Sample records for coupled wave-current model

  1. Simulation of Wave-Current Interaction Using a Three-Dimensional Hydrodynamic Model Coupled With a Phase Averaged Wave Model

    NASA Astrophysics Data System (ADS)

    Marsooli, R.; Orton, P. M.; Georgas, N.; Blumberg, A. F.

    2016-02-01

    The Stevens Institute of Technology Estuarine and Coastal Ocean Model (sECOM) has been coupled with a more advanced surface wave model to simulate wave‒current interaction, and results have been validated in estuarine and nearshore waters. sECOM is a three‒dimensional, hydrostatic, free surface, primitive equation model. It solves the Navier‒Stokes equations and the conservation equations for temperature and salinity using a finite‒difference method on an Arakawa C‒grid with a terrain‒following (sigma) vertical coordinate and orthogonal curvilinear horizontal coordinate system. The model is coupled with the surface wave model developed by Mellor et al. (2008), which solves the spectral equation and takes into account depth and current refraction, and deep and shallow water. The wave model parameterizes the energy distribution in frequency space and the wave‒wave interaction process by using a specified spectrum shape. The coupled wave‒hydrodynamic model considers the wave‒current interaction through wave‒induced bottom stress, depth‒dependent radiation stress, and wave effects on wind‒induced surface stress. The model is validated using the data collected at a natural sandy beach at Duck, North Carolina, during the DUCK94 experiment. This test case reveals the capability of the model to simulate the wave‒current interaction in nearshore coastal systems. The model is further validated using the data collected in Jamaica Bay, a semi‒enclosed body of water located in New York City region. This test reveals the applicability of the model to estuarine systems. These validations of the model and comparisons to its prior wave model, the Great Lakes Environmental Research Laboratory (GLERL) wave model (Donelan 1977), are presented and discussed. ReferencesG.L. Mellor, M.A. Donelan, and L‒Y. Oey, 2008, A Surface Wave Model for Coupling with Numerical Ocean Circulation Models. J. Atmos. Oceanic Technol., 25, 1785‒1807.Donelan, M. A 1977. A

  2. Ring Current Ion Coupling with Electromagnetic Ion Cyclotron Waves

    NASA Technical Reports Server (NTRS)

    Khazanov. G. V.; Gamayunov, K. V.; Jordanova, V. K.; Six, N. Frank (Technical Monitor)

    2002-01-01

    A new ring current global model has been developed that couples the system of two kinetic equations: one equation describes the ring current (RC) ion dynamic, and another equation describes wave evolution of electromagnetic ion cyclotron waves (EMIC). The coupled model is able to simulate, for the first time self-consistently calculated RC ion kinetic and evolution of EMIC waves that propagate along geomagnetic field lines and reflect from the ionosphere. Ionospheric properties affect the reflection index through the integral Pedersen and Hall conductivities. The structure and dynamics of the ring current proton precipitating flux regions, intensities of EMIC global RC energy balance, and some other parameters will be studied in detail for the selected geomagnetic storms.

  3. Ring Current Ion Coupling with Electromagnetic Ion Cyclotron Waves

    NASA Technical Reports Server (NTRS)

    Khazanov, George V.

    2002-01-01

    A new ring current global model has been developed for the first time that couples the system of two kinetic equations: one equation describes the ring current (RC) ion dynamic, and another equation describes wave evolution of electromagnetic ion cyclotron waves (EMIC). The coupled model is able to simulate, for the first time self-consistently calculated RC ion kinetic and evolution of EMIC waves that propagate along geomagnetic field lines and reflect from the ionosphere. Ionospheric properties affect the reflection index through the integral Pedersen and Hall coductivities. The structure and dynamics of the ring current proton precipitating flux regions, intensities of EMIC, global RC energy balance, and some other parameters will be studied in detail for the selected geomagnetic storms. The space whether aspects of RC modelling and comparison with the data will also be discussed.

  4. Mediterranea Forecasting System: a focus on wave-current coupling

    NASA Astrophysics Data System (ADS)

    Clementi, Emanuela; Delrosso, Damiano; Pistoia, Jenny; Drudi, Massimiliano; Fratianni, Claudia; Grandi, Alessandro; Pinardi, Nadia; Oddo, Paolo; Tonani, Marina

    2016-04-01

    The Mediterranean Forecasting System (MFS) is a numerical ocean prediction system that produces analyses, reanalyses and short term forecasts for the entire Mediterranean Sea and its Atlantic Ocean adjacent areas. MFS became operational in the late 90's and has been developed and continuously improved in the framework of a series of EU and National funded programs and is now part of the Copernicus Marine Service. The MFS is composed by the hydrodynamic model NEMO (Nucleus for European Modelling of the Ocean) 2-way coupled with the third generation wave model WW3 (WaveWatchIII) implemented in the Mediterranean Sea with 1/16 horizontal resolution and forced by ECMWF atmospheric fields. The model solutions are corrected by the data assimilation system (3D variational scheme adapted to the oceanic assimilation problem) with a daily assimilation cycle, using a background error correlation matrix varying seasonally and in different sub-regions of the Mediterranean Sea. The focus of this work is to present the latest modelling system upgrades and the related achieved improvements. In order to evaluate the performance of the coupled system a set of experiments has been built by coupling the wave and circulation models that hourly exchange the following fields: the sea surface currents and air-sea temperature difference are transferred from NEMO model to WW3 model modifying respectively the mean momentum transfer of waves and the wind speed stability parameter; while the neutral drag coefficient computed by WW3 model is passed to NEMO that computes the turbulent component. In order to validate the modelling system, numerical results have been compared with in-situ and remote sensing data. This work suggests that a coupled model might be capable of a better description of wave-current interactions, in particular feedback from the ocean to the waves might assess an improvement on the prediction capability of wave characteristics, while suggests to proceed toward a fully

  5. Assessment of the importance of the current-wave coupling in the shelf ocean forecasts

    NASA Astrophysics Data System (ADS)

    Jordà, G.; Bolaños, R.; Espino, M.; Sánchez-Arcilla, A.

    2006-10-01

    The effects of wave-current interactions on shelf ocean forecasts is investigated in the framework of the MFSTEP (Mediterranean Forecasting System Project Towards Enviromental Predictions) project. A one way sequential coupling approach is adopted to link the wave model (WAM) to the circulation model (SYMPHONIE). The coupling of waves and currents has been done considering four main processes: wave refraction due to currents, surface wind drag and bo€ttom drag modifications due to waves, and the wave induced mass flux. The coupled modelling system is implemented in the southern Catalan shelf (NW Mediterranean), a region with characteristics similar to most of the Mediterranean shelves. The sensitivity experiments are run in a typical operational configuration. The wave refraction by currents seems to be not very relevant in a microtidal context such as the western Mediterranean. The main effect of waves on current forecasts is through the modification of the wind drag. The Stokes drift also plays a significant role due to its spatial and temporal characteristics. Finally, the enhanced bottom friction is just noticeable in the inner shelf.

  6. Development of a three-dimensional, regional, coupled wave, current, and sediment-transport model

    USGS Publications Warehouse

    Warner, J.C.; Sherwood, C.R.; Signell, R.P.; Harris, C.K.; Arango, H.G.

    2008-01-01

    We are developing a three-dimensional numerical model that implements algorithms for sediment transport and evolution of bottom morphology in the coastal-circulation model Regional Ocean Modeling System (ROMS v3.0), and provides a two-way link between ROMS and the wave model Simulating Waves in the Nearshore (SWAN) via the Model-Coupling Toolkit. The coupled model is applicable for fluvial, estuarine, shelf, and nearshore (surfzone) environments. Three-dimensional radiation-stress terms have been included in the momentum equations, along with effects of a surface wave roller model. The sediment-transport algorithms are implemented for an unlimited number of user-defined non-cohesive sediment classes. Each class has attributes of grain diameter, density, settling velocity, critical stress threshold for erosion, and erodibility constant. Suspended-sediment transport in the water column is computed with the same advection-diffusion algorithm used for all passive tracers and an additional algorithm for vertical settling that is not limited by the CFL criterion. Erosion and deposition are based on flux formulations. A multi-level bed framework tracks the distribution of every size class in each layer and stores bulk properties including layer thickness, porosity, and mass, allowing computation of bed morphology and stratigraphy. Also tracked are bed-surface properties including active-layer thickness, ripple geometry, and bed roughness. Bedload transport is calculated for mobile sediment classes in the top layer. Bottom-boundary layer submodels parameterize wave-current interactions that enhance bottom stresses and thereby facilitate sediment transport and increase bottom drag, creating a feedback to the circulation. The model is demonstrated in a series of simple test cases and a realistic application in Massachusetts Bay. 

  7. Ring Current-Electromagnetic Ion Cyclotron Waves Coupling

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.

    2005-01-01

    The effect of Electromagnetic Ion Cyclotron (EMIC) waves, generated by ion temperature anisotropy in Earth s ring current (RC), is the best known example of wave- particle interaction in the magnetosphere. Also, there is much controversy over the importance of EMIC waves on RC depletion. Under certain conditions, relativistic electrons, with energies 21 MeV, can be removed from the outer radiation belt (RB) by EMIC wave scattering during a magnetic storm. That is why the calculation of EMIC waves must be a very critical part of the space weather studies. The new RC model that we have developed and present for the first time has several new features that we have combine together in a one single model: (a) several lower frequency cold plasma wave modes are taken into account; (b) wave tracing of these wave has been incorporated in the energy EMIC wave equation; (c) no assumptions regarding wave shape spectra have been made; (d) no assumptions regarding the shape of particle distribution have been made to calculate the growth rate; (e) pitch-angle, energy, and mix diffusions are taken into account together for the first time; (f) the exact loss-cone RC analytical solution has been found and coupled with bounce-averaged numerical solution of kinetic equation; (g) the EMIC waves saturation due to their modulation instability and LHW generation are included as an additional factor that contributes to this process; and (h) the hot ions were included in the real part of dielectric permittivity tensor. We compare our theoretical results with the different EMIC waves models as well as RC experimental data.

  8. Development of a coupled wave-flow-vegetation interaction model

    USGS Publications Warehouse

    Beudin, Alexis; Kalra, Tarandeep S.; Ganju, Neil K.; Warner, John C.

    2017-01-01

    Emergent and submerged vegetation can significantly affect coastal hydrodynamics. However, most deterministic numerical models do not take into account their influence on currents, waves, and turbulence. In this paper, we describe the implementation of a wave-flow-vegetation module into a Coupled-Ocean-Atmosphere-Wave-Sediment Transport (COAWST) modeling system that includes a flow model (ROMS) and a wave model (SWAN), and illustrate various interacting processes using an idealized shallow basin application. The flow model has been modified to include plant posture-dependent three-dimensional drag, in-canopy wave-induced streaming, and production of turbulent kinetic energy and enstrophy to parameterize vertical mixing. The coupling framework has been updated to exchange vegetation-related variables between the flow model and the wave model to account for wave energy dissipation due to vegetation. This study i) demonstrates the validity of the plant posture-dependent drag parameterization against field measurements, ii) shows that the model is capable of reproducing the mean and turbulent flow field in the presence of vegetation as compared to various laboratory experiments, iii) provides insight into the flow-vegetation interaction through an analysis of the terms in the momentum balance, iv) describes the influence of a submerged vegetation patch on tidal currents and waves separately and combined, and v) proposes future directions for research and development.

  9. Models for Convectively Coupled Tropical Waves

    NASA Astrophysics Data System (ADS)

    Majda, A. J.

    2001-05-01

    \\small{The tropical Western Pacific is a key area with large input on short-term climate. There are many recent observations of convective complexes feeding into equatorially trapped planetary waves [5], [6] which need a theoretical explanation and also are poorly treated in contemporary General Circulation Models (GCM's). This area presents wonderful new research opportunities for applied mathematicians interested in nonlinear waves interacting over many spatio-temporal scales. This talk describes some ongoing recent activities of the speaker related to these important issues. A simplified intermediate model for analyzing and parametrizing convectively coupled tropical waves is introduced in [2]. This model has two baroclinic modes of vertical structure, a direct heating mode and a stratiform mode. The key essential parameter in these models is the area fraction occupied by deep convection, σ c. The unstable convectively coupled waves that emerge from perturbation of a radiative convective equilibrium are discussed in detail through linearized stability analysis. Without any mean flow, for an overall cooling rate of 1 K/day as the area fraction parameter increases from σ c=0.001 to σ c=0.0014 the waves pass from a regime with stable moist convective damping (MCD) to a regime of ``stratiform'' instability with convectively coupled waves propagating at speeds of roughly 15~m~s-1,instabilities for a band wavelengths in the super-cluster regime, O(1000) to O(2000) km, and a vertical structure in the upper troposphere lags behind that in the lower troposphere - thus, these convectively coupled waves in the model reproduce several key features of convectively coupled waves in the troposphere processed from recent observational data by Wheeler and Kiladis ([5], [6]). As the parameter σ c is increased further to values such as σ c=0.01, the band of unstable waves increase and spreads toward mesoscale wavelengths of O(100) km while the same wave structure and

  10. Parallel Computation of Ocean-Atmosphere-Wave Coupled Storm Surge Model

    NASA Astrophysics Data System (ADS)

    Kim, K.; Yamashita, T.

    2003-12-01

    Ocean-atmosphere interactions are very important in the formation and development of tropical storms. These interactions are dominant in exchanging heat, momentum, and moisture fluxes. Heat flux is usually computed using a bulk equation. In this equation air-sea interface supplies heat energy to the atmosphere and to the storm. Dynamical interaction is most often one way in which it is the atmosphere that drives the ocean. The winds transfer momentum to both ocean surface waves and ocean current. The wind wave makes an important role in the exchange of the quantities of motion, heat and a substance between the atmosphere and the ocean. Storm surges can be considered as the phenomena of mean sea-level changes, which are the result of the frictional stresses of strong winds blowing toward the land and causing the set level and the low atmospheric pressure at the centre of the cyclone can additionally raise the sea level. In addition to the rise in water level itself, another wave factor must be considered. A rise of mean sea level due to white-cap wave dissipation should be considered. In bounded bodies of water, such as small seas, wind driven sea level set up is much serious than inverted barometer effects, in which the effects of wind waves on wind-driven current play an important role. It is necessary to develop the coupled system of the full spectral third-generation wind-wave model (WAM or WAVEWATCH III), the meso-scale atmosphere model (MM5) and the coastal ocean model (POM) for simulating these physical interactions. As the component of coupled system is so heavy for personal usage, the parallel computing system should be developed. In this study, first, we developed the coupling system of the atmosphere model, ocean wave model and the coastal ocean model, in the Beowulf System, for the simulation of the storm surge. It was applied to the storm surge simulation caused by Typhoon Bart (T9918) in the Yatsushiro Sea. The atmosphere model and the ocean model have

  11. An operational coupled wave-current forecasting system for the northern Adriatic Sea

    NASA Astrophysics Data System (ADS)

    Russo, A.; Coluccelli, A.; Deserti, M.; Valentini, A.; Benetazzo, A.; Carniel, S.

    2012-04-01

    Since 2005 an Adriatic implementation of the Regional Ocean Modeling System (AdriaROMS) is being producing operational short-term forecasts (72 hours) of some hydrodynamic properties (currents, sea level, temperature, salinity) of the Adriatic Sea at 2 km horizontal resolution and 20 vertical s-levels, on a daily basis. The main objective of AdriaROMS, which is managed by the Hydro-Meteo-Clima Service (SIMC) of ARPA Emilia Romagna, is to provide useful products for civil protection purposes (sea level forecasts, outputs to run other forecasting models as for saline wedge, oil spills and coastal erosion). In order to improve the forecasts in the coastal area, where most of the attention is focused, a higher resolution model (0.5 km, again with 20 vertical s-levels) has been implemented for the northern Adriatic domain. The new implementation is based on the Coupled-Ocean-Atmosphere-Wave-Sediment Transport Modeling System (COAWST)and adopts ROMS for the hydrodynamic and Simulating WAve Nearshore (SWAN) for the wave module, respectively. Air-sea fluxes are computed using forecasts produced by the COSMO-I7 operational atmospheric model. At the open boundary of the high resolution model, temperature, salinity and velocity fields are provided by AdriaROMS while the wave characteristics are provided by an operational SWAN implementation (also managed by SIMC). Main tidal components are imposed as well, derived from a tidal model. Work in progress is oriented now on the validation of model results by means of extensive comparisons with acquired hydrographic measurements (such as CTDs or XBTs from sea-truth campaigns), currents and waves acquired at observational sites (including those of SIMC, CNR-ISMAR network and its oceanographic tower, located off the Venice littoral) and satellite-derived wave-heights data. Preliminary results on the forecast waves denote how, especially during intense storms, the effect of coupling can lead to significant variations in the wave

  12. Non-Hydrostatic Modelling of Waves and Currents over Subtle Bathymetric Features

    NASA Astrophysics Data System (ADS)

    Gomes, E.; Mulligan, R. P.; McNinch, J.

    2014-12-01

    Localized areas with high rates of shoreline erosion on beaches, referred to as erosional hotspots, can occur near clusters of relict shore-oblique sandbars. Wave transformation and wave-driven currents over these morphological features could provide an understanding of the hydrodynamic-morphologic coupling mechanism that connects them to the occurrence of erosional hotspots. To investigate this, we use the non-hydrostatic SWASH model that phase-resolves the free surface and fluid motions throughout the water column, allowing for high resolution of wave propagation and breaking processes. In this study we apply a coupled system of nested models including SWAN over a large domain of the North Carolina shelf with smaller nested SWASH domains in areas of interest to determine the hydrodynamic processes occurring over shore oblique bars. In this presentation we focus on a high resolution grid (10 vertical layers, 10 m horizontal resolution) applied to the Duck region with model validation from acoustic wave and current data, and observations from the Coastal Lidar And Radar Imaging System (CLARIS). By altering the bathymetry input for each model run based on bathymetric surveys and comparing the predicted and observed wave heights and current profiles, the effects of subtle bathymetric perturbations have on wave refraction, wave breaking, surf zone currents and vorticity are investigated. The ability to predict wave breaking and hydrodynamics with a non-hydrostatic model may improve our understanding of surf zone dynamics in relation to morphologic conditions.

  13. On the dynamics of the Mouth of the Columbia River: Results from a three-dimensional fully coupled wave-current interaction model

    NASA Astrophysics Data System (ADS)

    Akan, Çiǧdem; Moghimi, Saeed; Özkan-Haller, H. Tuba; Osborne, John; Kurapov, Alexander

    2017-07-01

    Numerical simulations were performed using a 3-D ocean circulation model (ROMS) two-way coupled to a phase-averaged wave propagation model (SWAN), to expand our understanding of the dynamics of wave-current interactions at the Mouth of the Columbia River (MCR). First, model results are compared with water elevations, currents, temperature, salinity, and wave measurements obtained by the U.S. Army Corp of Engineers during the Mega-Transect Experiment in 2005. We then discuss the effects of the currents on the waves and vice versa. Results show that wave heights are intensified notably at the entrance of the mouth in the presence of the tidal currents, especially in ebb flows. We also find nonlocal modifications to the wave field because of wave focusing processes that redirect wave energy toward the inlet mouth from adjacent areas, resulting in the presence of a tidal signatures in areas where local currents are weak. The model also suggests significant wave amplification at the edge of the expanding plume in the later stages of ebb, some tens of kilometers offshore of the inlet mouth, with potential implications for navigation safety. The effect of waves on the location of the plume is also analyzed, and results suggest that the plume is shifted in the down-wave direction when wave effects are considered, and that this shift is more pronounced for larger waves, and consistent with the presence of alongshore advection terms in the salt advection equation, which are related to the Stokes velocities associated with waves.

  14. A coupling modulation model of capillary waves from gravity waves: Theoretical analysis and experimental validation

    NASA Astrophysics Data System (ADS)

    Chen, Pengzhen; Wang, Xiaoqing; Liu, Li; Chong, Jinsong

    2016-06-01

    According to Bragg theory, capillary waves are the predominant scatterers of high-frequency band (such as Ka-band) microwave radiation from the surface of the ocean. Therefore, understanding the modulation mechanism of capillary waves is an important foundation for interpreting high-frequency microwave remote sensing images of the surface of the sea. In our experiments, we discovered that modulations of capillary waves are significantly larger than the values predicted by the classical theory. Further, analysis shows that the difference in restoring force results in an inflection point while the phase velocity changes from gravity waves region to capillary waves region, and this results in the capillary waves being able to resonate with gravity waves when the phase velocity of the gravity waves is equal to the group velocity of the capillary waves. Consequently, we propose a coupling modulation model in which the current modulates the capillary wave indirectly by modulating the resonant gravity waves, and the modulation of the former is approximated by that of the latter. This model very effectively explains the results discovered in our experiments. Further, based on Bragg scattering theory and this coupling modulation model, we simulate the modulation of normalized radar cross section (NRCS) of typical internal waves and show that the high-frequency bands are superior to the low-frequency bands because of their greater modulation of NRCS and better radiometric resolution. This result provides new support for choice of radar band for observation of wave-current modulation oceanic phenomena such as internal waves, fronts, and shears.

  15. Electromagnetic backscattering from one-dimensional drifting fractal sea surface I: Wave-current coupled model

    NASA Astrophysics Data System (ADS)

    Tao, Xie; Shang-Zhuo, Zhao; William, Perrie; He, Fang; Wen-Jin, Yu; Yi-Jun, He

    2016-06-01

    To study the electromagnetic backscattering from a one-dimensional drifting fractal sea surface, a fractal sea surface wave-current model is derived, based on the mechanism of wave-current interactions. The numerical results show the effect of the ocean current on the wave. Wave amplitude decreases, wavelength and kurtosis of wave height increase, spectrum intensity decreases and shifts towards lower frequencies when the current occurs parallel to the direction of the ocean wave. By comparison, wave amplitude increases, wavelength and kurtosis of wave height decrease, spectrum intensity increases and shifts towards higher frequencies if the current is in the opposite direction to the direction of ocean wave. The wave-current interaction effect of the ocean current is much stronger than that of the nonlinear wave-wave interaction. The kurtosis of the nonlinear fractal ocean surface is larger than that of linear fractal ocean surface. The effect of the current on skewness of the probability distribution function is negligible. Therefore, the ocean wave spectrum is notably changed by the surface current and the change should be detectable in the electromagnetic backscattering signal. Project supported by the National Natural Science Foundation of China (Grant No. 41276187), the Global Change Research Program of China (Grant No. 2015CB953901), the Priority Academic Development Program of Jiangsu Higher Education Institutions (PAPD), Program for the Innovation Research and Entrepreneurship Team in Jiangsu Province, China, the Canadian Program on Energy Research and Development, and the Canadian World Class Tanker Safety Service.

  16. Helicon wave coupling in KSTAR plasmas for off-axis current drive in high electron pressure plasmas

    NASA Astrophysics Data System (ADS)

    Wang, S. J.; Wi, H. H.; Kim, H. J.; Kim, J.; Jeong, J. H.; Kwak, J. G.

    2017-04-01

    A helicon wave current drive is proposed as an efficient off-axis current drive in the high electron β plasmas that are expected in fusion reactors. A high frequency helicon wave coupling was analyzed using the surface impedance at a plasma boundary. A slow wave coupling, which may compete with the helicon wave coupling at a frequency of 500 MHz, is estimated to be lower than the fast wave coupling by an order of magnitude in the KSTAR edge plasma density and in practical Faraday shield misalignment with the magnetic pitch. A traveling wave antenna, which is a two port combline antenna, was analyzed using a simplified lumped element model. The results show that the traveling wave antenna provides load resiliency because of its insensitivity to loading resistance, provided that the loading resistance at a radiating element is limited within a practical range. The combline antenna is attractive because it does not require a matching system and exhibits a high selectivity of parallel refractive index. Based on the analysis, a seven element combline antenna was fabricated and installed at an off-mid-plane offset of 30 cm from the mid-plane in KSTAR. The low power RF characteristics measured during several plasma discharges showed no evidence of slow wave coupling. This is consistent with the expectation made through the surface impedance analysis which predicted low slow wave coupling. The wave coupling to the plasma is easily controlled by a radial outer-gap control and gas puffing. No plasma confinement degradation was observed during the radial outer-gap control of up to 3 cm in H-mode discharges. In a ELMy plasmas, only a small reflection peak was observed during a very short portion of the ELM bursting period. If the number of radiating elements is increased for high power operation, then complete load resiliency can be expected. A very large coupling can be problematic for maintaining a parallel refractive index, although this issue can be mitigated by

  17. Application of a wind-wave-current coupled model in the Catalan coast (NW Mediterranean sea), for wind energy purposes

    NASA Astrophysics Data System (ADS)

    María Palomares, Ana; Navarro, Jorge; Grifoll, Manel; Pallares, Elena; Espino, Manuel

    2016-04-01

    This work shows the main results of the HAREAMAR project (including HAREMAR, ENE2012-38772-C02-01 and DARDO, ENE2012-38772-C02-02 projects), concerning the local Wind, Wave and Current simulation at St. Jordi Bay (NW Mediterranean Sea). Offshore Wind Energy has become one of the main topics within the research in Wind Energy research. Although there are quite a few models with a high level of reliability for wind simulation and prediction in onshore places, the wind prediction needs further investigations for adaptation to the Offshore emplacements, taking into account the interaction atmosphere-ocean. The main problem in these ocean areas is the lack of wind data, which neither allows for characterizing the energy potential and wind behaviour in a particular place, nor validating the forecasting models. The main objective of this work is to reduce the local prediction errors, in order to make the meteo-oceanographic hindcast and forecast more reliable. The COAWST model (Coupled-Ocean-Atmosphere-Wave Sediment Transport Model; Warner et al., 2010) system has been implemented in the region considering a set of downscaling nested meshes to obtain high-resolution outputs in the region. The adaptation to this particular area, combining the different wind, wave and ocean model domains has been far from simple, because the grid domains for the three models differ significantly. This work shows the main results of the COAWST model implementation to this particular area, including both monthly and other set of tests in different atmospheric situations, especially chosen for their particular interest. The time period considered for the validation is the whole year 2012. A comparative study between the WRF, SWAN and ROMS model outputs (without coupling), the COWAST model outputs, and a buoy measurements moored in the region was performed for this year. References Warner, J.C., Armstrong, B., He, R., and Zambon, J.B., 2010, Development of a Coupled Ocean-Atmosphere-Wave

  18. Development and applications of a Coupled-Ocean-Atmosphere-Wave-Sediment Transport (COAWST) Modeling System

    NASA Astrophysics Data System (ADS)

    Warner, J. C.; Armstrong, B. N.; He, R.; Zambon, J. B.; Olabarrieta, M.; Voulgaris, G.; Kumar, N.; Haas, K. A.

    2012-12-01

    Understanding processes responsible for coastal change is important for managing both our natural and economic coastal resources. Coastal processes respond from both local scale and larger regional scale forcings. Understanding these processes can lead to significant insight into how the coastal zone evolves. Storms are one of the primary driving forces causing coastal change from a coupling of wave and wind driven flows. Here we utilize a numerical modeling approach to investigate these dynamics of coastal storm impacts. We use the Coupled Ocean - Atmosphere - Wave - Sediment Transport (COAWST) Modeling System that utilizes the Model Coupling Toolkit to exchange prognostic variables between the ocean model ROMS, atmosphere model WRF, wave model SWAN, and the Community Sediment Transport Modeling System (CSTMS) sediment routines. The models exchange fields of sea-surface temperature, ocean currents, water levels, bathymetry, wave heights, lengths, periods, bottom orbital velocities, and atmospheric surface heat and momentum fluxes, atmospheric pressure, precipitation, and evaporation. Data fields are exchanged using regridded flux conservative sparse matrix interpolation weights computed from the SCRIP spherical coordinate remapping interpolation package. We describe the modeling components and the model field exchange methods. As part of the system, the wave and ocean models run with cascading, refined, spatial grids to provide increased resolution, scaling down to resolve nearshore wave driven flows simulated by the vortex force formulation, all within selected regions of a larger, coarser-scale coastal modeling system. The ocean and wave models are driven by the atmospheric component, which is affected by wave dependent ocean-surface roughness and sea surface temperature which modify the heat and momentum fluxes at the ocean-atmosphere interface. We describe the application of the modeling system to several regions of multi-scale complexity to identify the

  19. Wave-current interaction: Effect on the wave field in a semi-enclosed basin

    NASA Astrophysics Data System (ADS)

    Benetazzo, A.; Carniel, S.; Sclavo, M.; Bergamasco, A.

    2013-10-01

    The effect on waves of the Wave-Current Interaction (WCI) process in the semi-enclosed Gulf of Venice (northern region of the Adriatic Sea) was investigated using the Coupled Ocean-Atmosphere-Wave-Sediment Transport (COAWST) modeling system. COAWST relies on the ocean model ROMS (Regional Ocean Modeling System), the wave model SWAN (Simulating WAves Nearshore), and the CSTMS (Community Sediment Transport Modeling System) routines. The two-way data transfer between circulation and wave models was synchronous via MCT (Model Coupling Toolkit), with ROMS providing: current field, free surface elevation, and bathymetry to SWAN. For coupling, the 3-D current profiles were averaged using a formulation which integrated the near-surface velocity over a depth controlled by the spectral mean wavenumber. COAWST system was implemented on a parent grid (with horizontal resolution of 2.0 km) covering the whole Adriatic Sea with one-way nesting to a child grid resolving the northern area (Gulf of Venice) at a resolution of 0.5 km. The meteorological forcings provided by the operational meteorological model COSMO-I7 (a mesoscale model developed in the framework of the COSMO Consortium) were used to drive the modeling system in the period bracketing September 2010-August 2011. The adopted winds and the simulated waves were compared with observations at the CNR-ISMAR Acqua Alta oceanographic tower, located off the Venice littoral. Wave heights and sea surface winds were also compared with satellite-derived data. The analysis of WCI was performed on the child grid over the winter season (January-March 2011) with particular focus on the waves generated by prevailing and dominant winds blowing on the Adriatic Sea: Bora and Sirocco. Due to the variable wind direction with respect to the ocean current direction different effects on WCI were depicted, showing that within the northern Adriatic Sea the ocean-wave interactions are strongly dependent on the wind forcing direction. Further

  20. Current-induced dissipation in spectral wave models

    NASA Astrophysics Data System (ADS)

    Rapizo, H.; Babanin, A. V.; Provis, D.; Rogers, W. E.

    2017-03-01

    Despite many recent developments of the parameterization for wave dissipation in spectral models, it is evident that when waves propagate onto strong adverse currents the rate of energy dissipation is not properly estimated. The issue of current-induced dissipation is studied through a comprehensive data set in the tidal inlet of Port Phillip Heads, Australia. The wave parameters analyzed are significantly modulated by the tidal currents. Wave height in conditions of opposing currents (ebb tide) can reach twice the offshore value, whereas during coflowing currents (flood), it can be reduced to half. The wind-wave model SWAN is able to reproduce the tide-induced modulation of waves and the results show that the variation of currents is the dominant factor in modifying the wave field. In stationary simulations, the model provides an accurate representation of wave height for slack and flood tides. During ebb tides, wave energy is highly overestimated over the opposing current jet. None of the four parameterizations for wave dissipation tested performs satisfactorily. A modification to enhance dissipation as a function of the local currents is proposed. It consists of the addition of a factor that represents current-induced wave steepening and it is scaled by the ratio of spectral energy to the threshold breaking level. The new term asymptotes to the original form as the current in the wave direction tends to zero. The proposed modification considerably improves wave height and mean period in conditions of adverse currents, whereas the good model performance in coflowing currents is unaltered.

  1. Air-Sea Momentum and Enthalpy Exchange in Coupled Atmosphere-Wave-Ocean Modeling of Tropical Cyclones

    NASA Astrophysics Data System (ADS)

    Curcic, M.; Chen, S. S.

    2016-02-01

    The atmosphere and ocean are coupled through momentum, enthalpy, and mass fluxes. Accurate representation of these fluxes in a wide range of weather and climate conditions is one of major challenges in prediction models. Their current parameterizations are based on sparse observations in low-to-moderate winds and are not suited for high wind conditions such as tropical cyclones (TCs) and winter storms. In this study, we use the Unified Wave INterface - Coupled Model (UWIN-CM), a high resolution, fully-coupled atmosphere-wave-ocean model, to better understand the role of ocean surface waves in mediating air-sea momentum and enthalpy exchange in TCs. In particular, we focus on the explicit treatment of wave growth and dissipation for calculating atmospheric and oceanic stress, and its role in upper ocean mixing and surface cooling in the wake of the storm. Wind-wave misalignment and local wave disequilibrium result in difference between atmospheric and oceanic stress being largest on the left side of the storm. We find that explicit wave calculation in the coupled model reduces momentum transfer into the ocean by more than 10% on average, resulting in reduced cooling in TC's wake and subsequent weakening of the storm. We also investigate the impacts of sea surface temperature and upper ocean parameterization on air-sea enthalpy fluxes in the fully coupled model. High-resolution UWIN-CM simulations of TCs with various intensities and structure are conducted in this study to better understand the complex TC-ocean interaction and improve the representation of air-sea coupling processes in coupled prediction models.

  2. Atmosphere-Wave-Ocean Coupling from Regional to Global Earth System Models for High-Impact Extreme Weather Prediction

    NASA Astrophysics Data System (ADS)

    Chen, S. S.; Curcic, M.

    2017-12-01

    The need for acurrate and integrated impact forecasts of extreme wind, rain, waves, and storm surge is growing as coastal population and built environment expand worldwide. A key limiting factor in forecasting impacts of extreme weather events associated with tropical cycle and winter storms is fully coupled atmosphere-wave-ocean model interface with explicit momentum and energy exchange. It is not only critical for accurate prediction of storm intensity, but also provides coherent wind, rian, ocean waves and currents forecasts for forcing for storm surge. The Unified Wave INterface (UWIN) has been developed for coupling of the atmosphere-wave-ocean models. UWIN couples the atmosphere, wave, and ocean models using the Earth System Modeling Framework (ESMF). It is a physically based and computationally efficient coupling sytem that is flexible to use in a multi-model system and portable for transition to the next generation global Earth system prediction mdoels. This standardized coupling framework allows researchers to develop and test air-sea coupling parameterizations and coupled data assimilation, and to better facilitate research-to-operation activities. It has been used and extensively tested and verified in regional coupled model forecasts of tropical cycles and winter storms (Chen and Curcic 2016, Curcic et al. 2016, and Judt et al. 2016). We will present 1) an overview of UWIN and its applications in fully coupled atmosphere-wave-ocean model predictions of hurricanes and coastal winter storms, and 2) implenmentation of UWIN in the NASA GMAO GEOS-5.

  3. Verification and Validation of COAMPS: Results from a Fully-Coupled Air/Sea/Wave Modeling System

    NASA Astrophysics Data System (ADS)

    Smith, T.; Allard, R. A.; Campbell, T. J.; Chu, Y. P.; Dykes, J.; Zamudio, L.; Chen, S.; Gabersek, S.

    2016-02-01

    The Coupled Ocean/Atmosphere Mesoscale Prediction System (COAMPS) is a state-of-the art, fully-coupled air/sea/wave modeling system that is currently being validated for operational transition to both the Naval Oceanographic Office (NAVO) and to the Fleet Numerical Meteorology and Oceanography Center (FNMOC). COAMPS is run at the Department of Defense Supercomputing Resource Center (DSRC) operated by the DoD High Performance Computing Modernization Program (HPCMP). A total of four models including the Naval Coastal Ocean Model (NCOM), Simulating Waves Nearshore (SWAN), WaveWatch III, and the COAMPS atmospheric model are coupled through both the Earth System Modeling Framework (ESMF). Results from regions of naval operational interests, including the Western Atlantic (U.S. East Coast), RIMPAC (Hawaii), and DYNAMO (Indian Ocean), will show the advantages of utilizing a coupled modeling system versus an uncoupled or stand alone model. Statistical analyses, which include model/observation comparisons, will be presented in the form of operationally approved scorecards for both the atmospheric and oceanic output. Also, computational logistics involving the HPC resources for the COAMPS simulations will be shown.

  4. Wave-current interaction in Willapa Bay

    USGS Publications Warehouse

    Olabarrieta, Maitane; Warner, John C.; Kumar, Nirnimesh

    2011-01-01

    This paper describes the importance of wave-current interaction in an inlet-estuary system. The three-dimensional, fully coupled, Coupled Ocean-Atmosphere-Wave-Sediment Transport (COAWST) modeling system was applied in Willapa Bay (Washington State) from 22 to 29 October 1998 that included a large storm event. To represent the interaction between waves and currents, the vortex-force method was used. Model results were compared with water elevations, currents, and wave measurements obtained by the U.S. Army Corp of Engineers. In general, a good agreement between field data and computed results was achieved, although some discrepancies were also observed in regard to wave peak directions in the most upstream station. Several numerical experiments that considered different forcing terms were run in order to identify the effects of each wind, tide, and wave-current interaction process. Comparison of the horizontal momentum balances results identified that wave-breaking-induced acceleration is one of the leading terms in the inlet area. The enhancement of the apparent bed roughness caused by waves also affected the values and distribution of the bottom shear stress. The pressure gradient showed significant changes with respect to the pure tidal case. During storm conditions the momentum balance in the inlet shares the characteristics of tidal-dominated and wave-dominated surf zone environments. The changes in the momentum balance caused by waves were manifested both in water level and current variations. The most relevant effect on hydrodynamics was a wave-induced setup in the inner part of the estuary.

  5. Experimental Test of Coupled Wave Model of Large Coils

    DTIC Science & Technology

    1985-06-01

    46556 Abstract: Recent data from Time Domain Pulse Reflectometry experiments on a three turn coil in the form of a race track corroborate the...Domain Pulse Reflectometry experiments on a three turn coil in the form of a race track corroborate the theory of coupled wave model for large coils...Gabriel, "Coupled Wave Model for Large Magnet Coils", NASA Contractor Report 3332, National Aeronautics and Space Administration, Washington, DC

  6. Self-Consistent Ring Current/Electromagnetic Ion Cyclotron Waves Modeling

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gamayunov, K. V.; Gallagher, D. L.

    2006-01-01

    The self-consistent treatment of the RC ion dynamics and EMIC waves, which are thought to exert important influences on the ion dynamical evolution, is an important missing element in our understanding of the storm-and recovery-time ring current evolution. For example, the EMlC waves cause the RC decay on a time scale of about one hour or less during the main phase of storms. The oblique EMIC waves damp due to Landau resonance with the thermal plasmaspheric electrons, and subsequent transport of the dissipating wave energy into the ionosphere below causes an ionosphere temperature enhancement. Under certain conditions, relativistic electrons, with energies 21 MeV, can be removed from the outer radiation belt by EMIC wave scattering during a magnetic storm. That is why the modeling of EMIC waves is critical and timely issue in magnetospheric physics. This study will generalize the self-consistent theoretical description of RC ions and EMIC waves that has been developed by Khazanov et al. [2002, 2003] and include the heavy ions and propagation effects of EMIC waves in the global dynamic of self-consistent RC - EMIC waves coupling. The results of our newly developed model that will be presented at the meeting, focusing mainly on the dynamic of EMIC waves and comparison of these results with the previous global RC modeling studies devoted to EMIC waves formation. We also discuss RC ion precipitations and wave induced thermal electron fluxes into the ionosphere.

  7. Wave-Current Interactions in a wind-jet region

    NASA Astrophysics Data System (ADS)

    Ràfols, Laura; Grifoll, Manel; Espino, Manuel; Cerralbo, Pablo; Sairouní, Abdel; Bravo, Manel; Sánchez-Arcilla, Agustín

    2017-04-01

    The Wave-Current Interactions (WCI) are investigated examining the influences of coupling two numerical models. The Regional Ocean Model System (ROMS; Shchepetkin and McWilliams, 2005) and the Simulating Waves Nearshore (SWAN; Booij et al. 1999) are used in a high resolution domain (350 m). For the initial and boundary conditions, data from the IBI-MFC products have been used and the atmospheric forcing fields have been obtained from the Catalan Meteorological Service (SMC). Results from uncoupled numerical models are compared with one-way and two-way coupling simulations. The study area is located at the northern margin of the Ebro Shelf (NW Mediterranean Sea), where episodes of strong cross-shelf wind occur. The results show that during these episodes, the water currents obtained in the two-way simulation have better agreement with the observations compared with the other simulations. Additionally, when the water currents are considered, the wave energy (and thus the significant wave heigh) decrease when the current flows in the same direction as waves propagate. The relative importance of the different terms of the momentum balance equation is also analyzed.

  8. Coupled wave model for large magnet coils

    NASA Technical Reports Server (NTRS)

    Gabriel, G. J.

    1980-01-01

    A wave coupled model based on field theory is evolved for analysis of fast electromagnetic transients on superconducting coils. It is expected to play a useful role in the design of protection methods against damage due to high voltages or any adverse effects that might arise from unintentional transients. The significant parameters of the coil are identified to be the turn to turn wave coupling coefficients and the travel time of an electromagnetic disturbance around a single turn. Unlike circuit theoretic inductor, the coil response evolves in discrete steps having durations equal to this travel time. It is during such intervals that high voltages are likely to occur. The model also bridges the gap between the low and high ends of the frequency spectrum.

  9. Coupled Atmosphere-Wave-Ocean Modeling of Tropical Cyclones: Progress, Challenges, and Ways Forward

    NASA Astrophysics Data System (ADS)

    Chen, Shuyi

    2015-04-01

    It has long been recognized that air-sea interaction plays an important role in tropical cyclones (TC) intensity change. However, most current numerical weather prediction (NWP) models are deficient in predicting TC intensity. The extreme high winds, intense rainfall, large ocean waves, and copious sea spray in TCs push the surface-exchange parameters for temperature, water vapor, and momentum into untested regimes. Parameterizations of air-sea fluxes in NWP models are often crude and create "manmade" energy source/sink that does not exist, especially in the absence of a fully interactive ocean in the model. The erroneous surface heat, moisture, and momentum fluxes can cause compounding errors in the model (e.g., precipitation, water vapor, boundary layer properties). The energy source (heat and moisture fluxes from the ocean) and sink (surface friction and wind-induced upper ocean cooling) are critical to TC intensity. However, observations of air-sea fluxes in TCs are very limited, especially in extreme high wind conditions underneath of the eyewall region. The Coupled Boundary Layer Air-Sea Transfer (CBLAST) program was designed to better understand the air-sea interaction, especially in high wind conditions, which included laboratory and coupled model experiments and field campaign in 2003-04 hurricane seasons. Significant progress has been made in better understanding of air-sea exchange coefficients up to 30 m/s, i.e., a leveling off in drag coefficient and relatively invariant exchange coefficient of enthalpy with wind speed. More recently, the Impact of Typhoon on the Ocean in the Pacific (ITOP) field campaign in 2010 has provided an unprecedented data set to study the air-sea fluxes in TCs and their impact on TC structure and intensity. More than 800 GPS dropsondes and 900 AXBTs/AXCTs as well as drifters, floats, and moorings were deployed in TCs, including Typhoons Fanapi and Malakas, and Supertyphoon Megi with a record peak wind speed of more than 80 m

  10. Estimation of oceanic subsurface mixing under a severe cyclonic storm using a coupled atmosphere-ocean-wave model

    NASA Astrophysics Data System (ADS)

    Prakash, Kumar Ravi; Nigam, Tanuja; Pant, Vimlesh

    2018-04-01

    A coupled atmosphere-ocean-wave model was used to examine mixing in the upper-oceanic layers under the influence of a very severe cyclonic storm Phailin over the Bay of Bengal (BoB) during 10-14 October 2013. The coupled model was found to improve the sea surface temperature over the uncoupled model. Model simulations highlight the prominent role of cyclone-induced near-inertial oscillations in subsurface mixing up to the thermocline depth. The inertial mixing introduced by the cyclone played a central role in the deepening of the thermocline and mixed layer depth by 40 and 15 m, respectively. For the first time over the BoB, a detailed analysis of inertial oscillation kinetic energy generation, propagation, and dissipation was carried out using an atmosphere-ocean-wave coupled model during a cyclone. A quantitative estimate of kinetic energy in the oceanic water column, its propagation, and its dissipation mechanisms were explained using the coupled atmosphere-ocean-wave model. The large shear generated by the inertial oscillations was found to overcome the stratification and initiate mixing at the base of the mixed layer. Greater mixing was found at the depths where the eddy kinetic diffusivity was large. The baroclinic current, holding a larger fraction of kinetic energy than the barotropic current, weakened rapidly after the passage of the cyclone. The shear induced by inertial oscillations was found to decrease rapidly with increasing depth below the thermocline. The dampening of the mixing process below the thermocline was explained through the enhanced dissipation rate of turbulent kinetic energy upon approaching the thermocline layer. The wave-current interaction and nonlinear wave-wave interaction were found to affect the process of downward mixing and cause the dissipation of inertial oscillations.

  11. Relationship Between the Electromagnetic Wave Energy Coupled by Overhead Lines and the Radiation Source Current Explored in the Laboratory

    NASA Astrophysics Data System (ADS)

    Li, Xiangchao; Wan, Zhicheng

    2018-04-01

    In order to solve the damage and interference problems to the electronic devices, which are induced by overvoltage excited by the coupling process between lightning electromagnetic wave and overhead lines, the lightning channel is set to be equivalent to a radiant wire antenna. Based on the integration model of lightning return stroke channel, transmission line, and ground, we take advantage of the derived formula gotten from the transmission line model. By combing the theoretical and experimental methods, we conduct a comparative analysis on the coupling process between natural/simulated lightning and overhead line. Besides, we also calculate the amplitude and energy of overvoltage, which is caused by the coupling process between lightning electromagnetic wave and overhead lines. Upon these experimental results, we can draw several conclusions as follows: when the amplitude of the lightning current in the channel is between 5 kA and 41 kA, it takes on an excellent linear relation between the amplitude of overvoltage and the magnitude of the lightning current, the relation between coupling energy and magnitude of the lightning current takes on an exponential trend. When lightning wave transmits on the transmission lines, the high-order mode will be excited. Through analysis on the high-order mode's characteristics, we find that the theoretical analysis is consistent with the experimental results, which has a certain reference value to the protection on overhead lines.

  12. Validation of the Fully-Coupled Air-Sea-Wave COAMPS System

    NASA Astrophysics Data System (ADS)

    Smith, T.; Campbell, T. J.; Chen, S.; Gabersek, S.; Tsu, J.; Allard, R. A.

    2017-12-01

    A fully-coupled, air-sea-wave numerical model, COAMPS®, has been developed by the Naval Research Laboratory to further enhance understanding of oceanic, atmospheric, and wave interactions. The fully-coupled air-sea-wave system consists of an atmospheric component with full physics parameterizations, an ocean model, NCOM (Navy Coastal Ocean Model), and two wave components, SWAN (Simulating Waves Nearshore) and WaveWatch III. Air-sea interactions between the atmosphere and ocean components are accomplished through bulk flux formulations of wind stress and sensible and latent heat fluxes. Wave interactions with the ocean include the Stokes' drift, surface radiation stresses, and enhancement of the bottom drag coefficient in shallow water due to the wave orbital velocities at the bottom. In addition, NCOM surface currents are provided to SWAN and WaveWatch III to simulate wave-current interaction. The fully-coupled COAMPS system was executed for several regions at both regional and coastal scales for the entire year of 2015, including the U.S. East Coast, Western Pacific, and Hawaii. Validation of COAMPS® includes observational data comparisons and evaluating operational performance on the High Performance Computing (HPC) system for each of these regions.

  13. Development of Operational Wave-Tide-Storm surges Coupling Prediction System

    NASA Astrophysics Data System (ADS)

    You, S. H.; Park, S. W.; Kim, J. S.; Kim, K. L.

    2009-04-01

    The Korean Peninsula is surrounded by the Yellow Sea, East China Sea, and East Sea. This complex oceanographic system includes large tides in the Yellow Sea and seasonally varying monsoon and typhoon events. For Korea's coastal regions, floods caused by wave and storm surges are among the most serious threats. To predict more accurate wave and storm surges, the development of coupling wave-tide-storm surges prediction system is essential. For the time being, wave and storm surges predictions are still made separately in KMA (Korea Meteorological Administration) and most operational institute. However, many researchers have emphasized the effects of tides and storm surges on wind waves and recommended further investigations into the effects of wave-tide-storm surges interactions and coupling module. In Korea, especially, tidal height and current give a great effect on the wave prediction in the Yellow sea where is very high tide and related research is not enough. At present, KMA has operated the wave (RWAM : Regional Wave Model) and storm surges/tide prediction system (STORM : Storm Surges/Tide Operational Model) for ocean forecasting. The RWAM is WAVEWATCH III which is a third generation wave model developed by Tolman (1989). The STORM is based on POM (Princeton Ocean Model, Blumberg and Mellor, 1987). The RWAM and STORM cover the northwestern Pacific Ocean from 115°E to 150°E and from 20°N to 52°N. The horizontal grid intervals are 1/12° in both latitudinal and longitudinal directions. These two operational models are coupled to simulate wave heights for typhoon case. The sea level and current simulated by storm surge model are used for the input of wave model with 3 hour interval. The coupling simulation between wave and storm surge model carried out for Typhoon Nabi (0514), Shanshan(0613) and Nari (0711) which were effected on Korea directly. We simulated significant wave height simulated by wave model and coupling model and compared difference between

  14. The role of satellite directional wave spectra for the improvement of the ocean-waves coupling

    NASA Astrophysics Data System (ADS)

    Aouf, Lotfi; Hauser, Danièle; Chapron, Bertrand

    2017-04-01

    Swell waves are well captured by the Synthetic Aperture Radar (SAR) which provides the directional wave spectra for waves roughly larger than 200 m. Since the launch of sentinel-1A and 1B SAR directional wave spectra are available to improve the swell wave forecasting and the coupling processes at the air-sea interface. Moreover next year CFOSAT mission will provide directional wave spectra for waves with wavelengths comprised between 70 to 500 m. This study aims to evaluate the assimilation of SAR and synthetic CFOSAT wave spectra on the coupling between the wave model MFWAM and the ocean model NEMO. Three coupling processes as described in Breivik et al. (2014) of Stokes-Coriolis forcing, the ocean side stress and the turbulence injected by the wave breaking in the ocean mixed layer have been used. a coupling run is performed with and without assimilation of directional wave spectra. the impact of SAR wave data on key parameters such as surface sea temperature, currents and salinity is investigated. Particular attention is carried out for ocean areas with swell dominant wave climate.

  15. Sediment Transport over a Dredge Pit, Sandy Point Southeast, west flank of the Mississippi River during Summer Upcoast Currents: a Coupled Wave, Current and Sediment Numerical Model

    NASA Astrophysics Data System (ADS)

    Chaichitehrani, N.; Li, C.; Xu, K.; Bentley, S. J.; Miner, M. D.

    2017-12-01

    Sandy Point southeast, an elongated sand resource, was dredged in November 2012 to restore Pelican Island, Louisiana. Hydrodynamics and wave propagation patterns along with fluvial sediments from the Mississippi River influence the sediment and bottom boundary layer dynamics over Sandy Point. A state-of-the-art numerical model, Delft3D, was implemented to investigate current variations and wave transformation on Sandy Point as well as sediment transport pattern. Delft3d FLOW and WAVE modules were coupled and validated using WAVCIS and NDBC data. Sediment transport model was run by introducing both bed and river sediments, consisted of mainly mud and a small fraction of sand. A sediment transport model was evaluated for surface sediment concentration using data derived from satellite images. The model results were used to study sediment dynamics and bottom boundary layer characteristics focused on the Sandy Point area during summer. Two contrasting bathymetric configurations, with and without the Sandy Point dredge pit, were used to conduct an experiment on the sediment and bottom boundary layer dynamics. Preliminary model results showed that the presence of the Sandy Point pit has very limited effect on the hydrodynamics and wave pattern at the pit location. Sediments from the Mississippi River outlets, especially in the vicinity of the pit, get trapped in the pit under the easterly to the northeasterly upcoast current which prevails in August. We also examined the wave-induced sediment reworking and river-borne fluvial sediment over Sandy Point. The effect of wind induced orbital velocity increases the bottom shear stress compared to the time with no waves, relatively small wave heights (lower than 1.5 meters) along the deepest part of the pit (about 20 meters) causes little bottom sediment rework during this period. The results showed that in the summertime, river water is more likely the source of sedimentation in the pit.

  16. Modulation of wave fields by current and wind intensifications off the Catalan coast

    NASA Astrophysics Data System (ADS)

    Pallares Lopez, Elena; Sánchez-Arcilla, Agustin; Espino, Manuel

    2017-04-01

    The coupling between waves, ocean and atmospheric models has been one of the main topics in the physical oceanography community for the last decade. The resulting challenge is more difficult and relevant in coastal areas, where the interaction between wind, waves and currents fields is far from negligible, and therefore some sort of model coupling is required. However, it is important to remark that it is only during energetic "enough" events that the coupling becomes quantitatively significant. The Western Mediterranean sea is an area characterised by calm periods most of the year. However, coastal areas often present highly variable and heterogeneous wind, wave and current conditions, which make the numerical prediction of meteo-oceanographic processes difficult and with large associated local errors. Specifically, the Catalan coast is frequently affected by offshore wind intensifications channel by river valleys and by local current intensifications associated to coastal "bulges" (e.g. deltaic forms) that can reach up to 1 m/s in the surface. In this study we present different coupling strategies applied to both calm periods and energetic events, represented by the wind jets or current intensifications mentioned before, with the objective to quantify the effect of model coupling on the resulting wave fields off the Catalan coast. The SWAN wave model is used to model the wave fields, together with the ROMS oceanic model and the WRF atmospheric model. Two different types of coupling are considered: the first is a one-way coupling consisting in introducing the current field as an input for the SWAN wave model; the second one, consists in running in parallel the ROMS circulation model, the WRF atmospheric model and the SWAN wave model. The second methodology is more complex and should better reproduce the physics involved in the interactions, but requires an important computational capacity, not always available, so a critical comparison between the two

  17. A numerical study of wave-current interaction through surface and bottom stresses: Coastal ocean response to Hurricane Fran of 1996

    NASA Astrophysics Data System (ADS)

    Xie, L.; Pietrafesa, L. J.; Wu, K.

    2003-02-01

    A three-dimensional wave-current coupled modeling system is used to examine the influence of waves on coastal currents and sea level. This coupled modeling system consists of the wave model-WAM (Cycle 4) and the Princeton Ocean Model (POM). The results from this study show that it is important to incorporate surface wave effects into coastal storm surge and circulation models. Specifically, we find that (1) storm surge models without coupled surface waves generally under estimate not only the peak surge but also the coastal water level drop which can also cause substantial impact on the coastal environment, (2) introducing wave-induced surface stress effect into storm surge models can significantly improve storm surge prediction, (3) incorporating wave-induced bottom stress into the coupled wave-current model further improves storm surge prediction, and (4) calibration of the wave module according to minimum error in significant wave height does not necessarily result in an optimum wave module in a wave-current coupled system for current and storm surge prediction.

  18. Investigation of hurricane Ivan using the coupled ocean-atmosphere-wave-sediment transport (COAWST) model

    USGS Publications Warehouse

    Zambon, Joseph B.; He, Ruoying; Warner, John C.

    2014-01-01

    The coupled ocean–atmosphere–wave–sediment transport (COAWST) model is used to hindcast Hurricane Ivan (2004), an extremely intense tropical cyclone (TC) translating through the Gulf of Mexico. Sensitivity experiments with increasing complexity in ocean–atmosphere–wave coupled exchange processes are performed to assess the impacts of coupling on the predictions of the atmosphere, ocean, and wave environments during the occurrence of a TC. Modest improvement in track but significant improvement in intensity are found when using the fully atmosphere–ocean-wave coupled configuration versus uncoupled (e.g., standalone atmosphere, ocean, or wave) model simulations. Surface wave fields generated in the fully coupled configuration also demonstrates good agreement with in situ buoy measurements. Coupled and uncoupled model-simulated sea surface temperature (SST) fields are compared with both in situ and remote observations. Detailed heat budget analysis reveals that the mixed layer temperature cooling in the deep ocean (on the shelf) is caused primarily by advection (equally by advection and diffusion).

  19. Assessment of current effect on waves in a semi-enclosed basin

    NASA Astrophysics Data System (ADS)

    Benetazzo, A.; Carniel, S.; Sclavo, M.; Bergamasco, A.

    2012-04-01

    The wave-current interaction process in the semi-enclosed Adriatic Sea is studied using the Coupled Ocean-Atmosphere-Wave-Sediment Transport (COAWST) modeling system, which is used to exchange data fields between the ocean model ROMS (Regional Ocean Modeling System) and the wave model SWAN (Simulating WAves Nearshore). The 2-way data transfer between circulation and wave models is synchronous with ROMS providing current fields, free surface elevation, and bathymetry to SWAN. In particular, the 3-D current profiles are averaged using a formulation that integrates the near-surface velocity over a depth controlled by the spectral mean wave number. This coupling procedure is carried out up to coastal areas by means of an offline grid nesting. The parent grid covers the whole Adriatic Sea and has a horizontal resolution of 2.0 km, whereas the child grid resolution increases to 0.5 km but it is limited to the northern Adriatic Sea (Gulf of Venice), where the current effect on waves is investigated. The most frequent winds blowing on the Adriatic Sea are the so-called Bora and Sirocco which cause high waves in the Adriatic Sea, although Bora waves are generally fetch-limited. In fact, Bora winds blow orthogonal to the main basin axis (approximately aligned with the NW-SE direction), while Sirocco has large spatial scale being a southeasterly wind. For the numerical simulations, the meteorological forcings are provided by the operational meteorological model COSMO-I7, which is the Italian version of the COSMO Model, a mesoscale model developed in the framework of the COSMO Consortium. During the analysis period, the simulated wind, current and wave are compared with observations at the ISMAR oceanographic tower located off the Venice littoral. Wave heights and sea surface winds are also compared with satellite-derived data. To account for the variability of sea states during a storm, the expected maximum individual wave height in a sea storm with a given history is also

  20. Multi-scale coupled modelling of waves and currents on the Catalan shelf.

    NASA Astrophysics Data System (ADS)

    Grifoll, M.; Warner, J. C.; Espino, M.; Sánchez-Arcilla, A.

    2012-04-01

    Catalan shelf circulation is characterized by a background along-shelf flow to the southwest (including some meso-scale features) plus episodic storm driven patterns. To investigate these dynamics, a coupled multi-scale modeling system is applied to the Catalan shelf (North-western Mediterranean Sea). The implementation consists of a set of increasing-resolution nested models, based on the circulation model ROMS and the wave model SWAN as part of the COAWST modeling system, covering from the slope and shelf region (~1 km horizontal resolution) down to a local area around Barcelona city (~40 m). The system is initialized with MyOcean products in the coarsest outer domain, and uses atmospheric forcing from other sources for the increasing resolution inner domains. Results of the finer resolution domains exhibit improved agreement with observations relative to the coarser model results. Several hydrodynamic configurations were simulated to determine dominant forcing mechanisms and hydrodynamic processes that control coastal scale processes. The numerical results reveal that the short term (hours to days) inner-shelf variability is strongly influenced by local wind variability, while sea-level slope, baroclinic effects, radiation stresses and regional circulation constitute second-order processes. Additional analysis identifies the significance of shelf/slope exchange fluxes, river discharge and the effect of the spatial resolution of the atmospheric fluxes.

  1. Evaluation of Simulated Marine Aerosol Production Using the WaveWatchIII Prognostic Wave Model Coupled to the Community Atmosphere Model within the Community Earth System Model

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

    Long, M. S.; Keene, William C.; Zhang, J.

    2016-11-08

    Primary marine aerosol (PMA) is emitted into the atmosphere via breaking wind waves on the ocean surface. Most parameterizations of PMA emissions use 10-meter wind speed as a proxy for wave action. This investigation coupled the 3 rd generation prognostic WAVEWATCH-III wind-wave model within a coupled Earth system model (ESM) to drive PMA production using wave energy dissipation rate – analogous to whitecapping – in place of 10-meter wind speed. The wind speed parameterization did not capture basin-scale variability in relations between wind and wave fields. Overall, the wave parameterization did not improve comparison between simulated versus measured AOD ormore » Na +, thus highlighting large remaining uncertainties in model physics. Results confirm the efficacy of prognostic wind-wave models for air-sea exchange studies coupled with laboratory- and field-based characterizations of the primary physical drivers of PMA production. No discernible correlations were evident between simulated PMA fields and observed chlorophyll or sea surface temperature.« less

  2. Wave-induced current considering wave-tide interaction in Haeundae

    NASA Astrophysics Data System (ADS)

    Lim, Hak Soo

    2017-04-01

    The Haeundae, located at the south eastern end of the Korean Peninsula, is a famous beach, which has an approximately 1.6 km long and 70 m wide coastline. The beach has been repeatedly eroded by the swell waves caused by typhoons in summer and high waves originating in the East Sea in winter. The Korean government conducted beach restoration projects including beach nourishment (620,000 m3) and construction of two submerged breakwaters near both ends of the beach. To prevent the beach erosion and to support the beach restoration project, the Korean government initiated a R&D project, the development of coastal erosion control technology since 2013. As a part of the project, we have been measuring waves and currents at a water depth of 22 m, 1.8 km away from the beach using an acoustic wave and current meter (AWAC) continuously for more than three years; we have also measured waves and currents intensively near the surf-zone in summer and winter. In this study, a numerical simulation using a wave and current coupled model (ROMS-SWAN) was conducted for determining the wave-induced current considering seasonal swell waves (Hs : 2.5 m, Tp: 12 s) and for better understanding of the coastal process near the surf-zone in Haeundae. By comparing the measured and simulated results, we found that cross-shore current during summer is mainly caused by the eddy produced by the wave-induced current near the beach, which in turn, is generated by the strong waves coming from the SSW and S directions. During other seasons, longshore wave-induced current is produced by the swell waves coming from the E and ESE directions. The longshore current heading west toward Dong-Back Island, west end of the beach, during all the seasons and eddy current toward Mipo-Port, east end of the beach, in summer which is well matched with the observed residual current. The wave-induced current with long-term measurement data is incorporated in simulation of sediment transport modeling for developing

  3. The Effect of the Leeuwin Current on Offshore Surface Gravity Waves in Southwest Western Australia

    NASA Astrophysics Data System (ADS)

    Wandres, Moritz; Wijeratne, E. M. S.; Cosoli, Simone; Pattiaratchi, Charitha

    2017-11-01

    The knowledge of regional wave regimes is critical for coastal zone planning, protection, and management. In this study, the influence of the offshore current regime on surface gravity waves on the southwest Western Australian (SWWA) continental shelf was examined. This was achieved by coupling the three dimensional, free surface, terrain-following hydrodynamic Regional Ocean Modelling System (ROMS) and the third generation wave model Simulating WAves Nearshore (SWAN) using the Coupled Ocean-Atmosphere-WaveSediment Transport (COAWST) model. Different representative states of the Leeuwin Current (LC), a strong pole-ward flowing boundary current with a persistent eddy field along the SWWA shelf edge were simulated and used to investigate their influence on different large wave events. The coupled wave-current simulations were compared to wave only simulations, which represented scenarios in the absence of a background current field. Results showed that the LC and the eddy field significantly impact SWWA waves. Significant wave heights increased (decreased) when currents were opposing (aligning with) the incoming wave directions. During a fully developed LC system significant wave heights were altered by up to ±25% and wave directions by up to ±20°. The change in wave direction indicates that the LC may modify nearshore wave dynamics and consequently alter sediment patterns. Operational regional wave forecasts and hindcasts may give flawed predictions if wave-current interaction is not properly accounted for.

  4. Wave-current interactions in megatidal environment

    NASA Astrophysics Data System (ADS)

    Bennis, A. C.; Pascal, B. D. B.; Feddy, A.; Garnier, V.; Accenti, M.; Dumas, F.; Ardhuin, F.

    2016-12-01

    The strongest tidal current in western Europe (up to 12 knots) occurs in Raz Blanchard (Normandy, France). High winds occur over six months which generate energetic wave conditions with breaking waves, hence the name of `Blanchard'. However, few studies have been conducted on the wave effects on the tidal current at this location because of the lack of measurements. Studies are now required to aid the creation of tidal farms. For this purpose, the 3D fully-coupled model MARS-WW3 is used with three nested ranks which are forced at boundaries by wave spectra from HOMERE database (Boudière et al., 2013) and by sea level from the French Navy (SHOM). The model is tested against ADCP data of IRSN at three locations near Raz Blanchard. Time series of current velocity and of mean sea level are consistent with ADCP data. A rephasing by waves of the tidal current is observed in comparison with simulations without waves, which fits the ADCP data. A strong dependence of the tidal current on bottom roughness is shown as well as the necessity to take into account its spatial heterogeneity. The simulated mean sea level is close to the measured one while it was underestimated for high tide in simulations without wave effects. The vertical shape of the tidal current is especially modified near the surface by waves as expected. Depending on the tidal cycle and wave direction, acceleration or deceleration of the surface current due to waves is observed. Lastly, several hydrodynamical scenarios for Raz Blanchard are carried out for different tidal and wave conditions pending the HYD2M'17 data (ADCP, ADV, drifting wave buoys, HF and VHF and X-Band radars). First results show the impacts of refractive, shoaling and blocking effects on the flood and ebb currents.

  5. Coupling hydrodynamic and wave propagation modeling for waveform modeling of SPE.

    NASA Astrophysics Data System (ADS)

    Larmat, C. S.; Steedman, D. W.; Rougier, E.; Delorey, A.; Bradley, C. R.

    2015-12-01

    The goal of the Source Physics Experiment (SPE) is to bring empirical and theoretical advances to the problem of detection and identification of underground nuclear explosions. This paper presents effort to improve knowledge of the processes that affect seismic wave propagation from the hydrodynamic/plastic source region to the elastic/anelastic far field thanks to numerical modeling. The challenge is to couple the prompt processes that take place in the near source region to the ones taking place later in time due to wave propagation in complex 3D geologic environments. In this paper, we report on results of first-principles simulations coupling hydrodynamic simulation codes (Abaqus and CASH), with a 3D full waveform propagation code, SPECFEM3D. Abaqus and CASH model the shocked, hydrodynamic region via equations of state for the explosive, borehole stemming and jointed/weathered granite. LANL has been recently employing a Coupled Euler-Lagrange (CEL) modeling capability. This has allowed the testing of a new phenomenological model for modeling stored shear energy in jointed material. This unique modeling capability has enabled highfidelity modeling of the explosive, the weak grout-filled borehole, as well as the surrounding jointed rock. SPECFEM3D is based on the Spectral Element Method, a direct numerical method for full waveform modeling with mathematical accuracy (e.g. Komatitsch, 1998, 2002) thanks to its use of the weak formulation of the wave equation and of high-order polynomial functions. The coupling interface is a series of grid points of the SEM mesh situated at the edge of the hydrodynamic code domain. Displacement time series at these points are computed from output of CASH or Abaqus (by interpolation if needed) and fed into the time marching scheme of SPECFEM3D. We will present validation tests and waveforms modeled for several SPE tests conducted so far, with a special focus on effect of the local topography.

  6. The Nonlinear Coupling of Electromagnetic Ion Cyclotron and Lower Hybrid Waves in the Ring Current Region

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.

    2004-01-01

    The excitation of lower hybrid waves (LHWs) is a widely discussed mechanism of interaction between plasma species in space, and is one of the unresolved questions of magnetospheric multi-ion plasmas. In this paper we present the morphology, dynamics, and level of LHW activity generated by electromagnetic ion cyclotron (EMIC) waves during the May 2-7, 1998 storm period on the global scale. The LHWs were calculated based on a newly developed self-consistent model (Khazanov et. al., 2002, 2003) that couples the system of two kinetic equations: one equation describes the ring current (RC) ion dynamic, and another equation describes the evolution of EMIC waves. It is found that the LHWs are excited by helium ions due to their mass dependent drift in the electric field of EMIC waves. The level of LHW activity is calculated assuming that the induced scattering process is the main saturation mechanism for these waves. The calculated LHWs electric fields are consistent with the observational data.

  7. A coupled "AB" system: Rogue waves and modulation instabilities.

    PubMed

    Wu, C F; Grimshaw, R H J; Chow, K W; Chan, H N

    2015-10-01

    Rogue waves are unexpectedly large and localized displacements from an equilibrium position or an otherwise calm background. For the nonlinear Schrödinger (NLS) model widely used in fluid mechanics and optics, these waves can occur only when dispersion and nonlinearity are of the same sign, a regime of modulation instability. For coupled NLS equations, rogue waves will arise even if dispersion and nonlinearity are of opposite signs in each component as new regimes of modulation instability will appear in the coupled system. The same phenomenon will be demonstrated here for a coupled "AB" system, a wave-current interaction model describing baroclinic instability processes in geophysical flows. Indeed, the onset of modulation instability correlates precisely with the existence criterion for rogue waves for this system. Transitions from "elevation" rogue waves to "depression" rogue waves are elucidated analytically. The dispersion relation as a polynomial of the fourth order may possess double pairs of complex roots, leading to multiple configurations of rogue waves for a given set of input parameters. For special parameter regimes, the dispersion relation reduces to a cubic polynomial, allowing the existence criterion for rogue waves to be computed explicitly. Numerical tests correlating modulation instability and evolution of rogue waves were conducted.

  8. Evaluating wave-current interaction in an urban estuary and flooding implications for coastal communities

    NASA Astrophysics Data System (ADS)

    Cifuentes-Lorenzen, A.; O'Donnell, J.; Howard-Strobel, M. M.; Fake, T.; McCardell, G.

    2016-12-01

    Accurate hydrodynamic-wave coupled coastal circulation models aid the prediction of storm impacts, particularly in areas where data is absent, and can inform mitigation options. They are essential everywhere to account for the effects of climate change. Here, the Finite Volume Community Ocean Model (FVCOM) was used to estimate the residual circulation inside a small urban estuary, Long Island Sound, during three severe weather events of different magnitude (i.e. 1/5, 1/25 and 1/50 year events). The effect of including wave coupling using a log-layer bottom boundary and the bottom wave-current coupling, following the approach of Madsen (1994) on the simulated residual circulation was assessed. Significant differences in the solutions were constrained to the near surface (s>-0.3) region. No significant difference in the depth-averaged residual circulation was detected. When the Madsen (1994) bottom boundary layer model for wave-current interaction was employed, differences in residual circulation resulted. The bottom wave-current interaction also plays an important role in the wave dynamics. Significant wave heights along the northern Connecticut shoreline were enhanced by up to 15% when the bottom wave-current interaction was included in the simulations. The wave-induced bottom drag enhancement has a substantial effect on tides in the Sound, possibly because it is nearly resonant at semidiurnal frequencies. This wave-current interaction current leads to severe tidal dampening ( 40% amplitude reduction) at the Western end of the estuary in the modeled sea surface displacement. The potential magnitude of these effects means that wave current interaction should be included and carefully evaluated in models of estuaries that are useful.

  9. Surface wave effects in the NEMO ocean model: Forced and coupled experiments

    NASA Astrophysics Data System (ADS)

    Breivik, Øyvind; Mogensen, Kristian; Bidlot, Jean-Raymond; Balmaseda, Magdalena Alonso; Janssen, Peter A. E. M.

    2015-04-01

    The NEMO general circulation ocean model is extended to incorporate three physical processes related to ocean surface waves, namely the surface stress (modified by growth and dissipation of the oceanic wavefield), the turbulent kinetic energy flux from breaking waves, and the Stokes-Coriolis force. Experiments are done with NEMO in ocean-only (forced) mode and coupled to the ECMWF atmospheric and wave models. Ocean-only integrations are forced with fields from the ERA-Interim reanalysis. All three effects are noticeable in the extratropics, but the sea-state-dependent turbulent kinetic energy flux yields by far the largest difference. This is partly because the control run has too vigorous deep mixing due to an empirical mixing term in NEMO. We investigate the relation between this ad hoc mixing and Langmuir turbulence and find that it is much more effective than the Langmuir parameterization used in NEMO. The biases in sea surface temperature as well as subsurface temperature are reduced, and the total ocean heat content exhibits a trend closer to that observed in a recent ocean reanalysis (ORAS4) when wave effects are included. Seasonal integrations of the coupled atmosphere-wave-ocean model consisting of NEMO, the wave model ECWAM, and the atmospheric model of ECMWF similarly show that the sea surface temperature biases are greatly reduced when the mixing is controlled by the sea state and properly weighted by the thickness of the uppermost level of the ocean model. These wave-related physical processes were recently implemented in the operational coupled ensemble forecast system of ECMWF.

  10. Preliminary Study on Coupling Wave-Tide-Storm Surges Prediction System

    NASA Astrophysics Data System (ADS)

    You, S.; Park, S.; Seo, J.; Kim, K.

    2008-12-01

    The Korean Peninsula is surrounded by the Yellow Sea, East China Sea, and East Sea. This complex oceanographic system includes large tides in the Yellow Sea and seasonally varying monsoon and typhoon events. For Korea's coastal regions, floods caused by wave and storm surges are among the most serious threats. To predict more accurate wave and storm surge, the development of coupling wave-tide-storm surges prediction system is essential. For the time being, wave and storm surges predictions are still made separately in KMA (Korea Meteorological Administration) and most operational institute. However, many researchers have emphasized the effects of tides and storm surges on wind waves and recommended further investigations into the effects of wave-tide-storm surges interactions and coupling module on wave heights. However, tidal height and current give a great effect on the wave prediction in the Yellow sea where is very high tide and related research is not enough. At present, KMA has operated the wave (RWAM : Regional Wave Model) and storm surges/tide prediction system (RTSM : Regional Tide/Storm Surges Model) for ocean forecasting. The RWAM is WAVEWATCH III which is a third generation wave model developed by Tolman (1989). The RTSM is based on POM (Princeton Ocean Model, Blumberg and Mellor, 1987). The RWAM and RTSM cover the northwestern Pacific Ocean from 115°E to 150°E and from 20°N to 52°N. The horizontal grid intervals are 1/12° in both latitudinal and longitudinal directions. The development, testing and application of a coupling module in which wave-tide-storm surges are incorporated within the frame of KMA Ocean prediction system, has been considered as a step forward in respect of ocean forecasting. In addition, advanced wave prediction model will be applicable to the effect of ocean in the weather forecasting system. The main purpose of this study is to show how the coupling module developed and to report on a series of experiments dealing with the

  11. Self-Consistent Model of Magnetospheric Electric Field, Ring Current, Plasmasphere, and Electromagnetic Ion Cyclotron Waves: Initial Results

    NASA Technical Reports Server (NTRS)

    Gamayunov, K. V.; Khazanov, G. V.; Liemohn, M. W.; Fok, M.-C.; Ridley, A. J.

    2009-01-01

    Further development of our self-consistent model of interacting ring current (RC) ions and electromagnetic ion cyclotron (EMIC) waves is presented. This model incorporates large scale magnetosphere-ionosphere coupling and treats self-consistently not only EMIC waves and RC ions, but also the magnetospheric electric field, RC, and plasmasphere. Initial simulations indicate that the region beyond geostationary orbit should be included in the simulation of the magnetosphere-ionosphere coupling. Additionally, a self-consistent description, based on first principles, of the ionospheric conductance is required. These initial simulations further show that in order to model the EMIC wave distribution and wave spectral properties accurately, the plasmasphere should also be simulated self-consistently, since its fine structure requires as much care as that of the RC. Finally, an effect of the finite time needed to reestablish a new potential pattern throughout the ionosphere and to communicate between the ionosphere and the equatorial magnetosphere cannot be ignored.

  12. A Dynamic Coupled Magnetosphere-Ionosphere-Ring Current Model

    NASA Astrophysics Data System (ADS)

    Pembroke, Asher

    In this thesis we describe a coupled model of Earth's magnetosphere that consists of the Lyon-Fedder-Mobarry (LFM) global magnetohydrodynamics (MHD) simulation, the MIX ionosphere solver and the Rice Convection Model (RCM). We report some results of the coupled model using idealized inputs and model parameters. The algorithmic and physical components of the model are described, including the transfer of magnetic field information and plasma boundary conditions to the RCM and the return of ring current plasma properties to the LFM. Crucial aspects of the coupling include the restriction of RCM to regions where field-line averaged plasma-beta ¡=1, the use of a plasmasphere model, and the MIX ionosphere model. Compared to stand-alone MHD, the coupled model produces a substantial increase in ring current pressure and reduction of the magnetic field near the Earth. In the ionosphere, stronger region-1 and region-2 Birkeland currents are seen in the coupled model but with no significant change in the cross polar cap potential drop, while the region-2 currents shielded the low-latitude convection potential. In addition, oscillations in the magnetic field are produced at geosynchronous orbit with the coupled code. The diagnostics of entropy and mass content indicate that these oscillations are associated with low-entropy flow channels moving in from the tail and may be related to bursty bulk flows and bubbles seen in observations. As with most complex numerical models, there is the ongoing challenge of untangling numerical artifacts and physics, and we find that while there is still much room for improvement, the results presented here are encouraging. Finally, we introduce several new methods for magnetospheric visualization and analysis, including a fluid-spatial volume for RCM and a field-aligned analysis mesh for the LFM. The latter allows us to construct novel visualizations of flux tubes, drift surfaces, topological boundaries, and bursty-bulk flows.

  13. On the Use of Coupled Wind, Wave, and Current Fields in the Simulation of Loads on Bottom-Supported Offshore Wind Turbines during Hurricanes: March 2012 - September 2015

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

    Kim, Eungsoo; Manuel, Lance; Curcic, Milan

    In the United States, potential offshore wind plant sites have been identified along the Atlantic seaboard and in the Gulf of Mexico. It is imperative that we define external conditions associated with hurricanes and severe winter storms and consider load cases for which wind turbines may need to be designed. We selected two hurricanes, Ike (2008) and Sandy (2012), and investigated the effect these tropical storms would have on bottom-supported offshore wind turbines that were hypothetically in or close to their path as they made landfall. For realistic turbine loads assessment, it is important that the coupled influences of themore » changing wind, wave, and current fields are simulated throughout the evolution of the hurricanes. We employed a coupled model--specifically, the University of Miami Coupled Model (UMCM)--that integrates atmospheric, wave, and ocean components to produce needed wind, wave, and current data. The wind data are used to generate appropriate vertical wind profiles and full wind velocity fields including turbulence; the current field over the water column is obtained by interpolated discrete output current data; and short-crested irregular second-order waves are simulated using output directional wave spectra from the coupled model. We studied two monopile-supported offshore wind turbines sited in 20 meters of water in the Gulf of Mexico to estimate loads during Hurricane Ike, and a jacket space-frame platform-supported offshore wind turbine sited in 50 meters of water in the mid-Atlantic region to estimate loads during Hurricane Sandy. In this report we discuss in detail how the simulated hurricane wind, wave, and current output data are used in turbine loads studies. In addition, important characteristics of the external conditions are studied, including the relative importance of swell versus wind seas, aerodynamic versus hydrodynamic forces, current velocity effects, yaw control options for the turbine, hydrodynamic drag versus inertia

  14. Validation of a coupled wave-flow model in a high-energy setting: the mouth of the Columbia River

    USGS Publications Warehouse

    Elias, Edwin P.L.; Gelfenbaum, Guy R.; van der Westhuysen, André J.

    2012-01-01

     A monthlong time series of wave, current, salinity, and suspended-sediment measurements was made at five sites on a transect across the Mouth of Columbia River (MCR). These data were used to calibrate and evaluate the performance of a coupled hydrodynamic and wave model for the MCR based on the Delft3D modeling system. The MCR is a dynamic estuary inlet in which tidal currents, river discharge, and wave-driven currents are all important. Model tuning consisted primarily of spatial adjustments to bottom drag coefficients. In combination with (near-) default parameter settings, the MCR model application is able to simulate the dominant features in the tidal flow, salinity and wavefields observed in field measurements. The wave-orbital averaged method for representing the current velocity profile in the wave model is considered the most realistic for the MCR. The hydrodynamic model is particularly effective in reproducing the observed vertical residual and temporal variations in current structure. Density gradients introduce the observed and modeled reversal of the mean flow at the bed and augment mean and peak flow in the upper half of the water column. This implies that sediment transport during calmer summer conditions is controlled by density stratification and is likely net landward due to the reversal of flow near the bed. The correspondence between observed and modeled hydrodynamics makes this application a tool to investigate hydrodynamics and associated sediment transport.

  15. Validation of a coupled wave-flow model in a high-energy setting: The mouth of the Columbia River

    NASA Astrophysics Data System (ADS)

    Elias, Edwin P. L.; Gelfenbaum, Guy; Van der Westhuysen, André J.

    2012-09-01

    A monthlong time series of wave, current, salinity, and suspended-sediment measurements was made at five sites on a transect across the Mouth of Columbia River (MCR). These data were used to calibrate and evaluate the performance of a coupled hydrodynamic and wave model for the MCR based on the Delft3D modeling system. The MCR is a dynamic estuary inlet in which tidal currents, river discharge, and wave-driven currents are all important. Model tuning consisted primarily of spatial adjustments to bottom drag coefficients. In combination with (near-) default parameter settings, the MCR model application is able to simulate the dominant features in the tidal flow, salinity and wavefields observed in field measurements. The wave-orbital averaged method for representing the current velocity profile in the wave model is considered the most realistic for the MCR. The hydrodynamic model is particularly effective in reproducing the observed vertical residual and temporal variations in current structure. Density gradients introduce the observed and modeled reversal of the mean flow at the bed and augment mean and peak flow in the upper half of the water column. This implies that sediment transport during calmer summer conditions is controlled by density stratification and is likely net landward due to the reversal of flow near the bed. The correspondence between observed and modeled hydrodynamics makes this application a tool to investigate hydrodynamics and associated sediment transport.

  16. Self-Consistent Ring Current Modeling with Propagating Electromagnetic Ion Cyclotron Waves in the Presence of Heavy Ions

    NASA Technical Reports Server (NTRS)

    Khazanov, George V.

    2006-01-01

    The self-consistent treatment of the RC ion dynamics and EMIC waves, which are thought to exert important influences on the ion dynamical evolution, is an important missing element in our understanding of the storm-and recovery-time ring current evolution. Under certain conditions, relativistic electrons, with energies 21 MeV, can be removed from the outer radiation belt by EMIC wave scattering during a magnetic storm. That is why the modeling of EMIC waves is critical and timely issue in magnetospheric physics. To describe the RC evolution itself this study uses the ring current-atmosphere interaction model (RAM). RAM solves the gyration and bounce-averaged Boltzmann-Landau equation inside of geosynchronous orbit. Originally developed at the University of Michigan, there are now several branches of this model currently in use as describe by Liemohn namely those at NASA Goddard Space Flight Center This study will generalize the self-consistent theoretical description of RC ions and EMIC waves that has been developed by Khazanov and include the heavy ions and propagation effects of EMIC waves in the global dynamic of self-consistent RC - EMIC waves coupling. The results of our newly developed model that will be presented at GEM meeting, focusing mainly on the dynamic of EMIC waves and comparison of these results with the previous global RC modeling studies devoted to EMIC waves formation. We also discuss RC ion precipitations and wave induced thermal electron fluxes into the ionosphere.

  17. Wave-induced stress and breaking of sea ice in a coupled hydrodynamic discrete-element wave-ice model

    NASA Astrophysics Data System (ADS)

    Herman, Agnieszka

    2017-11-01

    In this paper, a coupled sea ice-wave model is developed and used to analyze wave-induced stress and breaking in sea ice for a range of wave and ice conditions. The sea ice module is a discrete-element bonded-particle model, in which ice is represented as cuboid grains floating on the water surface that can be connected to their neighbors by elastic joints. The joints may break if instantaneous stresses acting on them exceed their strength. The wave module is based on an open-source version of the Non-Hydrostatic WAVE model (NHWAVE). The two modules are coupled with proper boundary conditions for pressure and velocity, exchanged at every wave model time step. In the present version, the model operates in two dimensions (one vertical and one horizontal) and is suitable for simulating compact ice in which heave and pitch motion dominates over surge. In a series of simulations with varying sea ice properties and incoming wavelength it is shown that wave-induced stress reaches maximum values at a certain distance from the ice edge. The value of maximum stress depends on both ice properties and characteristics of incoming waves, but, crucially for ice breaking, the location at which the maximum occurs does not change with the incoming wavelength. Consequently, both regular and random (Jonswap spectrum) waves break the ice into floes with almost identical sizes. The width of the zone of broken ice depends on ice strength and wave attenuation rates in the ice.

  18. The impact of sea surface currents in wave power potential modeling

    NASA Astrophysics Data System (ADS)

    Zodiatis, George; Galanis, George; Kallos, George; Nikolaidis, Andreas; Kalogeri, Christina; Liakatas, Aristotelis; Stylianou, Stavros

    2015-11-01

    The impact of sea surface currents to the estimation and modeling of wave energy potential over an area of increased economic interest, the Eastern Mediterranean Sea, is investigated in this work. High-resolution atmospheric, wave, and circulation models, the latter downscaled from the regional Mediterranean Forecasting System (MFS) of the Copernicus marine service (former MyOcean regional MFS system), are utilized towards this goal. The modeled data are analyzed by means of a variety of statistical tools measuring the potential changes not only in the main wave characteristics, but also in the general distribution of the wave energy and the wave parameters that mainly affect it, when using sea surface currents as a forcing to the wave models. The obtained results prove that the impact of the sea surface currents is quite significant in wave energy-related modeling, as well as temporally and spatially dependent. These facts are revealing the necessity of the utilization of the sea surface currents characteristics in renewable energy studies in conjunction with their meteo-ocean forecasting counterparts.

  19. Framework of distributed coupled atmosphere-ocean-wave modeling system

    NASA Astrophysics Data System (ADS)

    Wen, Yuanqiao; Huang, Liwen; Deng, Jian; Zhang, Jinfeng; Wang, Sisi; Wang, Lijun

    2006-05-01

    In order to research the interactions between the atmosphere and ocean as well as their important role in the intensive weather systems of coastal areas, and to improve the forecasting ability of the hazardous weather processes of coastal areas, a coupled atmosphere-ocean-wave modeling system has been developed. The agent-based environment framework for linking models allows flexible and dynamic information exchange between models. For the purpose of flexibility, portability and scalability, the framework of the whole system takes a multi-layer architecture that includes a user interface layer, computational layer and service-enabling layer. The numerical experiment presented in this paper demonstrates the performance of the distributed coupled modeling system.

  20. Coupling Hydrodynamic and Wave Propagation Codes for Modeling of Seismic Waves recorded at the SPE Test.

    NASA Astrophysics Data System (ADS)

    Larmat, C. S.; Rougier, E.; Delorey, A.; Steedman, D. W.; Bradley, C. R.

    2016-12-01

    The goal of the Source Physics Experiment (SPE) is to bring empirical and theoretical advances to the problem of detection and identification of underground nuclear explosions. For this, the SPE program includes a strong modeling effort based on first principles calculations with the challenge to capture both the source and near-source processes and those taking place later in time as seismic waves propagate within complex 3D geologic environments. In this paper, we report on results of modeling that uses hydrodynamic simulation codes (Abaqus and CASH) coupled with a 3D full waveform propagation code, SPECFEM3D. For modeling the near source region, we employ a fully-coupled Euler-Lagrange (CEL) modeling capability with a new continuum-based visco-plastic fracture model for simulation of damage processes, called AZ_Frac. These capabilities produce high-fidelity models of various factors believed to be key in the generation of seismic waves: the explosion dynamics, a weak grout-filled borehole, the surrounding jointed rock, and damage creation and deformations happening around the source and the free surface. SPECFEM3D, based on the Spectral Element Method (SEM) is a direct numerical method for full wave modeling with mathematical accuracy. The coupling interface consists of a series of grid points of the SEM mesh situated inside of the hydrodynamic code's domain. Displacement time series at these points are computed using output data from CASH or Abaqus (by interpolation if needed) and fed into the time marching scheme of SPECFEM3D. We will present validation tests with the Sharpe's model and comparisons of waveforms modeled with Rg waves (2-8Hz) that were recorded up to 2 km for SPE. We especially show effects of the local topography, velocity structure and spallation. Our models predict smaller amplitudes of Rg waves for the first five SPE shots compared to pure elastic models such as Denny &Johnson (1991).

  1. Coupling of WRF meteorological model to WAM spectral wave model through sea surface roughness at the Balearic Sea: impact on wind and wave forecasts

    NASA Astrophysics Data System (ADS)

    Tolosana-Delgado, R.; Soret, A.; Jorba, O.; Baldasano, J. M.; Sánchez-Arcilla, A.

    2012-04-01

    Meteorological models, like WRF, usually describe the earth surface characteristics by tables that are function of land-use. The roughness length (z0) is an example of such approach. However, over sea z0 is modeled by the Charnock (1955) relation, linking the surface friction velocity u*2 with the roughness length z0 of turbulent air flow, z0 = α-u2* g The Charnock coefficient α may be considered a measure of roughness. For the sea surface, WRF considers a constant roughness α = 0.0185. However, there is evidence that sea surface roughness should depend on wave energy (Donelan, 1982). Spectral wave models like WAM, model the evolution and propagation of wave energy as a function of wind, and include a richer sea surface roughness description. Coupling WRF and WAM is thus a common way to improve the sea surface roughness description of WRF. WAM is a third generation wave model, solving the equation of advection of wave energy subject to input/output terms of: wind growth, energy dissipation and resonant non-linear wave-wave interactions. Third generation models work on the spectral domain. WAM considers the Charnock coefficient α a complex yet known function of the total wind input term, which depends on the wind velocity and on the Charnock coefficient again. This is solved iteratively (Janssen et al., 1990). Coupling of meteorological and wave models through a common Charnock coefficient is operationally done in medium-range met forecasting systems (e.g., at ECMWF) though the impact of coupling for smaller domains is not yet clearly assessed (Warner et al, 2010). It is unclear to which extent the additional effort of coupling improves the local wind and wave fields, in comparison to the effects of other factors, like e.g. a better bathymetry and relief resolution, or a better circulation information which might have its influence on local-scale meteorological processes (local wind jets, local convection, daily marine wind regimes, etc.). This work, within the

  2. Particle transport model sensitivity on wave-induced processes

    NASA Astrophysics Data System (ADS)

    Staneva, Joanna; Ricker, Marcel; Krüger, Oliver; Breivik, Oyvind; Stanev, Emil; Schrum, Corinna

    2017-04-01

    Different effects of wind waves on the hydrodynamics in the North Sea are investigated using a coupled wave (WAM) and circulation (NEMO) model system. The terms accounting for the wave-current interaction are: the Stokes-Coriolis force, the sea-state dependent momentum and energy flux. The role of the different Stokes drift parameterizations is investigated using a particle-drift model. Those particles can be considered as simple representations of either oil fractions, or fish larvae. In the ocean circulation models the momentum flux from the atmosphere, which is related to the wind speed, is passed directly to the ocean and this is controlled by the drag coefficient. However, in the real ocean, the waves play also the role of a reservoir for momentum and energy because different amounts of the momentum flux from the atmosphere is taken up by the waves. In the coupled model system the momentum transferred into the ocean model is estimated as the fraction of the total flux that goes directly to the currents plus the momentum lost from wave dissipation. Additionally, we demonstrate that the wave-induced Stokes-Coriolis force leads to a deflection of the current. During the extreme events the Stokes velocity is comparable in magnitude to the current velocity. The resulting wave-induced drift is crucial for the transport of particles in the upper ocean. The performed sensitivity analyses demonstrate that the model skill depends on the chosen processes. The results are validated using surface drifters, ADCP, HF radar data and other in-situ measurements in different regions of the North Sea with a focus on the coastal areas. The using of a coupled model system reveals that the newly introduced wave effects are important for the drift-model performance, especially during extremes. Those effects cannot be neglected by search and rescue, oil-spill, transport of biological material, or larva drift modelling.

  3. Nonlinear Wave Chaos and the Random Coupling Model

    NASA Astrophysics Data System (ADS)

    Zhou, Min; Ott, Edward; Antonsen, Thomas M.; Anlage, Steven

    The Random Coupling Model (RCM) has been shown to successfully predict the statistical properties of linear wave chaotic cavities in the highly over-moded regime. It is of interest to extend the RCM to strongly nonlinear systems. To introduce nonlinearity, an active nonlinear circuit is connected to two ports of the wave chaotic 1/4-bowtie cavity. The active nonlinear circuit consists of a frequency multiplier, an amplifier and several passive filters. It acts to double the input frequency in the range from 3.5 GHz to 5 GHz, and operates for microwaves going in only one direction. Measurements are taken between two additional ports of the cavity and we measure the statistics of the second harmonic voltage over an ensemble of realizations of the scattering system. We developed an RCM-based model of this system as two chaotic cavities coupled by means of a nonlinear transfer function. The harmonics received at the output are predicted to be the product of three statistical quantities that describe the three elements correspondingly. Statistical results from simulation, RCM-based modeling, and direct experimental measurements will be compared. ONR under Grant No. N000141512134, AFOSR under COE Grant FA9550-15-1-0171,0 and the Maryland Center for Nanophysics and Advanced Materials.

  4. Analysis of the Tangjiaxi landslide-generated waves in the Zhexi Reservoir, China, by a granular flow coupling model

    NASA Astrophysics Data System (ADS)

    Huang, Bolin; Yin, Yueping; Wang, Shichang; Tan, Jianmin; Liu, Guangning

    2017-05-01

    A rocky granular flow is commonly formed after the failure of rocky bank slopes. An impulse wave disaster may also be initiated if the rocky granular flow rushes into a river with a high velocity. Currently, the granular mass-water body coupling study is an important trend in the field of landslide-induced impulse waves. In this paper, a full coupling numerical model for landslide-induced impulse waves is developed based on a non-coherent granular flow equation, i.e., the Mih equation. In this model, the Mih equation for continuous non-coherent granular flow controls movements of sliding mass, the two-phase flow equation regulates the interaction between sliding mass and water, and the renormalization group (RNG) turbulence model governs the movement of the water body. The proposed model is validated and applied for the 2014 Tangjiaxi landslide of the Zhexi Reservoir located in Hunan Province, China, to analyze the characteristics of both landslide motion and its following impulse waves. On 16 July 2014, a rocky debris flow was formed after the failure of the Tangjiaxi landslide, damming the Tangjiaxi stream and causing an impulse wave disaster with three dead and nine missing bodies. Based on the full coupling numerical analysis, the granular flow impacts the water with a maximum velocity of about 22.5 m s-1. Moreover, the propagation velocity of the generated waves reaches up to 12 m s-1. The maximum calculated run-up of 21.8 m is close enough to the real value of 22.7 m. The predicted landslide final deposit and wave run-up heights are in a good agreement with the field survey data. These facts verify the ability of the proposed model for simulating the real impulse wave generated by rocky granular flow events.

