Sample records for layer evolution model

  1. Thin layer model for nonlinear evolution of the Rayleigh-Taylor instability

    NASA Astrophysics Data System (ADS)

    Zhao, K. G.; Wang, L. F.; Xue, C.; Ye, W. H.; Wu, J. F.; Ding, Y. K.; Zhang, W. Y.

    2018-03-01

    On the basis of the thin layer approximation [Ott, Phys. Rev. Lett. 29, 1429 (1972)], a revised thin layer model for incompressible Rayleigh-Taylor instability has been developed to describe the deformation and nonlinear evolution of the perturbed interface. The differential equations for motion are obtained by analyzing the forces (the gravity and pressure difference) of fluid elements (i.e., Newton's second law). The positions of the perturbed interface are obtained from the numerical solution of the motion equations. For the case of vacuum on both sides of the layer, the positions of the upper and lower interfaces obtained from the revised thin layer approximation agree with that from the weakly nonlinear (WN) model of a finite-thickness fluid layer [Wang et al., Phys. Plasmas 21, 122710 (2014)]. For the case considering the fluids on both sides of the layer, the bubble-spike amplitude from the revised thin layer model agrees with that from the WN model [Wang et al., Phys. Plasmas 17, 052305 (2010)] and the expanded Layzer's theory [Goncharov, Phys. Rev. Lett. 88, 134502 (2002)] in the early nonlinear growth regime. Note that the revised thin layer model can be applied to investigate the perturbation growth at arbitrary Atwood numbers. In addition, the large deformation (the large perturbed amplitude and the arbitrary perturbed distributions) in the initial stage can also be described by the present model.

  2. Evolution of fault zones in carbonates with mechanical stratigraphy - Insights from scale models using layered cohesive powder

    NASA Astrophysics Data System (ADS)

    van Gent, Heijn W.; Holland, Marc; Urai, Janos L.; Loosveld, Ramon

    2010-09-01

    We present analogue models of the formation of dilatant normal faults and fractures in carbonate fault zones, using cohesive hemihydrate powder (CaSO 4·½H 2O). The evolution of these dilatant fault zones involves a range of processes such as fragmentation, gravity-driven breccia transport and the formation of dilatant jogs. To allow scaling to natural prototypes, extensive material characterisation was done. This showed that tensile strength and cohesion depend on the state of compaction, whereas the friction angle remains approximately constant. In our models, tensile strength of the hemihydrate increases with depth from 9 to 50 Pa, while cohesion increases from 40 to 250 Pa. We studied homogeneous and layered material sequences, using sand as a relatively weak layer and hemihydrate/graphite mixtures as a slightly stronger layer. Deformation was analyzed by time-lapse photography and Particle Image Velocimetry (PIV) to calculate the evolution of the displacement field. With PIV the initial, predominantly elastic deformation and progressive localization of deformation are observed in detail. We observed near-vertical opening-mode fractures near the surface. With increasing depth, dilational shear faults were dominant, with releasing jogs forming at fault-dip variations. A transition to non-dilatant shear faults was observed near the bottom of the model. In models with mechanical stratigraphy, fault zones are more complex. The inferred stress states and strengths in different parts of the model agree with the observed transitions in the mode of deformation.

  3. Modelling of active layer thickness evolution on James Ross Island in 2006-2015

    NASA Astrophysics Data System (ADS)

    Hrbáček, Filip; Uxa, Tomáš

    2017-04-01

    Antarctic Peninsula region has been considered as one of the most rapidly warming areas on the Earth. However, the recent studies (Turner et al., 2016; Oliva et al., 2017) showed that significant air temperature cooling began around 2000 and has continued until present days. The climate cooling led to reduction of active layer thickness in several parts of Antarctic Peninsula region during decade 2006-2015, but the information about spatiotemporal variability of active layer thickness across the region remains largely incoherent due to lack of active layer temperature data from deeper profiles. Valuable insights into active layer thickness evolution in Antarctic Peninsula region can be, however, provided by thermal modelling techniques. These have been widely used to study the active layer dynamics in different regions of Arctic since 1990s. By contrast, they have been employed much less in Antarctica. In this study, we present our first results from two equilibrium models, the Stefan and Kudryavtsev equations, that were applied to calculate the annual active layer thickness based on ground temperature data from depth of 5 cm on one site on James Ross Island, Eastern Antarctic Peninsula, in period 2006/07 to 2014/15. Study site (Abernethy Flats) is located in the central part of the major ice-free area of James Ross Island called Ulu Peninsula. Monitoring of air temperature 2 m above ground surface and ground temperature in 50 cm profile began on January 2006. The profile was extended under the permafrost table down to 75 cm in February 2012, which allowed precise determination of active layer thickness, defined as a depth of 0°C isotherm, in period 2012 to 2015. The active layer thickness in the entire observation period was reconstructed using the Stefan and Kudryavtsev models, which were driven by ground temperature data from depth of 5 cm and physical parameters of the ground obtained by laboratory analyses (moisture content and bulk density) and calculations

  4. Quasi-Steady Evolution of Hillslopes in Layered Landscapes: An Analytic Approach

    NASA Astrophysics Data System (ADS)

    Glade, R. C.; Anderson, R. S.

    2018-01-01

    Landscapes developed in layered sedimentary or igneous rocks are common on Earth, as well as on other planets. Features such as hogbacks, exposed dikes, escarpments, and mesas exhibit resistant rock layers adjoining more erodible rock in tilted, vertical, or horizontal orientations. Hillslopes developed in the erodible rock are typically characterized by steep, linear-to-concave slopes or "ramps" mantled with material derived from the resistant layers, often in the form of large blocks. Previous work on hogbacks has shown that feedbacks between weathering and transport of the blocks and underlying soft rock can create relief over time and lead to the development of concave-up slope profiles in the absence of rilling processes. Here we employ an analytic approach, informed by numerical modeling and field data, to describe the quasi-steady state behavior of such rocky hillslopes for the full spectrum of resistant layer dip angles. We begin with a simple geometric analysis that relates structural dip to erosion rates. We then explore the mechanisms by which our numerical model of hogback evolution self-organizes to meet these geometric expectations, including adjustment of soil depth, erosion rates, and block velocities along the ramp. Analytical solutions relate easily measurable field quantities such as ramp length, slope, block size, and resistant layer dip angle to local incision rate, block velocity, and block weathering rate. These equations provide a framework for exploring the evolution of layered landscapes and pinpoint the processes for which we require a more thorough understanding to predict their evolution over time.

  5. Steady evolution of hillslopes in layered landscapes: self-organization of a numerical hogback

    NASA Astrophysics Data System (ADS)

    Glade, R.; Anderson, R. S.

    2017-12-01

    Landscapes developed in layered sedimentary or igneous rocks are common across Earth, as well as on other planets. Features such as hogbacks, exposed dikes, escarpments and mesas exhibit resistant rock layers in tilted, vertical, or horizontal orientation­s adjoining more erodible rock. Hillslopes developed in the erodible rock are typically characterized by steep, linear-to-concave slopes or "ramps" mantled with material derived from the resistant layers, often in the form of large blocks. Our previous work on hogbacks has shown that feedbacks between weathering and transport of the blocks and underlying soft rock are fundamental to their formation; our numerical model incorporating these feedbacks explain the development of commonly observed concave-up slope profiles in the absence of rilling processes. Here we employ an analytic approach to describe the steady behavior of our model, in which hillslope form and erosion rates remain constant in the reference frame of the retreating feature. We first revisit a simple geometric analysis that relates structural dip to erosion rates. We then explore the mechanisms by which our numerical model of hogback evolution self-organizes to meet these geometric expectations. Autogenic adjustment of soil depth, slope and erosion rates enables efficient transport of resistant blocks; this allows erosion of the resistant layer to keep up with base level fall rate, leading to steady evolution of the feature. Analytic solutions relate easily measurable field quantities such as ramp length, slope, block size and resistant layer dip angle to local incision rate, block velocity, and block weathering rate. These equations provide a framework for exploring the evolution of layered landscapes, and pinpoint the processes for which we require a more thorough understanding to predict the evolution of such signature landscapes over time.

  6. Near-inertial kinetic energy budget of the mixed layer and shear evolution in the transition layer in the Arabian Sea during the monsoons

    NASA Astrophysics Data System (ADS)

    Majumder, Sudip; Tandon, Amit; Rudnick, Daniel L.; Thomas Farrar, J.

    2015-09-01

    We present the horizontal kinetic energy (KE) balance of near-inertial currents in the mixed layer and explain shear evolution in the transition layer using observations from a mooring at 15.26° N in the Arabian Sea during the southwest monsoon. The highly sheared and stratified transition layer at the mixed-layer base varies between 5 m and 35 m and correlates negatively with the wind stress. Results from the mixed layer near-inertial KE (NIKE) balance suggest that wind energy at times can energize the transition layer and at other times is fully utilized within the mixed layer. A simple two layer model is utilized to study the shear evolution in the transition layer and shown to match well with observations. The shear production in this model arises from alignment of wind stress and shear. Although the winds are unidirectional during the monsoon, the shear in the transition layer is predominantly near-inertial. The near-inertial shear bursts in the observations show the same phasing and magnitude at near-inertial frequencies as the wind-shear alignment term.

  7. In Situ Chemical Imaging of Solid-Electrolyte Interphase Layer Evolution in Li–S Batteries

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

    Nandasiri, Manjula I.; Camacho-Forero, Luis E.; Schwarz, Ashleigh M.

    Parasitic reactions of electrolyte and polysulfide with the Li-anode in lithium sulfur (Li-S) batteries lead to the formation of solid-electrolyte interphase (SEI) layers, which are the major reason behind severe capacity fading in these systems. Despite numerous studies, the evolution mechanism of the SEI layer and specific roles of polysulfides and other electrolyte components are still unclear. Here, we report an in-situ X-ray photoelectron spectroscopy (XPS) and chemical imaging analysis combined with ab initio molecular dynamics (AIMD) computational modeling to gain fundamental understanding regarding the evolution of SEI layers on Li-anodes within Li-S batteries. A multi-modal approach involving AIMD modelingmore » and in-situ XPS characterization uniquely reveals the chemical identity and distribution of active participants in parasitic reactions as well as the SEI layer evolution mechanism. The SEI layer evolution has three major stages: the formation of a primary composite mixture phase involving stable lithium compounds (Li 2S, LiF, Li 2O etc); and formation of a secondary matrix type phase due to cross interaction between reaction products and electrolyte components, which is followed by a highly dynamic mono-anionic polysulfide (i.e. LiS 5) fouling process. In conclusion, these new molecular-level insights into the SEI layer evolution on Li- anodes are crucial for delineating effective strategies for the development of Li–S batteries.« less

  8. In Situ Chemical Imaging of Solid-Electrolyte Interphase Layer Evolution in Li–S Batteries

    DOE PAGES

    Nandasiri, Manjula I.; Camacho-Forero, Luis E.; Schwarz, Ashleigh M.; ...

    2017-05-03

    Parasitic reactions of electrolyte and polysulfide with the Li-anode in lithium sulfur (Li-S) batteries lead to the formation of solid-electrolyte interphase (SEI) layers, which are the major reason behind severe capacity fading in these systems. Despite numerous studies, the evolution mechanism of the SEI layer and specific roles of polysulfides and other electrolyte components are still unclear. Here, we report an in-situ X-ray photoelectron spectroscopy (XPS) and chemical imaging analysis combined with ab initio molecular dynamics (AIMD) computational modeling to gain fundamental understanding regarding the evolution of SEI layers on Li-anodes within Li-S batteries. A multi-modal approach involving AIMD modelingmore » and in-situ XPS characterization uniquely reveals the chemical identity and distribution of active participants in parasitic reactions as well as the SEI layer evolution mechanism. The SEI layer evolution has three major stages: the formation of a primary composite mixture phase involving stable lithium compounds (Li 2S, LiF, Li 2O etc); and formation of a secondary matrix type phase due to cross interaction between reaction products and electrolyte components, which is followed by a highly dynamic mono-anionic polysulfide (i.e. LiS 5) fouling process. In conclusion, these new molecular-level insights into the SEI layer evolution on Li- anodes are crucial for delineating effective strategies for the development of Li–S batteries.« less

  9. In Situ Chemical Imaging of Solid-Electrolyte Interphase Layer Evolution in Li–S Batteries

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

    Nandasiri, Manjula I.; Camacho-Forero, Luis E.; Schwarz, Ashleigh M.

    Parasitic reactions of electrolyte and polysulfide with the Li-anode in lithium sulfur (Li-S) batteries lead to the for-mation of solid electrolyte interphase (SEI) layers, which are the major reason behind severe capacity fading in these systems. Despite numerous studies, the evolution mechanism of the SEI layer and specific roles of polysulfides and oth-er electrolyte components are still unclear. We report an in-situ X-ray photoelectron spectroscopy (XPS) and chemical imaging analysis combined with ab initio molecular dynamics (AIMD) computational modeling to gain fundamental understanding regarding the evolution of SEI layers on Li-anodes within Li-S batteries. A multi-modal approach in-volving AIMD modelingmore » and in-situ XPS characterization uniquely reveals the chemical identity and distribution of active participants in parasitic reactions as well as the SEI layer evolution mechanism. The SEI layer evolution has three major stages: the formation of a primary composite mixture phase involving stable lithium compounds (Li2S, LiF, Li2O etc); and formation of a secondary matrix type phase due to cross interaction between reaction products and elec-trolyte components, which is followed by a highly dynamic mono-anionic polysulfide (i.e. LiS5) fouling process. These new molecular-level insights into the SEI layer evolution on Li- anodes are crucial for delineating effective strategies for the development of Li–S batteries.« less

  10. Boundary layer evolution over the central Himalayas from radio wind profiler and model simulations

    NASA Astrophysics Data System (ADS)

    Singh, Narendra; Solanki, Raman; Ojha, Narendra; Janssen, Ruud H. H.; Pozzer, Andrea; Dhaka, Surendra K.

    2016-08-01

    We investigate the time evolution of the Local Boundary Layer (LBL) for the first time over a mountain ridge at Nainital (79.5° E, 29.4° N, 1958 m a.m.s.l.) in the central Himalayan region, using a radar wind profiler (RWP) during November 2011 to March 2012, as a part of the Ganges Valley Aerosol Experiment (GVAX). We restrict our analysis to clear-sunny days, resulting in a total of 78 days of observations. The standard criterion of the peak in the signal-to-noise ratio (S / N) profile was found to be inadequate in the characterization of mixed layer (ML) top at this site. Therefore, we implemented a criterion of S / N > 6 dB for the characterization of the ML and the resulting estimations are shown to be in agreement with radiosonde measurements over this site. The daytime average (05:00-10:00 UTC) observed boundary layer height ranges from 440 ± 197 m in November (late autumn) to 766 ± 317 m above ground level (a.g.l.) in March (early spring). The observations revealed a pronounced impact of mountain topography on the LBL dynamics during March, when strong winds (> 5.6 m s-1) lead to LBL heights of 650 m during nighttime. The measurements are further utilized to evaluate simulations from the Weather Research and Forecasting (WRF) model. WRF simulations captured the day-to-day variations up to an extent (r2 = 0.5), as well as the mean diurnal variations (within 1σ variability). The mean biases in the daytime average LBL height vary from -7 % (January) to +30 % (February) between model and observations, except during March (+76 %). Sensitivity simulations using a mixed layer model (MXL/MESSy) indicated that the springtime overestimation of LBL would lead to a minor uncertainty in simulated surface ozone concentrations. However, it would lead to a significant overestimation of the dilution of black carbon aerosols at this site. Our work fills a gap in observations of local boundary layer over this complex terrain in the Himalayas, and highlights the need for

  11. Numerical modeling studies of wake vortex transport and evolution within the planetary boundary layer

    NASA Technical Reports Server (NTRS)

    Lin, Yuh-Lang; Arya, S. Pal; Kaplan, Michael L.

    1994-01-01

    The proposed research involves four tasks. The first of these is to simulate accurately the turbulent processes in the atmospheric boundary layer. TASS was originally developed to study meso-gamma scale phenomena, such as tornadic storms, microbursts and windshear effects in terminal areas. Simulation of wake vortex evolution, however, will rely on appropriate representation of the physical processes in the surface layer and mixed layer. This involves two parts. First, a specified heat flux boundary condition must be implemented at the surface. Using this boundary condition, simulation results will be compared to experimental data and to other model results for validation. At this point, any necessary changes to the model will be implemented. Next, a surface energy budget parameterization will be added to the model. This will enable calculation of the surface fluxes by accounting for the radiative heat transfer to and from the ground and heat loss to the soil rather than simple specification of the fluxes. The second task involves running TASS with prescribed wake vortices in the initial condition. The vortex models will be supplied by NASA Langley Research Center. Sensitivity tests will be performed on different meteorological environments in the atmospheric boundary layer, which include stable, neutral, and unstable stratifications, calm and severe wind conditions, and dry and wet conditions. Vortex strength may be varied as well. Relevant non-dimensional parameters will include the following: Richardson number or Froude number, Bowen ratio, and height to length scale ratios. The model output will be analyzed and visualized to better understand the transport, decay, and growth rates of the wake vortices. The third task involves running simulations using observed data. MIT Lincoln Labs is currently planning field experiments at the Memphis airport to measure both meteorological conditions and wake vortex characteristics. Once this data becomes available, it can be

  12. Lidar observation of Eyjafjallajoekull ash layer evolution above the Swiss Plateau

    NASA Astrophysics Data System (ADS)

    Simeonov, Valentin; Dinoev, Todor; Parlange, Mark; Serikov, Ilya; Calpini, Bertrand; Wienhold, F.; Engel, I.; Brabec, M.; Crisian, A.; Peter, T.; Mitev, Valentin; Matthey, R.

    2010-05-01

    The Iceland volcano Eyjafjallajökull started to emit significant amounts of volcanic ash and SO2 on 15th April 2010, following the initial eruption on 20th March 2010. In the next days, the ash was dispersed over large parts of Europe resulting in the closure of the major part of the European airspace. Information about spatial and temporal evolution of the cloud was needed urgently to define the conditions for opening the airspace. Satellite, airborne and ground observations together with meteorological models were used to evaluate the cloud propagation and evolution. While the horizontal extents of the volcanic cloud were accurately captured by satellite images, it remained difficult to obtain accurate information about the cloud base and top height, density and dynamics. During this event lidars demonstrated that they were the only ground based instruments allowing monitoring of the vertical distribution of the volcanic ash. Here we present observational results showing the evolution of the volcanic layer over the Swiss plateau. The measurements were carried out by one Raman lidar located in Payerne, two elastic lidars located in Neuchatel and Zurich, and a backscatter sonde launched from Zurich. The observations by the lidars have shown very similar time evolution, coherent with the backscatter sonde profiles and characterized by the appearance of the ash layer on the evening of 16th, followed by descend to 2-3 km during the next day and final mixing with the ABL on 19th. Simultaneous water vapor data from the Payerne lidar show low water content of the ash layer. The CSEM and EPFL gratefully acknowledge the financial support by the European Commission under grant RICA-025991.

  13. Reversible adapting layer produces robust single-crystal electrocatalyst for oxygen evolution.

    PubMed

    Tung, Ching-Wei; Hsu, Ying-Ya; Shen, Yen-Ping; Zheng, Yixin; Chan, Ting-Shan; Sheu, Hwo-Shuenn; Cheng, Yuan-Chung; Chen, Hao Ming

    2015-08-28

    Electrochemically converting water into oxygen/hydrogen gas is ideal for high-density renewable energy storage in which robust electrocatalysts for efficient oxygen evolution play crucial roles. To date, however, electrocatalysts with long-term stability have remained elusive. Here we report that single-crystal Co3O4 nanocube underlay with a thin CoO layer results in a high-performance and high-stability electrocatalyst in oxygen evolution reaction. An in situ X-ray diffraction method is developed to observe a strong correlation between the initialization of the oxygen evolution and the formation of active metal oxyhydroxide phase. The lattice of skin layer adapts to the structure of the active phase, which enables a reversible facile structural change that facilitates the chemical reactions without breaking the scaffold of the electrocatalysts. The single-crystal nanocube electrode exhibits stable, continuous oxygen evolution for >1,000 h. This robust stability is attributed to the complementary nature of defect-free single-crystal electrocatalyst and the reversible adapting layer.

  14. The Evolution of Quasi-separatrix Layer in Two Solar Eruptive Events

    NASA Astrophysics Data System (ADS)

    Kang, K. F.; Yan, X. L.; Xu, Z.; Wu, N.; Lin, J.

    2017-05-01

    Quasi-separatrix layer, also called QSL, is a region where magnetic connectivity changes drastically and mostly well coincides with the location of flare ribbons in observations. The research on the relation between this topological structure and 3-dimensional magnetic reconnection, and solar flares has attracted more and more attention. In this paper, using the theory of QSL we investigate a C5.7 classical two-ribbon solar flare (event 1) which occurred at AR11384 on 2011 December 26 and an M6.5 solar flare (event 2) which occurred at AR12371 on 2015 June 22, respectively. Combining the multi-wavelength data of AIA (Atmospheric Imaging Assembly) and vector magnetogrames of HMI (Helioseismic and Magnetic Imager) onboard SDO (Solar Dynamics Observatory), we extrapolate the coronal magnetic field using the PF (Potential Field) model and NLFFF (Nonlinear Force Free Field) model, and calculate the evolution of the AR (Active Region) magnetic free energy first. Next, we calculate the slgQ maps of Q factor (magnetic squashing factor) at different heights away from solar photosphere with the extrapolation results of PF and NLFFF in order to decide the location of QSL. Then, we investigate the evolution relation between QSL at different heights away from solar photosphere and flaring brightening at the same layers. Finally, we study the multi-wavelength evolution features of the 2 flares. And, we calculate the observational slipping running speeds of event 2 in 304 Å and 335 Å, which are 4.6 km s-1 and 6.3 km s-1, respectively. We find that the location of QSL calculated in chromosphere and corona is in good agreement with the location of flare ribbons at the same height, and the QSL at different layers has almost the same evolutionary behavior in time with the flaring brightening of the corresponding layer, which highlights the role of QSL in the research of 3D magnetic reconnection and solar flare, and we suggest that the flare may be triggered by the QSL reconnection

  15. Evolution of Titan's High-Pressure Ice layer

    NASA Astrophysics Data System (ADS)

    Sotin, C.; Kalousova, K.

    2016-12-01

    Constraints on the present interior structure of Titan come from the gravity science experiment onboard the Cassini spacecraft and from the interpretation of the Extremely Low Frequency (ELF) wave observed by the Huygens probe [1, 2]. From the surface to the center, Titan would be composed of 4 layers: an icy crust, a global salty ocean, a layer of high-pressure ice (HP ice) and a core made of hydrated silicates [2, 3, 4]. The presence of a large amount of 40Ar in Titan's atmosphere argues for a geologically recent exchange process between the silicate core, where 40Ar is produced by the decay of 40K, and the atmosphere. Argon must then be able to be transported from the silicate core to the surface. This study investigates how volatiles can be transported through the HP ice layer.Recent numerical simulations [5] have demonstrated that the dynamics of the HP ice layer is controlled by convection processes in a two-phase material (water and high-pressure ice). The silicate / HP ice interface is maintained at the melting temperature, which might allow for the incorporation of volatiles such as 40Ar into the convecting HP ice. Above the hot thermal boundary layer, the temperature of the convecting HP ice is below the melting temperature, except for the upwelling plumes when they approach the cold thermal boundary layer. The upper part of the HP ice layer is at the melting point and permeable for water transport, providing a path for the transfer of volatiles trapped in the ice towards the ocean.Scaling laws are inferred from the numerical simulations [5]. They are then used to model the evolution of the HP ice layer. Specifically, we look at the effect of (i) ice viscosity, (ii) heat flux at the silicate/HP ice interface, and (iii) presence of anti-freeze compounds in the ocean, on the thickness of the HP ice layer. In addition, our results provide insights on possible resurfacing processes that could explain the geologically young age of Titan's surface. This work

  16. A Modeling Pattern for Layered System Interfaces

    NASA Technical Reports Server (NTRS)

    Shames, Peter M.; Sarrel, Marc A.

    2015-01-01

    Communications between systems is often initially represented at a single, high level of abstraction, a link between components. During design evolution it is usually necessary to elaborate the interface model, defining it from several different, related viewpoints and levels of abstraction. This paper presents a pattern to model such multi-layered interface architectures simply and efficiently, in a way that supports expression of technical complexity, interfaces and behavior, and analysis of complexity. Each viewpoint and layer of abstraction has its own properties and behaviors. System elements are logically connected both horizontally along the communication path, and vertically across the different layers of protocols. The performance of upper layers depends on the performance of lower layers, yet the implementation of lower layers is intentionally opaque to upper layers. Upper layers are hidden from lower layers except as sources and sinks of data. The system elements may not be linked directly at each horizontal layer but only via a communication path, and end-to-end communications may depend on intermediate components that are hidden from them, but may need to be shown in certain views and analyzed for certain purposes. This architectural model pattern uses methods described in ISO 42010, Recommended Practice for Architectural Description of Software-intensive Systems and CCSDS 311.0-M-1, Reference Architecture for Space Data Systems (RASDS). A set of useful viewpoints and views are presented, along with the associated modeling representations, stakeholders and concerns. These viewpoints, views, and concerns then inform the modeling pattern. This pattern permits viewing the system from several different perspectives and at different layers of abstraction. An external viewpoint treats the systems of interest as black boxes and focuses on the applications view, another view exposes the details of the connections and other components between the black boxes

  17. Impact of grain size evolution on necking and pinch-and-swell formation in calcite layers

    NASA Astrophysics Data System (ADS)

    Schmalholz, Stefan Markus; Duretz, Thibault

    2017-04-01

    The formation of necking zones and the associated formation of pinch-and-swell structure is one form of strain localization in extending, competent layers. Natural pinch-and-swell structure in centimetre-thick calcite layers typically shows a reduction of grain size from swell towards pinch. However, the impact of grain size evolution on necking and pinch-and-swell formation is incompletely understood. We perform zero-dimensional (0D) and 2D thermo-mechanical numerical simulations to quantify the impact of grain size evolution on necking for extension rates between 10-12s^-1and10^-14 s-1 and temperatures around 350°C. For a combination of diffusion and dislocation creep we calculate grain size evolution according to the paleowattmeter (grain size is proportional to mechanical work rate) or the paleopiezometer (grain size is proportional to stress). Numerical results fit two observations: (i) grain size reduction from swells towards pinches, and (ii) dislocation creep dominated deformation in swells and significant contribution of diffusion creep in pinches. Modelled grain size in pinches (10 to 60 μm) and swells (70 to 800 μm) is close to observed grain size in pinches (15 to 27 μm) and in swells (250 to 1500 μm). Grain size evolution has only a minor impact on necking suggesting that grain size evolution is a consequence, and not the cause of necking. Viscous shear heating and grain size evolution had a negligible thermal impact in the simulations.

  18. Overturn of magma ocean ilmenite cumulate layer: Implications for lunar magmatic evolution and formation of a lunar core

    NASA Technical Reports Server (NTRS)

    Hess, P. C.; Parmentier, E. M.

    1993-01-01

    We explore a model for the chemical evolution of the lunar interior that explains the origin and evolution of lunar magmatism and possibly the existence of a lunar core. A magma ocean formed during accretion differentiates into the anorthositic crust and chemically stratified cumulate mantle. The cumulative mantle is gravitationally unstable with dense ilmenite cumulate layers overlying olivine-orthopyroxene cumulates with Fe/Mg that decreases with depth. The dense ilmenite layer sinks to the center of the moon forming the core. The remainder of the gravitationally unstable cumulate pile also overturns. Any remaining primitive lunar mantle rises to its level of neutral buoyancy in the cumulate pile. Perhaps melting of primitive lunar mantle due to this decompression results in early lunar Mg-rich magmatism. Because of its high concentration of incompatible heat producing elements, the ilmenite core heats the overlying orthopyroxene-bearing cumulates. As a conductively thickening thermal boundary layer becomes unstable, the resulting mantle plumes rise, decompress, and partially melt to generate the mare basalts. This model explains both the timing and chemical characteristics of lunar magmatism.

  19. Evolution of flare ribbons, electric currents, and quasi-separatrix layers during an X-class flare

    NASA Astrophysics Data System (ADS)

    Janvier, M.; Savcheva, A.; Pariat, E.; Tassev, S.; Millholland, S.; Bommier, V.; McCauley, P.; McKillop, S.; Dougan, F.

    2016-07-01

    Context. The standard model for eruptive flares has been extended to three dimensions (3D) in the past few years. This model predicts typical J-shaped photospheric footprints of the coronal current layer, forming at similar locations as the quasi-separatrix layers (QSLs). Such a morphology is also found for flare ribbons observed in the extreme ultraviolet (EUV) band, and in nonlinear force-free field (NLFFF) magnetic field extrapolations and models. Aims: We study the evolution of the photospheric traces of the current density and flare ribbons, both obtained with the Solar Dynamics Observatory instruments. We aim to compare their morphology and their time evolution, before and during the flare, with the topological features found in a NLFFF model. Methods: We investigated the photospheric current evolution during the 06 September 2011 X-class flare (SOL2011-09-06T22:20) occurring in NOAA AR 11283 from observational data of the magnetic field obtained with the Helioseismic and Magnetic Imager aboard the Solar Dynamics Observatory. We compared this evolution with that of the flare ribbons observed in the EUV filters of the Atmospheric Imager Assembly. We also compared the observed electric current density and the flare ribbon morphology with that of the QSLs computed from the flux rope insertion method-NLFFF model. Results: The NLFFF model shows the presence of a fan-spine configuration of overlying field lines, due to the presence of a parasitic polarity, embedding an elongated flux rope that appears in the observations as two parts of a filament. The QSL signatures of the fan configuration appear as a circular flare ribbon that encircles the J-shaped ribbons related to the filament ejection. The QSLs, evolved via a magnetofrictional method, also show similar morphology and evolution as both the current ribbons and the EUV flare ribbons obtained several times during the flare. Conclusions: For the first time, we propose a combined analysis of the photospheric

  20. Evolution of inviscid Kelvin-Helmholtz instability from a piecewise linear shear layer

    NASA Astrophysics Data System (ADS)

    Guha, Anirban; Rahmani, Mona; Lawrence, Gregory

    2012-11-01

    Here we study the evolution of 2D, inviscid Kelvin-Helmholtz instability (KH) ensuing from a piecewise linear shear layer. Although KH pertaining to smooth shear layers (eg. Hyperbolic tangent profile) has been thorough investigated in the past, very little is known about KH resulting from sharp shear layers. Pozrikidis and Higdon (1985) have shown that piecewise shear layer evolves into elliptical vortex patches. This non-linear state is dramatically different from the well known spiral-billow structure of KH. In fact, there is a little acknowledgement that elliptical vortex patches can represent non-linear KH. In this work, we show how such patches evolve through the interaction of vorticity waves. Our work is based on two types of computational methods (i) Contour Dynamics: a boundary-element method which tracks the evolution of the contour of a vortex patch using Lagrangian marker points, and (ii) Direct Numerical Simulation (DNS): an Eulerian pseudo-spectral method heavily used in studying hydrodynamic instability and turbulence.

  1. Layering and Ordering in Electrochemical Double Layers

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

    Liu, Yihua; Kawaguchi, Tomoya; Pierce, Michael S.

    Electrochemical double layers (EDL) form at electrified interfaces. While Gouy-Chapman model describes moderately charged EDL, formation of Stern layers was predicted for highly charged EDL. Our results provide structural evidence for a Stern layer of cations, at potentials close to hydrogen evolution in alkali fluoride and chloride electrolytes. Layering was observed by x-ray crystal truncation rods and atomic-scale recoil responses of Pt(111) surface layers. Ordering in the layer is confirmed by glancing-incidence in-plane diffraction measurements.

  2. Coupling Landform Evolution and Soil Pedogenesis - Initial Results From the SSSPAM5D Model

    NASA Astrophysics Data System (ADS)

    Willgoose, G. R.; Welivitiya, W. D. D. P.; Hancock, G. R.; Cohen, S.

    2015-12-01

    Evolution of soil on a dynamic landform is a crucial next step in landscape evolution modelling. Some attempts have been taken such as MILESD by Vanwalleghem et al. to develop a first model which is capable of simultaneously evolving both the soil profile and the landform. In previous work we have presented physically based models for soil pedogenesis, mARM and SSSPAM. In this study we present the results of coupling a landform evolution model with our SSSPAM5D soil pedogenesis model. In previous work the SSSPAM5D soil evolution model was used to identify trends of the soil profile evolution on a static landform. Two pedogenetic processes, namely (1) armouring due to erosion, and (2) physical and chemical weathering were used in those simulations to evolve the soil profile. By incorporating elevation changes (due to erosion and deposition) we have advanced the SSSPAM5D modelling framework into the realm of landscape evolution. Simulations have been run using elevation and soil grading data of the engineered landform (spoil heap) at the Ranger Uranium Mine, Northern Territory, Australia. The results obtained for the coupled landform-soil evolution simulations predict the erosion of high slope areas, development of rudimentary channel networks in the landform and deposition of sediments in lowland areas, and qualitatively consistent with landform evolution models on their own. Examination of the soil profile characteristics revealed that hill crests are weathering dominated and tend to develop a thick soil layer. The steeper hillslopes at the edge of the landform are erosion dominated with shallow soils while the foot slopes are deposition dominated with thick soil layers. The simulation results of our coupled landform and soil evolution model provide qualitatively correct and timely characterization of the soil evolution on a dynamic landscape. Finally we will compare the characteristics of erosion and deposition predicted by the coupled landform-soil SSSPAM

  3. Thermal Evolution of The Moon With a Thicker Kreep Layer

    NASA Astrophysics Data System (ADS)

    Hess, P. C.; Parmentier, E. M.

    1998-01-01

    The canonical view of the magma ocean is of a monotonically cooling large magma body perhaps enveloping the entire Moon, which solidified within about 100 my of the formation of the Moon. This model is consistent with W-Hf Sm-Nd isotope data, the very old ages of FAN and some magnesian-suite norites and troctolites and the model ages for KREEP. Recently, Korotev and Wieczorek and Phillips have argued that the crystallization of the last dregs of the magma ocean was not only prolonged but large amounts of radiogenic heating resulted in the remelting and dissolution of mafic cumulates by the UrKREEP liquid. These melts are believed to be parent liquids to the magnesian-suite troctolites because they account for the combination of high contents of incompatible trace elements and the very refractory major element composition. This model requires that the heat budget changes from one that cools the magma ocean to one that initiates reheating. About the only way to reverse this cooling trend is to segregate the magma ocean under some portions of the crust. For example, if the residual liquids are locally doubled in thickness the surface cooling is reduced thus reversing the cooling tend. By mass balance some portions of the magma ocean would be thinned and thereby would experience an accelerated cooling.accelerated cooling. We have examined the thermal history of the upper Moon. We formulate models of radioactive heating and conductive cooling to examine the possible role of a thick KREEP-rich layer on lunar regional thermal evolution. The models treat heat transfer by conduction in a spherical geometry with a KREEP layer containing a prescribed rate of radiogenic heating. The region of thick KREEP presumably exists only within the Imbrium-Procellarum region of the Moon. The spherical model is a reasonable representation of this case since the lateral dimensions of the region are large compared to its depth. The edges of the thick KREEP region which are not treated

  4. Temperature-dependent evolution of the wetting layer thickness during Ge deposition on Si(001).

    PubMed

    Bergamaschini, R; Brehm, M; Grydlik, M; Fromherz, T; Bauer, G; Montalenti, F

    2011-07-15

    The evolution of the wetting layer (WL) thickness during Ge deposition on Si(001) is analyzed with the help of a rate-equation approach. The combined role of thickness, island volume and shape-dependent chemical potentials is considered. Several experimental observations, such as WL thinning following the pyramid-to-dome transformation, are captured by the model, as directly demonstrated by a close comparison with photoluminescence measurements (PL) on samples grown at three different temperatures. The limitations of the model in describing late stages of growth are critically addressed.

  5. The thermodynamic evolution of the hurricane boundary layer during eyewall replacement cycles

    NASA Astrophysics Data System (ADS)

    Williams, Gabriel J.

    2017-12-01

    Eyewall replacement cycles (ERCs) are frequently observed during the lifecycle of mature tropical cyclones. Although the kinematic structure and intensity changes during an ERC have been well-documented, comparatively little research has been done to examine the evolution of the tropical cyclone boundary layer (TCBL) during an ERC. This study will examine how the inner core thermal structure of the TCBL is affected by the presence of multiple concentric eyewalls using a high-resolution moist, hydrostatic, multilayer diagnostic boundary layer model. Within the concentric eyewalls above the cloud base, latent heat release and vertical advection (due to the eyewall updrafts) dominate the heat and moisture budgets, whereas vertical advection (due to subsidence) and vertical diffusion dominate the heat and moisture budgets for the moat region. Furthermore, it is shown that the development of a moat region within the TCBL depends sensitively on the moat width in the overlying atmosphere and the relative strength of the gradient wind field in the overlying atmosphere. These results further indicate that the TCBL contributes to outer eyewall formation through a positive feedback process between the vorticity in the nascent outer eyewall, boundary layer convergence, and boundary layer moist convection.

  6. Germ layers, the neural crest and emergent organization in development and evolution.

    PubMed

    Hall, Brian K

    2018-04-10

    Discovered in chick embryos by Wilhelm His in 1868 and named the neural crest by Arthur Milnes Marshall in 1879, the neural crest cells that arise from the neural folds have since been shown to differentiate into almost two dozen vertebrate cell types and to have played major roles in the evolution of such vertebrate features as bone, jaws, teeth, visceral (pharyngeal) arches, and sense organs. I discuss the discovery that ectodermal neural crest gave rise to mesenchyme and the controversy generated by that finding; the germ layer theory maintained that only mesoderm could give rise to mesenchyme. A second topic of discussion is germ layers (including the neural crest) as emergent levels of organization in animal development and evolution that facilitated major developmental and evolutionary change. The third topic is gene networks, gene co-option, and the evolution of gene-signaling pathways as key to developmental and evolutionary transitions associated with the origin and evolution of the neural crest and neural crest cells. © 2018 Wiley Periodicals, Inc.

  7. Evolution of Akaganeite in Rust Layers Formed on Steel Submitted to Wet/Dry Cyclic Tests

    PubMed Central

    Ye, Wei; Song, Xiaoping; Ma, Yuantai; Li, Ying

    2017-01-01

    The evolution of akaganeite in rust layers strongly impacts the atmospheric corrosion behavior of steel during long-term exposure; however, the factors affecting the evolution of akaganeite and its mechanism of formation are vague. In this work, wet-dry cyclic corrosion tests were conducted to simulate long-term exposure. Quantitative X-ray diffraction analysis was employed to analyze variations in the relative amounts of akaganeite; scanning electron microscopy and electron probe microanalysis were used to study the migration of relevant elements in the rust layer, which could help elucidate the mechanism of akaganeite evolution. The results indicate that the fraction of akaganeite tends to decrease as the corrosion process proceeded, which is a result of the decrease in the amount of soluble chloride available and the ability of the thick rust layer to block the migration of relevant ions. This work also explores the location of akaganeite formation within the rust layer. PMID:29099061

  8. Comparison of 2-3D convection models with parameterized thermal evolution models: Application to Mars

    NASA Astrophysics Data System (ADS)

    Thiriet, M.; Plesa, A. C.; Breuer, D.; Michaut, C.

    2017-12-01

    To model the thermal evolution of terrestrial planets, 1D parametrized models are often used as 2 or 3D mantle convection codes are very time-consuming. In these parameterized models, scaling laws that describe the convective heat transfer rate as a function of the convective parameters are derived from 2-3D steady state convection models. However, so far there has been no comprehensive comparison whether they can be applied to model the thermal evolution of a cooling planet. Here we compare 2D and 3D thermal evolution models in the stagnant lid regime with 1D parametrized models and use parameters representing the cooling of the Martian mantle. For the 1D parameterized models, we use the approach of Grasset and Parmentier (1998) and treat the stagnant lid and the convecting layer separately. In the convecting layer, the scaling law for a fluid with constant viscosity is valid with Nu (Ra/Rac) ?, with Rac the critical Rayleigh number at which the thermal boundary layers (TBL) - top or bottom - destabilize. ? varies between 1/3 and 1/4 depending on the heating mode and previous studies have proposed intermediate values of b 0.28-0.32 according to their model set-up. The base of the stagnant lid is defined by the temperature at which the mantle viscosity has increased by a factor of 10; it thus depends on the rate of viscosity change with temperature multiplied by a factor? , whose value appears to vary depending on the geometry and convection conditions. In applying Monte Carlo simulations, we search for the best fit to temperature profiles and heat flux using three free parameters, i.e. ? of the upper TBL, ? and the Rac of the lower TBL. We find that depending on the definition of the stagnant lid thickness in the 2-3D models several combinations of ? and ? for the upper TBL can retrieve suitable fits. E.g. combinations of ? = 0.329 and ? = 2.19 but also ? = 0.295 and ? = 2.97 are possible; Rac of the lower TBL is 10 for all best fits. The results show that

  9. Modelling the evolution of complex conductivity during calcite precipitation on glass beads

    NASA Astrophysics Data System (ADS)

    Leroy, Philippe; Li, Shuai; Jougnot, Damien; Revil, André; Wu, Yuxin

    2017-04-01

    When pH and alkalinity increase, calcite frequently precipitates and hence modifies the petrophysical properties of porous media. The complex conductivity method can be used to directly monitor calcite precipitation in porous media because it is sensitive to the evolution of the mineralogy, pore structure and its connectivity. We have developed a mechanistic grain polarization model considering the electrochemical polarization of the Stern and diffuse layers surrounding calcite particles. Our complex conductivity model depends on the surface charge density of the Stern layer and on the electrical potential at the onset of the diffuse layer, which are computed using a basic Stern model of the calcite/water interface. The complex conductivity measurements of Wu et al. on a column packed with glass beads where calcite precipitation occurs are reproduced by our surface complexation and complex conductivity models. The evolution of the size and shape of calcite particles during the calcite precipitation experiment is estimated by our complex conductivity model. At the early stage of the calcite precipitation experiment, modelled particles sizes increase and calcite particles flatten with time because calcite crystals nucleate at the surface of glass beads and grow into larger calcite grains. At the later stage of the calcite precipitation experiment, modelled sizes and cementation exponents of calcite particles decrease with time because large calcite grains aggregate over multiple glass beads and only small calcite crystals polarize.

  10. Nonlinear spatial evolution of inviscid instabilities on hypersonic boundary layers

    NASA Technical Reports Server (NTRS)

    Wundrow, David W.

    1996-01-01

    The spatial development of an initially linear vorticity-mode instability on a compressible flat-plate boundary layer is considered. The analysis is done in the framework of the hypersonic limit where the free-stream Mach number M approaches infinity. Nonlinearity is shown to become important locally, in a thin critical layer, when sigma, the deviation of the phase speed from unity, becomes o(M(exp -8/7)) and the magnitude of the pressure fluctuations becomes 0(sigma(exp 5/2)M(exp 2)). The unsteady flow outside the critical layer takes the form of a linear instability wave but with its amplitude completely determined by the nonlinear flow within the critical layer. The coupled set of equations which govern the critical-layer dynamics reflect a balance between spatial-evolution, (linear and nonlinear) convection and nonlinear vorticity-generation terms. The numerical solution to these equations shows that nonlinear effects produce a dramatic reduction in the instability-wave amplitude.

  11. Using TiO2 as a conductive protective layer for photocathodic H2 evolution.

    PubMed

    Seger, Brian; Pedersen, Thomas; Laursen, Anders B; Vesborg, Peter C K; Hansen, Ole; Chorkendorff, Ib

    2013-01-23

    Surface passivation is a general issue for Si-based photoelectrodes because it progressively hinders electron conduction at the semiconductor/electrolyte interface. In this work, we show that a sputtered 100 nm TiO(2) layer on top of a thin Ti metal layer may be used to protect an n(+)p Si photocathode during photocatalytic H(2) evolution. Although TiO(2) is a semiconductor, we show that it behaves like a metallic conductor would under photocathodic H(2) evolution conditions. This behavior is due to the fortunate alignment of the TiO(2) conduction band with respect to the hydrogen evolution potential, which allows it to conduct electrons from the Si while simultaneously protecting the Si from surface passivation. By using a Pt catalyst the electrode achieves an H(2) evolution onset of 520 mV vs NHE and a Tafel slope of 30 mV when illuminated by the red part (λ > 635 nm) of the AM 1.5 spectrum. The saturation photocurrent (H(2) evolution) was also significantly enhanced by the antireflective properties of the TiO(2) layer. It was shown that with proper annealing conditions these electrodes could run 72 h without significant degradation. An Fe(2+)/Fe(3+) redox couple was used to help elucidate details of the band diagram.

  12. Evolution and dynamics of shear-layer structures in near-wall turbulence

    NASA Technical Reports Server (NTRS)

    Johansson, Arne V.; Alfredsson, P. H.; Kim, John

    1991-01-01

    Near-wall flow structures in turbulent shear flows are analyzed, with particular emphasis on the study of their space-time evolution and connection to turbulence production. The results are obtained from investigation of a database generated from direct numerical simulation of turbulent channel flow at a Reynolds number of 180 based on half-channel width and friction velocity. New light is shed on problems associated with conditional sampling techniques, together with methods to improve these techniques, for use both in physical and numerical experiments. The results clearly indicate that earlier conceptual models of the processes associated with near-wall turbulence production, based on flow visualization and probe measurements need to be modified. For instance, the development of asymmetry in the spanwise direction seems to be an important element in the evolution of near-wall structures in general, and for shear layers in particular. The inhibition of spanwise motion of the near-wall streaky pattern may be the primary reason for the ability of small longitudinal riblets to reduce turbulent skin friction below the value for a flat surface.

  13. Evolution of wetting layer in InAs/GaAs quantum dot system

    PubMed Central

    Ye, XL; Wang, ZG

    2006-01-01

    For InAs/GaAs quantum dot system, the evolution of the wetting layer (WL) with the InAs deposition thickness has been studied by reflectance difference spectroscopy (RDS). Two transitions related to the heavy- and light-hole in the WL have been distinguished in RD spectra. Taking into account the strain and segregation effects, a model has been presented to deduce the InAs amount in the WL and the segregation coefficient of the indium atoms from the transition energies of heavy- and light-holes. The variation of the InAs amount in the WL and the segregation coefficient are found to rely closely on the growth modes. In addition, the huge dots also exhibits a strong effect on the evolution of the WL. The observed linear dependence of In segregation coefficient upon the InAs amount in the WL demonstrates that the segregation is enhanced by the strain in the WL.

  14. Growth model and structure evolution of Ag layers deposited on Ge films.

    PubMed

    Ciesielski, Arkadiusz; Skowronski, Lukasz; Górecka, Ewa; Kierdaszuk, Jakub; Szoplik, Tomasz

    2018-01-01

    We investigated the crystallinity and optical parameters of silver layers of 10-35 nm thickness as a function 2-10 nm thick Ge wetting films deposited on SiO 2 substrates. X-ray reflectometry (XRR) and X-ray diffraction (XRD) measurements proved that segregation of germanium into the surface of the silver film is a result of the gradient growth of silver crystals. The free energy of Ge atoms is reduced by their migration from boundaries of larger grains at the Ag/SiO 2 interface to boundaries of smaller grains near the Ag surface. Annealing at different temperatures and various durations allowed for a controlled distribution of crystal dimensions, thus influencing the segregation rate. Furthermore, using ellipsometric and optical transmission measurements we determined the time-dependent evolution of the film structure. If stored under ambient conditions for the first week after deposition, the changes in the transmission spectra are smaller than the measurement accuracy. Over the course of the following three weeks, the segregation-induced effects result in considerably modified transmission spectra. Two months after deposition, the slope of the silver layer density profile derived from the XRR spectra was found to be inverted due to the completed segregation process, and the optical transmission spectra increased uniformly due to the roughened surfaces, corrosion of silver and ongoing recrystallization. The Raman spectra of the Ge wetted Ag films were measured immediately after deposition and ten days later and demonstrated that the Ge atoms at the Ag grain boundaries form clusters of a few atoms where the Ge-Ge bonds are still present.

  15. Modeling Electrothermal Plasma with Boundary Layer Effects

    NASA Astrophysics Data System (ADS)

    AlMousa, Nouf Mousa A.

    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 current 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 boundary layer adjacent to the solid wall structure. The accumulating boundary 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 boundary 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 boundary 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 boundary 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 boundary layer. The models were validated by comparing the simulation results to experimental

  16. Simulation of Seasonal Snow Microwave TB Using Coupled Multi-Layered Snow Evolution and Microwave Emission Models

    NASA Technical Reports Server (NTRS)

    Brucker, Ludovic; Royer, Alain; Picard, Ghislain; Langlois, Alex; Fily, Michel

    2014-01-01

    The accurate quantification of SWE has important societal benefits, including improving domestic and agricultural water planning, flood forecasting and electric power generation. However, passive-microwave SWE algorithms suffer from variations in TB due to snow metamorphism, difficult to distinguish from those due to SWE variations. Coupled snow evolution-emission models are able to predict snow metamorphism, allowing us to account for emissivity changes. They can also be used to identify weaknesses in the snow evolution model. Moreover, thoroughly evaluating coupled models is a contribution toward the assimilation of TB, which leads to a significant increase in the accuracy of SWE estimates.

  17. Ultrathin platinum nanowires grown on single-layered nickel hydroxide with high hydrogen evolution activity.

    PubMed

    Yin, Huajie; Zhao, Shenlong; Zhao, Kun; Muqsit, Abdul; Tang, Hongjie; Chang, Lin; Zhao, Huijun; Gao, Yan; Tang, Zhiyong

    2015-03-02

    Design and synthesis of effective electrocatalysts for hydrogen evolution reaction in alkaline environments is critical to reduce energy losses in alkaline water electrolysis. Here we report a hybrid nanomaterial comprising of one-dimensional ultrathin platinum nanowires grown on two-dimensional single-layered nickel hydroxide. Judicious surface chemistry to generate the fully exfoliated nickel hydroxide single layers is explored to be the key for controllable growth of ultrathin platinum nanowires with diameters of about 1.8 nm. Impressively, this hybrid nanomaterial exhibits superior electrocatalytic activity for hydrogen evolution reaction in alkaline solution, which outperforms currently reported catalysts, and the obviously improved catalytic stability. We believe that this work may lead towards the development of single-layered metal hydroxide-based hybrid materials for applications in catalysis and energy conversion.

  18. Granular flows on erodible layers: type and evolution of flow and deposit structures

    NASA Astrophysics Data System (ADS)

    Crosta, G.; De Blasio, F.; De Caro, M.; Volpi, G.; Frattini, P.

    2012-04-01

    The interaction of a fast moving landslide mass with the basal layer over which movement takes place has been discussed in previous contributions. Nevertheless, the evolution of the structures within the moving mass and the erodible layer are still to be described in detail (Hungr and Evans, 2004; Crosta et al., 1992, 2006, 2009, 2011; Dufresne et al., 2010; Mangeney et al., 2010) and modeling results (Crosta et al., 2006, 2009, 2011; Mangeney et al., 2010). We present some of the results from a campaign of laboratory experiments aimed at studying the evolution of a granular flow at the impact with and during the successive spreading over a cohesionless erodible layer. We performed these test to study the processes and to collect data and evidences to compare them with the results of numerical simulations and to verify capabilities of numerical codes. The laboratory setup consists of an inclined slope and an horizontal sector where release and transport, and deposition take place, respectively. Materials used for the tests are: a uniform rounded siliceous sand (Hostun sand; 0.125-0.5 mm) commonly adopted in lab tests because free of scale effects, and a gravel made of angular elements (12 mm in ave. size). Both the materials have been tested in dry conditions. Different slope angles have been tested (40, 45, 50, 55, 50, 66°) as well as different thicknesses of the erodible layer (0, 0.5, 1, 2 cm) and volumes of the released material (1.5, 3, 5, 9.6 liters). Tests have been monitored by means of a high speed camera and the pre- and post-failure geometries have been surveyed by means of a laser scanner. Deposit description allowed also the computation of volumes and the characterization of the different structures developed and frozen into the deposit. Experiments allowed us to observe the extreme processes occurring during the movement and the mise en place of the deposits. In particular, we observe the formation of a clear wave-like feature developing during the

  19. Nonlinear evolution of Mack modes in a hypersonic boundary layer

    NASA Astrophysics Data System (ADS)

    Chokani, Ndaona

    2005-01-01

    In hypersonic boundary layer flows the nonlinear disturbance evolution occurs relatively slowly over a very long length scale and has a profound effect on boundary layer transition. In the case of low-level freestream disturbances and negligible surface roughness, the transition is due to the modal growth of exponentially growing Mack modes that are destabilized by wall cooling. Cross-bicoherence measurements, derived from hot-wire data acquired in a quiet hypersonic tunnel, are used to identify and quantify phase-locked, quadratic sum and difference interactions involving the Mack modes. In the early stages of the nonlinear disturbance evolution, cross-bicoherence measurements indicate that the energy exchange between the Mack mode and the mean flow first occurs to broaden the sidebands; this is immediately followed by a sum interaction of the Mack mode to generate the first harmonic. In the next stages of the nonlinear disturbance evolution, there is a difference interaction of the first harmonic, which is also thought to contribute to the mean flow distortion. This difference interaction, in the latter stages, is also accompanied by a difference interaction between Mack mode and first harmonic, and a sum interaction, which forces the second harmonic. Analysis using the digital complex demodulation technique, shows that the low-frequency, phase-locked interaction that is identified in the cross bicoherence when the Mack mode and first harmonic have large amplitudes, arises due to the amplitude modulation of Mack mode and first harmonic.

  20. Principle Component Analysis of the Evolution of the Saharan Air Layer and Dust Transport: Comparisons between a Model Simulation and MODIS Retrievals

    NASA Technical Reports Server (NTRS)

    Wong, S.; Colarco, P. R.; Dessler, A.

    2006-01-01

    The onset and evolution of Saharan Air Layer (SAL) episodes during June-September 2002 are diagnosed by applying principal component analysis to the NCEP reanalysis temperature anomalies at 850 hPa, where the largest SAL-induced temperature anomalies are located. The first principal component (PC) represents the onset of SAL episodes, which are associated with large warm anomalies located at the west coast of Africa. The second PC represents two opposite phases of the evolution of the SAL. The positive phase of the second PC corresponds to the southwestward extension of the warm anomalies into the tropical-subtropical North Atlantic Ocean, and the negative phase corresponds to the northwestward extension into the subtropical to mid-latitude North Atlantic Ocean and the southwest Europe. A dust transport model (CARMA) and the MODIS retrievals are used to study the associated effects on dust distribution and deposition. The positive (negative) phase of the second PC corresponds to a strengthening (weakening) of the offshore flows in the lower troposphere around 10deg - 20degN, causing more (less) dust being transported along the tropical to subtropical North Atlantic Ocean. The variation of the offshore flow indicates that the subseasonal variation of African Easterly Jet is associated with the evolution of the SAL. Significant correlation is found between the second PC time series and the daily West African monsoon index, implying a dynamical linkage between West African monsoon and the evolution of the SAL and Saharan dust transport.

  1. The Influence of Stratigraphic History on Landscape Evolution

    NASA Astrophysics Data System (ADS)

    Forte, A. M.; Yanites, B.; Whipple, K. X.

    2016-12-01

    Variation in rock erodibility can play a significant role in landscape evolution. Using a version of the CHILD landscape evolution model that allows for variations in rock erodibility, we found surprisingly complex landscape evolution in simulations with simple, two unit stratigraphies with contrasting erodibility. This work indicated that the stratigraphic order of units in terms of erodibility, the orientation of the contact with respect to the main drainage direction, and the contact dip angle all have pronounced effects on landscape evolution. Here we expand that work to explore the implications of more complicated stratigraphies on landscape evolution. Introducing multiple units adds additional controls on landscape evolution, namely the thicknesses and relative erodibility of rock layers. In models with a sequence of five alternating hard and soft units embedded within arbitrarily thick over- and underlying units, the number of individual layers that noticeably influence landscape morphology decreases as the thickness of individual layers reduces. Contacts with soft rocks over hard produce the most noticeable effect in model output such as erosion rate and channel steepness. For large contrasts in erodibility of 25 m thick layers, only one soft over hard contact is clearly manifest in the landscape. Between 50 and 75 m, two such contacts are manifest, and by 100 m thickness, all three of these contacts are manifest. However, for a given thickness of layers, more units are manifest in the landscape as the erodibility contrast between units decreases. This is true even though the magnitude of landscape effects away from steady-state erosion rates or channel steepness also decrease with decreasing erodibility contrast. Finally, we explore suites of models with alternating layers reflecting either `hardening-' or `softening-upwards' stratigraphies and find that the two scenarios result in decidedly different landscape forms. Hardening-upwards sections produce a

  2. Temporal evolution of crack propagation propensity in snow in relation to slab and weak layer properties

    NASA Astrophysics Data System (ADS)

    Schweizer, Jürg; Reuter, Benjamin; van Herwijnen, Alec; Richter, Bettina; Gaume, Johan

    2016-11-01

    If a weak snow layer below a cohesive slab is present in the snow cover, unstable snow conditions can prevail for days or even weeks. We monitored the temporal evolution of a weak layer of faceted crystals as well as the overlaying slab layers at the location of an automatic weather station in the Steintälli field site above Davos (Eastern Swiss Alps). We focussed on the crack propagation propensity and performed propagation saw tests (PSTs) on 7 sampling days during a 2-month period from early January to early March 2015. Based on video images taken during the tests we determined the mechanical properties of the slab and the weak layer and compared them to the results derived from concurrently performed measurements of penetration resistance using the snow micro-penetrometer (SMP). The critical cut length, observed in PSTs, increased overall during the measurement period. The increase was not steady and the lowest values of critical cut length were observed around the middle of the measurement period. The relevant mechanical properties, the slab effective elastic modulus and the weak layer specific fracture, overall increased as well. However, the changes with time differed, suggesting that the critical cut length cannot be assessed by simply monitoring a single mechanical property such as slab load, slab modulus or weak layer specific fracture energy. Instead, crack propagation propensity is the result of a complex interplay between the mechanical properties of the slab and the weak layer. We then compared our field observations to newly developed metrics of snow instability related to either failure initiation or crack propagation propensity. The metrics were either derived from the SMP signal or calculated from simulated snow stratigraphy (SNOWPACK). They partially reproduced the observed temporal evolution of critical cut length and instability test scores. Whereas our unique dataset of quantitative measures of snow instability provides new insights into the

  3. Wind-tunnel modelling of the tip-speed ratio influence on the wake evolution

    NASA Astrophysics Data System (ADS)

    Stein, Victor P.; Kaltenbach, Hans-Jakob

    2016-09-01

    Wind-tunnel measurements on the near-wake evolution of a three bladed horizontal axis wind turbine model (HAWT) in the scale 1:O(350) operating in uniform flow conditions and within a turbulent boundary layer at different tip speed ratios are presented. Operational conditions are chosen to exclude Reynolds number effects regarding the turbulent boundary layer as well as the rotor performance. Triple-wire anemometry is used to measure all three velocity components in the mid-vertical and mid-horizontal plane, covering the range from the near- to the far-wake region. In order to analyse wake properties systematically, power and thrust coefficients of the turbine were measured additionally. It is confirmed that realistic modelling of the wake evolution is not possible in a low-turbulence uniform approach flow. Profiles of mean velocity and turbulence intensity exhibit large deviations between the low-turbulence uniform flow and the turbulent boundary layer, especially in the far-wake region. For nearly constant thrust coefficients differences in the evolution of the near-wake can be identified for tip speed ratios in the range from 6.5 to 10.5. It is shown that with increasing downstream distances mean velocity profiles become indistinguishable whereas for turbulence statistics a subtle dependency on the tip speed ratio is still noticeable in the far-wake region.

  4. Modeling marine boundary-layer clouds with a two-layer model: A one-dimensional simulation

    NASA Technical Reports Server (NTRS)

    Wang, Shouping

    1993-01-01

    A two-layer model of the marine boundary layer is described. The model is used to simulate both stratocumulus and shallow cumulus clouds in downstream simulations. Over cold sea surfaces, the model predicts a relatively uniform structure in the boundary layer with 90%-100% cloud fraction. Over warm sea surfaces, the model predicts a relatively strong decoupled and conditionally unstable structure with a cloud fraction between 30% and 60%. A strong large-scale divergence considerably limits the height of the boundary layer and decreases relative humidity in the upper part of the cloud layer; thus, a low cloud fraction results. The efffects of drizzle on the boundary-layer structure and cloud fraction are also studied with downstream simulations. It is found that drizzle dries and stabilizes the cloud layer and tends to decouple the cloud from the subcloud layer. Consequently, solid stratocumulus clouds may break up and the cloud fraction may decrease because of drizzle.

  5. Modeling solute clustering in the diffusion layer around a growing crystal.

    PubMed

    Shiau, Lie-Ding; Lu, Yung-Fang

    2009-03-07

    The mechanism of crystal growth from solution is often thought to consist of a mass transfer diffusion step followed by a surface reaction step. Solute molecules might form clusters in the diffusion step before incorporating into the crystal lattice. A model is proposed in this work to simulate the evolution of the cluster size distribution due to the simultaneous aggregation and breakage of solute molecules in the diffusion layer around a growing crystal in the stirred solution. The crystallization of KAl(SO(4))(2)12H(2)O from aqueous solution is studied to illustrate the effect of supersaturation and diffusion layer thickness on the number-average degree of clustering and the size distribution of solute clusters in the diffusion layer.

  6. The Microcircuit Concept Applied to Cortical Evolution: from Three-Layer to Six-Layer Cortex

    PubMed Central

    Shepherd, Gordon M.

    2011-01-01

    Understanding the principles of organization of the cerebral cortex requires insight into its evolutionary history. This has traditionally been the province of anatomists, but evidence regarding the microcircuit organization of different cortical areas is providing new approaches to this problem. Here we use the microcircuit concept to focus first on the principles of microcircuit organization of three-layer cortex in the olfactory cortex, hippocampus, and turtle general cortex, and compare it with six-layer neocortex. From this perspective it is possible to identify basic circuit elements for recurrent excitation and lateral inhibition that are common across all the cortical regions. Special properties of the apical dendrites of pyramidal cells are reviewed that reflect the specific adaptations that characterize the functional operations in the different regions. These principles of microcircuit function provide a new approach to understanding the expanded functional capabilities elaborated by the evolution of the neocortex. PMID:21647397

  7. The nonlinear evolution of modes on unstable stratified shear layers

    NASA Technical Reports Server (NTRS)

    Blackaby, Nicholas; Dando, Andrew; Hall, Philip

    1993-01-01

    The nonlinear development of disturbances in stratified shear flows (having a local Richardson number of value less than one quarter) is considered. Such modes are initially fast growing but, like related studies, we assume that the viscous, non-parallel spreading of the shear layer results in them evolving in a linear fashion until they reach a position where their amplitudes are large enough and their growth rates have diminished sufficiently so that amplitude equations can be derived using weakly nonlinear and non-equilibrium critical-layer theories. Four different basic integro-differential amplitude equations are possible, including one due to a novel mechanism; the relevant choice of amplitude equation, at a particular instance, being dependent on the relative sizes of the disturbance amplitude, the growth rate of the disturbance, its wavenumber, and the viscosity of the fluid. This richness of choice of possible nonlinearities arises mathematically from the indicial Frobenius roots of the governing linear inviscid equation (the Taylor-Goldstein equation) not, in general, differing by an integer. The initial nonlinear evolution of a mode will be governed by an integro-differential amplitude equations with a cubic nonlinearity but the resulting significant increase in the size of the disturbance's amplitude leads on to the next stage of the evolution process where the evolution of the mode is governed by an integro-differential amplitude equations with a quintic nonlinearity. Continued growth of the disturbance amplitude is expected during this stage, resulting in the effects of nonlinearity spreading to outside the critical level, by which time the flow has become fully nonlinear.

  8. Numerical Modeling Studies of Wake Vortex Transport and Evolution Within the Planetary Boundary Layer

    NASA Technical Reports Server (NTRS)

    Lin, Yuh-Lang; Arya, S. Pal; Kaplan, Michael L.; Shen, Shaohua

    1998-01-01

    In support of the wake vortex effect of the Terminal Area Productivity program, we have put forward four tasks to be accomplished in our proposal. The first task is validation of two-dimensional wake vortex-turbulence interaction. The second task is investigation of three-dimensional interaction between wake vortices and atmospheric boundary layer (ABL) turbulence. The third task is ABL studies. The, fourth task is addition of a Klemp-Durran condition at the top boundary for TASS model. The accomplishment of these tasks will increase our understanding of the dynamics of wake vortex and improve forecasting systems responsible for air safety and efficiency. The first two tasks include following three parts: (a) Determine significant length scale for vortex decay and transport, especially the length scales associated with the onset of Crow instability (Crow, 1970); (b) Study the effects of atmospheric turbulence on the decay of the wake vortices; and (c) Determine the relationships between decay rate, transport properties and atmospheric parameters based on large eddy simulation (LES) results and the observational data. These parameters may include turbulence kinetic energy, dissipation rate, wind shear and atmospheric stratification. The ABL studies cover LES modeling of turbulence structure within planetary boundary layer under transition and stable stratification conditions. Evidences have shown that the turbulence in the stable boundary layer can be highly intermittent and the length scales of eddies are very small compared to those in convective case. We proposed to develop a nesting grid mesh scheme and a modified Klemp-Durran conditions (Klemp and Wilhelmson, 1978) at the top boundary for TASS model to simulate planetary boundary layer under stable stratification conditions. During the past year, our group has made great efforts to carry out the above mentioned four tasks simultaneously. The work accomplished in the last year will be described in the next

  9. Quasi-two-layer morphodynamic model for bedload-dominated problems: bed slope-induced morphological diffusion

    NASA Astrophysics Data System (ADS)

    Maldonado, Sergio; Borthwick, Alistair G. L.

    2018-02-01

    We derive a two-layer depth-averaged model of sediment transport and morphological evolution for application to bedload-dominated problems. The near-bed transport region is represented by the lower (bedload) layer which has an arbitrarily constant, vanishing thickness (of approx. 10 times the sediment particle diameter), and whose average sediment concentration is free to vary. Sediment is allowed to enter the upper layer, and hence the total load may also be simulated, provided that concentrations of suspended sediment remain low. The model conforms with established theories of bedload, and is validated satisfactorily against empirical expressions for sediment transport rates and the morphodynamic experiment of a migrating mining pit by Lee et al. (1993 J. Hydraul. Eng. 119, 64-80 (doi:10.1061/(ASCE)0733-9429(1993)119:1(64))). Investigation into the effect of a local bed gradient on bedload leads to derivation of an analytical, physically meaningful expression for morphological diffusion induced by a non-zero local bed slope. Incorporation of the proposed morphological diffusion into a conventional morphodynamic model (defined as a coupling between the shallow water equations, Exner equation and an empirical formula for bedload) improves model predictions when applied to the evolution of a mining pit, without the need either to resort to special numerical treatment of the equations or to use additional tuning parameters.

  10. Quasi-two-layer morphodynamic model for bedload-dominated problems: bed slope-induced morphological diffusion.

    PubMed

    Maldonado, Sergio; Borthwick, Alistair G L

    2018-02-01

    We derive a two-layer depth-averaged model of sediment transport and morphological evolution for application to bedload-dominated problems. The near-bed transport region is represented by the lower (bedload) layer which has an arbitrarily constant, vanishing thickness (of approx. 10 times the sediment particle diameter), and whose average sediment concentration is free to vary. Sediment is allowed to enter the upper layer, and hence the total load may also be simulated, provided that concentrations of suspended sediment remain low. The model conforms with established theories of bedload, and is validated satisfactorily against empirical expressions for sediment transport rates and the morphodynamic experiment of a migrating mining pit by Lee et al. (1993 J. Hydraul. Eng. 119 , 64-80 (doi:10.1061/(ASCE)0733-9429(1993)119:1(64))). Investigation into the effect of a local bed gradient on bedload leads to derivation of an analytical, physically meaningful expression for morphological diffusion induced by a non-zero local bed slope. Incorporation of the proposed morphological diffusion into a conventional morphodynamic model (defined as a coupling between the shallow water equations, Exner equation and an empirical formula for bedload) improves model predictions when applied to the evolution of a mining pit, without the need either to resort to special numerical treatment of the equations or to use additional tuning parameters.

  11. Spatial Evolution of Resonant Harmonic Mode Triads in a Blasius Boundary Layer

    NASA Technical Reports Server (NTRS)

    Davila, Jose B.; King, Rudolph A.

    2007-01-01

    Blasius boundary layer evolution is studies by means of bicoherence calculations. The layer is acoustically excited at the T-S frequency to provide a controlled transition. Measurements are made using a smooth surface as well as various roughness patterns. The bicoherence calculations are used to determine the extent to which frequency resonant velocity fluctuation waves can participate in energy exchange. The emphasis is on downstream variation of the individual interactions among harmonic modes. A limited picture of the role of quadratic wave interactions is revealed.

  12. Thermal evolution of the earth

    NASA Technical Reports Server (NTRS)

    Spohn, T.

    1984-01-01

    The earth's heat budget and models of the earth's thermal evolution are discussed. Sources of the planetary heat are considered and modes of heat transport are addressed, including conduction, convection, and chemical convection. Thermal and convectional models of the earth are covered, and models of thermal evolution are discussed in detail, including changes in the core, the influence of layered mantle convection on the thermal evolution, and the effect of chemical differentiation on the continents.

  13. Effects of Sn Layer Orientation on the Evolution of Cu/Sn Interfaces

    NASA Astrophysics Data System (ADS)

    Sun, Menglong; Zhao, Zhangjian; Hu, Fengtian; Hu, Anmin; Li, Ming; Ling, Huiqin; Hang, Tao

    2018-03-01

    The effects of Sn layer orientation on the evolution of Cu/Sn joint interfaces were investigated. Three Sn layers possessing (112), (321) and (420) orientations were electroplated on polycrystalline Cu substrates respectively. The orientations of Sn layer preserved during reflowing at 250 °C for 10 s. After aging at 150 °C for different time, the interfacial microstructures were observed from the cross-section and top-view. The alignment between the c-axis of Sn and Cu diffusion direction significantly sped up the Cu diffusion, leading to the thickest intermetallic compound layer formed in (112) joint. Two types of voids, namely, intracrystalline voids and grain islanding caused intercrystalline voids generated at Cu/Cu3Sn interfaces due to the different interdiffusion coefficients of Cu and Sn (112) oriented Sn/Cu joint produced many more voids than (321) joint, and no voids were detected in (420) joint. Therefore, to enhance the reliability of solder joints, using (420) oriented Sn as solder layer could be an efficient way.

  14. Electron microscopy observation of TiO2 nanocrystal evolution in high-temperature atomic layer deposition.

    PubMed

    Shi, Jian; Li, Zhaodong; Kvit, Alexander; Krylyuk, Sergiy; Davydov, Albert V; Wang, Xudong

    2013-01-01

    Understanding the evolution of amorphous and crystalline phases during atomic layer deposition (ALD) is essential for creating high quality dielectrics, multifunctional films/coatings, and predictable surface functionalization. Through comprehensive atomistic electron microscopy study of ALD TiO2 nanostructures at designed growth cycles, we revealed the transformation process and sequence of atom arrangement during TiO2 ALD growth. Evolution of TiO2 nanostructures in ALD was found following a path from amorphous layers to amorphous particles to metastable crystallites and ultimately to stable crystalline forms. Such a phase evolution is a manifestation of the Ostwald-Lussac Law, which governs the advent sequence and amount ratio of different phases in high-temperature TiO2 ALD nanostructures. The amorphous-crystalline mixture also enables a unique anisotropic crystal growth behavior at high temperature forming TiO2 nanorods via the principle of vapor-phase oriented attachment.

  15. Lidar network observation of dust layer evolution over the Gobi Desert in MAY 2013

    NASA Astrophysics Data System (ADS)

    Kawai, Kei; Kai, Kenji; Jin, Yoshitaka; Sugimoto, Nobuo; Batdorj, Dashdondog

    2018-04-01

    A lidar network captured the evolution of a dust layer in the Gobi Desert on 22-23 May 2013. The lidar network consists of a ceilometer and two AD-Net lidars in Mongolia. The dust layer was generated by a strong wind due to a cold front and elevated over the surface of the cold front by an updraft of the warm air in the cold-front system. It was evolving from the atmospheric boundary layer to the free troposphere while moving 600 km through the desert with the cold front.

  16. Nonlinear critical-layer evolution of a forced gravity wave packet

    NASA Astrophysics Data System (ADS)

    Campbell, L. J.; Maslowe, S. A.

    2003-10-01

    In this paper, numerical simulations are presented of the nonlinear critical-layer evolution of a forced gravity wave packet in a stratified shear flow. The wave packet, localized in the horizontal direction, is forced at the lower boundary of a two-dimensional domain and propagates vertically towards the critical layer. The wave mean-flow interactions in the critical layer are investigated numerically and contrasted with the results obtained using a spatially periodic monochromatic forcing. With the horizontally localized forcing, the net absorption of the disturbance at the critical layer continues for large time and the onset of the nonlinear breakdown is delayed compared with the case of monochromatic forcing. There is an outward flux of momentum in the horizontal direction so that the horizontal extent of the packet increases with time. The extent to which this happens depends on a number of factors including the amplitude and horizontal length of the forcing. It is also seen that the prolonged absorption of the disturbance stabilizes the solution to the extent that it is always convectively stable; the local Richardson number remains positive well into the nonlinear regime. In this respect, our results for the localized forcing differ from those in the case of monochromatic forcing where significant regions with negative Richardson number appear.

  17. A volumetric ablation model of EPDM considering complex physicochemical process in porous structure of char layer

    NASA Astrophysics Data System (ADS)

    Yang, Liu; Xiao-Jing, Yu; Jian-Ming, Ma; Yi-Wen, Guan; Jiang, Li; Qiang, Li; Sa, Yang

    2017-06-01

    A volumetric ablation model for EPDM (ethylene- propylene-diene monomer) is established in this paper. This model considers the complex physicochemical process in the porous structure of a char layer. An ablation physics model based on a porous structure of a char layer and another model of heterogeneous volumetric ablation char layer physics are then built. In the model, porosity is used to describe the porous structure of a char layer. Gas diffusion and chemical reactions are introduced to the entire porous structure. Through detailed formation analysis, the causes of the compact or loose structure in the char layer and chemical vapor deposition (CVD) reaction between pyrolysis gas and char layer skeleton are introduced. The Arrhenius formula is adopted to determine the methods for calculating carbon deposition rate C which is the consumption rate caused by thermochemical reactions in the char layer, and porosity evolution. The critical porosity value is used as a criterion for char layer porous structure failure under gas flow and particle erosion. This critical porosity value is obtained by fitting experimental parameters and surface porosity of the char layer. Linear ablation and mass ablation rates are confirmed with the critical porosity value. Results of linear ablation and mass ablation rate calculations generally coincide with experimental results, suggesting that the ablation analysis proposed in this paper can accurately reflect practical situations and that the physics and mathematics models built are accurate and reasonable.

  18. Temporal and Spatial Evolution Characteristics of Disturbance Wave in a Hypersonic Boundary Layer due to Single-Frequency Entropy Disturbance

    PubMed Central

    Lv, Hongqing; Shi, Jianqiang

    2014-01-01

    By using a high-order accurate finite difference scheme, direct numerical simulation of hypersonic flow over an 8° half-wedge-angle blunt wedge under freestream single-frequency entropy disturbance is conducted; the generation and the temporal and spatial nonlinear evolution of boundary layer disturbance waves are investigated. Results show that, under the freestream single-frequency entropy disturbance, the entropy state of boundary layer is changed sharply and the disturbance waves within a certain frequency range are induced in the boundary layer. Furthermore, the amplitudes of disturbance waves in the period phase are larger than that in the response phase and ablation phase and the frequency range in the boundary layer in the period phase is narrower than that in these two phases. In addition, the mode competition, dominant mode transformation, and disturbance energy transfer exist among different modes both in temporal and in spatial evolution. The mode competition changes the characteristics of nonlinear evolution of the unstable waves in the boundary layer. The development of the most unstable mode along streamwise relies more on the motivation of disturbance waves in the upstream than that of other modes on this motivation. PMID:25143983

  19. Temporal and spatial evolution characteristics of disturbance wave in a hypersonic boundary layer due to single-frequency entropy disturbance.

    PubMed

    Wang, Zhenqing; Tang, Xiaojun; Lv, Hongqing; Shi, Jianqiang

    2014-01-01

    By using a high-order accurate finite difference scheme, direct numerical simulation of hypersonic flow over an 8° half-wedge-angle blunt wedge under freestream single-frequency entropy disturbance is conducted; the generation and the temporal and spatial nonlinear evolution of boundary layer disturbance waves are investigated. Results show that, under the freestream single-frequency entropy disturbance, the entropy state of boundary layer is changed sharply and the disturbance waves within a certain frequency range are induced in the boundary layer. Furthermore, the amplitudes of disturbance waves in the period phase are larger than that in the response phase and ablation phase and the frequency range in the boundary layer in the period phase is narrower than that in these two phases. In addition, the mode competition, dominant mode transformation, and disturbance energy transfer exist among different modes both in temporal and in spatial evolution. The mode competition changes the characteristics of nonlinear evolution of the unstable waves in the boundary layer. The development of the most unstable mode along streamwise relies more on the motivation of disturbance waves in the upstream than that of other modes on this motivation.

  20. Computational modelling of large deformations in layered-silicate/PET nanocomposites near the glass transition

    NASA Astrophysics Data System (ADS)

    Figiel, Łukasz; Dunne, Fionn P. E.; Buckley, C. Paul

    2010-01-01

    Layered-silicate nanoparticles offer a cost-effective reinforcement for thermoplastics. Computational modelling has been employed to study large deformations in layered-silicate/poly(ethylene terephthalate) (PET) nanocomposites near the glass transition, as would be experienced during industrial forming processes such as thermoforming or injection stretch blow moulding. Non-linear numerical modelling was applied, to predict the macroscopic large deformation behaviour, with morphology evolution and deformation occurring at the microscopic level, using the representative volume element (RVE) approach. A physically based elasto-viscoplastic constitutive model, describing the behaviour of the PET matrix within the RVE, was numerically implemented into a finite element solver (ABAQUS) using an UMAT subroutine. The implementation was designed to be robust, for accommodating large rotations and stretches of the matrix local to, and between, the nanoparticles. The nanocomposite morphology was reconstructed at the RVE level using a Monte-Carlo-based algorithm that placed straight, high-aspect ratio particles according to the specified orientation and volume fraction, with the assumption of periodicity. Computational experiments using this methodology enabled prediction of the strain-stiffening behaviour of the nanocomposite, observed experimentally, as functions of strain, strain rate, temperature and particle volume fraction. These results revealed the probable origins of the enhanced strain stiffening observed: (a) evolution of the morphology (through particle re-orientation) and (b) early onset of stress-induced pre-crystallization (and hence lock-up of viscous flow), triggered by the presence of particles. The computational model enabled prediction of the effects of process parameters (strain rate, temperature) on evolution of the morphology, and hence on the end-use properties.

  1. Morphological and Microstructural Evolution of Phosphorous-Rich Layer in SnAgCu/Ni-P UBM Solder Joint

    NASA Astrophysics Data System (ADS)

    Lin, Yung-Chi; Shih, Toung-Yi; Tien, Shih-Kang; Duh, Jenq-Gong

    2007-11-01

    Interfacial morphologies and microstructure of Sn-3Ag-0.5Cu/Ni-P under bump metallization (UBM) with various phosphorous contents were investigated by transmission electron microscope (TEM) and field emission electron probe microanalyzer (FE-EPMA). It was revealed that as the Ni-Sn-P compound was formed between the solder matrix and Ni-P UBM, the conventionally so-called phosphorous-rich (P-rich) layer was transformed to a series of layer compounds, including Ni3P, Ni12P5 and Ni2P. The relationship between Ni-Sn-P formation and evolution of P-rich layers was probed by electron microscopic characterization with the aid of the phase diagram of Ni-P. On the basis of the TEM micrograph, the selected area diffraction (SAD) pattern, and the FE-EPMA results, the detailed phase evolution of P-rich layers in the SnAgCu/Ni-P joint was revealed and proposed.

  2. Direct Simulation of Evolution and Control of Three-Dimensional Instabilities in Attachment-Line Boundary Layers

    NASA Technical Reports Server (NTRS)

    Joslin, Ronald D.

    1995-01-01

    The spatial evolution of three-dimensional disturbances in an attachment-line boundary layer is computed by direct numerical simulation of the unsteady, incompressible Navier-Stokes equations. Disturbances are introduced into the boundary layer by harmonic sources that involve unsteady suction and blowing through the wall. Various harmonic- source generators are implemented on or near the attachment line, and the disturbance evolutions are compared. Previous two-dimensional simulation results and nonparallel theory are compared with the present results. The three-dimensional simulation results for disturbances with quasi-two-dimensional features indicate growth rates of only a few percent larger than pure two-dimensional results; however, the results are close enough to enable the use of the more computationally efficient, two-dimensional approach. However, true three-dimensional disturbances are more likely in practice and are more stable than two-dimensional disturbances. Disturbances generated off (but near) the attachment line spread both away from and toward the attachment line as they evolve. The evolution pattern is comparable to wave packets in at-plate boundary-layer flows. Suction stabilizes the quasi-two-dimensional attachment-line instabilities, and blowing destabilizes these instabilities; these results qualitatively agree with the theory. Furthermore, suction stabilizes the disturbances that develop off the attachment line. Clearly, disturbances that are generated near the attachment line can supply energy to attachment-line instabilities, but suction can be used to stabilize these instabilities.

  3. Frequency Domain Modelling of Electromagnetic Wave Propagation in Layered Media

    NASA Astrophysics Data System (ADS)

    Schmidt, Felix; Lünenschloss, Peter; Mai, Juliane; Wagner, Norman; Töpfer, Hannes; Bumberger, Jan

    2016-04-01

    The amount of water in porous media such as soils and rocks is a key parameter when water resources are under investigation. Especially the quantitative spatial distribution and temporal evolution of water contents in soil formations are needed. In high frequency electromagnetic applications soil water content is quantitatively derived from the propagation behavior of electromagnetic waves along waveguides embedded in soil formations. The spatial distribution of the dielectric material properties along the waveguide can be estimated by numerical solving of the inverse problem based on the full wave forward model in time or frequency domain. However, current approaches mostly neglect or approximate the frequency dependence of the electromagnetic material properties of transfer function of the waveguide. As a first prove of concept a full two port broadband frequency domain forward model for propagation of transverse electromagnetic (TEM) waves in coaxial waveguide has been implemented. It is based on the propagation matrix approach for layered transmission line sections. Depending on the complexity of the material different models for the frequency dependent complex permittivity were applied. For the validation of the model a broadband frequency domain measurement with network analyzer technique was used. The measurement is based on a 20 cm long 50 Ohm 20/46 coaxial transmission line cell considering inhomogeneous material distributions. This approach allows (i) an increase of the waveguide calibration accuracy in comparison to conventional TDR based technique and (ii) the consideration of the broadband permittivity spectrum of the porous material. In order to systematic analyze the model, theoretical results were compared with measurements as well as 3D broadband finite element modeling of homogeneous and layered media in the coaxial transmission line cell. Defined standards (Teflon, dry glass beads, de-ionized water) were placed inside the line as the dielectric

  4. Frequency Domain Modelling of Electromagnetic Wave Propagation in Layered Media

    NASA Astrophysics Data System (ADS)

    Schmidt, Felix; Wagner, Norman; Lünenschloß, Peter; Toepfer, Hannes; Dietrich, Peter; Kaliorias, Andreas; Bumberger, Jan

    2015-04-01

    The amount of water in porous media such as soils and rocks is a key parameter when water resources are under investigation. Especially the quantitative spatial distribution and temporal evolution of water contents in soil formations are needed. In high frequency electromagnetic applications soil water content is quantitatively derived from the propagation behavior of electromagnetic waves along waveguides embedded in soil formations. The spatial distribution of the dielectric material properties along the waveguide can be estimated by numerical solving of the inverse problem based on the full wave forward model in time or frequency domain. However, current approaches mostly neglect or approximate the frequency dependence of the electromagnetic material properties of transfer function of the waveguide. As a first prove of concept a full two port broadband frequency domain forward model for propagation of transverse electromagnetic (TEM) waves in coaxial waveguide has been implemented. It is based on the propagation matrix approach for layered transmission line sections Depending on the complexity of the material different models for the frequency dependent complex permittivity were applied. For the validation of the model a broadband frequency domain measurement with network analyzer technique was used. The measurement is based on a 20 cm long 50 Ohm 20/46 coaxial transmission line cell considering inhomogeneous material distributions. This approach allows (i) an increase of the waveguide calibration accuracy in comparison to conventional TDR based technique and (ii) the consideration of the broadband permittivity spectrum of the porous material. In order to systematic analyze the model, theoretical results were compared with measurements as well as 3D broadband finite element modeling of homogeneous and layered media in the coaxial transmission line cell. Defined standards (Teflon, dry glass beads, de-ionized water) were placed inside the line as the dielectric

  5. The Zodiacal Cloud Model applied to the Martian atmosphere. Diurnal variations in meteoric ion layers

    NASA Astrophysics Data System (ADS)

    Carrillo-Sánchez, J. D.; Plane, J. M. C.; Withers, P.; Fallows, K.; Nesvorny, D.; Pokorný, P.

    2016-12-01

    Sporadic metal layers have been detected in the Martian atmosphere by radio occultation measurements using the Mars Express Orbiter and Mars Global Surveyor spacecraft. More recently, metallic ion layers produced by the meteor storm event following the close encounter between Comet Siding Spring (C/2013 A1) and Mars were identified by the Imaging UltraViolet Spectrograph (IUVS) and the Neutral Gas and Ion Mass Spectrometer (NGIMS) on the Mars Atmosphere and Volatile EvolutioN (MAVEN) spacecraft. Work is now in progress to detect the background metal layers produced by the influx of sporadic meteors. In this study we predict the likely appearance of these layers. The Zodiacal Dust Cloud (ZDC) model for particle populations released by asteroids (AST), and dust grains from Jupiter Family Comets (JFCs) and Halley-Type Comets (HTCs) has been combined with a Monte Carlo sampling method and the Chemical ABlation MODel (CABMOD) to predict the ablation rates of Na, K, Fe, Si, Mg, Ca and Al above 40 km altitude in the Martian atmosphere. CABMOD considers the standard treatment of meteor physics, including the balance of frictional heating by radiative losses and the absorption of heat energy through temperature increases, melting phase transitions and vaporization, as well as sputtering by inelastic collisions with the air molecules. The vertical injection profiles are input into the Leeds 1-D Mars atmospheric model which includes photo-ionization, and gas-phase ion-molecule and neutral chemistry, in order to explore the evolution of the resulting metallic ions and atoms. We conclude that the dominant contributor in the Martian's atmosphere is the JFCs over other sources. Finally, we explore the changes of the neutral and ionized Na, Mg and Fe layers over a diurnal cycle.

  6. Multi-Model approach to reconstruct the Mediterranean Freshwater Evolution

    NASA Astrophysics Data System (ADS)

    Simon, Dirk; Marzocchi, Alice; Flecker, Rachel; Lunt, Dan; Hilgen, Frits; Meijer, Paul

    2016-04-01

    Today the Mediterranean Sea is isolated from the global ocean by the Strait of Gibraltar. This restricted nature causes the Mediterranean basin to react more sensitively to climatic and tectonic related phenomena than the global ocean. Not just eustatic sea-level and regional river run-off, but also gateway tectonics and connectivity between sub-basins are leaving an enhanced fingerprint in its geological record. To understand its evolution, it is crucial to understand how these different effects are coupled. The Miocene-Pliocene sedimentary record of the Mediterranean shows alternations in composition and colour and has been astronomically tuned. Around the Miocene-Pliocene Boundary the most extreme changes occur in the Mediterranean Sea. About 6% of the salt in the global ocean deposited in the Mediterranean Region, forming an approximately 2 km thick salt layer, which is still present today. This extreme event is named the Messinian Salinity Crisis (MSC, 5.97-5.33 Ma). The gateway and climate evolution is not well constrained for this time, which makes it difficult to distinguish which of the above mentioned drivers might have triggered the MSC. We, therefore, decided to tackle this problem via a multi-model approach: (1) We calculate the Mediterranean freshwater evolution via 30 atmosphere-ocean-vegetation simulations (using HadCM3L), to which we fitted to a function, using a regression model. This allows us to directly relate the orbital curves to evaporation, precipitation and run off. The resulting freshwater evolution can be directly correlated to other sedimentary and proxy records in the late Miocene. (2) By feeding the new freshwater evolution curve into a box/budget model we can predict the salinity and strontium evolution of the Mediterranean for a certain Atlantic-Mediterranean gateway. (3) By comparing these results to the known salinity thresholds of gypsum and halite saturation of sea water, but also to the late Miocene Mediterranean strontium

  7. Anomalous transport in discrete arcs and simulation of double layers in a model auroral circuit

    NASA Technical Reports Server (NTRS)

    Smith, Robert A.

    1987-01-01

    The evolution and long-time stability of a double layer (DL) in a discrete auroral arc requires that the parallel current in the arc, which may be considered uniform at the source, be diverted within the arc to charge the flanks of the U-shaped double layer potential structure. A simple model is presented in which this current redistribution is effected by anomalous transport based on electrostatic lower hybrid waves driven by the flank structure itself. This process provides the limiting constraint on the double layer potential. The flank charging may be represented as that of a nonlinear transmission line. A simplified model circuit, in which the transmission line is represented by a nonlinear impedance in parallel with a variable resistor, is incorporated in a one-dimensional simulation model to give the current density at the DL boundaries. Results are presented for the scaling of the DL potential as a function of the width of the arc and the saturation efficiency of the lower hybrid instability mechanism.

  8. Anomalous transport in discrete arcs and simulation of double layers in a model auroral circuit

    NASA Technical Reports Server (NTRS)

    Smith, Robert A.

