Sample records for deformation energy released

  1. Dike propagation energy balance from deformation modeling and seismic release

    NASA Astrophysics Data System (ADS)

    Bonaccorso, Alessandro; Aoki, Yosuke; Rivalta, Eleonora

    2017-06-01

    Magma is transported in the crust mainly by dike intrusions. In volcanic areas, dikes can ascend toward the free surface and also move by lateral propagation, eventually feeding flank eruptions. Understanding dike mechanics is a key to forecasting the expected propagation and associated hazard. Several studies have been conducted on dike mechanisms and propagation; however, a less in-depth investigated aspect is the relation between measured dike-induced deformation and the seismicity released during its propagation. We individuated a simple x that can be used as a proxy of the expected mechanical energy released by a propagating dike and is related to its average thickness. For several intrusions around the world (Afar, Japan, and Mount Etna), we correlate such mechanical energy to the seismic moment released by the induced earthquakes. We obtain an empirical law that quantifies the expected seismic energy released before arrest. The proposed approach may be helpful to predict the total seismic moment that will be released by an intrusion and thus to control the energy status during its propagation and the time of dike arrest.Plain Language SummaryDike propagation is a dominant mechanism for magma ascent, transport, and eruptions. Besides being an intriguing physical process, it has critical hazard implications. After the magma intrusion starts, it is difficult to predict when and where a specific horizontal dike is going to halt and what its final length will be. In our study, we singled an equation that can be used as a proxy of the expected mechanical <span class="hlt">energy</span> to be <span class="hlt">released</span> by the opening dike. We related this expected <span class="hlt">energy</span> to the seismic moment of several eruptive intrusions around the world (Afar region, Japanese volcanoes, and Mount Etna). The proposed novel approach is helpful to estimate the total seismic moment to be <span class="hlt">released</span>, therefore allowing potentially predicting when the dike will end its propagation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR41B2704B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR41B2704B"><span>Real-time noble gas <span class="hlt">release</span> signaling rock <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bauer, S. J.; Gardner, W. P.; Lee, H.</p> <p>2016-12-01</p> <p>We present empirical results/relationships of rock strain, microfracture density, acoustic emissions, and noble gas <span class="hlt">release</span> from laboratory triaxial experiments for a granite and basalt. Noble gases are contained in most crustal rock at inter/intra granular sites, their <span class="hlt">release</span> during natural and manmade stress and strain changes represents a signal of brittle/semi brittle <span class="hlt">deformation</span>. The gas composition depends on lithology, geologic history and age, fluids present, and uranium, thorium and potassium-40 concentrations in the rocks that affect radiogenic noble gases (helium, argon) production. Noble gas emission and its relationship to crustal processes have been studied, including correlations to tectonic velocities and qualitative estimates of deep permeability from surface measurements, finger prints of nuclear weapon detonation, and as potential precursory signals to earthquakes attributed to gas <span class="hlt">release</span> due to pre-seismic stress, dilatancy and/or rock fracturing. Helium emission has been shown as a precursor of volcanic activity. Real-time noble gas <span class="hlt">release</span> is observed using an experimental system utilizing mass spectrometers to measure gases <span class="hlt">released</span> during triaxial rock <span class="hlt">deformation</span>. Noble gas <span class="hlt">release</span> is shown to represent a sensitive precursor signal of rock <span class="hlt">deformation</span> by relating real-time noble gas <span class="hlt">release</span> to stress-strain state changes and acoustic emissions. We propose using noble gas <span class="hlt">release</span> to also signal rock <span class="hlt">deformation</span> in boreholes, mines and nuclear waste repositories. We postulate each rock exhibits a gas <span class="hlt">release</span> signature which is microstructure, stress/strain state, and or permanent <span class="hlt">deformation</span> dependent. Such relationships, when calibrated, may be used to sense rock <span class="hlt">deformation</span> and then develop predictive models. Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation, a wholly owned subsidiary of Lockheed Martin Corp., for the US Dept. of <span class="hlt">Energy</span>'s National Nuclear Security Administration under</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1418467-helium-release-during-shale-deformation-experimental-validation','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1418467-helium-release-during-shale-deformation-experimental-validation"><span>Helium <span class="hlt">release</span> during shale <span class="hlt">deformation</span>: Experimental validation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Bauer, Stephen J.; Gardner, W. Payton; Heath, Jason E.</p> <p>2016-07-01</p> <p>This paper describes initial experimental results of helium tracer <span class="hlt">release</span> monitoring during <span class="hlt">deformation</span> of shale. Naturally occurring radiogenic 4He is present in high concentration in most shales. During rock <span class="hlt">deformation</span>, accumulated helium could be <span class="hlt">released</span> as fractures are created and new transport pathways are created. We present the results of an experimental study in which confined reservoir shale samples, cored parallel and perpendicular to bedding, which were initially saturated with helium to simulate reservoir conditions, are subjected to triaxial compressive <span class="hlt">deformation</span>. During the <span class="hlt">deformation</span> experiment, differential stress, axial, and radial strains are systematically tracked. <span class="hlt">Release</span> of helium is dynamically measuredmore » using a helium mass spectrometer leak detector. Helium <span class="hlt">released</span> during <span class="hlt">deformation</span> is observable at the laboratory scale and the <span class="hlt">release</span> is tightly coupled to the shale <span class="hlt">deformation</span>. These first measurements of dynamic helium <span class="hlt">release</span> from rocks undergoing <span class="hlt">deformation</span> show that helium provides information on the evolution of microstructure as a function of changes in stress and strain.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1380203','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1380203"><span>Gas <span class="hlt">Release</span> as a <span class="hlt">Deformation</span> Signal</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Bauer, Stephen J.</p> <p></p> <p>Radiogenic noble gases are contained in crustal rock at inter and intra granular sites. The gas composition depends on lithology, geologic history, fluid phases, and the aging effect by decay of U, Th, and K. The isotopic signature of noble gases found in rocks is vastly different than that of the atmosphere which is contributed by a variety of sources. When rock is subjected to stress conditions exceeding about half its yield strength, micro-cracks begin to form. As rock <span class="hlt">deformation</span> progresses a fracture network evolves, <span class="hlt">releasing</span> trapped noble gases and changing the transport properties to gas migration. Thus, changes inmore » gas emanation and noble gas composition from rocks could be used to infer changes in stress-state and <span class="hlt">deformation</span>. The purpose of this study has been to evaluate the effect of <span class="hlt">deformation</span>/strain rate upon noble gas <span class="hlt">release</span>. Four triaxial experiments were attempted for a strain rate range of %7E10-8 /s (180,000s) to %7E 10-4/s (500s); the three fully successful experiments (at the faster strain rates) imply the following: (1) helium is measurably <span class="hlt">released</span> for all strain rates during <span class="hlt">deformation</span>, this <span class="hlt">release</span> is in amounts 1-2 orders of magnitude greater than that present in the air, and (2) helium gas <span class="hlt">release</span> increases with decreasing strain rate.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1411603-modeling-dynamic-helium-release-tracer-rock-deformation','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1411603-modeling-dynamic-helium-release-tracer-rock-deformation"><span>Modeling Dynamic Helium <span class="hlt">Release</span> as a Tracer of Rock <span class="hlt">Deformation</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Gardner, W. Payton; Bauer, Stephen J.; Kuhlman, Kristopher L.; ...</p> <p>2017-11-03</p> <p>Here, we use helium <span class="hlt">released</span> during mechanical <span class="hlt">deformation</span> of shales as a signal to explore the effects of <span class="hlt">deformation</span> and failure on material transport properties. A dynamic dual-permeability model with evolving pore and fracture networks is used to simulate gases <span class="hlt">released</span> from shale during <span class="hlt">deformation</span> and failure. Changes in material properties required to reproduce experimentally observed gas signals are explored. We model two different experiments of 4He flow rate measured from shale undergoing mechanical <span class="hlt">deformation</span>, a core parallel to bedding and a core perpendicular to bedding. We also found that the helium signal is sensitive to fracture development and evolutionmore » as well as changes in the matrix transport properties. We constrain the timing and effective fracture aperture, as well as the increase in matrix porosity and permeability. Increases in matrix permeability are required to explain gas flow prior to macroscopic failure, and the short-term gas flow postfailure. Increased matrix porosity is required to match the long-term, postfailure gas flow. This model provides the first quantitative interpretation of helium <span class="hlt">release</span> as a result of mechanical <span class="hlt">deformation</span>. The sensitivity of this model to changes in the fracture network, as well as to matrix properties during <span class="hlt">deformation</span>, indicates that helium <span class="hlt">release</span> can be used as a quantitative tool to evaluate the state of stress and strain in earth materials.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1411603-modeling-dynamic-helium-release-tracer-rock-deformation','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1411603-modeling-dynamic-helium-release-tracer-rock-deformation"><span>Modeling Dynamic Helium <span class="hlt">Release</span> as a Tracer of Rock <span class="hlt">Deformation</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gardner, W. Payton; Bauer, Stephen J.; Kuhlman, Kristopher L.</p> <p></p> <p>Here, we use helium <span class="hlt">released</span> during mechanical <span class="hlt">deformation</span> of shales as a signal to explore the effects of <span class="hlt">deformation</span> and failure on material transport properties. A dynamic dual-permeability model with evolving pore and fracture networks is used to simulate gases <span class="hlt">released</span> from shale during <span class="hlt">deformation</span> and failure. Changes in material properties required to reproduce experimentally observed gas signals are explored. We model two different experiments of 4He flow rate measured from shale undergoing mechanical <span class="hlt">deformation</span>, a core parallel to bedding and a core perpendicular to bedding. We also found that the helium signal is sensitive to fracture development and evolutionmore » as well as changes in the matrix transport properties. We constrain the timing and effective fracture aperture, as well as the increase in matrix porosity and permeability. Increases in matrix permeability are required to explain gas flow prior to macroscopic failure, and the short-term gas flow postfailure. Increased matrix porosity is required to match the long-term, postfailure gas flow. This model provides the first quantitative interpretation of helium <span class="hlt">release</span> as a result of mechanical <span class="hlt">deformation</span>. The sensitivity of this model to changes in the fracture network, as well as to matrix properties during <span class="hlt">deformation</span>, indicates that helium <span class="hlt">release</span> can be used as a quantitative tool to evaluate the state of stress and strain in earth materials.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26733653','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26733653"><span>Correcting <span class="hlt">deformity</span> in total knee arthroplasty: Techniques to avoid the <span class="hlt">release</span> of collateral ligaments in severely <span class="hlt">deformed</span> knees.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mullaji, A B; Shetty, G M</p> <p>2016-01-01</p> <p>Collateral ligament <span class="hlt">release</span> is advocated in total knee arthroplasty (TKA) to deal with significant coronal plane <span class="hlt">deformities</span>, but is also associated with significant disadvantages. We describe steps to avoid <span class="hlt">release</span> of the collateral (superficial medial and lateral collateral) ligaments during TKA in severely <span class="hlt">deformed</span> knees, while correcting <span class="hlt">deformity</span> and balancing the knee. ©2016 The British Editorial Society of Bone & Joint Surgery.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1418468','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1418468"><span><span class="hlt">Release</span> of radiogenic noble gases as a new signal of rock <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Bauer, Stephen J.; Gardner, W. Payton; Lee, Hyunwoo</p> <p></p> <p>In this paper we investigate the <span class="hlt">release</span> of radiogenic noble gas isotopes during mechanical <span class="hlt">deformation</span>. We developed an analytical system for dynamic mass spectrometry of noble gas composition and helium <span class="hlt">release</span> rate of gas produced during mechanical <span class="hlt">deformation</span> of rocks. Our results indicate that rocks <span class="hlt">release</span> accumulated radiogenic helium and argon from mineral grains as they undergo <span class="hlt">deformation</span>. We found that the <span class="hlt">release</span> of accumulated 4He and 40Ar from rocks follows a reproducible pattern and can provide insight into the <span class="hlt">deformation</span> process. Increased gas <span class="hlt">release</span> can be observed before dilation, and macroscopic failure is observed during high-pressure triaxial rock deformationmore » experiments. Accumulated radiogenic noble gases can be <span class="hlt">released</span> due to fracturing of mineral grains during small-scale strain in Earth materials. Helium and argon are highly mobile, conservative species and could be used to provide information on changes in the state of stress and strain in Earth materials, and as an early warning signal of macroscopic failure. These results pave the way for the use of noble gases to trace and monitor rock <span class="hlt">deformation</span> for earthquake prediction and a variety of other subsurface engineering projects.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1418468-release-radiogenic-noble-gases-new-signal-rock-deformation','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1418468-release-radiogenic-noble-gases-new-signal-rock-deformation"><span><span class="hlt">Release</span> of radiogenic noble gases as a new signal of rock <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Bauer, Stephen J.; Gardner, W. Payton; Lee, Hyunwoo</p> <p>2016-10-09</p> <p>In this paper we investigate the <span class="hlt">release</span> of radiogenic noble gas isotopes during mechanical <span class="hlt">deformation</span>. We developed an analytical system for dynamic mass spectrometry of noble gas composition and helium <span class="hlt">release</span> rate of gas produced during mechanical <span class="hlt">deformation</span> of rocks. Our results indicate that rocks <span class="hlt">release</span> accumulated radiogenic helium and argon from mineral grains as they undergo <span class="hlt">deformation</span>. We found that the <span class="hlt">release</span> of accumulated 4He and 40Ar from rocks follows a reproducible pattern and can provide insight into the <span class="hlt">deformation</span> process. Increased gas <span class="hlt">release</span> can be observed before dilation, and macroscopic failure is observed during high-pressure triaxial rock deformationmore » experiments. Accumulated radiogenic noble gases can be <span class="hlt">released</span> due to fracturing of mineral grains during small-scale strain in Earth materials. Helium and argon are highly mobile, conservative species and could be used to provide information on changes in the state of stress and strain in Earth materials, and as an early warning signal of macroscopic failure. These results pave the way for the use of noble gases to trace and monitor rock <span class="hlt">deformation</span> for earthquake prediction and a variety of other subsurface engineering projects.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21935538','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21935538"><span>Red blood cell dynamics: from cell <span class="hlt">deformation</span> to ATP <span class="hlt">release</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wan, Jiandi; Forsyth, Alison M; Stone, Howard A</p> <p>2011-10-01</p> <p>The mechanisms of red blood cell (RBC) <span class="hlt">deformation</span> under both static and dynamic, i.e., flow, conditions have been studied extensively since the mid 1960s. <span class="hlt">Deformation</span>-induced biochemical reactions and possible signaling in RBCs, however, were proposed only fifteen years ago. Therefore, the fundamental relationship between RBC <span class="hlt">deformation</span> and cellular signaling dynamics i.e., mechanotransduction, remains incompletely understood. Quantitative understanding of the mechanotransductive pathways in RBCs requires integrative studies of physical models of RBC <span class="hlt">deformation</span> and cellular biochemical reactions. In this article we review the physical models of RBC <span class="hlt">deformation</span>, spanning from continuum membrane mechanics to cellular skeleton dynamics under both static and flow conditions, and elaborate the mechanistic links involved in <span class="hlt">deformation</span>-induced ATP <span class="hlt">release</span>. This journal is © The Royal Society of Chemistry 2011</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22349292','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22349292"><span>The effects of membrane cholesterol and simvastatin on red blood cell <span class="hlt">deformability</span> and ATP <span class="hlt">release</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Forsyth, Alison M; Braunmüller, Susanne; Wan, Jiandi; Franke, Thomas; Stone, Howard A</p> <p>2012-05-01</p> <p>It is known that <span class="hlt">deformation</span> of red blood cells (RBCs) is linked to ATP <span class="hlt">release</span> from the cells. Further, membrane cholesterol has been shown to alter properties of the cell membrane such as fluidity and bending stiffness. Membrane cholesterol content is increased in some cardiovascular diseases, for example, in individuals with acute coronary syndromes and chronic stable angina, and therefore, because of the potential clinical relevance, we investigated the influence of altered RBC membrane cholesterol levels on ATP <span class="hlt">release</span>. Because of the correlation between statins and reduced membrane cholesterol in vivo, we also investigated the effects of simvastatin on RBC <span class="hlt">deformation</span> and ATP <span class="hlt">release</span>. We found that reducing membrane cholesterol increases cell <span class="hlt">deformability</span> and ATP <span class="hlt">release</span>. We also found that simvastatin increases <span class="hlt">deformability</span> by acting directly on the membrane in the absence of the liver, and that ATP <span class="hlt">release</span> was increased for cells with enriched cholesterol after treatment with simvastatin. Copyright © 2012 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ChJME..29.1167G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ChJME..29.1167G"><span>Dynamic soft tissue <span class="hlt">deformation</span> estimation based on <span class="hlt">energy</span> analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gao, Dedong; Lei, Yong; Yao, Bin</p> <p>2016-10-01</p> <p>The needle placement accuracy of millimeters is required in many needle-based surgeries. The tissue <span class="hlt">deformation</span>, especially that occurring on the surface of organ tissue, affects the needle-targeting accuracy of both manual and robotic needle insertions. It is necessary to understand the mechanism of tissue <span class="hlt">deformation</span> during needle insertion into soft tissue. In this paper, soft tissue surface <span class="hlt">deformation</span> is investigated on the basis of continuum mechanics, where a geometry model is presented to quantitatively approximate the volume of tissue <span class="hlt">deformation</span>. The <span class="hlt">energy</span>-based method is presented to the dynamic process of needle insertion into soft tissue based on continuum mechanics, and the volume of the cone is exploited to quantitatively approximate the <span class="hlt">deformation</span> on the surface of soft tissue. The external work is converted into potential, kinetic, dissipated, and strain <span class="hlt">energies</span> during the dynamic rigid needle-tissue interactive process. The needle insertion experimental setup, consisting of a linear actuator, force sensor, needle, tissue container, and a light, is constructed while an image-based method for measuring the depth and radius of the soft tissue surface <span class="hlt">deformations</span> is introduced to obtain the experimental data. The relationship between the changed volume of tissue <span class="hlt">deformation</span> and the insertion parameters is created based on the law of conservation of <span class="hlt">energy</span>, with the volume of tissue <span class="hlt">deformation</span> having been obtained using image-based measurements. The experiments are performed on phantom specimens, and an <span class="hlt">energy</span>-based analytical fitted model is presented to estimate the volume of tissue <span class="hlt">deformation</span>. The experimental results show that the <span class="hlt">energy</span>-based analytical fitted model can predict the volume of soft tissue <span class="hlt">deformation</span>, and the root mean squared errors of the fitting model and experimental data are 0.61 and 0.25 at the velocities 2.50 mm/s and 5.00 mm/s. The estimating parameters of the soft tissue surface <span class="hlt">deformations</span> are proven to be useful</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMNG23A1377S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMNG23A1377S"><span>Impact of methane flow through <span class="hlt">deformable</span> lake sediments on atmospheric <span class="hlt">release</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scandella, B.; Juanes, R.</p> <p>2010-12-01</p> <p>Methane is a potent greenhouse gas that is generated geothermally and biologically in lake and ocean sediments. Free gas bubbles may escape oxidative traps and contribute more to the atmospheric source than dissolved methane, but the details of the methane <span class="hlt">release</span> depend on the interactions between the multiple fluid phases and the <span class="hlt">deformable</span> porous medium. We present a model and supporting laboratory experiments of methane <span class="hlt">release</span> through “breathing” dynamic flow conduits that open in response to drops in the hydrostatic load on lake sediments, which has been validated against a high-resolution record of free gas flux and hydrostatic pressure in Upper Mystic Lake, MA. In contrast to previous linear elastic fracture mechanics analysis of gassy sediments, the evolution of gas transport in a <span class="hlt">deformable</span> compliant sediment is presented within the framework of multiphase poroplasticity. Experiments address how strongly the mode and rate of gas flow, captured by our model, impacts the size of bubbles <span class="hlt">released</span> into the water column. A bubble's size in turn determines how efficiently it transports methane to the atmosphere, and integrating this effect will be critical to improving estimates of the atmospheric methane source from lakes. Cross-sectional schematic of lake sediments showing two venting sites: one open at left and one closed at right. The vertical <span class="hlt">release</span> of gas bubbles (red) at the open venting site creates a local pressure drop, which drives both bubble formation from the methane-rich pore water (higher concentrations shaded darker red) and lateral advection of dissolved methane (purple arrows). Even as bubbles in the open site escape, those at the closed site remain trapped.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR51B2708M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR51B2708M"><span>Strain Rate Dependency of Fracture Toughness, <span class="hlt">Energy</span> <span class="hlt">Release</span> Rate and Geomechanical Attributes of Select Indian Shales</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mahanta, B.; Vishal, V.; Singh, T. N.; Ranjith, P.</p> <p>2016-12-01</p> <p>In addition to modern improved technology, it requires detailed understanding of rock fractures for the purpose of enhanced <span class="hlt">energy</span> extraction through hydraulic fracturing of gas shales and geothermal <span class="hlt">energy</span> systems. The understanding of rock fracture behavior, patterns and properties such as fracture toughness; <span class="hlt">energy</span> <span class="hlt">release</span> rate; strength and <span class="hlt">deformation</span> attributes during fracturing hold significance. Environmental factors like temperature, pressure, humidity, water vapor and experimental condition such as strain rate influence the estimation of these properties. In this study, the effects of strain rates on fracture toughness, <span class="hlt">energy</span> <span class="hlt">release</span> rate as well as geomechanical properties like uniaxial compressive strength, Young's modulus, failure strain, tensile strength, and brittleness index of gas shales were investigated. In addition to the rock-mechanical parameters, the fracture toughness and the <span class="hlt">energy</span> <span class="hlt">release</span> rates were measured for three different modes viz. mode I, mixed mode (I-II) and mode II. Petrographic and X-ray diffraction (XRD) analyses were performed to identify the mineral composition of the shale samples. Scanning electron microscope (SEM) analyses were conducted to have an insight about the strain rate effects on micro-structure of the rock. The results suggest that the fracture toughness; the <span class="hlt">energy</span> <span class="hlt">release</span> rate as well as other geomechanical properties are a function of strain rates. At high strain rates, the strength and stiffness of shale increases which in turn increases the fracture toughness and the <span class="hlt">energy</span> <span class="hlt">release</span> rate of shale that may be due to stress redistribution during grain fracturing. The fracture toughness and the strain <span class="hlt">energy</span> <span class="hlt">release</span> rates for all the modes (I/I-II/II) are comparable at lower strain rates, but they vary considerably at higher strain rates. In all the cases, mode I and mode II fracturing requires minimum and maximum applied <span class="hlt">energy</span>, respectively. Mode I <span class="hlt">energy</span> <span class="hlt">release</span> rate is maximum, compared to the other modes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950038652&hterms=Free+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DFree%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950038652&hterms=Free+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DFree%2Benergy"><span><span class="hlt">Energy</span> <span class="hlt">release</span> in solar flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Brown, John C.; Correia, Emilia; Farnik, Frantisek; Garcia, Howard; Henoux, Jean-Claude; La Rosa, Ted N.; Machado, Marcos E. (Compiler); Nakajima, Hiroshi; Priest, Eric R.</p> <p>1994-01-01</p> <p>Team 2 of the Ottawa Flares 22 Workshop dealt with observational and theoretical aspects of the characteristics and processes of <span class="hlt">energy</span> <span class="hlt">release</span> in flares. Main results summarized in this article stress the global character of the flaring phenomenon in active regions, the importance of discontinuities in magnetic connectivity, the role of field-aligned currents in free <span class="hlt">energy</span> storage, and the fragmentation of <span class="hlt">energy</span> <span class="hlt">release</span> in time and space.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR43D0492B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR43D0492B"><span>Noble Gas <span class="hlt">Release</span> Signal as a Precursor to Fracture</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bauer, S. J.; Lee, H.; Gardner, W. P.</p> <p>2017-12-01</p> <p>We present empirical results of rock strain, microfracturing, acoustic emissions, and noble gas <span class="hlt">release</span> from laboratory triaxial experiments for a granite, basalt, shale and bedded rock salt. Noble gases are <span class="hlt">released</span> and measured real-time during <span class="hlt">deformation</span> using mass spectrometry. The gas <span class="hlt">release</span> represents a precursive signal to macrofracture. Gas <span class="hlt">release</span> is associated with increased acoustic emissions indicating that microfracturing is required to <span class="hlt">release</span> gas and create pathways for the gas to be sensed. The gas <span class="hlt">released</span> depends on initial gas content, pore structure and its evolution during <span class="hlt">deformation</span>, the <span class="hlt">deformation</span> amount, matrix permeability, <span class="hlt">deformation</span> style and the stress/strain history. Gases are <span class="hlt">released</span> from inter and intracrystalline sites; <span class="hlt">release</span> rate increases as strain and microfracturing increases. The gas composition depends on lithology, geologic history and age, fluids present, and radioisotope concentrations that affect radiogenic noble gas isotope (e.g. 4He,40Ar) production. Noble gas emission and its relationship to crustal processes such as seismicity and volcanism, tectonic velocities, qualitative estimates of deep permeability, age dating of groundwater, and a signature of nuclear weapon detonation. Our result show that mechanical <span class="hlt">deformation</span> of crustal materials is an important process controlling gas <span class="hlt">release</span> from rocks and minerals, and should be considered in techniques which utilize gas <span class="hlt">release</span> and/or accumulation. We propose using noble gas <span class="hlt">release</span> to signal rock <span class="hlt">deformation</span> in boreholes, mines and waste repositories. We postulate each rock exhibits a gas <span class="hlt">release</span> signature which is microstructure, stress, strain, and/or permanent <span class="hlt">deformation</span> dependent. Calibration of such relationships, for example relating gas <span class="hlt">release</span> per rock unit volume to strain may be used to quantify rock <span class="hlt">deformation</span> and develop predictive models.Sandia National Laboratories is a multimission laboratory managed and operated by National Technology and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27852845','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27852845"><span>Honey Bee <span class="hlt">Deformed</span> Wing Virus Structures Reveal that Conformational Changes Accompany Genome <span class="hlt">Release</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Organtini, Lindsey J; Shingler, Kristin L; Ashley, Robert E; Capaldi, Elizabeth A; Durrani, Kulsoom; Dryden, Kelly A; Makhov, Alexander M; Conway, James F; Pizzorno, Marie C; Hafenstein, Susan</p> <p>2017-01-15</p> <p>The picornavirus-like <span class="hlt">deformed</span> wing virus (DWV) has been directly linked to colony collapse; however, little is known about the mechanisms of host attachment or entry for DWV or its molecular and structural details. Here we report the three-dimensional (3-D) structures of DWV capsids isolated from infected honey bees, including the immature procapsid, the genome-filled virion, the putative entry intermediate (A-particle), and the empty capsid that remains after genome <span class="hlt">release</span>. The capsids are decorated by large spikes around the 5-fold vertices. The 5-fold spikes had an open flower-like conformation for the procapsid and genome-filled capsids, whereas the putative A-particle and empty capsids that had <span class="hlt">released</span> the genome had a closed tube-like spike conformation. Between the two conformations, the spikes undergo a significant hinge-like movement that we predicted using a Robetta model of the structure comprising the spike. We conclude that the spike structures likely serve a function during host entry, changing conformation to <span class="hlt">release</span> the genome, and that the genome may escape from a 5-fold vertex to initiate infection. Finally, the structures illustrate that, similarly to picornaviruses, DWV forms alternate particle conformations implicated in assembly, host attachment, and RNA <span class="hlt">release</span>. Honey bees are critical for global agriculture, but dramatic losses of entire hives have been reported in numerous countries since 2006. <span class="hlt">Deformed</span> wing virus (DWV) and infestation with the ectoparasitic mite Varroa destructor have been linked to colony collapse disorder. DWV was purified from infected adult worker bees to pursue biochemical and structural studies that allowed the first glimpse into the conformational changes that may be required during transmission and genome <span class="hlt">release</span> for DWV. Copyright © 2017 American Society for Microbiology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018IJMPD..2750177D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018IJMPD..2750177D"><span>Time-varying q-<span class="hlt">deformed</span> dark <span class="hlt">energy</span> interacts with dark matter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dil, Emre; Kolay, Erdinç</p> <p></p> <p>We propose a new model for studying the dark constituents of the universe by regarding the dark <span class="hlt">energy</span> as a q-<span class="hlt">deformed</span> scalar field interacting with the dark matter, in the framework of standard general relativity. Here we assume that the number of particles in each mode of the q-<span class="hlt">deformed</span> scalar field varies in time by the particle creation and annihilation. We first describe the q-<span class="hlt">deformed</span> scalar field dark <span class="hlt">energy</span> quantum-field theoretically, then construct the action and the dynamical structure of these interacting dark sectors, in order to study the dynamics of the model. We perform the phase space analysis of the model to confirm and interpret our proposal by searching the stable attractor solutions implying the late-time accelerating phase of the universe. We then obtain the result that when interaction and equation-of-state parameter of the dark matter evolve from the present day values into a particular value, the dark <span class="hlt">energy</span> turns out to be a q-<span class="hlt">deformed</span> scalar field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1035972','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1035972"><span>Building an Efficient Model for Afterburn <span class="hlt">Energy</span> <span class="hlt">Release</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Alves, S; Kuhl, A; Najjar, F</p> <p>2012-02-03</p> <p>Many explosives will <span class="hlt">release</span> additional <span class="hlt">energy</span> after detonation as the detonation products mix with the ambient environment. This additional <span class="hlt">energy</span> <span class="hlt">release</span>, referred to as afterburn, is due to combustion of undetonated fuel with ambient oxygen. While the detonation <span class="hlt">energy</span> <span class="hlt">release</span> occurs on a time scale of microseconds, the afterburn <span class="hlt">energy</span> <span class="hlt">release</span> occurs on a time scale of milliseconds with a potentially varying <span class="hlt">energy</span> <span class="hlt">release</span> rate depending upon the local temperature and pressure. This afterburn <span class="hlt">energy</span> <span class="hlt">release</span> is not accounted for in typical equations of state, such as the Jones-Wilkins-Lee (JWL) model, used for modeling the detonation of explosives. Here wemore » construct a straightforward and efficient approach, based on experiments and theory, to account for this additional <span class="hlt">energy</span> <span class="hlt">release</span> in a way that is tractable for large finite element fluid-structure problems. Barometric calorimeter experiments have been executed in both nitrogen and air environments to investigate the characteristics of afterburn for C-4 and other materials. These tests, which provide pressure time histories, along with theoretical and analytical solutions provide an engineering basis for modeling afterburn with numerical hydrocodes. It is toward this end that we have constructed a modified JWL equation of state to account for afterburn effects on the response of structures to blast. The modified equation of state includes a two phase afterburn <span class="hlt">energy</span> <span class="hlt">release</span> to represent variations in the <span class="hlt">energy</span> <span class="hlt">release</span> rate and an afterburn <span class="hlt">energy</span> cutoff to account for partial reaction of the undetonated fuel.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..44.6771L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..44.6771L"><span>Time lag between <span class="hlt">deformation</span> and seismicity along monogenetic volcanic unrest periods: The case of El Hierro Island (Canary Islands)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lamolda, Héctor; Felpeto, Alicia; Bethencourt, Abelardo</p> <p>2017-07-01</p> <p>Between 2011 and 2014 there were at least seven episodes of magmatic intrusion in El Hierro Island, but only the first one led to a submarine eruption in 2011-2012. In order to study the relationship between GPS <span class="hlt">deformation</span> and seismicity during these episodes, we compare the temporal evolution of the <span class="hlt">deformation</span> with the cumulative seismic <span class="hlt">energy</span> <span class="hlt">released</span>. In some of the episodes both <span class="hlt">deformation</span> and seismicity evolve in a very similar way, but in others a time lag appears between them, in which the <span class="hlt">deformation</span> precedes the seismicity. Furthermore, a linear correlation between decimal logarithm of intruded magma volume and decimal logarithm of total seismic <span class="hlt">energy</span> <span class="hlt">released</span> along the different episodes has been observed. Therefore, if a future magmatic intrusion in El Hierro Island follows this behavior with a proper time lag, we could have an a priori estimate on the order of magnitude the seismic <span class="hlt">energy</span> <span class="hlt">released</span> would reach.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li class="active"><span>1</span></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_1 --> <div id="page_2" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_1");'>1</a></li> <li class="active"><span>2</span></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="21"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23880119','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23880119"><span><span class="hlt">Energy</span> monitoring and analysis during <span class="hlt">deformation</span> of bedded-sandstone: use of acoustic emission.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wasantha, P L P; Ranjith, P G; Shao, S S</p> <p>2014-01-01</p> <p>This paper investigates the mechanical behaviour and <span class="hlt">energy</span> <span class="hlt">releasing</span> characteristics of bedded-sandstone with bedding layers in different orientations, under uniaxial compression. Cylindrical sandstone specimens (54 mm diameter and 108 mm height) with bedding layers inclined at angles of 10°, 20°, 35°, 55°, and 83° to the minor principal stress direction, were produced to perform a series of Uniaxial Compressive Strength (UCS) tests. One of the two identical sample sets was fully-saturated with water before testing and the other set was tested under dry conditions. An acoustic emission system was employed in all the testing to monitor the acoustic <span class="hlt">energy</span> <span class="hlt">release</span> during the whole <span class="hlt">deformation</span> process of specimens. From the test results, the critical joint orientation was observed as 55° for both dry and saturated samples and the peak-strength losses due to water were 15.56%, 20.06%, 13.5%, 13.2%, and 13.52% for the bedding orientations 10°, 20°, 35°, 55°, and 83°, respectively. The failure mechanisms for the specimens with bedding layers in 10°, 20° orientations showed splitting type failure, while the specimens with bedding layers in 55°, 83° orientations were failed by sliding along a weaker bedding layer. The failure mechanism for the specimens with bedding layers in 35° orientation showed a mixed failure mode of both splitting and sliding types. Analysis of the acoustic <span class="hlt">energy</span>, captured from the acoustic emission detection system, revealed that the acoustic <span class="hlt">energy</span> <span class="hlt">release</span> is considerably higher in dry specimens than that of the saturated specimens at any bedding orientation. In addition, higher <span class="hlt">energy</span> <span class="hlt">release</span> was observed for specimens with bedding layers oriented in shallow angles (which were undergoing splitting type failures), whereas specimens with steeply oriented bedding layers (which were undergoing sliding type failures) showed a comparatively less <span class="hlt">energy</span> <span class="hlt">release</span> under both dry and saturated conditions. Moreover, a considerable amount of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030062779','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030062779"><span>Quantification of <span class="hlt">Energy</span> <span class="hlt">Release</span> in Composite Structures</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Minnetyan, Levon</p> <p>2003-01-01</p> <p><span class="hlt">Energy</span> <span class="hlt">release</span> rate is usually suggested as a quantifier for assessing structural damage tolerance. Computational prediction of <span class="hlt">energy</span> <span class="hlt">release</span> rate is based on composite mechanics with micro-stress level damage assessment, finite element structural analysis and damage progression tracking modules. This report examines several issues associated with <span class="hlt">energy</span> <span class="hlt">release</span> rates in composite structures as follows: Chapter I demonstrates computational simulation of an adhesively bonded composite joint and validates the computed <span class="hlt">energy</span> <span class="hlt">release</span> rates by comparison with acoustic emission signals in the overall sense. Chapter II investigates the effect of crack plane orientation with respect to fiber direction on the <span class="hlt">energy</span> <span class="hlt">release</span> rates. Chapter III quantifies the effects of contiguous constraint plies on the residual stiffness of a 90 ply subjected to transverse tensile fractures. Chapter IV compares ICAN and ICAN/JAVA solutions of composites. Chapter V examines the effects of composite structural geometry and boundary conditions on damage progression characteristics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030006690','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030006690"><span>Quantification of <span class="hlt">Energy</span> <span class="hlt">Release</span> in Composite Structures</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Minnetyan, Levon; Chamis, Christos C. (Technical Monitor)</p> <p>2003-01-01</p> <p><span class="hlt">Energy</span> <span class="hlt">release</span> rate is usually suggested as a quantifier for assessing structural damage tolerance. Computational prediction of <span class="hlt">energy</span> <span class="hlt">release</span> rate is based on composite mechanics with micro-stress level damage assessment, finite element structural analysis and damage progression tracking modules. This report examines several issues associated with <span class="hlt">energy</span> <span class="hlt">release</span> rates in composite structures as follows: Chapter I demonstrates computational simulation of an adhesively bonded composite joint and validates the computed <span class="hlt">energy</span> <span class="hlt">release</span> rates by comparison with acoustic emission signals in the overall sense. Chapter II investigates the effect of crack plane orientation with respect to fiber direction on the <span class="hlt">energy</span> <span class="hlt">release</span> rates. Chapter III quantifies the effects of contiguous constraint plies on the residual stiffness of a 90 deg ply subjected to transverse tensile fractures. Chapter IV compares ICAN and ICAN/JAVA solutions of composites. Chapter V examines the effects of composite structural geometry and boundary conditions on damage progression characteristics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15307797','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15307797"><span><span class="hlt">Deformation</span>-induced <span class="hlt">release</span> of ATP from erythrocytes in a poly(dimethylsiloxane)-based microchip with channels that mimic resistance vessels.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Price, Alexander K; Fischer, David J; Martin, R Scott; Spence, Dana M</p> <p>2004-08-15</p> <p>The ability of nitric oxide to relax smooth muscle cells surrounding resistance vessels in vivo is well documented. Here, we describe a series of studies designed to quantify amounts of adenosine triphosphate (ATP), a known stimulus of NO production in endothelial cells, <span class="hlt">released</span> from erythrocytes that are mechanically <span class="hlt">deformed</span> as these cells traverse microbore channels in lithographically patterned microchips. Results indicate that micromolar amounts of ATP are <span class="hlt">released</span> from erythrocytes flowing through channels having cross sectional dimensions of 60 x 38 micron (2.22 +/- 0.50 microM ATP). Microscopic images indicate that erythrocytes, when being pumped through the microchip channels, migrate toward the center of the channels, leaving a cell-free or skimming layer at the walls of the channel, a profile known to exist in circulatory vessels in vivo. A comparison of the amounts of ATP <span class="hlt">released</span> from RBCs mechanically <span class="hlt">deformed</span> in microbore tubing (2.54 +/- 0.15 microM) vs a microchip (2.59 +/- 0.32 microM) suggests that channels in microchips may serve as functional biomimics of the microvasculature. Control studies involving diamide, a membrane-stiffening agent, suggest that the RBC-derived ATP is not due to cell lysis but rather physical <span class="hlt">deformation</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NuPhA.952...18L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NuPhA.952...18L"><span>Nuclear <span class="hlt">energy</span> <span class="hlt">release</span> from fragmentation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Cheng; Souza, S. R.; Tsang, M. B.; Zhang, Feng-Shou</p> <p>2016-08-01</p> <p>It is well known that binary fission occurs with positive <span class="hlt">energy</span> gain. In this article we examine the energetics of splitting uranium and thorium isotopes into various numbers of fragments (from two to eight) with nearly equal size. We find that the <span class="hlt">energy</span> <span class="hlt">released</span> by splitting 230,232Th and 235,238U into three equal size fragments is largest. The statistical multifragmentation model (SMM) is applied to calculate the probability of different breakup channels for excited nuclei. By weighing the probability distributions of fragment multiplicity at different excitation <span class="hlt">energies</span>, we find the peaks of <span class="hlt">energy</span> <span class="hlt">release</span> for 230,232Th and 235,238U are around 0.7-0.75 MeV/u at excitation <span class="hlt">energy</span> between 1.2 and 2 MeV/u in the primary breakup process. Taking into account the secondary de-excitation processes of primary fragments with the GEMINI code, these <span class="hlt">energy</span> peaks fall to about 0.45 MeV/u.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AIPC.1683b0121L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AIPC.1683b0121L"><span>DEM code-based modeling of <span class="hlt">energy</span> accumulation and <span class="hlt">release</span> in structurally heterogeneous rock masses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lavrikov, S. V.; Revuzhenko, A. F.</p> <p>2015-10-01</p> <p>Based on discrete element method, the authors model loading of a physical specimen to describe its capacity to accumulate and <span class="hlt">release</span> elastic <span class="hlt">energy</span>. The specimen is modeled as a packing of particles with viscoelastic coupling and friction. The external elastic boundary of the packing is represented by particles connected by elastic springs. The latter means introduction of an additional special potential of interaction between the boundary particles, that exercises effect even when there is no direct contact between the particles. On the whole, the model specimen represents an element of a medium capable of accumulation of <span class="hlt">deformation</span> <span class="hlt">energy</span> in the form of internal stresses. The data of the numerical modeling of the physical specimen compression and the laboratory testing results show good qualitative consistency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MPLA...3350054D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MPLA...3350054D"><span>Pauli <span class="hlt">energy</span> spectrum for twist-<span class="hlt">deformed</span> spacetime</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Daszkiewicz, Marcin</p> <p>2018-04-01</p> <p>In this paper, we define the Pauli Hamiltonian function for the twist-<span class="hlt">deformed</span> N-enlarged Newton-Hooke spacetime provided by M. Daszkiewicz [Mod. Phys. Lett. A 27, 1250083 (2012)]. Further, we derive its <span class="hlt">energy</span> spectrum, i.e. we find the corresponding eigenvalues as well as the proper eigenfunctions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5253075','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5253075"><span>High probability neurotransmitter <span class="hlt">release</span> sites represent an <span class="hlt">energy</span> efficient design</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lu, Zhongmin; Chouhan, Amit K.; Borycz, Jolanta A.; Lu, Zhiyuan; Rossano, Adam J; Brain, Keith L.; Zhou, You; Meinertzhagen, Ian A.; Macleod, Gregory T.</p> <p>2016-01-01</p> <p>Nerve terminals contain multiple sites specialized for the <span class="hlt">release</span> of neurotransmitters. <span class="hlt">Release</span> usually occurs with low probability, a design thought to confer many advantages. High probability <span class="hlt">release</span> sites are not uncommon but their advantages are not well understood. Here we test the hypothesis that high probability <span class="hlt">release</span> sites represent an <span class="hlt">energy</span> efficient design. We examined <span class="hlt">release</span> site probabilities and <span class="hlt">energy</span> efficiency at the terminals of two glutamatergic motor neurons synapsing on the same muscle fiber in Drosophila larvae. Through electrophysiological and ultrastructural measurements we calculated <span class="hlt">release</span> site probabilities to differ considerably between terminals (0.33 vs. 0.11). We estimated the <span class="hlt">energy</span> required to <span class="hlt">release</span> and recycle glutamate from the same measurements. The <span class="hlt">energy</span> required to remove calcium and sodium ions subsequent to nerve excitation was estimated through microfluorimetric and morphological measurements. We calculated <span class="hlt">energy</span> efficiency as the number of glutamate molecules <span class="hlt">released</span> per ATP molecule hydrolyzed, and high probability <span class="hlt">release</span> site terminals were found to be more efficient (0.13 vs. 0.06). Our analytical model indicates that <span class="hlt">energy</span> efficiency is optimal (~0.15) at high <span class="hlt">release</span> site probabilities (~0.76). As limitations in <span class="hlt">energy</span> supply constrain neural function, high probability <span class="hlt">release</span> sites might ameliorate such constraints by demanding less <span class="hlt">energy</span>. <span class="hlt">Energy</span> efficiency can be viewed as one aspect of nerve terminal function, in balance with others, because high efficiency terminals depress significantly during episodic bursts of activity. PMID:27593375</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26087351','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26087351"><span>Effects of mechanical <span class="hlt">deformation</span> on <span class="hlt">energy</span> conversion efficiency of piezoelectric nanogenerators.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yoo, Jinho; Cho, Seunghyeon; Kim, Wook; Kwon, Jang-Yeon; Kim, Hojoong; Kim, Seunghyun; Chang, Yoon-Suk; Kim, Chang-Wan; Choi, Dukhyun</p> <p>2015-07-10</p> <p>Piezoelectric nanogenerators (PNGs) are capable of converting <span class="hlt">energy</span> from various mechanical sources into electric <span class="hlt">energy</span> and have many attractive features such as continuous operation, replenishment and low cost. However, many researchers still have studied novel material synthesis and interfacial controls to improve the power production from PNGs. In this study, we report the <span class="hlt">energy</span> conversion efficiency (ECE) of PNGs dependent on mechanical <span class="hlt">deformations</span> such as bending and twisting. Since the output power of PNGs is caused by the mechanical strain of the piezoelectric material, the power production and their ECE is critically dependent on the types of external mechanical <span class="hlt">deformations</span>. Thus, we examine the output power from PNGs according to bending and twisting. In order to clearly understand the ECE of PNGs in the presence of those external mechanical <span class="hlt">deformations</span>, we determine the ECE of PNGs by the ratio of output electrical <span class="hlt">energy</span> and input mechanical <span class="hlt">energy</span>, where we suggest that the input <span class="hlt">energy</span> is based only on the strain <span class="hlt">energy</span> of the piezoelectric layer. We calculate the strain <span class="hlt">energy</span> of the piezoelectric layer using numerical simulation of bending and twisting of the PNG. Finally, we demonstrate that the ECE of the PNG caused by twisting is much higher than that caused by bending due to the multiple effects of normal and lateral piezoelectric coefficients. Our results thus provide a design direction for PNG systems as high-performance power generators.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011APS..DFD.H2009L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011APS..DFD.H2009L"><span>Simulation of <span class="hlt">Deformation</span>, Momentum and <span class="hlt">Energy</span> Coupling Particles <span class="hlt">Deformed</span> by Intense Shocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lieberthal, B.; Stewart, D. S.; Bdzil, J. B.; Najjar, F. M.; Balachandar, S.; Ling, Y.</p> <p>2011-11-01</p> <p>Modern energetic materials have embedded solids and inerts in an explosive matrix. A detonation in condensed phase materials, generates intense shocks that <span class="hlt">deform</span> particles as the incident shock diffracts around them. The post-shock flow generates a wake behind the particle that is influenced by the shape changes of the particle. The gasdynamic flow in the explosive products and its interaction with the <span class="hlt">deformation</span> of the particle must be treated simultaneously. Direct numerical simulations are carried out that vary the particle-to-surrounding density and impedance ratios to consider heavier and lighter particle. The vorticity deposited on the interface due to shock interaction with the particle, the resulting particle <span class="hlt">deformation</span> and the net momentum and <span class="hlt">energy</span> transferred to the particle, on the acoustic and longer viscous time scale are considered. The LLNL multi-physics hydrodynamic code ALE3D is used to carry out the simulations. BL, DSS and JBB supported by AFRL/RW AF FA8651-10-1-0004 & DTRA, HDTRA1-10-1-0020 Off Campus. FMN's work supported by the U.S. DOE/ LLNL, Contract DE-AC52-07NA27344. LLNL-ABS-491794.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.865a2002S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.865a2002S"><span><span class="hlt">Energy</span> spectrum inverse problem of q-<span class="hlt">deformed</span> harmonic oscillator and entanglement of composite bosons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sang, Nguyen Anh; Thu Thuy, Do Thi; Loan, Nguyen Thi Ha; Lan, Nguyen Tri; Viet, Nguyen Ai</p> <p>2017-06-01</p> <p>Using the simple <span class="hlt">deformed</span> three-level model (D3L model) proposed in our early work, we study the entanglement problem of composite bosons. Consider three first <span class="hlt">energy</span> levels are known, we can get two <span class="hlt">energy</span> separations, and can define the level <span class="hlt">deformation</span> parameter δ. Using connection between q-<span class="hlt">deformed</span> harmonic oscillator and Morse-like anharmonic potential, the <span class="hlt">deform</span> parameter q also can be derived explicitly. Like the Einstein’s theory of special relativity, we introduce the observer e˙ects: out side observer (looking from outside the studying system) and inside observer (looking inside the studying system). Corresponding to those observers, the outside entanglement entropy and inside entanglement entropy will be defined.. Like the case of Foucault pendulum in the problem of Earth rotation, our <span class="hlt">deformation</span> <span class="hlt">energy</span> level investigation might be useful in prediction the environment e˙ect outside a confined box.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EPJWC..9402004P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EPJWC..9402004P"><span>An experimental investigation of <span class="hlt">energy</span> absorption in TRIP steel under impact three-point bending <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pham, Hang; Iwamoto, Takeshi</p> <p>2015-09-01</p> <p>TRIP (Transformation-induced Plasticity) steel is nowadays in widespread use in the automobile industry because of their favorable mechanical properties such as high strength, excellent formability and toughness because of strain-induced martensitic transformation. Moreover, when TRIP steel is applied to the components of the vehicles, it is expected that huge amount of kinetic <span class="hlt">energy</span> will be absorbed into both plastic <span class="hlt">deformation</span> and martensitic transformation during the collision. Basically, bending <span class="hlt">deformation</span> due to buckling is one of the major crash <span class="hlt">deformation</span> modes of automobile structures. Thus, an investigation of <span class="hlt">energy</span> absorption during bending <span class="hlt">deformation</span> at high impact velocity for TRIP steel is indispensable. Although TRIP steel have particularly attracted the recent interest of the scientific community, just few studies can be found on the <span class="hlt">energy</span> absorption characteristic of TRIP steel, especially at impact loading condition. In present study, experimental investigations of bending <span class="hlt">deformation</span> behaviors of TRIP steel are conducted in the three-point bending tests for both smooth and pre-cracked specimen. Then, <span class="hlt">energy</span> absorption characteristic during plastic <span class="hlt">deformation</span> and fracture process at high impact velocity in TRIP steel will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARK17003S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARK17003S"><span>Dynamical <span class="hlt">Energy</span> Gap Engineering in Graphene via Oscillating Out-of-Plane <span class="hlt">Deformations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sandler, Nancy; Zhai, Dawei</p> <p></p> <p>The close relation between electronic properties and mechanical <span class="hlt">deformations</span> in graphene has been the topic of active research in recent years. Interestingly, the effect of <span class="hlt">deformations</span> on electronic properties can be understood in terms of pseudo-magnetic fields, whose spatial distribution and intensity are controllable via the <span class="hlt">deformation</span> geometry. Previous results showed that electromagnetic fields (light) have the potential to induce dynamical gaps in graphene's <span class="hlt">energy</span> bands, transforming graphene from a semimetal to a semiconductor. However, laser frequencies required to achieve these regimes are in the THz regime, which imposes challenges for practical purposes. In this talk we report a novel method to create dynamical gaps using oscillating mechanical <span class="hlt">deformations</span>, i.e., via time-dependent pseudo-magnetic fields. Using the Floquet formalism we show the existence of a dynamical gap in the band structure at <span class="hlt">energies</span> set by the frequency of the oscillation, and with a magnitude tuned by the geometry of the <span class="hlt">deformation</span>. This dynamical-mechanical manipulation strategy appears as a promising venue to engineer electronic properties of suspended graphene devices. Work supported by NSF-DMR 1508325.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19990078564','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19990078564"><span>A Method for Calculating Strain <span class="hlt">Energy</span> <span class="hlt">Release</span> Rates in Preliminary Design of Composite Skin/Stringer Debonding Under Multi-Axial Loading</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Krueger, Ronald; Minguet, Pierre J.; OBrien, T. Kevin</p> <p>1999-01-01</p> <p>Three simple procedures were developed to determine strain <span class="hlt">energy</span> <span class="hlt">release</span> rates, G, in composite skin/stringer specimens for various combinations of unaxial and biaxial (in-plane/out-of-plane) loading conditions. These procedures may be used for parametric design studies in such a way that only a few finite element computations will be necessary for a study of many load combinations. The results were compared with mixed mode strain <span class="hlt">energy</span> <span class="hlt">release</span> rates calculated directly from nonlinear two-dimensional plane-strain finite element analyses using the virtual crack closure technique. The first procedure involved solving three unknown parameters needed to determine the <span class="hlt">energy</span> <span class="hlt">release</span> rates. Good agreement was obtained when the external loads were used in the expression derived. This superposition technique was only applicable if the structure exhibits a linear load/deflection behavior. Consequently, a second technique was derived which was applicable in the case of nonlinear load/<span class="hlt">deformation</span> behavior. The technique involved calculating six unknown parameters from a set of six simultaneous linear equations with data from six nonlinear analyses to determine the <span class="hlt">energy</span> <span class="hlt">release</span> rates. This procedure was not time efficient, and hence, less appealing. A third procedure was developed to calculate mixed mode <span class="hlt">energy</span> <span class="hlt">release</span> rates as a function of delamination lengths. This procedure required only one nonlinear finite element analysis of the specimen with a single delamination length to obtain a reference solution for the <span class="hlt">energy</span> <span class="hlt">release</span> rates and the scale factors. The delamination was extended in three separate linear models of the local area in the vicinity of the delamination subjected to unit loads to obtain the distribution of G with delamination lengths. This set of sub-problems was Although additional modeling effort is required to create the sub- models, this local technique is efficient for parametric studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21832138','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21832138"><span>Elastic <span class="hlt">deformation</span> and <span class="hlt">energy</span> loss of flapping fly wings.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lehmann, Fritz-Olaf; Gorb, Stanislav; Nasir, Nazri; Schützner, Peter</p> <p>2011-09-01</p> <p>During flight, the wings of many insects undergo considerable shape changes in spanwise and chordwise directions. We determined the origin of spanwise wing <span class="hlt">deformation</span> by combining measurements on segmental wing stiffness of the blowfly Calliphora vicina in the ventral and dorsal directions with numerical modelling of instantaneous aerodynamic and inertial forces within the stroke cycle using a two-dimensional unsteady blade elementary approach. We completed this approach by an experimental study on the wing's rotational axis during stroke reversal. The wing's local flexural stiffness ranges from 30 to 40 nN m(2) near the root, whereas the distal wing parts are highly compliant (0.6 to 2.2 nN m(2)). Local bending moments during wing flapping peak near the wing root at the beginning of each half stroke due to both aerodynamic and inertial forces, producing a maximum wing tip deflection of up to 46 deg. Blowfly wings store up to 2.30 μJ elastic potential <span class="hlt">energy</span> that converts into a mean wing <span class="hlt">deformation</span> power of 27.3 μW. This value equates to approximately 5.9 and 2.3% of the inertial and aerodynamic power requirements for flight in this animal, respectively. Wing elasticity measurements suggest that approximately 20% or 0.46 μJ of elastic potential <span class="hlt">energy</span> cannot be recovered within each half stroke. Local strain <span class="hlt">energy</span> increases from tip to root, matching the distribution of the wing's elastic protein resilin, whereas local strain <span class="hlt">energy</span> density varies little in the spanwise direction. This study demonstrates a source of mechanical <span class="hlt">energy</span> loss in fly flight owing to spanwise wing bending at the stroke reversals, even in cases in which aerodynamic power exceeds inertial power. Despite lower stiffness estimates, our findings are widely consistent with previous stiffness measurements on insect wings but highlight the relationship between local flexural stiffness, wing <span class="hlt">deformation</span> power and <span class="hlt">energy</span> expenditure in flapping insect wings.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..237a2004D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..237a2004D"><span>Numerical estimation of <span class="hlt">deformation</span> <span class="hlt">energy</span> of selected bulk oilseeds in compression loading</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Demirel, C.; Kabutey, A.; Herak, D.; Gurdil, G. A. K.</p> <p>2017-09-01</p> <p>This paper aimed at the determination of the <span class="hlt">deformation</span> <span class="hlt">energy</span> of some bulk oilseeds or kernels namely oil palm, sunflower, rape and flax in linear pressing applying the trapezoidal rule which is characterized by the area under the force and <span class="hlt">deformation</span> curve.The bulk samples were measured at the initial pressing height of 60 mm with the vessel diameter of 60 mm where they were compressed under the universal compression machine at a maximum force of 200 kN and speed of 5 mm/min.Based on the compression test, the optimal <span class="hlt">deformation</span> <span class="hlt">energy</span> for recovering the oil was observed at a force of 163 kN where there was no seed/kernel cake ejection in comparison to the initial maximum force used particularly for rape and flax bulk oilseeds.This information is needed for analyzing the <span class="hlt">energy</span> efficiency of the non-linear compression process involving a mechanical screw press or expeller.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3362563','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3362563"><span>Cytoplasmic Fungal Lipases <span class="hlt">Release</span> Fungicides from Ultra-<span class="hlt">Deformable</span> Vesicular Drug Carriers</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Steinberg, Gero</p> <p>2012-01-01</p> <p>The Transfersome® is a lipid vesicle that contains membrane softeners, such as Tween 80, to make it ultra-<span class="hlt">deformable</span>. This feature makes the Transfersome® an efficient carrier for delivery of therapeutic drugs across the skin barrier. It was reported that TDT 067 (a topical formulation of 15 mg/ml terbinafine in Transfersome® vesicles) has a much more potent antifungal activity in vitro compared with conventional terbinafine, which is a water-insoluble fungicide. Here we use ultra-structural studies and live imaging in a model fungus to describe the underlying mode of action. We show that terbinafine causes local collapse of the fungal endoplasmic reticulum, which was more efficient when terbinafine was delivered in Transfersome® vesicles (TFVs). When applied in liquid culture, fluorescently labeled TFVs rapidly entered the fungal cells (T1/2∼2 min). Entry was F-actin- and ATP-independent, indicating that it is a passive process. Ultra-structural studies showed that passage through the cell wall involves significant <span class="hlt">deformation</span> of the vesicles, and depends on a high concentration of the surfactant Tween 80 in their membrane. Surprisingly, the TFVs collapsed into lipid droplets after entry into the cell and the terbinafine was <span class="hlt">released</span> from their interior. With time, the lipid bodies were metabolized in an ATP-dependent fashion, suggesting that cytosolic lipases attack and degrade intruding TFVs. Indeed, the specific monoacylglycerol lipase inhibitor URB602 prevented Transfersome® degradation and neutralized the cytotoxic effect of Transfersome®-delivered terbinafine. These data suggest that (a) Transfersomes deliver the lipophilic fungicide Terbinafine to the fungal cell wall, (b) the membrane softener Tween 80 allows the passage of the Transfersomes into the fungal cell, and (c) fungal lipases digest the invading Transfersome® vesicles thereby <span class="hlt">releasing</span> their cytotoxic content. As this mode of action of Transfersomes is independent of the drug cargo</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29763310','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29763310"><span>Stability, Elastic Properties, and <span class="hlt">Deformation</span> of LiBN2: A Potential High-<span class="hlt">Energy</span> Material.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhu, Chunye; Zhu, Wenjun; Yang, Yanqiang</p> <p>2018-05-15</p> <p>Searching for high-<span class="hlt">energy</span>-density materials is of great interest in scientific research and for industrial applications. Using an unbiased structure prediction method and first-principles calculations, we investigated the phase stability of LiBN 2 from 0 to100 GPa. Two new structures with space groups P4̅2 1 m and Pnma were discovered. The theoretical calculations revealed that Pnma LiBN 2 is stable with respect to a mixture of 1 / 3 Li 3 N, BN, and 1 / 3 N 2 above 22 GPa. The electronic band structure revealed that Pnma LiBN 2 has an indirect band gap of 2.3 eV, which shows a nonmetallic feature. The Pnma phase has a high calculated bulk modulus and shear modulus, indicating its incompressible nature. The microscopic mechanism of the structural <span class="hlt">deformation</span> was demonstrated by ideal tensile shear strength calculations. It is worth mentioning that Pnma LiBN 2 is dynamically stable under ambient conditions. The decomposition of this phase is exothermic, <span class="hlt">releasing</span> an <span class="hlt">energy</span> of approximately 1.23 kJ/g at the PBE level. The results provide new thoughts for designing and synthesizing novel high-<span class="hlt">energy</span> compounds in ternary systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM33E..04G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM33E..04G"><span>High-<span class="hlt">Energy</span> Aspects of Small-Scale <span class="hlt">Energy</span> <span class="hlt">Release</span> at the Sun</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Glesener, L.; Vievering, J. T.; Wright, P. J.; Hannah, I. G.; Panchapakesan, S. A.; Ryan, D.; Krucker, S.; Hudson, H. S.; Grefenstette, B.; White, S. M.; Smith, D. M.; Marsh, A.; Kuhar, M.; Christe, S.; Buitrago-Casas, J. C.; Musset, S.; Inglis, A. R.</p> <p>2017-12-01</p> <p>Large, powerful solar flares have been investigated in detail for decades, but it is only recently that high-<span class="hlt">energy</span> aspects of small flares could be measured. These small-scale <span class="hlt">energy</span> <span class="hlt">releases</span> offer the opportunity to examine how particle acceleration characteristics scale down, which is critical for constraining <span class="hlt">energy</span> transfer theories such as magnetic reconnection. Probing to minuscule flare sizes also brings us closer to envisioning the characteristics of the small "nanoflares" that may be responsible for heating the corona. A new window on small-scale flaring activity is now opening with the use of focusing hard X-ray instruments to observe the Sun. Hard X-rays are emitted by flare-accelerated electrons and strongly heated plasma, providing a relatively direct method of measuring <span class="hlt">energy</span> <span class="hlt">release</span> and particle acceleration properties. This work will show the first observations of sub-A class microflares using the FOXSI sounding rocket and the NuSTAR astrophysics spacecraft, both of which directly focus hard X-rays but have limited observing time on the Sun. These instruments serve as precursors to a spacecraft version of FOXSI, which will explore <span class="hlt">energy</span> <span class="hlt">release</span> across the entire range of flaring activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004SPIE.5388..288C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004SPIE.5388..288C"><span>Mechanical strain <span class="hlt">energy</span> shuttle for aircraft morphing via wing twist or structural <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Clingman, Dan J.; Ruggeri, Robert T.</p> <p>2004-07-01</p> <p>Direct structural <span class="hlt">deformation</span> to achieve aerodynamic benefit is difficult because large actuators must supply <span class="hlt">energy</span> for structural strain and aerodynamic loads. This ppaer presents a mechanism that allows most of the <span class="hlt">energy</span> required to twist or <span class="hlt">deform</span> a wing to be stored in descrete springs. When this device is used, only sufficient <span class="hlt">energy</span> is provided to control the position of the wing. This concept allows lightweight actuators to perform wing twisting and other structural distortions, and it reduces the onboard mass of the wing-twist system. The <span class="hlt">energy</span> shuttle can be used with any actuator and it has been adapted for used with shape memory alloy, piezoelectric, and electromagnetic actuators.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_1");'>1</a></li> <li class="active"><span>2</span></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_2 --> <div id="page_3" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_1");'>1</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li class="active"><span>3</span></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="41"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880058310&hterms=rust&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Drust','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880058310&hterms=rust&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Drust"><span>Highlights of the study of <span class="hlt">energy</span> <span class="hlt">release</span> in flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rust, D. M.; Batchelor, D. A.</p> <p>1987-01-01</p> <p>From February 26 to March 1, 1979, 32 solar flare investigators attended a workshop at Cambridge, MA to define objectives and devise a scientific program for the study of <span class="hlt">energy</span> <span class="hlt">release</span> in flares (SERF) during the coming solar maximum. Herein, some major results of the ensuing five-year effort to observe and understand the flare <span class="hlt">energy</span> <span class="hlt">release</span> process and its effects (energetic particle production, coronal and chromospheric heating, electromagnetic radiations, and mass motions and ejections) are reviewed. The central issue - what processes store and <span class="hlt">release</span> the <span class="hlt">energy</span> liberated in flares - remains unresolved except in the most general terms (e.g., it is generally agreed that the <span class="hlt">energy</span> is stored in sheared or stressed magnetic fields and <span class="hlt">released</span> by field annihilation during some MHD instability). Resolving that issue is still one of the most important goals in solar physics, but the advances during the SERF program have brought it closer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999SPIE.3876..212R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999SPIE.3876..212R"><span>Microelectromechanical high-density <span class="hlt">energy</span> storage/rapid <span class="hlt">release</span> system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rodgers, M. Steven; Allen, James J.; Meeks, Kent D.; Jensen, Brian D.; Miller, Samuel L.</p> <p>1999-08-01</p> <p>One highly desirable characteristic of electrostatically driven microelectromechanical systems (MEMS) is that they consume very little power. The corresponding drawback is that the force they produce may be inadequate for many applications. It has previously been demonstrated that gear reduction units or microtransmissions can substantially increase the torque generated by microengines. Operating speed, however, is also reduced by the transmission gear ratio. Some applications require both high speed and high force. If this output is only required for a limited period of time, then <span class="hlt">energy</span> could be stored in a mechanical system and rapidly <span class="hlt">released</span> upon demand. We have designed, fabricated, and demonstrated a high-density <span class="hlt">energy</span> storage/rapid <span class="hlt">release</span> system that accomplishes this task. Built using a 5-level surface micromachining technology, the assembly closely resembles a medieval crossbow. <span class="hlt">Energy</span> <span class="hlt">releases</span> on the order of tens of nanojoules have already been demonstrated, and significantly higher <span class="hlt">energy</span> systems are under development.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20346901','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20346901"><span>An activated <span class="hlt">energy</span> approach for accelerated testing of the <span class="hlt">deformation</span> of UHMWPE in artificial joints.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Galetz, Mathias Christian; Glatzel, Uwe</p> <p>2010-05-01</p> <p>The <span class="hlt">deformation</span> behavior of ultrahigh molecular polyethylene (UHMWPE) is studied in the temperature range of 23-80 degrees C. Samples are examined in quasi-static compression, tensile and creep tests to determine the accelerated <span class="hlt">deformation</span> of UHMWPE at elevated temperatures. The <span class="hlt">deformation</span> mechanisms under compression load can be described by one strain rate and temperature dependent Eyring process. The activation <span class="hlt">energy</span> and volume of that process do not change between 23 degrees C and 50 degrees C. This suggests that the <span class="hlt">deformation</span> mechanism under compression remains stable within this temperature range. Tribological tests are conducted to transfer this activated <span class="hlt">energy</span> approach to the <span class="hlt">deformation</span> behavior under loading typical for artificial knee joints. While this approach does not cover the wear mechanisms close to the surface, testing at higher temperatures is shown to have a significant potential to reduce the testing time for lifetime predictions in terms of the macroscopic creep and <span class="hlt">deformation</span> behavior of artificial joints. Copyright 2010. Published by Elsevier Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA122182','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA122182"><span><span class="hlt">Energy</span> <span class="hlt">Release</span> in Solar Flares,</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1982-10-01</p> <p>Plasma Research, Stanford University P. Kaufmanu CRAA/CNPq -Conseiho lacional de Desenvolvimento Cientifico e Tecnologico, Slo Paulo, SP, Brasil D.F...three phases of <span class="hlt">energy</span> <span class="hlt">release</span> in solar flares (Sturrock, 1980). However, a recent article by Feldman e a.. (1982) points to a significant</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17888713','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17888713"><span>Effects of varying material properties on the load <span class="hlt">deformation</span> characteristics of heel cushions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sun, Pi-Chang; Wei, Hung-Wen; Chen, Chien-Hua; Wu, Chun-Hao; Kao, Hung-Chan; Cheng, Cheng-Kung</p> <p>2008-07-01</p> <p>Various insole materials were used in attenuation of heel-strike impact. This study presented a compression test to investigate the <span class="hlt">deformation</span> characteristics of common heel cushions. There were two materials (thermoplastic elastomer "TPE" and silicone) with three hardness and six thickness being analyzed. They underwent consecutive loading-unloading cycles with a load control mode. The displacement of material thickness was recorded during cyclic compression being applied and <span class="hlt">released</span> from 0 to 1050 N. The <span class="hlt">energy</span> input, return and dissipation were evaluated based on the load <span class="hlt">deformation</span> curves when new and after repeated compression. The TPE recovered more <span class="hlt">deformed</span> <span class="hlt">energy</span> and thickness than the silicone after the first loading cycle. The silicone would preserve more strain <span class="hlt">energy</span> with increasing its hardness for the elastic recovery in the unloading process. The <span class="hlt">deformed</span> <span class="hlt">energy</span> was decreased as the original thickness did not completely recover under cyclic tests. The reduction in hysteresis area was gradually converged within 20 cycles. The silicone attenuated more impact <span class="hlt">energy</span> in the initial cycles, but its <span class="hlt">energy</span> dissipation was reduced after repeated loading. To increase hardness or thickness should be considered to improve resilience or accommodate persistent compression without flattening. The careful selection of cushion materials is imperative to meet individual functional demands.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28843012','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28843012"><span>The main beam correction term in kinetic <span class="hlt">energy</span> <span class="hlt">release</span> from metastable peaks.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Petersen, Allan Christian</p> <p>2017-12-01</p> <p>The correction term for the precursor ion signal width in determination of kinetic <span class="hlt">energy</span> <span class="hlt">release</span> is reviewed, and the correction term is formally derived. The derived correction term differs from the traditionally applied term. An experimental finding substantiates the inaccuracy in the latter. The application of the "T-value" to study kinetic <span class="hlt">energy</span> <span class="hlt">release</span> is found preferable to kinetic <span class="hlt">energy</span> <span class="hlt">release</span> distributions when the metastable peaks are slim and simple Gaussians. For electronically predissociated systems, a "borderline zero" kinetic <span class="hlt">energy</span> <span class="hlt">release</span> can be directly interpreted in reaction dynamics with strong curvature in the reaction coordinate. Copyright © 2017 John Wiley & Sons, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/9508','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/9508"><span>A Microelectromechanical High-Density <span class="hlt">Energy</span> Storage/Rapid <span class="hlt">Release</span> System</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Rodgers, M. Steven; Allen, Jim J.; Meeks, Kent D.</p> <p>1999-07-21</p> <p>One highly desirable characteristic of electrostatically driven microelectromechanical systems (MEMS) is that they consume very little power. The corresponding drawback is that the force they produce may be inadequate for many applications. It has previously been demonstrated that gear reduction units or microtransmissions can substantially increase the torque generated by microengines. Operating speed, however, is also reduced by the transmission gear ratio. Some applications require both high speed and high force. If this output is only required for a limited period of time, then <span class="hlt">energy</span> could be stored in a mechanical system and rapidly <span class="hlt">released</span> upon demand. We have designed,more » fabricated, and demonstrated a high-density <span class="hlt">energy</span> storage/rapid <span class="hlt">release</span> system that accomplishes this task. Built using a 5-level surface micromachining technology, the assembly closely resembles a medieval crossbow. <span class="hlt">Energy</span> <span class="hlt">releases</span> on the order of tens of nanojoules have already been demonstrated, and significantly higher <span class="hlt">energy</span> systems are under development.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=kinetic+AND+energy&pg=3&id=EJ860250','ERIC'); return false;" href="https://eric.ed.gov/?q=kinetic+AND+energy&pg=3&id=EJ860250"><span><span class="hlt">Energy</span> and the Confused Student V: The <span class="hlt">Energy</span>/Momentum Approach to Problems Involving Rotating and <span class="hlt">Deformable</span> Systems</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Jewett, John W., Jr.</p> <p>2008-01-01</p> <p><span class="hlt">Energy</span> is a critical concept in physics problem-solving, but is often a major source of confusion for students if the presentation is not carefully crafted by the instructor or the textbook. A common approach to problems involving <span class="hlt">deformable</span> or rotating systems that has been discussed in the literature is to employ the work-kinetic <span class="hlt">energy</span> theorem…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://news.fnal.gov/2016/01/dark-energy-survey-releases-early-data','SCIGOVWS'); return false;" href="http://news.fnal.gov/2016/01/dark-energy-survey-releases-early-data"><span>Dark <span class="hlt">Energy</span> Survey <span class="hlt">releases</span> early data | News</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p><span class="hlt">released</span> to the public. Astronomers and <em>astronomy</em> buffs can download the data from the website for the of all the images taken for the Dark <span class="hlt">Energy</span> Survey. This is good news for the <em>astronomy</em> community, as Optical <em>Astronomy</em> Observatory's Cerro Tololo Inter-American Observatory in Chile. The Dark <span class="hlt">Energy</span> Survey</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..317a2004G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..317a2004G"><span>Characteristics of Crushing <span class="hlt">Energy</span> and Fractal of Magnetite Ore under Uniaxial Compression</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gao, F.; Gan, D. Q.; Zhang, Y. B.</p> <p>2018-03-01</p> <p>The crushing mechanism of magnetite ore is a critical theoretical problem on the controlling of <span class="hlt">energy</span> dissipation and machine crushing quality in ore material processing. Uniaxial crushing tests were carried out to research the <span class="hlt">deformation</span> mechanism and the laws of the <span class="hlt">energy</span> evolution, based on which the crushing mechanism of magnetite ore was explored. The compaction stage and plasticity and damage stage are two main compression <span class="hlt">deformation</span> stages, the main transitional forms from inner damage to fracture are plastic <span class="hlt">deformation</span> and stick-slip. In the process of crushing, plasticity and damage stage is the key link on <span class="hlt">energy</span> absorption for that the specimen tends to saturate <span class="hlt">energy</span> state approaching to the peak stress. The characteristics of specimen <span class="hlt">deformation</span> and <span class="hlt">energy</span> dissipation can synthetically reply the state of existed defects inner raw magnetite ore and the damage process during loading period. The fast <span class="hlt">releasing</span> of elastic <span class="hlt">energy</span> and the work done by the press machine commonly make raw magnetite ore thoroughly broken after peak stress. Magnetite ore fragments have statistical self-similarity and size threshold of fractal characteristics under uniaxial squeezing crushing. The larger ratio of <span class="hlt">releasable</span> elastic <span class="hlt">energy</span> and dissipation <span class="hlt">energy</span> and the faster <span class="hlt">energy</span> change rate is the better fractal properties and crushing quality magnetite ore has under uniaxial crushing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.eia.gov/outlooks/archive/aeo10/carbon_dioxide.html','EIAPUBS'); return false;" href="https://www.eia.gov/outlooks/archive/aeo10/carbon_dioxide.html"><span>Accounting for Carbon Dioxide Emissions from Biomass <span class="hlt">Energy</span> Combustion (<span class="hlt">released</span> in AEO2010)</span></a></p> <p><a target="_blank" href="http://www.eia.doe.gov/reports/">EIA Publications</a></p> <p></p> <p>2010-01-01</p> <p>Carbon Dioxide (CO2) emissions from the combustion of biomass to produce <span class="hlt">energy</span> are excluded from the <span class="hlt">energy</span>-related CO2 emissions reported in Annual <span class="hlt">Energy</span> Outlook 2010. According to current international convention, carbon <span class="hlt">released</span> through biomass combustion is excluded from reported <span class="hlt">energy</span>-related emissions. The <span class="hlt">release</span> of carbon from biomass combustion is assumed to be balanced by the uptake of carbon when the feedstock is grown, resulting in zero net emissions over some period of time]. However, analysts have debated whether increased use of biomass <span class="hlt">energy</span> may result in a decline in terrestrial carbon stocks, leading to a net positive <span class="hlt">release</span> of carbon rather than the zero net <span class="hlt">release</span> assumed by its exclusion from reported <span class="hlt">energy</span>-related emissions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22679462-simulation-radiation-energy-release-air-showers','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22679462-simulation-radiation-energy-release-air-showers"><span>Simulation of radiation <span class="hlt">energy</span> <span class="hlt">release</span> in air showers</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Glaser, Christian; Erdmann, Martin; Hörandel, Jörg R.</p> <p>2016-09-01</p> <p>A simulation study of the <span class="hlt">energy</span> <span class="hlt">released</span> by extensive air showers in the form of MHz radiation is performed using the CoREAS simulation code. We develop an efficient method to extract this radiation <span class="hlt">energy</span> from air-shower simulations. We determine the longitudinal profile of the radiation <span class="hlt">energy</span> <span class="hlt">release</span> and compare it to the longitudinal profile of the <span class="hlt">energy</span> deposit by the electromagnetic component of the air shower. We find that the radiation <span class="hlt">energy</span> corrected for the geometric dependence of the geomagnetic emission scales quadratically with the <span class="hlt">energy</span> in the electromagnetic component of the air shower with a second-order dependence on themore » atmospheric density at the position of the maximum shower development X {sub max}. In a measurement where X {sub max} is not accessible, this second order dependence can be approximated using the zenith angle of the incoming direction of the air shower with only a minor loss in accuracy. Our method results in an intrinsic uncertainty of 4% in the determination of the <span class="hlt">energy</span> in the electromagnetic air-shower component, which is well below current experimental uncertainties.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1242270-spatio-temporal-modeling-optimization-deformable-grating-compressor-short-high-energy-laser-pulses','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1242270-spatio-temporal-modeling-optimization-deformable-grating-compressor-short-high-energy-laser-pulses"><span>Spatio-temporal modeling and optimization of a <span class="hlt">deformable</span>-grating compressor for short high-<span class="hlt">energy</span> laser pulses</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Qiao, Jie; Papa, J.; Liu, X.</p> <p>2015-09-24</p> <p>Monolithic large-scale diffraction gratings are desired to improve the performance of high-<span class="hlt">energy</span> laser systems and scale them to higher <span class="hlt">energy</span>, but the surface <span class="hlt">deformation</span> of these diffraction gratings induce spatio-temporal coupling that is detrimental to the focusability and compressibility of the output pulse. A new <span class="hlt">deformable</span>-grating-based pulse compressor architecture with optimized actuator positions has been designed to correct the spatial and temporal aberrations induced by grating wavefront errors. An integrated optical model has been built to analyze the effect of grating wavefront errors on the spatio-temporal performance of a compressor based on four <span class="hlt">deformable</span> gratings. Moreover, a 1.5-meter <span class="hlt">deformable</span> gratingmore » has been optimized using an integrated finite-element-analysis and genetic-optimization model, leading to spatio-temporal performance similar to the baseline design with ideal gratings.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123.2513Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123.2513Z"><span>Coronal Flux Rope Catastrophe Associated With Internal <span class="hlt">Energy</span> <span class="hlt">Release</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhuang, Bin; Hu, Youqiu; Wang, Yuming; Zhang, Quanhao; Liu, Rui; Gou, Tingyu; Shen, Chenglong</p> <p>2018-04-01</p> <p>Magnetic <span class="hlt">energy</span> during the catastrophe was predominantly studied by the previous catastrophe works since it is believed to be the main <span class="hlt">energy</span> supplier for the solar eruptions. However, the contribution of other types of <span class="hlt">energies</span> during the catastrophe cannot be neglected. This paper studies the catastrophe of the coronal flux rope system in the solar wind background, with emphasis on the transformation of different types of <span class="hlt">energies</span> during the catastrophe. The coronal flux rope is characterized by its axial and poloidal magnetic fluxes and total mass. It is shown that a catastrophe can be triggered by not only an increase but also a decrease of the axial magnetic flux. Moreover, the internal <span class="hlt">energy</span> of the rope is found to be <span class="hlt">released</span> during the catastrophe so as to provide <span class="hlt">energy</span> for the upward eruption of the flux rope. As far as the magnetic <span class="hlt">energy</span> is concerned, it provides only part of the <span class="hlt">energy</span> <span class="hlt">release</span>, or even increases during the catastrophe, so the internal <span class="hlt">energy</span> may act as the dominant or even the unique <span class="hlt">energy</span> supplier during the catastrophe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=kinetic+AND+energy&pg=7&id=EJ528366','ERIC'); return false;" href="https://eric.ed.gov/?q=kinetic+AND+energy&pg=7&id=EJ528366"><span>Measurement of the Kinetic <span class="hlt">Energy</span> of a Body by Means of a <span class="hlt">Deformation</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Perez, Pedro J.; And Others</p> <p>1996-01-01</p> <p>Describes a technique that measures the <span class="hlt">deformation</span> produced in a plastic material by a falling ball in order to compute the ball's kinetic <span class="hlt">energy</span>. Varying the parameters produces accurate results and gives students a good understanding of the measurement of <span class="hlt">energy</span>. Combines various mechanical concepts that students have learned separately in…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/160811-flocculation-deformable-emulsion-droplets-interaction-energy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/160811-flocculation-deformable-emulsion-droplets-interaction-energy"><span>Flocculation of <span class="hlt">deformable</span> emulsion droplets. 2: Interaction <span class="hlt">energy</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Petsev, D.N.; Denkov, N.D.; Kralchevsky, P.A.</p> <p>1995-12-01</p> <p>The effect of different factors (drop radius, interfacial tension, Hamaker constant, electrolyte, micellar concentrations, etc.) on the interaction <span class="hlt">energy</span> of emulsion droplets is studied theoretically. It is demonstrated that the <span class="hlt">deformation</span> of the colliding droplets considerably affects the interaction <span class="hlt">energy</span>. The contributions of the electrostatic, van der Waals, depletion, steric, and oscillatory surface forces, as well as for the surface stretching and bending <span class="hlt">energies</span>, are estimated and discussed. The calculations show that the droplets interact as nondeformed spheres when the attractive interactions are weak. At stronger attractions an equilibrium plane parallel film is formed between the droplets, corresponding to minimummore » interaction <span class="hlt">energy</span> of the system. For droplets in concentrated micellar surfactant solutions the oscillatory surface forces become operative and one can observe several minima of the <span class="hlt">energy</span> surface,each corresponding to a metastable state with a different number of micellar layers inside the film formed between the droplets. The present theoretical analysis can find applications in predicting the behavior and stability of miniemulsions (containing micrometer and submicrometer droplets), as well as in interpretation of data obtained by light scattering, phase behavior, rheological and osmotic pressure measurements, etc.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29777038','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29777038"><span>Mechanical stability of the cell nucleus: roles played by the cytoskeleton in nuclear <span class="hlt">deformation</span> and strain recovery.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Xian; Liu, Haijiao; Zhu, Min; Cao, Changhong; Xu, Zhensong; Tsatskis, Yonit; Lau, Kimberly; Kuok, Chikin; Filleter, Tobin; McNeill, Helen; Simmons, Craig A; Hopyan, Sevan; Sun, Yu</p> <p>2018-05-18</p> <p>Extracellular forces transmitted through the cytoskeleton can <span class="hlt">deform</span> the cell nucleus. Large nuclear <span class="hlt">deformation</span> increases the risk of disrupting the nuclear envelope's integrity and causing DNA damage. Mechanical stability of the nucleus defines its capability of maintaining nuclear shape by minimizing nuclear <span class="hlt">deformation</span> and recovering strain when <span class="hlt">deformed</span>. Understanding the <span class="hlt">deformation</span> and recovery behavior of the nucleus requires characterization of nuclear viscoelastic properties. Here, we quantified the decoupled viscoelastic parameters of the cell membrane, cytoskeleton, and the nucleus. The results indicate that the cytoskeleton enhances nuclear mechanical stability by lowering the effective <span class="hlt">deformability</span> of the nucleus while maintaining nuclear sensitivity to mechanical stimuli. Additionally, the cytoskeleton decreases the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate of the nucleus and might thus prevent shape change-induced structural damage to chromatin. © 2018. Published by The Company of Biologists Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20120008792&hterms=ply&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3D.ply','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20120008792&hterms=ply&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3D.ply"><span>Adhesive-Bonded Composite Joint Analysis with Delaminated Surface Ply Using Strain-<span class="hlt">Energy</span> <span class="hlt">Release</span> Rate</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chadegani, Alireza; Yang, Chihdar; Smeltzer, Stanley S. III</p> <p>2012-01-01</p> <p>This paper presents an analytical model to determine the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate due to an interlaminar crack of the surface ply in adhesively bonded composite joints subjected to axial tension. Single-lap shear-joint standard test specimen geometry with thick bondline is followed for model development. The field equations are formulated by using the first-order shear-<span class="hlt">deformation</span> theory in laminated plates together with kinematics relations and force equilibrium conditions. The stress distributions for the adherends and adhesive are determined after the appropriate boundary and loading conditions are applied and the equations for the field displacements are solved. The system of second-order differential equations is solved to using the symbolic computation tool Maple 9.52 to provide displacements fields. The equivalent forces at the tip of the prescribed interlaminar crack are obtained based on interlaminar stress distributions. The strain <span class="hlt">energy</span> <span class="hlt">release</span> rate of the crack is then determined by using the crack closure method. Finite element analyses using the J integral as well as the crack closure method are performed to verify the developed analytical model. It has been shown that the results using the analytical method correlate well with the results from the finite element analyses. An attempt is made to predict the failure loads of the joints based on limited test data from the literature. The effectiveness of the inclusion of bondline thickness is justified when compared with the results obtained from the previous model in which a thin bondline and uniform adhesive stresses through the bondline thickness are assumed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10595E..10K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10595E..10K"><span><span class="hlt">Energy</span> <span class="hlt">release</span> for the actuation and deployment of muscle-inspired asymmetrically multistable chains</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kidambi, Narayanan; Zheng, Yisheng; Harne, Ryan L.; Wang, K. W.</p> <p>2018-03-01</p> <p>Animal locomotion and movement requires <span class="hlt">energy</span>, and the elastic potential <span class="hlt">energy</span> stored in skeletal muscle can facilitate movements that are otherwise energetically infeasible. A significant proportion of this <span class="hlt">energy</span> is captured and stored in the micro- and nano-scale constituents of muscle near the point of instability between asymmetric equilibrium states. This <span class="hlt">energy</span> may be quickly <span class="hlt">released</span> to enable explosive macroscopic motions or to reduce the metabolic cost of cyclic movements. Inspired by these behaviors, this research explores modular metastructures of bistable element chains and develops methods to <span class="hlt">release</span> the <span class="hlt">energy</span> stored in higher-potential system configurations. Quasi-static investigations reveal the role of state-transition pathways on the overall efficiency of the deployment event. It is shown that sequential, local <span class="hlt">release</span> of <span class="hlt">energy</span> from the bistable elements is more efficient than concurrent <span class="hlt">energy</span> <span class="hlt">release</span> achieved by applying a force at the free end of the structure. From dynamic analyses and experiments, it is shown that that the <span class="hlt">energy</span> <span class="hlt">released</span> from one bistable element can be used to activate the <span class="hlt">release</span> of <span class="hlt">energy</span> from subsequent links, reducing the actuation <span class="hlt">energy</span> required to extend or deploy the chain below that required for quasi-static deployment. This phenomenon is influenced by the level of asymmetry in the bistable constituents and the location of the impulse that initiates the deployment of the structure. The results provide insight into the design and behavior of asymmetrically multistable chains that can leverage stored potential <span class="hlt">energy</span> to enable efficient and effective system deployment and length change.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3827607','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3827607"><span>Novel characteristics of <span class="hlt">energy</span> spectrum for 3D Dirac oscillator analyzed via Lorentz covariant <span class="hlt">deformed</span> algebra</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Betrouche, Malika; Maamache, Mustapha; Choi, Jeong Ryeol</p> <p>2013-01-01</p> <p>We investigate the Lorentz-covariant <span class="hlt">deformed</span> algebra for Dirac oscillator problem, which is a generalization of Kempf <span class="hlt">deformed</span> algebra in 3 + 1 dimension of space-time, where Lorentz symmetry are preserved. The <span class="hlt">energy</span> spectrum of the system is analyzed by taking advantage of the corresponding wave functions with explicit spin state. We obtained entirely new results from our development based on Kempf algebra in comparison to the studies carried out with the non-Lorentz-covariant <span class="hlt">deformed</span> one. A novel result of this research is that the quantized relativistic <span class="hlt">energy</span> of the system in the presence of minimal length cannot grow indefinitely as quantum number n increases, but converges to a finite value, where c is the speed of light and β is a parameter that determines the scale of noncommutativity in space. If we consider the fact that the <span class="hlt">energy</span> levels of ordinary oscillator is equally spaced, which leads to monotonic growth of quantized <span class="hlt">energy</span> with the increment of n, this result is very interesting. The physical meaning of this consequence is discussed in detail. PMID:24225900</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_1");'>1</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li class="active"><span>3</span></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_3 --> <div id="page_4" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="61"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24225900','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24225900"><span>Novel characteristics of <span class="hlt">energy</span> spectrum for 3D Dirac oscillator analyzed via Lorentz covariant <span class="hlt">deformed</span> algebra.