Sample records for ocean wave power

  1. Power from Ocean Waves.

    ERIC Educational Resources Information Center

    Newman, J. N.

    1979-01-01

    Discussed is the utilization of surface ocean waves as a potential source of power. Simple and large-scale wave power devices and conversion systems are described. Alternative utilizations, environmental impacts, and future prospects of this alternative energy source are detailed. (BT)

  2. Hydroelectric power from ocean waves

    NASA Astrophysics Data System (ADS)

    Raghavendran, K.

    1981-02-01

    This paper describes a system which converts the variable energy of ocean waves into a steady supply of energy in a conventional form. The system consists of a set of floats and Persian wheels located off-shore and a storage reservoir on the shore. The floats oscillate vertically as the waves pass below them and turn their respective Persian wheels which lift sea water to a height and deliver to the reservoir through an interconnecting pipeline. The head of water in the reservoir operates a hydraulic turbine which in turn works a generator to supply electricity. Due to the recurrent wave action, water is maintained at the optimum level in the reservoir to ensure continuous power supply.

  3. A Wave Power Device with Pendulum Based on Ocean Monitoring Buoy

    NASA Astrophysics Data System (ADS)

    Chai, Hui; Guan, Wanchun; Wan, Xiaozheng; Li, Xuanqun; Zhao, Qiang; Liu, Shixuan

    2018-01-01

    The ocean monitoring buoy usually exploits solar energy for power supply. In order to improve power supply capacity, this paper proposes a wave power device according to the structure and moving character of buoy. The wave power device composes of pendulum mechanism that converts wave energy into mechanical energy and energy storage mechanism where the mechanical energy is transferred quantitatively to generator. The hydrodynamic equation for the motion of buoy system with generator devise is established based on the potential flow theory, and then the characteristics of pendulum motion and energy conversion properties are analysed. The results of this research show that the proposed wave power devise is able to efficiently and periodically convert wave energy into power, and increasing the stiffness of energy storage spring is benefit for enhancing the power supply capacity of the buoy. This study provides a theory reference for the development of technology on wave power generator for ocean monitoring buoy.

  4. Power inversion design for ocean wave energy harvesting

    NASA Astrophysics Data System (ADS)

    Talebani, Anwar N.

    The needs for energy sources are increasing day by day because of several factors, such as oil depletion, and global climate change due to the higher level of CO2, so the exploration of various renewable energy sources is very promising area of study. The available ocean waves can be utilized as free source of energy as the water covers 70% of the earth surface. This thesis presents the ocean wave energy as a source of renewable energy. By addressing the problem of designing efficient power electronics system to deliver 5 KW from the induction generator to the grid with less possible losses and harmonics as possible and to control current fed to the grid to successfully harvest ocean wave energy. We design an AC-DC full bridge rectifier converter, and a DC-DC boost converter to harvest wave energy from AC to regulated DC. In order to increase the design efficiency, we need to increase the power factor from (0.5-0.6) to 1. This is accomplished by designing the boost converter with power factor correction in continues mode with RC circuit as an input to the boost converter power factor correction. This design results in a phase shift between the input current and voltage of the full bridge rectifier to generate a small reactive power. The reactive power is injected to the induction generator to maintain its functionality by generating a magnetic field in its stator. Next, we design a single-phase pulse width modulator full bridge voltage source DC-AC grid-tied mode inverter to harvest regulated DC wave energy to AC. The designed inverter is modulated by inner current loop, to control current injected to the grid with minimal filter component to maintain power quality at the grid. The simulation results show that our design successfully control the current level fed to the grid. It is noteworthy that the simulated efficiency is higher than the calculated one since we used an ideal switch in the simulated circuit.

  5. Wave Power Demonstration Project at Reedsport, Oregon

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

    Mekhiche, Mike; Downie, Bruce

    2013-10-21

    Ocean wave power can be a significant source of large‐scale, renewable energy for the US electrical grid. The Electrical Power Research Institute (EPRI) conservatively estimated that 20% of all US electricity could be generated by wave energy. Ocean Power Technologies, Inc. (OPT), with funding from private sources and the US Navy, developed the PowerBuoy to generate renewable energy from the readily available power in ocean waves. OPT's PowerBuoy converts the energy in ocean waves to electricity using the rise and fall of waves to move the buoy up and down (mechanical stroking) which drives an electric generator. This electricity ismore » then conditioned and transmitted ashore as high‐voltage power via underwater cable. OPT's wave power generation system includes sophisticated techniques to automatically tune the system for efficient conversion of random wave energy into low cost green electricity, for disconnecting the system in large waves for hardware safety and protection, and for automatically restoring operation when wave conditions normalize. As the first utility scale wave power project in the US, the Wave Power Demonstration Project at Reedsport, OR, will consist of 10 PowerBuoys located 2.5 miles off the coast. This U.S. Department of Energy Grant funding along with funding from PNGC Power, an Oregon‐based electric power cooperative, was utilized for the design completion, fabrication, assembly and factory testing of the first PowerBuoy for the Reedsport project. At this time, the design and fabrication of this first PowerBuoy and factory testing of the power take‐off subsystem are complete; additionally the power take‐off subsystem has been successfully integrated into the spar.« less

  6. The influence of spatially and temporally high-resolution wind forcing on the power input to near-inertial waves in the ocean

    NASA Astrophysics Data System (ADS)

    Rimac, Antonija; von Storch, Jin-Song; Eden, Carsten

    2013-04-01

    The estimated power required to sustain global general circulation in the ocean is about 2 TW. This power is supplied with wind stress and tides. Energy spectrum shows pronounced maxima at near-inertial frequency. Near-inertial waves excited by high-frequency winds represent an important source for deep ocean mixing since they can propagate into the deep ocean and dissipate far away from the generation sites. The energy input by winds to near-inertial waves has been studied mostly using slab ocean models and wind stress forcing with coarse temporal resolution (e.g. 6-hourly). Slab ocean models lack the ability to reproduce fundamental aspects of kinetic energy balance and systematically overestimate the wind work. Also, slab ocean models do not account the energy used for the mixed layer deepening or the energy radiating downward into the deep ocean. Coarse temporal resolution of the wind forcing strongly underestimates the near-inertial energy. To overcome this difficulty we use an eddy permitting ocean model with high-frequency wind forcing. We establish the following model setup: We use the Max Planck Institute Ocean Model (MPIOM) on a tripolar grid with 45 km horizontal resolution and 40 vertical levels. We run the model with wind forcings that vary in horizontal and temporal resolution. We use high-resolution (1-hourly with 35 km horizontal resolution) and low-resolution winds (6-hourly with 250 km horizontal resolution). We address the following questions: Is the kinetic energy of near-inertial waves enhanced when high-resolution wind forcings are used? If so, is this due to higher level of overall wind variability or higher spatial or temporal resolution of wind forcing? How large is the power of near-inertial waves generated by winds? Our results show that near-inertial waves are enhanced and the near-inertial kinetic energy is two times higher (in the storm track regions 3.5 times higher) when high-resolution winds are used. Filtering high-resolution winds

  7. Infragravity waves in the ocean as a source of acoustic-gravity waves in the atmosphere

    NASA Astrophysics Data System (ADS)

    Zabotin, Nikolay A.; Godin, Oleg A.

    2013-04-01

    Infragravity waves (IGWs) are surface gravity waves in the ocean with periods longer than the longest periods (~30s) of wind-generated waves. IGWs propagate transoceanic distances with very little attenuation in deep water and, because of their long wavelengths (from ~1 km to hundreds of km), provide a mechanism for coupling wave processes in the ocean, ice shelves, the atmosphere, and the solid Earth. Here, we build on recent advances in understanding spectral and spatial variability of background infragravity waves in deep ocean to evaluate the IGW manifestations in the atmosphere. Water compressibility has a minor effect on IGWs. On the contrary, much larger compressibility and vertical extent of the atmosphere makes it necessary to treat IGW extension into the atmosphere as acoustic-gravity waves. There exist two distinct regimes of IGW penetration into the atmosphere. At higher frequencies, one has surface waves in the atmosphere propagating horizontally along the ocean surface and prominent up to heights of the order of the wavelength. At lower frequencies, IGWs are leaky waves, which continuously radiate their energy into the upper atmosphere. The transition between the two regimes occurs at a frequency of the order of 3 mHz, with the exact value of the transition frequency being a function of the ocean depth, the direction of IGW propagation and the vertical profiles of temperature and wind velocity. The transition frequency decreases with increasing ocean depth. Using recently obtained semi-empirical model of power spectra the IGWs over varying bathymetry [Godin O. A., Zabotin N. A., Sheehan A. F., Yang Z., and Collins J. A. Power spectra of infragravity waves in a deep ocean, Geophys. Res. Lett., under review (2012)], we derive an estimate of the flux of the mechanical energy from the deep ocean into the atmosphere due to IGWs. Significance will be discussed of the IGW contributions into the field of acoustic-gravity waves in the atmosphere.

  8. Ocean wave-radar modulation transfer functions from the West Coast experiment

    NASA Technical Reports Server (NTRS)

    Wright, J. W.; Plant, W. J.; Keller, W. C.; Jones, W. L.

    1980-01-01

    Short gravity-capillary waves, the equilibrium, or the steady state excitations of the ocean surface are modulated by longer ocean waves. These short waves are the predominant microwave scatterers on the ocean surface under many viewing conditions so that the modulation is readily measured with CW Doppler radar used as a two-scale wave probe. Modulation transfer functions (the ratio of the cross spectrum of the line-of-sight orbital speed and backscattered microwave power to the autospectrum of the line-of-sight orbital speed) were measured at 9.375 and 1.5 GHz (Bragg wavelengths of 2.3 and 13 cm) for winds up to 10 m/s and ocean wave periods from 2-18 s. The measurements were compared with the relaxation-time model; the principal result is that a source of modulation other than straining by the horizontal component of orbital speed, possibly the wave-induced airflow, is responsible for most of the modulation by waves of typical ocean wave period (10 s). The modulations are large; for unit coherence, spectra of radar images of deep-water waves should be proportional to the quotient of the slope spectra of the ocean waves by the ocean wave frequency.

  9. Scale-dependent Ocean Wave Turbulence

    NASA Technical Reports Server (NTRS)

    Glazman, R. E.

    1995-01-01

    Wave turbulence is a common feature of nonlinear wave motions observed when external forcing acts during a long period of time, resulting in developed spectral cascades of energy, momentum, and other conserved integrals. In the ocean, wave turbulence occurs on various scales from capillary ripples, and those of baroclinic inertia-gravity, to Rossby waves. Oceanic wave motions are discussed.

  10. Ocean Wave Simulation Based on Wind Field

    PubMed Central

    2016-01-01

    Ocean wave simulation has a wide range of applications in movies, video games and training systems. Wind force is the main energy resource for generating ocean waves, which are the result of the interaction between wind and the ocean surface. While numerous methods to handle simulating oceans and other fluid phenomena have undergone rapid development during the past years in the field of computer graphic, few of them consider to construct ocean surface height field from the perspective of wind force driving ocean waves. We introduce wind force to the construction of the ocean surface height field through applying wind field data and wind-driven wave particles. Continual and realistic ocean waves result from the overlap of wind-driven wave particles, and a strategy was proposed to control these discrete wave particles and simulate an endless ocean surface. The results showed that the new method is capable of obtaining a realistic ocean scene under the influence of wind fields at real time rates. PMID:26808718

  11. Ocean Wave Simulation Based on Wind Field.

    PubMed

    Li, Zhongyi; Wang, Hao

    2016-01-01

    Ocean wave simulation has a wide range of applications in movies, video games and training systems. Wind force is the main energy resource for generating ocean waves, which are the result of the interaction between wind and the ocean surface. While numerous methods to handle simulating oceans and other fluid phenomena have undergone rapid development during the past years in the field of computer graphic, few of them consider to construct ocean surface height field from the perspective of wind force driving ocean waves. We introduce wind force to the construction of the ocean surface height field through applying wind field data and wind-driven wave particles. Continual and realistic ocean waves result from the overlap of wind-driven wave particles, and a strategy was proposed to control these discrete wave particles and simulate an endless ocean surface. The results showed that the new method is capable of obtaining a realistic ocean scene under the influence of wind fields at real time rates.

  12. HARNESSING OCEAN WAVE ENERGY TO GENERATE ELECTRICITY

    EPA Science Inventory

    A technical challenge to sustainability is finding an energy source that is abundant enough to meet global demands without producing greenhouse gases or radioactive waste. Energy from ocean surface waves can provide the people of this planet a clean, endless power source to me...

  13. ONR Ocean Wave Dynamics Workshop

    NASA Astrophysics Data System (ADS)

    In anticipation of the start (in Fiscal Year 1988) of a new Office of Naval Research (ONR) Accelerated Research Initiative (ARI) on Ocean Surface Wave Dynamics, a workshop was held August 5-7, 1986, at Woods Hole, Mass., to discuss new ideas and directions of research. This new ARI on Ocean Surface Wave Dynamics is a 5-year effort that is organized by the ONR Physical Oceanography Program in cooperation with the ONR Fluid Mechanics Program and the Physical Oceanography Branch at the Naval Ocean Research and Development Activity (NORDA). The central theme is improvement of our understanding of the basic physics and dynamics of surface wave phenomena, with emphasis on the following areas: precise air-sea coupling mechanisms,dynamics of nonlinear wave-wave interaction under realistic environmental conditions,wave breaking and dissipation of energy,interaction between surface waves and upper ocean boundary layer dynamics, andsurface statistical and boundary layer coherent structures.

  14. Ocean power technology design optimization

    DOE PAGES

    van Rij, Jennifer; Yu, Yi -Hsiang; Edwards, Kathleen; ...

    2017-07-18

    For this study, the National Renewable Energy Laboratory and Ocean Power Technologies (OPT) conducted a collaborative code validation and design optimization study for OPT's PowerBuoy wave energy converter (WEC). NREL utilized WEC-Sim, an open-source WEC simulator, to compare four design variations of OPT's PowerBuoy. As an input to the WEC-Sim models, viscous drag coefficients for the PowerBuoy floats were first evaluated using computational fluid dynamics. The resulting WEC-Sim PowerBuoy models were then validated with experimental power output and fatigue load data provided by OPT. The validated WEC-Sim models were then used to simulate the power performance and loads for operationalmore » conditions, extreme conditions, and directional waves, for each of the four PowerBuoy design variations, assuming the wave environment of Humboldt Bay, California. And finally, ratios of power-to-weight, power-to-fatigue-load, power-to-maximum-extreme-load, power-to-water-plane-area, and power-to-wetted-surface-area were used to make a final comparison of the potential PowerBuoy WEC designs. Lastly, the design comparison methodologies developed and presented in this study are applicable to other WEC devices and may be useful as a framework for future WEC design development projects.« less

  15. Ocean power technology design optimization

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

    van Rij, Jennifer; Yu, Yi -Hsiang; Edwards, Kathleen

    For this study, the National Renewable Energy Laboratory and Ocean Power Technologies (OPT) conducted a collaborative code validation and design optimization study for OPT's PowerBuoy wave energy converter (WEC). NREL utilized WEC-Sim, an open-source WEC simulator, to compare four design variations of OPT's PowerBuoy. As an input to the WEC-Sim models, viscous drag coefficients for the PowerBuoy floats were first evaluated using computational fluid dynamics. The resulting WEC-Sim PowerBuoy models were then validated with experimental power output and fatigue load data provided by OPT. The validated WEC-Sim models were then used to simulate the power performance and loads for operationalmore » conditions, extreme conditions, and directional waves, for each of the four PowerBuoy design variations, assuming the wave environment of Humboldt Bay, California. And finally, ratios of power-to-weight, power-to-fatigue-load, power-to-maximum-extreme-load, power-to-water-plane-area, and power-to-wetted-surface-area were used to make a final comparison of the potential PowerBuoy WEC designs. Lastly, the design comparison methodologies developed and presented in this study are applicable to other WEC devices and may be useful as a framework for future WEC design development projects.« less

  16. Tracing Acoustic-Gravity Waves from the Ocean into the Ionosphere

    NASA Astrophysics Data System (ADS)

    Zabotin, N. A.; Godin, O. A.; Bullett, T. W.; Negrea, C.

    2013-12-01

    Ionospheric manifestations of tsunamis provide dramatic evidence of a connection between wave processes in the ocean and in the atmosphere. But tsunamis are only a transient feature of a more general phenomenon, infragravity waves (IGWs). IGWs are permanently present surface gravity waves in the ocean with periods longer than the longest periods (~30 s) of wind-generated waves. IGWs propagate transoceanic distances and, because of their long wavelengths (from ~1 km to hundreds of km), provide a mechanism for coupling wave processes in the ocean, atmosphere, and the solid Earth. The notion that tsunamis may generate waves in the upper atmosphere has existed for a long time but no quantitative coupling theory for the background waves has been proposed. We provide a strict physical justification for the influence of the background IGWs on the upper atmosphere. Taking into account both fluid compressibility and the gravity in a coupled atmosphere-ocean system, we show that there exist two distinct regimes of IGW penetration into the atmosphere. At higher frequencies, one has evanescent waves in the atmosphere propagating horizontally along the ocean surface. At lower frequencies, IGWs continuously radiate their energy into the upper atmosphere in the form of acoustic gravity waves (AGWs). The transition frequency depends on the ocean depth; it varies slowly near 3 mHz for typical depth values and drops to zero sharply only for extremely large depths. Using semi-empirical model of the IGW power spectrum, we derive an estimate of the flux of the mechanical energy and mechanical momentum from the deep ocean into the atmosphere due to background IGWs and predict specific forcing on the atmosphere in coastal regions. We compare spectra of wave processes in the ionosphere measured using Dynasonde technique over Wallops Island, VA and San Juan, PR and interpret the differences in terms of the oceanic effects. We conclude that AGWs of oceanic origin may have an observable

  17. The viscous lee wave problem and its implications for ocean modelling

    NASA Astrophysics Data System (ADS)

    Shakespeare, Callum J.; Hogg, Andrew McC.

    2017-05-01

    Ocean circulation models employ 'turbulent' viscosity and diffusivity to represent unresolved sub-gridscale processes such as breaking internal waves. Computational power has now advanced sufficiently to permit regional ocean circulation models to be run at sufficiently high (100 m-1 km) horizontal resolution to resolve a significant part of the internal wave spectrum. Here we develop theory for boundary generated internal waves in such models, and in particular, where the waves dissipate their energy. We focus specifically on the steady lee wave problem where stationary waves are generated by a large-scale flow acting across ocean bottom topography. We generalise the energy flux expressions of [Bell, T., 1975. Topographically generated internal waves in the open ocean. J. Geophys. Res. 80, 320-327] to include the effect of arbitrary viscosity and diffusivity. Applying these results for realistic parameter choices we show that in the present generation of models with O(1) m2s-1 horizontal viscosity/diffusivity boundary-generated waves will inevitably dissipate the majority of their energy within a few hundred metres of the boundary. This dissipation is a direct consequence of the artificially high viscosity/diffusivity, which is not always physically justified in numerical models. Hence, caution is necessary in comparing model results to ocean observations. Our theory further predicts that O(10-2) m2s-1 horizontal and O(10-4) m2s-1 vertical viscosity/diffusivity is required to achieve a qualitatively inviscid representation of internal wave dynamics in ocean models.

  18. SAR imaging of ocean waves - Theory

    NASA Technical Reports Server (NTRS)

    Jain, A.

    1981-01-01

    A SAR imaging integral for a rough surface is derived. Aspects of distributed target imaging and questions of ocean-wave imaging are considered. A description is presented of the results of analyses which are performed on aircraft and a spacecraft data in order to gain an understanding of the SAR imaging of ocean waves. The analyzed data illustrate the effect of radar resolution on the images of azimuthally traveling waves, the dependence of image distortion on the angle which the waves make with the radar flight path, and the dependence of the focusing parameter of the radar matched filter on the ocean wave period for azimuthally traveling waves. A dependence of ocean-wave modulation on significant wave height is also observed. The observed dependence of the modulations of azimuth waves on radar resolution is in contradiction to the hypothesis that these modulations are caused mainly by velocity bunching.

  19. Remote sensing of ocean wave spectra by interferometric synthetic aperture radar

    NASA Technical Reports Server (NTRS)

    Marom, M.; Thornton, E. B.; Goldstein, R. M.; Shemer, L.

    1990-01-01

    Ocean surface waves can be clearly observed by SAR in the interferometric configuration (INSAR) due to the ability of INSAR to provide images of the local surface velocity field. It is shown here that INSAR can be used to obtain wavenumber spectra that are in agreement with power spectra measured in situ. This new method has considerable potential to provide instantaneous spatial information about the structure of ocean wave fields.

  20. The influence of spatially and temporally high-resolution wind forcing on the power input to near-inertial waves in the ocean

    NASA Astrophysics Data System (ADS)

    Rimac, A.; Eden, C.; von Storch, J.

    2012-12-01

    Coexistence of stable stratification, the meridional overturning circulation and meso-scale eddies and their influence on the ocean's circulation still raise complex questions concerning the ocean energetics. Oceanic general circulation is mainly forced by the wind field and deep water tides. Its essential energetics are the conversion of kinetic energy of the winds and tides into oceanic potential and kinetic energy. Energy needed for the circulation is bound to internal wave fields. Direct internal wave generation by the wind at the sea surface is one of the sources of this energy. Previous studies using mixed-layer type of models and low frequency wind forcings (six-hourly and daily) left room for improvement. Using mixed-layer models it is not possible to assess the distribution of near-inertial energy into the deep ocean. Also, coarse temporal resolution of wind forcing strongly underestimates the near-inertial wave energy. To overcome this difficulty we use a high resolution ocean model with high frequency wind forcings. We establish the following model setup: We use the Max Planck Institute Ocean Model (MPIOM) on a tripolar grid with 45km horizontal resolution and 40 vertical levels. We run the model with wind forcings that vary in horizontal (250km versus 40km) and temporal resolution (six versus one-hourly). In our study we answer the following questions: How big is the wind kinetic energy input to the near-inertial waves? Is the kinetic energy of the near-inertial waves enhanced when high-frequency wind forcings are used? If so, by how much and why, due to higher level of temporal wind variability or due to better spatial representation of the near-inertial waves? How big is the total power of near-inertial waves generated by the wind at the surface of the ocean? We run the model for one year. Our model results show that the near-inertial waves are excited both using wind forcings of high and low horizontal and temporal resolution. Near-inertial energy is

  1. The Spectral Ocean Wave Model (SOWM), a Northern Hemisphere Computer Model for Specifying and Forecasting Ocean Wave Spectra

    DTIC Science & Technology

    1982-07-01

    directions. SIGNIFICANT WAVE HEIGHT A further sua-tion of (3) over the 15 frequency bands yields, within a linear model , the variance of a time history of...SPECTRAL Of.EAN WAVE MODEL (SOWM), A NORTHERN Final Report HEMtISPHEE COMPUTER MODELL Foyt SPECIFYING AND FORECASTING OCEAN WAVE .SftfTRA S EFRIGOG...Ocean Wave Model (SWM() In use at the Fleet Numerical Oceanography Center si.nce 1974 has been used to produce spectra for a 20- year ocean wave

  2. Design and characterization of an ocean wave powered lifejacket using 2DOF floating boards

    NASA Astrophysics Data System (ADS)

    Mi, Jia; Xu, Lin; Yang, Yaling; Zuo, Lei

    2018-04-01

    Lifejacket is an indispensable life-saving equipment for ships and airplanes. Traditional lifejacket is designed to prevent human from drowning. However, the water temperature is usually low, especially in winter, which significantly reduces the human body temperature and leads to death. Meanwhile, power is critical for drowning people to use emergency communication equipment. This paper proposed an ocean wave powered lifejacket using 2DOF floating boards to provide both buoyance and electricity for drowning people. Hence, they can use this continuous electric power to keep key body warm and send distress signal. This lifejacket is featured with two 2DOF floating boards and the mechanical motion rectifier (MMR) can convert the 2-DOF motions to the unidirectional rotation of generator. The design principle is illustrated and the dynamic modelling for the 2-DOF motions has been analyzed. Bench test and lake test have been conducted to validate the design concept.

  3. Near-inertial waves and deep ocean mixing

    NASA Astrophysics Data System (ADS)

    Shrira, V. I.; Townsend, W. A.

    2013-07-01

    For the existing pattern of global oceanic circulation to exist, there should be sufficiently strong turbulent mixing in the abyssal ocean, the mechanisms of which are not well understood as yet. The review discusses a plausible mechanism of deep ocean mixing caused by near-inertial waves in the abyssal ocean. It is well known how winds in the atmosphere generate near-inertial waves in the upper ocean, which then propagate downwards losing their energy in the process; only a fraction of the energy at the surface reaches the abyssal ocean. An open question is whether and, if yes, how these weakened inertial motions could cause mixing in the deep. We review the progress in the mathematical description of a mechanism that results in an intense breaking of near-inertial waves near the bottom of the ocean and thus enhances the mixing. We give an overview of the present state of understanding of the problem covering both the published and the unpublished results; we also outline the key open questions. For typical ocean stratification, the account of the horizontal component of the Earth's rotation leads to the existence of near-bottom wide waveguides for near-inertial waves. Due to the β-effect these waveguides are narrowing in the poleward direction. Near-inertial waves propagating poleward get trapped in the waveguides; we describe how in the process these waves are focusing more and more in the vertical direction, while simultaneously their group velocity tends to zero and wave-induced vertical shear significantly increases. This causes the development of shear instability, which is interpreted as wave breaking. Remarkably, this mechanism of local intensification of turbulent mixing in the abyssal ocean can be adequately described within the framework of linear theory. The qualitative picture is similar to wind wave breaking on a beach: the abyssal ocean always acts as a surf zone for near-inertial waves.

  4. The Coordinated Ocean Wave Climate Project

    NASA Astrophysics Data System (ADS)

    Hemer, Mark; Dobrynin, Mikhail; Erikson, Li; Lionello, Piero; Mori, Nobuhito; Semedo, Alvaro; Wang, Xiaolan

    2016-04-01

    Future 21st Century changes in wind-wave climate have broad implications for marine and coastal infrastructure and ecosystems. Atmosphere-ocean general circulation models (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-waves. To fill this information gap a growing number of studies are using GCM outputs and independently producing global and regional scale wind-wave climate projections. Furthermore, additional studies are actively coupling wind-wave dependent atmosphere-ocean exchanges into GCMs, to improve physical representation and quantify the impact of waves in the coupled climate system, and can also deliver wave 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-waves in the climate system and their projected changes, we present outcomes of the JCOMM supported Coordinated Ocean Wave Climate Project (COWCLIP). The objective of COWCLIP is twofold: to make community based ensembles of wave 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-waves in the coupled ocean-atmosphere climate system. We will present the current 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.

  5. numerical broadband modelling of ocean waves, from 1 to 300 s: implications for seismic wave sources and wave climate studies

    NASA Astrophysics Data System (ADS)

    Ardhuin, F.; Stutzmann, E.; Gualtieri, L.

    2014-12-01

    Ocean waves provide most of the energy that feeds the continuous vertical oscillations of the solid Earth. Three period bands are usually identified. The hum contains periods longer than 30 s, and the primary and secondary peaks are usually centered around 15 and 5 s, respectively. Motions in all three bands are recorded everywhere on our planet and can provide information on both the solid Earth structure and the ocean wave climate over the past century. Here we describe recent efforts to extend the range of validity of ocean wave models to cover periods from 1 to 300 s (Ardhuin et al., Ocean Modelling 2014), and the resulting public database of ocean wave spectra (http://tinyurl.com/iowagaftp/HINDCAST/ ). We particularly discuss the sources of uncertainty for building a numerical model of acoustic and seismic noise on this knowledge of ocean wave spectra. For acoustic periods shorter than 3 seconds, the main uncertainties are the directional distributions of wave energy (Ardhuin et al., J. Acoust. Soc. Amer. 2013). For intermediate periods (3 to 25 s), the propagation properties of seismic waves are probably the main source of error when producing synthetic spectra of Rayleigh waves (Ardhuin et al. JGR 2011, Stutzmann et al. GJI 2012). For the longer periods (25 to 300 s), the poor knowledge of the bottom topography details may be the limiting factor for estimating hum spectra or inverting hum measurements in properties of the infragravity wave field. All in all, the space and time variability of recorded seismic and acoustic spectra is generally well reproduced in the band 3 to 300 s, and work on shorter periods is under way. This direct model can be used to search for missing noise sources, such as wave scattering in the marginal ice zone, find events relevant for solid earth studies (e.g. Obrebski et al. JGR 2013) or invert wave climate properties from microseismic records. The figure shows measured spectra of the vertical ground acceleration, and modeled

  6. Measuring Ocean Surface Waves using Signal Reflections from Geostationary Satellites

    NASA Astrophysics Data System (ADS)

    Ouellette, J. D.; Dowgiallo, D. J.; Hwang, P. A.; Toporkov, J. V.

    2017-12-01

    The delay-Doppler response of communications signals (such as GNSS) reflected off the ocean surface is well-known to have properties which strongly correlate with surface wind conditions and ocean surface roughness. This study extends reflectometry techniques currently applied to the GNSS constellation to include geostationary communications satellites such as XM Radio. In this study, ocean wind conditions and significant wave height will be characterized using the delay-Doppler response of XM Radio signals reflected off of ocean surface waves. Using geostationary satellites for reflectometry-based remote sensing of oceans presents two primary advantages. First, longer coherent integration times can be achieved, which boosts signal processing gain and allows for finer Doppler resolution. Second, being designed for wide-area broadcast communications, the ground-received power of these geostationary satellite signals tends to be many orders of magnitude stronger than e.g. GNSS signals. Reflections of such signals from the ocean are strong enough to be received well outside of the specular region. This flexibility of viewing geometry allows signal processing to be performed on data received from multiple incidence/reception angles, which can provide a more complete characterization of ocean surface roughness and surface wind vectors. This work will include studies of simulated and measured delay-Doppler behavior of XM Radio signals reflected from dynamic ocean surfaces. Simulation studies will include inter-comparison between a number of hydrodynamic and electromagnetic models. Results from simulations will be presented as delay-Doppler plots and will be compared with delay-Doppler behavior observed in measured data. Measured data will include field campaign results from early- to mid-2017 in which the US Naval Research Laboratory's in-house XM reflectometer-receiver was deployed near the coasts of Virginia and North Carolina to observe reflections from wind

  7. Ocean wave electric generators

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

    Rosenberg, H.R.

    This patent describes an apparatus for generating electricity from ocean waves. It consists of: 1.) a hollow buoyant duck positioned in the path of waves including a core about the center axis of which the duck rotates, a lower chamber portion having liquid therein and an upper chamber portion having air therein. The air is alternately compressed and expanded by the liquid in the chamber during the rotational motion of the duck caused by waves. A turbine mounted in the upper portion of the duck is driven by the compressed and expanded air. A generator is coupled to the turbinemore » and operated to produce electrical energy and an air bulb; 2.) a spine having a transverse axial shaft anchoring the spine to the ocean floor. The upper portion of the spine engages the duck to maintain the duck in position. The spine has a curved configuration to concentrate and direct wave energy. The spine configuration acts as a scoop to increase the height of wave peaks and as a foil to increase the depth of wave troughs.« less

  8. Ocean wave characteristic in the Sunda Strait using Wave Spectrum Model

    NASA Astrophysics Data System (ADS)

    Rachmayani, R.; Ningsih, N. S.; Adiprabowo, S. R.; Nurfitri, S.

    2018-03-01

    The wave characteristics including significant wave height and direction, seas and swell in the Sunda Strait are analyzed seasonally to provide marine weather information. This is crucial for establishing secured marine activities between islands of Sumatera and Java. Ocean wave characteristics in the Sunda Strait are simulated for one year (July 1996–June 1977) by using SWAN numerical model. The ocean wave characteristics in the Sunda Strait are divided into three areas of interest; southern, centre and northern part of the Sunda Strait. Despite a weaker local wind, the maximum significant wave height is captured at the southern part with its height of 2.6 m in November compared to other seasonally months. This is associated with the dominated swell from the Indian Ocean contributes on wave energy toward the Sunda Strait. The 2D spectrum analysis exhibits the monthly wave characteristic at southern part that is dominated by seas along the year and swell propagating from the Indian Ocean to the Sunda Strait during December to February (northwest monsoon), May, and November. Seas and swell at northern part of the Sunda Strait are apprehended weaker compared to other parts of the Sunda Strait due to its location is farther from the Indian Ocean.

  9. Ocean Wave Separation Using CEEMD-Wavelet in GPS Wave Measurement.

    PubMed

    Wang, Junjie; He, Xiufeng; Ferreira, Vagner G

    2015-08-07

    Monitoring ocean waves plays a crucial role in, for example, coastal environmental and protection studies. Traditional methods for measuring ocean waves are based on ultrasonic sensors and accelerometers. However, the Global Positioning System (GPS) has been introduced recently and has the advantage of being smaller, less expensive, and not requiring calibration in comparison with the traditional methods. Therefore, for accurately measuring ocean waves using GPS, further research on the separation of the wave signals from the vertical GPS-mounted carrier displacements is still necessary. In order to contribute to this topic, we present a novel method that combines complementary ensemble empirical mode decomposition (CEEMD) with a wavelet threshold denoising model (i.e., CEEMD-Wavelet). This method seeks to extract wave signals with less residual noise and without losing useful information. Compared with the wave parameters derived from the moving average skill, high pass filter and wave gauge, the results show that the accuracy of the wave parameters for the proposed method was improved with errors of about 2 cm and 0.2 s for mean wave height and mean period, respectively, verifying the validity of the proposed method.

  10. Ocean Wave Separation Using CEEMD-Wavelet in GPS Wave Measurement

    PubMed Central

    Wang, Junjie; He, Xiufeng; Ferreira, Vagner G.

    2015-01-01

    Monitoring ocean waves plays a crucial role in, for example, coastal environmental and protection studies. Traditional methods for measuring ocean waves are based on ultrasonic sensors and accelerometers. However, the Global Positioning System (GPS) has been introduced recently and has the advantage of being smaller, less expensive, and not requiring calibration in comparison with the traditional methods. Therefore, for accurately measuring ocean waves using GPS, further research on the separation of the wave signals from the vertical GPS-mounted carrier displacements is still necessary. In order to contribute to this topic, we present a novel method that combines complementary ensemble empirical mode decomposition (CEEMD) with a wavelet threshold denoising model (i.e., CEEMD-Wavelet). This method seeks to extract wave signals with less residual noise and without losing useful information. Compared with the wave parameters derived from the moving average skill, high pass filter and wave gauge, the results show that the accuracy of the wave parameters for the proposed method was improved with errors of about 2 cm and 0.2 s for mean wave height and mean period, respectively, verifying the validity of the proposed method. PMID:26262620

  11. Ocean waves monitor system by inland microseisms

    NASA Astrophysics Data System (ADS)

    Lin, L. C.; Bouchette, F.; Chang, E. T. Y.

    2016-12-01

    Microseisms are continuous ground oscillations which have been wildly introduced for decades. It is well known that the microseismicity in the frequency band from 0.05 to about 1 Hz partly results from ocean waves, which has been first explained by Longuet-Higgins [1950]. The generation mechanism for such a microseismicity is based on nonlinear wave-wave interactions which drive pressure pulses within the seafloor. The resulting ground pressure fluctuations yield ground oscillations at a double frequency (DF) with respect to that of current ocean waves. In order to understand the characteristics of DF microseisms associated with different wave sources, we aim to analyze and interpret the spectra of DF microseisms by using the simple spectrum method [Rabinovich, 1997] at various inland seismometer along the Taiwan coast. This is the first monitoring system of ocean waves observed by inland seismometers in Taiwan. The method is applied to identify wave sources by estimating the spectral ratios of wave induced microseisms associated with local winds and typhoons to background spectra. Microseism amplitudes above 0.2 Hz show a good correlation with wind-driven waves near the coast. Comparison of microseism band between 0.1 and 0.2 Hz with buoys in the deep sea shows a strong correlation of seismic amplitude with storm generated waves, implying that such energy portion originates in remote regions. Results indicate that microseisms observed at inland sites can be a potential tool for the tracking of typhoon displacements and the monitoring of extreme ocean waves in real time. Real- time Microseism-Ocean Waves Monitoring Website (http://mwave.droppages.com/) Reference Rabinovich, A. B. (1997) "Spectral analysis of tsunami waves: Separation of source and topography effects," J. Geophys. Res., Vol. 102, p. 12,663-12,676. Longuet-Higgins, M.S. (1950) "A theory of origin of microseisms," Philos. Trans. R. Soc., A. 243, pp. 1-35.

  12. Soliton Turbulence in Shallow Water Ocean Surface Waves

    NASA Astrophysics Data System (ADS)

    Costa, Andrea; Osborne, Alfred R.; Resio, Donald T.; Alessio, Silvia; Chrivı, Elisabetta; Saggese, Enrica; Bellomo, Katinka; Long, Chuck E.

    2014-09-01

    We analyze shallow water wind waves in Currituck Sound, North Carolina and experimentally confirm, for the first time, the presence of soliton turbulence in ocean waves. Soliton turbulence is an exotic form of nonlinear wave motion where low frequency energy may also be viewed as a dense soliton gas, described theoretically by the soliton limit of the Korteweg-deVries equation, a completely integrable soliton system: Hence the phrase "soliton turbulence" is synonymous with "integrable soliton turbulence." For periodic-quasiperiodic boundary conditions the ergodic solutions of Korteweg-deVries are exactly solvable by finite gap theory (FGT), the basis of our data analysis. We find that large amplitude measured wave trains near the energetic peak of a storm have low frequency power spectra that behave as ˜ω-1. We use the linear Fourier transform to estimate this power law from the power spectrum and to filter densely packed soliton wave trains from the data. We apply FGT to determine the soliton spectrum and find that the low frequency ˜ω-1 region is soliton dominated. The solitons have random FGT phases, a soliton random phase approximation, which supports our interpretation of the data as soliton turbulence. From the probability density of the solitons we are able to demonstrate that the solitons are dense in time and highly non-Gaussian.

  13. Internal Waves, Indian Ocean

    NASA Technical Reports Server (NTRS)

    1990-01-01

    This photograph, taken in sunglint conditions, captures open ocean internal waves which are diffracting around shoals south of the Seychelle islands (4.5S, 55.5E) and recombining to form interference patterns. The clouds to the north of the waves cover two of the Seychelle islands: Silhouette and Mahe. Mahe is the main island of the archipelago. The small rocky island surrounded by reef around which the waves diffract is Platte Island.

  14. Sensitivity of Rogue Waves Predictions to the Oceanic Stratification

    NASA Astrophysics Data System (ADS)

    Guo, Qiuchen; Alam, Mohammad-Reza

    2014-11-01

    Oceanic rogue waves are short-lived very large amplitude waves (a giant crest typically followed or preceded by a deep trough) that appear and disappear suddenly in the ocean causing damages to ships and offshore structures. Assuming that the state of the ocean at the present time is perfectly known, then the upcoming rogue waves can be predicted via numerically solving the equations that govern the evolution of the waves. The state of the art radar technology can now provide accurate wave height measurement over large spatial domains and when combined with advanced wave-field reconstruction techniques together render deterministic details of the current state of the ocean (i.e. surface elevation and velocity field) at any given moment of the time with a very high accuracy. The ocean water density is, however, stratified (mainly due to the salinity and temperature differences). This density stratification, with today's technology, is very difficult to be measured accurately. As a result in most predictive schemes these density variations are neglected. While the overall effect of the stratification on the average state of the ocean may not be significant, here we show that these density variations can strongly affect the prediction of oceanic rogue waves. Specifically, we consider a broadband oceanic spectrum in a two-layer density stratified fluid, and study via extensive statistical analysis the effects of strength of the stratification (difference between densities) and the depth of the thermocline on the prediction of upcoming rogue waves.

  15. Evidence for infragravity wave-tide resonance in deep oceans.

    PubMed

    Sugioka, Hiroko; Fukao, Yoshio; Kanazawa, Toshihiko

    2010-10-05

    Ocean tides are the oscillatory motions of seawater forced by the gravitational attraction of the Moon and Sun with periods of a half to a day and wavelengths of the semi-Pacific to Pacific scale. Ocean infragravity (IG) waves are sea-surface gravity waves with periods of several minutes and wavelengths of several dozen kilometres. Here we report the first evidence of the resonance between these two ubiquitous phenomena, mutually very different in period and wavelength, in deep oceans. The evidence comes from long-term, large-scale observations with arrays of broadband ocean-bottom seismometers located at depths of more than 4,000 m in the Pacific Ocean. This observational evidence is substantiated by a theoretical argument that IG waves and the tide can resonantly couple and that such coupling occurs over unexpectedly wide areas of the Pacific Ocean. Through this resonant coupling, some of ocean tidal energy is transferred in deep oceans to IG wave energy.

  16. Radiative transfer in the earth's atmosphere and ocean: influence of ocean waves.

    PubMed

    Plass, G N; Kattawar, G W; Guinn, J A

    1975-08-01

    The radiance in the earth's atmosphere and ocean is calculated for a realistic model including an ocean surface with waves. Individual photons are followed in a Monte Carlo calculation. In the atmosphere, both Rayleigh scattering by the molecules and Mie scattering by the aerosols as well as molecular and aerosol absorption are taken into account. Similarly, in the ocean, both Rayleigh scattering by the water molecules and Mie scattering by the hydrosols as well as absorption by the water molecules and hydrosols are considered. Separate single-scattering functions are used which are calculated separately for the aerosols and the hydrosols from the Mie theory with appropriate and different size distributions in each case. The scattering angles are determined from the appropriate scattering function including the strong forwardscattering peak when there is aerosol or hydrosol scattering. Both the reflected and refracted rays, as well as the rays that undergo total internal reflection, are followed at the oceanc surface. The wave slope is chosen from the Cox-Munk distribution. Graphs show the influence of the waves on the upward radiance at the top of the atmosphere and just above the ocean surface and on the downward radiance just below the ocean surface as well as deeper within the ocean. The radiance changes are sufficient at the top of the atmosphere to determine the sea state from satellite measurements. Within the ocean the waves smooth out the abrupt transition that occurs at the edge of the allowed cone for radiation entering a calm ocean. The influence of the waves on the contrast between the sky and sea at the horizon is discussed. It is shown that the downward flux just below the surface increases with wind speed at all solar angles.

  17. Ocean floor mounting of wave energy converters

    DOEpatents

    Siegel, Stefan G

    2015-01-20

    A system for mounting a set of wave energy converters in the ocean includes a pole attached to a floor of an ocean and a slider mounted on the pole in a manner that permits the slider to move vertically along the pole and rotate about the pole. The wave energy converters can then be mounted on the slider to allow adjustment of the depth and orientation of the wave energy converters.

  18. Numerical Investigations of Wave-Induced Mixing in Upper Ocean Layer

    NASA Astrophysics Data System (ADS)

    Guan, Changlong

    2017-04-01

    The upper ocean layer is playing an important role in ocean-atmosphere interaction. The typical characteristics depicting the upper ocean layer are the sea surface temperature (SST) and the mixed layer depth (MLD). So far, the existing ocean models tend to over-estimate SST and to under-estimate MLD, due to the inadequate mixing in the mixing layer, which is owing to that several processes related mixing in physics are ignored in these ocean models. The mixing induced by surface gravity wave is expected to be able to enhance the mixing in the upper ocean layer, and therefore the over-estimation of SST and the under-estimate of MLD could be improved by including wave-induced mixing. The wave-induced mixing could be accomplished by the physical mechanisms, such as wave breaking (WB), wave-induced Reynolds stress (WR), and wave-turbulence interaction (WT). The General Ocean Turbulence Model (GOTM) is employed to investigate the effects of the three mechanisms concerning wave-induced mixing. The numerical investigation is carried out for three turbulence closure schemes, say, k-epsilon, k-omega and Mellor-Yamada (1982), with the observational data from OSC Papa station and wave data from ECMWF. The mixing enhancement by various waved-induced mixing mechanisms is investigated and verified.

  19. 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.

  20. Internal Waves, Western Indian Ocean

    NASA Image and Video Library

    1991-12-01

    STS044-79-077 (24 Nov.-1 Dec. 1991) --- This photograph, captured from the Earth-orbiting Space Shuttle Atlantis, shows sunglint pattern in the western tropical Indian Ocean. Several large internal waves reflect around a shallow area on the sea floor. NASA scientists studying the STS-44 photography believe the shallow area to be a sediment (a submerged mountain) on top of the Mascarene Plateau, located northeast of Madagascar at approximately 5.6 degrees south latitude and 55.7 degrees east longitude. Internal waves are similar to surface ocean waves, except that they travel inside the water column along the boundary between water layers of different density. At the surface, their passage is marked on the sea surface by bands of smooth and rough water. These bands appear in the sunglint pattern as areas of brighter or darker water. NASA scientists point out that, when the waves encounter an obstacle, such as a near-surface seamount, they bend or refract around the obstacle in the same manner as surface waves bend around an island or headland.

  1. Wave power potential in Malaysian territorial waters

    NASA Astrophysics Data System (ADS)

    Asmida Mohd Nasir, Nor; Maulud, Khairul Nizam Abdul

    2016-06-01

    Up until today, Malaysia has used renewable energy technology such as biomass, solar and hydro energy for power generation and co-generation in palm oil industries and also for the generation of electricity, yet, we are still far behind other countries which have started to optimize waves for similar production. Wave power is a renewable energy (RE) transported by ocean waves. It is very eco-friendly and is easily reachable. This paper presents an assessment of wave power potential in Malaysian territorial waters including waters of Sabah and Sarawak. In this research, data from Malaysia Meteorology Department (MetMalaysia) is used and is supported by a satellite imaginary obtained from National Aeronautics and Space Administration (NASA) and Malaysia Remote Sensing Agency (ARSM) within the time range of the year 1992 until 2007. There were two types of analyses conducted which were mask analysis and comparative analysis. Mask analysis of a research area is the analysis conducted to filter restricted and sensitive areas. Meanwhile, comparative analysis is an analysis conducted to determine the most potential area for wave power generation. Four comparative analyses which have been carried out were wave power analysis, comparative analysis of wave energy power with the sea topography, hot-spot area analysis and comparative analysis of wave energy with the wind speed. These four analyses underwent clipping processes using Geographic Information System (GIS) to obtain the final result. At the end of this research, the most suitable area to develop a wave energy converter was found, which is in the waters of Terengganu and Sarawak. Besides that, it was concluded that the average potential energy that can be generated in Malaysian territorial waters is between 2.8kW/m to 8.6kW/m.

  2. Effects of surface wave breaking on the oceanic boundary layer

    NASA Astrophysics Data System (ADS)

    He, Hailun; Chen, Dake

    2011-04-01

    Existing laboratory studies suggest that surface wave breaking may exert a significant impact on the formation and evolution of oceanic surface boundary layer, which plays an important role in the ocean-atmosphere coupled system. However, present climate models either neglect the effects of wave breaking or treat them implicitly through some crude parameterization. Here we use a one-dimensional ocean model (General Ocean Turbulence Model, GOTM) to investigate the effects of wave breaking on the oceanic boundary layer on diurnal to seasonal time scales. First a set of idealized experiments are carried out to demonstrate the basic physics and the necessity to include wave breaking. Then the model is applied to simulating observations at the northern North Sea and the Ocean Weather Station Papa, which shows that properly accounting for wave breaking effects can improve model performance and help it to successfully capture the observed upper ocean variability.

  3. Mechanical Extraction of Power From Ocean Currents and Tides

    NASA Technical Reports Server (NTRS)

    Jones, Jack; Chao, Yi

    2010-01-01

    A proposed scheme for generating electric power from rivers and from ocean currents, tides, and waves is intended to offer economic and environmental advantages over prior such schemes, some of which are at various stages of implementation, others of which have not yet advanced beyond the concept stage. This scheme would be less environmentally objectionable than are prior schemes that involve the use of dams to block rivers and tidal flows. This scheme would also not entail the high maintenance costs of other proposed schemes that call for submerged electric generators and cables, which would be subject to degradation by marine growth and corrosion. A basic power-generation system according to the scheme now proposed would not include any submerged electrical equipment. The submerged portion of the system would include an all-mechanical turbine/pump unit that would superficially resemble a large land-based wind turbine (see figure). The turbine axis would turn slowly as it captured energy from the local river flow, ocean current, tidal flow, or flow from an ocean-wave device. The turbine axis would drive a pump through a gearbox to generate an enclosed flow of water, hydraulic fluid, or other suitable fluid at a relatively high pressure [typically approx.500 psi (approx.3.4 MPa)]. The pressurized fluid could be piped to an onshore or offshore facility, above the ocean surface, where it would be used to drive a turbine that, in turn, would drive an electric generator. The fluid could be recirculated between the submerged unit and the power-generation facility in a closed flow system; alternatively, if the fluid were seawater, it could be taken in from the ocean at the submerged turbine/pump unit and discharged back into the ocean from the power-generation facility. Another alternative would be to use the pressurized flow to charge an elevated reservoir or other pumped-storage facility, from whence fluid could later be released to drive a turbine/generator unit at a

  4. Rogue waves in the ocean - review and progress

    NASA Astrophysics Data System (ADS)

    Pelinovsky, Efim; Kharif, Christian; Slunyaev, Alexey

    2010-05-01

    Rogue waves in the ocean and physical mechanisms of their appearance are discussed. Theyse waves are among waves naturally observed by people on the sea surface that represent inseparable feature of the Ocean. Rogue waves appear from nowhere, cause danger and disappear at once. They may occur at the surface of a relatively calm sea, reach not very high amplitudes, but be fatal for ships and crew due to their unexpectedness and abnormal features. The billows appear suddenly exceeding the surrounding waves twice and more, and obtained many names: abnormal, exceptional, extreme, giant, huge, sudden, episodic, freak, monster, rogue, vicious, killer, mad- or rabid-dog waves; cape rollers, holes in the sea, walls of water, three sisters… Freak monsters, though living for seconds, were able to arouse superstitious fear of the crew, cause damage, death of heedless sailors or the whole ship. All these epithets are full of human fear and feebleness. The serious studies of the phenomenon started about 20-30 years ago and have been intensified during the recent decade. The research is being conducted in different fields: in physics (search of physical mechanisms and adequate models of wave enhancement and statistics), in geoscience (determining the regions and weather conditions when rogue waves are most probable), and in ocean and coastal engineering (estimations of the wave loads on fixed and drifting floating structures). Thus, scientists and engineers specializing in different subject areas are involved in the solution of the problem. The state-of-art of the rogue wave study is summarized in our book [Kharif, Ch., Pelinovsky, E., and Slunyaev, A. Rogue Waves in the Ocean. Springer, 2009] and presented in given review. Firstly, we start with a brief introduction to the problem of freak waves aiming at formulating what is understood as rogue or freak waves, what consequences their existence imply in our life, why people are so worried about them. Then we discuss existing

  5. Book review: Extreme ocean waves

    USGS Publications Warehouse

    Geist, Eric L.

    2017-01-01

    “Extreme Ocean Waves”, edited by E. Pelinovsky and C. Kharif, second edition, Springer International Publishing, 2016; ISBN: 978-3-319-21574-7, ISBN (eBook): 978-3-319-21575-4The second edition of “Extreme Ocean Waves” published by Springer is an update of a collection of 12 papers edited by Efim Pelinovsky and Christian Kharif following the April 2007 meeting of the General Assembly of the European Geosciences Union. In this edition, three new papers have been added and three more have been substantially revised. Color figures are now included, which greatly aids in reading several of the papers, and is especially helpful in visualizing graphs as in the paper on symbolic computation of nonlinear wave resonance (Tobisch et al.). A note on terminology: extreme waves in this volume broadly encompass different types of waves, including deep-water and shallow-water rogue waves (which are alternatively termed freak waves), and internal waves. One new paper on tsunamis (Viroulet et al.) is now included in the second edition of this volume. Throughout the book, the reader will find a combination of laboratory, theoretical, and statistical/empirical treatment necessary for the complete examination of this subject. In the Introduction, the editors underscore the importance of studying extreme waves, documenting a dramatic instance of damaging extreme waves that recently occurred in 2014.

  6. Infragravity waves in the deep ocean: An upward revision

    NASA Astrophysics Data System (ADS)

    Aucan, J.; Ardhuin, F.

    2013-07-01

    Ocean infragravity waves are surface gravity waves with periods of several minutes and corresponding wavelengths of up to tens of kilometers. When propagating freely in the deep ocean, these waves are typically small, several centimeters at most, so they have been seldom studied. In the context of future wide-swath altimetry missions, these waves need to be better quantified as they have wavelengths that will be resolved by such instruments. Here, we analyze the global climatology and variability of infragravity waves in the deep ocean using data from over 40 open ocean locations, with depths larger than 2000 m. We show that typical infragravity wave heights are higher than previously estimated, with winter-averaged values up to 11 mm off the U.S. West Coast, and typically less than 6 mm in the tropics. The mid to high latitudes exhibit a strong seasonal cycle consistent with the local variability of the wind-waves, while the tropical Pacific has a higher energy level during the Austral winter that does not correlate well with the local wind-waves, suggesting a remote source for the recorded infragravity waves. These infragravity wave energies are expected to be a significant contribution to the error budget for possible measurements of sea level associated to sub-mesoscale currents at horizontal scales around 10 km. Hence, a global numerical model of infragravity waves will likely be necessary for the analysis of the planned Surface Water Ocean Topography mission.

  7. Intraseasonal sea surface warming in the western Indian Ocean by oceanic equatorial Rossby waves

    NASA Astrophysics Data System (ADS)

    Rydbeck, Adam V.; Jensen, Tommy G.; Nyadjro, Ebenezer S.

    2017-05-01

    A novel process is identified whereby equatorial Rossby (ER) waves maintain warm sea surface temperature (SST) anomalies against cooling by processes related to atmospheric convection in the western Indian Ocean. As downwelling ER waves enter the western Indian Ocean, SST anomalies of +0.15°C develop near 60°E. These SST anomalies are hypothesized to stimulate convective onset of the Madden-Julian Oscillation. The upper ocean warming that manifests in response to downwelling ER waves is examined in a mixed layer heat budget using observational and reanalysis products, respectively. In the heat budget, horizontal advection is the leading contributor to warming, in part due to an equatorial westward jet of 80 cm s-1 associated with downwelling ER waves. When anomalous currents associated with ER waves are removed in the budget, the warm intraseasonal temperature anomaly in the western Indian Ocean is eliminated in observations and reduced by 55% in reanalysis.

  8. Energy Harvesting from Surface River/Ocean Waves

    NASA Astrophysics Data System (ADS)

    Cai, Wenzheng

    The renewable energy is an important subject especially today as the world is facing the results of the pollution and depletion of the conventional energy resources. Around 70% of the Earth's surface is covered by water where the energy of the waves/tides could be used as alternative source of energy that is sustainable and environmental friendly. Most of the research efforts are focused on the development of the large-scale technologies that can operate in the open Ocean. The potential of the low-frequency and small-amplitude wave condition in shallow rivers and lakes where most of the world wave energy exists has not been explored yet. The objective of the current study is to design and develop new concepts for wave energy extraction, which depend on oscillatory wave motion and have the ability to convert the small and medium waves. The proposed devices are self-generating without any external sources, which makes them lightweight and naturally floating on the surface of the water. Feasibility studies of both designs were performed using numerical modeling and field experiments. The final prototypes achieved power output of 5.0+/-0.6mW and 0.25+/-0.01mW, respectively. Array systems implementing both concepts were also introduced to improve the performance of the devices.

  9. Laser probe for measuring 2-D wave slope spectra of ocean capillary waves

    NASA Technical Reports Server (NTRS)

    Palm, C. S.; Anderson, R. C.; Reece, A. M.

    1977-01-01

    A laser-optical instrument for use in determining the two-dimensional wave-slope spectrum of ocean capillary waves is described. The instrument measures up to a 35-deg tip angle of the surface normal by measuring the position of a refracted laser beam directed vertically upward through a water surface. A telescope, a continuous two-dimensional Schottky barrier photodiode, and a pair of analog dividers render the signals independent of water height and insensitive to laser-beam intensity fluctuations. Calibration is performed entirely in the laboratory before field use. Sample records and wave-slope spectra are shown for one-dimensional wave-tank tests and for two-dimensional ocean tests. These are presented along with comparison spectra for calm and choppy water conditions. A mechanical wave follower was used to adjust the instrument position in the presence of large ocean swell and tides.

  10. Strong and highly variable push of ocean waves on Southern Ocean sea ice.

    PubMed

    Stopa, Justin E; Sutherland, Peter; Ardhuin, Fabrice

    2018-06-05

    Sea ice in the Southern Ocean has expanded over most of the past 20 y, but the decline in sea ice since 2016 has taken experts by surprise. This recent evolution highlights the poor performance of numerical models for predicting extent and thickness, which is due to our poor understanding of ice dynamics. Ocean waves are known to play an important role in ice break-up and formation. In addition, as ocean waves decay, they cause a stress that pushes the ice in the direction of wave propagation. This wave stress could not previously be quantified due to insufficient observations at large scales. Sentinel-1 synthetic aperture radars (SARs) provide high-resolution imagery from which wave height is measured year round encompassing Antarctica since 2014. Our estimates give an average wave stress that is comparable to the average wind stress acting over 50 km of sea ice. We further reveal highly variable half-decay distances ranging from 400 m to 700 km, and wave stresses from 0.01 to 1 Pa. We expect that this variability is related to ice properties and possibly different floe sizes and ice thicknesses. A strong feedback of waves on sea ice, via break-up and rafting, may be the cause of highly variable sea-ice properties.

  11. An ocean kinetic energy converter for low-power applications using piezoelectric disk elements

    NASA Astrophysics Data System (ADS)

    Viñolo, C.; Toma, D.; Mànuel, A.; del Rio, J.

    2013-09-01

    The main problem facing long-term electronic system deployments in the sea, is to find a feasible way to supply them with the power they require. Harvesting mechanical energy from the ocean wave oscillations and converting it into electrical energy, provides an alternative method for creating self-contained power sources. However, the very low and varying frequency of ocean waves, which generally varies from 0.1 Hz to 2 Hz, presents a hurdle which has to be overcome if this mechanical energy is to be harvested. In this paper, a new sea wave kinetic energy converter is described using low-cost disk piezoelectric elements, which has no dependence on their excitement frequency, to feed low-consumption maritime-deployed electronic devices. The operating principles of the piezoelectric device technique are presented, including analytical formulations describing the transfer of energy. Finally, a prototypical design, which generates electrical energy from the motion of a buoy, is introduced. The paper concludes with the the behavior study of the piezoelectric prototype device as a power generator.

  12. Understanding Rossby wave trains forced by the Indian Ocean Dipole

    NASA Astrophysics Data System (ADS)

    McIntosh, Peter C.; Hendon, Harry H.

    2018-04-01

    Convective variations over the tropical Indian Ocean associated with ENSO and the Indian Ocean Dipole force a Rossby wave train that appears to emanate poleward and eastward to the south of Australia and which causes climate variations across southern Australia and more generally throughout the Southern Hemisphere extratropics. However, during austral winter, the subtropical jet that extends from the eastern Indian Ocean into the western Pacific at Australian latitudes should effectively prohibit continuous propagation of a stationary Rossby wave from the tropics into the extratropics because the meridional gradient of mean absolute vorticity goes to zero on its poleward flank. The observed wave train indeed exhibits strong convergence of wave activity flux upon encountering this region of vanishing vorticity gradient and with some indication of reflection back into the tropics, indicating the continuous propagation of the stationary Rossby wave train from low to high latitudes is inhibited across the south of Australia. However, another Rossby wave train appears to emanate upstream of Australia on the poleward side of the subtropical jet and propagates eastward along the waveguide of the eddy-driven (sub-polar) jet into the Pacific sector of the Southern Ocean. This combination of evanescent wave train from the tropics and eastward propagating wave train emanating from higher latitudes upstream of Australia gives the appearance of a continuous Rossby wave train propagating from the tropical Indian Ocean into higher southern latitudes. The extratropical Rossby wave source on the poleward side of the subtropical jet stems from induced changes in transient eddy activity in the main storm track of the Southern Hemisphere. During austral spring, when the subtropical jet weakens, the Rossby wave train emanating from Indian Ocean convection is explained more traditionally by direct dispersion from divergence forcing at low latitudes.

  13. Real world ocean rogue waves explained without the modulational instability.

    PubMed

    Fedele, Francesco; Brennan, Joseph; Ponce de León, Sonia; Dudley, John; Dias, Frédéric

    2016-06-21

    Since the 1990s, the modulational instability has commonly been used to explain the occurrence of rogue waves that appear from nowhere in the open ocean. However, the importance of this instability in the context of ocean waves is not well established. This mechanism has been successfully studied in laboratory experiments and in mathematical studies, but there is no consensus on what actually takes place in the ocean. In this work, we question the oceanic relevance of this paradigm. In particular, we analyze several sets of field data in various European locations with various tools, and find that the main generation mechanism for rogue waves is the constructive interference of elementary waves enhanced by second-order bound nonlinearities and not the modulational instability. This implies that rogue waves are likely to be rare occurrences of weakly nonlinear random seas.

  14. Real world ocean rogue waves explained without the modulational instability

    PubMed Central

    Fedele, Francesco; Brennan, Joseph; Ponce de León, Sonia; Dudley, John; Dias, Frédéric

    2016-01-01

    Since the 1990s, the modulational instability has commonly been used to explain the occurrence of rogue waves that appear from nowhere in the open ocean. However, the importance of this instability in the context of ocean waves is not well established. This mechanism has been successfully studied in laboratory experiments and in mathematical studies, but there is no consensus on what actually takes place in the ocean. In this work, we question the oceanic relevance of this paradigm. In particular, we analyze several sets of field data in various European locations with various tools, and find that the main generation mechanism for rogue waves is the constructive interference of elementary waves enhanced by second-order bound nonlinearities and not the modulational instability. This implies that rogue waves are likely to be rare occurrences of weakly nonlinear random seas. PMID:27323897

  15. A novel method for predicting the power outputs of wave energy converters

    NASA Astrophysics Data System (ADS)

    Wang, Yingguang

    2018-03-01

    This paper focuses on realistically predicting the power outputs of wave energy converters operating in shallow water nonlinear waves. A heaving two-body point absorber is utilized as a specific calculation example, and the generated power of the point absorber has been predicted by using a novel method (a nonlinear simulation method) that incorporates a second order random wave model into a nonlinear dynamic filter. It is demonstrated that the second order random wave model in this article can be utilized to generate irregular waves with realistic crest-trough asymmetries, and consequently, more accurate generated power can be predicted by subsequently solving the nonlinear dynamic filter equation with the nonlinearly simulated second order waves as inputs. The research findings demonstrate that the novel nonlinear simulation method in this article can be utilized as a robust tool for ocean engineers in their design, analysis and optimization of wave energy converters.

  16. Breaking Waves on the Ocean Surface

    NASA Astrophysics Data System (ADS)

    Schwendeman, Michael S.