    1987-01-01

    The evolution and long-time stability of a double layer in a discrete auroral arc requires that the parallel current in the arc, which may be considered uniform at the source, be diverted within the arc to charge the flanks of the U-shaped double-layer potential structure. A simple model is presented in which this current re-distribution is effected by anomalous transport based on electrostatic lower hybrid waves driven by the flank structure itself. This process provides the limiting constraint on the double-layer potential. The flank charging may be represented as that of a nonlinear transmission. A simplified model circuit, in which the transmission line is represented by a nonlinear impedance in parallel with a variable resistor, is incorporated in a 1-d simulation model to give the current density at the DL boundaries. Results are presented for the scaling of the DL potential as a function of the width of the arc and the saturation efficiency of the lower hybrid instability mechanism.

  9. Observations of the Evolution of Turbulent Dissipation within the Ocean Surface Boundary Layer: an OSMOSIS study

    NASA Astrophysics Data System (ADS)

    Lucas, N. S.; Allen, J.; Belcher, S. E.; Boyd, T.; Brannigan, L.; Inall, M.; Palmer, M.; Polton, J.; Rippeth, T. P.

    2016-02-01

    This study presents a new 9.5 day dataset showing the evolution of the Ocean Surface Boundary Layer (OSBL) and dissipation of turbulence kinetic energy (TKE), carried out as part of OSMOSIS[i], at a location in the North East Atlantic Ocean in September 2012. The TKE dissipation measurements were made using three methods; (i) repeated profiling between 100m and the surface by an Ocean Microstructure glider, (ii) three series of profiles made using a loosely tethered velocity microstructure glider and (iii) a moored pulse-pulse coherent high frequency ADCP. Supporting measurements show the evolution of the water column structure, including surface wave measurements from a TRIAXYS wave buoy. This data shows two distinct regimes; the first, spanning 4 days with relatively low winds, displays a distinct diurnal cycle with the deepening of the active mixing layer during the night which shoaled during the day. The second spanned a significant storm, (with maximum winds speeds reaching 20 m s-1 and significant wave heights reaching 6 m), during which, rather than a deepening of the mixed layer as predicted by classical theory, the primary effect was a broadening of the transition layer, similar to that found by Dohan and Davies (2011). During the storm, significant dissipation was observed throughout the surface mixed layer and into the transition layer, driving fluxes of heat downwards through the base of the surface mixed layer. [i] Ocean Surface Mixing and Submesoscale Interaction Study Dohan, K. & Davis, R.E., 2011. Mixing in the Transition Layer during Two Storm Events. Journal of Physical Oceanography. 41 (1). pp. 42-66.

  10. PARALLEL EVOLUTION OF QUASI-SEPARATRIX LAYERS AND ACTIVE REGION UPFLOWS

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

    Mandrini, C. H.; Cristiani, G. D.; Nuevo, F. A.

    2015-08-10

    Persistent plasma upflows were observed with Hinode’s EUV Imaging Spectrometer (EIS) at the edges of active region (AR) 10978 as it crossed the solar disk. We analyze the evolution of the photospheric magnetic and velocity fields of the AR, model its coronal magnetic field, and compute the location of magnetic null-points and quasi-sepratrix layers (QSLs) searching for the origin of EIS upflows. Magnetic reconnection at the computed null points cannot explain all of the observed EIS upflow regions. However, EIS upflows and QSLs are found to evolve in parallel, both temporarily and spatially. Sections of two sets of QSLs, calledmore » outer and inner, are found associated to EIS upflow streams having different characteristics. The reconnection process in the outer QSLs is forced by a large-scale photospheric flow pattern, which is present in the AR for several days. We propose a scenario in which upflows are observed, provided that a large enough asymmetry in plasma pressure exists between the pre-reconnection loops and lasts as long as a photospheric forcing is at work. A similar mechanism operates in the inner QSLs; in this case, it is forced by the emergence and evolution of the bipoles between the two main AR polarities. Our findings provide strong support for the results from previous individual case studies investigating the role of magnetic reconnection at QSLs as the origin of the upflowing plasma. Furthermore, we propose that persistent reconnection along QSLs does not only drive the EIS upflows, but is also responsible for the continuous metric radio noise-storm observed in AR 10978 along its disk transit by the Nançay Radio Heliograph.« less

  11. Modeling Co-evolution of Speech and Biology.

    PubMed

    de Boer, Bart

    2016-04-01

    Two computer simulations are investigated that model interaction of cultural evolution of language and biological evolution of adaptations to language. Both are agent-based models in which a population of agents imitates each other using realistic vowels. The agents evolve under selective pressure for good imitation. In one model, the evolution of the vocal tract is modeled; in the other, a cognitive mechanism for perceiving speech accurately is modeled. In both cases, biological adaptations to using and learning speech evolve, even though the system of speech sounds itself changes at a more rapid time scale than biological evolution. However, the fact that the available acoustic space is used maximally (a self-organized result of cultural evolution) is constant, and therefore biological evolution does have a stable target. This work shows that when cultural and biological traits are continuous, their co-evolution may lead to cognitive adaptations that are strong enough to detect empirically. Copyright © 2016 Cognitive Science Society, Inc.

  12. Synergy and Self-organization in Tribosystem’s evolution. Energy Model of Friction

    NASA Astrophysics Data System (ADS)

    Fedorov, S. V.; Assenova, E.

    2018-01-01

    Different approaches are known to treat self-organization in tribosystems, related to the structural adaptation in the formation of dissipative surface structures and of frictional or tribo-films, using of synergistic modifying of layers and coatings, e.g. of the selective material transfer during friction, etc. Regarding tribological processes in contact systems, self-organization is observed as spontaneous creation of higher ordered structures during the contact interaction. The proposed paper considers friction as process of transformation and dissipation of energy and process of elasto-plastic deformation localized in thin surface layers of the interacting bodies. Еnergetic interpretation of friction is proposed. Based on the energy balance equations of friction, the evolution of tribosystems is followed in its adaptive-dissipative character. It reflects the variable friction surfaces compatibility and the nonlinear dynamics of friction evolution. Structural-energy relationships in the contacting surfaces evolution are obtained. Maximum of tribosystem’s efficiency during the evolution is the stage of self-organzation of the friction surface layers, which is a state of abnormal low friction and wear.

  13. On the evolution of the Universe

    NASA Astrophysics Data System (ADS)

    Kondratenko, P. O.

    2014-12-01

    In this paper a model of creation and evolution of the universe in which the laws of physics are performed. The model implies that our Universe is a part of a Super-Universe as a separate layer in the fiber space, and the information communication exists between adjacent layers through the single point. During the formation of Super-Universe it was filled first a one-dimensional World of Field-time, then a two-dimensional (1+1) World was filled with energy and Planck's particles which carry the electric and magnetic charges. Completion of two-dimensional world filling leads to a "transfusion" of energy into the neighboring three-dimensional World which presents a world of known quarks which have the fractional electric charges, color charges, and spins. The next step is a "transfusion" of energy into the four-dimensional (3+1) World and the birth of the particles of this World. Evolution of this World has a completion by the brane creation of five-dimensional World. This evolution is accompanying by the birth of the entire set of stable and unstable heavy nuclei and atoms. A filling of each new layer at the fiber space does not bring the entropy into this space (i.e. cold and completely deterministic start of evolution). The proposed model supports the anthropic principle in the Universe.

  14. Modelling of surface fluxes and Urban Boundary Layer over an old mediterannean city core

    NASA Astrophysics Data System (ADS)

    Lemonsu, A.; Masson, V.; Grimmond, Cs. B.

    2003-04-01

    In the frameworks of the UBL(Urban Boundary Layer)-ESCOMPTE campaign, the Town Energy Balance (TEB) model was run in off-line mode for Marseille. TEB's performance is evaluated with observations of surface temperatures and surface energy balance fluxes collected during the campaign. Parameterization improvements allow to better represent the energy exchanges between the air inside the canyon and the atmosphere above the roof level. Then, high resolution Méso-NH simulations are done to study the 3-D structure and the evolution of the Urban Boundary Layer (UBL) over Marseille. Will will give a special attention to the impact of the seabord effects (sea-breeze circulation) on the UBL.

  15. Time-evolution of uniform momentum zones in a turbulent boundary layer

    NASA Astrophysics Data System (ADS)

    Laskari, Angeliki; Hearst, R. Jason; de Kat, Roeland; Ganapathisubramani, Bharathram

    2016-11-01

    Time-resolved planar particle image velocimetry (PIV) is used to analyse the organisation and evolution of uniform momentum zones (UMZs) in a turbulent boundary layer. Experiments were performed in a recirculating water tunnel on a streamwise-wall-normal plane extending approximately 0 . 5 δ × 1 . 8 δ , in x and y, respectively. In total 400,000 images were captured and for each of the resulting velocity fields, local peaks in the probability density distribution of the streamwise velocity were detected, indicating the instantaneous presence of UMZs throughout the boundary layer. The main characteristics of these zones are outlined and more specifically their velocity range and wall-normal extent. The variation of these characteristics with wall normal distance and total number of zones are also discussed. Exploiting the time information available, time-scales of zones that have a substantial coherence in time are analysed and results show that the zones' lifetime is dependent on both their momentum deficit level and the total number of zones present. Conditional averaging of the flow statistics seems to further indicate that a large number of zones is the result of a wall-dominant mechanism, while the opposite implies an outer-layer dominance.

  16. Boundary-layer cumulus over land: Some observations and conceptual models

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

    Stull, R.B.

    1993-09-01

    Starting in 1980, the Boundary Layer Research Team at the University of Wisconsin has been systematically studying the formation and evolution of nonprecipitating boundary-layer cumulus clouds (BLCu) in regions of fair weather (anticyclones) over land (Stull, 1980). Our approach is to quantify the average statistical characteristics of the surface, thermals, boundary layer, and clouds over horizontal regions of roughly 20 km in diameter. Within such a region over land, there is typically quite a variation in land use, and associated variations in surface albedo and moisture.

  17. The Internal Structure of Jupiter Family Comet Nuclei: The Talps or Layered Pile Model

    NASA Astrophysics Data System (ADS)

    Belton, Michael J.; Members of theDeep Impact Science Team

    2006-09-01

    The characteristics of layered structures seen on the nucleus of Tempel 1 in the Deep Impact images, and also seen on Wild 2 and Borrelly are noted. We consider the implications of the hypothesis that such structures are ubiquitous on Jupiter Family Comets and is an essential element of their internal stucture. If correct this hypothesis implies that the internal structure of JFCs are primordial remnants of the early agglomeration phase and that the physical structure of their interiors, except for possible compositional changes, is essentially as it was when they were formed. This hypothesis has implications for their place of origin and their subsequent collisional evolution. Current models of the latter are in conflict with this hypothesis. Possible resolutions of this conflict are noted. A new conceptual model of the interior of a typical JFC called the Talps or "layered pile" model is presented.

  18. A distributed snow-evolution modeling system (SnowModel)

    Treesearch

    Glen E. Liston; Kelly Elder

    2006-01-01

    SnowModel is a spatially distributed snow-evolution modeling system designed for application in landscapes, climates, and conditions where snow occurs. It is an aggregation of four submodels: MicroMet defines meteorological forcing conditions, EnBal calculates surface energy exchanges, SnowPack simulates snow depth and water-equivalent evolution, and SnowTran-3D...

  19. Thermal Rayleigh-Marangoni convection in a three-layer liquid-metal-battery model.

    PubMed

    Köllner, Thomas; Boeck, Thomas; Schumacher, Jörg

    2017-05-01

    The combined effects of buoyancy-driven Rayleigh-Bénard convection (RC) and surface tension-driven Marangoni convection (MC) are studied in a triple-layer configuration which serves as a simplified model for a liquid metal battery (LMB). The three-layer model consists of a liquid metal alloy cathode, a molten salt separation layer, and a liquid metal anode at the top. Convection is triggered by the temperature gradient between the hot electrolyte and the colder electrodes, which is a consequence of the release of resistive heat during operation. We present a linear stability analysis of the state of pure thermal conduction in combination with three-dimensional direct numerical simulations of the nonlinear turbulent evolution on the basis of a pseudospectral method. Five different modes of convection are identified in the configuration, which are partly coupled to each other: RC in the upper electrode, RC with internal heating in the molten salt layer, and MC at both interfaces between molten salt and electrode as well as anticonvection in the middle layer and lower electrode. The linear stability analysis confirms that the additional Marangoni effect in the present setup increases the growth rates of the linearly unstable modes, i.e., Marangoni and Rayleigh-Bénard instability act together in the molten salt layer. The critical Grashof and Marangoni numbers decrease with increasing middle layer thickness. The calculated thresholds for the onset of convection are found for realistic current densities of laboratory-sized LMBs. The global turbulent heat transfer follows scaling predictions for internally heated RC. The global turbulent momentum transfer is comparable with turbulent convection in the classical Rayleigh-Bénard case. In summary, our studies show that incorporating Marangoni effects generates smaller flow structures, alters the velocity magnitudes, and enhances the turbulent heat transfer across the triple-layer configuration.

  20. Thermal Rayleigh-Marangoni convection in a three-layer liquid-metal-battery model

    NASA Astrophysics Data System (ADS)

    Köllner, Thomas; Boeck, Thomas; Schumacher, Jörg

    2017-05-01

    The combined effects of buoyancy-driven Rayleigh-Bénard convection (RC) and surface tension-driven Marangoni convection (MC) are studied in a triple-layer configuration which serves as a simplified model for a liquid metal battery (LMB). The three-layer model consists of a liquid metal alloy cathode, a molten salt separation layer, and a liquid metal anode at the top. Convection is triggered by the temperature gradient between the hot electrolyte and the colder electrodes, which is a consequence of the release of resistive heat during operation. We present a linear stability analysis of the state of pure thermal conduction in combination with three-dimensional direct numerical simulations of the nonlinear turbulent evolution on the basis of a pseudospectral method. Five different modes of convection are identified in the configuration, which are partly coupled to each other: RC in the upper electrode, RC with internal heating in the molten salt layer, and MC at both interfaces between molten salt and electrode as well as anticonvection in the middle layer and lower electrode. The linear stability analysis confirms that the additional Marangoni effect in the present setup increases the growth rates of the linearly unstable modes, i.e., Marangoni and Rayleigh-Bénard instability act together in the molten salt layer. The critical Grashof and Marangoni numbers decrease with increasing middle layer thickness. The calculated thresholds for the onset of convection are found for realistic current densities of laboratory-sized LMBs. The global turbulent heat transfer follows scaling predictions for internally heated RC. The global turbulent momentum transfer is comparable with turbulent convection in the classical Rayleigh-Bénard case. In summary, our studies show that incorporating Marangoni effects generates smaller flow structures, alters the velocity magnitudes, and enhances the turbulent heat transfer across the triple-layer configuration.

  1. Layered Model for Radiation-Induced Chemical Evolution of Icy Surface Composition on Kuiper Belt and Oort Cloud Bodies

    NASA Technical Reports Server (NTRS)

    Cooper, John F.; Hill, Matthew E.; Richardson, John D.; Sturner, Steven J.

    2010-01-01

    The diversity of albedos and surface colors on observed Kuiper Belt and Inner Oort Cloud objects remains to be explained in terms of competition between primordial intrinsic versus exogenic drivers of surface and near-surface evolution. Earlier models have attempted without success to attribute this diversity to the relations between surface radiolysis from cosmic ray irradiation and gardening by meteoritic impacts. A more flexible approach considers the different depth-dependent radiation profiles produced by low-energy plasma, suprathermal, and maximally penetrating charged particles of the heliospheric and local interstellar radiation environments. Generally red objects of the dynamically cold (low inclination, circular orbit) Classical Kuiper Belt might be accounted for from erosive effects of plasma ions and reddening effects of high energy cosmic ray ions, while suprathermal keV-MeV ions could alternatively produce more color neutral surfaces. The deepest layer of more pristine ice can be brought to the surface from meter to kilometer depths by larger impact events and potentially by cryovolcanic activity. The bright surfaces of some larger objects, e.g. Eris, suggest ongoing resurfacing activity. Interactions of surface irradiation, resultant chemical oxidation, and near-surface cryogenic fluid reservoirs have been proposed to account for Enceladus cryovolcanism and may have further applications to other icy irradiated bodies. The diversity of causative processes must be understood to account for observationally apparent diversities of the object surfaces.

  2. Modeling crust-mantle evolution using radiogenic Sr, Nd, and Pb isotope systematics

    NASA Astrophysics Data System (ADS)

    Kumari, Seema; Paul, Debajyoti

    2015-04-01

    The present-day elemental and isotopic composition of Earth's terrestrial reservoirs can be used as geochemical constraints to study evolution of the crust-mantle system. A flexible open system evolutionary model of the Earth, comprising continental crust (CC), upper depleted mantle (UM) -source of mid-ocean ridge basalts (MORB), and lower mantle (LM) reservoir with a D" layer -source of ocean island basalts (OIB), and incorporating key radioactive isotope systematics (Rb-Sr, Sm-Nd, and U-Th-Pb), is solved numerically at 1 Ma time step for 4.55 Ga, the age of the Earth. The best possible solution is the one that produces the present-day concentrations as well as isotopic ratios in terrestrial reservoirs, compiled from published data. Different crustal growth scenarios (exponential, episodic, early and late growth), proposed in earlier studies, and its effect on the evolution of isotope systematics of terrestrial reservoirs is studied. Model simulations strongly favor a layered mantle structure satisfying majority of the isotopic constraints. In the successful model, which is similar to that proposed by Kellogg et al. (1999), the present-day UM comprises of 60% of mantle mass and extends to a depth 1600 km, whereas the LM becomes non-primitive and more enriched than the bulk silicate Earth, mainly due to addition of recycled crustal material. Modeling suggest that isotopic evolution of reservoirs is affected by the mode of crustal growth. Only two scenarios satisfied majority of the Rb-Sr and Sm-Nd isotopic constraints but failed to reproduce the present-day Pb-isotope systematics; exponential growth of crust (mean age, tc=2.3 Ga) and delayed and episodic growth (no growth for initial 900 Ma, tc=2.05 Ga) proposed by Patchett and Arndt (1986). However, assuming a slightly young Earth (4.45 Ga) better satisfies the Pb-isotope systematics. Although, the delayed crustal growth model satisfied Sr-Nd isotopic constraints, presence of early Hadean crust (4.03 and 4.4 Ga

  3. Simulation of double layers in a model auroral circuit with nonlinear impedance

    NASA Technical Reports Server (NTRS)

    Smith, R. A.

    1986-01-01

    A reduced circuit description of the U-shaped potential structure of a discrete auroral arc, consisting of the flank transmission line plus parallel-electric-field region, is used to provide the boundary condition for one-dimensional simulations of the double-layer evolution. The model yields asymptotic scalings of the double-layer potential, as a function of an anomalous transport coefficient alpha and of the perpendicular length scale l(a) of the arc. The arc potential phi(DL) scales approximately linearly with alpha, and for alpha fixed phi (DL) about l(a) to the z power. Using parameters appropriate to the auroral zone acceleration region, potentials of phi (DPL) 10 kV scale to projected ionospheric dimensions of about 1 km, with power flows of the order of magnitude of substorm dissipation rates.

  4. Mathematical modelling of cell layer growth in a hollow fibre bioreactor.

    PubMed

    Chapman, Lloyd A C; Whiteley, Jonathan P; Byrne, Helen M; Waters, Sarah L; Shipley, Rebecca J

    2017-04-07

    Generating autologous tissue grafts of a clinically useful volume requires efficient and controlled expansion of cell populations harvested from patients. Hollow fibre bioreactors show promise as cell expansion devices, owing to their potential for scale-up. However, further research is required to establish how to specify appropriate hollow fibre bioreactor operating conditions for expanding different cell types. In this study we develop a simple model for the growth of a cell layer seeded on the outer surface of a single fibre in a perfused hollow fibre bioreactor. Nutrient-rich culture medium is pumped through the fibre lumen and leaves the bioreactor via the lumen outlet or passes through the porous fibre walls and cell layer, and out via ports on the outer wall of the extra-capillary space. Stokes and Darcy equations for fluid flow in the fibre lumen, fibre wall, cell layer and extra-capillary space are coupled to reaction-advection-diffusion equations for oxygen and lactate transport through the bioreactor, and to a simple growth law for the evolution of the free boundary of the cell layer. Cells at the free boundary are assumed to proliferate at a rate that increases with the local oxygen concentration, and to die and detach from the layer if the local fluid shear stress or lactate concentration exceed critical thresholds. We use the model to predict operating conditions that maximise the cell layer growth for different cell types. In particular, we predict the optimal flow rate of culture medium into the fibre lumen and fluid pressure imposed at the lumen outlet for cell types with different oxygen demands and fluid shear stress tolerances, and compare the growth of the cell layer when the exit ports on the outside of the bioreactor are open with that when they are closed. Model simulations reveal that increasing the inlet flow rate and outlet fluid pressure increases oxygen delivery to the cell layer and, therefore, the growth rate of cells that are

  5. A Distributed Snow Evolution Modeling System (SnowModel)

    NASA Astrophysics Data System (ADS)

    Liston, G. E.; Elder, K.

    2004-12-01

    A spatially distributed snow-evolution modeling system (SnowModel) has been specifically designed to be applicable over a wide range of snow landscapes, climates, and conditions. To reach this goal, SnowModel is composed of four sub-models: MicroMet defines the meteorological forcing conditions, EnBal calculates surface energy exchanges, SnowMass simulates snow depth and water-equivalent evolution, and SnowTran-3D accounts for snow redistribution by wind. While other distributed snow models exist, SnowModel is unique in that it includes a well-tested blowing-snow sub-model (SnowTran-3D) for application in windy arctic, alpine, and prairie environments where snowdrifts are common. These environments comprise 68% of the seasonally snow-covered Northern Hemisphere land surface. SnowModel also accounts for snow processes occurring in forested environments (e.g., canopy interception related processes). SnowModel is designed to simulate snow-related physical processes occurring at spatial scales of 5-m and greater, and temporal scales of 1-hour and greater. These include: accumulation from precipitation; wind redistribution and sublimation; loading, unloading, and sublimation within forest canopies; snow-density evolution; and snowpack ripening and melt. To enhance its wide applicability, SnowModel includes the physical calculations required to simulate snow evolution within each of the global snow classes defined by Sturm et al. (1995), e.g., tundra, taiga, alpine, prairie, maritime, and ephemeral snow covers. The three, 25-km by 25-km, Cold Land Processes Experiment (CLPX) mesoscale study areas (MSAs: Fraser, North Park, and Rabbit Ears) are used as SnowModel simulation examples to highlight model strengths, weaknesses, and features in forested, semi-forested, alpine, and shrubland environments.

  6. Novel Approach for Modeling of Nonuniform Slag Layers and Air Gap in Continuous Casting Mold

    NASA Astrophysics Data System (ADS)

    Wang, Xudong; Kong, Lingwei; Yao, Man; Zhang, Xiaobing

    2017-02-01

    Various kinds of surface defects on the continuous casting slab usually originate from nonuniform heat transfer and mechanical behavior, especially during the initial solidification inside the mold. In this article, a model-coupled inverse heat transfer problem incorporating the effect of slag layers and air gap is developed to study the nonuniform distribution of liquid slag, solid slag, and air gap layers. The model considers not only the formation and evolution of slag layers and air gap but also the temperatures in the mold copper as measured by thermocouples. The simulation results from the model and the measured temperatures from experiments are shown to be in good agreement with each other. At the casting speed of 0.65 m/min, the liquid slag film disappears and transforms into solid slag entirely at about 400 mm away from meniscus, and an air gap begins to form. Until the mold exit, the maximum thickness of the solid slag layer and air gap gradually increases to 1.34 and 0.056 mm, respectively. The results illustrate that the magnitude and nonuniform distribution of the slag layers and air gap along the cross direction, correlating with heat flux between the shell and mold, eventually determine the temperature profiles of the mold hot face and slab surface. The proposed model may provide a convenient approach for analyzing nonuniform heat transfer and mechanical behaviors between the mold and slab in the real casting process.

  7. Performance Evaluation Model for Application Layer Firewalls.

    PubMed

    Xuan, Shichang; Yang, Wu; Dong, Hui; Zhang, Jiangchuan

    2016-01-01

    Application layer firewalls protect the trusted area network against information security risks. However, firewall performance may affect user experience. Therefore, performance analysis plays a significant role in the evaluation of application layer firewalls. This paper presents an analytic model of the application layer firewall, based on a system analysis to evaluate the capability of the firewall. In order to enable users to improve the performance of the application layer firewall with limited resources, resource allocation was evaluated to obtain the optimal resource allocation scheme in terms of throughput, delay, and packet loss rate. The proposed model employs the Erlangian queuing model to analyze the performance parameters of the system with regard to the three layers (network, transport, and application layers). Then, the analysis results of all the layers are combined to obtain the overall system performance indicators. A discrete event simulation method was used to evaluate the proposed model. Finally, limited service desk resources were allocated to obtain the values of the performance indicators under different resource allocation scenarios in order to determine the optimal allocation scheme. Under limited resource allocation, this scheme enables users to maximize the performance of the application layer firewall.

  8. Modelling language evolution: Examples and predictions

    NASA Astrophysics Data System (ADS)

    Gong, Tao; Shuai, Lan; Zhang, Menghan

    2014-06-01

    We survey recent computer modelling research of language evolution, focusing on a rule-based model simulating the lexicon-syntax coevolution and an equation-based model quantifying the language competition dynamics. We discuss four predictions of these models: (a) correlation between domain-general abilities (e.g. sequential learning) and language-specific mechanisms (e.g. word order processing); (b) coevolution of language and relevant competences (e.g. joint attention); (c) effects of cultural transmission and social structure on linguistic understandability; and (d) commonalities between linguistic, biological, and physical phenomena. All these contribute significantly to our understanding of the evolutions of language structures, individual learning mechanisms, and relevant biological and socio-cultural factors. We conclude the survey by highlighting three future directions of modelling studies of language evolution: (a) adopting experimental approaches for model evaluation; (b) consolidating empirical foundations of models; and (c) multi-disciplinary collaboration among modelling, linguistics, and other relevant disciplines.

  9. A stochastic model for tumor geometry evolution during radiation therapy in cervical cancer

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

    Liu, Yifang; Lee, Chi-Guhn; Chan, Timothy C. Y., E-mail: tcychan@mie.utoronto.ca

    2014-02-15

    Purpose: To develop mathematical models to predict the evolution of tumor geometry in cervical cancer undergoing radiation therapy. Methods: The authors develop two mathematical models to estimate tumor geometry change: a Markov model and an isomorphic shrinkage model. The Markov model describes tumor evolution by investigating the change in state (either tumor or nontumor) of voxels on the tumor surface. It assumes that the evolution follows a Markov process. Transition probabilities are obtained using maximum likelihood estimation and depend on the states of neighboring voxels. The isomorphic shrinkage model describes tumor shrinkage or growth in terms of layers of voxelsmore » on the tumor surface, instead of modeling individual voxels. The two proposed models were applied to data from 29 cervical cancer patients treated at Princess Margaret Cancer Centre and then compared to a constant volume approach. Model performance was measured using sensitivity and specificity. Results: The Markov model outperformed both the isomorphic shrinkage and constant volume models in terms of the trade-off between sensitivity (target coverage) and specificity (normal tissue sparing). Generally, the Markov model achieved a few percentage points in improvement in either sensitivity or specificity compared to the other models. The isomorphic shrinkage model was comparable to the Markov approach under certain parameter settings. Convex tumor shapes were easier to predict. Conclusions: By modeling tumor geometry change at the voxel level using a probabilistic model, improvements in target coverage and normal tissue sparing are possible. Our Markov model is flexible and has tunable parameters to adjust model performance to meet a range of criteria. Such a model may support the development of an adaptive paradigm for radiation therapy of cervical cancer.« less

  10. Lagrangian evolution of the marine boundary layer from the Cloud System Evolution in the Trades (CSET) campaign

    NASA Astrophysics Data System (ADS)

    Mohrmann, J.; Ghate, V. P.; McCoy, I. L.; Bretherton, C. S.; Wood, R.; Minnis, P.; Palikonda, R.

    2017-12-01

    The Cloud System Evolution in the Trades (CSET) field campaign took place July/August 2015 to study the evolution of clouds, precipitation, and aerosols in the stratocumulus-to-cumulus (Sc-Cu) transition region of the northeast Pacific marine boundary layer (MBL). Aircraft observations sampled across a wide range of cloud and aerosol conditions. The sampling strategy, where MBL airmasses were sampled with the NSF/NCAR Gulfstream-V (HIAPER) and resampled then at their advected location two days later, resulted in a dataset of 14 paired flights suitable for Lagrangian analysis. This analysis shows that Lagrangian coherence of long-lived species (namely CO and O3) across 48 hours are high, but that of subcloud aerosol, MBL depth, and cloud properties is limited. Geostationary satellite retrievals are compared against aircraft observations; these are combined with reanalysis data and HYSPLIT trajectories to document the Lagrangian evolution of cloud fraction, cloud droplet number concentration, liquid water path, estimated inversion strength (EIS), and MBL depth, which are used to expand upon and validate the aircraft-based analysis. Many of the trajectories sampled by the aircraft show a clear Sc-Cu transition. Although satellite cloud fraction and EIS were found to be strongly spatiotemporally correlated, changes in MBL cloud fraction along trajectories did not correlate with any measure of EIS forcing.

  11. A mathematical model of marine bacteriophage evolution.

    PubMed

    Pagliarini, Silvia; Korobeinikov, Andrei

    2018-03-01

    To explore how particularities of a host cell-virus system, and in particular host cell replication, affect viral evolution, in this paper we formulate a mathematical model of marine bacteriophage evolution. The intrinsic simplicity of real-life phage-bacteria systems, and in particular aquatic systems, for which the assumption of homogeneous mixing is well justified, allows for a reasonably simple model. The model constructed in this paper is based upon the Beretta-Kuang model of bacteria-phage interaction in an aquatic environment (Beretta & Kuang 1998 Math. Biosci. 149 , 57-76. (doi:10.1016/S0025-5564(97)10015-3)). Compared to the original Beretta-Kuang model, the model assumes the existence of a multitude of viral variants which correspond to continuously distributed phenotypes. It is noteworthy that the model is mechanistic (at least as far as the Beretta-Kuang model is mechanistic). Moreover, this model does not include any explicit law or mechanism of evolution; instead it is assumed, in agreement with the principles of Darwinian evolution, that evolution in this system can occur as a result of random mutations and natural selection. Simulations with a simplistic linear fitness landscape (which is chosen for the convenience of demonstration only and is not related to any real-life system) show that a pulse-type travelling wave moving towards increasing Darwinian fitness appears in the phenotype space. This implies that the overall fitness of a viral quasi-species steadily increases with time. That is, the simulations demonstrate that for an uneven fitness landscape random mutations combined with a mechanism of natural selection (for this particular system this is given by the conspecific competition for the resource) lead to the Darwinian evolution. It is noteworthy that in this system the speed of propagation of this wave (and hence the rate of evolution) is not constant but varies, depending on the current viral fitness and the abundance of susceptible

  12. Modeling the urban boundary layer

    NASA Technical Reports Server (NTRS)

    Bergstrom, R. W., Jr.

    1976-01-01

    A summary and evaluation is given of the Workshop on Modeling the Urban Boundary Layer; held in Las Vegas on May 5, 1975. Edited summaries from each of the session chairpersons are also given. The sessions were: (1) formulation and solution techniques, (2) K-theory versus higher order closure, (3) surface heat and moisture balance, (4) initialization and boundary problems, (5) nocturnal boundary layer, and (6) verification of models.

  13. An analytical model accounting for tip shape evolution during atom probe analysis of heterogeneous materials.

    PubMed

    Rolland, N; Larson, D J; Geiser, B P; Duguay, S; Vurpillot, F; Blavette, D

    2015-12-01

    An analytical model describing the field evaporation dynamics of a tip made of a thin layer deposited on a substrate is presented in this paper. The difference in evaporation field between the materials is taken into account in this approach in which the tip shape is modeled at a mesoscopic scale. It was found that the non-existence of sharp edge on the surface is a sufficient condition to derive the morphological evolution during successive evaporation of the layers. This modeling gives an instantaneous and smooth analytical representation of the surface that shows good agreement with finite difference simulations results, and a specific regime of evaporation was highlighted when the substrate is a low evaporation field phase. In addition, the model makes it possible to calculate theoretically the tip analyzed volume, potentially opening up new horizons for atom probe tomographic reconstruction. Copyright © 2015 Elsevier B.V. All rights reserved.

  14. Two types of asthenospheric layers and their evolution

    NASA Astrophysics Data System (ADS)

    Czechowski, Leszek; Grad, Marek

    2016-04-01

    -100 km, which could be interpreted as mechanical low Vp velocity zones, in contrast to thermal velocity zone in deeper asthenosphere. Conclusions 1. In general, two kinds of asthenospheres could exist: mainly of mechanical origin (or shear stress origin) and mainly of thermal origin. In our calculations the role of shear stresses and thermal effects is of the same order. 2. The evolution of σ could be very fast, so the asthenosphere of shear stress origin could be a transient, time-dependent feature. 3. The evolution of the system of two asthenospheres leads usually to origin of a thick lithosphere with characteristic two low S-wave velocity layers. We suggest that at least some of the observed thick continental lithospheres are of this origin. Acknowledgments This work was partially supported by the National Science Centre (grant 2011/01/B/ST10/06653). Computer resources of Interdisciplinary Centre for Mathematical and Computational Modeling of University of Warsaw were also used in the research

  15. Lagrangian mixed layer modeling of the western equatorial Pacific

    NASA Technical Reports Server (NTRS)

    Shinoda, Toshiaki; Lukas, Roger

    1995-01-01

    Processes that control the upper ocean thermohaline structure in the western equatorial Pacific are examined using a Lagrangian mixed layer model. The one-dimensional bulk mixed layer model of Garwood (1977) is integrated along the trajectories derived from a nonlinear 1 1/2 layer reduced gravity model forced with actual wind fields. The Global Precipitation Climatology Project (GPCP) data are used to estimate surface freshwater fluxes for the mixed layer model. The wind stress data which forced the 1 1/2 layer model are used for the mixed layer model. The model was run for the period 1987-1988. This simple model is able to simulate the isothermal layer below the mixed layer in the western Pacific warm pool and its variation. The subduction mechanism hypothesized by Lukas and Lindstrom (1991) is evident in the model results. During periods of strong South Equatorial Current, the warm and salty mixed layer waters in the central Pacific are subducted below the fresh shallow mixed layer in the western Pacific. However, this subduction mechanism is not evident when upwelling Rossby waves reach the western equatorial Pacific or when a prominent deepening of the mixed layer occurs in the western equatorial Pacific or when a prominent deepening of the mixed layer occurs in the western equatorial Pacific due to episodes of strong wind and light precipitation associated with the El Nino-Southern Oscillation. Comparison of the results between the Lagrangian mixed layer model and a locally forced Eulerian mixed layer model indicated that horizontal advection of salty waters from the central Pacific strongly affects the upper ocean salinity variation in the western Pacific, and that this advection is necessary to maintain the upper ocean thermohaline structure in this region.

  16. Layered Model for Radiation-Induced Chemical Evolution of Icy Surface Composition and Dynamics on Kuiper Belt and Oort Cloud Bodies

    NASA Technical Reports Server (NTRS)

    Cooper, John F.; Richardson, John D.

    2010-01-01

    The diversity of albedos and surface colors on observed Kuiper Belt and Inner Oort Cloud objects remains to be explained in terms of competition between primordial intrinsic versus exogenic drivers of surface and near-surface evolution. Earlier models have attempted without success to attribute this diversity to the relations between surface radiolysis from cosmic ray irradiation and gardening by meteoritic impacts. A more flexible approach considers the different depth-dependent radiation profiles produced by low-energy plasma, suprathermal, and maximally penetrating charged particles of the heliospheric and local interstellar radiation environment. Generally red objects of the dynamically cold (low inclination, circular orbit) Classical Kuiper Belt might be accounted for from erosive effects of plasma ions and reddening effects of high energy cosmic ray ions, while suprathermal keV-MeV ions could alternatively produce more color neutral surfaces. The deepest layer of more pristine ice can be brought to the surface from meter to kilometer depths by larger impact events and potentially by cryovolcanic activity. The bright surfaces of some larger objects, e.g. Eris, suggest ongoing resurfacing activity. Cycles of atmospheric formation and surface freezeout can further account for temporal variation as observed on Pluto. The diversity of causative processes must therefore be understood to account for observationally apparent diversities of the object surfaces.

  17. A Zonal Climate Model for the 1-D Mars Evolution Code: Explaining Meridiani Planum.

    NASA Astrophysics Data System (ADS)

    Manning, C. V.; McKay, C. P.; Zahnle, K. J.

    2005-12-01

    Recent MER Opportunity observations suggest there existed an extensive body of shallow water in the present Meridiani Planum during the late Noachian [1]. Observations of roughly contemporaneous valley networks show little net erosion [2]. Hypsometric analysis [3] finds that martian drainage basins are similar to terrestrial drainage basins in very arid regions. The immaturity of martian drainage basins suggests they were formed by infrequent fluvial action. If similar fluvial discharges are responsible for the laminations in the salt-bearing outcrops of Meridiani Planum, their explanation may require a climate model based on surface thermal equilibrium with diurnally averaged temperatures greater than freezing. In the context of Mars' chaotic obliquity, invoking a moderately thick atmosphere with seasonal insolation patterns may uncover the conditions under which the outcrops formed. We compounded a 1-D model of the evolution of Mars' inventories of CO2 over its lifetime called the Mars Evolution Code (MEC) [4]. We are assembling a zonal climate model that includes meridional heat transport, heat conduction to/from the regolith, latent heat deposition, and an albedo distribution based on the depositional patterns of ices. Since water vapor is an important greenhouse gas, and whose ice affects the albedo, we must install a full hydrological cycle. This requires a thermal model of the regolith to model diffusion of water vapor to/from a permafrost layer. Our model carries obliquity and eccentricity distributions consistent with Laskar et al. [5], so we will be able to model the movement of the ice cap with changes in obliquity. The climate model will be used to investigate the conditions under which ponded water could have occurred in the late Noachian, thus supplying a constraint on the free inventory of CO2 at that time. Our evolution code can then investigate Hesperian and Amazonian climates. The model could also be used to understand evidence of recent climate

  18. Modeling of Long-Term Evolution of Hydrophysical Fields of the Black Sea

    NASA Astrophysics Data System (ADS)

    Dorofeyev, V. L.; Sukhikh, L. I.

    2017-11-01

    The long-term evolution of the Black Sea dynamics (1980-2020) is reconstructed by numerical simulation. The model of the Black Sea circulation has 4.8 km horizontal spatial resolution and 40 levels in z-coordinates. The mixing processes in the upper layer are parameterized by Mellor-Yamada turbulent model. For the sea surface boundary conditions, atmospheric forcing functions were used, provided for the Black Sea region by the Euro mediterranean Center on Climate Change (CMCC) from the COSMO-CLM regional climate model. These data have a spatial resolution of 14 km and a daily temporal resolution. To evaluate the quality of the hydrodynamic fields derived from the simulation, they were compared with in-situ hydrological measurements and similar results from physical reanalysis of the Black Sea.

  19. Modeling of microstructure evolution in direct metal laser sintering: A phase field approach

    NASA Astrophysics Data System (ADS)

    Nandy, Jyotirmoy; Sarangi, Hrushikesh; Sahoo, Seshadev

    2017-02-01

    Direct Metal Laser Sintering (DMLS) is a new technology in the field of additive manufacturing, which builds metal parts in a layer by layer fashion directly from the powder bed. The process occurs within a very short time period with rapid solidification rate. Slight variations in the process parameters may cause enormous change in the final build parts. The physical and mechanical properties of the final build parts are dependent on the solidification rate which directly affects the microstructure of the material. Thus, the evolving of microstructure plays a vital role in the process parameters optimization. Nowadays, the increase in computational power allows for direct simulations of microstructures during materials processing for specific manufacturing conditions. In this study, modeling of microstructure evolution of Al-Si-10Mg powder in DMLS process was carried out by using a phase field approach. A MATLAB code was developed to solve the set of phase field equations, where simulation parameters include temperature gradient, laser scan speed and laser power. The effects of temperature gradient on microstructure evolution were studied and found that with increase in temperature gradient, the dendritic tip grows at a faster rate.

  20. Linearized Flux Evolution (LiFE): A technique for rapidly adapting fluxes from full-physics radiative transfer models

    NASA Astrophysics Data System (ADS)

    Robinson, Tyler D.; Crisp, David

    2018-05-01

    Solar and thermal radiation are critical aspects of planetary climate, with gradients in radiative energy fluxes driving heating and cooling. Climate models require that radiative transfer tools be versatile, computationally efficient, and accurate. Here, we describe a technique that uses an accurate full-physics radiative transfer model to generate a set of atmospheric radiative quantities which can be used to linearly adapt radiative flux profiles to changes in the atmospheric and surface state-the Linearized Flux Evolution (LiFE) approach. These radiative quantities describe how each model layer in a plane-parallel atmosphere reflects and transmits light, as well as how the layer generates diffuse radiation by thermal emission and by scattering light from the direct solar beam. By computing derivatives of these layer radiative properties with respect to dynamic elements of the atmospheric state, we can then efficiently adapt the flux profiles computed by the full-physics model to new atmospheric states. We validate the LiFE approach, and then apply this approach to Mars, Earth, and Venus, demonstrating the information contained in the layer radiative properties and their derivatives, as well as how the LiFE approach can be used to determine the thermal structure of radiative and radiative-convective equilibrium states in one-dimensional atmospheric models.

  1. A microwave scattering model for layered vegetation

    NASA Technical Reports Server (NTRS)

    Karam, Mostafa A.; Fung, Adrian K.; Lang, Roger H.; Chauhan, Narinder S.

    1992-01-01

    A microwave scattering model was developed for layered vegetation based on an iterative solution of the radiative transfer equation up to the second order to account for multiple scattering within the canopy and between the ground and the canopy. The model is designed to operate over a wide frequency range for both deciduous and coniferous forest and to account for the branch size distribution, leaf orientation distribution, and branch orientation distribution for each size. The canopy is modeled as a two-layered medium above a rough interface. The upper layer is the crown containing leaves, stems, and branches. The lower layer is the trunk region modeled as randomly positioned cylinders with a preferred orientation distribution above an irregular soil surface. Comparisons of this model with measurements from deciduous and coniferous forests show good agreements at several frequencies for both like and cross polarizations. Major features of the model needed to realize the agreement include allowance for: (1) branch size distribution, (2) second-order effects, and (3) tree component models valid over a wide range of frequencies.

  2. The evolution of nocturnal boundary-layer clouds in southern West Africa - a case study from DACCIWA

    NASA Astrophysics Data System (ADS)

    Adler, Bianca; Kalthoff, Norbert; Babić, Karmen; Lohou, Fabienne; Dione, Cheikh; Lothon, Marie; Pedruzo-Bagazgoitia, Xabier

    2017-04-01

    During the monsoon season, the atmospheric boundary layer in southern West Africa is characterised by various kinds of low-level clouds which experience a distinct diurnal cycle. During the night, extensive low-level stratiform clouds frequently form with a cloud base often less than few hundred metres above ground. After sunrise the cloud base slowly starts rising and eventually a transition to convective clouds occurs. While the existence of the clouds is documented in satellite images and synoptic observations, little is known about the mechanisms controlling their evolution. To provide observational evidence, a field campaign was conducted in southern West Africa in June and July 2016 within the framework of the Dynamics-aerosol-chemistry-cloud interactions in West Africa (DACCIWA) project. Comprehensive ground-based in situ and remote sensing measurements were performed at three different supersites in Ghana, Benin and Nigeria. In this contribution, we present the diurnal cycle of boundary-layer clouds for a typical day using data from a supersite at Savè in Benin. Due to the synergy of various instruments, we are able to obtain detailed information on the evolution of the clouds as well as on the boundary-layer structure with high temporal and vertical resolution. By combining ceilometer, cloud radar and microwave radiometer data we determined the cloud base, -depth and -density. The clouds form in the same layer as a nocturnal low-level jet (NLLJ), which we probe by sodar and UHF profiler. There is evidence for a strong link between the height and strength of the NLLJ and the density of the nocturnal clouds.

  3. The Imaging and Evolution of Seismic Layer 2A Thickness from a 0-70 Ma Oceanic Crustal Transect in the South Atlantic

    NASA Astrophysics Data System (ADS)

    Estep, J. D.; Reece, R.; Kardell, D. A.; Christeson, G. L.; Carlson, R. L.

    2017-12-01

    Seismic layer 2A, the uppermost igneous portion of oceanic crust, is commonly used to refer to the seismic velocities of upper crust that are bounded below by a steep vertical velocity gradient. Layer 2A velocities are known to increase with crustal age, from 2.5 km/s in crust <1 Ma to 4.5-5 km/s in crust >15 Ma. Thickness of layer 2A has been shown to increase by a factor of 2 within 1 Ma at fast spreading ridges and then remain relatively constant, while layer 2A maintains a fairly consistent thickness, irrespective of age, at slow-intermediate spreading ridges. Layer 2A thickness and velocity evolution studies to date have been largely focused on young oceanic crust very proximal to a spreading center with little investigation of changes (or lack thereof) that occur at crustal ages >10 Ma. We utilize a multichannel seismic dataset collected at 30° S in the western South Atlantic that continuously images 0 - 70 Ma oceanic crust along a single flowline generated at the slow-intermediate spreading Mid-Atlantic Ridge. We follow the methods of previous studies by processing the data to image the layer 2A event, which is then used for calculating thickness. 1D travel time forward modeling at regularly spaced age intervals across the transect provides for the conversion of time to depth thickness, and for determining the evolution of velocities with age. Our results show layer 2A in 20 Ma crust is roughly double the thickness of that in crust 0-5 Ma (830 vs. 440 m), but thickness does not appear to change beyond 20 Ma. The layer 2A event is readily observable in crust 0-50 Ma, is nearly completely absent in crust 50-65 Ma, and then reappears with anomalously high amplitude and lateral continuity in crust 65-70 Ma. Our results suggest that layer 2A thickens with age at the slow-intermediate spreading southern Mid-Atlantic Ridge, and that layer 2A either continues to evolve at the older crustal ages, well beyond the expected 10-15 Ma "mature age", or that external

  4. The polar layered deposits on Mars: Inference from thermal inertia modeling and geologic studies

    NASA Technical Reports Server (NTRS)

    Herkenhoff, K. E.

    1992-01-01

    It is widely believed that the Martian polar layered deposits record climate variations over at least the last 10 to 100 m.y., but the details of the processes involved and their relative roles in layer formation and evolution remain obscure. Weathering of the Martian layered deposits by sublimation of water ice can account for the thermal inertias, water vapor abundances, and geologic relationships observed in the Martian polar regions. The nonvolatile components of the layered deposits appears to consist mainly of bright red dust, with small amounts of dark dust. Dark dust, perhaps similar to the magnetic material found at the Viking Lander sites, may preferentially form filamentary residue particles upon weathering of the deposits. Once eroded, these particles may saltate to form the dark dunes found in both polar regions. This scenario for the origin and evolution of the dark material within the polar layered deposits is consistent with the available imaging and thermal data. Further experimental measurements of the thermophysical properties of magnetite and maghemite under Martian conditions are needed to better test this hypothesis.

  5. Considering bioactivity in modelling continental growth and the Earth's evolution

    NASA Astrophysics Data System (ADS)

    Höning, D.; Spohn, T.

    2013-09-01

    The complexity of planetary evolution increases with the number of interacting reservoirs. On Earth, even the biosphere is speculated to interact with the interior. It has been argued (e.g., Rosing et al. 2006; Sleep et al, 2012) that the formation of continents could be a consequence of bioactivity harvesting solar energy through photosynthesis to help build the continents and that the mantle should carry a chemical biosignature. Through plate tectonics, the surface biosphere can impact deep subduction zone processes and the interior of the Earth. Subducted sediments are particularly important, because they influence the Earth's interior in several ways, and in turn are strongly influenced by the Earth's biosphere. In our model, we use the assumption that a thick sedimentary layer of low permeability on top of the subducting oceanic crust, caused by a biologically enhanced weathering rate, can suppress shallow dewatering. This in turn leads to greater vailability of water in the source region of andesitic partial melt, resulting in an enhanced rate of continental production and regassing rate into the mantle. Our model includes (i) mantle convection, (ii) continental erosion and production, and (iii) mantle water degassing at mid-ocean ridges and regassing at subduction zones. The mantle viscosity of our model depends on (i) the mantle water concentration and (ii) the mantle temperature, whose time dependency is given by radioactive decay of isotopes in the Earth's mantle. Boundary layer theory yields the speed of convection and the water outgassing rate of the Earth's mantle. Our results indicate that present day values of continental surface area and water content of the Earth's mantle represent an attractor in a phase plane spanned by both parameters. We show that the biologic enhancement of the continental erosion rate is important for the system to reach this fixed point. An abiotic Earth tends to reach an alternative stable fixed point with a smaller

  6. Tailoring graphene layer-to-layer growth

    NASA Astrophysics Data System (ADS)

    Li, Yongtao; Wu, Bin; Guo, Wei; Wang, Lifeng; Li, Jingbo; Liu, Yunqi

    2017-06-01

    A layered material grown between a substrate and the upper layer involves complex interactions and a confined reaction space, representing an unusual growth mode. Here, we show multi-layer graphene domains grown on liquid or solid Cu by the chemical vapor deposition method via this ‘double-substrate’ mode. We demonstrate the interlayer-induced coupling effect on the twist angle in bi- and multi-layer graphene. We discover dramatic growth disunity for different graphene layers, which is explained by the ideas of a chemical ‘gate’ and a material transport process within a confined space. These key results lead to a consistent framework for understanding the dynamic evolution of multi-layered graphene flakes and tailoring the layer-to-layer growth for practical applications.

  7. A resonance based model of biological evolution

    NASA Astrophysics Data System (ADS)

    Damasco, Achille; Giuliani, Alessandro

    2017-04-01

    We propose a coarse grained physical model of evolution. The proposed model 'at least in principle' is amenable of an experimental verification even if this looks as a conundrum: evolution is a unique historical process and the tape cannot be reversed and played again. Nevertheless, we can imagine a phenomenological scenario tailored upon state transitions in physical chemistry in which different agents of evolution play the role of the elements of a state transition like thermal noise or resonance effects. The abstract model we propose can be of help for sketching hypotheses and getting rid of some well-known features of natural history like the so-called Cambrian explosion. The possibility of an experimental proof of the model is discussed as well.

  8. A Generative Angular Model of Protein Structure Evolution

    PubMed Central

    Golden, Michael; García-Portugués, Eduardo; Sørensen, Michael; Mardia, Kanti V.; Hamelryck, Thomas; Hein, Jotun

    2017-01-01

    Abstract Recently described stochastic models of protein evolution have demonstrated that the inclusion of structural information in addition to amino acid sequences leads to a more reliable estimation of evolutionary parameters. We present a generative, evolutionary model of protein structure and sequence that is valid on a local length scale. The model concerns the local dependencies between sequence and structure evolution in a pair of homologous proteins. The evolutionary trajectory between the two structures in the protein pair is treated as a random walk in dihedral angle space, which is modeled using a novel angular diffusion process on the two-dimensional torus. Coupling sequence and structure evolution in our model allows for modeling both “smooth” conformational changes and “catastrophic” conformational jumps, conditioned on the amino acid changes. The model has interpretable parameters and is comparatively more realistic than previous stochastic models, providing new insights into the relationship between sequence and structure evolution. For example, using the trained model we were able to identify an apparent sequence–structure evolutionary motif present in a large number of homologous protein pairs. The generative nature of our model enables us to evaluate its validity and its ability to simulate aspects of protein evolution conditioned on an amino acid sequence, a related amino acid sequence, a related structure or any combination thereof. PMID:28453724

  9. Coastal Foredune Evolution, Part 2: Modeling Approaches for Meso-Scale Morphologic Evolution

    DTIC Science & Technology

    2017-03-01

    ERDC/CHL CHETN-II-57 March 2017 Approved for public release; distribution is unlimited. Coastal Foredune Evolution, Part 2: Modeling Approaches...for Meso-Scale Morphologic Evolution by Margaret L. Palmsten1, Katherine L. Brodie2, and Nicholas J. Spore2 PURPOSE: This Coastal and Hydraulics...Engineering Technical Note (CHETN) is the second of two CHETNs focused on improving technologies to forecast coastal foredune evolution. Part 1

  10. Rosenzweig instability in a thin layer of a magnetic fluid

    NASA Astrophysics Data System (ADS)

    Korovin, V. M.

    2013-12-01

    A simple mathematical model of the initial stage of nonlinear evolution of the Rosenzweig instability in a thin layer of a nonlinearly magnetized viscous ferrofluid coating a horizontal nonmagnetizable plate is constructed on the basis of the system of equations and boundary conditions of ferrofluid dynamics. A dispersion relation is derived and analyzed using the linearized equations of this model. The critical magnetization of the initial layer with a flat free surface, the threshold wavenumber, and the characteristic time of evolution of the most rapidly growing mode are determined. The equation for the neutral stability curve, which is applicable for any physically admissible law of magnetization of a ferrofluid, is derived analytically.

  11. Misfit-layered Bi1.85 Sr2 Co1.85 O7.7-δ for the hydrogen evolution reaction: beyond van der Waals heterostructures.

    PubMed

    Chua, Chun Kiang; Sofer, Zdeněk; Jankovský, Ondřej; Pumera, Martin

    2015-03-16

    Recent research on stable 2D nanomaterials has led to the discovery of new materials for energy-conversion and energy-storage applications. A class of layered heterostructures known as misfit-layered chalcogenides consists of well-defined atomic layers and has previously been applied as thermoelectric materials for use as high-temperature thermoelectric batteries. The performance of such misfit-layered chalcogenides in electrochemical applications, specifically the hydrogen evolution reaction, is currently unexplored. Herein, a misfit-layered chalcogenide consisting of CoO2 layers interleaved with an SrO-BiO-BiO-SrO rock-salt block and having the formula Bi1.85 Sr2 Co1.85 O7.7-δ is synthesized and examined for its structural and electrochemical properties. The hydrogen-evolution performance of misfit-layered Bi1.85 Sr2 Co1.85 O7.7-δ , which has an overpotential of 589 mV and a Tafel slope of 51 mV per decade, demonstrates the promising potential of misfit-layered chalcogenides as electrocatalysts instead of classical carbon. © 2015 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.

  12. The Impact of Modeling Assumptions in Galactic Chemical Evolution Models

    NASA Astrophysics Data System (ADS)

    Côté, Benoit; O'Shea, Brian W.; Ritter, Christian; Herwig, Falk; Venn, Kim A.

    2017-02-01

    We use the OMEGA galactic chemical evolution code to investigate how the assumptions used for the treatment of galactic inflows and outflows impact numerical predictions. The goal is to determine how our capacity to reproduce the chemical evolution trends of a galaxy is affected by the choice of implementation used to include those physical processes. In pursuit of this goal, we experiment with three different prescriptions for galactic inflows and outflows and use OMEGA within a Markov Chain Monte Carlo code to recover the set of input parameters that best reproduces the chemical evolution of nine elements in the dwarf spheroidal galaxy Sculptor. This provides a consistent framework for comparing the best-fit solutions generated by our different models. Despite their different degrees of intended physical realism, we found that all three prescriptions can reproduce in an almost identical way the stellar abundance trends observed in Sculptor. This result supports the similar conclusions originally claimed by Romano & Starkenburg for Sculptor. While the three models have the same capacity to fit the data, the best values recovered for the parameters controlling the number of SNe Ia and the strength of galactic outflows, are substantially different and in fact mutually exclusive from one model to another. For the purpose of understanding how a galaxy evolves, we conclude that only reproducing the evolution of a limited number of elements is insufficient and can lead to misleading conclusions. More elements or additional constraints such as the Galaxy’s star-formation efficiency and the gas fraction are needed in order to break the degeneracy between the different modeling assumptions. Our results show that the successes and failures of chemical evolution models are predominantly driven by the input stellar yields, rather than by the complexity of the Galaxy model itself. Simple models such as OMEGA are therefore sufficient to test and validate stellar yields. OMEGA

  13. The Essential Role of Tethered Balloons in Characterizing Boundary Layer Structure and Evolution during Discover-AQ

    NASA Astrophysics Data System (ADS)

    Clark, R. D.

    2014-12-01

    The NASA DISCOVER-AQ (Deriving Information on Surface conditions from Column and Vertically Resolved Observations Relevant to Air Quality) provided the opportunity to observe the influence of local and regional circulations on the structure and evolution of the boundary layer (BL) and in turn study the associated effects on air quality and aerosol trends within four different airsheds. An extended network of ground-based instruments, balloon-borne profilers, and remote sensing instruments supported the in-situ airborne measurements made by the NASA aircraft in capturing the structure and evolution of the daytime BL. The Millersville University Atmospheric Research and Aerostat Facility (MARAF) is one of many assets deployed for DISCOVER-AQ. Central to MARAF is a heavy-lift-capacity tethered balloon (aerostat) used to obtain high resolution profiles of meteorological variables, trace gases, and particulates in the BL. The benefit of including a tethered balloon is that it can fill a data void between the surface and the lowest altitudes flown by the aircraft and provide critical time-height series for ground-based remote sensing instruments in the layer below their first range gate. MARAF also includes an acoustic sodar with RASS, MPL4 micropulse Lidar, 4-meter flux tower, rawinsonde system, and a suite of trace gas analyzers (O3, NOx/NO2/NO, CO, and SO2), 3-wavelength nephelometer, and particle sizers/counters spanning the range from 10 nm to 10 microns. MARAF is capable of providing a detailed and nearly continuous Eulerian characterization of the surface layer and lower BL, and with proper FAA airspace authorization, can be deployed both day and night. Three case studies will be presented that incorporate the MARAF into the combined assets of DISCOVER-AQ to better characterize: 1) bay breeze convergence, recirculation, and ramp-up events in Edgewood, MD in July 2011; 2) aerosol transport over Central Valley, CA in January 2013; and 3) multiple sea-bay breeze

  14. Statistics of certain models of evolution

    NASA Astrophysics Data System (ADS)

    Standish, Russell K.

    1999-02-01

    In a recent paper, Newman [J. Theo. Bio. 189, 235 (1997)] surveys the literature on power law spectra in evolution, self-organized criticality and presents a model of his own to arrive at a conclusion that self-organized criticality is not necessary for evolution. Not only did he miss a key model (Ecolab) that has a clear self-organized critical mechanism, but also Newman's model exhibits the same mechanism that gives rise to power law behavior, as does Ecolab. Newman's model is, in fact, a ``mean field'' approximation of a self-organized critical system. In this paper, I have also implemented Newman's model using the Ecolab software, removing the restriction that the number of species must remain constant. It turns out that the requirement of constant species number is nontrivial, leading to a global coupling between species that is similar in effect to the species interactions seen in Ecolab. In fact, the model must self-organize to a state where the long time average of speciations balances that of the extinctions; otherwise, the system either collapses or explodes. In view of this, Newman's model does not provide the hoped-for counterexample to the presence of self-organized criticality in evolution, but does provide a simple, almost analytic model that can be used to understand more intricate models such as Ecolab.

  15. Large Eddy Simulations of Continental Boundary Layer Clouds Observed during the RACORO Field Campaign

    NASA Astrophysics Data System (ADS)

    Endo, S.; Fridlind, A. M.; Lin, W.; Vogelmann, A. M.; Toto, T.; Liu, Y.

    2013-12-01

    Three cases of boundary layer clouds are analyzed in the FAst-physics System TEstbed and Research (FASTER) project, based on continental boundary-layer-cloud observations during the RACORO Campaign [Routine Atmospheric Radiation Measurement (ARM) Aerial Facility (AAF) Clouds with Low Optical Water Depths (CLOWD) Optical Radiative Observations] at the ARM Climate Research Facility's Southern Great Plains (SGP) site. The three 60-hour case study periods are selected to capture the temporal evolution of cumulus, stratiform, and drizzling boundary-layer cloud systems under a range of conditions, intentionally including those that are relatively more mixed or transitional in nature versus being of a purely canonical type. Multi-modal and temporally varying aerosol number size distribution profiles are derived from aircraft observations. Large eddy simulations (LESs) are performed for the three case study periods using the GISS Distributed Hydrodynamic Aerosol and Radiative Modeling Application (DHARMA) model and the WRF-FASTER model, which is the Weather Research and Forecasting (WRF) model implemented with forcing ingestion and other functions to constitute a flexible LES. The two LES models commonly capture the significant transitions of cloud-topped boundary layers in the three periods: diurnal evolution of cumulus layers repeating over multiple days, nighttime evolution/daytime diminution of thick stratus, and daytime breakup of stratus and stratocumulus clouds. Simulated transitions of thermodynamic structures of the cloud-topped boundary layers are examined by balloon-borne soundings and ground-based remote sensors. Aircraft observations are then used to statistically evaluate the predicted cloud droplet number size distributions under varying aerosol and cloud conditions. An ensemble approach is used to refine the model configuration for the combined use of observations with parallel LES and single-column model simulations. See Lin et al. poster for single

  16. Electromagnetic reflection from multi-layered snow models

    NASA Technical Reports Server (NTRS)

    Linlor, W. I.; Jiracek, G. R.

    1975-01-01

    The remote sensing of snow-pack characteristics with surface installations or an airborne system could have important applications in water-resource management and flood prediction. To derive some insight into such applications, the electromagnetic response of multilayered snow models is analyzed in this paper. Normally incident plane waves at frequencies ranging from 1 MHz to 10 GHz are assumed, and amplitude reflection coefficients are calculated for models having various snow-layer combinations, including ice layers. Layers are defined by thickness, permittivity, and conductivity; the electrical parameters are constant or prescribed functions of frequency. To illustrate the effect of various layering combinations, results are given in the form of curves of amplitude reflection coefficients versus frequency for a variety of models. Under simplifying assumptions, the snow thickness and effective dielectric constant can be estimated from the variations of reflection coefficient as a function of frequency.

  17. Numerical Modeling Studies of Wake Vortex Transport and Evolution Within the Planetary Boundary Layer

    NASA Technical Reports Server (NTRS)

    Lin, Yuh-Lang; Arya, S. Pal; Kaplan, Michael L.; Han, Jongil

    2000-01-01

    The fundamental objective of this research is study behavior of aircraft wake vortices within atmospheric boundary layer (ABL) in support of developing the system, Aircraft VOrtex Spacing System (AVOSS), under NASA's Terminal Area Productivity (TAR) program that will control aircraft spacing within the narrow approach corridors of airports. The purpose of the AVOSS system is to increase airport capacity by providing a safe reduction in separation of aircraft compared to the now-existing flight rules. In our first funding period (7 January 19994 - 6 April 1997), we have accomplished extensive model development and validation of ABL simulations. Using the validated model, in our second funding period (7 April 1997 - 6 April 2000) we have investigated the effects of ambient atmospheric turbulence on vortex decay and descent, Crow instability, and wake vortex interaction with the ground. Recognizing the crucial influence of ABL turbulence on wake vortex behavior, we have also developed a software generating vertical profiles of turbulent kinetic energy (TKE) or energy dissipation rate (EDR), which are, in turn, used as input data in the AVOSS prediction algorithms.

  18. Structural evolution in three and four-layer Aurivillius solid solutions: A comparative study versus relaxor properties

    NASA Astrophysics Data System (ADS)

    Tellier, Jenny; Boullay, Philippe; Ben Jennet, Dorra; Mercurio, Daniele

    2008-02-01

    Two solid solutions of three-layer Ba xBi 4- xNb xTi 3- xO 12 (0 ≤ x ≤ 1.2) and four-layer Aurivillius compounds (Na 0.5Bi 0.5) 1- xBa xBi 4Ti 4O 15 (0 ≤ x ≤ 1), which both present a ferroelectric to relaxor-like transition with increasing x, were synthesized by solid state reaction. The evolution of their crystal structures, as a function of x, was performed using Rietveld refinements from X-ray powder diffraction data. As x increases, the average crystal structures become less distorted with respect to the archetypal high temperature tetragonal one and the coordination number of Bi 3+ in M 2O 2 layers continuously changes from {4 + 2} to {4}. The relaxor behaviour which appears in samples for a tolerance factor t > 0.96 is associated with a general static disorder in A and M sites together with the presence of some Ba 2+ cations in M 2O 2 layers (less than 10%).

  19. Analytic Closed-Form Solution of a Mixed Layer Model for Stratocumulus Clouds

    NASA Astrophysics Data System (ADS)

    Akyurek, Bengu Ozge

    Stratocumulus clouds play an important role in climate cooling and are hard to predict using global climate and weather forecast models. Thus, previous studies in the literature use observations and numerical simulation tools, such as large-eddy simulation (LES), to solve the governing equations for the evolution of stratocumulus clouds. In contrast to the previous works, this work provides an analytic closed-form solution to the cloud thickness evolution of stratocumulus clouds in a mixed-layer model framework. With a focus on application over coastal lands, the diurnal cycle of cloud thickness and whether or not clouds dissipate are of particular interest. An analytic solution enables the sensitivity analysis of implicitly interdependent variables and extrema analysis of cloud variables that are hard to achieve using numerical solutions. In this work, the sensitivity of inversion height, cloud-base height, and cloud thickness with respect to initial and boundary conditions, such as Bowen ratio, subsidence, surface temperature, and initial inversion height, are studied. A critical initial cloud thickness value that can be dissipated pre- and post-sunrise is provided. Furthermore, an extrema analysis is provided to obtain the minima and maxima of the inversion height and cloud thickness within 24 h. The proposed solution is validated against LES results under the same initial and boundary conditions. Then, the proposed analytic framework is extended to incorporate multiple vertical columns that are coupled by advection through wind flow. This enables a bridge between the micro-scale and the mesoscale relations. The effect of advection on cloud evolution is studied and a sensitivity analysis is provided.

  20. Dual polarization micropulse lidar observations of the diurnal evolution of atmospheric boundary layer over a tropical coastal station

    NASA Astrophysics Data System (ADS)

    Rajeev, K.; Mishra, Manoj K.; Sunilkumar, S. V.; Sijikumar, S.

    2016-05-01

    High-resolution dual polarized micropulse lidar (MPL) observations have been used to investigate the diurnal evolution of atmospheric boundary layer (ABL) during winter (2008-2011) over Thiruvananthapuram (8.5°N, 77°E), a tropical coastal station located at southwest Peninsular India, adjoining the Arabian Sea. The lidar observations are compared with the boundary layer characteristics derived from concurrent balloon-borne radiosonde observations. This study shows that the mixed layer height over this coastal station generally increases from <300 m in the morning to 1500 m by the afternoon. Growth rate of the mixed layer height is rapid ( 350 m/hr) during 09-11 IST and slows down with time to <150 m/hr during 11-14 IST and <90 m/hr during 14-16 IST. Thermal internal boundary layer during the afternoon, caused by sea breeze circulation, extends up to 500 m altitude and is characterized by highly spherical aerosols, while a distinctly non-spherical aerosol layer appear above this altitude, in the return flow arising from the landmass.

  1. Modelling of backscatter from vegetation layers

    NASA Technical Reports Server (NTRS)

    Van Zyl, J. J.; Engheta, N.; Papas, C. H.; Elachi, C.; Zebker, H.

    1985-01-01

    A simple way to build up a library of models which may be used to distinguish between the different types of vegetation and ground surfaces by means of their backscatter properties is presented. The curve of constant power received by the antenna (Gamma sphere) is calculated for the given Stokes Scattering Operator, and model parameters are adopted of the most similar library model Gamma sphere. Results calculated for a single scattering model resembling coniferous trees are compared with the Gamma spheres of a model resembling tropical region trees. The polarization which would minimize the effect of either the ground surface or the vegetation layer can be calculated and used to analyze the backscatter from the ground surface/vegetation layer combination, and enhance the power received from the desired part of the combination.

  2. Enhanced photocatalytic hydrogen evolution from in situ formation of few-layered MoS2/CdS nanosheet-based van der Waals heterostructures.

    PubMed

    Iqbal, Shahid; Pan, Ziwei; Zhou, Kebin

    2017-05-25

    Here we report for the first time that the H 2 bubbles generated by photocatalytic water splitting are effective in the layer-by-layer exfoliation of MoS 2 nanocrystals (NCs) into few layers. The as-obtained few layers can be in situ assembled with CdS nanosheets (NSs) into van der Waals heterostructures (vdWHs) of few-layered MoS 2 /CdS NSs which, in turn, are effective in charge separation and transfer, leading to enhanced photocatalytic H 2 production activity. The few-layered MoS 2 /CdS vdWHs exhibited a H 2 evolution rate of 140 mmol g (CdS) -1 h -1 and achieved an apparent quantum yield of 66% at 420 nm.

  3. Simulation of Heterogeneous Atom Probe Tip Shapes Evolution during Field Evaporation Using a Level Set Method and Different Evaporation Models

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

    Xu, Zhijie; Li, Dongsheng; Xu, Wei

    2015-04-01

    In atom probe tomography (APT), accurate reconstruction of the spatial positions of field evaporated ions from measured detector patterns depends upon a correct understanding of the dynamic tip shape evolution and evaporation laws of component atoms. Artifacts in APT reconstructions of heterogeneous materials can be attributed to the assumption of homogeneous evaporation of all the elements in the material in addition to the assumption of a steady state hemispherical dynamic tip shape evolution. A level set method based specimen shape evolution model is developed in this study to simulate the evaporation of synthetic layered-structured APT tips. The simulation results ofmore » the shape evolution by the level set model qualitatively agree with the finite element method and the literature data using the finite difference method. The asymmetric evolving shape predicted by the level set model demonstrates the complex evaporation behavior of heterogeneous tip and the interface curvature can potentially lead to the artifacts in the APT reconstruction of such materials. Compared with other APT simulation methods, the new method provides smoother interface representation with the aid of the intrinsic sub-grid accuracy. Two evaporation models (linear and exponential evaporation laws) are implemented in the level set simulations and the effect of evaporation laws on the tip shape evolution is also presented.« less

  4. Nonlocal Poisson-Fermi double-layer models: Effects of nonuniform ion sizes on double-layer structure

    NASA Astrophysics Data System (ADS)

    Xie, Dexuan; Jiang, Yi

    2018-05-01

    This paper reports a nonuniform ionic size nonlocal Poisson-Fermi double-layer model (nuNPF) and a uniform ionic size nonlocal Poisson-Fermi double-layer model (uNPF) for an electrolyte mixture of multiple ionic species, variable voltages on electrodes, and variable induced charges on boundary segments. The finite element solvers of nuNPF and uNPF are developed and applied to typical double-layer tests defined on a rectangular box, a hollow sphere, and a hollow rectangle with a charged post. Numerical results show that nuNPF can significantly improve the quality of the ionic concentrations and electric fields generated from uNPF, implying that the effect of nonuniform ion sizes is a key consideration in modeling the double-layer structure.

  5. LEAMram (Trademark): Land Use Evolution and Impact Assessment Model Residential Attractiveness Model

    DTIC Science & Technology

    2006-09-01

    MEPLAN are popular in both the United States and overseas, and focus on identifying growth by income and housing costs. These and other models focus...CUF-2), SLEUTH, Landuse Evolution Assessment Model (LEAM™), Smart Places, and What If?: • CUF-2 uses a set of econometric models to project...ER D C/ CE R L TR -0 6 -2 8 LEAMram™: Land use Evolution and impact Assessment Model Residential Attractiveness Model James D

  6. Towards an alternative evolution model.

    PubMed

    van Waesberghe, H

    1982-01-01

    Lamarck and Darwin agreed on the inconstancy of species and on the exclusive gradualism of evolution (nature does not jump). Darwinism, revived as neo-Darwinism, was almost generally accepted from about 1930 till 1960. In the sixties the evolutionary importance of selection has been called in question by the neutralists. The traditional conception of the gene is disarranged by recent molecular-biological findings. Owing to the increasing confusion about the concept of genotype, this concept is reconsidered. The idea of the genotype as a cluster of genes is replaced by a cybernetical interpretation of the genotype. As nature does jump, exclusive gradualism is dismissed. Saltatory evolution is a natural phenomenon, provided by a sudden collapse of the thresholds which resist against evolution. The fossil record and the taxonomic system call for a macromutational interpretation. As Lamarck and Darwin overlooked the resistance of evolutionary thresholds, an alternative evolution model is needed, the first to be constructed on a palaeontological and taxonomic basis.

  7. Modeling the evolution of infrared galaxies: a parametric backward evolution model

    NASA Astrophysics Data System (ADS)

    Béthermin, M.; Dole, H.; Lagache, G.; Le Borgne, D.; Penin, A.

    2011-05-01

    Aims: We attempt to model the infrared galaxy evolution in as simple a way as possible and reproduce statistical properties such as the number counts between 15 μm and 1.1 mm, the luminosity functions, and the redshift distributions. We then use the fitted model to interpret observations from Spitzer, AKARI, BLAST, LABOCA, AzTEC, SPT, and Herschel, and make predictions for Planck and future experiments such as CCAT or SPICA. Methods: This model uses an evolution in density and luminosity of the luminosity function parametrized by broken power-laws with two breaks at redshift ~0.9 and 2, and contains the two populations of the Lagache model: normal and starburst galaxies. We also take into account the effect of the strong lensing of high-redshift sub-millimeter galaxies. This effect is significant in the sub-mm and mm range near 50 mJy. It has 13 free parameters and eight additional calibration parameters. We fit the parameters to the IRAS, Spitzer, Herschel, and AzTEC measurements with a Monte Carlo Markov chain. Results: The model adjusted to deep counts at key wavelengths reproduces the counts from mid-infrared to millimeter wavelengths, as well as the mid-infrared luminosity functions. We discuss the contribution to both the cosmic infrared background (CIB) and the infrared luminosity density of the different populations. We also estimate the effect of the lensing on the number counts, and discuss the discovery by the South Pole Telescope (SPT) of a very bright population lying at high redshift. We predict the contribution of the lensed sources to the Planck number counts, the confusion level for future missions using a P(D) formalism, and the Universe opacity to TeV photons caused by the CIB. Material of the model (software, tables and predictions) is available online.

  8. Dynamic Evolution Model Based on Social Network Services

    NASA Astrophysics Data System (ADS)

    Xiong, Xi; Gou, Zhi-Jian; Zhang, Shi-Bin; Zhao, Wen

    2013-11-01

    Based on the analysis of evolutionary characteristics of public opinion in social networking services (SNS), in the paper we propose a dynamic evolution model, in which opinions are coupled with topology. This model shows the clustering phenomenon of opinions in dynamic network evolution. The simulation results show that the model can fit the data from a social network site. The dynamic evolution of networks accelerates the opinion, separation and aggregation. The scale and the number of clusters are influenced by confidence limit and rewiring probability. Dynamic changes of the topology reduce the number of isolated nodes, while the increased confidence limit allows nodes to communicate more sufficiently. The two effects make the distribution of opinion more neutral. The dynamic evolution of networks generates central clusters with high connectivity and high betweenness, which make it difficult to control public opinions in SNS.

  9. Fluorine in the solar neighborhood: Chemical evolution models

    NASA Astrophysics Data System (ADS)

    Spitoni, E.; Matteucci, F.; Jönsson, H.; Ryde, N.; Romano, D.

    2018-04-01

    Context. In light of new observational data related to fluorine abundances in solar neighborhood stars, we present chemical evolution models testing various fluorine nucleosynthesis prescriptions with the aim to best fit those new data. Aim. We consider chemical evolution models in the solar neighborhood testing various nucleosynthesis prescriptions for fluorine production with the aim of reproducing the observed abundance ratios [F/O] versus [O/H] and [F/Fe] versus [Fe/H]. We study in detail the effects of various stellar yields on fluorine production. Methods: We adopted two chemical evolution models: the classical two-infall model, which follows the chemical evolution of halo-thick disk and thin disk phases; and the one-infall model, which is designed only for thin disk evolution. We tested the effects on the predicted fluorine abundance ratios of various nucleosynthesis yield sources, that is, asymptotic giant branch (AGB) stars, Wolf-Rayet (W-R) stars, Type II and Type Ia supernovae, and novae. Results: The fluorine production is dominated by AGB stars but the W-R stars are required to reproduce the trend of the observed data in the solar neighborhood with our chemical evolution models. In particular, the best model both for the two-infall and one-infall cases requires an increase by a factor of 2 of the W-R yields. We also show that the novae, even if their yields are still uncertain, could help to better reproduce the secondary behavior of F in the [F/O] versus [O/H] relation. Conclusions: The inclusion of the fluorine production by W-R stars seems to be essential to reproduce the new observed ratio [F/O] versus [O/H] in the solar neighborhood. Moreover, the inclusion of novae helps to reproduce the observed fluorine secondary behavior substantially.

  10. Self-optimizing, highly surface-active layered metal dichalcogenide catalysts for hydrogen evolution

    NASA Astrophysics Data System (ADS)

    Liu, Yuanyue; Wu, Jingjie; Hackenberg, Ken P.; Zhang, Jing; Wang, Y. Morris; Yang, Yingchao; Keyshar, Kunttal; Gu, Jing; Ogitsu, Tadashi; Vajtai, Robert; Lou, Jun; Ajayan, Pulickel M.; Wood, Brandon C.; Yakobson, Boris I.

    2017-09-01

    Low-cost, layered transition-metal dichalcogenides (MX2) based on molybdenum and tungsten have attracted substantial interest as alternative catalysts for the hydrogen evolution reaction (HER). These materials have high intrinsic per-site HER activity; however, a significant challenge is the limited density of active sites, which are concentrated at the layer edges. Here we unravel electronic factors underlying catalytic activity on MX2 surfaces, and leverage the understanding to report group-5 MX2 (H-TaS2 and H-NbS2) electrocatalysts whose performance instead mainly derives from highly active basal-plane sites, as suggested by our first-principles calculations and performance comparisons with edge-active counterparts. Beyond high catalytic activity, they are found to exhibit an unusual ability to optimize their morphology for enhanced charge transfer and accessibility of active sites as the HER proceeds, offering a practical advantage for scalable processing. The catalysts reach 10 mA cm-2 current density at an overpotential of ˜50-60 mV with a loading of 10-55 μg cm-2, surpassing other reported MX2 candidates without any performance-enhancing additives.

  11. 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

  12. Coupled wake boundary layer model of windfarms

    NASA Astrophysics Data System (ADS)

    Stevens, Richard; Gayme, Dennice; Meneveau, Charles

    2014-11-01

    We present a coupled wake boundary layer (CWBL) model that describes the distribution of the power output in a windfarm. The model couples the traditional, industry-standard wake expansion/superposition approach with a top-down model for the overall windfarm boundary layer structure. Wake models capture the effect of turbine positioning, while the top-down approach represents the interaction between the windturbine wakes and the atmospheric boundary layer. Each portion of the CWBL model requires specification of a parameter that is unknown a-priori. The wake model requires the wake expansion rate, whereas the top-down model requires the effective spanwise turbine spacing within which the model's momentum balance is relevant. The wake expansion rate is obtained by matching the mean velocity at the turbine from both approaches, while the effective spanwise turbine spacing is determined from the wake model. Coupling of the constitutive components of the CWBL model is achieved by iterating these parameters until convergence is reached. We show that the CWBL model predictions compare more favorably with large eddy simulation results than those made with either the wake or top-down model in isolation and that the model can be applied successfully to the Horns Rev and Nysted windfarms. The `Fellowships for Young Energy Scientists' (YES!) of the Foundation for Fundamental Research on Matter supported by NWO, and NSF Grant #1243482.

  13. Forecasting and modelling ice layer formation on the snowpack due to freezing precipitations in the Pyrenees

    NASA Astrophysics Data System (ADS)

    Quéno, Louis; Vionnet, Vincent; Cabot, Frédéric; Vrécourt, Dominique; Dombrowski-Etchevers, Ingrid

    2017-04-01

    In the Pyrenees, freezing precipitations in altitude occur at least once per winter, leading to the formation of a pure ice layer on the surface of the snowpack. It may lead to accidents and fatalities among mountaineers and skiers, with sometimes a higher human toll than avalanches. Such events are not predicted by the current operational systems for snow and avalanche hazard forecasting. A crowd-sourced database of surface ice layer occurrences is first built up, using reports from Internet mountaineering and ski-touring communities, to mitigate the lack of observations from conventional observation networks. A simple diagnostic of freezing precipitation is then developed, based on the cloud water content and screen temperature forecast by the Numerical Weather Prediction model AROME, operating at 2.5-km resolution. The performance of this diagnostic is assessed for the event of 5-6 January 2012, with a good representation of altitudinal and spatial distributions of the ice layer. An evaluation of the diagnostic for major events over five winters gives good skills of detection compared to the occurrences reported in the observation database. A new modelling of ice formation on the surface of the snowpack due to impinging supercooled water is added to the detailed snowpack model Crocus. It is combined to the atmospheric diagnostic of freezing precipitations and resulting snowpack simulations over a winter season capture well the formation of the main ice layers. Their influence on the snowpack stratigraphy is also realistically simulated. These simple methods enable to forecast the occurrence of surface ice layer formations with good confidence and to simulate their evolution within the snowpack, even if an accurate estimation of freezing precipitation amounts remains the main challenge.

  14. Modelling the evolution and diversity of cumulative culture

    PubMed Central

    Enquist, Magnus; Ghirlanda, Stefano; Eriksson, Kimmo

    2011-01-01

    Previous work on mathematical models of cultural evolution has mainly focused on the diffusion of simple cultural elements. However, a characteristic feature of human cultural evolution is the seemingly limitless appearance of new and increasingly complex cultural elements. Here, we develop a general modelling framework to study such cumulative processes, in which we assume that the appearance and disappearance of cultural elements are stochastic events that depend on the current state of culture. Five scenarios are explored: evolution of independent cultural elements, stepwise modification of elements, differentiation or combination of elements and systems of cultural elements. As one application of our framework, we study the evolution of cultural diversity (in time as well as between groups). PMID:21199845

  15. Chemical element transport in stellar evolution models

    PubMed Central

    Cassisi, Santi

    2017-01-01

    Stellar evolution computations provide the foundation of several methods applied to study the evolutionary properties of stars and stellar populations, both Galactic and extragalactic. The accuracy of the results obtained with these techniques is linked to the accuracy of the stellar models, and in this context the correct treatment of the transport of chemical elements is crucial. Unfortunately, in many respects calculations of the evolution of the chemical abundance profiles in stars are still affected by sometimes sizable uncertainties. Here, we review the various mechanisms of element transport included in the current generation of stellar evolution calculations, how they are implemented, the free parameters and uncertainties involved, the impact on the models and the observational constraints. PMID:28878972

  16. Chemical element transport in stellar evolution models.

    PubMed

    Salaris, Maurizio; Cassisi, Santi

    2017-08-01

    Stellar evolution computations provide the foundation of several methods applied to study the evolutionary properties of stars and stellar populations, both Galactic and extragalactic. The accuracy of the results obtained with these techniques is linked to the accuracy of the stellar models, and in this context the correct treatment of the transport of chemical elements is crucial. Unfortunately, in many respects calculations of the evolution of the chemical abundance profiles in stars are still affected by sometimes sizable uncertainties. Here, we review the various mechanisms of element transport included in the current generation of stellar evolution calculations, how they are implemented, the free parameters and uncertainties involved, the impact on the models and the observational constraints.

  17. Network evolution model for supply chain with manufactures as the core.

    PubMed

    Fang, Haiyang; Jiang, Dali; Yang, Tinghong; Fang, Ling; Yang, Jian; Li, Wu; Zhao, Jing

    2018-01-01

    Building evolution model of supply chain networks could be helpful to understand its development law. However, specific characteristics and attributes of real supply chains are often neglected in existing evolution models. This work proposes a new evolution model of supply chain with manufactures as the core, based on external market demand and internal competition-cooperation. The evolution model assumes the external market environment is relatively stable, considers several factors, including specific topology of supply chain, external market demand, ecological growth and flow conservation. The simulation results suggest that the networks evolved by our model have similar structures as real supply chains. Meanwhile, the influences of external market demand and internal competition-cooperation to network evolution are analyzed. Additionally, 38 benchmark data sets are applied to validate the rationality of our evolution model, in which, nine manufacturing supply chains match the features of the networks constructed by our model.

  18. Network evolution model for supply chain with manufactures as the core

    PubMed Central

    Jiang, Dali; Fang, Ling; Yang, Jian; Li, Wu; Zhao, Jing

    2018-01-01

    Building evolution model of supply chain networks could be helpful to understand its development law. However, specific characteristics and attributes of real supply chains are often neglected in existing evolution models. This work proposes a new evolution model of supply chain with manufactures as the core, based on external market demand and internal competition-cooperation. The evolution model assumes the external market environment is relatively stable, considers several factors, including specific topology of supply chain, external market demand, ecological growth and flow conservation. The simulation results suggest that the networks evolved by our model have similar structures as real supply chains. Meanwhile, the influences of external market demand and internal competition-cooperation to network evolution are analyzed. Additionally, 38 benchmark data sets are applied to validate the rationality of our evolution model, in which, nine manufacturing supply chains match the features of the networks constructed by our model. PMID:29370201

  19. Experimental evolution in silico: a custom-designed mathematical model for virulence evolution of Bacillus thuringiensis.

    PubMed

    Strauß, Jakob Friedrich; Crain, Philip; Schulenburg, Hinrich; Telschow, Arndt

    2016-08-01

    Most mathematical models on the evolution of virulence are based on epidemiological models that assume parasite transmission follows the mass action principle. In experimental evolution, however, mass action is often violated due to controlled infection protocols. This "theory-experiment mismatch" raises the question whether there is a need for new mathematical models to accommodate the particular characteristics of experimental evolution. Here, we explore the experimental evolution model system of Bacillus thuringiensis as a parasite and Caenorhabditis elegans as a host. Recent experimental studies with strict control of parasite transmission revealed that one-sided adaptation of B. thuringiensis with non-evolving hosts selects for intermediate or no virulence, sometimes coupled with parasite extinction. In contrast, host-parasite coevolution selects for high virulence and for hosts with strong resistance against B. thuringiensis. In order to explain the empirical results, we propose a new mathematical model that mimics the basic experimental set-up. The key assumptions are: (i) controlled parasite transmission (no mass action), (ii) discrete host generations, and (iii) context-dependent cost of toxin production. Our model analysis revealed the same basic trends as found in the experiments. Especially, we could show that resistant hosts select for highly virulent bacterial strains. Moreover, we found (i) that the evolved level of virulence is independent of the initial level of virulence, and (ii) that the average amount of bacteria ingested significantly affects the evolution of virulence with fewer bacteria ingested selecting for highly virulent strains. These predictions can be tested in future experiments. This study highlights the usefulness of custom-designed mathematical models in the analysis and interpretation of empirical results from experimental evolution. Copyright © 2016 The Authors. Published by Elsevier GmbH.. All rights reserved.

  20. Geological evolution of the North Sea: a dynamic 3D model including petroleum system elements

    NASA Astrophysics Data System (ADS)

    Sabine, Heim; Rüdiger, Lutz; Dirk, Kaufmann; Lutz, Reinhardt

    2013-04-01

    This study investigates the sedimentary basin evolution of the German North Sea with a focus on petroleum generation, migration and accumulation. The study is conducted within the framework of the project "Geoscientific Potential of the German North Sea (GPDN)", a joint project of federal (BGR, BSH) and state authorities (LBEG) with partners from industry and scientific institutions. Based on the structural model of the "Geotektonischer Atlas 3D" (GTA3D, LBEG), this dynamic 3D model contains additionally the northwestern part ("Entenschnabel" area) of the German North Sea. Geological information, e.g. lithostratigraphy, facies and structural data, provided by industry, was taken from published research projects, or literature data such as the Southern Permian Basin Atlas (SPBA; Doornenbal et al., 2010). Numerical modeling was carried out for a sedimentary succession containing 17 stratigraphic layers and several sublayers, representing the sedimentary deposition from the Devonian until Present. Structural details have been considered in terms of simplified faults and salt structures, as well as main erosion and salt movement events. Lithology, facies and the boundary conditions e.g. heat flow, paleo water-depth and sediment water interface temperature were assigned. The system calibration is based on geochemical and petrological data, such as maturity of organic matter (VRr) and present day temperature. Due to the maturity of the sedimentary organic matter Carboniferous layers are the major source rocks for gas generation. Main reservoir rocks are the Rotliegend sandstones, furthermore, sandstones of the Lower Triassic and Jurassic can serve as reservoir rocks in areas where the Zechstein salts are absent. The model provides information on the temperature and maturity distribution within the main source rock layers as well as information of potential hydrocarbon generation based on kinetic data for gas liberation. Finally, this dynamic 3D model offers a first

  1. Boundary-Layer Characteristics Over a Coastal Megacity

    NASA Astrophysics Data System (ADS)

    Melecio-Vazquez, D.; Ramamurthy, P.; Arend, M.; Moshary, F.; Gonzalez, J.

    2017-12-01

    Boundary-layer characteristics over New York City are analyzed for various local and synoptic conditions over several seasons. An array of vertical profilers, including a Doppler LiDAR, a micro-pulse LiDAR and a microwave radiometer are used to observe the structure and evolution of the boundary-layer. Additionally, an urbanized Weather Research and Forecasting (uWRF) model coupled to a high resolution landcover/land-use database is used to study the spatial variability in boundary layer characteristics. The summer daytime averaged potential temperature profile from the microwave radiometer shows the presence of a thermal internal boundary layer wherein a superadiabatic layer lies underneath a stable layer instead of a mixed-layer. Both the winter daytime and nighttime seasonal averages show that the atmosphere remains unstable near the surface and does not reach stable conditions during the nighttime. The mixing ratio seasonal averages show peaks in humidity near 200-m and 1100-m, above instrument level, which could result from sea breeze and anthropogenic sources. Ceilometer measurements show a high degree of variability in boundary layer height depending on wind direction. Comparison with uWRF results show that the model tends to overestimate convective efficiency for selected summer and winter cases and therefore shows a much deeper thermal boundary layer than the observed profiles. The model estimates a less humid atmosphere than seen in observations.

  2. A modeling study of marine boundary layer clouds

    NASA Technical Reports Server (NTRS)

    Wang, Shouping; Fitzjarrald, Daniel E.

