Sample records for boundary current final

  1. A new DMSP magnetometer and auroral boundary data set and estimates of field-aligned currents in dynamic auroral boundary coordinates

    NASA Astrophysics Data System (ADS)

    Kilcommons, Liam M.; Redmon, Robert J.; Knipp, Delores J.

    2017-08-01

    We have developed a method for reprocessing the multidecadal, multispacecraft Defense Meteorological Satellite Program Special Sensor Magnetometer (DMSP SSM) data set and have applied it to 15 spacecraft years of data (DMSP Flight 16-18, 2010-2014). This Level-2 data set improves on other available SSM data sets with recalculated spacecraft locations and magnetic perturbations, artifact signal removal, representations of the observations in geomagnetic coordinates, and in situ auroral boundaries. Spacecraft locations have been recalculated using ground-tracking information. Magnetic perturbations (measured field minus modeled main field) are recomputed. The updated locations ensure the appropriate model field is used. We characterize and remove a slow-varying signal in the magnetic field measurements. This signal is a combination of ring current and measurement artifacts. A final artifact remains after processing: step discontinuities in the baseline caused by activation/deactivation of spacecraft electronics. Using coincident data from the DMSP precipitating electrons and ions instrument (SSJ4/5), we detect the in situ auroral boundaries with an improvement to the Redmon et al. (2010) algorithm. We embed the location of the aurora and an accompanying figure of merit in the Level-2 SSM data product. Finally, we demonstrate the potential of this new data set by estimating field-aligned current (FAC) density using the Minimum Variance Analysis technique. The FAC estimates are then expressed in dynamic auroral boundary coordinates using the SSJ-derived boundaries, demonstrating a dawn-dusk asymmetry in average FAC location relative to the equatorward edge of the aurora. The new SSM data set is now available in several public repositories.

  2. Contrasting Boundary Scavenging in two Eastern Boundary Current Regimes

    NASA Astrophysics Data System (ADS)

    Anderson, R. F.; Fleisher, M. Q.; Pavia, F. J.; Vivancos, S. M.; Lu, Y.; Zhang, P.; Cheng, H.; Edwards, R. L.

    2016-02-01

    We use data from two US GEOTRACES expeditions to compare boundary scavenging intensity in two eastern boundary current systems: the Canary Current off Mauritania and the Humboldt Current off Peru. Boundary scavenging refers to the enhanced removal of trace elements from the ocean by sorption to sinking particles in regions of greater than average particle abundance. Both regimes experience high rates of biological productivity and generation of biogenic particles, with rates of productivity potentially a little greater off Peru, whereas dust fluxes are an order of magnitude greater off NW Africa (see presentation by Vivancos et al., this meeting). Despite greater productivity off Peru, we find greater intensity of scavenging off NW Africa as measured by the residence time of dissolved 230Th integrated from the surface to a depth of 2500 m (10-11 years off NW Africa vs. 15-17 years off Peru). Dissolved 231Pa/230Th ratios off NW Africa (Hayes et al., Deep Sea Res.-II 116 (2015) 29-41) are nearly twice the values observed off Peru. We attribute this difference to the well-known tendency for lithogenic phases (dust) to strongly fractionate in favor of Th uptake during scavenging and removal, leaving the dissolved phase enriched in Pa. This behavior needs to be considered when interpreting sedimentary 231Pa/230Th ratios as a paleo proxy.

  3. Conflict in the Currents: The Cross-boundary Consequences of Larval Dispersal

    NASA Astrophysics Data System (ADS)

    Rising, J. A.; Ramesh, N.; Dookie, D.

    2016-02-01

    As commercial fish populations decline in many regions, the increasing demand for ocean resources can create conflicts along international boundaries. Because fish stock ranges do not respect political boundaries, neighboring countries can impact each other through the management of the stocks within their exclusive economic zones. By combining spawning and larvae information from the FishBase database with current velocities from ocean reanalyses using a particle tracking scheme, we construct a measure of the cross-boundary diffusion of fish larvae for 40 major exploited species. These flows represent important connections both for fish populations and for fisheries and the people who depend on them, but these connections rely on fisheries management in the 'source' countries. We then use socioeconomic data on the national importance of these fish to identify hotspots for potential conflict. Finally, we consider how ranges will shift under climate change, and the social impacts of these shifts.

  4. Toroidal current asymmetry and boundary conditions in disruptions

    NASA Astrophysics Data System (ADS)

    Strauss, Henry

    2014-10-01

    It was discovered on JET that disruptions were accompanied by toroidal asymmetry of the plasma current. The toroidal current asymmetry ΔIϕ is proportional to the vertical current moment ΔMIZ , with positive sign for an upward vertical displacement event (VDE) and negative sign for a downward VDE. It was claimed that this could only be explained by Hiro current. It is shown that instead it is essentially a kinematic effect produced by the VDE displacement of a 3D magnetic perturbation. This is verified by M3D simulations. The simulation results do not require penetration of plasma into the boundary, as in the Hiro current model. It is shown that the normal velocity perpendicular to the magnetic field vanishes at the wall, in the small Larmor radius limit of electromagnetic sheath boundary conditions. Plasma is absorbed into the wall only via the parallel velocity, which is small, penetrates only an infinitesimal distance into the wall, and does not affect forces exerted by the plasma on the wall. Supported by USDOE and ITER.

  5. Surface capillary currents: Rediscovery of fluid-structure interaction by forced evolving boundary theory

    NASA Astrophysics Data System (ADS)

    Wang, Chunbai; Mitra, Ambar K.

    2016-01-01

    Any boundary surface evolving in viscous fluid is driven with surface capillary currents. By step function defined for the fluid-structure interface, surface currents are found near a flat wall in a logarithmic form. The general flat-plate boundary layer is demonstrated through the interface kinematics. The dynamics analysis elucidates the relationship of the surface currents with the adhering region as well as the no-slip boundary condition. The wall skin friction coefficient, displacement thickness, and the logarithmic velocity-defect law of the smooth flat-plate boundary-layer flow are derived with the advent of the forced evolving boundary method. This fundamental theory has wide applications in applied science and engineering.

  6. Biogeochemical and ecological impacts of boundary currents in the Indian Ocean

    NASA Astrophysics Data System (ADS)

    Hood, Raleigh R.; Beckley, Lynnath E.; Wiggert, Jerry D.

    2017-08-01

    Monsoon forcing and the unique geomorphology of the Indian Ocean basin result in complex boundary currents, which are unique in many respects. In the northern Indian Ocean, several boundary current systems reverse seasonally. For example, upwelling coincident with northward-flowing currents along the coast of Oman during the Southwest Monsoon gives rise to high productivity which also alters nutrient stoichiometry and therefore, the species composition of the resulting phytoplankton blooms. During the Northeast Monsoon most of the northern Indian Ocean boundary currents reverse and favor downwelling. Higher trophic level species have evolved behavioral responses to these seasonally changing conditions. Examples from the western Arabian Sea include vertical feeding migrations of a copepod (Calanoides carinatus) and the reproductive cycle of a large pelagic fish (Scomberomorus commerson). The impacts of these seasonal current reversals and changes in upwelling and downwelling circulations are also manifested in West Indian coastal waters, where they influence dissolved oxygen concentrations and have been implicated in massive fish kills. The winds and boundary currents reverse seasonally in the Bay of Bengal, though the associated changes in upwelling and productivity are less pronounced. Nonetheless, their effects are observed on the East Indian shelf as, for example, seasonal changes in copepod abundance and zooplankton community structure. In contrast, south of Sri Lanka seasonal reversals in the boundary currents are associated with dramatic changes in the intensity of coastal upwelling, chlorophyll concentration, and catch per unit effort of fishes. Off the coast of Java, monsoon-driven changes in the currents and upwelling strongly impact chlorophyll concentrations, seasonal vertical migrations of zooplankton, and sardine catch in Bali Strait. In the southern hemisphere the Leeuwin is a downwelling-favorable current that flows southward along western Australia

  7. Boundary Waves on the Ice Surface Created by Currents

    NASA Astrophysics Data System (ADS)

    Naito, K.; Izumi, N.; Yokokawa, M.; Yamada, T.; de Lima, A. C.

    2013-12-01

    The formation of periodic boundary waves, e.g. antidunes and cyclic steps (Parker & Izumi 2000) has been known to be caused by instabilities between flow and bed (e.g. Engelund 1970), and are observed not only on river beds or ocean floors but also on ice surfaces, such as the surface of glaciers and underside of river ice (Carey 1966). In addition, owing to recent advancements of remote sensing technology, it has been found that the surfaces of the polar ice caps on Mars as well as on the Earth have step-like formations (Smith & Holt 2010) which are assumed to be boundary waves, because they are generated perpendicularly to the direction of the currents. These currents acting on the polar ice caps are density airflow, i.e. katabatic wind (Howard et al 2000). The comprehension of the formation process of the Martian polar ice caps may reveal climate changes which have occurred on Mars. Although the formation of boundary waves on river beds or ocean floors has been studied by a number of researchers, there are few works on their formation on ice surfaces. Yokokawa et al (2013) suggested that the temperature distribution of the ambient air, fluid and ice is a factor which determines the direction of migration of boundary waves formed on ice surfaces through their experiments. In this study, we propose a mathematical model in order to describe the formation process of the boundary waves and the direction of their migration. We consider that a liquid is flowing through a flume filled with a flat ice layer on the bottom. The flow is assumed to be turbulent and its temperature is assumed to merge with the ambient temperature at the flow surface and with the melting point of ice at the bottom (ice surface). The ice surface evolution is dependent on the unbalance between the interfacial heat flux of the liquid and ice, and we employ the Reynolds-averaged Navier-Stokes equation, the continuity equation, heat transfer equations for the liquid and ice, and a heat balance

  8. 78 FR 56650 - Boundary Description and Final Map for Roaring Wild and Scenic River, Mount Hood National Forest...

    Federal Register 2010, 2011, 2012, 2013, 2014

    2013-09-13

    ... DEPARTMENT OF AGRICULTURE Forest Service Boundary Description and Final Map for Roaring Wild and... availability. SUMMARY: In accordance with section 3(b) of the Wild and Scenic Rivers Act, the USDA Forest Service, Washington Office, is transmitting the final boundary description and map of the Roaring Wild and...

  9. How to interpret current-voltage relationships of blocking grain boundaries in oxygen ionic conductors.

    PubMed

    Kim, Seong K; Khodorov, Sergey; Chen, Chien-Ting; Kim, Sangtae; Lubomirsky, Igor

    2013-06-14

    A new model based on a linear diffusion equation is proposed to explain the current-voltage characteristics of blocking grain boundaries in Y-doped CeO2 in particular. One can also expect that the model can be applicable to the ionic conductors with blocking grain boundaries, in general. The model considers an infinitely long chain of identical grains separated by grain boundaries, which are treated as regions in which depletion layers of mobile ions are formed due to trapping of immobile charges that do not depend on the applied voltage as well as temperature. The model assumes that (1) the grain boundaries do not represent physical blocking layers, which implies that if there is a second phase at the grain boundaries, then it is too thin to impede ion diffusion and (2) the ions follow Boltzmann distribution throughout the materials. Despite its simplicity, the model successfully reproduces the "power law": current proportional to voltage power n and illustrated with the experimental example of Y-doped ceria. The model also correctly predicts that the product nT, where T is the temperature in K, is constant and is proportional to the grain boundary potential as long as the charge at the grain boundaries remains trapped. The latter allows its direct determination from the current-voltage characteristics and promises considerable simplification in the analysis of the electrical characteristics of the grain boundaries with respect to the models currently in use.

  10. Current Dilemmas in Defining the Boundaries of Disease.

    PubMed

    Doust, Jenny; Jean Walker, Mary; Rogers, Wendy A

    2017-08-01

    Boorse's biostatistical theory states that diseases should be defined in ways that reflect disturbances of biological function and that are objective and value free. We use three examples from contemporary medicine that demonstrate the complex issues that arise when defining the boundaries of disease: polycystic ovary syndrome, chronic kidney disease, and myocardial infarction. We argue that the biostatistical theory fails to provide sufficient guidance on where the boundaries of disease should be drawn, contains ambiguities relating to choice of reference class, and is out of step with medical processes for identifying disease boundaries. Although proponents of the biostatistical theory might regard these practical issues as irrelevant to the aim of providing a theoretical account of disease, we take them to indicate the need for a theoretical account that is adequate for current needs-including limiting new forms of medicalization that are driven by the identification of disease based on dysfunction. Our processes for determining the boundaries for disease need to recognize that there is no value-free method for making these decisions. © The Author 2017. Published by Oxford University Press, on behalf of the Journal of Medicine and Philosophy Inc. All rights reserved. For permissions, please e-mail: journals.permissions@oup.com.

  11. Comparison of DMSP and SECS region-1 and region-2 ionospheric current boundary

    NASA Astrophysics Data System (ADS)

    Weygand, J. M.; Wing, S.

    2016-06-01

    The region-1 and region-2 boundary has traditionally been identified using data from a single spacecraft crossing the auroral region and measuring the large scale changes in the cross track magnetic field. With data from the AUTUMN, CANMOS, CARISMA, GIMA, DTU MGS, MACCS, McMAC, STEP, THEMIS, and USGS ground magnetometer arrays we applied a state-of-art technique based on spherical elementary current system (SECS) method developed by Amm and Viljanen (1999) in order to calculate maps of region-1 and region-2 current system over the North American and Greenland auroral region. Spherical elementary current (SEC) amplitude (proxy for vertical currents) maps can be inferred at 10 s temporal resolution, ~1.5° geographic latitude (Glat), and 3.5° geographic longitude (Glon) spatial resolution. We compare the location of the region-1 and region-2 boundary obtained by the DMSP spacecraft with the region-1 and region-2 boundary observed in the SEC current amplitudes. We find that the boundaries typically agree within 0.2°±1.3°. These results indicate that the location of the region-1 and region-2 boundary can reasonably be determined from ground magnetometer data. The SECS maps represent a value-added product from the magnetometer database and can be used for contextual interpretation in conjunction with other missions as well as help with our understanding of magnetosphere-ionosphere coupling mechanisms using the ground arrays and the magnetospheric spacecraft data.

  12. Comparison of DMSP and SECS region-1 and region-2 ionospheric current boundary.

    PubMed

    Weygand, J M; Wing, S

    2016-06-01

    The region-1 and region-2 boundary has traditionally been identified using data from a single spacecraft crossing the auroral region and measuring the large scale changes in the cross track magnetic field. With data from the AUTUMN, CANMOS, CARISMA, GIMA, DTU MGS, MACCS, McMAC, STEP, THEMIS, and USGS ground magnetometer arrays we applied a state-of-art technique based on spherical elementary current system (SECS) method developed by Amm and Viljanen (1999) in order to calculate maps of region-1 and region-2 current system over the North American and Greenland auroral region. Spherical elementary current (SEC) amplitude (proxy for vertical currents) maps can be inferred at 10 s temporal resolution, ~1.5° geographic latitude (Glat), and 3.5° geographic longitude (Glon) spatial resolution. We compare the location of the region-1 and region-2 boundary obtained by the DMSP spacecraft with the region-1 and region-2 boundary observed in the SEC current amplitudes. We find that the boundaries typically agree within 0.2° ± 1.3°. These results indicate that the location of the region-1 and region-2 boundary can reasonably be determined from ground magnetometer data. The SECS maps represent a value-added product from the magnetometer database and can be used for contextual interpretation in conjunction with other missions as well as help with our understanding of magnetosphere-ionosphere coupling mechanisms using the ground arrays and the magnetospheric spacecraft data.

  13. A western boundary current eddy characterisation study

    NASA Astrophysics Data System (ADS)

    Ribbe, Joachim; Brieva, Daniel

    2016-12-01

    The analysis of an eddy census for the East Australian Current (EAC) region yielded a total of 497 individual short-lived (7-28 days) cyclonic and anticyclonic eddies for the period 1993 to 2015. This was an average of about 23 eddies per year. 41% of the tracked individual cyclonic and anticyclonic eddies were detected off southeast Queensland between about 25 °S and 29 °S. This is the region where the flow of the EAC intensifies forming a swift western boundary current that impinges near Fraser Island on the continental shelf. This zone was also identified as having a maximum in detected short-lived cyclonic eddies. A total of 94 (43%) individual cyclonic eddies or about 4-5 per year were tracked in this region. The census found that these potentially displaced entrained water by about 115 km with an average displacement speed of about 4 km per day. Cyclonic eddies were likely to contribute to establishing an on-shelf longshore northerly flow forming the western branch of the Fraser Island Gyre and possibly presented an important cross-shelf transport process in the life cycle of temperate fish species of the EAC domain. In-situ observations near western boundary currents previously documented the entrainment, off-shelf transport and export of near shore water, nutrients, sediments, fish larvae and the renewal of inner shelf water due to short-lived eddies. This study found that these cyclonic eddies potentially play an important off-shelf transport process off the central east Australian coast.

  14. Pacific western boundary currents and their roles in climate.

    PubMed

    Hu, Dunxin; Wu, Lixin; Cai, Wenju; Gupta, Alex Sen; Ganachaud, Alexandre; Qiu, Bo; Gordon, Arnold L; Lin, Xiaopei; Chen, Zhaohui; Hu, Shijian; Wang, Guojian; Wang, Qingye; Sprintall, Janet; Qu, Tangdong; Kashino, Yuji; Wang, Fan; Kessler, William S

    2015-06-18

    Pacific Ocean western boundary currents and the interlinked equatorial Pacific circulation system were among the first currents of these types to be explored by pioneering oceanographers. The widely accepted but poorly quantified importance of these currents-in processes such as the El Niño/Southern Oscillation, the Pacific Decadal Oscillation and the Indonesian Throughflow-has triggered renewed interest. Ongoing efforts are seeking to understand the heat and mass balances of the equatorial Pacific, and possible changes associated with greenhouse-gas-induced climate change. Only a concerted international effort will close the observational, theoretical and technical gaps currently limiting a robust answer to these elusive questions.

  15. A western boundary current east of New Caledonia: Observed characteristics

    NASA Astrophysics Data System (ADS)

    Gasparin, Florent; Ganachaud, Alexandre; Maes, Christophe

    2011-09-01

    Waters from the South Equatorial Current (SEC), the northern branch of the South Pacific subtropical gyre, are a major supply of heat to the equatorial warm pool, and have an important contribution to climate variability and ENSO which motivated the Southwest Pacific Ocean and Climate Experiment (SPICE, CLIVAR/WCRP). Initially a broad westward current extending from the equator to 30°S, the SEC splits upon arriving at the major islands and archipelagoes of Fiji (18°S, 180°E), Vanuatu (16°S, 168°E), and New Caledonia (22°S, 165°E), resulting in a complex system of western boundary currents and zonal jets that feed the Coral and Solomon Seas. We focus here on the formation of one specific jet feeding the Coral Sea, the North Caledonian Jet (NCJ). Using a combination of recent oceanographic cruises, we describe the ocean circulation to the northeast of New Caledonia, where the SEC forms a western boundary current that ultimately becomes the NCJ. This current, which we document for the first time and propose to refer to as the East Caledonian Current (ECC), has its core located 10-100 km off the east coast of New Caledonia, and extends vertically to at least 1000 m depth. Water mass properties show continuous westward transports through the ECC, from the SEC to the NCJ in both the South Pacific Tropical Waters in the thermocline and Antarctic Intermediate Waters near 700 m depth. The ECC extends about 100 km horizontally; its average 0-1000 m transport was estimated at 14.5±3 Sv off the north tip of the New Caledonian reef, with a maximum of 20 Sv in May 2010. South of that the upstream branch of the ECC east of the Loyalty is close to 8 Sv suggesting an important additional contribution from central Pacific waters carried by the SEC at 16°S and diverted to our region through the western boundary current system east of Vanuatu.

  16. Break-up of the Atlantic deep western boundary current into eddies at 8 degrees S.

    PubMed

    Dengler, M; Schott, F A; Eden, C; Brandt, P; Fischer, J; Zantopp, R J

    2004-12-23

    The existence in the ocean of deep western boundary currents, which connect the high-latitude regions where deep water is formed with upwelling regions as part of the global ocean circulation, was postulated more than 40 years ago. These ocean currents have been found adjacent to the continental slopes of all ocean basins, and have core depths between 1,500 and 4,000 m. In the Atlantic Ocean, the deep western boundary current is estimated to carry (10-40) x 10(6) m3 s(-1) of water, transporting North Atlantic Deep Water--from the overflow regions between Greenland and Scotland and from the Labrador Sea--into the South Atlantic and the Antarctic circumpolar current. Here we present direct velocity and water mass observations obtained in the period 2000 to 2003, as well as results from a numerical ocean circulation model, showing that the Atlantic deep western boundary current breaks up at 8 degrees S. Southward of this latitude, the transport of North Atlantic Deep Water into the South Atlantic Ocean is accomplished by migrating eddies, rather than by a continuous flow. Our model simulation indicates that the deep western boundary current breaks up into eddies at the present intensity of meridional overturning circulation. For weaker overturning, continuation as a stable, laminar boundary flow seems possible.

  17. An Optimized Combined Wave and Current Bottom Boundary Layer Model for Arbitrary Bed Roughness

    DTIC Science & Technology

    2017-06-30

    Engineer Research and Development Center (ERDC), Coastal and Hydraulics Laboratory (CHL), Flood and Storm Protection Division (HF), Coastal ...ER D C/ CH L TR -1 7- 11 Coastal Inlets Research Program An Optimized Combined Wave and Current Bottom Boundary Layer Model for...client/default. Coastal Inlets Research Program ERDC/CHL TR-17-11 June 2017 An Optimized Combined Wave and Current Bottom Boundary Layer Model

  18. Observed bottom boundary layer transport and uplift on the continental shelf adjacent to a western boundary current

    NASA Astrophysics Data System (ADS)

    Schaeffer, A.; Roughan, M.; Wood, J. E.

    2014-08-01

    Western boundary currents strongly influence the dynamics on the adjacent continental shelf and in particular the cross-shelf transport and uplift through the bottom boundary layer. Four years of moored in situ observations on the narrow southeastern Australian shelf (in water depths of between 65 and 140 m) were used to investigate bottom cross-shelf transport, both upstream (30°S) and downstream (34°S) of the separation zone of the East Australian Current (EAC). Bottom transport was estimated and assessed against Ekman theory, showing consistent results for a number of different formulations of the boundary layer thickness. Net bottom cross-shelf transport was onshore at all locations. Ekman theory indicates that up to 64% of the transport variability is driven by the along-shelf bottom stress. Onshore transport in the bottom boundary layer was more intense and frequent upstream than downstream, occurring 64% of the time at 30°S. Wind-driven surface Ekman transport estimates did not balance the bottom cross-shelf flow. At both locations, strong variability was found in bottom water transport at periods of approximately 90-100 days. This corresponds with periodicity in EAC fluctuations and eddy shedding as evidenced from altimeter observations, highlighting the EAC as a driver of variability in the continental shelf waters. Ocean glider and HF radar observations were used to identify the bio-physical response to an EAC encroachment event, resulting in a strong onshore bottom flow, the uplift of cold slope water, and elevated coastal chlorophyll concentrations.

  19. 78 FR 56650 - Boundary Description and Final Map for Sandy Wild and Scenic River, Upper Portion, Mount Hood...

    Federal Register 2010, 2011, 2012, 2013, 2014

    2013-09-13

    ... DEPARTMENT OF AGRICULTURE Forest Service Boundary Description and Final Map for Sandy Wild and...: Notice of availability. SUMMARY: In accordance with section 3(b) of the Wild and Scenic Rivers Act, the... Sandy Wild and Scenic River, Upper Portion, to Congress. DATES: The boundaries and classification of the...

  20. Observation of chiral currents at the magnetic domain boundary of a topological insulator

    DOE PAGES

    Wang, Y. H.; Kirtley, J. R.; Katmis, F.; ...

    2015-08-28

    A magnetic domain boundary on the surface of a three-dimensional topological insulator is predicted to host a chiral edge state, but direct demonstration is challenging. Here, we used a scanning superconducting quantum interference device to show that current in a magnetized EuS/Bi 2Se 3 heterostructure flows at the edge when the Fermi level is gate-tuned to the surface band gap. We further induced micron-scale magnetic structures on the heterostructure, and detected a chiral edge current at the magnetic domain boundary. The chirality of the current was determined by magnetization of the surrounding domain and its magnitude by the local chemicalmore » potential rather than the applied current. As a result, such magnetic structures, provide a platform for detecting topological magnetoelectric effects and may enable progress in quantum information processing and spintronics.« less

  1. Theoretical model and experimental investigation of current density boundary condition for welding arc study

    NASA Astrophysics Data System (ADS)

    Boutaghane, A.; Bouhadef, K.; Valensi, F.; Pellerin, S.; Benkedda, Y.

    2011-04-01

    This paper presents results of theoretical and experimental investigation of the welding arc in Gas Tungsten Arc Welding (GTAW) and Gas Metal Arc Welding (GMAW) processes. A theoretical model consisting in simultaneous resolution of the set of conservation equations for mass, momentum, energy and current, Ohm's law and Maxwell equation is used to predict temperatures and current density distribution in argon welding arcs. A current density profile had to be assumed over the surface of the cathode as a boundary condition in order to make the theoretical calculations possible. In stationary GTAW process, this assumption leads to fair agreement with experimental results reported in literature with maximum arc temperatures of ~21 000 K. In contrast to the GTAW process, in GMAW process, the electrode is consumable and non-thermionic, and a realistic boundary condition of the current density is lacking. For establishing this crucial boundary condition which is the current density in the anode melting electrode, an original method is setup to enable the current density to be determined experimentally. High-speed camera (3000 images/s) is used to get geometrical dimensions of the welding wire used as anode. The total area of the melting anode covered by the arc plasma being determined, the current density at the anode surface can be calculated. For a 330 A arc, the current density at the melting anode surface is found to be of 5 × 107 A m-2 for a 1.2 mm diameter welding electrode.

  2. Ecological importance of the Southern Boundary of the Antarctic Circumpolar Current

    NASA Astrophysics Data System (ADS)

    Tynan, Cynthia T.

    1998-04-01

    The Southern Ocean surrounds the Antarctic continent and supports one of the most productive marine ecosystems. Migratory and endemic species of whales, seals and birds benefit from the high biomass of their principal prey, krill (Euphausia superba) and cephalopods, in this area. Most species of baleen whales and male sperm whales in the Southern Hemisphere migrate between low-latitude breeding grounds in winter and highly productive Antarctic feeding grounds in summer. Here I show the importance of the southernmost reaches of the strongest ocean current, the Antarctic Circumpolar Current (ACC), to a complex and predictable food web of the Southern Ocean. The circumpolar distributions of blue, fin and humpback whales from spring to midsummer trace the non-uniform high-latitude penetration of shoaled, nutrient-rich Upper Circumpolar Deep Water, which is carried eastward by the ACC. The poleward extent of this water mass delineates the Southern Boundary of the ACC and corresponds not only to the circumpolar distributions of baleen whales, but also to distributions of krill and to regions of high, seasonally averaged, phytoplankton biomass. Sperm whales, which feed on cephalopods, also congregate in highest densities near the Southern Boundary. The association of primary production, Krill, and whales with the Southern Boundary, suggests that it provides predictably productive foraging for many species, and is of critical importance to the function of the Southern Ocean ecosystem.

  3. Ring-slope interactions and the formation of the western boundary current in the Gulf of Mexico

    NASA Astrophysics Data System (ADS)

    Vidal, VíCtor M. V.; Vidal, Francisco V.; Meza, Eustorgio; Portilla, Josué; Zambrano, Lorenzo; Jaimes, BenjamíN.

    1999-09-01

    Hydrographic data from the Gulf of Mexico (gulf) provide evidence that a western boundary current was set up by the interaction of an anticyclonic Loop Current (LC) ring with the continental margin of the western gulf during March-August 1985. The March 1985 geostrophic circulation reveals a remnant anticyclonic ring colliding with the slope. During this collision, two cyclonic rings were shed as the anticyclone transferred vorticity to the surrounding slope water. During July-August 1985, the ring triad weakened and evolved into a ˜900-km-long, north flowing, along-slope, western boundary current and cyclonic-anticyclonic ring pairs distributed throughout the central and western gulf. This western boundary current attained maximum northward flow speeds of 25 cm s-1 and an 8.3-Sv mass transport between 94°-96°W at 25°N. Our March-August 1985 observations reveal that the residence time and decay period of LC anticyclones in the western gulf may exceed 150 days. Within this time period the western gulf's cyclonic-anticyclonic vorticity field decayed ˜50%. Thus the western boundary current's evolutionary period, from its gestation to its absolute decay, is estimated to be of the order of 300 days. Although the presence of a western boundary current in the gulf has been attributed to the annual wind stress curl cycle [Sturges, 1993], our analyses of the western gulf March and July-August 1985 ring-driven geostrophic circulation and corresponding (January, February and May, June 1985) monthly mean synoptic wind stress curl distributions reveal that these constitute competing forcing mechanisms for the gulf's regional circulation. However, when very strong local forcing such as large eddies are present, the wind-driven background circulation is overwhelmed by such eddy forcing.

  4. Observations of the magnetopause current layer: Cases with no boundary layer and tests of recent models

    NASA Technical Reports Server (NTRS)

    Eastman, Timothy E.

    1995-01-01

    Evidence for the probable existence of magnetospheric boundary layers was first presented by Hones, et al. (1972), based on VELA satellite plasma observations (no magnetic field measurements were obtained). This magnetotail boundary layer is now known to be the tailward extension of the high-latitude boundary layer or plasma mantle (first uniquely identified using HEOS 2 plasma and field observations by Rosenbauer et al., 1975) and the low-latitude boundary layer (first uniquely identified using IMP 6 plasma and field observations by Eastman et al., 1976). The magnetospheric boundary layer is the region of magnetosheath-like plasma located Earthward of, but generally contiguous with the magnetopause. This boundary layer is typically identified by comparing low-energy (less than 10 keV) ion spectra across the magnetopause. Low-energy electron measurements are also useful for identifying the boundary layer because the shocked solar wind or magnetosheath has a characteristic spectral signature for electrons as well. However, there are magnetopause crossings where low-energy electrons might suggest a depletion layer outside the magnetopause even though the traditional field-rotation signature indicates that this same region is a boundary layer Earthward of the current layer. Our analyses avoided crossings which exhibit such ambiguities. Pristine magnetopause crossings are magnetopause crossings for which the current layer is well defined and for which there is no adjoining magnetospheric boundary layer as defined above. Although most magnetopause models to date apply to such crossings, few comparisons between such theory and observations of pristine magnetopause crossings have been made because most crossings have an associated magnetospheric boundary layer which significantly affects the applicable boundary conditions for the magnetopause current layer. Furthermore, almost no observational studies of magnetopause microstructure have been done even though key

  5. Dynamics of Eastern Boundary Currents and Their Effects on Sound Speed Structure

    DTIC Science & Technology

    2006-06-01

    Canary Current System (NCCS) off Morocco and the Iberian Peninsula , and the Leeuwin Current System (LCS) off Western Australia. These systems...Africa and the Iberian Peninsula . This system is considered a classical EBC and marks the closing eastern boundary of the North Atlantic Gyre...with several narrow filaments of cooler water extending off the coast of the Iberian Peninsula (Fiuza and Sousa, 1989) and Cape Ghir in northwest Africa

  6. Theory and observations of upward field-aligned currents at the magnetopause boundary layer.

    PubMed

    Wing, Simon; Johnson, Jay R

    2015-11-16

    The dependence of the upward field-aligned current density ( J ‖ ) at the dayside magnetopause boundary layer is well described by a simple analytic model based on a velocity shear generator. A previous observational survey confirmed that the scaling properties predicted by the analytical model are applicable between 11 and 17 MLT. We utilize the analytic model to predict field-aligned currents using solar wind and ionospheric parameters and compare with direct observations. The calculated and observed parallel currents are in excellent agreement, suggesting that the model may be useful to infer boundary layer structures. However, near noon, where velocity shear is small, the kinetic pressure gradients and thermal currents, which are not included in the model, could make a small but significant contribution to J ‖ . Excluding data from noon, our least squares fit returns log( J ‖,max_cal ) = (0.96 ± 0.04) log( J ‖_obs ) + (0.03 ± 0.01) where J ‖,max_cal = calculated J ‖,max and J ‖_obs = observed J ‖ .

  7. Current Pattern Change in the Fram Strait at the Pliocene/Pleistocene Boundary

    NASA Astrophysics Data System (ADS)

    Gebhardt, C.; Geissler, W. H.; Matthiessen, J. J.; Jokat, W.

    2014-12-01

    Thick packages of drift-type sediments were identified in the northwestern and central part of the Fram Strait, mainly along the western Yermak Plateau flank, but also in the central, flat part of the Fram Strait. A large-scale field of sediment waves was found north of 80.5°, along the Yermak Plateau rise. This field separates two drift bodies, a deeper one towards west and a shallower one towards east. The drift bodies were deposited by bottom currents, most likely by the northbound Yermak Branch of the West Spitsbergen Current, but an influence of a southbound current on the westren drift body cannot be ruled out. Within the drift bodies and even more pronounced withing the sediment waves, a stratigraphic boundary is clearly visible. It separates a lower package of waves migrating upslope at a low angle of ~5° from an upper package with significantly increased wave crest migration at ~16.5°. Using the seismic network, this stratigraphic boundary could be tracked to ODP Leg 151, Site 911, where it corresponds to the lithostratigraphic boundary between units IA and IB dated to 2.7 Ma. The increase in wave-crest migration angle points at a shift towards higher sedimentation rates at 2.7 Ma. This corresponds to the intensification of the Northern Hemisphere glaciation with a major expansion of the Scandinavian, northern Barents Sea, North American and Greenland ice sheets. The Barents Shelf that was subaerially exposed and the expansion of the northern Barents Sea ice sheet (as well as Svalbard) are the likely sources for enhanced erosion and fluvial input along the pathway of the West Spitsbergen Current, resulting in higher sedimentation rates in the Fram Strait.

  8. Integrating Observations of the Boundary Current Flow around Sri Lanka

    DTIC Science & Technology

    2015-09-30

    around Sri Lanka Uwe Send and Matthias Lankhorst Scripps Institution of Oceanography 9500 Gilman Drive, Mail Code 0230 La Jolla, CA 92093-0230...of Bengal. For this, the flow around Sri Lanka is critical since it exchanges salt and freshwater between the Bay of Bengal and the Arabian Sea...OBJECTIVES In-situ continuous observations of the boundary current flow around Sri Lanka will be collected over a period of several years. In order

  9. The boundary current role on the transport and stranding of floating marine litter: The French Riviera case

    NASA Astrophysics Data System (ADS)

    Ourmieres, Yann; Mansui, Jérémy; Molcard, Anne; Galgani, François; Poitou, Isabelle

    2018-03-01

    The aim of the present study is to evidence the role of a boundary current and meteorological conditions in the transport and stranding of floating marine debris. The used data are from a beach survey and an inter-annual unique effort of marine debris sightings along the French Riviera in the North-Western Mediterranean region. Offshore data have been collected during oceanic cruises while beach surveys were performed around Antibes city. Debris were found on 97% of the ocean transects, with a large spatial and temporal variability, showing contrasted areas of low ( 1 item/km2) and of high (> 10 items/km2) debris densities. Results suggest that the debris spatio-temporal distribution is related to the Northern current (NC) dynamics, the regional boundary current, with accumulation patterns in its core and external edge. By playing a role in the alongshore transport, such a boundary current can form a cross-shore transport barrier. Stranding events can then occur after strong on-shore wind bursts modifying the sea surface dynamics and breaking this transport barrier. It is also shown that episodic enhancement of the stranding rate can be explained by combining the NC dynamics with the wind forcing and the rainfall effect via the local river run-off. Conversely, off-shore wind bursts could also free the marine litter from the boundary current and export them towards the open sea.

  10. Final report: Constructing comprehensive models of grain boundaries using high-throughput experiments

    DOE Office of Scientific and Technical Information (OSTI.GOV)

    Demkowicz, Michael; Schuh, Christopher; Marzouk, Youssef

    2016-08-29

    This is the final report on project DE-SC0008926. The goal of this project was to create capabilities for constructing, analyzing, and modeling experimental databases of the crystallographic characters and physical properties of thousands of individual grain boundaries (GBs) in polycrystalline metals. This project focused on gallium permeation through aluminum (Al) GBs and hydrogen uptake into nickel (Ni) GBs as model problems. This report summarizes the work done within the duration of this project (including the original three-year award and the subsequent one-year renewal), i.e. from August 1, 2012 until April 30, 2016.

  11. Production regimes in four eastern boundary current systems

    NASA Technical Reports Server (NTRS)

    Carr, M. E.; Kearns, E. J.

    2003-01-01

    High productivity (maxima 3 g C m(sup -2)day(sup -1)) of the Eastern Boundary Currents (EBCs), i.e. the California, Peru-Humboldt, Canary and Benguela Currents, is driven by a combination of local forcing and large-scale circulation. The characteristics of the deep water brought to the surface by upwelling favorable winds depend on the large-scale circulation patterns. Here we use a new hydrographic and nutrient climatology together with satellite measurements ofthe wind vector, sea-surface temperature (SST), chlorophyll concentration, and primary production modeled from ocean color to quantify the meridional and seasonal patterns of upwelling dynamics and biological response. The unprecedented combination of data sets allows us to describe objectively the variability for small regions within each current and to characterize the governing factors for biological production. The temporal and spatial environmental variability was due in most regions to large-scale circulation, alone or in combination with offshore transport (local forcing). The observed meridional and seasonal patterns of biomass and primary production were most highlycorrelated to components representing large-scale circulation. The biomass sustained by a given nutrient concentration in the Atlantic EBCs was twice as large as that of the Pacific EBCs. This apparent greater efficiency may be due toavailability of iron, physical retention, or differences in planktonic community structure.

  12. A High-Lift Building Block Flow: Turbulent Boundary Layer Relaminarization A Final Report

    NASA Technical Reports Server (NTRS)

    Bourassa, Corey; Thomas, Flint O.; Nelson, Robert C.

    2000-01-01

    Experimental evidence exists which suggests turbulent boundary layer relaminarization may play an important role in the inverse Reynolds number effect in high-lift systems. An experimental investigation of turbulent boundary layer relaminarization has been undertaken at the University of Notre Dame's Hessert Center for Aerospace Research in cooperation with NASA Dryden Flight Research Center. A wind tunnel facility has been constructed at the Hessert Center and relaminarization achieved. Preliminary evidence suggests the current predictive tools available are inadequate at determining the onset of relaminarization. In addition, an in-flight relaminarization experiment for the NASA Dryden FTF-II has been designed to explore relaminarization at Mach and Reynolds numbers more typical of commercial high-lift systems.

  13. Effects of Uncertainties in Electric Field Boundary Conditions for Ring Current Simulations

    NASA Astrophysics Data System (ADS)

    Chen, Margaret W.; O'Brien, T. Paul; Lemon, Colby L.; Guild, Timothy B.

    2018-01-01

    Physics-based simulation results can vary widely depending on the applied boundary conditions. As a first step toward assessing the effect of boundary conditions on ring current simulations, we analyze the uncertainty of cross-polar cap potentials (CPCP) on electric field boundary conditions applied to the Rice Convection Model-Equilibrium (RCM-E). The empirical Weimer model of CPCP is chosen as the reference model and Defense Meteorological Satellite Program CPCP measurements as the reference data. Using temporal correlations from a statistical analysis of the "errors" between the reference model and data, we construct a Monte Carlo CPCP discrete time series model that can be generalized to other model boundary conditions. RCM-E simulations using electric field boundary conditions from the reference model and from 20 randomly generated Monte Carlo discrete time series of CPCP are performed for two large storms. During the 10 August 2000 storm main phase, the proton density at 10 RE at midnight was observed to be low (< 1.4 cm-3) and the observed disturbance Dst index is bounded by the simulated Dst values. In contrast, the simulated Dst values during the recovery phases of the 10 August 2000 and 31 August 2005 storms tend to underestimate systematically the observed late Dst recovery. This suggests a need to improve the accuracy of particle loss calculations in the RCM-E model. Application of this technique can aid modelers to make efficient choices on either investing more effort on improving specification of boundary conditions or on improving descriptions of physical processes.

  14. Remote sensing of ocean current boundary layer. [Loop Current in Gulf of Mexico

    NASA Technical Reports Server (NTRS)

    Maul, G. A. (Principal Investigator)

    1973-01-01

    The author has identified the following significant results. A time series of the Loop Current in the Gulf of Mexico, covering an annual cycle of growth, spreading, and decay, has been obtained in synchronization with ERTS-1. Computer enhanced images, which are necessary to extract useful oceanic information, show that the current can be observed either by color or sea state effects associated with the cyclonic boundary. The color effect relates to the spectral variations in the optical properties of the water and its suspended particles, and is studied by radiative transfer theory. Significant oceanic parameters identified are: the probability of forward scattering, and the ratio of scattering to total attenuation. Several spectra of upwelling diffuse light are computed as a function of the concentration of particles and yellow substance. These calculations compare favorably with experimental measurements and show that the ratio of channels method gives ambiguous interpretative results. These results are used to discuss features in images where surface measurements were obtained and are extended to tentative explanation in others.

  15. Regional Wave Climates along Eastern Boundary Currents

    NASA Astrophysics Data System (ADS)

    Semedo, Alvaro; Soares, Pedro

    2016-04-01

    Two types of wind-generated gravity waves coexist at the ocean surface: wind sea and swell. Wind sea waves are waves under growing process. These young growing waves receive energy from the overlaying wind and are strongly coupled to the local wind field. Waves that propagate away from their generation area and no longer receive energy input from the local wind are called swell. Swell waves can travel long distances across entire ocean basins. A qualitative study of the ocean waves from a locally vs. remotely generation perspective is important, since the air sea interaction processes is strongly modulated by waves and vary accordingly to the prevalence of wind sea or swell waves in the area. A detailed climatology of wind sea and swell waves along eastern boundary currents (EBC; California Current, Canary Current, in the Northern Hemisphere, and Humboldt Current, Benguela Current, and Western Australia Current, in the Southern Hemisphere), based on the ECMWF (European Centre for Medium-Range Weather Forecasts) ERA-Interim reanalysis will be presented. The wind regime along EBC varies significantly from winter to summer. The high summer wind speeds along EBC generate higher locally generated wind sea waves, whereas lower winter wind speeds in these areas, along with stronger winter extratropical storms far away, lead to a predominance of swell waves there. In summer, the coast parallel winds also interact with coastal headlands, increasing the wind speed through a process called "expansion fan", which leads to an increase in the height of locally generated waves downwind of capes and points. Hence the spatial patterns of the wind sea or swell regional wave fields are shown to be different from the open ocean along EBC, due to coastal geometry and fetch dimensions. Swell waves will be shown to be considerably more prevalent and to carry more energy in winter along EBC, while in summer locally generated wind sea waves are either more comparable to swell waves or

  16. Physics of magnetospheric boundary layers

    NASA Technical Reports Server (NTRS)

    Cairns, I. H.

    1993-01-01

    The central ideas of this grant are that the magnetospheric boundary layers link disparate regions of the magnetosphere together, and the global behavior of the magnetosphere can be understood only by understanding the linking mechanisms. Accordingly the present grant includes simultaneous research on the global, meso-, and micro-scale physics of the magnetosphere and its boundary layers. These boundary layers include the bow shock, magnetosheath, the plasma sheet boundary layer, and the ionosphere. Analytic, numerical and simulation projects have been performed on these subjects, as well as comparison of theoretical results with observational data. Very good progress has been made, with four papers published or in press and two additional papers submitted for publication during the six month period 1 June - 30 November 1993. At least two projects are currently being written up. In addition, members of the group have given papers at scientific meetings. The further structure of this report is as follows: section two contains brief accounts of research completed during the last six months, while section three describes the research projects intended for the grant's final period.

  17. Boundary current-controlled turbidite deposition: A sedimentation model for the Southern Nares Abyssal Plain, Western North Atlantic

    NASA Astrophysics Data System (ADS)

    Kuijpers, A.; Duin, E. J. Th.

    1986-03-01

    Examination of 38 sediment cores, bottom photographs, 7,000 km of 3.5 kHz reflection profiles and other seismic data from the southern part of the Nares Abyssal Plain suggests that complex sedimentary patterns and high sedimentation rates can be largely attributed to effects of a deep boundary current flowing eastward along the north flank of the Greater Antilles Outer Ridge. It is concluded that the areal dispersal pattern of turbidites on the plain results mainly from Quaternary climatically-induced fluctuations of the boundary current intensity.

  18. Boundary conditions and formation of pure spin currents in magnetic field

    NASA Astrophysics Data System (ADS)

    Eliashvili, Merab; Tsitsishvili, George

    2017-09-01

    Schrödinger equation for an electron confined to a two-dimensional strip is considered in the presence of homogeneous orthogonal magnetic field. Since the system has edges, the eigenvalue problem is supplied by the boundary conditions (BC) aimed in preventing the leakage of matter away across the edges. In the case of spinless electrons the Dirichlet and Neumann BC are considered. The Dirichlet BC result in the existence of charge carrying edge states. For the Neumann BC each separate edge comprises two counterflow sub-currents which precisely cancel out each other provided the system is populated by electrons up to certain Fermi level. Cancelation of electric current is a good starting point for developing the spin-effects. In this scope we reconsider the problem for a spinning electron with Rashba coupling. The Neumann BC are replaced by Robin BC. Again, the two counterflow electric sub-currents cancel out each other for a separate edge, while the spin current survives thus modeling what is known as pure spin current - spin flow without charge flow.

  19. The Effects of Grain Boundaries on the Current Transport Properties in YBCO-Coated Conductors

    NASA Astrophysics Data System (ADS)

    Yang, Chao; Xia, Yudong; Xue, Yan; Zhang, Fei; Tao, Bowan; Xiong, Jie

    2015-10-01

    We report a detailed study of the grain orientations and grain boundary (GB) networks in Y2O3 films grown on Ni-5 at.%W substrates. Electron back scatter diffraction (EBSD) exhibited different GB misorientation angle distributions, strongly decided by Y2O3 films with different textures. The subsequent yttria-stabilized zirconia (YSZ) barrier and CeO2 cap layer were deposited on Y2O3 layers by radio frequency sputtering, and YBa2Cu3O7-δ (YBCO) films were deposited by pulsed laser deposition. For explicating the effects of the grain boundaries on the current carry capacity of YBCO films, a percolation model was proposed to calculate the critical current density ( J c) which depended on different GB misorientation angle distributions. The significantly higher J c for the sample with sharper texture is believed to be attributed to improved GB misorientation angle distributions.

  20. Net-phytoplankton communities in the Western Boundary Currents and their environmental correlations

    NASA Astrophysics Data System (ADS)

    Chen, Yunyan; Sun, Xiaoxia; Zhun, Mingliang

    2018-03-01

    This study investigated net-phytoplankton biomass, species composition, the phytoplankton abundance horizontal distribution, and the correlations between net-phytoplankton communities and mesoscale structure that were derived from the net samples taken from the Western Boundary Currents during summer, 2014. A total of 199 phytoplankton species belonging to 61 genera in four phyla were identified. The dominant species included Climacodium frauenfeldianum, Thalassiothrix longissima, Rhizosolenia styliformis var. styliformis, Pyrocystis noctiluca, Ceratium trichoceros, and Trichodesmium thiebautii. Four phytoplankton communities were divided by cluster analysis and the clusters were mainly associated with the North Equatorial Counter Current (NECC), the North Equatorial Current (NEC), the Subtropical Counter Current (STCC), and the Luzon Current (LC), respectively. The lowest phytoplankton cell abundance and the highest Trichodesmium filament abundance were recorded in the STCC region. The principal component analysis showed that T. thiebautii preferred warm and nutrient poor water. There was also an increase in phytoplankton abundance and biomass near 5°N in the NECC region, where they benefit from upwellings and eddies.

  1. Subauroral polarization stream on the outer boundary of the ring current during an energetic ion injection event

    NASA Astrophysics Data System (ADS)

    Yuan, Zhigang; Qiao, Zheng; Li, Haimeng; Huang, Shiyong; Wang, Dedong; Yu, Xiongdong; Yu, Tao