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Betrouche, Malika; Maamache, Mustapha; Choi, Jeong Ryeol</p> <p>2013-11-14</p> <p>We investigate the Lorentz-covariant <span class="hlt">deformed</span> algebra for Dirac oscillator problem, which is a generalization of Kempf <span class="hlt">deformed</span> algebra in 3 + 1 dimension of space-time, where Lorentz symmetry are preserved. The <span class="hlt">energy</span> spectrum of the system is analyzed by taking advantage of the corresponding wave functions with explicit spin state. We obtained entirely new results from our development based on Kempf algebra in comparison to the studies carried out with the non-Lorentz-covariant <span class="hlt">deformed</span> one. A novel result of this research is that the quantized relativistic <span class="hlt">energy</span> of the system in the presence of minimal length cannot grow indefinitely as quantum number n increases, but converges to a finite value, where c is the speed of light and β is a parameter that determines the scale of noncommutativity in space. If we consider the fact that the <span class="hlt">energy</span> levels of ordinary oscillator is equally spaced, which leads to monotonic growth of quantized <span class="hlt">energy</span> with the increment of n, this result is very interesting. The physical meaning of this consequence is discussed in detail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18823012','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18823012"><span>Mechanistic evaluation of alginate-HEC gelisphere compacts for controlled intrastriatal nicotine <span class="hlt">release</span> in Parkinson's disease.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Choonara, Yahya E; Pillay, Viness; Khan, Riaz A; Singh, Neha; du Toit, Lisa C</p> <p>2009-06-01</p> <p>This study focused on elucidating a mechanistic understanding in support of the multiple mechanisms which govern the formation of crosslinked alginate-hydroxyethylcellulose (Alg-HEC) gelispheres intended for the controlled intrastriatal <span class="hlt">release</span> of nicotine as a neuroprotectant in Parkinson's Disease. HEC was incorporated as a reinforcing "protective" colloidal polymer to induce interactions between the free carboxyl groups of alginate with hydroxylated HEC monomers. Gelispheres were compressed within an external poly(lactic-co-glycolic acid) (PLGA) matrix to further prolong the <span class="hlt">release</span> of nicotine. Sol-gel interconversion mechanisms, matrix <span class="hlt">deformability</span> moduli, matrix fracture <span class="hlt">energies</span> and chemometric models of the associated <span class="hlt">energy</span> paradigms were analyzed for their influence on the mechanism and extent of nicotine <span class="hlt">release</span>. Textural profiling demonstrated higher fracture <span class="hlt">energies</span> (7.94-26.69 x 10(-4) J) and lower <span class="hlt">deformability</span> moduli (12.24-58.36 N/mm) when gelispheres were cured in 2 M HCl as a postcuring step. Ba(2+) crosslinked gelispheres resulted in superiorly compact matrices with an increase in volume of 201-329% as compared to the Ca(2+) and Zn(2+) crosslinked matrices. The order of matrix compactness was as follows: Zn(2+) < Ca(2+) < Ba(2+). Molecular mechanisms of formation, interaction, conversion, and stability of sol-gel transitions depended on the type of crosslinker, crosslinking time, <span class="hlt">energy</span> transactions, and interactions with molecules of the hydration medium. Ba(2+) crosslinked gelispheres <span class="hlt">released</span> nicotine slower than Ca(2+) and Zn(2+) crosslinked gelispheres due to the higher <span class="hlt">energy</span> requirement for interconversion to sol while the <span class="hlt">energy</span> requirements for Ca(2+) and Zn(2+) was at a lower demand. Ba(2+) crosslinked gelispheres within PLGA matrices therefore retarded nicotine <span class="hlt">release</span> in a pseudo-zero-order manner over 21 days. (c) 2008 Wiley-Liss, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21690355','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21690355"><span>Multiscale approach to link red blood cell dynamics, shear viscosity, and ATP <span class="hlt">release</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Forsyth, Alison M; Wan, Jiandi; Owrutsky, Philip D; Abkarian, Manouk; Stone, Howard A</p> <p>2011-07-05</p> <p>RBCs are known to <span class="hlt">release</span> ATP, which acts as a signaling molecule to cause dilation of blood vessels. A reduction in the <span class="hlt">release</span> of ATP from RBCs has been linked to diseases such as type II diabetes and cystic fibrosis. Furthermore, reduced <span class="hlt">deformation</span> of RBCs has been correlated with myocardial infarction and coronary heart disease. Because ATP <span class="hlt">release</span> has been linked to cell <span class="hlt">deformation</span>, we undertook a multiscale approach to understand the links between single RBC dynamics, ATP <span class="hlt">release</span>, and macroscopic viscosity all at physiological shear rates. Our experimental approach included microfluidics, ATP measurements using a bioluminescent reaction, and rheology. Using microfluidics technology with high-speed imaging, we visualize the <span class="hlt">deformation</span> and dynamics of single cells, which are known to undergo motions such as tumbling, swinging, tanktreading, and <span class="hlt">deformation</span>. We report that shear thinning is not due to cellular <span class="hlt">deformation</span> as previously believed, but rather it is due to the tumbling-to-tanktreading transition. In addition, our results indicate that ATP <span class="hlt">release</span> is constant at shear stresses below a threshold (3 Pa), whereas above the threshold ATP <span class="hlt">release</span> is increased and accompanied by large cellular <span class="hlt">deformations</span>. Finally, performing experiments with well-known inhibitors, we show that the Pannexin 1 hemichannel is the main avenue for ATP <span class="hlt">release</span> both above and below the threshold, whereas, the cystic fibrosis transmembrane conductance regulator only contributes to <span class="hlt">deformation</span>-dependent ATP <span class="hlt">release</span> above the stress threshold.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28521230','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28521230"><span><span class="hlt">Energy</span> consumption and water-soluble protein <span class="hlt">release</span> by cell wall disruption of Nannochloropsis gaditana.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Safi, C; Cabas Rodriguez, L; Mulder, W J; Engelen-Smit, N; Spekking, W; van den Broek, L A M; Olivieri, G; Sijtsma, L</p> <p>2017-09-01</p> <p>Several cell disruption methods were tested on Nannochloropsis gaditana, to evaluate their efficiency in terms of cell disintegration, <span class="hlt">energy</span> input and <span class="hlt">release</span> of soluble proteins. High-pressure homogenization (HPH) and bead milling were the most efficient with >95% cell disintegration, ±50% (w/w) <span class="hlt">release</span> of total proteins and low <span class="hlt">energy</span> input (<0.5kWh.kg -1 biomass ). Enzymatic treatment required low <span class="hlt">energy</span> input (<0.34kWh.kg -1 biomass ), but it only <span class="hlt">released</span> ±35% protein (w/w). Pulsed Electric Field (PEF) was neither <span class="hlt">energy</span>-efficient (10.44kWh.kg -1 biomass ) nor successful for protein <span class="hlt">release</span> (only 10% proteins w/w) and cell disintegration. The <span class="hlt">release</span> of proteins after applying HPH and bead milling always required less intensive operating conditions for cell disruption. The <span class="hlt">energy</span> cost per unit of <span class="hlt">released</span> protein ranged from 0.15-0.25 €.kg Protein -1 in case of HPH, and up to 2-20 €.kg Protein -1 in case of PEF. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1402583-miniature-bulge-test-energy-release-rate-hiped-aluminum-aluminum-interfacial-fracture','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1402583-miniature-bulge-test-energy-release-rate-hiped-aluminum-aluminum-interfacial-fracture"><span>Miniature bulge test and <span class="hlt">energy</span> <span class="hlt">release</span> rate in HIPed aluminum/aluminum interfacial fracture</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Liu, C.; Lovato, M. L.; Clarke, K. D.</p> <p></p> <p>We summarize the development of a technique of using miniature bulge test combined with three-dimensional digital image correlation (3D-DIC) for measuring <span class="hlt">energy</span> <span class="hlt">release</span> rate or fracture toughness of bimaterial interface of thin metal foils. Furthermore, the <span class="hlt">energy</span> <span class="hlt">release</span> rate associated with the HIPed aluminum/aluminum interfacial delamination is determined experimentally using the proposed technique. Detailed discussions of the schemes of preparing and conducting the bulge test, and computing various quantities required for the determination of the <span class="hlt">energy</span> <span class="hlt">release</span> rate are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1402583-miniature-bulge-test-energy-release-rate-hiped-aluminum-aluminum-interfacial-fracture','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1402583-miniature-bulge-test-energy-release-rate-hiped-aluminum-aluminum-interfacial-fracture"><span>Miniature bulge test and <span class="hlt">energy</span> <span class="hlt">release</span> rate in HIPed aluminum/aluminum interfacial fracture</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Liu, C.; Lovato, M. L.; Clarke, K. D.; ...</p> <p>2017-10-13</p> <p>We summarize the development of a technique of using miniature bulge test combined with three-dimensional digital image correlation (3D-DIC) for measuring <span class="hlt">energy</span> <span class="hlt">release</span> rate or fracture toughness of bimaterial interface of thin metal foils. Furthermore, the <span class="hlt">energy</span> <span class="hlt">release</span> rate associated with the HIPed aluminum/aluminum interfacial delamination is determined experimentally using the proposed technique. Detailed discussions of the schemes of preparing and conducting the bulge test, and computing various quantities required for the determination of the <span class="hlt">energy</span> <span class="hlt">release</span> rate are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870052744&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DMagnetic%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870052744&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DMagnetic%2Benergy"><span>Observed form and action of the magnetic <span class="hlt">energy</span> <span class="hlt">release</span> in flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Machado, Marcos E.; Moore, Ronald L.</p> <p>1986-01-01</p> <p>The observable spatio-temporal characteristics of the <span class="hlt">energy</span> <span class="hlt">release</span> in flares and their association with the magnetic environment and tracers of field dynamics are reviewed. The observations indicate that impulsive phase manifestations, like particle acceleration, may be related to the formation of neutral sheets at the interface between interacting bipoles, but that the site for the bulk of the <span class="hlt">energy</span> <span class="hlt">release</span> is within closed loops rather than at the interaction site.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19850022925','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19850022925"><span>Residual thermal and moisture influences on the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate analysis of edge delamination</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Obrien, T. K.; Raju, I. S.; Garber, D. P.</p> <p>1985-01-01</p> <p>A laminated plate theory analysis is developed to calculate the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate associated with edge delamination growth in a composite laminate. The analysis includes the contribution of residual thermal and moisture stresses to the strain <span class="hlt">energy</span> <span class="hlt">released</span>. The strain <span class="hlt">energy</span> <span class="hlt">release</span> rate, G, increased when residual thermal effects were combined with applied mechanical strains, but then decreased when increasing moisture content was included. A quasi-three-dimensional finite element analysis indicated identical trends and demonstrated these same trends for the individual strain <span class="hlt">energy</span> <span class="hlt">release</span> rate components, G sub I and G sub II, associated with interlaminar tension and shear. An experimental study indicated that for T300/5208 graphite-epoxy composites, the inclusion of residual thermal and moisture stresses did not significantly alter the calculation of interlaminar fracture toughness from strain <span class="hlt">energy</span> <span class="hlt">release</span> rate analysis of edge delamination data taken at room temperature, ambient conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070038346','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070038346"><span>A Semi-Analytical Method for Determining the <span class="hlt">Energy</span> <span class="hlt">Release</span> Rate of Cracks in Adhesively-Bonded Single-Lap Composite Joints</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yang, Charles; Sun, Wenjun; Tomblin, John S.; Smeltzer, Stanley S., III</p> <p>2007-01-01</p> <p>A semi-analytical method for determining the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate due to a prescribed interface crack in an adhesively-bonded, single-lap composite joint subjected to axial tension is presented. The field equations in terms of displacements within the joint are formulated by using first-order shear <span class="hlt">deformable</span>, laminated plate theory together with kinematic relations and force equilibrium conditions. The stress distributions for the adherends and adhesive are determined after the appropriate boundary and loading conditions are applied and the equations for the field displacements are solved. Based on the adhesive stress distributions, the forces at the crack tip are obtained and the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate of the crack is determined by using the virtual crack closure technique (VCCT). Additionally, the test specimen geometry from both the ASTM D3165 and D1002 test standards are utilized during the derivation of the field equations in order to correlate analytical models with future test results. The system of second-order differential field equations is solved to provide the adherend and adhesive stress response using the symbolic computation tool, Maple 9. Finite element analyses using J-integral as well as VCCT were performed to verify the developed analytical model. The finite element analyses were conducted using the commercial finite element analysis software ABAQUS. The results determined using the analytical method correlated well with the results from the finite element analyses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1418771-total-kinetic-energy-release-fast-neutron-induced-fission','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1418771-total-kinetic-energy-release-fast-neutron-induced-fission"><span>The total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> in the fast neutron-induced fission of 232Th</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>King, Jonathan; Yanez, Ricardo; Loveland, Walter</p> <p></p> <p>Here, the post-emission total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> (TKE) in the neutron-induced fission of 232Th was measured (using white spectrum neutrons from LANSCE) for neutron <span class="hlt">energies</span> from E n=3 to 91MeV. In this <span class="hlt">energy</span> range the average post-neutron total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> decreases from 162.3±0.3 at E n=3 MeV to 154.9±0.3 MeV at E n=91 MeV. Analysis of the fission mass distributions indicates that the decrease in TKE with increasing neutron <span class="hlt">energy</span> is a combination of increasing yields of symmetric fission (which has a lower associated TKE) and a decrease in the TKE <span class="hlt">release</span> in asymmetric fission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1418771-total-kinetic-energy-release-fast-neutron-induced-fission','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1418771-total-kinetic-energy-release-fast-neutron-induced-fission"><span>The total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> in the fast neutron-induced fission of 232Th</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>King, Jonathan; Yanez, Ricardo; Loveland, Walter; ...</p> <p>2017-12-15</p> <p>Here, the post-emission total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> (TKE) in the neutron-induced fission of 232Th was measured (using white spectrum neutrons from LANSCE) for neutron <span class="hlt">energies</span> from E n=3 to 91MeV. In this <span class="hlt">energy</span> range the average post-neutron total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> decreases from 162.3±0.3 at E n=3 MeV to 154.9±0.3 MeV at E n=91 MeV. Analysis of the fission mass distributions indicates that the decrease in TKE with increasing neutron <span class="hlt">energy</span> is a combination of increasing yields of symmetric fission (which has a lower associated TKE) and a decrease in the TKE <span class="hlt">release</span> in asymmetric fission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1411605-observation-kaiser-effect-using-noble-gas-release-signals','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1411605-observation-kaiser-effect-using-noble-gas-release-signals"><span>Observation of the Kaiser Effect Using Noble Gas <span class="hlt">Release</span> Signals</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Bauer, Stephen J.</p> <p></p> <p>The Kaiser effect was defined in the early 1950s (Kaiser 1953) and was extensively reviewed and evaluated by Lavrov (2002) with a view toward understanding stress estimations. The Kaiser effect is a stress memory phenomenon which has most often been demonstrated in rock using acoustic emissions. During cyclic loading–unloading–reloading, the acoustic emissions are near zero until the load exceeds the level of the previous load cycle. Here, we sought to explore the Kaiser effect in rock using real-time noble gas <span class="hlt">release</span>. Laboratory studies using real-time mass spectrometry measurements during <span class="hlt">deformation</span> have quantified, to a degree, the types of gases releasedmore » (Bauer et al. 2016a, b), their <span class="hlt">release</span> rates and amounts during <span class="hlt">deformation</span>, estimates of permeability created from pore structure modifications during <span class="hlt">deformation</span> (Gardner et al. 2017) and the impact of mineral plasticity upon gas <span class="hlt">release</span>. We found that noble gases contained in brittle crystalline rock are readily <span class="hlt">released</span> during <span class="hlt">deformation</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1411605-observation-kaiser-effect-using-noble-gas-release-signals','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1411605-observation-kaiser-effect-using-noble-gas-release-signals"><span>Observation of the Kaiser Effect Using Noble Gas <span class="hlt">Release</span> Signals</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Bauer, Stephen J.</p> <p>2017-10-24</p> <p>The Kaiser effect was defined in the early 1950s (Kaiser 1953) and was extensively reviewed and evaluated by Lavrov (2002) with a view toward understanding stress estimations. The Kaiser effect is a stress memory phenomenon which has most often been demonstrated in rock using acoustic emissions. During cyclic loading–unloading–reloading, the acoustic emissions are near zero until the load exceeds the level of the previous load cycle. Here, we sought to explore the Kaiser effect in rock using real-time noble gas <span class="hlt">release</span>. Laboratory studies using real-time mass spectrometry measurements during <span class="hlt">deformation</span> have quantified, to a degree, the types of gases releasedmore » (Bauer et al. 2016a, b), their <span class="hlt">release</span> rates and amounts during <span class="hlt">deformation</span>, estimates of permeability created from pore structure modifications during <span class="hlt">deformation</span> (Gardner et al. 2017) and the impact of mineral plasticity upon gas <span class="hlt">release</span>. We found that noble gases contained in brittle crystalline rock are readily <span class="hlt">released</span> during <span class="hlt">deformation</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007APS..SHK.Q7003Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007APS..SHK.Q7003Z"><span>Post-Detonation <span class="hlt">Energy</span> <span class="hlt">Release</span> from TNT-Aluminum Explosives</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Fan; Anderson, John; Yoshinaka, Akio</p> <p>2007-06-01</p> <p>Detonation and post-detonation <span class="hlt">energy</span> <span class="hlt">release</span> from TNT and TNT-aluminum composite have been experimentally studied in an air-filled chamber, 26 m^3 in volume and 3 m in diameter. While TNT has a high oxygen deficiency, experiments with 1.1 kg to 4 kg charges yield <span class="hlt">energy</span> <span class="hlt">releases</span> reaching only 86% of theoretical equilibrium values, possibly due to the non-uniform mixing between the detonation products and air. In order to improve mixing and further increase afterburning <span class="hlt">energy</span>, large mass fractions of large aluminum particles are combined with TNT. The effect of particle distribution is also investigated in two composite configurations, whereby the aluminum particles are uniformly mixed in cast TNT or arranged in a shell surrounding a TNT cylinder. It is shown that the TNT-aluminum composite outperforms pure TNT, while improved performance is achieved for the shell configuration due to enhanced spatial mixing of hot fuels with oxidizing gases. Comparisons with the equilibrium theory and a liquid-based aluminized composite explosive (with an oxygen deficiency less than that of TNT) are conducted to further explore the mixing and afterburning mechanism.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014NatMa..13..501L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014NatMa..13..501L"><span>Pervasive nanoscale <span class="hlt">deformation</span> twinning as a catalyst for efficient <span class="hlt">energy</span> dissipation in a bioceramic armour</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Ling; Ortiz, Christine</p> <p>2014-05-01</p> <p>Hierarchical composite materials design in biological exoskeletons achieves penetration resistance through a variety of <span class="hlt">energy</span>-dissipating mechanisms while simultaneously balancing the need for damage localization to avoid compromising the mechanical integrity of the entire structure and to maintain multi-hit capability. Here, we show that the shell of the bivalve Placuna placenta (~99 wt% calcite), which possesses the unique optical property of ~80% total transmission of visible light, simultaneously achieves penetration resistance and <span class="hlt">deformation</span> localization via increasing <span class="hlt">energy</span> dissipation density (0.290 ± 0.072 nJ μm-3) by approximately an order of magnitude relative to single-crystal geological calcite (0.034 ± 0.013 nJ μm-3). P. placenta, which is composed of a layered assembly of elongated diamond-shaped calcite crystals, undergoes pervasive nanoscale <span class="hlt">deformation</span> twinning (width ~50 nm) surrounding the penetration zone, which catalyses a series of additional inelastic <span class="hlt">energy</span> dissipating mechanisms such as interfacial and intracrystalline nanocracking, viscoplastic stretching of interfacial organic material, and nanograin formation and reorientation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PCM....37..535P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PCM....37..535P"><span>The notion of ``distinguishability'' between bulk elastic parameters on the basis of the Gibbs <span class="hlt">deformation</span> <span class="hlt">energy</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pavese, Alessandro; Diella, Valeria</p> <p>2010-09-01</p> <p>The present work aims in discussing a principle that distinguishes between elastic parameters sets, \\{ Upphi \\} equiv \\{ K0 , K^', V0 ,ldots\\} , on the basis of an energetic criterion: once a reference set, \\{ UpphiR \\} , is given, another one can be fixed, left\\{ {Upphi_{ min } } right\\} , so that they are as close as possible to each other, but yield non-equivalent <span class="hlt">deformation</span> <span class="hlt">energy</span> curves Updelta G(\\{ Upphi \\} )_{text{<span class="hlt">deform</span>}} , i.e. they give Updelta G(\\{ UpphiR \\} )_{text{<span class="hlt">deform</span>}} and Updelta G(\\{ Upphi_{ min } \\} )_{text{<span class="hlt">deform</span>}} such that left| {Updelta G(\\{ Upphi_{ min } \\} )_{text{<span class="hlt">deform</span>}} - Updelta G(\\{ UpphiR \\} )_{text{<span class="hlt">deform</span>}} } right| ge 1× σ [Updelta G_{text{<span class="hlt">deform</span>}} ]. Δ G <span class="hlt">deform</span>, calculated using the equation of state (EoS), and its uncertainty σ[Δ G <span class="hlt">deform</span>], obtained by a propagation of the errors affecting \\{ Upphi \\} are crucial to fix which mineral assemblage forms at P- T conditions and allow one to assess the reliability of such a prediction. We explore some properties related to the principle introduced, using the average values of the elastic parameters found in literature and related uncertainties for di-octahedral mica, olivine, garnet and clinopyroxene. Two elementary applications are briefly discussed: the effect of refining V 0 in fitting EoSs to P-V experimental data, in the case of garnet and omphacite, and the phengite 3 T-2 M 1 relative stability, controlled by pressure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27762047','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27762047"><span>A Responsive Battery with Controlled <span class="hlt">Energy</span> <span class="hlt">Release</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Xiaopeng; Gao, Jian; Cheng, Zhihua; Chen, Nan; Qu, Liangti</p> <p>2016-11-14</p> <p>A new type of responsive battery with the fascinating feature of pressure perceptibility has been developed, which can spontaneously, timely and reliably control the power outputs (e.g., current and voltage) in response to pressure changes. The device design is based on the structure of the Zn-air battery, in which graphene-coated sponge serves as pressure-sensitive air cathode that endows the whole system with the capability of self-controlled <span class="hlt">energy</span> <span class="hlt">release</span>. The responsive batteries exhibit superior battery performance with high open-circuit voltage (1.3 V), and competitive areal capacity of 1.25 mAh cm -2 . This work presents an important move towards next-generation intelligent <span class="hlt">energy</span> storage devices with <span class="hlt">energy</span> management function. © 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AAS...23121901C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AAS...23121901C"><span>The Dark <span class="hlt">Energy</span> Survey First Data <span class="hlt">Release</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carrasco Kind, Matias</p> <p>2018-01-01</p> <p>In this talk I will announce and highlight the main components of the first public data <span class="hlt">release</span> (DR1) coming from the Dark <span class="hlt">Energy</span> Survey (DES).In January 2016, the DES survey made available, in a simple unofficial <span class="hlt">release</span> to the astronomical community, the first set of products. This data was taken and studied during the DES Science Verification period consisting on roughly 250 sq. degrees and 25 million objects at a mean depth of i=23.7 that led to over 80 publications from DES scientist.The DR1 <span class="hlt">release</span> is the first official <span class="hlt">release</span> from the main survey and it consists on the observations taken during the first 3 seasons from August 2013 to February 2016 (about 100 nights each season) of the survey which cover the entire DES footprint. All of the Single Epoch Images and the Year 3 Coadded images distributed in 10223 tiles are available for download in this <span class="hlt">release</span>. The catalogs provide astrometry, photometry and basic classification for near 400M objects in roughly 5000 sq. degrees on the southern hemisphere with a approximate mean depth of i=23.3. Complementary footprint, masking and depth information is also available. All of the software used during the generation of these products are open sourced and have been made available through the Github DES Organization. Images, data and other sub products have been possible through the international and collaborative effort of all 25 institutions involved in DES and are available for exploration and download through the interfaces provided by a partnership between NCSA, NOAO and LIneA.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017IJMPA..3250112N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017IJMPA..3250112N"><span><span class="hlt">Deforming</span> regular black holes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Neves, J. C. S.</p> <p>2017-06-01</p> <p>In this work, we have <span class="hlt">deformed</span> regular black holes which possess a general mass term described by a function which generalizes the Bardeen and Hayward mass functions. By using linear constraints in the <span class="hlt">energy</span>-momentum tensor to generate metrics, the solutions presented in this work are either regular or singular. That is, within this approach, it is possible to generate regular or singular black holes from regular or singular black holes. Moreover, contrary to the Bardeen and Hayward regular solutions, the <span class="hlt">deformed</span> regular black holes may violate the weak <span class="hlt">energy</span> condition despite the presence of the spherical symmetry. Some comments on accretion of <span class="hlt">deformed</span> black holes in cosmological scenarios are made.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28508907','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28508907"><span>An effective trigger for <span class="hlt">energy</span> <span class="hlt">release</span> of vinylheptafulvene-based solar heat batteries.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cacciarini, Martina; Vlasceanu, Alexandru; Jevric, Martyn; Nielsen, Mogens Brøndsted</p> <p>2017-05-30</p> <p>Stoichiometric copper(i) tetrakis(acetonitrile) is found to activate the thermal ring-closure reaction of a series of high-<span class="hlt">energy</span> vinylheptafulvene isomers to the corresponding low-<span class="hlt">energy</span> and photoactive dihydroazulenes, allowing the <span class="hlt">release</span> of <span class="hlt">energy</span> upon request.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_2");'>2</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li class="active"><span>4</span></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_4 --> <div id="page_5" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="81"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJC...78..243A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJC...78..243A"><span>Running of the spectral index in <span class="hlt">deformed</span> matter bounce scenarios with Hubble-rate-dependent dark <span class="hlt">energy</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arab, M.; Khodam-Mohammadi, A.</p> <p>2018-03-01</p> <p>As a <span class="hlt">deformed</span> matter bounce scenario with a dark <span class="hlt">energy</span> component, we propose a <span class="hlt">deformed</span> one with running vacuum model (RVM) in which the dark <span class="hlt">energy</span> density ρ _{Λ } is written as a power series of H^2 and \\dot{H} with a constant equation of state parameter, same as the cosmological constant, w=-1. Our results in analytical and numerical point of views show that in some cases same as Λ CDM bounce scenario, although the spectral index may achieve a good consistency with observations, a positive value of running of spectral index (α _s) is obtained which is not compatible with inflationary paradigm where it predicts a small negative value for α _s. However, by extending the power series up to H^4, ρ _{Λ }=n_0+n_2 H^2+n_4 H^4, and estimating a set of consistent parameters, we obtain the spectral index n_s, a small negative value of running α _s and tensor to scalar ratio r, which these reveal a degeneracy between <span class="hlt">deformed</span> matter bounce scenario with RVM-DE and inflationary cosmology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26897489','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26897489"><span>An Algorithmic, Pie-Crusting Medial Soft Tissue <span class="hlt">Release</span> Reduces the Need for Constrained Inserts Patients With Severe Varus <span class="hlt">Deformity</span> Undergoing Total Knee Arthroplasty.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Goudarz Mehdikhani, Kaveh; Morales Moreno, Beatriz; Reid, Jeremy J; de Paz Nieves, Ana; Lee, Yuo-Yu; González Della Valle, Alejandro</p> <p>2016-07-01</p> <p>We studied the need to use a constrained insert for residual intraoperative instability and the 1-year result of patients undergoing total knee arthroplasty (TKA) for a varus <span class="hlt">deformity</span>. In a control group, a "classic" subperiosteal <span class="hlt">release</span> of the medial soft tissue sleeve was performed as popularized by pioneers of TKA. In the study group, an algorithmic approach that selectively <span class="hlt">releases</span> and pie-crusts posteromedial structures in extension and anteromedial structures in flexion was used. All surgeries were performed by a single surgeon using measured resection technique, and posterior-stabilized, cemented implants. There were 228 TKAs in the control group and 188 in the study group. Outcome variables included the use of a constrained insert, and the Knee Society Score at 6 weeks, 4 months, and 1 year postoperatively. The effect of the <span class="hlt">release</span> technique on use of constrained inserts and clinical outcomes were analyzed in a multivariate model controlling for age, sex, body mass index, and severity of <span class="hlt">deformity</span>. The use of constrained inserts was significantly lower in study than in control patients (8% vs 18%; P = .002). There was no difference in the Knee Society Score and range of motion between the groups at last follow-up. No patient developed postoperative medial instability. This algorithmic, pie-crusting <span class="hlt">release</span> technique resulted in a significant reduction in the use of constrained inserts with no detrimental effects in clinical results, joint function, and stability. As constrained TKA implants are more costly than nonconstrained ones, if the adopted technique proves to be safe in the long term, it may cause a positive shift in value for hospitals and cost savings in the health care system. Copyright © 2016 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4823781','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4823781"><span>A <span class="hlt">deformation</span> <span class="hlt">energy</span>-based model for predicting nucleosome dyads and occupancy</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Liu, Guoqing; Xing, Yongqiang; Zhao, Hongyu; Wang, Jianying; Shang, Yu; Cai, Lu</p> <p>2016-01-01</p> <p>Nucleosome plays an essential role in various cellular processes, such as DNA replication, recombination, and transcription. Hence, it is important to decode the mechanism of nucleosome positioning and identify nucleosome positions in the genome. In this paper, we present a model for predicting nucleosome positioning based on DNA <span class="hlt">deformation</span>, in which both bending and shearing of the nucleosomal DNA are considered. The model successfully predicted the dyad positions of nucleosomes assembled in vitro and the in vitro map of nucleosomes in Saccharomyces cerevisiae. Applying the model to Caenorhabditis elegans and Drosophila melanogaster, we achieved satisfactory results. Our data also show that shearing <span class="hlt">energy</span> of nucleosomal DNA outperforms bending <span class="hlt">energy</span> in nucleosome occupancy prediction and the ability to predict nucleosome dyad positions is attributed to bending <span class="hlt">energy</span> that is associated with rotational positioning of nucleosomes. PMID:27053067</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1510426V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1510426V"><span><span class="hlt">Deformation</span> and failure of single- and multi-phase silicate liquids: seismic precursors and mechanical work</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vasseur, Jeremie; Lavallée, Yan; Hess, Kai-Uwe; Wassermann, Joachim; Dingwell, Donald B.</p> <p>2013-04-01</p> <p>Along with many others, volcanic unrest is regarded as a catastrophic material failure phenomenon and is often preceded by diverse precursory signals. Although a volcanic system intrinsically behave in a non-linear and stochastic way, these precursors display systematic evolutionary trends to upcoming eruptions. Seismic signals in particular are in general dramatically increasing prior to an eruption and have been extensively reported to show accelerating rates through time, as well as in the laboratory before failure of rock samples. At the lab-scale, acoustic emissions (AE) are high frequency transient stress waves used to track fracture initiation and propagation inside a rock sample. Synthesized glass samples featuring a range of porosities (0 - 30%) and natural rock samples from volcán de Colima, Mexico, have been failed under high temperature uniaxial compression experiments at constant stresses and strain rates. Using the monitored AEs and the generated mechanical work during <span class="hlt">deformation</span>, we investigated the evolutionary trends of <span class="hlt">energy</span> patterns associated to different degrees of heterogeneity. We observed that the failure of dense, poorly porous glasses is achieved by exceeding elevated strength and thus requires a significant accumulation of strain, meaning only pervasive small-scale cracking is occurring. More porous glasses as well as volcanic samples need much lower applied stress and <span class="hlt">deformation</span> to fail, as fractures are nucleating, propagating and coalescing into localized large-scale cracks, taking the advantage of the existence of numerous defects (voids for glasses, voids and crystals for volcanic rocks). These observations demonstrate that the mechanical work generated through cracking is efficiently distributed inside denser and more homogeneous samples, as underlined by the overall lower AE <span class="hlt">energy</span> <span class="hlt">released</span> during experiments. In contrast, the quicker and larger AE <span class="hlt">energy</span> <span class="hlt">released</span> during the loading of heterogeneous samples shows that the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140001072','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140001072"><span>The Role of Compressibility in <span class="hlt">Energy</span> <span class="hlt">Release</span> by Magnetic Reconnection</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Birn, J.; Borovosky, J. E.; Hesse, M.</p> <p>2012-01-01</p> <p>Using resistive compressible magnetohydrodynamics, we investigate the <span class="hlt">energy</span> <span class="hlt">release</span> and transfer by magnetic reconnection in finite (closed or periodic) systems. The emphasis is on the magnitude of <span class="hlt">energy</span> <span class="hlt">released</span> and transferred to plasma heating in configurations that range from highly compressible to incompressible, based on the magnitude of the background beta (ratio of plasma pressure over magnetic pressure) and of a guide field in two-dimensional reconnection. As expected, the system becomes more incompressible, and the role of compressional heating diminishes, with increasing beta or increasing guide field. Nevertheless, compressional heating may dominate over Joule heating for values of the guide field of 2 or 3 (in relation to the reconnecting magnetic field component) and beta of 5-10. This result stems from the strong localization of the dissipation near the reconnection site, which is modeled based on particle simulation results. Imposing uniform resistivity, corresponding to a Lundquist number of 10(exp 3) to 10(exp 4), leads to significantly larger Ohmic heating. Increasing incompressibility greatly reduces the magnetic flux transfer and the amount of <span class="hlt">energy</span> <span class="hlt">released</span>, from approx. 10% of the <span class="hlt">energy</span> associated with the reconnecting field component, for zero guide field and low beta, to approx. 0.2%-0.4% for large values of the guide field B(sub y0) > 5 or large beta. The results demonstrate the importance of taking into account plasma compressibility and localization of dissipation in investigations of heating by turbulent reconnection, possibly relevant for solar wind or coronal heating.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140002301','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140002301"><span>Fabrication Methods for Adaptive <span class="hlt">Deformable</span> Mirrors</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Toda, Risaku; White, Victor E.; Manohara, Harish; Patterson, Keith D.; Yamamoto, Namiko; Gdoutos, Eleftherios; Steeves, John B.; Daraio, Chiara; Pellegrino, Sergio</p> <p>2013-01-01</p> <p>Previously, it was difficult to fabricate <span class="hlt">deformable</span> mirrors made by piezoelectric actuators. This is because numerous actuators need to be precisely assembled to control the surface shape of the mirror. Two approaches have been developed. Both approaches begin by depositing a stack of piezoelectric films and electrodes over a silicon wafer substrate. In the first approach, the silicon wafer is removed initially by plasmabased reactive ion etching (RIE), and non-plasma dry etching with xenon difluoride (XeF2). In the second approach, the actuator film stack is immersed in a liquid such as deionized water. The adhesion between the actuator film stack and the substrate is relatively weak. Simply by seeping liquid between the film and the substrate, the actuator film stack is gently <span class="hlt">released</span> from the substrate. The <span class="hlt">deformable</span> mirror contains multiple piezoelectric membrane layers as well as multiple electrode layers (some are patterned and some are unpatterned). At the piezolectric layer, polyvinylidene fluoride (PVDF), or its co-polymer, poly(vinylidene fluoride trifluoroethylene P(VDF-TrFE) is used. The surface of the mirror is coated with a reflective coating. The actuator film stack is fabricated on silicon, or silicon on insulator (SOI) substrate, by repeatedly spin-coating the PVDF or P(VDFTrFE) solution and patterned metal (electrode) deposition. In the first approach, the actuator film stack is prepared on SOI substrate. Then, the thick silicon (typically 500-micron thick and called handle silicon) of the SOI wafer is etched by a deep reactive ion etching process tool (SF6-based plasma etching). This deep RIE stops at the middle SiO2 layer. The middle SiO2 layer is etched by either HF-based wet etching or dry plasma etch. The thin silicon layer (generally called a device layer) of SOI is removed by XeF2 dry etch. This XeF2 etch is very gentle and extremely selective, so the <span class="hlt">released</span> mirror membrane is not damaged. It is possible to replace SOI with silicon</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24681646','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24681646"><span>Pervasive nanoscale <span class="hlt">deformation</span> twinning as a catalyst for efficient <span class="hlt">energy</span> dissipation in a bioceramic armour.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Ling; Ortiz, Christine</p> <p>2014-05-01</p> <p>Hierarchical composite materials design in biological exoskeletons achieves penetration resistance through a variety of <span class="hlt">energy</span>-dissipating mechanisms while simultaneously balancing the need for damage localization to avoid compromising the mechanical integrity of the entire structure and to maintain multi-hit capability. Here, we show that the shell of the bivalve Placuna placenta (~99 wt% calcite), which possesses the unique optical property of ~80% total transmission of visible light, simultaneously achieves penetration resistance and <span class="hlt">deformation</span> localization via increasing <span class="hlt">energy</span> dissipation density (0.290 ± 0.072 nJ μm(-3)) by approximately an order of magnitude relative to single-crystal geological calcite (0.034 ± 0.013 nJ μm(-3)). P. placenta, which is composed of a layered assembly of elongated diamond-shaped calcite crystals, undergoes pervasive nanoscale <span class="hlt">deformation</span> twinning (width ~50 nm) surrounding the penetration zone, which catalyses a series of additional inelastic <span class="hlt">energy</span> dissipating mechanisms such as interfacial and intracrystalline nanocracking, viscoplastic stretching of interfacial organic material, and nanograin formation and reorientation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..294a2041C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..294a2041C"><span>Identification of exponent from load-<span class="hlt">deformation</span> relation for soft materials from impact tests</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ciornei, F. C.; Alaci, S.; Romanu, I. C.; Ciornei, M. C.; Sopon, G.</p> <p>2018-01-01</p> <p>When two bodies are brought into contact, the magnitude of occurring reaction forces increase together with the amplitude of <span class="hlt">deformations</span>. The load-<span class="hlt">deformation</span> dependency of two contacting bodies is described by a function having the form F = Cxα . An accurate illustration of this relationship assumes finding the precise coefficient C and exponent α. This representation proved to be very useful in hardness tests, in dynamic systems modelling or in considerations upon the elastic-plastic ratio concerning a Hertzian contact. The classical method for identification of the exponent consists in finding it from quasi-static tests. The drawback of the method is the fact that the accurate estimation of the exponent supposes precise identification of the instant of contact initiation. To overcome this aspect, the following observation is exploited: during an impact process, the dissipated <span class="hlt">energy</span> is converted into heat <span class="hlt">released</span> by internal friction in the materials and <span class="hlt">energy</span> for plastic <span class="hlt">deformations</span>. The paper is based on the remark that for soft materials the hysteresis curves obtained for a static case are similar to the ones obtained for medium velocities. Furthermore, utilizing the fact that for the restitution phase the load-<span class="hlt">deformation</span> dependency is elastic, a method for finding the α exponent for compression phase is proposed. The maximum depth of the plastic <span class="hlt">deformations</span> obtained for a series of collisions, by launching, from different heights, a steel ball in free falling on an immobile prism made of soft material, is evaluated by laser profilometry method. The condition that the area of the hysteresis loop equals the variation of kinetical <span class="hlt">energy</span> of the ball is imposed and two tests are required for finding the exponent. Five collisions from different launching heights of the ball were taken into account. For all the possible impact-pair cases, the values of the exponent were found and close values were obtained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JPhA...44J5303A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JPhA...44J5303A"><span>Accidental degeneracies in nonlinear quantum <span class="hlt">deformed</span> systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aleixo, A. N. F.; Balantekin, A. B.</p> <p>2011-09-01</p> <p>We construct a multi-parameter nonlinear <span class="hlt">deformed</span> algebra for quantum confined systems that includes many other <span class="hlt">deformed</span> models as particular cases. We demonstrate that such systems exhibit the property of accidental pairwise <span class="hlt">energy</span> level degeneracies. We also study, as a special case of our multi-parameter <span class="hlt">deformation</span> formalism, the extension of the Tamm-Dancoff cutoff <span class="hlt">deformed</span> oscillator and the occurrence of accidental pairwise degeneracy in the <span class="hlt">energy</span> levels of the <span class="hlt">deformed</span> system. As an application, we discuss the case of a trigonometric Rosen-Morse potential, which is successfully used in models for quantum confined systems, ranging from electrons in quantum dots to quarks in hadrons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ASPC..510..289P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ASPC..510..289P"><span>Flare <span class="hlt">Energy</span> <span class="hlt">Release</span>: Internal Conflict, Contradiction with High Resolution Observations, Possible Solutions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pustilnik, L.</p> <p>2017-06-01</p> <p>All accepted paradigm of solar and stellar flares <span class="hlt">energy</span> <span class="hlt">release</span> based on 2 whales: 1. Source of <span class="hlt">energy</span> is free <span class="hlt">energy</span> of non-potential force free magnetic field in atmosphere above active region; 2. Process of ultrafast dissipation of magnetic fields is Reconnection in Thin Turbulent Current Sheet (RTTCS). Progress in observational techniques in last years provided ultra-high spatial resolution and in physics of turbulent plasma showed that real situation is much more complicated and standard approach is in contradiction both with observations and with problem of RTTCS stability. We present critical analysis of classic models of pre-flare <span class="hlt">energy</span> accumulation and its dissipation during flare <span class="hlt">energy</span> <span class="hlt">release</span> from pioneer works Giovanelli (1939, 1947) up to topological reconnection. We show that all accepted description of global force-free fields as source of future flare cannot be agreed with discovered in last years fine and ultra-fine current-magnetic structure included numerouse arcs-threads with diameters up to 100 km with constant sequence from photosphere to corona. This magnetic skeleton of thin current magnetic threads with strong interaction between them is main source of reserved magnetic <span class="hlt">energy</span> insolar atmosphere. Its dynamics will be controlled by percolation of magnetic stresses through network of current-magnetic threads with transition to flare state caused by critical value of global current. We show that thin turbulent current sheet is absolutely unstable configuration both caused by splitting to numerous linear currents by dissipative modes like to tearing, and as sequence of suppress of plasma turbulence caused by anomalous heating of turbulent plasma. In result of these factors primary RTTCS will be disrupted in numerous turbulent and normal plasma domains like to resistors network. Current propagation through this network will have percolation character with all accompanied properties of percolated systems: self-organization with formation power</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29319351','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29319351"><span>Amniotic Constriction Bands: Secondary <span class="hlt">Deformities</span> and Their Treatments.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Drury, Benjamin T; Rayan, Ghazi M</p> <p>2018-01-01</p> <p>The purpose of this study was to report the surgical treatment experience of patients with amniotic constriction bands (ACB) over a 35-year interval and detail consequential limb <span class="hlt">deformities</span> with emphasis on hands and upper extremities, along with the nature and frequency of their surgical treatment methods. Fifty-one patients were identified; 26 were males and 25 females. The total number of <span class="hlt">deformities</span> was listed. The total number of operations, individual procedures, and operations plus procedures that were done for each patient and their frequency were recorded. The total number of operations was 117, and total number of procedures was 341. More procedures were performed on the upper extremity (85%) than the lower extremity (15%). Including the primary <span class="hlt">deformity</span> ACB, 16 different hand <span class="hlt">deformities</span> secondary to ACB were encountered. Sixteen different surgical methods for the upper extremity were utilized; a primary procedure for ACB and secondary reconstructions for all secondary <span class="hlt">deformities</span>. Average age at the time of the first procedure was 9.3 months. The most common procedures performed, in order of frequency, were excision of ACB plus Z-plasty, <span class="hlt">release</span> of partial syndactyly, <span class="hlt">release</span> of fenestrated syndactyly, full-thickness skin grafts, resection of digital bony overgrowth from amputation stumps, and deepening of first and other digital web spaces. Many hand and upper extremity <span class="hlt">deformities</span> secondary to ACB are encountered. Children with ACB may require more than one operation including multiple procedures. Numerous surgical methods of reconstruction for these children's secondary <span class="hlt">deformities</span> are necessary in addition to the customary primary procedure of excision of ACB and Z-plasty.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19770035709&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DMagnetic%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19770035709&hterms=Magnetic+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DMagnetic%2Benergy"><span><span class="hlt">Energy</span> <span class="hlt">released</span> by the interaction of coronal magnetic fields</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sheeley, N. R., Jr.</p> <p>1976-01-01</p> <p>Comparisons between coronal spectroheliograms and photospheric magnetograms are presented to support the idea that as coronal magnetic fields interact, a process of field-line reconnection usually takes place as a natural way of preventing magnetic stresses from building up in the lower corona. This suggests that the <span class="hlt">energy</span> which would have been stored in stressed fields is continuously <span class="hlt">released</span> as kinetic <span class="hlt">energy</span> of material being driven aside to make way for the reconnecting fields. However, this kinetic <span class="hlt">energy</span> is negligible compared with the thermal <span class="hlt">energy</span> of the coronal plasma. Therefore, it appears that these slow adjustments of coronal magnetic fields cannot account for even the normal heating of the corona, much less the energetic events associated with solar flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22745740','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22745740"><span>Blast shock wave mitigation using the hydraulic <span class="hlt">energy</span> redirection and <span class="hlt">release</span> technology.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Yun; Huang, Wei; Constantini, Shlomi</p> <p>2012-01-01</p> <p>A hydraulic <span class="hlt">energy</span> redirection and <span class="hlt">release</span> technology has been developed for mitigating the effects of blast shock waves on protected objects. The technology employs a liquid-filled plastic tubing as a blast overpressure transformer to transfer kinetic <span class="hlt">energy</span> of blast shock waves into hydraulic <span class="hlt">energy</span> in the plastic tubings. The hydraulic <span class="hlt">energy</span> is redirected through the plastic tubings to the openings at the lower ends, and then is quickly <span class="hlt">released</span> with the liquid flowing out through the openings. The samples of the specifically designed body armor in which the liquid-filled plastic tubings were installed vertically as the outer layer of the body armor were tested. The blast test results demonstrated that blast overpressure behind the body armor samples was remarkably reduced by 97% in 0.2 msec after the liquid flowed out of its appropriate volume through the openings. The results also suggested that a volumetric liquid surge might be created when kinetic <span class="hlt">energy</span> of blast shock wave was transferred into hydraulic <span class="hlt">energy</span> to cause a rapid physical movement or displacement of the liquid. The volumetric liquid surge has a strong destructive power, and can cause a noncontact, remote injury in humans (such as blast-induced traumatic brain injury and post-traumatic stress disorder) if it is created in cardiovascular system. The hydraulic <span class="hlt">energy</span> redirection and <span class="hlt">release</span> technology can successfully mitigate blast shock waves from the outer surface of the body armor. It should be further explored as an innovative approach to effectively protect against blast threats to civilian and military personnel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3379975','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3379975"><span>Blast Shock Wave Mitigation Using the Hydraulic <span class="hlt">Energy</span> Redirection and <span class="hlt">Release</span> Technology</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chen, Yun; Huang, Wei; Constantini, Shlomi</p> <p>2012-01-01</p> <p>A hydraulic <span class="hlt">energy</span> redirection and <span class="hlt">release</span> technology has been developed for mitigating the effects of blast shock waves on protected objects. The technology employs a liquid-filled plastic tubing as a blast overpressure transformer to transfer kinetic <span class="hlt">energy</span> of blast shock waves into hydraulic <span class="hlt">energy</span> in the plastic tubings. The hydraulic <span class="hlt">energy</span> is redirected through the plastic tubings to the openings at the lower ends, and then is quickly <span class="hlt">released</span> with the liquid flowing out through the openings. The samples of the specifically designed body armor in which the liquid-filled plastic tubings were installed vertically as the outer layer of the body armor were tested. The blast test results demonstrated that blast overpressure behind the body armor samples was remarkably reduced by 97% in 0.2 msec after the liquid flowed out of its appropriate volume through the openings. The results also suggested that a volumetric liquid surge might be created when kinetic <span class="hlt">energy</span> of blast shock wave was transferred into hydraulic <span class="hlt">energy</span> to cause a rapid physical movement or displacement of the liquid. The volumetric liquid surge has a strong destructive power, and can cause a noncontact, remote injury in humans (such as blast-induced traumatic brain injury and post-traumatic stress disorder) if it is created in cardiovascular system. The hydraulic <span class="hlt">energy</span> redirection and <span class="hlt">release</span> technology can successfully mitigate blast shock waves from the outer surface of the body armor. It should be further explored as an innovative approach to effectively protect against blast threats to civilian and military personnel. PMID:22745740</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MARH16003I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MARH16003I"><span>Unleashing elastic <span class="hlt">energy</span>: dynamics of <span class="hlt">energy</span> <span class="hlt">release</span> in rubber bands and impulsive biological systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ilton, Mark; Cox, Suzanne; Egelmeers, Thijs; Patek, S. N.; Crosby, Alfred J.</p> <p></p> <p>Impulsive biological systems - which include mantis shrimp, trap-jaw ants, and venus fly traps - can reach high speeds by using elastic elements to store and rapidly <span class="hlt">release</span> <span class="hlt">energy</span>. The material behavior and shape changes critical to achieving rapid <span class="hlt">energy</span> <span class="hlt">release</span> in these systems are largely unknown due to limitations of materials testing instruments operating at high speed and large displacement. In this work, we perform fundamental, proof-of-concept measurements on the tensile retraction of elastomers. Using high speed imaging, the kinematics of retraction are measured for elastomers with varying mechanical properties and geometry. Based on the kinematics, the rate of <span class="hlt">energy</span> dissipation in the material is determined as a function of strain and strain-rate, along with a scaling relation which describes the dependence of maximum velocity on material properties. Understanding this scaling relation along with the material failure limits of the elastomer allows the prediction of material properties required for optimal performance. We demonstrate this concept experimentally by optimizing for maximum velocity in our synthetic model system, and achieve retraction velocities that exceed those in biological impulsive systems. This model system provides a foundation for future work connecting continuum performance to molecular architecture in impulsive systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870011944','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870011944"><span>Convergence of strain <span class="hlt">energy</span> <span class="hlt">release</span> rate components for edge-delaminated composite laminates</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Raju, I. S.; Crews, J. H., Jr.; Aminpour, M. A.</p> <p>1987-01-01</p> <p>Strain <span class="hlt">energy</span> <span class="hlt">release</span> rates for edge delaminated composite laminates were obtained using quasi 3 dimensional finite element analysis. The problem of edge delamination at the -35/90 interfaces of an 8-ply composite laminate subjected to uniform axial strain was studied. The individual components of the strain <span class="hlt">energy</span> <span class="hlt">release</span> rates did not show convergence as the delamination tip elements were made smaller. In contrast, the total strain <span class="hlt">energy</span> <span class="hlt">release</span> rate converged and remained unchanged as the delamination tip elements were made smaller and agreed with that calculated using a classical laminated plate theory. The studies of the near field solutions for a delamination at an interface between two dissimilar isotropic or orthotropic plates showed that the imaginary part of the singularity is the cause of the nonconvergent behavior of the individual components. To evaluate the accuracy of the results, an 8-ply laminate with the delamination modeled in a thin resin layer, that exists between the -35 and 90 plies, was analyzed. Because the delamination exists in a homogeneous isotropic material, the oscillatory component of the singularity vanishes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29676571','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29676571"><span>Equilibrium Droplets on <span class="hlt">Deformable</span> Substrates: Equilibrium Conditions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Koursari, Nektaria; Ahmed, Gulraiz; Starov, Victor M</p> <p>2018-05-15</p> <p>Equilibrium conditions of droplets on <span class="hlt">deformable</span> substrates are investigated, and it is proven using Jacobi's sufficient condition that the obtained solutions really provide equilibrium profiles of both the droplet and the <span class="hlt">deformed</span> support. At the equilibrium, the excess free <span class="hlt">energy</span> of the system should have a minimum value, which means that both necessary and sufficient conditions of the minimum should be fulfilled. Only in this case, the obtained profiles provide the minimum of the excess free <span class="hlt">energy</span>. The necessary condition of the equilibrium means that the first variation of the excess free <span class="hlt">energy</span> should vanish, and the second variation should be positive. Unfortunately, the mentioned two conditions are not the proof that the obtained profiles correspond to the minimum of the excess free <span class="hlt">energy</span> and they could not be. It is necessary to check whether the sufficient condition of the equilibrium (Jacobi's condition) is satisfied. To the best of our knowledge Jacobi's condition has never been verified for any already published equilibrium profiles of both the droplet and the <span class="hlt">deformable</span> substrate. A simple model of the equilibrium droplet on the <span class="hlt">deformable</span> substrate is considered, and it is shown that the deduced profiles of the equilibrium droplet and <span class="hlt">deformable</span> substrate satisfy the Jacobi's condition, that is, really provide the minimum to the excess free <span class="hlt">energy</span> of the system. To simplify calculations, a simplified linear disjoining/conjoining pressure isotherm is adopted for the calculations. It is shown that both necessary and sufficient conditions for equilibrium are satisfied. For the first time, validity of the Jacobi's condition is verified. The latter proves that the developed model really provides (i) the minimum of the excess free <span class="hlt">energy</span> of the system droplet/<span class="hlt">deformable</span> substrate and (ii) equilibrium profiles of both the droplet and the <span class="hlt">deformable</span> substrate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23539703','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23539703"><span>Comparison of outcomes between proximal and distal chevron osteotomy, both with supplementary lateral soft-tissue <span class="hlt">release</span>, for severe hallux valgus <span class="hlt">deformity</span>: A prospective randomised controlled trial.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Park, H-W; Lee, K-B; Chung, J-Y; Kim, M-S</p> <p>2013-04-01</p> <p>Severe hallux valgus <span class="hlt">deformity</span> is conventionally treated with proximal metatarsal osteotomy. Distal metatarsal osteotomy with an associated soft-tissue procedure can also be used in moderate to severe <span class="hlt">deformity</span>. We compared the clinical and radiological outcomes of proximal and distal chevron osteotomy in severe hallux valgus <span class="hlt">deformity</span> with a soft-tissue <span class="hlt">release</span> in both. A total of 110 consecutive female patients (110 feet) were included in a prospective randomised controlled study. A total of 56 patients underwent a proximal procedure and 54 a distal operation. The mean follow-up was 39 months (24 to 54) in the proximal group and 38 months (24 to 52) in the distal group. At follow-up the hallux valgus angle, intermetatarsal angle, distal metatarsal articular angle, tibial sesamoid position, American Orthopaedic Foot and Ankle Society (AOFAS) hallux metatarsophalangeal-interphalangeal score, patient satisfaction level, and complications were similar in each group. Both methods showed significant post-operative improvement and high levels of patient satisfaction. Our results suggest that the distal chevron osteotomy with an associated distal soft-tissue procedure provides a satisfactory method for correcting severe hallux valgus <span class="hlt">deformity</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.S44A..02H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.S44A..02H"><span>Anomalous Seismic Radiation in the Shallow Subduction Zone Explained by Extensive Poroplastic <span class="hlt">Deformation</span> in the Overriding Wedge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hirakawa, E. T.; Ma, S.</p> <p>2012-12-01</p> <p>The deficiency of high-frequency seismic radiation from shallow subduction zone earthquakes was first recognized in tsunami earthquakes (Kanamori, 1972), which produce larger tsunamis than expected from short-period (20 s) surface wave excitation. Shallow subduction zone earthquakes were also observed to have unusually low <span class="hlt">energy</span>-to-moment ratios compared to regular subduction zone earthquakes (e.g., Newman and Okal, 1998; Venkataraman and Kanamori, 2004; Lay et al., 2012). What causes this anomalous radiation and how it relates to large tsunami generation has remained unclear. Here we show that these anomalous observations can be due to extensive poroplastic <span class="hlt">deformation</span> in the overriding wedge, which provides a unifying interpretation. Ma (2012) showed that the pore pressure increase in the wedge due to up-dip rupture propagation significantly weakens the wedge, leading to widespread Coulomb failure in the wedge. Widespread failure gives rise to slow rupture velocity and large seafloor uplift (landward from the trench) in the case of a shallow fault dip. Here we extend this work and demonstrate that the large seafloor uplift due to the poroplastic <span class="hlt">deformation</span> significantly dilates the fault behind the rupture front, which reduces the normal stress on the fault and increases the stress drop, slip, and rupture duration. The spectral amplitudes of the moment-rate time function is significantly less at high frequencies than those from elastic simulations. Large tsunami generation and deficiency of high-frequency radiation are thus two consistent manifestations of the same mechanism (poroplastic <span class="hlt">deformation</span>). Although extensive poroplastic <span class="hlt">deformation</span> in the wedge represents a significant portion of total seismic moment <span class="hlt">release</span>, the plastic <span class="hlt">deformation</span> is shown to act as a large <span class="hlt">energy</span> sink, leaving less <span class="hlt">energy</span> to be radiated and leading to low <span class="hlt">energy</span>-to-moment ratios as observed for shallow subduction zone earthquakes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18922780','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18922780"><span>Dynamics of shear-induced ATP <span class="hlt">release</span> from red blood cells.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wan, Jiandi; Ristenpart, William D; Stone, Howard A</p> <p>2008-10-28</p> <p>Adenosine triphosphate (ATP) is a regulatory molecule for many cell functions, both for intracellular and, perhaps less well known, extracellular functions. An important example of the latter involves red blood cells (RBCs), which help regulate blood pressure by <span class="hlt">releasing</span> ATP as a vasodilatory signaling molecule in response to the increased shear stress inside arterial constrictions. Although shear-induced ATP <span class="hlt">release</span> has been observed widely and is believed to be triggered by <span class="hlt">deformation</span> of the cell membrane, the underlying mechanosensing mechanism inside RBCs is still controversial. Here, we use an in vitro microfluidic approach to investigate the dynamics of shear-induced ATP <span class="hlt">release</span> from human RBCs with millisecond resolution. We demonstrate that there is a sizable delay time between the onset of increased shear stress and the <span class="hlt">release</span> of ATP. This response time decreases with shear stress, but surprisingly does not depend significantly on membrane rigidity. Furthermore, we show that even though the RBCs <span class="hlt">deform</span> significantly in short constrictions (duration of increased stress <3 ms), no measurable ATP is <span class="hlt">released</span>. This critical timescale is commensurate with a characteristic membrane relaxation time determined from observations of the cell <span class="hlt">deformation</span> by using high-speed video. Taken together our results suggest a model wherein the retraction of the spectrin-actin cytoskeleton network triggers the mechanosensitive ATP <span class="hlt">release</span> and a shear-dependent membrane viscosity controls the rate of <span class="hlt">release</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_3");'>3</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li class="active"><span>5</span></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_5 --> <div id="page_6" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="101"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009EGUGA..11.2323R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009EGUGA..11.2323R"><span>Influence of LOD variations on seismic <span class="hlt">energy</span> <span class="hlt">release</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Riguzzi, F.; Krumm, F.; Wang, K.; Kiszely, M.; Varga, P.</p> <p>2009-04-01</p> <p>Tidal friction causes significant time variations of geodynamical parameters, among them geometrical flattening. The axial despinning of the Earth due to tidal friction through the change of flattening generates incremental meridional and azimuthal stresses. The stress pattern in an incompressible elastic upper mantle and crust is symmetric to the equator and has its inflection points at the critical latitude close to ±45°. Consequently the distribution of seismic <span class="hlt">energy</span> <span class="hlt">released</span> by strong, shallow focus earthquakes should have also sharp maxima at this latitude. To investigate the influence of length of day (LOD) variations on earthquake activity an earthquake catalogue of strongest seismic events (M>7.0) was completed for the period 1900-2007. It is shown with the use of this catalogue that for the studied time-interval the catalogue is complete and consists of the seismic events responsible for more than 90% of <span class="hlt">released</span> seismic <span class="hlt">energy</span>. Study of the catalogue for earthquakes M>7.0 shows that the seismic <span class="hlt">energy</span> discharged by the strongest seismic events has significant maxima at ±45°, what renders probably that the seismic activity of our planet is influenced by an external component, i.e. by the tidal friction, which acts through the variation of the hydrostatic figure of the Earth caused by it. Distribution along the latitude of earthquake numbers and <span class="hlt">energies</span> was investigated also for the case of global linear tectonic structures, such as mid ocean ridges and subduction zones. It can be shown that the number of the shallow focus shocks has a repartition along the latitude similar to the distribution of the linear tectonic structures. This means that the position of foci of seismic events is mainly controlled by the tectonic activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120012409','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120012409"><span>Shape memory-based actuators and <span class="hlt">release</span> mechanisms therefrom</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vaidyanathan, Rajan (Inventor); Snyder, Daniel W. (Inventor); Schoenwald, David K. (Inventor); Lam, Nhin S. (Inventor); Watson, Daniel S. (Inventor); Krishnan, Vinu B. (Inventor); Noebe, Ronald D. (Inventor)</p> <p>2012-01-01</p> <p>SM-based actuators (110) and <span class="hlt">release</span> mechanisms (100) therefrom and systems (500) including one or more <span class="hlt">release</span> mechanisms (100). The actuators (110) comprise a SM member (118) and a <span class="hlt">deformable</span> member (140) mechanically coupled to the SM member (118) which <span class="hlt">deforms</span> upon a shape change of the SM member triggered by a phase transition of the SM member. A retaining element (160) is mechanically coupled to the <span class="hlt">deformable</span> member (140), wherein the retaining element (160) moves upon the shape change. <span class="hlt">Release</span> mechanism (100) include an actuator, a rotatable mechanism (120) including at least one restraining feature (178) for restraining rotational movement of the retaining element (160) before the shape change, and at least one spring (315) that provides at least one locked spring-loaded position when the retaining element is in the restraining feature and at least one <span class="hlt">released</span> position that is reached when the retaining element is in a position beyond the restraining feature (178). The rotatable mechanism (120) includes at least one load-bearing protrusion (310). A hitch (400) is for mechanically coupling to the load, wherein the hitch is supported on the load bearing protrusion (310) when the rotatable mechanism is in the locked spring-loaded position.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910020966','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910020966"><span>Residual thermal and moisture influences on the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate analysis of local delaminations from matrix cracks</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Obrien, T. K.</p> <p>1991-01-01</p> <p>An analysis utilizing laminated plate theory is developed to calculate the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate associated with local delaminations originating at off-axis, single ply, matrix cracks in laminates subjected to uniaxial loads. The analysis includes the contribution of residual thermal and moisture stresses to the strain <span class="hlt">energy</span> <span class="hlt">released</span>. Examples are calculated for the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate associated with local delaminations originating at 90 degrees and angle-ply (non-90 degrees) matrix ply cracks in glass epoxy and graphite epoxy laminates. The solution developed may be used to assess the relative contribution of mechanical, residual thermal, and moisture stresses on the strain <span class="hlt">energy</span> <span class="hlt">release</span> rate for local delamination for a variety of layups and materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JHEP...09..038F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JHEP...09..038F"><span>Modular Hamiltonians for <span class="hlt">deformed</span> half-spaces and the averaged null <span class="hlt">energy</span> condition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Faulkner, Thomas; Leigh, Robert G.; Parrikar, Onkar; Wang, Huajia</p> <p>2016-09-01</p> <p>We study modular Hamiltonians corresponding to the vacuum state for <span class="hlt">deformed</span> half-spaces in relativistic quantum field theories on {{R}}^{1,d-1} . We show that in addition to the usual boost generator, there is a contribution to the modular Hamiltonian at first order in the shape <span class="hlt">deformation</span>, proportional to the integral of the null components of the stress tensor along the Rindler horizon. We use this fact along with monotonicity of relative entropy to prove the averaged null <span class="hlt">energy</span> condition in Minkowski space-time. This subsequently gives a new proof of the Hofman-Maldacena bounds on the parameters appearing in CFT three-point functions. Our main technical advance involves adapting newly developed perturbative methods for calculating entanglement entropy to the problem at hand. These methods were recently used to prove certain results on the shape dependence of entanglement in CFTs and here we generalize these results to excited states and real time dynamics. We also discuss the AdS/CFT counterpart of this result, making connection with the recently proposed gravitational dual for modular Hamiltonians in holographic theories.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/865965','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/865965"><span>Method of achieving the controlled <span class="hlt">release</span> of thermonuclear <span class="hlt">energy</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Brueckner, Keith A.</p> <p>1986-01-01</p> <p>A method of achieving the controlled <span class="hlt">release</span> of thermonuclear <span class="hlt">energy</span> by illuminating a minute, solid density, hollow shell of a mixture of material such as deuterium and tritium with a high intensity, uniformly converging laser wave to effect an extremely rapid build-up of <span class="hlt">energy</span> in inwardly traveling shock waves to implode the shell creating thermonuclear conditions causing a reaction of deuterons and tritons and a resultant high <span class="hlt">energy</span> thermonuclear burn. Utilizing the resulting <span class="hlt">energy</span> as a thermal source and to breed tritium or plutonium. The invention also contemplates a laser source wherein the flux level is increased with time to reduce the initial shock heating of fuel and provide maximum compression after implosion; and, in addition, computations and an equation are provided to enable the selection of a design having a high degree of stability and a dependable fusion performance by establishing a proper relationship between the laser <span class="hlt">energy</span> input and the size and character of the selected material for the fusion capsule.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20060056392','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20060056392"><span>Influence of Finite Element Software on <span class="hlt">Energy</span> <span class="hlt">Release</span> Rates Computed Using the Virtual Crack Closure Technique</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Krueger, Ronald; Goetze, Dirk; Ransom, Jonathon (Technical Monitor)</p> <p>2006-01-01</p> <p>Strain <span class="hlt">energy</span> <span class="hlt">release</span> rates were computed along straight delamination fronts of Double Cantilever Beam, End-Notched Flexure and Single Leg Bending specimens using the Virtual Crack Closure Technique (VCCT). Th e results were based on finite element analyses using ABAQUS# and ANSYS# and were calculated from the finite element results using the same post-processing routine to assure a consistent procedure. Mixed-mode strain <span class="hlt">energy</span> <span class="hlt">release</span> rates obtained from post-processing finite elem ent results were in good agreement for all element types used and all specimens modeled. Compared to previous studies, the models made of s olid twenty-node hexahedral elements and solid eight-node incompatible mode elements yielded excellent results. For both codes, models made of standard brick elements and elements with reduced integration did not correctly capture the distribution of the <span class="hlt">energy</span> <span class="hlt">release</span> rate acr oss the width of the specimens for the models chosen. The results suggested that element types with similar formulation yield matching results independent of the finite element software used. For comparison, m ixed-mode strain <span class="hlt">energy</span> <span class="hlt">release</span> rates were also calculated within ABAQUS#/Standard using the VCCT for ABAQUS# add on. For all specimens mod eled, mixed-mode strain <span class="hlt">energy</span> <span class="hlt">release</span> rates obtained from ABAQUS# finite element results using post-processing were almost identical to re sults calculated using the VCCT for ABAQUS# add on.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA554571','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA554571"><span>Development of Techniques for Investigating <span class="hlt">Energy</span> Contributions to Target <span class="hlt">Deformation</span> and Penetration During Reactive Projectile Hypervelocity Impact</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2011-07-01</p> <p>a reactive and a non reactive shaped charge liner is in the <span class="hlt">energy</span> <span class="hlt">release</span> of the combustion ... reactive shaped charge jets the reaction is explained and the possible <span class="hlt">energy</span> <span class="hlt">release</span> of the metal combustion is estimated. Addition- ally the...Charges In a shaped charge a -in most cases- conical cavity in the explosive is covered with a liner. If the explosive detonates , a small portion</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820010912','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820010912"><span>Reports on crustal movements and <span class="hlt">deformations</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cohen, S. C.; Peck, T.</p> <p>1981-01-01</p> <p>Studies of tectonic plate motions, regional crustal <span class="hlt">deformations</span>, strain accumulation and <span class="hlt">release</span>, <span class="hlt">deformations</span> associated with earthquakes and fault motion, and micro-plate motion, were collected and are summarized. To a limited extent, papers dealing with global models of current plate motions and crustal stress are included. The data base is restricted to articles appearing in reveiwed technical journals during the years 1970-1980. The major journals searched include: Journal of Geophysical Research (solid earth), Tectonophysics, Bulletin of the Seismological Society of America, Geological Society of America Bulletin, Geophysical Journal of the Royal Astronomical Society, and the Journal of Geology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CG....113....1Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CG....113....1Z"><span>Forecasting of future earthquakes in the northeast region of India considering <span class="hlt">energy</span> <span class="hlt">released</span> concept</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zarola, Amit; Sil, Arjun</p> <p>2018-04-01</p> <p>This study presents the forecasting of time and magnitude size of the next earthquake in the northeast India, using four probability distribution models (Gamma, Lognormal, Weibull and Log-logistic) considering updated earthquake catalog of magnitude Mw ≥ 6.0 that occurred from year 1737-2015 in the study area. On the basis of past seismicity of the region, two types of conditional probabilities have been estimated using their best fit model and respective model parameters. The first conditional probability is the probability of seismic <span class="hlt">energy</span> (e × 1020 ergs), which is expected to <span class="hlt">release</span> in the future earthquake, exceeding a certain level of seismic <span class="hlt">energy</span> (E × 1020 ergs). And the second conditional probability is the probability of seismic <span class="hlt">energy</span> (a × 1020 ergs/year), which is expected to <span class="hlt">release</span> per year, exceeding a certain level of seismic <span class="hlt">energy</span> per year (A × 1020 ergs/year). The logarithm likelihood functions (ln L) were also estimated for all four probability distribution models. A higher value of ln L suggests a better model and a lower value shows a worse model. The time of the future earthquake is forecasted by dividing the total seismic <span class="hlt">energy</span> expected to <span class="hlt">release</span> in the future earthquake with the total seismic <span class="hlt">energy</span> expected to <span class="hlt">release</span> per year. The epicentre of recently occurred 4 January 2016 Manipur earthquake (M 6.7), 13 April 2016 Myanmar earthquake (M 6.9) and the 24 August 2016 Myanmar earthquake (M 6.8) are located in zone Z.12, zone Z.16 and zone Z.15, respectively and that are the identified seismic source zones in the study area which show that the proposed techniques and models yield good forecasting accuracy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JaJAP..57fHJ05S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JaJAP..57fHJ05S"><span>Development of <span class="hlt">energy</span>-harvesting system using <span class="hlt">deformation</span> of magnetic elastomer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shinoda, Hayato; Tsumori, Fujio</p> <p>2018-06-01</p> <p>In this paper, we propose a power generation method using the <span class="hlt">deformation</span> of a magnetic elastomer for vibration <span class="hlt">energy</span> harvesting. The magnetic flux lines in the structure of the magnetic elastomer could be markedly changed if the properly designed structure was expanded and contracted in a static magnetic field. We set a coil on the magnetic elastomer to generate electricity by capturing this change in magnetic flux flow. We fabricated a centimeter-scale device and demonstrated that it generated 10.5 mV of maximum voltage by 10 Hz vibration. We also simulated the change in the magnetic flux flow using finite element analysis, and compared the result with the experimental data. Furthermore, we evaluated the power generation of a miniaturized device.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NuPhA.975...77S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NuPhA.975...77S"><span>Sensitivity of the nuclear <span class="hlt">deformability</span> and fission barriers to the equation of state</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Seif, W. M.; Anwer, Hisham</p> <p>2018-07-01</p> <p>The model-dependent analysis of the fission data impacts the extracted fission-related quantities, which are not directly observables, such as the super- and hyperdeformed isomeric states and their <span class="hlt">energies</span>. We investigated the model dependence of the <span class="hlt">deformability</span> of a nucleus and its fission barriers on the nuclear equation of state. Within the microscopic-macroscopic model based on a large number of Skyrme nucleon-nucleon interactions, the total <span class="hlt">energy</span> surfaces and the double-humped fission barrier of 230Th are calculated in a multidimensional <span class="hlt">deformation</span> space. In addition to the ground-state (GS) and the superdeformed (SD) minima, all the investigated forces yielded a hyperdeformed (HD) minimum. The contour map of the shell-plus-pairing <span class="hlt">energy</span> clearly displayed the three minima. We found that the GS binding <span class="hlt">energy</span> and the <span class="hlt">deformation</span> <span class="hlt">energy</span> of the different <span class="hlt">deformation</span> modes along the fission path increase with the incompressibility coefficient K0, while the fission barrier heights and the excitation <span class="hlt">energies</span> of the SD and HD modes decrease with it. Conversely, the surface-<span class="hlt">energy</span> coefficient asurf, the symmetry-<span class="hlt">energy</span>, and its density-slope parameter decrease the GS <span class="hlt">energy</span> and the <span class="hlt">deformation</span> <span class="hlt">energies</span>, but increase the fission barrier heights and the excitation <span class="hlt">energies</span>. The obtained <span class="hlt">deformation</span> parameters of the different <span class="hlt">deformation</span> modes exhibit almost independence on K0, and on the symmetry-<span class="hlt">energy</span> and its density-slope. The principle <span class="hlt">deformation</span> parameters of the SD and HD isomeric states tend to decrease with asurf.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26947978','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26947978"><span>Active range of motion outcomes after reconstruction of burned wrist and hand <span class="hlt">deformities</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Afifi, Ahmed M; Mahboub, Tarek A; Ibrahim Fouad, Amr; Azari, Kodi; Khalil, Haitham H; McCarthy, James E</p> <p>2016-06-01</p> <p>This works aim is to evaluate the efficacy of skin grafts and flaps in reconstruction of post-burn hand and wrist <span class="hlt">deformities</span>. A prospective study of 57 burn contractures of the wrist and dorsum of the hand was performed. Flaps were used only if there was a non-vascularized structure after contracture <span class="hlt">release</span>, otherwise a skin graft was used. Active range of motion (ROM) was used to assess hand function. The extension <span class="hlt">deformity</span> cohort uniformly underwent skin graft following contracture <span class="hlt">release</span> with a mean improvement of 71 degrees (p<0.0001). The flexion <span class="hlt">deformity</span> cohort was treated with either skin grafts (8 patients) or flaps (9 patients) with a mean improvement of 44 degrees (p<0.0001). Skin grafts suffice for dorsal hand contractures to restore functional wrist ROM. For flexion contractures, flaps were more likely for contractures >6 months. Early <span class="hlt">release</span> of burn contracture is advisable to avoid deep structure contracture. Copyright © 2016 Elsevier Ltd and ISBI. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26410785','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26410785"><span>Highly fluorescent carbon dots for visible sensing of doxorubicin <span class="hlt">release</span> based on efficient nanosurface <span class="hlt">energy</span> transfer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Beibei; Wang, Shujun; Wang, Yanfang; Lv, Yan; Wu, Hao; Ma, Xiaojun; Tan, Mingqian</p> <p>2016-01-01</p> <p>To prepare fluorescent carbon dots for loading cationic anticancer drug through donor-quenched nanosurface <span class="hlt">energy</span> transfer in visible sensing of drug <span class="hlt">release</span>. Highly fluorescent carbon dots (CDs) were prepared by a facile hydrothermal approach from citric acid and o-phenylenediamine. The obtained CDs showed a high quantum yield of 46 % and exhibited good cytocompatibility even at 1 mg/ml. The cationic anticancer drug doxorubicin (DOX) can be loaded onto the negatively charged CDs through electrostatic interactions. Additionally, the fluorescent CDs feature reversible donor-quenched mode nanosurface <span class="hlt">energy</span> transfer. When loading the <span class="hlt">energy</span> receptor DOX, the donor CDs' fluorescence was switched "off", while it turned "on" again after DOX <span class="hlt">release</span> from the surface through endocytic uptake. Most DOX molecules were <span class="hlt">released</span> from the CDs after 6 h incubation and entered cell nuclear region after 8 h, suggesting the drug delivery system may have potential for visible sensing in drug <span class="hlt">release</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1347990','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=1347990"><span>Detachment of affinity-captured bioparticles by elastic <span class="hlt">deformation</span> of a macroporous hydrogel</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Dainiak, Maria B.; Kumar, Ashok; Galaev, Igor Yu.; Mattiasson, Bo</p> <p>2006-01-01</p> <p>Adsorption of bioparticles to affinity surfaces involves polyvalent interactions, complicating greatly the recovery of the adsorbed material. A unique system for the efficient binding and <span class="hlt">release</span> of different cells and particles is described. Affinity-bound bioparticles and synthetic particles are detached from the macroporous hydrogel matrix, a so-called cryogel, when the cryogel undergoes elastic <span class="hlt">deformation</span>. The particle detachment upon elastic <span class="hlt">deformation</span> is believed to be due to breaking of many of the multipoint attachments between the particles and the affinity matrix and the change in the distance between affinity ligands when the matrix is <span class="hlt">deformed</span>. However, no <span class="hlt">release</span> of affinity-bound protein occurred upon elastic <span class="hlt">deformation</span>. The phenomenon of particle detachment upon elastic <span class="hlt">deformation</span> is believed to be of a generic nature, because it was demonstrated for a variety of bioparticles of different sizes and for synthetic particles, for different ligand–receptor pairs (IgG–protein A, sugar–ConA, metal ion–chelating ligand), and when the <span class="hlt">deformation</span> was caused by either external forces (mechanical <span class="hlt">deformation</span>) or internal forces (the shrinkage of thermosensitive, macroporous hydrogel upon an increase in temperature). The elasticity of cryogel monoliths ensures high recovery of captured cells under mild conditions, with highly retained viability. This property, along with their continuous porous structure makes cryogel monoliths very attractive for applications in affinity cell separation. PMID:16418282</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1426668','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1426668"><span>The Dark <span class="hlt">Energy</span> Survey Data <span class="hlt">Release</span> 1</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Abbott, T.M.C.; et al.</p> <p></p> <p>We describe the first public data <span class="hlt">release</span> of the Dark <span class="hlt">Energy</span> Survey, DES DR1, consisting of reduced single epoch images, coadded images, coadded source catalogs, and associated products and services assembled over the first three years of DES science operations. DES DR1 is based on optical/near-infrared imaging from 345 distinct nights (August 2013 to February 2016) by the Dark <span class="hlt">Energy</span> Camera mounted on the 4-m Blanco telescope at Cerro Tololo Inter-American Observatory in Chile. We <span class="hlt">release</span> data from the DES wide-area survey covering ~5,000 sq. deg. of the southern Galactic cap in five broad photometric bands, grizY. DES DR1 hasmore » a median delivered point-spread function of g = 1.12, r = 0.96, i = 0.88, z = 0.84, and Y = 0.90 arcsec FWHM, a photometric precision of < 1% in all bands, and an astrometric precision of 151 mas. The median coadded catalog depth for a 1.95" diameter aperture at S/N = 10 is g = 24.33, r = 24.08, i = 23.44, z = 22.69, and Y = 21.44 mag. DES DR1 includes nearly 400M distinct astronomical objects detected in ~10,000 coadd tiles of size 0.534 sq. deg. produced from ~39,000 individual exposures. Benchmark galaxy and stellar samples contain ~310M and ~ 80M objects, respectively, following a basic object quality selection. These data are accessible through a range of interfaces, including query web clients, image cutout servers, jupyter notebooks, and an interactive coadd image visualization tool. DES DR1 constitutes the largest photometric data set to date at the achieved depth and photometric precision.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JPhCS.451a2014M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JPhCS.451a2014M"><span>Dynamic <span class="hlt">energy</span> <span class="hlt">release</span> rate in couple-stress elasticity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morini, L.; Piccolroaz, A.; Mishuris, G.</p> <p>2013-07-01</p> <p>This paper is concerned with <span class="hlt">energy</span> <span class="hlt">release</span> rate for dynamic steady state crack problems in elastic materials with microstructures. A Mode III semi-infinite crack subject to loading applied on the crack surfaces is considered. The micropolar behaviour of the material is described by the theory of couple-stress elasticity developed by Koiter. A general expression for the dynamic J-integral including both traslational and micro-rotational inertial contributions is derived, and the conservation of this integral on a path surrounding the crack tip is demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EPJWC.10703008M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EPJWC.10703008M"><span>Octupole <span class="hlt">deformations</span> in high-K isomeric states of heavy and superheavy nuclei</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Minkov, N.; Walker, P. M.</p> <p>2016-01-01</p> <p>We study the effects of quadrupole-octupole <span class="hlt">deformations</span> on the <span class="hlt">energy</span> and magnetic properties of high-K isomeric states in even-even heavy and superheavy nuclei. The neutron two-quasiparticle (2qp) isomeric <span class="hlt">energies</span> and magnetic dipole moments are calculated within a <span class="hlt">deformed</span> shell model with the Bardeen-Cooper- Schrieffer (BCS) pairing interaction over a wide range of quadrupole and octupole <span class="hlt">deformations</span>. We found that in most cases the magnetic moments exhibit a pronounced sensitivity to the octupole <span class="hlt">deformation</span>, while the 2qp <span class="hlt">energies</span> indicate regions of nuclei in which the presence of high-K isomeric states may be associated with the presence of octupole softness or even with octupole <span class="hlt">deformation</span>. In the present work we also examine the influence of the BCS pairing strength on the <span class="hlt">energy</span> of the blocked isomer configuration. We show that the formation of 2qp <span class="hlt">energy</span> minima in the space of quadrupole-octupole and eventually higher multipolarity <span class="hlt">deformations</span> is a subtle effect depending on nuclear pairing correlations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhPl...17a2109B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhPl...17a2109B"><span><span class="hlt">Energy</span> <span class="hlt">release</span> and transfer in guide field reconnection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Birn, J.; Hesse, M.</p> <p>2010-01-01</p> <p>Properties of <span class="hlt">energy</span> <span class="hlt">release</span> and transfer by magnetic reconnection in the presence of a guide field are investigated on the basis of 2.5-dimensional magnetohydrodynamic (MHD) and particle-in-cell (PIC) simulations. Two initial configurations are considered: a plane current sheet with a uniform guide field of 80% of the reconnecting magnetic field component and a force-free current sheet in which the magnetic field strength is constant but the field direction rotates by 180° through the current sheet. The onset of reconnection is stimulated by localized, temporally limited compression. Both MHD and PIC simulations consistently show that the outgoing <span class="hlt">energy</span> fluxes are dominated by (redirected) Poynting flux and enthalpy flux, whereas bulk kinetic <span class="hlt">energy</span> flux and heat flux (in the PIC simulation) are small. The Poynting flux is mainly associated with the magnetic <span class="hlt">energy</span> of the guide field which is carried from inflow to outflow without much alteration. The conversion of annihilated magnetic <span class="hlt">energy</span> to enthalpy flux (that is, thermal <span class="hlt">energy</span>) stems mainly from the fact that the outflow occurs into a closed field region governed by approximate force balance between Lorentz and pressure gradient forces. Therefore, the <span class="hlt">energy</span> converted from magnetic to kinetic <span class="hlt">energy</span> by Lorentz force acceleration becomes immediately transferred to thermal <span class="hlt">energy</span> by the work done by the pressure gradient force. Strong similarities between late stages of MHD and PIC simulations result from the fact that conservation of mass and entropy content and footpoint displacement of magnetic flux tubes, imposed in MHD, are also approximately satisfied in the PIC simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA.....9933F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA.....9933F"><span>Carbon dioxide degassing and thermal <span class="hlt">energy</span> <span class="hlt">release</span> at Vesuvio (Italy)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Frondini, F.; Chiodini, G.; Caliro, S.; Cardellini, C.; Granieri, D.</p> <p>2003-04-01</p> <p>At Vesuvio, basing on the data of the CO2 flux surveys carried out in April and May 2000, are discharged about 130 t d-1 of CO2 through soil diffuse degassing. In the crater area the distribution of the soil temperatures show a general correspondence between the CO2 flux anomalies and the high temperatures, suggesting that the heating of the soil is mainly due to the condensation of the rising volcanic-hydrothermal fluids. Considering that the original H2O/CO2 ratio of hydrothermal fluids is recorded by fumarolic effluents, the steam associated to the CO2 output has been computed and amount to is 475 t d-1. The <span class="hlt">energy</span> produced by the steam condensation and cooling of the liquid phase is 1.26 1012 J d-1 (14.6 MW). The amounts of gas and <span class="hlt">energy</span> <span class="hlt">released</span> by Vesuvio are comparable to those <span class="hlt">released</span> by other volcanic degassing areas of the world and their estimates, through periodical CO2 flux surveys, can constitute a powerful tool to monitor the activity of the volcano.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMMR43B0471A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMMR43B0471A"><span>The Role of <span class="hlt">Deformation</span> Energetics in Long-Term Tectonic Modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahamed, S.; Choi, E.</p> <p>2017-12-01</p> <p>The <span class="hlt">deformation</span>-related <span class="hlt">energy</span> budget is usually considered in the simplest form or even entirely omitted from the <span class="hlt">energy</span> balance equation. We derive a full <span class="hlt">energy</span> balance equation that accounts not only for heat <span class="hlt">energy</span> but also for mechanical (elastic, plastic and viscous) work. The derived equation is implemented in DES3D, an unstructured finite element solver for long-term tectonic <span class="hlt">deformation</span>. We verify the implementation by comparing numerical solutions to the corresponding semi-analytic solutions in three benchmarks extended from the classical oedometer test. We also investigate the long-term effects of <span class="hlt">deformation</span> energetics on the evolution of large offset normal faults. We find that the models considering the full <span class="hlt">energy</span> balance equation tend to produce more secondary faults and an elongated core complex. Our results for the normal fault system confirm that persistent inelastic <span class="hlt">deformation</span> has a significant impact on the long-term evolution of faults, motivating further exploration of the role of the full <span class="hlt">energy</span> balance equation in other geodynamic systems.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_4");'>4</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li class="active"><span>6</span></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_6 --> <div id="page_7" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="121"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/897937','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/897937"><span>Kinetic Modeling of Slow <span class="hlt">Energy</span> <span class="hlt">Release</span> in Non-Ideal Carbon Rich Explosives</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Vitello, P; Fried, L; Glaesemann, K</p> <p>2006-06-20</p> <p>We present here the first self-consistent kinetic based model for long time-scale <span class="hlt">energy</span> <span class="hlt">release</span> in detonation waves in the non-ideal explosive LX-17. Non-ideal, insensitive carbon rich explosives, such as those based on TATB, are believed to have significant late-time slow <span class="hlt">release</span> in <span class="hlt">energy</span>. One proposed source of this <span class="hlt">energy</span> is diffusion-limited growth of carbon clusters. In this paper we consider the late-time <span class="hlt">energy</span> <span class="hlt">release</span> problem in detonation waves using the thermochemical code CHEETAH linked to a multidimensional ALE hydrodynamics model. The linked CHEETAH-ALE model dimensional treats slowly reacting chemical species using kinetic rate laws, with chemical equilibrium assumed for speciesmore » coupled via fast time-scale reactions. In the model presented here we include separate rate equations for the transformation of the un-reacted explosive to product gases and for the growth of a small particulate form of condensed graphite to a large particulate form. The small particulate graphite is assumed to be in chemical equilibrium with the gaseous species allowing for coupling between the instantaneous thermodynamic state and the production of graphite clusters. For the explosive burn rate a pressure dependent rate law was used. Low pressure freezing of the gas species mass fractions was also included to account for regions where the kinetic coupling rates become longer than the hydrodynamic time-scales. The model rate parameters were calibrated using cylinder and rate-stick experimental data. Excellent long time agreement and size effect results were achieved.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1395542-modular-hamiltonians-deformed-half-spaces-averaged-null-energy-condition','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1395542-modular-hamiltonians-deformed-half-spaces-averaged-null-energy-condition"><span>Modular Hamiltonians for <span class="hlt">deformed</span> half-spaces and the averaged null <span class="hlt">energy</span> condition</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Faulkner, Thomas; Leigh, Robert G.; Parrikar, Onkar; ...</p> <p>2016-09-08</p> <p>We study modular Hamiltonians corresponding to the vacuum state for <span class="hlt">deformed</span> half-spaces in relativistic quantum field theories on R 1,d-1. We show that in addition to the usual boost generator, there is a contribution to the modular Hamiltonian at first order in the shape <span class="hlt">deformation</span>, proportional to the integral of the null components of the stress tensor along the Rindler horizon. We use this fact along with monotonicity of relative entropy to prove the averaged null <span class="hlt">energy</span> condition in Minkowski space-time. This subsequently gives a new proof of the Hofman-Maldacena bounds on the parameters appearing in CFT three-point functions. Ourmore » main technical advance involves adapting newly developed perturbative methods for calculating entanglement entropy to the problem at hand. Our methods were recently used to prove certain results on the shape dependence of entanglement in CFTs and here we generalize these results to excited states and real time dynamics. Finally, we discuss the AdS/CFT counterpart of this result, making connection with the recently proposed gravitational dual for modular Hamiltonians in holographic theories.