    1993-01-01

    Marine boundary layer (MBL) clouds are important components of the earth's climate system. These clouds drastically reduce the amount of solar radiation absorbed by the earth, but have little effect on the emitted infrared radiation on top of the atmosphere. In addition, these clouds are intimately involved in regulating boundary layer turbulent fluxes. For these reasons, it is important that general circulation models used for climate studies must realistically simulate the global distribution of the MBL. While the importance of these cloud systems is well recognized, many physical processes involved in these clouds are poorly understood and their representation in large-scale models remains an unresolved problem. The present research aims at the development and improvement of the parameterization of these cloud systems and an understanding of physical processes involved. This goal is addressed in two ways. One is to use regional modeling approach to validate and evaluate two-layer marine boundary layer models using satellite and ground-truth observations; the other is to combine this simple model with a high-order turbulence closure model to study the transition processes from stratocumulus to shallow cumulus clouds. Progress made in this effort is presented.

  3. THM large spatial-temporal model to simulate the past 2 Ma hydrogeological evolution of Paris Basin including natural tracer transport as part of site characterization for radwaste repository project Cigéo - France

    NASA Astrophysics Data System (ADS)

    Benabderrahmane, A., Sr.

    2017-12-01

    Hydrogeological site characterization for deep geological high level and intermediate level long lived radioactive waste repository cover a large time scale needed for safety analysis and calculation. Hydrogeological performance of a site relies also on the effects of geodynamic evolution as tectonic uplift, erosion/sedimentation and climate including glaciation on the groundwater flow and solute and heat transfer. Thermo-Hydro-Mechanical model of multilayered aquifer system of Paris Basin is developed to reproduce the present time flow and the natural tracer (Helium) concentration profiles based on the last 2 Ma of geodynamic evolution. Present time geological conceptual model consist of 27 layers at Paris Basin (Triassic-Tertiary) with refinement at project site scale (29 layers from Triassic to Portlandian). Target layers are the clay host formation of Callovo-Oxfrodian age (160 Ma) and the surrounding aquifer layers of Oxfordian and Dogger. Modelled processes are: groundwater flow, heat and solutes (natural tracers) transport, freezing and thawing of groundwater (expansion and retreat of permafrost), deformation of the multilayered aquifer system induced by differential tectonic uplift and the hydro-mechanical stress effect as caused by erosion of the outcropping layers. Numerical simulation considers a period from 2 Ma BP and up to the present. Transient boundary conditions are governed by geodynamic processes: (i) modification of the geometry of the basin and (ii) temperatures along the topography will change according to a series of 15 identical climate cycles with multiple permafrost (glaciation) periods. Numerical model contains 71 layers and 18 million cells. The solution procedure solves three coupled systems of equations, head, temperature and concentrations, by the use of a finite difference method, and by applying extensive parallel processing. The major modelling results related to the processes of importance for site characterization as hydraulic

  4. Modeling aeolian dune and dune field evolution

    NASA Astrophysics Data System (ADS)

    Diniega, Serina

    Aeolian sand dune morphologies and sizes are strongly connected to the environmental context and physical processes active since dune formation. As such, the patterns and measurable features found within dunes and dune fields can be interpreted as records of environmental conditions. Using mathematical models of dune and dune field evolution, it should be possible to quantitatively predict dune field dynamics from current conditions or to determine past field conditions based on present-day observations. In this dissertation, we focus on the construction and quantitative analysis of a continuum dune evolution model. We then apply this model towards interpretation of the formative history of terrestrial and martian dunes and dune fields. Our first aim is to identify the controls for the characteristic lengthscales seen in patterned dune fields. Variations in sand flux, binary dune interactions, and topography are evaluated with respect to evolution of individual dunes. Through the use of both quantitative and qualitative multiscale models, these results are then extended to determine the role such processes may play in (de)stabilization of the dune field. We find that sand flux variations and topography generally destabilize dune fields, while dune collisions can yield more similarly-sized dunes. We construct and apply a phenomenological macroscale dune evolution model to then quantitatively demonstrate how dune collisions cause a dune field to evolve into a set of uniformly-sized dunes. Our second goal is to investigate the influence of reversing winds and polar processes in relation to dune slope and morphology. Using numerical experiments, we investigate possible causes of distinctive morphologies seen in Antarctic and martian polar dunes. Finally, we discuss possible model extensions and needed observations that will enable the inclusion of more realistic physical environments in the dune and dune field evolution models. By elucidating the qualitative and

  5. Full three-dimensional morphology evolution of amorphous thin films for atomic layer deposition

    NASA Astrophysics Data System (ADS)

    Jin, Lingpeng; Li, Yawei; Hu, Zhigao; Chu, Junhao

    2018-04-01

    We introduce a Monte Carlo model based on random deposition and diffusion limited aggregation in order to study the morphological evolution of deposition of nanofilm, which is difficult to carry out by the experimental methods. The instantaneous evolution of morphology and the corresponding parameters are observed when employing a novel perspective, modeling the aggregation of nanoscale units. Despite simplifying the chemical details, the simulation results qualitatively describe experiments with bulky precursors, and the strong dependence of growth rate on steric hindrance is obtained. Moreover, the well know behavior that the delay before steady growth is accurately predicted and analyzed based solely on modeling. Through this work, the great influence of steric hindrance on the initial stage of ALD is described.

  6. Two years observations on the diurnal evolution of coastal atmospheric boundary layer features over Thiruvananthapuram (8.5∘ N, 76.9∘ E), India

    NASA Astrophysics Data System (ADS)

    Anurose, T. J.; Subrahamanyam, D. Bala; Sunilkumar, S. V.

    2018-01-01

    The atmospheric boundary layer (ABL) over a given coastal station is influenced by the presence of mesoscale sea breeze circulation, together with the local and synoptic weather, which directly or indirectly modulate the vertical thickness of ABL ( z ABL). Despite its importance in the characterization of lower tropospheric processes and atmospheric modeling studies, a reliable climatology on the temporal evolution of z ABL is not available over the tropics. Here, we investigate the challenges involved in determination of the ABL heights, and discuss an objective method to define the vertical structure of coastal ABL. The study presents a two year morphology on the diurnal evolution of the vertical thickness of sea breeze flow ( z SBF) and z ABL in association with the altitudes of lifting condensation level ( z LCL) over Thiruvananthapuram (8.5∘ N, 76.9∘ E), a representative coastal station on the western coastline of the Indian sub-continent. We make use of about 516 balloon-borne GPS sonde measurements in the present study, which were carried out as part of the tropical tropopause dynamics field experiment under the climate and weather of the sun-earth system (CAWSES)-India program. Results obtained from the present study reveal major differences in the temporal evolution of the ABL features in relation to the strength of sea breeze circulation and monsoonal wind flow during the winter and summer monsoon respectively. The diurnal evolution in z ABL is very prominent in the winter monsoon as against the summer monsoon, which is attributed to the impact of large-scale monsoonal flow over the surface layer meteorology. For a majority of the database, the z LCL altitudes are found to be higher than that of the z ABL, indicating a possible decoupling of the ABL with the low-level clouds.

  7. Cloud System Evolution in the Trades—CSET

    NASA Astrophysics Data System (ADS)

    Albrecht, B. A.; Zuidema, P.; Bretherton, C. S.; Wood, R.; Ghate, V. P.

    2015-12-01

    The Cloud System Evolution in the Trades (CSET) study was designed to describe and explain the evolution of the boundary layer aerosol, cloud, and thermodynamic structures along trajectories within the north-Pacific trade-winds. The observational component of this study centered on 7 round-trips made by the NSF NCAR Gulfstream V (GV) between Sacramento, CA and Kona, Hawaii between 1 July and 15 August 2015. The CSET observing strategy used a Lagrangian approach to sample aerosol, cloud, and boundary layer properties upwind from the transition zone over the North Pacific and to resample these areas two days later. GFS forecast trajectories were used to plan the outbound flight to Hawaii and then updated forecast trajectories helped set the return flight plan two days later. Two key elements of the CSET observing system were the newly developed HIAPER Cloud Radar (HCR) and the HIAPER Spectral Resolution Lidar (HSRL). Together they provided unprecedented characterizations of aerosol, cloud and precipitation structures. A full suite of probes on the aircraft were used for in situ measurements of aerosol, cloud, precipitation, and turbulence properties during the low-level aircraft profiling portions of the flights. A wide range of boundary layer structures and aerosol, cloud, and precipitation conditions were observed during CSET. The cloud systems sampled included solid stratocumulus infused with smoke from Canadian wildfires, mesoscale (100-200 km) cloud-precipitation complexes, and patches of shallow cumuli in environments with accumulation mode aerosol concentrations of less than 50 cm-3. Ultra clean layers (UCLs with accumulation mode concentrations of less than 10 cm-3) were observed frequently near the top of the boundary layer and were often associated with shallow, gray (optically thin) layered clouds—features that are the subject of focused investigations by the CSET science team. The extent of aerosol, cloud, drizzle and boundary layer sampling that was

  8. Stress generation and evolution in oxide heteroepitaxy

    NASA Astrophysics Data System (ADS)

    Fluri, Aline; Pergolesi, Daniele; Wokaun, Alexander; Lippert, Thomas

    2018-03-01

    Many physical properties of oxides can be changed by inducing lattice distortions in the crystal through heteroepitaxial growth of thin films. The average lattice strain can often be tuned by changing the film thickness or using suitable buffer layers between film and substrate. The exploitation of the full potential of strain engineering for sample or device fabrication rests on the understanding of the fundamental mechanisms of stress generation and evolution. For this study an optical measurement of the substrate curvature is used to monitor in situ how the stress builds up and relaxes during the growth of oxide thin films by pulsed laser deposition. The relaxation behavior is correlated with the growth mode, which is monitored simultaneously with reflection high-energy electron diffraction. The stress relaxation data is fitted and compared with theoretical models for stress evolution which were established for semiconductor epitaxy. The initial stage of the growth appears to be governed by surface stress and surface energy effects, while the subsequent stress relaxation is found to be fundamentally different between films grown on single-crystal substrates and on buffer layers. The first case can be rationalized with established theoretical models, but these models fail in the attempt to describe the growth on buffer layers. This is most probably due to the larger average density of crystalline defects in the buffer layers, which leads to a two-step stress relaxation mechanism, driven first by the nucleation and later by the migration of dislocation lines.

  9. Evolution of crystal structure during the initial stages of ZnO atomic layer deposition

    DOE PAGES

    Boichot, R.; Tian, L.; Richard, M. -I.; ...

    2016-01-05

    In this study, a complementary suite of in situ synchrotron X-ray techniques is used to investigate both structural and chemical evolution during ZnO growth by atomic layer deposition. Focusing on the first 10 cycles of growth, we observe that the structure formed during the coalescence stage largely determines the overall microstructure of the film. Furthermore, by comparing ZnO growth on silicon with a native oxide with that on Al 2O 3(001), we find that even with lattice-mismatched substrates and low deposition temperatures, the crystalline texture of the films depend strongly on the nature of the interfacial bonds.

  10. Thermal Evolution of Neutron Stars

    NASA Astrophysics Data System (ADS)

    Geppert, Ulrich R. M. E.

    The thermal evolution of neutron stars is a subject of intense research, both theoretical and observational. The evolution depends very sensitively on the state of dense matter at supranuclear densities, which essentially controls the neutrino emission. The evolution depends, too, on the structure of the stellar outer layers which control the photon emission. Various internal heating processes and the magnetic field strength and structure will influence the thermal evolution. Of great importance for the cooling processes is also whether, when, and where superfluidity and superconductivity appear within the neutron star. This article describes and discusses these issues and presents neutron star cooling calculations based on a broad collection of equations of state for neutron star matter and internal magnetic field geometries. X-ray observations provide reliable data, which allow conclusions about the surface temperatures of neutron stars. To verify the thermal evolution models, the results of model calculations are compared with the body of observed surface temperatures and their distribution. Through these comparisons, a better understanding can be obtained of the physical processes that take place under extreme conditions in the interior of neutron

  11. Computational modeling of bedform evolution in rivers with implications for predictions of flood stage and bed evolution

    USGS Publications Warehouse

    Nelson, Jonathan M.; Shimizu, Yasuyuki; Giri, Sanjay; McDonald, Richard R.

    2010-01-01

    Uncertainties in flood stage prediction and bed evolution in rivers are frequently associated with the evolution of bedforms over a hydrograph. For the case of flood prediction, the evolution of the bedforms may alter the effective bed roughness, so predictions of stage and velocity based on assuming bedforms retain the same size and shape over a hydrograph will be incorrect. These same effects will produce errors in the prediction of the sediment transport and bed evolution, but in this latter case the errors are typically larger, as even small errors in the prediction of bedform form drag can make very large errors in predicting the rates of sediment motion and the associated erosion and deposition. In situations where flows change slowly, it may be possible to use empirical results that relate bedform morphology to roughness and effective form drag to avoid these errors; but in many cases where the bedforms evolve rapidly and are in disequilibrium with the instantaneous flow, these empirical methods cannot be accurately applied. Over the past few years, computational models for bedform development, migration, and adjustment to varying flows have been developed and tested with a variety of laboratory and field data. These models, which are based on detailed multidimensional flow modeling incorporating large eddy simulation, appear to be capable of predicting bedform dimensions during steady flows as well as their time dependence during discharge variations. In the work presented here, models of this type are used to investigate the impacts of bedform on stage and bed evolution in rivers during flood hydrographs. The method is shown to reproduce hysteresis in rating curves as well as other more subtle effects in the shape of flood waves. Techniques for combining the bedform evolution models with larger-scale models for river reach flow, sediment transport, and bed evolution are described and used to show the importance of including dynamic bedform effects in river

  12. An Inherited Efficiencies Model of Non-Genomic Evolution

    NASA Technical Reports Server (NTRS)

    New, Michael H.; Pohorille, Andrew

    1999-01-01

    A model for the evolution of biological systems in the absence of a nucleic acid-like genome is proposed and applied to model the earliest living organisms -- protocells composed of membrane encapsulated peptides. Assuming that the peptides can make and break bonds between amino acids, and bonds in non-functional peptides are more likely to be destroyed than in functional peptides, it is demonstrated that the catalytic capabilities of the system as a whole can increase. This increase is defined to be non-genomic evolution. The relationship between the proposed mechanism for evolution and recent experiments on self-replicating peptides is discussed.

  13. The thermochemical structure and evolution of Earth's mantle: constraints and numerical models.

    PubMed

    Tackley, Paul J; Xie, Shunxing

    2002-11-15

    Geochemical observations place several constraints on geophysical processes in the mantle, including a requirement to maintain several distinct reservoirs. Geophysical constraints limit plausible physical locations of these reservoirs to a thin basal layer, isolated deep 'piles' of material under large-scale mantle upwellings, high-viscosity blobs/plums or thin strips throughout the mantle, or some combination of these. A numerical model capable of simulating the thermochemical evolution of the mantle is introduced. Preliminary simulations are more differentiated than Earth but display some of the proposed thermochemical processes, including the generation of a high-mu mantle reservoir by recycling of crust, and the generation of a high-(3)He/(4)He reservoir by recycling of residuum, although the resulting high-(3)He/(4)He material tends to aggregate near the top, where mid-ocean-ridge melting should sample it. If primitive material exists as a dense basal layer, it must be much denser than subducted crust in order to retain its primitive (e.g. high-(3)He) signature. Much progress is expected in the near future.

  14. Equatorial dynamics in a 2 {1}/{2}- layer model

    NASA Astrophysics Data System (ADS)

    McCreary, Julian P.; Yu, Zuojun

    A nonlinear, 2 {1}/{2}- layer model is used to study the dynamics of wind-driven equatorial ocean circulation, including the generation of mean flows and instabilities. The model allows water to entrain into, and detrain from, the upper layer, and as a consequence the temperatures of the two active layers can vary. The model ocean basin is rectangular, extends 100° zonally, and for most solutions has open boundaries at 15°S and 15°N. All solutions are forced by a switched-on wind field that is an idealized version of the Pacific trades: the wind is westward, uniform in the meridional direction (so it has no curl), located primarily in the central and eastern oceans, and in most cases it has an amplitude of 0.5 dyn cm -2. For reasonable choices of parameters, solutions adjust to have a realistic equatorial circulation with a westward surface jet, an eastward undercurrent, and with upwelling and cool sea surface temperature in the eastern ocean. Most of the meridional circulation (81% of the transport) is part of a closed tropical circulation cell, in which water upwells in the eastern, equatorial ocean and downwells elsewhere in the basin; the rest participates in a mid-latitude circulation cell with lower-layer water entering the basin and upper-layer water leaving it through the open boundaries. Three basic types of unstable disturbances are generated in the eastern ocean: two of them are antisymmetric about the equator, one being surface-trapped with a period of about 21 days (f 1), and the other predominantly a lower-layer oscillation with periods ranging from 35 to 53 days (f 2) that causes the undercurrent to meander; the third is symmetric with a period of about 28 days (f 0) and a structure like that of a first-meridional-mode Rossby wave. The amplitudes of the disturbances are sensitive to model parameters, and as parameter values are varied systematically solutions appear to follow variations of the quasi-periodic route to turbulence, one of the common

  15. Modelling the transitional boundary layer

    NASA Technical Reports Server (NTRS)

    Narasimha, R.

    1990-01-01

    Recent developments in the modelling of the transition zone in the boundary layer are reviewed (the zone being defined as extending from the station where intermittency begins to depart from zero to that where it is nearly unity). The value of using a new non-dimensional spot formation rate parameter, and the importance of allowing for so-called subtransitions within the transition zone, are both stressed. Models do reasonably well in constant pressure 2-dimensional flows, but in the presence of strong pressure gradients further improvements are needed. The linear combination approach works surprisingly well in most cases, but would not be so successful in situations where a purely laminar boundary layer would separate but a transitional one would not. Intermittency-weighted eddy viscosity methods do not predict peak surface parameters well without the introduction of an overshooting transition function whose connection with the spot theory of transition is obscure. Suggestions are made for further work that now appears necessary for developing improved models of the transition zone.

  16. Boundary layer integral matrix procedure: Verification of models

    NASA Technical Reports Server (NTRS)

    Bonnett, W. S.; Evans, R. M.

    1977-01-01

    The three turbulent models currently available in the JANNAF version of the Aerotherm Boundary Layer Integral Matrix Procedure (BLIMP-J) code were studied. The BLIMP-J program is the standard prediction method for boundary 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 boundary 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.

  17. Obliquity variation in a Mars climate evolution model

    NASA Technical Reports Server (NTRS)

    Tyler, D.; Haberle, Robert M.

    1993-01-01

    The existence of layered terrain in both polar regions of Mars is strong evidence supporting a cyclic variation in climate. It has been suggested that periods of net deposition have alternated with periods of net erosion in creating the layered structure that is seen today. The cause for this cyclic climatic behavior is variation in the annually averaged latitudinal distribution of solar insolation in response to obliquity cycles. For Mars, obliquity variation leads to major climatological excursion due to the condensation and sublimation of the major atmospheric constituent, CO2. The atmosphere will collapse into the polar caps, or existing caps will rapidly sublimate into the atmosphere, dependent upon the polar surface heat balance and the direction of the change in obliquity. It has been argued that variations in the obliquity of Mars cause substantial departures from the current climatological values of the surface pressure and the amount of CO2 stored in both the planetary regolith and polar caps. In this new work we have modified the Haberle et al. model to incorporate variable obliquity by allowing the polar and equatorial insolation to become functions of obliquity, which we assume to vary sinusoidally in time. As obliquity varies in the model, there can be discontinuities in the time evolution of the model equilibrium values for surface pressure, regolith, and polar cap storage. The time constant, tau r, for the regolith to find equilibrium with the climate is estimated--depending on the depth, thermal conductivity, and porosity of the regolith--between 10(exp 4) and 10(exp 6) yr. Thus, using 2000-yr timesteps to move smoothly through the 0.1250 m.y. obliquity cycles, we have an atmosphere/regolith system that cannot be assumed in equilibrium. We have dealt with this problem by limiting the rate at which CO2, can move between the atmosphere and regolith, mimicking the diffusive nature and effects of the temperature and pressure waves, by setting the time

  18. Shaping asteroid models using genetic evolution (SAGE)

    NASA Astrophysics Data System (ADS)

    Bartczak, P.; Dudziński, G.

    2018-02-01

    In this work, we present SAGE (shaping asteroid models using genetic evolution), an asteroid modelling algorithm based solely on photometric lightcurve data. It produces non-convex shapes, orientations of the rotation axes and rotational periods of asteroids. The main concept behind a genetic evolution algorithm is to produce random populations of shapes and spin-axis orientations by mutating a seed shape and iterating the process until it converges to a stable global minimum. We tested SAGE on five artificial shapes. We also modelled asteroids 433 Eros and 9 Metis, since ground truth observations for them exist, allowing us to validate the models. We compared the derived shape of Eros with the NEAR Shoemaker model and that of Metis with adaptive optics and stellar occultation observations since other models from various inversion methods were available for Metis.

  19. Synthetic, multi-layer, self-oscillating vocal fold model fabrication.

    PubMed

    Murray, Preston R; Thomson, Scott L

    2011-12-02

    Sound for the human voice is produced via flow-induced vocal fold vibration. The vocal folds consist of several layers of tissue, each with differing material properties. Normal voice production relies on healthy tissue and vocal folds, and occurs as a result of complex coupling between aerodynamic, structural dynamic, and acoustic physical phenomena. Voice disorders affect up to 7.5 million annually in the United States alone and often result in significant financial, social, and other quality-of-life difficulties. Understanding the physics of voice production has the potential to significantly benefit voice care, including clinical prevention, diagnosis, and treatment of voice disorders. Existing methods for studying voice production include in vivo experimentation using human and animal subjects, in vitro experimentation using excised larynges and synthetic models, and computational modeling. Owing to hazardous and difficult instrument access, in vivo experiments are severely limited in scope. Excised larynx experiments have the benefit of anatomical and some physiological realism, but parametric studies involving geometric and material property variables are limited. Further, they are typically only able to be vibrated for relatively short periods of time (typically on the order of minutes). Overcoming some of the limitations of excised larynx experiments, synthetic vocal fold models are emerging as a complementary tool for studying voice production. Synthetic models can be fabricated with systematic changes to geometry and material properties, allowing for the study of healthy and unhealthy human phonatory aerodynamics, structural dynamics, and acoustics. For example, they have been used to study left-right vocal fold asymmetry, clinical instrument development, laryngeal aerodynamics, vocal fold contact pressure, and subglottal acoustics (a more comprehensive list can be found in Kniesburges et al.) Existing synthetic vocal fold models, however, have either

  20. Clustering network layers with the strata multilayer stochastic block model.

    PubMed

    Stanley, Natalie; Shai, Saray; Taylor, Dane; Mucha, Peter J

    2016-01-01

    Multilayer networks are a useful data structure for simultaneously capturing multiple types of relationships between a set of nodes. In such networks, each relational definition gives rise to a layer. While each layer provides its own set of information, community structure across layers can be collectively utilized to discover and quantify underlying relational patterns between nodes. To concisely extract information from a multilayer network, we propose to identify and combine sets of layers with meaningful similarities in community structure. In this paper, we describe the "strata multilayer stochastic block model" (sMLSBM), a probabilistic model for multilayer community structure. The central extension of the model is that there exist groups of layers, called "strata", which are defined such that all layers in a given stratum have community structure described by a common stochastic block model (SBM). That is, layers in a stratum exhibit similar node-to-community assignments and SBM probability parameters. Fitting the sMLSBM to a multilayer network provides a joint clustering that yields node-to-community and layer-to-stratum assignments, which cooperatively aid one another during inference. We describe an algorithm for separating layers into their appropriate strata and an inference technique for estimating the SBM parameters for each stratum. We demonstrate our method using synthetic networks and a multilayer network inferred from data collected in the Human Microbiome Project.

  1. Galactic evolution. I - Single-zone models. [encompassing stellar evolution and gas-star dynamic theories

    NASA Technical Reports Server (NTRS)

    Thuan, T. X.; Hart, M. H.; Ostriker, J. P.

    1975-01-01

    The two basic approaches of physical theory required to calculate the evolution of a galactic system are considered, taking into account stellar evolution theory and the dynamics of a gas-star system. Attention is given to intrinsic (stellar) physics, extrinsic (dynamical) physics, and computations concerning the fractionation of an initial mass of gas into stars. The characteristics of a 'standard' model and its variants are discussed along with the results obtained with the aid of these models.

  2. Research on System Coherence Evolution of Different Environmental Models

    NASA Astrophysics Data System (ADS)

    Zhang, Si-Qi; Lu, Jing-Bin; Li, Hong; Liu, Ji-Ping; Zhang, Xiao-Ru; Liu, Han; Liang, Yu; Ma, Ji; Liu, Xiao-Jing; Wu, Xiang-Yao

    2018-04-01

    In this paper, we have studied the evolution curve of two-level atomic system that the initial state is excited state. At the different of environmental reservoir models, which include the single Lorentzian, ideal photon band-gap, double Lorentzian and square Lorentzian reservoir, we researched the influence of these environmental reservoir models on the evolution of energy level population. At static no modulation, comparing the four environmental models, the atomic energy level population oscillation of square Lorentzian reservoir model is fastest, and the atomic system decoherence is slowest. Under dynamic modulation, comparing the photon band-gap model with the single Lorentzian reservoir model, no matter what form of dynamic modulation, the time of atoms decay to the ground state is longer for the photonic band-gap model. These conclusions make the idea of using the environmental change to modulate the coherent evolution of atomic system become true.

  3. Chempy: A flexible chemical evolution model for abundance fitting. Do the Sun's abundances alone constrain chemical evolution models?

    NASA Astrophysics Data System (ADS)

    Rybizki, Jan; Just, Andreas; Rix, Hans-Walter

    2017-09-01

    Elemental abundances of stars are the result of the complex enrichment history of their galaxy. Interpretation of observed abundances requires flexible modeling tools to explore and quantify the information about Galactic chemical evolution (GCE) stored in such data. Here we present Chempy, a newly developed code for GCE modeling, representing a parametrized open one-zone model within a Bayesian framework. A Chempy model is specified by a set of five to ten parameters that describe the effective galaxy evolution along with the stellar and star-formation physics: for example, the star-formation history (SFH), the feedback efficiency, the stellar initial mass function (IMF), and the incidence of supernova of type Ia (SN Ia). Unlike established approaches, Chempy can sample the posterior probability distribution in the full model parameter space and test data-model matches for different nucleosynthetic yield sets. It is essentially a chemical evolution fitting tool. We straightforwardly extend Chempy to a multi-zone scheme. As an illustrative application, we show that interesting parameter constraints result from only the ages and elemental abundances of the Sun, Arcturus, and the present-day interstellar medium (ISM). For the first time, we use such information to infer the IMF parameter via GCE modeling, where we properly marginalize over nuisance parameters and account for different yield sets. We find that 11.6+ 2.1-1.6% of the IMF explodes as core-collapse supernova (CC-SN), compatible with Salpeter (1955, ApJ, 121, 161). We also constrain the incidence of SN Ia per 103M⊙ to 0.5-1.4. At the same time, this Chempy application shows persistent discrepancies between predicted and observed abundances for some elements, irrespective of the chosen yield set. These cannot be remedied by any variations of Chempy's parameters and could be an indication of missing nucleosynthetic channels. Chempy could be a powerful tool to confront predictions from stellar

  4. Material parameter computation for multi-layered vocal fold models.

    PubMed

    Schmidt, Bastian; Stingl, Michael; Leugering, Günter; Berry, David A; Döllinger, Michael

    2011-04-01

    Today, the prevention and treatment of voice disorders is an ever-increasing health concern. Since many occupations rely on verbal communication, vocal health is necessary just to maintain one's livelihood. Commonly applied models to study vocal fold vibrations and air flow distributions are self sustained physical models of the larynx composed of artificial silicone vocal folds. Choosing appropriate mechanical parameters for these vocal fold models while considering simplifications due to manufacturing restrictions is difficult but crucial for achieving realistic behavior. In the present work, a combination of experimental and numerical approaches to compute material parameters for synthetic vocal fold models is presented. The material parameters are derived from deformation behaviors of excised human larynges. The resulting deformations are used as reference displacements for a tracking functional to be optimized. Material optimization was applied to three-dimensional vocal fold models based on isotropic and transverse-isotropic material laws, considering both a layered model with homogeneous material properties on each layer and an inhomogeneous model. The best results exhibited a transversal-isotropic inhomogeneous (i.e., not producible) model. For the homogeneous model (three layers), the transversal-isotropic material parameters were also computed for each layer yielding deformations similar to the measured human vocal fold deformations.

  5. Bypass transition and spot nucleation in boundary layers

    NASA Astrophysics Data System (ADS)

    Kreilos, Tobias; Khapko, Taras; Schlatter, Philipp; Duguet, Yohann; Henningson, Dan S.; Eckhardt, Bruno

    2016-08-01

    The spatiotemporal aspects of the transition to turbulence are considered in the case of a boundary-layer flow developing above a flat plate exposed to free-stream turbulence. Combining results on the receptivity to free-stream turbulence with the nonlinear concept of a transition threshold, a physically motivated model suggests a spatial distribution of spot nucleation events. To describe the evolution of turbulent spots a probabilistic cellular automaton is introduced, with all parameters directly obtained from numerical simulations of the boundary layer. The nucleation rates are then combined with the cellular automaton model, yielding excellent quantitative agreement with the statistical characteristics for different free-stream turbulence levels. We thus show how the recent theoretical progress on transitional wall-bounded flows can be extended to the much wider class of spatially developing boundary-layer flows.

  6. Nonlinear evolution of the first mode supersonic oblique waves in compressible boundary layers. Part 1: Heated/cooled walls

    NASA Technical Reports Server (NTRS)

    Gajjar, J. S. B.

    1993-01-01

    The nonlinear stability of an oblique mode propagating in a two-dimensional compressible boundary layer is considered under the long wave-length approximation. The growth rate of the wave is assumed to be small so that the concept of unsteady nonlinear critical layers can be used. It is shown that the spatial/temporal evolution of the mode is governed by a pair of coupled unsteady nonlinear equations for the disturbance vorticity and density. Expressions for the linear growth rate show clearly the effects of wall heating and cooling and in particular how heating destabilizes the boundary layer for these long wavelength inviscid modes at O(1) Mach numbers. A generalized expression for the linear growth rate is obtained and is shown to compare very well for a range of frequencies and wave-angles at moderate Mach numbers with full numerical solutions of the linear stability problem. The numerical solution of the nonlinear unsteady critical layer problem using a novel method based on Fourier decomposition and Chebychev collocation is discussed and some results are presented.

  7. Modeling of Microstructure Evolution During Alloy Solidification

    NASA Astrophysics Data System (ADS)

    Zhu, Mingfang; Pan, Shiyan; Sun, Dongke

    In recent years, considerable advances have been achieved in the numerical modeling of microstructure evolution during solidification. This paper presents the models based on the cellular automaton (CA) technique and lattice Boltzmann method (LBM), which can reproduce a wide variety of solidification microstructure features observed experimentally with an acceptable computational efficiency. The capabilities of the models are addressed by presenting representative examples encompassing a broad variety of issues, such as the evolution of dendritic structure and microsegregation in two and three dimensions, dendritic growth in the presence of convection, divorced eutectic solidification of spheroidal graphite irons, and gas porosity formation. The simulations offer insights into the underlying physics of microstructure formation during alloy solidification.

  8. THE SIMULATION OF FINE SCALE NOCTURNAL BOUNDARY LAYER MOTIONS WITH A MESO-SCALE ATMOSPHERIC MODEL

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

    Werth, D.; Kurzeja, R.; Parker, M.

    A field project over the Atmospheric Radiation Measurement-Clouds and Radiation Testbed (ARM-CART) site during a period of several nights in September, 2007 was conducted to explore the evolution of the low-level jet (LLJ). Data was collected from a tower and a sodar and analyzed for turbulent behavior. To study the full range of nocturnal boundary layer (NBL) behavior, the Regional Atmospheric Modeling System (RAMS) was used to simulate the ARM-CART NBL field experiment and validated against the data collected from the site. This model was run at high resolution, and is ideal for calculating the interactions among the various motionsmore » within the boundary layer and their influence on the surface. The model reproduces adequately the synoptic situation and the formation and dissolution cycles of the low-level jet, although it suffers from insufficient cloud production and excessive nocturnal cooling. The authors suggest that observed heat flux data may further improve the realism of the simulations both in the cloud formation and in the jet characteristics. In a higher resolution simulation, the NBL experiences motion on a range of timescales as revealed by a wavelet analysis, and these are affected by the presence of the LLJ. The model can therefore be used to provide information on activity throughout the depth of the NBL.« less

  9. An operational large-scale marine planetary boundary layer model

    NASA Technical Reports Server (NTRS)

    Brown, R. A.; Liu, W. T.

    1982-01-01

    A marine planetary boundary layer (PBL) model is presented and compared with data from sea-based experiments. The PBL model comprises two layers, the outer an Ekman-Taylor layer with stratification-dependent secondary flow, and the logarithmic surface layer corrected for stratification and humidity effects and variable surface roughness. Corrections are noted for air much warmer than water in stable conditions and for low wind speeds. The layers are analytically defined along with similarity relations and a resistance law for inclusion in a program. An additional interfacial layer correction is developed and shown to be significant for heat flux calculations. Experimental data from GOASEX were used to predict the windfield in the Gulf of Alaska, and JASIN data was used for windfields SE of Iceland. The JASIN-derived wind field predictions were accurate to within 1 m/sec and 10 deg in a 200 km triangle.

  10. Interpretation of scrape-off layer profile evolution and first-wall ion flux statistics on JET using a stochastic framework based on fillamentary motion

    NASA Astrophysics Data System (ADS)

    Walkden, N. R.; Wynn, A.; Militello, F.; Lipschultz, B.; Matthews, G.; Guillemaut, C.; Harrison, J.; Moulton, D.; Contributors, JET

    2017-08-01

    This paper presents the use of a novel modelling technique based around intermittent transport due to filament motion, to interpret experimental profile and fluctuation data in the scrape-off layer (SOL) of JET during the onset and evolution of a density profile shoulder. A baseline case is established, prior to shoulder formation, and the stochastic model is shown to be capable of simultaneously matching the time averaged profile measurement as well as the PDF shape and autocorrelation function from the ion-saturation current time series at the outer wall. Aspects of the stochastic model are then varied with the aim of producing a profile shoulder with statistical measurements consistent with experiment. This is achieved through a strong localised reduction in the density sink acting on the filaments within the model. The required reduction of the density sink occurs over a highly localised region with the timescale of the density sink increased by a factor of 25. This alone is found to be insufficient to model the expansion and flattening of the shoulder region as the density increases, which requires additional changes within the stochastic model. An example is found which includes both a reduction in the density sink and filament acceleration and provides a consistent match to the experimental data as the shoulder expands, though the uniqueness of this solution can not be guaranteed. Within the context of the stochastic model, this implies that the localised reduction in the density sink can trigger shoulder formation, but additional physics is required to explain the subsequent evolution of the profile.

  11. LAPSUS: soil erosion - landscape evolution model

    NASA Astrophysics Data System (ADS)

    van Gorp, Wouter; Temme, Arnaud; Schoorl, Jeroen

    2015-04-01

    LAPSUS is a soil erosion - landscape evolution model which is capable of simulating landscape evolution of a gridded DEM by using multiple water, mass movement and human driven processes on multiple temporal and spatial scales. It is able to deal with a variety of human landscape interventions such as landuse management and tillage and it can model their interactions with natural processes. The complex spatially explicit feedbacks the model simulates demonstrate the importance of spatial interaction of human activity and erosion deposition patterns. In addition LAPSUS can model shallow landsliding, slope collapse, creep, solifluction, biological and frost weathering, fluvial behaviour. Furthermore, an algorithm to deal with natural depressions has been added and event-based modelling with an improved infiltration description and dust deposition has been pursued. LAPSUS has been used for case studies in many parts of the world and is continuously developing and expanding. it is now available for third-party and educational use. It has a comprehensive user interface and it is accompanied by a manual and exercises. The LAPSUS model is highly suitable to quantify and understand catchment-scale erosion processes. More information and a download link is available on www.lapsusmodel.nl.

  12. Quantifying the Stable Boundary Layer Structure and Evolution during T-REX 2006

    DTIC Science & Technology

    2014-09-30

    integrating surface observations, data from in-situ measurements, and a nested numerical model with two related topics was conducted in this project. the WRF ...as well as quantify differences at a fine scale model output using the different turbulent mixing/diffusion options in the WRF -ARW model; and (2... WRF model planetary boundary layer schemes were also conducted to study a downslope windstorm and rotors in Las Vegas valley. Two events (March 20

  13. Probability theory for 3-layer remote sensing radiative transfer model: univariate case.

    PubMed

    Ben-David, Avishai; Davidson, Charles E

    2012-04-23

    A probability model for a 3-layer radiative transfer model (foreground layer, cloud layer, background layer, and an external source at the end of line of sight) has been developed. The 3-layer model is fundamentally important as the primary physical model in passive infrared remote sensing. The probability model is described by the Johnson family of distributions that are used as a fit for theoretically computed moments of the radiative transfer model. From the Johnson family we use the SU distribution that can address a wide range of skewness and kurtosis values (in addition to addressing the first two moments, mean and variance). In the limit, SU can also describe lognormal and normal distributions. With the probability model one can evaluate the potential for detecting a target (vapor cloud layer), the probability of observing thermal contrast, and evaluate performance (receiver operating characteristics curves) in clutter-noise limited scenarios. This is (to our knowledge) the first probability model for the 3-layer remote sensing geometry that treats all parameters as random variables and includes higher-order statistics. © 2012 Optical Society of America

  14. Continuous "in vitro" Evolution of a Ribozyme Ligase: A Model Experiment for the Evolution of a Biomolecule

    ERIC Educational Resources Information Center

    Ledbetter, Michael P.; Hwang, Tony W.; Stovall, Gwendolyn M.; Ellington, Andrew D.

    2013-01-01

    Evolution is a defining criterion of life and is central to understanding biological systems. However, the timescale of evolutionary shifts in phenotype limits most classroom evolution experiments to simple probability simulations. "In vitro" directed evolution (IVDE) frequently serves as a model system for the study of Darwinian…

  15. Tectono-sedimentary evolution of the Permian-Triassic extension event in the Zagros basin (Iran): results from analogue modelling

    NASA Astrophysics Data System (ADS)

    Madani-kivi, M.; Zulauf, G.

    2015-12-01

    Since the 1970s, the largest oil and gas reservoirs have been discovered in the Permian-Early Triassic formationsin Saudi Arabia. Thus, this time period is important for the discovery of new oil reserves in Iran. The Arabian passivecontinental margin has undergone lithospheric extension during the Permian-Triassic, which led to the formation of theNeo-Tethys. The aim of this paper is to describe the development of the continental rift basin in the Zagros region basedon the tectono-sedimentological evolution. We have studied well-log data to specify the distribution of synrift depositsin the Zagros and have related this information to the modelling. Environmental changes indicated by various sedimentarysequences, from a siliciclastic basin to a carbonate platform setting, are described. The Cambrian Hormuz salt, whichoverlies the metamorphosed Precambrian basement, becomes effective as a basal detachment layer influencing the styleof overburden deformation during the Permian-Triassic extension event. We have investigated the formation of variousstructures linked to the presence or absence of the Hormuz layer by analogue modelling and relating these structures to theLate Palaeozoic sedimentation. Based on results of the analogue modelling, we argue that the basal detachment layer (Hormuzseries) has contributed to the various structural styles of the extensional basin development in the Fars domain and theLorestan domain.

  16. The effect of ilmenite viscosity on the dynamics and evolution of an overturned lunar cumulate mantle

    NASA Astrophysics Data System (ADS)

    Zhang, Nan; Dygert, Nick; Liang, Yan; Parmentier, E. M.

