katz # May the Fermat­Weber center of Q to the points in Q is at least #(P )/7, where #(P ) is the diameter of P­time approximation scheme for finding an approximate Fermat­Weber center of a convex polygon Q. 1 Introduction

Har-Peled, Sariel

258

On the FermatWeber Center of a Convex Object Paz Carmi # Sariel HarPeled + Matthew J. Katz #  

E-Print Network [OSTI]

On the Fermat­Weber Center of a Convex Object Paz Carmi # Sariel Har­Peled + Matthew J. Katz the Fermat­Weber center of Q to the points in Q is at least #(Q)/7, where #(Q) is the diameter of Q­time approximation scheme for finding an approximate Fermat­Weber center of a convex polygon Q. 1 Introduction

Katz, Matthew "Matya"

259

Exercise Session 1 (with Solutions) Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 1 (with Solutions) Alessandro Abate a.abate@tudelft.nl Pawel Stano p ­ Exercise Session 1 ­ sc4026 #12;A. Abate, P. Stano State-Space Model Consider the third-order model d3q dt32 + 4x1 = u, y = x1. ­ Ac.Yr. 2011/12, 1e Sem. Q1 ­ Exercise Session 1 ­ sc4026 1 #12;A. Abate, P

Abate, Alessandro

260

Exercise Session 6 (with solutions) Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 6 (with solutions) Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a Session 6 ­ sc4026 #12;A. Abate, A. Haber Linear Quadratic Regulator, in Theory Consider an object of mass ­ Ac.Yr. 2011/12, 1e Sem. Q1 ­ Exercise Session 6 ­ sc4026 1 #12;A. Abate, A. Haber it can be easily

Abate, Alessandro

Note: This page contains sample records for the topic "q4 q1 q1" 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

Exercise Session 1 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 1 Alessandro Abate a.abate@tudelft.nl Pawel Stano p ­ Exercise Session 1 ­ sc4026 #12;A. Abate, P. Stano State-Space Model Consider the third-order model d3q dt3. Simulate the model with Matlab. ­ Ac.Yr. 2011/12, 1e Sem. Q1 ­ Exercise Session 1 ­ sc4026 1 #12;A. Abate

Abate, Alessandro

262

Exercise Session 1 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 1 Alessandro Abate a.abate@tudelft.nl Jacopo Antonello j ­ Exercise Session 1 ­ sc4026 #12;A. Abate, J. Antonello State-Space Model Consider the third-order model d3q. Simulate the model with Matlab. ­ Ac.Yr. 2012/13, 1e Sem. Q1 ­ Exercise Session 1 ­ sc4026 1 #12;A. Abate

Abate, Alessandro

263

Exercise Session 1 Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 1 Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a Session 1 ­ sc4026 #12;A. Abate, A. Haber State-Space Model Consider the third-order model d3q dt3 + 2 d2q the model with Matlab. ­ Ac.Yr. 2010/11, 1e Sem. Q1 ­ Exercise Session 1 ­ sc4026 1 #12;A. Abate, A. Haber

Abate, Alessandro

264

Exercise Session 4 (with solutions) Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 4 (with solutions) Alessandro Abate a.abate@tudelft.nl Aleksandar Haber a Session 4­ sc4026 #12;A. Abate, A. Haber Lyapunov Stability Consider the planar system x = Ax = -2 0 0 -2 = 1 4(x2 1 + x2 2). 2 ­ Ac.Yr. 2011/12, 1e Sem. Q1 ­ Exercise Session 4­ sc4026 1 #12;A. Abate, A

Abate, Alessandro

265

Exercise Session 1 (with Solutions) Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 1 (with Solutions) Alessandro Abate a.abate@tudelft.nl Jacopo Antonello j ­ Exercise Session 1 ­ sc4026 #12;A. Abate, J. Antonello State-Space Model Consider the third-order model d3q2 + 4x1 = u, y = x1. ­ Ac.Yr. 2012/13, 1e Sem. Q1 ­ Exercise Session 1 ­ sc4026 1 #12;A. Abate, J

Abate, Alessandro

266

Exercise Session 4 (with solutions) Alessandro Abate  

E-Print Network [OSTI]

sc4026 Exercise Session 4 (with solutions) Alessandro Abate a.abate@tudelft.nl Jacopo Antonello j Session 4­ sc4026 #12;A. Abate, J. Antonello Lyapunov Stability Consider the planar system x = Ax = -2 0 0 = 1 4(x2 1 + x2 2). 2 ­ Ac.Yr. 2012/13, 1e Sem. Q1 ­ Exercise Session 4­ sc4026 1 #12;A. Abate, J

Abate, Alessandro

267

ISOPERIMETRIC CONSTANT OF A k-REGULAR GRAPH (A NOTE ON A THEOREM OF  

E-Print Network [OSTI]

ISOPERIMETRIC CONSTANT OF A k-REGULAR GRAPH (A NOTE ON A THEOREM OF BIGGS, MOHAR, AND SHAWE.2 in the paper [BMS] of Biggs, Mohar, and Shawe-Taylor we have instead of (1) and (2): i #21; 4(1 #26;) , #26 that #26; #20; q 1 i 2 k 2 . References BMS. N. Biggs, B. Mohar, J. Shawe-Taylor, The spectral radius of in

Smirnova-Nagnibeda, Tatiana

268

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.

269

PT-invariant one-dimensional Coulomb problem  

E-Print Network [OSTI]

The one-dimensional Coulomb-like potential with a real coupling constant beta, and a centrifugal-like core of strength G = alpha^2 - {1/4}, viz. V(x) = {alpha^2 - (1/4)}/{(x-ic)^2} + beta/|x-ic|, is discussed in the framework of PT-symmetry. The PT-invariant exactly solvable model so formed, is found to admit a double set of real and discrete energies, numbered by a quasi-parity q = +/- 1.

Anjana Sinha; Rajkumar Roychoudhury

2002-07-23T23:59:59.000Z

270

Generalized Bhattacharyya and Chernoff upper bounds on Bayes error using quasi-arithmetic means  

E-Print Network [OSTI]

1 = w1(c11 + c21) and a2 = w2(c12 + c22). The identity simplifies for probability of error Pe to Pe to the total variation met- ric distance TV(p, q) = 1 2 |p(x) - q(x)|dx by Be = a1+a2 2 - TV(a1p1, a2p2) with a

Nielsen, Frank

271

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

272

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

273

ROOT LOCUS TECHNIQUE 323 7.6.1 Hydro Power Plant Experiment  

E-Print Network [OSTI]

ROOT LOCUS TECHNIQUE 323 7.6.1 Hydro Power Plant Experiment The design of a static controller for a real hydro power plant is considered in Skatariâ?? c and Gajiâ?? c (1992). The hydro power plant is treated variables of this hydro power plant are represented by x T = [1` 1! 1u f 1/ d 1/ q 1/ f 1/D 1/Q ] where 1

Gajic, Zoran

274

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 Fund’s 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

275

A critical review of methods used in the estimation of natural gas reserves  

E-Print Network [OSTI]

greater than the recovery factor for oQ. 1a order to make an accurate determination of tbe recovery factor, it is accessary to predetermine the pressure history of the field by material-balance and water-iaQun calculations, or by extrapolating a curve...) past produc- tion compared with (a) rock-pressure decline, (b) capacity dsclhce. aad (c) liae delivery decline; (N) productioa curve where yrodactloa has besa maabaum and coatrolliag conditions uniform. (4) cocnparisea with per- formaace recorcis...

Gruy, Henry Jones

1956-01-01T23:59:59.000Z

276

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.

277

Geometric aspects of the non-extensive statistical theory  

SciTech Connect (OSTI)

The family of Tsallis entropies was introduced by Tsallis in 1988. The Shannon entropy belongs to this family as the limit case q{yields}1. The canonical distributions in R{sup n} that maximize this entropy under a covariance constraint are easily derived as Student-t (q<1) and Student-r (q>1) multivariate distributions. A nice geometrical result about these Student-r distributions is that they are marginal of uniform distributions on a sphere of larger dimension d with the relationship p = n+2+(2/q-1). As q{yields}1, we recover the famous Poincare's observation according to which a Gaussian vector can be viewed as the projection of a vector uniformly distributed on the infinite dimensional sphere. A related property in the case q<1 is also available. Often associated to Renyi-Tsallis entropies is the notion of escort distributions. We provide here a geometric interpretation of these distributions. Another result concerns a universal system in physics, the harmonic oscillator: in the usual quantum context, the waveform of the n-th state of the harmonic oscillator is a Gaussian waveform multiplied by the degree n Hermite polynomial. We show, starting from recent results by Carinena et al., that the quantum harmonic oscillator on spaces with constant curvature is described by maximal Tsallis entropy waveforms multiplied by the extended Hermite polynomials derived from this measure. This gives a neat interpretation of the non-extensive parameter q in terms of the curvature of the space the oscillator evolves on; as q{yields}1, the curvature of the space goes to 0 and we recover the classical harmonic oscillator in R{sup 3}.

Vignat, C. [Universite Paris-Est, LIGM, Universite de Marne la Vallee (France); Bercher, J.-F. [Universite Paris-Est, LIGM, ESIEE, 5 bd Descartes, 77454 Marne-la-Vallee Cedex 2 (France)

2009-12-08T23:59:59.000Z

278

A new localization mechanism and Hodge duality for $q-$form field  

E-Print Network [OSTI]

In this paper, through a general Kaluza-Klein decomposition we investigate a new localization mechanism for a massless $q-$form field on the $p-$brane world with codimension one. We obtain two Schr\\"{o}dinger-like equations for the Kaluza-Klein (KK) modes, from which we can find the mass spectra of the KK modes and analyze their characters. It is found that there are two types of massless KK modes, a massless $q-$form KK mode and a massless $(q-1)-$form one, which cannot be localized on the brane at the same time. Because of this the Hodge duality on the brane can be naturally satisfied, which indicates a duality between a localized massless $q-$form mode and a $(p-q-1)-$form one. While if there exist some bound massive KK modes, they will couple with a massless $(q-1)-$form mode with different coupling constants, and so does the bulk $(p-q)-$form field. In this case the effective $q-$form field is still dual to the $(p-q)-$form one, just as in the bulk, although the mass spectra of the KK modes for both fields are not the same.

Chun-E Fu; Yu-Xiao Liu; Heng Guo; Sheng-Li Zhang

2015-02-19T23:59:59.000Z

279

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 Eastman’s 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 DOE’s 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

280

Electric Fields and Chiral Magnetic Effect in Cu + Au Collisions  

E-Print Network [OSTI]

The non-central Cu + Au collisions can create strong out-of-plane magnetic fields and in-plane electric fields. By using the HIJING model, we study the general properties of the electromagnetic fields in Cu + Au collisions at 200 GeV and their impacts on the charge-dependent two-particle correlator $\\gamma_{q_1q_2}=$ (see main text for definition) which was used for the detection of the chiral magnetic effect (CME). Compared with Au + Au collisions, we find that the in-plane electric fields in Cu + Au collisions can strongly suppress the two-particle correlator or even reverse its sign if the lifetime of the electric fields is long. Combining with the expectation that if $\\gamma_{q_1q_2}$ is induced by elliptic-flow driven effects we would not see such strong suppression or reversion, our results suggest to use Cu + Au collisions to test CME and understand the mechanisms that underlie $\\gamma_{q_1q_2}$.

Wei-Tian Deng; Xu-Guang Huang

2015-02-16T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q1" 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

3Q/4Q00 Annual M-Area and Metallurgical Laboratory Hazardous Waste Management Facilities Groundwater Monitoring and Corrective-Action Report - Third and Fourth Quarters 2000 - Volumes I, II, and II  

SciTech Connect (OSTI)

This report describes the groundwater monitoring and corrective-action program at the M-Area Hazardous Waste Management Facility (HWMF) and the Metallurgical Laboratory (Met Lab) HWMF at the Savannah River Site (SRS) during 2000. This program is required by South Carolina Resource Conservation and Recovery Act (RCRA) Hazardous Waste Permit SC1890008989 and Section 264.100(g) of the South Carolina Hazardous Waste Management Regulations.

Cole, C.M. Sr.

2001-04-17T23:59:59.000Z

282

The effect of periodic unsteady wakes on boundary layer transition and heat transfer on a curved plate  

E-Print Network [OSTI]

generator cross section looking upstream: l. Upper wall, 2. Lower wall, 3. Side wall, 4 Timing belt pulley, 5. Rotating disk, 6. 2. 0 mm diameter cylindrical rod. Test Section: 1. Traversing system, 2. Nozzle, 3. Wake generator, 4. Electric motor, 5...-dimensional mean velocity at different s/s. locations on the heat transfer plate for 0= 0. 0 (0 rods). 39 41 43 Figure 13. Figure 14. Figure 15. Figure 16. Non-dimensional mean velocity at different s/s, locations on the heat transfer plate for Q= 1. 033...

Wright, Lance Cole

1996-01-01T23:59:59.000Z

283

University Downtown Center 67 Washington St., Binghamton  

E-Print Network [OSTI]

METERED PARKING Lot M2 Lot F3 LotH LotH LotI Lot F Lot G LotC Lot F1 Lot J LotJ1 LotJ2 LotJ3 Lot E1 Lot E Lot T LotO1 LotV Lot Q2 Lot 02 Lot Q1 Lot W Lot Y1 Lot R METERED PARKING METERED PARKING METERED Admissions Center Smart Energy Research and Development Facility Innovative Technologies Complex Innovative

Cho, Junghyun

284

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

285

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

286

Physical Constants k = 1/4 0 = 8.988 GNm2  

E-Print Network [OSTI]

/s = 1 ampere = 1 coulomb/second 1 = 1 V/A = 1 ohm = 1 J·s/C2 1 T = 1 N/A·m = 1 tesla = 1 newton/ampere·meter 1 G = 10-4 T = 1 gauss = 10-4 tesla Chapter 16 Equations Charges: Q = ±Ne, Q1 + Q2 = 0, e = 1 generator) V - E = IR (motor's counter-emf) E1 = -M I2 t (mutual inductance emf) VS/VP = NS/NP (transformer

Wysin, Gary

287

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

288

Random matrix theory for mixed regular-chaotic dynamics in the super-extensive regime  

SciTech Connect (OSTI)

We apply Tsallis's q-indexed nonextensive entropy to formulate a random matrix theory (RMT), which may be suitable for systems with mixed regular-chaotic dynamics. We consider the super-extensive regime of q<1. We obtain analytical expressions for the level-spacing distributions, which are strictly valid for 2 X2 random-matrix ensembles, as usually done in the standard RMT. We compare the results with spacing distributions, numerically calculated for random matrix ensembles describing a harmonic oscillator perturbed by Gaussian orthogonal and unitary ensembles.

El-Hady, A. Abd [Department of Physics, King Khalid University, Abha (Saudi Arabia); Department of Physics, Zagazig University, Zagazig (Egypt); Abul-Magd, A. Y. [Department of Mathematics, Zagazig University, Zagazig (Egypt); Faculty of Engineering Sciences, Sinai University, El-Arish (Egypt)

2011-10-27T23:59:59.000Z

289

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

290

Mexican border: an economic alternative for a meatpacking plant  

E-Print Network [OSTI]

be used to produce a given level of output. Figure 3 shows the combination of capital and labor and the Capital US k K 1 MX k K 2 0 L US 1 L Isoquant (output) L MX Labor 2 L Figure 3. Isoquant Map resulting substitution possibilities among... are increasingly demanding, and which require meticulous labor that machines are not able to perform. Figure 6 describes this situation. As was shown, to produce Q, output Capital K 1 K 0 Q 1 I I I Q Q USI 0 I I I Q MX 1 LUSL L US' L 0 L 1 2 L 3...

Chapa-Dominiguez, Hervey

1989-01-01T23:59:59.000Z

291

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

292

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

293

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

294

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

295

NGC2613, 3198, 6503, 7184: Case studies against `maximum' disks  

E-Print Network [OSTI]

Decompositions of the rotation curves of NGC2613, 3198, 6505, and 7184 are analysed. For these galaxies the radial velocity dispersions of the stars have been measured and their morphology is clearly discernible. If the parameters of the decompositions are chosen according to the `maximum' disk hypothesis, the Toomre Q stability parameter is systematically less than one and the multiplicities of the spiral arms as expected from density wave theory are inconsitent with the observed morphologies of the galaxies. The apparent Q<1 instability, in particular, is a strong argument against the `maximum' disk hypothesis.

B. Fuchs

1998-12-02T23:59:59.000Z

296

Update of MRST parton distributions.  

E-Print Network [OSTI]

knowledge of the partonic structure of the proton is an essential ingredient in the analysis of hard scattering data from pp or pŻp or ep high energy collisions. Much at- tention has recently been devoted to obtaining reliable uncertainties on the parton... photons than dnV (x) quarks. To a rough approximation, the photon distribution should be ?(x,Q2) = ? j e2j ? 2pi ln(Q2/m2q) ? 1 x dy y P?q(y) qj( x y ,Q2). So there is more photon momentum in the proton than in the neutron due to high-x up quarks radiating...

Thorne, Robert S; Martin, A D; Stirling, W James; Roberts, R G

297

From $sl_q(2)$ to a parabosonic Hopf algebra  

E-Print Network [OSTI]

A Hopf algebra with four generators among which an involution (reflection) operator, is introduced. The defining relations involve commutators and anticommutators. The discrete series representations are developed. Designated by $sl_{-1}(2)$, this algebra encompasses the Lie superalgebra $osp(1|2)$. It is obtained as a $q=-1$ limit of the $sl_q(2)$ algebra and seen to be equivalent to the parabosonic oscillator algebra in irreducible representations. It possesses a noncocommutative coproduct. The Clebsch-Gordan coefficients (CGC) of $sl_{-1}(2)$ are obtained and expressed in terms of the dual -1 Hahn polynomials. A generating function for the CGC is derived using a Bargmann realization.

Tsujimoto, Satoshi; Zhedanov, Alexei

2011-01-01T23:59:59.000Z

298

From $sl_q(2)$ to a Parabosonic Hopf Algebra  

E-Print Network [OSTI]

A Hopf algebra with four generators among which an involution (reflection) operator, is introduced. The defining relations involve commutators and anticommutators. The discrete series representations are developed. Designated by $sl_{-1}(2)$, this algebra encompasses the Lie superalgebra $osp(1|2)$. It is obtained as a $q=-1$ limit of the $sl_q(2)$ algebra and seen to be equivalent to the parabosonic oscillator algebra in irreducible representations. It possesses a noncocommutative coproduct. The Clebsch-Gordan coefficients (CGC) of $sl_{-1}(2)$ are obtained and expressed in terms of the dual -1 Hahn polynomials. A generating function for the CGC is derived using a Bargmann realization.

