National Library of Energy BETA

Sample records for balls bran ch

  1. Glass balls

    E-Print Network [OSTI]

    There is a building with 100 floors in it, and glass balls, and an integer k with the following property. If one drops a glass ball from the floor number k or higher, ...

  2. Ball Moss 

    E-Print Network [OSTI]

    Crow, William T.

    2000-04-18

    Ball moss is a bromeliad that grows on trees. It is not a parasite and does not take nutrients from trees. It can be controlled, if desired, by mechanical removal or by applying fungicides that contain copper.

  3. Biomass Rapid Analysis Network (BRAN)

    SciTech Connect (OSTI)

    Not Available

    2003-10-01

    Helping the emerging biotechnology industry develop new tools and methods for real-time analysis of biomass feedstocks, process intermediates and The Biomass Rapid Analysis Network is designed to fast track the development of modern tools and methods for biomass analysis to accelerate the development of the emerging industry. The network will be led by industry and organized and coordinated through the National Renewable Energy Lab. The network will provide training and other activities of interest to BRAN members. BRAN members will share the cost and work of rapid analysis method development, validate the new methods, and work together to develop the training for the future biomass conversion workforce.

  4. People's Physics Book Ch 20-1 The Big Ideas

    E-Print Network [OSTI]

    California at Santa Cruz, University of

    People's Physics Book Ch 20-1 The Big Ideas Einstein believed that the laws of physics do of physics. In other words, if you are on a moving train and drop a ball or if you are standing on a farm and drop a ball, the physics that describe the motion of that ball will be the same. Einstein realized

  5. Ball valve extractor

    DOE Patents [OSTI]

    Herndon, Charles (Walterboro, SC); Brown, Roger A. (North Augusta, SC)

    2002-01-01

    An apparatus and process for removing a ball valve is provided. The ball valve removal tool provides a handle sliding along the length of a shaft. One end of the shaft is secured within an interior cavity of a ball valve while the opposite end of the shaft defines a stop member. By providing a manual sliding force to the handle, the handle impacts the stop member and transmits the force to the ball valve. The direction of the force is along the shaft of the removal tool and disengages the ball valve from the ball valve housing.

  6. Brans-Dicke cylindrical wormholes

    SciTech Connect (OSTI)

    Eiroa, Ernesto F.; Simeone, Claudio

    2010-10-15

    Static axisymmetric thin-shell wormholes are constructed within the framework of the Brans-Dicke scalar-tensor theory of gravity. Examples of wormholes associated with vacuum and electromagnetic fields are studied. All constructions must be threaded by exotic matter, except in the case of geometries with a singularity of finite radius, associated with an electric field, which can have a throat supported by ordinary matter. These results are achieved with any of the two definitions of the flare-out condition considered.

  7. Theory of ball lightning

    E-Print Network [OSTI]

    Wu, H -C

    2014-01-01

    We present a comprehensive explanation on ball lightning, a luminous sphere occasionally witnessed after ordinary lightning. In the last decade, it has been well established that natural lightning routinely generates relativistic electrons, which account for observed x rays. So we assume that, in a ball lightning event, a well-defined relativistic electron bunch is produced by the stepped leader of lightning. When this electron bunch strikes various media, a powerful microwave pulse is emitted by the coherent transition radiation mechanism. This intense microwave ionizes air, evacuates plasmas by its radiation pressure to form a globular plasma cavity, and then gets trapped inside the cavity. This theory successfully explains all characteristics of ball lightning, especially the appearance of ball lightning in fully-screened aircraft. Moreover, the proposed radiation mechanism fully explains the strongest radio signals from lightning and nanosecond spikes in the signals are direct evidences on the generation ...

  8. Tunguska Dark Matter Ball

    E-Print Network [OSTI]

    C. D. Froggatt; H. B. Nielsen

    2015-05-10

    It is suggested that the Tunguska event in June 1908 cm-large was due to a cm-large ball of a condensate of bound states of 6 top and 6 anti-top quarks containing highly compressed ordinary matter. Such balls are supposed to make up the dark matter as we earlier proposed. The expected rate of impact of this kind of dark matter ball with the earth seems to crudely match a time scale of 200 years between the impacts. The main explosion of the Tunguska event is explained in our picture as material coming out from deep within the earth, where it has been heated and compressed by the ball penetrating to a depth of several thousand km. Thus the effect has some similarity with volcanic activity as suggested by Kundt. We discuss the possible identification of kimberlite pipes with earlier Tunguska-like events. A discussion of how the dark matter balls may have formed in the early universe is also given.

  9. Eddy Current Model of Ball Lightning

    E-Print Network [OSTI]

    Shelton, J D

    2011-01-01

    Eddy Current Model of Ball Lightning Calculations show that high-energy ball lightning may consist of a ball of plasma containing a large circular electric current arising as an eddy current generated by lightning. Synthetic ball lightning might serve as a method of plasma confinement for purposes of nuclear fusion. In this paper, three articles concerning ball lightning and the related phenomenon of large ball lightning are combined to provide insight into this rarely glimpsed occurrence.

  10. Eddy Current Model of Ball Lightning

    E-Print Network [OSTI]

    J. D. Shelton

    2011-02-07

    Eddy Current Model of Ball Lightning Calculations show that high-energy ball lightning may consist of a ball of plasma containing a large circular electric current arising as an eddy current generated by lightning. Synthetic ball lightning might serve as a method of plasma confinement for purposes of nuclear fusion. In this paper, three articles concerning ball lightning and the related phenomenon of large ball lightning are combined to provide insight into this rarely glimpsed occurrence.

  11. Supersymmetry Breaking and Fermi Balls

    E-Print Network [OSTI]

    J. R. Morris; D. Bazeia

    1996-07-22

    A simple model is presented where the disappearance of domain walls and the associated production of ``Fermi balls'', which have been proposed as candidates for cold dark matter, are features which arise rather naturally in response to softly broken supersymmetry.

  12. A Quintessence Scalar Field in Brans-Dicke Theory

    E-Print Network [OSTI]

    Narayan Banerjee; and Diego Pavon

    2000-12-27

    It is shown that a minimally coupled scalara field in Brans-Dicke theory yields a non-decelerated expansion for the present universe for open, flat and closed Friedmann-Robertson-Walker models.

  13. Exact Vacuum Solutions of Jordan, Brans-Dicke Field Equations

    E-Print Network [OSTI]

    Sergey Kozyrev

    2005-12-04

    We present the static spherically symmetric vacuum solutions of the Jordan, Brans-Dicke field equations. The new solutions are obtained by considering a polar Gaussian, isothermal and radial hyperbolic metrics.

  14. Spectra of Relic Gravitons and Brans-Dicke Theory

    E-Print Network [OSTI]

    B. K. Sahoo

    2004-06-11

    The spectra of relic gravitational waves produced as a result of cosmological expansion of the inflationary models are derived in Brans-Dicke theory of gravity.The time dependence of the very early Hubble parameter and matter energy density are derived from frequency dependent spectrum of relic gravitational waves.Also it is found that Brans-Dicke scalar field contributes to the energy density of relic gravitons.

  15. FIRST EXPERIMENTS WITH THE PLASTIC BALL

    E-Print Network [OSTI]

    Gutbrod, H.H.

    2010-01-01

    FIRST EXPERIMENTS WITH THE PLASTIC BALL H.H. Gutbrod, A.scheme for one module Plastic Soil Response (based on protonS Ropidity ——» Fig. 3. Plastic Ball acceptance in the plane

  16. A model of the ball lightning

    E-Print Network [OSTI]

    Ignatovich, V K

    1992-01-01

    The ball lightning is supposed to be a shock wave of a point explosion frozen with electrostriction forces of the internal strong laser discharge. The life time of the ball with modest parameters is calculated.

  17. A model of the ball lightning

    E-Print Network [OSTI]

    Vladimir K. Ignatovich

    2011-09-05

    The ball lightning is supposed to be a shock wave of a point explosion frozen with electrostriction forces of the internal strong laser discharge. The life time of the ball with modest parameters is calculated.

  18. Vacuum less global monopole in Brans-Dicke theory

    E-Print Network [OSTI]

    F. Rahaman; M. Kalam; R. Mukherjee; S. Das; T. Roy

    2007-02-28

    In the present work, the gravitational field of a vacuum less global monopole has been investigated in Brans-Dicke theory under weak field assumption of the field equations. It has been shown that the vacuum less global monopole exerts attractive gravitational effects on a test particle. It is dissimilar to the case studied in general relativity.

  19. Functionality of alkaline cooked corn bran on tortilla texture 

    E-Print Network [OSTI]

    Guajardo Flores, Sara

    1998-01-01

    The effect of pericarp and nixtamalized corn bran (NCB) level on corn tortilla attributes was evaluated. The effect of varying pH (4, 9 and 11) on fresh and dry mesa flour (pH 5, 7 and 10) tortillas was also evaluated. Nixtamal was washed at three...

  20. Ball Packings with Periodic Constraints

    E-Print Network [OSTI]

    Robert Connelly; Jeffrey D. Shen; Alexander D. Smith

    2013-01-04

    We call a periodic ball packing in d-dimensional Euclidean space periodically (strictly) jammed with respect to a period lattice if there are no nontrivial motions of the balls that preserve the period (that maintain some period with smaller or equal volume). In particular, we call a packing consistently periodically (strictly) jammed if it is periodically (strictly) jammed on every one of its periods. After extending a well-known bar framework and stress condition to strict jamming, we prove that a packing with period Lambda is consistently strictly jammed if and only if it is strictly jammed with respect to Lambda and consistently periodically jammed. We next extend a result about rigid unit mode spectra in crystallography to characterize periodic jamming on sublattices. After that, we prove that there are finitely many strictly jammed packings of m unit balls and other similar results. An interesting example shows that the size of the first sublattice on which a packing is first periodically unjammed is not bounded. Finally, we find an example of a consistently periodically jammed packing of low density \\delta = \\frac{4 \\pi}{6 \\sqrt{3} + 11} + \\epsilon ~ 0.59, where \\epsilon is an arbitrarily small positive number. Throughout the paper, the statements for the closely related notions of periodic infinitesimal rigidity and affine infinitesimal rigidity for tensegrity frameworks are also given.

  1. Ball feeder for replenishing evaporator feed

    DOE Patents [OSTI]

    Felde, David K. (Oak Ridge, TN); McKoon, Robert H. (San Ramon, CA)

    1993-01-01

    Vapor source material such as uranium, which is to be dropped into a melt in an evaporator, is made into many balls of identical diameters and placed inside a container. An elongated sloping pipe is connected to the container and leads to the evaporator such that these balls can travel sequentially therealong by gravity. A metering valve in this pipe for passing these balls one at a time is opened in response to a signal when it is ascertained by a detector that there is a ball ready to be passed. A gate in the pipe near the evaporator momentarily stops the motion of the traveling ball and is then opened to allow the ball drop into the melt at a reduced speed.

  2. Ball feeder for replenishing evaporator feed

    DOE Patents [OSTI]

    Felde, D.K.; McKoon, R.H.

    1993-03-23

    Vapor source material such as uranium, which is to be dropped into a melt in an evaporator, is made into many balls of identical diameters and placed inside a container. An elongated sloping pipe is connected to the container and leads to the evaporator such that these balls can travel sequentially therealong by gravity. A metering valve in this pipe for passing these balls one at a time is opened in response to a signal when it is ascertained by a detector that there is a ball ready to be passed. A gate in the pipe near the evaporator momentarily stops the motion of the traveling ball and is then opened to allow the ball drop into the melt at a reduced speed.

  3. Telescoping magnetic ball bar test gage

    DOE Patents [OSTI]

    Bryan, J.B.

    1982-03-15

    A telescoping magnetic ball bar test gage for determining the accuracy of machine tools, including robots, and those measuring machines having non-disengagable servo drives which cannot be clutched out. Two gage balls are held and separated from one another by a telescoping fixture which allows them relative radial motional freedom but not relative lateral motional freedom. The telescoping fixture comprises a parallel reed flexure unit and a rigid member. One gage ball is secured by a magnetic socket knuckle assembly which fixes its center with respect to the machine being tested. The other gage ball is secured by another magnetic socket knuckle assembly which is engaged or held by the machine in such manner that the center of that ball is directed to execute a prescribed trajectory, all points of which are equidistant from the center of the fixed gage ball. As the moving ball executes its trajectory, changes in the radial distance between the centers of the two balls caused by inaccuracies in the machine are determined or measured by a linear variable differential transformer (LVDT) assembly actuated by the parallel reed flexure unit. Measurements can be quickly and easily taken for multiple trajectories about several different fixed ball locations, thereby determining the accuracy of the machine.

  4. CHARGED PARTICLE IDENTIFICATION WITH MODULES OF THE PLASTIC BALL

    E-Print Network [OSTI]

    Gutbrod, H.H.

    2010-01-01

    WITH MODULES OF THE PLASTIC BALL H.H. Gutbrod, M.R. Maier,WITH MODULES OF THE PLASTIC BALL H.H. Gutbrod, M.R. Maier*,of modules of the Plastic Ball detector for positive pions

  5. Are perytons signatures of ball lighting?

    E-Print Network [OSTI]

    Dodin, I Y

    2014-01-01

    The enigmatic downchirped signals, called "perytons", that are detected by radio telescopes in the GHz frequency range may be produced by an atmospheric phenomenon known as ball lightning. Although this is still a hypothesis, the parallels between perytons and ball lightning are striking.

  6. Lightning Ball (Ball Lightning) Created by Thunder, Shock-Wave

    E-Print Network [OSTI]

    Domokos Tar

    2010-07-20

    Following his observation the author has described in the papers [1] to [4] the formation of a Lightning Ball (LB)with the help of a new theory of symmetry breaking of the vortex ring. In the frame of this theory he emphasizes the primordial rule of the thunder (shock-wave) during the lightning strike in the creation of the LB. The shock-waves and the sound waves propagate very fast but the subsequent enlargement of the vortex ring (air masses) is very slow. This is the reason why the rotating air ring (cylinder) only appeared some seconds later in the observation because of the great inertia of the system. As a consequence of the stationary Mach shock-waves reflections theory the stable distance of the LB to the ground and its very stable horizontal path, in spite of strong winds and rain can be explained.

  7. Lightning Ball (Ball Lightning) Created by Thunder, Shock-Wave

    E-Print Network [OSTI]

    Tar, Domokos

    2010-01-01

    Following his observation the author has described in the papers [1] to [4] the formation of a Lightning Ball (LB)with the help of a new theory of symmetry breaking of the vortex ring. In the frame of this theory he emphasizes the primordial rule of the thunder (shock-wave) during the lightning strike in the creation of the LB. The shock-waves and the sound waves propagate very fast but the subsequent enlargement of the vortex ring (air masses) is very slow. This is the reason why the rotating air ring (cylinder) only appeared some seconds later in the observation because of the great inertia of the system. As a consequence of the stationary Mach shock-waves reflections theory the stable distance of the LB to the ground and its very stable horizontal path, in spite of strong winds and rain can be explained.

  8. The bulking effect of dietary fiber in the rat large intestine: an in vivo study of cellulose, guar, pectin, wheat bran and oat bran 

    E-Print Network [OSTI]

    Gazzaniga, Jeanne Marie

    1985-01-01

    H. Chromium Concentration. IS 19 19 19 25 25 26 TABLE OF CONTENTS DISCUSSION. CONCLUSION. REFERENCES. . Page 32 47 50 LIST OF TABLES Page 1. COMPOSITION OF BASAI FIBER-FREE DIET. . . . 2. COMPOSITION OF THE EXPERIMENTAL DIETS. . . 13 3.... COMPOSITION OF WHEAT BRAN AND OAT BRAN SUPPLEMENTS. . 14 4. EFFECT OF FIBER SUPPLEMENTATION ON FOOD AND ENERGY INTAKE 5. EFFECT OF FIBER SUPPLEMENTATION ON WEIGHT GAIN. . 6. EFFECT OF FIBER ON 24-HOUR FECAL DRY WEIGHT. . . . . 20 21 22 7. EFFECT...

  9. CH Packaging Operations Manual

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2007-11-29

    This procedure provides instructions forassembling the following CH packaging payload: Drum payload assembly Standard Waste Box (SWB) assembly Ten-Drum Overpack (TDOP)

  10. CH Packaging Operations Manual

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2003-06-26

    Introduction - This procedure provides instructions for assembling the following CH packaging payload: -Drum payload assembly -Standard Waste Box (SWB) assembly -Ten-Drum Overpack (TDOP).

  11. Magnetic Interactions in Ball-Milled Spinel Ferrites

    E-Print Network [OSTI]

    Goya, Gerardo F

    2011-01-01

    Spinel Fe3O4 nanoparticles have been produced through ball milling in methyl-alcohol (CH3OH), aiming to obtain samples with similar average particle sizes and different interparticle interactions. Three samples having Fe3O4/CH3(OH) mass ratios R of 3 %, 10 % and 50 % wt. were milled for several hours until particle size reached a steady value ( ~ 7-10 nm). A detailed study of static and dynamic magnetic properties has been undertaken by measuring magnetization, ac susceptibility and M\\"ossbauer data. As expected for small particles, the Verwey transition was not observed, but instead superparamagnetic (SPM) behavior was found with transition to a blocked state at TB ~ 10-20 K. Spin disorder of the resulting particles, independent of its concentration, was inferred from the decrease of saturation magnetization MS at low temperatures. For samples having 3% wt. of magnetic particles, dynamic ac susceptibility measurements show a thermally activated Arrhenius dependence of the blocking temperature with applied f...

  12. A Nonsingular Brans Wormhole: An Analogue to Naked Black Holes

    E-Print Network [OSTI]

    Amrita Bhattacharya; Ramil Izmailov; Ettore Laserra; Kamal K. Nandi

    2011-07-28

    In a recent paper, we showed the Jordan frame vacuum Brans Class I solution provided a wormhole analogue to Horowitz-Ross naked black hole in the wormhole range -3/2naked black holes, as described by Horowitz and Ross, are spacetimes where the tidal forces attain their maxima above the black hole horizon. We show that in the non-singular Class II spacetime this maxima is attained above the throat and thus can be treated as a wormhole analogue. Some related issues are also addressed.

  13. Fossil fungi from America Pennsylvanian coal balls

    E-Print Network [OSTI]

    Baxter, R. W.

    1975-05-29

    THE UNIVERSITY OF KANSAS PALEONTOLOGICAL CONTRIBUTIONS May 29, 1975 Paper 77 FOSSIL FUNGI FROM AMERICAN PENNSYLVANIAN COAL BALLS' ROBERT W. BAXTER University of Kansas, Lawrence, Kansas ABSTRACT The current status of knowledge regarding fossil... fungi from American Pennsylvanian coal balls is discussed under the following general headings: 1) Phycomycetes, 2) Asco- mycetes, 3) Basidiomycetes, 4) fungal sclerotia, 5) mycorrhizal fungi, and 6) "fleshy fungi." Protoascon missouriensis...

  14. Nucleation of vacuum bubbles in Brans-Dicke type theory

    E-Print Network [OSTI]

    Hongsu Kim; Bum-Hoon Lee; Wonwoo Lee; Young Jae Lee; Dong-han Yeom

    2011-07-19

    In this paper, we explore the nucleation of vacuum bubbles in the Brans-Dicke type theory of gravity. In the Euclidean signature, we evaluate the fields at the vacuum bubbles as solutions of the Euler-Lagrange equations of motion as well as the bubble nucleation probabilities by integrating the Euclidean action. We illustrate three possible ways to obtain vacuum bubbles: true vacuum bubbles for \\omega>-3/2, false vacuum bubbles for \\omega-3/2 when the vacuum energy of the false vacuum in the potential of the Einstein frame is less than that of the true vacuum. After the bubble is nucleated at the t=0 surface, we can smoothly interpolate the field combinations to some solutions in the Lorentzian signature and consistently continue their subsequent evolutions. Therefore, we conclude that, in general scalar-tensor theories like this Brans-Dicke type theories, which may include and represent certain features of string theory, vacuum bubbles come in false vacuum bubbles as well as in true vacuum bubbles, as long as a special condition is assumed on the potential.

  15. Modified Brans-Dicke theory of gravity from five-dimensional vacuum

    E-Print Network [OSTI]

    Jose Edgar Madriz Aguilar; Carlos Romero; Adriano Barros

    2007-05-03

    We investigate, in the context of five-dimensional (5D) Brans-Dicke theory of gravity, the idea that macroscopic matter configurations can be generated from pure vacuum in five dimensions, an approach first proposed in the framework of general relativity. We show that the 5D Brans-Dicke vacuum equations when reduced to four dimensions lead to a modified version of Brans-Dicke theory in four dimensions (4D). As an application of the formalism, we obtain two five-dimensional extensions of four-dimensional O'Hanlon and Tupper vacuum solution and show that they lead two different cosmological scenarios in 4D.

  16. Dark Matter Balls Help Supernovae to Explode

    E-Print Network [OSTI]

    Colin D. Froggatt; Holger B. Nielsen

    2015-03-03

    As a solution to the well-known problem that the shock wave potentially responsible for the explosion of a supernova actually tends to stall, we propose a new energy source arising from our model for dark matter. Our earlier model proposed that dark matter should consist of cm-large white dwarf-like objects kept together by a skin separating two different sorts of vacua. These dark matter balls or pearls will collect in the middle of any star throughout its lifetime. At some stage during the development of a supernova the balls will begin to take in neutrons and then other surrounding material. By passing into a ball nucleons fall through a potential of order 10 MeV, causing a severe production of heat - of order 10 foe for a solar mass of material eaten by the balls. The temperature in the iron core will thereby be raised, splitting up the iron into smaller nuclei. This provides a mechanism for reviving the shock wave when it arrives and making the supernova explosion really occur. The onset of the heating due to the dark matter balls would at first stop the collapse of the supernova progenitor. This opens up the possibility of there being {\\em two} collapses giving two neutrino outbursts, as apparently seen in the supernova SN1987A - one in Mont Blanc, and one 4 hours 43 minutes later in both IMB and Kamiokande.

  17. Silicon ball grid array chip carrier

    DOE Patents [OSTI]

    Palmer, David W. (Albuquerque, NM); Gassman, Richard A. (Greensboro, NC); Chu, Dahwey (Albuquerque, NM)

    2000-01-01

    A ball-grid-array integrated circuit (IC) chip carrier formed from a silicon substrate is disclosed. The silicon ball-grid-array chip carrier is of particular use with ICs having peripheral bond pads which can be reconfigured to a ball-grid-array. The use of a semiconductor substrate such as silicon for forming the ball-grid-array chip carrier allows the chip carrier to be fabricated on an IC process line with, at least in part, standard IC processes. Additionally, the silicon chip carrier can include components such as transistors, resistors, capacitors, inductors and sensors to form a "smart" chip carrier which can provide added functionality and testability to one or more ICs mounted on the chip carrier. Types of functionality that can be provided on the "smart" chip carrier include boundary-scan cells, built-in test structures, signal conditioning circuitry, power conditioning circuitry, and a reconfiguration capability. The "smart" chip carrier can also be used to form specialized or application-specific ICs (ASICs) from conventional ICs. Types of sensors that can be included on the silicon ball-grid-array chip carrier include temperature sensors, pressure sensors, stress sensors, inertia or acceleration sensors, and/or chemical sensors. These sensors can be fabricated by IC processes and can include microelectromechanical (MEM) devices.

  18. CH Packaging Operations Manual

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2005-06-13

    This procedure provides instructions for assembling the CH Packaging Drum payload assembly, Standard Waste Box (SWB) assembly, Abnormal Operations and ICV and OCV Preshipment Leakage Rate Tests on the packaging seals, using a nondestructive Helium (He) Leak Test.

  19. Ball State building massive geothermal system

    Broader source: Energy.gov [DOE]

    Ball State University is building America’s largest ground source district geothermal heating and cooling system. The new operation will save the school millions of dollars, slash greenhouse gases and create jobs. The project will also “expand how America will define the use of geothermal technology on a district-wide scale,” and provide health benefits such as reducing asthma rates for Indiana residents, says Philip Sachtleben, Ball State’s associate vice president of governmental relations. The system will cool and heat nearly 50 buildings on Ball State’s Muncie, Ind., campus, replace four coal-burning boilers and span more than 600 acres. The switch to geothermal will save the university $2.2 million in fuel costs and cut its carbon footprint in half.

  20. CONSTRAINING THE ENVIRONMENT OF CH FORMATION WITH CH

    E-Print Network [OSTI]

    Oka, Takeshi

    CONSTRAINING THE ENVIRONMENT OF CH + FORMATION WITH CH + 3 OBSERVATIONS This article has been reserved. Printed in the U.S.A. CONSTRAINING THE ENVIRONMENT OF CH+ FORMATION WITH CH+ 3 OBSERVATIONS Nick of Illinois at Urbana-Champaign, Urbana, IL 61801, USA 2 Department of Astronomy and Astrophysics

  1. Brans--Dicke cosmology does not have the $?$CDM phase as an universal attractor

    E-Print Network [OSTI]

    Ricardo García-Salcedo; Tamé González; Israel Quiros

    2015-06-01

    In this paper we seek for relevant information on the asymptotic cosmological dynamics of the Brans--Dicke theory of gravity for several self-interaction potentials. By means of the simplest tools of the dynamical systems theory, it is shown that the general relativity de Sitter solution is an attractor of the Jordan frame (dilatonic) Brans--Dicke theory only for the exponential potential $U(\\vphi)\\propto\\exp\\vphi$, which corresponds to the quadratic potential $V(\\phi)\\propto\\phi^2$ in terms of the original Brans--Dicke field $\\phi=\\exp\\vphi$, or for potentials which asymptote to $\\exp\\vphi$. At the stable de Sitter critical point, as well as at the stiff-matter equilibrium configurations, the dilaton is necessarily massless. We find bounds on the Brans--Dicke coupling constant $\\omega_\\textsc{bd}$, which are consistent with well-known results.

  2. Phenotypic characterization of rhizobia that nodulate ball clover 

    E-Print Network [OSTI]

    Cepeda Hernandez, Martha Lucia

    2005-11-01

    A total of 43 Rhizobium leguminosarium bv. trifolii isolates were obtained from soil samples of two ball clover (Trifolium nigrescens) pastures from Iola and Kilgore (Texas) using ball clover as capture plants. The isolates were phenotypically...

  3. Energy conditions outside a dielectric ball

    SciTech Connect (OSTI)

    Graham, Noah; Olum, Ken D.; Schwartz-Perlov, Delia [Department of Physics, Middlebury College, Middlebury, Vermont 05753 (United States); Institute of Cosmology, Department of Physics and Astronomy, Tufts University, Medford, Massachusetts 02155 (United States)

    2004-11-15

    We show analytically that the vacuum electromagnetic stress-energy tensor outside a ball with constant dielectric constant and permeability always obeys the weak, null, dominant, and strong energy conditions. There are still no known examples in quantum field theory in which the averaged null energy condition in flat spacetime is violated.

  4. The harmonic measure of balls in random trees Nicolas Curien

    E-Print Network [OSTI]

    Le Gall, Jean-François

    The harmonic measure of balls in random trees Nicolas Curien and Jean-François Le Gall Abstract We study properties of the harmonic measure of balls in typical large discrete trees. For a ball of radius of the harmonic measure is supported on a boundary set of size approximately equal to n , where 0

  5. Andrew Moore Department of Physics, Ball State University

    E-Print Network [OSTI]

    Sites, James R.

    University #12;Organizations: American Physical Society (APS) Programming Languages/ Software: Java, CAndrew Moore Department of Physics, Ball State University 7755 Meadow Lane, Newburgh, IN 47630 812 2007-2011 M.S. of Physics, Ball State University B.S. of Physics, Ball State University Quantum

  6. SCHWARTZ TENNIS CENTER DAMPENERS, GRIPS, STRING, TENNIS BALLS

    E-Print Network [OSTI]

    Pittendrigh, Barry

    SCHWARTZ TENNIS CENTER DAMPENERS, GRIPS, STRING, TENNIS BALLS STRINGING:(We attempt to have all, Durability $34.00 Luxilon Big Banger Rough, Spin, Control, Durability $34.00 Prince Lightning, 16 g: $5.00 Wilson Pro Feel Plus Dampener: $4.00 TENNIS BALLS: Wilson US Open Tennis Balls: $3.25 SPECIAL

  7. Air fluidized balls in a background of smaller beads

    E-Print Network [OSTI]

    M. E. Beverland; L. J. Daniels; D. J. Durian

    2010-12-02

    We report on quasi-two-dimensional granular systems in which either one or two large balls is fluidized by an upflow of air in the presence of a background of several hundred smaller beads. A single large ball is observed to propel ballistically in nearly circular orbits, in direct contrast to the Brownian behavior of a large ball fluidized in the absence of this background. Further, the large ball motion satisfies a Langevin equation with an additional speed-dependent force acting in the direction of motion. This results in a non-zero average speed of the large ball that is an order of magnitude faster than the root mean square speed of the background balls. Two large balls fluidized in the absence of the small-bead background experience a repulsive force depending only on the separation of the two balls. With the background beads present, by contrast, the ball-ball interaction becomes velocity-dependent and attractive. The attraction is long-ranged and inconsistent with a depletion model; instead, it is mediated by local fluctuations in the density of the background beads which depends on the large balls' motion.

  8. Wormholes and Naked Singularities in Brans-Dicke cosmology

    E-Print Network [OSTI]

    Tretyakova, D A; Alexeyev, S O

    2015-01-01

    We perform analytical and numerical study of static spherically symmetric solutions in the context of Brans-Dicke-like cosmological model by Elizalde et al.. In this model the phantom regime arises without the appearance of any ghost degree of freedom due to the specific form of coupling. For the certain parameter ranges the model contains a regular solution which we interpret as a wormhole. The space-time structure is similar to Schwarzschild-AdS one, representing a wormhole in AdS Universe. We put several bounds on the parameter values: $\\omega<0 ,\\,\\, \\alpha^2/|\\omega|<10^{-5},0<\\!\\phi_0\\!\\lesssim5.1\\,$. The numerical solution could mimic the Schwarzschild one, so the original model is consistent with astrophysical and cosmological observational data. However differences between our solution and the Schwarzschild one can be quite large, so black hole observations could probably place further limits on the $\\phi_0$ value. We also derive a power-law correction to the gravitational potential for the ...

  9. A new Concept of Ball Lightning

    E-Print Network [OSTI]

    Tsintsadze, Levan N

    2008-01-01

    We suggest that the ball lightning (BL) is a weakly ionized gas, in which the electromagnetic radiation can be accumulated through the Bose-Einstein condensation and/or the photon trapping in the plasma density well. We derive the set of equations describing the stability of BL, and show that the BL moving along charged surface becomes unstable. Eventually the instability leads to explosion of BL and release of energy of the trapped photons and/or the Bose-Einstein condensate.

  10. Chemical, color, and sensory attributes of sorghum bran-enhanced beef patties in a high oxygen environment 

    E-Print Network [OSTI]

    Jenschke, Blaine Edward

    2006-04-12

    Bottom rounds were shipped to the Rosenthal Meat Science and Technology Center, ground and enhanced with one of the following predetermined treatments: control; 0.4% sodium phosphates and 0.3% salt; 0.25% sorghum bran; 2.0% sorghum bran; 0...

  11. Automatic ball bar for a coordinate measuring machine

    DOE Patents [OSTI]

    Jostlein, Hans (Naperville, IL)

    1997-01-01

    An automatic ball bar for a coordinate measuring machine determines the accuracy of a coordinate measuring machine having at least one servo drive. The apparatus comprises a first and second gauge ball connected by a telescoping rigid member. The rigid member includes a switch such that inward radial movement of the second gauge ball relative to the first gauge ball causes activation of the switch. The first gauge ball is secured in a first magnetic socket assembly in order to maintain the first gauge ball at a fixed location with respect to the coordinate measuring machine. A second magnetic socket assembly secures the second gauge ball to the arm or probe holder of the coordinate measuring machine. The second gauge ball is then directed by the coordinate measuring machine to move radially inward from a point just beyond the length of the ball bar until the switch is activated. Upon switch activation, the position of the coordinate measuring machine is determined and compared to known ball bar length such that the accuracy of the coordinate measuring machine can be determined.

  12. Automatic ball bar for a coordinate measuring machine

    DOE Patents [OSTI]

    Jostlein, H.

    1997-07-15

    An automatic ball bar for a coordinate measuring machine determines the accuracy of a coordinate measuring machine having at least one servo drive. The apparatus comprises a first and second gauge ball connected by a telescoping rigid member. The rigid member includes a switch such that inward radial movement of the second gauge ball relative to the first gauge ball causes activation of the switch. The first gauge ball is secured in a first magnetic socket assembly in order to maintain the first gauge ball at a fixed location with respect to the coordinate measuring machine. A second magnetic socket assembly secures the second gauge ball to the arm or probe holder of the coordinate measuring machine. The second gauge ball is then directed by the coordinate measuring machine to move radially inward from a point just beyond the length of the ball bar until the switch is activated. Upon switch activation, the position of the coordinate measuring machine is determined and compared to known ball bar length such that the accuracy of the coordinate measuring machine can be determined. 5 figs.

  13. Modified Brans-Dicke theory with space-time anisotropic parameters

    SciTech Connect (OSTI)

    Moon, Taeyoon [Center for Quantum Space-time, Sogang University, Seoul, 121-742 (Korea, Republic of); Oh, Phillial, E-mail: tymoon@inje.ac.kr, E-mail: ploh@skku.edu [Department of Physics and Institute of Basic Science, Sungkyunkwan University Suwon, 440-746 (Korea, Republic of)

    2014-03-01

    We consider the ADM formalism of the Brans-Dicke theory and propose a space-time anisotropic extension of the theory by introducing five free parameters. We find that the resulting theory reveals many interesting aspects which are not present in the original BD theory. We first discuss the ghost instability and strong coupling problems which are present in the gravity theory without the full diffeomorphism symmetry and show that they can be avoided in a region of the parameter space. We also perform the post-Newtonian approximation and show that the constraint of the Brans-Dicke parameter ?{sub BD} being large to be consistent with the solar system observations could be evaded in the extended theory. We also discuss that accelerating Universe can be achieved without the need of the potential for the Brans-Dicke scalar.

  14. Shear and Vorticity in an Accelerating Brans-Dicke Lambda-Universe with Torsion

    E-Print Network [OSTI]

    Marcelo Samuel Berman

    2008-08-06

    We study accelerating Universes with power-law scale-factors. We include shear and vorticity, a cosmological "constant" term, and spin from torsion, as in Einstein-Cartan's theory when a scalar-field of Brans-Dicke type acts in the model. We find a "no-hair" result, for shear and vorticity; we also make contact with the alternative Machian picture of the Universe. Keywords: Cosmology; Einstein; Brans-Dicke; Cosmological term; Shear; Spin; Vorticity; Inflation; Einstein-Cartan; Torsion; Accelerating Universe

  15. Ball lightning observation: an objective video-camera analysis report

    E-Print Network [OSTI]

    Sello, Stefano; Paganini, Enrico

    2011-01-01

    In this paper we describe a video-camera recording of a (probable) ball lightning event and both the related image and signal analyses for its photometric and dynamical characterization. The results strongly support the BL nature of the recorded luminous ball object and allow the researchers to have an objective and unique video document of a possible BL event for further analyses. Some general evaluations of the obtained results considering the proposed ball lightning models conclude the paper.