    2017-04-01

    Subauroral polarization stream (SAPS) electric field can play an important role in the coupling between the inner magnetosphere and ionosphere; however, the production mechanism of SAPS has not been yet solved. During an energetic ion injection event on 26 March 2004, at latitudes lower than the equatorward boundaries of precipitating plasma sheet electrons and ions, the Defense Meteorological Satellite Program (DMSP) F13 satellite simultaneously observed a strong SAPS with the peak velocity of 1294 m/s and downward flowing field-aligned currents (FACs). Conjugate observations of DMSP F13 and NOAA 15 satellites have shown that FACs flowing into the ionosphere just lie in the outer boundary of the ring current (RC). The downward flowing FACs were observed in a region of positive latitudinal gradients of the ion energy density, implying that the downward flowing FACs are more likely linked to the azimuthal gradient than the radial gradient of the RC ion pressure. Our result demonstrates that RC ion pressure gradients on the outer boundary of the RC in the evening sector during energetic ion injection events can lead to downward flowing FACs so as to cause strong SAPS in condition of low ionospheric conductivities.Plain Language SummaryThis paper provides a good case that the SAPS and FAC occurred in the outer <span class="hlt">boundary</span> of the ring <span class="hlt">current</span> during an energetic ion injection event. Our result demonstrates that RC ion pressure gradients on the outer <span class="hlt">boundary</span> of the RC in the evening sector during energetic ion injection events can lead to downward flowing FACs so as to cause strong SAPS in condition of low ionospheric conductivities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003AIPC..669..561H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003AIPC..669..561H"><span>Constructing Integrable Full-pressure Full-<span class="hlt">current</span> Free-<span class="hlt">boundary</span> Stellarator Magnetohydrodynamic Equilibria</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hudson, S. R.; Monticello, D. A.; Reiman, A. H.; Strickler, D. J.; Hirshman, S. P.</p> <p>2003-06-01</p> <p>For the (non-axisymmetric) stellarator class of plasma confinement devices to be feasible candidates for fusion power stations it is essential that, to a good approximation, the magnetic field lines lie on nested flux surfaces; however, the inherent lack of a continuous symmetry implies that magnetic islands are guaranteed to exist. Magnetic islands break the smooth topology of nested flux surfaces and chaotic field lines result when magnetic islands overlap. An analogous case occurs with 11/2-dimension Hamiltonian systems where resonant perturbations cause singularities in the transformation to action-angle coordinates and destroy integrability. The suppression of magnetic islands is a critical issue for stellarator design, particularly for small aspect ratio devices. Techniques for `healing' vacuum fields and fixed-<span class="hlt">boundary</span> plasma equilibria have been developed, but what is ultimately required is a procedure for designing stellarators such that the self-consistent plasma equilibrium <span class="hlt">currents</span> and the coil <span class="hlt">currents</span> combine to produce an integrable magnetic field, and such a procedure is presented here for the first time. Magnetic islands in free-<span class="hlt">boundary</span> full-pressure full-<span class="hlt">current</span> stellarator magnetohydrodynamic equilibria are suppressed using a procedure based on the Princeton Iterative Equilibrium Solver [A.H.Reiman & H.S.Greenside, Comp. Phys. Comm., 43:157, 1986.] which iterates the equilibrium equations to obtain the plasma equilibrium. At each iteration, changes to a Fourier representation of the coil geometry are made to cancel resonant fields produced by the plasma. As the iterations continue, the coil geometry and the plasma simultaneously converge to an equilibrium in which the island content is negligible. The method is applied to a candidate plasma and coil design for the National Compact Stellarator eXperiment [G.H.Neilson et.al., Phys. Plas., 7:1911, 2000.].</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFMOS41B..05D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFMOS41B..05D"><span>Gliders Measure Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> Transport from the South Pacific to the Equator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Davis, R. E.; Kessler, W. S.; Sherman, J. T.</p> <p>2011-12-01</p> <p>Since 2007, the Consortium on the Ocean's Role in Climate (CORC) has used repeated glider transects across the southern Solomon Sea to measure the previously nearly unsampled mass and heat transport from the South Pacific to the equatorial zone. Mean transport is dominated by the New Guinea Coastal Undercurrent (NGCUC). This low-latitude western <span class="hlt">boundary</span> <span class="hlt">current</span> is a major element of the shallow meridional overturning circulation, returning water from the subtropical South Pacific to the Equatorial Undercurrent (EUC) where it upwells. We find the mean NGCUC to be a jet less than 100 km wide, centered near 300 m depth, with equatorward velocities reaching 35 cm/s and salinity anomalies on isopycnals up to 0.05. Weaker poleward flow is found near the surface in the eastern basin. Equatorward transport above 700 m is typically 20 Sv, but nearly vanished during two La Niñas and reached 25 Sv during an El Niño. Within these events the seasonal cycle cannot yet be defined. Transport variability is strongest outside the <span class="hlt">boundary</span> <span class="hlt">current</span> and appears to consist of two independently moving layers with a <span class="hlt">boundary</span> near 250 m. ENSO variability is predominantly in the upper layer. The relation of Solomon Sea mass and heat transport with ENSO indicators will be discussed The ability to initiate and maintain measurements that support such quantitative analyses with a small effort in a remote site far from research institutions demonstrates that gliders can be a productive part of the global ocean observing system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/940164','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/940164"><span>A QR accelerated volume-to-surface <span class="hlt">boundary</span> condition for finite element solution of eddy <span class="hlt">current</span> problems</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>White, D; Fasenfest, B; Rieben, R</p> <p>2006-09-08</p> <p>We are concerned with the solution of time-dependent electromagnetic eddy <span class="hlt">current</span> problems using a finite element formulation on three-dimensional unstructured meshes. We allow for multiple conducting regions, and our goal is to develop an efficient computational method that does not require a computational mesh of the air/vacuum regions. This requires a sophisticated global <span class="hlt">boundary</span> condition specifying the total fields on the conductor <span class="hlt">boundaries</span>. We propose a Biot-Savart law based volume-to-surface <span class="hlt">boundary</span> condition to meet this requirement. This Biot-Savart approach is demonstrated to be very accurate. In addition, this approach can be accelerated via a low-rank QR approximation of the discretizedmore » Biot-Savart law.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1323555','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1323555"><span>The Role of Grain <span class="hlt">Boundary</span> Energy on Grain <span class="hlt">Boundary</span> Complexion Transitions</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>Bojarski, Stephanie A.; Rohrer, Gregory S.</p> <p></p> <p>Grain <span class="hlt">boundary</span> complexions are distinct equilibrium structures and compositions of a grain <span class="hlt">boundary</span> and complexion transformations are transition from a metastable to an equilibrium complexion at a specific thermodynamic and geometric conditions. Previous work indicates that, in the case of doped alumina, a complexion transition that increased the mobility of transformed <span class="hlt">boundaries</span> and resulted in abnormal grain growth also caused a decrease in the mean relative grain <span class="hlt">boundary</span> energy as well as an increase in the anisotropy of the grain <span class="hlt">boundary</span> character distribution (GBCD). The <span class="hlt">current</span> work will investigate the hypothesis that the rates of complexion transitions that result inmore » abnormal grain growth (AGG) depend on grain <span class="hlt">boundary</span> character and energy. Furthermore, the <span class="hlt">current</span> work expands upon this understanding and tests the hypothesis that it is possible to control when and where a complexion transition occurs by controlling the local grain <span class="hlt">boundary</span> energy distribution.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JAP...117d5311M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JAP...117d5311M"><span>The role of <span class="hlt">boundary</span> variability in polycrystalline grain-<span class="hlt">boundary</span> diffusion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moghadam, M. M.; Rickman, J. M.; Harmer, M. P.; Chan, H. M.</p> <p>2015-01-01</p> <p>We investigate the impact of grain-<span class="hlt">boundary</span> variability on mass transport in a polycrystal. More specifically, we perform both numerical and analytical studies of steady-state diffusion in prototypical microstructures in which there is either a discrete spectrum of grain-<span class="hlt">boundary</span> activation energies or else a complex distribution of grain-<span class="hlt">boundary</span> character, and hence a continuous spectrum of <span class="hlt">boundary</span> activation energies. An effective diffusivity is calculated for these structures using simplified multi-state models and, for the case of a continuous spectrum, employing experimentally obtained grain-<span class="hlt">boundary</span> energy data. We identify different diffusive regimes for these cases and quantify deviations from Arrhenius behavior using effective medium theory. <span class="hlt">Finally</span>, we examine the diffusion kinetics of a simplified model of an interfacial layering (i.e., complexion) transition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994PrOce..33..249S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994PrOce..33..249S"><span><span class="hlt">Boundary</span> <span class="hlt">current</span> instabilities, upwelling, shelf mixing and eutrophication processes in the Black Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sur, Hali˙l. İ.; Özsoy, Emi˙n.; Ünlüata, Ümi˙t.</p> <p></p> <p>Satellite and in situ data are utilized to investigate the mesoscale dynamics of the Black Sea <span class="hlt">boundary</span> <span class="hlt">current</span> system with special emphasis on aspects of transport and productivity. The satellite data are especially helpful in capturing rapid sub-mesoscale motions insufficiently resolved by the in situ measurements. Various forms of isolated features, including dipole eddies and river plumes, are identified in the satellite images. Unstable flow structures at these sites appear to transport materials and momentum across the continental shelf. Species differentiation and competition are evident along the <span class="hlt">boundary</span> <span class="hlt">current</span> system and at the frontal regions during the development of early summer productivity. A time series of Coastal Zone Colour Scanner (CZCS) images indicate dynamical modulation of the springtime surface productivity in the southern Black Sea. Unstable meandering motions generated at Sakarya Canyon propagate east with speeds of ∼10-15 km d -1. Within weeks, a turbulent jet is created which separates from the coast, covering the entire southwestern sector. The nutrients driving the phytoplankton production (mainly Emiliana huxleyi) of the <span class="hlt">current</span> system evidently originate from fluvial discharge entering from the northwestern region including the Danube river. The productivity pattern develops in early summer when the Danube inflow is at its peak, and through meandering motions spreads into an area several times wider than the continental shelf. In 1980, the CZCS data, and in 1991 and 1992, the Advanced Very High Resolution Radiometer (AVHRR) data indicate patches of upwelling along the west Anatolian coastline between Sakarya Canyon and Cape İnce ( Ince Burun) in summer. The upwelling phenomenon is outstanding because it occurs on a coast where normally the surface convergence near the coast implies downwelling, and under conditions of unfavorable winds. In 1992, the hydrographic data indicated the upwelling to be the result of a surface</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018DSRI..136...91S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018DSRI..136...91S"><span>Signature of Indian Ocean Dipole on the western <span class="hlt">boundary</span> <span class="hlt">current</span> of the Bay of Bengal</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sherin, V. R.; Durand, F.; Gopalkrishna, V. V.; Anuvinda, S.; Chaitanya, A. V. S.; Bourdallé-Badie, R.; Papa, F.</p> <p>2018-06-01</p> <p>This study uses an unprecedented collection of 27 years of repeated eXpendable Bathy Thermograph (XBT) sections crossing the western and north-western <span class="hlt">boundaries</span> of the Bay of Bengal (BoB). Our objective is to analyse the variability of the <span class="hlt">boundary</span> <span class="hlt">current</span> that flows there, known as the East India Coastal <span class="hlt">Current</span> (EICC). In the western BoB, in line with the past observational and modelling studies, our dataset confirms that the EICC seasonally flows poleward from February to July (with a peak transport of 5 Sv), then decays and reverses to equatorward towards the equator from October to December (with a peak transport of 3 Sv), reversing again to poleward in December. In the north-western BoB, the seasonal EICC prominently flows north-eastward, with a peak transport of 7 Sv in March. Over the rest of the climatological year, the transport remains north-westward and weak (of order 2 Sv at most). Beyond the seasonal climatology, the timespan of our dataset allows us to put a special emphasis on the departures from the seasonal cycle of the EICC velocity and transport. It is observed that this non-seasonal variability is actually larger than the seasonal climatology, so that the seasonal cycle may be completely distorted in any given year. This is true in the western <span class="hlt">boundary</span> region as well as further offshore in the central BoB and concerns the surface as well as the subsurface layers. Indian Ocean Dipole (IOD) events influence EICC variability, supposedly through remote forcing from the equatorial Indian Ocean and generate northward (southward) anomalous transport typically reaching 5 Sv (7 Sv) in winter during positive (negative) IOD events. In addition to IOD events, most of the variability observed at inter-annual timescales seems to be driven by ocean turbulence. A comparison of our observed <span class="hlt">current</span> with a suite of state-of-the-art ocean reanalyses and model products (SODA, ORAS4, MERCATOR-ORCA12) confirms this hypothesis, with non-eddy resolving models</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PPCF...59l4003M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PPCF...59l4003M"><span>The turbulent plasmasphere <span class="hlt">boundary</span> layer and the outer radiation belt <span class="hlt">boundary</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mishin, Evgeny; Sotnikov, Vladimir</p> <p>2017-12-01</p> <p>We report on observations of enhanced plasma turbulence and hot particle distributions in the plasmasphere <span class="hlt">boundary</span> layer formed by reconnection-injected hot plasma jets entering the plasmasphere. The data confirm that the electron pressure peak is formed just outward of the plasmapause in the premidnight sector. Free energy for plasma wave excitation comes from diamagnetic ion <span class="hlt">currents</span> near the inner edge of the <span class="hlt">boundary</span> layer due to the ion pressure gradient, electron diamagnetic <span class="hlt">currents</span> in the entry layer near the electron plasma sheet <span class="hlt">boundary</span>, and anisotropic (sometimes ring-like) ion distributions revealed inside, and further inward of, the inner <span class="hlt">boundary</span>. We also show that nonlinear parametric coupling between lower oblique resonance and fast magnetosonic waves significantly contributes to the VLF whistler wave spectrum in the plasmasphere <span class="hlt">boundary</span> layer. These emissions represent a distinctive subset of substorm/storm-related VLF activity in the region devoid of substorm injected tens keV electrons and could be responsible for the alteration of the outer radiation belt <span class="hlt">boundary</span> during (sub)storms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26780472','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26780472"><span>Event <span class="hlt">boundaries</span> and memory improvement.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pettijohn, Kyle A; Thompson, Alexis N; Tamplin, Andrea K; Krawietz, Sabine A; Radvansky, Gabriel A</p> <p>2016-03-01</p> <p>The structure of events can influence later memory for information that is embedded in them, with evidence indicating that event <span class="hlt">boundaries</span> can both impair and enhance memory. The <span class="hlt">current</span> study explored whether the presence of event <span class="hlt">boundaries</span> during encoding can structure information to improve memory. In Experiment 1, memory for a list of words was tested in which event structure was manipulated by having participants walk through a doorway, or not, halfway through the word list. In Experiment 2, memory for lists of words was tested in which event structure was manipulated using computer windows. <span class="hlt">Finally</span>, in Experiments 3 and 4, event structure was manipulated by having event shifts described in narrative texts. The consistent finding across all of these methods and materials was that memory was better when the information was distributed across two events rather than combined into a single event. Moreover, Experiment 4 demonstrated that increasing the number of event <span class="hlt">boundaries</span> from one to two increased the memory benefit. These results are interpreted in the context of the Event Horizon Model of event cognition. Copyright © 2015 Elsevier B.V. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1988PhFl...31.2962R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1988PhFl...31.2962R"><span>Free <span class="hlt">boundary</span> skin <span class="hlt">current</span> magnetohydrodynamic equilibria</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reusch, Michael F.</p> <p>1988-10-01</p> <p>Function theoretic methods in the complex plane are used to develop simple parametric hodograph formulas that generate sharp <span class="hlt">boundary</span> equilibria of arbitrary shape. The related method of Gorenflo [Z. Angew. Math. Phys. 16, 279 (1965)] and Merkel (Ph.D. thesis, University of Munich, 1965) is discussed. A numerical technique for the construction of solutions, based on one of the methods, is presented. A study is made of the bifurcations of an equilibrium of general form.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010080472','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010080472"><span>Representation of Clear and Cloudy <span class="hlt">Boundary</span> Layers in Climate Models. Chapter 14</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Randall, D. A.; Shao, Q.; Branson, M.</p> <p>1997-01-01</p> <p>The atmospheric general circulation models which are being used as components of climate models rely on their <span class="hlt">boundary</span> layer parameterizations to produce realistic simulations of the surface turbulent fluxes of sensible heat. moisture. and momentum: of the <span class="hlt">boundary</span>-layer depth over which these fluxes converge: of <span class="hlt">boundary</span> layer cloudiness: and of the interactions of the <span class="hlt">boundary</span> layer with the deep convective clouds that grow upwards from it. Two <span class="hlt">current</span> atmospheric general circulation models are used as examples to show how these requirements are being addressed: these are version 3 of the Community Climate Model. which has been developed at the U.S. National Center for Atmospheric Research. and the Colorado State University atmospheric general circulation model. The formulations and results of both models are discussed. <span class="hlt">Finally</span>, areas for future research are suggested.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012APS..DPPPP8068K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012APS..DPPPP8068K"><span>Effects of the <span class="hlt">current</span> <span class="hlt">boundary</span> conditions at the plasma-gun gap on density in SSPX</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kolesnikov, Roman; Lodestro, L. L.; Meyer, W. H.</p> <p>2012-10-01</p> <p>The Sustained Spheromak Physics Experiment (SSPX) was a toroidal magnetic-confinement device without toroidal magnetic-field coils or a central transformer but which generated core-plasma <span class="hlt">currents</span> by dynamo processes driven by coaxial plasma-gun injection into a flux-conserving vessel. Record electron temperatures in a spheromak (Te˜500eV) were achieved, and <span class="hlt">final</span> results of the SSPX program were reported in [1]. Plasma density, which depended strongly on wall conditions, was an important parameter in SSPX. It was observed that density rises with Igun and that confinement improved as the density was lowered. Shortly after the last experiments, a new feature was added to the Corsica code's solver used to reconstruct SSPX equilibria. Motivated by n=0 fields observed in NIMROD simulations of SSPX, an insulating <span class="hlt">boundary</span> condition was implemented at the plasma-gun gap. Using this option we will perform new reconstructions of SSPX equilibria and look for correlations between the location of the separatrix (which moves up the gun wall and onto the insulating gap as Igun increases) and plasma density and magnetic-flux amplification [2].[4pt] [1] H. S. McLean, APS, DPP, Dallas, TX, 2008.[0pt] [2] E. B. Hooper et al., Nucl. Fusion 47, 1064 (2007).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28541817','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28541817"><span>Gendered Cultural Identities: The Influences of Family and Privacy <span class="hlt">Boundaries</span>, Subjective Norms, and Stigma Beliefs on Family Health History Communication.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hong, Soo Jung</p> <p>2018-08-01</p> <p>This study investigates the effects of cultural norms on family health history (FHH) communication in the American, Chinese, and Korean cultures. More particularly, this study focuses on perceived family <span class="hlt">boundaries</span>, subjective norms, stigma beliefs, and privacy <span class="hlt">boundaries</span>, including age and gender, that affect people's FHH communication. For data analyses, hierarchical multiple regression and logistic regression methods were employed. The results indicate that participants' subjective norms, stigma beliefs, and perceived family/privacy <span class="hlt">boundaries</span> were positively associated with <span class="hlt">current</span> FHH communication. Age- and gender-related privacy <span class="hlt">boundaries</span> were negatively related to perceived privacy <span class="hlt">boundaries</span>, however. <span class="hlt">Finally</span>, the results show that gendered cultural identities have three-way interaction effects on two associations: (1) between perceived family <span class="hlt">boundaries</span> and perceived privacy <span class="hlt">boundaries</span> and (2) between perceived privacy <span class="hlt">boundaries</span> and <span class="hlt">current</span> FHH communication. The findings have meaningful implications for future cross-cultural studies on the roles of family systems, subjective norms, and stigma beliefs in FHH communication.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PPCF...60b5023P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PPCF...60b5023P"><span>Bootstrap <span class="hlt">current</span> control studies in the Wendelstein 7-X stellarator using the free-plasma-<span class="hlt">boundary</span> version of the SIESTA MHD equilibrium code</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peraza-Rodriguez, H.; Reynolds-Barredo, J. M.; Sanchez, R.; Tribaldos, V.; Geiger, J.</p> <p>2018-02-01</p> <p>The recently developed free-plasma-<span class="hlt">boundary</span> version of the SIESTA MHD equilibrium code (Hirshman et al 2011 Phys. Plasmas 18 062504; Peraza-Rodriguez et al 2017 Phys. Plasmas 24 082516) is used for the first time to study scenarios with considerable bootstrap <span class="hlt">currents</span> for the Wendelstein 7-X (W7-X) stellarator. Bootstrap <span class="hlt">currents</span> in the range of tens of kAs can lead to the formation of unwanted magnetic island chains or stochastic regions within the plasma and alter the <span class="hlt">boundary</span> rotational transform due to the small shear in W7-X. The latter issue is of relevance since the island divertor operation of W7-X relies on a proper positioning of magnetic island chains at the plasma edge to control the particle and energy exhaust towards the divertor plates. Two scenarios are examined with the new free-plasma-<span class="hlt">boundary</span> capabilities of SIESTA: a freely evolving bootstrap <span class="hlt">current</span> one that illustrates the difficulties arising from the dislocation of the <span class="hlt">boundary</span> islands, and a second one in which off-axis electron cyclotron <span class="hlt">current</span> drive (ECCD) is applied to compensate the effects of the bootstrap <span class="hlt">current</span> and keep the island divertor configuration intact. SIESTA finds that off-axis ECCD is indeed able to keep the location and phase of the edge magnetic island chain unchanged, but it may also lead to an undesired stochastization of parts of the confined plasma if the EC deposition radial profile becomes too narrow.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvE..96e2118C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvE..96e2118C"><span>Fluctuating hydrodynamics, <span class="hlt">current</span> fluctuations, and hyperuniformity in <span class="hlt">boundary</span>-driven open quantum chains</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carollo, Federico; Garrahan, Juan P.; Lesanovsky, Igor; Pérez-Espigares, Carlos</p> <p>2017-11-01</p> <p>We consider a class of either fermionic or bosonic noninteracting open quantum chains driven by dissipative interactions at the <span class="hlt">boundaries</span> and study the interplay of coherent transport and dissipative processes, such as bulk dephasing and diffusion. Starting from the microscopic formulation, we show that the dynamics on large scales can be described in terms of fluctuating hydrodynamics. This is an important simplification as it allows us to apply the methods of macroscopic fluctuation theory to compute the large deviation (LD) statistics of time-integrated <span class="hlt">currents</span>. In particular, this permits us to show that fermionic open chains display a third-order dynamical phase transition in LD functions. We show that this transition is manifested in a singular change in the structure of trajectories: while typical trajectories are diffusive, rare trajectories associated with atypical <span class="hlt">currents</span> are ballistic and hyperuniform in their spatial structure. We confirm these results by numerically simulating ensembles of rare trajectories via the cloning method, and by exact numerical diagonalization of the microscopic quantum generator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29347714','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29347714"><span>Fluctuating hydrodynamics, <span class="hlt">current</span> fluctuations, and hyperuniformity in <span class="hlt">boundary</span>-driven open quantum chains.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Carollo, Federico; Garrahan, Juan P; Lesanovsky, Igor; Pérez-Espigares, Carlos</p> <p>2017-11-01</p> <p>We consider a class of either fermionic or bosonic noninteracting open quantum chains driven by dissipative interactions at the <span class="hlt">boundaries</span> and study the interplay of coherent transport and dissipative processes, such as bulk dephasing and diffusion. Starting from the microscopic formulation, we show that the dynamics on large scales can be described in terms of fluctuating hydrodynamics. This is an important simplification as it allows us to apply the methods of macroscopic fluctuation theory to compute the large deviation (LD) statistics of time-integrated <span class="hlt">currents</span>. In particular, this permits us to show that fermionic open chains display a third-order dynamical phase transition in LD functions. We show that this transition is manifested in a singular change in the structure of trajectories: while typical trajectories are diffusive, rare trajectories associated with atypical <span class="hlt">currents</span> are ballistic and hyperuniform in their spatial structure. We confirm these results by numerically simulating ensembles of rare trajectories via the cloning method, and by exact numerical diagonalization of the microscopic quantum generator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21333913-effect-boundary-treatments-quantum-transport-current-green-function-wigner-distribution-methods-nano-scale-dg-mosfet','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21333913-effect-boundary-treatments-quantum-transport-current-green-function-wigner-distribution-methods-nano-scale-dg-mosfet"><span>Effect of <span class="hlt">boundary</span> treatments on quantum transport <span class="hlt">current</span> in the Green's function and Wigner distribution methods for a nano-scale DG-MOSFET</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>Jiang Haiyan; Department of Mathematics and Statistics, University of North Carolina at Charlotte, Charlotte, NC 28223-0001; Cai Wei</p> <p>2010-06-20</p> <p>In this paper, we conduct a study of quantum transport models for a two-dimensional nano-size double gate (DG) MOSFET using two approaches: non-equilibrium Green's function (NEGF) and Wigner distribution. Both methods are implemented in the framework of the mode space methodology where the electron confinements below the gates are pre-calculated to produce subbands along the vertical direction of the device while the transport along the horizontal channel direction is described by either approach. Each approach handles the open quantum system along the transport direction in a different manner. The NEGF treats the open <span class="hlt">boundaries</span> with <span class="hlt">boundary</span> self-energy defined by amore » Dirichlet to Neumann mapping, which ensures non-reflection at the device <span class="hlt">boundaries</span> for electron waves leaving the quantum device active region. On the other hand, the Wigner equation method imposes an inflow <span class="hlt">boundary</span> treatment for the Wigner distribution, which in contrast ensures non-reflection at the <span class="hlt">boundaries</span> for free electron waves entering the device active region. In both cases the space-charge effect is accounted for by a self-consistent coupling with a Poisson equation. Our goals are to study how the device <span class="hlt">boundaries</span> are treated in both transport models affects the <span class="hlt">current</span> calculations, and to investigate the performance of both approaches in modeling the DG-MOSFET. Numerical results show mostly consistent quantum transport characteristics of the DG-MOSFET using both methods, though with higher transport <span class="hlt">current</span> for the Wigner equation method, and also provide the <span class="hlt">current</span>-voltage (I-V) curve dependence on various physical parameters such as the gate voltage and the oxide thickness.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/5256723','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/5256723"><span>Free <span class="hlt">boundary</span> skin <span class="hlt">current</span> MHD (magnetohydrodynamic) equilibria</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>Reusch, M.F.</p> <p>1988-02-01</p> <p>Function theoretic methods in the complex plane are used to develop simple parametric hodograph formulae which generate sharp <span class="hlt">boundary</span> equilibria of arbitrary shape. The related method of Gorenflo and Merkel is discussed. A numerical technique for the construction of solutions, based on one of the methods is presented. A study is made of the bifurcations of an equilibrium of general form. 28 refs., 9 figs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSM51D2522O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSM51D2522O"><span>Field-aligned <span class="hlt">Currents</span> Induced by Electrostatic Polarization at the Ionosphere: Application to the Poleward <span class="hlt">Boundary</span> Intensification (PBI) of Auroral Emission</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ohtani, S.; Yoshikawa, A.</p> <p>2016-12-01</p> <p>Although the field-aligned <span class="hlt">currents</span> (Birkeland <span class="hlt">currents</span>) are generally considered to be driven by magnetospheric processes, it is possible that some field-aligned <span class="hlt">currents</span> are locally induced in the ionosphere in the presence of sharp conductance gradient. In this presentation we shall discuss the poleward <span class="hlt">boundary</span> intensification (PBI) of auroral emission as an example effect of such electrostatic polarization. The observations show that the PBIs are very often preceded by the fast polar cap convection approaching the nightside auroral oval. We propose that the ionospheric <span class="hlt">currents</span> driven by the associated electric field diverges/converges at the poleward <span class="hlt">boundary</span> of the auroral oval as the background ionospheric conductance changes sharply in space, and they close with field-aligned <span class="hlt">currents</span>. The associated upward field-aligned <span class="hlt">current</span> is accompanied by electron precipitation, which may cause auroral emission as observed as PBIs. We test this idea by modeling the ionosphere as a slab-shaped enhancement of conductance and the polar cap flow channel as a pair of upward and downward FACs. The results show that (i) a pair of upward and downward FACs is induced at the poleward <span class="hlt">boundary</span> when the front of the polar cap flow channel approaches the auroral oval; (ii) the upward FAC extends westward much wider in longitude than the flow channel; (iii) the peak FAC density is significantly larger than the incident FAC; and (iv) the induced upward and downward FACs are distributed almost symmetrically in longitude, indicating that the Pedersen polarization dominates the Hall polarization. These results are consistent with some general characteristics of PBIs, which are rather difficult to explain if the PBIs are the ionospheric manefestation of distant reconnection as often suggested.</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('http://adsabs.harvard.edu/abs/1994abl..book.....G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994abl..book.....G"><span>The Atmospheric <span class="hlt">Boundary</span> Layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garratt, J. R.</p> <p>1994-05-01</p> <p>A comprehensive and lucid account of the physics and dynamics of the lowest one to two kilometers of the Earth's atmosphere in direct contact with the Earth's surface, known as the atmospheric <span class="hlt">boundary</span> layer (ABL). Dr. Garratt emphasizes the application of the ABL problems to numerical modeling of the climate, which makes this book unique among recent texts on the subject. He begins with a brief introduction to the ABL before leading to the development of mean and turbulence equations and the many scaling laws and theories that are the cornerstone of any serious ABL treatment. Modeling of the ABL is crucially dependent for its realism on the surface <span class="hlt">boundary</span> conditions, so chapters four and five deal with aerodynamic and energy considerations, with attention given to both dry and wet land surfaces and the sea. The author next treats the structure of the clear-sky, thermally stratified ABL, including the convective and stable cases over homogeneous land, the marine ABL, and the internal <span class="hlt">boundary</span> layer at the coastline. Chapter seven then extends this discussion to the cloudy ABL. This is particularly relevant to <span class="hlt">current</span> research because the extensive stratocumulus regions over the subtropical oceans and stratus regions over the Arctic have been identified as key players in the climate system. In the <span class="hlt">final</span> chapters, Dr. Garratt summarizes the book's material by discussing appropriate ABL and surface parameterization schemes in general circulation models of the atmosphere that are being used for climate stimulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2834215','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2834215"><span>A VERSATILE SHARP INTERFACE IMMERSED <span class="hlt">BOUNDARY</span> METHOD FOR INCOMPRESSIBLE FLOWS WITH COMPLEX <span class="hlt">BOUNDARIES</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>Mittal, R.; Dong, H.; Bozkurttas, M.; Najjar, F.M.; Vargas, A.; von Loebbecke, A.</p> <p>2010-01-01</p> <p>A sharp interface immersed <span class="hlt">boundary</span> method for simulating incompressible viscous flow past three-dimensional immersed bodies is described. The method employs a multi-dimensional ghost-cell methodology to satisfy the <span class="hlt">boundary</span> conditions on the immersed <span class="hlt">boundary</span> and the method is designed to handle highly complex three-dimensional, stationary, moving and/or deforming bodies. The complex immersed surfaces are represented by grids consisting of unstructured triangular elements; while the flow is computed on non-uniform Cartesian grids. The paper describes the salient features of the methodology with special emphasis on the immersed <span class="hlt">boundary</span> treatment for stationary and moving <span class="hlt">boundaries</span>. Simulations of a number of canonical two- and three-dimensional flows are used to verify the accuracy and fidelity of the solver over a range of Reynolds numbers. Flow past suddenly accelerated bodies are used to validate the solver for moving <span class="hlt">boundary</span> problems. <span class="hlt">Finally</span> two cases inspired from biology with highly complex three-dimensional bodies are simulated in order to demonstrate the versatility of the method. PMID:20216919</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4357896','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4357896"><span>The relationship between grain <span class="hlt">boundary</span> structure, defect mobility, and grain <span class="hlt">boundary</span> sink efficiency</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Uberuaga, Blas Pedro; Vernon, Louis J.; Martinez, Enrique; Voter, Arthur F.</p> <p>2015-01-01</p> <p>Nanocrystalline materials have received great attention due to their potential for improved functionality and have been proposed for extreme environments where the interfaces are expected to promote radiation tolerance. However, the precise role of the interfaces in modifying defect behavior is unclear. Using long-time simulations methods, we determine the mobility of defects and defect clusters at grain <span class="hlt">boundaries</span> in Cu. We find that mobilities vary significantly with <span class="hlt">boundary</span> structure and cluster size, with larger clusters exhibiting reduced mobility, and that interface sink efficiency depends on the kinetics of defects within the interface via the in-<span class="hlt">boundary</span> annihilation rate of defects. Thus, sink efficiency is a strong function of defect mobility, which depends on <span class="hlt">boundary</span> structure, a property that evolves with time. Further, defect mobility at <span class="hlt">boundaries</span> can be slower than in the bulk, which has general implications for the properties of polycrystalline materials. <span class="hlt">Finally</span>, we correlate defect energetics with the volumes of atomic sites at the <span class="hlt">boundary</span>. PMID:25766999</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1190482-relationship-between-grain-boundary-structure-defect-mobility-grain-boundary-sink-efficiency','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1190482-relationship-between-grain-boundary-structure-defect-mobility-grain-boundary-sink-efficiency"><span>The relationship between grain <span class="hlt">boundary</span> structure, defect mobility, and grain <span class="hlt">boundary</span> sink efficiency</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Uberuaga, Blas Pedro; Vernon, Louis J.; Martinez, Enrique; ...</p> <p>2015-03-13</p> <p>Nanocrystalline materials have received great attention due to their potential for improved functionality and have been proposed for extreme environments where the interfaces are expected to promote radiation tolerance. However, the precise role of the interfaces in modifying defect behavior is unclear. Using long-time simulations methods, we determine the mobility of defects and defect clusters at grain <span class="hlt">boundaries</span> in Cu. We find that mobilities vary significantly with <span class="hlt">boundary</span> structure and cluster size, with larger clusters exhibiting reduced mobility, and that interface sink efficiency depends on the kinetics of defects within the interface via the in-<span class="hlt">boundary</span> annihilation rate of defects. Thus,more » sink efficiency is a strong function of defect mobility, which depends on <span class="hlt">boundary</span> structure, a property that evolves with time. Further, defect mobility at <span class="hlt">boundaries</span> can be slower than in the bulk, which has general implications for the properties of polycrystalline materials. <span class="hlt">Finally</span>, we correlate defect energetics with the volumes of atomic sites at the <span class="hlt">boundary</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA297513','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA297513"><span>Mithras Studies of the <span class="hlt">Boundary</span> Between Open and Closed Field Lines.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1994-01-31</p> <p>I ¸ . . A- : - <span class="hlt">Final</span> Report • March 1995 MITHRAS STUDIES OF THE <span class="hlt">BOUNDARY</span> BETWEEN OPEN AND CLOSED FIELD LINES John D. Kelly, Program Manager Richard A...Kelly, Program Manager Richard A. Doe, Research Physicist Geoscience and Engineering Center SRI Project 3245 Prepared for: Department of the Air...characteristic energy, energy flux, and an estimate for upward field-aligned <span class="hlt">current</span>. On the basis of coordinated radar/optical experiments, Vallance Jones et al</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JHEP...09..146L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JHEP...09..146L"><span>Holographic heat <span class="hlt">current</span> as Noether <span class="hlt">current</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Hai-Shan; Lü, H.; Pope, C. N.</p> <p>2017-09-01</p> <p>We employ the Noether procedure to derive a general formula for the radially conserved heat <span class="hlt">current</span> in AdS planar black holes with certain transverse and traceless perturbations, for a general class of gravity theories. For Einstein gravity, the general higher-order Lovelock gravities and also a class of Horndeski gravities, we derive the <span class="hlt">boundary</span> stress tensor and show that the resulting <span class="hlt">boundary</span> heat <span class="hlt">current</span> matches precisely the bulk Noether <span class="hlt">current</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25300341','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25300341"><span>The coordination of <span class="hlt">boundary</span> tones and its interaction with prominence.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Katsika, Argyro; Krivokapić, Jelena; Mooshammer, Christine; Tiede, Mark; Goldstein, Louis</p> <p>2014-05-01</p> <p>This study investigates the coordination of <span class="hlt">boundary</span> tones as a function of stress and pitch accent. <span class="hlt">Boundary</span> tone coordination has not been experimentally investigated previously, and the effect of prominence on this coordination, and whether it is lexical (stress-driven) or phrasal (pitch accent-driven) in nature is unclear. We assess these issues using a variety of syntactic constructions to elicit different <span class="hlt">boundary</span> tones in an Electromagnetic Articulography (EMA) study of Greek. The results indicate that the onset of <span class="hlt">boundary</span> tones co-occurs with the articulatory target of the <span class="hlt">final</span> vowel. This timing is further modified by stress, but not by pitch accent: <span class="hlt">boundary</span> tones are initiated earlier in words with non-<span class="hlt">final</span> stress than in words with <span class="hlt">final</span> stress regardless of accentual status. Visual data inspection reveals that phrase-<span class="hlt">final</span> words are followed by acoustic pauses during which specific articulatory postures occur. Additional analyses show that these postures reach their achievement point at a stable temporal distance from <span class="hlt">boundary</span> tone onsets regardless of stress position. Based on these results and parallel findings on <span class="hlt">boundary</span> lengthening reported elsewhere, a novel approach to prosody is proposed within the context of Articulatory Phonology: rather than seeing prosodic (lexical and phrasal) events as independent entities, a set of coordination relations between them is suggested. The implications of this account for prosodic architecture are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSM52A..05O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSM52A..05O"><span>The Poleward <span class="hlt">Boundary</span> Intensification (PBI) of Auroral Emission: Its Dynamics and Associated Field-aligned <span class="hlt">Current</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>Ohtani, S.; Motoba, T.; Gjerloev, J. W.</p> <p>2016-12-01</p> <p>The poleward <span class="hlt">boundary</span> intensification (PBI) of aurora emission is often addressed in terms of distant reconnection. Recently, however, Ohtani and Yoshikawa [2016] proposed that the PBIs, at least at the initial stage of their formation, are actually the effect of ionospheric polarization in the presence of the enhanced convection in the polar cap and conductance gradient at the poleward <span class="hlt">boundary</span> of the auroral oval. Whereas the ionospheric polarization itself is a transient process, it is known that the PBIs occasionally extend longitudinally suggesting that a 3D <span class="hlt">current</span> system forms subsequently, which electrodynamically couples the magnetosphere and ionosphere. In the present study we observationally examine the associated field-aligned <span class="hlt">current</span> (FAC) observed by the SWARM satellites and compare its characteristics with ground all-sky images. It is found that complex signatures of FACs as suggested by magnetic disturbances reflect the spatial structure of aurora (e.g., location and orientation), whereas the overall motion of PBIs is well explained in terms of the background convection suggested by the FAC distribution. We shall discuss the implications of these results for the responsible evolution process of the PBIs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4185973','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4185973"><span>The coordination of <span class="hlt">boundary</span> tones and its interaction with prominence1</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Katsika, Argyro; Krivokapić, Jelena; Mooshammer, Christine; Tiede, Mark; Goldstein, Louis</p> <p>2014-01-01</p> <p>This study investigates the coordination of <span class="hlt">boundary</span> tones as a function of stress and pitch accent. <span class="hlt">Boundary</span> tone coordination has not been experimentally investigated previously, and the effect of prominence on this coordination, and whether it is lexical (stress-driven) or phrasal (pitch accent-driven) in nature is unclear. We assess these issues using a variety of syntactic constructions to elicit different <span class="hlt">boundary</span> tones in an Electromagnetic Articulography (EMA) study of Greek. The results indicate that the onset of <span class="hlt">boundary</span> tones co-occurs with the articulatory target of the <span class="hlt">final</span> vowel. This timing is further modified by stress, but not by pitch accent: <span class="hlt">boundary</span> tones are initiated earlier in words with non-<span class="hlt">final</span> stress than in words with <span class="hlt">final</span> stress regardless of accentual status. Visual data inspection reveals that phrase-<span class="hlt">final</span> words are followed by acoustic pauses during which specific articulatory postures occur. Additional analyses show that these postures reach their achievement point at a stable temporal distance from <span class="hlt">boundary</span> tone onsets regardless of stress position. Based on these results and parallel findings on <span class="hlt">boundary</span> lengthening reported elsewhere, a novel approach to prosody is proposed within the context of Articulatory Phonology: rather than seeing prosodic (lexical and phrasal) events as independent entities, a set of coordination relations between them is suggested. The implications of this account for prosodic architecture are discussed. PMID:25300341</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1019754','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1019754"><span>Towards Natural Transition in Compressible <span class="hlt">Boundary</span> Layers</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2016-06-29</p> <p>AFRL-AFOSR-CL-TR-2016-0011 Towards natural transition in compressible <span class="hlt">boundary</span> layers Marcello Faraco de Medeiros FUNDACAO PARA O INCREMENTO DA...to 29-03-2016 Towards natural transition in compressible <span class="hlt">boundary</span> layers FA9550-11-1-0354 Marcello A. Faraco de Medeiros Germán Andrés Gaviria...unlimited. 109 <span class="hlt">Final</span> report Towards natural transition in compressible <span class="hlt">boundary</span> layers Principal Investigator: Marcello Augusto Faraco de Medeiros</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880052817&hterms=beans&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dbeans','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880052817&hterms=beans&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dbeans"><span>Simulation of electrostatic turbulence in the plasma sheet <span class="hlt">boundary</span> layer with electron <span class="hlt">currents</span> and bean-shaped ion beams</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nishikawa, K.-I.; Frank, L. A.; Huang, C. Y.</p> <p>1988-01-01</p> <p>Plasma data from ISEE-1 show the presence of electron <span class="hlt">currents</span> as well as energetic ion beams in the plasma sheet <span class="hlt">boundary</span> layer. Broadband electrostatic noise and low-frequency electromagnetic bursts are detected in the plasma sheet <span class="hlt">boundary</span> layer, especially in the presence of strong ion flows, <span class="hlt">currents</span>, and steep spacial gradients in the fluxes of few-keV electrons and ions. Particle simulations have been performed to investigate electrostatic turbulence driven by a cold electron beam and/or ion beams with a bean-shaped velocity distribution. The simulation results show that the counterstreaming ion beams as well as the counterstreaming of the cold electron beam and the ion beam excite ion acoustic waves with a given Doppler-shifted real frequency. However, the effect of the bean-shaped ion velocity distributions reduces the growth rates of ion acoustic instability. The simulation results also show that the slowing down of the ion bean is larger at the larger perpendicular velocity. The wave spectra of the electric fields at some points of the simulations show turbulence generated by growing waves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19840055604&hterms=scanning+electron+microscope&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dscanning%2Belectron%2Bmicroscope','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19840055604&hterms=scanning+electron+microscope&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dscanning%2Belectron%2Bmicroscope"><span>Analysis of the electron-beam-induced <span class="hlt">current</span> of a polycrystalline p-n junction when the diffusion lengths of the material on either side of a grain <span class="hlt">boundary</span> differ</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Von Roos, O.; Luke, K. L.</p> <p>1984-01-01</p> <p>The short circuit <span class="hlt">current</span> generated by the electron beam of a scanning electron microscope in p-n junctions is reduced by enhanced recombination at grain <span class="hlt">boundaries</span> in polycrystalline material. Frequently, grain <span class="hlt">boundaries</span> separate the semiconductor into regions possessing different minority carrier life times. This markedly affects the short circuit <span class="hlt">current</span> I(sc) as a function of scanning distance from the grain <span class="hlt">boundary</span>. It will be shown theoretically that (1) the minimum of the I(sc) in crossing the grain <span class="hlt">boundary</span> with the scanning electron beam is shifted away from the grain <span class="hlt">boundary</span> toward the region with smaller life time (shorter diffusion length), (2) the magnitude of the minimum differs markedly from those calculated under the assumption of equal diffusion lengths on either side of the grain <span class="hlt">boundary</span>, and (3) the minimum disappears altogether for small surface recombination velocities (s less than 10,000 cm/s). These effects become negligible, however, for large recombination velocities s at grain <span class="hlt">boundaries</span>. For p-type silicon this happens for s not less than 100,000 cm/s.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2013-04-08/pdf/2013-08030.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2013-04-08/pdf/2013-08030.pdf"><span>78 FR 20796 - Data Specifications for Collecting Study Area <span class="hlt">Boundaries</span></span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2013-04-08</p> <p>... Specifications for Collecting Study Area <span class="hlt">Boundaries</span> AGENCY: Federal Communications Commission. ACTION: <span class="hlt">Final</span> rule... for collecting study area <span class="hlt">boundaries</span> for purposes of implementing various reforms. The original... and Order, (Study Area <span class="hlt">Boundary</span> Order), released on November 6, 2012. DATES: Effective April 8, 2013...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA192272','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA192272"><span>Prediction of Continental Shelf Sediment Transport Using a Theoretical Model of the Wave-<span class="hlt">Current</span> <span class="hlt">Boundary</span> Layer.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1987-08-01</p> <p>to Ron Smith for not giving up on me; to Doug Toomey - for lots of music ; to Betsy Welsh for always questioning the assumptions; to Dave ".,-,k...limited degree, sediments on the frictional drag on <span class="hlt">currents</span>. In this dissertation, available models of <span class="hlt">boundary</span> shear stress, sediment entrainment ...Geophys. and Space Phys.,21, 5, 1181-1192. Nowell, A. R. M., P. A. Jumars and J. E. Eckman, 1981. Effects of biological activity on the entrainment of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170003265&hterms=layer&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dlayer','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170003265&hterms=layer&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dlayer"><span>Transient, Small-Scale Field-Aligned <span class="hlt">Currents</span> in the Plasma Sheet <span class="hlt">Boundary</span> Layer During Storm Time Substorms</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nakamura, R.; Sergeev, V. A.; Baumjohann, W.; Plaschke, F.; Magnes, W.; Fischer, D.; Varsani, A.; Schmid, D.; Nakamura, T. K. M.; Russell, C. T.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170003265'); toggleEditAbsImage('author_20170003265_show'); toggleEditAbsImage('author_20170003265_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170003265_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170003265_hide"></p> <p>2016-01-01</p> <p>We report on field-aligned <span class="hlt">current</span> observations by the four Magnetospheric Multiscale (MMS) spacecraft near the plasma sheet <span class="hlt">boundary</span> layer (PSBL) during two major substorms on 23 June 2015. Small-scale field-aligned <span class="hlt">currents</span> were found embedded in fluctuating PSBL flux tubes near the Separatrix region. We resolve, for the first time, short-lived earthward (downward) intense field-aligned <span class="hlt">current</span> sheets with thicknesses of a few tens of kilometers, which are well below the ion scale, on flux tubes moving equatorward earth ward during outward plasma sheet expansion. They coincide with upward field-aligned electron beams with energies of a few hundred eV. These electrons are most likely due to acceleration associated with a reconnection jet or high-energy ion beam-produced disturbances. The observations highlight coupling of multiscale processes in PSBL as a consequence of magnetotail reconnection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27867235','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27867235"><span>Transient, small-scale field-aligned <span class="hlt">currents</span> in the plasma sheet <span class="hlt">boundary</span> layer during storm time substorms.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nakamura, R; Sergeev, V A; Baumjohann, W; Plaschke, F; Magnes, W; Fischer, D; Varsani, A; Schmid, D; Nakamura, T K M; Russell, C T; Strangeway, R J; Leinweber, H K; Le, G; Bromund, K R; Pollock, C J; Giles, B L; Dorelli, J C; Gershman, D J; Paterson, W; Avanov, L A; Fuselier, S A; Genestreti, K; Burch, J L; Torbert, R B; Chutter, M; Argall, M R; Anderson, B J; Lindqvist, P-A; Marklund, G T; Khotyaintsev, Y V; Mauk, B H; Cohen, I J; Baker, D N; Jaynes, A N; Ergun, R E; Singer, H J; Slavin, J A; Kepko, E L; Moore, T E; Lavraud, B; Coffey, V; Saito, Y</p> <p>2016-05-28</p> <p>We report on field-aligned <span class="hlt">current</span> observations by the four Magnetospheric Multiscale (MMS) spacecraft near the plasma sheet <span class="hlt">boundary</span> layer (PSBL) during two major substorms on 23 June 2015. Small-scale field-aligned <span class="hlt">currents</span> were found embedded in fluctuating PSBL flux tubes near the separatrix region. We resolve, for the first time, short-lived earthward (downward) intense field-aligned <span class="hlt">current</span> sheets with thicknesses of a few tens of kilometers, which are well below the ion scale, on flux tubes moving equatorward/earthward during outward plasma sheet expansion. They coincide with upward field-aligned electron beams with energies of a few hundred eV. These electrons are most likely due to acceleration associated with a reconnection jet or high-energy ion beam-produced disturbances. The observations highlight coupling of multiscale processes in PSBL as a consequence of magnetotail reconnection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhPl...18f2503Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhPl...18f2503Z"><span>Edge plasma <span class="hlt">boundary</span> layer generated by kink modes in tokamaks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zakharov, Leonid E.</p> <p>2011-06-01</p> <p>This paper describes the structure of the electric <span class="hlt">current</span> generated by external wall touching and free <span class="hlt">boundary</span> kink modes at the plasma edge using the ideally conducting plasma model. Both kinds of modes generate δ-functional surface <span class="hlt">current</span> at the plasma edge. Free <span class="hlt">boundary</span> kink modes also perturb the core plasma <span class="hlt">current</span>, which in the plasma edge compensates the difference between the δ-functional surface <span class="hlt">currents</span> of free <span class="hlt">boundary</span> and wall touching kink modes. In addition, the resolution of an apparent paradox with the pressure balance across the plasma <span class="hlt">boundary</span> in the presence of the surface <span class="hlt">currents</span> is provided.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25491363','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25491363"><span>Intensified diapycnal mixing in the midlatitude western <span class="hlt">boundary</span> <span class="hlt">currents</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jing, Zhao; Wu, Lixin</p> <p>2014-12-10</p> <p>The wind work on oceanic near-inertial motions is suggested to play an important role in furnishing the diapycnal mixing in the deep ocean which affects the uptake of heat and carbon by the ocean as well as climate changes. However, it remains a puzzle where and through which route the near-inertial energy penetrates into the deep ocean. Using the measurements collected in the Kuroshio extension region during January 2005, we demonstrate that the diapycnal mixing in the thermocline and deep ocean is tightly related to the shear variance of wind-generated near-inertial internal waves with the diapycnal diffusivity 6 × 10(-5) m(2)s(-1) almost an order stronger than that observed in the circulation gyre. It is estimated that 45%-62% of the local near-inertial wind work 4.5 × 10(-3) Wm(-2) radiates into the thermocline and deep ocean and accounts for 42%-58% of the energy required to furnish mixing there. The elevated mixing is suggested to be maintained by the energetic near-inertial wind work and strong eddy activities causing enhanced downward near-inertial energy flux than earlier findings. The western <span class="hlt">boundary</span> <span class="hlt">current</span> turns out to be a key region for the penetration of near-inertial energy into the deep ocean and a hotspot for the diapycnal mixing in winter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4261176','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4261176"><span>Intensified Diapycnal Mixing in the Midlatitude Western <span class="hlt">Boundary</span> <span class="hlt">Currents</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>Jing, Zhao; Wu, Lixin</p> <p>2014-01-01</p> <p>The wind work on oceanic near-inertial motions is suggested to play an important role in furnishing the diapycnal mixing in the deep ocean which affects the uptake of heat and carbon by the ocean as well as climate changes. However, it remains a puzzle where and through which route the near-inertial energy penetrates into the deep ocean. Using the measurements collected in the Kuroshio extension region during January 2005, we demonstrate that the diapycnal mixing in the thermocline and deep ocean is tightly related to the shear variance of wind-generated near-inertial internal waves with the diapycnal diffusivity 6 × 10−5 m2s−1 almost an order stronger than that observed in the circulation gyre. It is estimated that 45%–62% of the local near-inertial wind work 4.5 × 10−3 Wm−2 radiates into the thermocline and deep ocean and accounts for 42%–58% of the energy required to furnish mixing there. The elevated mixing is suggested to be maintained by the energetic near-inertial wind work and strong eddy activities causing enhanced downward near-inertial energy flux than earlier findings. The western <span class="hlt">boundary</span> <span class="hlt">current</span> turns out to be a key region for the penetration of near-inertial energy into the deep ocean and a hotspot for the diapycnal mixing in winter. PMID:25491363</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27773955','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27773955"><span>The role of prominence in determining the scope of <span class="hlt">boundary</span>-related lengthening in Greek.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Katsika, Argyro</p> <p>2016-03-01</p> <p>This study aims at examining and accounting for the scope of the temporal effect of phrase <span class="hlt">boundaries</span>. Previous research has indicated that there is an interaction between <span class="hlt">boundary</span>-related lengthening and prominence such that the former extends towards the nearby prominent syllable. However, it is unclear whether this interaction is due to lexical stress and/or phrasal prominence (marked by pitch accent) and how far towards the prominent syllable the effect extends. Here, we use an electromagnetic articulography (EMA) study of Greek to examine the scope of <span class="hlt">boundary</span>-related lengthening as a function of lexical stress and pitch accent separately. <span class="hlt">Boundaries</span> are elicited by the means of a variety of syntactic constructions.. The results show an effect of lexical stress. Phrase-<span class="hlt">final</span> lengthening affects the articulatory gestures of the phrase-<span class="hlt">final</span> syllable that are immediately adjacent to the <span class="hlt">boundary</span> in words with <span class="hlt">final</span> stress, but is initiated earlier within phrase-<span class="hlt">final</span> words with non-<span class="hlt">final</span> stress. Similarly, the articulatory configurations during inter-phrasal pauses reach their point of achievement later in words with <span class="hlt">final</span> stress than in words with non-<span class="hlt">final</span> stress. These effects of stress hold regardless of whether the phrase-<span class="hlt">final</span> word is accented or de-accented. Phrase-initial lengthening, on the other hand, is consistently detected on the phrase-initial constriction, independently of where the stress is within the preceding, phrase-<span class="hlt">final</span>, word. These results indicate that the lexical aspect of prominence plays a role in determining the scope of <span class="hlt">boundary</span>-related lengthening in Greek. Based on these results, a gestural account of prosodic <span class="hlt">boundaries</span> in Greek is proposed in which lexical and phrasal prosody interact in a systematic and coordinated fashion. The cross-linguistic dimensions of this account and its implications for prosodic structure are discussed.</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/2018AnGeo..36..595H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AnGeo..36..595H"><span>Quantifying the relationship between the plasmapause and the inner <span class="hlt">boundary</span> of small-scale field-aligned <span class="hlt">currents</span>, as deduced from Swarm observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Heilig, Balázs; Lühr, Hermann</p> <p>2018-04-01</p> <p>This paper presents a statistical study of the equatorward <span class="hlt">boundary</span> of small-scale field-aligned <span class="hlt">currents</span> (SSFACs) and investigates the relation between this <span class="hlt">boundary</span> and the plasmapause (PP). The PP data used for validation were derived from in situ electron density observations of NASA's Van Allen Probes. We confirmed the findings of a previous study by the same authors obtained from the observations of the CHAMP satellite SSFAC and the NASA IMAGE satellite PP detections, namely that the two <span class="hlt">boundaries</span> respond similarly to changes in geomagnetic activity, and they are closely located in the near midnight MLT sector, suggesting a dynamic linkage. Dayside PP correlates with the delayed time history of the SSFAC <span class="hlt">boundary</span>. We interpreted this behaviour as a direct consequence of co-rotation: the new PP, formed on the night side, propagates to the dayside by rotating with Earth. This finding paves the way toward an efficient PP monitoring tool based on an SSFAC index derived from vector magnetic field observations at low-Earth orbit.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880013801','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880013801"><span>Two-Equation Low-Reynolds-Number Turbulence Modeling of Transitional <span class="hlt">Boundary</span> Layer Flows Characteristic of Gas Turbine Blades. Ph.D. Thesis. <span class="hlt">Final</span> Contractor Report</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schmidt, Rodney C.; Patankar, Suhas V.</p> <p>1988-01-01</p> <p>The use of low Reynolds number (LRN) forms of the k-epsilon turbulence model in predicting transitional <span class="hlt">boundary</span> layer flow characteristic of gas turbine blades is developed. The research presented consists of: (1) an evaluation of two existing models; (2) the development of a modification to <span class="hlt">current</span> LRN models; and (3) the extensive testing of the proposed model against experimental data. The prediction characteristics and capabilities of the Jones-Launder (1972) and Lam-Bremhorst (1981) LRN k-epsilon models are evaluated with respect to the prediction of transition on flat plates. Next, the mechanism by which the models simulate transition is considered and the need for additional constraints is discussed. <span class="hlt">Finally</span>, the transition predictions of a new model are compared with a wide range of different experiments, including transitional flows with free-stream turbulence under conditions of flat plate constant velocity, flat plate constant acceleration, flat plate but strongly variable acceleration, and flow around turbine blade test cascades. In general, calculational procedure yields good agreement with most of the experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4356959','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4356959"><span>Growth of a deep-water, predatory fish is influenced by the productivity of a <span class="hlt">boundary</span> <span class="hlt">current</span> system</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Nguyen, Hoang Minh; Rountrey, Adam N.; Meeuwig, Jessica J.; Coulson, Peter G.; Feng, Ming; Newman, Stephen J.; Waite, Anya M.; Wakefield, Corey B.; Meekan, Mark G.</p> <p>2015-01-01</p> <p>The effects of climate change on predatory fishes in deep shelf areas are difficult to predict because complex processes may govern food availability and temperature at depth. We characterised the net impact of recent environmental changes on hapuku (Polyprion oxygeneios), an apex predator found in continental slope habitats (>200 m depth) by using dendrochronology techniques to develop a multi-decadal record of growth from otoliths. Fish were sampled off temperate south-western Australia, a region strongly influenced by the Leeuwin <span class="hlt">Current</span>, a poleward-flowing, eastern <span class="hlt">boundary</span> <span class="hlt">current</span>. The common variance among individual growth records was relatively low (3.4%), but the otolith chronology was positively correlated (r = 0.61, p < 0.02) with sea level at Fremantle, a proxy for the strength of the Leeuwin <span class="hlt">Current</span>. The Leeuwin <span class="hlt">Current</span> influences the primary productivity of shelf ecosystems, with a strong <span class="hlt">current</span> favouring growth in hapuku. Leeuwin <span class="hlt">Current</span> strength is predicted to decline under climate change models and this study provides evidence that associated productivity changes may flow through to higher trophic levels even in deep water habitats. PMID:25761975</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25761975','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25761975"><span>Growth of a deep-water, predatory fish is influenced by the productivity of a <span class="hlt">boundary</span> <span class="hlt">current</span> system.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nguyen, Hoang Minh; Rountrey, Adam N; Meeuwig, Jessica J; Coulson, Peter G; Feng, Ming; Newman, Stephen J; Waite, Anya M; Wakefield, Corey B; Meekan, Mark G</p> <p>2015-03-12</p> <p>The effects of climate change on predatory fishes in deep shelf areas are difficult to predict because complex processes may govern food availability and temperature at depth. We characterised the net impact of recent environmental changes on hapuku (Polyprion oxygeneios), an apex predator found in continental slope habitats (>200 m depth) by using dendrochronology techniques to develop a multi-decadal record of growth from otoliths. Fish were sampled off temperate south-western Australia, a region strongly influenced by the Leeuwin <span class="hlt">Current</span>, a poleward-flowing, eastern <span class="hlt">boundary</span> <span class="hlt">current</span>. The common variance among individual growth records was relatively low (3.4%), but the otolith chronology was positively correlated (r = 0.61, p < 0.02) with sea level at Fremantle, a proxy for the strength of the Leeuwin <span class="hlt">Current</span>. The Leeuwin <span class="hlt">Current</span> influences the primary productivity of shelf ecosystems, with a strong <span class="hlt">current</span> favouring growth in hapuku. Leeuwin <span class="hlt">Current</span> strength is predicted to decline under climate change models and this study provides evidence that associated productivity changes may flow through to higher trophic levels even in deep water habitats.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003NucFu..43.1040H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003NucFu..43.1040H"><span>Constructing integrable high-pressure full-<span class="hlt">current</span> free-<span class="hlt">boundary</span> stellarator magnetohydrodynamic equilibrium solutions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hudson, S. R.; Monticello, D. A.; Reiman, A. H.; Strickler, D. J.; Hirshman, S. P.; Ku, L.-P.; Lazarus, E.; Brooks, A.; Zarnstorff, M. C.; Boozer, A. H.; Fu, G.-Y.; Neilson, G. H.</p> <p>2003-10-01</p> <p>For the (non-axisymmetric) stellarator class of plasma confinement devices to be feasible candidates for fusion power stations it is essential that, to a good approximation, the magnetic field lines lie on nested flux surfaces; however, the inherent lack of a continuous symmetry implies that magnetic islands responsible for breaking the smooth topology of the flux surfaces are guaranteed to exist. Thus, the suppression of magnetic islands is a critical issue for stellarator design, particularly for small aspect ratio devices. Pfirsch-Schlüter <span class="hlt">currents</span>, diamagnetic <span class="hlt">currents</span> and resonant coil fields contribute to the formation of magnetic islands, and the challenge is to design the plasma and coils such that these effects cancel. Magnetic islands in free-<span class="hlt">boundary</span> high-pressure full-<span class="hlt">current</span> stellarator magnetohydrodynamic equilibria are suppressed using a procedure based on the Princeton Iterative Equilibrium Solver (Reiman and Greenside 1986 Comput. Phys. Commun. 43 157) which iterates the equilibrium equations to obtain the plasma equilibrium. At each iteration, changes to a Fourier representation of the coil geometry are made to cancel resonant fields produced by the plasma. The changes are constrained to preserve certain measures of engineering acceptability and to preserve the stability of ideal kink modes. As the iterations continue, the coil geometry and the plasma simultaneously converge to an equilibrium in which the island content is negligible, the plasma is stable to ideal kink modes, and the coils satisfy engineering constraints. The method is applied to a candidate plasma and coil design for the National Compact Stellarator eXperiment (Reiman et al 2001 Phys. Plasma 8 2083).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18195435','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18195435"><span>Globally optimal grouping for symmetric closed <span class="hlt">boundaries</span> by combining <span class="hlt">boundary</span> and region information.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Stahl, Joachim S; Wang, Song</p> <p>2008-03-01</p> <p>Many natural and man-made structures have a <span class="hlt">boundary</span> that shows a certain level of bilateral symmetry, a property that plays an important role in both human and computer vision. In this paper, we present a new grouping method for detecting closed <span class="hlt">boundaries</span> with symmetry. We first construct a new type of grouping token in the form of symmetric trapezoids by pairing line segments detected from the image. A closed <span class="hlt">boundary</span> can then be achieved by connecting some trapezoids with a sequence of gap-filling quadrilaterals. For such a closed <span class="hlt">boundary</span>, we define a unified grouping cost function in a ratio form: the numerator reflects the <span class="hlt">boundary</span> information of proximity and symmetry and the denominator reflects the region information of the enclosed area. The introduction of the region-area information in the denominator is able to avoid a bias toward shorter <span class="hlt">boundaries</span>. We then develop a new graph model to represent the grouping tokens. In this new graph model, the grouping cost function can be encoded by carefully designed edge weights and the desired optimal <span class="hlt">boundary</span> corresponds to a special cycle with a minimum ratio-form cost. We <span class="hlt">finally</span> show that such a cycle can be found in polynomial time using a previous graph algorithm. We implement this symmetry-grouping method and test it on a set of synthetic data and real images. The performance is compared to two previous grouping methods that do not consider symmetry in their grouping cost functions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MNRAS.477.4824W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MNRAS.477.4824W"><span>Influence of the outer <span class="hlt">boundary</span> condition on models of AGB stars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wagstaff, G.; Weiss, A.</p> <p>2018-07-01</p> <p><span class="hlt">Current</span> implementations of the stellar atmosphere typically derive <span class="hlt">boundary</span> conditions for the interior model from either grey plane-parallel atmospheres or scaled solar atmospheres, neither of which can be considered to have appropriate underlying assumptions for the Thermally Pulsing Asymptotic Giant Branch (TP-AGB). This paper discusses the treatment and influence of the outer <span class="hlt">boundary</span> condition within stellar evolution codes, and the resulting effects on the AGB evolution. The complex interaction of processes, such as the third dredge up and mass-loss, governing the TP-AGB can be affected by varying the treatment of this <span class="hlt">boundary</span> condition. Presented here are the results from altering the geometry, opacities, and the implementation of a grid of MARCS/COMARCS model atmospheres in order to improve this treatment. Although there are changes in the TP-AGB evolution, observable quantities, such as the <span class="hlt">final</span> core mass, are not significantly altered as a result of the change of atmospheric treatment. During the course of the investigation, a previously unseen phenomenon in the AGB models was observed and further investigated. This is believed to be physical, although arising from specific conditions which make its presence unlikely. If it were present in stars, this phenomenon would increase the carbon-star lifetime above 10 Myr and increase the <span class="hlt">final</span> core mass by ˜0.1 M⊙ in the narrow initial-mass range where it was observed (˜2-2.3 M⊙).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MNRAS.tmp..858W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MNRAS.tmp..858W"><span>Influence of the Outer <span class="hlt">Boundary</span> Condition on models of AGB stars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wagstaff, G.; Weiss, A.</p> <p>2018-04-01</p> <p><span class="hlt">Current</span> implementations of the stellar atmosphere typically derive <span class="hlt">boundary</span> conditions for the interior model from either grey plane-parallel atmospheres or scaled solar atmospheres, neither of which can be considered to have appropriate underlying assumptions for the Thermally Pulsing Asymptotic Giant Branch (TP-AGB). This paper discusses the treatment and influence of the outer <span class="hlt">boundary</span> condition within stellar evolution codes, and the resulting effects on the AGB evolution. The complex interaction of processes, such as the third dredge up and mass loss, governing the TP-AGB can be affected by varying the treatment of this <span class="hlt">boundary</span> condition. Presented here are the results from altering the geometry, opacities and the implementation of a grid of MARCS/COMARCS model atmospheres in order to improve this treatment. Although there are changes in the TP-AGB evolution, observable quantities, such as the <span class="hlt">final</span> core mass, are not significantly altered as a result of the change of atmospheric treatment. During the course of the investigation, a previously unseen phenomena in the AGB models was observed and further investigated. This is believed to be physical, although arising from specific conditions which make its presence unlikely. If it were present in stars, this phenomenon would increase the carbon-star lifetime above 10Myr and increase the <span class="hlt">final</span> core mass by ˜0.1M⊙ in the narrow initial-mass range where it was observed (˜2 - 2.3M⊙).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MarGR.tmp...24K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MarGR.tmp...24K"><span>Monitoring the deep western <span class="hlt">boundary</span> <span class="hlt">current</span> in the western North Pacific by echo intensity measured with lowered acoustic Doppler <span class="hlt">current</span> profiler</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Komaki, Kanae; Nagano, Akira</p> <p>2018-05-01</p> <p>Oxidation of iron and manganese ions is predominant in the oxygen-rich deep western <span class="hlt">boundary</span> <span class="hlt">current</span> (DWBC) within the Pacific Ocean. By the faster removal of particulate iron hydroxide and manganese oxide, densities of the particulate matters are considered to be lower in the DWBC than the interior region. To detect the density variation of suspended particles between the DWBC and interior regions, we analyzed echo intensity (EI) measured in the western North Pacific by hydrographic casts with a 300 kHz lowered acoustic Doppler <span class="hlt">current</span> profiler (LADCP) in a whole water column. At depths greater than 3000 m ( 3000 dbar), EI is almost uniformly low between 12°N and 30°N but peaks sharply from 30°N to 35°N to a maximum north of 35°N. EI is found to be anomalously low in the DWBC compared to the background distribution. The DWBC pathways are identifiable by the low EI and high dissolved oxygen concentration. EI data by LADCPs and other acoustic instruments may be used to observe the temporal variations of the DWBC pathways.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/815091','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/815091"><span>Constructing Integrable High-pressure Full-<span class="hlt">current</span> Free-<span class="hlt">boundary</span> Stellarator Magnetohydrodynamic Equilibrium Solutions</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>S.R. Hudson; D.A. Monticello; A.H. Reiman</p> <p></p> <p>For the (non-axisymmetric) stellarator class of plasma confinement devices to be feasible candidates for fusion power stations it is essential that, to a good approximation, the magnetic field lines lie on nested flux surfaces; however, the inherent lack of a continuous symmetry implies that magnetic islands responsible for breaking the smooth topology of the flux surfaces are guaranteed to exist. Thus, the suppression of magnetic islands is a critical issue for stellarator design, particularly for small aspect ratio devices. Pfirsch-Schluter <span class="hlt">currents</span>, diamagnetic <span class="hlt">currents</span>, and resonant coil fields contribute to the formation of magnetic islands, and the challenge is to designmore » the plasma and coils such that these effects cancel. Magnetic islands in free-<span class="hlt">boundary</span> high-pressure full-<span class="hlt">current</span> stellarator magnetohydrodynamic equilibria are suppressed using a procedure based on the Princeton Iterative Equilibrium Solver [Reiman and Greenside, Comp. Phys. Comm. 43 (1986) 157] which iterate s the equilibrium equations to obtain the plasma equilibrium. At each iteration, changes to a Fourier representation of the coil geometry are made to cancel resonant fields produced by the plasma. The changes are constrained to preserve certain measures of engineering acceptability and to preserve the stability of ideal kink modes. As the iterations continue, the coil geometry and the plasma simultaneously converge to an equilibrium in which the island content is negligible, the plasma is stable to ideal kink modes, and the coils satisfy engineering constraints. The method is applied to a candidate plasma and coil design for the National Compact Stellarator Experiment [Reiman, et al., Phys. Plasmas 8 (May 2001) 2083].« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2008/1117/','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2008/1117/"><span>Using Molecular Genetic Markers to Resolve a Subspecies <span class="hlt">Boundary</span>: The Northern <span class="hlt">Boundary</span> of the Southwestern Willow Flycatcher in the Four-Corner 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>Paxton, Eben H.; Sogge, Mark K.; Theimer, Tad C.; Girard, Jessica; Keim, Paul</p> <p>2008-01-01</p> <p>*Executive Summary* The northern <span class="hlt">boundary</span> of the endangered Southwestern Willow Flycatcher (Empidonax traillii extimus) is <span class="hlt">currently</span> approximated as running through southern Colorado and Utah, but the exact placement is uncertain because this subspecies shares a border with the more northern and non-endangered E. t. adastus. To help resolve this issue, we evaluated the geographic distribution of mitochondrial and nuclear DNA by sampling breeding sites across the four-corner states (Arizona, Colorado, New Mexico, and Utah). We found that breeding sites clustered into two major groups generally consistent with the <span class="hlt">currently</span> designated <span class="hlt">boundary</span>, with the exception of three sites situated along the <span class="hlt">current</span> <span class="hlt">boundary</span>. However, delineating a precise <span class="hlt">boundary</span> that would separate the two subspecies is made difficult because (1) we found evidence for a region of intergradation along the <span class="hlt">boundary</span> area, suggesting the <span class="hlt">boundary</span> is not discreet, and (2) the <span class="hlt">boundary</span> region is sparsely populated, with too few extant breeding populations to precisely locate a <span class="hlt">boundary</span>. The <span class="hlt">boundary</span> region encompasses an area where elevation changes markedly over relatively short distances, with low elevation deserts to the south and more mesic, higher elevation habitats to the north. We hypothesized that latitudinal and elevational differences and their concomitant ecological effects could form an ecological barrier that inhibited gene flow between the subspecies, forming the basis for the subspecies <span class="hlt">boundary</span>. We modeled changes in geographic patterns of genetic markers as a function of latitude and elevation finding significant support for this relationship. The model was brought into a GIS environment to create multiple subspecies <span class="hlt">boundaries</span>, with the strength of each predicted <span class="hlt">boundary</span> evaluated on the basis of how much genetic variation it explained. The candidate <span class="hlt">boundary</span> that accounted for the most genetic variation was situated generally near the <span class="hlt">currently</span> recognized subspecies <span class="hlt">boundary</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26452376','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26452376"><span>Event <span class="hlt">boundaries</span> and anaphoric reference.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Thompson, Alexis N; Radvansky, Gabriel A</p> <p>2016-06-01</p> <p>The <span class="hlt">current</span> study explored the finding that parsing a narrative into separate events impairs anaphor resolution. According to the Event Horizon Model, when a narrative event <span class="hlt">boundary</span> is encountered, a new event model is created. Information associated with the prior event model is removed from working memory. So long as the event model containing the anaphor referent is <span class="hlt">currently</span> being processed, this information should still be available when there is no narrative event <span class="hlt">boundary</span>, even if reading has been disrupted by a working-memory-clearing distractor task. In those cases, readers may reactivate their prior event model, and anaphor resolution would not be affected. Alternatively, comprehension may not be as event oriented as this account suggests. Instead, any disruption of the contents of working memory during comprehension, event related or not, may be sufficient to disrupt anaphor resolution. In this case, reading comprehension would be more strongly guided by other, more basic language processing mechanisms and the event structure of the described events would play a more minor role. In the <span class="hlt">current</span> experiments, participants were given stories to read in which we included, between the anaphor and its referent, either the presence of a narrative event <span class="hlt">boundary</span> (Experiment 1) or a narrative event <span class="hlt">boundary</span> along with a working-memory-clearing distractor task (Experiment 2). The results showed that anaphor resolution was affected by narrative event <span class="hlt">boundaries</span> but not by a working-memory-clearing distractor task. This is interpreted as being consistent with the Event Horizon Model of event cognition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26302083','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26302083"><span>Transport Gap Opening and High On-Off <span class="hlt">Current</span> Ratio in Trilayer Graphene with Self-Aligned Nanodomain <span class="hlt">Boundaries</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wu, Han-Chun; Chaika, Alexander N; Huang, Tsung-Wei; Syrlybekov, Askar; Abid, Mourad; Aristov, Victor Yu; Molodtsova, Olga V; Babenkov, Sergey V; Marchenko, D; Sánchez-Barriga, Jaime; Mandal, Partha Sarathi; Varykhalov, Andrei Yu; Niu, Yuran; Murphy, Barry E; Krasnikov, Sergey A; Lübben, Olaf; Wang, Jing Jing; Liu, Huajun; Yang, Li; Zhang, Hongzhou; Abid, Mohamed; Janabi, Yahya T; Molotkov, Sergei N; Chang, Ching-Ray; Shvets, Igor</p> <p>2015-09-22</p> <p>Trilayer graphene exhibits exceptional electronic properties that are of interest both for fundamental science and for technological applications. The ability to achieve a high on-off <span class="hlt">current</span> ratio is the central question in this field. Here, we propose a simple method to achieve a <span class="hlt">current</span> on-off ratio of 10(4) by opening a transport gap in Bernal-stacked trilayer graphene. We synthesized Bernal-stacked trilayer graphene with self-aligned periodic nanodomain <span class="hlt">boundaries</span> (NBs) on the technologically relevant vicinal cubic-SiC(001) substrate and performed electrical measurements. Our low-temperature transport measurements clearly demonstrate that the self-aligned periodic NBs can induce a charge transport gap greater than 1.3 eV. More remarkably, the transport gap of ∼0.4 eV persists even at 100 K. Our results show the feasibility of creating new electronic nanostructures with high on-off <span class="hlt">current</span> ratios using graphene on cubic-SiC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17674484','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17674484"><span><span class="hlt">Current</span> good manufacturing practice in manufacturing, packaging, labeling, or holding operations for dietary supplements. <span class="hlt">Final</span> rule.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p></p> <p>2007-06-25</p> <p>The Food and Drug Administration (FDA) is issuing a <span class="hlt">final</span> rule regarding <span class="hlt">current</span> good manufacturing practice (CGMP) for dietary supplements. The <span class="hlt">final</span> rule establishes the minimum CGMPs necessary for activities related to manufacturing, packaging, labeling, or holding dietary supplements to ensure the quality of the dietary supplement. The <span class="hlt">final</span> rule is one of many actions related to dietary supplements that we are taking to promote and protect the public health.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16479693','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16479693"><span><span class="hlt">Current</span> good manufacturing practice regulation and investigational new drugs. Direct <span class="hlt">final</span> rule.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p></p> <p>2006-01-17</p> <p>The Food and Drug Administration (FDA) is amending its <span class="hlt">current</span> good manufacturing practice (CGMP) regulations for human drugs, including biological products, to exempt most investigational "Phase 1" drugs from complying with the requirements in FDA's regulations. FDA will instead exercise oversight of production of these drugs under the agency's general statutory CGMP authority and investigational new drug application (IND) authority. In addition, FDA is making available simultaneously with the publication of this direct <span class="hlt">final</span> rule, a guidance document setting forth recommendations on approaches to CGMP compliance for the exempted Phase 1 drugs. Elsewhere in this issue of the Federal Register, FDA is publishing a companion proposed rule, under FDA's usual procedure for notice-and-comment rulemaking, to provide a procedural framework to <span class="hlt">finalize</span> the rule in the event the agency receives any significant adverse comments and withdraws this direct <span class="hlt">final</span> rule. The companion proposed rule and direct <span class="hlt">final</span> rule are substantively identical. Elsewhere in this issue of the Federal Register, FDA is announcing the availability of a draft guidance for industry entitled "INDs--Approaches to Complying With CGMP During Phase 1" to provide further guidance on the subject.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5334705-redefinition-meramecian-chesterian-boundary-mississippian','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5334705-redefinition-meramecian-chesterian-boundary-mississippian"><span>Redefinition of the Meramecian/Chesterian <span class="hlt">boundary</span> (Mississippian)</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>Maples, C.G.; Waters, J.A.</p> <p>1987-07-01</p> <p>The Meramecian/Chesterian (Mississippi) <span class="hlt">boundary</span> in the type area is <span class="hlt">currently</span> defined as the highest occurrence of the crinoid Platycrinites penicillus and the lowest occurrence of the crinoid genera Agassizocrinus and Talarocrinus. Because these taxa have not been reported outside eastern North America, attempts have been made to use conodonts and Foraminifera to extend the Meramecian/Chesterian <span class="hlt">boundary</span> outside the type area. Unfortunately, changes in conodont and foraminiferal assemblages do not coincide with the <span class="hlt">currently</span> defined Meramecian/Chesterian <span class="hlt">boundary</span>, and use of these fossil groups does not allow exact placement of the <span class="hlt">boundary</span> outside of eastern North America. The authors suggest that themore » Meramecian/Chesterian <span class="hlt">boundary</span> be redefined as the <span class="hlt">boundary</span> between Foraminiferal Zones 15 and 16i of the Mamet scheme, irrespective of the occurrence of Platycrinites penicillus. This change in definition places the Ste. Genevieve Limestone (Genevievian Stage) in the lowermost part of the Chesterian Series, with which it is biotically and sedimentologically more allied than with the underlying St. Louis Limestone. This change provides a sound biostratigraphic base for correlating the Meramecian/Chesterian <span class="hlt">boundary</span> outside of the type area. Foraminifera, conodonts, brachiopods, and corals all show significant changes at or slightly below the St. Louis/Ste. Genevieve contact rather than at the Genevievian/Chesterian contact. 52 references.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=APICAL&pg=2&id=EJ117750','ERIC'); return false;" href="https://eric.ed.gov/?q=APICAL&pg=2&id=EJ117750"><span>Apical Coarticulation at Juncture <span class="hlt">Boundaries</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>Lewis, J.; And Others</p> <p>1975-01-01</p> <p>Sentences were read by six informants to determine the presence or absence of /n/ in /nth/ sequences. The sentences contained seven different levels of juncture with /nth/ occurring in word <span class="hlt">final</span> position, intervocalically, and across word <span class="hlt">boundaries</span>, among other places. Dental coarticulation was not hindered by most junctures. (SC)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20040020075&hterms=Plasma+Ring&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DPlasma%2BRing','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20040020075&hterms=Plasma+Ring&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DPlasma%2BRing"><span>Magnetosphere-Ionosphere Coupling and Associated Ring <span class="hlt">Current</span> Energization Processes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Liemohn, M. W.; Khazanov, G. V.</p> <p>2004-01-01</p> <p>Adiabatic processes in the ring <span class="hlt">current</span> are examined. In particular, an analysis of the factors that parameterize the net adiabatic energy gain in the inner magnetosphere during magnetic storms is presented. A single storm was considered, that of April 17, 2002. Three simulations were conducted with similar <span class="hlt">boundary</span> conditions but with different electric field descriptions. It is concluded that the best parameter for quantifying the net adiabatic energy gain in the inner magnetosphere during storms is the instantaneous value of the product of the maximum westward electric field at the outer simulation <span class="hlt">boundary</span> with the nightside plasma sheet density. However, all of the instantaneous magnetospheric quantities considered in this study produced large correlation coefficients. Therefore, they all could be considered useful predictors of the net adiabatic energy gain of the ring <span class="hlt">current</span>. Long integration times over the parameters lessen the significance of the correlation. <span class="hlt">Finally</span>, some significant differences exist in the correlation coefficients depending on the electric field description.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1422033-evidence-preferential-flux-flow-grain-boundaries-superconducting-rf-quality-niobium','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1422033-evidence-preferential-flux-flow-grain-boundaries-superconducting-rf-quality-niobium"><span>Evidence for preferential flux flow at the grain <span class="hlt">boundaries</span> of superconducting RF-quality niobium</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>Sung, Z. -H.; Lee, P. J.; Gurevich, A.</p> <p></p> <p>Here, the question of whether grain <span class="hlt">boundaries</span> (GBs) in niobium can be responsible for lowered operating field (B RF) or quality factor (Q 0) in superconducting radio-frequency (SRF) cavities is still controversial. Here, we show by direct DC transport across planar grain <span class="hlt">boundaries</span> isolated from a slice of very large-grain SRF-quality Nb that vortices can preferentially flow along the grain <span class="hlt">boundary</span> when the external magnetic field lies in the GB plane. However, increasing the misalignment between the GB plane and the external magnetic field vector markedly reduces preferential flux flow along GB. Importantly, we find that preferential GB flux flowmore » is more prominent for a buffered chemical polished than for an electropolished bi-crystal. The voltage-<span class="hlt">current</span> characteristics of GBs are similar to those seen in low angle grain <span class="hlt">boundaries</span> of high temperature superconductors where there is clear evidence of suppression of the superconducting order parameter at the GB. While local weakening of superconductivity at GBs in cuprates and pnictides is intrinsic, deterioration of <span class="hlt">current</span> transparency of GBs in Nb appears to be extrinsic, since the polishing method clearly affect the local GB degradation. The dependence of preferential GB flux flow on important cavity preparation and experimental variables, particularly, the <span class="hlt">final</span> chemical treatment and the angle between the magnetic field and the GB plane, suggests two more reasons why real cavity performance can be so variable.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1422033-evidence-preferential-flux-flow-grain-boundaries-superconducting-rf-quality-niobium','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1422033-evidence-preferential-flux-flow-grain-boundaries-superconducting-rf-quality-niobium"><span>Evidence for preferential flux flow at the grain <span class="hlt">boundaries</span> of superconducting RF-quality niobium</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Sung, Z. -H.; Lee, P. J.; Gurevich, A.; ...</p> <p>2018-02-19</p> <p>Here, the question of whether grain <span class="hlt">boundaries</span> (GBs) in niobium can be responsible for lowered operating field (B RF) or quality factor (Q 0) in superconducting radio-frequency (SRF) cavities is still controversial. Here, we show by direct DC transport across planar grain <span class="hlt">boundaries</span> isolated from a slice of very large-grain SRF-quality Nb that vortices can preferentially flow along the grain <span class="hlt">boundary</span> when the external magnetic field lies in the GB plane. However, increasing the misalignment between the GB plane and the external magnetic field vector markedly reduces preferential flux flow along GB. Importantly, we find that preferential GB flux flowmore » is more prominent for a buffered chemical polished than for an electropolished bi-crystal. The voltage-<span class="hlt">current</span> characteristics of GBs are similar to those seen in low angle grain <span class="hlt">boundaries</span> of high temperature superconductors where there is clear evidence of suppression of the superconducting order parameter at the GB. While local weakening of superconductivity at GBs in cuprates and pnictides is intrinsic, deterioration of <span class="hlt">current</span> transparency of GBs in Nb appears to be extrinsic, since the polishing method clearly affect the local GB degradation. The dependence of preferential GB flux flow on important cavity preparation and experimental variables, particularly, the <span class="hlt">final</span> chemical treatment and the angle between the magnetic field and the GB plane, suggests two more reasons why real cavity performance can be so variable.« 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_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('https://www.osti.gov/biblio/6952723-simulation-electrostatic-turbulence-plasma-sheet-boundary-layer-electron-currents-bean-shaped-ion-beams','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6952723-simulation-electrostatic-turbulence-plasma-sheet-boundary-layer-electron-currents-bean-shaped-ion-beams"><span>Simulation of electrostatic turbulence in the plasma sheet <span class="hlt">boundary</span> layer with electron <span class="hlt">currents</span> and bean-shaped ion beams</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>Nishikawa, K.; Frank, L.A.; Huang, C.Y.</p> <p></p> <p>Plasma data from ISEE 1 show the presence of electron <span class="hlt">currents</span> as well as energetic ion beams in the plasma sheet <span class="hlt">boundary</span> layer. Broadband electrostatic noise and low-frequency electromagnetic bursts are detected in the plasma sheet <span class="hlt">boundary</span> layer, especially in the presence of strong ion flows, <span class="hlt">currents</span>, and steep spacial gradients in the fluxes of few-keV electrons and ions. Particle simulations have been performed to investigate electrostatic turbulence driven by a cold electron beam and/or ion beams with a bean-shaped velocity distribution. The simulation results show that the counterstreaming ion beams as well as the counterstreaming of the cold electronmore » beam and the ion beam excite ion acoustic waves with the Doppler-shifted real frequency ..omega..approx. = +- k/sub parallel/(c/sub s/-V/sub i//sub //sub parallel/). However, the effect of the bean-shaped ion velocity distributions reduces the growth rates of ion acoustic instability. The simulation results also show that the slowing down of the ion beam is larger at the larger perpendicular velocity. The wave spectra of the electric fields at some points for simulations show turbulence generated by growing waves. The frequency of these spectra ranges from ..cap omega../sub i/ to ..omega../sub p//sub e/, which is in qualitative agreement with the satellite data. copyright American Geophysical Union 1988« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008GeoRL..3512607B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008GeoRL..3512607B"><span>Oxygen declines and the shoaling of the hypoxic <span class="hlt">boundary</span> in the California <span class="hlt">Current</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bograd, Steven J.; Castro, Carmen G.; Di Lorenzo, Emanuele; Palacios, Daniel M.; Bailey, Helen; Gilly, William; Chavez, Francisco P.</p> <p>2008-06-01</p> <p>We use hydrographic data from the California Cooperative Oceanic Fisheries Investigations program to explore the spatial and temporal variability of dissolved oxygen (DO) in the southern California <span class="hlt">Current</span> System (CCS) over the period 1984-2006. Large declines in DO (up to 2.1 μmol/kg/y) have been observed throughout the domain, with the largest relative DO declines occurring below the thermocline (mean decrease of 21% at 300 m). Linear trends were significant (p < 0.05) at the majority of stations down to 500 m. The hypoxic <span class="hlt">boundary</span> (~60 μmol/kg) has shoaled by up to 90 m within portions of the southern CCS. The observed trends are consistent with advection of low-DO waters into the region, as well as decreased vertical oxygen transport following near-surface warming and increased stratification. Expansion of the oxygen minimum layer could lead to cascading effects on benthic and pelagic ecosystems, including habitat compression and community reorganization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JCoPh.305..942G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JCoPh.305..942G"><span>Effective surface and <span class="hlt">boundary</span> conditions for heterogeneous surfaces with mixed <span class="hlt">boundary</span> conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Jianwei; Veran-Tissoires, Stéphanie; Quintard, Michel</p> <p>2016-01-01</p> <p>To deal with multi-scale problems involving transport from a heterogeneous and rough surface characterized by a mixed <span class="hlt">boundary</span> condition, an effective surface theory is developed, which replaces the original surface by a homogeneous and smooth surface with specific <span class="hlt">boundary</span> conditions. A typical example corresponds to a laminar flow over a soluble salt medium which contains insoluble material. To develop the concept of effective surface, a multi-domain decomposition approach is applied. In this framework, velocity and concentration at micro-scale are estimated with an asymptotic expansion of deviation terms with respect to macro-scale velocity and concentration fields. Closure problems for the deviations are obtained and used to define the effective surface position and the related <span class="hlt">boundary</span> conditions. The evolution of some effective properties and the impact of surface geometry, Péclet, Schmidt and Damköhler numbers are investigated. <span class="hlt">Finally</span>, comparisons are made between the numerical results obtained with the effective models and those from direct numerical simulations with the original rough surface, for two kinds of configurations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25181298','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25181298"><span>Identifying chemicals that are planetary <span class="hlt">boundary</span> threats.