Satoshi Tsujimoto; Luc Vinet; Alexei Zhedanov

2011-10-07T23:59:59.000Z

299

Heating Oil and Propane Update  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May JunDatastreamsmmcrcalgovInstrumentsruc DocumentationP-SeriesFlickr FlickrGuidedCH2M HILL SecretaryHazmat workFAQs for Respondents Q1:

300

Occupational Safety Performance  

Office of Environmental Management (EM)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "of EnergyEnergyENERGY TAXBalanced ScorecardReactor TechnologyOFFICE: I Oak Ridge,8 8EnergyQ1 2012 rates

Note: This page contains sample records for the topic "q4 q1 q1" 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

Occurrence Reporting Causal Analysis  

Office of Environmental Management (EM)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "of EnergyEnergyENERGY TAXBalanced ScorecardReactor TechnologyOFFICE: I Oak Ridge,8 8EnergyQ1 2012 rates

302

Occurrence Reporting Trends | Department of Energy  

Office of Environmental Management (EM)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "of EnergyEnergyENERGY TAXBalanced ScorecardReactor TechnologyOFFICE: I Oak Ridge,8 8EnergyQ1 2012

303

Ocean Thermal Extractable Energy Visualization: Final Technical Report |  

Office of Environmental Management (EM)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "of EnergyEnergyENERGY TAXBalanced ScorecardReactor TechnologyOFFICE: I Oak Ridge,8 8EnergyQ1

304

Oct 2009 final concurrence letter for BPA | Department of Energy  

Office of Environmental Management (EM)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "of EnergyEnergyENERGY TAXBalanced ScorecardReactor TechnologyOFFICE: I Oak Ridge,8 8EnergyQ1Oct 2009

305

October 12, 2011 SEAB Agenda | Department of Energy  

Office of Environmental Management (EM)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "of EnergyEnergyENERGY TAXBalanced ScorecardReactor TechnologyOFFICE: I Oak Ridge,8 8EnergyQ1OctOctober

306

October 2011 Energy Assurance Planning Bulletin Volume 2 No 4  

Office of Environmental Management (EM)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) "of EnergyEnergyENERGY TAXBalanced ScorecardReactor TechnologyOFFICE: I Oak Ridge,8 8EnergyQ1OctOctober3,

307

3dtab.xlsx  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May JunDatastreamsmmcrcalgovInstrumentsrucLasDelivered‰PNGExperience hands-onASTROPHYSICS H.CarbonMarch Value4 3.P D ATFOR M AlgeriaQ1

308

EIA - Natural Gas Pipeline Network - Depleted Reservoir Storage  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data CenterFranconia,(Million Barrels) Crude Oil Reserves in Nonproducing Reservoirs U.S. Department of EnergyD e s c r iQ1Configuration

309

Geomorphic Equations and Methods for Natural Channel Design  

E-Print Network [OSTI]

significant predictors of the Q1.2. This led to Equation 2.2: 1.26 3.17 1.101.2Q 0.00258 CDA MAP L?? (2.2) Sy bol Watershed Characteristic Units DA Contributing Drainage Area mi 2 Sh Basin Shape Factor -- Sl Average Slope of Main Channel ft/mi SP........................................................................................... 97 6.4 BSCR by Grain Size .............................................................................................................. 98 vi List of Figures 1.1 A restored chute on the Missouri River in Saline, MO...

Shelley, John Edwin

2012-05-31T23:59:59.000Z

310

PTG exam 2322011 short answers 75. For this cyclic process: 0dUQW  

E-Print Network [OSTI]

. 35 bar, 0 °C gas density = MCH4p/RT = 24,7 kg/m3 volume flow = 201,6 / 24,7 = 8,18 m3 /sPTG exam 2322011 ­ short answers 75. For this cyclic process: 0dUQW a. Q1 + W2 + Q2 = 10000 MJ/s 10000 MJ/s / 35,4 MJ/m3 n = 282,5 m3 n /s; ideal gas: n/V =p/RT 1 m3 n = 101300 / 8

Zevenhoven, Ron

311

FAL2001-03.pdf | Department of Energy  

Energy Savers [EERE]

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on Office of Inspector General Office of Audit|Department of Energy56Executive212-2012 June;' F=Q ~1-03.pdf

312

Requirements and Design Envelope for Volumetric Neutron Source Fusion Facilities for Fusion Nuclear Technology Development  

SciTech Connect (OSTI)

The paper shows that timely development of fusion nuclear technology (FNT) components, e.g. blanket, for DEMO requires the construction and operation of a fusion facility parallel to ITER. This facility, called VNS, will be dedicated to testing, developing and qualifying FNT components and material combinations. Without VNS, i.e. with ITER alone, the confidence level in achieving DEMO operating goals has been quantified and is unacceptably low (< 1 %). An attractive design envelope for VNS exists. Tokamak VNS designs with driven plasma (Q ~ 1-3), steady state plasma operation and normal copper toroidal field coils lead to small sized devices with moderate cost.

Abdou, M [University of California, Los Angeles] [University of California, Los Angeles; Peng, Yueng Kay Martin [ORNL] [ORNL

1995-01-01T23:59:59.000Z

313

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

314

Thermalization in collisions of large nuclei at high energies  

E-Print Network [OSTI]

Hydrodynamical analysis of experimental data of ultrarelativistic heavy ion collisions seems to indicate that the hot QCD matter created in the collisions thermalizes very quickly. Theoretically, we have no idea why this should be true. In this proceeding, I will describe how the thermalization takes place in the most theoretically clean limit -- that of large nuclei at asymptotically high energy per nucleon, where the system is described by weak-coupling QCD. In this limit, plasma instabilities dominate the dynamics from immediately after the collision until well after the plasma becomes nearly in equilibrium at time t \\alpha^(-5/2)Q^(-1).

Aleksi Kurkela

2013-03-19T23:59:59.000Z

315

Charge dependent relation between the masses of different generations and Neutrino masses  

E-Print Network [OSTI]

Despite the enormous achievements, the Standard model of Particle physics can not be consider as complete theory of fundamental interactions. Among other things, it can not describe the gravitational interaction and it depends on 19 parameters. The Standard model includes 12 fermions (matter elementary particles with spin $\\frac{1}{2}$) which are divided in three generations, groups with same interactions but different masses. Each generation can be classified into two leptons (with electric charges $Q=-1$, electron-like and $Q=0$, neutrino) and two quarks (with electric charges $Q=-\\frac{1}{3}$, down-type and $Q=\\frac{2}{3}$, up-type). However, the understanding of the relationship between generations and ratio of masses of different generations are unknown. Here we show that there exists the simple relation between masses of different generations which depend only on the electric charges for $Q=-1,\\, \\, Q=-\\frac{1}{3}$ and $Q=\\frac{2}{3}$. It is in pretty good agreement with experimental data. Assuming that...

Sazdovic, Branislav

2015-01-01T23:59:59.000Z

316

Charge dependent relation between the masses of different generations and Neutrino masses  

E-Print Network [OSTI]

Despite the enormous achievements, the Standard model of Particle physics can not be consider as complete theory of fundamental interactions. Among other things, it can not describe the gravitational interaction and it depends on 19 parameters. The Standard model includes 12 fermions (matter elementary particles with spin $\\frac{1}{2}$) which are divided in three generations, groups with same interactions but different masses. Each generation can be classified into two leptons (with electric charges $Q=-1$, electron-like and $Q=0$, neutrino) and two quarks (with electric charges $Q=-\\frac{1}{3}$, down-type and $Q=\\frac{2}{3}$, up-type). However, the understanding of the relationship between generations and ratio of masses of different generations are unknown. Here we show that there exists the simple relation between masses of different generations which depend only on the electric charges for $Q=-1,\\, \\, Q=-\\frac{1}{3}$ and $Q=\\frac{2}{3}$. It is in pretty good agreement with experimental data. Assuming that the same relation valid for $Q=0$, we are able to calculate neutrino masses. Therefore, our results could pave the way for further investigations beyond Standard model.

Branislav Sazdovic

2015-01-29T23:59:59.000Z

317

Interconnection Effects and W+W- Decays (a critical (p)(re)view)  

E-Print Network [OSTI]

Color reconnection and Bose-Einstein correlations not only can have an influence on the measurement of the W-mass in the fully hadronic W+W- decay channel at LEP2, but also can give essential information on the structure of the QCD vacuum and the space-time development of a q_1\\bar q_2 system. Recent developments are critically analyzed, with particular emphasis on the models used in this field. More sensitive variables are needed to distinguish between color reconnection models, while more experimental knowledge has to be built into the Bose-Einstein models and, above all, these two closely related phenomena have to be treated in common. Both effects are determined by the space-time overlap of the W+ and W- decay products. Vital experimental information on the space-time development of the decay of the q_1\\bar q_2 system is becoming available from the high-statistics data on hadronic Z decay and models will have to be able to explain this evidence before being used to predict interference effects in hadronic W+W- decay.

Wolfram Kittel

1999-06-29T23:59:59.000Z

318

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

SciTech Connect (OSTI)

This report documents trends in U.S. venture capital investments over the period 1980 through the third quarter of calendar year 2010 (2010 Q1+Q2+Q3). Particular attention is given to U.S. venture capital investments in the energy/industrial sector over the period 1980-2010 Q1+Q2+Q3 as well as in the more recently created cross-cutting category of CleanTech over the period 1995-2010 Q1+Q2+Q3. 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 $132 billion (in real 2010 US$) 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 $2.4 billion or slightly more than 13% of all venture capital invested that year. The total venture capital invested in energy/industrial during the first three quarters of 2010 is close to $2.4 billion accounting for slightly less than 15% of all venture capital investments during the first three quarters of 2010. In 2009, the aggregate amount invested in CleanTech was $2.1 billion (11% of the total US venture capital invested in that lean year) and for the first three quarters of 2010 US venture capital investments in CleanTech have already exceeded $2.8 billion (18% of all US venture capital investments made during the first three quarters 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.

2010-11-08T23:59:59.000Z

319

On Fusion Rules in Logarithmic Conformal Field Theories  

E-Print Network [OSTI]

We find the fusion rules for the c_{p,1} series of logarithmic conformal field theories. This completes our attempts to generalize the concept of rationality for conformal field theories to the logarithmic case. A novelty is the appearance of negative fusion coefficients which can be understood in terms of exceptional quantum group representations. The effective fusion rules (i.e. without signs and multiplicities) resemble the BPZ fusion rules for the virtual minimal models with conformal grid given via c = c_{3p,3}. This leads to the conjecture that (almost) all minimal models with c = c_{p,q}, gcd(p,q) > 1, belong to the class of rational logarithmic conformal field theories.

Michael Flohr

1996-06-10T23:59:59.000Z

320

OBSERVATION OF SUPRATHERMAL ELECTRONS DURING MAGNETIC RECONNECTION AT THE SAWTOOTH INSTABILITY IN DIII-D TOKAMAK  

SciTech Connect (OSTI)

OAK A271 OBSERVATION OF SUPRATHERMAL ELECTRONS DURING MAGNETIC RECONNECTION AT THE SAWTOOTH INSTABILITY IN DIII-D TOKAMAK. Intense bursts of x-ray and electron cyclotron emission are observed during sawtooth instabilities in high-temperature plasmas in the DIII-D tokamak. The bursts are initiated around the X-point of the m = 1, n = 1 magnetic island at the beginning of the sawtooth crash and are displaced to larger radii later during the temperature collapse. Reconstruction of the magnetic configuration using motional Stark effect (MSE) data and numerical simulations indicates that the bursts can be connected with suprathermal electrons (E{sub r} {approx} 30-40 keV) generated during reconnection of the magnetic field around the q = 1 surface.

SAVRUKHIN,RV; STRAIT,EJ

2002-11-01T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q1" 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

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

322

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

323

Testing the isotropy of space using rotating quartz oscillators  

E-Print Network [OSTI]

Violations of Lorentz invariance by matter and light can generate direction- and frame-dependent anisotropies in particles inertial masses and, hence, a measurable modulation of the oscillation frequency of rotating quartz crystal oscillators. This allows simple and low maintenance experiments that are ideally suited for long-term data taking. Using the Standard Model Extension (SME) as a parameterizing framework, we study the magnitude of this putative frequency modulation. A preliminary experiment with room-temperature SC-cut crystals yields a frequency resolution in the $10^{-15}$ range with $\\sim 120$ hours of data and a limit of $\\tilde c_Q=(-1.8 \\pm 2.2)\\times 10^{-14}$\\,GeV on the most weakly constrained neutron-sector $c-$coefficient of the SME. Future experiments with cryogenic oscillators promise additional improvements in accuracy, opening up the potential for improved tests of Lorentz symmetry in the neutron, proton, electron and photon sector.

Anthony Lo; Philipp Haslinger; Eli Mizrachi; Loic Anderegg; Holger Müller; Michael Hohensee; Maxim Goryachev; Michael E Tobar

2015-01-28T23:59:59.000Z

324

Reduction of statistical frequency distributions to the Chi Square integral  

E-Print Network [OSTI]

aistrioution with paramete -s ~, -, tnwn / and we can wL r'te P(x;w, P ) = P(x;P, g, m ), 3 w hi=I'i P(x; H, v, g ) M3 I 3 Gl ~" ( ? )-1 2 2 -( ? ) ( ? ') u (~u ?, j 3 3 IJ (2. 15) 11 1 -( ? ) ~2 2 2 (; -1 c = (=) 3 2 e 3 ' ( ? ) ' 2 L Q J (2. lo...). ~ 0 (4. 16) 9 To eval a e -erccn:aqc oo:nts x(c" ' & ). P os& the identity (?. 10) 2 x(c) =:: such ? h t 2q = G(X;v), 2 . . 2 where X =::, v = 1. Tnus /, 2 1 x(c) = g X (2c) 1) 2 (4. 1B) &(c; ?, C ) = u+q'/X (2q;1), c(? (4. 19) 2 where X (q...

Williamson, Morris Leeroy

2012-06-07T23:59:59.000Z

325

Iterative solutions of simultaneous equations  

E-Print Network [OSTI]

functions. (See Ayyendixf pages 29 $6 and 42, for results. ) Also, the sufficient condition for convergence is not satisfied. . Xf the f functions are defined by the method prescribed. on page 14, then 1 2 P = -2 -8 -20 27. g 20 &n' 0. 20128 -0. 0$1...$$ -0. 01661 0. 00&6$ -0. 0/128 9. 00967 9. 1/626 9 ~ 9'$$$6 0. 02008 0, 29128 fl ? 0. 0$1$$ f2 ? 0. 01661 0, 09/6/ fl ? 0, 0/128 f2 + 0. 90967 fy Q ~ 1/626 fl + 0. 09/$6 f2 + 0. 02908 f~ The Jacobi and. Gauss-Seidel methods convexged...

Laycock, Guyron Brantley

2012-06-07T23:59:59.000Z

326

M X(p), p M (Gaussian random field) 1  

E-Print Network [OSTI]

Sn-1 SpM TpSn-1 ( ) NpM = {v TpSn-1 | v, u 0, u SpM} TpSn-1 = SpM NpM q M Sn-1 minpM dist(q, p) p(NpM) ( S(NpM) = NpM Sn-1 ) q M pr(q) M q 2 p, p M pr(q) 1 ( ) M \\ M q q = p cos + v sin , p M, v S(p, v) = sup p M\\{p} v, p 1 - p, p NpM q = p cos + v sin q pr(q) = p p cos + v sin | v

Kuriki, Satoshi

327

MCMC methods for wavelet representations in single index models  

E-Print Network [OSTI]

(Xib) +ei; i =1; : : : ; n; (1.2) where E(yijXi) =r(Xib), Var(yijXi) <Ą, b is a p-column vector of unknown parameters, kbk = 1 and r( ) is an unknown function. The form (1.2) is equivalent to the traditional This dissertation follows the style and format...) =cos(qp) =1, 0 <q1 <2p, and p2

Park, Chun Gun

2004-09-30T23:59:59.000Z

328

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

329

Exotic Ungulate Production: Summary of Survey Results.  

E-Print Network [OSTI]

. 2.74 77 Gourmet restaurants 9.28 4. 10. 1.18 88 Specialty shop 8.48 O. 10. 2.09 85 Health food store 7.83 O. 10. 2.25 81 Mail order catalog 6.77 O. 10. 2.76 83 Overseas 5.61 O. 10. 3.68 77 Others 6.50 O. 10. 3.16 8 1Based on a scale of 0 to 10... of processor 6.65 O. 10. 2.81 89 Price of exotic meat 8.78 O. 1Q. 1.67 88 Development of a market 9.35 5. 10. 1.10 89 Management ability 8.35 O. 10. 2.04 88 Animal welfare activity 6.75 O. 10. 2.87 85 Luck 4.45 O. 10. 3.44 83 Others 7.30 O. 10. 4.00 10...

Mjelde, James W.; Conner, J. Richard; Stuth, Jerry W.; Jensen, James; Chang, Chia-Cheun; Jones, James B.

1992-01-01T23:59:59.000Z

330

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

331

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

332

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

333

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.

334

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

335

An analysis of the flow of heat from tubes buried in a concrete slab  

E-Print Network [OSTI]

T &vhoro dg i. tho amount oi' heat Ilovving in tho ti?e d&v& t!&rou, ", h on area A; n! . &;iotance vlL& owin!. to a to!r&&or?t&no dii'Torence d ~ t. !o . &star:. . I:. a~ing a thor&x~1 conductivity K. . & ncc i'cr con &?ct&& n in tho steady state, t... 12 2 ~ 000 10 1, 5 6, 0 4600 1. 19 4400 1o19 32 3 ~ OPO 1Q 1, 5 4 ~ 0 4200 lo307 3950 lo326 12 4 500 10 lo5 2 67 3300 lo442 3500 1 490 2I 0 TEST III 9 1. 0 36. 0 6450 O. 700 6900 0. 702 0, 312 9 1. 0 20. 0 6250 0, 723 6750 0, 710 o. 437 9 1. 0...

Holdredge, Ernest C

1951-01-01T23:59:59.000Z

336

An investigation of the applicability of the photo-electric cell to the determination of solubility  

E-Print Network [OSTI]

, sad silver chromato solutioas on ths intensity of light. Those 4sts sre represented bp ourvos in Charts II XVc VIy VIXI ~ YARIATIOE OF INTENSITY OF LIGHT WITS TIME FOR VARIOUS CONCl9lTRATIOMS OF SILVER CRLORmE 1. 00 x 10 aols A801 yor Kiter lo80... of RasGrOa mole 9or liter iisf lost isa soalo sivisisas Coassatrat ioa of Na, Cr0, mole psr liter Dsf loot ioa seals divisioas 0. 5 x 10"6 Qed X 10 O Oe9 x 10 0, 8 x10 Oe9x106 leOz105 l. lx106 12xlQ 1. 8 x 10-6 le4 x 10 led z 10 led x...

Nordsieck, Herbert Henry

1936-01-01T23:59:59.000Z

337

Orientation and alignment effects in ion-induced fragmentation of water: A triple coincidence study  

SciTech Connect (OSTI)

The technique of recoil ion momentum spectroscopy is employed to determine the complete momentum vectors for three fragment dissociation channels, [D{sub 2}O]{sup (q+2)} ? (D{sup +} + D{sup +} + O{sup q+}) with q = 1, 2, or 3 formed in collisions of isolated water molecules with 450 keV Xe{sup 9+} ions. The kinetic energy released in each of these dissociation channels is measured and angular correlations between the fragment momenta are determined. From the angular correlations of the three fragment ions with the direction of the incoming beam, a strong anisotropy in the emission of recoil fragments is reported. It is inferred that the molecular plane prefers to lie orthogonal to the incoming beam direction with certain orientations being more preferred than others and a clear signature of non-coplanar dissociation is also observed.

Rajput, Jyoti, E-mail: jyotirajput2803@gmail.com [Department of Physics and Astrophysics, University of Delhi, Delhi 110007 (India); Safvan, C. P. [Inter-University Accelerator Centre, Aruna Asaf Ali Marg, New Delhi 110067 (India)

2014-10-28T23:59:59.000Z

338

Big-Bang Nucleosynthesis verifies classical Maxwell-Boltzmann distribution  

E-Print Network [OSTI]

We provide the most stringent constraint to date on possible deviations from the usually-assumed Maxwell-Boltzmann (MB) velocity distribution for nuclei in the Big-Bang plasma. The impact of non-extensive Tsallis statistics on thermonuclear reaction rates involved in standard models of Big-Bang Nucleosynthesis (BBN) has been investigated. We find that the non-extensive parameter $q$ may deviate by, at most, $|\\delta q|$=6$\\times$10$^{-4}$ from unity for BBN predictions to be consistent with observed primordial abundances; $q$=1 represents the classical Boltzmann-Gibbs statistics. This constraint arises primarily from the {\\em super}sensitivity of endothermic rates on the value of $q$, which is found for the first time. As such, the implications of non-extensive statistics in other astrophysical environments should be explored. This may offer new insight into the nucleosynthesis of heavy elements.