  16. Ball lightning observation: an objective video-camera analysis report

    E-Print Network [OSTI]

    Stefano Sello; Paolo Viviani; Enrico Paganini

    2011-02-18

    In this paper we describe a video-camera recording of a (probable) ball lightning event and both the related image and signal analyses for its photometric and dynamical characterization. The results strongly support the BL nature of the recorded luminous ball object and allow the researchers to have an objective and unique video document of a possible BL event for further analyses. Some general evaluations of the obtained results considering the proposed ball lightning models conclude the paper.

  17. The Dependence of Bat Performance on Ball Properties Lloyd Smith and Joseph Duris

    E-Print Network [OSTI]

    Smith, Lloyd V.

    The Dependence of Bat Performance on Ball Properties Lloyd Smith and Joseph Duris School Coefficient of restitution vr Rebound ball speed m Ball mass Abstract The performance of baseball and softball considers the rate dependence of ball compression and the normalization of bat performance with ball weight

  18. RadBall Technology For Hot Cell Characterization

    Broader source: Energy.gov [DOE]

    A new, non-electrical, remote radiation mapping device known as RadBall has been developed by the National Nuclear Laboratory (NNL) in the United Kingdom.

  19. RadBall Technology For Hot Cell Characterization

    Office of Environmental Management (EM)

    accurately characterize different radiation sources is ongoing along with development and building of the 3D visualization part of the technology to overlay RadBall data onto...

  20. Linear Fractional Maps of the Ball and Their Composition Operators

    E-Print Network [OSTI]

    Abstract. In this paper, we describe a class of maps of the unit ball in CN into itself ... ?Supported by National Science Foundation grants DMS-9206965 and ...

  1. Observation of Lightning Ball (Ball Lightning): A new phenomenological description of the phenomenon

    E-Print Network [OSTI]

    Tar, Domokos

    2009-01-01

    The author (physicist)has observed the very strange,beautiful and frightening Lightning Ball (LB). He has never forgotten this phenomenon. During his working life he could not devote himself to the problem of LB-formation.Only two years ago as he has been reading different unbelievable models of LB-formation, he decided to work on this problem. By studying the literature and the crucial points of his observation the author succeeded in creating a completely new model of Lightning Ball(LB) and Ball Lightning(BL)-formation based on the symmetry breaking of the hydrodynamic vortex ring.This agrees fully with the observation and overcomes the shortcomings of current models of LB formation. This model provides answers to the questions: Why are LBs so rarely observed,why do BLs in rare cases have such a high energy and how can we generate LB in the laboratory? Moreover the author differentiates between LB and BL, the latter having a high energy and occuring in 5 % of the observations. Keywords: ball lightning, hydr...

  2. Observation of Lightning Ball (Ball Lightning): A new phenomenological description of the phenomenon

    E-Print Network [OSTI]

    Domokos Tar

    2009-10-05

    The author (physicist)has observed the very strange,beautiful and frightening Lightning Ball (LB). He has never forgotten this phenomenon. During his working life he could not devote himself to the problem of LB-formation.Only two years ago as he has been reading different unbelievable models of LB-formation, he decided to work on this problem. By studying the literature and the crucial points of his observation the author succeeded in creating a completely new model of Lightning Ball(LB) and Ball Lightning(BL)-formation based on the symmetry breaking of the hydrodynamic vortex ring.This agrees fully with the observation and overcomes the shortcomings of current models of LB formation. This model provides answers to the questions: Why are LBs so rarely observed,why do BLs in rare cases have such a high energy and how can we generate LB in the laboratory? Moreover the author differentiates between LB and BL, the latter having a high energy and occuring in 5 % of the observations. Keywords: ball lightning, hydrodynamic vortex ring, symmetry breaking, electroluminescence, triboelectrification.

  3. Exact metric for the exterior of a global string in the Brans-Dicke theory

    E-Print Network [OSTI]

    B. Boisseau; B. Linet

    1998-02-03

    We determine in closed form the general static solution with cylindrical symmetry to the Brans-Dicke equations for an energy-momentum tensor corresponding to the one of the straight U(1) global string outside the core radius assuming that the Goldstone boson field takes its asymptotic value

  4. Fourier-Laguerre transform, Convolution and Wavelets on the Ball

    E-Print Network [OSTI]

    McEwen, Jason

    Fourier-Laguerre transform, Convolution and Wavelets on the Ball Jason D. McEwen and Boris Leistedt.leistedt.11}@ucl.ac.uk Abstract--We review the Fourier-Laguerre transform, an al- ternative harmonic analysis on the three-dimensional ball to the usual Fourier-Bessel transform. The Fourier-Laguerre transform exhibits

  5. Dynamics of a bouncing ball in human performance Dagmar Sternad

    E-Print Network [OSTI]

    Sternad, Dagmar

    of a dynamically stable period-one regime. In a series of experiments, human subjects bounced a ball rhythmically human movement and physical experi- mental systems is that while the variables and parameters of physical experiments are under the experimenter's control, human subjects when bouncing a ball have

  6. Structural Properties of Screened Coulomb Balls M. Bonitz,1

    E-Print Network [OSTI]

    Bonitz, Michael

    Structural Properties of Screened Coulomb Balls M. Bonitz,1 D. Block,2 O. Arp,2 V. Golubnychiy,1 H, computer simulations, and theoretical analysis, the sensitivity of their structural properties to the type. Coulomb balls consist of hundreds of micrometer sized plastic spheres embedded in a gas plasma

  7. Mechatronic design of a ball-on-plate balancing system

    E-Print Network [OSTI]

    Awtar, Shorya

    Mechatronic design of a ball-on-plate balancing system Shorya Awtar, C. Bernard, N. Boklund, A the conception and development of a ball-on-plate balancing system based on mechatronic design principles was designed and built by students as part of the course Mechatronics System Design at Rensselaer. Ó 2002

  8. Resonant frequency method for bearing ball inspection

    DOE Patents [OSTI]

    Khuri-Yakub, B. T. (Palo Alto, CA); Hsieh, Chung-Kao (Stanford, CA)

    1993-01-01

    The present invention provides for an inspection system and method for detecting defects in test objects which includes means for generating expansion inducing energy focused upon the test object at a first location, such expansion being allowed to contract, thereby causing pressure wave within and on the surface of the test object. Such expansion inducing energy may be provided by, for example, a laser beam or ultrasonic energy. At a second location, the amplitudes and phases of the acoustic waves are detected and the resonant frequencies' quality factors are calculated and compared to predetermined quality factor data, such comparison providing information of whether the test object contains a defect. The inspection system and method also includes means for mounting the bearing ball for inspection.

  9. Resonant frequency method for bearing ball inspection

    DOE Patents [OSTI]

    Khuri-Yakub, B.T.; Chungkao Hsieh.

    1993-11-02

    The present invention provides for an inspection system and method for detecting defects in test objects which includes means for generating expansion inducing energy focused upon the test object at a first location, such expansion being allowed to contract, thereby causing pressure wave within and on the surface of the test object. Such expansion inducing energy may be provided by, for example, a laser beam or ultrasonic energy. At a second location, the amplitudes and phases of the acoustic waves are detected and the resonant frequencies' quality factors are calculated and compared to predetermined quality factor data, such comparison providing information of whether the test object contains a defect. The inspection system and method also includes means for mounting the bearing ball for inspection. 5 figures.

  10. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2007-02-15

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  11. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2005-08-15

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  12. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2006-09-15

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  13. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2007-09-20

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  14. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2005-01-15

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codesand corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  15. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2005-11-20

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  16. CH-TRU Waste Content Codes (CH TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2004-12-01

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  17. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2006-12-20

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  18. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2005-05-01

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  19. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2005-12-15

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  20. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2005-01-30

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  1. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2006-06-20

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  2. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2004-10-01

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  3. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2006-01-18

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  4. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2007-08-15

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  5. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2007-06-15

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  6. CH-TRU Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2005-10-15

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  7. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2005-06-20

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  8. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2006-08-15

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  9. CH-TRU Waste Content Codes (CH-TRUCON)

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2005-03-15

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  10. Chemical and Physical Properties of Breakfast Cereals and Snacks Made from Specialty Sorghums and Sorghum Bran Using Twin Screw Extruder 

    E-Print Network [OSTI]

    Asif, Muhammad

    2012-02-14

    and on in vitro starch digestibility of sorghum based cereals and snacks were observed. Gluten free and gluten containing breakfast cereal and snacks were developed with different physical, chemical and sensory characteristic. By increasing the sorghum and bran...

  11. CH-TRUCON Rev. 21, January 2008

    Office of Environmental Management (EM)

    DOEWIPP 01-3194 Rev. 21 CH-TRU WASTE CONTENT CODES (CH-TRUCON) Revision 21 January 2008 This document supercedes DOEWIPP 01-3194, Revision 20 CH-TRUCON, Rev. 21, January 2008...

  12. Prfungsleitung Master Mathematik Prof. Dr. Ch. Riedtmann

    E-Print Network [OSTI]

    Sola, Rolf Haenni

    CH-3012 Bern Tel. +41 031 631 88 34 christine.riedtmann@math.unibe.ch Sekretariat Tel. +41 031 631 88 Mathematisches Institut, Sidlerstrasse 5, CH-3012 Bern #12;

  13. Complete density perturbations in the Jordan-Fierz-Brans-Dicke theory

    E-Print Network [OSTI]

    J. A. R. Cembranos; A. de la Cruz Dombriz; L. Olano Garcia

    2013-07-01

    In the context of scalar-tensor theories we study the evolution of the density contrast for Jordan-Fierz-Brans-Dicke theories in a Friedmann-Lemaitre-Robertson-Walker Universe. Calculations are performed in the Einstein Frame with the cosmological background described as Lambda-Cold Dark Matter (Lambda-CDM) and supplemented by a Jordan-Fierz-Brans-Dicke field. By using a completely general procedure valid for all scalar-tensor theories, we obtain the exact fourth-order differential equation for the density contrast evolution in modes of arbitrary size. In the case of sub-Hubble modes, the expression reduces to a simpler but still fourth-order equation that is then compared with the standard (quasistatic) approximation. Differences with respect to the evolution as predicted by the standard Concordance Lambda-CDM model are observed depending on the value of the coupling.

  14. Phase transition of charged Black Holes in Brans-Dicke theory through geometrical thermodynamics

    E-Print Network [OSTI]

    Hendi, S H; Panah, B Eslam; Armanfard, Z

    2015-01-01

    In this paper, we take into account black hole solutions of Brans-Dicke-Maxwell theory and investigate their stability and phase transition points. We apply the concept of geometry in thermodynamics to obtain phase transition points and compare its results with those of calculated in canonical ensemble through heat capacity. We show that these black holes enjoy second order phase transitions. We also show that there is a lower bound for the horizon radius of physical charged black holes in Brans-Dicke theory which is originated from restrictions of positivity of temperature. In addition, we find that employing specific thermodynamical metric in the context of geometrical thermodynamics yields divergencies for thermodynamical Ricci scalar in places of phase transitions. It will be pointed out that due to characteristics behavior of thermodynamical Ricci scalar around its divergence points, one is able to distinguish the physical limitation point from the phase transitions.

  15. Design of a tree root ball transporting device

    E-Print Network [OSTI]

    Grossman, Christopher (Christopher M.)

    2007-01-01

    Tree root balls from nurseries are often too heavy for one or two people to lift and plant, but powerful machinery can be expensive for small landscaping organizations or the weekend home gardener. This thesis intends to ...

  16. Effect of antioxidants, color and sensory atributes of different sorghum brans in model baking systems 

    E-Print Network [OSTI]

    Guajardo Flores, David

    2009-05-15

    Attributes of Inclusion of Different Sorghum Brans in Model Baking Systems. (December 2007) David Guajardo Flores, B.S., Instituto Tecnologico y de Estudios Superiores de Monterrey Chair of Advisory Committee: Dr. Lloyd W. Rooney The effects... there when I needed them. I thank all my friends that I met during this process: Alejandro Perez, Emilio Villarreal, Marc Barron, Angelina de Castro, Vilma Calderon and her husband Pedro, Novie Alviola, Armando del Follo, Yolanda Nuñez and especially...

  17. A remark on Brans-Dicke dust cosmological solutions with negative $?$

    E-Print Network [OSTI]

    A. B. Batista; J. C. Fabris; R. de Sá Ribeiro

    2000-01-19

    Analysing the Brans-Dicke solutions for the dust phase, we show that, for negative values of $\\omega$, they contain scenarios that display an initial subluminal expansion followed by an inflationary phase. We discuss these solutions with respect to the results of the observation of high redshif supernova as well as the age problem and structure formation. We stablish possible connections of these solutions with those emerging from string effective models.

  18. The effects of oat bran and amaranth products in hypercholesterolemic men and women 

    E-Print Network [OSTI]

    Clay, Susan Marie

    1989-01-01

    Group Establishment of Baseline Parameters. X11 1 20 20 23 24 26 Sequential Serum Cholesterol Measurements . 32 Measurement of Diet Intake 36 Diet Instructions Data Analysis. RESULTS 39 42 Participation Baseline Data Effects... and Acceptability of Products The Extent of Diet Modification The Oat Bran Muffin Group. Page 140 142 143 147 CONCLUSION REPERENCES . 156 . 159 VITA . 172 LIST OP TABLES TABLE 1. Demographics of the sample at baseline for groups 1-4. Page 45 2...

  19. Supporting wormholes by spacetime parity and topology in Lovelock-Brans-Dicke gravity

    E-Print Network [OSTI]

    David Wenjie Tian

    2015-08-30

    Following the recent theory of Lovelock-Brans-Dicke gravity, we continue to investigate the conditions to support traversable wormholes by the gravitational effects of spacetime parity and topology, which arise from the nonminimal couplings of a background scalar field to the Chern-Pontryagin density and the Gauss-Bonnet invariant. The flaring-out condition indicates that a Morris-Thorne-type wormhole can be maintained by violating the generalized null energy condition, and thus also breaking down the generalized weak, strong, and dominant energy conditions; meanwhile, analyses of the zero-tidal-force solution show that the standard energy conditions in general relativity can still be respected by the physical matter threading the wormhole. In this situation, the two topological effects have to dominate over the ordinary-matter source of gravity, and the scalar field is preferred to be noncanonical. Also, we find that it is easier in Lovelock-Brans-Dicke than Brans-Dicke gravity to support wormholes while have the standard energy conditions protected.

  20. The Chameleon Effect in the Jordan Frame of the Brans--Dicke Theory

    E-Print Network [OSTI]

    Quiros, Israel; Gonzalez, Tame; Horta-Rangel, F Antonio

    2015-01-01

    In this paper we investigate the chameleon effect in the different conformal frames of the Brans--Dicke theory. Given that, in the standard literature on the subject, the chameleon is described in the Einstein frame almost exclusively, here we pay special attention to the description of this effect in the Jordan and in the string frames. It is shown that, in general, terrestrial and solar system bounds on the mass of the BD scalar field, and bounds of cosmological origin, are difficult to reconcile at once through a single chameleon potential. We point out that, in a cosmological context, provided that the effective chameleon potential has a minimum within a region of constant density of matter, the Brans--Dicke theory transmutes into general relativity with a cosmological constant, in that region. This result, however, can be only locally valid. In cosmological settings de Sitter--general relativity is a global attractor of the Brans--Dicke theory only for the quadratic potential $V(\\phi)=M^2\\phi^2$, or for ...

  1. The Chameleon Effect in the Jordan Frame of the Brans--Dicke Theory

    E-Print Network [OSTI]

    Israel Quiros; Ricardo García-Salcedo; Tame Gonzalez; F. Antonio Horta-Rangel

    2015-06-20

    In this paper we investigate the chameleon effect in the different conformal frames of the Brans--Dicke theory. Given that, in the standard literature on the subject, the chameleon is described in the Einstein frame almost exclusively, here we pay special attention to the description of this effect in the Jordan and in the string frames. It is shown that, in general, terrestrial and solar system bounds on the mass of the BD scalar field, and bounds of cosmological origin, are difficult to reconcile at once through a single chameleon potential. We point out that, in a cosmological context, provided that the effective chameleon potential has a minimum within a region of constant density of matter, the Brans--Dicke theory transmutes into general relativity with a cosmological constant, in that region. This result, however, can be only locally valid. In cosmological settings de Sitter--general relativity is a global attractor of the Brans--Dicke theory only for the quadratic potential $V(\\phi)=M^2\\phi^2$, or for potentials that asymptote to $M^2\\phi^2$.

  2. Interacting logarithmic entropy-corrected holographic dark energy model with different cut-offs in Brans-Dicke cosmology

    E-Print Network [OSTI]

    Darabi, F

    2015-01-01

    We study the Interacting Logarithmic Entropy-Corrected Holographic Dark Energy model with different cut-offs in Brans-Dicke cosmology and obtain the equation of state and the squared of sound speed for each cut-off. The former is used to describe the accelerating or decelerating behaviour and the later is used to describe the classical stability or instability of the universe. The correspondence between the scalar field models and the logarithmic entropy-corrected holographic dark energy densities allows us to reconstruct the potentials and the dynamics of the quintessence and tachyon scalar field models in Brans-Dicke cosmology. We show that these models can describe the observed accelerated expansion of our universe with a parameter space consistent with the most recent observational data. However, it turns out that there is fine-tuning problem concerning the value of Brans-Dicke parameter $\\omega$ at early universe which casts doubt on the viability of these dark energy models.

  3. Propagation of quantum particles in Brans-Dicke spacetime. The case of Gamma Ray Bursts

    E-Print Network [OSTI]

    Capozziello, S

    2015-01-01

    The propagation of boson particles in a gravitational field described by the Brans-Dicke theory of gravity is analyzed. We derive the wave function of the scalar particles, and the effective potential experienced by the quantum particles considering the role of the varying gravitational coupling. Besides, we calculate the probability to find the scalar particles near the region where a naked singularity is present. The extremely high energy radiated in such a situation could account for the huge emitted power observed in Gamma Ray Bursts.

  4. Propagation of quantum particles in Brans-Dicke spacetime. The case of Gamma Ray Bursts

    E-Print Network [OSTI]

    S. Capozziello; G. Lambiase

    2015-01-22

    The propagation of boson particles in a gravitational field described by the Brans-Dicke theory of gravity is analyzed. We derive the wave function of the scalar particles, and the effective potential experienced by the quantum particles considering the role of the varying gravitational coupling. Besides, we calculate the probability to find the scalar particles near the region where a naked singularity is present. The extremely high energy radiated in such a situation could account for the huge emitted power observed in Gamma Ray Bursts.

  5. Simulation and optimization of a two-wheeled, ball- flinging robot

    E-Print Network [OSTI]

    Chen, Po-Ting

    2010-01-01

    Wheeled, Ball-Flinging Robot A thesis submitted in partiala Two-Wheeled, Ball-Flinging Robot by Po-Ting Chen Master ofremote controlled robot. The robot is maneuverable and

  6. The experimental determination of the dynamic radial stiffness of an angular contact ball bearing 

    E-Print Network [OSTI]

    Schmidt, Brent Lee

    2001-01-01

    To evaluate the A. B. Jones bearing stiffness predictions on an angular contact ball bearing, experimental testing on an angular contact ball bearing was conducted. Objectives of the testing were to determine the effects of thrust load, rotational...

  7. A Look Through the Crystal Ball at the Future of Automobile Battery...

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

    A Look Through the Crystal Ball at the Future of Automobile Battery Recycling Title A Look Through the Crystal Ball at the Future of Automobile Battery Recycling Publication Type...

  8. 4, 31953227, 2007 Modelling CH4

    E-Print Network [OSTI]

    Boyer, Edmond

    Interactive Discussion EGU 1 Introduction Together with water vapour and carbon dioxide (CO2), CH4, hydrology, soil physical properties, vegetation type and NPP.15 For Kytalyk the simulated CH4 fluxes show

  9. THE PLASTIC BALL - A MULTI-DETECTOR, LARGE SOLID ANGLE SPECTROMETER WITH CHARGED PARTICLE IDENTIFICATION FOR THE BEVALAC

    E-Print Network [OSTI]

    Maier, M.R.

    2012-01-01

    of charged particles in a Plastic Ball module. (XBL 7910-of Califomia. THE PLASTIC BALL - A MULTI-DETECTOR, LARGEBerkeley, California Summary PLASTIC 8/>Ll PLASTIC WALL For

  10. Dilatonic Brans-Dicke Anisotropic Collapsing Fluid Sphere And de Broglie Quantum Wave Motion

    E-Print Network [OSTI]

    Hossein Ghaffarnejad

    2014-12-18

    Two dimensional analogue of vacuum sector of the Brans Dicke gravity [1] is studied to obtain dynamics of anisotropic spherical symmetric perfect fluid. Solutions of dynamical field equations are obtained in terms of time and radial coordinates. In static regime the obtained solutions leads to a dark matter fluid with state equation $\\gamma=\\frac{p(\\rho)}{\\varrho}=-0.25.$ For non-static regime the fluid can be treat as a regular matter with positive barotropic index $\\gamma>0.$ Evaluation of total mass of the fluid leads to choose particular values on the Brans Dick parameter as $\\omega>\\frac{2}{3};\\omegastatic regime. In case $\\omega>0$ the apparent horizon is covered by event horizon and hence the cosmic censorship hypothesis is still maintained as valid. \\\\ In second part of the paper we obtain de Broglie pilot wave of our fluid model. It can be describe particles ensemble which are distinguished from each other by $\\omega.$ Incident current density of particles ensemble is evaluated on the event and apparent horizon describing the `Hawking radiation` in statistical mechanics perspective. The quantum potential is calculated on the event horizon which is independent from $\\omega$ but the evaluated quantum potential on the apparent horizon is depended to particular value of $\\omega$.

  11. Whitey SCHe Ball Valves Provide Test Port Isolation

    SciTech Connect (OSTI)

    MISKA, C.R.

    2000-10-19

    These valves are 1/4-inch ball valves fabricated of 316 stainless steel. Packing is TFE (standard). They are used as normally closed isolation valves for test ports in the SCHe System between the gage root valve and the pressure indicator.

  12. Whitey SCHe Ball Valves Provide Test Port Isolation

    SciTech Connect (OSTI)

    MISKA, C.R.

    2000-09-15

    These valves are 1/4 inch ball valves fabricated of 316 stainless steel. Packing is TFE (standard). They are used as normally closed isolation valves for test ports in the SCHe System between the gage root valve and the pressure indicator.

  13. Billiards Digest November, 2012 "VEPP Part VIII: 8-Ball Pattern Drills" ILLUSTRATED PRINCIPLES

    E-Print Network [OSTI]

    Alciatore, David G.

    Billiards Digest November, 2012 "VEPP ­ Part VIII: 8-Ball Pattern Drills" ILLUSTRATED PRINCIPLES-dave-billiards.com/vepp. Last month, we looked at some useful 9-ball pattern drills from Disc III: "VEPP III ­ Patterns and Safety Play." This month, we look at some 8-ball pattern drills, also from the 3 rd DVD. You can work

  14. Comparison of Hydraulic-Burst and Ball-on-Ring Tests for Measuring Biaxial Strength

    E-Print Network [OSTI]

    Matthewson, M. John

    Comparison of Hydraulic-Burst and Ball-on-Ring Tests for Measuring Biaxial Strength Anupa Simpatico­0909 The statistics of failure of the hydraulic-burst (HB) test were compared with those of the ball-on-ring (BOR tests are ball-on-ring (BOR) and ring-on-ring (ROR); however, hydraulic-burst (HB) tests also have

  15. ARM - Datastreams - fullavhrr12ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1l DocumentationDatastreamsecmwfvarch2ch4ch2ch4ch2

  16. CH

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Outreach Home Room News PublicationsAudits &Bradbury Science Museum6 Shares1-0005-000CD .... --

  17. The Bianchi type-V Dark Energy Cosmology in Self Interacting Brans Dicke Theory of Gravity

    E-Print Network [OSTI]

    Singh, J K

    2016-01-01

    This paper deals with a spatially homogeneous and totally anisotropic Bianchi type-V cosmological model within the framework of self interacting Brans Dicke theory of gravity in the background of anisotropic dark energy (DE) with variable equation of state (EoS) parameter and constant deceleration parameter. Constant deceleration parameter leads to two models of universe, i.e. power law model and exponential model. EoS parameter {\\omega} and its existing range for the models is in good agreement with the most recent observational data. We notice that {\\omega} given by (37) i.e {\\omega}(t) = log(k1t) is more suitable in explaining the evolution of the universe. The physical behaviors of the solutions have also been discussed using some physical quantities. Finally, we observe that despite having several prominent features, both of the DE models discussed fail in details.

  18. Thermodynamics of charged rotating black branes in Brans-Dicke theory with quadratic scalar field potential

    SciTech Connect (OSTI)

    Dehghani, M. H.; Pakravan, J.; Hendi, S. H.

    2006-11-15

    We construct a class of charged rotating solutions in (n+1)-dimensional Maxwell-Brans-Dicke theory with flat horizon in the presence of a quadratic potential and investigate their properties. These solutions are neither asymptotically flat nor (anti)-de Sitter. We find that these solutions can present black brane, with inner and outer event horizons, an extreme black brane or a naked singularity provided the parameters of the solutions are chosen suitably. We compute the finite Euclidean action through the use of counterterm method, and obtain the conserved and thermodynamic quantities by using the relation between the action and free energy in grand-canonical ensemble. We find that these quantities satisfy the first law of thermodynamics, and the entropy does not follow the area law.

  19. Reconstruction from Radon projections and orthogonal expansion on a ball

    E-Print Network [OSTI]

    Yuan Xu

    2007-05-14

    The relation between Radon transform and orthogonal expansions of a function on the unit ball in $\\RR^d$ is exploited. A compact formula for the partial sums of the expansion is given in terms of the Radon transform, which leads to algorithms for image reconstruction from Radon data. The relation between orthogonal expansion and the singular value decomposition of the Radon transform is also exploited.

  20. ARM - Datastreams - fullavhrr11ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1l DocumentationDatastreamsecmwfvarch2ch4ch2ch4

  1. Thermodynamics of topological black holes in Brans-Dicke gravity with a power-law Maxwell field

    E-Print Network [OSTI]

    Zangeneh, M Kord; Sheykhi, A

    2015-01-01

    In this paper, we present a new class of higher dimensional exact topological black hole solutions of the Brans-Dicke theory in the presence of a power-law Maxwell field as the matter source. For this aim, we introduce a conformal transformation which transforms the Einstein-dilaton-power-law Maxwell gravity Lagrangian to the Brans-Dicke-power-law Maxwell theory one. Then, by using this conformal transformation, we obtain the desired solutions. Next, we study the properties of the solutions and conditions under which we have black holes. Interestingly enough, we show that there is a cosmological horizon in the presence of a negative cosmological constant. Finally, we calculate the temperature and charge and then by calculating the Euclidean action, we obtain the mass, the entropy and the electromagnetic potential energy. We find that the entropy does not respect the area law, and also the conserved and thermodynamic quantities are invariant under conformal transformation. Using these thermodynamic and conserv...

  2. Electrostatic Potential of a Point Charge in a Brans-Dicke Reissner-Nordstr\\"{o}m Field

    E-Print Network [OSTI]

    Watanabe, Maya

    2013-01-01

    We consider the Brans-Dicke Reissner-Nordstr\\"{o}m spacetime in isotropic coordinates and the electrostatic field of an electric point charge placed outside its surface of inversion. We treat the static electric point charge as a linear perturbation on the Brans-Dicke Reissner-Nordstr\\"{o}m background. We develop a method based upon the Copson method to convert the governing Maxwell equation on the electrostatic potential generated by the static electric point charge into a solvable linear second order ordinary differential equation. We obtain a closed form fundamental solution of the curved space Laplace equation arising from the background metric, which is shown to be regular everywhere except at the point charge and its image point inside the surface of inversion. We also develop a method that demonstrates that the solution does not contain any other charge that may creep into the region that lies beyond the surface of inversion and which is not covered by the isotropic coordinates. The Brans-Dicke Reissne...

  3. Ball lightning as a possible manifestation of high-temperature superconductivity in Nature

    E-Print Network [OSTI]

    B. L. Birbrair

    2001-02-06

    In the superconducting medium the circular current supported by its own magnetic field can exist giving rise to the possible underlying mechanism for the ball lightning.

  4. Ball lightning as a possible manifestation of high-temperature superconductivity in Nature

    E-Print Network [OSTI]

    Birbrair, B L

    2001-01-01

    In the superconducting medium the circular current supported by its own magnetic field can exist giving rise to the possible underlying mechanism for the ball lightning.

  5. Three-dimensional Plasmas R. L. Dewar; P. Cuthbert; R. Ball 70...

    Office of Scientific and Technical Information (OSTI)

    of Three-dimensional Plasmas R. L. Dewar; P. Cuthbert; R. Ball 70 PLASMA PHYSICS AND FUSION TECHNOLOGY; 75 CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY;...

  6. Little Black Holes:Dark Matter And Ball Lightning

    E-Print Network [OSTI]

    Mario Rabinowitz

    2002-12-11

    Small,quiescent black holes can be considered as candidates for the missing dark matter of the universe,and as the core energy source of ball lightning.By means of gravitational tunneling,directed radiation is emitted from black holes in a process much attenuated from that of Hawking radiation,P SH, which has proven elusive to detect.Gravitational tunneling emission is similar to electric field emission of electronsfrom a metal in that a second body is involved which lowers the barrier and gives the barrier a finite rather than infinite width.Hawking deals with a single isolated black hole.

  7. CH-TRU Waste Content Codes

    SciTech Connect (OSTI)

    Washington TRU Solutions LLC

    2008-01-16

    The CH-TRU Waste Content Codes (CH-TRUCON) document describes the inventory of the U.S. Department of Energy (DOE) CH-TRU waste within the transportation parameters specified by the Contact-Handled Transuranic Waste Authorized Methods for Payload Control (CH-TRAMPAC). The CH-TRAMPAC defines the allowable payload for the Transuranic Package Transporter-II (TRUPACT-II) and HalfPACT packagings. This document is a catalog of TRUPACT-II and HalfPACT authorized contents and a description of the methods utilized to demonstrate compliance with the CH-TRAMPAC. A summary of currently approved content codes by site is presented in Table 1. The CH-TRAMPAC describes "shipping categories" that are assigned to each payload container. Multiple shipping categories may be assigned to a single content code. A summary of approved content codes and corresponding shipping categories is provided in Table 2, which consists of Tables 2A, 2B, and 2C. Table 2A provides a summary of approved content codes and corresponding shipping categories for the "General Case," which reflects the assumption of a 60-day shipping period as described in the CH-TRAMPAC and Appendix 3.4 of the CH-TRU Payload Appendices. For shipments to be completed within an approximately 1,000-mile radius, a shorter shipping period of 20 days is applicable as described in the CH-TRAMPAC and Appendix 3.5 of the CH-TRU Payload Appendices. For shipments to WIPP from Los Alamos National Laboratory (LANL), Nevada Test Site, and Rocky Flats Environmental Technology Site, a 20-day shipping period is applicable. Table 2B provides a summary of approved content codes and corresponding shipping categories for "Close-Proximity Shipments" (20-day shipping period). For shipments implementing the controls specified in the CH-TRAMPAC and Appendix 3.6 of the CH-TRU Payload Appendices, a 10-day shipping period is applicable. Table 2C provides a summary of approved content codes and corresponding shipping categories for "Controlled Shipments" (10-day shipping period).

  8. Ball-grid array architecture for microfabricated ion traps

    E-Print Network [OSTI]

    Nicholas D. Guise; Spencer D. Fallek; Kelly E. Stevens; K. R. Brown; Curtis Volin; Alexa W. Harter; Jason M. Amini; Robert E. Higashi; Son Thai Lu; Helen M. Chanhvongsak; Thi A. Nguyen; Matthew S. Marcus; Thomas R. Ohnstein; Daniel W. Youngner

    2015-05-05

    State-of-the-art microfabricated ion traps for quantum information research are approaching nearly one hundred control electrodes. We report here on the development and testing of a new architecture for microfabricated ion traps, built around ball-grid array (BGA) connections, that is suitable for increasingly complex trap designs. In the BGA trap, through-substrate vias bring electrical signals from the back side of the trap die to the surface trap structure on the top side. Gold-ball bump bonds connect the back side of the trap die to an interposer for signal routing from the carrier. Trench capacitors fabricated into the trap die replace area-intensive surface or edge capacitors. Wirebonds in the BGA architecture are moved to the interposer. These last two features allow the trap die to be reduced to only the area required to produce trapping fields. The smaller trap dimensions allow tight focusing of an addressing laser beam for fast single-qubit rotations. Performance of the BGA trap as characterized with $^{40}$Ca$^+$ ions is comparable to previous surface-electrode traps in terms of ion heating rate, mode frequency stability, and storage lifetime. We demonstrate two-qubit entanglement operations with $^{171}$Yb$^+$ ions in a second BGA trap.

  9. Expanding (n+1)-dimensional wormhole solutions in Brans-Dicke cosmology

    SciTech Connect (OSTI)

    Ebrahimi, E.; Riazi, N.

    2010-01-15

    We have obtained two classes of (n+1)-dimensional wormhole solutions using a traceless energy-momentum tensor in the Brans-Dicke theory of gravity. The first class contains wormhole solutions in an open geometry, while the second contains wormhole solutions in both open and closed universes. In addition to wormhole geometries, naked singularities and maximally symmetric space-time also appear among the solutions as special cases. We have also considered the traversability of the wormhole solutions and have shown that they are indeed traversable. Finally, we have discussed the energy-momentum tensor which supports this geometry and have checked for the energy conditions. We have found that wormhole solutions in the first class of solutions violate the weak energy condition (WEC). In the second class, the wormhole geometries in a closed universe do violate the WEC, but in an open universe with a suitable choice of constants the supporting matter energy-momentum tensor can satisfy the WEC. However, even in this case the full effective energy-momentum tensor including the scalar field and the matter energy-momentum tensor still violates the WEC.

  10. QCD Phase Transition in Brans-Dicke DGP model of Brane Gravity

    E-Print Network [OSTI]

    T. Golanbari; A. Mohammadi; Kh. Saaidi

    2014-08-24

    A DGP brane-world model with a perfect fluid brane matter including a Brans-Dicke (BD) scalar field on brane has been utilized to investigate the problem of quark-hadron phase (QHP) transition in early times of the Universe evoltion. The presence of BD scalar field came up with some modification terms in the Friedmann equation, however we have a usual form of conservation equation for brane matter since scalar field only has a non-mnimally interaction with geometry. Behavior of phase transition strongly depends on the basic evolution equations. Then, even a small change in these relation might come to interesting results about the time of transition. Two different formalisms as smooth crossover formalism in which lattice QCD data is used for obtaining the matter equation of state and first-order phase transition formalism, have been used to investigate of the evolution of physical quatities relevant to quantitative of early times such as energy density $\\rho$, scale factor $a$, and temperature $T$. The obtained results show that the general behavior of temperature is similar in both of two formalisms and the QHP transition occurred at about micro-second after the Big Bang.

  11. ARM - Datastreams - avhrr17ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Datalacman Documentation7ch2ch4

  12. ARM - Datastreams - fullavhrr11ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1l DocumentationDatastreamsecmwfvarch2ch4ch2

  13. ARM - Datastreams - fullavhrr16ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1lch2 Documentation XDC documentation Datach2ch4ch2

  14. ARM - Datastreams - avhrr12ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Data Quality Plots ARM Data2ch2ch4

  15. Independent Oversight Review, Hanford Site CH2M Hill Plateau...

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

    CH2M Hill Plateau Remediation Company - November 2012 Independent Oversight Review, Hanford Site CH2M Hill Plateau Remediation Company - November 2012 November 2012 Review of the...