    In the open ocean, breaking waves are a critical mechanism for the transfer of energy, momentum, and mass between the atmosphere and the ocean. Despite much study, fundamental questions about wave breaking, such as what determines whether a wave will break, remain unresolved. Measurements of oceanic breakers, or "whitecaps," are often used to validate the hypotheses derived in simplified theoretical, numerical, or experimental studies. Real-world measurements are also used to improve the parameterizations of wave-breaking in large global models, such as those forecasting climate change. Here, measurements of whitecaps are presented using ship-based cameras, from two experiments in the North Pacific Ocean. First, a method for georectifying the camera imagery is described using the distant horizon, without additional instrumentation. Over the course of the experiment, this algorithm correctly identifies the horizon in 92% of images in which it is visible. In such cases, the calculation of camera pitch and roll is accurate to within 1 degree. The main sources of error in the final georectification are from mislabeled horizons due to clouds, rain, or poor lighting, and from vertical "heave" motions of the camera, which cannot be calculated with the horizon method. This method is used for correcting the imagery from the first experiment, and synchronizing the imagery from the second experiment to an onboard inertial motion package. Next, measurements of the whitecap coverage, W, are shown from both experiments. Although W is often used in models to represent whitecapping, large uncertainty remains in the existing parameterizations. The data show good agreement with recent measurements using the wind speed. Although wave steepness and dissipation are hypothesized to be more robust predictors of W, this is shown to not always be the case. Wave steepness shows comparable success to the wind parameterizations only when using a mean-square slope variable calculated over the

  17. The physical basis for estimating wave-energy spectra with the radar ocean-wave spectrometer

    NASA Technical Reports Server (NTRS)

    Jackson, Frederick C.

    1987-01-01

    The derivation of the reflectivity modulation spectrum of the sea surface for near-nadir-viewing microwave radars using geometrical optics is described. The equations required for the derivation are presented. The derived reflectivity modulation spectrum provides data on the physical basis of the radar ocean-wave spectrometer measurements of ocean-wave directional spectra.

  18. Internal Waves and Wave Attractors in Enceladus' Subsurface Ocean

    NASA Astrophysics Data System (ADS)

    van Oers, A. M.; Maas, L. R.; Vermeersen, B. L. A.

    2016-12-01

    One of the most peculiar features on Saturn moon Enceladus is its so-called tiger stripe pattern at the geologically active South Polar Terrain (SPT), as first observed in detail by the Cassini spacecraft early 2005. It is generally assumed that the four almost parallel surface lines that constitute this pattern are faults in the icy surface overlying a confined salty water reservoir. In 2013, we formulated the original idea [Vermeersen et al., AGU Fall Meeting 2013, abstract #P53B-1848] that the tiger stripe pattern is formed and maintained by induced, tidally and rotationally driven, wave-attractor motions in the ocean underneath the icy surface of the tiger-stripe region. Such wave-attractor motions are observed in water tank experiments in laboratories on Earth and in numerical experiments [Maas et al., Nature, 338, 557-561, 1997; Drijfhout and Maas, J. Phys. Oceanogr., 37, 2740-2763, 2007; Hazewinkel et al., Phys. Fluids, 22, 107102, 2010]. Numerical simulations show the persistence of wave attractors for a range of ocean shapes and stratifications. The intensification of the wave field near the location of the surface reflections of wave attractors has been numerically and experimentally confirmed. We measured the forces a wave attractor exerts on a solid surface, near a reflection point. These reflection points would correspond to the location of the tiger stripes. Combining experiments and numerical simulations we conclude that (1) wave attractors can exist in Enceladus' subsurface sea, (2) their shape can be matched to the tiger stripes, (3) the wave attractors cause a localized force at the water-ice boundaries, (4) this force could have been large enough to contribute to fracturing the ice and (5) the wave attractors localize energy (and particles) and cause dissipation along its path, helping explain Enceladus' enigmatic heat output at the tiger stripes.

  19. Book review: Nonlinear ocean waves and the inverse scattering transform

    USGS Publications Warehouse

    Geist, Eric L.

    2011-01-01

    Nonlinear Ocean Waves and the Inverse Scattering Transform is a comprehensive examination of ocean waves built upon the theory of nonlinear Fourier analysis. The renowned author, Alfred R. Osborne, is perhaps best known for the discovery of internal solitons in the Andaman Sea during the 1970s. In this book, he provides an extensive treatment of nonlinear water waves based on a nonlinear spectral theory known as the inverse scattering transform. The writing is exceptional throughout the book, which is particularly useful in explaining some of the more difficult mathematical concepts.  Review info: Nonlinear Ocean Waves and the Inverse Scattering Transform. By Alfred R. Osborne, 2010. ISBN: 978-125286299, 917 pp.

  20. Some case studies of ocean wave physical processes utilizing the GSFC airborne radar ocean wave spectrometer

    NASA Technical Reports Server (NTRS)

    Jackson, F. C.

    1984-01-01

    The NASA K sub u band Radar Ocean Wave Spectrometer (ROWS) is an experimental prototype of a possible future satellite instrument for low data rate global waves measurements. The ROWS technique, which utilizes short pulse radar altimeters in a conical scan mode near vertical incidence to map the directional slope spectrum in wave number and azimuth, is briefly described. The potential of the technique is illustrated by some specific case studies of wave physical processes utilizing the aircraft ROWS data. These include: (1) an evaluation of numerical hindcast model performance in storm sea conditions, (2) a study of fetch limited wave growth, and (3) a study of the fully developed sea state. Results of these studies, which are briefly summarized, show how directional wave spectral observations from a mobile platform can contribute enormously to our understanding of wave physical processes.

  1. Wave-Powered Unmanned Surface Vehicle as a Station-Keeping Gateway Node for Undersea Distributed Networks

    DTIC Science & Technology

    2012-09-01

    the vehicles has the same payload in order to determine performance differences and changes in ocean conditions between the Wave Gliders as they transit...and different materials for the vehicle, engineers were able to determine some characteristics of a wave-powered vehicle. The intended use of this wave...small waves, a pressure difference is created, making the wave larger and larger. The waves then coalesce with each other creating longer waves that

  2. 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.

  3. Open Ocean Internal Waves, South China Sea

    NASA Technical Reports Server (NTRS)

    1989-01-01

    These open ocean internal waves were seen in the south China Sea (19.5N, 114.5E). These sets of internal waves most likely coincide with tidal periods about 12 hours apart. The wave length (distance from crest to crest) varies between 1.5 and 5.0 miles and the crest lengths stretch across and beyond this photo for over 75 miles. At lower right, the surface waves are moving at a 30% angle to the internal waves, with parallel low level clouds.

  4. 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

  5. SAR imaging and hydrodynamic analysis of ocean bottom topographic waves

    NASA Astrophysics Data System (ADS)

    Zheng, Quanan; Li, Li; Guo, Xiaogang; Ge, Yong; Zhu, Dayong; Li, Chunyan

    2006-09-01

    The satellite synthetic aperture radar (SAR) images display wave-like patterns of the ocean bottom topographic features at the south outlet of Taiwan Strait (TS). Field measurements indicate that the most TS water body is vertically stratified. However, SAR imaging models available were developed for homogeneous waters. Hence explaining SAR imaging mechanisms of bottom features in a stratified ocean is beyond the scope of those models. In order to explore these mechanisms and to determine the quantitative relations between the SAR imagery and the bottom features, a two-dimensional, three-layer ocean model with sinusoidal bottom topographic features is developed. Analytical solutions and inferences of the momentum equations of the ocean model lead to the following conditions. (1) In the lower layer, the topography-induced waves (topographic waves hereafter) exist in the form of stationary waves, which satisfy a lower boundary resonance condition σ = kC0, here σ is an angular frequency of the stationary waves, k is a wavenumber of bottom topographic corrugation, and C0 is a background current speed. (2) As internal waves, the topographic waves may propagate vertically to the upper layer with an unchanged wavenumber k, if a frequency relation N3 < σ < N2 is satisfied, here N2 and N3 are the Brunt-Wäisälä frequencies of middle layer and upper layer, respectively. (3) The topographic waves are extremely amplified if an upper layer resonance condition is satisfied. The SAR image of topographic waves is derived on the basis of current-modulated small wave spectra. The results indicate that the topographic waves on SAR images have the same wavelength of bottom topographic corrugation, and the imagery brightness peaks are either inphase or antiphase with respect to the topographic corrugation, depending on a sign of a coupling factor. These theoretical predictions are verified by field observations. The results of this study provide a physical basis for quantitative

  6. Open ocean Internal Waves, Namibia Coast, Africa.

    NASA Image and Video Library

    1990-12-10

    These open ocean Internal Waves were seen off the Namibia Coast, Africa (23.0S, 14.0E). The periodic and regularly spaced sets of internal waves most likely coincide with tidal periods about 12 hours apart. The wave length (distance from crest to crest) varies between 1.5 and 5.0 miles and the crest lengths stretch across and beyond the distance of the photo. The waves are intersecting the Namibia coastline at about a 30 degree angle.

  7. Open ocean Internal Waves, Namibia Coast, Africa.

    NASA Technical Reports Server (NTRS)

    1990-01-01

    These open ocean Internal Waves were seen off the Namibia Coast, Africa (23.0S, 14.0E). The periodic and regularly spaced sets of internal waves most likely coincide with tidal periods about 12 hours apart. The wave length (distance from crest to crest) varies between 1.5 and 5.0 miles and the crest lengths stretch across and beyond the distance of the photo. The waves are intersecting the Namibia coastline at about a 30 degree angle.

  8. Rogue Waves in the Ocean

    NASA Astrophysics Data System (ADS)

    Waseda, Takuji

    2010-03-01

    Giant episodic ocean waves that suddenly soar like a wall of water out of an otherwise calm sea are not just a legend. Such waves—which in the past have been called “abnormal,” “exceptional,” “extreme,” and even “vicious killer” waves—are now commonly known as “rogue waves” or “freak waves.” These waves have sunk or severely damaged 22 supercarriers in the world and caused the loss of more than 500 lives in the past 40 years. The largest wave registered by reliable instruments reached 30 meters in height, and the largest wave recorded by visual observation reached about 34 meters, equivalent to the height of an eight-story building. Tales of seafarers from Christopher Columbus to the passengers of luxury cruise ships had long been undervalued by scientists, but in the past 10 or so years, those historical notes and modern testimonies have been scientifically dissected to reveal the nature of these monster waves.

  9. Effects of Offshore Wind Turbines on Ocean Waves

    NASA Astrophysics Data System (ADS)

    Wimer, Nicholas; Churchfield, Matthew; Hamlington, Peter

    2014-11-01

    Wakes from horizontal axis wind turbines create large downstream velocity deficits, thus reducing the available energy for downstream turbines while simultaneously increasing turbulent loading. Along with this deficit, however, comes a local increase in the velocity around the turbine rotor, resulting in increased surface wind speeds. For offshore turbines, these increased speeds can result in changes to the properties of wind-induced waves at the ocean surface. In this study, the characteristics and implications of such waves are explored by coupling a wave simulation code to the Simulator for Offshore Wind Farm Applications (SOWFA) developed by the National Renewable Energy Laboratory. The wave simulator and SOWFA are bi-directionally coupled using the surface wind field produced by an offshore wind farm to drive an ocean wave field, which is used to calculate a wave-dependent surface roughness that is fed back into SOWFA. The details of this combined framework are outlined. The potential for using the wave field created at offshore wind farms as an additional energy resource through the installation of on-site wave converters is discussed. Potential negative impacts of the turbine-induced wave field are also discussed, including increased oscillation of floating turbines.

  10. Nonlinear shallow ocean-wave soliton interactions on flat beaches.

    PubMed

    Ablowitz, Mark J; Baldwin, Douglas E

    2012-09-01

    Ocean waves are complex and often turbulent. While most ocean-wave interactions are essentially linear, sometimes two or more waves interact in a nonlinear way. For example, two or more waves can interact and yield waves that are much taller than the sum of the original wave heights. Most of these shallow-water nonlinear interactions look like an X or a Y or two connected Ys; at other times, several lines appear on each side of the interaction region. It was thought that such nonlinear interactions are rare events: they are not. Here we report that such nonlinear interactions occur every day, close to low tide, on two flat beaches that are about 2000 km apart. These interactions are closely related to the analytic, soliton solutions of a widely studied multidimensional nonlinear wave equation. On a much larger scale, tsunami waves can merge in similar ways.

  11. Ocean Wave Studies with Applications to Ocean Modeling and Improvement of Satellite Altimeter Measurements

    NASA Technical Reports Server (NTRS)

    Glazman, Roman E.

    1999-01-01

    Combining analysis of satellite data (altimeter, scatterometer, high-resolution visible and infrared images, etc.) with mathematical modeling of non-linear wave processes, we investigate various ocean wave fields (on scales from capillary to planetary), their role in ocean dynamics and turbulent transport (of heat and biogeochemical quantities), and their effects on satellite altimeter measuring accuracy. In 1998 my attention was focused on long internal gravity waves (10 to 1000 km), known also as baroclinic inertia-gravity (BIG) waves. We found these waves to be a major factor of altimeter measurements "noise," resulting in a greater uncertainty [up to 10 cm in terms of sea surface height (SSH) amplitude] in the measured SSH signal than that caused by the sea state bias variations (up to 5 cm or so). This effect still remains largely overlooked by the satellite altimeter community. Our studies of BIG waves address not only their influence on altimeter measurements but also their role in global ocean dynamics and in transport and turbulent diffusion of biogeochemical quantities. In particular, in collaboration with Prof Peter Weichman, Caltech, we developed a theory of turbulent diffusion caused by wave motions of most general nature. Applied to the problem of horizontal turbulent diffusion in the ocean, the theory yielded the effective diffusion coefficient as a function of BIG wave parameters obtainable from satellite altimeter data. This effort, begun in 1997, has been successfully completed in 1998. We also developed a theory that relates spatial fluctuations of scalar fields (such as sea surface temperature, chlorophyll concentration, drifting ice concentration, etc.) to statistical characteristics of BIG waves obtainable from altimeter measurements. A manuscript is in the final stages of preparation. In order to verify the theoretical predictions and apply them to observations, we are now analyzing Sea-viewing Wide Field of view Sensor (SeaWiFS) and Field of

  12. The relationship between significant wave height and Indian Ocean Dipole in the equatorial North Indian Ocean

    NASA Astrophysics Data System (ADS)

    Fu, Chen; Wang, Dongxiao; Yang, Lei; Luo, Yao; Zhou, Fenghua; Priyadarshana, Tilak; Yao, Jinglong

    2018-05-01

    Based on reanalysis data, we find that the Indian Ocean Dipole (IOD) plays an important role in the variability of wave climate in the equatorial Northern Indian Ocean (NIO). Significant wave height (SWH) in the equatorial NIO, especially over the waters southeast to Sri Lanka, exhibits strong interannual variations. SWH anomalies in the waters southeast to Sri Lanka correlate well with dipole mode index (DMI) during both summer and autumn. Negative SWH anomalies occur over the oceanic area southeast to Sri Lanka during positive IOD events and vary with different types of IOD. During positive prolonged (unseasonable) IOD, the SWH anomalies are the strongest in autumn (summer); while during positive normal IOD, the SWH anomalies are weak in both summer and autumn. Strong easterly wind anomalies over the southeast oceanic area of Sri Lanka during positive IOD events weaken the original equatorial westerly wind stress, which leads to the decrease in wind-sea waves. The longer wave period during positive IOD events further confirms less wind-sea waves. The SWH anomaly pattern during negative IOD events is nearly opposite to that during positive IOD events.

  13. The relationship between significant wave height and Indian Ocean Dipole in the equatorial North Indian Ocean

    NASA Astrophysics Data System (ADS)

    Fu, Chen; Wang, Dongxiao; Yang, Lei; Luo, Yao; Zhou, Fenghua; Priyadarshana, Tilak; Yao, Jinglong

    2018-06-01

    Based on reanalysis data, we find that the Indian Ocean Dipole (IOD) plays an important role in the variability of wave climate in the equatorial Northern Indian Ocean (NIO). Significant wave height (SWH) in the equatorial NIO, especially over the waters southeast to Sri Lanka, exhibits strong interannual variations. SWH anomalies in the waters southeast to Sri Lanka correlate well with dipole mode index (DMI) during both summer and autumn. Negative SWH anomalies occur over the oceanic area southeast to Sri Lanka during positive IOD events and vary with different types of IOD. During positive prolonged (unseasonable) IOD, the SWH anomalies are the strongest in autumn (summer); while during positive normal IOD, the SWH anomalies are weak in both summer and autumn. Strong easterly wind anomalies over the southeast oceanic area of Sri Lanka during positive IOD events weaken the original equatorial westerly wind stress, which leads to the decrease in wind-sea waves. The longer wave period during positive IOD events further confirms less wind-sea waves. The SWH anomaly pattern during negative IOD events is nearly opposite to that during positive IOD events.

  14. Upper Atmosphere Heating From Ocean-Generated Acoustic Wave Energy

    DOE PAGES

    Bowman, D. C.; Lees, J. M.

    2018-04-27

    We present that colliding sea surface waves generate the ocean microbarom, an acoustic signal that may transmit significant energy to the upper atmosphere. Previous estimates of acoustic energy flux from the ocean microbarom and mountain-wind interactions are on the order of 0.01 to 1 mW/m 2, heating the thermosphere by tens of Kelvins per day. We captured upgoing ocean microbarom waves with a balloon-borne infrasound microphone; the maximum acoustic energy flux was approximately 0.05 mW/m 2. This is about half the average value reported in previous ground-based microbarom observations spanning 8 years. The acoustic flux from the microbarom episode describedmore » here may have heated the thermosphere by several Kelvins per day while the source persisted. Lastly, we suggest that ocean wave models could be used to parameterize acoustically generated heating of the upper atmosphere based on sea state.« less

  15. Upper Atmosphere Heating From Ocean-Generated Acoustic Wave Energy

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

    Bowman, D. C.; Lees, J. M.

    We present that colliding sea surface waves generate the ocean microbarom, an acoustic signal that may transmit significant energy to the upper atmosphere. Previous estimates of acoustic energy flux from the ocean microbarom and mountain-wind interactions are on the order of 0.01 to 1 mW/m 2, heating the thermosphere by tens of Kelvins per day. We captured upgoing ocean microbarom waves with a balloon-borne infrasound microphone; the maximum acoustic energy flux was approximately 0.05 mW/m 2. This is about half the average value reported in previous ground-based microbarom observations spanning 8 years. The acoustic flux from the microbarom episode describedmore » here may have heated the thermosphere by several Kelvins per day while the source persisted. Lastly, we suggest that ocean wave models could be used to parameterize acoustically generated heating of the upper atmosphere based on sea state.« less

  16. Topographic coupling of surface and internal Kelvin waves. [of ocean

    NASA Technical Reports Server (NTRS)

    Chao, S.-Y.

    1980-01-01

    An analysis is presented for computing the diffraction of barotropic Kelvin waves by a localized topographical irregularity on flat-bottom ocean with an arbitrary vertical stratification. It was shown that all baroclinic Kelvin waves will be generated downstream of the bump, with the first baroclinic mode having the largest amplitude. The Poincare waves predominate in the lowest modes, and are more directionally anisotropic. It was concluded that baroclinic Poincare waves radiating offshore from the bump topography could contribute to the internal wave field in the open ocean and provide an alternative mechanism to dissipate the barotropic tides.

  17. Effects of Sea-Surface Waves and Ocean Spray on Air-Sea Momentum Fluxes

    NASA Astrophysics Data System (ADS)

    Zhang, Ting; Song, Jinbao

    2018-04-01

    The effects of sea-surface waves and ocean spray on the marine atmospheric boundary layer (MABL) at different wind speeds and wave ages were investigated. An MABL model was developed that introduces a wave-induced component and spray force to the total surface stress. The theoretical model solution was determined assuming the eddy viscosity coefficient varied linearly with height above the sea surface. The wave-induced component was evaluated using a directional wave spectrum and growth rate. Spray force was described using interactions between ocean-spray droplets and wind-velocity shear. Wind profiles and sea-surface drag coefficients were calculated for low to high wind speeds for wind-generated sea at different wave ages to examine surface-wave and ocean-spray effects on MABL momentum distribution. The theoretical solutions were compared with model solutions neglecting wave-induced stress and/or spray stress. Surface waves strongly affected near-surface wind profiles and sea-surface drag coefficients at low to moderate wind speeds. Drag coefficients and near-surface wind speeds were lower for young than for old waves. At high wind speeds, ocean-spray droplets produced by wind-tearing breaking-wave crests affected the MABL strongly in comparison with surface waves, implying that wave age affects the MABL only negligibly. Low drag coefficients at high wind caused by ocean-spray production increased turbulent stress in the sea-spray generation layer, accelerating near-sea-surface wind. Comparing the analytical drag coefficient values with laboratory measurements and field observations indicated that surface waves and ocean spray significantly affect the MABL at different wind speeds and wave ages.

  18. Linking source region and ocean wave parameters with the observed primary microseismic noise

    NASA Astrophysics Data System (ADS)

    Juretzek, C.; Hadziioannou, C.

    2017-12-01

    In previous studies, the contribution of Love waves to the primary microseismic noise field was found to be comparable to those of Rayleigh waves. However, so far only few studies analysed both wave types present in this microseismic noise band, which is known to be generated in shallow water and the theoretical understanding has mainly evolved for Rayleigh waves only. Here, we study the relevance of different source region parameters on the observed primary microseismic noise levels of Love and Rayleigh waves simultaneously. By means of beamforming and correlation of seismic noise amplitudes with ocean wave heights in the period band between 12 and 15 s, we analysed how source areas of both wave types compare with each other around Europe. The generation effectivity in different source regions was compared to ocean wave heights, peak ocean gravity wave propagation direction and bathymetry. Observed Love wave noise amplitudes correlate comparably well with near coastal ocean wave parameters as Rayleigh waves. Some coastal regions serve as especially effective sources for one or the other wave type. These coincide not only with locations of high wave heights but also with complex bathymetry. Further, Rayleigh and Love wave noise amplitudes seem to depend equally on the local ocean wave heights, which is an indication for a coupled variation with swell height during the generation of both wave types. However, the wave-type ratio varies directionally. This observation likely hints towards a spatially varying importance of different source mechanisms or structural influences. Further, the wave-type ratio is modulated depending on peak ocean wave propagation directions which could indicate a variation of different source mechanism strengths but also hints towards an imprint of an effective source radiation pattern. This emphasizes that the inclusion of both wave types may provide more constraints for the understanding of acting generation mechanisms.

  19. Novel wave power analysis linking pressure-flow waves, wave potential, and the forward and backward components of hydraulic power.

    PubMed

    Mynard, Jonathan P; Smolich, Joseph J

    2016-04-15

    Wave intensity analysis provides detailed insights into factors influencing hemodynamics. However, wave intensity is not a conserved quantity, so it is sensitive to diameter variations and is not distributed among branches of a junction. Moreover, the fundamental relation between waves and hydraulic power is unclear. We, therefore, propose an alternative to wave intensity called "wave power," calculated via incremental changes in pressure and flow (dPdQ) and a novel time-domain separation of hydraulic pressure power and kinetic power into forward and backward wave-related components (ΠP±and ΠQ±). Wave power has several useful properties:1) it is obtained directly from flow measurements, without requiring further calculation of velocity;2) it is a quasi-conserved quantity that may be used to study the relative distribution of waves at junctions; and3) it has the units of power (Watts). We also uncover a simple relationship between wave power and changes in ΠP±and show that wave reflection reduces transmitted power. Absolute values of ΠP±represent wave potential, a recently introduced concept that unifies steady and pulsatile aspects of hemodynamics. We show that wave potential represents the hydraulic energy potential stored in a compliant pressurized vessel, with spatial gradients producing waves that transfer this energy. These techniques and principles are verified numerically and also experimentally with pressure/flow measurements in all branches of a central bifurcation in sheep, under a wide range of hemodynamic conditions. The proposed "wave power analysis," encompassing wave power, wave potential, and wave separation of hydraulic power provides a potent time-domain approach for analyzing hemodynamics. Copyright © 2016 the American Physiological Society.

  20. Near Field Ocean Surface Waves Acoustic Radiation Observation and Modeling

    NASA Astrophysics Data System (ADS)

    Ardhuin, F.; Peureux, C.; Royer, J. Y.

    2016-12-01

    The acoustic noise generation by nonlinearly interacting surface gravity waves has been studied for a long time both theoretically and experimentally [Longuet-Higgins 1951]. The associated far field noise is continuously measured by a vast network of seismometers at the ocean bottom and on the continents. It can especially be used to infer the time variability of short ocean waves statistics [Peureux and Ardhuin 2016]. However, better quantitative estimates of the latter are made difficult due to a poor knowledge of the Earth's crust characteristics, whose coupling with acoustic modes can affect large uncertainties to the frequency response at the bottom of the ocean.The pressure field at depths less than an acoustic wave length to the surface is made of evanescent modes which vanish away from their sources (near field) [Cox and Jacobs 1989]. For this reason, they are less affected by the ocean bottom composition. This near field is recorded and analyzed in the frequency range 0.1 to 0.5 Hz approximately, at two locations : at a shallow site in the North-East Atlantic continental shelf and a deep water site in the Southern Indian ocean, where pressure measurements are performed at the ocean bottom (ca. 100 m) and at 300 m water depth respectively. Evanescent and propagating Rayleigh modes are compared against theoretical predictions. Comparisons against surface waves hindcast based on WAVEWATCH(R) III modeling framework help assessing its performances and can be used to help future model improvements.References Longuet-Higgins, M. S., A Theory of the Origin of Microseisms, Philos. Trans. Royal Soc. A, 1950, 243, 1-3. Peureux, C. and Ardhuin, F., Ocean bottom pressure records from the Cascadia array and short surface gravity waves, J. Geophys. Res. Oceans, 2016, 121, 2862-2873. Cox, C. S. & Jacobs, D. C., Cartesian diver observations of double frequency pressure fluctuations in the upper levels of the ocean, Geophys. Res. Lett., 1989, 16, 807-810.

  1. A Comparison Between Internal Waves Observed in the Southern Ocean and Lee Wave Generation Theory

    NASA Astrophysics Data System (ADS)

    Nikurashin, M.; Benthuysen, J.; Naveira Garabato, A.; Polzin, K. L.

    2016-02-01

    Direct observations in the Southern Ocean report enhanced internal wave activity and turbulence in a few kilometers above rough bottom topography. The enhancement is co-located with the deep-reaching fronts of the Antarctic Circumpolar Current, suggesting that the internal waves and turbulence are sustained by near-bottom flows interacting with rough topography. Recent numerical simulations confirm that oceanic flows impinging on rough small-scale topography are very effective generators of internal gravity waves and predict vigorous wave radiation, breaking, and turbulence within a kilometer above bottom. However, a linear lee wave generation theory applied to the observed bottom topography and mean flow characteristics has been shown to overestimate the observed rates of the turbulent energy dissipation. In this study, we compare the linear lee wave theory with the internal wave kinetic energy estimated from finestructure data collected as part of the Diapycnal and Isopycnal Mixing Experiment in the Southern Ocean (DIMES). We show that the observed internal wave kinetic energy levels are generally in agreement with the theory. Consistent with the lee wave theory, the observed internal wave kinetic energy scales quadratically with the mean flow speed, stratification, and topographic roughness. The correlation coefficient between the observed internal wave kinetic energy and mean flow and topography parameters reaches 0.6-0.8 for the 100-800 m vertical wavelengths, consistent with the dominant lee wave wavelengths, and drops to 0.2-0.5 for wavelengths outside this range. A better agreement between the lee wave theory and the observed internal wave kinetic energy than the observed turbulent energy dissipation suggests remote breaking of internal waves.

  2. Freak waves in random oceanic sea states.

    PubMed

    Onorato, M; Osborne, A R; Serio, M; Bertone, S

    2001-06-18

    Freak waves are very large, rare events in a random ocean wave train. Here we study their generation in a random sea state characterized by the Joint North Sea Wave Project spectrum. We assume, to cubic order in nonlinearity, that the wave dynamics are governed by the nonlinear Schrödinger (NLS) equation. We show from extensive numerical simulations of the NLS equation how freak waves in a random sea state are more likely to occur for large values of the Phillips parameter alpha and the enhancement coefficient gamma. Comparison with linear simulations is also reported.

  3. Modeling ocean wave propagation under sea ice covers

    NASA Astrophysics Data System (ADS)

    Zhao, Xin; Shen, Hayley H.; Cheng, Sukun

    2015-02-01

    Operational ocean wave models need to work globally, yet current ocean wave models can only treat ice-covered regions crudely. The purpose of this paper is to provide a brief overview of ice effects on wave 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 wave energy. Only long swells can penetrate deep into an ice cover. Being closest to open water, wave propagation in the marginal ice zone is the most complex to model. 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 models that describe wave propagation through an idealized ice cover: mass loading, thin elastic plate, and viscous layer models. From physical arguments we may conjecture that mass loading model is suitable for disjoint aggregates of ice floes much smaller than the wavelength, thin elastic plate model is suitable for a continuous ice sheet, and the viscous layer model is suitable for grease ice. For different sea ice types we may need different wave ice interaction models. A recently proposed viscoelastic model is able to synthesize all three classic models into one. Under suitable limiting conditions it converges to the three previous models. The complete theoretical framework for evaluating wave propagation through various ice covers need to be implemented in the operational ocean wave models. In this review, we introduce the sea ice types, previous wave ice interaction models, wave attenuation mechanisms, the methods to calculate wave reflection and transmission between different ice covers, and the effect of ice floe breaking on shaping the sea ice morphology

  4. Seismic Wave Propagation in Icy Ocean Worlds

    NASA Astrophysics Data System (ADS)

    Stähler, Simon C.; Panning, Mark P.; Vance, Steven D.; Lorenz, Ralph D.; van Driel, Martin; Nissen-Meyer, Tarje; Kedar, Sharon

    2018-01-01

    Seismology was developed on Earth and shaped our model of the Earth's interior over the twentieth century. With the exception of the Philae lander, all in situ extraterrestrial seismological effort to date was limited to other terrestrial planets. All have in common a rigid crust above a solid mantle. The coming years may see the installation of seismometers on Europa, Titan, and Enceladus, so it is necessary to adapt seismological concepts to the setting of worlds with global oceans covered in ice. Here we use waveform analyses to identify and classify wave types, developing a lexicon for icy ocean world seismology intended to be useful to both seismologists and planetary scientists. We use results from spectral-element simulations of broadband seismic wavefields to adapt seismological concepts to icy ocean worlds. We present a concise naming scheme for seismic waves and an overview of the features of the seismic wavefield on Europa, Titan, Ganymede, and Enceladus. In close connection with geophysical interior models, we analyze simulated seismic measurements of Europa and Titan that might be used to constrain geochemical parameters governing the habitability of a sub-ice ocean.

  5. Elastic parabolic equation solutions for oceanic T-wave generation and propagation from deep seismic sources.

    PubMed

    Frank, Scott D; Collis, Jon M; Odom, Robert I

    2015-06-01

    Oceanic T-waves are earthquake signals that originate when elastic waves interact with the fluid-elastic interface at the ocean bottom and are converted to acoustic waves in the ocean. These waves propagate long distances in the Sound Fixing and Ranging (SOFAR) channel and tend to be the largest observed arrivals from seismic events. Thus, an understanding of their generation is important for event detection, localization, and source-type discrimination. Recently benchmarked seismic self-starting fields are used to generate elastic parabolic equation solutions that demonstrate generation and propagation of oceanic T-waves in range-dependent underwater acoustic environments. Both downward sloping and abyssal ocean range-dependent environments are considered, and results demonstrate conversion of elastic waves into water-borne oceanic T-waves. Examples demonstrating long-range broadband T-wave propagation in range-dependent environments are shown. These results confirm that elastic parabolic equation solutions are valuable for characterization of the relationships between T-wave propagation and variations in range-dependent bathymetry or elastic material parameters, as well as for modeling T-wave receptions at hydrophone arrays or coastal receiving stations.

  6. Enhancing power generation of floating wave power generators by utilization of nonlinear roll-pitch coupling

    NASA Astrophysics Data System (ADS)

    Yerrapragada, Karthik; Ansari, M. H.; Karami, M. Amin

    2017-09-01

    We propose utilization of the nonlinear coupling between the roll and pitch motions of wave 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 waves. This significantly magnifies the motion of the vessel and thus improves the power production by several orders of magnitude. The ocean waves 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 coupled electro-mechanical system is modeled 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 coupled 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 waves. It is shown that the proposed method enhances the power output of the floating wave 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.

  7. Scattering of Acoustic Waves from Ocean Boundaries

    DTIC Science & Technology

    2013-09-30

    of predictive models that can account for the all of the physical processes and variability of acoustic propagation and scattering in ocean...collaboration with Dr. Nicholas Chotiros, particularly for theoretical development of bulk acoustic /sediment modeling and laser roughness measurements...G. Potty and J. Miller. Measurement and modeling of Scholte wave dispersion in coastal waters. In Proc. of Third Int. Conf. on Ocean Acoustics

  8. On the shape and likelihood of oceanic rogue waves.

    PubMed

    Benetazzo, Alvise; Ardhuin, Fabrice; Bergamasco, Filippo; Cavaleri, Luigi; Guimarães, Pedro Veras; Schwendeman, Michael; Sclavo, Mauro; Thomson, Jim; Torsello, Andrea

    2017-08-15

    We consider the observation and analysis of oceanic rogue waves collected within spatio-temporal (ST) records of 3D wave fields. This class of records, allowing a sea surface region to be retrieved, is appropriate for the observation of rogue waves, which come up as a random phenomenon that can occur at any time and location of the sea surface. To verify this aspect, we used three stereo wave imaging systems to gather ST records of the sea surface elevation, which were collected in different sea conditions. The wave with the ST maximum elevation (happening to be larger than the rogue threshold 1.25H s ) was then isolated within each record, along with its temporal profile. The rogue waves show similar profiles, in agreement with the theory of extreme wave groups. We analyze the rogue wave probability of occurrence, also in the context of ST extreme value distributions, and we conclude that rogue waves are more likely than previously reported; the key point is coming across them, in space as well as in time. The dependence of the rogue wave profile and likelihood on the sea state conditions is also investigated. Results may prove useful in predicting extreme wave occurrence probability and strength during oceanic storms.

  9. Wave effects on ocean-ice interaction in the marginal ice zone

    NASA Technical Reports Server (NTRS)

    Liu, Antony K.; Hakkinen, Sirpa; Peng, Chih Y.

    1993-01-01

    The effects of wave train on ice-ocean interaction in the marginal ice zone are studied through numerical modeling. A coupled two-dimensional ice-ocean model has been developed to include wave effects and wind stress for the predictions of ice edge dynamics. The sea ice model is coupled to the reduced-gravity ocean model through interfacial stresses. The main dynamic balance in the ice momentum is between water-ice stress, wind stress, and wave radiation stresses. By considering the exchange of momentum between waves and ice pack through radiation stress for decaying waves, a parametric study of the effects of wave stress and wind stress on ice edge dynamics has been performed. The numerical results show significant effects from wave action. The ice edge is sharper, and ice edge meanders form in the marginal ice zone owing to forcing by wave action and refraction of swell system after a couple of days. Upwelling at the ice edge and eddy formation can be enhanced by the nonlinear effects of wave action; wave action sharpens the ice edge and can produce ice meandering, which enhances local Ekman pumping and pycnocline anomalies. The resulting ice concentration, pycnocline changes, and flow velocity field are shown to be consistent with previous observations.

  10. El Nino as an element of a global-scale wave in the atmosphere-ocean system

    NASA Astrophysics Data System (ADS)

    Serykh, Ilya; Sonechkin, Dmitry

    2016-04-01

    The analyses of the real meteorological and oceanographical data, and long runs of the coupled atmosphere-ocean hydro- thermodynamical models identify a spatial-temporal structure of the main mode of the interannual to decadal climatic variations. This mode looks like a global-scale wave that extends from West to East around the Earth, and varies rhythmically. In fact, the establishment of this wave is a generalization and development of the well-known structures of the so-called "teleconnections" in the ocean-atmosphere system. The known regional structures like ENSO, IOD, PDO, IPO, PNA, NAO, AO, ACW and other can be considered as parts of this global-scale wave. Moving eastward around the Earth, this wave triggers El Nino - Southern oscillation events. An index of this wave is proposed as a sum of normalized anomalies of the sea level pressure and the near-surface temperature in 20 locations around the globe. It is proven that the power spectrum of this index is not continuous but discrete in its character. Thus, one can suppose that the dynamics of the global-scale wave is nonchaotic, and so predictable with no limit in principle. The index power spectrum reveals statistically significant peaks at the same periods that are inherent to the power spectra of the traditional ENSO indices. The main peaks are at the sub-harmonics of the well-known Chandler wobble (of the ~1.2 year period) in the Earth's pole motion: 3.6; 4.8; 2.4 years. Some other statistically significant peaks also are seen at the super-harmonics of the Luni-Solar nutation (of the ~18.6 year period), and combinational harmonics of the Schwabe's and Hale's solar activity cycles. Based on the eastward propagation of the global-scale wave, a predictor of ENSO events was suggested. It has high correlation (about 0.7) with Nino indices but leads them on about 12 months. The use of this predictor opens a possibility to overcome the Spring Predictability Barrier in ENSO forecasting.

  11. New observations of Yanai waves and equatorial inertia-gravity waves in the Pacific Ocean

    NASA Astrophysics Data System (ADS)

    Farrar, J. T.; Durland, T.

    2011-12-01

    In the 1970's and 1980's, there was a great deal of research activity on near-equatorial variability at periods of days to weeks associated with oceanic equatorial inertia-gravity waves and Yanai waves. At that time, the measurements available for studying these waves were much more limited than today: most of the available observations were from island tide gauges and a handful of short mooring records. We use more than a decade of the extensive modern data record from the TAO/TRITON mooring array in the Pacific Ocean to re-examine the internal-wave climate in the equatorial Pacific, with a focus on interpretation of the zonal-wavenumber/frequency spectrum of surface dynamic height relative to 500-m depth. Many equatorial-wave meridional modes can be identified, for both the first and second baroclinic mode. We also estimated zonal-wavenumber/frequency spectra for the zonal and meridional wind stress components. The location and extent of spectral peaks in dynamic height is readily rationalized using basic, linear theory of forced equatorial waves and the observed wind stress spectrum.

  12. Two new ways of mapping sea ice thickness using ocean waves

    NASA Astrophysics Data System (ADS)

    Wadhams, P.

    2010-12-01

    TWO NEW METHODS OF MAPPING SEA ICE THICKNESS USING OCEAN WAVES. P. Wadhams (1,2), Martin Doble (1,2) and F. Parmiggiani (3) (1) Dept. of Applied Mathematics and Theoretical Physics, University of Cambridge, Cambridge CB3 0WA, UK. (2) Laboratoire d’Océanographie de Villefranche, Université Pierre et Marie Curie, 06234 Villefranche-sur-Mer, France (2) ISAC-CNR, Bologna, Italy Two new methods of mapping ice thickness have been recently developed and tested, both making use of the dispersion relation of ocean waves in ice of radically different types. In frazil-pancake ice, a young ice type in which cakes less than 5 m across float in a suspension of individual ice crystals, the propagation of waves has been successfully modelled by treating the ice layer as a highly viscous fluid. The model predicts a shortening of wavelengths within the ice. Two-dimensional Fourier analysis of successive SAR subscenes to track the directional spectrum of a wave field as it enters an ice edge shows that waves do indeed shorten within the ice, and the change has been successfully used to predict the thickness of the frazil-pancake layer. Concurrent shipborne sampling in the Antarctic has shown that the method is accurate, and we now propose its use throughout the important frazil-pancake regimes in the world ocean (Antarctic circumpolar ice edge zone, Greenland Sea, Bering Sea and others). A radically different type of dispersion occurs when ocean waves enter the continuous icefields of the central Arctic, when they couple with the elastic ice cover to propagate as a flexural-gravity wave. A two-axis tiltmeter array has been used to measure the resulting change in the dispersion relation for long ocean swell (15-30 s) originating from storms in the Greenland Sea. The dispersion relation is slightly different from swell in the open ocean, so if two such arrays are placed a substantial distance (100s of km) apart and used to observe the changing wave period of arrivals from a given

  13. Book review: Rogue waves in the ocean

    USGS Publications Warehouse

    Geist, Eric L.

    2011-01-01

    Review info: Rogue Waves in the Ocean. Advances in Geophysical and Environmental Mechanics and Mathematics. By Christian Kharif, Efim Pelinovsky and Alexey Slunyaev, 2009. ISBN: 978-3540884187, xiii, 216 pp.

  14. The Wave Glider°: A New Autonomous Surface Vehicle to Augment MBARI's Growing Fleet of Ocean Observing Systems

    NASA Astrophysics Data System (ADS)

    Tougher, B. B.

    2011-12-01

    Monterey Bay Aquarium Research Institute's (MBARI) evolving fleet of ocean observing systems has made it possible to collect information and data about a wide variety of ocean parameters, enabling researchers to better understand marine ecosystems. In collaboration with Liquid Robotics Inc, the designer of the Wave Glider autonomous surface vehicle (ASV), MBARI is adding a new capability to its suite of ocean observing tools. This new technology will augment MBARI research programs that use satellites, ships, moorings, drifters, autonomous underwater vehicles (AUVs) and remotely operated vehicles (ROVs) to improve data collection of temporally and spatially variable oceanographic features. The Wave Glider ASV derives its propulsion from wave energy, while sensors and communications are powered through the use of two solar panels and batteries, enabling it to remain at sea indefinitely. Wave Gliders are remotely controlled via real-time Iridium burst communications, which also permit real-time data telemetry. MBARI has developed Ocean Acidification (OA) moorings to continuously monitor the chemical and physical changes occurring in the ocean as a result of increased levels of atmospheric carbon dioxide (CO2). The moorings are spatially restricted by being anchored to the seafloor, so during the summer of 2011 the ocean acidification sensor suite designed for moorings was integrated into a Wave Glider ASV to increase both temporal and spatial ocean observation capabilities. The OA sensor package enables the measurement of parameters essential to better understanding the changing acidity of the ocean, specifically pCO2, pH, oxygen, salinity and temperature. The Wave Glider will also be equipped with a meteorological sensor suite that will measure air temperature, air pressure, and wind speed and direction. The OA sensor integration into a Wave Glider was part of MBARI's 2011 summer internship program. This project involved designing a new layout for the OA sensors

  15. Freak Waves In The Ocean A~é­ We Need Continuous Measurements!

    NASA Astrophysics Data System (ADS)

    Liu, P.; Teng, C.; Mori, N.

    Freak waves, sometimes also known as rogue waves, are a particular kind of ocean waves that displays a singular, unexpected, and unusually high wave profile with an extraordinarily large and steep trough or crest. The existence of freak waves has be- come widely accepted while it always poses severe hazard to the navy fleets, merchant marines, offshore structures, and virtually all oceanic ventures. Multitudes of seagoing vessels and mariners have encountered freak waves over the years, many had resulted in disasters. The emerging interest in freak waves and the quest to grasp an understand- ing of the phenomenon have inspired numerous theoretical conjectures in recent years. But the practical void of actual field observation on freak waves renders even the well- developed theories remain unverified. Furthermore, the present wave measurement systems, which have been in practice for the last 5 decades, are not at all designed to capture freak waves. We wish therefore to propose and petition to all oceanic scientist and engineers to consider undertaking an unprecedented but technologically feasible practice of making continuous and uninterrupted wave measurements. As freak waves can happen anywhere in the ocean and at anytime, the continuous and uninterrupted measurements at a fixed station would certainly be warranted to document the occur- rence of freak waves, if present, and thus lead to basic realizations of the underlying driving mechanisms.

  16. Predicting dangerous ocean waves with spaceborne synthetic aperture radar

    NASA Technical Reports Server (NTRS)

    Beal, R. C.

    1984-01-01

    It is pointed out that catastrophes, related to the occurrence of strong winds and large ocean waves, can consume more lives and property than most naval battles. The generation of waves by wind are considered, Pierson et al. (1955) have incorporated statistical concepts into a wave forecast model. The concept of an 'ocean wave spectrum' was introduced, with the wind acting independently on each Fourier component. However, even after 30 years of research and debate, the generation, propagation, and dissipation of the spectrum under arbitrary conditions continue to be controversial. It has now been found that spaceborne SAR has a surprising ability to precisely monitor spatially evolving wind and wave fields. Approaches to overcome certain weaknesses of the SAR method are discussed, taking into account the second Shuttle Imaging Radar experiment, and a possible long-term solution provided by Spectrasat. Spectrasat should be a low-altitude (200 to 250 km) satellite with active drag compensation.

  17. On the interaction between ocean surface waves and seamounts

    NASA Astrophysics Data System (ADS)

    Sosa, Jeison; Cavaleri, Luigi; Portilla-Yandún, Jesús

    2017-12-01

    Of the many topographic features, more specifically seamounts, that are ubiquitous in the ocean floor, we focus our attention on those with relatively shallow summits that can interact with wind-generated surface waves. Among these, especially relatively long waves crossing the oceans (swells) and stormy seas are able to affect the water column up to a considerable depth and therefore interact with these deep-sea features. We quantify this interaction through numerical experiments using a numerical wave model (SWAN), in which a simply shaped seamount is exposed to waves of different length. The results show a strong interaction that leads to significant changes in the wave field, creating wake zones and regions of large wave amplification. This is then exemplified in a practical case where we analyze the interaction of more realistic sea conditions with a very shallow rock in the Yellow Sea. Potentially important for navigation and erosion processes, mutatis mutandis, these results are also indicative of possible interactions with emerged islands and sand banks in shelf seas.

  18. Altimeter Observations of Wave Climate in the Arctic Ocean

    NASA Astrophysics Data System (ADS)

    Babanin, A. V.; Liu, Q.; Zieger, S.

    2016-02-01

    Wind waves are a new physical phenomenon to the Arctic Seas, which in the past were covered with ice. Now, over summer months, ice coverage retreats up to high latitudes and waves are generated. The marginal open seas provide new opportunities and new problems. Navigation and other maritime activities become possible, but wave heights, storm surges and coastal erosion will likely increase. Air-sea interactions enter a completely new regime, with momentum, energy, heat, gas and moisture fluxes being moderated or produced by the waves, and impacting on upper-ocean mixing. All these issues require knowledge of the wave climate. We will report results of investigation of wave climate and its trends by means of satellite altimetry. This is a challenging, but important topic. On one hand, no statistical approach is possible since in the past for most of the Arctic Ocean there was limited wave activity. Extrapolations of the current observations into the future are not feasible, because ice cover and wind patterns in the Arctic are changing. On the other hand, information on the mean and extreme wave properties, such as wave height, period, direction, on the frequency of occurrence and duration of the storms is of great importance for oceanographic, meteorological, climate, naval and maritime applications in the Arctic Seas.

  19. Impact of Ocean Surface Waves on Air-Sea Momentum Flux

    NASA Astrophysics Data System (ADS)

    Tamura, H.; Drennan, W. M.; Collins, C. O., III; Graber, H. C.

    2016-02-01

    In this study, we investigated the structure of turbulent air flow over ocean waves. Observations of wind and waves were retrieved by air-sea interaction spar (ASIS) buoys during the shoaling waves experiment (SHOWEX) in Duck, NC in 1999. It is shown that the turbulent velocity spectra and co-spectra for pure wind sea conditions follow the universal forms estimated by Miyake et al [1970]. In the presence of strong swells, the wave boundary layer was extended and the universal spectral scaling of u'w' broke down [Drennan et al, 1999]. On the other hand, the use of the peak wave frequency (fp) to reproduce the "universal spectra" succeeded at explaining the spectral structure of turbulent flow field. The u'w' co-spectra become negative near the fp, which suggests the upward momentum transport (i.e., negative wind stress) induced by ocean waves. Finally, we propose three turbulent flow structures for different wind-wave regimes.

  20. Teleseismic P wave coda from oceanic trench and other bathymetric features

    NASA Astrophysics Data System (ADS)

    Wu, W.; Ni, S.

    2012-12-01

    Teleseismic P waves are essential for studying rupture processes of great earthquakes, either in the back projection method or in finite fault inversion method involving of quantitative waveform modeling. In these studies, P waves are assumed to be direct P waves generated by localized patches of the ruptured fault. However, for some oceanic earthquakes happening near the subductiontrenches or mid-ocean ridges, we observed strong signals between P and PP are often observed on theat telseseismic networkdistances. These P wave coda signals show strong coherence and their amplitudes are sometimes comparable with those of the direct P wave or even higher for some special frequenciesfrequency band. With array analysis, we find that the coda's slowness is very close to that of the direct P wave, suggesting that they are generated near the source region. As the earthquakes occur near the trenches or mid-ocean ridges which are both featured by rapid variation of bathymetry, the coda waves are very probably generated by the scattered surface wave or S wave at the irregular bathymetry. Then, we apply the realistic bathymetry data to calculate the 3D synthetics and the coda can be well predicted by the synthetics. So the topography/bathymetry is confirmed to be the main source of the coda. The coda waves are so strong that it may affect the imaging rupture processes of ocean earthquakes, so the topography/bathymetry effect should be taken into account. However, these strong coda waves can also be used utilized to locate the oceanic earthquakes. The 3D synthetics demonstrate that the coda waves are dependent on both the specific bathymetry and the location of the earthquake. Given the determined bathymetry, the earthquake location can be constrained by the coda, e.g. the distance between trench and the earthquake can be determine from the relative arrival between the P wave and its coda which is generated by the trench. In order to locate the earthquakes using the bathymetry

  1. Simulating Freak Waves in the Ocean with CFD Modeling

    NASA Astrophysics Data System (ADS)

    Manolidis, M.; Orzech, M.; Simeonov, J.

    2017-12-01

    Rogue, or freak, waves 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 wave formation. In our work we numerically simulate the formation of such waves 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 wave phenomena, such as soliton propagation and wave shoaling. We conducted a range of tests simulating rogue wave formation and horizontally varying currents to evaluate and compare the capabilities of the two software packages. Then we used each model to investigate the effect of ocean currents and current gradients on the formation of rogue waves. We present preliminary results.

  2. 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.

  3. Studying Nearshore Ocean Waves Using X-Band Radar

    NASA Astrophysics Data System (ADS)

    Laughlin, B.; Bland, R. W.

    2014-12-01

    In January of 2010, ocean waves generated by an unusually large storm caused major erosion damage to the San Francisco coastline, with an erosion "hot spot" partially collapsing a four-lane throughway and threatening important infrastructure. Every winter, swells from the northwest approach San Francisco's Ocean Beach by passing over the southern limb of the San Francisco Bar, an ebb-tidal delta seaward of the Golden Gate Bridge. Refraction of approaching wave-fronts causes focusing of wave energy at the southern end of Ocean Beach where the S.F. Bar meets the coast, possibly explaining the location of the 2010 hot spot. In 2011 an x-band radar system was installed on a site near the erosion hot spot, at an elevation of 13 m above low tide, about 40 m back from the high-tide line. The radar system collects images of wave crests out to 3 km from the scanner. Study of these images when offshore buoys report a single NW swell shows two swell patterns arriving at Ocean Beach, separated in direction by about 30 degrees, and producing a quilted interference pattern, as seen in the accompanying figure. We interpret these swells as following two different paths around the Bar. Preliminary ray-tracing studies tend to confirm this interpretation. To enhance these images we have employed two techniques. The first technique, which is concerned with identification and visualization of swells in the region of interest, involves iteration over possible swell periods: scans taken at integral multiples of a given period are added together, with the sharpest image determining the swell period (see figure) and providing an enhanced image for further analysis. The second technique involves displacement of images in time by phase incrementation in k-space, with subsequent addition of images. We will present results concerning the stability of the relative phase of the two swells, and the applicability to models for propagation of waves. Establishment of a tested propagation model would

  4. Near-Inertial Internal Gravity Waves in the Ocean.

    PubMed

    Alford, Matthew H; MacKinnon, Jennifer A; Simmons, Harper L; Nash, Jonathan D

    2016-01-01

    We review the physics of near-inertial waves (NIWs) in the ocean and the observations, theory, and models that have provided our present knowledge. NIWs appear nearly everywhere in the ocean as a spectral peak at and just above the local inertial period f, and the longest vertical wavelengths can propagate at least hundreds of kilometers toward the equator from their source regions; shorter vertical wavelengths do not travel as far and do not contain as much energy, but lead to turbulent mixing owing to their high shear. NIWs are generated by a variety of mechanisms, including the wind, nonlinear interactions with waves of other frequencies, lee waves over bottom topography, and geostrophic adjustment; the partition among these is not known, although the wind is likely the most important. NIWs likely interact strongly with mesoscale and submesoscale motions, in ways that are just beginning to be understood.

  5. CMIP5-based global wave climate projections including the entire Arctic Ocean

    NASA Astrophysics Data System (ADS)

    Casas-Prat, M.; Wang, X. L.; Swart, N.

    2018-03-01

    This study presents simulations of the global ocean wave climate corresponding to the surface winds and sea ice concentrations as simulated by five CMIP5 (Coupled Model Intercomparison Project Phase 5) climate models for the historical (1979-2005) and RCP8.5 scenario future (2081-2100) periods. To tackle the numerical complexities associated with the inclusion of the North Pole, the WAVEWATCH III (WW3) wave model was used with a customized unstructured Spherical Multi-Cell grid of ∼100 km offshore and ∼50 km along coastlines. The climate model simulated wind and sea ice data, and the corresponding WW3 simulated wave data, were evaluated against reanalysis and hindcast data. The results show that all the five sets of wave simulations projected lower waves in the North Atlantic, corresponding to decreased surface wind speeds there in the warmer climate. The selected CMIP5 models also consistently projected an increase in the surface wind speed in the Southern Hemisphere (SH) mid-high latitudes, which translates in an increase in the WW3 simulated significant wave height (Hs) there. The higher waves are accompanied with increased peak wave period and increased wave age in the East Pacific and Indian Oceans, and a significant counterclockwise rotation in the mean wave direction in the Southern Oceans. The latter is caused by more intense waves from the SH traveling equatorward and developing into swells. Future wave climate in the Arctic Ocean in summer is projected to be predominantly of mixed sea states, with the climatological mean of September maximum Hs ranging mostly 3-4 m. The new waves approaching Arctic coasts will be less fetch-limited as ice retreats since a predominantly southwards mean wave direction is projected in the surrounding seas.

  6. Ocean Wave Energy Estimation Using Active Satellite Imagery as a Solution of Energy Scarce in Indonesia Case Study: Poteran Island's Water, Madura

    NASA Astrophysics Data System (ADS)

    Nadzir, Z. A.; Karondia, L. A.; Jaelani, L. M.; Sulaiman, A.; Pamungkas, A.; Koenhardono, E. S.; Sulisetyono, A.

    2015-10-01

    Ocean wave energy is one of the ORE (Ocean Renewable Energies) sources, which potential, in which this energy has several advantages over fossil energy and being one of the most researched energy in developed countries nowadays. One of the efforts for mapping ORE potential is by computing energy potential generated from ocean wave, symbolized by Watt per area unit using various methods of observation. SAR (Synthetic Aperture Radar) is one of the hyped and most developed Remote Sensing method used to monitor and map the ocean wave energy potential effectively and fast. SAR imagery processing can be accomplished not only in remote sensing data applications, but using Matrices processing application as well such as MATLAB that utilizing Fast Fourier Transform and Band-Pass Filtering methods undergoing Pre-Processing stage. In this research, the processing and energy estimation from ALOSPALSAR satellite imagery acquired on the 5/12/2009 was accomplished using 2 methods (i.e Magnitude and Wavelength). This resulted in 9 potential locations of ocean wave energy between 0-228 W/m2, and 7 potential locations with ranged value between 182-1317 W/m2. After getting through buffering process with value of 2 km (to facilitate the construction of power plant installation), 9 sites of location were estimated to be the most potential location of ocean wave energy generation in the ocean with average depth of 8.058 m and annual wind speed of 6.553 knot.

  7. The Cooling Oceanic Lithosphere as Constrained by Surface Wave Dispersion Data

    NASA Astrophysics Data System (ADS)

    Hogg, C.; Laske, G.

    2003-12-01

    The tremendous improvement in resolution capabilities of global surface wave phase velocity maps now encourage us to search for anomalies that are caused by mantle plumes. On the other hand, the implications of even large--scale anomalies in such maps are still not well understood. One such anomaly is caused by the cooling oceanic lithosphere. Some studies investigate the cooling effects by fitting thermal models to the 3--dimensional mantle models resulting from tomographic inversions. The inversion of surface wave data for structure at depth is nonunique and the model often depends on the techniques applied. We prefer to compare the dispersion data directly with predictions from thermal models. Simple cooling models produce a signal that is roughly proportional to the square root of age. This signal is typically much smaller than the one caused by other lateral heterogeneity within the Earth's crust and upper mantle. In a careful analysis we are able to extract clear, roughly linear trends, in all major oceans. We explore the parameter space by fitting cooling half space as well as cooling plate models to the data. In the Pacific ocean, our data are inconsistent with standard parameters that are used to fit the observed bathymetry, and perhaps surface heat flux data. Instead of an initial temperature of 1350~deg C in the cooling half space model our data require a lower temperature (around 1200~deg C) to be well fit, especially the Love wave data. Regarding the cooling plate model, our data seem to require a thicker lithosphere to be well fit (135~km instead of the 'standard' 100 ~m). We observe similar trends for the other oceans investigated: the Indian ocean, the South and the North Atlantic oceans. For the Indian ocean in particular, a crust correction (removing the predictions caused by crustal structure including water depth and sediment thickness) is crucial to obtain an internally consistent dataset. For the Atlantic ocean, a large signal remains

  8. Measuring ocean waves from space; Proceedings of the Symposium, Johns Hopkins University, Laurel, MD, Apr. 15-17, 1986

    NASA Technical Reports Server (NTRS)

    Beal, Robert C. (Editor)

    1987-01-01

    Papers are presented on ocean-wave prediction; the quasi-universal form of the spectra of wind-generated gravity waves at different stages of their development; the limitations of the spectral measurements and observations of the group structure of surface waves; the effect of swell on the growth of wind wave; operational wave forecasting; ocean-wave models, and seakeeping using directional wave spectra. Consideration is given to microwave measurements of the ocean-wave directional spectra; SIR research; estimating wave energy spectra from SAR imagery, with the radar ocean-wave spectrometer, and SIR-B; the wave-measurement capabilities of the surface contour radar and the airborne oceanographic lidar; and SIR-B ocean-wave enhancement with fast-Fourier transform techniques. Topics discussed include wave-current interaction; the design and applicability of Spectrasat; the need for a global wave monitoring system; the age and source of ocean swell observed in Hurricane Josephine; and the use of satellite technology for insulin treatment.

  9. Hurricane Directional Wave Spectrum Spatial Variation in the Open Ocean and at Landfall

    NASA Technical Reports Server (NTRS)

    Walsh, E. J.; Wright, C. W.; Vandemark, D.; Krabill, W. B.; Garcia, A. W.; Houston, S. H.; Powell, M. D.; Black, P. G.; Marks, F. D.; Busalacchi, Antonio J. (Technical Monitor)

    2000-01-01

    The sea surface directional wave spectrum was measured for the first time in all quadrants of a hurricane in open water using the NASA airborne scanning radar altimeter (SRA) carried aboard one of the NOAA WP-3D hurricane hunter aircraft at 1.5 km height. The SRA measures the energetic portion of the directional wave spectrum by generating a topographic map of the sea surface. At 8 Hz, the SRA sweeps a radar beam of 1 E half-power width (two-way) across the aircraft ground track over a swath equal to 0.8 of the aircraft height, simultaneously measuring the backscattered power at its 36 GHz (8.3 mm) operating frequency and the range to the sea surface at 64 positions. These slant ranges are multiplied by the cosine of the incidence angles to determine the vertical distances from the aircraft to the sea surface. Subtracting these distances from the aircraft height produces the sea surface elevation map. The sea surface topography is interpolated to a uniform grid, transformed by a two-dimensional FFT, and Doppler corrected. The open-ocean data were acquired on 24 August 1998 when hurricane Bonnie was east of the Bahamas and moving slowly to the north. Individual waves with heights up to 18 m were observed and the spatial variation of the wave field was dramatic. The dominant waves generally propagated at significant angles to the downwind direction. At some positions there were three different wave fields of comparable energy crossing each other. The NOAA aircraft spent over five hours within 180 km of the hurricane Bonnie eye, and made five eye penetrations. A 3-minute animation of the directional wave spectrum spatial variation over this period will be shown as well as summary plots of the wave field spatial variation. On 26 August 1998, the NOAA aircraft flew at 2.2 km height when hurricane Bonnie was making landfall near Wilmington, NC, documenting the directional wave spectrum in the region between Charleston, SC and Cape Hatteras, NC. The aircraft ground track

  10. Partitioning Ocean Wave Spectra Obtained from Radar Observations

    NASA Astrophysics Data System (ADS)

    Delaye, Lauriane; Vergely, Jean-Luc; Hauser, Daniele; Guitton, Gilles; Mouche, Alexis; Tison, Celine

    2016-08-01

    2D wave spectra of ocean waves can be partitioned into several wave components to better characterize the scene. We present here two methods of component detection: one based on watershed algorithm and the other based on a Bayesian approach. We tested both methods on a set of simulated SWIM data, the Ku-band real aperture radar embarked on the CFOSAT (China- France Oceanography Satellite) mission which launch is planned mid-2018. We present the results and the limits of both approaches and show that Bayesian method can also be applied to other kind of wave spectra observations as those obtained with the radar KuROS, an airborne radar wave spectrometer.

  11. The damping of ocean surface waves by a monomolecular film measured by wave staffs and microwave radars

    NASA Technical Reports Server (NTRS)

    Huehnerfuss, H.; Alpers, W.; Jones, W. L.; Lange, P. A.; Richter, K.

    1981-01-01

    Open ocean and wave tank experiments were carried out with the aim of studying the damping of capillary and gravity waves by a monomolecular film. These films of biogenic origin influence air-sea interaction processes and thereby affect the use of remote sensing techniques in oceanography. Measurement was carried out by wave staffs, by a coherent X band microwave scatterometer mounted on a sea-based platform, and by an incoherent K band microwave scatterometer carried by an aircraft under moderate wind conditions. A wave attenuation of about 40-60% is observed in the frequency range between 3.2 and 16 Hz. Tank experiments show that a direct influence of oleyl alcohol surface films on wave damping is confined to frequencies equal to or greater than 2 Hz; a further indirect effect of films on the damping of ocean waves in the frequency range between 0.12 and 0.7 Hz (by modifying the wind input and wave-wave interaction mechanisms) is also indicated

  12. Electrokinetic Transduction of Acoustic Waves In Ocean Sediments

    DTIC Science & Technology

    2002-09-30

    acoustic —motion in ocean sediments. The Biot theory of poroelastic media captures much of the sediment physics left out by other models [2]. It fits...in subsurface acoustical imaging, Mine Counter- Measures, and Anti-Submarine Warfare. To obtain essential experimental data to support the modeling ...Electrokinetic Transduction of Acoustic Waves In Ocean Sediments Gareth I. Block Applied Research Laboratories, U.T. Austin P.O. Box 8029

  13. Listening to sounds from an exploding meteor and oceanic waves

    NASA Astrophysics Data System (ADS)

    Evers, L. G.; Haak, H. W.