S. Q. Hou; J. J. He; A. Parikh; K. Daid; C. Bertulani

2014-08-15T23:59:59.000Z

339

Fast subcritical assembly construction and use in basic integral data measurements  

E-Print Network [OSTI]

volu. , !e clc!vent of the spine!ical sy:;"iee!, equation (1) ~)' C can be !Eric ten as, P(E=D. O) ( 47Y ) 2 C '!" dr Jp i )E!Ee), 55)J 47)'re e i' dl 0 4!EI )i Q' QE=O. O)[ ? e ? c 'ie! ? ' + 'e 4 e ] '1 1 k! '. ~'he vui be= o f neu iron...FAST Sii SCRIT CAL ASS:. I iHLY COAST;UCTIOii Ar0 oS: l~', nABA I!i T' 4 i b J)A A i'~ ASUnJ i ii!. S A Thesis by i I 0-JI YUAN S!!b!i!ittec1 to tho Gradnate College of the Texas ~Q. 1? University in partial I, !Ifiili!cnt of the reo. !1 re...

Yuan, Liq-Ji

1969-01-01T23:59:59.000Z

340

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

Note: This page contains sample records for the topic "q4 q1 q1" 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.


341

BMW algebra, Quantized coordinate algebra and type C Schur--Weyl duality  

E-Print Network [OSTI]

We prove an integral version of the Schur--Weyl duality between the specialized Birman--Murakami--Wenzl algebra $B_n(-q^{2m+1},q)$ and the quantum algebra associated to the symplectic Lie algebra sp_{2m}. In particular, we deduce that this Schur--Weyl duality holds over arbitrary (commutative) ground rings, which answers a question of Lehrer and Zhang [Strongly multiplicity free modules for Lie algebras and quantum groups, J. Algebra (1) 306 (2006), 138--174] in the symplectic case. As a byproduct, we show that, as $Z[q,q^{-1}]$-algebra, the quantized coordinate algebra defined by Kashiwara is isomorphic to the quantized coordinate algebra arising from a generalized Faddeev--Reshetikhin--Takhtajan's construction.

Hu, Jun

2007-01-01T23:59:59.000Z

342

Safety-factor profile tailoring by improved electron cyclotron system for sawtooth control and reverse shear scenarios in ITER  

SciTech Connect (OSTI)

The effect of the predicted local electron cyclotron current driven by the optimized electron cyclotron system on ITER is discussed. A design variant was recently proposed to enlarge the physics program covered by the upper and equatorial launchers. By extending the functionality range of the upper launcher, significant control capabilities of the sawtooth period can be obtained. The upper launcher improvement still allows enough margin to exceed the requirements for neoclassical tearing mode stabilization, for which it was originally designed. The analysis of the sawtooth control is carried on with the ASTRA transport code, coupled with the threshold model by Por-celli, to study the control capabilities of the improved upper launcher on the sawtooth instability. The simulations take into account the significant stabilizing effect of the fusion alpha particles. The sawtooth period can be increased by a factor of 1.5 with co-ECCD outside the q = 1 surface, and decreased by at least 30% with co-ECCD inside q = 1. The present ITER base-line design has the electron cyclotron launchers providing only co-ECCD. The variant for the equatorial launcher proposes the possibility to drive counter-ECCD with 1 of the 3 rows of mirrors: the counter-ECCD can then be balanced with co-ECCD and provide pure ECH with no net driven current. The difference between full co-ECCD off-axis using all 20MW from the equatorial launcher and 20MW co-ECCD driven by 2/3 from the equatorial launcher and 1/3 from the upper launcher is shown to be negligible. Cnt-ECCD also offers greater control of the plasma current density, therefore this analysis addresses the performance of the equatorial launcher to control the central q profile. The equatorial launcher is shown to control very efficiently the value of q{sub 0.2}-q{sub min} in advanced scenarios, if one row provides counter-ECCD.

Zucca, C.; Sauter, O.; Fable, E. [Ecole Polytechnique Federate de Lausanne, Centre de Recherches en Physique des Plasmas, Association EURATOM-Confederation Suisse, CH-1015 Lausanne (Switzerland); Henderson, M. A.; Polevoi, A. [ITER Organization, CHD Dpt, CEN Cadarache 519/007, 13108 Saint-Paul-les-Durance (France); Farina, D.; Ramponi, G. [Istituto di Fisica del Plasma, EURATOM-Enea-CNR Association, Milano (Italy); Saibene, G. [Fusion for Energy, c/Josep Pla, 08019 Barcelona (Spain); Zohm, H. [Max Planck Institut fuer Plasmaphysik IPP-EURATOM Association, Garching (Germany)

2008-11-01T23:59:59.000Z

343

last updated 12/05/2013 Deliverable Quarter Due (Draft!)  

E-Print Network [OSTI]

Forecast Q3 2014 Draft Results of Flexibility and Balancing Analysis Q4 2014 Demand Forecast Updated Q4, forecasts and other inputs Ongoing Narratives on Power Planning Topics and Issues (RSAC) Identify Topics 2014 Load Forecast Updated Q4 2014 Conservation Supply Curves Updated Q4 2014 Conceptual Definition

344

Vol XXIV, Issue 7 In This Issue February 16, 2009  

E-Print Network [OSTI]

Enforcing Emissions Policies Pemex Seeks Bids for Gasoline Desulfurization Plants Canada's EnCana Q4

Nikolaou, Michael

345

The absence of inactive regions in turbulent flow: Evidence from light scattering experiments  

E-Print Network [OSTI]

prediction3) for large q,4 hasled to modelswhich imply that the turbulence consists of "active" regions

Pak, Hyuk Kyu

346

INDIANA FARMSTEAD ASSESSMENT PROGRAM P u r d u e U n i v e r s i t y C o o p e r a t i v e E x t e n s i o n S e r v i c e We s t L a f a y e t t e , I N 4 7 9 0 7  

E-Print Network [OSTI]

facilities) located at least 100 feet away and downhill from your well? q q 4. Have all abandoned wells

Holland, Jeffrey

347

Spectroscopic Study of Microwave Induced Plasma  

SciTech Connect (OSTI)

The results of the spatial distribution studies of electron densities, excitation and rotational temperatures and atomic line intensities of various elements in an atmospheric pressure mini-MIP torch with tangential argon flow. The electron number density, ne, is determined from the width of the hydrogen H{beta} 486.13 nm line while excitation temperature, Texc, is evaluated from the Boltzmann plot of relative line intensities either of carrier gas-argon or neutral iron that is introduced in the form of aerosols in MIP, The rotational temperatures, Trot, are determined from the relative intensities of OH (R2 and Q1 branch) electronic band A2{sigma} - X2{pi} (0,0) and to N{sub 2}{sup +} first negative system B{sup 2} {sigma}{sub u}{sup +} - X{sup 2} {sigma}{sub g}{sup +} (P branch). For the selected input power of 100 W, the influence of hydrogen in the wet and desolvated aerosols and support gas and the corresponding changes of the electron density, excitation and rotational temperature distributions are studied. The influence of potassium, low ionization potential element, to the spatial distribution of ne, Texc and Trot is studied also. Spatial intensity distributions and maximum intensities for investigate atomic line are determinate for the same conditions.

Jovicevic, S. [Institute of Physics, 11081 Belgrade P.O. Box 68 (Serbia and Montenegro)

2004-12-01T23:59:59.000Z

348

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

349

Complexities in human herpesvirus-6A and -6B binding to host cells  

SciTech Connect (OSTI)

Human herpesvirus-6A and -6B uses the cellular receptor CD46 for fusion and infection of the host cell. The viral glycoprotein complex gH-gL from HHV-6A binds to the short consensus repeat 2 and 3 in CD46. Although all the major isoforms of CD46 bind the virus, certain isoforms may have higher affinity than others for the virus. Within recent years, elucidation of the viral complex has identified additional HHV-6A and -6B specific glycoproteins. Thus, gH-gL associates with a gQ1-gQ2 dimer to form a heterotetrameric complex. In addition, a novel complex consisting of gH-gL-gO has been described that does not bind CD46. Accumulating evidence suggests that an additional HHV-6A and -6B receptor exists. The previous simple picture of HHV-6A/B-host cell contact therefore includes more layers of complexities on both the viral and the host cell side of the interaction.

Pedersen, Simon Metz [Institute of Medical Microbiology and Immunology, The Bartholin Building, University of Aarhus, DK-8000 Aarhus C (Denmark); Hoellsberg, Per [Institute of Medical Microbiology and Immunology, The Bartholin Building, University of Aarhus, DK-8000 Aarhus C (Denmark)]. E-mail: ph@microbiology.au.dk

2006-12-20T23:59:59.000Z

350

Representations of quantum superalgebra Uq[gl(2|1)] in a coherent state basis and generalization  

E-Print Network [OSTI]

The coherent state method has proved to be useful in quantum physics and mathematics. This method, more precisely, the vector coherent state method, has been used by some authors to construct representations of superalgebras but almost, to our knowledge, it has not yet been extended to quantum superalgebras, except $U_q[osp(1|2)]$, one of the smallest quantum superalgebras. In this article the method is applied to a bigger quantum superalgebra, namely $U_q[gl(2|1)]$, in constructing $q$--boson-fermion realizations and finite-dimensional representations which, when irreducible, are classified into typical and nontypical representations. This construction leads to a more general class of $q$--boson-fermion realizations and finite-dimensional representations of $U_q[gl(2|1)]$ and, thus, at $q=1$, of $gl(2|1)$. Both $gl(2|1)$ and $U_q[gl(2|1)]$ have found different physics applications, therefore, it is meaningful to construct their representations.

Nguyen Cong Kien; Nguyen Anh Ky; Le Ba Nam; Nguyen Thi Hong Van

2012-01-10T23:59:59.000Z

351

Nonextensive critical effects in relativistic nuclear mean field models  

E-Print Network [OSTI]

We present a possible extension of the usual relativistic nuclear mean field models widely used to describe nuclear matter towards accounting for the influence of possible intrinsic fluctuations caused by the environment. Rather than individually identifying their particular causes we concentrate on the fact that such effects can be summarily incorporated in the changing of the statistical background used, from the usual (extensive) Boltzman-Gibbs one to the nonextensive taken in the form proposed by Tsallis with a dimensionless nonextensivity parameter $q$ responsible for the above mentioned effects (for $q \\rightarrow 1$ one recovers the usual BG case). We illustrate this proposition on the example of the QCD-based Nambu - Jona-Lasinio (NJL) model of a many-body field theory describing the behavior of strongly interacting matter presenting its nonextensive version. We check the sensitivity of the usual NJL model to a departure from the BG scenario expressed by the value of $| q - 1|$, in particular in the vicinity of critical points.

J. Rozynek; G. Wilk

2011-02-22T23:59:59.000Z

352

AUTOMATED CLASSIFICATION OF VARIABLE STARS IN THE ASTEROSEISMOLOGY PROGRAM OF THE KEPLER SPACE MISSION  

SciTech Connect (OSTI)

We present the first results of the application of supervised classification methods to the Kepler Q1 long-cadence light curves of a subsample of 2288 stars measured in the asteroseismology program of the mission. The methods, originally developed in the framework of the CoRoT and Gaia space missions, are capable of identifying the most common types of stellar variability in a reliable way. Many new variables have been discovered, among which a large fraction are eclipsing/ellipsoidal binaries unknown prior to launch. A comparison is made between our classification from the Kepler data and the pre-launch class based on data from the ground, showing that the latter needs significant improvement. The noise properties of the Kepler data are compared to those of the exoplanet program of the CoRoT satellite. We find that Kepler improves on CoRoT by a factor of 2-2.3 in point-to-point scatter.

Blomme, J.; Debosscher, J.; De Ridder, J.; Aerts, C. [Instituut voor Sterrenkunde, Katholieke Universiteit Leuven, Celestijnenlaan 200D, B-3001 Leuven (Belgium); Gilliland, R. L. [Space Telescope Science Institute, 3700 San Martin Drive, Baltimore, MD 21218 (United States); Christensen-Dalsgaard, J.; Kjeldsen, H. [Department of Physics and Astronomy, Aarhus University, DK-8000 Aarhus C (Denmark); Brown, T. M. [Las Cumbres Observatory Global Telescope, Goleta, CA 93117 (United States); Borucki, W. J.; Koch, D. [NASA Ames Research Center, MS 244-30, Moffett Field, CA 94035 (United States); Jenkins, J. M. [SETI Institute/NASA Ames Research Center, MS 244-30, Moffett Field, CA 94035 (United States); Kurtz, D. W. [Jeremiah Horrocks Institute of Astrophysics, University of Central Lancashire, PR1 2HE (United Kingdom); Stello, D.; Derekas, A. [Sydney Institute for Astronomy (SIfA), School of Physics, University of Sydney, NSW 2006 (Australia); Stevens, I. R. [School of Physics and Astronomy, University of Birmingham, Edgbaston B15 2TT (United Kingdom); Suran, M. D. [Astronomical Institute of the Romanian Academy, Str. Cutitul de Argint 5, RO 40557, Bucharest, RO (Romania)

2010-04-20T23:59:59.000Z

353

Cielo Computational Environment Usage Model With Mappings to ACE Requirements for the General Availability User Environment Capabilities Release Version 1.1  

SciTech Connect (OSTI)

Cielo is a massively parallel supercomputer funded by the DOE/NNSA Advanced Simulation and Computing (ASC) program, and operated by the Alliance for Computing at Extreme Scale (ACES), a partnership between Los Alamos National Laboratory (LANL) and Sandia National Laboratories (SNL). The primary Cielo compute platform is physically located at Los Alamos National Laboratory. This Cielo Computational Environment Usage Model documents the capabilities and the environment to be provided for the Q1 FY12 Level 2 Cielo Capability Computing (CCC) Platform Production Readiness Milestone. This document describes specific capabilities, tools, and procedures to support both local and remote users. The model is focused on the needs of the ASC user working in the secure computing environments at Lawrence Livermore National Laboratory (LLNL), Los Alamos National Laboratory, or Sandia National Laboratories, but also addresses the needs of users working in the unclassified environment. The Cielo Computational Environment Usage Model maps the provided capabilities to the tri-Lab ASC Computing Environment (ACE) Version 8.0 requirements. The ACE requirements reflect the high performance computing requirements for the Production Readiness Milestone user environment capabilities of the ASC community. A description of ACE requirements met, and those requirements that are not met, are included in each section of this document. The Cielo Computing Environment, along with the ACE mappings, has been issued and reviewed throughout the tri-Lab community.

Vigil,Benny Manuel [Los Alamos National Laboratory; Ballance, Robert [SNL; Haskell, Karen [SNL

2012-08-09T23:59:59.000Z

354

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

355

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

356

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

357

Function of SiO/sub 2/ colloids in photoinduces redox reactions. Interfacial effects on the quenching, charge separation, and quantum yields. [Propyl viologen sulfonate  

SciTech Connect (OSTI)

The function of negatively charged colloidal SiO/sub 2/ particles in controlling photosensitized electron-transfer reactions by means of electrostatic interactions between the different components in the system has been studied under steady-state conditions of illumination and by flash photolysis. In particular, the photosensitized reduction of the zwitterionic electron acceptor, propyl viologen sufonate, PVS/sup 0/ (1), using tris(2,2'-bipyridinium)ruthenium(II), Ru(bpy)/sub 3//sup 2 +/, as sensitizer has been investigated in the SiO/sub 2/ colloid and compared to the homogeneous system. Fluorescence quenching studies indicate that the quenching reaction of Ru(bpy)/sub 3//sup 2 +/ with the neutral PVS/sup 0/ is not affected by electrostatic interactions exerted by the negatively charged SiO/sub 2/ interface (k/sub q/ = 1.5 x 10/sup 9/ M/sup -1/s/sup -1/). In contrast, the quenching of Ru(bpy)/sub 3//sup 2 +/ by the positively charged methylviologen, MV/sup 2 +/, is strongly enhanced by the SiO/sub 2/colloid (k/sub q/ = 5 x 10/sup 10/ M/sup -1/s/sup -1/.

Willner, I.; Yang, J.M.; Laane, C.; Otvos, J.W.; Calvin, M.

1981-10-29T23:59:59.000Z

358

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

359

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

360

Direct Searches for Scalar Leptoquarks at the Run II Tevatron  

SciTech Connect (OSTI)

This dissertation sets new limits on the mass of the scalar leptoquark from direct searches carried out at the Run II CDF detector using data from March 2001 to October 2003. The data analyzed has a total time-integrated measured luminosity of 198 pb{sup -1} of p{bar p} collisions with {radical}s = 1.96 TeV. Leptoquarks are assumed to be pair-produced and to decay into a lepton and a quark of the same generation. They consider two possible leptoquark decays: (1) {beta} = BR(LQ {yields} {mu}q) = 1.0, and (2) {beta} = BR(LQ {yields} {mu}q) = 0.5. For the {beta} = 1 channel, they focus on the signature represented by two isolated high-p{sub T} muons and two isolated high-p{sub T} jets. For the {beta} = 1/2 channel, they focus on the signature represented by one isolated high-p{sub T} muon, large missing transverse energy, and two isolated high-p{sub T} jets. No leptoquark signal is experimentally detected for either signature. Using the next to leading order theoretical cross section for scalar leptoquark production in p{bar p} collisions [1], they set new mass limits on second generation scalar leptoquarks. They exclude the existence of second generation scalar leptoquarks with masses below 221(175) GeV/c{sup 2} for the {beta} = 1(1/2) channels.

Ryan, Daniel E

2004-11-01T23:59:59.000Z

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361

Monitoring of tritium purity during long-term circulation in the KATRIN test experiment LOOPINO using laser Raman spectroscopy  

E-Print Network [OSTI]

The gas circulation loop LOOPINO has been set up and commissioned at Tritium Laboratory Karlsruhe (TLK) to perform Raman measurements of circulating tritium mixtures under conditions similar to the inner loop system of the neutrino-mass experiment KATRIN, which is currently under construction. A custom-made interface is used to connect the tritium containing measurement cell, located inside a glove box, with the Raman setup standing on the outside. A tritium sample (purity > 95%, 20 kPa total pressure) was circulated in LOOPINO for more than three weeks with a total throughput of 770 g of tritium. Compositional changes in the sample and the formation of tritiated and deuterated methanes CT_(4-n)X_n (X=H,D; n=0,1) were observed. Both effects are caused by hydrogen isotope exchange reactions and gas-wall interactions, due to tritium {\\beta} decay. A precision of 0.1% was achieved for the monitoring of the T_2 Q_1-branch, which fulfills the requirements for the KATRIN experiment and demonstrates the feasibility ...

Fischer, Sebastian; Schlösser, Magnus; Bornschein, Beate; Drexlin, Guido; Priester, Florian; Lewis, Richard J; Telle, Helmut H

2012-01-01T23:59:59.000Z

362

The basic K nuclear cluster K- pp and its enhanced formation in the p + p -> K+ + X reaction  

E-Print Network [OSTI]

We have studied the structure of K- pp nuclear cluster comprehensively by solving this three-body system exactly in a variational method starting from the Ansatz that the Lambda(1405) resonance (Lambda*) is a K-p bound state. We have found that our original prediction for the presence of K-pp as a compact bound system with M = 2322$ MeV/c2, B = 48 MeV and Gamma = 60 MeV remains unchanged by varying the Kba-rN and NN interactions widely as far as they reproduce Lambda(1405). The structure of K- pp reveals a molecular feature, namely, the K- in Lambda* as an "atomic center" plays a key role in producing strong covalent bonding with the other proton. We have shown that the elementary process, p + p -> K+ + Lambda* + p, which occurs in a short impact parameter and with a large momentum transfer (Q ~ 1.6$ GeV/c), leads to unusually large self-trapping of Lambda* by the participating proton, since the Lambda*-p system exists as a compact doorway state propagating to K- pp (R{Lambda*-p} ~ 1.67 fm).

