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Note: This page contains sample records for the topic "30-degree azimuth intervals" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
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1

ARM: W-Band Scanning ARM Cloud Radar (W-SACR) Hemispherical Sky RHI Scans (6 horizon-to-horizon scans at 30-degree azimuth intervals)  

DOE Data Explorer (OSTI)

W-Band Scanning ARM Cloud Radar (W-SACR) Hemispherical Sky RHI Scans (6 horizon-to-horizon scans at 30-degree azimuth intervals)

Widener, Kevin; Nelson, Dan; Bharadwaj, Nitin; Lindenmaier, Iosif [Andrei; Johnson, Karen

2

ARM: Ka-Band Scanning ARM Cloud Radar (KASACR) Hemispherical Sky RHI Scan (6 horizon-to-horizon scans at 30-degree azimuth intervals)  

DOE Data Explorer (OSTI)

Ka-Band Scanning ARM Cloud Radar (KASACR) Hemispherical Sky RHI Scan (6 horizon-to-horizon scans at 30-degree azimuth intervals)

Bharadwaj, Nitin; Widener, Kevin

3

ARM: X-Band Scanning ARM Cloud Radar (XSACR) Hemispherical Sky RHI Scans (6 horizon-to-horizon scans at 30-degree azimuth intervals)  

DOE Data Explorer (OSTI)

X-Band Scanning ARM Cloud Radar (XSACR) Hemispherical Sky RHI Scans (6 horizon-to-horizon scans at 30-degree azimuth intervals)

Widener, Kevin; Nelson, Dan; Bharadwaj, Nitin; Lindenmaier, Iosif [Andrei; Johnson, Karen

4

Definition: Azimuth | Open Energy Information  

Open Energy Info (EERE)

Azimuth Azimuth Jump to: navigation, search Dictionary.png Azimuth The angle between true south and the point on the horizon directly below the sun.[1] View on Wikipedia Wikipedia Definition An azimuth is an angular measurement in a spherical coordinate system. The vector from an observer to a point of interest is projected perpendicularly onto a reference plane; the angle between the projected vector and a reference vector on the reference plane is called the azimuth. An example is the position of a star in the sky. The star is the point of interest, the reference plane is the horizon or the surface of the sea, and the reference vector points north. The azimuth is the angle between the north vector and the perpendicular projection of the star down onto the horizon. Azimuth is usually measured in degrees (°). The concept is used

5

Precision stationkeeping with azimuthing thrusters  

E-Print Network (OSTI)

Precision positioning of an unmanned surface vehicle (USV) in a nautical environment is a difficult task. With a dual azimuthing thruster scheme, the optimization of thruster outputs uses an online method to minimize the ...

Doroski, Adam D

2011-01-01T23:59:59.000Z

6

In-flight Receptivity Experiments on a 30-degree Swept-wing using Micron-sized Discrete Roughness Elements  

E-Print Network (OSTI)

laminar flow control strategy. Results of a 3-year flight test program focused on receptivity measurements and laminar flow control on a 30-degree swept-wing are presented. A swept-wing test article was mounted on the port wing of a Cessna O-2A aircraft...

Carpenter, Andrew L.

2010-01-16T23:59:59.000Z

7

E-Print Network 3.0 - azimuthal asymmetry measured Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

coupled plasma etching reactors: Azimuthal symmetry, coil properties, and comparison Summary: and selectivity as a func- tion of azimuth and radius. Azimuthal...

8

Azimuthal Jet Tomography at RHIC and LHC  

E-Print Network (OSTI)

A generic jet-energy loss model that is coupled to state-of-the-art hydrodynamic fields and interpolates between a wide class of running coupling pQCD-based and AdS/CFT-inspired models is compared to recent data on the azimuthal and transverse momentum dependence of high-pT pion nuclear modification factors and high-pT elliptic flow measured at RHIC and LHC. We find that RHIC data are surprisingly consistent with various scenarios considered. However, extrapolations to LHC energies favor running coupling pQCD-based models of jet-energy loss. While conformal holographic models are shown to be inconsistent with data, recent non-conformal generalizations of AdS holography may provide an alternative description.

Barbara Betz; Miklos Gyulassy

2014-02-14T23:59:59.000Z

9

LRRR Emplacement Range and Azimuth From. LM for Fra Mauro  

E-Print Network (OSTI)

LRRR Emplacement Range and Azimuth From. LM for Fra Mauro Landing Site NO. A Tl\\1- WIO PAGE I REV abovt by LM or other lunar equipment (ALSEP), Potential damage to the .i RRR l'Ould be caused . (}~/ #12;.. ~ospace LRRR Emplacement Range and Azimuth From LM for Fra Mauro Landing Site NO. ATM-890 PAGE

Rathbun, Julie A.

10

The Azimuth Project: an open-access educational resource  

E-Print Network (OSTI)

other things, the Azimuth Project includes: 1. A project to explain climate physics with the help of the glacial cycle. #12;Among other things, the Azimuth Project includes: 1. A project to explain climate Project includes: 1. A project to explain climate physics with the help of software that runs on your

Baez, John

11

Analyses of azimuthal seismic anisotrophy in the vertically fractured Spraberry and Dean formations, Midland County, Texas  

E-Print Network (OSTI)

The configuration of a CDP gather from 3-D seismic reflection has source-receiver pairs located at different azimuths. This can be exploited to observe azimuthal variations of P- wave velocity related to azimuthal anisotropy in fractured media...

Sudarmo, Bernadus Supraptomo

2012-06-07T23:59:59.000Z

12

E-Print Network 3.0 - azimuthal di-hadron correlations Sample...  

NLE Websites -- All DOE Office Websites (Extended Search)

minimum of the azimuth modulation, which supports the theoretical correlation between wind direction... and azimuth angle). Combined, we term these parameters the observation...

13

Dynamics of acyclic interval maps  

E-Print Network (OSTI)

Vol. 6 (2009) Dynamics of acyclic interval maps [16] D.orbits and bifurcation of maps of the interval. SIAM J.Dynamics of acyclic interval maps Morris W. Hirsch He who

Hirsch, Morris W

2009-01-01T23:59:59.000Z

14

Azimuthal Resistivity to Characterize Fractures in a Glacial Till Mark Boris, University of Saskatchewan  

E-Print Network (OSTI)

of Saskatchewan Jim Merriam, University of Saskatchewan Abstract Azimuthal resistivity was used to characterize

Merriam, James

15

Phenomenology of SIDIS unpolarized cross sections and azimuthal asymmetries  

E-Print Network (OSTI)

I review the phenomenology of unpolarized cross sections and azimuthal asymmetries in semi-inclusive deeply inelastic scattering (SIDIS). The general theoretical framework is presented and the validity of the Gaussian model is discussed. A brief account of the existing analyses is provided.

Vincenzo Barone

2012-03-28T23:59:59.000Z

16

E-Print Network 3.0 - azimuthal signal variations Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

Summary: of the azimuth DTFs of the same ear with gray-scale coding for power (in dB). Note the huge variations in power... .8 The monaural duplex theory 6 1.9 Azimuth Cue...

17

E-Print Network 3.0 - azimuthal angle correlations Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

to form the swath and to obtain the nec- essary azimuth measurements in order to perform wind retrieval 2... , the resolution in the azimuth dimension is governed by the...

18

Azimuthal harmonics of color fields in a high energy nucleus  

E-Print Network (OSTI)

Recent experimental results have revealed a surprisingly rich structure of multiparticle azimuthal correlations in high energy proton-nucleus collisions. Final state collective effects can be responsible for many of the observed effects, but it has recently been argued that a part of these correlations are present already in the wavefunctions of the colliding particles. We evaluate the momentum space 2-particle cumulant azimuthal anisotropy coefficients v_n{2}, n=2,3,4 from fundamental representation Wilson line distributions describing the high energy nucleus. These would correspond to the flow coefficients in very forward proton nucleus scattering. We find significant differences beteen Wilson lines from the MV model and from JIMWLK evolution. The magnitude and transverse momentum dependence of the v_n{2} values suggest that the fluctuations present in the initial fields are a significant contribution to the observed anisotropies.

Lappi, T

2015-01-01T23:59:59.000Z

19

Azimuthal Anisotropies as Stringent Test for Nuclear Transport Models  

E-Print Network (OSTI)

Azimuthal distributions of charged particles and intermediate mass fragments emitted in Au+Au collisions at 600AMeV have been measured using the FOPI facility at GSI-Darmstadt. Data show a strong increase of the in-plane azimuthal anisotropy ratio with the charge of the detected fragment. Intermediate mass fragments are found to exhibit a strong momentum-space alignment with respect of the reaction plane. The experimental results are presented as a function of the polar center-of-mass angle and over a broad range of impact parameters. They are compared to the predictions of the Isospin Quantum Molecular Dynamics model using three different parametrisations of the equation of state. We show that such highly accurate data provide stringent test for microscopic transport models and can potentially constrain separately the stiffness of the nuclear equation of state and the momentum dependence of the nuclear interaction.

P. Crochet; F. Rami; R. Dona; the FOPI Collaboration

1997-09-15T23:59:59.000Z

20

Performance analysis of Azimuth Tracking Fixed Mirror Solar Concentrator  

Science Journals Connector (OSTI)

Abstract The fixed mirror solar collector (FMSC) fixes reflector and mobiles receiver to collect solar energy. However, this type of concentrator has a low efficiency and short operating duration in practical applications. In this paper, we propose to install the FMSC on an azimuth tracking device (ATFMSC) and the reflectors are arranged by intermission to avoid the shading of neighbor reflector for incidence angle of less than 10° to improve its optical performance. Through the integration of the reflected solar radiation distribution function over any reflection point, and then the whole collector aperture, we develop the analytical expressions of various system efficiencies to numerically simulate the performance of ATFMSC with evacuated tube receiver in different design parameters. It is validated by the ray tracing results. The result shows that the mean annual net heat efficiency of the whole system would be up to 61% with the operating temperature of 400 °C, which is higher than parabolic trough collector and traditional FMSC. This is because the longitudinal incidence angle of ATFMSC always remains zero by tracking the sun azimuth, so the end loss of the concentrator can be avoided and enables it to operate with high efficiency continually.

Longlong Li; Huairui Li; Qian Xu; Weidong Huang

2015-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

Optical performance of an azimuth tracking linear Fresnel solar concentrator  

Science Journals Connector (OSTI)

Abstracts In this paper, a linear Fresnel solar concentrator installed on a solar azimuth tracker is studied. Based on the integration of the effective source distribution for a reflection point and the whole reflector area, we develop an analytical model to calculate the intercept factor of the concentrator and analyze its performance over a year. The prediction of our analytical optical model agrees pretty well with that of the ray tracing program SolTRACE. Then we study the effects of the main design parameters on the performance of the system. The results show that annual mean total efficiency of 61% can be obtained in optimized design when the operational temperature of the receiver is 400 °C. The performance of the azimuth tracking linear Fresnel solar concentrator (ATLFSC) is compared with that of the parabolic trough collector. It is found that the cosine factor, intercept factor and total efficiency of the ATLFSC are better than those of parabolic trough collector, showing that the ATLFSC may have great potential for solar energy utilization.

Farong Huang; Longlong Li; Weidong Huang

2014-01-01T23:59:59.000Z

22

E-Print Network 3.0 - azimuthally anisotropic electron Sample...  

NLE Websites -- All DOE Office Websites (Extended Search)

low-porosity reser-voirs are largely governed by natural fracture networks. Summary: shale formation. A case study of azimuthal AVO analysis with anisotropic spreading...

23

E-Print Network 3.0 - azimuth transform interpolation Sample...  

NLE Websites -- All DOE Office Websites (Extended Search)

transform interpolation Search Powered by Explorit Topic List Advanced Search Sample search results for: azimuth transform interpolation Page: << < 1 2 3 4 5 > >> 1 IEEE...

24

E-Print Network 3.0 - azimuthal anisotropy etude Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

Resistivity to Characterize Fractures in a Glacial Till Mark Boris, University of Saskatchewan Summary: . There was no interpretable anisotropy in the azimuthal resistivity data....

25

E-Print Network 3.0 - azimuthal map projection Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

properties of tight, low-porosity reser-voirs are largely governed by natural fracture networks. Summary: with borehole measurements, fracture maps obtained from azimuthal...

26

E-Print Network 3.0 - azimuthal energy flow Sample Search Results  

NLE Websites -- All DOE Office Websites (Extended Search)

properties of tight, low-porosity reser-voirs are largely governed by natural fracture networks. Summary: inversion methods that operate with both 3D wide- azimuth surface...

27

E-Print Network 3.0 - azimuth spread estimation Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

properties of tight, low-porosity reser-voirs are largely governed by natural fracture networks. Summary: of MASC becomes nec- essary when the azimuthal variation of the...

28

E-Print Network 3.0 - azimuth Sample Search Results  

NLE Websites -- All DOE Office Websites (Extended Search)

properties of tight, low-porosity reser-voirs are largely governed by natural fracture networks. Summary: inversion methods that operate with both 3D wide- azimuth surface...

29

E-Print Network 3.0 - azimuthally symmetric theory Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

by natural fracture networks. Summary: moveout inversion in azimuthally anisotropic media with lateral velocity variation: Theory and a case... inversion methods that operate...

31

Frequent-Interval Seismic CPTu  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Frequent-Interval Frequent-Interval Seismic CPTu D. Bruce Nothdurft, MSCE, PE, PG SRS Geotechnical Engineering Department Savannah River Nuclear Solutions Alec V. McGillivray, PhD, PE Geotechnical Consultant Brent J. Gutierrez, PhD, PE NPH Engineering Manager, DOE-SR Motivation  The seismic piezocone penetration test (SCPTu) utilized at SRS because it provides rapid and thorough site characterization.  Evaluation of non-linear soil behavior...  detailed stratigraphy  small-strain velocity measurements  large-strain non-seismic measurements  Depth scale disparity  large-strain non-seismic measurements nearly continuous with depth  small-strain velocity measurements over 1 m depth intervals. 2 October 25-26, 2011 DOE NPH Conference

32

High resolution time interval meter  

DOE Patents (OSTI)

Method and apparatus are provided for measuring the time interval between two events to a higher resolution than reliability available from conventional circuits and component. An internal clock pulse is provided at a frequency compatible with conventional component operating frequencies for reliable operation. Lumped constant delay circuits are provided for generating outputs at delay intervals corresponding to the desired high resolution. An initiation START pulse is input to generate first high resolution data. A termination STOP pulse is input to generate second high resolution data. Internal counters count at the low frequency internal clock pulse rate between the START and STOP pulses. The first and second high resolution data are logically combined to directly provide high resolution data to one counter and correct the count in the low resolution counter to obtain a high resolution time interval measurement.

Martin, A.D.

1986-05-09T23:59:59.000Z

33

Frequent-Interval Seismic CPTu  

Energy.gov (U.S. Department of Energy (DOE))

Frequent-Interval Seismic CPTu D. Bruce Nothdurft, MSCE, PE, PG SRS Geotechnical Engineering Department Savannah River Nuclear Solutions Alec V. McGillivray, PhD, PE Geotechnical Consultant Brent J. Gutierrez, PhD, PE NPH Engineering Manager, DOE-SR

34

TESTING FOR AZIMUTHAL ABUNDANCE GRADIENTS IN M101  

SciTech Connect

New optical spectra of 28 H II regions in the M101 disk have been obtained, yielding 10 new detections of the [O III] {lambda}4363 auroral line. The oxygen abundance gradient measured from these data, combined with previous observations, displays a local scatter of 0.15 {+-} 0.03 dex along an arc in the west side of the galaxy, compared with a smaller scatter of 0.08 {+-} 0.01 dex in the rest of the disk. One of the H II regions in our sample (H27) has a significantly lower oxygen abundance than surrounding nebulae at a similar galactocentric distance, while an additional, relatively nearby one (H128) was already known to have a high oxygen abundance for its position in the galaxy. These results represent marginal evidence for the existence of moderate deviations from chemical abundance homogeneity in the interstellar medium of M101. Using a variety of strong-line abundance indicators, we find no evidence for significant large-scale azimuthal variations of the oxygen abundance across the whole disk of the galaxy.

Li, Yanxia; Bresolin, Fabio [Institute for Astronomy, 2680 Woodlawn Dr., Honolulu, HI 96822 (United States)] [Institute for Astronomy, 2680 Woodlawn Dr., Honolulu, HI 96822 (United States); Kennicutt, Robert C. Jr. [Institute of Astronomy, University of Cambridge, Madingley Road, Cambridge CB3 0HA (United Kingdom)] [Institute of Astronomy, University of Cambridge, Madingley Road, Cambridge CB3 0HA (United Kingdom)

2013-03-20T23:59:59.000Z

35

Azimuthal Asymmetries and Vibrational Modes in Bubble Pinch-off  

E-Print Network (OSTI)

The pressure-driven inertial collapse of a cylindrical void in an inviscid liquid is an integrable, Hamiltonian system that forms a finite-time singularity as the radius of the void collapses to zero. Here it is shown that when the natural cylindrical symmetry of the void is perturbed azimuthally, the perturbation modes neither grow nor decay, but instead cause constant amplitude vibrations about the leading-order symmetric collapse. Though the amplitudes are frozen in time, they grow relative to the mean radius which is collapsing to zero, eventually overtaking the leading-order symmetric implosion. Including weak viscous dissipation destroys the integrability of the underlying symmetric implosion, and the effect on the stability spectrum is that short-wavelength disturbances are now erased as the implosion proceeds. Introducing a weak rotational flow component to the symmetric implosion dynamics causes the vibrating shapes to spin as the mean radius collapses. The above theoretical scenario is compared to a closely related experimental realization of void implosion: the disconnection of an air bubble from an underwater nozzle. There, the thin neck connecting the bubble to the nozzle implodes primarily radially inward and disconnects. Recent experiments were able to induce vibrations of the neck shape by releasing the bubble from a slot-shaped nozzle. The frequency and amplitude of the observed vibrations are consistent with the theoretical prediction once surface tension effects are taken into account.

Laura E. Schmidt

2011-12-19T23:59:59.000Z

36

Heliostat tilt and azimuth angle charts and the heliostat orientation protractor  

SciTech Connect

This paper reports that using cartesian heliostat field coordinates analytical expressions were derived for the heliostat tilt angle s, and heliostat azimuth angle {gamma} (clockwise from south). These expressions are dependent on the field cartesian coordinates of the center of the heliostat and the solar zenith and azimuth angles (clockwise from south), {theta}{sub z} and {Psi}, respectively. Here, cylindrical coordinates are conveniently used to derive the expressions for the heliostat angles s and {gamma}. The expression of {gamma}is used to construct the so-called heliostat orientation protractor. The protractor is a useful tool to determine the instantaneous heliostat azimuth angle as will be illustrated.

Elsayed, M.M.; Al-Rabghi, O.M. (Thermal Energy Dept., King Abdulaziz Univ., Jeddah 21413 (SA))

1992-02-01T23:59:59.000Z

37

Comparison of Discrete Fracture and Effective Media Representation of Fractures on Azimuthal AVO  

E-Print Network (OSTI)

In fractured reservoir development, azimuthal AVO (AVOaz) properties of reflected PP waves from reservoir tops are often used to infer fracture properties. The fracture parameter inversion is based on either an effective ...

Zhang, Yang

2005-01-01T23:59:59.000Z

38

High performance path following for marine vehicles using azimuthing podded propulsion  

E-Print Network (OSTI)

Podded propulsion systems offer greater maneuvering possibilities for marine vehicles than conventional shaft and rudder systems. As the propulsion unit rotates about its vertical axis to a specified azimuth angle, the ...

Greytak, Matthew B. (Matthew Bardeen)

2006-01-01T23:59:59.000Z

39

About equivalent interval colorings of weighted graphs  

Science Journals Connector (OSTI)

Given a graph G=(V,E) with strictly positive integer weights @w"i on the vertices i@?V, a k-interval coloring of G is a function I that assigns an interval I(i)@?{1,...,k} of @w"i consecutive integers (called colors) to each vertex i@?V. If two adjacent ... Keywords: Equivalent colorings, Interval coloring problem, Weighted graphs

Mathieu Bouchard; Mirjana angalovi?; Alain Hertz

2009-10-01T23:59:59.000Z

40

Spectral Statistics of RR Intervals in ECG  

E-Print Network (OSTI)

The statistical properties (fluctuations) of heartbeat intervals (RR intervals) in ECG are studied and compared with the predictions of Random Matrix Theory (RMT). It is found that heartbeat intervals only locally exhibit the fluctuation patterns (universality) predicted by the RMT. This finding shows that heartbeat dynamics is of the mixed type where regular and irregular (chaotic) regimes coexist and the Berry-Robnik theory can be applied. It is also observed that the distribution of heartbeat intervals is well described by the one-parameter Brody distribution. The parameter $\\beta $ of the Brody distribution is seen to be connected with the dynamical state of the heart.

Martinis, M; Knezevic, A; Crnugelj, J

2003-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

Azimuthal asymmetries of charged hadrons produced by high-energy muons scattered off longitudinally polarised deuterons  

Science Journals Connector (OSTI)

Azimuthal asymmetries in semi-inclusive production of positive (h +) and negative hadrons (h ?) have been measured by scattering 160 GeV muons off longitudinally polarised deuteron...

M. G. Alekseev; V. Yu. Alexakhin; Yu. Alexandrov…

2010-11-01T23:59:59.000Z

42

Moveout inversion of wide-azimuth P-wave data for tilted TI media Xiaoxiang Wang1  

E-Print Network (OSTI)

to build an accurate initial anisotropic velocity model for processing of wide-azimuth surveys is typical for dipping shale layers

Tsvankin, Ilya

43

Detection of azimuthal anisotropy from 3-D p-wave seismic data  

E-Print Network (OSTI)

DETECTION OF AZIMUTHAL ANISOTROPV FROM 3-D P-WAVE SEISMIC DATA A Thesis by ALI YILDIZEL Submitted to the Office of Graduate Studies of Texas AkM University in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE May... 1992 Major Subject: Geophysics DETECTION OF AZIMUTHAL ANISOTROPY FROM 3-D P-WAVE SEISMIC DATA A Thesis by ALI YILDIZEL Approved as to style and content by: Steve I . Iarder (Chair of Committee) Joel S. Watkins (Member) Robert R. Berg...

Yildizel, Ali

2012-06-07T23:59:59.000Z

44

Energy Flow Energy Flow Energy Flow A.Ukleja, T.Tymieniecka, I.Skillicorn 1 Azimuthal asymmetry  

E-Print Network (OSTI)

Energy Flow Energy Flow Energy Flow A.Ukleja, T.Tymieniecka, I.Skillicorn 1 Azimuthal asymmetry using energy flow method Azimuthal angle distribution at Q2 >100 GeV2 Energy flow method.Ukleja on behalf of the ZEUS Collaboration #12; Energy Flow Energy Flow Energy Flow A.Ukleja, T.Tymieniecka, I

45

Anisotropic geometrical-spreading correction for wide-azimuth P-wave reflections  

E-Print Network (OSTI)

Anisotropic geometrical-spreading correction for wide-azimuth P-wave reflections Xiaoxia Xu1 spreading in stratified azi- muthally anisotropic media. The P-wave geometrical-spreading factor systems, nonhydrostatic stresses, or dipping trans- versely isotropic layers e.g., shales . The inversion

Tsvankin, Ilya

46

SAR image localization and target recognition research based on the azimuth circle adjustment  

Science Journals Connector (OSTI)

According to the work mechanism of space synthetic aperture radar (SAR), this text introduced the localization algorithms of SAR image and the method of system error adjustment. On the basis of the concept of the azimuth circle and the combination of ... Keywords: ITIL, ITSM, UML, framework, process model

Guang Yang; Xiaojuan Wang; Dejun Li; Bai Zhang; Kun Gao

2009-01-01T23:59:59.000Z

47

3-D shear wave radially and azimuthally anisotropic velocity model of the North American upper mantle  

Science Journals Connector (OSTI)

......partially during the subsequent tectonism of flat Farallon subduction (Humphreys et al...Thick-structured Proterozoic lithosphere of the Rocky Mountain region, GSA Today, 11, 4-9...azimuthal anisotropy beneath the Colorado Rocky Mountains, in The Rocky Mountain Region-An......

Huaiyu Yuan; Barbara Romanowicz; Karen M. Fischer; David Abt

2011-03-01T23:59:59.000Z

48

Frequency domain design of interval controller  

E-Print Network (OSTI)

significant role in the analysis and design of interval systems. Its external properties are also discussed. The image set approach & frequency domain criteria can be used to calculate the IP stability margin. The frequency domain criteria are used...

Park, Wunyong

1993-01-01T23:59:59.000Z

49

Extremal properties of interval control systems  

E-Print Network (OSTI)

EXTREMAL PROPERTIES OF INTERVAL CONTROL SYSTEMS A Thesis by FARIS RAGHEB KAMAL Submitted to the Office of Graduate Studies of Texas A&M University in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE May 1991 Major... Subject: Electrical Engineering EXTREMAL PROPERTIES OF INTERVAL CONTROL SYSTEMS A Thesis by FARIS RAGHEB I&AMAL Approved as to style and content b1 Mohammed A. Dahleh (Chair of Committee) ostas Georghiades (Member ) Ehsani Mehrdad (Member...

Kamal, Faris Ragheb

2012-06-07T23:59:59.000Z

50

Interval Data Systems Inc | Open Energy Information  

Open Energy Info (EERE)

Interval Data Systems Inc Interval Data Systems Inc Jump to: navigation, search Name Interval Data Systems Inc Address 135 Beaver Street Place Waltham, Massachusetts Zip 02452 Sector Efficiency Product Efficiency and monitoring solutions for buildings Website http://www.intdatsys.com/ Coordinates 42.384614°, -71.207508° Loading map... {"minzoom":false,"mappingservice":"googlemaps3","type":"ROADMAP","zoom":14,"types":["ROADMAP","SATELLITE","HYBRID","TERRAIN"],"geoservice":"google","maxzoom":false,"width":"600px","height":"350px","centre":false,"title":"","label":"","icon":"","visitedicon":"","lines":[],"polygons":[],"circles":[],"rectangles":[],"copycoords":false,"static":false,"wmsoverlay":"","layers":[],"controls":["pan","zoom","type","scale","streetview"],"zoomstyle":"DEFAULT","typestyle":"DEFAULT","autoinfowindows":false,"kml":[],"gkml":[],"fusiontables":[],"resizable":false,"tilt":0,"kmlrezoom":false,"poi":true,"imageoverlays":[],"markercluster":false,"searchmarkers":"","locations":[{"text":"","title":"","link":null,"lat":42.384614,"lon":-71.207508,"alt":0,"address":"","icon":"","group":"","inlineLabel":"","visitedicon":""}]}

51

Inversion of azimuthally dependent NMO velocity in transversely isotropic media with a tilted axis of symmetry  

SciTech Connect

Just as the transversely isotropic model with a vertical symmetry axis (VTI media) is typical for describing horizontally layered sediments, transverse isotropy with a tilted symmetry axis (TTI) describes dipping TI layers (such as tilted shale beds near salt domes) or crack systems. P-wave kinematic signatures in TTI media are controlled by the velocity V{sub PO} in the symmetry direction, Thomsen's anisotropic coefficients {xi} and {delta}, and the orientation (tilt {nu} and azimuth {beta}) of the symmetry axis. Here, the authors show that all five parameters can be obtained from azimuthally varying P-wave NMO velocities measured for two reflectors with different dips and/or azimuths (one of the reflectors can be horizontal). The shear-wave velocity V{sub SO} in the symmetry direction, which has negligible influence on P-wave kinematic signatures, can be found only from the moveout of shear waves. Using the exact NMO equation, the authors examine the propagation of errors in observed moveout velocities into estimated values of the anisotropic parameters and establish the necessary conditions for a stable inversion procedure. Since the azimuthal variation of the NMO velocity is elliptical, each reflection event provides them with up to three constraints on the model parameters. Generally, the five parameters responsible for P-wave velocity can be obtained from two P-wave ellipses, but the feasibility of the moveout inversion strongly depends on the tilt {nu}. While most of the analysis is carried out for a single layer, the authors also extend the inversion algorithm to vertically heterogeneous TTI media above a dipping reflector using the generalized Dix equation. A synthetic example for a strongly anisotropic, stratified TTI medium demonstrates a high accuracy of the inversion.

Grechka, V.; Tsvankin, I.

2000-02-01T23:59:59.000Z

52

The influence of the nonverticality of the azimuthal rotation axis of the concentrator (heliostat) on program tracking accuracy  

Science Journals Connector (OSTI)

It is shown that the nonverticality of the azimuthal axis has a significant influence on the accuracy of the program control of the concentrator (heliostat). To eliminate this error, it is...

A. A. Abdurakhmanov; S. A. Orlov; A. S. Saribaev; Kh. K. Fazilov

2010-12-01T23:59:59.000Z

53

On the analysis of small?angle scattering with elliptical azimuthal symmetry  

Science Journals Connector (OSTI)

Inhomogeneities which have azimuthal symmetry around some unique axis exhibit small?angle neutron scattering with elliptical symmetry. It is not necessary that these inhomogeneities have an ellipsoidal shape. The model of Debye e t a l. has been generalized to incorporate an anisotropic correlation length having this symmetry. A method is given for fitting two?dimensional intensity data to this model. This is illustrated by data taken for sections of slate and shale rock cut normal to the direction of the bedding planes and which exhibit both large? and small?pore anisotropies.

Peter L. Hall; D. F. R. Mildner

1983-01-01T23:59:59.000Z

54

Measurement of Dijet Azimuthal Decorrelations in pp Collisions at {radical}(s)=7 TeV  

SciTech Connect

Azimuthal decorrelations between the two central jets with the largest transverse momenta are sensitive to the dynamics of events with multiple jets. We present a measurement of the normalized differential cross section based on the full data set ({integral}Ldt=36 pb{sup -1}) acquired by the ATLAS detector during the 2010 {radical}(s)=7 TeV proton-proton run of the LHC. The measured distributions include jets with transverse momenta up to 1.3 TeV, probing perturbative QCD in a high-energy regime.

Aad, G.; Ahles, F.; Beckingham, M.; Bernhard, R.; Bitenc, U.; Bruneliere, R.; Caron, S.; Carpentieri, C.; Christov, A.; Dahlhoff, A.; Dietrich, J.; Eckert, S.; Fehling-Kaschek, M.; Flechl, M.; Glatzer, J. [Fakultaet fuer Mathematik und Physik, Albert-Ludwigs-Universitaet, Freiburg i.Br. (Germany); Abbott, B. [Homer L. Dodge Department of Physics and Astronomy, University of Oklahoma, Norman Oklahoma (United States); Abdallah, J.; Bosman, M.; Casado, M. P.; Cavalli-Sforza, M. [Institut de Fisica d'Altes Energies and Universitat Autonoma de Barcelona and ICREA, Barcelona (Spain)

2011-04-29T23:59:59.000Z

55

Optimal solar-PV tilt angle and azimuth: An Ontario (Canada) case-study  

Science Journals Connector (OSTI)

The purpose of this article is to determine the tilt angle and azimuth for a photovoltaic panel in Ontario (Canada) at which revenue is maximised. Measured and modelled solar radiation data, simulated photovoltaic panel performance, hourly electricity market data and details regarding pricing regimes from 2003 to 2008 are used to study two different locations. In all instances, the desired tilt angle is slightly less than latitude (depending upon the particular pricing regime, between 36° and 38° for Ottawa, which is at a latitude of 45°N, and between 32° and 35° for Toronto, which is at a latitude of 44°N), and the desired azimuth is close to due south (depending upon the particular pricing regime, between 4° west of due south and 6° east of due south for Ottawa, and between 1° west of due south and 2° east of due south for Toronto). In conclusion, the importance of solar electricity – particularly valuable because of when it is produced and where it can be produced – is highlighted, as are future priorities for research.

Ian H. Rowlands; Briana Paige Kemery; Ian Beausoleil-Morrison

2011-01-01T23:59:59.000Z

56

Preliminaries Conserved Interval Distance between Non-trivial  

E-Print Network (OSTI)

Outline Preliminaries Results Conclusion Conserved Interval Distance between Non-trivial Genomes.Rizzi@unitn.it August the 16th Guillaume Blin, Romeo Rizzi Conserved Interval Distance between Non-trivial Genomes #12 Guillaume Blin, Romeo Rizzi Conserved Interval Distance between Non-trivial Genomes #12;Outline

Blin, Guillaume

57

ASYMPTOTIC BEHAVIOR OF THE ENTROPY OF INTERVAL MAPS  

E-Print Network (OSTI)

ASYMPTOTIC BEHAVIOR OF THE ENTROPY OF INTERVAL MAPS ALEXANDER BLOKH AND JOZEF BOBOK Abstract. We obtain upper estimates on the entropy of interval maps of given modality and Sharkovskii type. Following our results we formulate a conjecture on asymptotic behavior of the entropy of interval maps. 1

Blokh, Alexander

58

Azimuthal Charged-Particle Correlations and Possible Local Strong Parity Violation  

SciTech Connect

Parity-odd domains, corresponding to non-trivial topological solutions of the QCD vacuum, might be created during relativistic heavy-ion collisions. These domains are predicted to lead to charge separation of quarks along the system's orbital momentum axis. We investigate a three particle azimuthal correlator which is a {Rho} even observable, but directly sensitive to the charge separation effect. We report measurements of charged hadrons near center-of-mass rapidity with this observable in Au+Au and Cu+Cu collisions at {radical}s{sub NN} = 200 GeV using the STAR detector. A signal consistent with several expectations from the theory is detected. We discuss possible contributions from other effects that are not related to parity violation.

STAR Collaboration; Abelev, Betty

2010-07-05T23:59:59.000Z

59

Collective flow by the azimuthal correlation of projectile fragments in relativistic heavy-ion collisions  

Science Journals Connector (OSTI)

An analysis that does not require the determination of reaction plane on an event-by-event basis, and involves only azimuthal correlation function of the projectile fragment pairs, has been employed to measure the collective flow of nuclear matter. Using this technique, we study the flow of projectile fragments of charge Z?2 produced in Au197 induced-emulsion reactions at 10.6A GeV. The collective flow is observed to be the most pronounced in semicentral collisions. The results are compared with those of Si28 at 14.5A GeV, U238 at 0.96A GeV, Kr84 at 1.52A GeV, and Fe56 at 1.7A GeV.

G. Singh and P. L. Jain

1994-06-01T23:59:59.000Z

60

Multiparticle azimuthal correlations of negative pions in nucleus-nucleus collisions  

SciTech Connect

Multiparticle azimuthal correlations of {pi}{sup -} mesons have been studied in dC, HeC, CC, CNe, MgMg, (d, He)Ta, CCu, CTa, and OPb collisions at momentum of 4.2, 4.5 GeV/c per nucleon within the standard transverse momentum analysis method of P. Danielewicz and G. Odyniec. The data were obtained by SKM-200-GIBS and Propane Bubble Chamber Collaborations of JINR. The axis has been selected in the phase space and with respect to this axis {pi}{sup -} meson correlations were observed. The values of the coefficient of the correlations linearly depend on the mass numbers of projectile (A{sub P}) and target (A{sub T}) nuclei. The Quark-Gluon String Model satisfactorily describes the experimental results.

Chkhaidze, L. V., E-mail: ichkhaidze@yahoo.com; Djobava, T. D.; Kharkhelauri, L. L. [Tbilisi State University, High Energy Physics Institute (Georgia); Kladnitskaya, E. N. [Joint Institute for Nuclear Research (Russian Federation)

2012-07-15T23:59:59.000Z

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61

Magnetic field stabilization by temperature control of an azimuthally varying field cyclotron magnet  

SciTech Connect

A magnetic field drift, gradual decrease of the order of 10{sup -4} in several tens of hours, was observed with the beam intensity decrease in an operation of an azimuthally varying field (AVF) cyclotron. From our experimental results, we show that the temperature increase of the magnet iron by the heat transfer from the excitation coils can induce such change of the magnetic field as to deteriorate the beam quality. The temperature control of the magnet iron was realized by thermal isolation between the main coil and the yoke and by precise control of the cooling water temperature of the trim coils attached to the pole surfaces in order to prevent temperature change of the magnet iron. The magnetic field stability of {+-}5x10{sup -6} and the beam intensity stability of {+-}2% have been achieved by this temperature control.

Okumura, S.; Arakawa, K.; Fukuda, M.; Nakamura, Y.; Yokota, W.; Ishimoto, T.; Kurashima, S.; Ishibori, I.; Nara, T.; Agematsu, T.; Sano, M.; Tachikawa, T. [Japan Atomic Energy Research Institute (JAERI), 1233 Watanuki, Takasaki, Gunma 370-1292 (Japan); Sumitomo Heavy Industries, Ltd. (SHI), 5-2 Soubiraki, Niihama, Ehime 792-8588 (Japan)

2005-03-01T23:59:59.000Z

62

Steam turbine-generator outage interval extension  

SciTech Connect

In the industry`s growing competitive climate, utilities are seeking ways to tap the economic benefits to be derived from maximizing intervals between major turbine-generator (T-G) inspections and overhauls--while ensuring protection of these assets. EPRI and others have developed a substantial body of technology which addresses many of the condition assessment issues that underlie T-G inspection and overhaul decisions. Examples include remaining life determination of critical components such as rotors and blades. While the initial focus of this technology had previously been to support T-G run-repair-replace decision making, this technology can also serve as a basis for run-inspect decisions. This paper describes EPRI`s initiative to develop and implement a T-G Health Management System. By providing key status reports reflecting the on-line health of critical components, in terms of life consumption, performance degradation and probability of failure, this system will provide a means to justify extending T-G operations between inspections and overhauls.

McCloskey, T.H. [Electric Power Research Institute, Palo Alto, CA (United States); Pollard, M. [Carolina Power & Light Company, Raleigh, NC (United States); Dewey, R.; Roemer, M. [Stress Technology Inc., Rochester, NY (United States)

1996-07-01T23:59:59.000Z

63

Estimation of interval anisotropy parameters using velocity-independent layer stripping  

E-Print Network (OSTI)

by VILS in the shale layer above the reservoir are more plausible and less influenced by noise than those homogeneous VTI overburden. For 3D wide-azimuth data from layered azimuthally anisotropic media, the effective . Unfortunately, NMO velocity often is insufficient to build the ve- locity field for anisotropic media, even

Tsvankin, Ilya

64

Monte Carlo approach for hadron azimuthal correlations in high energy proton and nuclear collisions  

E-Print Network (OSTI)

We use a Monte Carlo approach to study hadron azimuthal angular correlations in high energy proton-proton and central nucleus-nucleus collisions at the BNL Relativistic Heavy Ion Collider (RHIC) energies at mid-rapidity. We build a hadron event generator that incorporates the production of $2\\to 2$ and $2\\to 3$ parton processes and their evolution into hadron states. For nucleus-nucleus collisions we include the effect of parton energy loss in the Quark-Gluon Plasma using a modified fragmentation function approach. In the presence of the medium, for the case when three partons are produced in the hard scattering, we analyze the Monte Carlo sample in parton and hadron momentum bins to reconstruct the angular correlations. We characterize this sample by the number of partons that are able to hadronize by fragmentation within the selected bins. In the nuclear environment the model allows hadronization by fragmentation only for partons with momentum above a threshold $p_T^{{\\tiny{thresh}}}=2.4$ GeV. We argue that...

Ayala, Alejandro; Jalilian-Marian, Jamal; Magnin, J; Tejeda-Yeomans, Maria Elena

2012-01-01T23:59:59.000Z

65

Monte Carlo approach for hadron azimuthal correlations in high energy proton and nuclear collisions  

E-Print Network (OSTI)

We use a Monte Carlo approach to study hadron azimuthal angular correlations in high energy proton-proton and central nucleus-nucleus collisions at the BNL Relativistic Heavy Ion Collider (RHIC) energies at mid-rapidity. We build a hadron event generator that incorporates the production of $2\\to 2$ and $2\\to 3$ parton processes and their evolution into hadron states. For nucleus-nucleus collisions we include the effect of parton energy loss in the Quark-Gluon Plasma using a modified fragmentation function approach. In the presence of the medium, for the case when three partons are produced in the hard scattering, we analyze the Monte Carlo sample in parton and hadron momentum bins to reconstruct the angular correlations. We characterize this sample by the number of partons that are able to hadronize by fragmentation within the selected bins. In the nuclear environment the model allows hadronization by fragmentation only for partons with momentum above a threshold $p_T^{{\\tiny{thresh}}}=2.4$ GeV. We argue that one should treat properly the effect of those partons with momentum below the threshold, since their interaction with the medium may lead to showers of low momentum hadrons along the direction of motion of the original partons as the medium becomes diluted.

Alejandro Ayala; Isabel Dominguez; Jamal Jalilian-Marian; J. Magnin; Maria Elena Tejeda-Yeomans

2012-07-31T23:59:59.000Z

66

Exploration of jet energy loss via direct $?$-charged particle azimuthal correlation measurements  

E-Print Network (OSTI)

The multiplicities of charged particles azimuthally associated with direct photons and $\\pi^{0}$ have been measured for Au+Au, p+p, and d+Au collisions at $\\sqrt{s_{NN}}$ = 200 GeV in the STAR experiment. Charged particles with transverse momentum 0.5 $<$ $p_T^{h^{\\pm}}$ $<$ 16 GeV/c for p+p and d+Au, and 3 $<$ $p_T^{h^{\\pm}}$ $<$ 16 GeV/c for Au+Au and pseudorapidity $\\mid\\eta\\mid$ $\\leq$ 1.5 in coincidence with direct photons and $\\pi^{0}$ of high transverse momentum 8 $<$ $p_T^{\\gamma,\\pi^{0}}$ $<$ 16 GeV/c at $\\mid\\eta\\mid$ $\\leq$ 0.9 have been used for this analysis. Within the considered range of kinematics, the observed suppressions of the associated yields per direct $\\gamma$ in central Au+Au relative to p+p and d+Au are similar and constant with direct photon fractional energy $z_{T}$ ($z_{T}=p_{T}^{h^{\\pm}}/p_{T}^{\\gamma}$). The measured suppressions of the associated yields with direct $\\gamma$ are comparable to those with $\\pi^{0}$. The data are compared to theoretical predictions.

A. M. Hamed

2009-09-25T23:59:59.000Z

67

Analysis of interval-censored data with Weibull lifetime distribution  

E-Print Network (OSTI)

& OR Unit, Indian Statistical Institute, 203 B.T. Road, Kolkata, Pin 700108, India. Department of Mathematics and Statistics, Indian Institute of Technology Kanpur, Pin 208016, India. Corresponding author, e point. The event time is considered to be interval censored when an event occurs within some interval

Kundu, Debasis

68

Limitations in solar module azimuth and tilt angles in building integrated photovoltaics at low latitude tropical sites in Brazil  

Science Journals Connector (OSTI)

Abstract Photovoltaic (PV) generation depends directly on the amount of radiation received by solar modules at a given temperature, and annual irradiation varies according to site location and PV array position. In this paper, the limitations and the solar irradiation levels received by building surfaces in different positions (with azimuth and tilt angle variation) in capital cities in Brazil are shown, making use of the Brazilian global horizontal solar irradiation data provided by the SWERA (Solar and Wind Energy Resource Assessment) project. These data were processed to generate figures on the irradiation at various PV module orientations and slopes for each city, which show the relative radiation levels received on specific azimuth and tilt angles in relation to the ideal position. Results were validated using four real and operating PV systems. In general, variations in azimuth or slope did not cause large annual irradiation losses up to around 20° tilt angles. This shows to PV system planners that under these fairly flexible conditions it is possible to install PV on any orientation, keeping high levels of annual irradiation, and that limitations in orientation and tilt can be relatively low. It also allows a quick analysis of PV retrofit in building-applied photovoltaics (BAPV), when seeking the best building surfaces to incorporate PV.

Ísis Portolan dos Santos; Ricardo Rüther

2014-01-01T23:59:59.000Z

69

Low-amplitude magnetic vortex core reversal by non-linear interaction between azimuthal spin waves and the vortex gyromode  

SciTech Connect

We show, by experiments and micromagnetic simulations in vortex structures, that an active “dual frequency” excitation of both the sub-GHz vortex gyromode and multi-GHz spin waves considerably changes the frequency response of spin wave mediated vortex core reversal. Besides additional minima in the switching threshold, a significant broadband reduction of the switching amplitudes is observed, which can be explained by non-linear interaction between the vortex gyromode and the spin waves. We conclude that the well known frequency spectra of azimuthal spin waves in vortex structures are altered substantially, when the vortex gyromode is actively excited simultaneously.

Sproll, Markus; Noske, Matthias; Kammerer, Matthias; Dieterle, Georg; Weigand, Markus; Stoll, Hermann; Schütz, Gisela [Max Planck Institute for Intelligent Systems (formerly MPI for Metals Research), Heisenbergstr. 3, 70569 Stuttgart (Germany)] [Max Planck Institute for Intelligent Systems (formerly MPI for Metals Research), Heisenbergstr. 3, 70569 Stuttgart (Germany); Bauer, Hans; Gangwar, Ajay; Woltersdorf, Georg; Back, Christian H. [Department of Physics, University of Regensburg, Universitätsstr. 31, 93040 Regensburg (Germany)] [Department of Physics, University of Regensburg, Universitätsstr. 31, 93040 Regensburg (Germany)

2014-01-06T23:59:59.000Z

70

Transition from in-plane to out-of-plane azimuthal enhancement inAu+Au collisions  

SciTech Connect

The incident energy at which the azimuthal distributions in semi-central heavy ion collisions change from in-plane to out-of-plane enhancement--E{sub tran} is studied as a function of mass of emitted particles, their transverse momentum and centrality for Au+Au collisions. The analysis is performed in a reference frame rotated with the sidewards flow angle ({Theta}{sub flow}) relative to the beam axis. A systematic decrease of E{sub tran} as function of mass of the reaction products, their transverse momentum and collision centrality is evidenced. The predictions of a microscopic transport model (IQMD) are compared with the experimental results.

Andronic, A.; Stoicea, G.; Petrovici, M.; Simion, V.; Crochet,P.; Alard, J.P.; Averbeck, R.; Barret, V.; Basrak, Z.; Bastid, N.; Bendarag, A.; Berek, G.; Caplar, R.; Devismes, A.; Dupieux, Dzelalija M.; Eskef, M.; Finck, Ch.; Fodor, Z.; Gobbi, A.; Grishkin, Y.; Hartmann,O.N.; Herrmann, N.; Hildenbrand, K.D.; Hong, B.; Kecskemeti, J.; Kim,Y.J.; Kirejczyk, M.; Korolija, M.; Kotte, R.; Kress, T.; Kutsche, R.; Lebedev, A.; Lee, K.S.; Leifels, Y.; Manko, V.; Merlitz, H.; Neubert, W.; Pelte, D.; Plettner, C.; Rami, F.; Resdorf, W.; de Schauenberg, B.; Schull, D.; Seres, Z.; Sikora, B.; Sim, K.S.; Siwek-Wilczynska, K.; Smolyankin, V.; Stockmeier, M.R.; Vasiliev, M.; Wagner, P.; Wisniewski,K.; Wohlfarth, D.; Yushmanov, I.; Zhilin, A.

2000-08-09T23:59:59.000Z

71

Phase Structure of Gauge Theories on an Interval  

E-Print Network (OSTI)

We discuss gauge symmetry breaking in a general framework of gauge theories on an interval. We first derive a possible set of boundary conditions for a scalar field, which are compatible with several consistency requirements. It is shown that with these boundary conditions the scalar field can acquire a nontrivial vacuum expectation value even if the scalar mass square is positive. Any nonvanishing vacuum expectation value cannot be a constant but, in general, depends on the extra dimensional coordinate of the interval. The phase diagram of broken/unbroken gauge symmetry possesses a rich structure in the parameter space of the length of the interval, the scalar mass and the boundary conditions. We also discuss 4d chiral fermions and fermion mass hierarchies in our gauge symmetry breaking scenario.

Fujimoto, Yukihiro; Ohya, Satoshi; Sakamoto, Makoto

2011-01-01T23:59:59.000Z

72

Phase Structure of Gauge Theories on an Interval  

E-Print Network (OSTI)

We discuss gauge symmetry breaking in a general framework of gauge theories on an interval. We first derive a possible set of boundary conditions for a scalar field, which are compatible with several consistency requirements. It is shown that with these boundary conditions the scalar field can acquire a nontrivial vacuum expectation value even if the scalar mass square is positive. Any nonvanishing vacuum expectation value cannot be a constant but, in general, depends on the extra dimensional coordinate of the interval. The phase diagram of broken/unbroken gauge symmetry possesses a rich structure in the parameter space of the length of the interval, the scalar mass and the boundary conditions. We also discuss 4d chiral fermions and fermion mass hierarchies in our gauge symmetry breaking scenario.