  5. Equatorial waves in some CMIP5 coupled models (with stratosphere)

    NASA Astrophysics Data System (ADS)

    Maury, Pauline; Lott, François; Guez, Lionel

    2013-04-01

    The Kelvin and the Rossby Gravity Waves (RGWs) packets that dominate the day to day variability in the low equatorial stratosphere (50hPa) are analyzed in 7 ESMs that participate to CMIP5 and that include a well resolved stratosphere. The results are compared to ERAI. Two models are also used to quantify better (i) the impact of the QBO on these waves (MPI-P and MPI-MR), and (ii) the impact of convection (IPSL-CM5A and CM5B). In the stratosphere all models present quite coherent Kelvin waves and RGWs packets, which is good think since these waves dominate the day to day variability in the low stratosphere. The errors on these freely propagating waves seem therefore less pronounced then the differences seen by others on the convectively coupled waves in the troposphere. The difference between the models nevertheless stay very large, the models with a QBO have more pronounced waves, and represent better their life-cycle (this is particularly true for the RGWs). The sensitivity to the convection of the rather slow waves analysed here is not as pronounced as was found in the past for may be faster waves, but is nevertheless confirmed when we look at the same model with two drastically different convection parameterization. In the same spirit, the sensitivity of the RGWs to the QBO is confirmed by comparing almost the same model runs, one with a QBO and one without. Having a QBO nevertheless does not guarantee that the waves are realistic in all respects, as shows for instance the Temperature signature due to the RGWs in the UKMO model. There also seems to have an issue when the resolution changes drastically, the MRI model behaving quite differently from the other models when it comes to the simulations of these equatorial waves.

  6. Alfven Wave Reflection Model of Field-Aligned Currents at Mercury

    NASA Technical Reports Server (NTRS)

    Lyatsky, Wladislaw; Khazanov, George V.; Slavin, James

    2010-01-01

    An Alfven Wave Reflection (AWR) model is proposed that provides closure for strong field-aligned currents (FACs) driven by the magnetopause reconnection in the magnetospheres of planets having no significant ionospheric and surface electrical conductance. The model is based on properties of the Alfven waves, generated at high altitudes and reflected from the low-conductivity surface of the planet. When magnetospheric convection is very slow, the incident and reflected Alfven waves propagate along approximately the same path. In this case, the net field-aligned currents will be small. However, as the convection speed increases. the reflected wave is displaced relatively to the incident wave so that the incident and reflected waves no longer compensate each other. In this case, the net field-aligned current may be large despite the lack of significant ionospheric and surface conductivity. Our estimate shows that for typical solar wind conditions at Mercury, the magnitude of Region 1-type FACs in Mercury's magnetosphere may reach hundreds of kilo-Amperes. This AWR model of field-aligned currents may provide a solution to the long-standing problem of the closure of FACs in the Mercury's magnetosphere. c2009 Elsevier Inc. All rights reserved.

  7. Assessing the performance of formulations for nonlinear feedback of surface gravity waves on ocean currents over coastal waters

    NASA Astrophysics Data System (ADS)

    Wang, Pengcheng; Sheng, Jinyu; Hannah, Charles

    2017-08-01

    This study presents applications of a two-way coupled wave-circulation modelling system over coastal waters, with a special emphasis of performance assessments of two different methods for nonlinear feedback of ocean surface gravity waves on three-dimensional (3D) ocean currents. These two methods are the vortex force (VF) formulation suggested by Bennis et al. (2011) and the latest version of radiation stress (RS) formulation suggested by Mellor (2015). The coupled modelling system is first applied to two idealized test cases of surf-zone scales to validate implementations of these two methods in the coupled wave-circulation system. Model results show that the latest version of RS has difficulties in producing the undertow over the surf zone. The coupled system is then applied to Lunenburg Bay (LB) of Nova Scotia during Hurricane Juan in 2003. The coupled system using both the VF and RS formulations generates much stronger and more realistic 3D circulation in the Bay during Hurricane Juan than the circulation-only model, demonstrating the importance of surface wave forces to the 3D ocean circulation over coastal waters. However, the RS formulation generates some weak unphysical currents outside the wave breaking zone due to a less reasonable representation for the vertical distribution of the RS gradients over a slopping bottom. These weak unphysical currents are significantly magnified in a two-way coupled system when interacting with large surface waves, degrading the model performance in simulating currents at one observation site. Our results demonstrate that the VF formulation with an appropriate parameterization of wave breaking effects is able to produce reasonable results for applications over coastal waters during extreme weather events. The RS formulation requires a complex wave theory rather than the linear wave theory for the approximation of a vertical RS term to improve its performance under both breaking and non-breaking wave conditions.

  8. Mobility of maerl-siliciclastic mixtures: Impact of waves, currents and storm events

    NASA Astrophysics Data System (ADS)

    Joshi, Siddhi; Duffy, Garret Patrick; Brown, Colin

    2017-04-01

    Maerl beds are free-living, non-geniculate coralline algae habitats which form biogenic reefs with high micro-scale complexity supporting a diversity and abundance of rare epifauna and epiflora. These habitats are highly mobile in shallow marine environments where substantial maerl beds co-exist with siliciclastic sediment, exemplified by our study site of Galway Bay. Coupled hydrodynamic-wave-sediment transport models have been used to explore the transport patterns of maerl-siliciclastic sediment during calm summer conditions and severe winter storms. The sediment distribution is strongly influenced by storm waves even in water depths greater than 100 m. Maerl is present at the periphery of wave-induced residual current gyres during storm conditions. A combined wave-current Sediment Mobility Index during storm conditions shows correlation with multibeam backscatter and surficial sediment distribution. A combined wave-current Mobilization Frequency Index during storm conditions acts as a physical surrogate for the presence of maerl-siliciclastic mixtures in Galway Bay. Both indices can provide useful integrated oceanographic and sediment information to complement coupled numerical hydrodynamic, sediment transport and erosion-deposition models.

  9. Ocean-Wave Dynamics Analysis during Hurricane Ida and Norida Using a Fully Coupled Modeling System

    NASA Astrophysics Data System (ADS)

    Olabarrieta, M.; Warner, J. C.; Armstrong, B. N.

    2010-12-01

    Extreme storms, such as hurricanes and extratropical storms play a dominant role in shaping the beaches of the East and Gulf Coasts of the United States. Future tropical depressions will be more intense than in the present climate (Assessment Report of IPCC, 2007) and therefore coastal areas are likely to become more susceptible to their effects. The major damage caused by these extreme events is associated with the duration of the storm, storm intensity, waves, and the total water levels reached during the storm. Numerical models provide a useful approach to study the spatial and temporal distribution of these parameters. However, the correct estimation of the total water levels and wind wave heights through numerical modeling requires accurate representation of the air-sea interface dynamics. These processes are highly complex due to the variable interactions between winds, ocean waves and currents near the sea surface. In the present research we use the COAWST (Coupled Ocean-Atmosphere-Wave-Sediment Transport) modeling system (Warner et al., 2010) to address the key role of the atmosphere-ocean-wave interactions during Hurricane Ida and its posterior evolution to NorIda, November 2009. This northeastern storm was one of the most costly in the past two decades and likely in the top five of the past century. One interesting aspect of the considered period is that it includes two very different atmospheric extreme conditions, a hurricane and a northeastern storm, developed in regions with very different oceanographic characteristics. By performing a suite of numerical runs we are able to isolate the effect of the interaction terms between the atmosphere (WRF model), the ocean (ROMS model) and the wave propagation and generation model (SWAN). Special attention is given to the role of the ocean surface roughness and high resolution SST fields on the atmospheric boundary layers dynamics and consequently these effects on the wind wave generation, surface currents and

  10. A numerical study on the effects of wave-current-surge interactions on the height and propagation of sea surface waves in Charleston Harbor during Hurricane Hugo 1989

    NASA Astrophysics Data System (ADS)

    Liu, Huiqing; Xie, Lian

    2009-06-01

    The effects of wave-current interactions on ocean surface waves induced by Hurricane Hugo in and around the Charleston Harbor and its adjacent coastal waters are examined by using a three-dimensional (3D) wave-current coupled modeling system. The 3D storm surge modeling component of the coupled system is based on the Princeton Ocean Model (POM), the wave modeling component is based on the third generation wave model, Simulating WAves Nearshore (SWAN), and the inundation model is adopted from [Xie, L., Pietrafesa, L. J., Peng, M., 2004. Incorporation of a mass-conserving inundation scheme into a three-dimensional storm surge model. J. Coastal Res., 20, 1209-1223]. The results indicate that the change of water level associated with the storm surge is the primary cause for wave height changes due to wave-surge interaction. Meanwhile, waves propagating on top of surge cause a feedback effect on the surge height by modulating the surface wind stress and bottom stress. This effect is significant in shallow coastal waters, but relatively small in offshore deep waters. The influence of wave-current interaction on wave propagation is relatively insignificant, since waves generally propagate in the direction of the surface currents driven by winds. Wave-current interactions also affect the surface waves as a result of inundation and drying induced by the storm. Waves break as waters retreat in regions of drying, whereas waves are generated in flooded regions where no waves would have occurred without the flood water.

  11. Experimental characterization and modelling of non-linear coupling of the lower hybrid current drive power on Tore Supra

    NASA Astrophysics Data System (ADS)

    Preynas, M.; Goniche, M.; Hillairet, J.; Litaudon, X.; Ekedahl, A.; Colas, L.

    2013-01-01

    To achieve steady-state operation on future fusion devices, in particular on ITER, the coupling of the lower hybrid wave must be optimized on a wide range of edge conditions. However, under some specific conditions, deleterious effects on the lower hybrid current drive (LHCD) coupling are sometimes observed on Tore Supra. In this way, dedicated LHCD experiments have been performed using the LHCD system of Tore Supra, composed of two different conceptual designs of launcher: the fully active multi-junction (FAM) and the new passive active multi-junction (PAM) antennas. A non-linear interaction between the electron density and the electric field has been characterized in a thin plasma layer in front of the two LHCD antennas. The resulting dependence of the power reflection coefficient (RC) with the LHCD power is not predicted by the standard linear theory of the LH wave coupling. A theoretical model is suggested to describe the non-linear wave-plasma interaction induced by the ponderomotive effect and implemented in a new full wave LHCD code, PICCOLO-2D (ponderomotive effect in a coupling code of lower hybrid wave-2D). The code self-consistently treats the wave propagation in the antenna vicinity and its interaction with the local edge plasma density. The simulation reproduces very well the occurrence of a non-linear behaviour in the coupling observed in the LHCD experiments. The important differences and trends between the FAM and the PAM antennas, especially a larger increase in RC for the FAM, are also reproduced by the PICCOLO-2D simulation. The working hypothesis of the contribution of the ponderomotive effect in the non-linear observations of LHCD coupling is therefore validated through this comprehensive modelling for the first time on the FAM and PAM antennas on Tore Supra.

  12. Wave Coupling in the Atmosphere-Ionosphere System

    NASA Astrophysics Data System (ADS)

    Forbes, J. M.

    2016-12-01

    Vertically-propagating solar and lunar tides, Kelvin waves, gravity waves (GW) and planetary waves (PW) constitute the primary mechanism for transmitting lower atmosphere variability to the upper atmosphere and ionosphere. Vertically propagating waves grow exponentially with height into the more rarified atmosphere where they dissipate, deposit net momentum and heat, and induce net constituent transport. Some waves penetrate to the base of the exosphere (ca. 500-600 km). Over the past decade, a mature knowledge of the tidal part of the spectrum has emerged, in an average or climatological sense, up to about 110 km. This knowledge has largely accrued as a result of remote sensing observations made from the TIMED satellite. These observations have also enabled limited studies on day-to-day variability of atmospheric tides, the PW and Kelvin wave spectra up to 110 km, and PW-tide coupling. Complementary ionospheric observations made by GPS receivers, COSMIC, CHAMP, and ROCSAT contain signatures of plasma redistributions induced by these waves, and ionosphere-thermosphere (IT) general circulation models have been developed that provide a corroborating theoretical foundation. Pioneering theoretical and modeling work also demonstrate the importance of the GW part of the spectrum on thermosphere circulation and thermal structure. While significant strides have been made, critical shortcomings in our understanding of atmosphere-IT coupling remain. In particular, we are practically absent any observations of the vertical evolution and dissipation of the wave spectrum between 100 and 200 km, which is also the region where electric fields and currents are generated by dynamo action. Moreover, the day-to-day variability of the wave spectrum and secondary wave generation remain to be quantified in this critical region. In this talk, the above progress and knowledge gaps will be examined in light of imminent and potential future missions.

  13. Wave-Ice interaction in the Marginal Ice Zone: Toward a Wave-Ocean-Ice Coupled Modeling System

    DTIC Science & Technology

    2015-09-30

    MIZ using WW3 (3 frequency bins, ice retreat in August and ice advance in October); Blue (solid): Based on observations near Antarctica by Meylan...1 DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Wave- Ice interaction in the Marginal Ice Zone: Toward a...Wave-Ocean- Ice Coupled Modeling System W. E. Rogers Naval Research Laboratory, Code 7322 Stennis Space Center, MS 39529 phone: (228) 688-4727

  14. The effect of wave current interactions on the storm surge and inundation in Charleston Harbor during Hurricane Hugo 1989

    NASA Astrophysics Data System (ADS)

    Xie, Lian; Liu, Huiqing; Peng, Machuan

    The effects of wave-current interactions on the storm surge and inundation induced by Hurricane Hugo in and around the Charleston Harbor and its adjacent coastal regions are examined by using a three-dimensional (3-D) wave-current coupled modeling system. The 3-D storm surge and inundation modeling component of the coupled system is based on the Princeton ocean model (POM), whereas the wave modeling component is based on the third-generation wave model, simulating waves nearshore (SWAN). The results indicate that the effects of wave-induced surface, bottom, and radiation stresses can separately or in combination produce significant changes in storm surge and inundation. The effects of waves vary spatially. In some areas, the contribution of waves to peak storm surge during Hurricane Hugo reached as high as 0.76 m which led to substantial changes in the inundation and drying areas simulated by the storm surge model.

  15. Performance analysis of coupled and uncoupled hydrodynamic and wave models in the northern Adriatic Sea

    NASA Astrophysics Data System (ADS)

    Busca, Claudia; Coluccelli, Alessandro; Valentini, Andrea; Benetazzo, Alvise; Bonaldo, Davide; Bortoluzzi, Giovanni; Carniel, Sandro; Falcieri, Francesco; Paccagnella, Tiziana; Ravaioli, Mariangela; Riminucci, Francesco; Sclavo, Mauro; Russo, Aniello

    2014-05-01

    implementations currently running, there is the need to: assess their forecast skill; quantitatively evaluate if the new, coupled systems provide better performances than the uncoupled ones; individuate weaknesses and eventual time trends in the forecasts quality, their causes, and actions to improve the systems. This work presents a first effort aimed to satisfy such need. We employ in situ and remote sensing data collected starting from November 2011, in particular: temperature and salinity data collected during several oceanographic cruises, sea surface temperature derived from satellite measurements, waves, sea level and currents measurements from oceanographic buoys and platforms; specific observational activities funded by the Italian Flagship project RITMARE allowed to collect new measurements in NA coastal areas. Data-model comparison is firstly performed with exploratory qualitative comparisons in order to highlight discrepancies between observed and forecasted data, then a quantitative comparison is performed through the computation of standard statistical scores (root mean square error, mean error, mean bias, standard deviation, cross-correlation). Results are plotted in Taylor diagrams for a rapid evaluation of the overall performances.

  16. Wave Climate and Wave Mixing in the Marginal Ice Zones of Arctic Seas, Observations and Modelling

    DTIC Science & Technology

    2014-09-30

    At the same time, the PIs participate in Australian efforts of developing wave-ocean- ice coupled models for Antarctica . Specific new physics modules...Wave Mixing in the Marginal Ice Zones of Arctic Seas, Observations and Modelling Alexander V. Babanin Swinburne University of Technology, PO Box...operational forecast. Altimeter climatology and the wave models will be used to study the current and future wind/wave and ice trends. APPROACH

  17. Coupled Hydrodynamic and Wave Propagation Modeling for the Source Physics Experiment: Study of Rg Wave Sources for SPE and DAG series.

    NASA Astrophysics Data System (ADS)

    Larmat, C. S.; Delorey, A.; Rougier, E.; Knight, E. E.; Steedman, D. W.; Bradley, C. R.

    2017-12-01

    This presentation reports numerical modeling efforts to improve knowledge of the processes that affect seismic wave generation and propagation from underground explosions, with a focus on Rg waves. The numerical model is based on the coupling of hydrodynamic simulation codes (Abaqus, CASH and HOSS), with a 3D full waveform propagation code, SPECFEM3D. Validation datasets are provided by the Source Physics Experiment (SPE) which is a series of highly instrumented chemical explosions at the Nevada National Security Site with yields from 100kg to 5000kg. A first series of explosions in a granite emplacement has just been completed and a second series in alluvium emplacement is planned for 2018. The long-term goal of this research is to review and improve current existing seismic sources models (e.g. Mueller & Murphy, 1971; Denny & Johnson, 1991) by providing first principles calculations provided by the coupled codes capability. The hydrodynamic codes, Abaqus, CASH and HOSS, model the shocked, hydrodynamic region via equations of state for the explosive, borehole stemming and jointed/weathered granite. A new material model for unconsolidated alluvium materials has been developed and validated with past nuclear explosions, including the 10 kT 1965 Merlin event (Perret, 1971) ; Perret and Bass, 1975). We use the efficient Spectral Element Method code, SPECFEM3D (e.g. Komatitsch, 1998; 2002), and Geologic Framework Models to model the evolution of wavefield as it propagates across 3D complex structures. The coupling interface is a series of grid points of the SEM mesh situated at the edge of the hydrodynamic code domain. We will present validation tests and waveforms modeled for several SPE tests which provide evidence that the damage processes happening in the vicinity of the explosions create secondary seismic sources. These sources interfere with the original explosion moment and reduces the apparent seismic moment at the origin of Rg waves up to 20%.

  18. Using the Model Coupling Toolkit to couple earth system models

    USGS Publications Warehouse

    Warner, J.C.; Perlin, N.; Skyllingstad, E.D.

    2008-01-01

    Continued advances in computational resources are providing the opportunity to operate more sophisticated numerical models. Additionally, there is an increasing demand for multidisciplinary studies that include interactions between different physical processes. Therefore there is a strong desire to develop coupled modeling systems that utilize existing models and allow efficient data exchange and model control. The basic system would entail model "1" running on "M" processors and model "2" running on "N" processors, with efficient exchange of model fields at predetermined synchronization intervals. Here we demonstrate two coupled systems: the coupling of the ocean circulation model Regional Ocean Modeling System (ROMS) to the surface wave model Simulating WAves Nearshore (SWAN), and the coupling of ROMS to the atmospheric model Coupled Ocean Atmosphere Prediction System (COAMPS). Both coupled systems use the Model Coupling Toolkit (MCT) as a mechanism for operation control and inter-model distributed memory transfer of model variables. In this paper we describe requirements and other options for model coupling, explain the MCT library, ROMS, SWAN and COAMPS models, methods for grid decomposition and sparse matrix interpolation, and provide an example from each coupled system. Methods presented in this paper are clearly applicable for coupling of other types of models. ?? 2008 Elsevier Ltd. All rights reserved.

  19. Two-dimensional solitary waves and periodic waves on coupled nonlinear electrical transmission lines

    NASA Astrophysics Data System (ADS)

    Wang, Heng; Zheng, Shuhua

    2017-06-01

    By using the dynamical system approach, the exact travelling wave solutions for a system of coupled nonlinear electrical transmission lines are studied. Based on this method, the bifurcations of phase portraits of a dynamical system are given. The two-dimensional solitary wave solutions and periodic wave solutions on coupled nonlinear transmission lines are obtained. With the aid of Maple, the numerical simulations are conducted for solitary wave solutions and periodic wave solutions to the model equation. The results presented in this paper improve upon previous studies.

  20. Numerical simulation of wave-current interaction under strong wind conditions

    NASA Astrophysics Data System (ADS)

    Larrañaga, Marco; Osuna, Pedro; Ocampo-Torres, Francisco Javier

    2017-04-01

    Although ocean surface waves are known to play an important role in the momentum and other scalar transfer between the atmosphere and the ocean, most operational numerical models do not explicitly include the terms of wave-current interaction. In this work, a numerical analysis about the relative importance of the processes associated with the wave-current interaction under strong off-shore wind conditions in Gulf of Tehuantepec (the southern Mexican Pacific) was carried out. The numerical system includes the spectral wave model WAM and the 3D hydrodynamic model POLCOMS, with the vertical turbulent mixing parametrized by the kappa-epsilon closure model. The coupling methodology is based on the vortex-force formalism. The hydrodynamic model was forced at the open boundaries using the HYCOM database and the wave model was forced at the open boundaries by remote waves from the southern Pacific. The atmospheric forcing for both models was provided by a local implementation of the WRF model, forced at the open boundaries using the CFSR database. The preliminary analysis of the model results indicates an effect of currents on the propagation of the swell throughout the study area. The Stokes-Coriolis term have an impact on the transient Ekman transport by modifying the Ekman spiral, while the Stokes drift has an effect on the momentum advection and the production of TKE, where the later induces a deepening of the mixing layer. This study is carried out in the framework of the project CONACYT CB-2015-01 255377 and RugDiSMar Project (CONACYT 155793).

  1. Self-Consistent Ring Current Modeling with Propagating Electromagnetic Ion Cyclotron Waves in the Presence of Heavy Ions

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gamayunov, K. V.; Gallagher, D. L.; Kozyra, J. U.; Liemohn, M. W.

    2006-01-01

    The self-consistent treatment of the RC ion dynamics and EMlC waves, which are thought to exert important influences on the ion dynamical evolution, is an important missing element in our understanding of the storm-and recovery-time ring current evolution. Under certain conditions, relativistic electrons, with energies greater than or equal to 1 MeV, can be removed from the outer radiation belt by EMlC wave scattering during a magnetic storm (Summers and Thorne, 2003; Albert, 2003). That is why the modeling of EMlC waves is critical and timely issue in magnetospheric physics. This study will generalize the self-consistent theoretical description of RC ions and EMlC waves that has been developed by Khazanov et al. [2002, 2003] and include the heavy ions and propagation effects of EMlC waves in the global dynamic of self-consistent RC - EMlC waves coupling. The results of our newly developed model that will be presented at Huntsville 2006 meeting, focusing mainly on the dynamic of EMlC waves and comparison of these results with the previous global RC modeling studies devoted to EMlC waves formation. We also discuss RC ion precipitations and wave induced thermal electron fluxes into the ionosphere.

  2. Modelling of sediment transport and morphological evolution under the combined action of waves and currents

    NASA Astrophysics Data System (ADS)

    Franz, Guilherme; Delpey, Matthias T.; Brito, David; Pinto, Lígia; Leitão, Paulo; Neves, Ramiro

    2017-09-01

    Coastal defence structures are often constructed to prevent beach erosion. However, poorly designed structures may cause serious erosion problems in the downdrift direction. Morphological models are useful tools to predict such impacts and assess the efficiency of defence structures for different scenarios. Nevertheless, morphological modelling is still a topic under intense research effort. The processes simulated by a morphological model depend on model complexity. For instance, undertow currents are neglected in coastal area models (2DH), which is a limitation for simulating the evolution of beach profiles for long periods. Model limitations are generally overcome by predefining invariant equilibrium profiles that are allowed to shift offshore or onshore. A more flexible approach is described in this paper, which can be generalised to 3-D models. The present work is based on the coupling of the MOHID modelling system and the SWAN wave model. The impacts of different designs of detached breakwaters and groynes were simulated in a schematic beach configuration following a 2DH approach. The results of bathymetry evolution are in agreement with the patterns found in the literature for several existing structures. The model was also tested in a 3-D test case to simulate the formation of sandbars by undertow currents. The findings of this work confirmed the applicability of the MOHID modelling system to study sediment transport and morphological changes in coastal zones under the combined action of waves and currents. The same modelling methodology was applied to a coastal zone (Costa da Caparica) located at the mouth of a mesotidal estuary (Tagus Estuary, Portugal) to evaluate the hydrodynamics and sediment transport both in calm water conditions and during events of highly energetic waves. The MOHID code is available in the GitHub repository.

  3. Ocean surface waves in Hurricane Ike (2008) and Superstorm Sandy (2012): Coupled model predictions and observations

    NASA Astrophysics Data System (ADS)

    Chen, Shuyi S.; Curcic, Milan

    2016-07-01

    Forecasting hurricane impacts of extreme winds and flooding requires accurate prediction of hurricane structure and storm-induced ocean surface waves days in advance. The waves are complex, especially near landfall when the hurricane winds and water depth varies significantly and the surface waves refract, shoal and dissipate. In this study, we examine the spatial structure, magnitude, and directional spectrum of hurricane-induced ocean waves using a high resolution, fully coupled atmosphere-wave-ocean model and observations. The coupled model predictions of ocean surface waves in Hurricane Ike (2008) over the Gulf of Mexico and Superstorm Sandy (2012) in the northeastern Atlantic and coastal region are evaluated with the NDBC buoy and satellite altimeter observations. Although there are characteristics that are general to ocean waves in both hurricanes as documented in previous studies, wave fields in Ike and Sandy possess unique properties due mostly to the distinct wind fields and coastal bathymetry in the two storms. Several processes are found to significantly modulate hurricane surface waves near landfall. First, the phase speed and group velocities decrease as the waves become shorter and steeper in shallow water, effectively increasing surface roughness and wind stress. Second, the bottom-induced refraction acts to turn the waves toward the coast, increasing the misalignment between the wind and waves. Third, as the hurricane translates over land, the left side of the storm center is characterized by offshore winds over very short fetch, which opposes incoming swell. Landfalling hurricanes produce broader wave spectra overall than that of the open ocean. The front-left quadrant is most complex, where the combination of windsea, swell propagating against the wind, increasing wind-wave stress, and interaction with the coastal topography requires a fully coupled model to meet these challenges in hurricane wave and surge prediction.

  4. High Order Accurate Finite Difference Modeling of Seismo-Acoustic Wave Propagation in a Moving Atmosphere and a Heterogeneous Earth Model Coupled Across a Realistic Topography

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

    Petersson, N. Anders; Sjogreen, Bjorn

    Here, we develop a numerical method for simultaneously simulating acoustic waves in a realistic moving atmosphere and seismic waves in a heterogeneous earth model, where the motions are coupled across a realistic topography. We model acoustic wave propagation by solving the linearized Euler equations of compressible fluid mechanics. The seismic waves are modeled by the elastic wave equation in a heterogeneous anisotropic material. The motion is coupled by imposing continuity of normal velocity and normal stresses across the topographic interface. Realistic topography is resolved on a curvilinear grid that follows the interface. The governing equations are discretized using high ordermore » accurate finite difference methods that satisfy the principle of summation by parts. We apply the energy method to derive the discrete interface conditions and to show that the coupled discretization is stable. The implementation is verified by numerical experiments, and we demonstrate a simulation of coupled wave propagation in a windy atmosphere and a realistic earth model with non-planar topography.« less

  5. High Order Accurate Finite Difference Modeling of Seismo-Acoustic Wave Propagation in a Moving Atmosphere and a Heterogeneous Earth Model Coupled Across a Realistic Topography

    DOE PAGES

    Petersson, N. Anders; Sjogreen, Bjorn

    2017-04-18

    Here, we develop a numerical method for simultaneously simulating acoustic waves in a realistic moving atmosphere and seismic waves in a heterogeneous earth model, where the motions are coupled across a realistic topography. We model acoustic wave propagation by solving the linearized Euler equations of compressible fluid mechanics. The seismic waves are modeled by the elastic wave equation in a heterogeneous anisotropic material. The motion is coupled by imposing continuity of normal velocity and normal stresses across the topographic interface. Realistic topography is resolved on a curvilinear grid that follows the interface. The governing equations are discretized using high ordermore » accurate finite difference methods that satisfy the principle of summation by parts. We apply the energy method to derive the discrete interface conditions and to show that the coupled discretization is stable. The implementation is verified by numerical experiments, and we demonstrate a simulation of coupled wave propagation in a windy atmosphere and a realistic earth model with non-planar topography.« less

  6. Self-consistent Model of Magnetospheric Electric Field, RC and EMIC Waves

    NASA Technical Reports Server (NTRS)

    Gamayunov, K. V.; Khazanov, G. V.; Liemohn, M. W.; Fok, M.-C.

    2007-01-01

    Electromagnetic ion cyclotron (EMIC) waves are an important magnetospheric emission, which is excited near the magnetic equator with frequencies below the proton gyro-frequency. The source of bee energy for wave growth is provided by temperature anisotropy of ring current (RC) ions, which develops naturally during inward convection from the plasma sheet These waves strongly affect the dynamic s of resonant RC ions, thermal electrons and ions, and the outer radiation belt relativistic electrons, leading to non-adiabatic particle heating and/or pitch-angle scattering and loss to the atmosphere. The rate of ion and electron scattering/heating is strongly controlled by the Wave power spectral and spatial distributions, but unfortunately, the currently available observational information regarding EMIC wave power spectral density is poor. So combinations of reliable data and theoretical models should be utilized in order to obtain the power spectral density of EMIC waves over the entire magnetosphere throughout the different storm phases. In this study, we present the simulation results, which are based on two coupled RC models that our group has developed. The first model deals with the large-scale magnetosphere-ionosphere electrodynamic coupling, and provides a self-consistent description of RC ions/electrons and the magnetospheric electric field. The second model is based on a coupled system of two kinetic equations, one equation describes the RC ion dynamics and another equation describes the power spectral density evolution of EMIC waves, and self-consistently treats a micro-scale electrodynamic coupling of RC and EMIC waves. So far, these two models have been applied independently. However, the large-scale magnetosphere-ionosphere electrodynamics controls the convective patterns of both the RC ions and plasmasphere altering conditions for EMIC wave-particle interaction. In turn, the wave induced RC precipitation Changes the local field-aligned current

  7. Non-linear resonant coupling of tsunami edge waves using stochastic earthquake source models

    USGS Publications Warehouse

    Geist, Eric L.

    2016-01-01

    Non-linear resonant coupling of edge waves can occur with tsunamis generated by large-magnitude subduction zone earthquakes. Earthquake rupture zones that straddle beneath the coastline of continental margins are particularly efficient at generating tsunami edge waves. Using a stochastic model for earthquake slip, it is shown that a wide range of edge-wave modes and wavenumbers can be excited, depending on the variability of slip. If two modes are present that satisfy resonance conditions, then a third mode can gradually increase in amplitude over time, even if the earthquake did not originally excite that edge-wave mode. These three edge waves form a resonant triad that can cause unexpected variations in tsunami amplitude long after the first arrival. An M ∼ 9, 1100 km-long continental subduction zone earthquake is considered as a test case. For the least-variable slip examined involving a Gaussian random variable, the dominant resonant triad includes a high-amplitude fundamental mode wave with wavenumber associated with the along-strike dimension of rupture. The two other waves that make up this triad include subharmonic waves, one of fundamental mode and the other of mode 2 or 3. For the most variable slip examined involving a Cauchy-distributed random variable, the dominant triads involve higher wavenumbers and modes because subevents, rather than the overall rupture dimension, control the excitation of edge waves. Calculation of the resonant period for energy transfer determines which cases resonant coupling may be instrumentally observed. For low-mode triads, the maximum transfer of energy occurs approximately 20–30 wave periods after the first arrival and thus may be observed prior to the tsunami coda being completely attenuated. Therefore, under certain circumstances the necessary ingredients for resonant coupling of tsunami edge waves exist, indicating that resonant triads may be observable and implicated in late, large-amplitude tsunami arrivals.

  8. US Drought-Heat Wave Relationships in Past Versus Current Climates

    NASA Astrophysics Data System (ADS)

    Cheng, L.; Hoerling, M. P.; Eischeid, J.; Liu, Z.

    2017-12-01

    This study explores the relationship between droughts and heat waves over various regions of the contiguous United States that are distinguished by so-called energy-limited versus water-limited climatologies. We first examine the regional sensitivity of heat waves to soil moisture variability under 19th century climate conditions, and then compare to sensitivities under current climate that has been subjected to human-induced change. Our approach involves application of the conditional statistical framework of vine copula. Vine copula is known for its flexibility in reproducing various dependence structures exhibited by climate variables. Here we highlight its feature for evaluating the importance of conditional relationships between variables and processes that capture underlying physical factors involved in their interdependence during drought/heat waves. Of particular interest is identifying changes in coupling strength between heat waves and land surface conditions that may yield more extreme events as a result of land surface feedbacks. We diagnose two equilibrium experiments a coupled climate model (CESM1), one subjected to Year-1850 external forcing and the other to Year-2000 radiative forcing. We calculate joint heat wave/drought relationships for each climate state, and also calculate their change as a result of external radiative forcing changes across this 150-yr period. Our results reveal no material change in the dependency between heat waves and droughts, aside from small increases in coupling strength over the Great Plains. Overall, hot U.S. summer droughts of 1850-vintage do not become hotter in the current climate -- aside from the warming contribution of long-term climate change, in CESM1. The detectability of changes in hotter droughts as a consequence of anthropogenic forced changes in this single effect, i.e. coupling strength between soil moisture and hot summer temperature, is judged to be low at this time.

  9. A New Coupled Ocean-Waves-Atmosphere Model Designed for Tropical Storm Studies: Example of Tropical Cyclone Bejisa (2013-2014) in the South-West Indian Ocean

    NASA Astrophysics Data System (ADS)

    Pianezze, J.; Barthe, C.; Bielli, S.; Tulet, P.; Jullien, S.; Cambon, G.; Bousquet, O.; Claeys, M.; Cordier, E.

    2018-03-01

    Ocean-Waves-Atmosphere (OWA) exchanges are not well represented in current Numerical Weather Prediction (NWP) systems, which can lead to large uncertainties in tropical cyclone track and intensity forecasts. In order to explore and better understand the impact of OWA interactions on tropical cyclone modeling, a fully coupled OWA system based on the atmospheric model Meso-NH, the oceanic model CROCO, and the wave model WW3 and called MSWC was designed and applied to the case of tropical cyclone Bejisa (2013-2014). The fully coupled OWA simulation shows good agreement with the literature and available observations. In particular, simulated significant wave height is within 30 cm of measurements made with buoys and altimeters. Short-term (< 2 days) sensitivity experiments used to highlight the effect of oceanic waves coupling show limited impact on the track, the intensity evolution, and the turbulent surface fluxes of the tropical cyclone. However, it is also shown that using a fully coupled OWA system is essential to obtain consistent sea salt emissions. Spatial and temporal coherence of the sea state with the 10 m wind speed are necessary to produce sea salt aerosol emissions in the right place (in the eyewall of the tropical cyclone) and with the right size distribution, which is critical for cloud microphysics.

  10. Initial results from a dynamic coupled magnetosphere-ionosphere-ring current model

    NASA Astrophysics Data System (ADS)

    Pembroke, Asher; Toffoletto, Frank; Sazykin, Stanislav; Wiltberger, Michael; Lyon, John; Merkin, Viacheslav; Schmitt, Peter

    2012-02-01

    In this paper we describe a coupled model of Earth's magnetosphere that consists of the Lyon-Fedder-Mobarry (LFM) global magnetohydrodynamics (MHD) simulation, the MIX ionosphere solver and the Rice Convection Model (RCM) and report some results using idealized inputs and model parameters. The algorithmic and physical components of the model are described, including the transfer of magnetic field information and plasma boundary conditions to the RCM and the return of ring current plasma properties to the LFM. Crucial aspects of the coupling include the restriction of RCM to regions where field-line averaged plasma-β ≤ 1, the use of a plasmasphere model, and the MIX ionosphere model. Compared to stand-alone MHD, the coupled model produces a substantial increase in ring current pressure and reduction of the magnetic field near the Earth. In the ionosphere, stronger region-1 and region-2 Birkeland currents are seen in the coupled model but with no significant change in the cross polar cap potential drop, while the region-2 currents shielded the low-latitude convection potential. In addition, oscillations in the magnetic field are produced at geosynchronous orbit with the coupled code. The diagnostics of entropy and mass content indicate that these oscillations are associated with low-entropy flow channels moving in from the tail and may be related to bursty bulk flows and bubbles seen in observations. As with most complex numerical models, there is the ongoing challenge of untangling numerical artifacts and physics, and we find that while there is still much room for improvement, the results presented here are encouraging.

  11. Effects of wave-current interaction on storm surge in the Taiwan Strait: Insights from Typhoon Morakot

    NASA Astrophysics Data System (ADS)

    Yu, Xiaolong; Pan, Weiran; Zheng, Xiangjing; Zhou, Shenjie; Tao, Xiaoqin

    2017-08-01

    The effects of wave-current interaction on storm surge are investigated by a two-dimensional wave-current coupling model through simulations of Typhoon Morakot in the Taiwan Strait. The results show that wind wave and slope of sea floor govern wave setup modulations within the nearshore surf zone. Wave setup during Morakot can contribute up to 24% of the total storm surge with a maximum value of 0.28 m. The large wave setup commonly coincides with enhanced radiation stress gradient, which is itself associated with transfer of wave momentum flux. Water levels are to leading order in modulating significant wave height inside the estuary. High water levels due to tidal change and storm surge stabilize the wind wave and decay wave breaking. Outside of the estuary, waves are mainly affected by the current-induced modification of wind energy input to the wave generation. By comparing the observed significant wave height and water level with the results from uncoupled and coupled simulations, the latter shows a better agreement with the observations. It suggests that wave-current interaction plays an important role in determining the extreme storm surge and wave height in the study area and should not be neglected in a typhoon forecast.

  12. Modelling rogue waves through exact dynamical lump soliton controlled by ocean currents.

    PubMed

    Kundu, Anjan; Mukherjee, Abhik; Naskar, Tapan

    2014-04-08

    Rogue waves are extraordinarily high and steep isolated waves, which appear suddenly in a calm sea and disappear equally fast. However, though the rogue waves are localized surface waves, their theoretical models and experimental observations are available mostly in one dimension, with the majority of them admitting only limited and fixed amplitude and modular inclination of the wave. We propose two dimensions, exactly solvable nonlinear Schrödinger (NLS) equation derivable from the basic hydrodynamic equations and endowed with integrable structures. The proposed two-dimensional equation exhibits modulation instability and frequency correction induced by the nonlinear effect, with a directional preference, all of which can be determined through precise analytic result. The two-dimensional NLS equation allows also an exact lump soliton which can model a full-grown surface rogue wave with adjustable height and modular inclination. The lump soliton under the influence of an ocean current appears and disappears preceded by a hole state, with its dynamics controlled by the current term. These desirable properties make our exact model promising for describing ocean rogue waves.

  13. Modelling rogue waves through exact dynamical lump soliton controlled by ocean currents

    PubMed Central

    Kundu, Anjan; Mukherjee, Abhik; Naskar, Tapan

    2014-01-01

    Rogue waves are extraordinarily high and steep isolated waves, which appear suddenly in a calm sea and disappear equally fast. However, though the rogue waves are localized surface waves, their theoretical models and experimental observations are available mostly in one dimension, with the majority of them admitting only limited and fixed amplitude and modular inclination of the wave. We propose two dimensions, exactly solvable nonlinear Schrödinger (NLS) equation derivable from the basic hydrodynamic equations and endowed with integrable structures. The proposed two-dimensional equation exhibits modulation instability and frequency correction induced by the nonlinear effect, with a directional preference, all of which can be determined through precise analytic result. The two-dimensional NLS equation allows also an exact lump soliton which can model a full-grown surface rogue wave with adjustable height and modular inclination. The lump soliton under the influence of an ocean current appears and disappears preceded by a hole state, with its dynamics controlled by the current term. These desirable properties make our exact model promising for describing ocean rogue waves. PMID:24711719

  14. Self-Consistent Model of Magnetospheric Ring Current and Propagating Electromagnetic Ion Cyclotron Waves: Waves in Multi-Ion Magnetosphere

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gamayunov, K. V.; Gallagher, D. L.; Kozyra, J. U.

    2006-01-01

    The further development of a self-consistent theoretical model of interacting ring current ions and electromagnetic ion cyclotron waves (Khazanov et al., 2003) is presented In order to adequately take into account wave propagation and refraction in a multi-ion magnetosphere, we explicitly include the ray tracing equations in our previous self-consistent model and use the general form of the wave kinetic equation. This is a major new feature of the present model and, to the best of our knowledge, the ray tracing equations for the first time are explicitly employed on a global magnetospheric scale in order to self-consistently simulate the spatial, temporal, and spectral evolution of the ring current and of electromagnetic ion cyclotron waves To demonstrate the effects of EMIC wave propagation and refraction on the wave energy distribution and evolution, we simulate the May 1998 storm. The main findings of our simulation can be summarized as follows. First, owing to the density gradient at the plasmapause, the net wave refraction is suppressed, and He+-mode grows preferably at the plasmapause. This result is in total agreement with previous ray tracing studies and is very clearly found in presented B field spectrograms. Second, comparison of global wave distributions with the results from another ring current model (Kozyra et al., 1997) reveals that this new model provides more intense and more highly plasmapause-organized wave distributions during the May 1998 storm period Finally, it is found that He(+)-mode energy distributions are not Gaussian distributions and most important that wave energy can occupy not only the region of generation, i.e., the region of small wave normal angles, but all wave normal angles, including those to near 90 . The latter is extremely crucial for energy transfer to thermal plasmaspheric electrons by resonant Landau damping and subsequent downward heat transport and excitation of stable auroral red arcs.

  15. Wave-current interactions at the FloWave Ocean Energy Research Facility

    NASA Astrophysics Data System (ADS)

    Noble, Donald; Davey, Thomas; Steynor, Jeffrey; Bruce, Tom; Smith, Helen; Kaklis, Panagiotis

    2015-04-01

    Physical scale model testing is an important part of the marine renewable energy development process, allowing the study of forces and device behaviour in a controlled environment prior to deployment at sea. FloWave is a new state-of-the-art ocean energy research facility, designed to provide large scale physical modelling services to the tidal and wave sector. It has the unique ability to provide complex multi-directional waves that can be combined with currents from any direction in the 25m diameter circular tank. The facility is optimised for waves around 2s period and 0.4m height, and is capable of generating currents upwards of 1.6m/s. This offers the ability to model metocean conditions suitable for most renewable energy devices at a typical scale of between 1:10 and 1:40. The test section is 2m deep, which can be classed as intermediate-depth for most waves of interest, thus the full dispersion equation must be solved as the asymptotic simplifications do not apply. The interaction between waves and currents has been studied in the tank. This has involved producing in the tank sets of regular waves, focussed wave groups, and random sea spectra including multi-directional sea states. These waves have been both inline-with and opposing the current, as well as investigating waves at arbitrary angles to the current. Changes in wave height and wavelength have been measured, and compared with theoretical results. Using theoretical wave-current interaction models, methods have been explored to "correct" the wave height in the central test area of the tank when combined with a steady current. This allows the wave height with current to be set equal to that without a current. Thus permitting, for example, direct comparison of device motion response between tests with and without current. Alternatively, this would also permit a specific wave height and current combination to be produced in the tank, reproducing recorded conditions at a particular site of interest. The

  16. Reply to "Comment on 'A Self-Consistent Model of the Interacting Ring Current Ions and Electromagnetic Ion Cyclotron Waves, Initial Results: Waves and Precipitation Fluxes' and 'Self-Consistent Model of the Magnetospheric Ring Current and Propagating Electromagnetic Ion Cyclotron Waves: Waves in Multi-Ion Magnetosphere' by Khazanov et al. et al."

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gamayunov, K. V.; Gallagher, D. L.; Kozyra, J. W.

    2007-01-01

    It is well-known that the effects of electromagnetic ion cyclotron (EMIC) waves on ring current (RC) ion and radiation belt (RB) electron dynamics strongly depend on such particle/wave characteristics as the phase-space distribution function, frequency, wavenormal angle, wave energy, and the form of wave spectral energy density. The consequence is that accurate modeling of EMIC waves and RC particles requires robust inclusion of the interdependent dynamics of wave growth/damping, wave propagation, and[ particles. Such a self-consistent model is being progressively developed by Khazanov et al. [2002, 2006, 2007]. This model is based on a system of coupled kinetic equations for the RC and EMIC wave power spectral density along with the ray tracing equations. Thome and Home [2007] (hereafter referred to as TH2007) call the Khazanov et al. [2002, 2006] results into question in their Comment. The points in contention can be summarized as follows. TH2007 claim that: (1) "the important damping of waves by thermal heavy ions is completely ignored", and Landau damping during resonant interaction with thermal electrons is not included in our model; (2) EMIC wave damping due to RC O + is not included in our simulation; (3) non-linear processes limiting EMIC wave amplitude are not included in our model; (4) growth of the background fluctuations to a physically significantamplitude"must occur during a single transit of the unstable region" with subsequent damping below bi-ion latitudes,and consequently"the bounce averaged wave kinetic equation employed in the code contains a physically erroneous 'assumption". Our reply will address each of these points as well as other criticisms mentioned in the Comment. TH2007 are focused on two of our papers that are separated by four years. Significant progress in the self-consistent treatment of the RC-EMIC wave system has been achieved during those years. The paper by Khazanov et al. [2006] presents the latest version of our model, and in

  17. Free and Convectively Coupled Equatorial Waves Simulated by CMIP5 Climate Models

    NASA Astrophysics Data System (ADS)

    Marques, Carlos A. F.; Castanheira, José M.

    2015-04-01

    It is well known that precipitation in the equatorial belt does not occur randomly, but is often organized into synoptic to planetary-scale disturbances with time scales smaller than a season. Several studies have shown that a large fraction of the convection variability in such disturbances is associated with dynamical Equatorial Waves, such as the Kelvin, Equatorial Rossby, Mixed Rossby-Gravity, Eastward and Westward Inertio-Gravity waves (e.g. Kiladis et al., Rev. Geophys., 2009). The horizontal structures and dispersion characteristics of such Convectively Coupled Equatorial Waves (CCEWs) correspond to the solutions of the shallow water (SW) equations on an equatorial β-plane obtained by Matsuno (J. Meteor. Soc. Japan, 1966). CCEWs have broad impacts within the tropics, but their simulation in general circulation models is still problematic. Using space-time spectral analyses of a proxy field for tropical convection (e.g. outgoing long wave radiation (OLR)), it has been shown the existence of spectral peaks aligned along the dispersion curves of equatorially trapped wave modes of SW theory, which have been interpreted as the effect of equatorial wave processes (e.g. Takayabu, J. Meteor. Soc. Japan, 1994; Wheeler and Kiladis, JAS, 1999). However, different equatorial modes may not be well separated in the wavenumber-frequency domain due to a vertical variation of the horizontal basic flow, that may introduce Doppler shiftings and changes in the vertical heating profiles which may distort the theoretical dispersion curves (Yang et al., JAS, 2003). In this communication, we present a new methodology for the diagnosis of CCEWs, which is based on a pre-filtering of the geopotential and horizontal wind, via three-dimensional (3-D) normal mode functions of the adiabatic linearized equations of a resting atmosphere, followed by a space-time power and cross spectral analysis applied to the 3-D normal mode filtered fields and the OLR (or other fields that may be proxies

  18. Inductive-dynamic magnetosphere-ionosphere coupling via MHD waves

    NASA Astrophysics Data System (ADS)

    Tu, Jiannan; Song, Paul; Vasyliūnas, Vytenis M.

    2014-01-01

    In the present study, we investigate magnetosphere-ionosphere/thermosphere (M-IT) coupling via MHD waves by numerically solving time-dependent continuity, momentum, and energy equations for ions and neutrals, together with Maxwell's equations (Ampère's and Faraday's laws) and with photochemistry included. This inductive-dynamic approach we use is fundamentally different from those in previous magnetosphere-ionosphere (M-I) coupling models: all MHD wave modes are retained, and energy and momentum exchange between waves and plasma are incorporated into the governing equations, allowing a self-consistent examination of dynamic M-I coupling. Simulations, using an implicit numerical scheme, of the 1-D ionosphere/thermosphere system responding to an imposed convection velocity at the top boundary are presented to show how magnetosphere and ionosphere are coupled through Alfvén waves during the transient stage when the IT system changes from one quasi steady state to another. Wave reflection from the low-altitude ionosphere plays an essential role, causing overshoots and oscillations of ionospheric perturbations, and the dynamical Hall effect is an inherent aspect of the M-I coupling. The simulations demonstrate that the ionosphere/thermosphere responds to magnetospheric driving forces as a damped oscillator.

  19. The Nonlinear Coupling of Electromagnetic Ion Cyclotron and Lower Hybrid Waves in the Ring Current Region: The Magnetic Storm May 1-7 1998

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Krivorutsky, E.; Gamayunov, K.; Avanov, L.

    2003-01-01

    The excitation of lower hybrid waves (LHWs) is a widely discussed mechanism of interaction between plasma species in space, and is one of the unresolved questions of magnetospheric multi-ion plasmas. In this paper we present the morphology, dynamics, and level of LHW activity generated by electromagnetic ion cyclotron (EMIC) waves during the May 2-7, 1998 storm period on the global scale. The LHWs were calculated based on our newly developed self-consistent model that couples the system of two kinetic equations: one equation describes the ring current (RC) ion dynamic, and another equation describes the evolution of EMIC waves. It is found that the LHWs are excited by helium ions due to their mass dependent drift in the electric field of EMIC waves. The level of LHW activity is calculated assuming that the induced scattering process is the main saturation mechanism for these waves. The calculated LHWs electric fields are consistent with the observational data.

  20. Nonlinear transient waves in coupled phase oscillators with inertia.

    PubMed

    Jörg, David J

    2015-05-01

    Like the inertia of a physical body describes its tendency to resist changes of its state of motion, inertia of an oscillator describes its tendency to resist changes of its frequency. Here, we show that finite inertia of individual oscillators enables nonlinear phase waves in spatially extended coupled systems. Using a discrete model of coupled phase oscillators with inertia, we investigate these wave phenomena numerically, complemented by a continuum approximation that permits the analytical description of the key features of wave propagation in the long-wavelength limit. The ability to exhibit traveling waves is a generic feature of systems with finite inertia and is independent of the details of the coupling function.

  1. A coupled DEM-CFD method for impulse wave modelling

    NASA Astrophysics Data System (ADS)

    Zhao, Tao; Utili, Stefano; Crosta, GiovanBattista

    2015-04-01

    Rockslides can be characterized by a rapid evolution, up to a possible transition into a rock avalanche, which can be associated with an almost instantaneous collapse and spreading. Different examples are available in the literature, but the Vajont rockslide is quite unique for its morphological and geological characteristics, as well as for the type of evolution and the availability of long term monitoring data. This study advocates the use of a DEM-CFD framework for the modelling of the generation of hydrodynamic waves due to the impact of a rapid moving rockslide or rock-debris avalanche. 3D DEM analyses in plane strain by a coupled DEM-CFD code were performed to simulate the rockslide from its onset to the impact with still water and the subsequent wave generation (Zhao et al., 2014). The physical response predicted is in broad agreement with the available observations. The numerical results are compared to those published in the literature and especially to Crosta et al. (2014). According to our results, the maximum computed run up amounts to ca. 120 m and 170 m for the eastern and western lobe cross sections, respectively. These values are reasonably similar to those recorded during the event (i.e. ca. 130 m and 190 m respectively). In these simulations, the slope mass is considered permeable, such that the toe region of the slope can move submerged in the reservoir and the impulse water wave can also flow back into the slope mass. However, the upscaling of the grains size in the DEM model leads to an unrealistically high hydraulic conductivity of the model, such that only a small amount of water is splashed onto the northern bank of the Vajont valley. The use of high fluid viscosity and coarse grain model has shown the possibility to model more realistically both the slope and wave motions. However, more detailed slope and fluid properties, and the need for computational efficiency should be considered in future research work. This aspect has also been

  2. Self-Consistent Model of Magnetospheric Ring Current and Propagating Electromagnetic Ion Cyclotron Waves. 1; Waves in Multi Ion Magnetosphere

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gumayunov, K. V.; Gallagher, D. L.; Kozyra, J. U.

    2006-01-01

    The further development of a self-consistent theoretical model of interacting ring current ions and electromagnetic ion cyclotron waves [Khazanov et al., 2003] is presented. In order to adequately take into account the wave propagation and refraction in a multi-ion plasmasphere, we explicitly include the ray tracing equations in our previous self-consistent model and use the general form of the wave kinetic equation. This is a major new feature of the present model and, to the best of our knowledge, the ray tracing equations for the first time are explicitly employed on a global magnetospheric scale in order to self-consistently simulate spatial, temporal, and spectral evolutions of the ring current and electromagnetic ion cyclotron waves. To demonstrate the effects of EMIC wave propagation and refraction on the EMIC wave energy distributions and evolution we simulate the May 1998 storm. The main findings of our simulation can be summarized as follows. First, due to the density gradient at the plasmapause, the net wave refraction is suppressed, and He(+)-mode grows preferably at plasmapause. This result is in a total agreement with the previous ray tracing studies, and very clear observed in presented B-field spectrograms. Second, comparison the global wave distributions with the results from other ring current model [Kozyra et al., 1997] reveals that our model provides more intense and higher plasmapause organized distributions during the May, 1998 storm period. Finally, the found He(+)-mode energy distributions are not Gaussian distributions, and most important that wave energy can occupy not only the region of generation, i. e. the region of small wave normal angles, but the entire wave normal angle region and even only the region near 90 degrees. The latter is extremely crucial for energy transfer to thermal plasmaspheric electrons by resonant Landau damping, and subsequent downward heat transport and excitation of stable auroral red arcs.

  3. Self-consistent Model of Magnetospheric Ring Current and Propagating Electromagnetic Ion Cyclotron Waves. 2. Wave Induced Ring Current Precipitation and Thermal Electron Heating

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gamayunov, K. V.; Gallagher, D. L.; Kozyra, J. U.; Liemohn, M. W.

    2007-01-01

    This paper continues presentation and discussion of the results from our new global self-consistent theoretical model of interacting ring current ions and propagating electromagnetic ion cyclotron waves [Khazanov et al., 2006]. To study the effects of electromagnetic ion cyclotron wave propagation and refraction on the wave induced ring current precipitation and heating of the thermal plasmaspheric electrons, we simulate the May 1998 storm. The main findings after a simulation can be summarized as follows. Firstly, the wave induced ring current precipitation exhibits quite a lot of fine structure, and is highly organized by location of the plasmapause gradient. The strongest fluxes of about 4 x 10(exp 6) (cm(raised dot) s(raised dot) sr(raised dot) (sup -1)) are observed during the maill and early recovery phases of the storm. The very interesting and probably more important finding is that in a number of cases the most intense precipitating fluxes are not connected to the most intense waves in simple manner. The characteristics of the wave power spectral density distribution over the wave normal angle are extremely crucial for the effectiveness of the ring current ion scattering. Secondly, comparison of the global proton precipitating patterns with the results from RAM [Kozyra et al., 1997a] reveals that although we observe a qualitative agreement between the localizations of the wave induced precipitations in the models, there is no quantitative agreement between the magnitudes of the fluxes. The quantitative differences are mainly due to a qualitative difference between the characteristics of the wave power spectral density distributions over the wave normal angle in RAM and in our model. Thirdly, the heat fluxes to plasmaspheric electrons caused by Landau resonate energy absorption from electromagnetic ion cyclotron waves are observed in the postnoon-premidnight MLT sector, and can reach the magnitude of 10(exp 11) eV/(cm(sup 2)(raised dot)s). The Coulomb

  4. Three-dimensional wave-induced current model equations and radiation stresses

    NASA Astrophysics Data System (ADS)

    Xia, Hua-yong

    2017-08-01

    After the approach by Mellor (2003, 2008), the present paper reports on a repeated effort to derive the equations for three-dimensional wave-induced current. Via the vertical momentum equation and a proper coordinate transformation, the phase-averaged wave dynamic pressure is well treated, and a continuous and depth-dependent radiation stress tensor, rather than the controversial delta Dirac function at the surface shown in Mellor (2008), is provided. Besides, a phase-averaged vertical momentum flux over a sloping bottom is introduced. All the inconsistencies in Mellor (2003, 2008), pointed out by Ardhuin et al. (2008) and Bennis and Ardhuin (2011), are overcome in the presently revised equations. In a test case with a sloping sea bed, as shown in Ardhuin et al. (2008), the wave-driving forces derived in the present equations are in good balance, and no spurious vertical circulation occurs outside the surf zone, indicating that Airy's wave theory and the approach of Mellor (2003, 2008) are applicable for the derivation of the wave-induced current model.

  5. A Linearized Model for Wave Propagation through Coupled Volcanic Conduit-crack Systems Filled with Multiphase Magma

    NASA Astrophysics Data System (ADS)

    Liang, C.; Dunham, E. M.; OReilly, O. J.; Karlstrom, L.

    2015-12-01

    Both the oscillation of magma in volcanic conduits and resonance of fluid-filled cracks (dikes and sills) are appealing explanations for very long period signals recorded at many active volcanoes. While these processes have been studied in isolation, real volcanic systems involve interconnected networks of conduits and cracks. The overall objective of our work is to develop a model of wave propagation and ultimately eruptive fluid dynamics through this coupled system. Here, we present a linearized model for wave propagation through a conduit with multiple cracks branching off of it. The fluid is compressible and viscous, and is comprised of a mixture of liquid melt and gas bubbles. Nonequilibrium bubble growth and resorption (BGR) is quantified by introducing a time scale for mass exchange between phases, following the treatment in Karlstrom and Dunham (2015). We start by deriving the dispersion relation for crack waves travelling along the multiphase-magma-filled crack embedded in an elastic solid. Dissipation arises from magma viscosity, nonequilibrium BGR, and radiation of seismic waves into the solid. We next introduce coupling conditions between the conduit and crack, expressing conservation of mass and the balance of forces across the junction. Waves in the conduit, like those in the crack, are influenced by nonequilibrium BGR, but the deformability of the surrounding solid is far less important than for cracks. Solution of the coupled system of equations provides the evolution of pressure and fluid velocity within the conduit-crack system. The system has various resonant modes that are sensitive to fluid properties and to the geometry of the conduit and cracks. Numerical modeling of seismic waves in the solid allows us to generate synthetic seismograms.

  6. A Self-Consistent Model of the Interacting Ring Current Ions and Electromagnetic Ion Cyclotron Waves, Initial Results: Waves and Precipitating Fluxes

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gamayunov, K. V.; Jordanova, V. K.; Krivorutsky, E. N.

    2002-01-01

    Initial results from a newly developed model of the interacting ring current ions and ion cyclotron waves are presented. The model is based on the system of two kinetic equations: one equation describes the ring current ion dynamics, and another equation describes wave evolution. The system gives a self-consistent description of the ring current ions and ion cyclotron waves in a quasilinear approach. These equations for the ion phase space distribution function and for the wave power spectral density were solved on aglobal magnetospheric scale undernonsteady state conditions during the 2-5 May 1998 storm. The structure and dynamics of the ring current proton precipitating flux regions and the ion cyclotron wave-active zones during extreme geomagnetic disturbances on 4 May 1998 are presented and discussed in detail.

  7. ICRF fast wave current drive and mode conversion current drive in EAST tokamak

    NASA Astrophysics Data System (ADS)

    Yin, L.; Yang, C.; Gong, X. Y.; Lu, X. Q.; Du, D.; Chen, Y.

    2017-10-01

    Fast wave in the ion-cyclotron resonance frequency (ICRF) range is a promising candidate for non-inductive current drive (CD), which is essential for long pulse and high performance operation of tokamaks. A numerical study on the ICRF fast wave current drive (FWCD) and mode-conversion current drive (MCCD) in the Experimental Advanced Superconducting Tokamak (EAST) is carried out by means of the coupled full wave and Ehst-Karney parameterization methods. The results show that FWCD efficiency is notable in two frequency regimes, i.e., f ≥ 85 MHz and f = 50-65 MHz, where ion cyclotron absorption is effectively avoided, and the maximum on-axis driven current per unit power can reach 120 kA/MW. The sensitivity of the CD efficiency to the minority ion concentration is confirmed, owing to fast wave mode conversion, and the peak MCCD efficiency is reached for 22% minority-ion concentration. The effects of the wave-launch position and the toroidal wavenumber on the efficiency of current drive are also investigated.

  8. Mode-coupling and wave-particle interactions for unstable ion-acoustic waves.

    NASA Technical Reports Server (NTRS)

    Martin, P.; Fried, B. D.

    1972-01-01

    A theory for the spatial development of linearly unstable, coupled waves is presented in which both quasilinear and mode-coupling effects are treated in a self-consistent manner. Steady-state excitation of two waves is assumed at the boundary x = 0, the plasma being homogeneous in the y and z directions. Coupled equations are derived for the x dependence of the amplitudes of the primary waves and the secondary waves, correct through terms of second order in the wave amplitude, but without the usual approximation of small growth rates. This general formalism is then applied to the case of coupled ion-acoustic waves driven unstable by an ion beam streaming in the direction of the x axis. If the modifications of the ion beam by the waves (quasilinear effects) are ignored, explosive instabilities (singularities in all of the amplitudes at finite x) are found even when all of the waves have positive energy. If these wave-particle interactions are included, the solutions are no longer singular, and all of the amplitudes have finite maxima.

  9. Mode coupling and wave particle interactions for unstable ion acoustic waves

    NASA Technical Reports Server (NTRS)

    Martin, P.; Fried, B. D.

    1972-01-01

    A theory for the spatial development of linearly unstable, coupled waves is presented in which both quasi-linear and mode coupling effects are treated in a self-consistent manner. Steady state excitation of two waves is assumed at the boundary x = 0, the plasma being homogeneous in the y and z directions. Coupled equations are derived for the x dependence of the amplitudes of the primary waves and the secondary waves, correct through second order terms in the wave amplitude, but without usual approximation of small growth rates. This general formalism is then applied to the case of coupled ion acoustic waves driven unstable by an ion beam streaming in the direction of the x axis. If the modifications of the ion beam by the waves (quasi-linear effects) are ignored, explosive instabilities (singularities in all of the amplitudes at finite x) are found, even when all of the waves have positive energy. If these wave-particle interactions are included, the solutions are no longer singular, and all of the amplitudes have finite maxima.

  10. Rg-Lg coupling as a Lg-wave excitation mechanism

    NASA Astrophysics Data System (ADS)

    Ge, Z.; Xie, X.

    2003-12-01

    Regional phase Lg is predominantly comprised of shear wave energy trapped in the crust. Explosion sources are expected to be less efficient for excitation of Lg phases than earthquakes to the extent that the source can be approximated as isotropic. Shallow explosions generate relatively large surface wave Rg compared to deeper earthquakes, and Rg is readily disrupted by crustal heterogeneity. Rg energy may thus scatter into trapped crustal S-waves near the source region and contribute to low-frequency Lg wave. In this study, a finite-difference modeling plus the slowness analysis are used for investigating the above mentioned Lg-wave excitation mechanism. The method allows us to investigate near source energy partitioning in multiple domains including frequency, slowness and time. The main advantage of this method is that it can be applied at close range, before Lg is actually formed, which allows us to use very fine near source velocity model to simulate the energy partitioning process. We use a layered velocity structure as the background model and add small near source random velocity patches to the model to generate the Rg to Lg coupling. Two types of simulations are conducted, (1) a fixed shallow explosion source vs. randomness at different depths and (2) a fixed shallow randomness vs. explosion sources at different depths. The results show apparent couplings between the Rg and Lg waves at lower frequencies (0.3-1.5 Hz). A shallow source combined with shallow randomness generates the maximum Lg-wave, which is consistent with the Rg energy distribution of a shallow explosion source. The Rg energy and excited Lg energy show a near linear relationship. The numerical simulation and slowness analysis suggest that the Rg to Lg coupling is an effective excitation mechanism for low frequency Lg-waves from a shallow explosion source.

  11. An Arctic Ice/Ocean Coupled Model with Wave Interactions

    DTIC Science & Technology

    2013-09-30

    motion in the presence of currents and waves. In the wave attenuation experiments, between 35 and 80 ‘ice floes’ (0.99 m diameter wooden disks) were...moored with springs to the tank floor and plane waves were sent down, with an array of wave probes to measure the reflected and transmitted waves...waves propagating in the MIZ as opposed to the acoustic wave solution shown. This outcome offers significant new capabilities for tracking fully

  12. Coupling of wave and circulation models in coastal-ocean predicting systems: A case study for the German Bight

    NASA Astrophysics Data System (ADS)

    Staneva, Joanna; Wahle, Kathrin

    2015-04-01

    This study addresses the coupling between wind wave and circulation models on the example of the German Bight and its coastal area called the Wadden Sea (the area between the barrier islands and the coast). This topic reflects the increased interest in operational oceanography to reduce prediction errors of state estimates at coastal scales. The uncertainties in most of the presently used models result from the nonlinear feedback between strong tidal currents and wind-waves, which can no longer be ignored, in particular in the coastal zone where its role seems to be dominant. A nested modelling system is used in the Helmholtz-Zentrum Geesthacht to producing reliable now- and short-term forecasts of ocean state variables, including wind waves and hydrodynamics. In this study we present analysis of wave and hydrographic observations, as well as the results of numerical simulations. The data base includes ADCP observations and continuous measurements from data stations. The individual and collective role of wind, waves and tidal forcing are quantified. The performance of the forecasting system is illustrated for the cases of several extreme events. Effects of ocean waves on coastal circulation and SST simulations are investigated considering wave-dependent stress and wave breaking parameterization during extreme events, e.g. hurricane Xavier in December, 2013. Also the effect which the circulation exerts on the wind waves is tested for the coastal areas using different parameterizations. The improved skill resulting from the new developments in the forecasting system, in particular during extreme events, justifies further enhancements of the coastal pre-operational system for the North Sea and German Bight.

  13. Regional Wave Climates along Eastern Boundary Currents

    NASA Astrophysics Data System (ADS)

    Semedo, Alvaro; Soares, Pedro

    2016-04-01

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

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

    DTIC Science & Technology

    2017-06-30

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

  15. Ocean-atmosphere dynamics during Hurricane Ida and Nor'Ida: An application of the coupled ocean-atmosphere-wave-sediment transport (COAWST) modeling system

    USGS Publications Warehouse

    Olabarrieta, Maitane; Warner, John C.; Armstrong, Brandy N.; Zambon, Joseph B.; He, Ruoying

    2012-01-01

    The coupled ocean–atmosphere–wave–sediment transport (COAWST) modeling system was used to investigate atmosphere–ocean–wave interactions in November 2009 during Hurricane Ida and its subsequent evolution to Nor’Ida, which was one of the most costly storm systems of the past two decades. One interesting aspect of this event is that it included two unique atmospheric extreme conditions, a hurricane and a nor’easter storm, which developed in regions with different oceanographic characteristics. Our modeled results were compared with several data sources, including GOES satellite infrared data, JASON-1 and JASON-2 altimeter data, CODAR measurements, and wave and tidal information from the National Data Buoy Center (NDBC) and the National Tidal Database. By performing a series of numerical runs, we were able to isolate the effect of the interaction terms between the atmosphere (modeled with Weather Research and Forecasting, the WRF model), the ocean (modeled with Regional Ocean Modeling System (ROMS)), and the wave propagation and generation model (modeled with Simulating Waves Nearshore (SWAN)). Special attention was given to the role of the ocean surface roughness. Three different ocean roughness closure models were analyzed: DGHQ (which is based on wave age), TY2001 (which is based on wave steepness), and OOST (which considers both the effects of wave age and steepness). Including the ocean roughness in the atmospheric module improved the wind intensity estimation and therefore also the wind waves, surface currents, and storm surge amplitude. For example, during the passage of Hurricane Ida through the Gulf of Mexico, the wind speeds were reduced due to wave-induced ocean roughness, resulting in better agreement with the measured winds. During Nor’Ida, including the wave-induced surface roughness changed the form and dimension of the main low pressure cell, affecting the intensity and direction of the winds. The combined wave age- and wave steepness

  16. Activity of convective coupled equatorial wave in tropical Tropopause layer in reanalysis and high-top CMIP5 models

    NASA Astrophysics Data System (ADS)

    Harza, Alia; Lubis, Sandro W.; Setiawan, Sonni

    2018-05-01

    The activity of convectively coupled equatorial waves (CCEWs), including Kelvin waves, Mixed Rossby-Gravity (MRG), and Equatorial Rossby (ER), in the tropical tropopause layer (TTL) is investigated in the Reanalysis and nine high-top CMIP5 models using the zonal wave number-frequency spectral analysis with equatorially symmetric-antisymmetric decomposition. We found that the TTL activities in the high-top CMIP5 models show significant difference among the high-top CMIP5 models with respect to the observation. The MIROC and HadGEM2-CC models work best in simulating Kelvin wave in the TTL, while the HadGEM2-CC and MPI-ESM-LR models work best in simulating MRG waves. The ER waves in TTL are best simulated in the MRI-CGCM model. None of the models are good in simulating all waves at once. It is concluded that the broad range of wave activity found in the different CMIP5 models depend on the convective parameterization used by each model and the representation of the tropical stratosphere variability, including the QBO.

  17. Spiral waves in driven strongly coupled Yukawa systems

    NASA Astrophysics Data System (ADS)

    Kumar, Sandeep; Das, Amita

    2018-06-01

    Spiral wave formations are ubiquitous in nature. In the present paper, the excitation of spiral waves in the context of driven two-dimensional dusty plasma (Yukawa system) has been demonstrated at particle level using molecular-dynamics simulations. The interaction amidst dust particles is modeled by the Yukawa potential to take account of the shielding of dust charges by the lighter electron and ion species. The spatiotemporal evolution of these spiral waves has been characterized as a function of the frequency and amplitude of the driving force and dust neutral collisions. The effect of strong coupling has been studied, which shows that the excited spiral wave structures get clearer as the medium gets more strongly coupled. The radial propagation speed of the spiral wave is observed to remain unaltered with the coupling parameter. However, it is found to depend on the screening parameter of the dust medium and decreases when it is increased. In the crystalline phase (with screening parameter κ >0.58 ), the spiral wavefronts are shown to be hexagonal in shape. This shows that the radial propagation speed depends on the interparticle spacing.

  18. Evanescent wave coupling in terahertz waveguide arrays.

    PubMed

    Reichel, K S; Sakoda, N; Mendis, R; Mittleman, D M

    2013-07-15

    We study energy transfer among an array of identical finite-width parallel-plate waveguides in close proximity, via evanescent wave coupling of broadband terahertz waves. We observe stronger coupling with larger plate separations and longer propagation paths. This work establishes a platform to investigate new opportunities for THz components and devices based on evanescent wave coupling.

  19. Implementation of the vortex force formalism in the coupled ocean-atmosphere-wave-sediment transport (COAWST) modeling system for inner shelf and surf zone applications

    NASA Astrophysics Data System (ADS)

    Kumar, Nirnimesh; Voulgaris, George; Warner, John C.; Olabarrieta, Maitane

    The coupled ocean-atmosphere-wave-sediment transport modeling system (COAWST) enables simulations that integrate oceanic, atmospheric, wave and morphological processes in the coastal ocean. Within the modeling system, the three-dimensional ocean circulation module (ROMS) is coupled with the wave generation and propagation model (SWAN) to allow full integration of the effect of waves on circulation and vice versa. The existing wave-current coupling component utilizes a depth dependent radiation stress approach. In here we present a new approach that uses the vortex force formalism. The formulation adopted and the various parameterizations used in the model as well as their numerical implementation are presented in detail. The performance of the new system is examined through the presentation of four test cases. These include obliquely incident waves on a synthetic planar beach and a natural barred beach (DUCK' 94); normal incident waves on a nearshore barred morphology with rip channels; and wave-induced mean flows outside the surf zone at the Martha's Vineyard Coastal Observatory (MVCO). Model results from the planar beach case show good agreement with depth-averaged analytical solutions and with theoretical flow structures. Simulation results for the DUCK' 94 experiment agree closely with measured profiles of cross-shore and longshore velocity data from Garcez Faria et al. (1998, 2000). Diagnostic simulations showed that the nonlinear processes of wave roller generation and wave-induced mixing are important for the accurate simulation of surf zone flows. It is further recommended that a more realistic approach for determining the contribution of wave rollers and breaking induced turbulent mixing can be formulated using non-dimensional parameters which are functions of local wave parameters and the beach slope. Dominant terms in the cross-shore momentum balance are found to be the quasi-static pressure gradient and breaking acceleration. In the alongshore direction

  20. Wave scattering in spatially inhomogeneous currents

    NASA Astrophysics Data System (ADS)

    Churilov, Semyon; Ermakov, Andrei; Stepanyants, Yury

    2017-09-01

    We analytically study a scattering of long linear surface waves on stationary currents in a duct (canal) of constant depth and variable width. It is assumed that the background velocity linearly increases or decreases with the longitudinal coordinate due to the gradual variation of duct width. Such a model admits an analytical solution of the problem in hand, and we calculate the scattering coefficients as functions of incident wave frequency for all possible cases of sub-, super-, and transcritical currents. For completeness we study both cocurrent and countercurrent wave propagation in accelerating and decelerating currents. The results obtained are analyzed in application to recent analog gravity experiments and shed light on the problem of hydrodynamic modeling of Hawking radiation.

  1. Current-induced modulation of backward spin-waves in metallic microstructures

    NASA Astrophysics Data System (ADS)

    Sato, Nana; Lee, Seo-Won; Lee, Kyung-Jin; Sekiguchi, Koji

    2017-03-01

    We performed a propagating spin-wave spectroscopy for backward spin-waves in ferromagnetic metallic microstructures in the presence of electric-current. Even with the smaller current injection of 5× {{10}10} A m-2 into ferromagnetic microwires, the backward spin-waves exhibit a gigantic 200 MHz frequency shift and a 15% amplitude change, showing 60 times larger modulation compared to previous reports. Systematic experiments by measuring dependences on a film thickness of mirowire, on the wave-vector of spin-wave, and on the magnitude of bias field, we revealed that for the backward spin-waves a distribution of internal magnetic field generated by electric-current efficiently modulates the frequency and amplitude of spin-waves. The gigantic frequency and amplitude changes were reproduced by a micromagnetics simulation, predicting that the current-injection of 5× {{10}11} A m-2 allows 3 GHz frequency shift. The effective coupling between electric-current and backward spin-waves has a potential to build up a logic control method which encodes signals into the phase and amplitude of spin-waves. The metallic magnonics cooperating with electronics could suggest highly integrated magnonic circuits both in Boolean and non-Boolean principles.

  2. A coupled atmosphere-ocean-wave modeling approach for a Tropical Like Cyclone in the Mediterranean Sea

    NASA Astrophysics Data System (ADS)

    Ricchi, Antonio; Miglietta, M. Marcello; Barbariol, Francesco; Benetazzo, Alvise; Bonaldo, Davide; Falcieri, Francesco; Russo, Aniello; Sclavo, Mauro; Carniel, Sandro

    2016-04-01

    In November 6-8, 2011, in the Balearic islands an extra-tropical depression developed into a Tropical-Like Cyclone (TLC) characterized by a deep-warm core, leading to a mean sea level pressure minimum of about 991 hPa, 10 m wind speeds higher than 28 m/s around the eye, and very intense rainfall, especially in the Gulf of Lion. To explore in detail the effect of the sea surface temperature on the Medicane evolution, we employed the coupled modeling system COAWST, which consists of the ROMS model for the hydrodynamic part, the WRF model for the meteorological part, and the SWAN for the surface wave modeling. All model run over 5 km domain (same domain for ROMS and SWAN). COAWST was used with different configurations: in Stand Alone (SA) mode (that is, with only the atmospheric part), in atmosphere-ocean coupled mode (AO), and in a fully coupled version including also surface waves (AOW). Several sensitivity simulations performed with the SA approach were undertaken to simulate the TLC evolution. Especially in the later stage of the lifetime, when the cyclone was weaker, the predictability appears limited. Sensitivity simulations have considered the effect of the cumulus scheme (using an explicit scheme the Medicane does not develop and remains an extra-tropical depression) and the PBL scheme (using MYJ or MYNN resulting "Medicane" are extremely similar, although the roughness appears rather different among the two experiments). Comparing the three runs, the effects of different simulations on the Medicane tracks are significant only in the later stage of the cyclone lifetime. In the overall modeled basin, wind intensity is higher in the SA case w.r.t. both coupled runs. When compared to case AO, winds are about 1 m/s larger, even though the spatial distribution is very similar (possibly because of the lower SST produced by case AO). Case AOW produces less intense winds then SA and AO case in the areas where the wave is most developed (differences are about 2-4 m

  3. Body-wave traveltime and amplitude shifts from asymptotic travelling wave coupling

    USGS Publications Warehouse

    Pollitz, F.

    2006-01-01

    We explore the sensitivity of finite-frequency body-wave traveltimes and amplitudes to perturbations in 3-D seismic velocity structure relative to a spherically symmetric model. Using the approach of coupled travelling wave theory, we consider the effect of a structural perturbation on an isolated portion of the seismogram. By convolving the spectrum of the differential seismogram with the spectrum of a narrow window taper, and using a Taylor's series expansion for wavenumber as a function of frequency on a mode dispersion branch, we derive semi-analytic expressions for the sensitivity kernels. Far-field effects of wave interactions with the free surface or internal discontinuities are implicitly included, as are wave conversions upon scattering. The kernels may be computed rapidly for the purpose of structural inversions. We give examples of traveltime sensitivity kernels for regional wave propagation at 1 Hz. For the direct SV wave in a simple crustal velocity model, they are generally complicated because of interfering waves generated by interactions with the free surface and the Mohorovic??ic?? discontinuity. A large part of the interference effects may be eliminated by restricting the travelling wave basis set to those waves within a certain range of horizontal phase velocity. ?? Journal compilation ?? 2006 RAS.

  4. Modelling of radio frequency sheath and fast wave coupling on the realistic ion cyclotron resonant antenna surroundings and the outer wall

    NASA Astrophysics Data System (ADS)

    Lu, L.; Colas, L.; Jacquot, J.; Després, B.; Heuraux, S.; Faudot, E.; Van Eester, D.; Crombé, K.; Křivská, A.; Noterdaeme, J.-M.; Helou, W.; Hillairet, J.

    2018-03-01

    In order to model the sheath rectification in a realistic geometry over the size of ion cyclotron resonant heating (ICRH) antennas, the self-consistent sheaths and waves for ICH (SSWICH) code couples self-consistently the RF wave propagation and the DC SOL biasing via nonlinear RF and DC sheath boundary conditions applied at plasma/wall interfaces. A first version of SSWICH had 2D (toroidal and radial) geometry, rectangular walls either normal or parallel to the confinement magnetic field B 0 and only included the evanescent slow wave (SW) excited parasitically by the ICRH antenna. The main wave for plasma heating, the fast wave (FW) plays no role on the sheath excitation in this version. A new version of the code, 2D SSWICH-full wave, was developed based on the COMSOL software, to accommodate full RF field polarization and shaped walls tilted with respect to B 0 . SSWICH-full wave simulations have shown the mode conversion of FW into SW occurring at the sharp corners where the boundary shape varies rapidly. It has also evidenced ‘far-field’ sheath oscillations appearing at the shaped walls with a relatively long magnetic connection length to the antenna, that are only accessible to the propagating FW. Joint simulation, conducted by SSWICH-full wave within a multi-2D approach excited using the 3D wave coupling code (RAPLICASOL), has recovered the double-hump poloidal structure measured in the experimental temperature and potential maps when only the SW is modelled. The FW contribution on the potential poloidal structure seems to be affected by the 3D effects, which was ignored in the current stage. Finally, SSWICH-full wave simulation revealed the left-right asymmetry that has been observed extensively in the unbalanced strap feeding experiments, suggesting that the spatial proximity effects in RF sheath excitation, studied for SW only previously, is still important in the vicinity of the wave launcher under full wave polarizations.

  5. Efficient non-hydrostatic modelling of 3D wave-induced currents using a subgrid approach

    NASA Astrophysics Data System (ADS)

    Rijnsdorp, Dirk P.; Smit, Pieter B.; Zijlema, Marcel; Reniers, Ad J. H. M.

    2017-08-01

    Wave-induced currents are an ubiquitous feature in coastal waters that can spread material over the surf zone and the inner shelf. These currents are typically under resolved in non-hydrostatic wave-flow models due to computational constraints. Specifically, the low vertical resolutions adequate to describe the wave dynamics - and required to feasibly compute at the scales of a field site - are too coarse to account for the relevant details of the three-dimensional (3D) flow field. To describe the relevant dynamics of both wave and currents, while retaining a model framework that can be applied at field scales, we propose a two grid approach to solve the governing equations. With this approach, the vertical accelerations and non-hydrostatic pressures are resolved on a relatively coarse vertical grid (which is sufficient to accurately resolve the wave dynamics), whereas the horizontal velocities and turbulent stresses are resolved on a much finer subgrid (of which the resolution is dictated by the vertical scale of the mean flows). This approach ensures that the discrete pressure Poisson equation - the solution of which dominates the computational effort - is evaluated on the coarse grid scale, thereby greatly improving efficiency, while providing a fine vertical resolution to resolve the vertical variation of the mean flow. This work presents the general methodology, and discusses the numerical implementation in the SWASH wave-flow model. Model predictions are compared with observations of three flume experiments to demonstrate that the subgrid approach captures both the nearshore evolution of the waves, and the wave-induced flows like the undertow profile and longshore current. The accuracy of the subgrid predictions is comparable to fully resolved 3D simulations - but at much reduced computational costs. The findings of this work thereby demonstrate that the subgrid approach has the potential to make 3D non-hydrostatic simulations feasible at the scale of a

  6. Modeling of atmospheric-coupled Rayleigh waves on planets with atmosphere: From Earth observation to Mars and Venus perspectives.

    PubMed

    Lognonné, Philippe; Karakostas, Foivos; Rolland, Lucie; Nishikawa, Yasuhiro

    2016-08-01

    Acoustic coupling between solid Earth and atmosphere has been observed since the 1960s, first from ground-based seismic, pressure, and ionospheric sensors and since 20 years with various satellite measurements, including with global positioning system (GPS) satellites. This coupling leads to the excitation of the Rayleigh surface waves by local atmospheric sources such as large natural explosions from volcanoes, meteor atmospheric air-bursts, or artificial explosions. It contributes also in the continuous excitation of Rayleigh waves and associated normal modes by atmospheric winds and pressure fluctuations. The same coupling allows the observation of Rayleigh waves in the thermosphere most of the time through ionospheric monitoring with Doppler sounders or GPS. The authors review briefly in this paper observations made on Earth and describe the general frame of the theory enabling the computation of Rayleigh waves for models of telluric planets with atmosphere. The authors then focus on Mars and Venus and give in both cases the atmospheric properties of the Rayleigh normal modes and associated surface waves compared to Earth. The authors then conclude on the observation perspectives especially for Rayleigh waves excited by atmospheric sources on Mars and for remote ionospheric observations of Rayleigh waves excited by quakes on Venus.

  7. Dark forces coupled to nonconserved currents

    NASA Astrophysics Data System (ADS)

    Dror, Jeff A.; Lasenby, Robert; Pospelov, Maxim

    2017-10-01

    New light vectors with dimension-4 couplings to Standard Model states have (energy/vectormass)2-enhanced production rates unless the current they couple to is conserved. These processes allow us to derive new constraints on the couplings of such vectors, that are significantly stronger than the previous literature for a wide variety of models. Examples include vectors with axial couplings to quarks and vectors coupled to currents (such as baryon number) that are only broken by the chiral anomaly. Our new limits arise from a range of processes, including rare Z decays and flavor-changing meson decays, and rule out a number of phenomenologically motivated proposals.

  8. Strongly coupled stress waves in heterogeneous plates.

    NASA Technical Reports Server (NTRS)

    Wang, A. S. D.; Chou, P. C.; Rose, J. L.

    1972-01-01

    Consideration of coupled stress waves generated by an impulsive load applied at one end of a semiinfinite plate. For the field equations governing the one-dimensional coupled waves a hyperbolic system of equations is obtained in which a strong coupling in the second derivatives exists. The method of characteristics described by Chou and Mortimer (1967) is extended to cover the case of strong coupling, and a study is made of the transient stress waves in a semiinfinite plate subjected to an initial step input. Coupled discontinuity fronts are found to propagate at different velocities. The normal plate stress and the bending moment at different time regimes are illustrated by graphs.

  9. On wind-wave-current interactions during the Shoaling Waves Experiment

    NASA Astrophysics Data System (ADS)

    Zhang, Fei W.; Drennan, William M.; Haus, Brian K.; Graber, Hans C.

    2009-01-01

    This paper presents a case study of wind-wave-current interaction during the Shoaling Waves Experiment (SHOWEX). Surface current fields off Duck, North Carolina, were measured by a high-frequency Ocean Surface Current Radar (OSCR). Wind, wind stress, and directional wave data were obtained from several Air Sea Interaction Spar (ASIS) buoys moored in the OSCR scanning domain. At several times during the experiment, significant coastal currents entered the experimental area. High horizontal shears at the current edge resulted in the waves at the peak of wind-sea spectra (but not those in the higher-frequency equilibrium range) being shifted away from the mean wind direction. This led to a significant turning of the wind stress vector away from the mean wind direction. The interactions presented here have important applications in radar remote sensing and are discussed in the context of recent radar imaging models of the ocean surface.

  10. Coupled Waves on a Periodically Supported Timoshenko Beam

    NASA Astrophysics Data System (ADS)

    HECKL, MARIA A.

    2002-05-01

    A mathematical model is presented for the propagation of structural waves on an infinitely long, periodically supported Timoshenko beam. The wave types that can exist on the beam are bending waves with displacements in the horizontal and vertical directions, compressional waves and torsional waves. These waves are affected by the periodic supports in two ways: their dispersion relation spectra show passing and stopping bands, and coupling of the different wave types tends to occur. The model in this paper could represent a railway track where the beam represents the rail and an appropriately chosen support type represents the pad/sleeper/ballast system of a railway track. Hamilton's principle is used to calculate the Green function matrix of the free Timoshenko beam without supports. The supports are incorporated into the model by combining the Green function matrix with the superposition principle. Bloch's theorem is applied to describe the periodicity of the supports. This leads to polynomials with several solutions for the Bloch wave number. These solutions are obtained numerically for different combinations of wave types. Two support types are examined in detail: mass supports and spring supports. More complex support types, such as mass/spring systems, can be incorporated easily into the model.

  11. Scattering of plane evanescent waves by cylindrical shells and wave vector coupling conditions for exciting flexural waves

    NASA Astrophysics Data System (ADS)

    Marston, Philip L.

    2002-05-01

    The coupling of sound to buried targets can be associated with acoustic evanescent waves when the sea bottom is smooth. To understand the excitation of flexural waves on buried shells by acoustic evanescent waves, the partial wave series for the scattering is found for cylindrical shells at normal incidence in an unbounded medium. The formulation uses the simplifications of thin-shell dynamics. In the case of ordinary waves incident on a shell, a ray formulation is available to describe the coupling to subsonic flexural waves [P. L. Marston and N. H. Sun, J. Acoust. Soc. Am. 97, 777-783 (1995)]. When the incident wave is evanescent, the distance between propagating plane wavefronts is smaller than the ordinary acoustical wavelength at the same frequency and the coupling condition for the excitation of flexural waves on shells or plates is modified. Instead of matching the flexural wave number with the propagating part of the acoustic wave number only at the coincidence frequency, a second low-frequency wave number matching condition is found for highly evanescent waves. Numerical evaluation of the modified partial-wave-series appropriate for an evanescent wave is used to investigate the low-frequency coupling of evanescent waves with flexural wave resonances of shells.

  12. Directional bottom roughness associated with waves, currents, and ripples

    USGS Publications Warehouse

    Sherwood, Christopher R.; Rosati, Julie D.; Wang, Ping; Roberts, Tiffany M.

    2011-01-01

    Roughness lengths are used in wave-current bottom boundary layer models to parameterize drag associated with grain roughness, the effect of saltating grains during sediment transport, and small-scale bottom topography (ripples and biogenic features). We made field measurements of flow parameters and recorded sonar images of ripples at the boundary of a sorted-bedform at ~12-m depth on the inner shelf for a range of wave and current conditions over two months. We compared estimates of apparent bottom roughness inferred from the flow measurements with bottom roughness calculated using ripple geometry and the Madsen (1994) one-dimensional (vertical) wave-current bottom boundary layer model. One result of these comparisons was that the model over predicted roughness of flow from the dormant large ripples when waves were small. We developed a correction to the ripple-roughness model that incorporates an apparent ripple wavelength related to the combined wave-current flow direction. This correction provides a slight improvement for low-wave conditions, but does not address several other differences between observations and the modeled roughness.

  13. Multiphysics and Multiscale Model Coupling Using Gerris

    NASA Astrophysics Data System (ADS)

    Keen, T. R.; Dykes, J. D.; Campbell, T. J.

    2012-12-01

    This work is implementing oceanographic processes encompassing multiple physics and scales using the Gerris Flow Solver (GFS) in order to examine their interdependence and sensitivity to changes in the physical environment. The processes include steady flow due to tides and the wind, phase-averaged wave-forced flow and oscillatory currents, and sediment transport. The 2D steady flow is calculated by the Ocean module contained within GFS. This model solves the Navier-Stokes (N-S) equations using the finite volume method. The model domain is represented by quad-tree adaptive mesh refinement (AMR). A stationary wave field is computed for a specified wave spectrum is uniformly distributed over the domain as a tracer with local wind input parameterized as a source, and dissipation by friction and breaking as a sink. Alongshore flow is included by a radiation stress term; this current is added to the steady flow component from tides and wind. Wave-current interaction is parameterized using a bottom boundary layer model. Sediment transport as suspended and bed load is implemented using tracers that are transported via the advection equations. A bed-conservation equation is implemented to allow changes in seafloor elevation to be used in adjusting the AMR refinement. These processes are being coupled using programming methods that are inherent to GFS and that do not require modification or recompiling of the code. These techniques include passive tracers, C functions that operate as plug-ins, and user-defined C-type macros included with GFS. Our results suggest that the AMR model coupling method is useful for problems where the dynamics are governed by several processes. This study is examining the relative influence of the steady currents, wave field, and sedimentation. Hydrodynamic and sedimentation interaction in nearshore environments is being studied for an idealized beach and for the Sandy Duck storm of Oct. 1998. The potential behavior of muddy sediments on the

  14. On the convergence of the coupled-wave approach for lamellar diffraction gratings

    NASA Technical Reports Server (NTRS)

    Li, Lifeng; Haggans, Charles W.

    1992-01-01

    Among the many existing rigorous methods for analyzing diffraction of electromagnetic waves by diffraction gratings, the coupled-wave approach stands out because of its versatility and simplicity. It can be applied to volume gratings and surface relief gratings, and its numerical implementation is much simpler than others. In addition, its predictions were experimentally validated in several cases. These facts explain the popularity of the coupled-wave approach among many optical engineers in the field of diffractive optics. However, a comprehensive analysis of the convergence of the model predictions has never been presented, although several authors have recently reported convergence difficulties with the model when it is used for metallic gratings in TM polarization. Herein, three points are made: (1) in the TM case, the coupled-wave approach converges much slower than the modal approach of Botten et al; (2) the slow convergence is caused by the use of Fourier expansions for the permittivity and the fields in the grating region; and (3) is manifested by the slow convergence of the eigenvalues and the associated modal fields. The reader is assumed to be familiar with the mathematical formulations of the coupled-wave approach and the modal approach.

  15. Analytical coupled-wave model for photonic crystal surface-emitting quantum cascade lasers.

    PubMed

    Wang, Zhixin; Liang, Yong; Yin, Xuefan; Peng, Chao; Hu, Weiwei; Faist, Jérôme

    2017-05-15

    An analytical coupled-wave model is developed for surface-emitting photonic-crystal quantum cascade lasers (PhC-QCLs). This model provides an accurate and efficient analysis of full three-dimensional device structure with large-area cavity size. Various laser properties of interest including the band structure, mode frequency, cavity loss, mode intensity profile, and far field pattern (FFP), as well as their dependence on PhC structures and cavity size, are investigated. Comparison with numerical simulations confirms the accuracy and validity of our model. The calculated FFP and polarization profile well explain the previously reported experimental results. In particular, we reveal the possibility of switching the lasing modes and generating single-lobed FFP by properly tuning PhC structures.

  16. On the coupled evolution of oceanic internal waves and quasi-geostrophic flow

    NASA Astrophysics Data System (ADS)

    Wagner, Gregory LeClaire

    Oceanic motion outside thin boundary layers is primarily a mixture of quasi-geostrophic flow and internal waves with either near-inertial frequencies or the frequency of the semidiurnal lunar tide. This dissertation seeks a deeper understanding of waves and flow through reduced models that isolate their nonlinear and coupled evolution from the Boussinesq equations. Three physical-space models are developed: an equation that describes quasi-geostrophic evolution in an arbitrary and prescribed field of hydrostatic internal waves; a three-component model that couples quasi-geostrophic flow to both near-inertial waves and the near-inertial second harmonic; and a model for the slow evolution of hydrostatic internal tides in quasi-geostrophic flow of near-arbitrary scale. This slow internal tide equation opens the path to a coupled model for the energetic interaction of quasi-geostrophic flow and oceanic internal tides. Four results emerge. First, the wave-averaged quasi-geostrophic equation reveals that finite-amplitude waves give rise to a mean flow that advects quasi-geostrophic potential vorticity. Second is the definition of a new material invariant: Available Potential Vorticity, or APV. APV isolates the part of Ertel potential vorticity available for balanced-flow evolution in Eulerian frames and proves necessary in the separating waves and quasi-geostrophic flow. The third result, hashed out for near-inertial waves and quasi-geostrophic flow, is that wave-flow interaction leads to energy exchange even under conditions of weak nonlinearity. For storm-forced oceanic near-inertial waves the interaction often energizes waves at the expense of flow. We call this extraction of balanced quasi-geostrophic energy 'stimulated generation' since it requires externally-forced rather than spontaneously-generated waves. The fourth result is that quasi-geostrophic flow can encourage or 'catalyze' a nonlinear interaction between a near-inertial wave field and its second harmonic

  17. Nearshore Current Model Workshop Summary.

    DTIC Science & Technology

    1983-09-01

    dissipation , and wave-current interaction. b. Incorporation into models of wave-breaking. c. Parameterization of turbulence in models. d. Incorporation...into models of surf zone energy dissipation . e. Methods to specify waves and currents on the boundaries of the grid. f. Incorporation into models of...also recommended. Improvements should include nonlinear and irregular wave effects and improved models of wave-breaking and wave energy dissipation in

  18. Effects of obliquely opposing and following currents on wave propagation in a new 3D wave-current basin

    NASA Astrophysics Data System (ADS)

    Lieske, Mike; Schlurmann, Torsten

    2016-04-01

    INTRODUCTION & MOTIVATION The design of structures in coastal and offshore areas and their maintenance are key components of coastal protection. Usually, assessments of processes and loads on coastal structures are derived from experiments with flow and wave parameters in separate physical models. However, Peregrin (1976) already points out that processes in natural shallow coastal waters flow and sea state processes do not occur separately, but influence each other nonlinearly. Kemp & Simons (1982) perform 2D laboratory tests and study the interactions between a turbulent flow and following waves. They highlight the significance of wave-induced changes in the current properties, especially in the mean flow profiles, and draw attention to turbulent fluctuations and bottom shear stresses. Kemp & Simons (1983) also study these processes and features with opposing waves. Studies on the wave-current interaction in three-dimensional space for a certain wave height, wave period and water depth were conducted by MacIver et al. (2006). The research focus is set on the investigation of long-crested waves on obliquely opposing and following currents in the new 3D wave-current basin. METHODOLOGY In a first step the flow analysis without waves is carried out and includes measurements of flow profiles in the sweet spot of the basin at predefined measurement positions. Five measuring points in the water column have been delineated in different water depths in order to obtain vertical flow profiles. For the characterization of the undisturbed flow properties in the basin, an uniformly distributed flow was generated in the wave basin. In the second step wave analysis without current, the unidirectional wave propagation and wave height were investigated for long-crested waves in intermediate wave conditions. In the sweet spot of the wave basin waves with three different wave directions, three wave periods and uniform wave steepness were examined. For evaluation, we applied a common

  19. Seasonal variability of convectively coupled equatorial waves (CCEWs) in recent high-top CMIP5 models

    NASA Astrophysics Data System (ADS)

    Zakaria, Dzaki; Lubis, Sandro W.; Setiawan, Sonni

    2018-05-01

    Tropical weather system is controlled by periodic atmospheric disturbances ranging from daily to subseasonal time scales. One of the most prominent atmospheric disturbances in the tropics is convectively coupled equatorial waves (CCEWs). CCEWs are excited by latent heating due to a large-scale convective system and have a significant influence on weather system. They include atmospheric equatorial Kelvin wave, Mixed Rossby Gravity (MRG) wave, Equatorial Rossby (ER) wave and Tropical Depression (TD-type) wave. In this study, we will evaluate the seasonal variability of CCEWs activity in nine high-top CMIP5 models, including their spatial distribution in the troposphere. Our results indicate that seasonal variability of Kelvin waves is well represented in MPI-ESM-LR and MPI-ESM-MR, with maximum activity occurring during boreal spring. The seasonal variability of MRG waves is well represented in CanESM2, HadGEM2-CC, IPSL-CM5A-LR and IPSL-CM5A-MR, with maximum activity observed during boreal summer. On the other hand, ER waves are well captured by IPSL-CM5A-LR and IPSL-CM5A-MR and maximize during boreal fall; while TD-type waves, with maximum activity observed during boreal summer, are well observed in CanESM2, HadGEM2-CC, IPSL-CM5A-LR and IPSL-CM5A-MR. Our results indicate that the skill of CMIP5 models in representing seasonal variability of CCEWs highly depends on the convective parameterization and the spatial or vertical resolution used by each model.