Toshimitsu Yamazaki; Yoshinori Akaishi

2007-09-06T23:59:59.000Z

363

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

364

Recoils from unequal-mass, precessing black-hole binaries: The Intermediate Mass Ratio Regime  

E-Print Network [OSTI]

We revisit the modeling of the properties of the black-hole remnant resulting the merger of a black-hole binary as a function of the parameters of the binary. We provide a set of empirical formulas for the final mass, spin and recoil velocity of the final black hole as a function of the mass ratio and individual spins of the progenitor. In order to determine the fitting coefficients for these formulas, we perform a set of 126 new numerical evolutions of precessing, unequal-mass black-hole binaries, and fit to the resulting remnant mass, spin, and recoil. In order to reduce the complexity of the analysis, we chose configurations that have one of the black holes spinning, with dimensionless spin alpha=0.8, at different angles with respect to the orbital angular momentum, and the other non-spinning. In addition to evolving families of binaries with different spin-inclination angles, we also evolved binaries with mass ratios as small as q=1/6. We use the resulting empirical formulas to predict the probabilities o...

Zlochower, Yosef

2015-01-01T23:59:59.000Z

365

Chromosome region-specific libraries for human genome analysis. Final progress report, 1 March 1991--28 February 1994  

SciTech Connect (OSTI)

The objectives of this grant proposal include (1) development of a chromosome microdissection and PCR-mediated microcloning technology, (2) application of this microtechnology to the construction of region-specific libraries for human genome analysis. During this grant period, the authors have successfully developed this microtechnology and have applied it to the construction of microdissection libraries for the following chromosome regions: a whole chromosome 21 (21E), 2 region-specific libraries for the long arm of chromosome 2, 2q35-q37 (2Q1) and 2q33-q35 (2Q2), and 4 region-specific libraries for the entire short arm of chromosome 2, 2p23-p25 (2P1), 2p21-p23 (2P2), 2p14-p16 (wP3) and 2p11-p13 (2P4). In addition, 20--40 unique sequence microclones have been isolated and characterized for genomic studies. These region-specific libraries and the single-copy microclones from the library have been used as valuable resources for (1) isolating microsatellite probes in linkage analysis to further refine the disease locus; (2) isolating corresponding clones with large inserts, e.g. YAC, BAC, P1, cosmid and phage, to facilitate construction of contigs for high resolution physical mapping; and (3) isolating region-specific cDNA clones for use as candidate genes. These libraries are being deposited in the American Type Culture Collection (ATCC) for general distribution.

Kao, F.T.

1994-04-01T23:59:59.000Z

366

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

367

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

368

PARIS-JOURDAN SCIENCES ECONOMIQUES 48, BD JOURDAN E.N.S. 75014 PARIS  

E-Print Network [OSTI]

schemes: selected questions in analytical perspective Roger Guesnerie JEL Codes : D02, D6, D7, F18, Q4,Q5 of required attention. JEL : D02, D6, D7, F18, Q4,Q5 Institutional design, fossil fuels prices, ratchet e ect'elle mérite. JEL : D02, D6, D7, F18, Q4,Q5 Institutions, carburants fossiles, e et de cliquet, quantité contre

Paris-Sud XI, Université de

369

What Does a Scattering Pattern Tell US?  

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

Space sample light image Image Space lens Angular Space Q 4p sin(q) l Fourier Transform Scattering Pattern Fourier Transform Phase Problem Scattering Pattern Fourier...

370

NNSA Corporate CPEP Process NNSA Honeywell FM&T PER NNSA/NA-00...  

National Nuclear Security Administration (NNSA)

"meets expectations." Cyber Security - Honeywell's AOP metrics for Q4 and the year were Green, no issues. All AOP milestones were delivered on time. Cyber Security completed...

371

The Household Market for Electric Vehicles: Testing the Hybrid Household Hypothesis -- A Reflexively Designed Survey of New-Car-Buying Multi-Vehicle California Households  

E-Print Network [OSTI]

by electric and hybrid vehicles", SAETechmcal Papers No.$ not Q 4. If you chose the Hybrid Vehicle - can you specifymay response to hybrid vehicles Finally, we suggest that

Turrentine, Thomas; Kurani, Kenneth S.

2001-01-01T23:59:59.000Z

372

ON THE FORMATION OF DOUBLE WHITE DWARFS THROUGH STABLE MASS TRANSFER AND A COMMON ENVELOPE  

SciTech Connect (OSTI)

Although several dozen double white dwarfs (DWDs) have been observed, for many the exact nature of the evolutionary channel(s) by which they form remains uncertain. The canonical explanation calls for the progenitor binary system to undergo two subsequent mass-transfer events, both of which are unstable and lead to a common envelope (CE). However, it has been shown that if both CE events obey the standard {alpha}{sub CE}-prescription (parameterizing energy loss), it is not possible to reproduce all of the observed systems. The {gamma}-prescription was proposed as an alternative to this description, instead parameterizing the fraction of angular momentum carried away in dynamical-timescale mass loss. However, this too has proven problematic, and does not provide a clear physical mechanism. In this paper, we consider in detail the first episode of mass transfer in binary systems with initially low companion masses, with a primary mass in the range 1.0-1.3 M{sub Sun} and an initial mass ratio between the secondary and primary stars of 0.83-0.92. In these systems, the first episode of dramatic mass loss may be stable, non-conservative mass transfer. This strips the donor's envelope and dramatically raises the mass ratio; the considered progenitor binary systems can then evolve into DWDs after passing through a single CE during the second episode of mass loss. We find that such a mechanism reproduces the properties of the observed DWD systems which have an older component with M {approx}< 0.46 M{sub Sun} and mass ratios between the younger and older WDs of q {>=} 1.

Woods, T. E.; Ivanova, N. [Department of Physics, University of Alberta, 11322-89 Ave., Edmonton, AB T6G 2E7 (Canada); Van der Sluys, M. V. [Department of Astrophysics, Radboud University Nijmegen, P.O. Box 9010, NL-6500 GL Nijmegen (Netherlands); Chaichenets, S. [Department of Mathematical and Statistical Sciences, University of Alberta, CAB, Edmonton, AB T6G 2G1 (Canada)

2012-01-01T23:59:59.000Z

373

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

374

Real-time sawtooth control and neoclassical tearing mode preemption in ITER  

SciTech Connect (OSTI)

Real-time control of multiple plasma actuators is a requirement in advanced tokamaks; for example, for burn control, plasma current profile control and MHD stabilization—electron cyclotron (EC) wave absorption is ideally suited especially for the latter. On ITER, 24 EC sources can be switched between 56 inputs at the torus. In the torus, 5 launchers direct the power to various locations across the plasma profile via 11 steerable mirrors. For optimal usage of the available power, the aiming and polarization of the beams must be adapted to the plasma configuration and the needs of the scenario. Since the EC system performs many competing tasks, present day systems should demonstrate the ability of an EC plant to deal with several targets in parallel and/or to switch smoothly between goals to attain overall satisfaction. Based on pacing and locking experiments performed on TCV (Tokamak ŕ Configuration Variable), the real-time sawtooth control of ITER with this complex set of actuators is analyzed, as an example. It is shown that sawtooth locking and pacing are possible with various levels of powers, leading to different time delays between the end of the EC power phase and the next sawtooth crash. This timing is important since it allows use of the same launchers for neoclassical tearing mode (NTM) preemption at the q?=?1.5 or 2 surface, avoiding the need to switch power between launchers. These options are presented. It is also demonstrated that increasing the total EC power does not necessarily increase the range of control because of the geometry of the launchers.

Kim, D., E-mail: doohyun.kim@epfl.ch; Goodman, T. P.; Sauter, O. [École Polytechnique Fédérale de Lausanne (EPFL), Centre de Recherches en Physique des Plasmas (CRPP), CH-1015 Lausanne (Switzerland)

2014-06-15T23:59:59.000Z

375

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. Csanád; T. Csörg?; 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. -Ĺ. 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; Á. Kiss; E. Kistenev; A. Kiyomichi; J. Klay; C. Klein-Boesing; L. Kochenda; V. Kochetkov; B. Komkov; M. Konno; D. Kotchetkov; A. Kozlov; A. Král; 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. Liška; 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. Mašek; H. Masui; F. Matathias; M. C. McCain; M. McCumber; P. L. McGaughey; Y. Miake; P. Mikeš; 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. Tarján; T. L. Thomas; T. Todoroki; M. Togawa; A. Toia; J. Tojo; L. Tomášek; H. Torii; R. S. Towell; V-N. Tram; I. Tserruya; Y. Tsuchimoto; S. K. Tuli; H. Tydesjö; N. Tyurin; C. Vale; H. Valle

2014-12-02T23:59:59.000Z

376

Dynamical Transition and Heterogeneous Hydration Dynamics in RNA  

E-Print Network [OSTI]

Enhanced dynamical fluctuations of RNAs, facilitated by a network of water molecules with strong interactions with RNA, are suspected to be critical in their ability to respond to a variety of cellular signals. Using atomically detailed molecular dynamics simulations at various temperatures of purine (adenine)- and preQ$_1$ sensing riboswitch aptamers, we show that water molecules in the vicinity of RNAs undergo complex dynamics depending on the local structures of the RNAs. The overall lifetimes of hydrogen bonds (HBs) of surface bound waters are more than at least 1-2 orders of magnitude longer than bulk water. Slow hydration dynamics, revealed in non-Arrhenius behavior of the relaxation time, arises from high activation barriers to break water hydrogen bonds with a nucleotide and by reduced diffusion of water. The relaxation kinetics at specific locations in the two RNAs show a broad spectrum of time scales reminiscent of glass-like behavior, suggesting that the hydration dynamics is highly heterogeneous. Both RNAs undergo dynamic transition at $T = T_D \\gtrsim 200$ K as assessed by the mean square fluctuation of hydrogen atoms $\\langle x^2\\rangle$, which undergoes an abrupt harmonic-to-anharmonic transition at $T_D$. The near universal value of $T_D$ found for these RNAs and previously for tRNA is strongly correlated with changes in hydration dynamics as $T$ is altered. Hierarchical dynamics of waters associated with the RNA surface, revealed in the motions of distinct classes of water with well-separated time scales, reflects the heterogeneous local environment on the molecular surface of RNA. At low temperatures slow water dynamics predominates over structural transitions. Our study demonstrates that the complex interplay of dynamics between water and local environment in the RNA structures could be a key determinant of the functional activities of RNA.

Jeseong Yoon; Jong-Chin Lin; Changbong Hyeon; D. Thirumalai

2014-04-24T23:59:59.000Z

377

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

378

SOUTHEAST REGIONAL CARBON SEQUESTRATION PARTNERSHP (SECARB)  

SciTech Connect (OSTI)

The Southeast Regional Carbon Sequestration Partnership (SECARB) is on schedule and within budget projections for the work completed during the first 18-months of its two year program. Work during the semiannual period (fifth and sixth project quarters) of the project (October 1, 2004-March 31, 2005) was conducted within a ''Task Responsibility Matrix.'' Under Task 1.0 Define Geographic Boundaries of the Region, no changes occurred during the fifth or sixth quarters of the project. Under Task 2.0 Characterize the Region, refinements have been made to the general mapping and screening of sources and sinks. Integration and geographical information systems (GIS) mapping is ongoing. Characterization during this period was focused on smaller areas having high sequestration potential. Under Task 3.0 Identify and Address Issues for Technology Deployment, SECARB continues to expand upon its assessment of safety, regulatory, permitting, and accounting frameworks within the region to allow for wide-scale deployment of promising terrestrial and geologic sequestration approaches. Under Task 4.0 Develop Public Involvement and Education Mechanisms, SECARB has used results of a survey and focus group meeting to refine approaches that are being taken to educate and involve the public. Under Task 5.0 Identify the Most Promising Capture, Sequestration, and Transport Options, SECARB has evaluated findings from work performed during the first 18-months. The focus of the project team has shifted from region-wide mapping and characterization to a more detailed screening approach designed to identify the most promising opportunities. Under Task 6.0 Prepare Action Plans for Implementation and Technology Validation Activity, the SECARB team is developing an integrated approach to implementing the most promising opportunities and in setting up measurement, monitoring and verification (MMV) programs for the most promising opportunities. Milestones completed during the fifth and sixth project quarters included: (1) Q1-FY05--Assess safety, regulatory and permitting issues; and (2) Q2-FY05--Finalize inventory of major sources/sinks and refine GIS algorithms.

Kenneth J. Nemeth

2005-04-01T23:59:59.000Z

379

Generation of Free Oxygen Atoms O(3P) in Solution by Photolysis of 4-Benzoylpyridine N-Oxide  

SciTech Connect (OSTI)

Laser flash photolysis of 4-benzoylpyridine N-oxide (BPyO) at 308 nm in aqueous solutions generates a triplet excited state 3BPyO* that absorbs strongly in the visible, ?max 490 and 380 nm. 3BPyO* decays with the rate law kdecay/s?1 = (3.3 ± 0.9) × 104 + (1.5 ± 0.2) × 109 [BPyO] to generate a mixture of isomeric hydroxylated benzoylpyridines, BPy(OH), in addition to small amounts of oxygen atoms, O(3P). Molecular oxygen quenches 3BPyO*, kQ = 1.4 × 109 M?1 s?1, but the yields of O(3P) increase in O2-saturated solutions to 36%. Other triplet quenchers have a similar effect, which rules out the observed 3BPyO* as a source of O(3P). It is concluded that O(3P) is produced from either 1BPyO* or a short-lived, unobserved, higher energy triplet generated directly from 1BPyO*. 3BPyO* is reduced by Fe2+ and by ABTS2? to the radical anion BPyO?? which exhibits a maximum at 510 nm, ? = 2200 M?1 cm?1. The anion engages in back electron transfer with ABTS?? with k = 1.7 × 109 M?1 s?1. The same species can be generated by reducing ground state BPyO with ?C(CH3)2OH. The photochemistry of BPyO in acetonitrile is similar to that in aqueous solutions.

Carraher, Jack M. [Ames Laboratory; Bakac, Andreja [Ames Laboratory

2014-08-04T23:59:59.000Z

380

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

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381

WIDE COMPANIONS TO HIPPARCOS STARS WITHIN 67 pc OF THE SUN  

SciTech Connect (OSTI)

A catalog of common-proper-motion (CPM) companions to stars within 67 pc of the Sun is constructed based on the SUPERBLINK proper-motion survey. It contains 1392 CPM pairs with angular separations 30'' < {rho} < 1800'', relative proper motion between the two components less than 25 mas yr{sup -1}, and magnitudes and colors of the secondaries consistent with those of dwarfs in the (M{sub V} , V - J) diagram. In addition, we list 21 candidate white dwarf CPM companions with separations under 300'', about half of which should be physical. We estimate a 0.31 fraction of pairs with red dwarf companions to be physical systems (about 425 objects), while the rest (mostly wide pairs) are chance alignments. For each candidate companion, the probability of a physical association is evaluated. The distribution of projected separations s of the physical pairs between 2 kAU and 64 kAU follows f(s){proportional_to}s {sup -1.5}, which decreases faster than Oepik's law. We find that solar-mass dwarfs have no less than 4.4% {+-} 0.3% companions with separations larger than 2 kAU, or 3.8% {+-} 0.3% per decade of orbital separation in the 2-16 kAU range. The distribution of mass ratio of those wide companions is approximately uniform in the 0.1 < q < 1.0 range, although we observe a dip at q {approx_equal} 0.5 which, if confirmed, could be evidence of bimodal distribution of companion masses. New physical CPM companions to two exoplanet host stars are discovered.

Tokovinin, Andrei [Cerro Tololo Inter-American Observatory, Casilla 603, La Serena (Chile); Lepine, Sebastien, E-mail: atokovinin@ctio.noao.edu, E-mail: lepine@amnh.org [Department of Astrophysics, Division of Physical Sciences, American Museum of Natural History, Central Park West at 79th Street, New York, NY 10024 (United States)

2012-10-01T23:59:59.000Z

382

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

383

University of Delaware -Tribology Laboratory Atlantic Advanced O shore Wind Energy Consortium  

E-Print Network [OSTI]

Wind Energy Consortium Assessing Tribological Aspects of Gearbox Reliability in Wind Turbines Prof for analysis by the group. Downtime hours accumulated from 2003 to 2007 for wind turbines in Germany #12. Instrument Lewes Turbine - Evaluate the loads on a large-scale turbine; Q4 D. Collect Turbine Data; Q4-8 E

Firestone, Jeremy

384

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

385

The Transcription Factor Encyclopedia  

E-Print Network [OSTI]

f8nK 2f8nH 2f8nF 2f8nB 2f8nD 1p3iG 1p3aC 1p3aF 1p3aD 1p3oB 1p3bG 1p3pG 1p3fD 1p34B 1p3oF 1p3iD 1p3gD 1p3oD 1p3bH 1p3iC 1p3lH 1p34C 1p3bD 1p3kB 1p3pF 1p3mH 1p3lB 1p34H 1p3mC 1p3gG 1p3mD 1p34D 1p3kD 1p3oG 1p3lF 1p3bC 1p3kH 1p3pH 1p3iH 1p3pB 1p3gH 1p3kC... 02N 2o61A 2o61B 2as5N 2as5M 1gjiA 1gjiB 1nfkA 1nfkB 1s9kC 1owrP 1owrQ 1owrM 1owrN 1svcP 1le5A 1leiB 1le5E 1le9E 1le5B 1le9F 1le5F 1le9B 1le9A 1leiA DNA_pol_lambd_f 3c5fB 3c5gB 3c5fA 3c5gA 1huoB 1huoA 1huzA 1huzB 2i9gA 1tv9A 1tvaA 2fmsA 2fmpA 2fmqA 1...

Yusuf, Dimas; Butland, Stefanie L; Swanson, Magdalena I; Bolotin, Eugene; Ticoll, Amy; Cheung, Warren A; Cindy Zhang, Xiao Y; Dickman, Christopher TD; Fulton, Debra L; Lim, Jonathan S; Schnabl, Jake M; Luo, Xin M; Blank, Marissa C; Millen, Kathleen J; Sharlin, David S; Forrest, Douglas; Dahlman-Wright, Karin; Zhao, Chunyan; Mishima, Yuriko; Sinha, Satrajit; Chakrabarti, Rumela; Ramos, Oscar HP; Portales-Casamar, Elodie; Sladek, Frances M; Bradley, Philip H; Wasserman, Wyeth W; Vasseur-Cognet, Mireille; de Leeuw, Charles N; Simpson, Elizabeth M; Ryffel, Gerhart U; Lam, Eric W-F; Kist, Ralf; Wilson, Miranda SC; Marco-Ferreres, Raquel; Brosens, Jan J; Beccari, Leonardo L; Bovolenta, Paola; Benayoun, Bérénice A; Monteiro, Lara J; Schwenen, Helma DC; Grontved, Lars; Wederell, Elizabeth; Mandrup, Susanne; Veitia, Reiner A; Chakravarthy, Harini; Hoodless, Pamela A; Mancarelli, M Michela; Torbett, Bruce E; Banham, Alison H; Reddy, Sekhar P; Cullum, Rebecca L; Liedtke, Michaela; Tschan, Mario P; Vaz, Michelle; Rizzino, Angie; Zannini, Mariastella; Frietze, Seth; Farnham, Peggy J; Eijkelenboom, Astrid; Brown, Philip J; Laperričre, David; Leprince, Dominique; de Cristofaro, Tiziana; Prince, Kelly L; Putker, Marrit; del Peso, Luis; Camenisch, Gieri; Wenger, Roland H; Mikula, Michal; Rozendaal, Marieke; Mader, Sylvie; Ostrowski, Jerzy; Rhodes, Simon J; Van Rechem, Capucine; Boulay, Gaylor; Olechnowicz, Sam WZ; Breslin, Mary B; Lan, Michael S; Nanan, Kyster K; Wegner, Michael; Hou, Juan; Mullen, Rachel D; Colvin, Stephanie C; Noy, Peter J; Webb, Carol F; Witek, Matthew E; Ferrell, Scott; Daniel, Juliet M; Park, Jason; Waldman, Scott A; Peet, Daniel J; Taggart, Michael; Jayaraman, Padma-Sheela; Karrich, Julien J; Blom, Bianca; Vesuna, Farhad; O'Geen, Henriette; Sun, Yunfu; Gronostajski, Richard M; Woodcroft, Mark W; Hough, Margaret R; Chen, Edwin; Europe-Finner, G Nicholas; Karolczak-Bayatti, Magdalena; Bailey, Jarrod; Hankinson, Oliver; Raman, Venu; LeBrun, David P; Biswal, Shyam; Harvey, Christopher J; DeBruyne, Jason P; Hogenesch, John B; Hevner, Robert F; Héligon, Christophe

2012-03-29T23:59:59.000Z

386

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

387

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

388

What Does a Scattering Pattern Tell US?  