Yukihiro Fujimoto; Tomoaki Nagasawa; Satoshi Ohya; Makoto Sakamoto

2011-08-09T23:59:59.000Z

73

Flood control project selection using an interval type-2 entropy weight with interval type-2 fuzzy TOPSIS  

Science Journals Connector (OSTI)

Flood control project is a complex issue which takes economic social environment and technical attributes into account. Selection of the best flood control project requires the consideration of conflicting quantitative and qualitative evaluation criteria. When decision-makers’ judgment are under uncertainty it is relatively difficult for them to provide exact numerical values. The interval type-2 fuzzy set (IT2FS) is a strong tool which can deal with the uncertainty case of subjective incomplete and vague information. Besides it helps to solve for some situations where the information about criteria weights for alternatives is completely unknown. Therefore this paper is adopted the information interval type-2 entropy concept into the weighting process of interval type-2 fuzzy TOPSIS. This entropy weight is believed can effectively balance the influence of uncertainty factors in evaluating attribute. Then a modified ranking value is proposed in line with the interval type-2 entropy weight. Quantitative and qualitative factors that normally linked with flood control project are considered for ranking. Data in form of interval type-2 linguistic variables were collected from three authorised personnel of three Malaysian Government agencies. Study is considered for the whole of Malaysia. From the analysis it shows that diversion scheme yielded the highest closeness coefficient at 0.4807. A ranking can be drawn using the magnitude of closeness coefficient. It was indicated that the diversion scheme recorded the first rank among five causes.

2014-01-01T23:59:59.000Z

74

Interval estimation in calibration problems: an alternate approach  

E-Print Network (OSTI)

measurement of the dependent varia- ble. This interval will depend upon the dependent variable and also on the outcome of the calibration experiment. For each unknown a state- ment is made in the sense that it belongs to the interval. Then he searches... is computed as 2 n , 1(yi ? y) Ss n ? 2 and will also be denoted by NSE. (2. 2) In the calibration problem, the classical estimator of x* given an obsezvation y* is y* ? b 0 x* bl Under the normality assumption x" is the NLE of x* (Graybill 1976...

Quaino, Oscar Rodolfo

2012-06-07T23:59:59.000Z

75

Improved approximation algorithm for the jump number of interval orders  

Science Journals Connector (OSTI)

Abstract The jump number problem for posets is to find a linear extension in which the number of incomparable adjacent pairs is minimized. In this paper the class of interval orders is considered. Three 3/2-approximation algorithms for this problem have been known for some time. By a previous work of Mitas, the problem may be reformulated as a subgraph packing task. We prove that the problem reduces also to a set cover task, and we establish an improved bound of 1.484 to the approximation ratio of the jump number on interval orders.

Przemys?aw Krysztowiak

2013-01-01T23:59:59.000Z

76

Measurement of the Azimuthal Anisotropy of Neutral Pions in Pb-Pb Collisions at ?sNN=2.76??TeV  

First measurements of the azimuthal anisotropy of neutral pions produced in Pb-Pb collisions at a center-of-mass energy of ?sNN =2.76??TeV are presented. The amplitudes of the second Fourier component (v2) of the ?0 azimuthal distributions are extracted using an event-plane technique. The values of v2 are studied as a function of the neutral pion transverse momentum (pT) for different classes of collision centrality in the kinematic range 1.6T2(pT) are similar to previously reported ?0 azimuthal anisotropy results from ?sNN=200??GeV Au-Au collisions at RHIC, despite a factor of ?14 increase in the center-of-mass energy. In the momentum range 2.5T<5.0??GeV/c , the neutral pion anisotropies are found to be smaller than those observed by CMS for inclusive charged particles.

Chatrchyan, S.; Khachatryan, V.; Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Aguilo, E.; Bergauer, T.; Dragicevic, M.; Erö, J.; Fabjan, C.; Friedl, M.; Frühwirth, R.; Ghete, V. M.; Hammer, J.; Hörmann, N.; Hrubec, J.; Jeitler, M.; Kiesenhofer, W.; Knünz, V.; Krammer, M.; Krätschmer, I.; Liko, D.; Mikulec, I.; Pernicka, M.; Rahbaran, B.; Rohringer, C.; Rohringer, H.; Schöfbeck, R.; Strauss, J.; Taurok, A.; Waltenberger, W.; Walzel, G.; Widl, E.; Wulz, C.-E.; Mossolov, V.; Shumeiko, N.; Suarez Gonzalez, J.; Bansal, S.; Cornelis, T.; De Wolf, E. A.; Janssen, X.; Luyckx, S.; Mucibello, L.; Ochesanu, S.; Roland, B.; Rougny, R.; Selvaggi, M.; Staykova, Z.; Van Haevermaet, H.; Van Mechelen, P.; Van Remortel, N.; Van Spilbeeck, A.; Blekman, F.; Blyweert, S.; D’Hondt, J.; Gonzalez Suarez, R.; Kalogeropoulos, A.; Maes, M.; Olbrechts, A.; Van Doninck, W.; Van Mulders, P.; Van Onsem, G. P.; Villella, I.; Clerbaux, B.; De Lentdecker, G.; Dero, V.; Gay, A. P. R.; Hreus, T.; Léonard, A.; Marage, P. E.; Reis, T.; Thomas, L.; Vander Marcken, G.; Vander Velde, C.; Vanlaer, P.; Wang, J.; Adler, V.; Beernaert, K.; Cimmino, A.; Costantini, S.; Garcia, G.; Grunewald, M.; Klein, B.; Lellouch, J.; Marinov, A.; Mccartin, J.; Ocampo Rios, A. A.; Ryckbosch, D.; Strobbe, N.; Thyssen, F.; Tytgat, M.; Verwilligen, P.; Walsh, S.; Yazgan, E.; Zaganidis, N.; Basegmez, S.; Bruno, G.; Castello, R.; Ceard, L.; Delaere, C.; du Pree, T.; Favart, D.; Forthomme, L.; Giammanco, A.; Hollar, J.; Lemaitre, V.; Liao, J.; Militaru, O.; Nuttens, C.; Pagano, D.; Pin, A.; Piotrzkowski, K.; Schul, N.; Vizan Garcia, J. M.; Beliy, N.; Caebergs, T.; Daubie, E.; Hammad, G. H.; Alves, G. A.; Correa Martins Junior, M.; De Jesus Damiao, D.; Martins, T.; Pol, M. E.; Souza, M. H. G.; Aldá Júnior, W. L.; Carvalho, W.; Custódio, A.; Da Costa, E. M.; De Oliveira Martins, C.; Fonseca De Souza, S.; Matos Figueiredo, D.; Mundim, L.; Nogima, H.; Oguri, V.; Prado Da Silva, W. L.; Santoro, A.; Soares Jorge, L.; Sznajder, A.; Anjos, T. S.; Bernardes, C. A.; Dias, F. A.; Fernandez Perez Tomei, T. R.; Gregores, E. M.; Lagana, C.; Marinho, F.; Mercadante, P. G.; Novaes, S. F.; Padula, Sandra S.; Genchev, V.; Iaydjiev, P.; Piperov, S.; Rodozov, M.; Stoykova, S.; Sultanov, G.; Tcholakov, V.; Trayanov, R.; Vutova, M.; Dimitrov, A.; Hadjiiska, R.; Kozhuharov, V.; Litov, L.; Pavlov, B.; Petkov, P.; Bian, J. G.; Chen, G. M.; Chen, H. S.; Jiang, C. H.; Liang, D.; Liang, S.; Meng, X.; Tao, J.; Wang, J.; Wang, X.; Wang, Z.; Xiao, H.; Xu, M.; Zang, J.; Zhang, Z.; Asawatangtrakuldee, C.; Ban, Y.; Guo, S.; Guo, Y.; Li, W.; Liu, S.; Mao, Y.; Qian, S. J.; Teng, H.; Wang, D.; Zhang, L.; Zhu, B.; Zou, W.; Avila, C.; Gomez, J. P.; Gomez Moreno, B.; Osorio Oliveros, A. F.; Sanabria, J. C.; Godinovic, N.; Lelas, D.; Plestina, R.; Polic, D.; Puljak, I.; Antunovic, Z.; Kovac, M.; Brigljevic, V.; Duric, S.; Kadija, K.; Luetic, J.; Morovic, S.; Attikis, A.; Galanti, M.; Mavromanolakis, G.; Mousa, J.; Nicolaou, C.; Ptochos, F.; Razis, P. A.; Finger, M.; Finger, M.; Assran, Y.; Elgammal, S.; Ellithi Kamel, A.; Khalil, S.; Mahmoud, M. A.; Radi, A.; Kadastik, M.; Müntel, M.; Raidal, M.; Rebane, L.; Tiko, A.; Eerola, P.; Fedi, G.; Voutilainen, M.; Härkönen, J.; Heikkinen, A.; Karimäki, V.; Kinnunen, R.; Kortelainen, M. J.; Lampén, T.; Lassila-Perini, K.; Lehti, S.; Lindén, T.; Luukka, P.; Mäenpää, T.; Peltola, T.; Tuominen, E.; Tuominiemi, J.; Tuovinen, E.; Ungaro, D.; Wendland, L.; Banzuzi, K.; Karjalainen, A.; Korpela, A.; Tuuva, T.; Besancon, M.; Choudhury, S.; Dejardin, M.; Denegri, D.; Fabbro, B.; Faure, J. L.; Ferri, F.; Ganjour, S.; Givernaud, A.; Gras, P.; Hamel de Monchenault, G.; Jarry, P.; Locci, E.; Malcles, J.; Millischer, L.; Nayak, A.; Rander, J.; Rosowsky, A.; Shreyber, I.; Titov, M.; Baffioni, S.; Beaudette, F.; Benhabib, L.; Bianchini, L.; Bluj, M.; Broutin, C.; Busson, P.; Charlot, C.; Daci, N.; Dahms, T.; Dobrzynski, L.; Granier de Cassagnac, R.; Haguenauer, M.; Miné, P.; Mironov, C.; Naranjo, I. N.; Nguyen, M.; Ochando, C.; Paganini, P.; Sabes, D.; Salerno, R.; Sirois, Y.; Veelken, C.; Zabi, A.; Agram, J.-L.; Andrea, J.; Bloch, D.; Bodin, D.; Brom, J.-M.; Cardaci, M.; Chabert, E. C.; Collard, C.; Conte, E.; Drouhin, F.; Ferro, C.; Fontaine, J.-C.; Gelé, D.; Goerlach, U.; Juillot, P.; Le Bihan, A.-C.; Van Hove, P.; Fassi, F.; Mercier, D.; Beauceron, S.; Beaupere, N.; Bondu, O.; Boudoul, G.; Chasserat, J.; Chierici, R.; Contardo, D.; Depasse, P.; El Mamouni, H.; Fay, J.; Gascon, S.; Gouzevitch, M.; Ille, B.; Kurca, T.; Lethuillier, M.; Mirabito, L.; Perries, S.; Sordini, V.; Tschudi, Y.; Verdier, P.; Viret, S.; Tsamalaidze, Z.; Anagnostou, G.; Beranek, S.; Edelhoff, M.; Feld, L.; Heracleous, N.; Hindrichs, O.; Jussen, R.; Klein, K.; Merz, J.; Ostapchuk, A.

2013-01-01T23:59:59.000Z

77

Comparing Bacterial Genomes by Searching their Common Intervals  

E-Print Network (OSTI)

Comparing Bacterial Genomes by Searching their Common Intervals S´ebastien Angibaud, Damien. Comparing bacterial genomes implies the use of a dedicated measure. It relies on comparing circular genomes genomes that takes into account duplications. Its application on a concrete case, comparing E. coli and V

Fertin, Guillaume

78

Quantum ergodicity for graphs related to interval maps  

E-Print Network (OSTI)

We prove quantum ergodicity for a family of graphs that are obtained from ergodic one-dimensional maps of an interval using a procedure introduced by Pakonski et al (J. Phys. A, v. 34, 9303-9317 (2001)). As observables we take the L^2 functions on the interval. The proof is based on the periodic orbit expansion of a majorant of the quantum variance. Specifically, given a one-dimensional, Lebesgue-measure-preserving map of an interval, we consider an increasingly refined sequence of partitions of the interval. To this sequence we associate a sequence of graphs, whose directed edges correspond to elements of the partitions and on which the classical dynamics approximates the Perron-Frobenius operator corresponding to the map. We show that, except possibly for subsequences of density 0, the eigenstates of the quantum graphs equidistribute in the limit of large graphs. For a smaller class of observables we also show that the Egorov property, a correspondence between classical and quantum evolution in the semiclassical limit, holds for the quantum graphs in question.

G. Berkolaiko; J. P. Keating; U. Smilansky

2006-07-07T23:59:59.000Z

79

Stochastic EM algorithm for doubly interval-censored data  

Science Journals Connector (OSTI)

......the are sampled from a finite set of values. Recall that, for...vector for are based on the risk set at each event time (i.e...To ensure that the intervals cover most of the generated values...the th iteration: where is the set of parameters estimated from......

David Dejardin; Emmanuel Lesaffre

2013-09-01T23:59:59.000Z

80

Use of Utility Interval Meters in an Industrial Energy Audit  

E-Print Network (OSTI)

This paper describes a unique approach to an energy audit of a large tank farm. The audit was unusual in that it was located out-of-doors and the energy-using equipment was made up almost entirely of pumps. The auditors used the utility interval...

Wallace, M.

2007-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" from the National Library of EnergyBeta (NLEBeta).
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81

R-R interval based paroxysmal atrial fibrillation analysis  

Science Journals Connector (OSTI)

Detection and classification of Atrial complexes from the ECG is of considerable importance in critical patient care monitoring of dangerous heart conditions. Accurate detection of Paroxysmal Atrial Fibrillation (PAF) using Atrial Premature Complexes(APC) ... Keywords: APC, ECG, PAF, R-R interval, arrhythmia

S. S. Kadge; M. S. Panse

2011-02-01T23:59:59.000Z

82

Generalizing the Wilcoxon rank-sum test for interval data  

Science Journals Connector (OSTI)

Abstract Here we propose an adaption of Wilcoxon's two-sample rank-sum test to interval data. This adaption is interval-valued: it computes the minimum and maximum values of the statistic when we rank the set of all feasible samples (all joint samples compatible with the initial set-valued information). We prove that these bounds can be explicitly computed using a very low computational cost algorithm. Interpreting this generalized test is straightforward: if the obtained interval-valued p-value is on one side of the significance level, we will be able to make a decision (reject/no reject). Otherwise, we will conclude that our information is too vague to lead to a clear decision. Our method is also applicable to quantized data: in the presence of quantized information, the joint sample may contain a high proportion of draws, which can prevent the test from drawing a clear conclusion. According to the usual convention, when there are ties, the ranks for the observations in a tie are taken to be the average of the ranks for those observations. This convention can lead to wrong conclusions. Here, we consider the family of all possible rank permutations, such that a sample containing ties will not just be associated with a single value, but rather with a collection of values for the Wilcoxon's rank-sum statistic, with each one of them being associated with a different p-value. When the impact of quantization is too high to lead to a clear decision, our test provides an interval-valued p-value that includes the chosen significance level. It indicates that there is no clear conclusion according to this test. Two different experiments exemplify the properties of the generalized test: the first one illustrates its ability to avoid wrong decisions in the presence of quantized data. The second one shows the performance of the generalized test when used with interval data.

Julien Perolat; Inés Couso; Kevin Loquin; Olivier Strauss

2015-01-01T23:59:59.000Z

83

Single-spin Azimuthal Asymmetries in Electroproduction of Neutral Pions in Semi-inclusive Deep-inelastic Scattering  

E-Print Network (OSTI)

A single-spin asymmetry in the azimuthal distribution of neutral pions relative to the lepton scattering plane has been measured for the first time in deep-inelastic scattering of positrons off longitudinally polarized protons. The analysing power in the sin(phi) moment of the cross section is 0.019 +/- 0.007(stat.) +/- 0.003(syst.). This result is compared to single-spin asymmetries for charged pion production measured in the same kinematic range. The pi^0 asymmetry is of the same size as the pi^+ asymmetry and shows a similar dependence on the relevant kinematic variables. The asymmetry is described by a phenomenological calculation based on a fragmentation function that represents sensitivity to the transverse polarization of the struck quark.

Airapetian, A; Amarian, M; Aschenauer, E C; Avakian, H; Avakian, R; Avetisian, A; Avetissian, E; Bailey, P; Bains, B; Baturin, V; Baumgarten, C; Beckmann, M; Belostotskii, S; Bernreuther, S; Bianchi, N; Böttcher, Helmut B; Borisov, A; Bouhali, O; Bouwhuis, M; Brack, J; Brauksiepe, S; Brückner, W; Brüll, A; Brunn, I; Bulten, H J; Capitani, G P; Chumney, P; Cisbani, E; Ciullo, G; Court, G R; Dalpiaz, P F; De Leo, R; De Nardo, L; De Sanctis, E; De Schepper, D; Devitsin, E G; De Witt-Huberts, P K A; Di Nezza, P; Dzhordzhadze, V; Düren, M; Ehrenfried, M; Elbakian, G M; Ellinghaus, F; Ely, J; Fantoni, A; Feshchenko, A; Felawka, L; Filippone, B W; Fischer, H; Fox, B; Franz, J; Frullani, S; Gärber, Y; Garibaldi, F; Garutti, E; Gavrilov, G E; Karibian, V; Golendukhin, A; Graw, G; Grebenyuk, O; Green, P W; Greeniaus, L G; Gute, A; Haeberli, W; Hafidi, K; Hartig, M; Hasch, D; Heesbeen, D; Heinsius, F H; Henoch, M; Hertenberger, R; Hesselink, W H A; Hofman, G J; Holler, Y; Holt, R J; Hommez, B; Iarygin, G; Izotov, A A; Jackson, H E; Jgoun, A; Jung, P; Kaiser, R; Kanesaka, J; Kinney, E R; Kiselev, A; Kitching, P; Kobayashi, H; Koch, N; Königsmann, K C; Kolster, H; Korotkov, V A; Kotik, E; Kozlov, V; Krauss, B; Krivokhizhin, V G; Kyle, G S; Lagamba, L; Laziev, A; Lenisa, P; Liebing, P; Lindemann, T; Lorenzon, W; Maas, A; Makins, N C R; Marukyan, H O; Masoli, F; McAndrew, M; McIlhany, K; Meissner, F; Menden, F; Meyners, N; Miklukho, O; Miller, C A; Milner, R; Muccifora, V; Mussa, R; Nagaitsev, A P; Nappi, E; Naryshkin, Yu; Nass, A; Negodaeva, K; Nowak, Wolf-Dieter; Oganesyan, K A; O'Neill, T G; Owen, B R; Pate, S F; Potashov, S Yu; Potterveld, D H; Raithel, M; Rakness, G; Rappoport, V; Redwine, R P; Reggiani, D; Reolon, A R; Rith, K; Robinson, D; Rostomyan, A; Ruh, M; Ryckbosch, D; Sakemi, Y; Sanjiev, I; Sato, F; Savin, I A; Scarlett, C; Schäfer, A; Schill, C; Schmidt, F; Schnell, G; Schüler, K P; Schwind, A; Seibert, J; Seitz, B; Shibata, T A; Shutov, V B; Simani, M C; Simon, A; Sinram, K; Steffens, E; Steijger, J J M; Stewart, J; Stösslein, U; Suetsugu, K; Taroian, S P; Terkulov, A R; Teryaev, O V; Tessarin, S; Thomas, E; Tipton, B; Tytgat, M; Urciuoli, G M; Van den Brand, J F J; van der Steenhoven, G; Van de Vyver, R; Van Hunen, J J; Vetterli, Martin C; Vikhrov, V V; Vincter, M G; Visser, J; Weiskopf, C; Wendland, J; Wilbert, J; Wise, T; Yen, S; Yoneyama, S; Zohrabyan, H G

2000-01-01T23:59:59.000Z

84

ECG beats classification using waveform similarity and RR interval  

E-Print Network (OSTI)

This paper present an electrocardiogram (ECG) beat classification method based on waveform similarity and RR interval. The purpose of the method is to classify six types of heart beats (normal beat, atrial premature beat, paced beat, premature ventricular beat, left bundle branch block beat and right bundle branch block beat). The electrocardiogram signal is first denoised using wavelet transform based techniques. Heart beats of 128 samples data centered on the R peak are extracted from the ECG signal and thence reduced to 16 samples data to constitute a feature. RR intervals surrounding the beat are also exploited as feature. A database of annotated beats is built for the classifier for waveform comparison to unknown beats. Tested on 46 records in the MIT/BIH arrhythmia database, the method shows classification rate of 97.52%.

Ka, Ahmad Khoureich

2011-01-01T23:59:59.000Z

85

Computational fluid dynamics analyses of lateral heat conduction, coolant azimuthal mixing and heat transfer predictions in a BR2 fuel assembly geometry.  

SciTech Connect

To support the analyses related to the conversion of the BR2 core from highly-enriched (HEU) to low-enriched (LEU) fuel, the thermal-hydraulics codes PLTEMP and RELAP-3D are used to evaluate the safety margins during steady-state operation (PLTEMP), as well as after a loss-of-flow, loss-of-pressure, or a loss of coolant event (RELAP). In the 1-D PLTEMP and RELAP simulations, conduction in the azimuthal and axial directions is not accounted. The very good thermal conductivity of the cladding and the fuel meat and significant temperature gradients in the lateral directions (axial and azimuthal directions) could lead to a heat flux distribution that is significantly different than the power distribution. To evaluate the significance of the lateral heat conduction, 3-D computational fluid dynamics (CFD) simulations, using the CFD code STAR-CD, were performed. Safety margin calculations are typically performed for a hot stripe, i.e., an azimuthal region of the fuel plates/coolant channel containing the power peak. In a RELAP model, for example, a channel between two plates could be divided into a number of RELAP channels (stripes) in the azimuthal direction. In a PLTEMP model, the effect of azimuthal power peaking could be taken into account by using engineering factors. However, if the thermal mixing in the azimuthal direction of a coolant channel is significant, a stripping approach could be overly conservative by not taking into account this mixing. STAR-CD simulations were also performed to study the thermal mixing in the coolant. Section II of this document presents the results of the analyses of the lateral heat conduction and azimuthal thermal mixing in a coolant channel. Finally, PLTEMP and RELAP simulations rely on the use of correlations to determine heat transfer coefficients. Previous analyses showed that the Dittus-Boelter correlation gives significantly more conservative (lower) predictions than the correlations of Sieder-Tate and Petukhov. STAR-CD 3-D simulations were performed to compare heat transfer predictions from CFD and the correlations. Section III of this document presents the results of this analysis.

Tzanos, C. P.; Dionne, B. (Nuclear Engineering Division)

2011-05-23T23:59:59.000Z

86

Mapping musical intervals to affective qualities: A projective study  

Science Journals Connector (OSTI)

Many claim that the various musical intervals used in Western music create identifiable affective impressions which musicians use for musical communication. Alain Danielou has proposed furthermore that these affective impressions form a space with a three?dimensional structure isomorphic to the natural three?dimensional structure of the intervals themselves (ratios composed of positive and negative powers of 2 3 and 5). To test this hypothesis 36 Marathi?speaking college students at Ahmednagar College Maharastra India were asked to imagine that each of 24 complex?tone melodicintervals was the “sound?name” of a person in some distant village. They were then given 36 bipolar adjective pairs and asked to rate the personality of the parson they imagined on five?point scales. (Previous studies have shown that subjects make affective judgments about sounds far more easily when imagining personalities than when rating the sounds themselves.) Results indicate that Indian students associate the main intervals used in Western music with separable personalities and that these personalities compare well with those Western listeners reported in a previous study. [Work supported by the American Institute of Indian Studies.

Scott Makeig

1986-01-01T23:59:59.000Z

87

Observation of charge-dependent azimuthal correlations and possible local strong parity violation in heavy-ion collisions  

SciTech Connect

Parity-odd domains, corresponding to non-trivial topological solutions of the QCD vacuum, might be created during relativistic heavy-ion collisions. These domains are predicted to lead to charge separation of quarks along the orbital momentum of the system created in non-central collisions. To study this effect, we investigate a three particle mixed harmonics azimuthal correlator which is a {Rho}-even observable, but directly sensitive to the charge separation effect. We report measurements of this observable using the STAR detector in Au+Au and Cu+Cu collisions at {radical}s{sub NN} = 200 and 62 GeV. The results are presented as a function of collision centrality, particle separation in rapidity, and particle transverse momentum. A signal consistent with several of the theoretical expectations is detected in all four data sets. We compare our results to the predictions of existing event generators, and discuss in detail possible contributions from other effects that are not related to parity violation.

STAR Collaboration; Abelev, Betty

2010-07-05T23:59:59.000Z

88

Measurement of long-range pseudorapidity correlations and azimuthal harmonics in sNN=5.02 TeV proton-lead collisions with the ATLAS detector  

Science Journals Connector (OSTI)

Measurements of two-particle correlation functions and the first five azimuthal harmonics, v1 to v5, are presented, using 28 nb?1 of p+Pb collisions at a nucleon-nucleon center-of-mass energy of sNN=5.02 TeV measured with the ATLAS detector at the LHC. Significant long-range “ridgelike” correlations are observed for pairs with small relative azimuthal angle (|??|2?/3) over the transverse momentum range 0.44 GeV. The v2(pT), v3(pT), and v4(pT) are compared to the vn coefficients in Pb+Pb collisions at sNN=2.76 TeV with similar event multiplicities. Reasonable agreement is observed after accounting for the difference in the average pT of particles produced in the two collision systems.

G. Aad et al. (ATLAS Collaboration)

2014-10-09T23:59:59.000Z

89

Measurement of azimuthal correlations between forward and central jets in proton proton collisions at sqrt(s)=7 TeV  

E-Print Network (OSTI)

The azimuthal correlation between forward and central jets has been measured in proton--proton collisions at the LHC, at the centre-of-mass energy of 7~TeV. The forward jet is reconstructed in the hadronic forward calorimeter, within the pseudorapidity 3.2 $$ 35~GeV. The measurement of the azimuthal angle between the jets is performed for different separations in pseudorapidity, with the largest separation being $\\Delta\\eta$~=~7.5 units. The analysis is carried out for inclusive dijet events and for two subsamples, one where an additional jet is required between the forward and the central jet, and one where the additional jet is vetoed. Comparisons between data and several different Monte Carlo models and tunes show a large sensitivity to the modeling of QCD radiation.

CMS Collaboration

2014-01-01T23:59:59.000Z

90

Computing electricity spot price prediction intervals using quantile regression and forecast averaging  

Science Journals Connector (OSTI)

We examine possible accuracy gains from forecast averaging in the context of interval forecasts of electricity spot prices. First, we test whether constructing empirical prediction intervals (PI) from combined electricity

Jakub Nowotarski; Rafa? Weron

2014-08-01T23:59:59.000Z

91

Centrality dependence of dihadron correlations and azimuthal anisotropy harmonics in PbPb collisions at $\\sqrt{s_{NN}}= 2.76\\ \\mbox{TeV}$  

SciTech Connect

Measurements from the CMS experiment at the LHC of dihadron correlations for charged particles produced in PbPb collisions at a nucleon-nucleon centre-of-mass energy of 2.76 TeV are presented. The results are reported as a function of the particle transverse momenta (pt) and collision centrality over a broad range in relative pseudorapidity [Delta(eta)] and the full range of relative azimuthal angle [Delta(phi)]. The observed two-dimensional correlation structure in Delta(eta) and Delta(phi) is characterised by a narrow peak at (Delta(eta), Delta(phi)) approximately (0, 0) from jet-like correlations and a long-range structure that persists up to at least |Delta(eta)| = 4. An enhancement of the magnitude of the short-range jet peak is observed with increasing centrality, especially for particles of pt around 1-2 GeV/c. The long-range azimuthal dihadron correlations are extensively studied using a Fourier decomposition analysis. The extracted Fourier coefficients are found to factorise into a product of single-particle azimuthal anisotropies up to pt approximately 3-3.5 GeV/c for at least one particle from each pair, except for the second-order harmonics in the most central PbPb events. Various orders of the single-particle azimuthal anisotropy harmonics are extracted for associated particle pt of 1-3 GeV/c, as a function of the trigger particle pt up to 20 GeV/c and over the full centrality range.

Chatrchyan, Serguei; et al.

2012-05-01T23:59:59.000Z

92

Azimuthal anisotropies of reconstructed jets in Pb+Pb collisions at $\\sqrt{s_{_{\\rm NN}}}$ = 2.76 TeV in a multiphase transport model  

E-Print Network (OSTI)

Azimuthal anisotropies of reconstructed jets [$v_{n}^{jet} (n=2, 3)$] have been investigated in Pb+Pb collisions at the center of mass energy $\\sqrt{s_{_{\\rm NN}}}$ = 2.76 TeV within a framework of a multiphase transport (AMPT) model. The $v_{2}^{jet}$ is in good agreement with the recent ATLAS data. However, the $v_{3}^{jet}$ shows a smaller magnitude than $v_{2}^{jet}$, and approaches zero at a larger transverse momentum. It is attributed to the path-length dependence in which the jet energy loss fraction depends on the azimuthal angles with respect to different orders of event planes. The ratio $v_{n}^{jet}/\\varepsilon_{n}$ increases from peripheral to noncentral collisions, and $v_{n}^{jet}$ increases with the initial spatial asymmetry ($\\varepsilon_{n}$) for a given centrality bin. These behaviors indicate that the $v_{n}^{jet}$ is produced by the strong interactions between jet and the partonic medium with different initial geometry shapes. Therefore, azimuthal anisotropies of reconstructed jet are proposed as a good probe to study the initial spatial fluctuations, which are expected to provide constraints on the path-length dependence of jet quenching models.

Mao-Wu Nie; Guo-Liang Ma

2014-07-28T23:59:59.000Z

93

Azimuthal reflectivity inversion  

E-Print Network (OSTI)

derivation assumes an isotropic half-space over an anisotropic half-space. This assumption is ..... D., 2010, Principle stress estimation in shale plays using 3D.

mshepher

2012-10-30T23:59:59.000Z

94

Extending Sensor Calibration Intervals in Nuclear Power Plants  

SciTech Connect

Currently in the USA, sensor recalibration is required at every refueling outage, and it has emerged as a critical path item for shortening outage duration. International application of calibration monitoring, such as at the Sizewell B plant in UK, has shown that sensors may operate for eight years, or longer, within calibration tolerances. Online monitoring can be employed to identify those sensors which require calibration, allowing for calibration of only those sensors which need it. The US NRC accepted the general concept of online monitoring for sensor calibration monitoring in 2000, but no plants have been granted the necessary license amendment to apply it. This project addresses key issues in advanced recalibration methodologies and provides the science base to enable adoption of best practices for applying online monitoring, resulting in a public domain standardized methodology for sensor calibration interval extension. Research to develop this methodology will focus on three key areas: (1) quantification of uncertainty in modeling techniques used for calibration monitoring, with a particular focus on non-redundant sensor models; (2) accurate determination of acceptance criteria and quantification of the effect of acceptance criteria variability on system performance; and (3) the use of virtual sensor estimates to replace identified faulty sensors to extend operation to the next convenient maintenance opportunity.

Coble, Jamie B.; Meyer, Ryan M.; Ramuhalli, Pradeep; Bond, Leonard J.; Shumaker, Brent; Hashemian, Hash

2012-11-15T23:59:59.000Z

95

Computer-controlled time-interval generator for pulse EPR relaxometer  

SciTech Connect

This paper describes a time-interval generator with eleven output channels; the generator is controlled by an Elektronika D3-28 computer. High flexibility in the shaping of various pulse combinations allows automatic control of the EPR relaxometer under all research conditions. A maximum of 16 intervals can be generated in each channel. The interval range is 1 usec to 4 X 10/sup 3/ sec. The generator can also be used to control other pulse instruments for physics experiments.

Safonov, S.D.; Dudkov, V.N.; Ivanov, V.G.; Muromtsev, V.I.; Nyrtsov, I.V.; Sukharev, V.N.

1986-06-01T23:59:59.000Z

96

E-Print Network 3.0 - aware interval caching Sample Search Results  

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search results for: aware interval caching Page: << < 1 2 3 4 5 > >> 1 Technical Report No. 11980001 University of Rhode Island Summary: Engineering Kingston, RI 02881, USA...

97

Multiplicative scale uncertainties in the unified approach for constructing confidence intervals  

E-Print Network (OSTI)

We have investigated how uncertainties in the estimation of the detection efficiency affect the 90% confidence intervals in the unified approach for constructing confidence intervals. The study has been conducted for experiments where the number of detected events is large and can be described by a Gaussian probability density function. We also assume the detection efficiency has a Gaussian probability density and study the range of the relative uncertainties $\\sigma_\\epsilon$ between 0 and 30%. We find that the confidence intervals provide proper coverage over a wide signal range and increase smoothly and continuously from the intervals that ignore scale uncertainties with a quadratic dependence on $\\sigma_\\epsilon$.

E. S. Smith

2009-03-31T23:59:59.000Z

98

Measurement of higher-order harmonic azimuthal anisotropy in PbPb collisions at sqrt{s_{NN}} = 2.76 TeV  

SciTech Connect

Measurements are presented by the CMS Collaboration at the Large Hadron Collider (LHC) of the higher-order harmonic coefficients that describe the azimuthal anisotropy of charged particles emitted in sqrt(s[NN]) = 2.76 TeV PbPb collisions. Expressed in terms of the Fourier components of the azimuthal distribution, the n = 3-6 harmonic coefficients are presented for charged particles as a function of their transverse momentum (0.3 < pt < 8.0 GeV), collision centrality (0-70%), and pseudorapidity (abs(eta) < 2.0). The data are analyzed using the event plane, multiparticle cumulant, and Lee-Yang zeros methods, which provide different sensitivities to initial-state fluctuations. Taken together with earlier LHC measurements of elliptic flow (n = 2), the results on higher-order harmonic coefficients develop a more complete picture of the collective motion in high-energy heavy-ion collisions and shed light on the properties of the produced medium.

Chatrchyan, Serguei; et al.,

2014-04-01T23:59:59.000Z

99

OPTIMAL EXTERNAL MEMORY INTERVAL MANAGEMENT # LARS ARGE + AND JEFFREY SCOTT VITTER #  

E-Print Network (OSTI)

e#cient external data structures. Key words. interval management, stabbing queries, I/O e/O) transmits one page of B elements. We measure the e#ciency of an algorithm in terms of the number of IOPTIMAL EXTERNAL MEMORY INTERVAL MANAGEMENT # LARS ARGE + AND JEFFREY SCOTT VITTER # SIAM J. COMPUT

Arge, Lars

100

Interval type-2 fuzzy PID load frequency controller using Big Bang-Big Crunch optimization  

Science Journals Connector (OSTI)

This paper proposes an optimization based design methodology of interval type-2 fuzzy PID (IT2FPID) controllers for the load frequency control (LFC) problem. Hitherto, numerous fuzzy logic control structures are proposed as a solution of LFC. However, ... Keywords: Big Bang-Big Crunch optimization, Interval type-2 fuzzy PID controllers, Load frequency control

Engin Yesil

2014-02-01T23:59:59.000Z

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101

Curvewise DET confidence regions and pointwise EER confidence intervals using radial  

E-Print Network (OSTI)

Curvewise DET confidence regions and pointwise EER confidence intervals using radial sweep methodology to create pointwise confidence intervals for the equal error rate (EER). The EER is the rate methods to to estimate the variability in both the DET and the EER. Our radial sweep is based

Adler, Andy

102

Curvewise DET confidence regions and pointwise EER confidence intervals using radial  

E-Print Network (OSTI)

Curvewise DET confidence regions and pointwise EER confidence intervals using radial sweep methodology to create pointwise confidence intervals for the equal error rate (EER). The EER is the rate or bootstrap methods to estimate the variability in both the DET and the EER. Our radial sweep is based

Schuckers, Michael E.

103

Interval Methods for Sensitivity-Based Model-Predictive Control of  

E-Print Network (OSTI)

Interval Methods for Sensitivity-Based Model-Predictive Control of Solid Oxide Fuel Cell Systems and experiment for the thermal subprocess of a high-temperature solid oxide fuel cell system. Keywords: Interval analysis, model-predictive control, sensitivity analysis, tracking control, solid oxide fuel cells AMS

Kearfott, R. Baker

104

Holt’s exponential smoothing and neural network models for forecasting interval-valued time series  

Science Journals Connector (OSTI)

Interval-valued time series are interval-valued data that are collected in a chronological sequence over time. This paper introduces three approaches to forecasting interval-valued time series. The first two approaches are based on multilayer perceptron (MLP) neural networks and Holt’s exponential smoothing methods, respectively. In Holt’s method for interval-valued time series, the smoothing parameters are estimated by using techniques for non-linear optimization problems with bound constraints. The third approach is based on a hybrid methodology that combines the MLP and Holt models. The practicality of the methods is demonstrated through simulation studies and applications using real interval-valued stock market time series.

André Luis Santiago Maia; Francisco de A.T. de Carvalho

2011-01-01T23:59:59.000Z

105

?-Dominance relation and rough sets in interval-valued information systems  

Science Journals Connector (OSTI)

Abstract Though rough set has been widely used to study systems characterized by insufficient and incomplete information, its performance in dealing with initial interval-valued data needs to be seriously considered for improving the suitability and scalability. The aim of this paper is to present a parameterized dominance-based rough set approach to interval-valued information systems. First, by considering the degree that an interval-valued data is dominating another one, we propose the concept of ?-dominance relation. Second, we present the ?-dominance based rough set model in interval-valued decision systems. Finally, we introduce lower and upper approximate reducts into ?-dominance based rough set for simplifying decision rules, we also present the judgement theorems and discernibility functions, which describe how lower and upper approximate reducts can be calculated. This study suggests potential application areas and new research trends concerning rough set approach to interval-valued information systems.

Xibei Yang; Yong Qi; Dong-Jun Yu; Hualong Yu; Jingyu Yang

2015-01-01T23:59:59.000Z

106

Simulations of reflected sun beam traces over a target plane for an azimuth–elevation tracking heliostat with fixed geometric error sources  

Science Journals Connector (OSTI)

Abstract For a heliostat with geometric errors, the reflected central solar ray from the mirror surface center forms a curved error trace on the target plane during the day rather than staying fixed on one target point. A general azimuth–elevation tracking angle formula has been developed for a heliostat with a mirror-pivot offset and other typical geometric errors. This tracking angle formula is re-rewritten here as a series of easily solved expressions. This azimuth–elevation tracking angle formula is then used in a new complete geometric model of the sun-beam tracking errors for an azimuth–elevation tracking heliostat to simulate the sun beam tracking error trace on the target plane for a heliostat with fixed geometric errors. Here, the analysis is for a point sun and a point heliostat (or the heliostat considered as a small optical flat). The mirror surface center is defined as the orthogonal projection of the heliostat pivot on the mirror surface plane. The reflected sun-beam centre in the target plane is defined as the intersection of the mirror-surface-centre reflected central solar ray with the target plane. Due to a position tracking error in the target plane depending on the position and the orientation of the specific target plane, the position tracking error is further converted to the angular tracking error in the reflection direction to facilitate evaluation of the heliostat tracking performance. Simulations for the artificial #78 heliostat in the Beijing solar tower system on June 21st are shown to illustrate this heliostat tracking error model. This heliostat tracking error model can be used to reveal the effect of various geometrical errors in pedestal tilt etc. on the location of the beam at the target, and thus is useful in setting limits on the various geometrical errors. Essentially this paper allows one to estimate the offset of the reflected solar beam centre due to specific geometrical tracking errors, once the beam centre is computed by some other means. It also allows one to determine a limit on each error or set of errors which are allowable for a given purpose.

Minghuan Guo; Zhifeng Wang; Feihu Sun

2013-01-01T23:59:59.000Z

107

Particle-type dependence of azimuthal anisotropy and nuclearmodification of particle production in Au+Au collisions at sNN = 200GeV  

SciTech Connect

We present STAR measurements of the azimuthal anisotropy parameter v{sub 2} and the binary-collision scaled centrality ratio R{sub CP} for kaons and lambdas ({Lambda} + {bar {Lambda}}) at mid-rapidity in Au+Au collisions at {radical}s{sub NN} = 200 GeV. In combination, the v{sub 2} and R{sub CP} particle-type dependencies contradict expectations from partonic energy loss followed by standard fragmentation in vacuum. We establish p{sub T} {approx} 5 GeV/c as the value where the centrality dependent baryon enhancement ends. The K{sub S}{sup 0} and {Lambda} + {bar {Lambda}} v{sub 2} values are consistent with expectations of constituent-quark-number scaling from models of hadron formation by parton coalescence or recombination.

Adams, J.; Adler, C.; Aggarwal, M.M.; Ahammed, Z.; Amonett, J.; Anderson, B.D.; Anderson, M.; Arkhipkin, D.; Averichev, G.S.; Badyal,S.K.; Balewski, J.; Barannikova, O.; Barnby, L.S.; Baudot, J.; Bekele,S.; Belaga, V.V.; Bellwied, R.; Berger, J.; Bezverkhny, B.I.; Bhardwaj,S.; Bhaskar, P.; Bhati, A.K.; Billmeier, A.; Bland, L.C.; Blyth, C.O.; Bonner, B.E.; Botje, M.; Boucham, A.; Brandin, A.; Bravar, A.; Cadman,R.V.; Cai, X.Z.; Caines, H.; Calderon de la Barca Sanchez, M.; Carroll,J.; Castillo, J.; Castro, M.; Cebra, D.; Chaloupka, P.; Chattopadhyay,S.; Chen, H.F.; Chen, Y.; Chernenko, S.P.; Cherney, M.; Chikanian, A.; Choi, B.; Christie, W.; Coffin, J.P.; Cormier, T.M.; Cramer, J.G.; Crawford, H.J.; Das, D.; Das, S.; Derevschikov, A.A.; Didenko, L.; Dietel, T.; Dong, W.J.; Dong, X.; Draper, J.E.; Du, F.; Dubey, A.K.; Dunin, V.B.; Dunlop, J.C.; Dutta Majumdar, M.R.; Eckardt, V.; Efimov,L.G.; Emelianov, V.; Engelage, J.; Eppley, G.; Erazmus, B.; Fachini, P.; Faine, V.; Faivre, J.; Fatemi, R.; Filimonov, K.; Filip, P.; Finch, E.; Fisyak, Y.; Flierl, D.; Foley, K.J.; Fu, J.; Gagliardi, C.A.; Gagunashvili, N.; Gans, J.; Ganti, M.S.; Gutierrez, T.D.; Gaudichet, L.; Germain, M.; Geurts, F.; Ghazikhanian, V.; Ghosh, P.; Gonzalez, J.E.; Grachov, O.; Grigoriev, V.; Gronstal, S.; Drosnick, D.; Guedon, M.; Guertin, S.M.; Gushin, E.; Hallman, T.J.; Hardtke, D.; Harris, J.W.; Heinz, M.; Henry, T.W.; Heppelmann, S.; Herston, T.; Hippolyte, B.; Hirsch, A.; Hjort, E.; Hoffmann, G.W.; Horsley, M.; Huang, H.Z.; Huang,S.L.; Humanic, T.J.; Igo, G.; Ishihara, A.; Jacobs, P.; Jacobs, W.W.; Janik, M.; Johnson, I.; Jones, P.G.; Judd, E.G.; Kabana, S.; Kaneta, M.; Kaplan, M.; Keane, D.; Kiryluk, J.; Kisiel, A.; Klay, J.; Klein, S.R.; Klyachko, A.; Koetke, D.D.; Kollegger, T.; Konstantinov, A.; Kopytine,S.M.; Kotchenda, L.; Kovalenko, A.D.; Kramer, M.; Kravtsov, P.; Krueger,K.; Kuhn, C.; Kulikov, A.I.; Kunde, G.J.; Kunz, C.L.; Kutuev, R.K.; et al.

2003-06-18T23:59:59.000Z

108

Multiplicity dependence of azimuthal distributions for [sup 36]Ar+[sup 197]Au collisions at [ital E]/[ital A]=35 MeV  

SciTech Connect

Collisions between [sup 36]Ar projectile and [sup 197]Au target nuclei at [ital E]/[ital A]=35 MeV have been studied with the Michigan State University Miniball, a 4[pi] phoswich array with a low detection threshold. Azimuthal distributions of charged particles with respect to the reaction plane are determined via the transverse-momentum-tensor method. Dependence on the kinetic energy of the emitted particles, the collision geometry, and the associated charged particle multiplicity is investigated. Corrections for the intrinsic resolution of the experimental reaction plane determination are applied. Scaling implied by the coalescence model is explored and the data are compared to the results of microscopic calculations within the Boltzmann-Uehling-Uhlenbeck theory.

Tsang, M.B.; Bowman, D.R.; Carlin, N.; Danielewicz, P.; Gelbke, C.K.; Gong, W.G.; Kim, Y.D.; Lynch, W.G.; Phair, L.; de Souza, R.T.; Zhu, F. (National Superconducting Cyclotron Laboratory and Department of Physics Astronomy, Michigan State University, East Lansing, Michigan 48824 (United States))

1993-06-01T23:59:59.000Z

109

Measurement of the Azimuthal Correlation between the most Forward Jet and the Scattered Positron in Deep-Inelastic Scattering at HERA  

E-Print Network (OSTI)

Deep-inelastic positron-proton scattering events at low photon virtuality Q^2 with a forward jet, produced at small angles with respect to the proton beam, are measured with the H1 detector at HERA. A subsample of events with an additional jet in the central region is also studied. For both samples differential cross sections and normalised distributions are measured as a function of the azimuthal angle difference, Delta phi, between the forward jet and the scattered positron. The sensitivity to QCD evolution mechanisms is tested by comparing the data to predictions of Monte Carlo generators based on different evolution approaches as well as to next-to-leading order calculations.

Aaron, F D; Andreev, V; Backovic, S; Baghdasaryan, A; Baghdasaryan, S; Barrelet, E; Bartel, W; Begzsuren, K; Belousov, A; Belov, P; Bizot, J C; Boudry, V; Bozovic-Jelisavcic, I; Bracinik, J; Brandt, G; Brinkmann, M; Brisson, V; Britzger, D; Bruncko, D; Bunyatyan, A; Bystritskaya, L; Campbell, A J; Cantun Avila, K B; Ceccopieri, F; Cerny, K; Cerny, V; Chekelian, V; Contreras, J G; Coughlan, J A; Cvach, J; Dainton, J B; Daum, K; Delcourt, B; Delvax, J; De Wolf, E A; Diaconu, C; Dobre, M; Dodonov, V; Dossanov, A; Dubak, A; Eckerlin, G; Egli, S; Eliseev, A; Elsen, E; Favart, L; Fedotov, A; Felst, R; Feltesse, J; Ferencei, J; Fischer, D J; Fleischer, M; Fomenko, A; Gabathuler, E; Gayler, J; Ghazaryan, S; Glazov, A; Goerlich, L; Gogitidze, N; Gouzevitch, M; Grab, C; Grebenyuk, A; Greenshaw, T; Grell, B R; Grindhammer, G; Habib, S; Haidt, D; Helebrant, C; Henderson, R C W; Hennekemper, E; Henschel, H; Herbst, M; Herrera, G; Hildebrandt, M; Hiller, K H; Hoffmann, D; Horisberger, R; Hreus, T; Huber, F; Jacquet, M; Janssen, X; Jonsson, L; Jung, H; Kapichine, M; Kenyon, I R; Kiesling, C; Klein, M; Kleinwort, C; Kluge, T; Kogler, R; Kostka, P; Kraemer, M; Kretzschmar, J; Kruger, K; Landon, M P J; Lange, W; Lastovicka-Medin, G; Laycock, P; Lebedev, A; Lendermann, V; Levonian, S; Lipka, K; List, B; List, J; Lopez-Fernandez, R; Lubimov, V; Makankine, A; Malinovski, E; Marage, P; Martyn, H U; Maxfield, S J; Mehta, A; Meyer, A B; Meyer, H; Meyer, J; Mikocki, S; Milcewicz-Mika, I; Moreau, F; Morozov, A; Morris, J V; Mudrinic, M; Muller, K; Naumann, Th; Newman, P R; Niebuhr, C; Nikitin, D; Nowak, G; Nowak, K; Olsson, J E; Ozerov, D; Pahl, P; Palichik, V; Panagoulias, I; Pandurovic, M; Papadopoulou, Th; Pascaud, C; Patel, G D; Perez, E; Petrukhin, A; Picuric, I; Piec, S; Pirumov, H; Pitzl, D; Placakyte, R; Pokorny, B; Polifka, R; Povh, B; Radescu, V; Raicevic, N; Ravdandorj, T; Reimer, P; Rizvi, E; Robmann, P; Roosen, R; Rostovtsev, A; Rotaru, M; Ruiz Tabasco, J E; Rusakov, S; Salek, D; Sankey, D P C; Sauter, M; Sauvan, E; Schmitt, S; Schoeffel, L; Schoning, A; Schultz-Coulon, H C; Sefkow, F; Shtarkov, L N; Shushkevich, S; Sloan, T; Smiljanic, I; Soloviev, Y; Sopicki, P; South, D; Spaskov, V; Specka, A; Staykova, Z; Steder, M; Stella, B; Stoicea, G; Straumann, U; Sykora, T; Thompson, P D; Tran, T H; Traynor, D; Truol, P; Tsakov, I; Tseepeldorj, B; Turnau, J; Valkarova, A; Vallee, C; Van Mechelen, P; Vazdik, Y; Wegener, D; Wunsch, E; Zacek, J; Zalesak, J; Zhang, Z; Zhokin, A; Zohrabyan, H; Zomer, F

2012-01-01T23:59:59.000Z

110

Extension of multivariate regression trees to interval data. Application to electricity load profiling  

Science Journals Connector (OSTI)

Several data can be presented as interval curves where ... particular, this representation is well adapted for load profiles, which depict the electricity consumption of a class of customers. Electricity load pro...