  16. Prof. Roger Wattenhofer http://www.dcg.ethz.ch

    E-Print Network [OSTI]

    @tik.ee.ethz.ch, ETZ G61.3, · Philipp Sommer: sommer@tik.ee.ethz.ch, ETZ G64.1 · Roger Wattenhofer: wattenhofer

  17. Newport News in Review, ch. 47, segment includes TEDF groundbreaking...

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

    https:www.jlab.orgnewsarticlesnewport-news-review-ch-47-segment-includes-tedf-groundbreaking-event Newport News in Review, ch. 47, segment includes TEDF groundbreaking event...

  18. Experiment 13 The Motion of a Beach Ball in the Air

    E-Print Network [OSTI]

    Pantaleone, Jim

    103 Experiment 13 The Motion of a Beach Ball in the Air Purpose: The air surrounding a projectile and the added mass. The added mass is an increase in the projectile's inertia from the motion of the air around. Messer and J. Pantaleone, `The Effective Mass of a Ball in the Air', The Physics Teacher, Vol. 48, 52

  19. Method and apparatus for jetting, manufacturing and attaching uniform solder balls

    DOE Patents [OSTI]

    Yost, Frederick G. (Cedar Crest, NM); Frear, Darrel R. (Albuquerque, NM); Schmale, David T. (Albuquerque, NM)

    1999-01-01

    An apparatus and process for jetting molten solder in the form of balls directly onto all the metallized interconnects lands for a ball grid array package in one step with no solder paste required. Molten solder is jetted out of a grid of holes using a piston attached to a piezoelectric crystal. When voltage is applied to the crystal it expands forcing the piston to extrude a desired volume of solder through holes in the aperture plate. When the voltage is decreased the piston reverses motion creating an instability in the molten solder at the aperture plate surface and thereby forming spherical solder balls that fall onto a metallized substrate. The molten solder balls land on the substrate and form a metallurgical bond with the metallized lands. The size of the solder balls is determined by a combination of the size of the holes in the aperture plate, the duration of the piston pulse, and the displacement of the piston. The layout of the balls is dictated by the location of the hooks in the grid. Changes in ball size and layout can be easily accomplished by changing the grid plate. This invention also allows simple preparation of uniform balls for subsequent supply to BGA users.

  20. Billiards Digest October, 2012 "VEPP Part VII: 9-Ball Pattern Drills" ILLUSTRATED PRINCIPLES

    E-Print Network [OSTI]

    Alciatore, David G.

    Billiards Digest October, 2012 "VEPP ­ Part VII: 9-Ball Pattern Drills" ILLUSTRATED PRINCIPLES-dave-billiards.com/vepp. In the last few months, we've looked at useful position control drills from Disc II. This month, we look at some 9-ball pattern drills from Disc III: "VEPP III ­ Patterns and Safety Play." You can work on cut

  1. Ball-in-Tube Linearization Example Lab 5: Nonlinear Control for a Flexible Joint

    E-Print Network [OSTI]

    ), and the parameter C can be estimated from system data (e.g., by analyzing the acceleration of the ball when input u System Implementation Laboratory Abstract One of the laboratory design challenges is the balls applied to the motor. That is, T = Cv2 in (1) where T is the thrust generated by a van driven by voltage

  2. Welcome Apro 2015 kommunikation@unibe.ch

    E-Print Network [OSTI]

    Jäger, Gerhard

    .twitter.com/unibern http://www.youtube.com/ unibeweboffice Kommunikation & Marketing Hochschulstrasse 4 3012 Bern Tel. +41 Hochschulstrasse 4 CH-3012 Bern Tel. +41 31 631 80 44 The Communication & Marketing Office assists and advises

  3. Morphological and magnetic characterization of Fe, Co, and FeCo nanoplates and nanoparticles prepared by surfactants-assisted ball milling

    E-Print Network [OSTI]

    Liu, J. Ping

    a high-energy ball milling machine for 1­20 h with hardened steel balls. The handling of the starting

  4. On electromagnetic models of ball lightning with topological structure

    E-Print Network [OSTI]

    Donoso, J M; Trueba, J L

    2003-01-01

    It has been long admitted that a consequence of the virial theorem is that there can be no equilibrium configurations of a system of charges in electromagnetic interaction in the absence of external forces. However, recent results have shown that the virial theorem can not preclude the existence of certain nontrivial equilibrium configurations. Although some of these new results are based on an effective microscopic field theory, they are important for a theory of ball lightning that has been developed by the authors of the present work. Other theoretical results relative to magnetic force-free fields with field aligned currents and self-organized filamentary structures are also found to be relevant for this model.

  5. Risk management for CAT events Georg Ch. Pflug

    E-Print Network [OSTI]

    Pflug, Georg

    Outline Risk management for CAT events Georg Ch. Pflug 20.5.2005 Georg Ch. Pflug Risk management billion in reconstruction lending. Georg Ch. Pflug Risk management for CAT events #12;Outline Fundamentals, budget reallocation, additional taxation) Georg Ch. Pflug Risk management for CAT events #12;Outline

  6. Translational energy dependence of reaction mechanism: Xe++CH4?XeH++CH3

    E-Print Network [OSTI]

    Miller, G. D.; Strattan, L. W.; Cole, C. L.; Hierl, Peter M.

    1981-01-01

    The dynamics of the exoergic ion–molecule reaction Xe+(CH4,CH3)XeH+ were studied by chemical accelerator techniques over the relative translational energy range 0.2 to 8 eV. Results of the kinematicmeasurements are reported ...

  7. Chemical accelerator studies of reaction dynamics: Ar^+ + CH4 ? ArH^+ + CH3

    E-Print Network [OSTI]

    Wyatt, J. R.; Strattan, L. W.; Snyder, S. C.; Hierl, Peter M.

    1975-01-01

    Chemical accelerator studies on isotopic variants of the reaction Ar+ + CH4 ? ArH+ + CH3 are reported. Velocity and angular distributions of the ionic product as a function of initial translational energy have been measured over the energy range 0...

  8. Thermodynamics of topological black holes in Brans-Dicke gravity with a power-law Maxwell field

    E-Print Network [OSTI]

    M. Kord Zangeneh; M. H. Dehghani; A. Sheykhi

    2015-09-20

    In this paper, we present a new class of higher dimensional exact topological black hole solutions of the Brans-Dicke theory in the presence of a power-law Maxwell field as the matter source. For this aim, we introduce a conformal transformation which transforms the Einstein-dilaton-power-law Maxwell gravity Lagrangian to the Brans-Dicke-power-law Maxwell theory one. Then, by using this conformal transformation, we obtain the desired solutions. Next, we study the properties of the solutions and conditions under which we have black holes. Interestingly enough, we show that there is a cosmological horizon in the presence of a negative cosmological constant. Finally, we calculate the temperature and charge and then by calculating the Euclidean action, we obtain the mass, the entropy and the electromagnetic potential energy. We find that the entropy does not respect the area law, and also the conserved and thermodynamic quantities are invariant under conformal transformation. Using these thermodynamic and conserved quantities, we show that the first law of black hole thermodynamics is satisfied on the horizon.

  9. ARM - Datastreams - avhrr17ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Datalacman Documentation7ch2

  10. ARM - Datastreams - fullavhrr10ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1l DocumentationDatastreamsecmwfvarch2ch4

  11. ARM - Datastreams - fullavhrr15ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1lch2 Documentation XDC documentation Datach2ch4

  12. ARM - Datastreams - fullavhrr17ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1lch2 Documentation XDC documentationch2ch4

  13. ARM - Datastreams - avhrr10ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you! SendDatastreamsaoscpcDatastreamsaossmpsDatastreamsassistch2ch2ch4

  14. ARM - Datastreams - avhrr12ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Data Quality Plots ARM Data2ch2

  15. ARM - Datastreams - avhrr14ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Data Quality Plots ARMlacnau2rad4ch2

  16. ARM - Datastreams - avhrr16ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Data Quality4radgacnau6ch4

  17. Antioxidant, color and sensory properties of sorghum bran in pre-cooked ground beef patties varying in fat and iron content 

    E-Print Network [OSTI]

    Shin, Dae Keun

    2009-05-15

    each fat level, ground beef portions were weighed and randomly assigned to control, butylated hydroxanisole (BHA) and butylated hydroxytoluene (BHT) (0.001%), rosemary (0.25%) or sorghum bran (0.25, 0.5 or 1.0%). After mixing in the appropriate...

  18. MECHATRONIC DESIGN OF A BALL ON PLATE BALANCING SYSTEM Shorya Awtar

    E-Print Network [OSTI]

    Awtar, Shorya

    MECHATRONIC DESIGN OF A BALL ON PLATE BALANCING SYSTEM Shorya Awtar Kevin C. Craig Department system based on mechatronic design principles. Realization of the design is achieved of the course Mechatronics System Design at Rensselaer. 1. MECHATRONICS AT RENSSELAER Mechatronics

  19. Micro-Ball Lens Array Fabrication in Photoresist Using Ptfe Hydrophobic Effect

    E-Print Network [OSTI]

    Shyu Ruey Fang; Tsai Wen Ren; Tsai Jhy Cherng

    2007-01-01

    This paper presents a simple method to fabricate micro-ball lens and its array. The key technology is to use the hydrophobic characteristics of polyterafluoroethylene (PTFE) substrate. High contact angle between melted photoresist pattern and PTFE can generate micro-ball lens and its array. PTFE thin film was spun onto a silicon wafer and dried in oven. Photoresist AZ4620 was used to pattern micro-columns with different diameters 60, 70 and 80 $\\mu$m. A thermal reflow process then was applied to melt these micro-column patterns resulted in micro-ball lens array. The achieved micro-ball lens array with diameter 98 $\\mu$m was fabricated using 80 $\\mu$m in diameter patterns. This method provides a simple fabrication process and low material cost.

  20. Development of a Digital Controller for a Vertical Wind Tunnel (VWT) Prototype to Mitigate Ball Fluctuations 

    E-Print Network [OSTI]

    Silva, Ramon A.

    2011-08-08

    The objective of this research was to mitigate fluctuations of a levitated ping pong ball within a vertical wind tunnel (VWT) prototype. This was made possible by remodeling the VWT system with its inherent nonlinear characteristics instead...

  1. Exciton matter sustained by colossal dispersive interactions due to enhanced polarizability: Possible clue to ball lightning

    E-Print Network [OSTI]

    Georgiev, M; Georgiev, Mladen; Singh, Jai

    2005-01-01

    Recently Gilman has pointed out that the material state of a ball lightning is both highly cohesive and flexible. He makes a specific proposal for a cohesive state arising from (colossal) Van-der-Waals attraction between highly polarizable Rydberg atoms produced under a linear lightning. We accept his general suggestions but propose that the colossal Van-der-Waals coupling may also arise from the enhanced polarizability of surrogate molecular clusters, due to the polaron gap narrowing effect. We consider a few illuminating cases and present calculations for the ammonia molecule. Although being unable to identify the exact nature of the surrogate molecules at least for the time-being, we suggest a general scenario of photoexcited vibronic excitons forming a supersaturated surrogate gas phase in which a ball arises as a result of condensation. The orange color of the luminous ball is due to radiative exciton deexcitation and suggests that there may be a unique surrogate material for ball lightning.

  2. Porosity in collapsible Ball Grid Array solder joints

    SciTech Connect (OSTI)

    Gonzalez, C.A. |

    1998-05-01

    Ball Grid Array (BGA) technology has taken off in recent years due to the increased need for high interconnect density. Opposite to all the advantages BGA packages offer, porosity in collapsible BGA solder joints is often a major concern in the reliability of such packages. The effect of pores on the strength of collapsible BGA solder-joints was studied by manufacturing samples with different degrees of porosity and testing them under a shear load. It was found that the shear strength of the solder joints decreased in a linear fashion with increasing porosity. Failure occurred by internal necking of the interpore matrix. It was confirmed that entrapment of flux residues leads to porosity by manufacturing fluxless samples in a specially made furnace, and comparing them with samples assembled using flux. Also, contamination of Au electrodeposits (in substrate metallization) was determined to cause significant porosity. It was found that hard-Au (Co hardened Au) electrodeposits produce high degrees of porosity even in the absence of flux. Finally, increasing the time the solder spends in the molten state was proven to successfully decrease porosity.

  3. A SCORM-Conformant LMS Ch. Bouras,

    E-Print Network [OSTI]

    A SCORM-Conformant LMS Ch. Bouras, Computer Engineering and Informatics Dept., Univ. of Patras tsiatsos@cti.gr Abstract: In this paper we propose a sample Learning Management System (LMS) that will be conformant with the SCORM v1.3 Specification. In particular, the sample LMS we propose will make use of both

  4. Effect of antisymmetric C–H stretching excitation on the dynamics of O({sup 1}D) + CH{sub 4} ? OH + CH{sub 3}

    SciTech Connect (OSTI)

    Pan, Huilin; Yang, Jiayue; Zhang, Dong; Shuai, Quan; Jiang, Bo [State Key Laboratory of Molecular Reaction Dynamics, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian, Liaoning 116023 (China)] [State Key Laboratory of Molecular Reaction Dynamics, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian, Liaoning 116023 (China); Dai, Dongxu; Wu, Guorong, E-mail: wugr@dicp.ac.cn, E-mail: xmyang@dicp.ac.cn; Yang, Xueming, E-mail: wugr@dicp.ac.cn, E-mail: xmyang@dicp.ac.cn [State Key Laboratory of Molecular Reaction Dynamics, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian, Liaoning 116023 (China) [State Key Laboratory of Molecular Reaction Dynamics, Dalian Institute of Chemical Physics, Chinese Academy of Sciences, Dalian, Liaoning 116023 (China); Synergetic Innovation Center of Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, Anhui 230026 (China)

    2014-04-21

    The effect of antisymmetric C–H stretching excitation of CH{sub 4} on the dynamics and reactivity of the O({sup 1}D) + CH{sub 4} ? OH + CD{sub 3} reaction at the collision energy of 6.10 kcal/mol has been investigated using the crossed-beam and time-sliced velocity map imaging techniques. The antisymmetric C–H stretching mode excited CH{sub 4} molecule was prepared by direct infrared excitation. From the measured images of the CH{sub 3} products with the infrared laser on and off, the product translational energy and angular distributions were derived for both the ground and vibrationally excited reactions. Experimental results show that the vibrational energy of the antisymmetric stretching excited CH{sub 4} reagent is channeled exclusively into the vibrational energy of the OH co-products and, hence, the OH products from the excited-state reaction are about one vibrational quantum hotter than those from the ground-state reaction, and the product angular distributions are barely affected by the vibrational excitation of the CH{sub 4} reagent. The reactivity was found to be suppressed by the antisymmetric stretching excitation of CH{sub 4} for all observed CH{sub 3} vibrational states. The degree of suppression is different for different CH{sub 3} vibrational states: the suppression is about 40%–60% for the ground state and the umbrella mode excited CH{sub 3} products, while for the CH{sub 3} products with one quantum symmetric stretching mode excitation, the suppression is much less pronounced. In consequence, the vibrational state distribution of the CH{sub 3} product from the excited-state reaction is considerably different from that of the ground-state reaction.

  5. Microsoft Word - CH1311-11 CH2M HILL Awards $1B to Small Businesses

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

    price. Since receiving the contract in 2008, CH2M HILL awarded more than 1 billion in contracts to small businesses, representing 28 percent of the contract price to-date. Of...

  6. Internal RTI Program Terms Revised: CH 02232015 Page 1

    E-Print Network [OSTI]

    Michelson, David G.

    Internal RTI Program Terms Revised: CH 02232015 Page 1 Office of Research Services Phone: (250) 807;Internal RTI Program Terms Revised: CH 02232015 Page 2 Applications (free form) must include the following

  7. Formation mechanism of the atmospheric ball lightning using the triple Beltrami equation

    E-Print Network [OSTI]

    Taveira, A M A; Taveira, Ana Marcia Alves; Sakanaka, Paulo Hiroshi

    2004-01-01

    Ball lightning, also known as fire ball, is a luminous globe which occurs in the course of a thunderstorm. Taking as model of fire ball, the two fluid plasma consisting of electrons and one species ions, and considering that the plasma flow is a finite quantity, we can derive the equation of relaxed energy state, maintaining the helicity constant, in the form of triple Beltramiequations for the magnetic field: s curl x curl x curl x B + p curl x curl x B +q curl xB +r B = 0. Where B is the magnetic field s, p, q, and r are constants to be determined through boundary conditions. This equation is coupled with an equation which describes the hydrodynamic vortex. The problem of the formation of an isolated luminous mass in the sky and the moderate persistence of the resulting form combined with observations of ball lightning describing hollow globes, surface coronas and rapid rotation led to theories depicting ball lightning as a vortex. We explore the solutions of this equation using the method of Chandrasekhar-...

  8. New Revelation of Lightning Ball Observation and Proposal for a Nuclear Reactor Fusion Experiment

    E-Print Network [OSTI]

    Domokos Tar

    2009-10-12

    In this paper, the author brings further details regarding his Lightning Ball observation that were not mentioned in the first one (Ref.1-2). Additionally, he goes more into detail as the three forces that are necessary to allow the residual crescent form the hydrodynamic vortex ring to shrink into a sphere.Further topics are the similarities and analogies between the Lightning Ball formation's theory and the presently undertaken Tokamak-Stellarator-Spheromak fusion reactor experiments. A new theory and its experimental realisation are proposed as to make the shrinking of the hot plasma of reactors into a ball possible by means of the so called long range electromagnetic forces. In this way,the fusion ignition temperature could possibly atteined.

  9. Control design and robustness analysis of a ball and plate system by using polynomial chaos

    SciTech Connect (OSTI)

    Colón, Diego; Balthazar, José M.; Reis, Célia A. dos; Bueno, Átila M.; Diniz, Ivando S.; Rosa, Suelia de S. R. F.

    2014-12-10

    In this paper, we present a mathematical model of a ball and plate system, a control law and analyze its robustness properties by using the polynomial chaos method. The ball rolls without slipping. There is an auxiliary robot vision system that determines the bodies' positions and velocities, and is used for control purposes. The actuators are to orthogonal DC motors, that changes the plate's angles with the ground. The model is a extension of the ball and beam system and is highly nonlinear. The system is decoupled in two independent equations for coordinates x and y. Finally, the resulting nonlinear closed loop systems are analyzed by the polynomial chaos methodology, which considers that some system parameters are random variables, and generates statistical data that can be used in the robustness analysis.

  10. New Revelation of Lightning Ball Observation and Proposal for a Nuclear Reactor Fusion Experiment

    E-Print Network [OSTI]

    Tar, Domokos

    2009-01-01

    In this paper, the author brings further details regarding his Lightning Ball observation that were not mentioned in the first one (Ref.1-2). Additionally, he goes more into detail as the three forces that are necessary to allow the residual crescent form the hydrodynamic vortex ring to shrink into a sphere.Further topics are the similarities and analogies between the Lightning Ball formation's theory and the presently undertaken Tokamak-Stellarator-Spheromak fusion reactor experiments. A new theory and its experimental realisation are proposed as to make the shrinking of the hot plasma of reactors into a ball possible by means of the so called long range electromagnetic forces. In this way,the fusion ignition temperature could possibly atteined.

  11. New physics in a nutshell, or Q-ball as a power plant

    E-Print Network [OSTI]

    Gia Dvali; Alexander Kusenko; Mikhail Shaposhnikov

    1997-10-30

    Future experiments may discover new scalar particles with global charges and couplings that allow for solitonic states. If the effective potential has flat directions, the scalar VEV inside a large Q-ball can exceed the particle mass by many orders of magnitude. Models with low-energy supersymmetry breaking generically have both the scalars carrying some global charges, and the flat directions. The Q-ball interior can, therefore, provide an environment for exploring physics far beyond the TeV scale without the need for building colliders of ever-increasing energies. Some Standard Model processes, otherwise strongly suppressed, can also be studied inside the soliton, where the SU(2) symmetry can be restored, and the quark confinement may be absent. Baryon number violating processes catalyzed by the large VEV inside the Q-ball can provide an inexhaustible energy resource.

  12. Titania Prepared by Ball Milling: Its Characterization and Application as Liquefied Petroleum Gas Sensor

    E-Print Network [OSTI]

    Yadav, B C; Singh, Satyendra; Yadav, T P

    2012-01-01

    Present paper reports the LPG sensing of TiO2 obtained through ball milling. The milled powder was characterized by XRD, TEM and UV-visible spectroscopy. Further the ball milled powder was compressed in to pellet using hydraulic press. This pellet was investigated with the exposure of LPG. Variations in resistance with exposure of LPG to the sensing pellet were recorded. The sensitivity of the sensor was ~ 11 for 5 vol.% of LPG. Response and recovery times of the sensor were ~ 100 and 250 sec. The sensor was quite sensitive to LPG and results were found reproducible within 91%.

  13. Textures and conditions of formation of Middle Pennsylvanian coal balls, central United States

    E-Print Network [OSTI]

    Perkins, T. W.

    1976-04-30

    of the swamp water (Zone 3 of Fig. 5). Coal balls containing plant remains that are aligned in planes paralleling the coal laminae may have formed in parts of the swamp far enough inland from the sea that the tidal currents were not powerful enough to pulverize... of the swamp water (Zone 3 of Fig. 5). Coal balls containing plant remains that are aligned in planes paralleling the coal laminae may have formed in parts of the swamp far enough inland from the sea that the tidal currents were not powerful enough to pulverize...

  14. Discrete Elements Method: A New Kind of Initial Conditions - Tetrahedral Packing of Balls

    E-Print Network [OSTI]

    Mark A. Tsayger

    2014-12-15

    The Paper discusses the use of the regular packing of identical balls with the coordination number 4 as a model of a medium consisting of fluid and solid particles in the conditions of fluidization. It is proposed to use the examined packing of balls as an initial condition for the calculations by the Discrete Elements Method (DEM) in technological processes in the fluidized bed in industry, as well as in the modeling of processes that occur in hydraulic and pneumatic transport of granular materials. Filtration properties of such packing required for its use as an initial condition in calculations by DEM are estimated.

  15. Discrete Elements Method: A New Kind of Initial Conditions - Tetrahedral Packing of Balls

    E-Print Network [OSTI]

    Mark A. Tsayger

    2015-10-13

    The Paper discusses the use of the regular packing of identical balls with the coordination number 4 as a model of a medium consisting of fluid and solid particles in the conditions of fluidization. It is proposed to use the examined packing of balls as an initial condition for the calculations by the Discrete Elements Method (DEM) in technological processes in the fluidized bed in industry, as well as in the modeling of processes that occur in hydraulic and pneumatic transport of granular materials. Filtration properties of such packing required for its use as an initial condition in calculations by DEM are estimated.

  16. ARM - Datastreams - fullavhrr10ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1l DocumentationDatastreamsecmwfvarch2

  17. ARM - Datastreams - fullavhrr12ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1l

  18. ARM - Datastreams - fullavhrr14ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1lch2 Documentation XDC documentation Data Quality

  19. ARM - Datastreams - fullavhrr14ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1lch2 Documentation XDC documentation Data

  20. ARM - Datastreams - fullavhrr15ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1lch2 Documentation XDC documentation Datach2

  1. ARM - Datastreams - fullavhrr16ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1lch2 Documentation XDC documentation

  2. ARM - Datastreams - fullavhrr17ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4Datastreamsecmwfsfc1lch2 Documentation XDC documentationch2

  3. ARM - Datastreams - avhrr10ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you! SendDatastreamsaoscpcDatastreamsaossmpsDatastreamsassistch2ch2

  4. ARM - Datastreams - avhrr11ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Data Quality Plots ARM Data Discovery

  5. ARM - Datastreams - avhrr14ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Data Quality Plots

  6. ARM - Datastreams - avhrr15ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Data Quality4rad Documentation

  7. ARM - Datastreams - avhrr15ch4

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Data Quality4rad Documentationch4

  8. ARM - Datastreams - avhrr16ch2

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity ofkandz-cm11 Comments? We would love to hear from you!ch4 Documentation XDC documentation Data Quality4radgacnau6

  9. Structural and microstructural changes in monoclinic ZrO{sub 2} during the ball-milling with stainless steel assembly

    SciTech Connect (OSTI)

    Stefanic, G. . E-mail: stefanic@irb.hr; Music, S.; Gajovic, A.

    2006-04-13

    High-energy ball-milling of monoclinic ZrO{sub 2} was performed in air using the planetary ball mill with a stainless steel milling assembly. Structural and microstructural changes during the ball-milling were monitored using X-ray powder diffraction, Raman spectroscopy, Moessbauer spectroscopy, field emission scanning electron microscopy and energy dispersive X-ray spectrometry. The results of line broadening analysis indicated a decrease in the crystallite size and an increase in the microstrains with the ball-milling time increased up to {approx}150 min. The results of quantitative phase analysis indicated the presence of a very small amount of tetragonal ZrO{sub 2} phase in this early stage of ball-milling. The onset of m-ZrO{sub 2} {sup {yields}} t-ZrO{sub 2} transition occurred between 10 and 15 h of ball-milling, which resulted in a complete transition after 20 h of ball-milling. Further ball-milling caused a decrease of the t-ZrO{sub 2} lattice parameters followed by a probable transition into c-ZrO{sub 2}. It was concluded that the stabilization of t- and c-ZrO{sub 2} polymorphs at RT can be attributed to the incorporation of aliovalent cations (Fe{sup 2+}, Fe{sup 3+} and Cr{sup 3+}) introduced into the sample due to the wear and oxidation of the milling media.

  10. A Family-Centric Genealogy Visualization Paradigm Robert Ball and David Cook

    E-Print Network [OSTI]

    Ball, Robert

    A Family-Centric Genealogy Visualization Paradigm Robert Ball and David Cook Stephen F. Austin State University Department of Computer Science {ballrg | cookda}@sfasu.edu ABSTRACT Genealogy is a way for future behavior. Genealogical visualizations are used to help understand and share the story of the past

  11. Precision Stabilization Simulation of a Ball Joint Gimbaled Mirror Using Advanced MATLAB

    E-Print Network [OSTI]

    Hernandez, Orlando

    Precision Stabilization Simulation of a Ball Joint Gimbaled Mirror Using Advanced MATLAB, they suffer from the common problems of weight and power requirements, and mechanical envelope constraints gimbaled mirror using advanced MATLAB tools and packages. 1. Introduction Our goal in this work

  12. FOB Undergoing Test and Alignment in FAS at Ball Aerospace OPTICAL TESTS AND ALIGNMENTS

    E-Print Network [OSTI]

    Schneider, Glenn

    FOB Undergoing Test and Alignment in FAS at Ball Aerospace OPTICAL TESTS AND ALIGNMENTS After the FOB alignment is complete, and it passes environmental tests, it will be checked out in a second HST. The NICMOS FOB will relay simulated images from RAS/HOMS to a Photometrics CCD camera placed where the three

  13. Billiards Digest September, 2012 "VEPP Part VI: Line-of-Balls Drill" ILLUSTRATED PRINCIPLES

    E-Print Network [OSTI]

    Alciatore, David G.

    Billiards Digest September, 2012 "VEPP ­ Part VI: Line-of-Balls Drill" ILLUSTRATED PRINCIPLES David-dave-billiards.com/vepp. Last month, we looked at useful center-of-table drills from Disc II: "VEPP II ­ Position Control and English." This month, we'll look at another type of position control drill, also from the second DVD

  14. High-speed X-ray imaging of a ball impacting on loose sand

    E-Print Network [OSTI]

    Homan, Tess; Lohse, Detlef; van der Meer, Devaraj

    2014-01-01

    When a ball is dropped in fine, very loose sand, a splash and subsequently a jet are ob- served above the bed, followed by a granular eruption. To directly and quantitatively determine what happens inside the sand bed, high-speed X-ray tomography measurements are carried out in a custom-made setup that allows for imaging of a large sand bed at atmospheric pressures. Herewith we show that the jet originates from the pinch-off point created by the collapse of the air cavity formed behind the penetrating ball.Subsequently we measure how the entrapped air bubble rises through the sand and show that this is consistent with bubbles rising in continuously fluidized beds. Finally, we measure the packing fraction variation throughout the bed. From this we show that there is (i) a compressed area of sand in front of and next to the ball while the ball is moving down, (ii) a strongly compacted region at the pinch-off height after the cavity collapse; and (iii) a relatively loosely packed center in the wake of the rising...

  15. The photo-balls and static solutions in NCQED with time attended

    E-Print Network [OSTI]

    Abolfazl Jafari

    2011-05-26

    We drive the potential of photon interaction from Feynman diagrams amplitudes, and we show that the photo-balls, can be produced in noncommutative electrodynamics with time attended but for the static and localized fields, the static solutions (the lumps) can not be exited.

  16. The"Core"of the Workout Should Be on the Ball

    E-Print Network [OSTI]

    are restrictive, focusing on one component per movement, rather than blending many components into one. Core into strength and conditioning protocols as a fundamental component of core training. This type of training ball to encompass as many components in a single movement as expertise and performance increases

  17. Statistical properties of position-dependent ball-passing networks in football games

    E-Print Network [OSTI]

    Narizuka, Takuma; Yamazaki, Yoshihiro

    2013-01-01

    Statistical properties of position-dependent ball-passing networks in real football games are examined. We find that the networks have the small-world property, and their degree distributions are fitted well by a truncated gamma distribution function. In order to reproduce these properties of networks, a model based on a Markov chain is proposed.

  18. RECONSTRUCTION OF THE ORIENTATION DISTRIBUTION FUNCTION IN SINGLE AND MULTIPLE SHELL Q-BALL IMAGING WITHIN

    E-Print Network [OSTI]

    direction) from q-ball data uses linear radial projection, neglecting the change in the volume element along in a dimensionless and normalized ODF expression. Our model is flexible enough so ODFs can either be estimated from (DWMRI) provides valuable information about the fiber architecture of neural tissue by measuring

  19. Central Characterization Program (CCP) Contact-Handled (CH) TRU...

    Office of Environmental Management (EM)

    and Waste Information SystemWaste Data System (WWISWDS) Data Entry Central Characterization Program (CCP) Contact-Handled (CH) TRU Waste Certification and Waste Information...

  20. CH2D+, the Search for the Holy Grail

    E-Print Network [OSTI]

    Roueff, E; Lis, D C; Wootten, A; Marcelino, N; cernicharo, J; Tercero, B

    2013-01-01

    CH2D+, the singly deuterated counterpart of CH3+, offers an alternative way to mediate formation of deuterated species at temperatures of several tens of K, as compared to the release of deuterated species from grains. We report a longstanding observational search for this molecular ion, whose rotational spectroscopy is not yet completely secure. We summarize the main spectroscopic properties of this molecule and discuss the chemical network leading to the formation of CH2D+, with explicit account of the ortho/para forms of H2, H3+ and CH3+. Astrochemical models support the presence of this molecular ion in moderately warm environments at a marginal level.

  1. Capturing fleeting intermediates in a catalytic CH amination reaction cycle

    E-Print Network [OSTI]

    Zare, Richard N.

    for the mechanistic study of catalytic processes. mass spectrometry | transient intermediates | C­H oxidation | catalysis Catalytic methods for selective C­H oxidation rely on the exquisite choreography of a series oxidant (4, 5, 11). The fast rates of the on- and off-path steps in this catalytic process

  2. Approved Module Information for CH3117, 2014/5 Module Title/Name: Literature Research Project Module Code: CH3117

    E-Print Network [OSTI]

    Neirotti, Juan Pablo

    Approved Module Information for CH3117, 2014/5 Module Title/Name: Literature Research Project Module Code: CH3117 School: Engineering and Applied Science Module Type: Standard Module New Module? No Module Credits: 10 Module Management Information Module Leader Name Andrew James Sutherland Email Address

  3. Perspective on the reactions between F and CH3CH2F: The free energy landscape of the

    E-Print Network [OSTI]

    Nielsen, Steven O.

    Perspective on the reactions between F and CH3CH2F: The free energy landscape of the E2 and SN2, 2004) Recently, we computed the 3D free energy surface of the base- induced elimination reaction by the exploration of the six-dimensional free energy landscape, sampling, and mapping out the eight stable states

  4. Dusky Dolphin (Lagenorhynchus obscurus) Underwater Bait-Balling Behaviors and Acoustic Signals: A Comparison Between Argentina and New Zealand 

    E-Print Network [OSTI]

    Vaughn, Robin

    2011-07-14

    I characterized dusky dolphin (Lagenorhynchus obscurus) underwater bait-balling behaviors and acoustic signals, and compared data between Argentina and New Zealand (NZ) to investigate the roles of ecology versus social learning. I quantified prey...

  5. Report on the Discrete Analysis Programme at INI. Keith Ball, Franck Barthe, Ben Green and Assaf Naor

    E-Print Network [OSTI]

    Report on the Discrete Analysis Programme at INI. Keith Ball, Franck Barthe, Ben Green and Assaf. The INI decided to experiment with streaming the lectures of the first INI workshop to Paris so

  6. Hardness variation and cyclic crystalline-amorphous phase transformation in CuZr alloy during ball milling

    E-Print Network [OSTI]

    Schoen, David Taylor

    2005-01-01

    The hardness and percent crystallinity of Cu33Zr67 powder samples are measured through several cycles of a cyclic phase transformation during ball milling. Each are found to cycle with a period of approximately 320 minutes. ...

  7. Preparation of Micrometer-to Sub-micrometer-Sized Nanostructured Silica Particles Using High-Energy Ball Milling

    E-Print Network [OSTI]

    Mitchell, Brian S.

    ,* and Yunfeng Lu Department of Chemical and Biomolecular Engineering, Tulane University, New Orleans, Louisiana such as milling media (zirconia, stainless steel, or steel- centered nylon balls), milling time, and the presence

  8. Implications of Carbonate Petrology and Geochemistry for the Origin of Coal Balls from the Kalo Formation (Moscovian, Pennsylvanian) of Iowa 

    E-Print Network [OSTI]

    Jones, Courtney

    2012-10-19

    Coal balls are carbonate concretions formed in peat during the Pennsylvanian and early Permian. Microprobe and microscope analysis reveal that polycrystals of high-Mg calcite (HMC), which are also high in Sr, are the ...

  9. A Ball Lightning Model as a Possible Explanation of Recently Reported Cavity Lights

    SciTech Connect (OSTI)

    Fryberger, David; /SLAC

    2009-08-04

    The salient features of cavity lights, in particular, mobile luminous objects (MLO's), as have been experimentally observed in superconducting accelerator cavities, are summarized. A model based upon standard electromagnetic interactions between a small particle and the 1.5 GHz cavity excitation field is described. This model can explain some features of these data, in particular, the existence of particle orbits without wall contact. While this result is an important success for the model, it is detailed why the model as it stands is incomplete. It is argued that no avenues for a suitable extension of the model through established physics appear evident, which motivates an investigation of a model based upon a more exotic object, ball lightning. As discussed, further motivation derives from the fact that there are significant similarities in many of the qualitative features of ball lightning and MLO's, even though they appear in quite different circumstances and differ in scale by orders of magnitude. The ball lightning model, which incorporates electromagnetic charges and currents, is based on a symmetrized set of Maxwell's equations in which the electromagnetic sources and fields are characterized by a process called dyality rotation. It is shown that a consistent mathematical description of dyality rotation as a physical process can be achieved by adding suitable (phenomenological) current terms to supplement the usual current terms in the symmetrized Maxwell's equations. These currents, which enable the conservation of electric and magnetic charge, are called vacuum currents. It is shown that the proposed ball lightning model offers a good qualitative explanation of the perplexing aspects of the MLO data. Avenues for further study are indicated.