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>MacLeod, Matthew; Breitholtz, Magnus; Cousins, Ian T; de Wit, Cynthia A; Persson, Linn M; Rudén, Christina; McLachlan, Michael S</p> <p>2014-10-07</p> <p>Rockström et al. proposed a set of planetary <span class="hlt">boundaries</span> that delimit a "safe operating space for humanity". Many of the planetary <span class="hlt">boundaries</span> that have so far been identified are determined by chemical agents. Other chemical pollution-related planetary <span class="hlt">boundaries</span> likely exist, but are <span class="hlt">currently</span> unknown. A chemical poses an unknown planetary <span class="hlt">boundary</span> threat if it simultaneously fulfills three conditions: (1) it has an unknown disruptive effect on a vital Earth system process; (2) the disruptive effect is not discovered until it is a problem at the global scale, and (3) the effect is not readily reversible. In this paper, we outline scenarios in which chemicals could fulfill each of the three conditions, then use the scenarios as the basis to define chemical profiles that fit each scenario. The chemical profiles are defined in terms of the nature of the effect of the chemical and the nature of exposure of the environment to the chemical. Prioritization of chemicals in commerce against some of the profiles appears feasible, but there are considerable uncertainties and scientific challenges that must be addressed. Most challenging is prioritizing chemicals for their potential to have a <span class="hlt">currently</span> unknown effect on a vital Earth system process. We conclude that the most effective strategy <span class="hlt">currently</span> available to identify chemicals that are planetary <span class="hlt">boundary</span> threats is prioritization against profiles defined in terms of environmental exposure combined with monitoring and study of the biogeochemical processes that underlie vital Earth system processes to identify <span class="hlt">currently</span> unknown disruptive effects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28101648','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28101648"><span>The limits of <span class="hlt">boundaries</span>: unpacking localization and cognitive mapping relative to a <span class="hlt">boundary</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, Ruojing; Mou, Weimin</p> <p>2018-05-01</p> <p>Previous research (Zhou, Mou, Journal of Experimental Psychology: Learning, Memory and Cognition 42(8):1316-1323, 2016) showed that learning individual locations relative to a single landmark, compared to learning relative to a <span class="hlt">boundary</span>, led to more accurate inferences of inter-object spatial relations (cognitive mapping of multiple locations). Following our past findings, the <span class="hlt">current</span> study investigated whether the larger number of reference points provided by a homogeneous circular <span class="hlt">boundary</span>, as well as less accessible knowledge of direct spatial relations among the multiple reference points, would lead to less effective cognitive mapping relative to the <span class="hlt">boundary</span>. Accordingly, we manipulated (a) the number of primary reference points (one segment drawn from a circular <span class="hlt">boundary</span>, four such segments, vs. the complete <span class="hlt">boundary</span>) available when participants were localizing four objects sequentially (Experiment 1) and (b) the extendedness of each of the four segments (Experiment 2). The results showed that cognitive mapping was the least accurate in the whole <span class="hlt">boundary</span> condition. However, expanding each of the four segments did not affect the accuracy of cognitive mapping until the four were connected to form a continuous <span class="hlt">boundary</span>. These findings indicate that when encoding locations relative to a homogeneous <span class="hlt">boundary</span>, participants segmented the <span class="hlt">boundary</span> into differentiated pieces and subsequently chose the most informative local part (i.e., the segment closest in distance to one location) as the primary reference point for a particular location. During this process, direct spatial relations among the reference points were likely not attended to. These findings suggest that people might encode and represent bounded space in a fragmented fashion when localizing within a homogeneous <span class="hlt">boundary</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1097228','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1097228"><span>Immersed <span class="hlt">Boundary</span> Methods for High-Resolution Simulation of Atmospheric <span class="hlt">Boundary</span>-Layer Flow Over Complex Terrain</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>Lundquist, K A</p> <p></p> <p>Mesoscale models, such as the Weather Research and Forecasting (WRF) model, are increasingly used for high resolution simulations, particularly in complex terrain, but errors associated with terrain-following coordinates degrade the accuracy of the solution. Use of an alternative Cartesian gridding technique, known as an immersed <span class="hlt">boundary</span> method (IBM), alleviates coordinate transformation errors and eliminates restrictions on terrain slope which <span class="hlt">currently</span> limit mesoscale models to slowly varying terrain. In this dissertation, an immersed <span class="hlt">boundary</span> method is developed for use in numerical weather prediction. Use of the method facilitates explicit resolution of complex terrain, even urban terrain, in the WRF mesoscale model.more » First, the errors that arise in the WRF model when complex terrain is present are presented. This is accomplished using a scalar advection test case, and comparing the numerical solution to the analytical solution. Results are presented for different orders of advection schemes, grid resolutions and aspect ratios, as well as various degrees of terrain slope. For comparison, results from the same simulation are presented using the IBM. Both two-dimensional and three-dimensional immersed <span class="hlt">boundary</span> methods are then described, along with details that are specific to the implementation of IBM in the WRF code. Our IBM is capable of imposing both Dirichlet and Neumann <span class="hlt">boundary</span> conditions. Additionally, a method for coupling atmospheric physics parameterizations at the immersed <span class="hlt">boundary</span> is presented, making IB methods much more functional in the context of numerical weather prediction models. The two-dimensional IB method is verified through comparisons of solutions for gentle terrain slopes when using IBM and terrain-following grids. The canonical case of flow over a Witch of Agnesi hill provides validation of the basic no-slip and zero gradient <span class="hlt">boundary</span> conditions. Specified diurnal heating in a valley, producing anabatic winds, is used to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1221645-paint-click-unified-interactions-image-boundaries','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1221645-paint-click-unified-interactions-image-boundaries"><span>Paint and Click: Unified Interactions for Image <span class="hlt">Boundaries</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>Summa, B.; Gooch, A. A.; Scorzelli, G.</p> <p></p> <p>Image <span class="hlt">boundaries</span> are a fundamental component of many interactive digital photography techniques, enabling applications such as segmentation, panoramas, and seamless image composition. Interactions for image <span class="hlt">boundaries</span> often rely on two complementary but separate approaches: editing via painting or clicking constraints. In this work, we provide a novel, unified approach for interactive editing of pairwise image <span class="hlt">boundaries</span> that combines the ease of painting with the direct control of constraints. Rather than a sequential coupling, this new formulation allows full use of both interactions simultaneously, giving users unprecedented flexibility for fast <span class="hlt">boundary</span> editing. To enable this new approach, we provide technical advancements.more » In particular, we detail a reformulation of image <span class="hlt">boundaries</span> as a problem of finding cycles, expanding and correcting limitations of the previous work. Our new formulation provides <span class="hlt">boundary</span> solutions for painted regions with performance on par with state-of-the-art specialized, paint-only techniques. In addition, we provide instantaneous exploration of the <span class="hlt">boundary</span> solution space with user constraints. <span class="hlt">Finally</span>, we provide examples of common graphics applications impacted by our new approach.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDQ10009R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDQ10009R"><span><span class="hlt">Boundary</span>-layer effects in droplet splashing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Riboux, Guillaume; Gordillo, Jose Manuel</p> <p>2017-11-01</p> <p>A drop falling onto a solid substrate will disintegrate into smaller parts when its impact velocity exceeds the so called critical velocity for splashing. Under these circumstances, the very thin liquid sheet ejected tangentially to the solid after the drop touches the substrate, lifts off as a consequence of the aerodynamic forces exerted on it and <span class="hlt">finally</span> breaks into smaller droplets, violently ejected radially outwards, provoking the splash. Here, the tangential deceleration experienced by the fluid entering the thin liquid sheet is investigated making use of <span class="hlt">boundary</span> layer theory. The velocity component tangent to the solid, computed using potential flow theory provides the far field <span class="hlt">boundary</span> condition as well as the pressure gradient for the <span class="hlt">boundary</span> layer equations. The structure of the flow permits to find a self similar solution of the <span class="hlt">boundary</span> layer equations. This solution is then used to calculate the <span class="hlt">boundary</span> layer thickness at the root of the lamella as well as the shear stress at the wall. The splash model presented in, which is slightly modified to account for the results obtained from the <span class="hlt">boundary</span> layer analysis, provides a very good agreement between the measurements and the predicted values of the critical velocity for the splash.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRC..121.8115S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRC..121.8115S"><span>Time series measurements of transient tracers and tracer-derived transport in the Deep Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> between the Labrador Sea and the subtropical Atlantic Ocean at Line W</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, John N.; Smethie, William M.; Yashayev, Igor; Curry, Ruth; Azetsu-Scott, Kumiko</p> <p>2016-11-01</p> <p>Time series measurements of the nuclear fuel reprocessing tracer 129I and the gas ventilation tracer CFC-11 were undertaken on the AR7W section in the Labrador Sea (1997-2014) and on Line W (2004-2014), located over the US continental slope off Cape Cod, to determine advection and mixing time scales for the transport of Denmark Strait Overflow Water (DSOW) within the Deep Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> (DWBC). Tracer measurements were also conducted in 2010 over the continental rise southeast of Bermuda to intercept the equatorward flow of DSOW by interior pathways. The Labrador Sea tracer and hydrographic time series data were used as input functions in a <span class="hlt">boundary</span> <span class="hlt">current</span> model that employs transit time distributions to simulate the effects of mixing and advection on downstream tracer distributions. Model simulations of tracer levels in the <span class="hlt">boundary</span> <span class="hlt">current</span> core and adjacent interior (shoulder) region with which mixing occurs were compared with the Line W time series measurements to determine <span class="hlt">boundary</span> <span class="hlt">current</span> model parameters. These results indicate that DSOW is transported from the Labrador Sea to Line W via the DWBC on a time scale of 5-6 years corresponding to a mean flow velocity of 2.7 cm/s while mixing between the core and interior regions occurs with a time constant of 2.6 years. A tracer section over the southern flank of the Bermuda rise indicates that the flow of DSOW that separated from the DWBC had undergone transport through interior pathways on a time scale of 9 years with a mixing time constant of 4 years.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28573735','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28573735"><span>Contraction and elongation: Mechanics underlying cell <span class="hlt">boundary</span> deformations in epithelial tissue.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hara, Yusuke</p> <p>2017-06-01</p> <p>The cell-cell <span class="hlt">boundaries</span> of epithelial cells form cellular frameworks at the apical side of tissues. Deformations in these <span class="hlt">boundaries</span>, for example, <span class="hlt">boundary</span> contraction and elongation, and the associated forces form the mechanical basis of epithelial tissue morphogenesis. In this review, using data from recent Drosophila studies on cell <span class="hlt">boundary</span> contraction and elongation, I provide an overview of the mechanism underlying the bi-directional deformations in the epithelial cell <span class="hlt">boundary</span>, that are sustained by biased accumulations of junctional and apico-medial non-muscle myosin II. Moreover, how the junctional tensions exist on cell <span class="hlt">boundaries</span> in different <span class="hlt">boundary</span> dynamics and morphologies are discussed. <span class="hlt">Finally</span>, some future perspectives on how recent knowledge about single cell <span class="hlt">boundary</span>-level mechanics will contribute to our understanding of epithelial tissue morphogenesis are discussed. © 2017 Japanese Society of Developmental Biologists.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2013-07-30/pdf/2013-18253.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2013-07-30/pdf/2013-18253.pdf"><span>78 FR 45938 - <span class="hlt">Final</span> Flood Hazard Determinations</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2013-07-30</p> <p>...] <span class="hlt">Final</span> Flood Hazard Determinations AGENCY: Federal Emergency Management Agency, DHS. ACTION: <span class="hlt">Final</span> notice. SUMMARY: Flood hazard determinations, which may include additions or modifications of Base Flood Elevations (BFEs), base flood depths, Special Flood Hazard Area (SFHA) <span class="hlt">boundaries</span> or zone designations, or...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950016851','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950016851"><span>Physics of magnetospheric <span class="hlt">boundary</span> layers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cairns, Iver H.</p> <p>1995-01-01</p> <p>This <span class="hlt">final</span> report was concerned with the ideas that: (1) magnetospheric <span class="hlt">boundary</span> layers link disparate regions of the magnetosphere-solar wind system together; and (2) global behavior of the magnetosphere can be understood only by understanding its internal linking mechanisms and those with the solar wind. The research project involved simultaneous research on the global-, meso-, and micro-scale physics of the magnetosphere and its <span class="hlt">boundary</span> layers, which included the bow shock, the magnetosheath, the plasma sheet <span class="hlt">boundary</span> layer, and the ionosphere. Analytic, numerical, and simulation projects were performed on these subjects, as well as comparisons of theoretical results with observational data. Other related activity included in the research included: (1) prediction of geomagnetic activity; (2) global MHD (magnetohydrodynamic) simulations; (3) Alfven resonance heating; and (4) Critical Ionization Velocity (CIV) effect. In the appendixes are list of personnel involved, list of papers published; and reprints or photocopies of papers produced for this report.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SuScT..31d5001S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SuScT..31d5001S"><span>Evidence for preferential flux flow at the grain <span class="hlt">boundaries</span> of superconducting RF-quality niobium</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sung, Z.-H.; Lee, P. J.; Gurevich, A.; Larbalestier, D. C.</p> <p>2018-04-01</p> <p>The question of whether grain <span class="hlt">boundaries</span> (GBs) in niobium can be responsible for lowered operating field (B RF) or quality factor (Q 0) in superconducting radio frequency (SRF) cavities is still controversial. Here, we show by direct DC transport across planar GBs isolated from a slice of very large-grain SRF-quality Nb that vortices can preferentially flow along the grain <span class="hlt">boundary</span> when the external magnetic field lies in the GB plane. However, increasing the misalignment between the GB plane and the external magnetic field vector markedly reduces preferential flux flow along the GB. Importantly, we find that preferential GB flux flow is more prominent for a buffered chemical polished than for an electropolished bi-crystal. The voltage-<span class="hlt">current</span> characteristics of GBs are similar to those seen in low angle grain <span class="hlt">boundaries</span> of high temperature superconductors where there is clear evidence of suppression of the superconducting order parameter at the GB. While local weakening of superconductivity at GBs in cuprates and pnictides is intrinsic, deterioration of <span class="hlt">current</span> transparency of GBs in Nb appears to be extrinsic, since the polishing method clearly affect the local GB degradation. The dependence of preferential GB flux flow on important cavity preparation and experimental variables, particularly the <span class="hlt">final</span> chemical treatment and the angle between the magnetic field and the GB plane, suggests two more reasons why real cavity performance can be so variable.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSPO51B..02R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSPO51B..02R"><span>The Influence of a Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> on Continental Shelf Processes Along Southeastern Australia.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roughan, M.</p> <p>2016-02-01</p> <p>The East Australian <span class="hlt">Current</span> (EAC) flows as a jet over the narrow shelf of southeastern Australia, dominating shelf circulation, and shedding vast eddies at the highly variable separation point. These characteristics alone make it a dynamically challenging region to measure, model and predict. In recent years a significant effort has been placed on understanding continental shelf processes along the coast of SE Australia, adjacent to the EAC, our major Western <span class="hlt">Boundary</span> <span class="hlt">Current</span>. We have used a multi-pronged approach by combining state of the art in situ observations and data assimilation modelling. Observations are obtained from a network of moorings, HF Radar and ocean gliders deployed in shelf waters along SE Australia, made possible through Australia's Integrated Marine Observing System (IMOS). In addition, we have developed a high resolution reanalysis of the East Australian <span class="hlt">Current</span> using ROMS and 4DVar data Assimilation. In addition to the traditional data streams (SST, SSH and ARGO) we assimilate the newly available IMOS observations in the region. These include velocity and hydrographic observations from the EAC transport array, 1km HF radar measurements of surface <span class="hlt">currents</span>, CTD casts from ocean gliders, and temperature, salinity and velocity measurements from a network of shelf mooring arrays. We use these vast data sets and numerical modelling tools combined with satellite remote sensed data to understand spatio-temporal variability of shelf processes and water mass distributions on synoptic, seasonal and inter-annual timescales. We have quantified the cross shelf transport variability inshore of the EAC, the driving mechanisms, the seasonal cycles in shelf waters and to some extent variability in the biological (phytoplankton) response. I will present a review of some of the key results from a number of recent studies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14..470V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14..470V"><span>First studies of bottom <span class="hlt">boundary</span> <span class="hlt">currents</span> in the Ría de Vigo (NW Iberian upwelling system)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Villacieros-Robineau, N.; Herrera, J. H.; Castro, C. G.; Piedracoba, S.; Rosón, G.</p> <p>2012-04-01</p> <p>The NW Iberian Upwelling system has a set of physical and chemical characteristics that determine the ecology at the coast, specifically inside the Rías Baixas where activities like raft culture have a significant weight in the local economy. Although several studies have dealt with the physical processes driving the rías general circulation, no previous research has faced the study of bottom <span class="hlt">boundary</span> <span class="hlt">currents</span>. This work studies the behavior of bottom <span class="hlt">currents</span> inside the Rías Baixas and identifies their possible forcing mechanism. For tackling this issue, high resolution time series of bottom <span class="hlt">currents</span> by means of a downwards looking ADCP (3-5 meters above the bottom) were recorded at one site in the Ría de Vigo covering the four seasons of the climate year 2004 - 2005. Our analysis shows that most of the time (aprox. 70 -80%), the bottom <span class="hlt">currents</span> respond to a logarithmic profile being possible to apply the law of the wall. This pattern can be applied to the residual component and also to the tidal component of the <span class="hlt">currents</span>. Based on this logarithmic fit, we have obtained characteristic parameters like shear stress and shear velocity. Our results point to a coupling among shear stress, shelf winds and runoff. Other important conclusion is the relative importance of tidal shear stress versus residual shear stress because the typical assumption of tidal has more influence is not true always. In some occasions when there are neap tides and high shelf winds the residual stress could be just three times the tidal ones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1172948','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1172948"><span>Discovering the Role of Grain <span class="hlt">Boundary</span> Complexions in Materials</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>Harmer, Martin P.</p> <p></p> <p>Grain <span class="hlt">boundaries</span> are inherently an area of disorder in polycrystalline materials which define the transport and various other material properties. The relationship between the interfacial chemistry, structure and the material properties is not well understood. Among the various taxonomies for grain <span class="hlt">boundaries</span>, Grain <span class="hlt">Boundary</span> Complexion is a relatively new conceptual scheme that relates the structure and kinetic properties of grain <span class="hlt">boundaries</span>. In this classification scheme, grain <span class="hlt">boundaries</span> are considered to be distinct three dimensional (the thickness being considerably smaller as compared to the other two dimensions but nonetheless discernible) equilibrium thermodynamic phases abutted between two crystalline phases. The stability andmore » structure of these interfacial phases are dictated by various thermodynamic variables such as temperature, stress (pressure), interfacial chemistry (chemical potential) and most importantly by the energies of the adjoining crystal surfaces. These phases are only stable within the constraint of the adjoining grains. Although these interfacial phases are not stable in bulk form, they can transform from one complexion to another as a function of various thermodynamic variables analogous to the behavior of bulk phases. Examples of different complexions have been reported in various publications. However, a systematic investigation exploring the existence of grain <span class="hlt">boundary</span> complexions in material systems other than alumina remains to be done. Although the role of interfacial chemistry on grain <span class="hlt">boundary</span> complexions in alumina has been addressed, a clear understanding of the underlying thermodynamics governing complexion formation is lacking. <span class="hlt">Finally</span>, the effects of grain <span class="hlt">boundary</span> complexions in bulk material properties are widely unknown. Factors above urge a thorough exploration of grain <span class="hlt">boundary</span> complexions in a range of different materials systems The purpose of the <span class="hlt">current</span> program is to verify the existence of grain <span class="hlt">boundary</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960050129','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960050129"><span>A Model for Axial Magnetic Bearings Including Eddy <span class="hlt">Currents</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kucera, Ladislav; Ahrens, Markus</p> <p>1996-01-01</p> <p>This paper presents an analytical method of modelling eddy <span class="hlt">currents</span> inside axial bearings. The problem is solved by dividing an axial bearing into elementary geometric forms, solving the Maxwell equations for these simplified geometries, defining <span class="hlt">boundary</span> conditions and combining the geometries. The <span class="hlt">final</span> result is an analytical solution for the flux, from which the impedance and the force of an axial bearing can be derived. Several impedance measurements have shown that the analytical solution can fit the measured data with a precision of approximately 5%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996ApPhL..69.1755S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996ApPhL..69.1755S"><span>Simulation of electron transport across charged grain <span class="hlt">boundaries</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Srikant, V.; Clarke, D. R.; Evans, P. V.</p> <p>1996-09-01</p> <p>The I-V (<span class="hlt">current</span> density-electric field) characteristics of low-angle grain <span class="hlt">boundaries</span> consisting of periodic arrays of charged dislocations are computed using a quasiclassical molecular dynamics approach. Below a critical value of the grain <span class="hlt">boundary</span> misorientation, the computed I-V characteristics are linear whereas above they are nonlinear. The degree of nonlinearity and the voltage onset of nonlinearity are found to be dependent on the grain <span class="hlt">boundary</span> misorientation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015DSRI..100..105E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015DSRI..100..105E"><span>Characterising primary productivity measurements across a dynamic western <span class="hlt">boundary</span> <span class="hlt">current</span> region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Everett, Jason D.; Doblin, Martina A.</p> <p>2015-06-01</p> <p>Determining the magnitude of primary production (PP) in a changing ocean is a major research challenge. Thousands of estimates of marine PP exist globally, but there remain significant gaps in data availability, particularly in the Southern Hemisphere. In situ PP estimates are generally single-point measurements and therefore we rely on satellite models of PP in order to scale up over time and space. To reduce the uncertainty around the model output, these models need to be assessed against in situ measurements before use. This study examined the vertically-integrated productivity in four water-masses associated with the East Australian <span class="hlt">Current</span> (EAC), the major western <span class="hlt">boundary</span> <span class="hlt">current</span> (WBC) of the South Pacific. We calculated vertically integrated PP from shipboard 14C PP estimates and then compared them to estimates from four commonly used satellite models (ESQRT, VGPM, VGPM-Eppley, VGPM-Kameda) to assess their utility for this region. Vertical profiles of the water-column show each water-mass had distinct temperature-salinity signatures. The depth of the fluorescence-maximum (fmax) increased from onshore (river plume) to offshore (EAC) as light penetration increased. Depth integrated PP was highest in river plumes (792±181 mg C m-2 d-1) followed by the EAC (534±116 mg C m-2 d-1), continental shelf (140±47 mg C m-2 d-1) and cyclonic eddy waters (121±4 mg C m-2 d-1). Surface carbon assimilation efficiency was greatest in the EAC (301±145 mg C (mg Chl-a)-1 d-1) compared to other water masses. All satellite primary production models tested underestimated EAC PP and overestimated continental shelf PP. The ESQRT model had the highest skill and lowest bias of the tested models, providing the best first-order estimates of PP on the continental shelf, including at a coastal time-series station, Port Hacking, which showed considerable inter-annual variability (155-2957 mg C m-2 d-1). This work provides the first estimates of depth integrated PP associated with the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005EL.....72..341G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005EL.....72..341G"><span>Generic short-time propagation of sharp-<span class="hlt">boundaries</span> wave packets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Granot, E.; Marchewka, A.</p> <p>2005-11-01</p> <p>A general solution to the "shutter" problem is presented. The propagation of an arbitrary initially bounded wave function is investigated, and the general solution for any such function is formulated. It is shown that the exact solution can be written as an expression that depends only on the values of the function (and its derivatives) at the <span class="hlt">boundaries</span>. In particular, it is shown that at short times (t << 2mx2/hbar, where x is the distance to the <span class="hlt">boundaries</span>) the wave function propagation depends only on the wave function's values (or its derivatives) at the <span class="hlt">boundaries</span> of the region. <span class="hlt">Finally</span>, we generalize these findings to a non-singular wave function (i.e., for wave packets with finite-width <span class="hlt">boundaries</span>) and suggest an experimental verification.</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('http://adsabs.harvard.edu/abs/2013AGUFMMR33C..06M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMMR33C..06M"><span>Grain <span class="hlt">boundary</span> diffusion in olivine (Invited)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marquardt, K.; Dohmen, R.</p> <p>2013-12-01</p> <p>. Grain <span class="hlt">boundary</span> diffusion perpendicular to the dislocation lines of the small angle grain <span class="hlt">boundaries</span> proved to be about an order of magnitude faster than volume diffusion, whereas diffusion in high angle grain <span class="hlt">boundaries</span> is several orders of magnitude faster. We will discuss the variation of element diffusion rates with grain <span class="hlt">boundary</span> orientation and the temperature- and/or time-induced transition from one diffusion regime to the next regime. This is done using time series experiments and two-dimensional grain <span class="hlt">boundary</span> diffusion simulations. <span class="hlt">Finally</span>, we will debate the differences between our data and other data sets that result from different experimental setups, conditions and analyses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080023461','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080023461"><span>Infrared Imaging of <span class="hlt">Boundary</span> Layer Transition Flight Experiments</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Berry, Scott A.; Horvath, Thomas J., Jr.; Schwartz, Richard; Ross, Martin; Anderson, Brian; Campbell, Charles H.</p> <p>2008-01-01</p> <p>The Hypersonic Thermodynamic Infrared Measurement (HYTHIRM) project is presently focused on near term support to the Shuttle program through the development of an infrared imaging capability of sufficient spatial and temporal resolution to augment existing on-board Orbiter instrumentation. Significant progress has been made with the identification and inventory of relevant existing optical imaging assets and the development, maturation, and validation of simulation and modeling tools for assessment and mission planning purposes, which were intended to lead to the best strategies and assets for successful acquisition of quantitative global surface temperature data on the Shuttle during entry. However, there are longer-term goals of providing global infrared imaging support to other flight projects as well. A status of HYTHIRM from the perspective of how two NASA-sponsored <span class="hlt">boundary</span> layer transition flight experiments could benefit by infrared measurements is provided. Those two flight projects are the Hypersonic <span class="hlt">Boundary</span> layer Transition (HyBoLT) flight experiment and the Shuttle <span class="hlt">Boundary</span> Layer Transition Flight Experiment (BLT FE), which are both intended for reducing uncertainties associated with the extrapolation of wind tunnel derived transition correlations for flight application. Thus, the criticality of obtaining high quality flight data along with the impact it would provide to the Shuttle program damage assessment process are discussed. Two recent wind tunnel efforts that were intended as risk mitigation in terms of quantifying the transition process and resulting turbulent wedge locations are briefly reviewed. Progress is being made towards <span class="hlt">finalizing</span> an imaging strategy in support of the Shuttle BLT FE, however there are no plans <span class="hlt">currently</span> to image HyBoLT.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS.979a2071P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS.979a2071P"><span>Prediction of Tidal Elevations and Barotropic <span class="hlt">Currents</span> in the Gulf of Bone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Purnamasari, Rika; Ribal, Agustinus; Kusuma, Jeffry</p> <p>2018-03-01</p> <p>Tidal elevation and barotropic <span class="hlt">current</span> predictions in the gulf of Bone have been carried out in this work based on a two-dimensional, depth-integrated Advanced Circulation (ADCIRC-2DDI) model for 2017. Eight tidal constituents which were obtained from FES2012 have been imposed along the open <span class="hlt">boundary</span> conditions. However, even using these very high-resolution tidal constituents, the discrepancy between the model and the data from tide gauge is still very high. In order to overcome such issues, Green’s function approach has been applied which reduced the root-mean-square error (RMSE) significantly. Two different starting times are used for predictions, namely from 2015 and 2016. After improving the open <span class="hlt">boundary</span> conditions, RMSE between observation and model decreased significantly. In fact, RMSEs for 2015 and 2016 decreased 75.30% and 88.65%, respectively. Furthermore, the prediction for tidal elevations as well as tidal <span class="hlt">current</span>, which is barotropic <span class="hlt">current</span>, is carried out. This prediction was compared with the prediction conducted by Geospatial Information Agency (GIA) of Indonesia and we found that our prediction is much better than one carried out by GIA. <span class="hlt">Finally</span>, since there is no tidal <span class="hlt">current</span> observation available in this area, we assume that, when tidal elevations have been fixed, then the tidal <span class="hlt">current</span> will approach the actual <span class="hlt">current</span> velocity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900042236&hterms=gaussian+elimination&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dgaussian%2Belimination','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900042236&hterms=gaussian+elimination&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dgaussian%2Belimination"><span>Parallel computation using <span class="hlt">boundary</span> elements in solid mechanics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chien, L. S.; Sun, C. T.</p> <p>1990-01-01</p> <p>The inherent parallelism of the <span class="hlt">boundary</span> element method is shown. The <span class="hlt">boundary</span> element is formulated by assuming the linear variation of displacements and tractions within a line element. Moreover, MACSYMA symbolic program is employed to obtain the analytical results for influence coefficients. Three computational components are parallelized in this method to show the speedup and efficiency in computation. The global coefficient matrix is first formed concurrently. Then, the parallel Gaussian elimination solution scheme is applied to solve the resulting system of equations. <span class="hlt">Finally</span>, and more importantly, the domain solutions of a given <span class="hlt">boundary</span> value problem are calculated simultaneously. The linear speedups and high efficiencies are shown for solving a demonstrated problem on Sequent Symmetry S81 parallel computing system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://edg.epa.gov/metadata/catalog/search/resource/details.page?uuid=%7BD18EB5BA-3FF0-4A2C-93CF-B2A9316FD69F%7D','PESTICIDES'); return false;" href="https://edg.epa.gov/metadata/catalog/search/resource/details.page?uuid=%7BD18EB5BA-3FF0-4A2C-93CF-B2A9316FD69F%7D"><span>Tribal <span class="hlt">Boundaries</span>, U.S., 2014, EPA/OAR/OAQPS/AQAD</span></a></p> <p><a target="_blank" href="http://www.epa.gov/pesticides/search.htm">EPA Pesticide Factsheets</a></p> <p></p> <p></p> <p>This web service contains a layer depicting the union of TigerWEB AIANNHA map service layers 2 (Federal American Indian Reservations) and 3 (Off-Reservation Trust Lands) located at https://tigerweb.geo.census.gov/arcgis/rest/services/TIGERweb/AIANNHA/MapServerFederal (federal AIRs) are areas that have been set aside by the United States for the use of tribes, the exterior <span class="hlt">boundaries</span> of which are more particularly defined in the <span class="hlt">final</span> tribal treaties, agreements, executive orders, federal statutes, secretarial orders, or judicial determinations. The Bureau of Indian Affairs maintains a list of all federally recognized tribal governments and makes <span class="hlt">final</span> determination of the inventory federal AIRs. The Census Bureau recognizes federal reservations (and associated off-reservation trust lands) as territory over which American Indian tribes have primary governmental authority. American Indian reservations can be legally described as colonies, communities, Indian colonies, Indian communities, Indian rancheria, Indian reservations, Indian villages, pueblos, rancherias, ranches, reservations, reserves, settlements, or villages. The Census Bureau contacts representatives of American Indian tribal governments to identify the <span class="hlt">boundaries</span> for federal reservations through its annual <span class="hlt">Boundary</span> and Annexation Survey. Federal reservations may cross state and all other area <span class="hlt">boundaries</span>.State (state AIRs) are reservations established by some state governments for tribes recognized by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/355064-net-current-control-device-final-report','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/355064-net-current-control-device-final-report"><span>Net <span class="hlt">current</span> control device. <span class="hlt">Final</span> 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>Fugate, D.; Cooper, J.H.</p> <p>1998-11-01</p> <p>Net <span class="hlt">currents</span> generally result in elevated magnetic fields because the alternate paths are distant from the circuit conductors. Investigations have shown that one of the primary sources of power frequency magnetic fields in residential buildings is <span class="hlt">currents</span> that return to their source via paths other than the neutral conductors. As part of EPRI`s Magnetic Field Shielding Project, ferromagnetic devices, called net <span class="hlt">current</span> control (NCC) devices, were developed and tested for use in reducing net <span class="hlt">currents</span> on electric power cables and the resulting magnetic fields. Applied to a residential service drop, an NCC device reduces net <span class="hlt">current</span> by forcing <span class="hlt">current</span> offmore » local non-utility ground paths, and back onto the neutral conductor. Circuit models and basic design equations for the NCC concept were developed, and proof-of-principles tests were carried out on an actual residence with cooperation from the local utility. After proving the basic concepts, three prototype NCC devices were built and tested on a simulated neighborhood power system. Additional prototypes were built for testing by interested EPRI utility members. Results have shown that the NCC prototypes installed on residential service drops reduce net <span class="hlt">currents</span> to milliampere levels with compromising the safety of the ground system. Although the focus was on application to residential service cables, the NCC concept is applicable to single-phase and three-phase distribution systems as well.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25019882','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25019882"><span><span class="hlt">Boundary</span> streaming with Navier <span class="hlt">boundary</span> condition.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xie, Jin-Han; Vanneste, Jacques</p> <p>2014-06-01</p> <p>In microfluidic applications involving high-frequency acoustic waves over a solid <span class="hlt">boundary</span>, the Stokes <span class="hlt">boundary</span>-layer thickness δ is so small that some non-negligible slip may occur at the fluid-solid interface. This paper assesses the impact of this slip by revisiting the classical problem of steady acoustic streaming over a flat <span class="hlt">boundary</span>, replacing the no-slip <span class="hlt">boundary</span> condition with the Navier condition u|_{y=0}=L_{s}∂_{y}u|_{y=0}, where u is the velocity tangent to the <span class="hlt">boundary</span> y=0, and the parameter L_{s} is the slip length. A general expression is obtained for the streaming velocity across the <span class="hlt">boundary</span> layer as a function of the dimensionless parameter L_{s}/δ. The limit outside the <span class="hlt">boundary</span> layer provides an effective slip velocity satisfied by the interior mean flow. Particularizing to traveling and standing waves shows that the <span class="hlt">boundary</span> slip respectively increases and decreases the streaming velocity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015IJASE...7..143R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015IJASE...7..143R"><span><span class="hlt">Boundary</span> element analysis of post-tensioned slabs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rashed, Youssef F.</p> <p>2015-06-01</p> <p>In this paper, the <span class="hlt">boundary</span> element method is applied to carry out the structural analysis of post-tensioned flat slabs. The shear-deformable plate-bending model is employed. The effect of the pre-stressing cables is taken into account via the equivalent load method. The formulation is automated using a computer program, which uses quadratic <span class="hlt">boundary</span> elements. Verification samples are presented, and <span class="hlt">finally</span> a practical application is analyzed where results are compared against those obtained from the finite element method. The proposed method is efficient in terms of computer storage and processing time as well as the ease in data input and modifications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3941019','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3941019"><span>Ferroelectric translational antiphase <span class="hlt">boundaries</span> in nonpolar materials</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wei, Xian-Kui; Tagantsev, Alexander K.; Kvasov, Alexander; Roleder, Krystian; Jia, Chun-Lin; Setter, Nava</p> <p>2014-01-01</p> <p>Ferroelectric materials are heavily used in electro-mechanics and electronics. Inside the ferroelectric, domain walls separate regions in which the spontaneous polarization is differently oriented. Properties of ferroelectric domain walls can differ from those of the domains themselves, leading to new exploitable phenomena. Even more exciting is that a non-ferroelectric material may have domain <span class="hlt">boundaries</span> that are ferroelectric. Many materials possess translational antiphase <span class="hlt">boundaries</span>. Such <span class="hlt">boundaries</span> could be interesting entities to carry information if they were ferroelectric. Here we show first that antiphase <span class="hlt">boundaries</span> in antiferroelectrics may possess ferroelectricity. We then identify these <span class="hlt">boundaries</span> in the classical antiferroelectric lead zirconate and evidence their polarity by electron microscopy using negative spherical-aberration imaging technique. Ab initio modelling confirms the polar bi-stable nature of the walls. Ferroelectric antiphase <span class="hlt">boundaries</span> could make high-density non-volatile memory; in comparison with the magnetic domain wall memory, they do not require <span class="hlt">current</span> for operation and are an order of magnitude thinner. PMID:24398704</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860038155&hterms=destiny&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Ddestiny','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860038155&hterms=destiny&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Ddestiny"><span>Destiny of earthward streaming plasma in the plasmasheet <span class="hlt">boundary</span> layer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Green, J. L.; Horwitz, J. L.</p> <p>1986-01-01</p> <p>The dynamics of the earth's magnetotail have been investigated, and it has become clear that the plasmasheet <span class="hlt">boundary</span> layer field lines map into the Region I Field-Aligned <span class="hlt">Currents</span> (FAC) of the auroral zone. It is pointed out that the role of earthward streaming ions in the plasmasheet <span class="hlt">boundary</span> layer may be of fundamental importance in the understanding of magnetotail dynamics, auroral zone physics, and especially for ionospheric-magnetospheric interactions. The present paper has the objective to evaluate propagation characteristics for the earthward streaming ions observed in the plasmasheet <span class="hlt">boundary</span> layer. An investigation is conducted of the propagation characteristics of protons in the plasmasheet <span class="hlt">boundary</span> layer using independent single particle dynamics, and conclusions are discussed. The density of earthward streaming ions found in the plasmasheet <span class="hlt">boundary</span> layer should include the ring <span class="hlt">current</span> as well as the auroral zone precipitaiton and inner plasmasheet regions of the magnetosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5217449-boundary-boundary-principle-field-theories-issue-austerity-laws-physics','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5217449-boundary-boundary-principle-field-theories-issue-austerity-laws-physics"><span>The <span class="hlt">boundary</span> of a <span class="hlt">boundary</span> principle in field theories and the issue of austerity of the laws of physics</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>Kheyfets, A.; Miller, W.A.</p> <p></p> <p>The <span class="hlt">boundary</span> of a <span class="hlt">boundary</span> principle has been suggested by J. A. Wheeler as a realization of the austerity idea in field theories. This principle is described in three basic field theories---electrodynamics, Yang--Mills theory, and general relativity. It is demonstrated that it supplies a unified geometric interpretation of the source <span class="hlt">current</span> in each of the three theories in terms of a generalized E. Cartan moment of rotation. The extent to which the <span class="hlt">boundary</span> of a <span class="hlt">boundary</span> principle represents the austerity principle is discussed. It is concluded that it works in a way analogous to thermodynamic relations and it is arguedmore » that deeper principles might be needed to comprehend the nature of austerity.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991JMP....32.3168K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991JMP....32.3168K"><span>The <span class="hlt">boundary</span> of a <span class="hlt">boundary</span> principle in field theories and the issue of austerity of the laws of physics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kheyfets, Arkady; Miller, Warner A.</p> <p>1991-11-01</p> <p>The <span class="hlt">boundary</span> of a <span class="hlt">boundary</span> principle has been suggested by J. A. Wheeler as a realization of the austerity idea in field theories. This principle is described in three basic field theories—electrodynamics, Yang-Mills theory, and general relativity. It is demonstrated that it supplies a unified geometric interpretation of the source <span class="hlt">current</span> in each of the three theories in terms of a generalized E. Cartan moment of rotation. The extent to which the <span class="hlt">boundary</span> of a <span class="hlt">boundary</span> principle represents the austerity principle is discussed. It is concluded that it works in a way analogous to thermodynamic relations and it is argued that deeper principles might be needed to comprehend the nature of austerity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRC..123.2829H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRC..123.2829H"><span>The Deep Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> in the Labrador Sea From Observations and a High-Resolution Model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Handmann, Patricia; Fischer, Jürgen; Visbeck, Martin; Karstensen, Johannes; Biastoch, Arne; Böning, Claus; Patara, Lavinia</p> <p>2018-04-01</p> <p>Long-term observations from a 17 year long mooring array at the exit of the Labrador Sea at 53°N are compared to the output of a high-resolution model (VIKING20). Both are analyzed to define robust integral properties on basin and regional scale, which can be determined and evaluated equally well. While both, the observations and the model, show a narrow DWBC cyclonically engulfing the Labrador Sea, the model's <span class="hlt">boundary</span> <span class="hlt">current</span> system is more barotropic than in the observations and spectral analysis indicates stronger monthly to interannual transport variability. Compared to the model, the observations show a stronger density gradient, hence a stronger baroclinicity, from center to <span class="hlt">boundary</span>. Despite this, the observed temporal evolution of the temperature in the central Labrador Sea is reproduced. The model results yield a mean export of North Atlantic Deep Water (NADW) (33.0 ± 5.7 Sv), which is comparable to the observed transport (31.2 ± 5.5 Sv) at 53°N. The results also include a comparable spatial pattern and March mixed layer depth in the central Labrador Sea (maximum depth ˜2,000 m). During periods containing enhanced deep convection (1990s) our analyses show increased correlation between LSW and LNADW model transport at 53°N. Our results indicate that the transport variability in LSW and LNADW at 53°N is a result of a complex modulation of wind stress and buoyancy forcing on regional and basin wide scale.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97k5143R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97k5143R"><span>Unified bulk-<span class="hlt">boundary</span> correspondence for band insulators</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rhim, Jun-Won; Bardarson, Jens H.; Slager, Robert-Jan</p> <p>2018-03-01</p> <p>The bulk-<span class="hlt">boundary</span> correspondence, a topic of intensive research interest over the past decades, is one of the quintessential ideas in the physics of topological quantum matter. Nevertheless, it has not been proven in all generality and has in certain scenarios even been shown to fail, depending on the <span class="hlt">boundary</span> profiles of the terminated system. Here, we introduce bulk numbers that capture the exact number of in-gap modes, without any such subtleties in one spatial dimension. Similarly, based on these 1D bulk numbers, we define a new 2D winding number, which we call the pole winding number, that specifies the number of robust metallic surface bands in the gap as well as their topological character. The underlying general methodology relies on a simple continuous extrapolation from the bulk to the <span class="hlt">boundary</span>, while tracking the evolution of Green's function's poles in the vicinity of the bulk band edges. As a main result we find that all the obtained numbers can be applied to the known insulating phases in a unified manner regardless of the specific symmetries. Additionally, from a computational point of view, these numbers can be effectively evaluated without any gauge fixing problems. In particular, we directly apply our bulk-<span class="hlt">boundary</span> correspondence construction to various systems, including 1D examples without a traditional bulk-<span class="hlt">boundary</span> correspondence, and predict the existence of <span class="hlt">boundary</span> modes on various experimentally studied graphene edges, such as open <span class="hlt">boundaries</span> and grain <span class="hlt">boundaries</span>. <span class="hlt">Finally</span>, we sketch the 3D generalization of the pole winding number by in the context of topological insulators.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA493978','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA493978"><span>An Observational Study of the Kuroshio in the East China Sea: Local, Regional, and Basin-Wide Perspectives on a Western <span class="hlt">Boundary</span> <span class="hlt">Current</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2008-01-01</p> <p>a seamount (summit ~320 m depth); the northern section reaches ~460 m depth while the southern section reaches ~1400 m (Oka and Kawabe, 2003). East...AN OBSERVATIONAL STUDY OF THE KUROSHIO IN THE EAST CHINA SEA: LOCAL, REGIONAL, AND BASIN-WIDE PERSPECTIVES ON A WESTERN <span class="hlt">BOUNDARY</span> <span class="hlt">CURRENT</span>...BY MAGDALENA ANDRES A DISSERTATION SUBMITTED IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhRvB..91q4422L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhRvB..91q4422L"><span>Open Heisenberg chain under <span class="hlt">boundary</span> fields: A magnonic logic gate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Landi, Gabriel T.; Karevski, Dragi</p> <p>2015-05-01</p> <p>We study the spin transport in the quantum Heisenberg spin chain subject to <span class="hlt">boundary</span> magnetic fields and driven out of equilibrium by Lindblad dissipators. An exact solution is given in terms of matrix product states, which allows us to calculate exactly the spin <span class="hlt">current</span> for any chain size. It is found that the system undergoes a discontinuous spin-valve-like quantum phase transition from ballistic to subdiffusive spin <span class="hlt">current</span>, depending on the value of the <span class="hlt">boundary</span> fields. Thus, the chain behaves as an extremely sensitive magnonic logic gate operating with the <span class="hlt">boundary</span> fields as the base element.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910017151','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910017151"><span>The Kinematics of Turbulent <span class="hlt">Boundary</span> Layer Structure</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Robinson, Stephen Kern</p> <p>1991-01-01</p> <p>The long history of research into the internal structure of turbulent <span class="hlt">boundary</span> layers has not provided a unified picture of the physics responsible for turbulence production and dissipation. The goals of the present research are to: (1) define the <span class="hlt">current</span> state of <span class="hlt">boundary</span> layer structure knowledge; and (2) utilize direct numerical simulation results to help close the unresolved issues identified in part A and to unify the fragmented knowledge of various coherent motions into a consistent kinematic model of <span class="hlt">boundary</span> layer structure. The results of the <span class="hlt">current</span> study show that all classes of coherent motion in the low Reynolds number turbulent <span class="hlt">boundary</span> layer may be related to vortical structures, but that no single form of vortex is representative of the wide variety of vortical structures observed. In particular, ejection and sweep motions, as well as entrainment from the free-streem are shown to have strong spatial and temporal relationships with vortical structures. Disturbances of vortex size, location, and intensity show that quasi-streamwise vortices dominate the buffer region, while transverse vortices and vortical arches dominate the wake region. Both types of vortical structure are common in the log region. The interrelationships between the various structures and the population distributions of vortices are combined into a conceptual kinematic model for the <span class="hlt">boundary</span> layer. Aspects of vortical structure dynamics are also postulated, based on time-sequence animations of the numerically simulated flow.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3265378','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3265378"><span>Advantageous grain <span class="hlt">boundaries</span> in iron pnictide superconductors</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Katase, Takayoshi; Ishimaru, Yoshihiro; Tsukamoto, Akira; Hiramatsu, Hidenori; Kamiya, Toshio; Tanabe, Keiichi; Hosono, Hideo</p> <p>2011-01-01</p> <p>High critical temperature superconductors have zero power consumption and could be used to produce ideal electric power lines. The principal obstacle in fabricating superconducting wires and tapes is grain boundaries—the misalignment of crystalline orientations at grain <span class="hlt">boundaries</span>, which is unavoidable for polycrystals, largely deteriorates critical <span class="hlt">current</span> density. Here we report that high critical temperature iron pnictide superconductors have advantages over cuprates with respect to these grain <span class="hlt">boundary</span> issues. The transport properties through well-defined bicrystal grain <span class="hlt">boundary</span> junctions with various misorientation angles (θGB) were systematically investigated for cobalt-doped BaFe2As2 (BaFe2As2:Co) epitaxial films fabricated on bicrystal substrates. The critical <span class="hlt">current</span> density through bicrystal grain <span class="hlt">boundary</span> (JcBGB) remained high (>1 MA cm−2) and nearly constant up to a critical angle θc of ∼9°, which is substantially larger than the θc of ∼5° for YBa2Cu3O7–δ. Even at θGB>θc, the decay of JcBGB was much slower than that of YBa2Cu3O7–δ. PMID:21811238</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20080037569','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20080037569"><span><span class="hlt">Boundary</span>-Layer-Ingesting Inlet Flow Control</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Owens, Lewis R.; Allan, Brian G.; Gorton, Susan A.</p> <p>2008-01-01</p> <p>An experimental study was conducted to provide the first demonstration of an active flow control system for a flush-mounted inlet with significant <span class="hlt">boundary</span>-layer-ingestion in transonic flow conditions. The effectiveness of the flow control in reducing the circumferential distortion at the engine fan-face location was assessed using a 2.5%-scale model of a <span class="hlt">boundary</span>-layer-ingesting offset diffusing inlet. The inlet was flush mounted to the tunnel wall and ingested a large <span class="hlt">boundary</span> layer with a <span class="hlt">boundary</span>-layer-to-inlet height ratio of 35%. Different jet distribution patterns and jet mass flow rates were used in the inlet to control distortion. A vane configuration was also tested. <span class="hlt">Finally</span> a hybrid vane/jet configuration was tested leveraging strengths of both types of devices. Measurements were made of the onset <span class="hlt">boundary</span> layer, the duct surface static pressures, and the mass flow rates through the duct and the flow control actuators. The distortion and pressure recovery were measured at the aerodynamic interface plane. The data show that control jets and vanes reduce circumferential distortion to acceptable levels. The point-design vane configuration produced higher distortion levels at off-design settings. The hybrid vane/jet flow control configuration reduced the off-design distortion levels to acceptable ones and used less than 0.5% of the inlet mass flow to supply the jets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22596716-electric-field-domain-boundary-instability-weakly-coupled-semiconductor-superlattices','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22596716-electric-field-domain-boundary-instability-weakly-coupled-semiconductor-superlattices"><span>Electric-field domain <span class="hlt">boundary</span> instability in weakly coupled semiconductor superlattices</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>Rasulova, G. K., E-mail: rasulova@sci.lebedev.ru; Pentin, I. V.; Brunkov, P. N.</p> <p>2016-05-28</p> <p>Damped oscillations of the <span class="hlt">current</span> were observed in the transient <span class="hlt">current</span> pulse characteristics of a 30-period weakly coupled GaAs/AlGaAs superlattice (SL). The switching time of the <span class="hlt">current</span> is exponentially decreased as the voltage is verged towards the <span class="hlt">current</span> discontinuity region indicating that the space charge necessary for the domain <span class="hlt">boundary</span> formation is gradually accumulated in a certain SL period in a timescale of several hundreds ns. The spectral features in the electroluminescence spectra of two connected in parallel SL mesas correspond to the energy of the intersubband transitions and the resonance detuning of subbands caused by charge trapping in themore » quantum wells (QWs) residing in a region of the expanded domain <span class="hlt">boundary</span>. The obtained results support our understanding of the origin of self-oscillations as a cyclic dynamics of the subband structure in the QWs forming the expanded domain <span class="hlt">boundary</span>.« 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_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('https://www.ncbi.nlm.nih.gov/pubmed/29298139','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29298139"><span>The Bottom <span class="hlt">Boundary</span> Layer.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Trowbridge, John H; Lentz, Steven J</p> <p>2018-01-03</p> <p>The oceanic bottom <span class="hlt">boundary</span> layer extracts energy and momentum from the overlying flow, mediates the fate of near-bottom substances, and generates bedforms that retard the flow and affect benthic processes. The bottom <span class="hlt">boundary</span> layer is forced by winds, waves, tides, and buoyancy and is influenced by surface waves, internal waves, and stratification by heat, salt, and suspended sediments. This review focuses on the coastal ocean. The main points are that (a) classical turbulence concepts and modern turbulence parameterizations provide accurate representations of the structure and turbulent fluxes under conditions in which the underlying assumptions hold, (b) modern sensors and analyses enable high-quality direct or near-direct measurements of the turbulent fluxes and dissipation rates, and (c) the remaining challenges include the interaction of waves and <span class="hlt">currents</span> with the erodible seabed, the impact of layer-scale two- and three-dimensional instabilities, and the role of the bottom <span class="hlt">boundary</span> layer in shelf-slope exchange.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ARMS...10..397T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ARMS...10..397T"><span>The Bottom <span class="hlt">Boundary</span> Layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Trowbridge, John H.; Lentz, Steven J.</p> <p>2018-01-01</p> <p>The oceanic bottom <span class="hlt">boundary</span> layer extracts energy and momentum from the overlying flow, mediates the fate of near-bottom substances, and generates bedforms that retard the flow and affect benthic processes. The bottom <span class="hlt">boundary</span> layer is forced by winds, waves, tides, and buoyancy and is influenced by surface waves, internal waves, and stratification by heat, salt, and suspended sediments. This review focuses on the coastal ocean. The main points are that (a) classical turbulence concepts and modern turbulence parameterizations provide accurate representations of the structure and turbulent fluxes under conditions in which the underlying assumptions hold, (b) modern sensors and analyses enable high-quality direct or near-direct measurements of the turbulent fluxes and dissipation rates, and (c) the remaining challenges include the interaction of waves and <span class="hlt">currents</span> with the erodible seabed, the impact of layer-scale two- and three-dimensional instabilities, and the role of the bottom <span class="hlt">boundary</span> layer in shelf-slope exchange.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2010-02-19/pdf/2010-3127.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2010-02-19/pdf/2010-3127.pdf"><span>75 FR 7522 - United States Section; Notice of Availability of the <span class="hlt">Final</span> Environmental Impact Statement, Flood...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2010-02-19</p> <p>... <span class="hlt">Final</span> EIS: Biological resources, cultural resources, water resources, land use, socioeconomic resources... INTERNATIONAL <span class="hlt">BOUNDARY</span> AND WATER COMMISSION, UNITED STATES AND MEXICO United States Section..., International <span class="hlt">Boundary</span> and Water Commission (USIBWC). ACTION: Notice of Availability of <span class="hlt">Final</span> Environmental...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1132214-intra-variant-substructure-nimnga-martensite-conjugation-boundaries','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1132214-intra-variant-substructure-nimnga-martensite-conjugation-boundaries"><span>Intra-variant substructure in Ni–Mn–Ga martensite: Conjugation <span class="hlt">boundaries</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>Muntifering, B.; Pond, R. C.; Kovarik, L.</p> <p>2014-06-01</p> <p>The microstructure of a Ni–Mn–Ga alloy in the martensitic phase was investigated using transmission electron microscopy. Inter-variant twin <span class="hlt">boundaries</span> were observed separating non-modulated tetragonal martensite variants. In addition, intra-variant <span class="hlt">boundary</span> structures, referred to here as “conjugation boundaries”, were also observed. We propose that conjugation <span class="hlt">boundaries</span> originate at the transformation interface between austenite and a nascent martensite variant. In the alloy studied, deformation twinning was observed, consistent with being the mode of lattice-invariant deformation, and this can occur on either of two crystallographically equivalent conjugate View the MathML source{101}(101⁻) twinning systems: conjugation <span class="hlt">boundaries</span> separate regions within a single variant in whichmore » the active modes were distinct. The defect structure of conjugation <span class="hlt">boundaries</span> and the low-angle of misorientation across them are revealed in detail using high-resolution microscopy. <span class="hlt">Finally</span>, we anticipate that the mobility of such <span class="hlt">boundaries</span> is lower than that of inter-variant <span class="hlt">boundaries</span>, and is therefore likely to significantly affect the kinetics of deformation in the martensitic phase.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017OcMod.114....1R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017OcMod.114....1R"><span>A comparison of the structure, properties, and water mass composition of quasi-isotropic eddies in western <span class="hlt">boundary</span> <span class="hlt">currents</span> in an eddy-resolving ocean model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rykova, Tatiana; Oke, Peter R.; Griffin, David A.</p> <p>2017-06-01</p> <p>Using output from a near-global eddy-resolving ocean model, we analyse the properties and characteristics of quasi-isotropic eddies in five Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> (WBC) regions, including the extensions of the Agulhas, East Australian <span class="hlt">Current</span> (EAC), Brazil-Malvinas Confluence (BMC), Kuroshio and Gulf Stream regions. We assess the model eddies by comparing to satellite and in situ observations, and show that most aspects of the model's representation of eddies are realistic. We find that the mean eddies differ dramatically between these WBC regions - all with some unique and noteworthy characteristics. We find that the vertical displacement of isopycnals of Agulhas eddies is the greatest, averaging 350-450 m at depths of over 800-900 m. EAC (BMC) eddies are the least (most) barotropic, with only 50% (85-90%) of the velocity associated with the barotropic mode. Kuroshio eddies are the most stratified, resulting in small isopycnal displacement, even for strong eddies; and Gulf Stream eddies carry the most heat. Despite their differences, we explicitly show that the source waters for anticyclonic eddies are a mix of the WBC water (from the <span class="hlt">boundary</span> <span class="hlt">current</span> itself) and water that originates equatorward of the WBC eddy-field; and cyclonic eddies are a mix of WBC water and water that originates poleward of the WBC eddy-field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhFl...22d5102E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhFl...22d5102E"><span>Diffusion of drag-reducing polymer solutions within a rough-walled turbulent <span class="hlt">boundary</span> layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Elbing, Brian R.; Dowling, David R.; Perlin, Marc; Ceccio, Steven L.</p> <p>2010-04-01</p> <p>The influence of surface roughness on diffusion of wall-injected, drag-reducing polymer solutions within a turbulent <span class="hlt">boundary</span> layer was studied with a 0.94 m long flat-plate test model at speeds of up to 10.6 m s-1 and Reynolds numbers of up to 9×106. The surface was hydraulically smooth, transitionally rough, or fully rough. Mean concentration profiles were acquired with planar laser induced fluorescence, which was the primary flow diagnostic. Polymer concentration profiles with high injection concentrations (≥1000 wppm) had the peak concentration shifted away from the wall, which was partially attributed to a lifting phenomenon. The diffusion process was divided into three zones—initial, intermediate, and <span class="hlt">final</span>. Studies of polymer injection into a polymer ocean at concentrations sufficient for maximum drag reduction indicated that the maximum initial zone length is of the order of 100 <span class="hlt">boundary</span> layer thicknesses. The intermediate zone results indicate that friction velocity and roughness height are important scaling parameters in addition to flow and injection conditions. Lastly, the <span class="hlt">current</span> results were combined with those in Petrie et al. ["Polymer drag reduction with surface roughness in flat-plate turbulent <span class="hlt">boundary</span> layer flow," Exp. Fluids 35, 8 (2003)] to demonstrate that the influence of polymer degradation increases with increased surface roughness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA087028','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA087028"><span>Stability of <span class="hlt">Boundary</span> Layer Flow.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1980-03-01</p> <p>climato- logical frequency of convection in the North Atlantic, and offered recom- U mendations on the modelling of triggered convection. The <span class="hlt">current</span> ...support of the <span class="hlt">current</span> investigation we have carried out several additional calculations of the marine <span class="hlt">boundary</span> layer with SIGMET. These calculations...In a fixed coordinate system x ( positive eastward), y ( positive northward), and z ( positive vertically upward) the equations are au .U +vE + W+-U</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1236497','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1236497"><span>Clouds, Aerosol, and Precipitation in the Marine <span class="hlt">Boundary</span> Layer (CAP-MBL) <span class="hlt">Final</span> Campaign 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>Wood, R.</p> <p>2016-01-01</p> <p>The extensive coverage of low clouds over the subtropical eastern oceans greatly impacts the <span class="hlt">current</span> climate. In addition, the response of low clouds to changes in atmospheric greenhouse gases and aerosols is a major source of uncertainty, which thwarts accurate prediction of future climate change. Low clouds are poorly simulated in climate models, partly due to inadequate long-term simultaneous observations of their macrophysical and microphysical structure, radiative effects, and associated aerosol distribution in regions where their impact is greatest. The thickness and extent of subtropical low clouds is dependent on tight couplings between surface fluxes of heat and moisture, radiativemore » cooling, <span class="hlt">boundary</span> layer turbulence, and precipitation (much of which evaporates before reaching the ocean surface and is closely connected to the abundance of cloud condensation nuclei). These couplings have been documented as a result of past field programs and model studies. However, extensive research is still required to achieve a quantitative understanding sufficient for developing parameterizations, which adequately predict aerosol indirect effects and low cloud response to climate perturbations. This is especially true of the interactions between clouds, aerosol, and precipitation. These processes take place in an ever-changing synoptic environment that can confound interpretation of short time period observations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4143124','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4143124"><span>The study of surface wetting, nanobubbles and <span class="hlt">boundary</span> slip with an applied voltage: A review</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Pan, Yunlu; Zhao, Xuezeng</p> <p>2014-01-01</p> <p>Summary The drag of fluid flow at the solid–liquid interface in the micro/nanoscale is an important issue in micro/nanofluidic systems. Drag depends on the surface wetting, nanobubbles, surface charge and <span class="hlt">boundary</span> slip. Some researchers have focused on the relationship between these interface properties. In this review, the influence of an applied voltage on the surface wettability, nanobubbles, surface charge density and slip length are discussed. The contact angle (CA) and contact angle hysteresis (CAH) of a droplet of deionized (DI) water on a hydrophobic polystyrene (PS) surface were measured with applied direct <span class="hlt">current</span> (DC) and alternating <span class="hlt">current</span> (AC) voltages. The nanobubbles in DI water and three kinds of saline solution on a PS surface were imaged when a voltage was applied. The influence of the surface charge density on the nanobubbles was analyzed. Then the slip length and the electrostatic force on the probe were measured on an octadecyltrichlorosilane (OTS) surface with applied voltage. The influence of the surface charge on the <span class="hlt">boundary</span> slip and drag of fluid flow has been discussed. <span class="hlt">Finally</span>, the influence of the applied voltage on the surface wetting, nanobubbles, surface charge, <span class="hlt">boundary</span> slip and the drag of liquid flow are summarized. With a smaller surface charge density which could be achieved by applying a voltage on the surface, larger and fewer nanobubbles, a larger slip length and a smaller drag of liquid flow could be found. PMID:25161839</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25161839','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25161839"><span>The study of surface wetting, nanobubbles and <span class="hlt">boundary</span> slip with an applied voltage: A review.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pan, Yunlu; Bhushan, Bharat; Zhao, Xuezeng</p> <p>2014-01-01</p> <p>The drag of fluid flow at the solid-liquid interface in the micro/nanoscale is an important issue in micro/nanofluidic systems. Drag depends on the surface wetting, nanobubbles, surface charge and <span class="hlt">boundary</span> slip. Some researchers have focused on the relationship between these interface properties. In this review, the influence of an applied voltage on the surface wettability, nanobubbles, surface charge density and slip length are discussed. The contact angle (CA) and contact angle hysteresis (CAH) of a droplet of deionized (DI) water on a hydrophobic polystyrene (PS) surface were measured with applied direct <span class="hlt">current</span> (DC) and alternating <span class="hlt">current</span> (AC) voltages. The nanobubbles in DI water and three kinds of saline solution on a PS surface were imaged when a voltage was applied. The influence of the surface charge density on the nanobubbles was analyzed. Then the slip length and the electrostatic force on the probe were measured on an octadecyltrichlorosilane (OTS) surface with applied voltage. The influence of the surface charge on the <span class="hlt">boundary</span> slip and drag of fluid flow has been discussed. <span class="hlt">Finally</span>, the influence of the applied voltage on the surface wetting, nanobubbles, surface charge, <span class="hlt">boundary</span> slip and the drag of liquid flow are summarized. With a smaller surface charge density which could be achieved by applying a voltage on the surface, larger and fewer nanobubbles, a larger slip length and a smaller drag of liquid flow could be found.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003ASAJ..113.2834T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003ASAJ..113.2834T"><span>Effects of prosodic <span class="hlt">boundary</span> on /aC/ sequences: articulatory results</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tabain, Marija</p> <p>2003-05-01</p> <p>This study presents EMA (electromagnetic articulography) data on articulation of the vowel /a/ at different prosodic <span class="hlt">boundaries</span> in French. Three speakers of metropolitan French produced utterances containing the vowel /a/, preceded by /tee/ and followed by one of six consonants /bee dee gee eff ess sh/ (three stops and three fricatives), with different prosodic <span class="hlt">boundaries</span> intervening between the /a/ and the six different consonants. The prosodic <span class="hlt">boundaries</span> investigated are the Utterance, the Intonational phrase, the Accentual phrase, and the Word. Data for the Tongue Tip, Tongue Body, and Jaw are presented. The articulatory data presented here were recorded at the same time as the acoustic data presented in Tabain [J. Acoust. Soc. Am. 113, 516-531 (2003)]. Analyses show that there is a strong effect on peak displacement of the vowel according to the prosodic hierarchy, with the stronger prosodic <span class="hlt">boundaries</span> inducing a much lower Tongue Body and Jaw position than the weaker prosodic <span class="hlt">boundaries</span>. Durations of both the opening movement into and the closing movement out of the vowel are also affected. Peak velocity of the articulatory movements is also examined, and, contrary to results for phrase-<span class="hlt">final</span> lengthening, it is found that peak velocity of the opening movement into the vowel tends to increase with the higher prosodic <span class="hlt">boundaries</span>, together with the increased magnitude of the movement between the consonant and the vowel. Results for the closing movement out of the vowel and into the consonant are not so clear. Since one speaker shows evidence of utterance-level articulatory declension, it is suggested that the competing constraints of articulatory declension and prosodic effects might explain some previous results on phrase-<span class="hlt">final</span> lengthening.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005SPIE.5960.2163T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005SPIE.5960.2163T"><span>Voting based object <span class="hlt">boundary</span> reconstruction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tian, Qi; Zhang, Like; Ma, Jingsheng</p> <p>2005-07-01</p> <p>A voting-based object <span class="hlt">boundary</span> reconstruction approach is proposed in this paper. Morphological technique was adopted in many applications for video object extraction to reconstruct the missing pixels. However, when the missing areas become large, the morphological processing cannot bring us good results. Recently, Tensor voting has attracted people"s attention, and it can be used for <span class="hlt">boundary</span> estimation on curves or irregular trajectories. However, the complexity of saliency tensor creation limits its applications in real-time systems. An alternative approach based on tensor voting is introduced in this paper. Rather than creating saliency tensors, we use a "2-pass" method for orientation estimation. For the first pass, Sobel d*etector is applied on a coarse <span class="hlt">boundary</span> image to get the gradient map. In the second pass, each pixel puts decreasing weights based on its gradient information, and the direction with maximum weights sum is selected as the correct orientation of the pixel. After the orientation map is obtained, pixels begin linking edges or intersections along their direction. The approach is applied to various video surveillance clips under different conditions, and the experimental results demonstrate significant improvement on the <span class="hlt">final</span> extracted objects accuracy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007AGUSMSM41A..06S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007AGUSMSM41A..06S"><span>Field-Aligned <span class="hlt">Current</span> at Plasma Sheet <span class="hlt">Boundary</span> Layers During Storm Time: Cluster Observation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shi, J.; Cheng, Z.; Zhang, T.; Dunlop, M.; Liu, Z.</p> <p>2007-05-01</p> <p>The magnetic field data from the FGM instruments on board the four Cluster spacecrafts were used to study Field Aligned <span class="hlt">Current</span> (FAC) at the Plasma Sheet <span class="hlt">Boundary</span> Layers (PSBLs) with the so called "curlometer technique". We analyzed the date obtained in 2001 in the magnetotail and only two cases were found in the storm time. One (August 17, 2001) occurred from sudden commencement to main phase, and the other (October 1, 2001) lay in the main phase and recovery phase. The relationship between the FAC density and the AE index was studied and the results are shown as follows. (1) In the sudden commencement and the main phase the density of the FAC increases obviously, in the recovery phase the density of the FAC increases slightly. (2) From the sudden commencement to the initial stage of the main phase the FAC increases with decreasing AE index and decreases with increasing AE index. From the late stage of the main phase to initial stage of the recovery phase, the FAC increases with increasing AE index and decreases with decreasing AE index. In the late stage of the recovery phase the disturbance of the FAC is not so violent, so that the FAC varying with the AE index is not very obvious.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940012657','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940012657"><span>Structure of turbulence in three-dimensional <span class="hlt">boundary</span> layers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Subramanian, Chelakara S.</p> <p>1993-01-01</p> <p>This report provides an overview of the three dimensional turbulent <span class="hlt">boundary</span> layer concepts and of the <span class="hlt">currently</span> available experimental information for their turbulence modeling. It is found that more reliable turbulence data, especially of the Reynolds stress transport terms, is needed to improve the existing modeling capabilities. An experiment is proposed to study the three dimensional <span class="hlt">boundary</span> layer formed by a 'sink flow' in a fully developed two dimensional turbulent <span class="hlt">boundary</span> layer. Also, the mean and turbulence field measurement procedure using a three component laser Doppler velocimeter is described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24922980','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24922980"><span><span class="hlt">Current</span> good manufacturing practices, quality control procedures, quality factors, notification requirements, and records and reports, for infant formula. <span class="hlt">Final</span> rule.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p></p> <p>2014-06-10</p> <p>The Food and Drug Administration (FDA or we) is issuing a <span class="hlt">final</span> rule that adopts, with some modifications, the interim <span class="hlt">final</span> rule (IFR) entitled "<span class="hlt">Current</span> Good Manufacturing Practices, Quality Control Procedures, Quality Factors, Notification Requirements, and Records and Reports, for Infant Formula'' (February 10, 2014). This <span class="hlt">final</span> rule affirms the IFR's changes to FDA's regulations and provides additional modifications and clarifications. The <span class="hlt">final</span> rule also responds to certain comments submitted in response to the request for comments in the IFR.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040031476','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040031476"><span>Nonlinear Gulf Stream Interaction with the Deep Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> System: Observations and a Numerical Simulation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dietrich, David E.; Mehra, Avichal; Haney, Robert L.; Bowman, Malcolm J.; Tseng, Yu-Heng</p> <p>2003-01-01</p> <p>Gulf Stream (GS) separation near its observed Cape Hatteras (CH) separation location, and its ensuing path and dynamics, is a challenging ocean modeling problem. If a model GS separates much farther north than CH, then northward GS meanders, which pinch off warm core eddies (rings), are not possible or are strongly constrained by the Grand Banks shelfbreak. Cold core rings pinch off the southward GS meanders. The rings are often re-absorbed by the GS. The important warm core rings enhance heat exchange and, especially, affect the northern GS branch after GS bifurcation near the New England Seamount Chain. This northern branch gains heat by contact with the southern branch water upstream of bifurcation, and warms the Arctic Ocean and northern seas, thus playing a major role in ice dynamics, thermohaline circulation and possible global climate warming. These rings transport heat northward between the separated GS and shelf slope/Deep Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> system (DWBC). This region has nearly level time mean isopycnals. The eddy heat transport convergence/divergence enhances the shelfbreak and GS front intensities and thus also increases watermass transformation. The fronts are maintained by warm advection by the Florida <span class="hlt">Current</span> and cool advection by the DWBC. Thus, the GS interaction with the DWBC through the intermediate eddy field is climatologically important.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://rosap.ntl.bts.gov/view/dot/3980','DOTNTL'); return false;" href="https://rosap.ntl.bts.gov/view/dot/3980"><span>Baselining <span class="hlt">current</span> road weather information : <span class="hlt">final</span> report</span></a></p> <p><a target="_blank" href="http://ntlsearch.bts.gov/tris/index.do">DOT National Transportation Integrated Search</a></p> <p></p> <p>2009-06-10</p> <p>This <span class="hlt">final</span> report contains research findings on the characterization of the quality and value of road weather information resources used by members of the surface transportation community in their decision-making process. The objectives of the projec...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010Chaos..20a7507R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010Chaos..20a7507R"><span>Detecting dynamical <span class="hlt">boundaries</span> from kinematic data in biomechanics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ross, Shane D.; Tanaka, Martin L.; Senatore, Carmine</p> <p>2010-03-01</p> <p>Ridges in the state space distribution of finite-time Lyapunov exponents can be used to locate dynamical <span class="hlt">boundaries</span>. We describe a method for obtaining dynamical <span class="hlt">boundaries</span> using only trajectories reconstructed from time series, expanding on the <span class="hlt">current</span> approach which requires a vector field in the phase space. We analyze problems in musculoskeletal biomechanics, considered as exemplars of a class of experimental systems that contain separatrix features. Particular focus is given to postural control and balance, considering both models and experimental data. Our success in determining the <span class="hlt">boundary</span> between recovery and failure in human balance activities suggests this approach will provide new robust stability measures, as well as measures of fall risk, that <span class="hlt">currently</span> are not available and may have benefits for the analysis and prevention of low back pain and falls leading to injury, both of which affect a significant portion of the population.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..44..346K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..44..346K"><span>Submesoscale cyclones in the Agulhas <span class="hlt">current</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krug, M.; Swart, S.; Gula, J.</p> <p>2017-01-01</p> <p>Gliders were deployed for the first time in the Agulhas <span class="hlt">Current</span> region to investigate processes of interactions between western <span class="hlt">boundary</span> <span class="hlt">currents</span> and shelf waters. Continuous observations from the gliders in water depths of 100-1000 m and over a period of 1 month provide the first high-resolution observations of the Agulhas <span class="hlt">Current</span>'s inshore front. The observations collected in a nonmeandering Agulhas <span class="hlt">Current</span> show the presence of submesoscale cyclonic eddies, generated at the inshore <span class="hlt">boundary</span> of the Agulhas <span class="hlt">Current</span>. The submesoscale cyclones are often associated with warm water plumes, which extend from their western edge and exhibit strong northeastward <span class="hlt">currents</span>. These features are a result of shear instabilities and extract their energy from the mean Agulhas <span class="hlt">Current</span> jet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1060184','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1060184"><span>A TECHNICAL ASSESSMENT OF THE <span class="hlt">CURRENT</span> WATER POLICY <span class="hlt">BOUNDARY</span> AT U.S. DEPARTMENT OF ENERGY, PADUCAH GASEOUS DIFFUSION PLANT, PADUCAH, KENTUCKY</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>None</p> <p>2012-12-13</p> <p>In 1988, groundwater contaminated with trichloroethene (TCE) and technetium-99 (Tc-99) was identified in samples collected from residential water wells withdrawing groundwater from the Regional Gravel Aquifer (RGA) north of the Paducah Gaseous Diffusion Plant (PGDP) facility. In response, the U.S. Department of Energy (DOE) provided temporary drinking water supplies to approximately 100 potentially affected residents by initially supplying bottled water, water tanks, and water-treatment systems, and then by extending municipal water lines, all at no cost, to those persons whose wells could be affected by contaminated groundwater. The Water Policy <span class="hlt">boundary</span> was established in 1993. In the Policy, DOE agreedmore » to pay the reasonable monthly cost of water for homes and businesses and, in exchange, many of the land owners signed license agreements committing to cease using the groundwater via rural water wells. In 2012, DOE requested that Oak Ridge Associated Universities (ORAU), managing contractor of Oak Ridge Institute for Science and Education (ORISE), provide an independent assessment of the quality and quantity of the existing groundwater monitoring data and determine if there is sufficient information to support a modification to the <span class="hlt">boundary</span> of the <span class="hlt">current</span> Water Policy. As a result of the assessment, ORAU concludes that sufficient groundwater monitoring data exists to determine that a shrinkage and/or shift of the plume(s) responsible for the initial development of this policy has occurred. Specifically, there is compelling evidence that the TCE plume is undergoing shrinkage due to natural attenuation and associated degradation. The plume shrinkage (and migration) has also been augmented in local areas where large volumes of groundwater were recovered by pump-and treat remedial systems along the eastern and western <span class="hlt">boundaries</span> of the Northwest Plume, and in other areas where pump-and-treat systems have been deployed by DOE to remove source contaminants. The</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('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4184048','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4184048"><span>Algorithms for Discovery of Multiple Markov <span class="hlt">Boundaries</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>Statnikov, Alexander; Lytkin, Nikita I.; Lemeire, Jan; Aliferis, Constantin F.</p> <p>2013-01-01</p> <p>Algorithms for Markov <span class="hlt">boundary</span> discovery from data constitute an important recent development in machine learning, primarily because they offer a principled solution to the variable/feature selection problem and give insight on local causal structure. Over the last decade many sound algorithms have been proposed to identify a single Markov <span class="hlt">boundary</span> of the response variable. Even though faithful distributions and, more broadly, distributions that satisfy the intersection property always have a single Markov <span class="hlt">boundary</span>, other distributions/data sets may have multiple Markov <span class="hlt">boundaries</span> of the response variable. The latter distributions/data sets are common in practical data-analytic applications, and there are several reasons why it is important to induce multiple Markov <span class="hlt">boundaries</span> from such data. However, there are <span class="hlt">currently</span> no sound and efficient algorithms that can accomplish this task. This paper describes a family of algorithms TIE* that can discover all Markov <span class="hlt">boundaries</span> in a distribution. The broad applicability as well as efficiency of the new algorithmic family is demonstrated in an extensive benchmarking study that involved comparison with 26 state-of-the-art algorithms/variants in 15 data sets from a diversity of application domains. PMID:25285052</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DPPY11040S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DPPY11040S"><span>Solving free-plasma-<span class="hlt">boundary</span> problems with the SIESTA MHD code</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sanchez, R.; Peraza-Rodriguez, H.; Reynolds-Barredo, J. M.; Tribaldos, V.; Geiger, J.; Hirshman, S. P.; Cianciosa, M.</p> <p>2017-10-01</p> <p>SIESTA is a recently developed MHD equilibrium code designed to perform fast and accurate calculations of ideal MHD equilibria for 3D magnetic configurations. It is an iterative code that uses the solution obtained by the VMEC code to provide a background coordinate system and an initial guess of the solution. The <span class="hlt">final</span> solution that SIESTA finds can exhibit magnetic islands and stochastic regions. In its original implementation, SIESTA addressed only fixed-<span class="hlt">boundary</span> problems. This fixed <span class="hlt">boundary</span> condition somewhat restricts its possible applications. In this contribution we describe a recent extension of SIESTA that enables it to address free-plasma-<span class="hlt">boundary</span> situations, opening up the possibility of investigating problems with SIESTA in which the plasma <span class="hlt">boundary</span> is perturbed either externally or internally. As an illustration, the extended version of SIESTA is applied to a configuration of the W7-X stellarator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1422724','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1422724"><span>Nonlinear Dynamics of Vortices in Different Types of Grain <span class="hlt">Boundaries</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>Sheikhzada, Ahmad</p> <p></p> <p>As a major component of linear particle accelerators, superconducting radio-frequency (SRF) resonator cavities are required to operate with lowest energy dissipation and highest accelerating gradient. SRF cavities are made of polycrystalline materials in which grain <span class="hlt">boundaries</span> can limit maximum RF <span class="hlt">currents</span> and produce additional power dissipation sources due to local penetration of Josephson vortices. The essential physics of vortex penetration and mechanisms of dissipation of vortices driven by strong RF <span class="hlt">currents</span> along networks of grain <span class="hlt">boundaries</span> and their contribution to the residual surface resistance have not been well understood. To evaluate how GBs can limit the performance of SRF materials,more » particularly Nb and Nb3Sn, we performed extensive numerical simulations of nonlinear dynamics of Josephson vortices in grain <span class="hlt">boundaries</span> under strong dc and RF fields. The RF power due to penetration of vortices both in weakly-coupled and strongly-coupled grain <span class="hlt">boundaries</span> was calculated as functions of the RF field and frequency. The result of this calculation manifested a quadratic dependence of power to field amplitude at strong RF <span class="hlt">currents</span>, an illustration of resistive behavior of grain <span class="hlt">boundaries</span>. Our calculations also showed that the surface resistance is a complicated function of field controlled by penetration and annihilation of vortices and antivortices in strong RF fields which ultimately saturates to normal resistivity of grain <span class="hlt">boundary</span>. We found that Cherenkov radiation of rapidly moving vortices in grain <span class="hlt">boundaries</span> can produce a new instability causing generation of expanding vortex-antivortex pair which ultimately drives the entire GB in a resistive state. This effect is more pronounced in polycrystalline thin film and multilayer coating structures in which it can cause significant increase in power dissipation and results in hysteresis effects in I-V characteristics, particularly at low temperatures.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16290735','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16290735"><span>Direct measurement of concentration distribution within the <span class="hlt">boundary</span> layer of an ion-exchange membrane.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Choi, Jae-Hwan; Park, Jin-Soo; Moon, Seung-Hyeon</p> <p>2002-07-15</p> <p>In this study the concentration distributions within the diffusion <span class="hlt">boundary</span> layer were obtained by directly measuring the potential drops while the <span class="hlt">currents</span> (under- and overlimiting) passed through the Neosepta CMX cation-exchange membrane (Tokuyama Corp., Japan). Potential drops according to the distance from the membrane surface on the depleted side were measured using a microelectrode to obtain the concentration profile. From the concentration profiles obtained, it was observed that the diffusion <span class="hlt">boundary</span> layers existed in the range of 300-350 microm, which reasonably coincide with the theoretical diffusion <span class="hlt">boundary</span> layer thickness calculated from the limiting <span class="hlt">current</span> density. Although there were some deviations between the concentrations determined from the Nernst model and those from experiments, it was confirmed that the Nernst model effectively depicts the transport phenomena in the ion-exchange membrane system. In addition it was found that the salt concentration at the membrane surface increased when the <span class="hlt">currents</span> applied exceeded the limiting <span class="hlt">current</span>. It is thought that the concentration polarization formed in the diffusion <span class="hlt">boundary</span> layer at <span class="hlt">currents</span> near or lower than the limiting <span class="hlt">current</span> was disturbed by a turbulent convection when the <span class="hlt">current</span> was greater than the limiting <span class="hlt">current</span>. As a consequence, the concentration at the membrane surface increased to a sufficient level for generation of the overlimiting <span class="hlt">current</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.891a2061Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.891a2061Z"><span><span class="hlt">Boundary</span> layer and fundamental problems of hydrodynamics (compatibility of a logarithmic velocity profile in a turbulent <span class="hlt">boundary</span> layer with the experience values)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zaryankin, A. E.</p> <p>2017-11-01</p> <p>The compatibility of the semiempirical turbulence theory of L. Prandtl with the actual flow pattern in a turbulent <span class="hlt">boundary</span> layer is considered in this article, and the <span class="hlt">final</span> calculation results of the <span class="hlt">boundary</span> layer is analyzed based on the mentioned theory. It shows that accepted additional conditions and relationships, which integrate the differential equation of L. Prandtl, associating the turbulent stresses in the <span class="hlt">boundary</span> layer with the transverse velocity gradient, are fulfilled only in the near-wall region where the mentioned equation loses meaning and are inconsistent with the physical meaning on the main part of integration. It is noted that an introduced concept about the presence of a laminar sublayer between the wall and the turbulent <span class="hlt">boundary</span> layer is the way of making of a physical meaning to the logarithmic velocity profile, and can be defined as adjustment of the actual flow to the formula that is inconsistent with the actual <span class="hlt">boundary</span> conditions. It shows that coincidence of the experimental data with the actual logarithmic profile is obtained as a result of the use of not particular physical value, as an argument, but function of this value.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800004749','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800004749"><span>Investigation of blown <span class="hlt">boundary</span> layers with an improved wall jet system. Ph.D. Thesis. <span class="hlt">Final</span> Technical Report, 1 Jul. 1978 - Dec. 1979; [to prevent turbulent <span class="hlt">boundary</span> layer separation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Saripalli, K. R.; Simpson, R. L.</p> <p>1979-01-01</p> <p>The behavior of two dimensional incompressible turbulent wall jets submerged in a <span class="hlt">boundary</span> layer when they are used to prevent <span class="hlt">boundary</span> layer separation on plane surfaces is investigated. The experimental set-up and instrumentation are described. Experimental results of zero pressure gradient flow and adverse pressure gradient flow are presented. Conclusions are given and discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMSA42A..06K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMSA42A..06K"><span>Defense Meteorological Satellite Program Data in Dynamic Auroral <span class="hlt">Boundary</span> Coordinates: New insights into Polar Cap and Auroral Dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Knipp, D.</p> <p>2016-12-01</p> <p>Using reprocessed (Level-2) data from the Defense Meteorology Satellite Program magnetometer (SSM) and particle precipitation (SSJ) instruments we determine the <span class="hlt">boundaries</span> of the central plasma sheet auroral oval, and then consider the relative locations and intensities of field aligned <span class="hlt">currents</span>. Large-scale field-aligned <span class="hlt">currents</span> (FAC) are determined using the Minimum Variance Analysis technique, and their influence is then removed from the magnetic perturbations allowing us to estimate intensity and scale-size of the smaller-scale <span class="hlt">currents</span>. When sorted by dynamic auroral <span class="hlt">boundary</span> coordinates we find that large- scale Region 1 (R1) FAC are often within the polar cap and Region 2 (R2) FAC show a strong dawn-dusk asymmetry (as in Ohtani et al., 2010). We find that mesoscale FAC are stronger in the summer and are most consistently present in the vicinity of dawnside (downward) R1 FAC. Further, mesoscale FAC are confined to auroral latitudes and above on the dawnside, but can be subaroural on the dusk side. Hotspots of mesoscale FAC occur in pre-midnight regions especially during summer. <span class="hlt">Finally</span>, we show how this information can be combined with measurements from above and below the ionosphere-thermosphere to help explain significant perturbations in polar cap dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70016212','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70016212"><span>Iberian plate kinematics: A jumping plate <span class="hlt">boundary</span> between Eurasia and Africa</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Srivastava, S.P.; Schouten, Hans; Roest, W.R.; Klitgord, Kim D.; Kovacs, L.C.; Verhoef, J.; Macnab, R.</p> <p>1990-01-01</p> <p>THE rotation of Iberia and its relation to the formation of the Pyrenees has been difficult to decipher because of the lack of detailed sea-floor spreading data, although several models have been proposed1-7. Here we use detailed aeromagnetic measurements from the sea floor offshore of the Grand Banks of Newfoundland to show that Iberia moved as part of the African plate from late Cretaceous to mid-Eocene time, with a plate <span class="hlt">boundary</span> extending westward from the Bay of Biscay. When motion along this <span class="hlt">boundary</span> ceased, a <span class="hlt">boundary</span> linking extension in the King's Trough to compression along the Pyrenees came into existence. <span class="hlt">Finally</span>, since the late Oligocene, Iberia has been part of the Eurasian plate, with the <span class="hlt">boundary</span> between Eurasia and Africa situated along the Azores-Gibraltar fracture zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT.......189A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT.......189A"><span><span class="hlt">Boundary</span> conditions and unitarity in AdS/CFT</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Andrade, Tomas</p> <p></p> <p>This thesis investigates various issues regarding unitarity in the context of Anti-de Sitter/Conformal Field theory (AdS/CFT) dualities. When the <span class="hlt">boundary</span> duals are conformal, unitarity implies that there are lower bounds on the dimension of primary operators. Now, the AdS/CFT dictionary relates insertions of <span class="hlt">boundary</span> operators to different choices of <span class="hlt">boundary</span> conditions on the gravity side. Therefore, we expect the possible choices of <span class="hlt">boundary</span> conditions in AdS to be restricted accordingly. Our first main goal will be to identify what are the pathologies that occur in the gravitational side of the duality when the <span class="hlt">boundary</span> operators violate the pertinent unitarity bounds. In all the studied cases, we find that such bulk theories are ill-defined as expected, although unitarity is not nec- essarily violated. As our first example we consider a Klein-Gordon field in AdS, and extend the analysis to bosonic fields of spin 1 and 2 later on, with analogous results. Interestingly, it turns our that the bulk settings are pathological even in the absence of strict conformal invariance. Secondly, we argue that introducing a geometrical cut-off in spacetime along with the appropriate modifications of the <span class="hlt">boundary</span> conditions yields the resulting (IR) theories well-defined. By study- ing in detail a Klein-Gordon field with <span class="hlt">boundary</span> conditions that correspond to double-trace deformations, we are able to explicitly verify this claim. <span class="hlt">Finally</span>, we discuss future research directions which include generalizations of AdS/CFT-like dualities and potential applications for condensed matter theory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1813503R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1813503R"><span>Sensitivity to volcanic field <span class="hlt">boundary</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Runge, Melody; Bebbington, Mark; Cronin, Shane; Lindsay, Jan; Rashad Moufti, Mohammed</p> <p>2016-04-01</p> <p>Volcanic hazard analyses are desirable where there is potential for future volcanic activity to affect a proximal population. This is frequently the case for volcanic fields (regions of distributed volcanism) where low eruption rates, fertile soil, and attractive landscapes draw populations to live close by. Forecasting future activity in volcanic fields almost invariably uses spatial or spatio-temporal point processes with model selection and development based on exploratory analyses of previous eruption data. For identifiability reasons, spatio-temporal processes, and practically also spatial processes, the definition of a spatial region is required to which volcanism is confined. However, due to the complex and predominantly unknown sub-surface processes driving volcanic eruptions, definition of a region based solely on geological information is <span class="hlt">currently</span> impossible. Thus, the <span class="hlt">current</span> approach is to fit a shape to the known previous eruption sites. The class of <span class="hlt">boundary</span> shape is an unavoidable subjective decision taken by the forecaster that is often overlooked during subsequent analysis of results. This study shows the substantial effect that this choice may have on even the simplest exploratory methods for hazard forecasting, illustrated using four commonly used exploratory statistical methods and two very different regions: the Auckland Volcanic Field, New Zealand, and Harrat Rahat, Kingdom of Saudi Arabia. For Harrat Rahat, sensitivity of results to <span class="hlt">boundary</span> definition is substantial. For the Auckland Volcanic Field, the range of options resulted in similar shapes, nevertheless, some of the statistical tests still showed substantial variation in results. This work highlights the fact that when carrying out any hazard analysis on volcanic fields, it is vital to specify how the volcanic field <span class="hlt">boundary</span> has been defined, assess the sensitivity of <span class="hlt">boundary</span> choice, and to carry these assumptions and related uncertainties through to estimates of future activity and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Fract..2550042W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Fract..2550042W"><span>a Fractal Permeability Model Coupling <span class="hlt">Boundary</span>-Layer Effect for Tight Oil Reservoirs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Fuyong; Liu, Zhichao; Jiao, Liang; Wang, Congle; Guo, Hu</p> <p></p> <p>A fractal permeability model coupling non-flowing <span class="hlt">boundary</span>-layer effect for tight oil reservoirs was proposed. Firstly, pore structures of tight formations were characterized with fractal theory. Then, with the empirical equation of <span class="hlt">boundary</span>-layer thickness, Hagen-Poiseuille equation and fractal theory, a fractal torturous capillary tube model coupled with <span class="hlt">boundary</span>-layer effect was developed, and verified with experimental data. <span class="hlt">Finally</span>, the parameters influencing effective liquid permeability were quantitatively investigated. The research results show that effective liquid permeability of tight formations is not only decided by pore structures, but also affected by <span class="hlt">boundary</span>-layer distributions, and effective liquid permeability is the function of fluid type, fluid viscosity, pressure gradient, fractal dimension, tortuosity fractal dimension, minimum pore radius and maximum pore radius. For the tight formations dominated with nanoscale pores, <span class="hlt">boundary</span>-layer effect can significantly reduce effective liquid permeability, especially under low pressure gradient.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMEP41E..06E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMEP41E..06E"><span>Sediment Transport Capacity of Turbidity <span class="hlt">Currents</span>: from Microscale to Geological Scale.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eggenhuisen, J. T.; Tilston, M.; Cartigny, M.; Pohl, F.; de Leeuw, J.; van der Grind, G. J.