  20. Gravitational waves and Higgs boson couplings for exploring first order phase transition in the model with a singlet scalar field

    NASA Astrophysics Data System (ADS)

    Hashino, Katsuya; Kakizaki, Mitsuru; Kanemura, Shinya; Ko, Pyungwon; Matsui, Toshinori

    2017-03-01

    We calculate the spectrum of gravitational waves originated from strongly first order electroweak phase transition in the extended Higgs model with a real singlet scalar field. In order to calculate the bubble nucleation rate, we perform a two-field analysis and evaluate bounce solutions connecting the true and the false vacua using the one-loop effective potential at finite temperatures. Imposing the Sakharov condition of the departure from thermal equilibrium for baryogenesis, we survey allowed regions of parameters of the model. We then investigate the gravitational waves produced at electroweak bubble collisions in the early Universe, such as the sound wave, the bubble wall collision and the plasma turbulence. We find that the strength at the peak frequency can be large enough to be detected at future space-based gravitational interferometers such as eLISA, DECIGO and BBO. Predicted deviations in the various Higgs boson couplings are also evaluated at the zero temperature, and are shown to be large enough too. Therefore, in this model strongly first order electroweak phase transition can be tested by the combination of the precision study of various Higgs boson couplings at the LHC, the measurement of the triple Higgs boson coupling at future lepton colliders and the shape of the spectrum of gravitational wave detectable at future gravitational interferometers.

  1. Self-Consistent Model of Magnetospheric Ring Current and Electromagnetic Ion Cyclotron Waves: The 2-7 May 1998 Storm

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gamayunov, K. V.; Jordanova, V. K.

    2003-01-01

    A complete description of a self-consistent model of magnetospheric ring current interacting with electromagnetic ion cyclotron waves is presented. The model is based on the system of two kinetic equations; one equation describes the ring current ion dynamics, and another equation describes the wave evolution. The effects on ring current ions interacting with electromagnetic ion cyclotron waves and back on waves are considered self-consistently by solving both equations on a global magnetospheric scale under nonsteady state conditions. The developed model is employed to simulate the entire 2-7 May 1998 storm period. First, the trapped number fluxes of the ring current protons are calculated and presented along with comparison with the data measured by the three- dimensional hot plasma instrument Polar/HYDRA. Incorporating in the model the wave-particle interaction leads to much better agreement between the experimental data and the model results. Second, examining of the wave (MLT, L shell) distributions produced by the model during the storm progress reveals an essential intensification of the wave emission about 2 days after the main phase of the storm. This result is well consistent with the earlier ground-based observations. Finally, the theoretical shapes and the occurrence rates of the wave power spectral densities are studied. It is found that about 2 days after the storm s main phase on 4 May, mainly non-Gaussian shapes of power spectral densities are produced.

  2. Observations and Simulations of the Impact of Wave-Current Interaction on Wave Direction in the Surf Zone

    NASA Astrophysics Data System (ADS)

    Hopkins, Julia; Elgar, Steve; Raubenheimer, Britt

    2017-04-01

    Accurately characterizing the interaction of waves and currents can improve predictions of wave propagation and subsequent sediment transport in the nearshore. Along the southern shoreline of Martha's Vineyard, MA, waves propagate across strong tidal currents as they shoal, providing an ideal environment for investigating wave-current interaction. Wave directions and mean currents observed for two 1-month-long periods in 7- and 2-m water depths along 11 km of the Martha's Vineyard shoreline have strong tidal modulations. Wave directions shift by as much as 70 degrees over a tidal cycle in 7 m depth, and by as much as 25 degrees in 2 m depth. The magnitude of the tidal modulations in the wave field decreases alongshore to the west, consistent with the observed decrease in tidal currents from 2.1 to 0.2 m/s. The observations are reproduced accurately by a numerical model (SWAN and Deflt3D-FLOW) that simulates waves and currents over the observed bathymetry. Model simulations with and without wave-current interaction and tidal depth changes demonstrate that the observed tidal modulations of the wave field primarily are caused by wave-current interaction and not by tidal changes to water depths over the nearby complex shoals. Sediment transport estimates from simulated wave conditions using a range of tidal currents and offshore wave fields indicate that the modulation of the wave field at Martha's Vineyard can impact the direction of wave-induced alongshore sediment transport, sometimes driving transport opposing the direction of the offshore incident wave field. As such, the observations and model simulations suggest the importance of wave-current interaction to tidally averaged transport in mixed-energy wave-and-current nearshore environments. Supported by ASD(R&E), NSF, NOAA (Sea Grant), and ONR.

  3. Non-contact ultrasonic gas flow metering using air-coupled leaky Lamb waves.

    PubMed

    Fan, Zichuan; Jiang, Wentao; Wright, William M D

    2018-04-23

    This paper describes a completely non-contact ultrasonic method of gas flow metering using air-coupled leaky Lamb waves. To show proof of principle, a simplified representation of gas flow in a duct, comprising two separated thin isotropic plates with a gas flowing between them, has been modelled and investigated experimentally. An airborne compression wave emitted from an air-coupled capacitive ultrasonic transducer excited a leaky Lamb wave in the first plate in a non-contact manner. The leakage of this Lamb wave crossed the gas flow at an angle between the two plates as a compression wave, and excited a leaky Lamb wave in the second plate. An air-coupled capacitive ultrasonic transducer on the opposite side of this second plate then detected the airborne compression wave leakage from the second Lamb wave. As the gas flow shifted the wave field between the two plates, the point of Lamb wave excitation in the second plate was displaced in proportion to the gas flow rate. Two such measurements, in opposite directions, formed a completely non-contact contra-propagating Lamb wave flow meter, allowing measurement of the flow velocity between the plates. A COMSOL Multiphysics® model was used to visualize the wave fields, and accurately predicted the time differences that were then measured experimentally. Experiments using different Lamb wave frequencies and plate materials were also similarly verified. This entirely non-contact airborne approach to Lamb wave flow metering could be applied in place of clamp-on techniques in thin-walled ducts or pipes. Copyright © 2018 Elsevier B.V. All rights reserved.

  4. Role of ULF Waves in Radiation Belt and Ring Current Dynamics

    NASA Astrophysics Data System (ADS)

    Mann, I. R.; Murphy, K. R.; Rae, I. J.; Ozeke, L.; Milling, D. K.

    2013-12-01

    Ultra-low frequency (ULF) waves in the Pc4-5 band can be excited in the magnetosphere by the solar wind. Much recent work has shown how ULF wave power is strongly correlated with solar wind speed. However, little attention has been paid the dynamics of ULF wave power penetration onto low L-shells in the inner magnetosphere. We use more than a solar cycle of ULF wave data, derived from ground-based magnetometer networks, to examine this ULF wave power penetration and its dependence on solar wind and geomagnetic activity indices. In time domain data, we show very clearly that dayside ULF wave power, spanning more than 4 orders of magnitude, follows solar wind speed variations throughout the whole solar cycle - during periods of sporadic solar maximum ICMEs, during declining phase fast solar wind streams, and at solar minimum, alike. We also show that time domain ULF wave power increases during magnetic storms activations, and significantly demonstrate that a deeper ULF wave power penetration into the inner magnetosphere occurs during larger negative excursions in Dst. We discuss potential explanations for this low-L ULF wave power penetration, including the role of plasma mass density (such as during plasmaspheric erosion), or ring current ion instabilities during near-Earth ring current penetration. Interestingly, we also show that both ULF wave power and SAMPEX MeV electron flux show a remarkable similarity in their penetration to low-L, which suggests that ULF wave power penetration may be important for understanding and explaining radiation belt dynamics. Moreover, the correlation of ULF wave power with Dst, which peaks at one day lag, suggests the ULF waves might also be important for the inward transport of ions into the ring current. Current ring current models, which exclude long period ULF wave transport, under-estimate the ring current during fast solar wind streams which is consistent with a potential role for ULF waves in ring current energisation. The

  5. Self-Consistent Model of Magnetospheric Ring Current and Propagating Electromagnetic Ion Cyclotron Waves. 2; Waves, Precipitating Ring Current Ions, and Thermal Electron Heating

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gamayunov, K. V.; Gallagher, D. L.

    2006-01-01

    This paper is dedicated to further presentations and discussions of the results from our new global self-consistent theoretical model of interacting ring current ions and electromagnetic ion cyclotron waves [Khazanov et al., 2006; here referred to as Paper 1]. In order to adequately take into account the wave propagation and refraction in a multi-ion plasmasphere, we explicitly include the ray tracing equations in our previous self-consistent model and use the general form of the wave kinetic equation [for details see Paper 1]. To demonstrate the effects of the EMIC wave propagation and refraction on the RC proton precipitations and heating of the thermal plasmaspheric electrons we simulate the May 1998 storm. The main findings of our simulation can be summarized as follows. Firstly, the wave induced precipitations have a quite fine structure, and are highly organized by location of the plasmapause gradient. The strongest fluxes of about 4 (raised dot) 10(exp 6) [(cm (raised dot) s (raised dot) sr)(sup -l)] are observed during the main and early recovery phases of the storm. The very interesting and probably more important finding is that in a number of cases the most intense precipitating fluxes are not simply connected to the most intense EMIC waves. The character of the EMIC wave power spectral density distribution over the equatorial wave normal angle is an extremely crucial for the effectiveness of the RC ion scattering. Secondly, comparison of the global proton precipitating patterns with the results from other ring current model [Kozyra et al., 1997] reveals that although we observe a qualitative agreement between localizations of the wave induced fluxes in the models, there is no quantitative agreement between the magnitudes of these fluxes. These differences are mainly due to a qualitative difference between the characters of the EMIC wave power spectral density distributions over the equatorial wave normal angle. Finally, the two energy sources to the

  6. TOPLHA and ALOHA: comparison between Lower Hybrid wave coupling codes

    NASA Astrophysics Data System (ADS)

    Meneghini, Orso; Hillairet, J.; Goniche, M.; Bilato, R.; Voyer, D.; Parker, R.

    2008-11-01

    TOPLHA and ALOHA are wave coupling simulation tools for LH antennas. Both codes are able to account for realistic 3D antenna geometries and use a 1D plasma model. In the framework of a collaboration between MIT and CEA laboratories, the two codes have been extensively compared. In TOPLHA the EM problem is self consistently formulated by means of a set of multiple coupled integral equations having as domain the triangles of the meshed antenna surface. TOPLHA currently uses the FELHS code for modeling the plasma response. ALOHA instead uses a mode matching approach and its own plasma model. Comparisons have been done for several plasma scenarios on different antenna designs: an array of independent waveguides, a multi-junction antenna and a passive/active multi-junction antenna. When simulating the same geometry and plasma conditions the two codes compare remarkably well both for the reflection coefficients and for the launched spectra. The different approach of the two codes to solve the same problem strengthens the confidence in the final results.

  7. Spectral modification of seismic waves propagating through solids exhibiting a resonance frequency: a 1-D coupled wave propagation-oscillation model

    NASA Astrophysics Data System (ADS)

    Frehner, Marcel; Schmalholz, Stefan M.; Podladchikov, Yuri

    2009-02-01

    A 1-D model is presented that couples the microscale oscillations of non-wetting fluid blobs in a partially saturated poroelastic medium with the macroscale wave propagation through the elastic skeleton. The fluid oscillations are caused by surface tension forces that act as the restoring forces driving the oscillations. The oscillations are described mathematically with the equation for a linear oscillator and the wave propagation is described with the 1-D elastic wave equation. Coupling is done using Hamilton's variational principle for continuous systems. The resulting linear system of two partial differential equations is solved numerically with explicit finite differences. Numerical simulations are used to analyse the effect of solids exhibiting internal oscillations, and consequently a resonance frequency, on seismic waves propagating through such media. The phase velocity dispersion relation shows a higher phase velocity in the high-frequency limit and a lower phase velocity in the low-frequency limit. At the resonance frequency a singularity in the dispersion relation occurs. Seismic waves can initiate oscillations of the fluid by transferring energy from solid to fluid at the resonance frequency. Due to this transfer, the spectral amplitude of the solid particle velocity decreases at the resonance frequency. After initiation, the oscillatory movement of the fluid continuously transfers energy at the resonance frequency back to the solid. Therefore, the spectral amplitude of the solid particle velocity is increased at the resonance frequency. Once initiated, fluid oscillations decrease in amplitude with increasing time. Consequently, the spectral peak of the solid particle velocity at the resonance frequency decreases with time.

  8. Submesoscale features and their interaction with fronts and internal tides in a high-resolution coupled atmosphere-ocean-wave model of the Bay of Bengal

    NASA Astrophysics Data System (ADS)

    Jensen, Tommy G.; Shulman, Igor; Wijesekera, Hemantha W.; Anderson, Stephanie; Ladner, Sherwin

    2018-03-01

    Large freshwater fluxes into the Bay of Bengal by rainfall and river discharges result in strong salinity fronts in the bay. In this study, a high-resolution coupled atmosphere-ocean-wave model with comprehensive physics is used to model the weather, ocean circulation, and wave field in the Bay of Bengal. Our objective is to explore the submesoscale activity that occurs in a realistic coupled model that resolves mesoscales and allows part of the submesoscale field. Horizontal resolution in the atmosphere varies from 2 to 6 km and is 13 km for surface waves, while the ocean model is submesoscale permitting with resolutions as high as 1.5 km and a vertical resolution of 0.5 m in the upper 10 m. In this paper, three different cases of oceanic submesoscale features are discussed. In the first case, heavy rainfall and intense downdrafts produced by atmospheric convection are found to force submesoscale currents, temperature, and salinity anomalies in the oceanic mixed layer and impact the mesoscale flow. In a second case, strong solitary-like waves are generated by semidiurnal tides in the Andaman Sea and interact with mesoscale flows and fronts and affect submesoscale features generated along fronts. A third source of submesoscale variability is found further north in the Bay of Bengal where river outflows help maintain strong salinity gradients throughout the year. For that case, a comparison with satellite observations of sea surface height anomalies, sea surface temperature, and chlorophyll shows that the model captures the observed mesoscale eddy features of the flow field, but in addition, submesoscale upwelling and downwelling patterns associated with ageostrophic secondary circulations along density fronts are also captured by the model.

  9. Lithosphere-Atmosphere coupling: Spectral element modeling of the evolution of acoustic waves in the atmosphere from an underground source.

    NASA Astrophysics Data System (ADS)

    Averbuch, Gil; Price, Colin

    2015-04-01

    Lithosphere-Atmosphere coupling: Spectral element modeling of the evolution of acoustic waves in the atmosphere from an underground source. G. Averbuch, C. Price Department of Geosciences, Tel Aviv University, Israel Infrasound is one of the four Comprehensive Nuclear-Test Ban Treaty technologies for monitoring nuclear explosions. This technology measures the acoustic waves generated by the explosions followed by their propagation through the atmosphere. There are also natural phenomena that can act as an infrasound sources like sprites, volcanic eruptions and earthquakes. The infrasound waves generated from theses phenomena can also be detected by the infrasound arrays. In order to study the behavior of these waves, i.e. the physics of wave propagation in the atmosphere, their evolution and their trajectories, numerical methods are required. This presentation will deal with the evolution of acoustic waves generated by underground sources (earthquakes and underground explosions). A 2D Spectral elements formulation for lithosphere-atmosphere coupling will be presented. The formulation includes the elastic wave equation for the seismic waves and the momentum, mass and state equations for the acoustic waves in a moving stratified atmosphere. The coupling of the two media is made by boundary conditions that ensures the continuity of traction and velocity (displacement) in the normal component to the interface. This work has several objectives. The first is to study the evolution of acoustic waves in the atmosphere from an underground source. The second is to derive transmission coefficients for the energy flux with respect to the seismic magnitude and earth density. The third will be the generation of seismic waves from acoustic waves in the atmosphere. Is it possible?

  10. Generalized three-dimensional simulation of ferruled coupled-cavity traveling-wave-tube dispersion and impedance characteristics

    NASA Technical Reports Server (NTRS)

    Maruschek, Joseph W.; Kory, Carol L.; Wilson, Jeffrey D.

    1993-01-01

    The frequency-phase dispersion and Pierce on-axis interaction impedance of a ferruled, coupled-cavity, traveling-wave tube (TWT), slow-wave circuit were calculated using the three-dimensional simulation code Micro-SOS. The utilization of the code to reduce costly and time-consuming experimental cold tests is demonstrated by the accuracy achieved in calculating these parameters. A generalized input file was developed so that ferruled coupled-cavity TWT slow-wave circuits of arbitrary dimensions could be easily modeled. The practicality of the generalized input file was tested by applying it to the ferruled coupled-cavity slow-wave circuit of the Hughes Aircraft Company model 961HA TWT and by comparing the results with experimental results.

  11. A Three-Wave Model of the Stratosphere with Coupled Dynamics, Radiation and Photochemistry. Appendix M

    NASA Technical Reports Server (NTRS)

    Shia, Run-Lie; Zhou, Shuntai; Ko, Malcolm K. W.; Sze, Nien-Dak; Salstein, David; Cady-Pereira, Karen

    1997-01-01

    A zonal mean chemistry transport model (2-D CTM) coupled with a semi-spectral dynamical model is used to simulate the distributions of trace gases in the present day atmosphere. The zonal-mean and eddy equations for the velocity and the geopotential height are solved in the semi-spectral dynamical model. The residual mean circulation is derived from these dynamical variables and used to advect the chemical species in the 2- D CTM. Based on a linearized wave transport equation, the eddy diffusion coefficients for chemical tracers are expressed in terms of the amplitude, frequency and growth rate of dynamical waves; local chemical loss rates; and a time constant parameterizing small scale mixing. The contributions to eddy flux are from the time varying wave amplitude (transient eddy), chemical reactions (chemical eddy) and small scale mixing. In spite of the high truncation in the dynamical module (only three longest waves are resolved), the model has simulated many observed characteristics of stratospheric dynamics and distribution of chemical species including ozone. Compared with the values commonly used in 2-D CTMs, the eddy diffusion coefficients for chemical species calculated in this model are smaller, especially in the subtropics. It is also found that the chemical eddy diffusion has only a small effects in determining the distribution of most slow species, including ozone in the stratosphere.

  12. Role of entrainment in convectively-coupled equatorial waves in an aquaplanet model

    NASA Astrophysics Data System (ADS)

    Peatman, Simon; Methven, John; Woolnough, Steve

    2016-04-01

    Equatorially-trapped waves are known to be one of the key phenomena in determining the distribution of convective precipitation in the tropics as well as being crucial to the dynamics of the Madden-Julian Oscillation. However, numerical weather prediction models struggle to sustain such waves for a realistic length of time, which has a significant impact on forecasting precipitation for regions such as equatorial Africa. It has been found in the past that enhancing the rate of moisture entrainment can improve certain aspects of parametrized tropical convection in climate models. A parameter F controls the rate of entrainment into the convective plume for deep- and mid-level convection, with F = 1 denoting the control case. Here it is found in an aquaplanet simulation that F > 1 produces more convective precipitation at all zonal wavenumbers. Furthermore, Kelvin wave activity increases for waves with low frequency and zonal wavenumber but is slightly suppressed for shorter, higher-frequency waves, and vice versa for westward-propagating waves. A change in entrainment rate also brings about a change in the basic state wind and humidity fields. Therefore, the question arises as to whether changes in wave activity are due directly to changes in the coupling to the humidity in the waves by entrainment or due to changes in the basic state. An experiment was devised in which the convective parametrization scheme is allowed to entrain a weighted sum of the environmental humidity and a prescribed zonally-symmetric climatology, with a parameter α controlling the extent of the decoupling from the environment. Experiments with this new mechanism in the parametrization scheme reveal a complex relationship. For long waves at low frequency (period > ˜13 days), removing zonal asymmetry in the humidity seen by the entrainment scheme has very little influence on the ratio of eastward- to westward-propagating power. At higher frequencies and zonal wavenumbers, removing this zonal

  13. Wave Chaos and Coupling to EM Structures

    DTIC Science & Technology

    2006-07-01

    Antonsen, E. Ott and S. Anlage, Aspects of the Scattering and Impedance Properties of Chaotic Microwave Cavities, Acta Physica Polonica A 109, 65...other provision of law, no person shall be subject to a penalty for failing to comply with a collection of information if it does not display a ...currently valid OMB control number. 1. REPORT DATE JUL 2006 2. REPORT TYPE N/ A 3. DATES COVERED - 4. TITLE AND SUBTITLE Wave Chaos and Coupling

  14. Wave-Coupled Millimeter-Wave Electro-Optic Techniques

    DTIC Science & Technology

    2001-03-01

    This report details results on two antenna-coupled millimeter-wave electro - optic modulators, the slot-vee antenna-coupled modulator and a 94 GHz...study of the effects of velocity mismatch on linearized electro - optic modulators was made and the results published. A key result was that directional...drift in electro - optic modulators was made and protons were determined to be the cause. Several inventions were made to reduce or eliminate proton-caused bias drift.

  15. A Self-Consistent Model of the Interacting Ring Current Ions and Electromagnetic ICWs. Initial Results: Waves and Precipitation Fluxes

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gamayunov, K. V.; Jordanova, V. K.; Krivorutsky, E. N.; Whitaker, Ann F. (Technical Monitor)

    2001-01-01

    Initial results from the new developed model of the interacting ring current ions and ion cyclotron waves are presented. The model described by the system of two bound kinetic equations: one equation describes the ring current ion dynamics, and another one gives wave evolution. Such system gives a self-consistent description of the ring current ions and ion cyclotron waves in a quasilinear approach. Calculating ion-wave relationships, on a global scale under non steady-state conditions during May 2-5, 1998 storm, we presented the data at three time cuts around initial, main, and late recovery phases of May 4, 1998 storm phase. The structure and dynamics of the ring current proton precipitating flux regions and the wave active ones are discussed in detail.

  16. The Nonlinear Coupling of Alfven and Lower Hybrid Waves in Space Plasma

    NASA Technical Reports Server (NTRS)

    Khazanov, George V.

    2004-01-01

    Space plasmas support a wide variety of waves, and wave-particle interactions as well as wave-wave interactions which are of crucial importance to magnetospheric and ionospheric plasma behavior. The excitation of lower hybrid waves (LHWs) in particular is a widely discussed mechanism of interaction between plasma species in space and is one of the unresolved questions of magnetospheric multi-ion plasmas. It is demonstrated that large-amplitude Alfven waves may generate LHWs in the auroral zone and ring current region and in some cases (particularly in the inner magnetosphere) this serves as the Alfven wave saturation mechanism. We present several examples of observational data which illustrate that the proposed mechanism is a plausible candidate to explain certain classes of LHW generation events in the ionosphere and magnetosphere and demonstrate electron and ion energization involving these processes. We discuss the morphology dynamics and level of LHW activity generated by electromagnetic ion cyclotron (EMIC) waves during the May 2-7 1998 storm period on the global scale. The LHWs were calculated based on a newly developed self-consistent model (Khazanov et. al. 2002) that couples the system of two kinetic equations: one equation describes the ring current (RC) ion dynamic and another equation describes the evolution of EMIC waves. It is found that the LHWs are excited by helium ions due to their mass dependent drift in the electric field of EMIC waves. The level of LHW activity is calculated assuming that the induced scattering process is the main saturation mechanism for these waves. The calculated LHWs electric fields are consistent with the observational data.

  17. Double-temperature ratchet model and current reversal of coupled Brownian motors

    NASA Astrophysics Data System (ADS)

    Li, Chen-Pu; Chen, Hong-Bin; Zheng, Zhi-Gang

    2017-12-01

    On the basis of the transport features and experimental phenomena observed in studies of molecular motors, we propose a double-temperature ratchet model of coupled motors to reveal the dynamical mechanism of cooperative transport of motors with two heads, where the interactions and asynchrony between two motor heads are taken into account. We investigate the collective unidirectional transport of coupled system and find that the direction of motion can be reversed under certain conditions. Reverse motion can be achieved by modulating the coupling strength, coupling free length, and asymmetric coefficient of the periodic potential, which is understood in terms of the effective potential theory. The dependence of the directed current on various parameters is studied systematically. Directed transport of coupled Brownian motors can be manipulated and optimized by adjusting the pulsation period or the phase shift of the pulsation temperature.

  18. Small scale currents and ocean wave heights: from today's models to future satellite observations with CFOSAT and SKIM

    NASA Astrophysics Data System (ADS)

    Ardhuin, Fabrice; Gille, Sarah; Menemenlis, Dimitris; Rocha, Cesar; Rascle, Nicolas; Gula, Jonathan; Chapron, Bertrand

    2017-04-01

    Tidal currents and large oceanic currents, such as the Agulhas, Gulf Stream and Kuroshio, are known to modify ocean wave properties, causing extreme sea states that are a hazard to navigation. Recent advances in the understanding and modeling capability of ocean currents at scales of 10 km or less have revealed the ubiquitous presence of fronts and filaments. Based on realistic numerical models, we show that these structures can be the main source of variability in significant wave heights at scales less than 200 km, including important variations at 10 km. This current-induced variability creates gradients in wave heights that were previously overlooked and are relevant for extreme wave heights and remote sensing. The spectrum of significant wave heights is found to be of the order of 70⟨Hs ⟩2/(g2⟨Tm0,-1⟩2) times the current spectrum, where ⟨Hs ⟩ is the spatially-averaged significant wave height, ⟨Tm0,-1⟩ is the average energy period, and g is the gravity acceleration. This small scale variability is consistent with Jason-3 and SARAL along-track variability. We will discuss how future satellite mission with wave spectrometers can help observe these wave-current interactions. CFOSAT is due for launch in 2018, and SKIM is a proposal for ESA Earth Explorer 9.

  19. Scattering of plane evanescent waves by buried cylinders: Modeling the coupling to guided waves and resonances

    NASA Astrophysics Data System (ADS)

    Marston, Philip L.

    2003-04-01

    The coupling of sound to buried targets can be associated with acoustic evanescent waves when the sea bottom is smooth. To understand the excitation of guided waves on buried fluid cylinders and shells by acoustic evanescent waves and the associated target resonances, the two-dimensional partial wave series for the scattering is found for normal incidence in an unbounded medium. The shell formulation uses the simplifications of thin-shell dynamics. The expansion of the incident wave becomes a double summation with products of modified and ordinary Bessel functions [P. L. Marston, J. Acoust. Soc. Am. 111, 2378 (2002)]. Unlike the case of an ordinary incident wave, the counterpropagating partial waves of the same angular order have unequal magnitudes when the incident wave is evanescent. This is a consequence of the exponential dependence of the incident wave amplitude on depth. Some consequences of this imbalance of partial-wave amplitudes are given by modifying previous ray theory for the scattering [P. L. Marston and N. H. Sun, J. Acoust. Soc. Am. 97, 777-783 (1995)]. The exponential dependence of the scattering on the location of a scatterer was previously demonstrated in air [T. J. Matula and P. L. Marston, J. Acoust. Soc. Am. 93, 1192-1195 (1993)].

  20. Modeled and Observed Transitions Between Rip Currents and Alongshore Flows

    NASA Astrophysics Data System (ADS)

    Moulton, M.; Elgar, S.; Warner, J. C.; Raubenheimer, B.

    2014-12-01

    Predictions of rip currents, alongshore currents, and the temporal transitions between these circulation patterns are important for swimmer safety and for estimating the transport of sediments, biota, and pollutants in the nearshore. Here, field observations are combined with hydrodynamic modeling to determine the dominant processes that lead rip currents to turn on and off with changing waves, bathymetry, and tidal elevation. Waves, currents, mean sea levels, and bathymetry were measured near and within five shore-perpendicular channels (on average 2-m deep, 30-m wide) that were dredged with the propellers of a landing craft at different times on a long straight Atlantic Ocean beach near Duck, NC in summer 2012. The circulation was measured for a range of incident wave conditions and channel sizes, and included rapid transitions between strong (0.5 to 1 m/s) rip current jets flowing offshore through the channels and alongshore currents flowing across the channels with no rip currents. Meandering alongshore currents (alongshore currents combined with an offshore jet at the downstream edge of the channel) also were observed. Circulation patterns near and within idealized rip channels simulated with COAWST (a three-dimensional phase-averaged model that couples ROMS and SWAN) are compared with the observations. In addition, the model is used to investigate the hydrodynamic response to a range of wave conditions (angle, height, period) and bathymetries (channel width, depth, and length; tidal elevations; shape of sandbar or terrace). Rip current speeds are largest for the deepest perturbations, and decrease as incident wave angles become more oblique. For obliquely incident waves, the rip currents are shifted in the direction of the alongshore flow, with an increasing shift for increasing alongshore current speed or increasing bathymetric perturbation depth.

  1. Traveling-wave solutions in continuous chains of unidirectionally coupled oscillators

    NASA Astrophysics Data System (ADS)

    Glyzin, S. D.; Kolesov, A. Yu; Rozov, N. Kh

    2017-12-01

    Proposed is a mathematical model of a continuous annular chain of unidirectionally coupled generators given by certain nonlinear advection-type hyperbolic boundary value problem. Such problems are constructed by a limit transition from annular chains of unidirectionally coupled ordinary differential equations with an unbounded increase in the number of links. It is shown that any preassigned finite number of stable periodic motions of the traveling-wave type can coexist in the model.

  2. Self-Consistent Model of Magnetospheric Ring Current and Electromagnetic Ion Cyclotron Waves: The May 2-7, 1998, Storm

    NASA Technical Reports Server (NTRS)

    Khazanov, G. V.; Gamayunov, K. V.; Jordanova, V. K.

    2003-01-01

    Complete description of a self-consistent model for magnetospheric ring current interacting with electromagnetic ion cyclotron waves is presented. The model is based on the system of two kinetic equations; one equation describes the ring current ion dynamics, and another equation describes the wave evolution. The effects on ring current ions interacting with electromagnetic ion cyclotron waves, and back on waves, are considered self-consistently by solving both equations on a global magnetospheric scale under non steady-state conditions. In the paper by Khazanov et al. [2002] this self-consistent model has only been shortly outlined, and discussions of many the model related details have been omitted. For example, in present study for the first time a new algorithm for numerical finding of the resonant numbers for quasilinear wave-particle interaction is described, or it is demonstrated that in order to describe quasilinear interaction in a multi-ion thermal plasma correctly, both e and He(+) modes of electromagnetic ion cyclotron waves should be employed. The developed model is used to simulate the entire May 2-7, 1998 storm period. Trapped number fluxes of the ring current protons are calculated and presented along with their comparison with the data measured by the 3D hot plasma instrument Polar/HYDRA. Examining of the wave (MLT, L shell) distributions produced during the storm progress reveals an essential intensification of the wave emissions in about two days after main phase of storm. This result is well consistent with the earlier ground-based observations. Also the theoretical shapes and the occurrence rates for power spectral densities of electromagnetic ion cyclotron waves are studied. It is found that in about 2 days after the storm main phase on May 4, mainly non Gaussian shapes of power spectral densities are produced.

  3. Convectively Coupled Equatorial Waves in Reanalysis and CMIP5 Simulations

    NASA Astrophysics Data System (ADS)

    Castanheira, J. M.; Marques, C. A. F.

    2014-12-01

    Convectively coupled equatorial waves (CCEWs) are a result of the interplay between the physics and dynamics in the tropical atmosphere. As a result of such interplay, tropical convection appears often organized into synoptic to planetary-scale disturbances with time scales matching those of equatorial shallow water waves. CCEWs have broad impacts within the tropics, and their simulation in general circulation models is still problematic. Several studies showed that dispersion of those waves characteristics fit the dispersion curves derived from the Matsuno's (1966) solutions of the shallow water equations on the equatorial beta plane, namely, Kelvin, equatorial Rossby, mixed Rossby-gravity, and inertio-gravity waves. However, the more common methodology used to identify those waves is yet controversial. In this communication a new methodology for the diagnosis of CCEWs will be presented. It is based on a pre-filtering of the geopotential and horizontal wind, using 3--D normal modes functions of the adiabatic linearized equations of a resting atmosphere, followed by a space--time spectral analysis to identify the spectral regions of coherence. The methodology permits a direct detection of various types of equatorial waves, compares the dispersion characteristics of the coupled waves with the theoretical dispersion curves and allows an identification of which vertical modes are more involved in the convection. Moreover, the proposed methodology is able to show the existence of free dry waves and moist coupled waves with a common vertical structure, which is in conformity with the effect of convective heating/cooling on the effective static stability, as traduced in the gross moist stability concept. The methodology is also sensible to Doppler shifting effects. The methodology has been applied to the ERA-Interim horizontal wind and geopotential height fields and to the interpolated Outgoing Longwave Radiation (OLR) data produced by the National Oceanic and

  4. A Discrete Electromechanical Model for Human Cardiac Tissue: Effects of Stretch-Activated Currents and Stretch Conditions on Restitution Properties and Spiral Wave Dynamics

    PubMed Central

    Weise, Louis D.; Panfilov, Alexander V.

    2013-01-01

    We introduce an electromechanical model for human cardiac tissue which couples a biophysical model of cardiac excitation (Tusscher, Noble, Noble, Panfilov, 2006) and tension development (adjusted Niederer, Hunter, Smith, 2006 model) with a discrete elastic mass-lattice model. The equations for the excitation processes are solved with a finite difference approach, and the equations of the mass-lattice model are solved using Verlet integration. This allows the coupled problem to be solved with high numerical resolution. Passive mechanical properties of the mass-lattice model are described by a generalized Hooke's law for finite deformations (Seth material). Active mechanical contraction is initiated by changes of the intracellular calcium concentration, which is a variable of the electrical model. Mechanical deformation feeds back on the electrophysiology via stretch-activated ion channels whose conductivity is controlled by the local stretch of the medium. We apply the model to study how stretch-activated currents affect the action potential shape, restitution properties, and dynamics of spiral waves, under constant stretch, and dynamic stretch caused by active mechanical contraction. We find that stretch conditions substantially affect these properties via stretch-activated currents. In constantly stretched medium, we observe a substantial decrease in conduction velocity, and an increase of action potential duration; whereas, with dynamic stretch, action potential duration is increased only slightly, and the conduction velocity restitution curve becomes biphasic. Moreover, in constantly stretched medium, we find an increase of the core size and period of a spiral wave, but no change in rotation dynamics; in contrast, in the dynamically stretching medium, we observe spiral drift. Our results may be important to understand how altered stretch conditions affect the heart's functioning. PMID:23527160

  5. A discrete electromechanical model for human cardiac tissue: effects of stretch-activated currents and stretch conditions on restitution properties and spiral wave dynamics.

    PubMed

    Weise, Louis D; Panfilov, Alexander V

    2013-01-01

    We introduce an electromechanical model for human cardiac tissue which couples a biophysical model of cardiac excitation (Tusscher, Noble, Noble, Panfilov, 2006) and tension development (adjusted Niederer, Hunter, Smith, 2006 model) with a discrete elastic mass-lattice model. The equations for the excitation processes are solved with a finite difference approach, and the equations of the mass-lattice model are solved using Verlet integration. This allows the coupled problem to be solved with high numerical resolution. Passive mechanical properties of the mass-lattice model are described by a generalized Hooke's law for finite deformations (Seth material). Active mechanical contraction is initiated by changes of the intracellular calcium concentration, which is a variable of the electrical model. Mechanical deformation feeds back on the electrophysiology via stretch-activated ion channels whose conductivity is controlled by the local stretch of the medium. We apply the model to study how stretch-activated currents affect the action potential shape, restitution properties, and dynamics of spiral waves, under constant stretch, and dynamic stretch caused by active mechanical contraction. We find that stretch conditions substantially affect these properties via stretch-activated currents. In constantly stretched medium, we observe a substantial decrease in conduction velocity, and an increase of action potential duration; whereas, with dynamic stretch, action potential duration is increased only slightly, and the conduction velocity restitution curve becomes biphasic. Moreover, in constantly stretched medium, we find an increase of the core size and period of a spiral wave, but no change in rotation dynamics; in contrast, in the dynamically stretching medium, we observe spiral drift. Our results may be important to understand how altered stretch conditions affect the heart's functioning.

  6. Beta value coupled wave theory for nonslanted reflection gratings.

    PubMed

    Neipp, Cristian; Francés, Jorge; Gallego, Sergi; Bleda, Sergio; Martínez, Francisco Javier; Pascual, Inmaculada; Beléndez, Augusto

    2014-01-01

    We present a modified coupled wave theory to describe the properties of nonslanted reflection volume diffraction gratings. The method is based on the beta value coupled wave theory, which will be corrected by using appropriate boundary conditions. The use of this correction allows predicting the efficiency of the reflected order for nonslanted reflection gratings embedded in two media with different refractive indices. The results obtained by using this method will be compared to those obtained using a matrix method, which gives exact solutions in terms of Mathieu functions, and also to Kogelnik's coupled wave theory. As will be demonstrated, the technique presented in this paper means a significant improvement over Kogelnik's coupled wave theory.

  7. Beta Value Coupled Wave Theory for Nonslanted Reflection Gratings

    PubMed Central

    Neipp, Cristian; Francés, Jorge; Gallego, Sergi; Bleda, Sergio; Martínez, Francisco Javier; Pascual, Inmaculada; Beléndez, Augusto

    2014-01-01

    We present a modified coupled wave theory to describe the properties of nonslanted reflection volume diffraction gratings. The method is based on the beta value coupled wave theory, which will be corrected by using appropriate boundary conditions. The use of this correction allows predicting the efficiency of the reflected order for nonslanted reflection gratings embedded in two media with different refractive indices. The results obtained by using this method will be compared to those obtained using a matrix method, which gives exact solutions in terms of Mathieu functions, and also to Kogelnik's coupled wave theory. As will be demonstrated, the technique presented in this paper means a significant improvement over Kogelnik's coupled wave theory. PMID:24723811

  8. Session on coupled atmospheric/chemistry coupled models

    NASA Technical Reports Server (NTRS)

    Thompson, Anne

    1993-01-01

    The session on coupled atmospheric/chemistry coupled models is reviewed. Current model limitations, current issues and critical unknowns, and modeling activity are addressed. Specific recommendations and experimental strategies on the following are given: multiscale surface layer - planetary boundary layer - chemical flux measurements; Eulerian budget study; and Langrangian experiment. Nonprecipitating cloud studies, organized convective systems, and aerosols - heterogenous chemistry are also discussed.

  9. Current drive by helicon waves

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

    Paul, Manash Kumar; Bora, Dhiraj; ITER Organization, Cadarache Centre-building 519, 131008 St. Paul-Lez-Durance

    2009-01-01

    Helicity in the dynamo field components of helicon wave is examined during the novel study of wave induced helicity current drive. Strong poloidal asymmetry in the wave magnetic field components is observed during helicon discharges formed in a toroidal vacuum chamber of small aspect ratio. High frequency regime is chosen to increase the phase velocity of helicon waves which in turn minimizes the resonant wave-particle interactions and enhances the contribution of the nonresonant current drive mechanisms. Owing to the strong poloidal asymmetry in the wave magnetic field structures, plasma current is driven mostly by the dynamo-electric-field, which arise due tomore » the wave helicity injection by helicon waves. Small, yet finite contribution from the suppressed wave-particle resonance cannot be ruled out in the operational regime examined. A brief discussion on the parametric dependence of plasma current along with numerical estimations of nonresonant components is presented. A close agreement between the numerical estimation and measured plasma current magnitude is obtained during the present investigation.« less

  10. High-resolution modelling of waves, currents and sediment transport in the Catalan Sea.

    NASA Astrophysics Data System (ADS)

    Sánchez-Arcilla, Agustín; Grifoll, Manel; Pallares, Elena; Espino, Manuel

    2013-04-01

    In order to investigate coastal shelf dynamics, a sequence of high resolution multi-scale models have been implemented for the Catalan shelf (North-western Mediterranean Sea). The suite consists of a set of increasing-resolution nested models, based on the circulation model ROMS (Regional Ocean Modelling System), the wave model SWAN (Simulation Waves Nearshore) and the sediment transport model CSTM (Community Sediment Transport Model), covering different ranges of spatial (from ~1 km at shelf-slope regions to ~40 m around river mouth or local beaches) and temporal scales (from storms events to seasonal variability). Contributions in the understanding of local processes such as along-shelf dynamics in the inner-shelf, sediment dispersal from the river discharge or bi-directional wave-current interactions under different synoptic conditions and resolution have been obtained using the Catalan Coast as a pilot site. Numerical results have been compared with "ad-hoc" intensive field campaigns, data from observational models and remote sensing products. The results exhibit acceptable agreement with observations and the investigation has allowed developing generic knowledge and more efficient (process-based) strategies for the coastal and shelf management.

  11. Depth averaged wave-current interaction in the multi bank morphology of the southern North Sea

    NASA Astrophysics Data System (ADS)

    Komijani, Homayoon; Osuna, Pedro; Ocampo Torres, Francisco; Monbaliu, Jaak

    2017-04-01

    The effects of wind induced waves on the barotropic mean flow during a storm event in the southern North Sea are investigated. The well known radiation stress gradient theory of Longuet-Higgins and Stewart (1962, 1964) together with the influence of waves through the Stokes drift (Hasselmann, 1971 and Garret, 1976) are incorporated in the RANS equation system of the COHERENS circulation model (Luyten et al., 2005) following the methodology worked out by Bennis et al. (2011) . The SWAN spectral wave model (version 40.91, http://www.swan.tudelft.nl/) is used to provide the wave information. This allows us to take into account the dissipative terms of wave momentum flux to the mean flow such as depth induced wave breaking and bottom friction as well as the conservative terms of wave effects such as the vortex-force and wave induced pressure gradient. The resulting coupled COHERENS-SWAN model has been validated using the well known planar beach test case proposed by Haas and Warner (2009) in depth averaged mode. For the application in the southern North Sea, a series of nested grids using COHERENS (circulation model) and WAM cycle 4.5.3 (spectral wave model applied to the North Sea shelf area, Monbaliu et al. 2000; Günther, H. and A. Behrens, personal communications, May 2012) is set up to provide the hydrodynamic and wave boundary conditions for the COHERENS-SWAN two way coupled wave-current model for the Belgian coastal zone model. The improvements obtained in hindcasting the circulation processes in the Belgian coastal area during a storm event will be highlighted. But also difficulties faced in the coupling of the models and in the simulation of a real case storm will be discussed. In particular, some of the approaches for dealing with the numerical instabilities due to multi bank morphology of the southern North Sea will be addressed. References : Bennis, A.-C., F. Ardhuin, and F. Dumas (2011). "On the coupling of wave and three-dimensional circulation models

  12. Wave excitation by nonlinear coupling among shear Alfvén waves in a mirror-confined plasma

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

    Ikezoe, R., E-mail: ikezoe@prc.tsukuba.ac.jp; Ichimura, M.; Okada, T.

    2015-09-15

    A shear Alfvén wave at slightly below the ion-cyclotron frequency overcomes the ion-cyclotron damping and grows because of the strong anisotropy of the ion temperature in the magnetic mirror configuration, and is called the Alfvén ion-cyclotron (AIC) wave. Density fluctuations caused by the AIC waves and the ion-cyclotron range of frequencies (ICRF) waves used for ion heating have been detected using a reflectometer in a wide radial region of the GAMMA 10 tandem mirror plasma. Various wave-wave couplings are clearly observed in the density fluctuations in the interior of the plasma, but these couplings are not so clear in themore » magnetic fluctuations at the plasma edge when measured using a pick-up coil. A radial dependence of the nonlinearity is found, particularly in waves with the difference frequencies of the AIC waves; bispectral analysis shows that such wave-wave coupling is significant near the core, but is not so evident at the periphery. In contrast, nonlinear coupling with the low-frequency background turbulence is quite distinct at the periphery. Nonlinear coupling associated with the AIC waves may play a significant role in the beta- and anisotropy-limits of a mirror-confined plasma through decay of the ICRF heating power and degradation of the plasma confinement by nonlinearly generated waves.« less

  13. Develop and Test Coupled Physical Parameterizations and Tripolar Wave Model Grid: NAVGEM / WaveWatch III / HYCOM

    DTIC Science & Technology

    2013-09-30

    Tripolar Wave Model Grid: NAVGEM / WaveWatch III / HYCOM W. Erick Rogers Naval Research Laboratory, Code 7322 Stennis Space Center, MS 39529...Parameterizations and Tripolar Wave Model Grid: NAVGEM / WaveWatch III / HYCOM 5a. CONTRACT NUMBER 5b. GRANT NUMBER 5c. PROGRAM ELEMENT NUMBER 6

  14. Regional seismic wavefield computation on a 3-D heterogeneous Earth model by means of coupled traveling wave synthesis

    USGS Publications Warehouse

    Pollitz, F.F.

    2002-01-01

    I present a new algorithm for calculating seismic wave propagation through a three-dimensional heterogeneous medium using the framework of mode coupling theory originally developed to perform very low frequency (f < ???0.01-0.05 Hz) seismic wavefield computation. It is a Greens function approach for multiple scattering within a defined volume and employs a truncated traveling wave basis set using the locked mode approximation. Interactions between incident and scattered wavefields are prescribed by mode coupling theory and account for the coupling among surface waves, body waves, and evanescent waves. The described algorithm is, in principle, applicable to global and regional wave propagation problems, but I focus on higher frequency (typically f ??????0.25 Hz) applications at regional and local distances where the locked mode approximation is best utilized and which involve wavefields strongly shaped by propagation through a highly heterogeneous crust. Synthetic examples are shown for P-SV-wave propagation through a semi-ellipsoidal basin and SH-wave propagation through a fault zone.

  15. HB06 : Field Validation of Realtime Predictions of Surfzone Waves and Currents

    NASA Astrophysics Data System (ADS)

    Guza, R. T.; O'Reilly, W. C.; Feddersen, F.

    2006-12-01

    California shorelines can be contaminated by the discharge of polluted streams and rivers onto the beach face or into the surf zone. Management decisions (for example, beach closures) can be assisted by accurate characterization of the waves and currents that transport and mix these pollutants. A real-time, operational waves and alongshore current model, developed for a 5 km alongshore reach at Huntington Beach (http://cdip.ucsd.edu/hb06/), will be tested for a month during Fall 2006 as part of the HB06 field experiment. The model has two components: prediction of incident waves immediately seaward of the surf zone, and the transformation of breaking waves across the surf zone. The California Safe Boating Network Model (O'Reilly et al., California World Ocean Conference, 2006) is used to estimate incident wave properties. This regional wave model accounts for blocking and refraction by offshore islands and shoals, and variation of the shoreline orientation. At Huntington Beach, the network model uses four buoys exposed to the deep ocean to estimate swell, and four nearby buoys to estimate locally generated seas. The model predictions will be compared with directional wave buoy observations in 22 m depth, 1 km from the shore. The computationally fast model for surfzone waves and breaking-wave driven alongshore currents, appropriate for random waves on beaches with simple bathymetry, is based on concepts developed and tested by Ed Thornton and his colleagues over the last 30 years. Modeled alongshore currents at Huntington Beach, with incident waves predicted by the Network model, will be compared with waves and currents observed during HB06 along a transect extending from 4 m depth to the shoreline. Support from the California Coastal Conservancy, NOAA, and ONR is gratefully acknowledged.

  16. Direct-current nanogenerator driven by ultrasonic waves.

    PubMed

    Wang, Xudong; Song, Jinhui; Liu, Jin; Wang, Zhong Lin

    2007-04-06

    We have developed a nanowire nanogenerator that is driven by an ultrasonic wave to produce continuous direct-current output. The nanogenerator was fabricated with vertically aligned zinc oxide nanowire arrays that were placed beneath a zigzag metal electrode with a small gap. The wave drives the electrode up and down to bend and/or vibrate the nanowires. A piezoelectric-semiconducting coupling process converts mechanical energy into electricity. The zigzag electrode acts as an array of parallel integrated metal tips that simultaneously and continuously create, collect, and output electricity from all of the nanowires. The approach presents an adaptable, mobile, and cost-effective technology for harvesting energy from the environment, and it offers a potential solution for powering nanodevices and nanosystems.

  17. Rogue wave in coupled electric transmission line

    NASA Astrophysics Data System (ADS)

    Duan, J. K.; Bai, Y. L.

    2018-03-01

    Distributed electrical transmission lines that consist of a large number of identical sections have been theoretically studied in the present paper. The rogue wave is analyzed and predicted using the nonlinear Schrodinger equation (NLSE). The results indicate that, in the continuum limit, the voltage for the transmission line is described in some cases by the NLSE that is obtained using the traditional perturbation technique. The dependences of the characteristics of the rouge wave parameters on the coupled electric transmission line are shown in the paper. As is well known, rogue waves can be found for a large number of oceanic disasters, and such waves may be disastrous. However, the results of the present paper for coupled electric transmission lines may be useful.

  18. Millimeter Wave Systems for Airports and Short-Range Aviation Communications: A Survey of the Current Channel Models at mmWave Frequencies

    NASA Technical Reports Server (NTRS)

    Khatun, Mahfuza; Mehrpouyan, Hani; Matolak, David; Guvenc, Ismail

    2017-01-01

    Millimeter-wave (mmWave) communications will play a key role in enhancing the throughput, reliability, and security of next generation wireless networks. These advancements are achieved through the large bandwidth available in this band and through the use of highly directional links that will be used to overcome the large pathloss at these frequencies. Although the terrestrial application of mmWave systems is advancing at a rapid pace, the use of mmWave communication systems in aviation systems or airports is still in its infancy. This can be attributed to the challenges related to radio technology and lack of development, and characterization of mmWave wireless channels for the aviation field and the airport environment. Consequently, one of our goals is to develop methodologies that support mmWave air to ground links, and various links at airports, by applying new localization schemes that allow for application of highly directional links that can be deployed over longer distances despite the high path loss at mmWave frequencies. However, a very thorough understanding of the mmWave channel models are needed to enable such new applications. To this end, in this paper, we present a survey of the current channel models in the mmWave band. The 3-dimensional statistical channel model is also reviewed and its parameters and typical characteristics for this model are identified and computed through simulation for the Boise metropolitan area.

  19. The US Navy Coupled Ocean-Wave Prediction System

    DTIC Science & Technology

    2014-09-01

    Stokes drift to be the dominant wave effect and that it increased surface drift speeds by 35% and veered the current in the direction of the wind...ocean model has been modified to incorporate the effect of the Stokes drift current, wave radiation stresses due to horizontal gradients of the momentum...for fourth-order differences for horizontal baroclinic pressure gradients and for interpolation of Coriolis terms. There is an option to use the

  20. Modeling of Inner Magnetosphere Coupling Processes

    NASA Technical Reports Server (NTRS)

    Khazanov, George V.

    2011-01-01

    The Ring Current (RC) is the biggest energy player in the inner magnetosphere. It is the source of free energy for Electromagnetic Ion Cyclotron (EMIC) wave excitation provided by a temperature anisotropy of RC ions, which develops naturally during inward E B convection from the plasmasheet. The cold plasmasphere, which is under the strong influence of the magnetospheric electric field, strongly mediates the RC-EMIC wave-particle-coupling process and ultimately becomes part of the particle and energy interplay. On the other hand, there is a strong influence of the RC on the inner magnetospheric electric and magnetic field configurations and these configurations, in turn, are important to RC dynamics. Therefore, one of the biggest needs for inner magnetospheric research is the continued progression toward a coupled, interconnected system with the inclusion of nonlinear feedback mechanisms between the plasma populations, the electric and magnetic fields, and plasma waves. As we clearly demonstrated in our studies, EMIC waves strongly interact with electrons and ions of energies ranging from approx.1 eV to approx.10 MeV, and that these waves strongly affect the dynamics of resonant RC ions, thermal electrons and ions, and the outer RB relativistic electrons. As we found, the rate of ion and electron scattering/heating in the Earth's magnetosphere is not only controlled by the wave intensity-spatial-temporal distribution but also strongly depends on the spectral distribution of the wave power. The latter is also a function of the plasmaspheric heavy ion content, and the plasma density and temperature distributions along the magnetic field lines. The above discussion places RC-EMIC wave coupling dynamics in context with inner magnetospheric coupling processes and, ultimately, relates RC studies with plasmaspheric and Superthermal Electrons formation processes as well as with outer RB physics.

  1. Model Simulations of Waves in Hurricane Juan

    NASA Astrophysics Data System (ADS)

    Perrie, W.; Toulany, B.; Padilla-Hernandez, R.; Hu, Y.; Smith, P.; Zhang, W.; Zou, Q.; Ren, X.

    2004-05-01

    Hurricane Juan made landfall at 0300 UTC near Halifax Nova Scotia. This was a category 2 hurricane with winds of 44 m/s, the largest storm to pass over these coastal areas in several decades. Associated high ocean waves were experienced in coastal waters, from Peggy's Cove to Sheet Harbour, growing to epic proportions on the Scotian Shelf, and exceeding the 100-year return wave based on the present climatology. As part of the GoMOOS program (Gulf of Maine Ocean Observing System, www.gomoos.org), winds from the USA Navy COAMPS (Coupled Ocean Atmosphere Model Prediction System) were used to evaluate and compare three widely-used third generation numerical wave models, SWAN, WAM and WaveWatch-III (hereafter WW3) for accuracy, with in situ measurements. Model comparisons consist of a set of composite model systems, respectively nesting WAM, WW3 and SWAN in WAM and WW3. We report results from the intermediate-resolution grid for Hurricane Juan. Wave measurements were made using four operational deep-water buoys (C44258, C44142, C44137, 44005), by a conventional directional wave rider (DWR) moored offshore from Lunenburg Bay, and also by two acoustic Doppler current profiler (ADCP) located (1) near an oil rig on Sable Island Bank, in relatively shallow water, and (2) near the outer boundary of Lunenburg Bay. We discuss the reliability of DWR wave data compared to ADCP wave data. We show that all models provide reliable hindcasts for significant wave height (Hs) and for peak period (Tp) for Juan, although a clear under-estimation of Hs at the peak of the storm is evident, compared to observations. A feature in the COAMPS storm simulation is that the storm track appears to be slightly to the east of that of Quikscat scatterometer data. Comparisons between models and 2-dimensional wave spectra are presented. Preliminary results suggest that the recently released upgrade to the WW3 model shows slightly enhanced skill compared to the other models.

  2. A coupled wave-hydrodynamic model of an atoll with high friction: Mechanisms for flow, connectivity, and ecological implications

    NASA Astrophysics Data System (ADS)

    Rogers, Justin S.; Monismith, Stephen G.; Fringer, Oliver B.; Koweek, David A.; Dunbar, Robert B.

    2017-02-01

    We present a hydrodynamic analysis of an atoll system from modeling simulations using a coupled wave and three-dimensional hydrodynamic model (COAWST) applied to Palmyra Atoll in the Central Pacific. This is the first time the vortex force formalism has been applied in a highly frictional reef environment. The model results agree well with field observations considering the model complexity in terms of bathymetry, bottom roughness, and forcing (waves, wind, metrological, tides, regional boundary conditions), and open boundary conditions. At the atoll scale, strong regional flows create flow separation and a well-defined wake, similar to 2D flow past a cylinder. Circulation within the atoll is typically forced by waves and tides, with strong waves from the north driving flow from north to south across the atoll, and from east to west through the lagoon system. Bottom stress is significant for depths less than about 60 m, and in addition to the model bathymetry, is important for correct representation of flow in the model. Connectivity within the atoll system shows that the general trends follow the mean flow paths. However, some connectivity exists between all regions of the atoll system due to nonlinear processes such as eddies and tidal phasing. Moderate wave stress, short travel time (days since entering the reef system), and low temperature appear to be the most ideal conditions for high coral cover at this site.

  3. A coupled modal-finite element method for the wave propagation modeling in irregular open waveguides.

    PubMed

    Pelat, Adrien; Felix, Simon; Pagneux, Vincent

    2011-03-01

    In modeling the wave propagation within a street canyon, particular attention must be paid to the description of both the multiple reflections of the wave on the building facades and the radiation in the free space above the street. The street canyon being considered as an open waveguide with a discontinuously varying cross-section, a coupled modal-finite element formulation is proposed to solve the three-dimensional wave equation within. The originally open configuration-the street canyon open in the sky above-is artificially turned into a close waveguiding structure by using perfectly matched layers that truncate the infinite sky without introducing numerical reflection. Then the eigenmodes of the resulting waveguide are determined by a finite element method computation in the cross-section. The eigensolutions can finally be used in a multimodal formulation of the wave propagation along the canyon, given its geometry and the end conditions at its extremities: initial field condition at the entrance and radiation condition at the output. © 2011 Acoustical Society of America

  4. Waveform Modeling of the Crust and Upper Mantle Using S, Sp, SsPmP, and Shear-Coupled PL Waves

    DTIC Science & Technology

    2008-05-10

    and excitation of shear-coupled Pl waves with distance and corresponding phase velocity ( Vph )-period (T) curve: αN and βN are the P and S wave...Pulliam and Sen, 2005) (b) Propagation characteristics and excitation of shear-coupled Pl waves with distance and corresponding phase velocity ( Vph

  5. A 20-Year High-Resolution Wave Resource Assessment of Japan with Wave-Current Interactions

    NASA Astrophysics Data System (ADS)

    Webb, A.; Waseda, T.; Kiyomatsu, K.

    2016-02-01

    Energy harvested from surface ocean waves and tidal currents has the potential to be a significant source of green energy, particularly for countries with extensive coastlines such as Japan. As part of a larger marine renewable energy project*, The University of Tokyo (in cooperation with JAMSTEC) has conducted a state-of-the-art wave resource assessment (with uncertainty estimates) to assist with wave generator site identification and construction in Japan. This assessment will be publicly available and is based on a large-scale NOAA WAVEWATCH III (version 4.18) simulation using NCEP and JAMSTEC forcings. It includes several key components to improve model skill: a 20-year simulation to reduce aleatory uncertainty, a four-nested-layer approach to resolve a 1 km shoreline, and finite-depth and current effects included in all wave power density calculations. This latter component is particularly important for regions near strong currents such as the Kuroshio. Here, we will analyze the different wave power density equations, discuss the model setup, and present results from the 20-year assessment (with a focus on the role of wave-current interactions). Time permitting, a comparison will also be made with simulations using JMA MSM 5 km winds. *New Energy and Industrial Technology Development Organization (NEDO): "Research on the Framework and Infrastructure of Marine Renewable Energy; an Energy Potential Assessment"

  6. Wave-current interactions in three dimensions: why 3D radiation stresses are not practical

    NASA Astrophysics Data System (ADS)

    Ardhuin, Fabrice

    2017-04-01

    The coupling of ocean circulation and wave models is based on a wave-averaged mass and momentum conservation equations. Whereas several equivalent equations for the evolution of the current momentum have been proposed, implemented, and used, the possibility to formulate practical equations for the total momentum, which is the sum of the current and wave momenta, has been obscured by a series of publications. In a recent update on previous derivations, Mellor (J. Phys. Oceanogr. 2015) proposed a new set of wave-forced total momentum equations. Here we show that this derivation misses a term that integrates to zero over the vertical. This is because he went from his depth-integrated eq. (28) to the 3D equation (30) by simply removing the integral, but any extra zero-integrating term can be added. Corrected for this omission, the equations of motion are equivalent to the earlier equations by Mellor (2003) which are correct when expressed in terms of wave-induced pressure, horizontal velocity and vertical displacement. Namely the total momentum evolution is driven by the horizontal divergence of a horizontal momentum flux, ----- --- ∂^s- Sαβ = ^uα^uβ + δαβ ∂ς (^p- g^s) (1) and the vertical divergence of a vertical flux, Sαz = (p^-g^s)∂^s/∂xα, (2) where p is the wave-induced non-hydrostatic pressure, s is the wave-induced vertical displacement, and u^ α is the horizontal wave-induced velocity in direction α. So far, so good. Problems arise when p and s are evaluated. Indeend, Ardhuin et al. (J. Phys. Oceanogr. 2008) showed that, over a sloping bottom ∂Sαβ/∂xβ is of order of the slope, hence a consistent wave forcing requires an estimation of Sαz that must be estimated to first order in the bottom slope. For this, Airy wave theory, i.e. cosh(kz-+-kh) p ≃ ga cosh (kD ) cosψ, (3) is not enough. Ardhuin et al. (2008) has shown that using an exact solution of the Laplace equations the vertical flux can indeed be computed. The alternative of

  7. Coupling alongshore variations in wave energy to beach morphologic change using the SWAN wave model at Ocean Beach, San Francisco, CA

    USGS Publications Warehouse

    Eshleman, Jodi L.; Barnard, Patrick L.; Erikson, Li H.; Hanes, Daniel M.

    2007-01-01

    conditions to help isolate the effects of offshore wave direction and period on nearshore wave predictions. Alongshore varying average beach change statistics are computed at specific profile locations from topographic beach surveys and lidar data. The study area is located in the San Francisco Bight in central California. Ocean Beach is a seven kilometer long north-south trending sandy coastline located just south of the entrance to the San Francisco Bay Estuary (Figure 1). It contains an erosion hotspot in the southern part of the beach which has resulted in damage to local infrastructure and is the cause of continued concern. A wide range of field data collection and numerical modeling efforts have been focused here as part of the United States Geological Survey's (USGS) San Francisco Bight Coastal Processes Study, which began in October 2003 and represents the first comprehensive study of coastal processes at the mouth of San Francisco Bay. Ocean Beach is exposed to very strong tidal flows, with measured currents often in excess of 1 m/s at the north end of the beach. Current profiler measurements indicate that current magnitudes are greater in the northern portion of the beach, while wave energy is greater in the southern portion where erosion problems are greatest (Barnard et al., 2007). The sub-aerial beach volume fluctuates seasonally over a maximum envelope of 400,000 m3 for the seven kilometer stretch (Barnard et al, 2007). The wave climate in the region is dominated by an abundance of low frequency energy (greater than 20 s period) and prevailing northwest incident wave angles. The application of a wave model to the region is further complicated by the presence of the Farallon Islands 40 kilometers west, and a massive ebb tidal delta at the mouth of San Francisco Bay (~150 km2), which creates complicated refraction patterns as wave energy moves from offshore Ocean Beach; however the cost and threat of the energetic nearshore environment have limited the temporal

  8. Plate Wave Resonance with Air-Coupled Ultrasonics

    NASA Astrophysics Data System (ADS)

    Bar, H. N.; Dayal, V.; Barnard, D.; Hsu, D. K.

    2010-02-01

    Air-coupled ultrasonic transducers can excite plate waves in metals and composites. The coincidence effect, i.e., the wave vector of plate wave coincides with projection of exciting airborne sound vector, leads to a resonance which strongly amplifies the sound transmission through the plate. The resonance depends on the angle of incidence and the frequency. In the present study, the incidence angle for maximum transmission (θmax) is measured in plates of steel, aluminum, carbon fiber reinforced composites and honeycomb sandwich panels. The variations of (θmax) with plate thickness are compared with theoretical values in steel, aluminum and quasi-isotropic carbon fiber composites. The enhanced transmission of air-coupled ultrasound at oblique incidence can substantially improve the probability of flaw detection in plates and especially in honeycomb structures. Experimental air-coupled ultrasonic scan of subtle flaws in CFRP laminates showed definite improvement of signal-to-noise ratio with oblique incidence at θmax.

  9. PLATE WAVE RESONANCE WITH AIR-COUPLED ULTRASONICS

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

    Bar, H. N.; Dayal, V.; Barnard, D.

    2010-02-22

    Air-coupled ultrasonic transducers can excite plate waves in metals and composites. The coincidence effect, i.e., the wave vector of plate wave coincides with projection of exciting airborne sound vector, leads to a resonance which strongly amplifies the sound transmission through the plate. The resonance depends on the angle of incidence and the frequency. In the present study, the incidence angle for maximum transmission (theta{sub max}) is measured in plates of steel, aluminum, carbon fiber reinforced composites and honeycomb sandwich panels. The variations of (theta{sub max}) with plate thickness are compared with theoretical values in steel, aluminum and quasi-isotropic carbon fibermore » composites. The enhanced transmission of air-coupled ultrasound at oblique incidence can substantially improve the probability of flaw detection in plates and especially in honeycomb structures. Experimental air-coupled ultrasonic scan of subtle flaws in CFRP laminates showed definite improvement of signal-to-noise ratio with oblique incidence at theta{sub max}.« less

  10. Explicit wave action conservation for water waves on vertically sheared flows

    NASA Astrophysics Data System (ADS)

    Quinn, Brenda; Toledo, Yaron; Shrira, Victor

    2016-04-01

    Water waves almost always propagate on currents with a vertical structure such as currents directed towards the beach accompanied by an under-current directed back toward the deep sea or wind-induced currents which change magnitude with depth due to viscosity effects. On larger scales they also change their direction due to the Coriolis force as described by the Ekman spiral. This implies that the existing wave models, which assume vertically-averaged currents, is an approximation which is far from realistic. In recent years, ocean circulation models have significantly improved with the capability to model vertically-sheared current profiles in contrast with the earlier vertically-averaged current profiles. Further advancements have coupled wave action models to circulation models to relate the mutual effects between the two types of motion. Restricting wave models to vertically-averaged non-turbulent current profiles is obviously problematic in these cases and the primary goal of this work is to derive and examine a general wave action equation which accounts for these shortcoming. The formulation of the wave action conservation equation is made explicit by following the work of Voronovich (1976) and using known asymptotic solutions of the boundary value problem which exploit the smallness of the current magnitude compared to the wave phase velocity and/or its vertical shear and curvature. The adopted approximations are shown to be sufficient for most of the conceivable applications. This provides correction terms to the group velocity and wave action definition accounting for the shear effects, which are fitting for application to operational wave models. In the limit of vanishing current shear, the new formulation reduces to the commonly used Bretherton & Garrett (1968) no-shear wave action equation where the invariant is calculated with the current magnitude taken at the free surface. It is shown that in realistic oceanic conditions, the neglect of the vertical

  11. Secondary Flows and Sediment Transport due to Wave - Current Interaction

    NASA Astrophysics Data System (ADS)

    Ismail, Nabil; Wiegel, Robert

    2015-04-01

    expression, ρs is the seawater mass density, ρ is the river current mass density, a0 is the deep water wave amplitude, g is the acceleration of gravity, Cg is the wave group velocity, L is the deep water wave length, h is the average water depth near the river mouth, C0 is the deep water wave phase velocity, U is the average jet exit velocity and w is the river or the tidal inlet effective width. The values of the above number were found to be in the range between 1.0 and 6.0-8.0 for the examined laboratory and field case studies for non-buoyant jets. Upper bound corresponds to cases of higher wave activity on the coast while the lower bound corresponds to cases of tidal currents with minimum wave activity, Coastal Processes Modifications due to River and Ebb Current Interaction with Opposing Waves: Confirmation of the obtained theoretical expression was obtained by comparison against field data for shoreline variability at river mouths and the formation of accretion shoals and erosion spots at tidal inlets and ocean outfalls in the USA and the Nile delta coastline. The predicted extent of the coast reshaping process, due to shoreline erosion and subsequent accretion, due to the absence of the river Nile current after 1965, east of the Rosetta headland, was determined. The obtained shoreline erosion spatial extent using the above correlation showed that the long term length of coastline recession would be in the neighborhood of 16-20 km east of Rosetta headland (1990-2014). Such results were further confirmed by the recent satellite data (Ghoneim, et al, 2015). The results of the present work were well compared to the data on Fort Pierce Inlet, Florida, where severe erosion is known to exist on both sides of the inlet (Joshi, 1983). The current results are qualitatively in parallel to that obtained recently by the numerical model Delft3D coupled with the wave model SWAN ( Nardin, et al, 2013) on wave- current interaction at river mouths and the formation of mouth bars

  12. Response of water temperature to surface wave effects in the Baltic Sea: simulations with the coupled NEMO-WAM model

    NASA Astrophysics Data System (ADS)

    Alari, Victor; Staneva, Joanna; Breivik, Øyvind; Bidlot, Jean-Raymond; Mogensen, Kristian; Janssen, Peter

    2016-04-01

    The effects of wind waves on the Baltic Sea water temperature has been studied by coupling the hydrodynamical model NEMO with the wave model WAM. The wave forcing terms that have been taken into consideration are: Stokes-Coriolis force, seastate dependent energy flux and sea-state dependent momentum flux. The combined role of these processes as well as their individual contributions on simulated temperature is analysed. The results indicate a pronounced effect of waves on surface temperature, on the distribution of vertical temperature and on upwellinǵs. In northern parts of the Baltic Sea a warming of the surface layer occurs in the wave included simulations. This in turn reduces the cold bias between simulated and measured data. The warming is primarily caused by sea-state dependent energy flux. Wave induced cooling is mostly observed in near coastal areas and is mainly due to Stokes-Coriolis forcing. The latter triggers effect of intensifying upwellings near the coasts, depending on the direction of the wind. The effect of sea-state dependent momentum flux is predominantly to warm the surface layer. During the summer the wave induced water temperature changes were up to 1 °C.

  13. Coupled Transmission Line Based Slow Wave Structures for Traveling Wave Tubes Applications

    NASA Astrophysics Data System (ADS)

    Zuboraj, Md. Rashedul Alam

    High power microwave devices especially Traveling Wave Tubes (TWTs) and Backward Wave Oscillators (BWOs) are largely dependent on Slow Wave Structures for efficient beam to RF coupling. In this work, a novel approach of analyzing SWSs is proposed and investigated. Specifically, a rigorous study of helical geometries is carried out and a novel SWS "Half-Ring-Helix" is designed. This Half-Ring-Helix circuit achieves 27% miniaturization and delivers 10dB more gain than conventional helices. A generalization of the helix structures is also proposed in the form of Coupled Transmission Line (CTL). It is demonstrated that control of coupling among the CTLs leads to new propagation properties. With this in mind, a novel geometry referred to as "Curved Ring-Bar" is introduced. This geometry is shown to deliver 1MW power across a 33% bandwidth. Notably, this is the first demonstration of MW power TWT across large bandwidth. The CTL is further expanded to enable engineered propagation characteristics. This is done by introducing CTLs having non-identical transmission lines and CTLs with as many as four transmission lines in the same slow wave structure circuit. These non-identical CTLs are demonstrated to generate fourth order dispersion curves. Building on the property of CTLs, a `butterfly' slow wave structure is developed and demonstrated to provide degenerate band edge (DBE) mode. This mode are known to provide large feld enhancement that can be exploited to design high power backward wave oscillators.

  14. A multi-model assessment of the impact of currents, waves and wind in modelling surface drifters and oil spill

    NASA Astrophysics Data System (ADS)

    De Dominicis, M.; Bruciaferri, D.; Gerin, R.; Pinardi, N.; Poulain, P. M.; Garreau, P.; Zodiatis, G.; Perivoliotis, L.; Fazioli, L.; Sorgente, R.; Manganiello, C.

    2016-11-01

    Validation of oil spill forecasting systems suffers from a lack of data due to the scarcity of oil slick in situ and satellite observations. Drifters (surface drifting buoys) are often considered as proxy for oil spill to overcome this problem. However, they can have different designs and consequently behave in a different way at sea, making it not straightforward to use them for oil spill model validation purposes and to account for surface currents, waves and wind when modelling them. Stemming from the need to validate the MEDESS4MS (Mediterranean Decision Support System for Marine Safety) multi-model oil spill prediction system, which allows access to several ocean, wave and meteorological operational model forecasts, an exercise at sea was carried out to collect a consistent dataset of oil slick satellite observations, in situ data and trajectories of different type of drifters. The exercise, called MEDESS4MS Serious Game 1 (SG1), took place in the Elba Island region (Western Mediterranean Sea) during May 2014. Satellite images covering the MEDESS4MS SG1 exercise area were acquired every day and, in the case an oil spill was observed from satellite, vessels of the Italian Coast Guard (ITCG) were sent in situ to confirm the presence of the pollution. During the exercise one oil slick was found in situ and drifters, with different water-following characteristics, were effectively deployed into the oil slick and then monitored in the following days. Although it was not possible to compare the oil slick and drifter trajectories due to a lack of satellite observations of the same oil slick in the following days, the oil slick observations in situ and drifters trajectories were used to evaluate the quality of MEDESS4MS multi-model currents, waves and winds by using the MEDSLIK-II oil spill model. The response of the drifters to surface ocean currents, different Stokes drift parameterizations and wind drag has been examined. We found that the surface ocean currents

  15. Convectively coupled Kelvin waves in aquachannel simulations: 2. Life cycle and dynamical-convective coupling

    NASA Astrophysics Data System (ADS)

    Blanco, Joaquín. E.; Nolan, David S.; Mapes, Brian E.

    2016-10-01

    This second part of a two-part study uses Weather Research and Forecasting simulations with aquachannel and aquapatch domains to investigate the time evolution of convectively coupled Kelvin waves (CCKWs). Power spectra, filtering, and compositing are combined with object-tracking methods to assess the structure and phase speed propagation of CCKWs during their strengthening, mature, and decaying phases. In this regard, we introduce an innovative approach to more closely investigate the wave (Kelvin) versus entity (super cloud cluster or "SCC") dualism. In general, the composite CCKW structures represent a dynamical response to the organized convective activity. However, pressure and thermodynamic fields in the boundary layer behave differently. Further analysis of the time evolution of pressure and low-level moist static energy finds that these fields propagate eastward as a "moist" Kelvin wave (MKW), faster than the envelope of organized convection or SCC. When the separation is sufficiently large the SCC dissipates, and a new SCC generates to the east, in the region of strongest negative pressure perturbations. We revisit the concept itself of the "coupling" between convection and dynamics, and we also propose a conceptual model for CCKWs, with a clear distinction between the SCC and the MKW components.

  16. Quantifying the Role of Atmospheric Forcing in Ice Edge Retreat and Advance Including Wind-Wave Coupling

    DTIC Science & Technology

    2015-09-30

    Quantifying the Role of Atmospheric Forcing in Ice Edge Retreat and Advance Including Wind- Wave Coupling Peter S. Guest (NPS Technical Contact) Naval...surface fluxes and ocean waves in coupled models in the Beaufort and Chukchi Seas. 2. Understand the physics of heat and mass transfer from the ocean...to the atmosphere. 3. Improve forecasting of waves on the open ocean and in the marginal ice zone. 2 OBJECTIVES 1. Quantifying the open-ocean

  17. High-harmonic fast magnetosonic wave coupling, propagation, and heating in a spherical torus plasma

    NASA Astrophysics Data System (ADS)

    Menard, J.; Majeski, R.; Kaita, R.; Ono, M.; Munsat, T.; Stutman, D.; Finkenthal, M.

    1999-05-01

    A novel rotatable two-strap antenna has been installed in the current drive experiment upgrade (CDX-U) [T. Jones, Ph.D. thesis, Princeton University (1995)] in order to investigate high-harmonic fast wave coupling, propagation, and electron heating as a function of strap angle and strap phasing in a spherical torus plasma. Radio-frequency-driven sheath effects are found to fit antenna loading trends at very low power and become negligible above a few kilowatts. At sufficiently high power, the measured coupling efficiency as a function of strap angle is found to agree favorably with cold plasma wave theory. Far-forward microwave scattering from wave-induced density fluctuations in the plasma core tracks the predicted fast wave loading as the antenna is rotated. Signs of electron heating during rf power injection have been observed in CDX-U with central Thomson scattering, impurity ion spectroscopy, and Langmuir probes. While these initial results appear promising, damping of the fast wave on thermal ions at high ion-cyclotron-harmonic number may compete with electron damping at sufficiently high ion β—possibly resulting in a significantly reduced current drive efficiency and production of a fast ion population. Preliminary results from ray-tracing calculations which include these ion damping effects are presented.

  18. An Arctic Ice/Ocean Coupled Model with Wave Interactions

    DTIC Science & Technology

    2014-09-30

    for reducing this burden, to Washington Headquarters Services, Directorate for Information Operations and Reports, 1215 Jefferson Davis Highway, Suite...an AI on the current project, with remuneration that takes his salary to 1 FTE. SWARP will develop downstream services for sea ice and waves

  19. Coupled effects of chemotaxis and growth on traveling bacterial waves.

    PubMed

    Yan, Zhifeng; Bouwer, Edward J; Hilpert, Markus

    2014-08-01

    Traveling bacterial waves are capable of improving contaminant remediation in the subsurface. It is fairly well understood how bacterial chemotaxis and growth separately affect the formation and propagation of such waves. However, their interaction is not well understood. We therefore perform a modeling study to investigate the coupled effects of chemotaxis and growth on bacterial migration, and examine their effects on contaminant remediation. We study the waves by using different initial electron acceptor concentrations for different bacteria and substrate systems. Three types of traveling waves can occur: a chemotactic wave due to the biased movement of chemotactic bacteria resulting from metabolism-generated substrate concentration gradients; a growth/decay/motility wave due to a dynamic equilibrium between bacterial growth, decay and random motility; and an integrated wave due to the interaction between bacterial chemotaxis and growth. Chemotaxis hardly enhances the bacterial propagation if it is too weak to form a chemotactic wave or its wave speed is less than half of the growth/decay/motility wave speed. However, chemotaxis significantly accelerates bacterial propagation once its wave speed exceeds the growth/decay/motility wave speed. When convection occurs, it speeds up the growth/decay/motility wave but slows down or even eliminates the chemotactic wave due to the dispersion. Bacterial survival proves particularly important for bacterial propagation. Therefore we develop a conceptual model to estimate the speed of growth/decay/motility waves. Copyright © 2014 Elsevier B.V. All rights reserved.

  20. Gap Junction Coupling and Calcium Waves in the Pancreatic Islet

    PubMed Central

    Benninger, Richard K. P.; Zhang, Min; Head, W. Steven; Satin, Leslie S.; Piston, David W.

    2008-01-01

    The pancreatic islet is a highly coupled, multicellular system that exhibits complex spatiotemporal electrical activity in response to elevated glucose levels. The emergent properties of islets, which differ from those arising in isolated islet cells, are believed to arise in part by gap junctional coupling, but the mechanisms through which this coupling occurs are poorly understood. To uncover these mechanisms, we have used both high-speed imaging and theoretical modeling of the electrical activity in pancreatic islets under a reduction in the gap junction mediated electrical coupling. Utilizing islets from a gap junction protein connexin 36 knockout mouse model together with chemical inhibitors, we can modulate the electrical coupling in the islet in a precise manner and quantify this modulation by electrophysiology measurements. We find that after a reduction in electrical coupling, calcium waves are slowed as well as disrupted, and the number of cells showing synchronous calcium oscillations is reduced. This behavior can be reproduced by computational modeling of a heterogeneous population of β-cells with heterogeneous levels of electrical coupling. The resulting quantitative agreement between the data and analytical models of islet connectivity, using only a single free parameter, reveals the mechanistic underpinnings of the multicellular behavior of the islet. PMID:18805925

  1. Modeling and experimental investigation of thermal-mechanical-electric coupling dynamics in a standing wave ultrasonic motor

    NASA Astrophysics Data System (ADS)

    Li, Xiang; Yao, Zhiyuan; He, Yigang; Dai, Shichao

    2017-09-01

    Ultrasonic motor operation relies on high-frequency vibration of a piezoelectric vibrator and interface friction between the stator and rotor/slider, which can cause temperature rise of the motor under continuous operation, and can affect motor parameters and performance in turn. In this paper, an integral model is developed to study the thermal-mechanical-electric coupling dynamics in a typical standing wave ultrasonic motor. Stick-slip motion at the contact interface and the temperature dependence of material parameters of the stator are taken into account in this model. The elastic, piezoelectric and dielectric material coefficients of the piezoelectric ceramic, as a function of temperature, are determined experimentally using a resonance method. The critical parameters in the model are identified via measured results. The resulting model can be used to evaluate the variation in output characteristics of the motor caused by the thermal-mechanical-electric coupling effects. Furthermore, the dynamic temperature rise of the motor can be accurately predicted under different input parameters using the developed model, which will contribute to improving the reliable life of a motor for long-term running.

  2. On the Periodic Solutions of the Five-Dimensional Lorenz Equation Modeling Coupled Rosby Waves and Gravity Waves

    NASA Astrophysics Data System (ADS)

    Carvalho, Tiago; Llibre, Jaume

    2017-06-01

    Lorenz studied the coupled Rosby waves and gravity waves using the differential system U˙ = -VW + bVZ,V˙ = UW - bUZ,Ẇ = -UV,Ẋ = -Z,Ż = bUV + X. This system has the two first integrals H1 = U2 + V2,H 2 = V2 + W2 + X2 + Z2. Our main result shows that in each invariant set {H1 = h1 > 0}∩{H2 = h2 > 0} there are at least four (resp., 2) periodic solutions of the differential system with b≠0 and h2 > h1 (resp., h2 < h1).

  3. Crack Detection in Plates Using Coupled Rayleigh-Like Waves

    NASA Astrophysics Data System (ADS)

    Masserey, B.; Fromme, P.

    2008-02-01

    The use of coupled Rayleigh-like waves in aluminum plates with a view towards the non-destructive inspection of aircraft structures has been investigated experimentally and theoretically. Rayleigh-like waves transfer energy between both plate surfaces with a characteristic distance called the beatlength. A simple, analytical model and finite difference calculations are used to describe the reflection of Rayleigh-like waves at surface defects. Good agreement has been achieved with experimental results using either standard pulse-echo or laser interferometer measurements. The sensitivity for the detection and localization of small defects on both plate surfaces has been found to be very good. Selecting appropriate excitation frequency and position, a significant part of the energy of the Rayleigh-like wave can be transmitted past surface features, allowing the remote detection of defects in areas where access is restricted.

  4. Traveling wave ultrasonic motor: coupling effects in free stator.

    PubMed

    Frayssignes, H; Briot, R

    2003-03-01

    Generally a stator of traveling wave ultrasonic motor (TWUM) consists of piezoelectric transducers (annular plate or rods) coupled by the way of a metallic ring. These transducers divided into halves are excited independently by two electrical signals with different phases of about 90 degrees. So an elastic traveling wave propagates along the circumference of the ring and a rotor pressed on this vibrating surface is then driven by the stator via contact forces. Many difficulties appear in developing TWUM because the contact between the stator and the rotor via a frictional material is very important. However that may be, the first stage consists in obtaining a vibrating stator with optimum characteristics with two symmetrical phases. The aim of this paper is to discuss some coupling effects in a free stator through an enhanced equivalent circuit model. A simple experimental method based on impedance measurements is performed to estimate the coupling characteristics at a low driving voltage. This paper reports results obtained with the free stator of the well known piezoelectric ultrasonic motor "USR60" by Shinsei Co. Ltd. Since the stator behaves as an elastic body, interactions between the two electrical inputs might be described by the introduction of a coupling oscillator. The comparison of experimental and theoretical results leads to validate the new equivalent circuit of the free stator. The presence of coupling impedance could imply a change of electrical supply condition to optimize the TWUM efficiency. The effects of unbalanced features for each electrical input and the applicability of the proposed model to actual operating condition are discussed in the paper. Copyright 2002 Elsevier Science B.V.

  5. Traveling waves in a coupled reaction-diffusion and difference model of hematopoiesis

    NASA Astrophysics Data System (ADS)

    Adimy, M.; Chekroun, A.; Kazmierczak, B.

    2017-04-01

    The formation and development of blood cells is a very complex process, called hematopoiesis. This process involves a small population of cells called hematopoietic stem cells (HSCs). The HSCs are undifferentiated cells, located in the bone marrow before they become mature blood cells and enter the blood stream. They have a unique ability to produce either similar cells (self-renewal), or cells engaged in one of different lineages of blood cells: red blood cells, white cells and platelets (differentiation). The HSCs can be either in a proliferating or in a quiescent phase. In this paper, we distinguish between dividing cells that enter directly to the quiescent phase and dividing cells that return to the proliferating phase to divide again. We propose a mathematical model describing the dynamics of HSC population, taking into account their spatial distribution. The resulting model is a coupled reaction-diffusion equation and difference equation with delay. We study the existence of monotone traveling wave fronts and the asymptotic speed of spread.

  6. Modeling Wave-Ice Interactions in the Marginal Ice Zone

    NASA Astrophysics Data System (ADS)

    Orzech, Mark; Shi, Fengyan; Bateman, Sam; Veeramony, Jay; Calantoni, Joe

    2015-04-01

    The small-scale (O(m)) interactions between waves and ice floes in the marginal ice zone (MIZ) are investigated with a coupled model system. Waves are simulated with the non-hydrostatic finite-volume model NHWAVE (Ma et al., 2012) and ice floes are represented as bonded collections of smaller particles with the discrete element system LIGGGHTS (Kloss et al., 2012). The physics of fluid and ice are recreated as authentically as possible, to allow the coupled system to supplement and/or substitute for more costly and demanding field experiments. The presentation will first describe the development and validation of the coupled system, then discuss the results of a series of virtual experiments in which ice floe and wave characteristics are varied to examine their effects on energy dissipation, MIZ floe size distribution, and ice pack retreat rates. Although Wadhams et al. (1986) suggest that only a small portion (roughly 10%) of wave energy entering the MIZ is reflected, dissipation mechanisms for the remaining energy have yet to be delineated or measured. The virtual experiments are designed to focus on specific properties and processes - such as floe size and shape, collision and fracturing events, and variations in wave climate - and measure their relative roles the transfer of energy and momentum from waves to ice. Questions to be examined include: How is energy dissipated by ice floe collisions, fracturing, and drag, and how significant is the wave attenuation associated with each process? Do specific wave/floe length scale ratios cause greater wave attenuation? How does ice material strength affect the rate of wave energy loss? The coupled system will ultimately be used to test and improve upon wave-ice parameterizations for large-scale climate models. References: >Kloss, C., C. Goniva, A. Hager, S. Amberger, and S. Pirker (2012). Models, algorithms and validation for opensource DEM and CFD-DEM. Progress in Computational Fluid Dynamics 12(2/3), 140-152. >Ma, G

  7. Online coupled regional meteorology-chemistry models in Europe: current status and prospects

    NASA Astrophysics Data System (ADS)

    Baklanov, A.; Schluenzen, K. H.; Suppan, P.; Baldasano, J.; Brunner, D.; Aksoyoglu, S.; Carmichael, G.; Douros, J.; Flemming, J.; Forkel, R.; Galmarini, S.; Gauss, M.; Grell, G.; Hirtl, M.; Joffre, S.; Jorba, O.; Kaas, E.; Kaasik, M.; Kallos, G.; Kong, X.; Korsholm, U.; Kurganskiy, A.; Kushta, J.; Lohmann, U.; Mahura, A.; Manders-Groot, A.; Maurizi, A.; Moussiopoulos, N.; Rao, S. T.; Savage, N.; Seigneur, C.; Sokhi, R.; Solazzo, E.; Solomos, S.; Sørensen, B.; Tsegas, G.; Vignati, E.; Vogel, B.; Zhang, Y.

    2013-05-01

    paving the way towards a new generation of online integrated atmospheric chemical transport and meteorology modelling with two-way interactions between different atmospheric processes including dynamics, chemistry, clouds, radiation, boundary layer and emissions. As its first task, we summarise the current status of European modelling practices and experience with online coupled modelling of meteorology with atmospheric chemistry including feedback mechanisms and attempt reviewing the various issues connected to the different modules of such online coupled models but also providing recommendations for coping with them for the benefit of the modelling community at large.

  8. Current-induced spin wave Doppler shift

    NASA Astrophysics Data System (ADS)

    Bailleul, Matthieu

    2010-03-01

    In metal ferromagnets -namely Fe, Co and Ni and their alloys- magnetism and electrical transport are strongly entangled (itinerant magnetism). This results in a number of properties such as the tunnel and giant magnetoresistance (i.e. the dependence of the electrical resistance on the magnetic state) and the more recently addressed spin transfer (i.e. the ability to manipulate the magnetic state with the help of an electrical current). The spin waves, being the low-energy elementary excitations of any ferromagnet, also exist in itinerant magnets, but they are expected to exhibit some peculiar properties due the itinerant character of the carriers. Accessing these specific properties experimentally could shed a new light on the microscopic mechanism governing itinerant magnetism, which -in turn- could help in optimizing material properties for spintronics applications. As a simple example of these specific properties, it was predicted theoretically that forcing a DC current through a ferromagnetic metal should induce a shift of the frequency of the spin waves [1,2]. This shift can be identified to a Doppler shift undergone by the electron system when it is put in motion by the electrical current. We will show how detailed spin wave measurements allow one to access this current-induced Doppler shift [3]. From an experimental point of view, we will discuss the peculiarities of propagating spin wave spectroscopy experiments carried out at a sub-micrometer length-scale and with MHz frequency resolution. Then, we will discuss the measured value of the Doppler shift in the context of both the old two-current model of spin-polarized transport and the more recent model of adiabatic spin transfer torque. [4pt] [1] P.Lederer and D.L. Mills, Phys.Rev. 148, 542 (1966).[0pt] [2] J. Fernandez-Rossier et al., Phys. Rev. B 69, 174412 (2004)[0pt] [3] V. Vlaminck and M. Bailleul, Science 322, 410 (2008).