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1395542','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1395542"><span>Modular Hamiltonians for <span class="hlt">deformed</span> half-spaces and the averaged null <span class="hlt">energy</span> condition</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Faulkner, Thomas; Leigh, Robert G.; Parrikar, Onkar</p> <p></p> <p>We study modular Hamiltonians corresponding to the vacuum state for <span class="hlt">deformed</span> half-spaces in relativistic quantum field theories on R 1,d-1. We show that in addition to the usual boost generator, there is a contribution to the modular Hamiltonian at first order in the shape <span class="hlt">deformation</span>, proportional to the integral of the null components of the stress tensor along the Rindler horizon. We use this fact along with monotonicity of relative entropy to prove the averaged null <span class="hlt">energy</span> condition in Minkowski space-time. This subsequently gives a new proof of the Hofman-Maldacena bounds on the parameters appearing in CFT three-point functions. Ourmore » main technical advance involves adapting newly developed perturbative methods for calculating entanglement entropy to the problem at hand. Our methods were recently used to prove certain results on the shape dependence of entanglement in CFTs and here we generalize these results to excited states and real time dynamics. Finally, we discuss the AdS/CFT counterpart of this result, making connection with the recently proposed gravitational dual for modular Hamiltonians in holographic theories.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22661301-observable-signatures-energy-release-braided-coronal-loops','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22661301-observable-signatures-energy-release-braided-coronal-loops"><span>Observable Signatures of <span class="hlt">Energy</span> <span class="hlt">Release</span> in Braided Coronal Loops</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Pontin, D. I.; Janvier, M.; Tiwari, S. K.</p> <p></p> <p>We examine the turbulent relaxation of solar coronal loops containing non-trivial field line braiding. Such field line tangling in the corona has long been postulated in the context of coronal heating models. We focus on the observational signatures of <span class="hlt">energy</span> <span class="hlt">release</span> in such braided magnetic structures using MHD simulations and forward modeling tools. The aim is to answer the following question: if <span class="hlt">energy</span> <span class="hlt">release</span> occurs in a coronal loop containing braided magnetic flux, should we expect a clearly observable signature in emissions? We demonstrate that the presence of braided magnetic field lines does not guarantee a braided appearance to themore » observed intensities. Observed intensities may—but need not necessarily—reveal the underlying braided nature of the magnetic field, depending on the degree and pattern of the field line tangling within the loop. However, in all cases considered, the evolution of the braided loop is accompanied by localized heating regions as the loop relaxes. Factors that may influence the observational signatures are discussed. Recent high-resolution observations from Hi-C have claimed the first direct evidence of braided magnetic fields in the corona. Here we show that both the Hi-C data and some of our simulations give the appearance of braiding at a range of scales.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JEnM...28....1T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JEnM...28....1T"><span>Chemical <span class="hlt">Energy</span> <span class="hlt">Release</span> in Several Recently Discovered Detonation and Deflagration Flows</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tarver, Craig M.</p> <p>2010-10-01</p> <p>Several recent experiments on complex detonation and deflagration flows are analyzed in terms of the chemical <span class="hlt">energy</span> <span class="hlt">release</span> required to sustain these flows. The observed double cellular structures in detonating gaseous nitromethane-oxygen and NO2-fuel (H2, CH4, and C2H6) mixtures are explained by the amplification of two distinct pressure wave frequencies by two exothermic reactions, the faster reaction forming vibrationally excited NO* and the slower reaction forming highly vibrationally excited N2**. The establishment of a Chapman-Jouguet (C-J) deflagration behind a weak shock wave, the C-J detonation established after a head-on collision with a shock front, and the C-J detonation conditions established in reactive supersonic flows are quantitatively calculated using the chemical <span class="hlt">energy</span> <span class="hlt">release</span> of a H2 + Cl2 mixture. For these three reactive flows, these calculations illustrate that different fractions of the exothermic chemical <span class="hlt">energy</span> are used to sustain steady-state propagation. C-J detonation calculations on the various initial states using the CHEETAH chemical equilibrium code are shown to be in good agreement with experimental detonation velocity measurements for the head-on collision and supersonic flow detonations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930054261&hterms=solar+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsolar%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930054261&hterms=solar+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dsolar%2Benergy"><span>Numerical modeling of the <span class="hlt">energy</span> storage and <span class="hlt">release</span> in solar flares</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wu, S. T.; Weng, F. S.</p> <p>1993-01-01</p> <p>This paper reports on investigation of the photospheric magnetic field-line footpoint motion (usually referred to as shear motion) and magnetic flux emerging from below the surface in relation to <span class="hlt">energy</span> storage in a solar flare. These causality relationships are demonstrated by using numerical magnetohydrodynamic simulations. From these results, one may conclude that the <span class="hlt">energy</span> stored in solar flares is in the form of currents. The dynamic process through which these currents reach a critical value is discussed as well as how these currents lead to <span class="hlt">energy</span> <span class="hlt">release</span>, such as the explosive events of solar flares.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830014615','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830014615"><span>The <span class="hlt">energy</span> <span class="hlt">release</span> in earthquakes, and subduction zone seismicity and stress in slabs. Ph.D. Thesis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vassiliou, M. S.</p> <p>1983-01-01</p> <p><span class="hlt">Energy</span> <span class="hlt">release</span> in earthquakes is discussed. Dynamic <span class="hlt">energy</span> from source time function, a simplified procedure for modeling deep focus events, static <span class="hlt">energy</span> estimates, near source <span class="hlt">energy</span> studies, and <span class="hlt">energy</span> and magnitude are addressed. Subduction zone seismicity and stress in slabs are also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70012003','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70012003"><span>Gravitational potential as a source of earthquake <span class="hlt">energy</span></span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Barrows, L.; Langer, C.J.</p> <p>1981-01-01</p> <p>Some degree of tectonic stress within the earth originates from gravity acting upon density structures. The work performed by this "gravitational tectonics stress" must have formerly existed as gravitational potential <span class="hlt">energy</span> contained in the stress-causing density structure. According to the elastic rebound theory (Reid, 1910), the <span class="hlt">energy</span> of earthquakes comes from an elastic strain field built up by fairly continuous elastic <span class="hlt">deformation</span> in the period between events. For earthquakes resulting from gravitational tectonic stress, the elastic rebound theory requires the transfer of <span class="hlt">energy</span> from the gravitational potential of the density structures into an elastic strain field prior to the event. An alternate theory involves partial gravitational collapse of the stress-causing density structures. The earthquake <span class="hlt">energy</span> comes directly from a net decrease in gravitational potential <span class="hlt">energy</span>. The gravitational potential <span class="hlt">energy</span> <span class="hlt">released</span> at the time of the earthquake is split between the <span class="hlt">energy</span> <span class="hlt">released</span> by the earthquake, including work done in the fault zone and an increase in stored elastic strain <span class="hlt">energy</span>. The stress associated with this elastic strain field should oppose further fault slip. ?? 1981.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016IJMPE..2550047K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016IJMPE..2550047K"><span>Nonaxial hexadecapole <span class="hlt">deformation</span> effects on the fission barrier</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kardan, A.; Nejati, S.</p> <p>2016-06-01</p> <p>Fission barrier of the heavy nucleus 250Cf is analyzed in a multi-dimensional <span class="hlt">deformation</span> space. This space includes two quadrupole (ɛ2,γ) and three hexadecapole <span class="hlt">deformation</span> (ɛ40,ɛ42,ɛ44) parameters. The analysis is performed within an unpaired macroscopic-microscopic approach. Special attention is given to the effects of the axial and non-axial hexadecapole <span class="hlt">deformation</span> shapes. It is found that the inclusion of the nonaxial hexadecapole shapes does not change the fission barrier heights, so it should be sufficient to minimize the <span class="hlt">energy</span> in only one degree of freedom in the hexadecapole space ɛ4. The role of hexadecapole <span class="hlt">deformation</span> parameters is also discussed on the Lublin-Strasbourg drop (LSD) macroscopic and the Strutinsky shell <span class="hlt">energies</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007PhDT........62T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007PhDT........62T"><span><span class="hlt">Deformable</span> microparticles with multiple functions for drug delivery and device testing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thula, Taili T.</p> <p></p> <p>Since the HIV epidemic of the 1990s, researchers have attempted to develop a red blood cell analog. Even though some of these substitutes are now in Phase III of clinical trials, their use is limited by side effects and short half-life in the human body. As a result, there is still a need for an effective erythrocyte analog with minimum immunogenic and side effects, so that it can be used for multiple applications. Finding new approaches to develop more efficient blood substitutes will not only bring valuable advances in the clinical approach, but also in the area of in vitro testing of medical devices. We examined the feasibility of creating a <span class="hlt">deformable</span> multi-functional, biodegradable, biocompatible particle for applications in drug delivery and device testing. As a preliminary evaluation, we synthesized different types of microcapsules using natural and synthetic polymers, various cross-linking agents, and diverse manufacturing techniques. After fully characterizing of each system, we determined the most promising red blood cell analog in terms of <span class="hlt">deformability</span>, stability and toxicity. We also examined the encapsulation and <span class="hlt">release</span> of bovine serum albumin (BSA) within these <span class="hlt">deformable</span> particles. After removal of cross-linkers, zinc- and copper-alginate microparticles surrounded by multiple polyelectrolyte layers of chitosan oligosaccharide and alginate were <span class="hlt">deformable</span> and remained stable under physiological pressures applied by the micropipette technique. In addition, multiple coatings decreased toxicity of heavy-metal crosslinked particles. BSA encapsulation and <span class="hlt">release</span> from chitosan-alginate microspheres were contingent on the crosslinker and number of polyelectrolyte coatings, respectively. Further rheological studies are needed to determine how closely these particles simulate the behavior of erythrocytes. Also, studies on the encapsulation and <span class="hlt">release</span> of different proteins, including hemoglobin, are needed to establish the desired controlled <span class="hlt">release</span> of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1154960','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1154960"><span>Explosive Products EOS: Adjustment for detonation speed and <span class="hlt">energy</span> <span class="hlt">release</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Menikoff, Ralph</p> <p>2014-09-05</p> <p>Propagating detonation waves exhibit a curvature effect in which the detonation speed decreases with increasing front curvature. The curvature effect is due to the width of the wave profile. Numerically, the wave profile depends on resolution. With coarse resolution, the wave width is too large and results in a curvature effect that is too large. Consequently, the detonation speed decreases as the cell size is increased. We propose a modification to the products equation of state (EOS) to compensate for the effect of numerical resolution; i.e., to increase the CJ pressure in order that a simulation propagates a detonation wavemore » with a speed that is on average correct. The EOS modification also adjusts the <span class="hlt">release</span> isentrope to correct the <span class="hlt">energy</span> <span class="hlt">release</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992JCoMa..26.2028R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992JCoMa..26.2028R"><span>Method for computing <span class="hlt">energy</span> <span class="hlt">release</span> rate using the elastic work factor approach</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rhee, K. Y.; Ernst, H. A.</p> <p>1992-01-01</p> <p>The elastic work factor eta(el) concept was applied to composite structures for the calculation of total <span class="hlt">energy</span> <span class="hlt">release</span> rate by using a single specimen. Cracked lap shear specimens with four different unidirectional fiber orientation were used to examine the dependence of eta(el) on the material properties. Also, three different thickness ratios (lap/strap) were used to determine how geometric conditions affect eta(el). The eta(el) values were calculated in two different ways: compliance method and crack closure method. The results show that the two methods produce comparable eta(el) values and, while eta(el) is affected significantly by geometric conditions, it is reasonably independent of material properties for the given geometry. The results also showed that the elastic work factor can be used to calculate total <span class="hlt">energy</span> <span class="hlt">release</span> rate using a single specimen.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27547684','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27547684"><span><span class="hlt">Deformation</span> mechanisms in a coal mine roadway in extremely swelling soft rock.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Qinghai; Shi, Weiping; Yang, Renshu</p> <p>2016-01-01</p> <p>The problem of roadway support in swelling soft rock was one of the challenging problems during mining. For most geological conditions, combinations of two or more supporting approaches could meet the requirements of most roadways; however, in extremely swelling soft rock, combined approaches even could not control large <span class="hlt">deformations</span>. The purpose of this work was to probe the roadway <span class="hlt">deformation</span> mechanisms in extremely swelling soft rock. Based on the main return air-way in a coal mine, <span class="hlt">deformation</span> monitoring and geomechanical analysis were conducted, as well as plastic zone mechanical model was analysed. Results indicated that this soft rock was potentially very swelling. When the ground stress acted alone, the support strength needed in situ was not too large and combined supporting approaches could meet this requirement; however, when this potential <span class="hlt">released</span>, the roadway would undergo permanent <span class="hlt">deformation</span>. When the loose zone reached 3 m within surrounding rock, remote stress p ∞ and supporting stress P presented a linear relationship. Namely, the greater the swelling stress, the more difficult it would be in roadway supporting. So in this extremely swelling soft rock, a better way to control roadway <span class="hlt">deformation</span> was to control the <span class="hlt">releasing</span> of surrounding rock's swelling potential.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140013397','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140013397"><span><span class="hlt">Energy</span> <span class="hlt">Release</span> from Impacting Prominence Material Following the 2011 June 7 Eruption</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gilbert, H. R.; Inglis, A. R.; Mays, M. L.; Ofman, L.; Thompson, B. J.; Young, C. A.</p> <p>2013-01-01</p> <p>Solar filaments exhibit a range of eruptive-like dynamic activity, ranging from the full or partial eruption of the filament mass and surrounding magnetic structure as a coronal mass ejection to a fully confined or failed eruption. On 2011 June 7, a dramatic partial eruption of a filament was observed by multiple instruments on board the Solar Dynamics Observatory (SDO) and Solar-Terrestrial Relations Observatory. One of the interesting aspects of this event is the response of the solar atmosphere as non-escaping material falls inward under the influence of gravity. The impact sites show clear evidence of brightening in the observed extreme ultraviolet wavelengths due to <span class="hlt">energy</span> <span class="hlt">release</span>. Two plausible physical mechanisms for explaining the brightening are considered: heating of the plasma due to the kinetic <span class="hlt">energy</span> of impacting material compressing the plasma, or reconnection between the magnetic field of low-lying loops and the field carried by the impacting material. By analyzing the emission of the brightenings in several SDO/Atmospheric Imaging Assembly wavelengths, and comparing the kinetic <span class="hlt">energy</span> of the impacting material (7.6 × 10(exp 26) - 5.8 × 10(exp 27) erg) to the radiative <span class="hlt">energy</span> (approx. 1.9 × 10(exp 25) - 2.5 × 10(exp 26) erg), we find the dominant mechanism of <span class="hlt">energy</span> <span class="hlt">release</span> involved in the observed brightening is plasma compression.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PMB....63a5028Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PMB....63a5028Z"><span>Topology-guided <span class="hlt">deformable</span> registration with local importance preservation for biomedical images</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zheng, Chaojie; Wang, Xiuying; Zeng, Shan; Zhou, Jianlong; Yin, Yong; Feng, Dagan; Fulham, Michael</p> <p>2018-01-01</p> <p>The demons registration (DR) model is well recognized for its <span class="hlt">deformation</span> capability. However, it might lead to misregistration due to erroneous diffusion direction when there are no overlaps between corresponding regions. We propose a novel registration <span class="hlt">energy</span> function, introducing topology <span class="hlt">energy</span>, and incorporating a local <span class="hlt">energy</span> function into the DR in a progressive registration scheme, to address these shortcomings. The topology <span class="hlt">energy</span> that is derived from the topological information of the images serves as a direction inference to guide diffusion transformation to retain the merits of DR. The local <span class="hlt">energy</span> constrains the <span class="hlt">deformation</span> disparity of neighbouring pixels to maintain important local texture and density features. The <span class="hlt">energy</span> function is minimized in a progressive scheme steered by a topology tree graph and we refer to it as topology-guided <span class="hlt">deformable</span> registration (TDR). We validated our TDR on 20 pairs of synthetic images with Gaussian noise, 20 phantom PET images with artificial <span class="hlt">deformations</span> and 12 pairs of clinical PET-CT studies. We compared it to three methods: (1) free-form <span class="hlt">deformation</span> registration method, (2) <span class="hlt">energy</span>-based DR and (3) multi-resolution DR. The experimental results show that our TDR outperformed the other three methods in regard to structural correspondence and preservation of the local important information including texture and density, while retaining global correspondence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1331877','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1331877"><span><span class="hlt">Deformation</span> mechanisms of nanotwinned Al</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Zhang, Xinghang</p> <p></p> <p>The objective of this project is to investigate the role of different types of layer interfaces on the formation of high density stacking fault (SF) in Al in Al/fcc multilayers, and understand the corresponding <span class="hlt">deformation</span> mechanisms of the films. Stacking faults or twins can be intentionally introduced (via growth) into certain fcc metals with low stacking fault <span class="hlt">energy</span> (such as Cu, Ag and 330 stainless steels) to achieve high strength, high ductility, superior thermal stability and good electrical conductivity. However it is still a major challenge to synthesize these types of defects into metals with high stacking fault <span class="hlt">energy</span>, suchmore » as Al. Although <span class="hlt">deformation</span> twins have been observed in some nanocrystalline Al powders by low temperature, high strain rate cryomilling or in Al at the edge of crack tip or indentation (with the assistance of high stress intensity factor), these <span class="hlt">deformation</span> techniques typically introduce twins sporadically and the control of <span class="hlt">deformation</span> twin density in Al is still not feasible. This project is designed to test the following hypotheses: (1) Certain type of layer interfaces may assist the formation of SF in Al, (2) Al with high density SF may have <span class="hlt">deformation</span> mechanisms drastically different from those of coarse-grained Al and nanotwinned Cu. To test these hypotheses, we have performed the following tasks: (i) Investigate the influence of layer interfaces, stresses and deposition parameters on the formation and density of SF in Al. (ii) Understand the role of SF on the <span class="hlt">deformation</span> behavior of Al. In situ nanoindentation experiments will be performed to probe <span class="hlt">deformation</span> mechanisms in Al. The major findings related to the formation mechanism of twins and mechanical behavior of nanotwinned metals include the followings: 1) Our studies show that nanotwins can be introduced into metals with high stacking fault <span class="hlt">energy</span>, in drastic contrast to the general anticipation. 2) We show two strategies that can effectively introduce growth</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890012065','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890012065"><span>The interpretation of crustal dynamics data in terms of plate motions and regional <span class="hlt">deformation</span> near plate boundaries</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Solomon, Sean C.</p> <p>1989-01-01</p> <p>A particularly detailed set of observations in the vicinity of an intraplate, thrust earthquake (M 7.4) in Argentina, indicate a cyclic pattern of <span class="hlt">deformation</span> very similar to that reported previously for interplate earthquakes. This <span class="hlt">deformation</span> cycle, which may be characteristic of many seismically active areas, consists of: (1) steady strain accumulation, possibly punctuated by strain reversals; (2) coseismic strain <span class="hlt">release</span>; (3) a period of continued strain <span class="hlt">release</span> due to afterslip (persisting for perhaps a year or so); and (4) rapid postseismic strain accumulation which decreases exponentially and grades into steady strain accumulation. <span class="hlt">Deformation</span> associated with three earthquakes in the U.S. (1940, M7.1 Imperial Valley California; 1964, M8.4 Alaska; 1959, M7.5 Hebgen Lake, Montana) are interpreted in light of this general earthquake cycle and are used to investigate the mechanics of strain <span class="hlt">release</span> for these events. These examples indicate that large postseismic movements can occur for strike-slip, thrust, and normal fault events, and both viscoelastic relaxation and postseismic after-slip must be incorporated in models of earthquake related <span class="hlt">deformation</span>. The mechanics of the strain <span class="hlt">release</span> process revealed by these examples has implications for estimating earthquake repeat times from geodetic observations near active faults.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26199033','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26199033"><span>[Distal soft-tissue procedure in hallux valgus <span class="hlt">deformity</span>].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Arbab, D; Wingenfeld, C; Frank, D; Bouillon, B; König, D P</p> <p>2016-04-01</p> <p>Distal, lateral soft tissue <span class="hlt">release</span> to restore mediolateral balance of the first metatarsophalangeal (MTP) joint in hallux valgus <span class="hlt">deformity</span>. Incision of the adductor hallucis tendon from the fibular sesamoid, the lateral capsule, the lateral collateral ligament, and the lateral metatarsosesamoid ligament. Hallux valgus <span class="hlt">deformities</span> or recurrent hallux valgus <span class="hlt">deformities</span> with an incongruent MTP joint. General medical contraindications to surgical interventions. Painful stiffness of the MTP joint, osteonecrosis, congruent joint. Relative contraindications: connective tissue diseases (Marfan syndrome, Ehler-Danlos syndrome). Longitudinal, dorsal incision in the first intermetatarsal web space between the first and second MTP joint. Blunt dissection and identification of the adductor hallucis tendon. <span class="hlt">Release</span> of the adductor tendon from the fibular sesamoid. Incision of the lateral capsule, the lateral collateral ligament, and the lateral metatarsosesamoid ligament. Postoperative management depends on bony correction. In joint-preserving procedures, dressing for 3 weeks in corrected position. Subsequently hallux valgus orthosis at night and a toe spreader for a further 3 months. Passive mobilization of the first MTP joint. Postoperative weight-bearing according to the osteotomy. A total of 31 patients with isolated hallux valgus <span class="hlt">deformity</span> underwent surgery with a Chevron and Akin osteotomy and a distal medial and lateral soft tissue balancing. The mean preoperative intermetatarsal (IMA) angle was 12.3° (range 11-15°); the hallux valgus (HV) angle was 28.2° (25-36°). The mean follow-up was 16.4 months (range 12-22 months). The mean postoperative IMA correction ranged between 2 and 7° (mean 5.2°); the mean HV correction was 15.5° (range 9-21°). In all, 29 patients (93%) were satisfied or very satisfied with the postoperative outcome, while 2 patients (7%) were not satisfied due to one delayed wound healing and one recurrent hallux valgus <span class="hlt">deformity</span>. There were no</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.15307007T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.15307007T"><span>Precise calculation of neutron-capture reactions contribution in <span class="hlt">energy</span> <span class="hlt">release</span> for different types of VVER-1000 fuel assemblies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tikhomirov, Georgy; Bahdanovich, Rynat; Pham, Phu</p> <p>2017-09-01</p> <p>Precise calculation of <span class="hlt">energy</span> <span class="hlt">release</span> in a nuclear reactor is necessary to obtain the correct spatial power distribution and predict characteristics of burned nuclear fuel. In this work, previously developed method for calculation neutron-capture reactions - capture component - contribution in effective <span class="hlt">energy</span> <span class="hlt">release</span> in a fuel core of nuclear reactor is discussed. The method was improved and implemented to the different models of VVER-1000 reactor developed for MCU 5 and MCNP 4 computer codes. Different models of equivalent cell and fuel assembly in the beginning of fuel cycle were calculated. These models differ by the geometry, fuel enrichment and presence of burnable absorbers. It is shown, that capture component depends on fuel enrichment and presence of burnable absorbers. Its value varies for different types of hot fuel assemblies from 3.35% to 3.85% of effective <span class="hlt">energy</span> <span class="hlt">release</span>. Average capture component contribution in effective <span class="hlt">energy</span> <span class="hlt">release</span> for typical serial fresh fuel of VVER-1000 is 3.5%, which is 7 MeV/fission. The method will be used in future to estimate the dependency of capture <span class="hlt">energy</span> on fuel density, burn-up, etc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApPhL.107f2104K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApPhL.107f2104K"><span>Compositional bowing of band <span class="hlt">energies</span> and their <span class="hlt">deformation</span> potentials in strained InGaAs ternary alloys: A first-principles study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Khomyakov, Petr A.; Luisier, Mathieu; Schenk, Andreas</p> <p>2015-08-01</p> <p>Using first-principles calculations, we show that the conduction and valence band <span class="hlt">energies</span> and their <span class="hlt">deformation</span> potentials exhibit a non-negligible compositional bowing in strained ternary semiconductor alloys such as InGaAs. The electronic structure of these compounds has been calculated within the framework of local density approximation and hybrid functional approach for large cubic supercells and special quasi-random structures, which represent two kinds of model structures for random alloys. We find that the predicted bowing effect for the band <span class="hlt">energy</span> <span class="hlt">deformation</span> potentials is rather insensitive to the choice of the functional and alloy structural model. The direction of bowing is determined by In cations that give a stronger contribution to the formation of the InxGa1-xAs valence band states with x ≳ 0.5, compared to Ga cations.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_7 --> <div id="page_8" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="141"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10563E..2YR','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10563E..2YR"><span>Performance verification and environmental testing of a unimorph <span class="hlt">deformable</span> mirror for space applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rausch, Peter; Verpoort, Sven; Wittrock, Ulrich</p> <p>2017-11-01</p> <p>Concepts for future large space telescopes require an active optics system to mitigate aberrations caused by thermal <span class="hlt">deformation</span> and gravitational <span class="hlt">release</span>. Such a system would allow on-site correction of wave-front errors and ease the requirements for thermal and gravitational stability of the optical train. In the course of the ESA project "Development of Adaptive <span class="hlt">Deformable</span> Mirrors for Space Instruments" we have developed a unimorph <span class="hlt">deformable</span> mirror designed to correct for low-order aberrations and dedicated to be used in space environment. We briefly report on design and manufacturing of the <span class="hlt">deformable</span> mirror and present results from performance verifications and environmental testing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGP...128..199P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGP...128..199P"><span>Application of the moving frame method to <span class="hlt">deformed</span> Willmore surfaces in space forms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Paragoda, Thanuja</p> <p>2018-06-01</p> <p>The main goal of this paper is to use the theory of exterior differential forms in deriving variations of the <span class="hlt">deformed</span> Willmore <span class="hlt">energy</span> in space forms and study the minimizers of the <span class="hlt">deformed</span> Willmore <span class="hlt">energy</span> in space forms. We derive both first and second order variations of <span class="hlt">deformed</span> Willmore <span class="hlt">energy</span> in space forms explicitly using moving frame method. We prove that the second order variation of <span class="hlt">deformed</span> Willmore <span class="hlt">energy</span> depends on the intrinsic Laplace Beltrami operator, the sectional curvature and some special operators along with mean and Gauss curvatures of the surface embedded in space forms, while the first order variation depends on the extrinsic Laplace Beltrami operator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NuPhA.970...29S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NuPhA.970...29S"><span><span class="hlt">Deformation</span> effect on spectral statistics of nuclei</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sabri, H.; Jalili Majarshin, A.</p> <p>2018-02-01</p> <p>In this study, we tried to get significant relations between the spectral statistics of atomic nuclei and their different degrees of <span class="hlt">deformations</span>. To this aim, the empirical <span class="hlt">energy</span> levels of 109 even-even nuclei in the 22 ≤ A ≤ 196 mass region are classified as their experimental and calculated quadrupole, octupole, hexadecapole and hexacontatetrapole <span class="hlt">deformations</span> values and analyzed by random matrix theory. Our results show an obvious relation between the regularity of nuclei and strong quadrupole, hexadecapole and hexacontatetrapole <span class="hlt">deformations</span> and but for nuclei that their octupole <span class="hlt">deformations</span> are nonzero, we have observed a GOE-like statistics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JSMTE..05.3104Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JSMTE..05.3104Z"><span>Fluctuations of a q-<span class="hlt">deformed</span> fermion gas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zeng, Qijun; Ge, Jing; Luo, Yongsong</p> <p>2018-05-01</p> <p>The theory of q-<span class="hlt">deformed</span> fermions is one of the theories of q-<span class="hlt">deformed</span> oscillators. Within the framework of this theory and the traditional fluctuation theory, we investigate fluctuations of q-<span class="hlt">deformed</span> fermion gas and obtain the expressions of fluctuations of the internal <span class="hlt">energy</span> U, the particle number N and the correlation of fluctuations of the two physical quantities above. Further numerical calculation reveals that fluctuations of such a system have some interesting and particular features. We consider that this work may provide much insight into the theory of q fermions, and may also be helpful for the theory of q-<span class="hlt">deformed</span> oscillators.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23144694','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23144694"><span><span class="hlt">Deformation</span> of the Durom acetabular component and its impact on tribology in a cadaveric model--a simulator study.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Feng; Chen, Zhefeng; Gu, Yanqing; Wang, Qing; Cui, Weiding; Fan, Weimin</p> <p>2012-01-01</p> <p>Recent studies have shown that the acetabular component frequently becomes <span class="hlt">deformed</span> during press-fit insertion. The aim of this study was to explore the <span class="hlt">deformation</span> of the Durom cup after implantation and to clarify the impact of <span class="hlt">deformation</span> on wear and ion <span class="hlt">release</span> of the Durom large head metal-on-metal (MOM) total hips in simulators. Six Durom cups impacted into reamed acetabula of fresh cadavers were used as the experimental group and another 6 size-paired intact Durom cups constituted the control group. All 12 Durom MOM total hips were put through a 3 million cycle (MC) wear test in simulators. The 6 cups in the experimental group were all <span class="hlt">deformed</span>, with a mean <span class="hlt">deformation</span> of 41.78 ± 8.86 µm. The average volumetric wear rate in the experimental group and in the control group in the first million cycle was 6.65 ± 0.29 mm(3)/MC and 0.89 ± 0.04 mm(3)/MC (t = 48.43, p = 0.000). The ion levels of Cr and Co in the experimental group were also higher than those in the control group before 2.0 MC. However there was no difference in the ion levels between 2.0 and 3.0 MC. This finding implies that the non-modular acetabular component of Durom total hip prosthesis is likely to become <span class="hlt">deformed</span> during press-fit insertion, and that the <span class="hlt">deformation</span> will result in increased volumetric wear and increased ion <span class="hlt">release</span>. This study was determined to explore the <span class="hlt">deformation</span> of the Durom cup after implantation and to clarify the impact of <span class="hlt">deformation</span> on wear and ion <span class="hlt">release</span> of the prosthesis. <span class="hlt">Deformation</span> of the cup after implantation increases the wear of MOM bearings and the resulting ion levels. The clinical use of the Durom large head prosthesis should be with great care.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29845488','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29845488"><span>Soft tissue <span class="hlt">deformation</span> modelling through neural dynamics-based reaction-diffusion mechanics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Jinao; Zhong, Yongmin; Gu, Chengfan</p> <p>2018-05-30</p> <p>Soft tissue <span class="hlt">deformation</span> modelling forms the basis of development of surgical simulation, surgical planning and robotic-assisted minimally invasive surgery. This paper presents a new methodology for modelling of soft tissue <span class="hlt">deformation</span> based on reaction-diffusion mechanics via neural dynamics. The potential <span class="hlt">energy</span> stored in soft tissues due to a mechanical load to <span class="hlt">deform</span> tissues away from their rest state is treated as the equivalent transmembrane potential <span class="hlt">energy</span>, and it is distributed in the tissue masses in the manner of reaction-diffusion propagation of nonlinear electrical waves. The reaction-diffusion propagation of mechanical potential <span class="hlt">energy</span> and nonrigid mechanics of motion are combined to model soft tissue <span class="hlt">deformation</span> and its dynamics, both of which are further formulated as the dynamics of cellular neural networks to achieve real-time computational performance. The proposed methodology is implemented with a haptic device for interactive soft tissue <span class="hlt">deformation</span> with force feedback. Experimental results demonstrate that the proposed methodology exhibits nonlinear force-displacement relationship for nonlinear soft tissue <span class="hlt">deformation</span>. Homogeneous, anisotropic and heterogeneous soft tissue material properties can be modelled through the inherent physical properties of mass points. Graphical abstract Soft tissue <span class="hlt">deformation</span> modelling with haptic feedback via neural dynamics-based reaction-diffusion mechanics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23430327','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23430327"><span><span class="hlt">Energy</span> harvesting through arterial wall <span class="hlt">deformation</span>: design considerations for a magneto-hydrodynamic generator.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pfenniger, Alois; Obrist, Dominik; Stahel, Andreas; Koch, Volker M; Vogel, Rolf</p> <p>2013-07-01</p> <p>As the complexity of active medical implants increases, the task of embedding a life-long power supply at the time of implantation becomes more challenging. A periodic renewal of the <span class="hlt">energy</span> source is often required. Human <span class="hlt">energy</span> harvesting is, therefore, seen as a possible remedy. In this paper, we present a novel idea to harvest <span class="hlt">energy</span> from the pressure-driven <span class="hlt">deformation</span> of an artery by the principle of magneto-hydrodynamics. The generator relies on a highly electrically conductive fluid accelerated perpendicularly to a magnetic field by means of an efficient lever arm mechanism. An artery with 10 mm inner diameter is chosen as a potential implantation site and its ability to drive the generator is established. Three analytical models are proposed to investigate the relevant design parameters and to determine the existence of an optimal configuration. The predicted output power reaches 65 μW according to the first two models and 135 μW according to the third model. It is found that the generator, designed as a circular structure encompassing the artery, should not exceed a total volume of 3 cm³.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EP%26S...70...62J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EP%26S...70...62J"><span>Coseismic and postseismic <span class="hlt">deformation</span> associated with the 2016 Mw 7.8 Kaikoura earthquake, New Zealand: fault movement investigation and seismic hazard analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiang, Zhongshan; Huang, Dingfa; Yuan, Linguo; Hassan, Abubakr; Zhang, Lupeng; Yang, Zhongrong</p> <p>2018-04-01</p> <p>The 2016 moment magnitude (Mw) 7.8 Kaikoura earthquake demonstrated that multiple fault segments can undergo rupture during a single seismic event. Here, we employ Global Positioning System (GPS) observations and geodetic modeling methods to create detailed images of coseismic slip and postseismic afterslip associated with the Kaikoura earthquake. Our optimal geodetic coseismic model suggests that rupture not only occurred on shallow crustal faults but also to some extent at the Hikurangi subduction interface. The GPS-inverted moment <span class="hlt">release</span> during the earthquake is equivalent to a Mw 7.9 event. The near-field postseismic <span class="hlt">deformation</span> is mainly derived from right-lateral strike-slip motions on shallow crustal faults. The afterslip did not only significantly extend northeastward on the Needles fault but also appeared at the plate interface, slowly <span class="hlt">releasing</span> <span class="hlt">energy</span> over the past 6 months, equivalent to a Mw 7.3 earthquake. Coulomb stress changes induced by coseismic <span class="hlt">deformation</span> exhibit complex patterns and diversity at different depths, undoubtedly reflecting multi-fault rupture complexity associated with the earthquake. The Coulomb stress can reach several MPa during coseismic <span class="hlt">deformation</span>, which can explain the trigger mechanisms of afterslip in two high-slip regions and the majority of aftershocks. Based on the <span class="hlt">deformation</span> characteristics of the Kaikoura earthquake, interseismic plate coverage, and historical earthquakes, we conclude that Wellington is under higher seismic threat after the earthquake and great attention should be paid to potential large earthquake disasters in the near future.[Figure not available: see fulltext.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22522197-energy-release-initiation-sunquake-class-flare','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22522197-energy-release-initiation-sunquake-class-flare"><span><span class="hlt">ENERGY</span> <span class="hlt">RELEASE</span> AND INITIATION OF A SUNQUAKE IN A C-CLASS FLARE</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Sharykin, I. N.; Kosovichev, A. G.; Zimovets, I. V.</p> <p></p> <p>We present an analysis of the C7.0 solar flare from 2013 February 17, revealing a strong helioseismic response (sunquake) caused by a compact impact observed with the Helioseismic and Magnetic Imager on board the Solar Dynamics Observatory (SDO) in the low atmosphere. This is the weakest known C-class flare generating a sunquake event. To investigate the possible mechanisms of this event and understand the role of accelerated charged particles and photospheric electric currents, we use data from three space observatories: RHESSI, SDO, and Geostationary Operational Environmental Satellite. We find that the photospheric flare impact does not spatially correspond to themore » strongest hard X-ray emission source, but both of these events are parts of the same <span class="hlt">energy</span> <span class="hlt">release</span>. Our analysis reveals a close association of the flare <span class="hlt">energy</span> <span class="hlt">release</span> with a rapid increase in the electric currents and suggests that the sunquake initiation is unlikely to be caused by the impact of high-<span class="hlt">energy</span> electrons, but may be associated with rapid current dissipation or a localized impulsive Lorentz force in the lower layers of the solar atmosphere.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/10193638','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/10193638"><span><span class="hlt">Deformation</span> twinning: Influence of strain rate</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gray, G.T. III</p> <p></p> <p>Twins in most crystal structures, including advanced materials such as intermetallics, form more readily as the temperature of <span class="hlt">deformation</span> is decreased or the rate of <span class="hlt">deformation</span> is increased. Both parameters lead to the suppression of thermally-activated dislocation processes which can result in stresses high enough to nucleate and grow <span class="hlt">deformation</span> twins. Under high-strain rate or shock-loading/impact conditions <span class="hlt">deformation</span> twinning is observed to be promoted even in high stacking fault <span class="hlt">energy</span> FCC metals and alloys, composites, and ordered intermetallics which normally do not readily <span class="hlt">deform</span> via twinning. Under such conditions and in particular under the extreme loading rates typical of shockmore » wave <span class="hlt">deformation</span> the competition between slip and <span class="hlt">deformation</span> twinning can be examined in detail. In this paper, examples of <span class="hlt">deformation</span> twinning in the intermetallics TiAl, Ti-48Al-lV and Ni{sub 3}A as well in the cermet Al-B{sub 4}C as a function of strain rate will be presented. Discussion includes: (1) the microstructural and experimental variables influencing twin formation in these systems and twinning topics related to high-strain-rate loading, (2) the high velocity of twin formation, and (3) the influence of <span class="hlt">deformation</span> twinning on the constitutive response of advanced materials.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJP..133..161C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJP..133..161C"><span>κ-<span class="hlt">deformed</span> Dirac oscillator in an external magnetic field</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chargui, Y.; Dhahbi, A.; Cherif, B.</p> <p>2018-04-01</p> <p>We study the solutions of the (2 + 1)-dimensional κ-<span class="hlt">deformed</span> Dirac oscillator in the presence of a constant transverse magnetic field. We demonstrate how the <span class="hlt">deformation</span> parameter affects the <span class="hlt">energy</span> eigenvalues of the system and the corresponding eigenfunctions. Our findings suggest that this system could be used to detect experimentally the effect of the <span class="hlt">deformation</span>. We also show that the hidden supersymmetry of the non-<span class="hlt">deformed</span> system reduces to a hidden pseudo-supersymmetry having the same algebraic structure as a result of the κ-<span class="hlt">deformation</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Tecto..34.2514M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Tecto..34.2514M"><span>The <span class="hlt">deformation</span> record of olivine in mylonitic peridotites from the Finero Complex, Ivrea Zone: Separate <span class="hlt">deformation</span> cycles during exhumation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matysiak, Agnes K.; Trepmann, Claudia A.</p> <p>2015-12-01</p> <p>Mylonitic peridotites from the Finero complex are investigated to detect characteristic olivine microfabrics that can resolve separate <span class="hlt">deformation</span> cycles at different metamorphic conditions. The heterogeneous olivine microstructures are characterized by <span class="hlt">deformed</span> porphyroclasts surrounded by varying amounts of recrystallized grains. A well-developed but only locally preserved foam structure is present in recrystallized grain aggregates. This indicates an early stage of dynamic recrystallization and subsequent recovery and recrystallization at quasi-static stress conditions, where the strain <span class="hlt">energy</span> was reduced such that a reduction in surface <span class="hlt">energy</span> controlled grain boundary migration. Ultramylonites record a renewed stage of localized <span class="hlt">deformation</span> and recrystallization by a second generation of recrystallized grains that do not show a foam structure. This second generation of recrystallized grains as well as sutured grain and kink band boundaries of porphyroclasts indicate that these microstructures developed during a stage of localized <span class="hlt">deformation</span> after development of the foam structure. The heterogeneity of the microfabrics is interpreted to represent several (at least two) cycles of localized <span class="hlt">deformation</span> separated by a marked hiatus with quasi-static recrystallization and recovery and eventually grain growth. The second <span class="hlt">deformation</span> cycle did not only result in reactivation of preexisting shear zones but instead also locally affected the host rock that was not <span class="hlt">deformed</span> in the first stage. Such stress cycles can result from sudden increases in differential stress imposed by seismic events, i.e., high stress-loading rates, during exhumation of the Finero complex.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23303613','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23303613"><span>[Modified chevron osteotomy with lateral <span class="hlt">release</span> and screw fixation for treatment of severe hallux <span class="hlt">deformity</span>].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hofstaetter, S G; Schuh, R; Trieb, K; Trnka, H J</p> <p>2012-12-01</p> <p>This prospective study examined the clinical and radiological results of the Chevron osteotomy with screw fixation and distal soft tissue <span class="hlt">release</span> up to an intermetatarsal angle of 19°. Furthermore, the results are presented for patients over the age of 70 years, and whether or not there is a higher complication rate. 86 feet of patients between 23 and 81 years were included in the study. Apart from the overall group, a group with an intermetatarsal angle of 16° to 19° and a group of patients over 70 years old were eavaluated. They were evaluated preoperatively and at follow-up after an average of 3.3 years according to the American Orthopaedic Foot and Ankle Society score. The AOFAS score showed a significant improvement from 55 points preoperatively to 90 points at follow-up. The preoperative hallux valgus angle decreased significantly from 32° to 5° and the preoperative intermetatarsal angle decreased from 14° to 6°. Patient satisfaction in the overall group was rated in 92 % as excellent or good. Also, the patient group with 16° to 19° angles and the patients over 70 years showed a significant improvement of clinical and radiological parameters. The complication rate was very low in all groups. The results show that the Chevron osteotomy is a very good surgical technique with few complications for the correction of splay foot with hallux valgus <span class="hlt">deformity</span>. We showed that by using the modified technique with a long plantar arm, an excessive soft tissue <span class="hlt">release</span> and screw fixation, the indication can be extended up to an intermetatarsal angle of 19° when using screw fixation. Furthermore the patients over 70 years of age showed a significant improvement of clinical and radiological parameters without serious complications such as avascular necrosis or dislocation of the metatarsal head. Georg Thieme Verlag KG Stuttgart · New York.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/14704784','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/14704784"><span><span class="hlt">Deformation</span>-mechanism map for nanocrystalline metals by molecular-dynamics simulation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yamakov, V; Wolf, D; Phillpot, S R; Mukherjee, A K; Gleiter, H</p> <p>2004-01-01</p> <p>Molecular-dynamics simulations have recently been used to elucidate the transition with decreasing grain size from a dislocation-based to a grain-boundary-based <span class="hlt">deformation</span> mechanism in nanocrystalline f.c.c. metals. This transition in the <span class="hlt">deformation</span> mechanism results in a maximum yield strength at a grain size (the 'strongest size') that depends strongly on the stacking-fault <span class="hlt">energy</span>, the elastic properties of the metal, and the magnitude of the applied stress. Here, by exploring the role of the stacking-fault <span class="hlt">energy</span> in this crossover, we elucidate how the size of the extended dislocations nucleated from the grain boundaries affects the mechanical behaviour. Building on the fundamental physics of <span class="hlt">deformation</span> as exposed by these simulations, we propose a two-dimensional stress-grain size <span class="hlt">deformation</span>-mechanism map for the mechanical behaviour of nanocrystalline f.c.c. metals at low temperature. The map captures this transition in both the <span class="hlt">deformation</span> mechanism and the related mechanical behaviour with decreasing grain size, as well as its dependence on the stacking-fault <span class="hlt">energy</span>, the elastic properties of the material, and the applied stress level.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013IJMMM..20..529H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013IJMMM..20..529H"><span>Hot compression <span class="hlt">deformation</span> behavior of AISI 321 austenitic stainless steel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haj, Mehdi; Mansouri, Hojjatollah; Vafaei, Reza; Ebrahimi, Golam Reza; Kanani, Ali</p> <p>2013-06-01</p> <p>The hot compression behavior of AISI 321 austenitic stainless steel was studied at the temperatures of 950-1100°C and the strain rates of 0.01-1 s-1 using a Baehr DIL-805 <span class="hlt">deformation</span> dilatometer. The hot <span class="hlt">deformation</span> equations and the relationship between hot <span class="hlt">deformation</span> parameters were obtained. It is found that strain rate and <span class="hlt">deformation</span> temperature significantly influence the flow stress behavior of the steel. The work hardening rate and the peak value of flow stress increase with the decrease of <span class="hlt">deformation</span> temperature and the increase of strain rate. In addition, the activation <span class="hlt">energy</span> of <span class="hlt">deformation</span> ( Q) is calculated as 433.343 kJ/mol. The microstructural evolution during <span class="hlt">deformation</span> indicates that, at the temperature of 950°C and the strain rate of 0.01 s-1, small circle-like precipitates form along grain boundaries; but at the temperatures above 950°C, the dissolution of such precipitates occurs. <span class="hlt">Energy</span>-dispersive X-ray analyses indicate that the precipitates are complex carbides of Cr, Fe, Mn, Ni, and Ti.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28017574','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28017574"><span>Correcting Severe Varus <span class="hlt">Deformity</span> Using Trial Components During Total Knee Arthroplasty.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Man S; Koh, In J; Choi, Young J; Kim, Yong D; In, Yong</p> <p>2017-05-01</p> <p>Extensive medial soft tissue <span class="hlt">release</span> may be necessary to correct severe varus <span class="hlt">deformity</span> during total knee arthroplasty (TKA). However, this procedure may result in instability. Here, we describe a novel soft tissue balancing technique, which can minimize medial <span class="hlt">release</span> in severe varus <span class="hlt">deformity</span> during TKA. Fifty knees (40 patients) with hip-knee-ankle angle of more than 20° of varus were corrected using this technique (group 1). After achieving flexion gap balancing by needle puncturing and spreading of the superficial medial collateral ligament, extension gap balancing was obtained by gradual extension with the trial components in place. After group 1 was set, a one-to-one patient-matched control group who had mild varus <span class="hlt">deformity</span> was selected by propensity score matching (50 knees, 48 patients, group 2). At postoperative 1 year, mediolateral laxity was compared between the 2 groups using the stress radiographs. Clinical outcomes were also compared using the Knee Society Score and Western Ontario and McMaster Universities Osteoarthritis Index score. There were no differences in mean medial and lateral laxities between groups 1 and 2 at 1 year after the operation (medial laxity: 2.3° ± 1.4° and 2.7° ± 1.3°, respectively, P = .310) (lateral laxity: 3.6° ± 1.7° and 3.2° ± 2.0°, respectively, P = .459). There were no significant differences in postoperative clinical scores and knee alignment. Our technique of obtaining extension gap balancing using trial components led to safe and effective balancing by avoiding unnecessary extensive <span class="hlt">release</span> in severe varus <span class="hlt">deformity</span> during TKA. Copyright © 2016 Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28339258','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28339258"><span>Atomistic Origin of <span class="hlt">Deformation</span> Twinning in Biomineral Aragonite.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Jialin; Huang, Zaiwang; Pan, Zhiliang; Wei, Qiuming; Li, Xiaodong; Qi, Yue</p> <p>2017-03-10</p> <p><span class="hlt">Deformation</span> twinning rarely occurs in mineral materials which typically show brittle fracture. Surprisingly, it has recently been observed in the biomineral aragonite phase in nacre under high rate impact loading. In this Letter, the twinning tendency and the competition between fracture and <span class="hlt">deformation</span> twinning were revealed by first principles calculations. The ratio of the unstable stacking fault <span class="hlt">energy</span> and the stacking fault <span class="hlt">energy</span> in orthorhombic aragonite is hitherto the highest in a broad range of metallic and oxide materials. The underlining physics for this high ratio is the multineighbor shared ionic bonds and the unique relaxation process during sliding in the aragonite structure. Overall, the unique <span class="hlt">deformation</span> twining along with other highly coordinated <span class="hlt">deformation</span> mechanisms synergistically work in the hierarchical structure of nacre, leading to the remarkable strengthening and toughening of nacre upon dynamic loading, and thus protecting the mother-of-pearl from predatory attacks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21245354','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21245354"><span>Tension-dependent structural <span class="hlt">deformation</span> alters single-molecule transition kinetics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sudhanshu, B; Mihardja, S; Koslover, E F; Mehraeen, S; Bustamante, C; Spakowitz, A J</p> <p>2011-02-01</p> <p>We analyze the response of a single nucleosome to tension, which serves as a prototypical biophysical measurement where tension-dependent <span class="hlt">deformation</span> alters transition kinetics. We develop a statistical-mechanics model of a nucleosome as a wormlike chain bound to a spool, incorporating fluctuations in the number of bases bound, the spool orientation, and the conformations of the unbound polymer segments. With the resulting free-<span class="hlt">energy</span> surface, we perform dynamic simulations that permit a direct comparison with experiments. This simple approach demonstrates that the experimentally observed structural states at nonzero tension are a consequence of the tension and that these tension-induced states cease to exist at zero tension. The transitions between states exhibit substantial <span class="hlt">deformation</span> of the unbound polymer segments. The associated <span class="hlt">deformation</span> <span class="hlt">energy</span> increases with tension; thus, the application of tension alters the kinetics due to tension-induced <span class="hlt">deformation</span> of the transition states. This mechanism would arise in any system where the tether molecule is <span class="hlt">deformed</span> in the transition state under the influence of tension.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9056E..37F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9056E..37F"><span>Optimized <span class="hlt">deformation</span> behavior of a dielectric elastomer generator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Foerster, Florentine; Schlaak, Helmut F.</p> <p>2014-03-01</p> <p>Dielectric elastomer generators (DEGs) produce electrical <span class="hlt">energy</span> by converting mechanical into electrical <span class="hlt">energy</span>. Efficient operation requires an optimal <span class="hlt">deformation</span> of the DEG during the <span class="hlt">energy</span> harvesting cycle. However, the <span class="hlt">deformation</span> resulting from an external load has to be applied to the DEG. The <span class="hlt">deformation</span> behavior of the DEG is dependent on the type of the mechanical interconnection between the elastic DEG and a stiff support area. The maximization of the capacitance of the DEG in the <span class="hlt">deformed</span> state leads to the maximum absolute <span class="hlt">energy</span> gain. Therefore several configurations of mechanical interconnections between a single DEG module as well as multiple stacked DEG modules and stiff supports are investigated in order to find the optimal mechanical interconnection. The investigation is done with numerical simulations using the FEM software ANSYS. A DEG module consists of 50 active dielectric layers with a single layer thickness of 50 μm. The elastomer material is silicone (PDMS) while the compliant electrodes are made of graphite powder. In the simulation the real material parameters of the PDMS and the graphite electrodes are included to compare simulation results to experimental investigations in the future. The numerical simulations of the several configurations are carried out as coupled electro-mechanical simulation for the first step in an <span class="hlt">energy</span> harvesting cycle with constant external load strain. The simulation results are discussed and an optimal mechanical interconnection between DEG modules and stiff supports is derived.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Nanos...811924C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Nanos...811924C"><span>Analysing intracellular <span class="hlt">deformation</span> of polymer capsules using structured illumination microscopy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Xi; Cui, Jiwei; Sun, Huanli; Müllner, Markus; Yan, Yan; Noi, Ka Fung; Ping, Yuan; Caruso, Frank</p> <p>2016-06-01</p> <p>Understanding the behaviour of therapeutic carriers is important in elucidating their mechanism of action and how they are processed inside cells. Herein we examine the intracellular <span class="hlt">deformation</span> of layer-by-layer assembled polymer capsules using super-resolution structured illumination microscopy (SIM). Spherical- and cylindrical-shaped capsules were studied in three different cell lines, namely HeLa (human epithelial cell line), RAW264.7 (mouse macrophage cell line) and differentiated THP-1 (human monocyte-derived macrophage cell line). We observed that the <span class="hlt">deformation</span> of capsules was dependent on cell line, but independent of capsule shape. This suggests that the mechanical forces, which induce capsule <span class="hlt">deformation</span> during cell uptake, vary between cell lines, indicating that the capsules are exposed to higher mechanical forces in HeLa cells, followed by RAW264.7 and then differentiated THP-1 cells. Our study demonstrates the use of super-resolution SIM in analysing intracellular capsule <span class="hlt">deformation</span>, offering important insights into the cellular processing of drug carriers in cells and providing fundamental knowledge of intracellular mechanobiology. Furthermore, this study may aid in the design of novel drug carriers that are sensitive to <span class="hlt">deformation</span> for enhanced drug <span class="hlt">release</span> properties.Understanding the behaviour of therapeutic carriers is important in elucidating their mechanism of action and how they are processed inside cells. Herein we examine the intracellular <span class="hlt">deformation</span> of layer-by-layer assembled polymer capsules using super-resolution structured illumination microscopy (SIM). Spherical- and cylindrical-shaped capsules were studied in three different cell lines, namely HeLa (human epithelial cell line), RAW264.7 (mouse macrophage cell line) and differentiated THP-1 (human monocyte-derived macrophage cell line). We observed that the <span class="hlt">deformation</span> of capsules was dependent on cell line, but independent of capsule shape. This suggests that the mechanical forces</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSH14B..05K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSH14B..05K"><span>Triggers and Manifestations of Flare <span class="hlt">Energy</span> <span class="hlt">Release</span> in the Low Atmosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kosovichev, A. G.; Sharykin, I. N.; Sadykov, V. M.; Vargas, S.; Zimovets, I. V.</p> <p>2016-12-01</p> <p>The main goal is to understand triggers and manifestations of the flare <span class="hlt">energy</span> <span class="hlt">release</span> in the lower layers of the solar atmosphere (the photosphere and chromosphere) using high-resolution optical observations and magnetic field measurements. As a case study we present results for an M-class flare. We analyze optical images, HMI Dopplergrams and vector magnetograms, and use Non-Linear Force-Free Field (NLFFF) extrapolation for reconstruction of the magnetic topology. The NLFFF modelling reveals interaction of oppositely directed magnetic flux-tubes in the Polarity Inversion Line (PIL). These two interacting magnetic flux tubes are observed as a compact sheared arcade along the PIL in the high-resolution broad-band continuum images from New Solar Telescope (NST). In the vicinity of the PIL, the NST H-alpha observations reveal formation of a thin three-ribbon structure corresponding to the small-scale photospheric magnetic arcade. Magnetic reconnection is triggered by two interacting magnetic flux tubes with forming current sheet extended along the PIL. Presented observational results evidence in favor of location of the primary <span class="hlt">energy</span> <span class="hlt">release</span> site in the dense chromosphere where plasma is partially ionized in the region of strong electric currents concentrated near the polarity inversion line.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790006996','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790006996"><span>Enclosure fire hazard analysis using relative <span class="hlt">energy</span> <span class="hlt">release</span> criteria. [burning rate and combustion control</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Coulbert, C. D.</p> <p>1978-01-01</p> <p>A method for predicting the probable course of fire development in an enclosure is presented. This fire modeling approach uses a graphic plot of five fire development constraints, the relative <span class="hlt">energy</span> <span class="hlt">release</span> criteria (RERC), to bound the heat <span class="hlt">release</span> rates in an enclosure as a function of time. The five RERC are flame spread rate, fuel surface area, ventilation, enclosure volume, and total fuel load. They may be calculated versus time based on the specified or empirical conditions describing the specific enclosure, the fuel type and load, and the ventilation. The calculation of these five criteria, using the common basis of <span class="hlt">energy</span> <span class="hlt">release</span> rates versus time, provides a unifying framework for the utilization of available experimental data from all phases of fire development. The plot of these criteria reveals the probable fire development envelope and indicates which fire constraint will be controlling during a criteria time period. Examples of RERC application to fire characterization and control and to hazard analysis are presented along with recommendations for the further development of the concept.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/9366334','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/9366334"><span>Reconstruction of <span class="hlt">deformities</span> resulting from penile enlargement surgery.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Alter, G J</p> <p>1997-12-01</p> <p>More than 30 patients presented for reconstruction of penile <span class="hlt">deformities</span> secondary to penile enlargement surgery performed by other physicians. Lengthening was performed by <span class="hlt">releasing</span> the suspensory ligament of the penis and advancing pubic skin with a V-Y advancement flap. Girth was increased by injecting autologous fat. Specific complaints relating to the lengthening procedure involve hypertrophic and/or wide scars, a proximal penile hump from a thick, hair-bearing V-Y flap, and a low hanging penis. Complications relating to autologous fat injections include disappearance of fat, penile lumps and nodules, and shaft <span class="hlt">deformities</span>. The repair of these <span class="hlt">deformities</span> is described. From 1994 through October 1996, 19 men underwent 24 various combinations of reconstructive operations, such as scar revisions, V-Y advancement flap reversal, and removal of fat nodules and asymmetrical fat deposits. Penile appearance and function were improved. Complications include 1 hematoma requiring drainage, minor wound complications and 1 inadequately reversed V-Y flap. The methods of various repairs are discussed, including reconstructive limitations, timing and staging. Significant improvement can be achieved with proper reconstruction of penile <span class="hlt">deformities</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4423841','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4423841"><span>cAMP-Signalling Regulates Gametocyte-Infected Erythrocyte <span class="hlt">Deformability</span> Required for Malaria Parasite Transmission</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Thompson, Eloise; Breil, Florence; Lorthiois, Audrey; Dupuy, Florian; Cummings, Ross; Duffier, Yoann; Corbett, Yolanda; Mercereau-Puijalon, Odile; Vernick, Kenneth; Taramelli, Donatella; Baker, David A.; Langsley, Gordon; Lavazec, Catherine</p> <p>2015-01-01</p> <p>Blocking Plasmodium falciparum transmission to mosquitoes has been designated a strategic objective in the global agenda of malaria elimination. Transmission is ensured by gametocyte-infected erythrocytes (GIE) that sequester in the bone marrow and at maturation are <span class="hlt">released</span> into peripheral blood from where they are taken up during a mosquito blood meal. <span class="hlt">Release</span> into the blood circulation is accompanied by an increase in GIE <span class="hlt">deformability</span> that allows them to pass through the spleen. Here, we used a microsphere matrix to mimic splenic filtration and investigated the role of cAMP-signalling in regulating GIE <span class="hlt">deformability</span>. We demonstrated that mature GIE <span class="hlt">deformability</span> is dependent on reduced cAMP-signalling and on increased phosphodiesterase expression in stage V gametocytes, and that parasite cAMP-dependent kinase activity contributes to the stiffness of immature gametocytes. Importantly, pharmacological agents that raise cAMP levels in transmissible stage V gametocytes render them less <span class="hlt">deformable</span> and hence less likely to circulate through the spleen. Therefore, phosphodiesterase inhibitors that raise cAMP levels in P. falciparum infected erythrocytes, such as sildenafil, represent new candidate drugs to block transmission of malaria parasites. PMID:25951195</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT.......113D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT.......113D"><span>Understanding the Relationships Between Architecture, Chemistry, and <span class="hlt">Energy</span> <span class="hlt">Release</span> of Energetic Nanocomposites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>DeLisio, Jeffery Brandon</p> <p></p> <p>Energetic nanocomposites are a class of reactive material that incorporate nanosized materials or features in order to enhance reaction kinetics and <span class="hlt">energy</span> densities. Typically, these systems employ metal nanoparticles as the fuel source and have demonstrated reactivities orders of magnitude larger than more traditionally used micron-sized metal fuels. One drawback of using nanosized metals is that the nascent oxide shell comprises a significant weight percent as the particle size decreases. This shell also complicates the understanding of oxidation mechanisms of nanosized metal fuels. In this dissertation, I apply a two-fold approach to understanding the relationships between architecture, chemistry, and <span class="hlt">energy</span> <span class="hlt">release</span> of energetic nanocomposites by 1) investigating alternative metal fuels to develop a deeper understanding of the reaction mechanisms of energetic nanocomposites and 2) creating unique microstructures to tailor macroscopic properties allowing for customizability of energetic performance. In order to accurately study these systems, new analytical techniques capable of high heating rate analysis were developed. The oxidation mechanisms of tantalum nanoparticles was first probed using high heating rate TEM and Temperature-Jump Time-of-Flight Mass Spectrometry (T-Jump TOFMS) and shell crystallization was found to plan an important role in the mechanism. An air-sensitive sample holder was developed and employed to analyze the decomposition and oxidation of molecular aluminum compounds, which theoretically can achieve similar <span class="hlt">energy</span> <span class="hlt">release</span> rates to monomolecular explosives in addition to much higher <span class="hlt">energy</span> densities. In order to obtain simultaneous thermal and speciation data at high heating rates, a nanocalorimeter was integrated into the TOFMS system and measurements were performed on Al/CuO nanolaminates to probe the effect of bilayer thickness on <span class="hlt">energy</span> <span class="hlt">release</span>. An electrospray based approach to creating energetic nanocomposites with tunable</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28375346','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28375346"><span>High <span class="hlt">energy</span>, widely tunable Si-prism-array coupled terahertz-wave parametric oscillator with a <span class="hlt">deformed</span> pump and optimal crystal location for angle tuning.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Ruiliang; Qu, Yanchen; Zhao, Weijiang; Chen, Zhenlei</p> <p>2017-03-20</p> <p>A high <span class="hlt">energy</span>, widely tunable Si-prism-array coupled terahertz-wave parametric oscillator (TPO) has been demonstrated by using a <span class="hlt">deformed</span> pump. The <span class="hlt">deformed</span> pump is cut from a beam spot of 2 mm in diameter by a 1-mm-wide slit. In comparison with a small pump spot (1-mm diameter), the THz-wave coupling area for the <span class="hlt">deformed</span> pump is increased without limitation to the low-frequency end of the tuning range. Besides, the crystal location is specially designed to eliminate the alteration of the output position of the pump during angle tuning, so the initially adjusted nearest pumped region to the THz-wave exit surface is maintained throughout the tuning range. The tuning range is 0.58-2.5 THz for the <span class="hlt">deformed</span> pump, while its low frequency end is limited at approximately 1.2 THz for the undeformed pump with 2 mm diameter. The highest THz-wave output of 2 μJ, which is 2.25 times as large as that from the pump of 1 mm in diameter, is obtained at 1.15 THz under 38 mJ (300  MW/cm<sup>2</sup>) pumping. The <span class="hlt">energy</span> conversion efficiency is 5.3×10<sup>-5</sup>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22436671','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22436671"><span>Temperature-dependent ideal strength and stacking fault <span class="hlt">energy</span> of fcc Ni: a first-principles study of shear <span class="hlt">deformation</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shang, S L; Wang, W Y; Wang, Y; Du, Y; Zhang, J X; Patel, A D; Liu, Z K</p> <p>2012-04-18</p> <p>Variations of <span class="hlt">energy</span>, stress, and magnetic moment of fcc Ni as a response to shear <span class="hlt">deformation</span> and the associated ideal shear strength (τ(IS)), intrinsic (γ(SF)) and unstable (γ(US)) stacking fault <span class="hlt">energies</span> have been studied in terms of first-principles calculations under both the alias and affine shear regimes within the {111} slip plane along the <112> and <110> directions. It is found that (i) the intrinsic stacking fault <span class="hlt">energy</span> γ(SF) is nearly independent of the shear <span class="hlt">deformation</span> regimes used, albeit a slightly smaller value is predicted by pure shear (with relaxation) compared to the one from simple shear (without relaxation); (ii) the minimum ideal shear strength τ(IS) is obtained by pure alias shear of {111}<112>; and (iii) the dissociation of the 1/2[110] dislocation into two partial Shockley dislocations (1/6[211] + 1/6[121]) is observed under pure alias shear of {111}<110>. Based on the quasiharmonic approach from first-principles phonon calculations, the predicted γ(SF) has been extended to finite temperatures. In particular, using a proposed quasistatic approach on the basis of the predicted volume versus temperature relation, the temperature dependence of τ(IS) is also obtained. Both the γ(SF) and the τ(IS) of fcc Ni decrease with increasing temperature. The computed ideal shear strengths as well as the intrinsic and unstable stacking fault <span class="hlt">energies</span> are in favorable accord with experiments and other predictions in the literature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6120701','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/6120701"><span>Temperature actuated automatic safety rod <span class="hlt">release</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Hutter, E.; Pardini, J.A.; Walker, D.E.</p> <p>1984-03-13</p> <p>A temperature-actuated apparatus is disclosed for <span class="hlt">releasably</span> supporting a safety rod in a nuclear reactor, comprising a safety rod upper adapter having a retention means, a drive shaft which houses the upper adapter, and a bimetallic means supported within the drive shaft and having at least one ledge which engages a retention means of the safety rod upper adapter. A pre-determined increase in temperature causes the bimetallic means to <span class="hlt">deform</span> so that the ledge disengages from the retention means, whereby the bimetallic means <span class="hlt">releases</span> the safety rod into the core of the reactor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/866200','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/866200"><span>Temperature actuated automatic safety rod <span class="hlt">release</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Hutter, Ernest; Pardini, John A.; Walker, David E.</p> <p>1987-01-01</p> <p>A temperature-actuated apparatus is disclosed for <span class="hlt">releasably</span> supporting a safety rod in a nuclear reactor, comprising a safety rod upper adapter having a retention means, a drive shaft which houses the upper adapter, and a bimetallic means supported within the drive shaft and having at least one ledge which engages a retention means of the safety rod upper adapter. A pre-determined increase in temperature causes the bimetallic means to <span class="hlt">deform</span> so that the ledge disengages from the retention means, whereby the bimetallic means <span class="hlt">releases</span> the safety rod into the core of the reactor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1113436','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1113436"><span>Finite <span class="hlt">Deformation</span> of Magnetoelastic Film</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Barham, Matthew Ian</p> <p>2011-05-31</p> <p>A nonlinear two-dimensional theory is developed for thin magnetoelastic lms capable of large <span class="hlt">deformations</span>. This is derived directly from three-dimensional theory. Signi cant simpli cations emerge in the descent from three dimensions to two, permitting the self eld generated by the body to be computed a posteriori. The model is specialized to isotropic elastomers with two material models. First weak magnetization is investigated leading to a free <span class="hlt">energy</span> where magnetization and <span class="hlt">deformation</span> are un-coupled. The second closely couples the magnetization and <span class="hlt">deformation</span>. Numerical solutions are obtained to equilibrium boundary-value problems in which the membrane is subjected to lateral pressure andmore » an applied magnetic eld. An instability is inferred and investigated for the weak magnetization material model.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JHEP...02..165G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JHEP...02..165G"><span>Mass <span class="hlt">deformations</span> of 5d SCFTs via holography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gutperle, Michael; Kaidi, Justin; Raj, Himanshu</p> <p>2018-02-01</p> <p>Using six-dimensional Euclidean F (4) gauged supergravity we construct a holographic renormalization group flow for a CFT on S 5. Numerical solutions to the BPS equations are obtained and the free <span class="hlt">energy</span> of the theory on S 5 is determined holographically by calculation of the renormalized on-shell supergravity action. In the process, we deal with subtle issues such as holographic renormalization and addition of finite counterterms. We then propose a candidate field theory dual to these solutions. This tentative dual is a supersymmetry-preserving <span class="hlt">deformation</span> of the strongly-coupled non-Lagrangian SCFT derived from the D4-D8 system in string theory. In the IR, this theory is a mass <span class="hlt">deformation</span> of a USp(2 N ) gauge theory. A localization calculation of the free <span class="hlt">energy</span> is performed for this IR theory, which for reasonably small values of the <span class="hlt">deformation</span> parameter is found to have the same qualitative behaviour as the holographic free <span class="hlt">energy</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3483233','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3483233"><span><span class="hlt">Deformation</span> of the Durom Acetabular Component and Its Impact on Tribology in a Cadaveric Model—A Simulator Study</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gu, Yanqing; Wang, Qing; Cui, Weiding; Fan, Weimin</p> <p>2012-01-01</p> <p>Background Recent studies have shown that the acetabular component frequently becomes <span class="hlt">deformed</span> during press-fit insertion. The aim of this study was to explore the <span class="hlt">deformation</span> of the Durom cup after implantation and to clarify the impact of <span class="hlt">deformation</span> on wear and ion <span class="hlt">release</span> of the Durom large head metal-on-metal (MOM) total hips in simulators. Methods Six Durom cups impacted into reamed acetabula of fresh cadavers were used as the experimental group and another 6 size-paired intact Durom cups constituted the control group. All 12 Durom MOM total hips were put through a 3 million cycle (MC) wear test in simulators. Results The 6 cups in the experimental group were all <span class="hlt">deformed</span>, with a mean <span class="hlt">deformation</span> of 41.78±8.86 µm. The average volumetric wear rate in the experimental group and in the control group in the first million cycle was 6.65±0.29 mm3/MC and 0.89±0.04 mm3/MC (t = 48.43, p = 0.000). The ion levels of Cr and Co in the experimental group were also higher than those in the control group before 2.0 MC. However there was no difference in the ion levels between 2.0 and 3.0 MC. Conclusions This finding implies that the non-modular acetabular component of Durom total hip prosthesis is likely to become <span class="hlt">deformed</span> during press-fit insertion, and that the <span class="hlt">deformation</span> will result in increased volumetric wear and increased ion <span class="hlt">release</span>. Clinical Relevance This study was determined to explore the <span class="hlt">deformation</span> of the Durom cup after implantation and to clarify the impact of <span class="hlt">deformation</span> on wear and ion <span class="hlt">release</span> of the prosthesis. <span class="hlt">Deformation</span> of the cup after implantation increases the wear of MOM bearings and the resulting ion levels. The clinical use of the Durom large head prosthesis should be with great care. PMID:23144694</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8e6234G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8e6234G"><span>Effect of <span class="hlt">deformation</span> ratios on grain alignment and magnetic properties of hot pressing/hot <span class="hlt">deformation</span> Nd-Fe-B magnets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Zhaohui; Li, Mengyu; Wang, Junming; Jing, Zheng; Yue, Ming; Zhu, Minggang; Li, Wei</p> <p>2018-05-01</p> <p>The magnetic properties, microstructure and orientation degrees of hot pressing magnet and hot <span class="hlt">deformation</span> Nd-Fe-B magnets with different <span class="hlt">deformation</span> ratios have been investigated in this paper. The remanence (Br) and maximum magnetic <span class="hlt">energy</span> product ((BH)max) were enhanced gradually with the <span class="hlt">deformation</span> ratio increasing from 0% to 70%, whereas the coercivity (HCj) decreased. The scanning electron microscopy (SEM) images of fractured surfaces parallel to the pressure direction during hot <span class="hlt">deformation</span> show that the grains tend to extend perpendicularly to the c-axes of Nd2Fe14B grains under the pressure, and the aspect ratios of the grains increase with the increase of <span class="hlt">deformation</span> ratio. Besides, the compression stress induces the long axis of grains to rotate and the angle (θ) between c-axis and pressure direction decreases. The X-ray diffraction (XRD) patterns reveal that orientation degree improves with the increase of <span class="hlt">deformation</span> ratio, agreeing well with the SEM results. The hot <span class="hlt">deformation</span> magnet with a <span class="hlt">deformation</span> ratio of 70% has the best Br and (BH)max, and the magnetic properties are as followed: Br=1.40 T, HCj=10.73 kOe, (BH)max=42.30 MGOe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3033304','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3033304"><span>Tension-dependent structural <span class="hlt">deformation</span> alters single-molecule transition kinetics</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Sudhanshu, B.; Mihardja, S.; Koslover, E. F.; Mehraeen, S.; Bustamante, C.; Spakowitz, A. J.</p> <p>2011-01-01</p> <p>We analyze the response of a single nucleosome to tension, which serves as a prototypical biophysical measurement where tension-dependent <span class="hlt">deformation</span> alters transition kinetics. We develop a statistical-mechanics model of a nucleosome as a wormlike chain bound to a spool, incorporating fluctuations in the number of bases bound, the spool orientation, and the conformations of the unbound polymer segments. With the resulting free-<span class="hlt">energy</span> surface, we perform dynamic simulations that permit a direct comparison with experiments. This simple approach demonstrates that the experimentally observed structural states at nonzero tension are a consequence of the tension and that these tension-induced states cease to exist at zero tension. The transitions between states exhibit substantial <span class="hlt">deformation</span> of the unbound polymer segments. The associated <span class="hlt">deformation</span> <span class="hlt">energy</span> increases with tension; thus, the application of tension alters the kinetics due to tension-induced <span class="hlt">deformation</span> of the transition states. This mechanism would arise in any system where the tether molecule is <span class="hlt">deformed</span> in the transition state under the influence of tension. PMID:21245354</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.7472M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.7472M"><span>Experimental <span class="hlt">deformation</span> of a mafic rock - interplay between fracturing, reaction and viscous <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marti, Sina; Stünitz, Holger; Heilbronner, Renée; Plümper, Oliver; Drury, Martyn</p> <p>2016-04-01</p> <p> accommodate strain via dissolution precipitation creep. The transition from dominantly brittle, to dominantly viscous <span class="hlt">deformation</span> is determined by the onset of diffusive mass transport. In the transitional regime, reaction kinetics are strongly dependent on strain <span class="hlt">energy</span> and viscously <span class="hlt">deforming</span> SB form most likely from an initial brittle stage in a dominantly brittle behaving rock. Viscous <span class="hlt">deformation</span> in our experiments takes place at comparatively low experimental T, providing a realistic phase assemblage and likely <span class="hlt">deformation</span> mechanism for the lower crust.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1260431-interfacial-diffusion-aided-deformation-during-nanoindentation','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1260431-interfacial-diffusion-aided-deformation-during-nanoindentation"><span>Interfacial diffusion aided <span class="hlt">deformation</span> during nanoindentation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Samanta, Amit; E., Weinan</p> <p>2015-07-06</p> <p>Nanoindentation is commonly used to quantify the mechanical response of material surfaces. Despite its widespread use, a detailed understanding of the <span class="hlt">deformation</span> mechanisms responsible for plasticity during these experiments has remained elusive. Nanoindentation measurements often show stress values close to a material’s ideal strength which suggests that dislocation nucleation and subsequent dislocation activity dominates the <span class="hlt">deformation</span>. However, low strain-rate exponents and small activation volumes have also been reported which indicates high temperature sensitivity of the <span class="hlt">deformation</span> processes. Using an order parameter aided temperature accelerated sampling technique called adiabatic free <span class="hlt">energy</span> dynamics [J. B. Abrams and M. E. Tuckerman, J. Phys.more » Chem. B, 112, 15742 (2008)], and molecular dynamics we have probed the diffusive mode of <span class="hlt">deformation</span> during nanoindentation. Localized processes such as surface vacancy and ad-atom pair formation, vacancy diffusion are found to play an important role during indentation. Furthermore, our analysis suggests a change in the dominant <span class="hlt">deformation</span> mode from dislocation mediated plasticity to diffusional flow at high temperatures, slow indentation rates and small indenter tip radii.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28119554','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28119554"><span>The anelastic Ericksen problem: universal eigenstrains and <span class="hlt">deformations</span> in compressible isotropic elastic solids.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yavari, Arash; Goriely, Alain</p> <p>2016-12-01</p> <p>The elastic Ericksen problem consists of finding <span class="hlt">deformations</span> in isotropic hyperelastic solids that can be maintained for arbitrary strain-<span class="hlt">energy</span> density functions. In the compressible case, Ericksen showed that only homogeneous <span class="hlt">deformations</span> are possible. Here, we solve the anelastic version of the same problem, that is, we determine both the <span class="hlt">deformations</span> and the eigenstrains such that a solution to the anelastic problem exists for arbitrary strain-<span class="hlt">energy</span> density functions. Anelasticity is described by finite eigenstrains. In a nonlinear solid, these eigenstrains can be modelled by a Riemannian material manifold whose metric depends on their distribution. In this framework, we show that the natural generalization of the concept of homogeneous <span class="hlt">deformations</span> is the notion of covariantly homogeneous <span class="hlt">deformations</span> -<span class="hlt">deformations</span> with covariantly constant <span class="hlt">deformation</span> gradients. We prove that these <span class="hlt">deformations</span> are the only universal <span class="hlt">deformations</span> and that they put severe restrictions on possible universal eigenstrains . We show that, in a simply-connected body, for any distribution of universal eigenstrains the material manifold is a symmetric Riemannian manifold and that in dimensions 2 and 3 the universal eigenstrains are zero-stress.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CPL...693...66H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CPL...693...66H"><span>Tunneling and reflection in unimolecular reaction kinetic <span class="hlt">energy</span> <span class="hlt">release</span> distributions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hansen, K.</p> <p>2018-02-01</p> <p>The kinetic <span class="hlt">energy</span> <span class="hlt">release</span> distributions in unimolecular reactions is calculated with detailed balance theory, taking into account the tunneling and the reflection coefficient in three different types of transition states; (i) a saddle point corresponding to a standard RRKM-type theory, (ii) an attachment Langevin cross section, and (iii) an absorbing sphere potential at short range, without long range interactions. Corrections are significant in the one dimensional saddle point states. Very light and lightly bound absorbing systems will show measurable effects in decays from the absorbing sphere, whereas the Langevin cross section is essentially unchanged.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23899378','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23899378"><span>Reversible loss of Bernal stacking during the <span class="hlt">deformation</span> of few-layer graphene in nanocomposites.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gong, Lei; Young, Robert J; Kinloch, Ian A; Haigh, Sarah J; Warner, Jamie H; Hinks, Jonathan A; Xu, Ziwei; Li, Li; Ding, Feng; Riaz, Ibtsam; Jalil, Rashid; Novoselov, Kostya S</p> <p>2013-08-27</p> <p>The <span class="hlt">deformation</span> of nanocomposites containing graphene flakes with different numbers of layers has been investigated with the use of Raman spectroscopy. It has been found that there is a shift of the 2D band to lower wavenumber and that the rate of band shift per unit strain tends to decrease as the number of graphene layers increases. It has been demonstrated that band broadening takes place during tensile <span class="hlt">deformation</span> for mono- and bilayer graphene but that band narrowing occurs when the number of graphene layers is more than two. It is also found that the characteristic asymmetric shape of the 2D Raman band for the graphene with three or more layers changes to a symmetrical shape above about 0.4% strain and that it reverts to an asymmetric shape on unloading. This change in Raman band shape and width has been interpreted as being due to a reversible loss of Bernal stacking in the few-layer graphene during <span class="hlt">deformation</span>. It has been shown that the elastic strain <span class="hlt">energy</span> <span class="hlt">released</span> from the unloading of the inner graphene layers in the few-layer material (~0.2 meV/atom) is similar to the accepted value of the stacking fault <span class="hlt">energies</span> of graphite and few layer graphene. It is further shown that this loss of Bernal stacking can be accommodated by the formation of arrays of partial dislocations and stacking faults on the basal plane. The effect of the reversible loss of Bernal stacking upon the electronic structure of few-layer graphene and the possibility of using it to modify the electronic structure of few-layer graphene are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3789269','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3789269"><span>Reversible Loss of Bernal Stacking during the <span class="hlt">Deformation</span> of Few-Layer Graphene in Nanocomposites</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2013-01-01</p> <p>The <span class="hlt">deformation</span> of nanocomposites containing graphene flakes with different numbers of layers has been investigated with the use of Raman spectroscopy. It has been found that there is a shift of the 2D band to lower wavenumber and that the rate of band shift per unit strain tends to decrease as the number of graphene layers increases. It has been demonstrated that band broadening takes place during tensile <span class="hlt">deformation</span> for mono- and bilayer graphene but that band narrowing occurs when the number of graphene layers is more than two. It is also found that the characteristic asymmetric shape of the 2D Raman band for the graphene with three or more layers changes to a symmetrical shape above about 0.4% strain and that it reverts to an asymmetric shape on unloading. This change in Raman band shape and width has been interpreted as being due to a reversible loss of Bernal stacking in the few-layer graphene during <span class="hlt">deformation</span>. It has been shown that the elastic strain <span class="hlt">energy</span> <span class="hlt">released</span> from the unloading of the inner graphene layers in the few-layer material (∼0.2 meV/atom) is similar to the accepted value of the stacking fault <span class="hlt">energies</span> of graphite and few layer graphene. It is further shown that this loss of Bernal stacking can be accommodated by the formation of arrays of partial dislocations and stacking faults on the basal plane. The effect of the reversible loss of Bernal stacking upon the electronic structure of few-layer graphene and the possibility of using it to modify the electronic structure of few-layer graphene are discussed. PMID:23899378</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhRvC..83c4305N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhRvC..83c4305N"><span>Surface symmetry <span class="hlt">energy</span> of nuclear <span class="hlt">energy</span> density functionals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nikolov, N.; Schunck, N.; Nazarewicz, W.; Bender, M.; Pei, J.</p> <p>2011-03-01</p> <p>We study the bulk <span class="hlt">deformation</span> properties of the Skyrme nuclear <span class="hlt">energy</span> density functionals (EDFs). Following simple arguments based on the leptodermous expansion and liquid drop model, we apply the nuclear density functional theory to assess the role of the surface symmetry <span class="hlt">energy</span> in nuclei. To this end, we validate the commonly used functional parametrizations against the data on excitation <span class="hlt">energies</span> of superdeformed band heads in Hg and Pb isotopes and fission isomers in actinide nuclei. After subtracting shell effects, the results of our self-consistent calculations are consistent with macroscopic arguments and indicate that experimental data on strongly <span class="hlt">deformed</span> configurations in neutron-rich nuclei are essential for optimizing future nuclear EDFs. The resulting survey provides a useful benchmark for further theoretical improvements. Unlike in nuclei close to the stability valley, whose macroscopic <span class="hlt">deformability</span> hangs on the balance of surface and Coulomb terms, the <span class="hlt">deformability</span> of neutron-rich nuclei strongly depends on the surface symmetry <span class="hlt">energy</span>; hence, its proper determination is crucial for the stability of <span class="hlt">deformed</span> phases of the neutron-rich matter and description of fission rates for r-process nucleosynthesis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22314728-procedure-recovery-pin-pin-fields-energy-release-core-vver-type-reactor-bipr-code','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22314728-procedure-recovery-pin-pin-fields-energy-release-core-vver-type-reactor-bipr-code"><span>Procedure of recovery of pin-by-pin fields of <span class="hlt">energy</span> <span class="hlt">release</span> in the core of VVER-type reactor for the BIPR-8 code</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Gordienko, P. V., E-mail: gorpavel@vver.kiae.ru; Kotsarev, A. V.; Lizorkin, M. P.</p> <p>2014-12-15</p> <p>The procedure of recovery of pin-by-pin <span class="hlt">energy-release</span> fields for the BIPR-8 code and the algorithm of the BIPR-8 code which is used in nodal computation of the reactor core and on which the recovery of pin-by-pin fields of <span class="hlt">energy</span> <span class="hlt">release</span> is based are briefly described. The description and results of the verification using the module of recovery of pin-by-pin <span class="hlt">energy-release</span> fields and the TVS-M program are given.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70027555','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70027555"><span>Surface <span class="hlt">deformations</span> as indicators of deep ebullition fluxes in a large northern peatland</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Glaser, P.H.; Chanton, J.P.; Morin, P.; Rosenberry, D.O.; Siegel, D.I.; Ruud, O.; Chasar, L.I.; Reeve, A.S.</p> <p>2004-01-01</p> <p>Peatlands <span class="hlt">deform</span> elastically during precipitation cycles by small (??3 cm) oscillations in surface elevation. In contrast, we used a Global Positioning System network to measure larger oscillations that exceeded 20 cm over periods of 4-12 hours during two seasonal droughts at a bog and fen site in northern Minnesota. The second summer drought also triggered 19 depressuring cycles in an overpressured stratum under the bog site. The synchronicity between the largest surface <span class="hlt">deformations</span> and the depressuring cycles indicates that both phenomena are produced by the episodic <span class="hlt">release</span> of large volumes of gas from deep semi-elastic compartments confined by dense wood layers. We calculate that the three largest surface <span class="hlt">deformations</span> were associated with the <span class="hlt">release</span> of 136 g CH4 m-2, which exceeds by an order of magnitude the annual average chamber fluxes measured at this site. Ebullition of gas from the deep peat may therefore be a large and previously unrecognized source of radiocarbon depleted methane emissions from northern peatlands. Copyright 2004 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..362a2018W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..362a2018W"><span><span class="hlt">Energy</span> Evolution Mechanism and Confining Pressure Effect of Granite under Triaxial Loading-Unloading Cycles</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Hao; Miao, Sheng-jun</p> <p>2018-05-01</p> <p>Rock mass undergoes some <span class="hlt">deformational</span> failure under the action of external loads, a process known to be associated with <span class="hlt">energy</span> dissipation and <span class="hlt">release</span>. A triaxial loading-unloading cycle test was conducted on granite in order to investigate the <span class="hlt">energy</span> evolution pattern of rock mass under the action of external loads. The study results demonstrated: (1) The stress peaks increased by 50% and 22% respectively and the pre-peak weakening became more apparent in the ascending process of the confining pressure from 10MPa to 30MPa; the area enclosed by the hysteresis loop corresponding to 30MPa diminished by nearly 60% than that corresponding to 10MPa, indicating a higher confining pressure prohibits rock mass from plastic <span class="hlt">deformation</span> and shifts strain toward elastic <span class="hlt">deformation</span>. (2) In the vicinity of the strength limit, the slope of dissipation <span class="hlt">energy</span> increased to 1.6 from the original 0.7 and the dissipation <span class="hlt">energy</span> grew at an accelerating rate, demonstrating stronger propagation and convergence of internal cracks. (3) At a pressure of 70% of the stress peak, the elastic <span class="hlt">energy</span> of the granite accounted for 88% of its peak value, suggesting the rock mechanical <span class="hlt">energy</span> from the outside mostly changes into the elastic <span class="hlt">energy</span> inside the rock, with little <span class="hlt">energy</span> loss.(4) Prior to test specimen failure, the axial bearing capacity dropped with a decreasing confining pressure in an essentially linear way, and the existence of confirming pressure played a role in stabilizing the axial bearing capacity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5247530','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5247530"><span>The anelastic Ericksen problem: universal eigenstrains and <span class="hlt">deformations</span> in compressible isotropic elastic solids</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p></p> <p>2016-01-01</p> <p>The elastic Ericksen problem consists of finding <span class="hlt">deformations</span> in isotropic hyperelastic solids that can be maintained for arbitrary strain-<span class="hlt">energy</span> density functions. In the compressible case, Ericksen showed that only homogeneous <span class="hlt">deformations</span> are possible. Here, we solve the anelastic version of the same problem, that is, we determine both the <span class="hlt">deformations</span> and the eigenstrains such that a solution to the anelastic problem exists for arbitrary strain-<span class="hlt">energy</span> density functions. Anelasticity is described by finite eigenstrains. In a nonlinear solid, these eigenstrains can be modelled by a Riemannian material manifold whose metric depends on their distribution. In this framework, we show that the natural generalization of the concept of homogeneous <span class="hlt">deformations</span> is the notion of covariantly homogeneous deformations—<span class="hlt">deformations</span> with covariantly constant <span class="hlt">deformation</span> gradients. We prove that these <span class="hlt">deformations</span> are the only universal <span class="hlt">deformations</span> and that they put severe restrictions on possible universal eigenstrains. We show that, in a simply-connected body, for any distribution of universal eigenstrains the material manifold is a symmetric Riemannian manifold and that in dimensions 2 and 3 the universal eigenstrains are zero-stress. PMID:28119554</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25615343','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25615343"><span>Fluctuations of global <span class="hlt">energy</span> <span class="hlt">release</span> and crackling in nominally brittle heterogeneous fracture.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barés, J; Hattali, M L; Dalmas, D; Bonamy, D</p> <p>2014-12-31</p> <p>The temporal evolution of mechanical <span class="hlt">energy</span> and spatially averaged crack speed are both monitored in slowly fracturing artificial rocks. Both signals display an irregular burstlike dynamics, with power-law distributed fluctuations spanning a broad range of scales. Yet, the elastic power <span class="hlt">released</span> at each time step is proportional to the global velocity all along the process, which enables defining a material-constant fracture <span class="hlt">energy</span>. We characterize the intermittent dynamics by computing the burst statistics. This latter displays the scale-free features signature of crackling dynamics, in qualitative but not quantitative agreement with the depinning interface models derived for fracture problems. The possible sources of discrepancies are pointed out and discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27802110','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27802110"><span>Base <span class="hlt">Release</span> and Modification in Solid-Phase DNA Exposed to Low-<span class="hlt">Energy</span> Electrons.