</p> <p>2016-12-01</p> <p>A big question in sedimentology concerns the magnitude of fluxes of sediment particles, solute matter and dissolved gasses from shallow marine waters to deep basins by turbidity <span class="hlt">current</span> flow. Here we establish sediment transport capacity of turbidity <span class="hlt">current</span> flow on three levels. The most elementary level is set by the maximum amount of sediment that can be contained at the base of turbidity <span class="hlt">currents</span> without causing complete extinction of <span class="hlt">boundary</span> layer turbulence. The second level concerns the capacity in a vertical column within turbidity <span class="hlt">currents</span>. The third level involves the amount of sediment that can be transported in turbidite systems on geological timescales. The capacity parameter Γ compares turbulent forces near the <span class="hlt">boundary</span> of a turbulent suspension to gravity and buoyancy forces acting on suspended particles. The condition of Γ>1 coincides with complete suppression of coherent <span class="hlt">boundary</span> layer turbulence in Direct Numerical Simulations of sediment-laden turbulent flow. Γ=1 coincides with the upper limit of observed suspended particle concentrations in flume and field measurements. Γ is grainsize independent, yet capacity of the full vertical structure of turbidity <span class="hlt">currents</span> becomes grainsize dependent. This is due to the appearance of grainsize dependent vertical motions within turbulence as a primary control on the shape of the vertical concentration profile. We illustrate this dependence with experiments and theory and conclude that capacity depends on the competence of prevailing turbulence to suspend particle sizes. The concepts of capacity and competence are thus tangled. <span class="hlt">Finally</span>, the capacity of turbidity <span class="hlt">current</span> flow structure is coupled to geological constraints on recurrence times, channel and lobe life cycles, and allogenic forcing on system activity to arrive at system scale sediment transport capacity. We demonstrate a simple model that uses the fundamental process insight described above to estimate geological sediment budgets from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22397540','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22397540"><span>Addressing therapeutic <span class="hlt">boundaries</span> in social networking.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ginory, Almari; Sabatier, Laura Mayol; Eth, Spencer</p> <p>2012-01-01</p> <p>Facebook is the leading social networking website, with over 500 million users. Prior studies have shown an increasing number of housestaff accessing the site. While Facebook can be used to foster camaraderie, it can also create difficulties in the doctor-patient relationship, especially when <span class="hlt">boundaries</span> are crossed. This study explored the prevalence of such <span class="hlt">boundary</span> crossings and offers recommendations for training. An anonymous voluntary survey regarding Facebook use was distributed to <span class="hlt">current</span> psychiatry residents through the American Psychiatric Association (APA) listserv. Of the 182 respondents, 95.7% had <span class="hlt">current</span> Facebook profiles, and 9.7% had received friend requests from patients. In addition, 18.7% admitted to viewing patient profiles on Facebook. There is a substantial utilization of Facebook among psychiatric residents as compared with prior studies. Specific guidance regarding social media websites and the potential for ethical difficulties should be offered to trainees. © 2012 Guilford Publications, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JGRA..120.9484G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JGRA..120.9484G"><span>Swarm observations of field-aligned <span class="hlt">currents</span> associated with pulsating auroral patches</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gillies, D. M.; Knudsen, D.; Spanswick, E.; Donovan, E.; Burchill, J.; Patrick, M.</p> <p>2015-11-01</p> <p>We have performed a superposed epoch study of in situ field-aligned <span class="hlt">currents</span> located near the edges of regions of pulsating aurora observed simultaneously using ground-based optical data from the Time History of Events and Macroscale Interactions during Substorms (THEMIS) all-sky imager (ASI) network and magnetometers on board the Swarm satellites. A total of nine traversals of Swarm over regions of pulsating aurora identified using THEMIS ASI were studied. We determined that in the cases where a clear <span class="hlt">boundary</span> can be identified, strong downward <span class="hlt">currents</span> are seen just poleward and equatorward of the pulsating patches. A downward <span class="hlt">current</span> in the range of ~1-6 μA/m2 can be seen just poleward of the <span class="hlt">boundary</span>. A weaker upward <span class="hlt">current</span> of ~1-3 μA/m2 is observed throughout the interior of the patch. These observations indicate that <span class="hlt">currents</span> carried by precipitating electrons within patches could close through horizontal <span class="hlt">currents</span> and be returned at the edges, in agreement with Oguti and Hayashi (1984) and Hosokawa et al. (2010b). In addition to confirming these earlier results and adding to their statistical significance, the contribution of this study is to quantify the upward and downward <span class="hlt">current</span> magnitudes, in some cases using two satellites traversing the same pulsating regions. <span class="hlt">Finally</span>, we compare Swarm's two-satellite field-aligned <span class="hlt">current</span> product to the single-satellite results and determine that the data product can be compromised in regions of pulsating aurora, a phenomenon that occurs over widespread regions and tends to persist for long periods of time. These results underscore the importance of electrical coupling between the ionosphere and magnetosphere in regions of patchy pulsating aurora.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012ExA....33..491V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012ExA....33..491V"><span>EIDOSCOPE: particle acceleration at plasma <span class="hlt">boundaries</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vaivads, A.; Andersson, G.; Bale, S. D.; Cully, C. M.; De Keyser, J.; Fujimoto, M.; Grahn, S.; Haaland, S.; Ji, H.; Khotyaintsev, Yu. V.; Lazarian, A.; Lavraud, B.; Mann, I. R.; Nakamura, R.; Nakamura, T. K. M.; Narita, Y.; Retinò, A.; Sahraoui, F.; Schekochihin, A.; Schwartz, S. J.; Shinohara, I.; Sorriso-Valvo, L.</p> <p>2012-04-01</p> <p>We describe the mission concept of how ESA can make a major contribution to the Japanese Canadian multi-spacecraft mission SCOPE by adding one cost-effective spacecraft EIDO (Electron and Ion Dynamics Observatory), which has a comprehensive and optimized plasma payload to address the physics of particle acceleration. The combined mission EIDOSCOPE will distinguish amongst and quantify the governing processes of particle acceleration at several important plasma <span class="hlt">boundaries</span> and their associated <span class="hlt">boundary</span> layers: collisionless shocks, plasma jet fronts, thin <span class="hlt">current</span> sheets and turbulent <span class="hlt">boundary</span> layers. Particle acceleration and associated cross-scale coupling is one of the key outstanding topics to be addressed in the Plasma Universe. The very important science questions that only the combined EIDOSCOPE mission will be able to tackle are: 1) Quantitatively, what are the processes and efficiencies with which both electrons and ions are selectively injected and subsequently accelerated by collisionless shocks? 2) How does small-scale electron and ion acceleration at jet fronts due to kinetic processes couple simultaneously to large scale acceleration due to fluid (MHD) mechanisms? 3) How does multi-scale coupling govern acceleration mechanisms at electron, ion and fluid scales in thin <span class="hlt">current</span> sheets? 4) How do particle acceleration processes inside turbulent <span class="hlt">boundary</span> layers depend on turbulence properties at ion/electron scales? EIDO particle instruments are capable of resolving full 3D particle distribution functions in both thermal and suprathermal regimes and at high enough temporal resolution to resolve the relevant scales even in very dynamic plasma processes. The EIDO spin axis is designed to be sun-pointing, allowing EIDO to carry out the most sensitive electric field measurements ever accomplished in the outer magnetosphere. Combined with a nearby SCOPE Far Daughter satellite, EIDO will form a second pair (in addition to SCOPE Mother-Near Daughter) of closely</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.A33B0159D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.A33B0159D"><span>Observing the Vertical Extent of the Urban <span class="hlt">Boundary</span> Layer Over Jersey City, NJ: A Diurnal and Seasonal Analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dempsey, M. J.; Booth, J.; Arend, M.; Melecio-Vazquez, D.; Gonzalez, J.</p> <p>2015-12-01</p> <p>The atmospheric <span class="hlt">boundary</span> remains one of the more difficult components of the climate system to classify. One of the most important characteristics is the <span class="hlt">boundary</span> layer height, especially in urban settings. The <span class="hlt">current</span> study examines the <span class="hlt">boundary</span> layer height using the the New York City Meteorological Network or NYCMetNet. NYCMetNet is a network of weather stations, which report meteorological conditions in and around New York City, as part of the Optical Remote Sensing Laboratory of The City College of New York (ORSL). Of interest to this study is the data obtained from wind profiler station LSC01. The 915 MHz wind profiler is located 30m above the ground on the roof of the Liberty Science Center in Jersey City, NJ. It is a Vaisala Wind Profiler LAP 3000 with a wavelength of ~34cm, which means that the instrument responds primarily to Bragg backscattering. Can a seasonal urban <span class="hlt">boundary</span> layer climatology be extrapolated from the data obtained from the wind profiler? What is the timing of <span class="hlt">boundary</span> layer evolution and collapse over Jersey City? How effective is the profiler under cloudy skies and even in light rain or snow? This study examines the entire time period covered by the wind profile (2007 to present) and selects a series of clear days and a series of cloudy days. The top of the urban <span class="hlt">boundary</span> layer is subjectively located from each half hour time stamp of signal to noise values. The urban <span class="hlt">boundary</span> layer heights are recorded for clear and then cloudy days. Then the days are sorted seasonally (DJF, MAM, JJA, SON). A seasonal mean is calculated for every half hour time step. <span class="hlt">Finally</span> a time series of seasonal urban <span class="hlt">boundary</span> layer heights is constructed, and the timing of the urban <span class="hlt">boundary</span> layer height maximum and time evolution and collapse of the <span class="hlt">boundary</span> layer are generalized. A comparison is made against urban <span class="hlt">boundary</span> layer heights obtained from Modern-Era Retrospective Analysis For Research And Applications (MERRA).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA601364','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA601364"><span>Grain <span class="hlt">Boundary</span> Complexions</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2014-05-01</p> <p>for failing to comply with a collection of information if it does not display a <span class="hlt">currently</span> valid OMB control number. 1. REPORT DATE MAY 2014 2. REPORT...TYPE 3. DATES COVERED 00-00-2014 to 00-00-2014 4. TITLE AND SUBTITLE Grain <span class="hlt">boundary</span> complexions 5a. CONTRACT NUMBER 5b. GRANT NUMBER 5c...specific adsorption sites of rare- earth elements at IGF/grain inter- faces [142–144], and the viscosity [145] and mechanical strength [146–148] of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19880015916','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19880015916"><span>Curvature of blended rolled edge reflectors at the shadow <span class="hlt">boundary</span> contour</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ellingson, S. W.</p> <p>1988-01-01</p> <p>A technique is advanced for computing the radius of curvature of blended rolled edge reflector surfaces at the shadow <span class="hlt">boundary</span>, in the plane perpendicular to the shadow <span class="hlt">boundary</span> contour. This curvature must be known in order to compute the spurious endpoint contributions in the physical optics (PO) solution for the scattering from reflectors with rolled edges. The technique is applicable to reflectors with radially-defined rim-shapes and rolled edge terminations. The radius of curvature for several basic reflector systems is computed, and it is shown that this curvature can vary greatly along the shadow <span class="hlt">boundary</span> contour. <span class="hlt">Finally</span>, the total PO field in the target zone of a sample compact range system is computed and corrected using the shadow <span class="hlt">boundary</span> radius of curvature, obtained using the technique. It is shown that the fields obtained are a better approximation to the true scattered fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JMP....56g1705V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JMP....56g1705V"><span><span class="hlt">Boundary</span> transfer matrices and <span class="hlt">boundary</span> quantum KZ equations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vlaar, Bart</p> <p>2015-07-01</p> <p>A simple relation between inhomogeneous transfer matrices and <span class="hlt">boundary</span> quantum Knizhnik-Zamolodchikov (KZ) equations is exhibited for quantum integrable systems with reflecting <span class="hlt">boundary</span> conditions, analogous to an observation by Gaudin for periodic systems. Thus, the <span class="hlt">boundary</span> quantum KZ equations receive a new motivation. We also derive the commutativity of Sklyanin's <span class="hlt">boundary</span> transfer matrices by merely imposing appropriate reflection equations, in particular without using the conditions of crossing symmetry and unitarity of the R-matrix.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110007949','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110007949"><span>A <span class="hlt">Final</span> Approach Trajectory Model for <span class="hlt">Current</span> Operations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gong, Chester; Sadovsky, Alexander</p> <p>2010-01-01</p> <p>Predicting accurate trajectories with limited intent information is a challenge faced by air traffic management decision support tools in operation today. One such tool is the FAA's Terminal Proximity Alert system which is intended to assist controllers in maintaining safe separation of arrival aircraft during <span class="hlt">final</span> approach. In an effort to improve the performance of such tools, two <span class="hlt">final</span> approach trajectory models are proposed; one based on polynomial interpolation, the other on the Fourier transform. These models were tested against actual traffic data and used to study effects of the key <span class="hlt">final</span> approach trajectory modeling parameters of wind, aircraft type, and weight class, on trajectory prediction accuracy. Using only the limited intent data available to today's ATM system, both the polynomial interpolation and Fourier transform models showed improved trajectory prediction accuracy over a baseline dead reckoning model. Analysis of actual arrival traffic showed that this improved trajectory prediction accuracy leads to improved inter-arrival separation prediction accuracy for longer look ahead times. The difference in mean inter-arrival separation prediction error between the Fourier transform and dead reckoning models was 0.2 nmi for a look ahead time of 120 sec, a 33 percent improvement, with a corresponding 32 percent improvement in standard deviation.</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/2017JGRC..122.7488T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRC..122.7488T"><span>Moored observations of the Deep Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> in the NW Atlantic: 2004-2014</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Toole, John M.; Andres, Magdalena; Le Bras, Isabela A.; Joyce, Terrence M.; McCartney, Michael S.</p> <p>2017-09-01</p> <p>A moored array spanning the continental slope southeast of Cape Cod sampled the equatorward-flowing Deep Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> (DWBC) for a 10 year period: May 2004 to May 2014. Daily profiles of subinertial velocity, temperature, salinity, and neutral density are constructed for each mooring site and cross-line DWBC transport time series are derived for specified water mass layers. Time-averaged transports based on daily estimates of the flow and density fields in Stream coordinates are contrasted with those derived from the Eulerian-mean flow field, modes of DWBC transport variability are investigated through compositing, and comparisons are made to transport estimates for other latitudes. Integrating the daily velocity estimates over the neutral density range of 27.8-28.125 kg/m3 (encompassing Labrador Sea and Overflow Water layers), a mean equatorward DWBC transport of 22.8 × 106 ± 1.9 × 106 m3/s is obtained. Notably, a statistically significant trend of decreasing equatorward transport is observed in several of the DWBC components as well as the <span class="hlt">current</span> as a whole. The largest linear change (a 4% decrease per year) is seen in the layer of Labrador Sea Water that was renewed by deep convection in the early 1990s whose transport fell from 9.0 × 106 m3/s at the beginning of the field program to 5.8 × 106 m3/s at its end. The corresponding linear fit to the combined Labrador Sea and Overflow Water DWBC transport decreases from 26.4 × 106 to 19.1 × 106 m3/s. In contrast, no long-term trend is observed in upper ocean Slope Water transport. These trends are discussed in the context of decadal observations of the North Atlantic circulation, and subpolar air-sea interaction/water mass transformation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ISPAn.II5..329W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ISPAn.II5..329W"><span><span class="hlt">Boundaries</span> and <span class="hlt">Boundary</span> Marks - Substantive Cultural Heritage of Extensive Importance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Waldhaeusl, P.; Koenig, H.; Mansberger, R.</p> <p>2015-08-01</p> <p>The Austrian Society for surveying and Geoinformation (ASG) has proposed to submit "<span class="hlt">Boundaries</span> and <span class="hlt">Boundary</span> Marks" for the UNESCO World Heritage title. It was time that <span class="hlt">boundaries</span>, borders and limits of all types as well as ownership rights would find the proper attention in the global public. Landmarks symbolize the real property and the associated rights and obligations, in a figurative sense, the property generally and all legal limits. A democratic state of law is impossible at today's population density without a functioning land administration system with surveying and jurisdiction. As monumental World Heritage representatives of the geodetic artwork "<span class="hlt">Boundaries</span> and <span class="hlt">Boundary</span> Marks" are specifically proposed: remaining monuments of the original cadastral geodetic network, the first pan-Austrian surveying headquarters in Vienna, and a specific selection of outstanding <span class="hlt">boundary</span> monuments. Landmarks are monuments to the <span class="hlt">boundaries</span> which separate rights and obligations, but also connect the neighbors peacefully after written agreement. "And cursed be he who does not respect the <span class="hlt">boundaries</span>" you wrote already 3000 years ago. <span class="hlt">Boundaries</span> and <span class="hlt">Boundary</span> Marks are a real thing; they all belong to the tangible or material heritage of human history. In this context also the intangible heritage is discussed. This refers to oral tradition and expressions, performing arts; social practices, rituals and festive events; as well as to knowledge and practices handling nature and the universe. "<span class="hlt">Boundaries</span> and <span class="hlt">Boundary</span> Marks" do not belong to it, but clearly to the material cultural world heritage. "<span class="hlt">Boundary</span> and <span class="hlt">Boundary</span> Marks" is proposed to be listed according to the criteria (ii),(iv),(vi).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1912252L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1912252L"><span>On the age of the Jurassic-Cretaceous <span class="hlt">boundary</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lena, Luis; Ramos, Victor; Pimentel, Marcio; Aguirre-Urreta, Beatriz; Naipauer, Maximiliano; Schaltegger, Urs</p> <p>2017-04-01</p> <p> Ma, which is in conflict with the <span class="hlt">currently</span> set age of 145 Ma. Therefore, this suggests a revision of the age of the Jurassic-Cretaceous <span class="hlt">boundary</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvM...2e4404C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvM...2e4404C"><span>Coercivity degradation caused by inhomogeneous grain <span class="hlt">boundaries</span> in sintered Nd-Fe-B permanent magnets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Hansheng; Yun, Fan; Qu, Jiangtao; Li, Yingfei; Cheng, Zhenxiang; Fang, Ruhao; Ye, Zhixiao; Ringer, Simon P.; Zheng, Rongkun</p> <p>2018-05-01</p> <p>Quantitative correlation between intrinsic coercivity and grain <span class="hlt">boundaries</span> in three dimensions is critical to further improve the performance of sintered Nd-Fe-B permanent magnets. Here, we quantitatively reveal the local composition variation across and especially along grain <span class="hlt">boundaries</span> using the powerful atomic-scale analysis technique known as atom probe tomography. We also estimate the saturation magnetization, magnetocrystalline anisotropy constant, and exchange stiffness of the grain <span class="hlt">boundaries</span> on the basis of the experimentally determined structure and composition. <span class="hlt">Finally</span>, using micromagnetic simulations, we quantify the intrinsic coercivity degradation caused by inhomogeneous grain <span class="hlt">boundaries</span>. This approach can be applied to other magnetic materials for the analysis and optimization of magnetic properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CorRe..36.1039C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CorRe..36.1039C"><span>A case for redefining the <span class="hlt">boundaries</span> of the Mesoamerican Reef Ecoregion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chollett, Iliana; Garavelli, Lysel; Holstein, Daniel; Cherubin, Laurent; Fulton, Stuart; Box, Stephen J.</p> <p>2017-12-01</p> <p>The Mesoamerican Reef (MAR) is an interconnected system that supports the local economies of four countries through the provision of seafood and tourism. Considerable financial, research and management effort has been invested in this priority ecoregion, whose <span class="hlt">boundaries</span> were defined more than 18 yr ago based on best available data on oceanographic patterns, reef and watershed distribution. The long-term persistence of the MAR depends, however, on ensuring that all of its constituent parts are appropriately managed, and the <span class="hlt">current</span> <span class="hlt">boundaries</span> may not respond to this need. Here we assess the suitability of the <span class="hlt">current</span> <span class="hlt">boundaries</span> of the MAR using information on physical environments and larval connectivity of three key species. Our research indicates the <span class="hlt">boundaries</span> of the ecoregion require an adjustment, as the exclusion of key areas in eastern Honduras might jeopardize the persistence of the entire network of connected reefs, and areas in northern Yucatan belong to a different environmental regime and may require different management strategies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003CoTPh..40..247F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003CoTPh..40..247F"><span>Numerical Simulation on a Possible Formation Mechanism of Interplanetary Magnetic Cloud <span class="hlt">Boundaries</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fan, Quan-Lin; Wei, Feng-Si; Feng, Xue-Shang</p> <p>2003-08-01</p> <p>The formation mechanism of the interplanetary magnetic cloud (MC) <span class="hlt">boundaries</span> is numerically investigated by simulating the interactions between an MC of some initial momentum and a local interplanetary <span class="hlt">current</span> sheet. The compressible 2.5D MHD equations are solved. Results show that the magnetic reconnection process is a possible formation mechanism when an MC interacts with a surrounding <span class="hlt">current</span> sheet. A number of interesting features are found. For instance, the front <span class="hlt">boundary</span> of the MCs is a magnetic reconnection <span class="hlt">boundary</span> that could be caused by a driven reconnection ahead of the cloud, and the tail <span class="hlt">boundary</span> might be caused by the driving of the entrained flow as a result of the Bernoulli principle. Analysis of the magnetic field and plasma data demonstrates that at these two <span class="hlt">boundaries</span> appear large value of the plasma parameter β, clear increase of plasma temperature and density, distinct decrease of magnetic magnitude, and a transition of magnetic field direction of about 180 degrees. The outcome of the present simulation agrees qualitatively with the observational results on MC <span class="hlt">boundary</span> inferred from IMP-8, etc. The project supported by National Natural Science Foundation of China under Grant Nos. 40104006, 49925412, and 49990450</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhRvE..85a6711L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhRvE..85a6711L"><span>Immersed <span class="hlt">boundary</span> lattice Boltzmann model based on multiple relaxation times</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lu, Jianhua; Han, Haifeng; Shi, Baochang; Guo, Zhaoli</p> <p>2012-01-01</p> <p>As an alterative version of the lattice Boltzmann models, the multiple relaxation time (MRT) lattice Boltzmann model introduces much less numerical <span class="hlt">boundary</span> slip than the single relaxation time (SRT) lattice Boltzmann model if some special relationship between the relaxation time parameters is chosen. On the other hand, most <span class="hlt">current</span> versions of the immersed <span class="hlt">boundary</span> lattice Boltzmann method, which was first introduced by Feng and improved by many other authors, suffer from numerical <span class="hlt">boundary</span> slip as has been investigated by Le and Zhang. To reduce such a numerical <span class="hlt">boundary</span> slip, an immerse <span class="hlt">boundary</span> lattice Boltzmann model based on multiple relaxation times is proposed in this paper. A special formula is given between two relaxation time parameters in the model. A rigorous analysis and the numerical experiments carried out show that the numerical <span class="hlt">boundary</span> slip reduces dramatically by using the present model compared to the single-relaxation-time-based model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27834602','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27834602"><span>From <span class="hlt">boundaries</span> to <span class="hlt">boundary</span> work: middle managers creating inter-organizational change.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Oldenhof, Lieke; Stoopendaal, Annemiek; Putters, Kim</p> <p>2016-11-21</p> <p>Purpose In healthcare, organizational <span class="hlt">boundaries</span> are often viewed as barriers to change. The purpose of this paper is to show how middle managers create inter-organizational change by doing <span class="hlt">boundary</span> work: the dual act of redrawing <span class="hlt">boundaries</span> and coordinating work in new ways. Design/methodology/approach Theoretically, the paper draws on the concept of <span class="hlt">boundary</span> work from Science and Technology Studies. Empirically, the paper is based on an ethnographic investigation of middle managers that participate in a Dutch reform program across health, social care, and housing. Findings The findings show how middle managers create a sense of urgency for inter-organizational change by emphasizing "fragmented" service provision due to professional, sectoral, financial, and geographical <span class="hlt">boundaries</span>. Rather than eradicating these <span class="hlt">boundaries</span>, middle managers change the status quo gradually by redrawing composite <span class="hlt">boundaries</span>. They use <span class="hlt">boundary</span> objects and a <span class="hlt">boundary</span>-transcending vocabulary emphasizing the need for societal gains that go beyond production targets of individual organizations. As a result, work is coordinated in new ways in neighborhood teams and professional expertise is being reconfigured. Research limitations/implications Since <span class="hlt">boundary</span> workers create incremental change, it is necessary to follow their work for a longer period to assess whether <span class="hlt">boundary</span> work contributes to paradigm change. Practical implications Organizations should pay attention to conditions for <span class="hlt">boundary</span> work, such as legitimacy of <span class="hlt">boundary</span> workers and the availability of <span class="hlt">boundary</span> spaces that function as communities of practice. Originality/value By shifting the focus from <span class="hlt">boundaries</span> to <span class="hlt">boundary</span> work, this paper gives valuable insights into "how" <span class="hlt">boundaries</span> are redrawn and embodied in objects and language.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSPO24D2985S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSPO24D2985S"><span>Terdecadal Observations of Western <span class="hlt">Boundary</span> <span class="hlt">Currents</span> in the Coral Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Steinberg, C. R.; Burrage, D. M.</p> <p>2016-02-01</p> <p>Since 1985, a 30 year time series of <span class="hlt">current</span> and temperature data has been collected by AIMS and since 2007 in partnership with Australia's Integrated Marine Observing System. The data derive from a <span class="hlt">current</span> meter mooring pair along the continental shelf slope monitoring <span class="hlt">currents</span> in the Coral Sea adjacent to the Great Barrier Reef. The array was deployed to provide direct measurements of flow on the continental shelf and slope and estimates of geostrophic <span class="hlt">current</span> anomalies to compare with satellite altimeter derived <span class="hlt">currents</span>. The two locations are located near Jewell Reef at 14o S in 360m and near Myrmidon Reef at 18 o S in 200m water depth. Initially point Rotary <span class="hlt">Current</span> Meters were used but were replaced by Acoustic Doppler <span class="hlt">Current</span> Profilers from the late 1990s so the observations have evolved from a few points in the water column to true <span class="hlt">current</span> profiles. The northern mooring is located in the region where the Southern Equatorial <span class="hlt">Current</span> impacts on the North Queensland shelf causing it to bifurcate into the equatorward Gulf of Papua <span class="hlt">Current</span> and the poleward East Australian <span class="hlt">Current</span>. Embedded in these are eddies that cause pulsing and at times <span class="hlt">current</span> reversals that can significantly affect across shelf intrusions and cross shelf exchange. Being located in the sub-tropics the observations have captured multiple extreme tropical cyclone events and seasonal internal wave activity. The data is being used in conjunction with satellite altimetry to validate hindcasts of a number of hydrodynamic models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890046331&hterms=1041&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3D%2526%25231041','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890046331&hterms=1041&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3D%2526%25231041"><span>Time dependent inflow-outflow <span class="hlt">boundary</span> conditions for 2D acoustic systems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Watson, Willie R.; Myers, Michael K.</p> <p>1989-01-01</p> <p>An analysis of the number and form of the required inflow-outflow <span class="hlt">boundary</span> conditions for the full two-dimensional time-dependent nonlinear acoustic system in subsonic mean flow is performed. The explicit predictor-corrector method of MacCormack (1969) is used. The methodology is tested on both uniform and sheared mean flows with plane and nonplanar sources. Results show that the acoustic system requires three physical <span class="hlt">boundary</span> conditions on the inflow and one on the outflow <span class="hlt">boundary</span>. The most natural choice for the inflow <span class="hlt">boundary</span> conditions is judged to be a specification of the vorticity, the normal acoustic impedance, and a pressure gradient-density gradient relationship normal to the <span class="hlt">boundary</span>. Specification of the acoustic pressure at the outflow <span class="hlt">boundary</span> along with these inflow <span class="hlt">boundary</span> conditions is found to give consistent reliable results. A set of <span class="hlt">boundary</span> conditions developed earlier, which were intended to be nonreflecting is tested using the <span class="hlt">current</span> method and is shown to yield unstable results for nonplanar acoustic waves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM33B2649G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM33B2649G"><span>The Solar Wind-Mars Interaction <span class="hlt">Boundaries</span> in Three Dimensions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gruesbeck, J.; Espley, J. R.; Connerney, J. E. P.; DiBraccio, G. A.; Soobiah, Y. I. J.</p> <p>2017-12-01</p> <p>The Martian magnetosphere is a product of the interaction of Mars with the interplanetary magnetic field and the supersonic solar wind. A bow shock forms upstream of the planet as the solar wind is diverted around the planet. Closer to the planet another <span class="hlt">boundary</span> is located that separates the shock-heated solar wind plasma from the planetary plasma in the Martian magnetosphere. The Martian magnetosphere is induced by the pile-up of the interplanetary magnetic field. This induced magnetospheric <span class="hlt">boundary</span> (IMB) has been referred to by different names, in part due to the observations available at the time. The location of these <span class="hlt">boundaries</span> have been previously analyzed using data from Phobos 2, Mars Global Surveyor, and Mars Express resulting in models describing their average shapes. Observations of individual transitions demonstrate that it is a <span class="hlt">boundary</span> with a finite thickness. The MAVEN spacecraft has been in orbit about Mars since November 2014 resulting in many encounters of the spacecraft with the <span class="hlt">boundaries</span>. Using data from the Particle and Fields Package (PFP), we identify over 1000 bow shock crossings and over 4000 IMB crossings that we use to model the average locations. We model the <span class="hlt">boundaries</span> as a 3-dimensional surface allowing observations of asymmetry. The average location of the bow shock and IMB lies further from the planet in the southern hemisphere, where stronger crustal fields are present. The MAVEN PFP dataset allows concurrent observations of the magnetic field and plasma environment to investigate the nature of the IMB and the relationship of the <span class="hlt">boundary</span> to the different plasma signatures. <span class="hlt">Finally</span>, we model the upstream and downstream encounters of the <span class="hlt">boundaries</span> separately to produce shell models that quantify the finite thicknesses of the <span class="hlt">boundaries</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24061827','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24061827"><span>Analysis and Modeling of <span class="hlt">Boundary</span> Layer Separation Method (BLSM).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pethő, Dóra; Horváth, Géza; Liszi, János; Tóth, Imre; Paor, Dávid</p> <p>2010-09-01</p> <p>Nowadays rules of environmental protection strictly regulate pollution material emission into environment. To keep the environmental protection laws recycling is one of the useful methods of waste material treatment. We have developed a new method for the treatment of industrial waste water and named it <span class="hlt">boundary</span> layer separation method (BLSM). We apply the phenomena that ions can be enriched in the <span class="hlt">boundary</span> layer of the electrically charged electrode surface compared to the bulk liquid phase. The main point of the method is that the <span class="hlt">boundary</span> layer at correctly chosen movement velocity can be taken out of the waste water without being damaged, and the ion-enriched <span class="hlt">boundary</span> layer can be recycled. Electrosorption is a surface phenomenon. It can be used with high efficiency in case of large electrochemically active surface of electrodes. During our research work two high surface area nickel electrodes have been prepared. The value of electrochemically active surface area of electrodes has been estimated. The existence of diffusion part of the double layer has been experimentally approved. The electrical double layer capacity has been determined. Ion transport by <span class="hlt">boundary</span> layer separation has been introduced. <span class="hlt">Finally</span> we have tried to estimate the relative significance of physical adsorption and electrosorption.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JEI....25a3019J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JEI....25a3019J"><span>Salient object detection based on discriminative <span class="hlt">boundary</span> and multiple cues integration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiang, Qingzhu; Wu, Zemin; Tian, Chang; Liu, Tao; Zeng, Mingyong; Hu, Lei</p> <p>2016-01-01</p> <p>In recent years, many saliency models have achieved good performance by taking the image <span class="hlt">boundary</span> as the background prior. However, if all <span class="hlt">boundaries</span> of an image are equally and artificially selected as background, misjudgment may happen when the object touches the <span class="hlt">boundary</span>. We propose an algorithm called weighted contrast optimization based on discriminative <span class="hlt">boundary</span> (wCODB). First, a background estimation model is reliably constructed through discriminating each <span class="hlt">boundary</span> via Hausdorff distance. Second, the background-only weighted contrast is improved by fore-background weighted contrast, which is optimized through weight-adjustable optimization framework. Then to objectively estimate the quality of a saliency map, a simple but effective metric called spatial distribution of saliency map and mean saliency in covered window ratio (MSR) is designed. <span class="hlt">Finally</span>, in order to further promote the detection result using MSR as the weight, we propose a saliency fusion framework to integrate three other cues-uniqueness, distribution, and coherence from three representative methods into our wCODB model. Extensive experiments on six public datasets demonstrate that our wCODB performs favorably against most of the methods based on <span class="hlt">boundary</span>, and the integrated result outperforms all state-of-the-art methods.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EJASP2009....6A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EJASP2009....6A"><span>Video Shot <span class="hlt">Boundary</span> Detection Using QR-Decomposition and Gaussian Transition Detection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Amiri, Ali; Fathy, Mahmood</p> <p>2010-12-01</p> <p>This article explores the problem of video shot <span class="hlt">boundary</span> detection and examines a novel shot <span class="hlt">boundary</span> detection algorithm by using QR-decomposition and modeling of gradual transitions by Gaussian functions. Specifically, the authors attend to the challenges of detecting gradual shots and extracting appropriate spatiotemporal features that affect the ability of algorithms to efficiently detect shot <span class="hlt">boundaries</span>. The algorithm utilizes the properties of QR-decomposition and extracts a block-wise probability function that illustrates the probability of video frames to be in shot transitions. The probability function has abrupt changes in hard cut transitions, and semi-Gaussian behavior in gradual transitions. The algorithm detects these transitions by analyzing the probability function. <span class="hlt">Finally</span>, we will report the results of the experiments using large-scale test sets provided by the TRECVID 2006, which has assessments for hard cut and gradual shot <span class="hlt">boundary</span> detection. These results confirm the high performance of the proposed algorithm.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2012-10-02/pdf/2012-24229.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2012-10-02/pdf/2012-24229.pdf"><span>77 FR 60101 - <span class="hlt">Boundary</span> Establishment for White Salmon Wild and Scenic River “Lower Segment”, Gifford Pinchot...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2012-10-02</p> <p>... Establishment for White Salmon Wild and Scenic River ``Lower Segment'', Gifford Pinchot National Forest..., is transmitting the <span class="hlt">final</span> amended <span class="hlt">boundary</span> of the White Salmon Wild and Scenic River ``Lower Segment... Friday. SUPPLEMENTARY INFORMATION: The White Salmon Wild and Scenic River ``Lower Segment'' <span class="hlt">boundary</span> is...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JCoPh.231.4160A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JCoPh.231.4160A"><span><span class="hlt">Boundary</span> states at reflective moving <span class="hlt">boundaries</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Acosta Minoli, Cesar A.; Kopriva, David A.</p> <p>2012-06-01</p> <p>We derive and evaluate <span class="hlt">boundary</span> states for Maxwell's equations, the linear, and the nonlinear Euler gas-dynamics equations to compute wave reflection from moving <span class="hlt">boundaries</span>. In this study we use a Discontinuous Galerkin Spectral Element method (DGSEM) with Arbitrary Lagrangian-Eulerian (ALE) mapping for the spatial approximation, but the <span class="hlt">boundary</span> states can be used with other methods, like finite volume schemes. We present four studies using Maxwell's equations, one for the linear Euler equations, and one more for the nonlinear Euler equations. These are: reflection of light from a plane mirror moving at constant velocity, reflection of light from a moving cylinder, reflection of light from a vibrating mirror, reflection of sound from a plane wall and dipole sound generation by an oscillating cylinder in an inviscid flow. The studies show that the <span class="hlt">boundary</span> states preserve spectral convergence in the solution and in derived quantities like divergence and vorticity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29159678','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29159678"><span>On the predictability of event <span class="hlt">boundaries</span> in discourse: An ERP investigation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Delogu, Francesca; Drenhaus, Heiner; Crocker, Matthew W</p> <p>2018-02-01</p> <p>When reading a text describing an everyday activity, comprehenders build a model of the situation described that includes prior knowledge of the entities, locations, and sequences of actions that typically occur within the event. Previous work has demonstrated that such knowledge guides the processing of incoming information by making event <span class="hlt">boundaries</span> more or less expected. In the present ERP study, we investigated whether comprehenders' expectations about event <span class="hlt">boundaries</span> are influenced by how elaborately common events are described in the context. Participants read short stories in which a common activity (e.g., washing the dishes) was described either in brief or in an elaborate manner. The <span class="hlt">final</span> sentence contained a target word referring to a more predictable action marking a fine event <span class="hlt">boundary</span> (e.g., drying) or a less predictable action, marking a coarse event <span class="hlt">boundary</span> (e.g., jogging). The results revealed a larger N400 effect for coarse event <span class="hlt">boundaries</span> compared to fine event <span class="hlt">boundaries</span>, but no interaction with description length. Between 600 and 1000 ms, however, elaborate contexts elicited a larger frontal positivity compared to brief contexts. This effect was largely driven by less predictable targets, marking coarse event <span class="hlt">boundaries</span>. We interpret the P600 effect as indexing the updating of the situation model at event <span class="hlt">boundaries</span>, consistent with Event Segmentation Theory (EST). The updating process is more demanding with coarse event <span class="hlt">boundaries</span>, which presumably require the construction of a new situation model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930053288&hterms=Open+Field&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DOpen%2BField','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930053288&hterms=Open+Field&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DOpen%2BField"><span>Relationship between Birkeland <span class="hlt">current</span> regions, particle precipitation, and electric fields</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>De La Beaujardiere, O.; Watermann, J.; Newell, P.; Rich, F.</p> <p>1993-01-01</p> <p>The relationship of the large-scale dayside Birkeland <span class="hlt">currents</span> to large-scale particle precipitation patterns, <span class="hlt">currents</span>, and convection is examined using DMSP and Sondrestrom radar observations. It is found that the local time of the mantle <span class="hlt">currents</span> is not limited to the longitude of the cusp proper, but covers a larger local time extent. The mantle <span class="hlt">currents</span> flow entirely on open field lines. About half of region 1 <span class="hlt">currents</span> flow on open field lines, consistent with the assumption that the region 1 <span class="hlt">currents</span> are generated by the solar wind dynamo and flow within the surface that separates open and closed field lines. More than 80 percent of the Birkeland <span class="hlt">current</span> <span class="hlt">boundaries</span> do not correspond to particle precipitation <span class="hlt">boundaries</span>. Region 2 <span class="hlt">currents</span> extend beyond the plasma sheet poleward <span class="hlt">boundary</span>; region 1 <span class="hlt">currents</span> flow in part on open field lines; mantle <span class="hlt">currents</span> and mantle particles are not coincident. On most passes when a triple <span class="hlt">current</span> sheet is observed, the convection reversal is located on closed field lines.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..MARS23010G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..MARS23010G"><span>Kapitza resistance at segregated <span class="hlt">boundaries</span> in β-SiC</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Goel, Nipun; Webb, Edmund, III; Oztekin, Alparslan; Rickman, Jeffrey; Neti, Sudhakar</p> <p></p> <p>Silicon Carbide is a candidate material for high-temperature thermoelectric applications for harvesting waste heat associated with exhaust from automotive and furnaces as well hot surfaces in solar towers and power electronics. However, for SiC to be a viable thermoelectric material, its thermoelectric figure of merit must be improved significantly. In this talk we examine the role of grain-<span class="hlt">boundary</span> segregation on phononic thermal transport, an important factor in determining the figure of merit, via non-equilibrium molecular dynamics simulations. In particular, we consider the role of dopant concentration and dopant/matrix interactions on the enhancement of the Kapitza resistance of symmetric tilt grain <span class="hlt">boundaries</span>. We find that the calculated resistance depends on the segregation profile, with increases of more than a factor of 50 (relative to an unsegregated <span class="hlt">boundary</span>) at the highest dopant concentrations. <span class="hlt">Finally</span>, we relate the calculated phonon density of states to changes in the Kapitza resistance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JCoPh.235...52F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JCoPh.235...52F"><span><span class="hlt">Boundary</span> particle method for Laplace transformed time fractional diffusion equations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fu, Zhuo-Jia; Chen, Wen; Yang, Hai-Tian</p> <p>2013-02-01</p> <p>This paper develops a novel <span class="hlt">boundary</span> meshless approach, Laplace transformed <span class="hlt">boundary</span> particle method (LTBPM), for numerical modeling of time fractional diffusion equations. It implements Laplace transform technique to obtain the corresponding time-independent inhomogeneous equation in Laplace space and then employs a truly <span class="hlt">boundary</span>-only meshless <span class="hlt">boundary</span> particle method (BPM) to solve this Laplace-transformed problem. Unlike the other <span class="hlt">boundary</span> discretization methods, the BPM does not require any inner nodes, since the recursive composite multiple reciprocity technique (RC-MRM) is used to convert the inhomogeneous problem into the higher-order homogeneous problem. <span class="hlt">Finally</span>, the Stehfest numerical inverse Laplace transform (NILT) is implemented to retrieve the numerical solutions of time fractional diffusion equations from the corresponding BPM solutions. In comparison with finite difference discretization, the LTBPM introduces Laplace transform and Stehfest NILT algorithm to deal with time fractional derivative term, which evades costly convolution integral calculation in time fractional derivation approximation and avoids the effect of time step on numerical accuracy and stability. Consequently, it can effectively simulate long time-history fractional diffusion systems. Error analysis and numerical experiments demonstrate that the present LTBPM is highly accurate and computationally efficient for 2D and 3D time fractional diffusion equations.</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('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3076898','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3076898"><span>Time-dependent and outflow <span class="hlt">boundary</span> conditions for Dissipative Particle Dynamics</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lei, Huan; Fedosov, Dmitry A.; Karniadakis, George Em</p> <p>2011-01-01</p> <p>We propose a simple method to impose both no-slip <span class="hlt">boundary</span> conditions at fluid-wall interfaces and at outflow <span class="hlt">boundaries</span> in fully developed regions for Dissipative Particle Dynamics (DPD) fluid systems. The procedure to enforce the no-slip condition is based on a velocity-dependent shear force, which is a generalized force to represent the presence of the solid-wall particles and to maintain locally thermodynamic consistency. We show that this method can be implemented in both steady and time-dependent fluid systems and compare the DPD results with the continuum limit (Navier-Stokes) results. We also develop a force-adaptive method to impose the outflow <span class="hlt">boundary</span> conditions for fully developed flow with unspecified outflow velocity profile or pressure value. We study flows over the backward-facing step and in idealized arterial bifurcations using a combination of the two new <span class="hlt">boundary</span> methods with different flow rates. <span class="hlt">Finally</span>, we explore the applicability of the outflow method in time-dependent flow systems. The outflow <span class="hlt">boundary</span> method works well for systems with Womersley number of O(1), i.e., when the pressure and flowrate at the outflow are approximately in-phase. PMID:21499548</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100003043','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100003043"><span>Orbiter <span class="hlt">Boundary</span> Layer Transition Prediction Tool Enhancements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Berry, Scott A.; King, Rudolph A.; Kegerise, Michael A.; Wood, William A.; McGinley, Catherine B.; Berger, Karen T.; Anderson, Brian P.</p> <p>2010-01-01</p> <p>Updates to an analytic tool developed for Shuttle support to predict the onset of <span class="hlt">boundary</span> layer transition resulting from thermal protection system damage or repair are presented. The <span class="hlt">boundary</span> layer transition tool is part of a suite of tools that analyze the local aerothermodynamic environment to enable informed disposition of damage for making recommendations to fly as is or to repair. Using mission specific trajectory information and details of each d agmea site or repair, the expected time (and thus Mach number) of transition onset is predicted to help define proper environments for use in subsequent thermal and stress analysis of the thermal protection system and structure. The <span class="hlt">boundary</span> layer transition criteria utilized within the tool were updated based on new local <span class="hlt">boundary</span> layer properties obtained from high fidelity computational solutions. Also, new ground-based measurements were obtained to allow for a wider parametric variation with both protuberances and cavities and then the resulting correlations were calibrated against updated flight data. The end result is to provide correlations that allow increased confidence with the resulting transition predictions. Recently, a new approach was adopted to remove conservatism in terms of sustained turbulence along the wing leading edge. <span class="hlt">Finally</span>, some of the newer flight data are also discussed in terms of how these results reflect back on the updated correlations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/2813637','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/2813637"><span><span class="hlt">Boundaries</span> of dreams, <span class="hlt">boundaries</span> of dreamers: thin and thick <span class="hlt">boundaries</span> as a new personality measure.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hartmann, E</p> <p>1989-11-01</p> <p>Previous work by the author and his collaborators on frequent nightmare sufferers demonstrated that these people had striking personality characteristics which could be called "thin <span class="hlt">boundaries</span>" in a number of different senses. In order to measure thin and thick <span class="hlt">boundaries</span>, a 145-item questionnaire, the <span class="hlt">Boundary</span> Questionnaire, has been developed which has now been taken by over 1,000 persons. Preliminary results are presented indicating that, as predicted a priori, several new groups of nightmare sufferers and groups of art students scored usually "thin," whereas a group of naval officers had usually "thick" <span class="hlt">boundaries</span>. Overall, thinness on the <span class="hlt">Boundary</span> Questionnaire correlated highly positively (r = .40) with frequency of dream recall and also significantly (r = .16) with length of sleep.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930049292&hterms=FAC&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DFAC','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930049292&hterms=FAC&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DFAC"><span>Coupling of magnetopause-<span class="hlt">boundary</span> layer to the polar ionosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wei, C. Q.; Lee, L. C.</p> <p>1993-01-01</p> <p>The plasma dynamics in the low-latitude <span class="hlt">boundary</span> layer and its coupling to the polar ionosphere under <span class="hlt">boundary</span> conditions at the magnetopause are investigated. In the presence of a driven plasma flow along the magnetopause, the Kelvin-Helmholtz instability can develop, leading to the formation and growth of plasma vortices in the <span class="hlt">boundary</span> layer. The finite ionospheric conductivity leads to the decay of these vortices. The competing effect of the formation and decay of vortices leads to the formation of strong vortices only in a limited region. Several enhanced field-aligned power density regions associated with the <span class="hlt">boundary</span> layer vortices and the upward field-aligned <span class="hlt">current</span> (FAC) filaments can be found along the postnoon auroral oval. These enhanced field-aligned power density regions may account for the observed auroral bright spots.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29776090','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29776090"><span>Asymmetric simple exclusion process with position-dependent hopping rates: Phase diagram from <span class="hlt">boundary</span>-layer analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mukherji, Sutapa</p> <p>2018-03-01</p> <p>In this paper, we study a one-dimensional totally asymmetric simple exclusion process with position-dependent hopping rates. Under open <span class="hlt">boundary</span> conditions, this system exhibits <span class="hlt">boundary</span>-induced phase transitions in the steady state. Similarly to totally asymmetric simple exclusion processes with uniform hopping, the phase diagram consists of low-density, high-density, and maximal-<span class="hlt">current</span> phases. In various phases, the shape of the average particle density profile across the lattice including its <span class="hlt">boundary</span>-layer parts changes significantly. Using the tools of <span class="hlt">boundary</span>-layer analysis, we obtain explicit solutions for the density profile in different phases. A detailed analysis of these solutions under different <span class="hlt">boundary</span> conditions helps us obtain the equations for various phase <span class="hlt">boundaries</span>. Next, we show how the shape of the entire density profile including the location of the <span class="hlt">boundary</span> layers can be predicted from the fixed points of the differential equation describing the <span class="hlt">boundary</span> layers. We discuss this in detail through several examples of density profiles in various phases. The maximal-<span class="hlt">current</span> phase appears to be an especially interesting phase where the <span class="hlt">boundary</span> layer flows to a bifurcation point on the fixed-point diagram.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvE..97c2130M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvE..97c2130M"><span>Asymmetric simple exclusion process with position-dependent hopping rates: Phase diagram from <span class="hlt">boundary</span>-layer analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mukherji, Sutapa</p> <p>2018-03-01</p> <p>In this paper, we study a one-dimensional totally asymmetric simple exclusion process with position-dependent hopping rates. Under open <span class="hlt">boundary</span> conditions, this system exhibits <span class="hlt">boundary</span>-induced phase transitions in the steady state. Similarly to totally asymmetric simple exclusion processes with uniform hopping, the phase diagram consists of low-density, high-density, and maximal-<span class="hlt">current</span> phases. In various phases, the shape of the average particle density profile across the lattice including its <span class="hlt">boundary</span>-layer parts changes significantly. Using the tools of <span class="hlt">boundary</span>-layer analysis, we obtain explicit solutions for the density profile in different phases. A detailed analysis of these solutions under different <span class="hlt">boundary</span> conditions helps us obtain the equations for various phase <span class="hlt">boundaries</span>. Next, we show how the shape of the entire density profile including the location of the <span class="hlt">boundary</span> layers can be predicted from the fixed points of the differential equation describing the <span class="hlt">boundary</span> layers. We discuss this in detail through several examples of density profiles in various phases. The maximal-<span class="hlt">current</span> phase appears to be an especially interesting phase where the <span class="hlt">boundary</span> layer flows to a bifurcation point on the fixed-point diagram.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860008195','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860008195"><span>Low Reynold's number <span class="hlt">boundary</span> layers in a disturbed environment. Ph.D. Thesis - August, 1985 - <span class="hlt">Final</span> Report</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Paik, D. K.; Reshotko, E.</p> <p>1986-01-01</p> <p>Studies of flat plate <span class="hlt">boundary</span> layer development were made in a low speed wind tunnel at turbulence levels from 2%to 7%. Only transitional and turbulent flows were observed in the range 280 Re sub theta 700. The mean turbulent velocity profiles display law-of-the-wall behavior but have negligible wake component. The u' disturbance profiles compare well with those of other experiments, the peak value of u'/u sub tau being about 2.5. The effect of free-stream turbulence level on turbulent skin friction can be nicely correlated with those of other investigations on a plot of u sub e/u sub tau versus Re sub theta. A discussion on the u' spectra for the transitional <span class="hlt">boundary</span>-layers is presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvP...9d4005V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvP...9d4005V"><span>Grain-<span class="hlt">Boundary</span> Resistance in Copper Interconnects: From an Atomistic Model to a Neural Network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Valencia, Daniel; Wilson, Evan; Jiang, Zhengping; Valencia-Zapata, Gustavo A.; Wang, Kuang-Chung; Klimeck, Gerhard; Povolotskyi, Michael</p> <p>2018-04-01</p> <p>Orientation effects on the specific resistance of copper grain <span class="hlt">boundaries</span> are studied systematically with two different atomistic tight-binding methods. A methodology is developed to model the specific resistance of grain <span class="hlt">boundaries</span> in the ballistic limit using the embedded atom model, tight- binding methods, and nonequilibrium Green's functions. The methodology is validated against first-principles calculations for thin films with a single coincident grain <span class="hlt">boundary</span>, with 6.4% deviation in the specific resistance. A statistical ensemble of 600 large, random structures with grains is studied. For structures with three grains, it is found that the distribution of specific resistances is close to normal. <span class="hlt">Finally</span>, a compact model for grain-<span class="hlt">boundary</span>-specific resistance is constructed based on a neural network.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940019915','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940019915"><span>Incorporation of the planetary <span class="hlt">boundary</span> layer in atmospheric models</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Moeng, Chin-Hoh; Wyngaard, John; Pielke, Roger; Krueger, Steve</p> <p>1993-01-01</p> <p>The topics discussed include the following: perspectives on planetary <span class="hlt">boundary</span> layer (PBL) measurements; <span class="hlt">current</span> problems of PBL parameterization in mesoscale models; and convective cloud-PBL interactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1347869-assessing-state-art-capabilities-probing-atmospheric-boundary-layer-xpia-field-campaign','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1347869-assessing-state-art-capabilities-probing-atmospheric-boundary-layer-xpia-field-campaign"><span>Assessing State-of-the-Art Capabilities for Probing the Atmospheric <span class="hlt">Boundary</span> Layer: The XPIA Field Campaign</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>Lundquist, Julie K.; Wilczak, James M.; Ashton, Ryan</p> <p></p> <p>The synthesis of new measurement technologies with advances in high performance computing provides an unprecedented opportunity to advance our understanding of the atmosphere, particularly with regard to the complex flows in the atmospheric <span class="hlt">boundary</span> layer. To assess <span class="hlt">current</span> measurement capabilities for quantifying features of atmospheric flow within wind farms, the U.S. Dept. of Energy sponsored the eXperimental Planetary <span class="hlt">boundary</span> layer Instrumentation Assessment (XPIA) campaign at the Boulder Atmospheric Observatory (BAO) in spring 2015. Herein, we summarize the XPIA field experiment design, highlight novel approaches to <span class="hlt">boundary</span>-layer measurements, and quantify measurement uncertainties associated with these experimental methods. Line-of-sight velocities measured bymore » scanning lidars and radars exhibit close agreement with tower measurements, despite differences in measurement volumes. Virtual towers of wind measurements, from multiple lidars or dual radars, also agree well with tower and profiling lidar measurements. Estimates of winds over volumes,conducted with rapid lidar scans, agree with those from scanning radars, enabling assessment of spatial variability. Microwave radiometers provide temperature profiles within and above the <span class="hlt">boundary</span> layer with approximately the same uncertainty as operational remote sensing measurements. Using a motion platform, we assess motion-compensation algorithms for lidars to be mounted on offshore platforms. <span class="hlt">Finally</span>, we highlight cases that could be useful for validation of large-eddy simulations or mesoscale numerical weather prediction, providing information on accessing the archived dataset. We conclude that modern remote Lundquist et al. XPIA BAMS Page 4 of 81 sensing systems provide a generational improvement in observational capabilities, enabling resolution of refined processes critical to understanding 61 inhomogeneous <span class="hlt">boundary</span>-layer flows such as those found in wind farms.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29411925','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29411925"><span>A <span class="hlt">boundary</span> <span class="hlt">current</span> drives synchronous growth of marine fishes across tropical and temperate latitudes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ong, Joyce J L; Rountrey, Adam N; Black, Bryan A; Nguyen, Hoang Minh; Coulson, Peter G; Newman, Stephen J; Wakefield, Corey B; Meeuwig, Jessica J; Meekan, Mark G</p> <p>2018-05-01</p> <p>Entrainment of growth patterns of multiple species to single climatic drivers can lower ecosystem resilience and increase the risk of species extinction during stressful climatic events. However, predictions of the effects of climate change on the productivity and dynamics of marine fishes are hampered by a lack of historical data on growth patterns. We use otolith biochronologies to show that the strength of a <span class="hlt">boundary</span> <span class="hlt">current</span>, modulated by the El Niño-Southern Oscillation, accounted for almost half of the shared variance in annual growth patterns of five of six species of tropical and temperate marine fishes across 23° of latitude (3000 km) in Western Australia. Stronger flow during La Niña years drove increased growth of five species, whereas weaker flow during El Niño years reduced growth. Our work is the first to link the growth patterns of multiple fishes with a single oceanographic/climate phenomenon at large spatial scales and across multiple climate zones, habitat types, trophic levels and depth ranges. Extreme La Niña and El Niño events are predicted to occur more frequently in the future and these are likely to have implications for these vulnerable ecosystems, such as a limited capacity of the marine taxa to recover from stressful climatic events. © 2018 John Wiley & Sons Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2677716','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2677716"><span>The <span class="hlt">boundary</span> vector cell model of place cell firing and spatial memory</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Barry, Caswell; Lever, Colin; Hayman, Robin; Hartley, Tom; Burton, Stephen; O'Keefe, John; Jeffery, Kate; Burgess, Neil</p> <p>2009-01-01</p> <p>We review evidence for the <span class="hlt">boundary</span> vector cell model of the environmental determinants of the firing of hippocampal place cells. Preliminary experimental results are presented concerning the effects of addition or removal of environmental <span class="hlt">boundaries</span> on place cell firing and evidence that <span class="hlt">boundary</span> vector cells may exist in the subiculum. We review and update computational simulations predicting the location of human search within a virtual environment of variable geometry, assuming that <span class="hlt">boundary</span> vector cells provide one of the input representations of location used in mammalian spatial memory. <span class="hlt">Finally</span>, we extend the model to include experience-dependent modification of connection strengths through a BCM-like learning rule, and compare the effects to experimental data on the firing of place cells under geometrical manipulations to their environment. The relationship between neurophysiological results in rats and spatial behaviour in humans is discussed. PMID:16703944</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JSV...381...30G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JSV...381...30G"><span><span class="hlt">Boundary</span> layer effects on liners for aircraft engines</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gabard, Gwénaël</p> <p>2016-10-01</p> <p>The performance of acoustic treatments installed on aircraft engines is strongly influenced by the <span class="hlt">boundary</span> layer of the grazing flow on the surface of the liner. The parametric study presented in this paper illustrates the extent of this effect and identifies when it is significant. The acoustic modes of a circular duct with flow are calculated using a finite difference method. The parameters are representative of the flow conditions, liners and sound fields found in <span class="hlt">current</span> turbofan engines. Both the intake and bypass ducts are considered. Results show that there is a complex interplay between the <span class="hlt">boundary</span> layer thickness, the direction of propagation and the liner impedance and that the <span class="hlt">boundary</span> layer can have a strong impact on liner performance for typical configurations (including changes of the order of 30 dB on the attenuation of modes associated with tonal fan noise). A modified impedance condition including the effect of a small but finite <span class="hlt">boundary</span> layer thickness is considered and compared to the standard Myers condition based on an infinitely thin <span class="hlt">boundary</span> layer. We show how this impedance condition can be implemented in a mode calculation method by introducing auxiliary variables. This condition is able to capture the trends associated with the <span class="hlt">boundary</span> layer effects and in most cases provides improved predictions of liner performance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890018365','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890018365"><span><span class="hlt">Current</span> driven instabilities of an electromagnetically accelerated plasma</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chouetri, E. Y.; Kelly, A. J.; Jahn, R. G.</p> <p>1988-01-01</p> <p>A plasma instability that strongly influences the efficiency and lifetime of electromagnetic plasma accelerators was quantitatively measured. Experimental measurements of dispersion relations (wave phase velocities), spatial growth rates, and stability <span class="hlt">boundaries</span> are reported. The measured critical wave parameters are in excellent agreement with theoretical instability <span class="hlt">boundary</span> predictions. The instability is <span class="hlt">current</span> driven and affects a wide spectrum of longitudinal (electrostatic) oscillations. <span class="hlt">Current</span> driven instabilities, which are intrinsic to the high-<span class="hlt">current</span>-carrying magnetized plasma of the magnetoplasmadynmic (MPD) accelerator, were investigated with a kinetic theoretical model based on first principles. Analytical limits of the appropriate dispersion relation yield unstable ion acoustic waves for T(i)/T(e) much less than 1 and electron acoustic waves for T(i)/T(e) much greater than 1. The resulting set of nonlinear equations for the case of T(i)/T(e) = 1, of most interest to the MPD thruster Plasma Wave Experiment, was numerically solved to yield a multiparameter set of stability <span class="hlt">boundaries</span>. Under certain conditions, marginally stable waves traveling almost perpendicular to the magnetic field would travel at a velocity equal to that of the electron <span class="hlt">current</span>. Such waves were termed <span class="hlt">current</span> waves. Unstable <span class="hlt">current</span> waves near the upper stability <span class="hlt">boundary</span> were observed experimentally and are in accordance with theoretical predictions. This provides unambiguous proof of the existence of such instabilites in electromagnetic plasma accelerators.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhDT.......230P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhDT.......230P"><span>A Dynamic Coupled Magnetosphere-Ionosphere-Ring <span class="hlt">Current</span> Model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pembroke, Asher</p> <p></p> <p>In this thesis we describe a coupled model of Earth's magnetosphere that consists of the Lyon-Fedder-Mobarry (LFM) global magnetohydrodynamics (MHD) simulation, the MIX ionosphere solver and the Rice Convection Model (RCM). We report some results of the coupled model using idealized inputs and model parameters. The algorithmic and physical components of the model are described, including the transfer of magnetic field information and plasma <span class="hlt">boundary</span> conditions to the RCM and the return of ring <span class="hlt">current</span> plasma properties to the LFM. Crucial aspects of the coupling include the restriction of RCM to regions where field-line averaged plasma-beta ¡=1, the use of a plasmasphere model, and the MIX ionosphere model. Compared to stand-alone MHD, the coupled model produces a substantial increase in ring <span class="hlt">current</span> pressure and reduction of the magnetic field near the Earth. In the ionosphere, stronger region-1 and region-2 Birkeland <span class="hlt">currents</span> are seen in the coupled model but with no significant change in the cross polar cap potential drop, while the region-2 <span class="hlt">currents</span> shielded the low-latitude convection potential. In addition, oscillations in the magnetic field are produced at geosynchronous orbit with the coupled code. The diagnostics of entropy and mass content indicate that these oscillations are associated with low-entropy flow channels moving in from the tail and may be related to bursty bulk flows and bubbles seen in observations. As with most complex numerical models, there is the ongoing challenge of untangling numerical artifacts and physics, and we find that while there is still much room for improvement, the results presented here are encouraging. <span class="hlt">Finally</span>, we introduce several new methods for magnetospheric visualization and analysis, including a fluid-spatial volume for RCM and a field-aligned analysis mesh for the LFM. The latter allows us to construct novel visualizations of flux tubes, drift surfaces, topological <span class="hlt">boundaries</span>, and bursty-bulk flows.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26588523','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26588523"><span>Exact and Optimal Quantum Mechanics/Molecular Mechanics <span class="hlt">Boundaries</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sun, Qiming; Chan, Garnet Kin-Lic</p> <p>2014-09-09</p> <p>Motivated by recent work in density matrix embedding theory, we define exact link orbitals that capture all quantum mechanical (QM) effects across arbitrary quantum mechanics/molecular mechanics (QM/MM) <span class="hlt">boundaries</span>. Exact link orbitals are rigorously defined from the full QM solution, and their number is equal to the number of orbitals in the primary QM region. Truncating the exact set yields a smaller set of link orbitals optimal with respect to reproducing the primary region density matrix. We use the optimal link orbitals to obtain insight into the limits of QM/MM <span class="hlt">boundary</span> treatments. We further analyze the popular general hybrid orbital (GHO) QM/MM <span class="hlt">boundary</span> across a test suite of molecules. We find that GHOs are often good proxies for the most important optimal link orbital, although there is little detailed correlation between the detailed GHO composition and optimal link orbital valence weights. The optimal theory shows that anions and cations cannot be described by a single link orbital. However, expanding to include the second most important optimal link orbital in the <span class="hlt">boundary</span> recovers an accurate description. The second optimal link orbital takes the chemically intuitive form of a donor or acceptor orbital for charge redistribution, suggesting that optimal link orbitals can be used as interpretative tools for electron transfer. We further find that two optimal link orbitals are also sufficient for <span class="hlt">boundaries</span> that cut across double bonds. <span class="hlt">Finally</span>, we suggest how to construct "approximately" optimal link orbitals for practical QM/MM calculations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97k5443M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97k5443M"><span>Dynamics of edge <span class="hlt">currents</span> in a linearly quenched Haldane model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mardanya, Sougata; Bhattacharya, Utso; Agarwal, Amit; Dutta, Amit</p> <p>2018-03-01</p> <p>In a finite-time quantum quench of the Haldane model, the Chern number determining the topology of the bulk remains invariant, as long as the dynamics is unitary. Nonetheless, the corresponding <span class="hlt">boundary</span> attribute, the edge <span class="hlt">current</span>, displays interesting dynamics. For the case of sudden and adiabatic quenches the postquench edge <span class="hlt">current</span> is solely determined by the initial and the <span class="hlt">final</span> Hamiltonians, respectively. However for a finite-time (τ ) linear quench in a Haldane nanoribbon, we show that the evolution of the edge <span class="hlt">current</span> from the sudden to the adiabatic limit is not monotonic in τ and has a turning point at a characteristic time scale τ =τ0 . For small τ , the excited states lead to a huge unidirectional surge in the edge <span class="hlt">current</span> of both edges. On the other hand, in the limit of large τ , the edge <span class="hlt">current</span> saturates to its expected equilibrium ground-state value. This competition between the two limits lead to the observed nonmonotonic behavior. Interestingly, τ0 seems to depend only on the Semenoff mass and the Haldane flux. A similar dynamics for the edge <span class="hlt">current</span> is also expected in other systems with topological phases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.708a2012B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.708a2012B"><span>Large-eddy simulations of adverse pressure gradient turbulent <span class="hlt">boundary</span> layers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bobke, Alexandra; Vinuesa, Ricardo; Örlü, Ramis; Schlatter, Philipp</p> <p>2016-04-01</p> <p>Adverse pressure-gradient (APG) turbulent <span class="hlt">boundary</span> layers (TBL) are studied by performing well-resolved large-eddy simulations. The pressure gradient is imposed by defining the free-stream velocity distribution with the description of a power law. Different inflow conditions, box sizes and upper <span class="hlt">boundary</span> conditions are tested in order to determine the <span class="hlt">final</span> set-up. The statistics of turbulent <span class="hlt">boundary</span> layers with two different power-law coefficients and thus magnitudes of adverse pressure gradients are then compared to zero pressure-gradient (ZPG) data. The effect of the APG on TBLs is manifested in the mean flow through a much more prominent wake region and in the Reynolds stresses through the existence of an outer peak. The pre-multiplied energy budgets show that more energy is transported from the near-wall region to farther away from the wall.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5017441','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5017441"><span>Efficient Lane <span class="hlt">Boundary</span> Detection with Spatial-Temporal Knowledge Filtering</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Nan, Zhixiong; Wei, Ping; Xu, Linhai; Zheng, Nanning</p> <p>2016-01-01</p> <p>Lane <span class="hlt">boundary</span> detection technology has progressed rapidly over the past few decades. However, many challenges that often lead to lane detection unavailability remain to be solved. In this paper, we propose a spatial-temporal knowledge filtering model to detect lane <span class="hlt">boundaries</span> in videos. To address the challenges of structure variation, large noise and complex illumination, this model incorporates prior spatial-temporal knowledge with lane appearance features to jointly identify lane <span class="hlt">boundaries</span>. The model first extracts line segments in video frames. Two novel filters—the Crossing Point Filter (CPF) and the Structure Triangle Filter (STF)—are proposed to filter out the noisy line segments. The two filters introduce spatial structure constraints and temporal location constraints into lane detection, which represent the spatial-temporal knowledge about lanes. A straight line or curve model determined by a state machine is used to fit the line segments to <span class="hlt">finally</span> output the lane <span class="hlt">boundaries</span>. We collected a challenging realistic traffic scene dataset. The experimental results on this dataset and other standard dataset demonstrate the strength of our method. The proposed method has been successfully applied to our autonomous experimental vehicle. PMID:27529248</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29845128','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29845128"><span>Active fluids at circular <span class="hlt">boundaries</span>: swim pressure and anomalous droplet ripening.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jamali, Tayeb; Naji, Ali</p> <p>2018-06-13</p> <p>We investigate the swim pressure exerted by non-chiral and chiral active particles on convex or concave circular <span class="hlt">boundaries</span>. Active particles are modeled as non-interacting and non-aligning self-propelled Brownian particles. The convex and concave circular <span class="hlt">boundaries</span> are used to model a fixed inclusion immersed in an active bath and a cavity (or container) enclosing the active particles, respectively. We first present a detailed analysis of the role of convex versus concave <span class="hlt">boundary</span> curvature and of the chirality of active particles in their spatial distribution, chirality-induced <span class="hlt">currents</span>, and the swim pressure they exert on the bounding surfaces. The results will then be used to predict the mechanical equilibria of suspended fluid enclosures (generically referred to as 'droplets') in a bulk with active particles being present either inside the bulk fluid or within the suspended droplets. We show that, while droplets containing active particles behave in accordance with standard capillary paradigms when suspended in a normal bulk, those containing a normal fluid exhibit anomalous behaviors when suspended in an active bulk. In the latter case, the excess swim pressure results in non-monotonic dependence of the inside droplet pressure on the droplet radius; hence, revealing an anomalous regime of behavior beyond a threshold radius, in which the inside droplet pressure increases upon increasing the droplet size. Furthermore, for two interconnected droplets, mechanical equilibrium can occur also when the droplets have different sizes. We thus identify a regime of anomalous droplet ripening, where two unequal-sized droplets can reach a <span class="hlt">final</span> state of equal size upon interconnection, in stark contrast with the standard Ostwald ripening phenomenon, implying shrinkage of the smaller droplet in favor of the larger one.</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('http://adsabs.harvard.edu/abs/2006PhDT........47E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006PhDT........47E"><span>Supersonic turbulent <span class="hlt">boundary</span> layers with periodic mechanical non-equilibrium</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ekoto, Isaac Wesley</p> <p></p> <p>Previous studies have shown that favorable pressure gradients reduce the turbulence levels and length scales in supersonic flow. Wall roughness has been shown to reduce the large-scales in wall bounded flow. Based on these previous observations new questions have been raised. The fundamental questions this dissertation addressed are: (1) What are the effects of wall topology with sharp versus blunt leading edges? and (2) Is it possible that a further reduction of turbulent scales can occur if surface roughness and favorable pressure gradients are combined? To answer these questions and to enhance the <span class="hlt">current</span> experimental database, an experimental analysis was performed to provide high fidelity documentation of the mean and turbulent flow properties along with surface and flow visualizations of a high-speed (M = 2.86), high Reynolds number (Retheta ≈ 60,000) supersonic turbulent <span class="hlt">boundary</span> layer distorted by curvature-induced favorable pressure gradients and large-scale ( k+s ≈ 300) uniform surface roughness. Nine models were tested at three separate locations. Three pressure gradient models strengths (a nominally zero, a weak, and a strong favorable pressure gradient) and three roughness topologies (aerodynamically smooth, square, and diamond shaped roughness elements) were used. Highly resolved planar measurements of mean and fluctuating velocity components were accomplished using particle image velocimetry. Stagnation pressure profiles were acquired with a traversing Pitot probe. Surface pressure distributions were characterized using pressure sensitive paint. <span class="hlt">Finally</span> flow visualization was accomplished using schlieren photographs. Roughness topology had a significant effect on the <span class="hlt">boundary</span> layer mean and turbulent properties due to shock <span class="hlt">boundary</span> layer interactions. Favorable pressure gradients had the expected stabilizing effect on turbulent properties, but the improvements were less significant for models with surface roughness near the wall due to increased</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2012-09-25/pdf/2012-23559.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2012-09-25/pdf/2012-23559.pdf"><span>77 FR 58979 - <span class="hlt">Boundary</span> Establishment for the Au Sable, Bear Creek, Manistee, and the Pine Wild and Scenic...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2012-09-25</p> <p>... DEPARTMENT OF AGRICULTURE Forest Service <span class="hlt">Boundary</span> Establishment for the Au Sable, Bear Creek..., Washington Office, is transmitting the <span class="hlt">final</span> <span class="hlt">boundary</span> of the Au Sable, Bear Creek, Manistee, and the Pine..., Cadillac, MI 49601, (231) 775- 5023, ext. 8756. SUPPLEMENTARY INFORMATION: The Au Sable, Bear Creek...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JCoPh.356..261A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JCoPh.356..261A"><span>A <span class="hlt">boundary</span> element method for Stokes flows with interfaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alinovi, Edoardo; Bottaro, Alessandro</p> <p>2018-03-01</p> <p>The <span class="hlt">boundary</span> element method is a widely used and powerful technique to numerically describe multiphase flows with interfaces, satisfying Stokes' approximation. However, low viscosity ratios between immiscible fluids in contact at an interface and large surface tensions may lead to consistency issues as far as mass conservation is concerned. A simple and effective approach is described to ensure mass conservation at all viscosity ratios and capillary numbers within a standard <span class="hlt">boundary</span> element framework. Benchmark cases are initially considered demonstrating the efficacy of the proposed technique in satisfying mass conservation, comparing with approaches and other solutions present in the literature. The methodology developed is <span class="hlt">finally</span> applied to the problem of slippage over superhydrophobic surfaces.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010GeoRL..3716806G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010GeoRL..3716806G"><span>A plasmapause-like density <span class="hlt">boundary</span> at high latitudes in Saturn's magnetosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gurnett, D. A.; Persoon, A. M.; Kopf, A. J.; Kurth, W. S.; Morooka, M. W.; Wahlund, J.-E.; Khurana, K. K.; Dougherty, M. K.; Mitchell, D. G.; Krimigis, S. M.; Krupp, N.</p> <p>2010-08-01</p> <p>Here we report the discovery of a well-defined plasma density <span class="hlt">boundary</span> at high latitudes in Saturn's magnetosphere. The <span class="hlt">boundary</span> separates a region of relatively high density at L less than about 8 to 15 from a region with densities nearly three orders of magnitude lower at higher L values. Magnetic field measurements show that strong field-aligned <span class="hlt">currents</span>, probably associated with the aurora, are located just inside the <span class="hlt">boundary</span>. Analyses of the anisotropy of energetic electrons show that the magnetic field lines are usually closed inside the <span class="hlt">boundary</span> and open outside the <span class="hlt">boundary</span>, although exceptions sometimes occur. The location of the <span class="hlt">boundary</span> is also modulated at the ˜10.6 to 10.8 hr rotational period of the planet. Many of these characteristics are similar to those predicted by Brice and Ioannidis for the plasmapause at a strongly magnetized, rapidly rotating planet such as Saturn.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70012680','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70012680"><span>The complex variable <span class="hlt">boundary</span> element method: Applications in determining approximative <span class="hlt">boundaries</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>Hromadka, T.V.</p> <p>1984-01-01</p> <p>The complex variable <span class="hlt">boundary</span> element method (CVBEM) is used to determine approximation functions for <span class="hlt">boundary</span> value problems of the Laplace equation such as occurs in potential theory. By determining an approximative <span class="hlt">boundary</span> upon which the CVBEM approximator matches the desired constant (level curves) <span class="hlt">boundary</span> conditions, the CVBEM is found to provide the exact solution throughout the interior of the transformed problem domain. Thus, the acceptability of the CVBEM approximation is determined by the closeness-of-fit of the approximative <span class="hlt">boundary</span> to the study problem <span class="hlt">boundary</span>. ?? 1984.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26303531','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26303531"><span>Functional Requirements for Fab-7 <span class="hlt">Boundary</span> Activity in the Bithorax Complex.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wolle, Daniel; Cleard, Fabienne; Aoki, Tsutomu; Deshpande, Girish; Schedl, Paul; Karch, Francois</p> <p>2015-11-01</p> <p>Chromatin <span class="hlt">boundaries</span> are architectural elements that determine the three-dimensional folding of the chromatin fiber and organize the chromosome into independent units of genetic activity. The Fab-7 <span class="hlt">boundary</span> from the Drosophila bithorax complex (BX-C) is required for the parasegment-specific expression of the Abd-B gene. We have used a replacement strategy to identify sequences that are necessary and sufficient for Fab-7 <span class="hlt">boundary</span> function in the BX-C. Fab-7 <span class="hlt">boundary</span> activity is known to depend on factors that are stage specific, and we describe a novel ∼700-kDa complex, the late <span class="hlt">boundary</span> complex (LBC), that binds to Fab-7 sequences that have insulator functions in late embryos and adults. We show that the LBC is enriched in nuclear extracts from late, but not early, embryos and that it contains three insulator proteins, GAF, Mod(mdg4), and E(y)2. Its DNA binding properties are unusual in that it requires a minimal sequence of >65 bp; however, other than a GAGA motif, the three Fab-7 LBC recognition elements display few sequence similarities. <span class="hlt">Finally</span>, we show that mutations which abrogate LBC binding in vitro inactivate the Fab-7 <span class="hlt">boundary</span> in the BX-C. Copyright © 2015, American Society for Microbiology. All Rights Reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4589599','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4589599"><span>Functional Requirements for Fab-7 <span class="hlt">Boundary</span> Activity in the Bithorax Complex</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wolle, Daniel; Cleard, Fabienne; Aoki, Tsutomu; Deshpande, Girish; Karch, Francois</p> <p>2015-01-01</p> <p>Chromatin <span class="hlt">boundaries</span> are architectural elements that determine the three-dimensional folding of the chromatin fiber and organize the chromosome into independent units of genetic activity. The Fab-7 <span class="hlt">boundary</span> from the Drosophila bithorax complex (BX-C) is required for the parasegment-specific expression of the Abd-B gene. We have used a replacement strategy to identify sequences that are necessary and sufficient for Fab-7 <span class="hlt">boundary</span> function in the BX-C. Fab-7 <span class="hlt">boundary</span> activity is known to depend on factors that are stage specific, and we describe a novel ∼700-kDa complex, the late <span class="hlt">boundary</span> complex (LBC), that binds to Fab-7 sequences that have insulator functions in late embryos and adults. We show that the LBC is enriched in nuclear extracts from late, but not early, embryos and that it contains three insulator proteins, GAF, Mod(mdg4), and E(y)2. Its DNA binding properties are unusual in that it requires a minimal sequence of >65 bp; however, other than a GAGA motif, the three Fab-7 LBC recognition elements display few sequence similarities. <span class="hlt">Finally</span>, we show that mutations which abrogate LBC binding in vitro inactivate the Fab-7 <span class="hlt">boundary</span> in the BX-C. PMID:26303531</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050028442','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050028442"><span><span class="hlt">Boundary</span> Layer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Loitsianskii. L. G.</p> <p>1956-01-01</p> <p>The fundamental, practically the most important branch of the modern mechanics of a viscous fluid or a gas, is that branch which concerns itself with the study of the <span class="hlt">boundary</span> layer. The presence of a <span class="hlt">boundary</span> layer accounts for the origin of the resistance and lift force, the breakdown of the smooth flow about bodies, and other phenomena that are associated with the motion of a body in a real fluid. The concept of <span class="hlt">boundary</span> layer was clearly formulated by the founder of aerodynamics, N. E. Joukowsky, in his well-known work "On the Form of Ships" published as early as 1890. In his book "Theoretical Foundations of Air Navigation," Joukowsky gave an account of the most important properties of the <span class="hlt">boundary</span> layer and pointed out the part played by it in the production of the resistance of bodies to motion. The fundamental differential equations of the motion of a fluid in a laminar <span class="hlt">boundary</span> layer were given by Prandtl in 1904; the first solutions of these equations date from 1907 to 1910. As regards the turbulent <span class="hlt">boundary</span> layer, there does not exist even to this day any rigorous formulation of this problem because there is no closed system of equations for the turbulent motion of a fluid. Soviet scientists have done much toward developing a general theory of the <span class="hlt">boundary</span> layer, and in that branch of the theory which is of greatest practical importance at the present time, namely the study of the <span class="hlt">boundary</span> layer at large velocities of the body in a compressed gas, the efforts of the scientists of our country have borne fruit in the creation of a new theory which leaves far behind all that has been done previously in this direction. We shall herein enumerate the most important results by Soviet scientists in the development of the theory of the <span class="hlt">boundary</span> layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920021066','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920021066"><span>A <span class="hlt">boundary</span> element alternating method for two-dimensional mixed-mode fracture problems</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.; Krishnamurthy, T.</p> <p>1992-01-01</p> <p>A <span class="hlt">boundary</span> element alternating method, denoted herein as BEAM, is presented for two dimensional fracture problems. This is an iterative method which alternates between two solutions. An analytical solution for arbitrary polynomial normal and tangential pressure distributions applied to the crack faces of an embedded crack in an infinite plate is used as the fundamental solution in the alternating method. A <span class="hlt">boundary</span> element method for an uncracked finite plate is the second solution. For problems of edge cracks a technique of utilizing finite elements with BEAM is presented to overcome the inherent singularity in <span class="hlt">boundary</span> element stress calculation near the <span class="hlt">boundaries</span>. Several computational aspects that make the algorithm efficient are presented. <span class="hlt">Finally</span>, the BEAM is applied to a variety of two dimensional crack problems with different configurations and loadings to assess the validity of the method. The method gives accurate stress intensity factors with minimal computing effort.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930042364&hterms=environnement&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Denvironnement','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930042364&hterms=environnement&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Denvironnement"><span>Anomalous plasma diffusion and the magnetopause <span class="hlt">boundary</span> layer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Treumann, Rudolf A.; Labelle, James; Haerendel, Gerhard; Pottelette, Raymond</p> <p>1992-01-01</p> <p>An overview of the <span class="hlt">current</span> state of anomalous diffusion research at the magnetopause and its role in the formation of the magnetopause <span class="hlt">boundary</span> layer is presented. Plasma wave measurements in the <span class="hlt">boundary</span> layer indicate that most of the relevant unstable wave modes contribute negligibly to the diffusion process at the magnetopause under magnetically undisturbed northward IMF conditions. The most promising instability is the lower hybrid drift instability, which may yield diffusion coefficients of the right order if the highest measured wave intensities are assumed. It is concluded that global stationary diffusion due to wave-particle interactions does not take place at the magnetopause. Microscopic wave-particle interaction and anomalous diffusion may contribute to locally break the MD frozen-in conditions and help in transporting large amounts of magnetosheath plasma across the magnetospheric <span class="hlt">boundary</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19860004488','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860004488"><span>Stable <span class="hlt">boundary</span> conditions and difference schemes for Navier-Stokes equations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dutt, P.</p> <p>1985-01-01</p> <p>The Navier-Stokes equations can be viewed as an incompletely elliptic perturbation of the Euler equations. By using the entropy function for the Euler equations as a measure of energy for the Navier-Stokes equations, it was possible to obtain nonlinear energy estimates for the mixed initial <span class="hlt">boundary</span> value problem. These estimates are used to derive <span class="hlt">boundary</span> conditions which guarantee L2 boundedness even when the Reynolds number tends to infinity. <span class="hlt">Finally</span>, a new difference scheme for modelling the Navier-Stokes equations in multidimensions for which it is possible to obtain discrete energy estimates exactly analogous to those we obtained for the differential equation was proposed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19696466','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19696466"><span>Parametric <span class="hlt">boundary</span> reconstruction algorithm for industrial CT metrology application.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Yin, Zhye; Khare, Kedar; De Man, Bruno</p> <p>2009-01-01</p> <p> incorporated as prior knowledge to improve the convergence of an iterative approach. In this paper, the feasibility of parametric <span class="hlt">boundary</span> reconstruction algorithm is demonstrated with both simple and complex simulated objects. <span class="hlt">Finally</span>, the proposed algorithm is applied to the experimental industrial CT system data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985BGeod..59...11G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985BGeod..59...11G"><span>The free versus fixed geodetic <span class="hlt">boundary</span> value problem for different combinations of geodetic observables</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grafarend, E. W.; Heck, B.; Knickmeyer, E. H.</p> <p>1985-03-01</p> <p>Various formulations of the geodetic fixed and free <span class="hlt">boundary</span> value problem are presented, depending upon the type of <span class="hlt">boundary</span> data. For the free problem, <span class="hlt">boundary</span> data of type astronomical latitude, astronomical longitude and a pair of the triplet potential, zero and first-order vertical gradient of gravity are presupposed. For the fixed problem, either the potential or gravity or the vertical gradient of gravity is assumed to be given on the <span class="hlt">boundary</span>. The potential and its derivatives on the <span class="hlt">boundary</span> surface are linearized with respect to a reference potential and a reference surface by Taylor expansion. The Eulerian and Lagrangean concepts of a perturbation theory of the nonlinear geodetic <span class="hlt">boundary</span> value problem are reviewed. <span class="hlt">Finally</span> the <span class="hlt">boundary</span> value problems are solved by Hilbert space techniques leading to new generalized Stokes and Hotine functions. Reduced Stokes and Hotine functions are recommended for numerical reasons. For the case of a <span class="hlt">boundary</span> surface representing the topography a base representation of the solution is achieved by solving an infinite dimensional system of equations. This system of equations is obtained by means of the product-sum-formula for scalar surface spherical harmonics with Wigner 3j-coefficients.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=flow+AND+measurement&pg=4&id=EJ919403','ERIC'); return false;" href="https://eric.ed.gov/?q=flow+AND+measurement&pg=4&id=EJ919403"><span>Defining Neighborhood <span class="hlt">Boundaries</span> for Social Measurement: Advancing Social Work Research</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>Foster, Kirk A.; Hipp, J. Aaron</p> <p>2011-01-01</p> <p>Much of the <span class="hlt">current</span> neighborhood-based research uses variables aggregated on administrative <span class="hlt">boundaries</span> such as zip codes, census tracts, and block groups. However, other methods using <span class="hlt">current</span> technological advances in geographic sciences may broaden our ability to explore the spatial concentration of neighborhood factors affecting individuals and…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ISPAn.IV2...81C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ISPAn.IV2...81C"><span>Interactive Cadastral <span class="hlt">Boundary</span> Delineation from Uav Data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Crommelinck, S.; Höfle, B.; Koeva, M. N.; Yang, M. Y.; Vosselman, G.</p> <p>2018-05-01</p> <p>Unmanned aerial vehicles (UAV) are evolving as an alternative tool to acquire land tenure data. UAVs can capture geospatial data at high quality and resolution in a cost-effective, transparent and flexible manner, from which visible land parcel <span class="hlt">boundaries</span>, i.e., cadastral <span class="hlt">boundaries</span> are delineable. This delineation is to no extent automated, even though physical objects automatically retrievable through image analysis methods mark a large portion of cadastral <span class="hlt">boundaries</span>. This study proposes (i) a methodology that automatically extracts and processes candidate cadastral <span class="hlt">boundary</span> features from UAV data, and (ii) a procedure for a subsequent interactive delineation. Part (i) consists of two state-of-the-art computer vision methods, namely gPb contour detection and SLIC superpixels, as well as a classification part assigning costs to each outline according to local <span class="hlt">boundary</span> knowledge. Part (ii) allows a user-guided delineation by calculating least-cost paths along previously extracted and weighted lines. The approach is tested on visible road outlines in two UAV datasets from Germany. Results show that all roads can be delineated comprehensively. Compared to manual delineation, the number of clicks per 100 m is reduced by up to 86 %, while obtaining a similar localization quality. The approach shows promising results to reduce the effort of manual delineation that is <span class="hlt">currently</span> employed for indirect (cadastral) surveying.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170000312','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170000312"><span>An Immersed <span class="hlt">Boundary</span> Method for Solving the Compressible Navier-Stokes Equations with Fluid Structure Interaction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Brehm, Christoph; Barad, Michael F.; Kiris, Cetin C.</p> <p>2016-01-01</p> <p>An immersed <span class="hlt">boundary</span> method for the compressible Navier-Stokes equation and the additional infrastructure that is needed to solve moving <span class="hlt">boundary</span> problems and fully coupled fluid-structure interaction is described. All the methods described in this paper were implemented in NASA's LAVA solver framework. The underlying immersed <span class="hlt">boundary</span> method is based on the locally stabilized immersed <span class="hlt">boundary</span> method that was previously introduced by the authors. In the present paper this method is extended to account for all aspects that are involved for fluid structure interaction simulations, such as fast geometry queries and stencil computations, the treatment of freshly cleared cells, and the coupling of the computational fluid dynamics solver with a linear structural finite element method. The <span class="hlt">current</span> approach is validated for moving <span class="hlt">boundary</span> problems with prescribed body motion and fully coupled fluid structure interaction problems in 2D and 3D. As part of the validation procedure, results from the second AIAA aeroelastic prediction workshop are also presented. The <span class="hlt">current</span> paper is regarded as a proof of concept study, while more advanced methods for fluid structure interaction are <span class="hlt">currently</span> being investigated, such as geometric and material nonlinearities, and advanced coupling approaches.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940022098','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940022098"><span>Reconstruction of multiple cracks from experimental electrostatic <span class="hlt">boundary</span> measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bryan, Kurt; Liepa, Valdis; Vogelius, Michael</p> <p>1993-01-01</p> <p>An algorithm for recovering a collection of linear cracks in a homogeneous electrical conductor from <span class="hlt">boundary</span> measurements of voltages induced by specified <span class="hlt">current</span> fluxes is described. The technique is a variation of Newton's method and is based on taking weighted averages of the <span class="hlt">boundary</span> data. An apparatus that was constructed specifically for generating laboratory data on which to test the algorithm is also described. The algorithm is applied to a number of different test cases and the results are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/484534','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/484534"><span><span class="hlt">Boundary</span>-layer cumulus over heterogeneous landscapes: A subgrid GCM parameterization. <span class="hlt">Final</span> report, December 1991--November 1995</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>Stull, R.B.; Tripoli, G.</p> <p>1996-01-08</p> <p>The authors developed single-column parameterizations for subgrid <span class="hlt">boundary</span>-layer cumulus clouds. These give cloud onset time, cloud coverage, and ensemble distributions of cloud-base altitudes, cloud-top altitudes, cloud thickness, and the characteristics of cloudy and clear updrafts. They tested and refined the parameterizations against archived data from Spring and Summer 1994 and 1995 intensive operation periods (IOPs) at the Southern Great Plains (SGP) ARM CART site near Lamont, Oklahoma. The authors also found that: cloud-base altitudes are not uniform over a heterogeneous surface; tops of some cumulus clouds can be below the base-altitudes of other cumulus clouds; there is an overlap regionmore » near cloud base where clear and cloudy updrafts exist simultaneously; and the lognormal distribution of cloud sizes scales to the JFD of surface layer air and to the shape of the temperature profile above the <span class="hlt">boundary</span> layer.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24985623','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24985623"><span>Equilibrium limit of thermal conduction and <span class="hlt">boundary</span> scattering in nanostructures.