    2017-07-01

    Lunar cumulate mantle overturn and the subsequent upwelling of overturned mantle cumulates provide a potential framework for understanding the first-order thermochemical evolution of the Moon. Upwelling of ilmenite-bearing cumulates (IBCs) after the overturn has a dominant influence on the dynamics and long-term thermal evolution of the lunar mantle. An important parameter determining the stability and convective behavior of the IBC is its viscosity, which was recently constrained through rock deformation experiments. To examine the effect of IBC viscosity on the upwelling of overturned lunar cumulate mantle, here we conduct three-dimensional mantle convection models with an evolving core superposed by an IBC-rich layer, which resulted from mantle overturn after magma ocean solidification. Our modeling shows that a reduction of mantle viscosity by 1 order of magnitude, due to the presence of ilmenite, can dramatically change convective planform and long-term lunar mantle evolution. Our model results suggest a relatively stable partially molten IBC layer that has surrounded the lunar core to the present day.Plain Language SummaryThe Moon's mantle is locally ilmenite rich. Previous <span class="hlt">models</span> exploring the convective <span class="hlt">evolution</span> of the lunar mantle did not consider the effects of ilmenite viscosity. Recent rock deformation experiments demonstrate that Fe-Ti oxide (ilmenite) is a low viscosity phase compared to olivine and other silicate minerals. Our <span class="hlt">modeling</span> shows that ilmenite changes the lunar mantle plume process. An ilmenite-rich <span class="hlt">layer</span> around the lunar core would be highly stable throughout geologic time, consistent with a partially molten, low viscosity <span class="hlt">layer</span> around the core inferred from seismic attenuation and tidal dissipation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016MMI....22..915A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016MMI....22..915A"><span>Interfacial <span class="hlt">layers</span> <span class="hlt">evolution</span> during annealing in Ti-Al multi-laminated composite processed using hot press and roll bonding</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Assari, A. H.; Eghbali, B.</p> <p>2016-09-01</p> <p>Ti-Al multi-laminated composites have great potential in high strength and low weight structures. In the present study, tri-<span class="hlt">layer</span> Ti-Al composite was synthesized by hot press bonding under 40 MPa at 570 °C for 1 h and subsequent hot roll bonding at about 450 °C. This process was conducted in two accumulative passes to 30% and to 67% thickness reduction in initial and final passes, respectively. Then, the final annealing treatments were done at 550, 600, 650, 700 and 750 °C for 2, 4 and 6 h. Investigations on microstructural <span class="hlt">evolution</span> and thickening of interfacial <span class="hlt">layers</span> were performed by scanning electron microscopes, energy dispersive spectrometer, X-ray diffraction and micro-hardness tests. The results showed that the thickening of diffusion <span class="hlt">layers</span> corresponds to amount of deformation. In addition to thickening of the diffusion <span class="hlt">layers</span>, the thickness of aluminum <span class="hlt">layers</span> decreased and after annealing treatment at 750 °C for 6 h the aluminum <span class="hlt">layers</span> were consumed entirely, which occurred because of the enhanced interdiffusion of Ti and Al elements. Scanning electron microscope equipped with energy dispersive spectrometer showed that the sequence of interfacial <span class="hlt">layers</span> as Ti3Al-TiAl-TiAl2-TiAl3 which are believed to be the result of thermodynamic and kinetic of phase formation. Micro-hardness results presented the variation profile in accordance with the sequence of intermetallic phases and their different structures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26ES..101a2011H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26ES..101a2011H"><span>Thin <span class="hlt">Layer</span> Drying <span class="hlt">Model</span> of Bacterial Cellulose Film</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hadi Jatmiko, Tri; Taufika Rosyida, Vita; Wheni Indrianingsih, Anastasia; Apriyana, Wuri</p> <p>2017-12-01</p> <p>The bacterial cellulose film produced by Acetobacter xylinum using coconut water as a carbon source was dried at a temperature of 60 to 100 C. The drying process of bacterial cellulose film occur at falling rate drying period. Increasing drying temperature will shorten the drying time. The drying data fitted with thin <span class="hlt">layer</span> drying <span class="hlt">models</span> that widely used, Newton, Page and Henderson and Pabis <span class="hlt">models</span>. All thin <span class="hlt">layer</span> drying <span class="hlt">models</span> describe the experimental data well, but Page <span class="hlt">model</span> is better than the other <span class="hlt">models</span> on all various temperature with coefficients of determination (R2) range from 0.9908 to 0.9979, chi square range from 0.000212 to 0.000851 and RMSE range from 0.014307 to 0.0289458.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT.......151M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT.......151M"><span>The dynamics of <span class="hlt">layered</span> and non-<span class="hlt">layered</span> oscillatory double-diffusive convection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moll, Ryan D.</p> <p></p> <p>Oscillatory double diffusive convection (ODDC) is a double diffusive instability that occurs in fluids that are unstably stratified in temperature and stably stratified in chemical composition. Regions unstable to ODDC are common in the interiors of stars and giant planets, and knowing thermal and compositional transport through these regions is important for stellar and planetary <span class="hlt">evolution</span> <span class="hlt">models</span>. Using 3D direct numerical simulations, Rosenblum et al. 2011 first showed that ODDC can either lead to the spontaneous formation of convective <span class="hlt">layers</span>, or remain in a state dominated by large scale gravity waves. Subsequent studies focused on identifying the conditions for <span class="hlt">layer</span> formation (Mirouh et al. 2012), and quantifying transport through <span class="hlt">layered</span> systems (Wood et al. 2013). This document includes 3 works that build on the results of these earlier studies. The subject of the first is transport through non-<span class="hlt">layered</span> ODDC and shows that in the absence of <span class="hlt">layered</span> convection, ODDC is dominated by large scale gravity waves that grow to the size of the domain. We find that while these gravity waves induce small amounts of turbulent mixing, turbulent transport through non-<span class="hlt">layered</span> systems is not significant for the purposes of astrophysical <span class="hlt">modeling</span> (unlike in <span class="hlt">layered</span> convection). The second study pertains to ODDC in the presence of Coriolis forces, and shows that rotating systems can be categorized depending on the strength of the rotation. We find that in the slowly rotating regime, the presence of rotation does not significantly affect qualitative behavior, but leads to modest reductions in thermal and compositional transport, while in the fast rotation regime qualitative behaviors are radically different, and systems are dominated by vortices that affect thermal and compositional transport in complex ways. In the final work we study simulations of ODDC at non-<span class="hlt">layered</span> parameters that are forced into a <span class="hlt">layered</span> configuration by initial conditions. Our results show that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..MARY48004Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..MARY48004Y"><span><span class="hlt">Layered</span> Chalcogenides beyond Graphene: from Electronic Structure <span class="hlt">Evolution</span> to the Spin Transport</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yuan, Hongtao</p> <p>2014-03-01</p> <p>Recent efforts on graphene-like atomic <span class="hlt">layer</span> materials, aiming at novel electronic properties and quantum phenomena beyond graphene, have attracted much attention for potential electronics/spintronics applications. Compared to the weak spin-orbit-interaction (SOI) in graphene, metal chalcogenides MX2 have heavy 4d/5d elements with strong atomic SOI, providing a unique way for generating spin polarization based on valleytronics physics. Indeed, such a spin-polarized band structure has been demonstrated theoretically and supported by optical investigations. However, despite these exciting progresses, following two important issues in MX2 community remain elusive: 1. the quantitative band structure of MX2 compounds (where are the valleys -band maxima/minima- locating in the BZ) have not been experimentally confirmed. Especially for those cleaved ultrathin mono- and bi-<span class="hlt">layer</span> flakes hosting most of recently-reported exotic phenomena at the 2D limit, the direct detection for band dispersion becomes of great importance for valleytronics. 2. Spin transports have seldom been reported even though such a strong SOI system can serve as an ideal platform for the spin polarization and spin transport. In this work, we started from the basic electronic structures of representative MX2, obtained by ARPES, and investigated both the band variation between these compounds and their band <span class="hlt">evolution</span> from bulk to the monolayer limit. After having a systematic understanding on band structures, we reported a giant Zeeman-type spin-polarization generated and modulated by an external electric field in WSe2 electric-double-<span class="hlt">layer</span> transistors. The non-magnetic approach for realizing such an intriguing spin splitting not only keeps the system time-reversally invariant but also suggests a new paradigm for manipulating the spin-degrees of freedom of electrons. Acknowledge the support from DoE, BES, Division of MSE under contract DE-AC02-76SF00515.</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/2018PhRvB..97p5410D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97p5410D"><span>Temperature-driven <span class="hlt">evolution</span> of critical points, interlayer coupling, and <span class="hlt">layer</span> polarization in bilayer Mo S2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Du, Luojun; Zhang, Tingting; Liao, Mengzhou; Liu, Guibin; Wang, Shuopei; He, Rui; Ye, Zhipeng; Yu, Hua; Yang, Rong; Shi, Dongxia; Yao, Yugui; Zhang, Guangyu</p> <p>2018-04-01</p> <p>The recently emerging two-dimensional (2D) transition-metal dichalcogenides (TMDCs) have been a fertile ground for exploring abundant exotic physical properties. Critical points, the extrema or saddle points of electronic bands, are the cornerstone of condensed-matter physics and fundamentally determine the optical and transport phenomena of the TMDCs. However, for bilayer Mo S2 , a typical TMDC and the unprecedented electrically tunable venue for valleytronics, there has been a considerable controversy on its intrinsic electronic structure, especially for the conduction band-edge locations. Moreover, interlayer hopping and <span class="hlt">layer</span> polarization in bilayer Mo S2 which play vital roles in valley-spintronic applications have remained experimentally elusive. Here, we report the experimental observation of intrinsic critical points locations, interlayer hopping, <span class="hlt">layer</span>-spin polarization, and their <span class="hlt">evolution</span> with temperature in bilayer Mo S2 by performing temperature-dependent photoluminescence. Our measurements confirm that the conduction-band minimum locates at the Kc instead of Qc, and the energy splitting between Qc and Kc redshifts with a descent of temperature. Furthermore, the interlayer hopping energy for holes and temperature-dependent <span class="hlt">layer</span> polarization are quantitatively determined. Our observations are in good harmony with density-functional theory calculations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22413017-charge-carrier-transport-model-donor-acceptor-blend-layers','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22413017-charge-carrier-transport-model-donor-acceptor-blend-layers"><span>A charge carrier transport <span class="hlt">model</span> for donor-acceptor blend <span class="hlt">layers</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>Fischer, Janine, E-mail: janine.fischer@iapp.de; Widmer, Johannes; Koerner, Christian</p> <p>2015-01-28</p> <p>Highly efficient organic solar cells typically comprise donor-acceptor blend <span class="hlt">layers</span> facilitating effective splitting of excitons. However, the charge carrier mobility in the blends can be substantially smaller than in neat materials, hampering the device performance. Currently, available mobility <span class="hlt">models</span> do not describe the transport in blend <span class="hlt">layers</span> entirely. Here, we investigate hole transport in a <span class="hlt">model</span> blend system consisting of the small molecule donor zinc phthalocyanine (ZnPc) and the acceptor fullerene C{sub 60} in different mixing ratios. The blend <span class="hlt">layer</span> is sandwiched between p-doped organic injection <span class="hlt">layers</span>, which prevent minority charge carrier injection and enable exploiting diffusion currents for themore » characterization of exponential tail states from a thickness variation of the blend <span class="hlt">layer</span> using numerical drift-diffusion simulations. Trap-assisted recombination must be considered to correctly <span class="hlt">model</span> the conductivity behavior of the devices, which are influenced by local electron currents in the active <span class="hlt">layer</span>, even though the active <span class="hlt">layer</span> is sandwiched in between p-doped contacts. We find that the density of deep tail states is largest in the devices with 1:1 mixing ratio (E{sub t} = 0.14 eV, N{sub t} = 1.2 × 10{sup 18 }cm{sup −3}) directing towards lattice disorder as the transport limiting process. A combined field and charge carrier density dependent mobility <span class="hlt">model</span> are developed for this blend <span class="hlt">layer</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhyA..392.2240B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhyA..392.2240B"><span>A last updating <span class="hlt">evolution</span> <span class="hlt">model</span> for online social networks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bu, Zhan; Xia, Zhengyou; Wang, Jiandong; Zhang, Chengcui</p> <p>2013-05-01</p> <p>As information technology has advanced, people are turning to electronic media more frequently for communication, and social relationships are increasingly found on online channels. However, there is very limited knowledge about the actual <span class="hlt">evolution</span> of the online social networks. In this paper, we propose and study a novel <span class="hlt">evolution</span> network <span class="hlt">model</span> with the new concept of “last updating time”, which exists in many real-life online social networks. The last updating <span class="hlt">evolution</span> network <span class="hlt">model</span> can maintain the robustness of scale-free networks and can improve the network reliance against intentional attacks. What is more, we also found that it has the “small-world effect”, which is the inherent property of most social networks. Simulation experiment based on this <span class="hlt">model</span> show that the results and the real-life data are consistent, which means that our <span class="hlt">model</span> is valid.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5400296','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5400296"><span>Clustering network <span class="hlt">layers</span> with the strata multilayer stochastic block <span class="hlt">model</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>Stanley, Natalie; Shai, Saray; Taylor, Dane; Mucha, Peter J.</p> <p>2016-01-01</p> <p>Multilayer networks are a useful data structure for simultaneously capturing multiple types of relationships between a set of nodes. In such networks, each relational definition gives rise to a <span class="hlt">layer</span>. While each <span class="hlt">layer</span> provides its own set of information, community structure across <span class="hlt">layers</span> can be collectively utilized to discover and quantify underlying relational patterns between nodes. To concisely extract information from a multilayer network, we propose to identify and combine sets of <span class="hlt">layers</span> with meaningful similarities in community structure. In this paper, we describe the “strata multilayer stochastic block model” (sMLSBM), a probabilistic <span class="hlt">model</span> for multilayer community structure. The central extension of the <span class="hlt">model</span> is that there exist groups of <span class="hlt">layers</span>, called “strata”, which are defined such that all <span class="hlt">layers</span> in a given stratum have community structure described by a common stochastic block <span class="hlt">model</span> (SBM). That is, <span class="hlt">layers</span> in a stratum exhibit similar node-to-community assignments and SBM probability parameters. Fitting the sMLSBM to a multilayer network provides a joint clustering that yields node-to-community and <span class="hlt">layer</span>-to-stratum assignments, which cooperatively aid one another during inference. We describe an algorithm for separating <span class="hlt">layers</span> into their appropriate strata and an inference technique for estimating the SBM parameters for each stratum. We demonstrate our method using synthetic networks and a multilayer network inferred from data collected in the Human Microbiome Project. PMID:28435844</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009ApJ...695..552B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009ApJ...695..552B"><span>Photoionized Mixing <span class="hlt">Layer</span> <span class="hlt">Models</span> of the Diffuse Ionized Gas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Binette, Luc; Flores-Fajardo, Nahiely; Raga, Alejandro C.; Drissen, Laurent; Morisset, Christophe</p> <p>2009-04-01</p> <p>It is generally believed that O stars, confined near the galactic midplane, are somehow able to photoionize a significant fraction of what is termed the "diffuse ionized gas" (DIG) of spiral galaxies, which can extend up to 1-2 kpc above the galactic midplane. The heating of the DIG remains poorly understood, however, as simple photoionization <span class="hlt">models</span> do not reproduce the observed line ratio correlations well or the DIG temperature. We present turbulent mixing <span class="hlt">layer</span> (TML) <span class="hlt">models</span> in which warm photoionized condensations are immersed in a hot supersonic wind. Turbulent dissipation and mixing generate an intermediate region where the gas is accelerated, heated, and mixed. The emission spectrum of such <span class="hlt">layers</span> is compared with observations of Rand of the DIG in the edge-on spiral NGC 891. We generate two sequence of <span class="hlt">models</span> that fit the line ratio correlations between [S II]/Hα, [O I]/Hα, [N II]/[S II], and [O III]/Hβ reasonably well. In one sequence of <span class="hlt">models</span>, the hot wind velocity increases, while in the other, the ionization parameter and <span class="hlt">layer</span> opacity increase. Despite the success of the mixing <span class="hlt">layer</span> <span class="hlt">models</span>, the overall efficiency in reprocessing the stellar UV is much too low, much less than 1%, which compels us to reject the TML <span class="hlt">model</span> in its present form.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20010062307&hterms=mathematicians&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmathematicians','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20010062307&hterms=mathematicians&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dmathematicians"><span>Dynamics in <span class="hlt">Layer</span> <span class="hlt">Models</span> of Solid Flame Propagation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Aldushin, A. P.; Bayliss, A.; Matkowsky, B. J.; Gokoglu, S. (Technical Monitor)</p> <p>2000-01-01</p> <p>Self-propagating high-temperature synthesis (SHS) is a process in which combustion waves, e.g., "solid flames", which are considered here, are employed to synthesize desired materials. Like many other systems, SHS is a pattern forming system. The problem of describing experimentally observed patterns and of predicting new, as yet unobserved, patterns continues to attract the attention of scientists and mathematicians due to the fundamental significance of the phenomena in combustion in particular, and in nonlinear science in general. Here, we analyze the dynamics of solid flame propagation in a 2D region by considering the region to be composed of parallel, identical <span class="hlt">layers</span> aligned along the direction of propagation and having thermal contact. Each <span class="hlt">layer</span> is then described by wave propagation in 1D, with the transverse Laplacian replaced by a term describing heat exchange between neighboring <span class="hlt">layers</span>. This configuration is the simplest <span class="hlt">model</span> of a 2D system because it accounts, in a simple way, for the principal feature of the problem, i.e., heat exchange between neighbors in the transverse direction. For simplicity, we describe the situation for two <span class="hlt">layers</span>. Because the <span class="hlt">layers</span> are identical, uniformly propagating waves in each <span class="hlt">layer</span> must be identical, independent of the heat exchange rate alpha. When the Zeldovich number Z exceeds a critical value Z(sub c), which depends on alpha, uniformly propagating waves become unstable. The stability diagram for the two coupled <span class="hlt">layers</span> reproduces that for the full 2D problem after appropriate identification of parameters in the two problems. Depending on parameter values, we determine three different steady-state dynamical behaviors (though additional behaviors are also expected to occur). The three behaviors are: (i) waves in each <span class="hlt">layer</span> which pulsate in phase as they propagate, so that together they form a single pulsating propagating wave; (ii) the waves in each <span class="hlt">layer</span> are no longer identical, and antiphase pulsations occur, with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050139715','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050139715"><span>Lidar Applications in Atmospheric Dynamics: Measurements of Wind, Moisture and Boundary <span class="hlt">Layer</span> <span class="hlt">Evolution</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Demoz, Belay; Whiteman, David; Gentry, Bruce; Schwemmer, Geary; Evans, Keith; DiGirolamo, Paolo; Comer, Joseph</p> <p>2005-01-01</p> <p>A large array of state-of-the-art ground-based and airborne remote and in-situ sensors were deployed during the International H2O Project (THOP), a field experiment that took place over the Southern Great Plains (SGP) of the United States from 13 May to 30 June 2002. These instruments provided extensive measurements of water vapor mixing ratio in order to better understand the influence of its variability on convection and on the skill of quantitative precipitation prediction (Weckwerth et all, 2004). Among the instrument deployed were ground based lidars from NASA/GSFC that included the Scanning Raman Lidar (SRL), the Goddard Laboratory for Observing Winds (GLOW), and the Holographic Airborne Rotating Lidar Instrument Experiment (HARLIE). A brief description of the three lidars is given below. This study presents ground-based measurements of wind, boundary <span class="hlt">layer</span> structure and water vapor mixing ratio measurements observed by three co-located lidars during MOP at the MOP ground profiling site in the Oklahoma Panhandle (hereafter referred as Homestead). This presentation will focus on the <span class="hlt">evolution</span> and variability of moisture and wind in the boundary <span class="hlt">layer</span> when frontal and/or convergence boundaries (e.g. bores, dry lines, thunderstorm outflows etc) were observed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018LPICo2084.4024T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018LPICo2084.4024T"><span>A Mudball <span class="hlt">Model</span> for the <span class="hlt">Evolution</span> of Carbonaceous Asteroids</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Travis, B. J.; Bland, P. A.</p> <p>2018-05-01</p> <p>We simulation the <span class="hlt">evolution</span> of carbonaceous chondrite parent bodies from initially unconsolidated aggregations of rock grains and ice crystals. Application of the numerical <span class="hlt">model</span> MAGHNUM to <span class="hlt">evolution</span> of CM type planetesimals and Ceres is described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20170001424','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20170001424"><span>Approach to <span class="hlt">Modeling</span> Boundary <span class="hlt">Layer</span> Ingestion Using a Fully Coupled Propulsion-RANS <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gray, Justin S.; Mader, Charles A.; Kenway, Gaetan K. W.; Martins, Joaquim R. R. A.</p> <p>2017-01-01</p> <p>Airframe-propulsion integration concepts that use boundary <span class="hlt">layer</span> ingestion have the potential to reduce aircraft fuel burn. One concept that has been recently explored is NASA's Starc-ABL aircraft configuration, which offers the potential for 12% mission fuel burn reduction by using a turbo-electric propulsion system with an aft-mounted electrically driven boundary <span class="hlt">layer</span> ingestion propulsor. This large potential for improved performance motivates a more detailed study of the boundary <span class="hlt">layer</span> ingestion propulsor design, but to date, analyses of boundary <span class="hlt">layer</span> ingestion have used uncoupled methods. These methods account for only aerodynamic effects on the propulsion system or propulsion system effects on the aerodynamics, but not both simultaneously. This work presents a new approach for building fully coupled propulsive-aerodynamic <span class="hlt">models</span> of boundary <span class="hlt">layer</span> ingestion propulsion systems. A 1D thermodynamic cycle analysis is coupled to a RANS simulation to <span class="hlt">model</span> the Starc-ABL aft propulsor at a cruise condition and the effects variation in propulsor design on performance are examined. The results indicates that both propulsion and aerodynamic effects contribute equally toward the overall performance and that the fully coupled <span class="hlt">model</span> yields substantially different results compared to uncoupled. The most significant finding is that boundary <span class="hlt">layer</span> ingestion, while offering substantial fuel burn savings, introduces throttle dependent aerodynamics effects that need to be accounted for. This work represents a first step toward the multidisciplinary design optimization of boundary <span class="hlt">layer</span> ingestion propulsion systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24889376','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24889376"><span>Neutral null <span class="hlt">models</span> for diversity in serial transfer <span class="hlt">evolution</span> experiments.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Harpak, Arbel; Sella, Guy</p> <p>2014-09-01</p> <p><span class="hlt">Evolution</span> experiments with microorganisms coupled with genome-wide sequencing now allow for the systematic study of population genetic processes under a wide range of conditions. In learning about these processes in natural, sexual populations, neutral <span class="hlt">models</span> that describe the behavior of diversity and divergence summaries have played a pivotal role. It is therefore natural to ask whether neutral <span class="hlt">models</span>, suitably modified, could be useful in the context of <span class="hlt">evolution</span> experiments. Here, we introduce coalescent <span class="hlt">models</span> for polymorphism and divergence under the most common experimental <span class="hlt">evolution</span> assay, a serial transfer experiment. This relatively simple setting allows us to address several issues that could affect diversity patterns in <span class="hlt">evolution</span> experiments, whether selection is operating or not: the transient behavior of neutral polymorphism in an experiment beginning from a single clone, the effects of randomness in the timing of cell division and noisiness in population size in the dilution stage. In our analyses and discussion, we emphasize the implications for experiments aimed at measuring diversity patterns and making inferences about population genetic processes based on these measurements. © 2014 The Author(s). <span class="hlt">Evolution</span> © 2014 The Society for the Study of <span class="hlt">Evolution</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017A%26A...608A..62H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017A%26A...608A..62H"><span>Testing stellar <span class="hlt">evolution</span> <span class="hlt">models</span> with detached eclipsing binaries</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Higl, J.; Weiss, A.</p> <p>2017-12-01</p> <p>Stellar <span class="hlt">evolution</span> codes, as all other numerical tools, need to be verified. One of the standard stellar objects that allow stringent tests of stellar <span class="hlt">evolution</span> theory and <span class="hlt">models</span>, are detached eclipsing binaries. We have used 19 such objects to test our stellar <span class="hlt">evolution</span> code, in order to see whether standard methods and assumptions suffice to reproduce the observed global properties. In this paper we concentrate on three effects that contain a specific uncertainty: atomic diffusion as used for standard solar <span class="hlt">model</span> calculations, overshooting from convective regions, and a simple <span class="hlt">model</span> for the effect of stellar spots on stellar radius, which is one of the possible solutions for the radius problem of M dwarfs. We find that in general old systems need diffusion to allow for, or at least improve, an acceptable fit, and that systems with convective cores indeed need overshooting. Only one system (AI Phe) requires the absence of it for a successful fit. To match stellar radii for very low-mass stars, the spot <span class="hlt">model</span> proved to be an effective approach, but depending on <span class="hlt">model</span> details, requires a high percentage of the surface being covered by spots. We briefly discuss improvements needed to further reduce the freedom in <span class="hlt">modelling</span> and to allow an even more restrictive test by using these objects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.H34D..02M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.H34D..02M"><span>Adaptive Multiscale <span class="hlt">Modeling</span> of Geochemical Impacts on Fracture <span class="hlt">Evolution</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Molins, S.; Trebotich, D.; Steefel, C. I.; Deng, H.</p> <p>2016-12-01</p> <p>Understanding fracture <span class="hlt">evolution</span> is essential for many subsurface energy applications, including subsurface storage, shale gas production, fracking, CO2 sequestration, and geothermal energy extraction. Geochemical processes in particular play a significant role in the <span class="hlt">evolution</span> of fractures through dissolution-driven widening, fines migration, and/or fracture sealing due to precipitation. One obstacle to understanding and exploiting geochemical fracture <span class="hlt">evolution</span> is that it is a multiscale process. However, current geochemical <span class="hlt">modeling</span> of fractures cannot capture this multi-scale nature of geochemical and mechanical impacts on fracture <span class="hlt">evolution</span>, and is limited to either a continuum or pore-scale representation. Conventional continuum-scale <span class="hlt">models</span> treat fractures as preferential flow paths, with their permeability evolving as a function (often, a cubic law) of the fracture aperture. This approach has the limitation that it oversimplifies flow within the fracture in its omission of pore scale effects while also assuming well-mixed conditions. More recently, pore-scale <span class="hlt">models</span> along with advanced characterization techniques have allowed for accurate simulations of flow and reactive transport within the pore space (Molins et al., 2014, 2015). However, these <span class="hlt">models</span>, even with high performance computing, are currently limited in their ability to treat tractable domain sizes (Steefel et al., 2013). Thus, there is a critical need to develop an adaptive <span class="hlt">modeling</span> capability that can account for separate properties and processes, emergent and otherwise, in the fracture and the rock matrix at different spatial scales. Here we present an adaptive <span class="hlt">modeling</span> capability that treats geochemical impacts on fracture <span class="hlt">evolution</span> within a single multiscale framework. <span class="hlt">Model</span> development makes use of the high performance simulation capability, Chombo-Crunch, leveraged by high resolution characterization and experiments. The <span class="hlt">modeling</span> framework is based on the adaptive capability in Chombo</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=almonds&pg=3&id=EJ278600','ERIC'); return false;" href="https://eric.ed.gov/?q=almonds&pg=3&id=EJ278600"><span>The Creation-<span class="hlt">Evolution</span> Debate as a <span class="hlt">Model</span> of Issue Polarization.</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>Wielert, Jan S.</p> <p>1983-01-01</p> <p>The Almond <span class="hlt">model</span> of public opinion can be modified to produce an issue-polarization <span class="hlt">model</span> of the creation-<span class="hlt">evolution</span> debate. Suggests that the nonattentive public may hold more potential for expanding the ranks of pro-<span class="hlt">evolution</span> attentives than for expanding the ranks of those favoring creationism. (JN)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2987822','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2987822"><span><span class="hlt">Modelling</span> the <span class="hlt">Evolution</span> and Spread of HIV Immune Escape Mutants</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Fryer, Helen R.; Frater, John; Duda, Anna; Roberts, Mick G.; Phillips, Rodney E.; McLean, Angela R.</p> <p>2010-01-01</p> <p>During infection with human immunodeficiency virus (HIV), immune pressure from cytotoxic T-lymphocytes (CTLs) selects for viral mutants that confer escape from CTL recognition. These escape variants can be transmitted between individuals where, depending upon their cost to viral fitness and the CTL responses made by the recipient, they may revert. The rates of within-host <span class="hlt">evolution</span> and their concordant impact upon the rate of spread of escape mutants at the population level are uncertain. Here we present a mathematical <span class="hlt">model</span> of within-host <span class="hlt">evolution</span> of escape mutants, transmission of these variants between hosts and subsequent reversion in new hosts. The <span class="hlt">model</span> is an extension of the well-known SI <span class="hlt">model</span> of disease transmission and includes three further parameters that describe host immunogenetic heterogeneity and rates of within host viral <span class="hlt">evolution</span>. We use the <span class="hlt">model</span> to explain why some escape mutants appear to have stable prevalence whilst others are spreading through the population. Further, we use it to compare diverse datasets on CTL escape, highlighting where different sources agree or disagree on within-host evolutionary rates. The several dozen CTL epitopes we survey from HIV-1 gag, RT and nef reveal a relatively sedate rate of <span class="hlt">evolution</span> with average rates of escape measured in years and reversion in decades. For many epitopes in HIV, occasional rapid within-host <span class="hlt">evolution</span> is not reflected in fast <span class="hlt">evolution</span> at the population level. PMID:21124991</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MPLB...3150283Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MPLB...3150283Z"><span>A phase field crystal <span class="hlt">model</span> simulation of morphology <span class="hlt">evolution</span> and misfit dislocation generation in nanoheteroepitaxy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, J.; Chen, Z.; Cheng, C.; Wang, Y. X.</p> <p>2017-10-01</p> <p>A phase field crystal (PFC) <span class="hlt">model</span> is employed to study morphology <span class="hlt">evolution</span> of nanoheteroepitaxy and misfit dislocation generation when applied with enhanced supercooling, lattice mismatch and substrate vicinal angle conditions. Misfit strain that rises due to lattice mismatch causes rough surfaces or misfit dislocations, deteriorates film properties, hence, efforts taken to reveal their microscopic mechanism are significant for film quality improvement. Uniform islands, instead of misfit dislocations, are developed in subcritical thickness film, serving as a way of strain relief by surface mechanism. Misfit dislocations generate when strain relief by surface mechanism is deficient in higher supercooling, multilayers of misfit dislocations dominate, but the number of <span class="hlt">layers</span> reduces gradually when the supercooling is further enhanced. Rough surfaces like islands or cuspate pits are developed which is ascribed to lattice mismatch, multilayers of misfit dislocations generate to further enhance lattice mismatch. <span class="hlt">Layers</span> of misfit dislocations generate at a thickening position at enhanced substrate vicinal angle, this further enhancing the angle leading to sporadic generation of misfit dislocations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013BoLMe.148..585O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013BoLMe.148..585O"><span>Amendment to "Analytical Solution for the Convectively-Mixed Atmospheric Boundary <span class="hlt">Layer</span>": Inclusion of Subsidence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ouwersloot, H. G.; de Arellano, J. Vilà-Guerau</p> <p>2013-09-01</p> <p>In Ouwersloot and Vilà-Guerau de Arellano (Boundary-<span class="hlt">Layer</span> Meteorol. doi:<ExternalRef> <RefSource>10.1007/s10546-013-9816-z</RefSource> <RefTarget Address="10.1007/s10546-013-9816-z" TargetType="DOI"/> </ExternalRef>, <CitationRef CitationID="CR2">2013</CitationRef>, this issue), the analytical solutions for the boundary-<span class="hlt">layer</span> height and scalar <span class="hlt">evolutions</span> are derived for the convective boundary <span class="hlt">layer</span>, based on the prognostic equations of mixed-<span class="hlt">layer</span> slab <span class="hlt">models</span> without taking subsidence into account. Here, we include and quantify the added effect of subsidence if the subsidence velocity scales linearly with height throughout the atmosphere. This enables analytical analyses for a wider range of observational cases. As a demonstration, the sensitivity of the boundary-<span class="hlt">layer</span> height and the potential temperature jump to subsidence and the free tropospheric stability is graphically presented. The new relations show the importance of the temporal distribution of the surface buoyancy flux in determining the <span class="hlt">evolution</span> if there is subsidence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMEP33D..01W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMEP33D..01W"><span>A Physically Based Coupled Chemical and Physical Weathering <span class="hlt">Model</span> for Simulating Soilscape <span class="hlt">Evolution</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Willgoose, G. R.; Welivitiya, D.; Hancock, G. R.</p> <p>2015-12-01</p> <p>A critical missing link in existing landscape <span class="hlt">evolution</span> <span class="hlt">models</span> is a dynamic soil <span class="hlt">evolution</span> <span class="hlt">models</span> where soils co-evolve with the landform. Work by the authors over the last decade has demonstrated a computationally manageable <span class="hlt">model</span> for soil profile <span class="hlt">evolution</span> (soilscape <span class="hlt">evolution</span>) based on physical weathering. For chemical weathering it is clear that full geochemistry <span class="hlt">models</span> such as CrunchFlow and PHREEQC are too computationally intensive to be couplable to existing soilscape and landscape <span class="hlt">evolution</span> <span class="hlt">models</span>. This paper presents a simplification of CrunchFlow chemistry and physics that makes the task feasible, and generalises it for hillslope geomorphology applications. Results from this simplified <span class="hlt">model</span> will be compared with field data for soil pedogenesis. Other researchers have previously proposed a number of very simple weathering functions (e.g. exponential, humped, reverse exponential) as conceptual <span class="hlt">models</span> of the in-profile weathering process. The paper will show that all of these functions are possible for specific combinations of in-soil environmental, geochemical and geologic conditions, and the presentation will outline the key variables controlling which of these conceptual <span class="hlt">models</span> can be realistic <span class="hlt">models</span> of in-profile processes and under what conditions. The presentation will finish by discussing the coupling of this <span class="hlt">model</span> with a physical weathering <span class="hlt">model</span>, and will show sample results from our SSSPAM soilscape <span class="hlt">evolution</span> <span class="hlt">model</span> to illustrate the implications of including chemical weathering in the soilscape <span class="hlt">evolution</span> <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013APS..DPPBI3005D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013APS..DPPBI3005D"><span>Observation and <span class="hlt">modeling</span> of mixing-<span class="hlt">layer</span> development in HED blast-wave-driven shear flow</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>di Stefano, Carlos</p> <p>2013-10-01</p> <p>This talk describes work exploring the sensitivity to initial conditions of hydrodynamic mixing-<span class="hlt">layer</span> growth due to shear flow in the high-energy-density regime. This work features an approach in two parts, experimental and theoretical. First, an experiment, conducted at the OMEGA-60 laser facility, seeks to measure the development of such a mixing <span class="hlt">layer</span>. This is accomplished by placing a <span class="hlt">layer</span> of low-density (initially of either 0.05 or 0.1 g/cm3, to vary the system's Atwood number) carbon foam against a <span class="hlt">layer</span> of higher-density (initially 1.4 g/cm3) polyamide-imide that has been machined to a nominally-flat surface at its interface with the foam. Inherent roughness of this surface's finish is precisely measured and varied from piece to piece. Ten simultaneous OMEGA beams, comprising a 4.5 kJ, 1-ns pulse focused to a roughly 1-mm-diameter spot, irradiate a thin polycarbonate ablator, driving a blast wave into the foam, parallel to its interface with the polyamide-imide. The ablator is framed by a gold washer, such that the blast wave is driven only into the foam, and not into the polyamide-imide. The subsequent forward motion of the shocked foam creates the desired shear effect, and the system is imaged by X-ray radiography 35 ns after the beginning of the driving laser pulse. Second, a simulation is performed, intending to replicate the flow observed in the experiment as closely as possible. Using the resulting simulated flow parameters, an analytical <span class="hlt">model</span> can be used to predict the <span class="hlt">evolution</span> of the mixing <span class="hlt">layer</span>, as well as track the motion of the fluid in the experiment prior to the snapshot seen in the radiograph. The ability of the <span class="hlt">model</span> to predict growth of the mixing <span class="hlt">layer</span> under the various conditions observed in the experiment is then examined. This work is funded by the Predictive Sciences Academic Alliances Program in NNSA-ASC via grant DEFC52- 08NA28616, by the NNSA-DS and SC-OFES Joint Program in High-Energy-Density Laboratory Plasmas, grant number DE</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.7237C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.7237C"><span><span class="hlt">Modelling</span> landscape <span class="hlt">evolution</span> at the flume scale</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cheraghi, Mohsen; Rinaldo, Andrea; Sander, Graham C.; Barry, D. Andrew</p> <p>2017-04-01</p> <p>The ability of a large-scale Landscape <span class="hlt">Evolution</span> <span class="hlt">Model</span> (LEM) to simulate the soil surface morphological <span class="hlt">evolution</span> as observed in a laboratory flume (1-m × 2-m surface area) was investigated. The soil surface was initially smooth, and was subjected to heterogeneous rainfall in an experiment designed to avoid rill formation. Low-cohesive fine sand was placed in the flume while the slope and relief height were 5 % and 20 cm, respectively. Non-uniform rainfall with an average intensity of 85 mm h-1 and a standard deviation of 26 % was applied to the sediment surface for 16 h. We hypothesized that the complex overland water flow can be represented by a drainage discharge network, which was calculated via the micro-morphology and the rainfall distribution. Measurements included high resolution Digital Elevation <span class="hlt">Models</span> that were captured at intervals during the experiment. The calibrated LEM captured the migration of the main flow path from the low precipitation area into the high precipitation area. Furthermore, both <span class="hlt">model</span> and experiment showed a steep transition zone in soil elevation that moved upstream during the experiment. We conclude that the LEM is applicable under non-uniform rainfall and in the absence of surface incisions, thereby extending its applicability beyond that shown in previous applications. Keywords: Numerical simulation, Flume experiment, Particle Swarm Optimization, Sediment transport, River network <span class="hlt">evolution</span> <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMOS44A..02R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMOS44A..02R"><span>Using Remotely Piloted Aircraft System to Study the <span class="hlt">Evolution</span> of the Boundary <span class="hlt">Layer</span> Related to Fog Events</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Roberts, G. C.; Cayez, G.; Ronflé-Nadaud, C.; Albrand, M.; Dralet, J. P.; Momboisse, G.; Nicoll, K.; Seity, Y.; Bronz, M.; Hattenberger, G.; Gorraz, M.; Bustico, A.</p> <p>2014-12-01</p> <p>Over the past decade, the scientific community has embraced the use of RPAS (remotely piloted aircraft system) as a tool to improve observations of the Earth's surface and atmospheric phenomena. The use of small RPAS (Remotely Piloted Aircraft System) in atmospheric research has increased because of their relative low-cost, compact size and ease of operation. Small RPAS are especially adapted for observing the atmospheric boundary <span class="hlt">layer</span> processes at high vertical and temporal resolution. To this end, CNRM, ENAC, and ENM have developed the VOLTIGE (Vecteurs d'Observation de La Troposphere pour l'Investigation et la Gestion de l'Environnement) program to study the life cycle of fog with multiple, small RPAS. The instrumented RPAS flights have successfully observed the <span class="hlt">evolution</span> of the boundary <span class="hlt">layer</span> and dissipation of fog events. In addition, vertical profiles from the RPAS have been compared with Météo France forecast <span class="hlt">models</span>, and the results suggest that forecast <span class="hlt">models</span> may be improved using high resolution and frequent in-situ measurements. Within the VOLTIGE project, a flying-wing RPAS with four control surfaces was developed to separate elevator and aileron controls in order to reduce the pitch angle envelope and improve turbulence and albedo measurements. The result leads to a small RPAS with the capability of flying up to two hours with 150 grams of payload, while keeping the hand-launch capability as a constraint for regular atmospheric research missions. High frequency data logging has been integrated into the main autopilot in order to synchronize navigation and payload measurements, as well as allowing an efficient sensor-based navigation. The VOLTIGE program also encourages direct participation of students on the advancement of novel observing systems for atmospheric sciences, and provides a step towards deploying small RPAS in an operational network. VOLTIGE is funded by the Agence Nationale de Recherche (ANR-Blanc 2012) and supported by Aerospace</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999ApJ...510..795S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999ApJ...510..795S"><span>Hierarchical <span class="hlt">Model</span> for the <span class="hlt">Evolution</span> of Cloud Complexes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sánchez D., Néstor M.; Parravano, Antonio</p> <p>1999-01-01</p> <p>The structure of cloud complexes appears to be well described by a tree structure (i.e., a simplified ``stick man'') representation when the image is partitioned into ``clouds.'' In this representation, the parent-child relationships are assigned according to containment. Based on this picture, a hierarchical <span class="hlt">model</span> for the <span class="hlt">evolution</span> of cloud complexes, including star formation, is constructed. The <span class="hlt">model</span> follows the mass <span class="hlt">evolution</span> of each substructure by computing its mass exchange with its parent and children. The parent-child mass exchange (evaporation or condensation) depends on the radiation density at the interphase. At the end of the ``lineage,'' stars may be born or die, so that there is a nonstationary mass flow in the hierarchical structure. For a variety of parameter sets the system follows the same series of steps to transform diffuse gas into stars, and the regulation of the mass flux in the tree by previously formed stars dominates the <span class="hlt">evolution</span> of the star formation. For the set of parameters used here as a reference <span class="hlt">model</span>, the system tends to produce initial mass functions (IMFs) that have a maximum at a mass that is too high (~2 Msolar) and the characteristic times for <span class="hlt">evolution</span> seem too long. We show that these undesired properties can be improved by adjusting the <span class="hlt">model</span> parameters. The <span class="hlt">model</span> requires further physics (e.g., allowing for multiple stellar systems and clump collisions) before a definitive comparison with observations can be made. Instead, the emphasis here is to illustrate some general properties of this kind of complex nonlinear <span class="hlt">model</span> for the star formation process. Notwithstanding the simplifications involved, the <span class="hlt">model</span> reveals an essential feature that will likely remain if additional physical processes are included, that is, the detailed behavior of the system is very sensitive to the variations on the initial and external conditions, suggesting that a ``universal'' IMF is very unlikely. When an ensemble of IMFs corresponding to a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ApSS..453..365Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ApSS..453..365Z"><span>In-depth <span class="hlt">evolution</span> of chemical states and sub-10-nm-resolution crystal orientation mapping of nanograins in Ti(5 nm)/Au(20 nm)/Cr(3 nm) tri-<span class="hlt">layer</span> thin films</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Xiaoli; Todeschini, Matteo; Bastos da Silva Fanta, Alice; Liu, Lintao; Jensen, Flemming; Hübner, Jörg; Jansen, Henri; Han, Anpan; Shi, Peixiong; Ming, Anjie; Xie, Changqing</p> <p>2018-09-01</p> <p>The applications of Au thin films and their adhesion <span class="hlt">layers</span> often suffer from a lack of sufficient information about the chemical states of adhesion <span class="hlt">layers</span> and about the high-lateral-resolution crystallographic morphology of Au nanograins. Here, we demonstrate the in-depth <span class="hlt">evolution</span> of the chemical states of adhesive <span class="hlt">layers</span> at the interfaces and the crystal orientation mapping of gold nanograins with a lateral resolution of less than 10 nm in a Ti/Au/Cr tri-<span class="hlt">layer</span> thin film system. Using transmission electron microscopy, the variation in the interdiffusion at Cr/Au and Ti/Au interfaces was confirmed. From X-ray photoelectron spectroscopy (XPS) depth profiling, the chemical states of Cr, Au and Ti were characterized <span class="hlt">layer</span> by <span class="hlt">layer</span>, suggesting the insufficient oxidation of the adhesive <span class="hlt">layers</span>. At the interfaces the Au 4f peaks shift to higher binding energies and this behavior can be described by a proposed <span class="hlt">model</span> based on electron reorganization and substrate-induced final-state neutralization in small Au clusters supported by the partially oxidized Ti <span class="hlt">layer</span>. Utilizing transmission Kikuchi diffraction (TKD) in a scanning electron microscope, the crystal orientation of Au nanograins between two adhesion <span class="hlt">layers</span> was non-destructively characterized with sub-10 nm spatial resolution. The results provide nanoscale insights into the Ti/Au/Cr thin film system and contribute to our understanding of its behavior in nano-optic and nano-electronic devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ResPh...9...86S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ResPh...9...86S"><span>A <span class="hlt">model</span> for capillary rise in micro-tube restrained by a sticky <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shen, Anqi; Xu, Yun; Liu, Yikun; Cai, Bo; Liang, Shuang; Wang, Fengjiao</p> <p>2018-06-01</p> <p>Fluid transport in a microscopic capillary under the effects of a sticky <span class="hlt">layer</span> was theoretically investigated. A <span class="hlt">model</span> based on the classical Lucas-Washburn (LW) <span class="hlt">model</span> is proposed for the meniscus rise with the sticky <span class="hlt">layer</span> present. The sticky <span class="hlt">layer</span> consists of two parts: a fixed (located at the wall) and a movable part (located on the inside of the capillary), affecting the micro-capillary flow in different ways. Within our <span class="hlt">model</span>, the movable <span class="hlt">layer</span> is defined by the capillary radius and pressure gradient. From the <span class="hlt">model</span> it follows that the fixed sticky <span class="hlt">layer</span> leads to a decrease of capillary radius, while the movable sticky <span class="hlt">layer</span> increases flow resistance. The movable <span class="hlt">layer</span> thickness varies with the pressure gradient, which in turn varies with the rising of the meniscus. The results of our theoretical calculation also prove that the capillary radius has a greater effect on the meniscus height, rather than the additional resistance caused by the movable <span class="hlt">layer</span>. Moreover, the fixed sticky <span class="hlt">layer</span>, which affects the capillary radius, has a greater influence than the movable sticky <span class="hlt">layer</span>. We conclude that the sticky <span class="hlt">layer</span> causes a lower imbibition height than the LW <span class="hlt">model</span> predicts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880029351&hterms=duct+propeller&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dduct%2Bpropeller','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880029351&hterms=duct+propeller&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dduct%2Bpropeller"><span>A <span class="hlt">model</span> of the wall boundary <span class="hlt">layer</span> for ducted propellers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Eversman, Walter; Moehring, Willi</p> <p>1987-01-01</p> <p>The objective of the present study is to include a representation of a wall boundary <span class="hlt">layer</span> in an existing finite element <span class="hlt">model</span> of the propeller in the wind tunnel environment. The major consideration is that the new formulation should introduce only modest alterations in the numerical <span class="hlt">model</span> and should still be capable of producing economical predictions of the radiated acoustic field. This is accomplished by using a stepped approximation in which the velocity profile is piecewise constant in <span class="hlt">layers</span>. In the limit of infinitesimally thin <span class="hlt">layers</span>, the velocity profile of the stepped approximation coincides with that of the continuous profile. The approach described here could also be useful in <span class="hlt">modeling</span> the boundary <span class="hlt">layer</span> in other duct applications, particularly in the computation of the radiated acoustic field for sources contained in a duct.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GMD....10.4577S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GMD....10.4577S"><span>The SPACE 1.0 <span class="hlt">model</span>: a Landlab component for 2-D calculation of sediment transport, bedrock erosion, and landscape <span class="hlt">evolution</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shobe, Charles M.; Tucker, Gregory E.; Barnhart, Katherine R.</p> <p>2017-12-01</p> <p><span class="hlt">Models</span> of landscape <span class="hlt">evolution</span> by river erosion are often either transport-limited (sediment is always available but may or may not be transportable) or detachment-limited (sediment must be detached from the bed but is then always transportable). While several <span class="hlt">models</span> incorporate elements of, or transition between, transport-limited and detachment-limited behavior, most require that either sediment or bedrock, but not both, are eroded at any given time. <span class="hlt">Modeling</span> landscape <span class="hlt">evolution</span> over large spatial and temporal scales requires a <span class="hlt">model</span> that can (1) transition freely between transport-limited and detachment-limited behavior, (2) simultaneously treat sediment transport and bedrock erosion, and (3) run in 2-D over large grids and be coupled with other surface process <span class="hlt">models</span>. We present SPACE (stream power with alluvium conservation and entrainment) 1.0, a new <span class="hlt">model</span> for simultaneous <span class="hlt">evolution</span> of an alluvium <span class="hlt">layer</span> and a bedrock bed based on conservation of sediment mass both on the bed and in the water column. The <span class="hlt">model</span> treats sediment transport and bedrock erosion simultaneously, embracing the reality that many rivers (even those commonly defined as <q>bedrock</q> rivers) flow over a partially alluviated bed. SPACE improves on previous <span class="hlt">models</span> of bedrock-alluvial rivers by explicitly calculating sediment erosion and deposition rather than relying on a flux-divergence (Exner) approach. The SPACE <span class="hlt">model</span> is a component of the Landlab <span class="hlt">modeling</span> toolkit, a Python-language library used to create <span class="hlt">models</span> of Earth surface processes. Landlab allows efficient coupling between the SPACE <span class="hlt">model</span> and components simulating basin hydrology, hillslope <span class="hlt">evolution</span>, weathering, lithospheric flexure, and other surface processes. Here, we first derive the governing equations of the SPACE <span class="hlt">model</span> from existing sediment transport and bedrock erosion formulations and explore the behavior of local analytical solutions for sediment flux and alluvium thickness. We derive steady-state analytical solutions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhFl...29c6601R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhFl...29c6601R"><span>Geostrophic tripolar vortices in a two-<span class="hlt">layer</span> fluid: Linear stability and nonlinear <span class="hlt">evolution</span> of equilibria</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Reinaud, J. N.; Sokolovskiy, M. A.; Carton, X.</p> <p>2017-03-01</p> <p>We investigate equilibrium solutions for tripolar vortices in a two-<span class="hlt">layer</span> quasi-geostrophic flow. Two of the vortices are like-signed and lie in one <span class="hlt">layer</span>. An opposite-signed vortex lies in the other <span class="hlt">layer</span>. The families of equilibria can be spanned by the distance (called separation) between the two like-signed vortices. Two equilibrium configurations are possible when the opposite-signed vortex lies between the two other vortices. In the first configuration (called ordinary roundabout), the opposite signed vortex is equidistant to the two other vortices. In the second configuration (eccentric roundabouts), the distances are unequal. We determine the equilibria numerically and describe their characteristics for various internal deformation radii. The two branches of equilibria can co-exist and intersect for small deformation radii. Then, the eccentric roundabouts are stable while unstable ordinary roundabouts can be found. Indeed, ordinary roundabouts exist at smaller separations than eccentric roundabouts do, thus inducing stronger vortex interactions. However, for larger deformation radii, eccentric roundabouts can also be unstable. Then, the two branches of equilibria do not cross. The branch of eccentric roundabouts only exists for large separations. Near the end of the branch of eccentric roundabouts (at the smallest separation), one of the like-signed vortices exhibits a sharp inner corner where instabilities can be triggered. Finally, we investigate the nonlinear <span class="hlt">evolution</span> of a few selected cases of tripoles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014NPGD....1.1657G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014NPGD....1.1657G"><span>The double <span class="hlt">layers</span> in the plasma sheet boundary <span class="hlt">layer</span> during magnetic reconnection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, J.; Yu, B.</p> <p>2014-11-01</p> <p>We studied the <span class="hlt">evolutions</span> of double <span class="hlt">layers</span> which appear after the magnetic reconnection through two-dimensional electromagnetic particle-in-cell simulation. The simulation results show that the double <span class="hlt">layers</span> are formed in the plasma sheet boundary <span class="hlt">layer</span> after magnetic reconnection. At first, the double <span class="hlt">layers</span> which have unipolar structures are formed. And then the double <span class="hlt">layers</span> turn into bipolar structures, which will couple with another new weak bipolar structure. Thus a new double <span class="hlt">layer</span> or tripolar structure comes into being. The double <span class="hlt">layers</span> found in our work are about several ten Debye lengths, which accords with the observation results. It is suggested that the electron beam formed during the magnetic reconnection is responsible for the production of the double <span class="hlt">layers</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SpWea..13..339Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SpWea..13..339Y"><span><span class="hlt">Modeling</span> Chinese ionospheric <span class="hlt">layer</span> parameters based on EOF analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, You; Wan, Weixing; Xiong, Bo; Ren, Zhipeng; Zhao, Biqiang; Zhang, Yun; Ning, Baiqi; Liu, Libo</p> <p>2015-05-01</p> <p>Using 24-ionosonde observations in and around China during the 20th solar cycle, an assimilative <span class="hlt">model</span> is constructed to map the ionospheric <span class="hlt">layer</span> parameters (foF2, hmF2, M(3000)F2, and foE) over China based on empirical orthogonal function (EOF) analysis. First, we decompose the background maps from the International Reference Ionosphere <span class="hlt">model</span> 2007 (IRI-07) into different EOF modes. The obtained EOF modes consist of two factors: the EOF patterns and the corresponding EOF amplitudes. These two factors individually reflect the spatial distributions (e.g., the latitudinal dependence such as the equatorial ionization anomaly structure and the longitude structure with east-west difference) and temporal variations on different time scales (e.g., solar cycle, annual, semiannual, and diurnal variations) of the <span class="hlt">layer</span> parameters. Then, the EOF patterns and long-term observations of ionosondes are assimilated to get the observed EOF amplitudes, which are further used to construct the Chinese Ionospheric Maps (CIMs) of the <span class="hlt">layer</span> parameters. In contrast with the IRI-07 <span class="hlt">model</span>, the mapped CIMs successfully capture the inherent temporal and spatial variations of the ionospheric <span class="hlt">layer</span> parameters. Finally, comparison of the <span class="hlt">modeled</span> (EOF and IRI-07 <span class="hlt">model</span>) and observed values reveals that the EOF <span class="hlt">model</span> reproduces the observation with smaller root-mean-square errors and higher linear correlation coefficients. In addition, IRI discrepancy at the low latitude especially for foF2 is effectively removed by EOF <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.3887Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.3887Y"><span><span class="hlt">Modeling</span> Chinese ionospheric <span class="hlt">layer</span> parameters based on EOF analysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, You; Wan, Weixing</p> <p>2016-04-01</p> <p>Using 24-ionosonde observations in and around China during the 20th solar cycle, an assimilative <span class="hlt">model</span> is constructed to map the ionospheric <span class="hlt">layer</span> parameters (foF2, hmF2, M(3000)F2, and foE) over China based on empirical orthogonal function (EOF) analysis. First, we decompose the background maps from the International Reference Ionosphere <span class="hlt">model</span> 2007 (IRI-07) into different EOF modes. The obtained EOF modes consist of two factors: the EOF patterns and the corresponding EOF amplitudes. These two factors individually reflect the spatial distributions (e.g., the latitudinal dependence such as the equatorial ionization anomaly structure and the longitude structure with east-west difference) and temporal variations on different time scales (e.g., solar cycle, annual, semiannual, and diurnal variations) of the <span class="hlt">layer</span> parameters. Then, the EOF patterns and long-term observations of ionosondes are assimilated to get the observed EOF amplitudes, which are further used to construct the Chinese Ionospheric Maps (CIMs) of the <span class="hlt">layer</span> parameters. In contrast with the IRI-07 <span class="hlt">model</span>, the mapped CIMs successfully capture the inherent temporal and spatial variations of the ionospheric <span class="hlt">layer</span> parameters. Finally, comparison of the <span class="hlt">modeled</span> (EOF and IRI-07 <span class="hlt">model</span>) and observed values reveals that the EOF <span class="hlt">model</span> reproduces the observation with smaller root-mean-square errors and higher linear correlation co- efficients. In addition, IRI discrepancy at the low latitude especially for foF2 is effectively removed by EOF <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=226427&Lab=NERL&keyword=Eco+AND+technology&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=226427&Lab=NERL&keyword=Eco+AND+technology&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>Extending the Diffuse <span class="hlt">Layer</span> <span class="hlt">Model</span> of Surface Acidity Constant Behavior: IV. Diffuse <span class="hlt">Layer</span> Charge/Potential Relationships</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>Most current electrostatic surface complexation <span class="hlt">models</span> describing ionic binding at the particle/water interface rely on the use of Poisson - Boltzmann (PB) theory for relating diffuse <span class="hlt">layer</span> charge densities to diffuse <span class="hlt">layer</span> electrostatic potentials. PB theory is known to contain ...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008cosp...37.1757L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008cosp...37.1757L"><span>The Fast Debris <span class="hlt">Evolution</span> <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lewis, Hugh G.; Swinerd, Graham; Newland, Rebecca; Saunders, Arrun</p> <p></p> <p>The ‘Particles-in-a-box' (PIB) <span class="hlt">model</span> introduced by Talent (1992) removed the need for computerintensive Monte Carlo simulation to predict the gross characteristics of an evolving debris environment. The PIB <span class="hlt">model</span> was described using a differential equation that allows the stability of the low Earth orbit (LEO) environment to be tested by a straightforward analysis of the equation's coefficients. As part of an ongoing research effort to investigate more efficient approaches to evolutionary <span class="hlt">modelling</span> and to develop a suite of educational tools, a new PIB <span class="hlt">model</span> has been developed. The <span class="hlt">model</span>, entitled Fast Debris <span class="hlt">Evolution</span> (FaDE), employs a first-order differential equation to describe the rate at which new objects (˜ 10 cm) are added and removed from the environment. Whilst Talent (1992) based the collision theory for the PIB approach on collisions between gas particles and adopted specific values for the parameters of the <span class="hlt">model</span> from a number of references, the form and coefficients of the FaDE <span class="hlt">model</span> equations can be inferred from the outputs of future projections produced by high-fidelity <span class="hlt">models</span>, such as the DAMAGE <span class="hlt">model</span>. The FaDE <span class="hlt">model</span> has been implemented as a client-side, web-based service using Javascript embedded within a HTML document. Due to the simple nature of the algorithm, FaDE can deliver the results of future projections immediately in a graphical format, with complete user-control over key simulation parameters. Historical and future projections for the ˜ 10 cm low Earth orbit (LEO) debris environment under a variety of different scenarios are possible, including business as usual, no future launches, post-mission disposal and remediation. A selection of results is presented with comparisons with predictions made using the DAMAGE environment <span class="hlt">model</span>. The results demonstrate that the FaDE <span class="hlt">model</span> is able to capture comparable time-series of collisions and number of objects as predicted by DAMAGE in several scenarios. Further, and perhaps more importantly</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4949710','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4949710"><span>The near‐global mesospheric potassium <span class="hlt">layer</span>: Observations and <span class="hlt">modeling</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>Dawkins, E. C. M.; Chipperfield, M. P.; Feng, W.</p> <p>2015-01-01</p> <p>Abstract The meteoric metal <span class="hlt">layers</span> act as unique tracers of chemistry and dynamics in the upper atmosphere. Existing lidar studies from a few locations show that K exhibits a semiannual seasonality (winter and summer maxima), quite unlike the annual seasonality (winter maximum and summer minimum) seen with Na and Fe. This work uses spaceborne observations made with the Optical Spectrograph and InfraRed Imager System instrument on the Odin satellite to retrieve the near‐global K <span class="hlt">layer</span> for the first time. The satellite data (2004 to mid‐2013) are used to validate the implementation of a recently proposed potassium chemistry scheme in a whole atmosphere chemistry climate <span class="hlt">model</span>, which provides a chemical basis for this semiannual seasonal behavior. The satellite and <span class="hlt">model</span> data show that this semiannual seasonality is near global in extent, with the strongest variation at middle and high latitudes. The column abundance, centroid <span class="hlt">layer</span> height, and root‐mean‐square width of the K <span class="hlt">layer</span> are consistent with the limited available lidar record. The K data set is then used to investigate the impact of polar mesospheric clouds on the metal <span class="hlt">layers</span> at high latitudes during summer. Finally, the occurrence frequency of sporadic K <span class="hlt">layers</span> and their possible link to sporadic E <span class="hlt">layers</span> are examined. PMID:27478716</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016MNRAS.462S.146G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016MNRAS.462S.146G"><span><span class="hlt">Modelling</span> the <span class="hlt">evolution</span> of a comet subsurface: implications for 67P/Churyumov-Gerasimenko</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guilbert-Lepoutre, Aurélie; Rosenberg, Eric D.; Prialnik, Dina; Besse, Sébastien</p> <p>2016-11-01</p> <p><span class="hlt">Modelling</span> the <span class="hlt">evolution</span> of comets is a complex task aiming at providing constraints on physical processes and internal properties that are inaccessible to observations, although they could potentially bring key elements to our understanding of the origins of these primitive objects. This field has made a tremendous step forward in the post-Giotto area, owing to detailed space- and ground-based observations, as well as detailed laboratory simulations of comet nuclei. In this paper, we review studies that we believe are significant for interpreting the observations of 67P/Churyumov-Gerasimenko by the ESA/Rosetta mission, and provide new calculations where needed. These studies hold a strong statistical significance, which is exactly what is needed for this comet with an orbital <span class="hlt">evolution</span> that cannot be traced back accurately for more than hundreds of years. We show that radial and lateral differentiation may have occurred on 67P's chaotic path to the inner Solar system, and that internal inhomogeneities may result in an erratic activity pattern. Finally, we discuss the origins of circular depressions seen on several comets including 67P, and suggest that they could be considered as evidence of the past processing of subsurface <span class="hlt">layers</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhDT.......282H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhDT.......282H"><span><span class="hlt">Modelling</span> hazardous surface hoar <span class="hlt">layers</span> in the mountain snowpack over space and time</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Horton, Simon Earl</p> <p></p> <p>Surface hoar <span class="hlt">layers</span> are a common failure <span class="hlt">layer</span> in hazardous snow slab avalanches. Surface hoar crystals (frost) initially form on the surface of the snow, and once buried can remain a persistent weak <span class="hlt">layer</span> for weeks or months. Avalanche forecasters have difficulty tracking the spatial distribution and mechanical properties of these <span class="hlt">layers</span> in mountainous terrain. This thesis presents numerical <span class="hlt">models</span> and remote sensing methods to track the distribution and properties of surface hoar <span class="hlt">layers</span> over space and time. The formation of surface hoar was <span class="hlt">modelled</span> with meteorological data by calculating the downward flux of water vapour from the atmospheric boundary <span class="hlt">layer</span>. The timing of surface hoar formation and the <span class="hlt">modelled</span> crystal size was verified at snow study sites throughout western Canada. The major surface hoar <span class="hlt">layers</span> over several winters were predicted with fair success. Surface hoar formation was <span class="hlt">modelled</span> over various spatial scales using meteorological data from weather forecast <span class="hlt">models</span>. The largest surface hoar crystals formed in regions and elevation bands with clear skies, warm and humid air, cold snow surfaces, and light winds. Field surveys measured similar regional-scale patterns in surface hoar distribution. Surface hoar formation patterns on different slope aspects were observed, but were not <span class="hlt">modelled</span> reliably. Mechanical field tests on buried surface hoar <span class="hlt">layers</span> found <span class="hlt">layers</span> increased in shear strength over time, but had persistent high propensity for fracture propagation. <span class="hlt">Layers</span> with large crystals and <span class="hlt">layers</span> overlying hard melt-freeze crusts showed greater signs of instability. Buried surface hoar <span class="hlt">layers</span> were simulated with the snow cover <span class="hlt">model</span> SNOWPACK and verified with avalanche observations, finding most hazardous surface hoar <span class="hlt">layers</span> were identified with a structural stability index. Finally, the optical properties of surface hoar crystals were measured in the field with spectral instruments. Large plate-shaped crystals were less reflective at shortwave</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AGUFM.U12A..06B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AGUFM.U12A..06B"><span><span class="hlt">Evolution</span> of Subducted Oceanic Crust in Dynamic Mantle <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brandenburg, J.; van Keken, P. E.; Ballentine, C.; Hauri, E.</p> <p>2006-12-01</p> <p>Isotopic ratios measured in oceanic basalts indicate the persistence of a highly differentiated and ancient mantle component. The provenance and distribution of this component are the subject of much discussion. A number of geodynamic studies have focused on the preservation of a chemically dense <span class="hlt">layer</span> in the deepest mantle, while a smaller set of studies have explored the possibilities for its generation. We present an evaluation of the hypothesis that such a <span class="hlt">layer</span> may represent the accumulation of subducted oceanic crust, with critical examination of the role that plate tectonics plays in mantle differentiation. In geodynamic <span class="hlt">models</span> the treatment of plate tectonics controls crust production, subduction, and modulates the remixing rate. We use two methods for approximating plates in our <span class="hlt">models</span>; prescription of a velocity boundary condition, and the force-balance method [1]. Emphasis is placed on the force-balance method, in which a numerical solution for the conservation of momentum is constructed by superposition. The force balance method has a minimum of free parameters compared to complex rheological descriptions that yield plate like behavior, and does not have the potential to artificially drive or hinder convection introduced by prescribing velocity boundary conditions. The mixing properties of the various methods are examined by comparison of embedded geochemical <span class="hlt">models</span> for the isotopic <span class="hlt">evolution</span> of Pb,U,Sm,Nd,Re,Os, and the noble gases. We find that the incorporation of strong plates leads to a mantle with increased stratification of heterogeneity. Sequestration of old oceanic crust in dense pools in the lowermost mantle is observed. However, the size and longevity of these dense pools decline considerably as realistic convective vigor is approached. Parameter space analysis is used to quantify this variability within the selection of <span class="hlt">models</span> that reproduce Earth-like heat flow and plate velocities, and for comparison with the work of other authors. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20646132','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20646132"><span>Optimality <span class="hlt">models</span> in the age of experimental <span class="hlt">evolution</span> and genomics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Bull, J J; Wang, I-N</p> <p>2010-09-01</p> <p>Optimality <span class="hlt">models</span> have been used to predict <span class="hlt">evolution</span> of many properties of organisms. They typically neglect genetic details, whether by necessity or design. This omission is a common source of criticism, and although this limitation of optimality is widely acknowledged, it has mostly been defended rather than evaluated for its impact. Experimental adaptation of <span class="hlt">model</span> organisms provides a new arena for testing optimality <span class="hlt">models</span> and for simultaneously integrating genetics. First, an experimental context with a well-researched organism allows dissection of the evolutionary process to identify causes of <span class="hlt">model</span> failure--whether the <span class="hlt">model</span> is wrong about genetics or selection. Second, optimality <span class="hlt">models</span> provide a meaningful context for the process and mechanics of <span class="hlt">evolution</span>, and thus may be used to elicit realistic genetic bases of adaptation--an especially useful augmentation to well-researched genetic systems. A few studies of microbes have begun to pioneer this new direction. Incompatibility between the assumed and actual genetics has been demonstrated to be the cause of <span class="hlt">model</span> failure in some cases. More interestingly, <span class="hlt">evolution</span> at the phenotypic level has sometimes matched prediction even though the adaptive mutations defy mechanisms established by decades of classic genetic studies. Integration of experimental evolutionary tests with genetics heralds a new wave for optimality <span class="hlt">models</span> and their extensions that does not merely emphasize the forces driving <span class="hlt">evolution</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3355071','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3355071"><span>The <span class="hlt">Layer</span>-Oriented Approach to Declarative Languages for Biological <span class="hlt">Modeling</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>Raikov, Ivan; De Schutter, Erik</p> <p>2012-01-01</p> <p>We present a new approach to <span class="hlt">modeling</span> languages for computational biology, which we call the <span class="hlt">layer</span>-oriented approach. The approach stems from the observation that many diverse biological phenomena are described using a small set of mathematical formalisms (e.g. differential equations), while at the same time different domains and subdomains of computational biology require that <span class="hlt">models</span> are structured according to the accepted terminology and classification of that domain. Our approach uses distinct semantic <span class="hlt">layers</span> to represent the domain-specific biological concepts and the underlying mathematical formalisms. Additional functionality can be transparently added to the language by adding more <span class="hlt">layers</span>. This approach is specifically concerned with declarative languages, and throughout the paper we note some of the limitations inherent to declarative approaches. The <span class="hlt">layer</span>-oriented approach is a way to specify explicitly how high-level biological <span class="hlt">modeling</span> concepts are mapped to a computational representation, while abstracting away details of particular programming languages and simulation environments. To illustrate this process, we define an example language for describing <span class="hlt">models</span> of ionic currents, and use a general mathematical notation for semantic transformations to show how to generate <span class="hlt">model</span> simulation code for various simulation environments. We use the example language to describe a Purkinje neuron <span class="hlt">model</span> and demonstrate how the <span class="hlt">layer</span>-oriented approach can be used for solving several practical issues of computational neuroscience <span class="hlt">model</span> development. We discuss the advantages and limitations of the approach in comparison with other <span class="hlt">modeling</span> language efforts in the domain of computational biology and outline some principles for extensible, flexible <span class="hlt">modeling</span> language design. We conclude by describing in detail the semantic transformations defined for our language. PMID:22615554</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22615554','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22615554"><span>The <span class="hlt">layer</span>-oriented approach to declarative languages for biological <span class="hlt">modeling</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Raikov, Ivan; De Schutter, Erik</p> <p>2012-01-01</p> <p>We present a new approach to <span class="hlt">modeling</span> languages for computational biology, which we call the <span class="hlt">layer</span>-oriented approach. The approach stems from the observation that many diverse biological phenomena are described using a small set of mathematical formalisms (e.g. differential equations), while at the same time different domains and subdomains of computational biology require that <span class="hlt">models</span> are structured according to the accepted terminology and classification of that domain. Our approach uses distinct semantic <span class="hlt">layers</span> to represent the domain-specific biological concepts and the underlying mathematical formalisms. Additional functionality can be transparently added to the language by adding more <span class="hlt">layers</span>. This approach is specifically concerned with declarative languages, and throughout the paper we note some of the limitations inherent to declarative approaches. The <span class="hlt">layer</span>-oriented approach is a way to specify explicitly how high-level biological <span class="hlt">modeling</span> concepts are mapped to a computational representation, while abstracting away details of particular programming languages and simulation environments. To illustrate this process, we define an example language for describing <span class="hlt">models</span> of ionic currents, and use a general mathematical notation for semantic transformations to show how to generate <span class="hlt">model</span> simulation code for various simulation environments. We use the example language to describe a Purkinje neuron <span class="hlt">model</span> and demonstrate how the <span class="hlt">layer</span>-oriented approach can be used for solving several practical issues of computational neuroscience <span class="hlt">model</span> development. We discuss the advantages and limitations of the approach in comparison with other <span class="hlt">modeling</span> language efforts in the domain of computational biology and outline some principles for extensible, flexible <span class="hlt">modeling</span> language design. We conclude by describing in detail the semantic transformations defined for our language.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhDT.......464B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhDT.......464B"><span>Nanostructural <span class="hlt">Evolution</span> of Hard Turning <span class="hlt">Layers</span> in Carburized Steel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bedekar, Vikram</p> <p></p> <p>The mechanisms of failure for components subjected to contact fatigue are sensitive to the structure and properties of the material surface. Although, the bulk material properties are determined by the steel making, forming and the heat treatment; the near surface material properties are altered during final material removal processes such as hard turning or grinding. Therefore, the ability to optimize, modulate and predict the near surface properties during final metal removal operations would be extremely useful in the enhancement of service life of a component. Hard machining is known to induce severely deformed <span class="hlt">layers</span> causing dramatic microstructural transformations. These transformations occur via grain refinement or thermal phenomena depending upon cutting conditions. The aim of this work is to engineer the near surface nanoscale structure and properties during hard turning by altering strain, strain rate, temperature and incoming microstructure. The near surface material transformations due to hard turning were studied on carburized SAE 8620 bearing steel. Variations in parent material microstructures were introduced by altering the retained austenite content. The strain, strain rate and temperature achieved during final metal cutting were altered by varying insert geometry, insert wear and cutting speed. The subsurface <span class="hlt">evolution</span> was quantified by a series of advanced characterization techniques such as transmission electron microscopy (TEM), glancing angle X-ray diffraction (GAXRD), X-ray stress evaluation and nanoindentation which were coupled with numerical <span class="hlt">modeling</span>. Results showed that the grain size of the nanocrystalline near surface microstructure can be effectively controlled by altering the insert geometry, insert wear, cutting speed and the incoming microstructure. It was also evident that the near surface retained austenite decreased at lower cutting speed indicating transformation due to plastic deformation, while it increased at higher cutting</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19890016812','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19890016812"><span>A two-<span class="hlt">layer</span> multiple-time-scale turbulence <span class="hlt">model</span> and grid independence study</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kim, S.-W.; Chen, C.-P.</p> <p>1989-01-01</p> <p>A two-<span class="hlt">layer</span> multiple-time-scale turbulence <span class="hlt">model</span> is presented. The near-wall <span class="hlt">model</span> is based on the classical Kolmogorov-Prandtl turbulence hypothesis and the semi-empirical logarithmic law of the wall. In the two-<span class="hlt">layer</span> <span class="hlt">model</span> presented, the computational domain of the conservation of mass equation and the mean momentum equation penetrated up to the wall, where no slip boundary condition has been prescribed; and the near wall boundary of the turbulence equations has been located at the fully turbulent region, yet very close to the wall, where the standard wall function method has been applied. Thus, the conservation of mass constraint can be satisfied more rigorously in the two-<span class="hlt">layer</span> <span class="hlt">model</span> than in the standard wall function method. In most of the two-<span class="hlt">layer</span> turbulence <span class="hlt">models</span>, the number of grid points to be used inside the near-wall <span class="hlt">layer</span> posed the issue of computational efficiency. The present finite element computational results showed that the grid independent solutions were obtained with as small as two grid points, i.e., one quadratic element, inside the near wall <span class="hlt">layer</span>. Comparison of the computational results obtained by using the two-<span class="hlt">layer</span> <span class="hlt">model</span> and those obtained by using the wall function method is also presented.</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/2017AGUFM.A51A2028S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A51A2028S"><span>Improved <span class="hlt">Modeling</span> of Surface <span class="hlt">Layer</span> Parameters in a AGCM Using Refined Vertical Resolution in the Surface <span class="hlt">Layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shin, H. H.; Zhao, M.; Ming, Y.; Chen, X.; Lin, S. J.</p> <p>2017-12-01</p> <p>Surface <span class="hlt">layer</span> (SL) parameters in atmospheric <span class="hlt">models</span> - such as 2-m air temperature (T2), 10-m wind speed (U10), and surface turbulent fluxes - are computed by applying the Monin-Obukhov Similarity Theory (MOST) to the lowest <span class="hlt">model</span> level height (LMH) in the <span class="hlt">models</span>. The underlying assumption is that LMH is within surface <span class="hlt">layer</span> height (SLH), but most AGCMs hardly meet the condition in stable boundary <span class="hlt">layers</span> (SBLs) over land. To assess the errors in <span class="hlt">modeled</span> SL parameters caused by this, offline computations of the MOST are performed with different LMHs from 1 to 100 m, for an idealized SBL case with prescribed surface parameters (surface temperature, roughness length and Obukhov length), and vertical profiles of temperature and winds. The results show that when LMH is higher than SLH, T2 and U10 are underestimated by O(1 K) and O(1 m/s), respectively, and the biases increase as LMH increases. Based on this, the refined vertical resolution with an additional <span class="hlt">layer</span> in the SL is applied to the GFDL AGCM, and it reduces the systematic cold biases in T2 and the systematic underestimation of U10.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C13B0962T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C13B0962T"><span>Implementation of a physically-based scheme representing light-absorbing impurities deposition, <span class="hlt">evolution</span> and radiative impacts in the SURFEX/Crocus <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tuzet, F.; Dumont, M.; Lafaysse, M.; Hagenmuller, P.; Arnaud, L.; Picard, G.; Morin, S.</p> <p>2017-12-01</p> <p>Light-absorbing impurities decrease snow albedo, increasing the amount of solar energy absorbed by the snowpack. Its most intuitive impact is to accelerate snow melt. However the presence of a <span class="hlt">layer</span> highly concentrated in light-absorbing impurities in the snowpack also modify its temperature profile affecting snow metamorphism. New capabilities have been implemented in the detailed snowpack <span class="hlt">model</span> SURFEX/ISBA-Crocus (referred to as Crocus) to account for impurities deposition and <span class="hlt">evolution</span> within the snowpack (Tuzet et al., 2017, TCD). Once deposited, the <span class="hlt">model</span> computes impurities mass <span class="hlt">evolution</span> until snow melts out. Taking benefits of the recent inclusion of the spectral radiative transfer <span class="hlt">model</span> TARTES in Crocus, the <span class="hlt">model</span> explicitly represents the radiative impacts of light-absorbing impurities in snow. In the Pyrenees mountain range, strong sporadic Saharan dust deposition (referred to as dust outbreaks) can occur during the snow season leading some snow <span class="hlt">layers</span> in the snowpack to contain high concentrations of mineral dust. One of the major events of the past years occurred on February 2014, affecting the whole southern Europe. During the weeks following this dust outbreak a strong avalanche activity was reported in the Aran valley (Pyrenees, Spain). For now, the link between the dust outbreak and the avalanche activity is not demonstrated.We investigate the impact of this dust outbreak on the snowpack stability in the Aran valley using the Crocus <span class="hlt">model</span>, trying to determine whether the snowpack instability observed after the dust outbreak can be related to the presence of dust. SAFRAN-reanalysis meteorological data are used to drive the <span class="hlt">model</span> on several altitudes, slopes and aspects. For each slope configuration two different simulations are run; one without dust and one simulating the dust outbreak of February 2014.The two corresponding simulations are then compared to assess the role of impurities on snow metamorphism and stability.On this example, we</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17714501','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17714501"><span>The <span class="hlt">evolution</span> of dispersal in a Levins' type metapopulation <span class="hlt">model</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jansen, Vincent A A; Vitalis, Renaud</p> <p>2007-10-01</p> <p>We study the <span class="hlt">evolution</span> of the dispersal rate in a metapopulation <span class="hlt">model</span> with extinction and colonization dynamics, akin to the <span class="hlt">model</span> as originally described by Levins. To do so we extend the metapopulation <span class="hlt">model</span> with a description of the within patch dynamics. By means of a separation of time scales we analytically derive a fitness expression from first principles for this <span class="hlt">model</span>. The fitness function can be written as an inclusive fitness equation (Hamilton's rule). By recasting this equation in a form that emphasizes the effects of competition we show the effect of the local competition and the local population size on the <span class="hlt">evolution</span> of dispersal. We find that the <span class="hlt">evolution</span> of dispersal cannot be easily interpreted in terms of avoidance of kin competition, but rather that increased dispersal reduces the competitive ability. Our <span class="hlt">model</span> also yields a testable prediction in term of relatedness and life-history parameters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23770433','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23770433"><span>A new molecular <span class="hlt">evolution</span> <span class="hlt">model</span> for limited insertion independent of substitution.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lèbre, Sophie; Michel, Christian J</p> <p>2013-10-01</p> <p>We recently introduced a new molecular <span class="hlt">evolution</span> <span class="hlt">model</span> called the IDIS <span class="hlt">model</span> for Insertion Deletion Independent of Substitution [13,14]. In the IDIS <span class="hlt">model</span>, the three independent processes of substitution, insertion and deletion of residues have constant rates. In order to control the genome expansion during <span class="hlt">evolution</span>, we generalize here the IDIS <span class="hlt">model</span> by introducing an insertion rate which decreases when the sequence grows and tends to 0 for a maximum sequence length nmax. This new <span class="hlt">model</span>, called LIIS for Limited Insertion Independent of Substitution, defines a matrix differential equation satisfied by a vector P(t) describing the sequence content in each residue at <span class="hlt">evolution</span> time t. An analytical solution is obtained for any diagonalizable substitution matrix M. Thus, the LIIS <span class="hlt">model</span> gives an expression of the sequence content vector P(t) in each residue under <span class="hlt">evolution</span> time t as a function of the eigenvalues and the eigenvectors of matrix M, the residue insertion rate vector R, the total insertion rate r, the initial and maximum sequence lengths n0 and nmax, respectively, and the sequence content vector P(t0) at initial time t0. The derivation of the analytical solution is much more technical, compared to the IDIS <span class="hlt">model</span>, as it involves Gauss hypergeometric functions. Several propositions of the LIIS <span class="hlt">model</span> are derived: proof that the IDIS <span class="hlt">model</span> is a particular case of the LIIS <span class="hlt">model</span> when the maximum sequence length nmax tends to infinity, fixed point, time scale, time step and time inversion. Using a relation between the sequence length l and the <span class="hlt">evolution</span> time t, an expression of the LIIS <span class="hlt">model</span> as a function of the sequence length l=n(t) is obtained. Formulas for 'insertion only', i.e. when the substitution rates are all equal to 0, are derived at <span class="hlt">evolution</span> time t and sequence length l. Analytical solutions of the LIIS <span class="hlt">model</span> are explicitly derived, as a function of either <span class="hlt">evolution</span> time t or sequence length l, for two classical substitution matrices: the 3</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1419746-evolution-surface-structure-laser-preheated-perturbed-materials','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1419746-evolution-surface-structure-laser-preheated-perturbed-materials"><span><span class="hlt">Evolution</span> of surface structure in laser-preheated, perturbed materials</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Di Stefano, Carlos; Merritt, Elizabeth Catherine; Doss, Forrest William; ...</p> <p>2017-02-03</p> <p>Here, we report an experimental and computational study investigating the effects of laser preheat on the hydrodynamic behavior of a material <span class="hlt">layer</span>. In particular, we find that perturbation of the surface of the <span class="hlt">layer</span> results in a complex interaction, in which the bulk of the <span class="hlt">layer</span> develops density, pressure, and temperature structure and in which the surface experiences instability-like behavior, including mode coupling. A uniform one-temperature preheat <span class="hlt">model</span> is used to reproduce the experimentally observed behavior, and we find that this <span class="hlt">model</span> can be used to capture the <span class="hlt">evolution</span> of the <span class="hlt">layer</span>, while also providing evidence of complexities in themore » preheat behavior. Lastly, this result has important consequences for inertially confined fusion plasmas, which can be difficult to diagnose in detail, as well as for laser hydrodynamics experiments, which generally depend on assumptions about initial conditions in order to interpret their results.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFM.H23C1266S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFM.H23C1266S"><span><span class="hlt">Modeling</span> the Impact of Cracking in Low Permeability <span class="hlt">Layers</span> in a Groundwater Contamination Source Zone on Dissolved Contaminant Fate and Transport</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sievers, K. W.; Goltz, M. N.; Huang, J.; Demond, A. H.</p> <p>2011-12-01</p> <p> and compare four scenarios: (1) CAH diffusion only into cracks, (2) CAH advection-dispersion into cracks, (3) separate phase DNAPL movement into the cracks, and (4) CAH diffusion into an uncracked low permeability clay <span class="hlt">layer</span>. For each scenario, <span class="hlt">model</span> simulations are used to show the <span class="hlt">evolution</span> and persistence of groundwater contamination downgradient of the DNAPL source.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AdSpR..44..568L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AdSpR..44..568L"><span>The fast debris <span class="hlt">evolution</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lewis, H. G.; Swinerd, G. G.; Newland, R. J.; Saunders, A.</p> <p>2009-09-01</p> <p>The 'particles-in-a-box' (PIB) <span class="hlt">model</span> introduced by Talent [Talent, D.L. Analytic <span class="hlt">model</span> for orbital debris environmental management. J. Spacecraft Rocket, 29 (4), 508-513, 1992.] removed the need for computer-intensive Monte Carlo simulation to predict the gross characteristics of an evolving debris environment. The PIB <span class="hlt">model</span> was described using a differential equation that allows the stability of the low Earth orbit (LEO) environment to be tested by a straightforward analysis of the equation's coefficients. As part of an ongoing research effort to investigate more efficient approaches to evolutionary <span class="hlt">modelling</span> and to develop a suite of educational tools, a new PIB <span class="hlt">model</span> has been developed. The <span class="hlt">model</span>, entitled Fast Debris <span class="hlt">Evolution</span> (FADE), employs a first-order differential equation to describe the rate at which new objects ⩾10 cm are added and removed from the environment. Whilst Talent [Talent, D.L. Analytic <span class="hlt">model</span> for orbital debris environmental management. J. Spacecraft Rocket, 29 (4), 508-513, 1992.] based the collision theory for the PIB approach on collisions between gas particles and adopted specific values for the parameters of the <span class="hlt">model</span> from a number of references, the form and coefficients of the FADE <span class="hlt">model</span> equations can be inferred from the outputs of future projections produced by high-fidelity <span class="hlt">models</span>, such as the DAMAGE <span class="hlt">model</span>. The FADE <span class="hlt">model</span> has been implemented as a client-side, web-based service using JavaScript embedded within a HTML document. Due to the simple nature of the algorithm, FADE can deliver the results of future projections immediately in a graphical format, with complete user-control over key simulation parameters. Historical and future projections for the ⩾10 cm LEO debris environment under a variety of different scenarios are possible, including business as usual, no future launches, post-mission disposal and remediation. A selection of results is presented with comparisons with predictions made using the DAMAGE environment <span class="hlt">model</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26977761','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26977761"><span>Boosting water oxidation <span class="hlt">layer-by-layer</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hidalgo-Acosta, Jonnathan C; Scanlon, Micheál D; Méndez, Manuel A; Amstutz, Véronique; Vrubel, Heron; Opallo, Marcin; Girault, Hubert H</p> <p>2016-04-07</p> <p>Electrocatalysis of water oxidation was achieved using fluorinated tin oxide (FTO) electrodes modified with <span class="hlt">layer-by-layer</span> deposited films consisting of bilayers of negatively charged citrate-stabilized IrO2 NPs and positively charged poly(diallyldimethylammonium chloride) (PDDA) polymer. The IrO2 NP surface coverage can be fine-tuned by controlling the number of bilayers. The IrO2 NP films were amorphous, with the NPs therein being well-dispersed and retaining their as-synthesized shape and sizes. UV/vis spectroscopic and spectro-electrochemical studies confirmed that the total surface coverage and electrochemically addressable surface coverage of IrO2 NPs increased linearly with the number of bilayers up to 10 bilayers. The voltammetry of the modified electrode was that of hydrous iridium oxide films (HIROFs) with an observed super-Nernstian pH response of the Ir(III)/Ir(IV) and Ir(IV)-Ir(IV)/Ir(IV)-Ir(V) redox transitions and Nernstian shift of the oxygen <span class="hlt">evolution</span> onset potential. The overpotential of the oxygen <span class="hlt">evolution</span> reaction (OER) was essentially pH independent, varying only from 0.22 V to 0.28 V (at a current density of 0.1 mA cm(-2)), moving from acidic to alkaline conditions. Bulk electrolysis experiments revealed that the IrO2/PDDA films were stable and adherent under acidic and neutral conditions but degraded in alkaline solutions. Oxygen was evolved with Faradaic efficiencies approaching 100% under acidic (pH 1) and neutral (pH 7) conditions, and 88% in alkaline solutions (pH 13). This <span class="hlt">layer-by-layer</span> approach forms the basis of future large-scale OER electrode development using ink-jet printing technology.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMNH43B1857M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMNH43B1857M"><span><span class="hlt">Modeling</span> Tsunami Wave Generation Using a Two-<span class="hlt">layer</span> Granular Landslide <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ma, G.; Kirby, J. T., Jr.; Shi, F.; Grilli, S. T.; Hsu, T. J.</p> <p>2016-12-01</p> <p>Tsunamis can be generated by subaerial or submarine landslides in reservoirs, lakes, fjords, bays and oceans. Compared to seismogenic tsunamis, landslide or submarine mass failure (SMF) tsunamis are normally characterized by relatively shorter wave lengths and stronger wave dispersion, and potentially may generate large wave amplitudes locally and high run-up along adjacent coastlines. Due to a complex interplay between the landslide and tsunami waves, accurate simulation of landslide motion as well as tsunami generation is a challenging task. We develop and test a new two-<span class="hlt">layer</span> <span class="hlt">model</span> for granular landslide motion and tsunami wave generation. The landslide is described as a saturated granular flow, accounting for intergranular stresses governed by Coulomb friction. Tsunami wave generation is simulated by the three-dimensional non-hydrostatic wave <span class="hlt">model</span> NHWAVE, which is capable of capturing wave dispersion efficiently using a small number of discretized vertical levels. Depth-averaged governing equations for the granular landslide are derived in a slope-oriented coordinate system, taking into account the dynamic interaction between the lower-<span class="hlt">layer</span> granular landslide and upper-<span class="hlt">layer</span> water motion. The <span class="hlt">model</span> is tested against laboratory experiments on impulsive wave generation by subaerial granular landslides. <span class="hlt">Model</span> results illustrate a complex interplay between the granular landslide and tsunami waves, and they reasonably predict not only the tsunami wave generation but also the granular landslide motion from initiation to deposition.</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 <span class="hlt">modeling</span> of the transitional boundary <span class="hlt">layer</span> 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 boundary <span class="hlt">layer</span> becomes turbulent. We have chosen the flow over a flat plate as a prototype for boundary-<span class="hlt">layer</span> flows around bodies. Special attention was paid to the near-wall region in order to capture all levels of the boundary <span class="hlt">layer</span>. 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 <span class="hlt">model</span> is presently incorporated into a computer code suitable for the LES of developing flat-plate boundary <span class="hlt">layers</span>. Presently this <span class="hlt">model</span> is extended to the LES of the zero-pressure gradient, flat-plate turbulent boundary <span class="hlt">layer</span>. In current 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 <span class="hlt">models</span>. The transition <span class="hlt">models</span> significantly improve the prediction of the onset location compared to the fully turbulent <span class="hlt">models</span>.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://hdl.handle.net/2060/20010080472','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20010080472"><span>Representation of Clear and Cloudy Boundary <span class="hlt">Layers</span> in Climate <span class="hlt">Models</span>. 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 <span class="hlt">models</span> which are being used as components of climate <span class="hlt">models</span> rely on their boundary <span class="hlt">layer</span> parameterizations to produce realistic simulations of the surface turbulent fluxes of sensible heat. moisture. and momentum: of the boundary-<span class="hlt">layer</span> depth over which these fluxes converge: of boundary <span class="hlt">layer</span> cloudiness: and of the interactions of the boundary <span class="hlt">layer</span> with the deep convective clouds that grow upwards from it. Two current atmospheric general circulation <span class="hlt">models</span> are used as examples to show how these requirements are being addressed: these are version 3 of the Community Climate <span class="hlt">Model</span>. which has been developed at the U.S. National Center for Atmospheric Research. and the Colorado State University atmospheric general circulation <span class="hlt">model</span>. The formulations and results of both <span class="hlt">models</span> are discussed. Finally, areas for future research are suggested.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/6371540','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/6371540"><span>Mathematical <span class="hlt">modeling</span> and simulation analysis of hydraulic fracture propagation in three-<span class="hlt">layered</span> poro-elastic media</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>Moon, H.Y.; Advani, S.H.; Lee, T.S.</p> <p>1992-11-01</p> <p>Hydraulic fracturing plays a pivotal role in the enhancement of oil and gas production recovery from low permeability reservoirs. The process of hydraulic fracturing entails the generation of a fracture by pumping fluids blended with special chemicals and proppants into the payzone at high injection rates and pressures to extend and wedge fractures. The mathematical <span class="hlt">modeling</span> of hydraulically induced fractures generally incorporates coupling between the formation elasticity, fracture fluid flow, and fracture mechanics equations governing the formation structural responses, fluid pressure profile, and fracture growth. Two allied unsymmetric elliptic fracture <span class="hlt">models</span> are developed for fracture configuration <span class="hlt">evolutions</span> in three-<span class="hlt">layered</span> rockmore » formations. The first approach is based on a Lagrangian formulation incorporating pertinent energy components associated with the formation structural responses and fracture fluid flow. The second <span class="hlt">model</span> is based on a generalized variational principle, introducing an energy rate related functional. These <span class="hlt">models</span> initially simulate a penny-shaped fracture, which becomes elliptic if the crack tips encounters (upper and/or lower) barriers with differential reservoir properties (in situ stresses, 16 elastic moduli, and fracture toughness-contrasts and fluid leak-off characteristics). The energy rate component magnitudes are determined to interpret the governing hydraulic fracture mechanisms during fracture <span class="hlt">evolution</span>. The variational principle is extended to study the phenomenon and consequences of fluid lag in fractures. Finally, parametric sensitivity and energy rate investigations to evaluate the roles of controllable hydraulic treatment variables and uncontrollable reservoir property characterization parameters are performed. The presented field applications demonstrate the overall capabilities of the developed <span class="hlt">models</span>. These studies provide stimulation treatment guidelines for fracture configuration design, control, and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10250E..0DZ','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10250E..0DZ"><span>Monte Carlo <span class="hlt">model</span> of light transport in multi-<span class="hlt">layered</span> tubular organs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Yunyao; Zhu, Jingping; Zhang, Ning</p> <p>2017-02-01</p> <p>We present a Monte Carlo static light migration <span class="hlt">model</span> (Endo-MCML) to simulate endoscopic optical spectroscopy for tubular organs such as esophagus and colon. The <span class="hlt">model</span> employs multi-<span class="hlt">layered</span> hollow cylinder which emitting and receiving light both from the inner boundary to meet the conditions of endoscopy. Inhomogeneous sphere can be added in tissue <span class="hlt">layers</span> to <span class="hlt">model</span> cancer or other abnormal changes. The 3D light distribution and exit angle would be recorded as results. The accuracy of the <span class="hlt">model</span> has been verified by Multi-<span class="hlt">layered</span> Monte Carlo(MCML) method and NIRFAST. This <span class="hlt">model</span> can be used for the forward <span class="hlt">modeling</span> of light transport during endoscopically diffuse optical spectroscopy, light scattering spectroscopy, reflectance spectroscopy and other static optical detection or imaging technologies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhDT.......211A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhDT.......211A"><span>Galactic chemical <span class="hlt">evolution</span> in hierarchical formation <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arrigoni, Matias</p> <p>2010-10-01</p> <p>The chemical properties and abundance ratios of galaxies provide important information about their formation histories. Galactic chemical <span class="hlt">evolution</span> has been <span class="hlt">modelled</span> in detail within the monolithic collapse scenario. These <span class="hlt">models</span> have successfully described the abundance distributions in our Galaxy and other spiral discs, as well as the trends of metallicity and abundance ratios observed in early-type galaxies. In the last three decades, however, the paradigm of hierarchical assembly in a Cold Dark Matter (CDM) cosmology has revised the picture of how structure in the Universe forms and evolves. In this scenario, galaxies form when gas radiatively cools and condenses inside dark matter haloes, which themselves follow dissipationless gravitational collapse. The CDM picture has been successful at predicting many observed properties of galaxies (for example, the luminosity and stellar mass function of galaxies, color-magnitude or star formation rate vs. stellar mass distributions, relative numbers of early and late-type galaxies, gas fractions and size distributions of spiral galaxies, and the global star formation history), though many potential problems and open questions remain. It is therefore interesting to see whether chemical <span class="hlt">evolution</span> <span class="hlt">models</span>, when implemented within this modern cosmological context, are able to correctly predict the observed chemical properties of galaxies. With the advent of more powerfull telescopes and detectors, precise observations of chemical abundances and abundance ratios in various phases (stellar, ISM, ICM) offer the opportunity to obtain strong constraints on galaxy formation histories and the physics that shapes them. However, in order to take advantage of these observations, it is necessary to implement detailed <span class="hlt">modeling</span> of chemical <span class="hlt">evolution</span> into a modern cosmological <span class="hlt">model</span> of hierarchical assembly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19073195','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19073195"><span>In silico <span class="hlt">modelling</span> of directed <span class="hlt">evolution</span>: Implications for experimental design and stepwise <span class="hlt">evolution</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wedge, David C; Rowe, William; Kell, Douglas B; Knowles, Joshua</p> <p>2009-03-07</p> <p>We <span class="hlt">model</span> the process of directed <span class="hlt">evolution</span> (DE) in silico using genetic algorithms. Making use of the NK fitness landscape <span class="hlt">model</span>, we analyse the effects of mutation rate, crossover and selection pressure on the performance of DE. A range of values of K, the epistatic interaction of the landscape, are considered, and high- and low-throughput modes of <span class="hlt">evolution</span> are compared. Our findings suggest that for runs of or around ten generations' duration-as is typical in DE-there is little difference between the way in which DE needs to be configured in the high- and low-throughput regimes, nor across different degrees of landscape epistasis. In all cases, a high selection pressure (but not an extreme one) combined with a moderately high mutation rate works best, while crossover provides some benefit but only on the less rugged landscapes. These genetic algorithms were also compared with a "<span class="hlt">model</span>-based approach" from the literature, which uses sequential fixing of the problem parameters based on fitting a linear <span class="hlt">model</span>. Overall, we find that purely evolutionary techniques fare better than do <span class="hlt">model</span>-based approaches across all but the smoothest landscapes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19790060856&hterms=planetary+boundaries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dplanetary%2Bboundaries','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19790060856&hterms=planetary+boundaries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dplanetary%2Bboundaries"><span>A <span class="hlt">model</span> of the planetary boundary <span class="hlt">layer</span> over a snow surface</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Halberstam, I.; Melendez, R.</p> <p>1979-01-01</p> <p>A <span class="hlt">model</span> of the planetary boundary <span class="hlt">layer</span> over a snow surface has been developed. It contains the vertical heat exchange processes due to radiation, conduction, and atmospheric turbulence. Parametrization of the boundary <span class="hlt">layer</span> is based on similarity functions developed by Hoffert and Sud (1976), which involve a dimensionless variable, dependent on boundary-<span class="hlt">layer</span> height and a localized Monin-Obukhov length. The <span class="hlt">model</span> also contains the atmospheric surface <span class="hlt">layer</span> and the snowpack itself, where snowmelt and snow evaporation are calculated. The results indicate a strong dependence of surface temperatures, especially at night, on the bursts of turbulence which result from the frictional damping of surface-<span class="hlt">layer</span> winds during periods of high stability, as described by Businger (1973). The <span class="hlt">model</span> also shows the cooling and drying effect of the snow on the atmosphere, which may be the mechanism for air mass transformation in sub-Arctic regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JMPSo.111..490M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JMPSo.111..490M"><span>Mechanical <span class="hlt">model</span> of suture joints with fibrous connective <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Miroshnichenko, Kateryna; Liu, Lei; Tsukrov, Igor; Li, Yaning</p> <p>2018-02-01</p> <p>A composite <span class="hlt">model</span> for suture joints with a connective <span class="hlt">layer</span> of aligned fibers embedded in soft matrix is proposed. Based on the principle of complementary virtual work, composite cylinder assemblage (CCA) approach and generalized self-consistent micro-mechanical <span class="hlt">models</span>, a hierarchical homogenization methodology is developed to systematically quantify the synergistic effects of suture morphology and fiber orientation on the overall mechanical properties of sutures. Suture joints with regular triangular wave-form serve as an example material system to apply this methodology. Both theoretical and finite element mechanical <span class="hlt">models</span> are developed and compared to evaluate the overall normal stiffness of sutures as a function of wavy morphology of sutures, fiber orientation, fiber volume fraction, and the mechanical properties of fibers and matrix in the interfacial <span class="hlt">layer</span>. It is found that generally due to the anisotropy-induced coupling effects between tensile and shear deformation, the effective normal stiffness of sutures is highly dependent on the fiber orientation in the connective <span class="hlt">layer</span>. Also, the effective shear modulus of the connective <span class="hlt">layer</span> and the stiffness ratio between the fiber and matrix significantly influence the effects of fiber orientation. In addition, optimal fiber orientations are found to maximize the stiffness of suture joints.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012TCD.....6.5225G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012TCD.....6.5225G"><span>A balanced water <span class="hlt">layer</span> concept for subglacial hydrology in large scale ice sheet <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Goeller, S.; Thoma, M.; Grosfeld, K.; Miller, H.</p> <p>2012-12-01</p> <p>There is currently no doubt about the existence of a wide-spread hydrological network under the Antarctic ice sheet, which lubricates the ice base and thus leads to increased ice velocities. Consequently, ice <span class="hlt">models</span> should incorporate basal hydrology to obtain meaningful results for future ice dynamics and their contribution to global sea level rise. Here, we introduce the balanced water <span class="hlt">layer</span> concept, covering two prominent subglacial hydrological features for ice sheet <span class="hlt">modeling</span> on a continental scale: the <span class="hlt">evolution</span> of subglacial lakes and balance water fluxes. We couple it to the thermomechanical ice-flow <span class="hlt">model</span> RIMBAY and apply it to a synthetic <span class="hlt">model</span> domain inspired by the Gamburtsev Mountains, Antarctica. In our experiments we demonstrate the dynamic generation of subglacial lakes and their impact on the velocity field of the overlaying ice sheet, resulting in a negative ice mass balance. Furthermore, we introduce an elementary parametrization of the water flux-basal sliding coupling and reveal the predominance of the ice loss through the resulting ice streams against the stabilizing influence of less hydrologically active areas. We point out, that established balance flux schemes quantify these effects only partially as their ability to store subglacial water is lacking.