Véronique Cariou

2006-01-01T23:59:59.000Z

111

Relationship between cutoff frequency and accuracy in time-interval photon statistics applied to oscillating signals  

Science Journals Connector (OSTI)

In this paper the accuracy in the determination of the period of an oscillating signal, when obtained from the photon statistics time-interval probability, is studied as a function of...

Rebolledo, M A; Martinez-Betorz, J A

1989-01-01T23:59:59.000Z

112

No O(N) queries for checking if N intervals cover everything or for piercing N pairs of intervals. An O(N log N)-steps algorithm for piercing  

E-Print Network (OSTI)

The complexity of two related geometrical (indeed, combinatorial) problems is considered, measured by the number of queries needed to determine the solution. It is proved that one cannot check in a linear in N number of queries whether N intervals cover a whole interval, or whether for N pairs of intervals on two lines there is a pair of points intersecting each of these pairs of intervals ("piercing all pairs of intervals"). The proofs are related to examples which show that there is no "Helly property" here - the whole set of N may cover the whole interval (resp. may have no pair of points piercing all pairs of intervals) while any proper subset does not. Also, for the piercing problem we outline an algorithm, taking O(N log N) steps, to check whether there is a pair of points piercing all pairs of intervals and if there is, to find it.

Katchalski, Meir

2011-01-01T23:59:59.000Z

113

Interval analysis applied to the maximum loading point of electric power systems considering load data uncertainties  

Science Journals Connector (OSTI)

Abstract This paper proposes a simple and efficient power flow method to calculate, in an interval manner, the main variables corresponding to the maximum loading point, under load data uncertainties. The resulting interval nonlinear system of equations is solved using Krawczyk method. The proposed methodology is implemented in the Matlab environment using the Intlab toolbox. Results are compared with those obtainable by Monte Carlo simulations. IEEE 30 bus system and a South-southeastern Brazilian network are used to validate the proposed methodology.

L.E.S. Pereira; V.M. da Costa

2014-01-01T23:59:59.000Z

114

Confidence intervals for state probabilities of system capacity outages and for LOLP  

E-Print Network (OSTI)

CONFID"NC. , INTERVALS FO- S'TATE PROBABILITIES OF SYSTEM CAPACITY OUTAGES AND FOR LOLP A Thcsi. , bv ATHANASIOS STASINOS Submi. tted to the Graduate College of Texas A&M University in partial fulfillment of the requirement for the degree... of MASTER OF SCIENCE December 1974 Major Subject: Electrical Engineering CONFIDENCE INTERVALS FOR STA1'E PROBABILITIES OF STSTEM CAPACITY OVTAGES AND FOR LOLP A Thesis by ATHANASIOS STASINOS Approved as to style and content by: (Chairman...

Stasinos, Athanasios

1974-01-01T23:59:59.000Z

115

Time interval and lattice vibration in Raman effect, photoelectric effect and plane mirror reflection  

E-Print Network (OSTI)

Time interval between the incident and scattered photon in Raman effect and absorption of photon and emission of electron in photoelectric effect has not been determined till now. This is because there is no such high level instrument discovered till now to detect time interval to such a small level. But this can be calculated theoretically by applying a basic principle of physics like impulse is equal to the change in momentum. Considering the collision between electron and photon as perfect inelastic collision in photoelectric effect, elastic and inelastic collision in Raman effect and elastic collision in plane mirror reflection and the interaction between electron and photon as strong gravitational interaction we calculate the required time interval. During these phenomena there is lattice vibration which can be quantized as phonon particles.

M. Kumar; S. Sahoo

2012-07-02T23:59:59.000Z

116

Identified particle production, azimuthal anisotropy, and interferometry measurements in Au+Au collisions at sqrt sNN = 9.2 GeV  

SciTech Connect

We present the first measurements of identified hadron production, azimuthal anisotropy, and pion interferometry from Au+Au collisions below the nominal injection energy at the Relativistic Heavy-Ion Collider (RHIC) facility. The data were collected using the large acceptance STAR detector at {radical}s{sub NN} = 9.2 GeV from a test run of the collider in the year 2008. Midrapidity results on multiplicity density (dN/dy) in rapidity (y), average transverse momentum (), particle ratios, elliptic flow, and HBT radii are consistent with the corresponding results at similar {radical}s{sub NN} from fixed target experiments. Directed flow measurements are presented for both midrapidity and forward rapidity regions. Furthermore the collision centrality dependence of identified particle dN/dy, , and particle ratios are discussed. These results also demonstrate that the capabilities of the STAR detector, although optimized for {radical}s{sub NN} = 200 GeV, are suitable for the proposed QCD critical point search and exploration of the QCD phase diagram at RHIC.

STAR Collaboration; Abelev, Betty

2010-07-05T23:59:59.000Z

117

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...

Adare, A; Aidala, C; Ajitanand, N N; Akiba, Y; Al-Bataineh, H; Al-Jamel, A; Alexander, J; Aoki, K; Aphecetche, L; Armendariz, R; Aronson, S H; Asai, J; Atomssa, E T; Averbeck, R; Awes, T C; Azmoun, B; Babintsev, V; Baksay, G; Baksay, L; Baldisseri, A; Barish, K N; Barnes, P D; Bassalleck, B; Bathe, S; Batsouli, S; Baublis, V; Bauer, F; Bazilevsky, A; Belikov, S; Bennett, R; Berdnikov, Y; Bickley, A A; Bjorndal, M T; Boissevain, J G; Borel, H; Boyle, K; Brooks, M L; Brown, D S; Bucher, D; Buesching, H; Bumazhnov, V; Bunce, G; Burward-Hoy, J M; Butsyk, S; Campbell, S; Chai, J -S; Chang, B S; Charvet, J -L; Chernichenko, S; Chi, C Y; Chiba, J; Chiu, M; Choi, I J; Chujo, T; Chung, P; Churyn, A; Cianciolo, V; Cleven, C R; Cobigo, Y; Cole, B A; Comets, M P; Constantin, P; Csanád, M; Csörg?, T; Dahms, T; Das, K; David, G; Deaton, M B; Dehmelt, K; Delagrange, H; Denisov, A; d'Enterria, D; Deshpande, A; Desmond, E J; Dietzsch, O; Dion, A; Donadelli, M; Drachenberg, J L; Drapier, O; Drees, A; Dubey, A K; Durum, A; Dzhordzhadze, V; Efremenko, Y V; Egdemir, J; Ellinghaus, F; Emam, W S; Enokizono, A; En'yo, H; Espagnon, B; Esumi, S; Eyser, K O; Fields, D E; Finger, M; Finger, M; Jr., \\,; Fleuret, F; Fokin, S L; Forestier, B; Fraenkel, Z; Frantz, J E; Franz, A; Frawley, A D; Fujiwara, K; Fukao, Y; Fung, S -Y; Fusayasu, T; Gadrat, S; Garishvili, I; Gastineau, F; Germain, M; Glenn, A; Gong, H; Gonin, M; Gosset, J; Goto, Y; de Cassagnac, R Granier; Grau, N; Greene, S V; Perdekamp, M Grosse; Gunji, T; Gustafsson, H -Å; Hachiya, T; Henni, A Hadj; Haegemann, C; Haggerty, J S; Hagiwara, M N; Hamagaki, H; Han, R; Harada, H; Hartouni, E P; Haruna, K; Harvey, M; Haslum, E; Hasuko, K; Hayano, R; He, X; Heffner, M; Hemmick, T K; Hester, T; Heuser, J M; Hiejima, H; Hill, J C; Hobbs, R; Hohlmann, M; Holmes, M; Holzmann, W; Homma, K; Hong, B; Horaguchi, T; Hornback, D; Huang, S; Hur, M G; Ichihara, T; Iinuma, H; Imai, K; Inaba, M; Inoue, Y; Isenhower, D; Isenhower, L; Ishihara, M; Isobe, T; Issah, M; Isupov, A; Jacak, B V; Jia, J; Jin, J; Jinnouchi, O; Johnson, B M; Joo, K S; Jouan, D; Kajihara, F; Kametani, S; Kamihara, N; Kamin, J; Kaneta, M; Kang, J H; Kanou, H; Kawagishi, T; Kawall, D; Kazantsev, A V; Kelly, S; Khanzadeev, A; Kikuchi, J; Kim, D H; Kim, D J; Kim, E; Kim, Y -S; Kinney, E; Kiss, Á; Kistenev, E; Kiyomichi, A; Klay, J; Klein-Boesing, C; Kochenda, L; Kochetkov, V; Komkov, B; Konno, M; Kotchetkov, D; Kozlov, A; Král, A; Kravitz, A; Kroon, P J; Kubart, J; Kunde, G J; Kurihara, N; Kurita, K; Kweon, M J; Kwon, Y; Kyle, G S; Lacey, R; Lai, Y S; Lajoie, J G; Lebedev, A; Bornec, Y Le; Leckey, S; Lee, D M; Lee, M K; Lee, T; Leitch, M J; Leite, M A L; Lenzi, B; Li, X; Li, X H; Lim, H; Liška, T; Litvinenko, A; Liu, M X; Love, B; Lynch, D; Maguire, C F; Makdisi, Y I; Malakhov, A; Malik, M D; Manko, V I; Mao, Y; Mašek, L; Masui, H; Matathias, F; McCain, M C; McCumber, M; McGaughey, P L; Miake, Y; Mikeš, P; Miki, K; Miller, T E; Milov, A; Mioduszewski, S; Mishra, G C; Mishra, M; Mitchell, J T; Mitrovski, M; Morreale, A; Morrison, D P; Moss, J M; Moukhanova, T V; Mukhopadhyay, D; Murata, J; Nagamiya, S; Nagata, Y; Nagle, J L; Naglis, M; Nakagawa, I; Nakamiya, Y; Nakamura, T; Nakano, K; Newby, J; Nguyen, M; Norman, B E; Nouicer, R; Nyanin, A S; Nystrand, J; O'Brien, E; Oda, S X; Ogilvie, C A; Ohnishi, H; Ojha, I D; Oka, M; Okada, K; Omiwade, O O; Oskarsson, A; Otterlund, I; Ouchida, M; Ozawa, K; Pak, R; Pal, D; Palounek, A P T; Pantuev, V; Papavassiliou, V; Park, J; Park, W J; Pate, S F; Pei, H; Peng, J -C; Pereira, H; Peresedov, V; Peressounko, D Yu; Pinkenburg, C; Pisani, R P; Purschke, M L; Purwar, A K; Qu, H; Rak, J; Rakotozafindrabe, A; Ravinovich, I; Read, K F; Rembeczki, S; Reuter, M; Reygers, K; Riabov, V; Riabov, Y; Roche, G; Romana, A; Rosati, M; Rosendahl, S S E; Rosnet, P; Rukoyatkin, P; Rykov, V L; Ryu, S S; Sahlmueller, B; Saito, N; Sakaguchi, T; Sakai, S; Sakata, H; Samsonov, V; Sato, H D; Sato, S; Sawada, S; Seele, J; Seidl, R; Semenov, V; Seto, R; Sharma, D; Shea, T K; Shein, I; Shevel, A; Shibata, T -A; Shigaki, K; Shimomura, M; Shohjoh, T; Shoji, K; Sickles, A; Silva, C L; Silvermyr, D; Silvestre, C; Sim, K S; Singh, C P; Singh, V; Skutnik, S; Slune?ka, M; Smith, W C; Soldatov, A; Soltz, R A; Sondheim, W E; Sorensen, S P; Sourikova, I V; Staley, F; Stankus, P W; Stenlund, E; Stepanov, M; Ster, A; Stoll, S P; Sugitate, T; Suire, C; Sullivan, J P; Sziklai, J; Tabaru, T; Takagi, S; Takagui, E M; Taketani, A; Tanaka, K H; Tanaka, Y; Tanida, K; Tannenbaum, M J; Taranenko, A; Tarján, P; Thomas, T L; Todoroki, T; Togawa, M; Toia, A; Tojo, J; Tomášek, L; Torii, H; Towell, R S; Tram, V-N; Tserruya, I; Tsuchimoto, Y; Tuli, S K; Tydesjö, H; Tyurin, N; Vale, C; Valle, H; van Hecke, H W; Velkovska, J; Vértesi, R; Vinogradov, A A; Virius, M; Vrba, V; Vznuzdaev, E; Wagner, M; Walker, D; Wang, X R; Watanabe, Y; Wessels, J

2014-01-01T23:59:59.000Z

118

Deceleration of Alpha Particles in the Solar Wind by Instabilities and the Rotational Force: Implications for Heating, Azimuthal Flow, and the Parker Spiral Magnetic Field  

E-Print Network (OSTI)

Protons and alpha particles in the fast solar wind are only weakly collisional and exhibit a number of non-equilibrium features, including relative drifts between particle species. Two non-collisional mechanisms have been proposed for limiting differential flow between alpha particles and protons: plasma instabilities and the rotational force. Both mechanisms decelerate the alpha particles. In this paper, we derive an analytic expression for the rate $Q_{\\mathrm{flow}}$ at which energy is released by alpha-particle deceleration, accounting for azimuthal flow and conservation of total momentum. We find that $Q_{\\mathrm{flow}} > 0 $ at $r r_{\\mathrm{crit}}$. We compare the value of $Q_{\\mathrm{flow}}$ at $r< r_{\\mathrm{crit}}$ with empirical heating rates for protons and alpha particles, denoted $Q_{\\mathrm{p}}$ and $Q_{\\alpha}$, deduced from in-situ measurements of fast-wind streams from the Helios and Ulysses spacecraft. We find that $Q_{\\mathrm{flow}}$ exceeds $Q_{\\alpha}$ at $r < 1\\,\\mathrm{AU}$, $Q_{...

Verscharen, Daniel; Bourouaine, Sofiane; Hollweg, Joseph V

2014-01-01T23:59:59.000Z

119

Assessment of Interval Data and Their Potential Application to Residential Electricity End-Use Modeling, An  

Reports and Publications (EIA)

The Energy Information Administration (EIA) is investigating the potential benefits of incorporating interval electricity data into its residential energy end use models. This includes interval smart meter and submeter data from utility assets and systems. It is expected that these data will play a significant role in informing residential energy efficiency policies in the future. Therefore, a long-term strategy for improving the RECS end-use models will not be complete without an investigation of the current state of affairs of submeter data, including their potential for use in the context of residential building energy modeling.

2015-01-01T23:59:59.000Z

120

Azimuthal correlations between charged hadrons and direct photons at high-p$_{t}$ in $p+p$ and $Au+Au$ collisions at $\\sqrt{s_{NN}}$ = 200 GeV  

E-Print Network (OSTI)

Recent results at STAR for direct $\\gamma$-charged hadron azimuthal correlations in heavy-ion collisions are presented. These correlations are used to study the color charge density of the medium through the medium-induced modification of high-p$_T$ parton fragmentation. Azimuthal correlations of direct photons at high transverse energy 8 $<$ E$_T$ $<$ 16 GeV with away-side charged hadrons of transverse momentum 3 $<$ p$_T$ $<$ 6 GeV/c have been measured over a broad range of centrality for $Au+Au$ collisions and $p+p$ collisions at $\\sqrt{s_{NN}}$ = 200 GeV in the STAR experiment. The per-trigger away-side yield of direct $\\gamma$ is smaller than from $\\pi^{0}$ triggers in the same centrality class.

A. M. Hamed

2008-11-11T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

Physiological responses of reining horses to interval training versus conventional training procedures  

E-Print Network (OSTI)

concentrations at stopping and post-exercise times on d 28 when compared to d 0. However it was only following interval training that this increase in aerobic capacity response was repeated on d 31. On d 31 of the conventional protocol, plasma lactate...

Haney, Elizabeth anne

1998-01-01T23:59:59.000Z

122

40 Cognitive Science class intervals that are equally spread across the data  

E-Print Network (OSTI)

40 Cognitive Science class intervals that are equally spread across the data range. For example and geographic visualization. Englewood Cliffs, NJ: PearsonJPrentice Hall. COGNITIVE SCIENCE Cognitive science. Cognition includes perception, thinking, learning, memory, reasoning and problem solving, and linguistic

Montello, Daniel R.

123

TradeO# Between Sample Size and Accuracy: Case of Static Measurements under Interval  

E-Print Network (OSTI)

Trade­O# Between Sample Size and Accuracy: Case of Static Measurements under Interval Uncertainty situations, we are not satisfied with the accuracy of the existing measurements. There are two possible ways to improve the measurement accuracy: . first, instead of a single measurement, we can make repeated

Ward, Karen

124

Trade-Off Between Sample Size and Accuracy: Case of Measurements under Interval  

E-Print Network (OSTI)

Trade-Off Between Sample Size and Accuracy: Case of Measurements under Interval Uncertainty Hung T practical situations, we are not satisfied with the accuracy of the existing measurements. There are two possible ways to improve the measurement accuracy: · first, instead of a single measurement, we can make

Kreinovich, Vladik

125

Trade-Off Between Sample Size and Accuracy: Case of Static Measurements under Interval  

E-Print Network (OSTI)

Trade-Off Between Sample Size and Accuracy: Case of Static Measurements under Interval Uncertainty situations, we are not satisfied with the accuracy of the existing measurements. There are two possible ways to improve the measurement accuracy: · first, instead of a single measurement, we can make repeated

Ward, Karen

126

Application of SAFER-PC program to determine turbine rotor boresonic inspection intervals  

SciTech Connect

Public Service Company of Colorado (PSCC) used EPRI`s SAFER-PC Program to evaluate their HP/IP, LP, and generator rotors from Cherokee Station Unit 3, to determine appropriate boresonic re-inspection intervals. The program uses fracture mechanics to calculate critical crack sizes, which could lead to catastrophic failure of the rotors. Conservative stress and fracture mechanics analyses showed negligible fatigue crack growth of assumed bore surface cracks would occur over the proposed inspection interval of eighteen years. The evaluation assumed consistent operational start-up procedures for the inspection interval. If the unit experiences more severe operational procedures, the analysis may not be applicable, with smaller critical crack sizes and accelerated crack growth rates expected. The SAFER-PC analysis resulted in an extension of the previously recommended reinspection interval by eight years. By eliminating just this one inspection, PSCC achieved savings in the range of $100,000. Further savings are anticipated by utilizing the SAFER-PC Program to evaluate these and other PSCC rotors in the future.

Sachse, D.G.; Hellner, R.L.; Dupont, E.J. [Public Service Co., Denver, CO (United States)

1996-12-31T23:59:59.000Z

127

Fire-Return Intervals in Mixed-Conifer Forests of the Kings River Sustainable  

E-Print Network (OSTI)

Fire-Return Intervals in Mixed-Conifer Forests of the Kings River Sustainable Forest Ecosystems,070-ha study area in the Dinkey Creek watershed. Stumps in mixed-conifer forest were examined for fire a similar period in mixed-conifer forests at Redwood Mountain and Bearskin Creek, 40-50 km south of Dinkey

Standiford, Richard B.

128

VARIABILITY OF SOLAR RADIATION DATA OVER SHORT TIME INTERVALS Frank Vignola  

E-Print Network (OSTI)

radiation values obtained from models utilizing satellite or cloud cover observation data with solarVARIABILITY OF SOLAR RADIATION DATA OVER SHORT TIME INTERVALS Frank Vignola Department of Physics to evaluate satellite and cloud cover models, it is useful to understand the short-term variability of solar

Oregon, University of

129

A generalized interval probability-based optimization method for training generalized hidden Markov model  

Science Journals Connector (OSTI)

Recently a generalized hidden Markov model (GHMM) was proposed for solving the information fusion problems under aleatory and epistemic uncertainties in engineering application. In GHMM, aleatory uncertainty is captured by the probability measure whereas ... Keywords: Generalized Baum-Welch algorithm, Generalized Jensen inequality, Generalized hidden Markov model, Generalized interval probability, State recognition

Fengyun Xie; Bo Wu; Youmin Hu; Yan Wang; Guangfei Jia; Yao Cheng

2014-01-01T23:59:59.000Z

130

Fast Algorithms for Computing Statistics Under Interval and Fuzzy Uncertainty, and Their Applications  

E-Print Network (OSTI)

, including applications to the seismic inverse problem in geosciences, to chip design in computer engineering of a pollutant on the fish, we check on the fish daily; if a fish was alive on Day 5 but dead on Day 6, then the only information about the lifetime of this fish is that it is somewhere within the interval [5, 6]; we

Kreinovich, Vladik

131

Fast Algorithms for Computing Statistics Under Interval and Fuzzy Uncertainty, and Their Applications  

E-Print Network (OSTI)

, including applications to the seismic inverse problem in geosciences, to chip design in computer engineering#ect of a pollutant on the fish, we check on the fish daily; if a fish was alive on Day 5 but dead on Day 6, then the only information about the lifetime of this fish is that it is somewhere within the interval [5, 6]; we

Kreinovich, Vladik

132

Comparison of Rough-set and Interval-set Models for Uncertain Reasoning  

E-Print Network (OSTI)

Comparison of Rough-set and Interval-set Models for Uncertain Reasoning Y.Y. Yao and Xining Li Department of Computer Science Lakehead University Thunder Bay, Ontario, Canada P7B 5E1 Abstract In the rough-set of their extended set-theoretic operators. The operators in the rough-set model are not truth-functional, while

Yao, Yiyu

133

Towards an interval-valued estimation of the density Bilal Nehme and Olivier Strauss  

E-Print Network (OSTI)

belonging to the considered set. I. INTRODUCTION In the last ten years, there has been an increasing-valued pdf. This paper is organized as follows: section II introduces some necessary preliminary concepts. In section III we show how to built our interval-valued estimator based on a particular kernel. Section IV

Paris-Sud XI, Université de

134

Neurocomputing 70 (2007) 26922700 Inter-spike-intervals analysis of AER Poisson-like generator hardware  

E-Print Network (OSTI)

Neurocomputing 70 (2007) 2692­2700 Inter-spike-intervals analysis of AER Poisson-like generator Sevilla, Spain Available online 10 May 2007 Abstract Address­Event­Representation (AER) is a communication). In developing AER-based systems it is very convenient to have available some means of generating AER streams

Barranco, Bernabe Linares

135

Confidence Interval Estimation for Inequality Indices of the GiniFamily  

Science Journals Connector (OSTI)

In this paper we present some nonparametric bootstrap methods to construct distribution-free confidence intervals for inequality indices belonging to the Gini family. These methods have a coverage accuracy better than that obtained with the asymptotic ... Keywords: Gini index family, Monte Carlo experiment, income distribution, nonparametric bootstrap

Paola Palmitesta; Corrado Provasi; Cosimo Spera

2000-10-01T23:59:59.000Z

136

Proper Oil Sampling Intervals and Sample Collection Techniques Gasoline/Diesel/Natural Gas Engines  

E-Print Network (OSTI)

Proper Oil Sampling Intervals and Sample Collection Techniques Gasoline/Diesel/Natural Gas Engines: · Oil samples can be collected during oil changes. Follow manufacturers recommendations on frequency (hours, mileage, etc) of oil changes. · Capture a sample from the draining oil while the oil is still hot

137

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 $0.1

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. -Å. 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

138

CP(N-1) model on finite interval in the large N limit  

E-Print Network (OSTI)

The CP(N-1) \\sigma\\ model on finite interval of length R with Dirichlet boundary conditions is analysed in the 1/N expansion. The theory has two phases, separated by a phase transition at R ~ 1/\\Lambda, \\Lambda\\ is dynamical scale of the CP(N-1) model. The vacuum energy dependence of R, and especially Casimir-type scaling 1/R, is discussed.

A. Milekhin

2012-07-02T23:59:59.000Z

139

An analysis of beef cattle weights and gains measured at varying intervals  

E-Print Network (OSTI)

May 1967 Major Subject. Animal Breeding AN ANALYSIS OF BEEF CATTLE WEIGHTS AND GAINS MEASURED AT VARYING INTERVALS A Thesis JAMES DAVID FOX Approved as to style and content hy: (Chairman Co t e) j ('. (Head of Department) embe ) (Member (N..., and inaccuracy of the scale or scale operator. The standard error (the square root of the residual variance component) of a weight measures the amount of un- accountable variation. A main objective of this study was to analyze statistically the variation...

Fox, James David

1967-01-01T23:59:59.000Z

140

Differential properties and attracting sets of a simplest skew product of interval maps  

SciTech Connect

For a skew product of interval maps with a closed set of periodic points, the dependence of the structure of its {omega}-limit sets on its differential properties is investigated. An example of a map in this class is constructed which has the maximal differentiability properties (within a certain subclass) with respect to the variable x, is C{sup 1}-smooth in the y-variable and has one-dimensional {omega}-limit sets. Theorems are proved that give necessary conditions for one-dimensional {omega}-limit sets to exist. One of them is formulated in terms of the divergence of the series consisting of the values of a function of x; this function is the C{sup 0}-norm of the deviation of the restrictions of the fibre maps to some nondegenerate closed interval from the identity on the same interval. Another theorem is formulated in terms of the properties of the partial derivative with respect to x of the fibre maps. A complete description is given of the {omega}-limit sets of certain class of C{sup 1}-smooth skew products satisfying some natural conditions. Bibliography: 33 titles.

Efremova, Lyudmila S [N. I. Lobachevski State University of Nizhni Novgorod, Nizhnii Novgorod (Russian Federation)

2010-08-12T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

Chaotic data analysis of heart R-R interval EKG data  

SciTech Connect

Cardiac beat-to-beat interval data is analyzed with a chaotic data analysis toolkit. The embedding dimension of ten data sets from healthy subjects is 7 or at most 8. Ten of the eleven pathological data sets have an embedding dimension of 9 or greater. Statistically, the first local minimum of average mutual information for healthy hearts is larger than the pathological cases. But, there is a large standard deviation for this metric that blurs the distinction between the healthy and pathological data. {copyright} {ital 1996 American Institute of Physics.}

Frison, T.W. [Randle, Inc., P.O. Box 1010, Great Falls, Virginia 22066 (United States); Peng, C.K.; Goldberger, A. [Cardiovascular Division, Harvard Medical School, Beth Israel Hospital, Boston, Massachusetts 02215 (United States); Katz, R.A.

1996-06-01T23:59:59.000Z

142

Factors affecting the relationship between calving interval of cows and weaning weights of calves  

E-Print Network (OSTI)

that all F values of the additional variables were highly inflated. GESL was then deleted from the variables considered in the stepwise procedures, since DPCN and GESL form a linear combination for CI. These stepwise proce- dures also had similar... AS THE RESPONSE VARIABLE Variable a Abbreviation Interval INA INB INC IND INE INF ING INH IN I INJ INT INU INV INW INX INY 1NZ INAA INAB INAL INAM INAN INAO INAP INAQ INAR INAS INBB INBC INBD INBE INBF INBG Previous conception...

Doren, Philip Erich

1982-01-01T23:59:59.000Z

143

File:Table for Tip Speed Intervals of Length.pdf | Open Energy Information  

Open Energy Info (EERE)

source source History View New Pages Recent Changes All Special Pages Semantic Search/Querying Get Involved Help Apps Datasets Community Login | Sign Up Search File Edit History Facebook icon Twitter icon » File:Table for Tip Speed Intervals of Length.pdf Jump to: navigation, search File File history File usage Metadata File:Table for Tip Speed Intervals of Length.pdf Size of this preview: 463 × 599 pixels. Other resolution: 464 × 600 pixels. Full resolution ‎(1,275 × 1,650 pixels, file size: 99 KB, MIME type: application/pdf) File history Click on a date/time to view the file as it appeared at that time. Date/Time Thumbnail Dimensions User Comment current 09:37, 3 January 2014 Thumbnail for version as of 09:37, 3 January 2014 1,275 × 1,650 (99 KB) Foteri (Talk | contribs) Category:Wind for Schools Portal CurriculaCategory:Wind for Schools High School Curricula

144

Application of the CSP Approach and the Interval Computation for the Optimal Sizing of a Compression Spring  

Science Journals Connector (OSTI)

In this present study a new design approach based on intervals calculation method and Constraint Satisfaction Problem technique «CSP approach» was discussed. It has been ... dynamic of design steps), since with t...

Hassen Trabelsi; Pierre-Alain Yvars…

2013-01-01T23:59:59.000Z

145

Measurement of long-range pseudorapidity correlations and azimuthal harmonics in $\\sqrt{s_{\\mathrm{NN}}}$ = 5.02 TeV proton-lead collisions with the ATLAS detector  

E-Print Network (OSTI)

Measurements of two-particle correlation functions and the first five azimuthal harmonics, $v_1$ to $v_5$, are presented, using 28 $\\mathrm{nb}^{-1}$ of $p$+Pb collisions at a nucleon-nucleon center-of-mass energy of $\\sqrt{s_{\\mathrm{NN}}}=5.02$ TeV measured with the ATLAS detector at the LHC. Significant long-range ``ridge-like'' correlations are observed for pairs with small relative azimuthal angle ($|\\Delta\\phi|2\\pi/3$) over the transverse momentum range $0.44$ GeV. The $v_2(p_{\\rm T})$, $v_3(p_{\\rm T})$ and $v_4(p_{\\rm T})$ are compared to the $v_n$ coefficients in Pb+Pb collisions at $\\sqrt{s_{\\mathrm{NN}}} =2.76$ TeV with similar event multiplicities. Reasonable agreement is observed after accounting for the difference in the average $p_{\\rm T}$ of particles produced in the two collision systems.

ATLAS Collaboration

2014-09-05T23:59:59.000Z

146

Quality characteristics of vacuum-packaged beef as affected by postmortem chill, storage temperature and storage interval  

E-Print Network (OSTI)

QUALITY CHARACTERISTICS OF VACUUM-PACKAGED BEEF AS AFFECTED BY POSTMORTEM CHILL, STORAGE TEMPERATURE AND STORAGE INTERVAL A Thesis by SAMMY DENZIL BEEBE Submitted to the Graduate College of Texas A1IM University in partial fulfillment... of the requirement for the deoree of MASTER OF SCIENCE December 1975 Major Subject: Animal Science QUALITY CHARACTERISTICS OF VACUUM-PACKAGED BEEF AS AFFECTED BY POSTMORTEM CHILL, STORAGE TEMPERATURE AND STORAGE INTERVAL A Thesis by SAMMY DENZIL BEEBE...

Beebe, Sammy Denzil

1975-01-01T23:59:59.000Z

147

ARM - Datastreams - xsacrhsrhi  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsxsacrhsrhi Datastreamsxsacrhsrhi Documentation Data Quality Plots ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : XSACRHSRHI X-Band Scanning ARM Cloud Radar (XSACR) Hemispherical Sky RHI Scans (6 horizon-to-horizon scans at 30-degree azimuth intervals) Active Dates 2011.09.14 - 2013.05.31 Measurement Categories Cloud Properties Originating Instrument X-Band Scanning ARM Cloud Radar (XSACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Altitude m altitude Altitude above ground level m altitude_agl Antenna transition indicator, 1 if between sweeps, otherwise 0 unitless antenna_transition ( time )

148

Variable interval time/temperature (VITT) defrost-control-system evaluation  

SciTech Connect

Two variable-interval-time/temperature (VITT) heat pump defrost control systems are analyzed to determine if systems manufactured by Honeywell and Ranco qualify for credit for heat pumps with demand defrost control. The operation of the systems is described. VITT controls are not demand defrost control systems but utilize demand defrost control as backup systems in most Ranco models and all Honeywell models. The evaluations and results, intended to provide DOE information in making its determinations regarding credits for the control systems are discussed. The evaluation methodology utilizes a modified version of the Heat Pump Seasonal Performance Model (HPSPM) and the important modifications are discussed in Appendix A. Appendix B contains a detailed listing and discussion of the HPSPM output. (MCW)

None

1980-08-12T23:59:59.000Z

149

Interval Between Surgery and Neoadjuvant Chemoradiation Therapy for Distal Rectal Cancer: Does Delayed Surgery Have an Impact on Outcome?  

SciTech Connect

Background: The optimal interval between neoadjuvant chemoradiation therapy (CRT) and surgery in the treatment of patients with distal rectal cancer is controversial. The purpose of this study is to evaluate whether this interval has an impact on survival. Methods and Materials: Patients who underwent surgery after CRT were retrospectively reviewed. Patients with a sustained complete clinical response (cCR) 1 year after CRT were excluded from this study. Clinical and pathologic characteristics and overall and disease-free survival were compared between patients undergoing surgery 12 weeks or less from CRT and patients undergoing surgery longer than 12 weeks from CRT completion and between patients with a surgery delay caused by a suspected cCR and those with a delay for other reasons. Results: Two hundred fifty patients underwent surgery, and 48.4% had CRT-to-surgery intervals of 12 weeks or less. There were no statistical differences in overall survival (86% vs. 81.6%) or disease-free survival rates (56.5% and 58.9%) between patients according to interval ({<=}12 vs. >12 weeks). Patients with intervals of 12 weeks or less had significantly higher rates of Stage III disease (34% vs. 20%; p = 0.009). The delay in surgery was caused by a suspected cCR in 23 patients (interval, 48 {+-} 10.3 weeks). Five-year overall and disease-free survival rates for this subset were 84.9% and 51.6%, not significantly different compared with the remaining group (84%; p = 0.96 and 57.8%; p = 0.76, respectively). Conclusions: Delay in surgery for the evaluation of tumor response after neoadjuvant CRT is safe and does not negatively affect survival. These results support the hypothesis that shorter intervals may interrupt ongoing tumor necrosis.

Habr-Gama, Angelita [Habr-Gama Research Institute, Sao Paulo, SP (Brazil)], E-mail: gamange@uol.com.br; Perez, Rodrigo Oliva; Proscurshim, Igor; Nunes dos Santos, Rafael Miyashiro [Department of Gastroenterology, University of Sao Paulo School of Medicine, Sao Paulo, SP (Brazil); Kiss, Desiderio; Gama-Rodrigues, Joaquim; Cecconello, Ivan [Habr-Gama Research Institute, Sao Paulo, SP (Brazil); Department of Gastroenterology, University of Sao Paulo School of Medicine, Sao Paulo, SP (Brazil)

2008-07-15T23:59:59.000Z

150

Depositional facies, textural characteristics, and reservoir properties of dolomites in Frobisher-Alida interval in southwest North Dakota  

SciTech Connect

The Mississippian Frobisher-Alida interval is an upward-shoaling cycle that began with open-marine sedimentation and culminated with the deposition of a widespread sabkha-salina evaporite. This cycle is the most prolific oil-producing interval in the North Dakota portion of the Williston basin. Most Frobisher-Alida production in the southern Williston basin is from dolomite reservoirs. The six major facies defined in this paper are lithologic suites that represent sediments and precipitates deposited in similar environments. 20 figures, 5 tables.

Petty, D.M.

1988-10-01T23:59:59.000Z

151

Interval Set Clustering of Web Users using Modified Kohonen Self-Organizing Maps based on the Properties of Rough Sets  

E-Print Network (OSTI)

1 Interval Set Clustering of Web Users using Modified Kohonen Self-Organizing Maps based, 121 35 Prague 2, Czech Republic Abstract Web usage mining involves application of data mining techniques to discover usage patterns from the web data. Clustering is one of the important functions in web

152

Sensitivity of diabetic retinopathy associated vision loss to screening interval in an agent-based/discrete event simulation model  

Science Journals Connector (OSTI)

Objective: To examine the effect of changes to screening interval on the incidence of vision loss in a simulated cohort of Veterans with diabetic retinopathy (DR). This simulation allows us to examine potential interventions without putting patients ... Keywords: Agent based modeling, Diabetic eye screen, Diabetic retinopathy, Discrete event simulation

T. Eugene Day, Nathan Ravi, Hong Xian, Ann Brugh

2014-04-01T23:59:59.000Z

153

Biotic dynamics and carbonate microfacies of the conspicuous Darriwilian (Middle Ordovician) `Tljsten' interval, south-central Sweden  

E-Print Network (OSTI)

) `Täljsten' interval, south-central Sweden Mats E. Eriksson a, , Anders Lindskog a , Mikael Calner of Geology, Lund University, Sölvegatan 12, SE-223 62 Lund, Sweden b School of Earth Sciences, Division Ordovician Kinnekulle Sweden Enclosed in the Darriwilian (Middle Ordovician) part of the reddish

Calner, Mikael

154

Exercise overloading in the equine: cardiorespiratory and metabolic response to a combined long, slow, distance and interval training exercise regimen  

E-Print Network (OSTI)

output, and metabolic parameters such as blood lactate concentrations as being indicative measures of fitness. Cardiorespiratory and skeletal muscle responses to endurance or aerobic training have also been studied, However, physical training...EXERCISE OVERLOADING IN THE EQUINE CARDIORESPIRATORY AND METABOLIC RESPONSE TO A COMBINED LONG& SLOW, DISTANCE AND INTERVAL TRAINING EXERCISE REGIMEN A Thesis by LEANN FRANCINE DROZD Submitted to the Office of Graduate Studies of Texas A...

Drozd, Leann Francine

1988-01-01T23:59:59.000Z

155

An interval fixed-mix stochastic programming method for greenhouse gas mitigation in energy systems under uncertainty  

Science Journals Connector (OSTI)

In this study, an interval fixed-mix stochastic programming (IFSP) model is developed for greenhouse gas (GHG) emissions reduction management under uncertainties. In the IFSP model, methods of interval-parameter programming (IPP) and fixed-mix stochastic programming (FSP) are introduced into an integer programming framework, such that the developed model can tackle uncertainties described in terms of interval values and probability distributions over a multi-stage context. Moreover, it can reflect dynamic decisions for facility-capacity expansion during the planning horizon. The developed model is applied to a case of planning GHG-emission mitigation, demonstrating that IFSP is applicable to reflecting complexities of multi-uncertainty, dynamic and interactive energy management systems, and capable of addressing the problem of GHG-emission reduction. A number of scenarios corresponding to different GHG-emission mitigation levels are examined; the results suggest that reasonable solutions have been generated. They can be used for generating plans for energy resource/electricity allocation and capacity expansion and help decision makers identify desired GHG mitigation policies under various economic costs and environmental requirements.

Y.L. Xie; Y.P. Li; G.H. Huang; Y.F. Li

2010-01-01T23:59:59.000Z

156

A study of the sensitivity of topological dynamical systems and the Fourier spectrum of chaotic interval maps  

E-Print Network (OSTI)

of lifting some topological properties from a given dynamical system (Y,S) to an- other (X,T). After studying some basic facts about topological dynamical systems, we move to the particular case of interval maps. We know that through the knowl- edge... discussion with some basic concepts of what a dynamical system is and how the dynamic is generated. Definition 2.1. A dynamical system (X,T) consists of a topological compact metric space X and a surjective, continuous map T : X ?X. The first thing we have...

Roque Sol, Marco A.

2009-06-02T23:59:59.000Z

157

Intensity and interval of recovery in strength exercise influences performance: salivary lactate and alpha amylase as biochemical markers. A pilot study  

Science Journals Connector (OSTI)

The aim of the present study was to evaluate the effects of intensity and interval of recovery on performance in the bench press exercise, and the response of salivary lactate and alpha amylase levels.

Mateus K. Vuolo; Jonathann C. Possato; Loreana S. Silveira…

2014-12-01T23:59:59.000Z

158

Nanoparticle diffusion probing of the structure of water and aqueous organic solutions near a porous surface and in its bulk in a wide temperature interval  

Science Journals Connector (OSTI)

Scattering of laser radiation by nanoparticles (latex balls and silver nanoparticles) is investigated in a wide temperature interval. It is demonstrated that water is structured near the porous surface of a solid...

V. V. Bryukhanov; I. G. Samusev; A. M. Ivanov; N. A. Myslitskaya

2009-02-01T23:59:59.000Z

159

Eliminating livelock by assigning the same priority state to each message that is inputted into a flushable routing system during N time intervals  

DOE Patents (OSTI)

Livelock-free message routing is provided in a network of interconnected nodes that is flushable in time T. An input message processor generates sequences of at least N time intervals, each of duration T. An input register provides for receiving and holding each input message, where the message is assigned a priority state p during an nth one of the N time intervals. At each of the network nodes a message processor reads the assigned priority state and awards priority to messages with priority state (p-1) during an nth time interval and to messages with priority state p during an (n+1) th time interval. The messages that are awarded priority are output on an output path toward the addressed output message processor. Thus, no message remains in the network for a time longer than T.

Faber, Vance (Los Alamos, NM)

1994-01-01T23:59:59.000Z

160

Azimuthal –p analysis in anisotropic media  

Science Journals Connector (OSTI)

......horizontal layering of a shale formation. Periodic...medium, five basic anisotropic parameters are required...using several different anisotropic models. Synthetic Examples...results of brine saturated shale samples and another...Schoenberg Helbig (1997). Anisotropic and isotropic parameters......

Samik Sil; Mrinal K. Sen

2008-11-01T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

EFFECTS OF AN ANTIDEPRESSANT DOSE OF KETAMINE ON PREFRONTAL ASPARTATE, GLUTAMINE AND GABA LEVELS IN HEALTHY SUBJECTS: ASSESSING THE POST-INFUSION INTERVAL WITH 1H-MRS  

E-Print Network (OSTI)

IN HEALTHY SUBJECTS: ASSESSING THE POST-INFUSION INTERVAL WITH 1H-MRS Milan Scheidegger1,2 , Alexander Fuchs1 at investigating the neurometabolic changes in the 3-4 hour post-infusion interval when the antidepressant effect by a continuous infusion of 0.25 mg/kg/h over 40 minutes. Single voxel 1 H MRS data were acquired from a volume

162

Horizontal velocities in the central and eastern United States from GPS surveys during the 1987-1996 interval  

SciTech Connect

The National Geodetic Survey and the Nuclear Regulatory Commission jointly organized GPS surveys in 1987, 1990, 1993, and 1996 to search for crustal deformation in the central and eastern United States (east of longitude 108{degrees}W). We have analyzed the data of these four surveys in combination with VLBI data observed during the 1979-1995 interval and GPS data for 22 additional surveys observed during the 1990-1996 interval. These latter GPS surveys served to establish accurately positioned geodetic marks in various states. Accordingly, we have computed horizontal velocities for 64 GPS sites and 12 VLBI sites relative to a reference frame for which the interior of the North American plate is considered fixed on average. None of our derived velocities exceeds 6 mm/yr in magnitude. Moreover, the derived velocity at each GPS site is statistically zero at the 95% confidence level except for the site BOLTON in central Ohio and the site BEARTOWN in southeastern Pennsylvania. However, as statistical theory would allow approximately 5% of the 64 GPS sites to fall our zero-velocity hypothesis, we are uncertain whether or not these estimated velocities for BOLTON and BEARTOWN reflect actual motion relative to the North American plate. We also computed horizontal strain rates for the cells formed by a 1{degrees} by 1{degrees} grid spanning the central and eastern United States. Corresponding shearing rates are everywhere less than 60 nanoradians/yr in magnitude, and no shearing rate differs statistically from zero at the 95% confidence level except for a grid cell near BEARTOWN whose rate is 57 {+-} 26 nanoradians/yr. Also corresponding areal dilatation rates are everywhere less than 40 nanostrain/yr in magnitude, and no dilatation rate differs statistically from zero at the 95% confidence level.

Snay, R.A.; Strange, W.E.

1997-12-01T23:59:59.000Z

163

Subsurface definition of the Allegheny Group coalbed methane prospect interval in Southwestern Pennsylvania and new gas content results  

SciTech Connect

A preliminary reconnaissance of coalbed methane gas content data from exploratory coal cores and pre-existing data implies that the greater the depth and rank, the greater the total and cumulative gas content. The coal seams studied, ranging in age from the Pennsylvanian-Permian Dunkard Group to the Middle Pennsylvanian Allegheny Group, are from the Main Bituminous Field and two of the anthracite fields. Consequently, the Pennsylvania Geological Survey and the West Virginia Geological and Economic Survey conducted a mapping investigation to evaluate the regional geology of the coal-bearing intervals and its influence on coalbed methane potential. Phase I of this study involved the entire Pennsylvanian coal-bearing interval; Phase II focused on a stratigraphic delineation and evaluation of Allegheny coalbeds and associated sandstones. A variety of cross sections and isopach maps show several prospective coalbeds and facies relationships with channel-fill sandstones. This suggests that some of these sandstones may be traps for coalbed methane. Often overlooked in reservoir characterization is the quality of a coal seam. Coal rank, grade, and type influence the reserves and production of coalbed methane; the higher the rank, the greater adsorptive capacity of the coal. The integration of coal quality with other critical tools of exploration may increase the success rate of finding {open_quotes}sweet spots.{close_quotes} Additional Pennsylvania Geological Survey drilling occurred in Beaver, Lawrence, Somerset, and Washington counties. Gas contents were graphically displayed against depth, thickness, and time for a variety of samples from 21 coal seams; average gas composition and Btu values were determined for selected samples.

Markowski, A.K. [Pennsylvania Dept. of Conservation and Natural Resources-Bureau of Topographic and Geologic Survey, Harrisburg, PA (United States)

1996-09-01T23:59:59.000Z

164

300-Area VOC Program Slug Test Characterization Results for Selected Test/Depth Intervals Conducted During the Drilling of Well 399-3-21  

SciTech Connect

This report presents brief test descriptions and analysis results for multiple, stress-level slug tests that were performed at selected test/depth intervals within well 399-3-21 as part of the 300-Area volatile organic compound characterization program. The test intervals were characterized as the borehole was advanced to its final drill depth (45.7 m) and before its completion as a monitor-well facility. The primary objective of the slug tests was to provide information pertaining to the vertical distribution of hydraulic conductivity with depth at this location and to select the final screen-depth interval for the monitor well. This type of characterization information is important for predicting/simulating contaminant migration (i.e., numerical flow/transport modeling) and designing proper monitor-well strategies within this area.

Spane, Frank A.

2007-07-19T23:59:59.000Z

165

Application of interval 2-tuple linguistic MULTIMOORA method for health-care waste treatment technology evaluation and selection  

Science Journals Connector (OSTI)

Abstract The management of health-care waste (HCW) is a major challenge for municipalities, particularly in the cities of developing countries. Selection of the best treatment technology for HCW can be viewed as a complicated multi-criteria decision making (MCDM) problem which requires consideration of a number of alternatives and conflicting evaluation criteria. Additionally, decision makers often use different linguistic term sets to express their assessments because of their different backgrounds and preferences, some of which may be imprecise, uncertain and incomplete. In response, this paper proposes a modified MULTIMOORA method based on interval 2-tuple linguistic variables (named ITL-MULTIMOORA) for evaluating and selecting HCW treatment technologies. In particular, both subjective and objective importance coefficients of criteria are taken into consideration in the developed approach in order to conduct a more effective analysis. Finally, an empirical case study in Shanghai, the most crowded metropolis of China, is presented to demonstrate the proposed method, and results show that the proposed ITL-MULTIMOORA can solve the HCW treatment technology selection problem effectively under uncertain and incomplete information environment.

Hu-Chen Liu; Jian-Xin You; Chao Lu; Meng-Meng Shan

2014-01-01T23:59:59.000Z

166

The effect of socio-economic status and food availability on first birth interval in a pre-industrial human population  

Science Journals Connector (OSTI)

...Around 60% of the energy consumed by working...i) Social status and first birth interval...women had a positive energy balance [41,42...the lowest social status [45]. Nevertheless...availability and nutritional status shape fecundity...reproductive traits allowing us to show that even...

2014-01-01T23:59:59.000Z

167

Convergence and error theorems for Hermite function pseudo-RBFs: Interpolation on a finite interval by Gaussian-localized polynomials  

Science Journals Connector (OSTI)

Abstract Any basis set { ? j ( x ) } can be rearranged by linear combinations into a basis of cardinal functions C j ( x ) with the property that C j ( x k ) = ? j k where the x k are the interpolation points and ? j k is the usual Kronecker delta-function, equal to one when j = k and equal to zero otherwise. The interpolant to a function f ( x ) then takes the simple form f N ( x ) = ? j = 1 N f ( x j ) C j ( x ) . In a companion study, Boyd and Alfaro showed that the cardinal functions for five different spectrally accurate radial basis functions (RBFs) are well approximated by polynomial cardinal functions multiplied by a Gaussian function when the RBF kernels are wide and the number of interpolation points N is small or moderate. Here, we abandon \\{RBFs\\} by using interpolants that are Gaussian-localized polynomials. This basis is equivalent to Hermite functions, a widely used basis for unbounded domains. We prove a rigorous convergence theorem for uniform grid on a finite interval that asserts a geometric rate of convergence for such Gaussian localized polynomial interpolants. Experimentally, we show that Hermite functions are also successful for interpolation on finite irregular grids, even on random grids. If a simple formula for the construction of the cardinal basis is known, then this is great treasure: a costly dense matrix problem is unnecessary. Lagrange invented an explicit product form for polynomial cardinal functions; Hermite function cardinals can be constructed by merely multiplying Lagrange's product by a Gaussian, exp ? ( ? q x 2 ) . We give guidelines for choosing the constant q; theory is simple because the Gaussian localizer is the same for all N cardinal functions. Gaussian \\{RBFs\\} are much more costly, much more ill-conditioned than Gaussian-localized polynomial interpolants.