  9. Small-scale open ocean currents have large effects on wind wave heights

    NASA Astrophysics Data System (ADS)

    Ardhuin, Fabrice; Gille, Sarah T.; Menemenlis, Dimitris; Rocha, Cesar B.; Rascle, Nicolas; Chapron, Bertrand; Gula, Jonathan; Molemaker, Jeroen

    2017-06-01

    Tidal currents and large-scale oceanic currents are known to modify ocean wave properties, causing extreme sea states that are a hazard to navigation. Recent advances in the understanding and modeling capability of open ocean currents have revealed the ubiquitous presence of eddies, fronts, and filaments at scales 10-100 km. Based on realistic numerical models, we show that these structures can be the main source of variability in significant wave heights at scales less than 200 km, including important variations down to 10 km. Model results are consistent with wave height variations along satellite altimeter tracks, resolved at scales larger than 50 km. The spectrum of significant wave heights is found to be of the order of 70>>2/>(g2>>2>) times the current spectrum, where >> is the spatially averaged significant wave height, >> is the energy-averaged period, and g is the gravity acceleration. This variability induced by currents has been largely overlooked in spite of its relevance for extreme wave heights and remote sensing.Plain Language SummaryWe show that the variations in <span class="hlt">currents</span> at scales 10 to 100 km are the main source of variations in <span class="hlt">wave</span> heights at the same scales. Our work uses a combination of realistic numerical <span class="hlt">models</span> for <span class="hlt">currents</span> and <span class="hlt">waves</span> and data from the Jason-3 and SARAL/AltiKa satellites. This finding will be of interest for the investigation of extreme <span class="hlt">wave</span> heights, remote sensing, and air-sea interactions. As an immediate application, the present results will help constrain the error budget of the up-coming satellite missions, in particular the Surface Water and Ocean Topography (SWOT) mission, and decide how the data will have to be processed to arrive at accurate sea level and <span class="hlt">wave</span> measurements. It will also help in the analysis of <span class="hlt">wave</span> measurements by the CFOSAT satellite.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008JGRC..113.7018F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008JGRC..113.7018F"><span><span class="hlt">Waves</span> plus <span class="hlt">currents</span> at a right angle: The rippled bed case</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Faraci, C.; Foti, E.; Musumeci, R. E.</p> <p>2008-07-01</p> <p>The present paper deals with <span class="hlt">wave</span> plus <span class="hlt">current</span> flow over a fixed rippled bed. More precisely, modifications of the <span class="hlt">current</span> profiles due to the superimposition of orthogonal cylindrical <span class="hlt">waves</span> have been investigated experimentally. Since the experimental setup permitted only the <span class="hlt">wave</span> dominated regime to be investigated (i.e., the regime where orbital velocity is larger than <span class="hlt">current</span> velocity), also a numerical k-ɛ turbulence closure <span class="hlt">model</span> has been developed in order to study a wider range of parameters, thus including the <span class="hlt">current</span> dominated regime (i.e., where <span class="hlt">current</span> velocity is larger than <span class="hlt">wave</span> orbital one). In both cases a different response with respect to the flat bed case has been found. Indeed, in the flat bed case laminar <span class="hlt">wave</span> boundary layers in a <span class="hlt">wave</span> dominated regime induce a decrease in bottom shear stresses, while the presence of a rippled bed behaves as a macroroughness, which causes the <span class="hlt">wave</span> boundary layer to become turbulent and therefore the <span class="hlt">current</span> velocity near the bottom to be smaller than the one in the case of <span class="hlt">current</span> only, with a consequent increase in the <span class="hlt">current</span> bottom roughness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21117735','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21117735"><span>A finite difference method for a <span class="hlt">coupled</span> <span class="hlt">model</span> of <span class="hlt">wave</span> propagation in poroelastic materials.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Yang; Song, Limin; Deffenbaugh, Max; Toksöz, M Nafi</p> <p>2010-05-01</p> <p>A computational method for time-domain multi-physics simulation of <span class="hlt">wave</span> propagation in a poroelastic medium is presented. The medium is composed of an elastic matrix saturated with a Newtonian fluid, and the method operates on a digital representation of the medium where a distinct material phase and properties are specified at each volume cell. The dynamic response to an acoustic excitation is <span class="hlt">modeled</span> mathematically with a <span class="hlt">coupled</span> system of equations: elastic <span class="hlt">wave</span> equation in the solid matrix and linearized Navier-Stokes equation in the fluid. Implementation of the solution is simplified by introducing a common numerical form for both solid and fluid cells and using a rotated-staggered-grid which allows stable solutions without explicitly handling the fluid-solid boundary conditions. A stability analysis is presented which can be used to select gridding and time step size as a function of material properties. The numerical results are shown to agree with the analytical solution for an idealized porous medium of periodically alternating solid and fluid layers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002AGUFMNG21C0949L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002AGUFMNG21C0949L"><span><span class="hlt">Wave-Wave</span> <span class="hlt">Coupling</span> and Disasters: The 1985 Mexico Earthquake and the 2001 WTC Collapse</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lomnitz, C.</p> <p>2002-12-01</p> <p><span class="hlt">Wave-wave</span> <span class="hlt">coupling</span> occurs in the presence of weak nonlinearity. It can generate quite dramatic, unexpected effects. In the 1985 earthquake disaster in Mexico City more than 400 high-rise buildings collapsed on soft ground with a loss of life of around 10,000. The emergence of a large, monochromatic, coherent ground <span class="hlt">wave</span> was an unforeseen factor. Linear <span class="hlt">modeling</span> failed to reproduce the main features of this signal including the prominent spectral peak close to the resonant frequency of the high-rise buildings, and an extremely long time duration (more than five minutes). The signal was apparently due to <span class="hlt">coupling</span> of a fundamental Rayleigh mode to the quarter-wavelength shear resonance in the surface mud layer through their common frequency at 0.4 Hz. An additional unexpected feature was the low attenuation of these modes in the mud layer, and the presence of prograde particle motion. Prograde rotation, though not necessarily caused by nonlinear effects, will <span class="hlt">couple</span> with structural modes of vibration that tend to destabilize a tall building, much like a tall ship in ocean <span class="hlt">waves</span>. Such unanticipated features may play a critical role in earthquake disasters on soft ground. A related case is the World Trade Center disaster of 11 September 2001, which was presumed to be due to gradual heat softening of steel girders. If so, the Twin Towers should have leaned over sideways but actually the collapse occurred vertically and quite suddenly. A likely alternative is <span class="hlt">coupling</span> between a fireball caused by a phase transition between low- and high-oxygen consumption modes in burning jet fuel: (low-oxygen) 2CnH2n+2 + (n+1)O2 = nC2 + (2n+2)H2O, (1) (high-oxygen) 2CnH2n+2 + (3n+1)O2 = 2nCO2 + (2n+2)H2O, (2) and a pressure pulse propagating vertically inside the tubular structure. The pulse would have taken out the concrete floors, thus initiating collapse by implosion of the structural shell. Linear thinking may fail to anticipate <span class="hlt">coupling</span>, and thus appropriate preventive measures may</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19740022729','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19740022729"><span>Ocean dynamics studies. [of <span class="hlt">current-wave</span> interactions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1974-01-01</p> <p>Both the theoretical and experimental investigations into <span class="hlt">current-wave</span> interactions are discussed. The following three problems were studied: (1) the dispersive relation of a random gravity-capillary <span class="hlt">wave</span> field; (2) the changes of the statistical properties of surface <span class="hlt">waves</span> under the influence of <span class="hlt">currents</span>; and (3) the interaction of capillary-gravity with the nonuniform <span class="hlt">currents</span>. <span class="hlt">Wave</span> <span class="hlt">current</span> interaction was measured and the feasibility of using such measurements for remote sensing of surface <span class="hlt">currents</span> was considered. A laser probe was developed to measure the surface statistics, and the possibility of using <span class="hlt">current-wave</span> interaction as a means of <span class="hlt">current</span> measurement was demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMOS22A..04R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMOS22A..04R"><span>A <span class="hlt">coupled</span> <span class="hlt">wave</span>-hydrodynamic <span class="hlt">model</span> of a highly frictional atoll reef system: mechanisms for flow, connectivity, and ecological implications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rogers, J.; Monismith, S. G.; Fringer, O. B.; Koweek, D.; Dunbar, R. B.</p> <p>2016-12-01</p> <p>We present a hydrodynamic analysis of an atoll system from <span class="hlt">modeling</span> simulations using a <span class="hlt">coupled</span> <span class="hlt">wave</span> and three-dimensional hydrodynamic <span class="hlt">model</span> (COAWST) applied to Palmyra Atoll in the Central Pacific. This is the first time the vortex force formalism has been applied in a highly frictional reef environment. The <span class="hlt">model</span> results agree well with field observations considering the <span class="hlt">model</span> complexity in terms of bathymetry, bottom roughness, and forcing (<span class="hlt">waves</span>, wind, metrological, tides, regional boundary conditions), and open boundary conditions. At the atoll scale, strong regional flows create flow separation and a well-defined wake, similar to 2D flow past a cylinder. Circulation within the atoll is typically forced by <span class="hlt">waves</span> and tides, with strong <span class="hlt">waves</span> from the north driving flow from north to south across the atoll, and from east to west through the lagoon system. Bottom stress is significant for depths less than about 60 m, and in addition to the <span class="hlt">model</span> bathymetry, is important for correct representation of flow in the <span class="hlt">model</span>. Connectivity within the atoll system shows that the general trends follow the mean flow paths. However, some connectivity exists between all regions of the atoll system due to nonlinear processes such as eddies and tidal phasing. While high mean flow and travel time less than 20 hours appears to differentiate very productive coral regions, low temperature and moderate <span class="hlt">wave</span> stress appear to be the most ideal conditions for high coral cover on Palmyra.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MolPh.116.1483S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MolPh.116.1483S"><span>Diagonal Born-Oppenheimer correction for <span class="hlt">coupled</span>-cluster <span class="hlt">wave</span>-functions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shamasundar, K. R.</p> <p>2018-06-01</p> <p>We examine how geometry-dependent normalisation freedom of electronic <span class="hlt">wave</span>-functions affects extraction of a meaningful diagonal Born-Oppenheimer correction (DBOC) to the ground-state Born-Oppenheimer potential energy surface (PES). By viewing this freedom as a kind of gauge-freedom, it is shown that DBOC and the resulting associated mass-dependent adiabatic PES are gauge-invariant quantities. A sum-over-states (SOS) formula for DBOC which explicitly exhibits this invariance is derived. A biorthogonal formulation suitable for DBOC computations using standard unnormalised <span class="hlt">coupled</span>-cluster (CC) <span class="hlt">wave</span>-functions is presented. This is shown to lead to a biorthogonal version of SOS formula with similar properties. On this basis, different computational schemes for evaluating DBOC using approximate CC <span class="hlt">wave</span>-functions are derived. One of this agrees with the formula used in the <span class="hlt">current</span> literature. The connection to adiabatic-to-diabatic transformations in non-adiabatic dynamics is explored and complications arising from biorthogonal nature of CC theory are identified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014JPhA...47H5001L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014JPhA...47H5001L"><span>Sustained <span class="hlt">currents</span> in <span class="hlt">coupled</span> diffusive systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Larralde, Hernán; Sanders, David P.</p> <p>2014-08-01</p> <p><span class="hlt">Coupling</span> two diffusive systems may give rise to a nonequilibrium stationary state (NESS) with a non-trivial persistent, circulating <span class="hlt">current</span>. We study a simple example that is exactly soluble, consisting of random walkers with different biases towards a reflecting boundary, <span class="hlt">modelling</span>, for example, Brownian particles with different charge states in an electric field. We obtain analytical expressions for the concentrations and <span class="hlt">currents</span> in the NESS for this <span class="hlt">model</span>, and exhibit the main features of the system by numerical simulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhyD..325...25D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhyD..325...25D"><span>Traveling <span class="hlt">wave</span> solutions in a chain of periodically forced <span class="hlt">coupled</span> nonlinear oscillators</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Duanmu, M.; Whitaker, N.; Kevrekidis, P. G.; Vainchtein, A.; Rubin, J. E.</p> <p>2016-06-01</p> <p>Motivated by earlier studies of artificial perceptions of light called phosphenes, we analyze traveling <span class="hlt">wave</span> solutions in a chain of periodically forced <span class="hlt">coupled</span> nonlinear oscillators <span class="hlt">modeling</span> this phenomenon. We examine the discrete <span class="hlt">model</span> problem in its co-traveling frame and systematically obtain the corresponding traveling <span class="hlt">waves</span> in one spatial dimension. Direct numerical simulations as well as linear stability analysis are employed to reveal the parameter regions where the traveling <span class="hlt">waves</span> are stable, and these <span class="hlt">waves</span> are, in turn, connected to the standing <span class="hlt">waves</span> analyzed in earlier work. We also consider a two-dimensional extension of the <span class="hlt">model</span> and demonstrate the robust evolution and stability of planar fronts. Our simulations also suggest the radial fronts tend to either annihilate or expand and flatten out, depending on the phase value inside and the parameter regime. Finally, we observe that solutions that initially feature two symmetric fronts with bulged centers evolve in qualitative agreement with experimental observations of phosphenes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1257982-traveling-wave-solutions-chain-periodically-forced-coupled-nonlinear-oscillators','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1257982-traveling-wave-solutions-chain-periodically-forced-coupled-nonlinear-oscillators"><span>Traveling <span class="hlt">wave</span> solutions in a chain of periodically forced <span class="hlt">coupled</span> nonlinear oscillators</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Duanmu, M.; Whitaker, N.; Kevrekidis, P. G.; ...</p> <p>2016-02-27</p> <p>Artificial perceptions of light called phosphenes were motivated by earlier studies. We analyze traveling <span class="hlt">wave</span> solutions in a chain of periodically forced <span class="hlt">coupled</span> nonlinear oscillators <span class="hlt">modeling</span> this phenomenon. We examine the discrete <span class="hlt">model</span> problem in its co-traveling frame and systematically obtain the corresponding traveling <span class="hlt">waves</span> in one spatial dimension. Direct numerical simulations as well as linear stability analysis are employed to reveal the parameter regions where the traveling <span class="hlt">waves</span> are stable, and these <span class="hlt">waves</span> are, in turn, connected to the standing <span class="hlt">waves</span> analyzed in earlier work. We also consider a two-dimensional extension of the <span class="hlt">model</span> and demonstrate the robust evolutionmore » and stability of planar fronts. Moreover, our simulations also suggest the radial fronts tend to either annihilate or expand and flatten out, depending on the phase value inside and the parameter regime. Finally, we observe that solutions that initially feature two symmetric fronts with bulged centers evolve in qualitative agreement with experimental observations of phosphenes.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1257982','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1257982"><span>Traveling <span class="hlt">wave</span> solutions in a chain of periodically forced <span class="hlt">coupled</span> nonlinear oscillators</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>Duanmu, M.; Whitaker, N.; Kevrekidis, P. G.</p> <p></p> <p>Artificial perceptions of light called phosphenes were motivated by earlier studies. We analyze traveling <span class="hlt">wave</span> solutions in a chain of periodically forced <span class="hlt">coupled</span> nonlinear oscillators <span class="hlt">modeling</span> this phenomenon. We examine the discrete <span class="hlt">model</span> problem in its co-traveling frame and systematically obtain the corresponding traveling <span class="hlt">waves</span> in one spatial dimension. Direct numerical simulations as well as linear stability analysis are employed to reveal the parameter regions where the traveling <span class="hlt">waves</span> are stable, and these <span class="hlt">waves</span> are, in turn, connected to the standing <span class="hlt">waves</span> analyzed in earlier work. We also consider a two-dimensional extension of the <span class="hlt">model</span> and demonstrate the robust evolutionmore » and stability of planar fronts. Moreover, our simulations also suggest the radial fronts tend to either annihilate or expand and flatten out, depending on the phase value inside and the parameter regime. Finally, we observe that solutions that initially feature two symmetric fronts with bulged centers evolve in qualitative agreement with experimental observations of phosphenes.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMOS33A1802K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMOS33A1802K"><span>Observations of Convectively <span class="hlt">Coupled</span> Kelvin <span class="hlt">Waves</span> forced by Extratropical <span class="hlt">Wave</span> Activity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kiladis, G. N.; Biello, J. A.; Straub, K. H.</p> <p>2012-12-01</p> <p>It is well established by observations that deep tropical convection can in certain situations be forced by extratropical Rossby <span class="hlt">wave</span> activity. Such interactions are a well-known feature of regions of upper level westerly flow, and in particular where westerlies and equatorward <span class="hlt">wave</span> guiding by the basic state occur at low enough latitudes to interact with tropical and subtropical moisture sources. In these regions convection is commonly initiated ahead of upper level troughs, characteristic of forcing by quasi-geostrophic dynamics. However, recent observational evidence indicates that extratropical <span class="hlt">wave</span> activity is also associated with equatorial convection even in regions where there is a "critical line" to Rossby <span class="hlt">wave</span> propagation at upper levels, that is, where the zonal phase speed of the <span class="hlt">wave</span> is equal to the zonal flow speed. A common manifestation of this type of interaction involves the initiation of convectively <span class="hlt">coupled</span> Kelvin <span class="hlt">waves</span>, as well as mixed Rossby-gravity (MRG) <span class="hlt">waves</span>. These <span class="hlt">waves</span> are responsible for a large portion of the convective variability within the ITCZ over the Indian, Pacific, and Atlantic sectors, as well as within the Amazon Basin of South America. For example, Kelvin <span class="hlt">waves</span> originating within the western Pacific ITCZ are often triggered by Rossby <span class="hlt">wave</span> activity propagating into the Australasian region from the South Indian Ocean extratropics. At other times, Kelvin <span class="hlt">waves</span> are seen to originate along the eastern slope of the Andes. In the latter case the initial forcing is sometimes linked to a low-level "pressure surge," initiated by <span class="hlt">wave</span> activity propagating equatorward from the South Pacific storm track. In yet other cases, such as over Africa, the forcing appears to be related to <span class="hlt">wave</span> activity in the extratropics which is not necessarily propagating into low latitudes, but appears to "project" onto the Kelvin structure, in line with past theoretical and <span class="hlt">modeling</span> studies. Observational evidence for extratropical forcing of Kelvin and MRG</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/2018JPhCS.991a2061M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS.991a2061M"><span>Full thermomechanical <span class="hlt">coupling</span> in <span class="hlt">modelling</span> of micropolar thermoelasticity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Murashkin, E. V.; Radayev, Y. N.</p> <p>2018-04-01</p> <p>The present paper is devoted to plane harmonic <span class="hlt">waves</span> of displacements and microrotations propagating in fully <span class="hlt">coupled</span> thermoelastic continua. The analysis is carried out in the framework of linear conventional thermoelastic micropolar continuum <span class="hlt">model</span>. The reduced energy balance equation and the special form of the Helmholtz free energy are discussed. The constitutive constants providing fully <span class="hlt">coupling</span> of equations of motion and heat conduction are considered. The dispersion equation is derived and analysed in the form bi-cubic and bi-quadratic polynoms product. The equation are analyzed by the computer algebra system Mathematica. Algebraic forms expressed by complex multivalued square and cubic radicals are obtained for wavenumbers of transverse and longitudinal <span class="hlt">waves</span>. The exact forms of wavenumbers of a plane harmonic <span class="hlt">coupled</span> thermoelastic <span class="hlt">waves</span> are computed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA598030','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA598030"><span><span class="hlt">Wave-Current</span> Interaction in Coastal Inlets and River Mouths</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2013-09-30</p> <p>Astoria Canyon buoy operated by the Coastal Data Information Program ( CDIP , buoy # 46248). Three-dimensional <span class="hlt">current</span> fields and bathymetry were...The <span class="hlt">model</span> was initialized with <span class="hlt">wave</span> measurements from CDIP buoy 46248 located at the tip of the Astoria Canyon, and uses <span class="hlt">modeled</span> <span class="hlt">current</span> fields</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3693448','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3693448"><span>Turbulent Water <span class="hlt">Coupling</span> in Shock <span class="hlt">Wave</span> Lithotripsy</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Lautz, Jaclyn; Sankin, Georgy; Zhong, Pei</p> <p>2013-01-01</p> <p>Previous studies have demonstrated that stone comminution decreases with increased pulse repetition frequency as a result of bubble proliferation in the cavitation field of a shock <span class="hlt">wave</span> lithotripter (Pishchalnikov et al., 2011). If cavitation nuclei remain in the propagation path of successive lithotripter pulses, especially in the acoustic <span class="hlt">coupling</span> cushion of the shock <span class="hlt">wave</span> source, they will consume part of the incident <span class="hlt">wave</span> energy, leading to reduced tensile pressure in the focal region and thus lower stone comminution efficiency. We introduce a method to remove cavitation nuclei from the <span class="hlt">coupling</span> cushion between successive shock exposures using a jet of degassed water. As a result, pre-focal bubble nuclei lifetime quantified by B-mode ultrasound imaging was reduced from 7 s to 0.3 s by a jet with an exit velocity of 62 cm/s. Stone fragmentation (percent mass < 2 mm) after 250 shocks delivered at 1 Hz was enhanced from 22 ± 6% to 33 ± 5% (p = 0.007) in water without interposing tissue mimicking materials. Stone fragmentation after 500 shocks delivered at 2 Hz was increased from 18 ± 6% to 28 ± 8% (p = 0.04) with an interposing tissue phantom of 8 cm thick. These results demonstrate the critical influence of cavitation bubbles in the <span class="hlt">coupling</span> cushion on stone comminution and suggest a potential strategy to improve the efficacy of contemporary shock <span class="hlt">wave</span> lithotripters. PMID:23322027</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA580663','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA580663"><span><span class="hlt">Wave</span> <span class="hlt">Current</span> Interactions and <span class="hlt">Wave</span>-blocking Predictions Using NHWAVE <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>2013-03-01</p> <p>Navier-Stokes equation. In this approach, as with previous <span class="hlt">modeling</span> techniques, there is difficulty in simulating the free surface that inhibits accurate...hydrostatic, free - surface , rotational flows in multiple dimensions. It is useful in predicting transformations of surface <span class="hlt">waves</span> and rapidly varied...Stelling, G., and M. Zijlema, 2003: An accurate and efficient finite-differencing algorithm for non-hydrostatic free surface flow with application to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020068099&hterms=Plasma+Ring&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DPlasma%2BRing','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020068099&hterms=Plasma+Ring&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3DPlasma%2BRing"><span>Plasmaspheric Erosion via Plasmasphere <span class="hlt">Coupling</span> to Ring <span class="hlt">Current</span> Plasmas: EUV Observations and <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Adrian, M. L.; Gallagher, D. L.; Khazanov, G. V.; Chsang, S. W.; Liemohn, M. W.; Perez, J. D.; Green, J. L.; Sandel, B. R.; Mitchell, D. G.; Mende, S. B.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20020068099'); toggleEditAbsImage('author_20020068099_show'); toggleEditAbsImage('author_20020068099_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20020068099_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20020068099_hide"></p> <p>2002-01-01</p> <p>During a geomagnetic storm on 24 May 2000, the IMAGE Extreme Ultraviolet (EUV) camera observed a plasmaspheric density trough in the evening sector at L-values inside the plasmapause. Forward <span class="hlt">modeling</span> of this feature has indicated that plasmaspheric densities beyond the outer wall of the trough are well below <span class="hlt">model</span> expectations. This diminished plasma condition suggests the presence of an erosion process due to the interaction of the plasmasphere with ring <span class="hlt">current</span> plasmas. We present an overview of EUV, energetic neutral atom (ENA), and Far Ultraviolet (FUV) camera observations associated with the plasmaspheric density trough of 24 May 2000, as well as forward <span class="hlt">modeling</span> evidence of the lie existence of a plasmaspheric erosion process during this period. FUV proton aurora image analysis, convolution of ENA observations, and ring <span class="hlt">current</span> <span class="hlt">modeling</span> are then presented in an effort to associate the observed erosion with <span class="hlt">coupling</span> between the plasmasphere and ring-<span class="hlt">current</span> plasmas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930022679','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930022679"><span>An efficient <span class="hlt">model</span> for <span class="hlt">coupling</span> structural vibrations with acoustic radiation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Frendi, Abdelkader; Maestrello, Lucio; Ting, LU</p> <p>1993-01-01</p> <p>The scattering of an incident <span class="hlt">wave</span> by a flexible panel is studied. The panel vibration is governed by the nonlinear plate equations while the loading on the panel, which is the pressure difference across the panel, depends on the reflected and transmitted <span class="hlt">waves</span>. Two <span class="hlt">models</span> are used to calculate this structural-acoustic interaction problem. One solves the three dimensional nonlinear Euler equations for the flow-field <span class="hlt">coupled</span> with the plate equations (the fully <span class="hlt">coupled</span> <span class="hlt">model</span>). The second uses the linear <span class="hlt">wave</span> equation for the acoustic field and expresses the load as a double integral involving the panel oscillation (the decoupled <span class="hlt">model</span>). The panel oscillation governed by a system of integro-differential equations is solved numerically and the acoustic field is then defined by an explicit formula. Numerical results are obtained using the two <span class="hlt">models</span> for linear and nonlinear panel vibrations. The predictions given by these two <span class="hlt">models</span> are in good agreement but the computational time needed for the 'fully <span class="hlt">coupled</span> <span class="hlt">model</span>' is 60 times longer than that for 'the decoupled <span class="hlt">model</span>'.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUSMSM34A..08M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUSMSM34A..08M"><span>ULF <span class="hlt">Waves</span> in the Earth's Inner Magnetosphere: Role in Radiation Belt and Ring <span class="hlt">Current</span> Dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mann, I. R.; Murphy, K. R.; Rae, J.; Claudepierre, S. G.; Fennell, J. F.; Baker, D. N.; Reeves, G. D.; Spence, H. E.; Ozeke, L.; Milling, D. K.</p> <p>2013-05-01</p> <p>Ultra-low frequency (ULF) <span class="hlt">waves</span> in the Pc4-5 band can be excited in the magnetosphere by the solar wind. Much recent work has shown how ULF <span class="hlt">wave</span> power is strongly correlated with solar wind speed. However, little attention has been paid the dynamics of ULF <span class="hlt">wave</span> power penetration onto low L-shells in the inner magnetosphere. We use more than a solar cycle of ULF <span class="hlt">wave</span> data, derived from ground-based magnetometer networks, to examine this ULF <span class="hlt">wave</span> power penetration and its dependence on solar wind and geomagnetic activity indices. In time domain data, we show very clearly that dayside ULF <span class="hlt">wave</span> power, spanning more than 4 orders of magnitude, follows solar wind speed variations throughout the whole solar cycle - during periods of sporadic solar maximum ICMEs, during declining phase fast solar wind streams, and at solar minimum, alike. We also show that time domain ULF <span class="hlt">wave</span> power increases during magnetic storms activations, and significantly demonstrate that a deeper ULF <span class="hlt">wave</span> power penetration into the inner magnetosphere occurs during larger negative excursions in Dst. We discuss potential explanations for this low-L ULF <span class="hlt">wave</span> power penetration, including the role of plasma mass density (such as during plasmaspheric erosion), or ring <span class="hlt">current</span> ion instabilities during near-Earth ring <span class="hlt">current</span> penetration. Interestingly, we also show that both ULF <span class="hlt">wave</span> power and SAMPEX MeV electron flux show a remarkable similarity in their penetration to low-L, which suggests that ULF <span class="hlt">wave</span> power penetration may be important for understanding and explaining radiation belt dynamics. Moreover, the correlation of ULF <span class="hlt">wave</span> power with Dst, which peaks at one day lag, suggests the ULF <span class="hlt">waves</span> might also be important for the inward transport of ions into the ring <span class="hlt">current</span>. <span class="hlt">Current</span> ring <span class="hlt">current</span> <span class="hlt">models</span>, which exclude long period ULF <span class="hlt">wave</span> transport, under-estimate the ring <span class="hlt">current</span> during fast solar wind streams which is consistent with a potential role for ULF <span class="hlt">waves</span> in ring <span class="hlt">current</span> energisation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19945138','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19945138"><span><span class="hlt">Modelling</span> <span class="hlt">coupled</span> turbulence - dissolved oxygen dynamics near the sediment-water interface under wind <span class="hlt">waves</span> and sea swell.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chatelain, Mathieu; Guizien, Katell</p> <p>2010-03-01</p> <p>A one-dimensional vertical unsteady numerical <span class="hlt">model</span> for diffusion-consumption of dissolved oxygen (DO) above and below the sediment-water interface was developed to investigate DO profile dynamics under wind <span class="hlt">waves</span> and sea swell (high-frequency oscillatory flows with periods ranging from 2 to 30s). We tested a new approach to <span class="hlt">modelling</span> DO profiles that <span class="hlt">coupled</span> an oscillatory turbulent bottom boundary layer <span class="hlt">model</span> with a Michaelis-Menten based consumption <span class="hlt">model</span>. The flow regime controls both the mean value and the fluctuations of the oxygen mass transfer efficiency during a <span class="hlt">wave</span> cycle, as expressed by the non-dimensional Sherwood number defined with the maximum shear velocity (Sh). The Sherwood number was found to be non-dependent on the sediment biogeochemical activity (mu). In the laminar regime, both cycle-averaged and variance of the Sherwood number are very low (Sh <0.05, VAR(Sh)<0.1%). In the turbulent regime, the cycle-averaged Sherwood number is larger (Sh approximately 0.2). The Sherwood number also has intra-<span class="hlt">wave</span> cycle fluctuations that increase with the <span class="hlt">wave</span> Reynolds number (VAR(Sh) up to 30%). Our computations show that DO mass transfer efficiency under high-frequency oscillatory flows in the turbulent regime are water-side controlled by: (a) the diffusion time across the diffusive boundary layer and (b) diffusive boundary layer dynamics during a <span class="hlt">wave</span> cycle. As a result of these two processes, when the <span class="hlt">wave</span> period decreases, the Sh minimum increases and the Sh maximum decreases. Sh values vary little, ranging from 0.17 to 0.23. For periods up to 30s, oxygen penetration depth into the sediment did not show any intra-<span class="hlt">wave</span> fluctuations. Values for the laminar regime are small (<or=1mm for mu=2000gm(-3)d(-1)) and decrease when the flow period increases. In the turbulent regime, the oxygen penetration depth reaches values up to five times larger than those in the laminar regime, becoming asymptotic as the maximum shear velocity increases. Copyright 2009</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28804266','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28804266"><span>Modulational instability, beak-shaped rogue <span class="hlt">waves</span>, multi-dark-dark solitons and dynamics in pair-transition-<span class="hlt">coupled</span> nonlinear Schrödinger equations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Guoqiang; Yan, Zhenya; Wen, Xiao-Yong</p> <p>2017-07-01</p> <p>The integrable <span class="hlt">coupled</span> nonlinear Schrödinger equations with four-<span class="hlt">wave</span> mixing are investigated. We first explore the conditions for modulational instability of continuous <span class="hlt">waves</span> of this system. Secondly, based on the generalized N -fold Darboux transformation (DT), beak-shaped higher-order rogue <span class="hlt">waves</span> (RWs) and beak-shaped higher-order rogue <span class="hlt">wave</span> pairs are derived for the <span class="hlt">coupled</span> <span class="hlt">model</span> with attractive interaction in terms of simple determinants. Moreover, we derive the simple multi-dark-dark and kink-shaped multi-dark-dark solitons for the <span class="hlt">coupled</span> <span class="hlt">model</span> with repulsive interaction through the generalizing DT. We explore their dynamics and classifications by different kinds of spatial-temporal distribution structures including triangular, pentagonal, 'claw-like' and heptagonal patterns. Finally, we perform the numerical simulations to predict that some dark solitons and RWs are stable enough to develop within a short time. The results would enrich our understanding on nonlinear excitations in many <span class="hlt">coupled</span> nonlinear <span class="hlt">wave</span> systems with transition <span class="hlt">coupling</span> effects.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.2627G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.2627G"><span>Laboratory <span class="hlt">modelling</span> of resonant <span class="hlt">wave-current</span> interaction in the vicinity wind farm masts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gunnoo, Hans; Abcha, Nizar; Garcia-Hermosa, Maria-Isabel; Ezersky, Alexander</p> <p>2015-04-01</p> <p>In the nearest future, by 2020, about 4% of electricity in Europe will be supplied by sea stations operating from renewable sources: ocean thermal energy, <span class="hlt">wave</span> and tidal energy, wind farms. By now the wind stations located in the coastal zone, provide the most part of electricity in different European countries. Meanwhile, effects of wind farms on the environment are not sufficiently studied. We report results of laboratory simulations aimed at investigation of hydrodynamic fields arising in the vicinity of wind farm masts under the action of <span class="hlt">currents</span> and surface <span class="hlt">waves</span>. The main attention is paid to <span class="hlt">modeling</span> the resonance effects when the amplitude of velocity pulsations in the vicinity of the masts under the joint action of <span class="hlt">currents</span> and harmonic <span class="hlt">waves</span> demonstrate significant growth. This resonance can lead to an increase in Reynolds stress on the bottom, intensification of sediment transport and sound generation. The experiments are performed in the 17 meters hydrodynamical channel of laboratory Morphodynamique Continentale et Côtière UMR CNRS 6143. Mast are <span class="hlt">modeled</span> by vertical cylinder placed in a steady flow. Behind the cylinder turbulent Karman vortex street occurs. Results are obtained in interval of Reynolds numbers Re=103 - 104(Re=Ud/v, where U is the velocity of the flow, d is diameter of the cylinder, ν is cinematic viscosity). Harmonic surface <span class="hlt">waves</span> of small amplitude propagating upstream are excited by computer controlled <span class="hlt">wave</span> maker. In the absence of surface <span class="hlt">waves</span>, turbulent Karman street with averaged frequency f is observed. It is revealed experimentally that harmonic surface <span class="hlt">waves</span> with a frequencies closed to 2f can synchronize vortex shedding and increase the amplitude of velocity fluctuations in the wake of the cylinder. Map of regimes is found on the parameter plane amplitude of the surface <span class="hlt">wave</span> - <span class="hlt">wave</span> frequency. In order to distinguish the synchronization regimes, we defined phase of oscillations using the Hilbert transform technique. We</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25677527','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25677527"><span>Synchrony, <span class="hlt">waves</span> and ripple in spatially <span class="hlt">coupled</span> Kuramoto oscillators with Mexican hat connectivity.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Heitmann, Stewart; Ermentrout, G Bard</p> <p>2015-06-01</p> <p>Spatiotemporal <span class="hlt">waves</span> of synchronized activity are known to arise in oscillatory neural networks with lateral inhibitory <span class="hlt">coupling</span>. How such patterns respond to dynamic changes in <span class="hlt">coupling</span> strength is largely unexplored. The present study uses analysis and simulation to investigate the evolution of <span class="hlt">wave</span> patterns when the strength of lateral inhibition is varied dynamically. Neural synchronization was <span class="hlt">modeled</span> by a spatial ring of Kuramoto oscillators with Mexican hat lateral <span class="hlt">coupling</span>. Broad bands of coexisting stable <span class="hlt">wave</span> solutions were observed at all levels of inhibition. The stability of these <span class="hlt">waves</span> was formally analyzed in both the infinite ring and the finite ring. The broad range of multi-stability predicted hysteresis in transitions between neighboring <span class="hlt">wave</span> solutions when inhibition is slowly varied. Numerical simulation confirmed the predicted transitions when inhibition was ramped down from a high initial value. However, non-<span class="hlt">wave</span> solutions emerged from the uniform solution when inhibition was ramped upward from zero. These solutions correspond to spatially periodic deviations of phase that we call ripple states. Numerical continuation showed that stable ripple states emerge from synchrony via a supercritical pitchfork bifurcation. The normal form of this bifurcation was derived analytically, and its predictions compared against the numerical results. Ripple states were also found to bifurcate from <span class="hlt">wave</span> solutions, but these were locally unstable. Simulation also confirmed the existence of hysteresis and ripple states in two spatial dimensions. Our findings show that spatial synchronization patterns can remain structurally stable despite substantial changes in network connectivity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1402622-predicting-electromagnetic-ion-cyclotron-wave-amplitude-from-unstable-ring-current-plasma-conditions','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1402622-predicting-electromagnetic-ion-cyclotron-wave-amplitude-from-unstable-ring-current-plasma-conditions"><span>Predicting electromagnetic ion cyclotron <span class="hlt">wave</span> amplitude from unstable ring <span class="hlt">current</span> plasma conditions</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Fu, Xiangrong; Cowee, Misa M.; Jordanova, Vania K.; ...</p> <p>2016-11-01</p> <p>Electromagnetic ion cyclotron (EMIC) <span class="hlt">waves</span> in the Earth's inner magnetosphere are enhanced fluctuations driven unstable by ring <span class="hlt">current</span> ion temperature anisotropy. EMIC <span class="hlt">waves</span> can resonate with relativistic electrons and play an important role in precipitation of MeV radiation belt electrons. In this study, we investigate the excitation and saturation of EMIC instability in a homogeneous plasma using both linear theory and nonlinear hybrid simulations. We have explored a four-dimensional parameter space, carried out a large number of simulations, and derived a scaling formula that relates the saturation EMIC <span class="hlt">wave</span> amplitude to initial plasma conditions. Finally, such scaling can be usedmore » in conjunction with ring <span class="hlt">current</span> <span class="hlt">models</span> like ring <span class="hlt">current</span>-atmosphere interactions <span class="hlt">model</span> with self-consistent magnetic field to provide global dynamic EMIC <span class="hlt">wave</span> maps that will be more accurate inputs for radiation belt <span class="hlt">modeling</span> than statistical <span class="hlt">models</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770018428','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770018428"><span>Computer program for analysis of <span class="hlt">coupled</span>-cavity traveling <span class="hlt">wave</span> tubes</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Connolly, D. J.; Omalley, T. A.</p> <p>1977-01-01</p> <p>A flexible, accurate, large signal computer program was developed for the design of <span class="hlt">coupled</span> cavity traveling <span class="hlt">wave</span> tubes. The program is written in FORTRAN IV for an IBM 360/67 time sharing system. The beam is described by a disk <span class="hlt">model</span> and the slow <span class="hlt">wave</span> structure by a sequence of cavities, or cells. The computational approach is arranged so that each cavity may have geometrical or electrical parameters different from those of its neighbors. This allows the program user to simulate a tube of almost arbitrary complexity. Input and output couplers, severs, complicated velocity tapers, and other features peculiar to one or a few cavities may be <span class="hlt">modeled</span> by a correct choice of input data. The beam-<span class="hlt">wave</span> interaction is handled by an approach in which the radio frequency fields are expanded in solutions to the transverse magnetic <span class="hlt">wave</span> equation. All significant space harmonics are retained. The program was used to perform a design study of the traveling-<span class="hlt">wave</span> tube developed for the Communications Technology Satellite. Good agreement was obtained between the predictions of the program and the measured performance of the flight tube.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNH23E2795Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNH23E2795Z"><span>Satellite Remote Sensing of Ocean Winds, Surface <span class="hlt">Waves</span> and Surface <span class="hlt">Currents</span> during the Hurricanes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, G.; Perrie, W. A.; Liu, G.; Zhang, L.</p> <p>2017-12-01</p> <p>Hurricanes over the ocean have been observed by spaceborne aperture radar (SAR) since the first SAR images were available in 1978. SAR has high spatial resolution (about 1 km), relatively large coverage and capability for observations during almost all-weather, day-and-night conditions. In this study, seven C-band RADARSAT-2 dual-polarized (VV and VH) ScanSAR wide images from the Canadian Space Agency (CSA) Hurricane Watch Program in 2017 are collected over five hurricanes: Harvey, Irma, Maria, Nate, and Ophelia. We retrieve the ocean winds by applying our C-band Cross-Polarization <span class="hlt">Coupled</span>-Parameters Ocean (C-3PO) wind retrieval <span class="hlt">model</span> [Zhang et al., 2017, IEEE TGRS] to the SAR images. Ocean <span class="hlt">waves</span> are estimated by applying a relationship based on the fetch- and duration-limited nature of <span class="hlt">wave</span> growth inside hurricanes [Hwang et al., 2016; 2017, J. Phys. Ocean.]. We estimate the ocean surface <span class="hlt">currents</span> using the Doppler Shift extracted from VV-polarized SAR images [Kang et al., 2016, IEEE TGRS]. C-3PO <span class="hlt">model</span> is based on theoretical analysis of ocean surface <span class="hlt">waves</span> and SAR microwave backscatter. Based on the retrieved ocean winds, we estimate the hurricane center locations, maxima wind speeds, and radii of the five hurricanes by adopting the SHEW <span class="hlt">model</span> (Symmetric Hurricane Estimates for Wind) by Zhang et al. [2017, IEEE TGRS]. Thus, we investigate possible relations between hurricane structures and intensities, and especially some possible effects of the asymmetrical characteristics on changes in the hurricane intensities, such as the eyewall replacement cycle. The three SAR images of Ophelia include the north coast of Ireland and east coast of Scotland allowing study of ocean surface <span class="hlt">currents</span> respond to the hurricane. A system of methods capable of observing marine winds, surface <span class="hlt">waves</span>, and surface <span class="hlt">currents</span> from satellites is of value, even if these data are only available in near real-time or from SAR-related satellite images. Insight into high resolution ocean winds</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDD34007T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDD34007T"><span>Dense Gravity <span class="hlt">Currents</span> with Breaking Internal <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tanimoto, Yukinobu; Hogg, Charlie; Ouellette, Nicholas; Koseff, Jeffrey</p> <p>2017-11-01</p> <p>Shoaling and breaking internal <span class="hlt">waves</span> along a pycnocline may lead to mixing and dilution of dense gravity <span class="hlt">currents</span>, such as cold river inflows into lakes or brine effluent from desalination plants in near-coastal environments. In order to explore the interaction between gravity <span class="hlt">currents</span> and breaking interfacial <span class="hlt">waves</span> a series of laboratory experiments was performed in which a sequence of internal <span class="hlt">waves</span> impinge upon a shelf-slope gravity <span class="hlt">current</span>. The <span class="hlt">waves</span> are generated in a two-layer thin-interface ambient water column under a variety of conditions characterizing both the <span class="hlt">waves</span> and the gravity <span class="hlt">currents</span>. The mixing of the gravity <span class="hlt">current</span> is measured through both intrusive (CTD probe) and nonintrusive (Planar-laser inducted fluorescence) techniques. We will present results over a full range of Froude number (characterizing the <span class="hlt">waves</span>) and Richardson number (characterizing the gravity <span class="hlt">current</span>) conditions, and will discuss the mechanisms by which the gravity <span class="hlt">current</span> is mixed into the ambient environment including the role of turbulence in the process. National Science Foundation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ClDy...50.4211K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ClDy...50.4211K"><span>Convectively <span class="hlt">coupled</span> equatorial <span class="hlt">waves</span> within the MJO during CINDY/DYNAMO: slow Kelvin <span class="hlt">waves</span> as building blocks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kikuchi, Kazuyoshi; Kiladis, George N.; Dias, Juliana; Nasuno, Tomoe</p> <p>2018-06-01</p> <p>This study examines the relationship between the MJO and convectively <span class="hlt">coupled</span> equatorial <span class="hlt">waves</span> (CCEWs) during the CINDY2011/DYNAMO field campaign using satellite-borne infrared radiation data, in order to better understand the interaction between convection and the large-scale circulation. The spatio-temporal wavelet transform (STWT) enables us to document the convective signals within the MJO envelope in terms of CCEWs in great detail, through localization of space-time spectra at any given location and time. Three MJO events that occurred in October, November, and December 2011 are examined. It is, in general, difficult to find universal relationships between the MJO and CCEWs, implying that MJOs are diverse in terms of the types of disturbances that make up its convective envelope. However, it is found in all MJO events that the major convective body of the MJO is made up mainly by slow convectively <span class="hlt">coupled</span> Kelvin <span class="hlt">waves</span>. These Kelvin <span class="hlt">waves</span> have relatively fast phase speeds of 10-13 m s-1 outside of, and slow phase speeds of 8-9 m s-1 within the MJO. Sometimes even slower eastward propagating signals with 3-5 m s-1 phase speed show up within the MJO, which, as well as the slow Kelvin <span class="hlt">waves</span>, appear to comprise major building blocks of the MJO. It is also suggested that these eastward propagating <span class="hlt">waves</span> often occur coincident with n = 1 WIG <span class="hlt">waves</span>, which is consistent with the schematic <span class="hlt">model</span> from Nakazawa in 1988. Some practical aspects that facilitate use of the STWT are also elaborated upon and discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018Chaos..28d3104S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018Chaos..28d3104S"><span>Effect of P T symmetry on nonlinear <span class="hlt">waves</span> for three-<span class="hlt">wave</span> interaction <span class="hlt">models</span> in the quadratic nonlinear media</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shen, Yujia; Wen, Zichao; Yan, Zhenya; Hang, Chao</p> <p>2018-04-01</p> <p>We study the three-<span class="hlt">wave</span> interaction that <span class="hlt">couples</span> an electromagnetic pump <span class="hlt">wave</span> to two frequency down-converted daughter <span class="hlt">waves</span> in a quadratic optical crystal and P T -symmetric potentials. P T symmetric potentials are shown to modulate stably nonlinear modes in two kinds of three-<span class="hlt">wave</span> interaction <span class="hlt">models</span>. The first one is a spatially extended three-<span class="hlt">wave</span> interaction system with odd gain-and-loss distribution in the channel. Modulated by the P T -symmetric single-well or multi-well Scarf-II potentials, the system is numerically shown to possess stable soliton solutions. Via adiabatical change of system parameters, numerical simulations for the excitation and evolution of nonlinear modes are also performed. The second one is a combination of P T -symmetric <span class="hlt">models</span> which are <span class="hlt">coupled</span> via three-<span class="hlt">wave</span> interactions. Families of nonlinear modes are found with some particular choices of parameters. Stable and unstable nonlinear modes are shown in distinct families by means of numerical simulations. These results will be useful to further investigate nonlinear modes in three-<span class="hlt">wave</span> interaction <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDE20005C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDE20005C"><span>Strong <span class="hlt">wave</span>/mean-flow <span class="hlt">coupling</span> in baroclinic acoustic streaming</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chini, Greg; Michel, Guillaume</p> <p>2017-11-01</p> <p>Recently, Chini et al. demonstrated the potential for large-amplitude acoustic streaming in compressible channel flows subjected to strong background cross-channel density variations. In contrast with classic Rayleigh streaming, standing acoustic <span class="hlt">waves</span> of O (ɛ) amplitude acquire vorticity owing to baroclinic torques acting throughout the domain rather than via viscous torques acting in Stokes boundary layers. More significantly, these baroclinically-driven streaming flows have a magnitude that also is O (ɛ) , i.e. comparable to that of the sound <span class="hlt">waves</span>. In the present study, the consequent potential for fully two-way <span class="hlt">coupling</span> between the <span class="hlt">waves</span> and streaming flows is investigated using a novel WKBJ analysis. The analysis confirms that the <span class="hlt">wave</span>-driven streaming flows are sufficiently strong to modify the background density gradient, thereby modifying the leading-order acoustic <span class="hlt">wave</span> structure. Simulations of the <span class="hlt">wave</span>/mean-flow system enabled by the WKBJ analysis are performed to illustrate the nature of the two-way <span class="hlt">coupling</span>, which contrasts sharply with classic Rayleigh streaming, for which the <span class="hlt">waves</span> can first be determined and the streaming flows subsequently computed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70176567','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70176567"><span>Effect of roughness formulation on the performance of a <span class="hlt">coupled</span> <span class="hlt">wave</span>, hydrodynamic, and sediment transport <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>Ganju, Neil K.; Sherwood, Christopher R.</p> <p>2010-01-01</p> <p>A variety of algorithms are available for parameterizing the hydrodynamic bottom roughness associated with grain size, saltation, bedforms, and wave–<span class="hlt">current</span> interaction in coastal ocean <span class="hlt">models</span>. These parameterizations give rise to spatially and temporally variable bottom-drag coefficients that ostensibly provide better representations of physical processes than uniform and constant coefficients. However, few studies have been performed to determine whether improved representation of these variable bottom roughness components translates into measurable improvements in <span class="hlt">model</span> skill. We test the hypothesis that improved representation of variable bottom roughness improves performance with respect to near-bed circulation, bottom stresses, or turbulence dissipation. The inner shelf south of Martha’s Vineyard, Massachusetts, is the site of sorted grain-size features which exhibit sharp alongshore variations in grain size and ripple geometry over gentle bathymetric relief; this area provides a suitable testing ground for roughness parameterizations. We first establish the skill of a nested regional <span class="hlt">model</span> for <span class="hlt">currents</span>, <span class="hlt">waves</span>, stresses, and turbulent quantities using a uniform and constant roughness; we then gauge <span class="hlt">model</span> skill with various parameterization of roughness, which account for the influence of the <span class="hlt">wave</span>-boundary layer, grain size, saltation, and rippled bedforms. We find that commonly used representations of ripple-induced roughness, when combined with a wave–<span class="hlt">current</span> interaction routine, do not significantly improve skill for circulation, and significantly decrease skill with respect to stresses and turbulence dissipation. Ripple orientation with respect to dominant <span class="hlt">currents</span> and ripple shape may be responsible for complicating a straightforward estimate of the roughness contribution from ripples. In addition, sediment-induced stratification may be responsible for lower stresses than predicted by the wave–<span class="hlt">current</span> interaction <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21550238-analytical-ground-state-jaynes-cummings-model-ultrastrong-coupling','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21550238-analytical-ground-state-jaynes-cummings-model-ultrastrong-coupling"><span>Analytical ground state for the Jaynes-Cummings <span class="hlt">model</span> with ultrastrong <span class="hlt">coupling</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>Zhang Yuanwei; Institute of Theoretical Physics, Shanxi University, Taiyuan 030006; Chen Gang</p> <p>2011-06-15</p> <p>We present a generalized variational method to analytically obtain the ground-state properties of the Jaynes-Cummings <span class="hlt">model</span> with the ultrastrong <span class="hlt">coupling</span>. An explicit expression for the ground-state energy, which agrees well with the numerical simulation in a wide range of the experimental parameters, is given. In particular, the introduced method can successfully solve this Jaynes-Cummings <span class="hlt">model</span> with the positive detuning (the atomic resonant level is larger than the photon frequency), which cannot be treated in the adiabatical approximation and the generalized rotating-<span class="hlt">wave</span> approximation. Finally, we also demonstrate analytically how to control the mean photon number by means of the <span class="hlt">current</span> experimentalmore » parameters including the photon frequency, the <span class="hlt">coupling</span> strength, and especially the atomic resonant level.« 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('http://adsabs.harvard.edu/abs/2018JAP...123b4904V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123b4904V"><span>Nonlinear mechanisms of two-dimensional <span class="hlt">wave-wave</span> transformations in the initially <span class="hlt">coupled</span> acoustic structure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vorotnikov, K.; Starosvetsky, Y.</p> <p>2018-01-01</p> <p>The present study concerns two-dimensional nonlinear mechanisms of bidirectional and unidirectional channeling of longitudinal and shear <span class="hlt">waves</span> emerging in the locally resonant acoustic structure. The system under consideration comprises an oscillatory chain of the axially <span class="hlt">coupled</span> masses. Each mass of the chain is subject to the local linear potential along the lateral direction and incorporates the lightweight internal rotator. In the present work, we demonstrate the emergence of special resonant regimes of complete bi- and unidirectional transitions between the longitudinal and the shear <span class="hlt">waves</span> of the locally resonant chain. These regimes are manifested by the two-dimensional energy channeling between the longitudinal and the shear traveling <span class="hlt">waves</span> in the recurrent as well as the irreversible fashion. We show that the spatial control of the two dimensional energy flow between the longitudinal and the shear <span class="hlt">waves</span> is solely governed by the motion of the internal rotators. Nonlinear analysis of the regimes of a bidirectional <span class="hlt">wave</span> channeling unveils their global bifurcation structure and predicts the zones of their spontaneous transitions from a complete bi-directional <span class="hlt">wave</span> channeling to the one-directional entrapment. An additional regime of a complete irreversible resonant transformation of the longitudinal <span class="hlt">wave</span> into a shear <span class="hlt">wave</span> is analyzed in the study. The intrinsic mechanism governing the unidirectional <span class="hlt">wave</span> reorientation is described analytically. The results of the analysis of both mechanisms are substantiated by the numerical simulations of the full <span class="hlt">model</span> and are found to be in a good agreement.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GMD....10.4207V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GMD....10.4207V"><span>SURFEX v8.0 interface with OASIS3-MCT to <span class="hlt">couple</span> atmosphere with hydrology, ocean, <span class="hlt">waves</span> and sea-ice <span class="hlt">models</span>, from coastal to 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>Voldoire, Aurore; Decharme, Bertrand; Pianezze, Joris; Lebeaupin Brossier, Cindy; Sevault, Florence; Seyfried, Léo; Garnier, Valérie; Bielli, Soline; Valcke, Sophie; Alias, Antoinette; Accensi, Mickael; Ardhuin, Fabrice; Bouin, Marie-Noëlle; Ducrocq, Véronique; Faroux, Stéphanie; Giordani, Hervé; Léger, Fabien; Marsaleix, Patrick; Rainaud, Romain; Redelsperger, Jean-Luc; Richard, Evelyne; Riette, Sébastien</p> <p>2017-11-01</p> <p>This study presents the principles of the new <span class="hlt">coupling</span> interface based on the SURFEX multi-surface <span class="hlt">model</span> and the OASIS3-MCT coupler. As SURFEX can be plugged into several atmospheric <span class="hlt">models</span>, it can be used in a wide range of applications, from global and regional <span class="hlt">coupled</span> climate systems to high-resolution numerical weather prediction systems or very fine-scale <span class="hlt">models</span> dedicated to process studies. The objective of this development is to build and share a common structure for the atmosphere-surface <span class="hlt">coupling</span> of all these applications, involving on the one hand atmospheric <span class="hlt">models</span> and on the other hand ocean, ice, hydrology, and <span class="hlt">wave</span> <span class="hlt">models</span>. The numerical and physical principles of SURFEX interface between the different component <span class="hlt">models</span> are described, and the different <span class="hlt">coupled</span> systems in which the SURFEX OASIS3-MCT-based <span class="hlt">coupling</span> interface is already implemented are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018CMT...tmp...35R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018CMT...tmp...35R"><span>Seismic <span class="hlt">waves</span> and earthquakes in a global monolithic <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>Roubíček, Tomáš</p> <p>2018-03-01</p> <p>The philosophy that a single "monolithic" <span class="hlt">model</span> can "asymptotically" replace and <span class="hlt">couple</span> in a simple elegant way several specialized <span class="hlt">models</span> relevant on various Earth layers is presented and, in special situations, also rigorously justified. In particular, global seismicity and tectonics is <span class="hlt">coupled</span> to capture, e.g., (here by a simplified <span class="hlt">model</span>) ruptures of lithospheric faults generating seismic <span class="hlt">waves</span> which then propagate through the solid-like mantle and inner core both as shear (S) or pressure (P) <span class="hlt">waves</span>, while S-<span class="hlt">waves</span> are suppressed in the fluidic outer core and also in the oceans. The "monolithic-type" <span class="hlt">models</span> have the capacity to describe all the mentioned features globally in a unified way together with corresponding interfacial conditions implicitly involved, only when scaling its parameters appropriately in different Earth's layers. <span class="hlt">Coupling</span> of seismic <span class="hlt">waves</span> with seismic sources due to tectonic events is thus an automatic side effect. The global ansatz is here based, rather for an illustration, only on a relatively simple Jeffreys' viscoelastic damageable material at small strains whose various scaling (limits) can lead to Boger's viscoelastic fluid or even to purely elastic (inviscid) fluid. Self-induced gravity field, Coriolis, centrifugal, and tidal forces are counted in our global <span class="hlt">model</span>, as well. The rigorous mathematical analysis as far as the existence of solutions, convergence of the mentioned scalings, and energy conservation is briefly presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003ChPhL..20.2203X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003ChPhL..20.2203X"><span>Instability of Longitudinal <span class="hlt">Wave</span> in Magnetized Strongly <span class="hlt">Coupled</span> Dusty Plasma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xie, Bai-Song</p> <p>2003-12-01</p> <p>Instability of longitudinal <span class="hlt">wave</span> in magnetized strongly <span class="hlt">coupled</span> dusty plasmas is investigated. The dust charging relaxation is taken into account. It is found that there exists threshold of interdust distance for the instability of <span class="hlt">wave</span>, which is determined significantly by the dust charging relaxation, the <span class="hlt">coupling</span> parameter of high correlation of dust as well the strength of magnetic field.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..DFDR11011C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..DFDR11011C"><span>Rogue <span class="hlt">Wave</span> Modes for the Long <span class="hlt">Wave</span>-Short <span class="hlt">Wave</span> Resonance and the Derivative Nonlinear Schrödinger <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>Chan, Hiu Ning; Chow, Kwok Wing; Kedziora, David Jacob; Grimshaw, Roger Hamilton James; Ding, Edwin</p> <p>2014-11-01</p> <p>Rogue <span class="hlt">waves</span> are unexpectedly large displacements of the water surface and will obviously pose threat to maritime activities. Recently, the formation of rogue <span class="hlt">waves</span> is correlated with the onset of modulation instabilities of plane <span class="hlt">waves</span> of the system. The long <span class="hlt">wave</span>-short <span class="hlt">wave</span> resonance and the derivative nonlinear Schrödinger <span class="hlt">models</span> are considered. They are relevant in a two-layer fluid and a fourth order perturbation expansion of free surface <span class="hlt">waves</span> respectively. Analytical solutions of rogue <span class="hlt">wave</span> modes for the two <span class="hlt">models</span> are derived by the Hirota bilinear method. Properties and amplitudes of these rogue <span class="hlt">wave</span> modes are investigated. Conditions for modulation instability of the plane <span class="hlt">waves</span> are shown to be precisely the requirements for the occurrence of rogue <span class="hlt">waves</span>. In contrast with the nonlinear Schrödinger equation, rogue <span class="hlt">wave</span> modes for the derivative nonlinear Schrödinger <span class="hlt">model</span> exist even if the dispersion and cubic nonlinearity are of the opposite signs, provided that a sufficiently strong self-steepening nonlinearity is present. Extensions to the <span class="hlt">coupled</span> case (multiple waveguides) will be discussed. This work is partially supported by the Research Grants Council General Research Fund Contract HKU 711713E.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27475575','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27475575"><span>3D analysis of eddy <span class="hlt">current</span> loss in the permanent magnet <span class="hlt">coupling</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhu, Zina; Meng, Zhuo</p> <p>2016-07-01</p> <p>This paper first presents a 3D analytical <span class="hlt">model</span> for analyzing the radial air-gap magnetic field between the inner and outer magnetic rotors of the permanent magnet <span class="hlt">couplings</span> by using the Amperian <span class="hlt">current</span> <span class="hlt">model</span>. Based on the air-gap field analysis, the eddy <span class="hlt">current</span> loss in the isolation cover is predicted according to the Maxwell's equations. A 3D finite element analysis <span class="hlt">model</span> is constructed to analyze the magnetic field spatial distributions and vector eddy <span class="hlt">currents</span>, and then the simulation results obtained are analyzed and compared with the analytical method. Finally, the <span class="hlt">current</span> losses of two types of practical magnet <span class="hlt">couplings</span> are measured in the experiment to compare with the theoretical results. It is concluded that the 3D analytical method of eddy <span class="hlt">current</span> loss in the magnet <span class="hlt">coupling</span> is viable and could be used for the eddy <span class="hlt">current</span> loss prediction of magnet <span class="hlt">couplings</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26367426','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26367426"><span>Rigorous <span class="hlt">coupled</span> <span class="hlt">wave</span> analysis of acousto-optics with relativistic considerations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Xia, Guoqiang; Zheng, Weijian; Lei, Zhenggang; Zhang, Ruolan</p> <p>2015-09-01</p> <p>A relativistic analysis of acousto-optics is presented, and a rigorous <span class="hlt">coupled</span> <span class="hlt">wave</span> analysis is generalized for the diffraction of the acousto-optical effect. An acoustic <span class="hlt">wave</span> generates a grating with temporally and spatially modulated permittivity, hindering direct applications of the rigorous <span class="hlt">coupled</span> <span class="hlt">wave</span> analysis for the acousto-optical effect. In a reference frame which moves with the acoustic <span class="hlt">wave</span>, the grating is static, the medium moves, and the <span class="hlt">coupled</span> <span class="hlt">wave</span> equations for the static grating may be derived. Floquet's theorem is then applied to cast these equations into an eigenproblem. Using a Lorentz transformation, the electromagnetic fields in the grating region are transformed to the lab frame where the medium is at rest, and relativistic Doppler frequency shifts are introduced into various diffraction orders. In the lab frame, the boundary conditions are considered and the diffraction efficiencies of various orders are determined. This method is rigorous and general, and the plane <span class="hlt">waves</span> in the resulting expansion satisfy the dispersion relation of the medium and are propagation modes. Properties of various Bragg diffractions are results, rather than preconditions, of this method. Simulations of an acousto-optical tunable filter made by paratellurite, TeO(2), are given as examples.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AnPhy.324.1194G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AnPhy.324.1194G"><span><span class="hlt">Coupled</span> matter-<span class="hlt">wave</span> solitons in optical lattices</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Golam Ali, Sk; Talukdar, B.</p> <p>2009-06-01</p> <p>We make use of a potential <span class="hlt">model</span> to study the dynamics of two <span class="hlt">coupled</span> matter-<span class="hlt">wave</span> or Bose-Einstein condensate (BEC) solitons loaded in optical lattices. With separate attention to linear and nonlinear lattices we find some remarkable differences for response of the system to effects of these lattices. As opposed to the case of linear optical lattice (LOL), the nonlinear lattice (NOL) can be used to control the mutual interaction between the two solitons. For a given lattice <span class="hlt">wave</span> number k, the effective potentials in which the two solitons move are such that the well (Veff(NOL)), resulting from the juxtaposition of soliton interaction and nonlinear lattice potential, is deeper than the corresponding well Veff(LOL). But these effective potentials have opposite k dependence in the sense that the depth of Veff(LOL) increases as k increases and that of Veff(NOL) decreases for higher k values. We verify that the effectiveness of optical lattices to regulate the motion of the <span class="hlt">coupled</span> solitons depends sensitively on the initial locations of the motionless solitons as well as values of the lattice <span class="hlt">wave</span> number. For both LOL and NOL the two solitons meet each other due to mutual interaction if their initial locations are taken within the potential wells with the difference that the solitons in the NOL approach each other rather rapidly and take roughly half the time to meet as compared with the time needed for such coalescence in the LOL. In the NOL, the soliton profiles can move freely and respond to the lattice periodicity when the separation between their initial locations are as twice as that needed for a similar free movement in the LOL. We observe that, in both cases, slow tuning of the optical lattices by varying k with respect to a time parameter τ drags the oscillatory solitons apart to take them to different locations. In our potential <span class="hlt">model</span> the oscillatory solitons appear to propagate undistorted. But a fully numerical calculation indicates that during evolution</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25768624','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25768624"><span>Optical rogue <span class="hlt">waves</span> associated with the negative coherent <span class="hlt">coupling</span> in an isotropic medium.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Sun, Wen-Rong; Tian, Bo; Jiang, Yan; Zhen, Hui-Ling</p> <p>2015-02-01</p> <p>Optical rogue <span class="hlt">waves</span> of the <span class="hlt">coupled</span> nonlinear Schrödinger equations with negative coherent <span class="hlt">coupling</span>, which describe the propagation of orthogonally polarized optical <span class="hlt">waves</span> in an isotropic medium, are reported. We construct and discuss a family of the vector rogue-<span class="hlt">wave</span> solutions, including the bright rogue <span class="hlt">waves</span>, four-petaled rogue <span class="hlt">waves</span>, and dark rogue <span class="hlt">waves</span>. A bright rogue <span class="hlt">wave</span> without a valley can split up, giving birth to two bright rogue <span class="hlt">waves</span>, and an eye-shaped rogue <span class="hlt">wave</span> can split up, giving birth to two dark rogue <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97k5112S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97k5112S"><span>Delocalization of charge and <span class="hlt">current</span> in a chiral quasiparticle <span class="hlt">wave</span> packet</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sarkar, Subhajit</p> <p>2018-03-01</p> <p>A chiral quasiparticle <span class="hlt">wave</span> packet (c-QPWP) is defined as a conventional superposition of chiral quasiparticle states corresponding to an interacting electron system in two dimensions (2D) in the presence of Rashba spin-orbit <span class="hlt">coupling</span> (RSOC). I investigate its internal structure via studying the charge and the <span class="hlt">current</span> densities within the first-order perturbation in the electron-electron interaction. It is found that the c-QPWP contains a localized charge which is less than the magnitude of the bare charge and the remaining charge resides at the system boundary. The amount of charge delocalized turns out to be inversely proportional to the degenerate Fermi velocity v0(=√{α2+2 μ /m }) when RSOC (with strength α ) is weak, and therefore externally tunable. For strong RSOC, the magnitudes of both the delocalized charge and the <span class="hlt">current</span> further strongly depend on the direction of propagation of the <span class="hlt">wave</span> packet. Both the charge and the <span class="hlt">current</span> densities consist of an anisotropic r-2 tail away from the center of the <span class="hlt">wave</span> packet. Possible implications of such delocalizations in real systems corresponding to 2D semiconductor heterostructure are also discussed within the context of particle injection experiments.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22600007-coupling-acoustic-wave-shear-motion-due-viscous-heating','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22600007-coupling-acoustic-wave-shear-motion-due-viscous-heating"><span><span class="hlt">Coupling</span> of an acoustic <span class="hlt">wave</span> to shear motion due to viscous heating</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Liu, Bin; Goree, J.</p> <p>2016-07-15</p> <p>Viscous heating due to shear motion in a plasma can result in the excitation of a longitudinal acoustic <span class="hlt">wave</span>, if the shear motion is modulated in time. The <span class="hlt">coupling</span> mechanism is a thermal effect: time-dependent shear motion causes viscous heating, which leads to a rarefaction that can <span class="hlt">couple</span> into a longitudinal <span class="hlt">wave</span>, such as an acoustic <span class="hlt">wave</span>. This <span class="hlt">coupling</span> mechanism is demonstrated in an electrostatic three-dimensional (3D) simulation of a dusty plasma, in which a localized shear flow is initiated as a pulse, resulting in a delayed outward propagation of a longitudinal acoustic <span class="hlt">wave</span>. This <span class="hlt">coupling</span> effect can be profoundmore » in plasmas that exhibit localized viscous heating, such as the dusty plasma we simulated using parameters typical of the PK-4 experiment. We expect that a similar phenomenon can occur with other kinds of plasma <span class="hlt">waves</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..15..503C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15..503C"><span><span class="hlt">Wave</span> propagation against <span class="hlt">current</span> : a study of the effects of vertical shears of the mean <span class="hlt">current</span> on the geometrical focusing of water <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Charland, Jenna; Touboul, Julien; Rey, Vincent</p> <p>2013-04-01</p> <p> vertical shears, further theoretical expansions have considered this shearing following the hypothesis proposed by Kirby [3]. A numerical solver for this new equation is being developed. Results obtained with this new equation will be compared to a new set of experiments. This comparison will allow us to quantify the role of a sheared <span class="hlt">current</span> in the geometrical focusing of the <span class="hlt">wave</span>. References : [1] W. Chen, V. Panchang, and Z. Demirbilek. On the <span class="hlt">modeling</span> of <span class="hlt">wave-current</span> interaction using the elliptic mild-slope <span class="hlt">wave</span> equation. Ocean Engineering, 32 :2135-2164, 2005. [2] C. Kharif and E. Pelinovsky. Physical mechanisms of the rogue <span class="hlt">wave</span> phenomenon. European Journal of Mechanics B/Fluids, 22 : 603-634, 2003 [3] J. T. Kirby. A note on linear surface <span class="hlt">wave-current</span> interaction over slowly varying topography. Journal of Geophysical Research, 89(C1) : 745-747, January 20 1984. [4] V. Rey, F. Guinot, and J. Touboul. Large scale experimental study of <span class="hlt">wave</span> <span class="hlt">current</span> interactions in presence of a 3d bathymetry. Genoa : s.n., 2011. International Maritime Association of the Mediterranean.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvA..95d2115T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvA..95d2115T"><span>Spectra, <span class="hlt">current</span> flow, and <span class="hlt">wave</span>-function morphology in a <span class="hlt">model</span> PT -symmetric quantum dot with external interactions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tellander, Felix; Berggren, Karl-Fredrik</p> <p>2017-04-01</p> <p>In this paper we use numerical simulations to study a two-dimensional (2D) quantum dot (cavity) with two leads for passing <span class="hlt">currents</span> (electrons, photons, etc.) through the system. By introducing an imaginary potential in each lead the system is made symmetric under parity-time inversion (PT symmetric). This system is experimentally realizable in the form of, e.g., quantum dots in low-dimensional semiconductors, optical and electromagnetic cavities, and other classical <span class="hlt">wave</span> analogs. The computational <span class="hlt">model</span> introduced here for studying spectra, exceptional points (EPs), <span class="hlt">wave</span>-function symmetries and morphology, and <span class="hlt">current</span> flow includes thousands of interacting states. This supplements previous analytic studies of few interacting states by providing more detail and higher resolution. The Hamiltonian describing the system is non-Hermitian; thus, the eigenvalues are, in general, complex. The structure of the <span class="hlt">wave</span> functions and probability <span class="hlt">current</span> densities are studied in detail at and in between EPs. The statistics for EPs is evaluated, and reasons for a gradual dynamical crossover are identified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhyE..101..224Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhyE..101..224Y"><span><span class="hlt">Current</span> in nanojunctions: Effects of reservoir <span class="hlt">coupling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yadalam, Hari Kumar; Harbola, Upendra</p> <p>2018-07-01</p> <p>We study the effect of system reservoir <span class="hlt">coupling</span> on <span class="hlt">currents</span> flowing through quantum junctions. We consider two simple double-quantum dot configurations <span class="hlt">coupled</span> to two external fermionic reservoirs and study the net <span class="hlt">current</span> flowing between the two reservoirs. The net <span class="hlt">current</span> is partitioned into <span class="hlt">currents</span> carried by the eigenstates of the system and by the coherences between the eigenstates induced due to <span class="hlt">coupling</span> with the reservoirs. We find that <span class="hlt">current</span> carried by populations is always positive whereas <span class="hlt">current</span> carried by coherences are negative for large <span class="hlt">couplings</span>. This results in a non-monotonic dependence of the net <span class="hlt">current</span> on the <span class="hlt">coupling</span> strength. We find that in certain cases, the net <span class="hlt">current</span> can vanish at large <span class="hlt">couplings</span> due to cancellation between <span class="hlt">currents</span> carried by the eigenstates and by the coherences. These results provide new insights into the non-trivial role of system-reservoir <span class="hlt">couplings</span> on electron transport through quantum dot junctions. In the presence of weak coulomb interactions, net <span class="hlt">current</span> as a function of system reservoir <span class="hlt">coupling</span> strength shows similar trends as for the non-interacting case.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840019213','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840019213"><span>An improved dual-frequency technique for the remote sensing of ocean <span class="hlt">currents</span> and <span class="hlt">wave</span> spectra</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schuler, D. L.; Eng, W. P.</p> <p>1984-01-01</p> <p>A two frequency microwave radar technique for the remote sensing of directional ocean <span class="hlt">wave</span> spectra and surface <span class="hlt">currents</span> is investigated. This technique is conceptually attractive because its operational physical principle involves a spatial electromagnetic scattering resonance with a single, but selectable, long gravity <span class="hlt">wave</span>. Multiplexing of signals having different spacing of the two transmitted frequencies allows measurements of the entire long <span class="hlt">wave</span> ocean spectrum to be carried out. A new scatterometer is developed and experimentally tested which is capable of making measurements having much larger signal/background values than previously possible. This instrument <span class="hlt">couples</span> the resonance technique with coherent, frequency agility radar capabilities. This scatterometer is presently configured for supporting a program of surface <span class="hlt">current</span> measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010OcDyn..60.1061Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010OcDyn..60.1061Z"><span><span class="hlt">Coupled</span> assimilation for an intermediated <span class="hlt">coupled</span> ENSO prediction <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>Zheng, Fei; Zhu, Jiang</p> <p>2010-10-01</p> <p>The value of <span class="hlt">coupled</span> assimilation is discussed using an intermediate <span class="hlt">coupled</span> <span class="hlt">model</span> in which the wind stress is the only atmospheric state which is slavery to <span class="hlt">model</span> sea surface temperature (SST). In the <span class="hlt">coupled</span> assimilation analysis, based on the <span class="hlt">coupled</span> wind-ocean state covariance calculated from the <span class="hlt">coupled</span> state ensemble, the ocean state is adjusted by assimilating wind data using the ensemble Kalman filter. As revealed by a series of assimilation experiments using simulated observations, the <span class="hlt">coupled</span> assimilation of wind observations yields better results than the assimilation of SST observations. Specifically, the <span class="hlt">coupled</span> assimilation of wind observations can help to improve the accuracy of the surface and subsurface <span class="hlt">currents</span> because the correlation between the wind and ocean <span class="hlt">currents</span> is stronger than that between SST and ocean <span class="hlt">currents</span> in the equatorial Pacific. Thus, the <span class="hlt">coupled</span> assimilation of wind data can decrease the initial condition errors in the surface/subsurface <span class="hlt">currents</span> that can significantly contribute to SST forecast errors. The value of the <span class="hlt">coupled</span> assimilation of wind observations is further demonstrated by comparing the prediction skills of three 12-year (1997-2008) hindcast experiments initialized by the ocean-only assimilation scheme that assimilates SST observations, the <span class="hlt">coupled</span> assimilation scheme that assimilates wind observations, and a nudging scheme that nudges the observed wind stress data, respectively. The prediction skills of two assimilation schemes are significantly better than those of the nudging scheme. The prediction skills of assimilating wind observations are better than assimilating SST observations. Assimilating wind observations for the 2007/2008 La Niña event triggers better predictions, while assimilating SST observations fails to provide an early warning for that event.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29702125','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29702125"><span>Travelling <span class="hlt">waves</span> in somitogenesis: Collective cellular properties emerge from time-delayed juxtacrine oscillation <span class="hlt">coupling</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tomka, Tomas; Iber, Dagmar; Boareto, Marcelo</p> <p>2018-04-24</p> <p>The sculpturing of the vertebrate body plan into segments begins with the sequential formation of somites in the presomitic mesoderm (PSM). The rhythmicity of this process is controlled by travelling <span class="hlt">waves</span> of gene expression. These kinetic <span class="hlt">waves</span> emerge from <span class="hlt">coupled</span> cellular oscillators and sweep across the PSM. In zebrafish, the oscillations are driven by autorepression of her genes and are synchronized via Notch signalling. Mathematical <span class="hlt">modelling</span> has played an important role in explaining how collective properties emerge from the molecular interactions. Increasingly more quantitative experimental data permits the validation of those mathematical <span class="hlt">models</span>, yet leads to increasingly more complex <span class="hlt">model</span> formulations that hamper an intuitive understanding of the underlying mechanisms. Here, we review previous efforts, and design a mechanistic <span class="hlt">model</span> of the her1 oscillator, which represents the experimentally viable her7;hes6 double mutant. This genetically simplified system is ideally suited to conceptually recapitulate oscillatory entrainment and travelling <span class="hlt">wave</span> formation, and to highlight open questions. It shows that three key parameters, the autorepression delay, the juxtacrine <span class="hlt">coupling</span> delay, and the <span class="hlt">coupling</span> strength, are sufficient to understand the emergence of the collective period, the collective amplitude, and the synchronization of neighbouring Her1 oscillators. Moreover, two spatiotemporal time delay gradients, in the autorepression and in the juxtacrine signalling, are required to explain the collective oscillatory dynamics and synchrony of PSM cells. The highlighted developmental principles likely apply more generally to other developmental processes, including neurogenesis and angiogenesis. Copyright © 2018. Published by Elsevier Ltd.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016OcDyn..66..917A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016OcDyn..66..917A"><span>Surface <span class="hlt">wave</span> effects on water temperature in the Baltic Sea: simulations with the <span class="hlt">coupled</span> NEMO-WAM <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>Alari, Victor; Staneva, Joanna; Breivik, Øyvind; Bidlot, Jean-Raymond; Mogensen, Kristian; Janssen, Peter</p> <p>2016-08-01</p> <p><span class="hlt">Coupled</span> circulation (NEMO) and <span class="hlt">wave</span> <span class="hlt">model</span> (WAM) system was used to study the effects of surface ocean <span class="hlt">waves</span> on water temperature distribution and heat exchange at regional scale (the Baltic Sea). Four scenarios—including Stokes-Coriolis force, sea-state dependent energy flux (additional turbulent kinetic energy due to breaking <span class="hlt">waves</span>), sea-state dependent momentum flux and the combination these forcings—were simulated to test the impact of different terms on simulated temperature distribution. The scenario simulations were compared to a control simulation, which included a constant <span class="hlt">wave</span>-breaking coefficient, but otherwise was without any <span class="hlt">wave</span> effects. The results indicate a pronounced effect of <span class="hlt">waves</span> on surface temperature, on the distribution of vertical temperature and on upwelling's. Overall, when all three <span class="hlt">wave</span> effects were accounted for, did the estimates of temperature improve compared to control simulation. During the summer, the <span class="hlt">wave</span>-induced water temperature changes were up to 1 °C. In northern parts of the Baltic Sea, a warming of the surface layer occurs in the <span class="hlt">wave</span> included simulations in summer months. This in turn reduces the cold bias between simulated and measured data, e.g. the control simulation was too cold compared to measurements. The warming is related to sea-state dependent energy flux. This implies that a spatio-temporally varying <span class="hlt">wave</span>-breaking coefficient is necessary, because it depends on actual sea state. <span class="hlt">Wave</span>-induced cooling is mostly observed in near-coastal areas and is the result of intensified upwelling in the scenario, when Stokes-Coriolis forcing is accounted for. Accounting for sea-state dependent momentum flux results in modified heat exchange at the water-air boundary which consequently leads to warming of surface water compared to control simulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMOS53C..01T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMOS53C..01T"><span>On the Influence of Convectively <span class="hlt">Coupled</span> Kelvin <span class="hlt">Waves</span> on African Easterly <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thorncroft, C. D.; Brammer, A.</p> <p>2015-12-01</p> <p>While Convectively <span class="hlt">Coupled</span> Kelvin <span class="hlt">Waves</span> (CCKWs) are generally weaker in Boreal Summer than in Boreal Spring in the tropical West African region, previous reseach has shown that they can have a significant impact on African Easterly <span class="hlt">Waves</span> (AEWs) in the West African and tropical Atlantic regions. This talk will highlight the significance of CCKWs in determining variability in AEW behaviour including how they impact: (i) Initiation of AEWs, (ii) Convection within existing AEWs and (iii) Development of favorable AEW structures for tropical cyclogenesis in the tropical Atlantic. Reanalysis and satellite datasets will be combined to shed light on these interactions from both a climatological and a case-study perspective. A major conclusion from this work is the strong recognition that forecasters in the region should be closely monitoring the propagation of CCKWs into the region and that medium-range weather prediction efforts in the tropics should be paying close attention to the fidelity of <span class="hlt">models</span> to represent CCKWs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSHE24A1441S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSHE24A1441S"><span>Ice Floe Breaking in Contemporary Third Generation Operational <span class="hlt">Wave</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>Sévigny, C.; Baudry, J.; Gauthier, J. C.; Dumont, D.</p> <p>2016-02-01</p> <p>The dynamical zone observed at the edge of the consolidated ice area where are found the <span class="hlt">wave</span>-fractured floes (i.e. marginal ice zone or MIZ) has become an important topic in ocean <span class="hlt">modeling</span>. As both operational and climate ocean <span class="hlt">models</span> now seek to reproduce the complex atmosphere-ice-ocean system with realistic <span class="hlt">coupling</span> processes, many theoretical and numerical studies have focused on understanding and <span class="hlt">modeling</span> this zone. Few attempts have been made to embed <span class="hlt">wave</span>-ice interactions specific to the MIZ within a two-dimensional <span class="hlt">model</span>, giving the possibility to calculate both the attenuation of surface <span class="hlt">waves</span> by sea ice and the concomitant breaking of the sea ice-cover into smaller floes. One of the first challenges consists in improving the parameterization of <span class="hlt">wave</span>-ice dynamics in contemporary third generation operational <span class="hlt">wave</span> <span class="hlt">models</span>. A simple <span class="hlt">waves</span>-in-ice <span class="hlt">model</span> (WIM) similar to the one proposed by Williams et al. (2013a,b) was implemented in WAVEWATCH III. This WIM considers ice floes as floating elastic plates and predicts the dimensionless attenuation coefficient by the use of a lookup-table-based, <span class="hlt">wave</span> scattering scheme. As in Dumont et al. (2011), the different frequencies are treated individually and floe breaking occurs for a particular frequency when the expected <span class="hlt">wave</span> amplitude exceeds the allowed strain amplitude, which considers ice floes properties and wavelength in ice field. The <span class="hlt">model</span> is here further refined and tested in idealized two-dimensional cases, giving preliminary results of the performance and sensitivity of the parameterization to initial <span class="hlt">wave</span> and ice conditions. The effects of the <span class="hlt">wave</span>-ice <span class="hlt">coupling</span> over the incident <span class="hlt">wave</span> spectrum are analyzed as well as the resulting floe size distribution. The <span class="hlt">model</span> gives prognostic values of the lateral extent of the marginal ice zone with maximum ice floe diameter that progressively increases with distance from the ice edge.</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/2017OptEn..56j6114C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017OptEn..56j6114C"><span>Composite rogue <span class="hlt">waves</span> and modulation instability for the three-<span class="hlt">coupled</span> Hirota system in an optical fiber</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chai, Han-Peng; Tian, Bo; Chai, Jun; Du, Zhong</p> <p>2017-10-01</p> <p>We investigate the three-<span class="hlt">coupled</span> Hirota system, which is applied to <span class="hlt">model</span> the long distance communication and ultrafast signal routing systems governing the propagation of light pulses. With the aid of the Darboux dressing transformation, composite rogue <span class="hlt">wave</span> solutions are derived. Spatial-temporal structures, including the four-petaled structure for the three-<span class="hlt">coupled</span> Hirota system, are exhibited. We find that the four-petaled rogue <span class="hlt">waves</span> occur in two of the three components, whereas the eye-shaped rogue <span class="hlt">wave</span> occurs in the other one. The composite rogue <span class="hlt">waves</span> can split up into two or three single rogue <span class="hlt">waves</span>. The corresponding conditions for the occurrence of such phenomena are discussed and presented. We find that the relative position of every single rogue <span class="hlt">wave</span> is influenced by the ratios of certain parameters. Besides, the linear instability analysis is performed, and our results agree with those from the baseband modulation instability theory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvA..94f3824Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvA..94f3824Z"><span>Generalized squeezing rotating-<span class="hlt">wave</span> approximation to the isotropic and anisotropic Rabi <span class="hlt">model</span> in the ultrastrong-<span class="hlt">coupling</span> regime</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Yu-Yu</p> <p>2016-12-01</p> <p>Generalized squeezing rotating-<span class="hlt">wave</span> approximation (GSRWA) is proposed by employing both the displacement and the squeezing transformations. A solvable Hamiltonian is reformulated in the same form as the ordinary RWA ones. For a qubit <span class="hlt">coupled</span> to oscillators experiment, a well-defined Schrödinger-cat-like entangled state is given by the displaced-squeezed oscillator state instead of the original displaced state. For the isotropic Rabi case, the mean photon number and the ground-state energy are expressed analytically with additional squeezing terms, exhibiting a substantial improvement of the GSRWA. And the ground-state energy in the anisotropic Rabi <span class="hlt">model</span> confirms the effectiveness of the GSRWA. Due to the squeezing effect, the GSRWA improves the previous methods only with the displacement transformation in a wide range of <span class="hlt">coupling</span> strengths even for large atom frequency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DPPUP2036A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DPPUP2036A"><span>Non-linear Frequency Shifts, Mode <span class="hlt">Couplings</span>, and Decay Instability of Plasma <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Affolter, Mathew; Anderegg, F.; Driscoll, C. F.; Valentini, F.</p> <p>2015-11-01</p> <p>We present experiments and theory for non-linear plasma <span class="hlt">wave</span> decay to longer wavelengths, in both the oscillatory <span class="hlt">coupling</span> and exponential decay regimes. The experiments are conducted on non-neutral plasmas in cylindrical Penning-Malmberg traps, θ-symmetric standing plasma <span class="hlt">waves</span> have near acoustic dispersion ω (kz) ~kz - αkz2 , discretized by kz =mz (π /Lp) . Large amplitude <span class="hlt">waves</span> exhibit non-linear frequency shifts δf / f ~A2 and Fourier harmonic content, both of which are increased as the plasma dispersion is reduced. Non-linear <span class="hlt">coupling</span> rates are measured between large amplitude mz = 2 <span class="hlt">waves</span> and small amplitude mz = 1 <span class="hlt">waves</span>, which have a small detuning Δω = 2ω1 -ω2 . At small excitation amplitudes, this detuning causes the mz = 1 mode amplitude to ``bounce'' at rate Δω , with amplitude excursions ΔA1 ~ δn2 /n0 consistent with cold fluid theory and Vlasov simulations. At larger excitation amplitudes, where the non-linear <span class="hlt">coupling</span> exceeds the dispersion, phase-locked exponential growth of the mz = 1 mode is observed, in qualitative agreement with simple 3-<span class="hlt">wave</span> instability theory. However, significant variations are observed experimentally, and N-<span class="hlt">wave</span> theory gives stunningly divergent predictions that depend sensitively on the dispersion-moderated harmonic content. Measurements on higher temperature Langmuir <span class="hlt">waves</span> and the unusual ``EAW'' (KEEN) <span class="hlt">waves</span> are being conducted to investigate the effects of <span class="hlt">wave</span>-particle kinetics on the non-linear <span class="hlt">coupling</span> rates. Department of Energy Grants DE-SC0002451and DE-SC0008693.</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 layered lattice <span class="hlt">model</span> and generalized solitary <span class="hlt">waves</span> 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 <span class="hlt">waves</span> in a two-layered 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 <span class="hlt">waves</span> in a layered lattice with a soft middle (or bonding) layer are governed by a system of <span class="hlt">coupled</span> Boussinesq-type equations. For this system we find conservation laws and show that pure solitary <span class="hlt">waves</span>, which exist in a single equation and can exist in the <span class="hlt">coupled</span> system in the symmetric case, are structurally unstable and are replaced with generalized solitary <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMEP21C1863G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMEP21C1863G"><span><span class="hlt">Coupling</span> Effects of Unsteady River Discharges and <span class="hlt">Wave</span> Conditions on Mouth Bar Formation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gao, W.; Shao, D.; Zheng Bing, W.; Yang, W.; Sun, T.; Cui, B.</p> <p>2017-12-01</p> <p>As a key morphological unit at delta front, the evolution of mouth bar is of critical importance to channel bifurcation and the formation of deltaic distributaries, and therefore have received wide attention, primarily using numerical <span class="hlt">modelling</span> approaches. Notably, the existing numerical <span class="hlt">modelling</span> studies were mostly carried out under the assumption that most of the sediments are delivered to the ocean during bankfull discharge stages, so is the most significant deltaic morphological evolution, and hence periods of relatively low river discharge were `safely' neglected, leaving out the effects of unsteadiness of river discharge on the relevant morphodynamic processes altogether. However, the above assumption is worth reviewing in the context of combined fluvial and marine forcing as the relative <span class="hlt">wave</span> strength has been repeatedly proved to be a critical parameter in estuarine-deltaic morphodynamics. In natural deltas, the period of high river discharge may or may not coincide with the occurrence of maximum <span class="hlt">wave</span> strength, which further complicates their <span class="hlt">coupling</span> effects. To assess the <span class="hlt">coupling</span> effects of unsteady river discharges and <span class="hlt">wave</span> conditions on mouth bar formation, numerical experiments using Delft3D-SWAN were conducted in this study. A host of combined high-and-low river discharges <span class="hlt">coupled</span> with varying <span class="hlt">wave</span> strengths were assumed to mimic the natural variability. Numerical simulation results suggest the existence of three regimes for mouth bar formation, namely, nonexistence of mouth bar (G1), formation of ephemeral mouth bar (G2) and formation of stable mouth bar (G3), which were dictated by the relative <span class="hlt">wave</span> strength during both onset and reworking stages as well as the reworking time. Implications of the mouth bar formation regimes on delta distributary networks were also discussed. The findings have implications for coastal management at estuaries and deltas such as erosion prevention and mitigation, water and sediment regulation scheme, etc.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20110011701','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20110011701"><span><span class="hlt">Modeling</span> the Inner Magnetosphere: Radiation Belts, Ring <span class="hlt">Current</span>, and Composition</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Glocer, Alex</p> <p>2011-01-01</p> <p>The space environment is a complex system defined by regions of differing length scales, characteristic energies, and physical processes. It is often difficult, or impossible, to treat all aspects of the space environment relative to a particular problem with a single <span class="hlt">model</span>. In our studies, we utilize several <span class="hlt">models</span> working in tandem to examine this highly interconnected system. The methodology and results will be presented for three focused topics: 1) Rapid radiation belt electron enhancements, 2) Ring <span class="hlt">current</span> study of Energetic Neutral Atoms (ENAs), Dst, and plasma composition, and 3) Examination of the outflow of ionospheric ions. In the first study, we use a <span class="hlt">coupled</span> MHD magnetosphere - kinetic radiation belt <span class="hlt">model</span> to explain recent Akebono/RDM observations of greater than 2.5 MeV radiation belt electron enhancements occurring on timescales of less than a few hours. In the second study, we present initial results of a ring <span class="hlt">current</span> study using a newly <span class="hlt">coupled</span> kinetic ring <span class="hlt">current</span> <span class="hlt">model</span> with an MHD magnetosphere <span class="hlt">model</span>. Results of a dst study for four geomagnetic events are shown. Moreover, direct comparison with TWINS ENA images are used to infer the role that composition plays in the ring <span class="hlt">current</span>. In the final study, we directly <span class="hlt">model</span> the transport of plasma from the ionosphere to the magnetosphere. We especially focus on the role of photoelectrons and and <span class="hlt">wave</span>-particle interactions. The <span class="hlt">modeling</span> methodology for each of these studies will be detailed along with the results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EL.....9237010S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EL.....9237010S"><span>Charge creation and nucleation of the longitudinal plasma <span class="hlt">wave</span> in <span class="hlt">coupled</span> Josephson junctions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shukrinov, Yu. M.; Hamdipour, M.</p> <p>2010-11-01</p> <p>We study the phase dynamics in <span class="hlt">coupled</span> Josephson junctions described by a system of nonlinear differential equations. Results of detailed numerical simulations of charge creation in the superconducting layers and the longitudinal plasma <span class="hlt">wave</span> (LPW) nucleation are presented. We demonstrate the different time stages in the development of the LPW and present the results of FFT analysis at different values of bias <span class="hlt">current</span>. The correspondence between the breakpoint position on the outermost branch of <span class="hlt">current</span> voltage characteristics (CVC) and the growing region in time dependence of the electric charge in the superconducting layer is established. The effects of noise in the bias <span class="hlt">current</span> and the external microwave radiation on the charge dynamics of the <span class="hlt">coupled</span> Josephson junctions are found. These effects introduce a way to regulate the process of LPW nucleation in the stack of IJJ.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018AnGeo..36..425T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018AnGeo..36..425T"><span>Satellite observations of middle atmosphere-thermosphere vertical <span class="hlt">coupling</span> by gravity <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Trinh, Quang Thai; Ern, Manfred; Doornbos, Eelco; Preusse, Peter; Riese, Martin</p> <p>2018-03-01</p> <p>Atmospheric gravity <span class="hlt">waves</span> (GWs) are essential for the dynamics of the middle atmosphere. Recent studies have shown that these <span class="hlt">waves</span> are also important for the thermosphere/ionosphere (T/I) system. Via vertical <span class="hlt">coupling</span>, GWs can significantly influence the mean state of the T/I system. However, the penetration of GWs into the T/I system is not fully understood in <span class="hlt">modeling</span> as well as observations. In the <span class="hlt">current</span> study, we analyze the correlation between GW momentum fluxes observed in the middle atmosphere (30-90 km) and GW-induced perturbations in the T/I. In the middle atmosphere, GW momentum fluxes are derived from temperature observations of the Sounding of the Atmosphere using Broadband Emission Radiometry (SABER) satellite instrument. In the T/I, GW-induced perturbations are derived from neutral density measured by instruments on the Gravity field and Ocean Circulation Explorer (GOCE) and CHAllenging Minisatellite Payload (CHAMP) satellites. We find generally positive correlations between horizontal distributions at low altitudes (i.e., below 90 km) and horizontal distributions of GW-induced density fluctuations in the T/I (at 200 km and above). Two <span class="hlt">coupling</span> mechanisms are likely responsible for these positive correlations: (1) fast GWs generated in the troposphere and lower stratosphere can propagate directly to the T/I and (2) primary GWs with their origins in the lower atmosphere dissipate while propagating upwards and generate secondary GWs, which then penetrate up to the T/I and maintain the spatial patterns of GW distributions in the lower atmosphere. The mountain-<span class="hlt">wave</span> related hotspot over the Andes and Antarctic Peninsula is found clearly in observations of all instruments used in our analysis. Latitude-longitude variations in the summer midlatitudes are also found in observations of all instruments. These variations and strong positive correlations in the summer midlatitudes suggest that GWs with origins related to convection also propagate up to the T</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19940012862','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19940012862"><span>Review of rigorous <span class="hlt">coupled-wave</span> analysis and of homogeneous effective medium approximations for high spatial-frequency surface-relief gratings</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Glytsis, Elias N.; Brundrett, David L.; Gaylord, Thomas K.</p> <p>1993-01-01</p> <p>A review of the rigorous <span class="hlt">coupled-wave</span> analysis as applied to the diffraction of electro-magnetic <span class="hlt">waves</span> by gratings is presented. The analysis is valid for any polarization, angle of incidence, and conical diffraction. Cascaded and/or multiplexed gratings as well as material anisotropy can be incorporated under the same formalism. Small period rectangular groove gratings can also be <span class="hlt">modeled</span> using approximately equivalent uniaxial homogeneous layers (effective media). The ordinary and extraordinary refractive indices of these layers depend on the gratings filling factor, the refractive indices of the substrate and superstrate, and the ratio of the freespace wavelength to grating period. Comparisons of the homogeneous effective medium approximations with the rigorous <span class="hlt">coupled-wave</span> analysis are presented. Antireflection designs (single-layer or multilayer) using the effective medium <span class="hlt">models</span> are presented and compared. These ultra-short period antireflection gratings can also be used to produce soft x-rays. Comparisons of the rigorous <span class="hlt">coupled-wave</span> analysis with experimental results on soft x-ray generation by gratings are also included.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMOS51C1890R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMOS51C1890R"><span>Effects of <span class="hlt">Wave</span> Energy Converter (WEC) Arrays on <span class="hlt">Wave</span>, <span class="hlt">Current</span>, and Sediment Circulation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ruehl, K.; Roberts, J. D.; Jones, C.; Magalen, J.; James, S. C.