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1414818-structural-chemical-evolution-cds-window-layer-during-individual-cdte-solar-cell-processing-steps','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1414818-structural-chemical-evolution-cds-window-layer-during-individual-cdte-solar-cell-processing-steps"><span>Structural and chemical <span class="hlt">evolution</span> of the CdS:O window <span class="hlt">layer</span> during individual CdTe solar cell processing steps</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Abbas, A.; Meysing, D. M.; Reese, M. O.; ...</p> <p>2017-12-01</p> <p>Oxygenated cadmium sulfide (CdS:O) is often used as the n-type window <span class="hlt">layer</span> in high-performance CdTe heterojunction solar cells. The as-deposited <span class="hlt">layer</span> prepared by reactive sputtering is XRD amorphous, with a bulk composition of CdS0.8O1.2. Recently it was shown that this <span class="hlt">layer</span> undergoes significant transformation during device fabrication, but the roles of the individual high temperature processing steps was unclear. In this work high resolution transmission electron microscopy coupled to elemental analysis was used to understand the <span class="hlt">evolution</span> of the heterojunction region through the individual high temperature fabrication steps of CdTe deposition, CdCl2 activation, and back contact activation. It is foundmore » that during CdTe deposition by close spaced sublimation at 600 degrees C the CdS:O film undergoes recrystallization, accompanied by a significant (~30%) reduction in thickness. It is observed that oxygen segregates during this step, forming a bi-<span class="hlt">layer</span> morphology consisting of nanocrystalline CdS adjacent to the tin oxide contact and an oxygen-rich <span class="hlt">layer</span> adjacent to the CdTe absorber. This bilayer structure is then lost during the 400 degrees C CdCl2 treatment where the film transforms into a heterogeneous structure with cadmium sulfate clusters distributed randomly throughout the window <span class="hlt">layer</span>. The thickness of window <span class="hlt">layer</span> remains essentially unchanged after CdCl2 treatment, but a ~25 nm graded interfacial <span class="hlt">layer</span> between CdTe and the window region is formed. Finally, the rapid thermal processing step used to activate the back contact was found to have a negligible impact on the structure or composition of the heterojunction region.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1414818-structural-chemical-evolution-cds-window-layer-during-individual-cdte-solar-cell-processing-steps','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1414818-structural-chemical-evolution-cds-window-layer-during-individual-cdte-solar-cell-processing-steps"><span>Structural and chemical <span class="hlt">evolution</span> of the CdS:O window <span class="hlt">layer</span> during individual CdTe solar cell processing steps</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>Abbas, A.; Meysing, D. M.; Reese, M. O.</p> <p></p> <p>Oxygenated cadmium sulfide (CdS:O) is often used as the n-type window <span class="hlt">layer</span> in high-performance CdTe heterojunction solar cells. The as-deposited <span class="hlt">layer</span> prepared by reactive sputtering is XRD amorphous, with a bulk composition of CdS0.8O1.2. Recently it was shown that this <span class="hlt">layer</span> undergoes significant transformation during device fabrication, but the roles of the individual high temperature processing steps was unclear. In this work high resolution transmission electron microscopy coupled to elemental analysis was used to understand the <span class="hlt">evolution</span> of the heterojunction region through the individual high temperature fabrication steps of CdTe deposition, CdCl2 activation, and back contact activation. It is foundmore » that during CdTe deposition by close spaced sublimation at 600 degrees C the CdS:O film undergoes recrystallization, accompanied by a significant (~30%) reduction in thickness. It is observed that oxygen segregates during this step, forming a bi-<span class="hlt">layer</span> morphology consisting of nanocrystalline CdS adjacent to the tin oxide contact and an oxygen-rich <span class="hlt">layer</span> adjacent to the CdTe absorber. This bilayer structure is then lost during the 400 degrees C CdCl2 treatment where the film transforms into a heterogeneous structure with cadmium sulfate clusters distributed randomly throughout the window <span class="hlt">layer</span>. The thickness of window <span class="hlt">layer</span> remains essentially unchanged after CdCl2 treatment, but a ~25 nm graded interfacial <span class="hlt">layer</span> between CdTe and the window region is formed. Finally, the rapid thermal processing step used to activate the back contact was found to have a negligible impact on the structure or composition of the heterojunction region.« 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_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('https://www.osti.gov/pages/biblio/1185001-observation-electron-beam-induced-phase-evolution-mimicking-effect-chargedischarge-cycle-li-rich-layered-cathode-materials-used-li-ion-batteries','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1185001-observation-electron-beam-induced-phase-evolution-mimicking-effect-chargedischarge-cycle-li-rich-layered-cathode-materials-used-li-ion-batteries"><span>Observation of Electron-Beam-Induced Phase <span class="hlt">Evolution</span> Mimicking the Effect of the Charge–Discharge Cycle in Li-Rich <span class="hlt">Layered</span> Cathode Materials Used for Li Ion Batteries</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lu, Ping; Yan, Pengfei; Romero, Eric; ...</p> <p>2015-01-27</p> <p>Capacity loss, and voltage decrease upon electrochemical charge-discharge cycling observed in lithium-rich <span class="hlt">layered</span> cathode oxides (Li[Li xMn yTM 1-x-y]O 2, TM = Ni, Co or Fe) have recently been attributed to the formation of a surface reconstructed <span class="hlt">layer</span> (SRL) that evolves from a thin (<2 nm), defect spinel <span class="hlt">layer</span> upon the first charge, to a relatively thick (~5nm), spinel or rock-salt <span class="hlt">layer</span> upon continuous charge-discharge cycling. Here we report observations of a SRL and structural <span class="hlt">evolution</span> of the SRL on the Li[Li 0.2Ni 0.2Mn 0.6]O 2 (LNMO) particles, which are identical to those reported due to the charge-discharge cycle butmore » are a result of electron-beam irradiation during scanning transmission electron microscopy (STEM) imaging. Sensitivity of the lithium-rich <span class="hlt">layered</span> oxides to high-energy electrons leads to the formation of thin, defect spinel <span class="hlt">layer</span> on surfaces of the particles when exposed to a 200kV electron beam for as little as 30 seconds under normal high-resolution STEM imaging conditions. Further electron irradiation produces a thicker <span class="hlt">layer</span> of the spinel phase, ultimately producing a rock-salt <span class="hlt">layer</span> at a higher electron exposure. Atomic-scale chemical mapping by electron dispersive X-ray spectroscopy in STEM indicates the electron-beam-induced SRL formation on LNMO is accomplished by migration of the transition metal ions to the Li sites without breaking down the lattice. The observation through this study provides an insight for understanding the mechanism of forming the SRL and also possibly a mean to study structural <span class="hlt">evolution</span> in the Li-rich <span class="hlt">layered</span> oxides without involving the electrochemistry.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1611386C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1611386C"><span>Observations and <span class="hlt">modelling</span> of the boundary <span class="hlt">layer</span> using remotely piloted aircraft</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cayez, Gregoire; Dralet, Jean-Philippe; Seity, Yann; Momboisse, Geraud; Hattenberger, Gautier; Bronz, Murat; Roberts, Greg</p> <p>2014-05-01</p> <p>Over the past decade, the scientific community considers the RPAS (remotely piloted aircraft system) as a tool which can help to improve their knowledge of climate and atmospheric phenomena. RPAS equipped with instruments can now conduct measurements in areas that are too hazardous or remote for a manned plane. RPAS are especially adapted system for observing the atmospheric boundary <span class="hlt">layer</span> processes at high vertical and temporal resolution. The main objectives of VOLTIGE (Vecteur d'Observation de La Troposphère pour l'Investigation et la Gestion de l'Environnement) are to study the life cycle of fog with micro-RPAS, encourage direct participation of the students on the advancement and development of novel observing systems, and assess the feasibility of deploying RPAS in Météo-France's operational network. The instrumented RPAS flights successfully observed the <span class="hlt">evolution</span> of small-scale meteorological events. Before the arrival of the warm pseudo-front, profiles show a temperature inversion of a hundred meters, which overlaps a cold and wet atmospheric <span class="hlt">layer</span>. Subsequent profiles show the combination of the arrival of a marine air mass as well as the arrival of a higher level warm pseudo-front. A third case study characterizes the warm sector of the disturbance. Two distinct air masses are visible on the vertical profiles, and show a dry air above an air almost saturated and slightly colder. The temperature and the relative humidity profiles show < 1 meter vertical resolution with a difference between ascent and descent profiles within ± 0.5°C and ± 6 % RH. These results comply with the Météo-France standard limits of quality control. The RPAS profiles were compared with those of the Arome forecast <span class="hlt">model</span> (an operational <span class="hlt">model</span> at Météo France). The temperature and wind in the Arome <span class="hlt">model</span> profiles generally agree with those of the RPAS (less for relative humidity profiles). The Arome <span class="hlt">model</span> also suggests transitions between air masses occurred at a higher</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950016043','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950016043"><span>Forced free-shear <span class="hlt">layer</span> measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Leboeuf, Richard L.</p> <p>1994-01-01</p> <p>Detailed three-dimensional three-component phase averaged measurements of the spanwise and streamwise vorticity formation and <span class="hlt">evolution</span> in acoustically forced plane free-shear flows have been obtained. For the first time, phase-averaged measurements of all three velocity components have been obtained in both a mixing <span class="hlt">layer</span> and a wake on three-dimensional grids, yielding the spanwise and streamwise vorticity distributions without invoking Taylor's hypothesis. Initially, two-frequency forcing was used to phase-lock the roll-up and first pairing of the spanwise vortical structures in a plane mixing <span class="hlt">layer</span>. The objective of this study was to measure the near-field vortical structure morphology in a mixing <span class="hlt">layer</span> with 'natural' laminar initial boundary <span class="hlt">layers</span>. For the second experiment the second and third subharmonics of the fundamental roll-up frequency were added to the previous two-frequency forcing in order to phase-lock the roll-up and first three pairings of the spanwise rollers in the mixing <span class="hlt">layer</span>. The objective of this study was to determine the details of spanwise scale changes observed in previous time-averaged measurements and flow visualization of unforced mixing <span class="hlt">layers</span>. For the final experiment, single-frequency forcing was used to phase-lock the Karman vortex street in a plane wake developing from nominally two-dimensional laminar initial boundary <span class="hlt">layers</span>. The objective of this study was to compare measurements of the three-dimensional structure in a wake developing from 'natural' initial boundary <span class="hlt">layers</span> to existing <span class="hlt">models</span> of wake vortical structure.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25730297','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25730297"><span><span class="hlt">Layer-by-layer</span> <span class="hlt">evolution</span> of structure, strain, and activity for the oxygen <span class="hlt">evolution</span> reaction in graphene-templated Pt monolayers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Abdelhafiz, Ali; Vitale, Adam; Joiner, Corey; Vogel, Eric; Alamgir, Faisal M</p> <p>2015-03-25</p> <p>In this study, we explore the dimensional aspect of structure-driven surface properties of metal monolayers grown on a graphene/Au template. Here, surface limited redox replacement (SLRR) is used to provide precise <span class="hlt">layer-by-layer</span> growth of Pt monolayers on graphene. We find that after a few iterations of SLRR, fully wetted 4-5 monolayer Pt films can be grown on graphene. Incorporating graphene at the Pt-Au interface modifies the growth mechanism, charge transfers, equilibrium interatomic distances, and associated strain of the synthesized Pt monolayers. We find that a single <span class="hlt">layer</span> of sandwiched graphene is able to induce a 3.5% compressive strain on the Pt adlayer grown on it, and as a result, catalytic activity is increased due to a greater areal density of the Pt <span class="hlt">layers</span> beyond face-centered-cubic close packing. At the same time, the sandwiched graphene does not obstruct vicinity effects of near-surface electron exchange between the substrate Au and adlayers Pt. X-ray photoelectron spectroscopy (XPS) and extended X-ray absorption fine structure (EXAFS) techniques are used to examine charge mediation across the Pt-graphene-Au junction and the local atomic arrangement as a function of the Pt adlayer dimension. Cyclic voltammetry (CV) and the oxygen reduction reaction (ORR) are used as probes to examine the electrochemically active area of Pt monolayers and catalyst activity, respectively. Results show that the inserted graphene monolayer results in increased activity for the Pt due to a graphene-induced compressive strain, as well as a higher resistance against loss of the catalytically active Pt surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.811a2010P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.811a2010P"><span>Order reduction for a <span class="hlt">model</span> of marine bacteriophage <span class="hlt">evolution</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pagliarini, Silvia; Korobeinikov, Andrei</p> <p>2017-02-01</p> <p>A typical mechanistic <span class="hlt">model</span> of viral <span class="hlt">evolution</span> necessary includes several time scales which can differ by orders of magnitude. Such a diversity of time scales makes analysis of these <span class="hlt">models</span> difficult. Reducing the order of a <span class="hlt">model</span> is highly desirable when handling such a <span class="hlt">model</span>. A typical approach applied to such slow-fast (or singularly perturbed) systems is the time scales separation technique. Constructing the so-called quasi-steady-state approximation is the usual first step in applying the technique. While this technique is commonly applied, in some cases its straightforward application can lead to unsatisfactory results. In this paper we construct the quasi-steady-state approximation for a <span class="hlt">model</span> of <span class="hlt">evolution</span> of marine bacteriophages based on the Beretta-Kuang <span class="hlt">model</span>. We show that for this particular <span class="hlt">model</span> the quasi-steady-state approximation is able to produce only qualitative but not quantitative fit.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19930030581&hterms=order+mixed&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dorder%2Bmixed','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19930030581&hterms=order+mixed&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dorder%2Bmixed"><span>A second-order bulk boundary-<span class="hlt">layer</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Randall, David A.; Shao, Qingqiu; Moeng, Chin-Hoh</p> <p>1992-01-01</p> <p>Bulk mass-flux <span class="hlt">models</span> represent the large eddies that are primarily responsible for the turbulent fluxes in the planetary boundary <span class="hlt">layer</span> as convective circulations, with an associated convective mass flux. In order for such <span class="hlt">models</span> to be useful, it is necessary to determine the fractional area covered by rising motion in the convective circulations. This fraction can be used as an estimate of the cloud amount, under certain conditions. 'Matching' conditions have been developed that relate the convective mass flux to the ventilation and entrainment mass fluxes. These are based on conservation equations for the scalar means and variances in the entrainment and ventilation <span class="hlt">layers</span>. Methods are presented to determine both the fractional area covered by rising motion and the convective mass flux. The requirement of variance balance is used to relax the 'well-mixed' assumption. The vertical structures of the mean state and the turbulent fluxes are determined analytically. Several aspects of this simple <span class="hlt">model</span>'s formulation are evaluated using results from large-eddy simulations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009CMMPh..49.1493M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009CMMPh..49.1493M"><span>A discrete mathematical <span class="hlt">model</span> of the dynamic <span class="hlt">evolution</span> of a transportation network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Malinetskii, G. G.; Stepantsov, M. E.</p> <p>2009-09-01</p> <p>A dynamic <span class="hlt">model</span> of the <span class="hlt">evolution</span> of a transportation network is proposed. The main feature of this <span class="hlt">model</span> is that the <span class="hlt">evolution</span> of the transportation network is not a process of centralized transportation optimization. Rather, its dynamic behavior is a result of the system self-organization that occurs in the course of the satisfaction of needs in goods transportation and the <span class="hlt">evolution</span> of the infrastructure of the network nodes. Nonetheless, the possibility of soft control of the network <span class="hlt">evolution</span> direction is taken into account.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050051581','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050051581"><span>Boundary-<span class="hlt">Layer</span> Receptivity and Integrated Transition Prediction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chang, Chau-Lyan; Choudhari, Meelan</p> <p>2005-01-01</p> <p>The adjoint parabold stability equations (PSE) formulation is used to calculate the boundary <span class="hlt">layer</span> receptivity to localized surface roughness and suction for compressible boundary <span class="hlt">layers</span>. Receptivity efficiency functions predicted by the adjoint PSE approach agree well with results based on other nonparallel methods including linearized Navier-Stokes equations for both Tollmien-Schlichting waves and crossflow instability in swept wing boundary <span class="hlt">layers</span>. The receptivity efficiency function can be regarded as the Green's function to the disturbance amplitude <span class="hlt">evolution</span> in a nonparallel (growing) boundary <span class="hlt">layer</span>. Given the Fourier transformed geometry factor distribution along the chordwise direction, the linear disturbance amplitude <span class="hlt">evolution</span> for a finite size, distributed nonuniformity can be computed by evaluating the integral effects of both disturbance generation and linear amplification. The synergistic approach via the linear adjoint PSE for receptivity and nonlinear PSE for disturbance <span class="hlt">evolution</span> downstream of the leading edge forms the basis for an integrated transition prediction tool. Eventually, such physics-based, high fidelity prediction methods could simulate the transition process from the disturbance generation through the nonlinear breakdown in a holistic manner.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018BoLMe.167..349M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018BoLMe.167..349M"><span>Dispersion of a Passive Scalar Fluctuating Plume in a Turbulent Boundary <span class="hlt">Layer</span>. Part III: Stochastic <span class="hlt">Modelling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marro, Massimo; Salizzoni, Pietro; Soulhac, Lionel; Cassiani, Massimo</p> <p>2018-06-01</p> <p>We analyze the reliability of the Lagrangian stochastic micromixing method in predicting higher-order statistics of the passive scalar concentration induced by an elevated source (of varying diameter) placed in a turbulent boundary <span class="hlt">layer</span>. To that purpose we analyze two different <span class="hlt">modelling</span> approaches by testing their results against the wind-tunnel measurements discussed in Part I (Nironi et al., Boundary-<span class="hlt">Layer</span> Meteorology, 2015, Vol. 156, 415-446). The first is a probability density function (PDF) micromixing <span class="hlt">model</span> that simulates the effects of the molecular diffusivity on the concentration fluctuations by taking into account the background particles. The second is a new <span class="hlt">model</span>, named VPΓ, conceived in order to minimize the computational costs. This is based on the volumetric particle approach providing estimates of the first two concentration moments with no need for the simulation of the background particles. In this second approach, higher-order moments are computed based on the estimates of these two moments and under the assumption that the concentration PDF is a Gamma distribution. The comparisons concern the spatial distribution of the first four moments of the concentration and the <span class="hlt">evolution</span> of the PDF along the plume centreline. The novelty of this work is twofold: (i) we perform a systematic comparison of the results of micro-mixing Lagrangian <span class="hlt">models</span> against experiments providing profiles of the first four moments of the concentration within an inhomogeneous and anisotropic turbulent flow, and (ii) we show the reliability of the VPΓ <span class="hlt">model</span> as an operational tool for the prediction of the PDF of the concentration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018BoLMe.tmp....2M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018BoLMe.tmp....2M"><span>Dispersion of a Passive Scalar Fluctuating Plume in a Turbulent Boundary <span class="hlt">Layer</span>. Part III: Stochastic <span class="hlt">Modelling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Marro, Massimo; Salizzoni, Pietro; Soulhac, Lionel; Cassiani, Massimo</p> <p>2018-01-01</p> <p>We analyze the reliability of the Lagrangian stochastic micromixing method in predicting higher-order statistics of the passive scalar concentration induced by an elevated source (of varying diameter) placed in a turbulent boundary <span class="hlt">layer</span>. To that purpose we analyze two different <span class="hlt">modelling</span> approaches by testing their results against the wind-tunnel measurements discussed in Part I (Nironi et al., Boundary-<span class="hlt">Layer</span> Meteorology, 2015, Vol. 156, 415-446). The first is a probability density function (PDF) micromixing <span class="hlt">model</span> that simulates the effects of the molecular diffusivity on the concentration fluctuations by taking into account the background particles. The second is a new <span class="hlt">model</span>, named VPΓ, conceived in order to minimize the computational costs. This is based on the volumetric particle approach providing estimates of the first two concentration moments with no need for the simulation of the background particles. In this second approach, higher-order moments are computed based on the estimates of these two moments and under the assumption that the concentration PDF is a Gamma distribution. The comparisons concern the spatial distribution of the first four moments of the concentration and the <span class="hlt">evolution</span> of the PDF along the plume centreline. The novelty of this work is twofold: (i) we perform a systematic comparison of the results of micro-mixing Lagrangian <span class="hlt">models</span> against experiments providing profiles of the first four moments of the concentration within an inhomogeneous and anisotropic turbulent flow, and (ii) we show the reliability of the VPΓ <span class="hlt">model</span> as an operational tool for the prediction of the PDF of the concentration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28442318','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28442318"><span>Brownian <span class="hlt">model</span> of transcriptome <span class="hlt">evolution</span> and phylogenetic network visualization between tissues.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gu, Xun; Ruan, Hang; Su, Zhixi; Zou, Yangyun</p> <p>2017-09-01</p> <p>While phylogenetic analysis of transcriptomes of the same tissue is usually congruent with the species tree, the controversy emerges when multiple tissues are included, that is, whether species from the same tissue are clustered together, or different tissues from the same species are clustered together. Recent studies have suggested that phylogenetic network approach may shed some lights on our understanding of multi-tissue transcriptome <span class="hlt">evolution</span>; yet the underlying evolutionary mechanism remains unclear. In this paper we develop a Brownian-based <span class="hlt">model</span> of transcriptome <span class="hlt">evolution</span> under the phylogenetic network that can statistically distinguish between the patterns of species-clustering and tissue-clustering. Our <span class="hlt">model</span> can be used as a null hypothesis (neutral transcriptome <span class="hlt">evolution</span>) for testing any correlation in tissue <span class="hlt">evolution</span>, can be applied to cancer transcriptome <span class="hlt">evolution</span> to study whether two tumors of an individual appeared independently or via metastasis, and can be useful to detect convergent <span class="hlt">evolution</span> at the transcriptional level. Copyright © 2017. Published by Elsevier Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014acm..conf..444R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014acm..conf..444R"><span>A new <span class="hlt">model</span> of physical <span class="hlt">evolution</span> of Jupiter-family comets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rickman, H.; Szutowicz, S.; Wójcikowski, K.</p> <p>2014-07-01</p> <p>We aim to find the statistical physical lifetimes of Jupiter Family comets. For this purpose, we try to <span class="hlt">model</span> the processes that govern the dynamical and physical <span class="hlt">evolution</span> of comets. We pay special attention to physical <span class="hlt">evolution</span>; attempts at such <span class="hlt">modelling</span> have been made before, but we propose a more accurate <span class="hlt">model</span>, which will include more physical effects. The <span class="hlt">model</span> is tested on a sample of fictitious comets based on real Jupiter Family comets with some orbital elements changed to a state before the capture by Jupiter. We <span class="hlt">model</span> four different physical effects: erosion by sublimation, dust mantling, rejuvenation (mantle blow-off), and splitting. While for sublimation and splitting there already are some <span class="hlt">models</span>, like di Sisto et. al. (2009), and we only wish to make them more accurate, dust mantling and rejuvenation have not been included in previous, statistical physical <span class="hlt">evolution</span> <span class="hlt">models</span>. Each of these effects depends on one or more tunable parameters, which we establish by choosing the <span class="hlt">model</span> that best fits the observed comet sample in a way similar to di Sisto et. al. (2009). In contrast to di Sisto et. al., our comparison also involves the observed active fractions vs. nuclear radii.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMNS31A1935S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMNS31A1935S"><span>Inversion of Surface-wave Dispersion Curves due to Low-velocity-<span class="hlt">layer</span> <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shen, C.; Xia, J.; Mi, B.</p> <p>2016-12-01</p> <p>A successful inversion relies on exact forward <span class="hlt">modeling</span> methods. It is a key step to accurately calculate multi-mode dispersion curves of a given <span class="hlt">model</span> in high-frequency surface-wave (Rayleigh wave and Love wave) methods. For normal <span class="hlt">models</span> (shear (S)-wave velocity increasing with depth), their theoretical dispersion curves completely match the dispersion spectrum that is generated based on wave equation. For <span class="hlt">models</span> containing a low-velocity-<span class="hlt">layer</span>, however, phase velocities calculated by existing forward-<span class="hlt">modeling</span> algorithms (e.g. Thomson-Haskell algorithm, Knopoff algorithm, fast vector-transfer algorithm and so on) fail to be consistent with the dispersion spectrum at a high frequency range. They will approach a value that close to the surface-wave velocity of the low-velocity-<span class="hlt">layer</span> under the surface <span class="hlt">layer</span>, rather than that of the surface <span class="hlt">layer</span> when their corresponding wavelengths are short enough. This phenomenon conflicts with the characteristics of surface waves, which results in an erroneous inverted <span class="hlt">model</span>. By comparing the theoretical dispersion curves with simulated dispersion energy, we proposed a direct and essential solution to accurately compute surface-wave phase velocities due to low-velocity-<span class="hlt">layer</span> <span class="hlt">models</span>. Based on the proposed forward <span class="hlt">modeling</span> technique, we can achieve correct inversion for these types of <span class="hlt">models</span>. Several synthetic data proved the effectiveness of our method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940011278','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940011278"><span>Parametric resonant triad interactions in a free shear <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mallier, R.; Maslowe, S. A.</p> <p>1993-01-01</p> <p>We investigate the weakly nonlinear <span class="hlt">evolution</span> of a triad of nearly-neutral modes superimposed on a mixing <span class="hlt">layer</span> with velocity profile u bar equals Um + tanh y. The perturbation consists of a plane wave and a pair of oblique waves each inclined at approximately 60 degrees to the mean flow direction. Because the <span class="hlt">evolution</span> occurs on a relatively fast time scale, the critical <span class="hlt">layer</span> dynamics dominate the process and the amplitude <span class="hlt">evolution</span> of the oblique waves is governed by an integro-differential equation. The long-time solution of this equation predicts very rapid (exponential of an exponential) amplification and we discuss the pertinence of this result to vortex pairing phenomena in mixing <span class="hlt">layers</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Icar..299..133K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Icar..299..133K"><span>Two-phase convection in Ganymede's high-pressure ice <span class="hlt">layer</span> - Implications for its geological <span class="hlt">evolution</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kalousová, Klára; Sotin, Christophe; Choblet, Gaël; Tobie, Gabriel; Grasset, Olivier</p> <p>2018-01-01</p> <p>Ganymede, the largest moon in the solar system, has a fully differentiated interior with a <span class="hlt">layer</span> of high-pressure (HP) ice between its deep ocean and silicate mantle. In this paper, we study the dynamics of this <span class="hlt">layer</span> using a numerical <span class="hlt">model</span> of two-phase ice-water mixture in two-dimensional Cartesian geometry. While focusing on the generation of water at the silicate/HP ice interface and its upward migration towards the ocean, we investigate the effect of bottom heat flux, the <span class="hlt">layer</span> thickness, and the HP ice viscosity and permeability. Our results suggest that melt can be generated at the silicate/HP ice interface for small <span class="hlt">layer</span> thickness ( ≲ 200 km) and high values of heat flux ( ≳ 20 mW m-2) and viscosity ( ≳ 1015 Pa s). Once generated, the water is transported through the <span class="hlt">layer</span> by the upwelling plumes. Depending on the vigor of convection, it stays liquid or it may freeze before melting again as the plume reaches the temperate (partially molten) <span class="hlt">layer</span> at the boundary with the ocean. The thickness of this <span class="hlt">layer</span> as well as the amount of melt that is extracted from it is controlled by the permeability of the HP ice. This process constitutes a means of transporting volatiles and salts that might have dissolved into the melt present at the silicate/HP ice interface. As the moon cools down, the HP ice <span class="hlt">layer</span> becomes less permeable because the heat flux from the silicates decreases and the HP ice <span class="hlt">layer</span> thickens.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950008003','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950008003"><span>Discrete-<span class="hlt">Layer</span> Piezoelectric Plate and Shell <span class="hlt">Models</span> for Active Tip-Clearance Control</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Heyliger, P. R.; Ramirez, G.; Pei, K. C.</p> <p>1994-01-01</p> <p>The objectives of this work were to develop computational tools for the analysis of active-sensory composite structures with added or embedded piezoelectric <span class="hlt">layers</span>. The targeted application for this class of smart composite laminates and the analytical development is the accomplishment of active tip-clearance control in turbomachinery components. Two distinct theories and analytical <span class="hlt">models</span> were developed and explored under this contract: (1) a discrete-<span class="hlt">layer</span> plate theory and corresponding computational <span class="hlt">models</span>, and (2) a three dimensional general discrete-<span class="hlt">layer</span> element generated in curvilinear coordinates for <span class="hlt">modeling</span> laminated composite piezoelectric shells. Both <span class="hlt">models</span> were developed from the complete electromechanical constitutive relations of piezoelectric materials, and incorporate both displacements and potentials as state variables. This report describes the development and results of these <span class="hlt">models</span>. The discrete-<span class="hlt">layer</span> theories imply that the displacement field and electrostatic potential through-the-thickness of the laminate are described over an individual <span class="hlt">layer</span> rather than as a smeared function over the thickness of the entire plate or shell thickness. This is especially crucial for composites with embedded piezoelectric <span class="hlt">layers</span>, as the actuating and sensing elements within these <span class="hlt">layers</span> are poorly represented by effective or smeared properties. Linear Lagrange interpolation polynomials were used to describe the through-thickness laminate behavior. Both analytic and finite element approximations were used in the plane or surface of the structure. In this context, theoretical developments are presented for the discrete-<span class="hlt">layer</span> plate theory, the discrete-<span class="hlt">layer</span> shell theory, and the formulation of an exact solution for simply-supported piezoelectric plates. Finally, evaluations and results from a number of separate examples are presented for the static and dynamic analysis of the plate geometry. Comparisons between the different approaches are provided when</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830058154&hterms=LAYER+LIMIT&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DLAYER%2BLIMIT','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830058154&hterms=LAYER+LIMIT&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3DLAYER%2BLIMIT"><span>An interacting boundary <span class="hlt">layer</span> <span class="hlt">model</span> for cascades</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Davis, R. T.; Rothmayer, A. P.</p> <p>1983-01-01</p> <p>A laminar, incompressible interacting boundary <span class="hlt">layer</span> <span class="hlt">model</span> is developed for two-dimensional cascades. In the limit of large cascade spacing these equations reduce to the interacting boundary <span class="hlt">layer</span> equations for a single body immersed in an infinite stream. A fully implicit numerical method is used to solve the governing equations, and is found to be at least as efficient as the same technique applied to the single body problem. Solutions are then presented for a cascade of finite flat plates and a cascade of finite sine-waves, with cusped leading and trailing edges.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFDA11002C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFDA11002C"><span>The Equivalent Electrokinetic Circuit <span class="hlt">Model</span> of Ion Concentration Polarization <span class="hlt">Layer</span>: Electrical Double <span class="hlt">Layer</span>, Extended Space Charge and Electro-convection</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cho, Inhee; Huh, Keon; Kwak, Rhokyun; Lee, Hyomin; Kim, Sung Jae</p> <p>2016-11-01</p> <p>The first direct chronopotentiometric measurement was provided to distinguish the potential difference through the extended space charge (ESC) <span class="hlt">layer</span> which is formed with the electrical double <span class="hlt">layer</span> (EDL) near a perm-selective membrane. From this experimental result, the linear relationship was obtained between the resistance of ESC and the applied current density. Furthermore, we observed the step-wise distributions of relaxation time at the limiting current regime, confirming the existence of ESC capacitance other than EDL's. In addition, we proposed the equivalent electrokinetic circuit <span class="hlt">model</span> inside ion concentration polarization (ICP) <span class="hlt">layer</span> under rigorous consideration of EDL, ESC and electro-convection (EC). In order to elucidate the voltage configuration in chronopotentiometric measurement, the EC component was considered as the "dependent voltage source" which is serially connected to the ESC <span class="hlt">layer</span>. This <span class="hlt">model</span> successfully described the charging behavior of the ESC <span class="hlt">layer</span> with or without EC, where both cases determined each relaxation time, respectively. Finally, we quantitatively verified their values utilizing the Poisson-Nernst-Planck equations. Therefore, this unified circuit <span class="hlt">model</span> would provide a key insight of ICP system and potential energy-efficient applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007OcMod..19...53A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007OcMod..19...53A"><span>The use of Argo for validation and tuning of mixed <span class="hlt">layer</span> <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Acreman, D. M.; Jeffery, C. D.</p> <p></p> <p>We present results from validation and tuning of 1-D ocean mixed <span class="hlt">layer</span> <span class="hlt">models</span> using data from Argo floats and data from Ocean Weather Station Papa (145°W, 50°N). <span class="hlt">Model</span> tests at Ocean Weather Station Papa showed that a bulk <span class="hlt">model</span> could perform well provided it was tuned correctly. The Large et al. [Large, W.G., McWilliams, J.C., Doney, S.C., 1994. Oceanic vertical mixing: a review and a <span class="hlt">model</span> with a nonlocal boundary <span class="hlt">layer</span> parameterisation. Rev. Geophys. 32 (Novermber), 363-403] K-profile parameterisation (KPP) <span class="hlt">model</span> also gave a good representation of mixed <span class="hlt">layer</span> depth provided the vertical resolution was sufficiently high. <span class="hlt">Model</span> tests using data from a single Argo float indicated a tendency for the KPP <span class="hlt">model</span> to deepen insufficiently over an annual cycle, whereas the tuned bulk <span class="hlt">model</span> and general ocean turbulence <span class="hlt">model</span> (GOTM) gave a better representation of mixed <span class="hlt">layer</span> depth. The bulk <span class="hlt">model</span> was then tuned using data from a sample of Argo floats and a set of optimum parameters was found; these optimum parameters were consistent with the tuning at OWS Papa.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1334121-uncertainties-galactic-chemical-evolution-models','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1334121-uncertainties-galactic-chemical-evolution-models"><span>Uncertainties in Galactic Chemical <span class="hlt">Evolution</span> <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Cote, Benoit; Ritter, Christian; Oshea, Brian W.; ...</p> <p>2016-06-15</p> <p>Here we use a simple one-zone galactic chemical <span class="hlt">evolution</span> <span class="hlt">model</span> to quantify the uncertainties generated by the input parameters in numerical predictions for a galaxy with properties similar to those of the Milky Way. We compiled several studies from the literature to gather the current constraints for our simulations regarding the typical value and uncertainty of the following seven basic parameters: the lower and upper mass limits of the stellar initial mass function (IMF), the slope of the high-mass end of the stellar IMF, the slope of the delay-time distribution function of Type Ia supernovae (SNe Ia), the number ofmore » SNe Ia per M ⊙ formed, the total stellar mass formed, and the final mass of gas. We derived a probability distribution function to express the range of likely values for every parameter, which were then included in a Monte Carlo code to run several hundred simulations with randomly selected input parameters. This approach enables us to analyze the predicted chemical <span class="hlt">evolution</span> of 16 elements in a statistical manner by identifying the most probable solutions along with their 68% and 95% confidence levels. Our results show that the overall uncertainties are shaped by several input parameters that individually contribute at different metallicities, and thus at different galactic ages. The level of uncertainty then depends on the metallicity and is different from one element to another. Among the seven input parameters considered in this work, the slope of the IMF and the number of SNe Ia are currently the two main sources of uncertainty. The thicknesses of the uncertainty bands bounded by the 68% and 95% confidence levels are generally within 0.3 and 0.6 dex, respectively. When looking at the <span class="hlt">evolution</span> of individual elements as a function of galactic age instead of metallicity, those same thicknesses range from 0.1 to 0.6 dex for the 68% confidence levels and from 0.3 to 1.0 dex for the 95% confidence levels. The uncertainty in our chemical</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/2008AIPC.1027..603M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AIPC.1027..603M"><span>A Numerical <span class="hlt">Model</span> of Viscoelastic <span class="hlt">Layer</span> Entrainment by Airflow in Cough</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mitran, Sorin M.</p> <p>2008-07-01</p> <p>Coughing is an alternative mode of ensuring mucus clearance in the lung when normal cilia induced flow breaks down. A numerical <span class="hlt">model</span> of this process is presented with the following aspects. (1) A portion of the airway comprising the first three bronchus generations is <span class="hlt">modeled</span> as radially reinforced elastic tubes. Elasticity equations are solved to predict airway deformation under effect of airway pressure. (2) The compressible, turbulent flow induced by rapid lung contraction is <span class="hlt">modeled</span> by direct numerical simulation for Reynolds numbers in the range 5,000-10,000 and by Large Eddy Simulation for Reynolds numbers in the range 5,000-40,000. (3) A two-<span class="hlt">layer</span> <span class="hlt">model</span> of the airway surface liquid (ASL) covering the airway epithelial <span class="hlt">layer</span> is used. The periciliary liquid (PCL) in direct contact with the epithelial <span class="hlt">layer</span> is considered to be a Newtonian fluid. Forces <span class="hlt">modeling</span> cilia beating can act upon this <span class="hlt">layer</span>. The mucus <span class="hlt">layer</span> between the PCL and the interior airflow is <span class="hlt">modeled</span> as an Oldroyd-B fluid. The overall computation is a fluid-structure interaction simulation that tracks changes in ASL thickness and airway diameters that result from impulsive airflow boundary conditions imposed at bronchi ends. In particular, the amount of mucus that is evacuated from the system is computed as a function of cough intensity and mucus rheological properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22654277-internal-dynamics-twin-layer-solar-prominence','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22654277-internal-dynamics-twin-layer-solar-prominence"><span>INTERNAL DYNAMICS OF A TWIN-<span class="hlt">LAYER</span> SOLAR PROMINENCE</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>Xia, C.; Keppens, R.</p> <p></p> <p>Modern observations revealed rich dynamics within solar prominences. The globally stable quiescent prominences, characterized by the presence of thin vertical threads and falling knobs, are frequently invaded by small rising dark plumes. These dynamic phenomena are related to magnetic Rayleigh–Taylor instability, since prominence matter, 100 times denser than surrounding coronal plasma, is lifted against gravity by weak magnetic field. To get a deeper understanding of the physics behind these phenomena, we use three-dimensional magnetohydrodynamic simulations to investigate the nonlinear magnetoconvective motions in a twin-<span class="hlt">layer</span> prominence in a macroscopic <span class="hlt">model</span> from chromospheric <span class="hlt">layers</span> up to 30 Mm height. The properties ofmore » simulated falling “fingers” and uprising bubbles are consistent with those in observed vertical threads and rising plumes in quiescent prominences. Both sheets of the twin-<span class="hlt">layer</span> prominence show a strongly coherent <span class="hlt">evolution</span> due to their magnetic connectivity, and demonstrate collective kink deformation. Our <span class="hlt">model</span> suggests that the vertical threads of the prominence as seen in an edge-on view, and the apparent horizontal threads of the filament when seen top-down are different appearances of the same structures. Synthetic images of the <span class="hlt">modeled</span> twin-<span class="hlt">layer</span> prominence reflect the strong degree of mixing established over the entire prominence structure, in agreement with the observations.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4571576','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4571576"><span>Probabilistic <span class="hlt">models</span> of eukaryotic <span class="hlt">evolution</span>: time for integration</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lartillot, Nicolas</p> <p>2015-01-01</p> <p>In spite of substantial work and recent progress, a global and fully resolved picture of the macroevolutionary history of eukaryotes is still under construction. This concerns not only the phylogenetic relations among major groups, but also the general characteristics of the underlying macroevolutionary processes, including the patterns of gene family <span class="hlt">evolution</span> associated with endosymbioses, as well as their impact on the sequence evolutionary process. All these questions raise formidable methodological challenges, calling for a more powerful statistical paradigm. In this direction, <span class="hlt">model</span>-based probabilistic approaches have played an increasingly important role. In particular, improved <span class="hlt">models</span> of sequence <span class="hlt">evolution</span> accounting for heterogeneities across sites and across lineages have led to significant, although insufficient, improvement in phylogenetic accuracy. More recently, one main trend has been to move away from simple parametric <span class="hlt">models</span> and stepwise approaches, towards integrative <span class="hlt">models</span> explicitly considering the intricate interplay between multiple levels of macroevolutionary processes. Such integrative <span class="hlt">models</span> are in their infancy, and their application to the phylogeny of eukaryotes still requires substantial improvement of the underlying <span class="hlt">models</span>, as well as additional computational developments. PMID:26323768</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMED41A3429K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMED41A3429K"><span>Size <span class="hlt">Evolution</span> and Stochastic <span class="hlt">Models</span>: Explaining Ostracod Size through Probabilistic Distributions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Krawczyk, M.; Decker, S.; Heim, N. A.; Payne, J.</p> <p>2014-12-01</p> <p>The biovolume of animals has functioned as an important benchmark for measuring <span class="hlt">evolution</span> throughout geologic time. In our project, we examined the observed average body size of ostracods over time in order to understand the mechanism of size <span class="hlt">evolution</span> in these marine organisms. The body size of ostracods has varied since the beginning of the Ordovician, where the first true ostracods appeared. We created a stochastic branching <span class="hlt">model</span> to create possible evolutionary trees of ostracod size. Using stratigraphic ranges for ostracods compiled from over 750 genera in the Treatise on Invertebrate Paleontology, we calculated overall speciation and extinction rates for our <span class="hlt">model</span>. At each timestep in our <span class="hlt">model</span>, new lineages can evolve or existing lineages can become extinct. Newly evolved lineages are assigned sizes based on their parent genera. We parameterized our <span class="hlt">model</span> to generate neutral and directional changes in ostracod size to compare with the observed data. New sizes were chosen via a normal distribution, and the neutral <span class="hlt">model</span> selected new sizes differentials centered on zero, allowing for an equal chance of larger or smaller ostracods at each speciation. Conversely, the directional <span class="hlt">model</span> centered the distribution on a negative value, giving a larger chance of smaller ostracods. Our data strongly suggests that the overall direction of ostracod <span class="hlt">evolution</span> has been following a <span class="hlt">model</span> that directionally pushes mean ostracod size down, shying away from a neutral <span class="hlt">model</span>. Our <span class="hlt">model</span> was able to match the magnitude of size decrease. Our <span class="hlt">models</span> had a constant linear decrease while the actual data had a much more rapid initial rate followed by a constant size. The nuance of the observed trends ultimately suggests a more complex method of size <span class="hlt">evolution</span>. In conclusion, probabilistic methods can provide valuable insight into possible evolutionary mechanisms determining size <span class="hlt">evolution</span> in ostracods.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70018881','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70018881"><span>Chemical and isotopic <span class="hlt">evolution</span> of a <span class="hlt">layered</span> eastern U.S. snowpack and its relation to stream-water composition</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Shanley, J.B.; Kendall, C.; Albert, M.R.; Hardy, J.P.</p> <p>1995-01-01</p> <p>The chemical, isotopic, and morphologic <span class="hlt">evolution</span> of a <span class="hlt">layered</span> snowpack was investigated during the winter of 1993-94 at Sleepers River Research Watershed in Danville, Vermont. The snowpack was monitored at two small basins: a forested basin at 525 m elevation, and an agricultural basin at 292 m elevation. At each site, the snowpack morphology was characterized and individual <span class="hlt">layers</span> were sampled seven times during the season. Nitrate and 8d18O profiles in the snowpack remained relatively stable until peak accumulation in mid-March, except near the snow surface, where rain-on-snow events caused water and nitrate movement down to impeding ice <span class="hlt">layers</span>. Subsequently, water and nitrate moved more readily through the ripening snowpack. As the snowpack evolved, combined processes of preferential ion elution, isotopic fractionation, and infiltration of isotopically heavy rainfall caused the pack to become depleted in solutes and isotopically enriched. The release of nitrate and isotopically depleted water was reflected in patterns of nitrate concentrations and ??18O of meltwater and stream water. Results supported data from the previous year which suggested that streamflow in the forested basin during snowmelt was dominated by groundwater discharge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940008326','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940008326"><span>Turbulence <span class="hlt">modeling</span> of free shear <span class="hlt">layers</span> for high-performance aircraft</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sondak, Douglas L.</p> <p>1993-01-01</p> <p>The High Performance Aircraft (HPA) Grand Challenge of the High Performance Computing and Communications (HPCC) program involves the computation of the flow over a high performance aircraft. A variety of free shear <span class="hlt">layers</span>, including mixing <span class="hlt">layers</span> over cavities, impinging jets, blown flaps, and exhaust plumes, may be encountered in such flowfields. Since these free shear <span class="hlt">layers</span> are usually turbulent, appropriate turbulence <span class="hlt">models</span> must be utilized in computations in order to accurately simulate these flow features. The HPCC program is relying heavily on parallel computers. A Navier-Stokes solver (POVERFLOW) utilizing the Baldwin-Lomax algebraic turbulence <span class="hlt">model</span> was developed and tested on a 128-node Intel iPSC/860. Algebraic turbulence <span class="hlt">models</span> run very fast, and give good results for many flowfields. For complex flowfields such as those mentioned above, however, they are often inadequate. It was therefore deemed that a two-equation turbulence <span class="hlt">model</span> will be required for the HPA computations. The k-epsilon two-equation turbulence <span class="hlt">model</span> was implemented on the Intel iPSC/860. Both the Chien low-Reynolds-number <span class="hlt">model</span> and a generalized wall-function formulation were included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoRL..45.1518L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoRL..45.1518L"><span>Turbidity Currents With Equilibrium Basal Driving <span class="hlt">Layers</span>: A Mechanism for Long Runout</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Luchi, R.; Balachandar, S.; Seminara, G.; Parker, G.</p> <p>2018-02-01</p> <p>Turbidity currents run out over 100 km in lakes and reservoirs, and over 1,000 km in the ocean. They do so without dissipating themselves via excess entrainment of ambient water. Existing <span class="hlt">layer</span>-averaged formulations cannot capture this. We use a numerical <span class="hlt">model</span> to describe the temporal <span class="hlt">evolution</span> of a turbidity current toward steady state under condition of zero net sediment flux at the bed. The flow self-partitions itself into two <span class="hlt">layers</span>. The lower "driving <span class="hlt">layer</span>" approaches an invariant flow thickness, velocity profile, and suspended sediment concentration profile that sequesters nearly all of the suspended sediment. This <span class="hlt">layer</span> can continue indefinitely at steady state over a constant bed slope. The upper "driven <span class="hlt">layer</span>" contains a small fraction of the suspended sediment. The devolution of the flow into these two <span class="hlt">layers</span> likely allows the driving <span class="hlt">layer</span> to run out long distances.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhDT........97H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhDT........97H"><span>Impact of synoptic controls and boundary <span class="hlt">layer</span> processes on ground-level ozone <span class="hlt">evolution</span> at an urban site</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haman, Christine Lanier</p> <p></p> <p>Houston, Texas frequently exceeds the standard for ground-level ozone during the spring and fall. The large commuting population and vast number of industrial sources provide the necessary ingredients for photochemical ozone production in the presence of favorable meteorological conditions. The lack of continuous boundary <span class="hlt">layer</span> (BL) observations prevents a comprehensive understanding of its role in ozone <span class="hlt">evolution</span>. In this study, almost two years of BL observations are utilized to investigate the impacts of synoptic and micrometeorological-scale forcings on ozone. Aerosol gradients derived from ceilometer backscatter retrievals are used to identify the BL and residual <span class="hlt">layers</span> (RL). Overall agreement is found between ceilometer and sonde estimates of the RL and BL heights (BLH), but difficulty detecting the <span class="hlt">layers</span> occurs during cloud periods or immediately following precipitation. Large monthly variability is present in the peak afternoon BLH (e.g. mean August and December peaks are ˜2000 and 1100 m, respectively). Monthly nocturnal BLHs display much smaller differences. The majority of ozone exceedances occur during large-scale subsidence and weak winds in a postfrontal environment. These conditions result in turbulent kinetic energy, mechanical mixing, and ventilation processes that are 2--3 times weaker on exceedance days, which inhibit morning BL growth by an average of ˜100 m·hr-1 compared to low ozone days. The spring has higher nocturnal ozone levels, which is likely attributable to longer day lengths (˜78 minutes), stronger winds (˜0.78 m·s -1), and higher background ozone (˜5 ppbv) compared to the fall. Boundary <span class="hlt">layer</span> entrainment plays an important role in ozone <span class="hlt">evolution</span>. Exceedance days show a characteristic early morning rapid rise of ozone. Vertical ozone profiles indicate the RL ozone peak is ˜60 ppbv on exceedance days, which is ˜25 ppbv (+/- 10 ppbv) greater than low ozone days. The Integrated Profile Mixing (IPM) and Photochemical Budget (PB</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22156977-cosmological-evolution-tachyon-quintom-model-dark-energy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22156977-cosmological-evolution-tachyon-quintom-model-dark-energy"><span>Cosmological <span class="hlt">evolution</span> of a tachyon-quintom <span class="hlt">model</span> of dark energy</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>Shi, Shang-Gang; Piao, Yun-Song; Qiao, Cong-Feng, E-mail: shishanggang06@mails.gucas.ac.cn, E-mail: yspiao@gucas.ac.cn, E-mail: qiaocf@gucas.ac.cn</p> <p>2009-04-15</p> <p>In this work we study the cosmological <span class="hlt">evolution</span> of a dark energy <span class="hlt">model</span> with two scalar fields, i.e. the tachyon and the phantom tachyon. This <span class="hlt">model</span> enables the equation of state w to change from w > -1 to w < -1 in the <span class="hlt">evolution</span> of the universe. The phase-space analysis for such a system with inverse square potentials shows that there exists a unique stable critical point, which has power-law solution. In this paper, we also study another form of tachyon-quintom <span class="hlt">model</span> with two fields, which involves the interactions between both fields.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI33B0402O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI33B0402O"><span>Reconsideration of F-<span class="hlt">layer</span> seismic <span class="hlt">model</span> in the south polar region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ohtaki, T.; Kaneshima, S.</p> <p>2017-12-01</p> <p>Previously, we analyzed the seismic structure near the inner core boundary beneath Antarctica (Ohtaki et al., 2012). In the study, we determined the velocity of the lowermost outer core (F-<span class="hlt">layer</span>) using amplitude ratio observations between the inner-core phase (PKIKP) and the inner-core grazing/diffracted phase (PKPbc/c-diff). Because the observations are not so sensitive to the F-<span class="hlt">layer</span> structure, a constant velocity is assumed in the <span class="hlt">layer</span> to simplify the <span class="hlt">model</span>. The obtained <span class="hlt">model</span> (SPR) has a flat velocity zone with a 75 km thick on the inner core boundary. With this F-<span class="hlt">layer</span> structure and using travel times of these phases as well as the phase that reflects at the boundary, we determined the seismic structure of the inner core in the south polar region. However, a constant velocity <span class="hlt">layer</span> is unrealistic, although it is reasonable assumption.Recently, we determined F-<span class="hlt">layer</span> velocity structures more accurately using the combined observations of PKiKP-PKPbc differential travel times and of PKPbc/c-diff dispersion (Ohtaki et al., 2015, 2016). The former observation is sensitive to average velocity in the F-<span class="hlt">layer</span>; the latter to velocity gradient in the <span class="hlt">layer</span>. By analyzing these two observations together, we can determine the detailed velocity structure in the F-<span class="hlt">layer</span>. The surveyed areas are beneath the Northeast Pacific and Australia. The seismic velocity <span class="hlt">models</span> obtained are quite different between the two regions. Thus our results require laterally heterogeneous F-<span class="hlt">layer</span>, and show that F-<span class="hlt">layer</span> is more complicated than we ever imagined.Then there is one question; which structure is that of the south polar region close to? Unfortunately, the seismic waveforms that we analyzed in the previous study may not have quality high enough to analyze the PKiKP-PKPbc or PKPbc dispersion. However, it would be meaningful to reanalyze the amplitude data and reconsider the F-<span class="hlt">layer</span> velocity there. And we also estimate how large slope of velocity can be acceptable for the F-<span class="hlt">layer</span> velocity</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29068937','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29068937"><span>Three-Dimensional Computer-Assisted Two-<span class="hlt">Layer</span> Elastic <span class="hlt">Models</span> of the Face.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ueda, Koichi; Shigemura, Yuka; Otsuki, Yuki; Fuse, Asuka; Mitsuno, Daisuke</p> <p>2017-11-01</p> <p>To make three-dimensional computer-assisted elastic <span class="hlt">models</span> for the face, we decided on five requirements: (1) an elastic texture like skin and subcutaneous tissue; (2) the ability to take pen marking for incisions; (3) the ability to be cut with a surgical knife; (4) the ability to keep stitches in place for a long time; and (5) a <span class="hlt">layered</span> structure. After testing many elastic solvents, we have made realistic three-dimensional computer-assisted two-<span class="hlt">layer</span> elastic <span class="hlt">models</span> of the face and cleft lip from the computed tomographic and magnetic resonance imaging stereolithographic data. The surface <span class="hlt">layer</span> is made of polyurethane and the inner <span class="hlt">layer</span> is silicone. Using this elastic <span class="hlt">model</span>, we taught residents and young doctors how to make several typical local flaps and to perform cheiloplasty. They could experience realistic simulated surgery and understand three-dimensional movement of the flaps.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26172648','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26172648"><span>Anomalous diffusion in neutral <span class="hlt">evolution</span> of <span class="hlt">model</span> proteins.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nelson, Erik D; Grishin, Nick V</p> <p>2015-06-01</p> <p>Protein <span class="hlt">evolution</span> is frequently explored using minimalist polymer <span class="hlt">models</span>, however, little attention has been given to the problem of structural drift, or diffusion. Here, we study neutral <span class="hlt">evolution</span> of small protein motifs using an off-lattice heteropolymer <span class="hlt">model</span> in which individual monomers interact as low-resolution amino acids. In contrast to most earlier <span class="hlt">models</span>, both the length and folded structure of the polymers are permitted to change. To describe structural change, we compute the mean-square distance (MSD) between monomers in homologous folds separated by n neutral mutations. We find that structural change is episodic, and, averaged over lineages (for example, those extending from a single sequence), exhibits a power-law dependence on n. We show that this exponent depends on the alignment method used, and we analyze the distribution of waiting times between neutral mutations. The latter are more disperse than for <span class="hlt">models</span> required to maintain a specific fold, but exhibit a similar power-law tail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhRvE..91f0701N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhRvE..91f0701N"><span>Anomalous diffusion in neutral <span class="hlt">evolution</span> of <span class="hlt">model</span> proteins</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nelson, Erik D.; Grishin, Nick V.</p> <p>2015-06-01</p> <p>Protein <span class="hlt">evolution</span> is frequently explored using minimalist polymer <span class="hlt">models</span>, however, little attention has been given to the problem of structural drift, or diffusion. Here, we study neutral <span class="hlt">evolution</span> of small protein motifs using an off-lattice heteropolymer <span class="hlt">model</span> in which individual monomers interact as low-resolution amino acids. In contrast to most earlier <span class="hlt">models</span>, both the length and folded structure of the polymers are permitted to change. To describe structural change, we compute the mean-square distance (MSD) between monomers in homologous folds separated by n neutral mutations. We find that structural change is episodic, and, averaged over lineages (for example, those extending from a single sequence), exhibits a power-law dependence on n . We show that this exponent depends on the alignment method used, and we analyze the distribution of waiting times between neutral mutations. The latter are more disperse than for <span class="hlt">models</span> required to maintain a specific fold, but exhibit a similar power-law tail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JPhCS.490a2215I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JPhCS.490a2215I"><span>Differential <span class="hlt">Evolution</span> algorithm applied to FSW <span class="hlt">model</span> calibration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Idagawa, H. S.; Santos, T. F. A.; Ramirez, A. J.</p> <p>2014-03-01</p> <p>Friction Stir Welding (FSW) is a solid state welding process that can be <span class="hlt">modelled</span> using a Computational Fluid Dynamics (CFD) approach. These <span class="hlt">models</span> use adjustable parameters to control the heat transfer and the heat input to the weld. These parameters are used to calibrate the <span class="hlt">model</span> and they are generally determined using the conventional trial and error approach. Since this method is not very efficient, we used the Differential <span class="hlt">Evolution</span> (DE) algorithm to successfully determine these parameters. In order to improve the success rate and to reduce the computational cost of the method, this work studied different characteristics of the DE algorithm, such as the <span class="hlt">evolution</span> strategy, the objective function, the mutation scaling factor and the crossover rate. The DE algorithm was tested using a friction stir weld performed on a UNS S32205 Duplex Stainless Steel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19760038853&hterms=ocean+salinity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Docean%2Bsalinity','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19760038853&hterms=ocean+salinity&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Docean%2Bsalinity"><span>The salinity effect in a mixed <span class="hlt">layer</span> ocean <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Miller, J. R.</p> <p>1976-01-01</p> <p>A <span class="hlt">model</span> of the thermally mixed <span class="hlt">layer</span> in the upper ocean as developed by Kraus and Turner and extended by Denman is further extended to investigate the effects of salinity. In the tropical and subtropical Atlantic Ocean rapid increases in salinity occur at the bottom of a uniformly mixed surface <span class="hlt">layer</span>. The most significant effects produced by the inclusion of salinity are the reduction of the deepening rate and the corresponding change in the heating characteristics of the mixed <span class="hlt">layer</span>. If the net surface heating is positive, but small, salinity effects must be included to determine whether the mixed <span class="hlt">layer</span> temperature will increase or decrease. Precipitation over tropical oceans leads to the development of a shallow stable <span class="hlt">layer</span> accompanied by a decrease in the temperature and salinity at the sea surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhyA..474..380K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhyA..474..380K"><span>A <span class="hlt">model</span> for <span class="hlt">evolution</span> of overlapping community networks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Karan, Rituraj; Biswal, Bibhu</p> <p>2017-05-01</p> <p>A <span class="hlt">model</span> is proposed for the <span class="hlt">evolution</span> of network topology in social networks with overlapping community structure. Starting from an initial community structure that is defined in terms of group affiliations, the <span class="hlt">model</span> postulates that the subsequent growth and loss of connections is similar to the Hebbian learning and unlearning in the brain and is governed by two dominant factors: the strength and frequency of interaction between the members, and the degree of overlap between different communities. The temporal <span class="hlt">evolution</span> from an initial community structure to the current network topology can be described based on these two parameters. It is possible to quantify the growth occurred so far and predict the final stationary state to which the network is likely to evolve. Applications in epidemiology or the spread of email virus in a computer network as well as finding specific target nodes to control it are envisaged. While facing the challenge of collecting and analyzing large-scale time-resolved data on social groups and communities one faces the most basic questions: how do communities evolve in time? This work aims to address this issue by developing a mathematical <span class="hlt">model</span> for the <span class="hlt">evolution</span> of community networks and studying it through computer simulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.9810A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.9810A"><span>Using an atmospheric boundary <span class="hlt">layer</span> <span class="hlt">model</span> to force global ocean <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abel, Rafael; Böning, Claus</p> <p>2014-05-01</p> <p>Current practices in the atmospheric forcing of ocean <span class="hlt">model</span> simulations can lead to unphysical behaviours. The problem lies in the bulk formulation of the turbulent air-sea fluxes in the conjunction with a prescribed, and unresponsive, atmospheric state (as given by reanalysis products). This can have impacts both on mesoscale processes as well as on the dynamics of the large-scale circulation. First, a possible local mismatch between the given atmospheric state and evolving sea surface temperature (SST) signatures can occur, especially for mesoscale features such as frontal areas, eddies, or near the sea ice edge. Any ocean front shift or <span class="hlt">evolution</span> of mesoscale anomalies results in excessive, unrealistic surface fluxes due to the lack of atmospheric adaptation. Second, a subtle distortion in the sensitive balance of feedback processes being critical for the thermohaline circulation. Since the bulk formulations assume an infinite atmospheric heat capacity, resulting SST anomalies are strongly damped even on basin-scales (e.g. from trends in the Atlantic meridional overturning circulation). In consequence, an important negative feedback is eliminated, rendering the system excessively susceptible to small anomalies (or errors) in the freshwater fluxes. Previous studies (Seager et al., 1995, J. Clim.) have suggested a partial forcing issue remedy that aimed for a physically more realistic determination of air-sea fluxes by allowing some (thermodynamic) adaptation of the atmospheric boundary <span class="hlt">layer</span> to SST changes. In this study a modernized formulation of this approach (Deremble et al., 2013, Mon. Weather Rev.; 'CheapAML') is implemented in a global ocean-ice <span class="hlt">model</span> with moderate resolution (0.5°; ORCA05). In a set of experiments we explore the solution behaviour of this forcing approach (where only the winds are prescribed, while atmospheric temperature and humidity are computed), contrasting it with the solution obtained from the classical bulk formulation with a non</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23026724','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23026724"><span>Phenotypic <span class="hlt">models</span> of <span class="hlt">evolution</span> and development: geometry as destiny.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>François, Paul; Siggia, Eric D</p> <p>2012-12-01</p> <p>Quantitative <span class="hlt">models</span> of development that consider all relevant genes typically are difficult to fit to embryonic data alone and have many redundant parameters. Computational <span class="hlt">evolution</span> supplies <span class="hlt">models</span> of phenotype with relatively few variables and parameters that allows the patterning dynamics to be reduced to a geometrical picture for how the state of a cell moves. The clock and wavefront <span class="hlt">model</span>, that defines the phenotype of somitogenesis, can be represented as a sequence of two discrete dynamical transitions (bifurcations). The expression-time to space map for Hox genes and the posterior dominance rule are phenotypes that naturally follow from computational <span class="hlt">evolution</span> without considering the genetics of Hox regulation. Copyright © 2012 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5144128','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5144128"><span>The importance of structural softening for the <span class="hlt">evolution</span> and architecture of passive margins</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Duretz, T.; Petri, B.; Mohn, G.; Schmalholz, S. M.; Schenker, F. L.; Müntener, O.</p> <p>2016-01-01</p> <p>Lithospheric extension can generate passive margins that bound oceans worldwide. Detailed geological and geophysical studies in present and fossil passive margins have highlighted the complexity of their architecture and their multi-stage deformation history. Previous <span class="hlt">modeling</span> studies have shown the significant impact of coarse mechanical <span class="hlt">layering</span> of the lithosphere (2 to 4 <span class="hlt">layer</span> crust and mantle) on passive margin formation. We built upon these studies and design high-resolution (~100–300 m) thermo-mechanical numerical <span class="hlt">models</span> that incorporate finer mechanical <span class="hlt">layering</span> (kilometer scale) mimicking tectonically inherited heterogeneities. During lithospheric extension a variety of extensional structures arises naturally due to (1) structural softening caused by necking of mechanically strong <span class="hlt">layers</span> and (2) the establishment of a network of weak <span class="hlt">layers</span> across the deforming multi-<span class="hlt">layered</span> lithosphere. We argue that structural softening in a multi-<span class="hlt">layered</span> lithosphere is the main cause for the observed multi-stage <span class="hlt">evolution</span> and architecture of magma-poor passive margins. PMID:27929057</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhDT........75F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhDT........75F"><span>Magnetic islands produced by reconnection in large current <span class="hlt">layers</span>: A statistical approach to <span class="hlt">modeling</span> at global scales</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fermo, Raymond Luis Lachica</p> <p>2011-12-01</p> <p>Magnetic reconnection is a process responsible for the conversion of magnetic energy into plasma flows in laboratory, space, and astrophysical plasmas. A product of reconnection, magnetic islands have been observed in long current <span class="hlt">layers</span> for various space plasmas, including the magnetopause, the magnetotail, and the solar corona. In this thesis, a statistical <span class="hlt">model</span> is developed for the dynamics of magnetic islands in very large current <span class="hlt">layers</span>, for which conventional plasma simulations prove inadequate. An island distribution function f characterizes islands by the flux they contain psi and the area they enclose A. An integro-differential <span class="hlt">evolution</span> equation for f describes their creation at small scales, growth due to quasi-steady reconnection, convection along the current sheet, and their coalescence with one another. The steady-state solution of the <span class="hlt">evolution</span> equation predicts a distribution of islands in which the signature of island merging is an asymmetry in psi-- r phase space. A Hall MHD (magnetohydrodynamic) simulation of a very long current sheet with large numbers of magnetic islands is used to explore their dynamics, specifically their growth via two distinct mechanisms: quasi-steady reconnection and merging. The results of the simulation enable validation of the statistical <span class="hlt">model</span> and benchmarking of its parameters. A PIC (particle-in-cell) simulation investigates how secondary islands form in guide field reconnection, revealing that they are born at electron skin depth scales not as islands from the tearing instability but as vortices from a flow instability. A database of 1,098 flux transfer events (FTEs) observed by Cluster between 2001 and 2003 compares favorably with the <span class="hlt">model</span>'s predictions, and also suggests island merging plays a significant role in the magnetopause. Consequently, the magnetopause is likely populated by many FTEs too small to be recognized by spacecraft instrumentation. The results of this research suggest that a complete theory of</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://hdl.handle.net/2060/19920002081','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920002081"><span><span class="hlt">Modeling</span> of the heat transfer in bypass transitional boundary-<span class="hlt">layer</span> flows</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Simon, Frederick F.; Stephens, Craig A.</p> <p>1991-01-01</p> <p>A low Reynolds number k-epsilon turbulence <span class="hlt">model</span> and conditioned momentum, energy and turbulence equations were used to predict bypass transition heat transfer on a flat plate in a high-disturbance environment with zero pressure gradient. The use of conditioned equations was demonstrated to be an improvement over the use of the global-time-averaged equations for the calculation of velocity profiles and turbulence intensity profiles in the transition region of a boundary <span class="hlt">layer</span>. The approach of conditioned equations is extended to include heat transfer and a <span class="hlt">modeling</span> of transition events is used to predict transition onset and the extent of transition on a flat plate. The events, which describe the boundary <span class="hlt">layer</span> at the leading edge, result in boundary-<span class="hlt">layer</span> regions consisting of: (1) the laminar, (2) pseudolaminar, (3) transitional, and (4) turbulent boundary <span class="hlt">layers</span>. The <span class="hlt">modeled</span> transition events were incorporated into the TEXSTAN 2-D boundary-<span class="hlt">layer</span> code which is used to numerically predict the heat transfer. The numerical predictions in general compared well with the experimental data and revealed areas where additional experimental information is needed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1034013','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1034013"><span>Reference <span class="hlt">Models</span> for Multi-<span class="hlt">Layer</span> Tissue Structures</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2016-09-01</p> <p>simulation,  finite   element  analysis 16. SECURITY CLASSIFICATION OF: 17. LIMITATION OF ABSTRACT 18. NUMBER OF PAGES 19a. NAME OF RESPONSIBLE PERSON USAMRMC...Physiologically realistic, fully specimen-specific, nonlinear reference <span class="hlt">models</span>. Tasks. Finite element analysis of non-linear mechanics of cadaver...<span class="hlt">models</span>. Tasks. Finite element analysis of non-linear mechanics of multi-<span class="hlt">layer</span> tissue regions of human subjects. Deliverables. Partially subject- and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1713651Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1713651Z"><span>Nature, theory and <span class="hlt">modelling</span> of geophysical convective planetary boundary <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zilitinkevich, Sergej</p> <p>2015-04-01</p> <p>Geophysical convective planetary boundary <span class="hlt">layers</span> (CPBLs) are still poorly reproduced in oceanographic, hydrological and meteorological <span class="hlt">models</span>. Besides the mean flow and usual shear-generated turbulence, CPBLs involve two types of motion disregarded in conventional theories: 'anarchy turbulence' comprised of the buoyancy-driven plumes, merging to form larger plumes instead of breaking down, as postulated in conventional theory (Zilitinkevich, 1973), large-scale organised structures fed by the potential energy of unstable stratification through inverse energy transfer in convective turbulence (and performing non-local transports irrespective of mean gradients of transporting properties). C-PBLs are strongly mixed and go on growing as long as the boundary <span class="hlt">layer</span> remains unstable. Penetration of the mixed <span class="hlt">layer</span> into the weakly turbulent, stably stratified free flow causes turbulent transports through the CPBL outer boundary. The proposed theory, taking into account the above listed features of CPBL, is based on the following recent developments: prognostic CPBL-depth equation in combination with diagnostic algorithm for turbulence fluxes at the CPBL inner and outer boundaries (Zilitinkevich, 1991, 2012, 2013; Zilitinkevich et al., 2006, 2012), deterministic <span class="hlt">model</span> of self-organised convective structures combined with statistical turbulence-closure <span class="hlt">model</span> of turbulence in the CPBL core (Zilitinkevich, 2013). It is demonstrated that the overall vertical transports are performed mostly by turbulence in the surface <span class="hlt">layer</span> and entrainment <span class="hlt">layer</span> (at the CPBL inner and outer boundaries) and mostly by organised structures in the CPBL core (Hellsten and Zilitinkevich, 2013). Principal difference between structural and turbulent mixing plays an important role in a number of practical problems: transport and dispersion of admixtures, microphysics of fogs and clouds, etc. The surface-<span class="hlt">layer</span> turbulence in atmospheric and marine CPBLs is strongly enhanced by the velocity shears in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JBO....20a7001V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JBO....20a7001V"><span>Objective characterization of bruise <span class="hlt">evolution</span> using photothermal depth profiling and Monte Carlo <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vidovič, Luka; Milanič, Matija; Majaron, Boris</p> <p>2015-01-01</p> <p>Pulsed photothermal radiometry (PPTR) allows noninvasive determination of laser-induced temperature depth profiles in optically scattering <span class="hlt">layered</span> structures. The obtained profiles provide information on spatial distribution of selected chromophores such as melanin and hemoglobin in human skin. We apply the described approach to study time <span class="hlt">evolution</span> of incidental bruises (hematomas) in human subjects. By combining numerical simulations of laser energy deposition in bruised skin with objective fitting of the predicted and measured PPTR signals, we can quantitatively characterize the key processes involved in bruise <span class="hlt">evolution</span> (i.e., hemoglobin mass diffusion and biochemical decomposition). Simultaneous analysis of PPTR signals obtained at various times post injury provides an insight into the variations of these parameters during the bruise healing process. The presented methodology and results advance our understanding of the bruise <span class="hlt">evolution</span> and represent an important step toward development of an objective technique for age determination of traumatic bruises in forensic medicine.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/16875709','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/16875709"><span>A KLM-circuit <span class="hlt">model</span> of a multi-<span class="hlt">layer</span> transducer for acoustic bladder volume measurements.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Merks, E J W; Borsboom, J M G; Bom, N; van der Steen, A F W; de Jong, N</p> <p>2006-12-22</p> <p>In a preceding study a new technique to non-invasively measure the bladder volume on the basis of non-linear wave propagation was validated. It was shown that the harmonic level generated at the posterior bladder wall increases for larger bladder volumes. A dedicated transducer is needed to further verify and implement this approach. This transducer must be capable of both transmission of high-pressure waves at fundamental frequency and reception of up to the third harmonic. For this purpose, a multi-<span class="hlt">layer</span> transducer was constructed using a single element PZT transducer for transmission and a PVDF top-<span class="hlt">layer</span> for reception. To determine feasibility of the multi-<span class="hlt">layer</span> concept for bladder volume measurements, and to ensure optimal performance, an equivalent mathematical <span class="hlt">model</span> on the basis of KLM-circuit <span class="hlt">modeling</span> was generated. This <span class="hlt">model</span> was obtained in two subsequent steps. Firstly, the PZT transducer was <span class="hlt">modeled</span> without PVDF-<span class="hlt">layer</span> attached by means of matching the <span class="hlt">model</span> with the measured electrical input impedance. It was validated using pulse-echo measurements. Secondly, the <span class="hlt">model</span> was extended with the PVDF-<span class="hlt">layer</span>. The total <span class="hlt">model</span> was validated by considering the PVDF-<span class="hlt">layer</span> as a hydrophone on the PZT transducer surface and comparing the measured and simulated PVDF responses on a wave transmitted by the PZT transducer. The obtained results indicated that a valid <span class="hlt">model</span> for the multi-<span class="hlt">layer</span> transducer was constructed. The <span class="hlt">model</span> showed feasibility of the multi-<span class="hlt">layer</span> concept for bladder volume measurements. It also allowed for further optimization with respect to electrical matching and transmit waveform. Additionally, the <span class="hlt">model</span> demonstrated the effect of mechanical loading of the PVDF-<span class="hlt">layer</span> on the PZT transducer.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011GeoRL..38.7604H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011GeoRL..38.7604H"><span>Effects of surface wave breaking on the oceanic boundary <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>He, Hailun; Chen, Dake</p> <p>2011-04-01</p> <p>Existing laboratory studies suggest that surface wave breaking may exert a significant impact on the formation and <span class="hlt">evolution</span> of oceanic surface boundary <span class="hlt">layer</span>, which plays an important role in the ocean-atmosphere coupled system. However, present climate <span class="hlt">models</span> either neglect the effects of wave breaking or treat them implicitly through some crude parameterization. Here we use a one-dimensional ocean <span class="hlt">model</span> (General Ocean Turbulence <span class="hlt">Model</span>, GOTM) to investigate the effects of wave breaking on the oceanic boundary <span class="hlt">layer</span> on diurnal to seasonal time scales. First a set of idealized experiments are carried out to demonstrate the basic physics and the necessity to include wave breaking. Then the <span class="hlt">model</span> is applied to simulating observations at the northern North Sea and the Ocean Weather Station Papa, which shows that properly accounting for wave breaking effects can improve <span class="hlt">model</span> performance and help it to successfully capture the observed upper ocean variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4245229','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4245229"><span><span class="hlt">Modeling</span> Olfactory Bulb <span class="hlt">Evolution</span> through Primate Phylogeny</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Heritage, Steven</p> <p>2014-01-01</p> <p>Adaptive characterizations of primates have usually included a reduction in olfactory sensitivity. However, this inference of derivation and directionality assumes an ancestral state of olfaction, usually by comparison to a group of extant non-primate mammals. Thus, the accuracy of the inference depends on the assumed ancestral state. Here I present a phylogenetic <span class="hlt">model</span> of continuous trait <span class="hlt">evolution</span> that reconstructs olfactory bulb volumes for ancestral nodes of primates and mammal outgroups. Parent-daughter comparisons suggest that, relative to the ancestral euarchontan, the crown-primate node is plesiomorphic and that derived reduction in olfactory sensitivity is an attribute of the haplorhine lineage. The <span class="hlt">model</span> also suggests a derived increase in olfactory sensitivity at the strepsirrhine node. This oppositional diversification of the strepsirrhine and haplorhine lineages from an intermediate and non-derived ancestor is inconsistent with a characterization of graded reduction through primate <span class="hlt">evolution</span>. PMID:25426851</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012CG.....45..293R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012CG.....45..293R"><span>SIGNUM: A Matlab, TIN-based landscape <span class="hlt">evolution</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Refice, A.; Giachetta, E.; Capolongo, D.</p> <p>2012-08-01</p> <p>Several numerical landscape <span class="hlt">evolution</span> <span class="hlt">models</span> (LEMs) have been developed to date, and many are available as open source codes. Most are written in efficient programming languages such as Fortran or C, but often require additional code efforts to plug in to more user-friendly data analysis and/or visualization tools to ease interpretation and scientific insight. In this paper, we present an effort to port a common core of accepted physical principles governing landscape <span class="hlt">evolution</span> directly into a high-level language and data analysis environment such as Matlab. SIGNUM (acronym for Simple Integrated Geomorphological Numerical <span class="hlt">Model</span>) is an independent and self-contained Matlab, TIN-based landscape <span class="hlt">evolution</span> <span class="hlt">model</span>, built to simulate topography development at various space and time scales. SIGNUM is presently capable of simulating hillslope processes such as linear and nonlinear diffusion, fluvial incision into bedrock, spatially varying surface uplift which can be used to simulate changes in base level, thrust and faulting, as well as effects of climate changes. Although based on accepted and well-known processes and algorithms in its present version, it is built with a modular structure, which allows to easily modify and upgrade the simulated physical processes to suite virtually any user needs. The code is conceived as an open-source project, and is thus an ideal tool for both research and didactic purposes, thanks to the high-level nature of the Matlab environment and its popularity among the scientific community. In this paper the simulation code is presented together with some simple examples of surface <span class="hlt">evolution</span>, and guidelines for development of new modules and algorithms are proposed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940016210&hterms=plate+tectonics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dplate%2Btectonics','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940016210&hterms=plate+tectonics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dplate%2Btectonics"><span>Venus magmatic and tectonic <span class="hlt">evolution</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Phillips, R. J.; Hansen, V. L.</p> <p>1993-01-01</p> <p>Two years beyond the initial mapping by the Magellan spacecraft, hypotheses for the magmatic and tectonic <span class="hlt">evolution</span> of Venus have become refined and focused. We present our view of these processes, attempting to synthesize aspects of a <span class="hlt">model</span> for the tectonic and magmatic behavior of the planet. The ideas presented should be taken collectively as an hypothesis subject to further testing. The quintessence of our <span class="hlt">model</span> is that shear and buoyancy forces in the upper boundary <span class="hlt">layer</span> of mantle convection give rise to a spatially and temporally complex pattern of strain in a one-plate Venusian lithosphere and modulate the timing and occurrence of magmatism on a global basis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OcMod.121...90B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OcMod.121...90B"><span>Linear shoaling of free-surface waves in multi-<span class="hlt">layer</span> non-hydrostatic <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bai, Yefei; Cheung, Kwok Fai</p> <p>2018-01-01</p> <p>The capability to describe shoaling over sloping bottom is fundamental to <span class="hlt">modeling</span> of coastal wave transformation. The linear shoaling gradient provides a metric to measure this property in non-hydrostatic <span class="hlt">models</span> with <span class="hlt">layer</span>-integrated formulations. The governing equations in Boussinesq form facilitate derivation of the linear shoaling gradient, which is in the form of a [ 2 P + 2 , 2 P ] expansion of the water depth parameter kd with P equal to 1 for a one-<span class="hlt">layer</span> <span class="hlt">model</span> and (4 N - 4) for an N-<span class="hlt">layer</span> <span class="hlt">model</span>. The expansion reproduces the analytical solution from Airy wave theory at the shallow water limit and maintains a reasonable approximation up to kd = 1.2 and 2 for the one and two-<span class="hlt">layer</span> <span class="hlt">models</span>. Additional <span class="hlt">layers</span> provide rapid and monotonic convergence of the shoaling gradient into deep water. Numerical experiments of wave propagation over a plane slope illustrate manifestation of the shoaling errors through the transformation processes from deep to shallow water. Even though outside the zone of active wave transformation, shoaling errors from deep to intermediate water are cumulative to produce appreciable impact to the wave amplitude in shallow water.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26PSL.482..147K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26PSL.482..147K"><span>The thermal <span class="hlt">evolution</span> of Mercury's Fe-Si core</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Knibbe, Jurriën Sebastiaan; van Westrenen, Wim</p> <p>2018-01-01</p> <p>We have studied the thermal and magnetic field <span class="hlt">evolution</span> of planet Mercury with a core of Fe-Si alloy to assess whether an Fe-Si core matches its present-day partially molten state, Mercury's magnetic field strength, and the observed ancient crustal magnetization. The main advantages of an Fe-Si core, opposed to a previously assumed Fe-S core, are that a Si-bearing core is consistent with the highly reduced nature of Mercury and that no compositional convection is generated upon core solidification, in agreement with magnetic field indications of a stable <span class="hlt">layer</span> at the top of Mercury's core. This study also present the first implementation of a conductive temperature profile in the core where heat fluxes are sub-adiabatic in a global thermal <span class="hlt">evolution</span> <span class="hlt">model</span>. We show that heat migrates from the deep core to the outer part of the core as soon as heat fluxes at the outer core become sub-adiabatic. As a result, the deep core cools throughout Mercury's <span class="hlt">evolution</span> independent of the temperature <span class="hlt">evolution</span> at the core-mantle boundary, causing an early start of inner core solidification and magnetic field generation. The conductive <span class="hlt">layer</span> at the outer core suppresses the rate of core growth after temperature differences between the deep and shallow core are relaxed, such that a magnetic field can be generated until the present. Also, the outer core and mantle operate at higher temperatures than previously thought, which prolongs mantle melting and mantle convection. The results indicate that S is not a necessary ingredient of Mercury's core, bringing bulk compositional <span class="hlt">models</span> of Mercury more in line with reduced meteorite analogues.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920022990','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920022990"><span>Effects of fiber and interfacial <span class="hlt">layer</span> architectures on the thermoplastic response of metal matrix composites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pindera, Marek-Jerzy; Freed, Alan D.; Arnold, Steven M.</p> <p>1992-01-01</p> <p>Examined here is the effect of fiber and interfacial <span class="hlt">layer</span> morphologies on thermal fields in metal matrix composites (MMCs). A micromechanics <span class="hlt">model</span> based on an arbitrarily <span class="hlt">layered</span> concentric cylinder configuration is used to calculate thermal stress fields in MMCs subjected to spatially uniform temperature changes. The fiber is <span class="hlt">modelled</span> as a <span class="hlt">layered</span> material with isotropic or orthotropic elastic <span class="hlt">layers</span>, whereas the surrounding matrix, including interfacial <span class="hlt">layers</span>, is treated as a strain-hardening, elastoplastic, von Mises solid with temperature-dependent parameters. The solution to the boundary-value problem of an arbitrarily <span class="hlt">layered</span> concentric cylinder under the prescribed thermal loading is obtained using the local/global stiffness matrix formulation originally developed for stress analysis of multilayered elastic media. Examples are provided that illustrate how the morphology of the SCS6 silicon carbide fiber and the use of multiple compliant <span class="hlt">layers</span> at the fiber/matrix interface affect the <span class="hlt">evolution</span> of residual stresses in SiC/Ti composites during fabrication cool-down.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=60552&keyword=working+AND+policy&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=60552&keyword=working+AND+policy&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>ON AERODYNAMIC AND BOUNDARY <span class="hlt">LAYER</span> RESISTANCES WITHIN DRY DEPOSITION <span class="hlt">MODELS</span></span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>There have been many empirical parameterizations for the aerodynamic and boundary <span class="hlt">layer</span> resistances proposed in the literature, e.g. those of the Meyers Multi-<span class="hlt">Layer</span> Deposition <span class="hlt">Model</span> (MLM) used with the nation-wide dry deposition network. Many include arbitrary constants or par...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT.......184W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT.......184W"><span>Micromechanics and constitutive <span class="hlt">models</span> for soft active materials with phase <span class="hlt">evolution</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, Binglian</p> <p></p> <p>Soft active materials, such as shape memory polymers, liquid crystal elastomers, soft tissues, gels etc., are materials that can deform largely in response to external stimuli. Micromechanics analysis of heterogeneous materials based on finite element method is a typically numerical way to study the thermal-mechanical behaviors of soft active materials with phase <span class="hlt">evolution</span>. While the constitutive <span class="hlt">models</span> that can precisely describe the stress and strain fields of materials in the process of phase <span class="hlt">evolution</span> can not be found in the databases of some commercial finite element analysis (FEA) tools such as ANSYS or Abaqus, even the specific constitutive behavior for each individual phase either the new formed one or the original one has already been well-known. So developing a computationally efficient and general three dimensional (3D) thermal-mechanical constitutive <span class="hlt">model</span> for soft active materials with phase <span class="hlt">evolution</span> which can be implemented into FEA is eagerly demanded. This paper first solved this problem theoretically by recording the deformation history of each individual phase in the phase <span class="hlt">evolution</span> process, and adopted the idea of effectiveness by regarding all the new formed phase as an effective phase with an effective deformation to make this theory computationally efficient. A user material subroutine (UMAT) code based on this theoretical constitutive <span class="hlt">model</span> has been finished in this work which can be added into the material database in Abaqus or ANSYS and can be easily used for most soft active materials with phase <span class="hlt">evolution</span>. <span class="hlt">Model</span> validation also has been done through comparison between micromechanical FEA and experiments on a particular composite material, shape memory elastomeric composite (SMEC) which consisted of an elastomeric matrix and the crystallizable fibre. Results show that the micromechanics and the constitutive <span class="hlt">models</span> developed in this paper for soft active materials with phase <span class="hlt">evolution</span> are completely relied on.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA563740','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA563740"><span>Linking Dynamics of the Near-surface Flow to Deeper Boundary <span class="hlt">Layer</span> Forcing in the Nocturnal Boundary <span class="hlt">Layer</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2012-06-01</p> <p>Kaimal and Finnigan (1994), modified) Figure 2.2 illustrates the <span class="hlt">evolution</span> from unstable CBL to a nocturnal Stable Bound- ary <span class="hlt">Layer</span> ( SBL ) in the absence...mixed <span class="hlt">layer</span> acts as a cap for the SBL . The SBL persists through the night until sunrise when surface heating resumes and a new unstable <span class="hlt">layer</span> begins...to form at the surface, gradually returning to a CBL. 7 2.2.1 Dynamics of the stable boundary <span class="hlt">layer</span> Because the SBL is stably stratified, buoyancy</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JPCM...26B4109J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JPCM...26B4109J"><span>Dynamics of electrical double <span class="hlt">layer</span> formation in room-temperature ionic liquids under constant-current charging conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jiang, Xikai; Huang, Jingsong; Zhao, Hui; Sumpter, Bobby G.; Qiao, Rui</p> <p>2014-07-01</p> <p>We report detailed simulation results on the formation dynamics of an electrical double <span class="hlt">layer</span> (EDL) inside an electrochemical cell featuring room-temperature ionic liquids (RTILs) enclosed between two planar electrodes. Under relatively small charging currents, the <span class="hlt">evolution</span> of cell potential from molecular dynamics (MD) simulations during charging can be suitably predicted by the Landau-Ginzburg-type continuum <span class="hlt">model</span> proposed recently (Bazant et al 2011 Phys. Rev. Lett. 106 046102). Under very large charging currents, the cell potential from MD simulations shows pronounced oscillation during the initial stage of charging, a feature not captured by the continuum <span class="hlt">model</span>. Such oscillation originates from the sequential growth of the ionic space charge <span class="hlt">layers</span> near the electrode surface. This allows the <span class="hlt">evolution</span> of EDLs in RTILs with time, an atomistic process difficult to visualize experimentally, to be studied by analyzing the cell potential under constant-current charging conditions. While the continuum <span class="hlt">model</span> cannot predict the potential oscillation under such far-from-equilibrium charging conditions, it can nevertheless qualitatively capture the growth of cell potential during the later stage of charging. Improving the continuum <span class="hlt">model</span> by introducing frequency-dependent dielectric constant and density-dependent ion diffusion coefficients may help to further extend the applicability of the <span class="hlt">model</span>. The <span class="hlt">evolution</span> of ion density profiles is also compared between the MD and the continuum <span class="hlt">model</span>, showing good agreement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24919471','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24919471"><span>Dynamics of electrical double <span class="hlt">layer</span> formation in room-temperature ionic liquids under constant-current charging conditions.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jiang, Xikai; Huang, Jingsong; Zhao, Hui; Sumpter, Bobby G; Qiao, Rui</p> <p>2014-07-16</p> <p>We report detailed simulation results on the formation dynamics of an electrical double <span class="hlt">layer</span> (EDL) inside an electrochemical cell featuring room-temperature ionic liquids (RTILs) enclosed between two planar electrodes. Under relatively small charging currents, the <span class="hlt">evolution</span> of cell potential from molecular dynamics (MD) simulations during charging can be suitably predicted by the Landau-Ginzburg-type continuum <span class="hlt">model</span> proposed recently (Bazant et al 2011 Phys. Rev. Lett. 106 046102). Under very large charging currents, the cell potential from MD simulations shows pronounced oscillation during the initial stage of charging, a feature not captured by the continuum <span class="hlt">model</span>. Such oscillation originates from the sequential growth of the ionic space charge <span class="hlt">layers</span> near the electrode surface. This allows the <span class="hlt">evolution</span> of EDLs in RTILs with time, an atomistic process difficult to visualize experimentally, to be studied by analyzing the cell potential under constant-current charging conditions. While the continuum <span class="hlt">model</span> cannot predict the potential oscillation under such far-from-equilibrium charging conditions, it can nevertheless qualitatively capture the growth of cell potential during the later stage of charging. Improving the continuum <span class="hlt">model</span> by introducing frequency-dependent dielectric constant and density-dependent ion diffusion coefficients may help to further extend the applicability of the <span class="hlt">model</span>. The <span class="hlt">evolution</span> of ion density profiles is also compared between the MD and the continuum <span class="hlt">model</span>, showing good agreement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018IAUS..330..331M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018IAUS..330..331M"><span>Stellar Parameters, Chemical composition and <span class="hlt">Models</span> of chemical <span class="hlt">evolution</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mishenina, T.; Pignatari, M.; Côté, B.; Thielemann, F.-K.; Soubiran, C.; Basak, N.; Gorbaneva, T.; Korotin, S. A.; Kovtyukh, V. V.; Wehmeyer, B.; Bisterzo, S.; Travaglio, C.; Gibson, B. K.; Jordan, C.; Paul, A.; Ritter, C.; Herwig, F.</p> <p>2018-04-01</p> <p>We present an in-depth study of metal-poor stars, based high resolution spectra combined with newly released astrometric data from Gaia, with special attention to observational uncertainties. The results are compared to those of other studies, including Gaia benchmark stars. Chemical <span class="hlt">evolution</span> <span class="hlt">models</span> are discussed, highlighting few puzzles that are still affecting our understanding of stellar nucleosynthesis and of the <span class="hlt">evolution</span> of our Galaxy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvF...2j4601Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvF...2j4601Y"><span>Log-<span class="hlt">layer</span> mismatch and <span class="hlt">modeling</span> of the fluctuating wall stress in wall-<span class="hlt">modeled</span> large-eddy simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Xiang I. A.; Park, George Ilhwan; Moin, Parviz</p> <p>2017-10-01</p> <p>Log-<span class="hlt">layer</span> mismatch refers to a chronic problem found in wall-<span class="hlt">modeled</span> large-eddy simulation (WMLES) or detached-eddy simulation, where the <span class="hlt">modeled</span> wall-shear stress deviates from the true one by approximately 15 % . Many efforts have been made to resolve this mismatch. The often-used fixes, which are generally ad hoc, include modifying subgrid-scale stress <span class="hlt">models</span>, adding a stochastic forcing, and moving the LES-wall-<span class="hlt">model</span> matching location away from the wall. An analysis motivated by the integral wall-<span class="hlt">model</span> formalism suggests that log-<span class="hlt">layer</span> mismatch is resolved by the built-in physics-based temporal filtering. In this work we investigate in detail the effects of local filtering on log-<span class="hlt">layer</span> mismatch. We show that both local temporal filtering and local wall-parallel filtering resolve log-<span class="hlt">layer</span> mismatch without moving the LES-wall-<span class="hlt">model</span> matching location away from the wall. Additionally, we look into the momentum balance in the near-wall region to provide an alternative explanation of how LLM occurs, which does not necessarily rely on the numerical-error argument. While filtering resolves log-<span class="hlt">layer</span> mismatch, the quality of the wall-shear stress fluctuations predicted by WMLES does not improve with our remedy. The wall-shear stress fluctuations are highly underpredicted due to the implied use of LES filtering. However, good agreement can be found when the WMLES data are compared to the direct numerical simulation data filtered at the corresponding WMLES resolutions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27779830','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27779830"><span>Construction and histological analysis of a 3D human arterial wall <span class="hlt">model</span> containing vasa vasorum using a <span class="hlt">layer-by-layer</span> technique.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Shima, Fumiaki; Narita, Hirokazu; Hiura, Ayami; Shimoda, Hiroshi; Akashi, Mitsuru</p> <p>2017-03-01</p> <p>There is considerable global demand for three-dimensional (3D) functional tissues which mimic our native organs and tissues for use as in vitro drug screening systems and in regenerative medicine. In particular, there has been an increasing number of patients who suffer from arterial diseases such as arteriosclerosis. As such, in vitro 3D arterial wall <span class="hlt">models</span> that can evaluate the effects of novel medicines and a novel artificial graft for the treatment are required. In our previous study, we reported the rapid construction of 3D tissues by employing a <span class="hlt">layer-by-layer</span> (LbL) technique and revealed their potential applications in the pharmaceutical fields and tissue engineering. In this study, we successfully constructed a 3D arterial wall <span class="hlt">model</span> containing vasa vasorum by employing a LbL technique for the first time. The cells were coated with extracellular matrix nanofilms and seeded into a culture insert using a cell accumulation method. This <span class="hlt">model</span> had a three-<span class="hlt">layered</span> hierarchical structure: a fibroblast <span class="hlt">layer</span>, a smooth muscle <span class="hlt">layer</span>, and an endothelial <span class="hlt">layer</span>, which resembled the native arterial wall. Our method could introduce vasa vasorum into a fibroblast <span class="hlt">layer</span> in vitro and the 3D arterial wall <span class="hlt">model</span> showed barrier function which was evaluated by immunostaining and transendothelial electrical resistance measurement. Furthermore, electron microscopy observations revealed that the vasa vasorum was composed of single-<span class="hlt">layered</span> endothelial cells, and the endothelial tubes were surrounded by the basal lamina, which are known to promote maturation and stabilization in native blood capillaries. These <span class="hlt">models</span> should be useful for tissue engineering, regenerative medicine, and pharmaceutical applications. © 2016 Wiley Periodicals, Inc. J Biomed Mater Res Part A: 105A: 814-823, 2017. © 2016 Wiley Periodicals, Inc.</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/2012EGUGA..1413327S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..1413327S"><span>Wave-induced boundary-<span class="hlt">layer</span> separation: A case study comparing airborne observations and results from a mesoscale <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Strauss, L.; Serafin, S.; Grubišić, V.</p> <p>2012-04-01</p> <p>Wave-induced boundary-<span class="hlt">layer</span> separation (BLS) results from the adverse-pressure gradient forces that are exerted on the atmospheric boundary-<span class="hlt">layer</span> by internal gravity waves in flow over orography. BLS has received significant attention in recent years, particularly so, because it is a key ingredient in the formation of atmospheric rotors. Traditionally depicted as horizontal eddies in the lee of mountain ranges, rotors originate from the interaction between internal gravity waves and the atmospheric boundary-<span class="hlt">layer</span>. Our study focuses on the first observationally documented case of wave-induced BLS, which occurred on 26 Jan 2006 in the lee of the Medicine Bow Mountains in SE Wyoming (USA). Observations from the University of Wyoming King Air (UWKA) aircraft, in particular, the remote sensing measurements with the Wyoming Cloud Radar (WCR), reveal strong wave activity, downslope winds in excess of 30 m/s, and near-surface flow reversal in the lee of the mountain range. The fine resolution of WCR data (on the order of 40x40 m2 for two-dimensional velocity fields) exhibits fine-scale vortical structures ("subrotors") which are embedded within the main rotor zone. Our case study intends to complete the characterisation of the observed boundary-<span class="hlt">layer</span> separation event. <span class="hlt">Modelling</span> of the event with the mesoscale Weather Research and Forecast <span class="hlt">Model</span> (WRF) provides insight into the mesoscale triggers of wave-induced BLS and turbulence generation. Indeed, the mesoscale <span class="hlt">model</span> underpins the expected concurrence of the essential processes (gravity waves, wave breaking, downslope windstorms, etc.) leading to BLS. To exploit the recorded in situ and radar data to their full extent, a quantitative evaluation of the structure and intensity of turbulence is conducted by means of a power spectral analysis of the vertical wind component, measured along the flight track. An intercomparison of observational and <span class="hlt">modelling</span> results serves the purpose of <span class="hlt">model</span> verification and can shed some more</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830033195&hterms=planetary+boundaries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dplanetary%2Bboundaries','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830033195&hterms=planetary+boundaries&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dplanetary%2Bboundaries"><span>Simulation of the planetary boundary <span class="hlt">layer</span> with the UCLA general circulation <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Suarez, M. J.; Arakawa, A.; Randall, D. A.</p> <p>1981-01-01</p> <p>A planetary boundary <span class="hlt">layer</span> (PBL) <span class="hlt">model</span> is presented which employs a mixed <span class="hlt">layer</span> entrainment formulation to describe the mass exchange between the mixed <span class="hlt">layer</span> with the upper, laminar atmosphere. A modified coordinate system couples the mixed <span class="hlt">layer</span> <span class="hlt">model</span> with large scale and sub-grid scale processes of a general circulation <span class="hlt">model</span>. The vertical coordinate is configured as a sigma coordinate with the lower boundary, the top of the PBL, and the prescribed pressure level near the tropopause expressed as coordinate surfaces. The entrainment mass flux is parameterized by assuming the dissipation rate of turbulent kinetic energy to be proportional to the positive part of the generation by convection or mechanical production. The results of a simulation of July are presented for the entire globe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19730046976&hterms=constitution&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dconstitution','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19730046976&hterms=constitution&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dconstitution"><span>Internal constitution and <span class="hlt">evolution</span> of the moon.</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Solomon, S. C.; Toksoz, M. N.</p> <p>1973-01-01</p> <p>The composition, structure and <span class="hlt">evolution</span> of the moon's interior are narrowly constrained by a large assortment of physical and chemical data. <span class="hlt">Models</span> of the thermal <span class="hlt">evolution</span> of the moon that fit the chronology of igneous activity on the lunar surface, the stress history of the lunar lithosphere implied by the presence of mascons, and the surface concentrations of radioactive elements, involve extensive differentiation early in lunar history. This differentiation may be the result of rapid accretion and large-scale melting or of primary chemical <span class="hlt">layering</span> during accretion; differences in present-day temperatures for these two possibilities are significant only in the inner 1000 km of the moon and may not be resolvable.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790025845','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790025845"><span>Electrooptical <span class="hlt">model</span> of the first retina <span class="hlt">layers</span> of a visual analyzer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chibalashvili, Y. L.; Riabinin, A. D.; Svechnikov, S. V.; Chibalashvili, Y. L.; Shkvar, A. M.</p> <p>1979-01-01</p> <p>An electrooptical principle of converting and transmitting optical signals is proposed and used as the basis for constructing a <span class="hlt">model</span> of the upper <span class="hlt">layers</span> of the retina of the visual analyzer of animals. An evaluation of multichannel fibrous optical systems, in which the conversion of optical signals is based on the electrooptical principle, to <span class="hlt">model</span> the upper retina <span class="hlt">layers</span> is presented. The symbolic circuit of the <span class="hlt">model</span> and its algorithm are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016SPIE.9799E..1FO','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016SPIE.9799E..1FO"><span><span class="hlt">Modeling</span> and stabilization results for a charge or current-actuated active constrained <span class="hlt">layer</span> (ACL) beam <span class="hlt">model</span> with the electrostatic assumption</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Özer, Ahmet Özkan</p> <p>2016-04-01</p> <p>An infinite dimensional <span class="hlt">model</span> for a three-<span class="hlt">layer</span> active constrained <span class="hlt">layer</span> (ACL) beam <span class="hlt">model</span>, consisting of a piezoelectric elastic <span class="hlt">layer</span> at the top and an elastic host <span class="hlt">layer</span> at the bottom constraining a viscoelastic <span class="hlt">layer</span> in the middle, is obtained for clamped-free boundary conditions by using a thorough variational approach. The Rao-Nakra thin compliant <span class="hlt">layer</span> approximation is adopted to <span class="hlt">model</span> the sandwich structure, and the electrostatic approach (magnetic effects are ignored) is assumed for the piezoelectric <span class="hlt">layer</span>. Instead of the voltage actuation of the piezoelectric <span class="hlt">layer</span>, the piezoelectric <span class="hlt">layer</span> is proposed to be activated by a charge (or current) source. We show that, the closed-loop system with all mechanical feedback is shown to be uniformly exponentially stable. Our result is the outcome of the compact perturbation argument and a unique continuation result for the spectral problem which relies on the multipliers method. Finally, the <span class="hlt">modeling</span> methodology of the paper is generalized to the multilayer ACL beams, and the uniform exponential stabilizability result is established analogously.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JNuM..438S.484S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JNuM..438S.484S"><span>Implementation of a diffusion convection surface <span class="hlt">evolution</span> <span class="hlt">model</span> in WallDYN</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Schmid, K.