    Low frequency sound (infrasound) measurements have been selected within the Comprehensive Nuclear-Test-Ban Treaty (CTBT) as a technique to detect and identify possible nuclear explosions. The Seismology Division of the Royal Netherlands Meteorological Institute (KNMI) operates since 1999 an experimental infrasound array of 16 micro-barometers. Here we show the rare detection and identification of an exploding meteor above Northern Germany on November 8th, 1999 with data from the Deelen Infrasound Array (DIA). At the same time, sound was radiated from the Atlantic Ocean, South of Iceland, due to the atmospheric coupling of standing ocean waves, called microbaroms. Occurring with only 0.04 Hz difference in dominant frequency, DIA proved to be able to discriminate between the physically different sources of infrasound through its unique lay-out and instruments. The explosive power of the meteor being 1.5 kT TNT is in the range of nuclear explosions and therefore relevant to the CTBT.

  14. Open ocean Internal Waves, Namibia Coast, Africa.

    NASA Technical Reports Server (NTRS)

    1990-01-01

    These open ocean Internal Waves were seen off the Namibia Coast, Africa (19.5S, 11.5E). The periodic and regularly spaced sets of incoming internal appear to be diffracting against the coastline and recombining to form a network of interference patterns. They seem to coincide with tidal periods about 12 hours apart and wave length (distance from crest to crest) varies between 1.5 and 5.0 miles and the crest lengths stretch beyond the image.

  15. Open ocean Internal Waves, Namibia Coast, Africa.

    NASA Image and Video Library

    1990-12-10

    These open ocean Internal Waves were seen off the Namibia Coast, Africa (19.5S, 11.5E). The periodic and regularly spaced sets of incoming internal appear to be diffracting against the coastline and recombining to form a network of interference patterns. They seem to coincide with tidal periods about 12 hours apart and wave length (distance from crest to crest) varies between 1.5 and 5.0 miles and the crest lengths stretch beyond the image.

  16. 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.

  17. Short wind waves on the ocean: Wavenumber-frequency spectra

    NASA Astrophysics Data System (ADS)

    Plant, William J.

    2015-03-01

    Dominant surface waves on the ocean exhibit a dispersion relation that confines their energy to a curve in a wavenumber-frequency spectrum. Short wind waves on the ocean, on the other hand, are advected by these dominant waves so that they do not exhibit a well-defined dispersion relation over many realizations of the surface. Here we show that the short-wave analog to the dispersion relation is a distributed spectrum in the wavenumber-frequency plane that collapses to the standard dispersion relation in the absence of long waves. We compute probability distributions of short-wave wavenumber given a (frequency, direction) pair and of short-wave frequency given a (wavenumber, direction) pair. These two probability distributions must yield a single spectrum of surface displacements as a function of wavenumber and frequency, F(k,f). We show that the folded, azimuthally averaged version of this spectrum has a "butterfly" pattern in the wavenumber-frequency plane if significant long waves are present. Integration of this spectrum over frequency yields the well-known k-3 wavenumber spectrum. When integrated over wavenumber, the spectrum yields an f-4 form that agrees with measurement. We also show that a cut through the unfolded F(k,f) at constant k produces the well-known form of moderate-incidence-angle Doppler spectra for electromagnetic scattering from the sea. This development points out the dependence of the short-wave spectrum on the amplitude of the long waves.

  18. Two-component wind fields over ocean waves using atmospheric lidar and motion estimation algorithms

    NASA Astrophysics Data System (ADS)

    Mayor, S. D.

    2016-02-01

    Numerical models, such as large eddy simulations, are capable of providing stunning visualizations of the air-sea interface. One reason for this is the inherent spatial nature of such models. As compute power grows, models are able to provide higher resolution visualizations over larger domains revealing intricate details of the interactions of ocean waves and the airflow over them. Spatial observations on the other hand, which are necessary to validate the simulations, appear to lag behind models. The rough ocean environment of the real world is an additional challenge. One method of providing spatial observations of fluid flow is that of particle image velocimetry (PIV). PIV has been successfully applied to many problems in engineering and the geosciences. This presentation will show recent research results that demonstate that a PIV-style approach using pulsed-fiber atmospheric elastic backscatter lidar hardware and wavelet-based optical flow motion estimation software can reveal two-component wind fields over rough ocean surfaces. Namely, a recently-developed compact lidar was deployed for 10 days in March of 2015 in the Eureka, California area. It scanned over the ocean. Imagery reveal that breaking ocean waves provide copius amounts of particulate matter for the lidar to detect and for the motion estimation algorithms to retrieve wind vectors from. The image below shows two examples of results from the experiment. The left panel shows the elastic backscatter intensity (copper shades) under a field of vectors that was retrieved by the wavelet-based optical flow algorithm from two scans that took about 15 s each to acquire. The vectors, that reveal offshore flow toward the NW, were decimated for clarity. The bright aerosol features along the right edge of the sector scan were caused by ocean waves breaking on the beach. The right panel is the result of scanning over the ocean on a day when wave amplitudes ranged from 8-12 feet and whitecaps offshore beyond the

  19. 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

  20. Observed ocean waves by tropical cyclones

    NASA Astrophysics Data System (ADS)

    Zhang, Lin; Oey, Leo

    2017-04-01

    Ocean waves produced by tropical cyclones (TC) modify air-sea fluxes which in turn are crucial to the storms' intensity and development, yet they are poorly understood. Here we use 24 years (1992-2015) of observed waves, winds and TC-track information to stratify storm-centered composite maps of waves and winds according to TC intensities and translation speeds (Uh). While the wind field is rightward-asymmetric independent of Uh, the wave field is rightward-symmetric in concert with the wind for slow-translating TCs (Uh ≤ 3 m s-1), but right-rear asymmetric with strongest waves in the 4th quadrant for medium to fast-translating TCs (3 < Uh ≤ 7 m s-1), especially for the very fast storms (Uh > 7 m s-1), all independent of TC-intensity. The dominance of the right-rear asymmetry for fast-translating TCs appears to be related to the development of cross swells as the storms move faster, but further research using models are needed to understand the physical mechanisms.

  1. Directional measurement of short ocean waves with stereophotography

    NASA Technical Reports Server (NTRS)

    Shemdin, Omar H.; Tran, H. Minh; Wu, S. C.

    1988-01-01

    Stereophotographs of the sea surface, acquired during the Tower Ocean Wave and Radar Dependence experiment are analyzed to yield directional wave height spectra of short surface waves in the 6-80-cm range. The omnidirectional wave height spectra are found to deviate from the k exp -4 distribution, where k is the wave number. The stereo data processing errors are found to be within + or - 5 percent. The omnidirectional spectra yield 514 deg of freedom for 30-cm-long waves. The directional distribution of short waves is processed with a directional resolution of 30 deg, so as to yield 72 deg of freedom for 30-cm-long waves. The directional distributions show peaks that are aligned with the wind and swell directions. It is found that dynamically relevant measurements can be obtained with stereophotography, after removal of the mean surface associated with long waves.

  2. The Global Signature of Ocean Wave Spectra

    NASA Astrophysics Data System (ADS)

    Portilla-Yandún, Jesús

    2018-01-01

    A global atlas of ocean wave spectra is developed and presented. The development is based on a new technique for deriving wave spectral statistics, which is applied to the extensive ERA-Interim database from European Centre of Medium-Range Weather Forecasts. Spectral statistics is based on the idea of long-term wave systems, which are unique and distinct at every geographical point. The identification of those wave systems allows their separation from the overall spectrum using the partition technique. Their further characterization is made using standard integrated parameters, which turn out much more meaningful when applied to the individual components than to the total spectrum. The parameters developed include the density distribution of spectral partitions, which is the main descriptor; the identified wave systems; the individual distribution of the characteristic frequencies, directions, wave height, wave age, seasonal variability of wind and waves; return periods derived from extreme value analysis; and crossing-sea probabilities. This information is made available in web format for public use at http://www.modemat.epn.edu.ec/#/nereo. It is found that wave spectral statistics offers the possibility to synthesize data while providing a direct and comprehensive view of the local and regional wave conditions.

  3. The Occurrence of Tidal Hybrid Kelvin-Edge Waves in the Global Ocean

    NASA Astrophysics Data System (ADS)

    Kaur, H.; Buijsman, M. C.; Yankovsky, A. E.; Zhang, T.; Jeon, C. H.

    2017-12-01

    This study presents the analysis of hybrid Kelvin-edge waves on the continental shelves in a global ocean model. Our objective is to find areas where the transition occurs from Kelvin waves to hybrid Kelvin-edge waves. The change in continental shelf width may convert a Kelvin wave into a hybrid Kelvin-edge wave. In this process the group velocity reaches a minimum and tidal energy is radiated on and/or offshore [Zhang 2016]. We extract M2 SSH (Sea Surface Height) and velocity from the Hybrid Coordinate Ocean Model (HYCOM) and calculate barotropic energy fluxes. We analyze these three areas: the Bay of Biscay, the Amazon Shelf and North West Africa. In these three regions, the continental shelf widens in the propagation direction and the alongshore flux changes its direction towards the coast. A transect is taken at different points in these areas to compute the dispersion relations of the waves on the continental shelf. In model simulations, we change the bathymetry of the Bay of Biscay to study the behavior of the hybrid Kelvin-edge waves. BibliographyZhang, T., and A. E Yankovsky. (2016), On the nature of cross-isobath energy fluxes in topographically modified barotropic semidiurnal Kelvin waves, J. Geophys. Res. Oceans, 121, 3058-3074, doi:10.1002/2015JC011617.

  4. 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

  5. Variational stereo imaging of oceanic waves with statistical constraints.

    PubMed

    Gallego, Guillermo; Yezzi, Anthony; Fedele, Francesco; Benetazzo, Alvise

    2013-11-01

    An image processing observational technique for the stereoscopic reconstruction of the waveform of oceanic sea states is developed. The technique incorporates the enforcement of any given statistical wave law modeling the quasi-Gaussianity of oceanic waves observed in nature. The problem is posed in a variational optimization framework, where the desired waveform is obtained as the minimizer of a cost functional that combines image observations, smoothness priors and a weak statistical constraint. The minimizer is obtained by combining gradient descent and multigrid methods on the necessary optimality equations of the cost functional. Robust photometric error criteria and a spatial intensity compensation model are also developed to improve the performance of the presented image matching strategy. The weak statistical constraint is thoroughly evaluated in combination with other elements presented to reconstruct and enforce constraints on experimental stereo data, demonstrating the improvement in the estimation of the observed ocean surface.

  6. Impacts of climate changes on ocean surface gravity waves over the eastern Canadian shelf

    NASA Astrophysics Data System (ADS)

    Guo, Lanli; Sheng, Jinyu

    2017-05-01

    A numerical study is conducted to investigate the impact of climate changes on ocean surface gravity waves over the eastern Canadian shelf (ECS). The "business-as-usual" climate scenario known as Representative Concentration Pathway RCP8.5 is considered in this study. Changes in the ocean surface gravity waves over the study region for the period 1979-2100 are examined based on 3 hourly ocean waves simulated by the third-generation ocean wave model known as WAVEWATCHIII. The wave model is driven by surface winds and ice conditions produced by the Canadian Regional Climate Model (CanRCM4). The whole study period is divided into the present (1979-2008), near future (2021-2050) and far future (2071-2100) periods to quantify possible future changes of ocean waves over the ECS. In comparison with the present ocean wave conditions, the time-mean significant wave heights ( H s ) are expected to increase over most of the ECS in the near future and decrease over this region in the far future period. The time-means of the annual 5% largest H s are projected to increase over the ECS in both near and far future periods due mainly to the changes in surface winds. The future changes in the time-means of the annual 5% largest H s and 10-m wind speeds are projected to be twice as strong as the changes in annual means. An analysis of inverse wave ages suggests that the occurrence of wind seas is projected to increase over the southern Labrador and central Newfoundland Shelves in the near future period, and occurrence of swells is projected to increase over other areas of the ECS in both the near and far future periods.

  7. 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).

  8. Observations of Sea Surface Mean Square Slope During the Southern Ocean Waves Experiment

    NASA Technical Reports Server (NTRS)

    Walsh, E. J.; Vandemark, D. C.; Hines, D. E.; Banner, M. L.; Chen, W.; Swift, R. N.; Scott, J. F.; Jensen, J.; Lee, S.; Fandry, C.

    1999-01-01

    For the Southern Ocean Waves Experiment (SOWEX), conducted in June 1992 out of Hobart, Tasmania, the 36 GHz (8.3 mm) NASA Scanning Radar Altimeter (SRA) was shipped to Australia and installed on a CSIRO Fokker F-27 research aircraft instrumented to make comprehensive surface layer measurements of air-sea interaction fluxes. The sea surface mean square slope (mss), which is predominantly caused by the short waves, was determined from the backscattered power falloff with incidence angle measured by the SRA in the plane normal to the aircraft heading. On each flight, data were acquired at 240 m altitude while the aircraft was in a 7 deg roll attitude, interrogating off-nadir incidence angles from -15 deg through nadir to +29 deg. The aircraft turned azimuthally through 810 deg in this attitude, mapping the azimuthal dependence of the backscattered power falloff with incidence angle. Two sets of turning data were acquired on each day, before and after the aircraft measured wind stress at low altitude (12 m to 65 m). Wave topography and backscattered power for mss were also acquired during those level flight segments whenever the aircraft altitude was above the SRA minimum range of 35 m. A unique feature of this experiment was the use of a nadir-directed low-gain horn antenna (35 deg beamwidth) to acquire azimuthally integrated backscattered power data versus incidence angle before and after the turn data.

  9. 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.