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Haskins, Justin B; Kınacı, Alper; Sevik, Cem; Çağın, Tahir</p> <p>2014-06-28</p> <p>Determining the lattice thermal conductivity (κ) of nanostructures is especially challenging in that, aside from the phonon-phonon scattering present in large systems, the scattering of phonons from the system <span class="hlt">boundary</span> greatly influences heat transport, particularly when system length (L) is less than the average phonon mean free path (MFP). One possible route to modeling κ in these systems is through molecular dynamics (MD) simulations, inherently including both phonon-phonon and phonon-<span class="hlt">boundary</span> scattering effects in the classical limit. Here, we compare <span class="hlt">current</span> MD methods for computing κ in nanostructures with both L ⩽ MFP and L ≫ MFP, referred to as mean free path constrained (cMFP) and unconstrained (uMFP), respectively. Using a (10,0) CNT (carbon nanotube) as a benchmark case, we find that while the uMFP limit of κ is well-defined through the use of equilibrium MD and the time-correlation formalism, the standard equilibrium procedure for κ is not appropriate for the treatment of the cMFP limit because of the large influence of <span class="hlt">boundary</span> scattering. To address this issue, we define an appropriate equilibrium procedure for cMFP systems that, through comparison to high-fidelity non-equilibrium methods, is shown to be the low thermal gradient limit to non-equilibrium results. Further, as a means of predicting κ in systems having L ≫ MFP from cMFP results, we employ an extrapolation procedure based on the phenomenological, <span class="hlt">boundary</span> scattering inclusive expression of Callaway [Phys. Rev. 113, 1046 (1959)]. Using κ from systems with L ⩽ 3 μm in the extrapolation, we find that the equilibrium uMFP κ of a (10,0) CNT can be predicted within 5%. The equilibrium procedure is then applied to a variety of carbon-based nanostructures, such as graphene flakes (GF), graphene nanoribbons (GNRs), CNTs, and icosahedral fullerenes, to determine the influence of size and environment (suspended versus supported) on κ. Concerning the GF and GNR systems, we find that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4914704','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4914704"><span>BREACHING THE SEXUAL <span class="hlt">BOUNDARIES</span> IN THE DOCTOR–PATIENT RELATIONSHIP: SHOULD ENGLISH LAW RECOGNISE FIDUCIARY DUTIES?</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ost, Suzanne</p> <p>2016-01-01</p> <p>In this article, I argue that sexual exploitation in the doctor–patient relationship would be dealt with more appropriately by the law in England and Wales on the basis of a breach of fiduciary duty. Three different types of sexual <span class="hlt">boundary</span> breaches are discussed, and the particular focus is on breaches where the patient's consent is obtained through inducement. I contend that <span class="hlt">current</span> avenues of redress do not clearly catch this behaviour and, moreover, they fail to capture the essence of the wrong committed by the doctor—the knowing breach of trust for self-gain—and the calculated way in which consent is induced. <span class="hlt">Finally</span>, I demonstrate that the fiduciary approach is compatible with the contemporary pro-patient autonomy model of the doctor–patient relationship. PMID:26846652</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/2018JCoPh.362..264S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JCoPh.362..264S"><span>An isogeometric <span class="hlt">boundary</span> element method for electromagnetic scattering with compatible B-spline discretizations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Simpson, R. N.; Liu, Z.; Vázquez, R.; Evans, J. A.</p> <p>2018-06-01</p> <p>We outline the construction of compatible B-splines on 3D surfaces that satisfy the continuity requirements for electromagnetic scattering analysis with the <span class="hlt">boundary</span> element method (method of moments). Our approach makes use of Non-Uniform Rational B-splines to represent model geometry and compatible B-splines to approximate the surface <span class="hlt">current</span>, and adopts the isogeometric concept in which the basis for analysis is taken directly from CAD (geometry) data. The approach allows for high-order approximations and crucially provides a direct link with CAD data structures that allows for efficient design workflows. After outlining the construction of div- and curl-conforming B-splines defined over 3D surfaces we describe their use with the electric and magnetic field integral equations using a Galerkin formulation. We use Bézier extraction to accelerate the computation of NURBS and B-spline terms and employ H-matrices to provide accelerated computations and memory reduction for the dense matrices that result from the <span class="hlt">boundary</span> integral discretization. The method is verified using the well known Mie scattering problem posed over a perfectly electrically conducting sphere and the classic NASA almond problem. <span class="hlt">Finally</span>, we demonstrate the ability of the approach to handle models with complex geometry directly from CAD without mesh generation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97h5127S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97h5127S"><span>Alternating <span class="hlt">currents</span> and shear waves in viscous electronics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Semenyakin, M.; Falkovich, G.</p> <p>2018-02-01</p> <p>Strong interaction among charge carriers can make them move like viscous fluid. Here we explore alternating <span class="hlt">current</span> (ac) effects in viscous electronics. In the Ohmic case, incompressible <span class="hlt">current</span> distribution in a sample adjusts fast to a time-dependent voltage on the electrodes, while in the viscous case, momentum diffusion makes for retardation and for the possibility of propagating slow shear waves. We focus on specific geometries that showcase interesting aspects of such waves: <span class="hlt">current</span> parallel to a one-dimensional defect and <span class="hlt">current</span> applied across a long strip. We find that the phase velocity of the wave propagating along the strip respectively increases/decreases with the frequency for no-slip/no-stress <span class="hlt">boundary</span> conditions. This is so because when the frequency or strip width goes to zero (alternatively, viscosity go to infinity), the wavelength of the <span class="hlt">current</span> pattern tends to infinity in the no-stress case and to a finite value in a general case. We also show that for dc <span class="hlt">current</span> across a strip with a no-stress <span class="hlt">boundary</span>, there are only one pair of vortices, while there is an infinite vortex chain for all other types of <span class="hlt">boundary</span> conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.9415J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.9415J"><span>Transport of Iceland-Scotland Overflow waters in the Deep Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> along the Reykjanes Ridge</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Johns, William; Houk, Adam; Koman, Greg; Zou, Sijia; Lozier, Susan</p> <p>2017-04-01</p> <p>Since 2014, an array of <span class="hlt">current</span> meters deployed as part of the OSNAP trans-basin observing system has provided new measurements of the southward flow of Iceland-Scotland Overflow water (ISOW) along the eastern flank of the Reykjanes Ridge in the Iceland Basin. The location of the array, near 58-59°N, captures the ISOW Deep Western <span class="hlt">Boundary</span> <span class="hlt">Current</span> at the farthest downstream location in the Iceland Basin before significant amounts of ISOW can flow into the Irminger Basin through deep fractures in the Reykjanes Ridge. The transport of the ISOW DWBC at this location - based on the first two years of OSNAP observations (July 2014 to July 2016) - is 5.8 ± 0.9 Sv for σθ >27.8. Most of this transport is carried in a main branch of the DWBC along the upper ridge crest in depths from 1400-2200 m, while a secondary branch in depths of 2400-2700 m along the lower ridge crest carries about 1 Sv. The branching of the DWBC at this location is consistent with numerical model results and is caused by an upstream topographic plateau at mid-depths along the ridge crest. The T-S properties of the flow and backward trajectories computed from high-resolution FLAME and VIKING models confirm that the flow in both branches is derived from ISOW and its entrainment products. The transport of the ISOW plume varies over a considerable range, from about 2-10 Sv on weekly to monthly time scales (std. dev. = 2.4 Sv); however the mean <span class="hlt">currents</span> from two individual year-long deployments are very similar and indicate a robust mean flow structure. The observed ISOW transport at this location is larger by almost 2 Sv than previous values obtained (mostly) farther north in the Iceland Basin, suggesting that additional entrainment into the ISOW plume occurs as it approaches the southern tip of the Reykjanes Ridge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ChOE...32..365C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ChOE...32..365C"><span>Experimental Research on <span class="hlt">Boundary</span> Shear Stress in Typical Meandering Channel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Kai-hua; Xia, Yun-feng; Zhang, Shi-zhao; Wen, Yun-cheng; Xu, Hua</p> <p>2018-06-01</p> <p>A novel instrument named Micro-Electro-Mechanical System (MEMS) flexible hot-film shear stress sensor was used to study the <span class="hlt">boundary</span> shear stress distribution in the generalized natural meandering open channel, and the mean sidewall shear stress distribution along the meandering channel, and the lateral <span class="hlt">boundary</span> shear stress distribution in the typical cross-section of the meandering channel was analysed. Based on the measurement of the <span class="hlt">boundary</span> shear stress, a semi-empirical semi-theoretical computing approach of the <span class="hlt">boundary</span> shear stress was derived including the effects of the secondary flow, sidewall roughness factor, eddy viscosity and the additional Reynolds stress, and more importantly, for the first time, it combined the effects of the cross-section central angle and the Reynolds number into the expressions. Afterwards, a comparison between the previous research and this study was developed. Following the result, we found that the semi-empirical semi-theoretical <span class="hlt">boundary</span> shear stress distribution algorithm can predict the <span class="hlt">boundary</span> shear stress distribution precisely. <span class="hlt">Finally</span>, a single factor analysis was conducted on the relationship between the average sidewall shear stress on the convex and concave bank and the flow rate, water depth, slope ratio, or the cross-section central angle of the open channel bend. The functional relationship with each of the above factors was established, and then the distance from the location of the extreme sidewall shear stress to the bottom of the open channel was deduced based on the statistical theory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1235674-calculation-grain-boundary-normals-directly-from-microstructure-images','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1235674-calculation-grain-boundary-normals-directly-from-microstructure-images"><span>Calculation of grain <span class="hlt">boundary</span> normals directly from 3D microstructure images</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lieberman, E. J.; Rollett, A. D.; Lebensohn, R. A.; ...</p> <p>2015-03-11</p> <p>The determination of grain <span class="hlt">boundary</span> normals is an integral part of the characterization of grain <span class="hlt">boundaries</span> in polycrystalline materials. These normal vectors are difficult to quantify due to the discretized nature of available microstructure characterization techniques. The most common method to determine grain <span class="hlt">boundary</span> normals is by generating a surface mesh from an image of the microstructure, but this process can be slow, and is subject to smoothing issues. A new technique is proposed, utilizing first order Cartesian moments of binary indicator functions, to determine grain <span class="hlt">boundary</span> normals directly from a voxelized microstructure image. In order to validate the accuracymore » of this technique, the surface normals obtained by the proposed method are compared to those generated by a surface meshing algorithm. Specifically, the local divergence between the surface normals obtained by different variants of the proposed technique and those generated from a surface mesh of a synthetic microstructure constructed using a marching cubes algorithm followed by Laplacian smoothing is quantified. Next, surface normals obtained with the proposed method from a measured 3D microstructure image of a Ni polycrystal are used to generate grain <span class="hlt">boundary</span> character distributions (GBCD) for Σ3 and Σ9 <span class="hlt">boundaries</span>, and compared to the GBCD generated using a surface mesh obtained from the same image. <span class="hlt">Finally</span>, the results show that the proposed technique is an efficient and accurate method to determine voxelized fields of grain <span class="hlt">boundary</span> normals.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920045456&hterms=Magnetic+Flux&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DMagnetic%2BFlux','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920045456&hterms=Magnetic+Flux&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DMagnetic%2BFlux"><span>Plasma dynamics on <span class="hlt">current</span>-carrying magnetic flux tubes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Swift, Daniel W.</p> <p>1992-01-01</p> <p>A 1D numerical simulation is used to investigate the evolution of a plasma in a <span class="hlt">current</span>-carrying magnetic flux tube of variable cross section. A large potential difference, parallel to the magnetic field, is applied across the domain. The result is that density minimum tends to deepen, primarily in the cathode end, and the entire potential drop becomes concentrated across the region of density minimum. The evolution of the simulation shows some sensitivity to particle <span class="hlt">boundary</span> conditions, but the simulations inevitably evolve into a <span class="hlt">final</span> state with a nearly stationary double layer near the cathode end. The simulation results are at sufficient variance with observations that it appears unlikely that auroral electrons can be explained by a simple process of acceleration through a field-aligned potential drop.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790013876','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790013876"><span>Observations on streamwise vortices in laminar and turbulent <span class="hlt">boundary</span> layers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Morkovin, M. V.</p> <p>1979-01-01</p> <p>The frequent but often unsuspected presence of streamwise vortices in nominally two dimensional laminar and turbulent <span class="hlt">boundary</span> layers and some of their consequences are described. Since there is no body of systematic information on streamwise vortices imbedded in <span class="hlt">boundary</span> layers, a number of issues concerning their occurrence and behavior are discussed in the form of a set of succinct observations. Desirable experimental and numerical research to remedy the <span class="hlt">current</span> lack of knowledge is recommended.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3489504','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3489504"><span>Quality Tetrahedral Mesh Smoothing via <span class="hlt">Boundary</span>-Optimized Delaunay Triangulation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gao, Zhanheng; Yu, Zeyun; Holst, Michael</p> <p>2012-01-01</p> <p>Despite its great success in improving the quality of a tetrahedral mesh, the original optimal Delaunay triangulation (ODT) is designed to move only inner vertices and thus cannot handle input meshes containing “bad” triangles on <span class="hlt">boundaries</span>. In the <span class="hlt">current</span> work, we present an integrated approach called <span class="hlt">boundary</span>-optimized Delaunay triangulation (B-ODT) to smooth (improve) a tetrahedral mesh. In our method, both inner and <span class="hlt">boundary</span> vertices are repositioned by analytically minimizing the error between a paraboloid function and its piecewise linear interpolation over the neighborhood of each vertex. In addition to the guaranteed volume-preserving property, the proposed algorithm can be readily adapted to preserve sharp features in the original mesh. A number of experiments are included to demonstrate the performance of our method. PMID:23144522</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5116534','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5116534"><span>Prosodic <span class="hlt">Boundaries</span> in Writing: Evidence from a Keystroke 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>Fuchs, Susanne; Krivokapić, Jelena</p> <p>2016-01-01</p> <p>The aim of the paper is to investigate duration between successive keystrokes during typing in order to examine whether prosodic <span class="hlt">boundaries</span> are expressed in the process of writing. In particular, we are interested in interkey durations that occur next to punctuation marks (comma and full stops while taking keystrokes between words as a reference), since these punctuation marks are often realized with minor or major prosodic <span class="hlt">boundaries</span> during overt reading. A two-part experiment was conducted: first, participants’ keystrokes on a computer keyboard were recorded while writing an email to a close friend (in two conditions: with and without time pressure). Second, participants read the email they just wrote. Interkey durations were compared to pause durations at the same locations during read speech. Results provide evidence of significant differences between interkey durations between words, at commas and at full stops (from shortest to longest). These durations were positively correlated with silent pause durations during overt reading. A more detailed analysis of interkey durations revealed patterns that can be interpreted with respect to prosodic <span class="hlt">boundaries</span> in speech production, namely as phrase-<span class="hlt">final</span> and phrase-initial lengthening occurring at punctuation marks. This work provides initial evidence that prosodic <span class="hlt">boundaries</span> are reflected in the writing process. PMID:27917129</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27917129','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27917129"><span>Prosodic <span class="hlt">Boundaries</span> in Writing: Evidence from a Keystroke Analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fuchs, Susanne; Krivokapić, Jelena</p> <p>2016-01-01</p> <p>The aim of the paper is to investigate duration between successive keystrokes during typing in order to examine whether prosodic <span class="hlt">boundaries</span> are expressed in the process of writing. In particular, we are interested in interkey durations that occur next to punctuation marks (comma and full stops while taking keystrokes between words as a reference), since these punctuation marks are often realized with minor or major prosodic <span class="hlt">boundaries</span> during overt reading. A two-part experiment was conducted: first, participants' keystrokes on a computer keyboard were recorded while writing an email to a close friend (in two conditions: with and without time pressure). Second, participants read the email they just wrote. Interkey durations were compared to pause durations at the same locations during read speech. Results provide evidence of significant differences between interkey durations between words, at commas and at full stops (from shortest to longest). These durations were positively correlated with silent pause durations during overt reading. A more detailed analysis of interkey durations revealed patterns that can be interpreted with respect to prosodic <span class="hlt">boundaries</span> in speech production, namely as phrase-<span class="hlt">final</span> and phrase-initial lengthening occurring at punctuation marks. This work provides initial evidence that prosodic <span class="hlt">boundaries</span> are reflected in the writing process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850059791&hterms=FAC&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DFAC','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850059791&hterms=FAC&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DFAC"><span>ISEE-1 and 2 observations of field-aligned <span class="hlt">currents</span> in the distant midnight magnetosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Elphic, R. C.; Kelly, T. J.; Russell, C. T.</p> <p>1985-01-01</p> <p>Magnetic field measurements obtained in the nightside magnetosphere by the co-orbiting ISEE-1 and 2 spacecraft have been examined for signatures of field-aligned <span class="hlt">currents</span> (FAC). Such <span class="hlt">currents</span> are found on the <span class="hlt">boundary</span> of the plasma sheet both when the plasma sheet is expanding and when it is thinning. Evidence is often found for the existence of waves on the plasma sheet <span class="hlt">boundary</span>, leading to multiple crossings of the FAC sheet. At times the <span class="hlt">boundary</span> layer FAC sheet orientation is nearly parallel to the X-Z GSM plane, suggesting 'protrusions' of plasma sheet into the lobes. The <span class="hlt">boundary</span> layer <span class="hlt">current</span> polarity is, as expected, into the ionosphere in the midnight to dawn local time sector, and outward near dusk. <span class="hlt">Current</span> sheet thicknesses and velocities are essentially independent of plasma sheet expansion or thinning, having typical values of 1500 km and 20-40 km/s respectively. Characteristic <span class="hlt">boundary</span> layer <span class="hlt">current</span> densities are about 10 nanoamps per square meter.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1374344-revisiting-boundary-perturbation-theory-inhomogeneous-transport-problems','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1374344-revisiting-boundary-perturbation-theory-inhomogeneous-transport-problems"><span>Revisiting <span class="hlt">Boundary</span> Perturbation Theory for Inhomogeneous Transport Problems</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Favorite, Jeffrey A.; Gonzalez, Esteban</p> <p>2017-03-10</p> <p>Adjoint-based first-order perturbation theory is applied again to <span class="hlt">boundary</span> perturbation problems. Rahnema developed a perturbation estimate that gives an accurate first-order approximation of a flux or reaction rate within a radioactive system when the <span class="hlt">boundary</span> is perturbed. When the response of interest is the flux or leakage <span class="hlt">current</span> on the <span class="hlt">boundary</span>, the Roussopoulos perturbation estimate has long been used. The Rahnema and Roussopoulos estimates differ in one term. Our paper shows that the Rahnema and Roussopoulos estimates can be derived consistently, using different responses, from a single variational functional (due to Gheorghiu and Rahnema), resolving any apparent contradiction. In analyticmore » test problems, Rahnema’s estimate and the Roussopoulos estimate produce exact first derivatives of the response of interest when appropriately applied. We also present a realistic, nonanalytic test problem.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770017245','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770017245"><span><span class="hlt">Boundary</span> layer integral matrix procedure: Verification of models</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Bonnett, W. S.; Evans, R. M.</p> <p>1977-01-01</p> <p>The three turbulent models <span class="hlt">currently</span> available in the JANNAF version of the Aerotherm <span class="hlt">Boundary</span> Layer Integral Matrix Procedure (BLIMP-J) code were studied. The BLIMP-J program is the standard prediction method for <span class="hlt">boundary</span> layer effects in liquid rocket engine thrust chambers. Experimental data from flow fields with large edge-to-wall temperature ratios are compared to the predictions of the three turbulence models contained in BLIMP-J. In addition, test conditions necessary to generate additional data on a flat plate or in a nozzle are given. It is concluded that the Cebeci-Smith turbulence model be the recommended model for the prediction of <span class="hlt">boundary</span> layer effects in liquid rocket engines. In addition, the effects of homogeneous chemical reaction kinetics were examined for a hydrogen/oxygen system. Results show that for most flows, kinetics are probably only significant for stoichiometric mixture ratios.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JHEP...11..092B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JHEP...11..092B"><span>Vacuum <span class="hlt">currents</span> in braneworlds on AdS bulk with compact dimensions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bellucci, S.; Saharian, A. A.; Vardanyan, V.</p> <p>2015-11-01</p> <p>The two-point function and the vacuum expectation value (VEV) of the <span class="hlt">current</span> density are investigated for a massive charged scalar field with arbitrary curvature coupling in the geometry of a brane on the background of AdS spacetime with partial toroidal compactification. The presence of a gauge field flux, enclosed by compact dimensions, is assumed. On the brane the field obeys Robin <span class="hlt">boundary</span> condition and along compact dimensions periodicity conditions with general phases are imposed. There is a range in the space of the values for the coefficient in the <span class="hlt">boundary</span> condition where the Poincaré vacuum is unstable. This range depends on the location of the brane and is different for the regions between the brane and AdS <span class="hlt">boundary</span> and between the brane and the horizon. In models with compact dimensions the stability condition is less restrictive than that for the AdS bulk with trivial topology. The vacuum charge density and the components of the <span class="hlt">current</span> along non-compact dimensions vanish. The VEV of the <span class="hlt">current</span> density along compact dimensions is a periodic function of the gauge field flux with the period equal to the flux quantum. It is decomposed into the <span class="hlt">boundary</span>-free and brane-induced contributions. The asymptotic behavior of the latter is investigated near the brane, near the AdS <span class="hlt">boundary</span> and near the horizon. It is shown that, in contrast to the VEVs of the field squared an denergy-momentum tensor, the <span class="hlt">current</span> density is finite on the brane and vanishes for the special case of Dirichlet <span class="hlt">boundary</span> condition. Both the <span class="hlt">boundary</span>-free and brane-induced contributions vanish on the AdS <span class="hlt">boundary</span>. The brane-induced contribution vanishes on the horizon and for points near the horizon the <span class="hlt">current</span> is dominated by the <span class="hlt">boundary</span>-free part. In the near-horizon limit, the latter is connected to the corresponding quantity for a massless field in the Minkowski bulk by a simple conformal relation. Depending on the value of the Robin coefficient, the presence of the brane can either</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21793569','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21793569"><span>Crossing turbulent <span class="hlt">boundaries</span>: interfacial flux in environmental flows.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Grant, Stanley B; Marusic, Ivan</p> <p>2011-09-01</p> <p>Advances in the visualization and prediction of turbulence are shedding new light on mass transfer in the turbulent <span class="hlt">boundary</span> layer. These discoveries have important implications for many topics in environmental science and engineering, from the transport of earth-warming CO2 across the sea-air interface, to nutrient processing and sediment erosion in rivers, lakes, and the ocean, to pollutant removal in water and wastewater treatment systems. In this article we outline <span class="hlt">current</span> understanding of turbulent <span class="hlt">boundary</span> layer flows, with particular focus on coherent turbulence and its impact on mass transport across the sediment-water interface in marine and freshwater systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3704094','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3704094"><span>Retinal layer segmentation of macular OCT images using <span class="hlt">boundary</span> classification</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lang, Andrew; Carass, Aaron; Hauser, Matthew; Sotirchos, Elias S.; Calabresi, Peter A.; Ying, Howard S.; Prince, Jerry L.</p> <p>2013-01-01</p> <p>Optical coherence tomography (OCT) has proven to be an essential imaging modality for ophthalmology and is proving to be very important in neurology. OCT enables high resolution imaging of the retina, both at the optic nerve head and the macula. Macular retinal layer thicknesses provide useful diagnostic information and have been shown to correlate well with measures of disease severity in several diseases. Since manual segmentation of these layers is time consuming and prone to bias, automatic segmentation methods are critical for full utilization of this technology. In this work, we build a random forest classifier to segment eight retinal layers in macular cube images acquired by OCT. The random forest classifier learns the <span class="hlt">boundary</span> pixels between layers, producing an accurate probability map for each <span class="hlt">boundary</span>, which is then processed to <span class="hlt">finalize</span> the <span class="hlt">boundaries</span>. Using this algorithm, we can accurately segment the entire retina contained in the macular cube to an accuracy of at least 4.3 microns for any of the nine <span class="hlt">boundaries</span>. Experiments were carried out on both healthy and multiple sclerosis subjects, with no difference in the accuracy of our algorithm found between the groups. PMID:23847738</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4433113','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4433113"><span>Ion <span class="hlt">Current</span> Rectification, Limiting and Overlimiting Conductances in Nanopores</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>van Oeffelen, Liesbeth; Van Roy, Willem; Idrissi, Hosni; Charlier, Daniel; Lagae, Liesbet; Borghs, Gustaaf</p> <p>2015-01-01</p> <p>Previous reports on Poisson-Nernst-Planck (PNP) simulations of solid-state nanopores have focused on steady state behaviour under simplified <span class="hlt">boundary</span> conditions. These are Neumann <span class="hlt">boundary</span> conditions for the voltage at the pore walls, and in some cases also Donnan equilibrium <span class="hlt">boundary</span> conditions for concentrations and voltages at both entrances of the nanopore. In this paper, we report time-dependent and steady state PNP simulations under less restrictive <span class="hlt">boundary</span> conditions, including Neumann <span class="hlt">boundary</span> conditions applied throughout the membrane relatively far away from the nanopore. We simulated ion <span class="hlt">currents</span> through cylindrical and conical nanopores with several surface charge configurations, studying the spatial and temporal dependence of the <span class="hlt">currents</span> contributed by each ion species. This revealed that, due to slow co-diffusion of oppositely charged ions, steady state is generally not reached in simulations or in practice. Furthermore, it is shown that ion concentration polarization is responsible for the observed limiting conductances and ion <span class="hlt">current</span> rectification in nanopores with asymmetric surface charges or shapes. Hence, after more than a decade of collective research attempting to understand the nature of ion <span class="hlt">current</span> rectification in solid-state nanopores, a relatively intuitive model is retrieved. Moreover, we measured and simulated <span class="hlt">current</span>-voltage characteristics of rectifying silicon nitride nanopores presenting overlimiting conductances. The similarity between measurement and simulation shows that overlimiting conductances can result from the increased conductance of the electric double-layer at the membrane surface at the depletion side due to voltage-induced polarization charges. The MATLAB source code of the simulation software is available via the website http://micr.vub.ac.be. PMID:25978328</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26068843','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26068843"><span>SUSTAINABILITY. Comment on "Planetary <span class="hlt">boundaries</span>: Guiding human development on a changing planet".</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jaramillo, Fernando; Destouni, Georgia</p> <p>2015-06-12</p> <p>Steffen et al. (Research Articles, 13 February 2015, p. 736) recently assessed <span class="hlt">current</span> global freshwater use, finding it to be well below a corresponding planetary <span class="hlt">boundary</span>. However, they ignored recent scientific advances implying that the global consumptive use of freshwater may have already crossed the associated planetary <span class="hlt">boundary</span>. Copyright © 2015, American Association for the Advancement of Science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920010307','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920010307"><span>Linear and nonlinear dynamic analysis by <span class="hlt">boundary</span> element method. Ph.D. Thesis, 1986 <span class="hlt">Final</span> Report</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ahmad, Shahid</p> <p>1991-01-01</p> <p>An advanced implementation of the direct <span class="hlt">boundary</span> element method (BEM) applicable to free-vibration, periodic (steady-state) vibration and linear and nonlinear transient dynamic problems involving two and three-dimensional isotropic solids of arbitrary shape is presented. Interior, exterior, and half-space problems can all be solved by the present formulation. For the free-vibration analysis, a new real variable BEM formulation is presented which solves the free-vibration problem in the form of algebraic equations (formed from the static kernels) and needs only surface discretization. In the area of time-domain transient analysis, the BEM is well suited because it gives an implicit formulation. Although the integral formulations are elegant, because of the complexity of the formulation it has never been implemented in exact form. In the present work, linear and nonlinear time domain transient analysis for three-dimensional solids has been implemented in a general and complete manner. The formulation and implementation of the nonlinear, transient, dynamic analysis presented here is the first ever in the field of <span class="hlt">boundary</span> element analysis. Almost all the existing formulation of BEM in dynamics use the constant variation of the variables in space and time which is very unrealistic for engineering problems and, in some cases, it leads to unacceptably inaccurate results. In the present work, linear and quadratic isoparametric <span class="hlt">boundary</span> elements are used for discretization of geometry and functional variations in space. In addition, higher order variations in time are used. These methods of analysis are applicable to piecewise-homogeneous materials, such that not only problems of the layered media and the soil-structure interaction can be analyzed but also a large problem can be solved by the usual sub-structuring technique. The analyses have been incorporated in a versatile, general-purpose computer program. Some numerical problems are solved and, through comparisons</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19372616','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19372616"><span>Geometry-based ensembles: toward a structural characterization of the classification <span class="hlt">boundary</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pujol, Oriol; Masip, David</p> <p>2009-06-01</p> <p>This paper introduces a novel binary discriminative learning technique based on the approximation of the nonlinear decision <span class="hlt">boundary</span> by a piecewise linear smooth additive model. The decision border is geometrically defined by means of the characterizing <span class="hlt">boundary</span> points-points that belong to the optimal <span class="hlt">boundary</span> under a certain notion of robustness. Based on these points, a set of locally robust linear classifiers is defined and assembled by means of a Tikhonov regularized optimization procedure in an additive model to create a <span class="hlt">final</span> lambda-smooth decision rule. As a result, a very simple and robust classifier with a strong geometrical meaning and nonlinear behavior is obtained. The simplicity of the method allows its extension to cope with some of today's machine learning challenges, such as online learning, large-scale learning or parallelization, with linear computational complexity. We validate our approach on the UCI database, comparing with several state-of-the-art classification techniques. <span class="hlt">Finally</span>, we apply our technique in online and large-scale scenarios and in six real-life computer vision and pattern recognition problems: gender recognition based on face images, intravascular ultrasound tissue classification, speed traffic sign detection, Chagas' disease myocardial damage severity detection, old musical scores clef classification, and action recognition using 3D accelerometer data from a wearable device. The results are promising and this paper opens a line of research that deserves further attention.</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('http://adsabs.harvard.edu/abs/2014Metro..51.1013M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014Metro..51.1013M"><span><span class="hlt">Final</span> report on COOMET.EM-S11: Supplementary bilateral comparison of the measurement of <span class="hlt">current</span> transformers between UNIIM and PTB</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mohns, Enrico; Sychev, Y.; Roeissle, G.</p> <p>2014-01-01</p> <p>A bilateral comparison of the measurement of <span class="hlt">current</span> transformers was carried out between UNIIM (Russia) and PTB (Germany). For all of the <span class="hlt">current</span> ratio error measurements and the phase displacement measurements there is a close agreement between PTB and UNIIM. Extensive measurements with the travelling standards were carried out at 18 different <span class="hlt">current</span> ratios and at 5 different test points (1%, 5%, 20%, 100% and 120%) each. The range of tested primary <span class="hlt">currents</span> was from 10 mA to 60 kA. It can therefore be concluded that the results of each laboratory agree very well within the calculated measurement uncertainties. No outliers were observed. Considering especially the En factors, the calculated uncertainties seem to be too conservative to some extent. Here there is the possibility to slightly improve the uncertainty budgets in the future if there is a need. The worst En factors are within ±0.6 at 1 kA/5 A and ±0.8 at 3 kA. The <span class="hlt">current</span> comparator 'IW 32' from PTB may have caused that. This was subsequently confirmed. The primary <span class="hlt">current</span> induced a small voltage in the compensation winding. This problem has now been solved. Main text. To reach the main text of this paper, click on <span class="hlt">Final</span> Report. Note that this text is that which appears in Appendix B of the BIPM key comparison database kcdb.bipm.org/. The <span class="hlt">final</span> report has been peer-reviewed and approved for publication by the CCEM, according to the provisions of the CIPM Mutual Recognition Arrangement (CIPM MRA).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27833118','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27833118"><span>Enhanced critical-<span class="hlt">current</span> in P-doped BaFe2As2 thin films on metal substrates arising from poorly aligned grain <span class="hlt">boundaries</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sato, Hikaru; Hiramatsu, Hidenori; Kamiya, Toshio; Hosono, Hideo</p> <p>2016-11-11</p> <p>Thin films of the iron-based superconductor BaFe 2 (As 1-x P x ) 2 (Ba122:P) were fabricated on polycrystalline metal-tape substrates with two kinds of in-plane grain <span class="hlt">boundary</span> alignments (well aligned (4°) and poorly aligned (8°)) by pulsed laser deposition. The poorly aligned substrate is not applicable to cuprate-coated conductors because the in-plane alignment >4° results in exponential decay of the critical <span class="hlt">current</span> density (J c ). The Ba122:P film exhibited higher J c at 4 K when grown on the poorly aligned substrate than on the well-aligned substrate even though the crystallinity was poorer. It was revealed that the misorientation angles of the poorly aligned samples were less than 6°, which are less than the critical angle of an iron-based superconductor, cobalt-doped BaFe 2 As 2 (~9°), and the observed strong pinning in the Ba122:P is attributed to the high-density grain <span class="hlt">boundaries</span> with the misorientation angles smaller than the critical angle. This result reveals a distinct advantage over cuprate-coated conductors because well-aligned metal-tape substrates are not necessary for practical applications of the iron-based superconductors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110013660','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110013660"><span><span class="hlt">Boundary</span> Layer Transition Flight Experiment Overview</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Berger, Karen T.; Anderson, Brian P.; Campbell, Charles H.; Garske, Michael T.; Saucedo, Luis A.; Kinder, Gerald R.; Micklos, Ann M.</p> <p>2011-01-01</p> <p>In support of the <span class="hlt">Boundary</span> Layer Transition Flight Experiment (BLT FE) Project, a manufactured protuberance tile was installed on the port wing of Space Shuttle Orbiter Discovery for STS-119, STS-128, STS-131 and STS-133 as well as Space Shuttle Endeavour for STS-134. Additional instrumentation was installed in order to obtain more spatially resolved measurements downstream of the protuberance. This paper provides an overview of the BLT FE Project with emphasis on the STS-131 and STS-133 results. A high-level overview of the in-situ flight data is presented, along with a summary of the comparisons between pre- and post-flight analysis predictions and flight data. Comparisons show that empirically correlated predictions for <span class="hlt">boundary</span> layer transition onset time closely match the flight data, while predicted surface temperatures were significantly higher than observed flight temperatures. A thermocouple anomaly observed on a number of the missions is discussed as are a number of the mitigation actions that will be taken on the <span class="hlt">final</span> flight, STS-134, including potential alterations of the flight trajectory and changes to the flight instrumentation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18218499','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18218499"><span>Model-based estimation with <span class="hlt">boundary</span> side information or <span class="hlt">boundary</span> regularization [cardiac emission CT].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chiao, P C; Rogers, W L; Fessler, J A; Clinthorne, N H; Hero, A O</p> <p>1994-01-01</p> <p>The authors have previously developed a model-based strategy for joint estimation of myocardial perfusion and <span class="hlt">boundaries</span> using ECT (emission computed tomography). They have also reported difficulties with <span class="hlt">boundary</span> estimation in low contrast and low count rate situations. Here they propose using <span class="hlt">boundary</span> side information (obtainable from high resolution MRI and CT images) or <span class="hlt">boundary</span> regularization to improve both perfusion and <span class="hlt">boundary</span> estimation in these situations. To fuse <span class="hlt">boundary</span> side information into the emission measurements, the authors formulate a joint log-likelihood function to include auxiliary <span class="hlt">boundary</span> measurements as well as ECT projection measurements. In addition, they introduce registration parameters to align auxiliary <span class="hlt">boundary</span> measurements with ECT measurements and jointly estimate these parameters with other parameters of interest from the composite measurements. In simulated PET O-15 water myocardial perfusion studies using a simplified model, the authors show that the joint estimation improves perfusion estimation performance and gives <span class="hlt">boundary</span> alignment accuracy of <0.5 mm even at 0.2 million counts. They implement <span class="hlt">boundary</span> regularization through formulating a penalized log-likelihood function. They also demonstrate in simulations that simultaneous regularization of the epicardial <span class="hlt">boundary</span> and myocardial thickness gives comparable perfusion estimation accuracy with the use of <span class="hlt">boundary</span> side information.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15220143','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15220143"><span>Formation flying design and applications in weak stability <span class="hlt">boundary</span> regions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Folta, David</p> <p>2004-05-01</p> <p>Weak stability regions serve as superior locations for interferomertric scientific investigations. These regions are often selected to minimize environmental disturbances and maximize observation efficiency. Designs of formations in these regions are becoming ever more challenging as more complex missions are envisioned. The development of algorithms to enable the capability for formation design must be further enabled to incorporate better understanding of weak stability <span class="hlt">boundary</span> solution space. This development will improve the efficiency and expand the capabilities of <span class="hlt">current</span> approaches. The Goddard Space Flight Center (GSFC) is <span class="hlt">currently</span> supporting multiple formation missions in weak stability <span class="hlt">boundary</span> regions. This end-to-end support consists of mission operations, trajectory design, and control. It also includes both algorithm and software development. The Constellation-X, Maxim, and Stellar Imager missions are examples of the use of improved numeric methods to attain constrained formation geometries and control their dynamical evolution. This paper presents a survey of formation missions in the weak stability <span class="hlt">boundary</span> regions and a brief description of formation design using numerical and dynamical techniques.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4551391','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4551391"><span>Fixating picture <span class="hlt">boundaries</span> does not eliminate <span class="hlt">boundary</span> extension: Implications for scene representation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gagnier, Kristin Michod; Dickinson, Christopher A.; Intraub, Helene</p> <p>2015-01-01</p> <p>Observers frequently remember seeing more of a scene than was shown (<span class="hlt">boundary</span> extension). Does this reflect a lack of eye fixations to the <span class="hlt">boundary</span> region? Single-object photographs were presented for 14–15 s each. Main objects were either whole or slightly cropped by one <span class="hlt">boundary</span>, creating a salient marker of <span class="hlt">boundary</span> placement. All participants expected a memory test, but only half were informed that <span class="hlt">boundary</span> memory would be tested. Participants in both conditions made multiple fixations to the <span class="hlt">boundary</span> region and the cropped region during study. Demonstrating the importance of these regions, test-informed participants fixated them sooner, longer, and more frequently. <span class="hlt">Boundary</span> ratings (Experiment 1) and border adjustment tasks (Experiments 2–4) revealed <span class="hlt">boundary</span> extension in both conditions. The error was reduced, but not eliminated, in the test-informed condition. Surprisingly, test knowledge and multiple fixations to the salient cropped region, during study and at test, were insufficient to overcome <span class="hlt">boundary</span> extension on the cropped side. Results are discussed within a traditional visual-centric framework versus a multisource model of scene perception. PMID:23547787</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23547787','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23547787"><span>Fixating picture <span class="hlt">boundaries</span> does not eliminate <span class="hlt">boundary</span> extension: implications for scene representation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Michod Gagnier, Kristin; Dickinson, Christopher A; Intraub, Helene</p> <p>2013-01-01</p> <p>Observers frequently remember seeing more of a scene than was shown (<span class="hlt">boundary</span> extension). Does this reflect a lack of eye fixations to the <span class="hlt">boundary</span> region? Single-object photographs were presented for 14-15 s each. Main objects were either whole or slightly cropped by one <span class="hlt">boundary</span>, creating a salient marker of <span class="hlt">boundary</span> placement. All participants expected a memory test, but only half were informed that <span class="hlt">boundary</span> memory would be tested. Participants in both conditions made multiple fixations to the <span class="hlt">boundary</span> region and the cropped region during study. Demonstrating the importance of these regions, test-informed participants fixated them sooner, longer, and more frequently. <span class="hlt">Boundary</span> ratings (Experiment 1) and border adjustment tasks (Experiments 2-4) revealed <span class="hlt">boundary</span> extension in both conditions. The error was reduced, but not eliminated, in the test-informed condition. Surprisingly, test knowledge and multiple fixations to the salient cropped region, during study and at test, were insufficient to overcome <span class="hlt">boundary</span> extension on the cropped side. Results are discussed within a traditional visual-centric framework versus a multisource model of scene perception.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JCoPh.357..230M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JCoPh.357..230M"><span>Simulation of moving <span class="hlt">boundaries</span> interacting with compressible reacting flows using a second-order adaptive Cartesian cut-cell method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Muralidharan, Balaji; Menon, Suresh</p> <p>2018-03-01</p> <p>A high-order adaptive Cartesian cut-cell method, developed in the past by the authors [1] for simulation of compressible viscous flow over static embedded <span class="hlt">boundaries</span>, is now extended for reacting flow simulations over moving interfaces. The main difficulty related to simulation of moving <span class="hlt">boundary</span> problems using immersed <span class="hlt">boundary</span> techniques is the loss of conservation of mass, momentum and energy during the transition of numerical grid cells from solid to fluid and vice versa. Gas phase reactions near solid <span class="hlt">boundaries</span> can produce huge source terms to the governing equations, which if not properly treated for moving <span class="hlt">boundaries</span>, can result in inaccuracies in numerical predictions. The small cell clustering algorithm proposed in our previous work is now extended to handle moving <span class="hlt">boundaries</span> enforcing strict conservation. In addition, the cell clustering algorithm also preserves the smoothness of solution near moving surfaces. A second order Runge-Kutta scheme where the <span class="hlt">boundaries</span> are allowed to change during the sub-time steps is employed. This scheme improves the time accuracy of the calculations when the body motion is driven by hydrodynamic forces. Simple one dimensional reacting and non-reacting studies of moving piston are first performed in order to demonstrate the accuracy of the proposed method. Results are then reported for flow past moving cylinders at subsonic and supersonic velocities in a viscous compressible flow and are compared with theoretical and previously available experimental data. The ability of the scheme to handle deforming <span class="hlt">boundaries</span> and interaction of hydrodynamic forces with rigid body motion is demonstrated using different test cases. <span class="hlt">Finally</span>, the method is applied to investigate the detonation initiation and stabilization mechanisms on a cylinder and a sphere, when they are launched into a detonable mixture. The effect of the filling pressure on the detonation stabilization mechanisms over a hyper-velocity sphere launched into a hydrogen</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2011-11-08/pdf/2011-28855.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2011-11-08/pdf/2011-28855.pdf"><span>76 FR 69283 - Notice of Availability of the <span class="hlt">Final</span> Supplemental Environmental Assessment and Finding of No...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2011-11-08</p> <p>... INTERNATIONAL <span class="hlt">BOUNDARY</span> AND WATER COMMISSION, UNITED STATES AND MEXICO Notice of Availability of..., International <span class="hlt">Boundary</span> and Water Commission, United States and Mexico (USIBWC). ACTION: Notice of Availability... Council on Environmental Quality <span class="hlt">Final</span> Regulations (40 CFR Parts 1500 through 1508), and the United States...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25620801','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25620801"><span>Work-family <span class="hlt">boundary</span> strategies: Stability and alignment between preferred and enacted <span class="hlt">boundaries</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ammons, Samantha K</p> <p>2013-02-01</p> <p>Are individuals bounding work and family the way they would like? Much of the work-family <span class="hlt">boundary</span> literature focuses on whether employees are segmenting or integrating work with family, but does not explore the <span class="hlt">boundaries</span> workers would like to have, nor does it examine the fit between desired and enacted <span class="hlt">boundaries</span>, or assess <span class="hlt">boundary</span> stability. In this study, 23 respondents employed at a large Fortune 500 company were interviewed about their work-family <span class="hlt">boundaries</span> before and after their teams underwent a cultural change initiative that sought to loosen workplace norms and allow employees more autonomy to decide when and where they performed their job tasks. Four distinct <span class="hlt">boundary</span> strategies emerged from the data, with men and parents of young children having better alignment between preferred and enacted <span class="hlt">boundaries</span> than women and those without these caregiving duties. Implications for <span class="hlt">boundary</span> theory and research are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4303250','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4303250"><span>Work-family <span class="hlt">boundary</span> strategies: Stability and alignment between preferred and enacted <span class="hlt">boundaries</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>Ammons, Samantha K.</p> <p>2015-01-01</p> <p>Are individuals bounding work and family the way they would like? Much of the work-family <span class="hlt">boundary</span> literature focuses on whether employees are segmenting or integrating work with family, but does not explore the <span class="hlt">boundaries</span> workers would like to have, nor does it examine the fit between desired and enacted <span class="hlt">boundaries</span>, or assess <span class="hlt">boundary</span> stability. In this study, 23 respondents employed at a large Fortune 500 company were interviewed about their work-family <span class="hlt">boundaries</span> before and after their teams underwent a cultural change initiative that sought to loosen workplace norms and allow employees more autonomy to decide when and where they performed their job tasks. Four distinct <span class="hlt">boundary</span> strategies emerged from the data, with men and parents of young children having better alignment between preferred and enacted <span class="hlt">boundaries</span> than women and those without these caregiving duties. Implications for <span class="hlt">boundary</span> theory and research are discussed. PMID:25620801</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvD..97h5022D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvD..97h5022D"><span>Mode solutions for a Klein-Gordon field in anti-de Sitter spacetime with dynamical <span class="hlt">boundary</span> conditions of Wentzell type</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dappiaggi, Claudio; Ferreira, Hugo R. C.; Juárez-Aubry, Benito A.</p> <p>2018-04-01</p> <p>We study a real, massive Klein-Gordon field in the Poincaré fundamental domain of the (d +1 )-dimensional anti-de Sitter (AdS) spacetime, subject to a particular choice of dynamical <span class="hlt">boundary</span> conditions of generalized Wentzell type, whereby the <span class="hlt">boundary</span> data solves a nonhomogeneous, <span class="hlt">boundary</span> Klein-Gordon equation, with the source term fixed by the normal derivative of the scalar field at the <span class="hlt">boundary</span>. This naturally defines a field in the conformal <span class="hlt">boundary</span> of the Poincaré fundamental domain of AdS. We completely solve the equations for the bulk and <span class="hlt">boundary</span> fields and investigate the existence of bound state solutions, motivated by the analogous problem with Robin <span class="hlt">boundary</span> conditions, which are recovered as a limiting case. <span class="hlt">Finally</span>, we argue that both Robin and generalized Wentzell <span class="hlt">boundary</span> conditions are distinguished in the sense that they are invariant under the action of the isometry group of the AdS conformal <span class="hlt">boundary</span>, a condition which ensures in addition that the total flux of energy across the <span class="hlt">boundary</span> vanishes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1432516-grain-boundary-engineering-control-discontinuous-precipitation-multicomponent-u10mo-alloy','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1432516-grain-boundary-engineering-control-discontinuous-precipitation-multicomponent-u10mo-alloy"><span>Grain <span class="hlt">boundary</span> engineering to control the discontinuous precipitation in multicomponent U10Mo alloy</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Devaraj, Arun; Kovarik, Libor; Kautz, Elizabeth; ...</p> <p>2018-03-30</p> <p>Here, we demonstrate here that locally stabilized structure and compositional segregation at grain <span class="hlt">boundaries</span> in a complex multicomponent alloy can be modified using high temperature homogenization treatment to influence the kinetics of phase transformations initiating from grain <span class="hlt">boundaries</span> during subsequent low temperature annealing. Using aberration-corrected scanning transmission electron microscopy and atom probe tomography of a model multicomponent metallic alloy —uranium-10 wt% molybdenum (U-10Mo) a nuclear fuel, that is highly relevant to worldwide nuclear non-proliferation efforts, we demonstrate the ability to change the structure and compositional segregation at grain <span class="hlt">boundary</span>, which then controls the subsequent discontinuous precipitation kinetics during sub-eutectoid annealing.more » A change in grain <span class="hlt">boundary</span> from one characterized by segregation of Mo and impurities at grain <span class="hlt">boundary</span> to a phase <span class="hlt">boundary</span> with a distinct U 2MoSi 2C wetting phase precipitates introducing Ni and Al rich interphase complexions caused a pronounced reduction in area fraction of subsequent discontinuous precipitation. The broader implication of this work is in highlighting the role of grain <span class="hlt">boundary</span> structure and composition in metallic alloys on dictating the fate of grain <span class="hlt">boundary</span> initiated phase transformations like discontinuous precipitation or cellular transformation. This work highlights a new pathway to tune the grain <span class="hlt">boundary</span> structure and composition to tailor the <span class="hlt">final</span> microstructure of multicomponent metallic alloys.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1432516-grain-boundary-engineering-control-discontinuous-precipitation-multicomponent-u10mo-alloy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1432516-grain-boundary-engineering-control-discontinuous-precipitation-multicomponent-u10mo-alloy"><span>Grain <span class="hlt">boundary</span> engineering to control the discontinuous precipitation in multicomponent U10Mo alloy</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>Devaraj, Arun; Kovarik, Libor; Kautz, Elizabeth</p> <p></p> <p>Here, we demonstrate here that locally stabilized structure and compositional segregation at grain <span class="hlt">boundaries</span> in a complex multicomponent alloy can be modified using high temperature homogenization treatment to influence the kinetics of phase transformations initiating from grain <span class="hlt">boundaries</span> during subsequent low temperature annealing. Using aberration-corrected scanning transmission electron microscopy and atom probe tomography of a model multicomponent metallic alloy —uranium-10 wt% molybdenum (U-10Mo) a nuclear fuel, that is highly relevant to worldwide nuclear non-proliferation efforts, we demonstrate the ability to change the structure and compositional segregation at grain <span class="hlt">boundary</span>, which then controls the subsequent discontinuous precipitation kinetics during sub-eutectoid annealing.more » A change in grain <span class="hlt">boundary</span> from one characterized by segregation of Mo and impurities at grain <span class="hlt">boundary</span> to a phase <span class="hlt">boundary</span> with a distinct U 2MoSi 2C wetting phase precipitates introducing Ni and Al rich interphase complexions caused a pronounced reduction in area fraction of subsequent discontinuous precipitation. The broader implication of this work is in highlighting the role of grain <span class="hlt">boundary</span> structure and composition in metallic alloys on dictating the fate of grain <span class="hlt">boundary</span> initiated phase transformations like discontinuous precipitation or cellular transformation. This work highlights a new pathway to tune the grain <span class="hlt">boundary</span> structure and composition to tailor the <span class="hlt">final</span> microstructure of multicomponent metallic alloys.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950057067&hterms=Open+Field&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DOpen%2BField','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950057067&hterms=Open+Field&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DOpen%2BField"><span>Low-latitude <span class="hlt">boundary</span> layer near noon: An open field line model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lyons, L. R.; Schulz, M.; Pridmore-Brown, D. C.; Roeder, J. L.</p> <p>1994-01-01</p> <p>We propose that many features of the cusp and low-latitude <span class="hlt">boundary</span> layer (LLBL) observed near noon MLT can be explained by interpreting the LLBL as being on open lines with an inner <span class="hlt">boundary</span> at the separatrix between open and closed magnetic field lines. This interpretation places the poleward <span class="hlt">boundary</span> of the LLBL and equatorward <span class="hlt">boundary</span> of the cusp along the field line that bifurcates at the cusp neutral point. The interpretation accounts for the abrupt <span class="hlt">boundary</span> of magnetosheath particles at the inner edge of the LLBL, a feature that is inconsistent with LLBL formation by diffusion onto closed field lines, and for the distribution of magnetosheath particles appearing more as one continuous region than as two distinct regions across the noon cusp/LLBL <span class="hlt">boundary</span>. Furthermore, we can explain the existence of energetic radiation belt electrons and protons with differing pitch angle distributions within the LLBL and their abrupt cutoff at the poleward <span class="hlt">boundary</span> of the LLBL. By modeling the LLBL and cusp region quantitatively, we can account for a hemispherical difference in the location of the equatorial <span class="hlt">boundary</span> of the cusp that is observed to be dependent on the dipole tilt angle but not on the interplanetary magnetic field (IMF) x component. We also find important variations and hemispherical differences in that the size of the LLBL that should depend strongly upon the x component of the IMF. This prediction is observationally testable. <span class="hlt">Finally</span>, we find that when the IMF is strongly northward, the LLBL may include a narrow region adjacent to the magnetopause where field lines are detached (i.e., have both ends connected to the IMF).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960045440','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960045440"><span>Artificial <span class="hlt">Boundary</span> Conditions Based on the Difference Potentials Method</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tsynkov, Semyon V.</p> <p>1996-01-01</p> <p>While numerically solving a problem initially formulated on an unbounded domain, one typically truncates this domain, which necessitates setting the artificial <span class="hlt">boundary</span> conditions (ABC's) at the newly formed external <span class="hlt">boundary</span>. The issue of setting the ABC's appears to be most significant in many areas of scientific computing, for example, in problems originating from acoustics, electrodynamics, solid mechanics, and fluid dynamics. In particular, in computational fluid dynamics (where external problems present a wide class of practically important formulations) the proper treatment of external <span class="hlt">boundaries</span> may have a profound impact on the overall quality and performance of numerical algorithms. Most of the <span class="hlt">currently</span> used techniques for setting the ABC's can basically be classified into two groups. The methods from the first group (global ABC's) usually provide high accuracy and robustness of the numerical procedure but often appear to be fairly cumbersome and (computationally) expensive. The methods from the second group (local ABC's) are, as a rule, algorithmically simple, numerically cheap, and geometrically universal; however, they usually lack accuracy of computations. In this paper we first present a survey and provide a comparative assessment of different existing methods for constructing the ABC's. Then, we describe a relatively new ABC's technique of ours and review the corresponding results. This new technique, in our opinion, is <span class="hlt">currently</span> one of the most promising in the field. It enables one to construct such ABC's that combine the advantages relevant to the two aforementioned classes of existing methods. Our approach is based on application of the difference potentials method attributable to V. S. Ryaben'kii. This approach allows us to obtain highly accurate ABC's in the form of certain (nonlocal) <span class="hlt">boundary</span> operator equations. The operators involved are analogous to the pseudodifferential <span class="hlt">boundary</span> projections first introduced by A. P. Calderon and then</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUSMSM21A..01G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUSMSM21A..01G"><span>Plasmapause <span class="hlt">Boundary</span> Dynamics and the Interplanetary Magnetic Field Effect</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Goldstein, J.</p> <p>2006-05-01</p> <p>The plasmapause is the outer <span class="hlt">boundary</span> of the plasmasphere, the roughly toroidal region of cold, dense, corotating plasma that encircles the Earth and can extend several Earth radii (RE) out into space. The source of plasma in this region is ionospheric outflow (or upflow), which fills plasmaspheric field lines with a mixture of protons, helium ions, and oxygen ions on a timescale of several days. A distinct outer plasmapause <span class="hlt">boundary</span> forms when plasmaspheric plasma is removed, a process known as erosion. Plasmaspheric erosion occurs most strongly during times of southward interplanetary magnetic field (IMF), when magnetospheric convection is greatly enhanced. Decades of theory and observation support the idea that enhanced sunward convection (during southward IMF) forms large plumes of dense plasma that stretch sunward from the main plasmasphere during erosion. The plasmapause during erosion events is distorted: reduced on the nightside, elongated on the dayside, and in general, overlapping the <span class="hlt">boundaries</span> of regions of warmer plasmas (such as the ring <span class="hlt">current</span> and radiation belts) that experience increased loss rates from wave-particle interactions in the overlap regions. Thus, the plasmapause <span class="hlt">boundary</span> is of critical importance to the global dynamics of these warmer particles. In recent years, the southward IMF (i.e., convection) effect on the plasmapause has been fairly well characterized, but what has received less attention is the northward IMF effect. What happens at the plasmapause <span class="hlt">boundary</span> following disturbances, when convection is reduced but ionospheric outflow has not yet had enough time to refill the plasmaspheric flux tubes? Observations by CRRES, Polar, IMAGE, Cluster, and other spacecraft have shown a bewildering variety of fine-scale plasmapause density structure during recovery and deep quiet phases. Many plasmapause features have been classified, sorted and named, but nonetheless, remain unexplained. This paper will present our <span class="hlt">current</span> understanding</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3827872','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3827872"><span>No-<span class="hlt">boundary</span> thinking in bioinformatics research</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><span class="hlt">Currently</span> there are definitions from many agencies and research societies defining “bioinformatics” as deriving knowledge from computational analysis of large volumes of biological and biomedical data. Should this be the bioinformatics research focus? We will discuss this issue in this review article. We would like to promote the idea of supporting human-infrastructure (HI) with no-<span class="hlt">boundary</span> thinking (NT) in bioinformatics (HINT). PMID:24192339</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.episodes.co.in/www/backissues/244/239-244%20Metcalfe%20.pdf','USGSPUBS'); return false;" href="http://www.episodes.co.in/www/backissues/244/239-244%20Metcalfe%20.pdf"><span>The Permian-Triassic <span class="hlt">boundary</span> & mass extinction in China</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Metcalfe, I.; Nicoll, R.S.; Mundil, R.; Foster, C.; Glen, J.; Lyons, J.; Xiaofeng, W.; Cheng-Yuan, W.; Renne, P.R.; Black, L.; Xun, Q.; Xiaodong, M.</p> <p>2001-01-01</p> <p>The first appearance of Hindeodus parvus (Kozur & Pjatakova) at the Permian-Triassic (P-T) GSSP level (base of Bed 27c) at Meishan is here confirmed. Hindeodus changxingensis Wang occurs from Beds 26 to 29 at Meishan and appears to be restricted to the narrow <span class="hlt">boundary</span> interval immediately above the main mass extinction level in Bed 25. It is suggested that this species is therefore a valuable P-T <span class="hlt">boundary</span> interval index taxon. Our collections from the Shangsi section confirm that the first occurrence of Hindeodus parvus in that section is about 5 in above the highest level from which a typical Permian fauna is recovered. This may suggest that that some section may be missing at Meishan. The age of the <span class="hlt">currently</span> defined Permian-Triassic <span class="hlt">Boundary</span> is estimated by our own studies and a reassessment of previous worker's data at c. 253 Ma, slightly older than our IDTIMS 206Pb/238U age of 252.5 ??0.3 Ma for Bed 28, just 8 cm above the GSSP <span class="hlt">boundary</span> (Mundil et al., 2001). The age of the main mass extinction, at the base of Bed 25 at Meishan, is estimated at slightly older than 254 Ma based on an age of >254 Ma for the Bed 25 ash. Regardless of the absolute age of the <span class="hlt">boundary</span>, it is evident that the claimed <165,000 y short duration for the negative carbon isotope excursion at the P-T <span class="hlt">boundary</span> (Bowring et al., 1998) cannot be confirmed. Purportedly extraterrestrial fullerenes at the <span class="hlt">boundary</span> (Hecker et al., 2001) have equivocal significance due to their chronostratigraphic non-uniqueness and their occurrence in a volcanic ash.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19750030199&hterms=application+boundary+layer+flat+plate&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dapplication%2Bboundary%2Blayer%2Bflat%2Bplate','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19750030199&hterms=application+boundary+layer+flat+plate&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dapplication%2Bboundary%2Blayer%2Bflat%2Bplate"><span>An eddy-viscosity treatment of the unsteady turbulent <span class="hlt">boundary</span> layer on a flat plate in an expansion tube</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gupta, R. N.; Trimpi, R. L.</p> <p>1974-01-01</p> <p>An analysis is presented for the relaxation of a turbulent <span class="hlt">boundary</span> layer on a semiinfinite flat plate after passage of a shock wave and a trailing driver gas-driven gas interface. The problem has special application to expansion tube flows. The flow-governing equations have been transformed into the Lamcrocco variables. The numerical results indicate that a fully turbulent <span class="hlt">boundary</span> layer relaxes faster to the <span class="hlt">final</span> steady-state values of heat transfer and skin-friction than a fully laminar <span class="hlt">boundary</span> layer.</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('http://adsabs.harvard.edu/abs/2017JGRD..122.4578L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRD..122.4578L"><span>Evaluation of retrieval methods of daytime convective <span class="hlt">boundary</span> layer height based on lidar data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Hong; Yang, Yi; Hu, Xiao-Ming; Huang, Zhongwei; Wang, Guoyin; Zhang, Beidou; Zhang, Tiejun</p> <p>2017-04-01</p> <p>The atmospheric <span class="hlt">boundary</span> layer height is a basic parameter in describing the structure of the lower atmosphere. Because of their high temporal resolution, ground-based lidar data are widely used to determine the daytime convective <span class="hlt">boundary</span> layer height (CBLH), but the <span class="hlt">currently</span> available retrieval methods have their advantages and drawbacks. In this paper, four methods of retrieving the CBLH (i.e., the gradient method, the idealized backscatter method, and two forms of the wavelet covariance transform method) from lidar normalized relative backscatter are evaluated, using two artificial cases (an idealized profile and a case similar to real profile), to test their stability and accuracy. The results show that the gradient method is suitable for high signal-to-noise ratio conditions. The idealized backscatter method is less sensitive to the first estimate of the CBLH; however, it is computationally expensive. The results obtained from the two forms of the wavelet covariance transform method are influenced by the selection of the initial input value of the wavelet amplitude. Further sensitivity analysis using real profiles under different orders of magnitude of background counts show that when different initial input values are set, the idealized backscatter method always obtains consistent CBLH. For two wavelet methods, the different CBLH are always obtained with the increase in the wavelet amplitude when noise is significant. <span class="hlt">Finally</span>, the CBLHs as measured by three lidar-based methods are evaluated by as measured from L-band soundings. The <span class="hlt">boundary</span> layer heights from two instruments coincide with ±200 m in most situations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhPl...19h2103M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhPl...19h2103M"><span>Kink modes and surface <span class="hlt">currents</span> associated with vertical displacement events</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Manickam, Janardhan; Boozer, Allen; Gerhardt, Stefan</p> <p>2012-08-01</p> <p>The fast termination phase of a vertical displacement event (VDE) in a tokamak is modeled as a sequence of shrinking equilibria, where the core <span class="hlt">current</span> profile remains constant so that the safety-factor at the axis, qaxis, remains fixed and the qedge systematically decreases. At some point, the n = 1 kink mode is destabilized. Kink modes distort the magnetic field lines outside the plasma, and surface <span class="hlt">currents</span> are required to nullify the normal component of the B-field at the plasma <span class="hlt">boundary</span> and maintain equilibrium at finite pressure. If the plasma touches a conductor, the <span class="hlt">current</span> can be transferred to the conductor, and may be measurable by the halo <span class="hlt">current</span> monitors. This report describes a practical method to model the plasma as it evolves during a VDE, and determine the surface <span class="hlt">currents</span>, needed to maintain equilibrium. The main results are that the onset conditions for the disruption are that the growth-rate of the n = 1 kink exceeds half the Alfven time and the associated surface <span class="hlt">current</span> needed to maintain equilibrium exceeds one half of the core plasma <span class="hlt">current</span>. This occurs when qedge drops below a low integer, usually 2. Application to NSTX provides favorable comparison with non-axisymmetric halo-<span class="hlt">current</span> measurements. The model is also applied to ITER and shows that the 2/1 mode is projected to be the most likely cause of the <span class="hlt">final</span> disruption.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhFl...30d0911J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhFl...30d0911J"><span>Rotor <span class="hlt">boundary</span> layer development with inlet guide vane (IGV) wake impingement</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jia, Lichao; Zou, Tengda; Zhu, Yiding; Lee, Cunbiao</p> <p>2018-04-01</p> <p>This paper examines the transition process in a <span class="hlt">boundary</span> layer on a rotor blade under the impingement of an inlet guide vane wake. The effects of wake strengths and the reduced frequency on the unsteady <span class="hlt">boundary</span> layer development on a low-speed axial compressor were investigated using particle image velocimetry. The measurements were carried out at two reduced frequencies (fr = fIGVS0/U2i, fr = 1.35, and fr = 0.675) with the Reynolds number, based on the blade chord and the isentropic inlet velocity, being 97 500. At fr = 1.35, the flow separated at the trailing edge when the wake strength was weak. However, the separation was almost totally suppressed as the wake strength increased. For the stronger wake, both the wake's high turbulence and the negative jet behavior of the wake dominated the interaction between the unsteady wake and the separated <span class="hlt">boundary</span> layer on the suction surface of the airfoil. The <span class="hlt">boundary</span> layer displacement thickened first due to the negative jet effect. Then, as the disturbances developed underneath the wake, the <span class="hlt">boundary</span> layer thickness reduced gradually. The high disturbance region convected downstream at a fraction of the free-stream velocity and spread in the streamwise direction. The separation on the suction surface was suppressed until the next wake's arrival. Because of the long recovery time at fr = 0.675, the <span class="hlt">boundary</span> layer thickened gradually as the wake convected further downstream and <span class="hlt">finally</span> separated due to the adverse pressure gradient. The different <span class="hlt">boundary</span> layer states in turn affected the development of disturbances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15209372','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15209372"><span>How children remember neutral and emotional pictures: <span class="hlt">boundary</span> extension in children's scene memories.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Candel, Ingrid; Merckelbach, Harald; Houben, Katrijn; Vandyck, Inne</p> <p>2004-01-01</p> <p><span class="hlt">Boundary</span> extension is the tendency to remember more of a scene than was actually shown. The dominant interpretation of this memory illusion is that it originates from schemata that people construct when viewing a scene. Evidence of <span class="hlt">boundary</span> extension has been obtained primarily with adult participants who remember neutral pictures. The <span class="hlt">current</span> study addressed the developmental stability of this phenomenon. Therefore, we investigated whether children aged 10-12 years display <span class="hlt">boundary</span> extension for neutral pictures. Moreover, we examined emotional scene memory. Eighty-seven children drew pictures from memory after they had seen either neutral or emotional pictures. Both their neutral and emotional drawings revealed <span class="hlt">boundary</span> extension. Apparently, the schema construction that underlies <span class="hlt">boundary</span> extension is a robust and ubiquitous process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930039359&hterms=McCormick&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DMcCormick','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930039359&hterms=McCormick&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DMcCormick"><span><span class="hlt">Boundary</span> layer energization by means of optimized vortex generators</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Barber, T. J.; Mounts, J. S.; Mccormick, D. C.</p> <p>1993-01-01</p> <p>A three-dimensional, multi-block, multi-zone, Euler analysis has been developed and applied to analyze the flow processes induced by a lateral array of low profile vortex generators (VG). These vortex generators have been shown to alleviate <span class="hlt">boundary</span> layer separation through the generation of streamwise vorticity. The analysis has been applied to help develop improved VG configurations in an efficient manner. Special attention has been paid to determining the accuracy requirements of the solver for calculations in which vortical mechanisms are dominant. The analysis has been used to assess the effectiveness or <span class="hlt">boundary</span> layer energization capacity of different VG's, including the effect of scale and shape variation. <span class="hlt">Finally</span>, the analysis has been validated through comparisons with experimental data obtained in a large-scale low-speed wind tunnel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920029440&hterms=FAC&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DFAC','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920029440&hterms=FAC&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DFAC"><span>DMSP F7 observations of a substorm field-aligned <span class="hlt">current</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lopez, R. E.; Spence, H. E.; Meng, C.-I.</p> <p>1991-01-01</p> <p>Observations are described of a substorm field-aligned <span class="hlt">current</span> (FAC) system traversed by the DMSP F7 spacecraft just after 0300 UT on April 25, 1985. It is shown that the substorm FAC portion of the <span class="hlt">current</span> system was located equatorward of the <span class="hlt">boundary</span> between open and closed field lines. The equatorward <span class="hlt">boundary</span> of the substorm FAC into the magnetotail was mapped using the Tsyganenko (1987) model, showing that the <span class="hlt">boundary</span> corresponds to 6.9 earth radii. The result is consistent with the suggestion of Akasofu (1972) and Lopez and Lui (1990) that the region of substorm initiation lies relatively close to the earth and the concept that an essential feature of substorms is the disruption and diversion of the near-earth <span class="hlt">current</span> sheet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28135391','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28135391"><span>Managing Professional and Nurse-Patient Relationship <span class="hlt">Boundaries</span> in Mental Health.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Valente, Sharon M</p> <p>2017-01-01</p> <p>Caring nurse-patient relationships in mental health settings are key components in helping patients recover. These professional relationships provide a safe, trustworthy, reliable, and secure foundation for therapeutic interactions; however, nurses face challenges in setting and maintaining relationship <span class="hlt">boundaries</span>. Although patients ask for special privileges, romantic interactions, and social media befriending, or offer expensive gifts, nurses must recognize that these <span class="hlt">boundary</span> violations may erode trust and harm patients. These violations may also trigger discipline for nurses. Professional relationship guidelines must be applied with thoughtful consideration, and nurses must monitor their emotions and reactions in these relationships. The <span class="hlt">current</span> article is a sharing of personal experiences about <span class="hlt">boundaries</span> augmented by evidence in the literature, and focuses on managing potential <span class="hlt">boundary</span> violations (i.e., social media, sexuality, over-involvement, and gift giving) in mental health settings. [Journal of Psychosocial Nursing and Mental Health Services, 55(1), 45-51.]. Copyright 2017, SLACK Incorporated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004APS..DFD.JD005K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004APS..DFD.JD005K"><span><span class="hlt">Boundary</span>-Layer Control: In Memory of Bill Reynolds</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, John</p> <p>2004-11-01</p> <p>Professor Bill Reynolds (1933-2004) inspired many students and colleagues with his never-ending curiosity and thought-provoking ideas. Bill's relentless energy, together with his hallmark can-do character and do-it-yourself attitude, led to many seminal contributions to mechanical engineering in general, and fluid mechanics in particular. He has left a lasting impact on many of us, especially for those who had the privilege of working closely with him. Some of my <span class="hlt">current</span> work on <span class="hlt">boundary</span>-layer control, the use of neural networks in particular, were inspired by many discussions with Bill. He was among the first to see the potential of control-theoretic approaches for flow control, which has become the main thrust of my <span class="hlt">current</span> research. Without his continued encouragement, I would not have been deeply involved in this line of research; and perhaps, we would not have seen the <span class="hlt">current</span> flurry of research activities in applying modern control theories to flow control. In memory of Bill Reynolds, who himself has contributed much to flow control, an analysis of <span class="hlt">boundary</span>-layer control from a linear system perspective will be presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090026006&hterms=chemical+engineering&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dchemical%2Bengineering','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090026006&hterms=chemical+engineering&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dchemical%2Bengineering"><span>Roles of Engineering Correlations in Hypersonic Entry <span class="hlt">Boundary</span> Layer Transition Prediction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Campbell, Charles H.; Anderson, Brian P.; King, Rudolph A.; Kegerise, Michael A.; Berry, Scott A.; Horvath, Thomas J.</p> <p>2010-01-01</p> <p>Efforts to design and operate hypersonic entry vehicles are constrained by many considerations that involve all aspects of an entry vehicle system. One of the more significant physical phenomenon that affect entry trajectory and thermal protection system design is the occurrence of <span class="hlt">boundary</span> layer transition from a laminar to turbulent state. During the Space Shuttle Return To Flight activity following the loss of Columbia and her crew of seven, NASA's entry aerothermodynamics community implemented an engineering correlation based framework for the prediction of <span class="hlt">boundary</span> layer transition on the Orbiter. The methodology for this implementation relies upon similar correlation techniques that have been is use for several decades. What makes the Orbiter <span class="hlt">boundary</span> layer transition correlation implementation unique is that a statistically significant data set was acquired in multiple ground test facilities, flight data exists to assist in establishing a better correlation and the framework was founded upon state of the art chemical nonequilibrium Navier Stokes flow field simulations. Recent entry flight testing performed with the Orbiter Discovery now provides a means to validate this engineering correlation approach to higher confidence. These results only serve to reinforce the essential role that engineering correlations <span class="hlt">currently</span> exercise in the design and operation of entry vehicles. The framework of information related to the Orbiter empirical <span class="hlt">boundary</span> layer transition prediction capability will be utilized to establish a fresh perspective on this role, and to discuss the characteristics which are desirable in a next generation advancement. The details of the paper will review the experimental facilities and techniques that were utilized to perform the implementation of the Orbiter RTF BLT Vsn 2 prediction capability. Statistically significant results for multiple engineering correlations from a ground testing campaign will be reviewed in order to describe why only</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3951802','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3951802"><span><span class="hlt">Boundary</span> Development in the Field of International Nutrition Science12</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Centrone Stefani, Monique; Humphries, Debbie L.</p> <p>2014-01-01</p> <p>Using a sociological approach that elaborates on key observations of institutional entrepreneurs in international nutrition, this paper explores institutional <span class="hlt">boundaries</span> and <span class="hlt">boundary</span> work in international nutrition. Sociological concepts of “<span class="hlt">boundary</span> making” and “situated knowledge” are applied to the <span class="hlt">boundaries</span> between the nutrition sciences and lay nutrition knowledge in nutrition intervention. These concepts allow an analysis of how nutrition science creates <span class="hlt">boundaries</span> between its field and other sciences and between nutrition as a science and other nutrition practices, providing additional perspective on <span class="hlt">current</span> challenges in global food security and malnutrition. Analysis of <span class="hlt">boundary</span> processes in international nutrition can also illuminate the development of “implementation” or “delivery science” in the field of international nutrition as it attempts to strengthen effectiveness of global efforts to reduce malnutrition. Although some risk taking in the academic world is rewarded, the analysis indicates that there are underlying processes that may inhibit full partnership with local people in the course of intervention work that builds scientific nutrition knowledge. As nutrition science becomes increasingly central to development, the <span class="hlt">boundaries</span> that are reinforced by digging in heels over the implementation of programs with little local input or softened by inviting local stakeholders to publicly consider the problems in global nutrition together are important to consider in helping to create directions that favor viable solutions. PMID:24618761</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPCS..113..108N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPCS..113..108N"><span>Atomistic modeling of grain <span class="hlt">boundary</span> behavior under shear conditions in magnesium and magnesium-based 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>Nahhas, M. K.; Groh, S.</p> <p>2018-02-01</p> <p>In this study, the structure, the energetic, and the strength of a { 10 1 bar 1 } < 11 2 bar 0 > symmetric tilt grain <span class="hlt">boundary</span> in magnesium and magnesium binary alloys were analyzed in the framework of (semi-)empirical potentials. Following a systematic investigation of the transferability and accuracy of the interatomic potentials, atomistic calculations of the grain <span class="hlt">boundary</span> energy, the grain <span class="hlt">boundary</span> sliding energy, and the grain <span class="hlt">boundary</span> strength were performed in pure magnesium and in binary MgX alloys (X = Al, Ca, Gd, Li, Sn, Y, Ag, Nd, and Pb). The data gained in this study were analyzed to identify the most critical material parameters controlling the strength of the grain <span class="hlt">boundary</span>, and their consequence on atomic shuffling motions occurring at the grain <span class="hlt">boundary</span>. From the methodology perspective, the role of in-plane and out-of plane relaxation on the grain <span class="hlt">boundary</span> sliding energy curves was investigated. In pure magnesium, the results showed that in-plane relaxation is critical in activating b2{ 10 1 bar 1 } twinning dislocation resulting in grain <span class="hlt">boundary</span> migration. In the alloy systems, however, grain <span class="hlt">boundary</span> migration was disabled as a consequence of the pinning of the grain <span class="hlt">boundary</span> by segregated elements. <span class="hlt">Finally</span>, while the grain <span class="hlt">boundary</span> energy, the shape of the grain <span class="hlt">boundary</span> sliding energy curves, and the grain <span class="hlt">boundary</span> sliding energy are critical parameters controlling the grain <span class="hlt">boundary</span> strength in pure magnesium, only the grain <span class="hlt">boundary</span> energy and the segregation energy of the alloying elements at the grain <span class="hlt">boundary</span> were identified as critical material parameters in the alloys system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=alignment+AND+fit&pg=2&id=EJ1005892','ERIC'); return false;" href="https://eric.ed.gov/?q=alignment+AND+fit&pg=2&id=EJ1005892"><span>Work-Family <span class="hlt">Boundary</span> Strategies: Stability and Alignment between Preferred and Enacted <span class="hlt">Boundaries</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>Ammons, Samantha K.</p> <p>2013-01-01</p> <p>Are individuals bounding work and family the way they would like? Much of the work-family <span class="hlt">boundary</span> literature focuses on whether employees are segmenting or integrating work with family, but does not explore the <span class="hlt">boundaries</span> workers would like to have, nor does it examine the fit between desired and enacted <span class="hlt">boundaries</span>, or assess <span class="hlt">boundary</span> stability.…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997SurSc.371...79Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997SurSc.371...79Z"><span>Antiphase <span class="hlt">boundaries</span> on low-energy-ion bombarded Ge(001)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zandvliet, H. J. W.; de Groot, E.</p> <p>1997-01-01</p> <p>Surface vacancy and adatom clusters have been created on Ge(001) by bombarding the surface with 800 eV argon ions at various substrate temperatures ranging from room temperature to 600 K. The vacancies preferentially annihilate at the ends rather than at the sides of the dimer rows, resulting in monolayer deep vacancy islands which are elongated in a direction of the dimer rows of the upper terrace. As vacancy islands nucleate and expand, the dimer rows in neighbouring vacancy islands need not, in general, align with each other. An antiphase <span class="hlt">boundary</span> will develop if two growing vacancy islands meet, but their internal dimer rows are not in the same registry. In contrast to Si(001), where only one type of antiphase <span class="hlt">boundary</span> is found, we have found three different types of antiphase <span class="hlt">boundaries</span> on Ge(001). Higher dose (> several monolayers) room temperature ion bombardment followed by annealing at temperatures in the range 400-500 K results in a surface which contains a high density of valleys. In addition to the preference for the annihilation of dimer vacancies at descending versus ascending steps we also suggest that the development of antiphase <span class="hlt">boundaries</span> drives the roughening of this surface. <span class="hlt">Finally</span>, several atomic rearrangement events, which might be induced by the tunneling process, are observed after low-dose ion bombardment at room temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..1214170M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..1214170M"><span>Links Between the Deep Western <span class="hlt">Boundary</span> <span class="hlt">Current</span>, Labrador Sea Water Formation and Export, and the Meridional Overturning Circulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Myers, Paul G.; Kulan, Nilgun</p> <p>2010-05-01</p> <p>Based on an isopyncal analysis of historical data, 3-year overlapping triad fields of objectively analysed temperature and salinity are produced for the Labrador Sea, covering 1949-1999. These fields are then used to spectrally nudge an eddy-permitting ocean general circulation model of the sub-polar gyre, otherwise forced by inter annually varying surface forcing based upon the Coordinated Ocean Reference Experiment (CORE). High frequency output from the reanalysis is used to examine Labrador Sea Water formation and its export. A number of different apprpoaches are used to estimate Labrador Sea Water formation, including an instanteous kinematic approach to calculate the annual rate of water mass subduction at a given density range. Historical transports are computed along sections at 53 and 56N for several different water masses for comparison with recent observations, showing a decline in the stength of the deep western <span class="hlt">boundary</span> <span class="hlt">current</span> with time. The variability of the strength of the meridional overturning circulation (MOC) from the reanalysis is also examined in both depth and density space. Linkages between MOC variability and water mass formation variability is considered.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2011-11-23/pdf/2011-30167.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2011-11-23/pdf/2011-30167.pdf"><span>76 FR 72437 - Minor <span class="hlt">Boundary</span> Revision at Colorado National Monument</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2011-11-23</p> <p>...Notice is hereby given that, pursuant to 16 U.S.C. 460l- 9(c)(1), the <span class="hlt">boundary</span> of Colorado National Monument is modified to include an additional two and forty-five hundredths (2.45) acres of land identified as Tract 01-140, tax parcel number 2697-343-04-009. The land is located in Mesa County, Colorado, immediately adjacent to the <span class="hlt">current</span> eastern <span class="hlt">boundary</span> of Colorado National Monument. The <span class="hlt">boundary</span> revision is depicted on Map No. 119/106,532 dated January 2011. The map is available for inspection at the following locations: National Park Service, Intermountain Land Resources Program Center, 12795 W. Alameda Parkway, Lakewood, CO 80225-0287 and National Park Service, Department of the Interior, Washington, DC 20240.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvF...3c4101S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvF...3c4101S"><span>Non-self-similar viscous gravity <span class="hlt">currents</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sutherland, Bruce R.; Cote, Kristen; Hong, Youn Sub Dominic; Steverango, Luke; Surma, Chris</p> <p>2018-03-01</p> <p>Lock-release experiments are performed focusing upon the evolution of near-pure glycerol flowing into fresh water. If the lock height is sufficiently tall, the <span class="hlt">current</span> is found to propagate for many lock lengths close to the speed predicted for energy-conserving moderately non-Boussinesq gravity <span class="hlt">currents</span>. The <span class="hlt">current</span> then slows to a near stop as the <span class="hlt">current</span> head ceases to be elevated relative to its tail and the <span class="hlt">current</span> as a whole forms a wedge shape. By contrast, an experiment of near-pure glycerol advancing under air exhibits the well-known slowing of the <span class="hlt">current</span> such that the front position increases as a one-fifth power of time. The evolution of a viscous gravity <span class="hlt">current</span> in water is also qualitatively different from that for a high-Reynolds number gravity <span class="hlt">current</span> which transitions smoothly from a constant speed to self-similar to viscous regime. The reason a viscous gravity <span class="hlt">current</span> flowing under water moves initially at near-constant speed is not due to a lubrication layer forming below the <span class="hlt">current</span>. Rather it is due to the return flow of water into the lock establishing a <span class="hlt">current</span> with an elevated head that is taller than the viscous <span class="hlt">boundary</span> layer depth near the <span class="hlt">current</span> nose. The flow near the top of the head advances to the nose where it comes into contact with the tank bottom. Meanwhile the ambient fluid is pushed up and over the head rather than being drawn underneath it. The front slows rapidly to a near stop as the head height reduces to that comparable to the <span class="hlt">boundary</span> layer depth underneath the head. The initial speed and entrainment into the <span class="hlt">current</span> are shown to depend upon the ratio, Rℓ, of the starting <span class="hlt">current</span> height to the characteristic <span class="hlt">boundary</span> layer depth. In particular, entrainment via the turbulent shear flow over the head is found to increase the volume by less than 10 % during its evolution if Rℓ≲10 but increases by as much as 100 % for high-Reynolds number gravity <span class="hlt">currents</span>. A conceptual model is developed that captures the transition</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22370237-current-singularities-quasi-separatrix-layers-three-dimensional-magnetic-nulls','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22370237-current-singularities-quasi-separatrix-layers-three-dimensional-magnetic-nulls"><span><span class="hlt">Current</span> singularities at quasi-separatrix layers and three-dimensional magnetic nulls</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>Craig, I. J. D.; Effenberger, Frederic, E-mail: feffen@waikato.ac.nz</p> <p>2014-11-10</p> <p>The open problem of how singular <span class="hlt">current</span> structures form in line-tied, three-dimensional magnetic fields is addressed. A Lagrangian magneto-frictional relaxation method is employed to model the field evolution toward the <span class="hlt">final</span> near-singular state. Our starting point is an exact force-free solution of the governing magnetohydrodynamic equations that is sufficiently general to allow for topological features like magnetic nulls to be inside or outside the computational domain, depending on a simple set of parameters. Quasi-separatrix layers (QSLs) are present in these structures and, together with the magnetic nulls, they significantly influence the accumulation of <span class="hlt">current</span>. It is shown that perturbations affectingmore » the lateral <span class="hlt">boundaries</span> of the configuration lead not only to collapse around the magnetic null but also to significant QSL <span class="hlt">currents</span>. Our results show that once a magnetic null is present, the developing <span class="hlt">currents</span> are always attracted to that specific location and show a much stronger scaling with resolution than the <span class="hlt">currents</span> that form along the QSL. In particular, the null-point scalings can be consistent with models of 'fast' reconnection. The QSL <span class="hlt">currents</span> also appear to be unbounded but give rise to weaker singularities, independent of the perturbation amplitude.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT........85M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT........85M"><span>Grain <span class="hlt">boundaries</span> structures and wetting in doped silicon, nickel and copper</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meshinchi Asl, Kaveh</p> <p></p> <p>This thesis reports a series of fundamental investigations of grain <span class="hlt">boundary</span> wetting, adsorption and structural (phases) transitions in doped Ni, Cu and Si with technological relevance to liquid metal embrittlement, liquid metal corrosion and device applications. First, intrinsically ductile metals are prone to catastrophic failure when exposed to certain liquid metals, but the atomic level mechanism for this effect is not fully understood. A nickel sample infused with bismuth atoms was characterized and a bilayer interfacial phase that is the underlying cause of embrittlement was observed. In a second related study, we showed that addition of minor impurities can significantly enhance the intergranular penetration of bismuth based liquids in polycrystalline nickel and copper, thereby increasing the liquid metal corrosion rates. Furthermore, we extended a concept that was initially proposed in the Rice-Wang model for grain <span class="hlt">boundary</span> embrittlement to explain our observations of the impurity-enhanced intergranular penetration of liquid metals. <span class="hlt">Finally</span>, a grain-<span class="hlt">boundary</span> transition from a bilayer to an intrinsic is observed in the Si-Au system. This observation directly shows that a grain <span class="hlt">boundary</span> can exhibit a first-order "phase" transition, which often implies abrupt changes in properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013ERL.....8d4048A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013ERL.....8d4048A"><span>The topology of non-linear global carbon dynamics: from tipping points to planetary <span class="hlt">boundaries</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anderies, J. M.; Carpenter, S. R.; Steffen, Will; Rockström, Johan</p> <p>2013-12-01</p> <p>We present a minimal model of land use and carbon cycle dynamics and use it to explore the relationship between non-linear dynamics and planetary <span class="hlt">boundaries</span>. Only the most basic interactions between land cover and terrestrial, atmospheric, and marine carbon stocks are considered in the model. Our goal is not to predict global carbon dynamics as it occurs in the actual Earth System. Rather, we construct a conceptually reasonable heuristic model of a feedback system between different carbon stocks that captures the qualitative features of the actual Earth System and use it to explore the topology of the <span class="hlt">boundaries</span> of what can be called a ‘safe operating space’ for humans. The model analysis illustrates the existence of dynamic, non-linear tipping points in carbon cycle dynamics and the potential complexity of planetary <span class="hlt">boundaries</span>. <span class="hlt">Finally</span>, we use the model to illustrate some challenges associated with navigating planetary <span class="hlt">boundaries</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EPJB...85..189B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EPJB...85..189B"><span>Transport across nanogaps using self-consistent <span class="hlt">boundary</span> conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Biswas, D.; Kumar, R.</p> <p>2012-06-01</p> <p>Charge particle transport across nanogaps is studied theoretically within the Schrodinger-Poisson mean field framework. The determination of self-consistent <span class="hlt">boundary</span> conditions across the gap forms the central theme in order to allow for realistic interface potentials (such as metal-vacuum) which are smooth at the <span class="hlt">boundary</span> and do not abruptly assume a constant value at the interface. It is shown that a semiclassical expansion of the transmitted wavefunction leads to approximate but self consistent <span class="hlt">boundary</span> conditions without assuming any specific form of the potential beyond the gap. Neglecting the exchange and correlation potentials, the quantum Child-Langmuir law is investigated. It is shown that at zero injection energy, the quantum limiting <span class="hlt">current</span> density (Jc) is found to obey the local scaling law Jc ~ Vgα/D5-2α with the gap separation D and voltage Vg. The exponent α > 1.1 with α → 3/2 in the classical regime of small de Broglie wavelengths.</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('http://adsabs.harvard.edu/abs/2017PhLA..381.3909Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhLA..381.3909Z"><span>Effect of <span class="hlt">boundary</span> conditions on magnetocapacitance effect in a ring-type magnetoelectric structure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Juanjuan</p> <p>2017-12-01</p> <p>By considering the nonlinear magneto-elastic coupling relationships of magnetostrictive materials, an analytical model is proposed. The resonance frequencies can be accurately predicted by this theoretical model, and they are in good agreement with experimental data. Subsequently, the magnetocapacitance effect in a ring-type magnetoelectric (ME) structure with different <span class="hlt">boundary</span> conditions is investigated, and it is found that various mechanical <span class="hlt">boundaries</span>, the frequency, the magnetic field, the geometric size, and the interface bonding significantly affect the capacitance of the ME structure. Further, additional resonance frequencies can be predicted by considering appropriate imperfect interface bonding. <span class="hlt">Finally</span>, the influence of an external force on the capacitance is studied. The result shows that an external force on the <span class="hlt">boundary</span> changes the capacitance, but has only a weak influence on the resonance frequency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=home+AND+care+AND+service&pg=2&id=EJ783152','ERIC'); return false;" href="https://eric.ed.gov/?q=home+AND+care+AND+service&pg=2&id=EJ783152"><span>Renewing Occupational Cultures--Bridging <span class="hlt">Boundaries</span> in Learning Spaces</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>Kalliola, Satu; Nakari, Risto</p> <p>2007-01-01</p> <p>Professional bureaucracies of the Finnish municipal services are challenged by many modernization pressures manifested <span class="hlt">currently</span> in the form of New Public Management. Along with efficiency demands the new emphasis is on the provision of client-oriented services by the means of multi-professional teamwork crossing the traditional sector <span class="hlt">boundaries</span>.