</p> <p>2013-07-01</p> <p>In thermonuclear fusion experiments with multiple plasma facing materials the formation of mixed materials is inevitable. The formation of these mixed material <span class="hlt">layers</span> is a dynamic process driven the tight interaction between transport in the plasma scrape off <span class="hlt">layer</span> and erosion/(re-) deposition at the surface. To track this global material erosion/deposition balance and the resulting formation of mixed material <span class="hlt">layers</span> the WallDYN code has been developed which couples surface processes and plasma transport. The current surface <span class="hlt">model</span> in WallDYN cannot fully handle the growth of <span class="hlt">layers</span> nor does it include diffusion. However at elevated temperatures diffusion is a key process in the formation of mixed materials. To remedy this shortcoming a new surface <span class="hlt">model</span> has been developed which, for the first time, describes both <span class="hlt">layer</span> growth/recession and diffusion in a single continuous diffusion/convection equation. The paper will detail the derivation of the new surface <span class="hlt">model</span> and compare it to TRIDYN calculations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000038406&hterms=Tidal+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DTidal%2Bwaves','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000038406&hterms=Tidal+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DTidal%2Bwaves"><span><span class="hlt">Evolution</span> of Nonlinear Internal Waves in China Seas</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Liu, Antony K.; Hsu, Ming-K.; Liang, Nai K.</p> <p>1997-01-01</p> <p>Synthetic Aperture Radar (SAR) images from ERS-I have been used to study the characteristics of internal waves of Taiwan in the East China Sea, and east of Hainan Island in the South China Sea. Rank-ordered packets of internal solitons propagating shoreward from the edge of the continental shelf were observed in the SAR images. Based on the assumption of a semidiurnal tidal origin, the wave speed can be estimated and is consistent with the internal wave theory. By using the SAR images and hydrographic data, internal waves of elevation have been identified in shallow water due to a thicker mixed <span class="hlt">layer</span> as compared with the bottom <span class="hlt">layer</span> on the continental shelf. The generation mechanism includes the influences of the tide and the Kuroshio intrusion across the continental shelf for the formations of elevation internal waves. The effects of water depth on the <span class="hlt">evolution</span> of solitons and wave packets are <span class="hlt">modeled</span> by nonlinear Kortweg-deVries (KdV) type equation and linked to satellite image observations. The numerical calculations of internal wave <span class="hlt">evolution</span> on the continental shelf have been performed and compared with the SAR observations. For a case of depression waves in deep water, the solitons first disintegrate into dispersive wave trains and then evolve to a packet of elevation waves in the shallow water area after they pass through a turning point of approximately equal <span class="hlt">layer</span> depths has been observed in the SAR image and simulated by numerical <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CPL...693...46H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CPL...693...46H"><span>Enhanced activity of CaFeMg <span class="hlt">layered</span> double hydroxides-supported gold nanodendrites for the electrochemical <span class="hlt">evolution</span> of oxygen and hydrogen in alkaline media</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Havakeshian, Elaheh; Salavati, Hossein; Taei, Masoumeh; Hasheminasab, Fatemeh; Seddighi, Mohadeseh</p> <p>2018-02-01</p> <p>In this study, Au was electrodeposited on a support of CaFeMg <span class="hlt">layered</span> double hydroxide and then, its catalytic activity was investigated for oxygen <span class="hlt">evolution</span> reaction (OER) and hydrogen <span class="hlt">evolution</span> reaction (HER). Field emission scanning electron microscopy images showed that a uniform porous film of aggregated nano-particles of the LDH has been decorated with Au nanodendrite-like structures (AuNDs@LDH). The results obtained from polarization curves, Tafel plots and electrochemical impedance spectroscopy showed that the AuNDs@LDH exhibits lower overpotential, higher current density, faster kinetics and enhanced stability for both of the OER and HER, in comparison with the single AuNPs and LDH catalysts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140012663','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140012663"><span>Validation of the Two-<span class="hlt">Layer</span> <span class="hlt">Model</span> for Correcting Clear Sky Reflectance Near Clouds</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wen, Guoyong; Marshak, Alexander; Evans, K. Frank; Vamal, Tamas</p> <p>2014-01-01</p> <p>A two-<span class="hlt">layer</span> <span class="hlt">model</span> was developed in our earlier studies to estimate the clear sky reflectance enhancement near clouds. This simple <span class="hlt">model</span> accounts for the radiative interaction between boundary <span class="hlt">layer</span> clouds and molecular <span class="hlt">layer</span> above, the major contribution to the reflectance enhancement near clouds for short wavelengths. We use LES/SHDOM simulated 3D radiation fields to valid the two-<span class="hlt">layer</span> <span class="hlt">model</span> for reflectance enhancement at 0.47 micrometer. We find: (a) The simple <span class="hlt">model</span> captures the viewing angle dependence of the reflectance enhancement near cloud, suggesting the physics of this <span class="hlt">model</span> is correct; and (b) The magnitude of the 2-<span class="hlt">layer</span> <span class="hlt">modeled</span> enhancement agree reasonably well with the "truth" with some expected underestimation. We further extend our <span class="hlt">model</span> to include cloud-surface interaction using the Poisson <span class="hlt">model</span> for broken clouds. We found that including cloud-surface interaction improves the correction, though it can introduced some over corrections for large cloud albedo, large cloud optical depth, large cloud fraction, large cloud aspect ratio. This over correction can be reduced by excluding scenes (10 km x 10km) with large cloud fraction for which the Poisson <span class="hlt">model</span> is not designed for. Further research is underway to account for the contribution of cloud-aerosol radiative interaction to the enhancement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016DDA....4720301G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016DDA....4720301G"><span><span class="hlt">Modelling</span> <span class="hlt">evolution</span> of asteroid's rotation due to the YORP effect</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Golubov, Oleksiy; Lipatova, Veronika; Scheeres, Daniel J.</p> <p>2016-05-01</p> <p>The Yarkovsky--O'Keefe--Radzievskii--Paddack (or YORP) effect is influence of light pressure on rotation of asteroids. It is the most important factor for <span class="hlt">evolution</span> of rotation state of small asteroids, which can drastically alter their rotation rate and obliquity over cosmologic timescales.In the poster we present our program, which calculates <span class="hlt">evolution</span> of ratation state of small asteroids subject to the YORP effect. The program accounts for both axial and obliquity components of YORP, takes into account the thermal inertia of the asteroid's soil, and the tangential YORP. The axial component of YORP is computed using the <span class="hlt">model</span> by Steinberg and Sari (AJ, 141, 55). The thermal inertia is accounted for in the framework of Golubov et al. 2016 (MNRAS, stw540). Computation of the tangential YORP is based on a siple analytical <span class="hlt">model</span>, whose applicability is verified via comparison to exact numeric simulations.We apply the program to different shape <span class="hlt">models</span> of asteroids, and study coupled <span class="hlt">evolution</span> of their rotation rate and obliquity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26474036','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26474036"><span>Emergence of a Stern <span class="hlt">Layer</span> from the Incorporation of Hydration Interactions into the Gouy-Chapman <span class="hlt">Model</span> of the Electrical Double <span class="hlt">Layer</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Brown, Matthew A; Bossa, Guilherme Volpe; May, Sylvio</p> <p>2015-10-27</p> <p>In one of the most commonly used phenomenological descriptions of the electrical double <span class="hlt">layer</span>, a charged solid surface and a diffuse region of mobile ions are separated from each other by a thin charge-depleted Stern <span class="hlt">layer</span>. The Stern <span class="hlt">layer</span> acts as a capacitor that improves the classical Gouy-Chapman <span class="hlt">model</span> by increasing the magnitude of the surface potential and limiting the maximal counterion concentration. We show that very similar Stern-like properties of the diffuse double <span class="hlt">layer</span> emerge naturally from adding a nonelectrostatic hydration repulsion to the electrostatic Coulomb potential. The interplay of electrostatic attraction and hydration repulsion of the counterions and the surface leads to the formation of a diffuse counterion <span class="hlt">layer</span> that remains well separated from the surface. In addition, hydration repulsions between the ions limit and control the maximal ion concentration and widen the width of the diffuse double <span class="hlt">layer</span>. Our mean-field <span class="hlt">model</span>, which we express in terms of electrostatic and hydration potentials, is physically consistent and conceptually similar to the classical Gouy-Chapman <span class="hlt">model</span>. It allows the incorporation of ion specificity, accounts for hydration properties of charged surfaces, and predicts Stern <span class="hlt">layer</span> properties, which we analyze in terms of the effective size of the hydrated counterions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28565257','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28565257"><span>THE <span class="hlt">EVOLUTION</span> OF CANALIZATION AND THE BREAKING OF VON BAER'S LAWS: <span class="hlt">MODELING</span> THE <span class="hlt">EVOLUTION</span> OF DEVELOPMENT WITH EPISTASIS.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rice, Sean H</p> <p>1998-06-01</p> <p><span class="hlt">Evolution</span> can change the developmental processes underlying a character without changing the average expression of the character itself. This sort of change must occur in both the <span class="hlt">evolution</span> of canalization, in which a character becomes increasingly buffered against genetic or developmental variation, and in the phenomenon of closely related species that show similar adult phenotypes but different underlying developmental patterns. To study such phenomena, I develop a <span class="hlt">model</span> that follows <span class="hlt">evolution</span> on a surface representing adult phenotype as a function of underlying developmental characters. A contour on such a "phenotype landscape" is a set of states of developmental characters that produce the same adult phenotype. Epistasis induces curvature of this surface, and degree of canalization is represented by the slope along a contour. I first discuss the geometric properties of phenotype landscapes, relating epistasis to canalization. I then impose a fitness function on the phenotype and <span class="hlt">model</span> <span class="hlt">evolution</span> of developmental characters as a function of the fitness function and the local geometry of the surface. This <span class="hlt">model</span> shows how canalization evolves as a population approaches an optimum phenotype. It further shows that under some circumstances, "decanalization" can occur, in which the expression of adult phenotype becomes increasingly sensitive to developmental variation. This process can cause very similar populations to diverge from one another developmentally even when their adult phenotypes experience identical selection regimes. © 1998 The Society for the Study of <span class="hlt">Evolution</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21392574-numerical-modeling-coagulation-porosity-evolution-dust-aggregates','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21392574-numerical-modeling-coagulation-porosity-evolution-dust-aggregates"><span>NUMERICAL <span class="hlt">MODELING</span> OF THE COAGULATION AND POROSITY <span class="hlt">EVOLUTION</span> OF DUST AGGREGATES</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>Okuzumi, Satoshi; Sakagami, Masa-aki; Tanaka, Hidekazu, E-mail: satoshi.okuzumi@ax2.ecs.kyoto-u.ac.j</p> <p>2009-12-20</p> <p>Porosity <span class="hlt">evolution</span> of dust aggregates is crucial in understanding dust <span class="hlt">evolution</span> in protoplanetary disks. In this study, we present useful tools to study the coagulation and porosity <span class="hlt">evolution</span> of dust aggregates. First, we present a new numerical method for simulating dust coagulation and porosity <span class="hlt">evolution</span> as an extension of the conventional Smoluchowski equation. This method follows the <span class="hlt">evolution</span> of the mean porosity for each aggregate mass simultaneously with the <span class="hlt">evolution</span> of the mass distribution function. This method reproduces the results of previous Monte Carlo simulations with much less computational expense. Second, we propose a new collision <span class="hlt">model</span> for porous dustmore » aggregates on the basis of our N-body experiments on aggregate collisions. As the first step, we focus on 'hit-and-stick' collisions, which involve neither compression nor fragmentation of aggregates. We first obtain empirical data on porosity changes between the classical limits of ballistic cluster-cluster and particle-cluster aggregation. Using the data, we construct a recipe for the porosity change due to general hit-and-stick collisions as well as formulae for the aerodynamical and collisional cross sections. Our collision <span class="hlt">model</span> is thus more realistic than a previous <span class="hlt">model</span> of Ormel et al. based on the classical aggregation limits only. Simple coagulation simulations using the extended Smoluchowski method show that our collision <span class="hlt">model</span> explains the fractal dimensions of porous aggregates observed in a full N-body simulation and a laboratory experiment. By contrast, similar simulations using the collision <span class="hlt">model</span> of Ormel et al. result in much less porous aggregates, meaning that this <span class="hlt">model</span> underestimates the porosity increase upon unequal-sized collisions. Besides, we discover that aggregates at the high-mass end of the distribution can have a considerably small aerodynamical cross section per unit mass compared with aggregates of lower masses. This occurs when aggregates drift under</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19780036867&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=19780036867&hterms=application+boundary+layer+flat+plate&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3Dapplication%2Bboundary%2Blayer%2Bflat%2Bplate"><span>Thin-<span class="hlt">layer</span> approximation and algebraic <span class="hlt">model</span> for separated turbulent flows</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Baldwin, B.; Lomax, H.</p> <p>1978-01-01</p> <p>An algebraic turbulence <span class="hlt">model</span> for two- and three-dimensional separated flows is specified that avoids the necessity for finding the edge of the boundary <span class="hlt">layer</span>. Properties of the <span class="hlt">model</span> are determined and comparisons made with experiment for an incident shock on a flat plate, separated flow over a compression corner, and transonic flow over an airfoil. Separation and reattachment points from numerical Navier-Stokes solutions agree with experiment within one boundary-<span class="hlt">layer</span> thickness. Use of law-of-the-wall boundary conditions does not alter the predictions significantly. Applications of the <span class="hlt">model</span> to other cases are contained in companion papers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRE..123..131K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRE..123..131K"><span>Timing and Distribution of Single-<span class="hlt">Layered</span> Ejecta Craters Imply Sporadic Preservation of Tropical Subsurface Ice on Mars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kirchoff, Michelle R.; Grimm, Robert E.</p> <p>2018-01-01</p> <p>Determining the <span class="hlt">evolution</span> of tropical subsurface ice is a key component to understanding Mars's climate and geologic history. Study of an intriguing crater type on Mars—<span class="hlt">layered</span> ejecta craters, which likely form by tapping subsurface ice—may provide constraints on this <span class="hlt">evolution</span>. <span class="hlt">Layered</span> ejecta craters have a continuous ejecta deposit with a fluidized-flow appearance. Single-<span class="hlt">layered</span> ejecta (SLE) craters are the most common and dominate at tropical latitudes and therefore offer the best opportunity to derive new constraints on the temporal <span class="hlt">evolution</span> of low-latitude subsurface ice. We estimate <span class="hlt">model</span> formation ages of 54 SLE craters with diameter (<fi>D</fi>) ≥ 5 km using the density of small, superposed craters with <fi>D</fi> < 1 km on their continuous ejecta deposits. These <span class="hlt">model</span> ages indicate that SLE craters have formed throughout the Amazonian and at a similar rate expected for all Martian craters. This suggests that tropical ice has remained at relatively shallow depths at least where these craters formed. In particular, the presence of equatorial SLE craters with <fi>D</fi> 1 km indicates that ice could be preserved as shallow as 100 m or less at those locations. Finally, there is a striking spatial mixing in an area of highlands near the equator of <span class="hlt">layered</span> and radial (lunar-like ballistic) ejecta craters; the latter form where there are insufficient concentrations of subsurface ice. This implies strong spatial heterogeneity in the concentration of tropical subsurface ice.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090015399','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090015399"><span>Compressibility Considerations for kappa-omega Turbulence <span class="hlt">Models</span> in Hypersonic Boundary <span class="hlt">Layer</span> Applications</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rumsey, C. L.</p> <p>2009-01-01</p> <p>The ability of kappa-omega <span class="hlt">models</span> to predict compressible turbulent skin friction in hypersonic boundary <span class="hlt">layers</span> is investigated. Although uncorrected two-equation <span class="hlt">models</span> can agree well with correlations for hot-wall cases, they tend to perform progressively worse - particularly for cold walls - as the Mach number is increased in the hypersonic regime. Simple algebraic <span class="hlt">models</span> such as Baldwin-Lomax perform better compared to experiments and correlations in these circumstances. Many of the compressibility corrections described in the literature are summarized here. These include corrections that have only a small influence for kappa-omega <span class="hlt">models</span>, or that apply only in specific circumstances. The most widely-used general corrections were designed for use with jet or mixing-<span class="hlt">layer</span> free shear flows. A less well-known dilatation-dissipation correction intended for boundary <span class="hlt">layer</span> flows is also tested, and is shown to agree reasonably well with the Baldwin-Lomax <span class="hlt">model</span> at cold-wall conditions. It exhibits a less dramatic influence than the free shear type of correction. There is clearly a need for improved understanding and better overall physical <span class="hlt">modeling</span> for turbulence <span class="hlt">models</span> applied to hypersonic boundary <span class="hlt">layer</span> flows.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980213246','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980213246"><span>A <span class="hlt">Model</span> for the Thermal and Chemical <span class="hlt">Evolution</span> of the Moon's Interior: Implications for the Onset of Mare Volcanism</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hess, Paul C.; Parmentier, E. M.</p> <p>1995-01-01</p> <p>Crystallization of the lunar magma ocean creates a chemically stratified Moon consisting of an anorthositic crust and magma ocean cumulates overlying the primitive lunar interior. Within the magma ocean cumulates the last liquids to crystallize form dense, ilmenite-rich cumulates that contain high concentrations of incompatible radioactive elements. The underlying olivine-orthopyroxene cumulates are also stratified with later crystallized, denser, more Fe-rich compositions at the top. This paper explores the chemical and thermal consequences of an internal <span class="hlt">evolution</span> <span class="hlt">model</span> accounting for the possible role of these sources of chemical buoyancy. Rayleigh-Taylor instability causes the dense ilmenite-rich cumulate <span class="hlt">layer</span> and underlying Fe-rich cumulates to sink toward the center of the Moon, forming a dense lunar core. After this overturn, radioactive heating within the ilmenite-rich cumulate core heats the overlying mantle, causing it to melt. In this <span class="hlt">model</span>, the source region for high-TiO2 mare basalts is a convectively mixed <span class="hlt">layer</span> above the core-mantle boundary which would contain small and variable amounts of admixed ilmenite and KREEP. This deep high-pressure melting, as required for mare basalts, occurs after a reasonable time interval to explain the onset of mare basalt volcanism if the content of radioactive elements in the core and the chemical density gradients above the core are sufficiently high but within a range of values that might have been present in the Moon. Regardless of details implied by particular <span class="hlt">model</span> parameters, gravitational overturn driven by the high density of magma ocean Fe-rich cumulates should concentrate high-TiO2 mare basalt sources, and probably a significant fraction of radioactive heating, toward the center of the Moon. This will have important implications for both the thermal <span class="hlt">evolution</span> of the Moon and for mare basalt genesis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.H32B..02B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.H32B..02B"><span>Diurnal <span class="hlt">Evolution</span> and Annual Variability of Boundary <span class="hlt">Layer</span> Height in the Columbia River Gorge through the `Eye' of Wind Profiling Radars</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bianco, L.; Djalalova, I.; Konopleva-Akish, E.; Kenyon, J.; Olson, J. B.; Wilczak, J. M.</p> <p>2016-12-01</p> <p>The Second Wind Forecast Improvement Project (WFIP2) is a DoE- and NOAA-sponsored program whose goal is to improve the accuracy of numerical weather prediction (NWP) forecasts in complex terrain. WFIP2 consists of an 18-month (October 2015 - March 2017) field campaign held in the Columbia River basin, in the Pacific Northwest of the U.S. As part of WFIP2 a large suite of in-situ and remote sensing instrumentation has been deployed, including, among several others, a network of eight 915-MHz wind profiling radars (WPRs) equipped with radio acoustic sounding systems (RASSs), and many surface meteorological stations. The diurnal <span class="hlt">evolution</span> and annual variability of boundary <span class="hlt">layer</span> height in the area of WFIP2 will be investigated through the `eye' of WPRs, employing state-of-the-art automated algorithms, based on fuzzy logic and artificial intelligence. The results will be used to evaluate possible errors in NWP <span class="hlt">models</span> in this area of complex terrain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/4501113','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/4501113"><span>Nonmathematical <span class="hlt">models</span> for <span class="hlt">evolution</span> of altruism, and for group selection (peck order-territoriality-ant colony-dual-determinant <span class="hlt">model</span>-tri-determinant <span class="hlt">model</span>).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Darlington, P J</p> <p>1972-02-01</p> <p>Mathematical biologists have failed to produce a satisfactory general <span class="hlt">model</span> for <span class="hlt">evolution</span> of altruism, i.e., of behaviors by which "altruists" benefit other individuals but not themselves; kin selection does not seem to be a sufficient explanation of nonreciprocal altruism. Nonmathematical (but mathematically acceptable) <span class="hlt">models</span> are now proposed for <span class="hlt">evolution</span> of negative altruism in dual-determinant and of positive altruism in tri-determinant systems. Peck orders, territorial systems, and an ant society are analyzed as examples. In all <span class="hlt">models</span>, <span class="hlt">evolution</span> is primarily by individual selection, probably supplemented by group selection. Group selection is differential extinction of populations. It can act only on populations preformed by selection at the individual level, but can either cancel individual selective trends (effecting evolutionary homeostasis) or supplement them; its supplementary effect is probably increasingly important in the <span class="hlt">evolution</span> of increasingly organized populations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015DPS....4740406P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015DPS....4740406P"><span>Understanding the Early <span class="hlt">Evolution</span> of M dwarf Extreme Ultraviolet Radiation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peacock, Sarah; Barman, Travis; Shkolnik, Evgenya</p> <p>2015-11-01</p> <p>The chemistry and <span class="hlt">evolution</span> of planetary atmospheres depends on the <span class="hlt">evolution</span> of high-energy radiation emitted by its host star. High levels of extreme ultraviolet (EUV) radiation can drastically alter the atmospheres of terrestrial planets through ionizing, heating, expanding, chemically modifying and eroding them during the first few billion years of a planetary lifetime. While there is evidence that stars emit their highest levels of far and near ultraviolet (FUV; NUV) radiation in the earliest stages of their <span class="hlt">evolution</span>, we are currently unable to directly measure the EUV radiation. Most previous stellar atmosphere <span class="hlt">models</span> under-predict FUV and EUV emission from M dwarfs; here we present new <span class="hlt">models</span> for M stars that include prescriptions for the hot, lowest density atmospheric <span class="hlt">layers</span> (chromosphere, transition region and corona), from which this radiation is emitted. By comparing our <span class="hlt">model</span> spectra to GALEX near and far ultraviolet fluxes, we are able to predict the <span class="hlt">evolution</span> of EUV radiation for M dwarfs from 10 Myr to a few Gyr. This research is the next major step in the HAZMAT (HAbitable Zones and M dwarf Activity across Time) project to analyze how the habitable zone evolves with the evolving properties of stellar and planetary atmospheres.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28943404','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28943404"><span>Rethinking the <span class="hlt">evolution</span> of specialization: A <span class="hlt">model</span> for the <span class="hlt">evolution</span> of phenotypic heterogeneity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rubin, Ilan N; Doebeli, Michael</p> <p>2017-12-21</p> <p>Phenotypic heterogeneity refers to genetically identical individuals that express different phenotypes, even when in the same environment. Traditionally, "bet-hedging" in fluctuating environments is offered as the explanation for the <span class="hlt">evolution</span> of phenotypic heterogeneity. However, there are an increasing number of examples of microbial populations that display phenotypic heterogeneity in stable environments. Here we present an evolutionary <span class="hlt">model</span> of phenotypic heterogeneity of microbial metabolism and a resultant theory for the <span class="hlt">evolution</span> of phenotypic versus genetic specialization. We use two-dimensional adaptive dynamics to track the <span class="hlt">evolution</span> of the population phenotype distribution of the expression of two metabolic processes with a concave trade-off. Rather than assume a Gaussian phenotype distribution, we use a Beta distribution that is capable of describing genotypes that manifest as individuals with two distinct phenotypes. Doing so, we find that environmental variation is not a necessary condition for the <span class="hlt">evolution</span> of phenotypic heterogeneity, which can evolve as a form of specialization in a stable environment. There are two competing pressures driving the <span class="hlt">evolution</span> of specialization: directional selection toward the <span class="hlt">evolution</span> of phenotypic heterogeneity and disruptive selection toward genetically determined specialists. Because of the lack of a singular point in the two-dimensional adaptive dynamics and the fact that directional selection is a first order process, while disruptive selection is of second order, the <span class="hlt">evolution</span> of phenotypic heterogeneity dominates and often precludes speciation. We find that branching, and therefore genetic specialization, occurs mainly under two conditions: the presence of a cost to maintaining a high phenotypic variance or when the effect of mutations is large. A cost to high phenotypic variance dampens the strength of selection toward phenotypic heterogeneity and, when sufficiently large, introduces a singular point into</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910011771','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910011771"><span>Computation of turbulent high speed mixing <span class="hlt">layers</span> using a two-equation turbulence <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Narayan, J. R.; Sekar, B.</p> <p>1991-01-01</p> <p>A two-equation turbulence <span class="hlt">model</span> was extended to be applicable for compressible flows. A compressibility correction based on <span class="hlt">modelling</span> the dilational terms in the Reynolds stress equations were included in the <span class="hlt">model</span>. The <span class="hlt">model</span> is used in conjunction with the SPARK code for the computation of high speed mixing <span class="hlt">layers</span>. The observed trend of decreasing growth rate with increasing convective Mach number in compressible mixing <span class="hlt">layers</span> is well predicted by the <span class="hlt">model</span>. The predictions agree well with the experimental data and the results from a compressible Reynolds stress <span class="hlt">model</span>. The present <span class="hlt">model</span> appears to be well suited for the study of compressible free shear flows. Preliminary results obtained for the reacting mixing <span class="hlt">layers</span> are included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002EM%26P...90..489K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002EM%26P...90..489K"><span><span class="hlt">Modeling</span> of the Orbital <span class="hlt">Evolution</span> of 2060 Chiron</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kovalenko, Nataliya S.; Babenko, Yury G.; Churyumov, Klim I.</p> <p>2002-03-01</p> <p>The origin of Centaurs is one of the most interesting problems of Solar system science, and it has not yet been solved. To shed light on this problem one can investigate Centaurs' past and future orbital <span class="hlt">evolution</span>. In this paper we discuss the results of Chiron's orbital <span class="hlt">evolution</span> <span class="hlt">modeling</span>. It was the first discovered Centaur and is the brightest one. Numerical integration was produced for 1 Myr forward and backward from the present time. A program based on the Everhart single sequence method for integrating orbits was used.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940028699','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940028699"><span>A <span class="hlt">model</span> for the <span class="hlt">evolution</span> of CO2 on Mars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Haberle, Robert M.; Tyler, D.; Mckay, C. P.; Davis, W. L.</p> <p>1993-01-01</p> <p>Our MSATT work has focused on the <span class="hlt">evolution</span> of CO2 on Mars. We have constructed a <span class="hlt">model</span> that predicts the <span class="hlt">evolution</span> of CO2 on Mars from a specified initial amount at the end of the heavy bombardment to the present. The <span class="hlt">model</span> draws on published estimates of the main process believed to affect the fate of CO2 during this period: chemical weathering, regolith uptake, polar cap formation, and atmospheric escape. Except for escape, the rate at which these processes act is controlled by surface temperatures that we calculate using a modified version of the Gierasch and Toon energy balance <span class="hlt">model</span>. Various aspects of this work are covered.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRC..122.5075P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRC..122.5075P"><span>Turbulent entrainment in a strongly stratified barrier <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pham, H. T.; Sarkar, S.</p> <p>2017-06-01</p> <p>Large-eddy simulation (LES) is used to investigate how turbulence in the wind-driven ocean mixed <span class="hlt">layer</span> erodes the stratification of barrier <span class="hlt">layers</span>. The <span class="hlt">model</span> consists of a stratified Ekman <span class="hlt">layer</span> that is driven by a surface wind. Simulations at a wide range of N0/f are performed to quantify the effect of turbulence and stratification on the entrainment rate. Here, N0 is the buoyancy frequency in the barrier <span class="hlt">layer</span> and f is the Coriolis parameter. The <span class="hlt">evolution</span> of the mixed <span class="hlt">layer</span> follows two stages: a rapid initial deepening and a late-time growth at a considerably slower rate. During the first stage, the mixed <span class="hlt">layer</span> thickens to the depth that is proportional to u∗/<msqrt>fN0</msqrt> where u∗ is the frictional velocity. During the second stage, the turbulence in the mixed <span class="hlt">layer</span> continues to deepen further into the barrier <span class="hlt">layer</span>, and the turbulent length scale is shown to scale with u∗/N0, independent of f. The late-time entrainment rate E follows the law of E=0.035Ri∗-1/2 where Ri∗ is the Richardson number. The exponent of -1/2 is identical but the coefficient of 0.035 is much smaller relative to the value of 2-3/2 for the nonrotating boundary <span class="hlt">layer</span>. Simulations using the KPP <span class="hlt">model</span> (version applicable to this simple case without additional effects of Langmuir turbulence or surface buoyancy flux) also yield the entrainment scaling of E∝Ri∗-1/2; however, the proportionality coefficient varies with the stratification. The structure of the Ekman current is examined to illustrate the strong effect of stratification in the limit of large N0/f.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001AGUFM.H21C0330A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001AGUFM.H21C0330A"><span>Coupling of a Simple 3-<span class="hlt">Layer</span> Snow <span class="hlt">Model</span> to GISS GCM</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aleinov, I.</p> <p>2001-12-01</p> <p>Appropriate simulation of the snow cover dynamics is an important issue for the General Circulation <span class="hlt">Models</span> (GCMs). The presence of snow has a significant impact on ground albedo and on heat and moisture balance. A 3-<span class="hlt">layer</span> snow <span class="hlt">model</span> similar to the one proposed by Lynch-Stieglitz was developed with the purpose of using it inside the GCM developed in the NASA Goddard Institute for Space Studies (GISS). The water transport between the <span class="hlt">layers</span> is <span class="hlt">modeled</span> explicitly while the heat balance is computed implicitly between the snow <span class="hlt">layers</span> and semi-implicitly on the surface. The processes of melting and refreezing and compactification of <span class="hlt">layers</span> under the gravitational force are <span class="hlt">modeled</span> appropriately. It was noticed that implicit computation of the heat transport can cause a significant under- or over-estimation of the incoming heat flux when the temperature of the upper snow <span class="hlt">layer</span> is equal to 0 C. This may lead in particular to delayed snow melting in spring. To remedy this problem a special flux-control algorithm was added to the <span class="hlt">model</span>, which checks computed flux for possible errors and if such are detected the heat transport is recomputed again with the appropriate corrections. The <span class="hlt">model</span> was tested off-line with Sleepers River forcing data and exhibited a good agreement between simulated and observed quantities for snow depth, snow density and snow temperature. The <span class="hlt">model</span> was then incorporated into the GISS GCM. Inside the GCM the <span class="hlt">model</span> is driven completely by the data simulated by other parts of the GCM. The screening effect of the vegetation is introduced by means of masking depth. For a thin snowpack a fractional cover is implemented so that the total thickness of the the snow is never less then 10 cm (rather, the areal fraction of the snow cover decreases when it melts). The <span class="hlt">model</span> was tested with 6 year long GCM speed-up runs. It proved to be stable and produced reasonable results for the global snow cover. In comparison to the old GISS GCM snow <span class="hlt">model</span> (which was</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JHyd..551..328D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JHyd..551..328D"><span>Quantification of the specific yield in a two-<span class="hlt">layer</span> hard-rock aquifer <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Durand, Véronique; Léonardi, Véronique; de Marsily, Ghislain; Lachassagne, Patrick</p> <p>2017-08-01</p> <p>Hard rock aquifers (HRA) have long been considered to be two-<span class="hlt">layer</span> systems, with a mostly capacitive <span class="hlt">layer</span> just below the surface, the saprolite <span class="hlt">layer</span>, and a mainly transmissive <span class="hlt">layer</span> underneath, the fractured <span class="hlt">layer</span>. Although this hydrogeological conceptual <span class="hlt">model</span> is widely accepted today within the scientific community, it is difficult to quantify the respective storage properties of each <span class="hlt">layer</span> with an equivalent porous medium <span class="hlt">model</span>. Based on an HRA field site, this paper attempts to quantify in a distinct manner the respective values of the specific yield (Sy) in the saprolite and the fractured <span class="hlt">layer</span>, with the help of a deterministic hydrogeological <span class="hlt">model</span>. The study site is the Plancoët migmatitic aquifer located in north-western Brittany, France, with piezometric data from 36 observation wells surveyed every two weeks for eight years. Whereas most of the piezometers (26) are located where the water table lies within the saprolite, thus representing the specific yield of the unconfined <span class="hlt">layer</span> (Sy1), 10 of them are representative of the unconfined fractured <span class="hlt">layer</span> (Sy2), due to their position where the saprolite is eroded or unsaturated. The two-<span class="hlt">layer</span> <span class="hlt">model</span>, based on field observations of the <span class="hlt">layer</span> geometry, runs with the MODFLOW code. 81 values of the Sy1/Sy2 parameter sets were tested manually, as an inverse calibration was not able to calibrate these parameters. In order to calibrate the storage properties, a new quality-of-fit criterion called ;AdVar; was also developed, equal to the mean squared deviation of the seasonal piezometric amplitude variation. Contrary to the variance, AdVar is able to select the best values for the specific yield in each <span class="hlt">layer</span>. It is demonstrated that the saprolite <span class="hlt">layer</span> is about 2.5 times more capacitive than the fractured <span class="hlt">layer</span>, with Sy1 = 10% (7% < Sy1 < 15%) against Sy2 = 2% (1% < Sy2 < 3%), in this particular example.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120015711','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120015711"><span>Enthalpy-Based Thermal <span class="hlt">Evolution</span> of Loops: III. Comparison of Zero-Dimensional <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cargill, P. J.; Bradshaw, Stephen J.; Klimchuk, James A.</p> <p>2012-01-01</p> <p>Zero dimensional (0D) hydrodynamic <span class="hlt">models</span>, provide a simple and quick way to study the thermal <span class="hlt">evolution</span> of coronal loops subjected to time-dependent heating. This paper presents a comparison of a number of 0D <span class="hlt">models</span> that have been published in the past and is intended to provide a guide for those interested in either using the old <span class="hlt">models</span> or developing new ones. The principal difference between the <span class="hlt">models</span> is the way the exchange of mass and energy between corona, transition region and chromosphere is treated, as plasma cycles into and out of a loop during a heating-cooling cycle. It is shown that <span class="hlt">models</span> based on the principles of mass and energy conservation can give satisfactory results at some, or, in the case of the Enthalpy Based Thermal <span class="hlt">Evolution</span> of Loops (EBTEL) <span class="hlt">model</span>, all stages of the loop <span class="hlt">evolution</span>. Empirical <span class="hlt">models</span> can lead to low coronal densities, spurious delays between the peak density and temperature, and, for short heating pulses, overly short loop lifetimes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JPhCS.269a2016P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JPhCS.269a2016P"><span><span class="hlt">Modelling</span> the backscatter from spherical cavities in a solid matrix: Can an effective medium <span class="hlt">layer</span> <span class="hlt">model</span> mimic the scattering response?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pinfield, Valerie J.; Challis, Richard E.</p> <p>2011-01-01</p> <p>Industrial applications are increasingly turning to modern composite <span class="hlt">layered</span> materials to satisfy strength requirements whilst reducing component weight. An important group of such materials are fibre/resin composites in which long fibres are laid down in <span class="hlt">layers</span> in a resin matrix. Whilst delamination flaws, where <span class="hlt">layers</span> separate from each other, are detectable using traditional ultrasonic techniques, the presence of porosity in any particular <span class="hlt">layer</span> is harder to detect. The reflected signal from a <span class="hlt">layered</span> material can already be <span class="hlt">modelled</span> successfully by using the acoustic impedance of the <span class="hlt">layers</span> and summing reflections from <span class="hlt">layer</span> boundaries. However, it is not yet known how to incorporate porosity into such a <span class="hlt">model</span>. The aim of the work reported here was to <span class="hlt">model</span> the backscatter from randomly distributed spherical cavities within one <span class="hlt">layer</span>, and to establish whether an effective medium, with a derived acoustic impedance, could reproduce the characteristics of that scattering. Since effective medium <span class="hlt">models</span> are much more readily implemented in simulations of multi-<span class="hlt">layer</span> structures than scattering per se, it was felt desirable to simplify the scattering response into an effective medium representation. A <span class="hlt">model</span> was constructed in which spherical cavities were placed randomly in a solid continuous matrix and the system backscattering response was calculated. The scattering from the cavities was determined by using the Rayleigh partial-wave method, and taking the received signal at the transducer to be equivalent to the far field limit. It was concluded that even at relatively low porosity levels, the received signal was still "<span class="hlt">layer</span>-like" and an effective medium <span class="hlt">model</span> was a good approximation for the scattering behaviour.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://files.eric.ed.gov/fulltext/EJ1126661.pdf','ERIC'); return false;" href="http://files.eric.ed.gov/fulltext/EJ1126661.pdf"><span>Knowledge Growth: Applied <span class="hlt">Models</span> of General and Individual Knowledge <span class="hlt">Evolution</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>Silkina, Galina Iu.; Bakanova, Svetlana A.</p> <p>2016-01-01</p> <p>The article considers the mathematical <span class="hlt">models</span> of the growth and accumulation of scientific and applied knowledge since it is seen as the main potential and key competence of modern companies. The problem is examined on two levels--the growth and <span class="hlt">evolution</span> of objective knowledge and knowledge <span class="hlt">evolution</span> of a particular individual. Both processes are…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Icar..277..215N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Icar..277..215N"><span>Water-rich planets: How habitable is a water <span class="hlt">layer</span> deeper than on Earth?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Noack, L.; Höning, D.; Rivoldini, A.; Heistracher, C.; Zimov, N.; Journaux, B.; Lammer, H.; Van Hoolst, T.; Bredehöft, J. H.</p> <p>2016-10-01</p> <p>Water is necessary for the origin and survival of life as we know it. In the search for life-friendly worlds, water-rich planets therefore are obvious candidates and have attracted increasing attention in recent years. The surface H2O <span class="hlt">layer</span> on such planets (containing a liquid water ocean and possibly high-pressure ice below a specific depth) could potentially be hundreds of kilometres deep depending on the water content and the <span class="hlt">evolution</span> of the proto-atmosphere. We study possible constraints for the habitability of deep water <span class="hlt">layers</span> and introduce a new habitability classification relevant for water-rich planets (from Mars-size to super-Earth-size planets). A new ocean <span class="hlt">model</span> has been developed that is coupled to a thermal <span class="hlt">evolution</span> <span class="hlt">model</span> of the mantle and core. Our interior structure <span class="hlt">model</span> takes into account depth-dependent thermodynamic properties and the possible formation of high-pressure ice. We find that heat flowing out of the silicate mantle can melt an ice <span class="hlt">layer</span> from below (in some cases episodically), depending mainly on the thickness of the ocean-ice shell, the mass of the planet, the surface temperature and the interior parameters (e.g. radioactive mantle heat sources). The high pressure at the bottom of deep water-ice <span class="hlt">layers</span> could also impede volcanism at the water-mantle boundary for both stagnant lid and plate tectonics silicate shells. We conclude that water-rich planets with a deep ocean, a large planet mass, a high average density or a low surface temperature are likely less habitable than planets with an Earth-like ocean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1985BoLMe..32..307G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1985BoLMe..32..307G"><span>The inland boundary <span class="hlt">layer</span> at low latitudes</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>1985-08-01</p> <p>Observations from the Koorin boundary-<span class="hlt">layer</span> experiment in Australia (latitude 16 °S) were analysed in a study of the nocturnal jet development. For geostrophic winds in the range 10 20 m s-1, ageostrophic wind magnitudes of 5 10m s-1 were common above the surface <span class="hlt">layer</span> near sunset, with cross-isobar flow angles of about 40 °. The jet that then developed by midnight was probably the result of these large ageostrophic winds, strong surface cooling and favourable baroclinity and sloping terrain. The analysis is supported by numerical <span class="hlt">model</span> calculations with special emphasis on the role of long-wave radiative cooling on turbulent decay. Decay is rapid in the presence of radiation, although there is little influence on stress divergence levels. Evidence of sea-breeze influences on the jet <span class="hlt">evolution</span>, and on features of deeply penetrating sea breezes in general, will be presented and discussed in part 2 of this study (submitted to Boundary-<span class="hlt">Layer</span> Meteorol.).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT........57Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT........57Z"><span>Multi-Scale <span class="hlt">Modeling</span> of Microstructural <span class="hlt">Evolution</span> in Structural Metallic Systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Lei</p> <p></p> <p>Metallic alloys are a widely used class of structural materials, and the mechanical properties of these alloys are strongly dependent on the microstructure. Therefore, the scientific design of metallic materials with superior mechanical properties requires the understanding of the microstructural <span class="hlt">evolution</span>. Computational <span class="hlt">models</span> and simulations offer a number of advantages over experimental techniques in the prediction of microstructural <span class="hlt">evolution</span>, because they can allow studies of microstructural <span class="hlt">evolution</span> in situ, i.e., while the material is mechanically loaded (meso-scale simulations), and bring atomic-level insights into the microstructure (atomistic simulations). In this thesis, we applied a multi-scale <span class="hlt">modeling</span> approach to study the microstructural <span class="hlt">evolution</span> in several metallic systems, including polycrystalline materials and metallic glasses (MGs). Specifically, for polycrystalline materials, we developed a coupled finite element <span class="hlt">model</span> that combines phase field method and crystal plasticity theory to study the plasticity effect on grain boundary (GB) migration. Our <span class="hlt">model</span> is not only coupled strongly (i.e., we include plastic driving force on GB migration directly) and concurrently (i.e., coupled equations are solved simultaneously), but also it qualitatively captures such phenomena as the dislocation absorption by mobile GBs. The developed <span class="hlt">model</span> provides a tool to study the microstructural <span class="hlt">evolution</span> in plastically deformed metals and alloys. For MGs, we used molecular dynamics (MD) simulations to investigate the nucleation kinetics in the primary crystallization in Al-Sm system. We calculated the time-temperature-transformation curves for low Sm concentrations, from which the strong suppressing effect of Sm solute on Al nucleation and its influencing mechanism are revealed. Also, through the comparative analysis of both Al attachment and Al diffusion in MGs, it has been found that the nucleation kinetics is controlled by interfacial attachment of Al, and that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3477701','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3477701"><span>Finite element <span class="hlt">modeling</span> of mitral leaflet tissue using a <span class="hlt">layered</span> shell approximation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Ratcliffe, Mark B.; Guccione, Julius M.</p> <p>2012-01-01</p> <p>The current study presents a finite element <span class="hlt">model</span> of mitral leaflet tissue, which incorporates the anisotropic material response and approximates the <span class="hlt">layered</span> structure. First, continuum mechanics and the theory of <span class="hlt">layered</span> composites are used to develop an analytical representation of membrane stress in the leaflet material. This is done with an existing anisotropic constitutive law from literature. Then, the concept is implemented in a finite element (FE) <span class="hlt">model</span> by overlapping and merging two <span class="hlt">layers</span> of transversely isotropic membrane elements in LS-DYNA, which homogenizes the response. The FE <span class="hlt">model</span> is then used to simulate various biaxial extension tests and out-of-plane pressure loading. Both the analytical and FE <span class="hlt">model</span> show good agreement with experimental biaxial extension data, and show good mutual agreement. This confirms that the <span class="hlt">layered</span> composite approximation presented in the current study is able to capture the exponential stiffening seen in both the circumferential and radial directions of mitral leaflets. PMID:22971896</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1184842','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1184842"><span>Misfit <span class="hlt">layer</span> compounds and ferecrystals: <span class="hlt">Model</span> systems for thermoelectric nanocomposites</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>Merrill, Devin R.; Moore, Daniel B.; Bauers, Sage R.</p> <p></p> <p>A basic summary of thermoelectric principles is presented in a historical context, following the <span class="hlt">evolution</span> of the field from initial discovery to modern day high-zT materials. A specific focus is placed on nanocomposite materials as a means to solve the challenges presented by the contradictory material requirements necessary for efficient thermal energy harvest. Misfit <span class="hlt">layer</span> compounds are highlighted as an example of a highly ordered anisotropic nanocomposite system. Their <span class="hlt">layered</span> structure provides the opportunity to use multiple constituents for improved thermoelectric performance, through both enhanced phonon scattering at interfaces and through electronic interactions between the constituents. Recently, a class ofmore » metastable, turbostratically-disordered misfit <span class="hlt">layer</span> compounds has been synthesized using a kinetically controlled approach with low reaction temperatures. The kinetically stabilized structures can be prepared with a variety of constituent ratios and <span class="hlt">layering</span> schemes, providing an avenue to systematically understand structure-function relationships not possible in the thermodynamic compounds. We summarize the work that has been done to date on these materials. The observed turbostratic disorder has been shown to result in extremely low cross plane thermal conductivity and in plane thermal conductivities that are also very small, suggesting the structural motif could be attractive as thermoelectric materials if the power factor could be improved. The first 10 compounds in the [(PbSe) 1+δ] m(TiSe₂) n family (m, n ≤ 3) are reported as a case study. As n increases, the magnitude of the Seebeck coefficient is significantly increased without a simultaneous decrease in the in-plane electrical conductivity, resulting in an improved thermoelectric power factor.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1184842-misfit-layer-compounds-ferecrystals-model-systems-thermoelectric-nanocomposites','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1184842-misfit-layer-compounds-ferecrystals-model-systems-thermoelectric-nanocomposites"><span>Misfit <span class="hlt">layer</span> compounds and ferecrystals: <span class="hlt">Model</span> systems for thermoelectric nanocomposites</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Merrill, Devin R.; Moore, Daniel B.; Bauers, Sage R.; ...</p> <p>2015-04-22</p> <p>A basic summary of thermoelectric principles is presented in a historical context, following the <span class="hlt">evolution</span> of the field from initial discovery to modern day high-zT materials. A specific focus is placed on nanocomposite materials as a means to solve the challenges presented by the contradictory material requirements necessary for efficient thermal energy harvest. Misfit <span class="hlt">layer</span> compounds are highlighted as an example of a highly ordered anisotropic nanocomposite system. Their <span class="hlt">layered</span> structure provides the opportunity to use multiple constituents for improved thermoelectric performance, through both enhanced phonon scattering at interfaces and through electronic interactions between the constituents. Recently, a class ofmore » metastable, turbostratically-disordered misfit <span class="hlt">layer</span> compounds has been synthesized using a kinetically controlled approach with low reaction temperatures. The kinetically stabilized structures can be prepared with a variety of constituent ratios and <span class="hlt">layering</span> schemes, providing an avenue to systematically understand structure-function relationships not possible in the thermodynamic compounds. We summarize the work that has been done to date on these materials. The observed turbostratic disorder has been shown to result in extremely low cross plane thermal conductivity and in plane thermal conductivities that are also very small, suggesting the structural motif could be attractive as thermoelectric materials if the power factor could be improved. The first 10 compounds in the [(PbSe) 1+δ] m(TiSe₂) n family (m, n ≤ 3) are reported as a case study. As n increases, the magnitude of the Seebeck coefficient is significantly increased without a simultaneous decrease in the in-plane electrical conductivity, resulting in an improved thermoelectric power factor.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5507028','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5507028"><span>Misfit <span class="hlt">Layer</span> Compounds and Ferecrystals: <span class="hlt">Model</span> Systems for Thermoelectric Nanocomposites</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Merrill, Devin R.; Moore, Daniel B.; Bauers, Sage R.; Falmbigl, Matthias; Johnson, David C.</p> <p>2015-01-01</p> <p>A basic summary of thermoelectric principles is presented in a historical context, following the <span class="hlt">evolution</span> of the field from initial discovery to modern day high-zT materials. A specific focus is placed on nanocomposite materials as a means to solve the challenges presented by the contradictory material requirements necessary for efficient thermal energy harvest. Misfit <span class="hlt">layer</span> compounds are highlighted as an example of a highly ordered anisotropic nanocomposite system. Their <span class="hlt">layered</span> structure provides the opportunity to use multiple constituents for improved thermoelectric performance, through both enhanced phonon scattering at interfaces and through electronic interactions between the constituents. Recently, a class of metastable, turbostratically-disordered misfit <span class="hlt">layer</span> compounds has been synthesized using a kinetically controlled approach with low reaction temperatures. The kinetically stabilized structures can be prepared with a variety of constituent ratios and <span class="hlt">layering</span> schemes, providing an avenue to systematically understand structure-function relationships not possible in the thermodynamic compounds. We summarize the work that has been done to date on these materials. The observed turbostratic disorder has been shown to result in extremely low cross plane thermal conductivity and in plane thermal conductivities that are also very small, suggesting the structural motif could be attractive as thermoelectric materials if the power factor could be improved. The first 10 compounds in the [(PbSe)1+δ]m(TiSe2)n family (m, n ≤ 3) are reported as a case study. As n increases, the magnitude of the Seebeck coefficient is significantly increased without a simultaneous decrease in the in-plane electrical conductivity, resulting in an improved thermoelectric power factor. PMID:28788045</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4603630','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4603630"><span>Probabilistic <span class="hlt">modeling</span> of the <span class="hlt">evolution</span> of gene synteny within reconciled phylogenies</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>2015-01-01</p> <p>Background Most <span class="hlt">models</span> of genome <span class="hlt">evolution</span> concern either genetic sequences, gene content or gene order. They sometimes integrate two of the three levels, but rarely the three of them. Probabilistic <span class="hlt">models</span> of gene order <span class="hlt">evolution</span> usually have to assume constant gene content or adopt a presence/absence coding of gene neighborhoods which is blind to complex events modifying gene content. Results We propose a probabilistic evolutionary <span class="hlt">model</span> for gene neighborhoods, allowing genes to be inserted, duplicated or lost. It uses reconciled phylogenies, which integrate sequence and gene content <span class="hlt">evolution</span>. We are then able to optimize parameters such as phylogeny branch lengths, or probabilistic laws depicting the diversity of susceptibility of syntenic regions to rearrangements. We reconstruct a structure for ancestral genomes by optimizing a likelihood, keeping track of all evolutionary events at the level of gene content and gene synteny. Ancestral syntenies are associated with a probability of presence. We implemented the <span class="hlt">model</span> with the restriction that at most one gene duplication separates two gene speciations in reconciled gene trees. We reconstruct ancestral syntenies on a set of 12 drosophila genomes, and compare the evolutionary rates along the branches and along the sites. We compare with a parsimony method and find a significant number of results not supported by the posterior probability. The <span class="hlt">model</span> is implemented in the Bio++ library. It thus benefits from and enriches the classical <span class="hlt">models</span> and methods for molecular <span class="hlt">evolution</span>. PMID:26452018</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4298177','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4298177"><span>A <span class="hlt">Model</span> of Substitution Trajectories in Sequence Space and Long-Term Protein <span class="hlt">Evolution</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>Usmanova, Dinara R.; Ferretti, Luca; Povolotskaya, Inna S.; Vlasov, Peter K.; Kondrashov, Fyodor A.</p> <p>2015-01-01</p> <p>The nature of factors governing the tempo and mode of protein <span class="hlt">evolution</span> is a fundamental issue in evolutionary biology. Specifically, whether or not interactions between different sites, or epistasis, are important in directing the course of <span class="hlt">evolution</span> became one of the central questions. Several recent reports have scrutinized patterns of long-term protein <span class="hlt">evolution</span> claiming them to be compatible only with an epistatic fitness landscape. However, these claims have not yet been substantiated with a formal <span class="hlt">model</span> of protein <span class="hlt">evolution</span>. Here, we formulate a simple covarion-like <span class="hlt">model</span> of protein <span class="hlt">evolution</span> focusing on the rate at which the fitness impact of amino acids at a site changes with time. We then apply the <span class="hlt">model</span> to the data on convergent and divergent protein <span class="hlt">evolution</span> to test whether or not the incorporation of epistatic interactions is necessary to explain the data. We find that convergent <span class="hlt">evolution</span> cannot be explained without the incorporation of epistasis and the rate at which an amino acid state switches from being acceptable at a site to being deleterious is faster than the rate of amino acid substitution. Specifically, for proteins that have persisted in modern prokaryotic organisms since the last universal common ancestor for one amino acid substitution approximately ten amino acid states switch from being accessible to being deleterious, or vice versa. Thus, molecular <span class="hlt">evolution</span> can only be perceived in the context of rapid turnover of which amino acids are available for <span class="hlt">evolution</span>. PMID:25415964</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1992comb.symp....5K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1992comb.symp....5K"><span>Turbulent dusty boundary <span class="hlt">layer</span> in an ANFO surface-burst explosion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuhl, A. L.; Ferguson, R. E.; Chien, K. Y.; Collins, J. P.</p> <p>1992-01-01</p> <p>This paper describes the results of numerical simulations of the dusty, turbulent boundary <span class="hlt">layer</span> created by a surface burst explosion. The blast wave was generated by the detonation of a 600-T hemisphere of ANFO, similar to those used in large-scale field tests. The surface was assumed to be ideally noncratering but contained an initial loose <span class="hlt">layer</span> of dust. The dust-air mixture in this fluidized bed was <span class="hlt">modeled</span> as a dense gas (i.e., an equilibrium <span class="hlt">model</span>, valid for very small-diameter dust particles). The <span class="hlt">evolution</span> of the flow was calculated by a high-order Godunov code that solves the nonsteady conservation laws. Shock interactions with dense <span class="hlt">layer</span> generated vorticity near the wall, a result that is similar to viscous, no-slip effects found in clean flows. The resulting wall shear <span class="hlt">layer</span> was unstable, and rolled up into large-scale rotational structures. These structures entrained dense material from the wall <span class="hlt">layer</span> and created a chaotically striated flow. The boundary <span class="hlt">layer</span> grew due to merging of the large-scale structures and due to local entrainment of the dense material from the fluidized bed. The chaotic flow was averaged along similarity lines (i.e., lines of constant values of x = r/Rs and y = z/Rs where R(sub s) = ct(exp alpha)) to establish the mean-flow profiles and the r.m.s. fluctuating-flow profiles of the boundary <span class="hlt">layer</span>.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_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/20952258','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20952258"><span>A stochastic <span class="hlt">evolution</span> <span class="hlt">model</span> for residue Insertion-Deletion Independent from Substitution.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lèbre, Sophie; Michel, Christian J</p> <p>2010-12-01</p> <p>We develop here a new class of stochastic <span class="hlt">models</span> of gene <span class="hlt">evolution</span> based on residue Insertion-Deletion Independent from Substitution (IDIS). Indeed, in contrast to all existing <span class="hlt">evolution</span> <span class="hlt">models</span>, insertions and deletions are <span class="hlt">modeled</span> here by a concept in population dynamics. Therefore, they are not only independent from each other, but also independent from the substitution process. After a separate stochastic analysis of the substitution and the insertion-deletion processes, we obtain a matrix differential equation combining these two processes defining the IDIS <span class="hlt">model</span>. By deriving a general solution, we give an analytical expression of the residue occurrence probability at <span class="hlt">evolution</span> time t as a function of a substitution rate matrix, an insertion rate vector, a deletion rate and an initial residue probability vector. Various mathematical properties of the IDIS <span class="hlt">model</span> in relation with time t are derived: time scale, time step, time inversion and sequence length. Particular expressions of the nucleotide occurrence probability at time t are given for classical substitution rate matrices in various biological contexts: equal insertion rate, insertion-deletion only and substitution only. All these expressions can be directly used for biological evolutionary applications. The IDIS <span class="hlt">model</span> shows a strongly different stochastic behavior from the classical substitution only <span class="hlt">model</span> when compared on a gene dataset. Indeed, by considering three processes of residue insertion, deletion and substitution independently from each other, it allows a more realistic representation of gene <span class="hlt">evolution</span> and opens new directions and applications in this research field. Copyright © 2010 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24589998','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24589998"><span>A review of molecular <span class="hlt">modelling</span> of electric double <span class="hlt">layer</span> capacitors.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Burt, Ryan; Birkett, Greg; Zhao, X S</p> <p>2014-04-14</p> <p>Electric double-<span class="hlt">layer</span> capacitors are a family of electrochemical energy storage devices that offer a number of advantages, such as high power density and long cyclability. In recent years, research and development of electric double-<span class="hlt">layer</span> capacitor technology has been growing rapidly, in response to the increasing demand for energy storage devices from emerging industries, such as hybrid and electric vehicles, renewable energy, and smart grid management. The past few years have witnessed a number of significant research breakthroughs in terms of novel electrodes, new electrolytes, and fabrication of devices, thanks to the discovery of innovative materials (e.g. graphene, carbide-derived carbon, and templated carbon) and the availability of advanced experimental and computational tools. However, some experimental observations could not be clearly understood and interpreted due to limitations of traditional theories, some of which were developed more than one hundred years ago. This has led to significant research efforts in computational simulation and <span class="hlt">modelling</span>, aimed at developing new theories, or improving the existing ones to help interpret experimental results. This review article provides a summary of research progress in molecular <span class="hlt">modelling</span> of the physical phenomena taking place in electric double-<span class="hlt">layer</span> capacitors. An introduction to electric double-<span class="hlt">layer</span> capacitors and their applications, alongside a brief description of electric double <span class="hlt">layer</span> theories, is presented first. Second, molecular <span class="hlt">modelling</span> of ion behaviours of various electrolytes interacting with electrodes under different conditions is reviewed. Finally, key conclusions and outlooks are given. Simulations on comparing electric double-<span class="hlt">layer</span> structure at planar and porous electrode surfaces under equilibrium conditions have revealed significant structural differences between the two electrode types, and porous electrodes have been shown to store charge more efficiently. Accurate electrolyte and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25254039','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25254039"><span>A two-<span class="hlt">layered</span> diffusion <span class="hlt">model</span> traces the dynamics of information processing in the valuation-and-choice circuit of decision making.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Piu, Pietro; Fargnoli, Francesco; Innocenti, Alessandro; Rufa, Alessandra</p> <p>2014-01-01</p> <p>A circuit of evaluation and selection of the alternatives is considered a reliable <span class="hlt">model</span> in neurobiology. The prominent contributions of the literature to this topic are reported. In this study, valuation and choice of a decisional process during Two-Alternative Forced-Choice (TAFC) task are represented as a two-<span class="hlt">layered</span> network of computational cells, where information accrual and processing progress in nonlinear diffusion dynamics. The <span class="hlt">evolution</span> of the response-to-stimulus map is thus <span class="hlt">modeled</span> by two linked diffusive modules (2LDM) representing the neuronal populations involved in the valuation-and-decision circuit of decision making. Diffusion <span class="hlt">models</span> are naturally appropriate for describing accumulation of evidence over the time. This allows the computation of the response times (RTs) in valuation and choice, under the hypothesis of ex-Wald distribution. A nonlinear transfer function integrates the activities of the two <span class="hlt">layers</span>. The input-output map based on the infomax principle makes the 2LDM consistent with the reinforcement learning approach. Results from simulated likelihood time series indicate that 2LDM may account for the activity-dependent modulatory component of effective connectivity between the neuronal populations. Rhythmic fluctuations of the estimate gain functions in the delta-beta bands also support the compatibility of 2LDM with the neurobiology of DM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.879a2006C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.879a2006C"><span>Thickness optimization of the ZnO based TCO <span class="hlt">layer</span> in a CZTSSe solar cell. <span class="hlt">Evolution</span> of its performance with thickness when external temperature changes.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chadel, Meriem; Moustafa Bouzaki, Mohammed; Chadel, Asma; Aillerie, Michel; Benyoucef, Boumediene</p> <p>2017-07-01</p> <p>The influence of the thickness of a Zinc Oxide (ZnO) transparent conductive oxide (TCO) <span class="hlt">layer</span> on the performance of the CZTSSe solar cell is shown in detail. In a photovoltaic cell, the thickness of each <span class="hlt">layer</span> largely influence the performance of the solar cell and optimization of each <span class="hlt">layer</span> constitutes a complete work. Here, using the Solar Cell Capacitance Simulation (SCAPS) software, we present simulation results obtained in the analyze of the influence of the TCO <span class="hlt">layer</span> thickness on the performance of a CZTSSe solar cell, starting from performance of a CZTSSe solar cell commercialized in 2014 with an initial efficiency equal to 12.6%. In simulation, the temperature was considered as a functioning parameter and the <span class="hlt">evolution</span> of tthe performance of the cell for various thickness of the TCO <span class="hlt">layer</span> when the external temperature changes is simulated and discussed. The best efficiency of the solar cell based in CZTSSe is obtained with a ZnO thickness equal to 50 nm and low temperature. Based on the considered marketed cell, we show a technological possible increase of the global efficiency achieving 13% by optimization of ZnO based TCO <span class="hlt">layer</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910008215','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910008215"><span>Diurnal ocean surface <span class="hlt">layer</span> <span class="hlt">model</span> validation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hawkins, Jeffrey D.; May, Douglas A.; Abell, Fred, Jr.</p> <p>1990-01-01</p> <p>The diurnal ocean surface <span class="hlt">layer</span> (DOSL) <span class="hlt">model</span> at the Fleet Numerical Oceanography Center forecasts the 24-hour change in a global sea surface temperatures (SST). Validating the DOSL <span class="hlt">model</span> is a difficult task due to the huge areas involved and the lack of in situ measurements. Therefore, this report details the use of satellite infrared multichannel SST imagery to provide day and night SSTs that can be directly compared to DOSL products. This water-vapor-corrected imagery has the advantages of high thermal sensitivity (0.12 C), large synoptic coverage (nearly 3000 km across), and high spatial resolution that enables diurnal heating events to be readily located and mapped. Several case studies in the subtropical North Atlantic readily show that DOSL results during extreme heating periods agree very well with satellite-imagery-derived values in terms of the pattern of diurnal warming. The low wind and cloud-free conditions necessary for these events to occur lend themselves well to observation via infrared imagery. Thus, the normally cloud-limited aspects of satellite imagery do not come into play for these particular environmental conditions. The fact that the DOSL <span class="hlt">model</span> does well in extreme events is beneficial from the standpoint that these cases can be associated with the destruction of the surface acoustic duct. This so-called afternoon effect happens as the afternoon warming of the mixed <span class="hlt">layer</span> disrupts the sound channel and the propagation of acoustic energy.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SPIE.6169..190C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SPIE.6169..190C"><span>Vibration control of beams using stand-off <span class="hlt">layer</span> damping: finite element <span class="hlt">modeling</span> and experiments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chaudry, A.; Baz, A.</p> <p>2006-03-01</p> <p>Damping treatments with stand-off <span class="hlt">layer</span> (SOL) have been widely accepted as an attractive alternative to conventional constrained <span class="hlt">layer</span> damping (CLD) treatments. Such an acceptance stems from the fact that the SOL, which is simply a slotted spacer <span class="hlt">layer</span> sandwiched between the viscoelastic <span class="hlt">layer</span> and the base structure, acts as a strain magnifier that considerably amplifies the shear strain and hence the energy dissipation characteristics of the viscoelastic <span class="hlt">layer</span>. Accordingly, more effective vibration suppression can be achieved by using SOL as compared to employing CLD. In this paper, a comprehensive finite element <span class="hlt">model</span> of the stand-off <span class="hlt">layer</span> constrained damping treatment is developed. The <span class="hlt">model</span> accounts for the geometrical and physical parameters of the slotted SOL, the viscoelastic, <span class="hlt">layer</span> the constraining <span class="hlt">layer</span>, and the base structure. The predictions of the <span class="hlt">model</span> are validated against the predictions of a distributed transfer function <span class="hlt">model</span> and a <span class="hlt">model</span> built using a commercial finite element code (ANSYS). Furthermore, the theoretical predictions are validated experimentally for passive SOL treatments of different configurations. The obtained results indicate a close agreement between theory and experiments. Furthermore, the obtained results demonstrate the effectiveness of the CLD with SOL in enhancing the energy dissipation as compared to the conventional CLD. Extension of the proposed one-dimensional CLD with SOL to more complex structures is a natural extension to the present study.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1915731P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1915731P"><span>Effects of Land Surface Heterogeneity on Simulated Boundary-<span class="hlt">Layer</span> Structures from the LES to the Mesoscale</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Poll, Stefan; Shrestha, Prabhakar; Simmer, Clemens</p> <p>2017-04-01</p> <p>Land heterogeneity influences the atmospheric boundary <span class="hlt">layer</span> (ABL) structure including organized (secondary) circulations which feed back on land-atmosphere exchange fluxes. Especially the latter effects cannot be incorporated explicitly in regional and climate <span class="hlt">models</span> due to their coarse computational spatial grids, but must be parameterized. Current parameterizations lead, however, to uncertainties in <span class="hlt">modeled</span> surface fluxes and boundary <span class="hlt">layer</span> <span class="hlt">evolution</span>, which feed back to cloud initiation and precipitation. This study analyzes the impact of different horizontal grid resolutions on the simulated boundary <span class="hlt">layer</span> structures in terms of stability, height and induced secondary circulations. The ICON-LES (Icosahedral Nonhydrostatic in LES mode) developed by the MPI-M and the German weather service (DWD) and conducted within the framework of HD(CP)2 is used. ICON is dynamically downscaled through multiple scales of 20 km, 7 km, 2.8 km, 625 m, 312 m, and 156 m grid spacing for several days over Germany and partial neighboring countries for different synoptic conditions. We examined the entropy spectrum of the land surface heterogeneity at these grid resolutions for several locations close to measurement sites, such as Lindenberg, Jülich, Cabauw and Melpitz, and studied its influence on the surface fluxes and the <span class="hlt">evolution</span> of the boundary <span class="hlt">layer</span> profiles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1031991','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1031991"><span>Engineering Glass Passivation <span class="hlt">Layers</span> -<span class="hlt">Model</span> Results</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>Skorski, Daniel C.; Ryan, Joseph V.; Strachan, Denis M.</p> <p>2011-08-08</p> <p>The immobilization of radioactive waste into glass waste forms is a baseline process of nuclear waste management not only in the United States, but worldwide. The rate of radionuclide release from these glasses is a critical measure of the quality of the waste form. Over long-term tests and using extrapolations of ancient analogues, it has been shown that well designed glasses exhibit a dissolution rate that quickly decreases to a slow residual rate for the lifetime of the glass. The mechanistic cause of this decreased corrosion rate is a subject of debate, with one of the major theories suggesting thatmore » the decrease is caused by the formation of corrosion products in such a manner as to present a diffusion barrier on the surface of the glass. Although there is much evidence of this type of mechanism, there has been no attempt to engineer the effect to maximize the passivating qualities of the corrosion products. This study represents the first attempt to engineer the creation of passivating phases on the surface of glasses. Our approach utilizes interactions between the dissolving glass and elements from the disposal environment to create impermeable capping <span class="hlt">layers</span>. By drawing from other corrosion studies in areas where passivation <span class="hlt">layers</span> have been successfully engineered to protect the bulk material, we present here a report on mineral phases that are likely have a morphological tendency to encrust the surface of the glass. Our <span class="hlt">modeling</span> has focused on using the AFCI glass system in a carbonate, sulfate, and phosphate rich environment. We evaluate the minerals predicted to form to determine the likelihood of the formation of a protective <span class="hlt">layer</span> on the surface of the glass. We have also <span class="hlt">modeled</span> individual ions in solutions vs. pH and the addition of aluminum and silicon. These results allow us to understand the pH and ion concentration dependence of mineral formation. We have determined that iron minerals are likely to form a complete incrustation <span class="hlt">layer</span> and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140012853','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140012853"><span>The <span class="hlt">Evolution</span> of Transition Region Loops Using IRIS and AIA</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Winebarger, Amy R.; DePontieu, Bart</p> <p>2014-01-01</p> <p>Over the past 50 years, the <span class="hlt">model</span> for the structure of the solar transition region has evolved from a simple transition <span class="hlt">layer</span> between the cooler chromosphere to the hotter corona to a complex and diverse region that is dominated by complete loops that never reach coronal temperatures. The IRIS slitjaw images show many complete transition region loops. Several of the "coronal" channels in the SDO AIA instrument include contributions from weak transition region lines. In this work, we combine slitjaw images from IRIS with these channels to determine the <span class="hlt">evolution</span> of the loops. We develop a simple <span class="hlt">model</span> for the temperature and density <span class="hlt">evolution</span> of the loops that can explain the simultaneous observations. Finally, we estimate the percentage of AIA emission that originates in the transition region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JPhCS.734c2081C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JPhCS.734c2081C"><span>The friction coefficient <span class="hlt">evolution</span> of a MoS2/WC multi-<span class="hlt">layer</span> coating system during sliding wear</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chan, T. Y.; Hu, Y.; Gharbi, Mohammad M.; Politis, D. J.; Wang, L.</p> <p>2016-08-01</p> <p>This paper discusses the <span class="hlt">evolution</span> of friction coefficient for the multi-<span class="hlt">layered</span> Molybdenum Disulphide (MoS2) and WC coated substrate during sliding against Aluminium AA 6082 material. A soft MoS2 coating was prepared over a hard WC coated G3500 cast iron tool substrate and underwent friction test using a pin-on-disc tribometer. The lifetime of the coating was reduced with increasing load while the Aluminium debris accumulated on the WC hard coating surfaces, accelerated the breakdown of the coatings. The lifetime of the coating was represented by the friction coefficient and the sliding distance before MoS2 coating breakdown and was found to be affected by the load applied and the wear mechanism.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018BoLMe.tmp..179F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018BoLMe.tmp..179F"><span>Assessment of Planetary-Boundary-<span class="hlt">Layer</span> Schemes in the Weather Research and Forecasting <span class="hlt">Model</span> Within and Above an Urban Canopy <span class="hlt">Layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ferrero, Enrico; Alessandrini, Stefano; Vandenberghe, Francois</p> <p>2018-03-01</p> <p>We tested several planetary-boundary-<span class="hlt">layer</span> (PBL) schemes available in the Weather Research and Forecasting (WRF) <span class="hlt">model</span> against measured wind speed and direction, temperature and turbulent kinetic energy (TKE) at three levels (5, 9, 25 m). The Urban Turbulence Project dataset, gathered from the outskirts of Turin, Italy and used for the comparison, provides measurements made by sonic anemometers for more than 1 year. In contrast to other similar studies, which have mainly focused on short-time periods, we considered 2 months of measurements (January and July) representing both the seasonal and the daily variabilities. To understand how the WRF-<span class="hlt">model</span> PBL schemes perform in an urban environment, often characterized by low wind-speed conditions, we first compared six PBL schemes against observations taken by the highest anemometer located in the inertial sub-<span class="hlt">layer</span>. The availability of the TKE measurements allows us to directly evaluate the performances of the <span class="hlt">model</span>; results of the <span class="hlt">model</span> evaluation are presented in terms of quantile versus quantile plots and statistical indices. Secondly, we considered WRF-<span class="hlt">model</span> PBL schemes that can be coupled to the urban-surface exchange parametrizations and compared the simulation results with measurements from the two lower anemometers located inside the canopy <span class="hlt">layer</span>. We find that the PBL schemes accounting for TKE are more accurate and the <span class="hlt">model</span> representation of the roughness sub-<span class="hlt">layer</span> improves when the urban <span class="hlt">model</span> is coupled to each PBL scheme.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1834d0019Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1834d0019Y"><span><span class="hlt">Evolution</span> dynamics <span class="hlt">modeling</span> and simulation of logistics enterprise's core competence based on service innovation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Bo; Tong, Yuting</p> <p>2017-04-01</p> <p>With the rapid development of economy, the development of logistics enterprises in China is also facing a huge challenge, especially the logistics enterprises generally lack of core competitiveness, and service innovation awareness is not strong. Scholars in the process of studying the core competitiveness of logistics enterprises are mainly from the perspective of static stability, not from the perspective of dynamic <span class="hlt">evolution</span> to explore. So the author analyzes the influencing factors and the <span class="hlt">evolution</span> process of the core competence of logistics enterprises, using the method of system dynamics to study the cause and effect of the <span class="hlt">evolution</span> of the core competence of logistics enterprises, construct a system dynamics <span class="hlt">model</span> of <span class="hlt">evolution</span> of core competence logistics enterprises, which can be simulated by vensim PLE. The analysis for the effectiveness and sensitivity of simulation <span class="hlt">model</span> indicates the <span class="hlt">model</span> can be used as the fitting of the <span class="hlt">evolution</span> process of the core competence of logistics enterprises and reveal the process and mechanism of the <span class="hlt">evolution</span> of the core competence of logistics enterprises, and provide management strategies for improving the core competence of logistics enterprises. The construction and operation of computer simulation <span class="hlt">model</span> offers a kind of effective method for studying the <span class="hlt">evolution</span> of logistics enterprise core competence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JAMES...5..338W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JAMES...5..338W"><span>Shock-like structures in the tropical cyclone boundary <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Williams, Gabriel J.; Taft, Richard K.; McNoldy, Brian D.; Schubert, Wayne H.</p> <p>2013-06-01</p> <p>This paper presents high horizontal resolution solutions of an axisymmetric, constant depth, slab boundary <span class="hlt">layer</span> <span class="hlt">model</span> designed to simulate the radial inflow and boundary <span class="hlt">layer</span> pumping of a hurricane. Shock-like structures of increasing intensity appear for category 1-5 hurricanes. For example, in the category 3 case, the u>(∂u/∂r>) term in the radial equation of motion produces a shock-like structure in the radial wind, i.e., near the radius of maximum tangential wind the boundary <span class="hlt">layer</span> radial inflow decreases from approximately 22 m s-1 to zero over a radial distance of a few kilometers. Associated with this large convergence is a spike in the radial distribution of boundary <span class="hlt">layer</span> pumping, with updrafts larger than 22 m s-1 at a height of 1000 m. Based on these <span class="hlt">model</span> results, it is argued that observed hurricane updrafts of this magnitude so close to the ocean surface are attributable to the dry dynamics of the frictional boundary <span class="hlt">layer</span> rather than moist convective dynamics. The shock-like structure in the boundary <span class="hlt">layer</span> radial wind also has important consequences for the <span class="hlt">evolution</span> of the tangential wind and the vertical component of vorticity. On the inner side of the shock the tangential wind tendency is essentially zero, while on the outer side of the shock the tangential wind tendency is large due to the large radial inflow there. The result is the development of a U-shaped tangential wind profile and the development of a thin region of large vorticity. In many respects, the <span class="hlt">model</span> solutions resemble the remarkable structures observed in the boundary <span class="hlt">layer</span> of Hurricane Hugo (1989).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28098392','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28098392"><span>Bayesian nonparametric clustering in phylogenetics: <span class="hlt">modeling</span> antigenic <span class="hlt">evolution</span> in influenza.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Cybis, Gabriela B; Sinsheimer, Janet S; Bedford, Trevor; Rambaut, Andrew; Lemey, Philippe; Suchard, Marc A</p> <p>2018-01-30</p> <p>Influenza is responsible for up to 500,000 deaths every year, and antigenic variability represents much of its epidemiological burden. To visualize antigenic differences across many viral strains, antigenic cartography methods use multidimensional scaling on binding assay data to map influenza antigenicity onto a low-dimensional space. Analysis of such assay data ideally leads to natural clustering of influenza strains of similar antigenicity that correlate with sequence <span class="hlt">evolution</span>. To understand the dynamics of these antigenic groups, we present a framework that jointly <span class="hlt">models</span> genetic and antigenic <span class="hlt">evolution</span> by combining multidimensional scaling of binding assay data, Bayesian phylogenetic machinery and nonparametric clustering methods. We propose a phylogenetic Chinese restaurant process that extends the current process to incorporate the phylogenetic dependency structure between strains in the <span class="hlt">modeling</span> of antigenic clusters. With this method, we are able to use the genetic information to better understand the <span class="hlt">evolution</span> of antigenicity throughout epidemics, as shown in applications of this <span class="hlt">model</span> to H1N1 influenza. Copyright © 2017 John Wiley & Sons, Ltd. Copyright © 2017 John Wiley & Sons, Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.13301003G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.13301003G"><span>Growth and characterization of organic <span class="hlt">layers</span> deposited on porous-patterned Si surface</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gorbach, Tamara Ya.; Smertenko, Petro S.; Olkhovik, G. P.; Wisz, Grzegorz</p> <p>2017-01-01</p> <p>The organic <span class="hlt">layers</span> with the thickness from a few nanometers up to few micrometers have been deposited from the chemical solution at room temperature on porous patterned Si surfaces using two medical solutions: thiamine diphosphide (pH=1÷2) and metamizole sodium (pH=6÷7). Based on <span class="hlt">evolution</span> of morphology, structural and compositional features obtained by scanning electron microscopy, X-ray analysis, reflectance high energy electron diffraction the grown mechanisms in thin organic <span class="hlt">layers</span> are discussed in the terms of terrace-step-kink <span class="hlt">model</span> whereas self-organized assemblies evaluated more thick <span class="hlt">layers</span>. Transport mechanism features and possible photovoltaic properties are discussed on the base of differential current-voltage characteristics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SMaS...26l5008Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SMaS...26l5008Z"><span>A fully dynamic <span class="hlt">model</span> of a multi-<span class="hlt">layer</span> piezoelectric actuator incorporating the power amplifier</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhu, Wei; Yang, Fufeng; Rui, Xiaoting</p> <p>2017-12-01</p> <p>The dynamic input-output characteristics of the multi-<span class="hlt">layer</span> piezoelectric actuator (PA) are intrinsically rate-dependent and hysteresis. Meanwhile, aiming at the strong capacitive impedance of multi-<span class="hlt">layer</span> PA, the power amplifier of the actuator can greatly affect the dynamic performances of the actuator. In this paper, a novel dynamic <span class="hlt">model</span> that includes a <span class="hlt">model</span> of the electric circuit providing voltage to the actuator, an inverse piezoelectric effect <span class="hlt">model</span> describing the hysteresis and creep behavior of the actuator, and a mechanical <span class="hlt">model</span>, in which the vibration characteristics of the multi-<span class="hlt">layer</span> PA is described, is put forward. Validation experimental tests are conducted. Experimental results show that the proposed dynamic <span class="hlt">model</span> can accurately predict the fully dynamic behavior of the multi-<span class="hlt">layer</span> PA with different driving power.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940007828','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940007828"><span>Progress in <span class="hlt">modeling</span> hypersonic turbulent boundary <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Zeman, Otto</p> <p>1993-01-01</p> <p>A good knowledge of the turbulence structure, wall heat transfer, and friction in turbulent boundary <span class="hlt">layers</span> (TBL) at high speeds is required for the design of hypersonic air breathing airplanes and reentry space vehicles. This work reports on recent progress in the <span class="hlt">modeling</span> of high speed TBL flows. The specific research goal described here is the development of a second order closure <span class="hlt">model</span> for zero pressure gradient TBL's for the range of Mach numbers up to hypersonic speeds with arbitrary wall cooling requirements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007Icar..187..332B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007Icar..187..332B"><span>The internal structure of Jupiter family cometary nuclei from Deep Impact observations: The “talps” or “<span class="hlt">layered</span> pile” <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Belton, Michael J. S.; Thomas, Peter; Veverka, J.; Schultz, Peter; A'Hearn, Michael F.; Feaga, Lori; Farnham, Tony; Groussin, Olivier; Li, Jian-Yang; Lisse, Casey; McFadden, Lucy; Sunshine, Jessica; Meech, Karen J.; Delamere, W. Alan; Kissel, Jochen</p> <p>2007-03-01</p> <p>We consider the hypothesis that the <span class="hlt">layering</span> observed on the surface of Comet 9P/Tempel 1 from the Deep Impact spacecraft and identified on other comet nuclei imaged by spacecraft (i.e., 19P/Borrelly and 81P/Wild 2) is ubiquitous on Jupiter family cometary nuclei and is an essential element of their internal structure. The observational characteristics of the <span class="hlt">layers</span> on 9P/Tempel 1 are detailed and considered in the context of current theories of the accumulation and dynamical <span class="hlt">evolution</span> of cometary nuclei. The works of Donn [Donn, B.D., 1990. Astron. Astrophys. 235, 441-446], Sirono and Greenberg [Sirono, S.-I., Greenberg, J.M., 2000. Icarus 145, 230-238] and the experiments of Wurm et al. [Wurm, G., Paraskov, G., Krauss, O., 2005. Icarus 178, 253-263] on the collision physics of porous aggregate bodies are used as basis for a conceptual <span class="hlt">model</span> of the formation of <span class="hlt">layers</span>. Our hypothesis is found to have implications for the place of origin of the JFCs and their subsequent dynamical history. <span class="hlt">Models</span> of fragmentation and rubble pile building in the Kuiper belt in a period of collisional activity (e.g., [Kenyon, S.J., Luu, J.X., 1998. Astron. J. 115, 2136-2160; 1999a. Astron. J. 118, 1101-1119; 1999b. Astrophys. J. 526, 465-470; Farinella, P., Davis, D.R., Stern, S.A., 2000. In: Mannings, V., Boss, A.P., Russell, S.S. (Eds.), Protostars and Planets IV. Univ. of Arizona Press, Tucson, pp. 1255-1282; Durda, D.D., Stern, S.J., 2000. Icarus 145, 220-229]) following the formation of Neptune appear to be in conflict with the observed properties of the <span class="hlt">layers</span> and irreconcilable with the hypothesis. Long-term residence in the scattered disk [Duncan, M.J., Levison, H.F., 1997. Science 276, 1670-1672; Duncan, M., Levison, H., Dones, L., 2004. In: Festou, M., Keller, H.U., Weaver, H.A. (Eds.), Comets II. Univ. of Arizona Press, Tucson, pp. 193-204] and/or a change in fragmentation outcome <span class="hlt">modeling</span> may explain the long-term persistence of primordial <span class="hlt">layers</span>. In any event, the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007Icar..191S.573B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007Icar..191S.573B"><span>The internal structure of Jupiter family cometary nuclei from Deep Impact observations: The “talps” or “<span class="hlt">layered</span> pile” <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Belton, Michael J. S.; Thomas, Peter; Veverka, J.; Schultz, Peter; A'Hearn, Michael F.; Feaga, Lori; Farnham, Tony; Groussin, Olivier; Li, Jian-Yang; Lisse, Casey; McFadden, Lucy; Sunshine, Jessica; Meech, Karen J.; Delamere, W. Alan; Kissel, Jochen</p> <p></p> <p>We consider the hypothesis that the <span class="hlt">layering</span> observed on the surface of Comet 9P/Tempel 1 from the Deep Impact spacecraft and identified on other comet nuclei imaged by spacecraft (i.e., 19P/Borrelly and 81P/Wild 2) is ubiquitous on Jupiter family cometary nuclei and is an essential element of their internal structure. The observational characteristics of the <span class="hlt">layers</span> on 9P/Tempel 1 are detailed and considered in the context of current theories of the accumulation and dynamical <span class="hlt">evolution</span> of cometary nuclei. The works of Donn [Donn, B.D., 1990. Astron. Astrophys. 235, 441 446], Sirono and Greenberg [Sirono, S.-I., Greenberg, J.M., 2000. Icarus 145, 230 238] and the experiments of Wurm et al. [Wurm, G., Paraskov, G., Krauss, O., 2005. Icarus 178, 253 263] on the collision physics of porous aggregate bodies are used as basis for a conceptual <span class="hlt">model</span> of the formation of <span class="hlt">layers</span>. Our hypothesis is found to have implications for the place of origin of the JFCs and their subsequent dynamical history. <span class="hlt">Models</span> of fragmentation and rubble pile building in the Kuiper belt in a period of collisional activity (e.g., [Kenyon, S.J., Luu, J.X., 1998. Astron. J. 115, 2136 2160; 1999a. Astron. J. 118, 1101 1119; 1999b. Astrophys. J. 526, 465 470; Farinella, P., Davis, D.R., Stern, S.A., 2000. In: Mannings, V., Boss, A.P., Russell, S.S. (Eds.), Protostars and Planets IV. Univ. of Arizona Press, Tucson, pp. 1255 1282; Durda, D.D., Stern, S.J., 2000. Icarus 145, 220 229]) following the formation of Neptune appear to be in conflict with the observed properties of the <span class="hlt">layers</span> and irreconcilable with the hypothesis. Long-term residence in the scattered disk [Duncan, M.J., Levison, H.F., 1997. Science 276, 1670 1672; Duncan, M., Levison, H., Dones, L., 2004. In: Festou, M., Keller, H.U., Weaver, H.A. (Eds.), Comets II. Univ. of Arizona Press, Tucson, pp. 193 204] and/or a change in fragmentation outcome <span class="hlt">modeling</span> may explain the long-term persistence of primordial <span class="hlt">layers</span>. In any event, the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI14A..04C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI14A..04C"><span>Testing Lithospheric versus Deep-Mantle Dynamics on Post-100 Ma <span class="hlt">Evolution</span> of Western U.S. using Landscape <span class="hlt">Evolution</span> <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chang, C.; Liu, L.</p> <p>2017-12-01</p> <p>Driving mechanisms of the topographic <span class="hlt">evolution</span> of central-western North America from the Cretaceous Western Interior Seaway (WIS) to its present-day high elevation remain ellusive. Quantifying the effects of lithospheric deformation versus deep-mantle induced topography on the landscape <span class="hlt">evolution</span> of the region is a key to better constraining the history of North American tectonics and mantle dynamics. One way to tackle this problem is through running landscape <span class="hlt">evolution</span> simulation coupled with uplift histories characteristic to these tectonic processes. We then use available surface observations, e.g., sedimentation records, land erosion, and drainage <span class="hlt">evolution</span>, to infer the likely lithospheric and mantle processes that formed the WIS, the subsequent Laramide orogeny, and the present-day high topography of central-western North America. In practice, we use BadLands to simulate the <span class="hlt">evolution</span> of surface process. To validate a given uplift history, we quantitatively compare <span class="hlt">model</span> predictions with onshore and offshore stratigraphy data from the literature. Furthermore, critical forcings of landscape <span class="hlt">evolution</span>, such as climate, lithology and sea level, will also be examined to better attest the effects of different uplift scenarios. Preliminary results demonstrate that only with geographically migratory subsidence, as predicted by an inverse mantle convection <span class="hlt">model</span>, can we re-produce large scale tilted strata and shifting sediment deposition observed in the WIS basins. Ongoing work will also look into styles of Cenozoic uplift events that ended the WIS and produced the landscape features today. Eventually, we hope to place new constraints on the <span class="hlt">evolution</span> and properties of lithospheric and deep-mantle dynamics of North American and to locate the best-fit scenario of its coresponding surface <span class="hlt">evolution</span> since 100 Ma.</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=19810050987&hterms=Ankara&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DAnkara','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810050987&hterms=Ankara&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3DAnkara"><span>A magnetospheric signature of some F <span class="hlt">layer</span> positive storms</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Miller, N. J.; Mayr, H. G.; Grebowsky, J. M.; Harris, I.; Tulunay, Y. K.</p> <p>1981-01-01</p> <p>Calculations of electron density distributions in the global thermosphere-ionosphere system perturbed by high-latitude thermospheric heating are presented which indicate a link between the heating and magnetospheric plasma disturbances near the equator. The calculations were made using a self-consistent <span class="hlt">model</span> of the global sunlit thermosphere-ionosphere system describing the <span class="hlt">evolution</span> of equatorial plasma disturbances. The heat input is found to cause electron density enhancements that propagate along magnetic field lines from the F2 maximum over mid-latitudes to the equator in the magnetosphere and which correspond to the positive phase of an F <span class="hlt">layer</span> storm. The positive phase is shown to be generated by the induction of equatorward winds that raise the mid-latitude F <span class="hlt">layer</span> through momentum transfer from neutral atoms to ionospheric ions, which ions pull electrons with them. <span class="hlt">Model</span> results are used to identify plasma signatures of equatorward winds and an intensified magnetospheric electric field in Explorer 45 and Arial 4 measurements taken during the positive phase of an F <span class="hlt">layer</span> storm.</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 <span class="hlt">Model</span> Coupling Boundary-<span class="hlt">Layer</span> 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 <span class="hlt">model</span> coupling non-flowing boundary-<span class="hlt">layer</span> effect for tight oil reservoirs was proposed. Firstly, pore structures of tight formations were characterized with fractal theory. Then, with the empirical equation of boundary-<span class="hlt">layer</span> thickness, Hagen-Poiseuille equation and fractal theory, a fractal torturous capillary tube <span class="hlt">model</span> coupled with boundary-<span class="hlt">layer</span> effect was developed, and verified with experimental data. Finally, 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 boundary-<span class="hlt">layer</span> 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, boundary-<span class="hlt">layer</span> 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/2015APS..DPPYP2014R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DPPYP2014R"><span>L-H transitions driven by ion heating in scrape-off <span class="hlt">layer</span> turbulence (SOLT) <span class="hlt">model</span> simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Russell, D. A.; D'Ippolito, D. A.; Myra, J. R.</p> <p>2015-11-01</p> <p>The original SOLT <span class="hlt">model</span> now includes the <span class="hlt">evolution</span> of ion pressure consistent with drift-ordering. It is a two-dimensional, electrostatic reduced <span class="hlt">model</span> wherein closure relations, obtained by integrating the equations along the B-field, <span class="hlt">model</span> parallel physics that includes sheath-mediated current and heat flux in the scrape-off-<span class="hlt">layer</span> and electron drift waves inside the separatrix. Low (L) and high (H) confinement regimes are observed in SOLT simulations, depending on the strength of an ion pressure (i.e., ion heating) source localized inside the separatrix: With increasing heating, particle and energy confinement times at first decrease in the L-mode then rise in the H-mode. The L-H transition is marked by distinct changes in sheared-flow profiles. The addition of ion pressure dynamics enables <span class="hlt">modeling</span> the self-consistent interaction between the ion diamagnetic drift and the radial electric field (mean and zonal flows). The roles of these sheared flows in mediating the L-H transition are explored. A new diagnostic, based on the density correlation function, is applied to study blob velocities in different regimes. Work supported by the U.S. Department of Energy Office of Science, Office of Fusion Energy Sciences, under Award Number DE-FG02-97ER54392.</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 boundary <span class="hlt">layer</span> in atmospheric <span class="hlt">models</span></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 boundary <span class="hlt">layer</span> (PBL) measurements; current problems of PBL parameterization in mesoscale <span class="hlt">models</span>; and convective cloud-PBL interactions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMEP43A0943Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMEP43A0943Y"><span>Ecohydro-geomorphic implications of orographic precipitation on landform <span class="hlt">evolution</span> using a landscape <span class="hlt">evolution</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yetemen, O.; Saco, P. M.</p> <p>2016-12-01</p> <p>Orography induced precipitation and its implications on vegetation dynamics and landscape morphology have long been documented in the literature. However a numerical framework that integrates a range of ecohydrologic and geomorphic processes to explore the coupled ecohydro-geomorphic landscape response of catchments where pronounced orographic precipitation prevails has been missing. In this study, our aim is to realistically represent orographic-precipitation-driven ecohydrologic dynamics in a landscape <span class="hlt">evolution</span> <span class="hlt">model</span> (LEM). The <span class="hlt">model</span> is used to investigate how ecohydro-geomorphic differences caused by differential precipitation patterns on the leeward and windward sides of low-relief landscapes lead to differences in the organization of <span class="hlt">modelled</span> topography, soil moisture and plant biomass. We use the CHILD LEM equipped with a vegetation dynamics component that explicitly tracks above- and below-ground biomass, and a precipitation forcing component that simulates rainfall as a function of elevation and orientation. The preliminary results of the <span class="hlt">model</span> show how the competition between an increased shear stress through runoff production and an enhanced resistance force due to denser canopy cover shape the landscape. Moreover, orographic precipitation leads to not only the migration of the divide between leeward and windward slopes but also a change in the concavity of streams. These results clearly demonstrate the strong coupling between landform <span class="hlt">evolution</span> and climate processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940024420','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940024420"><span>A random distribution reacting mixing <span class="hlt">layer</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jones, Richard A.; Marek, C. John; Myrabo, Leik N.; Nagamatsu, Henry T.</p> <p>1994-01-01</p> <p>A methodology for simulation of molecular mixing, and the resulting velocity and temperature fields has been developed. The ideas are applied to the flow conditions present in the NASA Lewis Research Center Planar Reacting Shear <span class="hlt">Layer</span> (PRSL) facility, and results compared to experimental data. A gaussian transverse turbulent velocity distribution is used in conjunction with a linearly increasing time scale to describe the mixing of different regions of the flow. Equilibrium reaction calculations are then performed on the mix to arrive at a new species composition and temperature. Velocities are determined through summation of momentum contributions. The analysis indicates a combustion efficiency of the order of 80 percent for the reacting mixing <span class="hlt">layer</span>, and a turbulent Schmidt number of 2/3. The success of the <span class="hlt">model</span> is attributed to the simulation of large-scale transport of fluid. The favorable comparison shows that a relatively quick and simple PC calculation is capable of simulating the basic flow structure in the reacting and nonreacting shear <span class="hlt">layer</span> present in the facility given basic assumptions about turbulence properties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800028699&hterms=atmospheric+pollution&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Datmospheric%2Bpollution','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800028699&hterms=atmospheric+pollution&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Datmospheric%2Bpollution"><span>Finite-element numerical <span class="hlt">modeling</span> of atmospheric turbulent boundary <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Lee, H. N.; Kao, S. K.</p> <p>1979-01-01</p> <p>A dynamic turbulent boundary-<span class="hlt">layer</span> <span class="hlt">model</span> in the neutral atmosphere is constructed, using a dynamic turbulent equation of the eddy viscosity coefficient for momentum derived from the relationship among the turbulent dissipation rate, the turbulent kinetic energy and the eddy viscosity coefficient, with aid of the turbulent second-order closure scheme. A finite-element technique was used for the numerical integration. In preliminary results, the behavior of the neutral planetary boundary <span class="hlt">layer</span> agrees well with the available data and with the existing elaborate turbulent <span class="hlt">models</span>, using a finite-difference scheme. The proposed dynamic formulation of the eddy viscosity coefficient for momentum is particularly attractive and can provide a viable alternative approach to study atmospheric turbulence, diffusion and air pollution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920051368&hterms=design+graphic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Ddesign%2Bgraphic','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920051368&hterms=design+graphic&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Ddesign%2Bgraphic"><span><span class="hlt">Layer-by-layer</span> design method for soft-X-ray multilayers</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yamamoto, Masaki; Namioka, Takeshi</p> <p>1992-01-01</p> <p>A new design method effective for a nontransparent system has been developed for soft-X-ray multilayers with the aid of graphic representation of the complex amplitude reflectance in a Gaussian plane. The method provides an effective means of attaining the absolute maximum reflectance on a <span class="hlt">layer-by-layer</span> basis and also gives clear insight into the <span class="hlt">evolution</span> of the amplitude reflectance on a multilayer as it builds up. An optical criterion is derived for the selection of a proper pair of materials needed for designing a high-reflectance multilayer. Some examples are given to illustrate the usefulness of this design method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900051711&hterms=conceptual+framework&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dconceptual%2Bframework','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900051711&hterms=conceptual+framework&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dconceptual%2Bframework"><span>A perspective on coherent structures and conceptual <span class="hlt">models</span> for turbulent boundary <span class="hlt">layer</span> physics</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Robinson, Stephen K.</p> <p>1990-01-01</p> <p>Direct numerical simulations of turbulent boundary <span class="hlt">layers</span> have been analyzed to develop a unified conceptual <span class="hlt">model</span> for the kinematics of coherent motions in low Reynolds number canonical turbulent boundary <span class="hlt">layers</span>. All classes of coherent motions are considered in the <span class="hlt">model</span>, including low-speed streaks, ejections and sweeps, vortical structures, near-wall and outer-region shear <span class="hlt">layers</span>, sublayer pockets, and large-scale outer-region eddies. The <span class="hlt">model</span> reflects the conclusions from the study of the simulated boundary <span class="hlt">layer</span> that vortical structures are directly associated with the production of turbulent shear stresses, entrainment, dissipation of turbulence kinetic energy, and the fluctuating pressure field. These results, when viewed from the perspective of the large body of published work on the subject of coherent motions, confirm that vortical structures may be considered the central dynamic element in the maintenance of turbulence in the canonical boundary <span class="hlt">layer</span>. Vortical structures serve as a framework on which to construct a unified picture of boundary <span class="hlt">layer</span> structure, providing a means to relate the many known structural elements in a consistent way.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFM.H11E0850J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFM.H11E0850J"><span>Joint inversion of seismic refraction and resistivity data using <span class="hlt">layered</span> <span class="hlt">models</span> - applications to hydrogeology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Juhojuntti, N. G.; Kamm, J.</p> <p>2010-12-01</p> <p>We present a <span class="hlt">layered-model</span> approach to joint inversion of shallow seismic refraction and resistivity (DC) data, which we believe is a seldom tested method of addressing the problem. This method has been developed as we believe that for shallow sedimentary environments (roughly <100 m depth) a <span class="hlt">model</span> with a few <span class="hlt">layers</span> and sharp <span class="hlt">layer</span> boundaries better represents the subsurface than a smooth minimum-structure (grid) <span class="hlt">model</span>. Due to the strong assumption our <span class="hlt">model</span> parameterization implies on the subsurface, only a low number of well resolved <span class="hlt">model</span> parameters has to be estimated, and provided that this assumptions holds our method can also be applied to other environments. We are using a least-squares inversion, with lateral smoothness constraints, allowing lateral variations in the seismic velocity and the resistivity but no vertical variations. One exception is a positive gradient in the seismic velocity in the uppermost <span class="hlt">layer</span> in order to get diving rays (the refractions in the deeper <span class="hlt">layers</span> are <span class="hlt">modeled</span> as head waves). We assume no connection between seismic velocity and resistivity, and these parameters are allowed to vary individually within the <span class="hlt">layers</span>. The <span class="hlt">layer</span> boundaries are, however, common for both parameters. During the inversion lateral smoothing can be applied to the <span class="hlt">layer</span> boundaries as well as to the seismic velocity and the resistivity. The number of <span class="hlt">layers</span> is specified before the inversion, and typically we use <span class="hlt">models</span> with three <span class="hlt">layers</span>. Depending on the type of environment it is possible to apply smoothing either to the depth of the <span class="hlt">layer</span> boundaries or to the thickness of the <span class="hlt">layers</span>, although normally the former is used for shallow sedimentary environments. The smoothing parameters can be chosen independently for each <span class="hlt">layer</span>. For the DC data we use a finite-difference algorithm to perform the forward <span class="hlt">modeling</span> and to calculate the Jacobian matrix, while for the seismic data the corresponding entities are retrieved via ray-tracing, using components from the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19900010221','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19900010221"><span>Application of a Reynolds stress turbulence <span class="hlt">model</span> to the compressible shear <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Sarkar, S.; Balakrishnan, L.</p> <p>1990-01-01</p> <p>Theoretically based turbulence <span class="hlt">models</span> have had success in predicting many features of incompressible, free shear <span class="hlt">layers</span>. However, attempts to extend these <span class="hlt">models</span> to the high-speed, compressible shear <span class="hlt">layer</span> have been less effective. In the present work, the compressible shear <span class="hlt">layer</span> was studied with a second-order turbulence closure, which initially used only variable density extensions of incompressible <span class="hlt">models</span> for the Reynolds stress transport equation and the dissipation rate transport equation. The quasi-incompressible closure was unsuccessful; the predicted effect of the convective Mach number on the shear <span class="hlt">layer</span> growth rate was significantly smaller than that observed in experiments. Having thus confirmed that compressibility effects have to be explicitly considered, a new <span class="hlt">model</span> for the compressible dissipation was introduced into the closure. This <span class="hlt">model</span> is based on a low Mach number, asymptotic analysis of the Navier-Stokes equations, and on direct numerical simulation of compressible, isotropic turbulence. The use of the new <span class="hlt">model</span> for the compressible dissipation led to good agreement of the computed growth rates with the experimental data. Both the computations and the experiments indicate a dramatic reduction in the growth rate when the convective Mach number is increased. Experimental data on the normalized maximum turbulence intensities and shear stress also show a reduction with increasing Mach number.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.5017S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.5017S"><span>Parameterizing Urban Canopy <span class="hlt">Layer</span> transport in an Lagrangian Particle Dispersion <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stöckl, Stefan; Rotach, Mathias W.</p> <p>2016-04-01</p> <p>The percentage of people living in urban areas is rising worldwide, crossed 50% in 2007 and is even higher in developed countries. High population density and numerous sources of air pollution in close proximity can lead to health issues. Therefore it is important to understand the nature of urban pollutant dispersion. In the last decades this field has experienced considerable progress, however the influence of large roughness elements is complex and has as of yet not been completely described. Hence, this work studied urban particle dispersion close to source and ground. It used an existing, steady state, three-dimensional Lagrangian particle dispersion <span class="hlt">model</span>, which includes Roughness Sublayer parameterizations of turbulence and flow. The <span class="hlt">model</span> is valid for convective and neutral to stable conditions and uses the kernel method for concentration calculation. As most Lagrangian <span class="hlt">models</span>, its lower boundary is the zero-plane displacement, which means that roughly the lower two-thirds of the mean building height are not included in the <span class="hlt">model</span>. This missing <span class="hlt">layer</span> roughly coincides with the Urban Canopy <span class="hlt">Layer</span>. An earlier work "traps" particles hitting the lower <span class="hlt">model</span> boundary for a recirculation period, which is calculated under the assumption of a vortex in skimming flow, before "releasing" them again. The authors hypothesize that improving the lower boundary condition by including Urban Canopy <span class="hlt">Layer</span> transport could improve <span class="hlt">model</span> predictions. This was tested herein by not only trapping the particles, but also advecting them with a mean, parameterized flow in the Urban Canopy <span class="hlt">Layer</span>. Now the <span class="hlt">model</span> calculates the trapping period based on either recirculation due to vortex motion in skimming flow regimes or vertical velocity if no vortex forms, depending on incidence angle of the wind on a randomly chosen street canyon. The influence of this modification, as well as the <span class="hlt">model</span>'s sensitivity to parameterization constants, was investigated. To reach this goal, the <span class="hlt">model</span> was</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003AGUFMSM22D..07K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003AGUFMSM22D..07K"><span>Magnetospheric Substorm <span class="hlt">Evolution</span> in the Magnetotail: Challenge to Global MHD <span class="hlt">Modeling</span>.