</p> <p>2012-12-01</p> <p>The characterization of the physical environment and commensurate alteration of that environment due to <span class="hlt">Wave</span> Energy Conversion (WEC) devices, or arrays of devices, must be understood to make informed device-performance predictions, specifications of hydrodynamic loads, and environmental evaluations of eco-system responses (e.g., changes to circulation patterns, sediment dynamics, and water quality). Hydrodynamic and sediment issues associated with performance of <span class="hlt">wave</span>-energy devices will primarily be nearshore where WEC infrastructure (e.g., anchors, piles) are exposed to large forces from the surface-<span class="hlt">wave</span> action and <span class="hlt">currents</span>. <span class="hlt">Wave</span>-energy devices will be subject to additional corrosion, fouling, and wear of moving parts caused by suspended sediments in the water column. The alteration of the circulation and sediment transport patterns may also alter local ecosystems through changes in benthic habitat, circulation patterns, or other environmental parameters. Sandia National Laboratories is developing tools and performing studies to quantitatively characterize the environments where WEC devices may be installed and to assess potential affects to hydrodynamics and local sediment transport. The primary tools are <span class="hlt">wave</span>, hydrodynamic, and sediment transport <span class="hlt">models</span>. To ensure confidence in the resulting evaluation of system-wide effects, the <span class="hlt">models</span> are appropriately constrained and validated with measured data where available. An extension of the US EPA's EFDC code, SNL-EFDC, provides a suitable platform for <span class="hlt">modeling</span> the necessary hydrodynamics;it has been modified to directly incorporate output from a SWAN <span class="hlt">wave</span> <span class="hlt">model</span> of the region. <span class="hlt">Model</span> development and results are presented. In this work, a <span class="hlt">model</span> is exercised for Monterey Bay, near Santa Cruz where a WEC array could be deployed. Santa Cruz is located on the northern coast of Monterey Bay, in Central California, USA. This site was selected for preliminary research due to the readily available historical hydrodynamic data</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016NucFu..56g6009R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016NucFu..56g6009R"><span>Conceptual study of an ICRH traveling-<span class="hlt">wave</span> antenna system for low-<span class="hlt">coupling</span> conditions as expected in DEMO</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ragona, R.; Messiaen, A.</p> <p>2016-07-01</p> <p>For the central heating of a fusion reactor ion cyclotron radio frequency heating (ICRH) is the first choice method as it is able to <span class="hlt">couple</span> RF power to the ions without density limit. The drawback of this heating method is the problem of excitation of the magneto-sonic <span class="hlt">wave</span> through the plasma boundary layer from the antenna located along the wall, without exceeding its voltage standoff. The amount of <span class="hlt">coupling</span> depends on the antenna excitation and the surface admittance at the antenna output due to the plasma profile. The paper deals with the optimization of the antenna excitation by the use of sections of traveling-<span class="hlt">wave</span> antennas (TWAs) distributed all along the reactor wall between the blanket modules. They are mounted and fed in resonant ring system(s). First, the physics of the <span class="hlt">coupling</span> of a strap array is studied by simple <span class="hlt">models</span> and the <span class="hlt">coupling</span> code ANTITER II. Then, after the study of the basic properties of a TWA section, its feeding problem is solved by hybrids driving them in resonant ring circuit(s). The complete <span class="hlt">modeling</span> is obtained from the matrices of the TWA sections connected to one of the feeding hybrid(s). The solution is iterated with the <span class="hlt">coupling</span> code to determine the loading for a reference low-<span class="hlt">coupling</span> ITER plasma profile. The resulting <span class="hlt">wave</span> pattern up to the plasma bulk is derived. The proposed system is totally load resilient and allows us to obtain a very selective exciting <span class="hlt">wave</span> spectrum. A discussion of some practical implementation problems is added.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23860834','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23860834"><span>Attraction and repulsion of spiral <span class="hlt">waves</span> by inhomogeneity of conduction anisotropy--a <span class="hlt">model</span> of spiral <span class="hlt">wave</span> interaction with electrical remodeling of heart tissue.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kuklik, Pawel; Sanders, Prashanthan; Szumowski, Lukasz; Żebrowski, Jan J</p> <p>2013-01-01</p> <p>Various forms of heart disease are associated with remodeling of the heart muscle, which results in a perturbation of cell-to-cell electrical <span class="hlt">coupling</span>. These perturbations may alter the trajectory of spiral <span class="hlt">wave</span> drift in the heart muscle. We investigate the effect of spatially extended inhomogeneity of transverse cell <span class="hlt">coupling</span> on the spiral <span class="hlt">wave</span> trajectory using a simple active media <span class="hlt">model</span>. The spiral <span class="hlt">wave</span> was either attracted or repelled from the center of inhomogeneity as a function of cell excitability and gradient of the cell <span class="hlt">coupling</span>. High levels of excitability resulted in an attraction of the <span class="hlt">wave</span> to the center of inhomogeneity, whereas low levels resulted in an escape and termination of the spiral <span class="hlt">wave</span>. The spiral <span class="hlt">wave</span> drift velocity was related to the gradient of the <span class="hlt">coupling</span> and the initial position of the <span class="hlt">wave</span>. In a diseased heart, a region of altered transverse <span class="hlt">coupling</span> corresponds with local gap junction remodeling that may be responsible for stabilization-destabilization of spiral <span class="hlt">waves</span> and hence reflect potentially important targets in the treatment of heart arrhythmias.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70039994','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70039994"><span><span class="hlt">Coupled</span> atmosphere-ocean-<span class="hlt">wave</span> simulations of a storm event over the Gulf of Lion and Balearic Sea</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Renault, Lionel; Chiggiato, Jacopo; Warner, John C.; Gomez, Marta; Vizoso, Guillermo; Tintore, Joaquin</p> <p>2012-01-01</p> <p>The coastal areas of the North-Western Mediterranean Sea are one of the most challenging places for ocean forecasting. This region is exposed to severe storms events that are of short duration. During these events, significant air-sea interactions, strong winds and large sea-state can have catastrophic consequences in the coastal areas. To investigate these air-sea interactions and the oceanic response to such events, we implemented the <span class="hlt">Coupled</span> Ocean-Atmosphere-<span class="hlt">Wave</span>-Sediment Transport <span class="hlt">Modeling</span> System simulating a severe storm in the Mediterranean Sea that occurred in May 2010. During this event, wind speed reached up to 25 m.s-1 inducing significant sea surface cooling (up to 2°C) over the Gulf of Lion (GoL) and along the storm track, and generating surface <span class="hlt">waves</span> with a significant height of 6 m. It is shown that the event, associated with a cyclogenesis between the Balearic Islands and the GoL, is relatively well reproduced by the <span class="hlt">coupled</span> system. A surface heat budget analysis showed that ocean vertical mixing was a major contributor to the cooling tendency along the storm track and in the GoL where turbulent heat fluxes also played an important role. Sensitivity experiments on the ocean-atmosphere <span class="hlt">coupling</span> suggested that the <span class="hlt">coupled</span> system is sensitive to the momentum flux parameterization as well as air-sea and air-<span class="hlt">wave</span> <span class="hlt">coupling</span>. Comparisons with available atmospheric and oceanic observations showed that the use of the fully <span class="hlt">coupled</span> system provides the most skillful simulation, illustrating the benefit of using a fully <span class="hlt">coupled</span> ocean-atmosphere-<span class="hlt">wave</span> <span class="hlt">model</span> for the assessment of these storm events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25468351','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25468351"><span>Intrinsic islet heterogeneity and gap junction <span class="hlt">coupling</span> determine spatiotemporal Ca²⁺ <span class="hlt">wave</span> dynamics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Benninger, Richard K P; Hutchens, Troy; Head, W Steven; McCaughey, Michael J; Zhang, Min; Le Marchand, Sylvain J; Satin, Leslie S; Piston, David W</p> <p>2014-12-02</p> <p>Insulin is released from the islets of Langerhans in discrete pulses that are linked to synchronized oscillations of intracellular free calcium ([Ca(2+)]i). Associated with each synchronized oscillation is a propagating calcium <span class="hlt">wave</span> mediated by Connexin36 (Cx36) gap junctions. A computational islet <span class="hlt">model</span> predicted that <span class="hlt">waves</span> emerge due to heterogeneity in β-cell function throughout the islet. To test this, we applied defined patterns of glucose stimulation across the islet using a microfluidic device and measured how these perturbations affect calcium <span class="hlt">wave</span> propagation. We further investigated how gap junction <span class="hlt">coupling</span> regulates spatiotemporal [Ca(2+)]i dynamics in the face of heterogeneous glucose stimulation. Calcium <span class="hlt">waves</span> were found to originate in regions of the islet having elevated excitability, and this heterogeneity is an intrinsic property of islet β-cells. The extent of [Ca(2+)]i elevation across the islet in the presence of heterogeneity is gap-junction dependent, which reveals a glucose dependence of gap junction <span class="hlt">coupling</span>. To better describe these observations, we had to modify the computational islet <span class="hlt">model</span> to consider the electrochemical gradient between neighboring β-cells. These results reveal how the spatiotemporal [Ca(2+)]i dynamics of the islet depend on β-cell heterogeneity and cell-cell <span class="hlt">coupling</span>, and are important for understanding the regulation of coordinated insulin release across the islet. Copyright © 2014 Biophysical Society. Published by Elsevier Inc. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20120011991','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20120011991"><span>A Review of Low Frequency Electromagnetic <span class="hlt">Wave</span> Phenomena Related to Tropospheric-Ionospheric <span class="hlt">Coupling</span> Mechanisms</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Simoes, Fernando; Pfaff, Robert; Berthelier, Jean-Jacques; Klenzing, Jeffrey</p> <p>2012-01-01</p> <p>Investigation of <span class="hlt">coupling</span> mechanisms between the troposphere and the ionosphere requires a multidisciplinary approach involving several branches of atmospheric sciences, from meteorology, atmospheric chemistry, and fulminology to aeronomy, plasma physics, and space weather. In this work, we review low frequency electromagnetic <span class="hlt">wave</span> propagation in the Earth-ionosphere cavity from a troposphere-ionosphere <span class="hlt">coupling</span> perspective. We discuss electromagnetic <span class="hlt">wave</span> generation, propagation, and resonance phenomena, considering atmospheric, ionospheric and magnetospheric sources, from lightning and transient luminous events at low altitude to Alfven <span class="hlt">waves</span> and particle precipitation related to solar and magnetospheric processes. We review in situ ionospheric processes as well as surface and space weather phenomena that drive troposphere-ionosphere dynamics. Effects of aerosols, water vapor distribution, thermodynamic parameters, and cloud charge separation and electrification processes on atmospheric electricity and electromagnetic <span class="hlt">waves</span> are reviewed. We also briefly revisit ionospheric irregularities such as spread-F and explosive spread-F, sporadic-E, traveling ionospheric disturbances, Trimpi effect, and hiss and plasma turbulence. Regarding the role of the lower boundary of the cavity, we review transient surface phenomena, including seismic activity, earthquakes, volcanic processes and dust electrification. The role of surface and atmospheric gravity <span class="hlt">waves</span> in ionospheric dynamics is also briefly addressed. We summarize analytical and numerical tools and techniques to <span class="hlt">model</span> low frequency electromagnetic <span class="hlt">wave</span> propagation and solving inverse problems and summarize in a final section a few challenging subjects that are important for a better understanding of tropospheric-ionospheric <span class="hlt">coupling</span> mechanisms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013APS..SHK.O2003L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013APS..SHK.O2003L"><span>International Shock-<span class="hlt">Wave</span> Database: <span class="hlt">Current</span> Status</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Levashov, Pavel</p> <p>2013-06-01</p> <p>Shock-<span class="hlt">wave</span> and related dynamic material response data serve for calibrating, validating, and improving material <span class="hlt">models</span> over very broad regions of the pressure-temperature-density phase space. Since the middle of the 20th century vast amount of shock-<span class="hlt">wave</span> experimental information has been obtained. To systemize it a number of compendiums of shock-<span class="hlt">wave</span> data has been issued by LLNL, LANL (USA), CEA (France), IPCP and VNIIEF (Russia). In mid-90th the drawbacks of the paper handbooks became obvious, so the first version of the online shock-<span class="hlt">wave</span> database appeared in 1997 (http://www.ficp.ac.ru/rusbank). It includes approximately 20000 experimental points on shock compression, adiabatic expansion, measurements of sound velocity behind the shock front and free-surface-velocity for more than 650 substances. This is still a useful tool for the shock-<span class="hlt">wave</span> community, but it has a number of serious disadvantages which can't be easily eliminated: (i) very simple data format for points and references; (ii) minimalistic user interface for data addition; (iii) absence of history of changes; (iv) bad feedback from users. The new International Shock-<span class="hlt">Wave</span> database (ISWdb) is intended to solve these and some other problems. The ISWdb project objectives are: (i) to develop a database on thermodynamic and mechanical properties of materials under conditions of shock-<span class="hlt">wave</span> and other dynamic loadings, selected related quantities of interest, and the meta-data that describes the provenance of the measurements and material <span class="hlt">models</span>; and (ii) to make this database available internationally through the Internet, in an interactive form. The development and operation of the ISWdb is guided by an advisory committee. The database will be installed on two mirrored web-servers, one in Russia and the other in USA (<span class="hlt">currently</span> only one server is available). The database provides access to original experimental data on shock compression, non-shock dynamic loadings, isentropic expansion, measurements of sound</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70016373','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70016373"><span>Sediment movement along the U.S. east coast continental shelf-I. Estimates of bottom stress using the Grant-Madsen <span class="hlt">model</span> and near-bottom <span class="hlt">wave</span> and <span class="hlt">current</span> measurements</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Lyne, V.D.; Butman, B.; Grant, W.D.</p> <p>1990-01-01</p> <p>Bottom stress is calculated for several long-term time-series observations, made on the U.S. east coast continental shelf during winter, using the <span class="hlt">wave-current</span> interaction and moveable bed <span class="hlt">models</span> of Grant and Madsen (1979, Journal of Geophysical Research, 84, 1797-1808; 1982, Journal of Geophysical Research, 87, 469-482). The <span class="hlt">wave</span> and <span class="hlt">current</span> measurements were obtained by means of a bottom tripod system which measured <span class="hlt">current</span> using a Savonius rotor and vane and <span class="hlt">waves</span> by means of a pressure sensor. The variables were burst sampled about 10% of the time. <span class="hlt">Wave</span> energy was reasonably resolved, although aliased by <span class="hlt">wave</span> groupiness, and <span class="hlt">wave</span> period was accurate to 1-2 s during large storms. Errors in <span class="hlt">current</span> speed and direction depend on the speed of the mean <span class="hlt">current</span> relative to the <span class="hlt">wave</span> <span class="hlt">current</span>. In general, errors in bottom stress caused by uncertainties in measured <span class="hlt">current</span> speed and <span class="hlt">wave</span> characteristics were 10-20%. During storms, the bottom stress calculated using the Grant-Madsen <span class="hlt">models</span> exceeded stress computed from conventional drag laws by a factor of about 1.5 on average and 3 or more during storm peaks. Thus, even in water as deep as 80 m, oscillatory near-bottom <span class="hlt">currents</span> associated with surface gravity <span class="hlt">waves</span> of period 12 s or longer will contribute substantially to bottom stress. Given that the Grant-Madsen <span class="hlt">model</span> is correct, parameterizations of bottom stress that do not incorporate <span class="hlt">wave</span> effects will substantially underestimate stress and sediment transport in this region of the continental shelf.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22489342-guiding-bending-splitting-coupled-defect-surface-modes-surface-wave-photonic-crystal','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22489342-guiding-bending-splitting-coupled-defect-surface-modes-surface-wave-photonic-crystal"><span>Guiding, bending, and splitting of <span class="hlt">coupled</span> defect surface modes in a surface-<span class="hlt">wave</span> photonic crystal</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>Gao, Zhen; Gao, Fei; Zhang, Baile, E-mail: blzhang@ntu.edu.sg</p> <p>2016-01-25</p> <p>We experimentally demonstrate a type of waveguiding mechanism for <span class="hlt">coupled</span> surface-<span class="hlt">wave</span> defect modes in a surface-<span class="hlt">wave</span> photonic crystal. Unlike conventional spoof surface plasmon waveguides, waveguiding of <span class="hlt">coupled</span> surface-<span class="hlt">wave</span> defect modes is achieved through weak <span class="hlt">coupling</span> between tightly localized defect cavities in an otherwise gapped surface-<span class="hlt">wave</span> photonic crystal, as a classical <span class="hlt">wave</span> analogue of tight-binding electronic wavefunctions in solid state lattices. <span class="hlt">Wave</span> patterns associated with the high transmission of <span class="hlt">coupled</span> defect surface modes are directly mapped with a near-field microwave scanning probe for various structures including a straight waveguide, a sharp corner, and a T-shaped splitter. These results may find usemore » in the design of integrated surface-<span class="hlt">wave</span> devices with suppressed crosstalk.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/15728774','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/15728774"><span>Effect of electrical <span class="hlt">coupling</span> on ionic <span class="hlt">current</span> and synaptic potential measurements.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Rabbah, Pascale; Golowasch, Jorge; Nadim, Farzan</p> <p>2005-07-01</p> <p>Recent studies have found electrical <span class="hlt">coupling</span> to be more ubiquitous than previously thought, and <span class="hlt">coupling</span> through gap junctions is known to play a crucial role in neuronal function and network output. In particular, <span class="hlt">current</span> spread through gap junctions may affect the activation of voltage-dependent conductances as well as chemical synaptic release. Using voltage-clamp recordings of two strongly electrically <span class="hlt">coupled</span> neurons of the lobster stomatogastric ganglion and conductance-based <span class="hlt">models</span> of these neurons, we identified effects of electrical <span class="hlt">coupling</span> on the measurement of leak and voltage-gated outward <span class="hlt">currents</span>, as well as synaptic potentials. Experimental measurements showed that both leak and voltage-gated outward <span class="hlt">currents</span> are recruited by gap junctions from neurons <span class="hlt">coupled</span> to the clamped cell. Nevertheless, in spite of the strong <span class="hlt">coupling</span> between these neurons, the errors made in estimating voltage-gated conductance parameters were relatively minor (<10%). Thus in many cases isolation of <span class="hlt">coupled</span> neurons may not be required if a small degree of measurement error of the voltage-gated <span class="hlt">currents</span> or the synaptic potentials is acceptable. <span class="hlt">Modeling</span> results show, however, that such errors may be as high as 20% if the gap-junction position is near the recording site or as high as 90% when measuring smaller voltage-gated ionic <span class="hlt">currents</span>. Paradoxically, improved space clamp increases the errors arising from electrical <span class="hlt">coupling</span> because voltage control across gap junctions is poor for even the highest realistic <span class="hlt">coupling</span> conductances. Furthermore, the common procedure of leak subtraction can add an extra error to the conductance measurement, the sign of which depends on the maximal conductance.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70190327','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70190327"><span>Methodology for prediction of rip <span class="hlt">currents</span> using a three-dimensional numerical, <span class="hlt">coupled</span>, <span class="hlt">wave</span> <span class="hlt">current</span> <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>Voulgaris, George; Kumar, Nirnimesh; Warner, John C.; Leatherman, Stephen; Fletemeyer, John</p> <p>2011-01-01</p> <p>Rip <span class="hlt">current</span> <span class="hlt">currents</span> constitute one of the most common hazards in the nearshore that threaten the lives of the unaware public that makes recreational use of the coastal zone. Society responds to this danger through a number of measures that include: (a) the deployment of trained lifeguards; (b) public education related to the hidden hazards of the nearshore; and (c) establishment of warning systems.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_14 --> <div id="page_15" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li class="active"><span>15</span></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="281"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JNS....26.1767G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JNS....26.1767G"><span>Traveling and Standing <span class="hlt">Waves</span> in <span class="hlt">Coupled</span> Pendula and Newton's Cradle</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>García-Azpeitia, Carlos</p> <p>2016-12-01</p> <p>The existence of traveling and standing <span class="hlt">waves</span> is investigated for chains of <span class="hlt">coupled</span> pendula with periodic boundary conditions. The results are proven by applying topological methods to subspaces of symmetric solutions. The main advantage of this approach comes from the fact that only properties of the linearized forces are required. This allows to cover a wide range of <span class="hlt">models</span> such as Newton's cradle, the Fermi-Pasta-Ulam lattice, and the Toda lattice.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvE..97a2406L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvE..97a2406L"><span><span class="hlt">Wave</span> failure at strong <span class="hlt">coupling</span> in intracellular C a2 + signaling system with clustered channels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Xiang; Wu, Yuning; Gao, Xuejuan; Cai, Meichun; Shuai, Jianwei</p> <p>2018-01-01</p> <p>As an important intracellular signal, C a2 + ions control diverse cellular functions. In this paper, we discuss the C a2 + signaling with a two-dimensional <span class="hlt">model</span> in which the inositol 1,4,5-trisphosphate (I P3 ) receptor channels are distributed in clusters on the endoplasmic reticulum membrane. The <span class="hlt">wave</span> failure at large C a2 + diffusion <span class="hlt">coupling</span> is discussed in detail in the <span class="hlt">model</span>. We show that with varying <span class="hlt">model</span> parameters the <span class="hlt">wave</span> failure is a robust behavior with either deterministic or stochastic channel dynamics. We suggest that the <span class="hlt">wave</span> failure should be a general behavior in inhomogeneous diffusing systems with clustered excitable regions and may occur in biological C a2 + signaling systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhPl...19i2115A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhPl...19i2115A"><span>Linear and nonlinear dynamics of <span class="hlt">current</span>-driven <span class="hlt">waves</span> in dusty plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahmad, Ali; Ali Shan, S.; Haque, Q.; Saleem, H.</p> <p>2012-09-01</p> <p>The linear and nonlinear dynamics of a recently proposed plasma mode of dusty plasma is studied using kappa distribution for electrons. This electrostatic <span class="hlt">wave</span> can propagate in the plasma due to the sheared flow of electrons and ions parallel to the external magnetic field in the presence of stationary dust. The <span class="hlt">coupling</span> of this <span class="hlt">wave</span> with the usual drift <span class="hlt">wave</span> and ion acoustic <span class="hlt">wave</span> is investigated. D'Angelo's mode is also modified in the presence of superthermal electrons. In the nonlinear regime, the <span class="hlt">wave</span> can give rise to dipolar vortex structures if the shear in flow is weaker and tripolar vortices if the flow has steeper gradient. The results have been applied to Saturn's magnetosphere corresponding to negatively charged dust grains. But the theoretical <span class="hlt">model</span> is applicable for positively charged dust as well. This work will be useful for future observations and studies of dusty environments of planets and comets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT.......141G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT.......141G"><span><span class="hlt">Wave</span> <span class="hlt">Coupling</span> between the Lower and Middle Thermosphere as Viewed from Quasi-Sun-Synchronous Satellites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gasperini, Federico</p> <p></p> <p>In a society increasingly dependent on space technology, space weather has become a prominent scientific paradigm. In the last decade evidence has shown that terrestrial weather significantly influences space weather. Periodic absorption of solar radiation in local time and longitude by tropospheric water vapor and stratospheric ozone as well as latent heat release in clouds generate a spatially- and temporally-evolving spectrum of global-scale atmospheric <span class="hlt">waves</span> (i.e., tides, planetary <span class="hlt">waves</span> and Kelvin <span class="hlt">waves</span>). A subset of these <span class="hlt">waves</span> propagates vertically, evolving with height due to <span class="hlt">wave</span>-mean flow, <span class="hlt">wave-wave</span>, and <span class="hlt">wave</span>-plasma interactions, and driving electric fields of tidal origin in the dynamo region. While considerable improvements have been made on the understanding of MLT dynamics, driven in part by the development and deployment of new instruments and techniques, relatively little is known about the <span class="hlt">coupling</span> of <span class="hlt">waves</span> in the 120-300 km `thermospheric gap' between satellite remote-sensing and in-situ <span class="hlt">wave</span> diagnostics. The dissertation herein reveals vertical <span class="hlt">wave</span> <span class="hlt">coupling</span> in this height region and quantifies its role in determining thermospheric variability. This objective is accomplished employing quasi-Sun-synchronous satellite measurements (i.e., TIMED, CHAMP, and GOCE) and state-of-the-art numerical <span class="hlt">modeling</span> simulations (i.e., TIME-GCM/MERRA). Evidence is found for the vertical propagation from the lower to the middle thermosphere of the eastward propagating diurnal tide with zonal <span class="hlt">wave</span> number 3 (DE3) and the 3-day ultra-fast Kelvin <span class="hlt">wave</span> (UFKW), two major global-scale atmospheric oscillations of tropospheric origin. These <span class="hlt">waves</span> are shown to nonlinearly interact and produce secondary <span class="hlt">waves</span> responsible for significant longitudinal and day-to-day variability. For solar and geomagnetic quiet conditions, atmospheric <span class="hlt">waves</span> are found to be responsible for up to 60% of the total variability, demonstrating lower atmosphere <span class="hlt">coupling</span> as a key contributor to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PhRvB..92g5123D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PhRvB..92g5123D"><span>Strong competition between ΘI I-loop-<span class="hlt">current</span> order and d -<span class="hlt">wave</span> charge order along the diagonal direction in a two-dimensional hot spot <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>de Carvalho, Vanuildo S.; Kloss, Thomas; Montiel, Xavier; Freire, Hermann; Pépin, Catherine</p> <p>2015-08-01</p> <p>We study the fate of the so-called ΘI I-loop-<span class="hlt">current</span> order that breaks both time-reversal and parity symmetries in a two-dimensional hot spot <span class="hlt">model</span> with antiferromagnetically mediated interactions, using Fermi surfaces relevant to the phenomenology of the cuprate superconductors. We start from a three-band Emery <span class="hlt">model</span> describing the hopping of holes in the CuO2 plane that includes two hopping parameters tp p and tp d, local onsite Coulomb interactions Ud and Up, and nearest-neighbor Vp d <span class="hlt">couplings</span> between the fermions in the copper [Cu (3 dx2-y2) ] and oxygen [O (2 px) and O (2 py)] orbitals. By focusing on the lowest-energy band, we proceed to decouple the local interaction Ud of the Cu orbital in the spin channel using a Hubbard-Stratonovich transformation to arrive at the interacting part of the so-called spin-fermion <span class="hlt">model</span>. We also decouple the nearest-neighbor interaction Vp d to introduce the order parameter of the ΘI I-loop-<span class="hlt">current</span> order. In this way, we are able to construct a consistent mean-field theory that describes the strong competition between the composite order parameter made of a quadrupole-density <span class="hlt">wave</span> and d -<span class="hlt">wave</span> pairing fluctuations proposed in Efetov et al. [Nat. Phys. 9, 442 (2013), 10.1038/nphys2641] with the ΘI I-loop-<span class="hlt">current</span> order parameter that is argued to be relevant for explaining important aspects of the physics of the pseudogap phase displayed in the underdoped cuprates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22835663','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22835663"><span>Mechano-electrical feedback explains T-<span class="hlt">wave</span> morphology and optimizes cardiac pump function: insight from a multi-scale <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>Hermeling, Evelien; Delhaas, Tammo; Prinzen, Frits W; Kuijpers, Nico H L</p> <p>2012-01-01</p> <p>In the ECG, T- and R-<span class="hlt">wave</span> are concordant during normal sinus rhythm (SR), but discordant after a period of ventricular pacing (VP). Experiments showed that the latter phenomenon, called T-<span class="hlt">wave</span> memory, is mediated by a mechanical stimulus. By means of a mathematical <span class="hlt">model</span>, we investigated the hypothesis that slow acting mechano-electrical feedback (MEF) explains T-<span class="hlt">wave</span> memory. In our <span class="hlt">model</span>, electromechanical behavior of the left ventricle (LV) was simulated using a series of mechanically and electrically <span class="hlt">coupled</span> segments. Each segment comprised ionic membrane <span class="hlt">currents</span>, calcium handling, and excitation-contraction <span class="hlt">coupling</span>. MEF was incorporated by locally adjusting conductivity of L-type calcium <span class="hlt">current</span> (g(CaL)) to local external work. In our set-up, g(CaL) could vary up to 25%, 50%, 100% or unlimited amount around its default value. Four consecutive simulations were performed: normal SR (with MEF), acute VP, sustained VP (with MEF), and acutely restored SR. MEF led to T-<span class="hlt">wave</span> concordance in normal SR and to discordant T-<span class="hlt">waves</span> acutely after restoring SR. Simulated ECGs with a maximum of 25-50% adaptation closely resembled those during T-<span class="hlt">wave</span> memory experiments in vivo and also provided the best compromise between optimal systolic and diastolic function. In conclusion, these simulation results indicate that slow acting MEF in the LV can explain a) the relatively small differences in systolic shortening and mechanical work during SR, b) the small dispersion in repolarization time, c) the concordant T-<span class="hlt">wave</span> during SR, and d) T-<span class="hlt">wave</span> memory. The physiological distribution in electrophysiological properties, reflected by the concordant T-<span class="hlt">wave</span>, may serve to optimize cardiac pump function. Copyright © 2012 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017OcDyn..67..973Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017OcDyn..67..973Z"><span>Evolution of <span class="hlt">wave</span> and tide over vegetation region in nearshore waters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Mingliang; Zhang, Hongxing; Zhao, Kaibin; Tang, Jun; Qin, Huifa</p> <p>2017-08-01</p> <p>Coastal wetlands are an important ecosystem in nearshore regions, where complex flow characteristics occur because of the interactions among tides, <span class="hlt">waves</span>, and plants, especially in the discontinuous flow of the intertidal zone. In order to simulate the <span class="hlt">wave</span> and <span class="hlt">wave</span>-induced <span class="hlt">current</span> in coastal waters, in this study, an explicit depth-averaged hydrodynamic (HD) <span class="hlt">model</span> has been dynamically <span class="hlt">coupled</span> with a <span class="hlt">wave</span> spectral <span class="hlt">model</span> (CMS-<span class="hlt">Wave</span>) by sharing the tide and <span class="hlt">wave</span> data. The hydrodynamic <span class="hlt">model</span> is based on the finite volume method; the intercell flux is computed using the Harten-Lax-van Leer (HLL) approximate Riemann solver for computing the dry-to-wet interface; the drag force of vegetation is <span class="hlt">modeled</span> as the sink terms in the momentum equations. An empirical <span class="hlt">wave</span> energy dissipation term with plant effect has been derived from the <span class="hlt">wave</span> action balance equation to account for the resistance induced by aquatic vegetation in the CMS-<span class="hlt">Wave</span> <span class="hlt">model</span>. The results of the <span class="hlt">coupling</span> <span class="hlt">model</span> have been verified using the measured data for the case with <span class="hlt">wave</span>-tide-vegetation interactions. The results show that the <span class="hlt">wave</span> height decreases significantly along the <span class="hlt">wave</span> propagation direction in the presence of vegetation. In the rip channel system, the oblique <span class="hlt">waves</span> drive a meandering longshore <span class="hlt">current</span>; it moves from left to right past the cusps with oscillations. In the vegetated region, the <span class="hlt">wave</span> height is greatly attenuated due to the presence of vegetation, and the radiation stresses are noticeably changed as compared to the region without vegetation. Further, vegetation can affect the spatial distribution of mean velocity in a rip channel system. In the co-exiting environment of tides, <span class="hlt">waves</span>, and vegetation, the locations of <span class="hlt">wave</span> breaking and <span class="hlt">wave</span>-induced radiation stress also vary with the water level of flooding or ebb tide in wetland water, which can also affect the development and evolution of <span class="hlt">wave</span>-induced <span class="hlt">current</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18.6001G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18.6001G"><span>The effects of sea spray and atmosphere-<span class="hlt">wave</span> <span class="hlt">coupling</span> on air-sea exchange during a tropical cyclone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Garg, Nikhil; Kwee Ng, Eddie Yin; Narasimalu, Srikanth</p> <p>2018-04-01</p> <p>The study investigates the role of the air-sea interface using numerical simulations of Hurricane Arthur (2014) in the Atlantic. More specifically, the present study aims to discern the role ocean surface <span class="hlt">waves</span> and sea spray play in modulating the intensity and structure of a tropical cyclone (TC). To investigate the effects of ocean surface <span class="hlt">waves</span> and sea spray, numerical simulations were carried out using a <span class="hlt">coupled</span> atmosphere-<span class="hlt">wave</span> <span class="hlt">model</span>, whereby a sea spray microphysical <span class="hlt">model</span> was incorporated within the <span class="hlt">coupled</span> <span class="hlt">model</span>. Furthermore, this study also explores how sea spray generation can be <span class="hlt">modelled</span> using <span class="hlt">wave</span> energy dissipation due to whitecaps; whitecaps are considered as the primary mode of spray droplets generation at hurricane intensity wind speeds. Three different numerical simulations including the sea- state-dependent momentum flux, the sea-spray-mediated heat flux, and a combination of the former two processes with the sea-spray-mediated momentum flux were conducted. The foregoing numerical simulations were evaluated against the National Data Buoy Center (NDBC) buoy and satellite altimeter measurements as well as a control simulation using an uncoupled atmosphere <span class="hlt">model</span>. The results indicate that the <span class="hlt">model</span> simulations were able to capture the storm track and intensity: the surface <span class="hlt">wave</span> <span class="hlt">coupling</span> results in a stronger TC. Moreover, it is also noted that when only spray-mediated heat fluxes are applied in conjunction with the sea-state-dependent momentum flux, they result in a slightly weaker TC, albeit stronger compared to the control simulation. However, when a spray-mediated momentum flux is applied together with spray heat fluxes, it results in a comparably stronger TC. The results presented here allude to the role surface friction plays in the intensification of a TC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999APS..DFD..FC02G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999APS..DFD..FC02G"><span><span class="hlt">Models</span> for short-<span class="hlt">wave</span> instability in inviscid shear flows</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grimshaw, Roger</p> <p>1999-11-01</p> <p>The generation of instability in an invsicid fluid occurs by a resonance between two <span class="hlt">wave</span> modes, where here the resonance occurs by a coincidence of phase speeds for a finite, non-zero wavenumber. We show that in the weakly nonlinear limit, the appropriate <span class="hlt">model</span> consists of two <span class="hlt">coupled</span> equations for the envelopes of the <span class="hlt">wave</span> modes, in which the nonlinear terms are balanced with low-order cross-<span class="hlt">coupling</span> linear dispersive terms rather than the more familiar high-order terms which arise in the nonlinear Schrodinger equation, for instance. We will show that this system may either contain gap solitons as solutions in the linearly stable case, or <span class="hlt">wave</span> breakdown in the linearly unstable case. In this latter circumstance, the system either exhibits <span class="hlt">wave</span> collapse in finite time, or disintegration into fine-scale structures.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28341995','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28341995"><span>Performance of <span class="hlt">wave</span> function and density functional methods for water hydrogen bond spin-spin <span class="hlt">coupling</span> constants.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>García de la Vega, J M; Omar, S; San Fabián, J</p> <p>2017-04-01</p> <p>Spin-spin <span class="hlt">coupling</span> constants in water monomer and dimer have been calculated using several <span class="hlt">wave</span> function and density functional-based methods. CCSD, MCSCF, and SOPPA <span class="hlt">wave</span> functions methods yield similar results, specially when an additive approach is used with the MCSCF. Several functionals have been used to analyze their performance with the Jacob's ladder and a set of functionals with different HF exchange were tested. Functionals with large HF exchange appropriately predict 1 J O H , 2 J H H and 2h J O O <span class="hlt">couplings</span>, while 1h J O H is better calculated with functionals that include a reduced fraction of HF exchange. Accurate functionals for 1 J O H and 2 J H H have been tested in a tetramer water <span class="hlt">model</span>. The hydrogen bond effects on these intramolecular <span class="hlt">couplings</span> are additive when they are calculated by SOPPA(CCSD) <span class="hlt">wave</span> function and DFT methods. Graphical Abstract Evaluation of the additive effect of the hydrogen bond on spin-spin <span class="hlt">coupling</span> constants of water using WF and DFT methods.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017OcDyn..67.1461C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017OcDyn..67.1461C"><span>Extreme bottom velocities induced by wind <span class="hlt">wave</span> and <span class="hlt">currents</span> in the Gulf of Gdańsk</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cieślikiewicz, Witold; Dudkowska, Aleksandra; Gic-Grusza, Gabriela; Jędrasik, Jan</p> <p>2017-11-01</p> <p>The principal goal of this study is to get some preliminary insights about the intensity of water movement generated by wind <span class="hlt">waves</span>, and due to the <span class="hlt">currents</span> in the bottom waters of Gulf of Gdańsk, during severe storms. The Gulf of Gdańsk is located in the southern Baltic Sea. This paper presents the results of analysis of <span class="hlt">wave</span> and <span class="hlt">current</span>-induced velocities during extreme wind conditions, which are determined based on long-term historical records. The bottom velocity fields originated from wind <span class="hlt">wave</span> and wind <span class="hlt">currents</span>, during analysed extreme wind events, are computed independently of each other. The long-term wind <span class="hlt">wave</span> parameters for the Baltic Sea region are derived from the 44-year hindcast <span class="hlt">wave</span> database generated in the framework of the project HIPOCAS funded by the European Union. The output from the numerical <span class="hlt">wave</span> <span class="hlt">model</span> WAM provides the boundary conditions for the <span class="hlt">model</span> SWAN operating in high-resolution grid covering the area of the Gulf of Gdańsk. Wind <span class="hlt">current</span> velocities are calculated with the M3D hydrodynamic <span class="hlt">model</span> developed in the Institute of Oceanography of the University of Gdańsk based on the POM <span class="hlt">model</span>. The three dimensional <span class="hlt">current</span> fields together with trajectories of particle tracers spreading out of bottom boundary layer are <span class="hlt">modelled</span>, and the calculated fields of bottom velocities are presented in the form of 2D maps. During northerly winds, causing in the Gulf of Gdańsk extreme <span class="hlt">waves</span> and most significant wind-driven circulation, the <span class="hlt">wave</span>-induced bottom velocities are greater than velocities due to <span class="hlt">currents</span>. The <span class="hlt">current</span> velocities in the bottom layer appeared to be smaller by an order of magnitude than the <span class="hlt">wave</span>-induced bottom orbital velocities. Namely, during most severe northerly storms analysed, <span class="hlt">current</span> bottom velocities ranged about 0.1-0.15 m/s, while the root mean square of <span class="hlt">wave</span>-induced near-seabed velocities reached maximum values of up to 1.4 m/s in the southern part of Gulf of Gdańsk.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMOS23B1384S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMOS23B1384S"><span>Hindcasting of Storm Surges, <span class="hlt">Currents</span>, and <span class="hlt">Waves</span> at Lower Delaware Bay during Hurricane Isabel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Salehi, M.</p> <p>2017-12-01</p> <p>Hurricanes are a major threat to coastal communities and infrastructures including nuclear power plants located in low-lying coastal zones. In response, their sensitive elements should be protected by smart design to withstand against drastic impact of such natural phenomena. Accurate and reliable estimate of hurricane attributes is the first step to that effort. Numerical <span class="hlt">models</span> have extensively grown over the past few years and are effective tools in <span class="hlt">modeling</span> large scale natural events such as hurricane. The impact of low probability hurricanes on the lower Delaware Bay is investigated using dynamically <span class="hlt">coupled</span> meteorological, hydrodynamic, and <span class="hlt">wave</span> components of Delft3D software. Efforts are made to significantly reduce the computational overburden of performing such analysis for the industry, yet keeping the same level of accuracy at the area of study (AOS). The <span class="hlt">model</span> is comprised of overall and nested domains. The overall <span class="hlt">model</span> domain includes portion of Atlantic Ocean, Delaware, and Chesapeake bays. The nested <span class="hlt">model</span> domain includes Delaware Bay, its floodplain, and portion of the continental shelf. This study is portion of a larger <span class="hlt">modeling</span> effort to study the impact of low probability hurricanes on sensitive infrastructures located at the coastal zones prone to hurricane activity. The AOS is located on the east bank of Delaware Bay almost 16 miles upstream of its mouth. <span class="hlt">Model</span> generated wind speed, significant <span class="hlt">wave</span> height, water surface elevation, and <span class="hlt">current</span> are calibrated for hurricane Isabel (2003). The <span class="hlt">model</span> calibration results agreed reasonably well with field observations. Furthermore, sensitivity of surge and <span class="hlt">wave</span> responses to various hurricane parameters was tested. In line with findings from other researchers, accuracy of wind field played a major role in hindcasting the hurricane attributes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19950004077','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19950004077"><span>Ferruleless <span class="hlt">coupled</span>-cavity traveling-<span class="hlt">wave</span> tube cold-test characteristics simulated with micro-SOS</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Schroeder, Dana L.; Wilson, Jeffrey D.</p> <p>1993-01-01</p> <p>The three-dimensional, electromagnetic circuit analysis code, Micro-SOS, can be used to reduce expensive and time consuming experimental 'cold-testing' of traveling-<span class="hlt">wave</span> tube (TWT) circuits. The frequency-phase dispersion and beam interaction impedance characteristics of a ferruleless <span class="hlt">coupled</span>-cavity traveling-<span class="hlt">wave</span> tube slow-<span class="hlt">wave</span> circuit were simulated using the code. Computer results agree closely with experimental data. Variations in the cavity geometry dimensions of period length and gap-to-period ratio were <span class="hlt">modeled</span>. These variations can be used in velocity taper designs to reduce the radiofrequency (RF) phase velocity in synchronism with the decelerating electron beam. Such circuit designs can result in enhanced TWT power and efficiency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1325647','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1325647"><span>A new ionospheric electron precipitation module <span class="hlt">coupled</span> with RAM-SCB within the geospace general circulation <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>Yu, Yiqun; Jordanova, Vania K.; Ridley, Aaron J.</p> <p></p> <p>Electron precipitation down to the atmosphere due to <span class="hlt">wave</span>-particle scattering in the magnetosphere contributes significantly to the auroral ionospheric conductivity. In order to obtain the auroral conductivity in global MHD <span class="hlt">models</span> that are incapable of capturing kinetic physics in the magnetosphere, MHD parameters are often used to estimate electron precipitation flux for the conductivity calculation. Such an MHD approach, however, lacks self-consistency in representing the magnetosphere-ionosphere <span class="hlt">coupling</span> processes. In this study we improve the <span class="hlt">coupling</span> processes in global <span class="hlt">models</span> with a more physical method. We calculate the physics-based electron precipitation from the ring <span class="hlt">current</span> and map it to the ionosphericmore » altitude for solving the ionospheric electrodynamics. In particular, we use the BATS-R-US (Block Adaptive Tree Scheme-Roe type-Upstream) MHD <span class="hlt">model</span> <span class="hlt">coupled</span> with the kinetic ring <span class="hlt">current</span> <span class="hlt">model</span> RAM-SCB (Ring <span class="hlt">current</span>-Atmosphere interaction <span class="hlt">Model</span> with Self-Consistent Magnetic field (B)) that solves pitch angle-dependent electron distribution functions, to study the global circulation dynamics during the 25–26 January 2013 storm event. Since the electron precipitation loss is mostly governed by <span class="hlt">wave</span>-particle resonant scattering in the magnetosphere, we further investigate two loss methods of specifying electron precipitation loss associated with <span class="hlt">wave</span>-particle interactions: (1) using pitch angle diffusion coefficients D αα(E,α) determined from the quasi-linear theory, with <span class="hlt">wave</span> spectral and plasma density obtained from statistical observations (named as “diffusion coefficient method”) and (2) using electron lifetimes τ(E) independent on pitch angles inferred from the above diffusion coefficients (named as “lifetime method”). We found that both loss methods demonstrate similar temporal evolution of the trapped ring <span class="hlt">current</span> electrons, indicating that the impact of using different kinds of loss rates is small on the trapped electron population</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1325647-new-ionospheric-electron-precipitation-module-coupled-ram-scb-within-geospace-general-circulation-model','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1325647-new-ionospheric-electron-precipitation-module-coupled-ram-scb-within-geospace-general-circulation-model"><span>A new ionospheric electron precipitation module <span class="hlt">coupled</span> with RAM-SCB within the geospace general circulation <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Yu, Yiqun; Jordanova, Vania K.; Ridley, Aaron J.; ...</p> <p>2016-09-01</p> <p>Electron precipitation down to the atmosphere due to <span class="hlt">wave</span>-particle scattering in the magnetosphere contributes significantly to the auroral ionospheric conductivity. In order to obtain the auroral conductivity in global MHD <span class="hlt">models</span> that are incapable of capturing kinetic physics in the magnetosphere, MHD parameters are often used to estimate electron precipitation flux for the conductivity calculation. Such an MHD approach, however, lacks self-consistency in representing the magnetosphere-ionosphere <span class="hlt">coupling</span> processes. In this study we improve the <span class="hlt">coupling</span> processes in global <span class="hlt">models</span> with a more physical method. We calculate the physics-based electron precipitation from the ring <span class="hlt">current</span> and map it to the ionosphericmore » altitude for solving the ionospheric electrodynamics. In particular, we use the BATS-R-US (Block Adaptive Tree Scheme-Roe type-Upstream) MHD <span class="hlt">model</span> <span class="hlt">coupled</span> with the kinetic ring <span class="hlt">current</span> <span class="hlt">model</span> RAM-SCB (Ring <span class="hlt">current</span>-Atmosphere interaction <span class="hlt">Model</span> with Self-Consistent Magnetic field (B)) that solves pitch angle-dependent electron distribution functions, to study the global circulation dynamics during the 25–26 January 2013 storm event. Since the electron precipitation loss is mostly governed by <span class="hlt">wave</span>-particle resonant scattering in the magnetosphere, we further investigate two loss methods of specifying electron precipitation loss associated with <span class="hlt">wave</span>-particle interactions: (1) using pitch angle diffusion coefficients D αα(E,α) determined from the quasi-linear theory, with <span class="hlt">wave</span> spectral and plasma density obtained from statistical observations (named as “diffusion coefficient method”) and (2) using electron lifetimes τ(E) independent on pitch angles inferred from the above diffusion coefficients (named as “lifetime method”). We found that both loss methods demonstrate similar temporal evolution of the trapped ring <span class="hlt">current</span> electrons, indicating that the impact of using different kinds of loss rates is small on the trapped electron population</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19760008878','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19760008878"><span><span class="hlt">Models</span> of Jovian decametric radiation. [astronomical <span class="hlt">models</span> of decametric <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Smith, R. A.</p> <p>1975-01-01</p> <p>A critical review is presented of theoretical <span class="hlt">models</span> of Jovian decametric radiation, with particular emphasis on the Io-modulated emission. The problem is divided into three broad aspects: (1) the mechanism <span class="hlt">coupling</span> Io's orbital motion to the inner exosphere, (2) the consequent instability mechanism by which electromagnetic <span class="hlt">waves</span> are amplified, and (3) the subsequent propagation of the <span class="hlt">waves</span> in the source region and the Jovian plasmasphere. At present there exists no comprehensive theory that treats all of these aspects quantitatively within a single framework. Acceleration of particles by plasma sheaths near Io is proposed as an explanation for the <span class="hlt">coupling</span> mechanism, while most of the properties of the emission may be explained in the context of cyclotron instability of a highly anisotropic distribution of streaming particles.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018WRCM...28...15G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018WRCM...28...15G"><span>Lamb <span class="hlt">wave</span> extraction of dispersion curves in micro/nano-plates using <span class="hlt">couple</span> stress theories</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ghodrati, Behnam; Yaghootian, Amin; Ghanbar Zadeh, Afshin; Mohammad-Sedighi, Hamid</p> <p>2018-01-01</p> <p>In this paper, Lamb <span class="hlt">wave</span> propagation in a homogeneous and isotropic non-classical micro/nano-plates is investigated. To consider the effect of material microstructure on the <span class="hlt">wave</span> propagation, three size-dependent <span class="hlt">models</span> namely indeterminate-, modified- and consistent <span class="hlt">couple</span> stress theories are used to extract the dispersion equations. In the mentioned theories, a parameter called 'characteristic length' is used to consider the size of material microstructure in the governing equations. To generalize the parametric studies and examine the effect of thickness, propagation wavelength, and characteristic length on the behavior of miniature plate structures, the governing equations are nondimensionalized by defining appropriate dimensionless parameters. Then the dispersion curves for phase and group velocities are plotted in terms of a wide frequency-thickness range to study the lamb <span class="hlt">waves</span> propagation considering microstructure effects in very high frequencies. According to the illustrated results, it was observed that the <span class="hlt">couple</span> stress theories in the Cosserat type material predict more rigidity than the classical theory; so that in a plate with constant thickness, by increasing the thickness to characteristic length ratio, the results approach to the classical theory, and by reducing this ratio, <span class="hlt">wave</span> propagation speed in the plate is significantly increased. In addition, it is demonstrated that for high-frequency Lamb <span class="hlt">waves</span>, it converges to dispersive Rayleigh <span class="hlt">wave</span> velocity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25920829','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25920829"><span><span class="hlt">Coupling</span> of transverse and longitudinal <span class="hlt">waves</span> in piano strings.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Etchenique, Nikki; Collin, Samantha R; Moore, Thomas R</p> <p>2015-04-01</p> <p>The existence of longitudinal <span class="hlt">waves</span> in vibrating piano strings has been previously established, as has their importance in producing the characteristic sound of the piano. <span class="hlt">Modeling</span> of the <span class="hlt">coupling</span> between the transverse and longitudinal motion of strings indicates that the amplitude of the longitudinal <span class="hlt">waves</span> are quadratically related to the transverse displacement of the string, however, experimental verification of this relationship is lacking. In the work reported here this relationship is tested by driving the transverse motion of a piano string at only two frequencies, which simplifies the task of unambiguously identifying the constituent signals. The results indicate that the generally accepted relationship between the transverse motion and the longitudinal motion is valid. It is further shown that this dependence on transverse displacement is a good approximation when a string is excited by the impact of the hammer during normal play.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A14C..03J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A14C..03J"><span>Air-Sea Interaction in the Somali <span class="hlt">Current</span> Region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jensen, T. G.; Rydbeck, A.</p> <p>2017-12-01</p> <p>The western Indian Ocean is an area of high eddy-kinetic energy generated by local wind-stress curl, instability of boundary <span class="hlt">currents</span> as well as Rossby <span class="hlt">waves</span> from the west coast of India and the equatorial <span class="hlt">wave</span> guide as they reflect off the African coast. The presence of meso-scale eddies and coastal upwelling during the Southwest Monsoon affects the air-sea interaction on those scales. The U.S. Navy's <span class="hlt">Coupled</span> Ocean-Atmosphere Mesoscale Prediction System (COAMPS) is used to understand and quantify the surface flux, effects on surface <span class="hlt">waves</span> and the role of Sea Surface Temperature anomalies on ocean-atmosphere <span class="hlt">coupling</span> in that area. The COAMPS atmosphere <span class="hlt">model</span> component with 9 km resolution is fully <span class="hlt">coupled</span> to the Navy Coastal Ocean <span class="hlt">Model</span> (NCOM) with 3.5 km resolution and the Simulating <span class="hlt">WAves</span> Nearshore (SWAN) <span class="hlt">wave</span> <span class="hlt">model</span> with 10 km resolution. Data assimilation using a 3D-variational approach is included in hindcast runs performed daily since June 1, 2015. An interesting result is that a westward jet associated with downwelling equatorial Rossy <span class="hlt">waves</span> initiated the reversal from the southward Somali <span class="hlt">Current</span> found during the northeast monsoon to a northward flow in March 2016 more than a month before the beginning of the southwest monsoon. It is also found that warm SST anomalies in the Somali <span class="hlt">Current</span> eddies, locally increase surface wind speed due to an increase in the atmospheric boundary layer height. This results in an increase in significant <span class="hlt">wave</span> height and also an increase in heat flux to the atmosphere. Cold SST anomalies over upwelling filaments have the opposite impacts on air-sea fluxes.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvB..93k5144D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvB..93k5144D"><span>Coexistence of ΘI I-loop-<span class="hlt">current</span> order with checkerboard d -<span class="hlt">wave</span> CDW/PDW order in a hot-spot <span class="hlt">model</span> for cuprate superconductors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Carvalho, Vanuildo S.; Pépin, Catherine; Freire, Hermann</p> <p>2016-03-01</p> <p>We investigate the strong influence of the ΘI I-loop-<span class="hlt">current</span> order on both unidirectional and bidirectional d -<span class="hlt">wave</span> charge-density-<span class="hlt">wave/pair-density-wave</span> (CDW/PDW) composite orders along axial momenta (±Q0,0 ) and (0 ,±Q0) that emerge in an effective hot-spot <span class="hlt">model</span> departing from the three-band Emery <span class="hlt">model</span> relevant to the phenomenology of the cuprate superconductors. This study is motivated by the compelling evidence that the ΘI I-loop-<span class="hlt">current</span> order described by this <span class="hlt">model</span> may explain groundbreaking experiments such as spin-polarized neutron scattering performed in these materials. Here, we demonstrate, within a saddle-point approximation, that the ΘI I-loop-<span class="hlt">current</span> order clearly coexists with bidirectional (i.e., checkerboard) d -<span class="hlt">wave</span> CDW and PDW orders along axial momenta, but is visibly detrimental to the unidirectional (i.e., stripe) case. This result has potentially far-reaching implications for the physics of the cuprates and agrees well with very recent x-ray experiments on YBCO that indicate that at higher dopings the CDW order has indeed a tendency to be bidirectional.</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/2017AcMSn..33.1022W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AcMSn..33.1022W"><span>Reflection and transmission of elastic <span class="hlt">waves</span> through a <span class="hlt">couple</span>-stress elastic slab sandwiched between two half-spaces</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Changda; Chen, Xuejun; Wei, Peijun; Li, Yueqiu</p> <p>2017-12-01</p> <p>The reflection and transmission of elastic <span class="hlt">waves</span> through a <span class="hlt">couple</span>-stress elastic slab that is sandwiched between two <span class="hlt">couple</span>-stress elastic half-spaces are studied in this paper. Because of the <span class="hlt">couple</span>-stress effects, there are three types of elastic <span class="hlt">waves</span> in the <span class="hlt">couple</span>-stress elastic solid, two of which are dispersive. The interface conditions between two <span class="hlt">couple</span>-stress solids involve the surface <span class="hlt">couple</span> and rotation apart from the surface traction and displacement. The nontraditional interface conditions between the slab and two solid half-spaces are used to obtain the linear algebraic equation sets from which the amplitude ratios of reflection and transmission <span class="hlt">waves</span> to the incident <span class="hlt">wave</span> can be determined. Then, the energy fluxes carried by the various reflection and transmission <span class="hlt">waves</span> are calculated numerically and the normal energy flux conservation is used to validate the numerical results. The special case, <span class="hlt">couple</span>-stress elastic slab sandwiched by the classical elastic half-spaces, is also studied and compared with the situation that the classical elastic slab sandwiched by the classical elastic half-spaces. Incident longitudinal <span class="hlt">wave</span> (P <span class="hlt">wave</span>) and incident transverse <span class="hlt">wave</span> (SV <span class="hlt">wave</span>) are both considered. The influences of the <span class="hlt">couple</span>-stress are mainly discussed based on the numerical results. It is found that the <span class="hlt">couple</span>-stress mainly influences the transverse modes of elastic <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123..326P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123..326P"><span>Diagnosing the Role of Alfvén <span class="hlt">Waves</span> in Magnetosphere-Ionosphere <span class="hlt">Coupling</span>: Swarm Observations of Large Amplitude Nonstationary Magnetic Perturbations During an Interval of Northward IMF</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pakhotin, I. P.; Mann, I. R.; Lysak, R. L.; Knudsen, D. J.; Gjerloev, J. W.; Rae, I. J.; Forsyth, C.; Murphy, K. R.; Miles, D. M.; Ozeke, L. G.; Balasis, G.</p> <p>2018-01-01</p> <p>High-resolution multispacecraft Swarm data are used to examine magnetosphere-ionosphere <span class="hlt">coupling</span> during a period of northward interplanetary magnetic field (IMF) on 31 May 2014. The observations reveal a prevalence of unexpectedly large amplitude (>100 nT) and time-varying magnetic perturbations during the polar passes, with especially large amplitude magnetic perturbations being associated with large-scale downward field-aligned <span class="hlt">currents</span>. Differences between the magnetic field measurements sampled at 50 Hz from Swarm A and C, approximately 10 s apart along track, and the correspondence between the observed electric and magnetic fields at 16 samples per second, provide significant evidence for an important role for Alfvén <span class="hlt">waves</span> in magnetosphere-ionosphere <span class="hlt">coupling</span> even during northward IMF conditions. Spectral comparison between the <span class="hlt">wave</span> <fi>E</fi>- and <fi>B</fi>-fields reveals a frequency-dependent phase difference and amplitude ratio consistent with interference between incident and reflected Alfvén <span class="hlt">waves</span>. At low frequencies, the <fi>E</fi>/<fi>B</fi> ratio is in phase with an amplitude determined by the Pedersen conductance. At higher frequencies, the amplitude and phase change as a function of frequency in good agreement with an ionospheric Alfvén resonator <span class="hlt">model</span> including Pedersen conductance effects. Indeed, within this Alfvén <span class="hlt">wave</span> incidence, reflection, and interference paradigm, even quasi-static field-aligned <span class="hlt">currents</span> might be reasonably interpreted as very low frequency (<fi>ω</fi> → 0) Alfvén <span class="hlt">waves</span>. Overall, our results not only indicate the importance of Alfvén <span class="hlt">waves</span> for magnetosphere-ionosphere <span class="hlt">coupling</span> but also demonstrate a method for using Swarm data for the innovative experimental diagnosis of Pedersen conductance from low-Earth orbit satellite measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70137854','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70137854"><span>Effect of <span class="hlt">wave-current</span> interaction on wind-driven circulation in narrow, shallow embayments</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Signell, Richard P.; Beardsley, Robert C.; Graber, H. C.; Capotondi, A.</p> <p>1990-01-01</p> <p>The effect of wind <span class="hlt">waves</span> on the steady wind-driven circulation in a narrow, shallow bay is investigated with a two-dimensional (y, z) circulation <span class="hlt">model</span> and the Grant and Madsen [1979] bottom-boundary layer <span class="hlt">model</span>, which includes <span class="hlt">wave-current</span> interaction. A constant wind stress is applied in the along-channel x direction to a channel with a constant cross-sectional profile h(y). The wind-induced flushing of shallow bays is shown to be sensitive to both the shape of the cross section and the effects of surface <span class="hlt">waves</span>. The flushing increases with increasing , where h′ is the standard deviation of cross-channel depth and  is the mean depth. This is consistent with the findings of Hearn et al. [1987]. The flushing decreases, however, with the inclusion of surface <span class="hlt">wave</span> effects which act to increase the bottom drag felt by the <span class="hlt">currents</span>. Increasing effective bottom friction reduces the strength of the circulation, while the along-bay surface slope, bottom stress and the structure of <span class="hlt">current</span> profiles remain nearly unchanged. An implication of the circulation dependence on <span class="hlt">wave-current</span> interaction is that low-frequency oscillatory winds may drive a mean circulation when the <span class="hlt">wave</span> field changes with wind direction.x</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAP...123l3904A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAP...123l3904A"><span>Pure spin <span class="hlt">current</span> manipulation in antiferromagnetically exchange <span class="hlt">coupled</span> heterostructures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Avilés-Félix, L.; Butera, A.; González-Chávez, D. E.; Sommer, R. L.; Gómez, J. E.</p> <p>2018-03-01</p> <p>We present a <span class="hlt">model</span> to describe the spin <span class="hlt">currents</span> generated by ferromagnet/spacer/ferromagnet exchange <span class="hlt">coupled</span> trilayer systems and heavy metal layers with strong spin-orbit <span class="hlt">coupling</span>. By exploiting the magnitude of the exchange <span class="hlt">coupling</span> (oscillatory RKKY-like <span class="hlt">coupling</span>) and the spin-flop transition in the magnetization process, it has been possible to produce spin <span class="hlt">currents</span> polarized in arbitrary directions. The spin-flop transition of the trilayer system originates pure spin <span class="hlt">currents</span> whose polarization vector depends on the exchange field and the magnetization equilibrium angles. We also discuss a protocol to control the polarization sign of the pure spin <span class="hlt">current</span> injected into the metallic layer by changing the initial conditions of magnetization of the ferromagnetic layers previously to the spin pumping and inverse spin Hall effect experiments. The small differences in the ferromagnetic layers lead to a change in the magnetization vector rotation that permits the control of the sign of the induced voltage components due to the inverse spin Hall effect. Our results can lead to important advances in hybrid spintronic devices with new functionalities, particularly, the ability to control microscopic parameters such as the polarization direction and the sign of the pure spin <span class="hlt">current</span> through the variation of macroscopic parameters, such as the external magnetic field or the thickness of the spacer in antiferromagnetic exchange <span class="hlt">coupled</span> systems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018EPJC...78..303B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018EPJC...78..303B"><span>Gravitational <span class="hlt">waves</span> in theories with a non-minimal curvature-matter <span class="hlt">coupling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bertolami, Orfeu; Gomes, Cláudio; Lobo, Francisco S. N.</p> <p>2018-04-01</p> <p>Gravitational <span class="hlt">waves</span> in the presence of a non-minimal curvature-matter <span class="hlt">coupling</span> are analysed, both in the Newman-Penrose and perturbation theory formalisms. Considering a cosmological constant as a source, the non-minimally <span class="hlt">coupled</span> matter-curvature <span class="hlt">model</span> reduces to f( R) theories. This is in good agreement with the most recent data. Furthermore, a dark energy-like fluid is briefly considered, where the propagation equation for the tensor modes differs from the previous scenario, in that the scalar mode equation has an extra term, which can be interpreted as the longitudinal mode being the result of the mixture of two fundamental excitations δ R and δ ρ.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhPl...24b2122H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhPl...24b2122H"><span>A statistical <span class="hlt">model</span> of the <span class="hlt">wave</span> field in a bounded domain</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hellsten, T.</p> <p>2017-02-01</p> <p>Numerical simulations of plasma heating with radiofrequency <span class="hlt">waves</span> often require repetitive calculations of <span class="hlt">wave</span> fields as the plasma evolves. To enable effective simulations, bench marked formulas of the power deposition have been developed. Here, a statistical <span class="hlt">model</span> applicable to <span class="hlt">waves</span> with short wavelengths is presented, which gives the expected amplitude of the <span class="hlt">wave</span> field as a superposition of four <span class="hlt">wave</span> fields with weight coefficients depending on the single pass damping, as. The weight coefficient for the <span class="hlt">wave</span> field coherent with that calculated in the absence of reflection agrees with the coefficient for strong single pass damping of an earlier developed heuristic <span class="hlt">model</span>, for which the weight coefficients were obtained empirically using a full <span class="hlt">wave</span> code to calculate the <span class="hlt">wave</span> field and power deposition. Antennas launching electromagnetic <span class="hlt">waves</span> into bounded domains are often designed to produce localised <span class="hlt">wave</span> fields and power depositions in the limit of strong single pass damping. The reflection of the <span class="hlt">waves</span> changes the <span class="hlt">coupling</span> that partly destroys the localisation of the <span class="hlt">wave</span> field, which explains the apparent paradox arising from the earlier developed heuristic formula that only a fraction as2(2-as) and not as of the power is absorbed with a profile corresponding to the power deposition for the first pass of the rays. A method to account for the change in the <span class="hlt">coupling</span> spectrum caused by reflection for <span class="hlt">modelling</span> the <span class="hlt">wave</span> field with ray tracing in bounded media is proposed, which should be applicable to <span class="hlt">wave</span> propagation in non-uniform media in more general geometries.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPSJ...87d3702S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPSJ...87d3702S"><span>Spin <span class="hlt">Wave</span> Theory in Two-Dimensional <span class="hlt">Coupled</span> Antiferromagnets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shimahara, Hiroshi</p> <p>2018-04-01</p> <p>We apply spin <span class="hlt">wave</span> theory to two-dimensional <span class="hlt">coupled</span> antiferromagnets. In particular, we primarily examine a system that consists of small spins <span class="hlt">coupled</span> by a strong exchange interaction J1, large spins <span class="hlt">coupled</span> by a weak exchange interaction J2, and an anisotropic exchange interaction J12 between the small and large spins. This system is an effective <span class="hlt">model</span> of the organic antiferromagnet λ-(BETS)2FeCl4 in its insulating phase, in which intriguing magnetic phenomena have been observed, where the small and large spins correspond to π electrons and 3d spins, respectively. BETS stands for bis(ethylenedithio)tetraselenafulvalene. We obtain the antiferromagnetic transition temperature TN and the sublattice magnetizations m(T) and M(T) of the small and large spins, respectively, as functions of the temperature T. When T increases, m(T) is constant with a slight decrease below TN, even where M(T) decreases significantly. When J1 ≫ J12 and J2 = 0, an analytical expression for TN is derived. The estimated value of TN and the behaviors of m(T) and M(T) agree with the observations of λ-(BETS)2FeCl4.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19880062502&hterms=fashion+models&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfashion%2Bmodels','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19880062502&hterms=fashion+models&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfashion%2Bmodels"><span>Rossby <span class="hlt">wave</span> activity in a two-dimensional <span class="hlt">model</span> - Closure for <span class="hlt">wave</span> driving and meridional eddy diffusivity</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Hitchman, Matthew H.; Brasseur, Guy</p> <p>1988-01-01</p> <p>A parameterization of the effects of Rossby <span class="hlt">waves</span> in the middle atmosphere is proposed for use in two-dimensional <span class="hlt">models</span>. By adding an equation for conservation of Rossby <span class="hlt">wave</span> activity, closure is obtained for the meridional eddy fluxes and body force due to Rossby <span class="hlt">waves</span>. Rossby <span class="hlt">wave</span> activity is produced in a climatological fashion at the tropopause, is advected by a group velocity which is determined solely by <span class="hlt">model</span> zonal winds, and is absorbed where it converges. Absorption of Rossby <span class="hlt">wave</span> activity causes both an easterly torque and an irreversible mixing of potential vorticity, represented by the meridional eddy diffusivity, K(yy). The distribution of Rossby <span class="hlt">wave</span> driving determines the distribution of K(yy), which is applied to all of the chemical constituents. This provides a self-consistent <span class="hlt">coupling</span> of the <span class="hlt">wave</span> activity with the winds, tracer distributions and the radiative field. Typical winter stratospheric values for K(yy) of 2 million sq m/sec are obtained. Poleward tracer advection is enhanced and meridional tracer gradients are reduced where Rossby <span class="hlt">wave</span> activity is absorbed in the <span class="hlt">model</span>.</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 evolution <span class="hlt">models</span> to <span class="hlt">coupled</span> 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 Evolution <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, <span class="hlt">current</span> <span class="hlt">models</span> are not capable of simulating the dynamic interactions between these systems and their co-evolution at the meso-scale. Through a novel <span class="hlt">coupling</span> of numerical <span class="hlt">models</span>, this research is designed to explore <span class="hlt">coupled</span> 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 <span class="hlt">coupling</span> of the one-line Coastline Evolution <span class="hlt">Model</span> (CEM) with the hydrodynamic LEM CAESAR-Lisflood (C-L). The major issues faced with <span class="hlt">coupling</span> 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 <span class="hlt">wave</span> 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 evolution 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 <span class="hlt">currently</span> being completed to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009PhRvB..80a4512S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009PhRvB..80a4512S"><span>Effect of interjunction <span class="hlt">coupling</span> on superconducting <span class="hlt">current</span> and charge correlations in intrinsic Josephson junctions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shukrinov, Yu. M.; Hamdipour, M.; Kolahchi, M. R.</p> <p>2009-07-01</p> <p>Charge formations on superconducting layers and creation of the longitudinal plasma <span class="hlt">wave</span> in the stack of intrinsic Josephson junctions change crucially the superconducting <span class="hlt">current</span> through the stack. Investigation of the correlations of superconducting <span class="hlt">currents</span> in neighboring Josephson junctions and the charge correlations in neighboring superconducting layers allows us to predict the additional features in the <span class="hlt">current</span>-voltage characteristics. The charge autocorrelation functions clearly demonstrate the difference between harmonic and chaotic behavior in the breakpoint region. Use of the correlation functions gives us a powerful method for the analysis of the <span class="hlt">current</span>-voltage characteristics of <span class="hlt">coupled</span> Josephson junctions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070032060','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070032060"><span>Impact of Ring <span class="hlt">Current</span> Ions on Electromagnetic Ion Cyclotron <span class="hlt">Wave</span> Dispersion Relation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Khazanov, G. V.; Gamayunov, K. V.</p> <p>2007-01-01</p> <p>Effect of the ring <span class="hlt">current</span> ions in the real part of electromagnetic ion Cyclotron <span class="hlt">wave</span> dispersion relation is studied on global scale. Recent Cluster observations by Engebretson et al. showed that although the temperature anisotropy of is energetic (> 10 keV) ring <span class="hlt">current</span> protons was high during the entire 22 November 2003 perigee pass, electromagnetic ion cyclotron <span class="hlt">waves</span> were observed only in conjunction with intensification of the ion fluxes below 1 keV by over an order of magnitude. To study the effect of the ring <span class="hlt">current</span> ions on the <span class="hlt">wave</span> dispersive properties and the corresponding global <span class="hlt">wave</span> redistribution, we use a self-consistent <span class="hlt">model</span> of interacting ring <span class="hlt">current</span> and electromagnetic ion cyclotron <span class="hlt">waves</span>, and simulate the May 1998 storm. The main findings of our simulation can be summarized as follows: First, the plasma density enhancement in the night MLT sector during the main and recovery storm phases is mostly caused by injection of suprathermal plasma sheet H + (approximately < 1 keV), which dominate the thermal plasma density. Second, during the recovery storm phases, the ring <span class="hlt">current</span> modification of the <span class="hlt">wave</span> dispersion relation leads to a qualitative change of the <span class="hlt">wave</span> patterns in the postmidnight-dawn sector for L > 4.75. This "new" <span class="hlt">wave</span> activity is well organized by outward edges of dense suprathermal ring <span class="hlt">current</span> spots, and the <span class="hlt">waves</span> are not observed if the ring <span class="hlt">current</span> ions are not included in the real part of dispersion relation. Third, the most intense <span class="hlt">wave</span>-induced ring <span class="hlt">current</span> precipitation is located in the night MLT sector and caused by modification of the <span class="hlt">wave</span> dispersion relation. The strongest precipitating fluxes of about 8 X 10(exp 6)/ (cm(exp 2) - s X st) are found near L=5.75, MLT=2 during the early recovery phase on 4 May. Finally, the nightside precipitation is more intense than the dayside fluxes, even if there are less intense <span class="hlt">waves</span>, because the convection field moves ring <span class="hlt">current</span> ions into the loss cone on the nightside, but drives</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvD..96h4023B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvD..96h4023B"><span>Nonminimal <span class="hlt">couplings</span>, gravitational <span class="hlt">waves</span>, and torsion in Horndeski's theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barrientos, José; Cordonier-Tello, Fabrizio; Izaurieta, Fernando; Medina, Perla; Narbona, Daniela; Rodríguez, Eduardo; Valdivia, Omar</p> <p>2017-10-01</p> <p>The Horndeski Lagrangian brings together all possible interactions between gravity and a scalar field that yield second-order field equations in four-dimensional spacetime. As originally proposed, it only addresses phenomenology without torsion, which is a non-Riemannian feature of geometry. Since torsion can potentially affect interesting phenomena such as gravitational <span class="hlt">waves</span> and early universe inflation, in this paper we allow torsion to exist and propagate within the Horndeski framework. To achieve this goal, we cast the Horndeski Lagrangian in Cartan's first-order formalism and introduce <span class="hlt">wave</span> operators designed to act covariantly on p -form fields that carry Lorentz indices. We find that nonminimal <span class="hlt">couplings</span> and second-order derivatives of the scalar field in the Lagrangian are indeed generic sources of torsion. Metric perturbations <span class="hlt">couple</span> to the background torsion, and new torsional modes appear. These may be detected via gravitational <span class="hlt">waves</span> but not through Yang-Mills gauge bosons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMOS23A1979F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMOS23A1979F"><span>Numerical <span class="hlt">Modeling</span> of Infragravity <span class="hlt">Wave</span> Runup on Steep and Mildly Sloping Natural Beaches</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fiedler, J. W.; Smit, P.; Brodie, K. L.; McNinch, J.; Guza, R. T.; Gallien, T.</p> <p>2016-12-01</p> <p>We present ongoing work which aims to validate the non-hydrostatic <span class="hlt">model</span> SWASH for <span class="hlt">wave</span> runup and infragravity <span class="hlt">waves</span> generated by a range of different incident <span class="hlt">wave</span> spectra at the offshore boundary, including the effect of finite directional spread. Flume studies of <span class="hlt">wave</span> runup are limited to normally incident (1D) sea and infragravity <span class="hlt">waves</span>, but natural <span class="hlt">waves</span> are directionally spread (2D), with substantially different dynamics from 1D. For example, refractive trapping (edge <span class="hlt">waves</span>) is only possible with 2D <span class="hlt">waves</span>, and the bound infragravity <span class="hlt">wave</span> response to short <span class="hlt">wave</span> groups is highly amplified for the special case of normal incidence. Selected case studies are <span class="hlt">modeled</span> at Agate Beach, Oregon, a low slope (1:80) beach with maximum offshore <span class="hlt">wave</span> heights greater than 7m, and Cardiff, California, a steep (1:8) beach with maximum <span class="hlt">wave</span> heights of 2m. Peak periods ranged between 5-20 s at both sites. On both beaches, <span class="hlt">waves</span> were measured on a transect from approximately 10m depth to the runup, using pressure sensors, <span class="hlt">current</span> meters, and a scanning lidar. Bulk short <span class="hlt">wave</span> quantities, <span class="hlt">wave</span> runup, infragravity frequency spectra and energy fluxes are compared with SWASH. On the low slope beach with energetic incident <span class="hlt">waves</span>, the observed horizontal runup excursions reach 140m ( 100s periods). Swash front velocities reached up to several m/s, causing short <span class="hlt">waves</span> to stack up during runup drawdown. On reversal of the infragravity phase, the stacked short <span class="hlt">waves</span> are swept onshore with the long <span class="hlt">wave</span> front, effectively enhancing runup by phase <span class="hlt">coupling</span> long and short <span class="hlt">waves</span>. Statistical variability and nonlinearity in swash generation lead to time-varying runup heights. Here, we test these observations with 2D SWASH, as well as the sensitivity of <span class="hlt">modeled</span> runup to the parameterization of bottom friction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMEP13A0822L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMEP13A0822L"><span>Comparing <span class="hlt">wave</span> shoaling methods used in large-scale coastal evolution <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>Limber, P. W.; Adams, P. N.; Murray, A.</p> <p>2013-12-01</p> <p> output where <span class="hlt">wave</span> height is approximately one-half of the water depth (a standard <span class="hlt">wave</span> breaking threshold). The goal of this <span class="hlt">modeling</span> exercise is to understand under what conditions a simple <span class="hlt">wave</span> <span class="hlt">model</span> is sufficient for simulating coastline evolution, and when using a more complex shoaling routine can optimize a coastline <span class="hlt">model</span>. The Coastline Evolution <span class="hlt">Model</span> (CEM; Ashton and Murray, 2006) is used to show how different shoaling routines affect <span class="hlt">modeled</span> coastline behavior. The CEM <span class="hlt">currently</span> includes the most basic <span class="hlt">wave</span> shoaling approach to simulate cape and spit formation. We will instead <span class="hlt">couple</span> it to SWAN, using the insight from the comprehensive <span class="hlt">wave</span> <span class="hlt">model</span> (above) to guide its application. This will allow <span class="hlt">waves</span> transformed over complex bathymetry, such as cape-associated shoals and ridges, to be input for the CEM so that large-scale coastline behavior can be addressed in less idealized environments. Ashton, A., and Murray, A.B., 2006, High-angle <span class="hlt">wave</span> instability and emergent shoreline shapes: 1. <span class="hlt">Modeling</span> of sand <span class="hlt">waves</span>, flying spits, and capes: Journal of Geophysical Research, v. 111, p. F04011, doi:10.1029/2005JF000422.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..DPPGI2003M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..DPPGI2003M"><span>Validation of a <span class="hlt">coupled</span> core-transport, pedestal-structure, <span class="hlt">current</span>-profile and equilibrium <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>Meneghini, O.</p> <p>2015-11-01</p> <p>The first workflow capable of predicting the self-consistent solution to the <span class="hlt">coupled</span> core-transport, pedestal structure, and equilibrium problems from first-principles and its experimental tests are presented. Validation with DIII-D discharges in high confinement regimes shows that the workflow is capable of robustly predicting the kinetic profiles from on axis to the separatrix and matching the experimental measurements to within their uncertainty, with no prior knowledge of the pedestal height nor of any measurement of the temperature or pressure. Self-consistent <span class="hlt">coupling</span> has proven to be essential to match the experimental results, and capture the non-linear physics that governs the core and pedestal solutions. In particular, clear stabilization of the pedestal peeling ballooning instabilities by the global Shafranov shift and destabilization by additional edge bootstrap <span class="hlt">current</span>, and subsequent effect on the core plasma profiles, have been clearly observed and documented. In our <span class="hlt">model</span>, self-consistency is achieved by iterating between the TGYRO core transport solver (with NEO and TGLF for neoclassical and turbulent flux), and the pedestal structure predicted by the EPED <span class="hlt">model</span>. A self-consistent equilibrium is calculated by EFIT, while the ONETWO transport package evolves the <span class="hlt">current</span> profile and calculates the particle and energy sources. The capabilities of such workflow are shown to be critical for the design of future experiments such as ITER and FNSF, which operate in a regime where the equilibrium, the pedestal, and the core transport problems are strongly <span class="hlt">coupled</span>, and for which none of these quantities can be assumed to be known. Self-consistent core-pedestal predictions for ITER, as well as initial optimizations, will be presented. Supported by the US Department of Energy under DE-FC02-04ER54698, DE-SC0012652.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005Icar..178...84G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005Icar..178...84G"><span><span class="hlt">Coupling</span> of acoustic <span class="hlt">waves</span> to clouds in the jovian troposphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gaulme, Patrick; Mosser, Benoît</p> <p>2005-11-01</p> <p>Seismology is the best tool for investigating the interior structure of stars and giant planets. This paper deals with a photometric study of jovian global oscillations. The propagation of acoustic <span class="hlt">waves</span> in the jovian troposphere is revisited in order to estimate their effects on the planetary albedo. According to the standard <span class="hlt">model</span> of the jovian cloud structure there are three major ice cloud layers (e.g., [Atreya et al., 1999. A comparison of the atmospheres of Jupiter and Saturn: Deep atmospheric composition, cloud structure, vertical mixing, and origin. Planet Space Sci. 47, 1243-1262]). We consider only the highest layers, composed of ammonia ice, in the region where acoustic <span class="hlt">waves</span> are trapped in Jupiter's atmosphere. For a vertical <span class="hlt">wave</span> propagating in a plane parallel atmosphere with an ammonia ice cloud layer, we calculate first the relative variations of the reflected solar flux due to the smooth oscillations at about the ppm level. We then determine the phase transitions induced by the seismic <span class="hlt">waves</span> in the clouds. These phase changes, linked to ice particle growth, are limited by kinetics. A Mie <span class="hlt">model</span> [Mishchenko et al., 2002. Scattering, Absorption, and Emission of Light by Small Particles. Cambridge Univ. Press, Cambridge, pp. 158-190] <span class="hlt">coupled</span> with a simple radiation transfer <span class="hlt">model</span> allows us to estimate that the albedo fluctuations of the cloud perturbed by a seismic <span class="hlt">wave</span> reach relative variations of 70 ppm for a 3-mHz <span class="hlt">wave</span>. This albedo fluctuation is amplified by a factor of ˜70 relative to the previously published estimates that exclude the effect of the <span class="hlt">wave</span> on cloud properties. Our computed amplifications imply that jovian oscillations can be detected with very precise photometry, as proposed by the microsatellite JOVIS project, which is dedicated to photometric seismology [Mosser et al., 2004. JOVIS: A microsatellite dedicated to the seismic analysis of Jupiter. In: Combes, F., Barret, D., Contini, T., Meynadier, F., Pagani, L. (Eds.), SF2A-2004</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27668142','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27668142"><span>Global MHD <span class="hlt">modeling</span> of resonant ULF <span class="hlt">waves</span>: Simulations with and without a plasmasphere.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Claudepierre, S G; Toffoletto, F R; Wiltberger, M</p> <p>2016-01-01</p> <p>We investigate the plasmaspheric influence on the resonant mode <span class="hlt">coupling</span> of magnetospheric ultralow frequency (ULF) <span class="hlt">waves</span> using the Lyon-Fedder-Mobarry (LFM) global magnetohydrodynamic (MHD) <span class="hlt">model</span>. We present results from two different versions of the <span class="hlt">model</span>, both driven by the same solar wind conditions: one version that contains a plasmasphere (the LFM <span class="hlt">coupled</span> to the Rice Convection <span class="hlt">Model</span>, where the Gallagher plasmasphere <span class="hlt">model</span> is also included) and another that does not (the stand-alone LFM). We find that the inclusion of a cold, dense plasmasphere has a significant impact on the nature of the simulated ULF <span class="hlt">waves</span>. For example, the inclusion of a plasmasphere leads to a deeper (more earthward) penetration of the compressional (azimuthal) electric field fluctuations, due to a shift in the location of the <span class="hlt">wave</span> turning points. Consequently, the locations where the compressional electric field oscillations resonantly <span class="hlt">couple</span> their energy into local toroidal mode field line resonances also shift earthward. We also find, in both simulations, that higher-frequency compressional (azimuthal) electric field oscillations penetrate deeper than lower frequency oscillations. In addition, the compressional <span class="hlt">wave</span> mode structure in the simulations is consistent with a radial standing <span class="hlt">wave</span> oscillation pattern, characteristic of a resonant waveguide. The incorporation of a plasmasphere into the LFM global MHD <span class="hlt">model</span> represents an advance in the state of the art in regard to ULF <span class="hlt">wave</span> <span class="hlt">modeling</span> with such simulations. We offer a brief discussion of the implications for radiation belt <span class="hlt">modeling</span> techniques that use the electric and magnetic field outputs from global MHD simulations to drive particle dynamics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14.6621G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14.6621G"><span>Characteristics of inertial <span class="hlt">currents</span> observed in offshore <span class="hlt">wave</span> records</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gemmrich, J.; Garrett, C.</p> <p>2012-04-01</p> <p>It is well known that ambient <span class="hlt">currents</span> can change the amplitude, direction and frequency of ocean surface <span class="hlt">waves</span>. Regions with persistent strong <span class="hlt">currents</span>, such as the Agulhas <span class="hlt">current</span> off the east coast of South Africa, are known as areas of extreme <span class="hlt">waves</span>, and <span class="hlt">wave</span> height modulations of up to 50% observed in the shallow North Sea have been linked to tidal <span class="hlt">currents</span>. In the open ocean, inertial <span class="hlt">currents</span>, while intermittent, are typically the most energetic <span class="hlt">currents</span> with speeds up to 0.5 m/s, and can interact with the surface <span class="hlt">wave</span> field to create <span class="hlt">wave</span> modulation, though this has not previously been reported. We use long records of significant <span class="hlt">wave</span> heights from buoy observations in the northeast Pacific and show evidence of significant modulation at frequencies that are slightly higher than the local inertial frequency. Quite apart from the relevance to surface <span class="hlt">waves</span>, this result can provide a consistent and independent measurement, over a wide range of latitudes, of the frequency blue-shift, the strength and intermittency of ocean surface inertial <span class="hlt">currents</span>. Near-inertial <span class="hlt">waves</span> constitute the most energetic portion of the internal <span class="hlt">wave</span> band and play a significant role in deep ocean mixing. So far, observational data on near-surface inertial <span class="hlt">currents</span> has tended to come from short records that do not permit the reliable determination of the frequency blue-shift, though this is an important factor affecting the energy flux from the surface into deeper waters. Long records from routine <span class="hlt">wave</span> height observations are widely available and could help to shed new light globally on the blue-shift and on the characteristics of inertial <span class="hlt">currents</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1814128H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1814128H"><span>On the generation of internal <span class="hlt">wave</span> modes by surface <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Harlander, Uwe; Kirschner, Ian; Maas, Christian; Zaussinger, Florian</p> <p>2016-04-01</p> <p>Internal gravity <span class="hlt">waves</span> play an important role in the ocean since they transport energy and momentum and the can lead to mixing when they break. Surface <span class="hlt">waves</span> and internal gravity <span class="hlt">waves</span> can interact. On the one hand, long internal <span class="hlt">waves</span> imply a slow varying shear <span class="hlt">current</span> that modifies the propagation of surface <span class="hlt">waves</span>. Surface <span class="hlt">waves</span> generated by the atmosphere can, on the other hand, excite internal <span class="hlt">waves</span> by nonlinear interaction. Thereby a surface <span class="hlt">wave</span> packet consisting of two close frequencies can resonate with a low frequency internal <span class="hlt">wave</span> (Phillips, 1966). From a theoretical point of view, the latter has been studied intensively by using a 2-layer <span class="hlt">model</span>, i.e. a surface layer with a strong density contrast and an internal layer with a comparable weak density contrast (Ball, 1964; Craig et al., 2010). In the present work we analyse the <span class="hlt">wave</span> <span class="hlt">coupling</span> for a continuously stratified fluid using a fully non-linear 2D numerical <span class="hlt">model</span> (OpenFoam) and compare this with laboratory experiments (see Lewis et al. 1974). Surface <span class="hlt">wave</span> modes are used as initial condition and the time development of the dominant surface and internal <span class="hlt">waves</span> are studied by spectral and harmonic analysis. For the simple geometry of a box, the results are compared with analytical spectra of surface and gravity <span class="hlt">waves</span>. Ball, F.K. 1964: Energy transfer between external and internal gravity <span class="hlt">waves</span>. J. Fluid Mech. 19, 465. Craig, W., Guyenne, P., Sulem, C. 2010: <span class="hlt">Coupling</span> between internal and surface <span class="hlt">waves</span>. Natural Hazards 57, 617-642. Lewis, J.E., Lake, B.M., Ko, D.R.S 1974: On the interaction of internal <span class="hlt">waves</span> and surfacr gravity <span class="hlt">waves</span>, J. Fluid Mech. 63, 773-800. Phillips, O.M. 1966: The dynamics of the upper ocean, Cambridge University Press, 336pp.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29670936','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29670936"><span>Submesoscale Rossby <span class="hlt">waves</span> on the Antarctic circumpolar <span class="hlt">current</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Taylor, John R; Bachman, Scott; Stamper, Megan; Hosegood, Phil; Adams, Katherine; Sallee, Jean-Baptiste; Torres, Ricardo</p> <p>2018-03-01</p> <p>The eastward-flowing Antarctic circumpolar <span class="hlt">current</span> (ACC) plays a central role in the global ocean overturning circulation and facilitates the exchange of water between the ocean surface and interior. Submesoscale eddies and fronts with scales between 1 and 10 km are regularly observed in the upper ocean and are associated with strong vertical circulations and enhanced stratification. Despite their importance in other locations, comparatively little is known about submesoscales in the Southern Ocean. We present results from new observations, <span class="hlt">models</span>, and theories showing that submesoscales are qualitatively changed by the strong jet associated with the ACC in the Scotia Sea, east of Drake Passage. Growing submesoscale disturbances develop along a dense filament and are transformed into submesoscale Rossby <span class="hlt">waves</span>, which propagate upstream relative to the eastward jet. Unlike their counterparts in slower <span class="hlt">currents</span>, the submesoscale Rossby <span class="hlt">waves</span> do not destroy the underlying frontal structure. The development of submesoscale instabilities leads to strong net subduction of water associated with a dense outcropping filament, and later, the submesoscale Rossby <span class="hlt">waves</span> are associated with intense vertical circulations.</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.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5903883','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5903883"><span>Submesoscale Rossby <span class="hlt">waves</span> on the Antarctic circumpolar <span class="hlt">current</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>Bachman, Scott; Sallee, Jean-Baptiste</p> <p>2018-01-01</p> <p>The eastward-flowing Antarctic circumpolar <span class="hlt">current</span> (ACC) plays a central role in the global ocean overturning circulation and facilitates the exchange of water between the ocean surface and interior. Submesoscale eddies and fronts with scales between 1 and 10 km are regularly observed in the upper ocean and are associated with strong vertical circulations and enhanced stratification. Despite their importance in other locations, comparatively little is known about submesoscales in the Southern Ocean. We present results from new observations, <span class="hlt">models</span>, and theories showing that submesoscales are qualitatively changed by the strong jet associated with the ACC in the Scotia Sea, east of Drake Passage. Growing submesoscale disturbances develop along a dense filament and are transformed into submesoscale Rossby <span class="hlt">waves</span>, which propagate upstream relative to the eastward jet. Unlike their counterparts in slower <span class="hlt">currents</span>, the submesoscale Rossby <span class="hlt">waves</span> do not destroy the underlying frontal structure. The development of submesoscale instabilities leads to strong net subduction of water associated with a dense outcropping filament, and later, the submesoscale Rossby <span class="hlt">waves</span> are associated with intense vertical circulations. PMID:29670936</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JETPL..95..307S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JETPL..95..307S"><span>The c-axis charge traveling <span class="hlt">wave</span> in a <span class="hlt">coupled</span> system of Josephson junctions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shukrinov, Yu. M.; Hamdipour, M.</p> <p>2012-05-01</p> <p>We demonstrate a manifestation of the charge traveling <span class="hlt">wave</span> along the c axis (TW) in <span class="hlt">current</span> voltage characteristics of <span class="hlt">coupled</span> Josephson junctions in high- T c superconductors. The branches related to the TW with different wavelengths are found for the stacks with different number of Josephson junctions at different values of system's parameters. Transitions between the TW branches and the outermost branch are observed. The electric charge in the superconducting layers and charge-charge correlation functions for TW and outermost branches show different behavior with bias <span class="hlt">current</span>. We propose an experimental testing of the TW branching by microwave irradiation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMOS11C1660L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMOS11C1660L"><span>The Influence of Surface Gravity <span class="hlt">Waves</span> on Marine <span class="hlt">Current</span> Turbine Performance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lust, E.; Luznik, L.; Flack, K. A.; Walker, J.; Van Benthem, M.</p> <p>2013-12-01</p> <p>Surface gravity <span class="hlt">waves</span> can significantly impact operating conditions for a marine <span class="hlt">current</span> turbine, imparting unsteady velocities several orders of magnitude larger than the ambient turbulence. The influence of surface <span class="hlt">waves</span> on the performance characteristics of a two-bladed horizontal axis marine <span class="hlt">current</span> turbine was investigated experimentally in a large towing tank facility at the United States Naval Academy. The turbine <span class="hlt">model</span> had a 0.8 m diameter (D) rotor with a NACA 63-618 cross section, which is Reynolds number independent with respect to lift coefficient in the operating range of Rec ≈ 4 x 105. The torque, thrust and rotational speed were measured at a range of tip speed ratios (TSR) from 5 < TSR < 11. Tests were performed at two rotor depths (1.3D and 2.25D) with and without <span class="hlt">waves</span>. The average turbine performance characteristics were largely unchanged by depth or the presence of <span class="hlt">waves</span>. However, tests with <span class="hlt">waves</span> indicate large variations in thrust, rotational speed, and torque occurred with the passage of the <span class="hlt">wave</span>. These results demonstrate the impact of surface gravity <span class="hlt">waves</span> on power production and structural loading and suggest that turbines should be positioned vertically within the water column at a depth which maximizes power output while minimizing material fatigue. Keywords-- marine <span class="hlt">current</span> turbine, tidal turbine, towing-tank experiments, surface gravity <span class="hlt">waves</span>, fatigue loading, phase averaging</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFMSA31A0361S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFMSA31A0361S"><span>Simulations of Atmospheric Neutral <span class="hlt">Wave</span> <span class="hlt">Coupling</span> to the Ionosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Siefring, C. L.; Bernhardt, P. A.</p> <p>2005-12-01</p> <p>The densities in the E- and F-layer plasmas are much less than the density of background neutral atmosphere. Atmospheric neutral <span class="hlt">waves</span> are primary sources of plasma density fluctuations and are the sources for triggering plasma instabilities. The neutral atmosphere supports acoustic <span class="hlt">waves</span>, acoustic gravity <span class="hlt">waves</span>, and Kelvin Helmholtz <span class="hlt">waves</span> from wind shears. These <span class="hlt">waves</span> help determine the structure of the ionosphere by changes in neutral density that affect ion-electron recombination and by neutral velocities that <span class="hlt">couple</span> to the plasma via ion-neutral collisions. Neutral acoustic disturbances can arise from thunderstorms, chemical factory explosions and intentional high-explosive tests. Based on conservation of energy, acoustic <span class="hlt">waves</span> grow in amplitude as they propagate upwards to lower atmospheric densities. Shock <span class="hlt">waves</span> can form in an acoustic pulse that is eventually damped by viscosity. Ionospheric effects from acoustic <span class="hlt">waves</span> include transient perturbations of E- and F-Regions and triggering of E-Region instabilities. Acoustic-gravity <span class="hlt">waves</span> affect the ionosphere over large distances. Gravity <span class="hlt">wave</span> sources include thunderstorms, auroral region disturbances, Space Shuttle launches and possibly solar eclipses. Low frequency acoustic-gravity <span class="hlt">waves</span> propagate to yield traveling ionospheric disturbances (TID's), triggering of Equatorial bubbles, and possible periodic structuring of the E-Region. Gravity <span class="hlt">wave</span> triggering of equatorial bubbles is studied numerically by solving the equations for plasma continuity and ion velocity along with Ohms law to provide an equation for the induced electric potential. Slow moving gravity <span class="hlt">waves</span> provide density depressions on bottom of ionosphere and a gravitational Rayleigh-Taylor instability is initiated. Radar scatter detects field aligned irregularities in the resulting plasma bubble. Neutral Kelvin-Helmholtz <span class="hlt">waves</span> are produced by strong mesospheric wind shears that are also coincident with the formation of intense E-layers. An</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22496191-quasi-linear-modeling-lower-hybrid-current-drive-iter-demo','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22496191-quasi-linear-modeling-lower-hybrid-current-drive-iter-demo"><span>Quasi-linear <span class="hlt">modeling</span> of lower hybrid <span class="hlt">current</span> drive in ITER and DEMO</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>Cardinali, A., E-mail: alessandro.cardinali@enea.it; Cesario, R.; Panaccione, L.</p> <p>2015-12-10</p> <p>First pass absorption of the Lower Hybrid <span class="hlt">waves</span> in thermonuclear devices like ITER and DEMO is <span class="hlt">modeled</span> by <span class="hlt">coupling</span> the ray tracing equations with the quasi-linear evolution of the electron distribution function in 2D velocity space. As usually assumed, the Lower Hybrid <span class="hlt">Current</span> Drive is not effective in a plasma of a tokamak fusion reactor, owing to the accessibility condition which, depending on the density, restricts the parallel wavenumber to values greater than n{sub ∥crit} and, at the same time, to the high electron temperature that would enhance the <span class="hlt">wave</span> absorption and then restricts the RF power deposition to themore » very periphery of the plasma column (near the separatrix). In this work, by extensively using the “ray{sup star}” code, a parametric study of the propagation and absorption of the LH <span class="hlt">wave</span> as function of the <span class="hlt">coupled</span> <span class="hlt">wave</span> spectrum (as its width, and peak value), has been performed very accurately. Such a careful investigation aims at controlling the power deposition layer possibly in the external half radius of the plasma, thus providing a valuable aid to the solution of how to control the plasma <span class="hlt">current</span> profile in a toroidal magnetic configuration, and how to help the suppression of MHD mode that can develop in the outer part of the plasma. This analysis is useful not only for exploring the possibility of profile control of a pulsed operation reactor as well as the tearing mode stabilization, but also in order to reconsider the feasibility of steady state regime for DEMO.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017QSRv..169...13D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017QSRv..169...13D"><span><span class="hlt">Current</span> state and future perspectives on <span class="hlt">coupled</span> ice-sheet - sea-level <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>de Boer, Bas; Stocchi, Paolo; Whitehouse, Pippa L.; van de Wal, Roderik S. W.