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

e iwt Phase difference Phase difference S e i (ri Q) A(DK) fi A(Q) Fourier Transform ( ri ) DK Q 4p sin(q) l Lensless Imaging Sample Space Scattering Space sample...

389

E-Print Network 3.0 - amr ph gl Sample Search Results  

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

Algorithm using Adaptive Mesh Refinement Summary: the complexity for constructing the AMR tree is Odtn1 ph 1 p 6dm1 qh 1 q . 4.2 Data Clustering. The stage... of the AMR...

390

Microsoft Word - Agenda F&I Update 090804.doc | Department of...  

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

Agenda F&I Update 090804.doc Microsoft Word - Agenda F&I Update 090804.doc More Documents & Publications Agenda Slide 1 Microsoft Word - Issue FY2009 Q4 Draft 20090910.doc...

391

KAPL-4756 UC-901  

Office of Scientific and Technical Information (OSTI)

E q . (4), however, is virtually,identical to the -47.9 f6.6 Jmol-K value found by Johnson and Baumanml for dissolution of freshly precipitated, amorphous Fe(OH),. As shown in...

392

Final Report on DOE Conference Activities for May 11, 2012 to...  

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

2012 - 1-30-13.pdf More Documents & Publications Inspection Report: DOEIG-0913 Supercritical Carbon Dioxide Turbo-Expander - FY12 Q4 Algal Biofuels Strategy Workshop - Fall Event...

393

E-Print Network 3.0 - anti-inflammatory heat shock Sample Search...  

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

64.4 21.9 Q4 72.0 ... Source: Chow, Carson C.- Laboratory of Biological Modeling, NIDDK, NIH & Department of Mathematics, University of Pittsburgh Collection: Biology and Medicine...

394

Carbon Fiber Technology Facility  

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

FY13Q4 * Forecast finish FY13Q2 * Currently in design phase * Barriers addressed - Cost - Inadequate supply base - Manufacturability * 34.77M Budget - No cost share * All...

395

Integrated Biomass Gasification with Catalytic Partial Oxidation for Selective Tar Conversion  

SciTech Connect (OSTI)

Biomass gasification is a flexible and efficient way of utilizing widely available domestic renewable resources. Syngas from biomass has the potential for biofuels production, which will enhance energy security and environmental benefits. Additionally, with the successful development of low Btu fuel engines (e.g. GE Jenbacher engines), syngas from biomass can be efficiently used for power/heat co-generation. However, biomass gasification has not been widely commercialized because of a number of technical/economic issues related to gasifier design and syngas cleanup. Biomass gasification, due to its scale limitation, cannot afford to use pure oxygen as the gasification agent that used in coal gasification. Because, it uses air instead of oxygen, the biomass gasification temperature is much lower than well-understood coal gasification. The low temperature leads to a lot of tar formation and the tar can gum up the downstream equipment. Thus, the biomass gasification tar removal is a critical technology challenge for all types of biomass gasifiers. This USDA/DOE funded program (award number: DE-FG36-O8GO18085) aims to develop an advanced catalytic tar conversion system that can economically and efficiently convert tar into useful light gases (such as syngas) for downstream fuel synthesis or power generation. This program has been executed by GE Global Research in Irvine, CA, in collaboration with Professor Lanny Schmidt's group at the University of Minnesota (UoMn). Biomass gasification produces a raw syngas stream containing H2, CO, CO2, H2O, CH4 and other hydrocarbons, tars, char, and ash. Tars are defined as organic compounds that are condensable at room temperature and are assumed to be largely aromatic. Downstream units in biomass gasification such as gas engine, turbine or fuel synthesis reactors require stringent control in syngas quality, especially tar content to avoid plugging (gum) of downstream equipment. Tar- and ash-free syngas streams are a critical requirement for commercial deployment of biomass-based power/heat co-generation and biofuels production. There are several commonly used syngas clean-up technologies: (1) Syngas cooling and water scrubbing has been commercially proven but efficiency is low and it is only effective at small scales. This route is accompanied with troublesome wastewater treatment. (2) The tar filtration method requires frequent filter replacement and solid residue treatment, leading to high operation and capital costs. (3) Thermal destruction typically operates at temperatures higher than 1000oC. It has slow kinetics and potential soot formation issues. The system is expensive and materials are not reliable at high temperatures. (4) In-bed cracking catalysts show rapid deactivation, with durability to be demonstrated. (5) External catalytic cracking or steam reforming has low thermal efficiency and is faced with problematic catalyst coking. Under this program, catalytic partial oxidation (CPO) is being evaluated for syngas tar clean-up in biomass gasification. The CPO reaction is exothermic, implying that no external heat is needed and the system is of high thermal efficiency. CPO is capable of processing large gas volume, indicating a very compact catalyst bed and a low reactor cost. Instead of traditional physical removal of tar, the CPO concept converts tar into useful light gases (eg. CO, H2, CH4). This eliminates waste treatment and disposal requirements. All those advantages make the CPO catalytic tar conversion system a viable solution for biomass gasification downstream gas clean-up. This program was conducted from October 1 2008 to February 28 2011 and divided into five major tasks. - Task A: Perform conceptual design and conduct preliminary system and economic analysis (Q1 2009 ~ Q2 2009) - Task B: Biomass gasification tests, product characterization, and CPO tar conversion catalyst preparation. This task will be conducted after completing process design and system economics analysis. Major milestones include identification of syngas cleaning requirements for proposed system

Zhang, Lingzhi; Wei, Wei; Manke, Jeff; Vazquez, Arturo; Thompson, Jeff; Thompson, Mark

2011-05-28T23:59:59.000Z

396

[Interview]: Alexandre Shvartsburg, Pacific Northwest National Laboratory, Richland, WA, USA  

SciTech Connect (OSTI)

Q1. What are your main research activities in ion mobility mass spectrometry (past or present)? My early efforts focused on the structural characterization of atomic (carbon and semiconductor) clusters. After the production of bulk fullerenes, many hoped that other nanoclusters discovered in the gas phase could also coalesce into new materials. As these studies required accurate and robust mobility calculations for any ion geometry, I strived to build the needed theory and implement it in the Mobcal software widely employed today. Since 2004, I have been developing methods and novel applications of differential IMS (FAIMS) at PNNL. The principal achievement has been raising the resolving power by over tenfold (up to ~400 for multiply-charged peptides) using elevated fields, helium and hydrogen-rich buffers, and extended filtering times. This performance broadly allows previously unthinkable separations of very similar species, for example sequence inversions and post-translational modification localization isomers of peptides (including “middle-down” peptides such as histone tails), lipid regioisomers, and even isotopomers. Another major direction is investigating the dipole alignment of larger proteins, which creates an exceptionally strong FAIMS effect that is a potential tool for structural biology. Q2: What have been the most significant instrumentation or applications developments in the history of ion mobility - mass spectrometry? In 1995 when I started graduate research at Northwestern, only two groups worldwide worked with IMS/MS and “the literature” meant papers by Bowers (UCSB). Well-wishers counseled me to “learn something useful like HPLC, as IMS would never have real utility”. This booklet showcases the scale of change since. First, the practical IMS/ToF platforms for complex biological analyses demonstrated by Clemmer have turned IMS/MS from an esoteric physical chemistry technique into a powerful analytical tool. By commercializing the IMS/ToF technology in Synapt instruments, Waters has greatly increased its impact via expanded number and diversity of applications. Concurrently, Guevremont at Canadian NRC has perfected FAIMS coupled to MS, deployed it for real-world bio and environmental analyses, and widely distributed it in the Ionalytics Selectra system (subsequently installed on Thermo MS platforms). The latest breakthrough is ultra-FAIMS by Owlstone, where extreme fields allow numerous qualitatively new separations and operational modes that we just begin to explore. Q3: Where do you see ion mobility - mass spectrometry making the most impact in the next 5 years? Any predictions for where the field will go? Sciences dealing with perturbations in media (such as optics or acoustics) at some point shift from the linear to nonlinear paradigm, where propagation depends on the magnitude of perturbation or its driving force. While the linear part remains industrially important (e.g., eyewear and architectural glass for optics), frontline research moves to nonlinear phenomena. IMS is undergoing that transition now with the rise of FAIMS, which should continue as the fundamental understanding improves, new modalities and applications emerge, and more instrumentation is introduced by vendors. Modifying and augmenting FAIMS separations through vapor dopants that render ion mobilities less linear is becoming routine. I expect this area to advance, extending to more specific interactions and to complexation with solution additives. Another route to higher separation power is integrating FAIMS with conventional IMS; proliferation of both technologies would make such 2-D platforms common. Along with mass spectrometry and conventional IMS, FAIMS will address increasingly large macromolecules, including proteins and their complexes.

Shvartsburg, Alexandre A.

2012-12-01T23:59:59.000Z

397

Renewable Energy Finance Tracking Initiative (REFTI): Snapshot of Recent Geothermal Financing Terms, Fourth Quarter 2009 - Second Half 2011  

SciTech Connect (OSTI)

This report is a review of geothermal project financial terms as reported in the National Renewable Energy Laboratory's Renewable Energy Finance Tracking Initiative (REFTI). The data were collected over seven analysis periods from the fourth quarter (Q4) of 2009 to the second half (2H) of 2011.

Lowder, T.; Hubbell, R.; Mendelsohn, M.; Cory, K.

2012-09-01T23:59:59.000Z

398

DIS2001 Bologna 2701 May 2001  

E-Print Network [OSTI]

PDFs Herwig5.9: * MRSA for the proton * SaS1D­LO parametrization of #3; PDFs * GRV­LO parametrization(#22; 2 =Q 2 ) non­pQCD #24; Q -4 Lepto: * MRSA for the proton * direct photons only ­ Dorian Kcira

399

Page 1 of 7 Installation Name ____________________________________________________________  

E-Print Network [OSTI]

chlorine q liquid flow q ammonia (NH3) q other: _______________ q gas velocity q carbon dioxide (CO2) q other: _______________ q liquid velocity q carbon monoxide (CO) q other: _______________ b) Have any modular q loop q other:______________ #12;06/07/99 Page 3 of 7 c) The system is q 4-20 mA control wiring q

US Army Corps of Engineers

400

Optoelectronic Oscillators and Their Applications to 60-GHz Fiber-Fed  

E-Print Network [OSTI]

Optoelectronic Oscillators and Their Applications to 60-GHz Fiber-Fed Wireless Systems Kwang;Optoelectronic Oscillators and Their Applications to 60-GHz Fiber-Fed Wireless Systems by Kwang-Hyun Lee-1-2. Oscillator phase noise limited by resonator's Q.............................4 1-2. Optoelectronic oscillators

Choi, Woo-Young

Note: This page contains sample records for the topic "q4 q1 q1" 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.


401

S()l.9(.....Mws\\.i ,,~-Io;;"(k'-t-v liw.ikJ rea.c;(i6<-.S IAk cevr;;Jtr ~ -two ~~oJrytQl/i; a-... ~ 1{u. r-r{i&/tJ w.eei, ~  

E-Print Network [OSTI]

..fI,A- 1~.{i!)oQ4ecl. -10::'/ (11 l.,':PNA. Cal,! wti-vt (/k~ b..l ] SetH f)Jo.' 7T ~a.\\ rS,-lMo b'4rk

Potsdam, Universität

402

SC4250: Probabilistic Models in the Life Sciences Instructor: A. Abate  

E-Print Network [OSTI]

SC4250: Probabilistic Models in the Life Sciences Instructor: A. Abate Q4, S2, AC 2011-12 1 Contact · Office: room 8C-4-24 · Phone: +31-15-27-85606 · Email: a dot abate at tudelft dot nl 2 General

Abate, Alessandro

403

The Board of Trustees of Oregon State University 526 Kerr Administration Building  

E-Print Network [OSTI]

policies. Other agenda items include discussion of the FY15 operating budget, 2015-17 state funding process items include review and approval of the FY15 and FY16 committee work plan and meeting schedule and the FY14 Q4 operating management report and review and recommendation for Board approval of a proposed

Escher, Christine

404

REGIONAL IMPACTS OF THE GLOBAL CARBON STAKES: LONG-TERM PROSPECTIVE WITH THE TIMES INTEGRATED ASSESSMENT MODEL  

E-Print Network [OSTI]

, the progress of primary energy consumption and the energy mix. This paper compares global efforts on CO2 and Nadia MaĂŻzi 33rd IAEE International Conference: "The future of energy: global challenges, diverse the carbon constraints. JEL O21, Q29, Q4, Q54, Q58 Keywords Global energy system, CO2 mitigation targets

Paris-Sud XI, Université de

405

Small mammal response to red imported fire ant removal in a grassland community  

E-Print Network [OSTI]

points located in bare-ground areas than to those in areas dominated by grass Q = 4. 21, P & 0. 05, Q. f. = 2). Number of small maminal captures was independent of cover class in August, 1989 (Q = 3. 377, NS, g. f. = 6), April, 1990 (Q = 6. 721, NS, Il...

Killion, Michael James

1992-01-01T23:59:59.000Z

406

113-0033 7-3-1 153-8505 4-6-1-Ee405  

E-Print Network [OSTI]

13, Q2 87.8% Q4 12 6. MR CG MR HMD #12; 13. [1] R. Azuma "A Survey] R. Azuma, Y. Baillot, R. Behringer, S. Feiner, S. Julier, and B. MacIntyre "Recent Advances. Vlahakis, N. Ioannidis, J. Karigiannis, M. Tsotros, M.l Gounaris, D. Stricker, T. Gleue, P. Daehne and L

Tokyo, University of

407

The Smith Normal Form of the Incidence Matrix of Skew Lines in PG(3, q)  

E-Print Network [OSTI]

The Smith Normal Form of the Incidence Matrix of Skew Lines in PG(3, q) Peter Sin, University. In our case D = q4I. #12;Smith normal forms A, L define endomorphisms of the free Z-module on lines. Cokernel of A is called the Smith group and the torsion subgroup of the cokernel of L is known

Sin, Peter

408

Bill Bradbury Jennifer Anders  

E-Print Network [OSTI]

Updated Resource Needs Assessment Draft Resource and Action Plan Public Comment Q3 Q4 Q2 2015 Draft PlanForecast ModelModel EBaseline Energy Efficiency ResourceEnergy Efficiency Resource Potential AssessmentGenerating Resource Potential AssessmentAssessment Supply Side Resource Cost & Availability gygy efficiencyefficiency

409

Deutsche Telekom launches new integrated location-based services in selected markets across Europe  

E-Print Network [OSTI]

Deutsche Telekom launches new integrated location-based services in selected markets across Europe in Q4 last year, services will be available in 2010 in the Netherlands and other countries Deutsche and check the weather in the area. Deutsche Telekom's LBS service is truly for the mass market. From launch

Deutschmann, Rainer

410

Questions of Indigeneity and the (Re)-Emergent Ch'orti' Maya of Honduras  

E-Print Network [OSTI]

). Conversely, some argue that states such as Mexico and El Salvador have created more inclusive definitions of indigenousQ4 to manage potentially unruly, impoverished populations (Hale 2005, 2006b; Speed 2005; Mart?´nez Novo 2006; Tilley 2006). A strict social... their natural resources; and representation in Congress (Anderson 2007:393–394). Thus, while the state was accepting international investments for indigenous and eco-tourism, including support for the multinational Ruta Maya (Mayan Trail) project, it found...

Metz, Brent

2010-01-01T23:59:59.000Z

411

Factors influencing the growth of Sclerotium rolfsii in various soils  

E-Print Network [OSTI]

~ hssishanh taefossox of hho loyarhasah of Plant Sqrsiahogf ael Pnthologye 'glhRS 4 05ICSN%. XgSSII00%4 4 ~ t ~ 4 g 4 4 4 4+ ~ ~ 0 ~ 4 ~ ~ 1 I t 4* ~ +t gggS4F Q%%4%$$ O. 0 0 ~ 4 0 4 4 ~ ~ f 4 % ~ ~ 1 4'1 0 II 856% 4NP %@IIX@) 's ~ ~ ~ s a e'e ~ i o + t a...

Menon, Sankara Kochukrishna

1953-01-01T23:59:59.000Z

412

hepph/9512272 ON THE THEORETICAL STATUS OF  

E-Print Network [OSTI]

(š)N scattering processes are described by six further structure functions W š;\\Sigma 2 , xW š;\\Sigma 3 , F 2Z structure at short distances. Since both charged leptons (e \\Sigma ; ¯ \\Sigma ) and neutrinos (š; š) may ) collects couplings and propagator terms, e.g. P l \\Sigma ;fl (Q 2 ) = 2�ff 2 =Q 4 , P š;W +(Q 2 ) = G 2 F M

413

How to Observe with LWA-1 Steve Ellingson  

E-Print Network [OSTI]

B bandwidth ~ 2/3 rate) Output samples are 8-bit I + 8-bit Q This mode sets the data recorder throughput localization Science Uses Long duration "total power" transients Solar Riometry * Could also be done with beams n = 1..4 Each beam gets two "tunings" (10-88 MHz) Output samples are I4+Q4 250 kSPS -- 19.6 MSPS

Ellingson, Steven W.