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Choofong, Surakarn; Cloutier, Pierre; Sanche, Léon; Wagner, J Richard</p> <p>2016-11-01</p> <p>Ionization generates a large number of secondary low-<span class="hlt">energy</span> electrons (LEEs) with a most probable <span class="hlt">energy</span> of approximately 10 eV, which can break DNA bonds by dissociative electron attachment (DEA) and lead to DNA damage. In this study, we investigated radiation damage to dry DNA induced by X rays (1.5 keV) alone on a glass substrate or X rays combined with extra LEEs (average <span class="hlt">energy</span> of 5.8 eV) emitted from a tantalum (Ta) substrate under an atmosphere of N 2 and standard ambient conditions of temperature and pressure. The targets included calf-thymus DNA and double-stranded synthetic oligonucleotides. We developed analytical methods to measure the <span class="hlt">release</span> of non-modified DNA bases from DNA and the formation of several base modifications by LC-MS/MS with isotopic dilution for precise quantification. The results show that the yield of non-modified bases as well as base modifications increase by 20-30% when DNA is deposited on a Ta substrate compared to that on a glass substrate. The order of base <span class="hlt">release</span> (Gua > Ade > Thy ∼ Cyt) agrees well with several theoretical studies indicating that Gua is the most susceptible site toward sugar-phosphate cleavage. The formation of DNA damage by LEEs is explained by DEA leading to the <span class="hlt">release</span> of non-modified bases involving the initial cleavage of N1-C1', C3'-O3' or C5'-O5' bonds. The yield of base modifications was lower than the <span class="hlt">release</span> of non-modified bases. The main LEE-induced base modifications include 5,6-dihydrothymine (5,6-dHT), 5,6-dihydrouracil (5-dHU), 5-hydroxymethyluracil (5-HmU) and 5-formyluracil (5-ForU). The formation of base modifications by LEEs can be explained by DEA and cleavage of the C-H bond of the methyl group of Thy (giving 5-HmU and 5-ForU) and by secondary reactions of H atoms and hydride anions that are generated by primary LEE reactions followed by subsequent reaction with Cyt and Thy (giving 5,6-dHU and 5,6-dHT).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790006995','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790006995"><span>Application of the relative <span class="hlt">energy</span> <span class="hlt">release</span> criteria to enclosure fire testing. [aircraft compartments</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Roschke, E. J.; Coulbert, C. D.</p> <p>1979-01-01</p> <p>The five relative <span class="hlt">energy</span> <span class="hlt">release</span> criteria (RERC) which are a first step towards formulating a unified concept that can be applied to the development of fires in enclosures, place upper bounds on the rate and amount of <span class="hlt">energy</span> <span class="hlt">released</span> during a fire. They are independent, calculated readily, and may be applied generally to any enclosure regardless of size. They are useful in pretest planning and for interpreting experimental data. Data from several specific fire test programs were examined to evaluate the potential use of RERC to provide test planning guidelines. The RERC were compared with experimental data obtained in full-scale enclosures. These results confirm that in general the RERC do identify the proper limiting constraints on enclosure fire development and determine the bounds of the fire development envelope. Plotting actual fire data against the RERC reveals new valid insights into fire behavior and reveals the controlling constraints in fire development. The RERC were calculated and plotted for several descrpitions of full-scale fires in various aircraft compartments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70017342','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70017342"><span>Block versus continuum <span class="hlt">deformation</span> in the Western United States</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>King, G.; Oppenheimer, D.; Amelung, F.</p> <p>1994-01-01</p> <p>The relative role of block versus continuum <span class="hlt">deformation</span> of continental lithosphere is a current subject of debate. Continuous <span class="hlt">deformation</span> is suggested by distributed seismicity at continental plate margins and by cumulative seismic moment sums which yield slip estimates that are less than estimates from plate motion studies. In contrast, block models are favored by geologic studies of displacement in places like Asia. A problem in this debate is a lack of data from which unequivocal conclusions may be reached. In this paper we apply the techniques of study used in regions such as the Alpine-Himalayan belt to an area with a wealth of instrumental data-the Western United States. By comparing plate rates to seismic moment <span class="hlt">release</span> rates and assuming a typical seismogenic layer thickness of 15 km it appears that since 1850 about 60% of the Pacific-North America motion across the plate boundary in California and Nevada has occurred seismically and 40% aseismically. The San Francisco Bay area shows similar partitioning between seismic and aseismic <span class="hlt">deformation</span>, and it can be shown that within the seismogenic depth range aseismic <span class="hlt">deformation</span> is concentrated near the surface and at depth. In some cases this <span class="hlt">deformation</span> can be located on creeping surface faults, but elsewhere it is spread over a several kilometer wide zone adjacent to the fault. These superficial creeping <span class="hlt">deformation</span> zones may be responsible for the palaeomagnetic rotations that have been ascribed elsewhere to the surface expression of continuum <span class="hlt">deformation</span> in the lithosphere. Our results support the dominant role of non-continuum <span class="hlt">deformation</span> processes with the implication that <span class="hlt">deformation</span> localization by strain softening must occur in the lower crust and probably the upper mantle. Our conclusions apply only to the regions where the data are good, and even within the Western United States (i.e., the Basin and Range) <span class="hlt">deformation</span> styles remain poorly resolved. Nonetheless, we maintain that block motion is the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017IAUS..327...94D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017IAUS..327...94D"><span>Understanding the connection between the <span class="hlt">energy</span> <span class="hlt">released</span> during solar flares and their emission in the lower atmosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>da Costa, F. Rubio</p> <p>2017-10-01</p> <p>While progress has been made on understanding how <span class="hlt">energy</span> is <span class="hlt">released</span> and deposited along the solar atmosphere during explosive events such as solar flares, the chromospheric and coronal heating through the sudden <span class="hlt">release</span> of magnetic <span class="hlt">energy</span> remain an open problem in solar physics. Recent hydrodynamic models allow to investigate the <span class="hlt">energy</span> deposition along a flare loop and to study the response of the chromosphere. These results have been improved with the consideration of transport and acceleration of particles along the loop. RHESSI and Fermi/GBM X-ray and gamma-ray observations help to constrain the spectral properties of the injected electrons. The excellent spatial, spectral and temporal resolution of IRIS will also help us to constrain properties of explosive events, such as the continuum emission during flares or their emission in the chromosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CPM.....4..487B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CPM.....4..487B"><span>Modeling plasticity by non-continuous <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ben-Shmuel, Yaron; Altus, Eli</p> <p>2017-10-01</p> <p>Plasticity and failure theories are still subjects of intense research. Engineering constitutive models on the macroscale which are based on micro characteristics are very much in need. This study is motivated by the observation that continuum assumptions in plasticity in which neighbour material elements are inseparable at all-time are physically impossible, since local detachments, slips and neighbour switching must operate, i.e. non-continuous <span class="hlt">deformation</span>. Material microstructure is modelled herein by a set of point elements (particles) interacting with their neighbours. Each particle can detach from and/or attach with its neighbours during <span class="hlt">deformation</span>. Simulations on two- dimensional configurations subjected to uniaxial compression cycle are conducted. Stochastic heterogeneity is controlled by a single "disorder" parameter. It was found that (a) macro response resembles typical elasto-plastic behaviour; (b) plastic <span class="hlt">energy</span> is proportional to the number of detachments; (c) residual plastic strain is proportional to the number of attachments, and (d) volume is preserved, which is consistent with macro plastic <span class="hlt">deformation</span>. Rigid body displacements of local groups of elements are also observed. Higher disorder decreases the macro elastic moduli and increases plastic <span class="hlt">energy</span>. Evolution of anisotropic effects is obtained with no additional parameters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PAN....80.1683K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PAN....80.1683K"><span>Computer Simulation of Compression and <span class="hlt">Energy</span> <span class="hlt">Release</span> upon Laser Irradiation of Cylindrically Symmetric Target</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuzenov, V. V.</p> <p>2017-12-01</p> <p>The paper is devoted to the theoretical and computational study of compression and <span class="hlt">energy</span> <span class="hlt">release</span> for magneto-inertial plasma confinement. This approach makes it possible to create new high-density plasma sources, apply them in materials science experiments, and use them in promising areas of power engineering.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMED51A0870Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMED51A0870Z"><span>Developing a Virtual Rock <span class="hlt">Deformation</span> Laboratory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, W.; Ougier-simonin, A.; Lisabeth, H. P.; Banker, J. S.</p> <p>2012-12-01</p> <p>Experimental rock physics plays an important role in advancing earthquake research. Despite its importance in geophysics, reservoir engineering, waste deposits and <span class="hlt">energy</span> resources, most geology departments in U.S. universities don't have rock <span class="hlt">deformation</span> facilities. A virtual <span class="hlt">deformation</span> laboratory can serve as an efficient tool to help geology students naturally and internationally learn about rock <span class="hlt">deformation</span>. Working with computer science engineers, we built a virtual <span class="hlt">deformation</span> laboratory that aims at fostering user interaction to facilitate classroom and outreach teaching and learning. The virtual lab is built to center around a triaxial <span class="hlt">deformation</span> apparatus in which laboratory measurements of mechanical and transport properties such as stress, axial and radial strains, acoustic emission activities, wave velocities, and permeability are demonstrated. A student user can create her avatar to enter the virtual lab. In the virtual lab, the avatar can browse and choose among various rock samples, determine the testing conditions (pressure, temperature, strain rate, loading paths), then operate the virtual <span class="hlt">deformation</span> machine to observe how <span class="hlt">deformation</span> changes physical properties of rocks. Actual experimental results on the mechanical, frictional, sonic, acoustic and transport properties of different rocks at different conditions are compiled. The data acquisition system in the virtual lab is linked to the complied experimental data. Structural and microstructural images of <span class="hlt">deformed</span> rocks are up-loaded and linked to different <span class="hlt">deformation</span> tests. The integration of the microstructural image and the <span class="hlt">deformation</span> data allows the student to visualize how forces reshape the structure of the rock and change the physical properties. The virtual lab is built using the Game Engine. The geological background, outstanding questions related to the geological environment, and physical and mechanical concepts associated with the problem will be illustrated on the web portal. In</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DFDL14004M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DFDL14004M"><span>Self-sustained oscillations of a sinusoidally-<span class="hlt">deformed</span> plate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Muriel, Diego F.; Cowen, Edwin A.</p> <p>2015-11-01</p> <p>Motivated by <span class="hlt">energy</span> harvesting, the oscillatory motion of a <span class="hlt">deformed</span> elastic material with aspect ratio Length/Width=2, immerse in an incompressible flow is studied experimentally. To induce the wave-like <span class="hlt">deformation</span> a polycarbonate sheet is placed under longitudinal compression with external forcing provided by equispaced tension lines anchored in a frame. No additional constrains are placed in the material. Based on quantitative image-based edge detection, ADV, and PIV measurements, we document the existence of three natural states of motion. Bellow a critical velocity, a stable state presents a sinusoidal-like <span class="hlt">deformation</span> with weak small perturbations. Above a critical velocity, instability appears in the form of a traveling wave with predictable dominant frequency accompanied by higher-order harmonics. As the flow velocity increases the instability converges faster to its limit cycle in the phase plane (e.g., vertical velocity and position), until the stable oscillatory mode transitions to chaos showing a broad <span class="hlt">energy</span> spectrum and unstable limit cycle. The underlying objective is to induce the onset of the instability at lower critical velocities for higher bending rigidities, promoting possible <span class="hlt">energy</span> extraction and increasing the range at which stable oscillations appear.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016CPM.....3...69M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016CPM.....3...69M"><span>Plastic <span class="hlt">deformation</span> in a metallic granular chain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Musson, Ryan W.; Carlson, William</p> <p>2016-03-01</p> <p>Solitary wave response was investigated in a metallic granular chain-piston system using LS-DYNA. A power law hardening material model was used to show that localized plastic <span class="hlt">deformation</span> is present in a metallic granular chain for an impact velocity of 0.5 m/s. This loss due to plastic <span class="hlt">deformation</span> was quantified via impulse, and it was shown that the loss scales nearly linearly with impact velocity. Therefore, metallic grains may not be suitable for devices that require high-amplitude solitary waves. There would be too much <span class="hlt">energy</span> lost to plastic <span class="hlt">deformation</span>. One can assume that ceramics will behave elastically; therefore, the response of an aluminum oxide granular chain was compared to that of a steel chain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhL.109y3102C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhL.109y3102C"><span>Nanoscale <span class="hlt">deformations</span> in graphene by laser annealing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Coleman, Christopher; Erasmus, Rudolph; Bhattacharyya, Somnath</p> <p>2016-12-01</p> <p>We investigate a method of inducing nano to micron scale strained regions in graphene using a laser treatment monitored by Raman spectroscopy. The Raman G-peak of the strained region shows a splitting and redshift for graphene exposed to a laser power density above a certain threshold limit (20 mW). We also note blue-shifting of the positions of both Raman D and 2D-peaks and the decrease of both their intensities relative to the G-peak with increasing laser power. These features correspond to p-type doping effects that are believed to be caused by gas adsorbates <span class="hlt">released</span> from the substrate during the laser treatment. The induced strain is verified by AFM analysis, which shows the blister-like <span class="hlt">deformations</span> of the treated area and the corresponding strength of the induced gauge fields in the <span class="hlt">deformed</span> region. We find that, depending on the exact size and geometry of the blisters, the gauge fields can range between 0.4 mT and 300 T. This laser treatment procedure establishes an effective method for the local <span class="hlt">deformation</span> and doping of graphene, which may be useful for strain engineering in device fabrication.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23323731','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23323731"><span>Tapping-mode AFM study of tip-induced polymer <span class="hlt">deformation</span> under geometrical confinement.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Hong; Honda, Yukio; Takeoka, Shinji</p> <p>2013-02-05</p> <p>The morphological stability of polymer films is critically important to their application as functional materials. The <span class="hlt">deformation</span> of polymer surfaces on the nanoscale may be significantly influenced by geometrical confinement. Herein, we constructed a mechanically heterogeneous polymer surface by phase separation in a thin polymer film and investigated the <span class="hlt">deformation</span> behavior of its nanostructure (∼30 nm thickness and ∼100 nm average diameter) with tapping-mode atomic force microscopy. By changing different scan parameters, we could induce <span class="hlt">deformation</span> localized to the nanostructure in a controllable manner. A quantity called the <span class="hlt">deformation</span> index is defined and shown to be correlated to <span class="hlt">energy</span> dissipation by tip-sample interaction. We clarified that the plastic <span class="hlt">deformation</span> of a polymer on the nanoscale is <span class="hlt">energy</span>-dependent and is related to the glass-to-rubber transition. The mobility of polymer chains beneath the tapping tip is enhanced, and in the corresponding region a rubberlike <span class="hlt">deformation</span> with the lateral motion of the tip is performed. The method we developed can provide insight into the geometrical confinement effects on polymer behavior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JMPSo.116..290C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JMPSo.116..290C"><span>Isometric <span class="hlt">deformations</span> of unstretchable material surfaces, a spatial variational treatment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Yi-Chao; Fosdick, Roger; Fried, Eliot</p> <p>2018-07-01</p> <p>The stored <span class="hlt">energy</span> of an unstretchable material surface is assumed to depend only upon the curvature tensor. By control of its edge(s), the surface is <span class="hlt">deformed</span> isometrically from its planar undistorted reference configuration into an equilibrium shape. That shape is to be determined from a suitably constrained variational problem as a state of relative minimal potential <span class="hlt">energy</span>. We pose the variational problem as one of relative minimum potential <span class="hlt">energy</span> in a spatial form, wherein the <span class="hlt">deformation</span> of a flat, undistorted region D in E2 to its distorted form S in E3 is assumed specified. We then apply the principle that the first variation of the potential <span class="hlt">energy</span>, expressed as a functional over S ∪ ∂S , must vanish for all admissible variations that correspond to isometric <span class="hlt">deformations</span> from the distorted configuration S and that also contain the essence of flatness that characterizes the reference configuration D , but is not covered by the single statement that the variation of S correspond to an isometric <span class="hlt">deformation</span>. We emphasize the commonly overlooked condition that the spatial expression of the variational problem requires an additional variational constraint of zero Gaussian curvature to ensure that variations from S that are isometric <span class="hlt">deformations</span> also contain the notion of flatness. In this context, it is particularly revealing to observe that the two constraints produce distinct, but essential and complementary, conditions on the first variation of S. The resulting first variation integral condition, together with the constraints, may be applied, for example, to the case of a flat, undistorted, rectangular strip D that is <span class="hlt">deformed</span> isometrically into a closed ring S by connecting its short edges and specifying that its long edges are free of loading and, therefore, subject to zero traction and couple traction. The elementary example of a closed ring without twist as a state of relative minimum potential <span class="hlt">energy</span> is discussed in detail, and the bending of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1226128','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1226128"><span>Fission Fragment Mass Distributions and Total Kinetic <span class="hlt">Energy</span> <span class="hlt">Release</span> of 235-Uranium and 238-Uranium in Neutron-Induced Fission at Intermediate and Fast Neutron <span class="hlt">Energies</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Duke, Dana Lynn</p> <p>2015-11-12</p> <p>This Ph.D. dissertation describes a measurement of the change in mass distributions and average total kinetic <span class="hlt">energy</span> (TKE) <span class="hlt">release</span> with increasing incident neutron <span class="hlt">energy</span> for fission of 235U and 238U. Although fission was discovered over seventy-five years ago, open questions remain about the physics of the fission process. The <span class="hlt">energy</span> of the incident neutron, En, changes the division of <span class="hlt">energy</span> <span class="hlt">release</span> in the resulting fission fragments, however, the details of <span class="hlt">energy</span> partitioning remain ambiguous because the nucleus is a many-body quantum system. Creating a full theoretical model is difficult and experimental data to validate existing models are lacking. Additional fissionmore » measurements will lead to higher-quality models of the fission process, therefore improving applications such as the development of next-generation nuclear reactors and defense. This work also paves the way for precision experiments such as the Time Projection Chamber (TPC) for fission cross section measurements and the Spectrometer for Ion Determination in Fission (SPIDER) for precision mass yields.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25313463','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25313463"><span>Radiation <span class="hlt">release</span> at the nation's only operating deep geological repository--an independent monitoring perspective.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Thakur, P; Ballard, S; Hardy, R</p> <p>2014-11-04</p> <p>Recent incidents at the nation's only operating deep geologic nuclear waste repository, the Waste Isolation Pilot Plant (WIPP), resulted in the <span class="hlt">release</span> of americium and plutonium from one or more defense-related transuranic (TRU) waste containers into the environment. WIPP is a U.S. Department of <span class="hlt">Energy</span> mined geologic repository that has been in operation since March, 1999. Over 85,000 m3 of waste in various vented payload containers have been emplaced in the repository. The primary radionuclides within the disposed waste are 239+240Pu and 241Am, which account for more than 99% of the total TRU radioactivity disposed and scheduled for disposal in the repository. For the first time in its 15 years of operation, there was an airborne radiation <span class="hlt">release</span> from the WIPP at approximately 11:30 PM Mountain Standard Time (MST) on Friday, February 14, 2014. The radiation <span class="hlt">release</span> was likely caused by a chemical reaction inside a TRU waste drum that contained nitrate salts and organic sorbent materials. In a recent news <span class="hlt">release</span>, DOE announced that photos taken of the waste underground showed evidence of heat and gas pressure resulting in a <span class="hlt">deformed</span> lid, in material expelled through that <span class="hlt">deformation</span>, and in melted plastic and rubber and polyethylene in the vicinity of that drum. Recent entries into underground Panel 7 have confirmed that at least one waste drum containing a nitrate salt bearing waste stream from Los Alamos National Laboratory was breached underground and was the most likely source of the <span class="hlt">release</span>. Further investigation is underway to determine if other containers contributed to the <span class="hlt">release</span>. Air monitoring across the WIPP site intensified following the first reports of radiation detection underground to ascertain whether or not there were <span class="hlt">releases</span> to the ground surface. Independent analytical results of air filters from sampling stations on and near the WIPP facility have been <span class="hlt">released</span> by us at the Carlsbad Environmental Monitoring & Research Center and confirmed</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AIPC..955..885Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AIPC..955..885Z"><span>Post-Detonation <span class="hlt">Energy</span> <span class="hlt">Release</span> from Tnt-Aluminum Explosives</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Fan; Anderson, John; Yoshinaka, Akio</p> <p>2007-12-01</p> <p>TNT and TNT-aluminum composites were experimentally studied in an air-filled 26 m3 chamber for charge masses ranging from 1.1 to 4 kg. Large aluminum mass fractions (35 to 50%wt.) and particle sizes (36 μm) were combined with TNT in two configurations, whereby the aluminum particles were uniformly mixed in cast TNT or arranged into a shell surrounding a cast TNT cylinder. The results show that improved performance is achieved for the shell configuration versus the mixed version during the early afterburning phase (10-40 ms), while both approach the same quasi-static explosion overpressure (QSP) after a long duration. The QSP ratios with respect to TNT in nitrogen are in good agreement with equilibrium predictions. Thus, the large aluminum mass fraction improves spatial mixing of hot fuels with oxidizing gases in the detonation products and chamber air, resulting in more efficient afterburning <span class="hlt">energy</span> <span class="hlt">release</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890038958&hterms=end+theory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DThe%2Bend%2Btheory','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890038958&hterms=end+theory&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DThe%2Bend%2Btheory"><span>Strain <span class="hlt">energy</span> <span class="hlt">release</span> rate analysis of the end-notched flexure specimen using the finite-element method</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Salpekar, S. A.; Raju, I. S.; O'Brien, T. K.</p> <p>1988-01-01</p> <p>Two-dimensional finite-element analysis of the end-notched flexure specimen was performed using 8-node isoparametric, parabolic elements to evaluate compliance and mode II strain <span class="hlt">energy</span> <span class="hlt">release</span> rates, G sub II. The G sub II values were computed using two different techniques: the virtual crack-closure technique (VCCT) and the rate of change of compliance with crack length (compliance derivative method). The analysis was performed for various crack-length-to-semi-span (a/L) ratios ranging from 0.2 to 0.9. Three material systems representing a wide range of material properties were analyzed. The compliance and strain <span class="hlt">energy</span> <span class="hlt">release</span> rates of the specimen calculated with the present finite-element analysis agree very well with beam theory equations including transverse shear. The G sub II values calculated using the compliance derivative method compared extremely well with those calculated using the VCCT. The G sub II values obtained by the compliance derivative method using the top or bottom beam deflections agreed closely with each other. The strain <span class="hlt">energy</span> <span class="hlt">release</span> rates from a plane-stress analysis were higher than the plane-strain values by only a small percentage, indicating that either assumption may be used in the analysis. The G sub II values for one material system calculated from the finte-element analysis agreed with one solution in the literature and disagreed with the other solution in the literature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880004353','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880004353"><span>Strain-<span class="hlt">energy-release</span> rate analysis of the end-notched flexure specimen using the finite-element method</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Salpekar, S. A.; Raju, I. S.; Obrien, T. K.</p> <p>1987-01-01</p> <p>Two-dimensional finite-element analysis of the end-notched flexure specimen was performed using 8-node isoparametric, parabolic elements to evaluate compliance and mode II strain <span class="hlt">energy</span> <span class="hlt">release</span> rates, G sub II. The G sub II values were computed using two different techniques: the virtural crack-closure technique (VCCT) and the rate of change of compliance with crack length (compliance derivative method). The analysis was performed for various crack-length-to-semi-span (a/L) ratios ranging from 0.2 to 0.9. Three material systems representing a wide range of material properties were analyzed. The compliance and strain <span class="hlt">energy</span> <span class="hlt">release</span> rates of the specimen calculated with the present finite-element analysis agree very well with beam theory equations including transverse shear. The G sub II values calculated using the compliance derivative method compared extremely well with those calculated using the VCCT. The G sub II values obtained by the compliance derivative method using the top or bottom beam deflections agreed closely with each other. The strain <span class="hlt">energy</span> <span class="hlt">release</span> rates from a plane-stress analysis were higher than the plane-strain values by only a small percentage, indicating that either assumption may be used in the analysis. The G sub II values for one material system calculated from the finite-element analysis agreed with one solution in the literature and disagreed with the other solution in the literature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/32776','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/32776"><span>Relationships between <span class="hlt">energy</span> <span class="hlt">release</span>, fuel mass loss, and trace gas and aerosol emissions during laboratory biomass fires</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Patrick H. Freeborn; Martin J. Wooster; Wei Min Hao; Cecily A. Nordgren Ryan; Stephen P. Baker; Charles Ichoku</p> <p>2008-01-01</p> <p>Forty-four small-scale experimental fires were conducted in a combustion chamber to examine the relationship between biomass consumption, smoke production, convective <span class="hlt">energy</span> <span class="hlt">release</span>, and middle infrared (MIR) measurements of fire radiative <span class="hlt">energy</span> (FRE). Fuel bed weights, trace gas and aerosol particle concentrations, stack flow rate and temperature, and concurrent...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPA....8c5013J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPA....8c5013J"><span>The effect of explosive percentage on underwater explosion <span class="hlt">energy</span> <span class="hlt">release</span> of hexanitrohexaazaisowurtzitane and octogen based aluminized explosives</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiao, Qingjie; Wang, Qiushi; Nie, Jianxin; Guo, Xueyong; Zhang, Wei; Fan, Wenqi</p> <p>2018-03-01</p> <p>To control the explosion <span class="hlt">energy</span> output by optimizing explosive components is a key requirement in a number of different application areas. The effect of different Al/O Ratio on underwater explosion of aluminized explosives has been studied detailedly. However, the effect of explosive percentage in the same Al/O Ratio is rarely researched, especially for Hexanitrohexaazaisowurtzitane (CL-20) based aluminized explosives. In this study, we performed the underwater explosion experiments with 1.2-kilogram explosives in order to investigate the explosion <span class="hlt">energy</span> <span class="hlt">released</span> from CL-20 and Octogen (HMX) based aluminized explosives. The percentage of the explosive varied from 5% to 30% and it is shown that: the shockwave peak pressure (pm) grows gradually; shock wave <span class="hlt">energy</span> (Es) continues increasing, bubble <span class="hlt">energy</span> (Eb) increases then decreases peaking at 15% for both formulas, and the total <span class="hlt">energy</span> (E) and <span class="hlt">energy</span> <span class="hlt">release</span> rate (η) peak at 20% for CL-20 and 15% for HMX. This paper outlines the physical mechanism of Eb change under the influence of an aluminium initial reaction temperature and reaction active detonation product percentage coupling. The result shows that CL-20 is superior as a new high explosive and has promising application prospects in the regulation of explosive <span class="hlt">energy</span> output for underwater explosives.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860023437','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860023437"><span>Viscoelastic <span class="hlt">deformation</span> near active plate boundaries</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ward, S. N.</p> <p>1986-01-01</p> <p>Model <span class="hlt">deformations</span> near the active plate boundaries of Western North America using space-based geodetic measurements as constraints are discussed. The first six months of this project were spent gaining familarity with space-based measurements, accessing the Crustal Dynamics Data Information Computer, and building time independent <span class="hlt">deformation</span> models. The initial goal was to see how well the simplest elastic models can reproduce very long base interferometry (VLBI) baseline data. From the Crustal Dynamics Data Information Service, a total of 18 VLBI baselines are available which have been surveyed on four or more occasions. These data were fed into weighted and unweighted inversions to obtain baseline closure rates. Four of the better quality lines are illustrated. The <span class="hlt">deformation</span> model assumes that the observed baseline rates result from a combination of rigid plate tectonic motions plus a component resulting from elastic strain build up due to a failure of the plate boundary to slip at the full plate tectonic rate. The elastic <span class="hlt">deformation</span> resulting from the locked plate boundary is meant to portray interseismic strain accumulation. During and shortly after a large interplate earthquake, these strains are largely <span class="hlt">released</span>, and points near the fault which were previously retarded suddenly catch up to the positions predicted by rigid plate models. Researchers judge the quality of fit by the sum squares of weighted residuals, termed total variance. The observed baseline closures have a total variance of 99 (cm/y)squared. When the RM2 velocities are assumed to model the data, the total variance increases to 154 (cm/y)squared.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15259957','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15259957"><span>Sludge thermal oxidation processes: mineral recycling, <span class="hlt">energy</span> impact, and greenhouse effect gases <span class="hlt">release</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Guibelin, E</p> <p>2004-01-01</p> <p>Different treatment routes have been studied for a mixed sludge: the conventional agricultural use is compared with the thermal oxidation processes, including incineration (in gaseous phase) and wet air oxidation (in liquid phase). The interest of a sludge digestion prior to the final treatment has been also considered according to the two major criteria, which are the fossil <span class="hlt">energy</span> utilisation and the greenhouse effect gases (CO2, CH4, N2O) <span class="hlt">release</span>. Thermal <span class="hlt">energy</span> has to be recovered on thermal processes to make these processes environmentally friendly, otherwise their main interest is to extract or destroy micropollutants and pathogens from the carbon cycle. In case of continuous <span class="hlt">energy</span> recovery, incineration can produce more <span class="hlt">energy</span> than it consumes. Digestion is especially interesting for agriculture: according to these two schemes, the <span class="hlt">energy</span> final balance can also be in excess. As to wet air oxidation, it is probably one of the best ways to minimize greenhouse effect gases emission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22612719-deformation-properties-lead-isotopes','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22612719-deformation-properties-lead-isotopes"><span><span class="hlt">Deformation</span> properties of lead isotopes</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tolokonnikov, S. V.; Borzov, I. N.; Lutostansky, Yu. S.</p> <p>2016-01-15</p> <p>The <span class="hlt">deformation</span> properties of a long lead isotopic chain up to the neutron drip line are analyzed on the basis of the <span class="hlt">energy</span> density functional (EDF) in the FaNDF{sup 0} Fayans form. The question of whether the ground state of neutron-deficient lead isotopes can have a stable <span class="hlt">deformation</span> is studied in detail. The prediction of this <span class="hlt">deformation</span> is contained in the results obtained on the basis of the HFB-17 and HFB-27 Skyrme EDF versions and reported on Internet. The present analysis reveals that this is at odds with experimental data on charge radii and magnetic moments of odd lead isotopes.more » The Fayans EDF version predicts a spherical ground state for all light lead isotopes, but some of them (for example, {sup 180}Pb and {sup 184}Pb) prove to be very soft—that is, close to the point of a phase transition to a <span class="hlt">deformed</span> state. Also, the results obtained in our present study are compared with the predictions of some other Skyrme EDF versions, including SKM*, SLy4, SLy6, and UNE1. By and large, their predictions are closer to the results arising upon the application of the Fayans functional. For example, the SLy4 functional predicts, in just the same way as the FaNDF{sup 0} functional, a spherical shape for all nuclei of this region. The remaining three Skyrme EDF versions lead to a <span class="hlt">deformation</span> of some light lead isotopes, but their number is substantially smaller than that in the case of the HFB-17 and HFB-27 functionals. Moreover, the respective <span class="hlt">deformation</span> <span class="hlt">energy</span> is substantially lower, which gives grounds to hope for the restoration of a spherical shape upon going beyond the mean-field approximation, which we use here. Also, the <span class="hlt">deformation</span> properties of neutron-rich lead isotopes are studied up to the neutron drip line. Here, the results obtained with the FaNDF{sup 0} functional are compared with the predictions of the HFB-17, HFB-27, SKM*, and SLy4 Skyrme EDF versions. All of the EDF versions considered here predict the existence of a region where</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000SPIE.3979..458M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000SPIE.3979..458M"><span>3D <span class="hlt">deformable</span> image matching: a hierarchical approach over nested subspaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Musse, Olivier; Heitz, Fabrice; Armspach, Jean-Paul</p> <p>2000-06-01</p> <p>This paper presents a fast hierarchical method to perform dense <span class="hlt">deformable</span> inter-subject matching of 3D MR Images of the brain. To recover the complex morphological variations in neuroanatomy, a hierarchy of 3D <span class="hlt">deformations</span> fields is estimated, by minimizing a global <span class="hlt">energy</span> function over a sequence of nested subspaces. The nested subspaces, generated from a single scaling function, consist of <span class="hlt">deformation</span> fields constrained at different scales. The highly non linear <span class="hlt">energy</span> function, describing the interactions between the target and the source images, is minimized using a coarse-to-fine continuation strategy over this hierarchy. The resulting <span class="hlt">deformable</span> matching method shows low sensitivity to local minima and is able to track large non-linear <span class="hlt">deformations</span>, with moderate computational load. The performances of the approach are assessed both on simulated 3D transformations and on a real data base of 3D brain MR Images from different individuals. The method has shown efficient in putting into correspondence the principle anatomical structures of the brain. An application to atlas-based MRI segmentation, by transporting a labeled segmentation map on patient data, is also presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22340374-microstructure-characterization-based-type-deformed-grains-cold-rolled-cu-added-bake-hardenable-steel','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22340374-microstructure-characterization-based-type-deformed-grains-cold-rolled-cu-added-bake-hardenable-steel"><span>Microstructure characterization based on the type of <span class="hlt">deformed</span> grains in cold-rolled, Cu-added, bake-hardenable steel</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kim, J.S.; Kim, S.I.; Choi, S.-H., E-mail: shihoon@sunchon.ac.kr</p> <p>2014-06-01</p> <p>The electron backscatter diffraction technique has been used to characterize the microstructure of <span class="hlt">deformed</span> grains in cold-rolled, Cu-added, bake-hardenable steel. A new scheme based on the kind and number of average orientations, as determined from a unique grain map of the <span class="hlt">deformed</span> grains, was developed in order to classify <span class="hlt">deformed</span> grains by type. The α-fiber components, γ-fiber components and random orientations, those which could not be assigned to either γ-fiber or α-fiber components, were used to define the average orientation of unique grains within individual <span class="hlt">deformed</span> grains. The microstructures of <span class="hlt">deformed</span> grains in as-rolled specimens were analyzed based on themore » Taylor factor, stored <span class="hlt">energy</span>, and misorientation. The relative levels and distributions of the Taylor factor, the stored <span class="hlt">energy</span> and the misorientation were examined in terms of the types of <span class="hlt">deformed</span> grains. - Highlights: • We characterized the microstructure of Cu-added BH steel using EBSD. • A new scheme was developed in order to classify <span class="hlt">deformed</span> grains by type. • Stored <span class="hlt">energy</span> and misorientation are strongly dependent on the type of <span class="hlt">deformed</span> grains. • Microstructure was examined in terms of the types of <span class="hlt">deformed</span> grains.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20150010747&hterms=corona&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dcorona','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20150010747&hterms=corona&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dcorona"><span>Spatiotemporal Organization of <span class="hlt">Energy</span> <span class="hlt">Release</span> Events in the Quiet Solar Corona</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Uritsky, Vadim M.; Davila, Joseph M.</p> <p>2014-01-01</p> <p>Using data from the STEREO and SOHO spacecraft, we show that temporal organization of <span class="hlt">energy</span> <span class="hlt">release</span> events in the quiet solar corona is close to random, in contrast to the clustered behavior of flaring times in solar active regions. The locations of the quiet-Sun events follow the meso- and supergranulation pattern of the underling photosphere. Together with earlier reports of the scale-free event size statistics, our findings suggest that quiet solar regions responsible for bulk coronal heating operate in a driven self-organized critical state, possibly involving long-range Alfvenic interactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AIPC.1233...65G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AIPC.1233...65G"><span>Damage Analysis of Tensile <span class="hlt">Deformation</span> of Co-rolled SMATed 304SS</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, X.; Leung, A. Y. T.; Chen, A.; Ruan, H.; Lu, J.</p> <p>2010-05-01</p> <p>One of recent experimental progresses in strengthening and toughening metals simultaneously is to adopt techniques of surface mechanical attrition treatment (SMAT) and warm co-rolling to 304 stainless steel (SS). To capture <span class="hlt">deformation</span> behavior and associated damage initiation/evolution process in the co-rolled SMATed 304SS, cohesive finite element method (CFEM) is employed in this paper and simulation results are in agreement with experimental results. Both strengthening effect due to high yield stress of the nanograin layer and toughening effect due to non-localized damage in the nanograin layer are captured. Effect of <span class="hlt">energy</span> <span class="hlt">release</span> rate of nanograin layer on failure strain of layered co-rolled SMATed 304SS is investigated. It is found that the more brittle the nanograin layer is, the more potential necking sites in the nanograin layer are, and the more ductile the layered co-rolled SMATed 304SS is.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25666726','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25666726"><span>Direct design of an <span class="hlt">energy</span> landscape with bistable DNA origami mechanisms.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhou, Lifeng; Marras, Alexander E; Su, Hai-Jun; Castro, Carlos E</p> <p>2015-03-11</p> <p>Structural DNA nanotechnology provides a feasible technique for the design and fabrication of complex geometries even exhibiting controllable dynamic behavior. Recently we have demonstrated the possibility of implementing macroscopic engineering design approaches to construct DNA origami mechanisms (DOM) with programmable motion and tunable flexibility. Here, we implement the design of compliant DNA origami mechanisms to extend from prescribing motion to prescribing an <span class="hlt">energy</span> landscape. Compliant mechanisms facilitate motion via <span class="hlt">deformation</span> of components with tunable stiffness resulting in well-defined mechanical <span class="hlt">energy</span> stored in the structure. We design, fabricate, and characterize a DNA origami nanostructure with an <span class="hlt">energy</span> landscape defined by two stable states (local <span class="hlt">energy</span> minima) separated by a designed <span class="hlt">energy</span> barrier. This nanostructure is a four-bar bistable mechanism with two undeformed states. Traversing between those states requires <span class="hlt">deformation</span>, and hence mechanical <span class="hlt">energy</span> storage, in a compliant arm of the linkage. The <span class="hlt">energy</span> barrier for switching between two states was obtained from the conformational distribution based on a Boltzmann probability function and closely follows a predictive mechanical model. Furthermore, we demonstrated the ability to actuate the mechanism into one stable state via additional DNA inputs and then <span class="hlt">release</span> the actuation via DNA strand displacement. This controllable multistate system establishes a foundation for direct design of <span class="hlt">energy</span> landscapes that regulate conformational dynamics similar to biomolecular complexes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1910763C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1910763C"><span>Localization in Naturally <span class="hlt">Deformed</span> Systems - the Default State?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Clancy White, Joseph</p> <p>2017-04-01</p> <p>Based on the extensive literature on localized rock <span class="hlt">deformation</span>, conventional wisdom would interpret it to be a special behaviour within an anticipated background of otherwise uniform <span class="hlt">deformation</span>. The latter notwithstanding, the rock record is so rife with transient (cyclic), heterogeneous <span class="hlt">deformation</span>, notably shear localization, as to characterize localization as the anticipated 'normal' behaviour. The corollary is that steady, homogeneous <span class="hlt">deformation</span> is significantly less common, and if achieved must reflect some special set of conditions that are not representative of the general case. An issue central to natural <span class="hlt">deformation</span> is then not the existance of localized strain, but rather how the extant <span class="hlt">deformation</span> processes scale across tectonic phenomena and in turn organize to enable a coherent(?) descripion of Earth <span class="hlt">deformation</span>. <span class="hlt">Deformation</span> is fundamentally quantized, discrete (diffusion, glide, crack propagation) and reliant on the defect state of rock-forming minerals. The strain <span class="hlt">energy</span> distribution that drives thermo-mechanical responses is in the first instance established at the grain-scale where the non-linear interaction of defect-mediated micromechanical processes introduces heterogeneous behaviour described by various gradient theories, and evidenced by the defect microstructures of <span class="hlt">deformed</span> rocks. Hence, the potential for non-uniform response is embedded within even quasi-uniform, monomineralic materials, seen, for example, in the spatially discrete evolution of dynamic recrystallization. What passes as homogeneous or uniform <span class="hlt">deformation</span> at various scales is the aggregation of responses at some characteristic dimension at which heterogeneity is not registered or measured. Nevertheless, the aggregate response and associated normalized parameters (strain, strain rate) do not correspond to any condition actually experienced by the <span class="hlt">deforming</span> material. The more common types of macroscopic heterogeneity promoting localization comprise mechanically contrasting</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70190054','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70190054"><span>Vertical <span class="hlt">deformation</span> through a complete seismic cycle at Isla Santa María, Chile</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Wesson, Robert L.; Melnick, Daniel; Cisternas, Marco; Moreno, Marcos; Ely, Lisa</p> <p>2014-01-01</p> <p>Individual great earthquakes are posited to <span class="hlt">release</span> the elastic strain <span class="hlt">energy</span> that has accumulated over centuries by the gradual movement of tectonic plates1, 2. However, knowledge of plate <span class="hlt">deformation</span> during a complete seismic cycle—two successive great earthquakes and the intervening interseismic period—remains incomplete3. A complete seismic cycle began in south-central Chile in 1835 with an earthquake of about magnitude 8.5 (refs 4, 5) and ended in 2010 with a magnitude 8.8 earthquake6. During the first earthquake, an uplift of Isla Santa María by 2.4 to 3 m was documented4, 5. In the second earthquake, the island was uplifted7 by 1.8 m. Here we use nautical surveys made in 1804, after the earthquake in 1835 and in 1886, together with modern echo sounder surveys and GPS measurements made immediately before and after the 2010 earthquake, to quantify vertical <span class="hlt">deformation</span> through the complete seismic cycle. We find that in the period between the two earthquakes, Isla Santa María subsided by about 1.4 m. We simulate the patterns of vertical <span class="hlt">deformation</span> with a finite-element model and find that they agree broadly with predictions from elastic rebound theory2. However, comparison with geomorphic and geologic records of millennial coastline emergence8, 9 reveal that 10–20% of the vertical uplift could be permanent.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29133908','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29133908"><span>Optically-controlled long-term storage and <span class="hlt">release</span> of thermal <span class="hlt">energy</span> in phase-change materials.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Han, Grace G D; Li, Huashan; Grossman, Jeffrey C</p> <p>2017-11-13</p> <p>Thermal <span class="hlt">energy</span> storage offers enormous potential for a wide range of <span class="hlt">energy</span> technologies. Phase-change materials offer state-of-the-art thermal storage due to high latent heat. However, spontaneous heat loss from thermally charged phase-change materials to cooler surroundings occurs due to the absence of a significant <span class="hlt">energy</span> barrier for the liquid-solid transition. This prevents control over the thermal storage, and developing effective methods to address this problem has remained an elusive goal. Herein, we report a combination of photo-switching dopants and organic phase-change materials as a way to introduce an activation <span class="hlt">energy</span> barrier for phase-change materials solidification and to conserve thermal <span class="hlt">energy</span> in the materials, allowing them to be triggered optically to <span class="hlt">release</span> their stored latent heat. This approach enables the retention of thermal <span class="hlt">energy</span> (about 200 J g -1 ) in the materials for at least 10 h at temperatures lower than the original crystallization point, unlocking opportunities for portable thermal <span class="hlt">energy</span> storage systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSH43A2805I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSH43A2805I"><span><span class="hlt">Energy</span> <span class="hlt">release</span> from a stream of infalling prominence debris on 2011 September 7-8</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Inglis, A. R.; Gilbert, H. R.; Ofman, L.</p> <p>2017-12-01</p> <p>In recent years high-resolution and high-cadence EUV imaging has revealed a new phenomenon, impacting prominence debris, where prominence material from failed or partial eruptions can impact the lower atmosphere and <span class="hlt">release</span> <span class="hlt">energy</span>. We present a clear example of this phenomenon occurring on 2011 September 7-8. The initial eruption of prominence material was associated with an X1.8-class flare from AR11283, occurring at 22:30 UT on 2011 September 7, resulting in a semi-continuous stream of this material returning to the solar surface between 00:20 - 00:40 UT on 2011 September 8. A substantial area remote from the original active region experienced brightening in multiple EUV channels observed by SDO/AIA. Using the differential emission measure, we estimated the energetic properties of this event. We found that the radiated <span class="hlt">energy</span> of the impacted plasma was of order 10^27 ergs, while the upper limit on the thermal <span class="hlt">energy</span> peaked at 10^28 ergs. Based on these estimates we were able to determine the mass content of the debris to be in the range 2x10^14 < m < 2x10^15 g. Given typical promimence masses, the likely debris mass is towards the lower end of this range. This clear example of a prominence debris event shows that significant <span class="hlt">energy</span> <span class="hlt">release</span> takes place during these events, and that such impacts may be used as a novel diagnostic tool for investigating prominence material properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.4925Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.4925Z"><span>Late-Paleozoic-Mesozoic <span class="hlt">deformational</span> and <span class="hlt">deformation</span> related metamorphic structures of Kuznetsk-Altai region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zinoviev, Sergei</p> <p>2014-05-01</p> <p>Kuznetsk-Altai region is a part of the Central Asian Orogenic Belt. The nature and formation mechanisms of the observed structure of Kuznetsk-Altai region are interpreted by the author as the consequence of convergence of Tuva-Mongolian and Junggar lithospheric block structures and <span class="hlt">energy</span> of collision interaction between the blocks of crust in Late-Paleozoic-Mesozoic period. Tectonic zoning of Kuznetsk-Altai region is based on the principle of adequate description of geological medium (without methods of 'primary' state recovery). The initial indication of this convergence is the crust thickening in the zone of collision. On the surface the mechanisms of lateral compression form a regional elevation; with this elevation growth the 'mountain roots' start growing. With an approach of blocks an interblock elevation is divided into various fragments, and these fragments interact in the manner of collision. The physical expression of collision mechanisms are periodic pulses of seismic activity. The main tectonic consequence of the block convergence and collision of interblock units is formation of an ensemble of regional structures of the <span class="hlt">deformation</span> type on the basis of previous 'pre-collision' geological substratum [Chikov et al., 2012]. This ensemble includes: 1) allochthonous and autochthonous blocks of weakly <span class="hlt">deformed</span> substratum; 2) folded (folded-thrust) systems; 3) dynamic metamorphism zones of regional shears and main faults. Characteristic of the main structures includes: the position of sedimentary, magmatic and PT-metamorphic rocks, the degree of rock dynamometamorphism and variety rock body <span class="hlt">deformation</span>, as well as the styles and concentrations of mechanic <span class="hlt">deformations</span>. 1) block terranes have weakly elongated or isometric shape in plane, and they are the systems of block structures of pre-collision substratum separated by the younger zones of interblock <span class="hlt">deformations</span>. They stand out among the main <span class="hlt">deformation</span> systems, and the smallest are included into the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27730290','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27730290"><span>The impact of different types of talus <span class="hlt">deformation</span> after treatment of clubfeet.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kolb, Alexander; Willegger, Madeleine; Schuh, Reinhard; Kaider, Alexandra; Chiari, Catharina; Windhager, Reinhard</p> <p>2017-01-01</p> <p><span class="hlt">Deformation</span> of the talus in idiopathic congenital clubfeet is a known problem after treatment. However evidence on types of talus <span class="hlt">deformation</span> and clinical relevance is rare. The aims of this study were first to define different types of talus <span class="hlt">deformation</span>, and second, to evaluate the impact of these types on long-term results. At a minimum follow-up of ten years 40 idiopathic clubfeet treated by a modified dorsomedial <span class="hlt">release</span> were analyzed. Based on morphological appearance and the widened range of radius to length ratios (R/L-ratio) in treated clubfeet <span class="hlt">deformed</span> tali were divided into two groups: tali with decreased R/L-ratios were classified as small-dome talus <span class="hlt">deformation</span> (SD), tali with increased R/L-ratios were classified as flat-top talus <span class="hlt">deformation</span> (FT). The impact on degree of arthrosis in the ankle joint, clinical outcome, and ankle range of motion was analyzed. Small-dome talus <span class="hlt">deformation</span> (SD) was found in nine feet. This group showed decreased R/L-ratios and increased talus opening angles, which were linked to an increased range of motion of the ankle joint (p = 0.033). The impact on onset of arthrosis was not significant for this group (p = 0.056). The group of flat top talus <span class="hlt">deformation</span> (nine feet) showed increased R/L-ratios and decreased talus opening angles, decreased range of motion (p = 0.019), and a significant impact on onset of arthrosis (p = 0.010). Our study defines a new subgroup of talus <span class="hlt">deformation</span>: the small dome talus <span class="hlt">deformation</span> tends to show a better ankle joint range of motion and a lower risk of arthrosis compared to the classical flat dome talus <span class="hlt">deformation</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.B41E0368K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.B41E0368K"><span>Influence of ultrasonic <span class="hlt">energy</span> on dispersion of aggregates and <span class="hlt">released</span> amounts of organic matter and polyvalent cations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaiser, M.; Kleber, M.; Berhe, A. A.</p> <p>2010-12-01</p> <p>Aggregates play important roles in soil carbon storage and stabilization. Identification of scale-dependent mechanisms of soil aggregate formation and stability is necessary to predict and eventually manage the flow of carbon through terrestrial ecosystems. Application of ultrasonic <span class="hlt">energy</span> is a common tool to disperse soil aggregates. In this study, we used ultra sonic <span class="hlt">energy</span> (100 to 2000 J cm-3) to determine the amount of polyvalent cations and organic matter involved in aggregation processes in three arable and three forest soils that varied in soil mineral composition. To determine the amount of organic matter and cations <span class="hlt">released</span> after application of different amount of ultrasonic <span class="hlt">energy</span>, we removed the coarse fraction (>250 µm). The remaining residue (<250 µm) was mixed with water and ultrasonically dispersed by application of 100, 200, 400, 500, 1000, 1500 and 2000 J cm-3 <span class="hlt">energy</span>. After centrifugation the supernatant was filtered and the solid residue freeze dried before we analyzed the amounts of water-extracted organic carbon (OC), Fe, Al, Ca, Mn, and Mg in the filtrates. The extracted OM and solid residues were further characterized by Fourier Transformed Infra Red spectroscopy and Scanning Electron Microscopy. Our results show a linear increase in amount of dissolved OC with increasing amounts of ultra sonic <span class="hlt">energy</span> up to 1500 J cm-3 indicating maximum dispersion of soil aggregates at this <span class="hlt">energy</span> level independent from soil type or land use. In contrast to Mn, and Mg, the amounts of dissolved Ca, Fe, and Al increase with increasing ultra sonic <span class="hlt">energy</span> up to 1500 J cm-3. At 1500 J cm-3, the absolute amounts of OC, Ca, Fe, and Al <span class="hlt">released</span> were specific for each soil type, likely indicating differences in type of OM-mineral interactions involved in micro-scaled aggregation processes. The amounts of dissolved Fe, and Al <span class="hlt">released</span> after an application of 1500 J cm-3 are not related to oxalate- and dithionite- extractable, or total Al content indicating less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_11 --> <div id="page_12" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="221"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70016260','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70016260"><span><span class="hlt">Deformation</span> monitoring at Nevado del Ruiz, Colombia - October 1985 - March 1988</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Banks, N.G.; Carvajal, C.; Mora, H.; Tryggvason, E.</p> <p>1990-01-01</p> <p><span class="hlt">Deformation</span> studies began at Nevado del Ruiz 23 days before the devastating 13 November 1985 eruption, at least 12 months after precursory seismicity and fumarolic activity began. The late start in geodetic monitoring, limited number of stations in the pre-eruption network, and inconsistent patterns in the observed <span class="hlt">deformation</span> limit conclusions about intrusive activity in the months and weeks prior to the eruption. However, the data require that the magma source of the devastating eruption was either deeper than 7 km or, if shallow, recovered the same volume and position within one week of the eruption. Geodetic monitoring resumed 1 week after the eruption and, by April 1986, included 11 tilt-leveling stations, 38 EDM lines, and 7 short leveling lines - a network capable of detecting emplacement or movement of magma volumes as small as 3 MCM (3 ?? 106 m3) to a depth of 2-3 km (using a point-source model), 10 MCM to 7 km, 50 MCM to 10 km, and 200 MCM to 15 km beneath Ruiz. In addition, 4 telemetered tiltmeters provided the capability of detecting, in real time, the fairly rapid ascent of much smaller magma bodies. Stations established to detect instability of the summit ice cap after the eruption were discontinued in early 1986. The data collected from the geodetic networks have higher than normal variance but demonstrate that little or no cumulative <span class="hlt">deformation</span> of Ruiz occurred from October 1985 through March 1988. Thus, little, if any, magma intruded above 5 km beneath the summit during or after the 13 November 1985 eruption. This lack of significant intrusive activity agrees with the surprisingly low seismic <span class="hlt">energy</span> <span class="hlt">release</span> under Ruiz and makes direct degassing of a large batholith an improbable explanation of the large sulfur flux to date at Ruiz. Part of the variance in the geodetic data results from real but noncumulative <span class="hlt">deformation</span> that may in part be pressure-buffered by a fairly large geothermal water-gas mixture for which abundant physical evidence exists</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.7263G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.7263G"><span>Surface <span class="hlt">deformation</span> associated with the 2013 Mw7.7 Balochistan earthquake: Geologic slip rates may significantly underestimate strain <span class="hlt">release</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gold, Ryan; Reitman, Nadine; Briggs, Richard; Barnhart, William; Hayes, Gavin</p> <p>2015-04-01</p> <p>The 24 September 2013 Mw7.7 Balochistan, Pakistan earthquake ruptured a ~200 km-long stretch of the 60° ± 15° northwest-dipping Hoshab fault in southern Pakistan. The earthquake is notable because it produced the second-largest lateral surface displacement observed for a continental strike-slip earthquake. Surface displacements and geodetic and teleseismic inversions indicate that peak slip occurred within the upper 0-3 km of the crust. To explore along-strike and fault-perpendicular surface <span class="hlt">deformation</span> patterns, we remotely mapped the surface trace of the rupture and measured its surface <span class="hlt">deformation</span> using high-resolution (0.5 m) pre- and post-event satellite imagery. Post-event images were collected 7-114 days following the earthquake, so our analysis captures the sum of both the coseismic and post-seismic (e.g., after slip) <span class="hlt">deformation</span>. We document peak left-lateral offset of ~15 m using 289 near-field (±10 m from fault) laterally offset piercing points, such as streams, terrace risers, and roads. We characterize off-fault <span class="hlt">deformation</span> by measuring the medium- (±200 m from fault) and far-field (±10 km from fault) displacement using manual (242 measurements) and automated image cross-correlation methods. Off-fault peak lateral displacement values (medium- and far-field) are ~16 m and commonly exceed the on-fault displacement magnitudes. Our observations suggest that coseismic surface displacement typically increases with distance away from the surface trace of the fault; however, the majority of surface displacement is within 100 m of the primary fault trace and is most localized on sections of the rupture exhibiting narrow (<5 m) zones of observable surface <span class="hlt">deformation</span>. Furthermore, the near-field displacement measurements account for, on average, only 73% of the total coseismic displacement field and the pattern is highly heterogeneous. This analysis highlights the importance of identifying paleoseismic field study sites (e.g. trenches) that span fault</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720019047','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720019047"><span>Liquid rocket performance computer model with distributed <span class="hlt">energy</span> <span class="hlt">release</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Combs, L. P.</p> <p>1972-01-01</p> <p>Development of a computer program for analyzing the effects of bipropellant spray combustion processes on liquid rocket performance is described and discussed. The distributed <span class="hlt">energy</span> <span class="hlt">release</span> (DER) computer program was designed to become part of the JANNAF liquid rocket performance evaluation methodology and to account for performance losses associated with the propellant combustion processes, e.g., incomplete spray gasification, imperfect mixing between sprays and their reacting vapors, residual mixture ratio striations in the flow, and two-phase flow effects. The DER computer program begins by initializing the combustion field at the injection end of a conventional liquid rocket engine, based on injector and chamber design detail, and on propellant and combustion gas properties. It analyzes bipropellant combustion, proceeding stepwise down the chamber from those initial conditions through the nozzle throat.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008APS..DFD.AJ001F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008APS..DFD.AJ001F"><span>Red Blood Cell <span class="hlt">Deformation</span> Under Shear Flow: The Effect of Changing Cell Properties</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Forsyth, Alison M.; Wan, Jiandi; Ristenpart, William D.; Stone, Howard A.</p> <p>2008-11-01</p> <p>The <span class="hlt">deformability</span> of red blood cells plays a major role in the pathology of several diseases, including malaria, sickle cell anemia and spherocytosis. Moreover, <span class="hlt">deformations</span> are believed to trigger the <span class="hlt">release</span> of adenosine triphosphate, which helps regulate vascular tone and is consequently an important factor in various vascular diseases. Here we investigate single-cell viscoelastic responses to increased shear stress in poly(dimethylsiloxane) channels with a single constriction 2-4 times larger than a typical erythrocyte. These channels mimic arteriole-sized vessels, and have the advantage that the cell membrane is not in contact with the channel walls which have vastly different mechanical and material properties than living tissue. High-speed video and image analysis were used to quantify the trajectories and <span class="hlt">deformations</span> of cells exposed to varied doses of diamide, a chemical known to ``rigidify'' erythrocytes. Our results show that (i) <span class="hlt">deformation</span> is proportional to shear rate and (ii) the <span class="hlt">deformability</span> of diamide-treated cells is greater than that of untreated cells. The latter is an unforeseen result because micropipette aspiration experiments have shown the opposite. We expect that the experimental procedure described here will be useful for characterizing the effect of different therapeutic agents on cellular <span class="hlt">deformability</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JMPSo.114...31Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JMPSo.114...31Z"><span>Mechanics of adsorption-<span class="hlt">deformation</span> coupling in porous media</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Yida</p> <p>2018-05-01</p> <p>This work extends Coussy's macroscale theory for porous materials interacting with adsorptive fluid mixtures. The solid-fluid interface is treated as an independent phase that obeys its own mass, momentum and <span class="hlt">energy</span> balance laws. As a result, a surface strain <span class="hlt">energy</span> term appears in the free <span class="hlt">energy</span> balance equation of the solid phase, which further introduces the so-called adsorption stress in the constitutive equations of the porous skeleton. This establishes a fundamental link between the adsorption characteristics of the solid-fluid interface and the mechanical response of the porous media. The thermodynamic framework is quite general in that it recovers the coupled conduction laws, Gibbs isotherm and the Shuttleworth's equation for surface stress, and imposes no constraints on the magnitude of <span class="hlt">deformation</span> and the functional form of the adsorption isotherms. A rich variety of coupling between adsorption and <span class="hlt">deformation</span> is recovered as a result of combining different poroelastic models (isotropic vs. anisotropic, linear vs. nonlinear) and adsorption models (unary vs. mixture adsorption, uncoupled vs. stretch-dependent adsorption). These predictions are discussed against the backdrop of recent experimental data on coal swelling subjected to CO2 and CO2sbnd CH4 injections, showing the capability and versatility of the theory in capturing adsorption-induced <span class="hlt">deformation</span> of porous materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JHEP...02..035B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JHEP...02..035B"><span>Fast spinning strings on η <span class="hlt">deformed</span> AdS 5 × S 5</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Banerjee, Aritra; Bhattacharyya, Arpan; Roychowdhury, Dibakar</p> <p>2018-02-01</p> <p>In this paper, considering the correspondence between spin chains and string sigma models, we explore the rotating string solutions over η <span class="hlt">deformed</span> AdS 5 × S 5 in the so-called fast spinning limit. In our analysis, we focus only on the bosonic part of the full superstring action and compute the relevant limits on both ( R × S 3) η and ( R × S 5) η models. The resulting system reveals that in the fast spinning limit, the sigma model on η <span class="hlt">deformed</span> S 5 could be approximately thought of as the continuum limit of anisotropic SU(3) Heisenberg spin chain model. We compute the <span class="hlt">energy</span> for a certain class of spinning strings in <span class="hlt">deformed</span> S 5 and we show that this <span class="hlt">energy</span> can be mapped to that of a similar spinning string in the purely imaginary β <span class="hlt">deformed</span> background.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhFl...30a1902C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhFl...30a1902C"><span>Flow characteristics around a <span class="hlt">deformable</span> stenosis under pulsatile flow condition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, Woorak; Park, Jun Hong; Byeon, Hyeokjun; Lee, Sang Joon</p> <p>2018-01-01</p> <p>A specific portion of a vulnerable stenosis is <span class="hlt">deformed</span> periodically under a pulsatile blood flow condition. Detailed analysis of such <span class="hlt">deformable</span> stenosis is important because stenotic <span class="hlt">deformation</span> can increase the likelihood of rupture, which may lead to sudden cardiac death or stroke. Various diagnostic indices have been developed for a nondeformable stenosis by using flow characteristics and resultant pressure drop across the stenosis. However, the effects of the stenotic <span class="hlt">deformation</span> on the flow characteristics remain poorly understood. In this study, the flows around a <span class="hlt">deformable</span> stenosis model and two different rigid stenosis models were investigated under a pulsatile flow condition. Particle image velocimetry was employed to measure flow structures around the three stenosis models. The <span class="hlt">deformable</span> stenosis model was <span class="hlt">deformed</span> to achieve high geometrical slope and height when the flow rate was increased. The <span class="hlt">deformation</span> of the stenotic shape enhanced jet deflection toward the opposite vessel wall of the stenosis. The jet deflection in the <span class="hlt">deformable</span> model increased the rate of jet velocity and turbulent kinetic <span class="hlt">energy</span> (TKE) production as compared with those in the rigid models. The effect of stenotic <span class="hlt">deformation</span> on the pulsating waveform related with the pressure drop was analyzed using the TKE production rate. The <span class="hlt">deformable</span> stenosis model exhibited a phase delay of the peak point in the waveform. These results revealed the potential use of pressure drop waveform as a diagnostic index for <span class="hlt">deformable</span> stenosis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21839565','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21839565"><span>Seven fundamental procedures for definitive correction of unilateral secondary cleft lip nasal <span class="hlt">deformity</span> in soft tissue aspects.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Dong Won; Choi, Bong-Kyoon; Park, Be-Young Yun</p> <p>2011-11-01</p> <p>It is accepted that patients who undergo appropriate primary repair for cleft lip will have secondary <span class="hlt">deformities</span>. Because these <span class="hlt">deformities</span> are caused by complex and diverse patterns, the <span class="hlt">deformities</span> were categorized to provide a standardized treatment for each category. Pathologic characteristics of 1,170 patients were classified into 7 categories. Corrections were performed using 7 fundamental procedures corresponding to the surgical resolution of each <span class="hlt">deformity</span>: 1) transposition of the caudal septum; 2) <span class="hlt">release</span> of the septal-cartilaginous junction; 3) medial crus elevation; 4) lateral crus elevation; 5) <span class="hlt">release</span> of the orbicularis oris muscle from the lip elevators; 6) anchoring of the orbicularis oris muscle to the anterior nasal spine; and 7) philtral column formation. A satisfaction survey was performed to evaluate the overall outcomes in 171 patients and an anthropometric analysis was performed in 38 patients. Satisfactory scores obtained through postoperative follow-up were higher than preoperative scores, and there was no difference between postoperative scores obtained over the short and long term. All preoperative anthropometric measurements were different from the postoperative measurements, indicating that the fundamental procedure achieved effective outcomes. These proposed 7 fundamental procedures can be used as guidelines that can always be applied for the correction of any secondary cleft lip nasal <span class="hlt">deformity</span> to obtain ideal treatment outcomes. Copyright © 2011. Published by Elsevier Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1377897-situ-synchrotron-high-energy-ray-diffraction-study-microscopic-deformation-behavior-hard-soft-dual-phase-composite-containing-phase-transforming-matrix','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1377897-situ-synchrotron-high-energy-ray-diffraction-study-microscopic-deformation-behavior-hard-soft-dual-phase-composite-containing-phase-transforming-matrix"><span>In situ synchrotron high-<span class="hlt">energy</span> X-ray diffraction study of microscopic <span class="hlt">deformation</span> behavior of a hard-soft dual phase composite containing phase transforming matrix</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Zhang, Junsong; Hao, Shijie; Jiang, Daqiang</p> <p></p> <p>This study explored a novel intermetallic composite design concept based on the principle of lattice strain matching enabled by the collective atomic load transfer. It investigated the hard-soft microscopic <span class="hlt">deformation</span> behavior of a Ti3Sn/TiNi eutectic hard-soft dual phase composite by means of in situ synchrotron high-<span class="hlt">energy</span> X-ray diffraction (HE-XRD) during compression. The composite provides a unique micromechanical system with distinctive <span class="hlt">deformation</span> behaviors and mechanisms from the two components, with the soft TiNi matrix <span class="hlt">deforming</span> in full compliance via martensite variant reorientation and the hard Ti3Sn lamellae <span class="hlt">deforming</span> predominantly by rigid body rotation, producing a crystallographic texture for the TiNi matrixmore » and a preferred alignment for the Ti3Sn lamellae. HE-XRD reveals continued martensite variant reorientation during plastic <span class="hlt">deformation</span> well beyond the stress plateau of TiNi. The hard and brittle Ti3Sn is also found to produce an exceptionally large elastic strain of 1.95% in the composite. This is attributed to the effect of lattice strain matching between the transformation lattice distortion of the TiNi matrix and the elastic strain of Ti3Sn lamellae. With such unique micromechanic characteristics, the composite exhibits high strength and large ductility.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.T51I..07F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.T51I..07F"><span>Reconciling Pre- and Co-Seismic <span class="hlt">Deformation</span> at Megathrusts: Tohoku Informing Cascadia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Furlong, K. P.; Govers, R. M.</p> <p>2013-12-01</p> <p>One of the outstanding goals of earthquake science is to effectively anticipate the earthquake characteristics of a future event - magnitude, rupture area, slip history - through the judicious application of models that use observations of inter-earthquake <span class="hlt">deformation</span> and the history of earthquakes along that plate boundary segment. The series of great earthquakes over the past decade since the 2004 Mw 9.2 Sumatra earthquake have demonstrated both the sobering reality that our current models of subduction zone earthquake genesis are insufficient but more positively have provided a wealth of data and observations that can be used to develop improved framework models of the lithospheric behavior through the earthquake cycle in subduction zones. Some of the issues that recent observations raise are straightforward, while others imply aspects of the subduction process that have not been previously considered important. Based on observations of a range of great earthquakes since 2004, and with a particular focus on the 2011 Mw 9.0 Tohoku event we can identify a suite of key issues that include: (1) Patterns of inter-seismic <span class="hlt">deformation</span> (strain accumulation) are not simply the converse of the co-seismic elastic strain <span class="hlt">release</span>. (2) <span class="hlt">Deformation</span> of the slab during the earthquake cycle is a common occurrence and its role in buffering upper-plate <span class="hlt">deformation</span> is a key consideration in the potential tsunamigenic character of a subduction system. (3) Rates of pre-earthquake <span class="hlt">deformation</span> (e.g. observed upper-plate GPS displacements) and inferred slip deficit accumulation on the megathrust are inconsistent with co-seismic displacements/fault slip and recurrence intervals. (4) Patterns of megathrust locked patches, degrees of coupling and other parameterizations that are used to define earthquake potential have only a loose agreement with the actual patterns of slip and moment <span class="hlt">release</span> seen in the ensuing great earthquake. Simple elastic models do provide a general agreement between</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MS%26E..234a2006Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MS%26E..234a2006Z"><span>Numerical Investigations on Aerodynamic Forces of <span class="hlt">Deformable</span> Foils in Hovering Motions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Yong; Yin, Zhen; Su, Xiaohui; Zhang, Jiantao; Cao, Yuanwei</p> <p>2017-09-01</p> <p>The aerodynamic effects of wing <span class="hlt">deformation</span> for hover flight are numerically investigated by a two-dimensional finite-volume (FV) Arbitrary Langrangian Eulerian (ALE) Navier-Stokes solver. Two <span class="hlt">deformation</span> models are employed to study these effects in this paper, which are a full <span class="hlt">deformation</span> model and a partial <span class="hlt">deformation</span> one. Attentions are paid to the generation and development of leading edge vortex (LEV) and trailing edge vortex (TEV) which may illustrate the differences of lift force generation mechanisms from those of rigid wings. Moreover, lift coefficient Cl, drag coefficient Cd, and figure of merit, as well as <span class="hlt">energy</span> consumption in hovering motion for different <span class="hlt">deformation</span> foil models, are also studied. The results show that the <span class="hlt">deformed</span> amplitude, 0.1*chord, among the cases simulated is an optimized camber amplitude for full <span class="hlt">deformation</span>. The results obtained from the partial <span class="hlt">deformation</span> foil model show that both Cl and Cd decrease with the increase of camber amplitude. It is found that the effect of <span class="hlt">deformation</span> in the partial <span class="hlt">deformation</span> model does not enhance lift force due to unfavorable camber. But TEV is significantly changed by the local AOA due to the <span class="hlt">deformation</span> of the foil. Introduction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29869670','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29869670"><span>Yield of reversible colloidal gels during flow start-up: <span class="hlt">release</span> from kinetic arrest.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Johnson, Lilian C; Landrum, Benjamin J; Zia, Roseanna N</p> <p>2018-06-05</p> <p>Yield of colloidal gels during start-up of shear flow is characterized by an overshoot in shear stress that accompanies changes in network structure. Prior studies of yield of reversible colloidal gels undergoing strong flow model the overshoot as the point at which network rupture permits fluidization. However, yield under weak flow, which is of interest in many biological and industrial fluids shows no such disintegration. The mechanics of reversible gels are influenced by bond strength and durability, where ongoing rupture and re-formation impart aging that deepens kinetic arrest [Zia et al., J. Rheol., 2014, 58, 1121], suggesting that yield be viewed as <span class="hlt">release</span> from kinetic arrest. To explore this idea, we study reversible colloidal gels during start-up of shear flow via dynamic simulation, connecting rheological yield to detailed measurements of structure, bond dynamics, and potential <span class="hlt">energy</span>. We find that pre-yield stress grows temporally with the changing roles of microscopic transport processes: early time behavior is set by Brownian diffusion; later, advective displacements permit relative particle motion that stretches bonds and stores <span class="hlt">energy</span>. Stress accumulates in stretched, oriented bonds until yield, which is a tipping point to <span class="hlt">energy</span> <span class="hlt">release</span>, and is passed with a fully intact network, where the loss of very few bonds enables relaxation of many, easing glassy arrest. This is immediately followed by a reversal to growth in potential <span class="hlt">energy</span> during bulk plastic <span class="hlt">deformation</span> and condensation into larger particle domains, supporting the view that yield is an activated <span class="hlt">release</span> from kinetic arrest. The continued condensation of dense domains and shrinkage of network surfaces, along with a decrease in the potential <span class="hlt">energy</span>, permit the gel to evolve toward more complete phase separation, supporting our view that yield of weakly sheared gels is a 'non-equilibrium phase transition'. Our findings may be particularly useful for industrial or other coatings, where weak</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950008130','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950008130"><span>Thermocapillary motion of <span class="hlt">deformable</span> drops</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Haj-Hariri, Hossein; Shi, Qingping; Borhan, Ali</p> <p>1994-01-01</p> <p>The thermocapillary motion of initially spherical drops/bubbles driven by a constant temperature gradient in an unbounded liquid medium is simulated numerically. Effects of convection of momentum and <span class="hlt">energy</span>, as well as shape <span class="hlt">deformations</span>, are addressed. The method used is based on interface tracking on a base cartesian grid, and uses a smeared color or indicator function for the determination of the surface topology. Quad-tree adaptive refinement of the cartesian grid is implemented to enhance the fidelity of the surface tracking. It is shown that convection of <span class="hlt">energy</span> results in a slowing of the drop, as the isotherms get wrapped around the front of the drop. Shape <span class="hlt">deformation</span> resulting from inertial effects affect the migration velocity. The physical results obtained are in agreement with the existing literature. Furthermore, remarks are made on the sensitivity of the calculated solutions to the smearing of the fluid properties. Analysis and simulations show that the migration velocity depends very strongly on the smearing of the interfacial force whereas it is rather insensitive to the smearing of other properties, hence the adaptive grid.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890015386','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890015386"><span>Plate motions and <span class="hlt">deformations</span> from geologic and geodetic data</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jordan, Thomas H.</p> <p>1989-01-01</p> <p>The very long baseline interferometry (VLBI) measurements made in the western U.S. since 1979 provide discrete samples of the temporal and spatial <span class="hlt">deformation</span> field. The interpretation of the VLBI derived rates of <span class="hlt">deformation</span> requires an examination of geologic information and more densely sampled ground based geodetic data. Triangulation and trilateration data measured on two regional networks, one in the central Mojave Desert and one in the Coast Ranges east of the San Andreas fault, were processed. At the spatial scales spanned by these local geodetic networks, auxiliary geologic and geophysical data were utilized to examine the relation between measured incremental strain and the accommodation of strain seen in local geologic structures, strain <span class="hlt">release</span> in earthquakes, and principal stress directions inferred from in situ measurements. VLBI data was also processed from stations distributed across the Pacific-North America plate boundary zone in the western U.S. The VLBI data were used to constrain the integrated rate of <span class="hlt">deformation</span> across portions of the continental plate boundary in California and to provide a tectonic framework to interpret regional geodetic and geologic studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900052352&hterms=solar+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsolar%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900052352&hterms=solar+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dsolar%2Benergy"><span>Observational clues to the <span class="hlt">energy</span> <span class="hlt">release</span> process in impulsive solar bursts</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Batchelor, David</p> <p>1990-01-01</p> <p>The nature of the <span class="hlt">energy</span> <span class="hlt">release</span> process that produces impulsive bursts of hard X-rays and microwaves during solar flares is discussed, based on new evidence obtained using the method of Crannell et al. (1978). It is shown that the hard X-ray spectral index gamma is negatively correlated with the microwave peak frequency, suggesting a common source for the microwaves and X-rays. The thermal and nonthermal models are compared. It is found that the most straightforward explanations for burst time behavior are shock-wave particle acceleration in the nonthermal model and thermal conduction fronts in the thermal model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999JPhA...32.2091C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999JPhA...32.2091C"><span>Quantum mechanics on the h-<span class="hlt">deformed</span> quantum plane</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cho, Sunggoo</p> <p>1999-03-01</p> <p>We find the covariant <span class="hlt">deformed</span> Heisenberg algebra and the Laplace-Beltrami operator on the extended h-<span class="hlt">deformed</span> quantum plane and solve the Schrödinger equations explicitly for some physical systems on the quantum plane. In the commutative limit the behaviour of a quantum particle on the quantum plane becomes that of the quantum particle on the Poincaré half-plane, a surface of constant negative Gaussian curvature. We show that the bound state <span class="hlt">energy</span> spectra for particles under specific potentials depend explicitly on the <span class="hlt">deformation</span> parameter h. Moreover, it is shown that bound states can survive on the quantum plane in a limiting case where bound states on the Poincaré half-plane disappear.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16432318','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16432318"><span>Kirschner-wire fixation for postburn flexion contracture <span class="hlt">deformity</span> and consequences on articular surface.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sungur, Nezih; Ulusoy, Mustafa Gürhan; Boyacgil, Süreyya; Ortaparmak, Hülya; Akyüz, Mihriban; Ortak, Turgut; Koçer, Uğur; Sensöz, Omer</p> <p>2006-02-01</p> <p>Kirschner-wire (K-wire) fixation for 3-6 weeks is an approved method for stabilization of the fingers after the <span class="hlt">release</span> of flexion contracture <span class="hlt">deformity</span>. On the other hand, articular surface damage in small joints due to pin fixation is still a topic of debate. Reports claiming permanent joint destruction due to this procedure exist in the literature. To clarify this doubt, a prospective study was carried out in 72 patients with flexion contracture of the hand fingers. After the surgical <span class="hlt">release</span> of the <span class="hlt">deformity</span>, immobilization of the interphalangeal (IP) and metacarpophalangeal (MCP) joints was carried out with K-wire fixation for 3 weeks. Clinical evaluation of the patients was accomplished with total active motion (TAM), grip, and pinch force measurements, whereas magnetic resonance (MR) and radionuclide imaging were used as radiodiagnostic tools. Mean follow-up period of the patients was 32 months. Satisfactory results were obtained in terms of functional and esthetic aspects. Evaluation of the data derived from the clinical and radiologic measurements revealed no permanent articular surface damage. K-wire fixation was documented to be an invaluable therapeutic approach not only to prevent recurrence of the contracture <span class="hlt">deformity</span> but also to stabilize the skin graft effectively. This technique was concluded to provide effective immobilization without permanent articular damage.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22614032-energy-release-temperature-field-ultracold-neutron-source-wwr-reactor-petersburg-nuclear-physics-institute','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22614032-energy-release-temperature-field-ultracold-neutron-source-wwr-reactor-petersburg-nuclear-physics-institute"><span>The <span class="hlt">energy</span> <span class="hlt">release</span> and temperature field in the ultracold neutron source of the WWR-M reactor at the Petersburg Nuclear Physics Institute</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Serebrov, A. P., E-mail: serebrov@pnpi.spb.ru; Kislitsin, B. V.; Onegin, M. S.</p> <p>2016-12-15</p> <p>Results of calculations of <span class="hlt">energy</span> <span class="hlt">releases</span> and temperature fields in the ultracold neutron source under design at the WWR-M reactor are presented. It is shown that, with the reactor power of 18 MW, the power of <span class="hlt">energy</span> <span class="hlt">release</span> in the 40-L volume of the source with superfluid helium will amount to 28.5 W, while 356 W will be <span class="hlt">released</span> in a liquid-deuterium premoderator. The lead shield between the reactor core and the source reduces the radiative heat <span class="hlt">release</span> by an order of magnitude. A thermal power of 22 kW is <span class="hlt">released</span> in it, which is removed by passage of water.more » The distribution of temperatures in all components of the vacuum structure is presented, and the temperature does not exceed 100°C at full reactor power. The calculations performed make it possible to go to design of the source.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040090446','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040090446"><span>Effect of Shear <span class="hlt">Deformation</span> and Continuity on Delamination Modelling with Plate Elements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Glaessgen, E. H.; Riddell, W. T.; Raju, I. S.</p> <p>1998-01-01</p> <p>The effects of several critical assumptions and parameters on the computation of strain <span class="hlt">energy</span> <span class="hlt">release</span> rates for delamination and debond configurations modeled with plate elements have been quantified. The method of calculation is based on the virtual crack closure technique (VCCT), and models that model the upper and lower surface of the delamination or debond with two-dimensional (2D) plate elements rather than three-dimensional (3D) solid elements. The major advantages of the plate element modeling technique are a smaller model size and simpler geometric modeling. Specific issues that are discussed include: constraint of translational degrees of freedom, rotational degrees of freedom or both in the neighborhood of the crack tip; element order and assumed shear <span class="hlt">deformation</span>; and continuity of material properties and section stiffness in the vicinity of the debond front, Where appropriate, the plate element analyses are compared with corresponding two-dimensional plane strain analyses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JHEP...02..114G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JHEP...02..114G"><span>T\\overline{T} -<span class="hlt">deformations</span>, AdS/CFT and correlation functions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Giribet, Gaston</p> <p>2018-02-01</p> <p>A solvable irrelevant <span class="hlt">deformation</span> of AdS3/CFT2 correspondence leading to a theory with Hagedorn spectrum at high <span class="hlt">energy</span> has been recently proposed. It consists of a single trace <span class="hlt">deformation</span> of the boundary theory, which is inspired by the recent work on solvable T\\overline{T} <span class="hlt">deformations</span> of two-dimensional CFTs. Thought of as a worldsheet σ-model, the interpretation of the <span class="hlt">deformed</span> theory from the bulk viewpoint is that of string theory on a background that interpolates between AdS3 in the IR and a linear dilaton vacuum of little string theory in the UV. The insertion of the operator that realizes the <span class="hlt">deformation</span> in the correlation functions produces a logarithmic divergence, leading to the renormalization of the primary operators, which thus acquire an anomalous dimension. We compute this anomalous dimension explicitly, and this provides us with a direct way of determining the spectrum of the theory. We discuss this and other features of the correlation functions in presence of the <span class="hlt">deformation</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li class="active"><span>12</span></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_12 --> <div id="page_13" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="241"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008FrMS....2...72Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008FrMS....2...72Z"><span>Directly spheroidizing during hot <span class="hlt">deformation</span> in GCr15 steels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Guo-hui; Zheng, Gang</p> <p>2008-03-01</p> <p>The spheroidizing heat treatment is normally required prior to the cold forming in GCr15 steel in order to improve its machinability. In the conventional spheroidizing process, very long annealing time, generally more than 10 h, is needed to assure proper spheroidizing. It results in low productivity, high cost, and especially high <span class="hlt">energy</span> consumption. Therefore, the possibility of directly spheroidizing during hot <span class="hlt">deformation</span> in GCr15 steel is preliminarily explored. The effect of hot <span class="hlt">deformation</span> parameters on the final microstructure and hardness is investigated systematically in order to develop a directly spheroidizing technology. Experimental results illustrate that low <span class="hlt">deformation</span> temperature and slow cooling rate is the favorite in directly softening and/or spheroidizing during hot <span class="hlt">deformation</span>, which allows the properties of asrolled GCr15 to be applicable for post-machining without requirement of prior annealing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA516406','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA516406"><span>Short Term Innovative Research Program: Nanoengineered Reactive Materials for Tunable Ignition and <span class="hlt">Energy</span> <span class="hlt">Release</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2009-01-01</p> <p>Background Most conventional explosives can be roughly categorized into two classes – molecular materials and intermolecular composites. Molecular...materials refer to species such as the nitroalkanes (e.g. nitromethane ) and cyclic nitramines (e.g. TNAZ, RDX, HMX) that <span class="hlt">release</span> chemical <span class="hlt">energy</span>...alternative to conventional explosives that has been gaining increasing interest have been termed reactive materials, and are defined as systems in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26366443','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26366443"><span><span class="hlt">Deformability</span> and size-based cancer cell separation using an integrated microfluidic device.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pang, Long; Shen, Shaofei; Ma, Chao; Ma, Tongtong; Zhang, Rui; Tian, Chang; Zhao, Lei; Liu, Wenming; Wang, Jinyi</p> <p>2015-11-07</p> <p>Cell sorting by filtration techniques offers a label-free approach for cell separation on the basis of size and <span class="hlt">deformability</span>. However, filtration is always limited by the unpredictable variation of the filter hydrodynamic resistance due to cell accumulation and clogging in the microstructures. In this study, we present a new integrated microfluidic device for cell separation based on the cell size and <span class="hlt">deformability</span> by combining the microstructure-constricted filtration and pneumatic microvalves. Using this device, the cell populations sorted by the microstructures can be easily <span class="hlt">released</span> in real time for subsequent analysis. Moreover, the periodical sort and <span class="hlt">release</span> of cells greatly avoided cell accumulation and clogging and improved the selectivity. Separation of cancer cells (MCF-7, MDA-MB-231 and MDA231-LM2) with different <span class="hlt">deformability</span> showed that the mixture of the less flexible cells (MCF-7) and the flexible cells (MDA-MB-231 and MDA231-LM2) can be well separated with more than 75% purity. Moreover, the device can be used to separate cancer cells from the blood samples with more than 90% cell recovery and more than 80% purity. Compared with the current filtration methods, the device provides a new approach for cancer cell separation with high collection recovery and purity, and also, possesses practical potential to be applied as a sample preparation platform for fundamental studies and clinical applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005JMEP...14..671L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005JMEP...14..671L"><span><span class="hlt">Deformation</span> behavior of TC6 alloy in isothermal forging</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Xiaoli; Li, Miaoquan; Zhu, Dasong; Xiong, Aiming</p> <p>2005-10-01</p> <p>Isothermal compression of the TC6 alloy was carried out in a Thermecmaster-Z (Wuhan Iron and Steel Corporation, P.R. China) simulator at <span class="hlt">deformation</span> temperatures of 800˜1040 °C, strain rates of 0.001˜50.0 s-1, and maximum height reduction of 50%. The <span class="hlt">deformation</span> behavior of the TC6 alloy in isothermal forging was characterized based on stress-strain behavior and kinetic analysis. The activation <span class="hlt">energy</span> of <span class="hlt">deformation</span> obtained in the isothermal forging of the TC6 alloy was 267.49 kJ/mol in the β phase region and 472.76 kJ/mol in the α+β phase region. The processing map was constructed based on the dynamic materials model, and the optimal <span class="hlt">deformation</span> parameters were obtained. Constitutive equations describing the flow stress as a function of strain rate, strain, and <span class="hlt">deformation</span> temperature were proposed for the isothermal forging of the TC6 alloy, and a good agreement between the predicted and experimental stress-strain curves was achieved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1184278-linear-free-energy-correlations-fission-product-release-from-fukushima-daiichi-nuclear-accident','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1184278-linear-free-energy-correlations-fission-product-release-from-fukushima-daiichi-nuclear-accident"><span>Linear Free <span class="hlt">Energy</span> Correlations for Fission Product <span class="hlt">Release</span> from the Fukushima-Daiichi Nuclear Accident</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Abrecht, David G.; Schwantes, Jon M.</p> <p></p> <p>This paper extends the preliminary linear free <span class="hlt">energy</span> correlations for radionuclide <span class="hlt">release</span> performed by Schwantes, et al., following the Fukushima-Daiichi Nuclear Power Plant accident. Through evaluations of the molar fractionations of radionuclides deposited in the soil relative to modeled radionuclide inventories, we confirm the source of the radionuclides to be from active reactors rather than the spent fuel pool. Linear correlations of the form ln χ = -α (ΔG rxn°(T C))/(RT C)+β were obtained between the deposited concentration and the reduction potential of the fission product oxide species using multiple reduction schemes to calculate ΔG° rxn(T C). These models allowedmore » an estimate of the upper bound for the reactor temperatures of T C between 2130 K and 2220 K, providing insight into the limiting factors to vaporization and <span class="hlt">release</span> of fission products during the reactor accident. Estimates of the <span class="hlt">release</span> of medium-lived fission products 90Sr, 121mSn, 147Pm, 144Ce, 152Eu, 154Eu, 155Eu, 151Sm through atmospheric venting and <span class="hlt">releases</span> during the first month following the accident were performed, and indicate large quantities of 90Sr and radioactive lanthanides were likely to remain in the damaged reactor cores.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22392501-method-monitoring-metal-recrystallization-based-situ-measurement-elastic-energy-release-using-neutron-diffraction','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22392501-method-monitoring-metal-recrystallization-based-situ-measurement-elastic-energy-release-using-neutron-diffraction"><span>A method for the monitoring of metal recrystallization based on the in-situ measurement of the elastic <span class="hlt">energy</span> <span class="hlt">release</span> using neutron diffraction</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Christien, F., E-mail: frederic.christien@univ-nantes.fr; Le Gall, R.; Telling, M. T. F.</p> <p>2015-05-15</p> <p>A method is proposed for the monitoring of metal recrystallization using neutron diffraction that is based on the measurement of stored <span class="hlt">energy</span>. Experiments were performed using <span class="hlt">deformed</span> metal specimens heated in-situ while mounted at the sample position of the High Resolution Powder Diffractometer, HRPD (ISIS Facility), UK. Monitoring the breadth of the resulting Bragg lines during heating not only allows the time-dependence (or temperature-dependence) of the stored <span class="hlt">energy</span> to be determined but also the recrystallized fraction. The analysis method presented here was developed using pure nickel (Ni270) specimens with different <span class="hlt">deformation</span> levels from 0.29 to 0.94. In situ temperature rampingmore » as well as isothermal annealing was undertaken. The method developed in this work allows accurate and quantitative monitoring of the recrystallization process. The results from neutron diffraction are satisfactorily compared to data obtained from calorimetry and hardness measurements.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26026530','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26026530"><span>A method for the monitoring of metal recrystallization based on the in-situ measurement of the elastic <span class="hlt">energy</span> <span class="hlt">release</span> using neutron diffraction.