  10. 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 currents 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 models for currents 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 <span class="hlt">Ocean</span> 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://www.dtic.mil/docs/citations/ADA608731','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA608731"><span>The US Navy Coupled <span class="hlt">Ocean-Wave</span> Prediction System</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2014-09-01</p> <p>Stokes drift to be the dominant <span class="hlt">wave</span> effect and that it increased surface drift speeds by 35% and veered the current in the direction of the wind...<span class="hlt">ocean</span> model has been modified to incorporate the effect of the Stokes drift current, <span class="hlt">wave</span> 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</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20020022887&hterms=square&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dsquare','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20020022887&hterms=square&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dsquare"><span>Observations of Sea Surface Mean Square Slope During the Southern <span class="hlt">Ocean</span> <span class="hlt">Waves</span> Experiment</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Walsh, E. J.; Vandemark, D. C.; Wright, C. W.; Banner, M. L.; Chen, W.; Swift, R. N.; Scott, J. F.; Hines, D. E.; Jensen, J.; Lee, S.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20020022887'); toggleEditAbsImage('author_20020022887_show'); toggleEditAbsImage('author_20020022887_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20020022887_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20020022887_hide"></p> <p>2001-01-01</p> <p>For the Southern <span class="hlt">Ocean</span> <span class="hlt">Waves</span> Experiment (SOWEX), conducted in June 1992 out of Hobart, Tasmania, the NASA Scanning Radar Altimeter (SRA) was shipped to Australia and installed on a CSIRO Fokker F-27 research aircraft instrumented to make comprehensive surface layer measurements of air-sea interaction fluxes. The SRA sweeps a radar beam of P (two-way) half-<span class="hlt">power</span> width across the aircraft ground track over a swath equal to 0.8 of the aircraft height, simultaneously measuring the backscattered <span class="hlt">power</span> at its 36 GHz (8.3 mm) operating frequency and the range to the sea surface at 64 cross-track positions. In realtime, the slant ranges are multiplied by the cosine of the off-nadir incidence angles (including the effect of aircraft roll attitude) to determine the vertical distances from the aircraft to the sea surface. These distances are subtracted from the aircraft height to produce a sea-surface elevation map, which is displayed on a monitor in the aircraft to enable real-time assessments of data quality and <span class="hlt">wave</span> properties. The sea surface mean square slope (mss), which is predominantly caused by the short <span class="hlt">waves</span>, was determined from the backscattered <span class="hlt">power</span> falloff with incidence angle measured by the SRA in the plane normal to the aircraft heading. On each flight, data were acquired at 240 m altitude while the aircraft was in a 7 degree roll attitude, interrogating off-nadir incidence angles from -15 degrees through nadir to +29 degrees. The aircraft turned azimuthally through 810 degrees in this attitude, mapping the azimuthal dependence of the backscattered <span class="hlt">power</span> falloff with incidence angle. Two sets of turning data were acquired on each day, before and after the aircraft measured wind stress at low altitude (12 meters to 65 meters). <span class="hlt">Wave</span> topography and backscattered <span class="hlt">power</span> for mss were also acquired during those level flight segments whenever the aircraft altitude was above the SRA minimum range of 35 m. Data were collected over a wide range of wind and sea</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ClDy...50.1533W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ClDy...50.1533W"><span>The response of the southwest Western Australian <span class="hlt">wave</span> climate to Indian <span class="hlt">Ocean</span> climate variability</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wandres, Moritz; Pattiaratchi, Charitha; Hetzel, Yasha; Wijeratne, E. M. S.</p> <p>2018-03-01</p> <p>Knowledge of regional <span class="hlt">wave</span> climates is critical for coastal planning, management, and protection. In order to develop a regional <span class="hlt">wave</span> climate, it is important to understand the atmospheric systems responsible for <span class="hlt">wave</span> generation. This study examines the variability of the southwest Western Australian (SWWA) shelf and nearshore wind <span class="hlt">wave</span> climate and its relationship to southern hemisphere climate variability represented by various atmospheric indices: the southern oscillation index (SOI), the Southern Annular Mode (SAM), the Indian <span class="hlt">Ocean</span> Dipole Mode Index (DMI), the Indian <span class="hlt">Ocean</span> Subtropical Dipole (IOSD), the latitudinal position of the subtropical high-pressure ridge (STRP), and the corresponding intensity of the subtropical ridge (STRI). A 21-year <span class="hlt">wave</span> hindcast (1994-2014) of the SWWA continental shelf was created using the third generation <span class="hlt">wave</span> model Simulating <span class="hlt">WAves</span> Nearshore (SWAN), to analyse the seasonal and inter-annual <span class="hlt">wave</span> climate variability and its relationship to the atmospheric regime. Strong relationships between <span class="hlt">wave</span> heights and the STRP and the STRI, a moderate correlation between the <span class="hlt">wave</span> climate and the SAM, and no significant correlation between SOI, DMI, and IOSD and the <span class="hlt">wave</span> climate were found. Strong spatial, seasonal, and inter-annual variability, as well as seasonal longer-term trends in the mean <span class="hlt">wave</span> climate were studied and linked to the latitudinal changes in the subtropical high-pressure ridge and the Southern <span class="hlt">Ocean</span> storm belt. As the Southern <span class="hlt">Ocean</span> storm belt and the subtropical high-pressure ridge shifted southward (northward) <span class="hlt">wave</span> heights on the SWWA shelf region decreased (increased). The <span class="hlt">wave</span> height anomalies appear to be driven by the same atmospheric conditions that influence rainfall variability in SWWA.</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 <span class="hlt">ocean</span> surface currents</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><span class="hlt">Ocean</span> surface currents estimated from the satellite data consist of two terms: Ekman currents from the wind stress and geostrophic currents from the sea surface height (SSH). But the classical Ekman model 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 <span class="hlt">ocean</span> surface currents is investigated and the <span class="hlt">wave</span>-modified currents are formed. The products are validated by comparing with OSCAR currents and Lagrangian drifter velocity. The result shows that our products with the Stokes drift are better adapted to the in situ Lagrangian drifter currents. Especially in the Southern <span class="hlt">Ocean</span> region (40°S-65°S), 90% (91%) of the zonal (meridional) currents have been improved compared with currents that do not include Stokes drift. The correlation (RMSE) in the Southern <span class="hlt">Ocean</span> 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 <span class="hlt">ocean</span> circulation, and need to be represented in numerical simulations of the global <span class="hlt">ocean</span> 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('https://ntrs.nasa.gov/search.jsp?R=19890035213&hterms=models+linear&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dmodels%2Blinear','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19890035213&hterms=models+linear&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dmodels%2Blinear"><span>Comparison of Shuttle Imaging Radar-B <span class="hlt">ocean</span> <span class="hlt">wave</span> image spectra with linear model predictions based on aircraft measurements</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Monaldo, Frank M.; Lyzenga, David R.</p> <p>1988-01-01</p> <p>During October 1984, coincident Shuttle Imaging Radar-B synthetic aperture radar (SAR) imagery and <span class="hlt">wave</span> measurements from airborne instrumentation were acquired. The two-dimensional <span class="hlt">wave</span> spectrum was measured by both a radar <span class="hlt">ocean-wave</span> spectrometer and a surface-contour radar aboard the aircraft. In this paper, two-dimensional SAR image intensity variance spectra are compared with these independent measures of <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra to verify previously proposed models of the relationship between such SAR image spectra and <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra. The results illustrate both the functional relationship between SAR image spectra and <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra and the limitations imposed on the imaging of short-wavelength, azimuth-traveling <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/824331','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/824331"><span><span class="hlt">Ocean</span> Current <span class="hlt">Power</span> Generator. Final Report</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>O'Sullivan, G. A.</p> <p>2002-07-26</p> <p>The <span class="hlt">Ocean</span> <span class="hlt">Power</span> Generator is both technically and economically suitable for deployment in the Gulf Stream from the US Navy facility in Dania, Florida. Yet to be completed is the calibration test in the Chesapeake Bay with the prototype dual hydroturbine Underwater Electric Kite. For the production units a revised design includes two ballast tanks mounted as pontoons to provide buoyancy and depth control. The <span class="hlt">power</span> rating of the <span class="hlt">Ocean</span> <span class="hlt">Power</span> Generator has been doubled to 200 kW ready for insertion into the utility grid. The projected cost for a 10 MW installation is $3.38 per watt, a cost thatmore » is consistent with wind <span class="hlt">power</span> pricing when it was in its deployment infancy, and a cost that is far better than photovoltaics after 25 years of research and development. The Gulf Stream flows 24 hours per day, and water flow is both environmentally and ecologically perfect as a renewable energy source. No real estate purchases are necessary, and you cannot see, hear, smell, or touch an <span class="hlt">Ocean</span> <span class="hlt">Power</span> Generator.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMOS21E1548O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMOS21E1548O"><span><span class="hlt">Ocean-Wave</span> Dynamics Analysis during Hurricane Ida and Norida Using a Fully Coupled Modeling System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Olabarrieta, M.; Warner, J. C.; Armstrong, B. N.</p> <p>2010-12-01</p> <p>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, <span class="hlt">waves</span>, 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 <span class="hlt">wave</span> 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, <span class="hlt">ocean</span> <span class="hlt">waves</span> and currents near the sea surface. In the present research we use the COAWST (Coupled <span class="hlt">Ocean-Atmosphere-Wave</span>-Sediment Transport) modeling system (Warner et al., 2010) to address the key role of the atmosphere-<span class="hlt">ocean-wave</span> 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 <span class="hlt">ocean</span> (ROMS model) and the <span class="hlt">wave</span> propagation and generation model (SWAN). Special attention is given to the role of the <span class="hlt">ocean</span> surface roughness and high resolution SST fields on the atmospheric boundary layers dynamics and consequently these effects on the wind <span class="hlt">wave</span> generation, surface currents and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMOS41C1737D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMOS41C1737D"><span>Towards a quantification of <span class="hlt">ocean</span> <span class="hlt">wave</span> heights off the west coast of Ireland using land based seismic data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Donne, S.; Bean, C. J.; Lokmer, I.; Lambkin, K.; Creamer, C.</p> <p>2012-12-01</p> <p><span class="hlt">Ocean</span> gravity <span class="hlt">waves</span> are driven by atmospheric pressure systems. Their interactions with one another and reflection off coastlines generate pressure changes at the sea floor. These pressure fluctuations are the cause of continuous background seismic noise known as microseisms. The levels of microseism activity vary as a function of the sea state and increase during periods of intensive <span class="hlt">ocean</span> <span class="hlt">wave</span> activity. In 2011 a seismic network was deployed along the west coast of Ireland to continuously record microseisms generated in the Atlantic <span class="hlt">Ocean</span>, as part of the <span class="hlt">Wave</span> Observation (<span class="hlt">Wave</span>Obs) project based in University College Dublin. This project aims to determine the characteristics of the causative <span class="hlt">ocean</span> gravity <span class="hlt">waves</span> through calibration of the microseism data with <span class="hlt">ocean</span> buoy data. In initial tests we are using a Backpropagation Feed-forward Artificial Neural Network (BP ANN) to establish the underlying relationships between microseisms and <span class="hlt">ocean</span> <span class="hlt">waves</span>. ANNs were originally inspired by studies of the mammalian brain and nervous system and are designed to learn by example. If successful these tools could then be used to estimate <span class="hlt">ocean</span> <span class="hlt">wave</span> heights and <span class="hlt">wave</span> periods using a land-based seismic network and complement current <span class="hlt">wave</span> observations being made offshore by marine buoys. Preliminary ANN results are promising with the network successfully able to reconstruct trends in <span class="hlt">ocean</span> <span class="hlt">wave</span> heights and periods. Microseisms can provide significant information about <span class="hlt">oceanic</span> processes. With a deeper understanding of how these processes work there is potential for 1) locating and tracking the evolution of the largest <span class="hlt">waves</span> in the Atlantic and 2) reconstructing the <span class="hlt">wave</span> climate off the west coast of Ireland using legacy seismic data on a longer time scale than is currently available using marine based observations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2012-08-20/pdf/2012-20348.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2012-08-20/pdf/2012-20348.pdf"><span>77 FR 50062 - Safety Zone; Embry-Riddle Wings and <span class="hlt">Waves</span>, Atlantic <span class="hlt">Ocean</span>; Daytona Beach, FL</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2012-08-20</p> <p>... 1625-AA00 Safety Zone; Embry-Riddle Wings and <span class="hlt">Waves</span>, Atlantic <span class="hlt">Ocean</span>; Daytona Beach, FL AGENCY: Coast...-Riddle Wings and <span class="hlt">Waves</span> air show. The event is scheduled to take place from Thursday, October 11, 2012...: Sec. 165.T07-0653 Safety Zone; Embry Riddle Wings and <span class="hlt">Waves</span>, Atlantic <span class="hlt">Ocean</span>, Daytona Beach, FL. (a...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4134826','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=4134826"><span>An Optimal Control Method for Maximizing the Efficiency of Direct Drive <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Energy Extraction System</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Chen, Zhongxian; Yu, Haitao; Wen, Cheng</p> <p>2014-01-01</p> <p>The goal of direct drive <span class="hlt">ocean</span> <span class="hlt">wave</span> energy extraction system is to convert <span class="hlt">ocean</span> <span class="hlt">wave</span> energy into electricity. The problem explored in this paper is the design and optimal control for the direct drive <span class="hlt">ocean</span> <span class="hlt">wave</span> energy extraction system. An optimal control method based on internal model proportion integration differentiation (IM-PID) is proposed in this paper though most of <span class="hlt">ocean</span> <span class="hlt">wave</span> energy extraction systems are optimized by the structure, weight, and material. With this control method, the heavy speed of outer heavy buoy of the energy extraction system is in resonance with incident <span class="hlt">wave</span>, and the system efficiency is largely improved. Validity of the proposed optimal control method is verified in both regular and irregular <span class="hlt">ocean</span> <span class="hlt">waves</span>, and it is shown that IM-PID control method is optimal in that it maximizes the energy conversion efficiency. In addition, the anti-interference ability of IM-PID control method has been assessed, and the results show that the IM-PID control method has good robustness, high precision, and strong anti-interference ability. PMID:25152913</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_5");'>5</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li class="active"><span>7</span></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_7 --> <div id="page_8" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="141"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25152913','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25152913"><span>An optimal control method for maximizing the efficiency of direct drive <span class="hlt">ocean</span> <span class="hlt">wave</span> energy extraction system.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Chen, Zhongxian; Yu, Haitao; Wen, Cheng</p> <p>2014-01-01</p> <p>The goal of direct drive <span class="hlt">ocean</span> <span class="hlt">wave</span> energy extraction system is to convert <span class="hlt">ocean</span> <span class="hlt">wave</span> energy into electricity. The problem explored in this paper is the design and optimal control for the direct drive <span class="hlt">ocean</span> <span class="hlt">wave</span> energy extraction system. An optimal control method based on internal model proportion integration differentiation (IM-PID) is proposed in this paper though most of <span class="hlt">ocean</span> <span class="hlt">wave</span> energy extraction systems are optimized by the structure, weight, and material. With this control method, the heavy speed of outer heavy buoy of the energy extraction system is in resonance with incident <span class="hlt">wave</span>, and the system efficiency is largely improved. Validity of the proposed optimal control method is verified in both regular and irregular <span class="hlt">ocean</span> <span class="hlt">waves</span>, and it is shown that IM-PID control method is optimal in that it maximizes the energy conversion efficiency. In addition, the anti-interference ability of IM-PID control method has been assessed, and the results show that the IM-PID control method has good robustness, high precision, and strong anti-interference ability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19850038336&hterms=project+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dproject%2Bwaves','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19850038336&hterms=project+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Dproject%2Bwaves"><span>A comparison of in situ and airborne radar observations of <span class="hlt">ocean</span> <span class="hlt">wave</span> directionality</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jackson, F. C.; Walton, W. T.; Peng, C. Y.</p> <p>1985-01-01</p> <p>The directional spectrum of a fully arisen, about 3 m sea as measured by an experimental airborne radar, the NASA K(u)-band radar <span class="hlt">ocean</span> <span class="hlt">wave</span> spectrometer (ROWS), is compared to reference pitch-roll buoy data and to the classical SWOP (stereo <span class="hlt">wave</span> observations project) spectrum for fully developed conditions. The ROWS spectrum, inferred indirectly from backscattered <span class="hlt">power</span> measurements at 5-km altitude, is shown to be in excellent agreement with the buoy spectrum. Specifically, excellent agreement is found between the two nondirectional height spectra, and mean <span class="hlt">wave</span> directions and directional spreads as functions of frequency. A comparison of the ROWS and SWOP spectra shows the two spectra to be very similar, in detailed shape as well as in terms of the gross spreading characteristics. Both spectra are seen to exhibit bimodal structures which accord with the Phillips' (1958) resonance mechanism. This observation is thus seen to support Phillips' contention that the SWOP modes were indeed resonance modes, not statistical artifacts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNG21A0153Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNG21A0153Z"><span>Modeling internal <span class="hlt">wave</span> generation by seamounts in <span class="hlt">oceans</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, L.; Buijsman, M. C.; Comino, E. L.; Swinney, H.</p> <p>2017-12-01</p> <p>Recent global bathymetric data at 30 arc-sec resolution has revealed that there are 33,452 seamounts and 138,412 knolls in the <span class="hlt">oceans</span>. To develop an estimate for the energy converted from tidal flow to internal gravity <span class="hlt">waves</span>, we have conducted numerical simulations using the Massachusetts Institute of Technology circulation model (MITgcm) to compute the energy conversion by randomly distributed Gaussian-shaped seamounts. We find that for an isolated axisymmetric seamount of height 1100 m and radius 1600 m, which corresponds to the Wessel height-to-radius ratio 0.69, the conversion rate is 100 kW, assuming a tidal speed amplitude 1 cm/s, buoyancy frequency 1e-3 rad/s, and circularly polarized tidal motion, and taking into account the earth's rotation. The 100 kW estimate is about 60% less than the 3-D linear theory prediction because fluid goes around a seamount instead of over it. Our estimate accounts the suppression of energy conversion due to <span class="hlt">wave</span> interference at the generation site of closely spaced seamounts. We conclude that for randomly distributed Gaussian seamounts of varying widths and separations, separated on average by 18 km as in the <span class="hlt">oceans</span>, <span class="hlt">wave</span> interference reduces the energy conversion by seamounts by only about 16%. This result complements previous studies of <span class="hlt">wave</span> interference for 2-D ridges.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=3650&hterms=worlds+oceans&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dworlds%2Boceans','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=3650&hterms=worlds+oceans&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dworlds%2Boceans"><span>Deep <span class="hlt">Ocean</span> Tsunami <span class="hlt">Waves</span> off the Sri Lankan Coast</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>2004-01-01</p> <p>The initial tsunami <span class="hlt">waves</span> resulting from the undersea earthquake that occurred at 00:58:53 UTC (Coordinated Universal Time) on December 26, 2004, off the island of Sumatra, Indonesia, took a little over 2 hours to reach the teardrop-shaped island of Sri Lanka. Additional <span class="hlt">waves</span> continued to arrive for many hours afterward. At approximately 05:15 UTC, as NASA's Terra satellite passed overhead, the Multi-angle Imaging SpectroRadiometer (MISR) captured this image of deep <span class="hlt">ocean</span> tsunami <span class="hlt">waves</span> about 30-40 kilometers from Sri Lanka's southwestern coast. The <span class="hlt">waves</span> are made visible due to the effects of changes in sea-surface slope on the reflected sunglint pattern, shown here in MISR's 46-degree-forward-pointing camera. Sunglint occurs when sunlight reflects off a water surface in much the same way light reflects off a mirror, and the position of the Sun, angle of observation, and orientation of the sea surface determines how bright each part of the <span class="hlt">ocean</span> appears in the image. These large <span class="hlt">wave</span> features were invisible to MISR's nadir (vertical-viewing) camera. The image covers an area of 208 kilometers by 207 kilometers. The greatest impact of the tsunami was generally in an east-west direction, so the havoc caused by the tsunami along the southwestern shores of Sri Lanka was not as severe as along the eastern coast. However, substantial damage did occur in this region' as evidenced by the brownish debris in the water' because tsunami <span class="hlt">waves</span> can diffract around land masses. The ripple-like <span class="hlt">wave</span> pattern evident in this MISR image roughly correlates with the undersea boundary of the continental shelf. The surface <span class="hlt">wave</span> pattern is likely to have been caused by interaction of deep <span class="hlt">waves</span> with the <span class="hlt">ocean</span> floor, rather than by the more usually observed surface <span class="hlt">waves</span>, which are driven by winds. It is possible that this semi-concentric pattern represents <span class="hlt">wave</span> reflection from the continental land mass; however, a combination of <span class="hlt">wave</span> modeling and detailed bathymetric data is required to</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFM.C41D..08M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFM.C41D..08M"><span><span class="hlt">Ocean</span> <span class="hlt">wave</span> generation by collapsing ice shelves</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Macayeal, D. R.; Bassis, J. N.; Okal, E. A.; Aster, R. C.; Cathles, L. M.</p> <p>2008-12-01</p> <p>The 28-29 February, 2008, break-up of the Wilkins Ice Shelf, Antarctica, exemplifies the now-familiar, yet largely unexplained pattern of explosive ice-shelf break-up. While environmental warming is a likely ultimate cause of explosive break-up, several key aspects of their short-term behavior need to be explained: (1) The abrupt, near-simultaneous onset of iceberg calving across long spans of the ice front margin; (2) High outward drift velocity (about 0.3 m/s) of a leading phalanx of tabular icebergs that originate from the seaward edge of the intact ice shelf prior to break-up; (3) Rapid coverage of the <span class="hlt">ocean</span> surface in the wake of this leading phalanx by small, capsized and dismembered tabular icebergs; (4) Extremely large gravitational potential energy release rates, e.g., up to 3 × 1010 W; (5) Lack of proximal iceberg-calving triggers that control the timing of break-up onset and that maintain the high break-up calving rates through to the conclusion of the event. Motivated by seismic records obtained from icebergs and the Ross Ice Shelf that show hundreds of micro- tsunamis emanating from near the ice shelf front, we re-examine the basic dynamic features of ice- shelf/<span class="hlt">ocean-wave</span> interaction and, in particular, examine the possibility that collapsing ice shelves themselves are a source of <span class="hlt">waves</span> that stimulate the disintegration process. We propose that ice-shelf generated surface-gravity <span class="hlt">waves</span> associated with initial calving at an arbitrary seed location produce stress perturbations capable of triggering the onset of calving on the entire ice front. <span class="hlt">Waves</span> generated by parting detachment rifts, iceberg capsize and break-up act next to stimulate an inverted submarine landslide (ice- slide) process, where gravitational potential energy released by upward movement of buoyant ice is radiated as surface gravity <span class="hlt">waves</span> in the wake of the advancing phalanx of tabular icebergs. We conclude by describing how field research and remote sensing can be used to test the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820063958&hterms=Electromagnetic+Spectrum&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DElectromagnetic%2BSpectrum','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820063958&hterms=Electromagnetic+Spectrum&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DElectromagnetic%2BSpectrum"><span>Two-frequency /Delta k/ microwave scatterometer measurements of <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra from an aircraft</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Johnson, J. W.; Jones, W. L.; Weissman, D. E.</p> <p>1981-01-01</p> <p>A technique for remotely sensing the large-scale gravity <span class="hlt">wave</span> spectrum on the <span class="hlt">ocean</span> surface using a two frequency (Delta k) microwave scatterometer has been demonstrated from stationary platforms and proposed from moving platforms. This measurement takes advantage of Bragg type resonance matching between the electromagnetic wavelength at the difference frequency and the length of the large-scale surface <span class="hlt">waves</span>. A prominent resonance appears in the cross product <span class="hlt">power</span> spectral density (PSD) of the two backscattered signals. Ku-Band aircraft scatterometer measurements were conducted by NASA in the North Sea during the 1979 Maritime Remote Sensing (MARSEN) experiment. Typical examples of cross product PSD's computed from the MARSEN data are presented. They demonstrate strong resonances whose frequency and bandwidth agree with the surface characteristics and the theory. Directional modulation spectra of the surface reflectivity are compared to the gravity <span class="hlt">wave</span> spectrum derived from surface truth measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29439408','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29439408"><span>Flow Control in Wells Turbines for Harnessing Maximum <span class="hlt">Wave</span> <span class="hlt">Power</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Lekube, Jon; Garrido, Aitor J; Garrido, Izaskun; Otaola, Erlantz; Maseda, Javier</p> <p>2018-02-10</p> <p><span class="hlt">Oceans</span>, and particularly <span class="hlt">waves</span>, offer a huge potential for energy harnessing all over the world. Nevertheless, the performance of current energy converters does not yet allow us to use the <span class="hlt">wave</span> energy efficiently. However, new control techniques can improve the efficiency of energy converters. In this sense, the plant sensors play a key role within the control scheme, as necessary tools for parameter measuring and monitoring that are then used as control input variables to the feedback loop. Therefore, the aim of this work is to manage the rotational speed control loop in order to optimize the output <span class="hlt">power</span>. With the help of outward looking sensors, a Maximum <span class="hlt">Power</span> Point Tracking (MPPT) technique is employed to maximize the system efficiency. Then, the control decisions are based on the pressure drop measured by pressure sensors located along the turbine. A complete <span class="hlt">wave</span>-to-wire model is developed so as to validate the performance of the proposed control method. For this purpose, a novel sensor-based flow controller is implemented based on the different measured signals. Thus, the performance of the proposed controller has been analyzed and compared with a case of uncontrolled plant. The simulations demonstrate that the flow control-based MPPT strategy is able to increase the output <span class="hlt">power</span>, and they confirm both the viability and goodness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5855045','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5855045"><span>Flow Control in Wells Turbines for Harnessing Maximum <span class="hlt">Wave</span> <span class="hlt">Power</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>Garrido, Aitor J.; Garrido, Izaskun; Otaola, Erlantz; Maseda, Javier</p> <p>2018-01-01</p> <p><span class="hlt">Oceans</span>, and particularly <span class="hlt">waves</span>, offer a huge potential for energy harnessing all over the world. Nevertheless, the performance of current energy converters does not yet allow us to use the <span class="hlt">wave</span> energy efficiently. However, new control techniques can improve the efficiency of energy converters. In this sense, the plant sensors play a key role within the control scheme, as necessary tools for parameter measuring and monitoring that are then used as control input variables to the feedback loop. Therefore, the aim of this work is to manage the rotational speed control loop in order to optimize the output <span class="hlt">power</span>. With the help of outward looking sensors, a Maximum <span class="hlt">Power</span> Point Tracking (MPPT) technique is employed to maximize the system efficiency. Then, the control decisions are based on the pressure drop measured by pressure sensors located along the turbine. A complete <span class="hlt">wave</span>-to-wire model is developed so as to validate the performance of the proposed control method. For this purpose, a novel sensor-based flow controller is implemented based on the different measured signals. Thus, the performance of the proposed controller has been analyzed and compared with a case of uncontrolled plant. The simulations demonstrate that the flow control-based MPPT strategy is able to increase the output <span class="hlt">power</span>, and they confirm both the viability and goodness. PMID:29439408</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999AIPC..474..136J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999AIPC..474..136J"><span>High <span class="hlt">power</span> broadband millimeter <span class="hlt">wave</span> TWTs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>James, Bill G.</p> <p>1999-05-01</p> <p>In the early 1980's the requirement for high <span class="hlt">power</span> broadband millimeter <span class="hlt">wave</span> sources encouraged the development of microwave vacuum device amplifiers for radar and communication systems. Many government funded programs were implemented for the development of high <span class="hlt">power</span> broadband millimeter <span class="hlt">wave</span> amplifiers that would meet the needs of the high <span class="hlt">power</span> community. The tube design capable of meeting these goals was the slow <span class="hlt">wave</span> coupled cavity traveling <span class="hlt">wave</span> device, which had a proven technology base at the lower frequencies (X Band). However scaling this technology to the millimeter frequencies had severe shortcomings in both thermal and manufacturing design. These shortcomings were overcome with the development of the Ladder Circuit technology. In conjunction with the circuit development high <span class="hlt">power</span> electron beam systems had to be developed for the generation of high rf <span class="hlt">powers</span>. These beam systems had to be capable of many megawatts of beam <span class="hlt">power</span> density and high current densities. The cathode technology required to be capable of operating at current densities of 10 amperes per square centimeter at long pulse lengths and high duty cycle. Since the introduction of the Ladder Circuit technology a number of high <span class="hlt">power</span> broadband millimeter <span class="hlt">wave</span> amplifiers have been developed using this technology, and have been deployed in operating radar and communication systems. Broadband millimeter <span class="hlt">wave</span> sources have been manufactured in the frequency range from 27 GHz to 100 GHz with <span class="hlt">power</span> levels ranging from 100 watts to 50 kilowatts. Today the <span class="hlt">power</span> levels achieved by these devices are nearing the limits of this technology; therefore to gain a significant increase in <span class="hlt">power</span> at the millimeter <span class="hlt">wave</span> frequencies other technologies will have to be considered particularly fast <span class="hlt">wave</span> devices. This paper will briefly review the ladder circuit technology and present the designs of a number of broadband high <span class="hlt">power</span> devices developed at Ka and W band. The discussion will include the beam systems</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920052049&hterms=Rogue&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DRogue','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19920052049&hterms=Rogue&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3DRogue"><span>The local properties of <span class="hlt">ocean</span> surface <span class="hlt">waves</span> by the phase-time method</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Huang, Norden E.; Long, Steven R.; Tung, Chi-Chao; Donelan, Mark A.; Yuan, Yeli; Lai, Ronald J.</p> <p>1992-01-01</p> <p>A new approach using phase information to view and study the properties of frequency modulation, <span class="hlt">wave</span> group structures, and <span class="hlt">wave</span> breaking is presented. The method is applied to <span class="hlt">ocean</span> <span class="hlt">wave</span> time series data and a new type of <span class="hlt">wave</span> group (containing the large 'rogue' <span class="hlt">waves</span>) is identified. The method also has the capability of broad applications in the analysis of time series data in general.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19790019465','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19790019465"><span>Directional spectra of <span class="hlt">ocean</span> <span class="hlt">waves</span> from microwave backscatter: A physical optics solution with application to the short-pulse and two-frequency measurement techniques</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jackson, F. C.</p> <p>1979-01-01</p> <p>Two simple microwave radar techniques that are potentially capable of providing routine satellite measurements of the directional spectrum of <span class="hlt">ocean</span> <span class="hlt">waves</span> were developed. One technique, the short pulse technique, makes use of very short pulses to resolve <span class="hlt">ocean</span> surface <span class="hlt">wave</span> contrast features in the range direction; the other technique, the two frequency correlation technique makes use of coherency in the transmitted waveform to detect the large <span class="hlt">ocean</span> <span class="hlt">wave</span> contrast modulation as a beat or mixing frequency in the <span class="hlt">power</span> backscattered at two closely separated microwave frequencies. A frequency domain analysis of the short pulse and two frequency systems shows that the two measurement systems are essentially duals; they each operate on the generalized (three frequency) fourth-order statistical moment of the surface transfer function in different, but symmetrical ways, and they both measure the same directional contrast modulation spectrum. A three dimensional physical optics solution for the fourth-order moment was obtained for backscatter in the near vertical, specular regime, assuming Gaussian surface statistics.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998APS..APR.I1302J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998APS..APR.I1302J"><span>High <span class="hlt">Power</span> Broadband Millimeter <span class="hlt">Wave</span> TWTs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>James, Bill G.</p> <p>1998-04-01</p> <p>In the early 1980's the requirement for high <span class="hlt">power</span> broadband millimeter <span class="hlt">wave</span> sources encouraged the development of microwave vacuum device amplifiers for radar and communication systems. Many government funded programs were implemented for the development of high <span class="hlt">power</span> broadband millimeter <span class="hlt">wave</span> amplifiers that would meet the needs of the high <span class="hlt">power</span> community. The tube design capable of meeting these goals was the slow <span class="hlt">wave</span> coupled cavity traveling <span class="hlt">wave</span> device, which had a proven technology base at the lower frequencies (X Band). However scaling this technology to the millimeter frequencies had severe shortcomings in both thermal and manufacturing design. These shortcomings were overcome with the development of the Ladder Circuit technology. In conjunction with the circuit development high <span class="hlt">power</span> electron beam systems had to be developed for the generation of high rf <span class="hlt">powers</span>. These beam systems had to be capable of many megawatts of beam <span class="hlt">power</span> density and high current densities. The cathode technology required to be capable of operating at current densities of 10 amperes per square centimeter at long pulse lengths and high duty cycle. Since the introduction of the Ladder Circuit technology a number of high <span class="hlt">power</span> broadband millimeter <span class="hlt">wave</span> amplifiers have been developed and deployed in operating radar and communication systems. Broadband millimeter <span class="hlt">wave</span> sources have been manufactured in the frequency range from 27 GHz to 100 GHz with <span class="hlt">power</span> levels ranging from 100 watts CW to 10 kilowatts Peak at W band over a 2 GHz bandwidth. Also a 50 kW peak <span class="hlt">power</span> and 10 kW average <span class="hlt">power</span> device at Ka band with 2 GHz bandwidth has been developed. Today the <span class="hlt">power</span> levels achieved by these devices are nearing the limits of this technology; therefore to gain a significant increase in <span class="hlt">power</span> at the millimeter <span class="hlt">wave</span> frequencies, other technologies will have to be considered, particularly fast <span class="hlt">wave</span> devices. This paper will briefly review the ladder circuit technology and present the designs of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMOS52A..06G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMOS52A..06G"><span>Long Term Autonomous <span class="hlt">Ocean</span> Remote Sensing Utilizing the <span class="hlt">Wave</span> Glider</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Griffith, J.</p> <p>2012-12-01</p> <p>Rising costs of ship time and increasing budgetary restrictions make installation and maintenance of fixed <span class="hlt">ocean</span> buoys a logistical and financial challenge. The cost associated with launch, recovery, and maintenance has resulted in a limited number of deployed buoys, restricting data on <span class="hlt">oceanic</span> conditions. To address these challenges, Liquid Robotics (LRI) has developed the <span class="hlt">Wave</span> Glider, an autonomous, mobile remote sensing solution. This system utilizes <span class="hlt">wave</span> energy for propulsion allowing for long duration deployments of up to one year while providing real-time data on meteorological and oceanographic conditions. In November 2011, LRI deployed four <span class="hlt">Wave</span> Gliders on a mission to cross the Pacific <span class="hlt">Ocean</span> (the PacX) from San Francisco to Australia (two vehicles) or Japan (two vehicles) while transmitting data on weather conditions, <span class="hlt">wave</span> profiles, sea surface temperatures, and biological conditions in real-time. This report evaluates the vehicle's ability to operate as an <span class="hlt">ocean</span> going data platform by comparing data from the onboard weather sensors with two moored buoys, NDBC 46092 (Monterey Bay) and NDBC 51000 (200 nmi NE of Maui). The report also analyzes data transmitted from all four vehicles as they passed directly through a tropical storm 580 nmi NE of Hawaii. Upon arriving at one of the aforementioned buoys, the gliders continuously circled for a period of two days at a distance of three to eight nautical miles to build a comparative dataset. Data from both platforms were streamed in near real time enabling mid-mission evaluation of the performance of sensors. Overall, results varied from a <0.5% difference in barometric pressure between buoy NDBC 46092 and the gliders to high disagreement in wind speed and direction. While comparisons to moored buoy data can provide valuable insight into the relative accuracy of each platform, differences in agreement on variables such as wind speed and direction were attributed to micro-spatial variability in <span class="hlt">oceanic</span> conditions</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT........63W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT........63W"><span>On the coupled evolution of <span class="hlt">oceanic</span> internal <span class="hlt">waves</span> and quasi-geostrophic flow</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wagner, Gregory LeClaire</p> <p></p> <p><span class="hlt">Oceanic</span> motion outside thin boundary layers is primarily a mixture of quasi-geostrophic flow and internal <span class="hlt">waves</span> with either near-inertial frequencies or the frequency of the semidiurnal lunar tide. This dissertation seeks a deeper understanding of <span class="hlt">waves</span> 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 <span class="hlt">waves</span>; a three-component model that couples quasi-geostrophic flow to both near-inertial <span class="hlt">waves</span> 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 <span class="hlt">oceanic</span> internal tides. Four results emerge. First, the <span class="hlt">wave</span>-averaged quasi-geostrophic equation reveals that finite-amplitude <span class="hlt">waves</span> 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 <span class="hlt">waves</span> and quasi-geostrophic flow. The third result, hashed out for near-inertial <span class="hlt">waves</span> and quasi-geostrophic flow, is that <span class="hlt">wave</span>-flow interaction leads to energy exchange even under conditions of weak nonlinearity. For storm-forced <span class="hlt">oceanic</span> near-inertial <span class="hlt">waves</span> the interaction often energizes <span class="hlt">waves</span> 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 <span class="hlt">waves</span>. The fourth result is that quasi-geostrophic flow can encourage or 'catalyze' a nonlinear interaction between a near-inertial <span class="hlt">wave</span> field and its second harmonic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24711719','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24711719"><span>Modelling rogue <span class="hlt">waves</span> through exact dynamical lump soliton controlled by <span class="hlt">ocean</span> currents.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kundu, Anjan; Mukherjee, Abhik; Naskar, Tapan</p> <p>2014-04-08</p> <p>Rogue <span class="hlt">waves</span> are extraordinarily high and steep isolated <span class="hlt">waves</span>, which appear suddenly in a calm sea and disappear equally fast. However, though the rogue <span class="hlt">waves</span> are localized surface <span class="hlt">waves</span>, 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 <span class="hlt">wave</span>. 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 <span class="hlt">wave</span> with adjustable height and modular inclination. The lump soliton under the influence of an <span class="hlt">ocean</span> 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 <span class="hlt">ocean</span> rogue <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3928955','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3928955"><span>Modelling rogue <span class="hlt">waves</span> through exact dynamical lump soliton controlled by <span class="hlt">ocean</span> currents</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kundu, Anjan; Mukherjee, Abhik; Naskar, Tapan</p> <p>2014-01-01</p> <p>Rogue <span class="hlt">waves</span> are extraordinarily high and steep isolated <span class="hlt">waves</span>, which appear suddenly in a calm sea and disappear equally fast. However, though the rogue <span class="hlt">waves</span> are localized surface <span class="hlt">waves</span>, 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 <span class="hlt">wave</span>. 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 <span class="hlt">wave</span> with adjustable height and modular inclination. The lump soliton under the influence of an <span class="hlt">ocean</span> 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 <span class="hlt">ocean</span> rogue <span class="hlt">waves</span>. PMID:24711719</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/49319-directional-ocean-wave-measurements-coastal-setting-using-focused-array-imaging-radar','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/49319-directional-ocean-wave-measurements-coastal-setting-using-focused-array-imaging-radar"><span>Directional <span class="hlt">ocean</span> <span class="hlt">wave</span> measurements in a coastal setting using a focused array imaging radar</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>Frasier, S.J.; Liu, Y.; Moller, D.</p> <p>1995-03-01</p> <p>A unique focused array imaging Doppler radar was used to measure directional spectra of <span class="hlt">ocean</span> surface <span class="hlt">waves</span> in a nearshore experiment performed on the North Carolina Outer Banks. Radar images of the <span class="hlt">ocean</span> surface`s Doppler velocity were used to generate two dimensional spectra of the radial component of the <span class="hlt">ocean</span> surface velocity field. These are compared to simultaneous in-situ measurements made by a nearby array of submerged pressure sensors. Analysis of the resulting two-dimensional spectra include comparisons of dominant <span class="hlt">wave</span> lengths, <span class="hlt">wave</span> directions, and <span class="hlt">wave</span> energy accounting for relative differences in water depth at the measurement locations. Limited estimates ofmore » the two-dimensional surface displacement spectrum are derived from the radar data. The radar measurements are analogous to those of interferometric synthetic aperture radars (INSAR), and the equivalent INSAR parameters are shown. The agreement between the remote and in-situ measurements suggests that an imaging Doppler radar is effective for these <span class="hlt">wave</span> measurements at near grazing incidence angles.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19750012731','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19750012731"><span>Technical guidance and analytic services in support of SEASAT-A. [radar altimeters for altimetry and <span class="hlt">ocean</span> <span class="hlt">wave</span> height</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Brooks, W. L.; Dooley, R. P.</p> <p>1975-01-01</p> <p>The design of a high resolution radar for altimetry and <span class="hlt">ocean</span> <span class="hlt">wave</span> height estimation was studied. From basic principles, it is shown that a short pulse wide beam radar is the most appropriate and recommended technique for measuring both altitude and <span class="hlt">ocean</span> <span class="hlt">wave</span> height. To achieve a topographic resolution of + or - 10 cm RMS at 5.0 meter RMS <span class="hlt">wave</span> heights, as required for SEASAT-A, it is recommended that the altimeter design include an onboard adaptive processor. The resulting design, which assumes a maximum likelihood estimation (MLE) processor, is shown to satisfy all performance requirements. A design summary is given for the recommended radar altimeter, which includes a full deramp STRETCH pulse compression technique followed by an analog filter bank to separate range returns as well as the assumed MLE processor. The feedback loop implementation of the MLE on a digital computer was examined in detail, and computer size, estimation accuracies, and bias due to range sidelobes are given for the MLE with typical SEASAT-A parameters. The standard deviation of the altitude estimate was developed and evaluated for several adaptive and nonadaptive split-gate trackers. Split-gate tracker biases due to range sidelobes and transmitter noise are examined. An approximate closed form solution for the altimeter <span class="hlt">power</span> return is derived and evaluated. The feasibility of utilizing the basic radar altimeter design for the measurement of <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra was examined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27849059','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27849059"><span>Overlooked Role of Mesoscale Winds in <span class="hlt">Powering</span> <span class="hlt">Ocean</span> Diapycnal Mixing.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jing, Zhao; Wu, Lixin; Ma, Xiaohui; Chang, Ping</p> <p>2016-11-16</p> <p>Diapycnal mixing affects the uptake of heat and carbon by the <span class="hlt">ocean</span> as well as plays an important role in global <span class="hlt">ocean</span> circulations and climate. In the thermocline, winds provide an important energy source for furnishing diapycnal mixing primarily through the generation of near-inertial internal <span class="hlt">waves</span>. However, this contribution is largely missing in the current generation of climate models. In this study, it is found that mesoscale winds at scales of a few hundred kilometers account for more than 65% of near-inertial energy flux into the North Pacific basin and 55% of turbulent kinetic dissipation rate in the thermocline, suggesting their dominance in <span class="hlt">powering</span> diapycnal mixing in the thermocline. Furthermore, a new parameterization of wind-driven diapycnal mixing in the <span class="hlt">ocean</span> interior for climate models is proposed, which, for the first time, successfully captures both temporal and spatial variations of wind-driven diapycnal mixing in the thermocline. It is suggested that as mesoscale winds are not resolved by the climate models participated in the Coupled Model Intercomparison Project Phase 5 (CMIP5) due to insufficient resolutions, the diapycnal mixing is likely poorly represented, raising concerns about the accuracy and robustness of climate change simulations and projections.</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 <span class="hlt">Ocean</span> Winds, Surface <span class="hlt">Waves</span> and Surface Currents 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 <span class="hlt">ocean</span> 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 <span class="hlt">ocean</span> winds by applying our C-band Cross-Polarization Coupled-Parameters <span class="hlt">Ocean</span> (C-3PO) wind retrieval model [Zhang et al., 2017, IEEE TGRS] to the SAR images. <span class="hlt">Ocean</span> <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. <span class="hlt">Ocean</span>.]. We estimate the <span class="hlt">ocean</span> surface currents using the Doppler Shift extracted from VV-polarized SAR images [Kang et al., 2016, IEEE TGRS]. C-3PO model is based on theoretical analysis of <span class="hlt">ocean</span> surface <span class="hlt">waves</span> and SAR microwave backscatter. Based on the retrieved <span class="hlt">ocean</span> winds, we estimate the hurricane center locations, maxima wind speeds, and radii of the five hurricanes by adopting the SHEW model (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 <span class="hlt">ocean</span> surface currents respond to the hurricane. A system of methods capable of observing marine winds, surface <span class="hlt">waves</span>, and surface currents 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 <span class="hlt">ocean</span> winds</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_6");'>6</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li class="active"><span>8</span></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_8 --> <div id="page_9" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="161"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFM.C11A..04A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFM.C11A..04A"><span><span class="hlt">Ocean</span> <span class="hlt">Wave</span> Energy Regimes of the Circumpolar Coastal Zones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Atkinson, D. E.</p> <p>2004-12-01</p> <p><span class="hlt">Ocean</span> <span class="hlt">wave</span> activity is a major enviromental forcing agent of the ice-rich sediments that comprise large sections of the arctic coastal margins. While it is instructive to possess information about the wind regimes in these regions, direct application to geomorphological and engineering needs requires knowledge of the resultant <span class="hlt">wave</span>-energy regimes. <span class="hlt">Wave</span> energy information has been calculated at the regional scale using adjusted reanalysis model windfield data. Calculations at this scale are not designed to account for local-scale coastline/bathymetric irregularities and variability. Results will be presented for the circumpolar zones specified by the Arctic Coastal Dynamics Project.</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 coupled equatorial atmospheric Kelvin <span class="hlt">waves</span> over Indian <span class="hlt">Ocean</span> 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 coupled Kelvin <span class="hlt">waves</span> in the Indian <span class="hlt">Ocean</span> 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 <span class="hlt">Ocean</span>. 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 <span class="hlt">Ocean</span> 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 coupled 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://adsabs.harvard.edu/abs/2013EGUGA..15..462R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..15..462R"><span>Internal <span class="hlt">waves</span> and Equatorial dynamics: an observational study in the West Atlantic <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rabitti, Anna; Maas, Leo R. M.; van Haren, Hans; Gerkema, Theo</p> <p>2013-04-01</p> <p>Internal <span class="hlt">waves</span> present several fascinating aspects of great relevance for geo- and astro-physical fluid dynamics. These <span class="hlt">waves</span> are supported by all kinds of stratified and rotating fluids, such as, for example, our <span class="hlt">ocean</span>, atmosphere, a planet fluid core or a star. In a non linear regime, because of their oblique propagation, they are thought to play a key role in diapycnal mixing, as well as in angular momentum mixing. Unfortunately, a complete analytical description of internal <span class="hlt">waves</span> in arbitrarily shaped enclosed domains is still an ongoing challenge. On the other hand, internal <span class="hlt">wave</span> energy is observed travelling along rays, whose behaviour can be traced and whose reflections off the container's boundaries appears crucial in producing phenomena such as focussing of <span class="hlt">wave</span> energy onto specific trajectories (attractors), and in triggering localized instabilities. Ray tracing studies have shown that equatorial regions of stratified and/or rotating spherical shells are likely affected by these features, being the place where the simplest shaped and most energetic attractors occur. In this study we aim to investigate the possible presence and role of internal <span class="hlt">wave</span> attractors in determining the equatorial <span class="hlt">ocean</span> dynamics. Internal <span class="hlt">wave</span> attractors, observed in laboratory and numerical experiments, have not been observed in Nature, yet. A unique set of observations, collected in the deep Equatorial West Atlantic <span class="hlt">Ocean</span>, will be used here in order to explore this possibility, the dataset consisting of 1.5 year long time series of current measured acoustically and with current meters moored between 0°and 2°N, at 37°W, off the Brazilian coast. In particular, angular momentum mixing due to internal <span class="hlt">wave</span> focussing, is explored as a possible mechanism for maintaining the Equatorial Deep Jets. These jets are stacked alternating zonal currents that are ubiquitously observed in all the <span class="hlt">oceans</span> and whose nature is still largely unknown. Remarkably, jet like structures are also</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S22A..05G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S22A..05G"><span>Impact of <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Climate on Double-Frequency Microseisms and Evaluation of Seismic Site Effect in Northern Mississippi, USA</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Guo, Z.; Aydin, A.; Xue, M.</p> <p>2017-12-01</p> <p>This research presents the <span class="hlt">power</span> spectral density (PSD) of double-frequency (DF) microseisms in both vertical (V) and resultant horizontal (H) directions and horizontal-to-vertical spectral ratios (HVSR) of 13 continuous single point long-term ambient noise recordings (LTR) at 5 inland and 2 coastal locations selected in Mississippi Embayment, and frequency value and PSD at DF peak (PSD@DF), predominant frequency (f0) and HVSR value at f0 (HVSR@f0) at 234 single point short-term ambient noise recordings (STR) over a large range of unconsolidated sediment thickness (UST) in Northern Mississippi. By correlating PSD of LTRs with the simultaneous <span class="hlt">ocean</span> <span class="hlt">wave</span> climate data of Atlantic <span class="hlt">Ocean</span> and Gulf of Mexico, DF microseisms observed in Northern Mississippi were shown to be shaped by a combined impact of <span class="hlt">wave</span> climates of both Atlantic <span class="hlt">Ocean</span> and Gulf of Mexico. Polarization analysis conducted separately for LTRs and STRs strengthen this conclusion. The LTRs show stable estimates of f0, on the other hand, time-dependent variations on HVSR@f0 value. The plots of DFH-UST, rather than DFV-UST, coincide well with plots of f0-UST within area where UST is larger than 300 m, which indicates that the shear <span class="hlt">wave</span> resonance in thick sediments modifies the DF microseisms more obviously in horizontal direction than in vertical direction. Transfer functions between HVSR@f0 and <span class="hlt">ocean</span> data indicates that the variation of HVSR@f0 is caused by variations of source location and energy level of DF microseisms, i.e. <span class="hlt">ocean</span> <span class="hlt">wave</span> activities in Atlantic <span class="hlt">Ocean</span> and Gulf of Mexico. Additionally, 3D microseism spectra of each LTR and those of all STRs within each 100 m-UST group are converted into spatial spectral vectors and projected on stereographic nets. Patterns of the clusters formed by these projections show that the HVSR@f0 values are related to both UST and vibration source location and energy level.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820044061&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dfunction%2Bwave','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820044061&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dfunction%2Bwave"><span>Optimal spatial filtering and transfer function for SAR <span class="hlt">ocean</span> <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>Goldfinger, A. D.; Beal, R. C.; Tilley, D. G.</p> <p>1981-01-01</p> <p>The Seasat Synthetic Aperture Radar (SAR) has proved to be an instrument of great utility in the sensing of <span class="hlt">ocean</span> conditions on a global scale. An analysis of oceanographic and atmospheric aspects of Seasat data has shown that the features observed in the imagery are linked to <span class="hlt">ocean</span> phenomena such as storm sources and their resulting swell systems. However, there remains one central problem which has not been satisfactorily solved to date. This problem is related to the accurate measurement of wind-generated <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra. Investigations addressing this problem are currently being conducted. The problem has two parts, including the accurate measurement of the image spectra and the inference of actual surface <span class="hlt">wave</span> spectra from these measurements. A description is presented of the progress made towards solving the first part of the problem, taking into account a digital rather than optical computation of the image transforms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.C51B0970C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.C51B0970C"><span><span class="hlt">Ocean</span> <span class="hlt">Wave</span>-to-Ice Energy Transfer Determined from Seafloor Pressure and Ice Shelf Seismic Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Z.; Bromirski, P. D.; Gerstoft, P.; Stephen, R. A.; Wiens, D.; Aster, R. C.; Nyblade, A.</p> <p>2017-12-01</p> <p>Ice shelves play an important role in buttressing land ice from reaching the sea, thus restraining the rate of sea level rise. Long-period gravity <span class="hlt">wave</span> impacts excite vibrations in ice shelves that may trigger tabular iceberg calving and/or ice shelf collapse events. Three kinds of seismic plate <span class="hlt">waves</span> were continuously observed by broadband seismic arrays on the Ross Ice Shelf (RIS) and on the Pine Island Glacier (PIG) ice shelf: (1) flexural-gravity <span class="hlt">waves</span>, (2) flexural <span class="hlt">waves</span>, and (3) extensional Lamb <span class="hlt">waves</span>, suggesting that all West Antarctic ice shelves are subjected to similar gravity <span class="hlt">wave</span> excitation. <span class="hlt">Ocean</span> gravity <span class="hlt">wave</span> heights were estimated from pressure perturbations recorded by an <span class="hlt">ocean</span> bottom differential pressure gauge at the RIS front, water depth 741 m, about 8 km north of an on-ice seismic station that is 2 km from the shelf front. Combining the plate <span class="hlt">wave</span> spectrum, the frequency-dependent energy transmission and reflection at the ice-water interface were determined. In addition, Young's modulus and Poisson's ratio of the RIS are estimated from the plate <span class="hlt">wave</span> motions, and compared with the widely used values. Quantifying these ice shelf parameters from observations will improve modeling of ice shelf response to <span class="hlt">ocean</span> forcing, and ice shelf evolution.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70018602','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70018602"><span>Southern <span class="hlt">Ocean</span> monthly <span class="hlt">wave</span> fields for austral winters 1985-1988 by Geosat radar altimeter</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Josberger, E.G.; Mognard, N.M.</p> <p>1996-01-01</p> <p>Four years of monthly averaged <span class="hlt">wave</span> height fields for the austral winters 19851988 derived from the Geosat altimeter data show a spatial variability of the scale of 500-1000 km that varies monthly and annually. This variability is superimposed on the zonal patterns surrounding the Antarctic continent and characteristic of the climatology derived from the U.S. Navy [1992] Marine Climatic Atlas of the World. The location and the intensity of these large-scale features, which are not found in the climatological fields, exhibit strong monthly and yearly variations. A global underestimation of the climatological mean <span class="hlt">wave</span> heights by more than l m is also found over large regions of the Southern <span class="hlt">Ocean</span>. The largest monthly averaged significant <span class="hlt">wave</span> heights are above 5 m and are found during August of every year in the Indian <span class="hlt">Ocean</span>, south of 40??S. The monthly <span class="hlt">wave</span> fields show more variability in the Atlantic and Pacific <span class="hlt">Oceans</span> than in the Indian <span class="hlt">Ocean</span>. The Seasat data from 1978 and the Geosat data from 1985 and 1988 show an eastward rotation of the largest <span class="hlt">wave</span> heights. However, this rotation is absent in 1986 and 1987; the former was a year of unusually low sea states, and the latter was a year of unusually high sea states, which suggests a link to the El Nin??o-Southern Oscillation event of 1986. Copyright 1996 by the American Geophysical Union.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.S41C0813D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.S41C0813D"><span>Seismic <span class="hlt">Wave</span> Velocity in the Subducted <span class="hlt">Oceanic</span> Crust from Autocorrelation of Tectonic Tremor Signals</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ducellier, A.; Creager, K.</p> <p>2017-12-01</p> <p>Hydration and dehydration of minerals in subduction zones play a key role in the geodynamic processes that generate seismicity and that allow tectonic plates to subduct. Detecting the presence of water in the subducted plate is thus crucial to better understand the seismogenesis and the consequent seismic hazard. A landward dipping, low velocity layer has been detected in most subduction zones. In Cascadia, this low velocity zone is characterized by a low S-<span class="hlt">wave</span> velocity and a very high Poisson's ratio, which has been interpreted as high pore-fluid pressure in the upper half part of the subducted <span class="hlt">oceanic</span> crust. Most previous studies were based on seismic reflection imaging, receiver function analysis, or body <span class="hlt">wave</span> tomography, with seismic sources located far from the low velocity zone. In contrast, the sources of the tectonic tremors generated during Episodic Tremor and Slip (ETS) events are located on the plate boundary. As the sources of the tremors are much closer to the low velocity zone, seismic <span class="hlt">waves</span> recorded during ETS events should illuminate the area with greater precision. Most methods to detect and locate tectonic tremors and low-frequency earthquakes are based on the cross correlation of seismic signals; either signals at the same station for different events, or the same event at different stations. We use the autocorrelation of the seismic signal recorded by eight arrays of stations, located in the Olympic Peninsula, Washington. Each tremor, assumed to be on the plate boundary, generates a direct <span class="hlt">wave</span> and reflected and converted <span class="hlt">waves</span> from both the strong shear-<span class="hlt">wave</span> velocity contrast in the mid-<span class="hlt">oceanic</span> crust, and from the Moho of the subducted <span class="hlt">oceanic</span> crust. The time lag between the arrivals of these different <span class="hlt">waves</span> at a seismic station corresponds to a peak of amplitude on the autocorrelation signals. Using the time lags observed for different locations of the tremor source, we intend to invert for the seismic <span class="hlt">wave</span> velocity of the subducted <span class="hlt">oceanic</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.2132G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.2132G"><span><span class="hlt">Oceanic</span> Platform of the Canary Islands: an <span class="hlt">ocean</span> testbed for <span class="hlt">ocean</span> energy converters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>González, Javier; Hernández-Brito, Joaquín.; Llinás, Octavio</p> <p>2010-05-01</p> <p>The <span class="hlt">Oceanic</span> Platform of the Canary Islands (PLOCAN) is a Governmental Consortium aimed to build and operate an off-shore infrastructure to facilitate the deep sea research and speed up the technology associated. This Consortium is overseen by the Spanish Ministry of Science and Innovation and the Canarian Agency for Research and Innovation. The infrastructure consists of an <span class="hlt">oceanic</span> platform located in an area with depths between 50-100 meters, close to the continental slope and four kilometers off the coast of Gran Canaria, in the archipelago of the Canary Islands. The process of construction will start during the first months of 2010 and is expected to be finished in mid-year 2011. PLOCAN serves five strategic lines: an integral observatory able to explore from the deep <span class="hlt">ocean</span> to the atmosphere, an <span class="hlt">ocean</span> technology testbed, a base for underwater vehicles, an innovation platform and a highly specialized training centre. <span class="hlt">Ocean</span> energy is a suitable source to contribute the limited mix-energy conformed in the archipelago of the Canary Islands with a total population around 2 million people unequally distributed in seven islands. Islands of Gran Canaria and Tenerife support the 80% of the total population with 800.000 people each. PLOCAN will contribute to develop the <span class="hlt">ocean</span> energy sector establishing a marine testbed allowing prototypes testing at sea under a meticulous monitoring network provided by the integral observatory, generating valuable information to developers. Reducing costs throughout an integral project management is an essential objective to be reach, providing services such as transportation, customs and administrative permits. <span class="hlt">Ocean</span> surface for testing activities is around 8 km2 with a depth going from 50 to 100 meters, 4km off the coast. Selected areas for testing have off-shore wind <span class="hlt">power</span> conditions around 500-600 W/m2 and <span class="hlt">wave</span> <span class="hlt">power</span> conditions around 6 kW/m in the East coast and 10 kW/m in the North coast. Marine currents in the Canary Islands are</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1994PApGe.142..319C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1994PApGe.142..319C"><span>Excitation of T <span class="hlt">waves</span> in the Indian <span class="hlt">Ocean</span> between Srilanka and southern India</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chadha, R. K.</p> <p>1994-06-01</p> <p>T phases of three earthquakes from the Indian <span class="hlt">Ocean</span> region, recorded by a short-period vertical-component seismic station network located in the vicinity of Kanyakumari on the southernmost tip of India, are studied. Two of these earthquakes are located west of 90°E ridge and one in the Nicobar Island region. However, seven other earthquakes which occurred 150 200 km south of Kanyakumari in the <span class="hlt">ocean</span> did not produce T phases. An analysis of T-<span class="hlt">waves</span> (tertiary <span class="hlt">waves</span>) travel time reveals the zone of P-<span class="hlt">wave</span> to T-<span class="hlt">wave</span> conversion (i.e., PT phase) region to coincide with the western continental slope of Srilanka. Further, it is observed that the disposition of the bathymetry between Srilanka and southern India strongly favours the downslope propagation mechanism of T-<span class="hlt">wave</span> travel to the southern coast of India through SOFAR channel. These observations are reported for the first time from India.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5111103','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5111103"><span>Overlooked Role of Mesoscale Winds in <span class="hlt">Powering</span> <span class="hlt">Ocean</span> Diapycnal Mixing</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Jing, Zhao; Wu, Lixin; Ma, Xiaohui; Chang, Ping</p> <p>2016-01-01</p> <p>Diapycnal mixing affects the uptake of heat and carbon by the <span class="hlt">ocean</span> as well as plays an important role in global <span class="hlt">ocean</span> circulations and climate. In the thermocline, winds provide an important energy source for furnishing diapycnal mixing primarily through the generation of near-inertial internal <span class="hlt">waves</span>. However, this contribution is largely missing in the current generation of climate models. In this study, it is found that mesoscale winds at scales of a few hundred kilometers account for more than 65% of near-inertial energy flux into the North Pacific basin and 55% of turbulent kinetic dissipation rate in the thermocline, suggesting their dominance in <span class="hlt">powering</span> diapycnal mixing in the thermocline. Furthermore, a new parameterization of wind-driven diapycnal mixing in the <span class="hlt">ocean</span> interior for climate models is proposed, which, for the first time, successfully captures both temporal and spatial variations of wind-driven diapycnal mixing in the thermocline. It is suggested that as mesoscale winds are not resolved by the climate models participated in the Coupled Model Intercomparison Project Phase 5 (CMIP5) due to insufficient resolutions, the diapycnal mixing is likely poorly represented, raising concerns about the accuracy and robustness of climate change simulations and projections. PMID:27849059</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1400106-rule-based-phase-control-methodology-slider-crank-wave-energy-converter-power-take-off-system','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1400106-rule-based-phase-control-methodology-slider-crank-wave-energy-converter-power-take-off-system"><span>A rule-based phase control methodology for a slider-crank <span class="hlt">wave</span> energy converter <span class="hlt">power</span> take-off system</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Sang, Yuanrui; Karayaka, H. Bora; Yan, Yanjun</p> <p></p> <p>The slider crank is a proven mechanical linkage system with a long history of successful applications, and the slider-crank <span class="hlt">ocean</span> <span class="hlt">wave</span> energy converter (WEC) is a type of WEC that converts linear motion into rotation. This paper presents a control algorithm for a slider-crank WEC. In this study, a time-domain hydrodynamic analysis is adopted, and an AC synchronous machine is used in the <span class="hlt">power</span> take-off system to achieve relatively high system performance. Also, a rule-based phase control strategy is applied to maximize energy extraction, making the system suitable for not only regular sinusoidal <span class="hlt">waves</span> but also irregular <span class="hlt">waves</span>. Simulations aremore » carried out under regular sinusoidal <span class="hlt">wave</span> and synthetically produced irregular <span class="hlt">wave</span> conditions; performance validations are also presented with high-precision, real <span class="hlt">ocean</span> <span class="hlt">wave</span> surface elevation data. The influences of significant <span class="hlt">wave</span> height, and peak period upon energy extraction of the system are studied. Energy extraction results using the proposed method are compared to those of the passive loading and complex conjugate control strategies; results show that the level of energy extraction is between those of the passive loading and complex conjugate control strategies, and the suboptimal nature of this control strategy is verified.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002CG.....28..537W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002CG.....28..537W"><span>Teaching <span class="hlt">ocean</span> <span class="hlt">wave</span> forecasting using computer-generated visualization and animation—Part 1: sea forecasting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Whitford, Dennis J.</p> <p>2002-05-01</p> <p><span class="hlt">Ocean</span> <span class="hlt">waves</span> are the most recognized phenomena in oceanography. Unfortunately, undergraduate study of <span class="hlt">ocean</span> <span class="hlt">wave</span> dynamics and forecasting involves mathematics and physics and therefore can pose difficulties with some students because of the subject's interrelated dependence on time and space. Verbal descriptions and two-dimensional illustrations are often insufficient for student comprehension. Computer-generated visualization and animation offer a visually intuitive and pedagogically sound medium to present geoscience, yet there are very few oceanographic examples. A two-part article series is offered to explain <span class="hlt">ocean</span> <span class="hlt">wave</span> forecasting using computer-generated visualization and animation. This paper, Part 1, addresses forecasting of sea <span class="hlt">wave</span> conditions and serves as the basis for the more difficult topic of swell <span class="hlt">wave</span> forecasting addressed in Part 2. Computer-aided visualization and animation, accompanied by oral explanation, are a welcome pedagogical supplement to more traditional methods of instruction. In this article, several MATLAB ® software programs have been written to visualize and animate development and comparison of <span class="hlt">wave</span> spectra, <span class="hlt">wave</span> interference, and forecasting of sea conditions. These programs also set the stage for the more advanced and difficult animation topics in Part 2. The programs are user-friendly, interactive, easy to modify, and developed as instructional tools. By using these software programs, teachers can enhance their instruction of these topics with colorful visualizations and animation without requiring an extensive background in computer programming.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1013723','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1013723"><span><span class="hlt">Wave</span>-Ice interaction in the Marginal Ice Zone: Toward a <span class="hlt">Wave-Ocean</span>-Ice Coupled Modeling System</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>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. <span class="hlt">Wave</span>- Ice interaction in the Marginal Ice Zone: Toward a...<span class="hlt">Wave-Ocean</span>- Ice Coupled Modeling System W. E. Rogers Naval Research Laboratory, Code 7322 Stennis Space Center, MS 39529 phone: (228) 688-4727</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1201553-simulation-asteroid-impact-ocean-surfaces-subsequent-wave-generation-effect-us-shorelines','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1201553-simulation-asteroid-impact-ocean-surfaces-subsequent-wave-generation-effect-us-shorelines"><span>Simulation of asteroid impact on <span class="hlt">ocean</span> surfaces, subsequent <span class="hlt">wave</span> generation and the effect on US shorelines</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Ezzedine, Souheil M.; Lomov, Ilya; Miller, Paul L.; ...</p> <p>2015-05-19</p> <p>As part of a larger effort involving members of several other organizations, we have conducted numerical simulations in support of emergency-response exercises of postulated asteroid <span class="hlt">ocean</span> impacts. We have addressed the problem from source (asteroid entry) to <span class="hlt">ocean</span> impact (splash) to <span class="hlt">wave</span> generation, propagation and interaction with the U.S. shoreline. We simulated three impact sites. The first site is located off the east coast by Maryland's shoreline. The second site is located off of the West coast, the San Francisco bay. The third set of sites are situated in the Gulf of Mexico. Asteroid impacts on the <span class="hlt">ocean</span> surface aremore » conducted using LLNL's hydrocode GEODYN to create the impact <span class="hlt">wave</span> source for the shallow water <span class="hlt">wave</span> propagation code, SWWP, a shallow depth averaged water <span class="hlt">wave</span> code.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1201553','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1201553"><span>Simulation of asteroid impact on <span class="hlt">ocean</span> surfaces, subsequent <span class="hlt">wave</span> generation and the effect on US shorelines</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>Ezzedine, Souheil M.; Lomov, Ilya; Miller, Paul L.</p> <p></p> <p>As part of a larger effort involving members of several other organizations, we have conducted numerical simulations in support of emergency-response exercises of postulated asteroid <span class="hlt">ocean</span> impacts. We have addressed the problem from source (asteroid entry) to <span class="hlt">ocean</span> impact (splash) to <span class="hlt">wave</span> generation, propagation and interaction with the U.S. shoreline. We simulated three impact sites. The first site is located off the east coast by Maryland's shoreline. The second site is located off of the West coast, the San Francisco bay. The third set of sites are situated in the Gulf of Mexico. Asteroid impacts on the <span class="hlt">ocean</span> surface aremore » conducted using LLNL's hydrocode GEODYN to create the impact <span class="hlt">wave</span> source for the shallow water <span class="hlt">wave</span> propagation code, SWWP, a shallow depth averaged water <span class="hlt">wave</span> code.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010AGUFMOS51B1311F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010AGUFMOS51B1311F"><span>A unified spectral,parameterization for <span class="hlt">wave</span> breaking: from the deep <span class="hlt">ocean</span> to the surf zone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Filipot, J.</p> <p>2010-12-01</p> <p>A new <span class="hlt">wave</span>-breaking dissipation parameterization designed for spectral <span class="hlt">wave</span> models is presented. It combines <span class="hlt">wave</span> breaking basic physical quantities, namely, the breaking probability and the dissipation rate per unit area. The energy lost by <span class="hlt">waves</span> is fi[|#12#|]rst calculated in the physical space before being distributed over the relevant spectral components. This parameterization allows a seamless numerical model from the deep <span class="hlt">ocean</span> into the surf zone. This transition from deep to shallow water is made possible by a dissipation rate per unit area of breaking <span class="hlt">waves</span> that varies with the <span class="hlt">wave</span> height, wavelength and water depth.The parameterization is further tested in the WAVEWATCH III TM code, from the global <span class="hlt">ocean</span> to the beach scale. Model errors are smaller than with most specialized deep or shallow water parameterizations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFM.A14C..04C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFM.A14C..04C"><span>Atmosphere-<span class="hlt">Wave-Ocean</span> Coupling from Regional to Global Earth System Models for High-Impact Extreme Weather Prediction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, S. S.; Curcic, M.</p> <p>2017-12-01</p> <p>The need for acurrate and integrated impact forecasts of extreme wind, rain, <span class="hlt">waves</span>, 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-<span class="hlt">wave-ocean</span> 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, <span class="hlt">ocean</span> <span class="hlt">waves</span> and currents forecasts for forcing for storm surge. The Unified <span class="hlt">Wave</span> INterface (UWIN) has been developed for coupling of the atmosphere-<span class="hlt">wave-ocean</span> models. UWIN couples the atmosphere, <span class="hlt">wave</span>, and <span class="hlt">ocean</span> 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-<span class="hlt">wave-ocean</span> model predictions of hurricanes and coastal winter storms, and 2) implenmentation of UWIN in the NASA GMAO GEOS-5.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2002CG.....28..547W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2002CG.....28..547W"><span>Teaching <span class="hlt">ocean</span> <span class="hlt">wave</span> forecasting using computer-generated visualization and animation—Part 2: swell forecasting</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Whitford, Dennis J.</p> <p>2002-05-01</p> <p>This paper, the second of a two-part series, introduces undergraduate students to <span class="hlt">ocean</span> <span class="hlt">wave</span> forecasting using interactive computer-generated visualization and animation. Verbal descriptions and two-dimensional illustrations are often insufficient for student comprehension. Fortunately, the introduction of computers in the geosciences provides a tool for addressing this problem. Computer-generated visualization and animation, accompanied by oral explanation, have been shown to be a pedagogical improvement to more traditional methods of instruction. Cartographic science and other disciplines using geographical information systems have been especially aggressive in pioneering the use of visualization and animation, whereas oceanography has not. This paper will focus on the teaching of <span class="hlt">ocean</span> swell <span class="hlt">wave</span> forecasting, often considered a difficult oceanographic topic due to the mathematics and physics required, as well as its interdependence on time and space. Several MATLAB ® software programs are described and offered to visualize and animate group speed, frequency dispersion, angular dispersion, propagation, and <span class="hlt">wave</span> height forecasting of deep water <span class="hlt">ocean</span> swell <span class="hlt">waves</span>. Teachers may use these interactive visualizations and animations without requiring an extensive background in computer programming.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1184169-location-high-frequency-wave-microseismic-noise-pacific-ocean-using-multiple-small-aperture-arrays','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1184169-location-high-frequency-wave-microseismic-noise-pacific-ocean-using-multiple-small-aperture-arrays"><span>Location of high-frequency P <span class="hlt">wave</span> microseismic noise in the Pacific <span class="hlt">Ocean</span> using multiple small aperture arrays</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Pyle, Moira L.; Koper, Keith D.; Euler, Garrett G.; ...</p> <p>2015-04-20</p> <p>We investigate source locations of P-<span class="hlt">wave</span> microseisms within a narrow frequency band (0.67–1.33 Hz) that is significantly higher than the classic microseism band (~0.05–0.3 Hz). Employing a backprojection method, we analyze data recorded during January 2010 from five International Monitoring System arrays that border the Pacific <span class="hlt">Ocean</span>. We develop a ranking scheme that allows us to combine beam <span class="hlt">power</span> from multiple arrays to obtain robust locations of the microseisms. Some individual arrays exhibit a strong regional component, but results from the combination of all arrays show high-frequency P <span class="hlt">wave</span> energy emanating from the North Pacific basin, in general agreement withmore » previous observations in the double-frequency (DF) microseism band (~0.1–0.3 Hz). This suggests that the North Pacific source of ambient P noise covers a broad range of frequencies and that the <span class="hlt">wave-wave</span> interaction model is likely valid at shorter periods.