John P. Boyd

2015-01-01T23:59:59.000Z

168

ISEE 3 observations during the CDAW 8 intervals: Case studies of the distant geomagnetic tail covering a wide range of geomagnetic activity  

SciTech Connect

The data obtained by the ISEE 3 spacecraft during the eight Coordinated Data Analysis Workshop 8 (CDAW 8) intervals provide an excellent opportunity to study the structure and dynamics of the distant geomagnetic tail under a wide range of geomagnetic activity ranging from intervals of magnetic quiet punctuated by isolated substorms to extended intervals of strong disturbance. By examining the properties of the plasma sheet, evidence has been found for the persistence of reconnection in the tail during long intervals of magnetic quiet, with the neutral line lying {approx}100 to 200 R{sub E} or more downtail. The suggestion that the distant tail plasma sheet is populated exclusively by tailward moving closed flux tubes under quiet geomagnetic conditions is therefore not supported. However, a slow plasma sheet regime is also found during such conditions, in which closed flux tubes move slowly tailward in a thick region adjacent to the magnetopause, presumably due to some form of viscous momentum transfer from the magnetosheath. This process does not appear to simultaneously transfer mass into the tail, and there is some indication that the Kelvin-Helmholtz instability is involved. The observations strongly suggest that the closed flux tubes originate from the closed field line plasma sheet region earthward of the neutral line rather than, for example, from the near-Earth low-latitude boundary layer. Plasmoids are observed in the distant tail following disturbance enhancements, the time of their appearance being generally consistent with disconnection from the near-Earth region at the time of the enhancement. Their structure is entirely consistent with the neutral line model.

Richardson, I.G.; Owen, C.J.; Cowley, S.W.H. (Blackett Laboratory, Imperial College, London (GB)); Galvin, A.B. (Department of Physics and Astronomy, University of Maryland, College Park, Maryland (USA)); Sanderson, T.R. (Space Science Department, European Space Agency, European Space Research and Technology Centre, Noordwijk (Netherlands)); Scholer, M. (Max-Planck-Institut feur Physik und Astrophysik, Garching, (Federal Republic of Germany)); Slavin, J.A. (NASA Goddard Space Flight Center, Greenbelt, Maryland (USA)); Zwickl, R.D. (Los Alamos National Laboratory, Los Alamos, New Mexico (USA))

1989-11-01T23:59:59.000Z

169

Water and gas coning: two and three phase system correlations for the critical oil production rate and optimum location of the completion interval  

E-Print Network (OSTI)

WATER AND GAS COMING: TWO AND THREE PHASE SYSTEM CORRELATIONS FOR THE CRITICAL OIL PRODUCTION RATE AND OPTIMUM LOCATION OF THE COMPLETION INTERVAL A Thesis by FRANCISCO MANUEL GONZALEZ, JR. Submitted to the Graduate College of Texas A...&M University in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE December 1987 Major Subject: Petroleum Engineering WATER AND GAS CONING: TWO AND THREE PHASE SYSTEM CORRELATIONS FOR THE CRITICAL OIL PRODUCTION RATE AND OPTIMUM...

Gonzalez, Francisco Manuel

2012-06-07T23:59:59.000Z

170

Mastectomy With Immediate Expander-Implant Reconstruction, Adjuvant Chemotherapy, and Radiation for Stage II-III Breast Cancer: Treatment Intervals and Clinical Outcomes  

SciTech Connect

Purpose: To determine intervals between surgery and adjuvant chemotherapy and radiation in patients treated with mastectomy with immediate expander-implant reconstruction, and to evaluate locoregional and distant control and overall survival in these patients. Methods and Materials: Between May 1996 and March 2004, 104 patients with Stage II-III breast cancer were routinely treated at our institution under the following algorithm: (1) definitive mastectomy with axillary lymph node dissection and immediate tissue expander placement, (2) tissue expansion during chemotherapy, (3) exchange of tissue expander for permanent implant, (4) radiation. Patient, disease, and treatment characteristics and clinical outcomes were retrospectively evaluated. Results: Median age was 45 years. Twenty-six percent of patients were Stage II and 74% Stage III. All received adjuvant chemotherapy. Estrogen receptor staining was positive in 77%, and 78% received hormone therapy. Radiation was delivered to the chest wall with daily 0.5-cm bolus and to the supraclavicular fossa. Median dose was 5040 cGy. Median interval from surgery to chemotherapy was 5 weeks, from completion of chemotherapy to exchange 4 weeks, and from exchange to radiation 4 weeks. Median interval from completion of chemotherapy to start of radiation was 8 weeks. Median follow-up was 64 months from date of mastectomy. The 5-year rate for locoregional disease control was 100%, for distant metastasis-free survival 90%, and for overall survival 96%. Conclusions: Mastectomy with immediate expander-implant reconstruction, adjuvant chemotherapy, and radiation results in a median interval of 8 weeks from completion of chemotherapy to initiation of radiation and seems to be associated with acceptable 5-year locoregional control, distant metastasis-free survival, and overall survival.

Wright, Jean L. [Department of Radiation Oncology, Memorial Sloan-Kettering Cancer Center, New York, NY (United States); Cordeiro, Peter G. [Department of Surgery, Plastic and Reconstructive Service, Memorial Sloan-Kettering Cancer Center, New York, NY (United States); Ben-Porat, Leah [Department of Epidemiology and Biostatistics, Memorial Sloan-Kettering Cancer Center, New York, NY (United States); Van Zee, Kimberly J. [Department of Surgery, Memorial Sloan-Kettering Cancer Center, New York, NY (United States); Hudis, Clifford [Department of Medicine, Solid Tumor Division, Breast Cancer Medicine Service, Memorial Sloan-Kettering Cancer Center, New York, NY (United States); Beal, Kathryn [Department of Radiation Oncology, Memorial Sloan-Kettering Cancer Center, New York, NY (United States); McCormick, Beryl [Department of Radiation Oncology, Memorial Sloan-Kettering Cancer Center, New York, NY (United States)], E-mail: mccormib@mskcc.org

2008-01-01T23:59:59.000Z

171

A pseudo-optimal inexact stochastic interval T2 fuzzy sets approach for energy and environmental systems planning under uncertainty: A case study for Xiamen City of China  

Science Journals Connector (OSTI)

Abstract In this study, a new Pseudo-optimal Inexact Stochastic Interval Type-2 Fuzzy Sets Linear Programming (PIS-IT2FSLP) energy model is developed to support energy system planning and environment requirements under uncertainties for Xiamen City. The PIS-IT2FSLP model is based on an integration of interval Type 2 (T2) Fuzzy Sets (FS) boundary programming and stochastic linear programming techniques, enables it to have robust abilities to the tackle uncertainties expressed as T2 FS intervals and probabilistic distributions within a general optimization framework. This new model can sophisticatedly facilitate system analysis of energy supply and energy conversion processes, and environmental requirements as well as provide capacity expansion options with multiple periods. The PIS-IT2FSLP model was applied to a real case study of Xiamen energy systems. Based on a robust two-step solution algorithm, reasonable solutions have been obtained, which reflect tradeoffs between economic and environmental requirements, and among seasonal volatility energy demands of the right hand side constraints of Xiamen energy system. Thus, the lower and upper solutions of PIS-IT2FSLP would then help local energy authorities adjust current energy patterns, and discover an optimal energy strategy for the development of Xiamen City.

L. Jin; G.H. Huang; Y.R. Fan; L. Wang; T. Wu

2015-01-01T23:59:59.000Z

172

EVALUATION OF SPRING OPERATED RELIEF VALVE MAINTENANCE INTERVALS AND EXTENSION OF MAINTENANCE TIMES USING A WEIBULL ANALYSIS WITH MODIFIED BAYESIAN UPDATING  

SciTech Connect

The Savannah River Site (SRS) spring operated pressure relief valve (SORV) maintenance intervals were evaluated using an approach provided by the American Petroleum Institute (API RP 581) for risk-based inspection technology (RBI). In addition, the impact of extending the inspection schedule was evaluated using Monte Carlo Simulation (MCS). The API RP 581 approach is characterized as a Weibull analysis with modified Bayesian updating provided by SRS SORV proof testing experience. Initial Weibull parameter estimates were updated as per SRS's historical proof test records contained in the Center for Chemical Process Safety (CCPS) Process Equipment Reliability Database (PERD). The API RP 581 methodology was used to estimate the SORV's probability of failing on demand (PFD), and the annual expected risk. The API RP 581 methodology indicates that the current SRS maintenance plan is conservative. Cost savings may be attained in certain mild service applications that present low PFD and overall risk. Current practices are reviewed and recommendations are made for extending inspection intervals. The paper gives an illustration of the inspection costs versus the associated risks by using API RP 581 Risk Based Inspection (RBI) Technology. A cost effective maintenance frequency balancing both financial risk and inspection cost is demonstrated.

Harris, S.; Gross, R.; Mitchell, E.

2011-01-18T23:59:59.000Z

173

Vienna proposal for interval standardization  

E-Print Network (OSTI)

://www.mat.univie.ac.at/neum with improvements suggested by remarks of Bo Einarsson, Maarten van Emden, Michel Hack, Nate Hayes, Ulrich Kulisch above. In particular, comprehensive discussions with Michel Hack, who read and com- mented in detail

Neumaier, Arnold

174

Introduction Nested common intervals on permutations Nested common intervals on sequences Conclusion Finding Nested Common Intervals  

E-Print Network (OSTI)

Conclusion Comparing genomes Genomes evolved from a common ancestor tend to share the same varieties of gene clusters used in genomes comparison. . . . seeking for gene clusters between their genomes. A gene cluster = a set of genes appearing, in spatial proximity along the chromosome, in at least two genomes. G. Blin

Blin, Guillaume

175

Petrophysical properties and geology of selected intervals in the Frio Formation, Stratton field, South Texas for modeling interwell seismic logging response  

SciTech Connect

Seismic or continuity logging consists of locating a seismic source in one borehole near or in a low-velocity layer and deploying a detector array in a second borehole. Detection of guided waves transmitted between the two wells indicates bed connectivity. The guided wave signatures are either leaky modes or normal modes (or both). The technique has numerous applications in various types of heterogeneous geological environments, including many Gulf Coast gas reservoirs. It can be used to determine the continuity of beds between wells, estimate and locate variations in the thickness of beds, and estimate the average rock physical properties of the beds. Stratton field was selected as the Gulf-Coast-gas-play type field for a project to model interwell seismic logging responses. Stratton is a mature gas field located in the south Texas Gulf Coast, about 30 miles southwest of Corpus Christi. It encompasses over 120,000 acres in portions of Kleberg, Nueces, and Jim Wells counties. Stratton is one of 29 fields in the Frio Formation fluvial-deltaic lay associated with the Vicksburg fault zone along the Texas Gulf Coast Basin. This poster presentation explains the technique of interwell seismic logging, documents the petrophysical properties and geology of intervals in the upper and middle Frio, and presents the results of the forward modeling tests.

Collier, H.A. [Tarleton State Univ., Stephenville, TX (United States); Parra, J.O. [Southwest Research Inst., San Antonio, TX (United States)

1996-09-01T23:59:59.000Z

176

Determining Azimuthal Variations in Frontal Froude Number from SAR Imagery  

E-Print Network (OSTI)

supercritical to subcritical flow for 6-12 hours after high water. Internal wave generation occurs regularly plume and ambient coastal waters, contribute to coastal productivity, and exert a major impact

Hickey, Barbara

177

Azimuthal impact directions from oblique impact crater morphology  

Science Journals Connector (OSTI)

......methods: laboratory|methods: numerical|comets: general|minor planets, asteroids...craters made by the impact of asteroids and comets on the planets be as revealing? Craters...very limited areas around some Apollo landing sites. Fig. 9 shows a digital elevation......

D. Wallis; M. J. Burchell; A. C. Cook; C. J. Solomon; N. McBride

2005-05-21T23:59:59.000Z

178

Vacuum Calculations in Azimuthally Symmetric Geometry \\Lambda M. S. Chance  

E-Print Network (OSTI)

the volume integrated perturbed magnetic energy in the vacuum region or through the continuity requirements plasma­vacuum boundary. The method is based upon using Green's second identity and the method.S. Department of Energy Contract No. DE­AC02­76­CHO­3073. #12; shell since most tokamak devices need to have

179

Vacuum Calculations in Azimuthally Symmetric Geometry M. S. Chance  

E-Print Network (OSTI)

energy in the vacuum region or through the continuity requirements for the normal component. The method is based upon using Green's second identity and the method of collocation. As useful byproducts symmetric gap in the Work supported by U.S. Department of Energy Contract No. DE-AC02-76-CHO-3073. #12;shell

180

Tsunami response at Wake Island: azimuthal mode analysis  

E-Print Network (OSTI)

Committee: Dr. Andrew C. Vastano This is sn extension of previous studies (numerical and hydraulic) of the relative amplitude response at Wake Island associated with plane progressive incident waves of stipulated time history, whose spectrum includes... of the island, Van Dorn cautioned that the influence of Wake Island topography on the wave spectrum really remains unknown. In a later study of the same data, by Royer (1969), it was concluded that the island topography may modify waves of certain periods...

Creswell, Wiltie Austin

2012-06-07T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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.


181

Feedback Control of Azimuthal Oscillations in ExB Devices --...  

NLE Websites -- All DOE Office Websites (Extended Search)

efficiency of the thruster by increasing electron transport to the anode. Electromagnetic interference from plasma oscillations in the thruster can also interfere with satellite...

182

Beam-Helicity Azimuthal Asymmetry measured with the Recoil Detector  

E-Print Network (OSTI)

Wasserstoff- und Deuterium-Target von HERMES genommen. Die erste Kalibrierung und Rekonstruk- tion dieser¨uglich der Strahlhelizit¨at aus den Daten von 2007 am Wasserstoff-Target wurden in dieser Arbeit durchgef

183

Recurrence of Lung Adenocarcinoma After an Interval of 15 Years Revealed by Demonstration of the Same Type of EML4–ALK Fusion Gene  

Science Journals Connector (OSTI)

Abstract We carried out an experiment on a 58-year-old man with multiple left lung tumors and swelling of multiple lymph nodes. For clinical staging and therapeutic purposes, bronchoalveolar lavage (BAL) cytology and lung biopsy were performed. The biopsy specimen revealed the left lower lung mass to be immunohistochemically ALK (anaplastic lymphoma kinase)-positive adenocarcinoma. Using the BAL specimen from the left lower lung, EML4 (echinoderm microtubule-associated protein-like 4)-ALK variant 1 fusion gene was detected by reverse transcription-polymerase chain reaction (RT-PCR). His past history showed that he had undergone an operation for lung adenocarcinoma of the right lower lobe 15 years before, and the pathological specimen at that time revealed that the lung adenocarcinoma with pleural invasion and single metastasis of mediastinal lymph node showed a mucinous cribriform pattern and/or signet-ring cell pattern. The typical histology led us to examine the ALK rearrangement in the primary lung cancer and mediastinal metastatic tumor. Immunohistochemistry (IHC) for ALK was positive, and ALK break apart fluorescence in situ hybridization (FISH) showed a positive result. Moreover, RT-PCR using formalin-fixed, paraffin-embedded tissue from the right lung cancer also demonstrated EML4–ALK variant 1 fusion gene. Although there is a possibility that the left lung cancer is de novo one with multiple metastases, detection of the same fusion gene of the very rare EML4–ALK variant 1 in both tumors suggests that the left cancer is a recurrence of the right lung cancer after an interval of 15 years.

Yoshitane Tsukamoto; Kiyonobu Kanamori; Takahiro Watanabe; Koji Mikami; Ryuji Ieki; Takashi Nakano; Kazuyoshi Kajimoto; Seiichi Hirota

2014-01-01T23:59:59.000Z

184

Boron Neutron Capture Therapty (BNCT) in an Oral Precancer Model: Therapeutic Benefits and Potential Toxicity of a Double Application of BNCT with a Six-Week Interval  

SciTech Connect

Given the clinical relevance of locoregional recurrences in head and neck cancer, we developed a novel experimental model of premalignant tissue in the hamster cheek pouch for long-term studies and demonstrated the partial inhibitory effect of a single application of Boron Neutron Capture Therapy (BNCT) on tumor development from premalignant tissue. The aim of the present study was to evaluate the effect of a double application of BNCT with a 6 week interval in terms of inhibitory effect on tumor development, toxicity and DNA synthesis. We performed a double application, 6 weeks apart, of (1) BNCT mediated by boronophenylalanine (BPA-BNCT); (2) BNCT mediated by the combined application of decahydrodecaborate (GB-10) and BPA [(GB-10 + BPA)-BNCT] or (3) beam-only, at RA-3 nuclear reactor and followed the animals for 8 months. The control group was cancerized and sham-irradiated. BPA-BNCT, (GB- 10 + BPA)-BNCT and beam-only induced a reduction in tumor development from premalignant tissue that persisted until 8, 3, and 2 months respectively. An early maximum inhibition of 100% was observed for all 3 protocols. No normal tissue radiotoxicity was detected. Reversible mucositis was observed in premalignant tissue, peaking at 1 week and resolving by the third week after each irradiation. Mucositis after the second application was not exacerbated by the first application. DNA synthesis was significantly reduced in premalignant tissue 8 months post-BNCT. A double application of BPA-BNCT and (GB-10 + BPA)-BNCT, 6 weeks apart, could be used therapeutically at no additional cost in terms of radiotoxicity in normal and dose-limiting tissues.

Andrea Monti Hughes; Emiliano C.C. Pozzi; Elisa M. Heber; Silvia Thorp; Marcelo Miller; Maria E. Itoiz; Romina F. Aromando; Ana J. Molinari; Marcela A. Garabalino; David W. Nigg; Veronica A. Trivillin; Amanda E. Schwint

2011-11-01T23:59:59.000Z

185

Temperature changes with time in the slotted interval of a deep, shut-in geothermal well near thermal equilibrium: East Mesa Well 31-1, Imperial County, California, 1977-1982  

SciTech Connect

Five precision temperature logs were obtained over a five year period (1977-1982) beginning three years after drilling and one year after last significant testing in East Mesa well 31-1 (32/sup 0/48.6'N, 115/sup 0/15.7'W). A sensitivity of measurement of 0.001/sup 0/C was maintained to the bottom of the well (165/sup 0/C, 180 bars). Useable precision was limited by convective motions within the hole (0.01-0.3/sup 0/C depending on ambient geothermal gradient), fluid leakage through the lubricator at the well head (4 bars) and, occasionally, by electrical or electronic noise. Comparison of these continuous logs indicates a general warming in and just above the slotted interval (1647-1877 m) which is attributed to flow into the lower levels of the slotted interval and up the casing and out into permeable zones at higher levels. Some flow continued upward through an uncemented interval of the annulus between casing and hole and out into the formation where it is blocked by cement ( about 1594 m). Some points of entrance or egress of fluid are marked by small, sharp temperature anomalies which have persisted over the 5-year period. Apparently, the uncemented part of the annulus has partly filled in, and flow into the bottom of slotted interval has increased (1978-1982). Both of these changes may have been induced by the nearby ( about 30 km) Imperial Valley earthquake of 10/15/79, or by the production or testing of nearby wells.

Diment, W.H.; Urban, T.C.

1982-10-01T23:59:59.000Z

186

Probing Balitsky-Fadin-Kuraev-Lipatov dynamics in the dijet cross section at large rapidity intervals in p(p)over-bar collisions at root s=1800 and 630 GeV  

E-Print Network (OSTI)

(Received 15 December 1999) Inclusive dijet production at large pseudorapidity intervals (Dh) between the two jets has been sug- gested as a regime for observing Balitsky-Fadin-Kuraev-Lipatov (BFKL) dynamics. We have mea- sured the dijet cross section... for large Dh in p?p collisions at p s H33527 1800 and 630 GeV using the D0 5723 VOLUME 84, NUMBER 25 PHYSICAL REVIEW LETTERS 19JUNE 2000 where E T 1 (E T 2 ) and h 1 (h 2 ) are the transverse energy and pseudorapidity h 1 2h 2 $ transfer during ing...

Baringer, Philip S.; Bean, Alice; Coppage, Don; Hebert, C.

2000-06-01T23:59:59.000Z

187

Slug Test Characterization Results for Multi-Test/Depth Intervals Conducted During the Drilling of CERCLA Operable Unit OU ZP-1 Wells 299-W10-33 and 299-W11-48  

SciTech Connect

Slug-test results obtained from single and multiple, stress-level slug tests conducted during drilling and borehole advancement provide detailed hydraulic conductivity information at two Hanford Site Operable Unit (OU) ZP-1 test well locations. The individual test/depth intervals were generally sited to provide hydraulic-property information within the upper ~10 m of the unconfined aquifer (i.e., Ringold Formation, Unit 5). These characterization results complement previous and ongoing drill-and-test characterization programs at surrounding 200-West and -East Area locations (see Figure S.1).

Newcomer, Darrell R.

2007-09-30T23:59:59.000Z

188

INTRODUCTION Terminal Proterozoic glacial intervals are  

E-Print Network (OSTI)

, paleontologic, and chemostratigraphic records from sections in Spitsbergen, Canada, Australia, and the Congo synthesis by using detailed 13C and 87Sr/86Sr records from the Congo craton, where a thick succession (>1000 the Congo craton succession as one of the least ambiguous records of chemo- stratigraphic and geologic

Kennedy, Martin J.

189

E-Print Network 3.0 - azimuthal pinch devices linear Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

the devices must first be initialised. *Firstly... the sensors *Now depending upon which input devices you wish to use do one of the following steps; If you... are using the...

190

CHAOTIC NEOCLASSICAL TRANSPORT AT AZIMUTHALLY PERTURBED OR WAVE-MINGLED SEPARATRIX  

E-Print Network (OSTI)

neoclassical ripple transport as particles collisionally change (at rate n) from trapped to passing and back, CA 92093, USA, akabantsev@ucsd.edu * Budker Institute of Nuclear Physics, Novosibirsk 630090, Russia one another and from passing particles. The drift orbits for particles trapped in the two separate

California at San Diego, University of

191

Azimuthal anisotropy in Au plus Au collisions at root S-NN=200 GeV  

E-Print Network (OSTI)

. Vokal,12 S. A. Voloshin,46 M. Vznuzdaev,25 W. T. Waggoner,10 F. Wang,32 G. Wang,20 G. Wang,5 X. L. Wang,36 Y. Wang,40 Y. Wang,41 Z. M. Wang,36 H. Ward,40 J. W. Watson,20 J. C. Webb,17 R. Wells,28 G. D. Westfall,24 A. Wetzler,21 C. Whitten Jr.,8 H...

Adams, J.; Aggarwal, MM; Ahammed, Z.; Amonett, J.; Anderson, BD; Arkhipkin, D.; Averichev, GS; Badyal, SK; Bai, Y.; Balewski, J.; Barannikova, O.; Barnby, LS; Baudot, J.; Bekele, S.; Belaga, VV; Bellwied, R.; Berger, J.; Bezverkhny, BI; Bharadwaj, S.; Bhasin, A.; Bhati, AK; Bhatia, VS; Bichsel, H.; Bielcik, J.; Bielcikova, J.; Billmeier, A.; Bland, LC; Blyth, CO; Bonner, BE; Botje, M.; Boucham, A.; Brandin, AV; Bravar, A.; Bystersky, M.; Cadman, RV; Cai, XZ; Caines, H.; Sanchez, MCD; Castillo, J.; Catu, O.; Cebra, D.; Chajecki, Z.; Chaloupka, P.; Chattopadhyay, S.; Chen, HF; Chen, Y.; Cheng, J.; Cherney, M.; Chikanian, A.; Christie, W.; Coffin, JP; Cormier, TM; Cramer, JG; Crawford, HJ; Das, D.; Das, S.; de Moura, MM; Derevschikov, AA; Didenko, L.; Dietel, T.; Dogra, SM; Dong, WJ; Dong, X.; Draper, JE; Du, F.; Dubey, AK; Dunin, VB; Dunlop, JC; Mazumdar, MRD; Eckardt, V.; Edwards, WR; Efimov, LG; Emelianov, V.; Engelage, J.; Eppley, G.; Erazmus, B.; Estienne, M.; Fachini, P.; Faivre, J.; Fatemi, R.; Fedorisin, J.; Filimonov, K.; Filip, P.; Finch, E.; Fine, V.; Fisyak, Y.; Fomenko, K.; Fu, J.; Gagliardi, Carl A.; Gaillard, L.; Gans, J.; Ganti, MS; Gaudichet, L.; Guerts, F.; Ghazikhanian, V.; Ghosh, P.; Gonzalez, JE; Grachov, O.; Grebenyuk, O.; Grosnick, D.; Guertin, SM; Guo, Y.; Gupta, A.; Gutierrez, TD; Hallman, TJ; Hamed, A.; Hardtke, D.; Harris, JW; Heinz, M.; Henry, TW; Hepplemann, S.; Hippolyte, B.; Hirsch, A.; Hjort, E.; Hoffmann, GW; Huang, HZ; Huang, SL; Hughes, EW; Humanic, TJ; Igo, G.; Ishihara, A.; Jacobs, P.; Jacobs, WW; Janik, M.; Jiang, H.; Jones, PG; Judd, EG; Kabana, S.; Kang, K.; Kaplan, M.; Keane, D.; Khodyrev, VY; Kiryluk, J.; Kisiel, A.; Kislov, EM; Klay, J.; Klein, SR; Koetke, DD; Kollegger, T.; Kopytine, M.; Kotchenda, L.; Kramer, M.; Kravtsov, P.; Kravtsov, VI; Krueger, K.; Kuhn, C.; Kulikov, AI; Kumar, A.; Kutuev, RK; Kuznetsov, AA; Lamont, MAC; Landgraf, JM; Lange, S.; Laue, F.; Lauret, J.; Lebedev, A.; Lednicky, R.; Lehocka, S.; LeVine, MJ; Li, C.; Li, Q.; Li, Y.; Lin, G.; Lindenbaum, SJ; Lisa, MA; Liu, F.; Liu, L.; Liu, QJ; Liu, Z.; Ljubicic, T.; Llope, WJ; Long, H.; Langacre, RS; Lopez-Noriega, M.; Love, WA; Lu, Y.; Ludlam, T.; Lynn, D.; Ma, GL; Ma, JG; Ma, YG; Magestro, D.; Mahajan, S.; Mahapatra, DP; Majka, R.; Mangotra, LK; Manweiler, R.; Margetis, S.; Markert, C.; Martin, L.; Marx, JN; Matis, HS; Matulenko, YA; McClain, CJ; McShane, TS; Meissner, F.; Melnick, Y.; Meschanin, A.; Miller, ML; Minaev, NG; Mironov, C.; Mischke, A.; Mishra, DK; Mitchell, J.; Mohanty, B.; Molnar, L.; Moore, CF; Morozov, DA; Munhoz, MG; Nandi, BK; Nayak, SK; Nayak, TK; Nelson, JM; Netrakanti, PK; Nikitin, VA; Nogach, LV; Nurushev, SB; Odyniec, G.; Ogawa, A.; Okorokov, V.; Oldenburg, M.; Olson, D.; Pal, SK; Panebratsev, Y.; Panitkin, SY; Pavlinov, AI; Pawlak, T.; Peitzmann, T.; Perevoztchikov, V.; Perkins, C.; Peryt, W.; Petrov, VA; Phatak, SC; Picha, R.; Planinic, M.; Pluta, J.; Porile, N.; Porter, J.; Poskanzer, AM; Potekhin, M.; Potrebenikova, E.; Potukuchi, BVKS; Prindle, D.; Pruneau, C.; Putschke, J.; Rakness, G.; Raniwala, R.; Raniwala, S.; Ravel, O.; Ray, RL; Razin, SV; Reichhold, D.; Reid, JG; Renault, G.; Retiere, F.; Ridiger, A.; Ritter, HG; Roberts, JB; Rogachevskiy, OV; Romero, JL; Rose, A.; Roy, C.; Ruan, L.; Sahoo, R.; Sakrejda, I.; Salur, S.; Sandweiss, J.; Sarsour, M.; Savin, I.; Sazhin, PS; Schambach, J.; Scharenberg, RP; Schmitz, N.; Schweda, K.; Seger, J.; Seyboth, P.; Shahaliev, E.; Shao, M.; Shao, W.; Sharma, M.; Shen, WQ; Shestermanov, KE; Shimanskiy, SS; Sichtermann, E.; Simon, F.; Singaraju, RN; Skoro, G.; Smirnov, N.; Snellings, R.; Sood, G.; Sorensen, P.; Sowinski, J.; Speltz, J.; Spinka, H. M.; Srivastava, B.; Stadnik, A.; Stanislaus, TDS; Stock, R.; Stolpovsky, A.; Strikhanov, M.; Stringfellow, B.; Suaide, AAP; Sugarbaker, E.; Suire, C.; Sumbera, M.; Surrow, B.; Symons, TJM; de Toledo, AS; Szarwas, P.; Tai, A.; Takahashi, J.; Tang, AH; Tarnowsky, T.; Thein, D.; Thomas, JH; Timoshenko, S.; Tokarev, M.; Trainor, TA; Trentalange, S.; Tribble, Robert E.; Tsai, OD; Ulery, J.; Ullrich, T.; Underwood, DG; Urkinbaev, A.; van Buren, G.; van Leeuwen, M.; Molen, AMV; Varma, R.; Vasilevski, IM; Vasiliev, AN; Vernet, R.; Vigdor, SE; Viyogi, YP; Vokal, S.; Voloshin, SA; Vznuzdaev, M.; Waggoner, WT; Wang, F.; Wang, G.; Wang, G.; Wang, XL; Wang, Y.; Wang, Y.; Wang, ZM; Ward, H.; Watson, JW; Webb, JC; Wells, R.; Westfall, GD; Wetzler, A.; Whitten, C.; Wieman, H.; Wissink, SW; Witt, R.; Wood, J.; Wu, J.; Xu, N.; Xu, Z.; Xu, ZZ; Yamamoto, E.; Yepes, P.; Yurevich, VI; Zanevsky, YV; Zhang, H.; Zhang, WM; Zhang, ZP; Zoulkarneev, R.; Zoulkarneeva, Y.; Zubarev, AN; Braem, A.; Davenport, M.; Cataldo, GD; Bari, DD; Martinengo, P.; Nappi, E.; Paic, G.; Posa, E.; Puiz, F.; Schyns, E.; Star Collaboration; STAR-RICH Collaboration.

2005-01-01T23:59:59.000Z

192

On the dynamic nature of azimuthal thermoacoustic modes in annular gas turbine combustion chambers  

Science Journals Connector (OSTI)

...gas turbine combustor, it has...the dynamic pressure field which...requirements in real gas turbine applications...manner that high-amplitude...in annular gas turbines...bifurcations in gas turbine combustor. Int. J...effects on high-frequency...characteristics of pressure oscillations...

2013-01-01T23:59:59.000Z

193

E-Print Network 3.0 - azimuthally dependent transport Sample...  

NLE Websites -- All DOE Office Websites (Extended Search)

R. Astron. Soc. 339, 983992 (2003) The interaction of a giant planet with a disc with MHD turbulence I. Summary: a residual dependence on resolution (see Brandenburg et al....

194

High performance path following for marine vehicles using azimuthing podded propulsion .  

E-Print Network (OSTI)

??Podded propulsion systems offer greater maneuvering possibilities for marine vehicles than conventional shaft and rudder systems. As the propulsion unit rotates about its vertical axis… (more)

Greytak, Matthew B. (Matthew Bardeen)

2006-01-01T23:59:59.000Z

195

E-Print Network 3.0 - azimuthal line cusp Sample Search Results  

NLE Websites -- All DOE Office Websites (Extended Search)

H.U. FREY2, S.M. PETRINEC1, E.S. Summary: and magnetosheath field lines), the magnetic field lines that skim the magnetopause all map to this single cusp... neutral line,...

196

Azimuthal Turing Patterns, Bright and Dark Cavity Solitons in Kerr Combs Generated With  

E-Print Network (OSTI)

!þ "h! ! "h!#12; þ "h!, as long as they fulfill the requirements of energy and momentum conservation, 2013; accepted August 2, 2013. Date of publication August 8, 2013; date of current version August 23 Journal Solitons in Kerr Combs With WGM Resonators #12;in aerospace and communication engineering, as well

Maryland, Baltimore County, University of

197

E-Print Network 3.0 - azimuthal shear flows Sample Search Results  

NLE Websites -- All DOE Office Websites (Extended Search)

GeoSciences, Edinburgh Anisotropy Project Collection: Geosciences 57 Energy transient growth in the TaylorCouette problema... A lvaro Meseguerb) Summary: circular Couette flow by...

198

Effects of triangular flow on di-hadron azimuthal correlations in relativistic heavy ion collisions  

E-Print Network (OSTI)

. Lin, Phys. Rev. C 69, 031901(R) (2004). [38] B. Zhang, Comput. Phys. Commun. 109, 193 (1998). [39] B. A. Li and C. M. Ko, Phys. Rev. C 52, 2037 (1995). [40] A. M. Poskanzer and S. A. Voloshin, Phys. Rev. C 58, 1671 (1998). [41] G. L. Ma and X...

Xu, Jun; Ko, Che Ming.

2011-01-01T23:59:59.000Z

199

E-Print Network 3.0 - azimuthal anisotropy relative Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

revised methodology was developed where... electrical anisotropy, which is related to fracture direction and intensity. The method is applied... the electrical anisotropy from the...

200

E-Print Network 3.0 - azimuthal transverse momentum Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

au n o 6, Tome 48, juin 1987 Summary: IN THE TRANSVERSE MOMENTUM ANALYSIS P. DANIELEWICZ Institute of Theoretical Physics, Warsaw University, ul. Hoza 69... , PL-00-681...

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

E-Print Network 3.0 - azimuthal correlation measurements Sample...  

NLE Websites -- All DOE Office Websites (Extended Search)

- Department of Geophysics, Colorado School of Mines Collection: Geosciences 3 Microwave Wind Direction Retrieval over Antarctica David G. Long and Mark Drinkwater Summary:...

202

WTI Crude Oil Price: Base Case and 95% Confidence Interval  

Gasoline and Diesel Fuel Update (EIA)

7 7 Notes: Spot WTI prices broke $35 and even $36 per barrel in November as anticipated boosts to world supply from OPEC and other sources failed to find much realization in actual stocks data. The idea that stocks are still languishing at below-normal levels is particularly persuasive when one views current levels (for key consuming regions) relative to "normal" values which account for the long-term trend in OECD stocks. We believe that monthly average WTI prices will stay around $30 per barrel for the first part of 2001. This is a noticeable upward shift in our projected average prices from even a month ago. The shift reflects greater emphasis on the lack of stock builds and less emphasis on the assumption that supply from OPEC and non-OPEC suppliers may be exceeding demand by 1-2

203

WTI Crude Oil Price: Base Case and 95% Confidence Interval  

Gasoline and Diesel Fuel Update (EIA)

9 9 Notes: Spot WTI prices broke $35 and even $36 per barrel in November as anticipated boosts to world supply from OPEC and other sources did not show up in actual stocks data. The recent decline in prices seems to be more the result of an unraveling of speculative pressures than a change in underlying fundamentals. Prices had been running higher than supply/demand fundamentals would have indicated throughout the fall months as a result of rising Mideast tensions, concern over the adequacy of distillate supplies, and expectations of Iraqi supply interruptions. But Mideast tensions seemed to ease in December and the market appeared to perceive a quick return of Iraqi crude oil supplies at full capacity. Pledges by Saudi Arabia/OPEC to offset a longer term Iraqi

204

WTI Crude Oil Price: Base Case and 95% Confidence Interval  

Gasoline and Diesel Fuel Update (EIA)

6 6 Notes: Spot WTI crude oil prices broke $35 and even $36 per barrel in November as anticipated boosts to world supply from OPEC and other sources did not show up in actual stocks data. The recent decline in prices seems to be more the result of an unraveling of speculative pressures than a change in underlying fundamentals. Prices had been running higher than supply/demand fundamentals would have indicated throughout the fall months as a result of rising Mideast tensions, concern over the adequacy of distillate supplies, and expectations of Iraqi supply interruptions. But Mideast tensions seemed to ease in December and the market appeared to perceive a quick return of Iraqi crude oil supplies at full capacity. Pledges by Saudi Arabia/OPEC to offset a longer term Iraqi

205

Gauge Theories on an Interval: Unitarity Without a Higgs Boson  

E-Print Network (OSTI)

breaking without a Higgs boson. Gauge Theories on anscattering amplitude. The Higgs boson is localized at y = ?Rreal scalar ?eld, the Higgs boson. At tree level, the

Csaki, Csaba; Grojean, Christophe; Murayama, Hitoshi; Luigi, Pilo; Terning, John

2004-01-01T23:59:59.000Z

206

WHY INTERVALS? WHY FUZZY NUMBERS? TOWARDS A NEW  

E-Print Network (OSTI)

about the physical world is measurements; see, e.g., [20]. Measurements are never 100% accurate. As a result, the result #x of the measurement is, in general, di#erent from the (unknown) actual value x of the desired quantity. The di#erence #x def = #x - x between the measured and the actual values is usually

Kreinovich, Vladik

207

WHY INTERVALS? WHY FUZZY NUMBERS? TOWARDS A NEW  

E-Print Network (OSTI)

about the physical world is measurements; see, e.g., [20]. Measurements are never 100% accurate. As a result, the result x of the measurement is, in general, different from the (unknown) actual value x of the desired quantity. The difference x def = x - x between the measured and the actual values is usually

Kreinovich, Vladik

208

Why Intervals? Why Fuzzy Numbers? Towards a New Justification  

E-Print Network (OSTI)

: a practical explanation. One of the main source of information about the physical world is measure­ ments; see, e.g., [20]. Measurements are never 100% accurate. As a result, the result # x of the measurement is - x between the measured and the actual values is usually called a measurement error

Ward, Karen

209

Why Intervals? Why Fuzzy Numbers? Towards a New Justi cation  

E-Print Network (OSTI)

: a practical explanation. One of the main source of information about the physical world is measure- ments; see, e.g., [20]. Measurements are never 100% accurate. As a result, the result x of the measurement is between the measured and the actual values is usually called a measurement error. The manufacturers

Ward, Karen

210

Measurement and interpretation of electrocardiographic QT intervals in murine hearts  

E-Print Network (OSTI)

/min (Bredel peristaltic pumps, model 505S; Watson-Marlow, Falmouth, Cornwall, UK) with Krebs-Henseleit (KH) solution (in mM: NaCl 119, NaHCO3 25, KCl 4, KH2PO4 1.2, MgCl2 1, CaCl2 1.8, glucose Address for reprint requests and other correspondence: J. A. Fraser... . The anesthetized mice were placed on a heating pad with continuous monitoring of body temperature for three-lead ECG measurements in lead II for over 10 min using subcutaneous needle electrodes and a PowerLab 26T system (ADInstru- ments, Oxfordshire, UK...

Zhang, Yanmin; Wu, JingJing; King, James H.; Huang, Christopher L.-H.; Fraser, James A.

2014-04-04T23:59:59.000Z

211

INTERVAL COMPUTATIONS WITH INTLAB SIEGFRIED M. RUMP, HAMBURG  

E-Print Network (OSTI)

; A = rand(n); B = rand(n); C = zeros(n); tic for i=1:n for j=1:n for k=1:n C(i,j) = C(i,j) + A(i,k)*B(k,j); end end end toc C = zeros(n); tic for i=1:n for j=1:n C(i,j) = C(i,j) + A(i,:)*B(:,j); end end toc C = zeros(n); tic for i=1:n C(i,:) = C(i,:) + A(i,:)*B; end toc C = zeros(n); tic C = A*B; toc The following

Rump, Siegfried M.

212

Towards Combining Probabilistic, Interval, Fuzzy Uncertainty, and Constraints: On the  

E-Print Network (OSTI)

that there are resources such as miner- als at a certain location is to actually drill a borehole and analyze the materials different measurement results that can be obtained without actually drilling the boreholes: e.g., gravity half of the 20th century. The result was the discovery of many large relatively easy to locate

Kreinovich, Vladik

213

Towards Combining Probabilistic, Interval, Fuzzy Uncertainty, and Constraints: On the  

E-Print Network (OSTI)

that there are resources such as miner­ als at a certain location is to actually drill a borehole and analyze the materials different measurement results that can be obtained without actually drilling the boreholes: e.g., gravity half of the 20th century. The result was the discovery of many large relatively easy to locate

Kreinovich, Vladik

214

Applications of Fuzzy Measures and Intervals in Finance  

E-Print Network (OSTI)

investment assets in order to diversify risk and obtain a maximal return for the given acceptable level sought goals are max- imization of the return for a given acceptable level of risk and minimization, the problem of selecting an investment portfolio to guarantee a given return, at a minimal risk, have been

Magoc, Tanja

215

An Assessment of Interval Data and Their Potential Application...  

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

to collect residential AMI data. Over 43 million households and businesses currently use Green Button to access their energy usage data and dozens of utilities serving millions of...

216

Variation in human gait intervals on a treadmill  

E-Print Network (OSTI)

. The placement of the optical sensor and reflector is shown in figure 9. The reflective sensor consists of a narrow beam red LED and a modified infrared detector module. The reflective strip was detected when LED light was reflected back to the sensor. The red... LED was a useful light source because it was very tightly focused, with a half power angle of only three degrees. The light from the red LED was also visible which simplified the optimization of the geometry of the final reflective sensor...

Abrams, Mark Alan

1994-01-01T23:59:59.000Z

217

The velocity campaign for ignition on NIF  

SciTech Connect

Achieving inertial confinement fusion ignition requires a symmetric, high velocity implosion. Experiments show that we can reach 95 {+-} 5% of the required velocity by using a 420 TW, 1.6 MJ laser pulse. In addition, experiments with a depleted uranium hohlraum show an increase in capsule performance which suggests an additional 18 {+-} 5 {mu}m/ns of velocity with uranium hohlraums over gold hohlraums. Combining these two would give 99 {+-} 5% of the ignition velocity. Experiments show that we have the ability to tune symmetry using crossbeam transfer. We can control the second Legendre mode (P2) by changing the wavelength separation between the inner and outer cones of laser beams. We can control the azimuthal m = 4 asymmetry by changing the wavelength separation between the 23.5 and 30 degree beams on NIF. This paper describes our 'first pass' tuning the implosion velocity and shape on the National Ignition Facility laser [Moses et al., Phys. Plasmas, 16, 041006 (2009)].

Callahan, D. A.; Meezan, N. B.; Glenzer, S. H.; MacKinnon, A. J.; Benedetti, L. R.; Bradley, D. K.; Celeste, J. R.; Celliers, P. M.; Dixit, S. N.; Doeppner, T.; Dzentitis, E. G.; Glenn, S.; Haan, S. W.; Haynam, C. A.; Hicks, D. G.; Hinkel, D. E.; Jones, O. S.; Landen, O. L.; London, R. A.; MacPhee, A. G. [Lawrence Livermore National Laboratory, Livermore, California 94550 (United States); and others

2012-05-15T23:59:59.000Z

218

IEEE TRANSACTIONS ON GEOSCIENCE AND REMOTE SENSING, VOL. XX, NO. Y, MONTH 2000 100 Azimuth Variation in Microwave Scatterometer and  

E-Print Network (OSTI)

to produce roughness on various scales. Roughness ranges from broad, basin scale ice-sheet topography the Antarctic ice sheet wind-generated roughness and snowlaying combine to produce an anisotropic response, ice sheet and bedrock topography and the snow deposition, drift, and erosional environment combine

Long, David G.

219

Observation of charge-dependent azimuthal correlations and possible local strong parity violation in heavy-ion collisions  

E-Print Network (OSTI)

,13 G. M. S. Vasconcelos,7 A. N. Vasiliev,31 F. Videbaek,3 Y. P. Viyogi,46 S. Vokal,16 S. A. Voloshin,49 M. Wada,42 M. Walker,21 F. Wang,32 G. Wang,6 H. Wang,23 J. S. Wang,19 Q. Wang,32 X. Wang,43 X. L. Wang,37 Y. Wang,43 G. Webb,18 J. C. Webb,45 G...

Abelev, B. I.; Aggarwal, M. M.; Ahammed, Z.; Alakhverdyants, A. V.; Anderson, B. D.; Arkhipkin, D.; Averichev, G. S.; Balewski, J.; Barannikova, O.; Barnby, L. S.; Baumgart, S.; Beavis, D. R.; Bellwied, R.; Benedosso, F.; Betancourt, M. J.; Betts, R. R.; Bhasin, A.; Bhati, A. K.; Bichsel, H.; Bielcik, J.; Bielcikova, J.; Biritz, B.; Bland, L. C.; Bnzarov, I.; Bonner, B. E.; Bouchet, J.; Braidot, E.; Brandin, A. V.; Bridgeman, A.; Bruna, E.; Bueltmann, S.; Burton, T. P.; Cai, X. Z.; Caines, H.; Sanchez, M. Calderon de la Barca; Catu, O.; Cebra, D.; Cendejas, R.; Cervantes, M. C.; Chajecki, Z.; Chaloupka, P.; Chattopadhyay, S.; Chen, H. F.; Chen, J. H.; Chen, J. Y.; Cheng, J.; Cherney, M.; Chikanian, A.; Choi, K. E.; Christie, W.; Chung, P.; Clarke, R. F.; Codrington, M. J. M.; Corliss, R.; Cormier, T. M.; Cosentino, M. R.; Cramer, J. G.; Crawford, H. J.; Das, D.; Dash, S.; Daugherity, M.; De Silva, L. C.; Dedovich, T. G.; DePhillips, M.; Derevschikov, A. A.; de Souza, R. Derradi; Didenko, L.; Djawotho, P.; Dzhordzhadze, V.; Dogra, S. M.; Dong, X.; Drachenberg, J. L.; Draper, J. E.; Dunlop, J. C.; Mazumdar, M. R. Dutta; Efimov, L. G.; Elhalhuli, E.; Elnimr, M.; Engelage, J.; Eppley, G.; Erazmus, B.; Estienne, M.; Eun, L.; Fachini, P.; Fatemi, R.; Fedorisin, J.; Feng, A.; Filip, P.; Finch, E.; Fine, V.; Fisyak, Y.; Gagliardi, Carl A.; Gangadharan, D. R.; Ganti, M. S.; Garcia-Solis, E. J.; Geromitsos, A.; Geurts, F.; Ghazikhanian, V.; Ghosh, P.; Gorbunov, Y. N.; Gordon, A.; Grebenyuk, O.; Grosnick, D.; Grube, B.; Guertin, S. M.; Guimaraes, K. S. F. F.; Gupta, A.; Gupta, N.; Guryn, W.; Haag, B.; Hallman, T. J.; Hamed, A.; Harris, J. W.; Heinz, M.; Heppelmann, S.; Hirsch, A.; Hjort, E.; Hoffman, A. M.; Hoffmann, G. W.; Hofman, D. J.; Hollis, R. S.; Huang, H. Z.; Humanic, T. J.; Huo, L.; Igo, G.; Iordanova, A.; Jacobs, P.; Jacobs, W. W.; Jakl, P.; Jena, C.; Jin, F.; Jones, C. L.; Jones, P. G.; Joseph, J.; Judd, E. G.; Kabana, S.; Kajimoto, K.; Kang, K.; Kapitan, J.; Kauder, K.; Keane, D.; Kechechyan, A.; Kettler, D.; Khodyrev, V. Yu; Kikola, D. P.; Kiryluk, J.; Kisiel, A.; Klein, S. R.; Knospe, A. G.; Kocoloski, A.; Koetke, D. D.; Konzer, J.; Kopytine, M.; Koralt, I.; Korsch, W.; Kotchenda, L.; Kouchpil, V.; Kravtsov, P.; Kravtsov, V. I.; Krueger, K.; Krus, M.; Kumar, L.; Kurnadi, P.; Lamont, M. A. C.; Landgraf, J. M.; LaPointe, S.; Lauret, J.; Lebedev, A.; Lednicky, R.; Lee, C-H; Lee, J. H.; Leight, W.; LeVine, M. J.; Li, C.; Li, N.; Li, Y.; Lin, G.; Lindenbaum, S. J.; Lisa, M. A.; Liu, F.; Liu, H.; Liu, J.; Liu, L.; Ljubicic, T.; Llope, W. J.; Longacre, R. S.; Love, W. A.; Lu, Y.; Ludlam, T.; Ma, G. L.; Ma, Y. G.; Mahapatra, D. P.; Majka, R.; Mall, O. I.; Mangotra, L. K.; Manweiler, R.; Margetis, S.; Markert, C.; Masui, H.; Matis, H. S.; Matulenko, Yu A.; McDonald, D.; McShane, T. S.; Meschanin, A.; Milner, R.; Minaev, N. G.; Mioduszewski, Saskia; Mischke, A.; Mohanty, B.; Morozov, D. A.; Munhoz, M. G.; Nandi, B. K.; Nattrass, C.; Nayak, T. K.; Nelson, J. M.; Netrakanti, P. K.; Ng, M. J.; Nogach, L. V.; Nurushev, S. B.; Odyniec, G.; Ogawa, A.; Okada, H.; Okorokov, V.; Olson, D.; Pachr, M.; Page, B. S.; Pal, S. K.; Pandit, Y.; Panebratsev, Y.; Pawlak, T.; Peitzmann, T.; Perevoztchikov, V.; Perkins, C.; Peryt, W.; Phatak, S. C.; Pile, P.; Planinic, M.; Ploskon, M. A.; Pluta, J.; Plyku, D.; Poljak, N.; Poskanzer, A. M.; Potukuchi, B. V. K. S.; Prindle, D.; Pruneau, C.; Pruthi, N. K.; Pujahari, P. R.; Putschke, J.; Raniwala, R.; Raniwala, S.; Ray, R. L.; Redwine, R.; Reed, R.; Ridiger, A.; Ritter, H. G.; Roberts, J. B.; Rogachevskiy, O. V.; Romero, J. L.; Rose, A.; Roy, C.; Ruan, L.; Russcher, M. J.; Sahoo, R.; Sakai, S.; Sakrejda, I.; Sakuma, T.; Salur, S.; Sandweiss, J.; Schambach, J.; Scharenberg, R. P.; Schmitz, N.; Seele, J.; Seger, J.; Selyuzhenkov, I.; Semertzidis, Y.; Seyboth, P.; Shahaliev, E.; Shao, M.; Sharma, M.; Shi, S. S.; Shi, X-H; Sichtermann, E. P.; Simon, F.; Singaraju, R. N.; Skoby, M. J.; Smirnov, N.; Sorensen, P.; Sowinski, J.; Spinka, H. M.; Srivastava, B.; Stanislaus, T. D. S.; Staszak, D.; Strikhanov, M.; Stringfellow, B.; Suaide, A. A. P.; Suarez, M. C.; Subba, N. L.; Sumbera, M.; Sun, X. M.; Sun, Y.; Sun, Z.; Surrow, B.; Symons, T. J. M.; de Toledo, A. Szanto; Takahashi, J.; Tang, A. H.; Tang, Z.; Tarini, L. H.; Tarnowsky, T.; Thein, D.; Thomas, J. H.; Tian, J.; Timmins, A. R.; Timoshenko, S.; Tlusty, D.; Tokarev, M.; Tram, V. N.; Trentalange, S.; Tribble, Robert E.; Tsai, O. D.; Ulery, J.; Ullrich, T.; Underwood, D. G.; Van Buren, G.; Van Nieuwenhuizen, G.; Vanfossen, J. A., Jr.; Varma, R.; Vasconcelos, G. M. S.; Vasiliev, A. N.; Videbaek, F.; Viyogi, Y. P.; Vokal, S.; Voloshin, S. A.; Wada, M.; Walker, M.; Wang, F.; Wang, G.; Wang, H.; Wang, J. S.; Wang, Q.; Wang, X.