414

Playas Grid Reliability and Distributed Energy Research  

SciTech Connect (OSTI)

The future looks bright for solar and renewable energies in the United States. Recent studies claim that by 2050, solar power could supply a third of all electricity demand in the country’s western states. Technology advances, soft policy changes, and increased energy consciousness will all have to happen to achieve this goal. But the larger question is, what would it take to do more throughout the United States? The studies tie future solar and renewable growth in the United States to programs that aim to lower the soft costs of solar adoption, streamline utility interconnections, and increase technology advances through research and development. At the state and local levels, the most important steps are: • Net metering: Net metering policies lets customers offset their electric bills with onsite solar and receive reliable and fair compensation for the excess electricity they provide to the grid. Not surprisingly, what utilities consider fair is not necessarily a rate that’s favorable to solar customers. • Renewable portfolio standards (RPS): RPS policies require utilities to provide a certain amount of their power from renewable sources; some set specific targets for solar and other renewables. California’s aggressive RPS1 of 33% renewable energy by 2020 is not bankrupting the state, or its residents. • Strong statewide interconnection policies: Solar projects can experience significant delays and hassles just to get connected to the grid. Streamlined feasibility and impact analysis are needed. Good interconnection policies are crucial to the success of solar or renewable energy development. • Financing options: Financing is often the biggest obstacle to solar adoption. Those obstacles can be surmounted with policies that support creative financing options like third-party ownership (TPO) and property assessed clean energy (PACE). Attesting to the significance of TPO is the fact that in Arizona, it accounted for 86% of all residential photovoltaic (PV) installations in Q1 20132. Policies beyond those at the state level are also important for solar. The federal government must play a role including continuation of the federal Investment tax credit,3 responsible development of solar resources on public lands, and support for research and development (R&D) to reduce the cost of solar and help incorporate large amounts of solar into the grid. The local level can’t be ignored. Local governments should support: solar rights laws, feed-in tariffs (FITs), and solar-friendly zoning rules. A great example of how effective local policies can be is a city like Gainesville, Florida4, whose FIT policy has put it on the map as a solar leader. This is particularly noteworthy because the Sunshine State does not appear anywhere on the list of top solar states, despite its abundant solar resource. Lancaster, California5, began by streamlining the solar permitting process and now requires solar on every new home. Cities like these point to the power of local policies, and the ability of local governments to get things done. A conspicuously absent policy is Community Choice energy6, also called community choice aggregation (CCA). This model allows local governments to pool residential, business, and municipal electricity loads and to purchase or generate on their behalf. It provides rate stability and savings and allows more consumer choice and local control. The model need not be focused on clean energy, but it has been in California, where Marin Clean Energy7, the first CCA in California, was enabled by a state law -- highlighting the interplay of state and local action. Basic net metering8 has been getting a lot of attention. Utilities are attacking it9 in a number of states, claiming it’s unfair to ratepayers who don’t go solar. On the other hand, proponents of net metering say utilities’ fighting stance is driven by worries about their bottom line, not concern for their customers. Studies in California10, Vermont11, New York12, and Texas13 have found that the benefits of net metering (like savings on investments

Romero, Van; Weinkauf, Don; Khan, Mushtaq; Helgeson, Wes; Weedeward, Kevin; LeClerc, Corey; Fuierer, Paul

2012-06-30T23:59:59.000Z

415

.--,' , Meteorological Observatory 11 ,r . / r' . , ',~A.Iv' .',1 '" 7 , " "'(.)7()(} ES'T  

E-Print Network [OSTI]

)c 1.1 35 OF t-.JNvI/ R.H. '1'.:: '1c Ppn. Liq. 1900 24 hr, Mov. mi, Prevo DiL T 'y,. ~\\0'\\\\~p-p-n-.--c~:-4~---~--·~-~~--------~~-------7~~-------i-v~·~is-, ~) 0, in. in. mi. ~!; mi.~5 mi. Vis. tr in. I~M (~ mi. ,.;15 mi. j 0 mi. #12;t-:~~ T~:l'IY1S c1Q jq 1vJ: M TUNJ ,,;15 J [I II) '. q4

Thompson, Anne

416

A study of experimental techniques for analyzing threaded thick shell connections  

E-Print Network [OSTI]

and Solder Tabs Bottom of Encapsulated Gage Assembly. One Gage Assembly Bonded in Pin of Drill Collar Strain Gage Instrumented Drill Collar Pin Dimensions Used in Sample Calculations. Test Setup for Strain Gage Make-Up Data Inside Surface Hoop Stress vs... the specimens was limited to an in- side diameter of two inches. the strain gazes were prewired before being attached to the fixture. After the lead wire was soldered to the gQ4 aa Figure 3. Inside of Fixture Used to Bond Strain Gages. Figure 4. Assembled...

Asbill, William Thomas

2012-06-07T23:59:59.000Z

417

Process Integration of Industrial Heat Pumps  

E-Print Network [OSTI]

, COP Carnot T W---i Figure 6. Grand composite curve with electric drive system The COP for a prime heat system assumes the exhaust heat from the driver is used in the process. The COP is then the ratio of total heat delivered (Q4 + QZ.... Nomenclature is as given in Figures 6-8. The electric drive heat pump is the most widely understood system. It has the advantage of simplic ity and requires little disruption of the process. However, an electric drive may upset the utility power/heat...

Priebe, S. J.; Chappell, R. N.

418

Analytical solutions of compacting flow past a sphere  

E-Print Network [OSTI]

of Laplace’s equation is defined as the solution of ??2? = ?(3)(x) (3.16) where ?(3)(x) is the three-dimensional Dirac delta function. The fundamental solution is ? = 1 4pir (3.17) where r = |x|. This fundamental solution satisfies ?2? = 0 for r > 0... (4.8) where Q gives the total mass flux over the surface r = a and n is the outward normal. It is assumed that vs ? 0 and P ? 0 as |x| ? ?. This has solution A = ? Q 4pi , B = 0, (4.9) 8 John F. Rudge so that vs = Qx 4pir3 , q = 0, P = 0, (4...

Rudge, John F.

2014-04-03T23:59:59.000Z

419

The preparation and analysis of ammonia base sulfite pulping liquor  

E-Print Network [OSTI]

NH3 Concentrations . . . . . , ~ . ~ . . ~ ~ . ~ q IV The Distribution of S02 in a 2. 82$ RR3 Solution for Various Total SO2 Concentrations . . . . . . , . . . ~ . . . 31 FIGURES l. Variation of pH with Percent NH3 in Solution. . . . . ~. . . 25... 2. Variation of pH with S02 Concentration in Solutions of Various NH Concentrations . . . . ~ . . . ~ . ~ o ~ . o . ~ 27 3 ~ Composition of Solutions to give a Constant pH of T and 2. 5 , ~ 2Q 4. The Variation of the Ratio of Free S02 to Total SO2...

Honstead, John Frederick

1950-01-01T23:59:59.000Z

420

The toxicity and control of peavine, Astragalus emoryanus  

E-Print Network [OSTI]

, . . . . . . . . . . ~ ~ . . o 51 8% 'fCXZCXff AND COgfRg. lF Plkvlgg~ kKQQHR XlQIQIR Ths predestine of range livootook ie the ~)or indwtry of the ~Q4$ds area of QMC 'tones, Nskh of 'tbo Kighlands area is vithin yroeidio County~ nbioh 1e ono of tbo larger eonntios..., ~AIM, prllWlyLll1 UjaII~ ~ 1 texlo Co eatage, sheep, and geste in looal areas, and eas ohoson as tbe sob)oat fer this invostigati~ Tbs speoiosy Q ~ggmmmmk, ~ separated frca Je gg~~ in 1927 awhile tho fever spooies oonstltntod the balk af tho...

Gray, Robert G

1951-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q1" 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.


421

Growth of sheets in 3D confinements - a model for the C-S-H meso 2 structure  

E-Print Network [OSTI]

- and dicalcium silicate surfaces on particle aggre-41 gation [8]. Particle based models have also been used by the group of Ulm to successfully interpret nano42 indentation results [9]. Small-angle neutron scattering data of cement paste has been interpreted... -vectors, both curves show a q?4 dependence which corresponds to203 the experimental Porod regime. The simulated data is compared to experimental small-angle neutron204 scattering data for cement from Allen et al. (dashed) [30]. For large and intermediate...

Etzold, Merlin A.; McDonald, Peter J.; Routh, Alexander F.

2014-06-21T23:59:59.000Z

422

Economics of Cattle Feeding Systems for West Texas.  

E-Print Network [OSTI]

'9 1. /@ 2". * 4''@~ fQ4Q~ bchf~ '6 $9 "4; ,p*, d Economics of Cattle Feeding Systems for West Texas ,,5~'* ,LI~~ 3 TEXAS AGRICULTURAL EXPERIMENT STATION R. D. LEWIS, DIRECTOR, COLLEGE STATION, TEXAS SUMMARY The purpose of the study... reported here is to assist West Texas farmers to appraise the opportunities for marketing sorghum grain through cattle at a profit. To do this, systems of cattle feeding were selected which "fitted in" with cash-crop pro- duction, These systems were...

Hughes, W. F.; Fisher, C. E.; Marion, P. T.; Magee, A. C.

1957-01-01T23:59:59.000Z

423

DOE/EIA-0202(87/4Q) Energy Information Administration Short-Term  

Gasoline and Diesel Fuel Update (EIA)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"Click worksheet9,1,50022,3,,,,6,1,,781Title:DOBEIA-0202(83/4Q) Short-Term Energy3/P1Q)6/1Q)7/1Q)3Q)4Q)

424

DOE/EIA-0202(89/4Q) SHOKT-TERM  

Gasoline and Diesel Fuel Update (EIA)

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"Click worksheet9,1,50022,3,,,,6,1,,781Title:DOBEIA-0202(83/4Q) Short-Term2Q) Energy Information3Q)2Q)4Q)

425

Coal Distribution Database, 2008  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecemberSteam Coal Import96 4.87 1967-2010 ImportsCubic Feet) Oil3Q 20093Q4Q

426

Coal Supply Basin Destination State  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecemberSteam Coal Import96 4.87 1967-2010 ImportsCubic Feet) Oil3Q 20093Q4QReal

427

DOE/EIA-0321/HRIf Residential Energy Consumption Survey. Consumption  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82) Residential/HRIf

428

DOE/EIA-032171(84) Energy Information Administration Residential Energy  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)

429

DOE/EIA-0376(2006)  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6) November 2008

430

DOE/EIA-0376(2012)  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6) November

431

DOE/EIA-0482 Energy Information Administration  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6) November2

432

DOE/EIA-0555(94)71  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6) November271

433

DOE/EIA-0555(95)/2 Energy Consumption Series Measuring Energy Efficiency  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6) November2712

434

DOE/EIA-0555(96)/1  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6) November27121

435

DOE/EIA-0555(96)/2 Energy  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6) November271212

436

DOE/ELIA-0035(95/105), Monthly  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6)

437

DOETEIAO32l/2 Residential Energy Consumption Survey; Consumption  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6)k DOETEIAO32l/2

438

Data Files Monthly Natural Gas Gross Production Report  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6)k

439

December 2012 Short-Term Energy Outlook (STEO)  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6)k(STEO) ď‚· EIA

440

Demand and Price Outlook for Phase 2 Reformulated Gasoline, 2000  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6)k(STEO) ď‚·

Note: This page contains sample records for the topic "q4 q1 q1" 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.


441

Denver Gasoline and Diesel Retail Prices  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6)k(STEO) ď‚·272

442

Department of Defense Net Assessment Summer 2009  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr May Jun Jul(Summary) " ,"ClickPipelines AboutDecember 2005 (Thousand9, 2015Year109 AppendixCosts ofMarch2Q)4(82)6)k(STEO)

443

JOURNAL DE PHYSIQUE Colloque C3, supplkment au n09, Tome 48, septembre 1987  

E-Print Network [OSTI]

law of s c a t t e r i n g function, t h e spinodal theory and the dynamic scaling law. Article n ~ ) / i ) range (0.06rqr6 nm-1) w i t h tRe pulsed c o l d neutron small anqle scatterinq u n c t i o n p t t h e high $ side iin o t o i i y proportional t o q-2, q-4 an! 4-6.but i t obeys

Boyer, Edmond

444

Microsoft PowerPoint - C-Mod_quarterly_res_highlights_21.ppt  

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

AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE:1 First Use of Energy for All Purposes (Fuel and Nonfuel),Feet) Year Jan Feb Mar Apr MayAtmospheric Optical Depth7-1D: VegetationEquipment Surfaces andMapping theEnergyInnovationMichaelGE1PlanARM A.Highlights, Plans, andQ3Q4

445

The biological activity of hexahydrocoenzyme Q? in preventing the symptoms of vitamin E deficiency in chicks and poults  

E-Print Network [OSTI]

2. Basal + H CoQ~ 6 3. Basal + E 5 6 6 6 6 6 100 100 16 16 0 0 ]7 0 16 1. Basal diet is the unsupplemented Torula yeast ration. H CoQ~ represents &00 mg H 6CoQ&/&g body weight/day. E represents dl n-tocopherol acetate equivalent to 1 gm.../Kg diet. 2. Chicks dying in the first week were not included in this study. 37 Figure 3. Fffects of H 6CoQ4 and vitamin E on cathepsin activity (in units)I- in chicks fed a vitamin E deficeint diet. 120 Males Females @~III T*r. & 100 80 60 w 40...

Larsen, Maureen Hughes

2012-06-07T23:59:59.000Z

446

Low cost computer interface using eye tracking  

E-Print Network [OSTI]

/ANO PBO/Aa Pe I/AS PB2/AIO Pea/AII PB4/A12 Pea/Aia Pea/AI 4 Per/A15 PAOIIGS e Q 5 ii ( & 0 S MC88HC11A8 Pin Assignments (52 pin PLCC) Q41 ge Qae Q44 /44/ 042 04' fae/ Q4i 038 039 Qa) 089 Qaa 049 /DI 01 03 05 O' SO" 000' 0'0' ~I Oi..., Q? 0? 019 08 /De Q~) 026 Qze Q24 022 Qzo Ga 028 /07 boa 021 Pin assignments for 52- pin chip carrier socket Figure 7. Pin assignments of the microcontroller 24 tor and its line assembler facilities. Later coding and software tests were...

Zee, Bernard Chan Heng

2012-06-07T23:59:59.000Z

447

Refinement of freeway surveillance & control techniques by optical speed and occupancy detection  

E-Print Network [OSTI]

$pv't 1", h 'so''jT 07 7'77TT&(Ar S, p~rv; 7 Saon E: COP'SOJ ' j'CSIPZQ 7 3Y OTTTCAL SPT. " 'D '7'~D OCCU ACT D. '2~CT '-'i& A Thesis KZU77PTS GEANT COOM. ~'"' Subm tted to the Grec', uate Co13eSo o. ' the Texas l&Q4 Ur. iver sty in parti?1... stion. ". , " HRD Record 11o. 15 t, p. 2 t-)'(, lo67. CRAPTER II FFASIBII Ilv Ai, ALYSIS This cha?ter will d. eal with the Zeasibili+y of using a simple opt. i- cal speed trap as a s?pplement to pot detecLion in the measurement of traf'fic flow...

Courage, K. G

1968-01-01T23:59:59.000Z

448

202-328-5000 www.rff.orgSector Effects of the Shale Gas Revolution in the United States  

E-Print Network [OSTI]

This paper reviews the impact of the shale gas revolution on the sectors of electricity generation, transportation, and manufacturing in the United States. Natural gas is being substituted for other fuels, particularly coal, in electricity generation, resulting in lower greenhouse gas emissions from this sector. The use of natural gas in the transportation sector is currently negligible but is projected to increase with investments in refueling infrastructure and natural gas vehicle technologies. Petrochemical and other manufacturing industries have responded to lower natural gas prices by investing in domestically located manufacturing projects. This paper also speculates on the impact of a possible shale gas boom in China. Key Words: shale gas, electricity, transportation, and manufacturing JEL Classification Numbers: L71, L9, Q4 © 2013 Resources for the Future. All rights reserved. No portion of this paper may be reproduced without permission of the authors. Discussion papers are research materials circulated by their authors for purposes of information and discussion.

449

Measurement of the Electric Charge of the Top Quark in $\\boldsymbol{t\\bar{t}}$ Events  

E-Print Network [OSTI]

We present a measurement of the electric charge of top quarks using $t\\bar{t}$ events produced in $p\\bar{p}$ collisions at the Tevatron. The analysis is based on fully reconstructed $t\\bar{t}$ pairs in lepton+jets final states. Using data corresponding to 5.3 $\\rm fb^{-1}$ of integrated luminosity, we exclude the hypothesis that the top quark has a charge of $Q=-4/3\\,e$ at a significance greater than 5 standard deviations. We also place an upper limit of 0.46 on the fraction of such quarks that can be present in an admixture with the standard model top quarks ($Q=+2/3\\,e$) at a 95\\% confidence level.

D0 Collaboration

2014-09-25T23:59:59.000Z

450

Iterative cellular array multiplier using overlapped four-bit scanning technique and its application  

E-Print Network [OSTI]

. Qg Bs Q4 l4 Gs Hz G4 Hs G, Gp Hp Bp 0 FA8 FA4 FA1 FAO 1 Qrs Qw Brz Product 0 Hzs Hl 1 Gg Hs 0 FA16 FA12 FA9 Fig. 16. Logic Diagram of the Control Signals and the First Level CSA. 38 Z X V T R M K I H Y W U S N L I(+&& Q CSA CSA CSA...-tCSA + /sCLA (2. 38) (2+ 2 x 2+ 11)hg = 176g. Hence, the total delay time of the nonoverlapped two-bit scanning multiplier is /3T = +D-F/F + 8 X (17 + +D ? F/F) (4+ 21 x 8)A = 1726 . (2. 39) The occupied area is proportional to the (m + 1) operand...

Kim, Wu Woan

2012-06-07T23:59:59.000Z

451

Field Notes, Middle America (1956-1968)  

E-Print Network [OSTI]

jljUlSu IT & dL ISO2s &&dLdI f{. L & ? P'3< a3Lc t xLQc32s_? 42T3{3k VL!e Cat5 j/b) [&vvL,L t e{Q 4Ur te{Qc{3c2YLc p&?2e2&Q X r ?Z t e...

Davis, William B.

2012-04-09T23:59:59.000Z

452

Semiempirical range and stopping power values for heavy ions  

E-Print Network [OSTI]

0 CO CCI CO O O O rn UJ O r mU. m ~ ~ ~ OOOOO cl N O I N 4 O' ICI N w ~ Q ~ N ~ U 0 Q If Cl CO 0' M 0' In ICI ~ ~ 0 000 ~ ~ ~ Ln or o o Lnr o UO N Z O' pCI rn N w ~ ~ ~ ~ Q 4 ~ 0 N CCI OI 0 0 r UI Cr rll m ~ ~ N 0 m... O ~ ~ N U'. r co I ~ ~ N 0 O UO CO CO Q N N ~ ~ nd NI 0 0 ILI C3 CO 0 0 t CO r UJ O' rh ~ ~ cn 0 N 'Z \\ ~ CO m rn m ~ ~ U, 0 N CO cn N N ~ ~ 0 0 U I I 4 I ? 4 4 G V 4 a a LU N IU UJ CO O Lf 0 UJ...

Schilling, Ralph Franklin, III

2012-06-07T23:59:59.000Z

453

The effect of artificial drying temperature on the quality of early harvested pecan kernels  

E-Print Network [OSTI]

al C N 0 I aS 0, 0, N aS C N O 0 CS 0 19 who 0 0 0 u7 w K (o c& &codd~ 0 4 0 Cl 88881 o 2 sante~ ? e zaqunH rd I dl A (d (d o 0 4 Q 0 0 ) rn 4 Q ~ (d (d (d ~ I 0 Q xv (d 0 4 Q. C4 wE CE 0 g 0 CA 0 Q (d ~ 4... (d go O O 4 (rl '0 ) (d 4 o (d o + rfr Q ~ N N ~ 0 g l g (dan o (d ~4 rn (d 4 ~ (d &D Cd e 4 (d ~ rn 0 2 ~0 4 w o N Q 4 (d 0 o %(o cd 0 dr C4 g4 N cd g (d (d O 0 A o ~ 20 Cz Ea&40 0 0 0 If& D D lP C& (XI...

McLean, Roy William

2012-06-07T23:59:59.000Z

454

Uncertainty Quantification of the Pion-Nucleon Low-Energy Coupling Constants up to Fourth Order in Chiral Perturbation Theory  

E-Print Network [OSTI]

We extract the statistical uncertainties for the pion-nucleon ($\\pi N$) low energy constants (LECs) up to fourth order $\\mathcal{O}(Q^4)$ in the chiral expansion of the nuclear effective Lagrangian. The LECs are optimized with respect to experimental scattering data. For comparison, we also present an uncertainty quantification that is based solely on \\pin{} scattering phase shifts. Statistical errors on the LECs are critical in order to estimate the subsequent uncertainties in \\textit{ab initio} modeling of light and medium mass nuclei which exploit chiral effective field theory. As an example of the this, we present the first complete predictions with uncertainty quantification of peripheral phase shifts of elastic proton-neutron scattering.