« 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_7");'>7</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li class="active"><span>9</span></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_9 --> <div id="page_10" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="181"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017E%26ES...73a2010R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017E%26ES...73a2010R"><span>Model Predictive Control-based <span class="hlt">Power</span> take-off Control of an Oscillating Water Column <span class="hlt">Wave</span> Energy Conversion System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rajapakse, G.; Jayasinghe, S. G.; Fleming, A.; Shahnia, F.</p> <p>2017-07-01</p> <p>Australia’s extended coastline asserts abundance of <span class="hlt">wave</span> and tidal <span class="hlt">power</span>. The predictability of these energy sources and their proximity to cities and towns make them more desirable. Several tidal current turbine and <span class="hlt">ocean</span> <span class="hlt">wave</span> energy conversion projects have already been planned in the coastline of southern Australia. Some of these projects use air turbine technology with air driven turbines to harvest the energy from an oscillating water column. This study focuses on the <span class="hlt">power</span> take-off control of a single stage unidirectional oscillating water column air turbine generator system, and proposes a model predictive control-based speed controller for the generator-turbine assembly. The proposed method is verified with simulation results that show the efficacy of the controller in extracting <span class="hlt">power</span> from the turbine while maintaining the speed at the desired level.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014PhDT.......276H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014PhDT.......276H"><span>Investigation on the possibility of extracting <span class="hlt">wave</span> energy from the Texas coast</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Haces-Fernandez, Francisco</p> <p></p> <p>Due to the great and growing demand of energy consumption in the Texas Coast area, the generation of electricity from <span class="hlt">ocean</span> <span class="hlt">waves</span> is considered very important. The combination of the <span class="hlt">wave</span> energy with offshore wind <span class="hlt">power</span> is explored as a way to increase <span class="hlt">power</span> output, obtain synergies, maximize the utilization of assigned marine zones and reduce variability. Previously literature has assessed the <span class="hlt">wave</span> energy generation, combined with wind in different geographic locations such as California, Ireland and the Azores Island. In this research project, the electric <span class="hlt">power</span> generation from <span class="hlt">ocean</span> <span class="hlt">waves</span> on the Texas Coast was investigated, assessing its potential from the meteorological data provided by five buoys from National Data Buoy Center of the National <span class="hlt">Oceanic</span> and Atmospheric Administration, considering the Pelamis 750 kW <span class="hlt">Wave</span> Energy Converter (WEC) and the Vesta V90 3 MW Wind Turbine. The <span class="hlt">power</span> output from <span class="hlt">wave</span> energy was calculated for the year 2006 using Matlab, and the results in several locations were considered acceptable in terms of total <span class="hlt">power</span> output, but with a high temporal variability. To reduce its variability, <span class="hlt">wave</span> energy was combined with wind energy, obtaining a significant reduction on the coefficient of variation on the <span class="hlt">power</span> output. A Matlab based interface was created to calculate <span class="hlt">power</span> output and its variability considering data from longer periods of time.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA601654','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA601654"><span>Proving and Improving <span class="hlt">Wave</span> Models in the Arctic <span class="hlt">Ocean</span> and its MIZ</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><span class="hlt">wave</span> buoy was deployed in the <span class="hlt">ocean</span> near the berg throughout the experiment, and recorded a persistent swell from the SE. An array of tiltmeters and GPS...vertical movement sensors was placed on the berg near the edge. These recorded the berg response to the <span class="hlt">waves</span>, and on one occasion a calving event</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/17813707','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/17813707"><span><span class="hlt">Ocean</span> thermal gradient hydraulic <span class="hlt">power</span> plant.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Beck, E J</p> <p>1975-07-25</p> <p>Solar energy stored in the <span class="hlt">oceans</span> may be used to generate <span class="hlt">power</span> by exploiting ploiting thermal gradients. A proposed open-cycle system uses low-pressure steam to elevate vate water, which is then run through a hydraulic turbine to generate <span class="hlt">power</span>. The device is analogous to an air lift pump.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMOS53D..08P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMOS53D..08P"><span>The Future Potential of <span class="hlt">Wave</span> <span class="hlt">Power</span> in the US</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Previsic, M.; Epler, J.; Hand, M.; Heimiller, D.; Short, W.; Eurek, K.</p> <p>2012-12-01</p> <p>The theoretical <span class="hlt">ocean</span> <span class="hlt">wave</span> energy resource potential exceeds 50% of the annual domestic energy demand of the US, is located in close proximity of coastal population centers, and, although variable in nature, may be more consistent and predictable than some other renewable generation technologies. As renewable electricity generation technologies, <span class="hlt">ocean</span> <span class="hlt">wave</span> energy offers a low air pollutant option for diversifying the US electricity generation portfolio. Furthermore, the output characteristics of these technologies may complement other renewable technologies. This study addresses: (1) The energy extraction potential from the US <span class="hlt">wave</span> energy resource, (2) The present cost of <span class="hlt">wave</span> technology in /kW, (3) The estimated cost of energy in /kWh, and (4) Cost levels at which the technology should see significant deployment. RE Vision Consulting in collaboration with NREL engaged in various analyses to establish present-day and future cost profiles for MHK technologies, compiled existing resource assessments and <span class="hlt">wave</span> energy supply curves, and developed cost and deployment scenarios using the ReEDS analysis model to estimate the present-day technology cost reductions necessary to facilitate significant technology deployment in the US.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1980PhDT.......108P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1980PhDT.......108P"><span>O Electromagnetic <span class="hlt">Power</span> <span class="hlt">Waves</span> and <span class="hlt">Power</span> Density Components.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Petzold, Donald Wayne</p> <p>1980-12-01</p> <p>On January 10, 1884 Lord Rayleigh presented a paper entitled "On the Transfer of Energy in the Electromagnetic Field" to the Royal Society of London. This paper had been authored by the late Fellow of Trinity College, Cambridge, Professor J. H. Poynting and in it he claimed that there was a general law for the transfer of electromagnetic energy. He argued that associated with each point in space is a quantity, that has since been called the Poynting vector, that is a measure of the rate of energy flow per unit area. His analysis was concerned with the integration of this <span class="hlt">power</span> density vector at all points over an enclosing surface of a specific volume. The interpretation of this Poynting vector as a true measure of the local <span class="hlt">power</span> density was viewed with great skepticism unless the vector was integrated over a closed surface, as the development of the concept required. However, within the last decade or so Shadowitz indicates that a number of prominent authors have argued that the criticism of the interpretation of Poynting's vector as a local <span class="hlt">power</span> density vector is unjustified. The present paper is not concerned with these arguments but instead is concerned with a decomposition of Poynting's <span class="hlt">power</span> density vector into two and only two components: one vector which has the same direction as Poynting's vector and which is called the forward <span class="hlt">power</span> density vector, and another vector, directed opposite to the Poynting vector and called the reverse <span class="hlt">power</span> density vector. These new local forward and reverse <span class="hlt">power</span> density vectors will be shown to be dependent upon forward and reverse <span class="hlt">power</span> <span class="hlt">wave</span> vectors and these vectors in turn will be related to newly defined forward and reverse components of the electric and magnetic fields. The sum of these forward and reverse <span class="hlt">power</span> density vectors, which is simply the original Poynting vector, is associated with the total electromagnetic energy traveling past the local point. Another vector which is the difference between the forward</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000083900&hterms=3D+animation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3D3D%2Banimation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000083900&hterms=3D+animation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3D3D%2Banimation"><span>Hurricane Directional <span class="hlt">Wave</span> Spectrum Spatial Variation in the Open <span class="hlt">Ocean</span> and at Landfall</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Walsh, Edward J.; Wright, C. Wayne; Vandemark, Douglas C.; Krabill, William B.; Garcia, Andrew W.; Houston, Samuel H.; Powell, Mark D.; Black, Peter G.; Marks, Frank D.</p> <p>2000-01-01</p> <p>The sea surface directional <span class="hlt">wave</span> spectrum was measured for the first time in all quadrants of a hurricane in open water using the NASA airborne scanning radar altimeter (SRA) carried aboard one of the NOAA WP-3D hurricane hunter aircraft at 1.5 km height. The SRA measures the energetic portion of the directional <span class="hlt">wave</span> spectrum by generating a topographic map of the sea surface. At 8 Hz, the SRA sweeps a radar beam of 1' half-<span class="hlt">power</span> width (two-way) across the aircraft ground track over a swath equal to 0.8 of the aircraft height, simultaneously measuring the backscattered <span class="hlt">power</span> at its 36 GHz (8.3 mm) operating frequency and the range to the sea surface at 64 positions. These slant ranges are multiplied by the cosine of the off-nadir angles to determine the vertical distances from the aircraft to the sea surface. Subtracting these distances from the aircraft height produces the sea surface elevation map. The sea surface topography is interpolated to a uniform grid, transformed by a two dimensional FFT, and Doppler corrected. The open-<span class="hlt">ocean</span> data were acquired on 24 August 1998 when hurricane Bonnie was east of the Bahamas and moving toward 330 deg at about 5 m/s. Individual <span class="hlt">waves</span> up to 18 m height were observed and the spatial variation of the <span class="hlt">wave</span> field was dramatic. The dominant <span class="hlt">waves</span> generally propagated at significant angles to the downwind direction. At some positions there were three different <span class="hlt">wave</span> fields of comparable energy crossing each other. The NOAA aircraft spent over five hours within 180 km of the eye, and made five eye penetrations. On 26 August 1998, the NOAA aircraft flew at 2.2 km height when hurricane Bonnie was making landfall near Wilmington, NC, documenting the directional <span class="hlt">wave</span> spectrum in the region between Charleston, SC and Cape Hatteras, NC. The aircraft flight lines included segments near and along the shoreline as well as far offshore. Animations of the directional <span class="hlt">wave</span> spectrum spatial variation along the aircraft tracks on the two flights</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/12736682','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/12736682"><span>Redistribution of energy available for <span class="hlt">ocean</span> mixing by long-range propagation 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>Alford, Matthew H</p> <p>2003-05-08</p> <p><span class="hlt">Ocean</span> mixing, which affects pollutant dispersal, marine productivity and global climate, largely results from the breaking of internal gravity <span class="hlt">waves</span>--disturbances propagating along the <span class="hlt">ocean</span>'s internal stratification. A global map of internal-<span class="hlt">wave</span> dissipation would be useful in improving climate models, but would require knowledge of the sources of internal gravity <span class="hlt">waves</span> and their propagation. Towards this goal, I present here computations of horizontal internal-<span class="hlt">wave</span> propagation from 60 historical moorings and relate them to the source terms of internal <span class="hlt">waves</span> as computed previously. Analysis of the two most energetic frequency ranges--near-inertial frequencies and semidiurnal tidal frequencies--reveals that the fluxes in both frequency bands are of the order of 1 kW x m(-1) (that is, 15-50% of the energy input) and are directed away from their respective source regions. However, the energy flux due to near-inertial <span class="hlt">waves</span> is stronger in winter, whereas the tidal fluxes are uniform throughout the year. Both varieties of internal <span class="hlt">waves</span> can thus significantly affect the space-time distribution of energy available for global mixing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRF..122..153A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRF..122..153A"><span>Links between atmosphere, <span class="hlt">ocean</span>, and cryosphere from two decades of microseism observations on the Antarctic Peninsula</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anthony, Robert E.; Aster, Richard C.; McGrath, Daniel</p> <p>2017-01-01</p> <p>The lack of landmasses, climatological low pressure, and strong circumpolar westerly winds between the latitudes of 50°S to 65°S produce exceptional storm-driven <span class="hlt">wave</span> conditions in the Southern <span class="hlt">Ocean</span>. This combination makes the Antarctic Peninsula one of Earth's most notable regions of high-amplitude <span class="hlt">wave</span> activity and thus, <span class="hlt">ocean</span>-swell-driven microseism noise in both the primary (direct <span class="hlt">wave</span>-coastal region interactions) and secondary (direct <span class="hlt">ocean</span> floor forcing due to interacting <span class="hlt">wave</span> trains) period bands. Microseism observations are examined across 23 years (1993-2015) from Palmer Station (PMSA), on the west coast of the Antarctic Peninsula, and from East Falkland Island (EFI). These records provide a spatially integrative measure of both Southern <span class="hlt">Ocean</span> <span class="hlt">wave</span> amplitudes and the interactions between <span class="hlt">ocean</span> <span class="hlt">waves</span> and the solid Earth in the presence of sea ice, which can reduce <span class="hlt">wave</span> coupling with the continental shelf. We utilize a spatiotemporal correlation-based approach to illuminate how the distribution of sea ice influences seasonal microseism <span class="hlt">power</span>. We characterize primary and secondary microseism <span class="hlt">power</span> due to variations in sea ice and find that primary microseism energy is both more sensitive to sea ice and more capable of propagating across <span class="hlt">ocean</span> basins than secondary microseism energy. During positive phases of the Southern Annular Mode, sea ice is reduced in the Bellingshausen Sea and overall storm activity in the Drake Passage increases, thus strongly increasing microseism <span class="hlt">power</span> levels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780016832','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780016832"><span>Verification results for the Spectral <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Model (SOWM) by means of significant <span class="hlt">wave</span> height measurements made by the GEOS-3 spacecraft</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Pierson, W. J.; Salfi, R. E.</p> <p>1978-01-01</p> <p>Significant <span class="hlt">wave</span> heights estimated from the shape of the return pulse <span class="hlt">wave</span> form of the altimeter on GEOS-3 for forty-four orbit segments obtained during 1975 and 1976 are compared with the significant <span class="hlt">wave</span> heights specified by the spectral <span class="hlt">ocean</span> <span class="hlt">wave</span> model (SOWM), which is the presently operational numerical <span class="hlt">wave</span> forecasting model at the Fleet Numerical Weather Central. Except for a number of orbit segments with poor agreement and larger errors, the SOWM specifications tended to be biased from 0.5 to 1.0 meters too low and to have RMS errors of 1.0 to 1.4 meters. The much fewer larger errors can be attributed to poor wind data for some parts of the Northern Hemisphere <span class="hlt">oceans</span>. The bias can be attributed to the somewhat too light winds used to generate the <span class="hlt">waves</span> in the model. Other sources of error are identified in the equatorial and trade wind areas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012JGRC..117.0J08F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012JGRC..117.0J08F"><span>A unified spectral parameterization for <span class="hlt">wave</span> breaking: From the deep <span class="hlt">ocean</span> to the surf zone</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Filipot, J.-F.; Ardhuin, F.</p> <p>2012-11-01</p> <p>A new <span class="hlt">wave</span>-breaking dissipation parameterization designed for phase-averaged spectral <span class="hlt">wave</span> models is presented. It combines <span class="hlt">wave</span> breaking basic physical quantities, namely, the breaking probability and the dissipation rate per unit area. The energy lost by <span class="hlt">waves</span> is first explicitly calculated in physical space before being distributed over the relevant spectral components. The transition from deep to shallow water is made possible by using a dissipation rate per unit area of breaking <span class="hlt">waves</span> that varies with the <span class="hlt">wave</span> height, wavelength and water depth. This parameterization is implemented in the WAVEWATCH III modeling framework, which is applied to a wide range of conditions and scales, from the global <span class="hlt">ocean</span> to the beach scale. <span class="hlt">Wave</span> height, peak and mean periods, and spectral data are validated using in situ and remote sensing data. Model errors are comparable to those of other specialized deep or shallow water parameterizations. This work shows that it is possible to have a seamless parameterization from the deep <span class="hlt">ocean</span> to the surf zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015OcMod..92..149P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015OcMod..92..149P"><span>Spectral <span class="hlt">wave</span> conditions in the Colombian Pacific <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Portilla, Jesús; Caicedo, Ana Lucía; Padilla-Hernández, Roberto; Cavaleri, Luigi</p> <p>2015-08-01</p> <p>A comprehensive characterization of the <span class="hlt">wave</span> conditions in the Colombian Pacific based on <span class="hlt">wave</span> spectra is presented. The spectral approach offers a detailed description of the different <span class="hlt">wave</span> regimes, their associated meteorological conditions and their variation in time and geographical space. To this end, two complementary data sources are used, the first is representative for the near-shore zone and comes from observations of the local monitoring network. The second comes from numerical <span class="hlt">wave</span> model results that cover the open <span class="hlt">ocean</span>. The measured data used are the first systematically collected spectral <span class="hlt">wave</span> data in the Eastern Equatorial Pacific. Modelled spectra correspond to the ERA-Interim database of the European Centre for Medium-Range Weather Forecasts that spans 35 years. An indicator for statistical analysis of the <span class="hlt">wave</span> spectra has been introduced which basically consists of the occurrence probability of spectral partitions. This indicator has proved to be skilful for the task of defining spectral <span class="hlt">wave</span> systems of both model and, the more challenging, measured spectra. Following the spectral approach and using this new indicator, six main <span class="hlt">wave</span> regimes are found in the study area. Two of these systems have well defined swell characteristics that are originated outside the study area in the northern and southern hemispheres. Other three <span class="hlt">wave</span> systems are to a certain extent associated to the local winds, and in general may be classified as old wind-seas. These are found to flow northeastwards, westwards, and southwards. The sixth system is composed of locally generated wind <span class="hlt">waves</span> of relatively low magnitude that propagate in several directions. The time variability of these <span class="hlt">wave</span> systems is highly dependent on the boreal and austral winter storms and on the tropical conditions, in such a way that the <span class="hlt">wave</span> energy propagation to the region is rather constant along the year, but their origin and characteristics vary significantly.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFD.A5004C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFD.A5004C"><span>Observations of Equatorial Kelvin <span class="hlt">Waves</span> and their Convective Coupling with the Atmosphere/<span class="hlt">Ocean</span> Surface Layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Conry, Patrick; Fernando, H. J. S.; Leo, Laura; Blomquist, Byron; Amelie, Vincent; Lalande, Nelson; Creegan, Ed; Hocut, Chris; MacCall, Ben; Wang, Yansen; Jinadasa, S. U. P.; Wang, Chien; Yeo, Lik-Khian</p> <p>2016-11-01</p> <p>Intraseasonal disturbances with their genesis in the equatorial Indian <span class="hlt">Ocean</span> (IO) are an important component of global climate. The disturbances, which include Madden-Julian Oscillation and equatorial Kelvin and Rossby <span class="hlt">waves</span> in the atmosphere and <span class="hlt">ocean</span>, carry energy which affects El Niño, cyclogenesis, and monsoons. A recent field experiment in IO (ASIRI-RAWI) observed disturbances at three sites across IO with arrays of instruments probing from surface layer to lower stratosphere. During the field campaign the most pronounced planetary-scale disturbances were Kelvin <span class="hlt">waves</span> in tropical tropopause layer. In Seychelles, quasi-biweekly westerly wind bursts were documented and linked to the Kelvin <span class="hlt">waves</span> aloft, which breakdown in the upper troposphere due to internal shear instabilities. Convective coupling between <span class="hlt">waves</span>' phase in upper troposphere and surface initiates rapid (turbulent) vertical transport and resultant wind bursts at surface. Such phenomena reveal linkages between planetary-scale <span class="hlt">waves</span> and small-scale turbulence in the surface layer that can affect air-sea property exchanges and should be parameterized in atmosphere-<span class="hlt">ocean</span> general circulation models. Funded by ONR Grants N00014-14-1-0279 and N00014-13-1-0199.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.4821N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.4821N"><span><span class="hlt">Wave</span>-current interactions at the Flo<span class="hlt">Wave</span> <span class="hlt">Ocean</span> Energy Research Facility</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Noble, Donald; Davey, Thomas; Steynor, Jeffrey; Bruce, Tom; Smith, Helen; Kaklis, Panagiotis</p> <p>2015-04-01</p> <p>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. Flo<span class="hlt">Wave</span> is a new state-of-the-art <span class="hlt">ocean</span> energy research facility, designed to provide large scale physical modelling services to the tidal and <span class="hlt">wave</span> sector. It has the unique ability to provide complex multi-directional <span class="hlt">waves</span> that can be combined with currents from any direction in the 25m diameter circular tank. The facility is optimised for <span class="hlt">waves</span> 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 <span class="hlt">waves</span> of interest, thus the full dispersion equation must be solved as the asymptotic simplifications do not apply. The interaction between <span class="hlt">waves</span> and currents has been studied in the tank. This has involved producing in the tank sets of regular <span class="hlt">waves</span>, focussed <span class="hlt">wave</span> groups, and random sea spectra including multi-directional sea states. These <span class="hlt">waves</span> have been both inline-with and opposing the current, as well as investigating <span class="hlt">waves</span> at arbitrary angles to the current. Changes in <span class="hlt">wave</span> height and wavelength have been measured, and compared with theoretical results. Using theoretical <span class="hlt">wave</span>-current interaction models, methods have been explored to "correct" the <span class="hlt">wave</span> height in the central test area of the tank when combined with a steady current. This allows the <span class="hlt">wave</span> 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 <span class="hlt">wave</span> height and current combination to be produced in the tank, reproducing recorded conditions at a particular site of interest. The</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1919141S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1919141S"><span><span class="hlt">Wave</span> resource variability: Impacts on <span class="hlt">wave</span> <span class="hlt">power</span> supply over regional to international scales</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, Helen; Fairley, Iain; Robertson, Bryson; Abusara, Mohammad; Masters, Ian</p> <p>2017-04-01</p> <p>The intermittent, irregular and variable nature of the <span class="hlt">wave</span> energy resource has implications for the supply of <span class="hlt">wave</span>-generated electricity into the grid. Intermittency of renewable <span class="hlt">power</span> may lead to frequency and voltage fluctuations in the transmission and distribution networks. A matching supply of electricity must be planned to meet the predicted demand, leading to a need for gas-fired and back-up generating plants to supplement intermittent supplies, and potentially limiting the integration of intermittent <span class="hlt">power</span> into the grid. Issues relating to resource intermittency and their mitigation through the development of spatially separated sites have been widely researched in the wind industry, but have received little attention to date in the less mature <span class="hlt">wave</span> industry. This study analyses the <span class="hlt">wave</span> resource over three different spatial scales to investigate the potential impacts of the temporal and spatial resource variability on the grid supply. The primary focus is the Southwest UK, a region already home to multiple existing and proposed <span class="hlt">wave</span> energy test sites. Concurrent <span class="hlt">wave</span> buoy data from six locations, supported by SWAN <span class="hlt">wave</span> model hindcast data, are analysed to assess the correlation of the resource across the region and the variation in <span class="hlt">wave</span> <span class="hlt">power</span> with direction. <span class="hlt">Power</span> matrices for theoretical nearshore and offshore devices are used to calculate the maximum step change in generated <span class="hlt">power</span> across the region as the number of deployment sites is increased. The step change analysis is also applied across national and international spatial scales using output from the European Centre for Medium-range Weather Forecasting (ECMWF) ERA-Interim hindcast model. It is found that the deployment of multiple <span class="hlt">wave</span> energy sites, whether on a regional, national or international scale, results in both a reduction in step changes in <span class="hlt">power</span> and reduced times of zero generation, leading to an overall smoothing of the <span class="hlt">wave</span>-generated electrical <span class="hlt">power</span>. This has implications for the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27731411','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27731411"><span><span class="hlt">Ocean</span> rogue <span class="hlt">waves</span> and their phase space dynamics in the limit of a linear interference model.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Birkholz, Simon; Brée, Carsten; Veselić, Ivan; Demircan, Ayhan; Steinmeyer, Günter</p> <p>2016-10-12</p> <p>We reanalyse the probability for formation of extreme <span class="hlt">waves</span> using the simple model of linear interference of a finite number of elementary <span class="hlt">waves</span> with fixed amplitude and random phase fluctuations. Under these model assumptions no rogue <span class="hlt">waves</span> appear when less than 10 elementary <span class="hlt">waves</span> interfere with each other. Above this threshold rogue <span class="hlt">wave</span> formation becomes increasingly likely, with appearance frequencies that may even exceed long-term observations by an order of magnitude. For estimation of the effective number of interfering <span class="hlt">waves</span>, we suggest the Grassberger-Procaccia dimensional analysis of individual time series. For the <span class="hlt">ocean</span> system, it is further shown that the resulting phase space dimension may vary, such that the threshold for rogue <span class="hlt">wave</span> formation is not always reached. Time series analysis as well as the appearance of particular focusing wind conditions may enable an effective forecast of such rogue-<span class="hlt">wave</span> prone situations. In particular, extracting the dimension from <span class="hlt">ocean</span> time series allows much more specific estimation of the rogue <span class="hlt">wave</span> probability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5059714','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5059714"><span><span class="hlt">Ocean</span> rogue <span class="hlt">waves</span> and their phase space dynamics in the limit of a linear interference model</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Birkholz, Simon; Brée, Carsten; Veselić, Ivan; Demircan, Ayhan; Steinmeyer, Günter</p> <p>2016-01-01</p> <p>We reanalyse the probability for formation of extreme <span class="hlt">waves</span> using the simple model of linear interference of a finite number of elementary <span class="hlt">waves</span> with fixed amplitude and random phase fluctuations. Under these model assumptions no rogue <span class="hlt">waves</span> appear when less than 10 elementary <span class="hlt">waves</span> interfere with each other. Above this threshold rogue <span class="hlt">wave</span> formation becomes increasingly likely, with appearance frequencies that may even exceed long-term observations by an order of magnitude. For estimation of the effective number of interfering <span class="hlt">waves</span>, we suggest the Grassberger-Procaccia dimensional analysis of individual time series. For the <span class="hlt">ocean</span> system, it is further shown that the resulting phase space dimension may vary, such that the threshold for rogue <span class="hlt">wave</span> formation is not always reached. Time series analysis as well as the appearance of particular focusing wind conditions may enable an effective forecast of such rogue-<span class="hlt">wave</span> prone situations. In particular, extracting the dimension from <span class="hlt">ocean</span> time series allows much more specific estimation of the rogue <span class="hlt">wave</span> probability. PMID:27731411</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1999PhDT.......169M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1999PhDT.......169M"><span>Application of nonlinear deterministic decomposition to the prediction and energy dissipation of long-crested irregular <span class="hlt">ocean</span> 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>Meza Conde, Eustorgio</p> <p></p> <p>The Hybrid <span class="hlt">Wave</span> Model (HWM) is a deterministic nonlinear <span class="hlt">wave</span> model developed for the computation of <span class="hlt">wave</span> properties in the vicinity of <span class="hlt">ocean</span> <span class="hlt">wave</span> measurements. The HWM employs both Mode-Coupling and Phase Modulation Methods to model the <span class="hlt">wave-wave</span> interactions in an <span class="hlt">ocean</span> <span class="hlt">wave</span> field. Different from other nonlinear <span class="hlt">wave</span> models, the HWM decouples the nonlinear <span class="hlt">wave</span> interactions from <span class="hlt">ocean</span> <span class="hlt">wave</span> field measurements and decomposes the <span class="hlt">wave</span> field into a set of free-<span class="hlt">wave</span> components. In this dissertation the HWM is applied to the prediction of <span class="hlt">wave</span> elevation from pressure measurements and to the quantification of energy during breaking of long-crested irregular surface <span class="hlt">waves</span>. 1.A transient <span class="hlt">wave</span> train was formed in a two-dimensional <span class="hlt">wave</span> flume by sequentially generating a series of <span class="hlt">waves</span> from high to low frequencies that superposed at a downstream location. The predicted <span class="hlt">wave</span> elevation using the HWM based on the pressure measurement of a very steep transient <span class="hlt">wave</span> train is in excellent agreement with the corresponding elevation measurement, while that using Linear <span class="hlt">Wave</span> Theory (LWT) has relatively large discrepancies. Furthermore, the predicted elevation using the HWM is not sensitive to the choice of the cutoff frequency, while that using LWT is very sensitive. 2.Several transient <span class="hlt">wave</span> trains containing an isolated plunging or spilling breaker at a prescribed location were generated in a two-dimensional <span class="hlt">wave</span> flume using the same superposition technique. Surface elevation measurements of each transient <span class="hlt">wave</span> train were made at locations before and after breaking. Applying the HWM nonlinear deterministic decomposition to the measured elevation, the free-<span class="hlt">wave</span> components comprising the transient <span class="hlt">wave</span> train were derived. By comparing the free-<span class="hlt">wave</span> spectra before and after breaking it is found that energy loss was almost exclusively from <span class="hlt">wave</span> components at frequencies higher than the spectral peak frequency. Even though the <span class="hlt">wave</span> components near the peak frequency are the largest</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSEC14E1052C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSEC14E1052C"><span>Spatio-temporal variability of internal <span class="hlt">waves</span> in the northern Gulf of Mexico studied with the Navy Coastal <span class="hlt">Ocean</span> Model, NCOM</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cambazoglu, M. K.; Jacobs, G. A.; Howden, S. D.; Book, J. W.; Arnone, R.; Soto Ramos, I. M.; Vandermeulen, R. A.; Greer, A. T.; Miles, T. N.</p> <p>2016-02-01</p> <p>Internal <span class="hlt">waves</span> enhance mixing in the upper <span class="hlt">ocean</span>, transport nutrients and plankton over the water column and across the shelf from deeper waters to shallower coastal areas, and could also transport pollutants such as hydrocarbons onshore during an oil spill event. This study aims to characterize internal <span class="hlt">waves</span> in the northern Gulf of Mexico (nGoM) and investigate the possible generation and dissipation mechanisms using a high-resolution (1-km) application of the Navy Coastal <span class="hlt">Ocean</span> Model (NCOM). Three dimensional model products are used to detect the propagation patterns of internal <span class="hlt">waves</span>. The vertical structure of internal <span class="hlt">waves</span> is studied and the role of stratification is analyzed by looking at the temperature, salinity and velocity variations along the water column. The model predictions suggest the generation of internal <span class="hlt">waves</span> on the continental shelf, therefore the role of <span class="hlt">ocean</span> bottom topography interacting with tides and general circulation features such as the Loop Current Eddy front, on the internal <span class="hlt">wave</span> generation will be discussed. The time periods of internal <span class="hlt">wave</span> occurrences are identified from model predictions and compared to satellite <span class="hlt">ocean</span> color imagery. Further data analysis, e.g. Fourier analysis, is implemented to determine internal wavelengths and frequencies and to determine if the response of internal <span class="hlt">waves</span> are at tidal periods or at different frequencies. The atmospheric forcing provided to NCOM and meteorological data records are analyzed to define the interaction between wind forcing and internal <span class="hlt">wave</span> generation. Wavelet analysis characterizes the <span class="hlt">ocean</span> response to atmospheric events with periodic frequencies. <span class="hlt">Ocean</span> color satellite imagery was used to visualize the location of the Mississippi river plume (and other <span class="hlt">oceanic</span> features) and compared to the model predictions because the enhanced stratification from freshwater plumes which propagate across the Mississippi Bight can provide favorable conditions in coastal waters for internal <span class="hlt">wave</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMED41A0240B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMED41A0240B"><span>Harnessing Alternative Energy Sources to Enhance the Design of a <span class="hlt">Wave</span> Generator</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bravo, A.</p> <p>2017-12-01</p> <p><span class="hlt">Wave</span> energy has the <span class="hlt">power</span> to replace a non-renewable source of electricity for a home near the <span class="hlt">ocean</span>. I built a small-scale <span class="hlt">wave</span> generator capable of producing approximately 5 volts of electricity. The generator is an array of 16 small generators, each consisting of 200 feet of copper wire, 12 magnets, and a buoy. I tested my design in the Pacific <span class="hlt">Ocean</span> and was able to <span class="hlt">power</span> a string of lights I had attached to the generator. While the <span class="hlt">waves</span> in the <span class="hlt">ocean</span> moved my buoys, my design was <span class="hlt">powered</span> by the vertical motion of the <span class="hlt">waves</span>. My generator was hit with significant horizontal <span class="hlt">wave</span> motion, and I realized I wasn't taking advantage of that direction of motion. To make my generator produce more electricity, I experimented with capturing the energy of the horizontal motion of water and incorporated that into my generator design. My generator, installed in the <span class="hlt">ocean</span>, is also exposed to sun and wind, and I am exploring the potential of solar and wind energy collection in my design to increase the electricity output. Once I have maximized my electricity output, I would like to explore scaling up my design.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_8");'>8</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li class="active"><span>10</span></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_10 --> <div id="page_11" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_9");'>9</a></li> <li><a href="#" onclick='return showDiv("page_10");'>10</a></li> <li class="active"><span>11</span></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="201"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..1413162C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..1413162C"><span>On the influence of <span class="hlt">ocean</span> <span class="hlt">waves</span> on simulated GNSS-R delay-doppler maps</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Clarizia, M. P.; di Bisceglie, M.; Galdi, C.; Gommenginger, C.; Srokosz, M.</p> <p>2012-04-01</p> <p>Global Navigation Satellite System-Reflectometry (GNSS-R), is an established technique that exploits GNSS signals of opportunity reflected from the surface of the <span class="hlt">ocean</span>, to look primarily at the <span class="hlt">ocean</span> surface roughness. The strength of this technique, and the primary motivation to carry it forward, is in the fact that GNSS signals are available globally, all the time and over the long term, and could help dramatically improve the monitoring of <span class="hlt">ocean</span> wind and <span class="hlt">waves</span>. GNSS-R offers the prospect of high density global measurements of directional sea surface roughness, which are essential for scientific purposes (i.e. quantifying the air-sea exchanges of gases), operational weather and <span class="hlt">ocean</span> forecasting (i.e. prediction of high winds, dangerous sea states, risk of flooding and storm surges) and to support important climate-relevant Earth Observation techniques (IR SST, or surface salinity retrieval). The retrieval of <span class="hlt">ocean</span> roughness from GNSS-R data has now been demonstrated with a reasonable level of accuracy from both airborne [1] and spaceborne [2] platforms. In both cases, Directional Mean Square Slopes (DMSS) of the <span class="hlt">ocean</span> surface have been retrieved from GNSS-R data, in the form of Delay-Doppler Maps (DDMs), using an established theoretical scattering model by Zavorotny and Voronovich (Z-V) [3]. The need for a better assessment of the way the <span class="hlt">ocean</span> <span class="hlt">waves</span> influence the scattering of GPS signals has recently led to a different approach, consisting of simulating the scattering of such signals, using a more sophisticated large-scale scattering model than Z-V, and explicit simulations of realistic seas. Initial results produced from these simulations have been recently published in [4], where the emphasis has been put on the effects of different sea states on Radar Cross Section (RCS) and Polarization Ratio (PR) in space domain. Linear wind <span class="hlt">wave</span> surfaces have been simulated using the Elfouhaily wind <span class="hlt">wave</span> spectrum [5], for different wind speeds and directions, and with</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090034242&hterms=sss&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsss','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090034242&hterms=sss&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dsss"><span>Detection of Rossby <span class="hlt">Waves</span> in Multi-Parameters in Multi-Mission Satellite Observations and HYCOM Simulations in the Indian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Subrahmanyam, Bulusu; Heffner, David M.; Cromwell, David; Shriver, Jay F.</p> <p>2009-01-01</p> <p>Rossby <span class="hlt">waves</span> are difficult to detect with in situ methods. However, as we show in this paper, they can be clearly identified in multi-parameters in multi-mission satellite observations of sea surface height (SSH), sea surface temperature (SST) and <span class="hlt">ocean</span> color observations of chlorophyll-a (chl-a), as well as 1/12-deg global HYbrid Coordinate <span class="hlt">Ocean</span> Model (HYCOM) simulations of SSH, SST and sea surface salinity (SSS) in the Indian <span class="hlt">Ocean</span>. While the surface structure of Rossby <span class="hlt">waves</span> can be elucidated from comparisons of the signal in different sea surface parameters, models are needed to gain direct information about how these <span class="hlt">waves</span> affect the <span class="hlt">ocean</span> at depth. The first three baroclinic modes of the Rossby <span class="hlt">waves</span> are inferred from the Fast Fourier Transform (FFT), and two-dimensional Radon Transform (2D RT). At many latitudes the first and second baroclinic mode Rossby <span class="hlt">wave</span> phase speeds from satellite observations and model parameters are identified.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20170000013&hterms=tsunami&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtsunami','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20170000013&hterms=tsunami&qs=N%3D0%26Ntk%3DAll%26Ntx%3Dmode%2Bmatchall%26Ntt%3Dtsunami"><span>Tsunami <span class="hlt">Waves</span> Extensively Resurfaced the Shorelines of an Early Martian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Rodriguez, J. A. P.; Fairen, A. G.; Linares, R.; Zarroca, M.; Platz, T.; Komatsu, G.; Kargel, J. S.; Gulick, V.; Jianguo, Y.; Higuchi, K.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20170000013'); toggleEditAbsImage('author_20170000013_show'); toggleEditAbsImage('author_20170000013_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20170000013_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20170000013_hide"></p> <p>2016-01-01</p> <p>Viking image-based mapping of a widespread deposit covering most of the northern low-lands of Mars led to the proposal by Parker et al. that the deposit represents the vestiges of an enormous <span class="hlt">ocean</span> that existed approx. 3.4 Ga. Later identified as the Vastitas Borealis Formation, the latest geologic map of Mars identifies this deposit as the Late Hesperian lowland unit (lHl). This deposit is typically bounded by raised lobate margins. In addition, some margins have associated rille channels, which could have been produced sub-aerially by the back-wash of high-energy tsunami <span class="hlt">waves</span>. Radar-sounding data indicate that the deposit is ice-rich. However, until now, the lack of <span class="hlt">wave</span>-cut shoreline features and the presence of lobate margins have remained an im-pediment to the acceptance of the paleo-<span class="hlt">ocean</span> hypothesis.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70000147','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70000147"><span><span class="hlt">Ocean</span> wavenumber estimation from <span class="hlt">wave</span>-resolving time series imagery</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Plant, N.G.; Holland, K.T.; Haller, M.C.</p> <p>2008-01-01</p> <p>We review several approaches that have been used to estimate <span class="hlt">ocean</span> surface gravity wavenumbers from <span class="hlt">wave</span>-resolving remotely sensed image sequences. Two fundamentally different approaches that utilize these data exist. A <span class="hlt">power</span> spectral density approach identifies wavenumbers where image intensity variance is maximized. Alternatively, a cross-spectral correlation approach identifies wavenumbers where intensity coherence is maximized. We develop a solution to the latter approach based on a tomographic analysis that utilizes a nonlinear inverse method. The solution is tolerant to noise and other forms of sampling deficiency and can be applied to arbitrary sampling patterns, as well as to full-frame imagery. The solution includes error predictions that can be used for data retrieval quality control and for evaluating sample designs. A quantitative analysis of the intrinsic resolution of the method indicates that the cross-spectral correlation fitting improves resolution by a factor of about ten times as compared to the <span class="hlt">power</span> spectral density fitting approach. The resolution analysis also provides a rule of thumb for nearshore bathymetry retrievals-short-scale cross-shore patterns may be resolved if they are about ten times longer than the average water depth over the pattern. This guidance can be applied to sample design to constrain both the sensor array (image resolution) and the analysis array (tomographic resolution). ?? 2008 IEEE.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998JGR...10318649L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998JGR...10318649L"><span>Effects of subsurface <span class="hlt">ocean</span> dynamics on instability <span class="hlt">waves</span> in 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>Lawrence, Sean P.; Allen, Myles R.; Anderson, David L. T.; Llewellyn-Jones, David T.</p> <p>1998-08-01</p> <p>Tropical instability <span class="hlt">waves</span> in a primitive equation model of the tropical Pacific <span class="hlt">Ocean</span>, forced with analyzed wind stresses updated daily, show unexpectedly close phase correspondence with observation through the latter half of 1992. This suggests that these <span class="hlt">waves</span> are not pure instabilities developing from infinitesimal disturbances, but that their phases and phase speeds are at least partially determined by the wind stress forcing. To quantify and explain this observation, we perfomed several numerical experiments, which indicate that remotely forced Rossby <span class="hlt">waves</span> can influence both the phase and phase speed of tropical instability <span class="hlt">waves</span>. We suggest that a remote wind forcing determines the high model/observation phase correspondence of tropical instability <span class="hlt">waves</span> through a relatively realistic simulation of equatorial Kelvin and Rossby <span class="hlt">wave</span> activity.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015AGUFMIN33C1810O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015AGUFMIN33C1810O"><span>A Robotic Communications Gateway for <span class="hlt">Ocean</span> Observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Orcutt, J. A.; Berger, J.; Laske, G.; Babcock, J.</p> <p>2015-12-01</p> <p>We describe a new technology that can provide real-time telemetry of sensor data from the <span class="hlt">ocean</span> bottom. The breakthrough technology that makes this system possible is an autonomous surface vehicle called the <span class="hlt">Wave</span> Glider developed by Liquid Robotics, Inc. of Sunnyvale, CA., which harvests <span class="hlt">wave</span> and solar energy for motive and electrical <span class="hlt">power</span>. The free-floating surface communications gateway uses a Liquid Robotics <span class="hlt">wave</span> glider comprising a surfboard-sized float towed by a tethered, submerged glider, which converts <span class="hlt">wave</span> motion into thrust. For navigation, the <span class="hlt">wave</span> glider is equipped with a small computer, a GPS receiver, a rudder, solar panels and batteries, and an Iridium satellite modem. Acoustic communications connect the subsea instruments and the surface gateway while communications between the gateway and land are provided by the Iridium satellite constellation. <span class="hlt">Wave</span> gliders have demonstrated trans-<span class="hlt">oceanic</span> range and long-term station keeping capabilities. The topside acoustics communications package is mounted in a shallow tow body, which uses a WHOI micro modem and a Benthos low frequency, directional transducer. A matching bottom side modem and transducer are mounted on the <span class="hlt">ocean</span> bottom package. Tests of the surface gateway in 4000 m of water demonstrated an acoustic efficiency of approximately 256 bits/J. For example, it has the ability to send four channels of compressed, one sample per second data from the <span class="hlt">ocean</span> bottom to the gateway with an average <span class="hlt">power</span> draw of approximately 0.36 W and a latency of about three minutes. This gateway is used to send near-real-time data from a broadband <span class="hlt">ocean</span> bottom seismic observatory; we are presently designing and constructing a seafloor package with a two-year operational life. We have found that for frequencies f where f<10mHz, 35mHz < f < 120mHz and f>~3Hz, the vertical component, seafloor system noise characteristics are generally superior to similar observatories on land. Increasing the density of these stations over</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006AdAtS..23..442W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006AdAtS..23..442W"><span>Framework of distributed coupled atmosphere-<span class="hlt">ocean-wave</span> modeling system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wen, Yuanqiao; Huang, Liwen; Deng, Jian; Zhang, Jinfeng; Wang, Sisi; Wang, Lijun</p> <p>2006-05-01</p> <p>In order to research the interactions between the atmosphere and <span class="hlt">ocean</span> 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-<span class="hlt">ocean-wave</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015OcDyn..65.1547Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015OcDyn..65.1547Z"><span>The impact of sea surface currents in <span class="hlt">wave</span> <span class="hlt">power</span> potential modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zodiatis, George; Galanis, George; Kallos, George; Nikolaidis, Andreas; Kalogeri, Christina; Liakatas, Aristotelis; Stylianou, Stavros</p> <p>2015-11-01</p> <p>The impact of sea surface currents to the estimation and modeling of <span class="hlt">wave</span> energy potential over an area of increased economic interest, the Eastern Mediterranean Sea, is investigated in this work. High-resolution atmospheric, <span class="hlt">wave</span>, and circulation models, the latter downscaled from the regional Mediterranean Forecasting System (MFS) of the Copernicus marine service (former My<span class="hlt">Ocean</span> 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 <span class="hlt">wave</span> characteristics, but also in the general distribution of the <span class="hlt">wave</span> energy and the <span class="hlt">wave</span> parameters that mainly affect it, when using sea surface currents as a forcing to the <span class="hlt">wave</span> models. The obtained results prove that the impact of the sea surface currents is quite significant in <span class="hlt">wave</span> 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-<span class="hlt">ocean</span> forecasting counterparts.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19910006313','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19910006313"><span>Visualizing characteristics of <span class="hlt">ocean</span> data collected during the Shuttle Imaging Radar-B experiment</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tilley, David G.</p> <p>1991-01-01</p> <p>Topographic measurements of sea surface elevation collected by the Surface Contour Radar (SCR) during NASA's Shuttle Imaging Radar (SIR-B) experiment are plotted as three dimensional surface plots to observe <span class="hlt">wave</span> height variance along the track of a P-3 aircraft. <span class="hlt">Ocean</span> <span class="hlt">wave</span> spectra were computed from rotating altimeter measurements acquired by the Radar <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Spectrometer (ROWS). Fourier <span class="hlt">power</span> spectra computed from SIR-B synthetic aperture radar (SAR) images of the <span class="hlt">ocean</span> are compared to ROWS surface <span class="hlt">wave</span> spectra. Fourier inversion of SAR spectra, after subtraction of spectral noise and modeling of <span class="hlt">wave</span> height modulation, yields topography similar to direct measurements made by SCR. Visual perspectives on the SCR and SAR <span class="hlt">ocean</span> data are compared. Threshold distinctions between surface elevation and texture modulations of SAR data are considered within the context of a dynamic statistical model of rough surface scattering. The result of these endeavors is insight as to the physical mechanism governing the imaging of <span class="hlt">ocean</span> <span class="hlt">waves</span> with SAR.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ChJOL..34..847R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ChJOL..34..847R"><span>A joint method to retrieve directional <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra from SAR and <span class="hlt">wave</span> spectrometer data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ren, Lin; Yang, Jingsong; Zheng, Gang; Wang, Juan</p> <p>2016-07-01</p> <p>This paper proposes a joint method to simultaneously retrieve <span class="hlt">wave</span> spectra at different scales from spaceborne Synthetic Aperture Radar (SAR) and <span class="hlt">wave</span> spectrometer data. The method combines the output from the two different sensors to overcome retrieval limitations that occur in some sea states. The <span class="hlt">wave</span> spectrometer sensitivity coefficient is estimated using an effective significant <span class="hlt">wave</span> height (SWH), which is an average of SAR-derived and <span class="hlt">wave</span> spectrometer-derived SWH. This averaging extends the area of the sea surface sampled by the nadir beam of the <span class="hlt">wave</span> spectrometer to improve the accuracy of the estimated sensitivity coefficient in inhomogeneous sea states. <span class="hlt">Wave</span> spectra are then retrieved from SAR data using <span class="hlt">wave</span> spectrometer-derived spectra as first guess spectra to complement the short <span class="hlt">waves</span> lost in SAR data retrieval. In addition, the problem of 180° ambiguity in retrieved spectra is overcome using SAR imaginary cross spectra. Simulated data were used to validate the joint method. The simulations demonstrated that retrieved <span class="hlt">wave</span> parameters, including SWH, peak <span class="hlt">wave</span> length (PWL), and peak <span class="hlt">wave</span> direction (PWD), agree well with reference parameters. Collocated data from ENVISAT advanced SAR (ASAR), the airborne <span class="hlt">wave</span> spectrometer STORM, the PHAROS buoy, and the European Centre for Medium-Range Weather Forecasting (ECMWF) were then used to verify the proposed method. <span class="hlt">Wave</span> parameters retrieved from STORM and two ASAR images were compared to buoy and ECMWF <span class="hlt">wave</span> data. Most of the retrieved parameters were comparable to reference parameters. The results of this study show that the proposed joint retrieval method could be a valuable complement to traditional methods used to retrieve directional <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra, particularly in inhomogeneous sea states.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.5857T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.5857T"><span>Finite frequency P-<span class="hlt">wave</span> traveltime measurements on <span class="hlt">ocean</span> bottom seismometers and hydrophones in the western Indian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsekhmistrenko, Maria; Sigloch, Karin; Hosseini, Kasra; Barruol, Guilhem</p> <p>2016-04-01</p> <p>From 2011 to 2014, the RHUM-RUM project (Reunion Hotspot Upper Mantle - Reunions Unterer Mantel) instrumented a 2000x2000km2 area of Indian <span class="hlt">Ocean</span> seafloor, islands and Madagascar with broadband seismometers and hydrophones. The central component was a 13-month deployment of 57 German and French <span class="hlt">Ocean</span> Bottom Seismometers (OBS) in 2300-5600 m depth. This was supplemented by 2-3 year deployments of 37 island stations on Reunion, Mauritius, Rodrigues, the southern Seychelles, the Iles Eparses and southern Madagascar. Two partner projects contributed another 30+ stations on Madagascar. Our ultimate objective is multifrequency waveform tomography of the entire mantle column beneath the Reunion hotspot. Ideally we would use all passbands that efficiently transmit body <span class="hlt">waves</span> but this meets practical limits in the noise characteristics of <span class="hlt">ocean</span>-bottom recordings in particular. Here we present the preliminary data set of frequency-dependent P-<span class="hlt">wave</span> traveltime measurements on seismometers and hydrophones, obtained by cross-correlation of observed with predicted waveforms. The latter are synthesized from fully numerical Green's functions and carefully estimated, broadband source time functions. More than 200 teleseismic events during the 13-month long deployment yielded usable P-waveform measurements. We present our methods and discuss data yield and quality of <span class="hlt">ocean</span>-bottom versus land seismometers, and of OBS versus broadband hydrophones. Above and below the microseismic noise band, data yields are higher than within it, especially for OBS. The 48 German OBS, equipped with Guralp 60 s sensors, were afflicted by relatively high self-noise compared to the 9 French instruments equipped with Nanometrics Trillium 240 s sensors. The HighTechInc (model HTI-01 and HTI-04-PCA/ULF) hydrophones (100 s corner period) functioned particularly reliably but their waveforms are relatively more challenging to model due to reverberations in the water column. We obtain ~15000 combined cross</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1996JPhD...29..369B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1996JPhD...29..369B"><span>Pulsed discharges produced by high-<span class="hlt">power</span> 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>Böhle, A.; Ivanov, O.; Kolisko, A.; Kortshagen, U.; Schlüter, H.; Vikharev, A.</p> <p>1996-02-01</p> <p>The mechanisms of the ionization front advance in surface-<span class="hlt">wave</span>-produced discharges are investigated using two experimental set-ups. The high-<span class="hlt">power</span> surface <span class="hlt">waves</span> are excited in a 3 cm wavelength band by a surfaguide and a novel type of launcher (an E-plane junction). The ionization front velocity of the surface <span class="hlt">wave</span> is measured for a wide range of gas pressures, incident microwave <span class="hlt">power</span> and initial pre-ionization. The experimental results are compared with theoretical ones based on three different models. The comparison between theory and experiment allows one to suggest a new interpretation of the ionization front's advance. The ionization front velocity is determined by a breakdown <span class="hlt">wave</span> or an ionization <span class="hlt">wave</span> in the electric field of a high-<span class="hlt">power</span> surface <span class="hlt">wave</span> in the zone near the ionization front.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014APS..DFDK14001P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014APS..DFDK14001P"><span>In Pursuit of 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>Peacock, Thomas</p> <p>2014-11-01</p> <p>Orders of magnitude larger than surface <span class="hlt">waves</span>, and so <span class="hlt">powerful</span> that their generation impacts the lunar orbit, internal <span class="hlt">waves</span>, propagating disturbances of a density-stratified fluid, are ubiquitous throughout the <span class="hlt">ocean</span> and atmosphere. Following the discovery of the phenomenon of ``dead water'' by early Arctic explorers and the classic laboratory visualizations of the curious St. Andrew's Cross internal <span class="hlt">wave</span> pattern, there has been a resurgence of interest in internal <span class="hlt">waves</span>, inspired by their pivotal roles in local environmental and global climate processes, and their profound impact on <span class="hlt">ocean</span> and aerospace engineering. We detail our widespread pursuit of internal <span class="hlt">waves</span> through theoretical modeling, laboratory experiments and field studies, from the Pacific <span class="hlt">Ocean</span> one thousand miles north and south of Hawaii, to the South China Sea, and on to the Arctic <span class="hlt">Ocean</span>. We also describe our recent expedition to surf the most striking internal <span class="hlt">wave</span> phenomenon of them all: the Morning Glory cloud in remote Northwest Australia. This work was supported by the National Science Foundation through a CAREER Grant OCE-064559 and through Grants OCE-1129757 and OCE-1357434, and by the Office of Naval Research through Grants N00014-09-1-0282, N00014-08-1-0390 and N00014-05-1-0575.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010JGRA..115.7303T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010JGRA..115.7303T"><span>Variance of transionospheric VLF <span class="hlt">wave</span> <span class="hlt">power</span> absorption</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tao, X.; Bortnik, J.; Friedrich, M.</p> <p>2010-07-01</p> <p>To investigate the effects of D-region electron-density variance on <span class="hlt">wave</span> <span class="hlt">power</span> absorption, we calculate the <span class="hlt">power</span> reduction of very low frequency (VLF) <span class="hlt">waves</span> propagating through the ionosphere with a full <span class="hlt">wave</span> method using the standard ionospheric model IRI and in situ observational data. We first verify the classic absorption curves of Helliwell's using our full <span class="hlt">wave</span> code. Then we show that the IRI model gives overall smaller <span class="hlt">wave</span> absorption compared with Helliwell's. Using D-region electron densities measured by rockets during the past 60 years, we demonstrate that the <span class="hlt">power</span> absorption of VLF <span class="hlt">waves</span> is subject to large variance, even though Helliwell's absorption curves are within ±1 standard deviation of absorption values calculated from data. Finally, we use a subset of the rocket data that are more representative of the D region of middle- and low-latitude VLF <span class="hlt">wave</span> transmitters and show that the average quiet time <span class="hlt">wave</span> absorption is smaller than that of Helliwell's by up to 100 dB at 20 kHz and 60 dB at 2 kHz, which would make the model-observation discrepancy shown by previous work even larger. This result suggests that additional processes may be needed to explain the discrepancy.</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 <span class="hlt">ocean</span> currents 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 <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra and surface currents 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> <span class="hlt">ocean</span> 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 couples the resonance technique with coherent, frequency agility radar capabilities. This scatterometer is presently configured for supporting a program of surface current measurements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1004174','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1004174"><span>Microfabricated Millimeter-<span class="hlt">Wave</span> High-<span class="hlt">Power</span> Vacuum Electronic Amplifiers</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-01-01</p> <p>Applications filed 2012). In spite of the challenges, high <span class="hlt">power</span> sources of electromagnetic radiation are needed in the mmW bands for advanced DoD...Research Laboratory is demonstrating and developing millimeter-<span class="hlt">wave</span> vacuum electronic traveling <span class="hlt">wave</span> tube amplifiers at W- and G- band in the 10’ s to 100... s of watts <span class="hlt">power</span> range at several percent instantaneous bandwidth. Keywords: Traveling <span class="hlt">wave</span> tube; millimeter <span class="hlt">wave</span>; vacuum electron device</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S41A2761M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S41A2761M"><span>Extracting Rayleigh <span class="hlt">wave</span> dispersion from ambient noise across the Indian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ma, Z.; Dalton, C. A.</p> <p>2016-12-01</p> <p>Rayleigh <span class="hlt">wave</span> dispersion extracted from ambient seismic noise has been widely used to image crustal and uppermost mantle structure. Applications of this approach in continental settings are abundant, but there have been relatively few studies within <span class="hlt">ocean</span> basins. In this presentation, we will first demonstrate the feasibility of extracting high quality Rayleigh <span class="hlt">wave</span> dispersion information from ambient noise across the entire Indian <span class="hlt">Ocean</span> basin. Phase arrival times measured from ambient noise are largely consistent with the ones predicted from 2-D phase velocity maps that were determined from earthquake data alone. Secondly, we show that adding dispersion information extracted from ambient noise to existing earthquake data can indeed improve the resolution of phase velocity maps by about 20% in the western Indian <span class="hlt">Ocean</span> region where the station distribution is the densest. High quality Rayleigh <span class="hlt">wave</span> dispersion information can be obtained from stacking waveforms over less than two years at land stations and less than four years at island stations. After removing the age dependent average velocities, the 2-D phase velocity maps show slow anomalies associated with the Seychelles-Mascarene plateau. Forward modeling suggests that the crust is about 15-25 km thick in this area, which agrees with previous estimates obtained from gravity data. We also observe that the slow anomaly related to the Central Indian Ridge is asymmetric. The center of this slow anomaly lies to the west side of ridge, which is opposite to the ridge migration direction. This asymmetry probably reflects the interactions between the ridge and nearby hotspots.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1714282C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1714282C"><span>Coupled Atmosphere-<span class="hlt">Wave-Ocean</span> Modeling of Tropical Cyclones: Progress, Challenges, and Ways Forward</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Chen, Shuyi</p> <p>2015-04-01</p> <p>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 <span class="hlt">ocean</span> <span class="hlt">waves</span>, 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 <span class="hlt">ocean</span> 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 <span class="hlt">ocean</span>) and sink (surface friction and wind-induced upper <span class="hlt">ocean</span> 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 <span class="hlt">Ocean</span> 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</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1415600','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1415600"><span><span class="hlt">Wave</span> Energy Prize - 1/50th Testing - Atlas <span class="hlt">Ocean</span> Systems</span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Wesley Scharmen</p> <p>2015-12-04</p> <p>This submission of data includes all the 1/50th scale testing data completed on the <span class="hlt">Wave</span> Energy Prize for the Atlas <span class="hlt">Ocean</span> Systems team, and includes: 1/50th test data (raw & processed) 1/50th test data video and pictures 1/50th Test plans and testing documents SSTF_Submission (summarized results)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19840030376&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfunction%2Bwave','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19840030376&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfunction%2Bwave"><span>Parametric dependence of <span class="hlt">ocean</span> <span class="hlt">wave</span>-radar modulation transfer functions</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Plant, W. J.; Keller, W. C.; Cross, A.</p> <p>1983-01-01</p> <p>Microwave techniques at X and L band were used to determine the dependence of <span class="hlt">ocean-wave</span> radar modulation transfer functions (MTFs) on various environmental and radar parameters during the Marine Remote Sensing experiment of 1979 (MARSEN 79). These MIF are presented, as are coherence functions between the AM and FM parts of the backscattered microwave signal. It is shown that they both depend on several of these parameters. Besides confirming many of the properties of transfer functions reported by previous authors, indications are found that MTFs decrease with increasing angle between <span class="hlt">wave</span> propagation and antenna-look directions but are essentially independent of small changes in air-sea temperature difference. However, coherence functions are much smaller when the antennas are pointed perpendicular to long <span class="hlt">waves</span>. It is found that X band transfer functions measured with horizontally polarized microwave radiation have larger magnitudes than those obtained by using vertical polarization.</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/2016PhDT........34B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT........34B"><span>Image processing to optimize <span class="hlt">wave</span> energy converters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bailey, Kyle Marc-Anthony</p> <p></p> <p>The world is turning to renewable energies as a means of ensuring the planet's future and well-being. There have been a few attempts in the past to utilize <span class="hlt">wave</span> <span class="hlt">power</span> as a means of generating electricity through the use of <span class="hlt">Wave</span> Energy Converters (WEC), but only recently are they becoming a focal point in the renewable energy field. Over the past few years there has been a global drive to advance the efficiency of WEC. Placing a mechanical device either onshore or offshore that captures the energy within <span class="hlt">ocean</span> surface <span class="hlt">waves</span> to drive a mechanical device is how <span class="hlt">wave</span> <span class="hlt">power</span> is produced. This paper seeks to provide a novel and innovative way to estimate <span class="hlt">ocean</span> <span class="hlt">wave</span> frequency through the use of image processing. This will be achieved by applying a complex modulated lapped orthogonal transform filter bank to satellite images of <span class="hlt">ocean</span> <span class="hlt">waves</span>. The complex modulated lapped orthogonal transform filterbank provides an equal subband decomposition of the Nyquist bounded discrete time Fourier Transform spectrum. The maximum energy of the 2D complex modulated lapped transform subband is used to determine the horizontal and vertical frequency, which subsequently can be used to determine the <span class="hlt">wave</span> frequency in the direction of the WEC by a simple trigonometric scaling. The robustness of the proposed method is provided by the applications to simulated and real satellite images where the frequency is known.</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>Coupled atmosphere-<span class="hlt">ocean-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 <span class="hlt">ocean</span> 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 <span class="hlt">oceanic</span> response to such events, we implemented the Coupled <span class="hlt">Ocean-Atmosphere-Wave</span>-Sediment Transport Modeling 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 coupled system. A surface heat budget analysis showed that <span class="hlt">ocean</span> 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 <span class="hlt">ocean</span>-atmosphere coupling suggested that the coupled system is sensitive to the momentum flux parameterization as well as air-sea and air-<span class="hlt">wave</span> coupling. Comparisons with available atmospheric and <span class="hlt">oceanic</span> observations showed that the use of the fully coupled system provides the most skillful simulation, illustrating the benefit of using a fully coupled <span class="hlt">ocean-atmosphere-wave</span> model for the assessment of these storm events.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1013732','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1013732"><span><span class="hlt">Wave</span>-Ice and Air-Ice-<span class="hlt">Ocean</span> Interaction During the Chukchi Sea Ice Edge Advance</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-09-30</p> <p>1 DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. <span class="hlt">Wave</span> -Ice and Air-Ice-<span class="hlt">Ocean</span> Interaction During the...Chukchi Sea in the late summer have potentially changed the impact of fall storms by creating <span class="hlt">wave</span> fields in the vicinity of the advancing ice edge. A...first) <span class="hlt">wave</span> -ice interaction field experiment that adequately documents the relationship of a growing pancake ice cover with a time and space varying</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1986GeoRL..13..315M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1986GeoRL..13..315M"><span>3-dimensional structure of the Indian <span class="hlt">Ocean</span> inferred from long period 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>Montagner, Jean-Paul</p> <p>1986-04-01</p> <p>To improve the lateral resolution of the first global 3 - dimensional models of seismic <span class="hlt">wave</span> velocities, regional studies have to be undertaken. The dispersion of Rayleigh <span class="hlt">waves</span> along 86 paths across the Indian <span class="hlt">Ocean</span> and surrounding regions is investigated in the period range 40 - 300 s. The regionalization of group velocity according to the age of the sea floor shows an increase of velocity with age up to 150 s only, similar to the results in the Pacific <span class="hlt">Ocean</span>. But here, this relationship vanishes more quickly at long period. Therefore the correlation of the deep structure with surface tectonics seems to be shallower in the Indian <span class="hlt">Ocean</span> than in the Pacific <span class="hlt">Ocean</span>. A tomographic method is applied to compute the geographical distributions of group velocity and azimuthal anisotropy and then the 3-D structure of S-<span class="hlt">wave</span> velocity. Horizontal wavelengths of 2000 km for velocity and 3000 km for azimuthal anisotropy distribution can be resolved. Except for the central part of the South East Indian ridge which displays high velocities at all depths, the inversion corroborates a good correlation between lithospheric structure down to 120 km and surface tectonics: low velocities along the central and southeast Indian ridges, velocity increasing with the age of the sea floor, high velocities under African, Indian and Australian shields. At greater depths, the low velocity zones under the Gulf of Aden and the western part of the Southeast Indian ridges hold but the low velocity anomaly of the Central Indian ridge is offset eastward. The low velocity anomalies suggest uprising material and complex plate boundary.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060044025&hterms=regional+development&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dregional%2Bdevelopment','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060044025&hterms=regional+development&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dregional%2Bdevelopment"><span><span class="hlt">Power</span> systems for <span class="hlt">ocean</span> regional cabled observatories</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kojima, Junichi; Asakawa, Kenichi; Howe, Bruce M.; Kirkham, Harold</p> <p>2004-01-01</p> <p>Development of <span class="hlt">power</span> systems is the most challenging technical issue in the design of <span class="hlt">ocean</span> regional cabled observatories. ARENA and NEPTUNE are two <span class="hlt">ocean</span> regional cabled observatory networks with aims that are at least broadly similar. Yet the two designs are quite different in detail. This paper outlines the both systems and explores the reasons for the divergence of design, and shows that it arose because of differences in the priority of requirements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AdSR...13...75G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AdSR...13...75G"><span>Twenty-first century <span class="hlt">wave</span> climate projections for Ireland and surface winds in the North Atlantic <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gallagher, Sarah; Gleeson, Emily; Tiron, Roxana; McGrath, Ray; Dias, Frédéric</p> <p>2016-04-01</p> <p>Ireland has a highly energetic <span class="hlt">wave</span> and wind climate, and is therefore uniquely placed in terms of its <span class="hlt">ocean</span> renewable energy resource. The socio-economic importance of the marine resource to Ireland makes it critical to quantify how the <span class="hlt">wave</span> and wind climate may change in the future due to global climate change. Projected changes in winds, <span class="hlt">ocean</span> <span class="hlt">waves</span> and the frequency and severity of extreme weather events should be carefully assessed for long-term marine and coastal planning. We derived an ensemble of future <span class="hlt">wave</span> climate projections for Ireland using the EC-Earth global climate model and the WAVEWATCH III® <span class="hlt">wave</span> model, by comparing the future 30-year period 2070-2099 to the period 1980-2009 for the RCP4.5 and the RCP8.5 forcing scenarios. This dataset is currently the highest resolution <span class="hlt">wave</span> projection dataset available for Ireland. The EC-Earth ensemble predicts decreases in mean (up to 2 % for RCP4.5 and up to 3.5 % for RCP8.5) 10 m wind speeds over the North Atlantic <span class="hlt">Ocean</span> (5-75° N, 0-80° W) by the end of the century, which will consequently affect swell generation for the Irish <span class="hlt">wave</span> climate. The WAVEWATCH III® model predicts an overall decrease in annual and seasonal mean significant <span class="hlt">wave</span> heights around Ireland, with the largest decreases in summer (up to 15 %) and winter (up to 10 %) for RCP8.5. Projected decreases in mean significant <span class="hlt">wave</span> heights for spring and autumn were found to be small for both forcing scenarios (less than 5 %), with no significant decrease found for RCP4.5 off the west coast in those seasons.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870007903&hterms=1043&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3D%2526%25231043','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870007903&hterms=1043&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3D%2526%25231043"><span>Deriving Two-Dimensional <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Spectra and Surface Height Maps from the Shuttle Imaging Radar (SIR-B)</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tilley, D. G.</p> <p>1986-01-01</p> <p>Directional <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra were derived from Shuttle Imaging Radar (SIR-B) imagery in regions where nearly simultaneous aircraft-based measurements of the <span class="hlt">wave</span> spectra were also available as part of the NASA Shuttle Mission 41G experiments. The SIR-B response to a coherently speckled scene is used to estimate the stationary system transfer function in the 15 even terms of an eighth-order two-dimensional polynomial. Surface elevation contours are assigned to SIR-B <span class="hlt">ocean</span> scenes Fourier filtered using a empirical model of the modulation transfer function calibrated with independent measurements of <span class="hlt">wave</span> height. The empirical measurements of the <span class="hlt">wave</span> height distribution are illustrated for a variety of sea states.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S51C..04A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S51C..04A"><span>Multi-Decadal analysis of Global Trends in Microseism Intensity: A Proxy for Changes in Extremal Storm Activity and <span class="hlt">Oceanic</span> <span class="hlt">Wave</span> State</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anthony, R. E.; Aster, R. C.; Rowe, C. A.</p> <p>2016-12-01</p> <p>The Earth's seismic noise spectrum features two globally ubiquitous peaks near 8 and 16 s periods (secondary and primary bands) that arise when storm-generated <span class="hlt">ocean</span> gravity <span class="hlt">waves</span> are converted to seismic energy, predominantly into Rayleigh <span class="hlt">waves</span>. Because of its regionally integrative nature, microseism intensity and other seismographic data from long running sites can provide useful proxies for <span class="hlt">wave</span> state. Expanding an earlier study of global microseism trends (Aster et al., 2010), we analyze digitally-archived, up-to-date (through late 2016) multi-decadal seismic data from stations of global seismographic networks to characterize the spatiotemporal evolution of <span class="hlt">wave</span> climate over the past >20 years. The IRIS Noise Tool Kit (Bahavair et al., 2013) is used to produce ground motion <span class="hlt">power</span> spectral density (PSD) estimates in 3-hour overlapping time series segments. The result of this effort is a longer duration and more broadly geographically distributed PSD database than attained in previous studies, particularly for the primary microseism band. Integrating <span class="hlt">power</span> within the primary and secondary microseism bands enables regional characterization of spatially-integrated trends in <span class="hlt">wave</span> states and storm event statistics of varying thresholds. The results of these analyses are then interpreted within the context of recognized modes of atmospheric variability, including the particularly strong 2015-2016 El Niño. We note a number of statistically significant increasing trends in both raw microseism <span class="hlt">power</span> and storm activity occurring at multiple stations in the Northwest Atlantic and Southeast Pacific consistent with generally increased <span class="hlt">wave</span> heights and storminess in these regions. Such trends in <span class="hlt">wave</span> activity have the potential to significantly influence coastal environments particularly under rising global sea levels.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA096353','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA096353"><span>Experiments in <span class="hlt">Wave</span> Record Analysis.</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1980-09-01</p> <p>manipulation of <span class="hlt">wave</span> records in digital form to produce a <span class="hlt">power</span> density spectrum (PDS) with great efficiency. The PDS gives a presentation of the...instantaneous surface elevation digital points (the zero level reference). The individual period, Ti, was taken as the time difference between two successive...CONCLUSIONS This thesis presents the results of experiments in the analysis of <span class="hlt">ocean</span> <span class="hlt">wave</span> records. For this purpose 19 digitized records obtained from a <span class="hlt">wave</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70041533','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70041533"><span>The observed relationship between <span class="hlt">wave</span> conditions and beach response, <span class="hlt">Ocean</span> Beach, San Francisco, CA</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Hansen, J.E.; Barnard, P.L.</p> <p>2009-01-01</p> <p>Understanding how sandy beaches respond to storms is critical for effective sediment management and developing successful erosion mitigation efforts. However, only limited progress has been made in relating observed beach changes to <span class="hlt">wave</span> conditions, with one of the major limiting factors being the lack of temporally dense beach topography and nearshore <span class="hlt">wave</span> data in most studies. This study uses temporally dense beach topographic and offshore <span class="hlt">wave</span> data to directly link beach response and <span class="hlt">wave</span> forcing with generally good results. <span class="hlt">Ocean</span> Beach is an open coast high-energy sandy beach located in San Francisco, CA, USA. From April 2004 through the end of 2008, 60 three-dimensional topographic beach surveys were conducted on approximately a monthly basis, with more frequent “short-term surveys during the winters of 2005-06 and 2006-07. Shoreline position data from the short-term surveys show good correlation with offshore <span class="hlt">wave</span> height, period, and direction averaged over several days prior to the survey (mean R*=0.54 for entire beach). There is, however, considerable alongshore variation in model performance, with R- values ranging from 0.81 to 0.19 for individual sections of the beach. After <span class="hlt">wave</span> height, the direction of <span class="hlt">wave</span> approach was the most important factor in determining the response of the shoreline, followed by <span class="hlt">wave</span> period. Our results indicate that an empirical predictive model of beach response to <span class="hlt">wave</span> conditions at <span class="hlt">Ocean</span> Beach is possible with frequent beach mapping and <span class="hlt">wave</span> data, and that such a model could be useful to coastal managers. </p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19820015568','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19820015568"><span>Size distribution of <span class="hlt">oceanic</span> air bubbles entrained in sea-water by <span class="hlt">wave</span>-breaking</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Resch, F.; Avellan, F.