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Christien, F; Telling, M T F; Knight, K S; Le Gall, R</p> <p>2015-05-01</p> <p>A method is proposed for the monitoring of metal recrystallization using neutron diffraction that is based on the measurement of stored <span class="hlt">energy</span>. Experiments were performed using <span class="hlt">deformed</span> metal specimens heated in-situ while mounted at the sample position of the High Resolution Powder Diffractometer, HRPD (ISIS Facility), UK. Monitoring the breadth of the resulting Bragg lines during heating not only allows the time-dependence (or temperature-dependence) of the stored <span class="hlt">energy</span> to be determined but also the recrystallized fraction. The analysis method presented here was developed using pure nickel (Ni270) specimens with different <span class="hlt">deformation</span> levels from 0.29 to 0.94. In situ temperature ramping as well as isothermal annealing was undertaken. The method developed in this work allows accurate and quantitative monitoring of the recrystallization process. The results from neutron diffraction are satisfactorily compared to data obtained from calorimetry and hardness measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFM.T13E2661P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFM.T13E2661P"><span>Multiple <span class="hlt">deformation</span> mechanisms operating at seismogenic depths: Tectonic pseudotachylyte and associated <span class="hlt">deformation</span> from the central Sierra Nevada, California</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Prante, M. R.; Evans, J. P.</p> <p>2012-12-01</p> <p>Description and identification of fault-related <span class="hlt">deformation</span> products that are diagnostic of seismic slip have implications for the <span class="hlt">energy</span> budget of earthquakes, fault strength, and fault-rock assemblages. We describe tectonic pseduotachylyte, cataclastic rocks, crystal-plastic <span class="hlt">deformation</span>, and hydrothermal alteration form faults exhumed from seismogenic depths in the Volcanic Lakes area, in northern Sequoia and Kings Canyon National Park, CA, USA. Fault rock protoliths include Mesozoic granite and granodiorite plutonic and limited metasedimentary and metavolcanic rocks. These plutonic and metamorphic rocks are cross-cut by the E-W striking, steeply dipping, left-lateral strike-slip Granite Pass (GPF) and Glacier Lakes faults (GLF). Cross-cutting relationships and microstructural data suggest that the GPF is the oldest fault in the area and preserves evidence for coeval brittle and plastic crystal <span class="hlt">deformation</span>, and hydrothermal fluid-flow. Tectonic pseudotachylyte from the area has been dated using the 40Ar/39Ar method at 76.6 ± 0.3 Ma; when placed into a thermochronologic framework for the plutonic host rock it can be inferred that the pseudotachylyte formed at depths between 2.4-6.0 km with ambient temperatures between 110-160°C. Exceptionally well preserved tectonic pseudotachylyte from the GLF and GPF contain evidence for a frictional melt origin including: 1) plagioclase spherulites and microlites, 2) injection vein morphology, 3) amygdules, 4) viscous flow banding and folds, and 5) embayed and corroded clasts. Pseudotachylyte from the GPF and GLF is associated with brittle and plastic <span class="hlt">deformation</span> in the damage zone of the faults. Evidence for plastic <span class="hlt">deformation</span> includes undulose extinction, <span class="hlt">deformation</span> lamellae, subgrain development, and grain boundary bulging in quartz; and limited undulose extinction in feldspar. Additionally, abundant hydrothermal alteration and mineralization has been documented in the GPF and GLF fault zones, including, chlorite</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24595130','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24595130"><span>Erythrocyte <span class="hlt">deformability</span> and nitric oxide mobilization under pannexin-1 and PKC dependence.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Silva-Herdade, A S; Freitas, T; Almeida, J Pedro; Saldanha, C</p> <p>2015-01-01</p> <p>The erythrocyte adenosine triphosphate (ATP) is utilised for protein phosphorylation and exported through the pannexin 1 hemichannel (Px1) in the microcirculation. The physiological stimuli for ATP <span class="hlt">release</span> are dependent of blood shear rate level and of the tissue oxygen content. The deoxygenated and oxygenated states of haemoglobin are respectively bound and unbound to N terminal domain of the protein band 3 of the erythrocyte membrane in dependence of its degree of phosphorylation. The protein tyrosine kinase (PTK) and protein tyrosine phosphatase (PTP) contribute to the phosphorylation degree of band 3 and are modulated by protein kinase C (PKC). Chelerythrine (Che) is a competitive inhibitor of ATP for PKC and a negative modulator of erythrocyte <span class="hlt">deformability</span>. The aim of this study was to assess the mobilization of nitric oxide (NO) in erythrocyte in absence and presence of Che and Px1 inhibitor (carbenoxolone). Erythrocyte <span class="hlt">deformability</span> was evaluated in presence of carbenoxolone (Carb). Regarding the effects observed in the erythrocyte by presence of Che or Carb, the values of efflux of NO and the concentration of nitrosogluthatione are similar and with no changes in relation to their absence. Px1inhibition by Carb 10 μM ameliorates the erythrocyte <span class="hlt">deformability</span> at a shear force of 0.6 and 1.2 Pa. The PKC inhibitor shows similar effects to the Carb on the mobilization of nitric oxide in erythrocyte. The blockage of ATP <span class="hlt">release</span> by Carb from erythrocytes suggests a possible benefit to develop in ischemia reperfusion or in inflammatory response where will be needed to rescue the excess of NO present and ameliorate the red blood cell <span class="hlt">deformability</span> at low shear rates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1210096K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1210096K"><span>Soft computing analysis of the possible correlation between temporal and <span class="hlt">energy</span> <span class="hlt">release</span> patterns in seismic activity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Konstantaras, Anthony; Katsifarakis, Emmanouil; Artzouxaltzis, Xristos; Makris, John; Vallianatos, Filippos; Varley, Martin</p> <p>2010-05-01</p> <p>This paper is a preliminary investigation of the possible correlation of temporal and <span class="hlt">energy</span> <span class="hlt">release</span> patterns of seismic activity involving the preparation processes of consecutive sizeable seismic events [1,2]. The background idea is that during periods of low-level seismic activity, stress processes in the crust accumulate <span class="hlt">energy</span> at the seismogenic area whilst larger seismic events act as a decongesting mechanism <span class="hlt">releasing</span> considerable <span class="hlt">energy</span> [3,4]. A dynamic algorithm is being developed aiming to identify and cluster pre- and post- seismic events to the main earthquake following on research carried out by Zubkov [5] and Dobrovolsky [6,7]. This clustering technique along with <span class="hlt">energy</span> <span class="hlt">release</span> equations dependent on Richter's scale [8,9] allow for an estimate to be drawn regarding the amount of the <span class="hlt">energy</span> being <span class="hlt">released</span> by the seismic sequence. The above approach is being implemented as a monitoring tool to investigate the behaviour of the underlying <span class="hlt">energy</span> management system by introducing this information to various neural [10,11] and soft computing models [1,12,13,14]. The incorporation of intelligent systems aims towards the detection and simulation of the possible relationship between <span class="hlt">energy</span> <span class="hlt">release</span> patterns and time-intervals among consecutive sizeable earthquakes [1,15]. Anticipated successful training of the imported intelligent systems may result in a real-time, on-line processing methodology [1,16] capable to dynamically approximate the time-interval between the latest and the next forthcoming sizeable seismic event by monitoring the <span class="hlt">energy</span> <span class="hlt">release</span> process in a specific seismogenic area. Indexing terms: pattern recognition, long-term earthquake precursors, neural networks, soft computing, earthquake occurrence intervals References [1] Konstantaras A., Vallianatos F., Varley M.R. and Makris J. P.: ‘Soft computing modelling of seismicity in the southern Hellenic arc', IEEE Geoscience and Remote Sensing Letters, vol. 5 (3), pp. 323-327, 2008 [2] Eneva M. and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994PhLB..328..329P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994PhLB..328..329P"><span><span class="hlt">Deformed</span> coset models from gauged WZW actions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Park, Q.-Han</p> <p>1994-06-01</p> <p>A general Lagrangian formulation of integrably <span class="hlt">deformed</span> G/H-coset models is given. We consider the G/H-coset model in terms of the gauged Wess-Zumino-Witten action and obtain an integrable <span class="hlt">deformation</span> by adding a potential <span class="hlt">energy</span> term Tr(gTg -1overlineT) , where algebra elements T, overlineT belong to the center of the algebra h associated with the subgroup H. We show that the classical equation of motion of the <span class="hlt">deformed</span> coset model can be identified with the integrability condition of certain linear equations which makes the use of the inverse scattering method possible. Using the linear equation, we give a systematic way to construct infinitely many conserved currents as well as soliton solutions. In the case of the parafermionic SU(2)/U(1)-coset model, we derive n-solitons and conserved currents explicitly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23286040','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23286040"><span>Analytic regularization of uniform cubic B-spline <span class="hlt">deformation</span> fields.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shackleford, James A; Yang, Qi; Lourenço, Ana M; Shusharina, Nadya; Kandasamy, Nagarajan; Sharp, Gregory C</p> <p>2012-01-01</p> <p>Image registration is inherently ill-posed, and lacks a unique solution. In the context of medical applications, it is desirable to avoid solutions that describe physically unsound <span class="hlt">deformations</span> within the patient anatomy. Among the accepted methods of regularizing non-rigid image registration to provide solutions applicable to medical practice is the penalty of thin-plate bending <span class="hlt">energy</span>. In this paper, we develop an exact, analytic method for computing the bending <span class="hlt">energy</span> of a three-dimensional B-spline <span class="hlt">deformation</span> field as a quadratic matrix operation on the spline coefficient values. Results presented on ten thoracic case studies indicate the analytic solution is between 61-1371x faster than a numerical central differencing solution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29506108','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29506108"><span>Anterior Longitudinal Ligament <span class="hlt">Release</span> From the Minimally Invasive Lateral Retroperitoneal Transpsoas Approach: Technical Note.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Beckman, Joshua M; Marengo, Nicola; Murray, Gisela; Bach, Konrad; Uribe, Juan S</p> <p>2016-09-01</p> <p>The technique for minimally invasive anterior longitudinal ligament <span class="hlt">release</span> is a major advancement in lateral access surgery. This method provides hypermobility of lumbar segments to allow for aggressive lordosis restoration while maintaining the benefits of indirect decompression and minimally invasive access. To provide video demonstration of the lateral retroperitoneal transpsoas approach with anterior longitudinal ligament sectioning. A detailed surgical technique of the minimally invasive anterior column <span class="hlt">release</span> is described and illustrated in an elderly patient with adult spinal <span class="hlt">deformity</span> and low back pain (visual analog scale, 8 of 10) refractory to conservative measures. The 3-foot standing radiographs demonstrated a lumbar lordosis of 54.4°, pelvic incidence of 63.7°, and pelvic tilt of 17.5°. Computed tomography and magnetic resonance imaging showed generalized lumbar spondylosis and degenerative disc changes from L2 to L5. The patient underwent a multilevel minimally invasive <span class="hlt">deformity</span> correction with an anterior longitudinal ligament <span class="hlt">release</span> at the L3/L4 level through the lateral retroperitoneal transpsoas approach. Lumbar lordosis increased from 54.4° to 77° with a global improvement in sagittal vertical axis from 4.37 cm to 0 cm. Total blood loss was less than 25 mL, and there were no major neurological or vascular complications. The anterior longitudinal ligament <span class="hlt">release</span> using the minimally invasive lateral approach allows for <span class="hlt">deformity</span> correction without the morbidity and blood loss encountered by traditional open posterior approaches. However, the risk of major vascular/visceral complication warrants only experts in minimally invasive lateral surgery to attempt this technique.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhLA..380..327K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhLA..380..327K"><span>Towards classical spectrum generating algebras for f-<span class="hlt">deformations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kullock, Ricardo; Latini, Danilo</p> <p>2016-01-01</p> <p>In this paper we revise the classical analog of f-oscillators, a generalization of q-oscillators given in Man'ko et al. (1997) [8], in the framework of classical spectrum generating algebras (SGA) introduced in Kuru and Negro (2008) [9]. We write down the <span class="hlt">deformed</span> Poisson algebra characterizing the entire family of non-linear oscillators and construct its general solution algebraically. The latter, covering the full range of f-<span class="hlt">deformations</span>, shows an <span class="hlt">energy</span> dependence both in the amplitude and the frequency of the motion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhDT.......345K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhDT.......345K"><span>Atomistic simulations of <span class="hlt">deformation</span> mechanisms in ultralight weight Mg-Li alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Karewar, Shivraj</p> <p></p> <p>Mg alloys have spurred a renewed academic and industrial interest because of their ultra-light-weight and high specific strength properties. Hexagonal close packed Mg has low <span class="hlt">deformability</span> and a high plastic anisotropy between basal and non-basal slip systems at room temperature. Alloying with Li and other elements is believed to counter this deficiency by activating non-basal slip by reducing their nucleation stress. In this work I study how Li addition affects <span class="hlt">deformation</span> mechanisms in Mg using atomistic simulations. In the first part, I create a reliable and transferable concentration dependent embedded atom method (CD-EAM) potential for my molecular dynamics study of <span class="hlt">deformation</span>. This potential describes the Mg-Li phase diagram, which accurately describes the phase stability as a function of Li concentration and temperature. Also, it reproduces the heat of mixing, lattice parameters, and bulk moduli of the alloy as a function of Li concentration. Most importantly, our CD-EAM potential reproduces the variation of stacking fault <span class="hlt">energy</span> for basal, prismatic, and pyramidal slip systems that in uences the <span class="hlt">deformation</span> mechanisms as a function of Li concentration. This success of CD-EAM Mg-Li potential in reproducing different properties, as compared to literature data, shows its reliability and transferability. Next, I use this newly created potential to study the effect of Li addition on <span class="hlt">deformation</span> mechanisms in Mg-Li nanocrystalline (NC) alloys. Mg-Li NC alloys show basal slip, pyramidal type-I slip, tension twinning, and two-compression twinning <span class="hlt">deformation</span> modes. Li addition reduces the plastic anisotropy between basal and non-basal slip systems by modifying the energetics of Mg-Li alloys. This causes the solid solution softening. The inverse relationship between strength and ductility therefore suggests a concomitant increase in alloy ductility. A comparison of the NC results with single crystal <span class="hlt">deformation</span> results helps to understand the qualitative and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DNP.PF003N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DNP.PF003N"><span>Adiabatically describing rare earths using microscopic <span class="hlt">deformations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nobre, Gustavo; Dupuis, Marc; Herman, Michal; Brown, David</p> <p>2017-09-01</p> <p>Recent works showed that reactions on well-<span class="hlt">deformed</span> nuclei in the rare-earth region are very well described by an adiabatic method. This assumes a spherical optical potential (OP) accounting for non-rotational degrees of freedom while the <span class="hlt">deformed</span> configuration is described by couplings to states of the g.s. rotational band. This method has, apart from the global OP, only the <span class="hlt">deformation</span> parameters as inputs, with no additional fit- ted variables. For this reason, it has only been applied to nuclei with well-measured <span class="hlt">deformations</span>. With the new computational capabilities, microscopic large-scale calculations of <span class="hlt">deformation</span> parameters within the HFB method based on the D1S Gogny force are available in the literature. We propose to use such microscopic <span class="hlt">deformations</span> in our adi- abatic method, allowing us to reproduce the cross sections agreements observed in stable nuclei, and to reliably extend this description to nuclei far from stability, describing the whole rare-earth region. Since all cross sections, such as capture and charge exchange, strongly depend on the correct calculation of absorption from the incident channel (from direct reaction mechanisms), this approach significantly improves the accuracy of cross sections and transitions relevant to astrophysical studies. The work at BNL was sponsored by the Office of Nuclear Physics, Office of Science of the US Department of <span class="hlt">Energy</span>, under Contract No. DE-AC02-98CH10886 with Brookhaven Science Associates, LLC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70031123','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70031123"><span>Quantitative models for magma degassing and ground <span class="hlt">deformation</span> (bradyseism) at Campi Flegrei, Italy: Implications for future eruptions</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Bodnar, R.J.; Cannatelli, C.; de Vivo, B.; Lima, A.; Belkin, H.E.; Milia, A.</p> <p>2007-01-01</p> <p>Campi Flegrei (Phlegrean Fields) is an active volcanic center near Naples, Italy. Numerous eruptions have occurred here during the Quaternary, and repeated episodes of slow vertical ground movement (bradyseism) have been documented since Roman times. Here, we present a quantitative model that relates <span class="hlt">deformation</span> episodes to magma degassing and fracturing at the brittle-ductile transition in a magmatic-hydrothermal enviromnent. The model is consistent with field and laboratory observations and predicts that uplift between 1982 and 1984 was associated with crystallization of ???0.83 km3 of H2O-saturated magma at 6 km depth. During crystallization, ???6.2 ?? 1010 kg of H2O and 7.5 ?? 108 kg of CO2, exsolved from the magma and generated ???7 ?? 1015 J of mechanical (P??V) <span class="hlt">energy</span> to drive the observed uplift. For comparison, ???1017 J of thermal <span class="hlt">energy</span> was <span class="hlt">released</span> during the 18 May 1980 lateral blast at Mount St. Helens. ?? 2007 The Geological Society of America.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3946412','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3946412"><span>Noninvasive Fluorescence Resonance <span class="hlt">Energy</span> Transfer Imaging of in vivo Premature Drug <span class="hlt">Release</span> from Polymeric Nanoparticles</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Zou, Peng; Chen, Hongwei; Paholak, Hayley J.; Sun, Duxin</p> <p>2013-01-01</p> <p>Understanding in vivo drug <span class="hlt">release</span> kinetics is critical for the development of nanoparticle-based delivery systems. In this study, we developed a fluorescence resonance <span class="hlt">energy</span> transfer (FRET) imaging approach to noninvasively monitor in vitro and in vivo cargo <span class="hlt">release</span> from polymeric nanoparticles. The FRET donor dye (DiO or DiD) and acceptor dye (DiI or DiR) were individually encapsulated into poly(ethylene oxide)-b-polystyrene (PEO-PS) nanoparticles. When DiO (donor) nanoparticles and DiI (acceptor) nanoparticles were co-incubated with cancer cells for 2 h, increased FRET signals were observed from cell membranes, suggesting rapid <span class="hlt">release</span> of DiO and DiI to cell membranes. Similarly, increased FRET ratios were detected in nude mice after intravenous co-administration of DiD (donor) nanoparticles and DiR (acceptor) nanoparticles. In contrast, another group of nude mice i.v. administrated with DiD/DiR co-loaded nanoparticles showed decreased FRET ratios. Based on the difference in FRET ratios between the two groups, in vivo DiD/DiR <span class="hlt">release</span> half-life from PEO-PS nanoparticles was determined to be 9.2 min. In addition, it was observed that the presence of cell membranes facilitated burst <span class="hlt">release</span> of lipophilic cargos while incorporation of oleic acid-coated iron oxide into PEO-PS nanoparticles slowed the <span class="hlt">release</span> of DiD/DiR to cell membranes. The developed in vitro and in vivo FRET imaging techniques can be used to screening stable nano-formulations for lipophilic drug delivery. PMID:24033270</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29911386','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29911386"><span>New <span class="hlt">Deformation</span>-Induced Nanostructure in Silicon.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Bo; Zhang, Zhenyu; Chang, Keke; Cui, Junfeng; Rosenkranz, Andreas; Yu, Jinhong; Lin, Cheng-Te; Chen, Guoxin; Zang, Ketao; Luo, Jun; Jiang, Nan; Guo, Dongming</p> <p>2018-06-18</p> <p>Nanostructures in silicon (Si) induced by phase transformations have been investigated during the past 50 years. Performances of nanostructures are improved compared to that of bulk counterparts. Nevertheless, the confinement and loading conditions are insufficient to machine and fabricate high-performance devices. As a consequence, nanostructures fabricated by nanoscale <span class="hlt">deformation</span> at loading speeds of m/s have not been demonstrated yet. In this study, grinding or scratching at a speed of 40.2 m/s was performed on a custom-made setup by an especially designed diamond tip (calculated stress under the diamond tip in the order of 5.11 GPa). This leads to a novel approach for the fabrication of nanostructures by nanoscale <span class="hlt">deformation</span> at loading speeds of m/s. A new <span class="hlt">deformation</span>-induced nanostructure was observed by transmission electron microscopy (TEM), consisting of an amorphous phase, a new tetragonal phase, slip bands, twinning superlattices, and a single crystal. The formation mechanism of the new phase was elucidated by ab initio simulations at shear stress of about 2.16 GPa. This approach opens a new route for the fabrication of nanostructures by nanoscale <span class="hlt">deformation</span> at speeds of m/s. Our findings provide new insights for potential applications in transistors, integrated circuits, diodes, solar cells, and <span class="hlt">energy</span> storage systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15...48H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15...48H"><span>Research of dynamical Characteristics of slow <span class="hlt">deformation</span> Waves as Massif Responses on Explosions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hachay, Olga; Khachay, Oleg; Shipeev, Oleg</p> <p>2013-04-01</p> <p>The research of massif state with use of approaches of open system theory [1-3] was developed for investigation the criterions of dissipation regimes for real rock massifs, which are under heavy man-caused influence. For realization of that research we used the data of seismic catalogue of Tashtagol mine. As a result of the analyze of that data we defined character morphology of phase trajectories of massif response, which was locally in time in a stable state: on the phase plane with coordinates <span class="hlt">released</span> by the massif during the dynamic event <span class="hlt">energy</span> E and lg(dE/dt) there is a local area as a ball of twisted trajectories and some not great bursts from that ball, which are not greater than 105 joules. In some time intervals that burst can be larger, than 105 joules, achieving 106 joules and yet 109 joules. [3]. Evidently there are two reciprocal depend processes: the <span class="hlt">energy</span> accumulation in the attracted phase trajectories area and resonance fault of the accumulated <span class="hlt">energy</span>. But after the fault the system returns again to the same attracted phase trajectories area. For analyzing of the thin structure of the chaotic area we decided to add the method of processing of the seismic monitoring data by new parameters. We shall consider each point of explosion as a source of seismic or <span class="hlt">deformation</span> waves. Using the kinematic approach of seismic information processing we shall each point of the massif response use as a time point of the first arrival of the <span class="hlt">deformation</span> wave for calculation of the wave velocity, because additionally we know the coordinates of the fixed response and the coordinates of explosion. The use of additional parameter-velocity of slow <span class="hlt">deformation</span> wave propagation allowed us with use method of phase diagrams identify their hierarchic structure, which allow us to use that information for modeling and interpretation the propagation seismic and <span class="hlt">deformation</span> waves in hierarchic structures. It is researched with use of that suggested processing method the thin</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.eia.gov/consumption/manufacturing/reports/2010/early_estimates.cfm','EIAPUBS'); return false;" href="https://www.eia.gov/consumption/manufacturing/reports/2010/early_estimates.cfm"><span>Early-<span class="hlt">release</span> Estimates From the 2010 MECS Show That <span class="hlt">Energy</span> Consumption In the Manufacturing Sector Decreased Between 2006 and 2010</span></a></p> <p><a target="_blank" href="http://www.eia.doe.gov/reports/">EIA Publications</a></p> <p></p> <p>2012-01-01</p> <p><span class="hlt">Energy</span> consumption in the U.S. manufacturing sector fell from 21,098 trillion Btu (tBtu) in 2006 to 19,062 tBtu in 2010, a decline of almost 10% , based on preliminary estimates <span class="hlt">released</span> from the 2010 Manufacturing <span class="hlt">Energy</span> Consumption Survey (MECS). This decline continues the downward trend in manufacturing <span class="hlt">energy</span> use since the 1998 MECS report.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.T33H..05S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.T33H..05S"><span>Water weakening in experimentally <span class="hlt">deformed</span> milky quartz single crystals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stunitz, H.; Thust, A.; Kilian, R.; Heilbronner, R.; Behrens, H.; Tarantola, A.; Fitz Gerald, J. D.</p> <p>2015-12-01</p> <p>Natural single crystals of quartz have been experimentally <span class="hlt">deformed</span> in two orientations: (1) normal to one prism-plane, (2) In O+ orientation at temperatures of 900 and 1000°C, pressures of 1.0 and 1.5 GPa, and strain rates of ~1 x 10-6s-1. The starting material is milky quartz, consisting of dry quartz (H2O contents of <150 H/106Si) with fluid inclusions (FI). During pressurization many FI´s decrepitate. Cracks heal and small neonate FI´s form, increasing the number of FI´s drastically. During subsequent <span class="hlt">deformation</span>, the size of FI´s is further reduced (down to ~10 nm). Sample <span class="hlt">deformation</span> occurs by dominant dislocation glide on selected slip systems, accompanied by some dynamic recovery. Strongly <span class="hlt">deformed</span> regions show FTIR spectra with a pointed broad absorption band in the ~3400 cm-1 region as a superposition of molecular H2O bands and three discrete absorption bands (at 3367, 3400, and 3434 cm-1). In addition, there is a discrete absorption band at 3585 cm-1, which only occurs in <span class="hlt">deformed</span> regions. The 3585 cm-1 band is reduced or even disappears after annealing. This band is polarized and represents structurally bound H, its H-content is estimated to be 1-3% of the total H2O-content and appears to be associated with dislocations. The H2O weakening effect in our FI-bearing natural quartz crystals is assigned to the processes of dislocation generation and multiplication at small FI´s. The <span class="hlt">deformation</span> processes in these crystals represent a recycling of H2O between FI´s, dislocation generation at very small fluid inclusions, incorporation of structurally bound H into dislocation cores, and <span class="hlt">release</span> of H2O from dislocations back into FI´s during recovery. Cracking and crack healing play an important role in the recycling process and imply a close interrelationship between brittle and crystal plastic <span class="hlt">deformation</span>. The H2O weakening by this process is of a disequilibrium nature and thus depends on the amount of H2O available.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10173E..1RD','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10173E..1RD"><span>Influences of thermal <span class="hlt">deformation</span> of cavity mirrors induced by high <span class="hlt">energy</span> DF laser to beam quality under the simulated real physical circumstances</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Deng, Shaoyong; Zhang, Shiqiang; He, Minbo; Zhang, Zheng; Guan, Xiaowei</p> <p>2017-05-01</p> <p>The positive-branch confocal unstable resonator with inhomogeneous gain medium was studied for the normal used high <span class="hlt">energy</span> DF laser system. The fast changing process of the resonator's eigenmodes was coupled with the slow changing process of the thermal <span class="hlt">deformation</span> of cavity mirrors. Influences of the thermal <span class="hlt">deformation</span> of cavity mirrors to the outcoupled beam quality and transmission loss of high frequency components of high <span class="hlt">energy</span> laser were computed. The simulations are done through programs compiled by MATLAB and GLAD software and the method of combination of finite elements and Fox-li iteration algorithm was used. Effects of thermal distortion, misaligned of cavity mirrors and inhomogeneous distribution of gain medium were introduced to simulate the real physical circumstances of laser cavity. The wavefront distribution and beam quality (including RMS of wavefront, power in the bucket, Strehl ratio, diffraction limit β, position of the beam spot center, spot size and intensity distribution in far-field ) of the distorted outcoupled beam were studied. The conclusions of the simulation agree with the experimental results. This work would supply references of wavefront correction range to the adaptive optics system of interior alleyway.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016enma.book..473F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016enma.book..473F"><span>Hot <span class="hlt">deformation</span> constitutive equation and processing map of Alloy 690</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Feng, Han; Zhang, Songchuang; Ma, Mingjuan; Song, Zhigang</p> <p></p> <p>The hot <span class="hlt">deformation</span> behavior of alloy 690 was studied in the temperature range of 800-1300 C and strain rate range of 0.1-10 s-1 by hot compression tests in a Gleeble 1500+ thermal mechanical simulator. The results indicated that flow stress of alloy 690 is sensitive to <span class="hlt">deformation</span> temperature and strain rate and peak stress increases with decreasing of temperature and increasing of strain rate. In addition, the hot <span class="hlt">deformation</span> parameters of <span class="hlt">deformation</span> activation were calculated and the apparent activation <span class="hlt">energy</span> of this alloy is about 300 kJ/mol. The constitutive equation which can be used to relate peak stress to the absolute temperature and strain rate was obtained. It's further found that the processing maps exhibited two domains which are considered as the optimum windows for hot working. The microstructure observations of the specimens <span class="hlt">deformed</span> in this domain showed the full dynamic recrystallization (DRX) structure. There was a flow instability domain in the processing map where hot working should be avoided.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1339442-situ-high-energy-ray-diffraction-study-tensile-deformation-neutron-irradiated-polycrystalline-fe-cr-alloy','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1339442-situ-high-energy-ray-diffraction-study-tensile-deformation-neutron-irradiated-polycrystalline-fe-cr-alloy"><span>In situ high-<span class="hlt">energy</span> X-ray diffraction study of tensile <span class="hlt">deformation</span> of neutron-irradiated polycrystalline Fe-9%Cr alloy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Zhang, Xuan; Li, Meimei; Park, Jun -Sang; ...</p> <p>2016-12-30</p> <p>The effect of neutron irradiation on tensile <span class="hlt">deformation</span> of a Fe-9wt.%Cr alloy was investigated using in situ high-<span class="hlt">energy</span> synchrotron X-ray diffraction during room-temperature uniaxial tensile tests. New insights into the <span class="hlt">deformation</span> mechanisms were obtained through the measurements of lattice strain evolution and the analysis of diffraction peak broadening using the modified Williamson-Hall method. Two neutron-irradiated specimens, one irradiated at 300 °C to 0.01 dpa and the other at 450 °C to 0.01dpa, were tested along with an unirradiated specimen. The macroscopic stress–strain curves of the irradiated specimens showed increased strength, reduced ductility and work-hardening exponent compared to the unirradiated specimen.more » The evolutions of the lattice strain, the dislocation density and the coherent scattering domain size in the <span class="hlt">deformation</span> process revealed different roles of the submicroscopic defects in the 300°C/0.01 dpa specimen and the TEM-visible nanometer-sized dislocation loops in the 450°C/0.01 dpa specimen: submicroscopic defects extended the linear work hardening stage (stage II) to a higher strain, while irradiation-induced dislocation loops were more effective in dislocation pinning. Lastly, while the work hardening rate of stage II was unaffected by irradiation, significant dynamic recovery in stage III in the irradiated specimens led to the early onset of necking without stage IV as observed in the unirradiated specimen.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/10904900','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/10904900"><span>The effect of soft tissue <span class="hlt">release</span> of the hips on walking in myelomeningocele.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Correll, J; Gabler, C</p> <p>2000-06-01</p> <p>Walking and standing capacity in myelomeningocele is highly dependent on the level of the neurological lesion. <span class="hlt">Deformities</span>, mainly flexion <span class="hlt">deformities</span>, of the hip can severely interfere with mobility. In a retrospective study, undertaken in our hospital, we evaluated the role of soft tissue <span class="hlt">release</span> of the hip in patients with hip flexion contractures. A special surgical technique was performed in 55 hips. The results show a good effect on verticalization, even if the hip joints cannot be extended actively. A subluxated or dislocated hip did not influence the final outcome. During the mean follow-up of approximately 4 years, only a slight recurrence of the former <span class="hlt">deformity</span> was observed. Most of the patients obtained great advantage from the operation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19486628','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19486628"><span>Chevron osteotomy with lateral <span class="hlt">release</span> and adductor tenotomy for hallux valgus.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Potenza, Vito; Caterini, Roberto; Farsetti, Pasquale; Forconi, Fabrizio; Savarese, Eugenio; Nicoletti, Simone; Ippolito, Ernesto</p> <p>2009-06-01</p> <p>Distal chevron osteotomy is a procedure widely performed for the surgical treatment of painful hallux valgus. The risks and benefits of a lateral capsular <span class="hlt">release</span> and adductor tenotomy combined with chevron osteotomy are still debated. The aim of our study was to report the clinical and radiographic outcomes of this combined procedure in mild and moderate incongruent bunion <span class="hlt">deformities</span>, with a hallux valgus angle (HVA) up to 40 degrees and an intermetatarsal angle (IMA) up to 20 degrees. Forty-two patients (52 feet) who consecutively underwent chevron osteotomy combined with lateral <span class="hlt">release</span> and adductor tenotomy were reviewed 24-36 months after surgery. The mean age of the patients was 53.5 (range, 43 to 64) years. All the <span class="hlt">deformities</span> were mild to moderate, with a mean preoperative value of 28 degrees in the HVA (range, 16 degrees to 40 degrees) and of 13 degrees in the IMA (range, 9 degrees to 20 degrees). At followup, the AOFAS hallux score improved from an average of 46 to an average of 88. The HVA and IMA had an average postoperative decrease respectively of 12 degrees and 6 degrees; lateral sesamoid displacement decreased by a mean of 15%. In no case did we observe infection or nonunion of the osteotomy. In one case, painless avascular necrosis of the first metatarsal head developed. Our short-term results show that distal chevron osteotomy combined with lateral <span class="hlt">release</span> and adductor tenotomy is a feasible surgical option to address mild to moderate hallux valgus <span class="hlt">deformity</span>, even with an IM angle between 15 and 20 degrees. Clinical and radiographic outcomes are generally good and patient satisfaction is generally high.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3918705','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3918705"><span>Left Ventricular Endocardium Tracking by Fusion of Biomechanical and <span class="hlt">Deformable</span> Models</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gu, Jason</p> <p>2014-01-01</p> <p>This paper presents a framework for tracking left ventricular (LV) endocardium through 2D echocardiography image sequence. The framework is based on fusion of biomechanical (BM) model of the heart with the parametric <span class="hlt">deformable</span> model. The BM model constitutive equation consists of passive and active strain <span class="hlt">energy</span> functions. The <span class="hlt">deformations</span> of the LV are obtained by solving the constitutive equations using ABAQUS FEM in each frame in the cardiac cycle. The strain <span class="hlt">energy</span> functions are defined in two user subroutines for active and passive phases. Average fusion technique is used to fuse the BM and <span class="hlt">deformable</span> model contours. Experimental results are conducted to verify the detected contours and the results are evaluated by comparing themto a created gold standard. The results and the evaluation proved that the framework has the tremendous potential to track and segment the LV through the whole cardiac cycle. PMID:24587814</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10163E..24L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10163E..24L"><span><span class="hlt">Deformation</span> behavior of carbon-fiber reinforced shape-memory-polymer composites used for deployable structures (Conference Presentation)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lan, Xin; Liu, Liwu; Li, Fengfeng; Pan, Chengtong; Liu, Yanju; Leng, Jinsong</p> <p>2017-04-01</p> <p>Shape memory polymers (SMPs) are a new type of smart material, they perform large reversible <span class="hlt">deformation</span> with a certain external stimulus (e.g., heat and electricity). The properties (e.g., stiffness, strength and other mechanically static or quasi-static load-bearing capacity) are primarily considered for conventional resin-based composite materials which are mainly used for structural materials. By contrast, the mechanical actuating performance with finite <span class="hlt">deformation</span> is considered for the shape memory polymers and their composites which can be used for both structural materials and functional materials. For shape memory polymers and their composites, the performance of active <span class="hlt">deformation</span> is expected to further promote the development in smart active <span class="hlt">deformation</span> structures, such as deployable space structures and morphing wing aircraft. The shape memory polymer composites (SMPCs) are also one type of High Strain Composite (HSC). The space deployable structures based on carbon fiber reinforced shape memory polymer composites (SMPCs) show great prospects. Considering the problems that SMPCs are difficult to meet the practical applications in space deployable structures in the recent ten years, this paper aims to research the mechanics of <span class="hlt">deformation</span>, actuation and failure of SMPCs. In the overall view of the shape memory polymer material's nonlinearity (nonlinearity and stress softening in the process of pre-<span class="hlt">deformation</span> and recovery, relaxation in storage process, irreversible <span class="hlt">deformation</span>), by the multiple verifications among theory, finite element and experiments, one obtains the <span class="hlt">deformation</span> and actuation mechanism for the process of "pre-<span class="hlt">deformation</span>, <span class="hlt">energy</span> storage and actuation" and its non-fracture constraint domain. Then, the parameters of SMPCs will be optimized. Theoretical analysis is realized by the strain <span class="hlt">energy</span> function, additionally considering the interaction strain <span class="hlt">energy</span> between the fiber and the matrix. For the common resin-based or soft</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A41F2363C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A41F2363C"><span>Advancing Knowledge on Fugitive Natural Gas from <span class="hlt">Energy</span> Resource Development at a Controlled <span class="hlt">Release</span> Field Observatory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cahill, A. G.; Chao, J.; Forde, O.; Prystupa, E.; Mayer, K. U.; Black, T. A.; Tannant, D. D.; Crowe, S.; Hallam, S.; Mayer, B.; Lauer, R. M.; van Geloven, C.; Welch, L. A.; Salas, C.; Levson, V.; Risk, D. A.; Beckie, R. D.</p> <p>2017-12-01</p> <p>Fugitive gas, comprised primarily of methane, can be unintentionally <span class="hlt">released</span> from upstream oil and gas development either at surface from leaky infrastructure or in the subsurface through failure of <span class="hlt">energy</span> well bore integrity. For the latter, defective cement seals around <span class="hlt">energy</span> well casings may permit buoyant flow of natural gas from the deeper subsurface towards shallow aquifers, the ground surface and potentially into the atmosphere. Concerns associated with fugitive gas <span class="hlt">release</span> at surface and in the subsurface include contributions to greenhouse gas emissions, subsurface migration leading to accumulation in nearby infrastructure and impacts to groundwater quality. Current knowledge of the extent of fugitive gas leakage including how to best detect and monitor over time, and particularly its migration and fate in the subsurface, is incomplete. We have established an experimental field observatory for evaluating fugitive gas leakage in an area of historic and ongoing hydrocarbon resource development within the Montney Resource Play of the Western Canadian Sedimentary Basin, British Columbia, Canada. Natural gas will be intentionally <span class="hlt">released</span> at surface and up to 25 m below surface at various rates and durations. Resulting migration patterns and impacts will be evaluated through examination of the geology, hydrogeology, hydro-geochemistry, isotope geochemistry, hydro-geophysics, vadose zone and soil gas processes, microbiology, and atmospheric conditions. The use of unmanned aerial vehicles and remote sensors for monitoring and detection of methane will also be assessed for suitability as environmental monitoring tools. Here we outline the experimental design and describe initial research conducted to develop a detailed site conceptual model of the field observatory. Subsequently, results attained from pilot surface and sub-surface controlled natural gas <span class="hlt">releases</span> conducted in late summer 2017 will be presented as well as results of numerical modelling conducted</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15.3310H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15.3310H"><span>Coupled <span class="hlt">deformation</span> and dehydration processes in smectite-rich sediments constrained by laboratory experiments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Huepers, Andre; Kopf, Achim J.</p> <p>2013-04-01</p> <p>Subduction zones play a central role in the geological activity of the earth which is expressed as devastating events such as earthquakes, tsunamis and explosive volcanism. Many processes that lead to such catastrophic behavior are driven by fluids, which in turn affect the rock mechanical behavior. The kinetic reaction of hydrous smectite to illite is widely accepted as a fluid source in subduction zone forearcs that also affects the mechanical state of subduction zone sediments. The <span class="hlt">released</span> fluids are characterized by low-chlorinity and high volatile content. Also, previous workers demonstrated in uniaxial <span class="hlt">deformation</span> tests that smectite partially dehydrates with increasing effective stress. To shed light on this process we performed uniaxial <span class="hlt">deformation</span> experiments on smectite-rich samples from the Nankai and Costa Rica subduction zones. Experiments were conducted at temperatures of up to 100°C under constant rate of strain and effective stresses of up to ~100MPa. Fluids expelled during the experiments were analyzed for major and minor element content. The fluids are characterized by fluid-freshening and increasing volatile content that starts at ~1.3MPa effective stress. During the course of the experiments the smectite interlayer water content decreases from 27 wt-% to 20 wt-%. The <span class="hlt">released</span> interlayer water comprises up to 17% of the total fluid volume <span class="hlt">released</span> from the consolidating sediment. The onset of fluid freshening is characterized by a change in <span class="hlt">deformation</span> behavior of the samples. The porosity decrease with increasing effective stress is smaller at effective stresses greater 1.3MPa. We propose that dehydration of the low permeable smectite leads to excess pore pressures in the sample, which causes a load transfer from the solid phase to the pore fluid.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.nrel.gov/news/press/1996/','SCIGOVWS'); return false;" href="https://www.nrel.gov/news/press/1996/"><span>1996 News <span class="hlt">Releases</span> | NREL</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p>6 News <span class="hlt">Releases</span> Access news stories about the laboratory and renewable <em><span class="hlt">energy</span></em> and <em><span class="hlt">energy</span></em> efficiency Facility Slashes <em><span class="hlt">Energy</span></em> Use by 66 Percent - (10/3/96) Agreement Moves Nevada Solar Plant Step Closer to Converter Wins National Award - (7/25/96) Solar <em><span class="hlt">Energy</span></em> to Help Heat Major Commercial Facility - (6/21/96</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.G31A0947P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.G31A0947P"><span>Global synthesis of volcano <span class="hlt">deformation</span>: Results of the Volcano <span class="hlt">Deformation</span> Task Force</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pritchard, M. E.; Jay, J.; Biggs, J.; Ebmeier, S. K.; Delgado, F.</p> <p>2013-12-01</p> <p>Ground <span class="hlt">deformation</span> in volcanic regions is being observed more frequently -- the number of known <span class="hlt">deforming</span> volcanoes has increased from 44 in 1997 to more than 210 in 2013 thanks in large part thanks to the availability of satellite InSAR observations. With the launch of new SAR satellites in the coming years devoted to global <span class="hlt">deformation</span> monitoring, the number of well-studied episodes of volcano <span class="hlt">deformation</span> will continue to increase. But evaluating the significance of the observed <span class="hlt">deformation</span> is not always straightforward -- how often do <span class="hlt">deformation</span> episodes lead to eruption? Are there certain characteristics of the <span class="hlt">deformation</span> or the volcano that make the linkage between <span class="hlt">deformation</span> and eruption more robust -- for example the duration or magnitude of the ground <span class="hlt">deformation</span> and/or the composition and tectonic setting of the volcano? To answer these questions, a global database of volcano <span class="hlt">deformation</span> events is needed. Recognizing the need for global information on volcano <span class="hlt">deformation</span> and the opportunity to address it with InSAR and other techniques, we formed the Volcano <span class="hlt">Deformation</span> Database Task force as part of Global Volcano Model. The three objectives of our organization are: 1) to compile <span class="hlt">deformation</span> observations of all volcanoes globally into appropriate formats for WOVOdat and the Global Volcanism Program of the Smithsonian Institution. 2) document any relation between <span class="hlt">deformation</span> events and eruptions for the Global assessment of volcanic hazard and risk report for 2015 (GAR15) for the UN. 3) to better link InSAR and other remote sensing observations to volcano observatories. We present the first results from our global study of the relation between <span class="hlt">deformation</span> and eruptions, including case studies of particular eruptions. We compile a systematically-observed catalog of >500 volcanoes with observation windows up to 20 years. Of 90 volcanoes showing <span class="hlt">deformation</span>, 40 erupted. The positive predictive value (PPV = 0.44) linking <span class="hlt">deformation</span> and eruption on this</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JPhB...46x5201R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JPhB...46x5201R"><span>Ion-polycyclic aromatic hydrocarbon collisions: kinetic <span class="hlt">energy</span> <span class="hlt">releases</span> for specific fragmentation channels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reitsma, G.; Zettergren, H.; Boschman, L.; Bodewits, E.; Hoekstra, R.; Schlathölter, T.</p> <p>2013-12-01</p> <p>We report on 30 keV He2 + collisions with naphthalene (C10H8) molecules, which leads to very extensive fragmentation. To unravel such complex fragmentation patterns, we designed and constructed an experimental setup, which allows for the determination of the full momentum vector by measuring charged collision products in coincidence in a recoil ion momentum spectrometer type of detection scheme. The determination of fragment kinetic <span class="hlt">energies</span> is found to be considerably more accurate than for the case of mere coincidence time-of-flight spectrometers. In fission reactions involving two cationic fragments, typically kinetic <span class="hlt">energy</span> <span class="hlt">releases</span> of 2-3 eV are observed. The results are interpreted by means of density functional theory calculations of the reverse barriers. It is concluded that naphthalene fragmentation by collisions with keV ions clearly is much more violent than the corresponding photofragmentation with energetic photons. The ion-induced naphthalene fragmentation provides a feedstock of various small hydrocarbonic species of different charge states and kinetic <span class="hlt">energy</span>, which could influence several molecule formation processes in the cold interstellar medium and facilitates growth of small hydrocarbon species on pre-existing polycyclic aromatic hydrocarbons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1185851-universal-mechanism-thermo-mechanical-deformation-metallic-glasses','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1185851-universal-mechanism-thermo-mechanical-deformation-metallic-glasses"><span>Universal mechanism of thermo-mechanical <span class="hlt">deformation</span> in metallic glasses</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Dmowski, W.; Tong, Y.; Iwashita, T.; ...</p> <p>2015-02-11</p> <p>Here we investigated the atomistic structure of metallic glasses subjected to thermo-mechanical creep <span class="hlt">deformation</span> using high <span class="hlt">energy</span> x-ray diffraction and molecular dynamics simulation. The experiments were performed in-situ, at high temperatures as a time dependent <span class="hlt">deformation</span> in the elastic regime, and ex-situ on samples quenched under stress. We show that all the anisotropic structure functions of the samples undergone thermo-mechanical creep can be scaled into a single curve, regardless of the magnitude of anelastic strain, stress level and the sign of the stress, demonstrating universal behavior and pointing to unique atomistic unit of anelastic <span class="hlt">deformation</span>. The structural changes due tomore » creep are strongly localized within the second nearest neighbors, involving only a small group of atoms.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008epsc.conf..545V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008epsc.conf..545V"><span>Experimental high strain-rate <span class="hlt">deformation</span> products of carbonate-silicate rocks: Comparison with terrestrial impact materials</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van der Bogert, C. H.; Schultz, P. H.; Spray, J. G.</p> <p>2008-09-01</p> <p> similar in many aspects to impact products at terrestrial craters in mixed carbonate-silicate targets. The experiments show that decarbonation of carbonate targets and high temperature reactions between carbonate and silicates in the target rocks are not exclusive effects of shock <span class="hlt">deformation</span>. Shear <span class="hlt">deformation</span> alone can generate temperature and pressure conditions necessary to decarbonate dolomitic marble and generate calcitic melts. Thus, high strain-rate <span class="hlt">deformation</span> is a potentially major contributor to the total impact-related <span class="hlt">energy</span> deposited into the target, especially for oblique impacts. Shear <span class="hlt">deformation</span> occuring during and after shock <span class="hlt">deformation</span> could, in fact, enhance the <span class="hlt">release</span> of CO2 as a gas, by creating pathways that allow gases to escape from target materials. Understanding the relative importance and interaction of each CO2 <span class="hlt">releasing</span> or trapping mechanism is important for the determination of the environmental significance of impacts in targets containing carbonates. References. [1] Lange M. A. and Ahrens T. J. (1986) EPSL 77, 409-418. [2] Tyburczy J. A. and Ahrens T. J. (1986) JGR 91, 4730-4744. [3] Schultz P. H. (1996) GSA Abstracts, A384. [4] Agrinier P., et al. (2001) GCA 65, 2615-2632. [5] Spray J. G. (1995) Geology 23, 1119-1122. [6] van der Bogert C. H., et al. (2007) LPI Contribution No. 1360, 123-124. [7] Martinez I., et al. (1995) JGR 100, 15456-15476. [8] Ivanov B. A. and Deutsch A. (2002) Phys. Earth Planet. Int. 129, 131-143. [9] Martinez I., et al. (1994) EPSL 121, 559-574. [10] Redeker H.-J. and Stöffler D. (1988) Meteoritics 23, 185-196. [11] Skála R. and Jakes P. (1999). In Large Meteorite Impacts and Planetary Evolution II (eds. B. O. Dressler and V. L. Sharpton), pp. 205-214. [12] Osinski G. R. and Spray J. G. (2001) EPSL 194, 17-29. [13] Kenkmann T., et al. (1999) LPS XXX, Abstract #1561.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4471887','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4471887"><span>Mechanical Failure Mode of Metal Nanowires: Global <span class="hlt">Deformation</span> versus Local <span class="hlt">Deformation</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ho, Duc Tam; Im, Youngtae; Kwon, Soon-Yong; Earmme, Youn Young; Kim, Sung Youb</p> <p>2015-01-01</p> <p>It is believed that the failure mode of metal nanowires under tensile loading is the result of the nucleation and propagation of dislocations. Such failure modes can be slip, partial slip or twinning and therefore they are regarded as local <span class="hlt">deformation</span>. Here we provide numerical and theoretical evidences to show that global <span class="hlt">deformation</span> is another predominant failure mode of nanowires under tensile loading. At the global <span class="hlt">deformation</span> mode, nanowires fail with a large contraction along a lateral direction and a large expansion along the other lateral direction. In addition, there is a competition between global and local <span class="hlt">deformations</span>. Nanowires loaded at low temperature exhibit global failure mode first and then local <span class="hlt">deformation</span> follows later. We show that the global <span class="hlt">deformation</span> originates from the intrinsic instability of the nanowires and that temperature is a main parameter that decides the global or local <span class="hlt">deformation</span> as the failure mode of nanowires. PMID:26087445</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JMPSo..61.1877L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JMPSo..61.1877L"><span>A model for finite-<span class="hlt">deformation</span> nonlinear thermomechanical response of single crystal copper under shock conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luscher, Darby J.; Bronkhorst, Curt A.; Alleman, Coleman N.; Addessio, Francis L.</p> <p>2013-09-01</p> <p>A physically consistent framework for combining pressure-volume-temperature equations of state with crystal plasticity models is developed for the application of modeling the response of single and polycrystals under shock conditions. The particular model is developed for copper, thus the approach focuses on crystals of cubic symmetry although many of the concepts in the approach are applicable to crystals of lower symmetry. We employ a multiplicative decomposition of the <span class="hlt">deformation</span> gradient into isochoric elastic, thermoelastic dilation, and plastic parts leading to a definition of isochoric elastic Green-Lagrange strain. This finite <span class="hlt">deformation</span> kinematic decomposition enables a decomposition of Helmholtz free-<span class="hlt">energy</span> into terms reflecting dilatational thermoelasticity, strain <span class="hlt">energy</span> due to long-range isochoric elastic <span class="hlt">deformation</span> of the lattice and a term reflecting <span class="hlt">energy</span> stored in short range elastic lattice <span class="hlt">deformation</span> due to evolving defect structures. A model for the single crystal response of copper is implemented consistent with the framework into a three-dimensional Lagrangian finite element code. Simulations exhibit favorable agreement with single and bicrystal experimental data for shock pressures ranging from 3 to 110 GPa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28948693','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28948693"><span>DNA Microcapsule for Photo-Triggered Drug <span class="hlt">Release</span> Systems.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kamiya, Yukiko; Yamada, Yoshinobu; Muro, Takahiro; Matsuura, Kazunori; Asanuma, Hiroyuki</p> <p>2017-12-19</p> <p>In this study we constructed spherical photo-responsive microcapsules composed of three photo-switchable DNA strands. These strands first formed a three-way junction (TWJ) motif that further self-assembled to form microspheres through hybridization of the sticky-end regions of each branch. To serve as the photo-switch, multiple unmodified azobenzene (Azo) or 2,6-dimethyl-4-(methylthio)azobenzene (SDM-Azo) were introduced into the sticky-end regions via a d-threoninol linker. The DNA capsule structure <span class="hlt">deformed</span> upon trans-to-cis isomerization of Azo or SDM-Azo induced by specific light irradiation. In addition, photo-triggered <span class="hlt">release</span> of encapsulated small molecules from the DNA microcapsule was successfully achieved. Moreover, we demonstrated that photo-triggered <span class="hlt">release</span> of doxorubicin caused cytotoxicity to cultured cells. This biocompatible photo-responsive microcapsule has potential application as a photo-controlled drug-<span class="hlt">release</span> system. © 2017 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740015127&hterms=OLT&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DOLT','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740015127&hterms=OLT&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DOLT"><span>The effect of ultrasonics on the strength properties of carbon steel processed by cold plastic <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Atanasiu, N.; Dragan, O.; Atanasiu, Z.</p> <p>1974-01-01</p> <p>A study was made of the influence of ultrasounds on the mechanical properties of OLT 35 carbon steel tubes cold-drawn on a plug ultrasonically activated by longitudinal waves. Experimental results indicate that: 1. The reduction in the values of the flow limit and tensile strength is proportional to the increase in acoustic <span class="hlt">energy</span> introduced into the material subjected to <span class="hlt">deformation</span>. 2. The diminution in influence of ultrasounds on tensile strength and flow rate that is due to an increased degree of <span class="hlt">deformation</span> is explained by a reduction in specific density of the acoustic <span class="hlt">energy</span> at the focus of <span class="hlt">deformation</span>. 3. The relations calculated on the basis of the variation in the flow limit and tensile strength as a function of acoustic <span class="hlt">energy</span> intensity was verified experimentally.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21251711','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21251711"><span>Intracellularly monitoring/imaging the <span class="hlt">release</span> of doxorubicin from pH-responsive nanoparticles using Förster resonance <span class="hlt">energy</span> transfer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Ko-Jie; Chiu, Ya-Ling; Chen, Yu-Ming; Ho, Yi-Cheng; Sung, Hsing-Wen</p> <p>2011-04-01</p> <p>Stimuli-responsive nanoparticles (NPs) have been receiving much attention as a drug-delivery vehicle for therapeutic applications; once internalized into cells, the intracellular fate of NPs and their drug <span class="hlt">release</span> behavior in response to local stimuli must be understood for efficient delivery of therapeutics. In this study, we prepared pH-responsive doxorubicin (DOX)-loaded NPs, made of N-palmitoyl chitosan bearing a Cy5 moiety (Cy5-NPCS), as an anticancer delivery device. The results of our molecular dynamic simulations showed that the ability of Cy5-NPCS to self-associate offered the close proximity between the donor (DOX) and the acceptor (Cy5) required for Förster resonance <span class="hlt">energy</span> transfer (FRET), while the pH-driven structure transition prescribed the on-to-off switch of the <span class="hlt">energy</span> transfer. The caveolae-mediated pathway played a major role in the internalization of NPCS NPs. Using the concept of FRET, we found that the DOX fluorescence in the cytosol was first seen when NPCS NPs were present in the slightly acidic early endosomes. Following NPCS NPs trafficking into a more acidic organelle (late endosomes/lysosomes), a more evident <span class="hlt">release</span> of DOX into the cytosol was observed; the <span class="hlt">released</span> DOX was then gradually accumulated in the cell nuclei, leading to a significant cytotoxicity. Understanding the fate of NPs with respect to their intracellular localization and drug <span class="hlt">release</span> behavior is crucial for the rational design of drug carriers. Copyright © 2010 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ApPhL.107i1901J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ApPhL.107i1901J"><span>Formation of incoherent <span class="hlt">deformation</span> twin boundaries in a coarse-grained Al-7Mg alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jin, S. B.; Zhang, K.; Bjørge, R.; Tao, N. R.; Marthinsen, K.; Lu, K.; Li, Y. J.</p> <p>2015-08-01</p> <p><span class="hlt">Deformation</span> twinning has rarely been observed in coarse grained Al and its alloys except under some extreme conditions such as ultrahigh <span class="hlt">deformation</span> strain or strain rates. Here, we report that a significant amount of Σ3 <span class="hlt">deformation</span> twins could be generated in a coarse-grained Al-7 Mg alloy by dynamic plastic <span class="hlt">deformation</span> (DPD). A systematic investigation of the Σ3 boundaries shows that they are Σ3{112} type incoherent twin boundaries (ITBs). These ITBs have formed by gradual evolution from copious low-angle <span class="hlt">deformation</span> bands through <111>-twist Σ boundaries by lattice rotation. These findings provide an approach to generate <span class="hlt">deformation</span> twin boundaries in high stacking fault <span class="hlt">energy</span> metallic alloys. It is suggested that high solution content of Mg in the alloy and the special <span class="hlt">deformation</span> mode of DPD played an important role in formation of the Σ and ITBs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9302E..2XL','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9302E..2XL"><span><span class="hlt">Deformation</span> measurement for a rotating <span class="hlt">deformable</span> lap based on inverse fringe projection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liao, Min; Zhang, Qican</p> <p>2015-03-01</p> <p>The active <span class="hlt">deformable</span> lap (also namely stressed lap) is an efficient polishing tool in optical manufacturing. To measure the dynamic <span class="hlt">deformation</span> caused by outside force on a <span class="hlt">deformable</span> lap is important and helpful to the opticians to ensure the performance of a <span class="hlt">deformable</span> lap as expected. In this paper, a manual <span class="hlt">deformable</span> lap was designed to simulate the dynamic <span class="hlt">deformation</span> of an active stressed lap, and a measurement system was developed based on inverse projected fringe technique to restore the 3D shape. A redesigned inverse fringe has been projected onto the surface of the measured lap, and the <span class="hlt">deformations</span> of the tested lap become much obvious and can be easily and quickly evaluated by Fourier fringe analysis. Compared with the conventional projection, this technique is more obvious, and it should be a promising one in the <span class="hlt">deformation</span> measurement of the active stressed lap in optical manufacturing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JAP...117h5901G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JAP...117h5901G"><span>Morphological changes in polycrystalline Fe after compression and <span class="hlt">release</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gunkelmann, Nina; Tramontina, Diego R.; Bringa, Eduardo M.; Urbassek, Herbert M.</p> <p>2015-02-01</p> <p>Despite a number of large-scale molecular dynamics simulations of shock compressed iron, the morphological properties of simulated recovered samples are still unexplored. Key questions remain open in this area, including the role of dislocation motion and <span class="hlt">deformation</span> twinning in shear stress <span class="hlt">release</span>. In this study, we present simulations of homogeneous uniaxial compression and recovery of large polycrystalline iron samples. Our results reveal significant recovery of the body-centered cubic grains with some <span class="hlt">deformation</span> twinning driven by shear stress, in agreement with experimental results by Wang et al. [Sci. Rep. 3, 1086 (2013)]. The twin fraction agrees reasonably well with a semi-analytical model which assumes a critical shear stress for twinning. On reloading, twins disappear and the material reaches a very low strength value.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018IzPSE..54...22K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018IzPSE..54...22K"><span>Revealing the <span class="hlt">deformational</span> anomalies based on GNSS data in relation to the preparation and stress <span class="hlt">release</span> of large earthquakes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kaftan, V. I.; Melnikov, A. Yu.</p> <p>2018-01-01</p> <p>The results of Global Navigational Satellite System (GNSS) observations in the regions of large earthquakes are analyzed. The characteristics of the Earth's surface <span class="hlt">deformations</span> before, during, and after the earthquakes are considered. The obtained results demonstrate the presence of anomalous <span class="hlt">deformations</span> close to the epicenters of the events. Statistical estimates of the anomalous strains and their relationship with measurement errors are obtained. Conclusions are drawn about the probable use of local GNSS networks to assess the risk of the occurrence of strong seismic events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5315037-high-temperature-deformation-stoichiometric-sup-puo-sub','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5315037-high-temperature-deformation-stoichiometric-sup-puo-sub"><span>High-temperature <span class="hlt">deformation</span> of stoichiometric /sup 239/PuO/sub 2/</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Petrovic, J.J.; Land, C.C.</p> <p>1980-03-01</p> <p>The <span class="hlt">deformation</span> behavior of stoichiometric /sup 239/PuO/sub 2/ was examined at 800/sup 0/ to 1500/sup 0/C, using direct and diametral compression. Maximum ductility was observed at 1000/sup 0/C, but above this temperature both strength and ductility decreased and the fracture mode changed from transgranular to intergranular. The <span class="hlt">deformation</span> activation <span class="hlt">energy</span> measured at 1000/sup 0/C was 598 kJ/mol. Comparison to the <span class="hlt">deformation</span> behavior of hypostoichiometric /sup 239/PuO/sub 2-x/ suggests that high-temperature dislocation motion becomes more difficult with increasing O/Pu ratio due to effects of stoichiometry on diffusion rates. <span class="hlt">Deformation</span> mechanisms in /sup 239/PuO/sub 2/ appear to be a combination of dislocationmore » motion and grain-boundary sliding.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18160500','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18160500"><span>The incidence and treatment of rocker bottom <span class="hlt">deformity</span> as a complication of the conservative treatment of idiopathic congenital clubfoot.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Koureas, G; Rampal, V; Mascard, E; Seringe, R; Wicart, P</p> <p>2008-01-01</p> <p>Rocker bottom <span class="hlt">deformity</span> may occur during the conservative treatment of idiopathic congenital clubfoot. Between 1975 and 1996, we treated 715 patients (1120 clubfeet) conservatively. A total of 23 patients (36 feet; 3.2%) developed a rocker bottom <span class="hlt">deformity</span>. It is these patients that we have studied. The pathoanatomy of the rocker bottom <span class="hlt">deformity</span> is characterised by a plantar convexity appearing between three and six months of age with the hindfoot equinus position remaining constant. The convexity initially involves the medial column, radiologically identified by the talo-first metatarsal angle and secondly by the lateral column, revealed radiologically as the calcaneo-fifth metatarsal angle. The apex of the <span class="hlt">deformity</span> is usually at the midtrasal with a dorsal calcaneocuboid subluxation. Ideal management of clubfoot <span class="hlt">deformity</span> should avoid this complication, with adequate manipulation and splinting and early Achilles' percutaneous tenotomy if plantar convexity occurs. Adequate soft-tissue <span class="hlt">release</span> provides satisfactory correction for rocker bottom <span class="hlt">deformity</span>. However, this <span class="hlt">deformity</span> requires more extensive and complex procedures than the standard surgical treatment of clubfoot. The need for lateral radiographs to ensure that the rocker bottom <span class="hlt">deformity</span> is recognised early, is demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890006105','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890006105"><span>Geodetic measurement of <span class="hlt">deformation</span> in California. Ph.D. Thesis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sauber, Jeanne Marie</p> <p>1988-01-01</p> <p>The very long baseline interferometry (VLBI) measurements made in the western U.S. since 1979 as part of the NASA Crustal Dynamics Project provide discrete samples of the temporal and spatial <span class="hlt">deformation</span> field. The interpretation of the VLBI-derived rates of <span class="hlt">deformation</span> requires an examination of geologic information and more densely sampled ground-based geodetic data. In the first two of three related studies embodying this thesis triangulation and trilateration data measured on two regional networks are processed, one in the central Mojave Desert and one in the Coast Ranges east of the San Andreas fault. At the spatial scales spanned by these local geodetic networks, auxiliary geologic and geophysical data have been utilized to examine the relation between measured incremental strain and the accommodation of strain seen in local geological structures, strain <span class="hlt">release</span> in earthquakes, and principal stress directions inferred from in situ measurements. In the third study, VLBI data from stations distributed across the Pacific - North American plate boundary zone in the western United States are processed. The VLBI data have been used to constrain the integrated rate of <span class="hlt">deformation</span> across portions of the continental plate boundary in California and to provide a tectonic framework to interpret regional geodetic and geologic studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25675358','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25675358"><span>Linear free <span class="hlt">energy</span> correlations for fission product <span class="hlt">release</span> from the Fukushima-Daiichi nuclear accident.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Abrecht, David G; Schwantes, Jon M</p> <p>2015-03-03</p> <p>This paper extends the preliminary linear free <span class="hlt">energy</span> correlations for radionuclide <span class="hlt">release</span> performed by Schwantes et al., following the Fukushima-Daiichi Nuclear Power Plant accident. Through evaluations of the molar fractionations of radionuclides deposited in the soil relative to modeled radionuclide inventories, we confirm the initial source of the radionuclides to the environment to be from active reactors rather than the spent fuel pool. Linear correlations of the form In χ = −α ((ΔGrxn°(TC))/(RTC)) + β were obtained between the deposited concentrations, and the reduction potentials of the fission product oxide species using multiple reduction schemes to calculate ΔG°rxn (TC). These models allowed an estimate of the upper bound for the reactor temperatures of TC between 2015 and 2060 K, providing insight into the limiting factors to vaporization and <span class="hlt">release</span> of fission products during the reactor accident. Estimates of the <span class="hlt">release</span> of medium-lived fission products 90Sr, 121mSn, 147Pm, 144Ce, 152Eu, 154Eu, 155Eu, and 151Sm through atmospheric venting during the first month following the accident were obtained, indicating that large quantities of 90Sr and radioactive lanthanides were likely to remain in the damaged reactor cores.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JPCM...22M5003H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JPCM...22M5003H"><span><span class="hlt">Deformation</span> twinning in a creep-<span class="hlt">deformed</span> nanolaminate structure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hsiung, Luke L.</p> <p>2010-10-01</p> <p>The underlying mechanism of <span class="hlt">deformation</span> twinning occurring in a TiAl-(γ)/Ti3Al-(α2) nanolaminate creep <span class="hlt">deformed</span> at elevated temperatures has been studied. Since the multiplication and propagation of lattice dislocations in both γ and α2 thin lamellae are very limited, the total flow of lattice dislocations becomes insufficient to accommodate the accumulated creep strains. Consequently, the movement of interfacial dislocations along the laminate interfaces, i.e., interface sliding, becomes an alternative <span class="hlt">deformation</span> mode of the nanolaminate structure. Pile-ups of interfacial dislocations occur when interfacial ledges and impinged lattice dislocations act as obstacles to impede the movement of interfacial dislocations. <span class="hlt">Deformation</span> twinning can accordingly take place to relieve a stress concentration resulting from the pile-up of interfacial dislocations. An interface-controlled twinning mechanism driven by the pile-up and dissociation of interfacial dislocations is accordingly proposed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012SPIE.8314E..0EW','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012SPIE.8314E..0EW"><span>Representation of <span class="hlt">deformable</span> motion for compression of dynamic cardiac image data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Weinlich, Andreas; Amon, Peter; Hutter, Andreas; Kaup, André</p> <p>2012-02-01</p> <p>We present a new approach for efficient estimation and storage of tissue <span class="hlt">deformation</span> in dynamic medical image data like 3-D+t computed tomography reconstructions of human heart acquisitions. Tissue <span class="hlt">deformation</span> between two points in time can be described by means of a displacement vector field indicating for each voxel of a slice, from which position in the previous slice at a fixed position in the third dimension it has moved to this position. Our <span class="hlt">deformation</span> model represents the motion in a compact manner using a down-sampled potential function of the displacement vector field. This function is obtained by a Gauss-Newton minimization of the estimation error image, i. e., the difference between the current and the <span class="hlt">deformed</span> previous slice. For lossless or lossy compression of volume slices, the potential function and the error image can afterwards be coded separately. By assuming <span class="hlt">deformations</span> instead of translational motion, a subsequent coding algorithm using this method will achieve better compression ratios for medical volume data than with conventional block-based motion compensation known from video coding. Due to the smooth prediction without block artifacts, particularly whole-image transforms like wavelet decomposition as well as intra-slice prediction methods can benefit from this approach. We show that with discrete cosine as well as with Karhunen-Lo`eve transform the method can achieve a better <span class="hlt">energy</span> compaction of the error image than block-based motion compensation while reaching approximately the same prediction error <span class="hlt">energy</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21298168','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21298168"><span>Determination of differential cross sections and kinetic <span class="hlt">energy</span> <span class="hlt">release</span> of co-products from central sliced images in photo-initiated dynamic processes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Kuo-mei; Chen, Yu-wei</p> <p>2011-04-07</p> <p>For photo-initiated inelastic and reactive collisions, dynamic information can be extracted from central sliced images of state-selected Newton spheres of product species. An analysis framework has been established to determine differential cross sections and the kinetic <span class="hlt">energy</span> <span class="hlt">release</span> of co-products from experimental images. When one of the reactants exhibits a high recoil speed in a photo-initiated dynamic process, the present theory can be employed to analyze central sliced images from ion imaging or three-dimensional sliced fluorescence imaging experiments. It is demonstrated that the differential cross section of a scattering process can be determined from the central sliced image by a double Legendre moment analysis, for either a fixed or continuously distributed recoil speeds in the center-of-mass reference frame. Simultaneous equations which lead to the determination of the kinetic <span class="hlt">energy</span> <span class="hlt">release</span> of co-products can be established from the second-order Legendre moment of the experimental image, as soon as the differential cross section is extracted. The intensity distribution of the central sliced image, along with its outer and inner ring sizes, provide all the clues to decipher the differential cross section and the kinetic <span class="hlt">energy</span> <span class="hlt">release</span> of co-products.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25223967','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25223967"><span>Laxity after complete <span class="hlt">release</span> of the medial collateral ligament in primary total knee arthroplasty.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cho, Woo-Shin; Byun, Seong-Eun; Lee, Sang-Jun; Yoon, Jaeyoun</p> <p>2015-06-01</p> <p>Medial collateral ligament (MCL) <span class="hlt">release</span> is one of the essential steps toward the achievement of ligament balancing during the total knee arthroplasty (TKA) in patients with varus <span class="hlt">deformity</span>. When the varus <span class="hlt">deformity</span> is severe, complete <span class="hlt">release</span> of the MCL until balanced is often required. However, it is believed that complete MCL <span class="hlt">release</span> may lead to catastrophic laxity. The purpose of this prospective study is to compare the medial joint gap opening in postoperative valgus stress radiograph in patients with complete MCL <span class="hlt">release</span> against patients with partial <span class="hlt">release</span>. Out of 209 primary TKAs performed for degenerative osteoarthritis, complete MCL <span class="hlt">release</span> was required in 33 cases (group I) by sub-periosteal detachment at proximal tibia using periosteal elevator. For the remaining 176 knees (group II), partial <span class="hlt">release</span> of MCL was done. At postoperative 6 months and 1 year, both groups were evaluated for comparing the joint gap on valgus stress radiographs using modified Telos device in 0°, 45°, and 90° of flexion. Additional parameters which were analyzed included preoperative varus and valgus stress radiographs in full extension and pre- and postoperative mechanical alignment in each group. The knee range of motion (ROM) and clinical scores were evaluated at 1-year follow-up. The mean values of the joint opening on the postoperative valgus stress test with the knee joint extended, and in the 45° and 90° flexed states at 6 months and at 1 year postoperatively in group I were not statistically significantly different from those of group II. The clinical scores also did not show a statistically significant difference between two groups. There was a statistically significant difference in ROM between two groups, pre- and postoperatively and the difference was 5°, respectively. This study suggests that complete MCL <span class="hlt">release</span> for ligament balancing is a safe procedure and does not lead to postoperative laxity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810004372','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810004372"><span>Gas <span class="hlt">release</span> and conductivity modification studies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Linson, L. M.; Baxter, D. C.</p> <p>1979-01-01</p> <p>The behavior of gas clouds produced by <span class="hlt">releases</span> from orbital velocity in either a point <span class="hlt">release</span> or venting mode is described by the modification of snowplow equations valid in an intermediate altitude regime. Quantitative estimates are produced for the time dependence of the radius of the cloud, the average internal <span class="hlt">energy</span>, the translational velocity, and the distance traveled. The dependence of these quantities on the assumed density profile, the internal <span class="hlt">energy</span> of the gas, and the ratio of specific heats is examined. The new feature is the inclusion of the effect of the large orbital velocity. The resulting gas cloud models are used to calculate the characteristics of the field line integrated Pedersen conductivity enhancements that would be produced by the <span class="hlt">release</span> of barium thermite at orbital velocity in either the point <span class="hlt">release</span> or venting modes as a function of <span class="hlt">release</span> altitude and chemical payload weight.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.V23A0462G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.V23A0462G"><span>Post-eruptive <span class="hlt">Deformation</span> following the 2014 Holuhraun Rift, Iceland.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grapenthin, R.; Li, S.; Ofeigsson, B.; Sigmundsson, F.; Drouin, V.; Hreinsdottir, S.; Parks, M.; Friðriksdóttir, H. M.</p> <p>2017-12-01</p> <p>On August 16, 2014 an intense seismic swarm started below the eastern part of Bárdarbunga caldera at the NW edge of the Vatnajökull ice cap in Iceland. The seismicity migrated in 3 major segments changing direction at least twice until the advance stopped around 10 km south of Askja Volcano, more than 45 km from Bárdarbunga. The dike opening was accompanied by a 65 m collapse of the Bárdarbunga caldera floor and broad deflation due to magma removal from a 12 km deep reservoir (Gudmundsson et al., 2016). The area of the produced lava flow is 84 km2 with a volume of about 1.4 km3, which makes it the second largest eruption in Iceland since the Laki Fires in 1783 that produced an order of magnitude more lava. The caldera collapse was accompanied by over 40 M5 earthquakes; an immense seismic <span class="hlt">energy</span> <span class="hlt">release</span> for a volcano. The majority of seismicity in the dike clustered between 6-8 km depth. Sigmundsson et al. (2015) derive a maximum opening of 5 m shallower than 6 km from GPS and InSAR data. The co-eruptive <span class="hlt">deformation</span> is followed by a complex juxtaposition of predominantly viscoelastic post-eruptive processes that include post-rifting relaxation and isostatic adjustment to the new lava flow, which modulate the long-term processes of plate spreading, subsidence at Askja Volcano, reinflation at Bárdarbunga, and glacial isostatic adjustment due to the melting of the nearby ice caps. Here, we present first results deciphering this <span class="hlt">deformation</span> field using data from the continuous GPS network that was supplemented during the eruption specifically to capture these processes. We include InSAR analysis of Sentinel-1 data and analyze the observations through viscoelastic modeling approaches. GPS data show an asymmetric <span class="hlt">deformation</span> field around the rift with 2-year GPS velocities between 0.1-1.5 cm/yr predominantly moving away from the rift. Preliminary modeling suggests several centimeters of horizontal displacement in plate spreading directions due to post</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730010154','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730010154"><span>Apollo couch <span class="hlt">energy</span> absorbers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wesselski, C. J.; Drexel, R. E.</p> <p>1972-01-01</p> <p>Load attenuators for the Apollo spacecraft crew couch and its potential applications are described. <span class="hlt">Energy</span> absorption is achieved through friction and cyclic <span class="hlt">deformation</span> of material. In one concept, <span class="hlt">energy</span> absorption is accomplished by rolling a compressed ring of metal between two surfaces. In another concept, <span class="hlt">energy</span> is absorbed by forcing a plastically <span class="hlt">deformed</span> washer along a rod. Among the design problems that had to be solved were material selection, fatigue life, ring slippage, lubrication, and friction loading.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22420195-scaling-laws-deformation-mechanisms-nanoporous-copper-under-adiabatic-uniaxial-strain-compression','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22420195-scaling-laws-deformation-mechanisms-nanoporous-copper-under-adiabatic-uniaxial-strain-compression"><span>Scaling laws and <span class="hlt">deformation</span> mechanisms of nanoporous copper under adiabatic uniaxial strain compression</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Yuan, Fuping, E-mail: fpyuan@lnm.imech.ac.cn; Wu, Xiaolei, E-mail: xlwu@imech.ac.cn</p> <p>2014-12-15</p> <p>A series of large-scale molecular dynamics simulations were conducted to investigate the scaling laws and the related atomistic <span class="hlt">deformation</span> mechanisms of Cu monocrystal samples containing randomly placed nanovoids under adiabatic uniaxial strain compression. At onset of yielding, plastic <span class="hlt">deformation</span> is accommodated by dislocations emitted from void surfaces as shear loops. The collapse of voids are observed by continuous emissions of dislocations from void surfaces and their interactions with further plastic <span class="hlt">deformation</span>. The simulation results also suggest that the effect modulus, the yield stress and the <span class="hlt">energy</span> aborption density of samples under uniaxial strain are linearly proportional to the relative densitymore » ρ. Moreover, the yield stress, the average flow stress and the <span class="hlt">energy</span> aborption density of samples with the same relative density show a strong dependence on the void diameter d, expressed by exponential relations with decay coefficients much higher than -1/2. The corresponding atomistic mechanisms for scaling laws of the relative density and the void diameter were also presented. The present results should provide insights for understanding <span class="hlt">deformation</span> mechanisms of nanoporous metals under extreme conditions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhLA..380.2279B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhLA..380.2279B"><span>Perturbatively <span class="hlt">deformed</span> defects in Pöschl-Teller-driven scenarios for quantum mechanics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bernardini, Alex E.; da Rocha, Roldão</p> <p>2016-07-01</p> <p>Pöschl-Teller-driven solutions for quantum mechanical fluctuations are triggered off by single scalar field theories obtained through a systematic perturbative procedure for generating <span class="hlt">deformed</span> defects. The analytical properties concerning the quantum fluctuations in one-dimension, zero-mode states, first- and second-excited states, and <span class="hlt">energy</span> density profiles are all obtained from <span class="hlt">deformed</span> topological and non-topological structures supported by real scalar fields. Results are firstly derived from an integrated λϕ4 theory, with corresponding generalizations applied to starting λχ4 and sine-Gordon theories. By focusing our calculations on structures supported by the λϕ4 theory, the outcome of our study suggests an exact quantitative correspondence to Pöschl-Teller-driven systems. Embedded into the perturbative quantum mechanics framework, such a correspondence turns into a helpful tool for computing excited states and continuous mode solutions, as well as their associated <span class="hlt">energy</span> spectrum, for quantum fluctuations of perturbatively <span class="hlt">deformed</span> structures. Perturbative <span class="hlt">deformations</span> create distinct physical scenarios in the context of exactly solvable quantum systems and may also work as an analytical support for describing novel braneworld universes embedded into a 5-dimensional gravity bulk.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998PhRvE..58.4807E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998PhRvE..58.4807E"><span>Vesicle <span class="hlt">deformation</span> by microtubules: A phase diagram</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Emsellem, Virginie; Cardoso, Olivier; Tabeling, Patrick</p> <p>1998-10-01</p> <p>The experimental investigation of vesicles <span class="hlt">deformed</span> by the growth of encapsulated microtubules shows that the axisymmetric morphologies can be classified into ovals, lemons, φ, cherries, dumbbells, and pearls. A geometrical phase diagram is established. Numerical minimization of the elastic <span class="hlt">energy</span> of the membrane reproduces satisfactorily well the observed morphologies and the corresponding phase diagram.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/7168895-tensile-deformation-recovery-kinetics-alloy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/7168895-tensile-deformation-recovery-kinetics-alloy"><span>Tensile <span class="hlt">deformation</span> and recovery kinetics of Alloy 690</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Lo, C.F.; Mayo, W.E.; Weissmann, S.</p> <p>1992-07-01</p> <p>The effect of carbon content, grain size and thermal history on the <span class="hlt">deformation</span> behavior of nickel-base Alloy 690 has been investigated. Carbon content effects the yield strength of Mill Annealed (MA) material, but has no effect in Thermally Treated (TT) material. Also, no effect of carbon content on the workhardening rate was seen in either material. There was an effect of grain size as expected. An interesting aspect of this work showed that TT material consistently has a slightly higher Young's modulus than the MA. As <span class="hlt">deformation</span> moves into the plastic regime, the TT material displays a two stage hardeningmore » process. This consists of a low workhardening rate (n = 0.05), followed by a transition to the more normal workhardening rate (n=0.35). The MA material, on the other hand, does not exhibit the low n region. This unusual <span class="hlt">deformation</span> behavior is attributable to the presence of planar slip which initiates at the grain boundary over the strain range of 0.2 to 0.7%. These observations are useful to explain the unexpectedly fast strain relaxation behavior seen in this alloy. The recovery kinetics of the alloy have also been studied. Rapid recovery with an activation <span class="hlt">energy</span> of approximately 5.3 kj/mol occurs when the <span class="hlt">deformation</span> level is low. This was attributed to a grain boundary self diffusion process. At higher strain levels, recovery is much slower with an activation <span class="hlt">energy</span> of approximately 14 kJ/mol. This process was attributable to bulk diffusion. Based on TEM and X-ray rocking curve measurements, these results have been explained.« less</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_15 --> <div id="page_16" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="301"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/458903','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/458903"><span>{Delta}I = 2 <span class="hlt">energy</span> staggering in normal <span class="hlt">deformed</span> dysprosium nuclei</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Riley, M.A.; Brown, T.B.; Archer, D.E.</p> <p>1996-12-31</p> <p>Very high spin states (I{ge}50{Dirac_h}) have been observed in {sup 155,156,157}Dy. The long regular band sequences, free from sharp backbending effects, observed in these dysprosium nuclei offer the possibility of investigating the occurence of any {Delta}I = 2 staggering in normal <span class="hlt">deformed</span> nuclei. Employing the same analysis techniques as used in superdeformed nuclei, certain bands do indeed demonstrate an apparent staggering and this is discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.T21B1800H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.T21B1800H"><span>Role of coupled cataclasis-pressure solution <span class="hlt">deformation</span> in microearthquake activity along the creeping segment of the SAF: Inferences from studies of the SAFOD core samples</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hadizadeh, J.; Gratier, J.; Renard, F.; Mittempregher, S.; di Toro, G.</p> <p>2009-12-01</p> <p>Rocks encountered in the SAFOD drill hole represent <span class="hlt">deformation</span> in the southern-most extent of the creeping segment of the SAF north of the Parkfield. At the site and toward the northwest the SAF is characterized by aseismic creep as well as strain <span class="hlt">release</span> through repeating microearthquakes M<3. The activity is shown to be mostly distributed as clusters aligned in the slip direction, and occurring at depths of between 3 to 5 kilometers. It has been suggested that the events are due to frequent moment <span class="hlt">release</span> from high strength asperities constituting only about 1% or less of the total fault surface area within an otherwise weak fault gouge. We studied samples selected from the SAFOD phase 3 cores (3142m -3296m MD) using high resolution scanning electron microscopy, cathodoluminescence imaging, X-ray fluorescence mapping, and <span class="hlt">energy</span> dispersive X-ray spectroscopy. The observed microstructural <span class="hlt">deformation</span> that is apparently relevant to the seismological data includes clear evidence of cyclic <span class="hlt">deformation</span> events, cataclastic flow, and pressure solution creep with attendant vein sealing and fracture healing fabrics. Friction testing of drill cuttings and modeling by others suggest that the overall creep behavior in shale-siltstone gouge may be due to low bulk friction coefficient of 0.2-0.4 for the fault rock. Furthermore, the low resistivity zone extending to about 5km beneath the SAFOD-Middle Mountain area is believed to consist of a pod of fluid-filled fractured and porous rocks. Our microstructural data indicate that the foliated shale-siltstone cataclasites are, in a highly heterogeneous way, more porous and permeable than the host rock and therefore provide for structurally controlled enhanced fluid-rock interactions. This is consistent with the observed pressure solution <span class="hlt">deformation</span> and the microstructural indications of transiently high fluid pressures. We hypothesize that while the friction laws defining stable sliding are prevalent in bulk <span class="hlt">deformation</span> of the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AcAau.112..182L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AcAau.112..182L"><span><span class="hlt">Energy</span> <span class="hlt">release</span> properties of amorphous boron and boron-based propellant primary combustion products</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liang, Daolun; Liu, Jianzhong; Xiao, Jinwu; Xi, Jianfei; Wang, Yang; Zhang, Yanwei; Zhou, Junhu</p> <p>2015-07-01</p> <p>The microstructure of amorphous boron and the primary combustion products of boron-based fuel-rich propellant (hereafter referred to as primary combustion products) was analyzed by scanning electron microscope. Composition analysis of the primary combustion products was carried out by X-ray diffraction and X-ray photoelectron spectroscopy. The <span class="hlt">energy</span> <span class="hlt">release</span> properties of amorphous boron and the primary combustion products were comparatively studied by laser ignition experimental system and thermogravimetry-differential scanning calorimetry. The primary combustion products contain B, C, Mg, Al, B4C, B13C2, BN, B2O3, NH4Cl, H2O, and so on. The <span class="hlt">energy</span> <span class="hlt">release</span> properties of primary combustion products are different from amorphous boron, significantly. The full-time spectral intensity of primary combustion products at a wavelength of 580 nm is ~2% lower than that of amorphous boron. The maximum spectral intensity of the former at full wave is ~5% higher than that of the latter. The ignition delay time of primary combustion products is ~150 ms shorter than that of amorphous boron, and the self-sustaining combustion time of the former is ~200 ms longer than that of the latter. The thermal oxidation process of amorphous boron involves water evaporation (weight loss) and boron oxidation (weight gain). The thermal oxidation process of primary combustion products involves two additional steps: NH4Cl decomposition (weight loss) and carbon oxidation (weight loss). CL-20 shows better combustion-supporting effect than KClO4 in both the laser ignition experiments and the thermal oxidation experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002SPIE.4562..593M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002SPIE.4562..593M"><span>Low surface <span class="hlt">energy</span> polymeric <span class="hlt">release</span> coating for improved contact print lithography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mancini, David P.; Resnick, Douglas J.; Gehoski, Kathleen A.; Popovich, Laura L.; Chang, Daniel</p> <p>2002-03-01</p> <p>Contact printing has been used for decades in many various lithography applications in the microelectronic industry. While vacuum contact printing processes offer sub-micron resolution and high throughput, they often suffer from some important drawbacks. One of the most common problems is degradation in both resolution and defect density which occurs when the same mask si used for multiple exposures without frequent mask cleans. This is largely due to the relatively high surface <span class="hlt">energy</span> of both quartz and chrome and the tendency of most photoresists to adhere to these surfaces. As a result, when a mask and wafer are pressed into intimate contact, resist will tend to stick to the mask creating a defect on the wafer, effectively propagating defects to subsequent wafers. In this study, DuPont Teflon AF 1601S is used as a photomask coating and evaluated for its ability to act as a <span class="hlt">release</span> agent and reduce defects while maintaining resolution for multiple exposures. Teflon AF is an amorphous, transparent, low surface <span class="hlt">energy</span>, polymeric material that can be spin coated into a thin conformal film. Tests have shown that when using an uncoated mask in vacuum contact, resolution of 0.75 micrometers dense lines is severely degraded after less than 10 consecutive exposures. However, when the mask is coated, 0.75 micrometers dense lines were successfully resolved using vacuum contact for over 200 exposures without cleaning. In addition, it has been demonstrated that Teflon AF coatings impart to a mask a self-cleaning capability, since particles tend to stick to the photoresist rather than the mask. A coated mask, which was purposefully contaminated with particulates, resolved 0.75 micrometers dense lines on all but the first wafer of a series of 25 consecutive exposures. The patented mask <span class="hlt">releases</span> layer process has successfully been demonstrated with a positive novolak resist. Additional data which describes the system chemistry, dilution and coating process, and film morphology</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016IJGMM..1350018C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016IJGMM..1350018C"><span>Moyal <span class="hlt">deformations</span> of Clifford gauge theories of gravity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Castro, Carlos</p> <p>2016-12-01</p> <p>A Moyal <span class="hlt">deformation</span> of a Clifford Cl(3, 1) Gauge Theory of (Conformal) Gravity is performed for canonical noncommutativity (constant Θμν parameters). In the very special case when one imposes certain constraints on the fields, there are no first-order contributions in the Θμν parameters to the Moyal <span class="hlt">deformations</span> of Clifford gauge theories of gravity. However, when one does not impose constraints on the fields, there are first-order contributions in Θμν to the Moyal <span class="hlt">deformations</span> in variance with the previous results obtained by other authors and based on different gauge groups. Despite that the generators of U(2, 2),SO(4, 2),SO(2, 3) can be expressed in terms of the Clifford algebra generators this does not imply that these algebras are isomorphic to the Clifford algebra. Therefore one should not expect identical results to those obtained by other authors. In particular, there are Moyal <span class="hlt">deformations</span> of the Einstein-Hilbert gravitational action with a cosmological constant to first-order in Θμν. Finally, we provide a mechanism which furnishes a plausible cancellation of the huge vacuum <span class="hlt">energy</span> density.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900016760','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900016760"><span>Strain <span class="hlt">energy</span> <span class="hlt">release</span> rate analysis of delamination in a tapered laminate subjected to tension load</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Salpekar, S. A.; Raju, I. S.; Obrien, T. K.</p> <p>1990-01-01</p> <p>A tapered composite laminate subjected to tension load was analyzed using the finite-element method. The glass/epoxy laminate has a (+ or - 45)sub 3 group of plies dropped in three distinct steps, each 20 ply-thicknesses apart, thus forming a taper angle of 5.71 degrees. Steep gradients of interlaminar normal and shear stress on a potential delamination interface suggest the existence of stress singularities at the points of material and geometric discontinuities created by the internal plydrops. The delamination was assumed to initiate at the thin end of the taper on a -45/+45 interface and the delamination growth was simulated in both directions, i.e., along the taper and into the thin region. The strain-<span class="hlt">energy-release</span> rate for a delamination growing into the thin laminate consisted predominantly of mode I (opening) component. For a delamination growing along the tapered region, the strain-<span class="hlt">energy-release</span> rate was initially all mode I, but the proportion of mode I decreased with increase in delamination size until eventually total G was all mode II. The total G for both delamination tips increased with increase in delamination size, indicating that a delamination initiating at the end of the taper will grow unstably along the taper and into the thin laminate simultaneously.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017BVol...79...84M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017BVol...79...84M"><span>Volatiles and <span class="hlt">energy</span> <span class="hlt">released</span> by Puracé volcano</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Maldonado, Luisa Fernanda Meza; Inguaggiato, Salvatore; Jaramillo, Marco Tulio; Valencia, Gustavo Garzón; Mazot, Agnes</p> <p>2017-12-01</p> <p>Total CO2 output of Puracé volcano (Colombia) was estimated on the basis of fluids discharged by fumaroles, soil gases, and dissolved carbon species in the aquifer. The soil CO2 emission was computed from a field survey of 512 points of CO2 soil flux measurements at the main degassing areas of Puracé volcano. The CO2 flux from Puracé's plume was estimated using an indirect method, that used the SO2 plume flux and CO2/SO2 ratio of the main high temperature fumarole. The total output of CO2 was estimated at ≅ 1500 t/day. The main contribution of CO2 comes from the plume (summit degassing) and from soil degassing that emit 673 and 812 t/day, respectively. The contributions of summit and soil degassing areas are comparable, indicating an intermediate degassing style partitioned between closed and open conduit systems. The estimated water vapor discharge (as derived from the chemical composition of the fumaroles, the H2O/CO2 ratio, and the SO2 plume flux) allowed calculation of the total thermal <span class="hlt">energy</span> (fumarolic, soil degassing, and aquifer) <span class="hlt">released</span> from the Puracé volcanic system. This was 360 MW.