…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=dos+AND+commands&pg=5&id=EJ827295','ERIC'); return false;" href="https://eric.ed.gov/?q=dos+AND+commands&pg=5&id=EJ827295"><span>Students' Attitudes on the <span class="hlt">Boundaries</span> of Teachers' Authority</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>Yariv, Eliezer</p> <p>2009-01-01</p> <p>Educators in many countries are concerned about the decline in respect for authority by young people. The <span class="hlt">current</span> study explores how children perceive their teachers' authority, what the "<span class="hlt">boundaries</span>" (limits) to that authority are, and under what conditions they may decide to rebel. Over 200 Israeli elementary and middle school students…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23957281','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23957281"><span>The influence of context <span class="hlt">boundaries</span> on memory for the sequential order of events.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>DuBrow, Sarah; Davachi, Lila</p> <p>2013-11-01</p> <p>Episodic memory allows people to reexperience the past by recovering the sequences of events that characterize those prior experiences. Although experience is continuous, people are able to selectively retrieve and reexperience more discrete episodes from their past, raising the possibility that some elements become tightly related to each other in memory, whereas others do not. The <span class="hlt">current</span> series of experiments was designed to ask how shifts in context during an experience influence how people remember the past. Specifically, we asked how context shifts influence the ability to remember the relative order of past events, a hallmark of episodic memory. We found that memory for the order of events was enhanced within, rather than across, context shifts, or <span class="hlt">boundaries</span> (Experiment 1). Next, we showed that this relative enhancement in order memory was eliminated when across-item associative processing was disrupted (Experiment 2), suggesting that context shifts have a selective effect on sequential binding. <span class="hlt">Finally</span>, we provide evidence that the act of making order memory judgments involves the reactivation of representations that bridged the tested items (Experiment 3). Together, these data suggest that <span class="hlt">boundaries</span> may serve to parse continuous experience into sequences of contextually related events and that this organization facilitates remembering the temporal order of events that share the same context. PsycINFO Database Record (c) 2013 APA, all rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009APS..DFD.GL004W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009APS..DFD.GL004W"><span>Direct Numerical Simulation of dense particle-laden turbulent flows using immersed <span class="hlt">boundaries</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Fan; Desjardins, Olivier</p> <p>2009-11-01</p> <p>Dense particle-laden turbulent flows play an important role in many engineering applications, ranging from pharmaceutical coating and chemical synthesis to fluidized bed reactors. Because of the complexity of the physics involved in these flows, <span class="hlt">current</span> computational models for gas-particle processes, such as drag and heat transfer, rely on empirical correlations and have been shown to lack accuracy. In this work, direct numerical simulations (DNS) of dense particle-laden flows are conducted, using immersed <span class="hlt">boundaries</span> (IB) to resolve the flow around each particle. First, the accuracy of the proposed approach is tested on a range of 2D and 3D flows at various Reynolds numbers, and resolution requirements are discussed. Then, various particle arrangements and number densities are simulated, the impact on particle wake interaction is assessed, and existing drag models are evaluated in the case of fixed particles. In addition, the impact of the particles on turbulence dissipation is investigated. <span class="hlt">Finally</span>, a strategy for handling moving and colliding particles is discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005JSP...118...27V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005JSP...118...27V"><span>Large Deviations in Weakly Interacting <span class="hlt">Boundary</span> Driven Lattice Gases</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>van Wijland, Frédéric; Rácz, Zoltán</p> <p>2005-01-01</p> <p>One-dimensional, <span class="hlt">boundary</span>-driven lattice gases with local interactions are studied in the weakly interacting limit. The density profiles and the correlation functions are calculated to first order in the interaction strength for zero-range and short-range processes differing only in the specifics of the detailed-balance dynamics. Furthermore, the effective free-energy (large-deviation function) and the integrated <span class="hlt">current</span> distribution are also found to this order. From the former, we find that the <span class="hlt">boundary</span> drive generates long-range correlations only for the short-range dynamics while the latter provides support to an additivity principle recently proposed by Bodineau and Derrida.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/3686091','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/3686091"><span>Medical sociology and epidemiology: convergences, divergences and legitimate <span class="hlt">boundaries</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Spruit, I P; Kromhout, D</p> <p>1987-01-01</p> <p>For the purpose of exploring the existence of problem areas that may give rise to the question whether there is a tendency to (illegitimately) trespass across <span class="hlt">boundaries</span> between medical sociology and epidemiology, important convergences and divergences between both disciplines are described. To assemble arguments for the legitimacy of fields of study we trace comparatively the history of both disciplines, definitions of their fields under study and aims of study, as well as characteristic concepts and constructs. <span class="hlt">Current</span> research themes are taken from international journals; divergent interests are briefly described and potential 'trespassing' of <span class="hlt">boundaries</span> is discussed, referring to themes showing convergences of interest.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DFDL21008G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DFDL21008G"><span>Effect of Pulsed Plasma Jets on the Recovering <span class="hlt">Boundary</span> Layer Downstream of a Reflected Shock Interaction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Greene, Benton; Clemens, Noel; Magari, Patrick; Micka, Daniel; Ueckermann, Mattheus</p> <p>2015-11-01</p> <p>Shock-induced turbulent <span class="hlt">boundary</span> layer separation can have many detrimental effects in supersonic inlets including flow distortion and instability, structural fatigue, poor pressure recovery, and unstart. The <span class="hlt">current</span> study investigates the effect of pulsed plasma jets on the recovering <span class="hlt">boundary</span> layer downstream of a reflected shock wave-<span class="hlt">boundary</span> layer interaction. The effects of pitch and skew angle of the jet as well as the heating parameter and discharge time scale are tested using several pulsing frequencies. In addition, the effect of the plasma jets on the undisturbed <span class="hlt">boundary</span> layer at 6 mm and 11 mm downstream of the jets is measured. A pitot-static pressure probe is used to measure the velocity profile of the <span class="hlt">boundary</span> layer 35 mm downstream of the plasma jets, and the degree of <span class="hlt">boundary</span> layer distortion is compared between the different models and run conditions. Additionally, the effect of each actuator configuration on the shape of the mean separated region is investigated using surface oil flow visualization. Previous studies with lower energy showed a weak effect on the downstream <span class="hlt">boundary</span> layer. The <span class="hlt">current</span> investigation will attempt to increase this effect using a higher-energy discharge. Funded by AFRL through and SBIR in collaboration with Creare, LLC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1005459','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1005459"><span>Combined Wave and <span class="hlt">Current</span> Bottom <span class="hlt">Boundary</span> Layers: A Review</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2016-03-01</p> <p>18 3.2 Wave and <span class="hlt">currents</span> at arbitrary angles ....................................................................... 19 3.3 Eddy viscosity ...closure ................................................................................................. 22 3.3.1 Eddy viscosity for stratified fluids...23 3.3.2 Time-dependent eddy viscosities</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70031769','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70031769"><span>Desert bird associations with broad-scale <span class="hlt">boundary</span> length: Applications in avian conservation</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Gutzwiller, K.J.; Barrow, W.C.</p> <p>2008-01-01</p> <p>1. <span class="hlt">Current</span> understanding regarding the effects of <span class="hlt">boundaries</span> on bird communities has originated largely from studies of forest-non-forest <span class="hlt">boundaries</span> in mesic systems. To assess whether broad-scale <span class="hlt">boundary</span> length can affect bird community structure in deserts, and to identify patterns and predictors of species' associations useful in avian conservation, we studied relations between birds and <span class="hlt">boundary</span>-length variables in Chihuahuan Desert landscapes. Operationally, a <span class="hlt">boundary</span> was the border between two adjoining land covers, and broad-scale <span class="hlt">boundary</span> length was the total length of such borders in a large area. 2. Within 2-km radius areas, we measured six <span class="hlt">boundary</span>-length variables. We analysed bird-<span class="hlt">boundary</span> relations for 26 species, tested for assemblage-level patterns in species' associations with <span class="hlt">boundary</span>-length variables, and assessed whether body size, dispersal ability and cowbird-host status were correlates of these associations. 3. The abundances or occurrences of a significant majority of species were associated with <span class="hlt">boundary</span>-length variables, and similar numbers of species were related positively and negatively to <span class="hlt">boundary</span>-length variables. 4. Disproportionately small numbers of species were correlated with total <span class="hlt">boundary</span> length, land-cover <span class="hlt">boundary</span> length and shrubland-grassland <span class="hlt">boundary</span> length (variables responsible for large proportions of <span class="hlt">boundary</span> length). Disproportionately large numbers of species were correlated with roadside <span class="hlt">boundary</span> length and riparian vegetation-grassland <span class="hlt">boundary</span> length (variables responsible for small proportions of <span class="hlt">boundary</span> length). Roadside <span class="hlt">boundary</span> length was associated (positively and negatively) with the most species. 5. Species' associations with <span class="hlt">boundary</span>-length variables were not correlated with body size, dispersal ability or cowbird-host status. 6. Synthesis and applications. For the species we studied, conservationists can use the regressions we report as working models to anticipate influences of <span class="hlt">boundary</span>-length changes</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080010651&hterms=Genders&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DGenders','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080010651&hterms=Genders&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DGenders"><span>Derivation of <span class="hlt">Boundary</span> Manikins: A Principal Component Analysis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Young, Karen; Margerum, Sarah; Barr, Abbe; Ferrer, Mike A.; Rajulu, Sudhakar</p> <p>2008-01-01</p> <p>When designing any human-system interface, it is critical to provide realistic anthropometry to properly represent how a person fits within a given space. This study aimed to identify a minimum number of <span class="hlt">boundary</span> manikins or representative models of subjects anthropometry from a target population, which would realistically represent the population. The <span class="hlt">boundary</span> manikin anthropometry was derived using, Principal Component Analysis (PCA). PCA is a statistical approach to reduce a multi-dimensional dataset using eigenvectors and eigenvalues. The measurements used in the PCA were identified as those measurements critical for suit and cockpit design. The PCA yielded a total of 26 manikins per gender, as well as their anthropometry from the target population. Reduction techniques were implemented to reduce this number further with a <span class="hlt">final</span> result of 20 female and 22 male subjects. The anthropometry of the <span class="hlt">boundary</span> manikins was then be used to create 3D digital models (to be discussed in subsequent papers) intended for use by designers to test components of their space suit design, to verify that the requirements specified in the Human Systems Integration Requirements (HSIR) document are met. The end-goal is to allow for designers to generate suits which accommodate the diverse anthropometry of the user population.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050192103','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050192103"><span>Time-Shifted <span class="hlt">Boundary</span> Conditions Used for Navier-Stokes Aeroelastic Solver</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Srivastava, Rakesh</p> <p>1999-01-01</p> <p>Under the Advanced Subsonic Technology (AST) Program, an aeroelastic analysis code (TURBO-AE) based on Navier-Stokes equations is <span class="hlt">currently</span> under development at NASA Lewis Research Center s Machine Dynamics Branch. For a blade row, aeroelastic instability can occur in any of the possible interblade phase angles (IBPA s). Analyzing small IBPA s is very computationally expensive because a large number of blade passages must be simulated. To reduce the computational cost of these analyses, we used time shifted, or phase-lagged, <span class="hlt">boundary</span> conditions in the TURBO-AE code. These conditions can be used to reduce the computational domain to a single blade passage by requiring the <span class="hlt">boundary</span> conditions across the passage to be lagged depending on the IBPA being analyzed. The time-shifted <span class="hlt">boundary</span> conditions <span class="hlt">currently</span> implemented are based on the direct-store method. This method requires large amounts of data to be stored over a period of the oscillation cycle. On CRAY computers this is not a major problem because solid-state devices can be used for fast input and output to read and write the data onto a disk instead of storing it in core memory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21308329-hawking-radiation-covariant-boundary-conditions-vacuum-states','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21308329-hawking-radiation-covariant-boundary-conditions-vacuum-states"><span>Hawking radiation, covariant <span class="hlt">boundary</span> conditions, and vacuum states</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>Banerjee, Rabin; Kulkarni, Shailesh</p> <p>2009-04-15</p> <p>The basic characteristics of the covariant chiral <span class="hlt">current</span> <J{sub {mu}}> and the covariant chiral energy-momentum tensor <T{sub {mu}}{sub {nu}}> are obtained from a chiral effective action. These results are used to justify the covariant <span class="hlt">boundary</span> condition used in recent approaches of computing the Hawking flux from chiral gauge and gravitational anomalies. We also discuss a connection of our results with the conventional calculation of nonchiral <span class="hlt">currents</span> and stress tensors in different (Unruh, Hartle-Hawking and Boulware) states.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2995840','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2995840"><span>Robust Surface Reconstruction via Laplace-Beltrami Eigen-Projection and <span class="hlt">Boundary</span> Deformation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Shi, Yonggang; Lai, Rongjie; Morra, Jonathan H.; Dinov, Ivo; Thompson, Paul M.; Toga, Arthur W.</p> <p>2010-01-01</p> <p>In medical shape analysis, a critical problem is reconstructing a smooth surface of correct topology from a binary mask that typically has spurious features due to segmentation artifacts. The challenge is the robust removal of these outliers without affecting the accuracy of other parts of the <span class="hlt">boundary</span>. In this paper, we propose a novel approach for this problem based on the Laplace-Beltrami (LB) eigen-projection and properly designed <span class="hlt">boundary</span> deformations. Using the metric distortion during the LB eigen-projection, our method automatically detects the location of outliers and feeds this information to a well-composed and topology-preserving deformation. By iterating between these two steps of outlier detection and <span class="hlt">boundary</span> deformation, we can robustly filter out the outliers without moving the smooth part of the <span class="hlt">boundary</span>. The <span class="hlt">final</span> surface is the eigen-projection of the filtered mask <span class="hlt">boundary</span> that has the correct topology, desired accuracy and smoothness. In our experiments, we illustrate the robustness of our method on different input masks of the same structure, and compare with the popular SPHARM tool and the topology preserving level set method to show that our method can reconstruct accurate surface representations without introducing artificial oscillations. We also successfully validate our method on a large data set of more than 900 hippocampal masks and demonstrate that the reconstructed surfaces retain volume information accurately. PMID:20624704</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850016266&hterms=Plasma+Ring&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DPlasma%2BRing','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850016266&hterms=Plasma+Ring&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DPlasma%2BRing"><span>Ring <span class="hlt">current</span> dynamics and plasma sheet sources. [magnetic storms</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lyons, L. R.</p> <p>1984-01-01</p> <p>The source of the energized plasma that forms in geomagnetic storm ring <span class="hlt">currents</span>, and ring <span class="hlt">current</span> decay are discussed. The dominant loss processes for ring <span class="hlt">current</span> ions are identified as charge exchange and resonant interactions with ion-cyclotron waves. Ring <span class="hlt">current</span> ions are not dominated by protons. At L4 and energies below a few tens of keV, O+ is the most abundant ion, He+ is second, and protons are third. The plasma sheet contributes directly or indirectly to the ring <span class="hlt">current</span> particle population. An important source of plasma sheet ions is earthward streaming ions on the outer <span class="hlt">boundary</span> of the plasma sheet. Ion interactions with the <span class="hlt">current</span> across the geomagnetic tail can account for the formation of this <span class="hlt">boundary</span> layer. Electron interactions with the <span class="hlt">current</span> sheet are possibly an important source of plasma sheet electrons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22227923-numerical-magnetohydrodynamic-simulations-expanding-flux-ropes-influence-boundary-driving','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22227923-numerical-magnetohydrodynamic-simulations-expanding-flux-ropes-influence-boundary-driving"><span>Numerical magnetohydrodynamic simulations of expanding flux ropes: Influence of <span class="hlt">boundary</span> driving</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>Tacke, Thomas; Dreher, Jürgen; Sydora, Richard D.</p> <p>2013-07-15</p> <p>The expansion dynamics of a magnetized, <span class="hlt">current</span>-carrying plasma arch is studied by means of time-dependent ideal MHD simulations. Initial conditions model the setup used in recent laboratory experiments that in turn simulate coronal loops [J. Tenfelde et al., Phys. Plasmas 19, 072513 (2012); E. V. Stenson and P. M. Bellan, Plasma Phys. Controlled Fusion 54, 124017 (2012)]. <span class="hlt">Boundary</span> conditions of the electric field at the “lower” <span class="hlt">boundary</span>, intersected by the arch, are chosen such that poloidal magnetic flux is injected into the domain, either localized at the arch footpoints themselves or halfway between them. These conditions are motivated by themore » tangential electric field expected to exist in the laboratory experiments due to the external circuit that drives the plasma <span class="hlt">current</span>. The <span class="hlt">boundary</span> driving is found to systematically enhance the expansion velocity of the plasma arch. While perturbations at the arch footpoints also deform its legs and create characteristic elongated segments, a perturbation between the footpoints tends to push the entire structure upwards, retaining an ellipsoidal shape.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980206205','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980206205"><span>Minnowbrook II 1997 Workshop on <span class="hlt">Boundary</span> Layer Transition in Turbomachines</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>LaGraff John E. (Editor); Ashpis, David E. (Editor)</p> <p>1998-01-01</p> <p>The volume contains materials presented at the Minnowbrook II - 1997 Workshop on <span class="hlt">Boundary</span> Layer Transition in Turbomachines, held at Syracuse University Minnowbrook Conference Center, New York, on September 7-10, 1997. The workshop followed the informal format at the 1993 Minnowbrook I workshop, focusing on improving the understanding of late stage (<span class="hlt">final</span> breakdown) <span class="hlt">boundary</span> layer transition, with the engineering application of improving design codes for turbomachinery in mind. Among the physical mechanisms discussed were hydrodynamic instabilities, laminar to turbulent transition, bypass transition, turbulent spots, wake interaction with <span class="hlt">boundary</span> layers, calmed regions, and separation, all in the context of flow in turbomachinery, particularly in compressors and high and low pressure turbines. Results from experiments, DNS, computation, modeling and theoretical analysis were presented. Abstracts and copies of viewgraphs, a specifically commissioned summation paper prepared after the workshop, and a transcript of the extensive working group reports and discussions are included in this volume. They provide recommendations for future research and clearly highlight the need for continued vigorous research in the technologically important area of transition in turbomachines.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA496329','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA496329"><span><span class="hlt">Boundary</span> Avoidance Tracking: Consequences (and Uses) of Imposed <span class="hlt">Boundaries</span> on Pilot-Aircraft Performance</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2009-03-01</p> <p><span class="hlt">BOUNDARY</span> AVOIDANCE TRACKING: CONSEQUENCES (AND USES) OF IMPOSED <span class="hlt">BOUNDARIES</span> ON PILOT-AIRCRAFT...States Government. AFIT/GAE/ENY/09-M03 <span class="hlt">BOUNDARY</span> AVOIDANCE TRACKING: CONSEQUENCES (AND USES) OF IMPOSED <span class="hlt">BOUNDARIES</span> ON PILOT-AIRCRAFT PERFORMANCE...Case 2 (Gray, 2005) ....................................... 20 Figure 8. Effect of BAT Parameters on Tracking Success (Gray, 2005</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22475920-electrical-characterization-grain-boundaries-czts-thin-films-using-conductive-atomic-force-microscopy-techniques','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22475920-electrical-characterization-grain-boundaries-czts-thin-films-using-conductive-atomic-force-microscopy-techniques"><span>Electrical characterization of grain <span class="hlt">boundaries</span> of CZTS thin films using conductive atomic force microscopy techniques</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>Muhunthan, N.; Singh, Om Pal; Toutam, Vijaykumar, E-mail: toutamvk@nplindia.org</p> <p>2015-10-15</p> <p>Graphical abstract: Experimental setup for conducting AFM (C-AFM). - Highlights: • Cu{sub 2}ZnSnS{sub 4} (CZTS) thin film was grown by reactive co-sputtering. • The electronic properties were probed using conducting atomic force microscope, scanning Kelvin probe microscopy and scanning capacitance microscopy. • C-AFM <span class="hlt">current</span> flow mainly through grain <span class="hlt">boundaries</span> rather than grain interiors. • SKPM indicated higher potential along the GBs compared to grain interiors. • The SCM explains that charge separation takes place at the interface of grain and grain <span class="hlt">boundary</span>. - Abstract: Electrical characterization of grain <span class="hlt">boundaries</span> (GB) of Cu-deficient CZTS (Copper Zinc Tin Sulfide) thin films wasmore » done using atomic force microscopic (AFM) techniques like Conductive atomic force microscopy (CAFM), Kelvin probe force microscopy (KPFM) and scanning capacitance microscopy (SCM). Absorbance spectroscopy was done for optical band gap calculations and Raman, XRD and EDS for structural and compositional characterization. Hall measurements were done for estimation of carrier mobility. CAFM and KPFM measurements showed that the <span class="hlt">currents</span> flow mainly through grain <span class="hlt">boundaries</span> (GB) rather than grain interiors. SCM results showed that charge separation mainly occurs at the interface of grain and grain <span class="hlt">boundaries</span> and not all along the grain <span class="hlt">boundaries</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25481972','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25481972"><span>[<span class="hlt">Boundaries</span> and integrity in the "Social Contract for Spanish Science", 1907-1939].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gómez, Amparo</p> <p>2014-01-01</p> <p>This article analyzes the relationship between science and politics in Spain in the early 20th century from the perspective of the Social Contract for Science. The article shows that a genuine social contract for science was instituted in Spain during this period, although some <span class="hlt">boundary</span> and integrity problems emerged. These problems are analyzed, showing that the <span class="hlt">boundary</span> problems were a product of the conservative viewpoint on the relationship between science and politics, while the integrity problems involved the activation of networks of influence in the awarding of scholarships to study abroad. <span class="hlt">Finally</span>, the analysis reveals that these problems did not invalidate the Spanish social contract for science.</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('http://hdl.handle.net/2060/19940031468','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940031468"><span>The velocity field created by a shallow bump in a <span class="hlt">boundary</span> layer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gaster, Michael; Grosch, Chester E.; Jackson, Thomas L.</p> <p>1994-01-01</p> <p>We report the results of measurements of the disturbance velocity field generated in a <span class="hlt">boundary</span> layer by a shallow three-dimensional bump oscillating at a very low frequency on the surface of a flat plate. Profiles of the mean velocity, the disturbance velocity at the fundamental frequency and at the first harmonic are presented. These profiles were measured both upstream and downstream of the oscillating bump. Measurements of the disturbance velocity were also made at various spanwise and downstream locations at a fixed distance from the <span class="hlt">boundary</span> of one displacement thickness. <span class="hlt">Finally</span>, the spanwise spectrum of the disturbances at three locations downstream of the bump are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1358265','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1358265"><span>SILICON CARBIDE GRAIN <span class="hlt">BOUNDARY</span> DISTRIBUTIONS, IRRADIATION CONDITIONS, AND SILVER RETENTION IN IRRADIATED AGR-1 TRISO FUEL PARTICLES</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>Lillo, T. M.; Rooyen, I. J.; Aguiar, J. A.</p> <p></p> <p>Precession electron diffraction in the transmission electron microscope was used to map grain orientation and ultimately determine grain <span class="hlt">boundary</span> misorientation angle distributions, relative fractions of grain <span class="hlt">boundary</span> types (random high angle, low angle or coincident site lattice (CSL)-related <span class="hlt">boundaries</span>) and the distributions of CSL-related grain <span class="hlt">boundaries</span> in the SiC layer of irradiated TRISO-coated fuel particles. Two particles from the AGR-1 experiment exhibiting high Ag-110m retention (>80%) were compared to a particle exhibiting low Ag-110m retention (<19%). Irradiated particles with high Ag-110m retention exhibited a lower fraction of random, high angle grain <span class="hlt">boundaries</span> compared to the low Ag-110m retention particle. Anmore » inverse relationship between the random, high angle grain <span class="hlt">boundary</span> fraction and Ag-110m retention is found and is consistent with grain <span class="hlt">boundary</span> percolation theory. Also, comparison of the grain <span class="hlt">boundary</span> distributions with previously reported unirradiated grain <span class="hlt">boundary</span> distributions, based on SEM-based EBSD for similarly fabricated particles, showed only small differences, i.e. a greater low angle grain <span class="hlt">boundary</span> fraction in unirradiated SiC. It was, thus, concluded that SiC layers with grain <span class="hlt">boundary</span> distributions susceptible to Ag-110m release were present prior to irradiation. <span class="hlt">Finally</span>, irradiation parameters were found to have little effect on the association of fission product precipitates with specific grain <span class="hlt">boundary</span> types.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950011627','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950011627"><span>A spectrally accurate <span class="hlt">boundary</span>-layer code for infinite swept wings</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pruett, C. David</p> <p>1994-01-01</p> <p>This report documents the development, validation, and application of a spectrally accurate <span class="hlt">boundary</span>-layer code, WINGBL2, which has been designed specifically for use in stability analyses of swept-wing configurations. <span class="hlt">Currently</span>, we consider only the quasi-three-dimensional case of an infinitely long wing of constant cross section. The effects of streamwise curvature, streamwise pressure gradient, and wall suction and/or blowing are taken into account in the governing equations and <span class="hlt">boundary</span> conditions. The <span class="hlt">boundary</span>-layer equations are formulated both for the attachment-line flow and for the evolving <span class="hlt">boundary</span> layer. The <span class="hlt">boundary</span>-layer equations are solved by marching in the direction perpendicular to the leading edge, for which high-order (up to fifth) backward differencing techniques are used. In the wall-normal direction, a spectral collocation method, based upon Chebyshev polynomial approximations, is exploited. The accuracy, efficiency, and user-friendliness of WINGBL2 make it well suited for applications to linear stability theory, parabolized stability equation methodology, direct numerical simulation, and large-eddy simulation. The method is validated against existing schemes for three test cases, including incompressible swept Hiemenz flow and Mach 2.4 flow over an airfoil swept at 70 deg to the free stream.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70190320','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70190320"><span>Directional bottom roughness associated with waves, <span class="hlt">currents</span>, and ripples</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Sherwood, Christopher R.; Rosati, Julie D.; Wang, Ping; Roberts, Tiffany M.</p> <p>2011-01-01</p> <p>Roughness lengths are used in wave-<span class="hlt">current</span> bottom <span class="hlt">boundary</span> layer models to parameterize drag associated with grain roughness, the effect of saltating grains during sediment transport, and small-scale bottom topography (ripples and biogenic features). We made field measurements of flow parameters and recorded sonar images of ripples at the <span class="hlt">boundary</span> of a sorted-bedform at ~12-m depth on the inner shelf for a range of wave and <span class="hlt">current</span> conditions over two months. We compared estimates of apparent bottom roughness inferred from the flow measurements with bottom roughness calculated using ripple geometry and the Madsen (1994) one-dimensional (vertical) wave-<span class="hlt">current</span> bottom <span class="hlt">boundary</span> layer model. One result of these comparisons was that the model over predicted roughness of flow from the dormant large ripples when waves were small. We developed a correction to the ripple-roughness model that incorporates an apparent ripple wavelength related to the combined wave-<span class="hlt">current</span> flow direction. This correction provides a slight improvement for low-wave conditions, but does not address several other differences between observations and the modeled roughness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhyB..459..105C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhyB..459..105C"><span>Modulus spectroscopy of grain-grain <span class="hlt">boundary</span> binary system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cheng, Peng-Fei; Song, Jiang; Li, Sheng-Tao; Wang, Hui</p> <p>2015-02-01</p> <p>Understanding various polarization mechanisms in complex dielectric systems and specifying their physical origins are key issues in dielectric physics. In this paper, four different methods for representing dielectric properties were analyzed and compared. Depending on the details of the system under study, i.e., uniform or non-uniform, it was suggested that different representing approaches should be used to obtain more valuable information. Especially, for the grain-grain <span class="hlt">boundary</span> binary non-uniform system, its dielectric response was analyzed in detail in terms of modulus spectroscopy (MS). Furthermore, it was found that through MS, the dielectric responses between uniform and non-uniform systems, grain and grain <span class="hlt">boundary</span>, Maxwell-Wagner polarization and intrinsic polarization can be distinguished. <span class="hlt">Finally</span>, with the proposed model, the dielectric properties of CaCu3Ti4O12 (CCTO) ceramics were studied. The colossal dielectric constant of CCTO at low frequency was attributed to the pseudo relaxation process of grain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhDT.......283L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhDT.......283L"><span>Analytic Approximations to the Free <span class="hlt">Boundary</span> and Multi-dimensional Problems in Financial Derivatives Pricing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lau, Chun Sing</p> <p></p> <p>This thesis studies two types of problems in financial derivatives pricing. The first type is the free <span class="hlt">boundary</span> problem, which can be formulated as a partial differential equation (PDE) subject to a set of free <span class="hlt">boundary</span> condition. Although the functional form of the free <span class="hlt">boundary</span> condition is given explicitly, the location of the free <span class="hlt">boundary</span> is unknown and can only be determined implicitly by imposing continuity conditions on the solution. Two specific problems are studied in details, namely the valuation of fixed-rate mortgages and CEV American options. The second type is the multi-dimensional problem, which involves multiple correlated stochastic variables and their governing PDE. One typical problem we focus on is the valuation of basket-spread options, whose underlying asset prices are driven by correlated geometric Brownian motions (GBMs). Analytic approximate solutions are derived for each of these three problems. For each of the two free <span class="hlt">boundary</span> problems, we propose a parametric moving <span class="hlt">boundary</span> to approximate the unknown free <span class="hlt">boundary</span>, so that the original problem transforms into a moving <span class="hlt">boundary</span> problem which can be solved analytically. The governing parameter of the moving <span class="hlt">boundary</span> is determined by imposing the first derivative continuity condition on the solution. The analytic form of the solution allows the price and the hedging parameters to be computed very efficiently. When compared against the benchmark finite-difference method, the computational time is significantly reduced without compromising the accuracy. The multi-stage scheme further allows the approximate results to systematically converge to the benchmark results as one recasts the moving <span class="hlt">boundary</span> into a piecewise smooth continuous function. For the multi-dimensional problem, we generalize the Kirk (1995) approximate two-asset spread option formula to the case of multi-asset basket-spread option. Since the <span class="hlt">final</span> formula is in closed form, all the hedging parameters can also be derived in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1988CMaPh.117..215M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1988CMaPh.117..215M"><span>Diamagnetic <span class="hlt">currents</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Macris, N.; Martin, Ph. A.; Pulé, J. V.</p> <p>1988-06-01</p> <p>We study the diamagnetic surface <span class="hlt">currents</span> of particles in thermal equilibrium submitted to a constant magnetic field. The <span class="hlt">current</span> density of independent electrons with Boltzmann (respectively Fermi) statistics has a gaussian (respectively exponential) bound for its fall off into the bulk. For a system of interacting particles at low activity with Boltzmann statistics, the <span class="hlt">current</span> density is localized near to the <span class="hlt">boundary</span> and integrable when the two-body potential decays as |x|-α, α >4, α>4, in three dimensions. In all cases, the integral of the <span class="hlt">current</span> density is independent of the nature of the confining wall and correctly related to the bulk magnetisation. The results hold for hard and soft walls and all field strength. The analysis relies on the Feynman-Kac-Ito representation of the Gibbs state and on specific properties of the Brownian bridge process.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1426868-boundary-holographic-witten-diagrams','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1426868-boundary-holographic-witten-diagrams"><span><span class="hlt">Boundary</span> holographic Witten diagrams</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Karch, Andreas; Sato, Yoshiki</p> <p>2017-09-25</p> <p>In this paper we discuss geodesic Witten diagrams in generic holographic conformal field theories with <span class="hlt">boundary</span> or defect. <span class="hlt">Boundary</span> CFTs allow two different de-compositions of two-point functions into conformal blocks: <span class="hlt">boundary</span> channel and ambient channel. Building on earlier work, we derive a holographic dual of the <span class="hlt">boundary</span> channel decomposition in terms of bulk-to-bulk propagators on lower dimensional AdS slices. In the situation in which we can treat the <span class="hlt">boundary</span> or defect as a perturbation around pure AdS spacetime, we obtain the leading corrections to the two-point function both in <span class="hlt">boundary</span> and ambient channel in terms of geodesic Witten diagrams whichmore » exactly reproduce the decomposition into corresponding conformal blocks on the field theory side.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900008097','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900008097"><span>Predicted and measured <span class="hlt">boundary</span> layer refraction for advanced turboprop propeller noise</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dittmar, James H.; Krejsa, Eugene A.</p> <p>1990-01-01</p> <p><span class="hlt">Currently</span>, <span class="hlt">boundary</span> layer refraction presents a limitation to the measurement of forward arc propeller noise measured on an acoustic plate in the NASA Lewis 8- by 6-Foot Supersonic Wind Tunnel. The use of a validated <span class="hlt">boundary</span> layer refraction model to adjust the data could remove this limitation. An existing <span class="hlt">boundary</span> layer refraction model is used to predict the refraction for cases where <span class="hlt">boundary</span> layer refraction was measured. In general, the model exhibits the same qualitative behavior as the measured refraction. However, the prediction method does not show quantitative agreement with the data. In general, it overpredicts the amount of refraction for the far forward angles at axial Mach number of 0.85 and 0.80 and underpredicts the refraction at axial Mach numbers of 0.75 and 0.70. A more complete propeller source description is suggested as a way to improve the prediction method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/5648802-heat-transfer-turbulent-boundary-layer-short-strip-surface-roughness','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/5648802-heat-transfer-turbulent-boundary-layer-short-strip-surface-roughness"><span>Heat transfer in the turbulent <span class="hlt">boundary</span> layer with a short strip of surface roughness</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>Taylor, R.P.; Chakroun, W.M.</p> <p>1992-01-01</p> <p>The effects of a short strip of surface roughness on heat transfer and fluid flow in the turbulent <span class="hlt">boundary</span> layer are investigated experimentally. This is done by measuring Stanton number and skin friction distributions and mean velocity, turbulence intensity, and mean temperature profiles in a turbulent <span class="hlt">boundary</span> layer where the first 0.7 m length is smooth, the next 0.2 m is roughened with 1.27 mm hemispheres spaced 2 base diameters apart and the <span class="hlt">final</span> 1.5 m is smooth. These results are compared with previously published data from experiments wiht a rough leading portion and smooth <span class="hlt">final</span> portion and from experimentsmore » on an all-smooth surface. The influence of the roughness is large in the neighborhood of the rough strip, but the Stanton number and skin friction distributions are seen to quickly recover smooth-wall behavior downstream of the rough strip. 19 refs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1014367','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1014367"><span>Multiscale Study of <span class="hlt">Currents</span> Affected by Topography</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-09-30</p> <p>1 DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Multiscale Study of <span class="hlt">Currents</span> Affected by Topography ... topography on the ocean general circulation is challenging because of the multiscale nature of the flow interactions. Small-scale details of the... topography , and the waves, drag, and turbulence generated at the <span class="hlt">boundary</span>, from meter scale to mesoscale, interact in the <span class="hlt">boundary</span> layers to influence the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25119049','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25119049"><span>Gradual unlocking of plate <span class="hlt">boundary</span> controlled initiation of the 2014 Iquique earthquake.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Schurr, Bernd; Asch, Günter; Hainzl, Sebastian; Bedford, Jonathan; Hoechner, Andreas; Palo, Mauro; Wang, Rongjiang; Moreno, Marcos; Bartsch, Mitja; Zhang, Yong; Oncken, Onno; Tilmann, Frederik; Dahm, Torsten; Victor, Pia; Barrientos, Sergio; Vilotte, Jean-Pierre</p> <p>2014-08-21</p> <p>On 1 April 2014, Northern Chile was struck by a magnitude 8.1 earthquake following a protracted series of foreshocks. The Integrated Plate <span class="hlt">Boundary</span> Observatory Chile monitored the entire sequence of events, providing unprecedented resolution of the build-up to the main event and its rupture evolution. Here we show that the Iquique earthquake broke a central fraction of the so-called northern Chile seismic gap, the last major segment of the South American plate <span class="hlt">boundary</span> that had not ruptured in the past century. Since July 2013 three seismic clusters, each lasting a few weeks, hit this part of the plate <span class="hlt">boundary</span> with earthquakes of increasing peak magnitudes. Starting with the second cluster, geodetic observations show surface displacements that can be associated with slip on the plate interface. These seismic clusters and their slip transients occupied a part of the plate interface that was transitional between a fully locked and a creeping portion. Leading up to this earthquake, the b value of the foreshocks gradually decreased during the years before the earthquake, reversing its trend a few days before the Iquique earthquake. The mainshock <span class="hlt">finally</span> nucleated at the northern end of the foreshock area, which skirted a locked patch, and ruptured mainly downdip towards higher locking. Peak slip was attained immediately downdip of the foreshock region and at the margin of the locked patch. We conclude that gradual weakening of the central part of the seismic gap accentuated by the foreshock activity in a zone of intermediate seismic coupling was instrumental in causing <span class="hlt">final</span> failure, distinguishing the Iquique earthquake from most great earthquakes. <span class="hlt">Finally</span>, only one-third of the gap was broken and the remaining locked segments now pose a significant, increased seismic hazard with the potential to host an earthquake with a magnitude of >8.5.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1813245H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1813245H"><span><span class="hlt">Boundary</span> Layer Flow Over a Moving Wavy Surface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hendin, Gali; Toledo, Yaron</p> <p>2016-04-01</p> <p><span class="hlt">Boundary</span> Layer Flow Over a Moving Wavy Surface Gali Hendin(1), Yaron Toledo(1) January 13, 2016 (1)School of Mechanical Engineering, Tel-Aviv University, Israel Understanding the <span class="hlt">boundary</span> layer flow over surface gravity waves is of great importance as various atmosphere-ocean processes are essentially coupled through these waves. Nevertheless, there are still significant gaps in our understanding of this complex flow behaviour. The present work investigates the fundamentals of the <span class="hlt">boundary</span> layer air flow over progressive, small-amplitude waves. It aims to extend the well-known Blasius solution for a <span class="hlt">boundary</span> layer over a flat plate to one over a moving wavy surface. The <span class="hlt">current</span> analysis pro- claims the importance of the small curvature and the time-dependency as second order effects, with a meaningful impact on the similarity pattern in the first order. The air flow over the ocean surface is modelled using an outer, inviscid half-infinite flow, overlaying the viscous <span class="hlt">boundary</span> layer above the wavy surface. The assumption of a uniform flow in the outer layer, used in former studies, is now replaced with a precise analytical solution of the potential flow over a moving wavy surface with a known celerity, wavelength and amplitude. This results in a conceptual change from former models as it shows that the pressure variations within the <span class="hlt">boundary</span> layer cannot be neglected. In the <span class="hlt">boundary</span> layer, time-dependent Navier-Stokes equations are formulated in a curvilinear, orthogonal coordinate system. The formulation is done in an elaborate way that presents additional, formerly neglected first-order effects, resulting from the time-varying coordinate system. The suggested time-dependent curvilinear orthogonal coordinate system introduces a platform that can also support the formulation of turbulent problems for any surface shape. In order to produce a self-similar Blasius-type solution, a small wave-steepness is assumed and a perturbation method is applied. Consequently, a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3667468','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3667468"><span>Atom Probe Tomography Studies on the Cu(In,Ga)Se2 Grain <span class="hlt">Boundaries</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>Cojocaru-Mirédin, Oana; Schwarz, Torsten; Choi, Pyuck-Pa; Herbig, Michael; Wuerz, Roland; Raabe, Dierk</p> <p>2013-01-01</p> <p>Compared with the existent techniques, atom probe tomography is a unique technique able to chemically characterize the internal interfaces at the nanoscale and in three dimensions. Indeed, APT possesses high sensitivity (in the order of ppm) and high spatial resolution (sub nm). Considerable efforts were done here to prepare an APT tip which contains the desired grain <span class="hlt">boundary</span> with a known structure. Indeed, site-specific sample preparation using combined focused-ion-beam, electron backscatter diffraction, and transmission electron microscopy is presented in this work. This method allows selected grain <span class="hlt">boundaries</span> with a known structure and location in Cu(In,Ga)Se2 thin-films to be studied by atom probe tomography. <span class="hlt">Finally</span>, we discuss the advantages and drawbacks of using the atom probe tomography technique to study the grain <span class="hlt">boundaries</span> in Cu(In,Ga)Se2 thin-film solar cells. PMID:23629452</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003EAEJA.....9681C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003EAEJA.....9681C"><span>Recalibration of the Palaeocene-Eocene <span class="hlt">boundary</span> (P-E) using high precision U-Pb and Ar-Ar isotopic dating</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chambers, L.; Pringle, M.; Fitton, G.; Larsen, L. M.; Pedersen, A. K.; Parrish, R.</p> <p>2003-04-01</p> <p>In the <span class="hlt">current</span> time scales (Cande and Kent, 95; Berggren et al, 95) the P-E <span class="hlt">Boundary</span> is positioned at 55 Ma based primarily on the age of the -17 ash layer in Denmark. In the absence of a global stratigraphic section and point the <span class="hlt">boundary</span> is an interval of 1 m.y. from 55.5 to 54.5 Ma that includes all of the different means of calibrating the <span class="hlt">boundary</span> tie point, including the NP9/NP10 calcareous nannofossil zonal <span class="hlt">boundary</span>, the planktonic foraminiferal P5/P6a zonal <span class="hlt">boundary</span>, preliminary ages for the -17 and +19 ash layers (unpub.), the base of the London Clay Formation, and the δ13C spike. Here we present new Ar-Ar ages for the -17 and +19 ash layers in Denmark and combine this study with a calibration of the Ar-Ar with the U-Pb method. As Ar-Ar ages are relative to the known age of a standard or monitor, U-Pb ages on zircons from the same rocks from the British Tertiary Igneous Province provide an absolute age calibration for all of our Ar-Ar ages (including the monitors). An additional complication arises because the time scale is <span class="hlt">currently</span> being revised (J. Ogg, Pers. Comm.). In the new time scale the P-E <span class="hlt">boundary</span> will stay at 55 Ma and the K-T <span class="hlt">boundary</span> will move by 0.5 m.y. to 65.5 Ma. Our results have a direct impact on the positioning of the P-E <span class="hlt">Boundary</span> relative to the K-T <span class="hlt">boundary</span> as definitive K-T tektite is used as one of our Ar-Ar standards. Ar-Ar ages and U-Pb ages for the same sample from the BTIP are indistinguishable when the ages used for the Ar-Ar monitor minerals are those recommended in Renne et al (98). This means that the K-T tektite is 65.78 ± 0.03 Ma, the -17 ash is 54.52 ± 0.05Ma, and the +19 ash is 54.04 ± 0.14 Ma. If the P-E <span class="hlt">boundary</span> is taken to be between the -17 and +19 ash layers, as in DSDP Hole 550 (the ashes bracket the planktonic foraminiferal P5/P6a zonal <span class="hlt">boundary</span>) then the <span class="hlt">current</span> position at 55 Ma is too old. We therefore suggest that if the K-T <span class="hlt">boundary</span> moves to 65.5 Ma, then the P-E <span class="hlt">boundary</span> should not stay at 55 Ma, but</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUSM.H51B..14L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUSM.H51B..14L"><span>Changes in the lower <span class="hlt">boundary</span> condition of water fluxes in the NOAH land surface scheme</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lohmann, D.; Peters-Lidard, C. D.</p> <p>2002-05-01</p> <p>One problem with <span class="hlt">current</span> land surface schemes (LSS) used in weather prediction and climate models is their inabilty to reproduce streamflow in large river basins. This can be attributed to the weak representation of their upper (infiltration) and lower (baseflow) <span class="hlt">boundary</span> conditions in their water balance / transport equations. Operational (traditional) hydrological models, which operate on the same spatial scale as a LSS, on the other hand, are able to reproduce streamflow time series. Their infiltration and baseflow equations are often empirically based and therefore have been neglected by the LSS community. It must be argued that we need to include a better representation of long time scales (as represented by groundwater and baseflow) into the <span class="hlt">current</span> LSS to make valuable predictions of streamflow and water resources. This talk concentrates on the lower <span class="hlt">boundary</span> condition of water fluxes within LSS. It reviews briefly previous attempts to incorporate groundwater and more realistic lower <span class="hlt">boundary</span> conditions into LSS and summarizes the effect on the runoff (baseflow) production time scales as compared to <span class="hlt">currently</span> used lower <span class="hlt">boundary</span> conditions in LSS. The NOAH - LSM in the LDAS and DMIP setting is used to introduce a simplified groundwater model, based on the linearized Boussinesq equation, and the TOPMODEL. The NOAH - LSM will be coupled to a linear routing model to investigate the effects of the new lower <span class="hlt">boundary</span> condition on the water balance (in particular, streamflow) in small to medium sized catchments in the LDAS / DMIP domain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997CSR....17.1271L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997CSR....17.1271L"><span>Acoustic measurements of the spatial and temporal structure of the near-bottom <span class="hlt">boundary</span> layer in the 1990-1991 STRESS experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lynch, James F.; Irish, James D.; Gross, Thomas F.; Wiberg, Patricia L.; Newhall, Arthur E.; Traykovski, Peter A.; Warren, Joseph D.</p> <p>1997-08-01</p> <p>As part of the 1990-1991 Sediment TRansport Events on Shelves and Slopes (STRESS) experiment, a 5 MHz Acoustic BackScatter System (ABSS) was deployed in 90 m of water to measure vertical profiles of near-bottom suspended sediment concentration. By looking at the vertical profile of concentration from 0 to 50 cm above bottom (cmab) with 1 cm vertical resolution, the ABSS was able to examine the detailed structure of the bottom <span class="hlt">boundary</span> layer created by combined wave and <span class="hlt">current</span> stresses. The acoustic profiles clearly showed the wave-<span class="hlt">current</span> <span class="hlt">boundary</span> layer, which extends to (order) 10 cmab. The profiles also showed evidence of an "intermediate" <span class="hlt">boundary</span> layer, also influenced by combined wave and <span class="hlt">current</span> stresses, just above the wave-<span class="hlt">current</span> <span class="hlt">boundary</span> layer. This paper examines the <span class="hlt">boundary</span>-layer structure by comparing acoustic data obtained by the authors to a 1-D eddy viscosity model formulation. Specifically, these data are compared to a simple extension of the Grant-Glenn-Madsen model formulation. Also of interest is the appearance of apparently 3-D "advective plume" structures in these data. This is an interesting feature in a site which was initially chosen to be a good example of (temporally averaged) 1-D bottom <span class="hlt">boundary</span>-layer dynamics. Computer modeling and sector-scanning sonar images are presented to justify the plausibility of observing 3-D structure at the STRESS site. 1997 Elsevier Science Ltd</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ESuD....2..481M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ESuD....2..481M"><span>Tracing the <span class="hlt">boundaries</span> of Cenozoic volcanic edifices from Sardinia (Italy): a geomorphometric contribution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Melis, M. T.; Mundula, F.; DessÌ, F.; Cioni, R.; Funedda, A.</p> <p>2014-09-01</p> <p>Unequivocal delimitation of landforms is an important issue for different purposes, from science-driven morphometric analysis to legal issues related to land conservation. This study is aimed at giving a new contribution to the morphometric approach for the delineation of the <span class="hlt">boundaries</span> of volcanic edifices, applied to 13 monogenetic volcanoes (scoria cones) related to the Pliocene-Pleistocene volcanic cycle in Sardinia (Italy). External <span class="hlt">boundary</span> delimitation of the edifices is discussed based on an integrated methodology using automatic elaboration of digital elevation models together with geomorphological and geological observations. Different elaborations of surface slope and profile curvature have been proposed and discussed; among them, two algorithms based on simple mathematical functions combining slope and profile curvature well fit the requirements of this study. One of theses algorithms is a modification of a function introduced by Grosse et al. (2011), which better performs for recognizing and tracing the <span class="hlt">boundary</span> between the volcanic scoria cone and its basement. Although the geological constraints still drive the <span class="hlt">final</span> decision, the proposed method improves the existing tools for a semi-automatic tracing of the <span class="hlt">boundaries</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ESuDD...2..357M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ESuDD...2..357M"><span>Tracing the <span class="hlt">boundaries</span> of Cenozoic volcanic edifices from Sardinia (Italy): a geomorphometric contribution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Melis, M. T.; Mundula, F.; Dessì, F.; Cioni, R.; Funedda, A.</p> <p>2014-05-01</p> <p>Unequivocal delimitation of landforms is an important issue for different purposes, from science-driven morphometric analysis to legal issues related to land conservation. This study is aimed at giving a new contribution to the morphometric approach for the delineation of the <span class="hlt">boundaries</span> of volcanic edifices, applied to 13 monogenetic volcanoes (scoria cones) related to the Pliocene-Pleistocene volcanic cycle in Sardinia (Italy). External <span class="hlt">boundary</span> delimitation of the edifices is discussed based on an integrated methodology using automatic elaboration of digital elevation models together with geomorphological and geological observations. Different elaborations of surface slope and profile curvature have been proposed and discussed; among them, two algorithms based on simple mathematical functions combining slope and profile curvature well fit the requirements of this study. One of theses algorithms is a modification of a function already discussed by Grosse et al. (2011), which better perform for recognizing and tracing the <span class="hlt">boundary</span> between the volcanic scoria cone and its basement. Although the geological constraints still drive the <span class="hlt">final</span> decision, the proposed method improves the existing tools for a semi-automatic tracing of the <span class="hlt">boundaries</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29416042','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29416042"><span>Stratification of TAD <span class="hlt">boundaries</span> reveals preferential insulation of super-enhancers by strong <span class="hlt">boundaries</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gong, Yixiao; Lazaris, Charalampos; Sakellaropoulos, Theodore; Lozano, Aurelie; Kambadur, Prabhanjan; Ntziachristos, Panagiotis; Aifantis, Iannis; Tsirigos, Aristotelis</p> <p>2018-02-07</p> <p>The metazoan genome is compartmentalized in areas of highly interacting chromatin known as topologically associating domains (TADs). TADs are demarcated by <span class="hlt">boundaries</span> mostly conserved across cell types and even across species. However, a genome-wide characterization of TAD <span class="hlt">boundary</span> strength in mammals is still lacking. In this study, we first use fused two-dimensional lasso as a machine learning method to improve Hi-C contact matrix reproducibility, and, subsequently, we categorize TAD <span class="hlt">boundaries</span> based on their insulation score. We demonstrate that higher TAD <span class="hlt">boundary</span> insulation scores are associated with elevated CTCF levels and that they may differ across cell types. Intriguingly, we observe that super-enhancers are preferentially insulated by strong <span class="hlt">boundaries</span>. Furthermore, we demonstrate that strong TAD <span class="hlt">boundaries</span> and super-enhancer elements are frequently co-duplicated in cancer patients. Taken together, our findings suggest that super-enhancers insulated by strong TAD <span class="hlt">boundaries</span> may be exploited, as a functional unit, by cancer cells to promote oncogenesis.</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.ncbi.nlm.nih.gov/pubmed/25967336','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25967336"><span>Optic disc detection and <span class="hlt">boundary</span> extraction in retinal images.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Basit, A; Fraz, Muhammad Moazam</p> <p>2015-04-10</p> <p>With the development of digital image processing, analysis and modeling techniques, automatic retinal image analysis is emerging as an important screening tool for early detection of ophthalmologic disorders such as diabetic retinopathy and glaucoma. In this paper, a robust method for optic disc detection and extraction of the optic disc <span class="hlt">boundary</span> is proposed to help in the development of computer-assisted diagnosis and treatment of such ophthalmic disease. The proposed method is based on morphological operations, smoothing filters, and the marker controlled watershed transform. Internal and external markers are used to first modify the gradient magnitude image and then the watershed transformation is applied on this modified gradient magnitude image for <span class="hlt">boundary</span> extraction. This method has shown significant improvement over existing methods in terms of detection and <span class="hlt">boundary</span> extraction of the optic disc. The proposed method has optic disc detection success rate of 100%, 100%, 100% and 98.9% for the DRIVE, Shifa, CHASE_DB1, and DIARETDB1 databases, respectively. The optic disc <span class="hlt">boundary</span> detection achieved an average spatial overlap of 61.88%, 70.96%, 45.61%, and 54.69% for these databases, respectively, which are higher than <span class="hlt">currents</span> methods.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA324292','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA324292"><span>3D <span class="hlt">Boundary</span> Element Analysis for Composite Joints with discrete Damage. Part 1.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1996-11-15</p> <p>WHS/DIOR, Oct 94 Fracture Analysis Consultants, Inc. 121 Eastern Heights Dr. Ithaca, New York 14850 (607) 257-4970 SBIR Topic AF96 -150 3D <span class="hlt">Boundary</span>...41 1 F33615-96-C-5070 SBIR Topic AF96 -150: Phase I <span class="hlt">Final</span> Report Sunmmry Report WL/MLBM solicited Phase I SBIR proposals to develop a capability...materials; no precomputations are required. 2 F33615-96-C-5070 SBIR Topic AF96 -150: Phase I <span class="hlt">Final</span> Report Task 6. We have developed a fully 3D Galerkin BEM</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29129536','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29129536"><span>Event <span class="hlt">Boundaries</span> Trigger Rapid Memory Reinstatement of the Prior Events to Promote Their Representation in Long-Term Memory.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sols, Ignasi; DuBrow, Sarah; Davachi, Lila; Fuentemilla, Lluís</p> <p>2017-11-20</p> <p>Although everyday experiences unfold continuously over time, shifts in context, or event <span class="hlt">boundaries</span>, can influence how those events come to be represented in memory [1-4]. Specifically, mnemonic binding across sequential representations is more challenging at context shifts, such that successful temporal associations are more likely to be formed within than across contexts [1, 2, 5-9]. However, in order to preserve a subjective sense of continuity, it is important that the memory system bridge temporally adjacent events, even if they occur in seemingly distinct contexts. Here, we used pattern similarity analysis to scalp electroencephalographic (EEG) recordings during a sequential learning task [2, 3] in humans and showed that the detection of event <span class="hlt">boundaries</span> triggered a rapid memory reinstatement of the just-encoded sequence episode. Memory reactivation was detected rapidly (∼200-800 ms from the onset of the event <span class="hlt">boundary</span>) and was specific to context shifts that were preceded by an event sequence with episodic content. Memory reinstatement was not observed during the sequential encoding of events within an episode, indicating that memory reactivation was induced specifically upon context shifts. <span class="hlt">Finally</span>, the degree of neural similarity between neural responses elicited during sequence encoding and at event <span class="hlt">boundaries</span> correlated positively with participants' ability to later link across sequences of events, suggesting a critical role in binding temporally adjacent events in long-term memory. <span class="hlt">Current</span> results shed light onto the neural mechanisms that promote episodic encoding not only for information within the event, but also, importantly, in the ability to link across events to create a memory representation of continuous experience. Copyright © 2017 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19960021315&hterms=third+sector&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dthird%2Bsector','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19960021315&hterms=third+sector&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dthird%2Bsector"><span>The heliospheric sector <span class="hlt">boundary</span> as a distented magnetic cloud</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Crooker, N. U.; Intriligator, D. S.</p> <p>1995-01-01</p> <p>A magnetic cloud was detected both near Earth and by Pioneer 11 located 43 deg east of Earth at 4.8 AU. The magnetic field within the cloud rotated smoothly from toward to away polarity, marking sector <span class="hlt">boundary</span> passage. Interpreted as a flux rope, the cloud had a vertical axis, implying that its cylindrical cross-section in the ecliptic plane was distended along the sector <span class="hlt">boundary</span> by at least 43, forming an extensive occlusion in the heliospheric <span class="hlt">current</span> sheet. At 1 AU the cloud had plasma signatures typical of a fast coronal mass ejection with low temperature and a leading shock. In contrast, at 4.8 AU, only the cloud signature remained. Its radial dimension was the same at both locations, consistent with little expansion beyond 1 AU. Energetic particle data at 4.8 AU show high fluxes preceding the cloud but not extending forward to the corotating shock that marked entry into the interaction region containing the cloud. The streaming direction was antisunward, consistent with possible acceleration in a low-beta region of field line draping around the cloud's western (upstream) end. The fluxes dropped upon entry into the cloud and became essentially isotropic one third of the way through it. On the basis of sector <span class="hlt">boundary</span> characteristics published in the past, we suggest that distended clouds may be common heliospheric <span class="hlt">current</span> sheet occlusions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740017695','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740017695"><span>Relaxation of an unsteady turbulent <span class="hlt">boundary</span> layer on a flat plate in an expansion tube</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gurta, R. N.; Trimpi, R. L.</p> <p>1974-01-01</p> <p>An analysis is presented for the relaxation of a turbulent <span class="hlt">boundary</span> layer on a semi-infinite flat plate after passage of a shock wave and a trailing driver gas-driven gas interface. The problem has special application to expansion-tube flows. The flow-governing equations have been transformed into the Crocco variables, and a time-similar solution is presented in terms of the dimensionless distance-time variable alpha and the dimensionless velocity variable beta. An eddy-viscosity model, similar to that of time-steady <span class="hlt">boundary</span> layers, is applied to the inner and outer regions of the <span class="hlt">boundary</span> layer. A turbulent Prandtl number equal to the molecular Prandtl number is used to relate the turbulent heat flux to the eddy viscosity. The numerical results, obtained by using the Gauss-Seidel line-relaxation method, indicate that a fully turbulent <span class="hlt">boundary</span> layer relaxes faster to the <span class="hlt">final</span> steady-state values of heat transfer and skin friction than a laminar <span class="hlt">boundary</span> layer. The results also give a fairly good estimate of the local skin friction and heat transfer for near steady-flow conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011APS..DFD.E3007D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011APS..DFD.E3007D"><span>Large-wave simulation of spilling breaking and undertow <span class="hlt">current</span> over constant slope beach</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dimas, Athanassios; Kolokythas, Gerasimos; Dimakopoulos, Aggelos</p> <p>2011-11-01</p> <p>The three-dimensional, free-surface flow, developing by the propagation of nonlinear breaking waves over a constant slope bed, is numerically simulated. The main objective is to investigate the effect of spilling breaking on the characteristics of the induced undertow <span class="hlt">current</span> by performing large-wave simulations (LWS) based on the numerical solution of the Navier-Stokes equations subject to the fully nonlinear free-surface <span class="hlt">boundary</span> conditions and the appropriate bottom, inflow and outflow <span class="hlt">boundary</span> conditions. The equations are properly transformed so that the computational domain becomes time-independent. In the present study, the case of incoming waves with wavelength to inflow depth ratio λ/ d ~ 6.6 and wave steepness H/ λ ~0.025, over bed of slope tan β = 1/35, is investigated. The LWS predicts satisfactorily breaking parameters - height and depth - and wave dissipation in the surf zone, in comparison to experimental data. In the corresponding LES, breaking height and depth are smaller and wave dissipation in the surf zone is weaker. For the undertow <span class="hlt">current</span>, it is found that it is induced by the breaking process at the free surface, while its strength is controlled by the bed shear stress. <span class="hlt">Finally</span>, the amplitude of the bed shear stress increases substantially in the breaking zone, becoming up to six times larger than the respective amplitude at the outer region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA134702','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA134702"><span>Nearshore <span class="hlt">Current</span> Model Workshop Summary.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1983-09-01</p> <p>dissipation , and wave-<span class="hlt">current</span> interaction. b. Incorporation into models of wave-breaking. c. Parameterization of turbulence in models. d. Incorporation...into models of surf zone energy dissipation . e. Methods to specify waves and <span class="hlt">currents</span> on the <span class="hlt">boundaries</span> of the grid. f. Incorporation into models of...also recommended. Improvements should include nonlinear and irregular wave effects and improved models of wave-breaking and wave energy dissipation in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940002870&hterms=turbine+blade+design&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dturbine%2Bblade%2Bdesign','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940002870&hterms=turbine+blade+design&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dturbine%2Bblade%2Bdesign"><span>DESIGN OF TWO-DIMENSIONAL SUPERSONIC TURBINE ROTOR BLADES WITH <span class="hlt">BOUNDARY</span>-LAYER CORRECTION</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Goldman, L. J.</p> <p>1994-01-01</p> <p>A computer program has been developed for the design of supersonic rotor blades where losses are accounted for by correcting the ideal blade geometry for <span class="hlt">boundary</span> layer displacement thickness. The ideal blade passage is designed by the method of characteristics and is based on establishing vortex flow within the passage. <span class="hlt">Boundary</span>-layer parameters (displacement and momentum thicknesses) are calculated for the ideal passage, and the <span class="hlt">final</span> blade geometry is obtained by adding the displacement thicknesses to the ideal nozzle coordinates. The <span class="hlt">boundary</span>-layer parameters are also used to calculate the aftermixing conditions downstream of the rotor blades assuming the flow mixes to a uniform state. The computer program input consists essentially of the rotor inlet and outlet Mach numbers, upper- and lower-surface Mach numbers, inlet flow angle, specific heat ratio, and total flow conditions. The program gas properties are set up for air. Additional gases require changes to be made to the program. The computer output consists of the corrected rotor blade coordinates, the principal <span class="hlt">boundary</span>-layer parameters, and the aftermixing conditions. This program is written in FORTRAN IV for batch execution and has been implemented on an IBM 7094. This program was developed in 1971.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070023635','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070023635"><span>Orbiter Entry Aeroheating Working Group Viscous CFD <span class="hlt">Boundary</span> Layer Transition Trailblazer Solutions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wood, William A.; Erickson, David W.; Greene, Francis A.</p> <p>2007-01-01</p> <p><span class="hlt">Boundary</span> layer transition correlations for the Shuttle Orbiter have been previously developed utilizing a two-layer <span class="hlt">boundary</span> layer prediction technique. The particular two-layer technique that was used is limited to Mach numbers less than 20. To allow assessments at Mach numbers greater than 20, it is proposed to use viscous CFD to the predict <span class="hlt">boundary</span> layer properties. This report addresses if the existing Orbiter entry aeroheating viscous CFD solutions, which were originally intended to be used for heat transfer rate predictions, adequately resolve <span class="hlt">boundary</span> layer edge properties and if the existing two-layer results could be leveraged to reduce the number of needed CFD solutions. The <span class="hlt">boundary</span> layer edge parameters from viscous CFD solutions are extracted along the wind side centerline of the Space Shuttle Orbiter at reentry conditions, and are compared with results from the two-layer <span class="hlt">boundary</span> layer prediction technique. The differences between the viscous CFD and two-layer prediction techniques vary between Mach 6 and 18 flight conditions and Mach 6 wind tunnel conditions, and there is not a straightforward scaling between the viscous CFD and two-layer values. Therefore: it is not possible to leverage the existing two-layer Orbiter flight <span class="hlt">boundary</span> layer data set as a substitute for a viscous CFD data set; but viscous CFD solutions at the <span class="hlt">current</span> grid resolution are sufficient to produce a <span class="hlt">boundary</span> layer data set suitable for applying edge-based <span class="hlt">boundary</span> layer transition correlations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018WRR....54.3207W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018WRR....54.3207W"><span>A Semianalytical Model for Pumping Tests in Finite Heterogeneous Confined Aquifers With Arbitrarily Shaped <span class="hlt">Boundary</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Lei; Dai, Cheng; Xue, Liang</p> <p>2018-04-01</p> <p>This study presents a Laplace-transform-based <span class="hlt">boundary</span> element method to model the groundwater flow in a heterogeneous confined finite aquifer with arbitrarily shaped <span class="hlt">boundaries</span>. The <span class="hlt">boundary</span> condition can be Dirichlet, Neumann or Robin-type. The derived solution is analytical since it is obtained through the Green's function method within the domain. However, the numerical approximation is required on the <span class="hlt">boundaries</span>, which essentially renders it a semi-analytical solution. The proposed method can provide a general framework to derive solutions for zoned heterogeneous confined aquifers with arbitrarily shaped <span class="hlt">boundary</span>. The requirement of the <span class="hlt">boundary</span> element method presented here is that the Green function must exist for a specific PDE equation. In this study, the linear equations for the two-zone and three-zone confined aquifers with arbitrarily shaped <span class="hlt">boundary</span> is established in Laplace space, and the solution can be obtained by using any linear solver. Stehfest inversion algorithm can be used to transform it back into time domain to obtain the transient solution. The presented solution is validated in the two-zone cases by reducing the arbitrarily shaped <span class="hlt">boundaries</span> to circular ones and comparing it with the solution in Lin et al. (2016, https://doi.org/10.1016/j.jhydrol.2016.07.028). The effect of <span class="hlt">boundary</span> shape and well location on dimensionless drawdown in two-zone aquifers is investigated. <span class="hlt">Finally</span> the drawdown distribution in three-zone aquifers with arbitrarily shaped <span class="hlt">boundary</span> for constant-rate tests (CRT) and flow rate distribution for constant-head tests (CHT) are analyzed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10611E..15S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10611E..15S"><span>Automatic video shot <span class="hlt">boundary</span> detection using k-means clustering and improved adaptive dual threshold comparison</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sa, Qila; Wang, Zhihui</p> <p>2018-03-01</p> <p>At present, content-based video retrieval (CBVR) is the most mainstream video retrieval method, using the video features of its own to perform automatic identification and retrieval. This method involves a key technology, i.e. shot segmentation. In this paper, the method of automatic video shot <span class="hlt">boundary</span> detection with K-means clustering and improved adaptive dual threshold comparison is proposed. First, extract the visual features of every frame and divide them into two categories using K-means clustering algorithm, namely, one with significant change and one with no significant change. Then, as to the classification results, utilize the improved adaptive dual threshold comparison method to determine the abrupt as well as gradual shot <span class="hlt">boundaries.Finally</span>, achieve automatic video shot <span class="hlt">boundary</span> detection system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28914160','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28914160"><span>Making <span class="hlt">Boundaries</span> Great Again: Essentialism and Support for <span class="hlt">Boundary</span>-Enhancing Initiatives.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Roberts, Steven O; Ho, Arnold K; Rhodes, Marjorie; Gelman, Susan A</p> <p>2017-12-01</p> <p>Psychological essentialism entails a focus on category <span class="hlt">boundaries</span> (e.g., categorizing people as men or women) and an increase in the conceptual distance between those <span class="hlt">boundaries</span> (e.g., accentuating the differences between men and women). Across eight studies, we demonstrate that essentialism additionally entails an increase in support for <span class="hlt">boundary</span>-enhancing legislation, policies, and social services, and that it does so under conditions that disadvantage social groups, as well as conditions that benefit them. First, individual differences in essentialism were associated with support for legislation mandating that transgender people use restrooms corresponding with their biological sex, and with support for the <span class="hlt">boundary</span>-enhancing policies of the 2016 then-presumptive Republican presidential nominee (i.e., Donald Trump). Second, essentialism was associated with support for same-gender classrooms designed to promote student learning, as well as support for services designed to benefit LGBTQ (lesbian, gay, bisexual, transgender, queer) individuals. These findings demonstrate the <span class="hlt">boundary</span>-enhancing implications of essentialism and their social significance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3330568','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3330568"><span>Psychodynamic Perspective on Therapeutic <span class="hlt">Boundaries</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>Bridges, Nancy A.</p> <p>1999-01-01</p> <p>Discussion of <span class="hlt">boundaries</span> in therapeutic work most often focuses on <span class="hlt">boundary</span> maintenance, risk management factors, and <span class="hlt">boundary</span> violations. The psychodynamic meaning and clinical management of <span class="hlt">boundaries</span> in therapeutic relationships remains a neglected area of discourse. Clinical vignettes will illustrate a psychodynamic, developmental-relational perspective using <span class="hlt">boundary</span> dilemmas to deepen and advance the therapeutic process. This article contributes to the dialogue about the process of making meaning and constructing therapeutically useful and creative <span class="hlt">boundaries</span> that further the psychotherapeutic process. PMID:10523432</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1198233-grain-boundary-resistivity-yttria-stabilized-zirconia','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1198233-grain-boundary-resistivity-yttria-stabilized-zirconia"><span>Grain <span class="hlt">Boundary</span> Resistivity of Yttria-Stabilized Zirconia at 1400°C</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Wang, J.; Du, A.; Yang, Di; ...</p> <p>2013-01-01</p> <p>Tmore » he grain size dependence of the bulk resistivity of 3 mol% yttria-stabilized zirconia at 1400°C was determined from the effect of a dc electric field E a = 18.1  V/cm on grain growth and the corresponding electric <span class="hlt">current</span> during isothermal annealing tests. Employing the brick layer model, the present annealing test results were in accordance with extrapolations of the values obtained at lower temperature employing impedance spectroscopy and 4-point-probe dc. he combined values give that the magnitude of the grain <span class="hlt">boundary</span> resistivity ρ b = 133  ohm-cm. he electric field across the grain <span class="hlt">boundary</span> width was 28–43 times the applied field for the grain size and <span class="hlt">current</span> ranges in the present annealing test.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JEPT...90..366K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JEPT...90..366K"><span>The <span class="hlt">Boundary</span> Function Method. Fundamentals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kot, V. A.</p> <p>2017-03-01</p> <p>The <span class="hlt">boundary</span> function method is proposed for solving applied problems of mathematical physics in the region defined by a partial differential equation of the general form involving constant or variable coefficients with a Dirichlet, Neumann, or Robin <span class="hlt">boundary</span> condition. In this method, the desired function is defined by a power polynomial, and a <span class="hlt">boundary</span> function represented in the form of the desired function or its derivative at one of the <span class="hlt">boundary</span> points is introduced. Different sequences of <span class="hlt">boundary</span> equations have been set up with the use of differential operators. Systems of linear algebraic equations constructed on the basis of these sequences allow one to determine the coefficients of a power polynomial. Constitutive equations have been derived for initial <span class="hlt">boundary</span>-value problems of all the main types. With these equations, an initial <span class="hlt">boundary</span>-value problem is transformed into the Cauchy problem for the <span class="hlt">boundary</span> function. The determination of the <span class="hlt">boundary</span> function by its derivative with respect to the time coordinate completes the solution of the problem.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980237977','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980237977"><span>Physics of <span class="hlt">Boundaries</span> and their Interactions in Space Plasmas</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Omidi, Nojan; Karimabadi, Homayoun; Krauss-Varban, Dietmar</p> <p>1998-01-01</p> <p>This <span class="hlt">final</span> report describes a brief summary of our accomplishments during the complete contract period. Traditionally, due to computational limitations, it has been impossible to obtain a global view of the magnetosphere on ion time and spatial scales. As a result, kinetic simulations have concentrated on the local structure of different magnetospheric discontinuities and <span class="hlt">boundaries</span>. However, due to the emergence of low cost desktop superconductors, as well as by taking full advantage of latest advances in data mining and visualization technology, we were able to bypass our planned (proposed) regional simulations and proceed to large-scale 3-D and 2-D global hybrid simulations of the magnetosphere. As a result, although we are only finishing the second year of the proposed activity, much of the original scientific objectives have been surpassed and new avenues of investigation have been opened. Such simulations have led us to possible explanations of some long-standing issues in magnetospheric physics. They have also enabled us to make a number of important discoveries/predictions, which need to be looked for in satellite data. Examples include: (1) the finding that the bow shock can become unstable to the Kelvin-Helmholtz (KH;) (2) the discovery of a mechanism for intermittent reconnection due to ion physics which may be relevant to the explanation of the recurrence rate of flux transfer events (FTEs;) and (3) the finding that the <span class="hlt">current</span> sheet in the near-Earth magnetotail region can become unstable to KH with detectable, unique ionospheric signatures. Further, we demonstrated a viable mechanism for the onset of reconnection at the magnetopause, examined the detailed structure of the <span class="hlt">boundary</span> layer incorporating curvature effects, and provided an explanation for the large core fields observed within FTEs as well as flux ropes in the magnetotail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980235526','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980235526"><span>Physics of <span class="hlt">Boundaries</span> and their Interactions in Space Plasmas</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Omidi, Nojan; Karimabadi, Homayoun; Krauss-Varban, Dietmar</p> <p>1998-01-01</p> <p>This <span class="hlt">final</span> report describes a brief summary of our accomplishments during the complete contract period. Traditionally, due to computational limitations, it has been impossible to obtain a global view of the magnetosphere on ion time and spatial scales. As a result, kinetic-simulations have concentrated on the local structure of different magnetospheric discontinuities and <span class="hlt">boundaries</span>. However, due to the emergence of low cost supercomputers, as well as by taking full advantage of latest advances in data mining and visualization technology, we were able to bypass our planned (proposed) regional simulations and proceed to large-scale 3-D and 2-D global hybrid simulations of the magnetosphere. As a result, although we are only finishing the second year of the proposed activity, much of the original scientific objectives have been surpassed and new avenues of investigation have been opened. Such simulations have led us to possible explanations of some long-standing issues in magnetospheric physics. They have also enables us to make a number of important discoveries predictions, which need to be looked for in satellite data. Examples include the finding that the bow shock can become unstable to the Kelvin-Helmholtz (KH), (2) the discovery of a mechanism for intermittent reconnection due to ion physics which may be relevant to the explanation of the recurrence rate of flux transfer events (FTEs), and (3) this finding that the <span class="hlt">current</span> sheet in the near-Earth magnetotail region can become unstable to KH with detectable, unique ionospheric signatures. Further, we demonstrated a viable mechanism for the onset of reconnection at the magnetopause, examined the detailed structure of the <span class="hlt">boundary</span> layer incorporating curvature effects, and provided an explanation for the large core fields observed within FTEs as well as flux ropes in the magnetotail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810025313','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810025313"><span>Numerical <span class="hlt">Boundary</span> Condition Procedures</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1981-01-01</p> <p>Topics include numerical procedures for treating inflow and outflow <span class="hlt">boundaries</span>, steady and unsteady discontinuous surfaces, far field <span class="hlt">boundaries</span>, and multiblock grids. In addition, the effects of numerical <span class="hlt">boundary</span> approximations on stability, accuracy, and convergence rate of the numerical solution are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011ERL.....6a1001T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011ERL.....6a1001T"><span><span class="hlt">Boundary</span> issues</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Townsend, Alan R.; Porder, Stephen</p> <p>2011-03-01</p> <p>-centric <span class="hlt">boundary</span> (Filippelli 2008, Handoh and Lenton 2003). However, human alteration of the P cycle has multiple potential <span class="hlt">boundaries</span> (figure 1), including P-driven freshwater eutrophication (Smith and Schindler 2009), the potential for world P supply to place an ultimate limit on food production (Smil 2000, Childers et al 2011), and depletion of soil P stocks in some world regions (MacDonald et al 2011). Carpenter and Bennett revisit the P <span class="hlt">boundary</span> from the freshwater eutrophication perspective. Given the extraordinary variation in freshwater ecosystems across the globe, this is a challenging task, but the authors strengthen their analysis by using three different <span class="hlt">boundaries</span> with relevance to eutrophication, along with two water quality targets and a range of estimates of P flow to the sea. In doing so, they make a compelling case that if freshwater eutrophication is indeed a Rubicon, we have already crossed it. Importantly, Carpenter and Bennett go beyond the calculation of new <span class="hlt">boundaries</span> to make broader points about humanity's relationship with the P cycle. Disruptions of both the P and N cycles are mostly about our need for food (Galloway et al 2008, Cordell et al 2009), but unlike N, P supplies are finite and irreplaceable. Environmental concerns aside, we can fix all the N2 from the atmosphere we want—but deplete our economically viable P reserves and we're in trouble. Figure 1 Figure 1. Human alteration of the global P cycle has multiple possible <span class="hlt">boundaries</span>. These include the environmental risks posed by freshwater eutrophication and marine anoxic events, and the food security risks that come from depletion of soil P stocks in some world regions, as well as finite global supplies of high-value mineral P reserves. Photo credits beyond authors: upper left, Shelby Riskin; upper right, Pedro Sanchez. In effect, Carpenter and Bennett argue that among P's multiple <span class="hlt">boundaries</span>, the one for freshwaters is less forgiving of our <span class="hlt">current</span> activities (but no less important) than is</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21260185-repulsive-casimir-effect-from-extra-dimensions-robin-boundary-conditions-from-branes-pistons','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21260185-repulsive-casimir-effect-from-extra-dimensions-robin-boundary-conditions-from-branes-pistons"><span>Repulsive Casimir effect from extra dimensions and Robin <span class="hlt">boundary</span> conditions: From branes to pistons</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>Elizalde, E.; Odintsov, S. D.; Institucio Catalana de Recerca i Estudis Avanccats</p> <p>2009-03-15</p> <p>We evaluate the Casimir energy and force for a massive scalar field with general curvature coupling parameter, subject to Robin <span class="hlt">boundary</span> conditions on two codimension-one parallel plates, located on a (D+1)-dimensional background spacetime with an arbitrary internal space. The most general case of different Robin coefficients on the two separate plates is considered. With independence of the geometry of the internal space, the Casimir forces are seen to be attractive for special cases of Dirichlet or Neumann <span class="hlt">boundary</span> conditions on both plates and repulsive for Dirichlet <span class="hlt">boundary</span> conditions on one plate and Neumann <span class="hlt">boundary</span> conditions on the other. For Robinmore » <span class="hlt">boundary</span> conditions, the Casimir forces can be either attractive or repulsive, depending on the Robin coefficients and the separation between the plates, what is actually remarkable and useful. Indeed, we demonstrate the existence of an equilibrium point for the interplate distance, which is stabilized due to the Casimir force, and show that stability is enhanced by the presence of the extra dimensions. Applications of these properties in braneworld models are discussed. <span class="hlt">Finally</span>, the corresponding results are generalized to the geometry of a piston of arbitrary cross section.« 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_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('https://ntrs.nasa.gov/search.jsp?R=20000075647&hterms=Shrink&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DShrink','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000075647&hterms=Shrink&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3DShrink"><span>A <span class="hlt">Boundary</span> Scan Test Vehicle for Direct Chip Attach Testing</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Parsons, Heather A.; DAgostino, Saverio; Arakaki, Genji</p> <p>2000-01-01</p> <p>To facilitate the new faster, better and cheaper spacecraft designs, smaller more mass efficient avionics and instruments are using higher density electronic packaging technologies such as direct chip attach (DCA). For space flight applications, these technologies need to have demonstrated reliability and reasonably well defined fabrication and assembly processes before they will be accepted as baseline designs in new missions. As electronics shrink in size, not only can repair be more difficult, but 49 probing" circuitry can be very risky and it becomes increasingly more difficult to identify the specific source of a problem. To test and monitor these new technologies, the Direct Chip Attach Task, under NASA's Electronic Parts and Packaging Program (NEPP), chose the test methodology of <span class="hlt">boundary</span> scan testing. The <span class="hlt">boundary</span> scan methodology was developed for interconnect integrity and functional testing at hard to access electrical nodes. With <span class="hlt">boundary</span> scan testing, active devices are used and failures can be identified to the specific device and lead. This technology permits the incorporation of "built in test" into almost any circuit and thus gives detailed test access to the highly integrated electronic assemblies. This presentation will describe <span class="hlt">boundary</span> scan, discuss the development of the <span class="hlt">boundary</span> scan test vehicle for DCA and <span class="hlt">current</span> plans for testing of direct chip attach configurations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25615218','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25615218"><span>Influence of electrical <span class="hlt">boundary</span> conditions on molecular dynamics simulations of ionic liquid electrosprays.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Borner, Arnaud; Wang, Pengxiang; Levin, Deborah A</p> <p>2014-12-01</p> <p>Molecular dynamics (MD) simulations are coupled to solutions of Poisson's equation to study the effects of the electrical <span class="hlt">boundary</span> conditions on the emission modes of an electrospray thruster fed with an ionic liquid. A comparison of a new tip <span class="hlt">boundary</span> condition with an analytical model based on a semihyperboloidal shape offers good agreement, although the analytical model overestimates the maximum value of the tangential electric field since it does not take into account the space charge that reduces the field at the liquid surface. It is found that a constant electric field model gives similar agreement to the more rigorous and computationally expensive tip <span class="hlt">boundary</span> condition at lower flow rates. However, at higher mass flow rates the constant electric field produces extruded particles with higher Coulomb energy per ion, consistent with droplet formation. Furthermore, the MD simulations show that ion emission sites differ based on the <span class="hlt">boundary</span> condition and snapshots offer an explanation as to why some <span class="hlt">boundary</span> condition models will predict emission in a purely ionic mode, whereas others suggest a mixed ion-droplet regime. <span class="hlt">Finally</span>, specific impulses and thrusts are compared for the different models and are found to vary up to 30% due to differences in the average charge to mass ratio.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhRvE..90f3303B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhRvE..90f3303B"><span>Influence of electrical <span class="hlt">boundary</span> conditions on molecular dynamics simulations of ionic liquid electrosprays</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Borner, Arnaud; Wang, Pengxiang; Levin, Deborah A.</p> <p>2014-12-01</p> <p>Molecular dynamics (MD) simulations are coupled to solutions of Poisson's equation to study the effects of the electrical <span class="hlt">boundary</span> conditions on the emission modes of an electrospray thruster fed with an ionic liquid. A comparison of a new tip <span class="hlt">boundary</span> condition with an analytical model based on a semihyperboloidal shape offers good agreement, although the analytical model overestimates the maximum value of the tangential electric field since it does not take into account the space charge that reduces the field at the liquid surface. It is found that a constant electric field model gives similar agreement to the more rigorous and computationally expensive tip <span class="hlt">boundary</span> condition at lower flow rates. However, at higher mass flow rates the constant electric field produces extruded particles with higher Coulomb energy per ion, consistent with droplet formation. Furthermore, the MD simulations show that ion emission sites differ based on the <span class="hlt">boundary</span> condition and snapshots offer an explanation as to why some <span class="hlt">boundary</span> condition models will predict emission in a purely ionic mode, whereas others suggest a mixed ion-droplet regime. <span class="hlt">Finally</span>, specific impulses and thrusts are compared for the different models and are found to vary up to 30% due to differences in the average charge to mass ratio.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22332659','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22332659"><span>Chromatin insulator elements: establishing barriers to set heterochromatin <span class="hlt">boundaries</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barkess, Gráinne; West, Adam G</p> <p>2012-02-01</p> <p>Epigenomic profiling has revealed that substantial portions of genomes in higher eukaryotes are organized into extensive domains of transcriptionally repressive chromatin. The <span class="hlt">boundaries</span> of repressive chromatin domains can be fixed by DNA elements known as barrier insulators, to both shield neighboring gene expression and to maintain the integrity of chromosomal silencing. Here, we examine the <span class="hlt">current</span> progress in identifying vertebrate barrier elements and their binding factors. We overview the design of the reporter assays used to define enhancer-blocking and barrier insulators. We look at the mechanisms vertebrate barrier proteins, such as USF1 and VEZF1, employ to counteract Polycomb- and heterochromatin-associated repression. We also undertake a critical analysis of whether CTCF could also act as a barrier protein. There is good evidence that barrier elements in vertebrates can form repressive chromatin domain <span class="hlt">boundaries</span>. Future studies will determine whether barriers are frequently used to define repressive domain <span class="hlt">boundaries</span> in vertebrates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1129339-smoothed-particle-hydrodynamics-continuous-boundary-force-method-navier-stokes-equations-subject-robin-boundary-condition','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1129339-smoothed-particle-hydrodynamics-continuous-boundary-force-method-navier-stokes-equations-subject-robin-boundary-condition"><span>Smoothed Particle Hydrodynamics Continuous <span class="hlt">Boundary</span> Force method for Navier-Stokes equations subject to Robin <span class="hlt">boundary</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>Pan, Wenxiao; Bao, Jie; Tartakovsky, Alexandre M.</p> <p>2014-02-15</p> <p>Robin <span class="hlt">boundary</span> condition for the Navier-Stokes equations is used to model slip conditions at the fluid-solid <span class="hlt">boundaries</span>. A novel Continuous <span class="hlt">Boundary</span> Force (CBF) method is proposed for solving the Navier-Stokes equations subject to Robin <span class="hlt">boundary</span> condition. In the CBF method, the Robin <span class="hlt">boundary</span> condition at <span class="hlt">boundary</span> is replaced by the homogeneous Neumann <span class="hlt">boundary</span> condition at the <span class="hlt">boundary</span> and a volumetric force term added to the momentum conservation equation. Smoothed Particle Hydrodynamics (SPH) method is used to solve the resulting Navier-Stokes equations. We present solutions for two-dimensional and three-dimensional flows in domains bounded by flat and curved <span class="hlt">boundaries</span> subject to variousmore » forms of the Robin <span class="hlt">boundary</span> condition. The numerical accuracy and convergence are examined through comparison of the SPH-CBF results with the solutions of finite difference or finite element method. Taken the no-slip <span class="hlt">boundary</span> condition as a special case of slip <span class="hlt">boundary</span> condition, we demonstrate that the SPH-CBF method describes accurately both no-slip and slip conditions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920055060&hterms=wildfire&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dwildfire','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920055060&hterms=wildfire&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dwildfire"><span>Major wildfires at the Cretaceous-Tertiary <span class="hlt">boundary</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Anders, Edward; Wolbach, Wendy S.; Gilmour, Iain</p> <p>1991-01-01</p> <p>The <span class="hlt">current</span> status of the reconstruction of major biomass fire events at the Cretaceous-Tertiary <span class="hlt">boundary</span> is discussed. Attention is given to the sources of charcoal and soot, the identification of biomass and fossil carbon, and such ignition-related problems as delated fires, high atmospheric O2 content, ignition mechanisms, and the greenhouse-effect consequences of fire on the scale envisioned. Consequences of these factors for species extinction patterns are noted.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFM.T11A0841H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFM.T11A0841H"><span><span class="hlt">Current</span> Plate Motion Across the Southwest Indian Ridge: Implications for the Diffuse Oceanic Plate <span class="hlt">Boundary</span> Between Nubia and Somalia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Horner-Johnson, B. C.; Cowles, S. M.; Gordon, R. G.; Argus, D. F.</p> <p>2001-12-01</p> <p>Prior studies of plate motion data along the Southwest Indian Ridge (SWIR) have produced results that conflict in detail. Chu & Gordon [1999], from an analysis of 59 spreading rates averaged over 3 Myr and of the azimuths of active transform faults, found that the data are most consistent with a diffuse Nubia-Somalia plate <span class="hlt">boundary</span> where it intersects the SWIR. When they solve for the best-fitting hypothetical narrow <span class="hlt">boundary</span>, they find that it lies near 37° E, east of the Prince Edward fracture zone. They find a Nubia-Somalia pole of rotation near the east coast of South Africa. In contrast, Lemaux, Gordon, and Royer [2001], from an analysis of 237 crossings of marine magnetic anomaly 5 (11 Ma), find that most of the motion is accommodated in a narrow zone, most likely along the ``inactive'' trace of the Andrew Bain fracture zone complex (ABFZC), which intersects the SWIR near 32° E. They find a pole well to the west of, and probably to the southwest of, the pole of rotation found by Chu & Gordon. Their pole indicates mainly strike-slip motion along the ``inactive'' ABFZC. To resolve these conflicting results, we determined a new greatly expanded and spatially much denser set of 243 spreading rates and analyzed available bathymetric data of active transform faults along the SWIR. The data show that the African oceanic lithosphere spreading away from the SWIR cannot simply be two plates divided by a single narrow <span class="hlt">boundary</span>. Our interpretation of the data is as follows. Near the SWIR, there is a diffuse <span class="hlt">boundary</span> with a western limit near the ABFZC and an eastern limit near 63.5° E. Slip is partitioned in this wide <span class="hlt">boundary</span>. Somewhere near the ABFZC (most likely the ABFZC itself) is a concentrated locus of right-lateral shearing parallel to the ABFZC whereas contraction perpendicular to the ABFZC is accommodated east of the ABFZC, perhaps over a very broad zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994CSR....14.1239G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994CSR....14.1239G"><span>Bottom <span class="hlt">boundary</span> layer spectral dissipation estimates in the presence of wave motions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gross, T. F.; Williams, A. J.; Terray, E. A.</p> <p>1994-08-01</p> <p>Turbulence measurements are an essential element of the Sediment TRansport Events on Shelves and Slopes experiment (STRESS). Sediment transport under waves is initiated within the wave <span class="hlt">boundary</span> layer at the seabed, at most a few tens of centimeters deep. The suspended load is carried by turbulent diffusion above the wave <span class="hlt">boundary</span> layer. Quantification of the turbulent diffusion active above the wave <span class="hlt">boundary</span> layer requires estimates of shear stress or energy dissipation in the presence of oscillating flows. Measurements by Benthic Acoustic Stress Sensors of velocity fluctuations were used to derive the dissipation rate from the energy level of the spectral inertial range (the -5/3 spectrum). When the wave orbital velocity is of similar magnitude to the mean flow, kinematic effects on the estimation techniques of stress and dissipation must be included. Throughout the STRESS experiment there was always significant wave energy affecting the turbulent bottom <span class="hlt">boundary</span> layer. LUMLEY and TERRAY [(1983) Journal of Physical Oceanography, 13, 2000-2007] presented a theory describing the effect of orbital motions on kinetic energy spectra. Their model is used here with observations of spectra taken within a turbulent <span class="hlt">boundary</span> layer which is affected by wave motion. While their method was an explicit solution for circular wave orbits aligned with mean <span class="hlt">current</span> we extrapolated it to the case of near bed horizontal motions, not aligned with the <span class="hlt">current</span>. The necessity of accounting for wave orbital motion is demonstrated, but variability within the field setting limited our certainty of the improvement in accuracy the corrections afforded.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910008411','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910008411"><span><span class="hlt">Current</span> collection by high voltage anodes in near ionospheric conditions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Antoniades, John A.; Greaves, Rod G.; Boyd, D. A.; Ellis, R.