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kuznetsova, M. M.; Hesse, M.; Dorelli, J.; Rastaetter, L.</p> <p>2003-12-01</p> <p>Testing the ability of global MHD <span class="hlt">models</span> to describe magnetotail <span class="hlt">evolution</span> during substroms is one of the elements of science based validation efforts at CCMC. We perform simulations of magnetotail dynamics using global MHD <span class="hlt">models</span> residing at CCMC. We select solar wind conditions which drive the accumulation of magnetic field in the tail lobes and subsequent magnetic reconnection and energy release. We will analyze the effects of spatial resolution in the plasma sheet on <span class="hlt">modeled</span> expansion phase <span class="hlt">evolution</span>, maximum energy stored in the tail, and details of magnetotail reconnection. We will pay special attention to current sheet thinning and multiple plasmoid formation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApSS..426..177Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApSS..426..177Y"><span>Hydrothermal fabrication of few-<span class="hlt">layer</span> MoS2 nanosheets within nanopores on TiO2 derived from MIL-125(Ti) for efficient photocatalytic H2 <span class="hlt">evolution</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ye, Fei; Li, Houfen; Yu, Hongtao; Chen, Shuo; Quan, Xie</p> <p>2017-12-01</p> <p>Protons tend to bond strongly with unsaturated-coordinate S element located at the edge of nano-MoS2 and are consequently reduced to H2. Therefore, increasing the active S atoms quantity will be a feasible approach to enhance hydrogen <span class="hlt">evolution</span>. Herein we developed a porous TiO2 derived from metal organic frameworks (MOFs) as scaffold to restrict the growth and inhibit the aggregation of MoS2 nanosheets. As a result, the thickness of the prepared MoS2 nanosheets was less than 3 nm (1-4 <span class="hlt">layers</span>), with more edges and active S atoms being exposed. This few-<span class="hlt">layer</span> MoS2-porous TiO2 exhibits a H2 <span class="hlt">evolution</span> rate of 897.5 μmol h-1 g-1, which is nearly twice as much as free-stand MoS2 nanosheets and twenty times more than physical mixture of MoS2 with porous TiO2. The high performance is attributed to that more active edge sites in few-<span class="hlt">layer</span> MoS2-porous TiO2 are exposed than pure MoS2. This work provides a new method to construct MOFs derived porous structures for controlling MoS2 to expose active sites for HER.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1912896G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1912896G"><span>Exploring the impact of multiple grain sizes in numerical landscape <span class="hlt">evolution</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guerit, Laure; Braun, Jean; Yuan, Xiaoping; Rouby, Delphine</p> <p>2017-04-01</p> <p>Numerical <span class="hlt">evolution</span> <span class="hlt">models</span> have been widely developed in order to understand the <span class="hlt">evolution</span> of landscape over different time-scales, but also the response of the topography to changes in external conditions, such as tectonics or climate, or to changes in the bedrock characteristics, such as its density or its erodability. Few <span class="hlt">models</span> have coupled the <span class="hlt">evolution</span> of the relief in erosion to the <span class="hlt">evolution</span> of the related area in deposition, and in addition, such <span class="hlt">models</span> generally do not consider the role of the size of the sediments reached the depositional domain. Here, we present a preliminary work based on an enhanced version of Fastscape, a very-efficient <span class="hlt">model</span> solving the stream power equation, which now integrates a sedimentary basin at the front of a relief, together with the integration of multiple grain sizes in the system. Several simulations were performed in order to explore the impact of several grain sizes in terms of stratigraphy in the marine basin. A simple setting is considered, with uniform uplift rate, precipitation rate, and rock properties onshore. The pros and cons of this approach are discussed with respect to similar simulations performed considering only flux.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3959844','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3959844"><span>Reliable recovery of the optical properties of multi-<span class="hlt">layer</span> turbid media by iteratively using a <span class="hlt">layered</span> diffusion <span class="hlt">model</span> at multiple source-detector separations</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Liao, Yu-Kai; Tseng, Sheng-Hao</p> <p>2014-01-01</p> <p>Accurately determining the optical properties of multi-<span class="hlt">layer</span> turbid media using a <span class="hlt">layered</span> diffusion <span class="hlt">model</span> is often a difficult task and could be an ill-posed problem. In this study, an iterative algorithm was proposed for solving such problems. This algorithm employed a <span class="hlt">layered</span> diffusion <span class="hlt">model</span> to calculate the optical properties of a <span class="hlt">layered</span> sample at several source-detector separations (SDSs). The optical properties determined at various SDSs were mutually referenced to complete one round of iteration and the optical properties were gradually revised in further iterations until a set of stable optical properties was obtained. We evaluated the performance of the proposed method using frequency domain Monte Carlo simulations and found that the method could robustly recover the <span class="hlt">layered</span> sample properties with various <span class="hlt">layer</span> thickness and optical property settings. It is expected that this algorithm can work with photon transport <span class="hlt">models</span> in frequency and time domain for various applications, such as determination of subcutaneous fat or muscle optical properties and monitoring the hemodynamics of muscle. PMID:24688828</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002BoLMe.104..359H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002BoLMe.104..359H"><span>Evaluating <span class="hlt">Models</span> Of The Neutral, Barotropic Planetary Boundary <span class="hlt">Layer</span> Using Integral Measures: Part Ii. <span class="hlt">Modelling</span> Observed Conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hess, G. D.; Garratt, J. R.</p> <p></p> <p>The steady-state, horizontally homogeneous, neutral, barotropiccase forms the foundation of our theoretical understanding of the planetary boundary <span class="hlt">layer</span> (PBL).While simple analytical <span class="hlt">models</span> and first-order closure <span class="hlt">models</span> simulate atmospheric observationsof this case well, more sophisticated <span class="hlt">models</span>, in general, do not. In this paperwe examine how well three higher-order closure <span class="hlt">models</span>, E - - l, E - l, and LRR - l,which have been especially modified for PBL applications, perform in predicting the behaviour of thecross-isobaric angle 0, the geostrophic drag coefficient Cg, and the integral of the dissipationrate over the boundary <span class="hlt">layer</span>, as a function of the surface Rossby number Ro. For comparison we alsoexamine the performance of three first-order closure mixing-length <span class="hlt">models</span>, two proposed byA. K. Blackadar and one by H. H. Lettau, and the performance of the standard <span class="hlt">model</span> forsecond-order closure and a modification of it designed to reduce the overprediction of turbulence inthe upper part of the boundary <span class="hlt">layer</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26932662','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26932662"><span>Vocal Development as a Guide to <span class="hlt">Modeling</span> the <span class="hlt">Evolution</span> of Language.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Oller, D Kimbrough; Griebel, Ulrike; Warlaumont, Anne S</p> <p>2016-04-01</p> <p><span class="hlt">Modeling</span> of <span class="hlt">evolution</span> and development of language has principally utilized mature units of spoken language, phonemes and words, as both targets and inputs. This approach cannot address the earliest phases of development because young infants are unable to produce such language features. We argue that units of early vocal development-protophones and their primitive illocutionary/perlocutionary forces-should be targeted in evolutionary <span class="hlt">modeling</span> because they suggest likely units of hominin vocalization/communication shortly after the split from the chimpanzee/bonobo lineage, and because early development of spontaneous vocal capability is a logically necessary step toward vocal language, a root capability without which other crucial steps toward vocal language capability are impossible. <span class="hlt">Modeling</span> of language <span class="hlt">evolution</span>/development must account for dynamic change in early communicative units of form/function across time. We argue for interactive contributions of sender/infants and receiver/caregivers in a feedback loop involving both development and <span class="hlt">evolution</span> and propose to begin computational <span class="hlt">modeling</span> at the hominin break from the primate communicative background. Copyright © 2016 Cognitive Science Society, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011PhyA..390.3524G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011PhyA..390.3524G"><span>Calibration of a stochastic health <span class="hlt">evolution</span> <span class="hlt">model</span> using NHIS data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gupta, Aparna; Li, Zhisheng</p> <p>2011-10-01</p> <p>This paper presents and calibrates an individual's stochastic health <span class="hlt">evolution</span> <span class="hlt">model</span>. In this health <span class="hlt">evolution</span> <span class="hlt">model</span>, the uncertainty of health incidents is described by a stochastic process with a finite number of possible outcomes. We construct a comprehensive health status index (HSI) to describe an individual's health status, as well as a health risk factor system (RFS) to classify individuals into different risk groups. Based on the maximum likelihood estimation (MLE) method and the method of nonlinear least squares fitting, <span class="hlt">model</span> calibration is formulated in terms of two mixed-integer nonlinear optimization problems. Using the National Health Interview Survey (NHIS) data, the <span class="hlt">model</span> is calibrated for specific risk groups. Longitudinal data from the Health and Retirement Study (HRS) is used to validate the calibrated <span class="hlt">model</span>, which displays good validation properties. The end goal of this paper is to provide a <span class="hlt">model</span> and methodology, whose output can serve as a crucial component of decision support for strategic planning of health related financing and risk management.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090012459&hterms=supercritical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsupercritical','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090012459&hterms=supercritical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsupercritical"><span>The Supercritical Pile GRB <span class="hlt">Model</span>: The Prompt to Afterglow <span class="hlt">Evolution</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Mastichiadis, A.; Kazanas, D.</p> <p>2009-01-01</p> <p>The "Supercritical Pile" is a very economical GRB <span class="hlt">model</span> that provides for the efficient conversion of the energy stored in the protons of a Relativistic Blast Wave (RBW) into radiation and at the same time produces - in the prompt GRB phase, even in the absence of any particle acceleration - a spectral peak at energy approx. 1 MeV. We extend this <span class="hlt">model</span> to include the <span class="hlt">evolution</span> of the RBW Lorentz factor Gamma and thus follow its spectral and temporal features into the early GRB afterglow stage. One of the novel features of the present treatment is the inclusion of the feedback of the GRB produced radiation on the <span class="hlt">evolution</span> of Gamma with radius. This feedback and the presence of kinematic and dynamic thresholds in the <span class="hlt">model</span> can be the sources of rich time <span class="hlt">evolution</span> which we have began to explore. In particular. one can this may obtain afterglow light curves with steep decays followed by the more conventional flatter afterglow slopes, while at the same time preserving the desirable features of the <span class="hlt">model</span>, i.e. the well defined relativistic electron source and radiative processes that produce the proper peak in the (nu)F(sub nu), spectra. In this note we present the results of a specific set of parameters of this <span class="hlt">model</span> with emphasis on the multiwavelength prompt emission and transition to the early afterglow.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28347079','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28347079"><span>Surface <span class="hlt">Evolution</span> of Nano-Textured 4H-SiC Homoepitaxial <span class="hlt">Layers</span> after High Temperature Treatments: Morphology Characterization and Graphene Growth.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liu, Xingfang; Chen, Yu; Sun, Changzheng; Guan, Min; Zhang, Yang; Zhang, Feng; Sun, Guosheng; Zeng, Yiping</p> <p>2015-09-18</p> <p>Nano-textured 4H-SiC homoepitaxial <span class="hlt">layers</span> (NSiCLs) were grown on 4H-SiC(0001) substrates using a low pressure chemical vapor deposition technique (LPCVD), and subsequently were subjected to high temperature treatments (HTTs) for investigation of their surface morphology <span class="hlt">evolution</span> and graphene growth. It was found that continuously distributed nano-scale patterns formed on NSiCLs which were about submicrons in-plane and about 100 nanometers out-of-plane in size. After HTTs under vacuum, pattern sizes reduced, and the sizes of the remains were inversely proportional to the treatment time. Referring to Raman spectra, the establishment of multi-<span class="hlt">layer</span> graphene (MLG) on NSiCL surfaces was observed. MLG with sp ² disorders was obtained from NSiCLs after a high temperature treatment under vacuum at 1700 K for two hours, while MLG without sp ² disorders was obtained under Ar atmosphere at 1900 K.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.6661Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.6661Z"><span>Holocene <span class="hlt">evolution</span> of Hans Tausen Iskappe (Greenland): merging constraints and <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zekollari, Harry; Lecavalier, Benoit S.; Huybrechts, Philippe</p> <p>2017-04-01</p> <p>In this study the Holocene <span class="hlt">evolution</span> of Hans Tausen Iskappe (western Peary Land, Greenland) is investigated. Constraints on the ice cap <span class="hlt">evolution</span> are combined with climatic records in a numerical ice flow - surface mass balance (SMB) <span class="hlt">model</span> to better understand the palaeoenvironmental and climatic <span class="hlt">evolution</span> of this region. Our simulations suggest that after disconnecting from the Greenland Ice Sheet (GrIS) the ice cap had roughly its present-day size and geometry around 8.5-9 ka ago. An ice core drilled to the bed indicates that the southern part of the ice cap subsequently disappeared during the Holocene Thermal Maximum (HTM) and this collapse can be reproduced, but the <span class="hlt">model</span> suggests that the northern part of the ice cap most likely survived this warmer period. The late Holocene growth of the ice cap to its Little Ice Age (LIA) maximum neoglacial extent can be reproduced from the temperature reconstruction. The simulations suggest that over the last millennia the local precipitation may have been up to 70-80% higher than at present. By coupling the pre-industrial temperature forcing to a post-LIA warming trend, it is concluded that the warming between the end of the LIA and the period 1961-1990 was between 1 and 2°C. In all experiments the ice flow <span class="hlt">model</span> complexity and horizontal resolution have only a minor effect on the long-term <span class="hlt">evolution</span> of the ice cap, which is largely driven by SMB changes. On the other hand the glacial isostatic adjustments (GIA) need to be accounted for in a detailed manner, as this has a large impact on the <span class="hlt">modelled</span> Holocene ice cap <span class="hlt">evolution</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017M%26PS...52.1388M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017M%26PS...52.1388M"><span>Is the Linné impact crater morphology influenced by the rheological <span class="hlt">layering</span> on the Moon's surface? Insights from numerical <span class="hlt">modeling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Martellato, Elena; Vivaldi, Valerio; Massironi, Matteo; Cremonese, Gabriele; Marzari, Francesco; Ninfo, Andrea; Haruyama, Junichi</p> <p>2017-07-01</p> <p>Linné is a simple crater, with a diameter of 2.23 km and a depth of 0.52 km, located in northwestern Mare Serenitatis. Recent high-resolution data acquired by the Lunar Reconnaissance Orbiter Camera revealed that the shape of this impact structure is best described by an inverted truncated-cone. We perform morphometric measurements, including slope and profile curvature, on the Digital Terrain <span class="hlt">Model</span> of Linné, finding the possible presence of three subtle topographic steps, at the elevation of +20, -100, and -200 m relative to the target surface. The kink at -100 m might be related to the interface between two different rheological <span class="hlt">layers</span>. Using the iSALE shock physics code, we numerically <span class="hlt">model</span> the formation of Linné crater to derive hints on the possible impact conditions and target physical properties. In the initial setup, we adopt a basaltic projectile impacting the Moon with a speed of 18 km s-1. For the local surface, we consider either one or two <span class="hlt">layers</span>, in order to test the influence of material properties or composite rheologies on the final crater morphology. The one-<span class="hlt">layer</span> <span class="hlt">model</span> shows that the largest variations in the crater shape take place when either the cohesion or the friction coefficient is varied. In particular, a cohesion of 10 kPa marks the threshold between conical- and parabolic-shaped craters. The two-<span class="hlt">layer</span> <span class="hlt">model</span> shows that the interface between the two <span class="hlt">layers</span> would be exposed at the observed depth of 100 m when an intermediate value ( 200 m) for the upper fractured <span class="hlt">layer</span> is set. We have also found that the truncated-cone morphology of Linné might originate from an incomplete collapse of the crater wall, as the breccia lens remains clustered along the crater walls, while the high-albedo deposit on the crater floor can be interpreted as a very shallow lens of fallout breccia. The <span class="hlt">modeling</span> analysis allows us to derive important clues on the impactor size (under the assumption of a vertical impact and collision velocity equal to the mean</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFM.P14A..01R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFM.P14A..01R"><span>Saharan Air <span class="hlt">Layer</span> Interaction with Hurricane Claudette (2003)</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rothman, G. S.; Gill, T. E.; Chang, C.</p> <p>2004-12-01</p> <p>It has long been observed that the Saharan Air <span class="hlt">Layer</span> (SAL), a large and seasonally-persistent <span class="hlt">layer</span> of West African aeolian dust suspended over the Atlantic Ocean, may influence the variability and intensity of easterly waves and tropical cyclones in the Atlantic basin. The radiative and conductive properties of the Saharan aerosols may contribute to warming within the dust <span class="hlt">layer</span>, creating an anomalous baroclinic zone in the tropical North Atlantic. Environmental baroclinic instability is a mechanism for conversion of potential energy to eddy kinetic energy, facilitating wave growth. However, this same baroclinic mechanism, along with the dry properties of the SAL, could also promote asymmetry in a tropical cyclone, limiting its intensity. Detailed investigations of specific cases are necessary to better understand the radiative heating or cooling impact that the Saharan aerosols cause as well as potential influences on cyclone track and intensity stemming from the aeolian dust cloud. Here, we consider the case of Claudette in 2003. On June 29, 2003, an easterly wave embedded near the southern boundary of a broad Saharan dust <span class="hlt">layer</span> emerged from the West African Coastal Bend region into the Atlantic Ocean. The wave propagated westward, reaching tropical storm intensity as Claudette in the Caribbean and developing into a hurricane just before making landfall on the southern Texas Gulf of Mexico coast on July 15. The SAL propagated in phase with this system throughout almost its entire <span class="hlt">evolution</span>. Rapid intensification of Claudette into a hurricane in the last 15 hours prior to landfall was concurrent with a decoupling from the Saharan dust intrusion, with the two following separate tracks into North America at the end of the period. We performed an investigation to understand and diagnose the interaction between the Saharan Air <span class="hlt">Layer</span> and Claudette. HYSPLIT (Hybrid Single Particle Lagrangian Integrated Trajectory <span class="hlt">Model</span>) along-trajectory potential temperature plots as</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CSR...133...37P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CSR...133...37P"><span>A <span class="hlt">model</span> for thin <span class="hlt">layer</span> formation by delayed particle settling at sharp density gradients</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Prairie, Jennifer C.; White, Brian L.</p> <p>2017-02-01</p> <p>Thin <span class="hlt">layers</span> - regions where plankton or particles accumulate vertically on scales of a few meters or less - are common in coastal waters, and have important implications for both trophic dynamics and carbon cycling. These features can form by a variety of biological and physical mechanisms, including localized growth, shear-thinning, and directed swimming. An additional mechanism may result in the formation of thin <span class="hlt">layers</span> of marine aggregates, which have been shown to decrease their settling velocity when passing through sharp density gradients, a behavior termed delayed settling. Here, we apply a simple vertical advection-diffusion <span class="hlt">model</span> to predict the properties of aggregate thin <span class="hlt">layers</span> formed by this process. We assume a constant vertical flux of particles from the surface, which is parameterized by observations from laboratory experiments with marine aggregates. The formation, maintenance, and shape of the <span class="hlt">layers</span> are described in relation to non-dimensional numbers that depend on environmental conditions and particle settling properties. In particular, <span class="hlt">model</span> results demonstrate <span class="hlt">layer</span> intensity and sharpness both increase with higher Péclet number (Pe), that is, under conditions with weaker mixing relative to <span class="hlt">layer</span> formation. Similarly, more intense and sharper <span class="hlt">layers</span> are found when the delayed settling behavior of aggregates is characterized by a lower velocity minimum. The <span class="hlt">model</span> also predicts <span class="hlt">layers</span> that are vertically asymmetric and highly "peaky" when compared with a Gaussian distribution, features often seen in thin <span class="hlt">layers</span> in natural environments. Lastly, by comparing <span class="hlt">model</span> predictions with observations of thin <span class="hlt">layers</span> in the field, we are able to gain some insight into the applicability of delayed settling as a thin <span class="hlt">layer</span> formation mechanism in different environmental conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4265145','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4265145"><span>Cancer <span class="hlt">Evolution</span>: Mathematical <span class="hlt">Models</span> and Computational Inference</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Beerenwinkel, Niko; Schwarz, Roland F.; Gerstung, Moritz; Markowetz, Florian</p> <p>2015-01-01</p> <p>Cancer is a somatic evolutionary process characterized by the accumulation of mutations, which contribute to tumor growth, clinical progression, immune escape, and drug resistance development. Evolutionary theory can be used to analyze the dynamics of tumor cell populations and to make inference about the evolutionary history of a tumor from molecular data. We review recent approaches to <span class="hlt">modeling</span> the <span class="hlt">evolution</span> of cancer, including population dynamics <span class="hlt">models</span> of tumor initiation and progression, phylogenetic methods to <span class="hlt">model</span> the evolutionary relationship between tumor subclones, and probabilistic graphical <span class="hlt">models</span> to describe dependencies among mutations. Evolutionary <span class="hlt">modeling</span> helps to understand how tumors arise and will also play an increasingly important prognostic role in predicting disease progression and the outcome of medical interventions, such as targeted therapy. PMID:25293804</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011TCD.....5..811H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011TCD.....5..811H"><span><span class="hlt">Modelling</span> the temperature <span class="hlt">evolution</span> of permafrost and seasonal frost in southern Norway during the 20th and 21st century</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hipp, T.; Etzelmüller, B.; Farbrot, H.; Schuler, T. V.</p> <p>2011-03-01</p> <p>A heat flow <span class="hlt">model</span> was used to simulate both past and future ground temperatures of mountain permafrost in Southern Norway. A reconstructed air temperature series back to 1860 was used to evaluate the permafrost <span class="hlt">evolution</span> since the end of the Little Ice Age in the region. The impact of a changing climate on discontinuous mountain permafrost until 2100 is predicted by using downscaled temperatures from an ensemble of downscaled climate <span class="hlt">models</span> for the A1B scenario. From 13 borehole locations two consecutive years of ground temperature, air temperature and snow cover data are available for <span class="hlt">model</span> calibration and validation. The boreholes are located at different elevations and in substrates having different thermal properties. With an increase of air temperature of ~+1.5 °C over 1860-2010 and an additional warming of +2.8 °C towards 2100 in air temperature, we simulate the <span class="hlt">evolution</span> of ground temperatures for the borehole locations. According to <span class="hlt">model</span> results, the active-<span class="hlt">layer</span> thickness has increased since 1860 by about 0.5-5 m and >10 m for the sites Juvvass and Tron, respectively. The simulations also suggest that at an elevation of about 1900 m a.s.l. permafrost will degrade until the end of this century with a likelihood of 55-75% given the chosen A1B scenario.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24214216','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24214216"><span>Continuous in vitro <span class="hlt">evolution</span> of a ribozyme ligase: a <span class="hlt">model</span> experiment for the <span class="hlt">evolution</span> of a biomolecule.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ledbetter, Michael P; Hwang, Tony W; Stovall, Gwendolyn M; Ellington, Andrew D</p> <p>2013-01-01</p> <p><span class="hlt">Evolution</span> is a defining criterion of life and is central to understanding biological systems. However, the timescale of evolutionary shifts in phenotype limits most classroom <span class="hlt">evolution</span> experiments to simple probability simulations. In vitro directed <span class="hlt">evolution</span> (IVDE) frequently serves as a <span class="hlt">model</span> system for the study of Darwinian <span class="hlt">evolution</span> but produces noticeable phenotypic shifts in a matter of hours. An IVDE demonstration lab would serve to both directly demonstrate how Darwinian selection can act on a pool of variants and introduce students to an essential method of modern molecular biology. To produce an IVDE demonstration lab, continuous IVDE of a T500 ribozyme ligase population has been paired with a fluorescent strand displacement reporter system to visualize the selection of improved catalytic function. A ribozyme population is taken through rounds of isothermal amplification dependent on the self-ligation of a T7 promoter. As the population is selectively enriched with better ligase activity, the strand displacement system allows for the monitoring of the population's ligation rate. The strand displacement reporter system permits the detection of ligated ribozyme. Once ligated with the T7 promoter, the 5' end of the ribozyme displaces paired fluorophore-quencher oligonucleotides, in turn, generating visible signal upon UV light excitation. As the ligation rate of the population increases, due to the selection for faster ligating species, the fluorescent signal develops more rapidly. The pairing of the continuous isothermal system with the fluorescent reporting scheme allows any user, provided with minimal materials, to <span class="hlt">model</span> the continuous directed <span class="hlt">evolution</span> of a biomolecule. Copyright © 2013 Wiley-Liss, Inc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=214946&keyword=chemical+AND+pollution+AND+boundary&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50','EPA-EIMS'); return false;" href="https://cfpub.epa.gov/si/si_public_record_report.cfm?dirEntryId=214946&keyword=chemical+AND+pollution+AND+boundary&actType=&TIMSType=+&TIMSSubTypeID=&DEID=&epaNumber=&ntisID=&archiveStatus=Both&ombCat=Any&dateBeginCreated=&dateEndCreated=&dateBeginPublishedPresented=&dateEndPublishedPresented=&dateBeginUpdated=&dateEndUpdated=&dateBeginCompleted=&dateEndCompleted=&personID=&role=Any&journalID=&publisherID=&sortBy=revisionDate&count=50"><span>Atmospheric Boundary <span class="hlt">Layer</span> <span class="hlt">Modeling</span> for Combined Meteorology and Air Quality Systems</span></a></p> <p><a target="_blank" href="http://oaspub.epa.gov/eims/query.page">EPA Science Inventory</a></p> <p></p> <p></p> <p>Atmospheric Eulerian grid <span class="hlt">models</span> for mesoscale and larger applications require sub-grid <span class="hlt">models</span> for turbulent vertical exchange processes, particularly within the Planetary Boundary <span class="hlt">Layer</span> (PSL). In combined meteorology and air quality <span class="hlt">modeling</span> systems consistent PSL <span class="hlt">modeling</span> of wi...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Complex+AND+Adaptive+AND+Systems&pg=6&id=EJ691535','ERIC'); return false;" href="https://eric.ed.gov/?q=Complex+AND+Adaptive+AND+Systems&pg=6&id=EJ691535"><span>Acquisition of Complex Systemic Thinking: Mental <span class="hlt">Models</span> of <span class="hlt">Evolution</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>d'Apollonia, Sylvia T.; Charles, Elizabeth S.; Boyd, Gary M.</p> <p>2004-01-01</p> <p>We investigated the impact of introducing college students to complex adaptive systems on their subsequent mental <span class="hlt">models</span> of <span class="hlt">evolution</span> compared to those of students taught in the same manner but with no reference to complex systems. The students' mental <span class="hlt">models</span> (derived from similarity ratings of 12 evolutionary terms using the pathfinder algorithm)…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.C43E0454G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.C43E0454G"><span>A New, Two-<span class="hlt">layer</span> Canopy Module For The Detailed Snow <span class="hlt">Model</span> SNOWPACK</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gouttevin, I.; Lehning, M.; Jonas, T.; Gustafsson, D.; Mölder, M.</p> <p>2014-12-01</p> <p>A new, two-<span class="hlt">layer</span> canopy module with thermal inertia for the detailed snow <span class="hlt">model</span> SNOWPACK is presented. Compared to the old, one-<span class="hlt">layered</span> canopy formulation with no heat mass, this module now offers a level of physical detail consistent with the detailed snow and soil representation in SNOWPACK. The new canopy <span class="hlt">model</span> is designed to reproduce the difference in thermal regimes between leafy and woody canopy elements and their impact on the underlying snowpack energy balance. The new <span class="hlt">model</span> is validated against data from an Alpine and a boreal site. Comparisons of <span class="hlt">modelled</span> sub-canopy thermal radiations to stand-scale observations at Alptal, Switzerland, demonstrate the improvements induced by our new parameterizations. The main effect is a more realistic simulation of the canopy night-time drop in temperatures. The lower drop is induced by both thermal inertia and the two-<span class="hlt">layer</span> representation. A specific result is that such a performance cannot be achieved by a single-<span class="hlt">layered</span> canopy <span class="hlt">model</span>. The impact of the new parameterizations on the <span class="hlt">modelled</span> dynamics of the sub-canopy snowpack is analysed and yields consistent results, but the frequent occurrence of mixed-precipitation events at Alptal prevents a conclusive assessment of <span class="hlt">model</span> performances against snow data.Without specific tuning, the <span class="hlt">model</span> is also able to reproduce the measured summertime tree trunk temperatures and biomass heat storage at the boreal site of Norunda, Sweden, with an increased accuracy in amplitude and phase. Overall, the SNOWPACK <span class="hlt">model</span> with its enhanced canopy module constitutes a unique (in its physical process representation) atmosphere-to-soil-through-canopy-and-snow <span class="hlt">modelling</span> chain.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23782806','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23782806"><span>Plenoptic <span class="hlt">layer</span>-based <span class="hlt">modeling</span> for image based rendering.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Pearson, James; Brookes, Mike; Dragotti, Pier Luigi</p> <p>2013-09-01</p> <p>Image based rendering is an attractive alternative to <span class="hlt">model</span> based rendering for generating novel views because of its lower complexity and potential for photo-realistic results. To reduce the number of images necessary for alias-free rendering, some geometric information for the 3D scene is normally necessary. In this paper, we present a fast automatic <span class="hlt">layer</span>-based method for synthesizing an arbitrary new view of a scene from a set of existing views. Our algorithm takes advantage of the knowledge of the typical structure of multiview data to perform occlusion-aware <span class="hlt">layer</span> extraction. In addition, the number of depth <span class="hlt">layers</span> used to approximate the geometry of the scene is chosen based on plenoptic sampling theory with the <span class="hlt">layers</span> placed non-uniformly to account for the scene distribution. The rendering is achieved using a probabilistic interpolation approach and by extracting the depth <span class="hlt">layer</span> information on a small number of key images. Numerical results demonstrate that the algorithm is fast and yet is only 0.25 dB away from the ideal performance achieved with the ground-truth knowledge of the 3D geometry of the scene of interest. This indicates that there are measurable benefits from following the predictions of plenoptic theory and that they remain true when translated into a practical system for real world data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920043091&hterms=high+reaction+chemicals&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dhigh%2Breaction%2Bchemicals','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920043091&hterms=high+reaction+chemicals&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3Dhigh%2Breaction%2Bchemicals"><span><span class="hlt">Model</span> free simulations of a high speed reacting mixing <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Steinberger, Craig J.</p> <p>1992-01-01</p> <p>The effects of compressibility, chemical reaction exothermicity and non-equilibrium chemical <span class="hlt">modeling</span> in a combusting plane mixing <span class="hlt">layer</span> were investigated by means of two-dimensional <span class="hlt">model</span> free numerical simulations. It was shown that increased compressibility generally had a stabilizing effect, resulting in reduced mixing and chemical reaction conversion rate. The appearance of 'eddy shocklets' in the flow was observed at high convective Mach numbers. Reaction exothermicity was found to enhance mixing at the initial stages of the <span class="hlt">layer</span>'s growth, but had a stabilizing effect at later times. Calculations were performed for a constant rate chemical rate kinetics <span class="hlt">model</span> and an Arrhenius type kinetics prototype. The Arrhenius <span class="hlt">model</span> was found to cause a greater temperature increase due to reaction than the constant kinetics <span class="hlt">model</span>. This had the same stabilizing effect as increasing the exothermicity of the reaction. Localized flame quenching was also observed when the Zeldovich number was relatively large.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017A%26A...598A.121F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017A%26A...598A.121F"><span>Tracing the <span class="hlt">evolution</span> of the Galactic bulge with chemodynamical <span class="hlt">modelling</span> of alpha-elements</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Friaça, A. C. S.; Barbuy, B.</p> <p>2017-02-01</p> <p>Context. Galactic bulge abundances can be best understood as indicators of bulge formation and nucleosynthesis processes by comparing them with chemo-dynamical <span class="hlt">evolution</span> <span class="hlt">models</span>. Aims: The aim of this work is to study the abundances of alpha-elements in the Galactic bulge, including a revision of the oxygen abundance in a sample of 56 bulge red giants. Methods: Literature abundances for O, Mg, Si, Ca and Ti in Galactic bulge stars are compared with chemical <span class="hlt">evolution</span> <span class="hlt">models</span>. For oxygen in particular, we reanalysed high-resolution spectra obtained using FLAMES+UVES on the Very Large Telescope, now taking each star's carbon abundances, derived from CI and C2 lines, into account simultaneously. Results: We present a chemical <span class="hlt">evolution</span> <span class="hlt">model</span> of alpha-element enrichment in a massive spheroid that represents a typical classical bulge <span class="hlt">evolution</span>. The code includes multi-zone chemical <span class="hlt">evolution</span> coupled with hydrodynamics of the gas. Comparisons between the <span class="hlt">model</span> predictions and the abundance data suggest a typical bulge formation timescale of 1-2 Gyr. The main constraint on the bulge <span class="hlt">evolution</span> is provided by the O data from analyses that have taken the C abundance and dissociative equilibrium into account. Mg, Si, Ca and Ti trends are well reproduced, whereas the level of overabundance critically depends on the adopted nucleosynthesis prescriptions. Observations collected both at the European Southern Observatory, Paranal, Chile (ESO programmes 71.B-0617A, 73.B0074A, and GTO 71.B-0196)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29369715','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29369715"><span>The Institutional Approach for <span class="hlt">Modeling</span> the <span class="hlt">Evolution</span> of Human Societies.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Powers, Simon T</p> <p>2018-01-01</p> <p>Artificial life is concerned with understanding the dynamics of human societies. A defining feature of any society is its institutions. However, defining exactly what an institution is has proven difficult, with authors often talking past each other. This article presents a dynamic <span class="hlt">model</span> of institutions, which views them as political game forms that generate the rules of a group's economic interactions. Unlike most prior work, the framework presented here allows for the construction of explicit <span class="hlt">models</span> of the <span class="hlt">evolution</span> of institutional rules. It takes account of the fact that group members are likely to try to create rules that benefit themselves. Following from this, it allows us to determine the conditions under which self-interested individuals will create institutional rules that support cooperation-for example, that prevent a tragedy of the commons. The article finishes with an example of how a <span class="hlt">model</span> of the <span class="hlt">evolution</span> of institutional rewards and punishments for promoting cooperation can be created. It is intended that this framework will allow artificial life researchers to examine how human groups can themselves create conditions for cooperation. This will help provide a better understanding of historical human social <span class="hlt">evolution</span>, and facilitate the resolution of pressing societal social dilemmas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20030025288&hterms=moisture+condensation&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmoisture%2Bcondensation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20030025288&hterms=moisture+condensation&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dmoisture%2Bcondensation"><span>Lidar Measurements of Wind, Moisture and Boundary <span class="hlt">Layer</span> <span class="hlt">Evolution</span> in a Dryline During IHOP2002</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Demoz, Belay; Evans, Keith; DiGirolamo, Paolo; Wang, Zhien; Whiteman, David; Schwemmer, Geary; Gentry, Bruce; Miller, David</p> <p>2003-01-01</p> <p>Variability in the convective boundary <span class="hlt">layer</span> moisture, wind and temperature fields and their importance in the forecasting and understanding of storms have been discussed in the literature. These variations have been reported in relation to frontal zones, stationary boundaries and during horizontal convective rolls. While all three vary substantially in the convective boundary <span class="hlt">layer</span>, moisture poses a particular challenge. Moisture or water vapor concentration (expressed as a mass mixing ratio, g/kg), is conserved in all meteorological processes except condensation and evaporation. The water vapor mixing ratio often remains distinct across an air -mass boundary even when the temperature difference is indistinct. These properties make it an ideal choice in visualizing and understanding many of the atmosphere's dynamic features. However, it also presents a unique measurement challenge because water vapor content can vary by more than three orders of magnitude in the troposphere. Characterization of the 3D-distribution of water vapor is also difficult as water vapor observations can suffer from large sampling errors and substantial variability both in the vertical and horizontal. This study presents groundbased measurements of wind, boundary <span class="hlt">layer</span> structure and water vapor mixing ratio measurements observed by three co-located lidars. This presentation will focus on the <span class="hlt">evolution</span> and variability of moisture and wind in the boundary <span class="hlt">layer</span> during a dry line event that occurred on 22 May 2002. These data sets and analyses are unique in that they combine simultaneous measurements of wind, moisture and CBL structure to study the detailed thermal variability in and around clear air updrafts during a dryline event. It will quantify the variation caused by, in and around buoyant plumes and across a dryline. The data presented here were collected in the panhandle of Oklahoma as part of the International BO Project (IHOP-2002), a field experiment that took place over the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28618540','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28618540"><span>Six-vertex <span class="hlt">model</span> and Schramm-Loewner <span class="hlt">evolution</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kenyon, Richard; Miller, Jason; Sheffield, Scott; Wilson, David B</p> <p>2017-05-01</p> <p>Square ice is a statistical mechanics <span class="hlt">model</span> for two-dimensional ice, widely believed to have a conformally invariant scaling limit. We associate a Peano (space-filling) curve to a square ice configuration, and more generally to a so-called six-vertex <span class="hlt">model</span> configuration, and argue that its scaling limit is a space-filling version of the random fractal curve SLE_{κ}, Schramm-Loewner <span class="hlt">evolution</span> with parameter κ, where 4<κ≤12+8sqrt[2]. For square ice, κ=12. At the "free-fermion point" of the six-vertex <span class="hlt">model</span>, κ=8+4sqrt[3]. These unusual values lie outside the classical interval 2≤κ≤8.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JGRC..115.3011S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JGRC..115.3011S"><span>An analytical <span class="hlt">model</span> of capped turbulent oscillatory bottom boundary <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shimizu, Kenji</p> <p>2010-03-01</p> <p>An analytical <span class="hlt">model</span> of capped turbulent oscillatory bottom boundary <span class="hlt">layers</span> (BBLs) is proposed using eddy viscosity of a quadratic form. The common definition of friction velocity based on maximum bottom shear stress is found unsatisfactory for BBLs under rotating flows, and a possible extension based on turbulent kinetic energy balance is proposed. The <span class="hlt">model</span> solutions show that the flow may slip at the top of the boundary <span class="hlt">layer</span> due to capping by the water surface or stratification, reducing the bottom shear stress, and that the Earth's rotation induces current and bottom shear stress components perpendicular to the interior flow with a phase lag (or lead). Comparisons with field and numerical experiments indicate that the <span class="hlt">model</span> predicts the essential characteristics of the velocity profiles, although the agreement is rather qualitative due to assumptions of quadratic eddy viscosity with time-independent friction velocity and a well-mixed boundary <span class="hlt">layer</span>. On the other hand, the predicted linear friction coefficients, phase lead, and veering angle at the bottom agreed with available data with an error of 3%-10%, 5°-10°, and 5°-10°, respectively. As an application of the <span class="hlt">model</span>, the friction coefficients are used to calculate e-folding decay distances of progressive internal waves with a semidiurnal frequency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1986GApFD..35....1H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1986GApFD..35....1H"><span>The <span class="hlt">evolution</span> of an unsteady translating nonlinear rossby-wave critical <span class="hlt">layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haynes, Peter H.; Cowley, Stephen J.</p> <p></p> <p>When a monochromatic Rossby wave is forced on a flow which is slowly varying in time, the location of the critical line, where the phase speed of the wave is equal to that of the flow, also slowly changes. It is shown that this translation can play an important role in the vorticity balance near the critical line. The behavior of the translating critical <span class="hlt">layer</span> is analyzed for various values of y, a parameter which measures the relative importance of nonlinear advection and translation. First, the vorticity equation in the critical <span class="hlt">layer</span> is solved numerically in an important special case, where the velocity field in the critical <span class="hlt">layer</span> is independent of the vorticity distribution and constant in time. The solutions reveal a number of new aspects of the behavior which are introduced by the translation, including the formation of a wake behind the critical <span class="hlt">layer</span>, and the possibility of "trapping" of fluid particles in the critical <span class="hlt">layer</span> if y exceeds a threshold value. Viewed in a frame of reference moving with the critical line the vorticity distribution may tend to a steady state, except in a "vorticity front" far downstream in the wake. If streamlines in the critical <span class="hlt">layer</span> are open this steady state may be a predominantly inviscid one; if they are closed a steady state is possible only with non-zero dissipation. For both the unsteady and steady flows the translation allows the "logarithmic phase jump" across the critical <span class="hlt">layer</span>, 4, to be non-zero and negative. Hence, even when the viscosity is vanishingly small, the critical <span class="hlt">layer</span> can act as a strong "absorber" of Eliassen-Palm wave activity. Second, steady-state solutions are obtained numerically for a case when the velocity field in the critical <span class="hlt">layer</span> is not independent of the vorticity distribution there. The interaction restricts the formation of closed streamlines, and an asymptotic open-streamline solution for large y can be found. The critical <span class="hlt">layer</span> again acts an absorber of wave activity, but with decreasing e</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994STIN...9522080W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994STIN...9522080W"><span><span class="hlt">Modelling</span> multimedia teleservices with OSI upper <span class="hlt">layers</span> framework: Short paper</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Widya, I.; Vanrijssen, E.; Michiels, E.</p> <p></p> <p>The paper presents the use of the concepts and <span class="hlt">modelling</span> principles of the Open Systems Interconnection (OSI) upper <span class="hlt">layers</span> structure in the <span class="hlt">modelling</span> of multimedia teleservices. It puts emphasis on the revised Application <span class="hlt">Layer</span> Structure (OSI/ALS). OSI/ALS is an object based reference <span class="hlt">model</span> which intends to coordinate the development of application oriented services and protocols in a consistent and modular way. It enables the rapid deployment and integrated use of these services. The paper emphasizes further on the nesting structure defined in OSI/ALS which allows the design of scalable and user tailorable/controllable teleservices. OSI/ALS consistent teleservices are moreover implementable on communication platforms of different capabilities. An analysis of distributed multimedia architectures which can be found in the literature, confirms the ability of the OSI/ALS framework to <span class="hlt">model</span> the interworking functionalities of teleservices.</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('http://adsabs.harvard.edu/abs/2017AcGeo..65.1119P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AcGeo..65.1119P"><span>Effect of surface wave propagation in a four-<span class="hlt">layered</span> oceanic crust <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Paul, Pasupati; Kundu, Santimoy; Mandal, Dinbandhu</p> <p>2017-12-01</p> <p>Dispersion of Rayleigh type surface wave propagation has been discussed in four-<span class="hlt">layered</span> oceanic crust. It includes a sandy <span class="hlt">layer</span> over a crystalline elastic half-space and over it there are two more layers—on the top inhomogeneous liquid <span class="hlt">layer</span> and under it a liquid-saturated porous <span class="hlt">layer</span>. Frequency equation is obtained in the form of determinant. The effects of the width of different <span class="hlt">layers</span> as well as the inhomogeneity of liquid <span class="hlt">layer</span>, sandiness of sandy <span class="hlt">layer</span> on surface waves are depicted and shown graphically by considering all possible case of the particular <span class="hlt">model</span>. Some special cases have been deduced, few special cases give the dispersion equation of Scholte wave and Stoneley wave, some of which have already been discussed elsewhere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/678753-one-dimensional-sectional-model-simulate-multicomponent-aerosol-dynamics-marine-boundary-layer-model-application','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/678753-one-dimensional-sectional-model-simulate-multicomponent-aerosol-dynamics-marine-boundary-layer-model-application"><span>A one-dimensional sectional <span class="hlt">model</span> to simulate multicomponent aerosol dynamics in the marine boundary <span class="hlt">layer</span> 2. <span class="hlt">Model</span> application</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>Fitzgerald, James W.; Hoppel, William A.; Frick, Glendon M.</p> <p>1998-07-01</p> <p>The dynamics of aerosols in the marine boundary <span class="hlt">layer</span> (MBL) are simulated with the marine boundary <span class="hlt">layer</span> aerosol <span class="hlt">model</span> (MARBLES), a one-dimensional, multicomponent sectional aerosol <span class="hlt">model</span> [{ital Fitzgerald} {ital et al.}, this issue; {ital Gelbard} {ital et al.}, this issue]. First, to illustrate how the various aerosol processes influence the particle size distribution, the <span class="hlt">model</span> was run with one or two processes operating on the same initial size distribution. Because of current interest in the effects of cloud processing of aerosols and exchange of aerosols with the free troposphere (FT) on marine aerosol size distributions, these two processes are examinedmore » in considerable detail. The simulations show that the effect of cloud processing (characteristic double-peaked size distribution) in the upper part of the MBL is manifested at the surface on a timescale that is much faster than changes due to exchange with the FT, assuming a typical exchange velocity of 0.6 cmthinsps{sup {minus}1}. The <span class="hlt">model</span> predicts that the FT can be a significant source of particles for the MBL in the size range of the cloud-processing minimum, between the unactivated interstitial particles and the cloud condensation nuclei (CCN) which have grown as a result of conversion of dissolved SO{sub 2} to sulfate in cloud droplets. The <span class="hlt">model</span> was also used to simulate the <span class="hlt">evolution</span> of the aerosol size distribution in an air mass advecting from the east coast of the United States out over the ocean for up to 10 days. The modification of a continental aerosol size distribution to one that is remote marine in character occurs on a timescale of 6{endash}8 days. Nucleation was not observed in the base case 10-day advection simulation which assumed rather typical meteorological conditions. However, significant nucleation was predicted under a more favorable (albeit, atypical) combination of conditions which included significant precipitation scavenging (5 mmthinsph{sup {minus}1} of rain for 12</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008MNRAS.384..843M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008MNRAS.384..843M"><span>Validity of strong lensing statistics for constraints on the galaxy <span class="hlt">evolution</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Matsumoto, Akiko; Futamase, Toshifumi</p> <p>2008-02-01</p> <p>We examine the usefulness of the strong lensing statistics to constrain the <span class="hlt">evolution</span> of the number density of lensing galaxies by adopting the values of the cosmological parameters determined by recent Wilkinson Microwave Anisotropy Probe observation. For this purpose, we employ the lens-redshift test proposed by Kochanek and constrain the parameters in two <span class="hlt">evolution</span> <span class="hlt">models</span>, simple power-law <span class="hlt">model</span> characterized by the power-law indexes νn and νv, and the <span class="hlt">evolution</span> <span class="hlt">model</span> by Mitchell et al. based on cold dark matter structure formation scenario. We use the well-defined lens sample from the Sloan Digital Sky Survey (SDSS) and this is similarly sized samples used in the previous studies. Furthermore, we adopt the velocity dispersion function of early-type galaxies based on SDSS DR1 and DR5. It turns out that the indexes of power-law <span class="hlt">model</span> are consistent with the previous studies, thus our results indicate the mild <span class="hlt">evolution</span> in the number and velocity dispersion of early-type galaxies out to z = 1. However, we found that the values for p and q used by Mitchell et al. are inconsistent with the presently available observational data. More complete sample is necessary to withdraw more realistic determination on these parameters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..MARK38008Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..MARK38008Y"><span>First-principles study of oxygen <span class="hlt">evolution</span> reaction on Co doped NiFe-<span class="hlt">layered</span> double hydroxides</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, Jie; Perdew, John; Yan, Qimin</p> <p></p> <p>The conversion of solar energy to renewable fuels is a grand challenge. One of the crucial steps for this energy conversion process is the discovery of efficient catalysts with lower overpotential for the oxygen <span class="hlt">evolution</span> reaction (OER). <span class="hlt">Layered</span> double hydroxides (LDH) with earth abundant elements such as Ni and Fe have been found as promising OER catalysts and shown to be active for water oxidation. Doping is one of the feasible ways to even lower the overpotential of host materials and breaks the linear scaling law. In this talk we'll present our study on the reaction mechanism of OER on pure and Co-doped NiFe-LDH systems in alkaline solution. We study the absorption energetics of reaction intermediate states and calculate the thermodynamic reaction energy using density functional theory with the PBE +U and the newly developed SCAN functionals. It is shown that the NiFe-LDH system with Co dopants has lower overpotential and higher activity compared with the undoped system. The improvement in activity is related to the presence of Co states in the electronic structure. The work provides a clear clue for the further improvement of the OER activity of LDH systems by chemical doping. The work was supported as part of the Center for the Computational Design of Functional <span class="hlt">Layered</span> Materials, an Energy Frontier Research Center funded by the U.S. Department of Energy, Office of Science.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25215763','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25215763"><span>Punctuated equilibrium and shock waves in molecular <span class="hlt">models</span> of biological <span class="hlt">evolution</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Saakian, David B; Ghazaryan, Makar H; Hu, Chin-Kun</p> <p>2014-08-01</p> <p>We consider the dynamics in infinite population <span class="hlt">evolution</span> <span class="hlt">models</span> with a general symmetric fitness landscape. We find shock waves, i.e., discontinuous transitions in the mean fitness, in <span class="hlt">evolution</span> dynamics even with smooth fitness landscapes, which means that the search for the optimal <span class="hlt">evolution</span> trajectory is more complicated. These shock waves appear in the case of positive epistasis and can be used to represent punctuated equilibria in biological <span class="hlt">evolution</span> during long geological time scales. We find exact analytical solutions for discontinuous dynamics at the large-genome-length limit and derive optimal mutation rates for a fixed fitness landscape to send the population from the initial configuration to some final configuration in the fastest way.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980073396','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980073396"><span>Two-<span class="hlt">Layer</span> Variable Infiltration Capacity Land Surface Representation for General Circulation <span class="hlt">Models</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Xu, L.</p> <p>1994-01-01</p> <p>A simple two-<span class="hlt">layer</span> variable infiltration capacity (VIC-2L) land surface <span class="hlt">model</span> suitable for incorporation in general circulation <span class="hlt">models</span> (GCMs) is described. The <span class="hlt">model</span> consists of a two-<span class="hlt">layer</span> characterization of the soil within a GCM grid cell, and uses an aerodynamic representation of latent and sensible heat fluxes at the land surface. The effects of GCM spatial subgrid variability of soil moisture and a hydrologically realistic runoff mechanism are represented in the soil <span class="hlt">layers</span>. The <span class="hlt">model</span> was tested using long-term hydrologic and climatalogical data for Kings Creek, Kansas to estimate and validate the hydrological parameters. Surface flux data from three First International Satellite Land Surface Climatology Project Field Experiments (FIFE) intensive field compaigns in the summer and fall of 1987 in central Kansas, and from the Anglo-Brazilian Amazonian Climate Observation Study (ABRACOS) in Brazil were used to validate the mode-simulated surface energy fluxes and surface temperature.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016LaPhL..13c5105L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016LaPhL..13c5105L"><span><span class="hlt">Modeling</span> of the spectral <span class="hlt">evolution</span> in a narrow-linewidth fiber amplifier</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Wei; Kuang, Wenjun; Jiang, Man; Xu, Jiangming; Zhou, Pu; Liu, Zejin</p> <p>2016-03-01</p> <p>Efficient numerical <span class="hlt">modeling</span> of the spectral <span class="hlt">evolution</span> in a narrow-linewidth fiber amplifier is presented. By describing the seeds using a statistical <span class="hlt">model</span> and simulating the amplification process through power balanced equations combined with the nonlinear Schrödinger equations, the spectral <span class="hlt">evolution</span> of different seeds in the fiber amplifier can be evaluated accurately. The simulation results show that the output spectra are affected by the temporal stability of the seeds and the seeds with constant amplitude in time are beneficial to maintain the linewidth of the seed in the fiber amplifier.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000034095','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000034095"><span>A Melting <span class="hlt">Layer</span> <span class="hlt">Model</span> for Passive/Active Microwave Remote Sensing Applications. Part 1; <span class="hlt">Model</span> Formulation and Comparison with Observations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Olson, William S.; Bauer, Peter; Viltard, Nicolas F.; Johnson, Daniel E.; Tao, Wei-Kuo</p> <p>2000-01-01</p> <p>In this study, a 1-D steady-state microphysical <span class="hlt">model</span> which describes the vertical distribution of melting precipitation particles is developed. The <span class="hlt">model</span> is driven by the ice-phase precipitation distributions just above the freezing level at applicable gridpoints of "parent" 3-D cloud-resolving <span class="hlt">model</span> (CRM) simulations. It extends these simulations by providing the number density and meltwater fraction of each particle in finely separated size categories through the melting <span class="hlt">layer</span>. The depth of the <span class="hlt">modeled</span> melting <span class="hlt">layer</span> is primarily determined by the initial material density of the ice-phase precipitation. The radiative properties of melting precipitation at microwave frequencies are calculated based upon different methods for describing the dielectric properties of mixed phase particles. Particle absorption and scattering efficiencies at the Tropical Rainfall Measuring Mission Microwave Imager frequencies (10.65 to 85.5 GHz) are enhanced greatly for relatively small (approx. 0.1) meltwater fractions. The relatively large number of partially-melted particles just below the freezing level in stratiform regions leads to significant microwave absorption, well-exceeding the absorption by rain at the base of the melting <span class="hlt">layer</span>. Calculated precipitation backscatter efficiencies at the Precipitation Radar frequency (13.8 GHz) increase in proportion to the particle meltwater fraction, leading to a "bright-band" of enhanced radar reflectivities in agreement with previous studies. The radiative properties of the melting <span class="hlt">layer</span> are determined by the choice of dielectric <span class="hlt">models</span> and the initial water contents and material densities of the "seeding" ice-phase precipitation particles. Simulated melting <span class="hlt">layer</span> profiles based upon snow described by the Fabry-Szyrmer core-shell dielectric <span class="hlt">model</span> and graupel described by the Maxwell-Garnett water matrix dielectric <span class="hlt">model</span> lead to reasonable agreement with radar-derived melting <span class="hlt">layer</span> optical depth distributions. Moreover, control profiles</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JAP...120l3903I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JAP...120l3903I"><span>Micromagnetic <span class="hlt">modeling</span> of the shielding properties of nanoscale ferromagnetic <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Iskandarova, I. M.; Knizhnik, A. A.; Popkov, A. F.; Potapkin, B. V.; Stainer, Q.; Lombard, L.; Mackay, K.</p> <p>2016-09-01</p> <p>Ferromagnetic shields are widely used to concentrate magnetic fields in a target region of space. Such shields are also used in spintronic nanodevices such as magnetic random access memory and magnetic logic devices. However, the shielding properties of nanostructured shields can differ considerably from those of macroscopic samples. In this work, we investigate the shielding properties of nanostructured NiFe <span class="hlt">layers</span> around a current line using a finite element micromagnetic <span class="hlt">model</span>. We find that thin ferromagnetic <span class="hlt">layers</span> demonstrate saturation of magnetization under an external magnetic field, which reduces the shielding efficiency. Moreover, we show that the shielding properties of nanoscale ferromagnetic <span class="hlt">layers</span> strongly depend on the uniformity of the <span class="hlt">layer</span> thickness. Magnetic anisotropy in ultrathin ferromagnetic <span class="hlt">layers</span> can also influence their shielding efficiency. In addition, we show that domain walls in nanoscale ferromagnetic shields can induce large increases and decreases in the generated magnetic field. Therefore, ferromagnetic shields for spintronic nanodevices require careful design and precise fabrication.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008ConSc..20..135G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008ConSc..20..135G"><span>Exploring social structure effect on language <span class="hlt">evolution</span> based on a computational <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gong, Tao; Minett, James; Wang, William</p> <p>2008-06-01</p> <p>A compositionality-regularity coevolution <span class="hlt">model</span> is adopted to explore the effect of social structure on language emergence and maintenance. Based on this <span class="hlt">model</span>, we explore language <span class="hlt">evolution</span> in three experiments, and discuss the role of a popular agent in language <span class="hlt">evolution</span>, the relationship between mutual understanding and social hierarchy, and the effect of inter-community communications and that of simple linguistic features on convergence of communal languages in two communities. This work embodies several important interactions during social learning, and introduces a new approach that manipulates individuals' probabilities to participate in social interactions to study the effect of social structure. We hope it will stimulate further theoretical and empirical explorations on language <span class="hlt">evolution</span> in a social environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26PSL.460..293C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26PSL.460..293C"><span>The <span class="hlt">layered</span> <span class="hlt">evolution</span> of fabric and microstructure of snow at Point Barnola, Central East Antarctica</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Calonne, Neige; Montagnat, Maurine; Matzl, Margret; Schneebeli, Martin</p> <p>2017-02-01</p> <p>Snow fabric, defined as the distribution of the c-axis orientations of the ice crystals in snow, is poorly known. So far, only one study exits that measured snow fabric based on a statistically representative technique. This recent study has revealed the impact of temperature gradient metamorphism on the <span class="hlt">evolution</span> of fabric in natural snow, based on cold laboratory experiments. On polar ice sheets, snow properties are currently investigated regarding their strong variability in time and space, notably because of their potential influence on firn processes and consequently on ice core analysis. Here, we present measurements of fabric and microstructure of snow from Point Barnola, East Antarctica (close to Dome C). We analyzed a snow profile from 0 to 3 m depth, where temperature gradients occur. The main contributions of the paper are (1) a detailed characterization of snow in the upper meters of the ice sheet, especially by providing data on snow fabric, and (2) the study of a fundamental snow process, never observed up to now in a natural snowpack, namely the role of temperature gradient metamorphism on the <span class="hlt">evolution</span> of the snow fabric. Snow samples were scanned by micro-tomography to measure continuous profiles of microstructural properties (density, specific surface area and pore thickness). Fabric analysis was performed using an automatic ice texture analyzer on 77 representative thin sections cut out from the samples. Different types of snow fabric could be identified and persist at depth. Snow fabric is significantly correlated with snow microstructure, pointing to the simultaneous influence of temperature gradient metamorphism on both properties. We propose a mechanism based on preferential grain growth to explain the fabric <span class="hlt">evolution</span> under temperature gradients. Our work opens the question of how such a <span class="hlt">layered</span> profile of fabric and microstructure evolves at depth and further influences the physical and mechanical properties of snow and firn. More generally</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3855641','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3855641"><span>Spatial and Feature-Based Attention in a <span class="hlt">Layered</span> Cortical Microcircuit <span class="hlt">Model</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>Wagatsuma, Nobuhiko; Potjans, Tobias C.; Diesmann, Markus; Sakai, Ko; Fukai, Tomoki</p> <p>2013-01-01</p> <p>Directing attention to the spatial location or the distinguishing feature of a visual object modulates neuronal responses in the visual cortex and the stimulus discriminability of subjects. However, the spatial and feature-based modes of attention differently influence visual processing by changing the tuning properties of neurons. Intriguingly, neurons' tuning curves are modulated similarly across different visual areas under both these modes of attention. Here, we explored the mechanism underlying the effects of these two modes of visual attention on the orientation selectivity of visual cortical neurons. To do this, we developed a <span class="hlt">layered</span> microcircuit <span class="hlt">model</span>. This <span class="hlt">model</span> describes multiple orientation-specific microcircuits sharing their receptive fields and consisting of <span class="hlt">layers</span> 2/3, 4, 5, and 6. These microcircuits represent a functional grouping of cortical neurons and mutually interact via lateral inhibition and excitatory connections between groups with similar selectivity. The individual microcircuits receive bottom-up visual stimuli and top-down attention in different <span class="hlt">layers</span>. A crucial assumption of the <span class="hlt">model</span> is that feature-based attention activates orientation-specific microcircuits for the relevant feature selectively, whereas spatial attention activates all microcircuits homogeneously, irrespective of their orientation selectivity. Consequently, our <span class="hlt">model</span> simultaneously accounts for the multiplicative scaling of neuronal responses in spatial attention and the additive modulations of orientation tuning curves in feature-based attention, which have been observed widely in various visual cortical areas. Simulations of the <span class="hlt">model</span> predict contrasting differences between excitatory and inhibitory neurons in the two modes of attentional modulations. Furthermore, the <span class="hlt">model</span> replicates the modulation of the psychophysical discriminability of visual stimuli in the presence of external noise. Our <span class="hlt">layered</span> <span class="hlt">model</span> with a biologically suggested laminar structure describes</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1333335-late-time-mixing-sensitivity-initial-broadband-surface-roughness-high-energy-density-shear-layers','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1333335-late-time-mixing-sensitivity-initial-broadband-surface-roughness-high-energy-density-shear-layers"><span>Late-Time Mixing Sensitivity to Initial Broadband Surface Roughness in High-Energy-Density Shear <span class="hlt">Layers</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Flippo, K. A.; Doss, F. W.; Kline, J. L.; ...</p> <p>2016-11-23</p> <p>While using a large volume high-energy-density fluid shear experiment ( 8.5 cm 3 ) at the National Ignition Facility, we have demonstrated for the first time the ability to significantly alter the <span class="hlt">evolution</span> of a supersonic sheared mixing <span class="hlt">layer</span> by controlling the initial conditions of that <span class="hlt">layer</span>. Furthermore, by altering the initial surface roughness of the tracer foil, we demonstrate the ability to transition the shear mixing <span class="hlt">layer</span> from a highly ordered system of coherent structures to a randomly ordered system with a faster growing mix <span class="hlt">layer</span>, indicative of strong mixing in the <span class="hlt">layer</span> at a temperature of severalmore » tens of electron volts and at near solid density. Moreover, simulations using a turbulent-mix <span class="hlt">model</span> show good agreement with the experimental results and poor agreement without turbulent mix.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/467663-turbulence-structure-marine-stable-boundary-layer-over-baltic-sea','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/467663-turbulence-structure-marine-stable-boundary-layer-over-baltic-sea"><span>Turbulence structure of the marine stable boundary <span class="hlt">layer</span> over the Baltic Sea</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>Smedman, A.S.; Hoegstroem, U.</p> <p></p> <p>For more than half of the year the land surfaces surrounding the Baltic Sea is warmer than the sea surface, and the marine boundary <span class="hlt">layer</span> over the Baltic is stable. Observations, at various sites in the Baltic Sea area during the last decade. also indicate frequent occurrence of low-level jets at the top of the stable boundary <span class="hlt">layer</span>. In many cases the marine jet can be considered as an analogy in space to the <span class="hlt">evolution</span> of the nocturnal jet with time. The frictional decoupling occurs when warm air over the land is flowing out over the sea. Data from twomore » areas together with <span class="hlt">model</span> simulations are used in this study to characterize turbulence structure in the marine boundary <span class="hlt">layer</span>. The measurements include profiles of wind and temperature on towers situated at two isolated islands, together with turbulence recordings and aircraft measurements. Also wave height and water surface temperature have been measured. The <span class="hlt">model</span> simulations are performed with a second-order closure <span class="hlt">model</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70000446','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70000446"><span><span class="hlt">Modeling</span> the <span class="hlt">evolution</span> of channel shape: Balancing computational efficiency with hydraulic fidelity</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Wobus, C.W.; Kean, J.W.; Tucker, G.E.; Anderson, R. Scott</p> <p>2008-01-01</p> <p>The cross-sectional shape of a natural river channel controls the capacity of the system to carry water off a landscape, to convey sediment derived from hillslopes, and to erode its bed and banks. Numerical <span class="hlt">models</span> that describe the response of a landscape to changes in climate or tectonics therefore require formulations that can accommodate <span class="hlt">evolution</span> of channel cross-sectional geometry. However, fully two-dimensional (2-D) flow <span class="hlt">models</span> are too computationally expensive to implement in large-scale landscape <span class="hlt">evolution</span> <span class="hlt">models</span>, while available simple empirical relationships between width and discharge do not adequately capture the dynamics of channel adjustment. We have developed a simplified 2-D numerical <span class="hlt">model</span> of channel <span class="hlt">evolution</span> in a cohesive, detachment-limited substrate subject to steady, unidirectional flow. Erosion is assumed to be proportional to boundary shear stress, which is calculated using an approximation of the flow field in which log-velocity profiles are assumed to apply along vectors that are perpendicular to the local channel bed. <span class="hlt">Model</span> predictions of the velocity structure, peak boundary shear stress, and equilibrium channel shape compare well with predictions of a more sophisticated but more computationally demanding ray-isovel <span class="hlt">model</span>. For example, the mean velocities computed by the two <span class="hlt">models</span> are consistent to within ???3%, and the predicted peak shear stress is consistent to within ???7%. Furthermore, the shear stress distributions predicted by our <span class="hlt">model</span> compare favorably with available laboratory measurements for prescribed channel shapes. A modification to our simplified code in which the flow includes a high-velocity core allows the <span class="hlt">model</span> to be extended to estimate shear stress distributions in channels with large width-to-depth ratios. Our <span class="hlt">model</span> is efficient enough to incorporate into large-scale landscape <span class="hlt">evolution</span> codes and can be used to examine how channels adjust both cross-sectional shape and slope in response to tectonic and climatic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910061155&hterms=sarkar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dsarkar','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910061155&hterms=sarkar&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dsarkar"><span>Simulations of free shear <span class="hlt">layers</span> using a compressible k-epsilon <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yu, S. T.; Chang, C. T.; Marek, C. J.</p> <p>1991-01-01</p> <p>A two-dimensional, compressible Navier-Stokes equations with a k-epsilon turbulence <span class="hlt">model</span> are solved numerically to simulate the flows of compressible free shear <span class="hlt">layers</span>. The appropriate form of k and epsilon equations for compressible flows are discussed. Sarkar's <span class="hlt">modeling</span> is adopted to simulate the compressibility effects in the k and epsilon equations. The numerical results show that the spreading rate of the shear <span class="hlt">layers</span> decreases with increasing convective Mach number. In addition, favorable comparison was found between the calculated results and Goebel and Dutton's experimental data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19920014112','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19920014112"><span>Simulations of free shear <span class="hlt">layers</span> using a compressible kappa-epsilon <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Yu, S. T.; Chang, C. T.; Marek, C. J.</p> <p>1991-01-01</p> <p>A two-dimensional, compressible Navier-Stokes equation with a k-epsilon turbulence <span class="hlt">model</span> is solved numerically to simulate the flow of a compressible free shear <span class="hlt">layer</span>. The appropriate form of k and epsilon equations for compressible flow is discussed. Sarkar's <span class="hlt">modeling</span> is adopted to simulate the compressibility effects in the k and epsilon equations. The numerical results show that the spreading rate of the shear <span class="hlt">layers</span> decreases with increasing convective Mach number. In addition, favorable comparison was found between the calculated results and experimental data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JMPSo..64..170K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JMPSo..64..170K"><span>A two-scale <span class="hlt">model</span> for dynamic damage <span class="hlt">evolution</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Keita, Oumar; Dascalu, Cristian; François, Bertrand</p> <p>2014-03-01</p> <p>This paper presents a new micro-mechanical damage <span class="hlt">model</span> accounting for inertial effect. The two-scale damage <span class="hlt">model</span> is fully deduced from small-scale descriptions of dynamic micro-crack propagation under tensile loading (mode I). An appropriate micro-mechanical energy analysis is combined with homogenization based on asymptotic developments in order to obtain the macroscopic <span class="hlt">evolution</span> law for damage. Numerical simulations are presented in order to illustrate the ability of the <span class="hlt">model</span> to describe known behaviors like size effects for the structural response, strain-rate sensitivity, brittle-ductile transition and wave dispersion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19518581','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19518581"><span>Nonlinear <span class="hlt">layered</span> lattice <span class="hlt">model</span> and generalized solitary waves in imperfectly bonded structures.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Khusnutdinova, Karima R; Samsonov, Alexander M; Zakharov, Alexey S</p> <p>2009-05-01</p> <p>We study nonlinear waves in a two-<span class="hlt">layered</span> imperfectly bonded structure using a nonlinear lattice <span class="hlt">model</span>. The key element of the <span class="hlt">model</span> is an anharmonic chain of oscillating dipoles, which can be viewed as a basic lattice analog of a one-dimensional macroscopic waveguide. Long nonlinear longitudinal waves in a <span class="hlt">layered</span> lattice with a soft middle (or bonding) <span class="hlt">layer</span> are governed by a system of coupled Boussinesq-type equations. For this system we find conservation laws and show that pure solitary waves, which exist in a single equation and can exist in the coupled system in the symmetric case, are structurally unstable and are replaced with generalized solitary waves.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFDM32003Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFDM32003Y"><span><span class="hlt">Evolution</span> of vortex-surface fields in transitional boundary <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Yue; Zhao, Yaomin; Xiong, Shiying</p> <p>2016-11-01</p> <p>We apply the vortex-surface field (VSF), a Lagrangian-based structure-identification method, to the DNS database of transitional boundary <span class="hlt">layers</span>. The VSFs are constructed from the vorticity fields within a sliding window at different times and locations using a recently developed boundary-constraint method. The isosurfaces of VSF, representing vortex surfaces consisting of vortex lines with different wall distances in the laminar stage, show different evolutionary geometries in transition. We observe that the vortex surfaces with significant deformation evolve from wall-parallel planar sheets through hairpin-like structures and packets into a turbulent spot with regeneration of small-scale hairpins. From quantitative analysis, we show that a small number of representative or influential vortex surfaces can contribute significantly to the increase of the drag coefficient in transition, which implies a reduced-order <span class="hlt">model</span> based on VSF. This work has been supported in part by the National Natural Science Foundation of China (Grant Nos. 11472015, 11522215 and 11521091), and the Thousand Young Talents Program of China.</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://www.ncbi.nlm.nih.gov/pubmed/20151115','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20151115"><span>Stochasticity versus determinism: consequences for realistic gene regulatory network <span class="hlt">modelling</span> and <span class="hlt">evolution</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jenkins, Dafyd J; Stekel, Dov J</p> <p>2010-02-01</p> <p>Gene regulation is one important mechanism in producing observed phenotypes and heterogeneity. Consequently, the study of gene regulatory network (GRN) architecture, function and <span class="hlt">evolution</span> now forms a major part of modern biology. However, it is impossible to experimentally observe the <span class="hlt">evolution</span> of GRNs on the timescales on which living species evolve. In silico <span class="hlt">evolution</span> provides an approach to studying the long-term <span class="hlt">evolution</span> of GRNs, but many <span class="hlt">models</span> have either considered network architecture from non-adaptive <span class="hlt">evolution</span>, or <span class="hlt">evolution</span> to non-biological objectives. Here, we address a number of important <span class="hlt">modelling</span> and biological questions about the <span class="hlt">evolution</span> of GRNs to the realistic goal of biomass production. Can different commonly used simulation paradigms, in particular deterministic and stochastic Boolean networks, with and without basal gene expression, be used to compare adaptive with non-adaptive <span class="hlt">evolution</span> of GRNs? Are these paradigms together with this goal sufficient to generate a range of solutions? Will the interaction between a biological goal and evolutionary dynamics produce trade-offs between growth and mutational robustness? We show that stochastic basal gene expression forces shrinkage of genomes due to energetic constraints and is a prerequisite for some solutions. In systems that are able to evolve rates of basal expression, two optima, one with and one without basal expression, are observed. Simulation paradigms without basal expression generate bloated networks with non-functional elements. Further, a range of functional solutions was observed under identical conditions only in stochastic networks. Moreover, there are trade-offs between efficiency and yield, indicating an inherent intertwining of fitness and evolutionary dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA014878','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA014878"><span>Boundary <span class="hlt">Layer</span> Studies on a Spinning Tangent-Ogive-Cylinder <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1975-07-01</p> <p>ca) An experimental investigation of the Magnus effect on a seven caliber tangent-I ;’ ogive- cylinder <span class="hlt">model</span> in supersonic flow is reported. The...necessary and Identify by block number) Three-Dimiensional Boundary <span class="hlt">Layer</span> Compressible Flow Body of Revolution Magnus Effects Boundary <span class="hlt">Layer</span>...factors have resulted in renewed interest in the study of the Magnus effect . This report describes an experimental study of the effects of spin on</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4918933','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4918933"><span><span class="hlt">Modelling</span> Influence and Opinion <span class="hlt">Evolution</span> in Online Collective Behaviour</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Gend, Pascal; Rentfrow, Peter J.; Hendrickx, Julien M.; Blondel, Vincent D.</p> <p>2016-01-01</p> <p>Opinion <span class="hlt">evolution</span> and judgment revision are mediated through social influence. Based on a large crowdsourced in vitro experiment (n = 861), it is shown how a consensus <span class="hlt">model</span> can be used to predict opinion <span class="hlt">evolution</span> in online collective behaviour. It is the first time the predictive power of a quantitative <span class="hlt">model</span> of opinion dynamics is tested against a real dataset. Unlike previous research on the topic, the <span class="hlt">model</span> was validated on data which did not serve to calibrate it. This avoids to favor more complex <span class="hlt">models</span> over more simple ones and prevents overfitting. The <span class="hlt">model</span> is parametrized by the influenceability of each individual, a factor representing to what extent individuals incorporate external judgments. The prediction accuracy depends on prior knowledge on the participants’ past behaviour. Several situations reflecting data availability are compared. When the data is scarce, the data from previous participants is used to predict how a new participant will behave. Judgment revision includes unpredictable variations which limit the potential for prediction. A first measure of unpredictability is proposed. The measure is based on a specific control experiment. More than two thirds of the prediction errors are found to occur due to unpredictability of the human judgment revision process rather than to <span class="hlt">model</span> imperfection. PMID:27336834</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10596E..0AV','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10596E..0AV"><span>Analytical <span class="hlt">model</span> for a laminated shape memory alloy beam with piezoelectric <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Viet, N. V.; Zaki, W.; Umer, R.</p> <p>2018-03-01</p> <p>We propose an analytical <span class="hlt">model</span> for a laminated beam consisting of a superelastic shape memory alloy (SMA) core <span class="hlt">layer</span> bonded to two piezoelectric <span class="hlt">layers</span> on its top and bottom surfaces. The <span class="hlt">model</span> accounts for forward and reverse phase transformation between austenite and martensite during a full isothermal loading-unloading cycle starting a full austenite in the SMA <span class="hlt">layer</span>. In particular, the laminated composite beam has a rectangular cross section and is fixed at one end while the other end is subjected to a concentrated transverse force acting at the tip. The moment-curvature relation is analytically derived. The generated electric displacement output from the piezoelectric <span class="hlt">layers</span> is then determined using the linear piezoelectric theory. The results are compared to 3D simulations using finite element analysis (FEA). The comparison shows good agreement in terms of electric displacement, in general, throughout the loading cycle.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001PrSS...68..231S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001PrSS...68..231S"><span>Characterization and use of crystalline bacterial cell surface <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sleytr, Uwe B.; Sára, Margit; Pum, Dietmar; Schuster, Bernhard</p> <p>2001-10-01</p> <p>Crystalline bacterial cell surface <span class="hlt">layers</span> (S-<span class="hlt">layers</span>) are one of the most common outermost cell envelope components of prokaryotic organisms (archaea and bacteria). S-<span class="hlt">layers</span> are monomolecular arrays composed of a single protein or glycoprotein species and represent the simplest biological membranes developed during <span class="hlt">evolution</span>. S-<span class="hlt">layers</span> as the most abundant of prokaryotic cellular proteins are appealing <span class="hlt">model</span> systems for studying the structure, synthesis, genetics, assembly and function of proteinaceous supramolecular structures. The wealth of information existing on the general principle of S-<span class="hlt">layers</span> have revealed a broad application potential. The most relevant features exploited in applied S-<span class="hlt">layer</span> research are: (i) pores passing through S-<span class="hlt">layers</span> show identical size and morphology and are in the range of ultrafiltration membranes; (ii) functional groups on the surface and in the pores are aligned in well-defined positions and orientations and accessible for chemical modifications and binding functional molecules in very precise fashion; (iii) isolated S-<span class="hlt">layer</span> subunits from a variety of organisms are capable of recrystallizing as closed monolayers onto solid supports (e.g., metals, polymers, silicon wafers) at the air-water interface, on lipid films or onto the surface of liposomes; (iv) functional domains can be incorporated in S-<span class="hlt">layer</span> proteins by genetic engineering. Thus, S-<span class="hlt">layer</span> technologies particularly provide new approaches for biotechnology, biomimetics, molecular nanotechnology, nanopatterning of surfaces and formation of ordered arrays of metal clusters or nanoparticles as required for nanoelectronics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013GGG....14.3250G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013GGG....14.3250G"><span>Investigating seismic anisotropy beneath the Reykjanes Ridge using <span class="hlt">models</span> of mantle flow, crystallographic <span class="hlt">evolution</span>, and surface wave propagation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gallego, A.; Ito, G.; Dunn, R. A.</p> <p>2013-08-01</p> <p>Surface wave studies of the Reykjanes Ridge (RR) and the Iceland hotspot have imaged an unusual and enigmatic pattern of two zones of negative radial anisotropy on each side of the RR. We test previously posed and new hypotheses for the origin of this anisotropy, by considering lattice preferred orientation (LPO) of olivine A-type fabric in simple <span class="hlt">models</span> with 1-D, <span class="hlt">layered</span> structures, as well as in 2-D and 3-D geodynamic <span class="hlt">models</span> with mantle flow and LPO <span class="hlt">evolution</span>. Synthetic phase velocities of Love and Rayleigh waves traveling parallel to the ridge axis are produced and then inverted to mimic the previous seismic studies. Results of 1-D <span class="hlt">models</span> show that strong negative radial anisotropy can be produced when olivine a axes are preferentially aligned not only vertically but also subhorizontally in the plane of wave propagation. Geodynamic <span class="hlt">models</span> show that negative anisotropy on the sides of the RR can occur when plate spreading impels a corner flow, and in turn a subvertical alignment of olivine a axes, on the sides of the ridge axis. Mantle dehydration must be invoked to form a viscous upper <span class="hlt">layer</span> that minimizes the disturbance of the corner flow by the Iceland mantle plume. While the results are promising, important discrepancies still exist between the observed seismic structure and the predictions of this <span class="hlt">model</span>, as well as <span class="hlt">models</span> of a variety of types of mantle flow associated with plume-ridge interaction. Thus, other factors that influence seismic anisotropy, but not considered in this study, such as power-law rheology, water, melt, or time-dependent mantle flow, are probably important beneath the Reykjanes Ridge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930017690','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930017690"><span>Automata network <span class="hlt">models</span> of galaxy <span class="hlt">evolution</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Chappell, David; Scalo, John</p> <p>1993-01-01</p> <p>Two ideas appear frequently in theories of star formation and galaxy <span class="hlt">evolution</span>: (1) star formation is nonlocally excitatory, stimulating star formation in neighboring regions by propagation of a dense fragmenting shell or the compression of preexisting clouds; and (2) star formation is nonlocally inhibitory, making H2 regions and explosions which can create low-density and/or high temperature regions and increase the macroscopic velocity dispersion of the cloudy gas. Since it is not possible, given the present state of hydrodynamic <span class="hlt">modeling</span>, to estimate whether one of these effects greatly dominates the other, it is of interest to investigate the predicted spatial pattern of star formation and its temporal behavior in simple <span class="hlt">models</span> which incorporate both effects in a controlled manner. The present work presents preliminary results of such a study which is based on lattice galaxy <span class="hlt">models</span> with various types of nonlocal inhibitory and excitatory couplings of the local SFR to the gas density, temperature, and velocity field meant to <span class="hlt">model</span> a number of theoretical suggestions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AIPC.1650.1170M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AIPC.1650.1170M"><span><span class="hlt">Model</span>-based damage evaluation of <span class="hlt">layered</span> CFRP structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Munoz, Rafael; Bochud, Nicolas; Rus, Guillermo; Peralta, Laura; Melchor, Juan; Chiachío, Juan; Chiachío, Manuel; Bond, Leonard J.</p> <p>2015-03-01</p> <p>An ultrasonic evaluation technique for damage identification of <span class="hlt">layered</span> CFRP structures is presented. This approach relies on a <span class="hlt">model</span>-based estimation procedure that combines experimental data and simulation of ultrasonic damage-propagation interactions. The CFPR structure, a [0/90]4s lay-up, has been tested in an immersion through transmission experiment, where a scan has been performed on a damaged specimen. Most ultrasonic techniques in industrial practice consider only a few features of the received signals, namely, time of flight, amplitude, attenuation, frequency contents, and so forth. In this case, once signals are captured, an algorithm is used to reconstruct the complete signal waveform and extract the unknown damage parameters by means of <span class="hlt">modeling</span> procedures. A linear version of the data processing has been performed, where only Young modulus has been monitored and, in a second nonlinear version, the first order nonlinear coefficient β was incorporated to test the possibility of detection of early damage. The aforementioned physical simulation <span class="hlt">models</span> are solved by the Transfer Matrix formalism, which has been extended from linear to nonlinear harmonic generation technique. The damage parameter search strategy is based on minimizing the mismatch between the captured and simulated signals in the time domain in an automated way using Genetic Algorithms. Processing all scanned locations, a C-scan of the parameter of each <span class="hlt">layer</span> can be reconstructed, obtaining the information describing the state of each <span class="hlt">layer</span> and each interface. Damage can be located and quantified in terms of changes in the selected parameter with a measurable extension. In the case of the nonlinear coefficient of first order, evidence of higher sensitivity to damage than imaging the linearly estimated Young Modulus is provided.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005JAP....98e4906F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005JAP....98e4906F"><span>Surface morphological <span class="hlt">evolution</span> of epitaxial CrN(001) <span class="hlt">layers</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Frederick, J. R.; Gall, D.</p> <p>2005-09-01</p> <p>CrN <span class="hlt">layers</span>, 57 and 230 nm thick, were grown on MgO(001) at Ts=600-800 °C by ultrahigh-vacuum magnetron sputter deposition in pure N2 discharges from an oblique deposition angle α=80°. <span class="hlt">Layers</span> grown at 600 °C nucleate as single crystals with a cube-on-cube epitaxial relationship with the substrate. However, rough surfaces with cauliflower-type morphologies cause the nucleation of misoriented CrN grains that develop into cone-shaped grains that protrude out of the epitaxial matrix to form triangular faceted surface mounds. The surface morphology of epitaxial CrN(001) grown at 700 °C is characterized by dendritic ridge patterns extending along the orthogonal <110> directions superposed by square-shaped super mounds with <100> edges. The ridge patterns are attributed to a Bales-Zangwill instability while the supermounds form due to atomic shadowing which leads to the formation of epitaxial inverted pyramids that are separated from the surrounding <span class="hlt">layer</span> by tilted nanovoids. Growth at 800 °C yields complete single crystals with smooth surfaces. The root-mean-square surface roughness for 230-nm-thick <span class="hlt">layers</span> decreases from 18.8 to 9.3 to 1.1 nm as Ts is raised from 600 to 700 to 800 °C. This steep decrease is due to a transition in the roughening mechanism from atomic shadowing to kinetic roughening. Atomic shadowing is dominant at 600 and 700 °C, where misoriented grains and supermounds, respectively, capture a larger fraction of the oblique deposition flux in comparison to the surrounding epitaxial matrix, resulting in a high roughening rate that is described by a power law with an exponent β>0.5. In contrast, kinetic roughening controls the surface morphology for Ts=800 °C, as well as the epitaxial fraction of the <span class="hlt">layers</span> grown at 600 and 700 °C, yielding relatively smooth surfaces and β<=0.27.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940011759','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940011759"><span>Chemical differentiation, thermal <span class="hlt">evolution</span>, and catastrophic overturn on Venus: Predictions and geologic observations</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Head, James W.; Parmentier, E. M.; Hess, P. C.</p> <p>1993-01-01</p> <p>Observations from Magellan show that: (1) the surface of Venus is generally geologically young, (2) there is no evidence for widespread recent crustal spreading or subduction, (3) the crater population permits the hypothesis that the surface is in production, and (4) relatively few impact craters appear to be embayed by volcanic deposits suggesting that the volcanic flux has drastically decreased as a function of time. These observations have led to consideration of hypotheses suggesting that the geological history of Venus may have changed dramatically as a function of time due to general thermal <span class="hlt">evolution</span>, and/or thermal and chemical <span class="hlt">evolution</span> of a depleted mantle <span class="hlt">layer</span>, perhaps punctuated by catastrophic overturn of upper <span class="hlt">layers</span> or episodic plate tectonics. We have previously examined the geological implications of some of these <span class="hlt">models</span>, and here we review the predictions associated with two periods of Venus history. Stationary thick lithosphere and depleted mantle <span class="hlt">layer</span>, and development of regional to global development of regional to global instabilities, and compare these predictions to the geological characteristics of Venus revealed by Magellan.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1997ApJ...476..544S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1997ApJ...476..544S"><span><span class="hlt">Modeling</span> the <span class="hlt">Evolution</span> of Disk Galaxies. I. The Chemodynamical Method and the Galaxy <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Samland, M.; Hensler, G.; Theis, Ch.</p> <p>1997-02-01</p> <p>Here we present our two-dimensional chemodynamical code CoDEx, which we developed for the purpose of <span class="hlt">modeling</span> the <span class="hlt">evolution</span> of galaxies in a self-consistent manner. The code solves the hydrodynamical and momentum equations for three stellar components and the multiphase interstellar medium (clouds and intercloud medium), including star formation, Type I and Type II supernovae, planetary nebulae, stellar winds, evaporation and condensation, drag, cloud collisions, heating and cooling, and stellar nucleosynthesis. These processes are treated simultaneously, coupling a large range in temporal and spatial scales, to account for feedback and self-regulation processes, which play an extraordinarily important role in the galactic <span class="hlt">evolution</span>. The <span class="hlt">evolution</span> of galaxies of different masses and angular momenta is followed through all stages from the initial protogalactic clouds until now. In this first paper we present a representative <span class="hlt">model</span> of the Milky Way and compare it with observations. The capability of chemodynamical <span class="hlt">models</span> is convincingly proved by the excellent agreement with various observations. In addition, well-known problems (the G-dwarf problem, the discrepancy between local effective yields, etc.), which so far could be only explained by artificial constraints, are also solved in the global scenario. Starting from a rotating protogalactic gas cloud in virial equilibrium, which collapses owing to dissipative cloud-cloud collisions, we can follow the galactic <span class="hlt">evolution</span> in detail. Owing to the collapse, the gas density increases, stars are forming, and the first Type II supernovae explode. The collapse time is 1 order of magnitude longer than the dynamical free-fall time because of the energy release by Type II supernovae. The supernovae also drive hot metal-rich gas ejected from massive stars into the halo, and as a consequence, the clouds in the star-forming regions have lower metallicities than the clouds in the halo. The observed negative metallicity gradients</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3259953','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3259953"><span><span class="hlt">Modelling</span> rate distributions using character compatibility: implications for morphological <span class="hlt">evolution</span> among fossil invertebrates</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Wagner, Peter J.</p> <p>2012-01-01</p> <p>Rate distributions are important considerations when testing hypotheses about morphological <span class="hlt">evolution</span> or phylogeny. They also have implications about general processes underlying character <span class="hlt">evolution</span>. Molecular systematists often assume that rates are Poisson processes with gamma distributions. However, morphological change is the product of multiple probabilistic processes and should theoretically be affected by hierarchical integration of characters. Both factors predict lognormal rate distributions. Here, a simple inverse <span class="hlt">modelling</span> approach assesses the best single-rate, gamma and lognormal <span class="hlt">models</span> given observed character compatibility for 115 invertebrate groups. Tests reject the single-rate <span class="hlt">model</span> for nearly all cases. Moreover, the lognormal outperforms the gamma for character change rates and (especially) state derivation rates. The latter in particular is consistent with integration affecting morphological character <span class="hlt">evolution</span>. PMID:21795266</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21795266','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21795266"><span><span class="hlt">Modelling</span> rate distributions using character compatibility: implications for morphological <span class="hlt">evolution</span> among fossil invertebrates.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Wagner, Peter J</p> <p>2012-02-23</p> <p>Rate distributions are important considerations when testing hypotheses about morphological <span class="hlt">evolution</span> or phylogeny. They also have implications about general processes underlying character <span class="hlt">evolution</span>. Molecular systematists often assume that rates are Poisson processes with gamma distributions. However, morphological change is the product of multiple probabilistic processes and should theoretically be affected by hierarchical integration of characters. Both factors predict lognormal rate distributions. Here, a simple inverse <span class="hlt">modelling</span> approach assesses the best single-rate, gamma and lognormal <span class="hlt">models</span> given observed character compatibility for 115 invertebrate groups. Tests reject the single-rate <span class="hlt">model</span> for nearly all cases. Moreover, the lognormal outperforms the gamma for character change rates and (especially) state derivation rates. The latter in particular is consistent with integration affecting morphological character <span class="hlt">evolution</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26305258','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26305258"><span>Markov Chain-Like Quantum Biological <span class="hlt">Modeling</span> of Mutations, Aging, and <span class="hlt">Evolution</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Djordjevic, Ivan B</p> <p>2015-08-24</p> <p>Recent evidence suggests that quantum mechanics is relevant in photosynthesis, magnetoreception, enzymatic catalytic reactions, olfactory reception, photoreception, genetics, electron-transfer in proteins, and <span class="hlt">evolution</span>; to mention few. In our recent paper published in Life, we have derived the operator-sum representation of a biological channel based on codon basekets, and determined the quantum channel <span class="hlt">model</span> suitable for study of the quantum biological channel capacity. However, this <span class="hlt">model</span> is essentially memoryless and it is not able to properly <span class="hlt">model</span> the propagation of mutation errors in time, the process of aging, and <span class="hlt">evolution</span> of genetic information through generations. To solve for these problems, we propose novel quantum mechanical <span class="hlt">models</span> to accurately describe the process of creation spontaneous, induced, and adaptive mutations and their propagation in time. Different biological channel <span class="hlt">models</span> with memory, proposed in this paper, include: (i) Markovian classical <span class="hlt">model</span>, (ii) Markovian-like quantum <span class="hlt">model</span>, and (iii) hybrid quantum-classical <span class="hlt">model</span>. We then apply these <span class="hlt">models</span> in a study of aging and <span class="hlt">evolution</span> of quantum biological channel capacity through generations. We also discuss key differences of these <span class="hlt">models</span> with respect to a multilevel symmetric channel-based Markovian <span class="hlt">model</span> and a Kimura <span class="hlt">model</span>-based Markovian process. These <span class="hlt">models</span> are quite general and applicable to many open problems in biology, not only biological channel capacity, which is the main focus of the paper. We will show that the famous quantum Master equation approach, commonly used to describe different biological processes, is just the first-order approximation of the proposed quantum Markov chain-like <span class="hlt">model</span>, when the observation interval tends to zero. One of the important implications of this <span class="hlt">model</span> is that the aging phenotype becomes determined by different underlying transition probabilities in both programmed and random (damage) Markov chain-like <span class="hlt">models</span> of aging, which are mutually</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4598651','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4598651"><span>Markov Chain-Like Quantum Biological <span class="hlt">Modeling</span> of Mutations, Aging, and <span class="hlt">Evolution</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>Djordjevic, Ivan B.</p> <p>2015-01-01</p> <p>Recent evidence suggests that quantum mechanics is relevant in photosynthesis, magnetoreception, enzymatic catalytic reactions, olfactory reception, photoreception, genetics, electron-transfer in proteins, and <span class="hlt">evolution</span>; to mention few. In our recent paper published in Life, we have derived the operator-sum representation of a biological channel based on codon basekets, and determined the quantum channel <span class="hlt">model</span> suitable for study of the quantum biological channel capacity. However, this <span class="hlt">model</span> is essentially memoryless and it is not able to properly <span class="hlt">model</span> the propagation of mutation errors in time, the process of aging, and <span class="hlt">evolution</span> of genetic information through generations. To solve for these problems, we propose novel quantum mechanical <span class="hlt">models</span> to accurately describe the process of creation spontaneous, induced, and adaptive mutations and their propagation in time. Different biological channel <span class="hlt">models</span> with memory, proposed in this paper, include: (i) Markovian classical <span class="hlt">model</span>, (ii) Markovian-like quantum <span class="hlt">model</span>, and (iii) hybrid quantum-classical <span class="hlt">model</span>. We then apply these <span class="hlt">models</span> in a study of aging and <span class="hlt">evolution</span> of quantum biological channel capacity through generations. We also discuss key differences of these <span class="hlt">models</span> with respect to a multilevel symmetric channel-based Markovian <span class="hlt">model</span> and a Kimura <span class="hlt">model</span>-based Markovian process. These <span class="hlt">models</span> are quite general and applicable to many open problems in biology, not only biological channel capacity, which is the main focus of the paper. We will show that the famous quantum Master equation approach, commonly used to describe different biological processes, is just the first-order approximation of the proposed quantum Markov chain-like <span class="hlt">model</span>, when the observation interval tends to zero. One of the important implications of this <span class="hlt">model</span> is that the aging phenotype becomes determined by different underlying transition probabilities in both programmed and random (damage) Markov chain-like <span class="hlt">models</span> of aging, which are mutually</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910031494&hterms=vertical+integration&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dvertical%2Bintegration','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910031494&hterms=vertical+integration&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dvertical%2Bintegration"><span>Numerical <span class="hlt">modeling</span> of the atmosphere with an isentropic vertical coordinate</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hsu, Yueh-Jiuan G.; Arakawa, Akio</p> <p>1990-01-01</p> <p>A theta-coordinate <span class="hlt">model</span> simulating the nonlinear <span class="hlt">evolution</span> of a baroclinic wave is presented. In the <span class="hlt">model</span>, vertical discretization maintains important integral constraints such as conservation of the angular momentum and total energy. A massless-<span class="hlt">layer</span> approach is used in the treatment of the intersections of coordinate surfaces with the lower boundary. This formally eliminates the intersection problem, but raises other computational problems. Horizontal discretization of the continuity and momentum equations in the <span class="hlt">model</span> are designed to overcome these problems. Selected results from a 10-day integration with the 25-<span class="hlt">layer</span>, beta-plane version of the <span class="hlt">model</span> are presented. It is concluded that the <span class="hlt">model</span> can simulate the nonlinear <span class="hlt">evolution</span> of a baroclinic wave and associated dynamical processes without major computational difficulties.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRD..122.3492L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRD..122.3492L"><span><span class="hlt">Evolution</span> of trace elements in the planetary boundary <span class="hlt">layer</span> in southern China: Effects of dust storms and aerosol-cloud interactions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Tao; Wang, Yan; Zhou, Jie; Wang, Tao; Ding, Aijun; Nie, Wei; Xue, Likun; Wang, Xinfeng; Wang, Wenxing</p> <p>2017-03-01</p> <p>Aerosols and cloud water were analyzed at a mountaintop in the planetary boundary <span class="hlt">layer</span> in southern China during March-May 2009, when two Asian dust storms occurred, to investigate the effects of aerosol-cloud interactions (ACIs) on chemical <span class="hlt">evolution</span> of atmospheric trace elements. Fe, Al, and Zn predominated in both coarse and fine aerosols, followed by high concentrations of toxic Pb, As, and Cd. Most of these aerosol trace elements, which were affected by dust storms, exhibited various increases in concentrations but consistent decreases in solubility. Zn, Fe, Al, and Pb were the most abundant trace elements in cloud water. The trace element concentrations exhibited logarithmic inverse relationships with the cloud liquid water content and were found highly pH dependent with minimum concentrations at the threshold of pH 5.0. The calculation of Visual MINTEQ <span class="hlt">model</span> showed that 80.7-96.3% of Fe(II), Zn(II), Pb(II), and Cu(II) existed in divalent free ions, while 71.7% of Fe(III) and 71.5% of Al(III) were complexed by oxalate and fluoride, respectively. ACIs could markedly change the speciation distributions of trace elements in cloud water by pH modification. The in-cloud scavenging of aerosol trace elements likely reached a peak after the first 2-3 h of cloud processing, with scavenging ratios between 0.12 for Cr and 0.57 for Pb. The increases of the trace element solubility (4-33%) were determined in both in-cloud aerosols and postcloud aerosols. These results indicated the significant importance of aerosol-cloud interactions to the <span class="hlt">evolution</span> of trace elements during the first several cloud condensation/evaporation cycles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2001PhyA..291..583S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2001PhyA..291..583S"><span>Scaling in the Donangelo-Sneppen <span class="hlt">model</span> for <span class="hlt">evolution</span> of money</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stauffer, Dietrich; P. Radomski, Jan</p> <p>2001-03-01</p> <p>The <span class="hlt">evolution</span> of money from unsuccessful barter attempts, as <span class="hlt">modeled</span> by Donangelo and Sneppen, is modified by a deterministic instead of a probabilistic selection of the most desired product as money. We check in particular the characteristic times of the <span class="hlt">model</span> as a function of system size.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT.........1N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT.........1N"><span>Investigating evaporation of melting ice particles within a bin melting <span class="hlt">layer</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Neumann, Andrea J.</p> <p></p> <p>Single column <span class="hlt">models</span> have been used to help develop algorithms for remote sensing retrievals. Assumptions in the single-column <span class="hlt">models</span> may affect the assumptions of the remote sensing retrievals. Studies of the melting <span class="hlt">layer</span> that use single column <span class="hlt">models</span> often assume environments that are near or at water saturation. This study investigates the effects of evaporation upon melting particles to determine whether the assumption of negligible mass loss still holds within subsaturated melting <span class="hlt">layers</span>. A single column, melting <span class="hlt">layer</span> <span class="hlt">model</span> is modified to include the effects of sublimation and evaporation upon the particles. Other changes to the <span class="hlt">model</span> include switching the order in which the <span class="hlt">model</span> loops over particle sizes and <span class="hlt">model</span> <span class="hlt">layers</span>; including a particle sedimentation scheme; adding aggregation, accretion, and collision and coalescence processes; allowing environmental variables such as the water vapor diffusivity and the Schmidt number to vary with the changes in the environment; adding explicitly calculated particle temperature, changing the particle terminal velocity parameterization; and using a newly-derived effective density-dimensional relationship for use in particle mass calculations. Simulations of idealized melting <span class="hlt">layer</span> environments show that significant mass loss due to evaporation during melting is possible within subsaturated environments. Short melting distances, accelerating particle fall speeds, and short melting times help constrain the amount of mass lost due to evaporation while melting is occurring, even in subsaturated profiles. Sublimation prior to melting can also be a significant source of mass loss. The trends shown on the particle scale also appear in the bulk distribution parameters such as rainfall rate and ice water content. Simulations incorporating observed melting <span class="hlt">layer</span> environments show that significant mass loss due to evaporation during the melting process is possible under certain environmental conditions. A profile such as the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006SPIE.6284E..0IP','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006SPIE.6284E..0IP"><span>Light dosimetry for focused and defocused beam irradiation in multi-<span class="hlt">layered</span> tissue <span class="hlt">models</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Petrova, Kremena S.; Stoykova, Elena V.</p> <p>2006-09-01</p> <p>Treatment of acupuncture points, trigger points, joint inflammations in low level laser therapy as well as various applications of lasers for treatment of soft tissues in dental medicine, require irradiation by a narrow converging laser beam. The aim of this study is to compare light delivery produced by focused or defocused narrow beam irradiation in a multi-<span class="hlt">layered</span> skin tissue <span class="hlt">model</span> at increasing depth of the target. The task is solved by 3-D Monte-Carlo simulation for matched and mismatched refractive indices at the tissue/ambient medium interface. The <span class="hlt">modeled</span> light beams have a circular cross-section at the tissue entrance with uniform or Gaussian intensity distribution. Three are the tissue <span class="hlt">models</span> used in simulation : i) a bloodless skin <span class="hlt">layer</span>; ii) a bloodless skin <span class="hlt">layer</span> with embedded scattering object; iii) a skin <span class="hlt">layer</span> with small blood vessels of varying size, which are <span class="hlt">modeled</span> as infinite cylinders parallel to the tissue surface located at different depths. Optical properties (absorption coefficient, scattering coefficient, anisotropy factor, g, and index of refraction) of different tissue constituents are chosen from the literature.