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22488900-properties-deformed-hyperbolic-trigonometric-functions-quantum-deformation','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22488900-properties-deformed-hyperbolic-trigonometric-functions-quantum-deformation"><span>The properties of Q-<span class="hlt">deformed</span> hyperbolic and trigonometric functions in quantum <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Deta, U. A., E-mail: utamaalan@yahoo.co.id, E-mail: utamadeta@unesa.ac.id; Suparmi</p> <p>2015-09-30</p> <p>Quantum <span class="hlt">deformation</span> has been studied due to its relation with applications in nuclear physics, conformal field theory, and statistical-quantum theory. The q-<span class="hlt">deformation</span> of hyperbolic function was introduced by Arai. The application of q-<span class="hlt">deformed</span> functions has been widely used in quantum mechanics. The properties of this two kinds of system explained in this paper including their derivative. The graph of q-<span class="hlt">deformed</span> functions presented using Matlab. The special case is given for modified Poschl-Teller plus q-<span class="hlt">deformed</span> Scarf II trigonometry potentials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992PApGe.139..293T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992PApGe.139..293T"><span>Time-lag of the earthquake <span class="hlt">energy</span> <span class="hlt">release</span> between three seismic regions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsapanos, Theodoros M.; Liritzis, Ioannis</p> <p>1992-06-01</p> <p>Three complete data sets of strong earthquakes ( M≥5.5), which occurred in the seismic regions of Chile, Mexico and Kamchatka during the time period 1899 1985, have been used to test the existence of a time-lag in the seismic <span class="hlt">energy</span> <span class="hlt">release</span> between these regions. These data sets were cross-correlated in order to determine whether any pair of the sets are correlated. For this purpose statistical tests, such as the T-test, the Fisher's transformation and probability distribution have been applied to determine the significance of the obtained correlation coefficients. The results show that the time-lag between Chile and Kamchatka is -2, which means that Kamchatka precedes Chile by 2 years, with a correlation coefficient significant at 99.80% level, a weak correlation between Kamchatka-Mexico and noncorrelation for Mexico-Chile.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MMTA...48.4821T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MMTA...48.4821T"><span><span class="hlt">Deformation</span> Behavior of Cementite in <span class="hlt">Deformed</span> High Carbon Steel Observed by X-ray Diffraction with Synchrotron Radiation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Taniyama, Akira; Takayama, Toru; Arai, Masahiro; Hamada, Takanari</p> <p>2017-10-01</p> <p>The <span class="hlt">deformation</span> behavior of cementite in drawn pearlitic steel and spheroidal cementite steel, which have hypereutectoid composition, was investigated by X-ray diffraction using synchrotron radiation. A detailed analysis of diffraction peak profiles reveals that the <span class="hlt">deformation</span> behavior strongly depends on the shape of cementite in steel. The unit cell volume of the cementite in the drawn pearlitic steel compressively and elastically <span class="hlt">deforms</span> by 1.5 to 2 pct of the initial volume at the early stage of drawing, whereas that in the drawn spheroidal cementite steel is compressed by 1 pct of the initial volume even at a large true strain. The cementite in the drawn pearlitic steel fragments into small pieces with increasing the true strain, and these pieces change to amorphous cementite. The dislocation densities of the cementite in the drawn pearlitic steel and in the drawn spheroidal cementite steel are estimated to be 1013/m2 before drawing and 1014/m2 after drawing. Although the large strain is induced in the cementite by drawing, the maximum strain <span class="hlt">energy</span> in the cementite is too small to contribute to the dissolution of the cementite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApJ...835..214P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApJ...835..214P"><span>Stochastic Fermi Energization of Coronal Plasma during Explosive Magnetic <span class="hlt">Energy</span> <span class="hlt">Release</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pisokas, Theophilos; Vlahos, Loukas; Isliker, Heinz; Tsiolis, Vassilis; Anastasiadis, Anastasios</p> <p>2017-02-01</p> <p>The aim of this study is to analyze the interaction of charged particles (ions and electrons) with randomly formed particle scatterers (e.g., large-scale local “magnetic fluctuations” or “coherent magnetic irregularities”) using the setup proposed initially by Fermi. These scatterers are formed by the explosive magnetic <span class="hlt">energy</span> <span class="hlt">release</span> and propagate with the Alfvén speed along the irregular magnetic fields. They are large-scale local fluctuations (δB/B ≈ 1) randomly distributed inside the unstable magnetic topology and will here be called Alfvénic Scatterers (AS). We constructed a 3D grid on which a small fraction of randomly chosen grid points are acting as AS. In particular, we study how a large number of test particles evolves inside a collection of AS, analyzing the evolution of their <span class="hlt">energy</span> distribution and their escape-time distribution. We use a well-established method to estimate the transport coefficients directly from the trajectories of the particles. Using the estimated transport coefficients and solving the Fokker-Planck equation numerically, we can recover the <span class="hlt">energy</span> distribution of the particles. We have shown that the stochastic Fermi energization of mildly relativistic and relativistic plasma can heat and accelerate the tail of the ambient particle distribution as predicted by Parker & Tidman and Ramaty. The temperature of the hot plasma and the tail of the energetic particles depend on the mean free path (λsc) of the particles between the scatterers inside the energization volume.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoRL..45..620K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoRL..45..620K"><span>Effects of Friction and Plastic <span class="hlt">Deformation</span> in Shock-Comminuted Damaged Rocks on Impact Heating</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kurosawa, Kosuke; Genda, Hidenori</p> <p>2018-01-01</p> <p>Hypervelocity impacts cause significant heating of planetary bodies. Such events are recorded by a reset of 40Ar-36Ar ages and/or impact melts. Here we investigate the influence of friction and plastic <span class="hlt">deformation</span> in shock-generated comminuted rocks on the degree of impact heating using the iSALE shock-physics code. We demonstrate that conversion from kinetic to internal <span class="hlt">energy</span> in the targets with strength occurs during pressure <span class="hlt">release</span>, and additional heating becomes significant for low-velocity impacts (<10 km s-1). This additional heat reduces the impact-velocity thresholds required to heat the targets with the 0.1 projectile mass to temperatures for the onset of Ar loss and melting from 8 and 10 km s-1, respectively, for strengthless rocks to 2 and 6 km s-1 for typical rocks. Our results suggest that the impact conditions required to produce the unique features caused by impact heating span a much wider range than previously thought.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.8051S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.8051S"><span>X-ray microtomography analysis of soil structure <span class="hlt">deformation</span> caused by centrifugation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schlüter, Steffen; Leuther, Frederic; Vogler, Steffen; Vogel, Hans-Jörg</p> <p>2016-04-01</p> <p>Centrifugation provides a fast method to measure soil water retention curves over a wide moisture range. However, <span class="hlt">deformation</span> of soil structure may occur at high angular velocities in the centrifuge. The objective of this study was to capture these changes in soil structure with X-ray microtomography and to measure local <span class="hlt">deformations</span> via digital volume correlation. Two samples were investigated that differ in texture and rock content. A detailed analysis of the pore space reveals an interplay between shrinkage due to drying and soil compaction due to compression. Macroporosity increases at moderate angular velocity because of crack formation due to moisture <span class="hlt">release</span>. At higher angular velocities, corresponding to capillary pressure of <-100kPa, macroporosity decreases again because of structure <span class="hlt">deformation</span> due to compression. While volume changes due to swelling clay minerals are immanent to any drying process, the compaction of soil is a specific drawback of the centrifugation method. A new protocol for digital volume correlation was developed to analyze the spatial heterogeneity of <span class="hlt">deformation</span>. In both samples the displacement of soil constituents is highest in the top part of the sample and exhibits high lateral variability explained by the spatial distribution of macropores in the sample. Centrifugation should therefore only be applied after the completion of all other hydraulic or thermal experiments, or any other analysis that depends on the integrity of soil structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SolE....7..129S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SolE....7..129S"><span>X-ray microtomography analysis of soil structure <span class="hlt">deformation</span> caused by centrifugation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schlüter, S.; Leuther, F.; Vogler, S.; Vogel, H.-J.</p> <p>2016-01-01</p> <p>Centrifugation provides a fast method to measure soil water retention curves over a wide moisture range. However, <span class="hlt">deformation</span> of soil structure may occur at high angular velocities in the centrifuge. The objective of this study was to capture these changes in soil structure with X-ray microtomography and to measure local <span class="hlt">deformations</span> via digital volume correlation. Two samples were investigated that differ in texture and rock content. A detailed analysis of the pore space reveals an interplay between shrinkage due to drying and soil compaction due to compression. Macroporosity increases at moderate angular velocity because of crack formation due to moisture <span class="hlt">release</span>. At higher angular velocities, corresponding to capillary pressure of ψ < -100 kPa, macroporosity decreases again because of structure <span class="hlt">deformation</span> due to compression. While volume changes due to swelling clay minerals are immanent in any drying process, the compaction of soil is a specific drawback of the centrifugation method. A new protocol for digital volume correlation was developed to analyze the spatial heterogeneity of <span class="hlt">deformation</span>. In both samples the displacement of soil constituents is highest in the top part of the sample and exhibits high lateral variability explained by the spatial distribution of macropores in the sample. Centrifugation should therefore only be applied after the completion of all other hydraulic or thermal experiments, or any other analysis that depends on the integrity of soil structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AstSR..12..185G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AstSR..12..185G"><span>Models of determining <span class="hlt">deformations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gladilin, V. N.</p> <p>2016-12-01</p> <p>In recent years, a lot of functions designed to determine <span class="hlt">deformation</span> values that occur mostly as a result of settlement of structures and industrial equipment. Some authors suggest such advanced mathematical functions approximating <span class="hlt">deformations</span> as general methods for the determination of <span class="hlt">deformations</span>. The article describes models of <span class="hlt">deformations</span> as physical processes. When comparing static, cinematic and dynamic models, it was found that the dynamic model reflects the <span class="hlt">deformation</span> of structures and industrial equipment most reliably.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PMag...91.4345F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PMag...91.4345F"><span>Cyclic <span class="hlt">deformation</span> of bidisperse two-dimensional foams</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fátima Vaz, M.; Cox, S. J.; Teixeira, P. I. C.</p> <p>2011-12-01</p> <p>In-plane <span class="hlt">deformation</span> of foams was studied experimentally by subjecting bidisperse foams to cycles of traction and compression at a prescribed rate. Each foam contained bubbles of two sizes with given area ratio and one of three initial arrangements: sorted perpendicular to the axis of <span class="hlt">deformation</span> (iso-strain), sorted parallel to the axis of <span class="hlt">deformation</span> (iso-stress), or randomly mixed. Image analysis was used to measure the characteristics of the foams, including the number of edges separating small from large bubbles N sl , the perimeter (surface <span class="hlt">energy</span>), the distribution of the number of sides of the bubbles, and the topological disorder μ2(N). Foams that were initially mixed were found to remain mixed after the <span class="hlt">deformation</span>. The response of sorted foams, however, depended on the initial geometry, including the area fraction of small bubbles and the total number of bubbles. For a given experiment we found that (i) the perimeter of a sorted foam varied little; (ii) each foam tended towards a mixed state, measured through the saturation of N sl ; and (iii) the topological disorder μ2(N) increased up to an "equilibrium" value. The results of different experiments showed that (i) the change in disorder, ? decreased with the area fraction of small bubbles under iso-strain, but was independent of it under iso-stress; and (ii) ? increased with ? under iso-strain, but was again independent of it under iso-stress. We offer explanations for these effects in terms of elementary topological processes induced by the <span class="hlt">deformations</span> that occur at the bubble scale.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018TDR.....9..174L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018TDR.....9..174L"><span>Template-Based 3D Reconstruction of Non-rigid <span class="hlt">Deformable</span> Object from Monocular Video</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Yang; Peng, Xiaodong; Zhou, Wugen; Liu, Bo; Gerndt, Andreas</p> <p>2018-06-01</p> <p>In this paper, we propose a template-based 3D surface reconstruction system of non-rigid <span class="hlt">deformable</span> objects from monocular video sequence. Firstly, we generate a semi-dense template of the target object with structure from motion method using a subsequence video. This video can be captured by rigid moving camera orienting the static target object or by a static camera observing the rigid moving target object. Then, with the reference template mesh as input and based on the framework of classical template-based methods, we solve an <span class="hlt">energy</span> minimization problem to get the correspondence between the template and every frame to get the time-varying mesh to present the <span class="hlt">deformation</span> of objects. The <span class="hlt">energy</span> terms combine photometric cost, temporal and spatial smoothness cost as well as as-rigid-as-possible cost which can enable elastic <span class="hlt">deformation</span>. In this paper, an easy and controllable solution to generate the semi-dense template for complex objects is presented. Besides, we use an effective iterative Schur based linear solver for the <span class="hlt">energy</span> minimization problem. The experimental evaluation presents qualitative <span class="hlt">deformation</span> objects reconstruction results with real sequences. Compare against the results with other templates as input, the reconstructions based on our template have more accurate and detailed results for certain regions. The experimental results show that the linear solver we used performs better efficiency compared to traditional conjugate gradient based solver.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23931627','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23931627"><span>Novel vaginal drug delivery system: <span class="hlt">deformable</span> propylene glycol liposomes-in-hydrogel.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Vanić, Željka; Hurler, Julia; Ferderber, Kristina; Golja Gašparović, Petra; Škalko-Basnet, Nataša; Filipović-Grčić, Jelena</p> <p>2014-03-01</p> <p><span class="hlt">Deformable</span> propylene glycol-containing liposomes (DPGLs) incorporating metronidazole or clotrimazole were prepared and evaluated as an efficient drug delivery system to improve the treatment of vaginal microbial infections. The liposome formulations were optimized based on sufficient trapping efficiencies for both drugs and membrane elasticity as a prerequisite for successful permeability and therapy. An appropriate viscosity for vaginal administration was achieved by incorporating the liposomes into Carbopol hydrogel. DPGLs were able to penetrate through the hydrogel network more rapidly than conventional liposomes. In vitro studies of drug <span class="hlt">release</span> from the liposomal hydrogel under conditions simulating human treatment confirmed sustained and diffusion-based drug <span class="hlt">release</span>. Characterization of the rheological and textural properties of the DPGL-containing liposomal hydrogels demonstrated that the incorporation of DPGLs alone had no significant influence on mechanical properties of hydrogels compared to controls. These results support the great potential of DPGL-in-hydrogel as an efficient delivery system for the controlled and sustained <span class="hlt">release</span> of antimicrobial drugs in the vagina.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.G32A..02S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.G32A..02S"><span>Elastic strain budget and inelastic <span class="hlt">deformation</span> in northeast Japan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sagiya, T.; Meneses Gutierrez, A. D. V.</p> <p>2016-12-01</p> <p>A degree of magnitude discrepancy between geodetic and geologic strain rates of the Japan islands has been debated for a long time. Ikeda (1996) hypothesized that geodetic strain rate is affected by interseismic locking at the plate interface, which was later supported by the occurrence of the 2011 Tohoku-oki earthquake. The hypothesis also predicts that the interseismic elastic strain must be fully <span class="hlt">released</span> in association with large earthquakes and do not accumulates in time. However, there has been no such quantitative discussion about the elastic strain budget of the Japan Islands so far. A 261 km-long baseline connecting GEONET stations Ryotsu (950232) and Oshika (960550) runs across the northeast Japan in the E-W direction. The baseline length change shows interseismic contraction at 0.11 ppm/yr before 2011, and coseismic extension of about 20 ppm, which comprises only 200 years of interseismic strain. Geologically the recurrence interval of 2011-type giant earthquakes is estimated as 400-800 years, much longer than a prediction from the elastic strain budget. Menese-Gutierrez and Sagiya (2016) recently identified persistent crustal shortening of 4-10 mm/yr along the Japan Sea coastal area from continuous GPS data. This contribution of inelastic <span class="hlt">deformation</span> corresponds to 10 30% of the total interseismic shortening. The discrepancy can be also partly resolved by considering the effects of M7-class earthquakes and inelastic <span class="hlt">deformation</span> of the island arc. M7-class earthquakes such as the 1978 and 2005 Miyagi-oki earthquakes cause 0.05-0.10 cm of baseline extension every about 40 years, <span class="hlt">releasing</span> about 10 % of the totals strain. In addition, a postseismic extension still continues after 5 years from the main shock. By assuming this postseismic phase continues for about 50-100 years, the total elastic strain budget is balanced for a recurrence interval of about 400 yrs. If we assume a longer recurrence interval, we need additional ingredients such as inelastic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110014900','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110014900"><span>Temperature-Controlled Clamping and <span class="hlt">Releasing</span> Mechanism</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rosing, David; Ford, Virginia</p> <p>2005-01-01</p> <p>A report describes the development of a mechanism that automatically clamps upon warming and <span class="hlt">releases</span> upon cooling between temperature limits of approx. =180 K and approx. =293 K. The mechanism satisfied a need specific to a program that involved repeated excursions of a spectrometer between a room-temperature atmospheric environment and a cryogenic vacuum testing environment. The mechanism was also to be utilized in the intended application of the spectrometer, in which the spectrometer would be clamped for protection during launch of a spacecraft and <span class="hlt">released</span> in the cold of outer space to allow it to assume its nominal configuration for scientific observations. The mechanism is passive in the sense that its operation does not depend on a control system and does not require any power other than that incidental to heating and cooling. The clamping and <span class="hlt">releasing</span> action is effected by bolt-preloaded stacks of shape-memory-alloy (SMA) cylinders. In designing this mechanism, as in designing other, similar SMA mechanisms, it was necessary to account for the complex interplay among thermal expansion, elastic and inelastic <span class="hlt">deformation</span> under load, and SMA thermomechanical properties.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22366002','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22366002"><span>[Preliminary application of an improved Demons <span class="hlt">deformable</span> registration algorithm in tumor radiotherapy].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhou, Lu; Zhen, Xin; Lu, Wenting; Dou, Jianhong; Zhou, Linghong</p> <p>2012-01-01</p> <p>To validate the efficiency of an improved Demons <span class="hlt">deformable</span> registration algorithm and evaluate its application in registration of the treatment image and the planning image in image-guided radiotherapy (IGRT). Based on Brox's gradient constancy assumption and Malis's efficient second-order minimization algorithm, a grey value gradient similarity term was added into the original <span class="hlt">energy</span> function, and a formula was derived to calculate the update of transformation field. The limited Broyden-Fletcher-Goldfarb-Shanno (L-BFGS) algorithm was used to optimize the <span class="hlt">energy</span> function for automatic determination of the iteration number. The proposed algorithm was validated using mathematically <span class="hlt">deformed</span> images, physically <span class="hlt">deformed</span> phantom images and clinical tumor images. Compared with the original Additive Demons algorithm, the improved Demons algorithm achieved a higher precision and a faster convergence speed. Due to the influence of different scanning conditions in fractionated radiation, the density range of the treatment image and the planning image may be different. The improved Demons algorithm can achieve faster and more accurate radiotherapy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998PhDT........66D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998PhDT........66D"><span>Characterization of plastic <span class="hlt">deformation</span> and chemical reaction in titanium-polytetrafluoroethylene mixture</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davis, Jeffery Jon</p> <p>1998-09-01</p> <p>The subject of this dissertation is the <span class="hlt">deformation</span> process of a single metal - polymer system (titanium - polytetrafluoroethylene) and how this process leads to initiation of chemical reaction. Several different kinds of experiments were performed to characterize the behavior of this material to shock and impact. These mechanical conditions induce a rapid plastic <span class="hlt">deformation</span> of the sample. All of the samples tested had an initial porosity which increased the plastic flow condition. It is currently believed that during the <span class="hlt">deformation</span> process two important conditions occur: removal of the oxide layer from the metal and decomposition of the polymer. These conditions allow for rapid chemical reaction. The research from this dissertation has provided insight into the complex behavior of plastic <span class="hlt">deformation</span> and chemical reactions in titanium - polytetrafluoroethylene (PTFE, Teflon). A hydrodynamic computational code was used to model the plastic flow for correlation with the results from the experiments. The results from this work are being used to develop an ignition and growth model for metal/polymer systems. Three sets of experiments were used to examine <span class="hlt">deformation</span> of the 80% Ti and 20% Teflon materials: drop- weight, gas gun, and split-Hopkinson pressure bar. Recovery studies included post shot analysis of the samples using x-ray diffraction. Lagrangian hydrocode DYNA2D modeling of the drop-weight tests was performed for comparison with experiments. One of the reactions know to occur is Ti + C → TiC (s) which results in an exothermic <span class="hlt">release</span>. However, the believed initial reactions occur between Ti and fluorine which produces TixFy gases. The thermochemical code CHEETAH was used to investigate the detonation products and concentrations possible during Ti - Teflon reaction. CHEETAH shows that the Ti - fluorine reactions are thermodynamically favorable. This research represents the most comprehensive to date study of <span class="hlt">deformation</span> induced chemical reaction in metal/polymers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030112449','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030112449"><span>Elevated Temperature Creep <span class="hlt">Deformation</span> in Solid Solution <001> NiAL-3.6Ti Single Crystals</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Whittenberger, J. Daniel; Noebe, Ronald D.; Darolia, Ram</p> <p>2003-01-01</p> <p>The 1100 to 1500 K slow plastic strain rate compressive properties of <001> oriented NiAl-3.6Ti single crystals have been measured, and the results suggests that two <span class="hlt">deformation</span> processes exist. While the intermediate temperature/faster strain rate mechanism is uncertain, plastic flow at elevated temperature/slower strain rates in NiAl-3.6Ti appears to be controlled by solute drag as described by the Cottrell-Jaswon solute drag model for gliding b = a(sub 0)<101> dislocations. While the calculated activation <span class="hlt">energy</span> of <span class="hlt">deformation</span> is much higher (approximately 480 kJ/mol) than the activation <span class="hlt">energy</span> for diffusion (approximately 290 kJ/mol) used in the Cottrell-Jaswon creep model, a forced temperature compensated - power law fit using the activation <span class="hlt">energy</span> for diffusion was able to adequately (greater than 90%) predict the observed creep properties. Thus we conclude that the rejection of a diffusion controlled mechanism can not be simply based on a large numerical difference between the activation <span class="hlt">energies</span> for <span class="hlt">deformation</span> and diffusion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29055333','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29055333"><span>Anisotropic kinetic <span class="hlt">energy</span> <span class="hlt">release</span> and gyroscopic behavior of CO2 super rotors from an optical centrifuge.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Murray, Matthew J; Ogden, Hannah M; Mullin, Amy S</p> <p>2017-10-21</p> <p>An optical centrifuge is used to generate an ensemble of CO 2 super rotors with oriented angular momentum. The collision dynamics and <span class="hlt">energy</span> transfer behavior of the super rotor molecules are investigated using high-resolution transient IR absorption spectroscopy. New multipass IR detection provides improved sensitivity to perform polarization-dependent transient studies for rotational states with 76 ≤ J ≤ 100. Polarization-dependent measurements show that the collision-induced kinetic <span class="hlt">energy</span> <span class="hlt">release</span> is spatially anisotropic and results from both near-resonant <span class="hlt">energy</span> transfer between super rotor molecules and non-resonant <span class="hlt">energy</span> transfer between super rotors and thermal molecules. J-dependent studies show that the extent and duration of the orientational anisotropy increase with rotational angular momentum. The super rotors exhibit behavior akin to molecular gyroscopes, wherein molecules with larger amounts of angular momentum are less likely to change their angular momentum orientation through collisions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JChPh.147o4309M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JChPh.147o4309M"><span>Anisotropic kinetic <span class="hlt">energy</span> <span class="hlt">release</span> and gyroscopic behavior of CO2 super rotors from an optical centrifuge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Murray, Matthew J.; Ogden, Hannah M.; Mullin, Amy S.</p> <p>2017-10-01</p> <p>An optical centrifuge is used to generate an ensemble of CO2 super rotors with oriented angular momentum. The collision dynamics and <span class="hlt">energy</span> transfer behavior of the super rotor molecules are investigated using high-resolution transient IR absorption spectroscopy. New multipass IR detection provides improved sensitivity to perform polarization-dependent transient studies for rotational states with 76 ≤ J ≤ 100. Polarization-dependent measurements show that the collision-induced kinetic <span class="hlt">energy</span> <span class="hlt">release</span> is spatially anisotropic and results from both near-resonant <span class="hlt">energy</span> transfer between super rotor molecules and non-resonant <span class="hlt">energy</span> transfer between super rotors and thermal molecules. J-dependent studies show that the extent and duration of the orientational anisotropy increase with rotational angular momentum. The super rotors exhibit behavior akin to molecular gyroscopes, wherein molecules with larger amounts of angular momentum are less likely to change their angular momentum orientation through collisions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/14162','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/14162"><span>Impact of <span class="hlt">Released</span> Fual Moisture on Atmospheric Dynamics</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Brian E. Potter</p> <p>2003-01-01</p> <p>A common component of fire incident reports and prescribed burn preparations is an estimate of the <span class="hlt">energy</span> that was or will be <span class="hlt">released</span> by the fire. Typically, this is based on the <span class="hlt">energy</span> <span class="hlt">released</span> by combustion of the fuel load, reduced to account for the <span class="hlt">energy</span> that is required to evaporate moisture in the fuel materials. (e.g., Byram 1959, Anderson 1968, Simard et al...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PSST...23d3001D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PSST...23d3001D"><span>Non-thermal plasma instabilities induced by <span class="hlt">deformation</span> of the electron <span class="hlt">energy</span> distribution function</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dyatko, N. A.; Kochetov, I. V.; Napartovich, A. P.</p> <p>2014-08-01</p> <p>Non-thermal plasma is a key component in gas lasers, microelectronics, medical applications, waste gas cleaners, ozone generators, plasma igniters, flame holders, flow control in high-speed aerodynamics and others. A specific feature of non-thermal plasma is its high sensitivity to variations in governing parameters (gas composition, pressure, pulse duration, E/N parameter). This sensitivity is due to complex <span class="hlt">deformations</span> of the electron <span class="hlt">energy</span> distribution function (EEDF) shape induced by variations in electric field strength, electron and ion number densities and gas excitation degree. Particular attention in this article is paid to mechanisms of instabilities based on non-linearity of plasma properties for specific conditions: gas composition, steady-state and decaying plasma produced by the electron beam, or by an electric current pulse. The following effects are analyzed: the negative differential electron conductivity; the absolute negative electron mobility; the stepwise changes of plasma properties induced by the EEDF bi-stability; thermo-current instability and the constriction of the glow discharge column in rare gases. Some of these effects were observed experimentally and some of them were theoretically predicted and still wait for experimental confirmation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NatSR...745583C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NatSR...745583C"><span>Corrugated Textile based Triboelectric Generator for Wearable <span class="hlt">Energy</span> Harvesting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, A. Young; Lee, Chang Jun; Park, Jiwon; Kim, Dogyun; Kim, Youn Tae</p> <p>2017-03-01</p> <p>Triboelectric <span class="hlt">energy</span> harvesting has been applied to various fields, from large-scale power generation to small electronics. Triboelectric <span class="hlt">energy</span> is generated when certain materials come into frictional contact, e.g., static electricity from rubbing a shoe on a carpet. In particular, textile-based triboelectric <span class="hlt">energy</span>-harvesting technologies are one of the most promising approaches because they are not only flexible, light, and comfortable but also wearable. Most previous textile-based triboelectric generators (TEGs) generate <span class="hlt">energy</span> by vertically pressing and rubbing something. However, we propose a corrugated textile-based triboelectric generator (CT-TEG) that can generate <span class="hlt">energy</span> by stretching. Moreover, the CT-TEG is sewn into a corrugated structure that contains an effective air gap without additional spacers. The resulting CT-TEG can generate considerable <span class="hlt">energy</span> from various <span class="hlt">deformations</span>, not only by pressing and rubbing but also by stretching. The maximum output performances of the CT-TEG can reach up to 28.13 V and 2.71 μA with stretching and <span class="hlt">releasing</span> motions. Additionally, we demonstrate the generation of sufficient <span class="hlt">energy</span> from various activities of a human body to power about 54 LEDs. These results demonstrate the potential application of CT-TEGs for self-powered systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMMR51B2710K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMMR51B2710K"><span>The Time-Dependency of <span class="hlt">Deformation</span> in Porous Carbonate Rocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kibikas, W. M.; Lisabeth, H. P.; Zhu, W.</p> <p>2016-12-01</p> <p>Porous carbonate rocks are natural reservoirs for freshwater and hydrocarbons. More recently, due to their potential for geothermal <span class="hlt">energy</span> generation as well as carbon sequestration, there are renewed interests in better understanding of the <span class="hlt">deformation</span> behavior of carbonate rocks. We conducted a series of <span class="hlt">deformation</span> experiments to investigate the effects of strain rate and pore fluid chemistry on rock strength and transport properties of porous limestones. Indiana limestone samples with initial porosity of 16% are <span class="hlt">deformed</span> at 25 °C under effective pressures of 10, 30, and 50 MPa. Under nominally dry conditions, the limestone samples are <span class="hlt">deformed</span> under 3 different strain rates, 1.5 x 10-4 s-1, 1.5 x 10-5 s-1 and 1.5 x 10-6 s-1 respectively. The experimental results indicate that the mechanical behavior is both rate- and pressure-dependent. At low confining pressures, post-yielding <span class="hlt">deformation</span> changes from predominantly strain softening to strain hardening as strain rate decreases. At high confining pressures, while all samples exhibit shear-enhanced compaction, decreasing strain rate leads to an increase in compaction. Slower strain rates enhance compaction at all confining pressure conditions. The rate-dependence of <span class="hlt">deformation</span> behaviors of porous carbonate rocks at dry conditions indicates there is a strong visco-elastic coupling for the degradation of elastic modulus with increasing plastic <span class="hlt">deformation</span>. In fluid saturated samples, inelastic strain of limestone is partitioned among low temperature plasticity, cataclasis and solution transport. Comparison of inelastic behaviors of samples <span class="hlt">deformed</span> with distilled water and CO2-saturated aqueous solution as pore fluids provide experimental constraints on the relative activities of the various mechanisms. Detailed microstructural analysis is conducted to take into account the links between stress, microstructure and the inelastic behavior and failure mechanisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018IJMPD..2750025S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018IJMPD..2750025S"><span><span class="hlt">Deformation</span> of the quintom cosmological model and its consequences</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sadeghi, J.; Pourhassan, B.; Nekouee, Z.; Shokri, M.</p> <p></p> <p>In this paper, we investigate the effects of noncommutative phase-space on the quintom cosmological model. In that case, we discuss about some cosmological parameters and show that they depend on the <span class="hlt">deformation</span> parameters. We find that the noncommutative parameter plays important role which helps to re-arrange the divergency of cosmological constant. We draw time-dependent scale factor and investigate the effect of noncommutative parameters. Finally, we take advantage from noncommutative phase-space and obtain the <span class="hlt">deformed</span> Lagrangian for the quintom model. In order to discuss some cosmological phenomena as dark <span class="hlt">energy</span> and inflation, we employ Noether symmetry.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/874876','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/874876"><span>Direct charge radioisotope activation and power generation</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Lal, Amit; Li, Hui; Blanchard, James P.; Henderson, Douglass L.</p> <p>2002-01-01</p> <p>An activator has a base on which is mounted an elastically <span class="hlt">deformable</span> micromechanical element that has a section that is free to be displaced toward the base. An absorber of radioactively emitted particles is formed on the base or the displaceable section of the <span class="hlt">deformable</span> element and a source is formed on the other of the displaceable section or the base facing the absorber across a small gap. The radioactive source emits charged particles such as electrons, resulting in a buildup of charge on the absorber, drawing the absorber and source together and storing mechanical <span class="hlt">energy</span> as the <span class="hlt">deformable</span> element is bent. When the force between the absorber and the source is sufficient to bring the absorber into effective electrical contact with the source, discharge of the charge between the source and absorber allows the <span class="hlt">deformable</span> element to spring back, <span class="hlt">releasing</span> the mechanical <span class="hlt">energy</span> stored in the element. An electrical generator such as a piezoelectric transducer may be secured to the <span class="hlt">deformable</span> element to convert the <span class="hlt">released</span> mechanical <span class="hlt">energy</span> to electrical <span class="hlt">energy</span> that can be used to provide power to electronic circuits.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvC..94f4302K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvC..94f4302K"><span><span class="hlt">Deformation</span>-induced splitting of the isoscalar E 0 giant resonance: Skyrme random-phase-approximation analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kvasil, J.; Nesterenko, V. O.; Repko, A.; Kleinig, W.; Reinhard, P.-G.</p> <p>2016-12-01</p> <p>The <span class="hlt">deformation</span>-induced splitting of isoscalar giant monopole resonance (ISGMR) is systematically analyzed in a wide range of masses covering medium, rare-earth, actinide, and superheavy axial <span class="hlt">deformed</span> nuclei. The study is performed within the fully self-consistent quasiparticle random-phase-approximation method based on the Skyrme functional. Two Skyrme forces, one with a large (SV-bas) and one with a small (SkP) nuclear incompressibility, are considered. The calculations confirm earlier results that, because of the <span class="hlt">deformation</span>-induced E 0 -E 2 coupling, the isoscalar E 0 resonance attains a double-peak structure and significant <span class="hlt">energy</span> upshift. Our results are compared with available analytic estimations. Unlike earlier studies, we get a smaller <span class="hlt">energy</span> difference between the lower and upper peaks and thus a stronger E 0 -E 2 coupling. This in turn results in more pumping of E 0 strength into the lower peak and more pronounced splitting of ISGMR. We also discuss widths of the peaks and their negligible correlation with <span class="hlt">deformation</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDG11003B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDG11003B"><span><span class="hlt">Deformation</span> of an Elastic Substrate Due to a Resting Sessile Droplet</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bardall, Aaron; Daniels, Karen; Shearer, Michael</p> <p>2017-11-01</p> <p>On a sufficiently soft substrate, a resting fluid droplet will cause significant <span class="hlt">deformation</span> of the substrate. This <span class="hlt">deformation</span> is driven by a combination of capillary forces at the contact line and the fluid pressure at the solid surface. These forces are balanced at the surface by the solid traction stress induced by the substrate <span class="hlt">deformation</span>. Young's Law, which predicts the equilibrium contact angle of the droplet, also indicates an a priori radial force balance for rigid substrates, but not necessarily for soft substrates which <span class="hlt">deform</span> under loading. It remains an open question whether the contact line transmits a non-zero force tangent to the substrate surface in addition to the conventional normal force. This talk will present a model for the static <span class="hlt">deformation</span> of the substrate that includes a non-zero tangential contact line force as well as general interfacial <span class="hlt">energy</span> conditions governing the angle of a two-dimensional droplet. We discuss extensions of this model to non-symmetric droplets and their effect on the static configuration of the droplet/substrate system. NSF #DMS-1517291.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24622435','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24622435"><span>Total knee arthroplasty for severe valgus knee <span class="hlt">deformity</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhou, Xinhua; Wang, Min; Liu, Chao; Zhang, Liang; Zhou, Yixin</p> <p>2014-01-01</p> <p>Primary total knee arthroplasty (TKA) in severe valgus knees may prove challenging, and choice of implant depends on the severity of the valgus <span class="hlt">deformity</span> and the extent of soft-tissue <span class="hlt">release</span>. The purpose of this study was to review 8 to 11 years (mean, 10 years) follow-up results of primary TKA for varient-III valgus knee <span class="hlt">deformity</span> with use of different type implants. Between January 2002 and January 2005, 20 women and 12 men, aged 47 to 63 (mean, 57.19 ± 6.08) years old, with varient-III valgus knees underwent primary TKA. Of the 32 patients, 37 knees had varient-III <span class="hlt">deformities</span>. Pie crusting was carefully performed with small, multiple inside-out incisions, bone resection balanced the knee in lieu of soft tissue <span class="hlt">releases</span> that were not used in the series. Cruciate-retaining knees (Gemini MKII, Link Company, Germany) were used in 13 knees, Genesis II (Simth & Nephew Company, USA) in 14 knees, and hinged knee (Endo-Model Company, Germany) in 10 knees. In five patients with bilateral variant-III TKAs, three patients underwent 1-stage bilateral procedures, and two underwent 2-stage procedures. All implants were cemented and the patella was not resurfaced. The Hospital for Special Surgery (HSS) knee score was assessed. Patients were followed up from 8 to 11 years. The mean HSS knee score were improved from 50.33 ± 11.60 to 90.06 ± 3.07 (P < 0.001). The mean tibiofemoral alignment were improved from valgus 32.72° ± 9.68° pre-operation to 4.89° ± 0.90° post-operation (P < 0.001). The mean range of motion were improved from 93.72° ± 23.69° pre-operation to 116.61 ± 16.29° post-operation (P < 0.001). No patients underwent revision. One patient underwent open reduction and internal fixation using femoral condylar plates for supracondylar femoral fractures secondary to a fall at three years. Three patients developed transient peroneal nerve palsies, which resolved within nine months. Two patients developed symptomatic deep vein thrombosis that was managed with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.908a2018K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.908a2018K"><span>Influence of ceramic dental crown coating substrate thickness ratio on strain <span class="hlt">energy</span> <span class="hlt">release</span> rate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Khasnulhadi, K.; Daud, R.; Mat, F.; Noor, S. N. F. M.; Basaruddin, K. S.; Sulaiman, M. H.</p> <p>2017-10-01</p> <p>This paper presents the analysis of coating substrate thickness ratio effect on the crown coating fracture behaviour. The bi-layer material is examined under four point bending with pre-crack at the bottom of the core material by using finite element. Three different coating thickness of core/substrate was tested which is 1:1, 1:2 and 2:1. The fracture parameters are analysed based on bilayer and homogenous elastic interaction. The result shows that the ratio thickness of core/veneer provided a significant effect on <span class="hlt">energy</span> <span class="hlt">release</span> rate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvD..95a5001G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvD..95a5001G"><span>q -<span class="hlt">deformed</span> statistics and the role of light fermionic dark matter in SN1987A cooling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guha, Atanu; J, Selvaganapathy; Das, Prasanta Kumar</p> <p>2017-01-01</p> <p>The light dark matter (≃1 - 30 MeV ) particles pair produced in electron-positron annihilation e-e+→ γ χ χ ¯ inside the supernova core can take away the <span class="hlt">energy</span> <span class="hlt">released</span> in the supernova SN1987A explosion. Working within the formalism of q -<span class="hlt">deformed</span> statistics [with the average value of the supernovae core temperature (fluctuating) being TS N=30 MeV ] and using the Raffelt's criterion on the emissivity for any new channel ɛ ˙ (e+e-→χ χ ¯ )≤1 019 erg g-1 s-1 , we find that as the <span class="hlt">deformation</span> parameter q changes from 1.0 (undeformed scenario) to 1.1 (<span class="hlt">deformed</span> scenario), the lower bound on the scale Λ of the dark matter effective theory varies from 3.3 ×1 06 TeV to 3.2 ×1 07 TeV for a dark matter fermion of mass mχ=30 MeV . Using the optical depth criteria on the free streaming of the dark matter fermion, we find the lower bound on Λ ˜1 08 TeV for mχ=30 MeV . In a scenario, where the dark matter fermions are pair produced in the outermost sector of the supernova core [with radius 0.9 Rc≤r ≤Rc , Rc(=10 km ) being the supernova core radius or the radius of protoneutron star], we find that the bound on Λ (˜3 ×1 07 TeV ) obtained from SN cooling criteria (Raffelt's criteria) is comparable with the bound obtained from free streaming (optical depth criterion) for light fermion dark matter of mass mχ=10 - 30 MeV .</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ApPhL.109s1909Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ApPhL.109s1909Y"><span>Atomistic simulation on the plastic <span class="hlt">deformation</span> and fracture of bio-inspired graphene/Ni nanocomposites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Zhenyu; Wang, Dandan; Lu, Zixing; Hu, Wenjun</p> <p>2016-11-01</p> <p>Molecular dynamics simulations were performed to investigate the plastic <span class="hlt">deformation</span> and fracture behaviors of bio-inspired graphene/metal nanocomposites, which have a "brick-and-mortar" nanostructure, consisting of hard graphene single-layers embedded in a soft Ni matrix. The plastic <span class="hlt">deformation</span> mechanisms of the nanocomposites were analyzed as well as their effects on the mechanical properties with various geometrical variations. It was found that the strength and ductility of the metal matrix can be highly enhanced with the addition of the staggered graphene layers, and the plastic <span class="hlt">deformation</span> can be attributed to the interfacial sliding, dislocation nucleation, and cracks' combination. The strength of the nanocomposites strongly depends on the length scale of the nanostructure and the interlayer distance as well. In addition, slip at the interface <span class="hlt">releases</span> the stress in graphene layers, leading to the stress distribution on the graphene more uniform. The present results are expected to contribute to the design of the nanolayered graphene/metal composites with high performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhDT.......217A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhDT.......217A"><span>Active and long-lived permanent forearc <span class="hlt">deformation</span> driven by the subduction seismic cycle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aron Melo, Felipe Alejandro</p> <p></p> <p> above background levels occurred contemporaneous to megathrust ruptures. That correlation is stronger for normal fault events than reverse or strike-slip crustal earthquakes. More importantly, for any given megathrust the summation of the Mw accounted by the forearc normal fault aftershocks appears to have a positive linear correlation with the Mw of the subduction earthquake -- the larger the megathrust the larger the <span class="hlt">energy</span> <span class="hlt">released</span> by forearc events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3691712','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3691712"><span>Large <span class="hlt">Deformation</span> and Adhesive Contact Studies of Axisymmetric Membranes</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Laprade, Evan J.; Long, Rong; Pham, Jonathan; Lawrence, Jimmy; Emrick, Todd; Crosby, Alfred; Hui, Chung-Yuen; Shull, Kenneth R.</p> <p>2013-01-01</p> <p>A model membrane contact system consisting of an acrylic copolymer membrane and polydimethyl-siloxane substrate was utilized to evaluate a recently developed nonlinear large-<span class="hlt">deformation</span> adhesive contact analysis. Direct measurements of the local membrane apex strain during non-contact inflation indicated that the neo-Hookean model provides an accurate measure of membrane strain and supports its use as the strain <span class="hlt">energy</span> function for the analysis. A time dependent modulus emerges from the analysis, with principal tensions obtained from a comparison of predicted and experimental membrane profiles. A displacement controlled geometry was more easily modeled than the pressure controlled geometry, the applicability of the analysis was limited by wrinkling instabilities. The substantial viscoelastic behavior of these membranes made it difficult to describe the entire membrane with a single modulus, given the nonuniform <span class="hlt">deformation</span> history of the membranes. Given the difficulty in determining membrane tension from the measured pressure and profile fits using the model, the peel <span class="hlt">energy</span> was used as a simpler measure of adhesion. Using an analytical balance in the displacement controlled geometry, the membrane tension at the contact line was directly measured. Coupled with contact angle imaging, the peel <span class="hlt">energy</span> was determined. For the model membranes studied, this peel <span class="hlt">energy</span> described the membrane/substrate adhesive interactions quite well, giving well-defined peel <span class="hlt">energies</span> that were independent of the detailed strain state of the membrane. PMID:23289644</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18851297','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18851297"><span><span class="hlt">Deformation</span> induced microtwins and stacking faults in aluminum single crystal.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Han, W Z; Cheng, G M; Li, S X; Wu, S D; Zhang, Z F</p> <p>2008-09-12</p> <p>Microtwins and stacking faults in plastically <span class="hlt">deformed</span> aluminum single crystal were successfully observed by high-resolution transmission electron microscope. The occurrence of these microtwins and stacking faults is directly related to the specially designed crystallographic orientation, because they were not observed in pure aluminum single crystal or polycrystal before. Based on the new finding above, we propose a universal dislocation-based model to judge the preference or not for the nucleation of <span class="hlt">deformation</span> twins and stacking faults in various face-centered-cubic metals in terms of the critical stress for dislocation glide or twinning by considering the intrinsic factors, such as stacking fault <span class="hlt">energy</span>, crystallographic orientation, and grain size. The new finding of <span class="hlt">deformation</span> induced microtwins and stacking faults in aluminum single crystal and the proposed model should be of interest to a broad community.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_17 --> <div id="page_18" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="341"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.fs.usda.gov/treesearch/pubs/7473','TREESEARCH'); return false;" href="https://www.fs.usda.gov/treesearch/pubs/7473"><span>Spline curve matching with sparse knot sets: applications to <span class="hlt">deformable</span> shape detection and recognition</span></a></p> <p><a target="_blank" href="http://www.fs.usda.gov/treesearch/">Treesearch</a></p> <p>Sang-Mook Lee; A. Lynn Abbott; Neil A. Clark; Philip A. Araman</p> <p>2003-01-01</p> <p>Splines can be used to approximate noisy data with a few control points. This paper presents a new curve matching method for <span class="hlt">deformable</span> shapes using two-dimensional splines. In contrast to the residual error criterion, which is based on relative locations of corresponding knot points such that is reliable primarily for dense point sets, we use <span class="hlt">deformation</span> <span class="hlt">energy</span> of...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23897061','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23897061"><span>Highly <span class="hlt">deformation</span>-tolerant carbon nanotube sponges as supercapacitor electrodes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Peixu; Kong, Chuiyan; Shang, Yuanyuan; Shi, Enzheng; Yu, Yuntao; Qian, Weizhong; Wei, Fei; Wei, Jinquan; Wang, Kunlin; Zhu, Hongwei; Cao, Anyuan; Wu, Dehai</p> <p>2013-09-21</p> <p>Developing flexible and <span class="hlt">deformable</span> supercapacitor electrodes based on porous materials is of high interest in <span class="hlt">energy</span> related fields. Here, we show that carbon nanotube sponges, consisting of highly porous conductive networks, can serve as compressible and <span class="hlt">deformation</span>-tolerant supercapacitor electrodes in aqueous or organic electrolytes. In aqueous electrolytes, the sponges maintain a similar specific capacitance (>90% of the original value) under a predefined compressive strain of 50% (corresponding to a volume reduction of 50%), and retain more than 70% of the original capacitance under 80% strain while the volume normalized capacitance increases by 3-fold. The sponge electrode maintains a stable performance after 1000 large strain compression cycles. A coin-shaped cell assembled with these sponges shows excellent stability over 15,000 charging cycles with negligible degradation after 500 cycles. Our results indicate that carbon nanotube sponges have the potential to fabricate <span class="hlt">deformable</span> supercapacitor electrodes with stable performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19..248D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19..248D"><span>Pyrite <span class="hlt">deformation</span> and connections to gold mobility: insight from micro-structural analysis and trace element mapping</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dubosq, Renelle; Rogowitz, Anna; Lawley, Christopher; Schneider, David; Jackson, Simon</p> <p>2017-04-01</p> <p>Pyrite is an important and ubiquitous gold-bearing phase in many orogenic gold deposits making the study of its <span class="hlt">deformation</span> behaviour under metamorphic conditions crucial to the understanding of gold (re)mobilization. However, pyrite <span class="hlt">deformation</span> mechanisms and their influence on the retention or <span class="hlt">release</span> of trace elements during <span class="hlt">deformation</span> and metamorphism remain poorly understood. We propose a syn- to post-peak metamorphic and <span class="hlt">deformation</span> driven gold upgrading model where gold is remobilized through <span class="hlt">deformation</span>-induced diffusion pathways in the form of substructures in pyrite. The middle amphibolite facies assemblage (actinolite-biotite-plagioclase-almandine) of the Detour Lake deposit (Canada) makes it an ideal study area due to maximum temperatures reaching 550°C, exceeding the conditions for plastic <span class="hlt">deformation</span> in pyrite (450°C). The world-class Detour Lake deposit, containing 16.4 Moz of Au at 1 g/t, is a Neoarchean orogenic gold ore body located in the northern Abitibi district within the Superior Province. The mine is situated along the high strain, sub-vertical ductile-brittle Sunday Lake <span class="hlt">Deformation</span> Zone (SLDZ) parallel to the broadly E-W trending Abitibi greenstone belt. Herein we combine orientation contrast (OC) forescatter imaging, electron backscatter diffraction (EBSD) and 2D laser ablation inductively coupled plasma mass spectrometry (LA-ICP-MS) trace element pyrite mapping to evaluate the influence of pyrite brittle and plastic <span class="hlt">deformation</span> on the <span class="hlt">release</span> of trace elements during syn-metamorphic gold remobilization. Local misorientation patterns in pyrite exhibit parallel bands that can be described by continuous rotation around one of the <100> axes, whereas higher strain areas reveal more heterogeneous misorientation patterns and the development of low-angle grain boundaries with late fractures indicative of dislocation creep and strain hardening. These late fractures are an important micro-structural setting for gold and clusters of precious</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.7949B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.7949B"><span>Analysis of Mining Terrain <span class="hlt">Deformation</span> Characteristics with <span class="hlt">Deformation</span> Information System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Blachowski, Jan; Milczarek, Wojciech; Grzempowski, Piotr</p> <p>2014-05-01</p> <p>Mapping and prediction of mining related <span class="hlt">deformations</span> of the earth surface is an important measure for minimising threat to surface infrastructure, human population, the environment and safety of the mining operation itself arising from underground extraction of useful minerals. The number of methods and techniques used for monitoring and analysis of mining terrain <span class="hlt">deformations</span> is wide and increasing with the development of geographical information technologies. These include for example: terrestrial geodetic measurements, global positioning systems, remote sensing, spatial interpolation, finite element method modelling, GIS based modelling, geological modelling, empirical modelling using the Knothe theory, artificial neural networks, fuzzy logic calculations and other. The aim of this paper is to introduce the concept of an integrated <span class="hlt">Deformation</span> Information System (DIS) developed in geographic information systems environment for analysis and modelling of various spatial data related to mining activity and demonstrate its applications for mapping and visualising, as well as identifying possible mining terrain <span class="hlt">deformation</span> areas with various spatial modelling methods. The DIS concept is based on connected modules that include: the spatial database - the core of the system, the spatial data collection module formed by: terrestrial, satellite and remote sensing measurements of the ground changes, the spatial data mining module for data discovery and extraction, the geological modelling module, the spatial data modeling module with data processing algorithms for spatio-temporal analysis and mapping of mining <span class="hlt">deformations</span> and their characteristics (e.g. <span class="hlt">deformation</span> parameters: tilt, curvature and horizontal strain), the multivariate spatial data classification module and the visualization module allowing two-dimensional interactive and static mapping and three-dimensional visualizations of mining ground characteristics. The Systems's functionality has been presented on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007NIMPB.255..365K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007NIMPB.255..365K"><span>High <span class="hlt">energy</span> X-ray CT study on the central void formations and the fuel pin <span class="hlt">deformations</span> of FBR fuel assemblies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Katsuyama, Kozo; Nagamine, Tsuyoshi; Matsumoto, Shin-ichiro; Sato, Seichi</p> <p>2007-02-01</p> <p>The central void formations and <span class="hlt">deformations</span> of fuel pins were investigated in fuel assemblies irradiated to high burn-up, using a non-destructive X-ray CT (computer tomography) technique. In this X-ray CT, the effect of strong gamma ray activity could be reduced to a negligible degree by using the pulse of a high <span class="hlt">energy</span> X-ray source and detecting the intensity of the transmitted X-rays in synchronization with the generated X-rays. Clear cross-sectional images of fuel assemblies irradiated to high burn-up in a fast breeder reactor were successively obtained, in which the wrapping wires, cladding, pellets and central voids could be distinctly seen. The diameter of a typical central void measured by X-ray CT agreed with the one obtained by ceramography within an error of 0.1 mm. Based on this result, the dependence of the central void diameter on the linear heating rate was analyzed. In addition, the <span class="hlt">deformation</span> behavior of a fuel pin along its axial direction could be analyzed from 20 stepwise X-ray cross-sectional images obtained in a small interval, and the results obtained showed a good agreement with the predictions calculated by two computer codes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23890795','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23890795"><span>Minimally invasive soft tissue <span class="hlt">release</span> of foot and ankle contracture secondary to stroke.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Boffeli, Troy J; Collier, Rachel C</p> <p>2014-01-01</p> <p>Lower extremity contracture associated with stroke commonly results in a nonreducible, spastic equinovarus <span class="hlt">deformity</span> of the foot and ankle. Rigid contracture <span class="hlt">deformity</span> leads to gait instability, pain, bracing difficulties, and ulcerations. The classic surgical approach for stroke-related contracture of the foot and ankle has been combinations of tendon lengthening, tendon transfer, osteotomy, and joint fusion procedures. Recovery after traditional foot and ankle reconstructive surgery requires a period of non-weightbearing that is not typically practical for these patients. Little focus has been given in published studies on minimally invasive soft tissue <span class="hlt">release</span> of contracture. We present the case of a 61-year-old female with an equinovarus foot contracture <span class="hlt">deformity</span> secondary to stroke. The patient underwent Achilles tendon lengthening, posterior tibial tendon Z lengthening, and digital flexor tenotomy of each toe with immediate weightbearing in a walking boot, followed by transition to an ankle-foot orthosis. The surgical principles and technique tips are presented to demonstrate our minimally invasive approach to <span class="hlt">release</span> of foot and ankle contracture secondary to stroke. The main goal of this approach is to improve foot and ankle alignment for ease of bracing, which, in turn, will improve gait, reduce the risk of falls, decrease pain, and avoid the development of pressure sores. Copyright © 2014 American College of Foot and Ankle Surgeons. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999MMTA...30.2391K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999MMTA...30.2391K"><span><span class="hlt">Deformation</span> bands, the LEDS theory, and their importance in texture development: Part II. Theoretical conclusions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuhlmann-Wilsdorf, D.</p> <p>1999-09-01</p> <p>The facts regarding “regular” <span class="hlt">deformation</span> bands (DBs) outlined in Part I of this series of articles are related to the low-<span class="hlt">energy</span> dislocation structure (LEDS) theory of dislocation-based plasticity. They prompt an expansion of the theory by including the stresses due to strain gradients on account of changing selections of slip systems to the previously known dislocation driving forces. This last and until now neglected driving force is much smaller than the components considered hitherto, principally due to the applied stress and to mutual stress-screening among neighbor dislocations. As a result, it permits a near-proof of the LEDS hypothesis, to wit that among all structures which, in principle, are accessible to the dislocations, that one is realized which has the lowest free <span class="hlt">energy</span>. Specifically, the temperature rises that would result from annihilating the largest DBs amount to only several millidegrees Centigrade, meaning that they, and by implication the entire dislocation structures, are close to thermodynamical equilibrium. This is in stark contrast to the assumption of the presently widespread self-organizing dislocation structures (SODS) modeling that plastic <span class="hlt">deformation</span> occurs far from equilibrium and is subject to Prigogine’s thermodynamics of <span class="hlt">energy</span>-flow-through systems. It also holds out promise for future rapid advances in the construction of constitutive equations, since the LEDS hypothesis is the principal basis of the LEDS theory of plastic <span class="hlt">deformation</span> and follows directly from the second law of thermodynamics in conjunction with Newton’s third law. By contrast, all other known models of metal plasticity are in conflict with the LEDS hypothesis. In regard to texture modeling, the present analysis shows that Taylor’s criterion of minimum plastic work is incorrect and should be replaced by the criterion of minimum free <span class="hlt">energy</span> in the stressed state. Last, the LEDS hypothesis is but a special case of the more general low-<span class="hlt">energy</span> structure</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810008636&hterms=hmx&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dhmx','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810008636&hterms=hmx&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dhmx"><span>Effect of propellant <span class="hlt">deformation</span> on ignition and combustion processes in solid propellant cracks</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kumar, M.; Kuo, K. K.</p> <p>1980-01-01</p> <p>A comprehensive theoretical model was formulated to study the development of convective burning in a solid propellant crack which continually <span class="hlt">deforms</span> due to burning and pressure loading. In the theoretical model, the effect of interrelated structural <span class="hlt">deformation</span> and combustion processes was taken into account by considering (1) transient, one dimensional mass, momentum, and <span class="hlt">energy</span> conservation equations in the gas phase; (2) a transient, one dimensional heat conduction equation in the solid phase; and (3) quasi-static <span class="hlt">deformation</span> of the two dimensional, linear viscoelastic propellant crack caused by pressure loading. Partial closures may generate substantial local pressure peaks along the crack, implying a strong coupling between chamber pressurization, crack combustion, and propellant <span class="hlt">deformation</span>, especially when the cracks are narrow and the chamber pressurization rates high. The maximum pressure in the crack cavity is generally higher than that in the chamber. The initial flame-spreading process is not affected by propellant <span class="hlt">deformation</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EPJD...70..130R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EPJD...70..130R"><span>Kinetic-<span class="hlt">energy</span> <span class="hlt">release</span> distributions of fragment anions from collisions of potassium atoms with D-Ribose and tetrahydrofuran*</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rebelo, André; Cunha, Tiago; Mendes, Mónica; da Silva, Filipe Ferreira; García, Gustavo; Limão-Vieira, Paulo</p> <p>2016-06-01</p> <p>Kinetic-<span class="hlt">energy</span> <span class="hlt">release</span> distributions have been obtained from the width and shapes of the time-of-flight (TOF) negative ion mass peaks formed in collisions of fast potassium atoms with D-Ribose (DR) and tetrahydrofuran (THF) molecules. Recent dissociative ion-pair formation experiments yielding anion formation have shown that the dominant fragment from D-Ribose is OH- [D. Almeida, F. Ferreira da Silva, G. García, P. Limão-Vieira, J. Chem. Phys. 139, 114304 (2013)] whereas in the case of THF is O- [D. Almeida, F. Ferreira da Silva, S. Eden, G. García, P. Limão-Vieira, J. Phys. Chem. A 118, 690 (2014)]. The results for DR and THF show an <span class="hlt">energy</span> distribution profile reminiscent of statistical degradation via vibrational excitation and partly due to direct transformation of the excess <span class="hlt">energy</span> in translational <span class="hlt">energy</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21519079','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21519079"><span>Long-term results of total knee arthroplasty for valgus knees: soft-tissue <span class="hlt">release</span> technique and implant selection.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rajgopal, Ashok; Dahiya, Vivek; Vasdev, Attique; Kochhar, Hemanshu; Tyagi, Vipin</p> <p>2011-04-01</p> <p>To report long-term results of total knee arthroplasty (TKA) for valgus knees. 34 women and 19 men aged 39 to 84 (mean, 74) years with valgus knees underwent primary TKA by a senior surgeon. Of the 78 knees, 43, 29, and 6 had type-I, type-II, and type-III valgus <span class="hlt">deformities</span>, respectively. A preliminary lateral soft-tissue <span class="hlt">release</span> was performed, and the tibia and femur were prepared. The tight lateral structures were <span class="hlt">released</span> using the pie-crusting technique. In 92% of the knees, cruciate-retaining implants were used. In knees with severe <span class="hlt">deformity</span> and medial collateral ligament insufficiency, the posterior cruciate ligament was sacrificed and constrained implants were used. The Hospital for Special Surgery (HSS) knee score was assessed, as were tibiofemoral alignment, range of motion, stability, and evidence of loosening or osteolysis. Patients were followed up for 8 to 14 (mean, 10) years. All knees had a good patellar position and were clinically stable in both mediolateral and anteroposterior planes. No radiolucency was noted. The mean HSS knee score improved from 48 to 91 (p<0.001). The mean tibiofemoral alignment improved from valgus 20 to 5 degrees (p<0.001). The mean range of motion improved from 65 to 110 degrees (p<0.001). One patient developed a deep infection at year 4, and 2 had periprosthetic fractures at years 6 and 8. Adequate lateral soft-tissue <span class="hlt">release</span> is the key to successful TKAs in valgus knees. The choice of implant depends on the severity of the valgus <span class="hlt">deformity</span> and the extent of soft-tissue <span class="hlt">release</span> needed to obtain a stable, balanced flexion and extension gap, in order to achieve minimal constraint with maximum stability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21576739','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21576739"><span>Reconstructing 3D Face Model with Associated Expression <span class="hlt">Deformation</span> from a Single Face Image via Constructing a Low-Dimensional Expression <span class="hlt">Deformation</span> Manifold.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wang, Shu-Fan; Lai, Shang-Hong</p> <p>2011-10-01</p> <p>Facial expression modeling is central to facial expression recognition and expression synthesis for facial animation. In this work, we propose a manifold-based 3D face reconstruction approach to estimating the 3D face model and the associated expression <span class="hlt">deformation</span> from a single face image. With the proposed robust weighted feature map (RWF), we can obtain the dense correspondences between 3D face models and build a nonlinear 3D expression manifold from a large set of 3D facial expression models. Then a Gaussian mixture model in this manifold is learned to represent the distribution of expression <span class="hlt">deformation</span>. By combining the merits of morphable neutral face model and the low-dimensional expression manifold, a novel algorithm is developed to reconstruct the 3D face geometry as well as the facial <span class="hlt">deformation</span> from a single face image in an <span class="hlt">energy</span> minimization framework. Experimental results on simulated and real images are shown to validate the effectiveness and accuracy of the proposed algorithm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JVGR..202..117V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JVGR..202..117V"><span><span class="hlt">Deformation</span> of Copahue volcano: Inversion of InSAR data using a genetic algorithm</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Velez, Maria Laura; Euillades, Pablo; Caselli, Alberto; Blanco, Mauro; Díaz, Jose Martínez</p> <p>2011-04-01</p> <p>The Copahue volcano is one of the most active volcanoes in Argentina with eruptions having been reported as recently as 1992, 1995 and 2000. A <span class="hlt">deformation</span> analysis using the Differential Synthetic Aperture Radar technique (DInSAR) was performed on Copahue-Caviahue Volcanic Complex (CCVC) from Envisat radar images between 2002 and 2007. A <span class="hlt">deformation</span> rate of approximately 2 cm/yr was calculated, located mostly on the north-eastern flank of Copahue volcano, and assumed to be constant during the period of the interferograms. The geometry of the source responsible for the <span class="hlt">deformation</span> was evaluated from an inversion of the mean velocity <span class="hlt">deformation</span> measurements using two different models based on pressure sources embedded in an elastic homogeneous half-space. A genetic algorithm was applied as an optimization tool to find the best fit source. Results from inverse modelling indicate that a source located beneath the volcano edifice at a mean depth of 4 km is producing a volume change of approximately 0.0015 km/yr. This source was analysed considering the available studies of the area, and a conceptual model of the volcanic-hydrothermal system was designed. The source of <span class="hlt">deformation</span> is related to a depressurisation of the system that results from the <span class="hlt">release</span> of magmatic fluids across the boundary between the brittle and plastic domains. These leakages are considered to be responsible for the weak phreatic eruptions recently registered at the Copahue volcano.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.4136D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.4136D"><span><span class="hlt">Deformation</span> mechanisms in experimentally <span class="hlt">deformed</span> Boom Clay</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Desbois, Guillaume; Schuck, Bernhard; Urai, Janos</p> <p>2016-04-01</p> <p>Bulk mechanical and transport properties of reference claystones for deep disposal of radioactive waste have been investigated since many years but little is known about microscale <span class="hlt">deformation</span> mechanisms because accessing the relevant microstructure in these soft, very fine-grained, low permeable and low porous materials remains difficult. Recent development of ion beam polishing methods to prepare high quality damage free surfaces for scanning electron microscope (SEM) is opening new fields of microstructural investigation in claystones towards a better understanding of the <span class="hlt">deformation</span> behavior transitional between rocks and soils. We present results of Boom Clay <span class="hlt">deformed</span> in a triaxial cell in a consolidated - undrained test at a confining pressure of 0.375 MPa (i.e. close to natural value), with σ1 perpendicular to the bedding. Experiments stopped at 20 % strain. As a first approximation, the plasticity of the sample can be described by a Mohr-Coulomb type failure envelope with a coefficient of cohesion C = 0.117 MPa and an internal friction angle ϕ = 18.7°. After <span class="hlt">deformation</span> test, the bulk sample shows a shear zone at an angle of about 35° from the vertical with an offset of about 5 mm. We used the "Lamipeel" method that allows producing a permanent absolutely plane and large size etched micro relief-replica in order to localize and to document the shear zone at the scale of the <span class="hlt">deformed</span> core. High-resolution imaging of microstructures was mostly done by using the BIB-SEM method on key-regions identified after the "Lamipeel" method. Detailed BIB-SEM investigations of shear zones show the following: the boundaries between the shear zone and the host rock are sharp, clay aggregates and clastic grains are strongly reoriented parallel to the shear direction, and the porosity is significantly reduced in the shear zone and the grain size is smaller in the shear zone than in the host rock but there is no evidence for broken grains. Comparison of microstructures</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70021098','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70021098"><span>A generalized law for brittle <span class="hlt">deformation</span> of Westerly granite</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Lockner, D.A.</p> <p>1998-01-01</p> <p>A semiempirical constitutive law is presented for the brittle <span class="hlt">deformation</span> of intact Westerly granite. The law can be extended to larger displacements, dominated by localized <span class="hlt">deformation</span>, by including a displacement-weakening break-down region terminating in a frictional sliding regime often described by a rate- and state-dependent constitutive law. The intact <span class="hlt">deformation</span> law, based on an Arrhenius type rate equation, relates inelastic strain rate to confining pressure Pc, differential stress ????, inelastic strain ??i, and temperature T. The basic form of the law for <span class="hlt">deformation</span> prior to fault nucleation is In ????i = c - (E*/RT) + (????/a??o)sin-??(???? i/2??o) where ??o and ??o are normalization constants (dependent on confining pressure), a is rate sensitivity of stress, and ?? is a shape parameter. At room temperature, eight experimentally determined coefficients are needed to fully describe the stress-strain-strain rate response for Westerly granite from initial loading to failure. Temperature dependence requires apparent activation <span class="hlt">energy</span> (E* ??? 90 kJ/mol) and one additional experimentally determined coefficient. The similarity between the prefailure constitutive law for intact rock and the rate- and state-dependent friction laws for frictional sliding on fracture surfaces suggests a close connection between these brittle phenomena.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApPhL.112r1905W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApPhL.112r1905W"><span>Controllable helical <span class="hlt">deformations</span> on printed anisotropic composite soft actuators</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Dong; Li, Ling; Serjouei, Ahmad; Dong, Longteng; Weeger, Oliver; Gu, Guoying; Ge, Qi</p> <p>2018-04-01</p> <p>Helical shapes are ubiquitous in both nature and engineering. However, the development of soft actuators and robots that mimic helical motions has been hindered primarily due to the lack of efficient modeling approaches that take into account the material anisotropy and the directional change of the external loading point. In this work, we present a theoretical framework for modeling controllable helical <span class="hlt">deformations</span> of cable-driven, anisotropic, soft composite actuators. The framework is based on the minimum potential <span class="hlt">energy</span> method, and its model predictions are validated by experiments, where the microarchitectures of the soft composite actuators can be precisely defined by 3D printing. We use the developed framework to investigate the effects of material and geometric parameters on helical <span class="hlt">deformations</span>. The results show that material stiffness, volume fraction, layer thickness, and fiber orientation can be used to control the helical <span class="hlt">deformation</span> of a soft actuator. In particular, we found that a critical fiber orientation angle exists at which the twist of the actuator changes the direction. Thus, this work can be of great importance for the design and fabrication of soft actuators with tailored <span class="hlt">deformation</span> behavior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA.....1880P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA.....1880P"><span>From progressive to finite <span class="hlt">deformation</span>, and back: the universal <span class="hlt">deformation</span> matrix</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Provost, A.; Buisson, C.; Merle, O.</p> <p>2003-04-01</p> <p>It is widely accepted that any finite strain recorded in the field may be interpreted in terms of the simultaneous combination of a pure shear component with one or several simple shear components. To predict strain in geological structures, approximate solutions may be obtained by multiplying successive small increments of each elementary strain component. A more rigorous method consists in achieving the simultaneous combination in the velocity gradient tensor but solutions already proposed in the literature are valid for special cases only and cannot be used, e.g., for the general combination of a pure shear component and six elementary simple shear components. In this paper, we show that the combination of any strain components is as simple as a mouse click, both analytically and numerically. The finite <span class="hlt">deformation</span> matrix is given by L=exp(L.Δt) where L.Δt is the time-integrated velocity gradient tensor. This method makes it possible to predict finite strain for any combination of strain components. Reciprocally, L.Δt=ln(D) , which allows to unravel the simplest <span class="hlt">deformation</span> history that might be liable for a given finite <span class="hlt">deformation</span>. Given the strain ellipsoid only, it is still possible to constrain the range of compatible <span class="hlt">deformation</span> matrices and thus the range of strain component combinations. Interestingly, certain <span class="hlt">deformation</span> matrices, though geologically sensible, have no real logarithm so cannot be explained by a <span class="hlt">deformation</span> history implying strain rate components with constant proportions, what implies significant changes of the stress field during the history of <span class="hlt">deformation</span>. The study as a whole opens the possibility for further investigations on <span class="hlt">deformation</span> analysis in general, the method could be used wathever the configuration is.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999ChPhL..16..169Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999ChPhL..16..169Z"><span>Octupole <span class="hlt">Deformation</span> Bands of πh11/2 in Neutron-Rich 145,147La Nuclei</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Sheng-jiang; S, Zhu J.; Wang, Mu-ge; J, Hamilton H.; A, Ramayya V.; B, Babu R. S.; W, Ma C.; Long, Gui-lu; Zhu, Ling-yan; Li, Ming; A, Sakhaee; Gan, Cui-yun; Yang, Li-ming; J, Komicki; J, Cole D.; R, Aryaeinejad; M, Drigert W.; J, Rasmussen O.; M, Stoyer A.; S, Chu Y.; K, Gregorich E.; M, Mohar F.; S, Prussin G.; I, Lee Y.; Yu, Oganessian Ts; G, Ter-Akopian M.; A, Daniel V.</p> <p>1999-03-01</p> <p>Octupole <span class="hlt">deformation</span> bands built on πh11/2 orbital in neutron-rich odd-Z 145,147La nuclei have been investigated by measuring the prompt γ-rays emitted from the 252Cf source. The alternating parity band structures and strong E1 transitions observed between negative- and positive-parity bands in both nuclei indicate the octupole <span class="hlt">deformation</span> enhanced by the h11/2 single proton coupling. According to observed <span class="hlt">energy</span> displacements the octupole <span class="hlt">deformation</span> becomes stable at the intermediate spin states.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MSMSE..26c5004A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MSMSE..26c5004A"><span>Influence of the mode of <span class="hlt">deformation</span> on recrystallisation behaviour of titanium through experiments, mean field theory and phase field model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Athreya, C. N.; Mukilventhan, A.; Suwas, Satyam; Vedantam, Srikanth; Subramanya Sarma, V.</p> <p>2018-04-01</p> <p>The influence of the mode of <span class="hlt">deformation</span> on recrystallisation behaviour of Ti was studied by experiments and modelling. Ti samples were <span class="hlt">deformed</span> through torsion and rolling to the same equivalent strain of 0.5. The <span class="hlt">deformed</span> samples were annealed at different temperatures for different time durations and the recrystallisation kinetics were compared. Recrystallisation is found to be faster in the rolled samples compared to the torsion <span class="hlt">deformed</span> samples. This is attributed to the differences in stored <span class="hlt">energy</span> and number of nuclei per unit area in the two modes of <span class="hlt">deformation</span>. Considering decay in stored <span class="hlt">energy</span> during recrystallisation, the grain boundary mobility was estimated through a mean field model. The activation <span class="hlt">energy</span> for recrystallisation obtained from experiments matched with the activation <span class="hlt">energy</span> for grain boundary migration obtained from mobility calculation. A multi-phase field model (with mobility estimated from the mean field model as a constitutive input) was used to simulate the kinetics, microstructure and texture evolution. The recrystallisation kinetics and grain size distributions obtained from experiments matched reasonably well with the phase field simulations. The recrystallisation texture predicted through phase field simulations compares well with experiments though few additional texture components are present in simulations. This is attributed to the anisotropy in grain boundary mobility, which is not accounted for in the present study.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654051-tu-campus-jep1-dose-deformation-error-associated-deformable-image-registration-pathways','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654051-tu-campus-jep1-dose-deformation-error-associated-deformable-image-registration-pathways"><span>TU-H-CAMPUS-JeP1-05: Dose <span class="hlt">Deformation</span> Error Associated with <span class="hlt">Deformable</span> Image Registration Pathways</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Surucu, M; Woerner, A; Roeske, J</p> <p></p> <p>Purpose: To evaluate errors associated with using different <span class="hlt">deformable</span> image registration (DIR) pathways to <span class="hlt">deform</span> dose from planning CT (pCT) to cone-beam CT (CBCT). Methods: <span class="hlt">Deforming</span> dose is controversial because of the lack of quality assurance tools. We previously proposed a novel metric to evaluate dose <span class="hlt">deformation</span> error (DDE) by warping dose information using two methods, via dose and contour <span class="hlt">deformation</span>. First, isodose lines of the pCT were converted into structures and then <span class="hlt">deformed</span> to the CBCT using an image based <span class="hlt">deformation</span> map (dose/structure/<span class="hlt">deform</span>). Alternatively, the dose matrix from the pCT was <span class="hlt">deformed</span> to CBCT using the same <span class="hlt">deformation</span> map,more » and then the same isodose lines of the <span class="hlt">deformed</span> dose were converted into structures (dose/<span class="hlt">deform</span>/structure). The doses corresponding to each structure were queried from the <span class="hlt">deformed</span> dose and full-width-half-maximums were used to evaluate the dose dispersion. The difference between the FWHM of each isodose level structure is defined as the DDE. Three head-and-neck cancer patients were identified. For each patient, two DIRs were performed between the pCT and CBCT, either <span class="hlt">deforming</span> pCT-to-CBCT or CBCT-to-pCT. We evaluated the errors associated by using either of these pathways to <span class="hlt">deform</span> dose. A commercially available, Demons based DIR was used for this study, and 10 isodose levels (20% to 105%) were used to evaluate the errors in various dose levels. Results: The prescription dose for all patients was 70 Gy. The mean DDE for CT-to-CBCT <span class="hlt">deformation</span> was 1.0 Gy (range: 0.3–2.0 Gy) and this was increased to 4.3 Gy (range: 1.5–6.4 Gy) for CBCT-to-CT <span class="hlt">deformation</span>. The mean increase in DDE between the two <span class="hlt">deformations</span> was 3.3 Gy (range: 1.0–5.4 Gy). Conclusion: The proposed DDF was used to quantitatively estimate dose <span class="hlt">deformation</span> errors caused by different pathways to perform DIR. <span class="hlt">Deforming</span> dose using CBCT-to-CT <span class="hlt">deformation</span> produced greater error than CT-to-CBCT <span class="hlt">deformation</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SMaS...27e5001Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SMaS...27e5001Z"><span>Auxetic hexachiral structures with wavy ligaments for large elasto-plastic <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Yilin; Wang, Zhen-Pei; Hien Poh, Leong</p> <p>2018-05-01</p> <p>The hexachiral structure is in-plane isotropic in small <span class="hlt">deformation</span>. When subjected to large elasto-plastic <span class="hlt">deformation</span>, however, the hexachiral structure tends to lose its auxeticity and/or isotropy—properties which are desirable in many potential applications. The objective of this study is to improve these two mechanical properties, without significantly compromising the effective yield stress, in the regime with significant material and geometrical nonlinearity effects. It is found that the <span class="hlt">deformation</span> mechanisms underlying the auxeticity and isotropy properties of a hexachiral structure are largely influenced by the extent of rotation of the central ring in a unit cell. To facilitate the development of this <span class="hlt">deformation</span> mechanism, an improved design with wavy ligaments is proposed. The improved performance of the proposed hexachiral structure is demonstrated. An initial study on possible applications as a protective material is next carried out, where the improved hexachiral design is shown to exhibit higher specific <span class="hlt">energy</span> absorption capacity compared to the original design, as well as standard honeycomb structures.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARE17005L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARE17005L"><span>Tuning transport properties on graphene multiterminal structures by mechanical <span class="hlt">deformations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Latge, Andrea; Torres, Vanessa; Faria, Daiara</p> <p></p> <p>The realization of mechanical strain on graphene structures is viewed as a promise route to tune electronic and transport properties such as changing <span class="hlt">energy</span> band-gaps and promoting localization of states. Using continuum models, mechanical <span class="hlt">deformations</span> are described by effective gauge fields, mirrored as pseudomagnetic fields that may reach quite high values. Interesting symmetry features are developed due to out of plane <span class="hlt">deformations</span> on graphene; lift sublattice symmetry was predicted and observed in centrosymmetric bumps and strained nanobubbles. Here we discuss the effects of Gaussian-like strain on a hexagonal graphene flake connected to three leads, modeled as perfect graphene nanoribbons. The Green function formalism is used within a tight-binding approximation. For this particular <span class="hlt">deformation</span> sharp resonant states are achieved depending on the strained structure details. We also study a fold-strained structure in which the three leads are <span class="hlt">deformed</span> extending up to the very center of the hexagonal flake. We show that conductance suppressions can be controlled by the strain intensity and important transport features are modeled by the electronic band structure of the leads.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000JGR...10519111R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000JGR...10519111R"><span>Surface displacements and <span class="hlt">energy</span> <span class="hlt">release</span> rates for constant stress drop slip zones in joined elastic quarter spaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rodgers, Michael J.; Wen, Shengmin; Keer, Leon M.</p> <p>2000-08-01</p> <p>A three-dimensional quasi-static model of faulting in an elastic half-space with a horizontal change of material properties (i.e., joined elastic quarter spaces) is considered. A boundary element method is used with a stress drop slip zone approach so that the fault surface relative displacements as well as the free surface displacements are approximated in elements over their respective domains. Stress intensity factors and free surface displacements are calculated for a variety of cases to show the phenomenological behavior of faulting in such a medium. These calculations showed that the behavior could be distinguished from a uniform half-space. Slip in a stiffer material increases, while slip in a softer material decreases the <span class="hlt">energy</span> <span class="hlt">release</span> rate and the free surface displacements. Also, the 1989 Kalapana earthquake was located on the basis of a series of forward searches using this method and leveling data. The located depth is 8 km, which is the closer to the seismically inferred depth than that determined from other models. Finally, the <span class="hlt">energy</span> <span class="hlt">release</span> rate, which can be used as a fracture criterion for fracture at this depth, is calculated to be 11.1×106 J m-2.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19870004360','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19870004360"><span>Q3DG: A computer program for strain-<span class="hlt">energy-release</span> rates for delamination growth in composite laminates</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Raju, I. S.</p> <p>1986-01-01</p> <p>The Q3DG is a computer program developed to perform a quasi-three-dimensional stress analysis for composite laminates which may contain delaminations. The laminates may be subjected to mechanical, thermal, and hygroscopic loads. The program uses the finite element method and models the laminates with eight-noded parabolic isoparametric elements. The program computes the strain-<span class="hlt">energy-release</span> components and the total strain-<span class="hlt">energy</span> <span class="hlt">release</span> in all three modes for delamination growth. A rectangular mesh and data file generator, DATGEN, is included. The DATGEN program can be executed interactively and is user friendly. The documentation includes sections dealing with the Q3D analysis theory, derivation of element stiffness matrices and consistent load vectors for the parabolic element. Several sample problems with the input for Q3DG and output from the program are included. The capabilities of the DATGEN program are illustrated with examples of interactive sessions. A microfiche of all the examples is included. The Q3DG and DATGEN programs have been implemented on CYBER 170 class computers. Q3DG and DATGEN were developed at the Langley Research Center during the early eighties and documented in 1984 to 1985.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28773009','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28773009"><span>Understanding Drug <span class="hlt">Release</span> Data through Thermodynamic Analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Freire, Marjorie Caroline Liberato Cavalcanti; Alexandrino, Francisco; Marcelino, Henrique Rodrigues; Picciani, Paulo Henrique de Souza; Silva, Kattya Gyselle de Holanda E; Genre, Julieta; Oliveira, Anselmo Gomes de; Egito, Eryvaldo Sócrates Tabosa do</p> <p>2017-06-13</p> <p>Understanding the factors that can modify the drug <span class="hlt">release</span> profile of a drug from a Drug-Delivery-System (DDS) is a mandatory step to determine the effectiveness of new therapies. The aim of this study was to assess the Amphotericin-B (AmB) kinetic <span class="hlt">release</span> profiles from polymeric systems with different compositions and geometries and to correlate these profiles with the thermodynamic parameters through mathematical modeling. Film casting and electrospinning techniques were used to compare behavior of films and fibers, respectively. <span class="hlt">Release</span> profiles from the DDSs were performed, and the mathematical modeling of the data was carried out. Activation <span class="hlt">energy</span>, enthalpy, entropy and Gibbs free <span class="hlt">energy</span> of the drug <span class="hlt">release</span> process were determined. AmB <span class="hlt">release</span> profiles showed that the relationship to overcome the enthalpic barrier was PVA-fiber > PVA-film > PLA-fiber > PLA-film. Drug <span class="hlt">release</span> kinetics from the fibers and the films were better fitted on the Peppas-Sahlin and Higuchi models, respectively. The thermodynamic parameters corroborate these findings, revealing that the AmB <span class="hlt">release</span> from the evaluated systems was an endothermic and non-spontaneous process. Thermodynamic parameters can be used to explain the drug kinetic <span class="hlt">release</span> profiles. Such an approach is of utmost importance for DDS containing insoluble compounds, such as AmB, which is associated with an erratic bioavailability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5554032','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5554032"><span>Understanding Drug <span class="hlt">Release</span> Data through Thermodynamic Analysis</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Freire, Marjorie Caroline Liberato Cavalcanti; Alexandrino, Francisco; Marcelino, Henrique Rodrigues; Picciani, Paulo Henrique de Souza; Silva, Kattya Gyselle de Holanda e; Genre, Julieta; de Oliveira, Anselmo Gomes; do Egito, Eryvaldo Sócrates Tabosa</p> <p>2017-01-01</p> <p>Understanding the factors that can modify the drug <span class="hlt">release</span> profile of a drug from a Drug-Delivery-System (DDS) is a mandatory step to determine the effectiveness of new therapies. The aim of this study was to assess the Amphotericin-B (AmB) kinetic <span class="hlt">release</span> profiles from polymeric systems with different compositions and geometries and to correlate these profiles with the thermodynamic parameters through mathematical modeling. Film casting and electrospinning techniques were used to compare behavior of films and fibers, respectively. <span class="hlt">Release</span> profiles from the DDSs were performed, and the mathematical modeling of the data was carried out. Activation <span class="hlt">energy</span>, enthalpy, entropy and Gibbs free <span class="hlt">energy</span> of the drug <span class="hlt">release</span> process were determined. AmB <span class="hlt">release</span> profiles showed that the relationship to overcome the enthalpic barrier was PVA-fiber > PVA-film > PLA-fiber > PLA-film. Drug <span class="hlt">release</span> kinetics from the fibers and the films were better fitted on the Peppas–Sahlin and Higuchi models, respectively. The thermodynamic parameters corroborate these findings, revealing that the AmB <span class="hlt">release</span> from the evaluated systems was an endothermic and non-spontaneous process. Thermodynamic parameters can be used to explain the drug kinetic <span class="hlt">release</span> profiles. Such an approach is of utmost importance for DDS containing insoluble compounds, such as AmB, which is associated with an erratic bioavailability. PMID:28773009</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARC40012B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARC40012B"><span>Phyllotactic transformations as plastic <span class="hlt">deformations</span> of tubular crystals with defects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Beller, Daniel; Nelson, David</p> <p></p> <p>Tubular crystals are 2D lattices in cylindrical topologies, which could be realized as assemblies of colloidal particles, and occur naturally in biological microtubules and in single-walled carbon nanotubes. Their geometry can be understood in the language of phyllotaxis borrowed from botany. We study the mechanics of plastic <span class="hlt">deformations</span> in tubular crystals in response to tensile stress, as mediated by the formation and separation of dislocation pairs in a triangular lattice. Dislocation motion allows the growth of one phyllotactic arrangement at the expense of another, offering a low-<span class="hlt">energy</span>, stepwise mode of plastic <span class="hlt">deformation</span> in response to external stresses. Through theory and simulation, we examine how the tube's radius and helicity affects, and is in turn altered by, dislocation glide. The crystal's bending modulus is found to produce simple but important corrections to the tube's <span class="hlt">deformation</span> mechanics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17813913','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17813913"><span>Forearc <span class="hlt">deformation</span> and great subduction earthquakes: implications for cascadia offshore earthquake potential.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>McCaffrey, R; Goldfinger, C</p> <p>1995-02-10</p> <p>The maximum size of thrust earthquakes at the world's subduction zones appears to be limited by anelastic <span class="hlt">deformation</span> of the overriding plate. Anelastic strain in weak forearcs and roughness of the plate interface produced by faults cutting the forearc may limit the size of thrust earthquakes by inhibiting the buildup of elastic strain <span class="hlt">energy</span> or slip propagation or both. Recently discovered active strike-slip faults in the submarine forearc of the Cascadia subduction zone show that the upper plate there <span class="hlt">deforms</span> rapidly in response to arc-parallel shear. Thus, Cascadia, as a result of its weak, <span class="hlt">deforming</span> upper plate, may be the type of subduction zone at which great (moment magnitude approximately 9) thrust earthquakes do not occur.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..359a2014S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..359a2014S"><span>Study on Thermal <span class="hlt">Deformation</span> Behavior of TC4 – ELI Titanium Alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Song, Y.; Zhang, F. S.; Huang, T.; Song, K. X.</p> <p>2018-05-01</p> <p>The TC4-ELI titanium alloy was subjected to hot compression <span class="hlt">deformation</span> test by the Gleeble-1500D thermal simulation test machine. The thermal <span class="hlt">deformation</span> behavior of the TC4-ELI titanium alloy was studied under the condition of 850°C-1050°C, 0.001s-1-10s-1 strain rate and 50% <span class="hlt">deformation</span>. The constitutive equation of TC4-ELI titanium alloy was established based on the hyperbolic sine model of Arrhenius equation. The results show that the flow stress of TC4-ELI titanium alloy decreases with the increase of temperature at high temperature. The calculated heat activation <span class="hlt">energy</span> of TC4-ELI titanium alloy is 300367.5807J / mol.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003PhRvA..67b2114E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003PhRvA..67b2114E"><span>Normal and lateral Casimir forces between <span class="hlt">deformed</span> plates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Emig, Thorsten; Hanke, Andreas; Golestanian, Ramin; Kardar, Mehran</p> <p>2003-02-01</p> <p>The Casimir force between macroscopic bodies depends strongly on their shape and orientation. To study this geometry dependence in the case of two <span class="hlt">deformed</span> metal plates, we use a path-integral quantization of the electromagnetic field which properly treats the many-body nature of the interaction, going beyond the commonly used pairwise summation (PWS) of van der Waals forces. For arbitrary <span class="hlt">deformations</span> we provide an analytical result for the <span class="hlt">deformation</span> induced change in the Casimir <span class="hlt">energy</span>, which is exact to second order in the <span class="hlt">deformation</span> amplitude. For the specific case of sinusoidally corrugated plates, we calculate both the normal and the lateral Casimir forces. The <span class="hlt">deformation</span> induced change in the Casimir interaction of a flat and a corrugated plate shows an interesting crossover as a function of the ratio of the mean plate distance H to the corrugation length λ: For λ≪H we find a slower decay ˜H-4, compared to the H-5 behavior predicted by PWS which we show to be valid only for λ≫H. The amplitude of the lateral force between two corrugated plates which are out of registry is shown to have a maximum at an optimal wavelength of λ≈2.5 H. With increasing H/λ≳0.3 the PWS approach becomes a progressively worse description of the lateral force due to many-body effects. These results may be of relevance for the design and operation of novel microelectromechanical systems (MEMS) and other nanoscale devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1235336-deformation-failure-response-closed-cell-pmdi-foams-subjected-dynamic-impact-loading','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1235336-deformation-failure-response-closed-cell-pmdi-foams-subjected-dynamic-impact-loading"><span>The <span class="hlt">deformation</span> and failure response of closed-cell PMDI foams subjected to dynamic impact loading</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Koohbor, Behrad; Mallon, Silas; Kidane, Addis; ...</p> <p>2015-04-07</p> <p>The present work aims to investigate the bulk <span class="hlt">deformation</span> and failure response of closed-cell Polymeric Methylene Diphenyl Diisocyanate (PMDI) foams subjected to dynamic impact loading. First, foam specimens of different initial densities are examined and characterized in quasi-static loading conditions, where the <span class="hlt">deformation</span> behavior of the samples is quantified in terms of the compressive elastic modulus and effective plastic Poisson's ratio. Then, the <span class="hlt">deformation</span> response of the foam specimens subjected to direct impact loading is examined by taking into account the effects of material compressibility and inertia stresses developed during <span class="hlt">deformation</span>, using high speed imaging in conjunction with 3D digitalmore » image correlation. The stress-strain response and the <span class="hlt">energy</span> absorption as a function of strain rate and initial density are presented and the bulk failure mechanisms are discussed. As a result, it is observed that the initial density of the foam and the applied strain rates have a substantial influence on the strength, bulk failure mechanism and the <span class="hlt">energy</span> dissipation characteristics of the foam specimens.