</p> <p>1982-01-01</p> <p>The size of <span class="hlt">oceanic</span> air bubbles produced by whitecaps and <span class="hlt">wave</span>-breaking is determined. The production of liquid aerosols at the sea surface is predicted. These liquid aerosols are at the origin of most of the particulate materials exchanged between the <span class="hlt">ocean</span> and the atmosphere. A prototype was designed and built using an optical technique based on the principle of light scattering at an angle of ninety degrees from the incident light beam. The output voltage is a direct function of the bubble diameter. Calibration of the probe was carried out within a range of 300 microns to 1.2 mm. Bubbles produced by <span class="hlt">wave</span>-breaking in a large air-sea interaction simulating facility. Experimental results are given in the form of size spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940015965&hterms=gaussian&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dgaussian','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940015965&hterms=gaussian&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Dgaussian"><span>Near grazing scattering from non-Gaussian <span class="hlt">ocean</span> surfaces</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kim, Yunjin; Rodriguez, Ernesto</p> <p>1993-01-01</p> <p>We investigate the behavior of the scattered electromagnetic <span class="hlt">waves</span> from non-Gaussian <span class="hlt">ocean</span> surfaces at near grazing incidence. Even though the scattering mechanisms at moderate incidence angles are relatively well understood, the same is not true for near grazing rough surface scattering. However, from the experimental <span class="hlt">ocean</span> scattering data, it has been observed that the backscattering cross section of a horizontally polarized <span class="hlt">wave</span> can be as large as the vertical counterpart at near grazing incidence. In addition, these returns are highly intermittent in time. There have been some suggestions that these unexpected effects may come from shadowing or feature scattering. Using numerical scattering simulations, it can be shown that the horizontal backscattering cannot be larger than the vertical one for the Gaussian surfaces. Our main objective of this study is to gain a clear understanding of scattering mechanisms underlying the near grazing <span class="hlt">ocean</span> scattering. In order to evaluate the backscattering cross section from <span class="hlt">ocean</span> surfaces at near grazing incidence, both the hydrodynamic modeling of <span class="hlt">ocean</span> surfaces and an accurate near grazing scattering theory are required. For the surface modeling, we generate Gaussian surfaces from the <span class="hlt">ocean</span> surface <span class="hlt">power</span> spectrum which is derived using several experimental data. Then, weakly nonlinear large scale <span class="hlt">ocean</span> surfaces are generated following Longuet-Higgins. In addition, the modulation of small <span class="hlt">waves</span> by large <span class="hlt">waves</span> is included using the conservation of <span class="hlt">wave</span> action. For surface scattering, we use MOM (Method of Moments) to calculate the backscattering from scattering patches with the two scale shadowing approximation. The differences between Gaussian and non-Gaussian surface scattering at near grazing incidence are presented.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840019214','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840019214"><span>Measurements of <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra and modulation transfer function with the airborne two frequency scatterometer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Weissman, D. E.; Johnson, J. W.</p> <p>1984-01-01</p> <p>The directional spectrum and the microwave modulation transfer function of <span class="hlt">ocean</span> <span class="hlt">waves</span> can be measured with the airborne two frequency scatterometer technique. Similar to tower based observations, the aircraft measurements of the Modulation Transfer Function (MTF) show that it is strongly affected by both wind speed and sea state. Also detected are small differences in the magnitudes of the MTF between downwind and upwind radar look directions, and variations with <span class="hlt">ocean</span> wavenumber. The MTF inferred from the two frequency radar is larger than that measured using single frequency, <span class="hlt">wave</span> orbital velocity techniques such as tower based radars or ROWS measurements from low altitude aircraft. Possible reasons for this are discussed. The ability to measure the <span class="hlt">ocean</span> directional spectrum with the two frequency scatterometer, with supporting MTF data, is demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19860043880&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfunction%2Bwave','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19860043880&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfunction%2Bwave"><span>Measurements of <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra and modulation transfer function with the airborne two-frequency scatterometer</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Weissman, D. E.; Johnson, J. W.</p> <p>1986-01-01</p> <p>The directional spectrum and the microwave modulation transfer function of <span class="hlt">ocean</span> <span class="hlt">waves</span> can be measured with the airborne two frequency scatterometer technique. Similar to tower based observations, the aircraft measurements of the Modulation Transfer Function (MTF) show that it is strongly affected by both wind speed and sea state. Also detected are small differences in the magnitudes of the MTF between downwind and upwind radar look directions, and variations with <span class="hlt">ocean</span> wavenumber. The MTF inferred from the two frequency radar is larger than that measured using single frequency, <span class="hlt">wave</span> orbital velocity techniques such as tower based radars or ROWS measurements from low altitude aircraft. Possible reasons for this are discussed. The ability to measure the <span class="hlt">ocean</span> directional spectrum with the two frequency scatterometer, with supporting MTF data, is demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA590736','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA590736"><span><span class="hlt">Ocean</span> Surface <span class="hlt">Wave</span> Optical Roughness: Analysis of Innovative Measurements</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2013-12-16</p> <p>relationship of MSS to wind speed, and at times has shown a reversal of the Cox-Munk linear relationship. Furthermore, we observe measurable changes in...1985]. The variable speed allocation method has the effect of aliasing (cb) to slower <span class="hlt">waves</span>, thereby increasing the exponent –m. Our analysis based ...RaDyO) program. The primary research goals of the program are to (1) examine time -dependent <span class="hlt">oceanic</span> radiance distribution in relation to dynamic</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20060041879&hterms=level+topical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dlevel%2Btopical','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20060041879&hterms=level+topical&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3Dlevel%2Btopical"><span>A high-resolution OGCM simulation of the Tropical Pacific <span class="hlt">Ocean</span> during the 1985-1994 TOGA period. Part I: Long equatorial <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>Boulanger, J. P.; Delecluse, F.; Maes, C.; Levy, C.</p> <p>1995-01-01</p> <p>A high resolution <span class="hlt">oceanic</span> general circulation model of the three topical <span class="hlt">oceans</span> is used to investigate long equatorial <span class="hlt">wave</span> activity in the Pacific <span class="hlt">Ocean</span> during the 1985-1994 TOGA period. Zonal wind stress forcing and simulated dynamic height are interpreted using techniques previously applied to data. Kelvin and first Rossby <span class="hlt">waves</span> are observed propagating during all the period. A seasonal cycle and interannual anomalies are computed for each long equatorial <span class="hlt">wave</span>. The east Pacific basin is mainly dominated by seasonal cycle variations while strong interannual anomalies are observed west of the dateline. Long <span class="hlt">wave</span> interannual anomalies are then compared to <span class="hlt">wave</span> coefficients simulated by a simple wind-forced model. Our results outline the major role played by wind forcing on interannual time scales in generating long equatorial <span class="hlt">waves</span>. However, near both eastern and western boundaries, some differences can be attributed to long <span class="hlt">wave</span> reflections. A comparison to <span class="hlt">wave</span> coefficients calculated from GEOSAT sea-level data gives some insight of the model behavior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFMDI21C..04B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFMDI21C..04B"><span><span class="hlt">Oceanic</span> Lithosphere/Asthenosphere Boundary from surface <span class="hlt">wave</span> dispersion data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Burgos, G.; Montagner, J.; Beucler, E.; Capdeville, Y.; Mocquet, A.</p> <p>2013-12-01</p> <p>The nature of Lithosphere-Asthenosphere boundary (LAB) is controversial according to different types of observations. Using a massive dataset of surface <span class="hlt">wave</span> dispersions in a broad frequency range (15-300s), we have developed a 3-D tomographic model (1st order perturbation theory) of the upper-mantle at the global scale. It is used to derive maps of LAB from the resolved elastic parameters. The key effects of shallow layers and anisotropy are taken into account in the inversion process. We investigate LAB distributions primarily below <span class="hlt">oceans</span> according to three different proxies which corresponds to the base of the lithosphere from the vertically polarized shear velocity variation at depth, the top of the radial anisotropy positive anomaly and from the changes in orientation of the fast axis of azimuthal anisotropy. The LAB depth determinations of the different proxies are basically consistent for each <span class="hlt">oceanic</span> region. The estimations of the LAB depth based on the shear velocity proxy increase from thin (20 km) lithosphere in the ridges to thick (120--130 km) old <span class="hlt">ocean</span> lithosphere. The radial anisotropy proxy presents a very fast increase of the LAB depth from the ridges, from 50 km to older <span class="hlt">ocean</span> where it reaches a remarkable monotonic sub-horizontal profile (70--80 km). LAB depths inferred from azimuthal anisotropy proxy show deeper values for the increasing <span class="hlt">oceanic</span> lithosphere (130--135 km). The results present two types of pattern of the age of <span class="hlt">oceanic</span> lithosphere evolution with the LAB depth. The shear velocity and azimuthal anisotropy proxies show age-dependent profiles in agreement with thermal plate models while the LAB based on radial anisotropy is characterized by a shallower depth, defining a sub-horizontal interface with a very small age dependence for all three main <span class="hlt">oceans</span> (Pacific, Atlantic and Indian). These different patterns raise questions about the nature of the LAB in the <span class="hlt">oceanic</span> regions, and of the formation of <span class="hlt">oceanic</span> plates.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA617950','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA617950"><span>Proving and Improving <span class="hlt">Wave</span> Models in the Arctic <span class="hlt">Ocean</span> and its MIZ</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2014-09-30</p> <p>on a giant ice island in Baffin Bay, in which the response to a breakup event was measured and the size of the broken-out iceberg fragment tested...2014), In situ measurements and analysis of <span class="hlt">ocean</span> <span class="hlt">waves</span> in the Antarctic marginal ice zone, Geophys. Res. Lett., 41, 5046–5051, doi:10.1002...Symposium on Ice, Singapore, August 11 to 15, 2014. Doble, M. J., and J.-R. Bidlot, 2013. <span class="hlt">Wave</span> buoy measurements at the Antarctic sea ice edge</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ChOE...31..458T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ChOE...31..458T"><span><span class="hlt">Wave</span> <span class="hlt">power</span> focusing due to the Bragg resonance</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tao, Ai-feng; Yan, Jin; Wang, Yi; Zheng, Jin-hai; Fan, Jun; Qin, Chuan</p> <p>2017-08-01</p> <p><span class="hlt">Wave</span> energy has drawn much attention as an achievable way to exploit the renewable energy. At present, in order to enhance the <span class="hlt">wave</span> energy extraction, most efforts have been concentrated on optimizing the <span class="hlt">wave</span> energy convertor and the <span class="hlt">power</span> take-off system mechanically and electrically. However, focusing the <span class="hlt">wave</span> <span class="hlt">power</span> in specific <span class="hlt">wave</span> field could also be an alternative to improve the <span class="hlt">wave</span> energy extraction. In this experimental study, the Bragg resonance effect is applied to focus the <span class="hlt">wave</span> energy. Because the Bragg resonance effect of the rippled bottom largely amplifies the <span class="hlt">wave</span> reflection, leading to a significant increase of <span class="hlt">wave</span> focusing. Achieved with an energy conversion system consisting of a point absorber and a permanent magnet single phase linear motor, the <span class="hlt">wave</span> energy extracted in the <span class="hlt">wave</span> flume with and without Bragg resonance effect was measured and compared quantitatively in experiment. It shows that energy extraction by a point absorber from a standing <span class="hlt">wave</span> field resulted from Bragg resonance effect can be remarkably increased compared with that from a propagating <span class="hlt">wave</span> field (without Bragg resonance effect).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1911801A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1911801A"><span>Small scale currents and <span class="hlt">ocean</span> <span class="hlt">wave</span> heights: from today's models to future satellite observations with CFOSAT and SKIM</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; Gille, Sarah; Menemenlis, Dimitris; Rocha, Cesar; Rascle, Nicolas; Gula, Jonathan; Chapron, Bertrand</p> <p>2017-04-01</p> <p>Tidal currents and large <span class="hlt">oceanic</span> currents, such as the Agulhas, Gulf Stream and Kuroshio, are known to modify <span class="hlt">ocean</span> <span class="hlt">wave</span> properties, causing extreme sea states that are a hazard to navigation. Recent advances in the understanding and modeling capability of <span class="hlt">ocean</span> 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 <span class="hlt">wave</span> heights at scales less than 200 km, including important variations at 10 km. This current-induced variability creates gradients in <span class="hlt">wave</span> heights that were previously overlooked and are relevant for extreme <span class="hlt">wave</span> heights and remote sensing. The spectrum of significant <span class="hlt">wave</span> 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 <span class="hlt">wave</span> 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 <span class="hlt">wave</span> spectrometers can help observe these <span class="hlt">wave</span>-current interactions. CFOSAT is due for launch in 2018, and SKIM is a proposal for ESA Earth Explorer 9.</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/2017AcGeo..65.1119P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AcGeo..65.1119P"><span>Effect of surface <span class="hlt">wave</span> propagation in a four-layered <span class="hlt">oceanic</span> crust model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Paul, Pasupati; Kundu, Santimoy; Mandal, Dinbandhu</p> <p>2017-12-01</p> <p>Dispersion of Rayleigh type surface <span class="hlt">wave</span> propagation has been discussed in four-layered <span class="hlt">oceanic</span> crust. It includes a sandy layer over a crystalline elastic half-space and over it there are two more layers—on the top inhomogeneous liquid layer and under it a liquid-saturated porous layer. Frequency equation is obtained in the form of determinant. The effects of the width of different layers as well as the inhomogeneity of liquid layer, sandiness of sandy layer on surface <span class="hlt">waves</span> are depicted and shown graphically by considering all possible case of the particular model. Some special cases have been deduced, few special cases give the dispersion equation of Scholte <span class="hlt">wave</span> and Stoneley <span class="hlt">wave</span>, some of which have already been discussed elsewhere.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016OcMod.107...21Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016OcMod.107...21Z"><span>A diffusion approximation for <span class="hlt">ocean</span> <span class="hlt">wave</span> scatterings by randomly distributed ice floes</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</p> <p>2016-11-01</p> <p>This study presents a continuum approach using a diffusion approximation method to solve the scattering of <span class="hlt">ocean</span> <span class="hlt">waves</span> by randomly distributed ice floes. In order to model both strong and weak scattering, the proposed method decomposes the <span class="hlt">wave</span> action density function into two parts: the transmitted part and the scattered part. For a given <span class="hlt">wave</span> direction, the transmitted part of the <span class="hlt">wave</span> action density is defined as the part of <span class="hlt">wave</span> action density in the same direction before the scattering; and the scattered part is a first order Fourier series approximation for the directional spreading caused by scattering. An additional approximation is also adopted for simplification, in which the net directional redistribution of <span class="hlt">wave</span> action by a single scatterer is assumed to be the reflected <span class="hlt">wave</span> action of a normally incident <span class="hlt">wave</span> into a semi-infinite ice cover. Other required input includes the mean shear modulus, diameter and thickness of ice floes, and the ice concentration. The directional spreading of <span class="hlt">wave</span> energy from the diffusion approximation is found to be in reasonable agreement with the previous solution using the Boltzmann equation. The diffusion model provides an alternative method to implement <span class="hlt">wave</span> scattering into an operational <span class="hlt">wave</span> model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2011JPhCS.305a2088K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2011JPhCS.305a2088K"><span>Wireless <span class="hlt">power</span> transmission using ultrasonic 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>Kural, A.; Pullin, R.; Featherston, C.; Paget, C.; Holford, K.</p> <p>2011-07-01</p> <p>The unavailability of suitable <span class="hlt">power</span> supply at desired locations is currently an important obstacle in the development of distributed, wireless sensor networks for applications such as structural health monitoring of aircraft. Proposed solutions range from improved batteries to energy harvesting from vibration, temperature gradients and other sources. A novel approach is being investigated at Cardiff University School of Engineering in cooperation with Airbus. It aims to utilise ultrasonic guided Lamb <span class="hlt">waves</span> to transmit energy through the aircraft skin. A vibration generator is to be placed in a location where electricity supply is readily available. Ultrasonic <span class="hlt">waves</span> generated by this device will travel through the aircraft structure to a receiver in a remote wireless sensor node. The receiver will convert the mechanical vibration of the ultrasonic <span class="hlt">waves</span> back to electricity, which will be used to <span class="hlt">power</span> the sensor node. This paper describes the measurement and modelling of the interference pattern which emerges when Lamb <span class="hlt">waves</span> are transmitted continuously as in this <span class="hlt">power</span> transmission application. The discovered features of the pattern, such as a large signal amplitude variation and a relatively high frequency, are presented and their importance for the development of a <span class="hlt">power</span> transmission system is discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA470198','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA470198"><span>Tropical <span class="hlt">Wave</span>-Induced <span class="hlt">Oceanic</span> Eddies at Cabo Corrientes and the Maria Islands, Mexico</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2007-05-30</p> <p><span class="hlt">Waves</span> Induce <span class="hlt">Oceanic</span> Eddies at Cabo Corrientes and the Maria Islands, Mexico 5b. GRANT NUMBER 5c. PROGRAM ELEMENT NUMBER 0601153N 6. AUTHOR(S) 5d...Research Laboratory (NRL) Layered <span class="hlt">Ocean</span> Model (NLOM) show the existence of anticyclonic eddies in the Cabo Corrientes - Maria Islands region off the...Mexican West Coast. Analysis of the results demonstrates that: (1) The Cabo Corrientes - Maria Islands region is characterized by mean poleward coastal</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830005504','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830005504"><span>Exploitation of SAR data for measurement of <span class="hlt">ocean</span> currents and <span class="hlt">wave</span> velocities</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Shuchman, R. A.; Lyzenga, D. R.; Klooster, A., Jr.</p> <p>1981-01-01</p> <p>Methods of extracting information on <span class="hlt">ocean</span> currents and <span class="hlt">wave</span> orbital velocities from SAR data by an analysis of the Doppler frequency content of the data are discussed. The theory and data analysis methods are discussed, and results are presented for both aircraft and satellite (SEASAT) data sets. A method of measuring the phase velocity of a gravity <span class="hlt">wave</span> field is also described. This method uses the shift in position of the <span class="hlt">wave</span> crests on two images generated from the same data set using two separate Doppler bands. Results of the current measurements are pesented for 11 aircraft data sets and 4 SEASAT data sets.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1418672','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1418672"><span><span class="hlt">Wave</span> Energy Prize - 1/50th Testing - RTI <span class="hlt">Wave</span> <span class="hlt">Power</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Wesley Scharmen</p> <p>2015-12-18</p> <p>This submission of data includes all the 1/50th scale testing data completed on the <span class="hlt">Wave</span> Energy Prize for the RTI <span class="hlt">Wave</span> <span class="hlt">Power</span> team, and includes: 1/50th test data (raw & processed) 1/50th test data video and pictures 1/50th Test plans and testing documents SSTF_Submission (summarized results)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1415592','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1415592"><span><span class="hlt">Wave</span> Energy Prize - 1/20th Testing - RTI <span class="hlt">Wave</span> <span class="hlt">Power</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Scharmen, Wesley</p> <p>2016-09-30</p> <p>Data from the 1/20th scale testing data completed on the <span class="hlt">Wave</span> Energy Prize for the RTI <span class="hlt">Wave</span> <span class="hlt">Power</span> team, including the 1/20th Test Plan, raw test data, video, photos, and data analysis results. The top level objective of the 1/20th scale device testing is to obtain the necessary measurements required for determining Average Climate Capture Width per Characteristic Capital Expenditure (ACE) and the Hydrodynamic Performance Quality (HPQ), key metrics for determining the <span class="hlt">Wave</span> Energy Prize (WEP) winners.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1917132A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1917132A"><span>Wind <span class="hlt">waves</span> climatology of the Southeast Pacific <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Aguirre, Catalina; Rutllant, José; Falvey, Mark</p> <p>2017-04-01</p> <p>The Southeast Pacific coast still lacks a high-resolution <span class="hlt">wave</span> hindcast and a detailed description of its <span class="hlt">wave</span> climatology. Since buoy <span class="hlt">wave</span> measurements are particularly scarce along the coast of South America, a model hindcast forced with wind information derived from atmospheric Reanalysis seems an attractive way to generate a <span class="hlt">wave</span> climatology in this poorly studied region, providing far better spatial and temporal coverage than can be achieved using observational data alone. Here, the climatology of wind <span class="hlt">waves</span> over the Southeast Pacific is analyzed using a 32-year hindcast from the <span class="hlt">Wave</span>Watch III model, complemented by satellite-derived Significant <span class="hlt">Wave</span> Height (SWH) and buoy measurements for validation. Using partitioned spectral data, a regional climatology of wind sea and swell parameters was constructed. In general, the simulated SWH shows a good agreement with satellite and in-situ SWH measurements. The spatial pattern of SWH is clearly influenced by the meridional variation of mean surface wind speed, where the stronger winds over the Southern <span class="hlt">Ocean</span> play a significant role generating higher <span class="hlt">waves</span> at higher latitudes. Nevertheless, regional features are observed in the annual variability of SWH, which are associated with the existence of atmospheric coastal low-level jets off the coast of Peru and central Chile. In particular, the seasonal variation of these synoptic scale jets shows a direct relationship with the annual variability of SWH. Off the coast of Peru at 15°S the coastal low-level jet is strongest during austral winter, increasing the wind sea SWH. In contrast, off central Chile, there is an important increase of wind sea SWH during summer. The seasonal variation of the wind sea component leads to a contrasting seasonal variation of the total SWH at these locations: off Peru the coastal jet amplifies the annual variability of SWH, while off Central Chile the annual variability of SWH is suppressed by the presence of the coastal jet.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/23144824','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23144824"><span>Catching the right <span class="hlt">wave</span>: evaluating <span class="hlt">wave</span> energy resources and potential compatibility with existing marine and coastal uses.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Choong-Ki; Toft, Jodie E; Papenfus, Michael; Verutes, Gregory; Guerry, Anne D; Ruckelshaus, Marry H; Arkema, Katie K; Guannel, Gregory; Wood, Spencer A; Bernhardt, Joanna R; Tallis, Heather; Plummer, Mark L; Halpern, Benjamin S; Pinsky, Malin L; Beck, Michael W; Chan, Francis; Chan, Kai M A; Levin, Phil S; Polasky, Stephen</p> <p>2012-01-01</p> <p>Many hope that <span class="hlt">ocean</span> <span class="hlt">waves</span> will be a source for clean, safe, reliable and affordable energy, yet <span class="hlt">wave</span> energy conversion facilities may affect marine ecosystems through a variety of mechanisms, including competition with other human uses. We developed a decision-support tool to assist siting <span class="hlt">wave</span> energy facilities, which allows the user to balance the need for profitability of the facilities with the need to minimize conflicts with other <span class="hlt">ocean</span> uses. Our <span class="hlt">wave</span> energy model quantifies harvestable <span class="hlt">wave</span> energy and evaluates the net present value (NPV) of a <span class="hlt">wave</span> energy facility based on a capital investment analysis. The model has a flexible framework and can be easily applied to <span class="hlt">wave</span> energy projects at local, regional, and global scales. We applied the model and compatibility analysis on the west coast of Vancouver Island, British Columbia, Canada to provide information for ongoing marine spatial planning, including potential <span class="hlt">wave</span> energy projects. In particular, we conducted a spatial overlap analysis with a variety of existing uses and ecological characteristics, and a quantitative compatibility analysis with commercial fisheries data. We found that <span class="hlt">wave</span> <span class="hlt">power</span> and harvestable <span class="hlt">wave</span> energy gradually increase offshore as <span class="hlt">wave</span> conditions intensify. However, areas with high economic potential for <span class="hlt">wave</span> energy facilities were closer to cable landing points because of the cost of bringing energy ashore and thus in nearshore areas that support a number of different human uses. We show that the maximum combined economic benefit from <span class="hlt">wave</span> energy and other uses is likely to be realized if <span class="hlt">wave</span> energy facilities are sited in areas that maximize <span class="hlt">wave</span> energy NPV and minimize conflict with existing <span class="hlt">ocean</span> uses. Our tools will help decision-makers explore alternative locations for <span class="hlt">wave</span> energy facilities by mapping expected <span class="hlt">wave</span> energy NPV and helping to identify sites that provide maximal returns yet avoid spatial competition with existing <span class="hlt">ocean</span> uses.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3492388','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=3492388"><span>Catching the Right <span class="hlt">Wave</span>: Evaluating <span class="hlt">Wave</span> Energy Resources and Potential Compatibility with Existing Marine and Coastal Uses</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Kim, Choong-Ki; Toft, Jodie E.; Papenfus, Michael; Verutes, Gregory; Guerry, Anne D.; Ruckelshaus, Marry H.; Arkema, Katie K.; Guannel, Gregory; Wood, Spencer A.; Bernhardt, Joanna R.; Tallis, Heather; Plummer, Mark L.; Halpern, Benjamin S.; Pinsky, Malin L.; Beck, Michael W.; Chan, Francis; Chan, Kai M. A.; Levin, Phil S.; Polasky, Stephen</p> <p>2012-01-01</p> <p>Many hope that <span class="hlt">ocean</span> <span class="hlt">waves</span> will be a source for clean, safe, reliable and affordable energy, yet <span class="hlt">wave</span> energy conversion facilities may affect marine ecosystems through a variety of mechanisms, including competition with other human uses. We developed a decision-support tool to assist siting <span class="hlt">wave</span> energy facilities, which allows the user to balance the need for profitability of the facilities with the need to minimize conflicts with other <span class="hlt">ocean</span> uses. Our <span class="hlt">wave</span> energy model quantifies harvestable <span class="hlt">wave</span> energy and evaluates the net present value (NPV) of a <span class="hlt">wave</span> energy facility based on a capital investment analysis. The model has a flexible framework and can be easily applied to <span class="hlt">wave</span> energy projects at local, regional, and global scales. We applied the model and compatibility analysis on the west coast of Vancouver Island, British Columbia, Canada to provide information for ongoing marine spatial planning, including potential <span class="hlt">wave</span> energy projects. In particular, we conducted a spatial overlap analysis with a variety of existing uses and ecological characteristics, and a quantitative compatibility analysis with commercial fisheries data. We found that <span class="hlt">wave</span> <span class="hlt">power</span> and harvestable <span class="hlt">wave</span> energy gradually increase offshore as <span class="hlt">wave</span> conditions intensify. However, areas with high economic potential for <span class="hlt">wave</span> energy facilities were closer to cable landing points because of the cost of bringing energy ashore and thus in nearshore areas that support a number of different human uses. We show that the maximum combined economic benefit from <span class="hlt">wave</span> energy and other uses is likely to be realized if <span class="hlt">wave</span> energy facilities are sited in areas that maximize <span class="hlt">wave</span> energy NPV and minimize conflict with existing <span class="hlt">ocean</span> uses. Our tools will help decision-makers explore alternative locations for <span class="hlt">wave</span> energy facilities by mapping expected <span class="hlt">wave</span> energy NPV and helping to identify sites that provide maximal returns yet avoid spatial competition with existing <span class="hlt">ocean</span> uses. PMID:23144824</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JAMES..10..801P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JAMES..10..801P"><span>A New Coupled <span class="hlt">Ocean-Waves</span>-Atmosphere Model Designed for Tropical Storm Studies: Example of Tropical Cyclone Bejisa (2013-2014) in the South-West Indian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pianezze, J.; Barthe, C.; Bielli, S.; Tulet, P.; Jullien, S.; Cambon, G.; Bousquet, O.; Claeys, M.; Cordier, E.</p> <p>2018-03-01</p> <p><span class="hlt">Ocean-Waves</span>-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 <span class="hlt">oceanic</span> model CROCO, and the <span class="hlt">wave</span> 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 <span class="hlt">wave</span> height is within 30 cm of measurements made with buoys and altimeters. Short-term (< 2 days) sensitivity experiments used to highlight the effect of <span class="hlt">oceanic</span> <span class="hlt">waves</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..16.4707L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..16.4707L"><span>ADDOSS: Autonomously Deployed Deep-<span class="hlt">ocean</span> Seismic System - Communications Gateway for <span class="hlt">Ocean</span> Observatories</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Laske, Gabi; Berger, Jon; Orcutt, John; Babcock, Jeff</p> <p>2014-05-01</p> <p>We describe an autonomously deployable, communications gateway designed to provide long-term and near real-time data from <span class="hlt">ocean</span> observatories. The key features of this new system are its abilities to telemeter sensor data from the seafloor to shore without cables or moorings, and to be deployed without a ship, thereby greatly reducing life-cycle costs. The free-floating surface communications gateway utilizes a Liquid Robotics <span class="hlt">wave</span> glider comprising a surfboard-sized float towed by a tethered, submerged glider, which converts <span class="hlt">wave</span> motion into thrust. For navigation, the <span class="hlt">wave</span> glider is equipped with a small computer, a GPS receiver, a rudder, solar panels and batteries, and an Iridium satellite modem. Acoustic communications connect the subsea instruments and the surface gateway while communications between the gateway and land are provided by the Iridium satellite constellation. <span class="hlt">Wave</span> gliders have demonstrated trans-<span class="hlt">oceanic</span> range and long-term station keeping capabilities. The acoustics communications package is mounted in a shallow tow body which utilizes a WHOI micro modem and a Benthos low frequency, directional transducer. A matching modem and transducer is mounted on the <span class="hlt">ocean</span> bottom package. Tests of the surface gateway in 4350 m of water demonstrated an acoustic efficiency of approximately 396 bits/J. For example, it has the ability to send 4 channels of compressed, 1 sample per second data from the <span class="hlt">ocean</span> bottom to the gateway with an average <span class="hlt">power</span> draw of approximately 0.15 W and a latency of less than 3 minutes. This gateway is used to send near real-time data from a broadband <span class="hlt">ocean</span> bottom seismic observatory, first during short week-to-months long test deployments but will ultimately be designed for a two-year operational life. Such data from presently unobserved <span class="hlt">oceanic</span> areas are critical for both national and international agencies in monitoring and characterizing earthquakes, tsunamis, and nuclear explosions. We present initial results from a two short</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013EGUGA..1514021G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013EGUGA..1514021G"><span>Modelling of upper <span class="hlt">ocean</span> mixing by <span class="hlt">wave</span>-induced turbulence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ghantous, Malek; Babanin, Alexander</p> <p>2013-04-01</p> <p>Mixing of the upper <span class="hlt">ocean</span> affects the sea surface temperature by bringing deeper, colder water to the surface. Because even small changes in the surface temperature can have a large impact on weather and climate, accurately determining the rate of mixing is of central importance for forecasting. Although there are several mixing mechanisms, one that has until recently been overlooked is the effect of turbulence generated by non-breaking, wind-generated surface <span class="hlt">waves</span>. Lately there has been a lot of interest in introducing this mechanism into models, and real gains have been made in terms of increased fidelity to observational data. However our knowledge of the mechanism is still incomplete. We indicate areas where we believe the existing models need refinement and propose an alternative model. We use two of the models to demonstrate the effect on the mixed layer of <span class="hlt">wave</span>-induced turbulence by applying them to a one-dimensional mixing model and a stable temperature profile. Our modelling experiment suggests a strong effect on sea surface temperature due to non-breaking <span class="hlt">wave</span>-induced turbulent mixing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFMSM43C..05H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFMSM43C..05H"><span>Pc-5 <span class="hlt">wave</span> <span class="hlt">power</span> in the plasmasphere and trough: CRRES observations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hartinger, M.; Moldwin, M.; Angelopoulos, V.; Takahashi, K.; Singer, H. J.; Anderson, R. R.</p> <p>2009-12-01</p> <p>The CRRES (Combined Release and Radiation Effects Satellite) mission provides an opportunity to study the distribution of MHD <span class="hlt">wave</span> <span class="hlt">power</span> in the inner magnetosphere both inside the high-density plasmasphere and in the low-density trough. We present a statistical survey of Pc-5 <span class="hlt">wave</span> <span class="hlt">power</span> using CRRES magnetometer and plasma <span class="hlt">wave</span> data separated into plasmasphere and trough intervals. Using a database of plasmapause crossings, we examined differences in <span class="hlt">power</span> spectral density between the plasmasphere and trough regions. We found significant differences between the plasmasphere and trough in the radial profiles of Pc-5 <span class="hlt">wave</span> <span class="hlt">power</span>. On average, <span class="hlt">wave</span> <span class="hlt">power</span> was higher in the trough, but the difference in <span class="hlt">power</span> depended on magnetic local time. Our study shows that determining the plasmapause location is important for understanding and modeling the MHD <span class="hlt">wave</span> environment in the Pc-5 frequency band.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA539815','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA539815"><span>Forecasting <span class="hlt">Ocean</span> <span class="hlt">Waves</span>: Comparing a Physics-Based Model with Statistical Models</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2011-01-01</p> <p>m) 46029 (135 m) 46211 (38 m) ( CDIP -036) 42039 (307 m) 42040 (165 m) 42007 (14 m) Boundary forcing from NCEP WW3 ENP 15′×15′ resolution SWAN CNW-G1...<span class="hlt">wave</span> energy. Acronyms and abbreviations CenGOOS Central Gulf <span class="hlt">Ocean</span> Observing System CDIP Coastal Data Information Program CNW Coastal Northwest SWAN</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1415598','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1415598"><span><span class="hlt">Wave</span> Energy Prize - 1/50th Testing - Advanced <span class="hlt">Ocean</span> Energy @ VT</span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Wesley Scharmen</p> <p>2016-01-29</p> <p>This submission of data includes all the 1/50th scale testing data completed on the <span class="hlt">Wave</span> Energy Prize for the for the Advanced <span class="hlt">Ocean</span> Energy @VT team, and includes: 1/50th test data (raw & processed) 1/50th test data video and pictures 1/50th Test plans and testing documents SSTF_Submission (summarized results)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1032481','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1032481"><span>Radar Measurements of <span class="hlt">Ocean</span> Surface <span class="hlt">Waves</span> using Proper Orthogonal Decomposition</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2017-03-30</p> <p>rely on use of Fourier transforms (FFT) and filtering spectra on the linear dispersion relationship for <span class="hlt">ocean</span> surface <span class="hlt">waves</span>. This report discusses...the measured signal (e.g., Young et al., 1985). In addition, the methods often rely on filtering the FFT of radar backscatter or Doppler velocities...to those obtained with conventional FFT and dispersion curve filtering techniques (iv) Compare both results of(iii) to ground truth sensors (i .e</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19760017773','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19760017773"><span>Transformation of apparent <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra observed from an aircraft sensor platform</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Poole, L. R.</p> <p>1976-01-01</p> <p>The problem considered was transformation of a unidirectional apparent <span class="hlt">ocean</span> <span class="hlt">wave</span> spectrum observed from an aircraft sensor platform into the true spectrum that would be observed from a stationary platform. Spectral transformation equations were developed in terms of the linear <span class="hlt">wave</span> dispersion relationship and the <span class="hlt">wave</span> group speed. An iterative solution to the equations was outlined and used to transform reference theoretical apparent spectra for several assumed values of average water depth. Results show that changing the average water depth leads to a redistribution of energy density among the various frequency bands of the transformed spectrum. This redistribution is most severe when much of the energy density is expected, a priori, to reside at relatively low true frequencies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840019207','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840019207"><span>Synthetic aperture radar images of <span class="hlt">ocean</span> <span class="hlt">waves</span>, theories of imaging physics and experimental tests</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vesecky, J. F.; Durden, S. L.; Smith, M. P.; Napolitano, D. A.</p> <p>1984-01-01</p> <p>The physical mechanism for the synthetic Aperture Radar (SAR) imaging of <span class="hlt">ocean</span> <span class="hlt">waves</span> is investigated through the use of analytical models. The models are tested by comparison with data sets from the SEASAT mission and airborne SAR's. Dominant <span class="hlt">ocean</span> wavelengths from SAR estimates are biased towards longer wavelengths. The quasispecular scattering mechanism agrees with experimental data. The Doppler shift for ship wakes is that of the mean sea surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010RvGeo..48.4006W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010RvGeo..48.4006W"><span>Impact of a Cosmic Body into Earth's <span class="hlt">Ocean</span> and the Generation of Large Tsunami <span class="hlt">Waves</span>: Insight from Numerical Modeling</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wünnemann, K.; Collins, G. S.; Weiss, R.</p> <p>2010-12-01</p> <p>The strike of a cosmic body into a marine environment differs in several respects from impact on land. <span class="hlt">Oceans</span> cover approximately 70% of the Earth's surface, implying not only that <span class="hlt">oceanic</span> impact is a very likely scenario for future impacts but also that most impacts in Earth's history must have happened in marine environments. Therefore, the study of <span class="hlt">oceanic</span> impact is imperative in two respects: (1) to quantify the hazard posed by future <span class="hlt">oceanic</span> impacts, including the potential threat of large impact-generated tsunami-like <span class="hlt">waves</span>, and (2) to reconstruct Earth's impact record by accounting for the large number of potentially undiscovered crater structures in the <span class="hlt">ocean</span> crust. Reconstruction of the impact record is of crucial importance both for assessing the frequency of collision events in the past and for better predicting the probability of future impact. We summarize the advances in the study of <span class="hlt">oceanic</span> impact over the last decades and focus in particular on how numerical models have improved our understanding of cratering in the <span class="hlt">oceanic</span> environment and the generation of <span class="hlt">waves</span> by impact. We focus on insight gleaned from numerical modeling studies into the deceleration of the projectile by the water, cratering of the <span class="hlt">ocean</span> floor, the late stage modification of the crater due to gravitational collapse, and water resurge. Furthermore, we discuss the generation and propagation of large tsunami-like <span class="hlt">waves</span> as a result of a strike of a cosmic body in marine environments.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_11");'>11</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li class="active"><span>13</span></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_13 --> <div id="page_14" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_12");'>12</a></li> <li><a href="#" onclick='return showDiv("page_13");'>13</a></li> <li class="active"><span>14</span></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="261"> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/973333','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/973333"><span>Subsurface Hybrid <span class="hlt">Power</span> Options for Oil & Gas Production at Deep <span class="hlt">Ocean</span> Sites</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>Farmer, J C; Haut, R; Jahn, G</p> <p>2010-02-19</p> <p>An investment in deep-sea (deep-<span class="hlt">ocean</span>) hybrid <span class="hlt">power</span> systems may enable certain off-shore oil and gas exploration and production. Advanced deep-<span class="hlt">ocean</span> drilling and production operations, locally <span class="hlt">powered</span>, may provide commercial access to oil and gas reserves otherwise inaccessible. Further, subsea generation of electrical <span class="hlt">power</span> has the potential of featuring a low carbon output resulting in improved environmental conditions. Such technology therefore, enhances the energy security of the United States in a green and environmentally friendly manner. The objective of this study is to evaluate alternatives and recommend equipment to develop into hybrid energy conversion and storage systems for deep <span class="hlt">ocean</span> operations.more » Such <span class="hlt">power</span> systems will be located on the <span class="hlt">ocean</span> floor and will be used to <span class="hlt">power</span> offshore oil and gas exploration and production operations. Such <span class="hlt">power</span> systems will be located on the <span class="hlt">oceans</span> floor, and will be used to supply oil and gas exploration activities, as well as drilling operations required to harvest petroleum reserves. The following conceptual hybrid systems have been identified as candidates for <span class="hlt">powering</span> sub-surface oil and gas production operations: (1) PWR = Pressurized-Water Nuclear Reactor + Lead-Acid Battery; (2) FC1 = Line for Surface O{sub 2} + Well Head Gas + Reformer + PEMFC + Lead-Acid & Li-Ion Batteries; (3) FC2 = Stored O2 + Well Head Gas + Reformer + Fuel Cell + Lead-Acid & Li-Ion Batteries; (4) SV1 = Submersible Vehicle + Stored O{sub 2} + Fuel Cell + Lead-Acid & Li-Ion Batteries; (5) SV2 = Submersible Vehicle + Stored O{sub 2} + Engine or Turbine + Lead-Acid & Li-Ion Batteries; (6) SV3 = Submersible Vehicle + Charge at Docking Station + ZEBRA & Li-Ion Batteries; (7) PWR TEG = PWR + Thermoelectric Generator + Lead-Acid Battery; (8) WELL TEG = Thermoelectric Generator + Well Head Waste Heat + Lead-Acid Battery; (9) GRID = <span class="hlt">Ocean</span> Floor Electrical Grid + Lead-Acid Battery; and (10) DOC = Deep <span class="hlt">Ocean</span> Current + Lead-Acid Battery.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26963021','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26963021"><span>Spinal Cord Injuries in <span class="hlt">Wave</span>-Riding Sports: The Influence of Environmental and Sport-Specific Factors.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Falconi, Audrey; Flick, David; Ferguson, Jason; Glorioso, John E</p> <p>2016-01-01</p> <p>Spinal cord injury is a nonfatal, catastrophic consequence of <span class="hlt">wave</span>-riding sports. With surfing at the core, a multitude of activities have evolved that attempt to harness the <span class="hlt">power</span> of <span class="hlt">ocean</span> <span class="hlt">waves</span>. The unique qualities of each <span class="hlt">wave</span>-riding sport, in combination with the environmental factors of the <span class="hlt">ocean</span>, define the risk for potential injuries. As <span class="hlt">wave</span>-riding sports have become more advanced, athletes continue to push physical barriers. Taller <span class="hlt">waves</span> are attempted while incorporating aerial maneuvers, all without protective equipment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA586450','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA586450"><span>Impact of Parameterized Lee <span class="hlt">Wave</span> Drag on the Energy Budget of an Eddying Global <span class="hlt">Ocean</span> Model</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2013-08-26</p> <p>Teixeira, J., Peng, M., Hogan, T.F., Pauley, R., 2002. Navy Operational Global Atmospheric Prediction System (NOGAPS): Forcing for <span class="hlt">ocean</span> models...Impact of parameterized lee <span class="hlt">wave</span> drag on the energy budget of an eddying global <span class="hlt">ocean</span> model David S. Trossman a,⇑, Brian K. Arbic a, Stephen T...input and output terms in the total mechanical energy budget of a hybrid coordinate high-resolution global <span class="hlt">ocean</span> general circulation model forced by winds</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24116520','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24116520"><span>A numerical model for <span class="hlt">ocean</span> ultra-low frequency noise: <span class="hlt">wave</span>-generated acoustic-gravity and Rayleigh modes.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ardhuin, Fabrice; Lavanant, Thibaut; Obrebski, Mathias; Marié, Louis; Royer, Jean-Yves; d'Eu, Jean-François; Howe, Bruce M; Lukas, Roger; Aucan, Jerome</p> <p>2013-10-01</p> <p>The generation of ultra-low frequency acoustic noise (0.1 to 1 Hz) by the nonlinear interaction of <span class="hlt">ocean</span> surface gravity <span class="hlt">waves</span> is well established. More controversial are the quantitative theories that attempt to predict the recorded noise levels and their variability. Here a single theoretical framework is used to predict the noise level associated with propagating pseudo-Rayleigh modes and evanescent acoustic-gravity modes. The latter are dominant only within 200 m from the sea surface, in shallow or deep water. At depths larger than 500 m, the comparison of a numerical noise model with hydrophone records from two open-<span class="hlt">ocean</span> sites near Hawaii and the Kerguelen islands reveal: (a) Deep <span class="hlt">ocean</span> acoustic noise at frequencies 0.1 to 1 Hz is consistent with the Rayleigh <span class="hlt">wave</span> theory, in which the presence of the <span class="hlt">ocean</span> bottom amplifies the noise by 10 to 20 dB; (b) in agreement with previous results, the local maxima in the noise spectrum support the theoretical prediction for the vertical structure of acoustic modes; and (c) noise level and variability are well predicted for frequencies up to 0.4 Hz. Above 0.6 Hz, the model results are less accurate, probably due to the poor estimation of the directional properties of wind-<span class="hlt">waves</span> with frequencies higher than 0.3 Hz.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830005273','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830005273"><span>Aircraft and satellite measurement of <span class="hlt">ocean</span> <span class="hlt">wave</span> directional spectra using scanning-beam microwave radars</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jackson, F. C.; Walton, W. T.; Baker, P. L.</p> <p>1982-01-01</p> <p>A microwave radar technique for remotely measuring the vector <span class="hlt">wave</span> number spectrum of the <span class="hlt">ocean</span> surface is described. The technique, which employs short-pulse, noncoherent radars in a conical scan mode near vertical incidence, is shown to be suitable for both aircraft and satellite application, the technique was validated at 10 km aircraft altitude, where we have found excellent agreement between buoy and radar-inferred absolute <span class="hlt">wave</span> height spectra.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMIN41D..07B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMIN41D..07B"><span>A Deep-<span class="hlt">Ocean</span> Observatory with Near Real-time Telemetry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Berger, J.; Orcutt, J. A.; Laske, G.</p> <p>2014-12-01</p> <p>We describe an autonomously deployable, deep-<span class="hlt">ocean</span> observatory designed to provide long term and near-real-time observations from sites far offshore. The key feature of this new system is its ability to telemeter sensor data from the seafloor to shore without a cable or moored surface buoy. In the future the observatory will be deployable without a ship. The first application of this system is seismology. While permanent <span class="hlt">ocean</span> seismic stations on the seafloor have long been a goal of global seismology, today there are still no <span class="hlt">ocean</span> bottom stations in the Global Seismographic Network, mostly for reasons of life-cycle costs. Yet real-time data from stations in <span class="hlt">oceanic</span> areas are critical for both national and international agencies in monitoring and characterizing earthquakes, tsunamis, and nuclear explosions. The system comprises an <span class="hlt">ocean</span> bottom instrumentation package and a free-floating surface communications gateway, which uses a Liquid Robotics <span class="hlt">wave</span> glider. The glider consists of a surfboard-sized float propelled by a tethered, submerged glider, which converts <span class="hlt">wave</span> motion into thrust. For navigation, the <span class="hlt">wave</span> gliders are equipped with a small computer, a GPS receiver, a rudder, solar panels and batteries, and an Iridium satellite modem. <span class="hlt">Wave</span> gliders have demonstrated trans-<span class="hlt">oceanic</span> range combined with long-term station holding. The 'communications gateway,' which provides the means of communicating between the <span class="hlt">ocean</span> bottom package and land comprises a <span class="hlt">wave</span> glider and a towed acoustic communications 'tow body'. Acoustic communications connect the subsea instruments and the surface gateway while communications between the gateway and land is provided by the Iridium satellite constellation. Tests of the surface gateway in 4350 m of water demonstrated the ability to send four channels of compressed 24-bit, 1 sample per second data from the <span class="hlt">ocean</span> bottom to the gateway with an average <span class="hlt">power</span> draw of approximately 0.2 W.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014NPGeo..21..325G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014NPGeo..21..325G"><span>One-dimensional modelling of upper <span class="hlt">ocean</span> mixing by turbulence due to <span class="hlt">wave</span> orbital motion</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ghantous, M.; Babanin, A. V.</p> <p>2014-02-01</p> <p>Mixing of the upper <span class="hlt">ocean</span> affects the sea surface temperature by bringing deeper, colder water to the surface. Because even small changes in the surface temperature can have a large impact on weather and climate, accurately determining the rate of mixing is of central importance for forecasting. Although there are several mixing mechanisms, one that has until recently been overlooked is the effect of turbulence generated by non-breaking, wind-generated surface <span class="hlt">waves</span>. Lately there has been a lot of interest in introducing this mechanism into <span class="hlt">ocean</span> mixing models, and real gains have been made in terms of increased fidelity to observational data. However, our knowledge of the mechanism is still incomplete. We indicate areas where we believe the existing parameterisations need refinement and propose an alternative one. We use two of the parameterisations to demonstrate the effect on the mixed layer of <span class="hlt">wave</span>-induced turbulence by applying them to a one-dimensional mixing model and a stable temperature profile. Our modelling experiment suggests a strong effect on sea surface temperature due to non-breaking <span class="hlt">wave</span>-induced turbulent mixing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMOS43F..07K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMOS43F..07K"><span>Modeling the <span class="hlt">Ocean</span> Tide for Tidal <span class="hlt">Power</span> Generation Applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kawase, M.; Gedney, M.</p> <p>2014-12-01</p> <p>Recent years have seen renewed interest in the <span class="hlt">ocean</span> tide as a source of energy for electrical <span class="hlt">power</span> generation. Unlike in the 1960s, when the tidal barrage was the predominant method of <span class="hlt">power</span> extraction considered and implemented, the current methodology favors operation of a free-stream turbine or an array of them in strong tidal currents. As tidal <span class="hlt">power</span> generation moves from pilot-scale projects to actual array implementations, numerical modeling of tidal currents is expected to play an increasing role in site selection, resource assessment, array design, and environmental impact assessment. In this presentation, a simple, coupled <span class="hlt">ocean</span>/estuary model designed for research into fundamental aspects of tidal <span class="hlt">power</span> generation is described. The model consists of a Pacific <span class="hlt">Ocean</span>-size rectangular basin and a connected fjord-like embayment with dimensions similar to that of Puget Sound, Washington, one of the potential <span class="hlt">power</span> generation sites in the United States. The model is forced by an idealized lunar tide-generating potential. The study focuses on the energetics of a tidal system including tidal <span class="hlt">power</span> extraction at both global and regional scales. The hyperbolic nature of the governing shallow water equations means consequence of tidal <span class="hlt">power</span> extraction cannot be limited to the local waters, but is global in extent. Modeling <span class="hlt">power</span> extraction with a regional model with standard boundary conditions introduces uncertainties of 3 ~ 25% in the <span class="hlt">power</span> extraction estimate depending on the level of extraction. <span class="hlt">Power</span> extraction in the model has a well-defined maximum (~800 MW in a standard case) that is in agreement with previous theoretical studies. Natural energy dissipation and tidal <span class="hlt">power</span> extraction strongly interact; for a turbine array of a given capacity, the higher the level of natural dissipation the lower the <span class="hlt">power</span> the array can extract. Conversely, <span class="hlt">power</span> extraction leads to a decrease in the level of natural dissipation (Figure) as well as the tidal range and the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OcDyn..68..327D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OcDyn..68..327D"><span>Revisiting tropical instability <span class="hlt">wave</span> variability in the Atlantic <span class="hlt">ocean</span> using SODA reanalysis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>de Decco, Hatsue Takanaca; Torres Junior, Audalio Rebelo; Pezzi, Luciano Ponzi; Landau, Luiz</p> <p>2018-03-01</p> <p>The spatial and temporal variability of energy exchange in Tropical Instability <span class="hlt">Waves</span> (TIWs) in the Atlantic <span class="hlt">Ocean</span> were investigated. A spectral analysis was used to filter the 5-day mean results from Simple <span class="hlt">Ocean</span> Data Assimilation (SODA) reanalysis spanning from 1958 to 2008. TIWs were filtered over periods of 15 to 60 days and between wavelengths of 4 and 20 longitude degrees. The main approach of this study was the use of bidirectionally filtered TIW time series as the perturbation fields, and the difference in these time series from the SODA total results was considered to be the basic state for energetics analysis. The main result was that the annual cycle (period of 360 days) was the main source of variability of the <span class="hlt">waves</span>, and the semi-annual cycle (period of 180 days) was a secondary variation, which indicated that TIWs occurred throughout the year but with intensity that varies seasonally. In SODA, barotropic instability acts as the mechanism that feeds and extracts energy to/from TIWs at equatorial Atlantic. Baroclinic instability is the main mechanism that extracts energy from TIWs to the equatorial circulation north of the Equator. All TIW patterns of variability were observed western of 10° W. The present study reveals new evidences regarding TIW variability and suggests that future investigations should include a detailed description of TIW dynamics as part of Atlantic <span class="hlt">Ocean</span> equatorial circulation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CSR...146..102W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CSR...146..102W"><span>Assessing the performance of formulations for nonlinear feedback of surface gravity <span class="hlt">waves</span> on <span class="hlt">ocean</span> currents over coastal waters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Pengcheng; Sheng, Jinyu; Hannah, Charles</p> <p>2017-08-01</p> <p>This study presents applications of a two-way coupled <span class="hlt">wave</span>-circulation modelling system over coastal waters, with a special emphasis of performance assessments of two different methods for nonlinear feedback of <span class="hlt">ocean</span> surface gravity <span class="hlt">waves</span> on three-dimensional (3D) <span class="hlt">ocean</span> 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 <span class="hlt">wave</span>-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 <span class="hlt">wave</span> forces to the 3D <span class="hlt">ocean</span> circulation over coastal waters. However, the RS formulation generates some weak unphysical currents outside the <span class="hlt">wave</span> 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 <span class="hlt">waves</span>, degrading the model performance in simulating currents at one observation site. Our results demonstrate that the VF formulation with an appropriate parameterization of <span class="hlt">wave</span> breaking effects is able to produce reasonable results for applications over coastal waters during extreme weather events. The RS formulation requires a complex <span class="hlt">wave</span> theory rather than the linear <span class="hlt">wave</span> theory for the approximation of a vertical RS term to improve its performance under both breaking and non-breaking <span class="hlt">wave</span> conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19800000224&hterms=Tidal+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DTidal%2Bwaves','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19800000224&hterms=Tidal+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D70%26Ntt%3DTidal%2Bwaves"><span><span class="hlt">Oceanic-wave</span>-measurement system</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Holmes, J. F.; Miles, R. T.</p> <p>1980-01-01</p> <p>Barometer mounted on bouy senses <span class="hlt">wave</span> heights. As <span class="hlt">wave</span> motion raises and lowers barometer, pressure differential is proportional to <span class="hlt">wave</span> height. Monitoring circuit samples barometer output every half cycle of <span class="hlt">wave</span> motion and adds magnitudes of adjacent positive and negative peaks. Resulting output signals, proportional to <span class="hlt">wave</span> height, are transmitted to central monitoring station.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.7377K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.7377K"><span>Development of a GPS buoy system for monitoring tsunami, sea <span class="hlt">waves</span>, <span class="hlt">ocean</span> bottom crustal deformation and atmospheric water vapor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kato, Teruyuki; Terada, Yukihiro; Nagai, Toshihiko; Koshimura, Shun'ichi</p> <p>2010-05-01</p> <p>We have developed a GPS buoy system for monitoring tsunami for over 12 years. The idea was that a buoy equipped with a GPS antenna and placed offshore may be an effective way of monitoring tsunami before its arrival to the coast and to give warning to the coastal residents. The key technology for the system is real-time kinematic (RTK) GPS technology. We have successfully developed the system; we have detected tsunamis of about 10cm in height for three large earthquakes, namely, the 23 June 2001 Peru earthquake (Mw8.4), the 26 September 2003 Tokachi earthquake (Mw8.3) and the 5 September 2004 earthquake (Mw7.4). The developed GPS buoy system is also capable of monitoring sea <span class="hlt">waves</span> that are mainly caused by winds. Only the difference between tsunami and sea <span class="hlt">waves</span> is their frequency range and can be segregated each other by a simple filtering technique. Given the success of GPS buoy experiments, the system has been adopted as a part of the Nationwide <span class="hlt">Ocean</span> <span class="hlt">Wave</span> information system for Port and HArborS (NOWPHAS) by the Ministry of Land, Infrastructure, Transport and Tourism of Japan. They have established more than eight GPS buoys along the Japanese coasts and the system has been operated by the Port and Airport Research Institute. As a future scope, we are now planning to implement some other additional facilities for the GPS buoy system. The first application is a so-called GPS/Acoustic system for monitoring <span class="hlt">ocean</span> bottom crustal deformation. The system requires acoustic <span class="hlt">waves</span> to detect <span class="hlt">ocean</span> bottom reference position, which is the geometrical center of an array of transponders, by measuring distances between a position at the sea surface (vessel) and <span class="hlt">ocean</span> bottom equipments to return the received sonic <span class="hlt">wave</span>. The position of the vessel is measured using GPS. The system was first proposed by a research group at the Scripps Institution of Oceanography in early 1980's. The system was extensively developed by Japanese researchers and is now capable of detecting <span class="hlt">ocean</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018MS%26E..307a2009L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018MS%26E..307a2009L"><span>Research on Efficiency of a <span class="hlt">Wave</span> Energy Conversion System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lu, Zhongyue; Shang, Jianzhong; Luo, Zirong; Sun, Chongfei; Chen, Gewei</p> <p>2018-02-01</p> <p>The <span class="hlt">oceans</span> are rich in <span class="hlt">wave</span> energy that is green energy, and the <span class="hlt">wave</span> energy are now being used to generate electricity on a massive scale. It can also be used as a single generator for beacon, buoy or underwater vehicle. Micro small <span class="hlt">wave</span> energy <span class="hlt">power</span> generation device is a kind of <span class="hlt">wave</span> energy <span class="hlt">power</span> generation devices, main characteristic is mobility is good, and can be directly assembled on various kinds of equipment for the <span class="hlt">power</span> supply, with good prospects for development. The research object of the paper is a new adaptive reversing <span class="hlt">wave</span> energy generating device belongs to micro-sized <span class="hlt">wave</span> energy generating device. Using the upper and lower absorber blade groups, the low speed and large torque <span class="hlt">wave</span> energy can be converted into electric energy which can be used for load and lithium battery charging.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1415587','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1415587"><span><span class="hlt">Wave</span> Energy Prize - 1/20th Testing - Cal<span class="hlt">Wave</span> <span class="hlt">Power</span> Technologies</span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Scharmen, Wesley</p> <p>2016-09-09</p> <p>Data from the 1/20th scale testing data completed on the <span class="hlt">Wave</span> Energy Prize for the Cal<span class="hlt">Wave</span> <span class="hlt">Power</span> Technologies team, including the 1/20th scale test plan, raw test data, video, photos, and data analysis results. The top level objective of the 1/20th scale device testing is to obtain the necessary measurements required for determining Average Climate Capture Width per Characteristic Capital Expenditure (ACE) and the Hydrodynamic Performance Quality (HPQ), key metrics for determining the <span class="hlt">Wave</span> Energy Prize (WEP) winners.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017CG....107...28B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017CG....107...28B"><span>WASS: An open-source pipeline for 3D stereo reconstruction of <span class="hlt">ocean</span> <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>Bergamasco, Filippo; Torsello, Andrea; Sclavo, Mauro; Barbariol, Francesco; Benetazzo, Alvise</p> <p>2017-10-01</p> <p>Stereo 3D reconstruction of <span class="hlt">ocean</span> <span class="hlt">waves</span> is gaining more and more popularity in the oceanographic community and industry. Indeed, recent advances of both computer vision algorithms and computer processing <span class="hlt">power</span> now allow the study of the spatio-temporal <span class="hlt">wave</span> field with unprecedented accuracy, especially at small scales. Even if simple in theory, multiple details are difficult to be mastered for a practitioner, so that the implementation of a sea-<span class="hlt">waves</span> 3D reconstruction pipeline is in general considered a complex task. For instance, camera calibration, reliable stereo feature matching and mean sea-plane estimation are all factors for which a well designed implementation can make the difference to obtain valuable results. For this reason, we believe that the open availability of a well tested software package that automates the reconstruction process from stereo images to a 3D point cloud would be a valuable addition for future researches in this area. We present WASS (http://www.dais.unive.it/wass), an Open-Source stereo processing pipeline for sea <span class="hlt">waves</span> 3D reconstruction. Our tool completely automates all the steps required to estimate dense point clouds from stereo images. Namely, it computes the extrinsic parameters of the stereo rig so that no delicate calibration has to be performed on the field. It implements a fast 3D dense stereo reconstruction procedure based on the consolidated OpenCV library and, lastly, it includes set of filtering techniques both on the disparity map and the produced point cloud to remove the vast majority of erroneous points that can naturally arise while analyzing the optically complex nature of the water surface. In this paper, we describe the architecture of WASS and the internal algorithms involved. The pipeline workflow is shown step-by-step and demonstrated on real datasets acquired at sea.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14.6525W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14.6525W"><span>A generalized multivariate regression model for modelling <span class="hlt">ocean</span> <span class="hlt">wave</span> heights</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, X. L.; Feng, Y.; Swail, V. R.</p> <p>2012-04-01</p> <p>In this study, a generalized multivariate linear regression model is developed to represent the relationship between 6-hourly <span class="hlt">ocean</span> significant <span class="hlt">wave</span> heights (Hs) and the corresponding 6-hourly mean sea level pressure (MSLP) fields. The model is calibrated using the ERA-Interim reanalysis of Hs and MSLP fields for 1981-2000, and is validated using the ERA-Interim reanalysis for 2001-2010 and ERA40 reanalysis of Hs and MSLP for 1958-2001. The performance of the fitted model is evaluated in terms of Pierce skill score, frequency bias index, and correlation skill score. Being not normally distributed, <span class="hlt">wave</span> heights are subjected to a data adaptive Box-Cox transformation before being used in the model fitting. Also, since 6-hourly data are being modelled, lag-1 autocorrelation must be and is accounted for. The models with and without Box-Cox transformation, and with and without accounting for autocorrelation, are inter-compared in terms of their prediction skills. The fitted MSLP-Hs relationship is then used to reconstruct historical <span class="hlt">wave</span> height climate from the 6-hourly MSLP fields taken from the Twentieth Century Reanalysis (20CR, Compo et al. 2011), and to project possible future <span class="hlt">wave</span> height climates using CMIP5 model simulations of MSLP fields. The reconstructed and projected <span class="hlt">wave</span> heights, both seasonal means and maxima, are subject to a trend analysis that allows for non-linear (polynomial) trends.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.S11G..05N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.S11G..05N"><span>Mariscope: Observing P <span class="hlt">Waves</span> (and much more) Everywhere in the <span class="hlt">Oceans</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nolet, G.; Hello, Y.; Bonnieux, S.; Sukhovich, A.; Simons, F. J.</p> <p>2014-12-01</p> <p>The lack of stations on islands or the <span class="hlt">ocean</span> bottom deprives seismic tomographers of almost 2/3 of the information potentially available for global seismic tomography. The "Mermaid", developed at Geoazur, is an underwater seismograph, based on a TWR Apex float. P <span class="hlt">wave</span> signals are automatically identified and transmitted using the detection algorithm from Sukhovich et al. (GRL, 2011), GPS is used to locate the sensor at the time of transmission. We have studied the performance of Mermaids under different noise conditions in the Mediterranean, Indian <span class="hlt">Ocean</span> and most recently near the Galapagos islands and will show a selection of observations. In the Mediterranean, we regularly detect P <span class="hlt">waves</span> at teleseismic distances of earthquakes with magnitude 6, occasionally below that. Local and regional earthquakes of much lower magnitude, such as a M 4.9 earthquake near Barcelonette (figure), yield seismograms with a high signal to noise ratio.In the much noisier environment of the Indian <span class="hlt">Ocean</span> the threshold for useful seismograms is close to magnitude 6.5. Yet we were also able to record 235 low magnitude events when a Mermaid was close to a swarm near the Indian <span class="hlt">Ocean</span> triple junction, with the lowest magnitude estimated to be 2.1; this sequence also enabled us to put an upper limit of about 250 m to the error in sensor location at the time of recording. Preliminary data from the Galapagos indicate low noise conditions similar to those in the Mediterranean, with good recordings of events in the magnitude 5 range.A new prototype of a spherical "MultiMermaid" is currently being tested. It allows for multidisciplinary observations (seismic and kHz acoustics, magnetic field, temperature, bathymetry) and will function about five years with lithium batteries. A global deployment of such instruments in a five-year program is affordable: project MariScope aims for at least 300 floating seismometers in the world's <span class="hlt">oceans</span>. At the time of writing of this abstract, a proposal is being</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1325402','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1325402"><span>Characterization of U.S. <span class="hlt">Wave</span> Energy Converter (WEC) Test Sites: A Catalogue of Met-<span class="hlt">Ocean</span> Data, 2nd Edition</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>Ann R. Dallman; Neary, Vincent S.</p> <p></p> <p>This report presents met-<span class="hlt">ocean</span> data and <span class="hlt">wave</span> energy characteristics at eight U.S. <span class="hlt">wave</span> energy converter (WEC) test and potential deployment sites. Its purpose is to enable the comparison of <span class="hlt">wave</span> resource characteristics among sites as well as the selection of test sites that are most suitable for a developer's device and that best meet their testing needs and objectives. It also provides essential inputs for the design of WEC test devices and planning WEC tests, including the planning of deployment, and operations and maintenance. For each site, this report catalogues <span class="hlt">wave</span> statistics recommended in the International Electrotechnical Commission Technical Specimore » cation (IEC 62600-101 TS) on <span class="hlt">Wave</span> Energy Characterization, as well as the frequency of occurrence of weather windows and extreme sea states, and statistics on wind and <span class="hlt">ocean</span> currents. It also provides useful information on test site infrastructure and services.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017GGG....18.1926G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017GGG....18.1926G"><span>Seafloor age dependence of Rayleigh <span class="hlt">wave</span> phase velocities in the Indian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Godfrey, Karen E.; Dalton, Colleen A.; Ritsema, Jeroen</p> <p>2017-05-01</p> <p>Variations in the phase velocity of fundamental-mode Rayleigh <span class="hlt">waves</span> across the Indian <span class="hlt">Ocean</span> are determined using two inversion approaches. First, variations in phase velocity as a function of seafloor age are estimated using a pure-path age-dependent inversion method. Second, a two-dimensional parameterization is used to solve for phase velocity within 1.25° × 1.25° grid cells. Rayleigh <span class="hlt">wave</span> travel time delays have been measured between periods of 38 and 200 s. The number of measurements in the study area ranges between 4139 paths at a period of 200 s and 22,272 paths at a period of 40 s. At periods < 100 s, the phase velocity variations are strongly controlled by seafloor age and shown to be consistent with temperature variations predicted by the half-space-cooling model for a mantle potential temperature of 1400°C. The inferred thermal structure beneath the Indian <span class="hlt">Ocean</span> is most similar to the structure of the Pacific upper mantle, where phase velocities can also be explained by a half-space-cooling model. The thermal structure is not consistent with that of the Atlantic upper mantle, which is best fit by a plate-cooling model and requires a thin plate. Removing age-dependent phase velocity from the 2-D maps of the Indian <span class="hlt">Ocean</span> highlights anomalously high velocities at the Rodriguez Triple Junction and the Australian-Antarctic Discordance and anomalously low velocities immediately to the west of the Central Indian Ridge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRC..122.6110C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRC..122.6110C"><span>On the imprint of surfactant-driven stabilization of laboratory breaking <span class="hlt">wave</span> foam with comparison to <span class="hlt">oceanic</span> whitecaps</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Callaghan, A. H.; Deane, G. B.; Stokes, M. D.</p> <p>2017-08-01</p> <p>Surfactants are ubiquitous in the global <span class="hlt">oceans</span>: they help form the materially-distinct sea surface microlayer (SML) across which global <span class="hlt">ocean</span>-atmosphere exchanges take place, and they reside on the surfaces of bubbles and whitecap foam cells prolonging their lifetime thus altering <span class="hlt">ocean</span> albedo. Despite their importance, the occurrence, spatial distribution, and composition of surfactants within the upper <span class="hlt">ocean</span> and the SML remains under-characterized during conditions of vigorous <span class="hlt">wave</span> breaking when in-situ sampling methods are difficult to implement. Additionally, no quantitative framework exists to evaluate the importance of surfactant activity on <span class="hlt">ocean</span> whitecap foam coverage estimates. Here we use individual laboratory breaking <span class="hlt">waves</span> generated in filtered seawater and seawater with added soluble surfactant to identify the imprint of surfactant activity in whitecap foam evolution. The data show a distinct surfactant imprint in the decay phase of foam evolution. The area-time-integral of foam evolution is used to develop a time-varying stabilization function, ϕ>(t>) and a stabilization factor, Θ, which can be used to identify and quantify the extent of this surfactant imprint for individual breaking <span class="hlt">waves</span>. The approach is then applied to wind-driven <span class="hlt">oceanic</span> whitecaps, and the laboratory and <span class="hlt">ocean</span> Θ distributions overlap. It is proposed that whitecap foam evolution may be used to determine the occurrence and extent of <span class="hlt">oceanic</span> surfactant activity to complement traditional in-situ techniques and extend measurement capabilities to more severe sea states occurring at wind speeds in excess of about 10 m/s. The analysis procedure also provides a framework to assess surfactant-driven variability within and between whitecap coverage data sets.<abstract type="synopsis"><title type="main">Plain Language SummaryThe foam patches made by breaking <span class="hlt">waves</span>, also known as "whitecaps", are an important source of marine sea spray, which impacts weather and climate through 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_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://www.waveworkshop.org/10thWaves/ProgramFrameset.htm','USGSPUBS'); return false;" href="http://www.waveworkshop.org/10thWaves/ProgramFrameset.htm"><span>Coupling alongshore variations in <span class="hlt">wave</span> energy to beach morphologic change using the SWAN <span class="hlt">wave</span> model at <span class="hlt">Ocean</span> Beach, San Francisco, CA</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Eshleman, Jodi L.; Barnard, Patrick L.; Erikson, Li H.; Hanes, Daniel M.</p> <p>2007-01-01</p> <p>Coastal managers have faced increasing pressure to manage their resources wisely over the last century as a result of heightened development and changing environmental forcing. It is crucial to understand seasonal changes in beach volume and shape in order to identify areas vulnerable to accelerated erosion. Shepard (1950) was among the first to quantify seasonal beach cycles. Sonu and Van Beek (1971) and Wright et al. (1985) described commonly occurring beach states. Most studies utilize widest spaced 2-D cross shore profiles or shorelines extracted from aerial photographs (e.g. Winant et al. 1975; Aubrey, 1979, Aubrey and Ross, 1985; Larson and Kraus, 1994; Jimenez et al., 1977; Lacey and Peck, 1998; Guillen et al., 1999; Norcorss et al., 2002) to analyzed systematic changes in beach evolution. But with the exception of established field stations, such as Duck, NC (Birkemeier and Mason, 1984), ans Hazaki Oceanographical Research Station (HORS) in Japan (Katoh, 1997), there are very few beach change data sets with high temporal and spatial resolutions (e.g. Dail et al., 2000; Ruggiero et al., 2005; Yates et al., in press). Comprehensive sets of nearshore morphological data and local in situ measurements outside of these field stations are very rare and virtually non-existent high-energy coasts. Studied that have attempted to relate <span class="hlt">wave</span> statistics to beach morphology change require some knowledge of the nearshore <span class="hlt">wave</span> climate, and have had limited success using offshore measurement (Sonu and Van Beek, 1971; Dail et al., 2000). The primary objective of this study is to qualitatively compare spatially variable nearshore <span class="hlt">wave</span> predictions to beach change measurements in order to understand the processes responsible for a persistent erosion 'hotspot' at <span class="hlt">Ocean</span> Beach, San Francisco, CA. Local <span class="hlt">wave</span> measurements are used to calibrate and validate a <span class="hlt">wave</span> model that provides nearshore <span class="hlt">wave</span> prediction along the beach. The model is run for thousands of binned offshore <span class="hlt">wave</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130010928','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130010928"><span>Calibration of <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Measurements by the TOPEX, Jason-1, and Jason-2 Satellites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ray, Richard D.; Beckley, B. D.</p> <p>2012-01-01</p> <p>The calibration and validation of <span class="hlt">ocean</span> <span class="hlt">wave</span> height measurements by the TOPEX, Jason-1, and Jason-2 satellite altimeters is addressed by comparing the measurements internally among them- selves and against independent <span class="hlt">wave</span> measurements at moored buoys. The two six-month verification campaigns, when two of the satellites made near-simultaneous measurements along the same ground track, are invaluable for such work and reveal subtle aspects that otherwise might go undetected. The two Jason satellites are remarkably consistent; Topex reports <span class="hlt">waves</span> generally 1-2% larger. External calibration is complicated by some systematic errors in the buoy data. We confirm a recent report by Durrant et al. that Canadian buoys underestimate significant <span class="hlt">wave</span> heights by about 10% relative to U.S. buoys. <span class="hlt">Wave</span> heights from all three altimetric satellites require scaling upwards by 5 6% to be consistent with U.S. buoys.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016E%26SS....3...68B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016E%26SS....3...68B"><span>An <span class="hlt">ocean</span> bottom seismic observatory with near real-time telemetry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Berger, J.; Laske, G.; Babcock, J.; Orcutt, J.</p> <p>2016-02-01</p> <p>We describe a new technology that can provide near real-time telemetry of sensor data from the <span class="hlt">ocean</span> bottom without a moored buoy or a cable to shore. The breakthrough technology that makes this system possible is an autonomous surface vehicle called a <span class="hlt">Wave</span> Glider developed by Liquid Robotics, Inc. of Sunnyvale, CA, which harvests <span class="hlt">wave</span> and solar energy for motive and electrical <span class="hlt">power</span>. We present results from several deployments of a prototype system that demonstrate the feasibility of this concept. We also demonstrated that a <span class="hlt">wave</span> glider could tow a suitably designed <span class="hlt">ocean</span> bottom package with acceptable loss of speed. With further development such a system could be deployed autonomously and provide real-time telemetry of data from seafloor sensors.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29091662','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29091662"><span>Progress in high-<span class="hlt">power</span> continuous-<span class="hlt">wave</span> quantum cascade lasers [Invited].