</p> <p>2017-08-01</p> <p>The interaction between ice-sheet growth and retreat and sea-level change has been an established field of research for many years. However, recent advances in numerical <span class="hlt">modelling</span> have shed new light on the precise interaction of marine ice sheets with the change in near-field sea level, and the related stability of the grounding line position. Studies using fully <span class="hlt">coupled</span> ice-sheet - sea-level <span class="hlt">models</span> have shown that accounting for gravitationally self-consistent sea-level change will act to slow down the retreat and advance of marine ice-sheet grounding lines. Moreover, by simultaneously solving the 'sea-level equation' and <span class="hlt">modelling</span> ice-sheet flow, <span class="hlt">coupled</span> <span class="hlt">models</span> provide a global field of relative sea-level change that is consistent with dynamic changes in ice-sheet extent. In this paper we present an overview of recent advances, possible caveats, methodologies and challenges involved in <span class="hlt">coupled</span> ice-sheet - sea-level <span class="hlt">modelling</span>. We conclude by presenting a first-order comparison between a suite of relative sea-level data and output from a <span class="hlt">coupled</span> ice-sheet - sea-level <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRC..121.7326Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRC..121.7326Z"><span>A modulating effect of Tropical Instability <span class="hlt">Wave</span> (TIW)-induced surface wind feedback in a hybrid <span class="hlt">coupled</span> <span class="hlt">model</span> of the tropical Pacific</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Rong-Hua</p> <p>2016-10-01</p> <p>Tropical Instability <span class="hlt">Waves</span> (TIWs) and the El Niño-Southern Oscillation (ENSO) are two air-sea <span class="hlt">coupling</span> phenomena that are prominent in the tropical Pacific, occurring at vastly different space-time scales. It has been challenging to adequately represent both of these processes within a large-scale <span class="hlt">coupled</span> climate <span class="hlt">model</span>, which has led to a poor understanding of the interactions between TIW-induced feedback and ENSO. In this study, a novel <span class="hlt">modeling</span> system was developed that allows representation of TIW-scale air-sea <span class="hlt">coupling</span> and its interaction with ENSO. Satellite data were first used to derive an empirical <span class="hlt">model</span> for TIW-induced sea surface wind stress perturbations (τTIW). The <span class="hlt">model</span> was then embedded in a basin-wide hybrid-<span class="hlt">coupled</span> <span class="hlt">model</span> (HCM) of the tropical Pacific. Because τTIW were internally determined from TIW-scale sea surface temperatures (SSTTIW) simulated in the ocean <span class="hlt">model</span>, the wind-SST <span class="hlt">coupling</span> at TIW scales was interactively represented within the large-scale <span class="hlt">coupled</span> <span class="hlt">model</span>. Because the τTIW-SSTTIW <span class="hlt">coupling</span> part of the <span class="hlt">model</span> can be turned on or off in the HCM simulations, the related TIW wind feedback effects can be isolated and examined in a straightforward way. Then, the TIW-scale wind feedback effects on the large-scale mean ocean state and interannual variability in the tropical Pacific were investigated based on this embedded system. The interactively represented TIW-scale wind forcing exerted an asymmetric influence on SSTs in the HCM, characterized by a mean-state cooling and by a positive feedback on interannual variability, acting to enhance ENSO amplitude. Roughly speaking, the feedback tends to increase interannual SST variability by approximately 9%. Additionally, there is a tendency for TIW wind to have an effect on the phase transition during ENSO evolution, with slightly shortened interannual oscillation periods. Additional sensitivity experiments were performed to elucidate the details of TIW wind effects on SST evolution during ENSO</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016WRCM...26..243A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016WRCM...26..243A"><span>An investigation of stress <span class="hlt">wave</span> propagation in a shear deformable nanobeam based on modified <span class="hlt">couple</span> stress theory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Akbarzadeh Khorshidi, Majid; Shariati, Mahmoud</p> <p>2016-04-01</p> <p>This paper presents a new investigation for propagation of stress <span class="hlt">wave</span> in a nanobeam based on modified <span class="hlt">couple</span> stress theory. Using Euler-Bernoulli beam theory, Timoshenko beam theory, and Reddy beam theory, the effect of shear deformation is investigated. This nonclassical <span class="hlt">model</span> contains a material length scale parameter to capture the size effect and the Poisson effect is incorporated in the <span class="hlt">current</span> <span class="hlt">model</span>. Governing equations of motion are obtained by Hamilton's principle and solved explicitly. This solution leads to obtain two phase velocities for shear deformable beams in different directions. Effects of shear deformation, material length scale parameter, and Poisson's ratio on the behavior of these phase velocities are investigated and discussed. The results also show a dual behavior for phase velocities against Poisson's ratio.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011AGUFMSM34A..01P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011AGUFMSM34A..01P"><span>Shear Alfven <span class="hlt">Wave</span> Injection in the Magnetosphere by Ionospheric Modifications in the Absence of Electrojet <span class="hlt">Currents</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Papadopoulos, K.; Eliasson, B.; Shao, X.; Labenski, J.; Chang, C.</p> <p>2011-12-01</p> <p>A new concept of generating ionospheric <span class="hlt">currents</span> in the ULF/ELF range with modulated HF heating using ground-based transmitters even in the absence of electrojet <span class="hlt">currents</span> is presented. The new concept relies on using HF heating of the F-region to modulate the electron temperature and has been given the name Ionospheric <span class="hlt">Current</span> Drive (ICD). In ICD, the pressure gradient associated with anomalous or collisional F-region electron heating drives a local diamagnetic <span class="hlt">current</span> that acts as an antenna to inject mainly Magneto-Sonic (MS) <span class="hlt">waves</span> in the ionospheric plasma. The electric field associated with the MS <span class="hlt">wave</span> drives Hall <span class="hlt">currents</span> when it reaches the E region of the ionosphere. The Hall <span class="hlt">currents</span> act as a secondary antenna that inject <span class="hlt">waves</span> in the Earth-Ionosphere Waveguide (EIW) below and shear Alfven <span class="hlt">waves</span> or EMIC <span class="hlt">waves</span> upwards towards the conjugate regions. The paper presents: (i) Theoretical results using a cold Hall MHD <span class="hlt">model</span> to study ICD and the generation of ULF/ELF <span class="hlt">waves</span> by the modulation of the electron pressure at the F2-region with an intense HF electromagnetic <span class="hlt">wave</span>. The <span class="hlt">model</span> solves equations governing the dynamics of the shear Alfven and magnetosonic modes, of the damped modes in the diffusive Pedersen layer, and of the weakly damped helicon <span class="hlt">wave</span> mode in the Hall-dominated E-region. The <span class="hlt">model</span> incorporates realistic profile of the ionospheric conductivities and magnetic field configuration. We use the <span class="hlt">model</span> to simulate propagation and dynamics of the low-frequency <span class="hlt">waves</span> and their injection into the magnetosphere from the HAARP and Arecibo ionospheric heaters. (ii) Proof of principle experiments using the HAARP ionospheric heater in conjunction with measurements by the DEMETER satellite This work is supported by ONR MURI grant and DARPA BRIOCHE Program</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1510823M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1510823M"><span>Penetration of Solar Wind Driven ULF <span class="hlt">Waves</span> into the Earth's Inner Magnetosphere: Role in Radiation Belt and Ring <span class="hlt">Current</span> Dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mann, Ian; Murphy, Kyle; Rae, Jonathan; Ozeke, Louis; Milling, David</p> <p>2013-04-01</p> <p>Ultra-low frequency (ULF) <span class="hlt">waves</span> in the Pc4-5 band can be excited in the magnetosphere by the solar wind. Much recent work has shown how ULF <span class="hlt">wave</span> power is strongly correlated with solar wind speed. However, little attention has been paid the dynamics of ULF <span class="hlt">wave</span> power penetration onto low L-shells in the inner magnetosphere. We use more than a solar cycle of ULF <span class="hlt">wave</span> data, derived from ground-based magnetometer networks, to examine this ULF <span class="hlt">wave</span> power penetration and its dependence on solar wind and geomagnetic activity indices. In time domain data, we show very clearly that dayside ULF <span class="hlt">wave</span> power, spanning more than 4 orders of magnitude, follows solar wind speed variations throughout the whole solar cycle - during periods of sporadic solar maximum ICMEs, during declining phase fast solar wind streams, and at solar minimum, alike. We also show that time domain ULF <span class="hlt">wave</span> power increases during magnetic storms activations, and significantly demonstrate that a deeper ULF <span class="hlt">wave</span> power penetration into the inner magnetosphere occurs during larger negative excursions in Dst. We discuss potential explanations for this low-L ULF <span class="hlt">wave</span> power penetration, including the role of plasma mass density (such as during plasmaspheric erosion), or ring <span class="hlt">current</span> ion instabilities during near-Earth ring <span class="hlt">current</span> penetration. Interestingly, we also show that both ULF <span class="hlt">wave</span> power and SAMPEX MeV electron flux show a remarkable similarity in their penetration to low-L, which suggests that ULF <span class="hlt">wave</span> power penetration may be important for understanding and explaining radiation belt dynamics. Moreover, the correlation of ULF <span class="hlt">wave</span> power with Dst, which peaks at one day lag, suggests the ULF <span class="hlt">waves</span> might also be important for the inward transport of ions into the ring <span class="hlt">current</span>. <span class="hlt">Current</span> ring <span class="hlt">current</span> <span class="hlt">models</span>, which exclude long period ULF <span class="hlt">wave</span> transport, under-estimate the ring <span class="hlt">current</span> during fast solar wind streams which is consistent with a potential role for ULF <span class="hlt">waves</span> in ring <span class="hlt">current</span> energisation. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFMOS23E..01M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFMOS23E..01M"><span>An Asymptotic and Stochastic Theory for the Effects of Surface Gravity <span class="hlt">Waves</span> on <span class="hlt">Currents</span> and Infragravity <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>McWilliams, J. C.; Lane, E.; Melville, K.; Restrepo, J.; Sullivan, P.</p> <p>2004-12-01</p> <p>Oceanic surface gravity <span class="hlt">waves</span> are approximately irrotational, weakly nonlinear, and conservative, and they have a much shorter time scale than oceanic <span class="hlt">currents</span> and longer <span class="hlt">waves</span> (e.g., infragravity <span class="hlt">waves</span>) --- except where the primary surface <span class="hlt">waves</span> break. This provides a framework for an asymptotic theory, based on separation of time (and space) scales, of <span class="hlt">wave</span>-averaged effects associated with the conservative primary <span class="hlt">wave</span> dynamics combined with a stochastic representation of the momentum transfer and induced mixing associated with non-conservative <span class="hlt">wave</span> breaking. Such a theory requires only modest information about the primary <span class="hlt">wave</span> field from measurements or operational <span class="hlt">model</span> forecasts and thus avoids the enormous burden of calculating the <span class="hlt">waves</span> on their intrinsically small space and time scales. For the conservative effects, the result is a vortex force associated with the primary <span class="hlt">wave</span>'s Stokes drift; a <span class="hlt">wave</span>-averaged Bernoulli head and sea-level set-up; and an incremental material advection by the Stokes drift. This can be compared to the "radiation stress" formalism of Longuet-Higgins, Stewart, and Hasselmann; it is shown to be a preferable representation since the radiation stress is trivial at its apparent leading order. For the non-conservative breaking effects, a population of stochastic impulses is added to the <span class="hlt">current</span> and infragravity momentum equations with distribution functions taken from measurements. In offshore wind-<span class="hlt">wave</span> equilibria, these impulses replace the conventional surface wind stress and cause significant differences in the surface boundary layer <span class="hlt">currents</span> and entrainment rate, particularly when acting in combination with the conservative vortex force. In the surf zone, where breaking associated with shoaling removes nearly all of the primary <span class="hlt">wave</span> momentum and energy, the stochastic forcing plays an analogous role as the widely used nearshore radiation stress parameterizations. This talk describes the theoretical framework and presents some</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1357467','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/1357467"><span>Slot-<span class="hlt">coupled</span> CW standing <span class="hlt">wave</span> accelerating cavity</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Wang, Shaoheng; Rimmer, Robert; Wang, Haipeng</p> <p>2017-05-16</p> <p>A slot-<span class="hlt">coupled</span> CW standing <span class="hlt">wave</span> multi-cell accelerating cavity. To achieve high efficiency graded beta acceleration, each cell in the multi-cell cavity may include different cell lengths. Alternatively, to achieve high efficiency with acceleration for particles with beta equal to 1, each cell in the multi-cell cavity may include the same cell design. <span class="hlt">Coupling</span> between the cells is achieved with a plurality of axially aligned kidney-shaped slots on the wall between cells. The slot-<span class="hlt">coupling</span> method makes the design very compact. The shape of the cell, including the slots and the cone, are optimized to maximize the power efficiency and minimize the peak power density on the surface. The slots are non-resonant, thereby enabling shorter slots and less power loss.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRA..123..827N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRA..123..827N"><span>Exploring <span class="hlt">Wave-Wave</span> Interactions in a General Circulation <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>Nystrom, Virginia; Gasperini, Federico; Forbes, Jeffrey M.; Hagan, Maura E.</p> <p>2018-01-01</p> <p>Nonlinear interactions involving Kelvin <span class="hlt">waves</span> with (periods, zonal <span class="hlt">wave</span> numbers) = (3.7d, s =- 1) (UFKW1) and = (2.4d, s =- 1) (UFKW2) and s = 0 and s = 1 quasi 9 day <span class="hlt">waves</span> (Q9DW) with diurnal tides DW1, DW2, DW3, DE2, and DE3 are explored within a National Center for Atmospheric Research (NCAR) thermosphere-ionosphere-mesosphere electrodynamics general circulation <span class="hlt">model</span> (TIME-GCM) simulation driven at its ˜30 km lower boundary by interpolated 3-hourly output from Modern-Era Retrospective Analysis for Research and Applications (MERRA). The existence of nonlinear <span class="hlt">wave-wave</span> interactions between the above primary <span class="hlt">waves</span> is determined by the presence of secondary <span class="hlt">waves</span> (SWs) with frequencies and zonal <span class="hlt">wave</span> numbers that are the sums and differences of those of the primary (interacting) <span class="hlt">waves</span>. Focus is on 10-21 April 2009, when the nontidal dynamics in the mesosphere-lower thermosphere (MLT) region is dominated by UFKW and when identification of SW is robust. Fifteen SWs are identified in all. An interesting triad is identified involving UFKW1, DE3, and a secondary UFKW4 = (1.5d, s =- 2): The UFKW1-DE3 interaction produces UFKW4, the UFKW4-DE3 interaction produces UFKW1, and the UFKW1 interaction with UFKW4 produces DE3. At 120 km the dynamic range of the reconstructed latitude-longitude zonal wind field due to all of the SW is roughly half that of the primary <span class="hlt">waves</span>, which produced them. This suggests that nonlinear <span class="hlt">wave-wave</span> interactions could significantly modify the way that the lower atmosphere <span class="hlt">couples</span> with the ionosphere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.4148M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.4148M"><span>How important is mode-<span class="hlt">coupling</span> in global surface <span class="hlt">wave</span> tomography?</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mikesell, Dylan; Nolet, Guust; Voronin, Sergey; Ritsema, Jeroen; Van Heijst, Hendrik-Jan</p> <p>2016-04-01</p> <p>To investigate the influence of mode <span class="hlt">coupling</span> for fundamental mode Rayleigh <span class="hlt">waves</span> with periods between 64 and 174s, we analysed 3,505,902 phase measurements obtained along minor arc trajectories as well as 2,163,474 phases along major arcs. This is a selection of five frequency bands from the data set of Van Heijst and Woodhouse, extended with more recent earthquakes, that served to define upper mantle S velocity in <span class="hlt">model</span> S40RTS. Since accurate estimation of the misfits (as represented by χ2) is essential, we used the method of Voronin et al. (GJI 199:276, 2014) to obtain objective estimates of the standard errors in this data set. We adapted Voronin's method slightly to avoid that systematic errors along clusters of raypaths can be accommodated by source corrections. This was done by simultaneously analysing multiple clusters of raypaths originating from the same group of earthquakes but traveling in different directions. For the minor arc data, phase errors at the one sigma level range from 0.26 rad at a period of 174s to 0.89 rad at 64s. For the major arcs, these errors are roughly twice as high (0.40 and 2.09 rad, respectively). In the subsequent inversion we removed any outliers that could not be fitted at the 3 sigma level in an almost undamped inversion. Using these error estimates and the theory of finite-frequency tomography to include the effects of scattering, we solved for <span class="hlt">models</span> with χ2 = N (the number of data) both including and excluding the effect of mode <span class="hlt">coupling</span> between Love and Rayleigh <span class="hlt">waves</span>. We shall present some dramatic differences between the two <span class="hlt">models</span>, notably near ocean-continent boundaries (e.g. California) where mode conversions are likely to be largest. But a sharpening of other features, such as cratons and high-velocity blobs in the oceanic domain, is also observed when mode <span class="hlt">coupling</span> is taken into account. An investigation of the influence of <span class="hlt">coupling</span> on azimuthal anisotropy is still under way at the time of writing of this</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvB..95f4309B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..95f4309B"><span>Scattering of an electronic <span class="hlt">wave</span> packet by a one-dimensional electron-phonon-<span class="hlt">coupled</span> structure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Brockt, C.; Jeckelmann, E.</p> <p>2017-02-01</p> <p>We investigate the scattering of an electron by phonons in a small structure between two one-dimensional tight-binding leads. This <span class="hlt">model</span> mimics the quantum electron transport through atomic wires or molecular junctions <span class="hlt">coupled</span> to metallic leads. The electron-phonon-<span class="hlt">coupled</span> structure is represented by the Holstein <span class="hlt">model</span>. We observe permanent energy transfer from the electron to the phonon system (dissipation), transient self-trapping of the electron in the electron-phonon-<span class="hlt">coupled</span> structure (due to polaron formation and multiple reflections at the structure edges), and transmission resonances that depend strongly on the strength of the electron-phonon <span class="hlt">coupling</span> and the adiabaticity ratio. A recently developed TEBD algorithm, optimized for bosonic degrees of freedom, is used to simulate the quantum dynamics of a <span class="hlt">wave</span> packet launched against the electron-phonon-<span class="hlt">coupled</span> structure. Exact results are calculated for a single electron-phonon site using scattering theory and analytical approximations are obtained for limiting cases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ChPhB..25i0201X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ChPhB..25i0201X"><span>Localized <span class="hlt">waves</span> in three-component <span class="hlt">coupled</span> nonlinear Schrödinger equation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Tao; Chen, Yong</p> <p>2016-09-01</p> <p>We study the generalized Darboux transformation to the three-component <span class="hlt">coupled</span> nonlinear Schrödinger equation. First- and second-order localized <span class="hlt">waves</span> are obtained by this technique. In first-order localized <span class="hlt">wave</span>, we get the interactional solutions between first-order rogue <span class="hlt">wave</span> and one-dark, one-bright soliton respectively. Meanwhile, the interactional solutions between one-breather and first-order rogue <span class="hlt">wave</span> are also given. In second-order localized <span class="hlt">wave</span>, one-dark-one-bright soliton together with second-order rogue <span class="hlt">wave</span> is presented in the first component, and two-bright soliton together with second-order rogue <span class="hlt">wave</span> are gained respectively in the other two components. Besides, we observe second-order rogue <span class="hlt">wave</span> together with one-breather in three components. Moreover, by increasing the absolute values of two free parameters, the nonlinear <span class="hlt">waves</span> merge with each other distinctly. These results further reveal the interesting dynamic structures of localized <span class="hlt">waves</span> in the three-component <span class="hlt">coupled</span> system. Project supported by the Global Change Research Program of China (Grant No. 2015CB953904), the National Natural Science Foundation of China (Grant Nos. 11275072 and 11435005), the Doctoral Program of Higher Education of China (Grant No. 20120076110024), the Network Information Physics Calculation of Basic Research Innovation Research Group of China (Grant No. 61321064), and Shanghai Collaborative Innovation Center of Trustworthy Software for Internet of Things, China (Grant No. ZF1213).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvB..96n4428S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..96n4428S"><span>Toward nonlinear magnonics: Intensity-dependent spin-<span class="hlt">wave</span> switching in insulating side-<span class="hlt">coupled</span> magnetic stripes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sadovnikov, A. V.; Odintsov, S. A.; Beginin, E. N.; Sheshukova, S. E.; Sharaevskii, Yu. P.; Nikitov, S. A.</p> <p>2017-10-01</p> <p>We demonstrate that the nonlinear spin-<span class="hlt">wave</span> transport in two laterally parallel magnetic stripes exhibit the intensity-dependent power exchange between the adjacent spin-<span class="hlt">wave</span> channels. By the means of Brillouin light scattering technique, we investigate collective nonlinear spin-<span class="hlt">wave</span> dynamics in the presence of magnetodipolar <span class="hlt">coupling</span>. The nonlinear intensity-dependent effect reveals itself in the spin-<span class="hlt">wave</span> mode transformation and differential nonlinear spin-<span class="hlt">wave</span> phase shift in each adjacent magnetic stripe. The proposed analytical theory, based on the <span class="hlt">coupled</span> Ginzburg-Landau equations, predicts the geometry design involving the reduction of power requirement to the all-magnonic switching. A very good agreement between calculation and experiment was found. In addition, a micromagnetic and finite-element approach has been independently used to study the nonlinear behavior of spin <span class="hlt">waves</span> in adjacent stripes and the nonlinear transformation of spatial profiles of spin-<span class="hlt">wave</span> modes. Our results show that the proposed spin-<span class="hlt">wave</span> <span class="hlt">coupling</span> mechanism provides the basis for nonlinear magnonic circuits and opens the perspectives for all-magnonic computing architecture.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1392808-pic-simulations-wave-particle-interactions-initial-electron-velocity-distribution-from-kinetic-ring-current-model','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1392808-pic-simulations-wave-particle-interactions-initial-electron-velocity-distribution-from-kinetic-ring-current-model"><span>PIC simulations of <span class="hlt">wave</span>-particle interactions with an initial electron velocity distribution from a kinetic ring <span class="hlt">current</span> <span class="hlt">model</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Yu, Yiqun; Delzanno, Gian Luca; Jordanova, Vania Koleva; ...</p> <p>2017-07-15</p> <p>Whistler <span class="hlt">wave</span>-particle interactions play an important role in the Earth inner magnetospheric dynamics and have been the subject of numerous investigations. By running a global kinetic ring <span class="hlt">current</span> <span class="hlt">model</span> (RAM-SCB) in a storm event occurred on Oct 23–24 2002, we obtain the ring <span class="hlt">current</span> electron distribution at a selected location at MLT of 9 and L of 6 where the electron distribution is composed of a warm population in the form of a partial ring in the velocity space (with energy around 15 keV) in addition to a cool population with a Maxwellian-like distribution. The warm population is likely frommore » the injected plasma sheet electrons during substorm injections that supply fresh source to the inner magnetosphere. These electron distributions are then used as input in an implicit particle-in-cell code (iPIC3D) to study whistler-<span class="hlt">wave</span> generation and the subsequent <span class="hlt">wave</span>-particle interactions. Here, we find that whistler <span class="hlt">waves</span> are excited and propagate in the quasi-parallel direction along the background magnetic field. Several different <span class="hlt">wave</span> modes are instantaneously generated with different growth rates and frequencies. The <span class="hlt">wave</span> mode at the maximum growth rate has a frequency around 0.62ω ce, which corresponds to a parallel resonant energy of 2.5 keV. Linear theory analysis of <span class="hlt">wave</span> growth is in excellent agreement with the simulation results. These <span class="hlt">waves</span> grow initially due to the injected warm electrons and are later damped due to cyclotron absorption by electrons whose energy is close to the resonant energy and can effectively attenuate <span class="hlt">waves</span>. The warm electron population overall experiences net energy loss and anisotropy drop while moving along the diffusion surfaces towards regions of lower phase space density, while the cool electron population undergoes heating when the <span class="hlt">waves</span> grow, suggesting the cross-population interactions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1392808-pic-simulations-wave-particle-interactions-initial-electron-velocity-distribution-from-kinetic-ring-current-model','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1392808-pic-simulations-wave-particle-interactions-initial-electron-velocity-distribution-from-kinetic-ring-current-model"><span>PIC simulations of <span class="hlt">wave</span>-particle interactions with an initial electron velocity distribution from a kinetic ring <span class="hlt">current</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>Yu, Yiqun; Delzanno, Gian Luca; Jordanova, Vania Koleva</p> <p></p> <p>Whistler <span class="hlt">wave</span>-particle interactions play an important role in the Earth inner magnetospheric dynamics and have been the subject of numerous investigations. By running a global kinetic ring <span class="hlt">current</span> <span class="hlt">model</span> (RAM-SCB) in a storm event occurred on Oct 23–24 2002, we obtain the ring <span class="hlt">current</span> electron distribution at a selected location at MLT of 9 and L of 6 where the electron distribution is composed of a warm population in the form of a partial ring in the velocity space (with energy around 15 keV) in addition to a cool population with a Maxwellian-like distribution. The warm population is likely frommore » the injected plasma sheet electrons during substorm injections that supply fresh source to the inner magnetosphere. These electron distributions are then used as input in an implicit particle-in-cell code (iPIC3D) to study whistler-<span class="hlt">wave</span> generation and the subsequent <span class="hlt">wave</span>-particle interactions. Here, we find that whistler <span class="hlt">waves</span> are excited and propagate in the quasi-parallel direction along the background magnetic field. Several different <span class="hlt">wave</span> modes are instantaneously generated with different growth rates and frequencies. The <span class="hlt">wave</span> mode at the maximum growth rate has a frequency around 0.62ω ce, which corresponds to a parallel resonant energy of 2.5 keV. Linear theory analysis of <span class="hlt">wave</span> growth is in excellent agreement with the simulation results. These <span class="hlt">waves</span> grow initially due to the injected warm electrons and are later damped due to cyclotron absorption by electrons whose energy is close to the resonant energy and can effectively attenuate <span class="hlt">waves</span>. The warm electron population overall experiences net energy loss and anisotropy drop while moving along the diffusion surfaces towards regions of lower phase space density, while the cool electron population undergoes heating when the <span class="hlt">waves</span> grow, suggesting the cross-population interactions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1001475','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1001475"><span>Particle Tracking <span class="hlt">Model</span> (PTM) with Coastal <span class="hlt">Modeling</span> System (CMS)</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-11-04</p> <p>Coastal Inlets Research Program Particle Tracking <span class="hlt">Model</span> (PTM) with Coastal <span class="hlt">Modeling</span> System ( CMS ) The Particle Tracking <span class="hlt">Model</span> (PTM) is a Lagrangian...<span class="hlt">currents</span> and <span class="hlt">waves</span>. The Coastal Inlets Research Program (CIRP) supports the PTM with the Coastal <span class="hlt">Modeling</span> System ( CMS ), which provides <span class="hlt">coupled</span> <span class="hlt">wave</span>...and <span class="hlt">current</span> forcing for PTM simulations. CMS -PTM is implemented in the Surface-water <span class="hlt">Modeling</span> System, a GUI environment for input development</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/21895085','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21895085"><span>Fluid <span class="hlt">coupling</span> in a discrete <span class="hlt">model</span> of cochlear mechanics.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Elliott, Stephen J; Lineton, Ben; Ni, Guangjian</p> <p>2011-09-01</p> <p>A discrete <span class="hlt">model</span> of cochlear mechanics is introduced that includes a full, three-dimensional, description of fluid <span class="hlt">coupling</span>. This formulation allows the fluid <span class="hlt">coupling</span> and basilar membrane dynamics to be analyzed separately and then <span class="hlt">coupled</span> together with a simple piece of linear algebra. The fluid <span class="hlt">coupling</span> is initially analyzed using a wavenumber formulation and is separated into one component due to one-dimensional fluid <span class="hlt">coupling</span> and one comprising all the other contributions. Using the theory of acoustic <span class="hlt">waves</span> in a duct, however, these two components of the pressure can also be associated with a far field, due to the plane <span class="hlt">wave</span>, and a near field, due to the evanescent, higher order, modes. The near field components are then seen as one of a number of sources of additional longitudinal <span class="hlt">coupling</span> in the cochlea. The effects of non-uniformity and asymmetry in the fluid chamber areas can also be taken into account, to predict both the pressure difference between the chambers and the mean pressure. This allows the calculation, for example, of the effect of a short cochlear implant on the <span class="hlt">coupled</span> response of the cochlea. © 2011 Acoustical Society of America</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004PhyD..190..249U','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004PhyD..190..249U"><span>Standing <span class="hlt">waves</span>, clustering, and phase <span class="hlt">waves</span> in 1D simulations of kinetic relaxation oscillations in NO+NH 3 on Pt(1 0 0) <span class="hlt">coupled</span> by diffusion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Uecker, Hannes</p> <p>2004-04-01</p> <p>The Lombardo-Imbihl-Fink (LFI) ODE <span class="hlt">model</span> of the NO+NH 3 reaction on a Pt(1 0 0) surface shows stable relaxation oscillations with very sharp transitions for temperatures T between 404 and 433 K. Here we study numerically the effect of linear diffusive <span class="hlt">coupling</span> of these oscillators in one spatial dimension. Depending on the parameters and initial conditions we find a rich variety of spatio-temporal patterns which we group into four main regimes: bulk oscillations (BOs), standing <span class="hlt">waves</span> (SW), phase clusters (PC), and phase <span class="hlt">waves</span> (PW). Two key ingredients for SW and PC are identified, namely the relaxation type of the ODE oscillations and a nonlocal (and nonglobal) <span class="hlt">coupling</span> due to relatively fast diffusion of the kinetically slaved variables NH 3 and H. In particular, the latter replaces the global <span class="hlt">coupling</span> through the gas phase used to obtain SW and PC in <span class="hlt">models</span> of related surface reactions. The PW exist only under the assumption of (relatively) slow diffusion of NH 3 and H.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25871176','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25871176"><span>Synchronization of tunable asymmetric square-<span class="hlt">wave</span> pulses in delay-<span class="hlt">coupled</span> optoelectronic oscillators.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Martínez-Llinàs, Jade; Colet, Pere; Erneux, Thomas</p> <p>2015-03-01</p> <p>We consider a <span class="hlt">model</span> for two delay-<span class="hlt">coupled</span> optoelectronic oscillators under positive delayed feedback as prototypical to study the conditions for synchronization of asymmetric square-<span class="hlt">wave</span> oscillations, for which the duty cycle is not half of the period. We show that the scenario arising for positive feedback is much richer than with negative feedback. First, it allows for the coexistence of multiple in- and out-of-phase asymmetric periodic square <span class="hlt">waves</span> for the same parameter values. Second, it is tunable: The period of all the square-<span class="hlt">wave</span> periodic pulses can be tuned with the ratio of the delays, and the duty cycle of the asymmetric square <span class="hlt">waves</span> can be changed with the offset phase while the total period remains constant. Finally, in addition to the multiple in- and out-of-phase periodic square <span class="hlt">waves</span>, low-frequency periodic asymmetric solutions oscillating in phase may coexist for the same values of the parameters. Our analytical results are in agreement with numerical simulations and bifurcation diagrams obtained by using continuation techniques.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24580164','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24580164"><span>Dark- and bright-rogue-<span class="hlt">wave</span> solutions for media with long-<span class="hlt">wave-short-wave</span> resonance.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Shihua; Grelu, Philippe; Soto-Crespo, J M</p> <p>2014-01-01</p> <p>Exact explicit rogue-<span class="hlt">wave</span> solutions of intricate structures are presented for the long-<span class="hlt">wave-short-wave</span> resonance equation. These vector parametric solutions feature <span class="hlt">coupled</span> dark- and bright-field counterparts of the Peregrine soliton. Numerical simulations show the robustness of dark and bright rogue <span class="hlt">waves</span> in spite of the onset of modulational instability. Dark fields originate from the complex interplay between anomalous dispersion and the nonlinearity driven by the <span class="hlt">coupled</span> long <span class="hlt">wave</span>. This unusual mechanism, not available in scalar nonlinear <span class="hlt">wave</span> equation <span class="hlt">models</span>, can provide a route to the experimental realization of dark rogue <span class="hlt">waves</span> in, for instance, negative index media or with capillary-gravity <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28974675','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28974675"><span>Analog quantum simulation of the Rabi <span class="hlt">model</span> in the ultra-strong <span class="hlt">coupling</span> regime.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Braumüller, Jochen; Marthaler, Michael; Schneider, Andre; Stehli, Alexander; Rotzinger, Hannes; Weides, Martin; Ustinov, Alexey V</p> <p>2017-10-03</p> <p>The quantum Rabi <span class="hlt">model</span> describes the fundamental mechanism of light-matter interaction. It consists of a two-level atom or qubit <span class="hlt">coupled</span> to a quantized harmonic mode via a transversal interaction. In the weak <span class="hlt">coupling</span> regime, it reduces to the well-known Jaynes-Cummings <span class="hlt">model</span> by applying a rotating <span class="hlt">wave</span> approximation. The rotating <span class="hlt">wave</span> approximation breaks down in the ultra-strong <span class="hlt">coupling</span> regime, where the effective <span class="hlt">coupling</span> strength g is comparable to the energy ω of the bosonic mode, and remarkable features in the system dynamics are revealed. Here we demonstrate an analog quantum simulation of an effective quantum Rabi <span class="hlt">model</span> in the ultra-strong <span class="hlt">coupling</span> regime, achieving a relative <span class="hlt">coupling</span> ratio of g/ω ~ 0.6. The quantum hardware of the simulator is a superconducting circuit embedded in a cQED setup. We observe fast and periodic quantum state collapses and revivals of the initial qubit state, being the most distinct signature of the synthesized <span class="hlt">model</span>.An analog quantum simulation scheme has been explored with a quantum hardware based on a superconducting circuit. Here the authors investigate the time evolution of the quantum Rabi <span class="hlt">model</span> at ultra-strong <span class="hlt">coupling</span> conditions, which is synthesized by slowing down the system dynamics in an effective frame.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22184664','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22184664"><span><span class="hlt">Wave</span> energy extraction by <span class="hlt">coupled</span> resonant absorbers.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Evans, D V; Porter, R</p> <p>2012-01-28</p> <p>In this article, a range of problems and theories will be introduced that will build towards a new <span class="hlt">wave</span> energy converter (WEC) concept, with the acronym 'ROTA' standing for resonant over-topping absorber. First, classical results for <span class="hlt">wave</span> power absorption for WECs constrained to operate in a single degree of freedom will be reviewed and the role of resonance in their operation highlighted. Emphasis will then be placed on how the introduction of further resonances can improve power take-off characteristics by extending the range of frequencies over which the efficiency is close to a theoretical maximum. Methods for doing this in different types of WECs will be demonstrated. <span class="hlt">Coupled</span> resonant absorbers achieve this by connecting a WEC device equipped with its own resonance (determined from a hydrodynamic analysis) to a new system having separate mass/spring/damper characteristics. It is shown that a <span class="hlt">coupled</span> resonant effect can be realized by inserting a water tank into a WEC, and this idea forms the basis of the ROTA device. In essence, the idea is to exploit the <span class="hlt">coupling</span> between the natural sloshing frequencies of the water in the internal tank and the natural resonance of a submerged buoyant circular cylinder device that is tethered to the sea floor, allowing a rotary motion about its axis of attachment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22263886-experimental-characterization-modeling-non-linear-coupling-lhcd-power-tore-supra','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22263886-experimental-characterization-modeling-non-linear-coupling-lhcd-power-tore-supra"><span>Experimental characterization and <span class="hlt">modeling</span> of non-linear <span class="hlt">coupling</span> of the LHCD power on Tore Supra</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>Preynas, M.; Goniche, M.; Hillairet, J.</p> <p>2014-02-12</p> <p>To achieve steady state operation on future tokamaks, in particular on ITER, the unique capability of a LHCD system to efficiently drive off-axis non-inductive <span class="hlt">current</span> is needed. In this context, it is of prime importance to study and master the <span class="hlt">coupling</span> of LH <span class="hlt">wave</span> to the core plasma at high power density (tens of MW/m{sup 2}). In some specific conditions, deleterious effects on the LHCD <span class="hlt">coupling</span> are sometimes observed on Tore Supra. At high power the <span class="hlt">waves</span> may modify the edge parameters that change the <span class="hlt">wave</span> <span class="hlt">coupling</span> properties in a non-linear manner. In this way, dedicated LHCD experiments have beenmore » performed using the LHCD system of Tore Supra, composed of two different conceptual designs of launcher: the Fully Active Multijunction (FAM) and the new Passive Active Multijunction (PAM) antennas. A nonlinear interaction between the electron density and the electric field has been characterized in a thin plasma layer in front of the two LHCD antennas. The resulting dependence of the power reflection coefficient with the LHCD power, leading occasionally to trips in the output power, is not predicted by the standard linear theory of the LH <span class="hlt">wave</span> <span class="hlt">coupling</span>. Therefore, it is important to investigate and understand the possible origin of such non-linear effects in order to avoid their possible deleterious consequences. The PICCOLO-2D code, which self-consistently treats the <span class="hlt">wave</span> propagation in the antenna vicinity and its interaction with the local edge plasma density, is used to simulate Tore Supra discharges. The simulation reproduces very well the occurrence of a non-linear behavior in the <span class="hlt">coupling</span> observed in the LHCD experiments. The important differences and trends between the FAM and the PAM antennas, especially a larger increase in RC for the FAM, are also reproduced by the PICCOLO-2D simulation. The working hypothesis of the contribution of the ponderomotive effect in the non-linear observations of LHCD <span class="hlt">coupling</span> is therefore validated through this</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GeoRL..4412280A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GeoRL..4412280A"><span>Internal <span class="hlt">Waves</span> in the East Australian <span class="hlt">Current</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Alford, Matthew H.; Sloyan, Bernadette M.; Simmons, Harper L.</p> <p>2017-12-01</p> <p>Internal <span class="hlt">waves</span>, which drive most ocean turbulence and add "noise" to lower-frequency records, interact with low-frequency <span class="hlt">current</span> systems and topography in yet poorly known ways. Taking advantage of a heavily instrumented, 14 month mooring array, internal <span class="hlt">waves</span> in the East Australian <span class="hlt">Current</span> (EAC) are examined for the first time. Internal <span class="hlt">wave</span> horizontal kinetic energy (HKE) is within a factor of 2 of the Garrett-Munk (1976) spectrum. Continuum internal <span class="hlt">waves</span>, near-inertial <span class="hlt">waves</span>, and internal tides together constitute a significant percentage of the total velocity variance. Mode-1 internal tide energy fluxes are southward and much smaller than energy times group velocity, consistent with reflection at the continental slope of incident <span class="hlt">waves</span> generated from near New Caledonia and the Solomon Islands. Internal tide HKE is highly phase variable, consistent with refraction by the variable EAC. Mode-1 near-inertial <span class="hlt">wave</span> energy fluxes are of comparable magnitude and are equatorward and episodic, consistent with generation by storms farther poleward. These processes are considered together in the complex environment of the EAC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1439691-wave-resource-characterization-using-unstructured-grid-modeling-approach','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1439691-wave-resource-characterization-using-unstructured-grid-modeling-approach"><span><span class="hlt">Wave</span> Resource Characterization Using an Unstructured Grid <span class="hlt">Modeling</span> Approach</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>Wu, Wei-Cheng; Yang, Zhaoqing; Wang, Taiping</p> <p></p> <p>This paper presents a <span class="hlt">modeling</span> study conducted on the central Oregon coast for <span class="hlt">wave</span> resource characterization using the unstructured-grid SWAN <span class="hlt">model</span> <span class="hlt">coupled</span> with a nested-grid WWIII <span class="hlt">model</span>. The flexibility of <span class="hlt">models</span> of various spatial resolutions and the effects of open- boundary conditions simulated by a nested-grid WWIII <span class="hlt">model</span> with different physics packages were evaluated. The <span class="hlt">model</span> results demonstrate the advantage of the unstructured-grid <span class="hlt">modeling</span> approach for flexible <span class="hlt">model</span> resolution and good <span class="hlt">model</span> skills in simulating the six <span class="hlt">wave</span> resource parameters recommended by the International Electrotechnical Commission in comparison to the observed data in Year 2009 at National Data Buoy Centermore » Buoy 46050. Notably, spectral analysis indicates that the ST4 physics package improves upon the <span class="hlt">model</span> skill of the ST2 physics package for predicting <span class="hlt">wave</span> power density for large <span class="hlt">waves</span>, which is important for <span class="hlt">wave</span> resource assessment, device load calculation, and risk management. In addition, bivariate distributions show the simulated sea state of maximum occurrence with the ST4 physics package matched the observed data better than that with the ST2 physics package. This study demonstrated that the unstructured-grid <span class="hlt">wave</span> <span class="hlt">modeling</span> approach, driven by the nested-grid regional WWIII outputs with the ST4 physics package, can efficiently provide accurate <span class="hlt">wave</span> hindcasts to support <span class="hlt">wave</span> resource characterization. Our study also suggests that wind effects need to be considered if the dimension of the <span class="hlt">model</span> domain is greater than approximately 100 km, or O (10^2 km).« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDD34006K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDD34006K"><span>Influence of Internal <span class="hlt">Waves</span> on Transport by a Gravity <span class="hlt">Current</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koseff, Jeffrey; Hogg, Charlie; Ouillon, Raphael; Ouellette, Nicholas; Meiburg, Eckart</p> <p>2017-11-01</p> <p>Gravity <span class="hlt">currents</span> moving along the continental slope can be influenced by internal <span class="hlt">waves</span> shoaling on the slope resulting in mixing between the gravity <span class="hlt">current</span> and the ambient fluid. Whilst some observations of the potential influence of internal <span class="hlt">waves</span> on gravity <span class="hlt">currents</span> have been made, the process has not been studied systematically. We present laboratory experiments, and some initial numerical simulations, in which a gravity <span class="hlt">current</span> descends down a sloped boundary through a pycnocline at the same time as an internal <span class="hlt">wave</span> at the pycnocline shoals on the slope. Measurements of the downslope mass flux of the gravity <span class="hlt">current</span> fluid in cases with different amplitudes of the incident internal <span class="hlt">wave</span> will be discussed. For the parameter regime considered, the mass flux in the head of the gravity <span class="hlt">current</span> was found to reduce with increasingly larger incident amplitude <span class="hlt">waves</span>. This reduction was effectively caused by a ``decapitation'' process whereby the breaking internal <span class="hlt">wave</span> captures and moves fluid from the head of the gravity <span class="hlt">current</span> back up the slope. The significance of the impact of the internal <span class="hlt">waves</span> on gravity <span class="hlt">current</span> transport, strongly suggests that the local internal <span class="hlt">wave</span> climate may need to be considered when calculating gravity <span class="hlt">current</span> transport. The Bob and Norma Street Environmental Fluid Mechanics Laboratory.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016Chaos..26e3103C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016Chaos..26e3103C"><span>Heterogeneity and nearest-neighbor <span class="hlt">coupling</span> can explain small-worldness and <span class="hlt">wave</span> properties in pancreatic islets</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cappon, Giacomo; Pedersen, Morten Gram</p> <p>2016-05-01</p> <p>Many multicellular systems consist of <span class="hlt">coupled</span> cells that work as a syncytium. The pancreatic islet of Langerhans is a well-studied example of such a microorgan. The islets are responsible for secretion of glucose-regulating hormones, mainly glucagon and insulin, which are released in distinct pulses. In order to observe pulsatile insulin secretion from the β-cells within the islets, the cellular responses must be synchronized. It is now well established that gap junctions provide the electrical nearest-neighbor <span class="hlt">coupling</span> that allows excitation <span class="hlt">waves</span> to spread across islets to synchronize the β-cell population. Surprisingly, functional <span class="hlt">coupling</span> analysis of calcium responses in β-cells shows small-world properties, i.e., a high degree of local <span class="hlt">coupling</span> with a few long-range "short-cut" connections that reduce the average path-length greatly. Here, we investigate how such long-range functional <span class="hlt">coupling</span> can appear as a result of heterogeneity, nearest-neighbor <span class="hlt">coupling</span>, and <span class="hlt">wave</span> propagation. Heterogeneity is also able to explain a set of experimentally observed synchronization and <span class="hlt">wave</span> properties without introducing all-or-none cell <span class="hlt">coupling</span> and percolation theory. Our theoretical results highlight how local biological <span class="hlt">coupling</span> can give rise to functional small-world properties via heterogeneity and <span class="hlt">wave</span> propagation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDF19009M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDF19009M"><span>On resonant <span class="hlt">coupling</span> of acoustic <span class="hlt">waves</span> and gravity <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Millet, Christophe</p> <p>2017-11-01</p> <p>Acoustic propagation in the atmosphere is often <span class="hlt">modeled</span> using modes that are confined within waveguides causing the sound to propagate through multiple paths to the receiver. On the other hand, direct observations in the lower stratosphere show that the gravity <span class="hlt">wave</span> field is intermittent, and is often dominated by rather well defined large-amplitude <span class="hlt">wave</span> packets. In the present work, we use normal modes to describe both the gravity <span class="hlt">wave</span> field and the acoustic field. The gravity <span class="hlt">wave</span> spectrum is obtained by launching few monochromatic <span class="hlt">waves</span> whose properties are chosen stochastically to mimic the intermittency. Owing to the disparity of the gravity and acoustic length scales, the interactions between the gravity <span class="hlt">wave</span> field and each of the acoustic modes can be described using a multiple-scale analysis. The appropriate amplitude evolution equation for the acoustic field involves certain random terms that can be directly related to the gravity <span class="hlt">wave</span> sources. We will show that the cumulative effect of gravity <span class="hlt">wave</span> breakings makes the sensitivity of ground-based acoustic signals large, in that small changes in the gravity <span class="hlt">wave</span> parameterization can create or destroy specific acoustic features.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM53A..08Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM53A..08Y"><span>Improving the Ionospheric Auroral Conductance in a Global Ring <span class="hlt">Current</span> <span class="hlt">Model</span> and the Effects on the Ionospheric Electrodynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yu, Y.; Jordanova, V. K.; McGranaghan, R. M.; Solomon, S. C.</p> <p>2017-12-01</p> <p>The ionospheric conductance, height-integrated electric conductivity, can regulate both the ionospheric electrodynamics and the magnetospheric dynamics because of its key role in determining the electric field within the <span class="hlt">coupled</span> magnetosphere-ionosphere system. State-of-the-art global magnetosphere <span class="hlt">models</span> commonly adopt empirical conductance calculators to obtain the auroral conductance. Such specification can bypass the complexity of the ionosphere-thermosphere chemistry but on the other hand breaks the self-consistent link within the <span class="hlt">coupled</span> system. In this study, we <span class="hlt">couple</span> a kinetic ring <span class="hlt">current</span> <span class="hlt">model</span> RAM-SCB-E that solves for anisotropic particle distributions with a two-stream electron transport code (GLOW) to more self-consistently compute the height-dependent electric conductivity, provided the auroral electron precipitation from the ring <span class="hlt">current</span> <span class="hlt">model</span>. Comparisons with the traditional empirical formula are carried out. It is found that the newly <span class="hlt">coupled</span> <span class="hlt">modeling</span> framework reveals smaller Hall and Pedersen conductance, resulting in a larger electric field. As a consequence, the subauroral polarization streams demonstrate a better agreement with observations from DMSP satellites. It is further found that the commonly assumed Maxwellian spectrum of the particle precipitation is not globally appropriate. Instead, a full precipitation spectrum resulted from <span class="hlt">wave</span> particle interactions in the ring <span class="hlt">current</span> accounts for a more comprehensive precipitation spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1414919-pushing-particles-waves-current-drive-channeling','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1414919-pushing-particles-waves-current-drive-channeling"><span>Pushing Particles with <span class="hlt">Waves</span>: <span class="hlt">Current</span> Drive and α-Channeling</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>FISCH, Nathaniel J.</p> <p>2016-01-01</p> <p>It can be advantageous to push particles with <span class="hlt">waves</span> in tokamaks or other magnetic confinement devices, relying on <span class="hlt">wave</span>-particle resonances to accomplish specific goals. <span class="hlt">Waves</span> that damp on electrons or ions in toroidal fusion devises can drive <span class="hlt">currents</span> if the <span class="hlt">waves</span> are launched with toroidal asymmetry. Theses <span class="hlt">currents</span> are important for tokamaks, since they operate in the absence of an electric field with curl, enabling steady state operation. The lower hybrid <span class="hlt">wave</span> and the electron cyclotron <span class="hlt">wave</span> have been demonstrated to drive significant <span class="hlt">currents</span>. Non-inductive <span class="hlt">current</span> also stabilizes deleterious tearing modes. <span class="hlt">Waves</span> can also be used to broker the energymore » transfer between energetic alpha particles and the background plasma. Alpha particles born through fusion reactions in a tokamak reactor tend to slow down on electrons, but that could take up to hundreds of milliseconds. Before that happens, the energy in these alpha particles can destabilize on collisionless timescales toroidal Alfven modes and other <span class="hlt">waves</span>, in a way deleterious to energy confinement. However, it has been speculated that this energy might be instead be channeled instead into useful energy, that heats fuel ions or drives <span class="hlt">current</span>. Furthermore, an important question is the extent to which these effects can be accomplished together.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSPO14B2779C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSPO14B2779C"><span><span class="hlt">Wave</span> and Wind <span class="hlt">Model</span> Performance Metrics Tools</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, J. K.; Wang, D. W.</p> <p>2016-02-01</p> <p>Continual improvements and upgrades of Navy ocean <span class="hlt">wave</span> and wind <span class="hlt">models</span> are essential to the assurance of battlespace environment predictability of ocean surface <span class="hlt">wave</span> and surf conditions in support of Naval global operations. Thus, constant verification and validation of <span class="hlt">model</span> performance is equally essential to assure the progress of <span class="hlt">model</span> developments and maintain confidence in the predictions. Global and regional scale <span class="hlt">model</span> evaluations may require large areas and long periods of time. For observational data to compare against, altimeter winds and <span class="hlt">waves</span> along the tracks from past and <span class="hlt">current</span> operational satellites as well as moored/drifting buoys can be used for global and regional coverage. Using data and <span class="hlt">model</span> runs in previous trials such as the planned experiment, the Dynamics of the Adriatic in Real Time (DART), we demonstrated the use of accumulated altimeter wind and <span class="hlt">wave</span> data over several years to obtain an objective evaluation of the performance the SWAN (Simulating <span class="hlt">Waves</span> Nearshore) <span class="hlt">model</span> running in the Adriatic Sea. The assessment provided detailed performance of wind and <span class="hlt">wave</span> <span class="hlt">models</span> by using cell-averaged statistical variables maps with spatial statistics including slope, correlation, and scatter index to summarize <span class="hlt">model</span> performance. Such a methodology is easily generalized to other regions and at global scales. Operational technology <span class="hlt">currently</span> used by subject matter experts evaluating the Navy Coastal Ocean <span class="hlt">Model</span> and the Hybrid Coordinate Ocean <span class="hlt">Model</span> can be expanded to evaluate <span class="hlt">wave</span> and wind <span class="hlt">models</span> using tools developed for ArcMAP, a GIS application developed by ESRI. Recent inclusion of altimeter and buoy data into a format through the Naval Oceanographic Office's (NAVOCEANO) quality control system and the netCDF standards applicable to all <span class="hlt">model</span> output makes it possible for the fusion of these data and direct <span class="hlt">model</span> verification. Also, procedures were developed for the accumulation of match-ups of <span class="hlt">modelled</span> and observed parameters to form a data base</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGC22B..03O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGC22B..03O"><span>Improving <span class="hlt">wave</span> forecasting by integrating ensemble <span class="hlt">modelling</span> and machine learning</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>O'Donncha, F.; Zhang, Y.; James, S. C.</p> <p>2017-12-01</p> <p>Modern smart-grid networks use technologies to instantly relay information on supply and demand to support effective decision making. Integration of renewable-energy resources with these systems demands accurate forecasting of energy production (and demand) capacities. For <span class="hlt">wave</span>-energy converters, this requires <span class="hlt">wave</span>-condition forecasting to enable estimates of energy production. <span class="hlt">Current</span> operational <span class="hlt">wave</span> forecasting systems exhibit substantial errors with <span class="hlt">wave</span>-height RMSEs of 40 to 60 cm being typical, which limits the reliability of energy-generation predictions thereby impeding integration with the distribution grid. In this study, we integrate physics-based <span class="hlt">models</span> with statistical learning aggregation techniques that combine forecasts from multiple, independent <span class="hlt">models</span> into a single "best-estimate" prediction of the true state. The Simulating <span class="hlt">Waves</span> Nearshore physics-based <span class="hlt">model</span> is used to compute wind- and <span class="hlt">currents</span>-augmented <span class="hlt">waves</span> in the Monterey Bay area. Ensembles are developed based on multiple simulations perturbing input data (<span class="hlt">wave</span> characteristics supplied at the <span class="hlt">model</span> boundaries and winds) to the <span class="hlt">model</span>. A learning-aggregation technique uses past observations and past <span class="hlt">model</span> forecasts to calculate a weight for each <span class="hlt">model</span>. The aggregated forecasts are compared to observation data to quantify the performance of the <span class="hlt">model</span> ensemble and aggregation techniques. The appropriately weighted ensemble <span class="hlt">model</span> outperforms an individual ensemble member with regard to forecasting <span class="hlt">wave</span> conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM41A2676S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM41A2676S"><span>ULF <span class="hlt">Waves</span> in the Ionospheric Alfven Resonator: <span class="hlt">Modeling</span> of MICA Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Streltsov, A. V.; Tulegenov, B.</p> <p>2017-12-01</p> <p>We present results from a numerical study of physical processes responsible for the generation of small-scale, intense electromagnetic structures in the ultra-low-frequency range frequently observed in the close vicinity of bright discrete auroral arcs. In particular, our research is focused on the role of the ionosphere in generating these structures. A significant body of observations demonstrate that small-scale electromagnetic <span class="hlt">waves</span> with frequencies below 1 Hz are detected at high latitudes where the large-scale, downward magnetic field-aligned <span class="hlt">current</span> (FAC) interact with the ionosphere. Some theoretical studies suggest that these <span class="hlt">waves</span> can be generated by the ionospheric feedback instability (IFI) inside the ionospheric Alfven resonator (IAR). The IAR is the region in the low-altitude magnetosphere bounded by the strong gradient in the Alfven speed at high altitude and the conducting bottom of the ionosphere (ionospheric E-region) at low altitude. To study ULF <span class="hlt">waves</span> in this region we use a numerical <span class="hlt">model</span> developed from reduced two fluid MHD equations describing shear Alfven <span class="hlt">waves</span> in the ionosphere and magnetosphere of the earth. The active ionospheric feedback on structure and amplitude of magnetic FACs that interact with the ionosphere is implemented through the ionospheric boundary conditions that link the parallel <span class="hlt">current</span> density with the plasma density and the perpendicular electric field in the ionosphere. Our numerical results are compared with the in situ measurements performed by the Magnetosphere-Ionosphere <span class="hlt">Coupling</span> in the Alfven Resonator (MICA) sounding rocket, launched on February 19, 2012 from Poker Flat Research Range in Alaska to measure fields and particles during a passage through a discreet auroral arc. Parameters of the simulations are chosen to match actual MICA parameters, allowing the comparison in the most precise and rigorous way. <span class="hlt">Waves</span> generated in the numerical <span class="hlt">model</span> have frequencies between 0.30 and 0.45 Hz, while MICA measured</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996JGR...10120825B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996JGR...10120825B"><span>Ice-<span class="hlt">coupled</span> <span class="hlt">wave</span> propagation across an abrupt change in ice rigidity, density, or thickness</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barrett, Murray D.; Squire, Vernon A.</p> <p>1996-09-01</p> <p>The <span class="hlt">model</span> of Fox and Squire [1990, 1991, 1994], which discusses the oblique propagation of surface gravity <span class="hlt">waves</span> from the open sea into an ice sheet of constant thickness and properties, is augmented to include propagation across an abrupt transition of properties within a continuous ice sheet or across two dissimilar ice sheets that abut one another but are free to move independently. Rigidity, thickness, and/or density may change across the transition, allowing, for example, the <span class="hlt">modeling</span> of ice-<span class="hlt">coupled</span> <span class="hlt">waves</span> into, across, and out of refrozen leads and polynyas, across cracks, and through coherent pressure ridges. Reflection and transmission behavior is reported for various changes in properties under both types of transition conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NatPh..14..282T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NatPh..14..282T"><span>Spiral <span class="hlt">wave</span> chimera states in large populations of <span class="hlt">coupled</span> chemical oscillators</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Totz, Jan Frederik; Rode, Julian; Tinsley, Mark R.; Showalter, Kenneth; Engel, Harald</p> <p>2018-03-01</p> <p>The coexistence of coherent and incoherent dynamics in a population of identically <span class="hlt">coupled</span> oscillators is known as a chimera state1,2. Discovered in 20023, this counterintuitive dynamical behaviour has inspired extensive theoretical and experimental activity4-15. The spiral <span class="hlt">wave</span> chimera is a particularly remarkable chimera state, in which an ordered spiral <span class="hlt">wave</span> rotates around a core consisting of asynchronous oscillators. Spiral <span class="hlt">wave</span> chimeras were theoretically predicted in 200416 and numerically studied in a variety of systems17-23. Here, we report their experimental verification using large populations of nonlocally <span class="hlt">coupled</span> Belousov-Zhabotinsky chemical oscillators10,18 in a two-dimensional array. We characterize previously unreported spatiotemporal dynamics, including erratic motion of the asynchronous spiral core, growth and splitting of the cores, as well as the transition from the chimera state to disordered behaviour. Spiral <span class="hlt">wave</span> chimeras are likely to occur in other systems with long-range interactions, such as cortical tissues24, cilia carpets25, SQUID metamaterials26 and arrays of optomechanical oscillators9.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1013700','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1013700"><span>Extension of NHWAVE to <span class="hlt">Couple</span> LAMMPS for <span class="hlt">Modeling</span> <span class="hlt">Wave</span> Interactions with Arctic Ice Floes</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-09-30</p> <p><span class="hlt">Modelling</span>, in press. Orzech, M., Shi, F., Veeramony, J., Bateman , S., Calantoni, J., and Kirby, J. T., 2015, “Incorporating floating surface...objects into a fully dispersive surface <span class="hlt">wave</span> model”, Ocean <span class="hlt">Modelling</span>, submitted. Bateman , S. Shi, F., Orzech, M., Veeramony, J., and Calantoni, J., 2014...Orzech, M., Shi, F., Calantoni, J., Bateman , S., and Veeramony, J., “Small-scale <span class="hlt">modeling</span> of <span class="hlt">waves</span> and floes in the Marginal Ice Zone”, 2014 Fall Meeting of the American Geophysical Union.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li class="active"><span>18</span></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_18 --> <div id="page_19" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="361"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMOS43A1394C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMOS43A1394C"><span>Usefulness of <span class="hlt">Wave</span> Data Assimilation to the <span class="hlt">WAVE</span> WATCH III <span class="hlt">Modeling</span> System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Choi, J. K.; Dykes, J. D.; Yaremchuk, M.; Wittmann, P.</p> <p>2017-12-01</p> <p>In-situ and remote-sensed <span class="hlt">wave</span> data are more abundant <span class="hlt">currently</span> than in years past, with excellent accuracy at global scales. Forecast skill of the <span class="hlt">WAVE</span> WATCH III <span class="hlt">model</span> is improved by assimilation of these measurements and they are also useful for <span class="hlt">model</span> validation and calibration. It has been known that the impact of assimilation in wind-sea conditions is not large, but spectra that result in large swell with long term propagation are identified and assimilated, the improved accuracy of the initial conditions improve the long-term forecasts. The Navy's assimilation method started with the simple Optimal Interpolation (OI) method. Operationally, Fleet Numerical Meteorology and Oceanography Center uses the sequential 2DVar scheme, but a new approach has been tested based on an adjoint-free method to variational assimilation in <span class="hlt">WAVE</span> WATCH III. We will present the status of <span class="hlt">wave</span> data assimilation into the <span class="hlt">WAVE</span> WATCH III numerical <span class="hlt">model</span> and upcoming development of this new adjoint-free variational approach.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvB..96j4504V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvB..96j4504V"><span>TRILEX and G W +EDMFT approach to d -<span class="hlt">wave</span> superconductivity in the Hubbard <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>Vučičević, J.; Ayral, T.; Parcollet, O.</p> <p>2017-09-01</p> <p>We generalize the recently introduced TRILEX approach (TRiply irreducible local EXpansion) to superconducting phases. The method treats simultaneously Mott and spin-fluctuation physics using an Eliashberg theory supplemented by local vertex corrections determined by a self-consistent quantum impurity <span class="hlt">model</span>. We show that, in the two-dimensional Hubbard <span class="hlt">model</span>, at strong <span class="hlt">coupling</span>, TRILEX yields a d -<span class="hlt">wave</span> superconducting dome as a function of doping. Contrary to the standard cluster dynamical mean field theory (DMFT) approaches, TRILEX can capture d -<span class="hlt">wave</span> pairing using only a single-site effective impurity <span class="hlt">model</span>. We also systematically explore the dependence of the superconducting temperature on the bare dispersion at weak <span class="hlt">coupling</span>, which shows a clear link between strong antiferromagnetic (AF) correlations and the onset of superconductivity. We identify a combination of hopping amplitudes particularly favorable to superconductivity at intermediate doping. Finally, we study within G W +EDMFT the low-temperature d -<span class="hlt">wave</span> superconducting phase at strong <span class="hlt">coupling</span> in a region of parameter space with reduced AF fluctuations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1254688','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1254688"><span>Full-<span class="hlt">wave</span> <span class="hlt">modeling</span> of EMIC <span class="hlt">waves</span> near the He + gyrofrequency</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Kim, Eun -Hwa; Johnson, Jay R.</p> <p></p> <p>Electromagnetic ion cyclotron (EMIC) <span class="hlt">waves</span> are known to be excited by the cyclotron instability associated with hot and anisotropic ion distributions in the equatorial region of the magnetosphere and are thought to play a key role in radiation belt losses. Although detection of these <span class="hlt">waves</span> at the ground can provide a global view of the EMIC <span class="hlt">wave</span> environment, it is not clear what signatures, if any, would be expected. One of the significant scientific issues concerning EMIC <span class="hlt">waves</span> is to understand how these <span class="hlt">waves</span> are detected at the ground. In order to solve this puzzle, it is necessary to understandmore » the propagation characteristics of the field-aligned EMIC <span class="hlt">waves</span>, which include polarization reversal, cutoff, resonance, and mode <span class="hlt">coupling</span> between different <span class="hlt">wave</span> modes, in a dipolar magnetic field. However, the inability of ray tracing to adequately describe <span class="hlt">wave</span> propagation near the crossover cutoff-resonance frequencies in multi-ion plasmas is one of reasons why these scientific questions remain unsolved. Using a recently developed 2-D full-<span class="hlt">wave</span> code that solves the full-<span class="hlt">wave</span> equations in global magnetospheric geometry, we demonstrate how EMIC <span class="hlt">waves</span> propagate from the equatorial region to higher magnetic latitude in an electron-proton-He+ plasma. We find that polarization reversal occurs at the crossover frequency from left-hand polarization (LHP) to right-hand (RHP) polarization and such RHP EMIC <span class="hlt">waves</span> can either propagate to the inner magnetosphere or reflect to the outer magnetosphere at the Buchsbaum resonance location. Lastly, we also find that mode <span class="hlt">coupling</span> from guided LHP EMIC <span class="hlt">waves</span> to unguided RHP or LHP <span class="hlt">waves</span> (i.e., fast mode) occurs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1254688-full-wave-modeling-emic-waves-near-he+-gyrofrequency','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1254688-full-wave-modeling-emic-waves-near-he+-gyrofrequency"><span>Full-<span class="hlt">wave</span> <span class="hlt">modeling</span> of EMIC <span class="hlt">waves</span> near the He + gyrofrequency</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Kim, Eun -Hwa; Johnson, Jay R.</p> <p>2016-01-06</p> <p>Electromagnetic ion cyclotron (EMIC) <span class="hlt">waves</span> are known to be excited by the cyclotron instability associated with hot and anisotropic ion distributions in the equatorial region of the magnetosphere and are thought to play a key role in radiation belt losses. Although detection of these <span class="hlt">waves</span> at the ground can provide a global view of the EMIC <span class="hlt">wave</span> environment, it is not clear what signatures, if any, would be expected. One of the significant scientific issues concerning EMIC <span class="hlt">waves</span> is to understand how these <span class="hlt">waves</span> are detected at the ground. In order to solve this puzzle, it is necessary to understandmore » the propagation characteristics of the field-aligned EMIC <span class="hlt">waves</span>, which include polarization reversal, cutoff, resonance, and mode <span class="hlt">coupling</span> between different <span class="hlt">wave</span> modes, in a dipolar magnetic field. However, the inability of ray tracing to adequately describe <span class="hlt">wave</span> propagation near the crossover cutoff-resonance frequencies in multi-ion plasmas is one of reasons why these scientific questions remain unsolved. Using a recently developed 2-D full-<span class="hlt">wave</span> code that solves the full-<span class="hlt">wave</span> equations in global magnetospheric geometry, we demonstrate how EMIC <span class="hlt">waves</span> propagate from the equatorial region to higher magnetic latitude in an electron-proton-He+ plasma. We find that polarization reversal occurs at the crossover frequency from left-hand polarization (LHP) to right-hand (RHP) polarization and such RHP EMIC <span class="hlt">waves</span> can either propagate to the inner magnetosphere or reflect to the outer magnetosphere at the Buchsbaum resonance location. Lastly, we also find that mode <span class="hlt">coupling</span> from guided LHP EMIC <span class="hlt">waves</span> to unguided RHP or LHP <span class="hlt">waves</span> (i.e., fast mode) occurs.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018InJPh..92..557Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018InJPh..92..557Z"><span>Influence of the frequency detuning on the four-<span class="hlt">wave</span> mixing efficiency in three-level system <span class="hlt">coupled</span> by standing-<span class="hlt">wave</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhou, Hai-Tao; Che, Shao-Na; Han, Yu-Hong; Wang, Dan</p> <p>2018-05-01</p> <p>In a Λ-type three-level atomic system <span class="hlt">coupled</span> by an off-resonant standing-<span class="hlt">wave</span>, the reflected four-<span class="hlt">wave</span> mixing (FWM) spectrum is studied. It shows that the maximum reflection efficiency occurs when both of the <span class="hlt">coupling</span> and probe fields are tuned off resonances from the atomic transitions. The essence of enhanced reflection is that the nonlinear efficiency of the FWM based on coherent atoms is improved due to the significant reduction of phase mismatch. The theoretical analysis shows good agreement with the experimental results. Furthermore, the influence of the atomic number density on the <span class="hlt">coupling</span> frequency detuning of the optimum reflection efficiency and the linewidth are also investigated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28056020','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28056020"><span>Travelling <span class="hlt">Wave</span> Pulse <span class="hlt">Coupled</span> Oscillator (TWPCO) Using a Self-Organizing Scheme for Energy-Efficient Wireless Sensor Networks.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Al-Mekhlafi, Zeyad Ghaleb; Hanapi, Zurina Mohd; Othman, Mohamed; Zukarnain, Zuriati Ahmad</p> <p>2017-01-01</p> <p>Recently, Pulse <span class="hlt">Coupled</span> Oscillator (PCO)-based travelling <span class="hlt">waves</span> have attracted substantial attention by researchers in wireless sensor network (WSN) synchronization. Because WSNs are generally artificial occurrences that mimic natural phenomena, the PCO utilizes firefly synchronization of attracting mating partners for <span class="hlt">modelling</span> the WSN. However, given that sensor nodes are unable to receive messages while transmitting data packets (due to deafness), the PCO <span class="hlt">model</span> may not be efficient for sensor network <span class="hlt">modelling</span>. To overcome this limitation, this paper proposed a new scheme called the Travelling <span class="hlt">Wave</span> Pulse <span class="hlt">Coupled</span> Oscillator (TWPCO). For this, the study used a self-organizing scheme for energy-efficient WSNs that adopted travelling <span class="hlt">wave</span> biologically inspired network systems based on phase locking of the PCO <span class="hlt">model</span> to counteract deafness. From the simulation, it was found that the proposed TWPCO scheme attained a steady state after a number of cycles. It also showed superior performance compared to other mechanisms, with a reduction in the total energy consumption of 25%. The results showed that the performance improved by 13% in terms of data gathering. Based on the results, the proposed scheme avoids the deafness that occurs in the transmit state in WSNs and increases the data collection throughout the transmission states in WSNs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5215802','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5215802"><span>Travelling <span class="hlt">Wave</span> Pulse <span class="hlt">Coupled</span> Oscillator (TWPCO) Using a Self-Organizing Scheme for Energy-Efficient Wireless Sensor Networks</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Hanapi, Zurina Mohd; Othman, Mohamed; Zukarnain, Zuriati Ahmad</p> <p>2017-01-01</p> <p>Recently, Pulse <span class="hlt">Coupled</span> Oscillator (PCO)-based travelling <span class="hlt">waves</span> have attracted substantial attention by researchers in wireless sensor network (WSN) synchronization. Because WSNs are generally artificial occurrences that mimic natural phenomena, the PCO utilizes firefly synchronization of attracting mating partners for <span class="hlt">modelling</span> the WSN. However, given that sensor nodes are unable to receive messages while transmitting data packets (due to deafness), the PCO <span class="hlt">model</span> may not be efficient for sensor network <span class="hlt">modelling</span>. To overcome this limitation, this paper proposed a new scheme called the Travelling <span class="hlt">Wave</span> Pulse <span class="hlt">Coupled</span> Oscillator (TWPCO). For this, the study used a self-organizing scheme for energy-efficient WSNs that adopted travelling <span class="hlt">wave</span> biologically inspired network systems based on phase locking of the PCO <span class="hlt">model</span> to counteract deafness. From the simulation, it was found that the proposed TWPCO scheme attained a steady state after a number of cycles. It also showed superior performance compared to other mechanisms, with a reduction in the total energy consumption of 25%. The results showed that the performance improved by 13% in terms of data gathering. Based on the results, the proposed scheme avoids the deafness that occurs in the transmit state in WSNs and increases the data collection throughout the transmission states in WSNs. PMID:28056020</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Chaos..27j4611B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Chaos..27j4611B"><span><span class="hlt">Coupling</span> nonlinear optical <span class="hlt">waves</span> to photoreactive and phase-separating soft matter: <span class="hlt">Current</span> status and perspectives</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Biria, Saeid; Morim, Derek R.; An Tsao, Fu; Saravanamuttu, Kalaichelvi; Hosein, Ian D.</p> <p>2017-10-01</p> <p>Nonlinear optics and polymer systems are distinct fields that have been studied for decades. These two fields intersect with the observation of nonlinear <span class="hlt">wave</span> propagation in photoreactive polymer systems. This has led to studies on the nonlinear dynamics of transmitted light in polymer media, particularly for optical self-trapping and optical modulation instability. The irreversibility of polymerization leads to permanent capture of nonlinear optical patterns in the polymer structure, which is a new synthetic route to complex structured soft materials. Over time more intricate polymer systems are employed, whereby nonlinear optical dynamics can <span class="hlt">couple</span> to nonlinear chemical dynamics, opening opportunities for self-organization. This paper discusses the work to date on nonlinear optical pattern formation processes in polymers. A brief overview of nonlinear optical phenomenon is provided to set the stage for understanding their effects. We review the accomplishments of the field on studying nonlinear waveform propagation in photopolymerizable systems, then discuss our most recent progress in <span class="hlt">coupling</span> nonlinear optical pattern formation to polymer blends and phase separation. To this end, perspectives on future directions and areas of sustained inquiry are provided. This review highlights the significant opportunity in exploiting nonlinear optical pattern formation in soft matter for the discovery of new light-directed and light-stimulated materials phenomenon, and in turn, soft matter provides a platform by which new nonlinear optical phenomenon may be discovered.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhPl...24e3513W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhPl...24e3513W"><span>Broad ion energy distributions in helicon <span class="hlt">wave-coupled</span> helium plasma</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Woller, K. B.; Whyte, D. G.; Wright, G. M.</p> <p>2017-05-01</p> <p>Helium ion energy distributions were measured in helicon <span class="hlt">wave-coupled</span> plasmas of the dynamics of ion implantation and sputtering of surface experiment using a retarding field energy analyzer. The shape of the energy distribution is a double-peak, characteristic of radiofrequency plasma potential modulation. The broad distribution is located within a radius of 0.8 cm, while the quartz tube of the plasma source has an inner radius of 2.2 cm. The ion energy distribution rapidly changes from a double-peak to a single peak in the radius range of 0.7-0.9 cm. The average ion energy is approximately uniform across the plasma column including the double-peak and single peak regions. The widths of the broad distribution, ΔE , in the <span class="hlt">wave-coupled</span> mode are large compared to the time-averaged ion energy, ⟨E ⟩. On the axis (r = 0), ΔE / ⟨E ⟩ ≲ 3.4, and at a radius near the edge of the plasma column (r = 2.2 cm), ΔE / ⟨E ⟩ ˜ 1.2. The discharge parameter space is scanned to investigate the effects of the magnetic field, input power, and chamber fill pressure on the <span class="hlt">wave-coupled</span> mode that exhibits the sharp radial variation in the ion energy distribution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014SPIE.9064E..1BB','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014SPIE.9064E..1BB"><span>Electromagnetomechanical elastodynamic <span class="hlt">model</span> for Lamb <span class="hlt">wave</span> damage quantification in composites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Borkowski, Luke; Chattopadhyay, Aditi</p> <p>2014-03-01</p> <p>Physics-based <span class="hlt">wave</span> propagation computational <span class="hlt">models</span> play a key role in structural health monitoring (SHM) and the development of improved damage quantification methodologies. Guided <span class="hlt">waves</span> (GWs), such as Lamb <span class="hlt">waves</span>, provide the capability to monitor large plate-like aerospace structures with limited actuators and sensors and are sensitive to small scale damage; however due to the complex nature of GWs, accurate and efficient computation tools are necessary to investigate the mechanisms responsible for dispersion, <span class="hlt">coupling</span>, and interaction with damage. In this paper, the local interaction simulation approach (LISA) <span class="hlt">coupled</span> with the sharp interface <span class="hlt">model</span> (SIM) solution methodology is used to solve the fully <span class="hlt">coupled</span> electro-magneto-mechanical elastodynamic equations for the piezoelectric and piezomagnetic actuation and sensing of GWs in fiber reinforced composite material systems. The final framework provides the full three-dimensional displacement as well as electrical and magnetic potential fields for arbitrary plate and transducer geometries and excitation waveform and frequency. The <span class="hlt">model</span> is validated experimentally and proven computationally efficient for a laminated composite plate. Studies are performed with surface bonded piezoelectric and embedded piezomagnetic sensors to gain insight into the physics of experimental techniques used for SHM. The symmetric collocation of piezoelectric actuators is <span class="hlt">modeled</span> to demonstrate mode suppression in laminated composites for the purpose of damage detection. The effect of delamination and damage (i.e., matrix cracking) on the GW propagation is demonstrated and quantified. The developed <span class="hlt">model</span> provides a valuable tool for the improvement of SHM techniques due to its proven accuracy and computational efficiency.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRC..122.8753V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRC..122.8753V"><span>Characterization of the Deep Water Surface <span class="hlt">Wave</span> Variability in the California <span class="hlt">Current</span> Region</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Villas Bôas, Ana B.; Gille, Sarah T.; Mazloff, Matthew R.; Cornuelle, Bruce D.</p> <p>2017-11-01</p> <p>Surface <span class="hlt">waves</span> are crucial for the dynamics of the upper ocean not only because they mediate exchanges of momentum, heat, energy, and gases between the ocean and the atmosphere, but also because they determine the sea state. The surface <span class="hlt">wave</span> field in a given region is set by the combination of local and remote forcing. The present work characterizes the seasonal variability of the deep water surface <span class="hlt">wave</span> field in the California <span class="hlt">Current</span> region, as retrieved from over two decades of satellite altimetry data combined with <span class="hlt">wave</span> buoys and <span class="hlt">wave</span> <span class="hlt">model</span> hindcast (<span class="hlt">Wave</span>Watch III). In particular, the extent to which the local wind modulates the variability of the significant <span class="hlt">wave</span> height, peak period, and peak direction is assessed. During spring/summer, regional-scale wind events of up to 10 m/s are the dominant forcing for <span class="hlt">waves</span> off the California coast, leading to relatively short-period <span class="hlt">waves</span> (8-10 s) that come predominantly from the north-northwest. The <span class="hlt">wave</span> climatology throughout the California <span class="hlt">Current</span> region shows average significant <span class="hlt">wave</span> heights exceeding 2 m during most of the year, which may have implications for the planning and retrieval methods of the Surface Water and Ocean Topography (SWOT) satellite mission.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.15703023K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.15703023K"><span>A <span class="hlt">current</span> drive by using the fast <span class="hlt">wave</span> in frequency range higher than two timeslower hybrid resonance frequency on tokamaks</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kim, Sun Ho; Hwang, Yong Seok; Jeong, Seung Ho; Wang, Son Jong; Kwak, Jong Gu</p> <p>2017-10-01</p> <p>An efficient <span class="hlt">current</span> drive scheme in central or off-axis region is required for the steady state operation of tokamak fusion reactors. The <span class="hlt">current</span> drive by using the fast <span class="hlt">wave</span> in frequency range higher than two times lower hybrid resonance (w>2wlh) could be such a scheme in high density, high temperature reactor-grade tokamak plasmas. First, it has relatively higher parallel electric field to the magnetic field favorable to the <span class="hlt">current</span> generation, compared to fast <span class="hlt">waves</span> in other frequency range. Second, it can deeply penetrate into high density plasmas compared to the slow <span class="hlt">wave</span> in the same frequency range. Third, parasitic <span class="hlt">coupling</span> to the slow <span class="hlt">wave</span> can contribute also to the <span class="hlt">current</span> drive avoiding parametric instability, thermal mode conversion and ion heating occured in the frequency range w<2wlh. In this study, the propagation boundary, accessibility, and the energy flow of the fast <span class="hlt">wave</span> are given via cold dispersion relation and group velocity. The power absorption and <span class="hlt">current</span> drive efficiency are discussed qualitatively through the hot dispersion relation and the polarization. Finally, those characteristics are confirmed with ray tracing code GENRAY for the KSTAR plasmas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.893a2057N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.893a2057N"><span><span class="hlt">Modeling</span> and simulation of ocean <span class="hlt">wave</span> propagation using lattice Boltzmann method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nuraiman, Dian</p> <p>2017-10-01</p> <p>In this paper, we present on <span class="hlt">modeling</span> and simulation of ocean <span class="hlt">wave</span> propagation from the deep sea to the shoreline. This requires high computational cost for simulation with large domain. We propose to <span class="hlt">couple</span> a 1D shallow water equations (SWE) <span class="hlt">model</span> with a 2D incompressible Navier-Stokes equations (NSE) <span class="hlt">model</span> in order to reduce the computational cost. The <span class="hlt">coupled</span> <span class="hlt">model</span> is solved using the lattice Boltzmann method (LBM) with the lattice Bhatnagar-Gross-Krook (BGK) scheme. Additionally, a special method is implemented to treat the complex behavior of free surface close to the shoreline. The result shows the <span class="hlt">coupled</span> <span class="hlt">model</span> can reduce computational cost significantly compared to the full NSE <span class="hlt">model</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010cosp...38.1270K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010cosp...38.1270K"><span>On inter-hemispheric <span class="hlt">coupling</span> in the middle atmosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Karlsson, Bodil; Bailey, S.; Benze, S.; Gumbel, J.; Harvey, V. L.; Kürnich, H.; Lossow, S.; McLandress, D. Marsh, C.; Merkel, A. W.; Mills, M.; Randall, C. E.; Russell, J.; Shepherd, T. G.</p> <p></p> <p>On inter-hemispheric <span class="hlt">coupling</span> in the middle atmosphere From recent studies it is evident that planetary <span class="hlt">wave</span> activity in the winter hemisphere influences the high-latitude summer mesosphere on the opposite side of the globe. This is an extraordinary example of multi-scale <span class="hlt">wave</span>-mean flow interaction. The first indication of this inter-hemispheric <span class="hlt">coupling</span> came from a <span class="hlt">model</span> study by Becker and Schmitz (2003). Since then, the results have been reproduced in several <span class="hlt">models</span>, and observations have confirmed the existence of this link. We present <span class="hlt">current</span> understanding of inter-hemispheric <span class="hlt">coupling</span> and its consequences for the middle atmosphere, focusing on the summer mesosphere where polar mesospheric clouds (PMCs) form. The results shown are based on year-to-year and intra-seasonal variability in PMCs ob-served by the Odin satellite and the Aeronomy of Ice in the Mesosphere (AIM) satellite, as well as on <span class="hlt">model</span> results from the extended Canadian Middle Atmosphere <span class="hlt">Model</span> (CMAM), the Whole Atmosphere Community Climate <span class="hlt">Model</span> (WACCM) and the Kühlungsborn Mechanis-u tic general Circulation <span class="hlt">Model</span> (KMCM). The latter has been used to pinpoint the proposed mechanism behind the inter-hemispheric <span class="hlt">coupling</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014OcMod..83...26L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014OcMod..83...26L"><span>Integration of coastal inundation <span class="hlt">modeling</span> from storm tides to individual <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, Ning; Roeber, Volker; Yamazaki, Yoshiki; Heitmann, Troy W.; Bai, Yefei; Cheung, Kwok Fai</p> <p>2014-11-01</p> <p><span class="hlt">Modeling</span> of storm-induced coastal inundation has primarily focused on the surge generated by atmospheric pressure and surface winds with phase-averaged effects of the <span class="hlt">waves</span> as setup. Through an interoperable <span class="hlt">model</span> package, we investigate the role of phase-resolving <span class="hlt">wave</span> processes in simulation of coastal flood hazards. A spectral ocean <span class="hlt">wave</span> <span class="hlt">model</span> describes generation and propagation of storm <span class="hlt">waves</span> from deep to intermediate water, while a non-hydrostatic storm-tide <span class="hlt">model</span> has the option to <span class="hlt">couple</span> with a spectral coastal <span class="hlt">wave</span> <span class="hlt">model</span> for computation of phase-averaged processes in a near-shore region. The ocean <span class="hlt">wave</span> and storm-tide <span class="hlt">models</span> can alternatively provide the <span class="hlt">wave</span> spectrum and the surface elevation as the boundary and initial conditions for a nested Boussinesq <span class="hlt">model</span>. Additional surface-gradient terms in the Boussinesq equations maintain the quasi-steady, non-uniform storm tide for <span class="hlt">modeling</span> of phase-resolving surf and swash-zone processes as well as combined tide, surge, and <span class="hlt">wave</span> inundation. The two nesting schemes are demonstrated through a case study of Hurricane Iniki, which made landfall on the Hawaiian Island of Kauai in 1992. With input from a parametric hurricane <span class="hlt">model</span> and global reanalysis and tidal datasets, the two approaches produce comparable significant <span class="hlt">wave</span> heights and phase-averaged surface elevations in the surf zone. The nesting of the Boussinesq <span class="hlt">model</span> provides a seamless approach to augment the inundation due to the individual <span class="hlt">waves</span> in matching the recorded debris line along the coast.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.P33C2164B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.P33C2164B"><span><span class="hlt">Modelling</span> the Auroral Magnetosphere-Ionosphere <span class="hlt">Coupling</span> System at Jupiter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bunce, E. J.; Cowley, S.; Provan, G.</p> <p>2016-12-01</p> <p>The magnetosphere-ionosphere <span class="hlt">coupling</span> system at Jupiter is a topic of central significance in understanding the fundamental properties of its large-scale plasma environment. Theoretical discussion of this topic typically considers the properties of the field-aligned <span class="hlt">current</span> systems that form part of a large-scale magnetosphere-ionosphere <span class="hlt">coupling</span> <span class="hlt">current</span> system associated with momentum exchange between the ionosphere and the magnetosphere, communicated via the magnetic field. The <span class="hlt">current</span> system associated with the main oval is believed to be related to centrifugally-driven outward radial transport of iogenic plasma that leads to sub-corotation in the middle magnetosphere. In addition to the magnetosphere-ionosphere <span class="hlt">coupling</span> <span class="hlt">current</span> system, upward-directed field-aligned <span class="hlt">currents</span> may flow at the open-closed field line boundary due to the shear between outer closed field lines and open field lines, which may relate to emission poleward of the main oval. An axi-symmetric <span class="hlt">model</span> of the plasma flow in the jovian system, the related <span class="hlt">coupling</span> <span class="hlt">currents</span>, and the consequent auroral precipitation based on these combined ideas was initially devised to represent typical steady-state conditions for the system and later extended to consider auroral effects resulting from sudden compressions of the magnetosphere. More recently, the <span class="hlt">model</span> has been extended along <span class="hlt">model</span> magnetic field lines into the magnetosphere in order to relate them to in situ observations from the NASA Juno spacecraft at Jupiter. The field-aligned <span class="hlt">coupling</span> <span class="hlt">currents</span> associated with the <span class="hlt">modelled</span> <span class="hlt">current</span> systems produce a readily-observable azimuthal field signature that bends the field lines out of magnetic meridians. Here we show the computed azimuthal fields produced by our <span class="hlt">model</span> auroral <span class="hlt">current</span> system throughout the region between the ionosphere and the magnetic equator, and illustrate the results by evaluation of various <span class="hlt">model</span> parameters (e.g. field-aligned <span class="hlt">current</span> density, accelerating voltages, accelerated</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhRvL.105z3603C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhRvL.105z3603C"><span>Deep Strong <span class="hlt">Coupling</span> Regime of the Jaynes-Cummings <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>Casanova, J.; Romero, G.; Lizuain, I.; García-Ripoll, J. J.; Solano, E.</p> <p>2010-12-01</p> <p>We study the quantum dynamics of a two-level system interacting with a quantized harmonic oscillator in the deep strong <span class="hlt">coupling</span> regime (DSC) of the Jaynes-Cummings <span class="hlt">model</span>, that is, when the <span class="hlt">coupling</span> strength g is comparable or larger than the oscillator frequency ω (g/ω≳1). In this case, the rotating-<span class="hlt">wave</span> approximation cannot be applied or treated perturbatively in general. We propose an intuitive and predictive physical frame to describe the DSC regime where photon number <span class="hlt">wave</span> packets bounce back and forth along parity chains of the Hilbert space, while producing collapse and revivals of the initial population. We exemplify our physical frame with numerical and analytical considerations in the qubit population, photon statistics, and Wigner phase space.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SMaS...26b5020R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SMaS...26b5020R"><span>Visualization of stress <span class="hlt">wave</span> propagation via air-<span class="hlt">coupled</span> acoustic emission sensors</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rivey, Joshua C.; Lee, Gil-Yong; Yang, Jinkyu; Kim, Youngkey; Kim, Sungchan</p> <p>2017-02-01</p> <p>We experimentally demonstrate the feasibility of visualizing stress <span class="hlt">waves</span> propagating in plates using air-<span class="hlt">coupled</span> acoustic emission sensors. Specifically, we employ a device that embeds arrays of microphones around an optical lens in a helical pattern. By implementing a beamforming technique, this remote sensing system allows us to record <span class="hlt">wave</span> propagation events in situ via a single-shot and full-field measurement. This is a significant improvement over the conventional <span class="hlt">wave</span> propagation tracking approaches based on laser doppler vibrometry or digital image correlation techniques. In this paper, we focus on demonstrating the feasibility and efficacy of this air-<span class="hlt">coupled</span> acoustic emission technique by using large metallic plates exposed to external impacts. The visualization results of stress <span class="hlt">wave</span> propagation will be shown under various impact scenarios. The proposed technique can be used to characterize and localize damage by detecting the attenuation, reflection, and scattering of stress <span class="hlt">waves</span> that occurs at damage locations. This can ultimately lead to the development of new structural health monitoring and nondestructive evaluation methods for identifying hidden cracks or delaminations in metallic or composite plate structures, simultaneously negating the need for mounted contact sensors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SMaS...26i4003Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SMaS...26i4003Y"><span>Enhancing power generation of floating <span class="hlt">wave</span> power generators by utilization of nonlinear roll-pitch <span class="hlt">coupling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yerrapragada, Karthik; Ansari, M. H.; Karami, M. Amin</p> <p>2017-09-01</p> <p>We propose utilization of the nonlinear <span class="hlt">coupling</span> between the roll and pitch motions of <span class="hlt">wave</span> energy harvesting vessels to increase their power generation by orders of magnitude. Unlike linear vessels that exhibit unidirectional motion, our vessel undergoes both pitch and roll motions in response to frontal <span class="hlt">waves</span>. This significantly magnifies the motion of the vessel and thus improves the power production by several orders of magnitude. The ocean <span class="hlt">waves</span> result in roll and pitch motions of the vessel, which in turn causes rotation of an onboard pendulum. The pendulum is connected to an electric generator to produce power. The <span class="hlt">coupled</span> electro-mechanical system is <span class="hlt">modeled</span> using energy methods. This paper investigates the power generation of the vessel when the ratio between pitch and roll natural frequencies is about 2 to 1. In that case, a nonlinear energy transfer occurs between the roll and pitch motions, causing the vessel to perform <span class="hlt">coupled</span> pitch and roll motion even though it is only excited in the pitch direction. It is shown that co-existence of pitch and roll motions significantly enhances the pendulum rotation and power generation. A method for tuning the natural frequencies of the vessel is proposed to make the energy generator robust to variations of the frequency of the incident <span class="hlt">waves</span>. It is shown that the proposed method enhances the power output of the floating <span class="hlt">wave</span> power generators by multiple orders of magnitude. A small-scale prototype is developed for the proof of concept. The nonlinear energy transfer and the full rotation of the pendulum in the prototype are observed in the experimental tests.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhPl...23l2504L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhPl...23l2504L"><span><span class="hlt">Current</span> drive with combined electron cyclotron <span class="hlt">wave</span> and high harmonic fast <span class="hlt">wave</span> in tokamak plasmas</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, J. C.; Gong, X. Y.; Dong, J. Q.; Wang, J.; Zhang, N.; Zheng, P. W.; Yin, C. Y.</p> <p>2016-12-01</p> <p>The <span class="hlt">current</span> driven by combined electron cyclotron <span class="hlt">wave</span> (ECW) and high harmonic fast <span class="hlt">wave</span> is investigated using the GENRAY/CQL3D package. It is shown that no significant synergetic <span class="hlt">current</span> is found in a range of cases with a combined ECW and fast <span class="hlt">wave</span> (FW). This result is consistent with a previous study [Harvey et al., in Proceedings of IAEA TCM on Fast <span class="hlt">Wave</span> <span class="hlt">Current</span> Drive in Reactor Scale Tokamaks (Synergy and Complimentarily with LHCD and ECRH), Arles, France, IAEA, Vienna, 1991]. However, a positive synergy effect does appear with the FW in the lower hybrid range of frequencies. This positive synergy effect can be explained using a picture of the electron distribution function induced by the ECW and a very high harmonic fast <span class="hlt">wave</span> (helicon). The dependence of the synergy effect on the radial position of the power deposition, the <span class="hlt">wave</span> power, the <span class="hlt">wave</span> frequency, and the parallel refractive index is also analyzed, both numerically and physically.</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.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5054169','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5054169"><span>J <span class="hlt">Wave</span> Syndromes: History and <span class="hlt">Current</span> Controversies</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Liu, Tong; Zheng, Jifeng</p> <p>2016-01-01</p> <p>The concept of J <span class="hlt">wave</span> syndromes was first proposed in 2004 by Yan et al for a spectrum of electrocardiographic (ECG) manifestations of prominent J <span class="hlt">waves</span> that are associated with a potential to predispose affected individuals to ventricular fibrillation (VF). Although the concept of J <span class="hlt">wave</span> syndromes is widely used and accepted, there has been tremendous debate over the definition of J <span class="hlt">wave</span>, its ionic and cellular basis and arrhythmogenic mechanism. In this review article, we attempted to discuss the history from which the concept of J <span class="hlt">wave</span> syndromes (JWS) is evolved and <span class="hlt">current</span> controversies in JWS. PMID:27721848</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27194962','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27194962"><span><span class="hlt">Wave</span> <span class="hlt">Modeling</span> of the Solar Wind.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ofman, Leon</p> <p></p> <p>The acceleration and heating of the solar wind have been studied for decades using satellite observations and <span class="hlt">models</span>. However, the exact mechanism that leads to solar wind heating and acceleration is poorly understood. In order to improve the understanding of the physical mechanisms that are involved in these processes a combination of <span class="hlt">modeling</span> and observational analysis is required. Recent <span class="hlt">models</span> constrained by satellite observations show that <span class="hlt">wave</span> heating in the low-frequency (MHD), and high-frequency (ion-cyclotron) range may provide the necessary momentum and heat input to coronal plasma and produce the solar wind. This review is focused on the results of several recent solar <span class="hlt">modeling</span> studies that include <span class="hlt">waves</span> explicitly in the MHD and the kinetic regime. The <span class="hlt">current</span> status of the understanding of the solar wind acceleration and heating by <span class="hlt">waves</span> is reviewed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900063521&hterms=oceans+behavior&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Doceans%2Bbehavior','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900063521&hterms=oceans+behavior&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Doceans%2Bbehavior"><span>Intraseasonal and interannual oscillations in <span class="hlt">coupled</span> ocean-atmosphere <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>Hirst, Anthony C.; Lau, K.-M.</p> <p>1990-01-01</p> <p>An investigation is presented of <span class="hlt">coupled</span> ocean-atmosphere <span class="hlt">models</span>' behavior in an environment where atmospheric <span class="hlt">wave</span> speeds are substantially reduced from dry atmospheric values by such processes as condensation-moisture convergence. Modes are calculated for zonally periodic, unbounded ocean-atmosphere systems, emphasizing the importance of an inclusion of prognostic atmosphere equations in simple <span class="hlt">coupled</span> ocean-atmosphere <span class="hlt">models</span> with a view to simulations of intraseasonal variability and its possible interaction with interannual variability. The dynamics of low and high frequency modes are compared; both classes are sensitive to the degree to which surface wind anomalies are able to affect the evaporation rate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.S21A4419A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.S21A4419A"><span>Formation of Hydro-acoustic <span class="hlt">Waves</span> in Dissipative <span class="hlt">Coupled</span> Weakly Compressible Fluids</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Abdolali, A.; Kirby, J. T., Jr.; Bellotti, G.</p> <p>2014-12-01</p> <p>Recent advances in deep sea measurement technology provide an increasing opportunity to detect and interpret hydro-acoustic <span class="hlt">waves</span> as a component in improved Tsunami Early Warning Systems (TEWS). For the idealized case of a homogeneous water column above a moving but otherwise rigid bottom (in terms of assessing acoustic <span class="hlt">wave</span> interaction), the description of the infinite family of acoustic modes is characterized by local water depth at source area; i.e. the period of the first acoustic mode is given by four times the required time for sound to travel from the seabed to the surface. Spreading off from earthquake zone, the dominant spectrum is filtered and enriched by seamounts and barriers. This study focuses on the characteristics of hydro-acoustic <span class="hlt">waves</span> generated by sudden sea bottom motion in a weakly compressible fluid <span class="hlt">coupled</span> with an underlying sedimentary layer, where the added complexity of the sediment layer rheology leads to both the lowering of dominant spectral peaks and <span class="hlt">wave</span> attenuation across the full spectrum. To overcome the computational difficulties of three-dimensional <span class="hlt">models</span>, we derive a depth integrated equation valid for varying water depth and sediment thickness. Damping behavior of the two layered system is initially taken into account by introducing the viscosity of fluid-like sedimentary layer. We show that low frequency pressure <span class="hlt">waves</span> which are precursor components of tsunamis contain information of seafloor motion.