  10. Degree distribution of position-dependent ball-passing networks in football games

    E-Print Network [OSTI]

    Narizuka, Takuma; Yamazaki, Yoshihiro

    2015-01-01

    We propose a simple stochastic model describing the position-dependent ball-passing network in football games. In this network, a player on a certain area in the divided fields is a node, and a pass between two nodes corresponds to an edge. Our model is characterized by the consecutive choice of a node dependent on its intrinsic fitness. We derive the explicit expression of the degree distribution, and find that the derived distribution reproduces the real data quit well.

  11. Comments in support of the dipole model of ball lightning (BL)

    E-Print Network [OSTI]

    Soshnikov, V N

    2010-01-01

    The evaluations are presented justifying previously proposed dipole model of ball lightning (BL). The movement and energy supporting the dipole BL are due to the atmospheric electric field. Stability of the BL is due to the fundamental role of energy loss by radiation. An example is presented of calculating the stability of variant of BL. There is also a possible connection of stability BL with a statistical distributions of the atmospheric electric field in time and space.

  12. Standard Practice for Determining Resistance of Solar Collector Covers to Hail by Impact With Propelled Ice Balls

    E-Print Network [OSTI]

    American Society for Testing and Materials. Philadelphia

    1992-01-01

    1.1 This practice covers a procedure for determining the ability of cover plates for flat-plate solar collectors to withstand impact forces of falling hail. Propelled ice balls are used to simulate falling hailstones. This practice is not intended to apply to photovoltaic cells or arrays. 1.2 This practice defines two types of test specimens, describes methods for mounting specimens, specifies impact locations on each test specimen, provides an equation for determining the velocity of any size ice ball, provides a method for impacting the test specimens with ice balls, and specifies parameters that must be recorded and reported. 1.3 This practice does not establish pass or fail levels. The determination of acceptable or unacceptable levels of ice-ball impact resistance is beyond the scope of this practice. 1.4 The size of ice ball to be used in conducting this test is not specified in this practice. This practice can be used with various sizes of ice balls. 1.5 The categories of solar collector cover plat...

  13. Population SAMC, ChIP-chip Data Analysis and Beyond 

    E-Print Network [OSTI]

    Wu, Mingqi

    2011-02-22

    This dissertation research consists of two topics, population stochastics approximation Monte Carlo (Pop-SAMC) for Baysian model selection problems and ChIP-chip data analysis. The following two paragraphs give a brief introduction to each...

  14. Revised 6/5/13 CH369: Fundamentals of Biochemistry

    E-Print Network [OSTI]

    1 Revised 6/5/13 CH369: Fundamentals of Biochemistry Summer 2013 Syllabus and Course Policies What is biochemistry? Biochemistry is a branch of science biochemistry is its own distinctive discipline with regard to its emphasis

  15. Revised 9/28/2011 CH369: Fundamentals of Biochemistry

    E-Print Network [OSTI]

    1 Revised 9/28/2011 CH369: Fundamentals of Biochemistry Spring 2012 Syllabus and Course Policies What is biochemistry? Study of the structure and properties down. "Organic chemistry is the chemistry of carbon compounds. Biochemistry

  16. Understanding mechanisms for C-H bond activation 

    E-Print Network [OSTI]

    Vastine, Benjamin Alan

    2009-05-15

    The results from density functional theory (DFT) studies into C–H bond activation, hydrogen transfer, and alkyne–to–vinylidene isomerization are presented in this work. The reaction mechanism for the reductive elimination ...

  17. Analysis of the mouse embryonic stem cell regulatory networks obtained by ChIP-chip and ChIP-PET

    E-Print Network [OSTI]

    Mathur, Divya

    Background: Genome-wide approaches have begun to reveal the transcriptional networks responsible for pluripotency in embryonic stem (ES) cells. Chromatin Immunoprecipitation (ChIP) followed either by hybridization to a ...

  18. Generation of drugs coated iron nanoparticles through high energy ball milling

    SciTech Connect (OSTI)

    Radhika Devi, A.; Murty, B. S. [Department of Metallurgical and Materials Engineering, Indian Institute of Technology Madras, Chennai 600036 (India); Chelvane, J. A. [Defence Metallurgical Research Laboratory, Hyderabad 500058 (India); Prabhakar, P. K.; Padma Priya, P. V.; Doble, Mukesh [Department of Biotechnology, Indian Institute of Technology Madras, Chennai 600036 (India)

    2014-03-28

    The iron nanoparticles coated with oleic acid and drugs such as folic acid/Amoxicillin were synthesized by high energy ball milling and characterized by X-ray diffraction, Transmission electron microscope, zeta potential, dynamic light scattering, Fourier Transform Infra red (FT-IR) measurements, and thermo gravimetric analysis (TGA). FT-IR and TGA measurements show good adsorption of drugs on oleic acid coated nanoparticles. Magnetic measurements indicate that saturation magnetization is larger for amoxicillin coated particles compared to folic acid coated particles. The biocompatibility of the magnetic nanoparticles prepared was evaluated by in vitro cytotoxicity assay using L929 cells as model cells.

  19. CH4 sources estimated from atmospheric observations of CH4 and its C isotopic ratios: 1. Inverse modeling of source processes

    E-Print Network [OSTI]

    Fletcher, Sara E. Mikaloff

    , coal mining, biomass burning, and landfills. CH4 is also produced naturally by anaerobic bacteria in wetlands, dry tundra, and termites. The oceans evolve CH4 from anaerobic bacteria in surface waters, fossil

  20. Extended phase space thermodynamics and P-V criticality: Brans-Dicke-Born-Infeld vs Einstein-BI-dilaton black holes

    E-Print Network [OSTI]

    S. H. Hendi; R. Moradi; Z. Armanfard

    2015-11-25

    Following interesting resemblance between black holes and Van der Waals liquid/gas system, in this paper, we study $P-V$ criticality of both dilatonic Born-Infeld black holes and their conformal solutions, the so-called Brans-Dicke-Born-Infeld solutions. At first, we regard spherically symmetric nonlinearly charged black hole solutions in both Einstein and Jordan frames and calculate related conserved and thermodynamic quantities. Then, we take into account the cosmological constant proportional to thermodynamical pressure to extend the phase space. After that we obtain critical values of thermodynamic coordinates to plot proper $P-V$ and $G-T$ diagrams. Investigation of the mentioned diagrams helps us to study the possibility of the thermodynamical phase transition.

  1. Extended phase space thermodynamics and P-V criticality: Brans-Dicke-Born-Infeld vs Einstein-BI-dilaton black holes

    E-Print Network [OSTI]

    Hendi, S H; Armanfard, Z

    2015-01-01

    Following interesting resemblance between black holes and Van der Waals liquid/gas system, in this paper, we study $P-V$ criticality of both dilatonic Born-Infeld black holes and their conformal solutions, the so-called Brans-Dicke-Born-Infeld solutions. At first, we regard spherically symmetric nonlinearly charged black hole solutions in both Einstein and Jordan frames and calculate related conserved and thermodynamic quantities. Then, we take into account the cosmological constant proportional to thermodynamical pressure to extend the phase space. After that we obtain critical values of thermodynamic coordinates to plot proper $P-V$ and $G-T$ diagrams. Investigation of the mentioned diagrams helps us to study the possibility of the thermodynamical phase transition.

  2. Extended phase space thermodynamics and P-V criticality: Brans-Dicke-Born-Infeld vs Einstein-BI-dilaton black holes

    E-Print Network [OSTI]

    S. H. Hendi; R. Moradi; Z. Armanfard

    2015-10-23

    Following interesting resemblance between black holes and Van der Waals liquid/gas system, in this paper, we study $P-V$ criticality of both dilatonic Born-Infeld black holes and their conformal solutions, the so-called Brans-Dicke-Born-Infeld solutions. At first, we regard spherically symmetric nonlinearly charged black hole solutions in both Einstein and Jordan frames and calculate related conserved and thermodynamic quantities. Then, we take into account the cosmological constant proportional to thermodynamical pressure to extend the phase space. After that we obtain critical values of thermodynamic coordinates to plot proper $P-V$ and $G-T$ diagrams. Investigation of the mentioned diagrams helps us to study the possibility of the thermodynamical phase transition.

  3. Hydro-ball in-core instrumentation system and method of operation

    DOE Patents [OSTI]

    Tower, Stephen N. (Washington Township, Westmoreland County, PA); Veronesi, Luciano (O'Hara Township, Allegheny County, PA); Braun, Howard E. (Pittsburgh, PA)

    1990-01-01

    A hydro-ball in-core instrumentation system employs detector strings each comprising a wire having radiation sensitive balls affixed diametrically at spaced positions therealong and opposite tip ends of which are transportable by fluid drag through interior passageways. In the passageways primary coolant is caused to flow selectively in first and second opposite directions for transporting the detector strings from stored positions in an exterior chamber to inserted positions within the instrumentation thimbles of the fuel rod assemblies of a pressure vessel, and for return. The coolant pressure within the detector passageways is the same as that within the vessel; face contact, disconnectable joints between sections of the interior passageways within the vessel facilitate assembly and disassembly of the vessel for refueling and routine maintenance operations. The detector strings may pass through a very short bend radius thereby minimizing space requirements for the connections of the instrumentation system to the vessel and concomitantly the vessel containment structure. Improved radiation mapping and a significant reduction in potential exposure of personnel to radiation are provided. Both top head and bottom head penetration embodiments are disclosed.

  4. Physical conditions of the ball lightning ejection caused by interaction of electrical discharge with metal and polymer

    E-Print Network [OSTI]

    Emelin, S E; Skvortsov, G E; Bychkov, V L

    2001-01-01

    Physical conditions of formation of the ball lightning with high energy density considered as condensate of heavily excited atoms have been studied. In our approach the ball lightning formation processes is considered as a form of energy-structure self-organi-zation on the base of metastable substance and interchange. We propose different variants of the experimental method to create autonomous formation on the base of the closed capillary discharge allowing to obtain the objects with the life time up to 2s which burn through the foil, explode and can penetrate through the polymer wall without destroying it.

  5. Chung Qui Ch T i Cantor Ng Quang Hng

    E-Print Network [OSTI]

    Ngo, Hung Q.

    USD [20] và danh ti ng i vào l ch s khoa h c. Cng nh bài toán Fermat l n, b n thân câu tr l i cho bài này [11], thách hn n a th k nghiên c u c a các 1 #12;k s và khoa h c gia hàng u. Ng c l i, cng không

  6. Trans. Nonferrous Met. Soc. China 23(2013) 1356-1366 Effects of ball milling time on porous Ti-3Ag alloy and

    E-Print Network [OSTI]

    Zheng, Yufeng

    2013-01-01

    . A special powder metallurgy method was used to prepare the porous Ti-3Ag alloys [25]. The ball milling time time during powder metallurgy on porous Ti-3Ag alloys and its apatite-inducing ability in a modified alloys with 3% Ag were fabricated by powder metallurgy process with different ball milling Foundation

  7. Enantioselective nickel catalysis : exploiting activated C-H bonds

    E-Print Network [OSTI]

    Bencivenga, Nicholas Ernest

    2012-01-01

    A method for the nickel-catalyzed cross-coupling between benzoxazole and secondary halides was explored. This method was to make use of the activated C-H bond found in benzoxazole at the 2-position to generate the nucleophilic ...

  8. Ch.2 Solar Energy to Earth and the Seasons

    E-Print Network [OSTI]

    Pan, Feifei

    Ch.2 Solar Energy to Earth and the Seasons #12;Learning Objective One: The Solar System #12;Milky Aphelion ­ farthest, on July 4 152,083,000 km #12;Learning Objective Two: The Solar Energy #12;What is Solar Energy? Energy is the capacity of a physical system to do work. The unit is Joule (J). Solar

  9. AT 351 Lab 3: Seasons and Surface Temperature (Ch. 3)

    E-Print Network [OSTI]

    Rutledge, Steven

    an important role in an area's local vertical temperature distribution. Below, Figure 1 shows the verticalAT 351 Lab 3: Seasons and Surface Temperature (Ch. 3) Question #1: Seasons (20 pts) A. In your own words, describe the cause of the seasons. B. In the Northern Hemisphere we are closer to the sun during

  10. Revised 5/23/2012 CH369: Fundamentals of Biochemistry

    E-Print Network [OSTI]

    1 Revised 5/23/2012 CH369: Fundamentals of Biochemistry Summer 2012 Unique #90770: 10:00-11:30 am in WEL 2.246 Syllabus and Course Policies What is biochemistry is the chemistry of carbon compounds. Biochemistry is the study of carbon compounds

  11. Molecular Dynamics of Methanol Monocation (CH3OH+ ) in Strong

    E-Print Network [OSTI]

    Schlegel, H. Bernhard

    Molecular Dynamics of Methanol Monocation (CH3OH+ ) in Strong Laser Fields Bishnu Thapa and H surfaces of methanol neutral, monocation, and singlet and triplet dication were explored using the CBS in the presence of a 2.9 × 1014 W/cm2 800 nm laser field for methanol monocation on the ground state potential

  12. ChE 210A M. F. Doherty Thermodynamics

    E-Print Network [OSTI]

    Bigelow, Stephen

    ChE 210A M. F. Doherty Thermodynamics Instructor: Michael F. Doherty (mfd@engineering.ucsb.edu, 893 is an introduction to the fundamentals of classical and statistical thermodynamics. We focus on equilibrium are formulated using either classical or statistical thermodynamics, and these methods have found wide

  13. People's Physics book Ch 2-1 The Big Idea

    E-Print Network [OSTI]

    California at Santa Cruz, University of

    People's Physics book Ch 2-1 The Big Idea Energy is a measure of the amount of, or potential for, dynamical activity in something. The total amount of energy in the universe is always the same universe. A group of things (we'll use the word system) has a certain amount of energy. Energy can be added

  14. People's Physics Book Ch 5-1 The Big Idea

    E-Print Network [OSTI]

    California at Santa Cruz, University of

    People's Physics Book Ch 5-1 The Big Idea Acceleration is caused by force. All forces come in pairs of two bodies upon each other are always equal, and directed to contrary parts. Key Concepts · An object pairs must obey three rules: they must be of the same type of force, 1 Principia in modern English

  15. Seismic Tomography: Definitions Lapo Boschi (lapo@erdw.ethz.ch)

    E-Print Network [OSTI]

    Boschi, Lapo

    Seismic Tomography: Definitions Lapo Boschi (lapo@erdw.ethz.ch) September 14, 2009 Seismic Tomography Seismic tomography is the science of interpreting seismic measurements (seismograms) to derive information about the structure of the Earth. This course does not cover the techniques of seismic observation

  16. Whitey Swagelok SCHe Ball Valves Provide Isolation between SCHe Purge Lines C and D and the Process Vent

    SciTech Connect (OSTI)

    MISKA, C.R.

    2000-09-15

    These valves are 1/4 inch ball valves fabricated of 316 stainless steel. Packing is TFE (standard). They provide an isolation function betwen SCHe Purge Line C, (PV-V-*079), and Purge Line D, (PV-V-*080), and the Process Vent.

  17. Whitey Swagelok SCHe Ball Valves Provide Isolation between SCHe Purge Lines C and D and the Process Vent

    SciTech Connect (OSTI)

    VAN KATWIJK, C.

    2000-06-21

    These valves are 1/4 inch ball valves fabricated of 316 stainless steel. Packing is TFE (standard). They provide an isolation function between SCHe Purge Line C, (PV-V-*079), and Purge Line D, (PV-V-*080), and the Process Vent.

  18. Whitey Swagelok SCHe ball valves Provide Isolation between SCHe Purge Lines C and D and the Process Vent

    SciTech Connect (OSTI)

    MISKA, C.R.

    2000-09-03

    These valves are 1/4 inch ball valves fabricated of 316 stainless steel. Packing is TFE (standard). They provide an isolation function betwen SCHe Purge Line C, (PV-V-*079), and Purge Line D, (PV-V-*080), and the Process Vent.

  19. Crystal ball 2011mbt_245 109..137 In this feature, leading researchers in the field of microbial

    E-Print Network [OSTI]

    Angenent, Lars T.

    energy to be harvested by the microbial community catalysing the process (Hanselmann, 1991Crystal ball ­ 2011mbt_245 109..137 In this feature, leading researchers in the field of microbial). In theory, the bio- processing of organic substrates in an open microbial community-based process

  20. X-ray photoelectron emission spectromicroscopic analysis of arborescent lycopsid cell wall composition and Carboniferous coal ball preservation

    E-Print Network [OSTI]

    Boyce, C. Kevin

    composition and Carboniferous coal ball preservation C. Kevin Boyce a, , Mike Abrecht b , Dong Zhou b , P that were canopy dominants of many Pennsylvanian coal swamp forests. Its periderm or bark--the single greatest biomass contributor to many Late Paleozoic coals--is found to have a greater aliphatic content

  1. Non-stationary dynamics in the bouncing ball: A wavelet perspective

    SciTech Connect (OSTI)

    Behera, Abhinna K., E-mail: abhinna@iiserkol.ac.in; Panigrahi, Prasanta K., E-mail: pprasanta@iiserkol.ac.in [Department of Physical Sciences, Indian Institute of Science Education and Research (IISER) Kolkata, Mohanpur 741246 (India); Sekar Iyengar, A. N., E-mail: ansekar.iyengar@saha.ac.in [Plasma Physics Division, Saha Institute of Nuclear Physics (SINP), Sector 1, Block-AF, Bidhannagar, Kolkata 700064 (India)

    2014-12-01

    The non-stationary dynamics of a bouncing ball, comprising both periodic as well as chaotic behavior, is studied through wavelet transform. The multi-scale characterization of the time series displays clear signatures of self-similarity, complex scaling behavior, and periodicity. Self-similar behavior is quantified by the generalized Hurst exponent, obtained through both wavelet based multi-fractal detrended fluctuation analysis and Fourier methods. The scale dependent variable window size of the wavelets aptly captures both the transients and non-stationary periodic behavior, including the phase synchronization of different modes. The optimal time-frequency localization of the continuous Morlet wavelet is found to delineate the scales corresponding to neutral turbulence, viscous dissipation regions, and different time varying periodic modulations.

  2. Comments to support the Dipole Dynamical Model (DDM) of Ball Lightning (BL)

    E-Print Network [OSTI]

    V. N. Soshnikov

    2015-08-13

    I present estimates to justify previously proposed by me heuristic Dipole Dynamical Model (DDM) of Ball Lightning (BL). The movement and energy supplying to the dipole BL are due to the atmospheric electric field. Crucial for the detailed analysis of BL is using the new relation of balance of the force of atmospheric electric field (per unit mass of electron cloud) and dipole forces electrons-ions within BL dipole (per unit mass of BL) as the first necessary condition for the existance of BL as an integer. This model is unique because, unlike existing static models, fundamental condition for the existence of Ball Lightning is its forward motion. The virial theorem limiting BL power does not apply to BL which is not closed system like the Sun or Galaxy systems and is strongly dependent part of the infinitely extended in time and space large system. Stability of BL is due to two free parameters with the fundamental role of thermodynamic non-equilibrium, ionization, recombination and translational movement with energy loss by radiation and also excess volumetric positive charge. Stability of BL is not related to the presence of any external shells. Polarization degree of BL plasma is characterized by polarizability factor {\\gamma}. An example is presented of calculating the stability of option BL. There is also a possible connection of stability BL with statistical distributions of the atmospheric electric field in time and space. Destruction of BL can also occur due to arising kinematical instability at its accelerating (or decelerating) movement. Maximal energy density in BL DDM does not exceed the value Espec<(10(8) - 10(9)) J/m(3). Resulting indefinitely long BL lifetime is also discussed. BL has no outer shell and no any inner rigid microstructure elements.

  3. Comments to support the Dipole Dynamical Model (DDM) of Ball Lightning (BL)

    E-Print Network [OSTI]

    V. N. Soshnikov

    2015-10-03

    I present estimates to justify previously proposed by me heuristic Dipole Dynamical Model (DDM) of Ball Lightning (BL). The movement and energy supplying to the dipole BL are due to the atmospheric electric field. Crucial for the detailed analysis of BL is using the new relation of balance of the force of atmospheric electric field (per unit mass of electron cloud) and dipole forces electrons-ions within BL dipole (per unit mass of BL) as the first necessary condition for the existance of BL as an integer. This model is unique because, unlike existing static models, fundamental condition for the existence of Ball Lightning is its forward motion. The virial theorem limiting BL power does not apply to BL which is not closed system like the Sun or Galaxy systems and is strongly dependent part of the infinitely extended in time and space large system. Stability of BL is due to two free parameters with the fundamental role of thermodynamic non-equilibrium, ionization, recombination and translational movement with energy loss by radiation and also excess volumetric positive charge. Stability of BL is not related to the presence of any external shells. Polarization degree of BL plasma is characterized by polarizability factor {\\gamma}. An example is presented of calculating the stability of an option of BL. There is also a possible connection of stability BL with statistical distributions of the atmospheric electric field in time and space. Destruction of BL can also occur due to arising kinematical instability at its accelerating (or decelerating) movement. Maximal energy density in BL DDM does not exceed the value Espec<(10(8) - 10(9)) J/m(3) decreasing with the growing BL radius. Resulting indefinitely long BL lifetime is also discussed. BL has no outer shell and no any inner rigid or elastic microstructure elements.

  4. Vibrational relaxation of CH3I in the gas phase and in solution

    E-Print Network [OSTI]

    Elles, Christopher G.; Cox, M. Jocelyn; Crim, F. Fleming

    2004-03-30

    Transient electronic absorption measurements reveal the vibrational relaxation dynamics of CH(3)I following excitation of the C–H stretch overtone in the gas phase and in liquid solutions. The isolated molecule relaxes through two stages...

  5. Stoichiometry of CH4 and CO2 flux in a California Rice Paddy

    E-Print Network [OSTI]

    McMillan, Andrew M. S.; Goulden, Michael L.; Tyler, Stanley C.

    2007-01-01

    relationships between NEP, NPP and CH 4 emissions wouldfluxes of CH 4 and/or NEP. [ 7 ] Simultaneous measurements4.5% to 5.6% of preharvest NEP). During the growing season

  6. Quantitative Visualization of ChIP-chip Data by Using Linked...

    Office of Scientific and Technical Information (OSTI)

    Quantitative Visualization of ChIP-chip Data by Using Linked Views Citation Details In-Document Search Title: Quantitative Visualization of ChIP-chip Data by Using Linked Views...

  7. Voluntary Protection Program Onsite Review, CH2M HILL B&W West...

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

    CH2M HILL B&W West Valley LLC, West Valley Demonstration Project - October 2013 Voluntary Protection Program Onsite Review, CH2M HILL B&W West Valley LLC, West Valley Demonstration...

  8. Theoretical Studies of the sp2 C-H Bond Activation

    E-Print Network [OSTI]

    Burke, Kieron

    -picoline C-H activation chemistry is proceeded by -bond metathesis for both the thorium and uranium (C5Me5Theoretical Studies of the sp2 versus sp3 C-H Bond Activation Chemistry of 2-Picoline by (C5Me5)2An activation chemistry of (C5Me5)2Th(CH3)2 and (C5Me5)2U(CH3)2 with 2-picoline (2- methylpyridine) is examined

  9. Palladium-Catalysed CH Activation of Aliphatic Amines! to give Strained Nitrogen Heterocycles !

    E-Print Network [OSTI]

    Jackson, Sophie

    Palladium-Catalysed C­H Activation of Aliphatic Amines! to give Strained Nitrogen Heterocycles. The University of Cambridge, Lensfield Road, Cambridge, CB2 1EW.! Palladium-Catalyzed C­H Activation Modes cyclopalladation complex N H palladium catalyst directed C­H activation oxidant C­Pd functionalization 4-membered

  10. MODELING THE EMISSIONS OF NITROUS OXIDE (N20) AND METHANE (CH 4) FROM THE

    E-Print Network [OSTI]

    MODELING THE EMISSIONS OF NITROUS OXIDE (N20) AND METHANE (CH 4) FROM THE TERRESTRIAL BIOSPHERE;2 #12;MODELING THE EMISSIONS OF NITROUS OXIDE (N 20) AND METHANE (CH 4) FROM THE TERRESTRIAL BIOSPHERE cli- mate has on natural emissions of N2 0 and CH4 from the terrestrial biosphere to the atmosphere

  11. Modes of Activation of Organometallic Iridium Complexes for Catalytic Water and C-H Oxidation

    E-Print Network [OSTI]

    Zare, Richard N.

    Modes of Activation of Organometallic Iridium Complexes for Catalytic Water and C-H Oxidation - ) or (cod)IrI (cod = cyclooctadiene) complexes, which are water and C-H oxidation catalyst precursors. Extensive oxidation of the Cp* ligand is observed, likely beginning with electrophilic C-H hydroxylation

  12. 2001 by M. Kosticwww.kostic.niu.edu Ch.3: Measurement System Behavior

    E-Print Network [OSTI]

    Kostic, Milivoje M.

    1 ©2001 by M. Kosticwww.kostic.niu.edu Ch.3: Measurement System Behavior · Ch.3: Measurement System) · Magnitude ratio (2nd O.S.) · Phase shift (2nd O.S.) · 2nd Order System (MathCAD) · The End ©2001 by M. Kosticwww.kostic.niu.edu Ch.3:MeasurementSystem Behavior #12;2 ©2001 by M. Kosticwww

  13. A first principles study of CH 3 dehydrogenation on Ni(111) A. Michaelides and P. Hu

    E-Print Network [OSTI]

    Alavi, Ali

    step in funda- mental catalytic processes such as steam reforming and methanation. It is also); 10.1063/1.3297885 The internal energy of CO 2 produced by the catalytic oxidation of CH 3 OH by O 2 on Ni 111 , a crucial step in many important catalytic reactions. The reaction, CH3 ads CH2 ads H ads

  14. Volume 2, Chapter 1: A General Discussion on Construction of Ch'in

    E-Print Network [OSTI]

    Binkley, Jim

    to explain these mysteries in successive order starting from selecting materials, to construction, to repairs) ch'in handbook 7 . Nowadays these ch'in are seldom seen. Also if one examines all of the ch'in handbooks it is rare that one will find anything about construction. Some of them occasionally will mention

  15. Liu UCD Phy9B 07 1 Ch 35. Interference

    E-Print Network [OSTI]

    Yoo, S. J. Ben

    Liu UCD Phy9B 07 1 Ch 35. Interference #12;Liu UCD Phy9B 07 2 35-1. Interference & Coherence #12;Liu UCD Phy9B 07 4 35-2. Two Source Interference of Light Thomas Young's experiment (1800... Spacing between adjacent maxima /minima: R/d (R>>d, R>>ym) #12;Liu UCD Phy9B 07 6 35-3. Intensity

  16. Excitation functions for the reactions of Ar^+ with CH4, CD4, and CH2D2

    E-Print Network [OSTI]

    Wyatt, J. R.; Strattan, L. W.; Chivalak, S.; Hierl, Peter M.

    1975-01-01

    )-(3) are plotted in Figs. 6 and 7. It was found that the over-all shape of the excitation functions for Reactions (1)-(3) could be described rea­ sonably well (sQe Figs. 6 and 7) by a simple expreSSion of the general form {o if E"'Eo uR(E)= A(E_Eo)Be_C(E-EO... to IP: 129.237.46.100 On: Mon, 15 Sep 2014 13:25:50 Wyatt, Strattan, Chivalak, and Hierl: Reactions of Ar+ with CH4 , CD4 , and CH2 D2 4589 (0) 0.25 0 0 C\\l E u <:e I 0 cr b (b) C\\l E u <:e I Q cr b 0.15 0.0 o. FIG. 7. Integral...

  17. Decomposition and vibrational relaxation in CH{sub 3}I and self-reaction of CH{sub 3} radicals.

    SciTech Connect (OSTI)

    Yang, X.; Goldsmith, C. F.; Tranter, R. S.

    2009-07-01

    Vibrational relaxation and dissociation of CH{sub 3}I, 2-20% in krypton, have been investigated behind incident shock waves in a diaphragmless shock tube at 20, 66, 148, and 280 Torr and 630-2200 K by laser schlieren densitometry. The effective collision energy obtained from the vibrational relaxation experiments has a small, positive temperature dependence, {Delta}E{sub down} = 63 x (T/298){sup 0.56} cm{sup -1}. First-order rate coefficients for dissociation of CH{sub 3}I show a strong pressure dependence and are close to the low-pressure limit. Restricted-rotor Gorin model RRKM calculations fit the experimental results very well with {Delta}E{sub down} = 378 x (T/298){sup 0.457} cm{sup -1}. The secondary chemistry of this reaction system is dominated by reactions of methyl radicals and the reaction of the H atom with CH{sub 3}I. The results of the decomposition experiments are very well simulated with a model that incorporates methyl recombination and reactions of methylene. Second-order rate coefficients for ethane dissociation to two methyl radicals were derived from the experiments and yield k = (4.50 {+-} 0.50) x 10{sup 17} exp(-32709/T) cm{sup 3} mol{sup -1} s{sup -1}, in good agreement with previous measurements. Rate coefficients for H + CH{sub 3}I were also obtained and give k = (7.50 {+-} 1.0) x 10{sup 13} exp(-601/T) cm{sup 3} mol{sup -1} s{sup -1}, in reasonable agreement with a previous experimental value.

  18. Power-law and Logarithmic Entropy Corrected Holographic Dark Energy Models in Brans-Dicke Cosmology with Granda-Oliveros Cut-Off

    E-Print Network [OSTI]

    Antonio Pasqua; Surajit Chattopadhyay; Ratbay Myrzakulov

    2015-10-13

    In this paper, the cosmological implications of the Power Law Entropy Corrected Holographic Dark Energy (PLECHDE) and the Logarithmic Entropy Corrected Holographic Dark Energy (LECHDE) models in the context of Brans-Dicke (BD) cosmology for both non-interacting and interacting DE and Dark Matter (DM) are studied. As the system infrared cut-off, we choose the recently proposed Granda-Oliveros cut-off, which contains a term proportional to the first time derivative of the Hubble parameter and one term proportional to $H^2$, i.e. the Hubble parameter squared. We obtain the expressions of three quantities, i.e. the Equation of State (EoS) parameter $\\omega_D$, the deceleration parameter $q$ and the evolutionary form of the energy density parameter $\\Omega'_D$ of the PLECHDE and LECHDE models in a non-flat Universe for non-interacting and interacting DE and DM as well. Moreover, we investigate the limiting cases corresponding to: a) absence of entropy corrections; b) Einstein's gravity; and c) concomitantly absence of entropy corrections and Einstein's gravity. Furthermore, we consider the limiting case corresponding to the Ricci scale, which is recovered for some particular values of the parameters characterizing the Granda-Oliveros scale. We also study the statefinder diagnostic and the cosmographic parameters for both models considered in this work.

  19. Power-law and Logarithmic Entropy Corrected Holographic Dark Energy Models in Brans-Dicke Cosmology with Granda-Oliveros Cut-Off

    E-Print Network [OSTI]

    Pasqua, Antonio; Myrzakulov, Ratbay

    2015-01-01

    In this paper, the cosmological implications of the Power Law Entropy Corrected Holographic Dark Energy (PLECHDE) and the Logarithmic Entropy Corrected Holographic Dark Energy (LECHDE) models in the context of Brans-Dicke (BD) cosmology for both non-interacting and interacting DE and Dark Matter (DM) are studied. As the system infrared cut-off, we choose the recently proposed Granda-Oliveros cut-off, which contains a term proportional to the first time derivative of the Hubble parameter and one term proportional to $H^2$, i.e. the Hubble parameter squared. We obtain the expressions of three quantities, i.e. the Equation of State (EoS) parameter $\\omega_D$, the deceleration parameter $q$ and the evolutionary form of the energy density parameter $\\Omega'_D$ of the PLECHDE and LECHDE models in a non-flat Universe for non-interacting and interacting DE and DM as well. Moreover, we investigate the limiting cases corresponding to: a) absence of entropy corrections; b) Einstein's gravity; and c) concomitantly absenc...

  20. Application of Generalized Quantum Hydrodynamics In the Theory of Quantum Soliton's Evolution, Atom Structure and Lightning Ball

    E-Print Network [OSTI]

    Alexeev, Boris V

    2008-01-01

    Quantum solitons are discovered with the help of generalized quantum hydrodynamics (GQH). The solitons have the character of the stable quantum objects in the self consistent electric field. These effects can be considered as explanation of the existence of lightning balls. The delivered theory demonstrates the great possibilities of the generalized quantum hydrodynamics in investigation of the quantum solitons. The paper can be considered also as comments and prolongation of the materials published in the known author`s monograph (Boris V. Alexeev, Generalized Boltzmann Physical Kinetics. Elsevier. 2004). The theory leads to solitons as typical formations in the generalized quantum hydrodynamics. Key words: Foundations of the theory of transport processes; The theory of solitons; Generalized hydrodynamic equations; Foundations of quantum mechanics; The theory of lightning balls. PACS: 67.55.Fa, 67.55.Hc

  1. CITATION Professor Desmond Ball, School of International, Political and Strategic Studies, Strategic and Defence Studies Centre, ANU College of Asia and the Pacific

    E-Print Network [OSTI]

    CITATION ­ Professor Desmond Ball, School of International, Political and Strategic Studies contributions to understanding nuclear strategy, Australian defence, signals intelligence, regional security politics, and. most recently, conflict in Southeast Asia, have all been motivated by an unflinching

  2. Significantly improved dehydrogenation of ball-milled MgH2 doped with CoFe2O4 nanoparticles

    E-Print Network [OSTI]

    Volinsky, Alex A.

    Engineering, University of South Florida, Tampa, FL 33620, USA h i g h l i g h t s CoFe2O4 has strong 2014 Keywords: Cobalt ferrite Hydrogen storage Magnesium hydride Dehydrogenation temperature a b s t r a c t CoFe2O4 nanoparticles are added to magnesium hydride (MgH2) by high-energy ball milling in order

  3. Tune of Take Me Out To The Ball Game There is an end to the OIL game

    E-Print Network [OSTI]

    Nightingale, Peter

    Oil Game! Tune of Take Me Out To The Ball Game There is an end to the OIL game Soon we'll sit for the GREEN life The only way to SURVIVE Let's shout one, two, three, And break free, Of the OLD OIL GAME! Watch that hole in the OCEAN Spewing oil like the plague Killing the fish and the BIRDS and more

  4. Symmetry and degeneracy of the curved Coulomb potential on the S3 ball

    E-Print Network [OSTI]

    Rivera, Adrian Pallares; 10.1088/1751-8113/44/44/445302

    2012-01-01

    The "curved" Coulomb potential on the S3 ball, whose isometry group is SO(4), takes the form of a cotangent function, and when added to the four-dimensional squared angular momentum operator, one of the so(4) Casimir invariants, a Hamiltonian is obtained which describes a perturbance of the free geodesic motion that results peculiar in several aspects. The spectrum of such a motion has been studied on various occasions and is known to carry unexpectedly so(4) degeneracy patterns despite the non-commutativity of the perturbance with the Casimir operator. We here suggest an explanation for this behavior in designing a set of operators which close the so(4) algebra and whose Casimir invariant coincides with the Hamiltonian of the perturbed motion at the level of the eigenvalue problem. The above operators are related to the canonical geometric SO(4) generators on S3 by a non-unitary similarity transformation of the scaling type. In this fashion, we identify a complementary option to the deformed dynamical so(4) ...