</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Figueiredo, Pedro; Suttinger, Matthew; Go, Rowel; Tsvid, Eugene; Patel, C Kumar N; Lyakh, Arkadiy</p> <p>2017-11-01</p> <p>Multi-watt continuous-<span class="hlt">wave</span> room temperature operation with efficiency exceeding 10% has been demonstrated for quantum cascade lasers essentially in the entire mid-<span class="hlt">wave</span> and long-<span class="hlt">wave</span> infrared spectral regions. Along with interband cascade lasers, these devices are the only room-temperature lasers that directly convert electrical <span class="hlt">power</span> into mid- and long-infrared optical <span class="hlt">power</span>. In this paper, we review the progress in high-<span class="hlt">power</span> quantum cascade lasers made over the last 10 years. Specifically, an overview of the most important active region, waveguide, and thermal design techniques is presented, and various aspects of die packaging for high-<span class="hlt">power</span> applications are discussed. Prospects of <span class="hlt">power</span> scaling with lateral device dimensions for reaching optical <span class="hlt">power</span> level in the range from 10 W to 20 W are also analyzed. Finally, coherent and spectral beam-combining techniques for very high-<span class="hlt">power</span> infrared platforms are discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EP%26S...69...44O','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EP%26S...69...44O"><span>Effects of shallow-layer reverberation on measurement of teleseismic P-<span class="hlt">wave</span> travel times for <span class="hlt">ocean</span> bottom seismograph data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Obayashi, Masayuki; Ishihara, Yasushi; Suetsugu, Daisuke</p> <p>2017-03-01</p> <p>We conducted synthetic experiments to evaluate the effects of shallow-layer reverberation in <span class="hlt">oceanic</span> regions on P-<span class="hlt">wave</span> travel times measured by waveform cross-correlation. Time shift due to waveform distortion by the reverberation was estimated as a function of period. Reverberations in the crystalline crust advance the P-<span class="hlt">waves</span> by a frequency-independent time shift of about 0.3 s in <span class="hlt">oceans</span>. Sediment does not affect the time shifts in the mid-<span class="hlt">ocean</span> regions, but effects as large as -0.8 s or more occur where sediment thickness is greater than 600 m for periods longer than 15 s. The water layer causes time delays (+0.3 s) in the relatively shallow (<3500 m) water region for periods longer than 20 s. The time shift may influence mantle images obtained if the reverberation effects are not accounted for in seismic tomography. We propose a simple method to correct relative P-<span class="hlt">wave</span> travel times at two sites for shallow-layer reverberation by the cross-convolution of the crustal responses at the two sites. [Figure not available: see fulltext. Caption: .</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=function+AND+wave&pg=3&id=EJ794601','ERIC'); return false;" href="https://eric.ed.gov/?q=function+AND+wave&pg=3&id=EJ794601"><span>Accuracy of Satellite-Measured <span class="hlt">Wave</span> Heights in the Australian Region for <span class="hlt">Wave</span> <span class="hlt">Power</span> Applications</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Meath, Sian E.; Aye, Lu; Haritos, Nicholas</p> <p>2008-01-01</p> <p>This article focuses on the accuracy of satellite data, which may then be used in <span class="hlt">wave</span> <span class="hlt">power</span> applications. The satellite data are compared to data from <span class="hlt">wave</span> buoys, which are currently considered to be the most accurate of the devices available for measuring <span class="hlt">wave</span> characteristics. This article presents an analysis of satellite- (Topex/Poseidon) and…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2006OcScD...3.1825J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2006OcScD...3.1825J"><span>Assessment of the importance of the current-<span class="hlt">wave</span> coupling in the shelf <span class="hlt">ocean</span> forecasts</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jordà, G.; Bolaños, R.; Espino, M.; Sánchez-Arcilla, A.</p> <p>2006-10-01</p> <p>The effects of <span class="hlt">wave</span>-current interactions on shelf <span class="hlt">ocean</span> 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 <span class="hlt">wave</span> model (WAM) to the circulation model (SYMPHONIE). The coupling of <span class="hlt">waves</span> and currents has been done considering four main processes: <span class="hlt">wave</span> refraction due to currents, surface wind drag and bo€ttom drag modifications due to <span class="hlt">waves</span>, and the <span class="hlt">wave</span> 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 <span class="hlt">wave</span> refraction by currents seems to be not very relevant in a microtidal context such as the western Mediterranean. The main effect of <span class="hlt">waves</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ChOE...30..565Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ChOE...30..565Z"><span>An oscillating <span class="hlt">wave</span> energy converter with nonlinear snap-through <span class="hlt">Power</span>-Take-Off systems in regular <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>Zhang, Xian-tao; Yang, Jian-min; Xiao, Long-fei</p> <p>2016-07-01</p> <p>Floating oscillating bodies constitute a large class of <span class="hlt">wave</span> energy converters, especially for offshore deployment. Usually the <span class="hlt">Power</span>-Take-Off (PTO) system is a directly linear electric generator or a hydraulic motor that drives an electric generator. The PTO system is simplified as a linear spring and a linear damper. However the conversion is less <span class="hlt">powerful</span> with <span class="hlt">wave</span> periods off resonance. Thus, a nonlinear snap-through mechanism with two symmetrically oblique springs and a linear damper is applied in the PTO system. The nonlinear snap-through mechanism is characteristics of negative stiffness and double-well potential. An important nonlinear parameter γ is defined as the ratio of half of the horizontal distance between the two springs to the original length of both springs. Time domain method is applied to the dynamics of <span class="hlt">wave</span> energy converter in regular <span class="hlt">waves</span>. And the state space model is used to replace the convolution terms in the time domain equation. The results show that the energy harvested by the nonlinear PTO system is larger than that by linear system for low frequency input. While the <span class="hlt">power</span> captured by nonlinear converters is slightly smaller than that by linear converters for high frequency input. The <span class="hlt">wave</span> amplitude, damping coefficient of PTO systems and the nonlinear parameter γ affect <span class="hlt">power</span> capture performance of nonlinear converters. The oscillation of nonlinear <span class="hlt">wave</span> energy converters may be local or periodically inter well for certain values of the incident <span class="hlt">wave</span> frequency and the nonlinear parameter γ, which is different from linear converters characteristics of sinusoidal response in regular <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20100042213','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20100042213"><span><span class="hlt">Power</span> Amplifier Module with 734-mW Continuous <span class="hlt">Wave</span> Output <span class="hlt">Power</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fung, King Man; Samoska, Lorene A.; Kangaslahti, Pekka P.; Lamgrigtsen, Bjorn H.; Goldsmith, Paul F.; Lin, Robert H.; Soria, Mary M.; Cooperrider, Joelle T.; Micovic, Moroslav; Kurdoghlian, Ara</p> <p>2010-01-01</p> <p>Research findings were reported from an investigation of new gallium nitride (GaN) monolithic millimeter-<span class="hlt">wave</span> integrated circuit (MMIC) <span class="hlt">power</span> amplifiers (PAs) targeting the highest output <span class="hlt">power</span> and the highest efficiency for class-A operation in W-band (75-110 GHz). W-band PAs are a major component of many frequency multiplied submillimeter-<span class="hlt">wave</span> LO signal sources. For spectrometer arrays, substantial W-band <span class="hlt">power</span> is required due to the passive lossy frequency multipliers-to generate higher frequency signals in nonlinear Schottky diode-based LO sources. By advancing PA technology, the LO system performance can be increased with possible cost reductions compared to current GaAs PAs. High-<span class="hlt">power</span>, high-efficiency GaN PAs are cross-cutting and can enable more efficient local oscillator distribution systems for new astrophysics and planetary receivers and heterodyne array instruments. It can also allow for a new, electronically scannable solid-state array technology for future Earth science radar instruments and communications platforms.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA542499','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA542499"><span>Physics, Nonlinear Time Series Analysis, Data Assimilation and Hyperfast Modeling of Nonlinear <span class="hlt">Ocean</span> <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2010-09-30</p> <p>Hyperfast Modeling of Nonlinear <span class="hlt">Ocean</span> <span class="hlt">Waves</span> A. R. Osborne Dipartimento di Fisica Generale, Università di Torino Via Pietro Giuria 1, 10125...PERFORMING ORGANIZATION NAME(S) AND ADDRESS(ES) Universit?i Torino,Dipartimento di Fisica Generale,Via Pietro Giuria 1,10125 Torino, Italy, 8. PERFORMING</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009AGUFM.A31F0178S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009AGUFM.A31F0178S"><span>Quantifying the Benefits of Combining Offshore Wind and <span class="hlt">Wave</span> Energy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stoutenburg, E.; Jacobson, M. Z.</p> <p>2009-12-01</p> <p>For many locations the offshore wind resource and the <span class="hlt">wave</span> energy resource are collocated, which suggests a natural synergy if both technologies are combined into one offshore marine renewable energy plant. Initial meteorological assessments of the western coast of the United States suggest only a weak correlation in <span class="hlt">power</span> levels of wind and <span class="hlt">wave</span> energy at any given hour associated with the large <span class="hlt">ocean</span> basin <span class="hlt">wave</span> dynamics and storm systems of the North Pacific. This finding indicates that combining the two <span class="hlt">power</span> sources could reduce the variability in electric <span class="hlt">power</span> output from a combined wind and <span class="hlt">wave</span> offshore plant. A combined plant is modeled with offshore wind turbines and Pelamis <span class="hlt">wave</span> energy converters with wind and <span class="hlt">wave</span> data from meteorological buoys operated by the US National Buoy Data Center off the coast of California, Oregon, and Washington. This study will present results of quantifying the benefits of combining wind and <span class="hlt">wave</span> energy for the electrical <span class="hlt">power</span> system to facilitate increased renewable energy penetration to support reductions in greenhouse gas emissions, and air and water pollution associated with conventional fossil fuel <span class="hlt">power</span> plants.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA629945','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA629945"><span>Satellite Synthetic Aperture Radar Detection of <span class="hlt">Ocean</span> Internal <span class="hlt">Waves</span> in the South China Sea</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2006-09-30</p> <p><span class="hlt">waves</span> will occur and what effects they will have on the hydrodynamic and acoustic environment. This project focuses on the use of remotely sensed...variability of the ITF and its associated heat and freshwater flux exported into the Indian <span class="hlt">Ocean</span>. REFERENCES Boyer, T., and S. Levites , Quality</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2011-04-05/pdf/2011-7984.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2011-04-05/pdf/2011-7984.pdf"><span>76 FR 18750 - <span class="hlt">Ocean</span> Renewable <span class="hlt">Power</span> Company, LLC; Notice of Change in Docket Number</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2011-04-05</p> <p>... DEPARTMENT OF ENERGY Federal Energy Regulatory Commission [Project No. 12680-003; Project No. 12711-003] <span class="hlt">Ocean</span> Renewable <span class="hlt">Power</span> Company, LLC; Notice of Change in Docket Number On July 24, 2009, <span class="hlt">Ocean</span> Renewable <span class="hlt">Power</span> Company, LLC (ORPC) filed a draft hydrokinetic pilot license application (DLA) for the...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMED41A0827B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMED41A0827B"><span>Slowing <span class="hlt">Ocean</span> Acidification</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bravo, A.</p> <p>2016-12-01</p> <p>Currently our <span class="hlt">ocean</span>'s pH is 8.1, a decrease from 8.2 in the past 200 years since the beginning of the industrial revolution. The <span class="hlt">ocean</span> absorbs about a third of the carbon dioxide (CO2) from the atmosphere, which is helpful to us, since reducing the amount of CO2 in the atmosphere shows global warming. However, what is the impact of all that CO2 on the <span class="hlt">ocean</span>? I evaluated the effect of acidic water on bivalves, and found that the shells were broken down with exposure to increased acidity. I am concerned that continued <span class="hlt">ocean</span> acidification will impact organisms that are unable to adapt to the changing <span class="hlt">ocean</span> chemistry. While the US currently invests in alternative forms of energy including solar and wind, approximately 66% of our energy comes from sources that are releasing CO2 into the atmosphere. I want to explore the potential of <span class="hlt">wave</span> energy as another form of renewable energy. When wind blows over the surface of the <span class="hlt">ocean</span>, it creates a <span class="hlt">wave</span>. Could this <span class="hlt">wave</span> energy be a consistent clean energy source? Could a strategy to slow and reverse <span class="hlt">ocean</span> acidification be found in the <span class="hlt">ocean</span>?</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1991JGR....96.4531F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1991JGR....96.4531F"><span>Strain in shore fast ice due to incoming <span class="hlt">ocean</span> <span class="hlt">waves</span> and swell</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fox, Colin; Squire, Vernon A.</p> <p>1991-03-01</p> <p>Using a development from the theoretical model presented by Fox and Squire (1990), this paper investigates the strain field generated in shore fast ice by normally incident <span class="hlt">ocean</span> <span class="hlt">waves</span> and swell. After a brief description of the model and its convergence, normalized absolute strain (relative to a 1-m incident <span class="hlt">wave</span>) is found as a function of distance from the ice edge for various <span class="hlt">wave</span> periods, ice thicknesses, and water depths. The squared transfer function, giving the relative ability of incident <span class="hlt">waves</span> of different periods to generate strain in the ice, is calculated, and its consequences are discussed. The ice is then forced with a Pierson-Moskowitz spectrum, and the consequent strain spectra are plotted as a function of penetration into the ice sheet. Finally, rms strain, computed as the incoherent sum of the strains resulting from energy in the open water spectrum, is found. The results have implications to the breakup of shore fast ice and hence to the floe size distribution of the marginal ice zone.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016JIMTW..37.1096H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016JIMTW..37.1096H"><span>Concentric Parallel Combining Balun for Millimeter-<span class="hlt">Wave</span> <span class="hlt">Power</span> Amplifier in Low-<span class="hlt">Power</span> CMOS with High-<span class="hlt">Power</span> Density</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Han, Jiang-An; Kong, Zhi-Hui; Ma, Kaixue; Yeo, Kiat Seng; Lim, Wei Meng</p> <p>2016-11-01</p> <p>This paper presents a novel balun for a millimeter-<span class="hlt">wave</span> <span class="hlt">power</span> amplifier (PA) design to achieve high-<span class="hlt">power</span> density in a 65-nm low-<span class="hlt">power</span> (LP) CMOS process. By using a concentric winding technique, the proposed parallel combining balun with compact size accomplishes <span class="hlt">power</span> combining and unbalance-balance conversion concurrently. For calculating its <span class="hlt">power</span> combination efficiency in the condition of various amplitude and phase <span class="hlt">wave</span> components, a method basing on S-parameters is derived. Based on the proposed parallel combining balun, a fabricated 60-GHz industrial, scientific, and medical (ISM) band PA with single-ended I/O achieves an 18.9-dB gain and an 8.8-dBm output <span class="hlt">power</span> at 1-dB compression and 14.3-dBm saturated output <span class="hlt">power</span> ( P sat) at 62 GHz. This PA occupying only a 0.10-mm2 core area has demonstrated a high-<span class="hlt">power</span> density of 269.15 mW/mm2 in 65 nm LP CMOS.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000013567&hterms=3D+animation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3D3D%2Banimation','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000013567&hterms=3D+animation&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D50%26Ntt%3D3D%2Banimation"><span>Hurricane Directional <span class="hlt">Wave</span> Spectrum Spatial Variation in the Open <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wright, C. W.; Walsh, E. J.; Vandemark, D.; Krabill, W. B.; Garcia, A. W.</p> <p>1999-01-01</p> <p>The sea surface directional <span class="hlt">wave</span> spectrum was measured for the first time in all quadrants of a hurricane in open water using the NASA airborne scanning radar altimeter (SRA) carried aboard one of the NOAA WP-3D hurricane hunter aircraft at 1.5 km height. The SRA measures the energetic portion of the directional <span class="hlt">wave</span> spectrum by generating a topographic map of the sea surface. At 8 Hz, the SRA sweeps a radar beam of 1 deg half-<span class="hlt">power</span> width (two-way) across the aircraft ground track over a swath equal to 0. 8 of the aircraft height, simultaneously measuring the backscattered <span class="hlt">power</span> at its 36 GHz (8.3 mm) operating frequency and the range to the sea surface at 64 positions. These slant ranges are multiplied by the cosine of the incidence angles to determine the vertical distances from the aircraft to the sea surface. Subtracting these distances from the aircraft height produces the sea surface elevation map. The sea surface topography is interpolated to a uniform grid, transformed by a two-dimensional FFT, and Doppler corrected. The data presented were acquired on 24 August 1998 when hurricane Bonnie was east of the Bahamas and moving slowly to the north. <span class="hlt">Wave</span> heights up to 18 m were observed and the spatial variation of the <span class="hlt">wave</span> field was dramatic. The dominant <span class="hlt">waves</span> generally propagated at significant angles to the downwind direction and at times there were <span class="hlt">wave</span> fields traveling at right angles to each other. The NOAA aircraft spent over five hours within 180 km of the hurricane Bonnie eye, and made five eye penetrations. A 2-minute animation of the directional <span class="hlt">wave</span> spectrum spatial variation over this period will be shown.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26723303','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26723303"><span><span class="hlt">Ocean</span> acoustic reverberation tomography.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Dunn, Robert A</p> <p>2015-12-01</p> <p>Seismic wide-angle imaging using ship-towed acoustic sources and networks of <span class="hlt">ocean</span> bottom seismographs is a common technique for exploring earth structure beneath the <span class="hlt">oceans</span>. In these studies, the recorded data are dominated by acoustic <span class="hlt">waves</span> propagating as reverberations in the water column. For surveys with a small receiver spacing (e.g., <10 km), the acoustic <span class="hlt">wave</span> field densely samples properties of the water column over the width of the receiver array. A method, referred to as <span class="hlt">ocean</span> acoustic reverberation tomography, is developed that uses the travel times of direct and reflected <span class="hlt">waves</span> to image <span class="hlt">ocean</span> acoustic structure. Reverberation tomography offers an alternative approach for determining the structure of the <span class="hlt">oceans</span> and advancing the understanding of <span class="hlt">ocean</span> heat content and mixing processes. The technique has the potential for revealing small-scale <span class="hlt">ocean</span> thermal structure over the entire vertical height of the water column and along long survey profiles or across three-dimensional volumes of the <span class="hlt">ocean</span>. For realistic experimental geometries and data noise levels, the method can produce images of <span class="hlt">ocean</span> sound speed on a smaller scale than traditional acoustic tomography.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5713174','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5713174"><span>Ambient seismic <span class="hlt">wave</span> field</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>NISHIDA, Kiwamu</p> <p>2017-01-01</p> <p>The ambient seismic <span class="hlt">wave</span> field, also known as ambient noise, is excited by <span class="hlt">oceanic</span> gravity <span class="hlt">waves</span> primarily. This can be categorized as seismic hum (1–20 mHz), primary microseisms (0.02–0.1 Hz), and secondary microseisms (0.1–1 Hz). Below 20 mHz, pressure fluctuations of <span class="hlt">ocean</span> infragravity <span class="hlt">waves</span> reach the abyssal floor. Topographic coupling between seismic <span class="hlt">waves</span> and <span class="hlt">ocean</span> infragravity <span class="hlt">waves</span> at the abyssal floor can explain the observed shear traction sources. Below 5 mHz, atmospheric disturbances may also contribute to this excitation. Excitation of primary microseisms can be attributed to topographic coupling between <span class="hlt">ocean</span> swell and seismic <span class="hlt">waves</span> on subtle undulation of continental shelves. Excitation of secondary microseisms can be attributed to non-linear forcing by standing <span class="hlt">ocean</span> swell at the sea surface in both pelagic and coastal regions. Recent developments in source location based on body-<span class="hlt">wave</span> microseisms enable us to estimate forcing quantitatively. For a comprehensive understanding, we must consider the solid Earth, the <span class="hlt">ocean</span>, and the atmosphere as a coupled system. PMID:28769015</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFD.L2004R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFD.L2004R"><span>Characterization and Scaling of Heave Plates for <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Energy Converters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rosenberg, Brian; Mundon, Timothy</p> <p>2016-11-01</p> <p><span class="hlt">Ocean</span> <span class="hlt">waves</span> present a tremendous, untapped source of renewable energy, capable of providing half of global electricity demand by 2040. Devices developed to extract this energy are known as <span class="hlt">wave</span> energy converters (WECs) and encompass a wide range of designs. A somewhat common archetype is a two-body point-absorber, in which a surface float reacts against a submerged "heave" plate to extract energy. Newer WEC's are using increasingly complex geometries for the submerged plate and an emerging challenge in creating low-order models lies in accurately determining the hydrodynamic coefficients (added mass and drag) in the corresponding oscillatory flow regime. Here we present experiments in which a laboratory-scale heave plate is sinusoidally forced in translation (heave) and rotation (pitch) to characterize the hydrodynamic coefficients as functions of the two governing nondimensional parameters, Keulegan-Carpenter number (amplitude) and Reynolds number. Comparisons against CFD simulations are offered. As laboratory-scale physical model tests remain the standard for testing <span class="hlt">wave</span> energy devices, effects and implications of scaling (with respect to a full-scale device) are also investigated.</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://hdl.handle.net/2060/19860015629','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19860015629"><span>Studies related to <span class="hlt">ocean</span> dynamics. Task 3.2: Aircraft Field Test Program to investigate the ability of remote sensing methods to measure current/wind-<span class="hlt">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>Huang, N. E.; Flood, W. A.; Brown, G. S.</p> <p>1975-01-01</p> <p>The feasibility of remote sensing of current flows in the <span class="hlt">ocean</span> and the remote sensing of <span class="hlt">ocean</span> currents by backscattering cross section techniques was studied. It was established that for capillary <span class="hlt">waves</span>, small scale currents could be accurately measured through observation of <span class="hlt">wave</span> kinematics. Drastic modifications of <span class="hlt">waves</span> by changing currents were noted. The development of new methods for the measurement of capillary <span class="hlt">waves</span> are discussed. Improvement methods to resolve data processing problems are suggested.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1335573-balancing-power-absorption-fatigue-loads-irregular-waves-oscillating-surge-wave-energy-converter','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1335573-balancing-power-absorption-fatigue-loads-irregular-waves-oscillating-surge-wave-energy-converter"><span>Balancing <span class="hlt">Power</span> Absorption and Fatigue Loads in Irregular <span class="hlt">Waves</span> for an Oscillating Surge <span class="hlt">Wave</span> Energy Converter</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>Tom, Nathan M.; Yu, Yi-Hsiang; Wright, Alan D.</p> <p></p> <p>The aim of this paper is to describe how to control the <span class="hlt">power</span>-to-load ratio of a novel <span class="hlt">wave</span> energy converter (WEC) in irregular <span class="hlt">waves</span>. The novel WEC that is being developed at the National Renewable Energy Laboratory combines an oscillating surge <span class="hlt">wave</span> energy converter (OSWEC) with control surfaces as part of the structure; however, this work only considers one fixed geometric configuration. This work extends the optimal control problem so as to not solely maximize the time-averaged <span class="hlt">power</span>, but to also consider the <span class="hlt">power</span>-take-off (PTO) torque and foundation forces that arise because of WEC motion. The objective function of themore » controller will include competing terms that force the controller to balance <span class="hlt">power</span> capture with structural loading. Separate penalty weights were placed on the surge-foundation force and PTO torque magnitude, which allows the controller to be tuned to emphasize either <span class="hlt">power</span> absorption or load shedding. Results of this study found that, with proper selection of penalty weights, gains in time-averaged <span class="hlt">power</span> would exceed the gains in structural loading while minimizing the reactive <span class="hlt">power</span> requirement.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFDG14004F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFDG14004F"><span>Computational modeling of pitching cylinder-type <span class="hlt">ocean</span> <span class="hlt">wave</span> energy converters using 3D MPI-parallel simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Freniere, Cole; Pathak, Ashish; Raessi, Mehdi</p> <p>2016-11-01</p> <p><span class="hlt">Ocean</span> <span class="hlt">Wave</span> Energy Converters (WECs) are devices that convert energy from <span class="hlt">ocean</span> <span class="hlt">waves</span> into electricity. To aid in the design of WECs, an advanced computational framework has been developed which has advantages over conventional methods. The computational framework simulates the performance of WECs in a virtual <span class="hlt">wave</span> tank by solving the full Navier-Stokes equations in 3D, capturing the fluid-structure interaction, nonlinear and viscous effects. In this work, we present simulations of the performance of pitching cylinder-type WECs and compare against experimental data. WECs are simulated at both model and full scales. The results are used to determine the role of the Keulegan-Carpenter (KC) number. The KC number is representative of viscous drag behavior on a bluff body in an oscillating flow, and is considered an important indicator of the dynamics of a WEC. Studying the effects of the KC number is important for determining the validity of the Froude scaling and the inviscid potential flow theory, which are heavily relied on in the conventional approaches to modeling WECs. Support from the National Science Foundation is gratefully acknowledged.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008ESASP.676E...2L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008ESASP.676E...2L"><span>TerraSAR-X Measurements of Wind Fields, <span class="hlt">Ocean</span> <span class="hlt">Waves</span> and Currents</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lehner, S.; Schulz-Stellenfleth, J.; Brusch, S.</p> <p>2008-01-01</p> <p>TerraSAR-X is a new german X-band radar satellite launched on June 15, 2007. In this mission an operational spaceborne synthetic aperture radar (SAR) system with very high spatial resolution is set up producing remote sensing products for commercial and scientific use. TerraSAR-X is a scientific and technological continuation of the successful Space Shuttle missions SIR-C/X and SRTM.The spacecraft is equipped with a phased array X-band SAR, which can operate in different polarisations and has furthermore beam stearing capabilities. In addition the system has a split antenna mode, which is able to provide along track interferometric information. The instrument is designed for multiple imaging modes like Stripmap, Spotlight and ScanSAR.Due to its polarimetric and interferometric capabilities as well as the high spatial resolution of up to 1 m, the TerraSAR-X sensor is a very interesting tool for oceanography. The presentation will give an overview of several applications, which are of both scientific and commercial interest, like e.g. current and <span class="hlt">ocean</span> <span class="hlt">wave</span> measurements, monitoring of morphodynamical processes or high resolution wind field retrieval. The potential as well as limitations of the instrument will be summarized and compared with existing sensors. Necessary steps to translate existing C-band SAR inversion algorithms for wind and <span class="hlt">wave</span> measurements to X-band will be discussed. A strategy will be outlined to achieve this by a combination of theoretical investigations and the use of existing experimental data acquired by both airborne and groundbased X-band radar. First results on the adaption of existing C-band wind retrieval algorithms will be presented. Wind and <span class="hlt">ocean</span> <span class="hlt">wave</span> parameter retrievals will be presented, e.g., based on TerraSAR-X scenes taken over the English channel.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20090040787','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20090040787"><span>High-<span class="hlt">Power</span>, High-Efficiency Ka-Band Space Traveling-<span class="hlt">Wave</span> Tube</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Krawczyk, Richard; Wilson, Jeffrey; Simons, Rainee; Williams, Wallace; Bhasin, Kul; Robbins, Neal; Dibb, Daniel; Menninger, William; Zhai, Xiaoling; Benton, Robert; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20090040787'); toggleEditAbsImage('author_20090040787_show'); toggleEditAbsImage('author_20090040787_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20090040787_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20090040787_hide"></p> <p>2007-01-01</p> <p>The L-3 Communications Model 999H traveling-<span class="hlt">wave</span> tube (TWT) has been demonstrated to generate an output <span class="hlt">power</span> of 144 W at 60-percent overall efficiency in continuous-<span class="hlt">wave</span> operation over the frequency band from 31.8 to 32.3 GHz. The best TWT heretofore commercially available for operation in the affected frequency band is characterized by an output <span class="hlt">power</span> of only 35 W and an efficiency of 50 percent. Moreover, whereas prior TWTs are limited to single output <span class="hlt">power</span> levels, it has been shown that the output <span class="hlt">power</span> of the Model 999H can be varied from 54 to 144 W. A TWT is a vacuum electronic device used to amplify microwave signals. TWTs are typically used in free-space communication systems because they are capable of operating at <span class="hlt">power</span> and efficiency levels significantly higher than those of solid-state devices. In a TWT, an electron beam is generated by an electron gun consisting of a cathode, focusing electrodes, and an anode. The electrons pass through a hole in the anode and are focused into a cylindrical beam by a stack of periodic permanent magnets and travel along the axis of an electrically conductive helix, along which propagates an electromagnetic <span class="hlt">wave</span> that has been launched by an input signal that is to be amplified. The beam travels within the helix at a velocity close to the phase velocity of the electromagnetic <span class="hlt">wave</span>. The electromagnetic field decelerates some of the electrons and accelerates others, causing the beam to become formed into electron bunches, which further interact with the electromagnetic <span class="hlt">wave</span> in such a manner as to surrender kinetic energy to the <span class="hlt">wave</span>, thereby amplifying the <span class="hlt">wave</span>. The net result is to amplify the input signal by a factor of about 100,000. After the electrons have passed along the helix, they impinge on electrodes in a collector. The collector decelerates the electrons in such a manner as to recover most of the remaining kinetic energy and thereby significantly increase the <span class="hlt">power</span> efficiency of the TWT.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2010EGUGA..12.5333T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2010EGUGA..12.5333T"><span>Optical Rogue <span class="hlt">Waves</span>: Theory and Experiments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Taki, M.; Mussot, A.; Kudlinski, A.; Louvergneaux, E.; Kolobov, M.</p> <p>2010-05-01</p> <p>In the <span class="hlt">ocean</span>, giant <span class="hlt">waves</span> (also called killer <span class="hlt">waves</span>, freak or rogue <span class="hlt">waves</span>) are extremely rare and strong events. They are not well understood yet and the conditions which favour their emergence are unclear. Very recently, it was shown that the governing equations [1] as well as the statistical properties of an optical pulse propagating inside an optical fibre [2] mimic very well these gigantic surface <span class="hlt">waves</span> in the <span class="hlt">ocean</span>. Here we generate both experimentally and numerically optical rogue <span class="hlt">waves</span> in a photonic crystal fiber (microstructured fiber) with continuous <span class="hlt">wave</span> (CW) pumps. This is relevant for establishing an analogy with rogue <span class="hlt">waves</span> in an open <span class="hlt">ocean</span>. After recalling fundamental rogue <span class="hlt">waves</span> [3] known as Akhmediev breathers that are solutions of pure nonlinear Schrödinger (NLS) equation, we analytically demonstrate that a generalized NLS equation, which governs the propagation of light in the fiber, exhibits convective modulationnal instability [4]. The latter provides one of the main explanations of the optical rogue <span class="hlt">wave</span> extreme sensitivity to noisy initial conditions at the linear stage of their formation [5]. In the highly nonlinear regime, we provide the evidence that optical rogue <span class="hlt">waves</span> result from soliton collisions leading to the rapid appearance/disappearance of a <span class="hlt">powerful</span> optical pulse [6]. REFERENCES [1] C. Kharif, E. Pelinovsky, and A. Slunyaev, "Rogue <span class="hlt">Waves</span> in the <span class="hlt">ocean</span>", Springer Berlin Heidelberg, 2009 [2] D. R. Solli, C. Ropers, P. Koonath, and B. Jalali, "Optical rogue <span class="hlt">waves</span>" Nature 450, 1054-1058, (2008). [3] N. Akhmediev, A. Ankiewicz, and M. Taki, "<span class="hlt">Waves</span> that appear from nowhere and disappear without a trace", Phys. Lett. A 373, 675 (2009). [4] A. Mussot, E. Louvergneaux, N. Akhmediev, F. Reynaud, Delage, and M. Taki, "Optical fiber systems are convectively unstable", Phys. Rev. Lett. 101, 113904 (2008). [5] M. Taki, A. Mussot, A. Kudlinski, E. Louvergneaux, M. Kolobov, M. Douay, "Third-order dispersion for generating optical rogue solitons</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2012-02-06/pdf/2012-2571.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2012-02-06/pdf/2012-2571.pdf"><span>77 FR 5791 - <span class="hlt">Ocean</span> Renewable <span class="hlt">Power</span> Company Maine, LLC; Notice of Staff Participation in Meeting</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2012-02-06</p> <p>... DEPARTMENT OF ENERGY Federal Energy Regulatory Commission [Project No. 12711-005] <span class="hlt">Ocean</span> Renewable <span class="hlt">Power</span> Company Maine, LLC; Notice of Staff Participation in Meeting On February 15, 2012, Office of Energy Projects staff will participate in a meeting with representatives from <span class="hlt">Ocean</span> Renewable <span class="hlt">Power</span>...</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA279650','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA279650"><span>Ambient Noise and Surface <span class="hlt">Wave</span> Dissipation in the <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1993-06-21</p> <p>computed frmn a one hour <span class="hlt">wave</span> gauge record with U10 = 8 m/s. a ) <span class="hlt">Power</span> spectrum computed rom 1024-point FFr. used throughout this work . b) <span class="hlt">Power</span> specttrum...this work , equations relating U and N in the form of Equation 1.3 will be referred to as WOTAN equations’. Figure 1.2 shows a figure taken from Evans et...the found that a significant proportion of the dissipated energy (up to 50%) is due to work done by the liquid in entraining air against buoyancy</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004AGUFMOS21C1276E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004AGUFMOS21C1276E"><span>The Bidirectional Reflectance Distribution Function (BRDF) of the <span class="hlt">Ocean</span>: Effects of <span class="hlt">Wave</span> Representation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eide, H.; Stamnes, K.; Ottaviani, M.</p> <p>2004-12-01</p> <p>The specular reflection of the Sun off the <span class="hlt">ocean</span>, or sun glint, is of major concern for <span class="hlt">ocean</span> remote sensing. Typically, data from in and around the sunglint region are discarded because of the unknown contribution to the measured radiances or because of sensor saturation. On the other hand, accurate knowledge of the sunglint properties enables retrievals of atmospheric parameters. The challenge of the <span class="hlt">ocean</span> retrieval problem is to get the ``water leaving radiance'', Lw, by subtracting the Rayleigh scattering, aerosol scattering, water vapor, ozone, and sun glint from the measured radiances at the top of the atmosphere (TOA). Thus, the task is to correct for both the atmospheric contribution and for surface effects. Two simplifying assumptions that are frequently employed in <span class="hlt">ocean</span> remote sensing are that the <span class="hlt">ocean</span> BRDF is isotropic and that one can de-couple the radiative properties of the atmosphere from those of the surface. Our previous studies have shown that neglecting the inherit coupling between the atmosphere and surface can lead to large errors in the retrievals. In order to do retrievals over bright, as well as darker surfaces, it is necessary to account for this coupling between the surface and the atmosphere. In the present study we use models for the reflection of light off the <span class="hlt">ocean</span> surface to calculate the <span class="hlt">ocean</span> BRDF. The differences between the various models are investigated as is the effect of using different types of <span class="hlt">wave</span> statistics (e.g. Cox Munk). We present results from calculations where we vary the wind speed and direction as well as other parameters affecting the <span class="hlt">ocean</span> surface. The error introduced in <span class="hlt">ocean</span> retrievals by assuming an isotropic BRDF is assessed, and methods for improved treatment of sunglint are suggested.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016GeoRL..43.2773C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016GeoRL..43.2773C"><span>Hurricane-induced <span class="hlt">ocean</span> <span class="hlt">waves</span> and stokes drift and their impacts on surface transport and dispersion in the Gulf of Mexico</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Curcic, Milan; Chen, Shuyi S.; Özgökmen, Tamay M.</p> <p>2016-03-01</p> <p>Hurricane Isaac induced large surface <span class="hlt">waves</span> and a significant change in upper <span class="hlt">ocean</span> circulation in the Gulf of Mexico before making landfall at the Louisiana coast on 29 August 2012. Isaac was observed by 194 surface drifters during the Grand Lagrangian Deployment (GLAD). A coupled atmosphere-<span class="hlt">wave-ocean</span> model was used to forecast hurricane impacts during GLAD. The coupled model and drifter observations provide an unprecedented opportunity to study the impacts of hurricane-induced Stokes drift on <span class="hlt">ocean</span> surface currents. The Stokes drift induced a cyclonic (anticyclonic) rotational flow on the left (right) side of the hurricane and accounted for up to 20% of the average Lagrangian velocity. In a significant deviation from drifter measurements prior to Isaac, the scale-dependent relative diffusivity is estimated to be 6 times larger during the hurricane, which represents a deviation from Okubo's (1971) canonical results for lateral dispersion in nonhurricane conditions at the <span class="hlt">ocean</span> surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016APS..DFDG14003P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016APS..DFDG14003P"><span>Computational simulations of the interaction of water <span class="hlt">waves</span> with pitching flap-type <span class="hlt">ocean</span> <span class="hlt">wave</span> energy converters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Pathak, Ashish; Raessi, Mehdi</p> <p>2016-11-01</p> <p>Using an in-house computational framework, we have studied the interaction of water <span class="hlt">waves</span> with pitching flap-type <span class="hlt">ocean</span> <span class="hlt">wave</span> energy converters (WECs). The computational framework solves the full 3D Navier-Stokes equations and captures important effects, including the fluid-solid interaction, the nonlinear and viscous effects. The results of the computational tool, is first compared against the experimental data on the response of a flap-type WEC in a <span class="hlt">wave</span> tank, and excellent agreement is demonstrated. Further simulations at the model and prototype scales are presented to assess the validity of the Froude scaling. The simulations are used to address some important questions, such as the validity range of common WEC modeling approaches that rely heavily on the Froude scaling and the inviscid potential flow theory. Additionally, the simulations examine the role of the Keulegan-Carpenter (KC) number, which is often used as a measure of relative importance of viscous drag on bodies exposed to oscillating flows. The performance of the flap-type WECs is investigated at various KC numbers to establish the relationship between the viscous drag and KC number for such geometry. That is of significant importance because such relationship only exists for simple geometries, e.g., a cylinder. Support from the National Science Foundation is gratefully acknowledged.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19800023544','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19800023544"><span>The Seasat SAR Wind and <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Monitoring Capabilities: A case study for pass 1339m</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Beal, R. C.</p> <p>1980-01-01</p> <p>A well organized low energy 11 sec. swell system off the East Coast of the U.S. was detected with the Seasat Synthetic Aperture Radar and successfully tracked from deep water, across the continental shelf, and into shallow water. In addition, a less organized 7 sec. system was tentatively identified in the imagery. Both systems were independently confirmed with simultaneous <span class="hlt">wave</span> spectral measurements from a research pier, aircraft laser profilometer data, and Fleet Numerical Spectral <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018E%26ES..111a2008L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26ES..111a2008L"><span>Experimental Research of a New <span class="hlt">Wave</span> Energy Conversion Device</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lu, Zhongyue; Shang, Jianzhong; Luo, Zirong; Sun, Chongfei; Chen, Gewei</p> <p>2018-01-01</p> <p>With the increasing tension of contemporary social energy, the development and utilization of renewable energy has become an important development direction. As an important part of renewable energy, <span class="hlt">wave</span> energy has the characteristics of green environmental protection and abundant reserves, attracting more investment and research. For small marine equipment energy supply problem, this paper puts forward a micro <span class="hlt">wave</span> energy conversion device as the basic of heaving motion of <span class="hlt">waves</span> in the <span class="hlt">ocean</span>. This paper designed a new type of <span class="hlt">power</span> output device can solve the micro <span class="hlt">wave</span> energy conversion problem.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMDI11A0261T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMDI11A0261T"><span>Multifrequency tomography of the La Reunion mantle plume with P and S <span class="hlt">waves</span> using <span class="hlt">ocean</span> bottom seismometers in the Indian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tsekhmistrenko, M.; Sigloch, K.; Hosseini, K.</p> <p>2017-12-01</p> <p>The RHUM-RUM experiment (Reunion Hotspot Upper Mantle - Reunions Unterer Mantel) investigates the presence or absence of a whole mantle plume beneath the volcanic hotspot island of La Reunion. From 2011 to 2016, RHUM-RUM instrumented a 2000 km x 2000 km area of western Indian <span class="hlt">Ocean</span> seafloor, islands and Madagascar with broadband seismometers and hydrophones. The central component was a 13-month deployment of 57 German and French <span class="hlt">Ocean</span> Bottom Seismometers (OBS) in 2300-5600 m depth. This was supplemented by 2-3 years deployments of 37 island stations on Reunion, Mauritius, Rodrigues, the southern Seychelles, the Iles Eparses and southern Madagascar. Two partner projects contributed another 30+ stations on Madagascar. We present results of multifrequency P- and S-waveform tomography of the entire mantle column beneath the Reunion hotspot. We use all frequency passbands that efficiently transmit body <span class="hlt">waves</span> and rise above the considerable noise floor of OBS measurements. More than 200 teleseismic events during the 13-month long OBS deployment yielded usable measurements, and another 400 events before and after. We present our methods, discuss data yield and quality of <span class="hlt">ocean</span>-bottom versus island/land seismometers and hydrophones. 150,000 combined cross-correlations measurements were used in multifrequency P-<span class="hlt">wave</span> tomography, in passbands between 30 s and 2.7 s dominant period. Cross-correlation coefficients at permanent and temporal land stations are generally higher than on OBS, which are more affected by both microseismic and self-noise. Hydrophones worked more reliably, but strong reverberations from the water column mean that they are still less usable than seismograms. All measurements of the RHUM-RUM array are embedded in a global P-<span class="hlt">wave</span> inversion. Mantle structures obtained from this new, high resolution tomographic model of the La Reunion area are compared to existing tomographies. We also compare to local and global convection models in order to understand the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1013758','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1013758"><span>Proving and Improving <span class="hlt">Wave</span> Models in the Arctic <span class="hlt">Ocean</span> and its MIZ</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>in the central Arctic <span class="hlt">Ocean</span> (Hunkins, 1966); in the Antarctic MIZ, Weddell Sea, slightly larger values were reported ranging from 1.6 × 10-2 m2 s-1...unprecedented spatial resolution. Such vast fields of pancake ice have traditionally only been associated with the advancing Antarctic MIZ, and, on a smaller...achieved in an MIZ dominated by large <span class="hlt">waves</span>. Data on the break-up of a large tabular iceberg by swell, measured in Baffin Bay, were published</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1260511','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1260511"><span>Balancing <span class="hlt">Power</span> Absorption and Fatigue Loads in Irregular <span class="hlt">Waves</span> for an Oscillating Surge <span class="hlt">Wave</span> Energy Converter: Preprint</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>Tom, Nathan M.; Yu, Yi-Hsiang; Wright, Alan D.</p> <p></p> <p>The aim of this paper is to describe how to control the <span class="hlt">power</span>-to-load ratio of a novel <span class="hlt">wave</span> energy converter (WEC) in irregular <span class="hlt">waves</span>. The novel WEC that is being developed at the National Renewable Energy Laboratory combines an oscillating surge <span class="hlt">wave</span> energy converter (OSWEC) with control surfaces as part of the structure; however, this work only considers one fixed geometric configuration. This work extends the optimal control problem so as to not solely maximize the time-averaged <span class="hlt">power</span>, but to also consider the <span class="hlt">power</span>-take-off (PTO) torque and foundation forces that arise because of WEC motion. The objective function of themore » controller will include competing terms that force the controller to balance <span class="hlt">power</span> capture with structural loading. Separate penalty weights were placed on the surge-foundation force and PTO torque magnitude, which allows the controller to be tuned to emphasize either <span class="hlt">power</span> absorption or load shedding. Results of this study found that, with proper selection of penalty weights, gains in time-averaged <span class="hlt">power</span> would exceed the gains in structural loading while minimizing the reactive <span class="hlt">power</span> requirement.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-sts054-95-042.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-sts054-95-042.html"><span>Equatorial <span class="hlt">Wave</span> Line, Pacific <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>1993-01-19</p> <p>STS054-95-042 (13-19 Jan 1993) --- The Equatorial Pacific <span class="hlt">Ocean</span> is represented in this 70mm view. The international oceanographic research community is presently conducting a program called Joint Global <span class="hlt">Ocean</span> Flux Study (JGOFS) to study the global <span class="hlt">ocean</span> carbon budget. A considerable amount of effort within this program is presently being focused on the Equatorial Pacific <span class="hlt">Ocean</span> because of the high annual average biological productivity. The high productivity is the result of nearly constant easterly winds causing cool, nutrient-rich water to well up at the equator. In this view of the sun glint pattern was photographed at about 2 degrees north latitude, 103 degrees west longitude, as the Space Shuttle passed over the Equatorial Pacific. The long narrow line is the equatorial front, which defines the boundary between warm surface equatorial water and cool, recently upwelled water. Such features are of interest to the JGOFS researchers and it is anticipated that photographs such as this will benefit the JGOFS program.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20130012646','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20130012646"><span>Wind, <span class="hlt">Wave</span>, and Tidal Energy Without <span class="hlt">Power</span> Conditioning</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jones, Jack A.</p> <p>2013-01-01</p> <p>Most present wind, <span class="hlt">wave</span>, and tidal energy systems require expensive <span class="hlt">power</span> conditioning systems that reduce overall efficiency. This new design eliminates <span class="hlt">power</span> conditioning all, or nearly all, of the time. Wind, <span class="hlt">wave</span>, and tidal energy systems can transmit their energy to pumps that send high-pressure fluid to a central <span class="hlt">power</span> production area. The central <span class="hlt">power</span> production area can consist of a series of hydraulic generators. The hydraulic generators can be variable displacement generators such that the RPM, and thus the voltage, remains constant, eliminating the need for further <span class="hlt">power</span> conditioning. A series of wind blades is attached to a series of radial piston pumps, which pump fluid to a series of axial piston motors attached to generators. As the wind is reduced, the amount of energy is reduced, and the number of active hydraulic generators can be reduced to maintain a nearly constant RPM. If the axial piston motors have variable displacement, an exact RPM can be maintained for all, or nearly all, wind speeds. Analyses have been performed that show over 20% performance improvements with this technique over conventional wind turbines</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19840019211','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19840019211"><span><span class="hlt">Ocean</span> <span class="hlt">waves</span> and turbulence as observed with an adaptive coherent multifrequency radar</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Gjessing, D. T.; Hjelmstad, J.</p> <p>1984-01-01</p> <p>An adaptive coherent multifrequency radar system is developed for several applications. The velocity distribution (Doppler spectrum) and spectral intensity of 15 different irregularity scales (<span class="hlt">waves</span> and turbulence) can be measured simultaneously. Changing the azimuth angle of the antennas at regular intervals, the directivity of the <span class="hlt">wave</span>/turbulence pattern on the sea surface can also be studied. A series of measurements for different air/sea conditions are carried out from a coast based platform. Experiments in the Atlantic are also performed with the same equipment making use of the NASA Electra aircraft. The multifrequency radar allows the measurement of the velocity distribution (""coherent and incoherent component'') associated with 15 different <span class="hlt">ocean</span> irregularity scales simultaneously in a directional manner. It is possible to study the different air/sea mechanisms in some degree of detail.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOS.A33A..03R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOS.A33A..03R"><span>Novel Methods for Optically Measuring Whitecaps Under Natural <span class="hlt">Wave</span> Breaking Conditions in the Southern <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Randolph, K. L.; Dierssen, H. M.; Cifuentes-Lorenzen, A.; Balch, W. M.; Monahan, E. C.; Zappa, C. J.; Drapeau, D.; Bowler, B.</p> <p>2016-02-01</p> <p>Breaking <span class="hlt">waves</span> on the <span class="hlt">ocean</span> surface mark areas of significant importance to air-sea flux estimates of gas, aerosols, and heat. Traditional methods of measuring whitecap coverage using digital photography can miss features that are small in size or do not show high enough contrast to the background. The geometry of the images collected captures the near surface, bright manifestations of the whitecap feature and miss a portion of the bubble plume that is responsible for the production of sea salt aerosols and the transfer of lower solubility gases. Here, a novel method for accurately measuring both the fractional coverage of whitecaps and the intensity and decay rate of whitecap events using above water radiometry is presented. The methodology was developed using data collected during the austral summer in the Atlantic sector of the Southern <span class="hlt">Ocean</span> under a large range of wind (speeds of 1 to 15 m s-1) and <span class="hlt">wave</span> (significant <span class="hlt">wave</span> heights 2 to 8 m) conditions as part of the Southern <span class="hlt">Ocean</span> Gas Exchange experiment. Whitecap metrics were retrieved by employing a magnitude threshold based on the interquartile range of the radiance or reflectance signal for a single channel (411 nm) after a baseline removal, determined using a moving minimum/maximum filter. Breaking intensity and decay rate metrics were produced from the integration of, and the exponential fit to, radiance or reflectance over the lifetime of the whitecap. When compared to fractional whitecap coverage measurements obtained from high resolution digital images, radiometric estimates were consistently higher because they capture more of the decaying bubble plume area that is difficult to detect with photography. Radiometrically-retrieved whitecap measurements are presented in the context of concurrently measured meteorological (e.g., wind speed) and oceanographic (e.g., <span class="hlt">wave</span>) data. The optimal fit of the radiometrically estimated whitecap coverage to the instantaneous wind speed, determined using ordinary least</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_14");'>14</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li class="active"><span>16</span></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_16 --> <div id="page_17" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_15");'>15</a></li> <li><a href="#" onclick='return showDiv("page_16");'>16</a></li> <li class="active"><span>17</span></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="321"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012PhDT........34B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012PhDT........34B"><span>Software framework for prognostic health monitoring of <span class="hlt">ocean</span>-based <span class="hlt">power</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>Bowren, Mark</p> <p></p> <p>On August 5, 2010 the U.S. Department of Energy (DOE) has designated the Center for <span class="hlt">Ocean</span> Energy Technology (COET) at Florida Atlantic University (FAU) as a national center for <span class="hlt">ocean</span> energy research and development of prototypes for open-<span class="hlt">ocean</span> <span class="hlt">power</span> generation. Maintenance on <span class="hlt">ocean</span>-based machinery can be very costly. To avoid unnecessary maintenance it is necessary to monitor the condition of each machine in order to predict problems. This kind of prognostic health monitoring (PHM) requires a condition-based maintenance (CBM) system that supports diagnostic and prognostic analysis of large amounts of data. Research in this field led to the creation of ISO13374 and the development of a standard open-architecture for machine condition monitoring. This thesis explores an implementation of such a system for <span class="hlt">ocean</span>-based machinery using this framework and current open-standard technologies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.S41A2750G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.S41A2750G"><span>Rayleigh <span class="hlt">Wave</span> Phase Velocity in the Upper Mantle Beneath the Indian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Godfrey, K. E.; Dalton, C. A.; Ritsema, J.</p> <p>2016-12-01</p> <p>Most of what is currently understood about the seismic properties of <span class="hlt">oceanic</span> upper mantle is based on either global studies or regional studies of the upper mantle beneath the Pacific <span class="hlt">Ocean</span>. However, global seismic models and geochemical studies of mid-<span class="hlt">ocean</span> ridge basalts indicate differences in the properties of the upper mantle beneath the Pacific, Atlantic, and Indian <span class="hlt">oceans</span>. Though the Indian <span class="hlt">Ocean</span> is not as well studied seismically, it is host to a number of geologically interesting features including 16,000 km of mid-<span class="hlt">ocean</span> ridge with a range of spreading rates from 14 mm/yr along the Southwest Indian Ridge to 55-75 mm/yr along the Southeast Indian Ridge. The Indian <span class="hlt">Ocean</span> also contains multiple volcanic hotspots, the Australian-Antarctic Discordance, and a low geoid anomaly south of India, and it overlies a portion of a large low-shear-velocity province. We are using Rayleigh <span class="hlt">waves</span> to construct a high-resolution seismic velocity model of the Indian <span class="hlt">Ocean</span> upper mantle. We utilize a global dataset of phase delays measured at 20 periods, between 37 and 375 seconds; the dataset includes between 700 and 20,000 that traverse our study region exclusively, with a larger number of paths at shorter periods. We explore variations in phase velocity using two separate approaches. One, we allow phase velocity to vary only as a function of seafloor age. Two, we perform a damped least-squares inversion to solve for 2-D phase velocity maps at each period. Preliminary results indicate low velocities along the Southeast Indian Ridge and Central Indian Ridge, but the expected low velocities are less apparent along the slow-spreading Southwest Indian Ridge. We observe a region of fast velocities extending from Antarctica northward between the Kerguelen and Crozet hotspots, and lower than expected velocities beneath the Reunion hotspot. Additionally, we find low velocities associated with a region of extinct seafloor spreading in the Wharton basin.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..1710469S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..1710469S"><span>Coupling of <span class="hlt">wave</span> and circulation models in coastal-<span class="hlt">ocean</span> predicting systems: A case study for the German Bight</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; Wahle, Kathrin</p> <p>2015-04-01</p> <p>This study addresses the coupling between wind <span class="hlt">wave</span> 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-<span class="hlt">waves</span>, 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 <span class="hlt">ocean</span> state variables, including wind <span class="hlt">waves</span> and hydrodynamics. In this study we present analysis of <span class="hlt">wave</span> 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, <span class="hlt">waves</span> and tidal forcing are quantified. The performance of the forecasting system is illustrated for the cases of several extreme events. Effects of <span class="hlt">ocean</span> <span class="hlt">waves</span> on coastal circulation and SST simulations are investigated considering <span class="hlt">wave</span>-dependent stress and <span class="hlt">wave</span> breaking parameterization during extreme events, e.g. hurricane Xavier in December, 2013. Also the effect which the circulation exerts on the wind <span class="hlt">waves</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017LatJP..54d..23B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017LatJP..54d..23B"><span>Measurements of <span class="hlt">Wave</span> <span class="hlt">Power</span> in <span class="hlt">Wave</span> Energy Converter Effectiveness Evaluation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Berins, J.; Berins, J.; Kalnacs, A.</p> <p>2017-08-01</p> <p>The article is devoted to the technical solution of alternative budget measuring equipment of the water surface gravity <span class="hlt">wave</span> oscillation and the theoretical justification of the calculated oscillation <span class="hlt">power</span>. This solution combines technologies such as lasers, WEB-camera image digital processing, interpolation of defined function at irregular intervals, volatility of discrete Fourier transformation for calculating the spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMOS41B1959G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMOS41B1959G"><span>Reduction of Magnetic Noise Associated with <span class="hlt">Ocean</span> <span class="hlt">Waves</span> by Sage-Husa Adaptive Kalman Filter in Towed Overhauser Marine Magnetic Sensor</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>GE, J.; Dong, H.; Liu, H.; Luo, W.</p> <p>2016-12-01</p> <p>In the extreme sea conditions and deep-sea detection, the towed Overhauser marine magnetic sensor is easily affected by the magnetic noise associated with <span class="hlt">ocean</span> <span class="hlt">waves</span>. We demonstrate the reduction of the magnetic noise by Sage-Husa adaptive Kalman filter. Based on Weaver's model, we analyze the induced magnetic field variations associated with the different <span class="hlt">ocean</span> depths, <span class="hlt">wave</span> periods and amplitudes in details. Furthermore, we take advantage of the classic Kalman filter to reduce the magnetic noise and improve the signal to noise ratio of the magnetic anomaly data. In the practical marine magnetic surveys, the extreme sea conditions can change priori statistics of the noise, and may decrease the effect of Kalman filtering estimation. To solve this problem, an improved Sage-Husa adaptive filtering algorithm is used to reduce the dependence on the prior statistics. In addition, we implement a towed Overhauser marine magnetometer (Figure 1) to test the proposed method, and it consists of a towfish, an Overhauser total field sensor, a console, and other condition monitoring sensors. Over all, the comparisons of simulation experiments with and without the filter show that the <span class="hlt">power</span> spectral density of the magnetic noise is reduced to 0.1 nT/Hz1/2@1Hz from 1 nT/Hz1/2@1Hz. The contrasts between the Sage-Husa filter and the classic Kalman filter (Figure 2) show the filtering accuracy and adaptive capacity are improved.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005PhDT........22V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005PhDT........22V"><span>On the role of high frequency <span class="hlt">waves</span> in <span class="hlt">ocean</span> altimetry</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vandemark, Douglas C.</p> <p></p> <p>This work mines a coastal and open <span class="hlt">ocean</span> air-sea interaction field experiment data set where the goals are to refine satellite retrieval of wind, wind stress, and sea level using a microwave radar altimeter. The data were collected from a low-flying aircraft using a sensor suite designed to measure the surface <span class="hlt">waves</span>, radar backscatter, the atmospheric flow, and turbulent fluxes within the marine boundary layer. This uncommon ensemble provides the means to address several specific altimeter-related topics. First, we examine and document the impact that non wind-driven gravity <span class="hlt">wave</span> variability, e.g. swell, has upon the commonly-invoked direct relationship between altimeter backscatter and near surface wind speed. The demonstrated impact is larger in magnitude and more direct than previously suggested. The study also isolates the wind-dependence of short-scale slope variance and suggests its magnitude is somewhat lower than shown elsewhere while a second-order dependence on long <span class="hlt">waves</span> is also evident. A second study assesses the hypothesis that wind-aligned swell interacts with the atmospheric boundary flow leading to a depressed level of turbulence. Cases of reduced drag coefficient at moderate wind speeds were in evidence within the data set, and buoy observations indicate that swell was present and a likely control during these events. Coincidentally, short-scale <span class="hlt">wave</span> roughness was also depressed suggesting decreased wind stress. Attempts to confirm the theory failed, however, due to numerous limitations in the quantity and quality of the data in hand. A lesson learned is that decoupling atmospheric stability and <span class="hlt">wave</span> impacts in field campaigns requires both a very large amount of data as well as vertical resolution of fluxes within the first 10--20 m of the surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70033525','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70033525"><span>Surface drift prediction in the Adriatic Sea using hyper-ensemble statistics on atmospheric, <span class="hlt">ocean</span> and <span class="hlt">wave</span> models: Uncertainties and probability distribution areas</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Rixen, M.; Ferreira-Coelho, E.; Signell, R.</p> <p>2008-01-01</p> <p>Despite numerous and regular improvements in underlying models, surface drift prediction in the <span class="hlt">ocean</span> remains a challenging task because of our yet limited understanding of all processes involved. Hence, deterministic approaches to the problem are often limited by empirical assumptions on underlying physics. Multi-model hyper-ensemble forecasts, which exploit the <span class="hlt">power</span> of an optimal local combination of available information including <span class="hlt">ocean</span>, atmospheric and <span class="hlt">wave</span> models, may show superior forecasting skills when compared to individual models because they allow for local correction and/or bias removal. In this work, we explore in greater detail the potential and limitations of the hyper-ensemble method in the Adriatic Sea, using a comprehensive surface drifter database. The performance of the hyper-ensembles and the individual models are discussed by analyzing associated uncertainties and probability distribution maps. Results suggest that the stochastic method may reduce position errors significantly for 12 to 72??h forecasts and hence compete with pure deterministic approaches. ?? 2007 NATO Undersea Research Centre (NURC).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMNG21A0131P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMNG21A0131P"><span>The Stability of Outcropping <span class="hlt">Ocean</span> Eddies</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Paldor, N.; Cohen, Y.; Dvorkin, Y.</p> <p>2017-12-01</p> <p>In the end of the last century numerous ship-borne observations and linear instability studies have addressed the long life span of meso-scale <span class="hlt">ocean</span> eddies. These eddies are observed to persist in the <span class="hlt">ocean</span> for periods of 2-3 years with little deformation. As eddy instabilities occur because Rossby <span class="hlt">waves</span> in the surrounding (assumed motionless) <span class="hlt">ocean</span> interact with various <span class="hlt">waves</span> in the eddy itself, the stability was attributed to some eddy structure that hinders such <span class="hlt">wave-wave</span> interactions. However, instabilities with growthrates of the order of the inertial period were found in various multilayer models including hypothesized structures and several observed eddy structures. A solution to the difference between instability theory and observed stability was ultimately suggested by relaxing the assumption of a motionless <span class="hlt">ocean</span> that surrounds the eddy and prescribing the mean flow in the <span class="hlt">ocean</span> such that it counterbalances the depth changes imposed by the eddy while maintaining a constant PV-<span class="hlt">ocean</span>. This hypothesis was successfully applied to Gaussian eddies for mathematical simplicity. Yet, the Gaussian eddy has no surface front - thus avoiding instabilities that involve frontal <span class="hlt">waves</span> - and it disagrees with observation that clearly show that most eddies have surface fronts. Here the constant PV <span class="hlt">ocean</span> hypothesis is applied to two frontal eddies: constant PV-eddies and solidly rotating eddy. A complete account of the mean flow of the coupled eddy-<span class="hlt">ocean</span> system is analyzed using a canonical formulation of the gradient balance. The phase speeds of <span class="hlt">waves</span> in the eddy-<span class="hlt">ocean</span> system are computed by a shooting method. Both eddies are found to be unstable in motionless <span class="hlt">ocean</span>, yet in a constant PV-<span class="hlt">ocean</span> no instabilities are found using the exact same numerical search. While many eddy structures can be hypothesized there are only a handful of physical mechanisms for instability and in these eddies the assumed constant PV-<span class="hlt">ocean</span> negates many of these physical mechanisms for instability</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870051568&hterms=Wave+filter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DWave%2Bfilter','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870051568&hterms=Wave+filter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DWave%2Bfilter"><span>SIR-B <span class="hlt">ocean-wave</span> enhancement with fast Fourier transform techniques</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tilley, David G.</p> <p>1987-01-01</p> <p>Shuttle Imaging Radar (SIR-B) imagery is Fourier filtered to remove the estimated system-transfer function, reduce speckle noise, and produce <span class="hlt">ocean</span> scenes with a gray scale that is proportional to <span class="hlt">wave</span> height. The SIR-B system response to speckled scenes of uniform surfaces yields an estimate of the stationary wavenumber response of the imaging radar, modeled by the 15 even terms of an eighth-order two-dimensional polynomial. Speckle can also be used to estimate the dynamic wavenumber response of the system due to surface motion during the aperture synthesis period, modeled with a single adaptive parameter describing an exponential correlation along track. A Fourier filter can then be devised to correct for the wavenumber response of the remote sensor and scene correlation, with subsequent subtraction of an estimate of the speckle noise component. A linearized velocity bunching model, combined with a surface tilt and hydrodynamic model, is incorporated in the Fourier filter to derive estimates of <span class="hlt">wave</span> height from the radar intensities corresponding to individual picture elements.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OcMod.124...75C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OcMod.124...75C"><span>Extreme wind-<span class="hlt">wave</span> modeling and analysis in the south Atlantic <span class="hlt">ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Campos, R. M.; Alves, J. H. G. M.; Guedes Soares, C.; Guimaraes, L. G.; Parente, C. E.</p> <p>2018-04-01</p> <p>A set of <span class="hlt">wave</span> hindcasts is constructed using two different types of wind calibration, followed by an additional test retuning the input source term Sin in the <span class="hlt">wave</span> model. The goal is to improve the simulation in extreme <span class="hlt">wave</span> events in the South Atlantic <span class="hlt">Ocean</span> without compromising average conditions. Wind fields are based on Climate Forecast System Reanalysis (CFSR/NCEP). The first wind calibration applies a simple linear regression model, with coefficients obtained from the comparison of CFSR against buoy data. The second is a method where deficiencies of the CFSR associated with severe sea state events are remedied, whereby "defective" winds are replaced with satellite data within cyclones. A total of six wind datasets forced WAVEWATCH-III and additional three tests with modified Sin in WAVEWATCH III lead to a total of nine <span class="hlt">wave</span> hindcasts that are evaluated against satellite and buoy data for ambient and extreme conditions. The target variable considered is the significant <span class="hlt">wave</span> height (Hs). The increase of sea-state severity shows a progressive increase of the hindcast underestimation which could be calculated as a function of percentiles. The wind calibration using a linear regression function shows similar results to the adjustments to Sin term (increase of βmax parameter) in WAVEWATCH-III - it effectively reduces the average bias of Hs but cannot avoid the increase of errors with percentiles. The use of blended scatterometer winds within cyclones could reduce the increasing <span class="hlt">wave</span> hindcast errors mainly above the 93rd percentile and leads to a better representation of Hs at the peak of the storms. The combination of linear regression calibration of non-cyclonic winds with scatterometer winds within the cyclones generated a <span class="hlt">wave</span> hindcast with small errors from calm to extreme conditions. This approach led to a reduction of the percentage error of Hs from 14% to less than 8% for extreme <span class="hlt">waves</span>, while also improving the RMSE.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000013562','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000013562"><span><span class="hlt">Waves</span>: Internal Tides</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ray, Richard D.</p> <p>1999-01-01</p> <p><span class="hlt">Oceanic</span> internal tides are internal <span class="hlt">waves</span> with tidal periodicities. They are ubiquitous throughout the <span class="hlt">ocean</span>, although generally more pronounced near large bathymetric features such as mid-<span class="hlt">ocean</span> ridges and continental slopes. The internal vertical displacements associated with these <span class="hlt">waves</span> can be extraordinarily large. Near some shelf breaks where the surface tides are strong, internal displacements (e.g., of an isothermal surface) can exceed 200 meters. Displacements of 10 meters in the open <span class="hlt">ocean</span> are not uncommon. The associated current velocities are usually comparable to or larger than the currents of the surface tide. On continental shelves internal tides can occasionally generate packets of internal solitons, which are detectable in remote sensing imagery. Other common nonlinear features are generation of higher harmonics (e.g., 6-hr <span class="hlt">waves</span>) and <span class="hlt">wave</span> breaking. Internal tides are known to be an important energy source for mixing of shelf waters. Recent research suggests that they may also be a significant energy source for deep-<span class="hlt">ocean</span> mixing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUFMED53A0323L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUFMED53A0323L"><span>The <span class="hlt">Waves</span> and Tsunamis Project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lavin, M.; Strohschneider, D.; Maichle, R.; Frashure, K.; Micozzi, N.; Stephen, R. A.</p> <p>2005-12-01</p> <p>The goals of the <span class="hlt">Waves</span> and Tsunamis Project are "to make <span class="hlt">waves</span> real" to middle school students and to teach them some fundamental concepts of <span class="hlt">waves</span>. The curriculum was designed in Fall 2004 (before the Sumatra Tsunami) and involves an <span class="hlt">ocean</span> scientist classroom visit, hands-on demonstrations, and an interactive website designed to explain <span class="hlt">ocean</span> <span class="hlt">wave</span> properties. The website is called 'The Plymouth <span class="hlt">Wave</span> Lab' and it has had more than 40,000 hits since the Sumatra event. One inexpensive and interesting demonstration is based on a string composed of alternating elastic bands and paper clips. Washers can be added to the paper clips to construct strings with varying mass. For example, a tapered string with mass decreasing in the <span class="hlt">wave</span> propagation direction is an analog of tsunami <span class="hlt">waves</span> propagating from deep to shallow water. The <span class="hlt">Waves</span> and Tsunamis Project evolved as a collaborative effort involving an <span class="hlt">ocean</span> science researcher and middle school science teachers. It was carried out through the direction of the Centers of <span class="hlt">Ocean</span> Science Education Excellence New England (COSEE-NE) <span class="hlt">Ocean</span> Science Education Institute (OSEI). COSEE-NE is involved in developing models for sustainable involvement of <span class="hlt">ocean</span> science researchers in K-12 education ( http://necosee.net ). This work is supported by the National Science Foundation.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.5900W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.5900W"><span>Surface <span class="hlt">wave</span> effect on the upper <span class="hlt">ocean</span> in marine forecast</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Guansuo; Qiao, Fangli; Xia, Changshui; Zhao, Chang</p> <p>2015-04-01</p> <p>An Operational Coupled Forecast System for the seas off China and adjacent (OCFS-C) is constructed based on the paralleled <span class="hlt">wave</span>-circulation coupled model, which is tested with comprehensive experiments and operational since November 1st, 2007. The main feature of the system is that the <span class="hlt">wave</span>-induced mixing is considered in circulation model. Daily analyses and three day forecasts of three-dimensional temperature, salinity, currents and <span class="hlt">wave</span> height are produced. Coverage is global at 1/2 degreed resolution with nested models up to 1/24 degree resolution in China Sea. Daily remote sensing sea surface temperatures (SST) are taken to relax to an analytical product as hot restarting fields for OCFS-C by the Nudging techniques. Forecasting-data inter-comparisons are performed to measure the effectiveness of OCFS-C in predicting upper-<span class="hlt">ocean</span> quantities including SST, mixed layer depth (MLD) and subsurface temperature. The variety of performance with lead time and real-time is discussed as well using the daily statistic results for SST between forecast and satellite data. Several buoy observations and many Argo profiles are used for this validation. Except the conventional statistical metrics, non-dimension skill scores (SS) is taken to estimate forecast skill. Model SST comparisons with more one year-long SST time series from 2 buoys given a large SS value (more than 0.90). And skill in predicting the seasonal variability of SST is confirmed. Model subsurface temperature comparisons with that from a lot of Argo profiles indicated that OCFS-C has low skill in predicting subsurface temperatures between 80m and 120m. Inter-comparisons of MLD reveal that MLD from model is shallower than that from Argo profiles by about 12m. QCFS-C is successful and steady in predicting MLD. The daily statistic results for SST between 1-d, 2-d and 3-d forecast and data is adopted to describe variability of Skill in predicting SST with lead time or real time. In a word QCFS-C shows reasonable</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1998JASTP..60.1225B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1998JASTP..60.1225B"><span>Excitation of small-scale <span class="hlt">waves</span> in the F region of the ionosphere by <span class="hlt">powerful</span> HF radio <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>Blagoveshchenskaya, N. F.; Chernyshev, M. Y.; Kornienko, V. A.</p> <p>1998-01-01</p> <p>Ionospheric small-scale <span class="hlt">waves</span> in the F region, initiated by heating facilities in Nizhniy Novgorod, have been studied by the method of field-aligned scattering of diagnostic HF radio signals. Experimental data have been obtained on the radio path Kiev-N. Novgorod-St. Petersburg during heating campaigns with heater radiated <span class="hlt">power</span> ERP = 20 MW and 100 MW. Observations of scattered HF signals have been made by a Doppler spectrum device with high temporal resolution. Analysis of the experimental data shows a relation between the heater <span class="hlt">power</span> level and the parameters of ionospheric small-scale oscillations falling within the range of Pc 3-4 magnetic pulsations. It is found that the periods of <span class="hlt">wave</span> processes in the F region of the ionosphere, induced by the heating facility, decrease with increasing heating <span class="hlt">power</span>. The level of heating <span class="hlt">power</span> also has an impact on the horizontal east-west component of the electric field E, the vertical component of the Doppler velocity Vd and the amplitude of the vertical displacements M of the heated region. Typical magnitudes of these parameters are the following: E = 1.25 mVm, Vd = 6 ms, M = 600-1500 m for ERP = 20 MW and E = 2.5-4.5 mVm, Vd = 11-25 ms, M = 1000-5000 m for ERP = 100 MW. The results obtained confirm the hypothesis of excitation of the Alfvén resonator by <span class="hlt">powerful</span> HF radio <span class="hlt">waves</span> which leads to the generation of magnetic field oscillations in the heated region giving rise to artificial Pc 3-4 magnetic pulsations and ionospheric small-scale <span class="hlt">wave</span> processes. In this situation an increase of the heater <span class="hlt">power</span> would lead to a growth of the electric field of hydromagnetic <span class="hlt">waves</span> propagating in the ionosphere as well as the amplitude of the vertical displacements of the heated region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.7951D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.7951D"><span>Classification and Possible Causes of the Freaque <span class="hlt">Waves</span> Occurred in Taiwanese Coastal <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Doong, Dong-Jiing; Liu, Paul C.; Tsai, Cheng-Han; Tsai, Jen-Chih</p> <p>2015-04-01</p> <p>Freaque <span class="hlt">waves</span> occur frequently in Taiwanese coastal <span class="hlt">ocean</span>. This study collected and confirmed the media reported freaque <span class="hlt">wave</span> events since 2000. There were 90 shipwrecks struck by extreme large <span class="hlt">waves</span> or freaque <span class="hlt">waves</span> from 2003 to 2014. In addition, 284 events of people swept into the sea from the coasts by freaque <span class="hlt">waves</span> were recorded from 2000 to 2014. More than 950 persons in total were dead or injured for the past 15 years. This study classifies these cases according to their possible causes and the weather conditions of that time. It is found the probability of the events occurred during storm (typhoon) period is less than 15%. Most of the events occur in ordinary sea states. Analysis on the data from in-situ measurements that close to the event locations shows the average significant <span class="hlt">wave</span> height is 1.46m. This study uses this threshold and long-term observations on sea states to present the navigation risk of ships in Taiwanese sea. In addition, it was found the typhoon generated swell is one of the causes to trigger the giant coastal freaque <span class="hlt">waves</span>, experiences learning from the events occurred in typhoon Haiyan in 2013 (16 persons were swept into sea), typhoon Prapiroon in 2012 (3 persons and 2 cars were swept into sea), typhoon Neoguri in 2014 (7 persons were swept) and typhoon Vongfong in 2014 (1 motorcyclist was swept). Those typhoon swell induced coastal freaque <span class="hlt">wave</span> is the worst case because they always occur with good weather conditions. Analysis on the field data shows the swell direction is a crucial factor for the coastal freaque <span class="hlt">wave</span> occurrence.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/22071362','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/22071362"><span>Distribution of <span class="hlt">oceanic</span> 137Cs from the Fukushima Dai-ichi Nuclear <span class="hlt">Power</span> Plant simulated numerically by a regional <span class="hlt">ocean</span> model.