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DPPU11042C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DPPU11042C"><span>Nonlinear plasma <span class="hlt">wave</span> <span class="hlt">models</span> in 3D fluid simulations of laser-plasma interaction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chapman, Thomas; Berger, Richard; Arrighi, Bill; Langer, Steve; Banks, Jeffrey; Brunner, Stephan</p> <p>2017-10-01</p> <p>Simulations of laser-plasma interaction (LPI) in inertial confinement fusion (ICF) conditions require multi-mm spatial scales due to the typical laser beam size and durations of order 100 ps in order for numerical laser reflectivities to converge. To be computationally achievable, these scales necessitate a fluid-like treatment of light and plasma <span class="hlt">waves</span> with a spatial grid size on the order of the light <span class="hlt">wave</span> length. Plasma <span class="hlt">waves</span> experience many nonlinear phenomena not naturally described by a fluid treatment, such as frequency shifts induced by trapping, a nonlinear (typically suppressed) Landau damping, and mode <span class="hlt">couplings</span> leading to instabilities that can cause the plasma <span class="hlt">wave</span> to decay rapidly. These processes affect the onset and saturation of stimulated Raman and Brillouin scattering, and are of direct interest to the <span class="hlt">modeling</span> and prediction of deleterious LPI in ICF. It is not <span class="hlt">currently</span> computationally feasible to simulate these Debye length-scale phenomena in 3D across experimental scales. Analytically-derived and/or numerically benchmarked <span class="hlt">models</span> of processes occurring at scales finer than the fluid simulation grid offer a path forward. We demonstrate the impact of a range of kinetic processes on plasma reflectivity via <span class="hlt">models</span> included in the LPI simulation code pF3D. This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JGRC..121..410H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JGRC..121..410H"><span>The impact of <span class="hlt">wave</span>-induced Coriolis-Stokes forcing on satellite-derived ocean surface <span class="hlt">currents</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hui, Zhenli; Xu, Yongsheng</p> <p>2016-01-01</p> <p>Ocean surface <span class="hlt">currents</span> estimated from the satellite data consist of two terms: Ekman <span class="hlt">currents</span> from the wind stress and geostrophic <span class="hlt">currents</span> from the sea surface height (SSH). But the classical Ekman <span class="hlt">model</span> does not consider the <span class="hlt">wave</span> effects. By taking the <span class="hlt">wave</span>-induced Coriolis-Stokes forcing into account, the impact of <span class="hlt">waves</span> (primarily the Stokes drift) on ocean surface <span class="hlt">currents</span> is investigated and the <span class="hlt">wave</span>-modified <span class="hlt">currents</span> are formed. The products are validated by comparing with OSCAR <span class="hlt">currents</span> and Lagrangian drifter velocity. The result shows that our products with the Stokes drift are better adapted to the in situ Lagrangian drifter <span class="hlt">currents</span>. Especially in the Southern Ocean region (40°S-65°S), 90% (91%) of the zonal (meridional) <span class="hlt">currents</span> have been improved compared with <span class="hlt">currents</span> that do not include Stokes drift. The correlation (RMSE) in the Southern Ocean has also increased (decreased) from 0.78 (13) to 0.81 (10.99) for the zonal component and 0.76 (10.87) to 0.79 (10.09) for the meridional component. This finding provides the evidence that <span class="hlt">waves</span> indeed play an important role in the ocean circulation, and need to be represented in numerical simulations of the global ocean circulation. This article was corrected on 10 FEB 2016. See the end of the full text for details.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19770004351','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19770004351"><span>Radiation from a <span class="hlt">current</span> filament driven by a traveling <span class="hlt">wave</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Levine, D. M.; Meneghini, R.</p> <p>1976-01-01</p> <p>Solutions are presented for the electromagnetic fields radiated by an arbitrarily oriented <span class="hlt">current</span> filament located above a perfectly conducting ground plane and excited by a traveling <span class="hlt">current</span> <span class="hlt">wave</span>. Both an approximate solution, valid in the fraunhofer region of the filament and predicting the radiation terms in the fields, and an exact solution, which predicts both near and far field components of the electromagnetic fields, are presented. Both solutions apply to <span class="hlt">current</span> waveforms which propagate along the channel but are valid regardless of the actual waveshape. The exact solution is valid only for <span class="hlt">waves</span> which propagate at the speed of light, and the approximate solution is formulated for arbitrary velocity of propagation. The spectrum-magnitude of the fourier transform-of the radiated fields is computed by assuming a compound exponential <span class="hlt">model</span> for the <span class="hlt">current</span> waveform. The effects of channel orientation and length, as well as velocity of propagation of the <span class="hlt">current</span> waveform and location of the observer, are discussed. It is shown that both velocity of propagation and an effective channel length are important in determining the shape of the spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvA..97d0701Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvA..97d0701Z"><span>Universal relations for spin-orbit-<span class="hlt">coupled</span> Fermi gas near an s -<span class="hlt">wave</span> resonance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Pengfei; Sun, Ning</p> <p>2018-04-01</p> <p>Synthetic spin-orbit-<span class="hlt">coupled</span> quantum gases have been widely studied both experimentally and theoretically in the past decade. As shown in previous studies, this modification of single-body dispersion will in general <span class="hlt">couple</span> different partial <span class="hlt">waves</span> of the two-body scattering and thus distort the <span class="hlt">wave</span> function of few-body bound states which determines the short-distance behavior of many-body <span class="hlt">wave</span> function. In this work, we focus on the two-component Fermi gas with one-dimensional or three-dimensional spin-orbit <span class="hlt">coupling</span> (SOC) near an s -<span class="hlt">wave</span> resonance. Using the method of effective field theory and the operator product expansion, we derive universal relations for both systems, including the adiabatic theorem, viral theorem, and pressure relation, and obtain the momentum distribution matrix 〈ψa†(q ) ψb(q ) 〉 at large q (a ,b are spin indices). The momentum distribution matrix shows both spin-dependent and spatial anisotropic features. And the large momentum tail is modified at the subleading order thanks to the SOC. We also discuss the experimental implication of these results depending on the realization of the SOC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22356686-magnetoacoustic-waves-propagating-along-dense-slab-harris-current-sheet-wavelet-spectra','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22356686-magnetoacoustic-waves-propagating-along-dense-slab-harris-current-sheet-wavelet-spectra"><span>Magnetoacoustic <span class="hlt">waves</span> propagating along a dense slab and Harris <span class="hlt">current</span> sheet and their wavelet spectra</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>Mészárosová, Hana; Karlický, Marian; Jelínek, Petr</p> <p></p> <p><span class="hlt">Currently</span>, there is a common endeavor to detect magnetoacoustic <span class="hlt">waves</span> in solar flares. This paper contributes to this topic using an approach of numerical simulations. We studied a spatial and temporal evolution of impulsively generated fast and slow magnetoacoustic <span class="hlt">waves</span> propagating along the dense slab and Harris <span class="hlt">current</span> sheet using two-dimensional magnetohydrodynamic numerical <span class="hlt">models</span>. <span class="hlt">Wave</span> signals computed in numerical <span class="hlt">models</span> were used for computations of the temporal and spatial wavelet spectra for their possible comparison with those obtained from observations. It is shown that these wavelet spectra allow us to estimate basic parameters of waveguides and perturbations. It was foundmore » that the wavelet spectra of <span class="hlt">waves</span> in the dense slab and <span class="hlt">current</span> sheet differ in additional wavelet components that appear in association with the main tadpole structure. These additional components are new details in the wavelet spectrum of the signal. While in the dense slab this additional component is always delayed after the tadpole head, in the <span class="hlt">current</span> sheet this component always precedes the tadpole head. It could help distinguish a type of the waveguide in observed data. We present a technique based on wavelets that separates <span class="hlt">wave</span> structures according to their spatial scales. This technique shows not only how to separate the magnetoacoustic <span class="hlt">waves</span> and waveguide structure in observed data, where the waveguide structure is not known, but also how propagating magnetoacoustic <span class="hlt">waves</span> would appear in observations with limited spatial resolutions. The possibilities detecting these <span class="hlt">waves</span> in observed data are mentioned.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20110013511&hterms=bats&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dbats','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20110013511&hterms=bats&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dbats"><span>Dynamics of Ring <span class="hlt">Current</span> and Electric Fields in the Inner Magnetosphere During Disturbed Periods: CRCM-BATS-R-US <span class="hlt">Coupled</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>Buzulukova, N.; Fok, M.-C.; Pulkkinen, A.; Kuznetsova, M.; Moore, T. E.; Glocer, A.; Brandt, P. C.; Toth, G.; Rastaetter, L.</p> <p>2010-01-01</p> <p>We present simulation results from a one-way <span class="hlt">coupled</span> global MHD <span class="hlt">model</span> (Block-Adaptive-Tree Solar-Wind Roe-Type Upwind Scheme, BATS-R-US) and kinetic ring <span class="hlt">current</span> <span class="hlt">models</span> (Comprehensive Ring <span class="hlt">Current</span> <span class="hlt">Model</span>, CRCM, and Fok Ring <span class="hlt">Current</span>, FokRC). The BATS-R-US provides the CRCM/FokRC with magnetic field information and plasma density/temperature at the polar CRCM/FokRC boundary. The CRCM uses an electric potential from the BATS-R-US ionospheric solver at the polar CRCM boundary in order to calculate the electric field pattern consistent with the CRCM pressure distribution. The FokRC electric field potential is taken from BATS-R-US ionospheric solver everywhere in the <span class="hlt">modeled</span> region, and the effect of Region II <span class="hlt">currents</span> is neglected. We show that for an idealized case with southward-northward-southward Bz IMF turning, CRCM-BATS-R-US reproduces well known features of inner magnetosphere electrodynamics: strong/weak convection under the southward/northward Bz; electric field shielding/overshielding/penetration effects; an injection during the substorm development; Subauroral Ion Drift or Polarization Jet (SAID/PJ) signature in the dusk sector. Furthermore, we find for the idealized case that SAID/PJ forms during the substorm growth phase, and that substorm injection has its own structure of field-aligned <span class="hlt">currents</span> which resembles a substorm <span class="hlt">current</span> wedge. For an actual event (12 August 2000 storm), we calculate ENA emissions and compare with Imager for Magnetopause-to-Aurora Global Exploration/High Energy Neutral Atom data. The CRCM-BATS-R-US reproduces both the global morphology of ring <span class="hlt">current</span> and the fine structure of ring <span class="hlt">current</span> injection. The FokRC-BATS-R-US shows the effect of a realistic description of Region II <span class="hlt">currents</span> in ring <span class="hlt">current</span>-MHD <span class="hlt">coupled</span> <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26871105','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26871105"><span>Inducing rostrum interfacial <span class="hlt">waves</span> by fluid-solid <span class="hlt">coupling</span> in a Chinese river dolphin (Lipotesvexillifer).</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Song, Zhongchang; Zhang, Yu; Wei, Chong; Wang, Xianyan</p> <p>2016-01-01</p> <p>Through numerically solving the appropriate <span class="hlt">wave</span> equations, propagation of biosonar signals in a Chinese river dolphin (baiji) was studied. The interfacial <span class="hlt">waves</span> along the rostrum-tissue interfaces, including both compressional (longitudinal) and shear (transverse) <span class="hlt">waves</span> in the solid rostrum through fluid-solid <span class="hlt">coupling</span> were examined. The baiji's rostrum was found to effect acoustic beam formation not only as an interfacial <span class="hlt">wave</span> generator but also as a sound reflector. The <span class="hlt">wave</span> propagation patterns in the solid rostrum were found to significantly change the <span class="hlt">wave</span> movement through the bone. Vibrations in the rostrum, expressed in solid displacement, initially increased but eventually decreased from posterior to anterior sides, indicating a complex physical process. Furthermore, the comparisons among seven cases, including the combination of (1) the rostrum, melon, and air sacs; (2) rostrum-air sacs; (3) rostrum-melon; (4) only rostrum; (5) air sacs-melon; (6) only air sacs; and (7) only melon revealed that the cases including the rostrum were better able to approach the complete system by inducing rostrum-tissue interfacial <span class="hlt">waves</span> and reducing the differences in main beam angle and -3 dB beam width. The interfacial <span class="hlt">waves</span> in the rostrum were considered complementary with reflection to determine the obbligato role of the rostrum in the baiji's biosonar emission. The far-field beams formed from complete fluid-solid <span class="hlt">models</span> and non-fluid-solid <span class="hlt">models</span> were compared to reveal the effects brought by the consideration of shear <span class="hlt">waves</span> of the solid structures of the baiji. The results may provide useful information for further understanding the role of the rostrum in this odontocete species.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005JCli...18.1449C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005JCli...18.1449C"><span>Indian Ocean Dipolelike Variability in the CSIRO Mark 3 <span class="hlt">Coupled</span> Climate <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>Cai, Wenju; Hendon, Harry H.; Meyers, Gary</p> <p>2005-05-01</p> <p><span class="hlt">Coupled</span> ocean-atmosphere variability in the tropical Indian Ocean is explored with a multicentury integration of the Commonwealth Scientific and Industrial Research Organisation (CSIRO) Mark 3 climate <span class="hlt">model</span>, which runs without flux adjustment. Despite the presence of some common deficiencies in this type of <span class="hlt">coupled</span> <span class="hlt">model</span>, zonal dipolelike variability is produced. During July through November, the dominant mode of variability of sea surface temperature resembles the observed zonal dipole and has out-of-phase rainfall variations across the Indian Ocean basin, which are as large as those associated with the <span class="hlt">model</span> El Niño-Southern Oscillation (ENSO). In the positive dipole phase, cold SST anomaly and suppressed rainfall south of the equator on the Sumatra-Java coast drives an anticyclonic circulation anomaly that is consistent with the steady response (Gill <span class="hlt">model</span>) to a heat sink displaced south of the equator. The northwest-southeast tilting Sumatra-Java coast results in cold sea surface temperature (SST) centered south of the equator, which forces anticylonic winds that are southeasterly along the coast, which thus produces local upwelling, cool SSTs, and promotes more anticylonic winds; on the equator, the easterlies raise the thermocline to the east via upwelling Kelvin <span class="hlt">waves</span> and deepen the off-equatorial thermocline to the west via off-equatorial downwelling Rossby <span class="hlt">waves</span>. The <span class="hlt">model</span> dipole mode exhibits little contemporaneous relationship with the <span class="hlt">model</span> ENSO; however, this does not imply that it is independent of ENSO. The <span class="hlt">model</span> dipole often (but not always) develops in the year following El Niño. It is triggered by an unrealistic transmission of the <span class="hlt">model</span>'s ENSO discharge phase through the Indonesian passages. In the <span class="hlt">model</span>, the ENSO discharge Rossby <span class="hlt">waves</span> arrive at the Sumatra-Java coast some 6 to 9 months after an El Niño peaks, causing the majority of <span class="hlt">model</span> dipole events to peak in the year after an ENSO warm event. In the observed ENSO discharge, Rossby <span class="hlt">waves</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMEP43C1898H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMEP43C1898H"><span>An Eulerian two-phase flow <span class="hlt">model</span> for sediment transport under realistic surface <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hsu, T. J.; Kim, Y.; Cheng, Z.; Chauchat, J.</p> <p>2017-12-01</p> <p><span class="hlt">Wave</span>-driven sediment transport is of major importance in driving beach morphology. However, the complex mechanisms associated with unsteadiness, free-surface effects, and <span class="hlt">wave</span>-breaking turbulence have not been fully understood. Particularly, most existing <span class="hlt">models</span> for sediment transport adopt bottom boundary layer approximation that mimics the flow condition in oscillating water tunnel (U-tube). However, it is well-known that there are key differences in sediment transport when comparing to large <span class="hlt">wave</span> flume datasets, although the number of <span class="hlt">wave</span> flume experiments are relatively limited regardless of its importance. Thus, a numerical <span class="hlt">model</span> which can resolve the entire water column from the bottom boundary layer to the free surface can be a powerful tool. This study reports an on-going effort to better understand and quantify sediment transport under shoaling and breaking surface <span class="hlt">waves</span> through the creation of open-source numerical <span class="hlt">models</span> in the OpenFOAM framework. An Eulerian two-phase flow <span class="hlt">model</span>, SedFoam (Cheng et al., 2017, Coastal Eng.) is fully <span class="hlt">coupled</span> with a volume-of-fluid solver, interFoam/<span class="hlt">waves</span>2Foam (Jacobsen et al., 2011, Int. J. Num. Fluid). The fully <span class="hlt">coupled</span> <span class="hlt">model</span>, named Sed<span class="hlt">Wave</span>Foam, regards the air and water phases as two immiscible fluids with the interfaces evolution resolved, and the sediment particles as dispersed phase. We carried out <span class="hlt">model</span>-data comparisons with the large <span class="hlt">wave</span> flume sheet flow data for nonbreaking <span class="hlt">waves</span> reported by Dohmen-Janssen and Hanes (2002, J. Geophysical Res.) and good agreements were obtained for sediment concentration and net transport rate. By further simulating a case without free-surface (mimic U-tube condition), the effects of free-surface, most notably the boundary layer streaming effect on total transport, can be quantified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013JAP...114b7010L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013JAP...114b7010L"><span>Eddy-<span class="hlt">current</span> effect on resonant magnetoelectric <span class="hlt">coupling</span> in magnetostrictive-piezoelectric laminated composites</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Liu, Guoxi; Zhang, Chunli; Chen, Weiqiu; Dong, Shuxiang</p> <p>2013-07-01</p> <p>An analytical <span class="hlt">model</span> of resonant magnetoelectric (ME) <span class="hlt">coupling</span> in magnetostrictive (MS)-piezoelectric (PE) laminated composites in consideration of eddy-<span class="hlt">current</span> effect in MS layer using equivalent circuit method is presented. Numerical calculations show that: (1) the eddy-<span class="hlt">current</span> has a strong effect on ME <span class="hlt">coupling</span> in MS-PE laminated composites at resonant frequency; and (2) the resonant ME <span class="hlt">coupling</span> is then significantly dependent on the sizes of ME laminated composites, which were neglected in most previous theoretical analyses. The achieved results provide a theoretical guidance for the practice engineering design, manufacture, and application of ME laminated composites and devices.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMOS21B1735K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMOS21B1735K"><span>Wind and <span class="hlt">Wave</span> Driven Nearshore Circulation at Cape Hatteras Point</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kumar, N.; Voulgaris, G.; Warner, J. C.; List, J. H.</p> <p>2012-12-01</p> <p>We have used a measurement and <span class="hlt">modeling</span> approach to identify hydrodynamic processes responsible for alongshore transport of sediment that can support the maintenance of Diamond Shoals, NC, a large inner-shelf sedimentary convergent feature. As a part of Carolina Coastal Change Processes project, a one month field experiment was conducted around Cape Hatteras point during February, 2010. The instrumentation consisted of 15 acoustic <span class="hlt">current</span> meters (measuring pressure and velocity profile) deployed in water depths varying from 3-10m and a very high frequency (VHF) beam forming radar system providing surface <span class="hlt">waves</span> and <span class="hlt">currents</span> with a resolution of 150 m and a spatial coverage of 10-15 km2. Analysis of field observation suggests that wind-driven circulation and littoral <span class="hlt">current</span> dominate surf zone and inner shelf processes at least at an order higher than tidally rectified flows. However, the data analysis identified that relevant processes like non-linear advective acceleration, pressure gradient and vortex-force (due to interaction between <span class="hlt">wave</span>-induced drift and mean flow vorticity), may be significant, but were not assessed accurately due to instrument location and accuracy. To obtain a deeper physical understanding of the hydrodynamics in this study-site, we applied a three-dimensional <span class="hlt">Coupled-Ocean-Atmosphere-Wave</span>_Sediment-Transport (COAWST) numerical <span class="hlt">model</span>. The COAWST <span class="hlt">modeling</span> system is comprised of nested, <span class="hlt">coupled</span>, three-dimensional ocean-circulation <span class="hlt">model</span> (ROMS) and <span class="hlt">wave</span> propagation <span class="hlt">model</span> (SWAN), configured for the study site to simulate <span class="hlt">wave</span> height, direction, period and mean <span class="hlt">current</span> velocities (both Eulerian and Lagrangian). The nesting follows a two-way grid refinement process for the circulation module, and one-way for the <span class="hlt">wave</span> <span class="hlt">model</span>. The coarsest parent grid resolved processes on the spatial and temporal scales of mid-shelf to inner-shelf, and subsequent child grids evolved at inner-shelf and surf zone scales. Preliminary results show that the <span class="hlt">model</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFD.A5003D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFD.A5003D"><span><span class="hlt">Coupled</span> 0D-1D CFD <span class="hlt">Modeling</span> of Right Heart and Pulmonary Artery Morphometry Tree</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dong, Melody; Yang, Weiguang; Feinstein, Jeffrey A.; Marsden, Alison</p> <p>2017-11-01</p> <p>Pulmonary arterial hypertension (PAH) is characterized by elevated pulmonary artery (PA) pressure and remodeling of the distal PAs resulting in right ventricular (RV) dysfunction and failure. It is hypothesized that patients with untreated ventricular septal defects (VSD) may develop PAH due to elevated flows and pressures in the PAs. Wall shear stress (WSS), due to elevated flows, and circumferential stress, due to elevated pressures, are known to play a role in vascular mechanobiology. Thus, simulating VSD hemodynamics and wall mechanics may facilitate our understanding of mechanical stimuli leading to PAH initiation and progression. Although 3D CFD <span class="hlt">models</span> can capture detailed hemodynamics in the proximal PAs, they cannot easily <span class="hlt">model</span> hemodynamics and <span class="hlt">wave</span> propagation in the distal PAs, where remodeling occurs. To improve <span class="hlt">current</span> PA <span class="hlt">models</span>, we will present a new method that <span class="hlt">couples</span> distal PA hemodynamics with RV function. Our <span class="hlt">model</span> <span class="hlt">couples</span> a 0D lumped parameter <span class="hlt">model</span> of the RV to a 1D <span class="hlt">model</span> of the PA tree, based on human PA morphometry data, to characterize RV performance and WSS changes in the PA tree. We will compare a VSD 0D-1D <span class="hlt">model</span> and a 0D-3D <span class="hlt">model</span> <span class="hlt">coupled</span> to a mathematical morphometry tree <span class="hlt">model</span> to quantify WSS in the entire PA vascular tree.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..1413510O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..1413510O"><span>Interfacial <span class="hlt">waves</span> generated by gravity <span class="hlt">currents</span> in two-layer fluid.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>O'Leary, A.; Parker, D.; Peakall, J.; Ross, A.; Knippertz, P.; Marsham, J.</p> <p>2012-04-01</p> <p>The mesoscale convective systems of the West African Monsoon have a huge energetic impact on the surrounding environment. Energy is radiated away from these systems by internal <span class="hlt">waves</span> formed by the vigorous movements of air mass at their core, propagating over long range in the existence of a suitable waveguide. Gravity <span class="hlt">currents</span> formed by convective downdrafts are an exceedlingly common phenomenon around the monsoon, covering significant distances on the continental scale. The initiation of solitary <span class="hlt">waves</span> and bores by gravity <span class="hlt">currents</span> incident on a marine or nocturnal inversion is well documented, the Morning Glory of Northern Australia being a well known and spectacular example. The interior of the African continent exhibits a further mechanism for the propagation of <span class="hlt">wave</span> energy, with the environment of the Sahara often characterised by a deep convective boundary layer topped by a well mixed residual layer. This suggests a simple laboratory analogy for the idealised study of deep moist convection at the edge of the monsoon; that of a gravity <span class="hlt">current</span> generated by lock release into a two layer fluid. This work looks specifically at the <span class="hlt">waves</span> generated on the interface, especially with regard to their amplitude and propagation speed relative to the <span class="hlt">current</span>. A series of simple experiments have been performed in the laboratory and combined with data from previous work. In addition to improving the basic dynamical understanding of the idealised problem the aim of these experiments is to examine whether there exist regions in the bulk parameter space in which <span class="hlt">waves</span> are generated that are fast and of large amplitude. That is, were this an appropriate analog for the atmosphere, under which conditions are <span class="hlt">waves</span> produced that would favour the initiation of subsequent convection? Ultimately this work aims to bring together research from fluid dynamics, field observations and numerical <span class="hlt">modelling</span> to explore the phenomena of the convective environment of the Sahel. This</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SMaS...27d5014R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SMaS...27d5014R"><span><span class="hlt">Modeling</span> guided <span class="hlt">wave</span> excitation in plates with surface mounted piezoelectric elements: <span class="hlt">coupled</span> physics and normal mode expansion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ren, Baiyang; Lissenden, Cliff J.</p> <p>2018-04-01</p> <p>Guided <span class="hlt">waves</span> have been extensively studied and widely used for structural health monitoring because of their large volumetric coverage and good sensitivity to defects. Effectively and preferentially exciting a desired <span class="hlt">wave</span> mode having good sensitivity to a certain defect is of great practical importance. Piezoelectric discs and plates are the most common types of surface-mounted transducers for guided <span class="hlt">wave</span> excitation and reception. Their geometry strongly influences the proportioning between excited modes as well as the total power of the excited modes. It is highly desirable to predominantly excite the selected mode while the total transduction power is maximized. In this work, a fully <span class="hlt">coupled</span> multi-physics finite element analysis, which incorporates the driving circuit, the piezoelectric element and the <span class="hlt">wave</span> guide, is combined with the normal mode expansion method to study both the mode tuning and total <span class="hlt">wave</span> power. The excitation of circular crested <span class="hlt">waves</span> in an aluminum plate with circular piezoelectric discs is numerically studied for different disc and adhesive thicknesses. Additionally, the excitation of plane <span class="hlt">waves</span> in an aluminum plate, using a stripe piezoelectric element is studied both numerically and experimentally. It is difficult to achieve predominant single mode excitation as well as maximum power transmission simultaneously, especially for higher order modes. However, guidelines for designing the geometry of piezoelectric elements for optimal mode excitation are recommended.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ZNatA..72.1053X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ZNatA..72.1053X"><span>Localised Nonlinear <span class="hlt">Waves</span> in the Three-Component <span class="hlt">Coupled</span> Hirota Equations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Tao; Chen, Yong</p> <p>2017-10-01</p> <p>We construct the Lax pair and Darboux transformation for the three-component <span class="hlt">coupled</span> Hirota equations including higher-order effects such as third-order dispersion, self-steepening, and stimulated Raman scattering. A special vector solution of the Lax pair with 4×4 matrices for the three-component Hirota system is elaborately generated, based on this vector solution, various types of mixed higher-order localised <span class="hlt">waves</span> are derived through the generalised Darboux transformation. Instead of considering various arrangements of the three potential functions q1, q2, and q3, here, the same combination is considered as the same type solution. The first- and second-order localised <span class="hlt">waves</span> are mainly discussed in six mixed types: (1) the hybrid solutions degenerate to the rational ones and three components are all rogue <span class="hlt">waves</span>; (2) two components are hybrid solutions between rogue <span class="hlt">wave</span> (RW) and breather (RW+breather), and one component is interactional solution between RW and dark soliton (RW+dark soliton); (3) two components are RW+dark soliton, and one component is RW+bright soliton; (4) two components are RW+breather, and one component is RW+bright soliton; (5) two components are RW+dark soliton, and one component is RW+bright soliton; (6) three components are all RW+breather. Moreover, these nonlinear localised <span class="hlt">waves</span> merge with each other by increasing the absolute values of two free parameters α, β. These results further uncover some striking dynamic structures in the multicomponent <span class="hlt">coupled</span> system.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM21B..08J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM21B..08J"><span>Investigating EMIC <span class="hlt">Wave</span> Dynamics with RAM-SCB-E</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jordanova, V. K.; Fu, X.; Henderson, M. G.; Morley, S.; Welling, D. T.; Yu, Y.</p> <p>2017-12-01</p> <p>The distribution of ring <span class="hlt">current</span> ions and electrons in the inner magnetosphere depends strongly on their transport in realistic electric (E) and magnetic (B) fields and concurrent energization or loss. To investigate the high variability of energetic particle (H+, He+, O+, and electron) fluxes during storms selected by the GEM Surface Charging Challenge, we use our kinetic ring <span class="hlt">current</span> <span class="hlt">model</span> (RAM) two-way <span class="hlt">coupled</span> with a 3-D magnetic field code (SCB). This <span class="hlt">model</span> was just extended to include electric field calculations, making it a unique, fully self-consistent, anisotropic ring <span class="hlt">current</span>-atmosphere interactions <span class="hlt">model</span>, RAM-SCB-E. Recently we investigated electromagnetic ion cyclotron (EMIC) instability in a local plasma using both linear theory and nonlinear hybrid simulations and derived a scaling formula that relates the saturation EMIC <span class="hlt">wave</span> amplitude to initial plasma conditions. Global dynamic EMIC <span class="hlt">wave</span> maps obtained with our RAM-SCB-E <span class="hlt">model</span> using this scaling will be presented and compared with statistical <span class="hlt">models</span>. These plasma <span class="hlt">waves</span> can affect significantly both ion and electron precipitation into the atmosphere and the subsequent patterns of ionospheric conductance, as well as the global ring <span class="hlt">current</span> dynamics.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19950031117&hterms=recruitment&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Drecruitment','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19950031117&hterms=recruitment&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Drecruitment"><span><span class="hlt">Wave-current</span> interaction study in the Gulf of Alaska for detection of eddies by synthetic aperture radar</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.; Peng, Chich Y.; Schumacher, James D.</p> <p>1994-01-01</p> <p>High resolution Esa Remote Sensing Satellite-1 (ERS-1) Synthetic Aperture Radar (SAR) images are used to detect a mesoscale eddy. Such features limit dispersal of pollock larvae and therefore likely influence recruitment of fish in the Gulf of Alaska. During high sea states and high winds, the direct surface signature of the eddy was not clearly visible, but the <span class="hlt">wave</span> refraction in the eddy area was observed. The rays of the <span class="hlt">wave</span> field are traced out directly from the SAR image. The ray pattern gives information on the refraction pattern and on the relative variation of the <span class="hlt">wave</span> energy along a ray through <span class="hlt">wave</span> <span class="hlt">current</span> interaction. These observations are simulated by a ray-tracing <span class="hlt">model</span> which incorporates a surface <span class="hlt">current</span> field associated with the eddy. The numerical results of the <span class="hlt">model</span> show that the <span class="hlt">waves</span> are refracted and diverge in the eddy field with energy density decreasing. The <span class="hlt">model</span>-data comparison for each ray shows the <span class="hlt">model</span> predictions are in good agreement with the SAR data.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/18545312','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/18545312"><span><span class="hlt">Coupling</span> of free space sub-terahertz <span class="hlt">waves</span> into dielectric slabs using PC waveguides.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ghattan, Z; Hasek, T; Shahabadi, M; Koch, M</p> <p>2008-04-28</p> <p>The paper presents theoretical and experimental results on photonic crystal structures which work under the self-collimation condition to <span class="hlt">couple</span> free space <span class="hlt">waves</span> into dielectric slabs in the sub-terahertz range. Using a standard machining process, two-dimensional photonic crystal structures consisting of a square array of air holes in the dielectric medium are fabricated. One of the structures has two adjacent parallel line-defects that improve the <span class="hlt">coupling</span> efficiency. This leads to a combination of self-collimation and directional emission of electromagnetic <span class="hlt">waves</span>. The experimental results are in good agreement with those of the Finite- Element-Method calculations. Experimentally we achieve a <span class="hlt">coupling</span> efficiency of 63%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19900055529&hterms=Wave+Energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DWave%2BEnergy','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19900055529&hterms=Wave+Energy&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DWave%2BEnergy"><span><span class="hlt">Current</span>-driven plasma acceleration versus <span class="hlt">current</span>-driven energy dissipation. I - <span class="hlt">Wave</span> stability theory</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kelly, A. J.; Jahn, R. G.; Choueiri, E. Y.</p> <p>1990-01-01</p> <p>The dominant unstable electrostatic <span class="hlt">wave</span> modes of an electromagnetically accelerated plasma are investigated. The study is the first part of a three-phase program aimed at characterizing the <span class="hlt">current</span>-driven turbulent dissipation degrading the efficiency of Lorentz force plasma accelerators such as the MPD thruster. The analysis uses a kinetic theory that includes magnetic and thermal effects as well as those of an electron <span class="hlt">current</span> transverse to the magnetic field and collisions, thus combining all the features of previous <span class="hlt">models</span>. Analytical and numerical solutions allow a detailed description of threshold criteria, finite growth behavior, destabilization mechanisms and maximized-growth characteristics of the dominant unstable modes. The lower hybrid <span class="hlt">current</span>-driven instability is implicated as dominant and was found to preserve its character in the collisional plasma regime.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017APS..DFDM26007A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDM26007A"><span>A fast wind-farm boundary-layer <span class="hlt">model</span> to investigate gravity <span class="hlt">wave</span> effects and upstream flow deceleration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Allaerts, Dries; Meyers, Johan</p> <p>2017-11-01</p> <p>Wind farm design and control often relies on fast analytical wake <span class="hlt">models</span> to predict turbine wake interactions and associated power losses. Essential input to these <span class="hlt">models</span> are the inflow velocity and turbulent intensity at hub height, which come from prior measurement campaigns or wind-atlas data. Recent LES studies showed that in some situations large wind farms excite atmospheric gravity <span class="hlt">waves</span>, which in turn affect the upstream wind conditions. In the <span class="hlt">current</span> study, we develop a fast boundary-layer <span class="hlt">model</span> that computes the excitation of gravity <span class="hlt">waves</span> and the perturbation of the boundary-layer flow in response to an applied force. The core of the <span class="hlt">model</span> is constituted by height-averaged, linearised Navier-Stokes equations for the inner and outer layer, and the effect of atmospheric gravity <span class="hlt">waves</span> (excited by the boundary-layer displacement) is included via the pressure gradient. <span class="hlt">Coupling</span> with analytical wake <span class="hlt">models</span> allows us to study wind-farm wakes and upstream flow deceleration in various atmospheric conditions. Comparison with wind-farm LES results shows excellent agreement in terms of pressure and boundary-layer displacement levels. The authors acknowledge support from the European Research Council (FP7-Ideas, Grant No. 306471).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRC..117.6007S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRC..117.6007S"><span>Turbidity <span class="hlt">current</span> flow over an erodible obstacle and phases of sediment <span class="hlt">wave</span> generation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Strauss, Moshe; Glinsky, Michael E.</p> <p>2012-06-01</p> <p>We study the flow of particle-laden turbidity <span class="hlt">currents</span> down a slope and over an obstacle. A high-resolution 2-D computer simulation <span class="hlt">model</span> is used, based on the Navier-Stokes equations. It includes poly-disperse particle grain sizes in the <span class="hlt">current</span> and substrate. Particular attention is paid to the erosion and deposition of the substrate particles, including application of an active layer <span class="hlt">model</span>. Multiple flows are <span class="hlt">modeled</span> from a lock release that can show the development of sediment <span class="hlt">waves</span> (SW). These are stream-wise <span class="hlt">waves</span> that are triggered by the increasing slope on the downstream side of the obstacle. The initial obstacle is completely erased by the resuspension after a few flows leading to self consistent and self generated SW that are weakly dependant on the initial obstacle. The growth of these <span class="hlt">waves</span> is directly related to the turbidity <span class="hlt">current</span> being self sustaining, that is, the net erosion is more than the net deposition. Four system parameters are found to influence the SW growth: (1) slope, (2) <span class="hlt">current</span> lock height, (3) grain lock concentration, and (4) particle diameters. Three phases are discovered for the system: (1) "no SW," (2) "SW buildup," and (3) "SW growth". The second phase consists of a soliton-like SW structure with a preserved shape. The phase diagram of the system is defined by isolating regions divided by critical slope angles as functions of <span class="hlt">current</span> lock height, grain lock concentration, and particle diameters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20867308','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20867308"><span>Observation of beat oscillation generation by <span class="hlt">coupled</span> <span class="hlt">waves</span> associated with parametric decay during radio frequency <span class="hlt">wave</span> heating of a spherical tokamak plasma.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nagashima, Yoshihiko; Oosako, Takuya; Takase, Yuichi; Ejiri, Akira; Watanabe, Osamu; Kobayashi, Hiroaki; Adachi, Yuuki; Tojo, Hiroshi; Yamaguchi, Takashi; Kurashina, Hiroki; Yamada, Kotaro; An, Byung Il; Kasahara, Hiroshi; Shimpo, Fujio; Kumazawa, Ryuhei; Hayashi, Hiroyuki; Matsuzawa, Haduki; Hiratsuka, Junichi; Hanashima, Kentaro; Kakuda, Hidetoshi; Sakamoto, Takuya; Wakatsuki, Takuma</p> <p>2010-06-18</p> <p>We present an observation of beat oscillation generation by <span class="hlt">coupled</span> modes associated with parametric decay instability (PDI) during radio frequency (rf) <span class="hlt">wave</span> heating experiments on the Tokyo Spherical Tokamak-2. Nearly identical PDI spectra, which are characterized by the coexistence of the rf pump <span class="hlt">wave</span>, the lower-sideband <span class="hlt">wave</span>, and the low-frequency oscillation in the ion-cyclotron range of frequency, are observed at various locations in the edge plasma. A bispectral power analysis was used to experimentally discriminate beat oscillation from the resonant mode for the first time. The pump and lower-sideband <span class="hlt">waves</span> have resonant mode components, while the low-frequency oscillation is exclusively excited by nonlinear <span class="hlt">coupling</span> of the pump and lower-sideband <span class="hlt">waves</span>. Newly discovered nonlocal transport channels in spectral space and in real space via PDI are described.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005NucFu..45.1510L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005NucFu..45.1510L"><span><span class="hlt">Modelling</span> of minority ion cyclotron <span class="hlt">current</span> drive during the activated phase of ITER</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Laxåback, M.; Hellsten, T.</p> <p>2005-12-01</p> <p>Neoclassical tearing modes, triggered by the long-period sawteeth expected in tokamaks with large non-thermal α-particle populations, may impose a severe β limit on experiments with large fusion yields and on reactors. Sawtooth destabilization by localized <span class="hlt">current</span> drive could relax the β limit and improve plasma performance. 3He minority ion cyclotron <span class="hlt">current</span> drive around the sawtooth inversion radius has been planned for ITER. Several ion species, including beam injected D ions and fusion born α particles, are however also resonant in the plasma and may represent a parasitic absorption of RF power. <span class="hlt">Modelling</span> of minority ion cyclotron <span class="hlt">current</span> drive in an ITER-FEAT-like plasma is presented, including the effects of ion trapping, finite ion drift orbit widths, <span class="hlt">wave</span>-induced radial transport and the <span class="hlt">coupled</span> evolution of <span class="hlt">wave</span> fields and resonant ion distributions. The parasitic absorption of RF power by the other resonant species is concluded to be relatively small, but the 3He minority <span class="hlt">current</span> drive is nevertheless negligible due to the strong collisionality of the 3He ions and the drag <span class="hlt">current</span> by toroidally counter-rotating background ions and co-rotating electrons. H minority <span class="hlt">current</span> drive is found to be a significantly more effective alternative.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016RSPSA.47260715R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016RSPSA.47260715R"><span>Hydroelectromechanical <span class="hlt">modelling</span> of a piezoelectric <span class="hlt">wave</span> energy converter</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Renzi, E.</p> <p>2016-11-01</p> <p>We investigate the hydroelectromechanical-<span class="hlt">coupled</span> dynamics of a piezoelectric <span class="hlt">wave</span> energy converter. The converter is made of a flexible bimorph plate, clamped at its ends and forced to motion by incident ocean surface <span class="hlt">waves</span>. The piezoceramic layers are connected in series and transform the elastic motion of the plate into useful electricity by means of the piezoelectric effect. By using a distributed-parameter analytical approach, we <span class="hlt">couple</span> the linear piezoelectric constitutive equations for the plate with the potential-flow equations for the surface water <span class="hlt">waves</span>. The resulting system of governing partial differential equations yields a new hydroelectromechanical dispersion relation, whose complex roots are determined with a numerical approach. The effect of the piezoelectric <span class="hlt">coupling</span> in the hydroelastic domain generates a system of short- and long-crested weakly damped progressive <span class="hlt">waves</span> travelling along the plate. We show that the short-crested flexural <span class="hlt">wave</span> component gives a dominant contribution to the generated power. We determine the hydroelectromechanical resonant periods of the device, at which the power output is significant.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1914458S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1914458S"><span>Effects of <span class="hlt">wave</span>-induced forcing on a circulation <span class="hlt">model</span> of the North Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Staneva, Joanna; Alari, Victor; Breivik, Øyvind; Bidlot, Jean-Raymond; Mogensen, Kristian</p> <p>2017-04-01</p> <p>The effect of wind <span class="hlt">waves</span> on water level and <span class="hlt">currents</span> during two storms in the North Sea is investigated using a high-resolution NEMO <span class="hlt">model</span> forced with fluxes and fields from a high-resolution <span class="hlt">wave</span> <span class="hlt">model</span>. The additional terms accounting for <span class="hlt">wave-current</span> interaction that are considered in this study are the Stokes-Coriolis force and the sea-state dependent energy and momentum fluxes. The individual and collective role of these processes is quantified and the results are compared with a control run without <span class="hlt">wave</span> effects as well as against <span class="hlt">current</span> and water level measurements from coastal stations. We find a better agreement with observations when the circulation <span class="hlt">model</span> is forced by sea-state dependent fluxes, especially in extreme events. The two extreme events, the storm Christian (25-27 October 2013), and about a month later, the storm Xaver (5-7 December 2013), induce different <span class="hlt">wave</span> and surge conditions over the North Sea. Including the <span class="hlt">wave</span> effects in the circulation <span class="hlt">model</span> for the storm Xaver raises the <span class="hlt">modelled</span> surge by more than 40 cm compared with the control run in the German Bight area. For the storm Christian, a difference of 20-30 cm in the surge level between the <span class="hlt">wave</span>-forced and the stand-alone ocean <span class="hlt">model</span> is found over the whole southern part of the North Sea. Moreover, the <span class="hlt">modelled</span> vertical velocity profile fits the observations very well when the <span class="hlt">wave</span> forcing is accounted for. The contribution of <span class="hlt">wave</span>-induced forcing has been quantified indicating that this represents an important mechanism for improving water level and <span class="hlt">current</span> predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSHI51A..03Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSHI51A..03Y"><span>A test-bed <span class="hlt">modeling</span> study for <span class="hlt">wave</span> resource assessment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Yang, Z.; Neary, V. S.; Wang, T.; Gunawan, B.; Dallman, A.</p> <p>2016-02-01</p> <p>Hindcasts from phase-averaged <span class="hlt">wave</span> <span class="hlt">models</span> are commonly used to estimate standard statistics used in <span class="hlt">wave</span> energy resource assessments. However, the research community and <span class="hlt">wave</span> energy converter industry is lacking a well-documented and consistent <span class="hlt">modeling</span> approach for conducting these resource assessments at different phases of WEC project development, and at different spatial scales, e.g., from small-scale pilot study to large-scale commercial deployment. Therefore, it is necessary to evaluate <span class="hlt">current</span> <span class="hlt">wave</span> <span class="hlt">model</span> codes, as well as limitations and knowledge gaps for predicting sea states, in order to establish best <span class="hlt">wave</span> <span class="hlt">modeling</span> practices, and to identify future research needs to improve <span class="hlt">wave</span> prediction for resource assessment. This paper presents the first phase of an on-going <span class="hlt">modeling</span> study to address these concerns. The <span class="hlt">modeling</span> study is being conducted at a test-bed site off the Central Oregon Coast using two of the most widely-used third-generation <span class="hlt">wave</span> <span class="hlt">models</span> - <span class="hlt">Wave</span>WatchIII and SWAN. A nested-grid <span class="hlt">modeling</span> approach, with domain dimension ranging from global to regional scales, was used to provide <span class="hlt">wave</span> spectral boundary condition to a local scale <span class="hlt">model</span> domain, which has a spatial dimension around 60km by 60km and a grid resolution of 250m - 300m. <span class="hlt">Model</span> results simulated by <span class="hlt">Wave</span>WatchIII and SWAN in a structured-grid framework are compared to NOAA <span class="hlt">wave</span> buoy data for the six <span class="hlt">wave</span> parameters, including omnidirectional <span class="hlt">wave</span> power, significant <span class="hlt">wave</span> height, energy period, spectral width, direction of maximum directionally resolved <span class="hlt">wave</span> power, and directionality coefficient. <span class="hlt">Model</span> performance and computational efficiency are evaluated, and the best practices for <span class="hlt">wave</span> resource assessments are discussed, based on a set of standard error statistics and <span class="hlt">model</span> run times.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3762734','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3762734"><span>Spiral-<span class="hlt">Wave</span> Dynamics in a Mathematical <span class="hlt">Model</span> of Human Ventricular Tissue with Myocytes and Fibroblasts</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Nayak, Alok Ranjan; Shajahan, T. K.; Panfilov, A. V.; Pandit, Rahul</p> <p>2013-01-01</p> <p>Cardiac fibroblasts, when <span class="hlt">coupled</span> functionally with myocytes, can modulate the electrophysiological properties of cardiac tissue. We present systematic numerical studies of such modulation of electrophysiological properties in mathematical <span class="hlt">models</span> for (a) single myocyte-fibroblast (MF) units and (b) two-dimensional (2D) arrays of such units; our <span class="hlt">models</span> build on earlier ones and allow for zero-, one-, and two-sided MF <span class="hlt">couplings</span>. Our studies of MF units elucidate the dependence of the action-potential (AP) morphology on parameters such as , the fibroblast resting-membrane potential, the fibroblast conductance , and the MF gap-junctional <span class="hlt">coupling</span> . Furthermore, we find that our MF composite can show autorhythmic and oscillatory behaviors in addition to an excitable response. Our 2D studies use (a) both homogeneous and inhomogeneous distributions of fibroblasts, (b) various ranges for parameters such as , and , and (c) intercellular <span class="hlt">couplings</span> that can be zero-sided, one-sided, and two-sided connections of fibroblasts with myocytes. We show, in particular, that the plane-<span class="hlt">wave</span> conduction velocity decreases as a function of , for zero-sided and one-sided <span class="hlt">couplings</span>; however, for two-sided <span class="hlt">coupling</span>, decreases initially and then increases as a function of , and, eventually, we observe that conduction failure occurs for low values of . In our homogeneous studies, we find that the rotation speed and stability of a spiral <span class="hlt">wave</span> can be controlled either by controlling or . Our studies with fibroblast inhomogeneities show that a spiral <span class="hlt">wave</span> can get anchored to a local fibroblast inhomogeneity. We also study the efficacy of a low-amplitude control scheme, which has been suggested for the control of spiral-<span class="hlt">wave</span> turbulence in mathematical <span class="hlt">models</span> for cardiac tissue, in our MF <span class="hlt">model</span> both with and without heterogeneities. PMID:24023798</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://archives.datapages.com/data/gcags/data/047/047001/0529.htm','USGSPUBS'); return false;" href="http://archives.datapages.com/data/gcags/data/047/047001/0529.htm"><span><span class="hlt">Modeling</span> <span class="hlt">waves</span> and circulation in Lake Pontchartrain, Louisiana</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Signell, Richard P.; List, Jeffrey H.</p> <p>1997-01-01</p> <p>The U.S. Geological Survey is conducting a study of storm-driven sediment resuspension and transport in Lake Pontchartrain, Louisiana. Two critical processes related to sediment transport in the lake are (1) the resuspension of sediments due to wind-generated storm <span class="hlt">waves</span> and (2) the movement of resuspended material by lake <span class="hlt">currents</span> during storm wind events. The potential for sediment resuspension is being studied with the <span class="hlt">wave</span> prediction <span class="hlt">model</span> which simulates local generation of <span class="hlt">waves</span> by wind and shallow-water effects on <span class="hlt">waves</span> (refraction, shoaling, bottom friction, and breaking). Long-term wind measurements are then used to determine the regional "climate" of bottom orbital velocity (showing the spatial and temporal variability of <span class="hlt">wave</span>-induced <span class="hlt">currents</span> at the bottom). The circulation of the lake is being studied with a three-dimensional hydrodynamic <span class="hlt">model</span>. Results of the <span class="hlt">modeling</span> effort indicate that remote forcing due to water levels in Mississippi Sound dominate the circulation near the passes in the eastern end of the lake, while local wind forcing dominates water movement in the western end. During typical storms with winds from the north-northeast or the south-southeast, <span class="hlt">currents</span> along the south coast near New Orleans generally transport material westward, while material in the central region moves against the wind. When periods of sustained winds are followed by a drop in coastal sea level, a large amount of suspended sediment can be flushed from the lake.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26698978','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26698978"><span>Unconditionally stable WLP-FDTD method for the <span class="hlt">modeling</span> of electromagnetic <span class="hlt">wave</span> propagation in gyrotropic materials.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Li, Zheng-Wei; Xi, Xiao-Li; Zhang, Jin-Sheng; Liu, Jiang-fan</p> <p>2015-12-14</p> <p>The unconditional stable finite-difference time-domain (FDTD) method based on field expansion with weighted Laguerre polynomials (WLPs) is applied to <span class="hlt">model</span> electromagnetic <span class="hlt">wave</span> propagation in gyrotropic materials. The conventional Yee cell is modified to have the tightly <span class="hlt">coupled</span> <span class="hlt">current</span> density components located at the same spatial position. The perfectly matched layer (PML) is formulated in a stretched-coordinate (SC) system with the complex-frequency-shifted (CFS) factor to achieve good absorption performance. Numerical examples are shown to validate the accuracy and efficiency of the proposed method.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMEP21B1844M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMEP21B1844M"><span>New Insights About Large-Scale Delta Morphodynamics from a <span class="hlt">Coupled</span> <span class="hlt">Model</span> of Fluvial-Coastal Processes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Murray, A. B.; Ratliff, K. M.; Hutton, E.</p> <p>2017-12-01</p> <p>We use a newly developed delta <span class="hlt">model</span> to explore the combined effects of sea-level rise (SLR) and variable <span class="hlt">wave</span> influence on delta morphology, avulsion behavior, and autogenic sediment flux variability. Using the Community Surface Dynamics <span class="hlt">Modeling</span> System framework and tools, we <span class="hlt">couple</span> the River Avulsion and Floodplain Evolution <span class="hlt">Model</span> (RAFEM) to the Coastline Evolution <span class="hlt">Model</span> (CEM). RAFEM <span class="hlt">models</span> the fluvial processes, including river profile evolution, floodplain deposition, and avulsions. CEM uses gradients in alongshore sediment transport to distribute the fluvial sediment along the coastline. A suite of recent experiments using the <span class="hlt">coupled</span> <span class="hlt">model</span> and the Dakota software toolkit lead to several new insights: 1) A preferential avulsion location (which scales with the backwater length) can arise for geometric reasons that are independent of the recently suggested importance of alternation between flood and inter-flood periods. 2) The angular distribution of <span class="hlt">waves</span>, as well as the <span class="hlt">wave</span> height, affect the avulsion timescale. Previous work suggested that the time between avulsions will increase with greater <span class="hlt">wave</span> influence, and we find that this is true for an angular mix of <span class="hlt">waves</span> that tends to smooth a fairly straight coastline (coastline diffusion), where river mouth progradation is slowed and avulsions are delayed. However, if the angular distribution of <span class="hlt">waves</span> leads to locally smooth shorelines but large amplitude coastline features (anti-diffusive coastline evolution), then avulsion timescales are barely affected, even when <span class="hlt">wave</span> influence is high. 3) Increasing SLR rates are expected to cause more frequent avulsions, and it does in laboratory deltas. Unexpectedly, we find that this is not the case for the river-dominated deltas in our <span class="hlt">coupled</span> <span class="hlt">model</span>, in which SLR-related transgression effectively decreases progradation, offsetting base-level-rise effects. This finding raises potentially important questions about the geometric differences between prototypical and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70034373','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70034373"><span>Implementation and modification of a three-dimensional radiation stress formulation for surf zone and rip-<span class="hlt">current</span> applications</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Kumar, N.; Voulgaris, G.; Warner, John C.</p> <p>2011-01-01</p> <p>Regional Ocean <span class="hlt">Modeling</span> System (ROMS v 3.0), a three-dimensional numerical ocean <span class="hlt">model</span>, was previously enhanced for shallow water applications by including <span class="hlt">wave</span>-induced radiation stress forcing provided through <span class="hlt">coupling</span> to <span class="hlt">wave</span> propagation <span class="hlt">models</span> (SWAN, REF/DIF). This enhancement made it suitable for surf zone applications as demonstrated using examples of obliquely incident <span class="hlt">waves</span> on a planar beach and rip <span class="hlt">current</span> formation in longshore bar trough morphology (Haas and Warner, 2009). In this contribution, we present an update to the <span class="hlt">coupled</span> <span class="hlt">model</span> which implements a <span class="hlt">wave</span> roller <span class="hlt">model</span> and also a modified method of the radiation stress term based on Mellor (2008, 2011a,b,in press) that includes a vertical distribution which better simulates non-conservative (i.e., <span class="hlt">wave</span> breaking) processes and appears to be more appropriate for sigma coordinates in very shallow waters where <span class="hlt">wave</span> breaking conditions dominate. The improvements of the modified <span class="hlt">model</span> are shown through simulations of several cases that include: (a) obliquely incident spectral <span class="hlt">waves</span> on a planar beach; (b) obliquely incident spectral <span class="hlt">waves</span> on a natural barred beach (DUCK'94 experiment); (c) alongshore variable offshore <span class="hlt">wave</span> forcing on a planar beach; (d) alongshore varying bathymetry with constant offshore <span class="hlt">wave</span> forcing; and (e) nearshore barred morphology with rip-channels. Quantitative and qualitative comparisons to previous analytical, numerical, laboratory studies and field measurements show that the modified <span class="hlt">model</span> replicates surf zone recirculation patterns (onshore drift at the surface and undertow at the bottom) more accurately than previous formulations based on radiation stress (Haas and Warner, 2009). The results of the <span class="hlt">model</span> and test cases are further explored for identifying the forces operating in rip <span class="hlt">current</span> development and the potential implication for sediment transport and rip channel development. Also, <span class="hlt">model</span> analysis showed that rip <span class="hlt">current</span> strength is higher when <span class="hlt">waves</span> approach at angles of 5</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017OcDyn..67...81S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017OcDyn..67...81S"><span>Effects of <span class="hlt">wave</span>-induced forcing on a circulation <span class="hlt">model</span> of the North Sea</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Staneva, Joanna; Alari, Victor; Breivik, Øyvind; Bidlot, Jean-Raymond; Mogensen, Kristian</p> <p>2017-01-01</p> <p>The effect of wind <span class="hlt">waves</span> on water level and <span class="hlt">currents</span> during two storms in the North Sea is investigated using a high-resolution Nucleus for European <span class="hlt">Modelling</span> of the Ocean (NEMO) <span class="hlt">model</span> forced with fluxes and fields from a high-resolution <span class="hlt">wave</span> <span class="hlt">model</span>. The additional terms accounting for <span class="hlt">wave-current</span> interaction that are considered in this study are the Stokes-Coriolis force, the sea-state-dependent energy and momentum fluxes. The individual and collective role of these processes is quantified and the results are compared with a control run without <span class="hlt">wave</span> effects as well as against <span class="hlt">current</span> and water-level measurements from coastal stations. We find a better agreement with observations when the circulation <span class="hlt">model</span> is forced by sea-state-dependent fluxes, especially in extreme events. The two extreme events, the storm Christian (25-27 October 2013), and about a month later, the storm Xaver (5-7 December 2013), induce different <span class="hlt">wave</span> and surge conditions over the North Sea. Including the <span class="hlt">wave</span> effects in the circulation <span class="hlt">model</span> for the storm Xaver raises the <span class="hlt">modelled</span> surge by more than 40 cm compared with the control run in the German Bight area. For the storm Christian, a difference of 20-30 cm in the surge level between the <span class="hlt">wave</span>-forced and the stand-alone ocean <span class="hlt">model</span> is found over the whole southern part of the North Sea. Moreover, the <span class="hlt">modelled</span> vertical velocity profile fits the observations very well when the <span class="hlt">wave</span> forcing is accounted for. The contribution of <span class="hlt">wave</span>-induced forcing has been quantified indicating that this represents an important mechanism for improving water-level and <span class="hlt">current</span> predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1810725H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1810725H"><span>The Coordinated Ocean <span class="hlt">Wave</span> Climate Project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hemer, Mark; Dobrynin, Mikhail; Erikson, Li; Lionello, Piero; Mori, Nobuhito; Semedo, Alvaro; Wang, Xiaolan</p> <p>2016-04-01</p> <p>Future 21st Century changes in wind-<span class="hlt">wave</span> climate have broad implications for marine and coastal infrastructure and ecosystems. Atmosphere-ocean general circulation <span class="hlt">models</span> (GCM) are now routinely used for assessing and providing future projections of climatological parameters such as temperature and precipitation, but generally these provide no information on ocean wind-<span class="hlt">waves</span>. To fill this information gap a growing number of studies are using GCM outputs and independently producing global and regional scale wind-<span class="hlt">wave</span> climate projections. Furthermore, additional studies are actively <span class="hlt">coupling</span> wind-<span class="hlt">wave</span> dependent atmosphere-ocean exchanges into GCMs, to improve physical representation and quantify the impact of <span class="hlt">waves</span> in the <span class="hlt">coupled</span> climate system, and can also deliver <span class="hlt">wave</span> characteristics as another variable in the climate system. To consolidate these efforts, understand the sources of variance between projections generated by different methodologies and International groups, and ultimately provide a robust picture of the role of wind-<span class="hlt">waves</span> in the climate system and their projected changes, we present outcomes of the JCOMM supported Coordinated Ocean <span class="hlt">Wave</span> Climate Project (COWCLIP). The objective of COWCLIP is twofold: to make community based ensembles of <span class="hlt">wave</span> climate projections openly accessible, to provide the necessary information to support diligent marine and coastal impacts of climate change studies; and to understand the effects and feedback influences of wind-<span class="hlt">waves</span> in the <span class="hlt">coupled</span> ocean-atmosphere climate system. We will present the <span class="hlt">current</span> status of COWCLIP, providing an overview of the objectives, analysis and results of the initial phase - now complete - and the progress of ongoing phases of the project.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvF...2c4801N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvF...2c4801N"><span>Tunneling with a hydrodynamic pilot-<span class="hlt">wave</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>Nachbin, André; Milewski, Paul A.; Bush, John W. M.</p> <p>2017-03-01</p> <p>Eddi et al. [Phys. Rev Lett. 102, 240401 (2009), 10.1103/PhysRevLett.102.240401] presented experimental results demonstrating the unpredictable tunneling of a classical <span class="hlt">wave</span>-particle association as may arise when a droplet walking across the surface of a vibrating fluid bath approaches a submerged barrier. We here present a theoretical <span class="hlt">model</span> that captures the influence of bottom topography on this <span class="hlt">wave</span>-particle association and so enables us to investigate its interaction with barriers. The <span class="hlt">coupled</span> <span class="hlt">wave</span>-droplet dynamics results in unpredictable tunneling events. As reported in the experiments by Eddi et al. and as is the case in quantum tunneling [Gamow, Nature (London) 122, 805 (1928), 10.1038/122805b0], the predicted tunneling probability decreases exponentially with increasing barrier width. In the parameter regimes examined, tunneling between two cavities suggests an underlying stationary ergodic process for the droplet's position.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1060889','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1060889"><span>Benchmark <span class="hlt">Modeling</span> of the Near-Field and Far-Field <span class="hlt">Wave</span> Effects of <span class="hlt">Wave</span> Energy Arrays</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>Rhinefrank, Kenneth E; Haller, Merrick C; Ozkan-Haller, H Tuba</p> <p>2013-01-26</p> <p>This project is an industry-led partnership between Columbia Power Technologies and Oregon State University that will perform benchmark laboratory experiments and numerical <span class="hlt">modeling</span> of the near-field and far-field impacts of <span class="hlt">wave</span> scattering from an array of <span class="hlt">wave</span> energy devices. These benchmark experimental observations will help to fill a gaping hole in our present knowledge of the near-field effects of multiple, floating <span class="hlt">wave</span> energy converters and are a critical requirement for estimating the potential far-field environmental effects of <span class="hlt">wave</span> energy arrays. The experiments will be performed at the Hinsdale <span class="hlt">Wave</span> Research Laboratory (Oregon State University) and will utilize an array ofmore » newly developed Buoys' that are realistic, lab-scale floating power converters. The array of Buoys will be subjected to realistic, directional <span class="hlt">wave</span> forcing (1:33 scale) that will approximate the expected conditions (<span class="hlt">waves</span> and water depths) to be found off the Central Oregon Coast. Experimental observations will include comprehensive in-situ <span class="hlt">wave</span> and <span class="hlt">current</span> measurements as well as a suite of novel optical measurements. These new optical capabilities will include imaging of the 3D <span class="hlt">wave</span> scattering using a binocular stereo camera system, as well as 3D device motion tracking using a newly acquired LED system. These observing systems will capture the 3D motion history of individual Buoys as well as resolve the 3D scattered <span class="hlt">wave</span> field; thus resolving the constructive and destructive <span class="hlt">wave</span> interference patterns produced by the array at high resolution. These data combined with the device motion tracking will provide necessary information for array design in order to balance array performance with the mitigation of far-field impacts. As a benchmark data set, these data will be an important resource for testing of <span class="hlt">models</span> for <span class="hlt">wave</span>/buoy interactions, buoy performance, and far-field effects on <span class="hlt">wave</span> and <span class="hlt">current</span> patterns due to the presence of arrays. Under the proposed project we will</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AIPC.1689h0013T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AIPC.1689h0013T"><span>Plasma <span class="hlt">current</span> start-up using the lower hybrid <span class="hlt">wave</span> on the TST-2 spherical tokamak</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takase, Y.; Ejiri, A.; Inada, T.; Moeller, C. P.; Shinya, T.; Tsujii, N.; Yajima, S.; Furui, H.; Homma, H.; Imamura, K.; Nakamura, K.; Nakamura, K.; Sonehara, M.; Takeuchi, T.; Togashi, H.; Tsuda, S.; Yoshida, Y.</p> <p>2015-12-01</p> <p>Non-inductive plasma <span class="hlt">current</span> start-up, ramp-up and sustainment by <span class="hlt">waves</span> in the lower hybrid <span class="hlt">wave</span> (LHW) frequency range at 200 MHz were investigated on the TST-2 spherical tokamak (R0 ≤ 0.38 m, a ≤ 0.25 m, Bt0 ≤ 0.3T, Ip ≤ 0.14 MA). Experimental results obtained using three types of antenna were compared. Both the highest plasma <span class="hlt">current</span> (Ip = 18 kA) and the highest <span class="hlt">current</span> drive figure of merit ηCD≡n¯eIpR0/PRF=1.4 ×1017 A/W/m2 were achieved using the capacitively-<span class="hlt">coupled</span> combline (CCC) antenna, designed to excite the LHW with a sharp and highly directional wavenumber spectrum. For Ip greater than about 5 kA, high energy electrons accelerated by the LHW become the dominant carrier of plasma <span class="hlt">current</span>. The low value of ηCD observed so far are believed to be caused by a rapid loss of energetic electrons and parasitic losses of the LHW energy in the plasma periphery. ηCD is expected to improve by an order of magnitude by increasing the plasma <span class="hlt">current</span> to improve energetic electron confinement. In addition, edge power losses are expected to be reduced by increasing the toroidal magnetic field to improve <span class="hlt">wave</span> accessibility to the plasma core, and by launching the LHW from the inboard upper region of the torus to achieve better single-pass absorption.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_21 --> <div id="page_22" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="421"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JMPSo..95..501L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JMPSo..95..501L"><span><span class="hlt">Wave</span> mixing in <span class="hlt">coupled</span> phononic crystals via a variable stiffness mechanism</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lee, Gil-Yong; Chong, Christopher; Kevrekidis, Panayotis G.; Yang, Jinkyu</p> <p>2016-10-01</p> <p>We investigate <span class="hlt">wave</span> mixing effects in a phononic crystal that <span class="hlt">couples</span> the <span class="hlt">wave</span> dynamics of two channels - primary and control ones - via a variable stiffness mechanism. We demonstrate analytically and numerically that the <span class="hlt">wave</span> transmission in the primary channel can be manipulated by the control channel's signal. We show that the application of control <span class="hlt">waves</span> allows the selection of a specific mode through the primary channel. We also demonstrate that the mixing of two <span class="hlt">wave</span> modes is possible whereby a modulation effect is observed. A detailed study of the design parameters is also carried out to optimize the switching capabilities of the proposed system. Finally, we verify that the system can fulfill both switching and amplification functionalities, potentially enabling the realization of an acoustic transistor.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28559056','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28559056"><span>Fate of microplastics and mesoplastics carried by surface <span class="hlt">currents</span> and wind <span class="hlt">waves</span>: A numerical <span class="hlt">model</span> approach in the Sea of Japan.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Iwasaki, Shinsuke; Isobe, Atsuhiko; Kako, Shin'ichiro; Uchida, Keiichi; Tokai, Tadashi</p> <p>2017-08-15</p> <p>A numerical <span class="hlt">model</span> was established to reproduce the oceanic transport processes of microplastics and mesoplastics in the Sea of Japan. A particle tracking <span class="hlt">model</span>, where surface ocean <span class="hlt">currents</span> were given by a combination of a reanalysis ocean <span class="hlt">current</span> product and Stokes drift computed separately by a <span class="hlt">wave</span> <span class="hlt">model</span>, simulated particle movement. The <span class="hlt">model</span> results corresponded with the field survey. <span class="hlt">Modeled</span> results indicated the micro- and mesoplastics are moved northeastward by the Tsushima <span class="hlt">Current</span>. Subsequently, Stokes drift selectively moves mesoplastics during winter toward the Japanese coast, resulting in increased contributions of mesoplastics south of 39°N. Additionally, Stokes drift also transports micro- and mesoplastics out to the sea area south of the subpolar front where the northeastward Tsushima <span class="hlt">Current</span> carries them into the open ocean via the Tsugaru and Soya straits. Average transit time of <span class="hlt">modeled</span> particles in the Sea of Japan is drastically reduced when including Stokes drift in the <span class="hlt">model</span>. Copyright © 2017 The Authors. Published by Elsevier Ltd.. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvD..97h1303F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvD..97h1303F"><span>Production of gravitational <span class="hlt">waves</span> during preheating with nonminimal <span class="hlt">coupling</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fu, Chengjie; Wu, Puxun; Yu, Hongwei</p> <p>2018-04-01</p> <p>We study the preheating and the in-process production of gravitational <span class="hlt">waves</span> (GWs) after inflation in which the inflaton is nonminimally <span class="hlt">coupled</span> to the curvature in a self-interacting quartic potential with the method of lattice simulation. We find that the nonminimal <span class="hlt">coupling</span> enhances the amplitude of the density spectrum of inflaton quanta, and as a result, the peak value of the GW spectrum generated during preheating is enhanced as well and might reach the limit of detection in future GW experiments. The peaks of the GW spectrum not only exhibit distinctive characteristics as compared to those of minimally <span class="hlt">coupled</span> inflaton potentials but also imprint information on the nonminimal <span class="hlt">coupling</span> and the parametric resonance, and thus the detection of these peaks in the future will provide us a new avenue to reveal the physics of the early universe.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DPPN10064T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DPPN10064T"><span>Plasma <span class="hlt">current</span> ramp-up by lower hybrid <span class="hlt">wave</span> using innovative antennas on TST-2</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Takase, Yuichi; Ejiri, Akira; Moeller, Charles; Roidl, Benedikt; Shinya, Takahiro; Tsujii, Naoto; Yajima, Satoru; Yamazaki, Hibiki; Kitayama, Akichika; Matsumoto, Naoki; Sato, Akito; Sonehara, Masateru; Takahashi, Wataru; Tajiri, Yoshiyuki; Takei, Yuki; Togashi, Hiro; Toida, Kazuya; Yoshida, Yusuke</p> <p>2016-10-01</p> <p>Non-inductive plasma <span class="hlt">current</span> (Ip) ramp-up by RF power in the lower hybrid frequency range is being studied on the TST-2 spherical tokamak (R = 0.36 m, a = 0.23 m, Bt = 0.3 T, Ip = 0.1 MA). Up to 400 kW of RF power is available at a frequency of 200 MHz. An innovative antenna called the capacitively-<span class="hlt">coupled</span> combline (CCC) antenna was developed to excite a sharp, highly directional traveling <span class="hlt">wave</span> with the electric field polarized in the toroidal direction. It is an array of resonant circuit elements made of capacitance and inductance, <span class="hlt">coupled</span> to neighboring elements by mutual capacitance. Two CCC antennas are installed in TST-2, a 13-element outboard-launch antenna and a 6-element top-launch antenna. The latter was installed in March 2016 to improve accessibility to the core and to achieve single-pass damping. The suspected <span class="hlt">wave</span> power loss in the scrape-off layer plasma should also be avoided. Ip ramp-up to 25 kA has been achieved so far. An upgrade of the Bt power supply is planned to take advantage of the observed improvement of Ip ramp-up with Bt. Higher Bt for longer pulses should improve the Ip ramp-up efficiency by improving <span class="hlt">wave</span> accessibility and by reducing prompt orbit losses of energetic electrons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002ASAJ..112.2296S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002ASAJ..112.2296S"><span>Long codas of <span class="hlt">coupled</span> <span class="hlt">wave</span> systems in seismic basins</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Seligman, Thomas H.</p> <p>2002-11-01</p> <p>Quite some time ago it was pointed out that the damage patterns and Fourier spectra of the 1985 earthquake in Mexico City are only compatible with a resonant effect of horizontal <span class="hlt">waves</span> with the approximate speed of sound <span class="hlt">waves</span> in water [see Flores et al., Nature 326, 783 (1987)]. In a more recent paper it was pointed out that this indeed will occur with a very specific frequency selection for a <span class="hlt">coupled</span> system of Raleigh <span class="hlt">waves</span> at the interface of the bottom of the ancient lakebed with the more solid deposits, and an evanescent sound <span class="hlt">wave</span> in the mud above [see J. Flores et al., Bull. Seismol. Soc. Am. 89, 14-21 (1999)]. In the present talk we shall go over these arguments again and show that strong reflection at the edges of the lake must occur to account for the strong magnification entailing necessarily a long coda, and that the mecanism can be understood in the same terms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20366714','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20366714"><span>Solvable <span class="hlt">model</span> of spiral <span class="hlt">wave</span> chimeras.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Martens, Erik A; Laing, Carlo R; Strogatz, Steven H</p> <p>2010-01-29</p> <p>Spiral <span class="hlt">waves</span> are ubiquitous in two-dimensional systems of chemical or biological oscillators <span class="hlt">coupled</span> locally by diffusion. At the center of such spirals is a phase singularity, a topological defect where the oscillator amplitude drops to zero. But if the <span class="hlt">coupling</span> is nonlocal, a new kind of spiral can occur, with a circular core consisting of desynchronized oscillators running at full amplitude. Here, we provide the first analytical description of such a spiral <span class="hlt">wave</span> chimera and use perturbation theory to calculate its rotation speed and the size of its incoherent core.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhCS.991a2047K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhCS.991a2047K"><span><span class="hlt">Wave</span> propagation problem for a micropolar elastic waveguide</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kovalev, V. A.; Murashkin, E. V.; Radayev, Y. N.</p> <p>2018-04-01</p> <p>A propagation problem for <span class="hlt">coupled</span> harmonic <span class="hlt">waves</span> of translational displacements and microrotations along the axis of a long cylindrical waveguide is discussed at present study. Microrotations <span class="hlt">modeling</span> is carried out within the linear micropolar elasticity frameworks. The mathematical <span class="hlt">model</span> of the linear (or even nonlinear) micropolar elasticity is also expanded to a field theory <span class="hlt">model</span> by variational least action integral and the least action principle. The governing <span class="hlt">coupled</span> vector differential equations of the linear micropolar elasticity are given. The translational displacements and microrotations in the harmonic <span class="hlt">coupled</span> <span class="hlt">wave</span> are decomposed into potential and vortex parts. Calibrating equations providing simplification of the equations for the <span class="hlt">wave</span> potentials are proposed. The <span class="hlt">coupled</span> differential equations are then reduced to uncoupled ones and finally to the Helmholtz <span class="hlt">wave</span> equations. The <span class="hlt">wave</span> equations solutions for the translational and microrotational <span class="hlt">waves</span> potentials are obtained for a high-frequency range.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015PIAHS.367..134K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015PIAHS.367..134K"><span><span class="hlt">Wave-current</span> induced erosion of cohesive riverbanks in northern Manitoba, Canada</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kimiaghalam, N.; Clark, S.; Ahmari, H.; Hunt, J.</p> <p>2015-03-01</p> <p>The field of cohesive soil erosion is still not fully understood, in large part due to the many soil parameters that affect cohesive soil erodibility. This study is focused on two channels, 2-Mile and 8-Mile channels in northern Manitoba, Canada, that were built to connect Lake Winnipeg with Playgreen Lake and Playgreen Lake with Kiskikittogisu Lake, respectively. The banks of the channels consist of clay rich soils and alluvial deposits of layered clay, silts and sands. The study of erosion at the sites is further complicated because the flow-induced erosion is combined with the effects of significant <span class="hlt">wave</span> action due to the large fetch length on the adjacent lakes, particularly Lake Winnipeg that is the seventh largest lake in North America. The study included three main components: field measurements, laboratory experiments and numerical <span class="hlt">modelling</span>. Field measurements consisted of soil sampling from the banks and bed of the channels, <span class="hlt">current</span> measurements and water sampling. Grab soil samples were used to measure the essential physical and electrochemical properties of the riverbanks, and standard ASTM Shelby tube samples were used to estimate the critical shear stress and erodibility of the soil samples using an erosion measurement device (EMD). Water samples were taken to estimate the sediment concentration profile and also to monitor changes in sediment concentration along the channels over time. An Acoustic Doppler <span class="hlt">Current</span> Profiler (ADCP) was used to collect bathymetry and <span class="hlt">current</span> data, and two water level gauges have been installed to record water levels at the entrance and outlet of the channels. The MIKE 21 NSW <span class="hlt">model</span> was used to simulate <span class="hlt">waves</span> using historical winds and measured bathymetry of the channels and lakes. Finally, results from the <span class="hlt">wave</span> numerical <span class="hlt">model</span>, laboratory tests and <span class="hlt">current</span> measurement were used to estimate the effect of each component on erodibility of the cohesive banks.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhLA..382.1738X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhLA..382.1738X"><span>Breathers and solitons on two different backgrounds in a generalized <span class="hlt">coupled</span> Hirota system with four <span class="hlt">wave</span> mixing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Han-Xiang; Yang, Zhan-Ying; Zhao, Li-Chen; Duan, Liang; Yang, Wen-Li</p> <p>2018-07-01</p> <p>We study breathers and solitons on different backgrounds in optical fiber system, which is governed by generalized <span class="hlt">coupled</span> Hirota equations with four <span class="hlt">wave</span> mixing effect. On plane <span class="hlt">wave</span> background, a transformation between different types of solitons is discovered. Then, on periodic <span class="hlt">wave</span> background, we find breather-like nonlinear localized <span class="hlt">waves</span> of which formation mechanism are related to the energy conversion between two components. The energy conversion results from four <span class="hlt">wave</span> mixing. Furthermore, we prove that this energy conversion is controlled by amplitude and period of backgrounds. Finally, solitons on periodic <span class="hlt">wave</span> background are also exhibited. These results would enrich our knowledge of nonlinear localized <span class="hlt">waves</span>' excitation in <span class="hlt">coupled</span> system with four <span class="hlt">wave</span> mixing effect.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOS.A14B2547M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOS.A14B2547M"><span>Monsoon Variability in the Arabian Sea from Enhanced and Standard Horizontal Resolution <span class="hlt">Coupled</span> Climate <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>McClean, J.; Veneziani, C.; Maltrud, M. E.; Taylor, M.; Bader, D. C.; Branstetter, M. L.; Evans, K. J.; Mahajan, S.</p> <p>2016-02-01</p> <p>The circulation of the upper ocean in the Arabian Sea switches direction seasonally due to the change in direction of the prevailing winds associated with the Indian Monsoon. Predictability of the monsoon circulation, however, is uncertain due to incomplete understanding of the physical processes operating on the monsoon and other time scales, particularly interannual and intraseasonal. We use the Community Earth System <span class="hlt">Model</span> (CESM) with enhanced horizontal resolution in each of its components relative to standard <span class="hlt">coupled</span> climate <span class="hlt">model</span> resolution, to better understand these time scale interactions. A standard resolution CESM counterpart is used to assess how horizontal resolution impacts the depiction of these processes. In the enhanced resolution case, 0.25° Community Atmosphere <span class="hlt">Model</span> 5 (CAM5) is <span class="hlt">coupled</span> to, among other components, the tripolar nominal 0.1° Parallel Ocean Program 2 (POP2). The fine resolution CESM simulation was run for 85 years; constant 1850 preindustrial forcing was used throughout the run, allowing us to isolate internal variability of the <span class="hlt">coupled</span> system. <span class="hlt">Model</span> parameters were adjusted ("tuned") to produce an acceptably small top of the atmosphere radiation imbalance. The reversal of the Somali <span class="hlt">Current</span> (SC), the western boundary <span class="hlt">current</span> off northeast Africa, has typically been associated with that of the monsoon. The SC reverses from southwestward in boreal winter to northeastward in summer; coastal upwelling is induced by the summer monsoonal winds. Recently it has been shown from new observations that the SC starts to reverse prior to the monsoon switch. Westward propagating Rossby <span class="hlt">waves</span> have been implicated as responsible for the early SC reversal. We will discuss the sequencing of remote and local forcing on the timing of the spring inter-monsoonal switch in the direction of the SC and the appearance of the Great Whirl off the Oman Coast. Particularly, we consider how the Indian Ocean Dipole (IOD) acts to modify the seasonal strength and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhRvB..97h5127S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhRvB..97h5127S"><span>Alternating <span class="hlt">currents</span> and shear <span class="hlt">waves</span> in viscous electronics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Semenyakin, M.; Falkovich, G.</p> <p>2018-02-01</p> <p>Strong interaction among charge carriers can make them move like viscous fluid. Here we explore alternating <span class="hlt">current</span> (ac) effects in viscous electronics. In the Ohmic case, incompressible <span class="hlt">current</span> distribution in a sample adjusts fast to a time-dependent voltage on the electrodes, while in the viscous case, momentum diffusion makes for retardation and for the possibility of propagating slow shear <span class="hlt">waves</span>. We focus on specific geometries that showcase interesting aspects of such <span class="hlt">waves</span>: <span class="hlt">current</span> parallel to a one-dimensional defect and <span class="hlt">current</span> applied across a long strip. We find that the phase velocity of the <span class="hlt">wave</span> propagating along the strip respectively increases/decreases with the frequency for no-slip/no-stress boundary conditions. This is so because when the frequency or strip width goes to zero (alternatively, viscosity go to infinity), the wavelength of the <span class="hlt">current</span> pattern tends to infinity in the no-stress case and to a finite value in a general case. We also show that for dc <span class="hlt">current</span> across a strip with a no-stress boundary, there are only one pair of vortices, while there is an infinite vortex chain for all other types of boundary conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PhRvD..87d4052E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PhRvD..87d4052E"><span><span class="hlt">Couplings</span> of gravitational <span class="hlt">currents</span> with Chern-Simons gravities</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ertem, Ümit; Açık, Özgür</p> <p>2013-02-01</p> <p>The <span class="hlt">coupling</span> of conserved p-brane <span class="hlt">currents</span> with non-Abelian gauge theories is done consistently by using Chern-Simons forms. Conserved <span class="hlt">currents</span> localized on p-branes that have a gravitational origin can be constructed from Killing-Yano forms of the underlying spacetime. We propose a generalization of the <span class="hlt">coupling</span> procedure with Chern-Simons gravities to the case of gravitational conserved <span class="hlt">currents</span>. In odd dimensions, the field equations of <span class="hlt">coupled</span> Chern-Simons gravities that describe the local curvature on p-branes are obtained. In special cases of three and five dimensions, the field equations are investigated in detail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhRvE..93a2411S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhRvE..93a2411S"><span>Inducing rostrum interfacial <span class="hlt">waves</span> by fluid-solid <span class="hlt">coupling</span> in a Chinese river dolphin (Lipotes vexillifer )</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Song, Zhongchang; Zhang, Yu; Wei, Chong; Wang, Xianyan</p> <p>2016-01-01</p> <p>Through numerically solving the appropriate <span class="hlt">wave</span> equations, propagation of biosonar signals in a Chinese river dolphin (baiji) was studied. The interfacial <span class="hlt">waves</span> along the rostrum-tissue interfaces, including both compressional (longitudinal) and shear (transverse) <span class="hlt">waves</span> in the solid rostrum through fluid-solid <span class="hlt">coupling</span> were examined. The baiji's rostrum was found to effect acoustic beam formation not only as an interfacial <span class="hlt">wave</span> generator but also as a sound reflector. The <span class="hlt">wave</span> propagation patterns in the solid rostrum were found to significantly change the <span class="hlt">wave</span> movement through the bone. Vibrations in the rostrum, expressed in solid displacement, initially increased but eventually decreased from posterior to anterior sides, indicating a complex physical process. Furthermore, the comparisons among seven cases, including the combination of (1) the rostrum, melon, and air sacs; (2) rostrum-air sacs; (3) rostrum-melon; (4) only rostrum; (5) air sacs-melon; (6) only air sacs; and (7) only melon revealed that the cases including the rostrum were better able to approach the complete system by inducing rostrum-tissue interfacial <span class="hlt">waves</span> and reducing the differences in main beam angle and -3 dB beam width. The interfacial <span class="hlt">waves</span> in the rostrum were considered complementary with reflection to determine the obbligato role of the rostrum in the baiji's biosonar emission. The far-field beams formed from complete fluid-solid <span class="hlt">models</span> and non-fluid-solid <span class="hlt">models</span> were compared to reveal the effects brought by the consideration of shear <span class="hlt">waves</span> of the solid structures of the baiji. The results may provide useful information for further understanding the role of the rostrum in this odontocete species.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA583025','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA583025"><span>Lake St. Clair: Storm <span class="hlt">Wave</span> and Water Level <span class="hlt">Modeling</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2013-06-01</p> <p>R. A. Luettich, C. Dawson, V. J. Cardone , A. T. Cox, M. D. Powell, H. J. Westerink, and H. J. Roberts. 2010. A high resolution <span class="hlt">coupled</span> riverine flow...Storm <span class="hlt">Wave</span> and Water Level <span class="hlt">Modeling</span> 5a. CONTRACT NUMBER 5b. GRANT NUMBER 5c. PROGRAM ELEMENT NUMBER 6. AUTHOR(S) Tyler J. Hesser</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013PPCF...55g4007F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013PPCF...55g4007F"><span>Dynamical <span class="hlt">coupling</span> between magnetic equilibrium and transport in tokamak scenario <span class="hlt">modelling</span>, with application to <span class="hlt">current</span> ramps</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fable, E.; Angioni, C.; Ivanov, A. A.; Lackner, K.; Maj, O.; Medvedev, S. Yu; Pautasso, G.; Pereverzev, G. V.; Treutterer, W.; the ASDEX Upgrade Team</p> <p>2013-07-01</p> <p>The <span class="hlt">modelling</span> of tokamak scenarios requires the simultaneous solution of both the time evolution of the plasma kinetic profiles and of the magnetic equilibrium. Their dynamical <span class="hlt">coupling</span> involves additional complications, which are not present when the two physical problems are solved separately. Difficulties arise in maintaining consistency in the time evolution among quantities which appear in both the transport and the Grad-Shafranov equations, specifically the poloidal and toroidal magnetic fluxes as a function of each other and of the geometry. The required consistency can be obtained by means of iteration cycles, which are performed outside the equilibrium code and which can have different convergence properties depending on the chosen numerical scheme. When these external iterations are performed, the stability of the <span class="hlt">coupled</span> system becomes a concern. In contrast, if these iterations are not performed, the <span class="hlt">coupled</span> system is numerically stable, but can become physically inconsistent. By employing a novel scheme (Fable E et al 2012 Nucl. Fusion submitted), which ensures stability and physical consistency among the same quantities that appear in both the transport and magnetic equilibrium equations, a newly developed version of the ASTRA transport code (Pereverzev G V et al 1991 IPP Report 5/42), which is <span class="hlt">coupled</span> to the SPIDER equilibrium code (Ivanov A A et al 2005 32nd EPS Conf. on Plasma Physics (Tarragona, 27 June-1 July) vol 29C (ECA) P-5.063), in both prescribed- and free-boundary modes is presented here for the first time. The ASTRA-SPIDER <span class="hlt">coupled</span> system is then applied to the specific study of the <span class="hlt">modelling</span> of controlled <span class="hlt">current</span> ramp-up in ASDEX Upgrade discharges.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20070019767','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20070019767"><span>Effect of EMIC <span class="hlt">Wave</span> Normal Angle Distribution on Relativistic Electron Scattering Based on the Newly Developed Self-consistent RC/EMIC <span class="hlt">Waves</span> <span class="hlt">Model</span> by Khazanov et al. [2006</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Khazanov, G. V.; Gallagher, D. L.; Gamayunov, K.</p> <p>2007-01-01</p> <p>It is well known that the effects of EMIC <span class="hlt">waves</span> on RC ion and RB electron dynamics strongly depend on such particle/<span class="hlt">wave</span> characteristics as the phase-space distribution function, frequency, <span class="hlt">wave</span>-normal angle, <span class="hlt">wave</span> energy, and the form of <span class="hlt">wave</span> spectral energy density. Therefore, realistic characteristics of EMIC <span class="hlt">waves</span> should be properly determined by <span class="hlt">modeling</span> the RC-EMIC <span class="hlt">waves</span> evolution self-consistently. Such a selfconsistent <span class="hlt">model</span> progressively has been developing by Khaznnov et al. [2002-2006]. It solves a system of two <span class="hlt">coupled</span> kinetic equations: one equation describes the RC ion dynamics and another equation describes the energy density evolution of EMIC <span class="hlt">waves</span>. Using this <span class="hlt">model</span>, we present the effectiveness of relativistic electron scattering and compare our results with previous work in this area of research.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhPl...25d3118T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhPl...25d3118T"><span>Ion acoustic <span class="hlt">wave</span> assisted laser beat <span class="hlt">wave</span> terahertz generation in a plasma channel</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tyagi, Yachna; Tripathi, Deepak; Walia, Keshav; Garg, Deepak</p> <p>2018-04-01</p> <p>Resonant excitation of terahertz (THz) radiation by non-linear mixing of two lasers in the presence of an electrostatic <span class="hlt">wave</span> is investigated. The electrostatic <span class="hlt">wave</span> assists in k matching and contributes to non-linear <span class="hlt">coupling</span>. In this plasma channel, the electron plasma frequency becomes minimum on the axis. The beat frequency ponderomotive force imparts an oscillating velocity to the electrons. In the presence of an ion-acoustic <span class="hlt">wave</span>, density perturbation due to the ion-acoustic <span class="hlt">wave</span> <span class="hlt">couples</span> with the oscillating velocity of the electrons and give rise to non-linear <span class="hlt">current</span> that gives rise to an ion-acoustic <span class="hlt">wave</span> frequency assisted THz radiation field. The normalized field amplitude of ion acoustic <span class="hlt">wave</span> assisted THz varies inversely for ω/ωp . The field amplitude of ion acoustic <span class="hlt">wave</span> assisted THz decreases as ω/ωp increases.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22654179','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22654179"><span>Qualitative validation of the reduction from two reciprocally <span class="hlt">coupled</span> neurons to one self-<span class="hlt">coupled</span> neuron in a respiratory network <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>Dunmyre, Justin R</p> <p>2011-06-01</p> <p>The pre-Bötzinger complex of the mammalian brainstem is a heterogeneous neuronal network, and individual neurons within the network have varying strengths of the persistent sodium and calcium-activated nonspecific cationic <span class="hlt">currents</span>. Individually, these <span class="hlt">currents</span> have been the focus of <span class="hlt">modeling</span> efforts. Previously, Dunmyre et al. (J Comput Neurosci 1-24, 2011) proposed a <span class="hlt">model</span> and studied the interactions of these <span class="hlt">currents</span> within one self-<span class="hlt">coupled</span> neuron. In this work, I consider two identical, reciprocally <span class="hlt">coupled</span> <span class="hlt">model</span> neurons and validate the reduction to the self-<span class="hlt">coupled</span> case. I find that all of the dynamics of the two <span class="hlt">model</span> neuron network and the regions of parameter space where these distinct dynamics are found are qualitatively preserved in the reduction to the self-<span class="hlt">coupled</span> case.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AcMSn..31....1Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AcMSn..31....1Z"><span><span class="hlt">Modeling</span> ocean <span class="hlt">wave</span> propagation under sea ice covers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhao, Xin; Shen, Hayley H.; Cheng, Sukun</p> <p>2015-02-01</p> <p>Operational ocean <span class="hlt">wave</span> <span class="hlt">models</span> need to work globally, yet <span class="hlt">current</span> ocean <span class="hlt">wave</span> <span class="hlt">models</span> can only treat ice-covered regions crudely. The purpose of this paper is to provide a brief overview of ice effects on <span class="hlt">wave</span> propagation and different research methodology used in studying these effects. Based on its proximity to land or sea, sea ice can be classified as: landfast ice zone, shear zone, and the marginal ice zone. All ice covers attenuate <span class="hlt">wave</span> energy. Only long swells can penetrate deep into an ice cover. Being closest to open water, <span class="hlt">wave</span> propagation in the marginal ice zone is the most complex to <span class="hlt">model</span>. The physical appearance of sea ice in the marginal ice zone varies. Grease ice, pancake ice, brash ice, floe aggregates, and continuous ice sheet may be found in this zone at different times and locations. These types of ice are formed under different thermal-mechanical forcing. There are three classic <span class="hlt">models</span> that describe <span class="hlt">wave</span> propagation through an idealized ice cover: mass loading, thin elastic plate, and viscous layer <span class="hlt">models</span>. From physical arguments we may conjecture that mass loading <span class="hlt">model</span> is suitable for disjoint aggregates of ice floes much smaller than the wavelength, thin elastic plate <span class="hlt">model</span> is suitable for a continuous ice sheet, and the viscous layer <span class="hlt">model</span> is suitable for grease ice. For different sea ice types we may need different <span class="hlt">wave</span> ice interaction <span class="hlt">models</span>. A recently proposed viscoelastic <span class="hlt">model</span> is able to synthesize all three classic <span class="hlt">models</span> into one. Under suitable limiting conditions it converges to the three previous <span class="hlt">models</span>. The complete theoretical framework for evaluating <span class="hlt">wave</span> propagation through various ice covers need to be implemented in the operational ocean <span class="hlt">wave</span> <span class="hlt">models</span>. In this review, we introduce the sea ice types, previous <span class="hlt">wave</span> ice interaction <span class="hlt">models</span>, <span class="hlt">wave</span> attenuation mechanisms, the methods to calculate <span class="hlt">wave</span> reflection and transmission between different ice covers, and the effect of ice floe breaking on shaping the sea ice morphology</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21405399','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21405399"><span>Kuramoto <span class="hlt">model</span> of <span class="hlt">coupled</span> oscillators with positive and negative <span class="hlt">coupling</span> parameters: an example of conformist and contrarian oscillators.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Hong, Hyunsuk; Strogatz, Steven H</p> <p>2011-02-04</p> <p>We consider a generalization of the Kuramoto <span class="hlt">model</span> in which the oscillators are <span class="hlt">coupled</span> to the mean field with random signs. Oscillators with positive <span class="hlt">coupling</span> are "conformists"; they are attracted to the mean field and tend to synchronize with it. Oscillators with negative <span class="hlt">coupling</span> are "contrarians"; they are repelled by the mean field and prefer a phase diametrically opposed to it. The <span class="hlt">model</span> is simple and exactly solvable, yet some of its behavior is surprising. Along with the stationary states one might have expected (a desynchronized state, and a partially-synchronized state, with conformists and contrarians locked in antiphase), it also displays a traveling <span class="hlt">wave</span>, in which the mean field oscillates at a frequency different from the population's mean natural frequency.</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('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3433594','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3433594"><span>Axonal properties determine somatic firing in a <span class="hlt">model</span> of in vitro CA1 hippocampal sharp <span class="hlt">wave</span>/ripples and persistent gamma oscillations</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Traub, Roger D.; Schmitz, Dietmar; Maier, Nikolaus; Whittington, Miles A.; Draguhn, Andreas</p> <p>2012-01-01</p> <p>Evidence has been presented that CA1 pyramidal cells, during spontaneous in vitro sharp <span class="hlt">wave</span>/ripple (SPW-R) complexes, generate somatic action potentials that originate in axons. ‘Participating’ (somatically firing) pyramidal cells fire (almost always) at most once during a particular SPW-R whereas non-participating cells virtually never fire during an SPW-R. Somatic spikelets were small or absent, while ripple-frequency EPSCs and IPSCs occurred during the SPW-R in pyramidal neurons. These experimental findings could be replicated with a network <span class="hlt">model</span> in which electrical <span class="hlt">coupling</span> was present between small pyramidal cell axonal branches. Here, we explore this <span class="hlt">model</span> in more depth. Factors that influence somatic participation include: (i) the diameter of axonal branches that contain <span class="hlt">coupling</span> sites to other axons, because firing in larger branches injects more <span class="hlt">current</span> into the main axon, increasing antidromic firing probability; (ii) axonal K+ <span class="hlt">currents</span>; and (iii) somatic hyperpolarization and shunting. We predict that portions of axons fire at high frequency during SPW-R, while somata fire much less. In the <span class="hlt">model</span>, somatic firing can occur by occasional generation of full action potentials in proximal axonal branches, which are excited by high-frequency spikelets. When the network contains phasic synaptic inhibition, at the axonal gap junction site, gamma oscillations result, again with more frequent axonal firing than somatic firing. Combining the <span class="hlt">models</span>, so as to generate gamma followed by sharp <span class="hlt">waves</span>, leads to strong overlap between the population of cells firing during gamma the population of cells firing during a subsequent sharp <span class="hlt">wave</span>, as observed in vivo. PMID:22697272</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/21916678','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/21916678"><span>A computational <span class="hlt">model</span> of the cardiovascular system <span class="hlt">coupled</span> with an upper-arm oscillometric cuff and its application to studying the suprasystolic cuff oscillation <span class="hlt">wave</span>, concerning its value in assessing arterial stiffness.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Liang, Fuyou; Takagi, Shu; Himeno, Ryutaro; Liu, Hao</p> <p>2013-01-01</p> <p>A variety of methods have been proposed to noninvasively assess arterial stiffness using single or multiple oscillometric cuffs. A common pitfall of most of such methods is that the individual-specific accuracy of assessment is not clearly known due to an insufficient understanding of the relationships between the characteristics of cuff oscillometry and cardiovascular properties. To provide a tool for quantitatively investigating such relationships, we developed a computational <span class="hlt">model</span> of the cardiovascular system <span class="hlt">coupled</span> with an oscillometric cuff wrapped around the left upper arm. The <span class="hlt">model</span> was first examined by simulating the inflation-deflation process of the cuff. The simulated results reasonably reproduced the well-established characteristics of cuff oscillometry. The <span class="hlt">model</span> was then applied to study the oscillation <span class="hlt">wave</span> generated by a suprasystolic cuff that is <span class="hlt">currently</span> under considerable debate regarding its validity for assessing aortic stiffness. The simulated results confirmed the experimental observations that the suprasystolic cuff oscillation <span class="hlt">wave</span> resembles the blood pressure <span class="hlt">wave</span> in the proximal brachial artery and is characterised by the presence of two systolic peaks. A systemic analysis on the simulation results for various cardiovascular/physiological conditions revealed that neither the time lag nor the height difference between the two peaks is a direct indicator of aortic stiffness. These findings provided useful evidence for explaining the conflicts among previous studies. Finally, it was stressed that although the emphasis of this study has been placed on a suprasystolic upper-arm cuff, the <span class="hlt">model</span> could be employed to address more issues related to oscillometric cuffs.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFM.S33C2785S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFM.S33C2785S"><span>Spectral-Element Seismic <span class="hlt">Wave</span> Propagation Codes for both Forward <span class="hlt">Modeling</span> in Complex Media and Adjoint Tomography</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, J. A.; Peter, D. B.; Tromp, J.; Komatitsch, D.; Lefebvre, M. P.