2010-01-01T23:59:59.000Z

220

Parton energy loss in heavy-ion collisions via direct-photon and charged-particle azimuthal correlations  

E-Print Network (OSTI)

Nieuwenhuizen,22 J. A. Vanfossen Jr.,18 R. Varma,13 G. M. S. Vasconcelos,7 A. N. Vasiliev,32 F. Videbaek,3 S. E. Vigdor,14 Y. P. Viyogi,12 S. Vokal,17 S. A. Voloshin,50 M. Wada,43 M. Walker,22 F. Wang,33 G. Wang,6 H. Wang,24 J. S. Wang,20 Q. Wang,33 X. Wang,44... X. L. Wang,38 Y. Wang,44 G. Webb,19 J. C. Webb,46 G. D. Westfall,24 C. Whitten Jr.,6 H. Wieman,21 S. W. Wissink,14 R. Witt,45 Y. Wu,51 W. Xie,33 N. Xu,21 Q. H. Xu,39 Y. Xu,38 Z. Xu,3 Y. Yang,20 P. Yepes,36 K. Yip,3 I-K. Yoo,34 Q. Yue,44 M. Zawisza...

Abelev, B. I.; Aggarwal, M. M.; Ahammed, Z.; Alakhverdyants, A. V.; Anderson, B. D.; Arkhipkin, D.; Averichev, G. S.; Balewski, J.; Barannikova, O.; Barnby, L. S.; Baudot, J.; Baumgart, S.; Beavis, D. R.; Bellwied, R.; Benedosso, F.; Betancourt, M. J.; Betts, R. R.; Bhasin, A.; Bhati, A. K.; Bichsel, H.; Bielcik, J.; Bielcikova, J.; Biritz, B.; Bland, L. C.; Bnzarov, I.; Bombara, M.; Bonner, B. E.; Bouchet, J.; Braidot, E.; Brandin, A. V.; Bruna, E.; Bueltmann, S.; Burton, T. P.; Bystersky, M.; Cai, X. Z.; Caines, H.; Sanchez, M. Calderon de la Barca; Catu, O.; Cebra, D.; Cendejas, R.; Cervantes, M. C.; Chajecki, Z.; Chaloupka, P.; Chattopadhyay, S.; Chen, H. F.; Chen, J. H.; Chen, J. Y.; Cheng, J.; Cherney, M.; Chikanian, A.; Choi, K. E.; Christie, W.; Clarke, R. F.; Codrington, M. J. M.; Corliss, R.; Cormier, T. M.; Cosentino, M. R.; Cramer, J. G.; Crawford, H. J.; Das, D.; Dash, S.; Daugherity, M.; De Silva, L. C.; Dedovich, T. G.; DePhillips, M.; Derevschikov, A. A.; de Souza, R. Derradi; Didenko, L.; Djawotho, P.; Dogra, S. M.; Dong, X.; Drachenberg, J. L.; Draper, J. E.; Dunlop, J. C.; Mazumdar, M. R. Dutta; Efimov, L. G.; Elhalhuli, E.; Elnimr, M.; Engelage, J.; Eppley, G.; Erazmus, B.; Estienne, M.; Eun, L.; Fachini, P.; Fatemi, R.; Fedorisin, J.; Feng, A.; Filip, P.; Finch, E.; Fine, V.; Fisyak, Y.; Gagliardi, Carl A.; Gaillard, L.; Gangadharan, D. R.; Ganti, M. S.; Garcia-Solis, E. J.; Geromitsos, A.; Geurts, F.; Ghazikhanian, V.; Ghosh, P.; Gorbunov, Y. N.; Gordon, A.; Grebenyuk, O.; Grosnick, D.; Grube, B.; Guertin, S. M.; Guimaraes, K. S. F. F.; Gupta, A.; Gupta, N.; Guryn, W.; Haag, B.; Hallman, T. J.; Hamed, A.; Harris, J. W.; He, W.; Heinz, M.; Heppelmann, S.; Hippolyte, B.; Hirsch, A.; Hjort, E.; Hoffman, A. M.; Hoffmann, G. W.; Hofman, D. J.; Hollis, R. S.; Huang, H. Z.; Humanic, T. J.; Huo, L.; Igo, G.; Iordanova, A.; Jacobs, P.; Jacobs, W. W.; Jakl, P.; Jena, C.; Jin, F.; Jones, C. L.; Jones, P. G.; Joseph, J.; Judd, E. G.; Kabana, S.; Kajimoto, K.; Kang, K.; Kapitan, J.; Kauder, K.; Keane, D.; Kechechyan, A.; Kettler, D.; Khodyrev, V. Yu; Kikola, D. P.; Kiryluk, J.; Kisiel, A.; Klein, S. R.; Knospe, A. G.; Kocoloski, A.; Koetke, D. D.; Konzer, J.; Kopytine, M.; Koralt, I.; Korsch, W.; Kotchenda, L.; Kouchpil, V.; Kravtsov, P.; Kravtsov, V. I.; Krueger, K.; Krus, M.; Kuhn, C.; Kumar, L.; Kurnadi, P.; Lamont, M. A. C.; Landgraf, J. M.; LaPointe, S.; Lauret, J.; Lebedev, A.; Lednicky, R.; Lee, C-H; Lee, J. H.; Leight, W.; LeVine, M. J.; Li, C.; Li, N.; Li, Y.; Lin, G.; Lindenbaum, S. J.; Lisa, M. A.; Liu, F.; Liu, H.; Liu, J.; Liu, L.; Ljubicic, T.; Llope, W. J.; Longacre, R. S.; Love, W. A.; Lu, Y.; Ludlam, T.; Ma, G. L.; Ma, Y. G.; Mahapatra, D. P.; Majka, R.; Mall, O. I.; Mangotra, L. K.; Manweiler, R.; Margetis, S.; Markert, C.; Masui, H.; Matis, H. S.; Matulenko, Yu A.; McDonald, D.; McShane, T. S.; Meschanin, A.; Milner, R.; Minaev, N. G.; Mioduszewski, Saskia; Mischke, A.; Mohanty, B.; Morozov, D. A.; Munhoz, M. G.; Nandi, B. K.; Nattrass, C.; Nayak, T. K.; Nelson, J. M.; Netrakanti, P. K.; Ng, M. J.; Nogach, L. V.; Nurushev, S. B.; Odyniec, G.; Ogawa, A.; Okada, H.; Okorokov, V.; Olson, D.; Pachr, M.; Page, B. S.; Pal, S. K.; Pandit, Y.; Panebratsev, Y.; Pawlak, T.; Peitzmann, T.; Perevoztchikov, V.; Perkins, C.; Peryt, W.; Phatak, S. C.; Pile, P.; Planinic, M.; Ploskon, M. A.; Pluta, J.; Plyku, D.; Poljak, N.; Poskanzer, A. M.; Potukuchi, B. V. K. S.; Prindle, D.; Pruneau, C.; Pruthi, N. K.; Pujahari, P. R.; Putschke, J.; Raniwala, R.; Raniwala, S.; Ray, R. L.; Redwine, R.; Reed, R.; Ridiger, A.; Ritter, H. G.; Roberts, J. B.; Rogachevskiy, O. V.; Romero, J. L.; Rose, A.; Roy, C.; Ruan, L.; Russcher, M. J.; Sahoo, R.; Sakai, S.; Sakrejda, I.; Sakuma, T.; Salur, S.; Sandweiss, J.; Sarsour, M.; Schambach, J.; Scharenberg, R. P.; Schmitz, N.; Seger, J.; Selyuzhenkov, I.; Seyboth, P.; Shabetai, A.; Shahaliev, E.; Shao, M.; Sharma, M.; Shi, S. S.; Shi, X-H; Sichtermann, E. P.; Simon, F.; Singaraju, R. N.; Skoby, M. J.; Smirnov, N.; Sorensen, P.; Sowinski, J.; Spinka, H. M.; Srivastava, B.; Stanislaus, T. D. S.; Staszak, D.; Strikhanov, M.; Stringfellow, B.; Suaide, A. A. P.; Suarez, M. C.; Subba, N. L.; Sumbera, M.; Sun, X. M.; Sun, Y.; Sun, Z.; Surrow, B.; Symons, T. J. M.; de Toledo, A. Szanto; Takahashi, J.; Tang, A. H.; Tang, Z.; Tarini, L. H.; Tarnowsky, T.; Thein, D.; Thomas, J. H.; Tian, J.; Timmins, A. R.; Timoshenko, S.; Tlusty, D.; Tokarev, M.; Trainor, T. A.; Tram, V. N.; Trentalange, S.; Tribble, Robert E.; Tsai, O. D.; Ulery, J.; Ullrich, T.; Underwood, D. G.; Van Buren, G.; van Nieuwenhuizen, G.; Vanfossen, J. A., Jr.; Varma, R.; Vasconcelos, G. M. S.; Vasiliev, A. N.; Videbaek, F.; Vigdor, S. E.; Viyogi, Y. P.; Vokal, S.; Voloshin, S. A.; Wada, M.

2010-01-01T23:59:59.000Z

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221

Azimuthally sensitive hanbury brown-twiss interferometry in Au + Au collisions sqrt S sub NN = 200 GeV  

SciTech Connect

We present the results of a systematic study of the shape of the pion distribution in coordinate space at freeze-out in Au+Au collisions at RHIC using two-pion Hanbury Brown-Twiss (HBT) interferometry. Oscillations of the extracted HBT radii vs. emission angle indicate sources elongated perpendicular to the reaction plane. The results indicate that the pressure and expansion time of the collision system are not sufficient to completely quench its initial shape.

Adams, J.; Adler, C.; Aggarwal, M.M.; Ahammed, Z.; Amonett, J.; Anderson, B.D.; Arkhipkin, D.; Averichev, G.S.; Badyal, S.K.; Balewski, J.; Barannikova, O.; Barnby, L.S.; Baudot, J.; Bekele, S.; Belaga, V.V.; Bellwied, R.; Berger, J.; Bezverkhny, B.I.; Bhardwaj, S.; Bhati, A.K.; Bichsel, H.; Billmeier, A.; Bland, L.C.; Blyth, C.O.; Bonner, B.E.; Botje, M.; Boucham, A.; Brandin, A.; Bravar, A.; Cadman, R.V.; Cai, X.Z.; Caines, H.; Calderon de la Barca Sanchez, M.; Carroll, J.; Castillo, J.; Cebra, D.; Chaloupka, P.; Chattopadhyay, S.; Chen, H.F.; Chen, Y.; Chernenko, S.P.; Cherney, M.; Chikanian, A.; Christie, W.; Coffin, J.P.; Cormier, T.M.; Cramer, J.G.; Crawford, H.J.; Das, D.; Das, S.; Derevschikov, A.A.; Didenko, L.; Dietel, T.; Dong, W.J.; Dong, X.; Draper, J.E.; Du, F.; Dubey, A.K.; Dunin, V.B.; Dunlop, J.C.; Dutta Majumdar, M.R.; Eckardt, V.; Efimov, L.G.; Emelianov, V.; Engelage, J.; Eppley, G.; Erazmus, B.; Estienne, M.; Fachini, P.; Faine, V.; Faivre, J.; Fatemi, R.; Filimonov, K.; Filip, P.; Finch, E.; Fisyak, Y.; Flierl, D.; Foley, K.J.; Fu, J.; Gagliardi, C.A.; Gagunashvili, N.; Gans, J.; Gaudichet, L.; Geurts, F.; Ghazikhanian, V.; Ghosh, P.; Gonzalez, J.E.; Grachov, O.; Grebenyuk, O.; Gronstal, S.; Grosnick, D.; Guertin, S.M.; Gupta, A.; Gutierrez, T.D.; Hallman, T.J.; Hamed, A.; Hardtke, D.; Harris, J.W.; Heinz, M.; Henry, T.W.; Heppelmann, S.; Hippolyte, B.; Hirsch, A.; Hjort, E.; Hoffmann, G.W.; Horsley, M.; Huang, H.Z.; Huang, L.S.; Hughes, E.; Humanic, T.J.; Igo, G.; Ishihara, A.; Jacobs, P.; Jacobs, W.W.; Janik, M.; Jiang, H.; Johnson, I.; Jones, P.G.; Judd, E.G.; Kabana, S.; Kaplan, M.; Keane, D.; Khodyrev, V.Yu.; Kiryluk, J.; Kisiel, A.; Klay, J.; Klein, S.R.; Klyachko, A.; Koetke, D.D.; Kollegger, T.; Kopytine, M.; Kotchenda, L.; Kovalenko, A.D.; Kramer, M.; Kravtsov, V.I.; Kravtsov, P.; Krueger, K.; Kuhn, C.; Kulikov, A.I.; Kumar, A.; Kunde, G.J.; Kunz, C.L.; Kutuev, R.Kh.; Kuznetsov, A.A.; Lamont, M.A.C.; et al.

2004-06-30T23:59:59.000Z

222

Measurements of heavy-flavour production and azimuthal anisotropy in Pb--Pb collisions with the ALICE detector  

E-Print Network (OSTI)

Hadrons containing heavy quarks, i.e. charm or beauty, are unique probes of the properties of the hot and dense QCD medium produced in heavy-ion collisions. Due to their large masses, heavy quarks are produced at the initial stage of the collision, almost exclusively via hard partonic scattering processes. Therefore, they are expected to experience the full collision history propagating through the QCD medium losing energy via elastic and inelastic collisions with the medium constituents. The ALICE collaboration has measured the production of open heavy-flavour hadrons via their hadronic and semi-electronic decays at mid-rapidity and in the semi-muonic decay channel at \\mbox{forward rapidity} in pp, p--Pb and Pb--Pb collisions. In this talk the latest results on the open \\mbox{heavy-flavour nuclear modification factor, $R_\\mathrm{AA}$, and elliptic flow, $v_{2}$, are presented}.

Andrea Dubla; for the ALICE Collaboration

2014-10-17T23:59:59.000Z

223

Transition from in-plane to out-of-plane azimuthal enhancement in Au+Au collisions  

E-Print Network (OSTI)

A 553 (1993) 739c. [46] P. Danielewicz and G. Odyniec, Phys.247 (1990) 233. [50] P. Danielewicz, discussion during INT-94-3, Seattle. [51] P. Danielewicz and Q. Pan, Phys. Rev. C

2000-01-01T23:59:59.000Z

224

An Evaluation of the Carbon Sequestration Potential of the Cambro-Ordovician Strata of the Illinois and Michigan Basins: Part 1: Evaluation of Phase 2 CO{sub 2} Injection Testing in the Deep Saline Gunter Sandstone Reservoir (Cambro-Ordovician Knox Group), Marvin Blan No. 1 Hancock County, Kentucky Part 2: Time-lapse Three-Dimensional Vertical Seismic Profile (3D-VSP) of Sequestration Target Interval with Injected Fluids  

SciTech Connect

Part 1 of this report focuses on results of the western Kentucky carbon storage test, and provides a basis for evaluating injection and storage of supercritical CO{sub 2} in Cambro-Ordovician carbonate reservoirs throughout the U.S. Midcontinent. This test demonstrated that the Cambro- Ordovician Knox Group, including the Beekmantown Dolomite, Gunter Sandstone, and Copper Ridge Dolomite in stratigraphic succession from shallowest to deepest, had reservoir properties suitable for supercritical CO{sub 2} storage in a deep saline reservoir hosted in carbonate rocks, and that strata with properties sufficient for long-term confinement of supercritical CO{sub 2} were present in the deep subsurface. Injection testing with brine and CO{sub 2} was completed in two phases. The first phase, a joint project by the Kentucky Geological Survey and the Western Kentucky Carbon Storage Foundation, drilled the Marvin Blan No. 1 carbon storage research well and tested the entire Knox Group section in the open borehole � including the Beekmantown Dolomite, Gunter Sandstone, and Copper Ridge Dolomite � at 1152�2255 m, below casing cemented at 1116 m. During Phase 1 injection testing, most of the 297 tonnes of supercritical CO{sub 2} was displaced into porous and permeable sections of the lowermost Beekmantown below 1463 m and Gunter. The wellbore was then temporarily abandoned with a retrievable bridge plug in casing at 1105 m and two downhole pressure-temperature monitoring gauges below the bridge plug pending subsequent testing. Pressure and temperature data were recorded every minute for slightly more than a year, providing a unique record of subsurface reservoir conditions in the Knox. In contrast, Phase 2 testing, this study, tested a mechanically-isolated dolomitic-sandstone interval in the Gunter. Operations in the Phase 2 testing program commenced with retrieval of the bridge plug and long-term pressure gauges, followed by mechanical isolation of the Gunter by plugging the wellbore with cement below the injection zone at 1605.7 m, then cementing a section of a 14-cm casing at 1470.4�1535.6. The resultant 70.1-m test interval at 1535.6�1605.7 m included nearly all of the Gunter sandstone facies. During the Phase 2 injection, 333 tonnes of CO{sub 2} were injected into the thick, lower sand section in the sandy member of the Gunter. Following the completion of testing, the injection zone below casing at 1116 m in the Marvin Blan No. 1 well, and wellbore below 305 m was permanently abandoned with cement plugs and the wellsite reclaimed. The range of most-likely storage capacities found in the Knox in the Marvin Blan No. 1 is 1000 tonnes per surface hectare in the Phase 2 Gunter interval to 8685 tonnes per surface hectare if the entire Knox section were available including the fractured interval near the base of the Copper Ridge. By itself the Gunter lacks sufficient reservoir volume to be considered for CO{sub 2} storage, although it may provide up to 18% of the reservoir volume available in the Knox. Regional extrapolation of CO{sub 2} storage potential based on the results of a single well test can be problematic, although indirect evidence of porosity and permeability can be demonstrated in the form of active saltwater-disposal wells injecting into the Knox. The western Kentucky region suitable for CO{sub 2} storage in the Knox is limited updip, to the east and south, by the depth at which the base of the Maquoketa shale lies above the depth required to ensure storage of CO{sub 2} in its supercritical state and the deepest a commercial well might be drilled for CO{sub 2} storage. The resulting prospective region has an area of approximately 15,600 km{sup 2}, beyond which it is unlikely that suitable Knox reservoirs may be developed. Faults in the subsurface, which serve as conduits for CO{sub 2} migration and compromise sealing strata, may mitigate the area with Knox reservoirs suitable for CO{sub 2} storage. The results of the injection tes

Richard Bowersox; John Hickman; Hannes Leetaru

2012-12-01T23:59:59.000Z

225

The INTERVAL Trial to determine whether intervals between blood donations can be safely and acceptably decreased to optimise blood supply: study protocol for a randomised controlled trial  

E-Print Network (OSTI)

, and reproducibility). J Orthop Sci 2011, 16:7–13. 20. Hirsch JD, Lee SJ, Terkeltaub R, Khanna D, Singh J, Sarkin A, Harvey J, Kavanaugh A: Evaluation of an instrument assessing influence of gout on health-related quality of life. J Rheumatol 2008, 35:2406–2414. 21... Sci 2011, 16:7–13. 20. Hirsch JD, Lee SJ, Terkeltaub R, Khanna D, Singh J, Sarkin A, Harvey J, Kavanaugh A: Evaluation of an instrument assessing influence of gout on health-related quality of life. J Rheumatol 2008, 35...

Moore, Carmel; Sambrook, Jennifer; Walker, Matthew; Tolkien, Zoe; Kaptoge, Stephen; Allen, David; Mehenny, Susan; Mant, Jonathan; Di Angelantonio, Emanuele; Thompson, Simon G.; Ouwehand, Willem; Roberts, David J.; Danesh, John

2014-09-17T23:59:59.000Z

226

Performance of a multi-tube, large-area Each source, shown in Fig. 2, consisted of a helicon source 2" diam tube, a helical antenna of azimuthal  

E-Print Network (OSTI)

plasma into a "magnetic bucket," or processing chamber covered with a permanent magnet array to provide and field I coil still did not produce helicon discharges. These were ICPs (Inductively Coupled Plas- Fig. 8

Chen, Francis F.

227

GEOPHYSICS, VOL. 65, NO. 1 (JANUARY-FEBRUARY 2000); P. 232246, 11 FIGS., 2 TABLES. Inversion of azimuthally dependent NMO velocity in transversely  

E-Print Network (OSTI)

) is a common anisotropic model of the subsurface typical for massive shale formations or thin-bed sedimentary with a tilted symmetry axis (TTI) describes dipping TI lay- ers (such as tilted shale beds near salt domes examine the propagation of errors in observed moveout velocities into estimated values of the anisotropic

Tsvankin, Ilya

228

Identified particle production, azimuthal anisotropy, and interferometry measurements in Au plus Au collisions at root s(NN)=9.2 GeV  

E-Print Network (OSTI)

. Vanfossen Jr.,18 R. Varma,14 G. M. S. Vasconcelos,7 A. N. Vasiliev,32 F. Videbaek,3 Y. P. Viyogi,47 S. Vokal,17 S. A. Voloshin,50 M. Wada,43 M. Walker,22 F. Wang,33 G. Wang,6 H. Wang,24 J. S. Wang,20 Q. Wang,33 X. Wang,44 X. L. Wang,38 Y. Wang,44 G. Webb...

Abelev, B. I.; Aggarwal, M. M.; Ahammed, Z.; Alakhverdyants, A. V.; Anderson, B. D.; Arkhipkin, D.; Averichev, G. S.; Balewski, J.; Barannikova, O.; Barnby, L. S.; Baumgart, S.; Beavis, D. R.; Bellwied, R.; Benedosso, F.; Betancourt, M. J.; Betts, R. R.; Bhasin, A.; Bhati, A. K.; Bichsel, H.; Bielcik, J.; Bielcikova, J.; Biritz, B.; Bland, L. C.; Bnzarov, I.; Bonner, B. E.; Bouchet, J.; Braidot, E.; Brandin, A. V.; Bridgeman, A.; Bruna, E.; Bueltmann, S.; Burton, T. P.; Cai, X. Z.; Caines, H.; Sanchez, M. Calderon de la Barca; Catu, O.; Cebra, D.; Cendejas, R.; Cervantes, M. C.; Chajecki, Z.; Chaloupka, P.; Chattopadhyay, S.; Chen, H. F.; Chen, J. H.; Chen, J. Y.; Cheng, J.; Cherney, M.; Chikanian, A.; Choi, K. E.; Christie, W.; Chung, P.; Clarke, R. F.; Codrington, M. J. M.; Corliss, R.; Cramer, J. G.; Crawford, H. J.; Das, D.; Dash, S.; De Silva, L. C.; Debbe, R. R.; Dedovich, T. G.; DePhillips, M.; Derevschikov, A. A.; de Souza, R. Derradi; Didenko, L.; Djawotho, P.; Dogra, S. M.; Dong, X.; Drachenberg, J. L.; Draper, J. E.; Dunlop, J. C.; Mazumdar, M. R. Dutta; Efimov, L. G.; Elhalhuli, E.; Elnimr, M.; Engelage, J.; Eppley, G.; Erazmus, B.; Estienne, M.; Eun, L.; Fachini, P.; Fatemi, R.; Fedorisin, J.; Fersch, R. G.; Filip, P.; Finch, E.; Fine, V.; Fisyak, Y.; Gagliardi, Carl A.; Gangadharan, D. R.; Ganti, M. S.; Garcia-Solis, E. J.; Geromitsos, A.; Geurts, F.; Ghazikhanian, V.; Ghosh, P.; Gorbunov, Y. N.; Gordon, A.; Grebenyuk, O.; Grosnick, D.; Grube, B.; Guertin, S. M.; Gupta, A.; Gupta, N.; Guryn, W.; Haag, B.; Hallman, T. J.; Hamed, A.; Han, L. -X; Harris, J. W.; Hays-Wehle, J. P.; Heinz, M.; Heppelmann, S.; Hirsch, A.; Hjort, E.; Hoffman, A. M.; Hoffmann, G. W.; Hofman, D. J.; Hollis, R. S.; Huang, H. Z.; Humanic, T. J.; Huo, L.; Igo, G.; Iordanova, A.; Jacobs, P.; Jacobs, W. W.; Jakl, P.; Jena, C.; Jin, F.; Jones, C. L.; Jones, P. G.; Joseph, J.; Judd, E. G.; Kabana, S.; Kajimoto, K.; Kang, K.; Kapitan, J.; Kauder, K.; Keane, D.; Kechechyan, A.; Kettler, D.; Khodyrev, V. Yu; Kikola, D. P.; Kiryluk, J.; Kisiel, A.; Klein, S. R.; Knospe, A. G.; Kocoloski, A.; Koetke, D. D.; Kollegger, T.; Konzer, J.; Kopytine, M.; Koralt, I.; Korsch, W.; Kotchenda, L.; Kouchpil, V.; Kravtsov, P.; Kravtsov, V. I.; Krueger, K.; Krus, M.; Kumar, L.; Kurnadi, P.; Lamont, M. A. C.; Landgraf, J. M.; LaPointe, S.; Lauret, J.; Lebedev, A.; Lednicky, R.; Lee, C-H; Lee, J. H.; Leight, W.; LeVine, M. J.; Li, C.; Li, N.; Li, Y.; Li, Z.; Lin, G.; Lin, X.; Lindenbaum, S. J.; Lisa, M. A.; Liu, F.; Liu, H.; Liu, J.; Ljubicic, T.; Llope, W. J.; Longacre, R. S.; Love, W. A.; Lu, Y.; Ludlam, T.; Ma, G. L.; Ma, Y. G.; Mahapatra, D. P.; Majka, R.; Mall, O. I.; Mangotra, L. K.; Manweiler, R.; Margetis, S.; Markert, C.; Masui, H.; Matis, H. S.; Matulenko, Yu A.; McDonald, D.; McShane, T. S.; Meschanin, A.; Milner, R.; Minaev, N. G.; Mioduszewski, Saskia; Mischke, A.; Mitrovski, M. K.; Mohanty, B.; Morozov, D. A.; Munhoz, M. G.; Nandi, B. K.; Nattrass, C.; Nayak, T. K.; Nelson, J. M.; Netrakanti, P. K.; Ng, M. J.; Nogach, L. V.; Nurushev, S. B.; Odyniec, G.; Ogawa, A.; Okada, H.; Okorokov, V.; Olson, D.; Pachr, M.; Page, B. S.; Pal, S. K.; Pandit, Y.; Panebratsev, Y.; Pawlak, T.; Peitzmann, T.; Perevoztchikov, V.; Perkins, C.; Peryt, W.; Phatak, S. C.; Pile, P.; Planinic, M.; Ploskon, M. A.; Pluta, J.; Plyku, D.; Poljak, N.; Poskanzer, A. M.; Potukuchi, B. V. K. S.; Prindle, D.; Pruneau, C.; Pruthi, N. K.; Pujahari, P. R.; Putschke, J.; Raniwala, R.; Raniwala, S.; Ray, R. L.; Redwine, R.; Reed, R.; Rehberg, J. M.; Ridiger, A.; Ritter, H. G.; Roberts, J. B.; Rogachevskiy, O. V.; Romero, J. L.; Rose, A.; Roy, C.; Ruan, L.; Russcher, M. J.; Sahoo, R.; Sakai, S.; Sakrejda, I.; Sakuma, T.; Salur, S.; Sandweiss, J.; Schambach, J.; Scharenberg, R. P.; Schmitz, N.; Schuster, T. R.; Seele, J.; Seger, J.; Selyuzhenkov, I.; Seyboth, P.; Shahaliev, E.; Shao, M.; Sharma, M.; Shi, S. S.; Sichtermann, E. P.; Simon, F.; Singaraju, R. N.; Skoby, M. J.; Smirnov, N.; Sorensen, P.; Sowinski, J.; Spinka, H. M.; Srivastava, B.; Stanislaus, T. D. S.; Staszak, D.; Stephans, G. S. F.; Stock, R.; Strikhanov, M.; Stringfellow, B.; Suaide, A. A. P.; Suarez, M. C.; Subba, N. L.; Sumbera, M.; Sun, X. M.; Sun, Y.; Sun, Z.; Surrow, B.; Symons, T. J. M.; de Toledo, A. Szanto; Takahashi, J.; Tang, A. H.; Tang, Z.; Tarini, L. H.; Tarnowsky, T.; Thein, D.; Thomas, J. H.; Tian, J.; Timmins, A. R.; Timoshenko, S.; Tlusty, D.; Tokarev, M.; Trainor, T. A.; Tram, V. N.; Trentalange, S.; Tribble, Robert E.; Tsai, O. D.; Ulery, J.; Ullrich, T.; Underwood, D. G.; Van Buren, G.; van Nieuwenhuizen, G.; Vanfossen, J. A., Jr.; Varma, R.; Vasconcelos, G. M. S.; Vasiliev, A. N.; Videbaek, F.; Viyogi, Y. P.; Vokal, S.; Voloshin, S. A.; Wada, M.; Walker, M.; Wang, F.

2010-01-01T23:59:59.000Z

229

Azimuthal di-hadron correlations in d plus Au and Au plus Au collisions at root s(NN)=200 GeV measured at the STAR detector  

E-Print Network (OSTI)

. Vanfossen Jr.,19 R. Varma,14 G. M. S. Vasconcelos,7 A. N. Vasiliev,33 F. Videbaek,3 Y. P. Viyogi,48 S. Vokal,18 S. A. Voloshin,51 M. Wada,44 M. Walker,23 F. Wang,34 G. Wang,6 H. Wang,25 J. S. Wang,21 Q. Wang,34 X. L. Wang,39 Y. Wang,45 G. Webb,20 J. C...

Aggarwal, M. M.; Ahammed, Z.; Alakhverdyants, A. V.; Alekseev, I.; Alford, J.; Anderson, B. D.; Arkhipkin, D.; Averichev, G. S.; Balewski, J.; Barnby, L. S.; Baumgart, S.; Beavis, D. R.; Bellwied, R.; Betancourt, M. J.; Betts, R. R.; Bhasin, A.; Bhati, A. K.; Bichsel, H.; Bielcik, J.; Bielcikova, J.; Biritz, B.; Bland, L. C.; Bonner, B. E.; Bouchet, J.; Braidot, E.; Brandin, A. V.; Bridgeman, A.; Bruna, E.; Bueltmann, S.; Bunzarov, I.; Burton, T. P.; Cai, X. Z.; Caines, H.; Sanchez, M. Calderon de la Barca; Catu, O.; Cebra, D.; Cendejas, R.; Cervantes, M. C.; Chajecki, Z.; Chaloupka, P.; Chattopadhyay, S.; Chen, H. F.; Chen, J. H.; Chen, J. Y.; Cheng, J.; Cherney, M.; Chikanian, A.; Choi, K. E.; Christie, W.; Chung, P.; Clarke, R. F.; Codrington, M. J. M.; Corliss, R.; Cramer, J. G.; Crawford, H. J.; Das, D.; Dash, S.; Leyva, A. Davila; De Silva, L. C.; Debbe, R. R.; Dedovich, T. G.; Derevschikov, A. A.; de Souza, R. Derradi; Didenko, L.; Djawotho, P.; Dogra, S. M.; Dong, X.; Drachenberg, J. L.; Draper, J. E.; Dunlop, J. C.; Mazumdar, M. R. Dutta; Efimov, L. G.; Elhalhuli, E.; Elnimr, M.; Engelage, J.; Eppley, G.; Erazmus, B.; Estienne, M.; Eun, L.; Evdokimov, O.; Fachini, P.; Fatemi, R.; Fedorisin, J.; Fersch, R. G.; Filip, P.; Finch, E.; Fine, V.; Fisyak, Y.; Gagliardi, Carl A.; Gangadharan, D. R.; Ganti, M. S.; Garcia-Solis, E. J.; Geromitsos, A.; Geurts, F.; Ghazikhanian, V.; Ghosh, P.; Gorbunov, Y. N.; Gordon, A.; Grebenyuk, O.; Grosnick, D.; Guertin, S. M.; Gupta, A.; Gupta, N.; Guryn, W.; Haag, B.; Hamed, A.; Han, L. -X; Harris, J. W.; Hays-Wehle, J. P.; Heinz, M.; Heppelmann, S.; Hirsch, A.; Hjort, E.; Hoffman, A. M.; Hoffmann, G. W.; Hofman, D. J.; Horner, M. J.; Huang, B.; Huang, H. Z.; Humanic, T. J.; Huo, L.; Igo, G.; Jacobs, P.; Jacobs, W. W.; Jena, C.; Jin, F.; Jones, C. L.; Jones, P. G.; Joseph, J.; Judd, E. G.; Kabana, S.; Kajimoto, K.; Kang, K.; Kapitan, J.; Kauder, K.; Keane, D.; Kechechyan, A.; Kettler, D.; Kikola, D. P.; Kiryluk, J.; Kisiel, A.; Klein, S. R.; Knospe, A. G.; Kocoloski, A.; Koetke, D. D.; Kollegger, T.; Konzer, J.; Koralt, I.; Koroleva, L.; Korsch, W.; Kotchenda, L.; Kouchpil, V.; Kravtsov, P.; Krueger, K.; Krus, M.; Kumar, L.; Kurnadi, P.; Lamont, M. A. C.; Landgraf, J. M.; LaPointe, S.; Lauret, J.; Lebedev, A.; Lednicky, R.; Lee, C. -H; Lee, J. H.; Leight, W.; LeVine, M. J.; Li, C.; Li, L.; Li, N.; Li, W.; Li, X.; Li, X.; Li, Y.; Li, Z. M.; Lin, G.; Lindenbaum, S. J.; Lisa, M. A.; Liu, F.; Liu, H.; Liu, J.; Ljubicic, T.; Llope, W. J.; Longacre, R. S.; Love, W. A.; Lu, Y.; Luo, X.; Ma, G. L.; Ma, Y. G.; Mahapatra, D. P.; Majka, R.; Mall, O. I.; Mangotra, L. K.; Manweiler, R.; Margetis, S.; Markert, C.; Masui, H.; Matis, H. S.; Matulenko, Yu A.; McDonald, D.; McShane, T. S.; Meschanin, A.; Milner, R.; Minaev, N. G.; Mioduszewski, Saskia; Mischke, A.; Mitrovski, M. K.; Mohanty, B.; Mondal, M. M.; Morozov, B.; Morozov, D. A.; Munhoz, M. G.; Nandi, B. K.; Nattrass, C.; Nayak, T. K.; Nelson, J. M.; Netrakanti, P. K.; Ng, M. J.; Nogach, L. V.; Nurushev, S. B.; Odyniec, G.; Ogawa, A.; Okorokov, V.; Oldag, E. W.; Olson, D.; Pachr, M.; Page, B. S.; Pal, S. K.; Pandit, Y.; Panebratsev, Y.; Pawlak, T.; Peitzmann, T.; Perevoztchikov, V.; Perkins, C.; Peryt, W.; Phatak, S. C.; Pile, P.; Planinic, M.; Ploskon, M. A.; Pluta, J.; Plyku, D.; Poljak, N.; Poskanzer, A. M.; Potukuchi, B. V. K. S.; Powell, C. B.; Prindle, D.; Pruneau, C.; Pruthi, N. K.; Pujahari, P. R.; Putschke, J.; Raniwala, R.; Raniwala, S.; Ray, R. L.; Redwine, R.; Reed, R.; Ritter, H. G.; Roberts, J. B.; Rogachevskiy, O. V.; Romero, J. L.; Rose, A.; Roy, C.; Ruan, L.; Sahoo, R.; Sakai, S.; Sakrejda, I.; Sakuma, T.; Salur, S.; Sandweiss, J.; Sangaline, E.; Schambach, J.; Scharenberg, R. P.; Schmitz, N.; Schuster, T. R.; Seele, J.; Seger, J.; Selyuzhenkov, I.; Seyboth, P.; Shahaliev, E.; Shao, M.; Sharma, M.; Shi, S. S.; Sichtermann, E. P.; Simon, F.; Singaraju, R. N.; Skoby, M. J.; Smirnov, N.; Sorensen, P.; Sowinski, J.; Spinka, H. M.; Srivastava, B.; Stanislaus, T. D. S.; Staszak, D.; Stevens, J. R.; Stock, R.; Strikhanov, M.; Stringfellow, B.; Suaide, A. A. P.; Suarez, M. C.; Subba, N. L.; Sumbera, M.; Sun, X. M.; Sun, Y.; Sun, Z.; Surrow, B.; Svirida, D. N.; Symons, T. J. M.; de Toledo, A. Szanto; Takahashi, J.; Tang, A. H.; Tang, Z.; Tarini, L. H.; Tarnowsky, T.; Thein, D.; Thomas, J. H.; Tian, J.; Timmins, A. R.; Timoshenko, S.; Tlusty, D.; Tokarev, M.; Trainor, T. A.; Tram, V. N.; Trentalange, S.; Tribble, Robert E.; Tsai, O. D.; Ulery, J.; Ullrich, T.; Underwood, D. G.; Van Buren, G.; van Leeuwen, M.; van Nieuwenhuizen, G.; Vanfossen, J. A., Jr.; Varma, R.; Vasconcelos, G. M. S.; Vasiliev, A. N.; Videbaek, F.; Viyogi, Y. P.; Vokal, S.; Voloshin, S. A.; Wada, M.; Walker, M.; Wang, F.; Wang, G.

2010-01-01T23:59:59.000Z

230

AIMR (Azimuth and Inclination Modeling in Realtime): A Method for Prediction of Dog-Leg Severity based on Mechanical Specific Energy  

E-Print Network (OSTI)

Since the 1980’s horizontal drilling has been a game-changing technology as it allowed the oil and gas industry to produce from reservoirs previously considered marginal or uneconomic. However, while it is considered a mature technology...

Noynaert, Samuel F

2013-08-13T23:59:59.000Z

231

GEOPHYSICS, VOL. 64, NO. 4 (JULY-AUGUST 1999); P. 11261138, 7 FIGS. Coarse-layer stripping of vertically variable azimuthal  

E-Print Network (OSTI)

of stress and hence for prescriptions of well drilling plans which mini- mize borehole stability problems cracks are sufficiently large and interconnected; and 3) its implications for preferred directions

Tsvankin, Ilya

232

ARM - Datastreams - 915rwpwindcon  

NLE Websites -- All DOE Office Websites (Extended Search)

rwpwindcon rwpwindcon Documentation Data Quality Plots Citation DOI: 10.5439/1025135 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Example 915rwpwindcon Archive Data Plot Example 915rwpwindcon Archive Data Plot Datastream : 915RWPWINDCON 915-MHz Radar Wind Profiler/RASS (RWP915): wind consensus data Active Dates 2001.03.27 - 2014.01.02 Measurement Categories Atmospheric State Originating Instrument Radar Wind Profiler (RWP) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Averaging interval min avgint ( time, power ) Azimuth of beam 0 deg azimuth0 ( power )

233

Converting 15-Minute Interval Electricity Load Data into Reduced Demand, Energy Reduction and Cash Flow  

E-Print Network (OSTI)

, store managers are intimidated. 5 So what are the solutions? • A data acquisition system. • Pro-active with alarming and demand-response. Is there staff to maintain and ensure a response? • Passive. Acquire the data and then evaluate and assess... is not required, this will prevent the requirement for additional costs of installing an OAT sensor at the building and potentially adding costs to the datalogger hardware or configuration. If possible, it is best to use and on-site OAT sensor. If a demand-response...

Herrin, D. G.

234

A Magnetizer for Studying Transient Processes in Magnets over a Wide Time Interval  

Science Journals Connector (OSTI)

The magnetizer is intended for studies of transient processes ... planar films. The main element of the magnetizer is a strip line consisting of thin ... using a removable longitudinal sence loop. The magnetizer ...

O. S. Kolotov; A. V. Matyunin; O. A. Mironets…

2004-11-01T23:59:59.000Z

235

CruzDB: software for annotation of genomic intervals with UCSC genome-browser database  

Science Journals Connector (OSTI)

......and remotely hosted datasets. We showcase the syntax...indicating a role of nuclear organization in their...a recent report that nuclear clustering of olfactory...receptor-induced changes in nuclear architecture influence...and remotely hosted datasets, as well as annotation......

Brent S. Pedersen; Ivana V. Yang; Subhajyoti De

2013-12-01T23:59:59.000Z

236

E-Print Network 3.0 - anaerobic interval training Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

Resources which provide more detailed infor- mation on anaerobic digesters are listed. Biogas... Technology Biomethane (biogas) is an alternative and renewable energy source...

237

E-Print Network 3.0 - acute anaerobic interval Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

Ecology 19 THE JOURNAL OF EXPERIMENTAL ZOOLOGY 213:405-416 (1980) Anaerobic Metabolism, Gas Exchange, and Acid-Base Summary: THE JOURNAL OF EXPERIMENTAL ZOOLOGY 213:405-416...

238

Locating regional seismic events with global optimization based on interval arithmetic  

Science Journals Connector (OSTI)

......connected to the Helsinki bulletin locations with mislocation vectors. The explosion sites form clear clustering at Estonia oil shale quarries, mines in Russian Karelia, the Siilinja rvi mine in Central Finland and deep seabed excavation works in Bothnian......

Matti Tarvainen; Timo Tiira; Eystein S. Husebye

1999-09-01T23:59:59.000Z

239

Registering coherent change detection products associated with large image sets and long capture intervals  

DOE Patents (OSTI)

A set of co-registered coherent change detection (CCD) products is produced from a set of temporally separated synthetic aperture radar (SAR) images of a target scene. A plurality of transformations are determined, which transformations are respectively for transforming a plurality of the SAR images to a predetermined image coordinate system. The transformations are used to create, from a set of CCD products produced from the set of SAR images, a corresponding set of co-registered CCD products.

Perkins, David Nikolaus; Gonzales, Antonio I

2014-04-08T23:59:59.000Z

240

Continuous training versus interval training in deep water running: health effects for obese women  

Science Journals Connector (OSTI)

Objectives To search intermittent and continous trainning (IT and CT, respectively) effects through deep water running for the control and prevention of excessive body fat accumulation and improvement of quality of life. Methods Experimental study composed by 30 women, aged between 34 to 58 years old, during 12 weeks, three sessions per week, 47 minutes each. Body composition, cardiorespiratory condition and Quality of Life by WHOQOL-Brief were considered. Student's and Wilcoxon's non parametric tests were applied at 5% significance level. Results With the only exception for social domain of quality of life, all investigated variables revealed improvement in both groups for IT in comparison to CT. Conclusion Deep water running contributes to body fat reduction, physical fitness evolution and improvement of WHOQOL-Brief domains, regardless of the trainning type conducted.

S.R. Pasetti; A. Gonçalves; C.R. Padovani

2012-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" from the National Library of EnergyBeta (NLEBeta).
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241

From Interval Methods of Representing Uncertainty To A General Description of Uncertainty  

E-Print Network (OSTI)

hunguyen@nmsu.edu Abstract Measurements do not result in an exact value of the measured quantity; even of the measured quantity. Traditionally, in science and engineering, this uncertainty is character­ ized measurements. Some of this knowl­ edge comes not from measurements but from the ex­ pertise of scientists

Kreinovich, Vladik

242

Estimating Variance under Interval and Fuzzy Uncertainty: Case of Hierarchical Estimation  

E-Print Network (OSTI)

. In practice, these values come either from measurements or from expert estimates. In both case, we get only for these characteristics. It is desirable to estimate the accuracy of these approximations. Case of measurement uncertainty. Measurements are never 100% accurate. As a result, the result x of the measurement is, in general, different

Kreinovich, Vladik

243

Statistical Genetic Interval-Valued Type-2 Fuzzy System and its Application.  

E-Print Network (OSTI)

??In recent years, the type-2 fuzzy sets theory has been used to model and minimize the effects of uncertainties in rule-base fuzzy logic system. In… (more)

Qiu, Yu

2006-01-01T23:59:59.000Z

244

screened intervals (415421 m and 689695 m; Figure 2) in the observations wells will be useful  

E-Print Network (OSTI)

studies.We thank Bayshore Concrete and Ray Otten of the Sustainable Technology Park for access Chesapeake Bay Crater,522 pp.,Springer-Verlag, New York. Rieke,H.H.,and G.V.Chilingarian (1974),Compaction.Edwards,and Jean M. Self-Trail,USGS,Reston,Va.; and Roger H.Morin, USGS,Lakewood,Colo. For additional information

Sprintall, Janet

245

jfpe_425 1220..1233 BOOTSTRAP CONFIDENCE INTERVALS FOR THE KINETIC  

E-Print Network (OSTI)

.073 m) was heated in a steam retort at 126.7C. Antho- cyanin retention was measured by high bands, allows more accurate process design and cost-savings, potentially leading to higher-quality design and cost-savings, potentially leading to higher- quality nutraceutical products. INTRODUCTION

246

The maximum time interval of time-lapse photography for monitoring construction operations  

E-Print Network (OSTI)

, the use of CCTV systems has been diversified. The cameras, today, not only provide views, but also perceive objects, and, therefore, some traffic cameras can monitor the speed and detect speeding cars (Norris and Armstrong 1998). Besides, some more...

Choi, Ji Won

2005-11-01T23:59:59.000Z

247

Substantial narrowing of the Niemann–Pick C candidate interval by yeast artificial chromosome?complementation  

Science Journals Connector (OSTI)

...Christiano Cummings Jill A. Morris Stacie K. Loftus Dana Zhang Katherine G. Coleman Adele M. Cooney Marcy E. Comly Laura Fandino...Genet 6 : 59 – 68 , 9002671 . 21 Davison R L O’Malley K A Wheeler T B ( 1976 ) Somatic Cell Genet 3 : 271 – 280 . 22 Srivastava...

Jessie Z. Gu; Eugene D. Carstea; Christiano Cummings; Jill A. Morris; Stacie K. Loftus; Dana Zhang; Katherine G. Coleman; Adele M. Cooney; Marcy E. Comly; Laura Fandino; Calvin Roff; Danilo A. Tagle; William J. Pavan; Peter G. Pentchev; Melissa A. Rosenfeld

1997-01-01T23:59:59.000Z

248

Computing confidence intervals on solution costs for stochastic grid generation expansion problems.  

SciTech Connect

A range of core operations and planning problems for the national electrical grid are naturally formulated and solved as stochastic programming problems, which minimize expected costs subject to a range of uncertain outcomes relating to, for example, uncertain demands or generator output. A critical decision issue relating to such stochastic programs is: How many scenarios are required to ensure a specific error bound on the solution cost? Scenarios are the key mechanism used to sample from the uncertainty space, and the number of scenarios drives computational difficultly. We explore this question in the context of a long-term grid generation expansion problem, using a bounding procedure introduced by Mak, Morton, and Wood. We discuss experimental results using problem formulations independently minimizing expected cost and down-side risk. Our results indicate that we can use a surprisingly small number of scenarios to yield tight error bounds in the case of expected cost minimization, which has key practical implications. In contrast, error bounds in the case of risk minimization are significantly larger, suggesting more research is required in this area in order to achieve rigorous solutions for decision makers.