</p> <p>1990-01-01</p> <p>The authors experimentally identified three distinct regimes with large differences in <span class="hlt">current</span> collection in the presence of neutrals and weak magnetic fields. In magnetic field/anode voltage space the three regions are separated by very sharp transition <span class="hlt">boundaries</span>. The authors performed a series of laboratory experiments to study the dependence of the region <span class="hlt">boundaries</span> on several parameters, such as the ambient neutral density, plasma density, magnetic field strength, applied anode voltage, voltage pulsewidth, chamber material, chamber size and anode radius. The three observed regimes are: classical magnetic field limited collection; stable medium <span class="hlt">current</span> toroidal discharge; and large scale, high <span class="hlt">current</span> space glow discharge. There is as much as several orders of magnitude of difference in the amount of collected <span class="hlt">current</span> upon any <span class="hlt">boundary</span> crossing, particularly if one enters the space glow regime. They measured some of the properties of the plasma generated by the breakdown that is present in regimes II and III in the vicinity of the anode including the sheath modified electrostatic potential, I-V characteristics at high voltage as well as the local plasma density.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JLTP..178...35B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JLTP..178...35B"><span>Thermal Counterflow in a Periodic Channel with Solid <span class="hlt">Boundaries</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baggaley, Andrew W.; Laurie, Jason</p> <p>2015-01-01</p> <p>We perform numerical simulations of finite temperature quantum turbulence produced through thermal counterflow in superfluid He, using the vortex filament model. We investigate the effects of solid <span class="hlt">boundaries</span> along one of the Cartesian directions, assuming a laminar normal fluid with a Poiseuille velocity profile, whilst varying the temperature and the normal fluid velocity. We analyze the distribution of the quantized vortices, reconnection rates, and quantized vorticity production as a function of the wall-normal direction. We find that the quantized vortex lines tend to concentrate close to the solid <span class="hlt">boundaries</span> with their position depending only on temperature and not on the counterflow velocity. We offer an explanation of this phenomenon by considering the balance of two competing effects, namely the rate of turbulent diffusion of an isotropic tangle near the <span class="hlt">boundaries</span> and the rate of quantized vorticity production at the center. Moreover, this yields the observed scaling of the position of the peak vortex line density with the mutual friction parameter. <span class="hlt">Finally</span>, we provide evidence that upon the transition from laminar to turbulent normal fluid flow, there is a dramatic increase in the homogeneity of the tangle, which could be used as an indirect measure of the transition to turbulence in the normal fluid component for experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100002885','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100002885"><span>Excitation of Crossflow Instabilities in a Swept Wing <span class="hlt">Boundary</span> Layer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Carpenter, Mark H.; Choudhari, Meelan; Li, Fei; Streett, Craig L.; Chang, Chau-Lyan</p> <p>2010-01-01</p> <p>The problem of crossflow receptivity is considered in the context of a canonical 3D <span class="hlt">boundary</span> layer (viz., the swept Hiemenz <span class="hlt">boundary</span> layer) and a swept airfoil used recently in the SWIFT flight experiment performed at Texas A&M University. First, Hiemenz flow is used to analyze localized receptivity due to a spanwise periodic array of small amplitude roughness elements, with the goal of quantifying the effects of array size and location. Excitation of crossflow modes via nonlocalized but deterministic distribution of surface nonuniformity is also considered and contrasted with roughness induced acoustic excitation of Tollmien-Schlichting waves. <span class="hlt">Finally</span>, roughness measurements on the SWIFT model are used to model the effects of random, spatially distributed roughness of sufficiently small amplitude with the eventual goal of enabling predictions of initial crossflow disturbance amplitudes as functions of surface roughness parameters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27023887','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27023887"><span>Educator or Counselor? Navigating Uncertain <span class="hlt">Boundaries</span> in the Clinical Environment.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lane, Annette M; Corcoran, Lynn</p> <p>2016-04-01</p> <p>Nurse educators in the clinical environment experience great rewards and challenges in their work with undergraduate students. However, closely working with students can lead to the challenge of intervening with those who are emotionally distressed. How do nurse educators navigate the precarious and subtle territory between educating and counseling? This article briefly reviews how <span class="hlt">boundaries</span> are explored in nursing. Two case studies are presented to demonstrate how nurse educators can determine when their support and education begins to move into the counseling role. <span class="hlt">Finally</span>, future directions for nurse educators are suggested. Little research exists that examines how nurse educators navigate the <span class="hlt">boundaries</span> between educator and counselor roles with students in clinical settings. Navigating between the educator and counselor roles with students experiencing emotional distress in clinical settings can be challenging for nurse educators. Copyright 2016, SLACK Incorporated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApWS....7.1161D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApWS....7.1161D"><span>Identifying the groundwater basin <span class="hlt">boundaries</span>, using environmental isotopes: a case study</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Demiroğlu, Muhterem</p> <p>2017-06-01</p> <p>Groundwater, which is renewable under <span class="hlt">current</span> climatic conditions separately from other natural sources, in fact is a finite resource in terms of quality and fossil groundwater. Researchers have long emphasized the necessity of exploiting, operating, conserving and managing groundwater in an efficient and sustainable manner with an integrated water management approach. The management of groundwater needs reliable information about changes on groundwater quantity and quality. Environmental isotopes are the most important tools to provide this support. No matter which method we use to calculate the groundwater budget and flow equations, we need to determine <span class="hlt">boundary</span> conditions or the physical <span class="hlt">boundaries</span> of the domain. The Groundwater divide line or basin <span class="hlt">boundaries</span> that separate the two adjacent basin recharge areas from each other must be drawn correctly to be successful in defining complex groundwater basin <span class="hlt">boundary</span> conditions. Environmental isotope data, as well as other methods provide support for determining recharge areas of the aquifers, especially for karst aquifers, residence time and interconnections between aquifer systems. This study demonstrates the use of environmental isotope data to interpret and correct groundwater basin <span class="hlt">boundaries</span> giving as an example the Yeniçıkrı basin within the main Sakarya basin.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DFDD38009I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DFDD38009I"><span>Numerical modeling of the transitional <span class="hlt">boundary</span> layer over a flat plate</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ivanov, Dimitry; Chorny, Andrei</p> <p>2015-11-01</p> <p>Our example is connected with fundamental research on understanding how an initially laminar <span class="hlt">boundary</span> layer becomes turbulent. We have chosen the flow over a flat plate as a prototype for <span class="hlt">boundary</span>-layer flows around bodies. Special attention was paid to the near-wall region in order to capture all levels of the <span class="hlt">boundary</span> layer. In this study, the numerical software package OpenFOAM has been used in order to solve the flow field. The results were used in a comparative study with data obtained from Large Eddy Simulation (LES). The composite SGS-wall model is presently incorporated into a computer code suitable for the LES of developing flat-plate <span class="hlt">boundary</span> layers. Presently this model is extended to the LES of the zero-pressure gradient, flat-plate turbulent <span class="hlt">boundary</span> layer. In <span class="hlt">current</span> study the time discretization is based on a second order Crank-Nicolson/Adams-Bashforth method. LES solver using Smagorinsky and the one-equation LES turbulence models. The transition models significantly improve the prediction of the onset location compared to the fully turbulent models.LES methods appear to be the most promising new tool for the design and analysis of flow devices including transition regions of the turbulent flow.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005SPIE.5757..269S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005SPIE.5757..269S"><span>Transducer placement for robustness to variations in <span class="hlt">boundary</span> conditions for active structural acoustic control</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sprofera, Joseph D.; Clark, Robert L.; Cabell, Randolph H.; Gibbs, Gary P.</p> <p>2005-05-01</p> <p>Turbulent <span class="hlt">boundary</span> layer (TBL) noise is considered a primary contribution to the interior noise present in commercial airliners. There are numerous investigations of interior noise control devoted to aircraft panels; however, practical realization is a potential challenge since physical <span class="hlt">boundary</span> conditions are uncertain at best. In most prior studies, pinned or clamped <span class="hlt">boundary</span> conditions were assumed; however, realistic panels likely display a range of <span class="hlt">boundary</span> conditions between these two limits. Uncertainty in <span class="hlt">boundary</span> conditions is a challenge for control system designers, both in terms of the compensator implemented and the location of transducers required to achieve the desired control. The impact of model uncertainties, specifically uncertain <span class="hlt">boundaries</span>, on the selection of transducer locations for structural acoustic control is considered herein. The <span class="hlt">final</span> goal of this work is the design of an aircraft panel structure that can reduce TBL noise transmission through the use of a completely adaptive, single-input, single-output control system. The feasibility of this goal is demonstrated through the creation of a detailed analytical solution, followed by the implementation of a test model in a transmission loss apparatus. Successfully realizing a control system robust to variations in <span class="hlt">boundary</span> conditions can lead to the design and implementation of practical adaptive structures that could be used to control the transmission of sound to the interior of aircraft. Results from this research effort indicate it is possible to optimize the design of actuator and sensor location and aperture, minimizing the impact of <span class="hlt">boundary</span> conditions on the desired structural acoustic control.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22391984-impact-internal-crystalline-boundaries-lattice-thermal-conductivity-importance-boundary-structure-spacing','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22391984-impact-internal-crystalline-boundaries-lattice-thermal-conductivity-importance-boundary-structure-spacing"><span>Impact of internal crystalline <span class="hlt">boundaries</span> on lattice thermal conductivity: Importance of <span class="hlt">boundary</span> structure and spacing</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>Aghababaei, Ramin, E-mail: ramin.aghababaei@epfl.ch; Anciaux, Guillaume; Molinari, Jean-François</p> <p>2014-11-10</p> <p>The low thermal conductivity of nano-crystalline materials is commonly explained via diffusive scattering of phonons by internal <span class="hlt">boundaries</span>. In this study, we have quantitatively studied phonon-crystalline <span class="hlt">boundaries</span> scattering and its effect on the overall lattice thermal conductivity of crystalline bodies. Various types of crystalline <span class="hlt">boundaries</span> such as stacking faults, twins, and grain <span class="hlt">boundaries</span> have been considered in FCC crystalline structures. Accordingly, the specularity coefficient has been determined for different <span class="hlt">boundaries</span> as the probability of the specular scattering across <span class="hlt">boundaries</span>. Our results show that in the presence of internal <span class="hlt">boundaries</span>, the lattice thermal conductivity can be characterized by two parameters: (1)more » <span class="hlt">boundary</span> spacing and (2) <span class="hlt">boundary</span> excess free volume. We show that the inverse of the lattice thermal conductivity depends linearly on a non-dimensional quantity which is the ratio of <span class="hlt">boundary</span> excess free volume over <span class="hlt">boundary</span> spacing. This shows that phonon scattering across crystalline <span class="hlt">boundaries</span> is mainly a geometrically favorable process rather than an energetic one. Using the kinetic theory of phonon transport, we present a simple analytical model which can be used to evaluate the lattice thermal conductivity of nano-crystalline materials where the ratio can be considered as an average density of excess free volume. While this study is focused on FCC crystalline materials, where inter-atomic potentials and corresponding defect structures have been well studied in the past, the results would be quantitatively applicable for semiconductors in which heat transport is mainly due to phonon transport.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19730015646','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19730015646"><span>Remote sensing of ocean <span class="hlt">currents</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Maul, G. A. (Principal Investigator)</p> <p>1973-01-01</p> <p>The author has identified the following significant results. Monthly field experiments in support of the NOAA investigation of ocean color <span class="hlt">boundary</span> determination using ERTS-1 data have been conducted since June 1972. The <span class="hlt">boundary</span> between coastal waters and the Loop <span class="hlt">Current</span> has been detected by ERTS-1 as a result of sea state changes as well as color differences. Ocean information is contained in all 24 channels of the Bendix MSS flown on the C-130 in June 1972; this includes UV, visible, reflected IR, and emitted IR. Computer enhancement of MSS data is revealing many features not shown in the NDPF product.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JHyd..456..101C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JHyd..456..101C"><span>Generalized analytical solutions to sequentially coupled multi-species advective-dispersive transport equations in a finite domain subject to an arbitrary time-dependent source <span class="hlt">boundary</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>Chen, Jui-Sheng; Liu, Chen-Wuing; Liang, Ching-Ping; Lai, Keng-Hsin</p> <p>2012-08-01</p> <p>SummaryMulti-species advective-dispersive transport equations sequentially coupled with first-order decay reactions are widely used to describe the transport and fate of the decay chain contaminants such as radionuclide, chlorinated solvents, and nitrogen. Although researchers attempted to present various types of methods for analytically solving this transport equation system, the <span class="hlt">currently</span> available solutions are mostly limited to an infinite or a semi-infinite domain. A generalized analytical solution for the coupled multi-species transport problem in a finite domain associated with an arbitrary time-dependent source <span class="hlt">boundary</span> is not available in the published literature. In this study, we first derive generalized analytical solutions for this transport problem in a finite domain involving arbitrary number of species subject to an arbitrary time-dependent source <span class="hlt">boundary</span>. Subsequently, we adopt these derived generalized analytical solutions to obtain explicit analytical solutions for a special-case transport scenario involving an exponentially decaying Bateman type time-dependent source <span class="hlt">boundary</span>. We test the derived special-case solutions against the previously published coupled 4-species transport solution and the corresponding numerical solution with coupled 10-species transport to conduct the solution verification. <span class="hlt">Finally</span>, we compare the new analytical solutions derived for a finite domain against the published analytical solutions derived for a semi-infinite domain to illustrate the effect of the exit <span class="hlt">boundary</span> condition on coupled multi-species transport with an exponential decaying source <span class="hlt">boundary</span>. The results show noticeable discrepancies between the breakthrough curves of all the species in the immediate vicinity of the exit <span class="hlt">boundary</span> obtained from the analytical solutions for a finite domain and a semi-infinite domain for the dispersion-dominated condition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5647655','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5647655"><span>Comparison of DMSP and SECS region-1 and region-2 ionospheric <span class="hlt">current</span> boundary✩</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Weygand, J.M.; Wing, S.</p> <p>2017-01-01</p> <p>The region-1 and region-2 <span class="hlt">boundary</span> has traditionally been identified using data from a single spacecraft crossing the auroral region and measuring the large scale changes in the cross track magnetic field. With data from the AUTUMN, CANMOS, CARISMA, GIMA, DTU MGS, MACCS, McMAC, STEP, THEMIS, and USGS ground magnetometer arrays we applied a state-of-art technique based on spherical elementary <span class="hlt">current</span> system (SECS) method developed by Amm and Viljanen (1999) in order to calculate maps of region-1 and region-2 <span class="hlt">current</span> system over the North American and Greenland auroral region. Spherical elementary <span class="hlt">current</span> (SEC) amplitude (proxy for vertical <span class="hlt">currents</span>) maps can be inferred at 10 s temporal resolution, ~1.5° geographic latitude (Glat), and 3.5° geographic longitude (Glon) spatial resolution. We compare the location of the region-1 and region-2 <span class="hlt">boundary</span> obtained by the DMSP spacecraft with the region-1 and region-2 <span class="hlt">boundary</span> observed in the SEC <span class="hlt">current</span> amplitudes. We find that the <span class="hlt">boundaries</span> typically agree within 0.2° ± 1.3°. These results indicate that the location of the region-1 and region-2 <span class="hlt">boundary</span> can reasonably be determined from ground magnetometer data. The SECS maps represent a value-added product from the magnetometer database and can be used for contextual interpretation in conjunction with other missions as well as help with our understanding of magnetosphere-ionosphere coupling mechanisms using the ground arrays and the magnetospheric spacecraft data. PMID:29056861</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26846652','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26846652"><span>BREACHING THE SEXUAL <span class="hlt">BOUNDARIES</span> IN THE DOCTOR-PATIENT RELATIONSHIP: SHOULD ENGLISH LAW RECOGNISE FIDUCIARY DUTIES?</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ost, Suzanne</p> <p>2016-01-01</p> <p>In this article, I argue that sexual exploitation in the doctor-patient relationship would be dealt with more appropriately by the law in England and Wales on the basis of a breach of fiduciary duty. Three different types of sexual <span class="hlt">boundary</span> breaches are discussed, and the particular focus is on breaches where the patient's consent is obtained through inducement. I contend that <span class="hlt">current</span> avenues of redress do not clearly catch this behaviour and, moreover, they fail to capture the essence of the wrong committed by the doctor-the knowing breach of trust for self-gain-and the calculated way in which consent is induced. <span class="hlt">Finally</span>, I demonstrate that the fiduciary approach is compatible with the contemporary pro-patient autonomy model of the doctor-patient relationship. © The Author 2016. Published by Oxford University Press; all rights reserved. For Permissions, please email: journals.permissions@oup.com.</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('http://adsabs.harvard.edu/abs/2018JSP...171..599E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JSP...171..599E"><span>Stationary States of <span class="hlt">Boundary</span> Driven Exclusion Processes with Nonreversible <span class="hlt">Boundary</span> Dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Erignoux, C.; Landim, C.; Xu, T.</p> <p>2018-05-01</p> <p>We prove a law of large numbers for the empirical density of one-dimensional, <span class="hlt">boundary</span> driven, symmetric exclusion processes with different types of non-reversible dynamics at the <span class="hlt">boundary</span>. The proofs rely on duality techniques.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22288723-atom-probe-study-grain-boundary-segregation-technically-pure-molybdenum','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22288723-atom-probe-study-grain-boundary-segregation-technically-pure-molybdenum"><span>Atom probe study of grain <span class="hlt">boundary</span> segregation in technically pure molybdenum</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>Babinsky, K., E-mail: katharina.babinsky@stud.unileoben.ac.at; Weidow, J., E-mail: jonathan.weidow@chalmers.se; Knabl, W., E-mail: wolfram.knabl@plansee.com</p> <p>2014-01-15</p> <p>Molybdenum, a metal with excellent physical, chemical and high-temperature properties, is an interesting material for applications in lighting-technology, high performance electronics, high temperature furnace construction and coating technology. However, its applicability as a structural material is limited because of the poor oxidation resistance at high temperatures and a brittle-to-ductile transition around room temperature, which is influenced by the grain size and the content of interstitial impurities at the grain <span class="hlt">boundaries</span>. Due to the progress of the powder metallurgical production during the last decades, the amount of impurities in the <span class="hlt">current</span> quality of molybdenum has become so small that surface sensitivemore » techniques are not applicable anymore. Therefore, the atom probe, which allows the detection of small amounts of impurities as well as their location, seems to be a more suitable technique. However, a site-specific specimen preparation procedure for grain <span class="hlt">boundaries</span> in refractory metals with a dual focused ion beam/scanning electron microscope is still required. The present investigation describes the development and successful application of such a site-specific preparation technique for grain <span class="hlt">boundaries</span> in molybdenum, which is significantly improved by a combination with transmission electron microscopy. This complimentary technique helps to improve the visibility of grain <span class="hlt">boundaries</span> during the last preparation steps and to evidence the presence of grain and subgrain <span class="hlt">boundaries</span> without segregants in atom probe specimens. Furthermore, in industrially processed and recrystallized molybdenum sheets grain <span class="hlt">boundary</span> segregation of oxygen, nitrogen and potassium is successfully detected close to segregated regions which are believed to be former sinter pores. - Highlights: • First study of grain <span class="hlt">boundary</span> segregation in molybdenum by atom probe • Site-specific preparation technique by FIB and TEM successfully developed • Grain <span class="hlt">boundary</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJWC.17507004B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJWC.17507004B"><span>Thermal Simulations, Open <span class="hlt">Boundary</span> Conditions and Switches</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burnier, Yannis; Florio, Adrien; Kaczmarek, Olaf; Mazur, Lukas</p> <p>2018-03-01</p> <p>SU(N) gauge theories on compact spaces have a non-trivial vacuum structure characterized by a countable set of topological sectors and their topological charge. In lattice simulations, every topological sector needs to be explored a number of times which reflects its weight in the path integral. <span class="hlt">Current</span> lattice simulations are impeded by the so-called freezing of the topological charge problem. As the continuum is approached, energy barriers between topological sectors become well defined and the simulations get trapped in a given sector. A possible way out was introduced by Lüscher and Schaefer using open <span class="hlt">boundary</span> condition in the time extent. However, this solution cannot be used for thermal simulations, where the time direction is required to be periodic. In this proceedings, we present results obtained using open <span class="hlt">boundary</span> conditions in space, at non-zero temperature. With these conditions, the topological charge is not quantized and the topological barriers are lifted. A downside of this method are the strong finite-size effects introduced by the <span class="hlt">boundary</span> conditions. We also present some exploratory results which show how these conditions could be used on an algorithmic level to reshuffle the system and generate periodic configurations with non-zero topological charge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010IJC....83.1287T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010IJC....83.1287T"><span>Adaptive <span class="hlt">boundary</span> concentration control using Zakai equation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tenno, R.; Mendelson, A.</p> <p>2010-06-01</p> <p>A mean-variance control problem is formulated with respect to a partially observed nonlinear system that includes unknown constant parameters. A physical prototype of the system is the cathode surface reaction in an electrolysis cell, where the controller aim is to keep the <span class="hlt">boundary</span> concentration of species in the near vicinity of the cathode surface low but not zero. The <span class="hlt">boundary</span> concentration is a diffusion-controlled process observed through the measured <span class="hlt">current</span> density and, in practice, controlled through the applied voltage. The former incomplete data control problem is converted to complete data-to the so-called separated control problem whose solution is given by the infinite-dimensional Zakai equation. In this article, the separated control problem is solved numerically using pathwise integration of the Zakai equation. This article demonstrates precise tracking of the target trajectory with a rapid convergence of estimates to unknown parameters, which take place simultaneously with control.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5379487','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5379487"><span>Atomic structure and electronic properties of MgO grain <span class="hlt">boundaries</span> in tunnelling magnetoresistive devices</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bean, Jonathan J.; Saito, Mitsuhiro; Fukami, Shunsuke; Sato, Hideo; Ikeda, Shoji; Ohno, Hideo; Ikuhara, Yuichi; McKenna, Keith P.</p> <p>2017-01-01</p> <p>Polycrystalline metal oxides find diverse applications in areas such as nanoelectronics, photovoltaics and catalysis. Although grain <span class="hlt">boundary</span> defects are ubiquitous their structure and electronic properties are very poorly understood since it is extremely challenging to probe the structure of buried interfaces directly. In this paper we combine novel plan-view high-resolution transmission electron microscopy and first principles calculations to provide atomic level understanding of the structure and properties of grain <span class="hlt">boundaries</span> in the barrier layer of a magnetic tunnel junction. We show that the highly [001] textured MgO films contain numerous tilt grain <span class="hlt">boundaries</span>. First principles calculations reveal how these grain <span class="hlt">boundaries</span> are associated with locally reduced band gaps (by up to 3 eV). Using a simple model we show how shunting a proportion of the tunnelling <span class="hlt">current</span> through grain <span class="hlt">boundaries</span> imposes limits on the maximum magnetoresistance that can be achieved in devices. PMID:28374755</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGP32A..07Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGP32A..07Z"><span>Sharp <span class="hlt">Boundary</span> Inversion of 2D Magnetotelluric Data using Bayesian Method.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhou, S.; Huang, Q.</p> <p>2017-12-01</p> <p>Normally magnetotelluric(MT) inversion method cannot show the distribution of underground resistivity with clear <span class="hlt">boundary</span>, even if there are obviously different blocks. Aiming to solve this problem, we develop a Bayesian structure to inverse 2D MT sharp <span class="hlt">boundary</span> data, using <span class="hlt">boundary</span> location and inside resistivity as the random variables. Firstly, we use other MT inversion results, like ModEM, to analyze the resistivity distribution roughly. Then, we select the suitable random variables and change its data format to traditional staggered grid parameters, which can be used to do finite difference forward part. <span class="hlt">Finally</span>, we can shape the posterior probability density(PPD), which contains all the prior information and model-data correlation, by Markov Chain Monte Carlo(MCMC) sampling from prior distribution. The depth, resistivity and their uncertainty can be valued. It also works for sensibility estimation. We applied the method to a synthetic case, which composes two large abnormal blocks in a trivial background. We consider the <span class="hlt">boundary</span> smooth and the near true model weight constrains that mimic joint inversion or constrained inversion, then we find that the model results a more precise and focused depth distribution. And we also test the inversion without constrains and find that the <span class="hlt">boundary</span> could also be figured, though not as well. Both inversions have a good valuation of resistivity. The constrained result has a lower root mean square than ModEM inversion result. The data sensibility obtained via PPD shows that the resistivity is the most sensible, center depth comes second and both sides are the worst.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..MARW25005A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..MARW25005A"><span>Theoretical analysis of shock induced depolarization and <span class="hlt">current</span> generation in ferroelectrics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Agrawal, Vinamra; Bhattacharya, Kaushik</p> <p></p> <p>Ferroelectric generators are used to generate large magnitude <span class="hlt">current</span> pulse by impacting a polarized ferroelectric material. The impact causes depolarization of the material and at high impact speeds, dielectric breakdown. Depending on the loading conditions and the electromechanical <span class="hlt">boundary</span> conditions, the <span class="hlt">current</span> or voltage profiles obtained vary. In this study, we explore the large deformation dynamic response of a ferroelectric material. Using the Maxwell's equations, conservation laws and the second law of thermodynamics, we derive the governing equations for the phase <span class="hlt">boundary</span> propagation as well as the driving force acting on it. We allow for the phase <span class="hlt">boundary</span> to contain surface charges which introduces the contribution of curvature of phase <span class="hlt">boundary</span> in the governing equations and the driving force. This type of analysis accounts for the dielectric breakdown and resulting conduction in the material. Next, we implement the equations derived to solve a one dimensional impact problem on a ferroelectric material under different electrical <span class="hlt">boundary</span> conditions. The constitutive law is chosen to be piecewise quadratic in polarization and quadratic in the strain. We solve for the <span class="hlt">current</span> profile generated in short circuit case and for voltage profile in open circuited case. This work was made possible by the financial support of the US Air Force Office of Scientific Research through the Center of Excellence in High Rate Deformation Physics of Heterogeneous Materials (Grant: FA 9550-12-1-0091).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1358546-boundaries-mirror-symmetry-symplectic-duality-gauge-theory','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1358546-boundaries-mirror-symmetry-symplectic-duality-gauge-theory"><span><span class="hlt">Boundaries</span>, mirror symmetry, and symplectic duality in 3d N = 4 gauge theory</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Bullimore, Mathew; Dimofte, Tudor; Gaiotto, Davide; ...</p> <p>2016-10-20</p> <p>We introduce several families of N = (2, 2) UV <span class="hlt">boundary</span> conditions in 3d N=4 gauge theories and study their IR images in sigma-models to the Higgs and Coulomb branches. In the presence of Omega deformations, a UV <span class="hlt">boundary</span> condition defines a pair of modules for quantized algebras of chiral Higgs- and Coulomb-branch operators, respectively, whose structure we derive. In the case of abelian theories, we use the formalism of hyperplane arrangements to make our constructions very explicit, and construct a half-BPS interface that implements the action of 3d mirror symmetry on gauge theories and <span class="hlt">boundary</span> conditions. <span class="hlt">Finally</span>, by studyingmore » two-dimensional compactifications of 3d N = 4 gauge theories and their <span class="hlt">boundary</span> conditions, we propose a physical origin for symplectic duality $-$ an equivalence of categories of modules associated to families of Higgs and Coulomb branches that has recently appeared in the mathematics literature, and generalizes classic results on Koszul duality in geometric representation theory. We make several predictions about the structure of symplectic duality, and identify Koszul duality as a special case of wall crossing.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JPhCS.555a2071M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JPhCS.555a2071M"><span>Simulation of a 5MW wind turbine in an atmospheric <span class="hlt">boundary</span> layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Meister, Konrad; Lutz, Thorsten; Krämer, Ewald</p> <p>2014-12-01</p> <p>This article presents detached eddy simulation (DES) results of a 5MW wind turbine in an unsteady atmospheric <span class="hlt">boundary</span> layer. The evaluation performed in this article focuses on turbine blade loads as well as on the influence of atmospheric turbulence and tower on blade loads. Therefore, the turbulence transport of the atmospheric <span class="hlt">boundary</span> layer to the turbine position is analyzed. To determine the influence of atmospheric turbulence on wind turbines the blade load spectrum is evaluated and compared to wind turbine simulation results with uniform inflow. Moreover, the influences of different frequency regimes and the tower on the blade loads are discussed. <span class="hlt">Finally</span>, the normal force coefficient spectrum is analyzed at three different radial positions and the influence of tower and atmospheric turbulence is shown.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740002724','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740002724"><span><span class="hlt">Boundary</span>-integral methods in elasticity and plasticity. [solutions of <span class="hlt">boundary</span> value problems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mendelson, A.</p> <p>1973-01-01</p> <p>Recently developed methods that use <span class="hlt">boundary</span>-integral equations applied to elastic and elastoplastic <span class="hlt">boundary</span> value problems are reviewed. Direct, indirect, and semidirect methods using potential functions, stress functions, and displacement functions are described. Examples of the use of these methods for torsion problems, plane problems, and three-dimensional problems are given. It is concluded that the <span class="hlt">boundary</span>-integral methods represent a powerful tool for the solution of elastic and elastoplastic problems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JSP...167.1112B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JSP...167.1112B"><span>Exclusion Process with Slow <span class="hlt">Boundary</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baldasso, Rangel; Menezes, Otávio; Neumann, Adriana; Souza, Rafael R.</p> <p>2017-06-01</p> <p>We study the hydrodynamic and the hydrostatic behavior of the simple symmetric exclusion process with slow <span class="hlt">boundary</span>. The term slow <span class="hlt">boundary</span> means that particles can be born or die at the <span class="hlt">boundary</span> sites, at a rate proportional to N^{-θ }, where θ > 0 and N is the scaling parameter. In the bulk, the particles exchange rate is equal to 1. In the hydrostatic scenario, we obtain three different linear profiles, depending on the value of the parameter θ ; in the hydrodynamic scenario, we obtain that the time evolution of the spatial density of particles, in the diffusive scaling, is given by the weak solution of the heat equation, with <span class="hlt">boundary</span> conditions that depend on θ . If θ \\in (0,1), we get Dirichlet <span class="hlt">boundary</span> conditions, (which is the same behavior if θ =0, see Farfán in Hydrostatics, statical and dynamical large deviations of <span class="hlt">boundary</span> driven gradient symmetric exclusion processes, 2008); if θ =1, we get Robin <span class="hlt">boundary</span> conditions; and, if θ \\in (1,∞), we get Neumann <span class="hlt">boundary</span> conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030016586&hterms=flame+length&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dflame%2Blength','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030016586&hterms=flame+length&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dflame%2Blength"><span>Flame and Soot <span class="hlt">Boundaries</span> of Laminar Jet Diffusion Flames. Appendix A</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Xu, F.; Dai, Z.; Faeth, G. M.; Yuan, Z.-G. (Technical Monitor); Urban, D. L. (Technical Monitor); Yuan, Z.-G. (Technical Monitor)</p> <p>2002-01-01</p> <p>The shapes (flame-sheet and luminous-flame <span class="hlt">boundaries</span>) or steady weakly buoyant round hydrocarbon-fueled laminar-jet diffusion flames in still and coflowing air were studied both experimentally and theoretically. Flame-sheet shapes were measured from photographs using a CH optical filter to distinguish flame-sheet <span class="hlt">boundaries</span> in the presence of blue CO2 and OH emissions and yellow continuum radiation from soot. Present experimental conditions included acetylene-, methane-, propane-, and ethylene-fueled flames having initial reactant temperatures of 300 K. ambient pressures of 4-50 kPa, jet-exit Reynolds numbers of 3-54, initial air/fuel velocity ratios of 0-9, and luminous flame lengths of 5-55 mm; earlier measurements for propylene- and 1,3-butadiene-fueled flames for similar conditions were considered as well. Nonbuoyant flames in still air were observed at microgravity conditions; essentially nonbuoyant flames in coflowing air were observed at small pressures to control effects of buoyancy. Predictions of luminous flame <span class="hlt">boundaries</span> from soot luminosity were limited to laminar smoke-point conditions, whereas predictions of flame-sheet <span class="hlt">boundaries</span> ranged from soot-free to smoke-point conditions. Flame-shape predictions were based on simplified analyses using the <span class="hlt">boundary</span>-layer approximations along with empirical parameters to distinguish flame-sheet and luminous-flame (at the laminar smoke point) <span class="hlt">boundaries</span>. The comparison between measurements and predictions was remarkably good and showed that both flame-sheet and luminous-flame lengths are primarily controlled by fuel flow rates with lengths in coflowing air approaching 2/3 of the lengths in still air as coflowing air velocities are increased. <span class="hlt">Finally</span>, luminous flame lengths at laminar smoke-point conditions were roughly twice as long as flame-sheet lengths at comparable conditions because of the presence of luminous soot particles in the fuel-lean region of the flames.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123.1260N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123.1260N"><span>Multiscale <span class="hlt">Currents</span> Observed by MMS in the Flow Braking Region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nakamura, Rumi; Varsani, Ali; Genestreti, Kevin J.; Le Contel, Olivier; Nakamura, Takuma; Baumjohann, Wolfgang; Nagai, Tsugunobu; Artemyev, Anton; Birn, Joachim; Sergeev, Victor A.; Apatenkov, Sergey; Ergun, Robert E.; Fuselier, Stephen A.; Gershman, Daniel J.; Giles, Barbara J.; Khotyaintsev, Yuri V.; Lindqvist, Per-Arne; Magnes, Werner; Mauk, Barry; Petrukovich, Anatoli; Russell, Christopher T.; Stawarz, Julia; Strangeway, Robert J.; Anderson, Brian; Burch, James L.; Bromund, Ken R.; Cohen, Ian; Fischer, David; Jaynes, Allison; Kepko, Laurence; Le, Guan; Plaschke, Ferdinand; Reeves, Geoff; Singer, Howard J.; Slavin, James A.; Torbert, Roy B.; Turner, Drew L.</p> <p>2018-02-01</p> <p>We present characteristics of <span class="hlt">current</span> layers in the off-equatorial near-Earth plasma sheet <span class="hlt">boundary</span> observed with high time-resolution measurements from the Magnetospheric Multiscale mission during an intense substorm associated with multiple dipolarizations. The four Magnetospheric Multiscale spacecraft, separated by distances of about 50 km, were located in the southern hemisphere in the dusk portion of a substorm <span class="hlt">current</span> wedge. They observed fast flow disturbances (up to about 500 km/s), most intense in the dawn-dusk direction. Field-aligned <span class="hlt">currents</span> were observed initially within the expanding plasma sheet, where the flow and field disturbances showed the distinct pattern expected in the braking region of localized flows. Subsequently, intense thin field-aligned <span class="hlt">current</span> layers were detected at the inner <span class="hlt">boundary</span> of equatorward moving flux tubes together with Earthward streaming hot ions. Intense Hall <span class="hlt">current</span> layers were found adjacent to the field-aligned <span class="hlt">currents</span>. In particular, we found a Hall <span class="hlt">current</span> structure in the vicinity of the Earthward streaming ion jet that consisted of mixed ion components, that is, hot unmagnetized ions, cold E × B drifting ions, and magnetized electrons. Our observations show that both the near-Earth plasma jet diversion and the thin Hall <span class="hlt">current</span> layers formed around the reconnection jet <span class="hlt">boundary</span> are the sites where diversion of the perpendicular <span class="hlt">currents</span> take place that contribute to the observed field-aligned <span class="hlt">current</span> pattern as predicted by simulations of reconnection jets. Hence, multiscale structure of flow braking is preserved in the field-aligned <span class="hlt">currents</span> in the off-equatorial plasma sheet and is also translated to ionosphere to become a part of the substorm field-aligned <span class="hlt">current</span> system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29938154','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29938154"><span>Multiscale <span class="hlt">Currents</span> Observed by MMS in the Flow Braking Region.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nakamura, Rumi; Varsani, Ali; Genestreti, Kevin J; Le Contel, Olivier; Nakamura, Takuma; Baumjohann, Wolfgang; Nagai, Tsugunobu; Artemyev, Anton; Birn, Joachim; Sergeev, Victor A; Apatenkov, Sergey; Ergun, Robert E; Fuselier, Stephen A; Gershman, Daniel J; Giles, Barbara J; Khotyaintsev, Yuri V; Lindqvist, Per-Arne; Magnes, Werner; Mauk, Barry; Petrukovich, Anatoli; Russell, Christopher T; Stawarz, Julia; Strangeway, Robert J; Anderson, Brian; Burch, James L; Bromund, Ken R; Cohen, Ian; Fischer, David; Jaynes, Allison; Kepko, Laurence; Le, Guan; Plaschke, Ferdinand; Reeves, Geoff; Singer, Howard J; Slavin, James A; Torbert, Roy B; Turner, Drew L</p> <p>2018-02-01</p> <p>We present characteristics of <span class="hlt">current</span> layers in the off-equatorial near-Earth plasma sheet <span class="hlt">boundary</span> observed with high time-resolution measurements from the Magnetospheric Multiscale mission during an intense substorm associated with multiple dipolarizations. The four Magnetospheric Multiscale spacecraft, separated by distances of about 50 km, were located in the southern hemisphere in the dusk portion of a substorm <span class="hlt">current</span> wedge. They observed fast flow disturbances (up to about 500 km/s), most intense in the dawn-dusk direction. Field-aligned <span class="hlt">currents</span> were observed initially within the expanding plasma sheet, where the flow and field disturbances showed the distinct pattern expected in the braking region of localized flows. Subsequently, intense thin field-aligned <span class="hlt">current</span> layers were detected at the inner <span class="hlt">boundary</span> of equatorward moving flux tubes together with Earthward streaming hot ions. Intense Hall <span class="hlt">current</span> layers were found adjacent to the field-aligned <span class="hlt">currents</span>. In particular, we found a Hall <span class="hlt">current</span> structure in the vicinity of the Earthward streaming ion jet that consisted of mixed ion components, that is, hot unmagnetized ions, cold E × B drifting ions, and magnetized electrons. Our observations show that both the near-Earth plasma jet diversion and the thin Hall <span class="hlt">current</span> layers formed around the reconnection jet <span class="hlt">boundary</span> are the sites where diversion of the perpendicular <span class="hlt">currents</span> take place that contribute to the observed field-aligned <span class="hlt">current</span> pattern as predicted by simulations of reconnection jets. Hence, multiscale structure of flow braking is preserved in the field-aligned <span class="hlt">currents</span> in the off-equatorial plasma sheet and is also translated to ionosphere to become a part of the substorm field-aligned <span class="hlt">current</span> system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=ethnography&pg=7&id=EJ1027822','ERIC'); return false;" href="https://eric.ed.gov/?q=ethnography&pg=7&id=EJ1027822"><span>Symbolic <span class="hlt">Boundary</span> Work in Schools: Demarcating and Denying Ethnic <span class="hlt">Boundaries</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>Tabib-Calif, Yosepha; Lomsky-Feder, Edna</p> <p>2014-01-01</p> <p>This article examines the symbolic <span class="hlt">boundary</span> work that is carried out at a school whose student population is heterogeneous in terms of ethnicity and class. Based on ethnography, the article demonstrates how the school's staff seeks to neutralize ethnic <span class="hlt">boundaries</span> and their accompanying discourse, while the pupils try to bring ethnic…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhDT........50A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhDT........50A"><span>Teleseismic Array Studies of Earth's Core-Mantle <span class="hlt">Boundary</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alexandrakis, Catherine</p> <p>2011-12-01</p> <p>The core mantle <span class="hlt">boundary</span> (CMB) is an inaccessible and complex region, knowledge of which is vital to our understanding of many Earth processes. Above it is the heterogeneous lower-mantle. Below the <span class="hlt">boundary</span> is the outer-core, composed of liquid iron, and/or nickel and some lighter elements. Elucidation of how these two distinct layers interact may enable researchers to better understand the geodynamo, global tectonics, and overall Earth history. One parameter that can be used to study structure and limit potential chemical compositions is seismic-wave velocity. <span class="hlt">Current</span> global-velocity models have significant uncertainties in the 200 km above and below the CMB. In this thesis, these regions are studied using three methods. The upper outer core is studied using two seismic array methods. First, a modified vespa, or slant-stack method is applied to seismic observations at broadband seismic arrays, and at large, dense groups of broadband seismic stations dubbed 'virtual' arrays. Observations of core-refracted teleseismic waves, such as SmKS, are used to extract relative arrivaltimes. As with previous studies, lower -mantle heterogeneities influence the extracted arrivaltimes, giving significant scatter. To remove raypath effects, a new method was developed, called Empirical Transfer Functions (ETFs). When applied to SmKS waves, this method effectively isolates arrivaltime perturbations caused by outer core velocities. By removing raypath effects, the signals can be stacked further reducing scatter. The results of this work were published as a new 1D outer-core model, called AE09. This model describes a well-mixed outer core. Two array methods are used to detect lower mantle heterogeneities, in particular Ultra-Low Velocity Zones (ULVZs). The ETF method and beam forming are used to isolate a weak P-wave that diffracts along the CMB. While neither the ETF method nor beam forming could adequately image the low-amplitude phase, beam forms of two events indicate precursors</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27468309','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27468309"><span>Applying gene flow science to environmental policy needs: a <span class="hlt">boundary</span> work perspective.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ridley, Caroline E; Alexander, Laurie C</p> <p>2016-08-01</p> <p>One application of gene flow science is the policy arena. In this article, we describe two examples in which the topic of gene flow has entered into the U.S. national environmental policymaking process: regulation of genetically engineered crops and clarification of the jurisdictional scope of the Clean Water Act. We summarize both <span class="hlt">current</span> scientific understanding and the legal context within which gene flow science has relevance. We also discuss the process by which scientific knowledge has been synthesized and communicated to decision-makers in these two contexts utilizing the concept of '<span class="hlt">boundary</span> work'. <span class="hlt">Boundary</span> organizations, the work they engage in to bridge the worlds of science, policy, and practice, and the <span class="hlt">boundary</span> objects they produce to translate scientific knowledge existed in both examples. However, the specific activities and attributes of the objects produced varied based on the needs of the decision-makers. We close with suggestions for how scientists can contribute to or engage in <span class="hlt">boundary</span> work with policymakers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.S21A2369M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.S21A2369M"><span>The Plate <span class="hlt">Boundary</span> Observatory: <span class="hlt">Current</span> status and plans for the next five years</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mattioli, G. S.; Feaux, K.; Meertens, C. M.; Mencin, D.; Miller, M.</p> <p>2013-12-01</p> <p>UNAVCO <span class="hlt">currently</span> operates and maintains the NSF-funded Plate <span class="hlt">Boundary</span> Observatory (PBO), which is the geodetic facility of EarthScope. PBO was designed and built from 2003 to 2008 with $100M investment from the NSF Major Research Equipment and Facilities Construction (MREFC) Program. UNAVCO operated and maintained PBO under a Cooperative Agreement (CA) with NSF from 2008 to 2013 and will continue PBO O&M for the next five years as part of the new Geodesy Advancing Geosciences and EarthScope (GAGE) Facility. PBO is largest continuous GPS and borehole geophysical network in the Americas, with 1100 continuous Global Positioning System (cGPS) sites, including several with multiple monuments, 79 boreholes, with 75 tensor strainmeters, 78 short-period, 3-component seismometers, and pore pressure sensors at 23 sites. PBO also includes 26 tiltmeters deployed at volcanoes in Alaska, Mt St Helens, and Yellowstone caldera and 6 long-baseline laser strainmeters. Surface meteorological sensors are collocated at 154 GPS sites. UNAVCO provides high-rate (1 Hz), low-latency (<1 s) GPS data streams (RT-GPS) from 382 stations in PBO. UNAVCO has delivered over 62 Tb of geodetic data to the EarthScope community since its PBO's inception in 2004. Over the past year, data return for the cGPS component of PBO is 98%, well above the data return metric of 85% set by the NSF, a result of efforts to upgrade power systems and communications infrastructure. In addition, PBO has set the standard for the design, construction, and operation of other multi-hazard networks across the Americas, including COCONet in the Caribbean region and TLALOCNet in Mexico. Funding to support ongoing PBO O&M has declined from FY2012 CA levels under the new GAGE Facility. The implications for data return and data quality metrics as well as replacement of aging PBO GPS instruments with GNSS-compatible systems are as yet unknown. A process to assess the cost of specific PBO components, data rates, enhanced</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A51C2080Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A51C2080Y"><span><span class="hlt">Boundary</span>-layer diabatic processes, the virtual effect, and convective self-aggregation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, D.</p> <p>2017-12-01</p> <p>The atmosphere can self-organize into long-lasting large-scale overturning circulations over an ocean surface with uniform temperature. This phenomenon is referred to as convective self-aggregation and has been argued to be important for tropical weather and climate systems. Here we use a 1D shallow water model and a 2D cloud-resolving model (CRM) to show that <span class="hlt">boundary</span>-layer diabatic processes are essential for convective self-aggregation. We will show that <span class="hlt">boundary</span>-layer radiative cooling, convective heating, and surface buoyancy flux help convection self-aggregate because they generate available potential energy (APE), which sustains the overturning circulation. We will also show that evaporative cooling in the <span class="hlt">boundary</span> layer (cold pool) inhibits convective self-aggregation by reducing APE. Both the shallow water model and CRM results suggest that the enhanced virtual effect of water vapor can lead to convective self-aggregation, and this effect is mainly in the <span class="hlt">boundary</span> layer. This study proposes new dynamical feedbacks for convective self-aggregation and complements <span class="hlt">current</span> studies that focus on thermodynamic feedbacks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19740050642&hterms=green+theorem+show&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dgreen%2Btheorem%2Bshow','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19740050642&hterms=green+theorem+show&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dgreen%2Btheorem%2Bshow"><span>Use of Green's functions in the numerical solution of two-point <span class="hlt">boundary</span> value problems</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gallaher, L. J.; Perlin, I. E.</p> <p>1974-01-01</p> <p>This study investigates the use of Green's functions in the numerical solution of the two-point <span class="hlt">boundary</span> value problem. The first part deals with the role of the Green's function in solving both linear and nonlinear second order ordinary differential equations with <span class="hlt">boundary</span> conditions and systems of such equations. The second part describes procedures for numerical construction of Green's functions and considers briefly the conditions for their existence. <span class="hlt">Finally</span>, there is a description of some numerical experiments using nonlinear problems for which the known existence, uniqueness or convergence theorems do not apply. Examples here include some problems in finding rendezvous orbits of the restricted three body system.</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://www.ncbi.nlm.nih.gov/pubmed/25630390','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25630390"><span>Physical therapists' perceptions of sexual <span class="hlt">boundaries</span> in clinical practice in the United States.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Roush, Susan E; Cox, Kenneth; Garlick, John; Kane, Molly; Marchand, Lauren</p> <p>2015-07-01</p> <p>Physical therapists' perceptions of sexual <span class="hlt">boundaries</span> in clinic settings in the United States have not been studied. Given the magnitude of potential consequences of sexual <span class="hlt">boundary</span> violations, examination of this topic is imperative. The purpose of this study was to describe the perceptions of sexual <span class="hlt">boundaries</span> among licensed physical therapists in the United States. Licensed physical therapists from Arkansas, Kansas, Maine, Ohio, and Oregon were contacted by email and asked to complete a sexual <span class="hlt">boundaries</span> questionnaire via Survey Monkey™; 967 surveys (7.3%) were returned. While most physical therapists practice within the profession's Code of Ethics, there are practitioners who date <span class="hlt">current</span> and former patients, and condone patients' sexual banter in the clinic. Almost half (42%) of the participants acknowledged feeling sexually attracted to a patient. While gender differences were seen throughout the analyses, generally, the demographic and professional variables did not account for meaningful variance. Results were similar to previous research on physiotherapists in other countries. Sexuality is part of the physical therapy practice environment and physical therapists' understanding of sexual <span class="hlt">boundaries</span> is ambiguous. These data can inform professional conversation on sexual <span class="hlt">boundaries</span> in physical therapy practice leading to greater understanding and decreased potential for violations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRC..123.1016C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRC..123.1016C"><span>Nonlinear Dynamics of the Nearshore <span class="hlt">Boundary</span> Layer of a Large Lake (Lake Geneva)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cimatoribus, Andrea A.; Lemmin, U.; Bouffard, D.; Barry, D. A.</p> <p>2018-02-01</p> <p>We examine nearshore and pelagic <span class="hlt">current</span> variability in Lake Geneva, a large and deep lake in western Europe, using observations from several measurement locations and a three-dimensional numerical model for the period 2014-2016. Linear internal seiche modes excited by wind forcing clearly appear as peaks in the energy spectra for measurements in offshore locations. In contrast, spectra from the nearshore data, where <span class="hlt">currents</span> interact with the lake bed, reveal a negligible contribution of internal seiches to the total kinetic energy. A similar contrast is seen in the spectra obtained from the numerical model at the same locations. Comparing the contribution of the different terms in the vertically averaged momentum equation from the modeling results shows that the nonlinear advective term dominates in the nearshore <span class="hlt">boundary</span> layer. Its contribution decays with distance from shore. The width of this nearshore <span class="hlt">boundary</span> layer, which may extend for several kilometers, seems to be mainly determined by local topography. Both field measurements and modeling results indicate that nonlinear dynamics are of primary importance in the nearshore <span class="hlt">boundary</span> layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20180001494','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20180001494"><span>Reynolds-Stress Budgets in an Impinging Shock Wave/<span class="hlt">Boundary</span>-Layer Interaction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vyas, Manan A.; Yoder, Dennis A.; Gaitonde, Datta V.</p> <p>2018-01-01</p> <p>Implicit large-eddy simulation (ILES) of a shock wave/<span class="hlt">boundary</span>-layer interaction (SBLI) was performed. Comparisons with experimental data showed a sensitivity of the <span class="hlt">current</span> prediction to the modeling of the sidewalls. This was found to be common among various computational studies in the literature where periodic <span class="hlt">boundary</span> conditions were used in the spanwise direction, as was the case in the present work. Thus, although the experiment was quasi-two-dimensional, the present simulation was determined to be two-dimensional. Quantities present in the exact equation of the Reynolds-stress transport, i.e., production, molecular diffusion, turbulent transport, pressure diffusion, pressure strain, dissipation, and turbulent mass flux were calculated. Reynolds-stress budgets were compared with past large-eddy simulation and direct numerical simulation datasets in the undisturbed portion of the turbulent <span class="hlt">boundary</span> layer to validate the <span class="hlt">current</span> approach. The budgets in SBLI showed the growth in the production term for the primary normal stress and energy transfer mechanism was led by the pressure strain term in the secondary normal stresses. The pressure diffusion term, commonly assumed as negligible by turbulence model developers, was shown to be small but non-zero in the normal stress budgets, however it played a key role in the primary shear stress budget.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29566091','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29566091"><span>Food supply and bioenergy production within the global cropland planetary <span class="hlt">boundary</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Henry, R C; Engström, K; Olin, S; Alexander, P; Arneth, A; Rounsevell, M D A</p> <p>2018-01-01</p> <p>Supplying food for the anticipated global population of over 9 billion in 2050 under changing climate conditions is one of the major challenges of the 21st century. Agricultural expansion and intensification contributes to global environmental change and risks the long-term sustainability of the planet. It has been proposed that no more than 15% of the global ice-free land surface should be converted to cropland. Bioenergy production for land-based climate mitigation places additional pressure on limited land resources. Here we test normative targets of food supply and bioenergy production within the cropland planetary <span class="hlt">boundary</span> using a global land-use model. The results suggest supplying the global population with adequate food is possible without cropland expansion exceeding the planetary <span class="hlt">boundary</span>. Yet this requires an increase in food production, especially in developing countries, as well as a decrease in global crop yield gaps. However, under <span class="hlt">current</span> assumptions of future food requirements, it was not possible to also produce significant amounts of first generation bioenergy without cropland expansion. These results suggest that meeting food and bioenergy demands within the planetary <span class="hlt">boundaries</span> would need a shift away from <span class="hlt">current</span> trends, for example, requiring major change in the demand-side of the food system or advancing biotechnologies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5864037','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5864037"><span>Food supply and bioenergy production within the global cropland planetary <span class="hlt">boundary</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>Olin, S.; Alexander, P.; Arneth, A.; Rounsevell, M. D. A.</p> <p>2018-01-01</p> <p>Supplying food for the anticipated global population of over 9 billion in 2050 under changing climate conditions is one of the major challenges of the 21st century. Agricultural expansion and intensification contributes to global environmental change and risks the long-term sustainability of the planet. It has been proposed that no more than 15% of the global ice-free land surface should be converted to cropland. Bioenergy production for land-based climate mitigation places additional pressure on limited land resources. Here we test normative targets of food supply and bioenergy production within the cropland planetary <span class="hlt">boundary</span> using a global land-use model. The results suggest supplying the global population with adequate food is possible without cropland expansion exceeding the planetary <span class="hlt">boundary</span>. Yet this requires an increase in food production, especially in developing countries, as well as a decrease in global crop yield gaps. However, under <span class="hlt">current</span> assumptions of future food requirements, it was not possible to also produce significant amounts of first generation bioenergy without cropland expansion. These results suggest that meeting food and bioenergy demands within the planetary <span class="hlt">boundaries</span> would need a shift away from <span class="hlt">current</span> trends, for example, requiring major change in the demand-side of the food system or advancing biotechnologies. PMID:29566091</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29614841','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29614841"><span>Quantitative Detection of Cracks in Steel Using Eddy <span class="hlt">Current</span> Pulsed Thermography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shi, Zhanqun; Xu, Xiaoyu; Ma, Jiaojiao; Zhen, Dong; Zhang, Hao</p> <p>2018-04-02</p> <p>Small cracks are common defects in steel and often lead to catastrophic accidents in industrial applications. Various nondestructive testing methods have been investigated for crack detection; however, most <span class="hlt">current</span> methods focus on qualitative crack identification and image processing. In this study, eddy <span class="hlt">current</span> pulsed thermography (ECPT) was applied for quantitative crack detection based on derivative analysis of temperature variation. The effects of the incentive parameters on the temperature variation were analyzed in the simulation study. The crack profile and position are identified in the thermal image based on the Canny edge detection algorithm. Then, one or more trajectories are determined through the crack profile in order to determine the crack <span class="hlt">boundary</span> through its temperature distribution. The slope curve along the trajectory is obtained. <span class="hlt">Finally</span>, quantitative analysis of the crack sizes was performed by analyzing the features of the slope curves. The experimental verification showed that the crack sizes could be quantitatively detected with errors of less than 1%. Therefore, the proposed ECPT method was demonstrated to be a feasible and effective nondestructive approach for quantitative crack detection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvE..97d3305S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvE..97d3305S"><span>Choice of no-slip curved <span class="hlt">boundary</span> condition for lattice Boltzmann simulations of high-Reynolds-number flows</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sanjeevi, Sathish K. P.; Zarghami, Ahad; Padding, Johan T.</p> <p>2018-04-01</p> <p>Various curved no-slip <span class="hlt">boundary</span> conditions available in literature improve the accuracy of lattice Boltzmann simulations compared to the traditional staircase approximation of curved geometries. Usually, the required unknown distribution functions emerging from the solid nodes are computed based on the known distribution functions using interpolation or extrapolation schemes. On using such curved <span class="hlt">boundary</span> schemes, there will be mass loss or gain at each time step during the simulations, especially apparent at high Reynolds numbers, which is called mass leakage. Such an issue becomes severe in periodic flows, where the mass leakage accumulation would affect the computed flow fields over time. In this paper, we examine mass leakage of the most well-known curved <span class="hlt">boundary</span> treatments for high-Reynolds-number flows. Apart from the existing schemes, we also test different forced mass conservation schemes and a constant density scheme. The capability of each scheme is investigated and, <span class="hlt">finally</span>, recommendations for choosing a proper <span class="hlt">boundary</span> condition scheme are given for stable and accurate simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29758688','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29758688"><span>Choice of no-slip curved <span class="hlt">boundary</span> condition for lattice Boltzmann simulations of high-Reynolds-number flows.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sanjeevi, Sathish K P; Zarghami, Ahad; Padding, Johan T</p> <p>2018-04-01</p> <p>Various curved no-slip <span class="hlt">boundary</span> conditions available in literature improve the accuracy of lattice Boltzmann simulations compared to the traditional staircase approximation of curved geometries. Usually, the required unknown distribution functions emerging from the solid nodes are computed based on the known distribution functions using interpolation or extrapolation schemes. On using such curved <span class="hlt">boundary</span> schemes, there will be mass loss or gain at each time step during the simulations, especially apparent at high Reynolds numbers, which is called mass leakage. Such an issue becomes severe in periodic flows, where the mass leakage accumulation would affect the computed flow fields over time. In this paper, we examine mass leakage of the most well-known curved <span class="hlt">boundary</span> treatments for high-Reynolds-number flows. Apart from the existing schemes, we also test different forced mass conservation schemes and a constant density scheme. The capability of each scheme is investigated and, <span class="hlt">finally</span>, recommendations for choosing a proper <span class="hlt">boundary</span> condition scheme are given for stable and accurate simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhDT........38B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhDT........38B"><span>Relations and interactions between twinning and grain <span class="hlt">boundaries</span> in hexagonal close-packed structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barrett, Christopher Duncan</p> <p></p> <p>Improving the formability and crashworthiness of wrought magnesium alloys are the two biggest challenges in <span class="hlt">current</span> magnesium technology. Magnesium is the best material candidate for enabling required improvements in fuel economy of combustion engines and increases in ranges of electric vehicles. In hexagonal closed-packed (HCP) structures, effects of grain size/morphology and crystallographic texture are particularly important. Prior research has established a general understanding of the dependences of strength and strain anisotropy on grain morphology and texture. Unfortunately, deformation, recrystallization, and grain growth strategies that control the microstructures and textures of cubic metals and alloys have not generally worked for HCPs. For example, in Magnesium, the deformation texture induced by primary forming operations (rolling, extrusion, etc.) is not randomized by recrystallization and may strengthen during grain growth. A strong texture reduces formability during secondary forming (stamping, bending, hemming etc.) Thus, the inability to randomize texture has impeded the implementation of magnesium alloys in engineering applications. When rare earth solutes are added to magnesium alloys, distinct new textures are derived. However, `rare earth texture' derivation remains insufficiently explained. <span class="hlt">Currently</span>, it is hypothesized that unknown mechanisms of alloy processing are at work, arising from the effects of grain <span class="hlt">boundary</span> intrinsic defect structures on microstructural evolution. This dissertation is a comprehensive attempt to identify formal methodologies of analyzing the behavior of grain <span class="hlt">boundaries</span> in magnesium. We focus particularly on twin <span class="hlt">boundaries</span> and asymmetric tilt grain <span class="hlt">boundaries</span> using molecular dynamics. We begin by exploring twin nucleation in magnesium single crystals, elucidating effects of heterogeneities on twin nucleation and their relationships with concurrent slip. These efforts highlighted the necessity of imperfections to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750003114','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750003114"><span><span class="hlt">Boundary</span> layers in centrifugal compressors. [application of <span class="hlt">boundary</span> layer theory to compressor design</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Dean, R. C., Jr.</p> <p>1974-01-01</p> <p>The utility of <span class="hlt">boundary</span>-layer theory in the design of centrifugal compressors is demonstrated. <span class="hlt">Boundary</span>-layer development in the diffuser entry region is shown to be important to stage efficiency. The result of an earnest attempt to analyze this <span class="hlt">boundary</span> layer with the best tools available is displayed. Acceptable prediction accuracy was not achieved. The inaccuracy of <span class="hlt">boundary</span>-layer analysis in this case would result in stage efficiency prediction as much as four points low. Fluid dynamic reasons for analysis failure are discussed with support from flow data. Empirical correlations used today to circumnavigate the weakness of the theory are illustrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030068030','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030068030"><span>Evaluation of Flush-Mounted, S-Duct Inlets With Large Amounts of <span class="hlt">Boundary</span> Layer Ingestion</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Berrier, Bobby L.; Morehouse, Melissa B.</p> <p>2003-01-01</p> <p>A new high Reynolds number test capability for <span class="hlt">boundary</span> layer ingesting inlets has been developed for the NASA Langley Research Center 0.3-Meter Transonic Cryogenic Tunnel. Using this new capability, an experimental investigation of four S-duct inlet configurations with large amounts of <span class="hlt">boundary</span> layer ingestion (nominal <span class="hlt">boundary</span> layer thickness of about 40% of inlet height) was conducted at realistic operating conditions (high subsonic Mach numbers and full-scale Reynolds numbers). The objectives of this investigation were to 1) develop a new high Reynolds number, <span class="hlt">boundary</span>-layer ingesting inlet test capability, 2) evaluate the performance of several <span class="hlt">boundary</span> layer ingesting S-duct inlets, 3) provide a database for CFD tool validation, and 4) provide a baseline inlet for future inlet flow-control studies. Tests were conducted at Mach numbers from 0.25 to 0.83, Reynolds numbers (based on duct exit diameter) from 5.1 million to a fullscale value of 13.9 million, and inlet mass-flow ratios from 0.39 to 1.58 depending on Mach number. Results of this investigation indicate that inlet pressure recovery generally decreased and inlet distortion generally increased with increasing Mach number. Except at low Mach numbers, increasing inlet mass-flow increased pressure recovery and increased distortion. Increasing the amount of <span class="hlt">boundary</span> layer ingestion (by decreasing inlet throat height and increasing inlet throat width) or ingesting a <span class="hlt">boundary</span> layer with a distorted profile decreased pressure recovery and increased distortion. <span class="hlt">Finally</span>, increasing Reynolds number had almost no effect on inlet distortion but increased inlet recovery by about one-half percent at a Mach number near cruise.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhDT........20V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhDT........20V"><span>Tracking "Large" or "Smal": <span class="hlt">Boundaries</span> and their Consequences for Veterinary Students within the Tracking System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vermilya, Jenny R.</p> <p></p> <p>In this dissertation, I use 42 in-depth qualitative interviews with veterinary medical students to explore the experience of being in an educational program that tracks students based on the species of non-human animals that they wish to treat. Specifically, I examine how tracking produces multiple <span class="hlt">boundaries</span> for veterinary students. The <span class="hlt">boundaries</span> between different animal species produce consequences for the treatment of those animals; this has been well documented. Using a symbolic interactionist perspective, my research extends the body of knowledge on species <span class="hlt">boundaries</span> by revealing other consequences of this <span class="hlt">boundary</span> work. For example, I analyze the symbolic <span class="hlt">boundaries</span> involved in the gendering of animals, practitioners, and professions. I also examine how <span class="hlt">boundaries</span> influence the collective identity of students entering an occupation segmented into various specialties. The collective identity of veterinarian is one characterized by care, thus students have to construct different definitions of care to access and maintain the collective identity. The tracking system additionally produces consequences for the knowledge created and reproduced in different areas of animal medicine, creating a system of power and inequality based on whose knowledge is privileged, how, and why. <span class="hlt">Finally</span>, socially constructed <span class="hlt">boundaries</span> generated from tracking inevitably lead to cases that do not fit. In particular, horses serve as a "border species" for veterinary students who struggle to place them into the tracking system. I argue that border species, like other metaphorical borders, have the potential to challenge discourses and lead to social change.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PMag...97..867D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PMag...97..867D"><span>Grain <span class="hlt">boundary</span> engineering: fatigue fracture</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Das, Arpan</p> <p>2017-04-01</p> <p>Grain <span class="hlt">boundary</span> engineering has revealed significant enhancement of material properties by modifying the populations and connectivity of different types of grain <span class="hlt">boundaries</span> within the polycrystals. The character and connectivity of grain <span class="hlt">boundaries</span> in polycrystalline microstructures control the corrosion and mechanical behaviour of materials. A comprehensive review of the previous researches has been carried out to understand this philosophy. Present research thoroughly explores the effect of total strain amplitude on phase transformation, fatigue fracture features, grain size, annealing twinning, different grain connectivity and grain <span class="hlt">boundary</span> network after strain controlled low cycle fatigue deformation of austenitic stainless steel under ambient temperature. Electron backscatter diffraction technique has been used extensively to investigate the grain <span class="hlt">boundary</span> characteristics and morphologies. The nominal variation of strain amplitude through cyclic plastic deformation is quantitatively demonstrated completely in connection with the grain <span class="hlt">boundary</span> microstructure and fractographic features to reveal the mechanism of fatigue fracture of polycrystalline austenite. The extent of <span class="hlt">boundary</span> modifications has been found to be a function of the number of applied loading cycles and strain amplitudes. It is also investigated that cyclic plasticity induced martensitic transformation strongly influences grain <span class="hlt">boundary</span> characteristics and modifications of the material's microstructure/microtexture as a function of strain amplitudes. The experimental results presented here suggest a path to grain <span class="hlt">boundary</span> engineering during fatigue fracture of austenite polycrystals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DFDR39001P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DFDR39001P"><span>Microscopic suspension feeders near <span class="hlt">boundaries</span>: Effects of external water flow</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pepper, Rachel; Koehl, M. A. R.</p> <p>2015-11-01</p> <p>Microscopic sessile suspension feeders are an important part of aquatic ecosystems and form a vital link in the transfer of carbon in aquatic food webs. These suspension feeders live attached to <span class="hlt">boundaries</span>, consume bacteria and small detritus, and are in turn eaten by larger organisms. Many create a feeding <span class="hlt">current</span> that draws fluid towards them, and from which they filter their food. In still water, the feeding <span class="hlt">current</span> consists of recirculating eddies which form as a result of fluid forcing near a <span class="hlt">boundary</span>. These recirculating eddies can be depleted of food and significantly decrease nutrient uptake; a variety of strategies have been proposed for how attached feeders increase their access to undepleted water. We investigate the interaction of the flow produced by a microscopic suspension feeder with external environmental flow, such as the <span class="hlt">current</span> in a stream or ocean. We show through calculations that even very slow flow (on the order of microns per second) is sufficient to provide a constant supply of undepleted water to suspension feeders when the feeders are modeled with perfect nutrient capture efficiency and in the absence of diffusion. We also discuss which natural flow environments exceed the threshold to supply undepleted water and which do not, and we examine how characteristics of the suspension feeders themselves, such as stalk length and feeding disk size, influence feeding <span class="hlt">currents</span> and their interactions with external flows.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1184531','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1184531"><span>Enhancing critical <span class="hlt">current</span> density of cuprate superconductors</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Chaudhari, Praveen</p> <p>2015-06-16</p> <p>The present invention concerns the enhancement of critical <span class="hlt">current</span> densities in cuprate superconductors. Such enhancement of critical <span class="hlt">current</span> densities include using wave function symmetry and restricting movement of Abrikosov (A) vortices, Josephson (J) vortices, or Abrikosov-Josephson (A-J) vortices by using the half integer vortices associated with d-wave symmetry present in the grain <span class="hlt">boundary</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAP...123e5705A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123e5705A"><span>Recombination activity of grain <span class="hlt">boundaries</span> in high-performance multicrystalline Si during solar cell processing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Adamczyk, Krzysztof; Søndenâ, Rune; Stokkan, Gaute; Looney, Erin; Jensen, Mallory; Lai, Barry; Rinio, Markus; Di Sabatino, Marisa</p> <p>2018-02-01</p> <p>In this work, we applied internal quantum efficiency mapping to study the recombination activity of grain <span class="hlt">boundaries</span> in High Performance Multicrystalline Silicon under different processing conditions. Wafers were divided into groups and underwent different thermal processing, consisting of phosphorus diffusion gettering and surface passivation with hydrogen rich layers. After these thermal treatments, wafers were processed into heterojunction with intrinsic thin layer solar cells. Light Beam Induced <span class="hlt">Current</span> and Electron Backscatter Diffraction were applied to analyse the influence of thermal treatment during standard solar cell processing on different types of grain <span class="hlt">boundaries</span>. The results show that after cell processing, most random-angle grain <span class="hlt">boundaries</span> in the material are well passivated, but small-angle grain <span class="hlt">boundaries</span> are not well passivated. Special cases of coincidence site lattice grain <span class="hlt">boundaries</span> with high recombination activity are also found. Based on micro-X-ray fluorescence measurements, a change in the contamination level is suggested as the reason behind their increased activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70025828','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70025828"><span>A classification of ecological <span class="hlt">boundaries</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>Strayer, D.L.; Power, M.E.; Fagan, W.F.; Pickett, S.T.A.; Belnap, J.</p> <p>2003-01-01</p> <p>Ecologists use the term <span class="hlt">boundary</span> to refer to a wide range of real and conceptual structures. Because imprecise terminology may impede the search for general patterns and theories about ecological <span class="hlt">boundaries</span>, we present a classification of the attributes of ecological <span class="hlt">boundaries</span> to aid in communication and theory development. Ecological <span class="hlt">boundaries</span> may differ in their origin and maintenance, their spatial structure, their function, and their temporal dynamics. A classification system based on these attributes should help ecologists determine whether <span class="hlt">boundaries</span> are truly comparable. This system can be applied when comparing empirical studies, comparing theories, and testing theoretical predictions against empirical results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1261511-visualization-current-mapping-elements-quantum-dot-solar-cells','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1261511-visualization-current-mapping-elements-quantum-dot-solar-cells"><span>Visualization of <span class="hlt">Current</span> and Mapping of Elements in Quantum Dot Solar Cells</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Niezgoda, J. Scott; Ng, Amy; Poplawsky, Jonathan D.; ...</p> <p>2015-12-17</p> <p>The delicate influence of properties such as high surface state density and organic-inorganic <span class="hlt">boundaries</span> on the individual quantum dot electronic structure complicates pursuits toward forming quantitative models of quantum dot thin films ab initio. Our report describes the application of electron beam-induced <span class="hlt">current</span> (EBIC) microscopy to depleted-heterojunction colloidal quantum dot photovoltaics (DH-CQD PVs), a technique which affords one a map of <span class="hlt">current</span> production within the active layer of a PV device. The effects of QD sample size polydispersity as well as layer thickness in CQD active layers as they pertain to <span class="hlt">current</span> production within these PVs are imaged and explained.more » The results from these experiments compare well with previous estimations, and confirm the ability of EBIC to function as a valuable empirical tool for the design and betterment of DH-CQD PVs. Lastly, extensive and unexpected PbS QD penetration into the mesoporous TiO 2 layer is observed through imaging of device cross sections by energy-dispersive X-ray spectroscopy combined with scanning transmission electron microscopy. <span class="hlt">Finally</span>, the effects of this finding are discussed and corroborated with the EBIC studies on similar devices.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100025028','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100025028"><span>High-Speed <span class="hlt">Boundary</span>-Layer Transition Induced by an Isolated Roughness Element</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kegerise, Michael A.; Owens, Lewis R.; King, Rudolph A.</p> <p>2010-01-01</p> <p>Progress on an experimental effort to quantify the instability mechanisms associated with roughness-induced transition in a high-speed <span class="hlt">boundary</span> layer is reported in this paper. To simulate the low-disturbance environment encountered during high-altitude flight, the experimental study was performed in the NASA-Langley Mach 3.5 Supersonic Low-Disturbance Tunnel. A flat plate trip sizing study was performed first to identify the roughness height required to force transition. That study, which included transition onset measurements under both quiet and noisy freestream conditions, confirmed the sensitivity of roughness-induced transition to freestream disturbance levels. Surveys of the laminar <span class="hlt">boundary</span> layer on a 7deg half-angle sharp-tipped cone were performed via hot-wire anemometry and pitot-pressure measurements. The measured mean mass-flux and Mach-number profiles agreed very well with computed mean-flow profiles. <span class="hlt">Finally</span>, surveys of the <span class="hlt">boundary</span> layer developing downstream of an isolated roughness element on the cone were performed. The measurements revealed an instability in the far wake of the roughness element that grows exponentially and has peak frequencies in the 150 to 250 kHz range.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19970022794&hterms=heinemann&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dheinemann','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19970022794&hterms=heinemann&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dheinemann"><span>Inertial <span class="hlt">Currents</span> in Isotropic Plasma</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heinemann, M.; Erickson, G. M.; Pontius, D. H., Jr.</p> <p>1993-01-01</p> <p>The magnetospheric convection electric field contributes to Birkeland <span class="hlt">currents</span>. The effects of the field are to polarize the plasma by displacing the bounce paths of the ions from those of electrons, to redistribute the pressure so that it is not constant along magnetic field lines, and to enhance the pressure gradient by the gradient of the bulk speed. Changes in the polarization charge during the convection of the plasma are neutralized by electrons in the form of field-aligned <span class="hlt">currents</span> that close through the ionosphere. The pressure drives field-aligned <span class="hlt">currents</span> through its gradient in the same manner as in quasi-static plasma, but with modifications that are important if the bulk speed is of the order of the ion thermal speed; the variations in the pressure along field lines are maintained by a weak parallel potential drop. These effects are described in terms of the field-aligned <span class="hlt">currents</span> in steady state, isotropic, MED plasma. Solutions are developed by taking the MHD limit of two-fluid solutions and illustrated in the special case of Maxwellian plasma for which the temperature is constant along magnetic field lines. The expression for the Birkeland <span class="hlt">current</span> density is a generalization of Vasyliunas' expression for the field-aligned <span class="hlt">current</span> density in quasi-static plasma and provides a unifying expression when both pressure gradients and ion inertia operate simultaneously as sources of field-aligned <span class="hlt">currents</span>. It contains a full account of different aspects of the ion flow (parallel and perpendicular velocity and vorticity) that contribute to the <span class="hlt">currents</span>. Contributions of ion inertia to field-aligned <span class="hlt">currents</span> will occur in regions of strong velocity shear, electric field reversal, or large gradients in the parallel velocity or number density, and may be important in the low-latitude <span class="hlt">boundary</span> layer, plasma sheet <span class="hlt">boundary</span> layer, and the inner edge region of the plasma sheet.</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('https://ntrs.nasa.gov/search.jsp?R=19950033422&hterms=heinemann&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dheinemann','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950033422&hterms=heinemann&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dheinemann"><span>Inertial <span class="hlt">currents</span> in isotropic plasma</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heinemann, M.; Erickson, G. M.; Pontius, D. H. JR.</p> <p>1994-01-01</p> <p>The magnetospheric convection electric field contributes to Birkeland <span class="hlt">currents</span>. The effects of the field are to polarize the plasma by displacing the bounce paths of the ions from those of electrons, to redistribute the pressure so that it is not constant along magnetic field lines, and to enhance the pressure gradient by the gradient of the bulk speed. Changes in the polarization charge during the convection of the plasma are neutralized by electrons in the form of field-aligned <span class="hlt">currents</span> that close through the ionosphere. The pressure drives field-aligned <span class="hlt">currents</span> through its gradient in the same manner as in quasi-static plasma, but with modifications that are important if the bulk speed is of the order of the ion thermal speed; the variations in the pressure along field lines are maintained by a weak parallel potential drop. These effects are described in terms of the field-aligned <span class="hlt">currents</span> in steady state, isotropic, magnetohyrodynamic (MHD) plasma. Solutions are developed by taking the MHD limit of two-fluid solutions and illustrated in the special case of Maxwellian plasma for which the temperature is constant along magnetic field lines. The expression for the Birkeland <span class="hlt">current</span> density is a generalization of Vasyliunas' expression for the field-aligned <span class="hlt">current</span> density in quasi-static plasma and provides a unifying expression when both pressure gradients and ion inertia operate simultaneously as sources of field-aligned <span class="hlt">currents</span>. It contains a full account of different aspects of the ion flow (parallel and perpendicular velocity and vorticity) that contribute to the <span class="hlt">currents</span>. Contributions of ion inertia to field-aligned <span class="hlt">currents</span> will occur in regions of strong velocity shear, electric field reversal, or large gradients in the parallel velocity or number density, and may be important in the low-latitude <span class="hlt">boundary</span> layer, plasma sheet <span class="hlt">boundary</span> layer, and the inner edge region of the plasma sheet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960011455','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960011455"><span>Inertial <span class="hlt">currents</span> in isotropic plasma</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heinemann, M.; Erickson, G. M.; Pontius, D. H., Jr.</p> <p>1994-01-01</p> <p>The magnetospheric convection electric field contributes to Birkeland <span class="hlt">currents</span>. The effects of the field are to polarize the plasma by displacing the bounce paths of the ions from those of electrons, to redistribute the pressure so that it is not constant along magnetic field lines, and to enhance the pressure gradient by the gradient of the bulk speed. Changes in the polarization charge during the convection of the plasma are neutralized by electrons in the form of field-aligned <span class="hlt">currents</span> that close through the ionosphere. The pressure drives field-aligned <span class="hlt">currents</span> through its gradient in the same manner as in quasi-static plasmas, but with modifications that are important if the bulk speed is of the order of the ion thermal speed; the variations in the pressure along field lines are maintained by a weak parallel potential drop. These effects are described in terms of the field-aligned <span class="hlt">currents</span> in steady state, isotropic, MHD plasma. Solutions are developed by taking the MHD limit ot two-fluid solutions and illustrated in the special case of Maxwellian plasma for which the temperature is constant along magnetic field lines. The expression for the Birkeland <span class="hlt">current</span> density is a generalization of Vasyliunas' expression for the field-aligned <span class="hlt">current</span> density in quasi-static plasma and provides a unifying expression when both pressure gradients and ion inertia operate simultaneously as sources of field-aligned <span class="hlt">currents</span>. It contains a full account of different aspects of the ion flow (parallel and perpendicular velocity and vorticity) that contribute to the <span class="hlt">currents</span>. Contributions of ion inertia to field-aligned <span class="hlt">currents</span> will occur in regions of strong velocity shear, electric field reversal, or large gradients in the parallel velocity or number density, and may be important in the low-latitude <span class="hlt">boundary</span> layer, plasma sheet <span class="hlt">boundary</span> layer, and the inner edge region of the plasma sheet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1371710','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1371710"><span>Multi-region approach to free-<span class="hlt">boundary</span> three-dimensional tokamak equilibria and resistive wall instabilities</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>Ferraro, N. M.; Jardin, S. C.; Lao, L. L.</p> <p></p> <p>Free-<span class="hlt">boundary</span> 3D tokamak equilibria and resistive wall instabilities are calculated using a new resistive wall model in the two-fluid M3D-C1 code. In this model, the resistive wall and surround- ing vacuum region are included within the computational domain. Our implementation contrasts with the method typically used in fluid codes in which the resistive wall is treated as a <span class="hlt">boundary</span> condition on the computational domain <span class="hlt">boundary</span> and has the advantage of maintaining purely local coupling of mesh elements. We use this new capability to simulate perturbed, free-<span class="hlt">boundary</span> non- axisymmetric equilibria; the linear evolution of resistive wall modes; and the linear andmore » nonlinear evolution of axisymmetric vertical displacement events (VDEs). Calculated growth rates for a resistive wall mode with arbitrary wall thickness are shown to agree well with the analytic theory. Equilibrium and VDE calculations are performed in diverted tokamak geometry, at physically real- istic values of dissipation, and with resistive walls of finite width. Simulations of a VDE disruption extend into the <span class="hlt">current</span>-quench phase, in which the plasma becomes limited by the first wall, and strong <span class="hlt">currents</span> are observed to flow in the wall, in the SOL, and from the plasma to the wall.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22600112-multi-region-approach-free-boundary-three-dimensional-tokamak-equilibria-resistive-wall-instabilities','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22600112-multi-region-approach-free-boundary-three-dimensional-tokamak-equilibria-resistive-wall-instabilities"><span>Multi-region approach to free-<span class="hlt">boundary</span> three-dimensional tokamak equilibria and resistive wall instabilities</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>Ferraro, N. M., E-mail: nferraro@pppl.gov; Lao, L. L.; Jardin, S. C.</p> <p></p> <p>Free-<span class="hlt">boundary</span> 3D tokamak equilibria and resistive wall instabilities are calculated using a new resistive wall model in the two-fluid M3D-C1 code. In this model, the resistive wall and surrounding vacuum region are included within the computational domain. This implementation contrasts with the method typically used in fluid codes in which the resistive wall is treated as a <span class="hlt">boundary</span> condition on the computational domain <span class="hlt">boundary</span> and has the advantage of maintaining purely local coupling of mesh elements. This new capability is used to simulate perturbed, free-<span class="hlt">boundary</span> non-axisymmetric equilibria; the linear evolution of resistive wall modes; and the linear and nonlinear evolutionmore » of axisymmetric vertical displacement events (VDEs). Calculated growth rates for a resistive wall mode with arbitrary wall thickness are shown to agree well with the analytic theory. Equilibrium and VDE calculations are performed in diverted tokamak geometry, at physically realistic values of dissipation, and with resistive walls of finite width. Simulations of a VDE disruption extend into the <span class="hlt">current</span>-quench phase, in which the plasma becomes limited by the first wall, and strong <span class="hlt">currents</span> are observed to flow in the wall, in the SOL, and from the plasma to the wall.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhPl...23e6114F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhPl...23e6114F"><span>Multi-region approach to free-<span class="hlt">boundary</span> three-dimensional tokamak equilibria and resistive wall instabilities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ferraro, N. M.; Jardin, S. C.; Lao, L. L.; Shephard, M. S.; Zhang, F.</p> <p>2016-05-01</p> <p>Free-<span class="hlt">boundary</span> 3D tokamak equilibria and resistive wall instabilities are calculated using a new resistive wall model in the two-fluid M3D-C1 code. In this model, the resistive wall and surrounding vacuum region are included within the computational domain. This implementation contrasts with the method typically used in fluid codes in which the resistive wall is treated as a <span class="hlt">boundary</span> condition on the computational domain <span class="hlt">boundary</span> and has the advantage of maintaining purely local coupling of mesh elements. This new capability is used to simulate perturbed, free-<span class="hlt">boundary</span> non-axisymmetric equilibria; the linear evolution of resistive wall modes; and the linear and nonlinear evolution of axisymmetric vertical displacement events (VDEs). Calculated growth rates for a resistive wall mode with arbitrary wall thickness are shown to agree well with the analytic theory. Equilibrium and VDE calculations are performed in diverted tokamak geometry, at physically realistic values of dissipation, and with resistive walls of finite width. Simulations of a VDE disruption extend into the <span class="hlt">current</span>-quench phase, in which the plasma becomes limited by the first wall, and strong <span class="hlt">currents</span> are observed to flow in the wall, in the SOL, and from the plasma to the wall.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1371710-multi-region-approach-free-boundary-three-dimensional-tokamak-equilibria-resistive-wall-instabilities','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1371710-multi-region-approach-free-boundary-three-dimensional-tokamak-equilibria-resistive-wall-instabilities"><span>Multi-region approach to free-<span class="hlt">boundary</span> three-dimensional tokamak equilibria and resistive wall instabilities</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ferraro, N. M.; Jardin, S. C.; Lao, L. L.; ...</p> <p>2016-05-20</p> <p>Free-<span class="hlt">boundary</span> 3D tokamak equilibria and resistive wall instabilities are calculated using a new resistive wall model in the two-fluid M3D-C1 code. In this model, the resistive wall and surround- ing vacuum region are included within the computational domain. Our implementation contrasts with the method typically used in fluid codes in which the resistive wall is treated as a <span class="hlt">boundary</span> condition on the computational domain <span class="hlt">boundary</span> and has the advantage of maintaining purely local coupling of mesh elements. We use this new capability to simulate perturbed, free-<span class="hlt">boundary</span> non- axisymmetric equilibria; the linear evolution of resistive wall modes; and the linear andmore » nonlinear evolution of axisymmetric vertical displacement events (VDEs). Calculated growth rates for a resistive wall mode with arbitrary wall thickness are shown to agree well with the analytic theory. Equilibrium and VDE calculations are performed in diverted tokamak geometry, at physically real- istic values of dissipation, and with resistive walls of finite width. Simulations of a VDE disruption extend into the <span class="hlt">current</span>-quench phase, in which the plasma becomes limited by the first wall, and strong <span class="hlt">currents</span> are observed to flow in the wall, in the SOL, and from the plasma to the wall.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSPO51B..07K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSPO51B..07K"><span>Properties of the Agulhas <span class="hlt">Current</span>'s Inshore Front During The Shelf Agulhas Glider Experiment (SAGE)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krug, M.; Swart, S.; Goschen, W.</p> <p>2016-02-01</p> <p>The response of coastal and shelf regions to changes in the Agulhas <span class="hlt">Current</span> remains poorly studied. This is partly due to observational challenges associated with sampling western <span class="hlt">boundary</span> <span class="hlt">currents</span>. Cross-shelf exchange in such energetic <span class="hlt">current</span> systems occurs through a range of meso- ( 50-200 km) and sub-meso (<10 km) scale processes which are difficult to observe using moored <span class="hlt">current</span> arrays or Lagrangian platforms. Profiling gliders offer a revolutionary technology to continuously sample the energetic inshore regions of the Agulhas <span class="hlt">Current</span> at a high spatial (100's of meters to 3km - well within the sub-mesoscale range) and temporal (0.5-4 hourly) resolution. In April 2015, two SeaGliders were deployed off Port Elizabeth (34S) at the inshore edge of the Agulhas <span class="hlt">Current</span> as part of the Shelf Agulhas Glider Experiment (SAGE), testing for the very 1st time the feasibility of operating autonomous platforms in this highly turbulent and energetic western <span class="hlt">boundary</span> <span class="hlt">current</span> system. For a period of approximately two months, the Seagliders provided continuous observations at the inshore <span class="hlt">boundary</span> of the Agulhas <span class="hlt">Current</span> at an unprecedented spatial resolution. Observations from the Seagliders showed that at the inshore edge of the Agulhas <span class="hlt">Current</span>, both surface and depth averaged <span class="hlt">currents</span> are aligned in a south-west / north- east direction, with stronger flows encountered over deeper regions of the shelf, when the gliders are closer to the Agulhas <span class="hlt">Current</span>. In the absence of large meanders, the mean flow at the inshore <span class="hlt">boundary</span> of the Agulhas <span class="hlt">Current</span> is characterised by strong shear with a counter <span class="hlt">current</span> flowing in opposite direction to the mean <span class="hlt">current</span> field. Instances of counter <span class="hlt">currents</span> occur 45% of the time in the surface flow and 54% of the time in the depth-averaged record. More than 80% of return flow occurrences occur when glider is in water depth of less than 200m.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70015939','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70015939"><span>Bottom-<span class="hlt">boundary</span>-layer measurements on the continental shelf off the Ebro River, Spain</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Cacchione, D.A.; Drake, D.E.; Losada, M.A.; Medina, R.</p> <p>1990-01-01</p> <p>Measurements of <span class="hlt">currents</span>, waves and light transmission obtained with an instrumented bottom tripod (GEOPROBE) were used in conjunction with a theoretical bottom-<span class="hlt">boundary</span>-layer model for waves and <span class="hlt">currents</span> to investigate sediment transport on the continental shelf south of the Ebro River Delta, Spain. The <span class="hlt">current</span> data show that over a 48-day period during the fall of 1984, the average transport at 1 m above the seabed was alongshelf and slightly offshore toward the south-southwest at about 2 cm/s. A weak storm passed through the region during this period and caused elevated wave and <span class="hlt">current</span> speeds near the bed. The bottom-<span class="hlt">boundary</span>-layer model predicted correspondingly higher combined wave and <span class="hlt">current</span> bottom shear velocities at this time, but the GEOPROBE optical data indicate that little to no resuspension occurred. This result suggests that the fine-grained bottom sediment, which has a clay component of 80%, behaves cohesively and is more difficult to resuspend than noncohesive materials of similar size. Model computations also indicate that noncohesive very fine sand in shallow water (20 m deep) was resuspended and transported mainly as bedload during this storm. Fine-grained materials in shallow water that are resuspended and transported as suspended load into deeper water probably account for the slight increase in sediment concentration at the GEOPROBE sensors during the waning stages of the storm. The bottom-<span class="hlt">boundary</span>-layer data suggest that the belt of fine-grained bottom sediment that extends along the shelf toward the southwest is deposited during prolonged periods of low energy and southwestward bottom flow. This pattern is augmented by enhanced resuspension and transport toward the southwest during storms. ?? 1990.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1912050R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1912050R"><span>Dry intrusions: Lagrangian climatology and impact on the <span class="hlt">boundary</span> layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Raveh-Rubin, Shira; Wernli, Heini</p> <p>2017-04-01</p> <p>Dry air intrusions (DIs) are large-scale descending airstreams. A DI is typically referred to as a coherent airstream in the cold sector of an extratropical cyclone. Emerging evidence suggests that DIs are linked to severe surface wind gusts. However, there is yet no strict Lagrangian definition of DIs, and so their climatological frequency, dynamical characteristics as well as their seasonal and spatial distributions are unknown. Furthermore, the dynamical interaction between DIs and the planetary <span class="hlt">boundary</span> layer is not fully understood. Here, we suggest a Lagrangian definition for DI air parcels, namely a minimum pressure increase along a trajectory of 400 hPa in 48 hours. Based on this criterion, the open questions are addressed by: (i) a novel global Lagrangian climatology for the ECMWF ERA-Interim reanalysis dataset for the years 1979-2014; (ii) a case study illustrating the interaction between DIs and the <span class="hlt">boundary</span> layer. We find that DIs occur predominantly in winter. DIs coherently descend from the upper troposphere (their stratospheric origin is small), to the mid- and low levels, where they mix with their environment and diverge. Different physical characteristics typify DIs in the different regions and seasons. <span class="hlt">Finally</span>, we demonstrate the different mechanisms by which DIs can destabilize the <span class="hlt">boundary</span> layer and facilitate the formation of strong surface winds.