  5. Symmetry and degeneracy of the curved Coulomb potential on the S3 ball

    E-Print Network [OSTI]

    Adrian Pallares Rivera; Mariana Kirchbach

    2012-02-09

    The "curved" Coulomb potential on the S3 ball, whose isometry group is SO(4), takes the form of a cotangent function, and when added to the four-dimensional squared angular momentum operator, one of the so(4) Casimir invariants, a Hamiltonian is obtained which describes a perturbance of the free geodesic motion that results peculiar in several aspects. The spectrum of such a motion has been studied on various occasions and is known to carry unexpectedly so(4) degeneracy patterns despite the non-commutativity of the perturbance with the Casimir operator. We here suggest an explanation for this behavior in designing a set of operators which close the so(4) algebra and whose Casimir invariant coincides with the Hamiltonian of the perturbed motion at the level of the eigenvalue problem. The above operators are related to the canonical geometric SO(4) generators on S3 by a non-unitary similarity transformation of the scaling type. In this fashion, we identify a complementary option to the deformed dynamical so(4) Higgs algebra constructed in terms of the components of the ordinary angular momentum and a related Runge-Lenz vector.

  6. n-Dimensional Gravity Little Black Holes, Dark Matter, and Ball Lightning

    E-Print Network [OSTI]

    Rabinowitz, M

    2001-01-01

    The gravitational field, and radiation from quantized gravitational atoms and little black holes (LBH) are analyzed in n-space, i.e. in all dimensions from 0 to o to develop insights into possible additional compacted dimensions as predicted by hierarchy and string theory. It is shown that the entropy of LBH is significantly greater in higher dimensional space with potential implications to the initial entropy of the universe. A case is made that LBH are the dark matter of the universe, and can manifest themselves as the core energy source of ball lightning (BL). The LBH incidence rate on earth is related to BL occurrence and has the potential of aiding in the determination of the distribution of LBH and hence dark matter in the universe. Examination of LBH interactions with the atmosphere are found to be in accord with observations of BL. Possibilities are explored as to why Hawking radiation has been undetected in over 25 years. An alternate LBH tunneling radiation model is described.

  7. n-Dimensional Gravity: Little Black Holes, Dark Matter, and Ball Lightning

    E-Print Network [OSTI]

    Mario Rabinowitz

    2003-03-30

    The gravitational field, and radiation from quantized gravitational atoms and little black holes (LBH) are analyzed in n-space, i.e. in all dimensions to develop insights into possible additional compacted dimensions as predicted by hierarchy and string theory. It is shown that the entropy of LBH is significantly greater in higher dimensional space with potential implications to the initial entropy of the universe. A case is made that LBH are the dark matter of the universe, and can manifest themselves as the core energy source of ball lightning (BL). The LBH incidence rate on earth is related to BL occurrence and has the potential of aiding in the determination of the distribution of LBH and hence dark matter in the universe. Examination of LBH interactions with the atmosphere are found to be in accord with observations of BL. Possibilities are explored as to why Hawking radiation has been undetected in over 25 years. An alternate LBH tunneling radiation model is described.

  8. Role of impact parameter in branching reactions: Chemical accelerator studies of the reaction Xe++CH4?XeCH3 ++H

    E-Print Network [OSTI]

    Miller, G. D.; Strattan, L. W.; Hierl, Peter M.

    1981-01-01

    Integral reaction cross sections and product velocity distributions have been measured for the ion–molecule reaction Xe+(CH4,H)XeCH3 + over the relative reactant translational energy range of 0.7–5.5 eV by chemical accelerator ...

  9. Approved Module Information for CH3102, 2014/5 Module Title/Name: Advances in Biomaterials Science Module Code: CH3102

    E-Print Network [OSTI]

    Neirotti, Juan Pablo

    Approved Module Information for CH3102, 2014/5 Module Title/Name: Advances in Biomaterials Science Module Code: CH3102 School: Engineering and Applied Science Module Type: Standard Module New Module? No Module Credits: 10 Module Management Information Module Leader Name Brian J Tighe Email Address tighebj

  10. Selectivity of chemisorbed oxygen in CH bond activation and CO oxidation and kinetic consequences for CH4O2 catalysis on Pt and Rh clusters

    E-Print Network [OSTI]

    Iglesia, Enrique

    Available online 12 August 2011 Keywords: CH4 Catalytic partial oxidation Methane combustion Platinum, thus confirming that direct catalytic partial oxidation of CH4 to CO (and H2) does not occur the sequential reforming steps. Ó 2011 Elsevier Inc. All rights reser

  11. On the Interaction of Methyl Azide (CH3N3) Ices with Ionizing Radiation: Formation of Methanimine (CH2NH), Hydrogen Cyanide (HCN), and Hydrogen Isocyanide (HNC)

    E-Print Network [OSTI]

    Kaiser, Ralf I.

    On the Interaction of Methyl Azide (CH3N3) Ices with Ionizing Radiation: Formation of Methanimine in solar system analogue ices. Introduction Methyl azide (CH3N3) is an organic compound suggested to be present in Titan's atmosphere.1 To date, the Voyager Infrared Radiometer and Infrared Spectrometer (IRIS

  12. A Single Transition State Serves Two Mechanisms. The Branching Ratio for CH2O-+ CH3Cl on Improved Potential Energy Surfaces

    E-Print Network [OSTI]

    Schlegel, H. Bernhard

    for this reaction has been studied by ab initio molecular dynamics (AIMD). The energies of transition states change of the potential energy surface around the transition state may vary the branching ratioA Single Transition State Serves Two Mechanisms. The Branching Ratio for CH2O·- + CH3Cl on Improved

  13. ChEAS Data: The Chequamegon Ecosystem Atmosphere Study

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

    Davis, Kenneth J. [Penn State

    The Chequamegon Ecosystem-Atmosphere Study (ChEAS) is a multi-organizational research effort studying biosphere/atmosphere interactions within a northern mixed forest in Northern Wisconsin. A primary goal is to understand the processes controlling forest-atmosphere exchange of carbon dioxide and the response of these processes to climate change. Another primary goal is to bridge the gap between canopy-scale flux measurements and the global CO2 flask sampling network. The ChEAS flux towers participate in AmeriFlux, and the region is an EOS-validation site. The WLEF tower is a NOAA-CMDL CO2 sampling site. ChEAS sites are primarily located within or near the Chequamegon-Nicolet National Forest in northern Wisconsin, with one site in the Ottawa National Forest in the upper peninsula of Michigan. Current studies observe forest/atmosphere exchange of carbon dioxide at canopy and regional scales, forest floor respiration, photosynthesis and transpiration at the leaf level and use models to scale to canopy and regional levels. EOS-validation studies quantitatively assess the land cover of the area using remote sensing and conduct extensive ground truthing of new remote sensing data (i.e. ASTER and MODIS). Atmospheric remote sensing work is aimed at understanding atmospheric boundary layer dynamics, the role of entrainment in regulating the carbon dioxide mixing ratio profiles through the lower troposphere, and feedback between boundary layer dynamics and vegetation (especially via the hydrologic cycle). Airborne studies have included include balloon, kite and aircraft observations of the CO2 profile in the troposphere.

  14. ChBE 3130 Chemical Engineering Thermodynamics II (required course) Note: This course was previously numbered 3110

    E-Print Network [OSTI]

    Sherrill, David

    ChBE 3130 Chemical Engineering Thermodynamics II (required course) Note: This course was previously numbered 3110 Credit: 3-0-3 Instructor: Carson Meredith Textbook: Introduction to Chemical Engineering Principles (ChBE 2100), Numerical Methods (ChBE 2120), and Chemical Engineering Thermodynamics I (ChBE 2130

  15. Methanogenic Conversion of CO2 Into CH4

    SciTech Connect (OSTI)

    Stevens, S.H., Ferry, J.G., Schoell, M.

    2012-05-06

    This SBIR project evaluated the potential to remediate geologic CO2 sequestration sites into useful methane gas fields by application of methanogenic bacteria. Such methanogens are present in a wide variety of natural environments, converting CO2 into CH4 under natural conditions. We conclude that the process is generally feasible to apply within many of the proposed CO2 storage reservoir settings. However, extensive further basic R&D still is needed to define the precise species, environments, nutrient growth accelerants, and economics of the methanogenic process. Consequently, the study team does not recommend Phase III commercial application of the technology at this early phase.

  16. Manganese Porphyrins Catalyze Selective C-H Bond Halogenations

    SciTech Connect (OSTI)

    Liu, Wei; Groves, John T

    2010-01-01

    We report a manganese porphyrin mediated aliphatic C?H bond chlorination using sodium hypochlorite as the chlorine source. In the presence of catalytic amounts of phase transfer catalyst and manganese porphyrin Mn(TPP)Cl 1, reaction of sodium hypochlorite with different unactivated alkanes afforded alkyl chlorides as the major products with only trace amounts of oxygenation products. Substrates with strong C?H bonds, such as neopentane (BDE =?100 kcal/mol) can be also chlorinated with moderate yield. Chlorination of a diagnostic substrate, norcarane, afforded rearranged products indicating a long-lived carbon radical intermediate. Moreover, regioselective chlorination was achieved by using a hindered catalyst, Mn(TMP)Cl, 2. Chlorination of trans-decalin with 2 provided 95% selectivity for methylene-chlorinated products as well as a preference for the C2 position. This novel chlorination system was also applied to complex substrates. With 5?-cholestane as the substrate, we observed chlorination only at the C2 and C3 positions in a net 55% yield, corresponding to the least sterically hindered methylene positions in the A-ring. Similarly, chlorination of sclareolide afforded the equatorial C2 chloride in a 42% isolated yield. Regarding the mechanism, reaction of sodium hypochlorite with the Mn{sup III} porphyrin is expected to afford a reactive Mn{sup V}?O complex that abstracts a hydrogen atom from the substrate, resulting in a free alkyl radical and a Mn{sup IV}—OH complex. We suggest that this carbon radical then reacts with a Mn{sup IV}—OCl species, providing the alkyl chloride and regenerating the reactive Mn{sup V}?O complex. The regioselectivity and the preference for CH{sub 2} groups can be attributed to nonbonded interactions between the alkyl groups on the substrates and the aryl groups of the manganese porphyrin. The results are indicative of a bent [Mn{sup v}?O---H---C] geometry due to the C—H approach to the Mn{sup v}?O (d??p?)* frontier orbital.

  17. CH2 Contorhaus Hansestadt Hamburg | Open Energy Information

    Open Energy Info (EERE)

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Home Page on Google Bookmark EERE: Alternative Fuels Data Center Home Page on QA:QA J-E-1 SECTION JEnvironmentalBowerbank, Maine:Kansas: Energy Resources Jump to:EnergyCEEGObnovitelne zdroje sroCH2

  18. Test Plan: WIPP bin-scale CH TRU waste tests

    SciTech Connect (OSTI)

    Molecke, M.A.

    1990-08-01

    This WIPP Bin-Scale CH TRU Waste Test program described herein will provide relevant composition and kinetic rate data on gas generation and consumption resulting from TRU waste degradation, as impacted by synergistic interactions due to multiple degradation modes, waste form preparation, long-term repository environmental effects, engineered barrier materials, and, possibly, engineered modifications to be developed. Similar data on waste-brine leachate compositions and potentially hazardous volatile organic compounds released by the wastes will also be provided. The quantitative data output from these tests and associated technical expertise are required by the WIPP Performance Assessment (PA) program studies, and for the scientific benefit of the overall WIPP project. This Test Plan describes the necessary scientific and technical aspects, justifications, and rational for successfully initiating and conducting the WIPP Bin-Scale CH TRU Waste Test program. This Test Plan is the controlling scientific design definition and overall requirements document for this WIPP in situ test, as defined by Sandia National Laboratories (SNL), scientific advisor to the US Department of Energy, WIPP Project Office (DOE/WPO). 55 refs., 16 figs., 19 tabs.

  19. Voluntary Protection Program Onsite Review, CH2M WG LLC, Idaho Cleanup Project – March 2014

    Broader source: Energy.gov [DOE]

    Evaluation to determine whether CH2M WG LLC, Idaho Cleanup Project is performing at a level deserving DOE-VPP Star recognition.

  20. Preliminary Notice of Violation, CH2M-Washington Group Idaho...

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

    14, 2007 Issued to CH2M-Washington Group Idaho, LLC, related to Radiation Protection Program Deficiencies at the Radioactive Waste Management Complex - Accelerated Retrieval...

  1. Bimetallic cleavage of aromatic C-H bonds by rare-earth-metal complexes

    E-Print Network [OSTI]

    Huang, W; Huang, W; Dulong, F; Khan, SI; Cantat, T; Diaconescu, PL

    2014-01-01

    of Aromatic C-H Bonds by Rare Earth Metal Complexes Wenliangone week prior to use. Rare earth metal oxides (scandium,

  2. Stoichiometry of CH4 and CO2 flux in a California Rice Paddy

    E-Print Network [OSTI]

    McMillan, Andrew M. S.; Goulden, Michael L.; Tyler, Stanley C.

    2007-01-01

    Measurements of carbon sequestration by long-term eddyemission versus carbon sequestration, Tellus, Ser. B,which to estimate carbon sequestration from F CH4 data since

  3. DOE Selects CH2M Hill Plateau Remediation Company for Plateau...

    Energy Savers [EERE]

    by CH2M Hill Constructors, Inc. The team also includes AREVA Federal Services, LLC; East Tennessee Materials & Energy Corporation, Inc.; and Fluor Federal Services, Inc. as...

  4. Recrossing and tunnelling in the kinetics study of the OH + CH4 -> H2O + CH3 reaction

    E-Print Network [OSTI]

    Suleimanov, Yury V

    2015-01-01

    Thermal rate constants and several kinetic isotope effects were evaluated for the OH + CH4 hydrogen abstraction reaction using two kinetics approaches, ring polymer molecular dynamics (RPMD), and variational transition state theory with multidimensional tunnelling(VTST/MT), based on a refined full-dimensional analytical potential energy surface, PES-2014, in the temperature range 200-2000 K. For the OH + CH4 reaction, at low temperatures, T = 200 K, where the quantum tunnelling effect is more important, RPMD overestimates the experimental rate constants due to problems associated with PES-2014 in the deep tunnelling regime and to the known overestimation of this method in asymmetric reactions, while VTST/MT presents a better agreement, differences about 10%, due to compensation of several factors, inaccuracy of PES-2014 and ignoring anharmonicity. In the opposite extreme, T = 1000 K, recrossing effects play the main role, and the difference between both methods is now smaller, by a factor of 1.5. Given that R...

  5. On the amorphization behavior and hydrogenation performance of high-energy ball-milled Mg{sub 2}Ni alloys

    SciTech Connect (OSTI)

    Kou, Hongchao; Hou, Xiaojiang; Zhang, Tiebang, E-mail: tiebangzhang@nwpu.edu.cn; Hu, Rui; Li, Jinshan; Xue, Xiangyi

    2013-06-15

    Amorphous Mg{sub 2}Ni alloy was prepared by high energy ball-milling starting with polycrystalline Mg{sub 2}Ni which was prepared with the help of a metallurgy method by using a SPEX 8000D mill. The microstructural and phase structure characterization of the prepared materials was performed via scanning electron microscopy, transition electron microscope and X-ray diffraction. The thermal stabilities were investigated by differential scanning calorimetry. The apparent activation energies were determined by means of the Kissinger method. The first and second crystallization reactions take place at ? 255 °C and ? 410 °C, and the corresponding activation energy of crystallization is E{sub a1} = 276.9 and E{sub a2} = 382.4 kJ/mol, respectively. At 3 MPa hydrogen pressure and 250 °C, the hydrogen absorption capacities of crystalline, partially and fully amorphous Mg{sub 2}Ni alloy are 2.0 wt.%, 3.2 wt.% and 3.5 wt.% within 30 min, respectively. - Graphical Abstract: We mainly focus on the amorphization behavior of crystalline Mg{sub 2}Ni alloy in the high energy ball-milling process and the crystallization behavior of the amorphous Mg{sub 2}Ni alloy in a follow-up heating process. The relationship of milling, microstructure and hydrogenation properties is established and explained by models. - Highlights: • Amorphous Mg{sub 2}Ni has been obtained by high energy ball milling the as-cast alloy. • The amorphization behavior of polycrystalline Mg{sub 2}Ni is presented. • The crystallization behavior of the amorphous Mg{sub 2}Ni alloy is illustrated. • Establish the relationship of milling, microstructure and hydrogenation properties.

  6. Thermal desorption of CH4 retained in CO2 ice

    E-Print Network [OSTI]

    Luna, R; Domingo, M; Satorre, M A

    2008-01-01

    CO2 ices are known to exist in different astrophysical environments. In spite of this, its physical properties (structure, density, refractive index) have not been as widely studied as those of water ice. It would be of great value to study the adsorption properties of this ice in conditions related to astrophysical environments. In this paper, we explore the possibility that CO2 traps relevant molecules in astrophysical environments at temperatures higher than expected from their characteristic sublimation point. To fulfil this aim we have carried out desorption experiments under High Vacuum conditions based on a Quartz Crystal Microbalance and additionally monitored with a Quadrupole Mass Spectrometer. From our results, the presence of CH4 in the solid phase above the sublimation temperature in some astrophysical scenarios could be explained by the presence of several retaining mechanisms related to the structure of CO2 ice.

  7. Thermal desorption of CH4 retained in CO2 ice

    E-Print Network [OSTI]

    R. Luna; C. Millan; M. Domingo; M. A. Satorre

    2008-01-21

    CO2 ices are known to exist in different astrophysical environments. In spite of this, its physical properties (structure, density, refractive index) have not been as widely studied as those of water ice. It would be of great value to study the adsorption properties of this ice in conditions related to astrophysical environments. In this paper, we explore the possibility that CO2 traps relevant molecules in astrophysical environments at temperatures higher than expected from their characteristic sublimation point. To fulfil this aim we have carried out desorption experiments under High Vacuum conditions based on a Quartz Crystal Microbalance and additionally monitored with a Quadrupole Mass Spectrometer. From our results, the presence of CH4 in the solid phase above the sublimation temperature in some astrophysical scenarios could be explained by the presence of several retaining mechanisms related to the structure of CO2 ice.

  8. TransCom model simulations of CH? and related species: linking transport, surface flux and chemical loss with CH? variability in the troposphere and lower stratosphere

    E-Print Network [OSTI]

    Patra, P. K.

    A chemistry-transport model (CTM) intercomparison experiment (TransCom-CH?) has been designed to investigate the roles of surface emissions, transport and chemical loss in simulating the global methane distribution. Model ...

  9. Evidence for Methane -Complexes in Reductive Elimination Reactions from TpRh(L)(CH3)H

    E-Print Network [OSTI]

    Jones, William D.

    Evidence for Methane -Complexes in Reductive Elimination Reactions from TpRh(L)(CH3)H Douglas D of methane from TpRh(L)(CH3)H in benzene/perfluorobenzene solvent mixtures is found to be dependent upon the concentration of benzene, indicating an associative component to the reductive elimination of methane. Both

  10. Fates of methane from different lake habitats: Connecting whole-lake budgets and CH4 emissions

    E-Print Network [OSTI]

    Pace, Michael L.

    Fates of methane from different lake habitats: Connecting whole-lake budgets and CH4 emissions September 2007; revised 3 February 2008; accepted 28 February 2008; published 24 May 2008. [1] Methane (CH4 clear. We quantified internal cycling and methane emissions in three lakes during summer stratification

  11. SimpleMonitorUSBXPress User Guide Tobi Delbruck, tobi@ini.phys.ethz.ch

    E-Print Network [OSTI]

    Delbruck, Tobi

    SimpleMonitorUSBXPress User Guide Tobi Delbruck, tobi@ini.phys.ethz.ch Allows monitoring AER over at the University of Sevilla and the second by Tobi Delbruck at INI in Zurich. The firmware and host code is written. Last modified 8/20/2005 Under subversion https://svn.ini.unizh.ch/repos/avlsi/CAVIAR/wp5/USBAER

  12. ChBE 2120 Numerical Methods in Chemical Engineering (required course) Credit: 3-0-3

    E-Print Network [OSTI]

    Sherrill, David

    ChBE 2120 Numerical Methods in Chemical Engineering (required course) Credit: 3-0-3 Prerequisite(s): Chemical Process Principles (ChBE 2100), minimum grade of "C" and Computing for Engineers (CS 1371 of chemical engineering problems. An introduction to chemical process simulation, and the appropriate software

  13. 1997-2001 by M. Kostic Ch.5: Uncertainty/Error Analysis

    E-Print Network [OSTI]

    Kostic, Milivoje M.

    1 ©1997-2001 by M. Kostic Ch.5: Uncertainty/Error Analysis · Introduction · Bias and Precision Summation/Propagation (Expanded Combined Uncertainty) · Problem 5-30 ©1997-2001 by M. Kostic Ch.5) at corresponding Probability (%P) Remember: u = d%P = t,%PS (@ %P); z=t=d/S #12;2 ©1997-2001 by M. Kostic Bias

  14. DISCOVERY OF THE FIRST METHANOL (CH [subscript 3] OH) MASER IN THE ANDROMEDA GALAXY (M31)

    E-Print Network [OSTI]

    Sjouwerman, Loránt O.

    We present the first detection of a 6.7 GHz Class II methanol (CH[subscript 3]OH) maser in the Andromeda galaxy (M31). The CH[subscript 3]OH maser was found in a VLA survey during the fall of 2009. We have confirmed the ...

  15. A CH O Hydrogen Bond Stabilized Polypeptide Chain Reversal Motif at the C Terminus of Helices

    E-Print Network [OSTI]

    Babu, M. Madan

    A C­H· · ·O Hydrogen Bond Stabilized Polypeptide Chain Reversal Motif at the C Terminus of Helices of Science Bangalore 560012, India The serendipitous observation of a C­H· · ·O hydrogen bond mediated­N hydrogen bond involving the side- chain of residue T 2 4 and the N­H group of residue T þ 3. In as many

  16. Ground state of CH2 : Experimental aspects and theoretical implications M. Grieser,2

    E-Print Network [OSTI]

    Zajfman, Daniel

    by the Coulomb explosion imaging method at different stages of cooling. The bending angle distributions were. The purpose of this paper is to disclose data on the structure of CH2 , which demonstrates the inad- equacy are the bending angle distributions of ensembles of CH2 ions at different excitation levels. The bending angle

  17. Temperature and peat type control CO2 and CH4 production in Alaskan permafrost peats

    E-Print Network [OSTI]

    Temperature and peat type control CO2 and CH4 production in Alaskan permafrost peats C . C . T R E poorly under- stood despite the potential for a significant positive feedback to climate change. Our dioxide (CO2) and methane (CH4) emissions from peat samples collected at active layer and permafrost

  18. TOUR HYDROS.CH -Duba Hong-Kong-Singapore-Monaco-Brazil USA Records & conferences

    E-Print Network [OSTI]

    Psarrakos, Panayiotis

    ;· · · · 10 #12;· · · 11 #12;12 #12;13 #12;14 #12;15 #12;16 #12;VOILES DE SAINT- TROPEZ TOUR HYDROS.CH - Dubaï19-23 July 2016 Energy Efficiency Global Forum Washington May, 12-13 TOUR HYDROS.CH ­ Records

  19. Photolysis of CH{sub 3}CHO at 248 nm: Evidence of triple fragmentation from primary quantum yield of CH{sub 3} and HCO radicals and H atoms

    SciTech Connect (OSTI)

    Morajkar, Pranay; Schoemaecker, Coralie; Fittschen, Christa; Bossolasco, Adriana

    2014-06-07

    Radical quantum yields have been measured following the 248 nm photolysis of acetaldehyde, CH{sub 3}CHO. HCO radical and H atom yields have been quantified by time resolved continuous wave Cavity Ring Down Spectroscopy in the near infrared following their conversion to HO{sub 2} radicals by reaction with O{sub 2}. The CH{sub 3} radical yield has been determined using the same technique following their conversion into CH{sub 3}O{sub 2}. Absolute yields have been deduced for HCO radicals and H atoms through fitting of time resolved HO{sub 2} profiles, obtained under various O{sub 2} concentrations, to a complex model, while the CH{sub 3} yield has been determined relative to the CH{sub 3} yield from 248 nm photolysis of CH{sub 3}I. Time resolved HO{sub 2} profiles under very low O{sub 2} concentrations suggest that another unknown HO{sub 2} forming reaction path exists in this reaction system besides the conversion of HCO radicals and H atoms by reaction with O{sub 2}. HO{sub 2} profiles can be well reproduced under a large range of experimental conditions with the following quantum yields: CH{sub 3}CHO?+?h?{sub 248nm} ? CH{sub 3}CHO{sup *}, CH{sub 3}CHO{sup *} ? CH{sub 3}?+?HCO??{sub 1a} = 0.125?±?0.03, CH{sub 3}CHO{sup *} ? CH{sub 3}?+?H?+?CO??{sub 1e} = 0.205?±?0.04, CH{sub 3}CHO{sup *}?{sup o{sub 2}}CH{sub 3}CO?+?HO{sub 2}??{sub 1f} = 0.07?±?0.01. The CH{sub 3}O{sub 2} quantum yield has been determined in separate experiments as ?{sub CH{sub 3}} = 0.33 ± 0.03 and is in excellent agreement with the CH{sub 3} yields derived from the HO{sub 2} measurements considering that the triple fragmentation (R1e) is an important reaction path in the 248 nm photolysis of CH{sub 3}CHO. From arithmetic considerations taking into account the HO{sub 2} and CH{sub 3} measurements we deduce a remaining quantum yield for the molecular pathway: CH{sub 3}CHO{sup *} ? CH{sub 4}?+?CO??{sub 1b} = 0.6. All experiments can be consistently explained with absence of the formerly considered pathway: CH{sub 3}CHO{sup *} ? CH{sub 3}CO?+?H??{sub 1c} = 0.

  20. THE ROTATIONAL SPECTRUM OF ANTI-ETHYLAMINE (CH3CH2NH2) FROM 10 TO 270 GHz: A LABORATORY STUDY AND ASTRONOMICAL SEARCH IN SGR B2(N)

    E-Print Network [OSTI]

    Ziurys, Lucy M.

    AND ASTRONOMICAL SEARCH IN SGR B2(N) A. J. Apponi, M. Sun, D. T. Halfen,1 and L. M. Ziurys Departments of Chemistry identification of methylamine (CH3NH2) and ethylamine (CH3CH2NH2) in the aerogel collectors (Sandford et al. 2006

  1. Independent Oversight Review, Richland Operations Office and CH2M Hill Plateau Remediation Company and Mission Support Alliance- April 2012

    Office of Energy Efficiency and Renewable Energy (EERE)

    Review of Richland Operations Office and CH2M Hill Plateau Remediation Company and Mission Support Alliance Conduct of Operations

  2. ChBE 4505/4525 Chemical Process Design/Biochemical Process Design Basic Curriculum and Learning Outcomes.

    E-Print Network [OSTI]

    Sherrill, David

    Outcomes. Credit: 3-0-3 Instructor: Matthew J. Realff Textbook: Product & Process Design Principles, Third Edition, Wiley 2009. W.D. Seider, J.D. Seader, D.R. Lewin, S. Widagdo, Catalog Description: Principles Phen. II (ChBE 3210), Kinetics & Reactor Design (ChBE 4300), and separation processes (ChBE 3225

  3. Ion imaging study of reaction dynamics in the N+ + CH4 system Linsen Pei and James M. Farrar

    E-Print Network [OSTI]

    Farrar, James M.

    map ion imaging method is applied to the ion-molecule reactions of N+ with CH4. The velocity spaceIon imaging study of reaction dynamics in the N+ + CH4 system Linsen Pei and James M. Farrar OF CHEMICAL PHYSICS 137, 154312 (2012) Ion imaging study of reaction dynamics in the N+ + CH4 system Linsen

  4. New C-H Stretching Vibrational Spectral Features in the Raman Spectra of Gaseous and Liquid Ethanol

    E-Print Network [OSTI]

    Liu, Shilin

    New C-H Stretching Vibrational Spectral Features in the Raman Spectra of Gaseous and Liquid Ethanol Traditionally, the Raman spectrum of ethanol in the C-H vibrational stretching region between 2800 cm-1 and 3100, and the -CH3 antisymmetric stretching. In this report, new Raman spectral features were observed for ethanol

  5. Part I 7-Minute Questions 1. A tennis ball of mass m is held just above a basketball of mass M ! m and

    E-Print Network [OSTI]

    Yavuz, Deniz

    does the tennis ball rebound? 2. A copper wire has length L, mass M, cross sectional area A, and Young, but the center point is fixed in space. a. Find the quantum mechanically allowed energy levels of this rigid rotor. b. What are the degeneracies of the energy levels? 6. A beam of particles of mass µ and momentum

  6. Dielectric and photocatalytic properties of sulfur doped TiO{sub 2} nanoparticles prepared by ball milling

    SciTech Connect (OSTI)

    Jalalah, Mohammed [Promising Centre for Sensors and Electronic Devices (PCSED), Advanced Materials and Nano-Research Centre, Najran University, P.O. Box 1988, Najran, 11001 (Saudi Arabia); Electrical Engineering Department, College of Engineering, Najran University, P.O. Box 1988, Najran, 11001 (Saudi Arabia); Faisal, M. [Promising Centre for Sensors and Electronic Devices (PCSED), Advanced Materials and Nano-Research Centre, Najran University, P.O. Box 1988, Najran, 11001 (Saudi Arabia); Bouzid, Houcine [Promising Centre for Sensors and Electronic Devices (PCSED), Advanced Materials and Nano-Research Centre, Najran University, P.O. Box 1988, Najran, 11001 (Saudi Arabia); Department of Physics, Faculty of Sciences and Arts, Najran University, P.O. Box 1988, Najran, 11001 (Saudi Arabia); Ismail, Adel A., E-mail: adelali141@yahoo.com [Promising Centre for Sensors and Electronic Devices (PCSED), Advanced Materials and Nano-Research Centre, Najran University, P.O. Box 1988, Najran, 11001 (Saudi Arabia); Nanostructured and Nanotechnology Materials Division, Central Metallurgical R and D Institute, CMRDI, P.O. Box 87, Helwan, 11421, Cairo (Egypt); Chemistry Department, Science and Art at Sharurah, Najran University (Saudi Arabia); Al-Sayari, Saleh A. [Promising Centre for Sensors and Electronic Devices (PCSED), Advanced Materials and Nano-Research Centre, Najran University, P.O. Box 1988, Najran, 11001 (Saudi Arabia); Chemistry Department, Science and Art at Sharurah, Najran University (Saudi Arabia)

    2013-09-01

    Graphical abstract: - Highlights: • Designing of visible light responsive photocatalyst utilizing ball milling. • Sulphur used as dopant in commercial TiO{sub 2} P25 at different atomic percentage. • S doping resulted in an intense increase in absorption in the visible light region. • Newly design photocatalyst exhibited excellent photocatalytic performance. • 0.11 at.% S-doped TiO{sub 2} shows 3-times higher activity than that of TiO{sub 2} P25. - Abstract: Sulfur (S) doped commercial TiO{sub 2} P-25 has been achieved by changing the amount of thiourea using ball milling technique. The results of XRD clearly reveal biphasial anatase and rutile mixtures for all prepared samples and doping of S does not change the morphology of the TiO{sub 2}. The optical absorption edge of S-doped TiO{sub 2} was red shifted with indirect bandgap energy of 2.8 eV. The dielectric studies confirm that the dielectric constant of TiO{sub 2} increases after doping, however it becomes more conductive. Newly designed S-doped TiO{sub 2} photocatalysts exhibited excellent photocatalytic performance for the degradation of methylene blue (MB) under visible light. The overall photocatalytic activity of 0.11 at.% S-doped TiO{sub 2} was significantly 3-times higher than that of commercial TiO{sub 2} P-25 and complete degradation of MB has taken place after 90 min of irradiation under visible light while only 35% dye degraded when the reaction has been carried out in the presence of undoped TiO{sub 2}.

  7. Rice Bran for Fattening Hogs. 

    E-Print Network [OSTI]

    McConnell, O. E.; Williams, D. W. (David Willard)

    1922-01-01

    . . . . . . . . . . . leaf fat, 46.5" C., hack fat, 41.9" C. No. 2, grazed on peanuts. . . . . . . . . . .leaf fat, 44.8" C., back fat, 43.8" C. No. 3, no peanuts. . . . . . . . . . . . . . . . . leaf fat, 44.9 " C., back fat, 41.7" C. No. 4, no peanuts...

  8. Intern experience at CH?M Hill, Inc.: an internship report 

    E-Print Network [OSTI]

    Winter, William John, 1949-

    2013-03-13

    (standards) imposed upon the mill by the State of Washington Department of Ecology and the U.S. Environmental Protection Agency. The author's assignment also entailed necessary interaction with the project manager and other CH?M HILL design...

  9. Joint DOE-CH2M HILL News Release Media Contact: For Immediate...

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

    price. Since receiving the contract in 2008, CH2M HILL awarded more than 1 billion in contracts to small businesses, representing 28 percent of the contract price to date....

  10. Tetra-substituted olefin synthesis using palladium-catalysed C-H activation 

    E-Print Network [OSTI]

    Lopez Suarez, Laura; Suarez, Laura Lopez

    2012-06-22

    In an effort to obtain more efficient and greener chemical transformations, a substantial amount of research interest has been directed towards the use of arene C-H bonds as functional groups. Hydroarylation of alkynes ...

  11. Fundamental Understanding of Methane-Carbon Dioxide-Water (CH4...

    Office of Scientific and Technical Information (OSTI)

    Fundamental Understanding of Methane-Carbon Dioxide-Water (CH4-CO2-H2O) Interactions in Shale Nanopores under Reservoir Conditions. Citation Details In-Document Search Title:...

  12. Fundamental Understanding of Methane-Carbon Dioxide-Water (CH4...

    Office of Scientific and Technical Information (OSTI)

    Technical Report: Fundamental Understanding of Methane-Carbon Dioxide-Water (CH4-CO2-H2O) Interactions in Shale Nanopores under Reservoir Conditions. Citation Details In-Document...

  13. Park, Y.J.; Hofmayer, C.H. [Brookhaven National Lab., Upton,...

    Office of Scientific and Technical Information (OSTI)

    Understanding seismic design criteria for Japanese nuclear power plants Park, Y.J.; Hofmayer, C.H. Brookhaven National Lab., Upton, NY (United States); Costello, J.F. US Nuclear...

  14. Credal Networks for Military Identification aIDSIA, Galleria 2, CH-6928 Manno (Lugano), Switzerland

    E-Print Network [OSTI]

    Zaffalon, Marco

    ), Switzerland bArmasuisse (W+T), Feuerwerkerstrasse 39, CH-3600 Thun, Switzerland Alessandro Antonucci a , Ralph targets surveyed by the Armed Forces has become usual prac- tice, also in neutral states like Switzerland

  15. EG39CH12-Jackson ARI 27 September 2014 12:18 The Environmental Costs

    E-Print Network [OSTI]

    Jackson, Robert B.

    EG39CH12-Jackson ARI 27 September 2014 12:18 The Environmental Costs and Benefits of Fracking by horizontal drilling and hydraulic fracturing (fracking) is driving an economic boom, with con- sequences

  16. NOx-Mediated Homogeneous Pathways for the Synthesis of Formaldehyde from CH4-O2 Mixtures

    E-Print Network [OSTI]

    Iglesia, Enrique

    NOx-Mediated Homogeneous Pathways for the Synthesis of Formaldehyde from CH4-O2 Mixtures Jeffrey M-NOx reactions is used to estimate maximum attainable formaldehyde (and methanol) yields

  17. Variable carbon isotope fractionation expressed by aerobic CH4-oxidizing bacteria

    E-Print Network [OSTI]

    Chu, Kung-Hui "Bella"

    in biomass carbon isotopes is primarily due to differences in the fraction- ation effect at the formaldehyde in the production and consumption of CH4 oc- cur (e.g., Bergamaschi, 1997; Conrad et al., 1999; Avery and Martens

  18. Hydrogen Storage in Carbon Nanotubes Through Formation of C-H...

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

    Hydrogen Storage in Carbon Nanotubes Through Formation of C-H Bonds Print Two of the major challenges for humanity in the next 20 years are the shrinking availability of fossil...