K. A. Wendt; B. D. Carlsson; A. Ekström

2014-10-02T23:59:59.000Z

455

The effect of benzene hexachloride-DDT spray on the insect population and the cotton plant  

E-Print Network [OSTI]

IOXSMI) ~ oatteeasoeoe ~ sasooaaeeo?eeosotap ~ of ~~ ~ed ~ INK ~IILX%4 @5+ W N@l@+~)tasaosesagfoat' ~ aaO3ya9u of T~ ~) (T3O38 E~+mA)ya. . . t a3ao fcneQ 4o he ~ effeet4ve Se ooutraQ5ng the hgt waepLl g@@gcigg @~i~ Bobcat?aul 4hs oottou a~ ~ ~gggg ~? X... pears Caro haa heeu cL yuMcraX 4zemk Rn menp areas frau the uae of Gusts 4o %he uae of ~ fouuuhrhious or cdl ema1sious Ln cotton Sxreo4 eoutaeX. $5s usa 4he msem uaeL to so%vs the geohbe of vol em%4 Beck~ 9e 4he spgf;oe4tou ef e chN4 8ytzya seu ha ep...

Lloyd, Edwin Phillips

1952-01-01T23:59:59.000Z

456

An accounting system for motor taxicab companies  

E-Print Network [OSTI]

gQ 4Qg~p~", . W l' 'I l. ~j I "'fYlATl Q~TQJQ Q;gtpl TQI'M Joe ". . M~tvxa . *. a~is , , ". itlPOV" ' " tel . ,' ~ 'z". . i' ":~&1 O'WtC", L" 1GGN "K!~20(3: Chairman ef Ccmmi&ee A'; AQCOD&F", Fi !'TZ. "~; M!& 'K)TOH TAX1CA3 C':"iP~u'KFJ Joe...~, '", 1"G;, *OZ, "&:. 0'i? . G?". . 'i, '""'. GS 99 "tX:". ;l', L t;Q "C:-"&':. ". uQ ?"2'NilHl 'ilO:. "'". p~ 'ZO "Ql':. "~~:j(F~)CQ. ~Hi'""LGQ :" OX". :% G"-%U . ACOl'QG PAGE n e Drcwe'~e %eat ter Bbeof Gash Weet~~t, end '. 'queutue Jeux~ Gush...

Morris, Joe Milton

1950-01-01T23:59:59.000Z

457

T"hy"la Issue 6  

E-Print Network [OSTI]

S C J J ,a r t- 0 " D ,D '- t) rt O "J O O a I J J CT I- i| -4 T3 -i) O " - t) 0) -i> O r tX J ? 3" r+ X I? -< H H B W H Ft W O CD CT C (1 r tC HI ^ , r t (l h M 3 ? B Q.I Q 3 H B... Q 4 P O H 3 (D ;J S U W 3 4 M O M O .O a M 3 p v C f+ a 0) C O n m n O S C L - i) !-? ?l- ? 3 W r r H H i+ H H H O J H -3 H -C D O H - CD 3 3 I? '3 H - - b ? I? ' O - 2^ J...

Multiple Contributors

2013-11-27T23:59:59.000Z

458

FY12 Quarter 3 Computing Utilization Report – LANL  

SciTech Connect (OSTI)

DSW continues to dominate the capacity workload, with a focus in Q3 on common model baselining runs in preparation for the Annual Assessment Review (AAR) of the weapon systems. There remains unmet demand for higher fidelity simulations, and for increased throughput of simulations. Common model baselining activities would benefit from doubling the resolution of the models and running twice as many simulations. Capacity systems were also utilized during the quarter to prepare for upcoming Level 2 milestones. Other notable DSW activities include validation of new physics models and safety studies. The safety team used the capacity resources extensively for projects involving 3D computer simulations for the Furrow series of experiments at DARHT (a Level 2 milestone), fragment impact, surety theme, PANTEX assessments, and the 120-day study. With the more than tripling of classified capacity computing resources with the addition of the Luna system and the safety team's imminent access to the Cielo system, demand has been met for current needs. The safety team has performed successful scaling studies on Luna up to 16K PE size-jobs with linear scaling, running the large 3D simulations required for the analysis of Furrow. They will be investigating scaling studies on the Cielo system with the Lustre file system in Q4. Overall average capacity utilization was impacted by negative effects of the LANL Voluntary Separation Program (VSP) at the beginning of Q3, in which programmatic staffing was reduced by 6%, with further losses due to management backfills and attrition, resulting in about 10% fewer users. All classified systems were impacted in April by a planned 2 day red network outage. ASC capacity workload continues to focus on code development, regression testing, and verification and validation (V&V) studies. Significant capacity cycles were used in preparation for a JOWOG in May and several upcoming L2 milestones due in Q4. A network transition has been underway on the unclassified networks to increase access of all ASC users to the unclassified systems through the Yellow Turquoise Integration (YeTI) project. This will help to alleviate the longstanding shortage of resources for ASC unclassified code development and regression testing, and also make a broader palette of machines available to unclassified ASC users, including PSAAP Alliance users. The Moonlight system will be the first capacity resource to be made available through the YETI project, and will make available a significant increase in cycles, as well as GPGPU accelerator technology. The Turing and Lobo machines will be decommissioned in the next quarter. ASC projects running on Cielo as part of the CCC-3 include turbulence, hydrodynamics, burn, asteroids, polycrystals, capability and runtime performance improvements, and materials including carbon and silicone.

Wampler, Cheryl L. [Los Alamos National Laboratory; McClellan, Laura Ann [Los Alamos National Laboratory

2012-07-25T23:59:59.000Z

459

Quantum gravity and inventory accumulation  

E-Print Network [OSTI]

We begin by studying inventory accumulation at a LIFO (last-in-first-out) retailer with two products. In the simplest version, the following occur with equal probability at each time step: first product ordered, first product produced, second product ordered, second product produced. The inventory thus evolves as a simple random walk on Z^2. In more interesting versions, a p fraction of customers orders the "freshest available" product regardless of type. We show that the corresponding random walks scale to Brownian motions with diffusion matrices depending on p. We then turn our attention to the critical Fortuin-Kastelyn random planar map model, which gives, for each q>0, a probability measure on random (discretized) two-dimensional surfaces decorated by loops, related to the q-state Potts model. A longstanding open problem is to show that as the discretization gets finer, the surfaces converge in law to a limiting (loop-decorated) random surface. The limit is expected to be a Liouville quantum gravity surface decorated by a conformal loop ensemble, with parameters depending on q. Thanks to a bijection between decorated planar maps and inventory trajectories (closely related to bijections of Bernardi and Mullin), our results about the latter imply convergence of the former in a particular topology. A phase transition occurs at p = 1/2, q=4.

Scott Sheffield

2011-08-10T23:59:59.000Z

460

Minimally non-local nucleon-nucleon potentials with chiral two-pion exchange including Delta resonances  

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

We construct a coordinate-space chiral potential, including $\\Delta$-isobar intermediate states in its two-pion-exchange component up to order $Q^3$ ($Q$ denotes generically the low momentum scale).The contact interactions entering at next-to-leading and next-to-next-to-next-to-leading orders ($Q^2$ and $Q^4$, respectively) are rearranged by Fierz transformations to yield terms at most quadratic in the relative momentum operator of the two nucleons. The low-energy constant multiplying these contact interactions are fitted to the 2013 Granada database, consisting of 2309 $pp$ and 2982 $np$ data (including, respectively, 148 and 218 normalizations) in the laboratory-energy range 0--300 MeV. For the total 5291 $pp$ and $np$ data in this range, we obtain a $\\chi^2$/datum of roughly 1.3 for a set of three models characterized by long- and short-range cutoffs, $R_{\\rm L}$ and $R_{\\rm S}$ respectively, ranging from $(R_{\\rm L},R_{\\rm S})=(1.2,0.8)$ fm down to $(0.8,0.6)$ fm. The long-range (short-range) cutoff regularizes the one- and two-pion exchange (contact) part of the potential.

Piarulli, M; Girlanda, L; Schiavilla, R; Perez, R Navarro; Amaro, J E; Arriola, E Ruiz

2015-02-01T23:59:59.000Z

Note: This page contains sample records for the topic "q4 q1 q1" 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

The Giant Gemini GMOS survey of z>4.4 quasars - I. Measuring the mean free path across cosmic time  

E-Print Network [OSTI]

We have obtained spectra of 163 quasars at $z_\\mathrm{em}>4.4$ with the Gemini Multi Object Spectrometers on the Gemini North and South telescopes, the largest publicly available sample of high-quality, low-resolution spectra at these redshifts. From this homogeneous data set, we generated stacked quasar spectra in three redshift intervals at $z\\sim 5$. We have modelled the flux below the rest-frame Lyman limit ($\\lambda_\\mathrm{r}<912$\\AA) to assess the mean free path $\\lambda_\\mathrm{mfp}^{912}$ of the intergalactic medium to HI-ionizing radiation. At mean redshifts $z_\\mathrm{q}=4.56$, 4.86 and 5.16, we measure $\\lambda_\\mathrm{mfp}^{912}=(22.2\\pm 2.3, 15.1\\pm 1.8, 10.3\\pm 1.6)h_{70}^{-1}$ proper Mpc with uncertainties dominated by sample variance. Combining our results with $\\lambda_\\mathrm{mfp}^{912}$ measurements from lower redshifts, the data are well modelled by a simple power-law $\\lambda_\\mathrm{mfp}^{912}=A[(1+z)/5]^\\eta$ with $A=(37\\pm 2)h_{70}^{-1}$ Mpc and $\\eta = -5.4\\pm 0.4$ between $z=2.3$...

Worseck, Gábor; O'Meara, John M; Becker, George D; Ellison, Sara; Lopez, Sebastian; Meiksin, Avery; Ménard, Brice; Murphy, Michael T; Fumagalli, Michele

2014-01-01T23:59:59.000Z

462

http://homepages.inf.ed.ac.uk/stark Webquines, The Collatz Graph  

E-Print Network [OSTI]

Iy2bkwAyULxfaPclFmQQllYvBh9qlz zX9B0GIBv1pC4bQAbzpXduFoANZEAG5tzAnVR4UMr7FlaAUT78BkwB5w7mTwaz72CaC8BNIMGR7ADon0HcAAiAfwPuP4OXPz1f/n48vcMevJzoA30HD6cPMIhLB2QwIy2bkwAyULxfaPclFmQQllYvBh9qlz zX9B0GIBv1pC4bQAbzpXduFoANZEAG5tzAnVR4UMr7FlaAUT78BkwB5w7mTwaz72CaC8AGXqkWATDM/QgXx+zBFaUc poMz+hmvqI7gHFRL33yiMhTnqQ4qCzUE1DJVQC0

Stark, Ian

463

The cardiovascular effects of intravenous hemoglobin administration in dogs  

E-Print Network [OSTI]

- 0 A td 8 rd C 0 rd 0 W 0 + rd 4I w rd 0 0 0 tlt A M 6 P O 0 '0 W 8 0 8 0 '6 0 8 rd . n I 8 M rd 0 8 8 Ill rd rd 4I A 8 0 0 E-r W 8 0 0 W III 6 Q r-I V CI 6 Q 4 U 0 0 4I OA Z Q 8 0 0 0 0 +I +I +I +I 0 M M... M 0 0 0 I I 8 8 4I Il t4 I4 A I I 8 M 0 A I I Cl '0 A A I I M '0 0 8 0 0 0 0 0 0 0 0 +I +I +I +I +I +I +I +I 0 0 O 0 H H 0 0 lt +I g W 0 ~ O tent C4 g '0 8 Ul 0 Ew 8 O W 0 8 C E 0 '0 rd 0 g 8 . R . nA 0 0 0 4 8 4r...

Moody, Gary Monroe

1979-01-01T23:59:59.000Z

464

Pauli graph and finite projective lines/geometries  

E-Print Network [OSTI]

The commutation relations between the generalized Pauli operators of N-qudits (i. e., N p-level quantum systems), and the structure of their maximal sets of commuting bases, follow a nice graph theoretical/geometrical pattern. One may identify vertices/points with the operators so that edges/lines join commuting pairs of them to form the so-called Pauli graph P_{p^N} . As per two-qubits (p = 2, N = 2) all basic properties and partitionings of this graph are embodied in the geometry of the symplectic generalized quadrangle of order two, W(2). The structure of the two-qutrit (p = 3, N = 2) graph is more involved; here it turns out more convenient to deal with its dual in order to see all the parallels with the two-qubit case and its surmised relation with the geometry of generalized quadrangle Q(4, 3), the dual of W(3). Finally, the generalized adjacency graph for multiple (N > 3) qubits/qutrits is shown to follow from symplectic polar spaces of order two/three. The relevance of these mathematical concepts to mutually unbiased bases and to quantum entanglement is also highlighted in some detail.

Michel R. P. Planat; Metod Saniga

2007-03-16T23:59:59.000Z

465

The unexpected role of D waves in low-energy neutral pion photoproduction  

E-Print Network [OSTI]

It has been commonly assumed that low-energy neutral pion photoproduction from the proton can be described accounting only for S and P waves, and that higher partial waves are irrelevant. We have found that this assumption is not correct and that the inclusion of D waves is necessary to obtain a reliable extraction of the $E_{0+}$ multipole from experimental data. This is due in large measure to the spontaneous breaking of chiral symmetry in QCD which leads to very small S-wave contributions. This makes the usual partial wave expansion less accurate and although D waves are small, their contribution is enhanced through the interference with P waves, which compromises the S-wave extraction from data if D waves are not taken into account. In our work we have used Heavy Baryon Chiral Perturbation Theory to one loop, and up to ${\\cal O}(q^4)$, to account for the S and P waves, while D waves are added in an almost model-independent way using standard Born terms and vector mesons. We also show that higher partial waves do not play an important role.

C. Fernandez-Ramirez

2009-12-21T23:59:59.000Z

466

Information media used by cotton farmers in producing cotton in a ten-county area of North Central Texas  

E-Print Network [OSTI]

~~/%M~(~ ~ . , gP'Z'1$'+19'f. . W~jF ' ' ~Q. , "f Q9&'1+~ , gp @P '~ 8p ~~AC/. 9g"55!, QP y'4~3'6~ @1+ $4~ Q4~ f~'. t$, QM~gg8Z Z$;, '3'TOKgQg ppj7 8&, ", ~ Otp gC Q2~ Slp89p&Q, ~Q C$ pRH@p%Q~~ 1 ': ' I I l '$ '~CP1&p 4' . ~", I t 'C Fi... ' . 4~$AJ"1~9"~3'i7~ . . KK W:~1ivjg' ~ ~gg:yg grq-'gg~g gg +'~ ~~ y? ~g gg~' ~0@ @gal g~ QlfCL@CQ @AQ, ~'ALVJQ9 ~, QQS g1'~gi~i+1 5$ a J+S $+QgfQq ~~7$+Vl:g ( 'Vx'pi~i~('f8 &M~ ~':~'g8CM 4O ~M~ ~ 4i 3s K~-;JAy A"w&i?8POV 88%. p R &~lC 4'W~ Wo RQL...

Anwarul Karim, A. M

2012-06-07T23:59:59.000Z

467

Thermal conduction by dark matter with velocity and momentum-dependent cross-sections  

E-Print Network [OSTI]

We use the formalism of Gould and Raffelt to compute the dimensionless thermal conduction coefficients for scattering of dark matter particles with standard model nucleons via cross-sections that depend on the relative velocity or momentum exchanged between particles. Motivated by models invoked to reconcile various recent results in direct detection, we explicitly compute the conduction coefficients $\\alpha$ and $\\kappa$ for cross-sections that go as $v_{\\rm rel}^2$, $v_{\\rm rel}^4$, $v_{\\rm rel}^{-2}$, $q^2$, $q^4$ and $q^{-2}$, where $v_{\\rm rel}$ is the relative DM-nucleus velocity and $q$ is the momentum transferred in the collision. We find that a $v_{\\rm rel}^{-2}$ dependence can significantly enhance energy transport from the inner solar core to the outer core. The same can true for any $q$-dependent coupling, if the dark matter mass lies within some specific range for each coupling. This effect can complement direct searches for dark matter; combining these results with state-of-the-art Solar simulations should greatly increase sensitivity to certain DM models. It also seems possible that the so-called Solar Abundance Problem could be resolved by enhanced energy transport in the solar core due to such velocity- or momentum-dependent scatterings.

Aaron C. Vincent; Pat Scott

2014-04-23T23:59:59.000Z

468

BDOS: An open-ended, basic disk operating system for a Nova/Diablo system  

E-Print Network [OSTI]

4- Z O LJ 2 Vj 2 Z M X Z K CC CW 0 4J I- 4. Q 4 O H Vj LII Q W 2 ILC CI M i Z C N I- C 4l I4 0 ) O O I- 0 0 W V' CI O C ZQ I- W Vj CC cC 4J Z lfl I C W 2 P I- CY X C 4J I- CJ Na ~ 0 W 4I jN M O jo 3 4I W VJ Z I H I I... QO Z 2OCV 4I Y O jN Z H Z j EP cC 4J Vj CI CC c Q 0 ct I 4l Vj ) Q ct 3 Vl Q O O I- 4J ~ LL C 4J Vj WCCJ N Z 4J VIWr Q N Y o xa HWCCI O I-4J QC QN VJCC j M VJLV N H W Z IJ CC M W j jQ'0 jCNO I- ct cJ ") cC Vj Vj O cC W ~ ? I...

Koontz, Joseph Patrick

1972-01-01T23:59:59.000Z

469

The performance of the small-angle diffractometer, SAND at IPNS.  

SciTech Connect (OSTI)

The time-of-flight small-angle diffractometer SAND has been serving the scientific user community since 1996. One notable feature of SAND is its capability to measure the scattered intensity in a wide Q (4{pi}sin{theta}/{lambda}, where 2{theta} is the scattering angle and {lambda} is the wavelength of the neutrons) range of 0.0035 to 0.5 {angstrom}{sup {minus}1} in a single measurement. The optical alignment system makes it easy to set up the instrument and the sample. The cryogenically cooled MgO filter reduces the fast neutrons over two orders of magnitude, while still transmitting over 70% of the cold neutrons. A drum chopper running at 15 Hz suppresses the delayed neutron background. SAND has a variety of ancillary equipment to control the sample environment. In this paper we describe the features of the SAND instrument, compare its data on a few standard samples with those measured at well established centers in the world, and display two scientific examples which take advantage of measuring data in a wide Q-range in a single measurement. With a new set of tight collimators the Q{sub min} can be lowered to 0.002 {angstrom}{sup {minus}1} and the presently installed high-angle bank of detectors will extend the Q{sub max} to 2 {angstrom}{sup {minus}1}.

Thiyagarajan, P.

1998-07-17T23:59:59.000Z

470

Selected income tax problems of closely-held corporations  

E-Print Network [OSTI]

yolaeaagL ao roly ea Qe a?eh Me ?aalay aea ho?a Lae yenta?L eag a eeh?1oaaQ4 eho?hhoiLgerr ?ho Oae?L??4?aor eeeiL4 aoa haea q?oea4eno4 Me 4eaa?LL?a~ ?ho eel& fee?4 ihah, Qe La?a? ~ ae 4?ga?LtL?aa far ra?L ae?o La taea ?eah Ca aha ab??ace at pe?et Qa... Lhe eecA?l ysyeaA c?e aa4o, havleg ycocN?e?4 iL L~ a ~aLcacc aaa?, The Sc?L Lhaa Lhe ~ of ~ op INpk&loo yai4 aeo ?~A ea Lhe cacw?A ef pc?fiL? ae?4 ?eL b? ~c?4 if il aah bo ohococ LhcA Lho csee& ?f pc?fib? ?arne?4 io ?LLrgnAal4? Lo gaia?eh teal ao4...