Woodruff, David L..; Watson, Jean-Paul

2010-12-01T23:59:59.000Z

249

STATISTICA INFERENZIALE SHEDA N. 2 INTERVALLI DI CONFIDENZA PER IL VALORE ATTESO E LA FREQUENZA  

E-Print Network (OSTI)

dati campionari. In questa scheda costruiremo un intervallo nel quale ci aspettiamo stia il parametro

Rogantin, Maria Piera

250

Predictive multiple sampling algorithm with overlapping integration intervals for linear wide dynamic range integrating image sensors  

E-Print Network (OSTI)

Machine vision systems are used in a wide range of applications such as security, automated quality control and intelligent transportation systems. Several of these systems need to extract information from natural scenes ...

Acosta Serafini, Pablo M. (Pablo Manuel), 1971-

2004-01-01T23:59:59.000Z

251

Confidence Intervals Estimation in the Identification of Electromechanical Modes from Ambient Noise  

E-Print Network (OSTI)

from ambient data resulting from random load switching throughout the day in power systems effectiveness in reducing the number of trials, which would be beneficial for on-line power system monitoring-- Power system oscillations, modal analysis, power system monitoring, system identification, prediction

Cañizares, Claudio A.

252

Semi-Heuristic Target-Based Fuzzy Decision Procedures: Towards a New Interval Justification  

E-Print Network (OSTI)

by the values of several quantities. For example, when we buy a car, we are interested in its cost, its energy], [11], [14]) deal with the problems in which the quality of each possible alternative is characterized range of values. Sometimes, there is only one alternative that satisfies all these requirements

Ward, Karen

253

Interval-valued Fuzzy-Rough Feature Selection and Application for Handling Missing Values in Datasets  

E-Print Network (OSTI)

, UK {rkj,qqs}@aber.ac.uk Abstract One of the many successful applications of rough set theory has been to the area of feature selection. The rough set ideol- ogy of using only the supplied data and no other information has many benefits, where most other methods require sup- plementary knowledge. Fuzzy-rough set

Lucas, Simon M.

254

Interval-Based Model-Predictive Control for Uncertain Dynamic Systems with Actuator Constraints  

E-Print Network (OSTI)

and for the control of the thermal behavior of high-temperature fuel cell stacks. This application scenario uncertainty due to limited measurement facilities in the interior of the fuel cell stack can be expressed performance by the minimization of suitable cost functions in real time. These criteria typically take

Appelrath, Hans-Jürgen

255

Towards Combining Probabilistic, Interval, Fuzzy Uncertainty, and Constraints: An Example Using the Inverse Problem in Geophysics  

E-Print Network (OSTI)

at a certain location is to actually drill a borehole and analyze the materials extracted. How­ ever actually drilling the boreholes: e.g., gravity and magnetic measurements, analyzing the travel century. The result was the discovery of many large relatively easy to locate resources such as the oil

Kreinovich, Vladik

256

Towards Combining Probabilistic, Interval, Fuzzy Uncertainty, and Constraints: An Example Using the Inverse Problem in Geophysics  

E-Print Network (OSTI)

at a certain location is to actually drill a borehole and analyze the materials extracted. How- ever actually drilling the boreholes: e.g., gravity and magnetic measurements, analyzing the travel century. The result was the discovery of many large relatively easy to locate resources such as the oil

Kreinovich, Vladik

257

Interval operations in rounding to nearest submitted for publication, February 2007  

E-Print Network (OSTI)

and finite c := fl(a b) the monotonicity (2) implies a b [c1, c2] where c1 := fl(fl(c - 2u|c|) - ) and c2 := fl(fl(c + 2u|c|) + ). (4) (Note that the above remains true if a b is replaced by any real y

Rump, Siegfried M.

258

Common variants at ten loci influence QT interval duration in the QTGEN Study  

E-Print Network (OSTI)

Hofman4,16, Susan R Heckbert9,12,17, Christopher J O'Donnell3,18,19, Andre´ G Uitterlinden4,8,16, Bruce M Psaty9,10,12,17,20, Thomas Lumley5,23, Martin G Larson3,7,23 & Bruno H Ch Stricker4,8,15,16,21,23 QT

de Bakker, Paul

259

A Fuzzy Formal Logic for Interval-valued Residuated Lattices B. Van Gasse  

E-Print Network (OSTI)

that this truth- functional approach, along with the residu- ation principle, has some consequences that seem truth values instead of only `true' and `false'. A wide range of such logics were introduced cases it may be preferable to work with graded truth values, e.g. for propositions like `a cat

Gent, Universiteit

260

Modernization Magnitude: An Interval Measure Applicable to Post- and Pre-Industrial Societies  

E-Print Network (OSTI)

to reflect. Qatar, and several other oil producing nations,X in oil producing countries such as Qatar and Bahrain. (NoTable 8. Oil producing countries such as Qatar and Bahrain

Denton, Trevor D.

2008-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

Principal Component Analysis for Interval-Valued Observations A. Douzal-Chouakria1  

E-Print Network (OSTI)

of the merits of some entity (e.g., wine quality) can be along the lines of 90 ± with = 5 when reasonably sure and = 10 when the uncertainty increases. Rather than uncertainty, in order to protect confidentialities

Boyer, Edmond

262

Case Studies in Using Whole Building Interval Data to Determine Annualized Electrical Savings  

E-Print Network (OSTI)

. Joint Solar Engineering Conference, 1995. Reddy, T.A., Claridge, D.E., 2000. Uncertainty of ?Measured? Energy Savings from Statistical Baseline Models. HVAC&R Research. ESL-IC-09-11-23 Proceedings of the Ninth International Conference...

Effinger, M.; Anthony, J.; Webster, L.

263

Analyzing and simulating the variability of solar irradiance and solar PV powerplants  

E-Print Network (OSTI)

tracking solar panel. 44and azimuth angles for solar panels were calculated for aannual azimuth for a solar panel, and can be combined with

Lave, Matthew S.

2012-01-01T23:59:59.000Z

264

SUBMITTED FOR PUBLICATION TO: IEEE COMPUTER, 2002, JANUARY 28, 2002 1 Interval Set Clustering of Web Users with  

E-Print Network (OSTI)

of Web Users with Rough K-means Pawan Lingras Chad West Abstract Data collection and analysis in web mining faces certain unique challenges. Due to a variety of reasons inherent in web browsing and web techniques in web mining need to accommodate such data. Fuzzy and rough sets provide the ability to deal

265

Calculation of probabilities of transfer, recurrence intervals, and positional indices for linear compartment models. Environmental Sciences Division Publication no. 1544  

SciTech Connect

Six indices are presented for linear compartment systems that quantify the probable pathways of matter or energy transfer, the likelihood of recurrence if the model contains feedback loops, and the number of steps (transfers) through the system. General examples are used to illustrate how these indices can simplify the comparison of complex systems or organisms in unrelated systems.

Carney, J.H.; DeAngelis, D.L.; Gardner, R.H.; Mankin, J.B.; Post, W.M.

1981-02-01T23:59:59.000Z

266

Energy Consumption Estimation for Room Air-conditioners Using Room Temperature Simulation with One-Minute Intervals  

E-Print Network (OSTI)

time can be known so that its energy consumption can be estimated accurately. In order to verify the simulation accuracy, an actual room equipped with a gas-engine heat pump (GHP) air-conditioning system is studied by both simulation and measurement...

Wang, F.; Yoshida, H.; Matsumoto, K.

2006-01-01T23:59:59.000Z

267

The Cane Creek clastic interval of the Pennsylvanian Paradox formation - an exciting new horizontal target; Part I: Regional Geology  

SciTech Connect

The Cane Creek is a fractured, abnormally pressured, self-sourcing reservoir, making it a good candidate for exploitation through horizontal technology. This concept was successfully applied to the Cane Creek in 1991 when Columbia Gas Development and Exxon Company USA, on an Enserch farmout, completed the Kane Springs Federal 27-1 for 914 BOPD. Since that time, two additional horizontal discoveries have potentialed for 1158 and 1325 BOPD, respectively. The Cane Creek was deposited in a partly restricted evaporitic environment in the Paradox basin during the Pennsylvanian. The Cane Creek consists of fifth-order shoaling-upward cycles within the transgressive to early highstand systems tracts. The reservoir comprises 20-30 ft of organic-rich, dolomitic siltstone and shale directly overlain and underlain by interbedded anhydrite, shale, and siltstone. In most areas, the Cane Creek is sealed above and below by halite, which maintains the abnormal pressure in the reservoir. Core information and reservoir engineering data indicate the Cane Creek produces from fracture porosity with minor contribution from the matrix. Initial fracture development may have occurred as a result of movement along basement-involved faults during the Pennsylvanian, followed by or coincident with salt mobilization from Pennsylvania-Jurassic. Hydrocarbon generation and overpressuring during maximum burial in the Late Cretaceous-early Tertiary created additional fractures or enhanced existing ones. The dominant fracture orientation is northeast-southwest to north-south, which is consistent with the regional stress regime during Late Cretaceous-early Tertiary.

Rawlins, D.M. (Exxon Company USA, Midland, TX (United States))

1993-08-01T23:59:59.000Z

268

Effect of Alfaprostol, Lasalocid and Once Daily Suckling on postpartum interval in Brahman and Brahman crossbred cattle  

E-Print Network (OSTI)

by age, breed and date of calving to one of 8 treatments (Table 1): 1) Control; 2) Lasalocid (Hoffmann-LaRoche, Inc. , Nutley, N. J. ); 3) Once daily suckling; 4) Alfaprostol (Hoffmann-LaRoche, Inc. , Nutley, N. J. ); 5) Lasalocid and once daily... by age, breed and date of calving to one of 8 treatments (Table 1): 1) Control; 2) Lasalocid (Hoffmann-LaRoche, Inc. , Nutley, N. J. ); 3) Once daily suckling; 4) Alfaprostol (Hoffmann-LaRoche, Inc. , Nutley, N. J. ); 5) Lasalocid and once daily...

Del Vecchio, Ronald Paul

2012-06-07T23:59:59.000Z

269

Dopamine or thyrotropin-releasing hormone effects on luteinizing hormone secretion in heifers and on the postpartum interval in cows  

E-Print Network (OSTI)

and Dr. D. W. Forrest for devoting many hours in the planning and critique of this manuscript. Appreciation is also extended to Dr. J. D. Williams and Dr. P. G. Harms for support and instruction as members of the authors graduate committee.... 6 + 0. 3 ng/ml, respectively). Carruthers and Hafs (5) observed that ovulation occurred on days )9. 7 and 21. 2, respectively, for suckled and nonsuckled dairy cows. Both frequency and amplitude of episodic LH peaks was reduced on days 7 and 14...

Lovin, Jeffrey Clay

2012-06-07T23:59:59.000Z

270

Interrelationship of endogenous and exogenous prostaglandins with uterine involution and postpartum interval in beef cows and heifers  

E-Print Network (OSTI)

versus C. 100 90 80 +I 70 60 e 50 +J 40 m 30 20 10 / / / / / 25 30 35 40 45 50 55 60 65 70 75 80 85 90 95 100 105 * Do not differ (p&, 05) Days postpartum Figure 6. Treatment effects on cumu1ative frequency of return to estrus... frequency of return to estrus in Hrangus cows. APP versus UP. 100 90 4J 70 60 o 50 40 E 30 20 10 / / / r , /~ I I / I / I / I / / I 30 35 40 45 50 55 60 65 70 75 80 85 90 95 100 105 * Differ at p&, 05 Days postpartum Treatment...

Tolleson, Douglas Ray

2012-06-07T23:59:59.000Z

271

A reliable and accurate calculation of excitation capacitance value for an induction generator based on interval computation technique  

Science Journals Connector (OSTI)

A squirrel cage induction generator (SCIG) offers many advantages for wind...C exct ) is very crucial for the selfexcitation and voltage build-up as well as volt...

Rajesh Kumar Thakur; Vivek Agarwal…

2011-11-01T23:59:59.000Z

272

Testing and interval estimation for two-sample survival comparisons with small sample sizes and unequal censoring  

Science Journals Connector (OSTI)

......CHSS model. Journal of Statistical Planning and Inference (2004) 126:535-551. Breslow NE . A generalized Kruskal-Wallis test for comparing K-samples subject to unequal patterns of censoring. Biometrika (1970) 57:579-594. Cox......

Rui Wang; Stephen W. Lagakos; Robert J. Gray

2010-10-01T23:59:59.000Z

273

The General, Linear Let a1 (x) , a2 (x) , . . . , an (x) be continuous functions defined on the interval  

E-Print Network (OSTI)

c1 and c2, u = c1u1+c2u2 is also a solution of this equation. · Suppose u1 and u2 are solutions c1 and c2, u = c1u1+c2u2 is a solution of the inhomogeneous equation Lu = r where r = c1r1 + c2r2

Lebovitz, Norman

274

Annual Precise Time and Time Interval (PTTI) Systems and Applications Meeting NEW IMPROVED SYSTEM FOR WWVB BROADCAST  

E-Print Network (OSTI)

by use of a binary coded decimal (BCD) format, allowing the reception of a time-of-day code. However The WWVB broadcast of the time-code signal has undergone no major changes in its communications protocol

275

Analysis of Cardiac Micro-Acceleration Signals for the Estimation of Systolic and Diastolic Time Intervals in Cardiac Resynchronization Therapy  

E-Print Network (OSTI)

error and coefficient stability. Models for mitral valve closing, aor- tic valve closing and opening, fitted between CMA features and echo timings, were eval- uated with their correlation coefficient, model instants showed satisfactory results, whereas the estimation of the opening instant of the mitral valve

Boyer, Edmond

276

Neutron Scattering at 25 Teslas: MagLab Completes Conical Bore...  

NLE Websites -- All DOE Office Websites (Extended Search)

central field with a unique conical warm bore with 30 degree opening angles suitable for neutron scattering experiments. Development and fabrication of this Conical Bore Resistive...

277

Combined microseismic and 4D to calibrate and confirm surface 3D azimuthal AVO/LMR predictions of completions performance and well production in the Horn River gas shales of NEBC  

Science Journals Connector (OSTI)

...core) and the geologic environment which describes the...limitations in resolution and impact of systematic and random...completeness estimation will impact the b-value. For...movies, is that repeated fracking of toe stages may have...fracture density caused by fracking and second the influence...

Bill Goodway; Dave Monk; Marco Perez; Greg Purdue; Paul Anderson; Andrew Iverson; Virginia Vera; David Cho

278

Measurements of Non-photonic Electron Production and Azimuthal Anisotropy in $\\sqrt {s_{NN}} = 39$, 62.4 and 200 GeV \\auau\\ Collisions from STAR at RHIC  

E-Print Network (OSTI)

During RHIC 2010 run, STAR has collected a large amount of minimum-bias, central and high $p_{T}$ trigger data in Au+Au collisions at $\\sqrt{s_{NN}} = 39$, 62.4 and 200 GeV with detector configuration for minimum photonic conversion background. In this article we report on a new high precision measurement of non-photonic electron mid-rapidity invariant yield, improved nuclear modification factor and $v_{2}$ in Au+Au collisions at $\\sqrt{s_{NN}} = 200$ GeV. We also present measurements of mid-rapidity invariant yield at $\\sqrt{s_{NN}} = 62.4$ and $v_{2}$ at $\\sqrt{s_{NN}} = 39$ and 62.4 GeV.

Mustafa Mustafa

2014-06-18T23:59:59.000Z

279

Measurement of the elliptic anisotropy of charged particles produced in PbPb collisions at ?sNN=2.76 TeV  

E-Print Network (OSTI)

The anisotropy of the azimuthal distributions of charged particles produced in [? over s[subscript NN

Bauer, Gerry P.

280

DESY05158 arXiv:hepph/0509107  

E-Print Network (OSTI)

-158 AZIMUTHAL DEPENDENCE IN DIFFRACTIVE PROCESSES a M. DIEHL Deutsches Elektronen-Synchroton DESY, 22603 Hamburg

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

Natural and Induced Fracture Diagnostics from 4-D VSP in low Permeability Gas Reservoirs  

SciTech Connect

Tight gas sand reservoirs generally contain thick gas-charged intervals that often have low porosity and very low permeability. Natural and induced fractures provide the only means of production. The objective of this work is to locate and characterize natural and induced fractures from analysis of scattered waves recorded on 4-D (time lapse) VSP data in order to optimize well placement and well spacing in these gas reservoirs. Using model data simulating the scattering of seismic energy from hydraulic fractures, we first show that it is possible to characterize the quality of fracturing based upon the amount of scattering. In addition, the picked arrival times of recorded microseismic events provide the velocity moveout for isolating the scattered energy on the 4-D VSP data. This concept is applied to a field dataset from the Jonah Field in Wyoming to characterize the quality of the induced hydraulic fractures. The time lapse (4D) VSP data from this field are imaged using a migration algorithm that utilizes shot travel time tables derived from the first breaks of the 3D VSPs and receiver travel time tables based on the microseismic arrival times and a regional velocity model. Four azimuthally varying shot tables are derived from picks of the first breaks of over 200 VSP records. We create images of the fracture planes through two of the hydraulically fractured wells in the field. The scattered energy shows correlation with the locations of the microseismic events. In addition, the azimuthal scattering is different from the azimuthal reflectivity of the reservoir, giving us more confidence that we have separated the scattered signal from simple formation reflectivity. Variation of the scattered energy along the image planes suggests variability in the quality of the fractures in three distinct zones.

Mark Willis; Daniel Burns; M. Nafi Toksoz

2008-09-30T23:59:59.000Z

282

The Coso EGS Project, recent developments (in International collaboration  

Open Energy Info (EERE)

Coso EGS Project, recent developments (in International collaboration Coso EGS Project, recent developments (in International collaboration for geothermal energy in the Americas) Jump to: navigation, search GEOTHERMAL ENERGYGeothermal Home Conference Proceedings: The Coso EGS Project, recent developments (in International collaboration for geothermal energy in the Americas) Details Activities (3) Areas (1) Regions (0) Abstract: A preliminary fracture/stress analysis was conducted for the recently drilled well 38C-9 as part of a continuing effort to characterize the stress state within the east flank of the Coso geothermal field. Electric Micro Imager (EMI) data were analyzed over the logged interval of 5,881-9,408 ft. Naturally occurring fractures were analyzed in order to determine both fracture dip and azimuth. Most of the fractures dip steeply

283

ENTOMOLOGY O.B. Kovanci et al. (2005) Phytoparasitica 33(4):334-342 Effects of Application Rate and Interval on the Efficacy of  

E-Print Network (OSTI)

ENTOMOLOGY O.B. Kovanci et al. (2005) Phytoparasitica 33(4):334-342 Effects of Application Rate sustain themselves in apples alone in NC, Received Nov. 22, 2004; accepted March 12, 2005; http://www.phytoparasitica

284

3-D structural and seismic stratigraphic interpretation of the Guasare-Misoa Interval, VLE 196 Area, Block V, Lamar Field, Lake Maracaibo, Venezuela  

E-Print Network (OSTI)

In this study, the structure, depositional system, and the seismic stratigraphy of the VLE 196 area, Block V in Lamar Field were interpreted using 3-D seismic data and well logs to characterize structural and depositional settings of the Guasare...

Arzuman, Sadun

2004-09-30T23:59:59.000Z

285

Subsurface Geology of Arsenic-Bearing Permian Sedimentary Rocks in the Garber-Wellington Interval of the Central Oklahoma Aquifer, Cleveland County, Oklahoma.  

E-Print Network (OSTI)

??The Central Oklahoma Aquifer is an important source of drinking water in central Oklahoma. The major formations making up the aquifer, the Garber Sandstone and… (more)

Abbott, Ben Nicholas

2005-01-01T23:59:59.000Z

286

Challenges and Opportunities in Implementing the FDA Default Parametric Tolerance Interval Two One-Sided Test for Delivered Dose Uniformity of Orally Inhaled Products  

Science Journals Connector (OSTI)

In 2009, the International Pharmaceutical Aerosol Consortium on Regulation and Science (IPAC-RS) conducted DDU Seminars in order to discuss with member companies industry’s experiences with the PTI-TOST. During t...

Greg Larner; Andrew Cooper; Svetlana Lyapustina; Stefan Leiner…

2011-12-01T23:59:59.000Z

287

DMSP-IEES: A Stochastic Programming Model Based on Dual-Interval and Multi-Stage Scenarios Modeling Approaches for Energy Systems Management and GHG Emissions Control  

Science Journals Connector (OSTI)

Energy-related activities contribute a major portion of anthropogenic greenhouse gas (GHG) emissions into the atmosphere. In this ... -environment systems management, in which issues of GHG-emission mitigation ca...

G. C. Li; G. H. Huang; Z. F. Liu

2014-10-01T23:59:59.000Z

288

Quiz # 4, STAT 383, Prof. Suman Sanyal, March 25, 2009 Q10 (Page 301). Each of the following is a confidence interval for = true average  

E-Print Network (OSTI)

@clarkson.edu #12;Q12 (Page 302). Heavy-metal pollution of various ecosystem is a serious environmen- tal threat

Sanyal, Suman

289

Understanding the Impact of Open-Framework Conglomerates on Water-Oil Displacements: Victor Interval of the Ivishak Reservoir, Prudhoe Bay Field, Alaska  

E-Print Network (OSTI)

The Victor Unit of the Ivishak Formation in the Prudhoe Bay Oilfield is characterized by high net-to-gross fluvial sandstones and conglomerates. The highest permeability is found within sets of cross-strata of open-framework conglomerate (OFC). They are preserved within unit bar deposits and assemblages of unit bar deposits within compound (braid) bar deposits. They are thief zones limiting enhanced oil recovery. We incorporate recent research that has quantified important attributes of their sedimentary architecture within preserved deposits. We use high-resolution models to demonstrate the fundamental aspects of their control on oil production rate, water breakthrough time, and spatial and temporal distribution of residual oil saturation. We found that when the pressure gradient is oriented perpendicular to the paleoflow direction, the total oil production and the water breakthrough time are larger, and remaining oil saturation is smaller, than when it is oriented parallel to paleoflow. The pressure differe...

Gershenzon, Naum I; Ritzi, Robert W; Dominic, David F

2014-01-01T23:59:59.000Z

290

Optimum fixed orientations and benefits of tracking for capturing solar radiation in the continental United States  

E-Print Network (OSTI)

a two-axis tracking solar panel. Figure 5b: Map of theand azimuth angles for solar panels were calculated for aannual azimuth for a solar panel, and can be combined with

Lave, Matthew; Kleissl, Jan

2011-01-01T23:59:59.000Z

291

Optimum fixed orientations and benefits of tracking for capturing solar radiation in the continental United States  

E-Print Network (OSTI)

solar collector, Solar & Wind Technology. 4 (1987) 407-410.to the solar azimuth. While other tracking technologies such

Lave, Matthew; Kleissl, Jan

2011-01-01T23:59:59.000Z

292

Optimum fixed orientations and benefits of tracking for capturing solar radiation in the continental United States  

E-Print Network (OSTI)

Mexico, and along the Pacific Coastline. A due south azimuth would suggest that equal amounts of solar

Lave, Matthew; Kleissl, Jan

2011-01-01T23:59:59.000Z

293

Analyzing and simulating the variability of solar irradiance and solar PV powerplants  

E-Print Network (OSTI)

Mexico, and along the Pacific Coastline. A due south azimuth would suggest that equal amounts of solar

Lave, Matthew S.

2012-01-01T23:59:59.000Z

294

Regional mapping of the crustal structure in southern California from receiver functions  

E-Print Network (OSTI)

is found between the NW and SE back-azimuthal groups of station DAN in the Fenner Valley. Asymmetric

Clayton, Robert W.

295

High-resolution x-ray diffraction microscopy of specifically labeled yeast cells (CXIDB ID 8)  

DOE Data Explorer (OSTI)

This is the fifth of five exposures of the same sample at different tilts. This one is at -30 degrees tilt. Check CXI IDs 4 to 8 for the complete set.

Nelson, Johanna

296

High-resolution x-ray diffraction microscopy of specifically labeled yeast cells (CXIDB ID 6)  

DOE Data Explorer (OSTI)

This is the third of five exposures of the same sample at different tilts. This one is at +30 degrees tilt. Check CXI IDs 4 to 8 for the complete set.

Nelson, Johanna

297

ECONOMIC RECOVERY OF OIL TRAPPED AT FAN MARGINS USING HIGH ANGLE WELLS AND MULTIPLE HYDRAULIC FRACTURES  

SciTech Connect

This project attempts to demonstrate the effectiveness of exploiting thin-layered, low-energy deposits at the distal margin of a prograding turbidite complex through the use of hydraulically fractured horizontal or high-angle wells. The combination of a horizontal or high-angle well and hydraulic fracturing will allow greater pay exposure than can be achieved with conventional vertical wells while maintaining vertical communication between thin interbedded layers and the wellbore. A high-angle well will be drilled in the fan-margin portion of a slope-basin clastic reservoir and will be completed with multiple hydraulic-fracture treatments. Geologic modeling, reservoir characterization, and fine-grid reservoir simulation will be used to select the well location and orientation. Design parameters for the hydraulic-fracture treatments will be determined, in part, by fracturing an existing test well. Fracture azimuth will be predicted by passive seismic monitoring of a fracture-stimulation treatment in the test well using logging tools in an offset well. The long radius, near horizontal well was drilled during the first quarter of 1996. Well conditions resulted in the 7 in. production liner sticking approximately 900 ft off bottom. Therefore, a 5 in. production liner was necessary to case this portion of the target formation. Swept-out sand intervals and a poor cement bond behind the 5 in. liner precluded two of the three originally planned hydraulic fracture treatments. As a result, all pay intervals behind the 5 in. liner were perforated and stimulated with a non-acid reactive fluid. Following a short production period, the remaining pay intervals in the well (behind the 7 in. liner) were perforated. The well was returned to production to observe production trends and pressure behavior and assess the need to stimulate the new perforations.

Mike L. Laue

2001-09-28T23:59:59.000Z

298

Effects of egg incubation condition on the post-hatching growth and performance of the snapping turtle, Chelydra serpentina  

SciTech Connect

The effect of incubation temperature on the post-hatching growth and performance capacities of the common snapping turtle, Chelydra serpentina was investigated in the laboratory. Turtle eggs were collected from four sites in New York State and randomly assigned to four incubation temperature treatments to produce males (constant 26{degree}C and downshifted 30-26-30{degree}C) and females (constant 30{degree}C and upshifted 26-30-26{degree}C) under constant and altered temperature regimes. The incubation conditions resulted in 92% males from the constant 26{degree}C group and 93% males from the downshifted group. 100% females resulted from both the constant 30{degree}C group and the upshifted group. Turtles hatching from eggs incubated constantly at 26{degree}C were significantly larger than hatchlings from eggs incubated at a constant 30{degree}C or downshifted. Hatchlings were raised in individual aquaria at 25{degree}C and fed earthworms and fish. After a 9-month growth period, turtles which had been incubated at a constant 30{degree}C gained significantly more mass than did turtles from eggs which had been downshifted or upshifted. There was no extended effect of incubation condition on Post-hatching performance and learning ability as measured by righting and feeding responses. Thus, the mass gain differences seen in this study suggest that physiological differences do result as the consequence of incubation condition. However, these physiological differences are not reflected in normal locomotive or feeding behavior.

Ryan, K.M.

1990-12-01T23:59:59.000Z

299

Effects of egg incubation condition on the post-hatching growth and performance of the snapping turtle, Chelydra serpentina  

SciTech Connect

The effect of incubation temperature on the post-hatching growth and performance capacities of the common snapping turtle, Chelydra serpentina was investigated in the laboratory. Turtle eggs were collected from four sites in New York State and randomly assigned to four incubation temperature treatments to produce males (constant 26[degree]C and downshifted 30-26-30[degree]C) and females (constant 30[degree]C and upshifted 26-30-26[degree]C) under constant and altered temperature regimes. The incubation conditions resulted in 92% males from the constant 26[degree]C group and 93% males from the downshifted group. 100% females resulted from both the constant 30[degree]C group and the upshifted group. Turtles hatching from eggs incubated constantly at 26[degree]C were significantly larger than hatchlings from eggs incubated at a constant 30[degree]C or downshifted. Hatchlings were raised in individual aquaria at 25[degree]C and fed earthworms and fish. After a 9-month growth period, turtles which had been incubated at a constant 30[degree]C gained significantly more mass than did turtles from eggs which had been downshifted or upshifted. There was no extended effect of incubation condition on Post-hatching performance and learning ability as measured by righting and feeding responses. Thus, the mass gain differences seen in this study suggest that physiological differences do result as the consequence of incubation condition. However, these physiological differences are not reflected in normal locomotive or feeding behavior.

Ryan, K.M.

1990-12-01T23:59:59.000Z

300

Recognizing Critical Behavior amidst Minijets at the Large Hadron Collider  

E-Print Network (OSTI)

The transition from quarks to hadrons in a heavy-ion collision at high energy is usually studied in two different contexts that involve very different transverse scales: local and non-local. Models that are concerned with the $p_T$ spectra and azimuthal anisotropy belong to the former, i.e., hadronization at a local point in $(\\eta,\\phi)$ space, such as the recombination model. The non-local problem has to do with quark-hadron phase transition where collective behavior through near-neighbor interaction can generate patterns of varying sizes in the $(\\eta,\\phi)$ space. The two types of problems are put together in this paper both as brief reviews separately and to discuss how they are related to each other. In particular, we ask how minijets produced at LHC can affect the investigation of multiplicity fluctuations as signals of critical behavior. It is suggested that the existing data from LHC have sufficient multiplicities in small $p_T$ intervals to make feasible the observation of distinctive features of clustering of soft particles, as well as voids, that characterize the critical behavior at phase transition from quarks to hadrons, without any ambiguity posed by the clustering of jet particles.

Rudolph C. Hwa

2014-11-22T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

Recognizing Critical Behavior amidst Minijets at the Large Hadron Collider  

E-Print Network (OSTI)

The transition from quarks to hadrons in a heavy-ion collision at high energy is usually studied in two different contexts that involve very different transverse scales: local and non-local. Models that are concerned with the $p_T$ spectra and azimuthal anisotropy belong to the former, i.e., hadronization at a local point in $(\\eta,\\phi)$ space, such as the recombination model. The non-local problem has to do with quark-hadron phase transition where collective behavior through near-neighbor interaction can generate patterns of varying sizes in the $(\\eta,\\phi)$ space. The two types of problems are put together in this paper both as brief reviews separately and to discuss how they are related to each other. In particular, we ask how minijets produced at LHC can affect the investigation of multiplicity fluctuations as signals of critical behavior. It is suggested that the existing data from LHC have sufficient multiplicities in small $p_T$ intervals to make feasible the observation of distinctive features of cl...

Hwa, Rudolph C

2014-01-01T23:59:59.000Z

302

The High-Acceptance Dielectron Spectrometer HADES  

E-Print Network (OSTI)

HADES is a versatile magnetic spectrometer aimed at studying dielectron production in pion, proton and heavy-ion induced collisions. Its main features include a ring imaging gas Cherenkov detector for electron-hadron discrimination, a tracking system consisting of a set of 6 superconducting coils producing a toroidal field and drift chambers and a multiplicity and electron trigger array for additional electron-hadron discrimination and event characterization. A two-stage trigger system enhances events containing electrons. The physics program is focused on the investigation of hadron properties in nuclei and in the hot and dense hadronic matter. The detector system is characterized by an 85% azimuthal coverage over a polar angle interval from 18 to 85 degree, a single electron efficiency of 50% and a vector meson mass resolution of 2.5%. Identification of pions, kaons and protons is achieved combining time-of-flight and energy loss measurements over a large momentum range. This paper describes the main features and the performance of the detector system.

The HADES Collaboration; G. Agakishiev; A. Balanda; B. Bannier; R. Bassini; D. Belver; A. V. Belyaev; A. Blanco; M. Boehmer; J. L. Boyard; P. Braun-Munzinger; P. Cabanelas; E. Castro; S. Chernenko; T. Christ; M. Destefanis; J. Diaz; F. Dohrmann; A. Dybczak; T. Eberl; W. Enghardt; L. Fabbietti; O. V. Fateev; P. Finocchiaro; P. Fonte; J. Friese; I. Froehlich; T. Galatyuk; J. A. Garzon; R. Gernhaeuser; A. Gil; C. Gilardi; M. Golubeva; D. Gonzalez-Diaz; F. Guber; M. Heilmann; T. Heinz; T. Hennino; R. Holzmann; A. Ierusalimov; I. Iori; A. Ivashkin; M. Jurkovic; B. Kaempfer; K. Kanaki; T. Karavicheva; D. Kirschner; I. Koenig; W. Koenig; B. W. Kolb; R. Kotte; F. Krizek; R. Kruecken; W. Kuehn; A. Kugler; A. Kurepin; S. Lang; J. S. Lange; K. Lapidus; T. Liu; L. Lopes; M. Lorenz; L. Maier; A. Mangiarotti; J. Markert; V. Metag; B. Michalska; J. Michel; D. Mishra; E. Moriniere; J. Mousa; C. Muentz; L. Naumann; J. Otwinowski; Y. C. Pachmayer; M. Palka; Y. Parpottas; V. Pechenov; O. Pechenova; T. PerezCavalcanti; J. Pietraszko; W. Przygoda; B. Ramstein; A. Reshetin; M. Roy-Stephan; A. Rustamov; A. Sadovsky; B. Sailer; P. Salabura; A. Schmah; E. Schwab; Yu. G. Sobolev; S. Spataro; B. Spruck; H. Stroebele; J. Stroth; C. Sturm; M. Sudol; A. Tarantola; K. Teilab; P. Tlusty; M. Traxler; R. Trebac; H. Tsertos; V. Wagner; M. Weber; M. Wisniowski; T. Wojcik; J. Wuestenfel; S. Yurevich; Y. V. Zanevsky; P. Zhou; P. Zumbruch

2009-03-09T23:59:59.000Z

303

The High-Acceptance Dielectron Spectrometer HADES  

E-Print Network (OSTI)

HADES is a versatile magnetic spectrometer aimed at studying dielectron production in pion, proton and heavy-ion induced collisions. Its main features include a ring imaging gas Cherenkov detector for electron-hadron discrimination, a tracking system consisting of a set of 6 superconducting coils producing a toroidal field and drift chambers and a multiplicity and electron trigger array for additional electron-hadron discrimination and event characterization. A two-stage trigger system enhances events containing electrons. The physics program is focused on the investigation of hadron properties in nuclei and in the hot and dense hadronic matter. The detector system is characterized by an 85% azimuthal coverage over a polar angle interval from 18 to 85 degree, a single electron efficiency of 50% and a vector meson mass resolution of 2.5%. Identification of pions, kaons and protons is achieved combining time-of-flight and energy loss measurements over a large momentum range. This paper describes the main featur...

Agakichiev, G; Bannier, B; Bassini, R; Belver, D; Belyaev, A V; Blanco, A; Boehmer, M; Boyard, J L; Braun-Munzinger, P; Cabanelas, P; Castro, E; Chernenko, S; Christ, T; Destefanis, M; Díaz, J; Dohrmann, F; Dybczak, A; Eberl, T; Enghardt, W; Fabbietti, L; Fateev, O V; Finocchiaro, P; Fonte, Paulo J R; Friese, J; Fröhlich, I; Galatyuk, T; Garzón, J A; Gernhäuser, R; Gil1, A; Gilardi, C; Golubeva, M; Gonzalez-Diaz, D; Guber, F; Heilmann, M; Heinz, T; Hennino, T; Holzmann, R; Ierusalimov, A; Iori, I; Ivashkin, A; Jurkovic, M; Kämpfer, B; Kanaki, K; Karavicheva, T; Kirschner, D; König, I; König, W; Kolb, B W; Kotte, R; Krizek, F; Krücken, R; Kühn, W; Kugler, A; Kurepin, A; Lang, S; Lange, J S; Lapidus, K; Liu, T; Lopes, L; Lorenz, M; Maier, L; Mangiarotti, A; Markert, J; Metag, V; Michalska, B; Michel, J; Mishra, D; Moriniere, E; Mousa, J; Müntz, C; Naumann, Lutz; Otwinowski, J; Pachmayer, Y C; Palka, M; Parpottas, Y; Pechenov, V; Pechenova, O; PerezCavalcanti, T; Pietraszko, J; Przygoda, W; Ramstein, B; Reshetin, A; Roy-Stephan, M; Rustamov, A; Sadovskii, A; Sailer, B; Salabura, P; Schmah, A; Schwab, E; Sobolev, Yu G; Spataro, S; Spruck, B; Ströbele, H; Stroth, J; Sturm, C; Sudol, M; Tarantola, A; Teilab, K; Tlustý, P; Traxler, M; Trebac, R; Tsertos, H; Wagner, V; Weber, M; Wisniowski, M; Wojcik, T; Wuestenfel, J; Yurevich, S; Zanevsky, Yu V; Zhou, P; Zumbruch, P

2009-01-01T23:59:59.000Z

304

E-Print Network 3.0 - automated ultrasonic inspection Sample...  

NLE Websites -- All DOE Office Websites (Extended Search)

: a geometric approach to increasing ultrasonic sensor azimuth accuracy', IEEE Trans. Robot. Autom., 2003, 19... Accurate profile extraction and mapping by intelligent processing...

305

ARM - Measurements  

NLE Websites -- All DOE Office Websites (Extended Search)

Measurement Instrument Sponsor Aircraft State PositionVelocity @ 10Hz Trimble DSM(tm) AAF PitchRollAzimuth Trimble Advanced Navigation System (TANS)10Hz AAF...

306

Newsletter Southern Great Plains  

NLE Websites -- All DOE Office Websites (Extended Search)

channels. The instrument has azimuth and elevation motors controlled by differential sun sensors that rotate a tracking head to lock onto the solar beam and keep the detectors...

307

Microsoft Word - S06297_LTSP  

Office of Legacy Management (LM)

Type: Digital File Name Azimuth Field Inspection Photo No. Trip Report PL No. Post on Web Photo Caption Lead Inspector: ; Assistant Inspector: Remarks: Electronic File Location:...

308

Microsoft Word - S02013_LTS&MP.doc  

Office of Legacy Management (LM)

File Name Film Frame No. Azimuth Field Inspection Photo No. Trip Report PL No. Post on Web (YN) Photo Caption Lead Inspector: ; Assistant Inspector: Remarks: Electronic File...

309

A New Table of Observed Travel-Times of Earthquake Waves for Distances of 10° and 180° at One-Degree Intervals Applicable Only to Earthquakes of Shallow Focus  

Science Journals Connector (OSTI)

...excep- tion the fundamental requirement that...interior- wall of boiler-room. This...the buildings safe for operation and providing...amperes for normal operation. A Laon tube...0.1, the fundamental REPORTS AND PAPERS...

J. B. Macelwane; S.J.

310

Increased Dose Density Is Feasible: A Pilot Study of Adjuvant Epirubicin and Cyclophosphamide followed by Paclitaxel, at 10- or 11-Day Intervals with Filgrastim Support in Women with Breast Cancer  

Science Journals Connector (OSTI)

...feasibility of dose-dense FEC followed by alternating weekly taxanes in...four or more node-positive breast cancer...INT C9741: dose-dense chemotherapy...adjuvant epirubicin and cyclophosphamide followed by paclitaxel, at 10...

Monica N. Fornier; Andrew D. Seidman; Diana Lake; Gabriella D'Andrea; Jacqueline Bromberg; Mark Robson; Catherine Van Poznak; Katherine S. Panageas; Marietta Atienza; Larry Norton; and Clifford Hudis

2007-01-01T23:59:59.000Z

311

Advertising Installation Rates (rates include printing costs) Ads can be purchased at two-week or monthly intervals. Clients can request to have ads removed before the end of the scheduled display dates; however, clients  

E-Print Network (OSTI)

Advertising Installation Rates (rates include printing costs) Ads can be purchased at two are responsible for designing all advertisements. Approved ads must be 11 inches high and 17 inches wide. Allow Services will print, install and remove all ads. Submission Complete an advertising request form

Bennett, Gisele

312

Sequence stratigraphy, depositional environments, and regional mapping of the late Devonian interval, upper Three Forks Formation, Sanish Member, and lower Bakken Shale, U.S. portion of the Williston Basin.  

E-Print Network (OSTI)

??Cores of the Late Devonian upper Three Forks, Sanish, and lower Bakken units from eight wells were examined and described at the North Dakota core… (more)

Sesack, Steven A.

2011-01-01T23:59:59.000Z

313

ROUGHNESS LENGTHS FOR THE SAVANNAH RIVER SITE  

SciTech Connect

Surface roughness values for the areas surrounding the H, D and N-Area meteorological towers were computed from archived 2010 meteorological data. These 15-minute-averaged data were measured with cup anemometers and bidirectional wind vanes (bivanes) 61 m above the surface. The results of the roughness calculation using the standard deviation of elevation angle {sigma}{sub E}, and applying the simple formula based on tree canopy height, gave consistent estimates for roughness around the H-Area tower in the range of 1.76 to 1.86 m (95% confidence interval) with a mean value of 1.81 m. Application of the {sigma}{sub E} method for the 61-m level at D and N-Areas gave mean values of 1.71 and 1.81 with confidence ranges of 1.62-1.81 and 1.73-1.88 meters, respectively. Roughness results are azimuth dependent, and thus are presented as averages over compass sectors spanning 22.5 degrees. Calculated values were compared to other methods of determining roughness, including the standard deviation of the azimuth direction, {sigma}{sub A}, and standard deviation of the wind speed, {sigma}{sub U}. Additional data was obtained from a sonic anemometer at 61-m on the H-Area tower during a period of a few weeks in 2010. Results from the sonic anemometer support our use of {sigma}{sub E} to calculate roughness. Based on the H-Area tower results, a surface roughness of 1.8 m using is recommended for use in dispersion modeling applications that consider the impacts of a contaminant release to individuals along the Site boundary. The canopy surrounding the H-Area tower is relatively uniform (i.e., little variance in roughness by upwind direction), and data supplied by the U.S. Forest Service at Savannah River show that the canopy height and composition surrounding the H-Area tower is reasonably representative of forested areas throughout the SRS reservation. For dispersion modeling analyses requiring assessments of a co-located worker within the respective operations area, recommended area-specific values range from 0.3 m for E Area to 0.7 m for A Area at the Savannah River National Laboratory. These area-specific values, summarized in Table 4-1, were determined using the Environmental Protection Agency's AERSURFACE computer algorithm.

Hunter, C.

2012-03-28T23:59:59.000Z

314

Brigham Young University Department of Electrical and  

E-Print Network (OSTI)

The azimuthal modulation characteristics of Antarctic sea ice are evaluated us- ing techniques developed by David S. Early for the ERS-1 AMI scatterometer. Azimuthal modulation can produce adverse a ects. Several regions of sea ice and glacial ice are selected for the experiment. Incidence angle dependence

Long, David G.

315

Scaled physical modelling of anisotropic wave propagation: multioffset profiles over an orthorhombic medium  

Science Journals Connector (OSTI)

......in an azimuthally anisotropic medium: A physical...velocities in Cretaceous shales from the Williston...propagation in arbitrary anisotropic media, complexitie...modelled as Greenhorn shale (Jones & Wang 1981...in an azimuthally anisotropic medium: A physical...velocities in Cretaceous shales from the Williston......

R. James Brown; Don C. Lawton; Scott P. Cheadle

1991-12-01T23:59:59.000Z

316

This is an author-deposited version published in : http://oatao.univ-toulouse.fr/ Eprints ID : 8579  

E-Print Network (OSTI)

-Dominik and Poinsot, Thierry Acoustic and Large Eddy Simulation studies of azimuthal modes in annular combustion-oatao@listes.diff.inp-toulouse.fr #12;Acoustic and Large Eddy Simulation studies of azimuthal modes in annular combustion chambers. P) Large Eddy Simulation (LES) methods and (2) acoustic solvers. These strong com- bustion instabilities

Mailhes, Corinne

317

Anisotropy of the semi-classical gluon field of a large nucleus at high energy  

E-Print Network (OSTI)

The McLerran-Venugopalan model describes a highly boosted hadron/nucleus as a sheet of random color charges which source soft classical Weizs\\"acker-Williams gluon fields. We show that due to fluctuations, individual configurations are azimuthally anisotropic. We compute the first four azimuthal Fourier amplitudes of the S-matrix of a fundamental dipole in such background fields.

Dumitru, Adrian

2014-01-01T23:59:59.000Z

318

Bio-Climatic Analysis and Thermal Performance of Upper Egypt A Case Study Kharga Region  

E-Print Network (OSTI)

and Upper Egypt. In the recent century the most attentions of the government is the creation of new wadi parallel to Nile wadi in the west desert. Kharga Oasis is 25 degrees 26'56?North latitude and 30 degrees 32'24?East longitude. This oasis, is the largest...

Khalil, M. H.

2012-01-01T23:59:59.000Z

319

Engineering of thermotolerant Bacillus coagulans for production of D(-)-lactic acid  

DOE Patents (OSTI)

Genetically modified microorganisms having the ability to produce D(-)-lactic acid at temperatures between 30.degree. C. and 55.degree. C. are provided. In various embodiments, the microorganisms may have the chromosomal lactate dehydrogenase (ldh) gene and/or the chromosomal acetolactate synthase (alsS) gene inactivated. Exemplary microorganisms for use in the disclosed methods are Bacillus spp., such as Bacillus coagulans.

Wang, Qingzhao; Shanmugam, Keelnatham T; Ingram, Lonnie O

2014-12-02T23:59:59.000Z

320

Development of the Moon  

Science Journals Connector (OSTI)

...allowing creation of a lunar electrical grid. 4.3.7. Manufacturing. Propellants...conductor buses Aluminum, fused silica (flywheel), silver, copper 90 - Switches, energy...corresponds to 180 W longitude; 30-degree grid shown, resolution is 0.25/pixel...

Michael B. Duke; Lisa R. Gaddis; G. Jeffrey Taylor; Harrison H. Schmitt

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

Do quasi-regular structures really exist in the solar photosphere? I. Observational evidence  

E-Print Network (OSTI)

Two series of solar-granulation images -- the La Palma series of 5 June 1993 and the SOHO MDI series of 17--18 January 1997 -- are analysed both qualitatively and quantitatively. New evidence is presented for the existence of long-lived, quasi-regular structures (first reported by Getling and Brandt (2002)), which no longer appear unusual in images averaged over 1--2-h time intervals. Such structures appear as families of light and dark concentric rings or families of light and dark parallel strips (``ridges'' and ``trenches'' in the brightness distributions). In some cases, rings are combined with radial ``spokes'' and can thus form ``web'' patterns. The characteristic width of a ridge or trench is somewhat larger than the typical size of granules. Running-average movies constructed from the series of images are used to seek such structures. An algorithm is developed to obtain, for automatically selected centres, the radial distributions of the azimuthally averaged intensity, which highlight the concentric-ring patterns. We also present a time-averaged granulation image processed with a software package intended for the detection of geological structures in aerospace images. A technique of running-average-based correlations between the brightness variations at various points of the granular field is developed and indications are found for a dynamical link between the emergence and sinking of hot and cool parcels of the solar plasma. In particular, such a correlation analysis confirms our suggestion that granules -- overheated blobs -- may repeatedly emerge on the solar surface. Based on our study, the critical remarks by Rast (2002) on the original paper by Getling and Brandt (2002) can be dismissed.

A. V. Getling

2006-10-24T23:59:59.000Z

322

Scaling Properties of Fluctuation and Correlation Results from PHENIX  

E-Print Network (OSTI)

Recent surveys of multiplicity fluctuations, transverse momentum fluctuations, and two-particle azimuthal correlations are presented for several collision systems as a function of centrality and transverse momentum. Both multiplicity and transverse momentum fluctuations exhibit a power law scaling as a function of the number of participants that is independent of the collision system. Although these observations are consistent with critical behavior, the critical exponent $\\eta$ measured using azimuthal correlations is seen to be independent of centrality and collision system. Also observed in the azimuthal correlations is a displaced away side peak in central Au+Au collisions when the pairs are restricted to low transverse momentum.