  19. Interpretation of observed atmospheric variations of CO2 and CH4. 

    E-Print Network [OSTI]

    Barlow, James Mathew

    2015-06-30

    The overarching theme of my thesis is understanding observed variations of northern hemisphere atmospheric carbon dioxide (CO2) and methane (CH4) concentrations. I focus my analysis on high-latitude observations of these gases, as there are large...

  20. 28 BIts&ChIps 17 november 2005 Energetiq Technology heeft een licht-

    E-Print Network [OSTI]

    Cambridge, University of

    28 · BIts&ChIps · 17 november 2005 Energetiq Technology heeft een licht- bron gelanceerd voor extreem ultravi- olet (EUV) metrologie. Deze Electrode- less Z-Pinch EUV-source, of EQ-10M, genereert EUV

  1. Proton transfer and unimolecular decay in the reaction HCO/sup +/ + CH/sub 3/OH. -->. CH/sub 3/OH/sub 2//sup +/ + CO

    SciTech Connect (OSTI)

    Moryl, J.E.; Farrar, J.M.

    1982-05-27

    We report a study of the title reaction over the relative energy range from 0.45 to 3.59 eV. The proton-transfer reaction proceeds in a direct, impulsive manner at all energies with 33 to 70% of the available energy appearing in product translation. Dissociation of the protonated methanol product via CH/sub 3//sup +/ formation or elimination of H/sub 2/ to CH/sub 2/OH/sup +/ becomes important at higher collision energies. Measurement of the threshold for CH/sub 3//sup +/ production demonstrates that > 90% of the HCO/sup +/ reagents are in the ground vibrational state. Abnormally small product translational energy release for H/sub 2/ elimination provides evidence that quantum mechanical tunneling through the exit channel barrier determines the dynamics of this process. Isotopic labeling studies, in which the parent ion CH/sub 3/ODH/sup +/ may eliminate H/sub 2/ or HD, show that k/sub H/sub 2///k/sub HD/ = 3.0, confirming the role of tunneling in the elimination step.

  2. MeteoSvizzera, 6605 Locarno, Switzerland email: Katja.Friedrich@meteoswiss.ch http://www.meteoswiss.ch P11B8: Effects of Radar Beam Shielding on Rainfall

    E-Print Network [OSTI]

    ://www.meteoswiss.ch P11B8: Effects of Radar Beam Shielding on Rainfall Estimation for Polarimetric C-band Radar Katja In the case of radar beam shielding, a weaker transmitted signal reaches precipitation at further ranges 1998 with: Complete shielding in Partial shielding in No shielding to the South 1 2 3 2 4 Height

  3. Ion imaging study of reaction dynamics in the N{sup +}+ CH{sub 4} system

    SciTech Connect (OSTI)

    Pei, Linsen; Farrar, James M. [Department of Chemistry, University of Rochester, Rochester, New York 14627 (United States)

    2012-10-21

    The velocity map ion imaging method is applied to the ion-molecule reactions of N{sup +} with CH{sub 4}. The velocity space images are collected at collision energies of 0.5 and 1.8 eV, providing both product kinetic energy and angular distributions for the reaction products CH{sub 4}{sup +}, CH{sub 3}{sup +}, and HCNH{sup +}. The charge transfer process is energy resonant and occurs by long-range electron transfer that results in minimal deflection of the products. The formation of the most abundant product, CH{sub 3}{sup +}, proceeds by dissociative charge transfer rather than hydride transfer, as reported in earlier publications. The formation of HCNH{sup +} by C-N bond formation appears to proceed by two different routes. The triplet state intermediates CH{sub 3}NH{sup +} and CH{sub 2}NH{sub 2}{sup +} that are formed as N{sup +}({sup 3}P) approaches CH{sub 4} may undergo sequential loss of two hydrogen atoms to form ground state HCNH{sup +} products on a spin-allowed pathway. However, the kinetic energy distributions for formation of HCNH{sup +} extend past the thermochemical limit to form HCNH{sup +}+ 2H, implying that HCNH{sup +} may also be formed in concert with molecular hydrogen, and requiring that intersystem crossing to the singlet manifold must occur in a significant ({approx}25%) fraction of reactive collisions. We also report GAUSSIAN G2 calculations of the energies and structures of important singlet and triplet [CNH{sub 4}{sup +}] complexes that serve as precursors to product formation.

  4. Photodissociation and photoisomerization dynamics of CH{sub 2}=CHCHO in solution

    SciTech Connect (OSTI)

    Wu Weiqiang; Yang Chunfan; Zhao Hongmei; Liu Kunhui; Su Hongmei

    2010-03-28

    By means of time-resolved Fourier transform infrared absorption spectroscopy, we have investigated the 193 nm photodissociation and photoisomerization dynamics of the prototype molecule of {alpha},{beta}-enones, acrolein (CH{sub 2}=CHCHO) in CH{sub 3}CN solution. The primary photolysis channels and absolute branching ratios are determined. The most probable reaction mechanisms are clarified by control experiments monitoring the product yields varied with the triplet quencher addition. The predominant channel is the 1,3-H migration yielding the rearrangement product CH{sub 3}CH=C=O with a branching ratio of 0.78 and the less important channel is the {alpha} cleavage of C-H bond yielding radical fragments CH{sub 2}=CHCO+H with a branching ratio of only 0.12. The 1,3-H migration is strongly suggested to correlate with the triplet {sup 3}({pi}{pi}{sup *}) state rather than the ground S{sub 0} state and the {alpha} cleavage of C-H bond is more likely to proceed in the singlet S{sub 1} {sup 1}(n{pi}{sup *}) state. From the solution experiments we have not only acquired clues clarifying the previous controversial mechanisms, but also explored different photochemistry in solution. Compared to the gas phase photolysis which is dominated by photodissociation channels, the most important channel in solution is the photoisomerization of 1,3-H migration. The reason leading to the different photochemistry in solution is further ascribed to the solvent cage effect.

  5. Dances and Balls: Cotton Ball - 3 

    E-Print Network [OSTI]

    Eagle photo by Gene Dennis

    2006-01-01

    Since a comprehensive upgrade of the US National Lightning Detection Network (NLDN) in 1994, the mean peak current of detected cloud-to-ground (CG) lightning flashes has decreased, the number of detected flashes has increased, and the percentage...

  6. Dances and Balls: Fancy Dress Ball - 1 

    E-Print Network [OSTI]

    Unknown

    2006-01-01

    Two mesoscale convective systems (MCSs) passed over the Houston Lightning Detection and Ranging (LDAR) network on 31 October 2005 and 21 April 2006. As the MCSs traverse the LDAR network, the systems slowly mature with a weakening convective line...

  7. Insights into the structure of mixed CO2/CH4 in gas hydrates

    SciTech Connect (OSTI)

    Everett, Susan M; Rawn, Claudia J; Chakoumakos, Bryan C; Keffer, David J.; Huq, Ashfia; Phelps, Tommy Joe

    2015-01-01

    The exchange of CO2 for CH4 in natural gas hydrates is an attractive approach to methane for energy production while simultaneously sequestering CO2. In addition to the energy and environmental implications, the solid solution of clathrate hydrate (CH4)1-x(CO2)x 5.75H2O provides a model system to study how the distinct bonding and shapes of CH4 and CO2 influence the structure and properties of the compound. High-resolution neutron diffraction was used to examine mixed CO2/CH4 gas hydrates. CO2-rich hydrates had smaller lattice parameters, which were attributed to the higher affinity of the CO2 molecule interacting with H2O molecules that form the surrounding cages, and resulted in a reduction in the unit cell volume. Experimental nuclear scattering densities illustrate how the cage occupants and energy landscape change with composition. These results provide important insights on the impact and mechanisms for exchanging CH4 and CO2.

  8. Ion imaging study of dissociative charge transfer in the N{sub 2}{sup +}+ CH{sub 4} system

    SciTech Connect (OSTI)

    Pei Linsen; Farrar, James M. [Department of Chemistry, University of Rochester, Rochester, New York 14627 (United States)

    2013-03-28

    The velocity map ion imaging method is applied to the dissociative charge transfer reactions of N{sub 2}{sup +} with CH{sub 4} studied in crossed beams. The velocity space images are collected at four collision energies between 0.5 and 1.5 eV, providing both product kinetic energy and angular distributions for the reaction products CH{sub 3}{sup +} and CH{sub 2}{sup +}. The general shapes of the images are consistent with long range electron transfer from CH{sub 4} to N{sub 2}{sup +} preceding dissociation, and product kinetic energy distributions are consistent with energy resonance in the initial electron transfer step. The branching ratio for CH{sub 3}{sup +}:CH{sub 2}{sup +} is 85:15 over the full collision energy range, consistent with literature reports.

  9. Interlayer magnetoresistance peak in -,,BEDTTTF...2SF5CH2CF2SO3 X. Su and F. Zuoa)

    E-Print Network [OSTI]

    Zuo, Fulin

    Interlayer magnetoresistance peak in -,,BEDT­TTF...2SF5CH2CF2SO3 X. Su and F. Zuoa) Department crystals of organic superconductor -(BEDT­TTF 2SF5CH2CF2SO3 . The magnetoresistance is found to display measurement on a highly two-dimensional organic superconductor -(BEDT­TTF 2 SF5CH2CF2SO3 . Similar to other ET

  10. Housing Guide 2015 A GUIDE '15I SPY a hanger, a golf ball, a comb; nine bears, and a place for a home.

    E-Print Network [OSTI]

    Hart, Gus

    Housing Guide 2015 A HOUSING GUIDE '15I SPY a hanger, a golf ball, a comb; nine bears, and a place CONCeRT SeRIeS · DOwNTOwN PROVO ReSTAuRANTS · PROVO FARMeRS MARkeT IN The SuMMeR #12;Housing Guide 2015 3 HOUSING GUIDE 8 Why BYU contracted housing 12 HOUSING MAP 16 O -Campus Housing advice 24 O -Campus

  11. J. Chem. Thermodynamics 1996, 28, 521538 Volumetric properties for {(1-x)CO2+xCH4},

    E-Print Network [OSTI]

    Bodnar, Robert J.

    J. Chem. Thermodynamics 1996, 28, 521­538 Volumetric properties for {(1-x)CO2+xCH4}, {(1-x)CO2+xN2, U.S.A. Densities r of pure CO2, CH4, and {(1-x)CO2+xCH4}, {(1-x)CO2+xN2}, and {(1-x)CH4+xN2} were from mole fraction x=0 to x=1. The results were obtained with a custom-designed, high-pressure, high-temperature

  12. Observation of CH4 and other Non-CO2 Green House Gas Emissions from California

    SciTech Connect (OSTI)

    Fischer, Marc L.; Zhao, Chuanfeng; Riley, William J.; Andrews, Arlyn C.

    2009-01-09

    In 2006, California passed the landmark assembly bill AB-32 to reduce California's emissions of greenhouse gases (GHGs) that contribute to global climate change. AB-32 commits California to reduce total GHG emissions to 1990 levels by 2020, a reduction of 25 percent from current levels. To verify that GHG emission reductions are actually taking place, it will be necessary to measure emissions. We describe atmospheric inverse model estimates of GHG emissions obtained from the California Greenhouse Gas Emissions Measurement (CALGEM) project. In collaboration with NOAA, we are measuring the dominant long-lived GHGs at two tall-towers in central California. Here, we present estimates of CH{sub 4} emissions obtained by statistical comparison of measured and predicted atmospheric mixing ratios. The predicted mixing ratios are calculated using spatially resolved a priori CH{sub 4} emissions and surface footprints, that provide a proportional relationship between the surface emissions and the mixing ratio signal at tower locations. The footprints are computed using the Weather Research and Forecast (WRF) coupled to the Stochastic Time-Inverted Lagrangian Transport (STILT) model. Integral to the inverse estimates, we perform a quantitative analysis of errors in atmospheric transport and other factors to provide quantitative uncertainties in estimated emissions. Regressions of modeled and measured mixing ratios suggest that total CH{sub 4} emissions are within 25% of the inventory estimates. A Bayesian source sector analysis obtains posterior scaling factors for CH{sub 4} emissions, indicating that emissions from several of the sources (e.g., landfills, natural gas use, petroleum production, crops, and wetlands) are roughly consistent with inventory estimates, but livestock emissions are significantly higher than the inventory. A Bayesian 'region' analysis is used to identify spatial variations in CH{sub 4} emissions from 13 sub-regions within California. Although, only regions near the tower are significantly constrained by the tower measurements, CH{sub 4} emissions from the south Central Valley appear to be underestimated in a manner consistent with the under-prediction of livestock emissions. Finally, we describe a pseudo-experiment using predicted CH{sub 4} signals to explore the uncertainty reductions that might be obtained if additional measurements were made by a future network of tall-tower stations spread over California. These results show that it should be possible to provide high-accuracy estimates of surface CH{sub 4} emissions for multiple regions as a means to verify future emissions reductions.

  13. Cyclic Versus Linear Isomers Produced by Reaction of the Methylidyne Radical (CH) with Small Unsaturated Hydrocarbons

    SciTech Connect (OSTI)

    Goulay, Fabien; Trevitt, Adam J.; Meloni, Giovanni; Selby, Talitha M.; Osborn, David L.; Taatjes, Craig A.; Vereecken, Luc; Leone, Stephen R.

    2008-12-05

    The reactions of the methylidyne radical (CH) with ethylene, acetylene, allene, and methylacetylene are studied at room temperature using tunable vacuum ultraviolet (VUV) photoionization and time-resolved mass spectrometry. The CH radicals are prepared by 248 nm multiphoton photolysis of CHBr3 at 298 K and react with the selected hydrocarbon in a helium gas flow. Analysis of photoionization efficiency versus VUV photon wavelength permits isomer-specific detection of the reaction products and allows estimation of the reaction product branching ratios. The reactions proceed by either CH insertion or addition followed by H atom elimination from the intermediate adduct. In the CH + C2H4 reaction the C3H5 intermediate decays by H atom loss to yield 70(+-8)percent allene, 30(+-8)percent methylacetylene and less than 10percent cyclopropene, in agreement with previous RRKM results. In the CH + acetylene reaction, detection of mainly the cyclic C3H2 isomer is contrary to a previous RRKM calculation that predicted linear triplet propargylene to be 90percent of the total H-atom co-products. High-level CBS-APNO quantum calculations and RRKM calculation for the CH + C2H2 reaction presented in this manuscript predict a higher contribution of the cyclic C3H2 (27.0percent) versus triplet propargylene (63.5percent) than these earlier predictions. Extensive calculations on the C3H3 and C3H2D system combined with experimental isotope ratios for the CD + C2H2 reaction indicate that H-atom assisted isomerization in the present experiments is responsible for the discrepancy between the RRKM calculations and the experimental results. Cyclic isomers are also found to represent 30(+-6)percent of the detected products in the case of CH + methylacetylene, together with 33(+-6)percent 1,2,3-butatriene and 37(+-6)percent vinylacetylene. The CH + allene reaction gives 23(+-5)percent 1,2,3-butatriene and 77(+-5)percent vinylacetylene, whereas cyclic isomers are produced below the detection limit in this reaction. The reaction exit channels deduced by comparing the product distributions for the aforementioned reactions are discussed in detail.

  14. Constraints on Asian and European sources of methane from CH4 -C2H6-CO correlations in Asian outflow

    E-Print Network [OSTI]

    Jacob, Daniel J.

    of emissions from coal mining and landfills. 2 #12;1. Introduction Atmospheric methane (CH4) is an important, landfills, fossil fuel production and consumption (natural gas venting, leakage and coal mining a global CH4 source inventory constrained with NOAA/CMDL surface observations [Wang et al., 2003]. We find

  15. 2590 J. Am. Chem. SOC.1995,117, 2590-2599 The C-H Bond Energy of Benzene

    E-Print Network [OSTI]

    Ellison, Barney

    2590 J. Am. Chem. SOC.1995,117, 2590-2599 The C-H Bond Energy of Benzene Gustavo E. Davico ion with benzene and phenide ion with ammonia: c&6 +NH2- C6H5- +NH3. The ratio of these rate constants for derived. The enthalpy of deprotonationof benzene, the C-H bond dissociationenergy, and the electron

  16. Synthesis, Structure, and Reactivity of O-Donor Ir(III) Complexes: C-H Activation Studies with Benzene

    E-Print Network [OSTI]

    Goddard III, William A.

    with Benzene Gaurav Bhalla, Xiang Yang Liu, Jonas Oxgaard, William A. Goddard, III, and Roy A. Periana. All the R-Ir-Py complexes undergo quantitative, intermolecular CH activation reactions with benzene to benzene to generate a discrete benzene complex, cis-R-Ir-PhH; and (D) rapid C-H cleavage. Kinetic isotope

  17. Computational identification of a metal organic framework for high selectivity membrane-based CO2/CH4 separations

    E-Print Network [OSTI]

    Nair, Sankar

    CH4/CO2 mixtures with low cost are required. Membranes offer a powerful general approachComputational identification of a metal organic framework for high selectivity membrane-based CO2 for CO2/CH4 mixtures could revolutionize this industrially important separation. We predict using

  18. Electronic Effects of Rh(II)-Mediated Carbenoid Intramolecular C-H Insertion: A Linear Free Energy Correlation Study

    E-Print Network [OSTI]

    Wang, Jianbo

    Electronic Effects of Rh(II)-Mediated Carbenoid Intramolecular C-H Insertion: A Linear Free Energy. The mechanistic significance of these Hammett correlations is discussed. Introduction The electronic effects of Rh is enhanced by an electron-donating group while an electron-withdrawing group retards the C-H insertion, thus

  19. Energetics of C-H Bond Activation of Fluorinated Aromatic Hydrocarbons Using a [TpRh(CNneopentyl)] Complex

    E-Print Network [OSTI]

    Jones, William D.

    Energetics of C-H Bond Activation of Fluorinated Aromatic Hydrocarbons Using a [Tp activation of fluorinated aromatic hydrocarbons by [TpRh(CNneopentyl)] resulted in the formation of products of homogeneous transition-metal catalysts to activate and functionalize C-H bonds of hydrocarbons for industrial

  20. Ultrafast UV Pump/IR Probe Studies of C-H Activation in Linear, Cyclic, and Aryl Hydrocarbons

    E-Print Network [OSTI]

    Harris, Charles B.

    Ultrafast UV Pump/IR Probe Studies of C-H Activation in Linear, Cyclic, and Aryl Hydrocarbons, cyclic, and aromatic hydrocarbon solvents on a femtosecond to microsecond time scale. These results have revealed that the structure of the hydrocarbon substrate affects the final C-H bond activation step, which

  1. FL47CH15-Goldstein ARI 25 November 2014 9:45 Green Algae as Model

    E-Print Network [OSTI]

    Goldstein, Raymond E.

    FL47CH15-Goldstein ARI 25 November 2014 9:45 Green Algae as Model Organisms for Biological Fluid green algae, spanning from the unicellular Chlamydomonas to multicellular Volvox, have emerged as model of flagellar synchronization. Green algae are well suited to the study of such problems because of their range

  2. Dynamic isotope effect on the product energy partitioning in CH2OH ~CHO H2

    E-Print Network [OSTI]

    Kim, Myung Soo

    Dynamic isotope effect on the product energy partitioning in CH2OH ~CHO H2 Young Min Rheea March 1998; accepted 1 July 1998 The deuterium isotope effect on the product energy partitioning. Close inspection of the potential energy surface revealed that the isotope effect on KER and the product

  3. BENDIX SYSTEMS DIVISION ANN AIt 1 o I, MI CH NO. Plan for Operational Contingency

    E-Print Network [OSTI]

    Rathbun, Julie A.

    8/29/66 BENDIX SYSTEMS DIVISION ANN AIt 1 o I, MI CH NO. ATM-396 Plan for Operational Contingency of the operational plans and the system design and to study methods of recovery from partial failure through the use. ATM- 396 RIV.MO. A I I f..r I (I IOperational Contingency Study 2 PAGI OP

  4. PREPARED FORTHE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DEAC0276CH03073

    E-Print Network [OSTI]

    PREPARED FORTHE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE­AC02­76CH03073 PRINCETON PLASMA Acceleration the Field­reversed Configuration (FRC) Slowly Rotating Odd­parity Magnetic Fields (RMF ) Alan Plasma Physics Laboratory Publications Reports web site Calendar Year 2001. The home PPPL Reports

  5. PREPARED FORTHE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DEAC0276CH03073

    E-Print Network [OSTI]

    of Reversed Configuration (FRC). a compact toroid negligible toroidal in which plasma confined a poloidal. Introduction The FRC a compact toroid with negligible toroidal in which plasma confined a poloidal magneticPREPARED FORTHE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE­AC02­76CH03073 PRINCETON PLASMA

  6. Do Water Molecules Mediate Protein-DNA Recognition? Ch. Koti Reddy, Achintya Das and B. Jayaram*

    E-Print Network [OSTI]

    Jayaram, Bhyravabotla

    Do Water Molecules Mediate Protein-DNA Recognition? Ch. Koti Reddy, Achintya Das and B. Jayaram analysis of interfacial water molecules in the structures of 109 unique protein-DNA complexes is presented together with a new view on their role in protein-DNA recognition. Location of interfacial water molecules

  7. PREPARED FORTHE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DEAC0276CH03073

    E-Print Network [OSTI]

    PREPARED FORTHE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE­AC02­76CH03073 PRINCETON PLASMA.K. Ram, Bers, R.W. Harvey, C.B. Forest May 2001 #12; PPPL Reports Disclaimer report prepared account work Department Energy's Princeton Plasma Physics Laboratory Publications Reports web site Calendar Year 2001

  8. Twofold C?H Functionalization: Palladium-Catalyzed Ortho Arylation of Anilides

    E-Print Network [OSTI]

    Brasche, Gordon

    The ortho arylation of anilides to form biphenyls via a twofold C?H functionalization/C?C bond-forming process is described. The oxidative coupling takes place in the presence of 5?10 mol % of Pd(OAc)[subscript 2], 10?20 ...

  9. Steady and unsteady flow within an axisymmetric tube dilatation Ch. Stamatopoulos a

    E-Print Network [OSTI]

    Papaharilaou, Yannis

    Accepted 20 February 2010 Keywords: Tube dilatation Wall shear Vortex Flow separation­reattachment a bSteady and unsteady flow within an axisymmetric tube dilatation Ch. Stamatopoulos a , Y s t r a c t The flow field in an axisymmetric tube dilatation is studied employing a 2D PIV system

  10. Soil chemistry versus environmental controls on production of CH4 and CO2 in northern peatlands

    E-Print Network [OSTI]

    Williams, Christopher J.

    . B. YAVITT a , C. J. WILLIAMS b & R. K. WIEDER c a Department of Natural Resources, Cornell Rates of organic carbon mineralization (to CO2 and CH4) vary widely in peat soil. We transplanted four peat soils with different chemical composition into six sites with different environmental conditions

  11. TraCE -TRANSPORTATION CENTER EPFL 09 Sep 2009 sonia.lavadinho@epfl.ch STRC Ascona

    E-Print Network [OSTI]

    Bierlaire, Michel

    & capillary walking (TUBE & WALK LONDON) #12;TraCE - TRANSPORTATION CENTER EPFL 09 Sep 2009 soniaTraCE - TRANSPORTATION CENTER EPFL 09 Sep 2009 sonia.lavadinho@epfl.ch STRC Ascona 11 Potentials for combining walking and public transport at the agglomeration scale THE MULTIMODAL WALKER #12;Tra

  12. PREPARED FORTHE U.S. DEPARTMENT ENERGY, UNDER CONTRACT DEAC0276CH03073

    E-Print Network [OSTI]

    ions [1,2] beneficial they "channel" energy from the ion population thermal population (rather thanPREPARED FORTHE U.S. DEPARTMENT ENERGY, UNDER CONTRACT DE­AC02­76CH03073 PRINCETON PLASMA PHYSICS herein specific commercial product, process, or service trade name, trademark, manufacturer, otherwise

  13. CH 5 MANAGEMENT PLAN.DOC 5-1 5 Management Plan

    E-Print Network [OSTI]

    CH 5 MANAGEMENT PLAN.DOC 5-1 5 Management Plan 5.1 Vision The Willamette Subbasin Plan Oversight. The ecosystem processes that have undergone the most disruptive change are flow, channel form, and connectivity. Disruptions in these processes, in turn, have created a host of negative habitat changes, including

  14. BE12CH08-Zare ARI 22 April 2010 20:22 Microfluidic Platforms

    E-Print Network [OSTI]

    Zare, Richard N.

    BE12CH08-Zare ARI 22 April 2010 20:22 R E V I E W S IN A D V A N CE Microfluidic Platforms, genetic analysis Abstract Microfluidics, the study and control of the fluidic behavior in microstruc to analyze various types of intracellular components quantitatively. The microfluidic approach offers a rapid

  15. ChBE 4300 Kinetics and Reactor Design (required course) Credit: 3-0-3

    E-Print Network [OSTI]

    Sherrill, David

    , and (ii) reactor design for the homogeneous reaction systems. The design principles for ideal homogeneousChBE 4300 Kinetics and Reactor Design (required course) Credit: 3-0-3 Prerequisite in terms of reaction mechanisms, kinetics, and reactor design. Both homogeneous and heterogeneous reactions

  16. ChBE 4310 Bioprocess Engineering (required course) Credit: 3-0-3

    E-Print Network [OSTI]

    Sherrill, David

    Description: Integrating several ChBE core concepts, bioprocess engineering applies the engineering principles) or Biochemistry II (Chem 4511) minimum grade "D", and Kinetics and Reactor Design, minimum grade "C" Objectives: Specifically, after completing the course, students should be able to: 1.) Apply engineering principles

  17. Binary properties of CH and Carbon-Enhanced Metal-Poor stars

    E-Print Network [OSTI]

    Jorissen, A; Van Winckel, H; Merle, T; Boffin, H M J; Andersen, J; Nordstroem, B; Udry, S; Masseron, T; Lenaerts, L; Waelkens, C

    2015-01-01

    The HERMES spectrograph installed on the 1.2-m Mercator telescope has been used to monitor the radial velocity of 13 low-metallicity carbon stars, among which 7 Carbon-Enhanced Metal-Poor (CEMP) stars and 6 CH stars. All stars but one show clear evidence for binarity. New orbits are obtained for 8 systems. The sample covers an extended range in orbital periods, extending from 3.4 d (for the dwarf carbon star HE 0024-2523) to about 54 yr (for the CH star HD 26, the longest known among barium, CH and extrinsic S stars). Three systems exhibit low-amplitude velocity variations with periods close to 1 yr superimposed on a long-term trend. In the absence of an accurate photometric monitoring of these systems, it is not clear yet whether these variations are the signature of a very low-mass companion, or of regular envelope pulsations. The period - eccentricity (P - e) diagram for the 40 low-metallicity carbon stars with orbits now available shows no difference between CH and CEMP-s stars (the latter corresponding t...

  18. A Practical Agent Programming Language Mehdi Dastani and John-Jules Ch. Meyer

    E-Print Network [OSTI]

    Dastani, Mehdi

    A Practical Agent Programming Language Mehdi Dastani and John-Jules Ch. Meyer Utrecht University-based agent- oriented programming language. It proposes an alternative by presenting the syn- tax and semantics of a programming language, called 2APL (A Practical Agent Programming Language). This programming

  19. Physics of thin-film ferroelectric oxides DPMC, University of Geneva, CH-1211, Geneva 4, Switzerland

    E-Print Network [OSTI]

    Wu, Zhigang

    Physics of thin-film ferroelectric oxides M. Dawber* DPMC, University of Geneva, CH-1211, Geneva 4 of thin-film ferroelectric oxides, the strongest emphasis being on those aspects particular to ferroelectrics in thin-film form. The authors introduce the current state of development in the application

  20. Liu UCD Phy9B 07 1 Ch 19. The First Law of Thermodynamics

    E-Print Network [OSTI]

    Yoo, S. J. Ben

    Liu UCD Phy9B 07 1 Ch 19. The First Law of Thermodynamics #12;Liu UCD Phy9B 07 2 19-1. Thermodynamic Systems Thermodynamic system: A system that can interact (and exchange energy) with its surroundings Thermodynamic process: A process in which there are changes in the state of a thermodynamic system

  1. X-ray Thomson scattering measurements of temperature and density from multi-shocked CH capsules

    SciTech Connect (OSTI)

    Fletcher, L. B. [Department of Physics, University of California, Berkeley, California 94720 (United States)] [Department of Physics, University of California, Berkeley, California 94720 (United States); Kritcher, A.; Pak, A.; Ma, T.; Döppner, T.; Divol, L.; Landen, O. L.; Glenzer, S. H. [Lawrence Livermore National Laboratory, 7000 East Av., Livermore, California 94550 (United States)] [Lawrence Livermore National Laboratory, 7000 East Av., Livermore, California 94550 (United States); Fortmann, C. [Lawrence Livermore National Laboratory, 7000 East Av., Livermore, California 94550 (United States) [Lawrence Livermore National Laboratory, 7000 East Av., Livermore, California 94550 (United States); University of California, Los Angeles, California 90095 (United States); Vorberger, J.; Gericke, D. O. [Department of Physics, Centre for Fusion, Space, and Astrophysics, University of Warwick, Coventry CV4 7AL (United Kingdom)] [Department of Physics, Centre for Fusion, Space, and Astrophysics, University of Warwick, Coventry CV4 7AL (United Kingdom); Chapman, D. A. [Department of Physics, Centre for Fusion, Space, and Astrophysics, University of Warwick, Coventry CV4 7AL (United Kingdom) [Department of Physics, Centre for Fusion, Space, and Astrophysics, University of Warwick, Coventry CV4 7AL (United Kingdom); Plasma Physics Department, AWE plc, Aldermaston (United Kingdom); Falcone, R. W. [Department of Physics, University of California, Berkeley, California 94720 (United States) [Department of Physics, University of California, Berkeley, California 94720 (United States); Lawrence Berkeley National Laboratory, Berkeley, California 94720 (United States)

    2013-05-15

    Proof-of-principle measurements of the electron densities, temperatures, and ionization states of spherically compressed multi-shocked CH (polystyrene) capsules have been achieved using spectrally resolved x-ray Thomson scattering. A total energy of 13.5 kJ incident on target is used to compress a 70 ?m thick CH shell above solid-mass density using three coalescing shocks. Separately, a laser-produced zinc He-? x-ray source at 9 keV delayed 200 ps-800 ps after maximum compression is used to probe the plasma in the non-collective scattering regime. The data show that x-ray Thomson scattering enables a complete description of the time-dependent hydrodynamic evolution of shock-compressed CH capsules, with a maximum measured density of ? > 6 g cm{sup ?3}. In addition, the results demonstrate that accurate measurements of x-ray scattering from bound-free transitions in the CH plasma demonstrate strong evidence that continuum lowering is the primary ionization mechanism of carbon L-shell electrons.

  2. FL43CH19-Shelley ARI 10 September 2010 19:30 Flapping and Bending Bodies

    E-Print Network [OSTI]

    Shelley, Michael

    FL43CH19-Shelley ARI 10 September 2010 19:30 R E V I E W S IN A D V A N CE Flapping and Bending, flutter, flexible bodies, instability, drag reduction Abstract The flapping or bending of a flexible is important to applications such as paper processing (Watanabe et al. 2002), as well as to possible approaches

  3. Mechanistic Analysis of Iridium Heteroatom C-H Activation: Evidence for an Internal Electrophilic Substitution Mechanism

    E-Print Network [OSTI]

    Goddard III, William A.

    Substitution Mechanism Jonas Oxgaard,*, William J. Tenn, III, Robert J. Nielsen, Roy A. Periana, and William A: The mechanism responsible for C-H actiVation in Ir(acac)2(OCH3)(C6H6) has been identified and described as an internal electrophilic substitution (IES) mechanism, on the basis of orbital changes and predicted reacti

  4. Large-Scale Quality Analysis of Published ChIP-seq Data

    E-Print Network [OSTI]

    Kundaje, Anshul

    ChIP-seq has become the primary method for identifying in vivo protein–DNA interactions on a genome-wide scale, with nearly 800 publications involving the technique appearing in PubMed as of December 2012. Individually and ...

  5. Ch 1: Suspect Subjectivity March 16, 2012 SUBJECTIVITY: EXPOSURE, CARE, AND RESPONSE

    E-Print Network [OSTI]

    Doyle, Robert

    Ch 1: Suspect Subjectivity March 16, 2012 1 ONE SUBJECTIVITY: EXPOSURE, CARE, AND RESPONSE For many't. There is the notorious "truth is subjectivity" and the oft-cited "passionate leap of faith." Setting aside the tangles around `leaps of faith,' what is Kierkegaard promoting under the heading of subjectivity? My aim here

  6. 16. Wave-particle interaction Reading: Shu, Vol.II, Ch.29

    E-Print Network [OSTI]

    Pohl, Martin Karl Wilhelm

    16. Wave-particle interaction Reading: Shu, Vol.II, Ch.29 16.1 Landau damping We started our discussion of hydromagnetic waves with simple one-dimensional electrostatic fluctuations, the Langmuir waves, whose dispersion relation is = p = e2 ne 0 me Can the waves change plasma properties or, vice versa

  7. Active Seismic BENDIX SYSTEMS DIVISION ANN A R8 0 R, M I CH NO.

    E-Print Network [OSTI]

    Rathbun, Julie A.

    Active Seismic ,'1~ y · ~net'¥· BENDIX SYSTEMS DIVISION ANN A R8 0 R, M I CH NO. ATM-463 REV in the word format of the Active Seismic Experiment. It also serves to document Action Item B6-0805-5B, which and compares three different word formats for the Active Seismic Experiment. These are designated Present DE

  8. Catalytic C-H Activation and Functionalization: Some Applications in Organic Synthesis

    E-Print Network [OSTI]

    Stoltz, Brian M.

    Non-hydro renewables Hydro power Natural Gas Transportation is Costly - CH4 major constituent,000 3,000 4,000 5,000 6,000 1970 1980 1990 2000 2010 2020 2030 Mtoe Oil Natural gas Coal Nuclear power to the cost of methane production. - Pipelines are roughly $1M/km to build. · Ind

  9. A Study of Transition of the Expansion of the Universe from a Phase of Deceleration to Acceleration through a Conversion of Matter into Dark Energy in the Framework of Brans-Dicke Theory

    E-Print Network [OSTI]

    Roy, Sudipto

    2015-01-01

    The present study is based on a generalized form of Brans-Dicke (BD) theory where, the dimensionless BD parameter is regarded as a function of the scalar field, which is reciprocal of the gravitational constant. The field equations have been solved by incorporating an empirical function f(t) in the expression representing the conservation of matter. This function f(t) has been chosen to account for a conversion of matter (both dark and baryonic) into some other form, possibly dark energy, which is known to be responsible for the accelerated expansion of universe. The requirement of a signature flip of the deceleration parameter (q), which is evident from other studies, sets the boundary conditions to be satisfied by the function f(t), leading to the formulation of its time dependence. A simple empirical relation was initially assumed to represent the time dependence of f(t), and the constants in this expression have been determined from these boundary conditions. The BD parameter has been found to have a nega...