</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/2018PhFl...30b2107E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhFl...30b2107E"><span>A two-<span class="hlt">layer</span> <span class="hlt">model</span> for buoyant inertial displacement flows in inclined pipes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Etrati, Ali; Frigaard, Ian A.</p> <p>2018-02-01</p> <p>We investigate the inertial flows found in buoyant miscible displacements using a two-<span class="hlt">layer</span> <span class="hlt">model</span>. From displacement flow experiments in inclined pipes, it has been observed that for significant ranges of Fr and Re cos β/Fr, a two-<span class="hlt">layer</span>, stratified flow develops with the heavier fluid moving at the bottom of the pipe. Due to significant inertial effects, thin-film/lubrication <span class="hlt">models</span> developed for laminar, viscous flows are not effective for predicting these flows. Here we develop a displacement <span class="hlt">model</span> that addresses this shortcoming. The complete <span class="hlt">model</span> for the displacement flow consists of mass and momentum equations for each fluid, resulting in a set of four non-linear equations. By integrating over each <span class="hlt">layer</span> and eliminating the pressure gradient, we reduce the system to two equations for the area and mean velocity of the heavy fluid <span class="hlt">layer</span>. The wall and interfacial stresses appear as source terms in the reduced system. The final system of equations is solved numerically using a robust, shock-capturing scheme. The equations are stabilized to remove non-physical instabilities. A linear stability analysis is able to predict the onset of instabilities at the interface and together with numerical solution, is used to study displacement effectiveness over different parametric regimes. Backflow and instability onset predictions are made for different viscosity ratios.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPSJ...86h4801Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPSJ...86h4801Y"><span><span class="hlt">Modeling</span> <span class="hlt">Evolution</span> on Nearly Neutral Network Fitness Landscapes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yakushkina, Tatiana; Saakian, David B.</p> <p>2017-08-01</p> <p>To describe virus <span class="hlt">evolution</span>, it is necessary to define a fitness landscape. In this article, we consider the microscopic <span class="hlt">models</span> with the advanced version of neutral network fitness landscapes. In this problem setting, we suppose a fitness difference between one-point mutation neighbors to be small. We construct a modification of the Wright-Fisher <span class="hlt">model</span>, which is related to ordinary infinite population <span class="hlt">models</span> with nearly neutral network fitness landscape at the large population limit. From the microscopic <span class="hlt">models</span> in the realistic sequence space, we derive two versions of nearly neutral network <span class="hlt">models</span>: with sinks and without sinks. We claim that the suggested <span class="hlt">model</span> describes the evolutionary dynamics of RNA viruses better than the traditional Wright-Fisher <span class="hlt">model</span> with few sequences.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015SPIE.9489E..0HR','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015SPIE.9489E..0HR"><span>Terahertz reflection interferometry for automobile paint <span class="hlt">layer</span> thickness measurement</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rahman, Aunik; Tator, Kenneth; Rahman, Anis</p> <p>2015-05-01</p> <p>Non-destructive terahertz reflection interferometry offers many advantages for sub-surface inspection such as interrogation of hidden defects and measurement of <span class="hlt">layers</span>' thicknesses. Here, we describe a terahertz reflection interferometry (TRI) technique for non-contact measurement of paint panels where the paint is comprised of different <span class="hlt">layers</span> of primer, basecoat, topcoat and clearcoat. Terahertz interferograms were generated by reflection from different <span class="hlt">layers</span> of paints on a metallic substrate. These interferograms' peak spacing arising from the delay-time response of respective <span class="hlt">layers</span>, allow one to <span class="hlt">model</span> the thicknesses of the constituent <span class="hlt">layers</span>. Interferograms generated at different incident angles show that the interferograms are more pronounced at certain angles than others. This "optimum" angle is also a function of different paint and substrate combinations. An automated angular scanning algorithm helps visualizing the <span class="hlt">evolution</span> of the interferograms as a function of incident angle and also enables the identification of optimum reflection angle for a given paint-substrate combination. Additionally, scanning at different points on a substrate reveals that there are observable variations from one point to another of the same sample over its entire surface area. This ability may be used as a quality control tool for in-situ inspection in a production line. Keywords: Terahertz reflective interferometry, Paint and coating <span class="hlt">layers</span>, Non-destructive</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20040028003','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20040028003"><span>Dynamic Turbulence <span class="hlt">Modelling</span> in Large-eddy Simulations of the Cloud-topped Atmospheric Boundary <span class="hlt">Layer</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kirkpatrick, M. P.; Mansour, N. N.; Ackerman, A. S.; Stevens, D. E.</p> <p>2003-01-01</p> <p>The use of large eddy simulation, or LES, to study the atmospheric boundary <span class="hlt">layer</span> dates back to the early 1970s when Deardor (1972) used a three-dimensional simulation to determine velocity and temperature scales in the convective boundary <span class="hlt">layer</span>. In 1974 he applied LES to the problem of mixing <span class="hlt">layer</span> entrainment (Deardor 1974) and in 1980 to the cloud-topped boundary <span class="hlt">layer</span> (Deardor 1980b). Since that time the LES approach has been applied to atmospheric boundary <span class="hlt">layer</span> problems by numerous authors. While LES has been shown to be relatively robust for simple cases such as a clear, convective boundary <span class="hlt">layer</span> (Mason 1989), simulation of the cloud-topped boundary <span class="hlt">layer</span> has proved more of a challenge. The combination of small length scales and anisotropic turbulence coupled with cloud microphysics and radiation effects places a heavy burden on the turbulence <span class="hlt">model</span>, especially in the cloud-top region. Consequently, over the past few decades considerable effort has been devoted to developing turbulence <span class="hlt">models</span> that are better able to parameterize these processes. Much of this work has involved taking parameterizations developed for neutral boundary <span class="hlt">layers</span> and deriving corrections to account for buoyancy effects associated with the background stratification and local buoyancy sources due to radiative and latent heat transfer within the cloud (see Lilly 1962; Deardor 1980a; Mason 1989; MacVean & Mason 1990, for example). In this paper we hope to contribute to this effort by presenting a number of turbulence <span class="hlt">models</span> in which the <span class="hlt">model</span> coefficients are calculated dynamically during the simulation rather than being prescribed a priori.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NJPh...18h3045K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NJPh...18h3045K"><span>Dynamical origins of the community structure of an online multi-<span class="hlt">layer</span> society</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Klimek, Peter; Diakonova, Marina; Eguíluz, Víctor M.; San Miguel, Maxi; Thurner, Stefan</p> <p>2016-08-01</p> <p>Social structures emerge as a result of individuals managing a variety of different social relationships. Societies can be represented as highly structured dynamic multiplex networks. Here we study the dynamical origins of the specific community structures of a large-scale social multiplex network of a human society that interacts in a virtual world of a massive multiplayer online game. There we find substantial differences in the community structures of different social actions, represented by the various <span class="hlt">layers</span> in the multiplex network. Community sizes distributions are either fat-tailed or appear to be centered around a size of 50 individuals. To understand these observations we propose a voter <span class="hlt">model</span> that is built around the principle of triadic closure. It explicitly <span class="hlt">models</span> the co-<span class="hlt">evolution</span> of node- and link-dynamics across different <span class="hlt">layers</span> of the multiplex network. Depending on link and node fluctuation probabilities, the <span class="hlt">model</span> exhibits an anomalous shattered fragmentation transition, where one <span class="hlt">layer</span> fragments from one large component into many small components. The observed community size distributions are in good agreement with the predicted fragmentation in the <span class="hlt">model</span>. This suggests that several detailed features of the fragmentation in societies can be traced back to the triadic closure processes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25293804','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25293804"><span>Cancer <span class="hlt">evolution</span>: mathematical <span class="hlt">models</span> and computational inference.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Beerenwinkel, Niko; Schwarz, Roland F; Gerstung, Moritz; Markowetz, Florian</p> <p>2015-01-01</p> <p>Cancer is a somatic evolutionary process characterized by the accumulation of mutations, which contribute to tumor growth, clinical progression, immune escape, and drug resistance development. Evolutionary theory can be used to analyze the dynamics of tumor cell populations and to make inference about the evolutionary history of a tumor from molecular data. We review recent approaches to <span class="hlt">modeling</span> the <span class="hlt">evolution</span> of cancer, including population dynamics <span class="hlt">models</span> of tumor initiation and progression, phylogenetic methods to <span class="hlt">model</span> the evolutionary relationship between tumor subclones, and probabilistic graphical <span class="hlt">models</span> to describe dependencies among mutations. Evolutionary <span class="hlt">modeling</span> helps to understand how tumors arise and will also play an increasingly important prognostic role in predicting disease progression and the outcome of medical interventions, such as targeted therapy. © The Author(s) 2014. Published by Oxford University Press on behalf of the Society of Systematic Biologists.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002JSV...252..493S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002JSV...252..493S"><span><span class="hlt">Modelling</span> and Vibration Control of Beams with Partially Debonded Active Constrained <span class="hlt">Layer</span> Damping Patch</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>SUN, D.; TONG, L.</p> <p>2002-05-01</p> <p>A detailed <span class="hlt">model</span> for the beams with partially debonded active constraining damping (ACLD) treatment is presented. In this <span class="hlt">model</span>, the transverse displacement of the constraining <span class="hlt">layer</span> is considered to be non-identical to that of the host structure. In the perfect bonding region, the viscoelastic core is <span class="hlt">modelled</span> to carry both peel and shear stresses, while in the debonding area, it is assumed that no peel and shear stresses be transferred between the host beam and the constraining <span class="hlt">layer</span>. The adhesive <span class="hlt">layer</span> between the piezoelectric sensor and the host beam is also considered in this <span class="hlt">model</span>. In active control, the positive position feedback control is employed to control the first mode of the beam. Based on this <span class="hlt">model</span>, the incompatibility of the transverse displacements of the active constraining <span class="hlt">layer</span> and the host beam is investigated. The passive and active damping behaviors of the ACLD patch with different thicknesses, locations and lengths are examined. Moreover, the effects of debonding of the damping <span class="hlt">layer</span> on both passive and active control are examined via a simulation example. The results show that the incompatibility of the transverse displacements is remarkable in the regions near the ends of the ACLD patch especially for the high order vibration modes. It is found that a thinner damping <span class="hlt">layer</span> may lead to larger shear strain and consequently results in a larger passive and active damping. In addition to the thickness of the damping <span class="hlt">layer</span>, its length and location are also key factors to the hybrid control. The numerical results unveil that edge debonding can lead to a reduction of both passive and active damping, and the hybrid damping may be more sensitive to the debonding of the damping <span class="hlt">layer</span> than the passive damping.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CMT...tmp..100F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CMT...tmp..100F"><span>A mechano-biological <span class="hlt">model</span> of multi-tissue <span class="hlt">evolution</span> in bone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Frame, Jamie; Rohan, Pierre-Yves; Corté, Laurent; Allena, Rachele</p> <p>2017-12-01</p> <p>Successfully simulating tissue <span class="hlt">evolution</span> in bone is of significant importance in predicting various biological processes such as bone remodeling, fracture healing and osseointegration of implants. Each of these processes involves in different ways the permanent or transient formation of different tissue types, namely bone, cartilage and fibrous tissues. The tissue <span class="hlt">evolution</span> in specific circumstances such as bone remodeling and fracturing healing is currently able to be <span class="hlt">modeled</span>. Nevertheless, it remains challenging to predict which tissue types and organization can develop without any a priori assumptions. In particular, the role of mechano-biological coupling in this selective tissue <span class="hlt">evolution</span> has not been clearly elucidated. In this work, a multi-tissue <span class="hlt">model</span> has been created which simultaneously describes the <span class="hlt">evolution</span> of bone, cartilage and fibrous tissues. The coupling of the biological and mechanical factors involved in tissue formation has been <span class="hlt">modeled</span> by defining two different tissue states: an immature state corresponding to the early stages of tissue growth and representing cell clusters in a weakly neo-formed Extra Cellular Matrix (ECM), and a mature state corresponding to well-formed connective tissues. This has allowed for the cellular processes of migration, proliferation and apoptosis to be described simultaneously with the changing ECM properties through strain driven diffusion, growth, maturation and resorption terms. A series of finite element simulations were carried out on idealized cantilever bending geometries. Starting from a tissue composition replicating a mid-diaphysis section of a long bone, a steady-state tissue formation was reached over a statically loaded period of 10,000 h (60 weeks). The results demonstrated that bone formation occurred in regions which are optimally physiologically strained. In two additional 1000 h bending simulations both cartilaginous and fibrous tissues were shown to form under specific geometrical and loading</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910026464&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dfunction%2Bwave','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910026464&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dfunction%2Bwave"><span>ISEE observations of low frequency waves and ion distribution function <span class="hlt">evolution</span> in the plasma sheet boundary <span class="hlt">layer</span></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.; Gary, S. P.</p> <p>1990-01-01</p> <p>This paper describes ISEE plasma and magnetic fluctuation observations during two crossings of the plasma sheet boundary <span class="hlt">layer</span> (PSBL) in the earth's magnetotail. Distribution function observations show that the counterstreaming ion components undergo pitch-angle scattering and evolve into a shell distribution in velocity space. This <span class="hlt">evolution</span> is correlated with the development of low frequency, low amplitude magnetic fluctuations. However, the measured wave amplitudes are insufficient to accomplish the observed degree of ion pitch-angle scatttering locally; the near-earth distributions may be the result of processes occurring much farther down the magnetotail. Results show a clear correlation between the ion component beta and the relative streaming speed of the two components, suggesting that electromagnetic ion/ion instabilities do play an important role in the scattering of PSBL ions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhyA..391.3708S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhyA..391.3708S"><span>Space <span class="hlt">evolution</span> <span class="hlt">model</span> and empirical analysis of an urban public transport network</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sui, Yi; Shao, Feng-jing; Sun, Ren-cheng; Li, Shu-jing</p> <p>2012-07-01</p> <p>This study explores the space <span class="hlt">evolution</span> of an urban public transport network, using empirical evidence and a simulation <span class="hlt">model</span> validated on that data. Public transport patterns primarily depend on traffic spatial-distribution, demands of passengers and expected utility of investors. <span class="hlt">Evolution</span> is an iterative process of satisfying the needs of passengers and investors based on a given traffic spatial-distribution. The temporal change of urban public transport network is evaluated both using topological measures and spatial ones. The simulation <span class="hlt">model</span> is validated using empirical data from nine big cities in China. Statistical analyses on topological and spatial attributes suggest that an <span class="hlt">evolution</span> network with traffic demands characterized by power-law numerical values which distribute in a mode of concentric circles tallies well with these nine cities.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ewas.confE...3D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ewas.confE...3D"><span>A Double Zone Dynamical <span class="hlt">Model</span> For The Tidal <span class="hlt">Evolution</span> Of The Obliquity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Damiani, Cilia</p> <p>2017-10-01</p> <p>It is debated wether close-in giants planets can form in-situ and if not, which mechanisms are responsible for their migration. One of the observable tests for migration theories is the current value of the obliquity. But after the main migration mechanism has ended, the combined effects of tidal dissipation and the magnetic braking of the star lead to the <span class="hlt">evolution</span> of both the obliquity and the semi-major axis. The observed correlation between effective temperature and measured projected obliquity has been taken as evidence of such mechanisms being at play. Here I present an improved <span class="hlt">model</span> for the tidal <span class="hlt">evolution</span> of the obliquity. It includes all the components of the dynamical tide for circular misaligned systems. It uses an analytical formulation for the frequency-averaged dissipation for each mode, depending only on global stellar parameters, giving a measure of the dissipative properties of the convective zone of the host as it evolves in time. The <span class="hlt">model</span> also includes the effect of magnetic braking in the framework of the double zone <span class="hlt">model</span>. This results in the estimation of different tidal <span class="hlt">evolution</span> timescales for the <span class="hlt">evolution</span> of the planet's semi-major axis and obliquity depending on the properties of the stellar host. This <span class="hlt">model</span> can be used to test migration theories, provided that a good determination of stellar radii, masses and ages can be obtained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1916114M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1916114M"><span>The development and application of landscape <span class="hlt">evolution</span> <span class="hlt">models</span> to coupled coast-estuarine environments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Morris, Chloe; Coulthard, Tom; Parsons, Daniel R.; Manson, Susan; Barkwith, Andrew</p> <p>2017-04-01</p> <p>Landscape <span class="hlt">Evolution</span> <span class="hlt">Models</span> (LEMs) are proven to be useful tools in understanding the morphodynamics of coast and estuarine systems. However, perhaps owing to the lack of research in this area, current <span class="hlt">models</span> are not capable of simulating the dynamic interactions between these systems and their co-<span class="hlt">evolution</span> at the meso-scale. Through a novel coupling of numerical <span class="hlt">models</span>, this research is designed to explore coupled coastal-estuarine interactions, controls on system behaviour and the influence that environmental change could have. This will contribute to the understanding of the morphodynamics of these systems and how they may behave and evolve over the next century in response to climate changes, with the aim of informing management practices. This goal is being achieved through the modification and coupling of the one-line Coastline <span class="hlt">Evolution</span> <span class="hlt">Model</span> (CEM) with the hydrodynamic LEM CAESAR-Lisflood (C-L). The major issues faced with coupling these programs are their differing complexities and the limited graphical visualisations produced by the CEM that hinder the dissemination of results. The work towards overcoming these issues and reported here, include a new version of the CEM that incorporates a range of more complex geomorphological processes and boasts a graphical user interface that guides users through <span class="hlt">model</span> set-up and projects a live output during <span class="hlt">model</span> runs. The improved version is a stand-alone tool that can be used for further research projects and for teaching purposes. A sensitivity analysis using the Morris method has been completed to identify which key variables, including wave climate, erosion and weathering values, dominate the control of <span class="hlt">model</span> behaviour. The <span class="hlt">model</span> is being applied and tested using the <span class="hlt">evolution</span> of the Holderness Coast, Humber Estuary and Spurn Point on the east coast of England (UK), which possess diverse geomorphologies and complex, co-evolving sediment pathways. Simulations using the modified CEM are currently being completed to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980237907','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980237907"><span>Cloud-Scale Numerical <span class="hlt">Modeling</span> of the Arctic Boundary <span class="hlt">Layer</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Krueger, Steven K.</p> <p>1998-01-01</p> <p>The interactions between sea ice, open ocean, atmospheric radiation, and clouds over the Arctic Ocean exert a strong influence on global climate. Uncertainties in the formulation of interactive air-sea-ice processes in global climate <span class="hlt">models</span> (GCMs) result in large differences between the Arctic, and global, climates simulated by different <span class="hlt">models</span>. Arctic stratus clouds are not well-simulated by GCMs, yet exert a strong influence on the surface energy budget of the Arctic. Leads (channels of open water in sea ice) have significant impacts on the large-scale budgets during the Arctic winter, when they contribute about 50 percent of the surface fluxes over the Arctic Ocean, but cover only 1 to 2 percent of its area. Convective plumes generated by wide leads may penetrate the surface inversion and produce condensate that spreads up to 250 km downwind of the lead, and may significantly affect the longwave radiative fluxes at the surface and thereby the sea ice thickness. The effects of leads and boundary <span class="hlt">layer</span> clouds must be accurately represented in climate <span class="hlt">models</span> to allow possible feedbacks between them and the sea ice thickness. The FIRE III Arctic boundary <span class="hlt">layer</span> clouds field program, in conjunction with the SHEBA ice camp and the ARM North Slope of Alaska and Adjacent Arctic Ocean site, will offer an unprecedented opportunity to greatly improve our ability to parameterize the important effects of leads and boundary <span class="hlt">layer</span> clouds in GCMs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17708768','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17708768"><span>The Biological Big Bang <span class="hlt">model</span> for the major transitions in <span class="hlt">evolution</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Koonin, Eugene V</p> <p>2007-08-20</p> <p>Major transitions in biological <span class="hlt">evolution</span> show the same pattern of sudden emergence of diverse forms at a new level of complexity. The relationships between major groups within an emergent new class of biological entities are hard to decipher and do not seem to fit the tree pattern that, following Darwin's original proposal, remains the dominant description of biological <span class="hlt">evolution</span>. The cases in point include the origin of complex RNA molecules and protein folds; major groups of viruses; archaea and bacteria, and the principal lineages within each of these prokaryotic domains; eukaryotic supergroups; and animal phyla. In each of these pivotal nexuses in life's history, the principal "types" seem to appear rapidly and fully equipped with the signature features of the respective new level of biological organization. No intermediate "grades" or intermediate forms between different types are detectable. Usually, this pattern is attributed to cladogenesis compressed in time, combined with the inevitable erosion of the phylogenetic signal. I propose that most or all major evolutionary transitions that show the "explosive" pattern of emergence of new types of biological entities correspond to a boundary between two qualitatively distinct evolutionary phases. The first, inflationary phase is characterized by extremely rapid <span class="hlt">evolution</span> driven by various processes of genetic information exchange, such as horizontal gene transfer, recombination, fusion, fission, and spread of mobile elements. These processes give rise to a vast diversity of forms from which the main classes of entities at the new level of complexity emerge independently, through a sampling process. In the second phase, <span class="hlt">evolution</span> dramatically slows down, the respective process of genetic information exchange tapers off, and multiple lineages of the new type of entities emerge, each of them evolving in a tree-like fashion from that point on. This biphasic <span class="hlt">model</span> of <span class="hlt">evolution</span> incorporates the previously developed</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1366713-evaluation-alternative-atomistic-models-incipient-growth-zno-atomic-layer-deposition','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1366713-evaluation-alternative-atomistic-models-incipient-growth-zno-atomic-layer-deposition"><span>Evaluation of Alternative Atomistic <span class="hlt">Models</span> for the Incipient Growth of ZnO by Atomic <span class="hlt">Layer</span> Deposition</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>Chu, Manh-Hung; Tian, Liang; Chaker, Ahmad</p> <p></p> <p>ZnO thin films are interesting for applications in several technological fields, including optoelectronics and renewable energies. Nanodevice applications require controlled synthesis of ZnO structures at nanometer scale, which can be achieved via atomic <span class="hlt">layer</span> deposition (ALD). However, the mechanisms governing the initial stages of ALD had not been addressed until very recently. Investigations into the initial nucleation and growth as well as the atomic structure of the heterointerface are crucial to optimize the ALD process and understand the structure-property relationships for ZnO. We have used a complementary suite of in situ synchrotron x-ray techniques to investigate both the structural andmore » chemical <span class="hlt">evolution</span> during ZnO growth by ALD on two different substrates, i.e., SiO2 and Al2O3, which led us to formulate an atomistic <span class="hlt">model</span> of the incipient growth of ZnO. The <span class="hlt">model</span> relies on the formation of nanoscale islands of different size and aspect ratio and consequent disorder induced in the Zn neighbors' distribution. However, endorsement of our <span class="hlt">model</span> requires testing and discussion of possible alternative <span class="hlt">models</span> which could account for the experimental results. In this work, we review, test, and rule out several alternative <span class="hlt">models</span>; the results confirm our view of the atomistic mechanisms at play, which influence the overall microstructure and resulting properties of the final thin film.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22590604-theory-multiple-quantum-dot-formation-strained-layer-heteroepitaxy','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22590604-theory-multiple-quantum-dot-formation-strained-layer-heteroepitaxy"><span>Theory of multiple quantum dot formation in strained-<span class="hlt">layer</span> heteroepitaxy</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>Du, Lin; Maroudas, Dimitrios, E-mail: maroudas@ecs.umass.edu</p> <p>2016-07-11</p> <p>We develop a theory for the experimentally observed formation of multiple quantum dots (QDs) in strained-<span class="hlt">layer</span> heteroepitaxy based on surface morphological stability analysis of a coherently strained epitaxial thin film on a crystalline substrate. Using a fully nonlinear <span class="hlt">model</span> of surface morphological <span class="hlt">evolution</span> that accounts for a wetting potential contribution to the epitaxial film's free energy as well as surface diffusional anisotropy, we demonstrate the formation of multiple QD patterns in self-consistent dynamical simulations of the <span class="hlt">evolution</span> of the epitaxial film surface perturbed from its planar state. The simulation predictions are supported by weakly nonlinear analysis of the epitaxial filmmore » surface morphological stability. We find that, in addition to the Stranski-Krastanow instability, long-wavelength perturbations from the planar film surface morphology can trigger a nonlinear instability, resulting in the splitting of a single QD into multiple QDs of smaller sizes, and predict the critical wavelength of the film surface perturbation for the onset of the nonlinear tip-splitting instability. The theory provides a fundamental interpretation for the observations of “QD pairs” or “double QDs” and other multiple QDs reported in experimental studies of epitaxial growth of semiconductor strained <span class="hlt">layers</span> and sets the stage for precise engineering of tunable-size nanoscale surface features in strained-<span class="hlt">layer</span> heteroepitaxy by exploiting film surface nonlinear, pattern forming phenomena.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JSSCh.203...19B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JSSCh.203...19B"><span>Synthesis and controlled release properties of 2,4-dichlorophenoxy acetate-zinc <span class="hlt">layered</span> hydroxide nanohybrid</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bashi, Abbas M.; Hussein, Mohd Zobir; Zainal, Zulkarnain; Tichit, Didier</p> <p>2013-07-01</p> <p>Direct reaction of ZnO with 2,4-dichlorophenoxyacetic acid (24D) solutions of different concentrations allows obtaining new organic-inorganic nanohybrid materials formed by intercalation of 24D into interlayers of zinc <span class="hlt">layered</span> hydroxide (ZLH). XRD patterns show a progressive <span class="hlt">evolution</span> of the structure as 24D concentration increases. The nanohybrid obtained at higher 24D concentration (24D-ZLH(0.4)) reveals a well ordered <span class="hlt">layered</span> structure with two different basal spacings at 25.2 Å and 24 Å. The FTIR spectrum showing the vibrations bands of the functional groups of 24D and of the ZLH confirms the intercalation. SEM images are in agreement with the structural <span class="hlt">evolution</span> observed by XRD and reveal the ribbon morphology of the nanohybrids. The release studies of 24D showed a rapid release of 94% for the first 100 min governed by the pseudo-second order kinetic <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015JAMES...7..188W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015JAMES...7..188W"><span>The effects of vortex structure and vortex translation on the tropical cyclone boundary <span class="hlt">layer</span> wind field</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Williams, Gabriel J.</p> <p>2015-03-01</p> <p>The effects of vortex translation and radial vortex structure in the distribution of boundary <span class="hlt">layer</span> winds in the inner core of mature tropical cyclones are examined using a high-resolution slab <span class="hlt">model</span> and a multilevel <span class="hlt">model</span>. It is shown that the structure and magnitude of the wind field (and the corresponding secondary circulation) depends sensitively on the radial gradient of the gradient wind field above the boundary <span class="hlt">layer</span>. Furthermore, it is shown that vortex translation creates low wave number asymmetries in the wind field that rotate anticyclonically with height. A budget analysis of the steady state wind field for both <span class="hlt">models</span> was also performed in this study. Although the agradient force drives the <span class="hlt">evolution</span> of the boundary <span class="hlt">layer</span> wind field for both <span class="hlt">models</span>, it is shown that the manner in which the boundary <span class="hlt">layer</span> flow responds to this force differs between the two <span class="hlt">model</span> representations. In particular, the inner core boundary <span class="hlt">layer</span> flow in the slab <span class="hlt">model</span> is dominated by the effects of horizontal advection and horizontal diffusion, leading to the development of shock structures in the <span class="hlt">model</span>. Conversely, the inner core boundary <span class="hlt">layer</span> flow in the multilevel <span class="hlt">model</span> is primarily influenced by the effects of vertical advection and vertical diffusion, which eliminates shock structures in this <span class="hlt">model</span>. These results further indicate that special care is required to ensure that qualitative applications from slab <span class="hlt">models</span> are not unduly affected by the neglect of vertical advection. This article was corrected on 31 MAR 2015. See the end of the full text for details.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/990150-rationality-validation-layered-decision-model-network-defense','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/990150-rationality-validation-layered-decision-model-network-defense"><span>Rationality Validation of a <span class="hlt">Layered</span> Decision <span class="hlt">Model</span> for Network Defense</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>Wei, Huaqiang; Alves-Foss, James; Zhang, Du</p> <p>2007-08-31</p> <p>We propose a cost-effective network defense strategy built on three key: three decision <span class="hlt">layers</span>: security policies, defense strategies, and real-time defense tactics for countering immediate threats. A <span class="hlt">layered</span> decision <span class="hlt">model</span> (LDM) can be used to capture this decision process. The LDM helps decision-makers gain insight into the hierarchical relationships among inter-connected entities and decision types, and supports the selection of cost-effective defense mechanisms to safeguard computer networks. To be effective as a business tool, it is first necessary to validate the rationality of <span class="hlt">model</span> before applying it to real-world business cases. This paper describes our efforts in validating the LDMmore » rationality through simulation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27031686','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27031686"><span>Artery buckling analysis using a two-<span class="hlt">layered</span> wall <span class="hlt">model</span> with collagen dispersion.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Mottahedi, Mohammad; Han, Hai-Chao</p> <p>2016-07-01</p> <p>Artery buckling has been proposed as a possible cause for artery tortuosity associated with various vascular diseases. Since microstructure of arterial wall changes with aging and diseases, it is essential to establish the relationship between microscopic wall structure and artery buckling behavior. The objective of this study was to developed arterial buckling equations to incorporate the two-<span class="hlt">layered</span> wall structure with dispersed collagen fiber distribution. Seven porcine carotid arteries were tested for buckling to determine their critical buckling pressures at different axial stretch ratios. The mechanical properties of these intact arteries and their intima-media <span class="hlt">layer</span> were determined via pressurized inflation test. Collagen alignment was measured from histological sections and <span class="hlt">modeled</span> by a modified von-Mises distribution. Buckling equations were developed accordingly using microstructure-motivated strain energy function. Our results demonstrated that collagen fibers disperse around two mean orientations symmetrically to the circumferential direction (39.02°±3.04°) in the adventitia <span class="hlt">layer</span>; while aligning closely in the circumferential direction (2.06°±3.88°) in the media <span class="hlt">layer</span>. The microstructure based two-<span class="hlt">layered</span> <span class="hlt">model</span> with collagen fiber dispersion described the buckling behavior of arteries well with the <span class="hlt">model</span> predicted critical pressures match well with the experimental measurement. Parametric studies showed that with increasing fiber dispersion parameter, the predicted critical buckling pressure increases. These results validate the microstructure-based <span class="hlt">model</span> equations for artery buckling and set a base for further studies to predict the stability of arteries due to microstructural changes associated with vascular diseases and aging. Copyright © 2016 Elsevier Ltd. All rights reserved.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A52C..07J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A52C..07J"><span><span class="hlt">Modeling</span> of Shallow Marine Cloud Topped Boundary <span class="hlt">Layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Janjic, Z.</p> <p>2017-12-01</p> <p>A common problem in many atmospheric <span class="hlt">models</span> is excessive expansion over cold water of shallow marine planetary boundary <span class="hlt">layer</span> (PBL) topped by a thin cloud <span class="hlt">layer</span>. This phenomenon is often accompanied by spurious light precipitation. The "Cloud Top Entrainment Instability" (CTEI) was proposed as an explanation of the mechanism controlling this process and thus preventing spurious enlargement of the cloudy area and widely spread light precipitation observed in the <span class="hlt">models</span>. A key element of this hypothesis is evaporative cooling at the PBL top. However, the CTEI hypothesis remains controversial. For example, a recent direct simulation experiment indicated that the evaporative cooling couldn't explain the break-up of the cloudiness as hypothesized by the CTEI. Here, it is shown that the cloud break-up can be achieved in numerical <span class="hlt">models</span> by a further modification of the nonsingular implementation of the nonsingular Mellor-Yamada Level 2.5 turbulence closure <span class="hlt">model</span> (MYJ) developed at the National Centers for Environmental Prediction (NCEP) Washington. Namely, the impact of moist convective instability is included into the turbulent energy production/dissipation equation if (a) the stratification is stable, (b) the lifting condensation level (LCL) for a particle starting at a <span class="hlt">model</span> level is below the next upper <span class="hlt">model</span> level, and (c) there is enough turbulent kinetic energy so that, due to random vertical turbulent motions, a particle starting from a <span class="hlt">model</span> level can reach its LCL. The criterion (c) should be sufficiently restrictive because otherwise the cloud cover can be completely removed. A real data example will be shown demonstrating the ability of the method to break the spurious cloud cover during the day, but also to allow its recovery over night.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JMEP...25.5382P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JMEP...25.5382P"><span><span class="hlt">Evolution</span> of Initial Atmospheric Corrosion of Carbon Steel in an Industrial Atmosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pan, Chen; Han, Wei; Wang, Zhenyao; Wang, Chuan; Yu, Guocai</p> <p>2016-12-01</p> <p>The <span class="hlt">evolution</span> of initial corrosion of carbon steel exposed to an industrial atmosphere in Shenyang, China, has been investigated by gravimetric, XRD, SEM/EDS and electrochemical techniques. The kinetics of the corrosion process including the acceleration and deceleration processes followed the empirical equation D = At n . The rust formed on the steel surface was bi-<span class="hlt">layered</span>, comprised of an inner and outer <span class="hlt">layer</span>. The outer <span class="hlt">layer</span> was formed within the first 245 days and had lower iron content compared to the inner <span class="hlt">layer</span>. However, the outer <span class="hlt">layer</span> disappeared after 307 days of exposure, which is considered to be associated with the depletion of Fe3O4. The <span class="hlt">evolution</span> of the rust <span class="hlt">layer</span> formed on the carbon steel has also been discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2007SPIE.6632E..0EM','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2007SPIE.6632E..0EM"><span>Space-time <span class="hlt">modeling</span> of the photon diffusion in a three-<span class="hlt">layered</span> <span class="hlt">model</span>: application to the study of muscular oxygenation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mansouri, C.; L'Huillier, J. P.; Piron, V.</p> <p>2007-07-01</p> <p>This work presents results on the <span class="hlt">modeling</span> of the photon diffusion in a three-<span class="hlt">layered</span> <span class="hlt">model</span>, (skin, fat and muscle). The Finite Element method was performed in order to calculate the temporal response of the above-mentioned structure. The thickness of the fat <span class="hlt">layer</span> was varied from 1 to 15 mm to investigate the effects of increasing fat thickness on the muscle <span class="hlt">layer</span> absorption coefficient measurements for a source-detector spacing of 30 mm. The simulated time-resolved reflectance data, at different wavelengths, were fitted to the diffusion <span class="hlt">model</span> to yield the scattering and absorption coefficients of muscle. The errors in estimating muscle absorption coefficients μ α depend on the thickness of the fat <span class="hlt">layer</span> and its optical properties. In addition, it was shown that it is possible to recover with a good precision (~2.6 % of error) the absorption coefficient of muscle and this up to a thickness of the fat <span class="hlt">layer</span> not exceeding 4mm. Beyond this limit a correction is proposed in order to make measurements coherent. The muscle-corrected absorption coefficient can be then used to calculate hemoglobin oxygenation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20080037787&hterms=supercritical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsupercritical','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20080037787&hterms=supercritical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dsupercritical"><span>The Supercritical Pile GRB <span class="hlt">Model</span>: The Prompt to Afterglow <span class="hlt">Evolution</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kazanas, Demosthenes</p> <p>2008-01-01</p> <p>The 'Supercritical Pile' is a very economical gamma ray burst (GRB) <span class="hlt">model</span> that provides for the efficient conversion of the energy stored in the protons of a Relativistic Blast Wave (RBW) into radiation and at the same time produces - in the prompt GRB phase, even in the absence of any particle acceleration - a spectral peak at an energy sim 1 MeV. We extend this <span class="hlt">model</span> to include also the <span class="hlt">evolution</span> of the RBW Lorentz factor Gamma and thus follow the spectral and temporal features of this <span class="hlt">model</span> into the early GRB afterglow stage. One of the novel features of the present treatment is the inclusion of the feedback of the GRB produced radiation on the <span class="hlt">evolution</span> of Gamma with radius. This feedback and the presence of kinematic and dynamic thresholds in the <span class="hlt">model</span> can be the sources of rich time <span class="hlt">evolution</span> which we have begun to explore. In particular, one can this way obtain afterglow light curves with steep decays followed by the more conventional flatter afterglow slopes, while at the same time preserving the desirable features of the <span class="hlt">model</span>, i.e. the well defined relativistic electron source and radiative processes that produce the proper peak in the nu F spectra. Furthermore, the existence of a kinematic threshold in this <span class="hlt">model</span> provides for a operational distinction of the prompt and afterglow GRB stages; in fact, the afterglow stage sets in when the RBW Lorentz factor cannot anymore fulfill the kinematic condition for pair formation in the photon - proton pair production reactions that constitute the fundamental process for the dissipation of the blast wave kinetic energy. We present the results of a specific set of parameters of this <span class="hlt">model</span> with emphasis on the multiwavelength prompt emission and transition to the early afterglow.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1343950','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1343950"><span>Phase field <span class="hlt">modeling</span> of microstructure <span class="hlt">evolution</span> and concomitant effective conductivity change in solid oxide fuel cell electrodes</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>Lei, Yinkai; Cheng, Tian -Le; Wen, You -Hai</p> <p></p> <p>Microstructure <span class="hlt">evolution</span> plays an important role in the performance degradation of SOFC electrodes. In this work, we propose a much improved phase field <span class="hlt">model</span> to simulate the microstructure <span class="hlt">evolution</span> in the electrodes of solid oxide fuel cell. We demonstrate that the tunability of the interfacial energy in this <span class="hlt">model</span> has been significantly enhanced. Parameters are set to fit for the interfacial energies of a typical Ni-YSZ anode, an LSM-YSZ cathode and an artificial reference electrode, respectively. The contact angles at various triple junctions and the microstructure <span class="hlt">evolutions</span> in two dimensions are calibrated to verify the <span class="hlt">model</span>. As a demonstration ofmore » the capabilities of the <span class="hlt">model</span>, three dimensional microstructure <span class="hlt">evolutions</span> are simulated applying the <span class="hlt">model</span> to the three different electrodes. The time <span class="hlt">evolutions</span> of grain size and triple phase boundary density are analyzed. In addition, a recently proposed bound charge successive approximation algorithm is employed to calculate the effective conductivity of the electrodes during microstructure <span class="hlt">evolution</span>. Furthermore, the effective conductivity of all electrodes are found to decrease during the microstructure <span class="hlt">evolution</span>, which is attributed to the increased tortuosity and the loss of percolated volume fraction of the electrode phase.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1343950-phase-field-modeling-microstructure-evolution-concomitant-effective-conductivity-change-solid-oxide-fuel-cell-electrodes','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1343950-phase-field-modeling-microstructure-evolution-concomitant-effective-conductivity-change-solid-oxide-fuel-cell-electrodes"><span>Phase field <span class="hlt">modeling</span> of microstructure <span class="hlt">evolution</span> and concomitant effective conductivity change in solid oxide fuel cell electrodes</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Lei, Yinkai; Cheng, Tian -Le; Wen, You -Hai</p> <p>2017-02-13</p> <p>Microstructure <span class="hlt">evolution</span> plays an important role in the performance degradation of SOFC electrodes. In this work, we propose a much improved phase field <span class="hlt">model</span> to simulate the microstructure <span class="hlt">evolution</span> in the electrodes of solid oxide fuel cell. We demonstrate that the tunability of the interfacial energy in this <span class="hlt">model</span> has been significantly enhanced. Parameters are set to fit for the interfacial energies of a typical Ni-YSZ anode, an LSM-YSZ cathode and an artificial reference electrode, respectively. The contact angles at various triple junctions and the microstructure <span class="hlt">evolutions</span> in two dimensions are calibrated to verify the <span class="hlt">model</span>. As a demonstration ofmore » the capabilities of the <span class="hlt">model</span>, three dimensional microstructure <span class="hlt">evolutions</span> are simulated applying the <span class="hlt">model</span> to the three different electrodes. The time <span class="hlt">evolutions</span> of grain size and triple phase boundary density are analyzed. In addition, a recently proposed bound charge successive approximation algorithm is employed to calculate the effective conductivity of the electrodes during microstructure <span class="hlt">evolution</span>. Furthermore, the effective conductivity of all electrodes are found to decrease during the microstructure <span class="hlt">evolution</span>, which is attributed to the increased tortuosity and the loss of percolated volume fraction of the electrode phase.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5765341','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5765341"><span><span class="hlt">Modeling</span> the <span class="hlt">Evolution</span> of Female Meiotic Drive in Maize</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Hall, David W.; Dawe, R. Kelly</p> <p>2017-01-01</p> <p>Autosomal drivers violate Mendel’s law of segregation in that they are overrepresented in gametes of heterozygous parents. For drivers to be polymorphic within populations rather than fixing, their transmission advantage must be offset by deleterious effects on other fitness components. In this paper, we develop an analytical <span class="hlt">model</span> for the <span class="hlt">evolution</span> of autosomal drivers that is motivated by the neocentromere drive system found in maize. In particular, we <span class="hlt">model</span> both the transmission advantage and deleterious fitness effects on seed viability, pollen viability, seed to adult survival mediated by maternal genotype, and seed to adult survival mediated by offspring genotype. We derive general, biologically intuitive conditions for the four most likely evolutionary outcomes and discuss the expected <span class="hlt">evolution</span> of autosomal drivers given these conditions. Finally, we determine the expected equilibrium allele frequencies predicted by the <span class="hlt">model</span> given recent estimates of fitness components for all relevant genotypes and show that the predicted equilibrium is within the range observed in maize land races for levels of drive at the low end of what has been observed. PMID:29122849</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AIPC..727..578B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AIPC..727..578B"><span>Firework <span class="hlt">Model</span>: Time Dependent Spectral <span class="hlt">Evolution</span> of GRB</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barbiellini, Guido; Longo, Francesco; Ghirlanda, G.; Celotti, A.; Bosnjak, Z.</p> <p>2004-09-01</p> <p>The energetics of the long duration GRB phenomenon is compared with <span class="hlt">models</span> of a rotating BH in a strong magnetic field generated by an accreting torus. The GRB energy emission is attributed to magnetic field vacuum breakdown that gives origin to a e +/- fireball. Its subsequent <span class="hlt">evolution</span> is hypothesized in analogy with the in-flight decay of an elementary particle. An anisotropy in the fireball propagation is thus naturally produced. The recent discovery in some GRB of an initial phase characterized by a thermal spectrum could be interpreted as the photon emission of the fireball photosphere when it becomes transparent. In particular, the temporal <span class="hlt">evolution</span> of the emission can be explained as the effect of a radiative deceleration of the out-moving ejecta.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23369823','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23369823"><span>A three-<span class="hlt">layer</span> <span class="hlt">model</span> of natural image statistics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Gutmann, Michael U; Hyvärinen, Aapo</p> <p>2013-11-01</p> <p>An important property of visual systems is to be simultaneously both selective to specific patterns found in the sensory input and invariant to possible variations. Selectivity and invariance (tolerance) are opposing requirements. It has been suggested that they could be joined by iterating a sequence of elementary selectivity and tolerance computations. It is, however, unknown what should be selected or tolerated at each level of the hierarchy. We approach this issue by learning the computations from natural images. We propose and estimate a probabilistic <span class="hlt">model</span> of natural images that consists of three processing <span class="hlt">layers</span>. Two natural image data sets are considered: image patches, and complete visual scenes downsampled to the size of small patches. For both data sets, we find that in the first two <span class="hlt">layers</span>, simple and complex cell-like computations are performed. In the third <span class="hlt">layer</span>, we mainly find selectivity to longer contours; for patch data, we further find some selectivity to texture, while for the downsampled complete scenes, some selectivity to curvature is observed. Copyright © 2013 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MNRAS.469S.741P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MNRAS.469S.741P"><span>A three-dimensional <span class="hlt">modelling</span> of the <span class="hlt">layered</span> structure of comet 67P/Churyumov-Gerasimenko</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Penasa, L.; Massironi, M.; Naletto, G.; Simioni, E.; Ferrari, S.; Pajola, M.; Lucchetti, A.; Preusker, F.; Scholten, F.; Jorda, L.; Gaskell, R.; Ferri, F.; Marzari, F.; Davidsson, B.; Mottola, S.; Sierks, H.; Barbieri, C.; Lamy, P. L.; Rodrigo, R.; Koschny, D.; Rickman, H.; Keller, H. U.; Agarwal, J.; A'Hearn, M. F.; Barucci, M. A.; Bertaux, J. L.; Bertini, I.; Cremonese, G.; Da Deppo, V.; Debei, S.; De Cecco, M.; Deller, J.; Feller, C.; Fornasier, S.; Frattin, E.; Fulle, M.; Groussin, O.; Gutierrez, P. J.; Güttler, C.; Hofmann, M.; Hviid, S. F.; Ip, W. H.; Knollenberg, J.; Kramm, J. R.; Kührt, E.; Küppers, M.; La Forgia, F.; Lara, L. M.; Lazzarin, M.; Lee, J.-C.; Lopez Moreno, J. J.; Oklay, N.; Shi, X.; Thomas, N.; Tubiana, C.; Vincent, J. B.</p> <p>2017-07-01</p> <p>We provide a three-dimensional <span class="hlt">model</span> of the inner <span class="hlt">layered</span> structure of comet 67P based on the hypothesis of an extended <span class="hlt">layering</span> independently wrapping each lobe. A large set of terrace orientations was collected on the latest shape <span class="hlt">model</span> and then used as a proxy for the local orientation of the surfaces of discontinuity which defines the <span class="hlt">layers</span>. We <span class="hlt">modelled</span> the terraces as a family of concentric ellipsoidal shells with fixed axis ratios, producing a <span class="hlt">model</span> that is completely defined by just eight free parameters. Each lobe of 67P has been <span class="hlt">modelled</span> independently, and the two sets of parameters have been estimated by means of non-linear optimization of the measured terrace orientations. The proposed <span class="hlt">model</span> is able to predict the orientation of terraces, the elongation of cliffs, the linear traces observed in the Wosret and Hathor regions and the peculiar alignment of boulder-like features which has been observed in the Hapi region, which appears to be related to the inner <span class="hlt">layering</span> of the big lobe. Our analysis allowed us to identify a plane of junction between the two lobes, further confirming the independent nature of the lobes. Our <span class="hlt">layering</span> <span class="hlt">models</span> differ from the best-fitting topographic ellipsoids of the surface, demonstrating that the terraces are aligned to an internal structure of discontinuities, which is unevenly exposed on the surface, suggesting a complex history of localized material removal from the nucleus.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19980201071','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19980201071"><span>A <span class="hlt">Model</span> with Ellipsoidal Scatterers for Polarimetric Remote Sensing of Anisotropic <span class="hlt">Layered</span> Media</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Nghiem, S. V.; Kwok, R.; Kong, J. A.; Shin, R. T.</p> <p>1993-01-01</p> <p>This paper presents a <span class="hlt">model</span> with ellipsoidal scatterers for applications to polarimetric remote sensing of anisotropic <span class="hlt">layered</span> media at microwave frequencies. The physical configuration includes an isotropic <span class="hlt">layer</span> covering an anisotropic <span class="hlt">layer</span> above a homogeneous half space. The isotropic <span class="hlt">layer</span> consists of randomly oriented spheroids. The anisotropic <span class="hlt">layer</span> contains ellipsoidal scatterers with a preferential vertical alignment and random azimuthal orientations. Effective permittivities of the scattering media are calculated with the strong fluctuation theory extended to account for the nonspherical shapes and the scatterer orientation distributions. On the basis of the analytic wave theory, dyadic Green's functions for <span class="hlt">layered</span> media are used to derive polarimetric backscattering coefficients under the distorted Born approximation. The ellipsoidal shape of the scatterers gives rise to nonzero cross-polarized returns from the untilted anisotropic medium in the first-order approximation. Effects of rough interfaces are estimated by an incoherent addition method. Theoretical results and experimental data are matched at 9 GHz for thick first-year sea ice with a bare surface and with a snow cover at Point Barrow, Alaska. The <span class="hlt">model</span> is then used to study the sensitivity of polarimetric backscattering coefficients with respect to correlation lengths representing the geometry of brine inclusions. Polarimetric signatures of bare and snow-covered sea ice are also simulated based on the <span class="hlt">model</span> to investigate effects of different scattering mechanisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.A11M0190C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.A11M0190C"><span>Experimental Findings from Aircraft Measurements in the Residual <span class="hlt">Layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Caputi, D.; Conley, S. A.; Faloona, I. C.; Trousdell, J.</p> <p>2016-12-01</p> <p>The southern San Joaquin Valley of California is home to some of the highest ozone pollution in the United States. Thus, a complete understanding of boundary <span class="hlt">layer</span> dynamics in this area during high ozone events is crucial for better ozone forecasting and effective attainment planning. This work will discuss the results from five aircraft deployments, spanning two summers, in which a Mooney aircraft operated by Scientific Aviation Inc. was flown between Fresno and Bakersfield throughout the diurnal cycle, measuring ozone, NOx, and methane. Under a simple budgeting <span class="hlt">model</span>, changes in any species within the boundary <span class="hlt">layer</span> can occur from advection, chemical production or loss, surface fluxes or deposition, and entrainment between the boundary <span class="hlt">layer</span> and free troposphere. The advection of ozone appears to be most appreciable at night with stronger winds in the residual <span class="hlt">layer</span>, and are on the order of 2 to 4 ppb hr-1. The nighttime chemical loss of ozone due to interaction with NO2 can be estimated by simple numerical <span class="hlt">modeling</span> of observed quantities and reaction rates, and is found to often roughly compensate for the advection, with typical calculated values of -1 to -3 ppb hr-1. The mixing component is more difficult to directly quantify, but attempts are being made to estimate eddy viscosity by solving for this term in the budget equation. Additionally, small-scale features, such as nocturnal elevated mixed <span class="hlt">layers</span>, localized BRN (bulk Richardson number) minimums, and low level jets are spotted in systematic ways throughout the flight data, and it is speculated that these may have a role in the transfer of ozone from the residual <span class="hlt">layer</span> to the surface <span class="hlt">layer</span>. Ultimately, the preliminary data is promising for the eventual goal of linking together the observed boundary <span class="hlt">layer</span> <span class="hlt">evolution</span> with ozone production during air pollution episodes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJB...90..226T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJB...90..226T"><span>Constraints and entropy in a <span class="hlt">model</span> of network <span class="hlt">evolution</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tee, Philip; Wakeman, Ian; Parisis, George; Dawes, Jonathan; Kiss, István Z.</p> <p>2017-11-01</p> <p>Barabási-Albert's "Scale Free" <span class="hlt">model</span> is the starting point for much of the accepted theory of the <span class="hlt">evolution</span> of real world communication networks. Careful comparison of the theory with a wide range of real world networks, however, indicates that the <span class="hlt">model</span> is in some cases, only a rough approximation to the dynamical <span class="hlt">evolution</span> of real networks. In particular, the exponent γ of the power law distribution of degree is predicted by the <span class="hlt">model</span> to be exactly 3, whereas in a number of real world networks it has values between 1.2 and 2.9. In addition, the degree distributions of real networks exhibit cut offs at high node degree, which indicates the existence of maximal node degrees for these networks. In this paper we propose a simple extension to the "Scale Free" <span class="hlt">model</span>, which offers better agreement with the experimental data. This improvement is satisfying, but the <span class="hlt">model</span> still does not explain why the attachment probabilities should favor high degree nodes, or indeed how constraints arrive in non-physical networks. Using recent advances in the analysis of the entropy of graphs at the node level we propose a first principles derivation for the "Scale Free" and "constraints" <span class="hlt">model</span> from thermodynamic principles, and demonstrate that both preferential attachment and constraints could arise as a natural consequence of the second law of thermodynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18226554','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18226554"><span>Wood-feeding cockroaches as <span class="hlt">models</span> for termite <span class="hlt">evolution</span> (Insecta: Dictyoptera): Cryptocercus vs. Parasphaeria boleiriana.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Klass, Klaus-Dieter; Nalepa, Christine; Lo, Nathan</p> <p>2008-03-01</p> <p>Isoptera are highly specialized cockroaches and are one of the few eusocial insect lineages. Cryptocercus cockroaches have appeared to many as ideal <span class="hlt">models</span> for inference on the early <span class="hlt">evolution</span> of termites, due to their possible phylogenetic relationship and several shared key attributes in life history. Recently, Pellens, Grandcolas, and colleagues have proposed the blaberid cockroach Parasphaeria boleiriana to be an alternative <span class="hlt">model</span> for the early <span class="hlt">evolution</span> in termites. We compare the usefulness of Cryptocercus and P. boleiriana as <span class="hlt">models</span> for termite <span class="hlt">evolution</span>. Cryptocercus and lower Isoptera (1) can both feed on comparatively recalcitrant wood, (2) have an obligate, rich and unique hypermastigid and oxymonadid fauna in the hindgut, (3) transfer these flagellates to the next generation by anal trophallaxis, (4) have social systems that involve long-lasting biparental care, and, finally, (5) are strongly suggested to be sister groups, so that the key attributes (1)-(4) appear to be homologous between the two taxa. On the other hand, P. boleiriana (1) feeds on soft, ephemeral wood sources, (2) shows no trace of the oxymonadid and hypermastigid hindgut fauna unique to Cryptocercus and lower Isoptera, nor does it have any other demonstrated obligate relationship with hindgut flagellates, (3) is likely to lack anal trophallaxis, (4) has only a short period of uniparental brood care, and (5) is phylogenetically remote from the Cryptocercus+Isoptera clade. These facts would argue against any reasonable usage of P. boleiriana as a <span class="hlt">model</span> for the early <span class="hlt">evolution</span> of Isoptera or even of the clade Cryptocercus+Isoptera. Cryptocercus thus remains an appropriate <span class="hlt">model</span>-taxon-by-homology for early termite <span class="hlt">evolution</span>. As compared to P. boleiriana, some other Blaberidae (such as the Panesthiinae Salganea) appear more useful as <span class="hlt">model</span>-taxa-by-homoplasy for the early <span class="hlt">evolution</span> of the Cryptocercus+Isoptera clade, as their brooding behavior is more elaborate than in P. boleiriana.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMOS21C..04S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMOS21C..04S"><span>Subgrid <span class="hlt">Modeling</span> Geomorphological and Ecological Processes in Salt Marsh <span class="hlt">Evolution</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shi, F.; Kirby, J. T., Jr.; Wu, G.; Abdolali, A.; Deb, M.</p> <p>2016-12-01</p> <p>Numerical <span class="hlt">modeling</span> a long-term <span class="hlt">evolution</span> of salt marshes is challenging because it requires an extensive use of computational resources. Due to the presence of narrow tidal creeks, variations of salt marsh topography can be significant over spatial length scales on the order of a meter. With growing availability of high-resolution bathymetry measurements, like LiDAR-derived DEM data, it is increasingly desirable to run a high-resolution <span class="hlt">model</span> in a large domain and for a long period of time to get trends of sedimentation patterns, morphological change and marsh <span class="hlt">evolution</span>. However, high spatial-resolution poses a big challenge in both computational time and memory storage, when simulating a salt marsh with dimensions of up to O(100 km^2) with a small time step. In this study, we have developed a so-called Pre-storage, Sub-grid <span class="hlt">Model</span> (PSM, Wu et al., 2015) for simulating flooding and draining processes in salt marshes. The simulation of Brokenbridge salt marsh, Delaware, shows that, with the combination of the sub-grid <span class="hlt">model</span> and the pre-storage method, over 2 orders of magnitude computational speed-up can be achieved with minimal loss of <span class="hlt">model</span> accuracy. We recently extended PSM to include a sediment transport component and <span class="hlt">models</span> for biomass growth and sedimentation in the sub-grid <span class="hlt">model</span> framework. The sediment transport <span class="hlt">model</span> is formulated based on a newly derived sub-grid sediment concentration equation following Defina's (2000) area-averaging procedure. Suspended sediment transport is <span class="hlt">modeled</span> by the advection-diffusion equation in the coarse grid level, but the local erosion and sedimentation rates are integrated over the sub-grid level. The morphological <span class="hlt">model</span> is based on the existing morphological <span class="hlt">model</span> in NearCoM (Shi et al., 2013), extended to include organic production from the biomass <span class="hlt">model</span>. The vegetation biomass is predicted by a simple logistic equation <span class="hlt">model</span> proposed by Marani et al. (2010). The biomass component is loosely coupled with hydrodynamic and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70047820','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70047820"><span>Effects of <span class="hlt">model</span> <span class="hlt">layer</span> simplification using composite hydraulic properties</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Sepúlveda, Nicasio; Kuniansky, Eve L.</p> <p>2010-01-01</p> <p>The effects of simplifying hydraulic property <span class="hlt">layering</span> within an unconfined aquifer and the underlying confining unit were assessed. The hydraulic properties of lithologic units within the unconfined aquifer and confining unit were computed by analyzing the aquifer-test data using radial, axisymmetric two-dimensional (2D) flow. Time-varying recharge to the unconfined aquifer and pumping from the confined Upper Floridan aquifer (USA) were simulated using 3D flow. Conceptual flow <span class="hlt">models</span> were developed by gradually reducing the number of lithologic units in the unconfined aquifer and confining unit by calculating composite hydraulic properties for the simplified lithologic units. Composite hydraulic properties were calculated using either thickness-weighted averages or inverse <span class="hlt">modeling</span> using regression-based parameter estimation. No significant residuals were simulated when all lithologic units comprising the unconfined aquifer were simulated as one <span class="hlt">layer</span>. The largest residuals occurred when the unconfined aquifer and confining unit were aggregated into a single <span class="hlt">layer</span> (quasi-3D), with residuals over 100% for the leakage rates to the confined aquifer and the heads in the confining unit. Residuals increased with contrasts in vertical hydraulic conductivity between the unconfined aquifer and confining unit. Residuals increased when the constant-head boundary at the bottom of the Upper Floridan aquifer was replaced with a no-flow boundary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.U41A..01N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.U41A..01N"><span>Observations of the Summertime Boundary <span class="hlt">Layer</span> over the Ross Ice Shelf, Antarctica Using SUMO UAVs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nigro, M. A.; Cassano, J. J.; Jolly, B.; McDonald, A.</p> <p>2014-12-01</p> <p>During January 2014 Small Unmanned Meteorological Observer (SUMO) unmanned aerial vehicles (UAVs) were used to observe the boundary <span class="hlt">layer</span> over the Ross Ice Shelf, Antarctica. A total of 41 SUMO flights were completed during a 9-day period with a maximum of 11 flights during a single day. Flights occurred as frequently as every 1.5 hours so that the time <span class="hlt">evolution</span> of the boundary <span class="hlt">layer</span> could be documented. On almost all of the flights the boundary <span class="hlt">layer</span> was well mixed from the surface to a depth of less than 50 m to over 350 m. The depth of the well-mixed <span class="hlt">layer</span> was observed to both increase and decrease over the course of an individual day suggesting that processes other than entrainment were altering the boundary <span class="hlt">layer</span> depth. The well-mixed <span class="hlt">layer</span> was observed to both warm and cool during the field campaign indicating that advective processes as well as surface fluxes were acting to control the temporal <span class="hlt">evolution</span> of the boundary <span class="hlt">layer</span> temperature. Only a small number of weakly stably stratified boundary <span class="hlt">layers</span> were observed. Strong, shallow inversions, of up to 6 K, were observed above the top of the boundary <span class="hlt">layer</span>. Observations from a 30 m automatic weather station and two temporary automatic weather stations 10 km south and west of the main field campaign location provide additional data for understanding the boundary <span class="hlt">layer</span> <span class="hlt">evolution</span> observed by the SUMO UAVs during this 9-day period. This presentation will discuss the observed <span class="hlt">evolution</span> of the summertime boundary <span class="hlt">layer</span> as well as comment on lessons learned operating the SUMO UAVs at a remote Antarctic field camp.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70036006','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70036006"><span>Approximation to cutoffs of higher modes of Rayleigh waves for a <span class="hlt">layered</span> earth <span class="hlt">model</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>Xu, Y.; Xia, J.; Miller, R.D.</p> <p>2009-01-01</p> <p>A cutoff defines the long-period termination of a Rayleigh-wave higher mode and, therefore is a key characteristic of higher mode energy relationship to several material properties of the subsurface. Cutoffs have been used to estimate the shear-wave velocity of an underlying half space of a <span class="hlt">layered</span> earth <span class="hlt">model</span>. In this study, we describe a method that replaces the multilayer earth <span class="hlt">model</span> with a single surface <span class="hlt">layer</span> overlying the half-space <span class="hlt">model</span>, accomplished by harmonic averaging of velocities and arithmetic averaging of densities. Using numerical comparisons with theoretical <span class="hlt">models</span> validates the single-<span class="hlt">layer</span> approximation. Accuracy of this single-<span class="hlt">layer</span> approximation is best defined by values of the calculated error in the frequency and phase velocity estimate at a cutoff. Our proposed method is intuitively explained using ray theory. Numerical results indicate that a cutoffs frequency is controlled by the averaged elastic properties within the passing depth of Rayleigh waves and the shear-wave velocity of the underlying half space. ?? Birkh??user Verlag, Basel 2009.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/39109','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/39109"><span>Viscous diffusion of vorticity in unsteady wall <span class="hlt">layers</span> using the diffusion velocity concept</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>Strickland, J.H.; Kempka, S.N.; Wolfe, W.P.</p> <p>1995-03-01</p> <p>The primary purpose of this paper is to provide a careful evaluation of the diffusion velocity concept with regard to its ability to predict the diffusion of vorticity near a moving wall. A computer code BDIF has been written which simulates the <span class="hlt">evolution</span> of the vorticity field near a wall of infinite length which is moving in an arbitrary fashion. The simulations generated by this code are found to give excellent results when compared to several exact solutions. We also outline a two-dimensional unsteady viscous boundary <span class="hlt">layer</span> <span class="hlt">model</span> which utilizes the diffusion velocity concept and is compatible with vortex methods.more » A primary goal of this boundary <span class="hlt">layer</span> <span class="hlt">model</span> is to minimize the number of vortices generated on the surface at each time step while achieving good resolution of the vorticity field near the wall. Preliminary results have been obtained for simulating a simple two-dimensional laminar boundary <span class="hlt">layer</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25171457','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25171457"><span>Asymmetric bi-<span class="hlt">layer</span> PFSA membranes as <span class="hlt">model</span> systems for the study of water management in the PEMFC.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Peng, Z; Peng, A Z; Morin, A; Huguet, P; Lanteri, Y; Deabate, S</p> <p>2014-10-14</p> <p>New bi-<span class="hlt">layer</span> PFSA membranes made of Nafion® NRE212 and Aquivion™ E79-05s with different equivalent weights are prepared with the aim of managing water repartition in the PEMFC. The membrane water transport properties, i.e. back-diffusion and electroosmosis, as well as the electrochemical performances, are compared to those of state-of-art materials. The actual water content (the inner water concentration profile across the membrane thickness) is measured under operation in the fuel cell by in situ Raman microspectroscopy. The orientation of the equivalent weight gradient with respect to the water external gradient and to the proton flow direction affects the membrane water content, the water transport ability and, thus, the fuel cell performances. Higher power outputs, related to lower ohmic losses, are observed when the membrane is assembled with the lower equivalent weight <span class="hlt">layer</span> (Aquivion™) at the anode side. This orientation, corresponding to enhanced water transport by back-flow while electroosmosis remains unaffected, results in the higher hydration of the membrane and of the anode active <span class="hlt">layer</span> during operation. Also, polarization data suggest a different water repartition in the fuel cell along the on-plane direction. Even if the interest in multi-<span class="hlt">layer</span> PFSA membranes as perspective electrolytes for PEMFCs is not definitively attested, these materials appear to be excellent <span class="hlt">model</span> systems to establish relationships between the membrane transport properties, the water distribution in the fuel cell and the electrochemical performances. Thanks to the micrometric resolution, in situ Raman microspectroscopy proves to be a unique tool to measure the actual hydration of the membrane at the surface swept by the hydrated feed gases during operation, so that it can be used as a local probe of the water concentration <span class="hlt">evolution</span> along the gas distribution channels according to changing working conditions.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22590802-anomalous-temperature-dependence-layer-spacing-de-vries-liquid-crystals-compensation-model','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22590802-anomalous-temperature-dependence-layer-spacing-de-vries-liquid-crystals-compensation-model"><span>Anomalous temperature dependence of <span class="hlt">layer</span> spacing of de Vries liquid crystals: Compensation <span class="hlt">model</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>Merkel, K.; Kocot, A.; Vij, J. K., E-mail: jvij@tcd.ie</p> <p></p> <p>Smectic liquid crystals that exhibit temperature independent <span class="hlt">layer</span> thickness offer technological advantages for their use in displays and photonic devices. The dependence of the <span class="hlt">layer</span> spacing in SmA and SmC phases of de Vries liquid crystals is found to exhibit distinct features. On entering the SmC phase, the <span class="hlt">layer</span> thickness initially decreases below SmA to SmC (T{sub A–C}) transition temperature but increases anomalously with reducing temperature despite the molecular tilt increasing. This anomalous observation is being explained quantitatively. Results of IR spectroscopy show that <span class="hlt">layer</span> shrinkage is caused by tilt of the mesogen's rigid core, whereas the expansion is causedmore » by the chains getting more ordered with reducing temperature. This mutual compensation arising from molecular fragments contributing to the <span class="hlt">layer</span> thickness differs from the previous <span class="hlt">models</span>. The orientational order parameter of the rigid core of the mesogen provides direct evidence for de Vries cone <span class="hlt">model</span> in the SmA phase for the two compounds investigated.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994JGR....99.2053H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994JGR....99.2053H"><span>Episodic large-scale overturn of two-<span class="hlt">layer</span> mantles in terrestrial planets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Herrick, D. L.; Parmentier, E. M.</p> <p>1994-01-01</p> <p>It is usually assumed that the upper and lower mantles of a chemically stratified planet are arranged so that the upper mantle is chemically less dense and that these <span class="hlt">layers</span> convect separately. Possible buoyant overturn of the two mantle <span class="hlt">layers</span> has not previously been considered. Such overturn would initially occur when thermal expansion of a chemically denser lower mantle more than offsets the compositional density difference between the <span class="hlt">layers</span>, reversing the relative sense of buoyancy. Once overturn has occurred, the chemically denser, but thermally less dense upper mantle cools more efficiently than the lower mantle and loses its relative thermal buoyancy. If mixing is slow, this leads to repeated overturns that result in thermal histories that differ radically from those obtained without this large-scale overturning. Thermal <span class="hlt">evolution</span> calculations, for a two-<span class="hlt">layer</span> mantle over a wide range of parameter space, show that large-scale overturn occurs cyclically with a well-defined period. This period depends most strongly on the viscosity of the lower mantle, to which it is approximately proportional. Geologically interesting overturn periods on the order of 107 to 109 years result for lower mantle viscosities of 1022 to 1024 Pa s for the Earth and Venus, and 1021 to 1023 Pa s for Mars. The mantles of Mercury and the Moon are too thin to permit two-<span class="hlt">layer</span> convection, and therefore the <span class="hlt">model</span> is not appropriate for them. Overturn cannot occur on Earth or Venus if the compositional density difference between the <span class="hlt">layers</span> exceeds about 4%, or on Mars if it exceeds about 2%. Large-scale mantle overturn could have significant tectonic consequences such as the initiation of a new plate tectonic cycle on the Earth or a major resurfacing event on Mars or Venus. Such episodic events in the <span class="hlt">evolution</span> of a planet are not easily explained by whole mantle thermal convection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22380438','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22380438"><span>Fitting <span class="hlt">models</span> of continuous trait <span class="hlt">evolution</span> to incompletely sampled comparative data using approximate Bayesian computation.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Slater, Graham J; Harmon, Luke J; Wegmann, Daniel; Joyce, Paul; Revell, Liam J; Alfaro, Michael E</p> <p>2012-03-01</p> <p>In recent years, a suite of methods has been developed to fit multiple rate <span class="hlt">models</span> to phylogenetic comparative data. However, most methods have limited utility at broad phylogenetic scales because they typically require complete sampling of both the tree and the associated phenotypic data. Here, we develop and implement a new, tree-based method called MECCA (<span class="hlt">Modeling</span> <span class="hlt">Evolution</span> of Continuous Characters using ABC) that uses a hybrid likelihood/approximate Bayesian computation (ABC)-Markov-Chain Monte Carlo approach to simultaneously infer rates of diversification and trait <span class="hlt">evolution</span> from incompletely sampled phylogenies and trait data. We demonstrate via simulation that MECCA has considerable power to choose among single versus multiple evolutionary rate <span class="hlt">models</span>, and thus can be used to test hypotheses about changes in the rate of trait <span class="hlt">evolution</span> across an incomplete tree of life. We finally apply MECCA to an empirical example of body size <span class="hlt">evolution</span> in carnivores, and show that there is no evidence for an elevated rate of body size <span class="hlt">evolution</span> in the pinnipeds relative to terrestrial carnivores. ABC approaches can provide a useful alternative set of tools for future macroevolutionary studies where likelihood-dependent approaches are lacking. © 2011 The Author(s). <span class="hlt">Evolution</span>© 2011 The Society for the Study of <span class="hlt">Evolution</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20050170989','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20050170989"><span>A GCM Recent History of Northern Martian Polar <span class="hlt">Layered</span> Deposits: Contribution from Past Equatorial Ice Reservoirs</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Levrard, B.; Laskar, J.; Montmessin, F.; Forget, F.</p> <p>2005-01-01</p> <p>Polar <span class="hlt">layered</span> deposits are exposed in the walls of the troughs cutting the north polar cap of Mars. They consist of alternating ice and dust <span class="hlt">layers</span> or <span class="hlt">layers</span> of an ice-dust mixture with varying proportions and are found throughout the cap. <span class="hlt">Layers</span> thickness ranges from meters to several tens of meters with an approximately 30 meter dominant wavelength. Although their formation processes is not known, they are presumed to reflect changes in ice and dust stability over orbital and axial variations. Intensive 3-D LMD GCM simulations of the martian water cycle have been thus performed to determine the annual rates of exchange of surface ice between the northern cap and tropical areas for a wide range of obliquity and orbital parameters values.These rates have been employed to reconstruct an history of the northern cap and test simple <span class="hlt">models</span> of dust-ice <span class="hlt">layers</span> formation over the last 10 Ma orbital variations. We use the 3-D water cycle <span class="hlt">model</span> simulated by the 3-D LMD GCM with an intermediate grid resolution (7.5 longitude x 5.625 latitude) and 25 vertical levels. The dust opacity is constant and set to 0,15. No exchange of ice with regolith is allowed. The <span class="hlt">evolution</span> of the northern cap over obliquity and orbital changes (eccentricity, Longitude of perihelion) has been recently described with this <span class="hlt">model</span>. High summer insolation favors transfer of ice from the northern pole to the Tharsis and Olympus Montes, while at low obliquity, unstable equatorial ice is redeposited in high-latitude and polar areas of both hemisphere. The disappearance of the equatorial ice reservoir leads to a poleward recession of icy high latitude reservoirs, providing an additional source for the cap accumulation during each obliquity or orbital cycle. Furthering the efforts, a quantitative <span class="hlt">evolution</span> of ice reservoirs is here investigated for various astronomical conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002ClDy...19..397G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002ClDy...19..397G"><span>The atmospheric boundary <span class="hlt">layer</span> in the CSIRO global climate <span class="hlt">model</span>: simulations versus observations</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.; Rotstayn, L. D.; Krummel, P. B.</p> <p>2002-07-01</p> <p>A 5-year simulation of the atmospheric boundary <span class="hlt">layer</span> in the CSIRO global climate <span class="hlt">model</span> (GCM) is compared with detailed boundary-<span class="hlt">layer</span> observations at six locations, two over the ocean and four over land. Field observations, in the form of surface fluxes and vertical profiles of wind, temperature and humidity, are generally available for each hour over periods of one month or more in a single year. GCM simulations are for specific months corresponding to the field observations, for each of five years. At three of the four land sites (two in Australia, one in south-eastern France), <span class="hlt">modelled</span> rainfall was close to the observed climatological values, but was significantly in deficit at the fourth (Kansas, USA). Observed rainfall during the field expeditions was close to climatology at all four sites. At the Kansas site, <span class="hlt">modelled</span> screen temperatures (Tsc), diurnal temperature amplitude and sensible heat flux (H) were significantly higher than observed, with <span class="hlt">modelled</span> evaporation (E) much lower. At the other three land sites, there is excellent correspondence between the diurnal amplitude and phase and absolute values of each variable (Tsc, H, E). Mean monthly vertical profiles for specific times of the day show strong similarities: over land and ocean in vertical shape and absolute values of variables, and in the mixed-<span class="hlt">layer</span> and nocturnal-inversion depths (over land) and the height of the elevated inversion or height of the cloud <span class="hlt">layer</span> (over the sea). Of special interest is the presence climatologically of early morning humidity inversions related to dewfall and of nocturnal low-level jets; such features are found in the GCM simulations. The observed day-to-day variability in vertical structure is captured well in the <span class="hlt">model</span> for most sites, including, over a whole month, the temperature range at all levels in the boundary <span class="hlt">layer</span>, and the mix of shallow and deep mixed <span class="hlt">layers</span>. Weaknesses or unrealistic structure include the following, (a) unrealistic <span class="hlt">model</span> mixed-<span class="hlt">layer</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNG21A0148P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNG21A0148P"><span><span class="hlt">Modeling</span> the Conducting Stably-Stratified <span class="hlt">Layer</span> of the Earth's Core</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Petitdemange, L.; Philidet, J.; Gissinger, C.</p> <p>2017-12-01</p> <p>Observations of the Earth magnetic field as well as recent theoretical works tend to show that the Earth's outer liquid core is mostly comprised of a convective zone in which the Earth's magnetic field is generated - likely by dynamo action -, but also features a thin, stably stratified <span class="hlt">layer</span> at the top of the core.We carry out direct numerical simulations by <span class="hlt">modeling</span> this thin <span class="hlt">layer</span> as an axisymmetric spherical Couette flow for a stably stratified fluid embedded in a dipolar magnetic field. The dynamo region is <span class="hlt">modeled</span> by a conducting inner core rotating slightly faster than the insulating mantle due to magnetic torques acting on it, such that a weak differential rotation (low Rossby limit) can develop in the stably stratified <span class="hlt">layer</span>.In the case of a non-stratified fluid, the combined action of the differential rotation and the magnetic field leads to the well known regime of `super-rotation', in which the fluid rotates faster than the inner core. Whereas in the classical case, this super-rotation is known to vanish in the magnetostrophic limit, we show here that the fluid stratification significantly extends the magnitude of the super-rotation, keeping this phenomenon relevant for the Earth core. Finally, we study how the shear <span class="hlt">layers</span> generated by this new state might give birth to magnetohydrodynamic instabilities or waves impacting the secular variations or jerks of the Earth's magnetic field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19831072','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19831072"><span>Eco-genetic <span class="hlt">modeling</span> of contemporary life-history <span class="hlt">evolution</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dunlop, Erin S; Heino, Mikko; Dieckmann, Ulf</p> <p>2009-10-01</p> <p>We present eco-genetic <span class="hlt">modeling</span> as a flexible tool for exploring the course and rates of multi-trait life-history <span class="hlt">evolution</span> in natural populations. We build on existing <span class="hlt">modeling</span> approaches by combining features that facilitate studying the ecological and evolutionary dynamics of realistically structured populations. In particular, the joint consideration of age and size structure enables the analysis of phenotypically plastic populations with more than a single growth trajectory, and ecological feedback is readily included in the form of density dependence and frequency dependence. Stochasticity and life-history trade-offs can also be implemented. Critically, eco-genetic <span class="hlt">models</span> permit the incorporation of salient genetic detail such as a population's genetic variances and covariances and the corresponding heritabilities, as well as the probabilistic inheritance and phenotypic expression of quantitative traits. These inclusions are crucial for predicting rates of evolutionary change on both contemporary and longer timescales. An eco-genetic <span class="hlt">model</span> can be tightly coupled with empirical data and therefore may have considerable practical relevance, in terms of generating testable predictions and evaluating alternative management measures. To illustrate the utility of these <span class="hlt">models</span>, we present as an example an eco-genetic <span class="hlt">model</span> used to study harvest-induced <span class="hlt">evolution</span> of multiple traits in Atlantic cod. The predictions of our <span class="hlt">model</span> (most notably that harvesting induces a genetic reduction in age and size at maturation, an increase or decrease in growth capacity depending on the minimum-length limit, and an increase in reproductive investment) are corroborated by patterns observed in wild populations. The predicted genetic changes occur together with plastic changes that could phenotypically mask the former. Importantly, our analysis predicts that evolutionary changes show little signs of reversal following a harvest moratorium. This illustrates how predictions offered by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPSJ...86h4803S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPSJ...86h4803S"><span><span class="hlt">Evolution</span> <span class="hlt">Models</span> with Conditional Mutation Rates: Strange Plateaus in Population Distribution</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Saakian, David B.</p> <p>2017-08-01</p> <p>Cancer is related to clonal <span class="hlt">evolution</span> with a strongly nonlinear, collective behavior. Here we investigate a slightly advanced version of the popular Crow-Kimura <span class="hlt">evolution</span> <span class="hlt">model</span>, suggested recently, by simply assuming a conditional mutation rate. We investigated the steady-state solution and found a highly intriguing plateau in the distribution. There are selective and nonselective phases, with a rather narrow plateau in the distribution at the peak in the first phase, and a wide plateau for many Hamming classes (a collection of genomes with the same number of mutations from the reference genome) in the second phase. We analytically solved the steady state distribution in the selective and nonselective phases, calculating the widths of the plateaus. Numerically, we also found an intermediate phase with several plateaus in the steady-state distribution, related to large finite-genome-length corrections. We assume that the newly observed phenomena should exist in other versions of <span class="hlt">evolution</span> dynamics when the parameters of the <span class="hlt">model</span> are conditioned to the population distribution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.gcags.org/','USGSPUBS'); return false;" href="http://www.gcags.org/"><span><span class="hlt">Modeling</span> the mesozoic-cenozoic structural <span class="hlt">evolution</span> of east texas</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Pearson, Ofori N.; Rowan, Elisabeth L.; Miller, John J.</p> <p>2012-01-01</p> <p>The U.S. Geological Survey (USGS) recently assessed the undiscovered technically recoverable oil and gas resources within Jurassic and Cretaceous strata of the onshore coastal plain and State waters of the U.S. Gulf Coast. Regional 2D seismic lines for key parts of the Gulf Coast basin were interpreted in order to examine the <span class="hlt">evolution</span> of structural traps and the burial history of petroleum source rocks. Interpretation and structural <span class="hlt">modeling</span> of seismic lines from eastern Texas provide insights into the structural <span class="hlt">evolution</span> of this part of the Gulf of Mexico basin. Since completing the assessment, the USGS has acquired additional regional seismic lines in east Texas; interpretation of these new lines, which extend from the Texas-Oklahoma state line to the Gulf Coast shoreline, show how some of the region's prominent structural elements (e.g., the Talco and Mount Enterprise fault zones, the East Texas salt basin, and the Houston diapir province) vary along strike. The interpretations also indicate that unexplored structures may lie beneath the current drilling floor. Structural restorations based upon interpretation of these lines illustrate the <span class="hlt">evolution</span> of key structures and show the genetic relation between structural growth and movement of the Jurassic Louann Salt. 1D thermal <span class="hlt">models</span> that integrate kinetics and burial histories were also created for the region's two primary petroleum source rocks, the Oxfordian Smackover Formation and the Cenomanian-Turonian Eagle Ford Shale. Integrating results from the thermal <span class="hlt">models</span> with the structural restorations provides insights into the distribution and timing of petroleum expulsion from the Smackover Formation and Eagle Ford Shale in eastern Texas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015LatJP..52f..49G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015LatJP..52f..49G"><span>Mathematical <span class="hlt">Modeling</span> of Dual <span class="hlt">Layer</span> Shell Type Recuperation System for Biogas Dehumidification</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gendelis, S.; Timuhins, A.; Laizans, A.; Bandeniece, L.</p> <p>2015-12-01</p> <p>The main aim of the current paper is to create a mathematical <span class="hlt">model</span> for dual <span class="hlt">layer</span> shell type recuperation system, which allows reducing the heat losses from the biomass digester and water amount in the biogas without any additional mechanical or chemical components. The idea of this system is to reduce the temperature of the outflowing gas by creating two-<span class="hlt">layered</span> counter-flow heat exchanger around the walls of biogas digester, thus increasing a thermal resistance and the gas temperature, resulting in a condensation on a colder surface. Complex mathematical <span class="hlt">model</span>, including surface condensation, is developed for this type of biogas dehumidifier and the parameter study is carried out for a wide range of parameters. The <span class="hlt">model</span> is reduced to 1D case to make numerical calculations faster. It is shown that latent heat of condensation is very important for the total heat balance and the condensation rate is highly dependent on insulation between <span class="hlt">layers</span> and outside temperature. <span class="hlt">Modelling</span> results allow finding optimal geometrical parameters for the known gas flow and predicting the condensation rate for different system setups and seasons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015DPS....4731005L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015DPS....4731005L"><span>Microphysical <span class="hlt">Modeling</span> of Titan's Detached Haze <span class="hlt">Layer</span> in a 3D GCM</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Larson, Erik J.; Toon, Owen B.; West, Robert A.; Friedson, A. James</p> <p>2015-11-01</p> <p>We investigate the formation and seasonal cycle of the detached haze <span class="hlt">layer</span> in Titan’s upper atmosphere using a 3D GCM with coupled aerosol microphysics. The base of the detached haze <span class="hlt">layer</span> is defined by a local minimum in the vertical extinction profile. The detached haze is seen at all latitudes including the south pole as seen in Cassini images from 2005-2012. The <span class="hlt">layer</span> merges into the winter polar haze at high latitudes where the Hadley circulation carries the particles downward. The hemisphere in which the haze merges with the polar haze varies with season. We find that the base of the detached haze <span class="hlt">layer</span> occurs where there is a near balance between vertical winds and particle fall velocities. Generally the vertical variation of particle concentration in the detached haze region is simply controlled by sedimentation, so the concentration and the extinction vary roughly in proportion to air density. This variation explains why the upper part of the main haze <span class="hlt">layer</span>, and the bulk of the detached haze <span class="hlt">layer</span> follow exponential profiles. However, the shape of the profile is modified in regions where the vertical wind velocity is comparable to the particle fall velocity. Our simulations closely match the period when the base of the detached <span class="hlt">layer</span> in the tropics is observed to begin its seasonal drop in altitude, and the total range of the altitude drop. However, the simulations have the base of the detached <span class="hlt">layer</span> about 100 km lower than observed, and the time for the base to descend is slower in the simulations than observed. These differences may point to the <span class="hlt">model</span> having somewhat lower vertical winds than occur on Titan, or somewhat too large of particle sizes, or some combination of both. Our <span class="hlt">model</span> is consistent with a dynamical origin for the detached haze rather than a chemical or microphysical one. This balance between the vertical wind and particle fall velocities occurs throughout the summer hemisphere and tropics. The particle concentration gradients that</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPS...372..221D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPS...372..221D"><span>Zinc electrodeposition from flowing alkaline zincate solutions: Role of hydrogen <span class="hlt">evolution</span> reaction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dundálek, Jan; Šnajdr, Ivo; Libánský, Ondřej; Vrána, Jiří; Pocedič, Jaromír; Mazúr, Petr; Kosek, Juraj</p> <p>2017-12-01</p> <p>The hydrogen <span class="hlt">evolution</span> reaction is known as a parasitic reaction during the zinc electrodeposition from alkaline zincate solutions and is thus responsible for current efficiency losses during the electrolysis. Besides that, the rising hydrogen bubbles may cause an extra convection within a diffusion <span class="hlt">layer</span>, which leads to an enhanced mass transport of zincate ions to an electrode surface. In this work, the mentioned phenomena were studied experimentally in a flow through electrolyzer and the obtained data were subsequently evaluated by mathematical <span class="hlt">models</span>. The results prove the indisputable influence of the rising hydrogen bubbles on the additional mixing of the diffusion <span class="hlt">layer</span>, which partially compensates the drop of the current efficiency of the zinc deposition at higher current flows. Moreover, the results show that the current density ratio (i.e., the ratio of an overall current density to a zinc limiting current density) is not suitable for the description of the zinc deposition, because the hydrogen <span class="hlt">evolution</span> current density is always involved in the overall current density.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18244310','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18244310"><span>Ultrasound transducer <span class="hlt">modeling</span>-received voltage signals and the use of half-wavelength window <span class="hlt">layers</span> with acoustic coupling <span class="hlt">layers</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Willatzen, M</p> <p>1999-01-01</p> <p>A general set of <span class="hlt">modeling</span> equations for lossless one-dimensional multilayer ultrasound transducers is presented based on first principles. In particular, a direct relationship between ultrasound transducer results and the underlying physical principles of electroacoustics is given. As such, the <span class="hlt">model</span> may provide better physical understanding for designers not fully versed in electrical circuits theory or in linear system analyses. The <span class="hlt">model</span> is suitable for time-domain analysis and monofrequency design. Special attention is given to the determination of the time-dependent voltage across the receiver electrodes subject to a general voltage input, but information on any (dynamic) variable of interest is provided. The basic equations governing the dynamics of the multilayer structure acting as transmitter as well as receiver are solved by Fourier analysis and by imposing continuity of velocity and pressure between <span class="hlt">layers</span>. Sound transmission between the two piezoelectric circuits is assumed to take place in a water bath such that the Rayleigh equation can be used to obtain the incoming pressure at the receiver aperture from the acceleration of the opposing transmitter aperture. Comparison with experimental results is possible by allowing coupling to external electric impedances. A numerical test case using a multilayered 1-MHz transducer for flow meter applications was considered and good agreement with experiments was obtained in terms of voltage signals. The transducer contains a half-wavelength stainless steel <span class="hlt">layer</span> needed to resist corrosion, the ability to operate at temperatures in a wide range from 20 to 150 degrees Celsius, resistance to impact from flowing particles in the medium, high pressure or vacuum, and pH values up to 10 in some locations. The influence of epoxy glue and grease acoustic coupling <span class="hlt">layers</span>-between the piezoceramics and the stainless steel <span class="hlt">layer</span>-in the range from 1 to 70 mum was examined. It was shown that, for the same <span class="hlt">layer</span> thickness, epoxy</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25562378','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25562378"><span><span class="hlt">Evolution</span> of electronic structure as a function of <span class="hlt">layer</span> thickness in group-VIB transition metal dichalcogenides: emergence of localization prototypes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Lijun; Zunger, Alex</p> <p>2015-02-11</p> <p><span class="hlt">Layered</span> group-VIB transition metal dichalcogenides (with the formula of MX2) are known to show a transition from an indirect band gap in the thick n-monolayer stack (MX2)n to a direct band gap at the n = 1 monolayer limit, thus converting the system into an optically active material suitable for a variety of optoelectronic applications. The origin of this transition has been attributed predominantly to quantum confinement effect at reduced n. Our analysis of the <span class="hlt">evolution</span> of band-edge energies and wave functions as a function of n using ab initio density functional calculations including the long-range dispersion interaction reveals (i) the indirect-to-direct band gap transformation is triggered not only by (kinetic-energy controlled) quantum confinement but also by (potential-energy controlled) band repulsion and localization. On its own, neither of the two effects can explain by itself the energy <span class="hlt">evolution</span> of the band-edge states relevant to the transformation; (ii) when n decreased, there emerge distinct regimes with characteristic localization prototypes of band-edge states deciding the optical response of the system. They are distinguished by the real-space direct/indirect in combination with momentum-space direct/indirect nature of electron and hole states and give rise to distinct types of charge distribution of the photoexcited carriers that control excitonic behaviors; (iii) the various regimes associated with different localization prototypes are predicted to change with modification of cations and anions in the complete MX2 (M = Cr, Mo, W and X = S, Se, Te) series. These results offer new insight into understanding the excitonic properties (e.g., binding energy, lifetime etc.) of multiple <span class="hlt">layered</span> MX2 and their heterostructures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhDT.......272H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhDT.......272H"><span>Large Eddy Simulation of Spatially Developing Turbulent Reacting Shear <span class="hlt">Layers</span> with the One-Dimensional Turbulence <span class="hlt">Model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hoffie, Andreas Frank</p> <p></p> <p>Large eddy simulation (LES) combined with the one-dimensional turbulence (ODT) <span class="hlt">model</span> is used to simulate spatially developing turbulent reacting shear <span class="hlt">layers</span> with high heat release and high Reynolds numbers. The LES-ODT results are compared to results from direct numerical simulations (DNS), for <span class="hlt">model</span> development and validation purposes. The LES-ODT approach is based on LES solutions for momentum and pressure on a coarse grid and solutions for momentum and reactive scalars on a fine, one-dimensional, but three-dimensionally coupled ODT subgrid, which is embedded into the LES computational domain. Although one-dimensional, all three velocity components are transported along the ODT domain. The low-dimensional spatial and temporal resolution of the subgrid scales describe a new <span class="hlt">modeling</span> paradigm, referred to as autonomous microstructure <span class="hlt">evolution</span> (AME) <span class="hlt">models</span>, which resolve the multiscale nature of turbulence down to the Kolmogorv scales. While this new concept aims to mimic the turbulent cascade and to reduce the number of input parameters, AME enables also regime-independent combustion <span class="hlt">modeling</span>, capable to simulate multiphysics problems simultaneously. The LES as well as the one-dimensional transport equations are solved using an incompressible, low Mach number approximation, however the effects of heat release are accounted for through variable density computed by the ideal gas equation of state, based on temperature variations. The computations are carried out on a three-dimensional structured mesh, which is stretched in the transverse direction. While the LES momentum equation is integrated with a third-order Runge-Kutta time-integration, the time integration at the ODT level is accomplished with an explicit Forward-Euler method. Spatial finite-difference schemes of third (LES) and first (ODT) order are utilized and a fully consistent fractional-step method at the LES level is used. Turbulence closure at the LES level is achieved by utilizing the Smagorinsky</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21578316-extremely-metal-poor-stars-hierarchical-chemical-evolution-model','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21578316-extremely-metal-poor-stars-hierarchical-chemical-evolution-model"><span>EXTREMELY METAL-POOR STARS AND A HIERARCHICAL CHEMICAL <span class="hlt">EVOLUTION</span> <span class="hlt">MODEL</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>Komiya, Yutaka</p> <p>2011-07-20</p> <p>Early phases of the chemical <span class="hlt">evolution</span> of the Galaxy and formation history of extremely metal-poor (EMP) stars are investigated using hierarchical galaxy formation <span class="hlt">models</span>. We build a merger tree of the Galaxy according to the extended Press-Schechter theory. We follow the chemical <span class="hlt">evolution</span> along the tree and compare the <span class="hlt">model</span> results to the metallicity distribution function and abundance ratio distribution of the Milky Way halo. We adopt three different initial mass functions (IMFs). In a previous study, we argued that the typical mass, M{sub md}, of EMP stars should be high, M{sub md} {approx} 10 M{sub sun}, based on studiesmore » of binary origin carbon-rich EMP stars. In this study, we show that only the high-mass IMF can explain an observed small number of EMP stars. For relative element abundances, the high-mass IMF and the Salpeter IMF predict similar distributions. We also investigate dependence on nucleosynthetic yields of supernovae (SNe). The theoretical SN yields by Kobayashi et al. and Chieffi and Limongi show reasonable agreement with observations for {alpha}-elements. Our <span class="hlt">model</span> predicts a significant scatter of element abundances at [Fe/H] < -3. We adopted the stellar yields derived in the work of Francois et al., which produce the best agreement between the observational data and the one-zone chemical <span class="hlt">evolution</span> <span class="hlt">model</span>. Their yields well reproduce a trend of the averaged abundances of EMP stars but predict much larger scatter than do the observations. The <span class="hlt">model</span> with hypernovae predicts Zn abundance, in agreement with the observations, but other <span class="hlt">models</span> predict lower [Zn/Fe]. Ejecta from the hypernovae with large explosion energy is mixed in large mass and decreases the scatter of the element abundances.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1990JGR....9516149C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1990JGR....9516149C"><span>Numerical experiments with a wind- and buoyancy-driven two-and-a-half-<span class="hlt">layer</span> upper ocean <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cherniawsky, J. Y.; Yuen, C. W.; Lin, C. A.; Mysak, L. A.</p> <p>1990-09-01</p> <p>We describe numerical experiments with a limited domain (15°-67°N, 65° west to east) coarse-resolution two-and-a-half-<span class="hlt">layer</span> upper ocean <span class="hlt">model</span>. The <span class="hlt">model</span> consists of two active variable density <span class="hlt">layers</span>: a Niiler and Kraus (1977) type mixed <span class="hlt">layer</span> and a pycnocline <span class="hlt">layer</span>, which overlays a semipassive deep ocean. The mixed <span class="hlt">layer</span> is forced with a cosine wind stress and Haney type heat and precipitation-evaporation fluxes, which were derived from zonally averaged climatological (Levitus, 1982) surface temperatures and salinities for the North Atlantic. The second <span class="hlt">layer</span> is forced from below with (1) Newtonian cooling to climatological temperatures and salinities at the lower boundary, (2) convective adjustment, which occurs whenever the density of the second <span class="hlt">layer</span> is unstable with respect to climatology, and (3) mass entrainment in areas of strong upwelling, when the deep ocean ventilates through the bottom surface. The sensitivity of this <span class="hlt">model</span> to changes in its internal (mixed <span class="hlt">layer</span>) and external (e.g., a Newtonian coupling coefficient) parameters is investigated and compared to the results from a control experiment. We find that the <span class="hlt">model</span> is not overly sensitive to changes in most of the parameters that were tested, albeit these results may depend to some extent on the choice of the control experiment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996PhDT........13L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996PhDT........13L"><span>Numerical Investigation of a Heated, Sheared Planetary Boundary <span class="hlt">Layer</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liou, Yu-Chieng</p> <p>1996-01-01</p> <p>A planetary boundary <span class="hlt">layer</span> (PBL) developed on 11 July, 1987 during the First International Satellites Land Surface Climatology Project (ISLSCP) Field Experiment (FIFE) is investigated numerically by a two dimensional and a three dimensional large eddy simulation (LES) <span class="hlt">model</span>. Most of the simulated mean and statistical properties are utilized to compare or verify against the observational results extracted from single Doppler lidar scans conducted by Gal-Chen et al. (1992) on the same day. Through the methods of field measurements and numerical simulations, it is found that this PBL, in contrast to the well-known convective boundary <span class="hlt">layer</span> (CBL), is driven by not only buoyancy but also wind shear. Large eddies produced by the surface heating, as well as internal gravity waves excited by the convection, are both present in the boundary <span class="hlt">layer</span>. The most unique feature is that in the stable <span class="hlt">layer</span>, the momentum flux ({overlinerm u^' w^'}), transported by the gravity waves, is counter-gradient. The occurrence of this phenomenon is interpreted by Gal-Chen et al. (1992) using the theory of critical <span class="hlt">layer</span> singularity, and is confirmed by the numerical simulations in this study. Qualitative agreements are achieved between the <span class="hlt">model</span>-generated and lidar-derived results. However, quantitative comparisons are less satisfactory. The most serious discrepancy is that in the stable <span class="hlt">layer</span> the magnitudes of the observed momentum flux ({overlinerm u^ ' w^'}) and vertical velocity variance ({overlinerm w^'^2}) are much larger than their simulated counterparts. Nevertheless, through the technique of numerical simulation, evidence is collected to show inconsistencies among the observations. Thus, the lidar measurements of {overline rm u^' w^'} and {overlinerm w^ '^2} seem to be doubtful. A Four Dimensional Data Assimilation (FDDA) experiment is performed in order to connect the <span class="hlt">evolution</span> of the <span class="hlt">model</span> integration with the observations. The results indicate that the dynamical relaxation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800015777','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800015777"><span>Simple turbulence <span class="hlt">models</span> and their application to boundary <span class="hlt">layer</span> separation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wadcock, A. J.</p> <p>1980-01-01</p> <p>Measurements in the boundary <span class="hlt">layer</span> and wake of a stalled airfoil are presented in two coordinate systems, one aligned with the airfoil chord, the other being conventional boundary <span class="hlt">layer</span> coordinates. The NACA 4412 airfoil is studied at a single angle of attack corresponding to maximum lift, the Reynolds number based on chord being 1.5 x 10 to the 6th power. Turbulent boundary <span class="hlt">layer</span> separation occurred at the 85 percent chord position. The two-dimensionality of the flow was documented and the momentum integral equation studied to illustrate the importance of turbulence contributions as separation is approached. The assumptions of simple eddy-viscosity and mixing-length turbulence <span class="hlt">models</span> are checked directly against experiment. Curvature effects are found to be important as separation is approached.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAP...123r5305C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123r5305C"><span>Kinetic <span class="hlt">model</span> for thin film stress including the effect of grain growth</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chason, Eric; Engwall, A. M.; Rao, Z.; Nishimura, T.</p> <p>2018-05-01</p> <p>Residual stress during thin film deposition is affected by the <span class="hlt">evolution</span> of the microstructure. This can occur because subsurface grain growth directly induces stress in the film and because changing the grain size at the surface affects the stress in new <span class="hlt">layers</span> as they are deposited. We describe a new <span class="hlt">model</span> for stress <span class="hlt">evolution</span> that includes both of these effects. It is used to explain stress in films that grow with extensive grain growth (referred to as zone II) so that the grain size changes throughout the thickness of the <span class="hlt">layer</span> as the film grows. Equations are derived for different cases of high or low atomic mobility where different assumptions are used to describe the diffusion of atoms that are incorporated into the grain boundary. The <span class="hlt">model</span> is applied to measurements of stress and grain growth in evaporated Ni films. A single set of <span class="hlt">model</span> parameters is able to explain stress <span class="hlt">evolution</span> in films grown at multiple temperatures and growth rates. The <span class="hlt">model</span> explains why the slope of the curvature measurements changes continuously with thickness and attributes it to the effect of grain size on new <span class="hlt">layers</span> deposited on the film.</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. Their policies may differ from this site.</div> </div><!-- container --> <footer><a id="backToTop" href="#top"> </a><nav><a id="backToTop" href="#top"> </a><ul class="links"><a id="backToTop" href="#top"> </a><li><a id="backToTop" href="#top"></a><a href="/sitemap.html">Site Map</a></li> <li><a href="/members/index.html">Members Only</a></li> <li><a href="/website-policies.html">Website Policies</a></li> <li><a href="https://doe.responsibledisclosure.com/hc/en-us" target="_blank">Vulnerability Disclosure Program</a></li> <li><a href="/contact.html">Contact Us</a></li> </ul> <div class="small">Science.gov is maintained by the U.S. Department of Energy's <a href="https://www.osti.gov/" target="_blank">Office of Scientific and Technical Information</a>, in partnership with <a href="https://www.cendi.gov/" target="_blank">CENDI</a>.</div> </nav> </footer> <script type="text/javascript"><!-- // var lastDiv = ""; function showDiv(divName) { // hide last div if (lastDiv) { document.getElementById(lastDiv).className = "hiddenDiv"; } //if value of the box is not nothing and an object with that name exists, then change the class if (divName && document.getElementById(divName)) { document.getElementById(divName).className = "visibleDiv"; lastDiv = divName; } } //--> </script> <script> /** * Function that tracks a click on an outbound link in Google Analytics. * This function takes a valid URL string as an argument, and uses that URL string * as the event label. */ var trackOutboundLink = function(url,collectionCode) { try { h = window.open(url); setTimeout(function() { ga('send', 'event', 'topic-page-click-through', collectionCode, url); }, 1000); } catch(err){} }; </script> <!-- Google Analytics --> <script> (function(i,s,o,g,r,a,m){i['GoogleAnalyticsObject']=r;i[r]=i[r]||function(){ (i[r].q=i[r].q||[]).push(arguments)},i[r].l=1*new Date();a=s.createElement(o), m=s.getElementsByTagName(o)[0];a.async=1;a.src=g;m.parentNode.insertBefore(a,m) })(window,document,'script','//www.google-analytics.com/analytics.js','ga'); ga('create', 'UA-1122789-34', 'auto'); ga('send', 'pageview'); </script> <!-- End Google Analytics --> <script> showDiv('page_1') </script> </body> </html>