J. T. Mitchell

2007-01-25T23:59:59.000Z

323

ARM - Datastreams - swacrblrhi  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsswacrblrhi Datastreamsswacrblrhi Documentation Data Quality Plots ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : SWACRBLRHI S-WACR Boundary-layer Range-Height Indicator scan Active Dates 2010.04.28 - 2010.05.31 Measurement Categories Cloud Properties Originating Instrument W-Band (95 GHz) ARM Cloud Radar, mounted to scan (SWACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Current pedestal azimuth position relative to North degrees Azimuth_current ( time ) Rate of pedestal motion in the azimuth degrees/sec Azimuth_scan_rate ( time ) Current pedestal elevation position degrees Elevation_current ( time )

324

ARM - Datastreams - swacrcal  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsswacrcal Datastreamsswacrcal Documentation Data Quality Plots Citation DOI: 10.5439/1025288 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : SWACRCAL S-WACR calibration information Active Dates 2010.03.15 - 2010.04.23 Measurement Categories Cloud Properties Originating Instrument W-Band (95 GHz) ARM Cloud Radar, mounted to scan (SWACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Current pedestal azimuth position relative to North degrees Azimuth_current ( time ) Rate of pedestal motion in the azimuth degrees/sec Azimuth_scan_rate ( time ) Current pedestal elevation position degrees Elevation_current ( time )

325

ARM - Datastreams - swacrcwrhi  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsswacrcwrhi Datastreamsswacrcwrhi Documentation Data Quality Plots Citation DOI: 10.5439/1025289 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : SWACRCWRHI S-WACR Cross-Wind Range-Height Indicator scan Active Dates 2009.10.26 - 2010.05.31 Measurement Categories Cloud Properties Originating Instrument W-Band (95 GHz) ARM Cloud Radar, mounted to scan (SWACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Current pedestal azimuth position relative to North degrees Azimuth_current ( time ) Rate of pedestal motion in the azimuth degrees/sec Azimuth_scan_rate ( time )

326

ARM - Datastreams - swacrppi  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsswacrppi Datastreamsswacrppi Documentation Data Quality Plots Citation DOI: 10.5439/1025292 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : SWACRPPI S-WACR Plan Position Indicator scan Active Dates 2009.10.05 - 2011.04.25 Measurement Categories Cloud Properties Originating Instrument W-Band (95 GHz) ARM Cloud Radar, mounted to scan (SWACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Current pedestal azimuth position relative to North degrees Azimuth_current ( time ) Rate of pedestal motion in the azimuth degrees/sec Azimuth_scan_rate ( time ) Current pedestal elevation position degrees Elevation_current ( time )

327

ARM - Datastreams - swacrvpt  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsswacrvpt Datastreamsswacrvpt Documentation Data Quality Plots Citation DOI: 10.5439/1025297 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : SWACRVPT S-WACR Vertical PoinTing scan Active Dates 2009.10.05 - 2011.04.25 Measurement Categories Cloud Properties Originating Instrument W-Band (95 GHz) ARM Cloud Radar, mounted to scan (SWACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Current pedestal azimuth position relative to North degrees Azimuth_current ( time ) Rate of pedestal motion in the azimuth degrees/sec Azimuth_scan_rate ( time ) Current pedestal elevation position degrees Elevation_current ( time )

328

Quantum States Allowing Minimum Uncertainty Product of angular position and momentum  

E-Print Network (OSTI)

We provide necessary and sufficient conditions for states to have an arbitrarily small uncertainty product of the azimuthal angle $\\phi $ and its canonical moment $L_{z}$. We illustrate our results with analytical examples.

Tiago Pereira; D. H. U. Marchetti

2008-10-16T23:59:59.000Z

329

Viscosity and the Soft Ridge at RHIC  

E-Print Network (OSTI)

Correlation studies exhibit a ridge-like feature in rapidity and azimuthal angle, with and without a jet trigger. We ask whether the feature in untriggered correlations can be a consequence of transverse flow and viscous diffusion.

Sean Gavin; George Moschelli

2008-06-26T23:59:59.000Z

330

GEOPHYSICS, VOL. 64, NO. 1 (JANUARY-FEBRUARY 1999); P. 146161, 9 FIGS., 2 TABLES. Joint inversion of P-and PS-waves in orthorhombic media  

E-Print Network (OSTI)

- imuthally dependent NMO velocities of the pure shear modes and to find the anisotropic parameters associatedwithfracturesystemsortransverselyisotropiclayers (e.g., shales) with a tilted symmetry axis. Substantial azimuthal Manuscript received

Tsvankin, Ilya

331

Anisotropy in multi-offset deep-crustal seismic experiments  

Science Journals Connector (OSTI)

......wide-angle models when the Earth is anisotropic. It is equally important...introduced by interpreting anisotropic seismic data with isotropic...The elastic anisotropy of shales, J. geophys. Res., 99...seismology over azimuthally anisotropic media, Geophysics, 53......

K. Jones; M. Warner; J. Brittan

1999-08-01T23:59:59.000Z

332

Evaluation of Tropical Cyclone Center Identification Methods in Numerical Models  

Science Journals Connector (OSTI)

Identifying the center of a tropical cyclone in a high-resolution model simulation has a number of operational and research applications, including constructing a track, calculating azimuthal means and perturbations, and diagnosing vortex tilt. ...

Leon T. Nguyen; John Molinari; Diana Thomas

2014-11-01T23:59:59.000Z

333

Non-uniform emission studies of a magnetron injection gun  

E-Print Network (OSTI)

This thesis investigates the experimental measurement and theoretical simulation of the effects of azimuthal emission non-uniformity of a 96 kV, 40 amp magnetron injection gun (MIG) used in a gyrotron. The accomplishments ...

Marchewka, Chad D. (Chad Daniel)

2006-01-01T23:59:59.000Z

334

Measurements of dynamics in an orientationally anisotropic system  

E-Print Network (OSTI)

(cont.) coefficients, and these were compared to the "effective" coefficients yielded by the former. Because scattering from a nematic domain is limited to a narrow azimuthal range, while an isotropic domain scatters ...

Borthwick, Matthew A. (Matthew Alan), 1973-

2004-01-01T23:59:59.000Z

335

Kaon dispersion relation and flow in relativistic heavy-ion collisions  

E-Print Network (OSTI)

Within the framework of a relativistic transport model (ART) for heavy-ion collisions at AGS energies, we examine the effects of a kaon dispersion relation on the transverse flow of kaons and their transverse momentum and azimuthal angle...

Li, Ba; Ko, Che Ming.

1996-01-01T23:59:59.000Z

336

Sea Mammal Research Unit Report on recent seal mortalities in UK  

E-Print Network (OSTI)

......................................................... 11 7. Mechanism of Injury: Ducted propellers ........................................ 12 8 sharks ......................................................... 15 8.6. Tidal turbines through a ducted propeller such as a Kort nozzle or some types of Azimuth thrusters. Such systems

Brierley, Andrew

337

Chaos in Robert Hooke's inverted cone BY MEDERIC ARGENTINA  

E-Print Network (OSTI)

Chaos in Robert Hooke's inverted cone BY ME´DE´RIC ARGENTINA 1,2 , PIERRE COULLET 1,2 , JEAN of the cone and the angle f indicates its azimuthal position) minus the conservation of energy

Argentina, Mederic

338

E-Print Network 3.0 - ac electric arc Sample Search Results  

NLE Websites -- All DOE Office Websites (Extended Search)

Search Powered by Explorit Topic List Advanced Search Sample search results for: ac electric arc Page: << < 1 2 3 4 5 > >> 1 The response of the azimuthal component of the...

339

High-Frequency Radars: Beamforming Calibrations Using Ships as Reflectors  

Science Journals Connector (OSTI)

Linear array antennas and beamforming techniques offer some advantages compared to direction finding using squared arrays. The azimuthal resolution depends on the number of antenna elements and their spacing. Assuming an ideal beam pattern and no ...

X. Flores-Vidal; P. Flament; R. Durazo; C. Chavanne; K.-W. Gurgel

2013-03-01T23:59:59.000Z

340

U.S. Department of Energy 2012 Annual Inspection - Parkersburg...  

Office of Legacy Management (LM)

compliance with 40 CFR 192. No corrective action was required in 2012. 9.0 Photographs Photo Location Number Azimuth Photograph Description 1 315 View down northeast fence line. 2...

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

A diagnostic method for probing the possible twist of magnetic field lines in sunspots  

Science Journals Connector (OSTI)

In order to study the three-dimensional structure of sunspot magnetic fields it is necessary to determine whether the field lines are twisted, i.e., if the azimuthal angle of transverse field changes with depth. ...

Shi-Hui Ye; Jie-Hai Jin

1990-10-01T23:59:59.000Z

342

Relative Short-Range Forecast Impact from Aircraft, Profiler, Radiosonde, VAD, GPS-PW, METAR, and Mesonet Observations via the RUC Hourly Assimilation Cycle  

Science Journals Connector (OSTI)

An assessment is presented on the relative forecast impact on the performance of a numerical weather prediction model from eight different observation data types: aircraft, profiler, radiosonde, velocity azimuth display (VAD), GPS-derived ...

Stanley G. Benjamin; Brian D. Jamison; William R. Moninger; Susan R. Sahm; Barry E. Schwartz; Thomas W. Schlatter

2010-04-01T23:59:59.000Z

343

Central neural coding of sky polarization in insects  

Science Journals Connector (OSTI)

...Neurobiology, University of Massachusetts Medical School, Worcester...associated with changes in solar elevation. In the central...unambiguous information on solar azimuth and, therefore, on...the animal to distinguish the solar from the anti-solar hemisphere...

2011-01-01T23:59:59.000Z

344

Electron-Muon Correlations in Proton+Proton and Deuteron+Gold Collisions at PHENIX.  

E-Print Network (OSTI)

??This dissertation presents the first measurement of electron-muon azimuthal correlations at the PHENIX experiment at RHIC in 200 GeV proton-proton and deuteron-gold collisions. Electron-muon pairs… (more)

Engelmore, Tatia

2011-01-01T23:59:59.000Z

345

Design and manufacture of a modular cylindrical apparatus for ferrofluid experimentation  

E-Print Network (OSTI)

Ferrofluids, colloidal suspensions of coated magnetic nanoparticles inside a carrier fluid, respond to externally applied magnetic fields. This thesis addresses the behavior of these fluids when subjected to an azimuthally ...

Schoen, Katrina Leigh

2011-01-01T23:59:59.000Z

346

Phenomenology of transverse-spin and transverse-momentum effects in hard processes  

E-Print Network (OSTI)

Some recent analyses of single-spin and azimuthal asymmetries in SIDIS and Drell-Yan processes, focusing in particular on Collins, Sivers and Boer-Mulders effects, are briefly reviewed. The perspectives for future phenomenological studies are also outlined.

Vincenzo Barone

2011-02-03T23:59:59.000Z

347

Paleomagnetic Measurements At Neal Hot Springs Geothermal Area...  

Open Energy Info (EERE)

pipe drill. Core samples were oriented by azimuth and hade using a magnetic compass and sun dial, then marked before being removed from the host rock. The core samples were then...

348

Asymmetric radar echo patterns from insects.  

Science Journals Connector (OSTI)

Radar echoes from insects, birds, and bats in the atmosphere exhibit both symmetry and asymmetry in polarimetric patterns. Symmetry refers to similar magnitudes of polarimetric variables at opposite azimuths, and asymmetry relegates to differences ...

Valery M. Melnikov; Michael J. Istok; John K. Westbroo

349

Analysis of the Texas A&M impact lightning detector to determine detection efficiency and site error corrections  

E-Print Network (OSTI)

and azimuth, site errors, signal strength, attenuation coefficient, and peak current. Cloud-to-ground (CG) return stroke measurements from the IMPACT detector were compared to National Lightning Detection Network (NLDN) measurements to determine...

Leahy, Frank Byron

2012-06-07T23:59:59.000Z

350

URBAN EXTENTS Congo, Democra  

E-Print Network (OSTI)

URBAN EXTENTS Congo, Democra Rwanda United Rep. of GRUMPv1 ´ 0 25 50 Km Lambert Azimuthal Equal. Available at:http://sedac.ciesin.columbia.edu/gpw/ United Republic of Tanzania Democratic Republic of Congo

Columbia University

351

2D and 3D Acoustic Source Localization Using the AML Algorithm and ENSBox Nodes  

E-Print Network (OSTI)

Networked Sensing 2D and 3D Acoustic Source Localizationhairs, median red square) 3D bearing estimates: (azimuth,1.37,1.52) (2.38,1.82) Node 153 3D AML performance UCLA –

2007-01-01T23:59:59.000Z

352

A Theoretical Study of the Effect of Discharge Parameters on the Plasma Layer in a Filippov Type Plasma Focus Device  

Science Journals Connector (OSTI)

In this paper, the theoretical ML model has been used to study the effect of three preliminary parameters (gas pressure, discharge voltage and the kind of the gas), to the current, azimuthal magnetic flux density...

M. A. Tafreshi

2014-10-01T23:59:59.000Z

353

A 25m2 Target-Aligned Heliostat with Closed-Loop Control  

Science Journals Connector (OSTI)

A 25m2 target-aligned research heliostat with closed-loop control, with a theoretical ... built at CSIR in South Africa. The heliostat has four degrees of freedom: Azimuth,...2 target-aligned miniheliostat. A tra...

Thomas Roos; Ndumiso Zwane; Eu’odia Kruger…

2009-01-01T23:59:59.000Z

354

Development, design and experimental testing of fuzzy-based controllers for a laboratory scale sun-tracking heliostat  

Science Journals Connector (OSTI)

The objective of this study is to develop and design fuzzy-based controllers for experimental examination and application to a laboratory scale sun tracking heliostat with dynamic movement about azimuth and eleva...

M. M. Ardehali; S. H. Emam

2011-09-01T23:59:59.000Z

355

Design Wind Speed  

Science Journals Connector (OSTI)

Wind is characterized by various different parameters. They include the following items: (1) wind speed, such as the mean wind speed and maximum instantaneous wind speed; (2) wind direction such as the azimuth di...

Yozo Fujino; Kichiro Kimura; Hiroshi Tanaka

2012-01-01T23:59:59.000Z

356

Structure of the solid D2 bilayer on graphite  

Science Journals Connector (OSTI)

Low-energy electron-diffraction (LEED) measurements for a solid D2 bilayer physisorbed on graphite are used to investigate the bilayer structure and its azimuthal orientation relative to the substrate. The LEED spot positions are consistent with the mutually commensurate oblique unit cell inferred from neutron-diffraction measurement. Given the azimuthal orientation of the bilayer LEED spots, the possibility of a bilayer composed of two incommensurate layers with mutually modulated triangular lattices is ruled out.

Wei Liu and S. C. Fain; Jr.

1993-06-15T23:59:59.000Z

357

Pleistocene deposition and structure: Galveston South OCS, offshore Texas  

SciTech Connect

Mapping of four Pleistocene sequences in the Galveston South and northern East Breaks areas shows three depopods containing over 1000 m of sediment. Depopods A, B, and C are located in (A) East Breaks Block 108, (B) Galveston South Blocks 244-245, and (C) Galveston South Blocks 219-220. Depopod A shifts slightly landward with time because of salt withdrawal. The later position of the depopod coincides with the shelf break for that unit as indicated by sigmoidal progradation. The other two depopods shift slightly basinward and are centered on faults with rollover. All depopods contain hydrocarbon indicators. Faults dominate the southern portion of the region. The faults cut the present shelf edge at 30/degrees/, suggesting that the Pleistocene shelf edge lay roughly 30/degrees/ to the present one. Salt diapirs evident in the southern part of the area formed because of sediment loading at the shelf edge. The diapirism dies out northward on the shelf.

Brooks, S.E.; Watkins, J.S.

1989-03-01T23:59:59.000Z

358

New MS-Windows-Based Educational Software for Teaching the Sunpath Diagram and Shading Mask Protractor  

E-Print Network (OSTI)

Mask 1 Degrees South Latitude. This combined le sunpath diagram and shading mask yrurr uuurjur u gertical surface facing 30 degrees east of south. FIGURE 7: Data Input Summaryfor the Partial Shading Device. The dimensions of the partial shading..., the shac similarly dimensioned device published in thc In Figure 7 and 8 the front shade is actually the has been rotated 90 degrees, re-sized and moved 1 directly below the horizontal shade. Architectural Graphics Standard is shown in Figure 9...

Oh, J. K. W.; Haberl, J. S.

1996-01-01T23:59:59.000Z

359

Leaf morphology in Cowpea [Vigna unguiculata (L.) Walp]: QTL analysis, physical mapping and identifying a candidate gene using synteny with model legume species  

E-Print Network (OSTI)

Interval Mapping and Kruskal-Wallis analysis (only IntervalMapping analysis, KW = Kruskal-Wallis analysis. Pottorff etStatistical analysis The Kruskal-Wallis and Interval Mapping

Pottorff, Marti; Ehlers, Jeffrey D; Fatokun, Christian; Roberts, Philip A; Close, Timothy J

2012-01-01T23:59:59.000Z

360

Dependence of Solar-Wind Power Spectra on the Direction of the Local Mean Magnetic Field  

Science Journals Connector (OSTI)

Wavelet analysis can be used to measure the power spectrum of solar-wind fluctuations along a line in any direction (?, ) with respect to the local mean magnetic field B 0. This technique is applied to study solar-wind turbulence in high-speed streams in the ecliptic plane near solar minimum using magnetic field measurements with a cadence of eight vectors per second. The analysis of nine high-speed streams shows that the reduced spectrum of magnetic field fluctuations (trace power) is approximately azimuthally symmetric about B 0 in both the inertial range and dissipation range; in the inertial range the spectra are characterized by a power-law exponent that changes continuously from 1.6 ± 0.1 in the direction perpendicular to the mean field to 2.0 ± 0.1 in the direction parallel to the mean field. The large uncertainties suggest that the perpendicular power-law indices 3/2 and 5/3 are both consistent with the data. The results are similar to those found by Horbury et al. at high heliographic latitudes. Comparisons between solar-wind observations and the theories of strong incompressible MHD turbulence developed by Goldreich & Sridhar and Boldyrev are not rigorously justified because these theories only apply to turbulence with vanishing cross-helicity although the normalized cross-helicity of solar-wind turbulence is not negligible. Assuming these theories can be generalized in such a way that the three-dimensional wavevector spectra have similar functional forms when the cross-helicity is nonzero, then for the interval of Ulysses data analyzed by Horbury et al. the ratio of the spectra perpendicular and parallel to B 0 is more consistent with the Goldreich & Sridhar scaling P ?/P ? ? ?1/3 than with the Boldyrev scaling ?1/2. The analysis of high-speed streams in the ecliptic plane does not yield a reliable measurement of this scaling law. The transition from a turbulent MHD-scale energy cascade to a kinetic Alfvén wave (KAW) cascade occurs when k ?? i 1, which coincides with the spectral break. At slightly higher wavenumbers, in the dissipation range, there is a peak in the power ratio with P ?/P ? 1. The decay of this peak may be caused by the damping of KAWs, which is predicted to occur near k ?? i 4.

J. J. Podesta

2009-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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.


361

E-Print Network 3.0 - accelerated birnbaum-saunders models Sample...  

NLE Websites -- All DOE Office Websites (Extended Search)

8 Point and Interval Estimations for the Two-parameter Birnbaum-Saunders Summary: Point and Interval Estimations for the Two-parameter Birnbaum-Saunders Distribution based...

362

2011 Wind Technologies Market Report  

E-Print Network (OSTI)

study. Regions with fast energy markets, for example, changeis set aside in one energy market interval is then releasedto be dispatched in a later energy market interval, whereas

Bolinger, Mark

2013-01-01T23:59:59.000Z

363

BPA Metering Services Editing and Estimating Procedures  

NLE Websites -- All DOE Office Websites (Extended Search)

Editing and Estimating Interval Data 1. Introduction This section defines the meter interval data editing and estimation techniques performed by BPA's Metering Services...

364

Automating Shallow Seismic Imaging  

SciTech Connect

This seven-year, shallow-seismic reflection research project had the aim of improving geophysical imaging of possible contaminant flow paths. Thousands of chemically contaminated sites exist in the United States, including at least 3,700 at Department of Energy (DOE) facilities. Imaging technologies such as shallow seismic reflection (SSR) and ground-penetrating radar (GPR) sometimes are capable of identifying geologic conditions that might indicate preferential contaminant-flow paths. Historically, SSR has been used very little at depths shallower than 30 m, and even more rarely at depths of 10 m or less. Conversely, GPR is rarely useful at depths greater than 10 m, especially in areas where clay or other electrically conductive materials are present near the surface. Efforts to image the cone of depression around a pumping well using seismic methods were only partially successful (for complete references of all research results, see the full Final Technical Report, DOE/ER/14826-F), but peripheral results included development of SSR methods for depths shallower than one meter, a depth range that had not been achieved before. Imaging at such shallow depths, however, requires geophone intervals of the order of 10 cm or less, which makes such surveys very expensive in terms of human time and effort. We also showed that SSR and GPR could be used in a complementary fashion to image the same volume of earth at very shallow depths. The primary research focus of the second three-year period of funding was to develop and demonstrate an automated method of conducting two-dimensional (2D) shallow-seismic surveys with the goal of saving time, effort, and money. Tests involving the second generation of the hydraulic geophone-planting device dubbed the ''Autojuggie'' showed that large numbers of geophones can be placed quickly and automatically and can acquire high-quality data, although not under rough topographic conditions. In some easy-access environments, this device could make SSR surveying considerably more efficient and less expensive, particularly when geophone intervals of 25 cm or less are required. The most recent research analyzed the difference in seismic response of the geophones with variable geophone spike length and geophones attached to various steel media. Experiments investigated the azimuthal dependence of the quality of data relative to the orientation of the rigidly attached geophones. Other experiments designed to test the hypothesis that the data are being amplified in much the same way that an organ pipe amplifies sound have so far proved inconclusive. Taken together, the positive results show that SSR imaging within a few meters of the earth's surface is possible if the geology is suitable, that SSR imaging can complement GPR imaging, and that SSR imaging could be made significantly more cost effective, at least in areas where the topography and the geology are favorable. Increased knowledge of the Earth's shallow subsurface through non-intrusive techniques is of potential benefit to management of DOE facilities. Among the most significant problems facing hydrologists today is the delineation of preferential permeability paths in sufficient detail to make a quantitative analysis possible. Aquifer systems dominated by fracture flow have a reputation of being particularly difficult to characterize and model. At chemically contaminated sites, including U.S. Department of Energy (DOE) facilities and others at Department of Defense (DOD) installations worldwide, establishing the spatial extent of the contamination, along with the fate of the contaminants and their transport-flow directions, is essential to the development of effective cleanup strategies. Detailed characterization of the shallow subsurface is important not only in environmental, groundwater, and geotechnical engineering applications, but also in neotectonics, mining geology, and the analysis of petroleum reservoir analogs. Near-surface seismology is in the vanguard of non-intrusive approaches to increase knowledge of the shallow subsurface; our

Steeples, Don W.

2004-12-09T23:59:59.000Z

365

Contained Modes In Mirrors With Sheared Rotation  

SciTech Connect

In mirrors with E × B rotation, a fixed azimuthal perturbation in the lab frame can appear as a wave in the rotating frame. If the rotation frequency varies with radius, the plasma-frame wave frequency will also vary radially due to the Doppler shift. A wave that propagates in the high rotation plasma region might therefore be evanescent at the plasma edge. This can lead to radially localized Alfven eigenmodes with high azimuthal mode numbers. Contained Alfven modes are found both for peaked and non-peaked rotation profiles. These modes might be useful for alpha channeling or ion heating, as the high azimuthal wave number allows the plasma wave frequency in the rotating frame to exceed the ion cyclotron frequency. __________________________________________________

Abraham J. Fetterman and Nathaniel J. Fisch

2010-10-08T23:59:59.000Z

366

Validity of First-Order Approximations to Describe Parameter Uncertainty in Soil Hydrologic Models  

E-Print Network (OSTI)

Jasper A. Vrugt* and Willem Bouten ABSTRACT system under study. Confidence intervals on the cali- brated

Vrugt, Jasper A.

367

Multiway Range Trees: Scalable IP Lookup with Fast Updates  

E-Print Network (OSTI)

on prefix lengths'' [9], ``Lulea compressed tries'' [1], or ``binary search on intervals'' [5] perform

Varghese, George

368

MRI-compatible Haptics: Strain sensing for real-time estimation of three dimensional needle deflection in MRI environments , S. Elayaperumal1  

E-Print Network (OSTI)

discharge machining (EDM), along the neutral axis of the needle at 120-degree intervals. Three fibers

Park, Yong-Lae

369

HIV-related sexual behaviors, drugs, and violence among high risk populations in Baja California, Mexico  

E-Print Network (OSTI)

Crude Odds Ratio Confidence Interval Sociodemographic characteristics Born in the United States Born in Mexico

Volkmann, Tyson Alexander

2012-01-01T23:59:59.000Z

370

Particle Deconfinement in a Bent Magnetic Mirror  

SciTech Connect

Coils misalignment in a magnetic mirror can produce additional particle transport. The magnetic field non axi-symmetry is responsible for radial and longitudinal drifts in a way much similar to the neo-classical transport in a tandem mirror cell distorted by end plugs. Accordingly, a regime exhibiting large radial displacements - similar to the resonant regime in tandem mirrors - can be obtained by confining ions azimuthally, for example by means of a properly tuned radial electric field. Because of the mass dependence of the magnetic field non-homogeneity drift velocities, the azimuthal trapping is mass specific, allowing in principle the filtering of a specific species based on its mass.

Renaud Gueroult and Nathaniel J. Fisch

2012-09-06T23:59:59.000Z

371

The muon charge ratio in cosmic ray air showers  

E-Print Network (OSTI)

The muon charge ratio of the lateral muon density distributions in single EAS is studied by simulations, in context of recent proposals to measure this observable in coincidence with EAS observations. While effects of the hadronic interaction do not lead to significant differences of the total muon plus and muon minus content, the differences of the azimuthal variation of the muon densities of opposite charges and the azimuthal variation of the muon charge ratio appear to be very much pronounced, dependent on the direction of EAS incidence. This is due to the influence of the geomagnetic field which induces related effects in radio emission from extended air showers.

H. Rebel; O. Sima; A. Haungs; C. Manailescu; B. Mitrica; C. Morariu

2008-06-29T23:59:59.000Z

372

Solar radiation on variously oriented sloping surfaces  

SciTech Connect

Monthly average daily irradiation on surfaces tilted towards the equator and also inclined at various azimuth angles are estimated for two locations in Lesotho and the results are presented. The isotropic model suggested by Liu and Jordan (Trans. of Ashrae, 526, 1962) along with the modified equation of Klein (Solar Energy, 19, 4, 1977) are employed for the estimation purposes. Surface orientations are selected at three inclinations for six different azimuth angles. Conclusions are reached for optimum tilt and orientation for summer, winter and annual collection. Total annual radiation values are computed for all the slopes and orientations.

Gopinathan, K.K. (National Univ. of Lesotho, Roma (South Africa))

1991-01-01T23:59:59.000Z

373

ATLAS measurements of soft particle production and diffraction  

SciTech Connect

The ATLAS Collaboration has measured a wide range of properties of soft particle production in {radical}(s) = 900GeV and {radical}(s) = 7TeV proton-proton collisions at the Large Hadron Collider (LHC). These include forward-backward and azimuthal correlations, azimuthal ordering of hadron production, underlying event properties and their dependence on aspects of the hard scattering process. The inelastic and diffractive cross sections have also been measured, using particle forward flow and rapidity gaps. Many of these measurements are used to develop and tune models for soft particle production.

Todorova-Nova, Sarka [Tufts University, Medford, MA (United States); Collaboration: ATLAS Collaboration

2012-10-23T23:59:59.000Z

374

Guide to Passive Solar Home Design  

Energy.gov (U.S. Department of Energy (DOE)) Indexed Site

Elements of Passive Solar Design Elements of Passive Solar Design To design a completely passive solar home, you need to incorporate what are considered the five elements of passive solar design: 1. Aperture (Windows) - Windows should face within 30 degrees of true south, and during winter months they should not be shaded from 9 a.m. to 3 p.m. The windows in living areas should face south, while the windows in bedrooms should face north. In colder climates, reduce the window area

375

Bulk synthesis of nanoporous palladium and platinum powders  

DOE Patents (OSTI)

Disclosed is a method for providing nanoporous palladium and platinum powders. These materials were synthesized on milligram to gram scales by chemical reduction of tetrahalo-complexes with ascorbate in a concentrated aqueous surfactant at temperatures between -20.degree. C. and 30.degree. C. The prepared particles have diameters of approximately 50 nm, wherein each particle is perforated by pores having diameters of approximately 3 nm, as determined by electron tomography. These materials are of potential value for hydrogen and electrical charge storage applications.

Robinson, David B. (Fremont, CA); Fares, Stephen J. (Pleasanton, CA); Tran, Kim L. (Livermore, CA); Langham, Mary E. (Pleasanton, CA)

2012-04-17T23:59:59.000Z

376

Bulk synthesis of nanoporous palladium and platinum powders  

DOE Patents (OSTI)

Disclosed is a method for providing nanoporous palladium and platinum powders. These materials were synthesized on milligram to gram scales by chemical reduction of tetrahalo-complexes with ascorbate in a concentrated aqueous surfactant at temperatures between -20.degree. C. and 30.degree. C. The prepared particles have diameters of approximately 50 nm, wherein each particle is perforated by pores having diameters of approximately 3 nm, as determined by electron tomography. These materials are of potential value for hydrogen and electrical charge storage applications.

Robinson, David B; Fares, Stephen J; Tran, Kim L; Langham, Mary E

2014-04-15T23:59:59.000Z

377

TESTING COWLING'S ANTIDYNAMO THEOREM NEAR A ROTATING BLACK HOLE AXEL BRANDENBURG1  

E-Print Network (OSTI)

hole. In the cases investigated it is found that a magnetic field cannot be sustained against ohmic-excited axisymmetric solutions. In practice, therefore, Cowling's antidynamo theorem may still hold in Kerr geometry of processes depicted above, only changes in the azimuthal electric and magnetic fields by stretching

Brandenburg, Axel

378

Near-surface study at the Valhall oil field from ambient noise surface wave tomography  

Science Journals Connector (OSTI)

......there is still a strong domination of the 155 azimuth even...Fourier transform. We set up the time window deltaT...frequency band. 3.2 Locating noise sources at intermediate...vertical-to-vertical data set and allows us to significantly...interpretation of the full set of frequencies is out......

A. Mordret; M. Landès; N. M. Shapiro; S. C. Singh; P. Roux; O. I. Barkved

2013-01-01T23:59:59.000Z

379

This paper was prepared for presentation at the 2005 SPE Technical Symposium of Saudi Arabia Section held in Dhahran, Saudi Arabia, 14-16 May 2005.  

E-Print Network (OSTI)

. Controllable factors include mud weight, wellbore azimuth and inclination. A proper drilling program optimizes by the Technical Symposium Program Committee following review of information contained in full manuscript submitted a platform. Drilling an ingauge hole is an interplay of two factors: uncontrollable and controllable

Al-Majed, Abdulaziz Abdullah

380

Electron Coherence in a Melting Lead Monolayer  

Science Journals Connector (OSTI)

...the Pb(1,0) spots in the LEED patterns of Fig. 1, B to D...azimuthal modulation of the LEED intensities above Tm is likely not a manifestation...associated with the particular LEED spot, and {xi} is the temperature-dependent...British Columbia V6T1Z4, Canada. Electron coherence in a melting...

F. Baumberger; W. Auwärter; T. Greber; J. Osterwalder

2004-12-24T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


381

Electron Coherence in a Melting Lead Monolayer  

Science Journals Connector (OSTI)

...azimuthal modulation of the LEED intensities above Tm is likely...sixfold symmetric elementary building blocks of the 2D liquid. The slight anisotropy...associated with the particular LEED spot, and {xi} is the temperature-dependent...British Columbia V6T1Z4, Canada. Electron coherence in a melting...

F. Baumberger; W. Auwärter; T. Greber; J. Osterwalder

2004-12-24T23:59:59.000Z

382

Report from NA49  

E-Print Network (OSTI)

The signatures of the onset of deconfinement, found by the NA49 experiment at low SPS energies, are confronted with new results from the Beam Energy Scan (BES) program at BNL RHIC and CERN LHC results. Additionally, new NA49 results on chemical (particle ratio) fluctuations, azimuthal angle fluctuations, intermittency of di-pions, etc. are presented.

Katarzyna Grebieszkow; for the NA49 Collaboration

2011-12-04T23:59:59.000Z

383

Anisotropic inversion of refracted waves in vertical cable data in the presence of dip  

E-Print Network (OSTI)

the anisotropic parameters of these shales in situ. In these studies, seismic lines were laid out parallelAnisotropic inversion of refracted waves in vertical cable data in the presence of dip Hejie Wang1 isotropic and anisotropic media. Two sets of transversely isotropic models are used to analyse the azimuthal

Edinburgh, University of

384

The nature of X-ray selected extremely red objects  

Science Journals Connector (OSTI)

......the effective areas of the individual...periods of good atmospheric transparency...and 450-mum atmospheric passbands. The...in azimuth. Atmospheric transparency...with the Very Large Array (VLA...s in 3.25-MHz channels, 28...optically-thin thermal plasma model with Galactic......

J. A. Stevens; M. J. Page; R. J. Ivison; Ian Smail; I. Lehmann; G. Hasinger; G. Szokoly

2003-06-11T23:59:59.000Z

385

CP violation in the cubic coupling of neutral gauge bosons  

Science Journals Connector (OSTI)

We investigate the CP-violating form factor of the ZZZ and ZZ? vertices in the pair production of Z0 bosons. Useful observables in azimuthal distributions are constructed to probe CP nonconservation which may originate from these vertices. A simple two-Higgs-doublet model of CP violation is used as an illustration.

Darwin Chang; Wai-Yee Keung; Palash B. Pal

1995-02-01T23:59:59.000Z

386

Rotation Angle for the Optimum Tracking of One-Axis Trackers  

SciTech Connect

An equation for the rotation angle for optimum tracking of one-axis trackers is derived along with equations giving the relationships between the rotation angle and the surface tilt and azimuth angles. These equations are useful for improved modeling of the solar radiation available to a collector with tracking constraints and for determining the appropriate motor revolutions for optimum tracking.

Marion, W. F.; Dobos, A. P.

2013-07-01T23:59:59.000Z

387

Few layers graphene on 6H-SiC(000-1): an STM study Franois Varchon, Pierre Mallet, Laurence Magaud, and Jean-Yves Veuillen  

E-Print Network (OSTI)

1 Few layers graphene on 6H-SiC(000-1): an STM study François Varchon, Pierre Mallet, Laurence) graphene layers grown on the C terminated face of 6H-SiC in order to identify the nature of the azimuthal to electronic properties reminiscent of single layer graphene even for multilayer samples. Our results indicate

Boyer, Edmond

388

Clustering phenomena from two-particle angular correlations in proton-proton and heavy ion collisions  

E-Print Network (OSTI)

Results on two-particle angular correlations in proton-proton (/-s = 200 and 410 GeV) ,Cu+Cu and Au+Au collisions (js = 200 GeV) are presented over a broad range of pseudorapidity ([eta]) and azimuthal angle ([phi]). The ...

Li, Wei, Ph. D. Massachusetts Institute of Technology

2009-01-01T23:59:59.000Z

389

MAGNETIC FIELD CONFINEMENT IN THE SOLAR CORONA. II. FIELD-PLASMA INTERACTION B. Fornberg,2  

E-Print Network (OSTI)

MAGNETIC FIELD CONFINEMENT IN THE SOLAR CORONA. II. FIELD-PLASMA INTERACTION N. Flyer,1 B. Fornberg numerically to generate a continuum of solutions with two parameters to control the total azimuthal flux from the study to the solar corona and the energetics of coronal mass ejections and flares. Subject

Fornberg, Bengt

390

Fluidic Control of a Turret Wake: Aerodynamic and Aero-Optical Effects  

E-Print Network (OSTI)

optical window are investigated at M = 0.3 and ReD = 4.46·106 (with additional measurements at M = 0 and hot-film measurements within the separated flow domain. In addition, the suppression of optical-mean-square = height of turret base = azimuthal angle of pressure ports = elevation angle of optical window s = flow

Jumper, Eric

391

Directed Energy Beam Improvement Using Binary Control for the Advanced Tactical Laser (DEBI-BATL)  

E-Print Network (OSTI)

conformal optical window are investigated at M = 0.3 and ReD = 4.46·106 (with additional measurements at M and hot-film measurements within the separated flow domain. In addition, the suppression of optical = azimuthal angle of pressure ports = elevation angle of optical window s = flow separation angle

Gordeyev, Stanislav

392

Magnetic insulation (reply)  

Science Journals Connector (OSTI)

... DR WINTERBERG REPLIES: Contrary to Blewett's belief, magnetic insulation has not only been experimentally confirmed2 since I proposed it several years ago1, but ... generators (for example, the MJ Aurora machine). The magnetic field needed for the insulation effect in this case is generated by the strong azimuthal self-induced field of the ...

F. WINTERBERG

1974-06-28T23:59:59.000Z

393

J. Fluid Mech. (2005), vol. 525, pp. 115159. c 2005 Cambridge University Press DOI: 10.1017/S0022112004002629 Printed in the United Kingdom  

E-Print Network (OSTI)

being dominant. Here, m is the azimuthal wavenumber, and the positive sign represents the counter-winding of the flow fields in natural, forced and transient experiments, we suggest that the helical wave m = +2 absolute instability in the wake region of the breakdown structure. This self-excited oscillation first

Maxworthy, Tony

394

28th International Cosmic Ray Conference 369 Asymmetries Observed In Giant Air Showers Using Water  

E-Print Network (OSTI)

, Universidad Nacional de La Plata, C.C. 67 - 1900 La Plata, Argentina (2) PAO, Av. San Martin Norte 304, (5613) Malargue, Argentina Abstract Evidence of azimuthal asymmetries in the time structure and signal size has of the foremost issues in astrophysics today is the origin of the ultra high energy cosmic rays (UHECR

395

Enhanced Joule Heating in Umbral Dots  

E-Print Network (OSTI)

We present a study of magnetic profiles of umbral dots (UDs) and its consequences on the Joule heating mechanisms. Hamedivafa (2003) studied Joule heating using vertical component of magnetic field. In this paper UDs magnetic profile has been investigated including the new azimuthal component of magnetic field which might explain the relatively larger enhancement of Joule heating causing more brightness near circumference of UD.

Chandan Joshi; Lokesh Bharti; S. N. A. Jaaffrey

2007-05-08T23:59:59.000Z

396

Journal of Turbulence Volume 7, No. 73, 2006  

E-Print Network (OSTI)

streams is desired. In small-scale combustors such as micro gas turbines, mixing enhancement between fuel of the inner jet. Unlike in the natural jet, streamwise vortices appear in the inner shear layer that the azimuthal wavelength under the present control scheme is almost the same as that of the natural jet

Tokyo, University of

397

Polarization sensitivity as a contrast enhancer in pelagic predators: lessons from in situ polarization imaging of transparent zooplankton  

Science Journals Connector (OSTI)

...extremely clear Bahamian and Gulf of Mexico waters (Jerlov type I), the...the exact angle depended on solar elevation and azimuth and water...boat operations in the Gulf of Mexico and the Bahamas. We thank Canon...north west Atlantic and Gulf of Mexico. Biol. Bull. 195, 337-348...

2011-01-01T23:59:59.000Z

398

Geophysical Journal International Geophys. J. Int. (2012) 190, 12971310 doi: 10.1111/j.1365-246X.2012.05562.x  

E-Print Network (OSTI)

in the upper mantle flow field and its rheological structure have thus far hindered our ability to constrain rotations of azimuthal anisotropy to invert for hori- zontal pressure gradients everywhere). An idealized Couette flow (also called a shear-driven flow) in- volves viscous shearing between parallel flat

Conrad, Clint

399

V+jets production at the CMS  

E-Print Network (OSTI)

Measurements of Vector Boson production in association with jets are presented, using p-p collision data at sqrt{s} = 7 TeV. The measurements presented include Z + jets azimuthal correlations, event shapes, vector boson + jets differential cross section measurements, hard double-parton scattering using W + jets events and electroweak Z + forward - backward jet production.

B. Bilin; for the CMS Collaboration

2014-10-22T23:59:59.000Z

400

Cryptic and conspicuous coloration in the pelagic environment  

Science Journals Connector (OSTI)

...taking into account solar elevation and azimuth...pho- tons of lower energy and therefore longer...long-wavelength `solar' photons. The ability...A simple spectral solar irradiance model...radiance. Sol. Energy 41, 387392. Hemmings...Atlantic and Gulf of Mexico. Biol. Bull. 195...

2002-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

Interaction of p modes with a collection of thin magnetic tubes  

Science Journals Connector (OSTI)

......plane-parallel atmosphere with constant...assumption is that the plasma beta is constant...neutrally stable atmosphere for which acoustic-gravity...between 3 and 4 mHz followed by a decrease beyond 4 mHz. Azimuthal averaging...field-free atmosphere. Also, is the...magnetic flux and plasma beta parameter......

R. Jain; A. Gascoyne; B. W. Hindman

2011-08-01T23:59:59.000Z

402

Fast high resolution echelle spectroscopy of a laboratory plasma C. D. Cothran,a  

E-Print Network (OSTI)

to investigate radial and toroidal azimuthal midplane flows and ion heating during counterhelicity spheromak merging experiments10 at the Swarthmore Spheromak Experiment SSX . Magnetic reconnection is the dominant dynamical process at play while two spheromaks of equal but opposite sign magnetic helicity merge axially

Brown, Michael R.

403

Stabilization of the spheromak tilt instability  

Science Journals Connector (OSTI)

A stability criterion for the tilt mode of a spheromak?ion ring hybrid configuration has been developed for the case where the ring current is small compared to the spheromak azimuthal current. It is shown that the stability is related to the distortion of the spheromak separatrix.

C. Litwin; R. N. Sudan; A. D. Turnbull

1984-01-01T23:59:59.000Z

404

Simulation-guided optimization of small-angle analyzer geometry in the neutron backscattering spectrometer SPHERES  

SciTech Connect

The resolution of neutron backscattering spectrometers deteriorates at small scattering angles where analyzers deviate from exact backscattering. By reducing the azimuth angle range of the analyzers, the resolution can be improved with little loss of peak intensity. Measurements at the spectrometer SPHERES are in excellent agreement with simulations, which proves the dominance of geometric effects.

Wuttke, Joachim; Zamponi, Michaela [Forschungszentrum Jülich GmbH, Jülich Centre for Neutron Science at MLZ, Lichtenbergstraße 1, 85747 Garching (Germany)] [Forschungszentrum Jülich GmbH, Jülich Centre for Neutron Science at MLZ, Lichtenbergstraße 1, 85747 Garching (Germany)

2013-11-15T23:59:59.000Z

405

A QuikSCAT climatology of tropical cyclone size  

E-Print Network (OSTI)

QuikSCAT data of near-surface wind vectors for the years 1999–2008 are used to create a climatology of tropical cyclone (TC) size, defined as the radius of vanishing winds. The azimuthally-averaged radius of 12 ms?1 [ms ...

Chavas, Daniel Robert

406

MHD modelling of a disc wind from a high-mass protobinary: the case of Orion Source I  

Science Journals Connector (OSTI)

......and the poloidal velocity is updated each time...permits to set the flow velocity along the poloidal...p). Thus, the mass flux at the disc...1 MHD-driven wind profiles At the onset...poloidal and azimuthal velocities of the wind are shown...Overlaid on the density map are the temperature......

B. Vaidya; C. Goddi

2013-01-01T23:59:59.000Z

407

aeroacoustics volume 9 number 3 2010 pages 253272 253 Aeroacoustic investigation of a single  

E-Print Network (OSTI)

and unsteady pressure measurements on the airfoil and the casing plate as well as far field pressure in fan-OGV secondary flows, not to mention compressor, turbine, and combustion noise that are believed important but not acoustically since the azimuthal velocity is much lower at the hub; stator self noise

Paris-Sud XI, Université de

408

Detection of slow atoms confined in a Cesium vapor cell by spatially separated pump and probe laser beams  

E-Print Network (OSTI)

Detection of slow atoms confined in a Cesium vapor cell by spatially separated pump and probe laser distribution of atoms in a thermal gas is usually described through a Maxwell-Boltzman distribution of energy, and assumes isotropy. As a consequence, the probability for an atom to leave the surface under an azimuth

Boyer, Edmond

409

Measurement of flow harmonics with multi-particle cumulants in Pb+Pb collisions at ?s[subscript NN] = 2.76 TeV with the ATLAS detector  

E-Print Network (OSTI)

ATLAS measurements of the azimuthal anisotropy in lead–lead collisions at ?s[subscript NN] = 2.76 TeV are shown using a dataset of approximately 7 ? b [superscript ?1] collected at the LHC in 2010. The measurements are ...

Taylor, Frank E.

410

Concept tests: Wind tunnel tests in controlled wind Comparison tests: Free field comparison to 3D sonic anemometer  

E-Print Network (OSTI)

: Measurements with three 1D sonics and one azimuth sensor Advantage: Pure virginal wind in front of wind turbine, and for wind, power performance and loads verification Full scale tests: Measurements on 3,6MW wind turbineConcept tests: Wind tunnel tests in controlled wind Comparison tests: Free field comparison to 3D

411

Journal of Quantitative Spectroscopy & Radiative Transfer 64 (2000) 219}226  

E-Print Network (OSTI)

of the discrete-ordinates approximation to the transport equation in plane geometry. The Green's function of papers [1}3] concerning radiation-transport problems in plane geometry, linear-algebra techniques were of the Fourier-component (m50) problems basic to the general azimuth-dependent transport equation [6], and since

Siewert, Charles E.

412

SUBJECT INDEX advection, pore water, A:3031  

E-Print Network (OSTI)

, A:29 Atlantic Ocean, hydrothermal processes, B2:1­12 Azimuthal Resistivity Imager, Site 395A, A:4 calcium pore water, A:31 vs. depth, A:32 caliper logs, vs. depth, A:18; B2:10 carbonate content. depth, A:31, 33 computed gamma ray logs, vs. depth, A:19 crust, oceanic, off-axis hydrothermal processes

413

Influence of weather conditions on the flight of migrating black storks  

Science Journals Connector (OSTI)

...parameters (temperature, humidity, wind direction, thermal convection...significant rise in flight speed, but wind often produced a side azimuth...wild turkey population. J. Wildlife Manage. 47, 281-290...Leshem 2003 b The effect of wind, season and latitude on the...

2010-01-01T23:59:59.000Z

414

Jet Measurements and Extraction of the Strong Coupling Constant at HERA  

E-Print Network (OSTI)

Results on jet measurements in neutral current deep inelastic scattering at HERA are presented. The low-$x_{Bj}$ and low-$Q^2$ region is explicitly investigated using forward jet production and the azimuthal asymmetry between jets in dijet production. Recent results on the determination of the strong coupling constant, $\\alpha_s(M_Z)$, are discussed.

A. A. Savin

2005-05-22T23:59:59.000Z

415

Charge Correlation in Near Side Hadron-Hadron Jets at sqrt(sNN)=200GeV in PHENIX  

E-Print Network (OSTI)

We analyze the relative azimuthal ($\\Delta\\phi$) distribution of same-charge and opposite-charge particle pairs. We then remove elliptic flow background using the ZYAM method. Comparisons between near angle $\\Delta\\phi$ peak widths are presented for various centralities.

A. Kravitz

2006-01-31T23:59:59.000Z

416

Discrimination among Small Magnitude Events on Nevada Test Site  

Science Journals Connector (OSTI)

......among Small Magnitude Events on Nevada Test Site W. A. Peppin T. V. McEvilly...than 500 km) azimuthally about Nevada Test Site (NTS), allow investigation...August 1971 and its Aftershocks, Nevada Test Site, U.S.G.S. Paper 474-149......

W. A. Peppin; T. V. McEvilly

1974-05-01T23:59:59.000Z

417

Numerical simulation and analysis of plasma turbulence the Large Plasma M. V. Umansky,1,b)  

E-Print Network (OSTI)

spectra exhibit direct and inverse cascades in both azimuthal and axial wavenumbers and indicate coupling applications and beyond. In particular, designing magnetic fusion reactors could be done more effi- ciently, these devices are highly diagnosable, providing for detailed comparison against code predictions. A relatively

California at Los Angles, University of

418

Complex component analysis of shear-wave splitting: case studies  

Science Journals Connector (OSTI)

......geophones (Bush & Crampin 1987). We shall process only the S1 offset at 272m. This case...of the two shear-wave arrivals. The process depends on the coherency of the polarization...azimuthal anisotropy, 56th Ann. h i . SEG Mtg, Houston, Expanded Abstracts, pp......

Xiang-Yang Li; Stuart Crampin

1991-12-01T23:59:59.000Z

419

Land Surface Reflectance: A Possible Earth Science  

E-Print Network (OSTI)

are in magenta, water bodies are outlined in white. MODIS Surface Reflectance South Africa From: E. Vermote, UMD information ­ Viewing geometry (view and solar zenith and azimuth angles) ­ Geolocation (lat 15, 2005 - Wolfe - San Diego 5 Target Communities · Land earth science community ­ Energy Balance

420

MICROSTRUCTURE AND CRYSTALLOGRAPHIC PREFERRED ORIENTATION (CPO) OF HEMATITE ORES FROM THE SISHEN MINE, NORTHERN CAPE PROVINCE, SOUTH AFRICA  

Science Journals Connector (OSTI)

...by neutron diffraction texture analysis was performed at the Research Centers Ja¼lich (Jansen et al., 2000) and GKSS Geesthacht (Brokmeier et al., 1998). The measured intensity data dependent on pole angle i and azimuth angle i are processed with...