  10. A Study of Transition of the Expansion of the Universe from a Phase of Deceleration to Acceleration through a Conversion of Matter into Dark Energy in the Framework of Brans-Dicke Theory

    E-Print Network [OSTI]

    Sudipto Roy

    2015-11-06

    The present study is based on a generalized form of Brans-Dicke (BD) theory where, the dimensionless BD parameter is regarded as a function of the scalar field, which is reciprocal of the gravitational constant. The field equations have been solved by incorporating an empirical function f(t) in the expression representing the conservation of matter. This function f(t) has been chosen to account for a conversion of matter (both dark and baryonic) into some other form, possibly dark energy, which is known to be responsible for the accelerated expansion of universe. The requirement of a signature flip of the deceleration parameter (q), which is evident from other studies, sets the boundary conditions to be satisfied by the function f(t), leading to the formulation of its time dependence. A simple empirical relation was initially assumed to represent the time dependence of f(t), and the constants in this expression have been determined from these boundary conditions. The BD parameter has been found to have a negative value throughout the range of study. The dependence of BD parameter upon the scalar field has been depicted graphically. A smooth transition of the universe, from a decelerated to an accelerated phase of expansion, is found to occur due to a conversion of matter into dark energy. The gravitational constant is found to be increasing with time.

  11. Turbulence and combustion interaction: High resolution local flame front structure visualization using simultaneous single-shot PLIF imaging of CH, OH, and CH{sub 2}O in a piloted premixed jet flame

    SciTech Connect (OSTI)

    Li, Z.S.; Li, B.; Sun, Z.W.; Alden, M. [Division of Combustion Physics, Lund University, P.O. Box 118, S-221 00 Lund (Sweden); Bai, X.S. [Division of Fluid Mechanics, Lund University, P.O. Box 118, S-221 00 Lund (Sweden)

    2010-06-15

    High resolution planar laser-induced fluorescence (PLIF) was applied to investigate the local flame front structures of turbulent premixed methane/air jet flames in order to reveal details about turbulence and flame interaction. The targeted turbulent flames were generated on a specially designed coaxial jet burner, in which low speed stoichiometric gas mixture was fed through the outer large tube to provide a laminar pilot flame for stabilization of the high speed jet flame issued through the small inner tube. By varying the inner tube flow speed and keeping the mixture composition as that of the outer tube, different flames were obtained covering both the laminar and turbulent flame regimes with different turbulent intensities. Simultaneous CH/CH{sub 2}O, and also OH PLIF images were recorded to characterize the influence of turbulence eddies on the reaction zone structure, with a spatial resolution of about 40 {mu}m and temporal resolution of around 10 ns. Under all experimental conditions, the CH radicals were found to exist only in a thin layer; the CH{sub 2}O were found in the inner flame whereas the OH radicals were seen in the outer flame with the thin CH layer separating the OH and CH{sub 2}O layers. The outer OH layer is thick and it corresponds to the oxidation zone and post-flame zone; the CH{sub 2}O layer is thin in laminar flows; it becomes broad at high speed turbulent flow conditions. This phenomenon was analyzed using chemical kinetic calculations and eddy/flame interaction theory. It appears that under high turbulence intensity conditions, the small eddies in the preheat zone can transport species such as CH{sub 2}O from the reaction zones to the preheat zone. The CH{sub 2}O species are not consumed in the preheat zone due to the absence of H, O, and OH radicals by which CH{sub 2}O is to be oxidized. The CH radicals cannot exist in the preheat zone due to the rapid reactions of this species with O{sub 2} and CO{sub 2} in the inner-layer of the reaction zones. The local PLIF intensities were evaluated using an area integrated PLIF signal. Substantial increase of the CH{sub 2}O signal and decrease of CH signal was observed as the jet velocity increases. These observations raise new challenges to the current flamelet type models. (author)

  12. Rare-earth transition-metal gallium chalcogenides RE{sub 3}MGaCh{sub 7} (M=Fe, Co, Ni; Ch=S, Se)

    SciTech Connect (OSTI)

    Rudyk, Brent W.; Stoyko, Stanislav S.; Oliynyk, Anton O.; Mar, Arthur, E-mail: arthur.mar@ualberta.ca

    2014-02-15

    Six series of quaternary rare-earth transition-metal chalcogenides RE{sub 3}MGaCh{sub 7} (M=Fe, Co, Ni; Ch=S, Se), comprising 33 compounds in total, have been prepared by reactions of the elements at 1050 °C (for the sulphides) or 900 °C (for the selenides). They adopt noncentrosymmetric hexagonal structures (ordered Ce{sub 3}Al{sub 1.67}S{sub 7}-type, space group P6{sub 3}, Z=2) with cell parameters in the ranges of a=9.5–10.2 Å and c=6.0–6.1 Å for the sulphides and a=10.0–10.5 Å and c=6.3–6.4 Å for the selenides as refined from powder X-ray diffraction data. Single-crystal structures were determined for five members of the sulphide series RE{sub 3}FeGaS{sub 7} (RE=La, Pr, Tb) and RE{sub 3}CoGaS{sub 7} (RE=La, Tb). The highly anisotropic crystal structures consist of one-dimensional chains of M-centred face-sharing octahedra and stacks of Ga-centred tetrahedra all pointing in the same direction. Magnetic measurements on the sulphides reveal paramagnetic behaviour in some cases and long-range antiferromagnetic behaviour with low Néel temperatures (15 K or lower) in others. Ga L-edge XANES spectra support the presence of highly cationic Ga tetrahedral centres with a tendency towards more covalent Ga–Ch character on proceeding from the sulphides to the selenides. Band structure calculations on La{sub 3}FeGaS{sub 7} indicate that the electronic structure is dominated by Fe 3d-based states near the Fermi level. - Graphical abstract: The series of chalcogenides RE{sub 3}MGaS{sub 7}, which form for a wide range of rare-earth and transition metals (M=Fe, Co, Ni), adopt highly anisotropic structures containing chains of M-centred octahedra and stacks of Ga-centred tetrahedra. Display Omitted - Highlights: • Six series (comprising 33 compounds) of chalcogenides RE{sub 3}MGaCh{sub 7} were prepared. • They adopt noncentrosymmetric hexagonal structures with high anisotropy. • Most compounds are paramagnetic; some show antiferromagnetic ordering. • Ga L-edge XANES confirms presence of cationic Ga species.

  13. Influence of ball milling on atomic structure and magnetic properties of Co{sub 40}Fe{sub 22}Ta{sub 8}B{sub 30} glassy alloy

    SciTech Connect (OSTI)

    Taghvaei, Amir Hossein, E-mail: Amirtaghvaei@gmail.com [Department of Materials Science and Engineering, School of Engineering, Shiraz University, Shiraz (Iran, Islamic Republic of); Department of Materials Science and Engineering, Shiraz University of Technology, Shiraz (Iran, Islamic Republic of); Stoica, Mihai [IFW Dresden, Institute for Complex Materials, Helmholtzstr. 20, 01069 Dresden (Germany); Politehnica University of Timisoara, P-ta Victoriei 2, Timisoara (Romania); Bednar?ik, Jozef [HASYLAB at DESY, Notkestrasse 85, 22603 Hamburg (Germany); Kaban, Ivan [IFW Dresden, Institute for Complex Materials, Helmholtzstr. 20, 01069 Dresden (Germany); TU Dresden, Institut für Werkstoffwissenschaft, 01062 Dresden (Germany); Shahabi, Hamed Shakur; Khoshkhoo, Mohsen Samadi [IFW Dresden, Institute for Complex Materials, Helmholtzstr. 20, 01069 Dresden (Germany); Janghorban, Kamal [Department of Materials Science and Engineering, School of Engineering, Shiraz University, Shiraz (Iran, Islamic Republic of); Eckert, Jürgen [IFW Dresden, Institute for Complex Materials, Helmholtzstr. 20, 01069 Dresden (Germany); TU Dresden, Institut für Werkstoffwissenschaft, 01062 Dresden (Germany)

    2014-06-01

    The influence of ball milling on the atomic structure and magnetic properties of the Co{sub 40}Fe{sub 22}Ta{sub 8}B{sub 30} metallic glass with a high thermal stability and excellent soft magnetic properties has been investigated. After 14 h of milling, the obtained powders were found to consist mainly of an amorphous phase and a small fraction of the (Co,Fe){sub 21}Ta{sub 2}B{sub 6} nanocrystals. The changes in the reduced pair correlation functions suggest noticeable changes in the atomic structure of the amorphous upon ball milling. Furthermore, it has been shown that milling is accompanied by introduction of compressive and dilatational sites in the glassy phase and increasing the fluctuation of the atomic-level hydrostatic stress without affecting the coordination number of the nearest neighbors. Ball milling has decreased the thermal stability and significantly affected the magnetic properties through increasing the saturation magnetization, Curie temperature of the amorphous phase and coercivity. - Highlights: • Ball milling affected the atomic structure of Co{sub 40}Fe{sub 22}Ta{sub 8}B{sub 30} metallic glass. • Mechanically-induced crystallization started after 4 h milling. • Milling increased the fluctuation of the atomic-level hydrostatic stress in glass. • Ball milling influenced the thermal stability and magnetic properties.

  14. C-H vs C-C Bond Activation of Acetonitrile and Benzonitrile via Oxidative Addition: Rhodium vs Nickel and Cp* vs Tp

    E-Print Network [OSTI]

    Jones, William D.

    or benzene leads to thermal rearrangement to the C-C activation product, (C5Me5)Rh(PMe3)(CH3)(CN) (4C-H vs C-C Bond Activation of Acetonitrile and Benzonitrile via Oxidative Addition: Rhodium vs of the C-H activation product, (C5Me5)Rh(PMe3)(CH2CN)H (2). Thermolysis of this product in acetonitrile

  15. Analysis of the Crystal Ball data on $K^-p\\to?^0?^0$ reaction with center-of-mass energies of $1536\\sim 1676$ MeV

    E-Print Network [OSTI]

    Jun Shi; Bing-Song Zou

    2014-11-03

    With an effective Lagrangian approach, we analyze the $K^-p\\to \\pi^0\\Sigma^0$ reaction to study the $\\Lambda$ hyperon resonances by fitting the Crystal Ball data on differential cross sections and $\\Sigma^0$ polarization with the center-of-mass energies of $1536\\sim 1676$ MeV. Besides well established PDG 4-star $\\Lambda$ resonances around this energy range, the $\\Lambda(1600){1\\over 2}^+$ resonance, listed as a 3-star resonance in PDG, is found to be definitely needed. In addition, there is strong evidence for the existence of a new $\\Lambda({3\\over 2}^+)$ resonance around 1680 MeV.

  16. Helios movable Hartmann ball

    SciTech Connect (OSTI)

    Tucker, H.E.; Day, R.D.; Hedges, R.O.; Hanlon, J.A.; Kortegaard, B.L.

    1981-01-01

    The MHB has been in operation for about nine months and has been performing quite well. It has provided the Helios laser fusion facility with additional target illumination flexibility so that many additional parameters can be investigated in the realm of target implosion physics.

  17. Ping Pong Ball Anemometer

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration wouldMass mapSpeeding access| DepartmentPeerFederal FleetUp inrdPilot summer programPing Pong

  18. Ping Pong Ball Anemometers

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power Administration wouldMass mapSpeeding access| DepartmentPeerFederal FleetUp inrdPilot summer programPing Pong*

  19. CH-{\\pi} interaction-induced deep orbital deformation in a benzene-methane weak binding system

    E-Print Network [OSTI]

    Li, Jianfu

    2015-01-01

    The nonbonding interaction between benzene and methane, called CH-{\\pi} interaction, plays an important role in physical, chemical, and biological fields. CH-{\\pi} interaction can decrease the system total energy and promote the formation of special geometric configurations. This work investigates systemically the orbital distribution and composition of the benzene-methane complex for the first time using ab initio calculation based on different methods and basis sets. Surprisingly, we find strong deformation in HOMO-4 and LUMO+2 induced by CH-{\\pi} interaction, extending the general view that nonbonding interaction does not cause orbital change of molecules.

  20. The Spectra of Main Sequence Stars in Galactic Globular Clusters II. CH and CN Bands in M71

    E-Print Network [OSTI]

    J. G. Cohen

    1999-01-26

    Spectra with a high signal-to-noise ratio of 79 stars which are just below the main sequence turnoff of M71 are presented. They yield indices for the strength of the G band of CH and the ultraviolet CN band at 3885 \\AA. These indices are each to first order bimodal and they are anti-correlated. There are approximately equal numbers of CN weak/CH strong and CN strong/CH weak main sequence stars in M71. It is not yet clear whether these star-to-star variations arise from primordial variations or from mixing within a fraction of individual stars as they evolve.

  1. CO2 CH4 flux Air temperature Soil temperature and Soil moisture, Barrow, Alaska 2013 ver. 1

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

    Margaret Torn

    2015-01-14

    This dataset consists of field measurements of CO2 and CH4 flux, as well as soil properties made during 2013 in Areas A-D of Intensive Site 1 at the Next-Generation Ecosystem Experiments (NGEE) Arctic site near Barrow, Alaska. Included are i) measurements of CO2 and CH4 flux made from June to September (ii) Calculation of corresponding Gross Primary Productivity (GPP) and CH4 exchange (transparent minus opaque) between atmosphere and the ecosystem (ii) Measurements of Los Gatos Research (LGR) chamber air temperature made from June to September (ii) measurements of surface layer depth, type of surface layer, soil temperature and soil moisture from June to September.

  2. CO2 CH4 flux Air temperature Soil temperature and Soil moisture, Barrow, Alaska 2013 ver. 1

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

    Margaret Torn

    This dataset consists of field measurements of CO2 and CH4 flux, as well as soil properties made during 2013 in Areas A-D of Intensive Site 1 at the Next-Generation Ecosystem Experiments (NGEE) Arctic site near Barrow, Alaska. Included are i) measurements of CO2 and CH4 flux made from June to September (ii) Calculation of corresponding Gross Primary Productivity (GPP) and CH4 exchange (transparent minus opaque) between atmosphere and the ecosystem (ii) Measurements of Los Gatos Research (LGR) chamber air temperature made from June to September (ii) measurements of surface layer depth, type of surface layer, soil temperature and soil moisture from June to September.

  3. CH2M Hill Heat Stress Mitigation Efforts During Tank Farm Work Activities

    SciTech Connect (OSTI)

    Smoot, W.L. [CH2M HILL Hanford Group, Inc., Richland, WA (United States)

    2007-07-01

    In the past, while working under the hot summer sun at the Hanford Tank Farms, workers were assigned a protective work-rest regimen and heat stress mitigation efforts were applied to prevent heat-related illnesses and minimize impacts to project schedules. In February 2006, CH2M HILL kicked off a heat stress improvement initiative led by an experienced person emphasizing the importance of worker involvement, employee education, and the application of the ALARA, or As Low As Reasonably Achievable, concepts of engineered controls, administrative controls, personal protective equipment, and physiological and work site monitoring. As a result of this initiative built upon previous years' efforts, CH2M HILL experienced increased 'wrench time' during the summer of 2006 with fewer heat-related illnesses than in previous years. (authors)

  4. Charge-Separation in Uranium Diazomethane Complexes Leading to C-H Activation and Chemical Transformation

    E-Print Network [OSTI]

    Meyer, Karsten

    Charge-Separation in Uranium Diazomethane Complexes Leading to C-H Activation and Chemical of diphenyldiazomethane with [((t-Bu ArO)3tacn)UIII ] (1) results in an 2 -bound diphenyldiazomethane uranium complex-shell ligand, [((t-Bu ArO)3tacn)UIV (2 -NNCPh2)] (2). Treating Ph2CN2 with a uranium complex that contains

  5. Chandra ACIS Survey of M33 (ChASeM33): A First Look

    E-Print Network [OSTI]

    Paul P. Plucinsky; Benjamin Williams; Knox S. Long; Terrance J. Gaetz; Manami Sasaki; Wolfgang Pietsch; Ralph Tuellmann; Randall K. Smith; William P. Blair; David Helfand; John P. Hughes; P. Frank Winkler; Miguel de Avillez; Luciana Bianchi; Dieter Breitschwerdt; Richard J. Edgar; Parviz Ghavamian; Jonathan Grindlay; Frank Haberl; Robert Kirshner; Kip Kuntz; Tsevi Mazeh; Thomas G. Pannuti; Avi Shporer; David A. Thilker

    2007-09-26

    We present an overview of the Chandra ACIS Survey of M33 (ChASeM33): A Deep Survey of the Nearest Face-on Spiral Galaxy. The 1.4 Ms survey covers the galaxy out to $R \\approx 18\\arcmin (\\approx 4$ kpc). These data provide the most intensive, high spatial resolution assessment of the X-ray source populations available for the confused inner regions of M33. Mosaic images of the ChASeM33 observations show several hundred individual X-ray sources as well as soft diffuse emission from the hot interstellar medium. Bright, extended emission surrounds the nucleus and is also seen from the giant \\hii regions NGC 604 and IC 131. Fainter extended emission and numerous individual sources appear to trace the inner spiral structure. The initial source catalog, arising from $\\sim$~2/3 of the expected survey data, includes 394 sources significant at the $3\\sigma$ confidence level or greater, down to a limiting luminosity (absorbed) of $\\sim$1.6\\ergs{35} (0.35 -- 8.0 keV). The hardness ratios of the sources separate those with soft, thermal spectra such as supernova remnants from those with hard, non-thermal spectra such as X-ray binaries and background active galactic nuclei. Emission extended beyond the Chandra point spread function is evident in 23 of the 394 sources. Cross-correlation of the ChASeM33 sources against previous catalogs of X-ray sources in M33 results in matches for the vast majority of the brighter sources and shows 28 ChASeM33 sources within 10\\arcsec of supernova remnants identified by prior optical and radio searches. This brings the total number of such associations to 31 out of 100 known supernova remnants in M33.

  6. Modeling binary CO{sub 2}/CH{sub 4} flow through coal media

    SciTech Connect (OSTI)

    Gumrah, F.; Balan, H.O.; Atay, M.U. [Middle East Technical University, Ankara (Turkey)

    2008-07-01

    CO{sub 2} can be sequestered in coal seams considering the environmental issues. By means of injecting CO{sub 2} into the coal seams, both sequestration of CO{sub 2} and the enhanced recovery of methane inside the coal seam can be realized. One-dimensional simulation regarding the binary CO{sub 2}/CH{sub 4} flow in a coal seam core was studied by using an analytical solution method. The simulation results were compared with experimental data by matching the effluent concentrations of CO{sub 2} and CH{sub 4}. The transport parameters such as longitudinal dispersion coefficient, retardation factor, and distribution coefficient were determined. It was seen that the amount of CO{sub 2} captured inside the coal sample during binary displacement was much lower than the maximum adsorption capacity of the coal at the same pressure. Then the transport behavior of CO{sub 2} and CH{sub 4} inside the coal seam was simulated. The results of analytical solution were in good agreement with the measured ones within the acceptable error range.

  7. Communication: Ultraviolet photodissociation dynamics of the simplest Criegee intermediate CH{sub 2}OO

    SciTech Connect (OSTI)

    Lehman, Julia H.; Li, Hongwei; Beames, Joseph M.; Lester, Marsha I.

    2013-10-14

    The velocity and angular distributions of O {sup 1}D photofragments arising from UV excitation of the CH{sub 2}OO intermediate on the B {sup 1}A??X {sup 1}A? transition are characterized using velocity map ion imaging. The anisotropic angular distribution yields the orientation of the transition dipole moment, which reflects the ?*?? character of the electronic transition associated with the COO group. The total kinetic energy release distributions obtained at several photolysis wavelengths provide detail on the internal energy distribution of the formaldehyde cofragments and the dissociation energy of CH{sub 2}OO X {sup 1}A? to O {sup 1}D + H{sub 2}CO X {sup 1}A{sub 1}. A common termination of the total kinetic energy distributions, after accounting for the different excitation energies, gives an upper limit for the CH{sub 2}OO X {sup 1}A? dissociation energy of D{sub 0}? 54 kcal mol{sup ?1}, which is compared with theoretical predictions including high level multi-reference ab initio calculations.

  8. Synthesis of Fe/SiO{sub 2} and iron oxides/SiO{sub 2} nanocomposites by long-term ball milling

    SciTech Connect (OSTI)

    Pozo López, G.; Condó, A.M.; Urreta, S.E.; Silvetti, S.P.

    2014-01-01

    Graphical abstract: - Highlights: • Iron–iron oxides/silica composites are synthesized by long term dry ball-milling. • Bcc iron and ?-quartz powders are used as precursors. • Surface effects enhance coercivity in iron/silica nanocomposites. • In spite of their small size, about 10 nm, iron particles are ferromagnetic. • Ferro and superparamagnetic particles are found in maghemite/silica composites. - Abstract: Iron oxide/SiO{sub 2} nanocomposites are synthesized by dry ball-milling a mixture of bcc Fe and ?-quartz powders for prolonged times. A sequence of nanocomposites is obtained, with small magnetic particles dispersed in a non magnetic, amorphous matrix. The powders are characterized by X-ray diffraction and transmission electron microscopy. The magnetic hysteresis properties are investigated in the range 50–300 K. After 120 h milling, deformed, non-spherical, ?-Fe nanocrystallites of about 10 nm in size and very few small (<10 nm) maghemite particles are found. At room temperature, iron particles are ferromagnetic and a large effective magnetic anisotropy is estimated, which is mainly attributed to surface effects. Between 160 and 200 h milling, maghemite nanoparticles are observed while after 220 h grinding, hematite phase appears; after 340 h milling, the sample consists of ferromagnetic hematite particles with a broad size distribution (5–50 nm) embedded in an amorphous matrix.

  9. [(CH3)4N][(C5H5NH)0.8((CH3)3NH)0.2]U2Si9O23F4 (USH-8): An Organically Templated Open-Framework Uranium Silicate

    E-Print Network [OSTI]

    Wang, Xiqu

    -Framework Uranium Silicate Xiqu Wang, Jin Huang, and Allan J. Jacobson* Department of Chemistry, Uni pyramids we obtained also a number of open-framework uranium silicates.18,19 These new compounds were-framework uranium fluorosilicate [(CH3)4N][(C5H5NH)0.8((CH3)3NH)0.2]U2Si9O23F4 (USH- 8) that has been synthesized

  10. The Breathing Orbital Valence Bond Method in Diffusion Monte Carlo: C-H Bond Dissociation of Acetylene

    E-Print Network [OSTI]

    Braida, Benoit

    2009-01-01

    Quantum Chem. 2005, (19) Barnett, R. N. ; Sun, Z. ; Lester,In a systematic DMC study, Barnett et al. 19 explored thefor the C-H bond distance. Barnett et al. reported 1-CSF DMC

  11. Experimental realization of catalytic CH4 hydroxylation predicted for an iridium NNC pincer complex, demonstrating thermal, protic,

    E-Print Network [OSTI]

    Goddard III, William A.

    Experimental realization of catalytic CH4 hydroxylation predicted for an iridium NNC pincer complex; functionalization using NaIO4 and KIO3 gives the oxy-ester. The most efficient methane hydroxylation catalysts

  12. 40 CFR Ch. I (7105 Edition) 190.10 period in which he is engaged in car-

    E-Print Network [OSTI]

    or emissions therefrom and car- rying out inspection and enforcement activities to assure compliance6 40 CFR Ch. I (7­1­05 Edition)§ 190.10 period in which he is engaged in car- rying out any

  13. The role of CO2 in CH4 exsolution from deep brine: Implications for geologic carbon sequestration

    E-Print Network [OSTI]

    Oldenburg, C.M.

    2014-01-01

    spreading under the shale where gas saturation is higher duecomposition of the gas above the shale is mainly CH 4 , andeffect of the shale remains as higher gas saturations are

  14. C-H Bond Strengths and Acidities in Aromatic Systems: Effects of Nitrogen Incorporation in Mono-, Di-, and Triazines

    E-Print Network [OSTI]

    Lineberger, W. Carl

    afterglow-selected ion tube (FA-SIFT) mass spectrometry to obtain deprotonation enthalpies (acidH298 of the corresponding radical in a thermochemical cycle to determine the corresponding C-H bond dissociation energy (BDE

  15. Aerobic C-H Acetoxylation of 8-Methylquinoline in PdII-Pyridinecarboxylic Acid Systems: Some Structure-Reactivity Relationships

    SciTech Connect (OSTI)

    Wang, Daoyong; Zavalij, Peter Y.; Vedernikov, Andrei N.

    2013-09-09

    Catalytic oxidative C–H acetoxylation of 8-methylquinoline as a model substrate with O2 as oxidant was performed using palladium(II) carboxylate catalysts derived from four different pyridinecarboxylic acids able to form palladium(II) chelates of different size. A comparison of the rates of the substrate C–H activation and the O2 activation steps shows that the C–H activation step is rate-limiting, whereas the O2 activation occurs at a much faster rate already at 20 °C. The chelate ring size and the chelate ring strain of the catalytically active species are proposed to be the key factors affecting the rate of the C–H activation.

  16. 1646 Organometallics 1994, 13, 1646-1655 A Static Agostic a-CH-M Interaction Observable by NMR

    E-Print Network [OSTI]

    Girolami, Gregory S.

    a function of temperature indicatesthat the molecule undergoestwo different dynamic processes. One process form close contacts with the carbon atoms of the a-CH2 groups. Important bond distances and angles: Cr

  17. ch_1

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    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The CarbonDetectorDiscovery1.0

  18. ch_10

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  19. ch_11

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    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.0 Response Response to

  20. ch_12

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  1. ch_13

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  2. ch_2

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  3. ch_2

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  4. ch_2

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  5. ch_3

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  6. ch_3

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  7. ch_3

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  8. ch_3

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  9. ch_3

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  10. ch_4

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  11. ch_4

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  12. ch_4

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  13. ch_4

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  14. ch_4

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  15. ch_4

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  16. ch_4

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

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  17. ch_4

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

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  18. ch_5

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.071 DOE/EIS-0287

  19. ch_5

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.071 DOE/EIS-028722

  20. ch_5

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.071 DOE/EIS-02872244

  1. ch_5

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.071

  2. ch_5

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.07125 DOE/EIS-0287

  3. ch_5

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.07125 DOE/EIS-028745

  4. ch_5

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.07125

  5. ch_6

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.07125 6.0 Sta Sta

  6. ch_7

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.07125 6.0 Sta Sta0 7.0

  7. ch_8

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.07125 6.0 Sta Sta0

  8. ch_9

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.07125 6.0 Sta Sta0.0

  9. ch_9

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.07125 6.0 Sta Sta0.0

  10. ch_9

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantityBonneville Power AdministrationRobust,Field-effectWorkingLos AlamosSimulation Initiative ccsi.jpg The0 11.07125 6.0 Sta

  11. Thermal decomposition of CH{sub 3}CHO studied by matrix infrared spectroscopy and photoionization mass spectroscopy

    SciTech Connect (OSTI)

    Vasiliou, AnGayle K. [Department of Chemistry and Biochemistry, University of Colorado, Boulder, Colorado 80309-0215 (United States); National Renewable Energy Laboratory, 1617 Cole Blvd., Golden, Colorado 80401 (United States); Piech, Krzysztof M.; Reed, Beth; Ellison, G. Barney [Department of Chemistry and Biochemistry, University of Colorado, Boulder, Colorado 80309-0215 (United States); Zhang Xu [Jet Propulsion Laboratory, California Institute of Technology, 4800 Oak Grove Drive, Pasadena, California 91109-8099 (United States); Nimlos, Mark R. [National Renewable Energy Laboratory, 1617 Cole Blvd., Golden, Colorado 80401 (United States); Ahmed, Musahid; Golan, Amir; Kostko, Oleg [Chemical Sciences Division, LBNL MS 6R-2100, Berkeley, California 94720 (United States); Osborn, David L. [Combustion Research Facility, Sandia National Laboratories, P.O. Box 969 MS 9055, Livermore, California 94551-0969 (United States); David, Donald E. [Integrated Instrument Design Facility, CIRES, University of Colorado, Boulder, Colorado 80309-0216 (United States); Urness, Kimberly N.; Daily, John W. [Center for Combustion and Environmental Research, Department of Mechanical Engineering, University of Colorado at Boulder, Boulder, Colorado 80309-0427 (United States); Stanton, John F. [Institute for Theoretical Chemistry, Department of Chemistry, University of Texas, Austin, Texas 78712 (United States)

    2012-10-28

    A heated SiC microtubular reactor has been used to decompose acetaldehyde and its isotopomers (CH{sub 3}CDO, CD{sub 3}CHO, and CD{sub 3}CDO). The pyrolysis experiments are carried out by passing a dilute mixture of acetaldehyde (roughly 0.1%-1%) entrained in a stream of a buffer gas (either He or Ar) through a heated SiC reactor that is 2-3 cm long and 1 mm in diameter. Typical pressures in the reactor are 50-200 Torr with the SiC tube wall temperature in the range 1200-1900 K. Characteristic residence times in the reactor are 50-200 {mu}s after which the gas mixture emerges as a skimmed molecular beam at a pressure of approximately 10 {mu}Torr. The reactor has been modified so that both pulsed and continuous modes can be studied, and results from both flow regimes are presented. Using various detection methods (Fourier transform infrared spectroscopy and both fixed wavelength and tunable synchrotron radiation photoionization mass spectrometry), a number of products formed at early pyrolysis times (roughly 100-200 {mu}s) are identified: H, H{sub 2}, CH{sub 3}, CO, CH{sub 2}=CHOH, HC{identical_to}CH, H{sub 2}O, and CH{sub 2}=C=O; trace quantities of other species are also observed in some of the experiments. Pyrolysis of rare isotopomers of acetaldehyde produces characteristic isotopic signatures in the reaction products, which offers insight into reaction mechanisms that occur in the reactor. In particular, while the principal unimolecular processes appear to be radical decomposition CH{sub 3}CHO (+M) {yields} CH{sub 3}+ H + CO and isomerization of acetaldehyde to vinyl alcohol, it appears that the CH{sub 2}CO and HCCH are formed (perhaps exclusively) by bimolecular reactions, especially those involving hydrogen atom attacks.

  12. The Radiative Transfer Of CH{sub 4}-N{sub 2} Plasma Arc

    SciTech Connect (OSTI)

    Benallal, R.; Liani, B.

    2008-09-23

    Any physical modelling of a circuit-breaker arc therefore requires an understanding of the radiated energy which is taken into account in the form of a net coefficient. The evaluation of the net emission coefficient is performed by the knowledge of the chemical plasma composition and the resolution of the radiative transfer equation. In this paper, the total radiation which escapes from a CH{sub 4}-N{sub 2} plasma is calculated in the temperature range between 5000 and 30000K on the assumption of a local thermodynamic equilibrium and we have studied the nitrogen effect in the hydrocarbon plasmas.

  13. Enforcement Letter, CH2M Hill - October 4, 2004 | Department of Energy

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergyTher i n cEnergyNatural GasDepartment ofDepartment2 Issued to04 Issued to CH2M

  14. Consent Order, CH2M Hill Hanford Group, Inc. - EA-2000-09 | Department of

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergy A plug-in electric vehicle (PEV)Day-June 22,FresnoSky)Nuclear SafetyEnergy CH2M

  15. Consent Order, CH2M-WG Idaho, LLC - WCO-2011-01 | Department of Energy

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

    AFDC Printable Version Share this resource Send a link to EERE: Alternative Fuels Data Center Home Page to someone by E-mail Share EERE: Alternative Fuels Data Center Home Page on Facebook Tweet about EERE: Alternative Fuels Data Center Home Page on Twitter Bookmark EERE: Alternative Fuels Data Center Homesum_a_epg0_fpd_mmcf_m.xls" ,"Available from WebQuantity of Natural GasAdjustmentsShirleyEnergy A plug-in electric vehicle (PEV)Day-June 22,FresnoSky)Nuclear SafetyEnergy CH2M1

  16. A new measurement of the rare decay eta -> pi^0 gamma gamma with the Crystal Ball/TAPS detectors at the Mainz Microtron

    SciTech Connect (OSTI)

    Nefkens, B M; Prakhov, S; Aguar-Bartolom??, P; Annand, J R; Arends, H J; Bantawa, K; Beck, R; Bekrenev, V; Bergh??user, H; Braghieri, A; Briscoe, W J; Brudvik, J; Cherepnya, S; Codling, R F; Collicott, C; Costanza, S; Danilkin, I V; Denig, A; Demissie, B; Dieterle, M; Downie, E J; Drexler, P; Fil'kov, L V; Fix, A; Garni, S; Glazier, D I; Gregor, R; Hamilton, D; Heid, E; Hornidge, D; Howdle, D; Jahn, O; Jude, T C; Kashevarov, V L; K??ser, A; Keshelashvili, I; Kondratiev, R; Korolija, M; Kotulla, M; Koulbardis, A; Kruglov, S; Krusche, B; Lisin, V; Livingston, K; MacGregor, I J; Maghrbi, Y; Mancel, J; Manley, D M; McNicoll, E F; Mekterovic, D; Metag, V; Mushkarenkov, A; Nikolaev, A; Novotny, R; Oberle, M; Ortega, H; Ostrick, M; Ott, P; Otte, P B; Oussena, B; Pedroni, P; Polonski, A; Robinson, J; Rosner, G; Rostomyan, T; Schumann, S; Sikora, M H; Starostin, A; Strakovsky, I I; Strub, T; Suarez, I M; Supek, I; Tarbert, C M; Thiel, M; Thomas, A; Unverzagt, M; Watts, D P; Werthmueller, D; Witthauer, L

    2014-08-01

    A new measurement of the rare, doubly radiative decay eta->pi^0 gamma gamma was conducted with the Crystal Ball and TAPS multiphoton spectrometers together with the photon tagging facility at the Mainz Microtron MAMI. New data on the dependence of the partial decay width, Gamma(eta->pi^0 gamma gamma), on the two-photon invariant mass squared, m^2(gamma gamma), as well as a new, more precise value for the decay width, Gamma(eta->pi^0 gamma gamma) = (0.33+/-0.03_tot) eV, are based on analysis of 1.2 x 10^3 eta->pi^0 gamma gamma decays from a total of 6 x 10^7 eta mesons produced in the gamma p -> eta p reaction. The present results for dGamma(eta->pi^0 gamma gamma)/dm^2(gamma gamma) are in good agreement with previous measurements and recent theoretical calculations for this dependence.

  17. The peculiar distribution of CH3CN in IRC+10216 seen by ALMA

    E-Print Network [OSTI]

    Agundez, M; Quintana-Lacaci, G; Prieto, L Velilla; Castro-Carrizo, A; Marcelino, N; Guelin, M

    2015-01-01

    IRC+10216 is a circumstellar envelope around a carbon-rich evolved star which contains a large variety of molecules. According to interferometric observations, molecules are distributed either concentrated around the central star or as a hollow shell with a radius of 15". We present ALMA Cycle 0 band 6 observations of the J=14-13 rotational transition of CH3CN in IRC+10216, obtained with an angular resolution of 0.76x0.61. The bulk of the emission is distributed as a hollow shell located at just 2" from the star, with a void of emission in the central region up to a radius of 1". This spatial distribution is markedly different from those found to date in this source for other molecules. Our analysis indicate that methyl cyanide is not formed neither in the stellar photosphere nor far in the outer envelope, but at radial distances as short as 1-2", reaching a maximum abundance of 5e-8 with respect to H2 at about 6" from the star. Standard chemical models of IRC+10216 predict that CH3CN should form farther out ...

  18. CHIRON: a package for ChPT numerical results at two loops

    E-Print Network [OSTI]

    Johan Bijnens

    2014-12-02

    This document describes the package CHIRON which includes two libraries, chiron itself and jbnumlib. CHIRON is a set of routines useful for two-loop numerical results in Chiral Perturbation Theory (ChPT). It includes programs for the needed one- and two-loop integrals as well as routines to deal with the ChPT parameters. The present version includes everything needed for the masses, decay constants and quark-antiquark vacuum-expectation-values. An added routine calculates consistent values for the masses and decay constants when the pion and kaon masses are varied. In addition a number of finite volume results are included: one-loop tadpole integrals, two-loop sunset integrals and the results for masses and decay constants. The numerical routine library jbnumlib contains the numerical routines used in chiron. Many are to a large extent simple C++ versions of routines in the CERNLIB numerical library. Notable exceptions are the dilogarithm and the Jacobi theta function implementations. This paper describes what is included in CHIRON v0.50.