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040031730','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040031730"><span>Evaluation of Flush-Mounted, S-Duct Inlets with Large Amounts of <span class="hlt">Boundary</span> Layer Ingestion</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Berrier, Bobby L.; Morehouse, Melissa B.</p> <p>2003-01-01</p> <p>A new high Reynolds number test capability for <span class="hlt">boundary</span> layer ingesting inlets has been developed for the NASA Langley Research Center 0.3-Meter Transonic Cryogenic Tunnel. Using this new capability, an experimental investigation of four S-duct inlet configurations with large amounts of <span class="hlt">boundary</span> layer ingestion (nominal <span class="hlt">boundary</span> layer thickness of about 40% of inlet height) was conducted at realistic operating conditions (high subsonic Mach numbers and full-scale Reynolds numbers). The objectives of this investigation were to 1) provide a database for CFD tool validation on <span class="hlt">boundary</span> layer ingesting inlets operating at realistic conditions and 2) provide a baseline inlet for future inlet flow-control studies. Tests were conducted at Mach numbers from 0.25 to 0.83, Reynolds numbers (based on duct exit diameter) from 5.1 million to a full-scale value of 13.9 million, and inlet mass-flow ratios from 0.39 to 1.58 depending on Mach number. Results of this investigation indicate that inlet pressure recovery generally decreased and inlet distortion generally increased with increasing Mach number. Except at low Mach numbers, increasing inlet mass-flow increased pressure recovery and increased distortion. Increasing the amount of <span class="hlt">boundary</span> layer ingestion (by decreasing inlet throat height) or ingesting a <span class="hlt">boundary</span> layer with a distorted (adverse) profile decreased pressure recovery and increased distortion. <span class="hlt">Finally</span>, increasing Reynolds number had almost no effect on inlet distortion but increased inlet recovery by about one-half percent at a Mach number near cruise.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810054730&hterms=survey+research+design&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsurvey%2Bresearch%2Bdesign','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810054730&hterms=survey+research+design&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dsurvey%2Bresearch%2Bdesign"><span>A survey of heating and turbulent <span class="hlt">boundary</span> layer characteristics of several hypersonic research aircraft configurations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lawing, P. L.</p> <p>1981-01-01</p> <p>Four of the configurations investigated during a proposed NASA-Langley hypersonic research aircraft program were selected for phase-change-paint heat-transfer testing and forebody <span class="hlt">boundary</span> layer pitot surveys. In anticipation of future hypersonic aircraft, both published and unpublished data and results are reviewed and presented with the purpose of providing a synoptic heat-transfer data base from the research effort. Engineering heat-transfer predictions are compared with experimental data on both a global and a local basis. The global predictions are shown to be sufficient for purposes of configuration development, and even the local predictions can be adequate when interpreted in light of the proper flow field. In that regard, cross flow in the forebody <span class="hlt">boundary</span> layers was examined for significant heating and aerodynamic effect on the scramjet engines. A design philosophy which evolved from the research airplane effort is used to design a forebody shape that produces thin, uniform, forebody <span class="hlt">boundary</span> layers on a hypersonic airbreathing missile. <span class="hlt">Finally</span>, heating/<span class="hlt">boundary</span> layer phenomena which are not predictable with state-of-the-art knowledge and techniques are shown and discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA623034','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA623034"><span>Wave-<span class="hlt">Current</span> Interaction in Coastal Inlets and River Mouths</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2014-09-30</p> <p>the Astoria Canyon buoy operated by the Coastal Data Information Program ( CDIP , buoy # 46248). Three-dimensional <span class="hlt">current</span> fields and bathymetry were...bar show considerable differences. The SWAN model uses observations from CDIP buoy # 46248 as <span class="hlt">boundary</span> condition; three- dimensional <span class="hlt">current</span> data and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..SHK.F9067A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..SHK.F9067A"><span>Shock induced phase transitions and <span class="hlt">current</span> generation in ferroelectric ceramics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Agrawal, Vinamra; Bhattacharya, Kaushik</p> <p>2017-06-01</p> <p>Ferroelectric materials are used as ferroelectric generators to obtain pulsed power by subjecting them to a shock loading. The impact induces a phase transition and at high impact speeds, dielectric breakdown. Depending on the loading conditions and the electromechanical <span class="hlt">boundary</span> conditions, the <span class="hlt">current</span> or voltage profiles obtained vary. We explore the phenomenon of large deformation dynamic behavior and the associated electro-thermo-mechanical coupling of ferroelectric materials in adiabatic environments. Using conservation laws, Maxwell's equations and second law of thermodynamics, we obtain a set of governing equations for the material and the driving force acting on the propagating phase <span class="hlt">boundary</span>. We also account for the possibility of surface charges on the phase <span class="hlt">boundary</span> in case of dielectric breakdown which introduces contribution of curvature of the phase <span class="hlt">boundary</span> in the equations. Next, the governing equations are used to solve a plate impact problem. The Helmholtz energy of the material is chosen be a combination of piecewise quadratic potential in polarization and thermo-elastic material capable of undergoing phase transformation. We obtain <span class="hlt">current</span> profiles for short circuit <span class="hlt">boundary</span> conditions along with strain, particle velocity and temperature maps. US AFOSR through Center of Excellence in High Rate Deformation of Heterogeneous Materials FA 9550-12-1-0091.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930006612','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930006612"><span>Bypass transition in compressible <span class="hlt">boundary</span> layers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vandervegt, J. J.</p> <p>1992-01-01</p> <p>Transition to turbulence in aerospace applications usually occurs in a strongly disturbed environment. For instance, the effects of free-stream turbulence, roughness and obstacles in the <span class="hlt">boundary</span> layer strongly influence transition. Proper understanding of the mechanisms leading to transition is crucial in the design of aircraft wings and gas turbine blades, because lift, drag and heat transfer strongly depend on the state of the <span class="hlt">boundary</span> layer, laminar or turbulent. Unfortunately, most of the transition research, both theoretical and experimental, has focused on natural transition. Many practical flows, however, defy any theoretical analysis and are extremely difficult to measure. Morkovin introduced in his review paper the concept of bypass transition as those forms of transition which bypass the known mechanisms of linear and non-linear transition theories and are <span class="hlt">currently</span> not understood by experiments. In an effort to better understand the mechanisms leading to transition in a disturbed environment, experiments are conducted studying simpler cases, viz. the effects of free stream turbulence on transition on a flat plate. It turns out that these experiments are very difficult to conduct, because generation of free stream turbulence with sufficiently high fluctuation levels and reasonable homogeneity is non trivial. For a discussion see Morkovin. Serious problems also appear due to the fact that at high Reynolds numbers the <span class="hlt">boundary</span> layers are very thin, especially in the nose region of the plate where the transition occurs, which makes the use of very small probes necessary. The effects of free-stream turbulence on transition are the subject of this research and are especially important in a gas turbine environment, where turbulence intensities are measured between 5 and 20 percent, Wang et al. Due to the fact that the Reynolds number for turbine blades is considerably lower than for aircraft wings, generally a larger portion of the blade will be in a laminar</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT.......258K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT.......258K"><span>A complex-lamellar description of <span class="hlt">boundary</span> layer transition</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kolla, Maureen Louise</p> <p></p> <p>Flow transition is important, in both practical and phenomenological terms. However, there is <span class="hlt">currently</span> no method for identifying the spatial locations associated with transition, such as the start and end of intermittency. The concept of flow stability and experimental correlations have been used, however, flow stability only identifies the location where disturbances begin to grow in the laminar flow and experimental correlations can only give approximations as measuring the start and end of intermittency is difficult. Therefore, the focus of this work is to construct a method to identify the start and end of intermittency, for a natural <span class="hlt">boundary</span> layer transition and a separated flow transition. We obtain these locations by deriving a complex-lamellar description of the velocity field that exists between a fully laminar and fully turbulent <span class="hlt">boundary</span> condition. Mathematically, this complex-lamellar decomposition, which is constructed from the classical Darwin-Lighthill-Hawthorne drift function and the transport of enstrophy, describes the flow that exists between the fully laminar Pohlhausen equations and Prandtl's fully turbulent one seventh power law. We approximate the difference in enstrophy density between the <span class="hlt">boundary</span> conditions using a power series. The slope of the power series is scaled by using the shape of the universal intermittency distribution within the intermittency region. We solve the complex-lamellar decomposition of the velocity field along with the slope of the difference in enstrophy density function to determine the location of the laminar and turbulent <span class="hlt">boundary</span> conditions. Then from the difference in enstrophy density function we calculate the start and end of intermittency. We perform this calculation on a natural <span class="hlt">boundary</span> layer transition over a flat plate for zero pressure gradient flow and for separated shear flow over a separation bubble. We compare these results to existing experimental results and verify the accuracy of our transition</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998APS..DPP.C2Q09D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998APS..DPP.C2Q09D"><span>Improved Design of Stellarator Coils for <span class="hlt">Current</span> Carrying Plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Drevlak, M.; Strumberger, E.; Hirshman, S.; Boozer, A.; Brooks, A.; Valanju, P.</p> <p>1998-11-01</p> <p>The method of automatic optimization (P. Merkel, Nucl. Fus. 27), (1987) 867; P. Merkel, M. Drevlak, Proc 25th EPS Conf. on Cont. Fus. and Plas. Phys., Prague, in print. for the design of stellarator coils consists essentially of determining filaments such that the average relative field error int dS [ (B_coil + B_j) \\cdot n]^2/B^2_coil is minimized on the prescribed plasma <span class="hlt">boundary</span>. Bj is the magnetic field produced by the plasma <span class="hlt">currents</span> of the given finite β fixed <span class="hlt">boundary</span> equilibrium. For equilibria of the W7-X type, Bj can be neglected, because of the reduced parallel plasma <span class="hlt">currents</span>. This is not true for quasi-axisymmetric stellarator (QAS) configurations (A. Reiman, et al., to be published.) with large equilibrium and net plasma (bootstrap) <span class="hlt">currents</span>. Although the coils for QAS exhibit low values of the field error, free <span class="hlt">boundary</span> calculations indicate that the shape of the plasma is usually not accurately reproduced , particularly when saddle coils are used. We investigate if the surface reconstruction can be improved by introducing a modified measure of the field error based on a measure of the resonant components of the normal field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5432205','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5432205"><span><span class="hlt">Boundary</span> Negotiating Artifacts in Personal Informatics: Patient-Provider Collaboration with Patient-Generated Data</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chung, Chia-Fang; Dew, Kristin; Cole, Allison; Zia, Jasmine; Fogarty, James; Kientz, Julie A.; Munson, Sean A.</p> <p>2017-01-01</p> <p>Patient-generated data is increasingly common in chronic disease care management. Smartphone applications and wearable sensors help patients more easily collect health information. However, <span class="hlt">current</span> commercial tools often do not effectively support patients and providers in collaboration surrounding these data. This paper examines patient expectations and <span class="hlt">current</span> collaboration practices around patient-generated data. We survey 211 patients, interview 18 patients, and re-analyze a dataset of 21 provider interviews. We find that collaboration occurs in every stage of self-tracking and that patients and providers create <span class="hlt">boundary</span> negotiating artifacts to support the collaboration. Building upon <span class="hlt">current</span> practices with patient-generated data, we use these theories of patient and provider collaboration to analyze misunderstandings and privacy concerns as well as identify opportunities to better support these collaborations. We reflect on the social nature of patient-provider collaboration to suggest future development of the stage-based model of personal informatics and the theory of <span class="hlt">boundary</span> negotiating artifacts. PMID:28516171</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20160007543','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20160007543"><span>Transient Growth Analysis of Compressible <span class="hlt">Boundary</span> Layers with Parabolized Stability Equations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Paredes, Pedro; Choudhari, Meelan M.; Li, Fei; Chang, Chau-Lyan</p> <p>2016-01-01</p> <p>The linear form of parabolized linear stability equations (PSE) is used in a variational approach to extend the previous body of results for the optimal, non-modal disturbance growth in <span class="hlt">boundary</span> layer flows. This methodology includes the non-parallel effects associated with the spatial development of <span class="hlt">boundary</span> layer flows. As noted in literature, the optimal initial disturbances correspond to steady counter-rotating stream-wise vortices, which subsequently lead to the formation of stream-wise-elongated structures, i.e., streaks, via a lift-up effect. The parameter space for optimal growth is extended to the hypersonic Mach number regime without any high enthalpy effects, and the effect of wall cooling is studied with particular emphasis on the role of the initial disturbance location and the value of the span-wise wavenumber that leads to the maximum energy growth up to a specified location. Unlike previous predictions that used a basic state obtained from a self-similar solution to the <span class="hlt">boundary</span> layer equations, mean flow solutions based on the full Navier-Stokes (NS) equations are used in select cases to help account for the viscous-inviscid interaction near the leading edge of the plate and also for the weak shock wave emanating from that region. These differences in the base flow lead to an increasing reduction with Mach number in the magnitude of optimal growth relative to the predictions based on self-similar mean-flow approximation. <span class="hlt">Finally</span>, the maximum optimal energy gain for the favorable pressure gradient <span class="hlt">boundary</span> layer near a planar stagnation point is found to be substantially weaker than that in a zero pressure gradient Blasius <span class="hlt">boundary</span> layer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25782971','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25782971"><span><span class="hlt">Boundary</span> Engineering for the Thermoelectric Performance of Bulk Alloys Based on Bismuth Telluride.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mun, Hyeona; Choi, Soon-Mok; Lee, Kyu Hyoung; Kim, Sung Wng</p> <p>2015-07-20</p> <p>Thermoelectrics, which transports heat for refrigeration or converts heat into electricity directly, is a key technology for renewable energy harvesting and solid-state refrigeration. Despite its importance, the widespread use of thermoelectric devices is constrained because of the low efficiency of thermoelectric bulk alloys. However, <span class="hlt">boundary</span> engineering has been demonstrated as one of the most effective ways to enhance the thermoelectric performance of conventional thermoelectric materials such as Bi2 Te3 , PbTe, and SiGe alloys because their thermal and electronic transport properties can be manipulated separately by this approach. We review our recent progress on the enhancement of the thermoelectric figure of merit through <span class="hlt">boundary</span> engineering together with the processing technologies for <span class="hlt">boundary</span> engineering developed most recently using Bi2 Te3 -based bulk alloys. A brief discussion of the principles and <span class="hlt">current</span> status of <span class="hlt">boundary</span>-engineered bulk alloys for the enhancement of the thermoelectric figure of merit is presented. We focus mainly on (1) the reduction of the thermal conductivity by grain <span class="hlt">boundary</span> engineering and (2) the reduction of thermal conductivity without deterioration of the electrical conductivity by phase <span class="hlt">boundary</span> engineering. We also discuss the next potential approach using two <span class="hlt">boundary</span> engineering strategies for a breakthrough in the area of bulk thermoelectric alloys. © 2015 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70015275','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70015275"><span>Flow separation of <span class="hlt">currents</span> in shallow water</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Signell, Richard P.</p> <p>1989-01-01</p> <p>Flow separation of <span class="hlt">currents</span> in shallow coastal areas is investigated using a <span class="hlt">boundary</span> layer model for two-dimensional (depth-averaged) tidal flow past an elliptic headland. If the shoaling region near the coast is narrow compared to the scale of the headland, bottom friction causes the flow to separate just downstream of the point where the pressure gradient switches from favoring to adverse. As long as the shoaling region at the coast is well resolved, the inclusion of eddy viscosity and a no-slip <span class="hlt">boundary</span> condition have no effect on this result. An approximate analytic solution for the pressure gradient along the <span class="hlt">boundary</span> is obtained by assuming the flow away from the immediate vicinity of the <span class="hlt">boundary</span> is irrotational. On the basis of the pressure gradient obtained from the irrotational flow solution, flow separation is a strong function of the headland aspect ratio, an equivalent Reynolds number, and a Keulegan-Carpenter number.</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/2004JGRA..10912213S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004JGRA..10912213S"><span>Two types of energy-dispersed ion structures at the plasma sheet <span class="hlt">boundary</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sauvaud, J.-A.; Kovrazhkin, R. A.</p> <p>2004-12-01</p> <p> VDIS are observed mainly during magnetically quiet times and during the recovery phase of substorms, while sporadic and recurrent TDIS are observed during the onset and main phases of substorms and magnetic storms and, although less frequently, during substorm recovery phases. From the slope of the (velocity)-1 versus time dispersions of TDIS, we conclude that they have a sporadic source located at the outer <span class="hlt">boundary</span> of the central plasma sheet, at distances from 8 to 40 RE in the equatorial plane. The disappearance of the PSBL associated with TDIS can be tentatively linked to a reconfiguration of the magnetotail, which disconnects from the Earth the field lines forming the "quiet" PSBL. We show that VDIS consist of ion beams ejected from an extended <span class="hlt">current</span> sheet at different distances. These ion beams could be formed in the neutral sheet at distance ranging from ˜30 RE to ˜100 RE from the Earth. Inside each substructure the time-of-flight dispersion of ions generally dominate over any latitudinal dispersion induced by a dawn-dusk electric field. These two main types of energy-dispersed ion structures reflect probably two main states of the magnetotail, quiet and active. <span class="hlt">Finally</span>, it must be stressed that only ˜49% (246 over 501) of the Interball-Auroral auroral zone-polar cap <span class="hlt">boundary</span> crossings can be described as VDIS or TDIS. On the other 51% of the crossings of the plasma sheet <span class="hlt">boundary</span>, no well-defined ion dispersed structures were observed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JNuM..439...57L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JNuM..439...57L"><span>Atomic scale study of grain <span class="hlt">boundary</span> segregation before carbide nucleation in Ni-Cr-Fe Alloys</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Hui; Xia, Shuang; Liu, Wenqing; Liu, Tingguang; Zhou, Bangxin</p> <p>2013-08-01</p> <p>Three dimensional chemical information concerning grain <span class="hlt">boundary</span> segregation before carbide nucleation was characterized by atom probe tomography in two Ni-Cr-Fe alloys which were aged at 500 °C for 0.5 h after homogenizing treatment. B, C and Si atoms segregation at grain <span class="hlt">boundary</span> in Alloy 690 was observed. B, C, N and P atoms segregation at grain <span class="hlt">boundary</span> in 304 austenitic stainless steel was observed. C atoms co-segregation with Cr atoms at the grain <span class="hlt">boundaries</span> both in Alloy 690 and 304 austenitic stainless steel was found, and its effect on the carbide nucleation was discussed. The amount of each segregated element at grain <span class="hlt">boundaries</span> in the two Ni-Cr-Fe alloys were analyzed quantitatively. Comparison of the grain <span class="hlt">boundary</span> segregation features of the two Ni-Cr-Fe alloys were carried out based on the experimental results. The impurity and solute atoms segregate inhomogeneously in the same grain <span class="hlt">boundary</span> both in 304 SS and Alloy 690. The grain <span class="hlt">boundary</span> segregation tendencies (Sav) are B (11.8 ± 1.4) > P (5.4 ± 1.4) > N (4.7 ± 0.3) > C (3.7 ± 0.4) in 304 SS, and B (6.9 ± 0.9) > C (6.7 ± 0.4) > Si (1.5 ± 0.2) in Alloy 690. Cr atoms may co-segregate with C atoms at grain <span class="hlt">boundaries</span> before carbide nucleation at the grain <span class="hlt">boundaries</span> both in 304 SS and Alloy 690. Ni atoms generally deplete at grain <span class="hlt">boundary</span> both in 304 SS and Alloy 690. The literature shows that the Ni atoms may co-segregate with P atoms at grain <span class="hlt">boundaries</span> [28], but the P atoms segregation do not leads to Ni segregation in the <span class="hlt">current</span> study. In the <span class="hlt">current</span> study, Fe atoms may segregate or deplete at grain <span class="hlt">boundary</span> in Alloy 690. But Fe atoms generally deplete at grain <span class="hlt">boundary</span> in 304 SS. B atoms have the strongest grain <span class="hlt">boundary</span> segregation tendency both in 304 SS and Alloy 690. The grain <span class="hlt">boundary</span> segregation tendency and Gibbs free energy of B in 304 SS is higher than in Alloy 690. C atoms are easy to segregate at grain <span class="hlt">boundaries</span> both in 304 SS and Alloy 690. The grain <span class="hlt">boundary</span> segregation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29066813','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29066813"><span>Planetary <span class="hlt">boundaries</span> for a blue planet.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nash, Kirsty L; Cvitanovic, Christopher; Fulton, Elizabeth A; Halpern, Benjamin S; Milner-Gulland, E J; Watson, Reg A; Blanchard, Julia L</p> <p>2017-11-01</p> <p>Concepts underpinning the planetary <span class="hlt">boundaries</span> framework are being incorporated into multilateral discussions on sustainability, influencing international environmental policy development. Research underlying the <span class="hlt">boundaries</span> has primarily focused on terrestrial systems, despite the fundamental role of marine biomes for Earth system function and societal wellbeing, seriously hindering the efficacy of the <span class="hlt">boundary</span> approach. We explore <span class="hlt">boundaries</span> from a marine perspective. For each <span class="hlt">boundary</span>, we show how improved integration of marine systems influences our understanding of the risk of crossing these limits. Better integration of marine systems is essential if planetary <span class="hlt">boundaries</span> are to inform Earth system governance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20604638','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20604638"><span>Development and initial evaluation of an enhanced measure of <span class="hlt">boundary</span> flexibility for the work and family domains.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Matthews, Russell A; Barnes-Farrell, Janet L</p> <p>2010-07-01</p> <p>This manuscript reports the development of a measure of work and family domain <span class="hlt">boundary</span> flexibility. Building on previous research, we propose an expanded definition of <span class="hlt">boundary</span> flexibility that includes two components-flexibility-ability and flexibility-willingness-and we develop a measure designed to capture this more comprehensive definition of <span class="hlt">boundary</span> flexibility. Flexibility-ability is conceptualized as an individual's perception of personal and situational constraints that affect <span class="hlt">boundary</span> management, and flexibility-willingness is conceptualized as an individual difference variable that captures the motivation to engage in <span class="hlt">boundary</span> flexing. An additional feature of domain <span class="hlt">boundaries</span>, permeability, is also examined. Data are presented from two studies. Study 1 (N = 244) describes the development of a multiscale measure that extends <span class="hlt">current</span> conceptual definitions of <span class="hlt">boundary</span> flexibility. Study 2 (N = 225) describes the refinement and evaluation of this measure. Confirmatory factor analysis, reliability evidence, interscale correlations, and correlations with important work-family constructs (e.g., domain centrality, work-family conflict) provide initial construct validity evidence for the measure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title15-vol3/pdf/CFR-2010-title15-vol3-sec922-110.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title15-vol3/pdf/CFR-2010-title15-vol3-sec922-110.pdf"><span>15 CFR 922.110 - <span class="hlt">Boundary</span>.</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>... MARINE SANCTUARY PROGRAM REGULATIONS Cordell Bank National Marine Sanctuary § 922.110 <span class="hlt">Boundary</span>. The Cordell Bank National Marine Sanctuary (Sanctuary) <span class="hlt">boundary</span> encompasses a total area of approximately 399... California approximately 50 miles west-northwest of San Francisco, California. The Sanctuary <span class="hlt">boundary</span> extends...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29758713','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29758713"><span>Entanglement entropy of a three-spin-interacting spin chain with a time-reversal-breaking impurity at one <span class="hlt">boundary</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nag, Tanay; Rajak, Atanu</p> <p>2018-04-01</p> <p>We investigate the effect of a time-reversal-breaking impurity term (of strength λ_{d}) on both the equilibrium and nonequilibrium critical properties of entanglement entropy (EE) in a three-spin-interacting transverse Ising model, which can be mapped to a p-wave superconducting chain with next-nearest-neighbor hopping and interaction. Importantly, we find that the logarithmic scaling of the EE with block size remains unaffected by the application of the impurity term, although, the coefficient (i.e., central charge) varies logarithmically with the impurity strength for a lower range of λ_{d} and eventually saturates with an exponential damping factor [∼exp(-λ_{d})] for the phase <span class="hlt">boundaries</span> shared with the phase containing two Majorana edge modes. On the other hand, it receives a linear correction in term of λ_{d} for an another phase <span class="hlt">boundary</span>. <span class="hlt">Finally</span>, we focus to study the effect of the impurity in the time evolution of the EE for the critical quenching case where the impurity term is applied only to the <span class="hlt">final</span> Hamiltonian. Interestingly, it has been shown that for all the phase <span class="hlt">boundaries</span>, contrary to the equilibrium case, the saturation value of the EE increases logarithmically with the strength of impurity in a certain regime of λ_{d} and <span class="hlt">finally</span>, for higher values of λ_{d}, it increases very slowly dictated by an exponential damping factor. The impurity-induced behavior of EE might bear some deep underlying connection to thermalization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvE..97d2108N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvE..97d2108N"><span>Entanglement entropy of a three-spin-interacting spin chain with a time-reversal-breaking impurity at one <span class="hlt">boundary</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nag, Tanay; Rajak, Atanu</p> <p>2018-04-01</p> <p>We investigate the effect of a time-reversal-breaking impurity term (of strength λd) on both the equilibrium and nonequilibrium critical properties of entanglement entropy (EE) in a three-spin-interacting transverse Ising model, which can be mapped to a p -wave superconducting chain with next-nearest-neighbor hopping and interaction. Importantly, we find that the logarithmic scaling of the EE with block size remains unaffected by the application of the impurity term, although, the coefficient (i.e., central charge) varies logarithmically with the impurity strength for a lower range of λd and eventually saturates with an exponential damping factor [˜exp(-λd) ] for the phase <span class="hlt">boundaries</span> shared with the phase containing two Majorana edge modes. On the other hand, it receives a linear correction in term of λd for an another phase <span class="hlt">boundary</span>. <span class="hlt">Finally</span>, we focus to study the effect of the impurity in the time evolution of the EE for the critical quenching case where the impurity term is applied only to the <span class="hlt">final</span> Hamiltonian. Interestingly, it has been shown that for all the phase <span class="hlt">boundaries</span>, contrary to the equilibrium case, the saturation value of the EE increases logarithmically with the strength of impurity in a certain regime of λd and <span class="hlt">finally</span>, for higher values of λd, it increases very slowly dictated by an exponential damping factor. The impurity-induced behavior of EE might bear some deep underlying connection to thermalization.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MPLA...3250077K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MPLA...3250077K"><span>A Neumann <span class="hlt">boundary</span> term for gravity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krishnan, Chethan; Raju, Avinash</p> <p>2017-05-01</p> <p>The Gibbons-Hawking-York (GHY) <span class="hlt">boundary</span> term makes the Dirichlet problem for gravity well-defined, but no such general term seems to be known for Neumann <span class="hlt">boundary</span> conditions. In this paper, we view Neumann not as fixing the normal derivative of the metric (“velocity”) at the <span class="hlt">boundary</span>, but as fixing the functional derivative of the action with respect to the <span class="hlt">boundary</span> metric (“momentum”). This leads directly to a new <span class="hlt">boundary</span> term for gravity: the trace of the extrinsic curvature with a specific dimension-dependent coefficient. In three dimensions, this <span class="hlt">boundary</span> term reduces to a “one-half” GHY term noted in the literature previously, and we observe that our action translates precisely to the Chern-Simons action with no extra <span class="hlt">boundary</span> terms. In four dimensions, the <span class="hlt">boundary</span> term vanishes, giving a natural Neumann interpretation to the standard Einstein-Hilbert action without <span class="hlt">boundary</span> terms. We argue that in light of AdS/CFT, ours is a natural approach for defining a “microcanonical” path integral for gravity in the spirit of the (pre-AdS/CFT) work of Brown and York.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5095442','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5095442"><span>Deleterious localized stress fields: the effects of <span class="hlt">boundaries</span> and stiffness tailoring in anisotropic laminated plates</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Weaver, P. M.</p> <p>2016-01-01</p> <p>The safe design of primary load-bearing structures requires accurate prediction of stresses, especially in the vicinity of geometric discontinuities where deleterious three-dimensional stress fields can be induced. Even for thin-walled structures significant through-thickness stresses arise at edges and <span class="hlt">boundaries</span>, and this is especially precarious for laminates of advanced fibre-reinforced composites because through-thickness stresses are the predominant drivers in delamination failure. Here, we use a higher-order equivalent single-layer model derived from the Hellinger–Reissner mixed variational principle to examine <span class="hlt">boundary</span> layer effects in laminated plates comprising constant-stiffness and variable-stiffness laminae and deforming statically in cylindrical bending. The results show that zigzag deformations, which arise due to layerwise differences in the transverse shear moduli, drive <span class="hlt">boundary</span> layers towards clamped edges and are therefore critically important in quantifying localized stress gradients. The relative significance of the <span class="hlt">boundary</span> layer scales with the degree of layerwise anisotropy and the thickness to characteristic length ratio. <span class="hlt">Finally</span>, we demonstrate that the phenomenon of alternating positive and negative transverse shearing deformation through the thickness of composite laminates, previously only observed at clamped <span class="hlt">boundaries</span>, can also occur at other locations as a result of smoothly varying the material properties over the in-plane dimensions of the laminate. PMID:27843401</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900024674&hterms=road+limit&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Droad%2Blimit','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900024674&hterms=road+limit&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Droad%2Blimit"><span>Road <span class="hlt">boundary</span> detection</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sowers, J.; Mehrotra, R.; Sethi, I. K.</p> <p>1989-01-01</p> <p>A method for extracting road <span class="hlt">boundaries</span> using the monochrome image of a visual road scene is presented. The statistical information regarding the intensity levels present in the image along with some geometrical constraints concerning the road are the basics of this approach. Results and advantages of this technique compared to others are discussed. The major advantages of this technique, when compared to others, are its ability to process the image in only one pass, to limit the area searched in the image using only knowledge concerning the road geometry and previous <span class="hlt">boundary</span> information, and dynamically adjust for inconsistencies in the located <span class="hlt">boundary</span> information, all of which helps to increase the efficacy of this technique.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28761098','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28761098"><span>Seismological evidence for a localized mushy zone at the Earth's inner core <span class="hlt">boundary</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tian, Dongdong; Wen, Lianxing</p> <p>2017-08-01</p> <p>Although existence of a mushy zone in the Earth's inner core has been hypothesized several decades ago, no seismic evidence has ever been reported. Based on waveform modeling of seismic compressional waves that are reflected off the Earth's inner core <span class="hlt">boundary</span>, here we present seismic evidence for a localized 4-8 km thick zone across the inner core <span class="hlt">boundary</span> beneath southwest Okhotsk Sea with seismic properties intermediate between those of the inner and outer core and of a mushy zone. Such a localized mushy zone is found to be surrounded by a sharp inner core <span class="hlt">boundary</span> nearby. These seismic results suggest that, in the <span class="hlt">current</span> thermo-compositional state of the Earth's core, the outer core composition is close to eutectic in most regions resulting in a sharp inner core <span class="hlt">boundary</span>, but deviation from the eutectic composition exists in some localized regions resulting in a mushy zone with a thickness of 4-8 km.The existence of a mushy zone in the Earth's inner core has been suggested, but has remained unproven. Here, the authors have discovered a 4-8 km thick mushy zone at the inner core <span class="hlt">boundary</span> beneath the Okhotsk Sea, indicating that there may be more localized mushy zones at the inner core <span class="hlt">boundary</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17953495','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17953495"><span>Work and personal life <span class="hlt">boundary</span> management: <span class="hlt">boundary</span> strength, work/personal life balance, and the segmentation-integration continuum.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bulger, Carrie A; Matthews, Russell A; Hoffman, Mark E</p> <p>2007-10-01</p> <p>While researchers are increasingly interested in understanding the <span class="hlt">boundaries</span> surrounding the work and personal life domains, few have tested the propositions set forth by theory. <span class="hlt">Boundary</span> theory proposes that individuals manage the <span class="hlt">boundaries</span> between work and personal life through processes of segmenting and/or integrating the domains. The authors investigated <span class="hlt">boundary</span> management profiles of 332 workers in an investigation of the segmentation-integration continuum. Cluster analysis indicated consistent clusters of <span class="hlt">boundary</span> management practices related to varying segmentation and integration of the work and personal life domains. But, the authors suggest that the segmentation-integration continuum may be more complicated. Results also indicated relationships between <span class="hlt">boundary</span> management practices and work-personal life interference and work-personal life enhancement. Less flexible and more permeable <span class="hlt">boundaries</span> were related to more interference, while more flexible and more permeable <span class="hlt">boundaries</span> were related to more enhancement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1167615-improving-subtropical-boundary-layer-cloudiness-ncep-gfs','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1167615-improving-subtropical-boundary-layer-cloudiness-ncep-gfs"><span>Improving Subtropical <span class="hlt">Boundary</span> Layer Cloudiness in the 2011 NCEP GFS</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>Fletcher, J. K.; Bretherton, Christopher S.; Xiao, Heng</p> <p>2014-09-23</p> <p>The <span class="hlt">current</span> operational version of National Centers for Environmental Prediction (NCEP) Global Forecasting System (GFS) shows significant low cloud bias. These biases also appear in the Coupled Forecast System (CFS), which is developed from the GFS. These low cloud biases degrade seasonal and longer climate forecasts, particularly of short-wave cloud radiative forcing, and affect predicted sea surface temperature. Reducing this bias in the GFS will aid the development of future CFS versions and contributes to NCEP's goal of unified weather and climate modelling. Changes are made to the shallow convection and planetary <span class="hlt">boundary</span> layer parameterisations to make them more consistentmore » with <span class="hlt">current</span> knowledge of these processes and to reduce the low cloud bias. These changes are tested in a single-column version of GFS and in global simulations with GFS coupled to a dynamical ocean model. In the single-column model, we focus on changing parameters that set the following: the strength of shallow cumulus lateral entrainment, the conversion of updraught liquid water to precipitation and grid-scale condensate, shallow cumulus cloud top, and the effect of shallow convection in stratocumulus environments. Results show that these changes improve the single-column simulations when compared to large eddy simulations, in particular through decreasing the precipitation efficiency of <span class="hlt">boundary</span> layer clouds. These changes, combined with a few other model improvements, also reduce <span class="hlt">boundary</span> layer cloud and albedo biases in global coupled simulations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009ECSS...83..443G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009ECSS...83..443G"><span>Does the poleward <span class="hlt">boundary</span> <span class="hlt">current</span> off Western Australia exert a dominant influence on coastal chaetognaths and siphonophores?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gaughan, D. J.; Pearce, A. F.; Lewis, P. D.</p> <p>2009-08-01</p> <p>A transect that extended 40 km offshore across the continental shelf off Perth, Western Australia, was sampled monthly during 1997 and 1998. Zooplankton was sampled at 5 km intervals with a 300 micron-mesh bongo net deployed vertically to within 3 m of the bottom, or to a maximum depth of 70 m. Numbers of species of chaetognaths and siphonores were quantified, as were abundances of the common species from these groups and of the hydromedusae Auglaura hemistoma. The potential influences of four environmental variables (sea-level, sea surface temperature, salinity and chlorophyll concentration) on variability in diversity and abundance were assessed using generalized additive modeling. A combination of factors were found to influence the seasonal and spatial biological variability and, of these factors, non-linear relationships always contributed to the best fitting models. In all but one case, each of the environmental variables was included in the <span class="hlt">final</span> model. The seasonally variable Leeuwin <span class="hlt">Current</span>, whose strength is measured as variations in local sea-level, is the dominant mesoscale oceanographic feature in the study region but was not found to have an overriding influence on the shelf zooplankton. This contrasts a previous hypothesis that subjectively attributed seasonal variability of the same taxa examined in this study to seasonal variations in the Leeuwin <span class="hlt">Current</span>. There remains a poor understanding of shelf zooplankton off Western Australia and, in particular, of the processes that influence seasonal and spatial variability. A more complete understanding of potential causative influences of the Leeuwin <span class="hlt">Current</span> on the shelf plankton community of south-western Australia must be cognizant of a range of biophysical factors operating at both the broader mesoscale and at smaller scales within the shelf pelagic ecosystem.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840017873','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840017873"><span>Scaling and modeling of three-dimensional, end-wall, turbulent <span class="hlt">boundary</span> layers. Ph.D. Thesis - <span class="hlt">Final</span> Report</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Goldberg, U. C.; Reshotko, E.</p> <p>1984-01-01</p> <p>The method of matched asymptotic expansion was employed to identify the various subregions in three dimensional, turbomachinery end wall turbulent <span class="hlt">boundary</span> layers, and to determine the proper scaling of these regions. The two parts of the b.l. investigated are the 3D pressure driven part over the endwall, and the 3D part located at the blade/end wall juncture. Models are proposed for the 3d law of the wall and law of the wake. These models and the data of van den Berg and Elsenaar and of Mueller are compared and show good agreement between models and experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1377895-microscopic-distributions-defect-luminescence-from-subgrain-boundaries-multicrystalline-silicon-wafers','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1377895-microscopic-distributions-defect-luminescence-from-subgrain-boundaries-multicrystalline-silicon-wafers"><span>Microscopic Distributions of Defect Luminescence From Subgrain <span class="hlt">Boundaries</span> in Multicrystalline Silicon Wafers</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>Nguyen, Hieu T.; Jensen, Mallory A.; Li, Li</p> <p></p> <p>We investigate the microscopic distributions of sub-band-gap luminescence emission (the so-called D-lines D1/D2/D3/D4) and the band-to-band luminescence intensity, near recombination-active sub-grain <span class="hlt">boundaries</span> in multicrystalline silicon wafers for solar cells. We find that the sub-band-gap luminescence from decorating defects/impurities (D1/D2) and from intrinsic dislocations (D3/D4) have distinctly different spatial distributions, and are asymmetric across the sub-grain <span class="hlt">boundaries</span>. The presence of D1/D2 is correlated with a strong reduction in the band-to-band luminescence, indicating a higher recombination activity. In contrast, D3/D4 emissions are not strongly correlated with the band-to-band intensity. Based on spatially-resolved, synchrotron-based micro-X-ray fluorescence measurements of metal impurities, we confirm thatmore » high densities of metal impurities are present at locations with strong D1/D2 emission but low D3/D4 emission. <span class="hlt">Finally</span>, we show that the observed asymmetry of the sub-band-gap luminescence across the sub-grain <span class="hlt">boundaries</span> is due to their inclination below the wafer surface. Based on the luminescence asymmetries, the sub-grain <span class="hlt">boundaries</span> are shown to share a common inclination locally, rather than be orientated randomly.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001PhDT........98R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001PhDT........98R"><span>Microstructural investigation of <span class="hlt">current</span> barriers in high temperature superconducting tapes and coated conductors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reeves, Jodi Lynn</p> <p></p> <p>Microstructural barriers to supercurrent occur on many length scales in all high temperature oxide superconductors. Eliminating microstructural barriers is key to making these potentially valuable materials more favorable for commercial applications. In silver-sheathed Bi2Sr2CaCu 2Ox (Bi-2212) tapes and multifilaments, the principal barriers on the scale of 10--100's of micrometers are bubbling, porosity, second phase particles, and poorly aligned grains. In state-of-the-art YBa2 Cu3Ox (YBCO) coated conductors, supercurrent barriers on the 0.1--100mum scale are grain <span class="hlt">boundaries</span>. This thesis work clarifies the role of grain <span class="hlt">boundaries</span> in the nickel substrate of RABiTS (Rolling Assisted Biaxially Textured Substrate) coated conductors. Plan-view SEM imaging, focused ion beam cutting, magneto-optical imaging and grain orientation mapping were used to determine barriers to supercurrent. Experiments showed enhanced magnetic flux penetration, and hence reduced Jc, in the YBCO above nearly all nickel grain <span class="hlt">boundaries</span> with misorientation angles (theta) greater than 5°, independent of the rotation axis. Monochromatic backscattered electron Kikuchi pattern percolation maps imply there is a fully connected <span class="hlt">current</span> path through the YBCO microstructure within the chosen tolerance angle criterion of the map. However, it is the grain <span class="hlt">boundary</span> map that displays the constrictions of the <span class="hlt">current</span> path. Therefore, grain <span class="hlt">boundary</span> maps are better tools for illustrating supercurrent barriers than percolation maps. Grain <span class="hlt">boundary</span> maps and grain orientation maps were used to investigate how the texture of the substrate was transferred to the buffer layers and to the superconductor. Most grasp <span class="hlt">boundaries</span> in the nickel were replicated in the buffer and superconductor layers with the same misorientation angle. Anisotropic growth and/or surface energy minimization may be responsible for the improvement in c-axis alignment in the YBCO over the buffer layer. However, the YBCO mosaic spread did</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6607915-free-boundary-resistive-modes-tokamaks','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6607915-free-boundary-resistive-modes-tokamaks"><span>Free <span class="hlt">boundary</span> resistive modes in tokamaks</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>Huysmans, G.T.A.; Goedbloed, J.P.; Kerner, W.</p> <p>1993-05-01</p> <p>There exist a number of observations of magnetohydrodynamic (MHD) activity that can be related to resistive MHD modes localized near the plasma <span class="hlt">boundary</span>. To study the stability of these modes, a free <span class="hlt">boundary</span> description of the plasma is essential. The resistive plasma--vacuum <span class="hlt">boundary</span> conditions have been implemented in the fully toroidal resistive spectral code CASTOR (Complex Alfven Spectrum in Toroidal Geometry) [[ital Proceedings] [ital of] [ital the] 18[ital th] [ital Conference] [ital on] [ital Controlled] [ital Fusion] [ital and] [ital Plasma] [ital Physics], Berlin, edited by P. Bachmann and D. C. Robinson (European Physical Society, Petit-Lancy, Switzerland, 1991), p. 89].more » The influence of a free <span class="hlt">boundary</span>, as compared to a fixed <span class="hlt">boundary</span> on the stability of low-[ital m] tearing modes, is studied. It is found that the stabilizing (toroidal) effect of a finite pressure due the plasma compression is lost in the free <span class="hlt">boundary</span> case for modes localized near the <span class="hlt">boundary</span>. Since the stabilization due to the favorable average curvature in combination with a pressure gradient near the <span class="hlt">boundary</span> is small, the influence of the pressure on the stability is much less important for free <span class="hlt">boundary</span> modes than for fixed <span class="hlt">boundary</span> modes.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006ApPhL..89b2115X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006ApPhL..89b2115X"><span>Electrical transport through individual nanowires with transverse grain <span class="hlt">boundaries</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xue, X. Y.; Feng, P.; Wang, C.; Chen, Y. J.; Wang, Y. G.; Wang, T. H.</p> <p>2006-07-01</p> <p>V2O4•0.25H2O nanowires are synthesized via hydrothermal route. The nanowires are of metastable phase, and transverse grain <span class="hlt">boundaries</span> are observed in their microstructures. Transport through individual V2O4•0.25H2O nanowires shows nonlinear <span class="hlt">current</span>-voltage (I-V) characteristics in the bias range of -3to3V. The resistance rapidly decreases from 2.54to0.5MΩ as the bias is raised from 0to1V. Such behaviors can be attributed to the presence of the barrier at the transverse grain <span class="hlt">boundary</span>. By analyzing the I-V curves at various temperatures, the effective barrier height is estimated to be about 0.13eV. Our results provide important information about how the microstructure mismatch affects the electrical properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/CFR-2010-title15-vol3/pdf/CFR-2010-title15-vol3-sec922-130.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title15-vol3/pdf/CFR-2010-title15-vol3-sec922-130.pdf"><span>15 CFR 922.130 - <span class="hlt">Boundary</span>.</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>... MARINE SANCTUARY PROGRAM REGULATIONS Monterey Bay National Marine Sanctuary § 922.130 <span class="hlt">Boundary</span>. The Monterey Bay National Marine Sanctuary (Sanctuary) consists of two separate areas. (a) The first area... northern terminus of the Sanctuary <span class="hlt">boundary</span> is located along the southern <span class="hlt">boundary</span> of the Gulf of the...</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('https://www.gpo.gov/fdsys/pkg/CFR-2010-title15-vol3/pdf/CFR-2010-title15-vol3-sec922-80.pdf','CFR'); return false;" href="https://www.gpo.gov/fdsys/pkg/CFR-2010-title15-vol3/pdf/CFR-2010-title15-vol3-sec922-80.pdf"><span>15 CFR 922.80 - <span class="hlt">Boundary</span>.</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>... MARINE SANCTUARY PROGRAM REGULATIONS Gulf of the Farallones National Marine Sanctuary § 922.80 <span class="hlt">Boundary</span>. The Gulf of the Farallones National Marine Sanctuary (Sanctuary) <span class="hlt">boundary</span> encompasses a total area of... extent of the Sanctuary <span class="hlt">boundary</span> is a geodetic line extending westward from Bodega Head approximately 6...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1438652-twin-related-domains-microstructures-conventionally-processed-grain-boundary-engineered-materials','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1438652-twin-related-domains-microstructures-conventionally-processed-grain-boundary-engineered-materials"><span>Twin related domains in 3D microstructures of conventionally processed and grain <span class="hlt">boundary</span> engineered materials</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lind, Jonathan; Li, Shiu Fai; Kumar, Mukul</p> <p>2016-05-20</p> <p>The concept of twin-limited microstructures has been explored in the literature as a crystallographically constrained grain <span class="hlt">boundary</span> network connected via only coincident site lattice (CSL) <span class="hlt">boundaries</span>. The advent of orientation imaging has made classification of twin-related domains (TRD) or any other orientation cluster experimentally accessible in 2D using EBSD. With the emergence of 3D orientation mapping, a comparison of TRDs in measured 3D microstructures is performed in this paper and compared against their 2D counterparts. The TRD analysis is performed on a conventionally processed (CP) and a grain <span class="hlt">boundary</span> engineered (EM) high purity copper sample that have been subjected tomore » successive anneal procedures to promote grain growth. <span class="hlt">Finally</span>, the EM sample shows extremely large TRDs which begin to approach that of a twin-limited microstructure, while the TRDs in the CP sample remain relatively small and remote.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27026894','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27026894"><span>A numerical solution of a singular <span class="hlt">boundary</span> value problem arising in <span class="hlt">boundary</span> layer theory.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hu, Jiancheng</p> <p>2016-01-01</p> <p>In this paper, a second-order nonlinear singular <span class="hlt">boundary</span> value problem is presented, which is equivalent to the well-known Falkner-Skan equation. And the one-dimensional third-order <span class="hlt">boundary</span> value problem on interval [Formula: see text] is equivalently transformed into a second-order <span class="hlt">boundary</span> value problem on finite interval [Formula: see text]. The finite difference method is utilized to solve the singular <span class="hlt">boundary</span> value problem, in which the amount of computational effort is significantly less than the other numerical methods. The numerical solutions obtained by the finite difference method are in agreement with those obtained by previous authors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2012-03-29/pdf/2012-7560.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2012-03-29/pdf/2012-7560.pdf"><span>77 FR 18997 - <span class="hlt">Boundary</span> Establishment for the Presque Isle National Wild and Scenic River, Ottawa National...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2012-03-29</p> <p>... AGENCY: Forest Service, USDA. ACTION: Notice of availability. SUMMARY: In accordance with Section 3(b) of the Wild and Scenic Rivers Act, the USDA Forest Service, Washington Office, is transmitting the <span class="hlt">final</span>... Wild and Scenic River <span class="hlt">boundary</span> is available for review at the following offices: USDA Forest Service...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JMS...174...25H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JMS...174...25H"><span>Recirculation of the Canary <span class="hlt">Current</span> in fall 2014</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hernández-Guerra, Alonso; Espino-Falcón, Elisabet; Vélez-Belchí, Pedro; Dolores Pérez-Hernández, M.; Martínez-Marrero, Antonio; Cana, Luis</p> <p>2017-10-01</p> <p>Hydrographic measurements together with Ship mounted Acoustic Doppler <span class="hlt">Current</span> Profilers and Lowered Acoustic Doppler <span class="hlt">Current</span> Profilers (LADCP) obtained in October 2014 are used to describe water masses, geostrophic circulation and mass transport of the Canary <span class="hlt">Current</span> System, as the Eastern <span class="hlt">Boundary</span> of the North Atlantic Subtropical Gyre. Geostrophic velocities are adjusted to velocities from LADCP data to estimate an initial velocity at the reference layer. The adjustment results in a northward circulation at the thermocline layers over the African slope from an initial convergent flow. <span class="hlt">Final</span> reference velocities and consequently absolute circulation are estimated from an inverse box model applied to an ocean divided into 13 neutral density layers. This allows us to evaluate mass fluxes consistent with the thermal wind equation and mass conservation. Ekman transport is estimated from the wind data derived from the Weather Research and Forecasting model. Ekman transport is added to the first layer and adjusted with the inverse model. The Canary <span class="hlt">Current</span> located west of Lanzarote Island transports to the south a mass of - 1.5 ± 0.7 Sv (1 Sv = 106 m3 s- 1 ≈ 109 kg s- 1) of North Atlantic Central Water at the surface and thermocline layers ( 0-700 m). In fall 2014, hydrographic data shows that the Canary <span class="hlt">Current</span> in the thermocline (below at about 80 m depth to 700 m) recirculates to the north over the African slope and flows through the Lanzarote Passage. At intermediate layers ( 700-1400 m), the Intermediate Poleward Undercurrent transports northward a relatively fresh Antarctic Intermediate Water in the range of 0.8 ± 0.4 Sv through the Lanzarote Passage and west of Lanzarote Island beneath the recirculation of the Canary <span class="hlt">Current</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21315155','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21315155"><span>The <span class="hlt">boundary</span> structure in the analysis of reversibly interacting systems by sedimentation velocity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhao, Huaying; Balbo, Andrea; Brown, Patrick H; Schuck, Peter</p> <p>2011-05-01</p> <p>Sedimentation velocity (SV) experiments of heterogeneous interacting systems exhibit characteristic <span class="hlt">boundary</span> structures that can usually be very easily recognized and quantified. For slowly interacting systems, the <span class="hlt">boundaries</span> represent concentrations of macromolecular species sedimenting at different rates, and they can be interpreted directly with population models based solely on the mass action law. For fast reactions, migration and chemical reactions are coupled, and different, but equally easily discernable <span class="hlt">boundary</span> structures appear. However, these features have not been commonly utilized for data analysis, for the lack of an intuitive and computationally simple model. The recently introduced effective particle theory (EPT) provides a suitable framework. Here, we review the motivation and theoretical basis of EPT, and explore practical aspects for its application. We introduce an EPT-based design tool for SV experiments of heterogeneous interactions in the software SEDPHAT. As a practical tool for the first step of data analysis, we describe how the <span class="hlt">boundary</span> resolution of the sedimentation coefficient distribution c(s) can be further improved with a Bayesian adjustment of maximum entropy regularization to the case of heterogeneous interactions between molecules that have been previously studied separately. This can facilitate extracting the characteristic <span class="hlt">boundary</span> features by integration of c(s). In a second step, these are assembled into isotherms as a function of total loading concentrations and fitted with EPT. Methods for addressing concentration errors in isotherms are discussed. <span class="hlt">Finally</span>, in an experimental model system of alpha-chymotrypsin interacting with soybean trypsin inhibitor, we show that EPT provides an excellent description of the experimental sedimentation <span class="hlt">boundary</span> structure of fast interacting systems. Published by Elsevier Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29270446','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29270446"><span>Event <span class="hlt">Boundaries</span> in Memory and Cognition.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Radvansky, Gabriel A; Zacks, Jeffrey M</p> <p>2017-10-01</p> <p>Research on event cognition is rapidly developing and is revealing fundamental aspects of human cognition. In this paper, we review recent and <span class="hlt">current</span> work that is driving this field forward. We first outline the Event Horizon Model, which broadly describes the impact of event <span class="hlt">boundaries</span> on cognition and memory. Then, we address recent work on event segmentation, the role of event cognition in working memory and long-term memory, including event model updating, and long term retention. Throughout we also consider how event cognition varies across individuals and groups of people and consider the neural mechanisms involved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JEMat..43.4386T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JEMat..43.4386T"><span>Effect of Grain <span class="hlt">Boundary</span> Misorientation on Electromigration in Lead-Free Solder Joints</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tasooji, Amaneh; Lara, Leticia; Lee, Kyuoh</p> <p>2014-12-01</p> <p>Reduction in microelectronic interconnect size gives rise to solder bumps consisting of few grains, approaching a single- or bicrystal grain morphology in C4 bumps. Single grain anisotropy, individual grain orientation, presence of easy diffusion paths along grain <span class="hlt">boundaries</span>, and the increased <span class="hlt">current</span> density in these small solder bumps aggravate electromigration. This reduces the reliability of the entire microelectronic system. This paper focuses on electromigration behavior in Pb-free solder, specifically the Sn-0.7 wt.%Cu alloy. We discuss the effects of texture, grain orientation, and grain <span class="hlt">boundary</span> misorientation angle on electromigration (EM) and intermetallic compound formation in EM-tested C4 bumps. The detailed electron backscatter diffraction (EBSD) analysis used in this study reveals the greater influence of grain <span class="hlt">boundary</span> misorientation on solder bump electromigration compared with the effect associated with individual grain orientation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/863477','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/863477"><span>Magnetic thin-film split-domain <span class="hlt">current</span> sensor-recorder</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Hsieh, Edmund J.</p> <p>1979-01-01</p> <p>A sensor-recorder for recording a representation of the direction and peak amplitude of a transient <span class="hlt">current</span>. A magnetic thin film is coated on a glass substrate under the influence of a magnetic field so that the finished film is magnetically uniaxial and anisotropic. The film is split into two oppositely magnetized contiguous domains with a central <span class="hlt">boundary</span> by subjecting adjacent portions of the film simultaneously to magnetic fields that are opposed 180.degree.. With the split-domain sensor-recorder placed with the film plane and domain <span class="hlt">boundary</span> either perpendicular or parallel to the expected conductive path of a transient <span class="hlt">current</span>, the occurrence of the transient causes switching of a portion of one domain to the direction of the other domain. The amount of the switched domain portion is indicative of the amplitude of the peak <span class="hlt">current</span> of the transient, while the particular domain that is switched is indicative of the direction of the <span class="hlt">current</span>. The resulting domain patterns may be read with a passive magnetic tape viewer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhLB..765..260P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhLB..765..260P"><span>Quantum "violation" of Dirichlet <span class="hlt">boundary</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>Park, I. Y.</p> <p>2017-02-01</p> <p>Dirichlet <span class="hlt">boundary</span> conditions have been widely used in general relativity. They seem at odds with the holographic property of gravity simply because a <span class="hlt">boundary</span> configuration can be varying and dynamic instead of dying out as required by the conditions. In this work we report what should be a tension between the Dirichlet <span class="hlt">boundary</span> conditions and quantum gravitational effects, and show that a quantum-corrected black hole solution of the 1PI action no longer obeys, in the naive manner one may expect, the Dirichlet <span class="hlt">boundary</span> conditions imposed at the classical level. We attribute the 'violation' of the Dirichlet <span class="hlt">boundary</span> conditions to a certain mechanism of the information storage on the <span class="hlt">boundary</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA146381','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA146381"><span>Large-Eddy Simulation. Guidelines for Its Application to Planetary <span class="hlt">Boundary</span> Layer Research</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1984-08-01</p> <p>34 engineering application of L98 was Deardorff’s simulation of turbulent channel flow, which was carried out at the National Center for Atmospheric...over the past 20 years, and yet in the perception of some observers * the applications of the resulting basic science to practical problem remain...COVERED -- Large Eddy Simulation: Guidelines for its .0 application to planetary <span class="hlt">boundary</span> layer research <span class="hlt">Final</span> Report Oct 83-Aug 84 S. PERFORMING ORG</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA518413','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA518413"><span>FIEFDom: A Transparent Domain <span class="hlt">Boundary</span> Recognition System using a Fuzzy Mean Operator</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2008-12-04</p> <p>to search for matching fragments by running the PSI-BLAST program a second time. During this step, the expectation value threshold ( e -value) is set at...statistical significance (or low e -value), and therefore have low scores. <span class="hlt">Finally</span>, the domain <span class="hlt">boundaries</span> (if any) are predicted using the scored...neighbor (match) is weighted by its e -value, the relative contribution of each neighbor is apparent. This is contrary to black-box models in which the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/932019-mechanisms-enhanced-supercurrent-across-meandered-grain-boundaries-high-temperature-superconductors','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/932019-mechanisms-enhanced-supercurrent-across-meandered-grain-boundaries-high-temperature-superconductors"><span>Mechanisms for Enhanced Supercurrent Across Meandered Grain <span class="hlt">Boundaries</span> in High-Temperature Superconductors</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>Feldmann, D. M.; Holesinger, T. G.; Feenstra, Roeland</p> <p>2007-01-01</p> <p>It has been well established that the critical <span class="hlt">current</span> density J{sub c} across grain <span class="hlt">boundaries</span> (GBs) in high-temperature superconductors decreases exponentially with misorientation angle {theta} beyond {approx}2-3 degrees. This rapid decrease is due to a suppression of the superconducting order parameter at the grain <span class="hlt">boundary</span>, giving rise to weakly pinned Abrikosov-Josephson (AJ) vortices. Here we show that if the GB plane meanders, this exponential dependence no longer holds, permitting greatly enhanced J{sub c} values: up to six times at 0 T and four times at 1 T at {theta}{approx}4-6 degrees. This enhancement is due to an increase in the <span class="hlt">current</span>-carryingmore » cross section of the GBs and the appearance of short AJ vortex segments in the GB plane, confined by the interaction with strongly pinned Abrikosov (A) vortices in the grains.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/62830-ceramic-transactions-materials-processing-design-grain-boundary-controlled-properties-fine-ceramics-ii-volume','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/62830-ceramic-transactions-materials-processing-design-grain-boundary-controlled-properties-fine-ceramics-ii-volume"><span>Ceramic transactions - Materials processing and design: Grain-<span class="hlt">boundary</span>-controlled properties of fine ceramics II. Volume 44</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>Niihara, Koichi; Ishizaki, Kozo; Isotani, Mitsuo</p> <p></p> <p>This volume contains selected papers presented at a workshop by the Japan Fine Ceramics Center, `Materials Processing and Design Through Better Control of Grain <span class="hlt">Boundaries</span>: Emphasizing Fine Ceramics II,` which was held March 17-19, 1994, in Koda-cho, Aichi, Japan. The focus of the workshop was the application of grain <span class="hlt">boundary</span> phenomena to materials processing and design. The topics covered included electronic materials, evaluation methods, structural materials, and interfaces. Also included is an illuminating overview of the <span class="hlt">current</span> status of work on grain <span class="hlt">boundary</span> assisted materials processing and design, particularly for fine ceramics. The volume`s chapter titles are: Electron Microscopy, Evaluation,more » Grain <span class="hlt">Boundary</span> Control and Design, Functional Ceramics, Composite Materials, Synthesis and Sintering, and Mechanical Properties.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97p1112M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97p1112M"><span>Pulsating flow and <span class="hlt">boundary</span> layers in viscous electronic hydrodynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moessner, Roderich; Surówka, Piotr; Witkowski, Piotr</p> <p>2018-04-01</p> <p>Motivated by experiments on a hydrodynamic regime in electron transport, we study the effect of an oscillating electric field in such a setting. We consider a long two-dimensional channel of width L , whose geometrical simplicity allows an analytical study as well as hopefully permitting an experimental realization. The response depends on viscosity ν , driving frequency ω , and ohmic heating coefficient γ via the dimensionless complex variable L/2ν (i ω +γ ) =i Ω +Σ . While at small Ω , we recover the static solution, a different regime appears at large Ω with the emergence of a <span class="hlt">boundary</span> layer. This includes a splitting of the location of maximal flow velocity from the center towards the edges of the <span class="hlt">boundary</span> layer, an increasingly reactive nature of the response, with the phase shift of the response varying across the channel. The scaling of the total optical conductance with L differs between the two regimes, while its frequency dependence resembles a Drude form throughout, even in the complete absence of ohmic heating, against which, at the same time, our results are stable. <span class="hlt">Current</span> estimates for transport coefficients in graphene and delafossites suggest that the <span class="hlt">boundary</span>-layer regime should be experimentally accessible.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SMaS...25i5020F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SMaS...25i5020F"><span>A discrete twin-<span class="hlt">boundary</span> approach for simulating the magneto-mechanical response of Ni-Mn-Ga</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Faran, Eilon; Shilo, Doron</p> <p>2016-09-01</p> <p>The design and optimization of ferromagnetic shape memory alloys (FSMA)-based devices require quantitative understanding of the dynamics of twin <span class="hlt">boundaries</span> within these materials. Here, we present a discrete twin <span class="hlt">boundary</span> modeling approach for simulating the behavior of an FSMA Ni-Mn-Ga crystal under combined magneto-mechanical loading conditions. The model is based on experimentally measured kinetic relations that describe the motion of individual twin <span class="hlt">boundaries</span> over a wide range of velocities. The resulting calculations capture the dynamic response of Ni-Mn-Ga and reveal the relations between fundamental material parameters and actuation performance at different frequencies of the magnetic field. In particular, we show that at high field rates, the magnitude of the lattice barrier that resists twin <span class="hlt">boundary</span> motion is the important property that determines the level of actuation strain, while the contribution of twinning stress property is minor. Consequently, type II twin <span class="hlt">boundaries</span>, whose lattice barrier is smaller compared to type I, are expected to show better actuation performance at high rates, irrespective of the differences in the twinning stress property between the two <span class="hlt">boundary</span> types. In addition, the simulation enables optimization of the actuation strain of a Ni-Mn-Ga crystal by adjusting the magnitude of the bias mechanical stress, thus providing direct guidelines for the design of actuating devices. <span class="hlt">Finally</span>, we show that the use of a linear kinetic law for simulating the twinning-based response is inadequate and results in incorrect predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhFl...27a5106M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhFl...27a5106M"><span>Vortex rings impinging on permeable <span class="hlt">boundaries</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mujal-Colilles, Anna; Dalziel, Stuart B.; Bateman, Allen</p> <p>2015-01-01</p> <p>Experiments with vortex rings impinging permeable and solid <span class="hlt">boundaries</span> are presented in order to investigate the influence of permeability. Utilizing Particle Image Velocimetry, we compared the behaviour of a vortex ring impinging four different reticulated foams (with permeability k ˜ 26 - 85 × 10-8 m2) and a solid <span class="hlt">boundary</span>. Results show how permeability affects the stretching phenomena of the vortex ring and the formation and evolution of the secondary vortex ring with opposite sign. Moreover, permeability also affects the macroscopic no-slip <span class="hlt">boundary</span> condition found on the solid <span class="hlt">boundary</span>, turning it into an apparent slip <span class="hlt">boundary</span> condition for the most permeable <span class="hlt">boundary</span>. The apparent slip-<span class="hlt">boundary</span> condition and the flux exchange between the ambient fluid and the foam are jointly responsible for both the modified formation of the secondary vortex and changes on the vortex ring diameter increase.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002PhDT........31V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002PhDT........31V"><span>CFD determination of flow perturbation <span class="hlt">boundary</span> conditions for seal rotordynamic modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Venkatesan, Ganesh</p> <p>2002-09-01</p> <p>A new approach has been developed and utilized to determine the flow field perturbations (i.e. disturbance due to rotor eccentricity and/or motion) upstream of and within a non-contacting seal. The results are proposed for use with bulk-flow perturbation and CFD-perturbation seal rotordynamic models, as well as in fully 3-D CFD models, to specify approximate <span class="hlt">boundary</span> conditions for the first-order variables at the computational domain inlet. The perturbation quantities were evaluated by subtracting the numerical flow field solutions corresponding to the concentric rotor position from that for an eccentric rotor position. The disturbance pressure quantities predicted from the numerical solutions were validated by comparing with previous pressure measurements. A parametric study was performed to understand the influence of upstream chamber height, seal clearance, shaft speed, whirl speed, zeroth-order streamwise and swirl velocities, and downstream pressure on the distribution of the first-order quantities in the upstream chamber, seal inlet and seal exit regions. Radially bulk-averaged first-order quantities were evaluated in the upstream chamber, as well as at the seal inlet and exit. The results were <span class="hlt">finally</span> presented in the form of generalized dimensionless <span class="hlt">boundary</span> condition correlations so that they can be applied to seal rotordynamic models over a wide range of operating conditions and geometries. To examine the effect of the proposed, approximate first-order <span class="hlt">boundary</span> conditions on the solutions of the fully 3-D CFD rotordynamic models, the first-order <span class="hlt">boundary</span> condition correlations for the upstream chamber were used to adjust the circumferential distribution of domain inlet values. The benefit of the <span class="hlt">boundary</span> condition expressions was assessed for two previously measured test cases, one for a gas seal and the other for a liquid seal. For the gas seal case, a significant improvement in the prediction of the cross-coupled stiffness, when including the proposed</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMSA33B1999H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMSA33B1999H"><span>Investigating TIME-GCM Atmospheric Tides for Different Lower <span class="hlt">Boundary</span> Conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haeusler, K.; Hagan, M. E.; Lu, G.; Forbes, J. M.; Zhang, X.; Doornbos, E.</p> <p>2013-12-01</p> <p>It has been recently established that atmospheric tides generated in the lower atmosphere significantly influence the geospace environment. In order to extend our knowledge of the various coupling mechanisms between the different atmospheric layers, we rely on model simulations. <span class="hlt">Currently</span> there exist two versions of the Global Scale Wave Model (GSWM), i.e. GSWM02 and GSWM09, which are used as a lower <span class="hlt">boundary</span> (ca. 30 km) condition for the Thermosphere-Ionosphere-Mesosphere-Electrodynamics General Circulation Model (TIME-GCM) and account for the upward propagating atmospheric tides that are generated in the troposphere and lower stratosphere. In this paper we explore the various TIME-GCM upper atmospheric tidal responses for different lower <span class="hlt">boundary</span> conditions and compare the model diagnostics with tidal results from satellite missions such as TIMED, CHAMP, and GOCE. We also quantify the differences between results associated with GSWM02 and GSWM09 forcing and results of TIMEGCM simulations using Modern-Era Retrospective Analysis for Research and Application (MERRA) data as a lower <span class="hlt">boundary</span> condition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920023250','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920023250"><span>Swept shock/<span class="hlt">boundary</span> layer interaction experiments in support of CFD code validation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Settles, G. S.; Lee, Y.</p> <p>1992-01-01</p> <p>Research on the topic of shock wave/turbulent <span class="hlt">boundary</span>-layer interaction was carried out during the past three years at the Penn State Gas Dynamics Laboratory. This report describes the experimental research program which provides basic knowledge and establishes new data on heat transfer in swept shock wave/<span class="hlt">boundary</span>-layer interactions. An equilibrium turbulent <span class="hlt">boundary</span>-layer on a flat plate is subjected to impingement by swept planar shock waves generated by a sharp fin. Five different interactions with fin angle ranging from 10 deg to 20 deg at freestream Mach numbers of 3.0 and 4.0 produce a variety of interaction strengths from weak to very strong. A foil heater generates a uniform heat flux over the flat plate surface, and miniature thin-film-resistance sensors mounted on it are used to measure the local surface temperature. The heat convection equation is then solved for the heat transfer distribution within an interaction, yielding a total uncertainty of about +/- 10 percent. These experimental data are compared with the results of numerical Navier-Stokes solutions which employ a k-epsilon turbulence model. <span class="hlt">Finally</span>, a simplified form of the peak heat transfer correlation for fin interactions is suggested.</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('http://adsabs.harvard.edu/abs/2018TMP...195..607J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018TMP...195..607J"><span>Quantum Gravitational Effects on the <span class="hlt">Boundary</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>James, F.; Park, I. Y.</p> <p>2018-04-01</p> <p>Quantum gravitational effects might hold the key to some of the outstanding problems in theoretical physics. We analyze the perturbative quantum effects on the <span class="hlt">boundary</span> of a gravitational system and the Dirichlet <span class="hlt">boundary</span> condition imposed at the classical level. Our analysis reveals that for a black hole solution, there is a contradiction between the quantum effects and the Dirichlet <span class="hlt">boundary</span> condition: the black hole solution of the one-particle-irreducible action no longer satisfies the Dirichlet <span class="hlt">boundary</span> condition as would be expected without going into details. The analysis also suggests that the tension between the Dirichlet <span class="hlt">boundary</span> condition and loop effects is connected with a certain mechanism of information storage on the <span class="hlt">boundary</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790025962','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790025962"><span>Interplanetary sector <span class="hlt">boundaries</span>, 1971 - 1973</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Klein, L.; Burlaga, L. F.</p> <p>1979-01-01</p> <p>Eighteen interplanetary sector <span class="hlt">boundary</span> crossings observed at 1 AU by the magnetometer on the IMP-6 spacecraft are discussed. The events were examined on many different time scales ranging from days on either side of the <span class="hlt">boundary</span> to high resolution measurements of 12.5 vectors per second. Two categories of <span class="hlt">boundaries</span> were found, one group being relatively thin and the other being thick. In many cases the field vector rotated in a plane from one polarity to the other. Only two of the transitions were null sheets. Using the minimum variance analysis to determine the normals to the plane of rotation, and assuming that this is the same as the normal to the sector <span class="hlt">boundary</span> surface, it was found that the normals were close to the ecliptic plane. An analysis of tangential discontinuities contained in 4-day periods about the events showed that their orientations were generally not related to the orientations of the sector <span class="hlt">boundary</span> surface, but rather their characteristics were about the same as those for discontinuities outside the sector <span class="hlt">boundaries</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19680000383','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19680000383"><span>Effects of high frequency <span class="hlt">current</span> in welding aluminum alloy 6061</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fish, R. E.</p> <p>1968-01-01</p> <p>Uncontrolled high frequency <span class="hlt">current</span> causes cracking in the heat-affected zone of aluminum alloy 6061 weldments during tungsten inert gas ac welding. Cracking developed when an improperly adjusted superimposed high frequency <span class="hlt">current</span> was agitating the semimolten metal in the areas of grain <span class="hlt">boundary</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/10150977','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/10150977"><span>Recursive recovery of Markov transition probabilities from <span class="hlt">boundary</span> value data</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>Patch, Sarah Kathyrn</p> <p>1994-04-01</p> <p>In an effort to mathematically describe the anisotropic diffusion of infrared radiation in biological tissue Gruenbaum posed an anisotropic diffusion <span class="hlt">boundary</span> value problem in 1989. In order to accommodate anisotropy, he discretized the temporal as well as the spatial domain. The probabilistic interpretation of the diffusion equation is retained; radiation is assumed to travel according to a random walk (of sorts). In this random walk the probabilities with which photons change direction depend upon their previous as well as present location. The forward problem gives <span class="hlt">boundary</span> value data as a function of the Markov transition probabilities. The inverse problem requiresmore » finding the transition probabilities from <span class="hlt">boundary</span> value data. Problems in the plane are studied carefully in this thesis. Consistency conditions amongst the data are derived. These conditions have two effects: they prohibit inversion of the forward map but permit smoothing of noisy data. Next, a recursive algorithm which yields a family of solutions to the inverse problem is detailed. This algorithm takes advantage of all independent data and generates a system of highly nonlinear algebraic equations. Pluecker-Grassmann relations are instrumental in simplifying the equations. The algorithm is used to solve the 4 x 4 problem. <span class="hlt">Finally</span>, the smallest nontrivial problem in three dimensions, the 2 x 2 x 2 problem, is solved.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880042081&hterms=high+current+electron+beam&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dhigh%2Bcurrent%2Belectron%2Bbeam','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880042081&hterms=high+current+electron+beam&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dhigh%2Bcurrent%2Belectron%2Bbeam"><span>A study of field-aligned <span class="hlt">currents</span> observed at high and low altitudes in the nightside magnetosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Elphic, R. C.; Craven, J. D.; Frank, L. A.; Sugiura, M.</p> <p>1988-01-01</p> <p>Field-aligned <span class="hlt">current</span> structures on auroral field lines observed at low and high altitudes using DE 1 and ISEE 2 magnetometer, and particle data observed when the spacecraft are in magnetic conjunction in the near-midnight magnetosphere, are investigated. To minimize latitudinal ambiguity, the plasma-sheet <span class="hlt">boundary</span> layer observed with ISEE 2 and the discrete aurora at the poleward edge of the auroral oval with DE 1 are studied. The overall <span class="hlt">current</span> observed at highest latitudes is flowing into the ionosphere, and is likely to be carried by ionospheric electrons flowing upward. There are, however, smaller-scale <span class="hlt">current</span> structures within this region. The sense and magnitude of the field-aligned <span class="hlt">currents</span> agree at the two sites. The ISEE 2 data suggests that the high-latitude downward <span class="hlt">current</span> corresponds to the high-latitude <span class="hlt">boundary</span> of the plasma-sheet <span class="hlt">boundary</span> layer, and may be associated with the ion beams observed there.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/306244-wiedemann-endash-franz-law-boundaries','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/306244-wiedemann-endash-franz-law-boundaries"><span>Wiedemann{endash}Franz law at <span class="hlt">boundaries</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>Mahan, G.D.; Bartkowiak, M.</p> <p>1999-02-01</p> <p>The full equations are derived for the resistances to the transport of heat and electricity through <span class="hlt">boundaries</span> of thermoelectrics. We show that the <span class="hlt">boundary</span> resistances of heat and electricity are proportional. This relationship is a <span class="hlt">boundary</span> form of the Wiedemann{endash}Franz law. We also show there is a <span class="hlt">boundary</span> Seebeck coefficient. {copyright} {ital 1999 American Institute of Physics.}</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19890037702&hterms=interactional+quality&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dinteractional%2Bquality','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890037702&hterms=interactional+quality&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dinteractional%2Bquality"><span>Vortex/<span class="hlt">boundary</span> layer interactions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cutler, A. D.; Bradshaw, P.</p> <p>1989-01-01</p> <p>Detailed and high quality measurements with hot-wires and pressure probes are presented for two different interactions between a vortex pair with common flow down and a turbulent <span class="hlt">boundary</span> layer. The interactions studied have larger values of the vortex circulation parameter than those studied previously. The results indicate that the <span class="hlt">boundary</span> layer under the vortex pair is thinned by lateral divergence and that <span class="hlt">boundary</span> layer fluid is entrained into the vortex. The effect of the interaction on the vortex core (other than the inviscid effect of the image vortices behind the surface) is small.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT.......186A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT.......186A"><span>Modeling Electrothermal Plasma with <span class="hlt">Boundary</span> Layer Effects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>AlMousa, Nouf Mousa A.</p> <p></p> <p>Electrothermal plasma sources produce high-density (1023-10 28 /m3) and high temperature (1-5 eV) plasmas that are of interest for a variety of applications such as hypervelocity launch devices, fusion reactor pellet injectors, and pulsed thrusters for small satellites. Also, the high heat flux (up to 100 GW/m2) and high pressure (100s MPa) of electrothermal (ET) plasmas allow for the use of such facilities as a source of high heat flux to simulate off-normal events in Tokamak fusion reactors. Off-normal events like disruptions, thermal and <span class="hlt">current</span> quenches, are the perfect recipes for damage of plasma facing components (PFC). Successful operation of a fusion reactor requires comprehensive understanding of material erosion behavior. The extremely high heat fluxes deposited in PFCs melt and evaporate or directly sublime the exposed surfaces, which results in a thick vapor/melt <span class="hlt">boundary</span> layer adjacent to the solid wall structure. The accumulating <span class="hlt">boundary</span> layers provide a self-protecting nature by attenuating the radiant energy transport to the PFCs. The ultimate goal of this study is to develop a reliable tool to adequately simulate the effect of the <span class="hlt">boundary</span> layers on the formation and flow of the energetic ET plasma and its impact on exposed surfaces erosion under disruption like conditions. This dissertation is a series of published journals/conferences papers. The first paper verified the existence of the vapor shield that evolved at the <span class="hlt">boundary</span> layer under the typical operational conditions of the NC State University ET plasma facilities PIPE and SIRENS. Upon the verification of the vapor shield, the second paper proposed novel model to simulate the evolution of the <span class="hlt">boundary</span> layer and its effectiveness in providing a self-protecting nature for the exposed plasma facing surfaces. The developed models simulate the radiant heat flux attenuation through an optically thick <span class="hlt">boundary</span> layer. The models were validated by comparing the simulation results to experimental</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18517516','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18517516"><span>Wind and <span class="hlt">boundary</span> layers in Rayleigh-Bénard convection. II. <span class="hlt">Boundary</span> layer character and scaling.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>van Reeuwijk, Maarten; Jonker, Harm J J; Hanjalić, Kemo</p> <p>2008-03-01</p> <p>The scaling of the kinematic <span class="hlt">boundary</span> layer thickness lambda(u) and the friction factor C(f) at the top and bottom walls of Rayleigh-Bénard convection is studied by direct numerical simulation (DNS). By a detailed analysis of the friction factor, a new parameterisation for C(f) and lambda(u) is proposed. The simulations were made of an L/H=4 aspect-ratio domain with periodic lateral <span class="hlt">boundary</span> conditions at Ra=(10(5), 10(6), 10(7), 10(8)) and Pr=1. The continuous spectrum, as well as significant forcing due to Reynolds stresses, clearly indicates a turbulent character of the <span class="hlt">boundary</span> layer, while viscous effects cannot be neglected, judging from the scaling of classical integral <span class="hlt">boundary</span> layer parameters with Reynolds number. Using a conceptual wind model, we find that the friction factor C(f) should scale proportionally to the thermal <span class="hlt">boundary</span> layer thickness as C(f) proportional variant lambda(Theta)/H, while the kinetic <span class="hlt">boundary</span> layer thickness lambda(u) scales inversely proportionally to the thermal <span class="hlt">boundary</span> layer thickness and wind Reynolds number lambda(u)/H proportional variant (lambda(Theta)/H)(-1)Re(-1). The predicted trends for C(f) and lambda(u) are in agreement with DNS results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008JGRC..113.7018F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008JGRC..113.7018F"><span>Waves plus <span class="hlt">currents</span> at a right angle: The rippled bed case</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Faraci, C.; Foti, E.; Musumeci, R. E.</p> <p>2008-07-01</p> <p>The present paper deals with wave plus <span class="hlt">current</span> flow over a fixed rippled bed. More precisely, modifications of the <span class="hlt">current</span> profiles due to the superimposition of orthogonal cylindrical waves have been investigated experimentally. Since the experimental setup permitted only the wave dominated regime to be investigated (i.e., the regime where orbital velocity is larger than <span class="hlt">current</span> velocity), also a numerical k-ɛ turbulence closure model has been developed in order to study a wider range of parameters, thus including the <span class="hlt">current</span> dominated regime (i.e., where <span class="hlt">current</span> velocity is larger than wave orbital one). In both cases a different response with respect to the flat bed case has been found. Indeed, in the flat bed case laminar wave <span class="hlt">boundary</span> layers in a wave dominated regime induce a decrease in bottom shear stresses, while the presence of a rippled bed behaves as a macroroughness, which causes the wave <span class="hlt">boundary</span> layer to become turbulent and therefore the <span class="hlt">current</span> velocity near the bottom to be smaller than the one in the case of <span class="hlt">current</span> only, with a consequent increase in the <span class="hlt">current</span> bottom roughness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NuPhB.915..119W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NuPhB.915..119W"><span>Thermodynamic limit and <span class="hlt">boundary</span> energy of the su(3) spin chain with non-diagonal <span class="hlt">boundary</span> fields</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wen, Fakai; Yang, Tao; Yang, Zhanying; Cao, Junpeng; Hao, Kun; Yang, Wen-Li</p> <p>2017-02-01</p> <p>We investigate the thermodynamic limit of the su (n)-invariant spin chain models with unparallel <span class="hlt">boundary</span> fields. It is found that the contribution of the inhomogeneous term in the associated T-Q relation to the ground state energy does vanish in the thermodynamic limit. This fact allows us to calculate the <span class="hlt">boundary</span> energy of the system. Taking the su (2) (or the XXX) spin chain and the su (3) spin chain as concrete examples, we have studied the corresponding <span class="hlt">boundary</span> energies of the models. The method used in this paper can be generalized to study the thermodynamic properties and <span class="hlt">boundary</span> energy of other high rank models with non-diagonal <span class="hlt">boundary</span> fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JPhA...47H5001L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JPhA...47H5001L"><span>Sustained <span class="hlt">currents</span> in coupled diffusive systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Larralde, Hernán; Sanders, David P.</p> <p>2014-08-01</p> <p>Coupling two diffusive systems may give rise to a nonequilibrium stationary state (NESS) with a non-trivial persistent, circulating <span class="hlt">current</span>. We study a simple example that is exactly soluble, consisting of random walkers with different biases towards a reflecting <span class="hlt">boundary</span>, modelling, for example, Brownian particles with different charge states in an electric field. We obtain analytical expressions for the concentrations and <span class="hlt">currents</span> in the NESS for this model, and exhibit the main features of the system by numerical simulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20010091016','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010091016"><span>Antimatter Production at a Potential <span class="hlt">Boundary</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>LaPointe, Michael R.; Reddy, Dhanireddy (Technical Monitor)</p> <p>2001-01-01</p> <p><span class="hlt">Current</span> antiproton production techniques rely on high-energy collisions between beam particles and target nuclei to produce particle and antiparticle pairs, but inherently low production and capture efficiencies render these techniques impractical for the cost-effective production of antimatter for space propulsion and other commercial applications. Based on Dirac's theory of the vacuum field, a new antimatter production concept is proposed in which particle-antiparticle pairs are created at the <span class="hlt">boundary</span> of a steep potential step formed by the suppression of the local vacuum fields. <span class="hlt">Current</span> antimatter production techniques are reviewed, followed by a description of Dirac's relativistic quantum theory of the vacuum state and corresponding solutions for particle tunneling and reflection from a potential barrier. The use of the Casimir effect to suppress local vacuum fields is presented as a possible technique for generating the sharp potential gradients required for particle-antiparticle pair creation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24123651','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24123651"><span>Creating technological <span class="hlt">boundaries</span> to protect bedtime: examining work-home <span class="hlt">boundary</span> management, psychological detachment and sleep.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Barber, Larissa K; Jenkins, Jade S</p> <p>2014-08-01</p> <p>This study examined the mechanism by which information and communication technology (ICT) use at home for work purposes may affect sleep. In this investigation, data from 315 employees were used to examine the indirect effect of ICT use at home on sleep outcomes through psychological detachment, and how <span class="hlt">boundary</span> creation may moderate this effect. Results revealed the indirect effect of increased work-home <span class="hlt">boundary</span> crossing on sleep (quantity, quality and consistency) through psychological detachment occurred only among individuals with low <span class="hlt">boundaries</span> around ICT use and not among those with high <span class="hlt">boundaries</span>. These results suggest that creating <span class="hlt">boundaries</span> around work-relevant ICT use while at home is beneficial to sleep as a recovery process through being able to psychologically disengage from work. Copyright © 2013 John Wiley & Sons, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS1015e2005D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS1015e2005D"><span>Research of Steel-dielectric Transition Using Subminiature Eddy-<span class="hlt">current</span> Transducer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dmitriev, S. F.; Malikov, V. N.; Sagalakov, A. M.; Ishkov, A. V.</p> <p>2018-05-01</p> <p>The research aims to develop a subminiature transducer for electrical steel investigation. The authors determined the capability to study steel characteristics at different depths based on variations of eddy-<span class="hlt">current</span> transducer amplitude at the steel-dielectric <span class="hlt">boundary</span>. A subminiature transformer-type transducer was designed, which enables to perform local investigations of ferromagnetic materials using an eddy-<span class="hlt">current</span> method based on local studies of the steel electrical conductivity. Having the designed transducer as a basis, a hardware-software complex was built to perform experimental studies of steel at the interface <span class="hlt">boundary</span>. Test results are reported for a specimen with continuous and discrete measurements taken at different frequencies. The article provides the key technical information about the eddy <span class="hlt">current</span> transformer used and describes the methodology of measurements that makes it possible to control steel to dielectric transition.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19720017651','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19720017651"><span>Transpiration and film cooling <span class="hlt">boundary</span> layer computer program. Volume 2: Computer program and user's manual</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gloss, R. J.</p> <p>1971-01-01</p> <p>A finite difference turbulent <span class="hlt">boundary</span> layer computer program which allows for mass transfer wall cooling and equilibrium chemistry effects is presented. The program is capable of calculating laminar or turbulent <span class="hlt">boundary</span> layer solutions for an arbitrary ideal gas or an equilibrium hydrogen oxygen system. Either two dimensional or axisymmetric geometric configurations may be considered. The equations are solved, in nondimension-alized physical coordinates, using the implicit Crank-Nicolson technique. The finite difference forms of the conservation of mass, momentum, total enthalpy and elements equations are linearized and uncoupled, thereby generating easily solvable tridiagonal sets of algebraic equations. A detailed description of the computer program, as well as a program user's manual is provided. Detailed descriptions of all <span class="hlt">boundary</span> layer subroutines are included, as well as a section defining all program symbols of principal importance. Instructions are then given for preparing card input to the program and for interpreting the printed output. <span class="hlt">Finally</span>, two sample cases are included to illustrate the use of the program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NatCo...814685L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NatCo...814685L"><span>MicroRNA filters Hox temporal transcription noise to confer <span class="hlt">boundary</span> formation in the spinal cord</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Chung-Jung; Hong, Tian; Tung, Ying-Tsen; Yen, Ya-Ping; Hsu, Ho-Chiang; Lu, Ya-Lin; Chang, Mien; Nie, Qing; Chen, Jun-An</p> <p>2017-03-01</p> <p>The initial rostrocaudal patterning of the neural tube leads to differential expression of Hox genes that contribute to the specification of motor neuron (MN) subtype identity. Although several 3' Hox mRNAs are expressed in progenitors in a noisy manner, these Hox proteins are not expressed in the progenitors and only become detectable in postmitotic MNs. MicroRNA biogenesis impairment leads to precocious expression and propagates the noise of Hoxa5 at the protein level, resulting in an imprecise Hoxa5-Hoxc8 <span class="hlt">boundary</span>. Here we uncover, using in silico simulation, two feed-forward Hox-miRNA loops accounting for the precocious and noisy Hoxa5 expression, as well as an ill-defined <span class="hlt">boundary</span> phenotype in Dicer mutants. <span class="hlt">Finally</span>, we identify mir-27 as a major regulator coordinating the temporal delay and spatial <span class="hlt">boundary</span> of Hox protein expression. Our results provide a novel trans Hox-miRNA circuit filtering transcription noise and controlling the timing of protein expression to confer robust individual MN identity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050217285','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050217285"><span>Microgravity Effects on Plant <span class="hlt">Boundary</span> Layers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Stutte, Gary; Monje, Oscar</p> <p>2005-01-01</p> <p>The goal of these series of experiment was to determine the effects of microgravity conditions on the developmental <span class="hlt">boundary</span> layers in roots and leaves and to determine the effects of air flow on <span class="hlt">boundary</span> layer development. It is hypothesized that microgravity induces larger <span class="hlt">boundary</span> layers around plant organs because of the absence of buoyancy-driven convection. These larger <span class="hlt">boundary</span> layers may affect normal metabolic function because they may reduce the fluxes of heat and metabolically active gases (e.g., oxygen, water vapor, and carbon dioxide. These experiments are to test whether there is a change in <span class="hlt">boundary</span> layer associated with microgravity, quantify the change if it exists, and determine influence of air velocity on <span class="hlt">boundary</span> layer thickness under different gravity conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28663902','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28663902"><span>Automatic segmentation of nine retinal layer <span class="hlt">boundaries</span> in OCT images of non-exudative AMD patients using deep learning and graph search.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Fang, Leyuan; Cunefare, David; Wang, Chong; Guymer, Robyn H; Li, Shutao; Farsiu, Sina</p> <p>2017-05-01</p> <p>We present a novel framework combining convolutional neural networks (CNN) and graph search methods (termed as CNN-GS) for the automatic segmentation of nine layer <span class="hlt">boundaries</span> on retinal optical coherence tomography (OCT) images. CNN-GS first utilizes a CNN to extract features of specific retinal layer <span class="hlt">boundaries</span> and train a corresponding classifier to delineate a pilot estimate of the eight layers. Next, a graph search method uses the probability maps created from the CNN to find the <span class="hlt">final</span> <span class="hlt">boundaries</span>. We validated our proposed method on 60 volumes (2915 B-scans) from 20 human eyes with non-exudative age-related macular degeneration (AMD), which attested to effectiveness of our proposed technique.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27812226','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27812226"><span>How Students View the <span class="hlt">Boundaries</span> Between Their Science and Religious Education Concerning the Origins of Life and the Universe.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Billingsley, Berry; Brock, Richard; Taber, Keith S; Riga, Fran</p> <p>2016-05-01</p> <p>Internationally in secondary schools, lessons are typically taught by subject specialists, raising the question of how to accommodate teaching which bridges the sciences and humanities. This is the first study to look at how students make sense of the teaching they receive in two subjects (science and religious education [RE]) when one subject's curriculum explicitly refers to cross-disciplinary study and the other does not. Interviews with 61 students in seven schools in England suggested that students perceive a permeable <span class="hlt">boundary</span> between science and their learning in science lessons and also a permeable <span class="hlt">boundary</span> between religion and their learning in RE lessons, yet perceive a firm <span class="hlt">boundary</span> between science lessons and RE lessons. We concluded that it is unreasonable to expect students to transfer instruction about cross-disciplinary perspectives across such impermeable subject <span class="hlt">boundaries</span>. <span class="hlt">Finally</span>, we consider the implications of these findings for the successful management of cross-disciplinary education.</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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