</p> <p>2015-12-01</p> <p>We present both SPECFEM3D_Cartesian and SPECFEM3D_GLOBE open-source codes, representing high-performance numerical <span class="hlt">wave</span> solvers simulating seismic <span class="hlt">wave</span> propagation for local-, regional-, and global-scale application. These codes are suitable for both forward propagation in complex media and tomographic imaging. Both solvers compute highly accurate seismic <span class="hlt">wave</span> fields using the continuous Galerkin spectral-element method on unstructured meshes. Lateral variations in compressional- and shear-<span class="hlt">wave</span> speeds, density, as well as 3D attenuation Q <span class="hlt">models</span>, topography and fluid-solid <span class="hlt">coupling</span> are all readily included in both codes. For global simulations, effects due to rotation, ellipticity, the oceans, 3D crustal <span class="hlt">models</span>, and self-gravitation are additionally included. Both packages provide forward and adjoint functionality suitable for adjoint tomography on high-performance computing architectures. We highlight the most recent release of the global version which includes improved performance, simultaneous MPI runs, OpenCL and CUDA support via an automatic source-to-source transformation library (BOAST), parallel I/O readers and writers for databases using ADIOS and seismograms using the recently developed Adaptable Seismic Data Format (ASDF) with built-in provenance. This makes our spectral-element solvers <span class="hlt">current</span> state-of-the-art, open-source community codes for high-performance seismic <span class="hlt">wave</span> propagation on arbitrarily complex 3D <span class="hlt">models</span>. Together with these solvers, we provide full-waveform inversion tools to image the Earth's interior at unprecedented resolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OcDyn..68....1D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OcDyn..68....1D"><span>Hindcast of breaking <span class="hlt">waves</span> and its impact at an island sheltered coast, Karwar</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dora, G. Udhaba; Kumar, V. Sanil</p> <p>2018-01-01</p> <p>Variability in the characteristics of depth-induced <span class="hlt">wave</span> breakers along a non-uniform coastal topography and its impact on the morpho-sedimentary processes is examined at the island sheltered <span class="hlt">wave</span>-dominated micro-tidal coast, Karwar, west coast of India. <span class="hlt">Waves</span> are simulated using the <span class="hlt">coupled</span> wind <span class="hlt">wave</span> <span class="hlt">model</span>, SWAN nested in WAVEWATCH III, forced by the reanalysis winds from different sources (NCEP/NCAR, ECMWF, and NCEP/CFSR). Impact of the <span class="hlt">wave</span> breakers is evaluated through mean longshore <span class="hlt">current</span> and sediment transport for various <span class="hlt">wave</span> energy conditions across different coastal morphology. Study revealed that the NCEP/CFSR wind is comparatively reasonable in simulation of nearshore <span class="hlt">waves</span> using the SWAN <span class="hlt">model</span> nested by 2D <span class="hlt">wave</span> spectra generated from WAVEWATCH III. The Galvin formula for estimating mean longshore <span class="hlt">current</span> using the crest <span class="hlt">wave</span> period and the Kamphuis approximation for longshore sediment transport is observed realistically at the sheltered coastal environment while the coast interacts with spilling and plunging breakers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.14612031M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.14612031M"><span>Optical <span class="hlt">model</span> with multiple band <span class="hlt">couplings</span> using soft rotator structure</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Martyanov, Dmitry; Soukhovitskii, Efrem; Capote, Roberto; Quesada, Jose Manuel; Chiba, Satoshi</p> <p>2017-09-01</p> <p>A new dispersive <span class="hlt">coupled</span>-channel optical <span class="hlt">model</span> (DCCOM) is derived that describes nucleon scattering on 238U and 232Th targets using a soft-rotator-<span class="hlt">model</span> (SRM) description of the collective levels of the target nucleus. SRM Hamiltonian parameters are adjusted to the observed collective levels of the target nucleus. SRM nuclear <span class="hlt">wave</span> functions (mixed in K quantum number) have been used to calculate <span class="hlt">coupling</span> matrix elements of the generalized optical <span class="hlt">model</span>. Five rotational bands are <span class="hlt">coupled</span>: the ground-state band, β-, γ-, non-axial- bands, and a negative parity band. Such <span class="hlt">coupling</span> scheme includes almost all levels below 1.2 MeV of excitation energy of targets. The "effective" deformations that define inter-band <span class="hlt">couplings</span> are derived from SRM Hamiltonian parameters. Conservation of nuclear volume is enforced by introducing a monopolar deformed potential leading to additional <span class="hlt">couplings</span> between rotational bands. The present DCCOM describes the total cross section differences between 238U and 232Th targets within experimental uncertainty from 50 keV up to 200 MeV of neutron incident energy. SRM <span class="hlt">couplings</span> and volume conservation allow a precise calculation of the compound-nucleus (CN) formation cross sections, which is significantly different from the one calculated with rigid-rotor potentials with any number of <span class="hlt">coupled</span> levels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25113099','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25113099"><span>Resilience of branching and massive corals to <span class="hlt">wave</span> loading under sea level rise--a <span class="hlt">coupled</span> computational fluid dynamics-structural analysis.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Baldock, Tom E; Karampour, Hassan; Sleep, Rachael; Vyltla, Anisha; Albermani, Faris; Golshani, Aliasghar; Callaghan, David P; Roff, George; Mumby, Peter J</p> <p>2014-09-15</p> <p>Measurements of coral structural strength are <span class="hlt">coupled</span> with a fluid dynamics-structural analysis to investigate the resilience of coral to <span class="hlt">wave</span> loading under sea level rise and a typical Great Barrier Reef lagoon <span class="hlt">wave</span> climate. The measured structural properties were used to determine the <span class="hlt">wave</span> conditions and flow velocities that lead to structural failure. Hydrodynamic <span class="hlt">modelling</span> was subsequently used to investigate the type of the bathymetry where coral is most vulnerable to breakage under cyclonic <span class="hlt">wave</span> conditions, and how sea level rise (SLR) changes this vulnerability. Massive corals are determined not to be vulnerable to <span class="hlt">wave</span> induced structural damage, whereas branching corals are susceptible at <span class="hlt">wave</span> induced orbital velocities exceeding 0.5m/s. <span class="hlt">Model</span> results from a large suite of idealised bathymetry suggest that SLR of 1m or a loss of skeleton strength of order 25% significantly increases the area of reef flat where branching corals are exposed to damaging <span class="hlt">wave</span> induced flows. Copyright © 2014 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/20389341','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/20389341"><span>Prism-<span class="hlt">coupled</span> Cherenkov phase-matched terahertz <span class="hlt">wave</span> generation using a DAST crystal.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Suizu, Koji; Shibuya, Takayuki; Uchida, Hirohisa; Kawase, Kodo</p> <p>2010-02-15</p> <p>Terahertz (THz) <span class="hlt">wave</span> generation based on nonlinear frequency conversion is a promising method for realizing a tunable monochromatic high-power THz-<span class="hlt">wave</span> source. Unfortunately, many nonlinear crystals have strong absorption in the THz frequency region. This limits efficient and widely tunable THz-<span class="hlt">wave</span> generation. The Cherenkov phase-matching method is one of the most promising techniques for overcoming these problems. Here, we propose a prism-<span class="hlt">coupled</span> Cherenkov phase-matching (PCC-PM) method, in which a prism with a suitable refractive index at THz frequencies is <span class="hlt">coupled</span> to a nonlinear crystal. This has the following advantages. Many crystals can be used as THz-<span class="hlt">wave</span> emitters; the phase-matching condition inside the crystal does not have to be observed; the absorption of the crystal does not prevent efficient generation of radiation; and pump sources with arbitrary wavelengths can be employed. Here we demonstrate PCC-PM THz-<span class="hlt">wave</span> generation using the organic crystal 4-dimethylamino-N-metyl-4-stilbazolium tosylate (DAST) and a Si prism coupler. We obtain THz-<span class="hlt">wave</span> radiation with tunability of approximately 0.1 to 10 THz and with no deep absorption features resulting from the absorption spectrum of the crystal. The obtained spectra did not depend on the pump wavelength in the range 1300 to 1450 nm. This simple technique shows promise for generating THz radiation using a wide variety of nonlinear crystals.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2722927','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2722927"><span>Surface <span class="hlt">Current</span> Density Mapping for Identification of Gastric Slow <span class="hlt">Wave</span> Propagation</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Bradshaw, L. A.; Cheng, L. K.; Richards, W. O.; Pullan, A. J.</p> <p>2009-01-01</p> <p>The magnetogastrogram records clinically relevant parameters of the electrical slow <span class="hlt">wave</span> of the stomach noninvasively. Besides slow <span class="hlt">wave</span> frequency, gastric slow <span class="hlt">wave</span> propagation velocity is a potentially useful clinical indicator of the state of health of gastric tissue, but it is a difficult parameter to determine from noninvasive bioelectric or biomagnetic measurements. We present a method for computing the surface <span class="hlt">current</span> density (SCD) from multichannel magnetogastrogram recordings that allows computation of the propagation velocity of the gastric slow <span class="hlt">wave</span>. A moving dipole source <span class="hlt">model</span> with hypothetical as well as realistic biomagnetometer parameters demonstrates that while a relatively sparse array of magnetometer sensors is sufficient to compute a single average propagation velocity, more detailed information about spatial variations in propagation velocity requires higher density magnetometer arrays. Finally, the method is validated with simultaneous MGG and serosal EMG measurements in a porcine subject. PMID:19403355</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000032540&hterms=project+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dproject%2Bwaves','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000032540&hterms=project+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dproject%2Bwaves"><span>Laboratory Study of Water Surface Roughness Generation by <span class="hlt">Wave-Current</span> Interaction</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Klinke, Jochen</p> <p>2000-01-01</p> <p>Within the framework of this project, the blocking of <span class="hlt">waves</span> by inhomogeneous <span class="hlt">currents</span> was studied. A laboratory experiment was conducted in collaboration with Steven R. Long at the linear <span class="hlt">wave</span> tank of the NASA Air-Sea Interaction Facility, Wallops Island, VA during May 1999. Mechanically-generated <span class="hlt">waves</span> were blocked approximately 3m upstream from the <span class="hlt">wave</span> paddle by an opposing <span class="hlt">current</span>. A false bottom was used to obtain a spatially varying flow field in the measurement section of the <span class="hlt">wave</span> tank. We used an imaging slope gauge, which was mounted directly underneath the sloping section of the false tank bottom to observe the <span class="hlt">wave</span> field. For a given <span class="hlt">current</span> speed, the amplitude and the frequency of the <span class="hlt">waves</span> was adjusted so that the blocking occurred within the observed footprint. Image sequences of up to 600 images at up 100 Hz sampling rate were recorded for an area of approximately 25cm x 25cm. Unlike previous measurements with <span class="hlt">wave</span> wire gauges, the captured image sequences show the generation of the capillary <span class="hlt">waves</span> at the blocking point and give detailed insight into the spatial and temporal evolution of the blocking process. The image data were used to study the <span class="hlt">wave-current</span> interaction for <span class="hlt">currents</span> from 5 to 25 cm/s and <span class="hlt">waves</span> with frequencies between 1 and 3 Hz. First the images were calibrated with regard to size and slope. Then standard Fourier techniques as well the empirical mode decomposition method developed by Dr. Norden Huang and Dr. Steven R. Long were employed to quantify the <span class="hlt">wave</span> number downshift from the gravity to the capillary regime.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://dx.doi.org/10.1016/j.ocemod.2011.12.008','USGSPUBS'); return false;" href="http://dx.doi.org/10.1016/j.ocemod.2011.12.008"><span>Ocean-atmosphere dynamics during Hurricane Ida and Nor'Ida: An application of the <span class="hlt">coupled</span> ocean-;atmosphere–wave–sediment transport (COAWST) <span class="hlt">modeling</span> system</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Olabarrieta, Maitane; Warner, John C.; Armstrong, Brandy N.; Zambon, Joseph B.; He, Ruoying</p> <p>2012-01-01</p> <p>The <span class="hlt">coupled</span> ocean–atmosphere–wave–sediment transport (COAWST) <span class="hlt">modeling</span> system was used to investigate atmosphere–ocean–<span class="hlt">wave</span> interactions in November 2009 during Hurricane Ida and its subsequent evolution to Nor'Ida, which was one of the most costly storm systems of the past two decades. One interesting aspect of this event is that it included two unique atmospheric extreme conditions, a hurricane and a nor'easter storm, which developed in regions with different oceanographic characteristics. Our <span class="hlt">modeled</span> results were compared with several data sources, including GOES satellite infrared data, JASON-1 and JASON-2 altimeter data, CODAR measurements, and <span class="hlt">wave</span> and tidal information from the National Data Buoy Center (NDBC) and the National Tidal Database. By performing a series of numerical runs, we were able to isolate the effect of the interaction terms between the atmosphere (<span class="hlt">modeled</span> with Weather Research and Forecasting, the WRF <span class="hlt">model</span>), the ocean (<span class="hlt">modeled</span> with Regional Ocean <span class="hlt">Modeling</span> System (ROMS)), and the <span class="hlt">wave</span> propagation and generation <span class="hlt">model</span> (<span class="hlt">modeled</span> with Simulating <span class="hlt">Waves</span> Nearshore (SWAN)). Special attention was given to the role of the ocean surface roughness. Three different ocean roughness closure <span class="hlt">models</span> were analyzed: DGHQ (which is based on <span class="hlt">wave</span> age), TY2001 (which is based on <span class="hlt">wave</span> steepness), and OOST (which considers both the effects of <span class="hlt">wave</span> age and steepness). Including the ocean roughness in the atmospheric module improved the wind intensity estimation and therefore also the wind <span class="hlt">waves</span>, surface <span class="hlt">currents</span>, and storm surge amplitude. For example, during the passage of Hurricane Ida through the Gulf of Mexico, the wind speeds were reduced due to <span class="hlt">wave</span>-induced ocean roughness, resulting in better agreement with the measured winds. During Nor'Ida, including the <span class="hlt">wave</span>-induced surface roughness changed the form and dimension of the main low pressure cell, affecting the intensity and direction of the winds. The combined <span class="hlt">wave</span> age- and <span class="hlt">wave</span> steepness</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1995PhyC..250..282R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1995PhyC..250..282R"><span>Origin of intrinsic Josephson <span class="hlt">coupling</span> in the cuprates and its relation to order parameter symmetry: An incoherent hopping <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>Radtke, R. J.; Levin, K.</p> <p>1995-02-01</p> <p>Experiments on the cuprate superconductors demonstrate that these materials may be viewed as a stack of Josephson junctions along the direction normal to the CuO 2 planes (the c-axis). In this paper, we present a <span class="hlt">model</span> which describes this intrinsic Josephson <span class="hlt">coupling</span> in terms of incherent quasiparticle hopping along the c-axis arising from <span class="hlt">wave</span>-function overlap, impurity-assisted hopping, and boson-assised hopping. We use this <span class="hlt">model</span> to compute the magnitude and temperature T dependence of the resulting Josephson critical <span class="hlt">current</span> jc( T) for s- and d-<span class="hlt">wave</span> superconductors. Contrary to other approaches, d-<span class="hlt">wave</span> pairing in this <span class="hlt">model</span> is compatible with an intrinsic Josephson effect at all hole concentrations and leads to jc( T) αT at low T. By parameterizing our theory with c-axis resistivity data from YBa 2Cu 3O 7-δ (YBCO), we estimate jc( T) for optimally doped and underdoped members of this family. jc( T) can be measured either directly or indirectly through microwave penetration depth experiments, and <span class="hlt">current</span> measurements on Bi 2Sr 2CaCu 2O 8 and La 2- xSr xCuO 4 are found to be consistent with s-<span class="hlt">wave</span> pairing and the dominance of assisted hopping processes. The situation in YBCO is still unclear, but our estimates suggest that further experiments on this compound would be of great help in elucidating the validity of our <span class="hlt">model</span> in general and the pairing symmetry in particular.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22599917-coupling-electrostatic-ion-cyclotron-ion-acoustic-waves-solar-wind','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22599917-coupling-electrostatic-ion-cyclotron-ion-acoustic-waves-solar-wind"><span><span class="hlt">Coupling</span> of electrostatic ion cyclotron and ion acoustic <span class="hlt">waves</span> in the solar wind</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>Sreeraj, T., E-mail: sreerajt13@iigs.iigm.res.in; Singh, S. V., E-mail: satyavir@iigs.iigm.res.in; Lakhina, G. S., E-mail: gslakhina@gmail.com</p> <p>2016-08-15</p> <p>The <span class="hlt">coupling</span> of electrostatic ion cyclotron and ion acoustic <span class="hlt">waves</span> is examined in three component magnetized plasma consisting of electrons, protons, and alpha particles. In the theoretical <span class="hlt">model</span> relevant to solar wind plasma, electrons are assumed to be superthermal with kappa distribution and protons as well as alpha particles follow the fluid dynamical equations. A general linear dispersion relation is derived for such a plasma system which is analyzed both analytically and numerically. For parallel propagation, electrostatic ion cyclotron (proton and helium cyclotron) and ion acoustic (slow and fast) modes are decoupled. For oblique propagation, <span class="hlt">coupling</span> between the cyclotron andmore » acoustic modes occurs. Furthermore, when the angle of propagation is increased, the separation between acoustic and cyclotron modes increases which is an indication of weaker <span class="hlt">coupling</span> at large angle of propagation. For perpendicular propagation, only cyclotron modes are observed. The effect of various parameters such as number density and temperature of alpha particles and superthermality on dispersion characteristics is examined in details. The <span class="hlt">coupling</span> between various modes occurs for small values of wavenumber.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1156603','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1156603"><span><span class="hlt">Wave</span> Energy Converter (WEC) Array Effects on <span class="hlt">Wave</span> <span class="hlt">Current</span> and Sediment Circulation: Monterey Bay CA.</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>Roberts, Jesse D.; Jones, Craig; Magalen, Jason</p> <p>2014-09-01</p> <p>The goal s of this study were to develop tools to quantitatively characterize environments where <span class="hlt">wave</span> energy converter ( WEC ) devices may be installed and to assess e ffects on hydrodynamics and lo cal sediment transport. A large hypothetical WEC array was investigated using <span class="hlt">wave</span>, hydrodynamic, and sediment transport <span class="hlt">models</span> and site - specific average and storm conditions as input. The results indicated that there were significant changes in sediment s izes adjacent to and in the lee of the WEC array due to reduced <span class="hlt">wave</span> energy. The circulation in the lee of the array was also altered; moremore » intense onshore <span class="hlt">currents</span> were generated in the lee of the WECs . In general, the storm case and the average case show ed the same qualitative patterns suggesting that these trends would be maintained throughout the year. The framework developed here can be used to design more efficient arrays while minimizing impacts on nearshore environmen ts.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28505714','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28505714"><span>Interactions of localized <span class="hlt">wave</span> structures and dynamics in the defocusing <span class="hlt">coupled</span> nonlinear Schrödinger equations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Guoqiang; Yan, Zhenya; Wen, Xiao-Yong; Chen, Yong</p> <p>2017-04-01</p> <p>We investigate the defocusing <span class="hlt">coupled</span> nonlinear Schrödinger equations from a 3×3 Lax pair. The Darboux transformations with the nonzero plane-<span class="hlt">wave</span> solutions are presented to derive the newly localized <span class="hlt">wave</span> solutions including dark-dark and bright-dark solitons, breather-breather solutions, and different types of new vector rogue <span class="hlt">wave</span> solutions, as well as interactions between distinct types of localized <span class="hlt">wave</span> solutions. Moreover, we analyze these solutions by means of parameters modulation. Finally, the perturbed <span class="hlt">wave</span> propagations of some obtained solutions are explored by means of systematic simulations, which demonstrates that nearly stable and strongly unstable solutions. Our research results could constitute a significant contribution to explore the distinct nonlinear <span class="hlt">waves</span> (e.g., dark solitons, breather solutions, and rogue <span class="hlt">wave</span> solutions) dynamics of the <span class="hlt">coupled</span> system in related fields such as nonlinear optics, plasma physics, oceanography, and Bose-Einstein condensates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014ApJ...789..109G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014ApJ...789..109G"><span>Energy Loss of Solar p Modes due to the Excitation of Magnetic Sausage Tube <span class="hlt">Waves</span>: Importance of <span class="hlt">Coupling</span> the Upper Atmosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gascoyne, A.; Jain, R.; Hindman, B. W.</p> <p>2014-07-01</p> <p>We consider damping and absorption of solar p modes due to their energy loss to magnetic tube <span class="hlt">waves</span> that can freely carry energy out of the acoustic cavity. The <span class="hlt">coupling</span> of p modes and sausage tube <span class="hlt">waves</span> is studied in a <span class="hlt">model</span> atmosphere composed of a polytropic interior above which lies an isothermal upper atmosphere. The sausage tube <span class="hlt">waves</span>, excited by p modes, propagate along a magnetic fibril which is assumed to be a vertically aligned, stratified, thin magnetic flux tube. The deficit of p-mode energy is quantified through the damping rate, Γ, and absorption coefficient, α. The variation of Γ and α as a function of frequency and the tube's plasma properties is studied in detail. Previous similar studies have considered only a subphotospheric layer, <span class="hlt">modeled</span> as a polytrope that has been truncated at the photosphere. Such studies have found that the resulting energy loss by the p modes is very sensitive to the upper boundary condition, which, due to the lack of an upper atmosphere, have been imposed in a somewhat ad hoc manner. The <span class="hlt">model</span> presented here avoids such problems by using an isothermal layer to <span class="hlt">model</span> the overlying atmosphere (chromosphere, and, consequently, allows us to analyze the propagation of p-mode-driven sausage <span class="hlt">waves</span> above the photosphere. In this paper, we restrict our attention to frequencies below the acoustic cut off frequency. We demonstrate the importance of <span class="hlt">coupling</span> all <span class="hlt">waves</span> (acoustic, magnetic) in the subsurface solar atmosphere with the overlying atmosphere in order to accurately <span class="hlt">model</span> the interaction of solar f and p modes with sausage tube <span class="hlt">waves</span>. In calculating the absorption and damping of p modes, we find that for low frequencies, below ≈3.5 mHz, the isothermal atmosphere, for the two-region <span class="hlt">model</span>, behaves like a stress-free boundary condition applied at the interface (z = -z 0).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhRvB..86p5408W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhRvB..86p5408W"><span>Dynamics of <span class="hlt">coupled</span> plasmon polariton <span class="hlt">wave</span> packets excited at a subwavelength slit in optically thin metal films</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Lei-Ming; Zhang, Lingxiao; Seideman, Tamar; Petek, Hrvoje</p> <p>2012-10-01</p> <p>We study by numerical simulations the excitation and propagation dynamics of <span class="hlt">coupled</span> surface plasmon polariton (SPP) <span class="hlt">wave</span> packets (WPs) in optically thin Ag films and a bulk Ag/vacuum interface under the illumination of a subwavelength slit by 400 nm continuous <span class="hlt">wave</span> (cw) and femtosecond pulsed light. The generated surface fields include contributions from both SPPs and quasicylindrical <span class="hlt">waves</span>, which dominate in different regimes. We explore aspects of the <span class="hlt">coupled</span> SPP modes in Ag thin films, including symmetry, propagation, attenuation, and the variation of <span class="hlt">coupling</span> with incident angle and film thickness. Simulations of the electromagnetic transients initiated with femtosecond pulses reveal new features of <span class="hlt">coupled</span> SPP WP generation and propagation in thin Ag films. Our results show that, under pulsed excitation, the SPP modes in an Ag thin film break up into two distinct bound surface <span class="hlt">wave</span> packets characterized by marked differences in symmetries, group velocities, attenuation lengths, and dispersion properties. The nanometer spatial and femtosecond temporal scale excitation and propagation dynamics of the <span class="hlt">coupled</span> SPP WPs are revealed in detail by movies recording the evolution of their transient field distributions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhLA..382..412E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhLA..382..412E"><span>Bifurcation analysis for ion acoustic <span class="hlt">waves</span> in a strongly <span class="hlt">coupled</span> plasma including trapped electrons</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>El-Labany, S. K.; El-Taibany, W. F.; Atteya, A.</p> <p>2018-02-01</p> <p>The nonlinear ion acoustic <span class="hlt">wave</span> propagation in a strongly <span class="hlt">coupled</span> plasma composed of ions and trapped electrons has been investigated. The reductive perturbation method is employed to derive a modified Korteweg-de Vries-Burgers (mKdV-Burgers) equation. To solve this equation in case of dissipative system, the tangent hyperbolic method is used, and a shock <span class="hlt">wave</span> solution is obtained. Numerical investigations show that, the ion acoustic <span class="hlt">waves</span> are significantly modified by the effect of polarization force, the trapped electrons and the viscosity coefficients. Applying the bifurcation theory to the dynamical system of the derived mKdV-Burgers equation, the phase portraits of the traveling <span class="hlt">wave</span> solutions of both of dissipative and non-dissipative systems are analyzed. The present results could be helpful for a better understanding of the <span class="hlt">waves</span> nonlinear propagation in a strongly <span class="hlt">coupled</span> plasma, which can be produced by photoionizing laser-cooled and trapped electrons [1], and also in neutron stars or white dwarfs interior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020022491&hterms=hydra&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dhydra','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020022491&hterms=hydra&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dhydra"><span>A Self-Consistent <span class="hlt">Model</span> of the Interacting Ring <span class="hlt">Current</span> Ions with Electromagnetic ICWs</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Khazanov, G. V.; Gamayunov, K. V.; Jordanova, V. K.; Krivorutsky, E. N.; Whitaker, Ann F. (Technical Monitor)</p> <p>2001-01-01</p> <p>Initial results from a newly developed <span class="hlt">model</span> of the interacting ring <span class="hlt">current</span> ions and ion cyclotron <span class="hlt">waves</span> are presented. The <span class="hlt">model</span> is based on the system of two bound kinetic equations: one equation describes the ring <span class="hlt">current</span> ion dynamics, and another equation describes <span class="hlt">wave</span> evolution. The system gives a self-consistent description of ring <span class="hlt">current</span> ions and ion cyclotron <span class="hlt">waves</span> in a quasilinear approach. These two equations were solved on a global scale under non steady-state conditions during the May 2-5, 1998 storm. The structure and dynamics of the ring <span class="hlt">current</span> proton precipitating flux regions and the <span class="hlt">wave</span> active zones at three time cuts around initial, main, and late recovery phases of the May 4, 1998 storm phase are presented and discussed in detail. Comparisons of the <span class="hlt">model</span> <span class="hlt">wave</span>-ion data with the Polar/HYDRA and Polar/MFE instruments results are presented..</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..19.2037D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..19.2037D"><span>Future Evolution of Marine Heat <span class="hlt">Waves</span> in the Mediterranean: <span class="hlt">Coupled</span> Regional Climate Projections</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Darmaraki, Sofia; Somot, Samuel; Sevault, Florence; Nabat, Pierre; Cavicchia, Leone; Djurdjevic, Vladimir; Cabos, William; Sein, Dmitry</p> <p>2017-04-01</p> <p>FUTURE EVOLUTION OF MARINE HEAT <span class="hlt">WAVES</span> IN THE MEDITERRANEAN : <span class="hlt">COUPLED</span> REGIONAL CLIMATE PROJECTIONS The Mediterranean area is identified as a « Hot Spot » region, vulnerable to future climate change with potentially strong impacts over the sea. By 2100, climate <span class="hlt">models</span> predict increased warming over the sea surface, with possible implications on the Mediterranean thermohaline and surface circulation,associated also with severe impacts on the ecosystems (e.g. fish habitat loss, species extinction and migration, invasive species). However, a robust assesment of the future evolution of the extreme marine temperatures remains still an open issue of primary importance, under the anthropogenic pressure. In this context, we study here the probability and characteristics of marine heat <span class="hlt">wave</span> (MHW) occurrence in the Mediterranean Sea in future climate projections. To this end, we use an ensemble of fully <span class="hlt">coupled</span> regional climate system <span class="hlt">models</span> (RCSM) from the Med- CORDEX initiative. This multi-<span class="hlt">model</span> approach includes a high-resolution representation of the atmospheric, land and ocean component, with a free air-sea interface.Specifically, dedicated simulations for the 20th and the 21st century are carried out with respect to the different IPCC-AR5 socioeconomic scenarios (1950-2100, RCP8.5, RCP4.5, RCP2.6). <span class="hlt">Model</span> evaluation for the historical period is performed using satellite and in situ data. Then, the variety of factors that can cause the MHW (e.g. direct radiative forcing, ocean advection, stratification change) are examined to disentangle the dominant driving force. Finally, the spatial variability and temporal evolution of MHW are analyzed on an annual basis, along with additional integrated indicators, useful for marine ecosystems.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070002065&hterms=Plasma+Ring&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DPlasma%2BRing','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070002065&hterms=Plasma+Ring&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3DPlasma%2BRing"><span>Are Ring <span class="hlt">Current</span> Ions Lost in Electromagnetic Ion Cyclotron <span class="hlt">Wave</span> Dispersion Relation?</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Khazanov, G. V.; Gamayunov, K. V.</p> <p>2006-01-01</p> <p>Electromagnetic ion cyclotron (EMIC) <span class="hlt">waves</span> are widely observed in the inner and outer magnetosphere, at geostationary orbit, at high latitudes along the plasmapause, and at the ionospheric altitudes. Interaction of the Ring <span class="hlt">Current</span> (RC) ions and EMIC <span class="hlt">waves</span> causes ion scattering into the loss cone and leads to decay of the RC, especially during the main phase of storms when the RC decay times of about one hour or less are observed. The oblique EMIC <span class="hlt">waves</span> damp due to Landau resonance with the thermal plasmaspheric electrons, and subsequent transport of the dissipating <span class="hlt">wave</span> energy into the ionosphere below causes an ionosphere temperature enhancement. Induced scattering of these <span class="hlt">waves</span> by the plasmaspheric thermal ions leads to ion temperature enhancement, and forms a so-called hot zone near the plasmapause where the temperature of core plasma ions can reach tens of thousands of degrees. Relativistic electrons in the outer radiation belt also interact well with the EMIC <span class="hlt">waves</span>, and during the main and/or recovery phases of the storms these electrons can easily be scattered into the loss cone over a time scale from several hours to a day. The plasma density distribution in the magnetosphere and the ion content play a critical role in EMIC <span class="hlt">wave</span> generation and propagation, but the <span class="hlt">wave</span> dispersion relation in the known RC-EMIC <span class="hlt">wave</span> interaction <span class="hlt">models</span> is assumed to be determined by the thermal plasma distribution only. In these <span class="hlt">models</span>, the modification of the EMIC <span class="hlt">wave</span> dispersion relation caused by the RC ions is not taken into account, and the RC ions are only treated as a source of free energy in order to generate EMIC <span class="hlt">waves</span>. At the same time, the RC ions can dominate the thermal magnetospheric content in the night MLT sector at great L shells during the main and/or recovery storm phase. In this study, using our self-consistent RC-EMIC <span class="hlt">wave</span> <span class="hlt">model</span> [Khazanov et al., 2006], we simulate the May 1998 storm in order to quantify the global EMIC <span class="hlt">wave</span> redistribution caused by</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_23 --> <div id="page_24" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="461"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20070002141&hterms=Plasma+Ring&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DPlasma%2BRing','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20070002141&hterms=Plasma+Ring&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3DPlasma%2BRing"><span>Effect of Ring <span class="hlt">Current</span> Ions on Electromagnetic Ion Cyclotron <span class="hlt">Wave</span> Dispersion Relation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gamayunov, K. V.; Khazanov, G. V.</p> <p>2006-01-01</p> <p>Electromagnetic ion cyclotron (EMIC) <span class="hlt">waves</span> are widely observed in the inner and outer magnetosphere, at geostationary orbit, at high latitudes along the plasmapause, and at the ionospheric altitudes. Interaction of the Ring <span class="hlt">Current</span> (RC) ions and EMIC <span class="hlt">waves</span> causes ion scattering into the loss cone and leads to decay of the RC, especially during the main phase of storms when the RC decay times of about one hour or less are observed. The oblique EMIC <span class="hlt">waves</span> damp due to Landau resonance with the thermal plasmaspheric electrons, and subsequent transport of the dissipating <span class="hlt">wave</span> energy into the ionosphere below causes an ionosphere temperature enhancement. Induced scattering of these <span class="hlt">waves</span> by the plasmaspheric thermal ions leads to ion temperature enhancement, and forms a so-called hot zone near the plasmapause where the temperature of core plasma ions can reach tens of thousands of degrees. Relativistic electrons in the outer radiation belt also interact well with the EMIC <span class="hlt">waves</span>, and during the main and/or recovery phases of the storms these electrons can easily be scattered into the loss cone over a time scale from several hours to a day. The plasma density distribution in the magnetosphere and the ion content play a critical role in EMIC <span class="hlt">wave</span> generation and propagation, but the <span class="hlt">wave</span> dispersion relation in the known RC-EMIC <span class="hlt">wave</span> interaction <span class="hlt">models</span> is assumed to be determined by the thermal plasma distribution only. In these <span class="hlt">models</span>, the modification of the EMIC <span class="hlt">wave</span> dispersion relation caused by the RC ions is not taken into account, and the RC ions are only treated as a source of free energy in order to generate EMIC <span class="hlt">waves</span>. At the same time, the RC ions can dominate the thermal magnetospheric content in the night MLT sector at great L shells during the main and/or recovery storm phase. In this study, using our self-consistent RC-EMIC <span class="hlt">wave</span> <span class="hlt">model</span> [Khazanov et al., 2006], we simulate the May 1998 storm in order to quantify the global EMIC <span class="hlt">wave</span> redistribution caused by</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/4301320','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/biblio/4301320"><span>SQUARE <span class="hlt">WAVE</span> AMPLIFIER</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Leavitt, M.A.; Lutz, I.C.</p> <p>1958-08-01</p> <p>An amplifier circuit is described for amplifying sigmals having an alternating <span class="hlt">current</span> component superimposed upon a direct <span class="hlt">current</span> component, without loss of any segnnent of the alternating <span class="hlt">current</span> component. The general circuit arrangement includes a vibrator, two square <span class="hlt">wave</span> amplifiers, and recombination means. The amplifier input is connected to the vibrating element of the vibrator and is thereby alternately applied to the input of each square <span class="hlt">wave</span> amplifier. The detailed circuitry of the recombination means constitutes the novelty of the annplifier and consists of a separate, dual triode amplifier <span class="hlt">coupled</span> to the output of each square <span class="hlt">wave</span> amplifier with a recombination connection from the plate of one amplifier section to a grid of one section of the other amplifier. The recombination circuit has provisions for correcting distortion caused by overlapping of the two square <span class="hlt">wave</span> voltages from the square <span class="hlt">wave</span> amplifiers.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25615346','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25615346"><span>Spatiotemporal splitting of global eigenmodes due to cross-field <span class="hlt">coupling</span> via vortex dynamics in drift <span class="hlt">wave</span> turbulence.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Brandt, C; Thakur, S C; Light, A D; Negrete, J; Tynan, G R</p> <p>2014-12-31</p> <p>Spatiotemporal splitting events of drift <span class="hlt">wave</span> (DW) eigenmodes due to nonlinear <span class="hlt">coupling</span> are investigated in a cylindrical helicon plasma device. DW eigenmodes in the radial-azimuthal cross section have been experimentally observed to split at radial locations and recombine into the global eigenmode with a time shorter than the typical DW period (t≪fDW(-1)). The number of splits correlates with the increase of turbulence. The observed dynamics can be theoretically reproduced by a Kuramoto-type <span class="hlt">model</span> of a network of radially <span class="hlt">coupled</span> azimuthal eigenmodes. <span class="hlt">Coupling</span> by E×B-vortex convection cell dynamics and ion gyro radii motion leads to cross-field synchronization and occasional mode splitting events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26871083','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26871083"><span>Rogue <span class="hlt">waves</span> for a system of <span class="hlt">coupled</span> derivative nonlinear Schrödinger equations.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chan, H N; Malomed, B A; Chow, K W; Ding, E</p> <p>2016-01-01</p> <p>Rogue <span class="hlt">waves</span> (RWs) are unexpectedly strong excitations emerging from an otherwise tranquil background. The nonlinear Schrödinger equation (NLSE), a ubiquitous <span class="hlt">model</span> with wide applications to fluid mechanics, optics, plasmas, etc., exhibits RWs only in the regime of modulation instability (MI) of the background. For a system of multiple waveguides, the governing <span class="hlt">coupled</span> NLSEs can produce regimes of MI and RWs, even if each component has dispersion and cubic nonlinearity of opposite signs. A similar effect is demonstrated here for a system of <span class="hlt">coupled</span> derivative NLSEs (DNLSEs) where the special feature is the nonlinear self-steepening of narrow pulses. More precisely, these additional regimes of MI and RWs for <span class="hlt">coupled</span> DNLSEs depend on the mismatch in group velocities between the components, and the parameters for cubic nonlinearity and self-steepening. RWs considered in this paper differ from those of the NLSEs in terms of the amplification ratio and criteria of existence. Applications to optics and plasma physics are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1911744A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1911744A"><span>Progress on <span class="hlt">wave</span>-ice interactions: satellite observations and <span class="hlt">model</span> parameterizations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ardhuin, Fabrice; Boutin, Guillaume; Dumont, Dany; Stopa, Justin; Girard-Ardhuin, Fanny; Accensi, Mickael</p> <p>2017-04-01</p> <p>In the open ocean, numerical <span class="hlt">wave</span> <span class="hlt">models</span> have their largest errors near sea ice, and, until recently, virtually no <span class="hlt">wave</span> data was available in the sea ice to. Further, <span class="hlt">wave</span>-ice interaction processes may play an important role in the Earth system. In particular, <span class="hlt">waves</span> may break up an ice layer into floes, with significant impact on air-sea fluxes. With thinner Arctic ice, this process may contribut to the growing similarity between Arctic and Antarctic sea ice. In return, the ice has a strong damping impact on the <span class="hlt">waves</span> that is highly variable and not understood. Here we report progress on parameterizations of <span class="hlt">waves</span> interacting with a single ice layer, as implemented in the WAVEWATCH III <span class="hlt">model</span> (WW3 Development Group, 2016), and based on few in situ observations, but extensive data derived from Synthetic Aperture Radars (SARs). Our parameterizations combine three processes. First a parameterization for the energy-conserving scattering of <span class="hlt">waves</span> by ice floes (assuming isotropic back-scatter), which has very little effect on dominant <span class="hlt">waves</span> of periods larger than 7 s, consistent with the observed narrow directional spectra and short travel times. Second, we implemented a basal friction below the ice layer (Stopa et al. The Cryosphere, 2016). Third, we use a secondary creep associated with ice flexure (Cole et al. 1998) adapted to random <span class="hlt">waves</span>. These three processes (scattering, friction and creep) are strongly dependent on the maximum floe size. We have thus included an estimation of the potential floe size based on an ice flexure failure estimation adapted from Williams et al. (2013). This combination of dissipation and scattering is tested against measured patterns of <span class="hlt">wave</span> height and directional spreading, and evidence of ice break-up, all obtained from SAR imagery (Ardhuin et al. 2017), and some in situ data (Collins et al. 2015). The combination of creep and friction is required to reproduce a strong reduction in <span class="hlt">wave</span> attenuation in broken ice as observed by Collins</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSHI51A..04L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSHI51A..04L"><span>The Effect of <span class="hlt">Waves</span> on the Tidal-Stream Energy Resource</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lewis, M. J.; Neill, S. P.; Robins, P. E.; Hashemi, M. R.</p> <p>2016-02-01</p> <p>The tidal-stream energy resource is typically estimated using depth-averaged "tide-only" hydrodynamic <span class="hlt">models</span> and do not consider the influence of <span class="hlt">waves</span>. We find that <span class="hlt">waves</span> will reduce the available resource, and the <span class="hlt">wave</span> climate needs to be considered when designing a resilient and efficient tidal-stream energy device. Using well-validated oceanographic <span class="hlt">models</span> of the Irish Sea and Northwest European shelf, we show tidal-stream energy sites with quiescent <span class="hlt">wave</span> climates are extremely limited, with limited sea-space and limited scope for future development. To fully realise the potential of tidal-stream energy and to ensure globally deployable devices, the influence of <span class="hlt">waves</span> on the resource and turbines must be considered. The effect of <span class="hlt">waves</span> upon the tidal <span class="hlt">current</span> was investigated using observations (ADCP and <span class="hlt">wave</span> buoy time-series), and a state-of-the-art, 3-dimensional, dynamically <span class="hlt">coupled</span> <span class="hlt">wave</span>-tide <span class="hlt">model</span> (COAWST). The presence of <span class="hlt">waves</span> reduced the depth-averaged tidal <span class="hlt">current</span>, which reduced the potential extractable power by 10% per metre <span class="hlt">wave</span> height increase. To ensure resilience and survivability, tidal-stream energy device may cease to produce electricity during extremes (often called downtime), however the <span class="hlt">wave</span> conditions threshold for device shut-down is unknown, and requires future work. The presence of <span class="hlt">waves</span> will also effect turbine performance and design criteria; for example, the presence of <span class="hlt">waves</span> was found to alter the shape of the velocity profile, and <span class="hlt">wave-current</span> misalignment (<span class="hlt">waves</span> propagating at an angle oblique to the plane of tidal flow) was found to occur for a significant amount of time at many potential tidal-stream energy sites. Therefore, <span class="hlt">waves</span> reduced the available resource, furthermore the influence of <span class="hlt">waves</span> on the interaction between tidal energy devices and the tidal-stream resource needs to be characterised in physically-scaled tank experiments and computational fluid dynamics (CFD) numerical <span class="hlt">models</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ECSS..202....1B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ECSS..202....1B"><span><span class="hlt">Wave-current</span> generated turbulence over hemisphere bottom roughness</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barman, Krishnendu; Roy, Sayahnya; Debnath, Koustuv</p> <p>2018-03-01</p> <p>The present paper explores the effect of <span class="hlt">wave-current</span> interaction on the turbulence characteristics and the distribution of eddy structure over artificially crammed rough bed prepared with hemispheres. The effect of the surface <span class="hlt">wave</span> on temporal and spatial-averaged mean velocity, intensity, Reynolds shear stress over, within cavity and above the hemispherical bed are discussed. Detailed three-dimensional time series velocity components were measured in a tilting flume using 3-D Micro-Acoustic Doppler Velocimeter (ADV) at a Reynolds number, 62 × 103. This study reports the fractional contributions of burst-sweep cycles dominating the total shear stress near hemispherical rough surface both for <span class="hlt">current</span> only flow as well as for <span class="hlt">wave</span>-induced cases. Wavelet analysis of the fluctuating velocity signal shows that the superimposed <span class="hlt">wave</span> of frequency 1 Hz is capable of modulating the energy containing a range of velocity fluctuations at the mid-depth of the cavity region (formed due to the crammed arrangement of the hemispheres). As a result, the large-scale eddies (with large values of wavelet coefficients) are concentrated at a pseudo-frequency which is equal to the <span class="hlt">wave</span> oscillating frequency. On the other hand, it is observed that the higher <span class="hlt">wave</span> frequency (2 Hz) is incapable of modulating the eddy structures at that particular region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017RSPSA.47370258M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017RSPSA.47370258M"><span><span class="hlt">Modelling</span> <span class="hlt">wave</span>-induced sea ice break-up in the marginal ice zone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Montiel, F.; Squire, V. A.</p> <p>2017-10-01</p> <p>A <span class="hlt">model</span> of ice floe break-up under ocean <span class="hlt">wave</span> forcing in the marginal ice zone (MIZ) is proposed to investigate how floe size distribution (FSD) evolves under repeated <span class="hlt">wave</span> break-up events. A three-dimensional linear <span class="hlt">model</span> of ocean <span class="hlt">wave</span> scattering by a finite array of compliant circular ice floes is <span class="hlt">coupled</span> to a flexural failure <span class="hlt">model</span>, which breaks a floe into two floes provided the two-dimensional stress field satisfies a break-up criterion. A closed-feedback loop algorithm is devised, which (i) solves the <span class="hlt">wave</span>-scattering problem for a given FSD under time-harmonic plane <span class="hlt">wave</span> forcing, (ii) computes the stress field in all the floes, (iii) fractures the floes satisfying the break-up criterion, and (iv) generates an updated FSD, initializing the geometry for the next iteration of the loop. The FSD after 50 break-up events is unimodal and near normal, or bimodal, suggesting <span class="hlt">waves</span> alone do not govern the power law observed in some field studies. Multiple scattering is found to enhance break-up for long <span class="hlt">waves</span> and thin ice, but to reduce break-up for short <span class="hlt">waves</span> and thick ice. A break-up front marches forward in the latter regime, as <span class="hlt">wave</span>-induced fracture weakens the ice cover, allowing <span class="hlt">waves</span> to travel deeper into the MIZ.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMOS43A1395M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMOS43A1395M"><span>Simulating Freak <span class="hlt">Waves</span> in the Ocean with CFD <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>Manolidis, M.; Orzech, M.; Simeonov, J.</p> <p>2017-12-01</p> <p>Rogue, or freak, <span class="hlt">waves</span> constitute an active topic of research within the world scientific community, as various maritime authorities around the globe seek to better understand and more accurately assess the risks that the occurrence of such phenomena entail. Several experimental studies have shed some light on the mechanics of rogue <span class="hlt">wave</span> formation. In our work we numerically simulate the formation of such <span class="hlt">waves</span> in oceanic conditions by means of Computational Fluid Dynamics (CFD) software. For this purpose we implement the NHWAVE and OpenFOAM software packages. Both are non-hydrostatic, turbulent flow solvers, but NHWAVE implements a shock-capturing scheme at the free surface-interface, while OpenFOAM utilizes the Volume Of Fluid (VOF) method. NHWAVE has been shown to accurately reproduce highly nonlinear surface <span class="hlt">wave</span> phenomena, such as soliton propagation and <span class="hlt">wave</span> shoaling. We conducted a range of tests simulating rogue <span class="hlt">wave</span> formation and horizontally varying <span class="hlt">currents</span> to evaluate and compare the capabilities of the two software packages. Then we used each <span class="hlt">model</span> to investigate the effect of ocean <span class="hlt">currents</span> and <span class="hlt">current</span> gradients on the formation of rogue <span class="hlt">waves</span>. We present preliminary results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850044800&hterms=Plasma+Ring&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DPlasma%2BRing','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850044800&hterms=Plasma+Ring&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DPlasma%2BRing"><span><span class="hlt">Coupled</span> low-energy - ring <span class="hlt">current</span> plasma diffusion in the Jovian magnetosphere</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Summers, D.; Siscoe, G. L.</p> <p>1985-01-01</p> <p>The outwardly diffusing Iogenic plasma and the simultaneously inwardly diffusing ring <span class="hlt">current</span> plasma in the Jovian magnetosphere are described using a <span class="hlt">coupled</span> diffusion <span class="hlt">model</span> which incorporates the effects of the pressure gradient of the ring <span class="hlt">current</span> into the cross-L diffusion coefficient. The <span class="hlt">coupled</span> diffusion coefficient is derived by calculating the total energy available to drive the diffusion process. The condition is imposed that the diffusion coefficient takes on a local minimum value at some point in the region L = 7-8, at which point the gradient of the Io plasma density is specified as ramp value given by Siscoe et al. (1981). The hypothesis that the pressure gradient of the ring <span class="hlt">current</span> causes the diminution of radial plasma transport is tested, and solution profiles for the Iogenic and ring <span class="hlt">current</span> plasma densities are obtained which imply that the Io plasma ramp is caused by a high-density, low-energy component of the ring <span class="hlt">current</span> hitherto unobserved directly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23736481','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23736481"><span>Polarization characteristics of Whispering-Gallery-Mode fiber lasers based on evanescent-<span class="hlt">wave-coupled</span> gain.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Zhang, Yuan-Xian; Pu, Xiao-Yun; Feng, Li; Han, De-Yu; Ren, Yi-Tao</p> <p>2013-05-20</p> <p>The polarization characteristics of Whispering-Gallery-Mode (WGM) fiber lasers based on evanescent-<span class="hlt">wave-coupled</span> gain are investigated. For the laser gain is excited by side-pumping scheme, it is found that the polarization property of lasing emission is simply dependent on the polarized states of the pump beams. The polarization property of lasing emission depends on the propagating situation of the pump beams in an optical fiber if the laser gain is excited by evanescent-<span class="hlt">wave</span> pumping scheme, that is, if the pump beams within the fiber are meridional beams, the lasing emission is a transverse electric (TE) <span class="hlt">wave</span> that forms a special radial polarization emission. However, if the pump beams within the fiber are skew beams, both transverse magnetic (TM) and TE <span class="hlt">waves</span> exist simultaneously in lasing emission that forms a special axially and radially mixed polarization emission. Pumped by skew beams, the <span class="hlt">wave</span>-number differences between TE and TM <span class="hlt">waves</span> are also investigated quantitatively, the results demonstrate that the <span class="hlt">wave</span>-number difference decreases with the increase of the fiber diameter and the refractive index (RI) of the cladding solution. The observed polarization characteristics have been well explained based on lasing radiation mechanism of WGM fiber laser of gain <span class="hlt">coupled</span> by evanescent <span class="hlt">wave</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24023798','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24023798"><span>Spiral-<span class="hlt">wave</span> dynamics in a mathematical <span class="hlt">model</span> of human ventricular tissue with myocytes and fibroblasts.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Nayak, Alok Ranjan; Shajahan, T K; Panfilov, A V; Pandit, Rahul</p> <p>2013-01-01</p> <p>Cardiac fibroblasts, when <span class="hlt">coupled</span> functionally with myocytes, can modulate the electrophysiological properties of cardiac tissue. We present systematic numerical studies of such modulation of electrophysiological properties in mathematical <span class="hlt">models</span> for (a) single myocyte-fibroblast (MF) units and (b) two-dimensional (2D) arrays of such units; our <span class="hlt">models</span> build on earlier ones and allow for zero-, one-, and two-sided MF <span class="hlt">couplings</span>. Our studies of MF units elucidate the dependence of the action-potential (AP) morphology on parameters such as [Formula: see text], the fibroblast resting-membrane potential, the fibroblast conductance [Formula: see text], and the MF gap-junctional <span class="hlt">coupling</span> [Formula: see text]. Furthermore, we find that our MF composite can show autorhythmic and oscillatory behaviors in addition to an excitable response. Our 2D studies use (a) both homogeneous and inhomogeneous distributions of fibroblasts, (b) various ranges for parameters such as [Formula: see text], and [Formula: see text], and (c) intercellular <span class="hlt">couplings</span> that can be zero-sided, one-sided, and two-sided connections of fibroblasts with myocytes. We show, in particular, that the plane-<span class="hlt">wave</span> conduction velocity [Formula: see text] decreases as a function of [Formula: see text], for zero-sided and one-sided <span class="hlt">couplings</span>; however, for two-sided <span class="hlt">coupling</span>, [Formula: see text] decreases initially and then increases as a function of [Formula: see text], and, eventually, we observe that conduction failure occurs for low values of [Formula: see text]. In our homogeneous studies, we find that the rotation speed and stability of a spiral <span class="hlt">wave</span> can be controlled either by controlling [Formula: see text] or [Formula: see text]. Our studies with fibroblast inhomogeneities show that a spiral <span class="hlt">wave</span> can get anchored to a local fibroblast inhomogeneity. We also study the efficacy of a low-amplitude control scheme, which has been suggested for the control of spiral-<span class="hlt">wave</span> turbulence in mathematical <span class="hlt">models</span> for cardiac</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1710218B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1710218B"><span>Phase locking of convectively <span class="hlt">coupled</span> equatorial atmospheric Kelvin <span class="hlt">waves</span> over Indian Ocean basin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Baranowski, Dariusz; Flatau, Maria; Flatau, Piotr; Matthews, Adrian</p> <p>2015-04-01</p> <p>The properties of convectively <span class="hlt">coupled</span> Kelvin <span class="hlt">waves</span> in the Indian Ocean and their propagation over the Maritime Continent are studied. It is shown that Kelvin <span class="hlt">waves</span> are longitude - diurnal cycle phase locked over the Maritime Continent, Africa and the Indian Ocean. Thus, it is shown that they tend to propagate over definite areas during specific times of the day. Over the Maritime Continent, longitude-diurnal cycle phase locking is such that it agrees with mean, local diurnal cycle of convection. The strength of the longitude-diurnal cycle phase locking differs between 'non-blocked' Kelvin <span class="hlt">waves</span>, which make successful transition over the Maritime Continent, and 'blocked' <span class="hlt">waves</span> that terminated within it. It is shown that a specific combination of Kelvin <span class="hlt">wave</span> phase speed and time of the day at which a <span class="hlt">wave</span> approaches the Maritime Continent influence the chance of successful transition into the Western Pacific. Kelvin <span class="hlt">waves</span> that maintain phase speed of 10 to 11 degrees per day over the central-eastern Indian Ocean and arrive at 90E between 9UTC and 18UTC have the highest chance of being 'non-blocked' by the Maritime Continent. The distance between the islands of Sumatra and Borneo agrees with the distance travelled by an average convectively <span class="hlt">coupled</span> Kelvin <span class="hlt">wave</span> in one day. This suggests that the Maritime Continent may act as a 'filter' for Kelvin <span class="hlt">waves</span> favoring successful propagation of those <span class="hlt">waves</span> for which propagation is in phase with the local diurnal cycle of precipitation. The AmPm index, a simple measure of local diurnal cycle for propagating disturbances, is introduced and shown to be useful metric depicting key characteristics of the convection associated with propagating Kelvin <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA495774','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA495774"><span>A <span class="hlt">Model-Coupling</span> Framework for Nearshore <span class="hlt">Waves</span>, <span class="hlt">Currents</span>, Sediment Transport, and Seabed Morphology</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2009-01-01</p> <p>1008.3 ADOR/Director NCST E. R. Franchi , 7000 1. Paper or abstract was released 2. A copy is filed in this office. WfcfeF Public Affairs...have been developed to simulate and predict their behaviors in the past few decades. For example, <span class="hlt">models</span> have been designed to forecast global ...Smedstad LF. Rhodes RC Validation of interannual simulations from the 1/8° global Navy Coastal Ocean <span class="hlt">Model</span> (NCOM). Ocean <span class="hlt">Model</span> 2006;11:376-98. |5| Van</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017NatCo...814896M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017NatCo...814896M"><span>Human seizures <span class="hlt">couple</span> across spatial scales through travelling <span class="hlt">wave</span> dynamics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Martinet, L.-E.; Fiddyment, G.; Madsen, J. R.; Eskandar, E. N.; Truccolo, W.; Eden, U. T.; Cash, S. S.; Kramer, M. A.</p> <p>2017-04-01</p> <p>Epilepsy--the propensity toward recurrent, unprovoked seizures--is a devastating disease affecting 65 million people worldwide. Understanding and treating this disease remains a challenge, as seizures manifest through mechanisms and features that span spatial and temporal scales. Here we address this challenge through the analysis and <span class="hlt">modelling</span> of human brain voltage activity recorded simultaneously across microscopic and macroscopic spatial scales. We show that during seizure large-scale neural populations spanning centimetres of cortex coordinate with small neural groups spanning cortical columns, and provide evidence that rapidly propagating <span class="hlt">waves</span> of activity underlie this increased inter-scale <span class="hlt">coupling</span>. We develop a corresponding computational <span class="hlt">model</span> to propose specific mechanisms--namely, the effects of an increased extracellular potassium concentration diffusing in space--that support the observed spatiotemporal dynamics. Understanding the multi-scale, spatiotemporal dynamics of human seizures--and connecting these dynamics to specific biological mechanisms--promises new insights to treat this devastating disease.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010PhPro...3..185K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010PhPro...3..185K"><span>Air- <span class="hlt">coupled</span> ultrasonic testing of CFRP rods by means of guided <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kažys, Rymantas; Raišutis, Renaldas; Žukauskas, Egidijus; Mažeika, Liudas; Vladišauskas, Alfonsas</p> <p>2010-01-01</p> <p>One of the most important parts of the gliders is a lightweight longeron reinforcement made of carbon fibre reinforced plastics (CFRP) rods. These small diameter (a few millimetres) rods during manufacturing are glued together in epoxy filled matrix in order to build the arbitrary spar profile. However, the defects presenting in the rods such as brake of fibres, lack of bonding, reduction of density affect essentially the strength of the construction and are very complicated in repairing. Therefore, appropriate non-destructive testing techniques of carbon fibber rods should be applied before gluing them together. The objective of the presented work was development of NDT technique of CFRP rods used for aerospace applications, which is based on air- <span class="hlt">coupled</span> excitation/reception of guided <span class="hlt">waves</span>. The regularities of ultrasonic guided <span class="hlt">waves</span> propagating in both circular and rectangular cross-section CFRP rods immersed into water were investigated and it was shown that the guided <span class="hlt">waves</span> propagating along sample of the rod create leaky <span class="hlt">waves</span> which are radiated into a surrounding medium. The ultrasonic receiver scanned over the rod enables to pick-up the leaky <span class="hlt">waves</span> and to determine the non-uniformities of propagation caused by the defects. Theoretical investigations were carried out by means of numerical simulations based on a 2D and 3D finite differences method. By <span class="hlt">modelling</span> and experimental investigations it was demonstrated that presence of any type of the defect disturbs the leaky <span class="hlt">wave</span> and enables to detect them. So, the spatial position of defects can be determined also. It was shown that such important defects as a disbond of the plies essentially reduce or even completely suppress the leaky <span class="hlt">wave</span>, so they can be detected quit easily.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAG...150..126X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAG...150..126X"><span>Effective <span class="hlt">modeling</span> and reverse-time migration for novel pure acoustic <span class="hlt">wave</span> in arbitrary orthorhombic anisotropic media</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xu, Shigang; Liu, Yang</p> <p>2018-03-01</p> <p>The conventional pseudo-acoustic <span class="hlt">wave</span> equations (PWEs) in arbitrary orthorhombic anisotropic (OA) media usually have <span class="hlt">coupled</span> P- and SV-<span class="hlt">wave</span> modes. These <span class="hlt">coupled</span> equations may introduce strong SV-<span class="hlt">wave</span> artifacts and numerical instabilities in P-<span class="hlt">wave</span> simulation results and reverse-time migration (RTM) profiles. However, pure acoustic <span class="hlt">wave</span> equations (PAWEs) completely decouple the P-<span class="hlt">wave</span> component from the full elastic wavefield and naturally solve all the aforementioned problems. In this article, we present a novel PAWE in arbitrary OA media and compare it with the conventional <span class="hlt">coupled</span> PWEs. Through decomposing the solution of the corresponding eigenvalue equation for the original PWE into an ellipsoidal differential operator (EDO) and an ellipsoidal scalar operator (ESO), the new PAWE in time-space domain is constructed by applying the combination of these two solvable operators and can effectively describe P-<span class="hlt">wave</span> features in arbitrary OA media. Furthermore, we adopt the optimal finite-difference method (FDM) to solve the newly derived PAWE. In addition, the three-dimensional (3D) hybrid absorbing boundary condition (HABC) with some reasonable modifications is developed for reducing artificial edge reflections in anisotropic media. To improve computational efficiency in 3D case, we adopt graphic processing unit (GPU) with Compute Unified Device Architecture (CUDA) instead of traditional central processing unit (CPU) architecture. Several numerical experiments for arbitrary OA <span class="hlt">models</span> confirm that the proposed schemes can produce pure, stable and accurate P-<span class="hlt">wave</span> <span class="hlt">modeling</span> results and RTM images with higher computational efficiency. Moreover, the 3D numerical simulations can provide us with a comprehensive and real description of <span class="hlt">wave</span> propagation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1013731','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1013731"><span>An Arctic Ice/Ocean <span class="hlt">Coupled</span> <span class="hlt">Model</span> with <span class="hlt">Wave</span> Interactions</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-09-30</p> <p>seas within and in the waters adjoining MIZs, using a conservative, multiple <span class="hlt">wave</span> scattering approach in a medium with random geometrical properties...relating to <span class="hlt">wave</span>-ice interactions have been collected since the MIZEX campaign of the 1980s, aside from a small number of ad hoc field experiments. This...from the better technology and analysis tools now available, including those related to the field experiments supported by an intensive remote sensing</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.usgs.gov/of/2014/1130/pdf/ofr2014-1130.pdf','USGSPUBS'); return false;" href="https://pubs.usgs.gov/of/2014/1130/pdf/ofr2014-1130.pdf"><span>Coastal circulation and water-column properties in the War in the Pacific National Historical Park, Guam: measurements and <span class="hlt">modeling</span> of <span class="hlt">waves</span>, <span class="hlt">currents</span>, temperature, salinity, and turbidity, April-August 2012</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Storlazzi, Curt D.; Cheriton, Olivia M.; Lescinski, Jamie M.R.; Logan, Joshua B.</p> <p>2014-01-01</p> <p>The U.S. Geological Survey (USGS) Pacific Coastal and Marine Science Center (PCMSC) initiated an investigation in the National Park Service’s (NPS) War in the Pacific National Historical Park (WAPA) to provide baseline scientific information on coastal circulation and water-column properties along west-central Guam, focusing on WAPA’s Agat Unit, as it relates to the transport and settlement of coral larvae, fish, and other marine organisms. The oceanographic data and numerical circulation <span class="hlt">modeling</span> results from this study demonstrate that circulation in Agat Bay was strongly driven by winds and <span class="hlt">waves</span> at longer (>1 day) timescales and by the tides at shorter (<1 day) timescales; near-surface <span class="hlt">currents</span> in deep water were primarily controlled by the winds, whereas <span class="hlt">currents</span> on the shallow reef flats were dominated by <span class="hlt">wave</span>-driven motions. Water-column properties exhibited strong seasonality <span class="hlt">coupled</span> to the shift from the trade wind to the non-trade wind season. During the dry trade-wind season, waters were cooler and more saline. When the winds shifted to a more variable pattern, waters warmed and became less saline because of a combination of increased thermal insolation from lack of wind forcing and higher rainfall. Turbidity was relatively low in Agat Bay and was similar to levels measured elsewhere along west-central Guam. The numerical circulation <span class="hlt">modeling</span> results provide insight into the potential paths of buoyant material released from a series of locations along west-central Guam under summer non-trade wind forcing conditions that characterize coral spawning events. This information may be useful in evaluating the potential zones of influence/impact resulting from transport by surface <span class="hlt">currents</span> of material released from these select locations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1814548G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1814548G"><span>Rogue <span class="hlt">wave</span> variational <span class="hlt">modelling</span> through the interaction of two solitary <span class="hlt">waves</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gidel, Floriane; Bokhove, Onno</p> <p>2016-04-01</p> <p>The extreme and unexpected characteristics of Rogue <span class="hlt">waves</span> have made them legendary for centuries. It is only on the 1st of January 1995 that these mariners' tales started to raise scientist's curiosity, when such a <span class="hlt">wave</span> was recorded in the North Sea; a sudden wall of water hit the Draupner offshore platform, more than twice higher than the other <span class="hlt">waves</span>, providing evidence of the existence of rogue or freak <span class="hlt">waves</span>. Since then, studies have shown that these surface gravity <span class="hlt">waves</span> of high amplitude (at least twice the height of the other sea <span class="hlt">waves</span> [Dyste et al., 2008]) appear in non-linear dispersive water motion [Drazin and Johnson, 1989], at any depth, and have caused a lot of damage in recent years [Nikolkina and Didenkulova, 2011 ]. So far, most of the studies have tried to determine their probability of occurrence, but no conclusion has been achieved yet, which means that we are <span class="hlt">currently</span> unenable to predict or avoid these monster <span class="hlt">waves</span>. An accurate mathematical and numerical water-<span class="hlt">wave</span> <span class="hlt">model</span> would enable simulation and observation of this external forcing on boats and offshore structures and hence reduce their threat. In this work, we aim to <span class="hlt">model</span> rogue <span class="hlt">waves</span> through a soliton splash generated by the interaction of two solitons coming from different channels at a specific angle. Kodama indeed showed that one way to produce extreme <span class="hlt">waves</span> is through the intersection of two solitary <span class="hlt">waves</span>, or one solitary <span class="hlt">wave</span> and its oblique reflection on a vertical wall [Yeh, Li and Kodama, 2010 ]. While he <span class="hlt">modelled</span> Mach reflection from Kadomtsev-Petviashvili (KP) theory, we aim to <span class="hlt">model</span> rogue <span class="hlt">waves</span> from the three-dimensional potential flow equations and/or their asymptotic equivalent described by Benney and Luke [Benney and Luke, 1964]. These theories have the advantage to allow <span class="hlt">wave</span> propagation in several directions, which is not the case with KP equations. The initial solitary <span class="hlt">waves</span> are generated by removing a sluice gate in each channel. The equations are derived through a</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li class="active"><span>24</span></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_24 --> <div id="page_25" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="481"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvC..95f4306H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvC..95f4306H"><span>Combining symmetry collective states with <span class="hlt">coupled</span>-cluster theory: Lessons from the Agassi <span class="hlt">model</span> Hamiltonian</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hermes, Matthew R.; Dukelsky, Jorge; Scuseria, Gustavo E.</p> <p>2017-06-01</p> <p>The failures of single-reference <span class="hlt">coupled</span>-cluster theory for strongly correlated many-body systems is flagged at the mean-field level by the spontaneous breaking of one or more physical symmetries of the Hamiltonian. Restoring the symmetry of the mean-field determinant by projection reveals that <span class="hlt">coupled</span>-cluster theory fails because it factorizes high-order excitation amplitudes incorrectly. However, symmetry-projected mean-field <span class="hlt">wave</span> functions do not account sufficiently for dynamic (or weak) correlation. Here we pursue a merger of symmetry projection and <span class="hlt">coupled</span>-cluster theory, following previous work along these lines that utilized the simple Lipkin <span class="hlt">model</span> system as a test bed [J. Chem. Phys. 146, 054110 (2017), 10.1063/1.4974989]. We generalize the concept of a symmetry-projected mean-field <span class="hlt">wave</span> function to the concept of a symmetry projected state, in which the factorization of high-order excitation amplitudes in terms of low-order ones is guided by symmetry projection and is not exponential, and combine them with <span class="hlt">coupled</span>-cluster theory in order to <span class="hlt">model</span> the ground state of the Agassi Hamiltonian. This <span class="hlt">model</span> has two separate channels of correlation and two separate physical symmetries which are broken under strong correlation. We show how the combination of symmetry collective states and <span class="hlt">coupled</span>-cluster theory is effective in obtaining correlation energies and order parameters of the Agassi <span class="hlt">model</span> throughout its phase diagram.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19045637','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19045637"><span>Acoustic mode <span class="hlt">coupling</span> induced by shallow water nonlinear internal <span class="hlt">waves</span>: sensitivity to environmental conditions and space-time scales of internal <span class="hlt">waves</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Colosi, John A</p> <p>2008-09-01</p> <p>While many results have been intuited from numerical simulation studies, the precise connections between shallow-water acoustic variability and the space-time scales of nonlinear internal <span class="hlt">waves</span> (NLIWs) as well as the background environmental conditions have not been clearly established analytically. Two-dimensional <span class="hlt">coupled</span> mode propagation through NLIWs is examined using a perturbation series solution in which each order n is associated with nth-order multiple scattering. Importantly, the perturbation solution gives resonance conditions that pick out specific NLIW scales that cause <span class="hlt">coupling</span>, and seabed attenuation is demonstrated to broaden these resonances, fundamentally changing the <span class="hlt">coupling</span> behavior at low frequency. Sound-speed inhomogeneities caused by internal solitary <span class="hlt">waves</span> (ISWs) are primarily considered and the dependence of mode <span class="hlt">coupling</span> on ISW amplitude, range width, depth structure, location relative to the source, and packet characteristics are delineated as a function of acoustic frequency. In addition, it is seen that significant energy transfer to modes with initially low or zero energy involves at least a second order scattering process. Under moderate scattering conditions, comparisons of first order, single scattering theoretical predictions to direct numerical simulation demonstrate the accuracy of the approach for acoustic frequencies upto 400 Hz and for single as well as multiple ISW <span class="hlt">wave</span> packets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22600224-observation-dust-acoustic-shock-wave-strongly-coupled-dusty-plasma','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22600224-observation-dust-acoustic-shock-wave-strongly-coupled-dusty-plasma"><span>Observation of dust acoustic shock <span class="hlt">wave</span> in a strongly <span class="hlt">coupled</span> dusty plasma</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>Sharma, Sumita K., E-mail: sumita-sharma82@yahoo.com; Boruah, A.; Nakamura, Y.</p> <p>2016-05-15</p> <p>Dust acoustic shock <span class="hlt">wave</span> is observed in a strongly <span class="hlt">coupled</span> laboratory dusty plasma. A supersonic flow of charged microparticles is allowed to perturb a stationary dust fluid to excite dust acoustic shock <span class="hlt">wave</span>. The evolution process beginning with steepening of initial <span class="hlt">wave</span> front and then formation of a stable shock structure is similar to the numerical results of the Korteweg-de Vries-Burgers equation. The measured Mach number of the observed shock <span class="hlt">wave</span> agrees with the theoretical results. Reduction of shock amplitude at large distances is also observed due to the dust neutral collision and viscosity effects. The dispersion relation and themore » spatial damping of a linear dust acoustic <span class="hlt">wave</span> are also measured and compared with the relevant theory.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22611777-micromagnetic-analysis-current-induced-domain-wall-motion-bilayer-nanowire-synthetic-antiferromagnetic-coupling','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22611777-micromagnetic-analysis-current-induced-domain-wall-motion-bilayer-nanowire-synthetic-antiferromagnetic-coupling"><span>Micromagnetic analysis of <span class="hlt">current</span>-induced domain wall motion in a bilayer nanowire with synthetic antiferromagnetic <span class="hlt">coupling</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>Komine, Takashi, E-mail: komine@mx.ibaraki.ac.jp; Aono, Tomosuke</p> <p></p> <p>We demonstrate <span class="hlt">current</span>-induced domain wall motion in bilayer nanowire with synthetic antiferromagnetic (SAF) <span class="hlt">coupling</span> by <span class="hlt">modeling</span> two body problems for motion equations of domain wall. The influence of interlayer exchange <span class="hlt">coupling</span> and magnetostatic interactions on <span class="hlt">current</span>-induced domain wall motion in SAF nanowires was also investigated. By assuming the rigid wall <span class="hlt">model</span> for translational motion, the interlayer exchange <span class="hlt">coupling</span> and the magnetostatic interaction between walls and domains in SAF nanowires enhances domain wall speed without any spin-orbit-torque. The enhancement of domain wall speed was discussed by energy distribution as a function of wall angle configuration in bilayer nanowires.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhDT........21K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhDT........21K"><span>Computational <span class="hlt">Modeling</span> of Bloch Surface <span class="hlt">Waves</span> in One-Dimensional Periodic and Aperiodic Multilayer Structures</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Koju, Vijay</p> <p></p> <p>Photonic crystals and their use in exciting Bloch surface <span class="hlt">waves</span> have received immense attention over the past few decades. This interest is mainly due to their applications in bio-sensing, <span class="hlt">wave</span>-guiding, and other optical phenomena such as surface field enhanced Raman spectroscopy. Improvement in numerical <span class="hlt">modeling</span> techniques, state of the art computing resources, and advances in fabrication techniques have also assisted in growing interest in this field. The ability to <span class="hlt">model</span> photonic crystals computationally has benefited both the theoretical as well as experimental communities. It helps the theoretical physicists in solving complex problems which cannot be solved analytically and helps to acquire useful insights that cannot be obtained otherwise. Experimentalists, on the other hand, can test different variants of their devices by changing device parameters to optimize performance before fabrication. In this dissertation, we develop two commonly used numerical techniques, namely transfer matrix method, and rigorous <span class="hlt">coupled</span> <span class="hlt">wave</span> analysis, in C++ and MATLAB, and use two additional software packages, one open-source and another commercial, to <span class="hlt">model</span> one-dimensional photonic crystals. Different variants of one-dimensional multilayered structures such as perfectly periodic dielectric multilayers, quasicrystals, aperiodic multilayer are <span class="hlt">modeled</span>, along with one-dimensional photonic crystals with gratings on the top layer. Applications of Bloch surface <span class="hlt">waves</span>, along with new and novel aperiodic dielectric multilayer structures that support Bloch surface <span class="hlt">waves</span> are explored in this dissertation. We demonstrate a slow light configuration that makes use of Bloch Surface <span class="hlt">Waves</span> as an intermediate excitation in a double-prism tunneling configuration. This method is simple compared to the more usual techniques for slowing light using the phenomenon of electromagnetically induced transparency in atomic gases or doped ionic crystals operated at temperatures below 4K. Using a semi</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008NuPhA.810..142B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008NuPhA.810..142B"><span>Asymptotics of QCD traveling <span class="hlt">waves</span> with fluctuations and running <span class="hlt">coupling</span> effects</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Beuf, Guillaume</p> <p>2008-09-01</p> <p>Extending the Balitsky-Kovchegov (BK) equation independently to running <span class="hlt">coupling</span> or to fluctuation effects due to pomeron loops is known to lead in both cases to qualitative changes of the traveling-<span class="hlt">wave</span> asymptotic solutions. In this paper we study the extension of the forward BK equation, including both running <span class="hlt">coupling</span> and fluctuations effects, extending the method developed for the fixed <span class="hlt">coupling</span> case [E. Brunet, B. Derrida, A.H. Mueller, S. Munier, Phys. Rev. E 73 (2006) 056126, cond-mat/0512021]. We derive the exact asymptotic behavior in rapidity of the probabilistic distribution of the saturation scale.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015OcMod..96...36M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015OcMod..96...36M"><span>On tridimensional rip <span class="hlt">current</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>Marchesiello, Patrick; Benshila, Rachid; Almar, Rafael; Uchiyama, Yusuke; McWilliams, James C.; Shchepetkin, Alexander</p> <p>2015-12-01</p> <p>Do lateral shear instabilities of nearshore circulation account for a substantial part of Very Low-Frequency (VLF) variability? If yes, it would promote stirring and mixing of coastal waters and surf-shelf exchanges. Another question is whether tridimensional transient processes are important for instability generation. An innovative <span class="hlt">modeling</span> system with tridimensional <span class="hlt">wave-current</span> interactions was designed to investigate transient nearshore <span class="hlt">currents</span> and interactions between nearshore and innershelf circulations. We present here some validation of rip <span class="hlt">current</span> <span class="hlt">modeling</span> for the Aquitanian coast of France, using in-situ and remote video sensing. We then proceed to show the benefits of 3D versus 2D (depth-mean flow) <span class="hlt">modeling</span> of rip <span class="hlt">currents</span> and their low-frequency variability. It appears that a large part of VLF motions is due to intrinsic variability of the tridimensional flow. 3D <span class="hlt">models</span> may thus provide a valuable, only marginally more expensive alternative to conventional 2D approaches that miss the vertical flow structure and its nonlinear interaction with the depth-averaged flow.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19960021669','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19960021669"><span>Water Surface <span class="hlt">Currents</span>, Short Gravity-Capillary <span class="hlt">Waves</span> and Radar Backscatter</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Atakturk, Serhad S.; Katsaros, Kristina B.</p> <p>1993-01-01</p> <p>Despite their importance for air-sea interaction and microwave remote sensing of the ocean surface, intrinsic properties of short gravity-capillary <span class="hlt">waves</span> are not well established. This is largely due to water surface <span class="hlt">currents</span> and their effects on the direct measurements of <span class="hlt">wave</span> parameters conducted at a fixed point. Frequencies of small scale <span class="hlt">waves</span> propagating on a surface which itself is in motion, are subject to Doppler shifts. Hence, the high frequency tail of the <span class="hlt">wave</span> spectra obtained from such temporal observations is smeared. Conversion of this smeared measured-frequency spectra to intrinsic-frequency (or wavenumber) spectra requires corrections for the Doppler shifts. Such attempts in the past have not been very successful in particular when field data were used. This becomes evident if the amplitude modulation of short <span class="hlt">waves</span> by underlying long <span class="hlt">waves</span> is considered. Microwave radar studies show that the amplitude of a short <span class="hlt">wave</span> component attains its maximum value near the crests and its minimum in the troughs of the long <span class="hlt">waves</span>. Doppler-shifted <span class="hlt">wave</span> data yield similar results but much larger in modulation magnitude, as expected. In general, Doppler shift corrections reduce the modulation magnitude. Overcorrection may result in a negligible modulation or even in a strong modulation with the maximum amplitude in the <span class="hlt">wave</span> troughs. The latter situation is clearly contradictory to our visual observations as well as the radar results and imply that the advection by <span class="hlt">currents</span> is overestimated. In this study, a differential-advection approach is used in which small scale <span class="hlt">waves</span> are advected by the <span class="hlt">currents</span> evaluated not at the free surface, but at a depth proportional to their wavelengths. Applicability of this approach is verified by the excellent agreement in phase and magnitude of short-<span class="hlt">wave</span> modulation between results based on radar and on <span class="hlt">wave</span>-gauge measurements conducted on a lake.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSEC14C1009M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSEC14C1009M"><span><span class="hlt">Wave</span> Dissipation over Nearshore Beach Morphology: Insights from High-Resolution LIDAR Observations and the SWASH <span class="hlt">Wave</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>Mulligan, R. P.; Gomes, E.; McNinch, J.; Brodie, K. L.</p> <p>2016-02-01</p> <p>Numerical <span class="hlt">modelling</span> of the nearshore zone can be computationally intensive due to the complexity of <span class="hlt">wave</span> breaking, and the need for high temporal and spatial resolution. In this study we apply the SWASH non-hydrostatic <span class="hlt">wave</span>-flow <span class="hlt">model</span> that phase-resolves the free surface and fluid motions in the water column at high resolution. The <span class="hlt">model</span> is forced using observed directional energy spectra, and results are compared to <span class="hlt">wave</span> observations during moderate storm events. Observations are collected outside the surf zone using acoustic <span class="hlt">wave</span> and <span class="hlt">currents</span> sensors, and inside the surf zone over a 100 m transect using high-resolution LIDAR measurements of the sea surface from a sensor mounted on a tower on the beach dune at the Field Research Facility in Duck, NC. The <span class="hlt">model</span> is applied to four cases with different <span class="hlt">wave</span> conditions and bathymetry, and used to predict the spatial variability in <span class="hlt">wave</span> breaking, and correlation between energy dissipation and morphologic features. <span class="hlt">Model</span> results compare well with observations of spectral evolution outside the surf zone, and with the remotely sensed observations of <span class="hlt">wave</span> transformation inside the surf zone. The results indicate the importance of nearshore bars, rip-channels, and larger features (major scour depression under the pier following large <span class="hlt">waves</span> from Hurricane Irene) on the location of <span class="hlt">wave</span> breaking and alongshore variability in <span class="hlt">wave</span> energy dissipation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018NJPh...20b3038L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018NJPh...20b3038L"><span>Engineering drag <span class="hlt">currents</span> in Coulomb <span class="hlt">coupled</span> quantum dots</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lim, Jong Soo; Sánchez, David; López, Rosa</p> <p>2018-02-01</p> <p>The Coulomb drag phenomenon in a Coulomb-<span class="hlt">coupled</span> double quantum dot system is revisited with a simple <span class="hlt">model</span> that highlights the importance of simultaneous tunneling of electrons. Previously, cotunneling effects on the drag <span class="hlt">current</span> in mesoscopic setups have been reported both theoretically and experimentally. However, in both cases the sequential tunneling contribution to the drag <span class="hlt">current</span> was always present unless the drag level position were too far away from resonance. Here, we consider the case of very large Coulomb interaction between the dots, whereby the drag <span class="hlt">current</span> needs to be assisted by cotunneling events. As a consequence, a quantum coherent drag effect takes place. Further, we demonstrate that by properly engineering the tunneling probabilities using band tailoring it is possible to control the sign of the drag and drive <span class="hlt">currents</span>, allowing them to flow in parallel or antiparallel directions. We also show that the drag <span class="hlt">current</span> can be manipulated by varying the drag gate potential and is thus governed by electron- or hole-like transport.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015APS..GECKW2005E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015APS..GECKW2005E"><span>Observation of helicon <span class="hlt">wave</span> with m = 0 antenna in a weakly magnetized inductively <span class="hlt">coupled</span> plasma source</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ellingboe, Bert; Sirse, Nishant; Moloney, Rachel; McCarthy, John</p> <p>2015-09-01</p> <p>Bounded whistler <span class="hlt">wave</span>, called ``helicon <span class="hlt">wave</span>,'' is known to produce high-density plasmas and has been exploited as a high density plasma source for many applications, including electric propulsion for spacecraft. In a helicon plasma source, an antenna wrapped around the magnetized plasma column launches a low frequency <span class="hlt">wave</span>, ωce/2 >ωhelicon >ωce/100, in the plasma which is responsible for maintaining high density plasma. Several antenna designs have been proposed in order to match efficiently the <span class="hlt">wave</span> modes. In our experiment, helicon <span class="hlt">wave</span> mode is observed using an m = 0 antenna. A floating B dot probe, compensated to the capacitively <span class="hlt">coupled</span> E field, is employed to measure axial-<span class="hlt">wave</span>-field-profiles (z, r, and θ components) in the plasma at multiple radial positions as a function of rf power and pressure. The Bθ component of the rf-field is observed to be unaffected as the <span class="hlt">wave</span> propagates in the axial direction. Power <span class="hlt">coupling</span> between the antenna and the plasma column is identified and agrees with the E, H, and <span class="hlt">wave</span> <span class="hlt">coupling</span> regimes previously seen in M =1 antenna systems. That is, the Bz component of the rf-field is observed at low plasma density as the Bz component from the antenna penetrates the plasma. The Bz component becomes very small at medium density due to shielding at the centre of the plasma column; however, with increasing density, a sudden ``jump'' occurs in the Bz component above which a standing <span class="hlt">wave</span> under the antenna with a propagating <span class="hlt">wave</span> away from the antenna are observed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/6739833-current-wave-spectra-coupling-project-volume-iii-cumulative-distribution-forces-structures-subjected-combined-action-currents-random-waves-potential-otec-sites-keahole-point-hawaii-year-hurricane-punta-tuna-puerto-rico-year-hurricane-new-orleans-louisiana-year-hurricane-west-coast-florida-year-hurricane-cufor-code','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/6739833-current-wave-spectra-coupling-project-volume-iii-cumulative-distribution-forces-structures-subjected-combined-action-currents-random-waves-potential-otec-sites-keahole-point-hawaii-year-hurricane-punta-tuna-puerto-rico-year-hurricane-new-orleans-louisiana-year-hurricane-west-coast-florida-year-hurricane-cufor-code"><span><span class="hlt">Current-wave</span> spectra <span class="hlt">coupling</span> project. Volume III. Cumulative distribution of forces on structures subjected to the combined action of <span class="hlt">currents</span> and random <span class="hlt">waves</span> for potential OTEC sites: (A) Keahole Point, Hawaii, 100 year hurricane; (B) Punta Tuna, Puerto Rico, 100 year hurricane; (C) New Orleans, Louisiana, 100 year hurricane; (D) West Coast of Florida, 100 year hurricane. [CUFOR code</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Venezian, G.; Bretschneider, C.L.</p> <p>1980-08-01</p> <p>This volume details a new methodology to analyze statistically the forces experienced by a structure at sea. Conventionally a <span class="hlt">wave</span> climate is defined using a spectral function. The <span class="hlt">wave</span> climate is described using a joint distribution of <span class="hlt">wave</span> heights and periods (<span class="hlt">wave</span> lengths), characterizing actual sea conditions through some measured or estimated parameters like the significant <span class="hlt">wave</span> height, maximum spectral density, etc. Random <span class="hlt">wave</span> heights and periods satisfying the joint distribution are then generated. <span class="hlt">Wave</span> kinetics are obtained using linear or non-linear theory. In the case of <span class="hlt">currents</span> a linear <span class="hlt">wave-current</span> interaction theory of Venezian (1979) is used. The peakmore » force experienced by the structure for each individual <span class="hlt">wave</span> is identified. Finally, the probability of exceedance of any given peak force on the structure may be obtained. A three-parameter Longuet-Higgins type joint distribution of <span class="hlt">wave</span> heights and periods is discussed in detail. This joint distribution was used to <span class="hlt">model</span> sea conditions at four potential OTEC locations. A uniform cylindrical pipe of 3 m diameter, extending to a depth of 550 m was used as a sample structure. <span class="hlt">Wave-current</span> interactions were included and forces computed using Morison's equation. The drag and virtual mass coefficients were interpolated from published data. A Fortran program CUFOR was written to execute the above procedure. Tabulated and graphic results of peak forces experienced by the structure, for each location, are presented. A listing of CUFOR is included. Considerable flexibility of structural definition has been incorporated. The program can easily be modified in the case of an alternative joint distribution or for inclusion of effects like non-linearity of <span class="hlt">waves</span>, transverse forces and diffraction.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA31B..07S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA31B..07S"><span>Vertical <span class="hlt">Coupling</span> and Observable Effects of Evanescent Acoustic-Gravity <span class="hlt">Waves</span> in the Mesosphere and Thermosphere</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Snively, J. B.</p> <p>2017-12-01</p> <p>Our understanding of acoustic-gravity <span class="hlt">wave</span> (AGW) dynamics at short periods ( minutes to hour) and small scales ( 10s to 100s km) in the mesosphere, thermosphere, and ionosphere (MTI) has benefited considerably from horizontally- and vertically-resolved measurements of layered species. These include, for example, imagery of the mesopause ( 80-100 km) airglow layers and vertical profiles of the sodium layer via lidar [e.g., Taylor and Hapgood, PSS, 36(10), 1988; Miller et al., PNAS, 112(49), 2015; Cao et al., JGR, 121, 2016]. In the thermosphere-ionosphere, AGW perturbations are also revealed in electron density profiles [Livneh et al., JGR, 112, 2007] and maps of total electron content (TEC) from global positioning system (GPS) receivers [Nishioka et al., GRL, 40(21), 2013]. To the extent that AGW signatures in layered species can be quantified, and the ambient atmospheric state measured or estimated, numerical <span class="hlt">models</span> enable investigations of dynamics at intermediate altitudes that cannot readily be measured (e.g., above and below the 80-100 km mesopause region). Here, new 2D and 3D versions of the <span class="hlt">Model</span> for Acoustic-Gravity <span class="hlt">Wave</span> Interactions and <span class="hlt">Coupling</span> (MAGIC) [e.g., Snively and Pasko, JGR, 113(A6), 2008, and references therein] are introduced and applied to investigate spectra of short-period AGW that can pass through the mesopause region to reach and impact the thermosphere. Simulation case studies are constructed to investigate both their signatures through the hydroxyl airglow layer [e.g., Snively et al., JGR 115(A11), 2010] and their effects above. These <span class="hlt">waves</span>, with large vertical wavelengths and fast horizontal phase speeds, also include those that may be subject to evanescence at mesopause or in the middle-thermosphere, with potential for ducting or dissipation between where static stability is higher. Despite complicating interpretations of momentum fluxes, evanescence plays an under-appreciated role in vertical <span class="hlt">coupling</span> by AGW [Walterscheid and Hecht</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1987JAP....62.3173B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1987JAP....62.3173B"><span>Study of the dislocation mechanism responsible for the Bordoni relaxation in aluminum by the two-<span class="hlt">wave</span> acoustic <span class="hlt">coupling</span> method</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bujard, M.; Gremaud, G.; Benoit, W.</p> <p>1987-10-01</p> <p>The most realistic <span class="hlt">model</span> for the interpretation of the Bordoni relaxation observed by internal friction experiments is the mechanism of kink pair formation (KPF) on the dislocations. However, according to this <span class="hlt">model</span>, high values of the critical resolved shear stress should also be measured at low temperature in face-centered-cubic (fcc) metals, but this has never been observed. Using the newly developed two-<span class="hlt">wave</span> acoustic <span class="hlt">coupling</span> method, we have studied the reality of the KPF <span class="hlt">model</span> as an explanation for the Bordoni relaxation in aluminum. The results are in very good agreement with the predictions of the KPF <span class="hlt">model</span> and thus confirm this <span class="hlt">model</span>. On the other hand, experimental evidence that the kink mobility is very high in aluminum have been found. Therefore, the diffusion time of the kinks is negligibly small for the KPF process in fcc metals. Values of the internal stress field in cold-worked samples have also been obtained using the two-<span class="hlt">wave</span> acoustic <span class="hlt">coupling</span> approach. A description of the experimental method and the theoretical approach for the interpretation of the results will also be given in this paper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018PhLA..382.1633L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018PhLA..382.1633L"><span>Effect of Floquet engineering on the p-<span class="hlt">wave</span> superconductor with second-neighbor <span class="hlt">couplings</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Li, X. P.; Li, C. F.; Wang, L. C.; Zhou, L.</p> <p>2018-06-01</p> <p>The influence of the Floquet engineering on a particular one-dimensional p-<span class="hlt">wave</span> superconductor, Kitaev <span class="hlt">model</span>, with second-neighbor <span class="hlt">couplings</span> is investigated in this paper. The effective Hamiltonians in the rotated reference frames have been obtained, and the convergent regions of the approximated Hamiltonian as well as the topological phase diagrams have been analyzed and discussed. We show that by modulating the external driving field amplitude, frequency as well as the second-neighbor hopping amplitude, the rich phase diagrams and transitions between different topological phases can be obtained.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27476427','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27476427"><span>Effects of internal loading on phosphorus distribution in the Taihu Lake driven by wind <span class="hlt">waves</span> and lake <span class="hlt">currents</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Huang, Lei; Fang, Hongwei; He, Guojian; Jiang, Helong; Wang, Changhui</p> <p>2016-12-01</p> <p>Wind-driven sediment resuspension exerts significant effects on the P behavior in shallow lake ecosystems. In this study, a comprehensive dynamic phosphorus (P) <span class="hlt">model</span> that integrates hydrodynamic, wind <span class="hlt">wave</span> and sediment transport is proposed to assess the importance of internal P cycling due to sediment resuspension on water column P levels. The primary contribution of the <span class="hlt">model</span> is detailed <span class="hlt">modeling</span> and rigorous <span class="hlt">coupling</span> of sediment and P dynamics. The proposed <span class="hlt">model</span> is applied to predict the P behavior in the shallow Taihu Lake, which is the third largest lake in China, and quantitatively estimate the effects of wind <span class="hlt">waves</span> and lake <span class="hlt">currents</span> on P release and distribution. Both the prevailing southeast winds in summer and northwest winds in winter are applied for the simulation, and different wind speeds of 5 m/s and 10 m/s are also considered. Results show that sediment resuspension and the resulting P release have a dominant effect on P levels in Taihu Lake, and likely similar shallow lakes. Wind-driven <span class="hlt">waves</span> at higher wind speeds significantly enhance sediment resuspension and suspended sediment concentration (SSC). Total P concentration in the water column is also increased but not in proportion to the SSC. The different lake circulations resulting from the different prevailing wind directions also affect the distribution of suspended sediment and P around the lake ultimately influencing where eutrophication is likely to occur. The proposed <span class="hlt">model</span> demonstrates that internal cycling in the lake is a dominant factor in the lake P and must be considered when trying to manage water quality in this and similar lakes. The <span class="hlt">model</span> is used to demonstrate the potential effectiveness of remediation of an area where historical releases have led to P accumulation on overall lake quality. Copyright © 2016 Elsevier Ltd. All rights reserved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22304084-nonlinear-coupling-left-right-handed-circularly-polarized-dispersive-alfven-wave','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22304084-nonlinear-coupling-left-right-handed-circularly-polarized-dispersive-alfven-wave"><span>Nonlinear <span class="hlt">coupling</span> of left and right handed circularly polarized dispersive Alfvén <span class="hlt">wave</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>Sharma, R. P., E-mail: rpsharma@ces.iitd.ac.in; Sharma, Swati, E-mail: swati.sharma704@gmail.com; Gaur, Nidhi, E-mail: nidhiphysics@gmail.com</p> <p>2014-07-15</p> <p>The nonlinear phenomena are of prominent interests in understanding the particle acceleration and transportation in the interplanetary space. The ponderomotive nonlinearity causing the filamentation of the parallel propagating circularly polarized dispersive Alfvén <span class="hlt">wave</span> having a finite frequency may be one of the mechanisms that contribute to the heating of the plasmas. The contribution will be different of the left (L) handed mode, the right (R) handed mode, and the mix mode. The contribution also depends upon the finite frequency of the circularly polarized <span class="hlt">waves</span>. In the present paper, we have investigated the effect of the nonlinear <span class="hlt">coupling</span> of the Lmore » and R circularly polarized dispersive Alfvén <span class="hlt">wave</span> on the localized structures formation and the respective power spectra. The dynamical equations are derived in the presence of the ponderomotive nonlinearity of the L and R pumps and then studied semi-analytically as well as numerically. The ponderomotive nonlinearity accounts for the nonlinear <span class="hlt">coupling</span> between both the modes. In the presence of the adiabatic response of the density fluctuations, the nonlinear dynamical equations satisfy the modified nonlinear Schrödinger equation. The equations thus obtained are solved in solar wind regime to study the <span class="hlt">coupling</span> effect on localization and the power spectra. The effect of <span class="hlt">coupling</span> is also studied on Faraday rotation and ellipticity of the <span class="hlt">wave</span> caused due to the difference in the localization of the left and the right modes with the distance of propagation.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/5003591','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/5003591"><span>Study of ICRF <span class="hlt">wave</span> propagation and plasma <span class="hlt">coupling</span> efficiency in a linear magnetic mirror device</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>Peng, S.Y.</p> <p>1991-07-01</p> <p>Ion Cyclotron Range of Frequency (ICRF) <span class="hlt">wave</span> propagation in an inhomogeneous axial magnetic field in a cylindrical plasma-vacuum system has historically been inadequately <span class="hlt">modelled</span>. Previous works either sacrifice the cylindrical geometry in favor of a simpler slab geometry, concentrate on the resonance region, use a single mode to represent the entire field structure, or examine only radial propagation. This thesis performs both analytical and computational studies to <span class="hlt">model</span> the ICRF <span class="hlt">wave</span>-plasma <span class="hlt">coupling</span> and propagation problem. Experimental analysis is also conducted to compare experimental results with theoretical predictions. Both theoretical as well as experimental analysis are undertaken as part of themore » thesis. The theoretical studies simulate the propagation of ICRF <span class="hlt">waves</span> in an axially inhomogeneous magnetic field and in cylindrical geometry. Two theoretical analysis are undertaken - an analytical study and a computational study. The analytical study treats the inhomogeneous magnetic field by transforming the (r,z) coordinate into another coordinate system ({rho},{xi}) that allows the solution of the fields with much simpler boundaries. The plasma fields are then Fourier transformed into two <span class="hlt">coupled</span> convolution-integral equations which are then differenced and solved for both the perpendicular mode number {alpha} as well as the complete EM fields. The computational study involves a multiple eigenmode computational analysis of the fields that exist within the plasma-vacuum system. The inhomogeneous axial field is treated by dividing the geometry into a series of transverse axial slices and using a constant dielectric tensor in each individual slice. The slices are then connected by longitudinal boundary conditions.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2000APS..DPPMI1002H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2000APS..DPPMI1002H"><span>Neoclassical <span class="hlt">Current</span> Drive by <span class="hlt">Waves</span> with a Symmetric Spectrum</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Helander, Per</p> <p>2000-10-01</p> <p>It is well known that plasma <span class="hlt">waves</span> can produce electric <span class="hlt">currents</span> if the <span class="hlt">waves</span> have an asymmetric spectrum, so that they either interact preferentially with electrons travelling in one direction along the magnetic field or impart net parallel momentum to the electrons [1]. This directionality creates an asymmetry in the electron distribution function and thereby produces a <span class="hlt">current</span> parallel to the field. We demonstrate, somewhat surprisingly, that in a plasma confined by a curved magnetic field no such spectral asymmetry is necessary for <span class="hlt">current</span> drive if the effect of collisions is properly taken into account. For instance, in a toroidal plasma a <span class="hlt">current</span> can be produced by a spectrally symmetric <span class="hlt">wave</span> field if this field is instead up-down asymmetric, which is frequently the case for electron cyclotron <span class="hlt">current</span> drive (ECCD) in tokamaks. We have calculated the resulting <span class="hlt">current</span> drive efficiency and found it to be smaller than that of the conventional <span class="hlt">current</span> drive mechanism in the banana regime, but not insignificant in the plateau regime. The results will be compared with experiments in DIII-D, where the measured efficiency exceeds the classical prediction [2]. Our calculations are focused on this case of ECCD in tokamaks, but the basic physical mechanism is much more general. It is of a universal neoclassical nature and applies to all <span class="hlt">wave</span>-particle interaction in curved magnetic fields. [1] N.J. Fisch, Rev. Mod. Phys. 59, 175 (1987). [2] Y. R. Lin-Liu et al., 26th EPS Conf. on Contr. Fusion and Plasma Phys.(European Phys. Soc. Paris, 1999) Vol. 23J, p 1245.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1013695','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1013695"><span><span class="hlt">Wave</span> Climate and <span class="hlt">Wave</span> Mixing in the Marginal Ice Zones of Arctic Seas, Observations and <span class="hlt">Modelling</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-09-30</p> <p>ababanin.com/ LONG-TERM GOALS The long-term goals of the present project are two: wind/<span class="hlt">wave</span> climatology for the Arctic Seas, and their <span class="hlt">current</span>...OBJECTIVES The wind/<span class="hlt">wave</span> climatology for the Arctic Seas will be developed based on altimeter observations. It will have a major scientific and...applied significance as presently there is no reference climatology for this region of the ocean available. The new versions of <span class="hlt">wave</span> <span class="hlt">models</span> for the</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. 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