  19. Cooperative, Multicentered CH/ Interaction-Controlled Supramolecular Self-Assembly Processes

    SciTech Connect (OSTI)

    Li, Qing; Han, Chengbo; Horton, Scott R; Fuentes-Cabrera, Miguel A; Sumpter, Bobby G; Lu, Wenchang; Bernholc, J.; Maksymovych, Petro; Pan, Minghu

    2012-01-01

    Supramolecular self-assembly on well-defined surfaces provides access to a multitude of nanoscale architectures, including clusters of distinct symmetry and size. The driving forces underlying supramolecular structures generally involve both graphoepitaxy and weak directional nonconvalent interactions. Here we show that functionalizing a benzene molecule with an ethyne group introduces attractive interactions in a 2D geometry, which would otherwise be dominated by intermolecular repulsion. Furthermore, the attractive interactions enable supramolecular self-assembly, wherein a subtle balance between very weak CH/{pi} bonding and molecule-surface interactions produces a well-defined 'magic' dimension and chirality of supramolecular clusters. The nature of the process is corroborated by extensive scanning tunneling microscopy/spectroscopy (STM/S) measurements and ab initio calculations, which emphasize the cooperative, multicenter characters of the CH/{pi} interaction. This work points out new possibilities for chemical functionalization of {pi}-conjugated hydrocarbon molecules that may allow for the rational design of supramolecular clusters with a desired shape and size.

  20. CO2 and CH4 Fluxes across Polygon Geomorphic Types, Barrow, Alaska, 2006-2010

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

    Tweedie,Craig; Lara, Mark

    2014-09-17

    Carbon flux data are reported as Net Ecosystem Exchange (NEE), Gross Ecosystem Exchange (GEE), Ecosystem Respiration (ER), and Methane (CH4) flux. Measurements were made at 82 plots across various polygon geomorphic classes at research sites on the Barrow Environmental Observatory (BEO), the Biocomplexity Experiment site on the BEO, and the International Biological Program (IBP) site a little west of the BEO. This product is a compilation of data from 27 plots as presented in Lara et al. (2012), data from six plots presented in Olivas et al. (2010); and from 49 plots described in (Lara et al. 2014). Measurements were made during the peak of the growing seasons during 2006 to 2010. At each of the measurement plots (except Olivas et al., 2010) four different thicknesses of shade cloth were used to generate CO2 light response curves. Light response curves were used to normalize photosynthetically active radiation that is diurnally variable to a peak growing season average ~400 umolm-2sec-1. At the Olivas et al. (2010) plots, diurnal patterns were characterized by repeated sampling. CO2 measurements were made using a closed-chamber photosynthesis system and CH4 measurements were made using a photo-acoustic multi-gas analyzer. In addition, plot-level measurements for thaw depth (TD), water table depth (WTD), leaf area index (LAI), and normalized difference vegetation index (NDVI) are summarized by geomorphic polygon type.

  1. Class I methanol (CH{sub 3}OH) maser conditions near supernova remnants

    SciTech Connect (OSTI)

    McEwen, Bridget C.; Pihlström, Ylva M.; Sjouwerman, Loránt O.

    2014-10-01

    We present results from calculations of the physical conditions necessary for the occurrence of 36.169 (4{sub –1}-3{sub 0} E), 44.070 (7{sub 0}-6{sub 1} A {sup +}), 84.521 (5{sub –1}-4{sub 0} E), and 95.169 (8{sub 0}-7{sub 1} A {sup +}) GHz methanol (CH{sub 3}OH) maser emission lines near supernova remnants (SNRs), using the MOLPOP-CEP program. The calculations show that given a sufficient methanol abundance, methanol maser emission arises over a wide range of densities and temperatures, with optimal conditions at n ? 10{sup 4}-10{sup 6} cm{sup –3} and T > 60 K. The 36 GHz and 44 GHz transitions display more significant maser optical depths compared to the 84 GHz and 95 GHz transitions over the majority of physical conditions. It is also shown that line ratios are an important and applicable probe of the gas conditions. The line ratio changes are largely a result of the E-type transitions becoming quenched faster at increasing densities. The modeling results are discussed using recent observations of CH{sub 3}OH and hydroxyl (OH) masers near the SNRs G1.4–0.1, W28, and Sgr A East.

  2. Barrierless proton transfer across weak CH?O hydrogen bonds in dimethyl ether dimer

    SciTech Connect (OSTI)

    Yoder, Bruce L. West, Adam H. C.; Signorell, Ruth; Bravaya, Ksenia B.; Bodi, Andras; Sztáray, Bálint

    2015-03-21

    We present a combined computational and threshold photoelectron photoion coincidence study of two isotopologues of dimethyl ether, (DME ? h{sub 6}){sub n} and (DME ? d{sub 6}){sub n}n = 1 and 2, in the 9–14 eV photon energy range. Multiple isomers of neutral dimethyl ether dimer were considered, all of which may be present, and exhibited varying C–H?O interactions. Results from electronic structure calculations predict that all of them undergo barrierless proton transfer upon photoionization to the ground electronic state of the cation. In fact, all neutral isomers were found to relax to the same radical cation structure. The lowest energy dissociative photoionization channel of the dimer leads to CH{sub 3}OHCH{sub 3}{sup +} by the loss of CH{sub 2}OCH{sub 3} with a 0 K appearance energy of 9.71 ± 0.03 eV and 9.73 ± 0.03 eV for (DME ? h{sub 6}){sub 2} and deuterated (DME ? d{sub 6}){sub 2}, respectively. The ground state threshold photoelectron spectrum band of the dimethyl ether dimer is broad and exhibits no vibrational structure. Dimerization results in a 350 meV decrease of the valence band appearance energy, a 140 meV decrease of the band maximum, thus an almost twofold increase in the ground state band width, compared with DME ? d{sub 6} monomer.

  3. CO2 and CH4 Fluxes across Polygon Geomorphic Types, Barrow, Alaska, 2006-2010

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

    Tweedie,Craig; Lara, Mark

    Carbon flux data are reported as Net Ecosystem Exchange (NEE), Gross Ecosystem Exchange (GEE), Ecosystem Respiration (ER), and Methane (CH4) flux. Measurements were made at 82 plots across various polygon geomorphic classes at research sites on the Barrow Environmental Observatory (BEO), the Biocomplexity Experiment site on the BEO, and the International Biological Program (IBP) site a little west of the BEO. This product is a compilation of data from 27 plots as presented in Lara et al. (2012), data from six plots presented in Olivas et al. (2010); and from 49 plots described in (Lara et al. 2014). Measurements were made during the peak of the growing seasons during 2006 to 2010. At each of the measurement plots (except Olivas et al., 2010) four different thicknesses of shade cloth were used to generate CO2 light response curves. Light response curves were used to normalize photosynthetically active radiation that is diurnally variable to a peak growing season average ~400 umolm-2sec-1. At the Olivas et al. (2010) plots, diurnal patterns were characterized by repeated sampling. CO2 measurements were made using a closed-chamber photosynthesis system and CH4 measurements were made using a photo-acoustic multi-gas analyzer. In addition, plot-level measurements for thaw depth (TD), water table depth (WTD), leaf area index (LAI), and normalized difference vegetation index (NDVI) are summarized by geomorphic polygon type.

  4. Research by BNL investigators was performed under the auspices of the U.S. Department of Energy under Contract No. DE-AC02-98CH10886.

    E-Print Network [OSTI]

    of Energy under Contract No. DE-AC02-98CH10886. A MEASUREMENT TECHNIQUE FOR HYDROXYACETONE P. J. Klotz, E. S #12;A MEASUREMENT TECHNIQUE FOR HYDROXYACETONE P. J. Klotz, E. S. C. Kwok, X. Zhou, J. H. Lee, and Y of hydrocarbons of the type, CH3(R)C=CH2. Tuazon and Atkinson (1990) reported HA yield of 41% from the OH

  5. Anisotropic magnetoresistance in the organic superconductor -,,BEDT-TTF...2SF5CH2CF2SO3 X. Su and F. Zuo

    E-Print Network [OSTI]

    Zuo, Fulin

    Anisotropic magnetoresistance in the organic superconductor -,,BEDT-TTF...2SF5CH2CF2SO3 X. Su and F direction in an all organic superconductor - BEDT-TTF 2SF5CH2CF2SO3. For H I, the isothermal superconductor - BEDT-TTF 2SF5CH2CF2SO3.16,19,20 The structure contains layers of nearly parallel BEDT

  6. Anomalous low-temperature and high-field magnetoresistance in the organic superconductor -,,BEDT-TTF...2SF5CH2CF2SO3

    E-Print Network [OSTI]

    Zuo, Fulin

    -TTF...2SF5CH2CF2SO3 F. Zuo, X. Su, and P. Zhang Department of Physics, University of Miami, Coral Gables superconductor -(BEDT-TTF)2SF5CH2CF2SO3. Unlike other BEDT-TTF based organic superconductors, a nonmetallic discovered all organic supercon- ductor -(BEDT-TTF)2SF5CH2CF2SO3. Resistance mea- surements at low

  7. Memorandum CH2M WG Idaho, LLC, Request for Variance to Title 10, Code of Federal Regulations Part 851, "Worker Safety and Health Program"

    Broader source: Energy.gov [DOE]

    Memorandum CH2M WG Idaho, LLC, Request for Variance to Title 10, Code of Federal Regulations Part 851, "Worker Safety and Health Program"

  8. Research by BNL investigators was performed under the auspices of the U.S. Department of Energy under Contract No. DE-AC02-98CH10886.

    E-Print Network [OSTI]

    of Energy under Contract No. DE-AC02-98CH10886. BNL-64805 (Abstract) OZONE PRODUCTION IN THE NEW YORK CITY

  9. A concise and scalable strategy for the total synthesis of dictyodendrin B based on sequential C–H functionalization

    E-Print Network [OSTI]

    Pitts, Andrew K.; O'Hara, Fionn; Snell, Robert H.; Gaunt, Matthew J.

    2015-02-23

    –H functionalizations’ (comprising of metal-catalyzed C–H activation, electrophilic aromatic substitution, radical addition and directed metalation) we reasoned we would be well equipped to meet the ever-changing demands of the evolving molecule as the synthesis... and Scheme 4a).16 Although we investigated metal-catalyzed C–H insertion processes using the azide, none of these methods resulted in the desired heterocycle.17 Carbazole 14 could be isolated using Tokuyama’s batch conditions for the thermal decomposition...

  10. Liu Shao-Ch'i and "People's War": A Report on the Creation of Base Areas in 1938

    E-Print Network [OSTI]

    Schwarz, Henry G.

    1969-01-01

    and the methods they used in dealing with those problems. The document is a report by Liu Shao-ch'i on the creation of Chin-Ch'a-Chi, formally the Shansi-Chahar-Hopei Border region, and other resistance cen ters behind Japanese lines. It was said to have been... provinces of Hopei, Chahar, Suiyiian, Shan tung, and Shansi. Only the East Hopei Autonomous Council 5 under General Yin Ju-keng materialized from the Japanese ef forts. Along the northern periphery of North China, bordering on the Gobi desert...

  11. Detection of class I methanol (CH{sub 3}OH) maser candidates in supernova remnants

    SciTech Connect (OSTI)

    Pihlström, Y. M.; Mesler, R. A.; McEwen, B. C. [Department of Physics and Astronomy, University of New Mexico, MSC07 4220, Albuquerque, NM 87131 (United States); Sjouwerman, L. O.; Frail, D. A.; Claussen, M. J., E-mail: ylva@unm.edu [National Radio Astronomy Observatory, P.O. Box 0, Lopezville Road 1001, Socorro, NM 87801 (United States)

    2014-04-01

    We have used the Karl G. Jansky Very Large Array to search for 36 GHz and 44 GHz methanol (CH{sub 3}OH) lines in a sample of 21 Galactic supernova remnants (SNRs). Mainly the regions of the SNRs with 1720 MHz OH masers were observed. Despite the limited spatial extent covered in our search, methanol masers were detected in both G1.4–0.1 and W28. Additional masers were found in Sgr A East. More than 40 masers were found in G1.4–0.1, which we deduce are due to interactions between the SNR and at least two separate molecular clouds. The six masers in W28 are associated with the molecular cloud that is also associated with the OH maser excitation. We discuss the possibility that the methanol maser may be more numerous in SNRs than the OH maser, but harder to detect due to observational constraints.

  12. Detection of Class I Methanol (CH3OH) Maser Candidates in Supernova Remnants

    E-Print Network [OSTI]

    Pihlström, Y M; Frail, D A; Claussen, M J; Mesler, R A; McEwen, B C

    2013-01-01

    We have used the Karl G. Jansky Very Large Array (VLA) to search for 36 GHz and 44 GHz methanol (CH3OH) lines in a sample of 21 Galactic supernova remnants (SNRs). Mainly the regions of the SNRs with 1720 MHz OH masers were observed. Despite the limited spatial extent covered in our search, methanol masers were detected in both G1.4-0.1 and W28. Additional masers were found in SgrAEast. More than 40 masers were found in G1.4-0.1 which we deduce are due to interactions between the SNR and at least two separate molecular clouds. The six masers in W28 are associated with the molecular cloud that is also associated with the OH maser excitation. We discuss the possibility that the methanol maser may be more numerous in SNRs than the OH maser, but harder to detect due to observational constraints.

  13. Casualties of Heritage Distancing: Children, Ch’orti’ Indigeneity, and the Copán Archaeoscape

    E-Print Network [OSTI]

    McAnany, Patricia A.; Parks, Shoshaunna; Metz, Brent

    2012-01-01

    infrastructure and programs (L. Mortensen , personal c o m m u n i c a t i o n , 2 0 0 6 ) . W h i l e H o n d u r a n C h ' o r t i ' identity is c o m p l e x and di­ versely expressed, it does fol low the general t rends o f the indigenous-r ights discourse... for the conservation o f cultural heritage in the Copän Valley. Examined here is a collaborative education program that balances heritage education with site conservation and creates space for a dialogue about the value o f the past. Designed for Ch 'or t i...

  14. Rhodium-Catalyzed C-C Bond Formation via Heteroatom-Directed C-H Bond Activation

    SciTech Connect (OSTI)

    Colby, Denise; Bergman, Robert; Ellman, Jonathan

    2010-05-13

    Once considered the 'holy grail' of organometallic chemistry, synthetically useful reactions employing C-H bond activation have increasingly been developed and applied to natural product and drug synthesis over the past decade. The ubiquity and relative low cost of hydrocarbons makes C-H bond functionalization an attractive alternative to classical C-C bond forming reactions such as cross-coupling, which require organohalides and organometallic reagents. In addition to providing an atom economical alternative to standard cross - coupling strategies, C-H bond functionalization also reduces the production of toxic by-products, thereby contributing to the growing field of reactions with decreased environmental impact. In the area of C-C bond forming reactions that proceed via a C-H activation mechanism, rhodium catalysts stand out for their functional group tolerance and wide range of synthetic utility. Over the course of the last decade, many Rh-catalyzed methods for heteroatom-directed C-H bond functionalization have been reported and will be the focus of this review. Material appearing in the literature prior to 2001 has been reviewed previously and will only be introduced as background when necessary. The synthesis of complex molecules from relatively simple precursors has long been a goal for many organic chemists. The ability to selectively functionalize a molecule with minimal pre-activation can streamline syntheses and expand the opportunities to explore the utility of complex molecules in areas ranging from the pharmaceutical industry to materials science. Indeed, the issue of selectivity is paramount in the development of all C-H bond functionalization methods. Several groups have developed elegant approaches towards achieving selectivity in molecules that possess many sterically and electronically similar C-H bonds. Many of these approaches are discussed in detail in the accompanying articles in this special issue of Chemical Reviews. One approach that has seen widespread success involves the use of a proximal heteroatom that serves as a directing group for the selective functionalization of a specific C-H bond. In a survey of examples of heteroatom-directed Rh catalysis, two mechanistically distinct reaction pathways are revealed. In one case, the heteroatom acts as a chelator to bind the Rh catalyst, facilitating reactivity at a proximal site. In this case, the formation of a five-membered metallacycle provides a favorable driving force in inducing reactivity at the desired location. In the other case, the heteroatom initially coordinates the Rh catalyst and then acts to stabilize the formation of a metal-carbon bond at a proximal site. A true test of the utility of a synthetic method is in its application to the synthesis of natural products or complex molecules. Several groups have demonstrated the applicability of C-H bond functionalization reactions towards complex molecule synthesis. Target-oriented synthesis provides a platform to test the effectiveness of a method in unique chemical and steric environments. In this respect, Rh-catalyzed methods for C-H bond functionalization stand out, with several syntheses being described in the literature that utilize C-H bond functionalization in a key step. These syntheses are highlighted following the discussion of the method they employ.

  15. Near-infrared spectroscopy of CH{sub 2} by frequency modulated diode laser absorption

    SciTech Connect (OSTI)

    Marr, A.J.; Sears, T.J.; Chang, B.

    1998-09-01

    A diode laser spectrometer incorporating a multi-pass Herriott type cell and frequency modulation detection was used to record a previously unaccessed region of the near-infrared singlet{l_arrow}singlet absorption spectrum of methylene between 10thinsp000 cm{sup {minus}1} and 10thinsp600 cm{sup {minus}1}. With this spectrometer, signal-to-noise ratios close to the quantum noise limit have been attained. Identification of rovibronic transitions to five previously unobserved levels, K=1 {tilde a}(0,9,0), K=2thinsp{tilde b}(0,1,0), K=2thinsp{tilde a}(1,6,0), K=3thinsp{tilde b}(0,1,0) and K=3thinsp{tilde a}(0,10,0), was made. Despite the fact that the present spectra access levels within approximately 1300 cm{sup {minus}1} of the barrier to linearity, the spectrum is dense and perturbed, characteristics in common with spectra recorded in many previous studies at shorter wavelengths. Recent spectroscopic observations of halomethylenes [J. Mol. Spectrosc. {bold 188}, 68 (1998)] had suggested that the CH{sub 2} spectrum might become simpler at longer wavelengths, but this was not evident in the observed spectra. The mixed nature of the singlet states is evidenced by the assignment of rovibronic transitions to levels containing primarily {tilde a}thinsp{sup 1}A{sub 1} state character. The new measurements provide a stringent test for modern theoretical models for CH{sub 2} and will enable refinement of the electronic potential surfaces. {copyright} {ital 1998 American Institute of Physics.}

  16. Sorghum Bran in Meat and Poultry 

    E-Print Network [OSTI]

    Hesteande, Blake E

    2014-01-27

    lipid oxidation as a free radical mediated phenomenon that deteriorates polyunsaturated fatty acids (PUFAs). These highly unstable free radicals also react with amino acids, heme groups in pigments, and vitamins with conjugated double bonds, forming...., 2001). However, with the increase in the amount of unsaturated fatty acids, there is a greater possibility for lipid oxidation to occur. There are several ways to minimize lipid oxidation, some of which involve animal feeding (Decker and Xu, 1998...

  17. Vibrational assignment and FranckCondon analysis of the mass-analyzed threshold ionization ,,MATI... spectrum of CH2ClI: The effect of strong

    E-Print Network [OSTI]

    Kim, Myung Soo

    to a high l and high ml state, which is usually called a ZEKE state. Then, application of electric radiation generated by four-wave mixing is getting popular.9­11 Recently, we reported the one-photon MATI spectrum of CH2ClI.12 The vibrational fundamentals of CH2ClI+ could be readily identified simply

  18. The determination of phase relations in the CH?-H?O-NaCl system at 2 and 5 kbars, 300 to 600° C using synthetic fluid inclusions 

    E-Print Network [OSTI]

    McShane, Christopher Joseph

    1999-01-01

    Fluid inclusions were synthesized, using quartz and fluorite as host minerals, to determine the phase relations of the CH?-H?O-NaCl system at pressures of 2 and 5 kbars and temperatures of 300, 400, 500, and 600°C . Known quantities of CH?, H?O...

  19. Effects of Collision and Vibrational Energy on the Reaction of CH3CHO+() with C2D4 Ho-Tae Kim, Jianbo Liu, and Scott L. Anderson*

    E-Print Network [OSTI]

    Anderson, Scott L.

    , we calculated the structures and energetics of 13 different complexes that potentially could serve vibrational state. REMPI through different vibrational levels of the B~ electronic state is used to produce CH dynamics with increasing energy. For the CH3CHO+- C2H4 system, there is an important direct mechanism even

  20. CH O Hydrogen Bonds at Protein-Protein Interfaces*S Received for publication, May 8, 2002, and in revised form, July 8, 2002

    E-Print Network [OSTI]

    Luhua, Lai

    CH O Hydrogen Bonds at Protein-Protein Interfaces*S Received for publication, May 8, 2002, a statistical potential has been de- veloped to quantitatively describe the CH O hydrogen bonding interaction-protein interaction studies. The conventional hydrogen bonds of the type X­H Y (where X and Y N or O) have been widely

  1. Quantum cascade laser investigations of CH4 and C2H2 interconversion in hydrocarbon/H2 gas mixtures during microwave plasma

    E-Print Network [OSTI]

    Bristol, University of

    Quantum cascade laser investigations of CH4 and C2H2 interconversion in hydrocarbon/H2 gas mixtures, Russia Received 31 July 2008; accepted 19 June 2009; published online 5 August 2009 CH4 and C2H2 molecules and their interconversion in hydrocarbon/rare gas/H2 gas mixtures in a microwave reactor used

  2. SCHOOL OF CHEMICAL & BIOMOLECULAR ENGINEERING, GEORGIA INSTITUTE OF TECHNOLOGY Checklist of Required and Recommended Safety Training for ChBE Researchers

    E-Print Network [OSTI]

    Gallivan, Martha A.

    training module completion records/certificates. · Faculty/PIs: It is recommended that you request the two modules on Receiving and Making Shipments. ____ Required: Fire Safety Training Online: http://www.ehs.gatech.edu/fire/fire_training of Required and Recommended Safety Training for ChBE Researchers · "ChBE Researcher" refers to any researcher

  3. Crossed beam studies of the reactions:O(3P,1D) + CH Direct evidence of intersystem crossing

    E-Print Network [OSTI]

    Nijmegen, University of

    on the triplet potential energy surface with rebound dynamics and via a long-lived complex mechanism following experiments with a rotating mass] CH 3 I spectrometer detector at collision energies of 55.2 and 64.0 kJ mol~1. The center of mass product angular and translational energy distributions for both the O(3P) and O(1D

  4. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    the equilibrium from having zero net current. 1 #12;I. INTRODUCTION Helically symmetric MHD equilibria represent of a current. This allows conventional stellarator equilibria to have zero net current in each flux surfacePREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA

  5. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA. Availability This report is posted on the U.S. Department of Energy's Princeton Plasma Physics Laboratory Publications and Reports web site in Fiscal Year 2003. The home page for PPPL Reports and Publications is: http

  6. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    , translation properties, and high plasma beta1,2 . One of the most important issues is FRC stabilityPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA agency thereof. Availability This report is posted on the U.S. Department of Energy's Princeton Plasma

  7. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    -Reversed Configuration (FRC) is a compact toroid with negligible toroidal field, in which plasma is confined fusion reactor potential of the FRC (compact and simple geometry, translation properties and high plasmaPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA

  8. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA Acceleration in the Field-reversed Configuration (FRC) by Slowly Rotating Odd-parity Magnetic Fields (RMFo agency thereof. Availability This report is posted on the U.S. Department of Energy's Princeton Plasma

  9. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    properties, and high plasma beta. One of the most important is- sues is FRC stability with respect to low] to investigate a variety of non-ideal MHD effects, including plasma flow and kinetic effects on FRC stabilityPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA

  10. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    carried by the plasma. It has been known for some time that a MHD model of the FRC is unstable to manyPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA on the U.S. Department of Energy's Princeton Plasma Physics Laboratory Publications and Reports web site

  11. Ligand-Enabled Catalytic C–H Arylation of Aliphatic Amines via a Four Membered Ring Cyclopalladation Pathway

    E-Print Network [OSTI]

    He, Chuan; Gaunt, Matthew J.

    2015-01-01

    A palladium-catalyzed C–H arylation of aliphatic amines with arylboronic esters is described via a four membered ring cyclopalladation pathway. Crucial to the successful outcome of this reaction is the action of an amino acid derived ligand. A range...

  12. CH(A-X) and OH(A-X) Optical Emission in an Axisymmetric Laminar Diffusion Flame

    E-Print Network [OSTI]

    Long, Marshall B.

    CH(A-X) and OH(A-X) Optical Emission in an Axisymmetric Laminar Diffusion Flame J. LUQUE, J. B an axisymmetric laminar diffusion flame [K. T. Walsh, M. B. Long, M. A. Tanoff, and M. D. Smooke, Twenty axisymmetric laminar methane/air diffusion flame studied here has been exten- sively characterized both

  13. Physical and chemical properties of dust produced in a N{sub 2}-CH{sub 4} RF plasma discharge

    SciTech Connect (OSTI)

    Ouni, F.; Alcouffe, G.; Szopa, C.; Carrasco, N.; Cernogora, G.; Adande, G.; Thissen, R.; Quirico, E.; Brissaud, O.; Schmitz-Afonso, I.; Laprevote, O.

    2008-09-07

    Titan's atmospheric chemistry is simulated using a Capacitively Coupled Plasma discharge produced in a N{sub 2}-CH{sub 4} mixture. The produced solid particles are analysed ex-situ. Chemical properties are deduced from: elemental composition, FTIR and LTQ-Orbitrap mass spectrometer. Optical properties are deduced from reflectivity in visible and IR range.

  14. TpPt(IV)Me(H)2 Forms a -CH4 Complex That Is Kinetically Resistant to Methane Liberation

    E-Print Network [OSTI]

    Keinan, Ehud

    TpPt(IV)Me(H)2 Forms a -CH4 Complex That Is Kinetically Resistant to Methane Liberation H demonstra- tion that methane can be catalytically activated by an organometallic complex of Pt(II).2 report that although 1 has a very high energy barrier for the liberation of methane, it readily forms

  15. 1/4Peter Debye Nobelpreis fr Chemie 1936www.nobelpreis.uzh.ch/debye.html traditionellen Frhlingsfest, dem Sech-

    E-Print Network [OSTI]

    Zürich, Universität

    1/4Peter Debye ­ Nobelpreis für Chemie 1936www.nobelpreis.uzh.ch/debye.html traditionellen Moleküle gibt, die permanente elektri- sche Dipole sind. Das «Dipolmoment» Nobelpreis für Chemie 1936 «für für Chemie 1936 Der Leonardo der Physik April 1914: Mit grossen Feierlichkei- ten eröffnet die

  16. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    per pulse. The pulse energy is limited by the thermal damage to the compression gratings which becomePREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does

  17. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    of looking at ions in both the thermal and suprathermal energy ranges, neutron detectors, and a Faraday cupPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does

  18. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA Propagation and Absorption in Plasmas with Non-thermal Populations by R.J. Dumont, C.K. Phillips, and D specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does

  19. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA PHYSICS LABORATORY PRINCETON UNIVERSITY, PRINCETON, NEW JERSEY PPPL-3698 PPPL-3698 UC-70 Thermal Response by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its

  20. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    in that they "channel" energy from the fast ion population to the thermal ion population [3] (rather than the thermalPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA, manufacturer, or otherwise, does not necessarily constitute or imply its endorsement, recommendation

  1. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA Conversion of Thermal Electron Bernstein Waves to the Extraordinary Electromagnetic Mode on the National specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does

  2. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    laser pulses [2, 3] with up to 500 J per pulse. The pulse energy is limited by the thermal damagePREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does

  3. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    provide a mechanism for direct energy trans- fer from super-Alfv´enic beam ions to thermal ions [3PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does

  4. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA PHYSICS LABORATORY PRINCETON UNIVERSITY, PRINCETON, NEW JERSEY PPPL-3790 PPPL-3790 UC-70 Truncated Thermal commercial product, process, or service by trade name, trademark, manufacturer, or otherwise, does

  5. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA of the Effect of Compressional Alfvén Modes on Thermal Transport in the National Spherical Torus Experiment by E by trade name, trademark, manufacturer, or otherwise, does not necessarily constitute or imply its

  6. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    elds: di usion | methods: analytical | plasmas 1. Introduction The problem of thermal conductionPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA on the U.S. Department of Energy's Princeton Plasma Physics Laboratory Publications and Reports web site

  7. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    a practical reality ­ an alternative energy source. The Year 2000 marked the second year of National SphericalPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA on the U.S. Department of Energy's Princeton Plasma Physics Laboratory Publications and Reports web site

  8. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    alternative for measuring the energy of fast escaping neutrals when the high-energy ion component producedPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA on the U.S. Department of Energy's Princeton Plasma Physics Laboratory Publications and Reports web site

  9. Communication: Spectroscopic characterization of an alkyl substituted Criegee intermediate syn-CH{sub 3}CHOO through pure rotational transitions

    SciTech Connect (OSTI)

    Nakajima, Masakazu; Endo, Yasuki

    2014-01-07

    An alkyl-substituted Criegee intermediate syn-CH{sub 3}CHOO was detected in the gas phase through Fourier-transform microwave spectroscopy. Observed pure rotational transitions show a small splitting corresponding to the A/E components due to the threefold methyl internal rotation. The rotational constants and the barrier height of the hindered methyl rotation were determined to be A = 17?586.5295(15) MHz, B = 7133.4799(41) MHz, C = 5229.1704(40) MHz, and V{sub 3} = 837.1(17) cm{sup ?1}. High-level ab initio calculations which reproduce the experimentally determined values well indicate that the in-plane C–H bond in the methyl moiety is trans to the C–O bond, and other two protons are directed to the terminal oxygen atom for the most stable structure of syn-CH{sub 3}CHOO. The torsional barrier of the methyl top is fairly large in syn-CH{sub 3}CHOO, implying a significant interaction between the terminal oxygen and the protons of the methyl moiety, which may be responsible for the high production yields of the OH radical from energized alkyl-substituted Criegee intermediates.

  10. Hydroxylation of Methane by Non-Heme Diiron Enzymes: Molecular Orbital Analysis of C-H Bond Activation by

    E-Print Network [OSTI]

    Gherman, Benjamin F.

    Hydroxylation of Methane by Non-Heme Diiron Enzymes: Molecular Orbital Analysis of C-H Bond, 2002 Abstract: The electronic structures of key species involved in methane hydroxylation performed that govern the details of the hydroxylation. Introduction The selective catalytic hydroxylation of methane

  11. Role of hydrogen-bonding and its interplay with octahedral tilting in CH3NH3PbI3

    E-Print Network [OSTI]

    Lee, Jung-Hoon; Bristowe, Nicholas C.; Bristowe, Paul D.; Cheetham, Anthony K.

    2015-03-05

    First principles calculations on the hybrid perovskite CH3NH3PbI3 predict strong hydrogen-bonding which influences the structure and dynamics of the methylammonium cation and reveal its interaction with the tilting of the PbI6 octahedra...

  12. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA on the U.S. Department of Energy's Princeton Plasma Physics Laboratory Publications and Reports web site and DOE Contractors can obtain copies of this report from: U.S. Department of Energy Office of Scientific

  13. Gibbs and Helmholtz energies of formation of sI clathrate hydrates from CO$_2$, CH$_4$ and water

    E-Print Network [OSTI]

    K. S. Glavatskiy; T. J. H. Vlugt; S. Kjelstrup

    2013-07-26

    We determine thermodynamic stability conditions in terms of Helmholtz and Gibbs energies for sI clathrate hydrates with CH$_4$ and CO$_2$ at 278 K. Helmholtz energies are relevant for processing from porous rocks (constant volume), while Gibbs energies are relevant for processing from layers on the ocean floor (constant pressure). We define three steps leading to hydrate formation, and find Helmholtz energy differences from molecular simulations for two of them using grand-canonical Monte Carlo simulations at constant temperature and volume; while the third step was calculated from literature data. The Gibbs energy change for the same steps are also determined. From the variations in the total Helmholtz and Gibbs energies we suggest thermodynamic paths for exchange of CH$_4$ by CO$_2$ in the isothermal hydrate, for constant volume or pressure, respectively. We show how these paths for the mixed hydrate can be understood from single-component occupancy isotherms, where CO$_2$, but not CH$_4$, can distinguish between large and small cages. The strong preference for CH$_4$ for a range of compositions can be explained by these.

  14. Ultralow Absorption Coefficient and Temperature Dependence of Radiative Recombination of CH3NH3PbI3 Perovskite from

    E-Print Network [OSTI]

    Perovskite from Photoluminescence Chog Barugkin, Jinjin Cong, The Duong, Shakir Rahman, Hieu T. Nguyen perovskite methylammonium lead iodide (CH3NH3PbI3) films from 675 to 1400 nm. Unlike other methods used of organic-inorganic halide perovskite- based solar cells has attracted enormous interest from the entire PV

  15. Theoretical Study of Mechanism and Selectivity of Copper-Catalyzed C-H Bond Amidation of Indoles

    E-Print Network [OSTI]

    Liao, Rongzhen

    Theoretical Study of Mechanism and Selectivity of Copper-Catalyzed C-H Bond Amidation of Indoles theory calculations are used to study the reaction mechanism and origins of C2 selectivity in a copper the observed regioselectivity. Instead, an unprecedented mechanism based on a four-center reductive elimination

  16. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    ]) is a data acquisition and storage system used at several fusion facilities world-wide. The majorityPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA on the U.S. Department of Energy's Princeton Plasma Physics Laboratory Publications and Reports web site

  17. Mixing, Lyapunov instability, and the approach to equilibrium in a hard-sphere gas Ch. Dellago and H. A. Posch

    E-Print Network [OSTI]

    Dellago, Christoph

    Mixing, Lyapunov instability, and the approach to equilibrium in a hard-sphere gas Ch. Dellago, Austria Received 31 July 1996 We present maximum Lyapunov exponents 1 and related Kolmogorov time of a one-particle distribution. At low densities the Lyapunov time 1/ 1 is much smaller than

  18. THE FORMATION OF ACETIC ACID (CH3COOH) IN INTERSTELLAR ICE ANALOGS Chris J. Bennett and Ralf I. Kaiser

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    Kaiser, Ralf I.

    THE FORMATION OF ACETIC ACID (CH3COOH) IN INTERSTELLAR ICE ANALOGS Chris J. Bennett and Ralf I, 1195, 1160, 1051, and 957 cmÀ1 ; two dimeric forms of acetic acid were assigned via absorptions at 1757 of the col- umn densities of the acetic acid molecule suggest that the initial step of the formation process

  19. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

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    production in hydrogen ion sources) a negative chlorine current density of 45 mA/cm2 was obtained underPREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA agency thereof. Availability This report is posted on the U.S. Department of Energy's Princeton Plasma

  20. PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073

    E-Print Network [OSTI]

    PREPARED FOR THE U.S. DEPARTMENT OF ENERGY, UNDER CONTRACT DE-AC02-76CH03073 PRINCETON PLASMA (Princeton, NJ USA) and the Max-Planck-Institut für Plasmaphysik, (Garching, Germany)and the Max-Planck-Institut für Plasmaphysik, (Garching, Germany)and the Max-Planck-Institut für Plasmaphysik, (Garching, Germany