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009JSDD....3...47S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009JSDD....3...47S"><span>Skill Analysis of the Wrist <span class="hlt">Release</span> in the Golf Swings Utilizing Shaft Elasticity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suzuki, Soichiro; Hoshino, Yohei; Kobayashi, Yukinori</p> <p></p> <p>This study analyzes the skill component of the wrist <span class="hlt">release</span> in the golf swing by employing a three-dimensional dynamic model considering vibration of the club shaft. It is observed that professional and expert golfers relax their wrists in the swing motion as a "natural" or "late" <span class="hlt">release</span>. Thus, the relationship between the timing of the wrist <span class="hlt">release</span> and the shaft vibration is examined in this study. First, it is demonstrated that "natural <span class="hlt">release</span>" at the zero-crossing point of the bending vibration of the shaft efficiently increases the head speed at impact. In the next step, the "late hitting" condition is imposed upon the model. It is demonstrated that "late hitting" could further improve the efficiency of the swing motion. Finally, the skill component in the wrist <span class="hlt">release</span> for the long drive is experimentally verified by measuring the movement of the wrist and the dynamic <span class="hlt">deformation</span> of the shaft during the downswing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29038576','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29038576"><span>Size effect on the <span class="hlt">deformation</span> mechanisms of nanocrystalline platinum thin films.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shu, Xinyu; Kong, Deli; Lu, Yan; Long, Haibo; Sun, Shiduo; Sha, Xuechao; Zhou, Hao; Chen, Yanhui; Mao, Shengcheng; Liu, Yinong</p> <p>2017-10-16</p> <p>This paper reports a study of time-resolved <span class="hlt">deformation</span> process at the atomic scale of a nanocrystalline Pt thin film captured in situ under a transmission electron microscope. The main mechanism of plastic <span class="hlt">deformation</span> was found to evolve from full dislocation activity-enabled plasticity in large grains (with grain size d > 10 nm), to partial dislocation plasticity in smaller grains (with grain size 10 nm < d < 6 nm), and grain boundary-mediated plasticity in the matrix with grain sizes d < 6 nm. The critical grain size for the transition from full dislocation activity to partial dislocation activity was estimated based on consideration of stacking fault <span class="hlt">energy</span>. For grain boundary-mediated plasticity, the possible contributions to strain rate of grain creep, grain sliding and grain rotation to plastic <span class="hlt">deformation</span> were estimated using established models. The contribution of grain creep is found to be negligible, the contribution of grain rotation is effective but limited in magnitude, and grain sliding is suggested to be the dominant <span class="hlt">deformation</span> mechanism in nanocrystalline Pt thin films. This study provided the direct evidence of these <span class="hlt">deformation</span> processes at the atomic scale.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GeoRL..42.3305F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GeoRL..42.3305F"><span>Coseismic and postseismic <span class="hlt">deformation</span> due to the 2007 M5.5 Ghazaband fault earthquake, Balochistan, Pakistan</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fattahi, H.; Amelung, F.; Chaussard, E.; Wdowinski, S.</p> <p>2015-05-01</p> <p>Time series analysis of interferometric synthetic aperture radar data reveals coseismic and postseismic surface displacements associated with the 2007 M5.5 earthquake along the southern Ghazaband fault, a major but little studied fault in Pakistan. Modeling indicates that the coseismic surface <span class="hlt">deformation</span> was caused by ~9 cm of strike-slip displacement along a shallow subvertical fault. The earthquake was followed by at least 1 year of afterslip, <span class="hlt">releasing</span> ~70% of the moment of the main event, equivalent to a M5.4 earthquake. This high aseismic relative to the seismic moment <span class="hlt">release</span> is consistent with previous observations for moderate earthquakes (M < 6) and suggests that smaller earthquakes are associated with a higher aseismic relative to seismic moment <span class="hlt">release</span> than larger earthquakes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Litho.310...86D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Litho.310...86D"><span>Pyrite <span class="hlt">deformation</span> and connections to gold mobility: Insight from micro-structural analysis and trace element mapping</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dubosq, R.; Lawley, C. J. M.; Rogowitz, A.; Schneider, D. A.; Jackson, S.</p> <p>2018-06-01</p> <p>The metamorphic transition of pyrite to pyrrhotite results in the liberation of lattice-bound and nano-particulate metals initially hosted within early sulphide minerals. This process forms the basis for the metamorphic-driven Au-upgrading model applied to many orogenic Au deposits, however the role of syn-metamorphic pyrite <span class="hlt">deformation</span> in controlling the retention and <span class="hlt">release</span> of Au and related pathfinder elements is poorly understood. The lower amphibolite facies metamorphic mineral assemblage (Act-Bt-Pl-Ep-Alm ± Cal ± Qz ± Ilm; 550 °C) of Canada's giant Detour Lake deposit falls within the range of pressure-temperature conditions (450 °C) for crystal plastic <span class="hlt">deformation</span> of pyrite. We have applied a complementary approach of electron backscatter diffraction (EBSD) mapping and laser ablation inductively coupled plasma mass spectrometry (LA-ICP-MS) 2D element mapping on pyrite from the Detour Lake deposit. Chemical element maps document an early generation of Au-rich sieve textured pyrite domains and a later stage of syn-metamorphic oscillatory-zoned Au-poor pyrite. Both pyrite types are cut by Au-rich fractures as a consequence of remobilization of Au with trace element enrichment of first-row transition elements, post-transition metals, chalcogens and metalloids during a late brittle <span class="hlt">deformation</span> stage. However, similar enrichment in trace elements and Au can be observed along low-angle grain boundaries within otherwise Au-poor pyrite, indicating that heterogeneous microstructural misorientation patterns and higher strain domains are also relatively Au-rich. We therefore propose that the close spatial relationship between pyrite and Au at the microscale, features typical of orogenic Au deposits, reflects the entrapment of Au within <span class="hlt">deformation</span>-induced microstructures in pyrite rather than the <span class="hlt">release</span> of Au during the metamorphic transition from pyrite to pyrrhotite. Moreover, mass balance calculations at the deposit scale suggest that only a small percentage</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017RJPCA..91.2070Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017RJPCA..91.2070Z"><span>Thermally induced processes in mixtures of aluminum with organic acids after plastic <span class="hlt">deformations</span> under high pressure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhorin, V. A.; Kiselev, M. R.; Roldugin, V. I.</p> <p>2017-11-01</p> <p>DSC is used to measure the thermal effects of processes in mixtures of solid organic dibasic acids with powdered aluminum, subjected to plastic <span class="hlt">deformation</span> under pressures in the range of 0.5-4.0 GPa using an anvil-type high-pressure setup. Analysis of thermograms obtained for the samples after plastic <span class="hlt">deformation</span> suggests a correlation between the exothermal peaks observed around the temperatures of degradation of the acids and the thermally induced chemical reactions between products of acid degradation and freshly formed surfaces of aluminum particles. The <span class="hlt">release</span> of heat in the mixtures begins at 30-40°C. The thermal effects in the mixtures of different acids change according to the order of acid reactivity in solutions. The extreme baric dependences of enthalpies of thermal effects are associated with the rearrangement of the electron subsystem of aluminum upon plastic <span class="hlt">deformation</span> at high pressures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFM.U22A..06H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFM.U22A..06H"><span>Sumatra-Andaman Megathrust Earthquake Slip: Insights From Mechanical Modeling of ICESat Surface <span class="hlt">Deformation</span> Measurements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harding, D. J.; Miuller, J. R.</p> <p>2005-12-01</p> <p>Modeling the kinematics of the 2004 Great Sumatra-Andaman earthquake is limited in the northern two-thirds of the rupture zone by a scarcity of near-rupture geodetic <span class="hlt">deformation</span> measurements. Precisely repeated Ice, Cloud, and Land Elevation Satellite (ICESat) profiles across the Andaman and Nicobar Islands provide a means to more fully document the spatial pattern of surface vertical displacements and thus better constrain geomechanical modeling of the slip distribution. ICESat profiles that total ~45 km in length cross Car Nicobar, Kamorta, and Katchall in the Nicobar chain. Within the Andamans, the coverage includes ~350 km on North, Central, and South Andaman Islands along two NNE and NNW-trending profiles that provide elevations on both the east and west coasts of the island chain. Two profiles totaling ~80 km in length cross South Sentinel Island, and one profile ~10 km long crosses North Sentinel Island. With an average laser footprint spacing of 175 m, the total coverage provides over 2700 georeferenced surface elevations measurements for each operations period. Laser backscatter waveforms recorded for each footprint enable detection of forest canopy top and underlying ground elevations with decimeter vertical precision. Surface elevation change is determined from elevation profiles, acquired before and after the earthquake, that are repeated with a cross-track separation of less than 100 m by precision pointing of the ICESat spacecraft. Apparent elevation changes associated with cross-track offsets are corrected according to local slopes calculated from multiple post-earthquake repeated profiles. The surface <span class="hlt">deformation</span> measurements recorded by ICESat are generally consistent with the spatial distribution of uplift predicted by a preliminary slip distribution model. To predict co-seismic surface <span class="hlt">deformation</span>, we apply a slip distribution, derived from the <span class="hlt">released</span> <span class="hlt">energy</span> distribution computed by Ishii et al. (2005), as the displacement discontinuity</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28349995','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28349995"><span>Formation mechanism of fivefold <span class="hlt">deformation</span> twins in a face-centered cubic alloy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Zhenyu; Huang, Siling; Chen, Leilei; Zhu, Zhanwei; Guo, Dongming</p> <p>2017-03-28</p> <p>The formation mechanism considers fivefold <span class="hlt">deformation</span> twins originating from the grain boundaries in a nanocrystalline material, resulting in that fivefold <span class="hlt">deformation</span> twins derived from a single crystal have not been reported by molecular dynamics simulations. In this study, fivefold <span class="hlt">deformation</span> twins are observed in a single crystal of face-centered cubic (fcc) alloy. A new formation mechanism is proposed for fivefold <span class="hlt">deformation</span> twins in a single crystal. A partial dislocation is emitted from the incoherent twin boundaries (ITBs) with high <span class="hlt">energy</span>, generating a stacking fault along {111} plane, and resulting in the nucleating and growing of a twin by the successive emission of partials. A node is fixed at the intersecting center of the four different slip {111} planes. With increasing stress under the indentation, ITBs come into being close to the node, leading to the emission of a partial from the node. This generates a stacking fault along a {111} plane, nucleating and growing a twin by the continuous emission of the partials. This process repeats until the formation of fivefold <span class="hlt">deformation</span> twins.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NatSR...745405Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NatSR...745405Z"><span>Formation mechanism of fivefold <span class="hlt">deformation</span> twins in a face-centered cubic alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Zhenyu; Huang, Siling; Chen, Leilei; Zhu, Zhanwei; Guo, Dongming</p> <p>2017-03-01</p> <p>The formation mechanism considers fivefold <span class="hlt">deformation</span> twins originating from the grain boundaries in a nanocrystalline material, resulting in that fivefold <span class="hlt">deformation</span> twins derived from a single crystal have not been reported by molecular dynamics simulations. In this study, fivefold <span class="hlt">deformation</span> twins are observed in a single crystal of face-centered cubic (fcc) alloy. A new formation mechanism is proposed for fivefold <span class="hlt">deformation</span> twins in a single crystal. A partial dislocation is emitted from the incoherent twin boundaries (ITBs) with high <span class="hlt">energy</span>, generating a stacking fault along {111} plane, and resulting in the nucleating and growing of a twin by the successive emission of partials. A node is fixed at the intersecting center of the four different slip {111} planes. With increasing stress under the indentation, ITBs come into being close to the node, leading to the emission of a partial from the node. This generates a stacking fault along a {111} plane, nucleating and growing a twin by the continuous emission of the partials. This process repeats until the formation of fivefold <span class="hlt">deformation</span> twins.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18617778','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18617778"><span>High prevalence of morphometric vertebral <span class="hlt">deformities</span> in patients with inflammatory bowel disease.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Heijckmann, Anna Caroline; Huijberts, Maya S P; Schoon, Erik J; Geusens, Piet; de Vries, Jolanda; Menheere, Paul P C A; van der Veer, Eveline; Wolffenbuttel, Bruce H R; Stockbrugger, Reinhold W; Dumitrescu, Bianca; Nieuwenhuijzen Kruseman, Arie C</p> <p>2008-08-01</p> <p>Earlier studies have documented that the prevalence of decreased bone mineral density (BMD) is elevated in patients with inflammatory bowel disease. The objective of this study was to investigate the prevalence of vertebral <span class="hlt">deformities</span> in inflammatory bowel disease patients and their relation with BMD and bone turnover. One hundred and nine patients with Crohn's disease (CD) and 72 with ulcerative colitis (UC) (age 44.5+/-14.2 years) were studied. BMD of the hip (by dual X-ray absorptiometry) was measured and a lateral single <span class="hlt">energy</span> densitometry of the spine for assessment of vertebral <span class="hlt">deformities</span> was performed. Serum markers of bone resorption (carboxy-terminal cross-linked telopeptide of type I collagen) and formation (procollagen type I amino-terminal propeptide) were measured, and determinants of prevalent vertebral <span class="hlt">deformities</span> were assessed using logistic regression analysis. Vertebral <span class="hlt">deformities</span> were found in 25% of both CD and UC patients. Comparing patients with and without vertebral <span class="hlt">deformities</span>, no significant difference was found between Z-scores and T-scores of BMD, or levels of serum carboxy-terminal cross-linked telopeptide of type I collagen and serum procollagen type I amino-terminal propeptide. Using logistic regression analysis the only determinant of any morphometric vertebral <span class="hlt">deformity</span> was sex. The presence of multiple vertebral <span class="hlt">deformities</span> was associated with older age and glucocorticoid use. The prevalence of morphometric vertebral <span class="hlt">deformities</span> is high in CD and UC. Male sex, but neither disease activity, bone turnover markers, clinical risk factors, nor BMD predicted their presence. The determinants for having more than one vertebral <span class="hlt">deformity</span> were age and glucocorticoid use. This implies that in addition to screening for low BMD, morphometric assessment of vertebral <span class="hlt">deformities</span> is warranted in CD and UC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PASJ..tmp....6S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PASJ..tmp....6S"><span>Observational study on the fine structure and dynamics of a solar jet. II. <span class="hlt">Energy</span> <span class="hlt">release</span> process revealed by spectral analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sakaue, Takahito; Tei, Akiko; Asai, Ayumi; Ueno, Satoru; Ichimoto, Kiyoshi; Shibata, Kazunari</p> <p>2018-01-01</p> <p>We report on a solar jet phenomenon associated with the C5.4 class flare on 2014 November 11. The data of the jet was provided by the Solar Dynamics Observatory, the X-Ray Telescope (XRT) aboard Hinode, and the Interface Region Imaging Spectrograph and Domeless Solar Telescope (DST) at Hida Observatory, Kyoto University. These plentiful data enabled us to present this series of papers to discuss all the processes of the observed phenomena, including <span class="hlt">energy</span> storage, event trigger, and <span class="hlt">energy</span> <span class="hlt">release</span>. In this paper, we focus on the <span class="hlt">energy</span> <span class="hlt">release</span> process of the observed jet, and mainly describe our spectral analysis on the Hα data of DST to investigate the internal structure of the Hα jet and its temporal evolution. This analysis reveals that in the physical quantity distributions of the Hα jet, such as line-of-sight velocity and optical thickness, there is a significant gradient in the direction crossing the jet. We interpret this internal structure as the consequence of the migration of the <span class="hlt">energy</span> <span class="hlt">release</span> site, based on the idea of ubiquitous reconnection. Moreover, by measuring the horizontal flow of the fine structures in the jet, we succeeded in deriving the three-dimensional velocity field and the line-of-sight acceleration field of the Hα jet. The analysis result indicates that part of the ejecta in the Hα jet experienced additional acceleration after it had been ejected from the lower atmosphere. This secondary acceleration was found to occur in the vicinity of the intersection between the trajectories of the Hα jet and the X-ray jet observed by Hinode/XRT. We propose that a fundamental cause of this phenomenon is magnetic reconnection involving the plasmoid in the observed jet.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25433200','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25433200"><span>Relationships between surface free <span class="hlt">energy</span>, surface texture parameters and controlled drug <span class="hlt">release</span> in hydrophilic matrices.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Saurí, J; Suñé-Negre, J M; Díaz-Marcos, J; Vilana, J; Millán, D; Ticó, J R; Miñarro, M; Pérez-Lozano, P; García-Montoya, E</p> <p>2015-01-15</p> <p>The study of controlled <span class="hlt">release</span> and drug <span class="hlt">release</span> devices has been dominated by considerations of the bulk or average properties of material or devices. Yet the outermost surface atoms play a central role in their performance. The objective of this article has been to characterize the surface of hydrophilic matrix tablets using the contact angle (CA) method to ascertain the surface free <span class="hlt">energy</span>, and atomic force microscopy (AFM) and confocal microscopy (CM) for the physical characterization of the surface of the hydrophilic matrix. The surface free <span class="hlt">energy</span> results obtained show that hydroxypropylmethylcellulose K15M hinders the spreading of water on the surface of the tablet, such that the concentration of HPMC K15M increases the reaction rate of the hydrophobic interactions between the chains of HPMC K15M which increases with respect to the rate of penetration of water into the tablet. In this study, we developed a new method to characterize the swelling of the tablets and established a relationship between the new method based on microswelling and the swelling ratio parameter. The surface texture parameters have been determined and the morphology of the tablets of the different formulations and the evolution of the surface morphology after interacting with the water, swelling and forming a gel layer were characterized. This work represents significant progress in the characterization of matrix tablets. Copyright © 2014 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995JPhA...28L.225A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995JPhA...28L.225A"><span>Jordanian <span class="hlt">deformation</span> of SL(2) as a contraction of its Drinfeld-Jimbo <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aghamohammadi, A.; Khorrami, M.; Shariati, A.</p> <p>1995-04-01</p> <p>We show that $h$-<span class="hlt">deformation</span> can be obtained, by a singular limit of a similarity transformation, from $q$-<span class="hlt">deformation</span>; to be specefic, we obtain $\\GL_h(2)$, its differential structure, its inhomogenous extension, and $\\Uh{\\sl(2)}$ from their $q$-<span class="hlt">deformed</span> counterparts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvC..97b4616H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvC..97b4616H"><span>Sub-barrier quasifission in heavy element formation reactions with <span class="hlt">deformed</span> actinide target nuclei</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hinde, D. J.; Jeung, D. Y.; Prasad, E.; Wakhle, A.; Dasgupta, M.; Evers, M.; Luong, D. H.; du Rietz, R.; Simenel, C.; Simpson, E. C.; Williams, E.</p> <p>2018-02-01</p> <p>Background: The formation of superheavy elements (SHEs) by fusion of two massive nuclei is severely inhibited by the competing quasifission process. Low excitation <span class="hlt">energies</span> favor SHE survival against fusion-fission competition. In "cold" fusion with spherical target nuclei near 208Pb, SHE yields are largest at beam <span class="hlt">energies</span> significantly below the average capture barrier. In "hot" fusion with statically <span class="hlt">deformed</span> actinide nuclei, this is not the case. Here the elongated <span class="hlt">deformation</span>-aligned configurations in sub-barrier capture reactions inhibits fusion (formation of a compact compound nucleus), instead favoring rapid reseparation through quasifission. Purpose: To determine the probabilities of fast and slow quasifission in reactions with prolate statically <span class="hlt">deformed</span> actinide nuclei, through measurement and quantitative analysis of the dependence of quasifission characteristics at beam <span class="hlt">energies</span> spanning the average capture barrier <span class="hlt">energy</span>. Methods: The Australian National University Heavy Ion Accelerator Facility and CUBE fission spectrometer have been used to measure fission and quasifission mass and angle distributions for reactions with projectiles from C to S, bombarding Th and U target nuclei. Results: Mass-asymmetric quasifission occurring on a fast time scale, associated with collisions with the tips of the prolate actinide nuclei, shows a rapid increase in probability with increasing projectile charge, the transition being centered around projectile atomic number ZP=14 . For mass-symmetric fission events, deviations of angular anisotropies from expectations for fusion fission, indicating a component of slower quasifission, suggest a similar transition, but centered around ZP˜8 . Conclusions: Collisions with the tips of statically <span class="hlt">deformed</span> prolate actinide nuclei show evidence for two distinct quasifission processes of different time scales. Their probabilities both increase rapidly with the projectile charge. The probability of fusion can be severely</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16965044','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16965044"><span>High translational <span class="hlt">energy</span> <span class="hlt">release</span> in H2 (D2) associative desorption from H (D) chemisorbed on C(0001).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Baouche, S; Gamborg, G; Petrunin, V V; Luntz, A C; Baurichter, A; Hornekaer, L</p> <p>2006-08-28</p> <p>Highly energetic translational <span class="hlt">energy</span> distributions are reported for hydrogen and deuterium molecules desorbing associatively from the atomic chemisorption states on highly oriented pyrolytic graphite (HOPG). Laser assisted associative desorption is used to measure the time of flight of molecules desorbing from a hydrogen (deuterium) saturated HOPG surface produced by atomic exposure from a thermal atom source at around 2100 K. The translational <span class="hlt">energy</span> distributions normal to the surface are very broad, from approximately 0.5 to approximately 3 eV, with a peak at approximately 1.3 eV. The highest translational <span class="hlt">energy</span> measured is close to the theoretically predicted barrier height. The angular distribution of the desorbing molecules is sharply peaked along the surface normal and is consistent with thermal broadening contributing to <span class="hlt">energy</span> <span class="hlt">release</span> parallel to the surface. All results are in qualitative agreement with recent density functional theory calculations suggesting a lowest <span class="hlt">energy</span> para-type dimer recombination path.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1910188A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1910188A"><span>Interplay between <span class="hlt">deformation</span>, fluid <span class="hlt">release</span> and migration across a nascent subduction interface: evidence from Oman-UAE and implications for warm subduction zones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Agard, Philippe; Prigent, Cécile; Soret, Mathieu; Guillot, Stéphane; Dubacq, Benoît</p> <p>2017-04-01</p> <p>Frozen-in subduction plate interfaces preserving the first 1-2 My of the subduction history are found beneath ophiolites. These contacts are a key target to study the inception of mantle wedge metasomatism and the mechanical coupling between the upper plate and the top part of the sinking slab shortly after subduction initiation. Combining structural field and EBSD data, detailed petrology, thermodynamic modelling and geochemistry on both sides, i.e. the base of the mantle wedge (Oman-UAE basal peridotites) and the underlying accreted crustal fragments from the subducting slab (metamorphic soles), this study documents the continuous evolution of the plate contact from 1 GPa 900-750°C to 0.6 GPa 750-600°C, with emphasis on strain localization and feedbacks between <span class="hlt">deformation</span> and fluid migration. In the mantle wedge, the (<span class="hlt">de)formation</span> of proto-ultramylonitic peridotites is coeval with mantle metasomatism by focused hydrous fluid migration. Peridotite metasomatism results in the precipitation of new minerals (clinopyroxene, amphibole and spinel ± olivine and orthopyroxene) and their enrichment in FMEs (particularly B, Li and Cs, with concentrations up to 40 times that of the PM). Boron concentrations and isotopes (δ11B of metasomatized peridotites up to +25‰) suggest that these fluids with a "subduction signature" are probably sourced from the dehydrating amphibolitic metamorphic sole. Concomitantly, <span class="hlt">deformation</span> in the lower plate results in the stepwise formation, detachment and accretion to the mylonitic s.l. mantle of successive slices of HT metabasalts from the downgoing slab, equilibrated at amphibolite/granulite conditions (900-750°C). Two major stages may be outlined: - between 900 and 750°C, the garnet-clinopyroxene-amphibole bearing sinking crust (with melting < 6 vol%) gets juxtaposed and mechanically coupled to the mantle, leading to the transfer of subduction fluids and metasomatism (possibly into the arc zone ultimately). <span class="hlt">Deformation</span> is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS1011a2083R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS1011a2083R"><span>Solution of Einsteins Equation for <span class="hlt">Deformation</span> of a Magnetized Neutron Star</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rizaldy, R.; Sulaksono, A.</p> <p>2018-04-01</p> <p>We studied the effect of very large and non-uniform magnetic field existed in the neutron star on the <span class="hlt">deformation</span> of the neutron star. We used in our analytical calculation, multipole expansion of the tensor metric and the momentum-<span class="hlt">energy</span> tensor in Legendre polynomial expansion up to the quadrupole order. In this way we obtain the solutions of Einstein’s equation with the correction factors due to the magnetic field are taken into account. We obtain from our numerical calculation that the degree of <span class="hlt">deformation</span> (ellipticity) is increased when the the mass is decreased.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFM.T31B0842V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFM.T31B0842V"><span>Numerical Modeling of the <span class="hlt">Deformation</span> Behavior of Fault Bounded Lens Shaped Bodies in 2D</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van der Zee, W.; Urai, J. L.</p> <p>2001-12-01</p> <p>Fault zones cause dramatic discontinuous changes in mechanical properties. The early stages of evolution of fault zones are important for its long-term behavior. We consider faults which develop from <span class="hlt">deformation</span> bands or pre-existing joints which are the initially unconnected discontinuities. With further <span class="hlt">deformation</span>, these coalesce into a connected network, and develop into a 'mature' fault gouge. When segments are not coplanar, soft linkage or bends in the fault plane (<span class="hlt">releasing</span> and restraining bends, fault bounded lens-shaped bodies etc) necessarily occurs. Further movement causes additional <span class="hlt">deformation</span>, and the fault zone has a strongly variable thickness. Here, we present the results of detailed fieldwork combined with numerical modeling on the <span class="hlt">deformation</span> of fault bounded lens-shaped bodies in the fault zone. Detailed study of a number of lenses in the field shows that the lens is invariably more <span class="hlt">deformed</span> than the surrounding material. This observation can be explained in several ways. In one end member most of the <span class="hlt">deformation</span> in the future lens occurs before full coalescence of the slip planes and the formation of the lens. The other end member is that the slip planes coalesce before plastic <span class="hlt">deformation</span> of the lens is occurring. The internal <span class="hlt">deformation</span> of the lens occurs after the lens is formed, due to the redistributed stresses in the structure. If this is the case, then lens shaped bodies can be always expected to <span class="hlt">deform</span> preferentially. Finite element models were used to investigate the shear behavior of a planar fault with a lens shaped body or a sinus-shaped asperity. In a sensitivity analysis, we consider different lens shapes and fault friction coefficients. Results show that 1) during slip, the asperity shears off to form a lens shaped body 2) lens interior <span class="hlt">deforms</span> more than the surroundings, due to the redistribution of stresses 3) important parameters in this system are the length-thickness ratio of the lens and the fault friction coefficient 4</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1358549-deformations-superconformal-theories','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1358549-deformations-superconformal-theories"><span><span class="hlt">Deformations</span> of superconformal theories</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Córdova, Clay; Dumitrescu, Thomas T.; Intriligator, Kenneth</p> <p>2016-11-22</p> <p>Here, we classify possible supersymmetry-preserving relevant, marginal, and irrelevant <span class="hlt">deformations</span> of unitary superconformal theories in d ≥ 3 dimensions. Our method only relies on symmetries and unitarity. Hence, the results are model independent and do not require a Lagrangian description. Two unifying themes emerge: first, many theories admit <span class="hlt">deformations</span> that reside in multiplets together with conserved currents. Such <span class="hlt">deformations</span> can lead to modifications of the supersymmetry algebra by central and noncentral charges. Second, many theories with a sufficient amount of supersymmetry do not admit relevant or marginal <span class="hlt">deformations</span>, and some admit neither. The classification is complicated by the fact thatmore » short superconformal multiplets display a rich variety of sporadic phenomena, including supersymmetric <span class="hlt">deformations</span> that reside in the middle of a multiplet. We illustrate our results with examples in diverse dimensions. In particular, we explain how the classification of irrelevant supersymmetric <span class="hlt">deformations</span> can be used to derive known and new constraints on moduli-space effective actions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1237699-room-temperature-deformation-mechanisms-alumina-particles-observed-from-situ-micro-compression-atomistic-simulations','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1237699-room-temperature-deformation-mechanisms-alumina-particles-observed-from-situ-micro-compression-atomistic-simulations"><span>Room temperature <span class="hlt">deformation</span> mechanisms of alumina particles observed from in situ micro-compression and atomistic simulations.</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Sarobol, Pylin; Chandross, Michael E.; Carroll, Jay D.; ...</p> <p>2015-09-22</p> <p>Aerosol deposition (AD) is a solid-state deposition technology that has been developed to fabricate ceramic coatings nominally at room temperature. Sub-micron ceramic particles accelerated by pressurized gas impact, <span class="hlt">deform</span>, and consolidate on substrates under vacuum. Ceramic particle consolidation in AD coatings is highly dependent on particle <span class="hlt">deformation</span> and bonding; these behaviors are not well understood. In this work, atomistic simulations and in situ micro-compressions in the scanning electron microscope, and the transmission electron microscope (TEM) were utilized to investigate fundamental mechanisms responsible for plastic <span class="hlt">deformation</span>/fracture of particles under applied compression. Results showed that highly defective micron-sized alumina particles, initially containingmore » numerous dislocations or a grain boundary, exhibited no observable shape change before fracture/fragmentation. Simulations and experimental results indicated that particles containing a grain boundary only accommodate low strain <span class="hlt">energy</span> per unit volume before crack nucleation and propagation. In contrast, nearly defect-free, sub-micron, single crystal alumina particles exhibited plastic <span class="hlt">deformation</span> and fracture without fragmentation. Dislocation nucleation/motion, significant plastic <span class="hlt">deformation</span>, and shape change were observed. Simulation and TEM in situ micro-compression results indicated that nearly defect-free particles accommodate high strain <span class="hlt">energy</span> per unit volume associated with dislocation plasticity before fracture. As a result, the identified <span class="hlt">deformation</span> mechanisms provide insight into feedstock design for AD.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..APR.M9007P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..APR.M9007P"><span>Constrained Hartree-Fock Theory and Study of <span class="hlt">Deformed</span> Structures of Closed Shell Nuclei</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Praharaj, Choudhury</p> <p>2016-03-01</p> <p>We have studied some N or Z = 50 nuclei in a microscopic model with effective interaction in a reasonably large shell model space. Excitation of particles across 50 shell closure leads to well-<span class="hlt">deformed</span> excited prolate configurations. The potential <span class="hlt">energy</span> surfaces of nuclei are studied using Hartree-Fock theory with quadrupole constraint to explore the various <span class="hlt">deformed</span> configurations of N = 50 nuclei 82Ge , 84Se and 86Kr . <span class="hlt">Energy</span> spectra are calculated from various intrinsic states using Peierls-Yoccoz angular momentum projection technique. Results of spectra and electromagnetic moments and transitions will be presented for N = 50 nuclei and for Z = 50 114Sn nucleus. Supported by Grant No SB/S2/HEP-06/2013 of DST.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26870379','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26870379"><span>Comparison between diffraction contrast tomography and high-<span class="hlt">energy</span> diffraction microscopy on a slightly <span class="hlt">deformed</span> aluminium alloy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Renversade, Loïc; Quey, Romain; Ludwig, Wolfgang; Menasche, David; Maddali, Siddharth; Suter, Robert M; Borbély, András</p> <p>2016-01-01</p> <p>The grain structure of an Al-0.3 wt%Mn alloy <span class="hlt">deformed</span> to 1% strain was reconstructed using diffraction contrast tomography (DCT) and high-<span class="hlt">energy</span> diffraction microscopy (HEDM). 14 equally spaced HEDM layers were acquired and their exact location within the DCT volume was determined using a generic algorithm minimizing a function of the local disorientations between the two data sets. The microstructures were then compared in terms of the mean crystal orientations and shapes of the grains. The comparison shows that DCT can detect subgrain boundaries with disorientations as low as 1° and that HEDM and DCT grain boundaries are on average 4 µm apart from each other. The results are important for studies targeting the determination of grain volume. For the case of a polycrystal with an average grain size of about 100 µm, a relative deviation of about ≤10% was found between the two techniques.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAP...122b4104X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAP...122b4104X"><span>Effect of temperature-driven phase transition on <span class="hlt">energy</span>-storage and -<span class="hlt">release</span> properties of Pb0.97La0.02[Zr0.55Sn0.30Ti0.15]O3 ceramics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Ran; Tian, Jingjing; Zhu, Qingshan; Feng, Yujun; Wei, Xiaoyong; Xu, Zhuo</p> <p>2017-07-01</p> <p>Temperature-driven phase transition of Pb0.97La0.02[Zr0.55Sn0.30Ti0.15]O3 ceramics was studied, and the consecutive ferroelectric-antiferroelectric-paraelectric (FE-AFE-PE) switching was confirmed. The materials have better dielectric tunability (-82% to 50%) in the AFE state than in the FE state. Also, the phase transition influences the <span class="hlt">energy</span>-storage and -<span class="hlt">release</span> performance significantly. A sharp increase in <span class="hlt">releasable</span> <span class="hlt">energy</span> density and efficiency was observed due to the temperature-driven FE-AFE transition. Highest <span class="hlt">releasable</span> <span class="hlt">energy</span> density, current density, and peak power density were achieved at 130 °C, which was attributed to the highest backward transition field. The stored charge was <span class="hlt">released</span> completely in AFE and PE states in the microseconds scale, while only a small part of it was <span class="hlt">released</span> in the FE state. The above results indicate the huge impact of temperature-driven phase transition on dielectrics' performance, which is significant when developing AFE materials working in a wide temperature range.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5368658','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5368658"><span>Corrugated Textile based Triboelectric Generator for Wearable <span class="hlt">Energy</span> Harvesting</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Choi, A Young; Lee, Chang Jun; Park, Jiwon; Kim, Dogyun; Kim, Youn Tae</p> <p>2017-01-01</p> <p>Triboelectric <span class="hlt">energy</span> harvesting has been applied to various fields, from large-scale power generation to small electronics. Triboelectric <span class="hlt">energy</span> is generated when certain materials come into frictional contact, e.g., static electricity from rubbing a shoe on a carpet. In particular, textile-based triboelectric <span class="hlt">energy</span>-harvesting technologies are one of the most promising approaches because they are not only flexible, light, and comfortable but also wearable. Most previous textile-based triboelectric generators (TEGs) generate <span class="hlt">energy</span> by vertically pressing and rubbing something. However, we propose a corrugated textile-based triboelectric generator (CT-TEG) that can generate <span class="hlt">energy</span> by stretching. Moreover, the CT-TEG is sewn into a corrugated structure that contains an effective air gap without additional spacers. The resulting CT-TEG can generate considerable <span class="hlt">energy</span> from various <span class="hlt">deformations</span>, not only by pressing and rubbing but also by stretching. The maximum output performances of the CT-TEG can reach up to 28.13 V and 2.71 μA with stretching and <span class="hlt">releasing</span> motions. Additionally, we demonstrate the generation of sufficient <span class="hlt">energy</span> from various activities of a human body to power about 54 LEDs. These results demonstrate the potential application of CT-TEGs for self-powered systems. PMID:28349928</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CompM..60..703R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CompM..60..703R"><span>Advantages of formulating an evolution equation directly for elastic distortional <span class="hlt">deformation</span> in finite <span class="hlt">deformation</span> plasticity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rubin, M. B.; Cardiff, P.</p> <p>2017-11-01</p> <p>Simo (Comput Methods Appl Mech Eng 66:199-219, 1988) proposed an evolution equation for elastic <span class="hlt">deformation</span> together with a constitutive equation for inelastic <span class="hlt">deformation</span> rate in plasticity. The numerical algorithm (Simo in Comput Methods Appl Mech Eng 68:1-31, 1988) for determining elastic distortional <span class="hlt">deformation</span> was simple. However, the proposed inelastic <span class="hlt">deformation</span> rate caused plastic compaction. The corrected formulation (Simo in Comput Methods Appl Mech Eng 99:61-112, 1992) preserves isochoric plasticity but the numerical integration algorithm is complicated and needs special methods for calculation of the exponential map of a tensor. Alternatively, an evolution equation for elastic distortional <span class="hlt">deformation</span> can be proposed directly with a simplified constitutive equation for inelastic distortional <span class="hlt">deformation</span> rate. This has the advantage that the physics of inelastic distortional <span class="hlt">deformation</span> is separated from that of dilatation. The example of finite <span class="hlt">deformation</span> J2 plasticity with linear isotropic hardening is used to demonstrate the simplicity of the numerical algorithm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1342519-shock-compression-release-axis-magnesium-single-crystals-anisotropy-time-dependent-inelastic-response','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1342519-shock-compression-release-axis-magnesium-single-crystals-anisotropy-time-dependent-inelastic-response"><span>Shock compression and <span class="hlt">release</span> of a-axis magnesium single crystals: Anisotropy and time dependent inelastic response</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Renganathan, P.; Winey, J. M.; Gupta, Y. M.</p> <p>2017-01-19</p> <p>Here, to gain insight into inelastic <span class="hlt">deformation</span> mechanisms for shocked hexagonal close-packed (hcp) metals, particularly the role of crystal anisotropy, magnesium (Mg) single crystals were subjected to shock compression and <span class="hlt">release</span> along the a-axis to 3.0 and 4.8 GPa elastic impact stresses. Wave profiles measured at several thicknesses, using laser interferometry, show a sharply peaked elastic wave followed by the plastic wave. Additionally, a smooth and featureless <span class="hlt">release</span> wave is observed following peak compression. When compared to wave profiles measured previously for c-axis Mg, the elastic wave amplitudes for a-axis Mg are lower for the same propagation distance, and less attenuation of elastic wave amplitude is observed for a given peak stress. The featureless <span class="hlt">release</span> wave for a-axis Mg is in marked contrast to the structured features observed for c-axis unloading. Numerical simulations, using a time-dependent anisotropic modeling framework, showed that the wave profiles calculated using prismatic slip or (10more » $$\\bar{1}$$2) twinning, individually, do not match the measured compression profiles for a-axis Mg. However, a combination of slip and twinning provides a good overall match to the measured compression profiles. In contrast to compression,prismatic slip alone provides a reasonable match to the measured <span class="hlt">release</span> wave profiles; (10$$\\bar{1}$$2) twinning due to its uni-directionality is not activated during <span class="hlt">release</span>. The experimental results and wave profile simulations for a-axis Mg presented here are quite different from the previously published c-axis results, demonstrating the important role of crystal anisotropy on the time-dependent inelastic <span class="hlt">deformation</span> of Mg single crystals under shock compression and <span class="hlt">release</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1342519','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1342519"><span>Shock compression and <span class="hlt">release</span> of a-axis magnesium single crystals: Anisotropy and time dependent inelastic response</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Renganathan, P.; Winey, J. M.; Gupta, Y. M.</p> <p></p> <p>Here, to gain insight into inelastic <span class="hlt">deformation</span> mechanisms for shocked hexagonal close-packed (hcp) metals, particularly the role of crystal anisotropy, magnesium (Mg) single crystals were subjected to shock compression and <span class="hlt">release</span> along the a-axis to 3.0 and 4.8 GPa elastic impact stresses. Wave profiles measured at several thicknesses, using laser interferometry, show a sharply peaked elastic wave followed by the plastic wave. Additionally, a smooth and featureless <span class="hlt">release</span> wave is observed following peak compression. When compared to wave profiles measured previously for c-axis Mg, the elastic wave amplitudes for a-axis Mg are lower for the same propagation distance, and less attenuation of elastic wave amplitude is observed for a given peak stress. The featureless <span class="hlt">release</span> wave for a-axis Mg is in marked contrast to the structured features observed for c-axis unloading. Numerical simulations, using a time-dependent anisotropic modeling framework, showed that the wave profiles calculated using prismatic slip or (10more » $$\\bar{1}$$2) twinning, individually, do not match the measured compression profiles for a-axis Mg. However, a combination of slip and twinning provides a good overall match to the measured compression profiles. In contrast to compression,prismatic slip alone provides a reasonable match to the measured <span class="hlt">release</span> wave profiles; (10$$\\bar{1}$$2) twinning due to its uni-directionality is not activated during <span class="hlt">release</span>. The experimental results and wave profile simulations for a-axis Mg presented here are quite different from the previously published c-axis results, demonstrating the important role of crystal anisotropy on the time-dependent inelastic <span class="hlt">deformation</span> of Mg single crystals under shock compression and <span class="hlt">release</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18534536','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18534536"><span>Quantification of effect of sequential posteromedial <span class="hlt">release</span> on flexion and extension gaps: a computer-assisted study in cadaveric knees.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mullaji, Arun; Sharma, Amit; Marawar, Satyajit; Kanna, Raj</p> <p>2009-08-01</p> <p>A novel sequence of posteromedial <span class="hlt">release</span> consistent with surgical technique of total knee arthroplasty was performed in 15 cadaveric knees. Medial and lateral flexion and extension gaps were measured after each step of the <span class="hlt">release</span> using a computed tomography-free computer navigation system. A spring-loaded distractor and a manual distractor were used to distract the joint. Posterior cruciate ligament <span class="hlt">release</span> increased flexion more than extension gap; deep medial collateral ligament <span class="hlt">release</span> had a negligible effect; semimembranosus <span class="hlt">release</span> increased the flexion gap medially; reduction osteotomy increased medial flexion and extension gaps; superficial medial collateral ligament <span class="hlt">release</span> increased medial joint gap more in flexion and caused severe instability. This sequence of <span class="hlt">release</span> led to incremental and differential effects on flexion-extension gaps and has implications in correcting varus <span class="hlt">deformity</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013SPIE.8768E..0BL','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013SPIE.8768E..0BL"><span>A <span class="hlt">deformable</span> spherical planet exploration robot</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liang, Yi-shan; Zhang, Xiu-li; Huang, Hao; Yang, Yan-feng; Jin, Wen-tao; Sang, Zhong-xun</p> <p>2013-03-01</p> <p>In this paper, a <span class="hlt">deformable</span> spherical planet exploration robot has been introduced to achieve the task of environmental detection in outer space or extreme conditions. The robot imitates the morphology structure and motion mechanism of tumbleweeds. The robot is wind-driven. It consists of an axle, a spherical steel skeleton and twelve airbags. The axle is designed as two parts. The robot contracts by contracting the two-part axle. The spherical robot installs solar panels to provide <span class="hlt">energy</span> for its control system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/11016964','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/11016964"><span><span class="hlt">Deformation</span> and seismicity of Taiwan.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Vita-Finzi, C</p> <p>2000-10-10</p> <p>14C-dated Holocene coastal uplift, conventional and satellite geodetic measurements, and coseismic and aseismic fault slip reveal the pattern of distributed <span class="hlt">deformation</span> at Taiwan resulting from convergence between the Philippine Sea plate and Eurasia; as in other subduction orogenic settings, the locus of strain <span class="hlt">release</span> and accumulation is strongly influenced by changes in fault geometry across strike. Uplift evidence from the islands of Lutao and Lanhsu is consistent with progressive oblique collision between the Luzon arc and the Chinese continental margin. In the Coastal Range, geodetic and seismic records show that shortening is taken up serially by discontinuous slip on imbricate faults. The geodetic data point to net extension across the Central Range, but <span class="hlt">deformed</span> Holocene shorelines in the Hengchun Peninsula at its southern extremity suggest that the extension is a superficial effect partly caused by blind reverse faulting. The fastest shortening rates indicated by geodesy are recorded on the Longitudinal Valley fault and across the Chukou fault within the fold-and-thrust belt. In the former, the strain is dissipated mainly as aseismic reverse and strike-slip displacement. In contrast, the fold-and-thrust belt has witnessed five earthquakes with magnitudes of 6.5 or above in the 20th century, including the 1999.9.21 Chi-Chi earthquake (magnitude approximately 7.6) on a branch of the Chukou fault. The neotectonic and geodetic data for Taiwan as a whole suggest that the fold-and-thrust belt will continue to host the majority of great earthquakes on the island.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880009586','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880009586"><span><span class="hlt">Deformations</span> in VLBI antennas</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Clark, T. A.; Thomsen, P.</p> <p>1988-01-01</p> <p>A study is presented of <span class="hlt">deformations</span> in antennas with the emphasis on their influence on VLBI measurements. The GIFTS structural analysis program has been used to model the VLBI antenna in Fairbanks (Alaska). The report identifies key <span class="hlt">deformations</span> and studies the effect of gravity, wind, and temperature. Estimates of expected <span class="hlt">deformations</span> are given.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920042095&hterms=Free+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DFree%2Benergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920042095&hterms=Free+energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DFree%2Benergy"><span>Stress versus temperature dependence of activation <span class="hlt">energies</span> for creep</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Freed, A. D.; Raj, S. V.; Walker, K. P.</p> <p>1992-01-01</p> <p>The activation <span class="hlt">energy</span> for creep at low stresses and elevated temperatures is associated with lattice diffusion, where the rate controlling mechanism for <span class="hlt">deformation</span> is dislocation climb. At higher stresses and intermediate temperatures, the rate controlling mechanism changes from dislocation climb to obstacle-controlled dislocation glide. Along with this change in <span class="hlt">deformation</span> mechanism occurs a change in the activation <span class="hlt">energy</span>. When the rate controlling mechanism for <span class="hlt">deformation</span> is obstacle-controlled dislocation glide, it is shown that a temperature-dependent Gibbs free <span class="hlt">energy</span> does better than a stress-dependent Gibbs free <span class="hlt">energy</span> in correlating steady-state creep data for both copper and LiF-22mol percent CaF2 hypereutectic salt.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARC33002O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARC33002O"><span><span class="hlt">Energy</span> conversion in polyelectrolyte hydrogels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Olvera de La Cruz, Monica; Erbas, Aykut; Olvera de la Cruz Team</p> <p></p> <p><span class="hlt">Energy</span> conversion and storage have been an active field of research in nanotechnology parallel to recent interests towards renewable <span class="hlt">energy</span>. Polyelectrolyte (PE) hydrogels have attracted considerable attention in this field due to their mechanical flexibility and stimuli-responsive properties. Ideally, when a hydrogel is <span class="hlt">deformed</span>, applied mechanical work can be converted into electrostatic, elastic and steric-interaction <span class="hlt">energies</span>. In this talk, we discuss the results of our extensive molecular dynamics simulations of PE hydrogels. We demonstrate that, on <span class="hlt">deformation</span>, hydrogels adjust their <span class="hlt">deformed</span> state predominantly by altering electrostatic interactions between their charged groups rather than excluded-volume and bond <span class="hlt">energies</span>. This is due to the hydrogel's inherent tendency to preserve electro-neutrality in its interior, in combination with correlations imposed by backbone charges. Our findings are valid for a wide range of compression ratios and ionic strengths. The electrostatic-<span class="hlt">energy</span> alterations that we observe in our MD simulations may induce pH or redox-potential changes inside the hydrogels. The resulting energetic difference can be harvested, for instance, analogously to a Carnot engine, or facilitated for sensor applications. Center for Bio-inspired <span class="hlt">Energy</span> Science (CBES).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IJMPA..3050036F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IJMPA..3050036F"><span><span class="hlt">Deformation</span> of second and third quantization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Faizal, Mir</p> <p>2015-03-01</p> <p>In this paper, we will <span class="hlt">deform</span> the second and third quantized theories by <span class="hlt">deforming</span> the canonical commutation relations in such a way that they become consistent with the generalized uncertainty principle. Thus, we will first <span class="hlt">deform</span> the second quantized commutator and obtain a <span class="hlt">deformed</span> version of the Wheeler-DeWitt equation. Then we will further <span class="hlt">deform</span> the third quantized theory by <span class="hlt">deforming</span> the third quantized canonical commutation relation. This way we will obtain a <span class="hlt">deformed</span> version of the third quantized theory for the multiverse.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/10175151-tensile-deformation-recovery-kinetics-alloy-final-report','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/10175151-tensile-deformation-recovery-kinetics-alloy-final-report"><span>Tensile <span class="hlt">deformation</span> and recovery kinetics of Alloy 690. Final report</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Lo, C.F.; Mayo, W.E.; Weissmann, S.</p> <p>1992-07-01</p> <p>The effect of carbon content, grain size and thermal history on the <span class="hlt">deformation</span> behavior of nickel-base Alloy 690 has been investigated. Carbon content effects the yield strength of Mill Annealed (MA) material, but has no effect in Thermally Treated (TT) material. Also, no effect of carbon content on the workhardening rate was seen in either material. There was an effect of grain size as expected. An interesting aspect of this work showed that TT material consistently has a slightly higher Young`s modulus than the MA. As <span class="hlt">deformation</span> moves into the plastic regime, the TT material displays a two stage hardeningmore » process. This consists of a low workhardening rate (n = 0.05), followed by a transition to the more normal workhardening rate (n=0.35). The MA material, on the other hand, does not exhibit the low n region. This unusual <span class="hlt">deformation</span> behavior is attributable to the presence of planar slip which initiates at the grain boundary over the strain range of 0.2 to 0.7%. These observations are useful to explain the unexpectedly fast strain relaxation behavior seen in this alloy. The recovery kinetics of the alloy have also been studied. Rapid recovery with an activation <span class="hlt">energy</span> of approximately 5.3 kj/mol occurs when the <span class="hlt">deformation</span> level is low. This was attributed to a grain boundary self diffusion process. At higher strain levels, recovery is much slower with an activation <span class="hlt">energy</span> of approximately 14 kJ/mol. This process was attributable to bulk diffusion. Based on TEM and X-ray rocking curve measurements, these results have been explained.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21583297-wilson-loops-warped-resolved-deformed-conifolds','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21583297-wilson-loops-warped-resolved-deformed-conifolds"><span>Wilson loops in warped resolved <span class="hlt">deformed</span> conifolds</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Bennett, Stephen, E-mail: pystephen@swansea.ac.uk</p> <p></p> <p>We calculate quark-antiquark potentials using the relationship between the expectation value of the Wilson loop and the action of a probe string in the string dual. We review and categorise the possible forms of the dependence of the <span class="hlt">energy</span> on the separation between the quarks. In particular, we examine the possibility of there being a minimum separation for probe strings which do not penetrate close to the origin of the bulk space, and derive a condition which determines whether this is the case. We then apply these considerations to the flavoured resolved <span class="hlt">deformed</span> conifold background of Gaillard et al. (2010)more » . We suggest that the unusual behaviour that we observe in this solution is likely to be related to the IR singularity which is not present in the unflavoured case. - Highlights: > We calculate quark-antiquark potentials using the Wilson loop and the action of a probe string in the string dual. > We review and categorise the possible forms of the dependence of the <span class="hlt">energy</span> on the separation between the quarks. > We look in particular at the flavoured resolved <span class="hlt">deformed</span> conifold. > There appears to be unusual behaviour which seems likely to be related to the IR singularity introduced by flavours.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JHEP...03..173K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JHEP...03..173K"><span><span class="hlt">Deformations</span> of the Almheiri-Polchinski model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kyono, Hideki; Okumura, Suguru; Yoshida, Kentaroh</p> <p>2017-03-01</p> <p>We study <span class="hlt">deformations</span> of the Almheiri-Polchinski (AP) model by employing the Yang-Baxter <span class="hlt">deformation</span> technique. The general <span class="hlt">deformed</span> AdS2 metric becomes a solution of a <span class="hlt">deformed</span> AP model. In particular, the dilaton potential is <span class="hlt">deformed</span> from a simple quadratic form to a hyperbolic function-type potential similarly to integrable <span class="hlt">deformations</span>. A specific solution is a <span class="hlt">deformed</span> black hole solution. Because the <span class="hlt">deformation</span> makes the spacetime structure around the boundary change drastically and a new naked singularity appears, the holographic interpretation is far from trivial. The Hawking temperature is the same as the undeformed case but the Bekenstein-Hawking entropy is modified due to the <span class="hlt">deformation</span>. This entropy can also be reproduced by evaluating the renormalized stress tensor with an appropriate counter-term on the regularized screen close to the singularity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70035283','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70035283"><span>Early Tertiary transtension-related <span class="hlt">deformation</span> and magmatism along the Tintina fault system, Alaska</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Till, A.B.; Roeske, S.M.; Bradley, D.C.; Friedman, R.; Layer, P.W.</p> <p>2007-01-01</p> <p>Transtensional <span class="hlt">deformation</span> was concentrated in a zone adjacent to the Tintina strike-slip fault system in Alaska during the early Tertiary. The <span class="hlt">deformation</span> occurred along the Victoria Creek fault, the trace of the Tintina system that connects it with the Kaltag fault; together the Tintina and Kaltag fault systems girdle Alaska from east to west. Over an area of ???25 by 70 km between the Victoria Creek and Tozitna faults, bimodal volcanics erupted; lacustrine and fluvial rocks were deposited; plutons were emplaced and <span class="hlt">deformed</span>; and metamorphic rocks cooled, all at about the same time. Plutonic and volcanic rocks in this zone yield U-Pb zircon ages of ca. 60 Ma; 40Ar/ 39Ar cooling ages from those plutons and adjacent metamorphic rocks are also ca. 60 Ma. Although early Tertiary magmatism occurred over a broad area in central Alaska, meta- morphism and ductile <span class="hlt">deformation</span> accompanied that magmatism in this one zone only. Within the zone of <span class="hlt">deformation</span>, pluton aureoles and metamorphic rocks display consistent NE-SW-stretching lineations parallel to the Victoria Creek fault, suggesting that <span class="hlt">deformation</span> processes involved subhorizontal elongation of the package. The most deeply buried metamorphic rocks, kyanite-bearing metapelites, occur as lenses adjacent to the fault, which cuts the crust to the Moho (Beaudoin et al., 1997). Geochronologic data and field relationships suggest that the amount of early Tertiary exhumation was greatest adjacent to the Victoria Creek fault. The early Tertiary crustal-scale events that may have operated to produce transtension in this area are (1) increased heat flux and related bimodal within-plate magmatism, (2) movement on a <span class="hlt">releasing</span> stepover within the Tintina fault system or on a regional scale involving both the Tintina and the Kobuk fault systems, and (3) oroclinal bending of the Tintina-Kaltag fault system with counterclockwise rotation of western Alaska. ?? 2007 The Geological Society of America. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.G11A0467L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.G11A0467L"><span>Spatial scale of <span class="hlt">deformation</span> constrained by combinations of InSAR and GPS observations in Southern California</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lohman, R. B.; Scott, C. P.</p> <p>2014-12-01</p> <p>Efforts to understand the buildup and <span class="hlt">release</span> of strain within the Earth's crust often rely on well-characterized observations of ground <span class="hlt">deformation</span>, over time scales that include interseismic periods, earthquakes, and transient <span class="hlt">deformation</span> episodes. Constraints on current rates of surface <span class="hlt">deformation</span> in 1-, 2- or 3-dimensions can be obtained by examining sets of GPS and Interferometric Synthetic Aperture Radar (InSAR) observations, both alone and in combination. Contributions to the observed signal often include motion along faults, seasonal cycles of subsidence and recharge associated with aquifers, anthropogenic extraction of hydrocarbons, and variations in atmospheric water vapor and ionospheric properties. Here we examine methods for extracting time-varying ground <span class="hlt">deformation</span> signals from combinations of InSAR and GPS data, real and synthetic, applied to Southern California. We show that two methods for combining the data through removal of a GPS-constrained function (a plane, and filtering) from the InSAR result in a clear tradeoff between the contribution from the two datatypes at diffferent spatial scales. We also show that the contribution to the secular rates at GPS sites from seasonal signals is large enough to be a significant error in this estimation process, and should be accounted for.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA261703','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA261703"><span>Defect Initiation/Growth and <span class="hlt">Energy</span> Dissipation Induced by <span class="hlt">Deformation</span> and Fracture</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1993-01-01</p> <p><span class="hlt">deformation</span> in MgO single crystals . 4 III. Molecular CO emission accompanying fracture of polycarbonate: evidence for chain cleavage J. T. Dickinson, L. C... Crystal MgO Although not a polymer, we wish to point out that the fracture-induced phE and EE from the fracture of single crystal MgQ 17 (Fig. 7) is...long times. This is a good qualitative description of the behavior exhibited by EE from in some systems. C. Single Crystal MgO Williams et al. have</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6897955','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/6897955"><span>Shock wave absorber having a <span class="hlt">deformable</span> liner</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Youngdahl, C.K.; Wiedermann, A.H.; Shin, Y.W.; Kot, C.A.; Ockert, C.E.</p> <p>1983-08-26</p> <p>This invention discloses a shock wave absorber for a piping system carrying liquid. The absorber has a plastically <span class="hlt">deformable</span> liner defining the normal flow boundary for an axial segment of the piping system, and a nondeformable housing is spaced outwardly from the liner so as to define a gas-tight space therebetween. The flow capacity of the liner generally corresponds to the flow capacity of the piping system line, but the liner has a noncircular cross section and extends axially of the piping system line a distance between one and twenty times the diameter thereof. Gas pressurizes the gas-tight space equal to the normal liquid pressure in the piping system. The liner has sufficient structural capacity to withstand between one and one-half and two times this normal liquid pressures; but at greater pressures it begins to plastically <span class="hlt">deform</span> initially with respect to shape to a more circular cross section, and then with respect to material extension by circumferentially stretching the wall of the liner. A high <span class="hlt">energy</span> shock wave passing through the liner thus plastically <span class="hlt">deforms</span> the liner radially into the gas space and progressively also as needed in the axial direction of the shock wave to minimize transmission of the shock wave beyond the absorber.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvC..94c4321H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvC..94c4321H"><span><span class="hlt">Deformation</span> of the proton emitter 113Cs from electromagnetic transition and proton-emission rates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hodge, D.; Cullen, D. M.; Taylor, M. J.; Nara Singh, B. S.; Ferreira, L. S.; Maglione, E.; Smith, J. F.; Scholey, C.; Rahkila, P.; Grahn, T.; Braunroth, T.; Badran, H.; Capponi, L.; Girka, A.; Greenlees, P. T.; Julin, R.; Konki, J.; Mallaburn, M.; Nefodov, O.; O'Neill, G. G.; Pakarinen, J.; Papadakis, P.; Partanen, J.; Ruotsalainen, P.; Sandzelius, M.; Sarén, J.; Smolen, M.; Sorri, J.; Stolze, S.; Uusitalo, J.</p> <p>2016-09-01</p> <p>The lifetime of the (11 /2+ ) state in the band above the proton-emitting (3 /2+ ) state in 113Cs has been measured to be τ =24 (6 ) ps from a recoil-decay-tagged differential-plunger experiment. The measured lifetime was used to deduce the <span class="hlt">deformation</span> of the states using wave functions from a nonadiabatic quasiparticle model to independently calculate both proton-emission and electromagnetic γ -ray transition rates as a function of <span class="hlt">deformation</span>. The only quadrupole <span class="hlt">deformation</span>, which was able to reproduce the experimental excitation <span class="hlt">energies</span> of the states, the electromagnetic decay rate of the (11 /2+ ) state and the proton-emission rate of the (3 /2+ ) state, was found to be β2=0.22 (6 ) . This <span class="hlt">deformation</span> is in agreement with the earlier proton emission studies which concluded that 113Cs was best described as a <span class="hlt">deformed</span> proton emitter, however, it is now more firmly supported by the present measurement of the electromagnetic transition rate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991navy.reptS....G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991navy.reptS....G"><span>Geothermal <span class="hlt">energy</span> conversion system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Goldstein, David</p> <p>1991-04-01</p> <p>A generator having a tubular gear made of shape memory alloy in sheet-form floatingly supported for rotation about an axis fixedly spaced from the rotational axis of a roller gear presented. The tubular gear is sequentially <span class="hlt">deformed</span> by exposure to a geothermal heat source and meshing engagement with the roller gear. Such sequential <span class="hlt">deformation</span> of the tubular gear is controlled by a temperature differential to induce and sustain rotation of the gears in response to which the heat <span class="hlt">energy</span> is converted into electrical <span class="hlt">energy</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJWC.16900024T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJWC.16900024T"><span>Fission fragment yields and total kinetic <span class="hlt">energy</span> <span class="hlt">release</span> in neutron-induced fission of235,238U,and239Pu</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tovesson, F.; Duke, D.; Geppert-Kleinrath, V.; Manning, B.; Mayorov, D.; Mosby, S.; Schmitt, K.</p> <p>2018-03-01</p> <p>Different aspects of the nuclear fission process have been studied at Los Alamos Neutron Science Center (LANSCE) using various instruments and experimental techniques. Properties of the fragments emitted in fission have been investigated using Frisch-grid ionization chambers, a Time Projection Chamber (TPC), and the SPIDER instrument which employs the 2v-2E method. These instruments and experimental techniques have been used to determine fission product mass yields, the <span class="hlt">energy</span> dependent total kinetic <span class="hlt">energy</span> (TKE) <span class="hlt">release</span>, and anisotropy in neutron-induced fission of U-235, U-238 and Pu-239.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25365458','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25365458"><span>Wireless sensor networks for heritage object <span class="hlt">deformation</span> detection and tracking algorithm.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xie, Zhijun; Huang, Guangyan; Zarei, Roozbeh; He, Jing; Zhang, Yanchun; Ye, Hongwu</p> <p>2014-10-31</p> <p><span class="hlt">Deformation</span> is the direct cause of heritage object collapse. It is significant to monitor and signal the early warnings of the <span class="hlt">deformation</span> of heritage objects. However, traditional heritage object monitoring methods only roughly monitor a simple-shaped heritage object as a whole, but cannot monitor complicated heritage objects, which may have a large number of surfaces inside and outside. Wireless sensor networks, comprising many small-sized, low-cost, low-power intelligent sensor nodes, are more useful to detect the <span class="hlt">deformation</span> of every small part of the heritage objects. Wireless sensor networks need an effective mechanism to reduce both the communication costs and <span class="hlt">energy</span> consumption in order to monitor the heritage objects in real time. In this paper, we provide an effective heritage object <span class="hlt">deformation</span> detection and tracking method using wireless sensor networks (EffeHDDT). In EffeHDDT, we discover a connected core set of sensor nodes to reduce the communication cost for transmitting and collecting the data of the sensor networks. Particularly, we propose a heritage object boundary detecting and tracking mechanism. Both theoretical analysis and experimental results demonstrate that our EffeHDDT method outperforms the existing methods in terms of network traffic and the precision of the <span class="hlt">deformation</span> detection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4279500','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4279500"><span>Wireless Sensor Networks for Heritage Object <span class="hlt">Deformation</span> Detection and Tracking Algorithm</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Xie, Zhijun; Huang, Guangyan; Zarei, Roozbeh; He, Jing; Zhang, Yanchun; Ye, Hongwu</p> <p>2014-01-01</p> <p><span class="hlt">Deformation</span> is the direct cause of heritage object collapse. It is significant to monitor and signal the early warnings of the <span class="hlt">deformation</span> of heritage objects. However, traditional heritage object monitoring methods only roughly monitor a simple-shaped heritage object as a whole, but cannot monitor complicated heritage objects, which may have a large number of surfaces inside and outside. Wireless sensor networks, comprising many small-sized, low-cost, low-power intelligent sensor nodes, are more useful to detect the <span class="hlt">deformation</span> of every small part of the heritage objects. Wireless sensor networks need an effective mechanism to reduce both the communication costs and <span class="hlt">energy</span> consumption in order to monitor the heritage objects in real time. In this paper, we provide an effective heritage object <span class="hlt">deformation</span> detection and tracking method using wireless sensor networks (EffeHDDT). In EffeHDDT, we discover a connected core set of sensor nodes to reduce the communication cost for transmitting and collecting the data of the sensor networks. Particularly, we propose a heritage object boundary detecting and tracking mechanism. Both theoretical analysis and experimental results demonstrate that our EffeHDDT method outperforms the existing methods in terms of network traffic and the precision of the <span class="hlt">deformation</span> detection. PMID:25365458</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009JAP...106h3512W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009JAP...106h3512W"><span>A quantitative link between microplastic instability and macroscopic <span class="hlt">deformation</span> behaviors in metallic glasses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wu, Y.; Chen, G. L.; Hui, X. D.; Liu, C. T.; Lin, Y.; Shang, X. C.; Lu, Z. P.</p> <p>2009-10-01</p> <p>Based on mechanical instability of individual shear transformation zones (STZs), a quantitative link between the microplastic instability and macroscopic <span class="hlt">deformation</span> behavior of metallic glasses was proposed. Our analysis confirms that macroscopic metallic glasses comprise a statistical distribution of STZ embryos with distributed values of activation <span class="hlt">energy</span>, and the microplastic instability of all the individual STZs dictates the macroscopic <span class="hlt">deformation</span> behavior of amorphous solids. The statistical model presented in this paper can successfully reproduce the macroscopic stress-strain curves determined experimentally and readily be used to predict strain-rate effects on the macroscopic responses with the availability of the material parameters at a certain strain rate, which offer new insights into understanding the actual <span class="hlt">deformation</span> mechanism in amorphous solids.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JOM....67e.966K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JOM....67e.966K"><span>Modeling the Hot Ductility of AA6061 Aluminum Alloy After Severe Plastic <span class="hlt">Deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Khamei, A. A.; Dehghani, K.; Mahmudi, R.</p> <p>2015-05-01</p> <p>Solutionized AA6061 aluminum alloy was processed by equal-channel angular pressing followed by cold rolling. The hot ductility of the material was studied after severe plastic <span class="hlt">deformation</span>. The hot tensile tests were carried out in the temperature range of 300-500°C and at the strain rates of 0.0005-0.01 s-1. Depending on the temperature and strain rate, the applied strain level exhibited significant effects on the hot ductility, strain-rate sensitivity, and activation <span class="hlt">energy</span>. It can be suggested that the possible mechanism dominated the hot <span class="hlt">deformation</span> during tensile testing is dynamic recovery and dislocation creep. Constitutive equations were developed to model the hot ductility of the severe plastic <span class="hlt">deformed</span> AA6061 alloy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012NatCo...3E1164L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012NatCo...3E1164L"><span>High strain rate <span class="hlt">deformation</span> of layered nanocomposites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Jae-Hwang; Veysset, David; Singer, Jonathan P.; Retsch, Markus; Saini, Gagan; Pezeril, Thomas; Nelson, Keith A.; Thomas, Edwin L.</p> <p>2012-11-01</p> <p>Insight into the mechanical behaviour of nanomaterials under the extreme condition of very high <span class="hlt">deformation</span> rates and to very large strains is needed to provide improved understanding for the development of new protective materials. Applications include protection against bullets for body armour, micrometeorites for satellites, and high-speed particle impact for jet engine turbine blades. Here we use a microscopic ballistic test to report the responses of periodic glassy-rubbery layered block-copolymer nanostructures to impact from hypervelocity micron-sized silica spheres. Entire <span class="hlt">deformation</span> fields are experimentally visualized at an exceptionally high resolution (below 10 nm) and we discover how the microstructure dissipates the impact <span class="hlt">energy</span> via layer kinking, layer compression, extreme chain conformational flattening, domain fragmentation and segmental mixing to form a liquid phase. Orientation-dependent experiments show that the dissipation can be enhanced by 30% by proper orientation of the layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23132014','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23132014"><span>High strain rate <span class="hlt">deformation</span> of layered nanocomposites.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Jae-Hwang; Veysset, David; Singer, Jonathan P; Retsch, Markus; Saini, Gagan; Pezeril, Thomas; Nelson, Keith A; Thomas, Edwin L</p> <p>2012-01-01</p> <p>Insight into the mechanical behaviour of nanomaterials under the extreme condition of very high <span class="hlt">deformation</span> rates and to very large strains is needed to provide improved understanding for the development of new protective materials. Applications include protection against bullets for body armour, micrometeorites for satellites, and high-speed particle impact for jet engine turbine blades. Here we use a microscopic ballistic test to report the responses of periodic glassy-rubbery layered block-copolymer nanostructures to impact from hypervelocity micron-sized silica spheres. Entire <span class="hlt">deformation</span> fields are experimentally visualized at an exceptionally high resolution (below 10 nm) and we discover how the microstructure dissipates the impact <span class="hlt">energy</span> via layer kinking, layer compression, extreme chain conformational flattening, domain fragmentation and segmental mixing to form a liquid phase. Orientation-dependent experiments show that the dissipation can be enhanced by 30% by proper orientation of the layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.bssaonline.org/content/84/3/835.abstract','USGSPUBS'); return false;" href="http://www.bssaonline.org/content/84/3/835.abstract"><span>Triggered seismicity and <span class="hlt">deformation</span> between the Landers, California, and Little Skull Mountain, Nevada, earthquakes</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Bodin, Paul; Gomberg, Joan</p> <p>1994-01-01</p> <p>This article presents evidence for the channeling of strain <span class="hlt">energy</span> <span class="hlt">released</span> by the Ms = 7.4 Landers, California, earthquake within the eastern California shear zone (ECSZ). We document an increase in seismicity levels during the 22-hr period starting with the Landers earthquake and culminating 22 hr later with the Ms = 5.4 Little Skull Mountain (LSM), Nevada, earthquake. We evaluate the completeness of regional seismicity catalogs during this period and find that the continuity of post-Landers strain <span class="hlt">release</span> within the ECSZ is even more pronounced than is evident from the catalog data. We hypothesize that regional-scale connectivity of faults within the ECSZ and LSM region is a critical ingredient in the unprecedented scale and distribution of remotely triggered earthquakes and geodetically manifest strain changes that followed the Landers earthquake. The viability of static strain changes as triggering agents is tested using numerical models. Modeling results illustrate that regional-scale fault connectivity can increase the static strain changes by approximately an order of magnitude at distances of at least 280 km, the distance between the Landers and LSM epicenters. This is possible for models that include both a network of connected faults that slip “sympathetically” and realistic levels of tectonic prestrain. Alternatively, if dynamic strains are a more significant triggering agent than static strains, ECSZ structure may still be important in determining the distribution of triggered seismic and aseismic <span class="hlt">deformation</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JHEP...01..132F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JHEP...01..132F"><span><span class="hlt">Deformed</span> supersymmetric quantum mechanics with spin variables</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fedoruk, Sergey; Ivanov, Evgeny; Sidorov, Stepan</p> <p>2018-01-01</p> <p>We quantize the one-particle model of the SU(2|1) supersymmetric multiparticle mechanics with the additional semi-dynamical spin degrees of freedom. We find the relevant <span class="hlt">energy</span> spectrum and the full set of physical states as functions of the mass-dimension <span class="hlt">deformation</span> parameter m and SU(2) spin q\\in (Z_{>0,}1/2+Z_{≥0}) . It is found that the states at the fixed <span class="hlt">energy</span> level form irreducible multiplets of the supergroup SU(2|1). Also, the hidden superconformal symmetry OSp(4|2) of the model is revealed in the classical and quantum cases. We calculate the OSp(4|2) Casimir operators and demonstrate that the full set of the physical states belonging to different <span class="hlt">energy</span> levels at fixed q are unified into an irreducible OSp(4|2) multiplet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70197477','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70197477"><span>Injection-induced moment <span class="hlt">release</span> can also be aseismic</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>McGarr, Arthur; Barbour, Andrew J.</p> <p>2018-01-01</p> <p>The cumulative seismic moment is a robust measure of the earthquake response to fluid injection for injection volumes ranging from 3100 to about 12 million m3. Over this range, the moment <span class="hlt">release</span> is limited to twice the product of the shear modulus and the volume of injected fluid. This relation also applies at the much smaller injection volumes of the field experiment in France reported by Guglielmi, et al. (2015) and laboratory experiments to simulate hydraulic fracturing described by Goodfellow, et al. (2015). In both of these studies, the relevant moment <span class="hlt">release</span> for comparison with the fluid injection was aseismic and consistent with the scaling that applies to the much larger volumes associated with injection-induced earthquakes with magnitudes extending up to 5.8. Neither the micro-earthquakes, at the site in France, nor the acoustic emission in the laboratory samples contributed significantly to the <span class="hlt">deformation</span> due to fluid injection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/2283442','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/2283442"><span>Frame junction vibration transmission with a modified frame <span class="hlt">deformation</span> model.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Moore, J A</p> <p>1990-12-01</p> <p>A previous paper dealt with vibration transmission through junctions of connected frame members where the allowed frame <span class="hlt">deformations</span> included bending, torsion, and longitudinal motions [J.A. Moore, J. Acoust. Soc. Am. 88, 2766-2776 (1990)]. In helicopter and aircraft structures the skin panels can constitute a high impedance connection along the length of the frames that effectively prohibits in-plane motion at the elevation of the skin panels. This has the effect of coupling in-plane bending and torsional motions within the frame. This paper discusses the transmission behavior through frame junctions that accounts for the in-plane constraint in idealized form by assuming that the attached skin panels completely prohibit inplane motion in the frames. Also, transverse shear <span class="hlt">deformation</span> is accounted for in describing the relatively deep web frame constructions common in aircraft structures. Longitudinal motion in the frames is not included in the model. Transmission coefficient predictions again show the importance of out-of-plane bending <span class="hlt">deformation</span> to the transmission of vibratory <span class="hlt">energy</span> in an aircraft structure. Comparisons are shown with measured vibration transmission data along the framing in the overhead of a helicopter airframe, with good agreement. The frame junction description has been implemented within a general purpose statistical <span class="hlt">energy</span> analysis (SEA) computer code in modeling the entire airframe structure including skin panels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2011-title10-vol1/pdf/CFR-2011-title10-vol1-sec20-2003.pdf','CFR2011'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2011-title10-vol1/pdf/CFR-2011-title10-vol1-sec20-2003.pdf"><span>10 CFR 20.2003 - Disposal by <span class="hlt">release</span> into sanitary sewerage.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2011&page.go=Go">Code of Federal Regulations, 2011 CFR</a></p> <p></p> <p>2011-01-01</p> <p>... 10 <span class="hlt">Energy</span> 1 2011-01-01 2011-01-01 false Disposal by <span class="hlt">release</span> into sanitary sewerage. 20.2003 Section 20.2003 <span class="hlt">Energy</span> NUCLEAR REGULATORY COMMISSION STANDARDS FOR PROTECTION AGAINST RADIATION Waste Disposal § 20.2003 Disposal by <span class="hlt">release</span> into sanitary sewerage. (a) A licensee may discharge licensed...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2013-title10-vol1/pdf/CFR-2013-title10-vol1-sec20-2003.pdf','CFR2013'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2013-title10-vol1/pdf/CFR-2013-title10-vol1-sec20-2003.pdf"><span>10 CFR 20.2003 - Disposal by <span class="hlt">release</span> into sanitary sewerage.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2013&page.go=Go">Code of Federal Regulations, 2013 CFR</a></p> <p></p> <p>2013-01-01</p> <p>... 10 <span class="hlt">Energy</span> 1 2013-01-01 2013-01-01 false Disposal by <span class="hlt">release</span> into sanitary sewerage. 20.2003 Section 20.2003 <span class="hlt">Energy</span> NUCLEAR REGULATORY COMMISSION STANDARDS FOR PROTECTION AGAINST RADIATION Waste Disposal § 20.2003 Disposal by <span class="hlt">release</span> into sanitary sewerage. (a) A licensee may discharge licensed...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title10-vol1/pdf/CFR-2010-title10-vol1-sec20-2003.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title10-vol1/pdf/CFR-2010-title10-vol1-sec20-2003.pdf"><span>10 CFR 20.2003 - Disposal by <span class="hlt">release</span> into sanitary sewerage.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2010&page.go=Go">Code of Federal Regulations, 2010 CFR</a></p> <p></p> <p>2010-01-01</p> <p>... 10 <span class="hlt">Energy</span> 1 2010-01-01 2010-01-01 false Disposal by <span class="hlt">release</span> into sanitary sewerage. 20.2003 Section 20.2003 <span class="hlt">Energy</span> NUCLEAR REGULATORY COMMISSION STANDARDS FOR PROTECTION AGAINST RADIATION Waste Disposal § 20.2003 Disposal by <span class="hlt">release</span> into sanitary sewerage. (a) A licensee may discharge licensed...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2014-title10-vol1/pdf/CFR-2014-title10-vol1-sec20-2003.pdf','CFR2014'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2014-title10-vol1/pdf/CFR-2014-title10-vol1-sec20-2003.pdf"><span>10 CFR 20.2003 - Disposal by <span class="hlt">release</span> into sanitary sewerage.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2014&page.go=Go">Code of Federal Regulations, 2014 CFR</a></p> <p></p> <p>2014-01-01</p> <p>... 10 <span class="hlt">Energy</span> 1 2014-01-01 2014-01-01 false Disposal by <span class="hlt">release</span> into sanitary sewerage. 20.2003 Section 20.2003 <span class="hlt">Energy</span> NUCLEAR REGULATORY COMMISSION STANDARDS FOR PROTECTION AGAINST RADIATION Waste Disposal § 20.2003 Disposal by <span class="hlt">release</span> into sanitary sewerage. (a) A licensee may discharge licensed...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2012-title10-vol1/pdf/CFR-2012-title10-vol1-sec20-2003.pdf','CFR2012'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2012-title10-vol1/pdf/CFR-2012-title10-vol1-sec20-2003.pdf"><span>10 CFR 20.2003 - Disposal by <span class="hlt">release</span> into sanitary sewerage.</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collectionCfr.action?selectedYearFrom=2012&page.go=Go">Code of Federal Regulations, 2012 CFR</a></p> <p></p> <p>2012-01-01</p> <p>... 10 <span class="hlt">Energy</span> 1 2012-01-01 2012-01-01 false Disposal by <span class="hlt">release</span> into sanitary sewerage. 20.2003 Section 20.2003 <span class="hlt">Energy</span> NUCLEAR REGULATORY COMMISSION STANDARDS FOR PROTECTION AGAINST RADIATION Waste Disposal § 20.2003 Disposal by <span class="hlt">release</span> into sanitary sewerage. (a) A licensee may discharge licensed...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MMTB...49....1Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MMTB...49....1Z"><span>Hot Ductility and Compression <span class="hlt">Deformation</span> Behavior of TRIP980 at Elevated Temperatures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Mei; Li, Haiyang; Gan, Bin; Zhao, Xue; Yao, Yi; Wang, Li</p> <p>2018-02-01</p> <p>The hot ductility tests of a kind of 980 MPa class Fe-0.31C (wt pct) TRIP steel (TRIP980) with the addition of Ti/V/Nb were conducted on a Gleeble-3500 thermomechanical simulator in the temperatures ranging from 873 K to 1573 K (600 °C to 1300 °C) at a constant strain rate of 0.001 s-1. It is found that the hot ductility trough ranges from 873 K to 1123 K (600 °C to 850 °C). The recommended straightening temperatures are from 1173 K to 1523 K (900 °C to 1250 °C). The isothermal hot compression <span class="hlt">deformation</span> behavior was also studied by means of Gleeble-3500 in the temperatures ranging from 1173 K to 1373 K (900 °C to 1100 °C) at strain rates ranging from 0.01 s-1 to 10 s-1. The results show that the peak stress decreases with the increasing temperature and the decreasing strain rate. The <span class="hlt">deformation</span> activation <span class="hlt">energy</span> of the test steel is 436.7 kJ/mol. The hot <span class="hlt">deformation</span> equation of the steel has been established, and the processing maps have been developed on the basis of experimental data and the principle of dynamic materials model (DMM). By analyzing the processing maps of strains of 0.5, 0.7, and 0.9, it is found that dynamic recrystallization occurs in the peak power dissipation efficiency domain, which is the optimal area of hot working. Finally, the factors influencing hot ductility and thermal activation <span class="hlt">energy</span> of the test steel were investigated by means of microscopic analysis. It indicates that the additional microalloying elements play important roles both in the loss of hot ductility and in the enormous increase of <span class="hlt">deformation</span> activation <span class="hlt">energy</span> for the TRIP980 steel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MMTA...48.1310D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MMTA...48.1310D"><span>Hot <span class="hlt">Deformation</span> Behavior and Dynamic Recrystallization of Medium Carbon LZ50 Steel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Du, Shiwen; Chen, Shuangmei; Song, Jianjun; Li, Yongtang</p> <p>2017-03-01</p> <p>Hot <span class="hlt">deformation</span> and dynamic recrystallization behaviors of a medium carbon steel LZ50 were systematically investigated in the temperature range from 1143 K to 1443 K (870 °C to 1170 °C) at strain rates from 0.05 to 3s-1 using a Gleeble-3500 thermo-simulation machine. The flow stress constitutive equation for hot <span class="hlt">deformation</span> of this steel was developed with the two-stage Laasraoui equation. The activation <span class="hlt">energy</span> of the tested steel was 304.27 KJ/mol, which was in reasonable agreement with those reported previously. The flow stress of this steel in hot <span class="hlt">deformation</span> was mainly controlled by dislocation climb during their intragranular motion. The effect of Zener-Hollomon parameter on the characteristic points of the flow curves was studied, and the dependence of critical strain on peak strain obeyed a linear equation. Dynamic recrystallization was the most important softening mechanism for the tested steel during hot <span class="hlt">deformation</span>. Kinetic equation of this steel was also established based on the flow stress. The austenite grain size of complete dynamic recrystallization was a power law function of Zener-Hollomon parameter with an exponent of -0.2956. Moreover, the microstructures induced under different <span class="hlt">deformation</span> conditions were analyzed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22494119-su-evaluation-accuracy-various-deformable-image-registrations-virtual-deformation-qa-software','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22494119-su-evaluation-accuracy-various-deformable-image-registrations-virtual-deformation-qa-software"><span>SU-E-J-104: Evaluation of Accuracy for Various <span class="hlt">Deformable</span> Image Registrations with Virtual <span class="hlt">Deformation</span> QA Software</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Han, S; Kim, K; Kim, M</p> <p></p> <p>Purpose: The accuracy of <span class="hlt">deformable</span> image registration (DIR) has a significant dosimetric impact in radiation treatment planning. We evaluated accuracy of various DIR algorithms using virtual <span class="hlt">deformation</span> QA software (ImSimQA, Oncology System Limited, UK). Methods: The reference image (Iref) and volume (Vref) was first generated with IMSIMQA software. We <span class="hlt">deformed</span> Iref with axial movement of <span class="hlt">deformation</span> point and Vref depending on the type of <span class="hlt">deformation</span> that are the <span class="hlt">deformation</span>1 is to increase the Vref (relaxation) and the <span class="hlt">deformation</span> 2 is to decrease the Vref (contraction) .The <span class="hlt">deformed</span> image (Idef) and volume (Vdef) were inversely <span class="hlt">deformed</span> to Iref and Vref usingmore » DIR algorithms. As a Result, we acquired <span class="hlt">deformed</span> image (Iid) and volume (Vid). The DIR algorithms were optical flow (HS, IOF) and demons (MD, FD) of the DIRART. The image similarity evaluation between Iref and Iid was calculated by Normalized Mutual Information (NMI) and Normalized Cross Correlation (NCC). The value of Dice Similarity Coefficient (DSC) was used for evaluation of volume similarity. Results: When moving distance of <span class="hlt">deformation</span> point was 4 mm, the value of NMI was above 1.81 and NCC was above 0.99 in all DIR algorithms. Since the degree of <span class="hlt">deformation</span> was increased, the degree of image similarity was decreased. When the Vref increased or decreased about 12%, the difference between Vref and Vid was within ±5% regardless of the type of <span class="hlt">deformation</span>. The value of DSC was above 0.95 in <span class="hlt">deformation</span>1 except for the MD algorithm. In case of <span class="hlt">deformation</span> 2, that of DSC was above 0.95 in all DIR algorithms. Conclusion: The Idef and Vdef have not been completely restored to Iref and Vref and the accuracy of DIR algorithms was different depending on the degree of <span class="hlt">deformation</span>. Hence, the performance of DIR algorithms should be verified for the desired applications.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28113125','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28113125"><span>Mechanism of drug <span class="hlt">release</span> from silica-gelatin aerogel-Relationship between matrix structure and <span class="hlt">release</span> kinetics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Veres, Péter; Kéri, Mónika; Bányai, István; Lázár, István; Fábián, István; Domingo, Concepción; Kalmár, József</p> <p>2017-04-01</p> <p>Specific features of a silica-gelatin aerogel (3 wt.% gelatin content) in relation to drug delivery has been studied. It was confirmed that the <span class="hlt">release</span> of both ibuprofen (IBU) and ketoprofen (KET) is about tenfold faster from loaded silica-gelatin aerogel than from pure silica aerogel, although the two matrices are structurally very similar. The main goal of the study was to understand the mechanistic background of the striking difference between the delivery properties of these closely related porous materials. Hydrated and dispersed silica-gelatin aerogel has been characterized by NMR cryoporometry, diffusiometry and relaxometry. The pore structure of the silica aerogel remains intact when it disintegrates in water. In contrast, dispersed silica-gelatin aerogel develops a strong hydration sphere, which reshapes the pore walls and <span class="hlt">deforms</span> the pore structure. The drug <span class="hlt">release</span> kinetics was studied on a few minutes time scale with 1s time resolution. Simultaneous evaluation of all relevant kinetic and structural information confirmed that strong hydration of the silica-gelatin skeleton facilitates the rapid desorption and dissolution of the drugs from the loaded aerogel. Such a driving force is not operative in pure silica aerogels. Copyright © 2017 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.T24B..01P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.T24B..01P"><span>Plastic <span class="hlt">Deformation</span> of Quartz: Unfinished business?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Paterson, M. S.</p> <p>2011-12-01</p> <p>Starting at Harvard in the mid-1930's, David Griggs built a series of high pressure machines for experimental rock <span class="hlt">deformation</span>. One persistent aim was to achieve the plastic <span class="hlt">deformation</span> of quartz. Each time he built a new machine for higher pressure and/or temperature, one of the first materials he tested would be quartz. This search went on through a 500 MPa liquid-medium machine at temperatures up to 300°C, then with a gas-medium machine for temperatures up to 800°C, and finally with a solid-medium machine for higher pressures and temperatures. Quartz proved stubbornly resistant to <span class="hlt">deformation</span> except at extremely high stresses until, finally and somewhat serendipitously, it was found possible to <span class="hlt">deform</span> quartz at relatively low stresses in the presence of water under special conditions. The breakthrough came in an experiment in a 1500 MPa solid-medium apparatus in which talc was used as pressure medium. At the temperature of the experiment, the talc dehydrated and so <span class="hlt">released</span> water. Under these conditions, natural quartz proved to be very weak and to readily undergo plastic <span class="hlt">deformation</span>, a phenomenon that became known as "hydrolytic weakening". Soon after this discovery, it was also found that certain synthetic single crystals could be easily <span class="hlt">deformed</span> ab initio. These crystals were from a particular set that had been grown rapidly under hydrothermal conditions and had incorporated water during growth. Attempts in our laboratory to weaken crystals in a gas-medium apparatus at around 300 MPa by cooking dry quartz in the presence of added water were all unsuccessful, although we could <span class="hlt">deform</span> wet synthetic crystals. There was considerable speculation about a role of high pressure in promoting hydrolytic weakening, but the dilemma was eventually clarified by electron microscope studies by Fitz Gerald and coworkers. These studies showed that crystals that had been subjected to high pressure and temperature in the solid-medium apparatus were extensively microcracked</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1811894S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1811894S"><span>Infrared absorption band in <span class="hlt">deformed</span> qtz crystals analyzed by combining different microstructural methods</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stunitz, Holger; Thust, Anja; Behrens, Harald; Heilbronner, Renee; Kilian, Ruediger</p> <p>2016-04-01</p> <p>Natural single crystals of quartz have been experimentally <span class="hlt">deformed</span> in two orientations: (1) normal to one prism-plane, (2) In O+ orientation at temperatures of 900 and 1000°C, pressures of 1.0 and 1.5 GPa, and strain rates of ~1 x 10-6s-1. The starting material is milky quartz, consisting of dry quartz (H2O contents of <150 H/106Si) with fluid inclusions (FI). During pressurization many FÍs decrepitate. Cracks heal and small neonate FÍs form, increasing the number of FÍs drastically. During subsequent <span class="hlt">deformation</span>, the size of FÍs is further reduced (down to ~10 nm). Sample <span class="hlt">deformation</span> occurs by dominant dislocation glide on selected slip systems, accompanied by some dynamic recovery. Strongly <span class="hlt">deformed</span> regions show FTIR spectra with a pointed broad absorption band in the ~3400 cm-1 region as a superposition of molecular H2O bands and three discrete absorption bands (at 3367, 3400, and 3434 cm-1). In addition, there is a discrete absorption band at 3585 cm-1, which only occurs in <span class="hlt">deformed</span> regions. The 3585 cm-1 band is reduced or even disappears after annealing. This band is polarized and represents structurally bound H, its H-content is estimated to be 1-3% of the total H2O-content and appears to be associated with dislocations. The H2O weakening effect in our FI-bearing natural quartz crystals is assigned to the processes of dislocation generation and multiplication at small FÍs. The <span class="hlt">deformation</span> processes in these crystals represent a recycling of H2O between FÍs, dislocation generation at very small fluid inclusions, incorporation of structurally bound H into dislocation cores, and <span class="hlt">release</span> of H2O from dislocations back into FÍs during recovery. Cracking and crack healing play an important role in the recycling process and imply a close interrelationship between brittle and crystal plastic <span class="hlt">deformation</span>. The H2O weakening by this process is of a disequilibrium nature and thus depends on the amount of H2O available.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1248866-nuclear-ground-state-masses-deformations-frdm','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1248866-nuclear-ground-state-masses-deformations-frdm"><span>Nuclear ground-state masses and <span class="hlt">deformations</span>: FRDM(2012)</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Moller, P.; Sierk, A. J.; Ichikawa, T.; ...</p> <p>2016-03-25</p> <p>Here, we tabulate the atomic mass excesses and binding <span class="hlt">energies</span>, ground-state shell-plus-pairing corrections, ground-state microscopic corrections, and nuclear ground-state <span class="hlt">deformations</span> of 9318 nuclei ranging from 16O to A=339. The calculations are based on the finite-range droplet macroscopic and the folded-Yukawa single-particle microscopic nuclear-structure models, which are completely specified. Relative to our FRDM(1992) mass table in Möller et al. (1995), the results are obtained in the same model, but with considerably improved treatment of <span class="hlt">deformation</span> and fewer of the approximations that were necessary earlier, due to limitations in computer power. The more accurate execution of the model and the more extensivemore » and more accurate experimental mass data base now available allow us to determine one additional macroscopic-model parameter, the density-symmetry coefficient LL, which was not varied in the previous calculation, but set to zero. Because we now realize that the FRDM is inaccurate for some highly <span class="hlt">deformed</span> shapes occurring in fission, because some effects are derived in terms of perturbations around a sphere, we only adjust its macroscopic parameters to ground-state masses.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSH21A2064G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSH21A2064G"><span>Intermittent Flare <span class="hlt">Energy</span> <span class="hlt">Release</span>: A Signature of Contracting Magnetic Islands from Reconnection?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guidoni, S. E.; Karpen, J. T.; DeVore, C.</p> <p>2013-12-01</p> <p>Many flares show short-lived enhancements of emission that protrude above their smooth underlying emission. These spikes have been observed over a vast <span class="hlt">energy</span> spectrum, from radio to hard x-rays. In hard X-rays, for example, their duration ranges from 0.2 to 2 s, with the majority occurring during the flare impulsive phase (Cheng 2012). In most cases, this intermittent <span class="hlt">energy</span> <span class="hlt">release</span> is situated at the footpoints of flare arcades where ionized particles, previously accelerated to high <span class="hlt">energies</span> at coronal heights, are decelerated by the dense solar surface. It is not yet understood what mechanisms accelerate ionized particles to the <span class="hlt">energies</span> required to produce the observed emission spikes. Drake et al. (2006) proposed a kinetic mechanism for accelerating electrons from contracting magnetic islands that form as reconnection proceeds, analogous to the <span class="hlt">energy</span> gain of a ball bouncing between converging walls. They estimated that multi-island regions of macroscopic dimensions might account for the required acceleration rates in flares, but at this time it is impractical to simulate large-scale systems in kinetic models. On the other hand, our recent high-resolution MHD simulations of a breakout eruptive flare (Karpen et al. 2012) allow us to resolve in detail the generation and evolution of macroscopic magnetic islands in a flare current sheet. Incorporating a rigorous kinetic model into our global simulations is not feasible at present. However, we intend to breach the gap between kinetic and fluid models by characterizing the contractions of islands as they move away from the main reconnection site, to determine their plausibility as candidates for the observed bursts of radiation. With our null-tracking capabilities, we follow the creation and evolution of the X- and O-type (island) nulls that result from spatially and temporally localized reconnection. Different regimes of current-sheet reconnection (slow/fast), island sizes, rates of island coalescence, and rates</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhRvL.106q5504L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhRvL.106q5504L"><span>High Resolution Transmission Electron Microscope Observation of Zero-Strain <span class="hlt">Deformation</span> Twinning Mechanisms in Ag</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, L.; Wang, J.; Gong, S. K.; Mao, S. X.