H. SIEMES

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

A Doppler Radar Emulator with an Application to the Detectability of Tornadic Signatures  

E-Print Network (OSTI)

System (ARPS). Several metrics for tornado intensity are examined, including peak Doppler velocity range, if standard metrics such as azimuthal gate-to-gate shear from a single radar are used for detection. 1. Introduction The design of a weather radar system and its scan- ning strategy involves trade

Xue, Ming

422

Heliostat control  

SciTech Connect

An improvement in a system and method of controlling heliostat in which the heliostat is operable in azimuth and elevation by respective stepper motors and including the respective steps or means for calculating the position for the heliostat to be at a commanded position, determining the number of steps in azimuth and elevation for each respective motor to get to the commanded position and energizing both the azimuth and elevation stepper motors to run in parallel until predetermined number of steps away from the closest commanded position in azimuth and elevation so that the closest position has been achieved, and thereafter energizing only the remaining motor to bring it to its commanded position. In this way, the heliostat can be started from a stowed position in the morning and operated by a computer means to its commanded position and kept correctly oriented throughout the day using only the time of the day without requiring the usual sensors and feedback apparatus. A computer, or microprocessor, can then control a plurality of many heliostats easily and efficiently throughout the day.

Kaehler, James A. (Littleton, CO)

1984-01-01T23:59:59.000Z

423

Heliostat control  

SciTech Connect

An improvement in a system and method of controlling heliostat in which the heliostat is operable in azimuth and elevation by respective stepper motors and including the respective steps or means for calculating the position for the heliostat to be at a commanded position, determining the number of steps in azimuth and elevation for each respective motor to get to the commanded position and energizing both the azimuth and elevation stepper motors to run in parallel until predetermined number of steps away from the closest commanded position in azimuth and elevation so that the closest position has been achieved, and thereafter energizing only the remaining motor to bring it to its commanded position. In this way, the heliostat can be started from a stowed position in the morning and operated by a computer means to its commanded position and kept correctly oriented throughout the day using only the time of the day without requiring the usual sensors and feedback apparatus. A computer, or microprocessor, can then control a plurality of many heliostats easily and efficiently throughout the day.

Kaehler, J.A.

1984-04-03T23:59:59.000Z

424

JOURNAL OF GEOPHYSICAL RESEARCH, VOL. ???, XXXX, DOI:10.1029/, Characterization of Mars' Scandia Tholi moated1  

E-Print Network (OSTI)

resolution images show mantling and, rarely, boulder-11 rich layers. Azimuthally averaged radial profiles process was most significant in filling the basin? Possibilities include basaltic35 flood volcanism [Head & Kreslavsky, 2002], ocean sedimentation and catastrophic flood36 deposits [Fairen et al., 2003], debris flows

Kite, Edwin

425

Optical Rotatory and Circular Dichroic Scattering Werner Kaminsky,* Morten Andreas Geday, Javier Herreros-Cedres, and Bart Kahr*  

E-Print Network (OSTI)

Optical Rotatory and Circular Dichroic Scattering Werner Kaminsky,* Morten Andreas Geday, Javier, Washington 98195-1700 ReceiVed: June 23, 2002; In Final Form: NoVember 5, 2002 Optical effects are observed in regularly dyed crystals that serve to mimic optical rotation and circular dichroism by rotating the azimuth

Kaminsky, Werner

426

Jess S. Jackson Sustainable Winery Building WATER STORAGE  

E-Print Network (OSTI)

from an 8-foot-high CMU wall and concrete slab passively cool the structure ADAPTIVE TO NEW TECHNOLOGY and confirmed during commissioning). Daylighting helps keep the lighting loads reduced to a lighting power with a 150° azimuth. These panels are coupled with a SMA America Sunny Boy 5000-US inverter located

Schladow, S. Geoffrey

427

Continuous cryopump with a method for removal of solidified gases  

DOE Patents (OSTI)

An improved cryopump for the removal of gases from a high vacuum, comprising a cryopanel incorporating honeycomb structure, refrigerant means thermally connected to the cryopanel, and a rotatable channel moving azimuthally around an axis located near the center of the cryopanel, removing gases adsorbed within the honeycomb structure by subliming them and conducting them outside the vacuum vessel. 4 figs.

Carlson, L.W.; Herman, H.

1988-05-05T23:59:59.000Z

428

Identification and selection rules of the spin-wave eigen-modes in a normally magnetized nano-pillar  

E-Print Network (OSTI)

Identification and selection rules of the spin-wave eigen-modes in a normally magnetized nano nano-pillar (Permalloy-Copper-Permalloy) by means of a Magnetic Resonance Force Microscope (MRFM). We azimuthal index = 0, the RF cur- rent flowing through the nano-pillar, creating a circular RF Oersted field

429

Extinction Transition on a Pie  

E-Print Network (OSTI)

Extinction transition of bacteria under forced rotation is analyzed in pie geometry. Under convection, separation of the radial and the azimuthal degrees of freedom is not possible, and the linearized evolution operator is diagonalized numerically. Some characteristics scales are compared with the results of recent experiments, and the ``integrable'' limit of the theory at narrow growth region is analyzed.

Nadav M. Shnerb

2000-07-04T23:59:59.000Z

430

13th SAC ISTC Seminar "New Perspectives of High Energy Physics"  

E-Print Network (OSTI)

-fold azimuthal symmetry around the calorimeters. This fundamental choice has driven the design of the rest momentum measurements (with Si-tracker and pixels) Stand-alone electron identification TRANSITION RADIATION TRACKER BARREL END-CAPs Geometry Linear Radial Straw length 144 cm 39 cm Electronic channels ~ 105 000

431

Fluidic Control of a Turret Wake: Aerodynamic and Aero-Optical Effects  

E-Print Network (OSTI)

kinetic energy M = Mach number OPD = optical path difference OPDrms = root-mean-square of optical path; = azimuthal angle of pressure ports = elevation angle of optical aperture s = flow separation angle-based optical system must satisfy more demanding requirements in comparison to separation control over external

Gordeyev, Stanislav

432

Erratum: High-NA aberration retrieval with the Extended Nijboer-Zernike  

E-Print Network (OSTI)

of Technology, Lorentzweg 1, NL-2628 CJ Delft, The Netherlands P. Dirksen, A.J.E.M. Janssen Philips Research Europe, Professor Holstlaan 4, NL-5656 AA Eindhoven, The Netherlands In the paper "High-NA aberration regrettable notation errors are present in Eq.(10), page 06004-3. The expression gives the azimuthal Fourier

433

Weather Radar Monitoring using the Sun Iwan Holleman and Hans Beekhuis  

E-Print Network (OSTI)

the Do- minion Radio Astrophysical Observatory (DRAO) in Canada introduced the 10.7 cm solar flux monitor-272, 2004 #12;2 #12;Contents 1 Introduction 5 2 Detection of solar interferences 7 2.1 Solar artifacts and azimuthal averaging 13 2.5 Corrected solar power 15 3 Position of the sun 17 3.1 Celestial sphere

Stoffelen, Ad

434

Analytical description of the scattering of cellulose nanocrystals in tracheid wood cells  

Science Journals Connector (OSTI)

A model is described which allows the azimuthal X-ray diffraction pattern to be calculated for any hkl reflection of tracheid cells in any orientation. The same description can also be applied to fibers with an additional level of organization, e.g. twisted fibers.

Ogurreck, M.

2010-03-05T23:59:59.000Z

435

A theoretical study on area compensation for non-directly-south-facing solar collectors  

Science Journals Connector (OSTI)

Solar energy integrated with the building is an important approach for the synchronous development of solar energy and architecture. The energy gain of the solar collector integrated with the pitched roof has been greatly influenced by the roof azimuth and tilted angle. Investment cost of the collectors is mainly decided by the size of the collector area. Accordingly, it is significant for solar building design to economically determinate the area compensation of the solar collector at different azimuth and tilted angles. Take Kunming and Beijing as examples, area compensation for the flat-plate tube-fin solar collector used in southern regions and the evacuated tube collector with cylindrical absorbers used in northern regions in China have been theoretically calculated. The results to some extent show that the daily horizontal solar radiation, ambient temperature, the azimuth and tilted angle of the collector integrated into the roof have an influence on the area compensation. The azimuth angle and tilted angle of the roof are the main factors that influence the A/A0, which is defined as the collector area ratio of the non-south-facing collectors to the south-facing ones with the optimal tilted angle. Comparative studies found that the range of A/A0 for the evacuated tube collector used in the northern regions is close to that for the flat-plate tube-fin solar collector used in the southern regions. When the pitched roof tilted angle ? ? [25°, 45°] and the azimuth angle ??? ? 30°, the collectors can intercept a lot of solar radiant-energy. Considering the economic situations of the ordinary consumers in China, the optimal area compensation A/A0 ? 1.30 is recommended in this paper.

Sheng-Xian Wei; Li Ming; Xi-Zheng Zhou

2007-01-01T23:59:59.000Z

436

Effects of paleolatitude on coal quality - model for organic sulfur distribution in US coal  

SciTech Connect

In the conterminous US, most Carboniferous peats accumulated at latitudes of 0/degrees/-15/degrees/S, Cretaceous Rocky Mountain province peats at 30/degrees/-45/degrees/N, Tertiary northern Great Plains peats at 40/degrees/-55/degrees/N, and Tertiary Gulf Coast peats at 30/degrees/-40/degrees/N. Alaskan Cretaceous and Tertiary peats accumulated at latitudes above 70/degrees/N. A comparison of paleolatitudes calculated from paleomagnetic poles and organic sulfur contents for more than 7000 coal samples indicates that the higher the latitude in which a peat swamp developed, the lower the mean organic sulfur content of the subsequent coal (correlation coefficient - 0.4; significant at the 99% confidence level). Mean organic sulfur contents range from 0.90% (range = 0.01-5.08%, standard deviation = 0.56) in low-latitude Carboniferous coal to 0.25% (range = 0.01-1.41%, standard deviation = 0.23) in high-latitude Alaskan Cretaceous and Tertiary coal.

Affolter, R.H.; Stricker, G.D.

1989-03-01T23:59:59.000Z

437

A Comparative Study of RF and Induction Linac Approaches to Phase Rotation of a Muon Bunch in the Production Region of a muon + - muon- Collider  

E-Print Network (OSTI)

until pion decay is Fig.l: Muon energy versus arrival time.we therefore chose a pion/muon kinetic energy interval 50 toAs the pions/muons in this energy interval propagate a

Turner, W.C.

2011-01-01T23:59:59.000Z

438

High resolution data acquisition  

DOE Patents (OSTI)

A high resolution event interval timing system measures short time intervals such as occur in high energy physics or laser ranging. Timing is provided from a clock (38) pulse train (37) and analog circuitry (44) for generating a triangular wave (46) synchronously with the pulse train (37). The triangular wave (46) has an amplitude and slope functionally related to the time elapsed during each clock pulse in the train. A converter (18, 32) forms a first digital value of the amplitude and slope of the triangle wave at the start of the event interval and a second digital value of the amplitude and slope of the triangle wave at the end of the event interval. A counter (26) counts the clock pulse train (37) during the interval to form a gross event interval time. A computer (52) then combines the gross event interval time and the first and second digital values to output a high resolution value for the event interval.

Thornton, Glenn W. (Los Alamos, NM); Fuller, Kenneth R. (Los Alamos, NM)

1993-01-01T23:59:59.000Z

439

High resolution data acquisition  

DOE Patents (OSTI)

A high resolution event interval timing system measures short time intervals such as occur in high energy physics or laser ranging. Timing is provided from a clock, pulse train, and analog circuitry for generating a triangular wave synchronously with the pulse train (as seen in diagram on patent). The triangular wave has an amplitude and slope functionally related to the time elapsed during each clock pulse in the train. A converter forms a first digital value of the amplitude and slope of the triangle wave at the start of the event interval and a second digital value of the amplitude and slope of the triangle wave at the end of the event interval. A counter counts the clock pulse train during the interval to form a gross event interval time. A computer then combines the gross event interval time and the first and second digital values to output a high resolution value for the event interval.

Thornton, G.W.; Fuller, K.R.

1993-04-06T23:59:59.000Z

440

Modeling velocity dispersion In Gypsy site, Oklahoma  

E-Print Network (OSTI)

Discrepancies in interval velocities estimated from vertical well measurements made with different source central frequencies at Gypsy site could be primarily explained in terms of intrinsic attenuation. Four intervals ...

Alsaadan, Sami Ibrahim

2010-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

Feed Intake and Feeding Behavior Associations with Performance and Feed Efficiency of Feedlot Cattle Fed a Corn-based Diet  

E-Print Network (OSTI)

The objective of the first study was to determine which combination of bimodal (2-population) distribution models best fit non-feeding interval data to distinguish intervals within (1st population) and between (2nd population) meals in beef cattle...

Bailey, Jayton

2012-02-14T23:59:59.000Z

442

Study of Oil Degradation in Extended Idle Operation Heavy Duty Vehicles  

E-Print Network (OSTI)

Advances in engine oil technology and increased combustion efficiency has resulted in the longer oil intervals in vehicles. Current oil change interval practice only takes into account the mileage a vehicle has driven and does not consider other...

Kader, Michael Kirk

2013-01-18T23:59:59.000Z

443

Cyclic AMP modulates electrical signaling in a weakly electric fish  

Science Journals Connector (OSTI)

Electric fish are typically described as "pulse" or "wave" fish based on the regularity of the EOD. "Pulse" species produce brief EOD pulses at variable intervals with the interpulse ... interpulse interval are o...

L. McAnelly; A. Silva; H. H. Zakon

2003-04-01T23:59:59.000Z

444

Patterns of the electric organ discharge during courtship and spawning in the mormyrid fish, Pollimyrus isidori  

Science Journals Connector (OSTI)

Pollimyrus isidori's electric organ discharge (EOD) is of the pulse type. Patterns of EOD intervals were investigated prior to, during and...n=15) showed characteristic discharge interval pattern...

B. O. Bratton; B. Kramer

1989-06-01T23:59:59.000Z

445

A scale-free analysis of magnetic holes in the solar wind  

E-Print Network (OSTI)

Magnetic holes are isolated intervals of depleted interplanetary magnetic field (IMF) strength on timescales of several seconds to several hours. These intervals have been seen as often as several times per day in the ...

Stevens, M. L. (Michael Louis)

2006-01-01T23:59:59.000Z

446

E-Print Network 3.0 - antibodies predict relapse Sample Search...  

NLE Websites -- All DOE Office Websites (Extended Search)

relapse-free interval (hazard ratio (HR) 1.77, 95% confidence interval (CI): 1 Source: Price, Paul A. - Division of Biological Sciences, University of California at San Diego...

447

Independent Major -Undergraduate Post Graduate Activities Detail & History  

E-Print Network (OSTI)

Estimating Realistic Confidence Intervals for the Activation Energy Determined from of Chemistry, University of Utah, 315 South, 1400 East, Salt Lake City, Utah 84112 Astatisticalprocedureisproposedforestimatingrealistic confidence intervals for the activation energy determined by using an advanced isoconversional

Lipson, Michal

448

2013, Latin American Public Opinion Project www.AmericasBarometer.org  

E-Print Network (OSTI)

Suriname Guatemala Guyana 0 10 20 30 40 50 Trust in Iranian Government 95% Confidence Interval (Design

Bordenstein, Seth

449

MIT Big Data Challenge: Transportation in the City of Boston Model of Prediction Challenge  

E-Print Network (OSTI)

and for periods before and after the prediction interval. When available, the number of MBTA T rides at nearby

Oliva, Aude

450

The Development of Instrumentation and Methods for Measurement of Air-Sea Interaction and Coastal Processes from Manned and Unmanned Aircraft /  

E-Print Network (OSTI)

sonic anemometer (Campbell Scien- tific CSAT3). The vertical bar indicates the 95% confidence interval, calculated as described by Young (

Reineman, Benjamin D.

2013-01-01T23:59:59.000Z

451

The Development of Instrumentation and Methods for Measurement of Air-Sea Interaction and Coastal Processes from Manned and Unmanned Aircraft /  

E-Print Network (OSTI)

anemometer (Campbell Scien- tific CSAT3). The vertical bar indicates the 95% confidence interval, calculated as described by Young (

Reineman, Benjamin D.

2013-01-01T23:59:59.000Z

452

GEOLOGY | September 2014 | www.gsapubs.org 1 INTRODUCTION  

E-Print Network (OSTI)

temperature changes (Sun et al., 2012) may have contributed to the prolonged interval of recovery of marine

Saltzman, Matthew R.

453

THE LOMA PRIETA, CALIFORNIA, EARTHQUAKEOF OCTOBER 17,1989: EARTHQUAKEOCCURRENCE  

E-Print Network (OSTI)

variations in geothermal wells (Silver and Valette-Silver, 1987) or changes in the interval between eruption

Silver, Paul

454

Impact of water resource development on the hydrology and sedimentology of the Brazos River system  

E-Print Network (OSTI)

. Christopher C. Mathewson Major dam and reservoir development within the Brazos River Basin is correlative with a significant decrease in the suspended sediment load of the river and with increased coastal erosion rates near the delta. A hydrologic analysis... Interval 1: 1920' s ? 41. Interval 2: 1942 ? 51. . . . . . . ~ . . - - ~ ~ ~ ~ ~ ~ - ~ ~ Interval 5: 1952 ? 74. Interval 4: 1942 ? 74. Discharge Control During Flood Stages 20 25 25 25 51 54 54 SEDIMENTOLOGY. Suspended Load. Bed Load. Coastal...

Minter, Larry Lane

1976-01-01T23:59:59.000Z

455

PHYSICAL OCEANOGRAPHIC STUDIES OF NARRAGANSETT BAY, 1957 and 1958  

E-Print Network (OSTI)

thermometer attached to the Nansen bottle. A thermistor thermometer was used at every 1- or 2-meter interval

456

A parametric building energy cost optimization tool based on a genetic algorithm  

E-Print Network (OSTI)

........................................................64 Fig. 13. Two decision variables case 95% confidence intervals for genetic algorithm solution with population size P = 5.................................................67 Fig. 14. Two decision variables case 95% confidence intervals... for genetic algorithm solutions with population size P = 10 .............................................68 Fig. 15. Two decision variables case 95% confidence intervals for genetic algorithm solutions with population size P = 20...

Tan, Xiaowei

2007-09-17T23:59:59.000Z

457

Theoretical Population Biology 53, 256 271 (1998) Microsatellite Behavior with Range Constraints  

E-Print Network (OSTI)

Interval Research Corporation, Palo Alto, California 94304; and Department of Mathematical Biology Research Corporation, Palo Alto, CA 94304 Marcus W. Feldman Interval Research Corporation, Palo Alto and David B. Goldstein Interval Research Corporation, Palo Alto, CA 94304; and Department of Zoology

Pollock, David

458

Eastern Renewable Generation Integration Study Solar Dataset (Presentation)  

SciTech Connect

The National Renewable Energy Laboratory produced solar power production data for the Eastern Renewable Generation Integration Study (ERGIS) including "real time" 5-minute interval data, "four hour ahead forecast" 60-minute interval data, and "day-ahead forecast" 60-minute interval data for the year 2006. This presentation provides a brief overview of the three solar power datasets.

Hummon, M.

2014-04-01T23:59:59.000Z

459

Precipitable water structure in tropical systems as estimated from TOVS  

E-Print Network (OSTI)

and OLR . . . 28 67 85 6. Annual and semi-annual cycle effect estimates for selected areas . . . 89 LIST OF FIGURES Figure Page 1. PW fields from three models for 8 Feb 1988. Contour intervals are. 5 cm. . 34 2. PW fields from three models for 10... Feb 1988. Contour intervals are. 5 cm. 35 3. PW field for 9 Jan 1988. Contour intervals are . 5 cm. . 37 4. OLR field for 9 Jan 1988. Contour intervals are 25 Wm-2. . . . 38 5. PW fields from three models for 15 Aug 1990. Contour intervals are . 5...

Hatfield, Eric

2012-06-07T23:59:59.000Z

460

Local rollback for fault-tolerance in parallel computing systems  

DOE Patents (OSTI)

A control logic device performs a local rollback in a parallel super computing system. The super computing system includes at least one cache memory device. The control logic device determines a local rollback interval. The control logic device runs at least one instruction in the local rollback interval. The control logic device evaluates whether an unrecoverable condition occurs while running the at least one instruction during the local rollback interval. The control logic device checks whether an error occurs during the local rollback. The control logic device restarts the local rollback interval if the error occurs and the unrecoverable condition does not occur during the local rollback interval.

Blumrich, Matthias A. (Yorktown Heights, NY); Chen, Dong (Yorktown Heights, NY); Gara, Alan (Yorktown Heights, NY); Giampapa, Mark E. (Yorktown Heights, NY); Heidelberger, Philip (Yorktown Heights, NY); Ohmacht, Martin (Yorktown Heights, NY); Steinmacher-Burow, Burkhard (Boeblingen, DE); Sugavanam, Krishnan (Yorktown Heights, NY)

2012-01-24T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" 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

ARM - Datastreams - xsacrvpt  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsxsacrvpt Datastreamsxsacrvpt Documentation Data Quality Plots ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : XSACRVPT X-Band Scanning ARM Cloud Radar (XSACR) Vertically Pointing Scan Active Dates 2011.09.14 - 2013.07.29 Measurement Categories Cloud Properties Originating Instrument X-Band Scanning ARM Cloud Radar (XSACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Altitude m altitude Altitude above ground level m altitude_agl Antenna transition indicator, 1 if between sweeps, otherwise 0 unitless antenna_transition ( time ) Azimuth angle from true north degrees azimuth ( time )

462

ARM - Datastreams - 1290rwpwindmom  

NLE Websites -- All DOE Office Websites (Extended Search)

rwpwindmom rwpwindmom Documentation Data Quality Plots Citation DOI: 10.5439/1025032 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : 1290RWPWINDMOM 1290-MHz Radar Wind Profiler/RASS (RWP1290): wind moments Active Dates 2007.03.19 - 2012.03.31 Measurement Categories Cloud Properties Originating Instrument Radar Wind Profiler (RWP) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Base time in Epoch seconds since 1970-1-1 0:00:00 0:00 base_time Beam azimuth angle deg beam_azimuth ( time ) Beam elevation angle deg beam_elevation ( time )

463

ARM - Datastreams - 50rwpwindspec  

NLE Websites -- All DOE Office Websites (Extended Search)

rwpwindspec rwpwindspec Documentation Data Quality Plots ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : 50RWPWINDSPEC 50-MHz Radar Wind Profiler/RASS (RWP50): wind spectra Active Dates 2001.04.01 - 2006.05.04 Measurement Categories Aerosols, Cloud Properties Originating Instrument Radar Wind Profiler (50 MHz) (50RWP) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Base time in Epoch seconds since 1970-1-1 0:00:00 0:00 base_time Beam azimuth angle deg beam_azimuth ( time ) Beam elevation angle deg beam_elevation ( time ) Spectral bin number unitless bins ( bins )

464

ARM - Datastreams - dlrhi  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsdlrhi Datastreamsdlrhi Documentation Data Quality Plots Citation DOI: 10.5439/1046188 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : DLRHI Doppler LIDAR Range-Height Indicator scan Active Dates 2011.07.21 - 2012.03.31 Measurement Categories Aerosols, Cloud Properties Originating Instrument Doppler Lidar (DL) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Backscattered radiation Attenuated backscatter 1/(m sr) attenuated_backscatter ( time, range ) Azimuth relative to true north degrees azimuth ( time ) Base time in Epoch seconds since 1970-1-1 0:00:00 0:00 base_time

465

ARM - Datastreams - wsacrppi  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamswsacrppi Datastreamswsacrppi Documentation Data Quality Plots ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : WSACRPPI W-Band Scanning ARM Cloud Radar (W-SACR) PPI Scan Active Dates 2011.05.24 - 2013.12.10 Measurement Categories Cloud Properties Originating Instrument Scanning ARM Cloud Radar, tuned to W-Band (95GHz) (WSACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Altitude m altitude Altitude above ground level m altitude_agl Antenna transition indicator, 1 if between sweeps, otherwise 0 unitless antenna_transition ( time ) Azimuth angle from true north degrees azimuth ( time )

466

ARM - Datastreams - dlcal1  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsdlcal1 Datastreamsdlcal1 Documentation Data Quality Plots Citation DOI: 10.5439/1025183 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : DLCAL1 Doppler Lidar - calibration channel 1 Active Dates 2010.10.30 - 2010.12.21 Measurement Categories Aerosols, Cloud Properties Originating Instrument Doppler Lidar (DL) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Backscattered radiation Attenuated backscatter 1/(m sr) attenuated_backscatter ( time, range ) Azimuth relative to true north degrees azimuth ( time ) Base time in Epoch seconds since 1970-1-1 0:00:00 0:00 base_time

467

ARM - Datastreams - xsacrblrhi  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsxsacrblrhi Datastreamsxsacrblrhi Documentation Data Quality Plots ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : XSACRBLRHI X-Band Scanning ARM Cloud Radar (XSACR) Boundary Layer RHI Scan Active Dates 2011.09.14 - 2011.10.20 Measurement Categories Cloud Properties Originating Instrument X-Band Scanning ARM Cloud Radar (XSACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Altitude m altitude Altitude above ground level m altitude_agl Antenna transition indicator, 1 if between sweeps, otherwise 0 unitless antenna_transition ( time ) Azimuth angle from true north degrees azimuth ( time )

468

ARM - Datastreams - dlrhi2  

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Datastreamsdlrhi2 Datastreamsdlrhi2 Documentation Data Quality Plots Citation DOI: 10.5439/1025188 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : DLRHI2 Doppler Lidar - Range-Height Indicator #2 Active Dates 2010.10.21 - 2010.11.21 Measurement Categories Aerosols, Cloud Properties Originating Instrument Doppler Lidar (DL) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Backscattered radiation Attenuated backscatter 1/(m sr) attenuated_backscatter ( time, range ) Azimuth relative to true north degrees azimuth ( time ) Base time in Epoch seconds since 1970-1-1 0:00:00 0:00 base_time

469

ARM - Datastreams - xsacrawrhi  

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Datastreamsxsacrawrhi Datastreamsxsacrawrhi Documentation Data Quality Plots ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : XSACRAWRHI X-Band Scanning ARM Cloud Radar (XSACR) Along-Wind RHI Scan Active Dates 2011.09.14 - 2012.10.21 Measurement Categories Cloud Properties Originating Instrument X-Band Scanning ARM Cloud Radar (XSACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Altitude m altitude Altitude above ground level m altitude_agl Antenna transition indicator, 1 if between sweeps, otherwise 0 unitless antenna_transition ( time ) Azimuth angle from true north degrees azimuth ( time )

470

ARM - Datastreams - nimfr  

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Datastreamsnimfr Datastreamsnimfr Documentation Data Quality Plots Citation DOI: 10.5439/1025258 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Example nimfr Archive Data Plot Example nimfr Archive Data Plot Datastream : NIMFR Normal Incidence Multi-Filter Radiometer (NIMFR): direct normal irradiances Active Dates 1997.10.16 - 2014.01.09 Measurement Categories Radiometric Originating Instrument Normal Incidence Multifilter Radiometer (NIMFR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Airmass unitless airmass ( time ) Altitude above mean sea level m alt Azimuth angle degrees azimuth_angle ( time )

471

ARM - Datastreams - mfr10m  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsmfr10m Datastreamsmfr10m Documentation Data Quality Plots Citation DOI: 10.5439/1025224 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Example mfr10m Archive Data Plot Example mfr10m Archive Data Plot Datastream : MFR10M Multi-Filter Radiometer (MFR): upwelling irradiance at 10-meter height Active Dates 1994.03.26 - 2014.01.02 Measurement Categories Radiometric Originating Instrument Multifilter Radiometer (MFR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Airmass unitless airmass ( time ) Altitude above mean sea level m alt Azimuth angle degrees azimuth_angle ( time )

472

ARM - Datastreams - mwrp  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsmwrp Datastreamsmwrp Documentation Data Quality Plots Citation DOI: 10.5439/1025254 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : MWRP Microwave Radiometer data (MWR Profiles - QME), water vapor, temp, cloud liquid water, precip water retrievals Active Dates 2004.02.19 - 2014.01.01 Measurement Categories Atmospheric State, Cloud Properties Originating Instrument Microwave Radiometer Profiler (MWRP) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Azimuth angle degrees azimuth Base time in Epoch seconds since 1970-1-1 0:00:00 0:00 base_time

473

ARM - Datastreams - mwr3c  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsmwr3c Datastreamsmwr3c Documentation Data Quality Plots Citation DOI: 10.5439/1025248 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : MWR3C Microwave Radiometer, 3 Channel Active Dates 2011.01.11 - 2014.01.02 Measurement Categories Radiometric Originating Instrument Microwave Radiometer, 3 Channel (MWR3C) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Azimuth deg azimuth ( time ) Base time in Epoch seconds since 1970-1-1 0:00:00 0:00 base_time Elevation deg elevation ( time ) Hail accumulation hit/cm^2 hail_accumulation ( time )

474

Building Energy Software Tools Directory: Solar Rater  

NLE Websites -- All DOE Office Websites (Extended Search)

Solar Rater Solar Rater Solar Rater logo Solar Rater app for Android devices makes it easy to determine the solar energy potential for any location on Earth, and calculates the appropriate size for a photovoltaic (PV) system at that location. Key features include: Automatic location detection with GPS, Wi-Fi, or cell tower identification Automatic orientation detection measures the azimuth and pitch of solar panels Automatic magnetic declination conversion gives azimuth based on true north Automatic solar radiation determination based on location and orientation (model result) Outputs the appropriate size of a PV system in DC Watts Data can also be entered manually for offsite use Great teaching tool for novices Accurate results for solar energy professionals Outputs environmental benefits (e.g., greenhouse gas emissions,

475

ARM - Datastreams - mfr25m  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsmfr25m Datastreamsmfr25m Documentation Data Quality Plots Citation DOI: 10.5439/1025225 [ What is this? ] Generate Citation ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Example mfr25m Archive Data Plot Example mfr25m Archive Data Plot Datastream : MFR25M Multi-Filter Radiometer (MFR): upwelling irradiance at 25-meter height Active Dates 1994.04.17 - 2014.01.02 Measurement Categories Radiometric Originating Instrument Multifilter Radiometer (MFR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Airmass unitless airmass ( time ) Altitude above mean sea level m alt Azimuth angle degrees azimuth_angle ( time )

476

Single Spin Asymmetries in l p(transv. pol.) --> h X processes and transverse momentum dependent factorization  

SciTech Connect

Some estimates for the transverse Single Spin Asymmetry, A_N, in the inclusive processes l p(transv. Pol.) --> h X, given in a previous paper, are expanded and compared with new experimental data. The predictions are based on the Sivers distributions and the Collins fragmentation functions which fit the azimuthal asymmetries measured in Semi-Inclusive Deep Inelastic Scattering (SIDIS) processes (l p(transv. Pol.) --> l' h X). The factorisation in terms of Transverse Momentum Dependent distribution and fragmentation functions (TMD factorisation) -- i.e., the theoretical framework in which SIDIS azimuthal asymmetries are analysed -- is assumed to hold also for the inclusive process l p --> h X at large P_T. The values of A_N thus obtained agree in sign and shape with the data. Some predictions are given for future experiments.

Anselmino, Mauro; Boglione Mariaelena; D'Alesio, Umberto; Melis, Stefano; Murgia, Francesco; Prokudin, Alexey [JLAB

2014-06-01T23:59:59.000Z

477

Estimation of Heavy Ion Densities From Linearly Polarized EMIC Waves At Earth  

SciTech Connect

Linearly polarized EMIC waves are expected to concentrate at the location where their wave frequency satisfies the ion-ion hybrid (IIH) resonance condition as the result of a mode conversion process. In this letter, we evaluate absorption coefficients at the IIH resonance in the Earth geosynchronous orbit for variable concentrations of helium and azimuthal and field-aligned wave numbers in dipole magnetic field. Although wave absorption occurs for a wide range of heavy ion concentration, it only occurs for a limited range of azimuthal and field-aligned wave numbers such that the IIH resonance frequency is close to, but not exactly the same as the crossover frequency. Our results suggest that, at L = 6.6, linearly polarized EMIC waves can be generated via mode conversion from the compressional waves near the crossover frequency. Consequently, the heavy ion concentration ratio can be estimated from observations of externally generated EMIC waves that have polarization.

Kim, Eun-Hwa; Johnson, Jay R.; Lee, Dong-Hun

2014-02-24T23:59:59.000Z

478

Apparatus and method for mapping an area of interest  

DOE Patents (OSTI)

An apparatus and method are provided for mapping an area of interest using polar coordinates or Cartesian coordinates. The apparatus includes a range finder, an azimuth angle measuring device to provide a heading and an inclinometer to provide an angle of inclination of the range finder as it relates to primary reference points and points of interest. A computer is provided to receive signals from the range finder, inclinometer and azimuth angle measurer to record location data and calculate relative locations between one or more points of interest and one or more primary reference points. The method includes mapping of an area of interest to locate points of interest relative to one or more primary reference points and to store the information in the desired manner. The device may optionally also include an illuminator which can be utilized to paint the area of interest to indicate both points of interest and primary points of reference during and/or after data acquisition.

Staab, Torsten A. (Los Alamos, NM) Cohen, Daniel L. (Ithaca, NY); Feller, Samuel (Fairfax, VA)

2009-12-01T23:59:59.000Z

479

Detailed HBT measurements with respect to the event plane and collision energy in Au+Au collisions at PHENIX  

E-Print Network (OSTI)

The azimuthal dependence of 3D HBT radii relative to the event plane gives us information about the source shape at freeze-out. It also provides information on the system's evolution by comparing it to the initial source shape. In recent studies, higher harmonic event planes and flow have been measured at RHIC and the LHC, which result primarily from spatial fluctuations of the initial density across the collision area. If the shape caused by initial fluctuations still exists at freeze-out, the HBT measurement relative to higher order event plane may show these features. We present recent results of azimuthal HBT measurements relative to $2^{nd}$- and $3^{rd}$-order event planes in Au+Au 200 GeV collisions with the PHENIX experiment. Recent HBT measurements at lower energies will be also shown and compared with the 200 GeV result.

Takafumi Niida for the PHENIX Collaboration

2013-04-10T23:59:59.000Z

480

3-D GRMHD Simulations of Generating Jets  

E-Print Network (OSTI)

We have performed a first fully 3-D GRMHD simulation with Schwarzschild black hole with a free falling corona. The initial simulation results show that a jet is created as in the previous simulations using the axisymmetric geometry with the mirror symmetry at the equator. However, the time to generate the jet is longer than in the 2-D axisymmetric simulations. We expect that due to the additional freedom in the azimuthal dimension without axisymmetry with respect to the z axis and reflection symmetry with respect to the equatorial plane, the dynamics of jet formation can be modified. Further simulations are required for the study of instabilities along the azimuthal direction such as accretion-eject instability

Nishikawa, K I; Shibata, K; Kudoh, T; Sol, H

2002-01-01T23:59:59.000Z

Note: This page contains sample records for the topic "30-degree azimuth intervals" from the National Library of EnergyBeta (NLEBeta).
While these samples are representative of the content of NLEBeta,
they are not comprehensive nor are they the most current set.
We encourage you to perform a real-time search of NLEBeta
to obtain the most current and comprehensive results.


481

3-D GRMHD Simulations of Generating Jets  

E-Print Network (OSTI)

We have performed a first fully 3-D GRMHD simulation with Schwarzschild black hole with a free falling corona. The initial simulation results show that a jet is created as in the previous simulations using the axisymmetric geometry with the mirror symmetry at the equator. However, the time to generate the jet is longer than in the 2-D axisymmetric simulations. We expect that due to the additional freedom in the azimuthal dimension without axisymmetry with respect to the z axis and reflection symmetry with respect to the equatorial plane, the dynamics of jet formation can be modified. Further simulations are required for the study of instabilities along the azimuthal direction such as accretion-eject instability

K. -I. Nishikawa; S. Koide; K. Shibata; T. Kudoh; H. Sol

2002-08-05T23:59:59.000Z

482

Beam Energy and System Size Dependence of Dynamical Net Charge Fluctuations  

SciTech Connect

We present measurements of net charge fluctuations in Au + Au collisions at {radical}s{sub NN} = 19.6, 62.4, 130, and 200 GeV, Cu + Cu collisions at {radical}s{sub NN} = 62.4, 200 GeV, and p + p collisions at {radical}s = 200 GeV using the dynamical net charge fluctuations measure {nu}{sub {+-},dyn}. We observe that the dynamical fluctuations are non-zero at all energies and exhibit a modest dependence on beam energy. A weak system size dependence is also observed. We examine the collision centrality dependence of the net charge fluctuations and find that dynamical net charge fluctuations violate 1/N{sub ch} scaling, but display approximate 1/N{sub part} scaling. We also study the azimuthal and rapidity dependence of the net charge correlation strength and observe strong dependence on the azimuthal angular range and pseudorapidity widths integrated to measure the correlation.

STAR Coll

2008-07-21T23:59:59.000Z

483

ARM - Datastreams - xsacrcwrhi  

NLE Websites -- All DOE Office Websites (Extended Search)

Datastreamsxsacrcwrhi Datastreamsxsacrcwrhi Documentation Data Quality Plots ARM Data Discovery Browse Data Comments? We would love to hear from you! Send us a note below or call us at 1-888-ARM-DATA. Send Datastream : XSACRCWRHI X-Band Scanning ARM Cloud Radar (XSACR) Cross-Wind RHI Scan Active Dates 2011.09.14 - 2012.10.21 Measurement Categories Cloud Properties Originating Instrument X-Band Scanning ARM Cloud Radar (XSACR) Measurements Only measurements considered scientifically relevant are shown below by default. Show all measurements Measurement Units Variable Altitude above mean sea level m alt Altitude m altitude Altitude above ground level m altitude_agl Antenna transition indicator, 1 if between sweeps, otherwise 0 unitless antenna_transition ( time ) Azimuth angle from true north degree azimuth ( time )

484

Axisymmetric Plasma-Optic Mass Separators  

SciTech Connect

A systematic description is given of the principles of operation of axisymmetric plasma-optic mass separators with azimuthators that are compatible with stationary plasma thrusters with closed electron drift. Two schemes of plasma-optic separators (with electrostatic and with magnetic ion focusing) are considered. Results are presented from calculations of the parameters of model devices for separating ions whose masses are on the order of those of xenon ions.

Morozov, A.I. [Nuclear Fusion Institute, Russian Research Centre Kurchatov Institute, pl. Kurchatova 1, Moscow, 123182 (Russian Federation); Savel'ev, V.V. [Keldysh Institute of Applied Mathematics, Russian Academy of Sciences, Miusskaya pl. 4, Moscow, 125047 (Russian Federation)

2005-05-15T23:59:59.000Z

485

On the role of the Sivers effect in A{sub N} for inclusive particle production in pp collisions  

SciTech Connect

Single spin asymmetries, A{sub N} , for inclusive particle production in pp collisions are considered within a generalized parton model with inclusion of spin and tranverse momentum effects. We consider the potential role of the Sivers effect in A{sub N} , as extracted from a careful analysis of azimuthal asymmetries in SIDIS, and discuss its phenomenological consequences in connection with a recently updated study of the Collins effect.

Anselmino, Mauro [INFN-Torino (Italy); Boglione, Mariaelena [INFN-Torino (Italy); D'Alesio, Umberto [INFN Cagliari (Italy); Melis, Stefano [INFN-Torino (Italy); Murgia, Francesco [INFN Cagliari (Italy); Prokudin, Alexei [JLAB, Newport News, VA (United States)

2014-01-01T23:59:59.000Z

486

Extraction of Transversity and Collins Functions  

SciTech Connect

We present a global re-analysis of recent experimental data on azimuthal asymmetries in semi-inclusive deep inelastic scattering, from the HERMES and COMPASS Collaborations, and in e{sup +}e{sup -} --> h_1h_2X processes, from the Belle Collaboration. The transversity distribution and the Collins functions are extracted simultaneously, in a revised analysis which also takes into account a new parameterization of the unknown functions.

Anselmino, Mauro [INFN-Torino (Italy); Boglione, Mariaelena [INFN-Torino (Italy); D'Alesio, Umberto [INFN Cagliari (Italy); Melis, Stefano [INFN-Torino (Italy); Murgia, Francesco [INFN Cagliari (Italy); Prokudin, Alexei [JLAB, Newport News, VA (United States)

2014-01-01T23:59:59.000Z

487

A_N in inclusive lepton-proton collisions  

SciTech Connect

Some estimates for the transverse single spin asymmetry, A_N, in the inclusive processes l p(transv. Pol.) -> h X are compared with new experimental data. The calculations are based on the Sivers and Collins functions as extracted from SIDIS azimuthal asymmetries, within a transverse momentum dependent factorization approach. The values of A_N thus obtained agree in sign and shape with the data. Predictions for future experiments are also given.

Prokudin, Alexey; Anselmino, Mauro; Boglione, Mariaelena; D'Alesio, Umberto; Melis, Stefano; Murgia, Francesco

2014-11-01T23:59:59.000Z

488

Austin chalk fracture mapping using frequency data derived from seismic data  

E-Print Network (OSTI)

and below the fractured layer. The Austin Chalk in South Central Texas is a fractured layer, and it produces hydrocarbons from fracture zones with the layer (Sweet Spots). 2D and 3 D P-wave seismic data are used from Burleson and Austin Counties... showing how azimuths were taken for the two additional data sets derived from the initial 3 D data..............??????????..........18 Figure 9. Burleson County 2D data represented as line locations...........????..?.20 Figure 10. Seismic section...

Najmuddin, Ilyas Juzer

2004-09-30T23:59:59.000Z

489

Studies of QCD at the Tevatron with the D0 detector  

SciTech Connect

QCD studies at Fermilab`s Tevatron encompass a rich variety of topics. We present some of the latest results from the D0 experiment including probes of the standard model given by the inclusive jet cross section, the dijet invariant mass spectrum and several studies with direct photons. To complement these probes, we also present new results from precision examinations of the color interactions including studies of color coherence and jet azimuthal decorrelation. 22 refs., 14 figs.

Stephens, R.W. [Texas Univ., Arlington, TX (United States); D0 Collaboration

1996-12-01T23:59:59.000Z

490

Electric field in 3D gravity with torsion  

E-Print Network (OSTI)

It is shown that in static and spherically symmetric configurations of the system of Maxwell field coupled to 3D gravity with torsion, at least one of the Maxwell field components has to vanish. Restricting our attention to the electric sector of the theory, we find an interesting exact solution, corresponding to the azimuthal electric field. Its geometric structure is to a large extent influenced by the values of two different central charges, associated to the asymptotic AdS structure of spacetime.

M. Blagojevi?; B. Cvetkovi?

2008-09-01T23:59:59.000Z

491

Mach number correlation for a two-dimensional helicopter rotor-blade analysis in the tip region  

E-Print Network (OSTI)

. Comparison of chordwise pressure distributions between TRANDES and flight test (TAAT) results. Flight condition B, P = 90 degrees, radius = 86. 4 percent 16 17 3 c. Comparison of chordwise pressure distributions between TRANDES and flight test (TAAT.... 066 CP/SIG = 0. 008 Figure 3 c. Comparison of chordwise TRANDES and flight test 90 degrees, radius AZIMUTH = 90. 0 / RADIUS = 91. 0 MRCH NQ. (QRTRHAPI = 0. 813 CN = 0. 104 RLP(TRRNDESI = 0. 414 pressure distributions between (TAAT) results...

Schillings, John Joseph

1983-01-01T23:59:59.000Z

492

Mach number dependence of the coherent structure in high speed subsonic jets  

E-Print Network (OSTI)

by Armstrong , morrison 32 and Nattanachayakul , and the current investigation. The 33 two later investigations used two hot-wire probes positioned at the radial location of maximum flow fluctuation level with an azimuthal separation of 180 0 Armstrong... 12 X/0 :-igure 21. Axial phase distributions, . '1=0. 8 figures show that all frequencies studied were coherent over the same region of the jet. This result was also observable in the data of Armstrong . Since the 32 frequencies studied included...

Whitaker, Kevin William

1982-01-01T23:59:59.000Z

493

Spatiotemporal Signal Analysis via the Phase Velocity Transform  

Science Journals Connector (OSTI)

The phase velocity transform (PVT) is an integral transform that divides a function of space and time into components that propagate at uniform phase velocities without distortion. This paper examines the PVT as a method to analyze spatiotemporal fluctuation data. The transform is extended to systems with discretely sampled data on a periodic domain, and applied to data from eight azimuthally distributed probes on the Sustained Spheromak Physics Experiment (SSPX). This reveals features not shown by Fourier analysis, particularly regarding nonsinusoidal mode structure.

Nathan Mattor

2000-06-26T23:59:59.000Z

494

Mechanical Measurements of the ALMA Prototype Antennas  

E-Print Network (OSTI)

The specifications of the Atacama Large Millimeter Array (ALMA) have placed stringent requirements on the mechanical performance of its antennas. As part of the evaluation process of the VertexRSI and Alcatel EIE Consortium (AEC) ALMA prototype antennas, measurements of the path length, thermal, and azimuth bearing performance were made under a variety of weather conditions and observing modes. The results of mechanical measurements, reported here, are compared to the antenna specifications.

A. Greve; J. G. Mangum

2007-10-30T23:59:59.000Z

495

Spherical waves r Legendre polynomials  

E-Print Network (OSTI)

1 Impedance · Spherical waves r er e e Impedance · Legendre polynomials P0(x) = 1 P1(x) = x P2(x · Spherical waves ­ Spherical Hankel functions hn (2)(kr)=jn(kr)-iyn(kr) Impedance · Spherical waves Order: 0 1 4 Circumferential And azimuthal: 0,0 1,1 3,2 #12;3 Impedance · Spherical waves ­ Arbitrary

Berlin,Technische Universität

496

A fast method for solving both the time-dependent Schroedinger equation in angular coordinates and its associated 'm-mixing' problem  

SciTech Connect

An efficient split-operator technique for solving the time-dependent Schroedinger equation in an angular coordinate system is presented, where a fast spherical harmonics transform accelerates the conversions between angle and angular momentum representations. Unlike previous techniques, this method features facile inclusion of azimuthal asymmetries (solving the ''m-mixing'' problem), adaptive time stepping, and favorable scaling, while simultaneously avoiding the need for both kinetic and potential energy matrix elements. Several examples are presented.

Reuter, Matthew G.; Ratner, Mark A.; Seideman, Tamar [Department of Chemistry, Northwestern University, Evanston, Illinois 60208-3113 (United States)

2009-09-07T23:59:59.000Z

497

Probing High Parton Densities at Low-$x$ in d+Au Collisions at PHENIX Using the New Forward and Backward Muon Piston Calorimeters  

E-Print Network (OSTI)

The new forward Muon Piston Calorimeters allow PHENIX to explore low-$x$ parton distributions in d+Au collisions with hopes of observing gluon saturation. We present a two-particle azimuthal $\\Delta \\phi$ correlation measurement made between a mid-rapidity particle ($|\\eta_1| < 0.35$) and a forward $\\pi^0$ ($3.1 < \\eta_2 < 3.9$) wherein we compare correlation widths in d+Au to p+p and compute $I_{dA}$.

Beau Meredith

2009-09-29T23:59:59.000Z

498

Decomposition of harmonic and jet contributions to particle-pair correlations at ultrarelativistic energies  

SciTech Connect

Methodology is presented for analysis of two-particle azimuthal angle correlation functions obtained in collisions at ultrarelativistic energies. We show that harmonic and di-jet contributions to these correlation functions can be reliably decomposed by two techniques to give an accurate measurement of the jet-pair distribution. Results from detailed Monte Carlo simulations are used to demonstrate the efficacy of these techniques in the study of possible modifications to jet topologies in heavy ion reactions.

Ajitanand, N.N.; Alexander, J.M.; Chung, P.; Holzmann, W.G.; Issah, M.; Lacey, Roy A.; Shevel, A.; Taranenko, A.; Danielewicz, P. [Department of Chemistry, State University of New York at Stony Brook, Stony Brook, New York 11794 (United States); Michigan State University, East Lansing, Michigan 48824-1321 (United States)

2005-07-01T23:59:59.000Z

499

Decomposition of Harmonic and Jet Contributions to Particle-pair Correlations at Ultra-relativistic Energies  

E-Print Network (OSTI)

Methodology is presented for analysis of two-particle azimuthal angle correlation functions obtained in collisions at ultra-relativistic energies. We show that harmonic and di-jet contributions to these correlation functions can be reliably decomposed by two techniques to give an accurate measurement of the jet-pair distribution. Results from detailed Monte Carlo simulations are used to demonstrate the efficacy of these techniques in the study of possible modifications to jet topologies in heavy ion reactions.

N. N. Ajitanand; J. M. Alexander; P. Chung; W. G. Holzmann; M. Issah; Roy A. Lacey; A. Shevel; A. Taranenko; P. Danielewicz

2005-01-25T23:59:59.000Z

500

Control system for heliostats and method  

SciTech Connect

A control system and method for a heliostat or a system of heliostats which operates to maintain the sunbeam properly centered with respect to an associated tracking head and tracks the sun for proper elevational and azimuthal orientation of the heliostat. The tracking date is stored in memory and utilized to reset the heliostat at night for proper orientation during the next days tracking and/or for proper orientation during sunless periods of the day. Each heliostat is therefore self-tracking.

Gerwin, H. L.

1985-05-28T23:59:59.000Z