Cunningham, Thomas Martin

1952-01-01T23:59:59.000Z

471

Catalytic fast pyrolysis of lignocellulosic biomass  

SciTech Connect (OSTI)

Increasing energy demand, especially in the transportation sector, and soaring CO2 emissions necessitate the exploitation of renewable sources of energy. Despite the large variety of new energy Q3 carriers, liquid hydrocarbon still appears to be the most attractive and feasible form of transportation fuel taking into account the energy density, stability and existing infrastructure. Biomass is an abundant, renewable source of energy; however, utilizing it in a cost-effective way is still a substantial challenge. Lignocellulose is composed of three major biopolymers, namely cellulose, hemicellulose and lignin. Fast pyrolysis of biomass is recognized as an efficient and feasible process to selectively convert lignocellulose into a liquid fuel—bio-oil. However bio-oil from fast pyrolysis contains a large amount of oxygen, distributed in hundreds of oxygenates. These oxygenates are the cause of many negative properties, such as low heating values, high corrosiveness, high viscosity, and instability; they also greatly Q4 limit the application of bio-oil particularly as transportation fuel. Hydrocarbons derived from biomass are most attractive because of their high energy density and compatibility with the existing infrastructure. Thus, converting lignocellulose into transportation fuels via catalytic fast pyrolysis has attracted much attention. Many studies related to catalytic fast pyrolysis of biomass have been published. The main challenge of this process is the development of active and stable catalysts that can deal with a large variety of decomposition intermediates from lignocellulose. This review starts with the current understanding of the chemistry in fast pyrolysis of lignocellulose and focuses on the development of catalysts in catalytic fast pyrolysis. Recent progress in the experimental studies on catalytic fast pyrolysis of biomass is also summarized with the emphasis on bio-oil yields and quality.

Liu, Changjun; Wang, Huamin; Karim, Ayman M.; Sun, Junming; Wang, Yong

2014-11-21T23:59:59.000Z

472

Phonon-roton modes of liquid 4He beyond the roton in MCM-41  

SciTech Connect (OSTI)

We present neutron scattering measurements of the phonon-roton (P-R) mode of superfluid 4He confined in 47 A MCM-41 at T = 0.5 K at wave vectors, Q, beyond the roton wave vector (QR = 1.92 A-1). Measurements beyond the roton require access to high wave vectors (up to Q = 4 A-1) with excellent energy resolution and high statistical precision. The present results show for the first time that at T = 0.5 K the P-R mode in MCM-41 extends out to wave-vector Q 3.6 A-1 with the same energy and zero width (within precision) as observed in bulk superfluid 4He. Layer modes in the roton region are also observed. Specifically, the P-R mode energy, !Q, increases with Q for Q > QR and reaches a plateau at a maximum energy !Q = 2 where is the roton energy, = 0.74 0.01 meV in MCM-41. This upper limit means the P-R mode decays to two rotons when its energy exceeds 2 . It also means that the P-R mode does not decay to two layers modes. If the P-R could decay to two layer modes, !Q would plateau at a lower energy, !Q = 2 L where L = 0.60 meV is the energy of the roton like minimum of the layer mode. The observation of the P-R mode with energy up to 2 shows that the P-R mode and the layer modes are independent modes with apparently little interaction between them.

Azuah, Richard T [NIST Center for Neutron Research (NCRN), Gaithersburg, MD] NIST Center for Neutron Research (NCRN), Gaithersburg, MD; Omar Diallo, Souleymane [ORNL] ORNL; Adams, Mark A. [ISIS Facility, Rutherford Appleton Laboratory (ISIS)] ISIS Facility, Rutherford Appleton Laboratory (ISIS); Kirichek, Oleg [ISIS Facility, Rutherford Appleton Laboratory (ISIS)] ISIS Facility, Rutherford Appleton Laboratory (ISIS); Glyde, Henry R [University of Delaware] University of Delaware

2013-01-01T23:59:59.000Z

473

Heavy Truck Engine Program  

SciTech Connect (OSTI)

The Heavy Duty Truck Engine Program at Cummins embodied three significant development phases. All phases of work strove to demonstrate a high level of diesel engine efficiency in the face of increasingly stringent emission requirements. Concurrently, aftertreatment system development and refinement was pursued in support of these efficiency demonstrations. The program's first phase focused on the demonstration in-vehicle of a high level of heavy duty diesel engine efficiency (45% Brake Thermal Efficiency) at a typical cruise condition while achieving composite emissions results which met the 2004 U.S. EPA legislated standards. With a combination of engine combustion calibration tuning and the development and application of Urea-based SCR and particulate aftertreatment, these demonstrations were successfully performed by Q4 of 2002. The second phase of the program directed efforts towards an in-vehicle demonstration of an engine system capable of meeting 2007 U.S. EPA legislated emissions requirements while achieving 45% Brake Thermal Efficiency at cruise conditions. Through further combustion optimization, the refinement of Cummins Cooled EGR architecture, the application of a high pressure common rail fuel system and the incorporation of optimized engine parasitics, Cummins Inc. successfully demonstrated these deliverables in Q2 of 2004. The program's final phase set a stretch goal of demonstrating 50% Brake Thermal Efficiency from a heavy duty diesel engine system capable of meeting 2010 U.S. EPA legislated emissions requirements. Cummins chose to pursue this goal through further combustion development and refinement of the Cooled EGR system architecture and also applied a Rankine cycle Waste Heat Recovery technique to convert otherwise wasted thermal energy to useful power. The engine and heat recovery system was demonstrated to achieve 50% Brake Thermal Efficiency while operating at a torque peak condition in second quarter, 2006. The 50% efficient engine system was capable of meeting 2010 emissions requirements through the application of NOx and particulate matter reduction techniques proven earlier in the program.

Nelson, Christopher

2009-01-08T23:59:59.000Z

474

Measurements on the 3He+?System at ANKE  

E-Print Network [OSTI]

The differential and total cross-sections for the dp \\to 3He \\eta reaction have been measured in a high precision high statistics COSY-ANKE experiment near threshold using a continuous beam energy ramp up to an excess energy Q of 11.3 MeV with essentially 100% acceptance. The kinematics allowed the mean value of Q to be determined to about 9 keV. Evidence is found for the effects of higher partial waves for Q > 4 MeV. The very rapid rise of the total cross-section to its maximum value within 0.5 MeV of threshold implies a very large \\eta 3He scattering length and hence the presence of a quasi-bound state extremely close to threshold. In addition, differential and total cross-sections have been measured at excess energies of 19.5, 39.4, and 59.4 MeV over the full angular range. While at 19.5 MeV the results can be described in terms of s- and p-wave production, by 59.4 MeV higher partial waves are required. Including the 19.5 MeV point together with the near-threshold data in a global s- and p-wave fit gives a poorer overall description of the data though the position of the pole in the \\eta 3He scattering amplitude, corresponding to the quasi-bound or virtual state, is hardly changed.

A. Khoukaz

2010-11-03T23:59:59.000Z

475

PLANETARY AND OTHER SHORT BINARY MICROLENSING EVENTS FROM THE MOA SHORT-EVENT ANALYSIS  

SciTech Connect (OSTI)

We present the analysis of four candidate short-duration binary microlensing events from the 2006-2007 MOA Project short-event analysis. These events were discovered as a by-product of an analysis designed to find short-timescale single-lens events that may be due to free-floating planets. Three of these events are determined to be microlensing events, while the fourth is most likely caused by stellar variability. For each of the three microlensing events, the signal is almost entirely due to a brief caustic feature with little or no lensing attributable mainly to the lens primary. One of these events, MOA-bin-1, is due to a planet, and it is the first example of a planetary event in which the stellar host is only detected through binary microlensing effects. The mass ratio and separation are q (4.9 {+-} 1.4) Multiplication-Sign 10{sup -3} and s = 2.10 {+-} 0.05, respectively. A Bayesian analysis based on a standard Galactic model indicates that the planet, MOA-bin-1Lb, has a mass of m{sub p} = 3.7 {+-} 2.1 M{sub Jup} and orbits a star of M{sub *} = 0.75{sub -0.41}{sup +}0{sup .33} M{sub Sun} at a semimajor axis of a = 8.3{sub -2.7}{sup +4.5} AU. This is one of the most massive and widest separation planets found by microlensing. The scarcity of such wide-separation planets also has implications for interpretation of the isolated planetary mass objects found by this analysis. If we assume that we have been able to detect wide-separation planets with an efficiency at least as high as that for isolated planets, then we can set limits on the distribution of planets in wide orbits. In particular, if the entire isolated planet sample found by Sumi et al. consists of planets bound in wide orbits around stars, we find that it is likely that the median orbital semimajor axis is >30 AU.

Bennett, D. P. [Department of Physics, University of Notre Dame, Notre Dame, IN 46556 (United States); Sumi, T. [Department of Earth and Space Science, Osaka University, Osaka 560-0043 (Japan); Bond, I. A.; Ling, C. H. [Institute for Information and Mathematical Sciences, Massey University, Auckland 1330 (New Zealand); Kamiya, K.; Abe, F.; Fukui, A.; Furusawa, K.; Itow, Y.; Masuda, K.; Matsubara, Y.; Miyake, N.; Muraki, Y. [Solar-Terrestrial Environment Laboratory, Nagoya University, Nagoya 464-8601 (Japan); Botzler, C. S.; Rattenbury, N. J. [Department of Physics, University of Auckland, Private Bag 92-019, Auckland 1001 (New Zealand); Korpela, A. V.; Sullivan, D. J. [School of Chemical and Physical Sciences, Victoria University, Wellington (New Zealand); Kilmartin, P. M. [Mt. John Observatory, P.O. Box 56, Lake Tekapo 8770 (New Zealand); Ohnishi, K. [Nagano National College of Technology, Nagano 381-8550 (Japan); Saito, To., E-mail: bennett@nd.edu [Tokyo Metropolitan College of Aeronautics, Tokyo 116-8523 (Japan); Collaboration: MOA Collaboration; and others

2012-10-01T23:59:59.000Z

476

The role of parallel heat transport in the relation between upstream scrape-off layer widths and target heat flux width in H-mode plasmas of NSTX.  

SciTech Connect (OSTI)

The physics of parallel heat transport was tested in the Scrape-off Layer (SOL) plasma of the National Spherical Torus Experiment (NSTX) [M. Ono, et al., Nucl. Fusion 40, 557 (2000) and S. M. Kaye, et al., Nucl. Fusion 45, S168 (2005)] tokamak by comparing the upstream electron temperature (T{sub e}) and density (n{sub e}) profiles measured by the mid-plane reciprocating probe to the heat flux (q{sub {perpendicular}}) profile at the divertor plate measured by an infrared (IR) camera. It is found that electron conduction explains the near SOL width data reasonably well while the far SOL, which is in the sheath limited regime, requires an ion heat flux profile broader than the electron one to be consistent with the experimental data. The measured plasma parameters indicate that the SOL energy transport should be in the conduction-limited regime for R-R{sub sep} (radial distance from the separatrix location) < 2-3 cm. The SOL energy transport should transition to the sheath-limited regime for R-R{sub sep} > 2-3cm. The T{sub e}, n{sub e}, and q{sub {perpendicular}} profiles are better described by an offset exponential function instead of a simple exponential. The conventional relation between mid plane electron temperature decay length ({lambda}{sub Te}) and target heat flux decay length ({lambda}{sub q}) is {lambda}{sub Te} = 7/2{lambda}{sub q}, whereas the newly-derived relation, assuming offset exponential functional forms, implies {lambda}{sub Te} = (2-2.5){lambda}{sub q}. The measured values of {lambda}{sub Te}/{lambda}{sub q} differ from the new prediction by 25-30%. The measured {lambda}{sub q} values in the far SOL (R-R{sub sep} > 2-3cm) are 9-10cm, while the expected values are 2.7 < {lambda}{sub q} < 4.9 cm (for sheath-limited regime). We propose that the ion heat flux profile is substantially broader than the electron heat flux profile as an explanation for this discrepancy in the far SOL.

Ahn, J W; Boedo, J A; Maingi, R; Soukhanovskii, V A

2009-01-05T23:59:59.000Z

477

SOUTHEAST REGIONAL CARBON SEQUESTRATION PARTNERSHIP (SECARB)  

SciTech Connect (OSTI)

The Southeast Regional Carbon Sequestration Partnership (SECARB) is on schedule and within budget projections for the work completed during the first year of its two year program. Work during the semiannual period (third and fourth quarter) of the project (April 1--September 30, 2004) was conducted within a ''Task Responsibility Matrix.'' Under Task 1.0 Define Geographic Boundaries of the Region, Texas and Virginia were added during the second quarter of the project and no geographical changes occurred during the third or fourth quarter of the project. Under Task 2.0 Characterize the Region, general mapping and screening of sources and sinks has been completed, with integration and Geographical Information System (GIS) mapping ongoing. The first step focused on the macro level characterization of the region. Subsequent characterization will focus on smaller areas having high sequestration potential. Under Task 3.0 Identify and Address Issues for Technology Deployment, SECARB has completed a preliminary assessment of safety, regulatory, permitting, and accounting frameworks within the region to allow for wide-scale deployment of promising terrestrial and geologic sequestration approaches. Under Task 4.0 Develop Public Involvement and Education Mechanisms, SECARB has conducted a survey and focus group meeting to gain insight into approaches that will be taken to educate and involve the public. Task 5.0 and 6.0 will be implemented beginning October 1, 2004. Under Task 5.0 Identify the Most Promising Capture, Sequestration, and Transport Options, SECARB will evaluate findings from work performed during the first year and shift the focus of the project team from region-wide mapping and characterization to a more detailed screening approach designed to identify the most promising opportunities. Under Task 6.0 Prepare Action Plans for Implementation and Technology Validation Activity, the SECARB team will develop an integrated approach to implementing and setting up measurement, monitoring and verification (MMV) programs for the most promising opportunities. During this semiannual period special attention was provided to Texas and Virginia, which were added to the SECARB region, to ensure a smooth integration of activities with the other 9 states. Milestones completed and submitted during the third and fourth quarter included: Q3-FY04--Complete initial development of plans for GIS; and Q4-FYO4--Complete preliminary action plan and assessment for overcoming public perception issues.

Kenneth J. Nemeth

2004-09-01T23:59:59.000Z

478

Insights into Silicate Carbonation Processes in Water-Bearing Supercritical CO2 Fluids  

SciTech Connect (OSTI)

Long-term geologic storage of carbon dioxide (CO2) is considered an integral part to moderating CO2 concentrations in the atmosphere and subsequently minimizing effects of global climate change. Although subsurface injection of CO2 is common place in certain industries, deployment at the scale required for emission reduction is unprecedented and therefore requires a high degree of predictability. Accurately modeling geochemical processes in the subsurface requires experimental derived data for mineral reactions occurring between the CO2, water, and rocks. Most work in this area has focused on aqueous-dominated systems in which dissolved CO2 reacts to form crystalline carbonate minerals. Comparatively little laboratory research has been conducted on reactions occurring between minerals in the host rock and the wet supercritical fluid phase. In this work, we studied the carbonation of wollastonite [CaSiO3] exposed to variably hydrated supercritical CO2 (scCO2) at a range of temperatures (50, 55 and 70 °C) and pressures (90,120 and 160 bar) that simulate conditions in geologic repositories. Mineral transformation reactions were followed by three novel in situ high pressure techniques, including x-ray diffraction that tracked the rate and extents of wollastonite conversion to calcite. Increased dissolved water concentrations in the supercritical CO2 resulted in increased silicate carbonation approaching ~50 wt. %. Development of thin water films on the mineral surface were directly observed with infrared spectroscopy and determined to be critical for facilitating carbonation processes. Even in extreme low water conditions, magic angle spinning nuclear magnetic resonance detected formation of Q3 [Si(OSi)3OH] and Q4 [Si(OSi)4] amorphous silica species. Unlike the thick (<10 ?m) passivating silica layers observed in the fully water saturated scCO2 experiments, images obtained from a focused ion beam sectioned sample indicted these coatings were chemically wollastonite but structurally amorphous. In addition, evidence of an intermediate hydrated amorphous calcium carbonate forming under these conditions further emphasize the importance of understanding geochemical processes occurring in water bearing scCO2 fluids.

Miller, Quin RS; Thompson, Christopher J.; Loring, John S.; Windisch, Charles F.; Bowden, Mark E.; Hoyt, David W.; Hu, Jian Z.; Arey, Bruce W.; Rosso, Kevin M.; Schaef, Herbert T.

2013-07-01T23:59:59.000Z

479

Annual Hanford Seismic Report for Fiscal Year 2010  

SciTech Connect (OSTI)

The Hanford Seismic Assessment Program (HSAP) provides an uninterrupted collection of high-quality raw and processed seismic data from the Hanford Seismic Network for the U.S. Department of Energy and its contractors. The HSAP is responsible for locating and identifying sources of seismic activity and monitoring changes in the historical pattern of seismic activity at the Hanford Site. The data are compiled, archived, and published for use by the Hanford Site for waste management, natural phenomena hazards assessments, and engineering design and construction. In addition, the HSAP works with the Hanford Site Emergency Services Organization to provide assistance in the event of a significant earthquake on the Hanford Site. The Hanford Seismic Network and the Eastern Washington Regional Network consist of 44 individual sensor sites and 15 radio relay sites maintained by the Hanford Seismic Assessment Team. During FY 2010, the Hanford Seismic Network recorded 873 triggers on the seismometer system, which included 259 seismic events in the southeast Washington area and an additional 324 regional and teleseismic events. There were 210 events determined to be local earthquakes relevant to the Hanford Site. One hundred and fifty-five earthquakes were detected in the vicinity of Wooded Island, located about eight miles north of Richland just west of the Columbia River. The Wooded Island events recorded this fiscal year were a continuation of the swarm events observed during fiscal year 2009 and reported in previous quarterly and annual reports (Rohay et al. 2009a, 2009b, 2009c, 2010a, 2010b, and 2010c). Most events were considered minor (coda-length magnitude [Mc] less than 1.0) with the largest event recorded on February 4, 2010 (3.0Mc). The estimated depths of the Wooded Island events are shallow (averaging approximately 1.5 km deep) placing the swarm within the Columbia River Basalt Group. Based upon the last two quarters (Q3 and Q4) data, activity at the Wooded Island area swarm has largely subsided. Pacific Northwest National Laboratory will continue to monitor for activity at this location. The highest-magnitude events (3.0Mc) were recorded on February 4, 2010 within the Wooded Island swarm (depth 2.4 km) and May 8, 2010 on or near the Saddle Mountain anticline (depth 3.0 km). This latter event is not considered unusual in that earthquakes have been previously recorded at this location, for example, in October 2006 (Rohay et al. 2007). With regard to the depth distribution, 173 earthquakes were located at shallow depths (less than 4 km, most likely in the Columbia River basalts), 18 earthquakes were located at intermediate depths (between 4 and 9 km, most likely in the pre-basalt sediments), and 19 earthquakes were located at depths greater than 9 km, within the crystalline basement. Geographically, 178 earthquakes were located in known swarm areas, 4 earthquakes occurred on or near a geologic structure (Saddle Mountain anticline), and 28 earthquakes were classified as random events. The Hanford Strong Motion Accelerometer (SMA) network was triggered several times by the Wooded Island swarm events and the events located on or near the Saddle Mountain anticline. The maximum acceleration value recorded by the SMA network during fiscal year 2010 occurred February 4, 2010 (Wooded Island swarm event), approximately 2 times lower than the reportable action level for Hanford facilities (2% g) with no action required.

Rohay, Alan C.; Clayton, Ray E.; Sweeney, Mark D.; Devary, Joseph L.; Hartshorn, Donald C.

2010-12-27T23:59:59.000Z