</p> <p>2011-04-01</p> <p>We have observed a new <span class="hlt">deformation</span>-twinning mechanism using the high resolution transmission electron microscope in polycrystalline Ag films, zero-strain twinning via nucleation, and the migration of a Σ3{112} incoherent twin boundary (ITB). This twinning mechanism produces a near zero macroscopic strain because the net Burgers vectors either equal zero or are equivalent to a Shockley partial dislocation. This observation provides new insight into the understanding of <span class="hlt">deformation</span> twinning and confirms a previous hypothesis: detwinning could be accomplished via the nucleation and migration of Σ3{112} ITBs. The zero-strain twinning mechanism may be unique to low staking fault <span class="hlt">energy</span> metals with implications for their <span class="hlt">deformation</span> behavior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AIPC..894.1691A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AIPC..894.1691A"><span>An RF Therapy System for Breast Cancer Using Dual <span class="hlt">Deformable</span> Mirrors — Computational Study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arunachalam, Kavitha; Udpa, Satish S.; Udpa, Lalita</p> <p>2007-03-01</p> <p>Breast cancer is the second leading cause of cancer deaths amongst women in the United States. In the past two decades, the potential of non-ionizing high power RF waves to destroy cancerous biological tissues is actively investigated for cancer therapy. This paper presents the computational feasibility study of an alternative mode of electromagnetic radiation therapy that employs dual source and <span class="hlt">deformable</span> mirror. The adaptive focusing capability of the <span class="hlt">deformable</span> mirror is exploited for preferential <span class="hlt">energy</span> deposition at the tumor site in the breast irradiated by electromagnetic radiation. The outcome of the computational study for the proposed <span class="hlt">deformable</span> mirror-based thermal therapy for breast cancer is presented in this paper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25570715','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25570715"><span>Multi-classification of cell <span class="hlt">deformation</span> based on object alignment and run length statistic.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Heng; Liu, Zhiwen; An, Xing; Shi, Yonggang</p> <p>2014-01-01</p> <p>Cellular morphology is widely applied in digital pathology and is essential for improving our understanding of the basic physiological processes of organisms. One of the main issues of application is to develop efficient methods for cell <span class="hlt">deformation</span> measurement. We propose an innovative indirect approach to analyze dynamic cell morphology in image sequences. The proposed approach considers both the cellular shape change and cytoplasm variation, and takes each frame in the image sequence into account. The cell <span class="hlt">deformation</span> is measured by the minimum <span class="hlt">energy</span> function of object alignment, which is invariant to object pose. Then an indirect analysis strategy is employed to overcome the limitation of gradual <span class="hlt">deformation</span> by run length statistic. We demonstrate the power of the proposed approach with one application: multi-classification of cell <span class="hlt">deformation</span>. Experimental results show that the proposed method is sensitive to the morphology variation and performs better than standard shape representation methods.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990Tecto...9..585L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990Tecto...9..585L"><span>Kinematics of wrench and divergent-wrench <span class="hlt">deformation</span> along a central part of the Border Ranges Fault System, Northern Chugach Mountains, Alaska</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Little, Timothy A.</p> <p>1990-08-01</p> <p>The Border Ranges fault system (BRFS) bounds the inboard edge of the subduction-accretion complex of southern Alaska. In Eocene time a central segment of this fault system was reactivated as a zone of dextral wrench- and oblique-slip faulting having a cumulative strike-slip offset of at least several tens of kilometers, but probably less than 100 km. Early wrench folds are upright, trend at less than 45° to the strike of adjacent faults and developed with fold axes oriented subparallel to the axis of maximum incremental stretch λ1. These en echelon folds rotated and tightened with progressive <span class="hlt">deformation</span> and then were overprinted by younger wrench folds that trend at about 60° to adjacent throughgoing faults. The latter folds are interpreted as forming during a late increment of distributed wrench <span class="hlt">deformation</span> within the BRFS that included a component of extension (divergence) orthogonal to the mean strike of the fault system. A sharp <span class="hlt">releasing</span> bend in exposures of a strike-slip fault originally at >4 km depth today coincides with a narrow pull-apart graben bounded by oblique-normal faults that dip toward the basin. Widening of this pull-apart graben by brittle faulting and dike intrusion accommodated less than 2 km of strike-slip and was a late-stage phenomenon, possibly occurring at supracrustal levels. Prior to formation of this graben during a period of predominantly ductile <span class="hlt">deformation</span> at deeper structural levels, wrench-folded rocks on one side of the nonplanar fault were translated around the <span class="hlt">releasing</span> bend without significant faulting or loss of coherence. Kinematically, the earlier <span class="hlt">deformation</span> was accomplished by fault-bend folding and rotation of a relatively <span class="hlt">deformable</span> block as it passed through a system of upright megakinks. Such a ductile mechanism of fault block translation around a strike-slip bend may be typical of intermediate levels of the crust beneath pull-apart grabens and may be transitional downward into heterogeneous laminar flow occuring</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PMag...95.2513S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PMag...95.2513S"><span>Effect of <span class="hlt">deformation</span> twin on toughness in magnesium binary alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Somekawa, Hidetoshi; Inoue, Tadanobu; Tsuzaki, Kaneaki</p> <p>2015-08-01</p> <p>The impact of alloying elements on toughness was investigated using eight kinds of Mg-0.3 at.% X (X = Al, Ag, Ca, Gd, Mn, Pb, Y and Zn) binary alloys with meso-grained structures. These binary alloys had an average grain size of approximately 20 μm. The fracture toughness and crack propagation behaviour were influenced by the alloying elements; the Mg-Ag and Mg-Pb alloys had the highest and the lowest toughness amongst the alloys, respectively, irrespective of presence in their ? type <span class="hlt">deformation</span> twins. The twin boundaries affected the crack propagation behaviour in most of the alloys; in contrast, not only was the fracture related to the twin boundaries, but also the intergranular fracture occurred in the alloys that included rare earth elements. The influential factor for toughness in the meso- and the coarse-grained magnesium alloys, which readily formed <span class="hlt">deformation</span> twins during plastic <span class="hlt">deformation</span>, was not the change in lattice parameter with chemical composition, but the twin boundary segregation <span class="hlt">energy</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20371014','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20371014"><span>Comparison of distal chevron osteotomy with and without lateral soft tissue <span class="hlt">release</span> for the treatment of hallux valgus.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lee, Ho-Jin; Chung, Jin-Wha; Chu, In-Tak; Kim, Yoon-Chung</p> <p>2010-04-01</p> <p>A lateral soft tissue <span class="hlt">release</span> is often performed with distal chevron osteotomy for the correction of hallux valgus <span class="hlt">deformities</span>. However, many complications of lateral soft tissue <span class="hlt">release</span> have been reported. To define the necessity of lateral soft tissue <span class="hlt">release</span>, the authors compared the clinical and radiographic results of distal chevron osteotomy with and without it. 86 consecutive patients (152 feet) were enrolled in this prospective study. In Group A, 45 patients (74 feet) underwent a chevron osteotomy with lateral soft tissue <span class="hlt">release</span>. In Group B, 41 patients (78 feet) underwent a chevron osteotomy without it. Mean followup was 1.7 years and 2.1 years, respectively. The hallux valgus angle (HVA) and intermetatarsal angle (IMA), and AOFAS score were measured preoperatively, and 1-year followup postoperatively and complications were evaluated. The change in HVA, IMA and AOFAS score were insignificant (p > 0.05) between Group A and Group B, however, the range of motion of the first metatarsophalangeal joint was significantly less in Group A (p < 0.05). Complications of digital neuritis and cosmetically dissatisfied scarring of the dorsal web space were seen only in Group A. No cases had avascular necrosis of the metatarsal head, malunion or nonunion. Lateral soft tissue <span class="hlt">release</span> may not be needed for mild or moderate hallux valgus <span class="hlt">deformities</span> which may prevent decreased range of motion of the first metatarsophalangeal joint, neuritis of dorsal or plantar lateral digital nerve and cosmetic dissatisfaction of a dorsal scar.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26512339','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26512339"><span>Effects of High-Intensity Training on Anaerobic and Aerobic Contributions to Total <span class="hlt">Energy</span> <span class="hlt">Release</span> During Repeated Supramaximal Exercise in Obese Adults.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jabbour, Georges; Iancu, Horia-Daniel; Paulin, Anne</p> <p></p> <p>Studying relative anaerobic and aerobic metabolism contributions to total <span class="hlt">energy</span> <span class="hlt">release</span> during exercise may be valuable in understanding exercise energetic demands and the energetic adaptations that occur in response to acute or chronic exercise in obese adults. The aim of the present study is to evaluate the effects of 6 weeks of high-intensity training (HIT) on relative anaerobic and aerobic contributions to total <span class="hlt">energy</span> <span class="hlt">release</span> and on peak power output during repeated supramaximal cycling exercises (SCE) in obese adults. Twenty-four obese adults (body mass index = ± 33 kg.m -2 ) were randomized into a control group ( n  = 12) and an HIT group ( n  = 12). Accumulated oxygen deficits (ml.min -1 ) and anaerobic and aerobic contributions (%) were measured in all groups before and after training via repeated SCE. In addition, the peak power output performed during SCE was determined using the force-velocity test. Before HIT, anaerobic contributions to repeated SCE did not differ between the groups and decreased significantly during the third and fourth repetitions. After HIT, anaerobic contributions increased significantly in the HIT group (+11 %, p  < 0.01) and were significantly higher than those of the control group ( p  < 0.01). Moreover, the peak power obtained during SCE increased significantly in the HIT group (+110 W.kg -1 , p  < 0.01) and correlated positively with increases in anaerobic contributions ( r  = 0.9, p  < 0.01). In obese adults, HIT increased anaerobic contributions to <span class="hlt">energy</span> <span class="hlt">release</span> which were associated with peak power enhancement in response to repeated SCE. Consequently, HIT may be an appropriate approach for improving <span class="hlt">energy</span> contributions and muscle power among obese adults.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMNH14A..04S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMNH14A..04S"><span>High Resolution Rapid Revisits Insar Monitoring of Surface <span class="hlt">Deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Singhroy, V.; Li, J.; Charbonneau, F.</p> <p>2014-12-01</p> <p>Monitoring surface <span class="hlt">deformation</span> on strategic <span class="hlt">energy</span> and transportation corridors requires high resolution spatial and temporal InSAR images for mitigation and safety purposes. High resolution air photos, lidar and other satellite images are very useful in areas where the landslides can be fatal. Recently, radar interferometry (InSAR) techniques using more rapid revisit images from several radar satellites are increasingly being used in active <span class="hlt">deformation</span> monitoring. The Canadian RADARSAT Constellation (RCM) is a three-satellite mission that will provide rapid revisits of four days interferometric (InSAR) capabilities that will be very useful for complex <span class="hlt">deformation</span> monitoring. For instance, the monitoring of surface <span class="hlt">deformation</span> due to permafrost activity, complex rock slide motion and steam assisted oil extraction will benefit from this new rapid revisit capability. This paper provide examples of how the high resolution (1-3 m) rapid revisit InSAR capabilities will improve our monitoring of surface <span class="hlt">deformation</span> and provide insights in understanding triggering mechanisms. We analysed over a hundred high resolution InSAR images over a two year period on three geologically different sites with various configurations of topography, geomorphology, and geology conditions. We show from our analysis that the more frequent InSAR acquisitions are providing more information in understanding the rates of movement and failure process of permafrost triggered retrogressive thaw flows; the complex motion of an asymmetrical wedge failure of an active rock slide and the identification of over pressure zones related to oil extraction using steam injection. Keywords: High resolution, InSAR, rapid revisits, triggering mechanisms, oil extraction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPS...332..406K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPS...332..406K"><span>Stretchable spiral thin-film battery capable of out-of-plane <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kammoun, Mejdi; Berg, Sean; Ardebili, Haleh</p> <p>2016-11-01</p> <p>There is a compelling need for innovative design concepts in <span class="hlt">energy</span> storage devices such as flexible and stretchable batteries that can simultaneously provide electrochemical and mechanical functions to accommodate nonconventional applications including wearable and implantable devices. In this study, we report on the design and fabrication of a stretchable spiral thin-film lithium ion battery that is capable of large out-of-plane <span class="hlt">deformation</span> of 1300% while exhibiting simultaneous electrochemical functionality. The spiral battery is fabricated using a flexible solid polymer nanocomposite electrolyte film that offers enhanced safety and stability compared to the conventional organic liquid-based electrolyte. The spiral lithium ion battery exhibits robust mechanical stretchability over 9000 stretching cycles and an <span class="hlt">energy</span> density of 4.862 mWh/cm3 at ∼650% out-of-plane <span class="hlt">deformation</span>. Finite element analysis of the spiral battery offers insights about the nature of stresses and strains during battery stretching.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.eia.gov/outlooks/archive/aeo10/demand.html','EIAPUBS'); return false;" href="https://www.eia.gov/outlooks/archive/aeo10/demand.html"><span><span class="hlt">Energy</span> Demand (<span class="hlt">released</span> in AEO2010)</span></a></p> <p><a target="_blank" href="http://www.eia.doe.gov/reports/">EIA Publications</a></p> <p></p> <p>2010-01-01</p> <p>Growth in U.S. <span class="hlt">energy</span> use is linked to population growth through increases in demand for housing, commercial floorspace, transportation, manufacturing, and services. This affects not only the level of <span class="hlt">energy</span> use, but also the mix of fuels and consumption by sector.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2683897','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2683897"><span><span class="hlt">Deformation</span> Invariant Attribute Vector for <span class="hlt">Deformable</span> Registration of Longitudinal Brain MR Images</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Li, Gang; Guo, Lei; Liu, Tianming</p> <p>2009-01-01</p> <p>This paper presents a novel approach to define <span class="hlt">deformation</span> invariant attribute vector (DIAV) for each voxel in 3D brain image for the purpose of anatomic correspondence detection. The DIAV method is validated by using synthesized <span class="hlt">deformation</span> in 3D brain MRI images. Both theoretic analysis and experimental studies demonstrate that the proposed DIAV is invariant to general nonlinear <span class="hlt">deformation</span>. Moreover, our experimental results show that the DIAV is able to capture rich anatomic information around the voxels and exhibit strong discriminative ability. The DIAV has been integrated into a <span class="hlt">deformable</span> registration algorithm for longitudinal brain MR images, and the results on both simulated and real brain images are provided to demonstrate the good performance of the proposed registration algorithm based on matching of DIAVs. PMID:19369031</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018LMaPh.tmp...51V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018LMaPh.tmp...51V"><span>Nearly associative <span class="hlt">deformation</span> quantization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vassilevich, Dmitri; Oliveira, Fernando Martins Costa</p> <p>2018-04-01</p> <p>We study several classes of non-associative algebras as possible candidates for <span class="hlt">deformation</span> quantization in the direction of a Poisson bracket that does not satisfy Jacobi identities. We show that in fact alternative <span class="hlt">deformation</span> quantization algebras require the Jacobi identities on the Poisson bracket and, under very general assumptions, are associative. At the same time, flexible <span class="hlt">deformation</span> quantization algebras exist for any Poisson bracket.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..MARS26013H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..MARS26013H"><span>Effect of slow <span class="hlt">energy</span> <span class="hlt">releasing</span> on divergent detonation of Insensitive High Explosives</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hu, Xiaomian; Pan, Hao; Huang, Yong; Wu, Zihui</p> <p>2014-03-01</p> <p>There exists a slow <span class="hlt">energy</span> <span class="hlt">releasing</span> (SER) process in the slow reaction zone located behind the detonation wave due to the carbon cluster in the detonation products of Insensitive High Explosives (IHEs), and the process will affect the divergent detonation wave's propagation and the driving process of the explosives. To study the potential effect, a new artificial burn model including the SER process based on the programmed burn model is proposed in the paper. Quasi-steady analysis of the new model indicates that the nonlinearity of the detonation speed as a function of front curvature owes to the significant change of the reaction rate and the reaction zone length at the sonic state. What's more, in simulating the detonation of IHE JB-9014, the new model including the slow reaction can predict a slower jump-off velocity, in good agreement with the result of the test.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MMI....24..401K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MMI....24..401K"><span>Post <span class="hlt">Deformation</span> at Room and Cryogenic Temperature Cooling Media on Severely <span class="hlt">Deformed</span> 1050-Aluminum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Khorrami, M. Sarkari; Kazeminezhad, M.</p> <p>2018-03-01</p> <p>The annealed 1050-aluminum sheets were initially subjected to the severe plastic <span class="hlt">deformation</span> through two passes of constrained groove pressing (CGP) process. The obtained specimens were post-<span class="hlt">deformed</span> by friction stir processing at room and cryogenic temperature cooling media. The microstructure evolutions during mentioned processes in terms of grain structure, misorientation distribution, and grain orientation spread (GOS) were characterized using electron backscattered diffraction. The annealed sample contained a large number of "recrystallized" grains and relatively large fraction (78%) of high-angle grain boundaries (HAGBs). When CGP process was applied on the annealed specimen, the elongated grains with interior substructure were developed, which was responsible for the formation of 80% low-angle grain boundaries. The GOS map of the severely <span class="hlt">deformed</span> specimen manifested the formation of 43% "distorted" and 51% "substructured" grains. The post <span class="hlt">deformation</span> of severely <span class="hlt">deformed</span> aluminum at room temperature led to the increase in the fraction of HAGBs from 20 to 60%. Also, it gave rise to the formation of "recrystallized" grains with the average size of 13 μm, which were coarser than the grains predicted by Zener-Hollomon parameter. This was attributed to the occurrence of appreciable grain growth during post <span class="hlt">deformation</span>. In the case of post <span class="hlt">deformation</span> at cryogenic temperature cooling medium, the grain size was decreased, which was in well agreement with the predicted grain size. The cumulative distribution of misorientation was the same for both processing routes. Mechanical properties characterizations in terms of nano-indentation and tensile tests revealed that the post <span class="hlt">deformation</span> process led to the reduction in hardness, yield stress, and ultimate tensile strength of the severely <span class="hlt">deformed</span> aluminum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhRvL.113z2503A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhRvL.113z2503A"><span>Nuclear <span class="hlt">Deformation</span> at Finite Temperature</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alhassid, Y.; Gilbreth, C. N.; Bertsch, G. F.</p> <p>2014-12-01</p> <p><span class="hlt">Deformation</span>, a key concept in our understanding of heavy nuclei, is based on a mean-field description that breaks the rotational invariance of the nuclear many-body Hamiltonian. We present a method to analyze nuclear <span class="hlt">deformations</span> at finite temperature in a framework that preserves rotational invariance. The auxiliary-field Monte Carlo method is used to generate a statistical ensemble and calculate the probability distribution associated with the quadrupole operator. Applying the technique to nuclei in the rare-earth region, we identify model-independent signatures of <span class="hlt">deformation</span> and find that <span class="hlt">deformation</span> effects persist to temperatures higher than the spherical-to-<span class="hlt">deformed</span> shape phase-transition temperature of mean-field theory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5450442-radioactive-materials-released-from-nuclear-power-plants','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5450442-radioactive-materials-released-from-nuclear-power-plants"><span>Radioactive materials <span class="hlt">released</span> from nuclear power plants</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Tichler, J.; Benkovitz, C.</p> <p></p> <p><span class="hlt">Releases</span> of radioactive materials in airborne and liquid effluents from commercial light water reactors during 1979 have been compiled and reported. Data on solid waste shipments as well as selected operating information have been included. This report supplements earlier annual reports issued by the former Atomic <span class="hlt">Energy</span> Commission and the Nuclear Regulatory Commission. The 1979 <span class="hlt">release</span> data are compared with previous year's <span class="hlt">releases</span> in tabular form. Data covering specific radionuclides are summarized.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27455513','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27455513"><span>Effects of levomilnacipran extended-<span class="hlt">release</span> on motivation/<span class="hlt">energy</span> and functioning in adults with major depressive disorder.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Thase, Michael E; Gommoll, Carl; Chen, Changzheng; Kramer, Kenneth; Sambunaris, Angelo</p> <p>2016-11-01</p> <p>The objective of this post-hoc analysis was to investigate the relationship between motivation/<span class="hlt">energy</span> and functional impairment in patients with major depressive disorder (MDD). Data were taken from a phase 3 trial of levomilnacipran extended-<span class="hlt">release</span> (ER) in adults with MDD (NCT01034462; N=429) that used the 18-item Motivation and <span class="hlt">Energy</span> Inventory (MEI) to assess motivation/<span class="hlt">energy</span>. Two subgroups with lower and higher motivation/<span class="hlt">energy</span> were defined using baseline MEI total scores (≤28 and >28, respectively). Change from baseline in the Sheehan Disability Scale (SDS) total score was analyzed in the intent-to-treat (ITT) population and both subgroups. Path analyses were carried out in the ITT population and a lower MEI subgroup to assess the direct and indirect effects of levomilnacipran ER on SDS total score change. In the ITT population and the lower MEI subgroup, significant differences were found between levomilnacipran ER and placebo for changes in the SDS total score (-2.6 and -3.9, both P<0.01), but not in the higher MEI subgroup. The indirect effect of levomilnacipran ER on SDS total score improvement, as mediated by MEI total score change, was 79.9% in the lower MEI subgroup and 67.2% in the ITT population. Levomilnacipran ER was previously shown to improve motivation/<span class="hlt">energy</span> in adults with MDD. The current analysis indicates that improvements in functional impairment were considerably mediated by improvements in motivation/<span class="hlt">energy</span>, particularly in patients with lower motivation/<span class="hlt">energy</span> at baseline.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvC..96c4313J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvC..96c4313J"><span>Generalized seniority on a <span class="hlt">deformed</span> single-particle basis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jia, L. Y.</p> <p>2017-09-01</p> <p>Recently, I proposed a fast computing scheme for generalized seniority on a spherical single-particle basis [J. Phys. G: Nucl. Part. Phys. 42, 115105 (2015), 10.1088/0954-3899/42/11/115105]. This work redesigns the scheme to make it applicable to <span class="hlt">deformed</span> single-particle basis. The algorithm is applied to the rare-earth-metal nucleus 94 64 158Gd for intrinsic (body-fixed frame) neutron excitations under the low-momentum NN interaction Vlow -k. By allowing as many as four broken pairs, I compute the lowest 300 intrinsic states of several multipolarities. These states converge well to the exact ones, showing generalized seniority is very effective in truncating the <span class="hlt">deformed</span> shell model. Under realistic interactions, the picture remains approximately valid: The ground state is a coherent pair condensate and the pairs gradually break up as excitation <span class="hlt">energy</span> increases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1263864-situ-tube-burst-testing-high-temperature-deformation-behavior-candidate-materials-accident-tolerant-fuel-cladding','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1263864-situ-tube-burst-testing-high-temperature-deformation-behavior-candidate-materials-accident-tolerant-fuel-cladding"><span>In-situ tube burst testing and high-temperature <span class="hlt">deformation</span> behavior of candidate materials for accident tolerant fuel cladding</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Byun, Thak Sang; Yamamoto, Yukinori; Maloy, Stuart A.; ...</p> <p>2015-08-25</p> <p>Here, one of the most essential properties of accident tolerant fuel (ATF) for maintaining structural integrity during a loss-of-coolant accident (LOCA) is high resistance of the cladding to plastic <span class="hlt">deformation</span> and burst failure, since the <span class="hlt">deformation</span> and burst behavior governs the cooling efficiency of flow channels and the process of fission product <span class="hlt">release</span>. To simulate and evaluate the <span class="hlt">deformation</span> and burst process of thin-walled cladding, an in-situ testing and evaluation method has been developed on the basis of visual imaging and image analysis techniques. The method uses a specialized optics system consisting of a high-resolution video camera, a light filteringmore » unit, and monochromatic light sources. The in-situ testing is performed using a 50 mm long pressurized thin-walled tubular specimen set in a programmable furnace. As the first application, ten (10) candidate cladding materials for ATF, i.e., five FeCrAl alloys and five nanostructured steels, were tested using the newly developed method, and the time-dependent images were analyzed to produce detailed <span class="hlt">deformation</span> and burst data such as true hoop stress, strain (creep) rate, and failure stress. Relatively soft FeCrAl alloys <span class="hlt">deformed</span> and burst below 800 °C, while negligible strain rates were measured for higher strength alloys.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70145550','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70145550"><span>Two stages of <span class="hlt">deformation</span> and fluid migration in the central Brooks Range fold-and-thrust belt</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Moore, Thomas E.; Potter, Christopher J.; O'Sullivan, Paul B.; Shelton, Kevin L.; Underwood, Michael B.</p> <p>2004-01-01</p> <p>We conclude that hydrocarbon generation from Triassic and Jurassic source strata and migration into stratigraphic traps occurred primarily by sedimentary burial principally at 100-90 Ma, between the times of the two major episodes of <span class="hlt">deformation</span>. Subsequent sedimentary burial caused deep stratigraphic traps to become overmature, cracking oil to gas, and initiated some new hydrocarbon generation progressively higher in the section. Structural disruption of the traps in the early Tertiary <span class="hlt">released</span> sequestered hydrocarbons. The hydrocarbons remigrated into newly formed structural traps, which formed at higher structural levels or were lost to the surface. Because of the generally high maturation of the Colville basin at the time of the <span class="hlt">deformation</span> and remigration, most of the hydrocarbons available to fill traps were gas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://care.american-rhinologic.org/cosmetic_functional_nasal_deformities','NIH-MEDLINEPLUS'); return false;" href="http://care.american-rhinologic.org/cosmetic_functional_nasal_deformities"><span>Cosmetic and Functional Nasal <span class="hlt">Deformities</span></span></a></p> <p><a target="_blank" href="http://medlineplus.gov/">MedlinePlus</a></p> <p></p> <p></p> <p>... nasal complaints. Nasal <span class="hlt">deformity</span> can be categorized as “cosmetic” or “functional.” Cosmetic <span class="hlt">deformity</span> of the nose results in a less ... taste , nose bleeds and/or recurrent sinusitis . A cosmetic or functional nasal <span class="hlt">deformity</span> may occur secondary to ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JAP...109g4304Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JAP...109g4304Z"><span>Mechanical <span class="hlt">deformation</span> of carbon nanotube nano-rings on flat substrate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zheng, Meng; Ke, Changhong</p> <p>2011-04-01</p> <p>We present a numerical analysis of the mechanical <span class="hlt">deformation</span> of carbon nanotube (CNT) nano-rings on flat graphite substrates, which is motivated by our recent experimental findings on the elastic <span class="hlt">deformation</span> of CNT nano-rings. Our analysis considers a perfectly circular CNT ring formed by bending a straight individual or bundled single-walled nanotube to connect its two ends. The seamless CNT ring is placed vertically on a flat graphite substrate and its respective <span class="hlt">deformation</span> curvatures under zero external force, compressive, and tensile forces are determined using a continuum model based on nonlinear elastica theory. Our results show that the van der Waals interaction between the CNT ring and the substrate has profound effects on the <span class="hlt">deformation</span> of the CNT ring, and that the interfacial binding interaction between the CNT ring and the substrate is strongly modulated by the ring <span class="hlt">deformation</span>. Our results demonstrate that the CNT ring in force-free conditions has a flat ring segment in contact with the substrate if the ring radius R ≥√EI/2Wvdw , in which EI is the flexural rigidity of the nanotube and Wvdw is the per-unit-length van der Waals <span class="hlt">energy</span> between the flat ring segment and the substrate. Our results reveal that the load-<span class="hlt">deformation</span> profiles of the CNT ring under tensile loadings exhibit bifurcation behavior, which is ascribed to its van der Waals interaction with the substrate and is dependent on its relaxed conformation on the substrate. Our work suggests that CNT nano-rings are promising for a number of applications, such as ultrasensitive force sensors and stretchable and flexible structural components in nanoscale mechanical and electromechanical systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830009328','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830009328"><span>Strain <span class="hlt">energy</span> <span class="hlt">release</span> rate analysis of cyclic delamination growth in compressively loaded laminates</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Whitcomb, J. D.</p> <p>1983-01-01</p> <p>Delamination growth in compressively loaded composite laminates was studied analytically and experimentally. The configuration used was a laminate with an across-the-width delamination. An approximate super-position stress analysis was developed to quantify the effects of various geometric, material, and load parameters on mode 2 and mode 2 strain <span class="hlt">energy</span> <span class="hlt">release</span> rates G sub/1 and G sub 2, respectively. Calculated values of G sub 1 and G sub 2 were then compared with measured cyclic delamination growth rates to determine the relative importance of G sub 1 and G sub 2. High growth rates were observed only when G sub 1 was large. However, slow growth was observed even when G sub 1 was negligibly small. This growth apparently was due to a large value of G sub 2.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24841759','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24841759"><span>Investigation of an outbreak of craniofacial <span class="hlt">deformity</span> in yellow-eyed penguin (Megadyptes antipodes) chicks.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Buckle, K N; Young, M J; Alley, M R</p> <p>2014-09-01</p> <p>To investigate an outbreak of severe craniofacial <span class="hlt">deformity</span> in yellow-eyed penguin (Megadyptes antipodes, hōiho) chicks at a single breeding site on the Otago Peninsula in the South Island of New Zealand. Morbidity and mortality of yellow-eyed penguins breeding on the coastal regions of Otago was monitored from November 2008 to March 2009. Dead chicks and unhatched eggs were recovered and examined. Between October and December 2008 32 eggs were recorded at 17 nests in the Okia Reserve. Eleven chicks survived to about 90 days of age, of which eight were found to have moderate to severe craniofacial <span class="hlt">deformity</span>. The six most severe chicks were subject to euthanasia and examined in detail at necropsy, and the remaining two affected chicks were <span class="hlt">released</span> to the wild after a period of care in a rehabilitation centre. Post-mortem samples were analysed for inorganic and organic toxins. The six <span class="hlt">deformed</span> chicks all had severe shortening of the mandible and maxilla by 20-50 mm. The rostral and caudal regions of the skull were approximately 40 and 80% of normal length, respectively. Other, more variable lesions included cross bill <span class="hlt">deformity</span>, malformed bill keratin, microphthalmia with misshapen scleral ossicles and oral soft tissue excess thought to be secondary to bony malformations. During the same year, mild sporadic bill <span class="hlt">deformities</span> were also reported in 10 unrelated chicks from >167 chicks at other breeding sites on the southern Otago coast. Concentrations of organic toxins and heavy metals in body tissues from affected chicks were apparently similar to those in unaffected chicks on other beaches. No cause of this outbreak of craniofacial <span class="hlt">deformity</span> could be established although the high prevalence at a single site suggests that it was due to an unidentified local teratogen.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.T21A0538W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.T21A0538W"><span>Fault Mechanics and Post-seismic <span class="hlt">Deformation</span> at Bam, SE Iran</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wimpenny, S. E.; Copley, A.</p> <p>2017-12-01</p> <p>The extent to which aseismic <span class="hlt">deformation</span> relaxes co-seismic stress changes on a fault zone is fundamental to assessing the future seismic hazard following any earthquake, and in understanding the mechanical behaviour of faults. We used models of stress-driven afterslip and visco-elastic relaxation, in conjunction with a dense time series of post-seismic InSAR measurements, to show that there has been minimal <span class="hlt">release</span> of co-seismic stress changes through post-seismic <span class="hlt">deformation</span> following the 2003 Mw 6.6 Bam earthquake. Our modelling indicates that the faults at Bam may remain predominantly locked, and that the co- plus inter-seismically accumulated elastic strain stored down-dip of the 2003 rupture patch may be <span class="hlt">released</span> in a future Mw 6 earthquake. Modelling also suggests parts of the fault that experienced post-seismic creep between 2003-2009 overlapped with areas that also slipped co-seismically. Our observations and models also provide an opportunity to probe how aseismic fault slip leads to the growth of topography at Bam. We find that, for our modelled afterslip distribution to be consistent with forming the sharp step in the local topography at Bam over repeated earthquake cycles, and also to be consistent with the geodetic observations, requires either (1) far-field tectonic loading equivalent to a 2-10 MPa deviatoric stress acting across the fault system, which suggests it supports stresses 60-100 times less than classical views of static fault strength, or (2) that the fault surface has some form of mechanical anisotropy, potentially related to corrugations on the fault plane, that controls the sense of slip.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JMPSo..61.1784D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JMPSo..61.1784D"><span>A nonaffine network model for elastomers undergoing finite <span class="hlt">deformations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davidson, Jacob D.; Goulbourne, N. C.</p> <p>2013-08-01</p> <p>In this work, we construct a new physics-based model of rubber elasticity to capture the strain softening, strain hardening, and <span class="hlt">deformation</span>-state dependent response of rubber materials undergoing finite <span class="hlt">deformations</span>. This model is unique in its ability to capture large-stretch mechanical behavior with parameters that are connected to the polymer chemistry and can also be easily identified with the important characteristics of the macroscopic stress-stretch response. The microscopic picture consists of two components: a crosslinked network of Langevin chains and an entangled network with chains confined to a nonaffine tube. These represent, respectively, changes in entropy due to thermally averaged chain conformations and changes in entropy due to the magnitude of these conformational fluctuations. A simple analytical form for the strain <span class="hlt">energy</span> density is obtained using Rubinstein and Panyukov's single-chain description of network behavior. The model only depends on three parameters that together define the initial modulus, extent of strain softening, and the onset of strain hardening. Fits to large stretch data for natural rubber, silicone rubber, VHB 4905 (polyacrylate rubber), and b186 rubber (a carbon black-filled rubber) are presented, and a comparison is made with other similar constitutive models of large-stretch rubber elasticity. We demonstrate that the proposed model provides a complete description of elastomers undergoing large <span class="hlt">deformations</span> for different applied loading configurations. Moreover, since the strain <span class="hlt">energy</span> is obtained using a clear set of physical assumptions, this model may be tested and used to interpret the results of computer simulation and experiments on polymers of known microscopic structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015GeoJI.201..856E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015GeoJI.201..856E"><span>Geodetic slip solutions for the Mw = 7.4 Champerico (Guatemala) earthquake of 2012 November 7 and its postseismic <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ellis, Andria P.; DeMets, Charles; Briole, Pierre; Molina, Enrique; Flores, Omar; Rivera, Jeffrey; Lasserre, Cécile; Lyon-Caen, Hélène; Lord, Neal</p> <p>2015-05-01</p> <p>As the first large subduction thrust earthquake off the coast of western Guatemala in the past several decades, the 2012 November 7 Mw = 7.4 earthquake offers the first opportunity to study coseismic and postseismic behaviour along a segment of the Middle America trench where frictional coupling makes a transition from weak coupling off the coast of El Salvador to strong coupling in southern Mexico. We use measurements at 19 continuous GPS sites in Guatemala, El Salvador and Mexico to estimate the coseismic slip and postseismic <span class="hlt">deformation</span> of the November 2012 Champerico (Guatemala) earthquake. An inversion of the coseismic offsets, which range up to ˜47 mm at the surface near the epicentre, indicates that up to ˜2 m of coseismic slip occurred on a ˜30 × 30 km rupture area between ˜10 and 30 km depth, which is near the global CMT centroid. The geodetic moment of 13 × 1019 N m and corresponding magnitude of 7.4 both agree well with independent seismological estimates. Transient postseismic <span class="hlt">deformation</span> that was recorded at 11 GPS sites is attributable to a combination of fault afterslip and viscoelastic flow in the lower crust and/or mantle. Modelling of the viscoelastic <span class="hlt">deformation</span> suggests that it constituted no more than ˜30 per cent of the short-term postseismic <span class="hlt">deformation</span>. GPS observations that extend six months after the earthquake are well fit by a model in which most afterslip occurred at the same depth or directly downdip from the rupture zone and <span class="hlt">released</span> <span class="hlt">energy</span> equivalent to no more than ˜20 per cent of the coseismic moment. An independent seismological slip solution that features more highly concentrated coseismic slip than our own fits the GPS offsets well if its slip centroid is translated ˜50 km to the west to a position close to our slip centroid. The geodetic and seismologic slip solutions thus suggest bounds of 2-7 m for the peak slip along a region of the interface no larger than 30 × 30 km.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003GeoJI.152...94K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003GeoJI.152...94K"><span>Maximum earthquake magnitudes in the Aegean area constrained by tectonic moment <span class="hlt">release</span> rates</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ch. Koravos, G.; Main, I. G.; Tsapanos, T. M.; Musson, R. M. W.</p> <p>2003-01-01</p> <p>Seismic moment <span class="hlt">release</span> is usually dominated by the largest but rarest events, making the estimation of seismic hazard inherently uncertain. This uncertainty can be reduced by combining long-term tectonic <span class="hlt">deformation</span> rates with short-term recurrence rates. Here we adopt this strategy to estimate recurrence rates and maximum magnitudes for tectonic zones in the Aegean area. We first form a merged catalogue for historical and instrumentally recorded earthquakes in the Aegean, based on a recently published catalogue for Greece and surrounding areas covering the time period 550BC-2000AD, at varying degrees of completeness. The historical data are recalibrated to allow for changes in damping in seismic instruments around 1911. We divide the area up into zones that correspond to recent determinations of <span class="hlt">deformation</span> rate from satellite data. In all zones we find that the Gutenberg-Richter (GR) law holds at low magnitudes. We use Akaike's information criterion to determine the best-fitting distribution at high magnitudes, and classify the resulting frequency-magnitude distributions of the zones as critical (GR law), subcritical (gamma density distribution) or supercritical (`characteristic' earthquake model) where appropriate. We determine the ratio η of seismic to tectonic moment <span class="hlt">release</span> rate. Low values of η (<0.5) corresponding to relatively aseismic <span class="hlt">deformation</span>, are associated with higher b values (>1.0). The seismic and tectonic moment <span class="hlt">release</span> rates are then combined to constrain recurrence rates and maximum credible magnitudes (in the range 6.7-7.6 mW where the results are well constrained) based on extrapolating the short-term seismic data. With current earthquake data, many of the tectonic zones show a characteristic distribution that leads to an elevated probability of magnitudes around 7, but a reduced probability of larger magnitudes above this value when compared with the GR trend. A modification of the generalized gamma distribution is suggested to account</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000Natur.408..998L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000Natur.408..998L"><span>Controlled growth factor <span class="hlt">release</span> from synthetic extracellular matrices</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Kuen Yong; Peters, Martin C.; Anderson, Kenneth W.; Mooney, David J.</p> <p>2000-12-01</p> <p>Polymeric matrices can be used to grow new tissues and organs, and the delivery of growth factors from these matrices is one method to regenerate tissues. A problem with engineering tissues that exist in a mechanically dynamic environment, such as bone, muscle and blood vessels, is that most drug delivery systems have been designed to operate under static conditions. We thought that polymeric matrices, which <span class="hlt">release</span> growth factors in response to mechanical signals, might provide a new approach to guide tissue formation in mechanically stressed environments. Critical design features for this type of system include the ability to undergo repeated <span class="hlt">deformation</span>, and a reversible binding of the protein growth factors to polymeric matrices to allow for responses to repeated stimuli. Here we report a model delivery system that can respond to mechanical signalling and upregulate the <span class="hlt">release</span> of a growth factor to promote blood vessel formation. This approach may find a number of applications, including regeneration and engineering of new tissues and more general drug-delivery applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21685963','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21685963"><span>Actively mode-locked fiber laser using a <span class="hlt">deformable</span> micromirror.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fabert, Marc; Kermène, Vincent; Desfarges-Berthelemot, Agnès; Blondy, Pierre; Crunteanu, Aurelian</p> <p>2011-06-15</p> <p>We present what we believe to be the first fiber laser system that is actively mode-locked by a <span class="hlt">deformable</span> micromirror. The micromirror device is placed within the laser cavity and performs a dual function of modulator and end-cavity mirror. The mode-locked laser provides ~1-ns-long pulses with 20 nJ/pulse <span class="hlt">energy</span> at 5 MHz repetition rates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EPJWC..9404046C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EPJWC..9404046C"><span><span class="hlt">Deformation</span> of compound shells under action of internal shock wave loading</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chernobryvko, Marina; Kruszka, Leopold; Avramov, Konstantin</p> <p>2015-09-01</p> <p>The compound shells under the action of internal shock wave loading are considered. The compound shell consists of a thin cylindrical shell and two thin parabolic shells at the edges. The boundary conditions in the shells joints satisfy the equality of displacements. The internal shock wave loading is modelled as the surplus pressure surface. This pressure is a function of the shell coordinates and time. The strain rate <span class="hlt">deformation</span> of compound shell takes place in both the elastic and in plastic stages. In the elastic stage the equations of the structure motions are obtained by the assumed-modes method, which uses the kinetic and potential <span class="hlt">energies</span> of the cylindrical and two parabolic shells. The dynamic behaviour of compound shells is treated. In local plastic zones the 3-D thermo-elastic-plastic model is used. The <span class="hlt">deformations</span> are described by nonlinear model. The stress tensor elements are determined using dynamic <span class="hlt">deformation</span> theory. The <span class="hlt">deformation</span> properties of materials are influenced by the strain rate behaviour, the influence of temperature parameters, and the elastic-plastic properties of materials. The dynamic yield point of materials and Pisarenko-Lebedev's criterion of destruction are used. The modified adaptive finite differences method of numerical analysis is suggested for those simulations. The accuracy of the numerical simulation is verified on each temporal step of calculation and in the case of large <span class="hlt">deformation</span> gradients.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AIPC.1959d0008E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AIPC.1959d0008E"><span><span class="hlt">Energy</span> <span class="hlt">release</span> estimation for fragmenting meteoroid</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Egorova, L. A.; Lokhin, V. V.</p> <p>2018-05-01</p> <p>It is known that for the adequate interpretation of fireball observations it is necessary to take into account its fragmentation in the Earth's atmosphere. Various models for large cosmic body destruction in the atmosphere are known. Presented work continues our previous research on the fragmentation of fireballs. Proposing a model for the destruction of a fireball we also submit a model for the transition of its kinetic <span class="hlt">energy</span> to thermal one. The meteoroid destruction under consideration is similar to the destruction of a solid body during an explosion. The kinetic <span class="hlt">energy</span> of the moving particles of the crashing meteoric body transform into the thermal <span class="hlt">energy</span> of the gas volume in which their motion occurs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997APS..MAR.O1706P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997APS..MAR.O1706P"><span><span class="hlt">Energy</span> and Momentum Relaxation Times of 2D Electrons Due to Near Surface <span class="hlt">Deformation</span> Potential Scattering</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pipa, Viktor; Vasko, Fedor; Mitin, Vladimir</p> <p>1997-03-01</p> <p>The low temperature <span class="hlt">energy</span> and momentum relaxation rates of 2D electron gas placed near the free or clamped surface of a semi-infinit sample are calculated. To describe the electron-acoustic phonon interaction with allowance of the surface effect the method of elasticity theory Green functions was used. This method allows to take into account the reflection of acoustic waves from the surface and related mutual conversion of LA and TA waves. It is shown that the strength of the <span class="hlt">deformation</span> potential scattering at low temperatures substantially depends on the mechanical conditions at the surface: relaxation rates are suppressed for the free surface while for the rigid one the rates are enhanced. The dependence of the conductivity on the distance between the 2D layer and the surface is discussed. The effect is most pronounced in the range of temperatures 2 sl pF < T < (2 hbar s_l)/d, where pF is the Fermi momentum, sl is the velocity of LA waves, d is the width of the quantum well.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NuPhA.972...86J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NuPhA.972...86J"><span>Study of phase transition of even and odd nuclei based on q-<span class="hlt">deforme</span> SU(1,1) algebraic model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jafarizadeh, M. A.; Amiri, N.; Fouladi, N.; Ghapanvari, M.; Ranjbar, Z.</p> <p>2018-04-01</p> <p>The q-<span class="hlt">deformed</span> Hamiltonian for the SO (6) ↔ U (5) transitional case in s, d interaction boson model (IBM) can be constructed by using affine SUq (1 , 1) Lie algebra in the both IBM-1 and 2 versions and IBFM. In this research paper, we have studied the <span class="hlt">energy</span> spectra of 120-128Xe isotopes and 123-131Xe isotopes and B(E2) transition probabilities of 120-128Xe isotopes in the shape phase transition region between the spherical and gamma unstable <span class="hlt">deformed</span> shapes of the theory of quantum <span class="hlt">deformation</span>. The theoretical results agree with the experimental data fairly well. It is shown that the q-<span class="hlt">deformed</span> SO (6) ↔ U (5) transitional dynamical symmetry remains after <span class="hlt">deformation</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.nrel.gov/news/program/2018/new-open-source-version-of-floris-released.html','SCIGOVWS'); return false;" href="https://www.nrel.gov/news/program/2018/new-open-source-version-of-floris-released.html"><span>New Open-Source Version of FLORIS <span class="hlt">Released</span> | News | NREL</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p>New <em>Open</em>-Source Version of FLORIS <span class="hlt">Released</span> New <em>Open</em>-Source Version of FLORIS <span class="hlt">Released</span> January 26 , 2018 National Renewable <span class="hlt">Energy</span> Laboratory (NREL) researchers recently <span class="hlt">released</span> an updated <em>open</em>-source simplified and documented. Because of the living, <em>open</em>-source nature of the newly updated utility, NREL</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.4495P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.4495P"><span>A fundamental discussion of what triggers localized <span class="hlt">deformation</span> in geological materials</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peters, Max; Paesold, Martin; Poulet, Thomas; Herwegh, Marco; Regenauer-Lieb, Klaus; Veveakis, Manolis</p> <p>2015-04-01</p> <p> critical amount of dissipative work translated into heat over the diffusive capacity of the system by an instability study designed for such materials (Gruntfest, 1963). With respect to our numerical experiments, this critical parameter determines the timing when the entire amount of <span class="hlt">deformation</span> <span class="hlt">energy</span> translated into heat cannot be diffusively transported out of the system anymore. The resulting local temperature rise then induces strain localization. In contrast to classical shear heating scenarios with (catastrophic) thermal runaways, temperature variations of less than 1 K are sufficient for this localization mode to occur due to the balance between heat producing (e.g. dislocation creep) and consuming (grain growth) processes in the present setup. We demonstrate that this rise in latent heat is sufficient to provoke grain growth, operating as an endothermic reaction, stabilizing the simulated localized structure in turn. Various localized ductile structures, such as folded or boudinaged layers, can therefore be placed at the same material failure mode due to fundamental <span class="hlt">energy</span> bifurcations triggered by dissipative work out of homogeneous state. Finally, we will discuss situations, in which structural heterogeneities are considered negligible and where the <span class="hlt">energy</span> theory described here plays an underlying role by means of a comparison between numerical experiments and natural examples. REFERENCES Austin, N. and Evans, B. (2007). Paleowattmeters: A scaling relation for dynamically recrystallized grain size. Geology, 35. Gruntfest, I.J. (1963). Thermal feedback in liquid flow, plane shear at constant stress. Transactions of the Society of Rheology, 7. Hansen, L.N. and Zimmermann, M.E. and Dillman, A.M. and Kohlstedt, D.L (2012). Strain localization in olivine aggregates at high temperature: a laboratory comparison of constant-strain-rate and constant-stress boundary conditions. Earth and Planetary Science Letters, 333-334. Herwegh, M., Poulet, T., Karrech, A. and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1215314H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1215314H"><span>Experimental <span class="hlt">Deformation</span> of Dehydrating Antigorite: Challenging Models of Dehydration Embrittlement</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hirth, Greg; Chernak, Linda</p> <p>2010-05-01</p> <p>C, 1.5 GPa and a strain rate of 10-5 s-1. This sample had a strength of 300 MPa, which is significantly higher than samples <span class="hlt">deformed</span> at the same conditions without olivine present; strengths were approximately 100 MPa for these samples. We hypothesize that the highly porous and permeable olivine layer provided a reservoir for the water <span class="hlt">released</span> by the dehydration reaction and suggests that the presence of water causes the strength of antigorite to decrease.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/2090822','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/2090822"><span><span class="hlt">Deformation</span> of crowns during cementation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wilson, P R; Goodkind, R J; Delong, R; Sakaguchi, R</p> <p>1990-11-01</p> <p><span class="hlt">Deformation</span> of crowns during cementation was investigated by a simple loading system of defined crowns with silicone fluids as cements. <span class="hlt">Deformation</span> of the crowns was measured by long stain gauges that encircled the cervical margins. Die spacing was simulated by etching the die. Venting was simulated by removing a small screw. <span class="hlt">Deformation</span> of the crowns was decreased by decreasing the viscosity of fluid, increasing the thickness of the crowns, and venting. Etching the die decreased the seating times of the crowns, but did not alter the level of <span class="hlt">deformation</span>. Terminal cementation with zinc phosphate cement confirmed the presence of crown <span class="hlt">deformation</span> during cementation. The results have consequences for bonded and all-ceramic crowns, and explain several clinical phenomena. It is suggested that low viscosity cements, low seating forces, and die spacing be used to decrease the <span class="hlt">deformation</span> of crowns during seating. The importance of passive fitting of the crown to the tooth is stressed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9056E..1FF','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9056E..1FF"><span>Loading system mechanism for dielectric elastomer generators with equi-biaxial state of <span class="hlt">deformation</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fontana, M.; Moretti, G.; Lenzo, B.; Vertechy, R.</p> <p>2014-03-01</p> <p>Dielectric Elastomer Generators (DEGs) are devices that employ a cyclically variable membrane capacitor to produce electricity from oscillating sources of mechanical <span class="hlt">energy</span>. Capacitance variation is obtained thanks to the use of dielectric and conductive layers that can undergo different states of <span class="hlt">deformation</span> including: uniform or non-uniform and uni- or multi-axial stretching. Among them, uniform equi-biaxial stretching is reputed as being the most effective state of <span class="hlt">deformation</span> that maximizes the amount of <span class="hlt">energy</span> that can be extracted in a cycle by a unit volume of Dielectric Elastomer (DE) material. This paper presents a DEG concept, with linear input motion and tunable impedance, that is based on a mechanical loading system for inducing uniform equi-biaxial states of <span class="hlt">deformation</span>. The presented system employs two circular DE membrane capacitors that are arranged in an agonist-antagonist configuration. An analytical model of the overall system is developed and used to find the optimal design parameters that make it possible to tune the elastic response of the generator over the range of motion of interest. An apparatus is developed for the equi-biaxial testing of DE membranes and used for the experimental verification of the employed numerical models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014cosp...40E3437U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014cosp...40E3437U"><span>The statistical analysis of <span class="hlt">energy</span> <span class="hlt">release</span> in small-scale coronal structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ulyanov, Artyom; Kuzin, Sergey; Bogachev, Sergey</p> <p></p> <p>We present the results of statistical analysis of impulsive flare-like brightenings, which numerously occur in the quiet regions of solar corona. For our study, we utilized high-cadence observations performed with two EUV-telescopes - TESIS/Coronas-Photon and AIA/SDO. In total, we processed 6 sequences of images, registered throughout the period between 2009 and 2013, covering the rising phase of the 24th solar cycle. Based on high-speed DEM estimation method, we developed a new technique to evaluate the main parameters of detected events (geometrical sizes, duration, temperature and thermal <span class="hlt">energy</span>). We then obtained the statistical distributions of these parameters and examined their variations depending on the level of solar activity. The results imply that near the minimum of the solar cycle the <span class="hlt">energy</span> <span class="hlt">release</span> in quiet corona is mainly provided by small-scale events (nanoflares), whereas larger events (microflares) prevail on the peak of activity. Furthermore, we investigated the coronal conditions that had specified the formation and triggering of registered flares. By means of photospheric magnetograms obtained with MDI/SoHO and HMI/SDO instruments, we examined the topology of local magnetic fields at different stages: the pre-flare phase, the peak of intensity and the ending phase. To do so, we introduced a number of topological parameters including the total magnetic flux, the distance between magnetic sources and their mutual arrangement. The found correlation between the change of these parameters and the formation of flares may offer an important tool for application of flare forecasting.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018FrMat...5...17V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018FrMat...5...17V"><span>Effect of Length, Diameter, Chirality, <span class="hlt">Deformation</span>, and Strain on Contact Thermal Conductance between Single Wall Carbon Nanotubes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Varshney, Vikas; Lee, Jonghoon; Brown, Joshua S.; Farmer, Barry L.; Voevodin, Andrey A.; Roy, Ajit K.</p> <p>2018-04-01</p> <p>Thermal <span class="hlt">energy</span> transfer across physically interacting single-wall carbon nanotube (SWCNT) interconnects has been investigated using non-equilibrium molecular dynamics simulations. The role of various geometrical and structural (length, diameter, chirality) as well as external (<span class="hlt">deformation</span> and strain) carbon nanotube (CNT) parameters has been explored to estimate total as well as area-normalized thermal conductance across cross-contact interconnects. It is shown that the CNT aspect ratio and degree of lateral as well as tensile <span class="hlt">deformation</span> play a significant role in determining the extent of thermal <span class="hlt">energy</span> exchange across CNT contacts, while CNT chirality has a negligible influence on thermal transport. Depending on the CNT diameter, aspect ratio, and degree of <span class="hlt">deformation</span> at the contact interface, the thermal conductance values can vary significantly –by more than an order of magnitude for total conductance and a factor of 3 to 4 for area-normalized conductance. The observed trends are discussed from the perspective of modulation in number of low frequency out-of-plane (transverse, flexural, and radial) phonons that transmit thermal <span class="hlt">energy</span> across the contact and govern the conductance across the interface. The established general dependencies for phonon governed thermal transport at CNT contacts are anticipated to help design and performance prediction of CNT-based flexible nanoelectronic devices, where CNT-CNT contact <span class="hlt">deformation</span> and strain are routinely encountered during device operations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010SPIE.7626E..1XT','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010SPIE.7626E..1XT"><span>Dealing with difficult <span class="hlt">deformations</span>: construction of a knowledge-based <span class="hlt">deformation</span> atlas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thorup, S. S.; Darvann, T. A.; Hermann, N. V.; Larsen, P.; Ólafsdóttir, H.; Paulsen, R. R.; Kane, A. A.; Govier, D.; Lo, L.-J.; Kreiborg, S.; Larsen, R.</p> <p>2010-03-01</p> <p>Twenty-three Taiwanese infants with unilateral cleft lip and palate (UCLP) were CT-scanned before lip repair at the age of 3 months, and again after lip repair at the age of 12 months. In order to evaluate the surgical result, detailed point correspondence between pre- and post-surgical images was needed. We have previously demonstrated that non-rigid registration using B-splines is able to provide automated determination of point correspondences in populations of infants without cleft lip. However, this type of registration fails when applied to the task of determining the complex <span class="hlt">deformation</span> from before to after lip closure in infants with UCLP. The purpose of the present work was to show that use of prior information about typical <span class="hlt">deformations</span> due to lip closure, through the construction of a knowledge-based atlas of <span class="hlt">deformations</span>, could overcome the problem. Initially, mean volumes (atlases) for the pre- and post-surgical populations, respectively, were automatically constructed by non-rigid registration. An expert placed corresponding landmarks in the cleft area in the two atlases; this provided prior information used to build a knowledge-based <span class="hlt">deformation</span> atlas. We model the change from pre- to post-surgery using thin-plate spline warping. The registration results are convincing and represent a first move towards an automatic registration method for dealing with difficult <span class="hlt">deformations</span> due to this type of surgery.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24374231','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24374231"><span>Foldover-free shape <span class="hlt">deformation</span> for biomedicine.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yu, Hongchuan; Zhang, Jian J; Lee, Tong-Yee</p> <p>2014-04-01</p> <p>Shape <span class="hlt">deformation</span> as a fundamental geometric operation underpins a wide range of applications, from geometric modelling, medical imaging to biomechanics. In medical imaging, for example, to quantify the difference between two corresponding images, 2D or 3D, one needs to find the <span class="hlt">deformation</span> between both images. However, such <span class="hlt">deformations</span>, particularly <span class="hlt">deforming</span> complex volume datasets, are prone to the problem of foldover, i.e. during <span class="hlt">deformation</span>, the required property of one-to-one mapping no longer holds for some points. Despite numerous research efforts, the construction of a mathematically robust foldover-free solution subject to positional constraints remains open. In this paper, we address this challenge by developing a radial basis function-based <span class="hlt">deformation</span> method. In particular we formulate an effective iterative mechanism which ensures the foldover-free property is satisfied all the time. The experimental results suggest that the resulting <span class="hlt">deformations</span> meet the internal positional constraints. In addition to radial basis functions, this iterative mechanism can also be incorporated into other <span class="hlt">deformation</span> approaches, e.g. B-spline based FFDs, to develop different <span class="hlt">deformable</span> approaches for various applications. Crown Copyright © 2013. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JNuM..504...41K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JNuM..504...41K"><span>Understanding thermally activated plastic <span class="hlt">deformation</span> behavior of Zircaloy-4</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kumar, N.; Alomari, A.; Murty, K. L.</p> <p>2018-06-01</p> <p>Understanding micromechanics of plastic <span class="hlt">deformation</span> of existing materials is essential for improving their properties further and/or developing advanced materials for much more severe load bearing applications. The objective of the present work was to understand micromechanics of plastic <span class="hlt">deformation</span> of Zircaloy-4, a zirconium-based alloy used as fuel cladding and channel (in BWRs) material in nuclear reactors. The Zircaloy-4 in recrystallized (at 973 K for 4 h) condition was subjected to uniaxial tensile testing at a constant cross-head velocity at temperatures in the range 293 K-1073 K and repeated stress relaxation tests at 293 K, 573 K, and 773 K. The minimum in the total elongation was indicative of dynamic strain aging phenomenon in this alloy in the intermediate temperature regime. The yield stress of the alloy was separated into effective and athermal components and the transition from thermally activated dislocation glide to athermal regime took place at around 673 K with the athermal stress estimated to be 115 MPa. The activation volume was found to be in the range of 40 b3 to 160 b3. The activation volume values and the data analyses using the solid-solution models in literature indicated dislocation-solute interaction to be a potential <span class="hlt">deformation</span> mechanism in thermally activated regime. The activation <span class="hlt">energy</span> calculated at 573 K was very close to that found for diffusivity of oxygen in α-Zr that was suggestive of dislocations-oxygen interaction during plastic <span class="hlt">deformation</span>. This type of information may be helpful in alloy design in selecting different elements to control the <span class="hlt">deformation</span> behavior of the material and impart desired mechanical properties in those materials for specific applications.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28565910','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28565910"><span>Photochemical <span class="hlt">Energy</span> Storage and Electrochemically Triggered <span class="hlt">Energy</span> <span class="hlt">Release</span> in the Norbornadiene-Quadricyclane System: UV Photochemistry and IR Spectroelectrochemistry in a Combined Experiment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Brummel, Olaf; Waidhas, Fabian; Bauer, Udo; Wu, Yanlin; Bochmann, Sebastian; Steinrück, Hans-Peter; Papp, Christian; Bachmann, Julien; Libuda, Jörg</p> <p>2017-07-06</p> <p>The two valence isomers norbornadiene (NBD) and quadricyclane (QC) enable solar <span class="hlt">energy</span> storage in a single molecule system. We present a new photoelectrochemical infrared reflection absorption spectroscopy (PEC-IRRAS) experiment, which allows monitoring of the complete <span class="hlt">energy</span> storage and <span class="hlt">release</span> cycle by in situ vibrational spectroscopy. Both processes were investigated, the photochemical conversion from NBD to QC using the photosensitizer 4,4'-bis(dimethylamino)benzophenone (Michler's ketone, MK) and the electrochemically triggered cycloreversion from QC to NBD. Photochemical conversion was obtained with characteristic conversion times on the order of 500 ms. All experiments were performed under full potential control in a thin-layer configuration with a Pt(111) working electrode. The vibrational spectra of NBD, QC, and MK were analyzed in the fingerprint region, permitting quantitative analysis of the spectroscopic data. We determined selectivities for both the photochemical conversion and the electrochemical cycloreversion and identified the critical steps that limit the reversibility of the storage cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3140238','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3140238"><span>Management of Congenital Chest Wall <span class="hlt">Deformities</span></span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Blanco, Felix C.; Elliott, Steven T.; Sandler, Anthony D.</p> <p>2011-01-01</p> <p>Congenital chest wall <span class="hlt">deformities</span> are considered to be anomalies in chest wall growth. These can be categorized as either rib cage overgrowth or <span class="hlt">deformities</span> related to inadequate growth (aplasia or dysplasia). Rib cage overgrowth leads to depression of the sternum (pectus excavatum) or protuberance of the sternum (pectus carinatum) and accounts for greater than 90% of congenital chest wall <span class="hlt">deformities</span>. The remaining <span class="hlt">deformities</span> are a result of inadequate growth. Evolution in the management of congenital chest wall <span class="hlt">deformities</span> has made significant progress over the past 25 years. This article will review chest wall <span class="hlt">deformities</span> and the current management strategies of these interesting anomalies. PMID:22294949</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21733437','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21733437"><span>Role of intraoperative varus stress test for lateral soft tissue <span class="hlt">release</span> during chevron bunion procedure.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Hyong-Nyun; Suh, Dong-Hyun; Hwang, Pil-Sung; Yu, Sun-O; Park, Yong-Wook</p> <p>2011-04-01</p> <p>The purpose of this study was to evaluate the clinical results of distal chevron osteotomy performed in conjunction with selective lateral soft tissue <span class="hlt">release</span>. The criterion for doing a lateral soft tissue <span class="hlt">release</span> was assessed by determining the ease and completeness of passive hallux valgus correction at the time of surgery. Between August 2005 and November 2007, 48 feet in 43 patients classified as having mild to moderate hallux valgus were retrospectively studied. Distal chevron osteotomy without lateral soft tissue <span class="hlt">release</span> was performed in 26 cases (Group 1) when passive correction of the hallux valgus <span class="hlt">deformity</span> was possible. Distal chevron osteotomy with lateral soft tissue <span class="hlt">release</span> was performed in 22 cases (Group 2) when passive correction was not possible. Average followup was 23 (range, 12 to 28) months. Clinical results were assessed using radiographic parameters [hallux valgus angle (HVA), first and second intermetatarsal angle (1,2 IMA)], AOFAS scale and patient's subjective satisfaction. For Group 1: the average correction of HVA was 12.8 degrees, the average correction of IMA was 4.7 degrees, and the AOFAS score improved an average of 29.2 points at the last followup. Thirteen patients were very satisfied and ten patients were satisfied with the results. No patient was dissatisfied. For Group 2: the average correction of HVA was 19.1 degrees, the average correction of IMA was 7 degrees and AOFAS score improved at an average of 31.8 points at the last followup. Twelve patients were very satisfied, seven patients were satisfied and one patient, who had stiffness of the first metatarsophalangeal joint, was dissatisfied with the result. Distal chevron osteotomy with selective lateral soft tissue <span class="hlt">release</span> based on the ability to passively correct the hallux valgus <span class="hlt">deformity</span> lead to safe and stable correction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MAR.M1187S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MAR.M1187S"><span>Interfacial Bubble <span class="hlt">Deformations</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Seymour, Brian; Shabane, Parvis; Cypull, Olivia; Cheng, Shengfeng; Feitosa, Klebert</p> <p></p> <p>Soap bubbles floating at an air-water experience <span class="hlt">deformations</span> as a result of surface tension and hydrostatic forces. In this experiment, we investigate the nature of such <span class="hlt">deformations</span> by taking cross-sectional images of bubbles of different volumes. The results show that as their volume increases, bubbles transition from spherical to hemispherical shape. The <span class="hlt">deformation</span> of the interface also changes with bubble volume with the capillary rise converging to the capillary length as volume increases. The profile of the top and bottom of the bubble and the capillary rise are completely determined by the volume and pressure differences. James Madison University Department of Physics and Astronomy, 4VA Consortium, Research Corporation for Advancement of Science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JMPSo.110..137Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JMPSo.110..137Z"><span>A micro-macro constitutive model for finite-<span class="hlt">deformation</span> viscoelasticity of elastomers with nonlinear viscosity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhou, Jianyou; Jiang, Liying; Khayat, Roger E.</p> <p>2018-01-01</p> <p>Elastomers are known to exhibit viscoelastic behavior under <span class="hlt">deformation</span>, which is linked to the diffusion processes of the highly mobile and flexible polymer chains. Inspired by the theories of polymer dynamics, a micro-macro constitutive model is developed to study the viscoelastic behaviors and the relaxation process of elastomeric materials under large <span class="hlt">deformation</span>, in which the material parameters all have a microscopic foundation or a microstructural justification. The proposed model incorporates the nonlinear material viscosity into the continuum finite-<span class="hlt">deformation</span> viscoelasticity theories which represent the polymer networks of elastomers with an elastic ground network and a few viscous subnetworks. The developed modeling framework is capable of adopting most of strain <span class="hlt">energy</span> density functions for hyperelastic materials and thermodynamics evolution laws of viscoelastic solids. The modeling capacity of the framework is outlined by comparing the simulation results with the experimental data of three commonly used elastomeric materials, namely, VHB4910, HNBR50 and carbon black (CB) filled elastomers. The comparison shows that the stress responses and some typical behaviors of filled and unfilled elastomers can be quantitatively predicted by the model with suitable strain <span class="hlt">energy</span> density functions. Particularly, the strain-softening effect of elastomers could be explained by the <span class="hlt">deformation</span>-dependent (nonlinear) viscosity of the polymer chains. The presented modeling framework is expected to be useful as a modeling platform for further study on the performance of different type of elastomeric materials.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.490..151N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.490..151N"><span><span class="hlt">Deformation</span>-induced crystallographic-preferred orientation of hcp-iron: An experimental study using a <span class="hlt">deformation</span>-DIA apparatus</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nishihara, Yu; Ohuchi, Tomohiro; Kawazoe, Takaaki; Seto, Yusuke; Maruyama, Genta; Higo, Yuji; Funakoshi, Ken-ichi; Tange, Yoshinori; Irifune, Tetsuo</p> <p>2018-05-01</p> <p>Shear and uniaxial <span class="hlt">deformation</span> experiments on hexagonal close-packed iron (hcp-Fe) was conducted using a <span class="hlt">deformation</span>-DIA apparatus at a pressure of 13-17 GPa and a temperature of 723 K to determine its <span class="hlt">deformation</span>-induced crystallographic-preferred orientation (CPO). Development of the CPO in the <span class="hlt">deforming</span> sample is determined in-situ based on two-dimensional X-ray diffraction using monochromatic synchrotron X-rays. In the shear <span class="hlt">deformation</span> geometry, the <0001> and < 11 2 bar 0 > axes gradually align to be sub-parallel to the shear plane normal and shear direction, respectively, from the initial random texture. In the uniaxial compression and tensile geometry, the <0001> and < 11 2 bar 0 > axes, respectively, gradually align along the direction of the uniaxial <span class="hlt">deformation</span> axis. These results suggest that basal slip (0001) < 11 2 bar 0 > is the dominant slip system in hcp-Fe under the studied <span class="hlt">deformation</span> conditions. The P-wave anisotropy for a shear <span class="hlt">deformed</span> sample was calculated using elastic constants at the inner core condition by recent ab-initio calculations. Strength of the calculated anisotropy was comparable to or higher than axisymmetric anisotropy in Earth's inner core.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..SHK.B5005A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..SHK.B5005A"><span>Strain-Rate Dependence of <span class="hlt">Deformation</span>-Twinning in Tantalum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abeywardhana, Jayalath; Germann, Tim; Ravelo, Ramon</p> <p>2017-06-01</p> <p>Large-Scale molecular dynamics (MD) simulations are used to model quasi-isentropic compression and expansion (QIC) in tantalum crystals varying the rate of <span class="hlt">deformation</span> between the range 108 -1012s-1 and compressive pressures up to 100 GPa. The atomic interactions were modeled employing an embedded-atom method (EAM) potential of Ta. Isentropic expansion was done employing samples initially compressed to pressures of 60 and 100 GPa followed by uniaxial and quasi-isentropically expansion to zero pressure. The effect of initial dislocation density on twinning was also examined by varying the initial defect density of the Ta samples (1010 -1012cm-2). At these high-strain rates, a threshold in strain-rate on <span class="hlt">deformation</span> twining is observed. Under expansion or compression, <span class="hlt">deformation</span> twinning increases with strain rate for strain-rates >109s-1 . Below this value, small fraction of twins nucleates but anneal out with time. Samples with lower fraction of twins equilibrate to defect states containing higher screw dislocation densities from those with initially higher twinning fractions. This work was supported by the Department of <span class="hlt">Energy</span> under contract DE-AC52-06NA25396 and by the Air Force Office of Scientific Research under AFOSR Award No. FA9550-12-1-0476.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000PCM....27..480D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000PCM....27..480D"><span>Evidence for stable grain boundary melt films in experimentally <span class="hlt">deformed</span> olivine-orthopyroxene rocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Kloe, R.; Drury, M. R.; van Roermund, H. L. M.</p> <p></p> <p>The microstructure of olivine-olivine grain boundaries has been studied in experimentally <span class="hlt">deformed</span> (1200-1227°C, 300MPa) partially molten olivine and olivine-orthopyroxene rocks. In-situ melting produced 1vol% melt in all samples studied. Grain boundary analyses were carried out using a number of transmission electron microscopy techniques. The grain boundary chemistry in undeformed olivine-orthopyroxene starting material showed evidence for the presence of an intergranular phase along some, but not all, of the olivine-olivine boundaries. In the <span class="hlt">deformed</span> samples, ultrathin Si-rich, Al- and Ca-bearing amorphous films have been observed along all investigated olivine-olivine grain boundaries. The chemistry of the grain boundaries, which is considered to be indicative for the presence of a thin film, was measured with <span class="hlt">energy</span>-dispersive X-ray spectroscopy (EDX) and <span class="hlt">energy</span>-filtering imaging. The amorphous nature of the films was confirmed with diffuse dark field imaging, Fresnel fringe imaging, and high-resolution electron microscopy. The films range in thickness from 0.6 to 3.0nm, and EDX analyses show that the presence of Al and Ca is restricted to this ultrathin film along the grain boundaries. Because thin melt films have been observed in all the samples, they are thought to be stable features of the melt microstructure in <span class="hlt">deformed</span> partially molten rocks. The transition from the occasional presence of films in the undeformed starting material to the general occurrence of the films in <span class="hlt">deformed</span> materials suggests that <span class="hlt">deformation</span> promotes the formation and distribution of the films. Alternatively, hot-pressing may be too short for films to develop along all grain boundaries. A difference in creep strength between the studied samples could not be attributed to grain boundary melt films, as these have been found in all <span class="hlt">deformed</span> samples. However, a weakening effect of grain boundary melt films on olivine rheology could not be ruled out due to the lack of confirmed melt</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5049949','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5049949"><span>Effects of levomilnacipran extended-<span class="hlt">release</span> on motivation/<span class="hlt">energy</span> and functioning in adults with major depressive disorder</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gommoll, Carl; Chen, Changzheng; Kramer, Kenneth; Sambunaris, Angelo</p> <p>2016-01-01</p> <p>The objective of this post-hoc analysis was to investigate the relationship between motivation/<span class="hlt">energy</span> and functional impairment in patients with major depressive disorder (MDD). Data were taken from a phase 3 trial of levomilnacipran extended-<span class="hlt">release</span> (ER) in adults with MDD (NCT01034462; N=429) that used the 18-item Motivation and <span class="hlt">Energy</span> Inventory (MEI) to assess motivation/<span class="hlt">energy</span>. Two subgroups with lower and higher motivation/<span class="hlt">energy</span> were defined using baseline MEI total scores (≤28 and >28, respectively). Change from baseline in the Sheehan Disability Scale (SDS) total score was analyzed in the intent-to-treat (ITT) population and both subgroups. Path analyses were carried out in the ITT population and a lower MEI subgroup to assess the direct and indirect effects of levomilnacipran ER on SDS total score change. In the ITT population and the lower MEI subgroup, significant differences were found between levomilnacipran ER and placebo for changes in the SDS total score (−2.6 and −3.9, both P<0.01), but not in the higher MEI subgroup. The indirect effect of levomilnacipran ER on SDS total score improvement, as mediated by MEI total score change, was 79.9% in the lower MEI subgroup and 67.2% in the ITT population. Levomilnacipran ER was previously shown to improve motivation/<span class="hlt">energy</span> in adults with MDD. The current analysis indicates that improvements in functional impairment were considerably mediated by improvements in motivation/<span class="hlt">energy</span>, particularly in patients with lower motivation/<span class="hlt">energy</span> at baseline. PMID:27455513</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhA...50O5401S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhA...50O5401S"><span>Homogeneous Yang-Baxter <span class="hlt">deformations</span> as generalized diffeomorphisms</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sakamoto, Jun-ichi; Sakatani, Yuho; Yoshida, Kentaroh</p> <p>2017-10-01</p> <p>Yang-Baxter (YB) <span class="hlt">deformations</span> of string sigma model provide <span class="hlt">deformed</span> target spaces. We propose that homogeneous YB <span class="hlt">deformations</span> always lead to a certain class of β-twisted backgrounds and represent the bosonic part of the supergravity fields in terms of the classical r-matrix associated with the YB <span class="hlt">deformation</span>. We then show that various β-twisted backgrounds can be realized by considering generalized diffeomorphisms in the undeformed background. Our result extends the notable relation between the YB <span class="hlt">deformations</span> and (non-commuting) TsT transformations. We also discuss more general <span class="hlt">deformations</span> beyond the YB <span class="hlt">deformations</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23518230','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23518230"><span>Distal chevron osteotomy with lateral soft tissue <span class="hlt">release</span> for moderate to severe hallux valgus decided using intraoperative varus stress radiographs.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Hyong-Nyun; Park, Yoo-Jung; Kim, Gab-Lae; Park, Yong-Wook</p> <p>2013-01-01</p> <p>The purpose of the present study was to investigate the outcomes of distal chevron osteotomy with lateral soft tissue <span class="hlt">release</span> for moderate to severe hallux valgus. The patients were selected using criteria that included the degree of lateral soft tissue contracture and metatarsocuneiform joint flexibility. The contracture and flexibility were determined from intraoperative varus stress radiographs. From April 2007 to May 2009, 56 feet in 51 consecutive patients with moderate to severe hallux valgus had undergone distal chevron osteotomy with lateral soft tissue <span class="hlt">release</span>. This was done when the lateral soft tissue contracture was not so severe that passive correction of the hallux valgus <span class="hlt">deformity</span> was not possible and when the metatarsocuneiform joint was flexible enough to permit additional correction of the first intermetatarsal angle after lateral soft tissue <span class="hlt">release</span>. The mean patient age was 45.2 (range 23 to 54) years, and the duration of follow-up was 27.5 (range 24 to 46) months. The mean hallux abductus angle decreased from 33.5° ± 3.1° to 11.6° ± 3.3°, and the first intermetatarsal angle decreased from 16.4° ± 2.7° to 9.7° ± 2.1°. The mean American Orthopaedic Foot and Ankle Society hallux-interphalangeal scores increased from 66.6° ± 10.7° to 92.6° ± 9.4° points, and 46 of the 51 patients (90%) were either very satisfied or satisfied with the outcome. No recurrence of <span class="hlt">deformity</span> or osteonecrosis of the metatarsal head occurred. When lateral soft tissue contracture is not severe and when the metatarsocuneiform joint is flexible enough, distal chevron osteotomy with lateral soft tissue <span class="hlt">release</span> can be a useful and effective choice for moderate to severe hallux valgus <span class="hlt">deformity</span>. Copyright © 2013 American College of Foot and Ankle Surgeons. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910048398&hterms=process+accounting&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dprocess%2Baccounting','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910048398&hterms=process+accounting&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dprocess%2Baccounting"><span>Collisionless coupling processes in AMPTE <span class="hlt">releases</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lui, A. T. Y.</p> <p>1990-01-01</p> <p>An evaluation is made of results obtained to date by in situ measurements, numerical simulations, and theoretical considerations of Active Magnetospheric Particle Tracer Explorer chemical <span class="hlt">releases</span> bearing on the nature of collisionless coupling processes. It is noted that both laminar and turbulent forces act to couple the solar wind momentum and <span class="hlt">energy</span> to the <span class="hlt">release</span> cloud; the magnetic field compression formed in this interaction plays an important intermediary role in coupling the two plasmas, and the intense electrostatic turbulence generated enhances the interaction. A scenario accounting for several features in the observed evolution of the December 27, 1984 artificial comet <span class="hlt">release</span> is presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006NIMPB.242..523P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006NIMPB.242..523P"><span>Anisotropic <span class="hlt">deformation</span> of metallo-dielectric core shell colloids under MeV ion irradiation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Penninkhof, J. J.; van Dillen, T.; Roorda, S.; Graf, C.; van Blaaderen, A.; Vredenberg, A. M.; Polman, A.</p> <p>2006-01-01</p> <p>We have studied the <span class="hlt">deformation</span> of metallo-dielectric core-shell colloids under 4 MeV Xe, 6 and 16 MeV Au, 30 MeV Si and 30 MeV Cu ion irradiation. Colloids of silica surrounded by a gold shell, with a typical diameter of 400 nm, show anisotropic plastic <span class="hlt">deformation</span> under MeV ion irradiation, with the metal flowing conform the anisotropically <span class="hlt">deforming</span> silica core. The 20 nm thick metal shell imposes a mechanical constraint on the <span class="hlt">deforming</span> silica core, reducing the net <span class="hlt">deformation</span> strain rate compared to that of pure silica. In colloids consisting of a Au core and a silica shell, the silica expands perpendicular to the ion beam, while the metal core shows a large elongation along the ion beam direction, provided the silica shell is thick enough (>40 nm). A minimum electronic <span class="hlt">energy</span> loss of 3.3 keV/nm is required for shape transformation of the metal core. Silver cores embedded in a silica shell show no elongation, but rather disintegrate. Also in planar SiO2 films, Au and Ag colloids show entirely different behavior under MeV irradiation. We conclude that the <span class="hlt">deformation</span> model of core-shell colloids must include ion-induced particle disintegration in combination with thermodynamical effects, possibly in combination with mechanical effects driven by stresses around the ion tracks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1236599-deformation-metallic-glasses-studied-synchrotron-ray-diffraction','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1236599-deformation-metallic-glasses-studied-synchrotron-ray-diffraction"><span><span class="hlt">Deformation</span> in metallic glasses studied by synchrotron x-ray diffraction</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Dmowski, Wojciech; Egami, Takeshi; Tong, Yang</p> <p>2016-01-11</p> <p>In this study, high mechanical strength is one of the superior properties of metallic glasses which render them promising as a structural material. However, understanding the process of mechanical <span class="hlt">deformation</span> in strongly disordered matter, such as metallic glass, is exceedingly difficult because even an effort to describe the structure qualitatively is hampered by the absence of crystalline periodicity. In spite of such challenges, we demonstrate that high-<span class="hlt">energy</span> synchrotron X-ray diffraction measurement under stress, using a two-dimensional detector coupled with the anisotropic pair-density function (PDF) analysis, has greatly facilitated the effort of unraveling complex atomic rearrangements involved in the elastic, anelastic,more » and plastic <span class="hlt">deformation</span> of metallic glasses. Even though PDF only provides information on the correlation between two atoms and not on many-body correlations, which are often necessary in elucidating various properties, by using stress as means of exciting the system we can garner rich information on the nature of the atomic structure and local atomic rearrangements during <span class="hlt">deformation</span> in glasses.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.9188M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.9188M"><span>The use of Remotely Piloted Aircraft Systems for the Innovative Methodologies in thermal <span class="hlt">Energy</span> <span class="hlt">Release</span> monitoring</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marotta, Enrica; Avino, Rosario; Avvisati, Gala; Belviso, Pasquale; Caliro, Stefano; Caputo, Teresa; Carandente, Antonio; Peluso, Rosario; Sangianantoni, Agata; Sansivero, Fabio; Vilardo, Giuseppe</p> <p>2017-04-01</p> <p>Last years have been characterized by a fast development of Remotely Piloted Aircraft Systems which are becoming cheaper, lighter and more powerful. The concurrent development of high resolution, lightweight and <span class="hlt">energy</span> saving sensors sometimes specifically designed for air-borne applications are together rapidly changing the way in which it is possible to perform monitoring and surveys in hazardous environments such as volcanoes. An example of this convergence is the new methodology we are currently developing at the INGV-Osservatorio Vesuviano for the estimation of the thermal <span class="hlt">energy</span> <span class="hlt">release</span> of volcanic diffuse degassing areas using the ground temperatures from thermal infrared images. Preliminary experiments, carried out during many-years campaigns performed inside at La Solfatara crater by using thermal infrared images and K type thermocouples inserted into the ground at various depths, found a correlation between surface temperature and shallow gradient. Due to the large extent of areas affected by thermal anomalies, an effective and expedite tool to acquire the IR images is a RPAS equipped with high-resolution thermal and visible cameras. These acquisitions allow to quickly acquire the data to produce a heat <span class="hlt">release</span> map. This map is then orthorectified and geocoded in order to be superimposed on digital terrain models or on the orthophotogrammetric mosaic obtained after processing photos acquired by RPAS. Such expedite maps of heat flux, taking in account accurate filtering of atmospheric influence, represents a useful tool for volcanic surveillance monitoring purposes. In order to start all the activities of these drones we had to acquire all necessary permissions required by the complex Italian normative.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5700758','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5700758"><span>PBxplore: a tool to analyze local protein structure and <span class="hlt">deformability</span> with Protein Blocks</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Craveur, Pierrick; Joseph, Agnel Praveen; Jallu, Vincent</p> <p>2017-01-01</p> <p>This paper describes the development and application of a suite of tools, called PBxplore, to analyze the dynamics and <span class="hlt">deformability</span> of protein structures using Protein Blocks (PBs). Proteins are highly dynamic macromolecules, and a classical way to analyze their inherent flexibility is to perform molecular dynamics simulations. The advantage of using small structural prototypes such as PBs is to give a good approximation of the local structure of the protein backbone. More importantly, by reducing the conformational complexity of protein structures, PBs allow analysis of local protein <span class="hlt">deformability</span> which cannot be done with other methods and had been used efficiently in different applications. PBxplore is able to process large amounts of data such as those produced by molecular dynamics simulations. It produces frequencies, entropy and information logo outputs as text and graphics. PBxplore is available at https://github.com/pierrepo/PBxplore and is <span class="hlt">released</span> under the open-source MIT license. PMID:29177113</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.2926A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.2926A"><span>Polygonal <span class="hlt">deformation</span> bands in sandstone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Antonellini, Marco; Nella Mollema, Pauline</p> <p>2017-04-01</p> <p>We report for the first time the occurrence of polygonal faults in sandstone, which is compelling given that layer-bound polygonal fault systems have been observed so far only in fine-grained sediments such as clay and chalk. The polygonal faults are dm-wide zones of shear <span class="hlt">deformation</span> bands that developed under shallow burial conditions in the lower portion of the Jurassic Entrada Fm (Utah, USA). The edges of the polygons are 1 to 5 meters long. The shear <span class="hlt">deformation</span> bands are organized as conjugate faults along each edge of the polygon and form characteristic horst-like structures. The individual <span class="hlt">deformation</span> bands have slip magnitudes ranging from a few mm to 1.5 cm; the cumulative average slip magnitude in a zone is up to 10 cm. The <span class="hlt">deformation</span> bands heaves, in aggregate form, accommodate a small isotropic horizontal extension (strain < 0.005). The individual shear <span class="hlt">deformation</span> bands show abutting T-junctions, veering, curving, and merging where they mechanically interact. Crosscutting relationships are rare. The interactions of the <span class="hlt">deformation</span> bands are similar to those of mode I opening fractures. Density inversion, that takes place where under-compacted and over-pressurized layers (Carmel Fm) lay below normally compacted sediments (Entrada Sandstone), may be an important process for polygonal <span class="hlt">deformation</span> bands formation. The gravitational sliding and soft sediment structures typically observed within the Carmel Fm support this hypothesis. Soft sediment <span class="hlt">deformation</span> may induce polygonal faulting in the section of the Entrada Sandstone just above the Carmel Fm. The permeability of the polygonal <span class="hlt">deformation</span> bands is approximately 10-14 to 10-13 m2, which is less than the permeability of the host, Entrada Sandstone (range 10-12 to 10-11 m2). The documented fault networks have important implications for evaluating the geometry of km-scale polygonal fault systems in the subsurface, top seal integrity, as well as constraining paleo-tectonic stress regimes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20122847','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20122847"><span>Metabolic and stress-related roles of prolactin-<span class="hlt">releasing</span> peptide.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Onaka, Tatsushi; Takayanagi, Yuki; Leng, Gareth</p> <p>2010-05-01</p> <p>In the modern world, improvements in human health can be offset by unhealthy lifestyle factors, including the deleterious consequences of stress and obesity. For <span class="hlt">energy</span> homeostasis, humoral factors and neural afferents from the gastrointestinal tract, in combination with long-term nutritional signals, communicate information to the brain to regulate <span class="hlt">energy</span> intake and expenditure. <span class="hlt">Energy</span> homeostasis and stress interact with each other, and stress affects both food intake and <span class="hlt">energy</span> expenditure. Prolactin-<span class="hlt">releasing</span> peptide, synthesized in discrete neuronal populations in the hypothalamus and brainstem, plays an important role in integrating these responses. This review describes how prolactin-<span class="hlt">releasing</span> peptide neurons receive information concerning both internal metabolic states and environmental conditions, and play a key role in <span class="hlt">energy</span> homeostasis and stress responses. 2010 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C21F1173Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C21F1173Y"><span>InSAR observation of seasonal ground surface <span class="hlt">deformation</span> in permafrost area near Batagay, Siberia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yanagiya, K.; Furuya, M.</p> <p>2017-12-01</p> <p>Thawing of permafrost can lead to ground <span class="hlt">deformation</span>. Ground <span class="hlt">deformation</span> has been studied as a serious problem in the Arctic Ocean coastal area such as Russia for a long time, because the <span class="hlt">deformation</span> causes damage to architectures at these areas. However, there have been no quantitative observation data, and the spatial and temporal distributions have hardly been investigated. On the other hand, by the recently global warming influence, the importance of organic carbon stored in permafrost is pointed out. Although the <span class="hlt">release</span> of methane gas is confirmed in some thermokarst lakes, it is very difficult to observe the permafrost in a wide area by field study. Instead, it is technically possible to monitor the subsidence and uplift of the ground over the permafrost area, which could potentially make a significant contribution to the monitoring thawing process of permafrost. In this study, we attempted to detect ground <span class="hlt">deformation</span> signal in permafrost area by remote sensing using interferometric synthetic aperture radar (InSAR). Using the data of two SAR satellites ALOS and ALOS2 launched by JAXA, we observed recent ground <span class="hlt">deformation</span> from 2007 to 2016. Particularly recent observations of ALOS2 from 2014 to 2016 discovered distant displacements towards the LOS direction in the northeast region from the town of Batagay,Siberia. The diameter of the displacements area covers about 7.7 km. In this study, we considered that this signal is likely to be due to permafrost thawing, we also investigated the seasonal characteristics and looked back ALOS data of this area. In addition, since the high latitude area, observation results include noise due to the ionosphere, so we tried to remove the noise.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007NuPhB.787...55A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007NuPhB.787...55A"><span>Complex marginal <span class="hlt">deformations</span> of D3-brane geometries, their Penrose limits and giant gravitons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Avramis, Spyros D.; Sfetsos, Konstadinos; Zoakos, Dimitrios</p> <p>2007-12-01</p> <p>We apply the Lunin-Maldacena construction of gravity duals to β-<span class="hlt">deformed</span> gauge theories to a class of type IIB backgrounds with U(1 global symmetry, which include the multicenter D3-brane backgrounds dual to the Coulomb branch of N=4 super-Yang-Mills and the rotating D3-brane backgrounds dual to the theory at finite temperature and chemical potential. After a general discussion, we present the full form of the <span class="hlt">deformed</span> metrics for three special cases, which can be used for the study of various aspects of the marginally-<span class="hlt">deformed</span> gauge theories. We also construct the Penrose limits of the solutions dual to the Coulomb branch along a certain set of geodesics and, for the resulting PP-wave metrics, we examine the effect of β-<span class="hlt">deformations</span> on the giant graviton states. We find that giant gravitons exist only up to a critical value of the σ-<span class="hlt">deformation</span> parameter, are not degenerate in <span class="hlt">energy</span> with the point graviton, and remain perturbatively stable. Finally, we probe the σ-<span class="hlt">deformed</span> multicenter solutions by examining the static heavy-quark potential by means of Wilson loops. We find situations that give rise to complete screening as well as linear confinement, with the latter arising is an intriguing way reminiscent of phase transitions in statistical systems.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. 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