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Tsumune, Daisuke; Tsubono, Takaki; Aoyama, Michio; Hirose, Katsumi</p> <p>2012-09-01</p> <p>Radioactive materials were released to the environment from the Fukushima Dai-ichi Nuclear <span class="hlt">Power</span> Plant as a result of the reactor accident after the Tohoku earthquake and tsunami of 11 March 2011. The measured (137)Cs concentration in a seawater sample near the Fukushima Dai-ichi Nuclear <span class="hlt">Power</span> Plant site reached 68 kBq L(-1) (6.8 × 10(4)Bq L(-1)) on 6 April. The two major likely pathways from the accident site to the <span class="hlt">ocean</span> existed: direct release of high radioactive liquid wastes to the <span class="hlt">ocean</span> and the deposition of airborne radioactivity to the <span class="hlt">ocean</span> surface. By analysis of the (131)I/(137)Cs activity ratio, we determined that direct release from the site contributed more to the measured (137)Cs concentration than atmospheric deposition did. We then used a regional <span class="hlt">ocean</span> model to simulate the (137)Cs concentrations resulting from the direct release to the <span class="hlt">ocean</span> off Fukushima and found that from March 26 to the end of May the total amount of (137)Cs directly released was 3.5 ± 0.7 PBq ((3.5 ± 0.7) × 10(15)Bq). The simulated temporal change in (137)Cs concentrations near the Fukushima Daini Nuclear <span class="hlt">Power</span> Plant site agreed well with observations. Our simulation results showed that (1) the released (137)Cs advected southward along the coast during the simulation period; (2) the eastward-flowing Kuroshio and its extension transported (137)C during May 2011; and (3) (137)Cs concentrations decreased to less than 10 BqL(-1) by the end of May 2011 in the whole simulation domain as a result of <span class="hlt">oceanic</span> advection and diffusion. We compared the total amount and concentration of (137)Cs released from the Fukushima Dai-ichi reactors to the <span class="hlt">ocean</span> with the (137)Cs released to the <span class="hlt">ocean</span> by global fallout. Even though the measured (137)Cs concentration from the Fukushima accident was the highest recorded, the total released amount of (137)Cs was not very large. Therefore, the effect of (137)Cs released from the Fukushima Dai-ichi reactors on concentration in the whole North</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1914904P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1914904P"><span><span class="hlt">Wave</span>SAX device: design optimization through scale modelling and a PTO strategical control system</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Peviani, Maximo; Danelli, Andrea; Dadone, Gianluca; Dalmasso, Alberto</p> <p>2017-04-01</p> <p><span class="hlt">Wave</span>SAX is an innovative OWC (Oscillating Water Column) device for the generation of electricity from <span class="hlt">wave</span> <span class="hlt">power</span>, conceived to be installed in coastal marine structures, such as ports and harbours. The device - especially designed for the typical <span class="hlt">wave</span> climate of Mediterranean Sea - is characterized by two important aspects: flexibility to fit in different structural configurations and replication in a large number of units. A model of the <span class="hlt">Wave</span>SAX device on a scale 1:5 has been built and tested in the <span class="hlt">ocean</span> tank at Ecole Centrale de Nantes (France). The study aimed to analyse the behaviour of the device, including two Wells turbine configurations (with three and four blades), with regular and irregular <span class="hlt">wave</span> conditions in the <span class="hlt">ocean</span> <span class="hlt">wave</span> tank. The model and the <span class="hlt">wave</span> basin were equipped with a series of sensors which allowed to measure the following parameters during the tests: pressure in different points inside the device, the free water surface displacement inside and outside the device, the rotational velocity and the torque at the top of the axis. The tests had the objective to optimize the device design, especially as far as the characteristics of the rotor of the turbine is concern. Although the performance of the <span class="hlt">Wave</span>SAX has been satisfactory for regular <span class="hlt">wave</span> conditions, the behaviour of the Wells turbines for irregular <span class="hlt">wave</span> climate has shown limitations in terms of maintaining the capacity to transform hydraulics energy into mechanical <span class="hlt">power</span>. To optimize the efficiency of the turbine, an electronical system has been built on the basis of the <span class="hlt">ocean</span> tank tests. It allows to continuously monitor and command the rotational speed and the torque of the rotor connected with the turbine, and to control in real time the electrical flow of a motor-generator, either absorbing energy as a generator, or providing <span class="hlt">power</span> to the turbine working as an engine. Two strategies - based on the velocity and the torque control - have been investigate in the electronic test bench</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19810003785','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19810003785"><span>An analysis of short pulse and dual frequency radar techniques for measuring <span class="hlt">ocean</span> <span class="hlt">wave</span> spectra from satellites</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Jackson, F. C.</p> <p>1980-01-01</p> <p>Scanning beam microwave radars were used to measure <span class="hlt">ocean</span> <span class="hlt">wave</span> directional spectra from satellites. In principle, surface <span class="hlt">wave</span> spectral resolution in <span class="hlt">wave</span> number can be obtained using either short pulse (SP) or dual frequency (DF) techniques; in either case, directional resolution obtains naturally as a consequence of a Bragg-like <span class="hlt">wave</span> front matching. A four frequency moment characterization of backscatter from the near vertical using physical optics in the high frequency limit was applied to an analysis of the SP and DF measurement techniques. The intrinsic electromagnetic modulation spectrum was to the first order in <span class="hlt">wave</span> steepness proportional to the large <span class="hlt">wave</span> directional slope spectrum. Harmonic distortion was small and was a minimum near 10 deg incidence. NonGaussian <span class="hlt">wave</span> statistics can have an effect comparable to that in the second order of scattering from a normally distributed sea surface. The SP technique is superior to the DF technique in terms of measurement signal to noise ratio and contrast ratio.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20180002915&hterms=oceans+climate+changes&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Doceans%2Bclimate%2Bchanges','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20180002915&hterms=oceans+climate+changes&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D80%26Ntt%3Doceans%2Bclimate%2Bchanges"><span>Effect of Gravity <span class="hlt">Waves</span> from Small Islands in the Southern <span class="hlt">Ocean</span> on the Southern Hemisphere Atmospheric Circulation</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Garfinkel, C. I.; Oman, L. D.</p> <p>2018-01-01</p> <p>The effect of small islands in the Southern <span class="hlt">Ocean</span> on the atmospheric circulation in the Southern Hemisphere is considered with a series of simulations using the NASA Goddard Earth Observing System Chemistry-Climate Model in which the gravity <span class="hlt">wave</span> stress generated by these islands is increased to resemble observed values. The enhanced gravity <span class="hlt">wave</span> drag leads to a 2 K warming of the springtime polar stratosphere, partially ameliorating biases in this region. Resolved <span class="hlt">wave</span> drag declines in the stratospheric region in which the added orographic gravity <span class="hlt">waves</span> deposit their momentum, such that changes in gravity <span class="hlt">waves</span> are partially compensated by changes in resolved <span class="hlt">waves</span>, though resolved <span class="hlt">wave</span> drag increases further poleward. The orographic drag from these islands has impacts for surface climate, as biases in tropospheric jet position are also partially ameliorated. These results suggest that these small islands are likely contributing to the missing drag near 60 degrees S in the upper stratosphere evident in many data assimilation products.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26148491','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26148491"><span>Energy Flux in the Cochlea: Evidence Against <span class="hlt">Power</span> Amplification of the Traveling <span class="hlt">Wave</span>.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>van der Heijden, Marcel; Versteegh, Corstiaen P C</p> <p>2015-10-01</p> <p>Traveling <span class="hlt">waves</span> in the inner ear exhibit an amplitude peak that shifts with frequency. The peaking is commonly believed to rely on motile processes that amplify the <span class="hlt">wave</span> by inserting energy. We recorded the vibrations at adjacent positions on the basilar membrane in sensitive gerbil cochleae and tested the putative <span class="hlt">power</span> amplification in two ways. First, we determined the energy flux of the traveling <span class="hlt">wave</span> at its peak and compared it to the acoustic <span class="hlt">power</span> entering the ear, thereby obtaining the net cochlear <span class="hlt">power</span> gain. For soft sounds, the energy flux at the peak was 1 ± 0.6 dB less than the middle ear input <span class="hlt">power</span>. For more intense sounds, increasingly smaller fractions of the acoustic <span class="hlt">power</span> actually reached the peak region. Thus, we found no net <span class="hlt">power</span> amplification of soft sounds and a strong net attenuation of intense sounds. Second, we analyzed local <span class="hlt">wave</span> propagation on the basilar membrane. We found that the <span class="hlt">waves</span> slowed down abruptly when approaching their peak, causing an energy densification that quantitatively matched the amplitude peaking, similar to the growth of sea <span class="hlt">waves</span> approaching the beach. Thus, we found no local <span class="hlt">power</span> amplification of soft sounds and strong local attenuation of intense sounds. The most parsimonious interpretation of these findings is that cochlear sensitivity is not realized by amplifying acoustic energy, but by spatially focusing it, and that dynamic compression is realized by adjusting the amount of dissipation to sound intensity.</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('http://adsabs.harvard.edu/abs/2016RSPSA.47260715R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016RSPSA.47260715R"><span>Hydroelectromechanical modelling 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-coupled 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 <span class="hlt">ocean</span> 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 couple 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 coupling 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 <span class="hlt">power</span>. We determine the hydroelectromechanical resonant periods of the device, at which the <span class="hlt">power</span> output is significant.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005mmmp.book.....B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005mmmp.book.....B"><span>Modern Microwave and Millimeter-<span class="hlt">Wave</span> <span class="hlt">Power</span> Electronics</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Barker, Robert J.; Luhmann, Neville C.; Booske, John H.; Nusinovich, Gregory S.</p> <p>2005-04-01</p> <p>A comprehensive study of microwave vacuum electronic devices and their current and future applications While both vacuum and solid-state electronics continue to evolve and provide unique solutions, emerging commercial and military applications that call for higher <span class="hlt">power</span> and higher frequencies to accommodate massive volumes of transmitted data are the natural domain of vacuum electronics technology. Modern Microwave and Millimeter-<span class="hlt">Wave</span> <span class="hlt">Power</span> Electronics provides systems designers, engineers, and researchers-especially those with primarily solid-state training-with a thoroughly up-to-date survey of the rich field of microwave vacuum electronic device (MVED) technology. This book familiarizes the R&D and academic communities with the capabilities and limitations of MVED and highlights the exciting scientific breakthroughs of the past decade that are dramatically increasing the compactness, efficiency, cost-effectiveness, and reliability of this entire class of devices. This comprehensive text explores a wide range of topics: * Traveling-<span class="hlt">wave</span> tubes, which form the backbone of satellite and airborne communications, as well as of military electronic countermeasures systems * Microfabricated MVEDs and advanced electron beam sources * Klystrons, gyro-amplifiers, and crossed-field devices * "Virtual prototyping" of MVEDs via advanced 3-D computational models * High-<span class="hlt">Power</span> Microwave (HPM) sources * Next-generation microwave structures and circuits * How to achieve linear amplification * Advanced materials technologies for MVEDs * A Web site appendix providing a step-by-step walk-through of a typical MVED design process Concluding with an in-depth examination of emerging applications and future possibilities for MVEDs, Modern Microwave and Millimeter-<span class="hlt">Wave</span> <span class="hlt">Power</span> Electronics ensures that systems designers and engineers understand and utilize the significant potential of this mature, yet continually developing technology. SPECIAL NOTE: All of the editors' royalties realized from</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=oceans+AND+tide&pg=2&id=EJ376771','ERIC'); return false;" href="https://eric.ed.gov/?q=oceans+AND+tide&pg=2&id=EJ376771"><span>The Physical <span class="hlt">Ocean</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>NatureScope, 1988</p> <p>1988-01-01</p> <p>Examines the physical properties of the <span class="hlt">ocean</span> (including the composition of seawater; <span class="hlt">waves</span>, currents, and tides) and the topography of the <span class="hlt">ocean</span> floor. Included are (1) activities on <span class="hlt">oceans</span>, saltwater, and the sea floor; and (2) questions, and a puzzle which can be copied. (Author/RT)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1357747-pseudo-spectral-control-novel-oscillating-surge-wave-energy-converter-regular-waves-power-optimization-including-load-reduction','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1357747-pseudo-spectral-control-novel-oscillating-surge-wave-energy-converter-regular-waves-power-optimization-including-load-reduction"><span>Pseudo-spectral control of a novel oscillating surge <span class="hlt">wave</span> energy converter in regular <span class="hlt">waves</span> for <span class="hlt">power</span> optimization including load reduction</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Tom, Nathan M.; Yu, Yi -Hsiang; Wright, Alan D.; ...</p> <p>2017-04-18</p> <p>The aim of this study is to describe a procedure to maximize the <span class="hlt">power</span>-to-load ratio of a novel <span class="hlt">wave</span> energy converter (WEC) that combines an oscillating surge <span class="hlt">wave</span> energy converter with variable structural components. The control of the <span class="hlt">power</span>-take-off torque will be on a <span class="hlt">wave-to-wave</span> timescale, whereas the structure will be controlled statically such that the geometry remains the same throughout the <span class="hlt">wave</span> period. Linear hydrodynamic theory is used to calculate the upper and lower bounds for the time-averaged absorbed <span class="hlt">power</span> and surge foundation loads while assuming that the WEC motion remains sinusoidal. Previous work using pseudo-spectral techniques to solvemore » the optimal control problem focused solely on maximizing absorbed energy. This work extends the optimal control problem to include a measure of the surge foundation force in the optimization. The objective function includes two competing terms that force the optimizer to maximize <span class="hlt">power</span> capture while minimizing structural loads. A penalty weight was included with the surge foundation force that allows control of the optimizer performance based on whether emphasis should be placed on <span class="hlt">power</span> absorption or load shedding. Results from pseudo-spectral optimal control indicate that a unit reduction in time-averaged <span class="hlt">power</span> can be accompanied by a greater reduction in surge-foundation force.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1357747','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1357747"><span>Pseudo-spectral control of a novel oscillating surge <span class="hlt">wave</span> energy converter in regular <span class="hlt">waves</span> for <span class="hlt">power</span> optimization including load reduction</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>Tom, Nathan M.; Yu, Yi -Hsiang; Wright, Alan D.</p> <p></p> <p>The aim of this study is to describe a procedure to maximize the <span class="hlt">power</span>-to-load ratio of a novel <span class="hlt">wave</span> energy converter (WEC) that combines an oscillating surge <span class="hlt">wave</span> energy converter with variable structural components. The control of the <span class="hlt">power</span>-take-off torque will be on a <span class="hlt">wave-to-wave</span> timescale, whereas the structure will be controlled statically such that the geometry remains the same throughout the <span class="hlt">wave</span> period. Linear hydrodynamic theory is used to calculate the upper and lower bounds for the time-averaged absorbed <span class="hlt">power</span> and surge foundation loads while assuming that the WEC motion remains sinusoidal. Previous work using pseudo-spectral techniques to solvemore » the optimal control problem focused solely on maximizing absorbed energy. This work extends the optimal control problem to include a measure of the surge foundation force in the optimization. The objective function includes two competing terms that force the optimizer to maximize <span class="hlt">power</span> capture while minimizing structural loads. A penalty weight was included with the surge foundation force that allows control of the optimizer performance based on whether emphasis should be placed on <span class="hlt">power</span> absorption or load shedding. Results from pseudo-spectral optimal control indicate that a unit reduction in time-averaged <span class="hlt">power</span> can be accompanied by a greater reduction in surge-foundation force.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=faraday&pg=4&id=EJ723767','ERIC'); return false;" href="https://eric.ed.gov/?q=faraday&pg=4&id=EJ723767"><span>Starting to Experiment with <span class="hlt">Wave</span> <span class="hlt">Power</span></span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Hare, Jonathan; McCallie, Ellen</p> <p>2005-01-01</p> <p>Outlined is a simple design for a working <span class="hlt">wave-powered</span> electrical generator based on one made on the BBC "Rough Science" TV series. The design has been kept deliberately simple to facilitate rapid pupil/student involvement and most importantly so that there is much scope for their own ingenuity and ideas. The generator works on the principle of…</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10422E..1HS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10422E..1HS"><span>Damping of surface <span class="hlt">waves</span> due to oil emulsions in application to <span class="hlt">ocean</span> remote sensing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sergievskaya, I.; Ermakov, S.; Lazareva, T.; Lavrova, O.</p> <p>2017-10-01</p> <p>Applications of different radar and optical methods for detection of oil pollutions based on the effect of damping of short wind <span class="hlt">waves</span> by surface films have been extensively studied last decades. The main problem here is poor knowledge of physical characteristics of oil films, in particular, emulsified oil layers (EOL). The latter are ranged up to 70% of all pollutants. Physical characteristics of EOL which are responsible for <span class="hlt">wave</span> damping and respectively for possibilities of their remote sensing depend on conditions of emulsification processes, e.g., mixing due to <span class="hlt">wave</span> breaking, on percentage of water in the oil, etc. and are not well studied by now. In this paper results of laboratory studies of damping of gravity-capillary <span class="hlt">waves</span> due to EOL on water are presented and compared to oil layers (OL). A laboratory method used previously for monomolecular films and OL, and based on measuring the damping coefficient and wavelength of parametrically generated standing <span class="hlt">waves</span> has been applied for determination of EOL characteristics. Investigations of characteristics of crude oil, oil emulsions and crude OL and EOL have been carried out in a wide range of surface <span class="hlt">wave</span> frequencies (from 10 to 25 Hz) and OL and EOL film thickness (from hundredths of millimeter to a few millimeters. The selected frequency range corresponds to Bragg <span class="hlt">waves</span> for microwave, X- to Ka-band radars typically used for <span class="hlt">ocean</span> remote sensing. An effect of enhanced <span class="hlt">wave</span> damping due to EOL compared to non emulsified crude OL is revealed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017SPIE10466E..4VS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017SPIE10466E..4VS"><span>Cloud manifestations of atmospheric gravity <span class="hlt">waves</span> over the water area of the Kuril Islands during the propagation of <span class="hlt">powerful</span> transoceanic tsunamis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Skorokhodov, A. V.; Shevchenko, G. V.; Astafurov, V. G.</p> <p>2017-11-01</p> <p>The investigation results of atmospheric gravity <span class="hlt">waves</span> cloudy manifestations observed over the water area of the Kuril Island ridge during the propagation of <span class="hlt">powerful</span> transoceanic tsunami 2009-2010 are shown. The description of tsunami characteristics is based on the use of information from autonomous deep-water stations of the Institute of Marine Geology and Geophysics FEB RAS in the Southern Kuril Islands and the Tsunami Warning Service telemetering recorder located in one of the ports on Paramushir Island. The environment condition information was extracted from the results of remote sensing of the Earth from space by the MODIS sensor and aerological measurements at the meteorological station of Severo-Kurilsk. The results of analyzing the characteristics of <span class="hlt">wave</span> processes in the atmosphere and the <span class="hlt">ocean</span> are discussed and their comparison is carried out.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMED41A3455L','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMED41A3455L"><span>Feasibility of <span class="hlt">Wave</span> Energy in Hong Kong</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Lu, M.; Hodgson, P.</p> <p>2014-12-01</p> <p>Kinetic energy produced by the movement of <span class="hlt">ocean</span> <span class="hlt">waves</span> can be harnessed by <span class="hlt">wave</span> energy converter equipment such as <span class="hlt">wave</span> turbines to <span class="hlt">power</span> onshore electricity generators, creating a valuable source of renewable energy. This experiment measures the potential of <span class="hlt">wave</span> energy in Hoi Ha Wan Marine Park, Hong Kong using a data buoy programmed to send data through wireless internet every five minutes. <span class="hlt">Wave</span> <span class="hlt">power</span> (known as '<span class="hlt">wave</span> energy flux') is proportional to <span class="hlt">wave</span> energy periodicity and to the square of <span class="hlt">wave</span> height, and can be calculated using the equation: P = 0.5 kW/(m3)(s) x Hs2 x Tp P = <span class="hlt">wave</span> energy flux (<span class="hlt">wave</span> energy per unit of <span class="hlt">wave</span> crest length in kW/m) Hs = significant <span class="hlt">wave</span> height (m) Tp = <span class="hlt">wave</span> period (seconds) Acoustic Doppler Current Profilers (ADCPs), or ultrasonic sensors, were installed on the seabed at three monitoring locations to measure Significant <span class="hlt">Wave</span> Heights (Hs), Significant <span class="hlt">Wave</span> Periods (Tp) and Significant <span class="hlt">Wave</span> Direction (Wd). Over a twelve month monitoring period, Significant <span class="hlt">Wave</span> Heights ranged from 0 ~ 8.63m. Yearly averages were 1.051m. Significant <span class="hlt">Wave</span> Period ranged from 0 ~ 14.9s. Yearly averages were 6.846s. The maximum <span class="hlt">wave</span> energy amount recorded was 487.824 kW/m. These results implied that electricity sufficient to <span class="hlt">power</span> a small marine research center could be supplied by a generator running at 30% efficiency or greater. A <span class="hlt">wave</span> piston driven generator prototype was designed that could meet output objectives without using complex hydraulics, expensive mechanical linkages, or heavy floating buoys that might have an adverse impact on marine life. The result was a design comprising a water piston connected by an air pipe to a rotary turbine <span class="hlt">powered</span> generator. A specially designed air valve allowed oscillating bidirectional airflow generated in the piston to be converted into unidirectional flow through the turbine, minimizing kinetic energy loss. A 35cm <span class="hlt">wave</span> with a one second period could generate 139.430W of electricity, with an efficiency of 37.6%.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018SPIE10553E..0PS','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018SPIE10553E..0PS"><span>Continuous <span class="hlt">wave</span> <span class="hlt">power</span> scaling in high <span class="hlt">power</span> broad area quantum cascade lasers</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Suttinger, M.; Leshin, J.; Go, R.; Figueiredo, P.; Shu, H.; Lyakh, A.</p> <p>2018-02-01</p> <p>Experimental and model results for high <span class="hlt">power</span> broad area quantum cascade lasers are presented. Continuous <span class="hlt">wave</span> <span class="hlt">power</span> scaling from 1.62 W to 2.34 W has been experimentally demonstrated for 3.15 mm-long, high reflection-coated 5.6 μm quantum cascade lasers with 15 stage active region for active region width increased from 10 μm to 20 μm. A semi-empirical model for broad area devices operating in continuous <span class="hlt">wave</span> mode is presented. The model uses measured pulsed transparency current, injection efficiency, waveguide losses, and differential gain as input parameters. It also takes into account active region self-heating and sub-linearity of pulsed <span class="hlt">power</span> vs current laser characteristic. The model predicts that an 11% improvement in maximum CW <span class="hlt">power</span> and increased wall plug efficiency can be achieved from 3.15 mm x 25 μm devices with 21 stages of the same design but half doping in the active region. For a 16-stage design with a reduced stage thickness of 300Å, pulsed roll-over current density of 6 kA/cm2 , and InGaAs waveguide layers; optical <span class="hlt">power</span> increase of 41% is projected. Finally, the model projects that <span class="hlt">power</span> level can be increased to 4.5 W from 3.15 mm × 31 μm devices with the baseline configuration with T0 increased from 140 K for the present design to 250 K.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015Natur.521...65A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015Natur.521...65A"><span>The formation and fate of internal <span class="hlt">waves</span> in the South China Sea</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.; Peacock, Thomas; MacKinnon, Jennifer A.; Nash, Jonathan D.; Buijsman, Maarten C.; Centuroni, Luca R.; Chao, Shenn-Yu; Chang, Ming-Huei; Farmer, David M.; Fringer, Oliver B.; Fu, Ke-Hsien; Gallacher, Patrick C.; Graber, Hans C.; Helfrich, Karl R.; Jachec, Steven M.; Jackson, Christopher R.; Klymak, Jody M.; Ko, Dong S.; Jan, Sen; Johnston, T. M. Shaun; Legg, Sonya; Lee, I.-Huan; Lien, Ren-Chieh; Mercier, Matthieu J.; Moum, James N.; Musgrave, Ruth; Park, Jae-Hun; Pickering, Andrew I.; Pinkel, Robert; Rainville, Luc; Ramp, Steven R.; Rudnick, Daniel L.; Sarkar, Sutanu; Scotti, Alberto; Simmons, Harper L.; St Laurent, Louis C.; Venayagamoorthy, Subhas K.; Wang, Yu-Huai; Wang, Joe; Yang, Yiing J.; Paluszkiewicz, Theresa; (David) Tang, Tswen-Yung</p> <p>2015-05-01</p> <p>Internal gravity <span class="hlt">waves</span>, the subsurface analogue of the familiar surface gravity <span class="hlt">waves</span> that break on beaches, are ubiquitous in the <span class="hlt">ocean</span>. Because of their strong vertical and horizontal currents, and the turbulent mixing caused by their breaking, they affect a panoply of <span class="hlt">ocean</span> processes, such as the supply of nutrients for photosynthesis, sediment and pollutant transport and acoustic transmission; they also pose hazards for man-made structures in the <span class="hlt">ocean</span>. Generated primarily by the wind and the tides, internal <span class="hlt">waves</span> can travel thousands of kilometres from their sources before breaking, making it challenging to observe them and to include them in numerical climate models, which are sensitive to their effects. For over a decade, studies have targeted the South China Sea, where the <span class="hlt">oceans</span>' most <span class="hlt">powerful</span> known internal <span class="hlt">waves</span> are generated in the Luzon Strait and steepen dramatically as they propagate west. Confusion has persisted regarding their mechanism of generation, variability and energy budget, however, owing to the lack of in situ data from the Luzon Strait, where extreme flow conditions make measurements difficult. Here we use new observations and numerical models to (1) show that the <span class="hlt">waves</span> begin as sinusoidal disturbances rather than arising from sharp hydraulic phenomena, (2) reveal the existence of >200-metre-high breaking internal <span class="hlt">waves</span> in the region of generation that give rise to turbulence levels >10,000 times that in the open <span class="hlt">ocean</span>, (3) determine that the Kuroshio western boundary current noticeably refracts the internal <span class="hlt">wave</span> field emanating from the Luzon Strait, and (4) demonstrate a factor-of-two agreement between modelled and observed energy fluxes, which allows us to produce an observationally supported energy budget of the region. Together, these findings give a cradle-to-grave picture of internal <span class="hlt">waves</span> on a basin scale, which will support further improvements of their representation in numerical climate predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/25951285','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/25951285"><span>The formation and fate of internal <span class="hlt">waves</span> in the South China Sea.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Alford, Matthew H; Peacock, Thomas; MacKinnon, Jennifer A; Nash, Jonathan D; Buijsman, Maarten C; Centurioni, Luca R; Centuroni, Luca R; Chao, Shenn-Yu; Chang, Ming-Huei; Farmer, David M; Fringer, Oliver B; Fu, Ke-Hsien; Gallacher, Patrick C; Graber, Hans C; Helfrich, Karl R; Jachec, Steven M; Jackson, Christopher R; Klymak, Jody M; Ko, Dong S; Jan, Sen; Johnston, T M Shaun; Legg, Sonya; Lee, I-Huan; Lien, Ren-Chieh; Mercier, Matthieu J; Moum, James N; Musgrave, Ruth; Park, Jae-Hun; Pickering, Andrew I; Pinkel, Robert; Rainville, Luc; Ramp, Steven R; Rudnick, Daniel L; Sarkar, Sutanu; Scotti, Alberto; Simmons, Harper L; St Laurent, Louis C; Venayagamoorthy, Subhas K; Wang, Yu-Huai; Wang, Joe; Yang, Yiing J; Paluszkiewicz, Theresa; Tang, Tswen-Yung David</p> <p>2015-05-07</p> <p>Internal gravity <span class="hlt">waves</span>, the subsurface analogue of the familiar surface gravity <span class="hlt">waves</span> that break on beaches, are ubiquitous in the <span class="hlt">ocean</span>. Because of their strong vertical and horizontal currents, and the turbulent mixing caused by their breaking, they affect a panoply of <span class="hlt">ocean</span> processes, such as the supply of nutrients for photosynthesis, sediment and pollutant transport and acoustic transmission; they also pose hazards for man-made structures in the <span class="hlt">ocean</span>. Generated primarily by the wind and the tides, internal <span class="hlt">waves</span> can travel thousands of kilometres from their sources before breaking, making it challenging to observe them and to include them in numerical climate models, which are sensitive to their effects. For over a decade, studies have targeted the South China Sea, where the <span class="hlt">oceans</span>' most <span class="hlt">powerful</span> known internal <span class="hlt">waves</span> are generated in the Luzon Strait and steepen dramatically as they propagate west. Confusion has persisted regarding their mechanism of generation, variability and energy budget, however, owing to the lack of in situ data from the Luzon Strait, where extreme flow conditions make measurements difficult. Here we use new observations and numerical models to (1) show that the <span class="hlt">waves</span> begin as sinusoidal disturbances rather than arising from sharp hydraulic phenomena, (2) reveal the existence of >200-metre-high breaking internal <span class="hlt">waves</span> in the region of generation that give rise to turbulence levels >10,000 times that in the open <span class="hlt">ocean</span>, (3) determine that the Kuroshio western boundary current noticeably refracts the internal <span class="hlt">wave</span> field emanating from the Luzon Strait, and (4) demonstrate a factor-of-two agreement between modelled and observed energy fluxes, which allows us to produce an observationally supported energy budget of the region. Together, these findings give a cradle-to-grave picture of internal <span class="hlt">waves</span> on a basin scale, which will support further improvements of their representation in numerical climate predictions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1828b0025W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1828b0025W"><span>Feasibility study of tuned liquid column damper for <span class="hlt">ocean</span> <span class="hlt">wave</span> energy extraction</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wong, Yihong; King, Yeong-Jin; Lai, An-Chow; Chong, Kok-Keong; Lim, Boon-Han</p> <p>2017-04-01</p> <p>Intermittent nature and low efficiency are the major issues in renewable energy supply. To overcome these issues, one of the possible methods is through a hybrid system where multiple sources of renewable energy are combined to compensate each other's weaknesses. The hybrid of solar energy and <span class="hlt">wave</span> energy becomes possible through the introduction of a stable floating platform which enables solar energy generation above it and <span class="hlt">wave</span> energy harvesting underneath it. This paper is intended to study the feasibility of harnessing <span class="hlt">ocean</span> <span class="hlt">wave</span> energy using a tuned liquid column damper (TLCD), a type of passive damping device that is designed to suppress externally induced vibration force at a specific frequency range. The proposed TLCD is to be implemented within a floating offshore structure to serve as a vibration mitigating mechanism by reducing the dynamic response of the structure and simultaneously utilize the flowing motion of liquid within the TLCD for generating electricity. The constructed TLCD prototype is tuned according to theoretical study and tested using a shaking table with a predetermined frequency range. The oscillating motion of water within the TLCD and the potential of installation of hydro turbine generator in term of recoverable amount of energy are studied.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-PIA01915.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-PIA01915.html"><span>Internal <span class="hlt">Ocean</span> <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2006-07-17</p> <p>The false-color VNIR image from NASA Terra spacecraft was acquired off the island of Tsushima in the Korea Strait shows the signatures of several internal <span class="hlt">wave</span> packets, indicating a northern propagation direction.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=PIA01915&hterms=wetlands+built&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dwetlands%2Bbuilt','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=PIA01915&hterms=wetlands+built&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dwetlands%2Bbuilt"><span>Internal <span class="hlt">Ocean</span> <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></p> <p>2006-01-01</p> <p><p/> Internal <span class="hlt">waves</span> are <span class="hlt">waves</span> that travel within the interior of a fluid. The <span class="hlt">waves</span> propagate at the interface or boundary between two layers with sharp density differences, such as temperature. They occur wherever strong tides or currents and stratification occur in the neighborhood of irregular topography. They can propagate for several hundred kilometers. The ASTER false-color VNIR image off the island of Tsushima in the Korea Strait shows the signatures of several internal <span class="hlt">wave</span> packets, indicating a northern propagation direction. <p/> With its 14 spectral bands from the visible to the thermal infrared wavelength region, and its high spatial resolution of 15 to 90 meters (about 50 to 300 feet), ASTER images Earth to map and monitor the changing surface of our planet. <p/> ASTER is one of five Earth-observing instruments launched December 18, 1999, on NASA's Terra satellite. The instrument was built by Japan's Ministry of Economy, Trade and Industry. A joint U.S./Japan science team is responsible for validation and calibration of the instrument and the data products. <p/> The broad spectral coverage and high spectral resolution of ASTER provides scientists in numerous disciplines with critical information for surface mapping, and monitoring of dynamic conditions and temporal change. Example applications are: monitoring glacial advances and retreats; monitoring potentially active volcanoes; identifying crop stress; determining cloud morphology and physical properties; wetlands evaluation; thermal pollution monitoring; coral reef degradation; surface temperature mapping of soils and geology; and measuring surface heat balance. <p/> The U.S. science team is located at NASA's Jet Propulsion Laboratory, Pasadena, Calif. The Terra mission is part of NASA's Science Mission Directorate. <p/> Size: 60 by 120 kilometers (37.2 by 74.4 miles) Location: 34.6 degrees North latitude, 129.5 degrees East longitude Orientation: North at top Image Data: ASTER bands 3, 2, and 1</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AIPA....6h5313W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AIPA....6h5313W"><span>Performance of arrays of direct-driven <span class="hlt">wave</span> energy converters under optimal <span class="hlt">power</span> take-off damping</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Liguo; Engström, Jens; Leijon, Mats; Isberg, Jan</p> <p>2016-08-01</p> <p>It is well known that the total <span class="hlt">power</span> converted by a <span class="hlt">wave</span> energy farm is influenced by the hydrodynamic interactions between <span class="hlt">wave</span> energy converters, especially when they are close to each other. Therefore, to improve the performance of a <span class="hlt">wave</span> energy farm, the hydrodynamic interaction between converters must be considered, which can be influenced by the <span class="hlt">power</span> take-off damping of individual converters. In this paper, the performance of arrays of <span class="hlt">wave</span> energy converters under optimal hydrodynamic interaction and <span class="hlt">power</span> take-off damping is investigated. This is achieved by coordinating the <span class="hlt">power</span> take-off damping of individual converters, resulting in optimal hydrodynamic interaction as well as higher production of time-averaged <span class="hlt">power</span> converted by the farm. Physical constraints on motion amplitudes are considered in the solution, which is required for the practical implementation of <span class="hlt">wave</span> energy converters. Results indicate that the natural frequency of a <span class="hlt">wave</span> energy converter under optimal damping will not vary with sea states, but the production performance of a <span class="hlt">wave</span> energy farm can be improved significantly while satisfying the motion constraints.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20030093729','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20030093729"><span>Simultaneous <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Measurements by the Jason and Topex Satellites, With Buoy and Model Comparisons</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Ray, Richard D.; Beckley, B. D.</p> <p>2003-01-01</p> <p>The verification phase of the Jason-1 satellite altimeter mission presents a unique opportunity for comparing near-simultaneous, independent satellite measurements. We here examine simultaneous significant <span class="hlt">wave</span> height measurements by the Jason-1 and Topex/Poseidon altimeters. These data are also compared with in-situ measurements from deep-<span class="hlt">ocean</span> buoys and with predicted <span class="hlt">wave</span> heights from the <span class="hlt">Wave</span> Watch 111 operational model. The rms difference between Jason and Topex <span class="hlt">wave</span> heights is 21 cm, and this can be further lowered by application of median filters to reduce high-frequency noise. This noise is slightly larger in the Jason dataset, amounting to about 7 cm rms for frequencies above 0.05 Hz, which is the frequency at which the coherence between Topex and Jason measurements drops to zero. The probability density function for Jason shows a dearth of small <span class="hlt">waves</span> relative to Topex. Buoy comparisons confirm that this problem lies with the Jason measurements. The buoy comparisons confirm previous reports that Topex <span class="hlt">wave</span> heights are roughly 5% smaller than buoy measurements for <span class="hlt">waves</span> between 2 and 5m; Jason heights in general are 2.7% smaller than Topex. Spurious dips in the Topex density function for 3- and 6-meter <span class="hlt">waves</span>, a problem that has existed since the beginning of the mission, can be solved by waveform retracking..</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1097434','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1097434"><span>Advanced, High <span class="hlt">Power</span>, Next Scale, <span class="hlt">Wave</span> Energy Conversion 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>Mekhiche, Mike; Dufera, Hiz; Montagna, Deb</p> <p>2012-10-29</p> <p>The project conducted under DOE contract DE‐EE0002649 is defined as the Advanced, High <span class="hlt">Power</span>, Next Scale, <span class="hlt">Wave</span> Energy Converter. The overall project is split into a seven‐stage, gated development program. The work conducted under the DOE contract is OPT Stage Gate III work and a portion of Stage Gate IV work of the seven stage product development process. The project effort includes Full Concept Design & Prototype Assembly Testing building on our existing <span class="hlt">Power</span>Buoy technology to deliver a device with much increased <span class="hlt">power</span> delivery. Scaling‐up from 150kW to 500kW <span class="hlt">power</span> generating capacity required changes in the <span class="hlt">Power</span>Buoy design that addressedmore » cost reduction and mass manufacturing by implementing a Design for Manufacturing (DFM) approach. The design changes also focused on reducing <span class="hlt">Power</span>Buoy Installation, Operation and Maintenance (IO&M) costs which are essential to reducing the overall cost of energy. In this design, changes to the core <span class="hlt">Power</span>Buoy technology were implemented to increase capability and reduce both CAPEX and OPEX costs. OPT conceptually envisaged moving from a floating structure to a seabed structure. The design change from a floating structure to seabed structure would provide the implementation of stroke‐ unlimited <span class="hlt">Power</span> Take‐Off (PTO) which has a potential to provide significant <span class="hlt">power</span> delivery improvement and transform the <span class="hlt">wave</span> energy industry if proven feasible.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009ApSS..255.5721W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009ApSS..255.5721W"><span>Effects of half-<span class="hlt">wave</span> and full-<span class="hlt">wave</span> <span class="hlt">power</span> source on the anodic oxidation process on AZ91D magnesium alloy</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Ximei; Zhu, Liqun; Li, Weiping; Liu, Huicong; Li, Yihong</p> <p>2009-03-01</p> <p>Anodic films have been prepared on the AZ91D magnesium alloys in 1 mol/L Na 2SiO 3 with 10 vol.% silica sol addition under the constant voltage of 60 V at room temperature by half-<span class="hlt">wave</span> and full-<span class="hlt">wave</span> <span class="hlt">power</span> sources. The weight of the anodic films has been scaled by analytical balance, and the thickness has been measured by eddy current instrument. The surface morphologies, chemical composition and structure of the anodic films have been characterized by scanning electron microscopy (SEM), energy dispersion spectrometry (EDS), X-ray diffraction (XRD) and transmission electron microscopy (TEM). The results show that the thickness and weight of the anodic films formed by the two <span class="hlt">power</span> sources both increase with the anodizing time, and the films anodized by full-<span class="hlt">wave</span> <span class="hlt">power</span> source grow faster than that by half-<span class="hlt">wave</span> one. Furthermore, we have fitted polynomial to the scattered data of the weight and thickness in a least-squares sense with MATLAB, which could express the growth process of the anodic films sufficiently. The full-<span class="hlt">wave</span> <span class="hlt">power</span> source is inclined to accelerate the growth of the anodic films, and the half-<span class="hlt">wave</span> one is mainly contributed to the uniformity and fineness of the films. The anodic film consists of crystalline Mg 2SiO 4 and amorphous SiO 2.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015EGUGA..17.1337K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015EGUGA..17.1337K"><span>Acoustic-gravity <span class="hlt">waves</span>, theory and application</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kadri, Usama; Farrell, William E.; Munk, Walter</p> <p>2015-04-01</p> <p>Acoustic-gravity <span class="hlt">waves</span> (AGW) propagate in the <span class="hlt">ocean</span> under the influence of both the compressibility of sea water and the restoring force of gravity. The gravity dependence vanishes if the <span class="hlt">wave</span> vector is normal to the <span class="hlt">ocean</span> surface, but becomes increasingly important as the <span class="hlt">wave</span> vector acquires a horizontal tilt. They are excited by many sources, including non-linear surface <span class="hlt">wave</span> interactions, disturbances of the <span class="hlt">ocean</span> bottom (submarine earthquakes and landslides) and underwater explosions. In this introductory lecture on acoustic-gravity <span class="hlt">waves</span>, we describe their properties, and their relation to organ pipe modes, to microseisms, and to deep <span class="hlt">ocean</span> signatures by short surface <span class="hlt">waves</span>. We discuss the generation of AGW by underwater earthquakes; knowledge of their behaviour with water depth can be applied for the early detection of tsunamis. We also discuss their generation by the non-linear interaction of surface gravity <span class="hlt">waves</span>, which explains the major role they play in transforming energy from the <span class="hlt">ocean</span> surface to the crust, as part of the microseisms phenomenon. Finally, they contribute to horizontal water transport at depth, which might affect benthic life.</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/2012OcMod..47...65K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012OcMod..47...65K"><span>Implementation of the vortex force formalism in the coupled <span class="hlt">ocean-atmosphere-wave</span>-sediment transport (COAWST) modeling system for inner shelf and surf zone applications</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kumar, Nirnimesh; Voulgaris, George; Warner, John C.; Olabarrieta, Maitane</p> <p></p> <p>The coupled <span class="hlt">ocean-atmosphere-wave</span>-sediment transport modeling system (COAWST) enables simulations that integrate <span class="hlt">oceanic</span>, atmospheric, <span class="hlt">wave</span> and morphological processes in the coastal <span class="hlt">ocean</span>. Within the modeling system, the three-dimensional <span class="hlt">ocean</span> circulation module (ROMS) is coupled with the <span class="hlt">wave</span> generation and propagation model (SWAN) to allow full integration of the effect of <span class="hlt">waves</span> on circulation and vice versa. The existing <span class="hlt">wave</span>-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 <span class="hlt">waves</span> on a synthetic planar beach and a natural barred beach (DUCK' 94); normal incident <span class="hlt">waves</span> on a nearshore barred morphology with rip channels; and <span class="hlt">wave</span>-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 <span class="hlt">wave</span> roller generation and <span class="hlt">wave</span>-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 <span class="hlt">wave</span> rollers and breaking induced turbulent mixing can be formulated using non-dimensional parameters which are functions of local <span class="hlt">wave</span> 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</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1987STIN...8820722.','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1987STIN...8820722."><span>Federal <span class="hlt">Ocean</span> Energy Technology</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p></p> <p>1987-10-01</p> <p>The Department of Energy's (DOE) <span class="hlt">Ocean</span> Energy Technology (OET) Program is looking for cost-effective ways to harness <span class="hlt">ocean</span> energy to help <span class="hlt">power</span> tomorrow's world. Federally sponsored researchers are studying methods to transform the solar heat stored in the <span class="hlt">ocean</span>'s surface waters into electricity as well as new ways to convert <span class="hlt">wave</span> energy into mechanical energy or electricity. This report provides a summary of research completed during FY86. Four major research areas are addressed in the work covered by this report: Thermodynamic Research and Analysis addresses the process and system analyses which provide the underlying understanding of physical effects which constitute the energy conversion processes, Experimental Verification and Testing provides confirmation of the analytical projections and empirical relationships, Materials and Structural Research addresses special materials compatibility issues related to operation in the sea. Much of its focus is on concepts for the system CWP which is a major technology cost driver, and Oceanographic, Environmental, and Geotechnical Research addresss those unique design requirements imposed by construction in steep slope coastal areas.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1393399-edge-loss-high-harmonic-fast-wave-heating-power-nstx-cylindrical-model','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1393399-edge-loss-high-harmonic-fast-wave-heating-power-nstx-cylindrical-model"><span>Edge loss of high-harmonic fast-<span class="hlt">wave</span> heating <span class="hlt">power</span> in NSTX: a cylindrical model</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Perkins, R. J.; Hosea, J. C.; Bertelli, N.; ...</p> <p>2017-09-04</p> <p>Efficient high-harmonic fast-<span class="hlt">wave</span> (HHFW) heating in the National Spherical Torus Experiment Upgrade (NSTX-U) would facilitate experiments in turbulence, transport, fast-ion studies, and more. However, previous HHFW operation in NSTX exhibited a large loss of fast-<span class="hlt">wave</span> <span class="hlt">power</span> to the divertor along the scrape-off layer field lines for edge densities above the fast-<span class="hlt">wave</span> cutoff. It was postulated that the <span class="hlt">wave</span> amplitude is enhanced in the scrapeoff layer due to cavity-like modes, and that these enhanced fields drive sheath losses through RF rectification. As part of ongoing work to confirm this hypothesis, we have developed a cylindrical cold-plasma model to identify and understandmore » scenarios where a substantial fraction of <span class="hlt">wave</span> <span class="hlt">power</span> is confined to the plasma periphery. We previously identified a peculiar class of modes, named annulus resonances, that conduct approximately half of their <span class="hlt">wave</span> <span class="hlt">power</span> in the periphery and can also account for a significant fraction of the total <span class="hlt">wave</span> <span class="hlt">power</span>. Here, we study the influence of annulus resonances on <span class="hlt">wave</span> field reconstructions and find instances where annulus-resonant modes dominate the spectrum and trap over half of the total <span class="hlt">wave</span> <span class="hlt">power</span> at the edge. The work is part of an ongoing effort to determine the mechanism underlying these scrape-off layer losses in NSTX, identify optimal conditions for operation in NSTX-U, and predict whether similar losses occur for the ion-cyclotron minority heating scheme for both current experiments and future devices such as ITER.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1393399-edge-loss-high-harmonic-fast-wave-heating-power-nstx-cylindrical-model','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1393399-edge-loss-high-harmonic-fast-wave-heating-power-nstx-cylindrical-model"><span>Edge loss of high-harmonic fast-<span class="hlt">wave</span> heating <span class="hlt">power</span> in NSTX: a cylindrical model</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>Perkins, R. J.; Hosea, J. C.; Bertelli, N.</p> <p></p> <p>Efficient high-harmonic fast-<span class="hlt">wave</span> (HHFW) heating in the National Spherical Torus Experiment Upgrade (NSTX-U) would facilitate experiments in turbulence, transport, fast-ion studies, and more. However, previous HHFW operation in NSTX exhibited a large loss of fast-<span class="hlt">wave</span> <span class="hlt">power</span> to the divertor along the scrape-off layer field lines for edge densities above the fast-<span class="hlt">wave</span> cutoff. It was postulated that the <span class="hlt">wave</span> amplitude is enhanced in the scrapeoff layer due to cavity-like modes, and that these enhanced fields drive sheath losses through RF rectification. As part of ongoing work to confirm this hypothesis, we have developed a cylindrical cold-plasma model to identify and understandmore » scenarios where a substantial fraction of <span class="hlt">wave</span> <span class="hlt">power</span> is confined to the plasma periphery. We previously identified a peculiar class of modes, named annulus resonances, that conduct approximately half of their <span class="hlt">wave</span> <span class="hlt">power</span> in the periphery and can also account for a significant fraction of the total <span class="hlt">wave</span> <span class="hlt">power</span>. Here, we study the influence of annulus resonances on <span class="hlt">wave</span> field reconstructions and find instances where annulus-resonant modes dominate the spectrum and trap over half of the total <span class="hlt">wave</span> <span class="hlt">power</span> at the edge. The work is part of an ongoing effort to determine the mechanism underlying these scrape-off layer losses in NSTX, identify optimal conditions for operation in NSTX-U, and predict whether similar losses occur for the ion-cyclotron minority heating scheme for both current experiments and future devices such as ITER.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSPO14C2805A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSPO14C2805A"><span>The internal gravity <span class="hlt">wave</span> spectrum in two high-resolution global <span class="hlt">ocean</span> models</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Arbic, B. K.; Ansong, J. K.; Buijsman, M. C.; Kunze, E. L.; Menemenlis, D.; Müller, M.; Richman, J. G.; Savage, A.; Shriver, J. F.; Wallcraft, A. J.; Zamudio, L.</p> <p>2016-02-01</p> <p>We examine the internal gravity <span class="hlt">wave</span> (IGW) spectrum in two sets of high-resolution global <span class="hlt">ocean</span> simulations that are forced concurrently by atmospheric fields and the astronomical tidal potential. We analyze global 1/12th and 1/25th degree HYCOM simulations, and global 1/12th, 1/24th, and 1/48th degree simulations of the MITgcm. We are motivated by the central role that IGWs play in <span class="hlt">ocean</span> mixing, by operational considerations of the US Navy, which runs HYCOM as an <span class="hlt">ocean</span> forecast model, and by the impact of the IGW continuum on the sea surface height (SSH) measurements that will be taken by the planned NASA/CNES SWOT wide-swath altimeter mission. We (1) compute the IGW horizontal wavenumber-frequency spectrum of kinetic energy, and interpret the results with linear dispersion relations computed from the IGW Sturm-Liouville problem, (2) compute and similarly interpret nonlinear spectral kinetic energy transfers in the IGW band, (3) compute and similarly interpret IGW contributions to SSH variance, (4) perform comparisons of modeled IGW kinetic energy frequency spectra with moored current meter observations, and (5) perform comparisons of modeled IGW kinetic energy vertical wavenumber-frequency spectra with moored observations. This presentation builds upon our work in Muller et al. (2015, GRL), who performed tasks (1), (2), and (4) in 1/12th and 1/25th degree HYCOM simulations, for one region of the North Pacific. New for this presentation are tasks (3) and (5), the inclusion of MITgcm solutions, and the analysis of additional <span class="hlt">ocean</span> regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017MsT.........13C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017MsT.........13C"><span>Inertial Sea <span class="hlt">Wave</span> Energy Converter from Mediterranean Sea to <span class="hlt">Ocean</span> - Design Optimization</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Calleri, Marco</p> <p></p> <p>Optimization of the number of gyroscopes and flywheel rotational speed of a <span class="hlt">Wave</span> Energy Converter able to produce 725 kW as the nominal <span class="hlt">power</span>, in the chosen installation site, respecting some imposed constraints and some dimensions from the previous design, by minimizing the cost of the device and the bearing <span class="hlt">power</span> losses, through the minimization of the LCOE of the device.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19810061709&hterms=refraction&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Drefraction','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19810061709&hterms=refraction&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3Drefraction"><span>Refraction of coastal <span class="hlt">ocean</span> <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>Shuchman, R. A.; Kasischke, E. S.</p> <p>1981-01-01</p> <p>Refraction of gravity <span class="hlt">waves</span> in the coastal area off Cape Hatteras, NC as documented by synthetic aperture radar (SAR) imagery from Seasat orbit 974 (collected on September 3, 1978) is discussed. An analysis of optical Fourier transforms (OFTs) from more than 70 geographical positions yields estimates of wavelength and <span class="hlt">wave</span> direction for each position. In addition, independent estimates of the same two quantities are calculated using two simple theoretical <span class="hlt">wave</span>-refraction models. The OFT results are then compared with the theoretical results. A statistical analysis shows a significant degree of linear correlation between the data sets. This is considered to indicate that the Seasat SAR produces imagery whose clarity is sufficient to show the refraction of gravity <span class="hlt">waves</span> in shallow water.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2004JFM...507..143S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2004JFM...507..143S"><span>The <span class="hlt">oceanic</span> boundary layer driven by <span class="hlt">wave</span> breaking with stochastic variability. Part 1. Direct numerical simulations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Sullivan, Peter P.; McWilliams, James C.; Melville, W. Kendall</p> <p>2004-05-01</p> <p>We devise a stochastic model for the effects of breaking <span class="hlt">waves</span> and fit its distribution functions to laboratory and field data. This is used to represent the space time structure of momentum and energy forcing of the <span class="hlt">oceanic</span> boundary layer in turbulence-resolving simulations. The aptness of this breaker model is evaluated in a direct numerical simulation (DNS) of an otherwise quiescent fluid driven by an isolated breaking <span class="hlt">wave</span>, and the results are in good agreement with laboratory measurements. The breaker model faithfully reproduces the bulk features of a breaking event: the mean kinetic energy decays at a rate approaching t(-1) , and a long-lived vortex (eddy) is generated close to the water surface. The long lifetime of this vortex (more than 50 <span class="hlt">wave</span> periods) makes it effective in energizing the surface region of <span class="hlt">oceanic</span> boundary layers. Next, a comparison of several different DNS of idealized <span class="hlt">oceanic</span> boundary layers driven by different surface forcing (i.e. constant current (as in Couette flow), constant stress, or a mixture of constant stress plus stochastic breakers) elucidates the importance of intermittent stress transmission to the underlying currents. A small amount of active breaking, about 1.6% of the total water surface area at any instant in time, significantly alters the instantaneous flow patterns as well as the ensemble statistics. Near the water surface a vigorous downwelling upwelling pattern develops at the head and tail of each three-dimensional breaker. This enhances the vertical velocity variance and generates both negative- and positive-signed vertical momentum flux. Analysis of the mean velocity and scalar profiles shows that breaking effectively increases the surface roughness z_o by more than a factor of 30; for our simulations z_o/lambda {≈} 0.04 to 0.06, where lambda is the wavelength of the breaking <span class="hlt">wave</span>. Compared to a flow driven by a constant current, the extra mixing from breakers increases the mean eddy viscosity by more than a</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSHI52A..02W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSHI52A..02W"><span>A 20-Year High-Resolution <span class="hlt">Wave</span> Resource Assessment of Japan with <span class="hlt">Wave</span>-Current Interactions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Webb, A.; Waseda, T.; Kiyomatsu, K.</p> <p>2016-02-01</p> <p>Energy harvested from surface <span class="hlt">ocean</span> <span class="hlt">waves</span> 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 <span class="hlt">wave</span> resource assessment (with uncertainty estimates) to assist with <span class="hlt">wave</span> 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 <span class="hlt">wave</span> <span class="hlt">power</span> density calculations. This latter component is particularly important for regions near strong currents such as the Kuroshio. Here, we will analyze the different <span class="hlt">wave</span> <span class="hlt">power</span> density equations, discuss the model setup, and present results from the 20-year assessment (with a focus on the role of <span class="hlt">wave</span>-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"</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/14512611','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/14512611"><span><span class="hlt">Ocean</span> science. Enhanced: internal tides and <span class="hlt">ocean</span> mixing.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Garrett, Chris</p> <p>2003-09-26</p> <p>Recent satellite and in situ observations have shown that at <span class="hlt">ocean</span> ridges and other seafloor topographic features, a substantial amount of energy is transferred from the main <span class="hlt">ocean</span> tides into "internal tides." In his Perspective, Garrett explains how these internal <span class="hlt">waves</span> with tidal periods propagate through the density-stratified deep <span class="hlt">ocean</span> and eventually break down into turbulence. The resulting mixing affects <span class="hlt">ocean</span> stratification and <span class="hlt">ocean</span> circulation. It thus influences climate as well as biological production. The energy for the internal tides is derived from the rotational energy of the Earth-Moon system changes of the length of the day and the distance to the Moon.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70104616','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70104616"><span>The significance of ultra-refracted surface gravity <span class="hlt">waves</span> on sheltered coasts, with application to San Francisco Bay</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Hanes, D.M.; Erikson, L.H.</p> <p>2013-01-01</p> <p><span class="hlt">Ocean</span> surface gravity <span class="hlt">waves</span> propagating over shallow bathymetry undergo spatial modification of propagation direction and energy density, commonly due to refraction and shoaling. If the bathymetric variations are significant the <span class="hlt">waves</span> can undergo changes in their direction of propagation (relative to deepwater) greater than 90° over relatively short spatial scales. We refer to this phenomenon as ultra-refraction. Ultra-refracted swell <span class="hlt">waves</span> can have a <span class="hlt">powerful</span> influence on coastal areas that otherwise appear to be sheltered from <span class="hlt">ocean</span> <span class="hlt">waves</span>. Through a numerical modeling investigation it is shown that San Francisco Bay, one of the earth's largest and most protected natural harbors, is vulnerable to ultra-refracted <span class="hlt">ocean</span> <span class="hlt">waves</span>, particularly southwest incident swell. The flux of <span class="hlt">wave</span> energy into San Francisco Bay results from <span class="hlt">wave</span> transformation due to the bathymetry and orientation of the large ebb tidal delta, and deep, narrow channel through the Golden Gate. For example, ultra-refracted swell <span class="hlt">waves</span> play a critical role in the intermittent closure of the entrance to Crissy Field Marsh, a small restored tidal wetland located on the sheltered north-facing coast approximately 1.5 km east of the Golden Gate Bridge.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMGC41A1066K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMGC41A1066K"><span>Progress Report on the GROWTH (GNSS Reflectometry for <span class="hlt">Ocean</span> <span class="hlt">Waves</span>, Tides, and Height) Research Project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kitazawa, Y.; Ichikawa, K.; Akiyama, H.; Ebinuma, T.; Isoguchi, O.; Kimura, N.; Konda, M.; Kouguchi, N.; Tamura, H.; Tomita, H.; Yoshikawa, Y.; Waseda, T.</p> <p>2016-12-01</p> <p>Global Navigation Satellite Systems (GNSS), such as GPS is a system of satellites that provide autonomous geo-spatial positioning with global coverage. It allows small electronic receivers to determine their location to high precision using radio signals transmitted from satellites, GNSS reflectometry (GNSS-R) involves making measurements from the reflections from the Earth of navigation signals from GNSS satellites. Reflected signals from sea surface are considered that those are useful to observe sea state and sea surface height. We have started a research program for GNSS-R applications on oceanographic observations under the contract with MEXT (Ministry of Education Culture, Sports, Science and Technology, JAPAN) and launched a Japanese research consortium, GROWTH (GNSS Reflectometry for <span class="hlt">Ocean</span> <span class="hlt">Waves</span>, Tides, and Height). It is aiming to evaluate the capabilities of GNSS-R observations for oceanographic phenomena with different time scales, such as <span class="hlt">ocean</span> <span class="hlt">waves</span> (1/10 to tens of seconds), tides (one or half days), and sea surface dynamic height (a few days to years). In situ observations of <span class="hlt">ocean</span> <span class="hlt">wave</span> spectrum, wind speed vertical profile, and sea surface height will be quantitatively compared with equivalent estimates from simultaneous GNSS-R measurements. The GROWTH project will utilize different types of observation platforms; marine observation towers (about 20 m height), multi-copters (about 100 to 150 m height), and much higher-altitude CYGNSS data. Cross-platform data, together with in situ oceanographic observations, will be compared after adequate temporal averaging that accounts differences of the footprint sizes and temporal and spatial scales of oceanographic phenomena. This paper will provide overview of the GROWTH project, preliminary test results, obtained by the multi-sensor platform at observation towers, suggest actual footprint sizes and identification of swell. Preparation status of a ground station which will be supplied to receive CYGNSS data</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.4994B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.4994B"><span>Performance of an autonomously deployable telemetered deep <span class="hlt">ocean</span> seismic observatory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Berger, Jonathan; Laske, Gabe; Orcutt, John; Babcock, Jeffrey</p> <p>2016-04-01</p> <p>We describe a transformative technology that can provide near real-time telemetry of sensor data from the <span class="hlt">ocean</span> bottom without a moored buoy or a cable to shore. The breakthrough technology that makes this system possible is an autonomous surface vehicle called a <span class="hlt">Wave</span> Glider developed by Liquid Robotics, which harvests <span class="hlt">wave</span> and solar energy for motive and electrical <span class="hlt">power</span>. For navigation, the <span class="hlt">wave</span> glider is equipped with a small computer, a GPS receiver, a rudder, solar panels and batteries, AIS ship detection receiver, weather station, and an Iridium satellite modem. <span class="hlt">Wave</span> gliders have demonstrated trans-<span class="hlt">oceanic</span> range and long-term station keeping capabilities. We present results from several deployments of a prototype system that demonstrate the feasibility of this concept. The system comprises <span class="hlt">ocean</span> bottom package (OBP) and an <span class="hlt">ocean</span> surface gateway (OSG). Acoustic communications connect the OBP instruments with OSG while communications between the gateway and land are provided by the Iridium satellite constellation. The most recent deployment of the OBP was off the edge of the Patton Escarpment some 300 km west of San Diego in 4000 m of water. The OSG was launched about 30 km west of San Diego harbor and programmed to navigate to the site of the <span class="hlt">ocean</span> bottom package. Arriving after 161 hours, the OSG then commenced holding station at the site for the next 68 days. Speeds over-the-ground varied with wind, <span class="hlt">wave</span>, and surface current conditions but averaged 0.5 m/s while winds varied between 0 m/s and 17 m/s and <span class="hlt">wave</span> heights between 0.2 m and 5.9 m. Over this period the median total data latency was 260 s and the data loss less that 0.2% when the <span class="hlt">wave</span> glider was within 1.5 km of the central point. We have also tested a full-scale model of a towable <span class="hlt">ocean</span> bottom package, which demonstrated that a <span class="hlt">wave</span> glider could tow and navigate an autonomously deployable <span class="hlt">ocean</span> bottom package. Taken together, these tests have demonstrated that the concept is viable for long</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OcDyn..68..391J','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OcDyn..68..391J"><span>Submesoscale features and their interaction with fronts and internal tides in a high-resolution coupled atmosphere-<span class="hlt">ocean-wave</span> model of the Bay of Bengal</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Jensen, Tommy G.; Shulman, Igor; Wijesekera, Hemantha W.; Anderson, Stephanie; Ladner, Sherwin</p> <p>2018-03-01</p> <p>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-<span class="hlt">ocean-wave</span> model with comprehensive physics is used to model the weather, <span class="hlt">ocean</span> circulation, and <span class="hlt">wave</span> 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 <span class="hlt">waves</span>, while the <span class="hlt">ocean</span> 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 <span class="hlt">oceanic</span> 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 <span class="hlt">oceanic</span> mixed layer and impact the mesoscale flow. In a second case, strong solitary-like <span class="hlt">waves</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22600055-ka-band-radial-relativistic-backward-wave-oscillator-gw-class-output-power','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22600055-ka-band-radial-relativistic-backward-wave-oscillator-gw-class-output-power"><span>A Ka-band radial relativistic backward <span class="hlt">wave</span> oscillator with GW-class output <span class="hlt">power</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>Zhu, Jiaxin; Zhang, Xiaoping, E-mail: zhangxiaoping@nudt.edu.cn; Dang, Fangchao</p> <p></p> <p>A novel radial relativistic backward <span class="hlt">wave</span> oscillator with a reflector is proposed and designed to generate GW-level high <span class="hlt">power</span> microwaves at Ka-band. The segmented radial slow <span class="hlt">wave</span> structure and the reflector are matched to enhance interaction efficiency. We choose the volume <span class="hlt">wave</span> TM{sub 01} mode as the working mode due to the volume <span class="hlt">wave</span> characteristic. The main structural parameters of the novel device are optimized by particle-in-cell simulation. High <span class="hlt">power</span> microwaves with <span class="hlt">power</span> of 2 GW and a frequency of 29.4 GHz are generated with 30% efficiency when the electron beam voltage is 383 kV, the beam current is 17 kA, and themore » guiding magnetic field is only 0.6 T. Simultaneously, the highest electric field in the novel Ka-band device is just about 960 kV/cm in second slow <span class="hlt">wave</span> structure.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JCoPh.355..144C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JCoPh.355..144C"><span>Fluid-structure interaction simulation of floating structures interacting with complex, large-scale <span class="hlt">ocean</span> <span class="hlt">waves</span> and atmospheric turbulence with application to floating offshore wind turbines</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Calderer, Antoni; Guo, Xin; Shen, Lian; Sotiropoulos, Fotis</p> <p>2018-02-01</p> <p>We develop a numerical method for simulating coupled interactions of complex floating structures with large-scale <span class="hlt">ocean</span> <span class="hlt">waves</span> and atmospheric turbulence. We employ an efficient large-scale model to develop offshore wind and <span class="hlt">wave</span> environmental conditions, which are then incorporated into a high resolution two-phase flow solver with fluid-structure interaction (FSI). The large-scale wind-<span class="hlt">wave</span> interaction model is based on a two-fluid dynamically-coupled approach that employs a high-order spectral method for simulating the water motion and a viscous solver with undulatory boundaries for the air motion. The two-phase flow FSI solver is based on the level set method and is capable of simulating the coupled dynamic interaction of arbitrarily complex bodies with airflow and <span class="hlt">waves</span>. The large-scale <span class="hlt">wave</span> field solver is coupled with the near-field FSI solver with a one-way coupling approach by feeding into the latter <span class="hlt">waves</span> via a pressure-forcing method combined with the level set method. We validate the model for both simple <span class="hlt">wave</span> trains and three-dimensional directional <span class="hlt">waves</span> and compare the results with experimental and theoretical solutions. Finally, we demonstrate the capabilities of the new computational framework by carrying out large-eddy simulation of a floating offshore wind turbine interacting with realistic <span class="hlt">ocean</span> wind and <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26425384','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26425384"><span>THE FUNDAMENTAL SOLUTIONS FOR MULTI-TERM MODIFIED <span class="hlt">POWER</span> LAW <span class="hlt">WAVE</span> EQUATIONS IN A FINITE DOMAIN.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Jiang, H; Liu, F; Meerschaert, M M; McGough, R J</p> <p>2013-01-01</p> <p>Fractional partial differential equations with more than one fractional derivative term in time, such as the Szabo <span class="hlt">wave</span> equation, or the <span class="hlt">power</span> law <span class="hlt">wave</span> equation, describe important physical phenomena. However, studies of these multi-term time-space or time fractional <span class="hlt">wave</span> equations are still under development. In this paper, multi-term modified <span class="hlt">power</span> law <span class="hlt">wave</span> equations in a finite domain are considered. The multi-term time fractional derivatives are defined in the Caputo sense, whose orders belong to the intervals (1, 2], [2, 3), [2, 4) or (0, n ) ( n > 2), respectively. Analytical solutions of the multi-term modified <span class="hlt">power</span> law <span class="hlt">wave</span> equations are derived. These new techniques are based on Luchko's Theorem, a spectral representation of the Laplacian operator, a method of separating variables and fractional derivative techniques. Then these general methods are applied to the special cases of the Szabo <span class="hlt">wave</span> equation and the <span class="hlt">power</span> law <span class="hlt">wave</span> equation. These methods and techniques can also be extended to other kinds of the multi-term time-space fractional models including fractional Laplacian.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ChOE...31..510M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ChOE...31..510M"><span><span class="hlt">Power</span> maximization of a point absorber <span class="hlt">wave</span> energy converter using improved model predictive control</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Milani, Farideh; Moghaddam, Reihaneh Kardehi</p> <p>2017-08-01</p> <p>This paper considers controlling and maximizing the absorbed <span class="hlt">power</span> of <span class="hlt">wave</span> energy converters for irregular <span class="hlt">waves</span>. With respect to physical constraints of the system, a model predictive control is applied. Irregular <span class="hlt">waves</span>' behavior is predicted by Kalman filter method. Owing to the great influence of controller parameters on the absorbed <span class="hlt">power</span>, these parameters are optimized by imperialist competitive algorithm. The results illustrate the method's efficiency in maximizing the extracted <span class="hlt">power</span> in the presence of unknown excitation force which should be predicted by Kalman filter.</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>Modeling and simulation of <span class="hlt">ocean</span> <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 modeling and simulation of <span class="hlt">ocean</span> <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 couple a 1D shallow water equations (SWE) model with a 2D incompressible Navier-Stokes equations (NSE) model in order to reduce the computational cost. The coupled model 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 coupled model can reduce computational cost significantly compared to the full NSE model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/27840786','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/27840786"><span>A statistical survey of ultralow-frequency <span class="hlt">wave</span> <span class="hlt">power</span> and polarization in the Hermean magnetosphere.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>James, Matthew K; Bunce, Emma J; Yeoman, Timothy K; Imber, Suzanne M; Korth, Haje</p> <p>2016-09-01</p> <p>We present a statistical survey of ultralow-frequency <span class="hlt">wave</span> activity within the Hermean magnetosphere using the entire MErcury Surface, Space ENvironment, GEochemistry, and Ranging magnetometer data set. This study is focused upon <span class="hlt">wave</span> activity with frequencies <0.5 Hz, typically below local ion gyrofrequencies, in order to determine if field line resonances similar to those observed in the terrestrial magnetosphere may be present. <span class="hlt">Wave</span> activity is mapped to the magnetic equatorial plane of the magnetosphere and to magnetic latitude and local times on Mercury using the KT14 magnetic field model. <span class="hlt">Wave</span> <span class="hlt">power</span> mapped to the planetary surface indicates the average location of the polar cap boundary. Compressional <span class="hlt">wave</span> <span class="hlt">power</span> is dominant throughout most of the magnetosphere, while azimuthal <span class="hlt">wave</span> <span class="hlt">power</span> close to the dayside magnetopause provides evidence that interactions between the magnetosheath and the magnetopause such as the Kelvin-Helmholtz instability may be driving <span class="hlt">wave</span> activity. Further evidence of this is found in the average <span class="hlt">wave</span> polarization: left-handed polarized <span class="hlt">waves</span> dominate the dawnside magnetosphere, while right-handed polarized <span class="hlt">waves</span> dominate the duskside. A possible field line resonance event is also presented, where a time-of-flight calculation is used to provide an estimated local plasma mass density of ∼240 amu cm -3 .</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_17");'>17</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li class="active"><span>19</span></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_19 --> <div id="page_20" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="381"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JIMTW..38..176F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JIMTW..38..176F"><span>Design of a Millimeter-<span class="hlt">Wave</span> Concentrator for Beam Reception in High-<span class="hlt">Power</span> Wireless <span class="hlt">Power</span> Transfer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Fukunari, Masafumi; Wongsuryrat, Nat; Yamaguchi, Toshikazu; Nakamura, Yusuke; Komurasaki, Kimiya; Koizumi, Hiroyuki</p> <p>2017-02-01</p> <p>This study examined the performance of a developed taper-tube concentrator for 94-GHz millimeter-<span class="hlt">wave</span> beam reception during wireless <span class="hlt">power</span> transfer. The received energy is converted into kinetic energy of a working gas in the tube to drive an engine or thruster. The concentrator, which is assumed to have mirror reflection of millimeter <span class="hlt">waves</span> in it, is designed to be shorter than conventional tapered waveguides of millimeter <span class="hlt">waves</span>. A dimensionless design law of a concentrator is proposed based on geometric optics theory. Because the applicability of geometric optics theory is unclear, the ratio of its bore diameter to its wavelength was set as small compared to those in other possible applications. Then, the discrepancy between the designed and measured <span class="hlt">power</span> reception was examined. Results show that the maximum discrepancy was as low as 7 % for the bore-to-wavelength ratio of 20 at the narrow end of the concentrator.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSPO34C3077C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSPO34C3077C"><span>Measurements of a Lee <span class="hlt">Wave</span> in the Southern <span class="hlt">Ocean</span>: Energy and Momentum Fluxes and Mixing</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cusack, J. M.; Naveira Garabato, A.; Smeed, D.; Girton, J. B.</p> <p>2016-02-01</p> <p>Lee <span class="hlt">waves</span>, internal <span class="hlt">waves</span> generated by stratified flow over topographic features are thought to break and generate a significant proportion of the turbulent mixing required to close the abyssal overturning circulation. A lack of observations means that there is large uncertainty in the magnitude of contribution that lee <span class="hlt">waves</span> make to turbulent transformations, as well as their importance in local and global momentum and energy budgets. Two EM-APEX profiling floats deployed in the Drake Passage during the Diapycnal and Isopycnal Mixing Experiment (DIMES) independently measured a large lee <span class="hlt">wave</span> over the Shackleton Fracture Zone. A model for steady EM-APEX motion is presented and used to calculate absolute vertical water velocity in addition to horizontal velocity measurements made by the floats. The <span class="hlt">wave</span> is observed to have velocity fluctuations in all three directions of over 15 cm s-1 and a frequency close to the local buoyancy frequency. Furthermore, the <span class="hlt">wave</span> has a measured peak vertical flux of horizontal momentum of 6 N m-2, a value that is two orders of magnitude larger than the time mean wind forcing on the Southern <span class="hlt">Ocean</span>. Linear internal <span class="hlt">wave</span> theory was used to estimate <span class="hlt">wave</span> energy density and fluxes, while a mixing parameterisation was used to estimate the magnitude of turbulent kinetic energy dissipation, which was found to be elevated above typical background levels by two orders of magnitude. This work provides the first direct measurement of a lee <span class="hlt">wave</span> generated by ACC flow over topography with simultaneous estimates of energy fluxes and mixing.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1397155','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1397155"><span>Balancing the <span class="hlt">Power</span>-to-Load Ratio for a Novel Variable Geometry <span class="hlt">Wave</span> Energy Converter with Nonideal <span class="hlt">Power</span> Take-Off in Regular <span class="hlt">Waves</span>: Preprint</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>Tom, Nathan M; Yu, Yi-Hsiang; Wright, Alan D</p> <p></p> <p>This work attempts to balance <span class="hlt">power</span> absorption against structural loading for a novel variable geometry <span class="hlt">wave</span> energy converter. The variable geometry consists of four identical flaps that will be opened in ascending order starting with the flap closest to the seafloor and moving to the free surface. The influence of a pitch motion constraint on <span class="hlt">power</span> absorption when utilizing a nonideal <span class="hlt">power</span> take-off (PTO) is examined and found to reduce the losses associated with bidirectional energy flow. The <span class="hlt">power</span>-to-load ratio is evaluated using pseudo-spectral control to determine the optimum PTO torque based on a multiterm objective function. The pseudo-spectral optimalmore » control problem is extended to include load metrics in the objective function, which may now consist of competing terms. Separate penalty weights are attached to the surge-foundation force and PTO control torque to tune the optimizer performance to emphasize either <span class="hlt">power</span> absorption or load shedding. PTO efficiency is not included in the objective function, but the penalty weights are utilized to limit the force and torque amplitudes, thereby reducing losses associated with bidirectional energy flow. Results from pseudo-spectral control demonstrate that shedding a portion of the available <span class="hlt">wave</span> energy can provide greater reductions in structural loads and reactive <span class="hlt">power</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/872506','DOE-PATENT-XML'); return false;" href="https://www.osti.gov/servlets/purl/872506"><span>High <span class="hlt">power</span> water load for microwave and millimeter-<span class="hlt">wave</span> radio frequency sources</span></a></p> <p><a target="_blank" href="http://www.osti.gov/doepatents">DOEpatents</a></p> <p>Ives, R. Lawrence; Mizuhara, Yosuke M.; Schumacher, Richard V.; Pendleton, Rand P.</p> <p>1999-01-01</p> <p>A high <span class="hlt">power</span> water load for microwave and millimeter <span class="hlt">wave</span> radio frequency sources has a front wall including an input port for the application of RF <span class="hlt">power</span>, a cylindrical dissipation cavity lined with a dissipating material having a thickness which varies with depth, and a rear wall including a rotating reflector for the reflection of <span class="hlt">wave</span> energy inside the cylindrical cavity. The dissipation cavity includes a water jacket for removal of heat generated by the absorptive material coating the dissipation cavity, and this absorptive material has a thickness which is greater near the front wall than near the rear wall. <span class="hlt">Waves</span> entering the cavity reflect from the rotating reflector, impinging and reflecting multiple times on the absorptive coating of the dissipation cavity, dissipating equal amounts of <span class="hlt">power</span> on each internal reflection.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/1980JGR....85.3285E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/1980JGR....85.3285E"><span>Evidence for a continuous spectrum of equatorial <span class="hlt">waves</span> in the Indian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Eriksen, Charles C.</p> <p>1980-06-01</p> <p>Seven-month records of current and temperature measurements from a moored array centered at 53°E on the equator in the Indian <span class="hlt">Ocean</span> are consistent with a continuous spectrum of equatorially trapped internal inertial-gravity, mixed Rossby-gravity, and Kelvin <span class="hlt">waves</span>. A model spectrum of free linear <span class="hlt">waves</span> analogous to those for mid-latitude internal gravity <span class="hlt">waves</span> is used to compute spectra of observed quantities at depths greater than about 2000 m. Model parameters are adjusted to fit general patterns in the observed spectra over periods from roughly 2 days to 1 month. Measurements at shallower depths presumably include forced motions which we have not attempted to model. This `straw-person' spectrum is consistent with the limited data available. The model spectru Ē (n, m, ω) = K · B(m) · C(n, ω), where Ē is an average local energy density in the equatorial <span class="hlt">wave</span> guide which has amplitude K, <span class="hlt">wave</span> number shape B(m) ∝ (1 + m/m*)-3, where m is vertical mode number and the bandwidth parameter m* is between 4 and 8, and frequency shape C(n, ω) ∝ [(2n + 1 + s2)½ · σ3]-1 where n is meridional mode number, and s and σ are dimensionless zonal <span class="hlt">wave</span> number and frequency related by the usual dispersion relation. The scales are (β/cm)½ and (β · cm)½ for horizontal <span class="hlt">wave</span> number and frequency, where cm is the Kelvin <span class="hlt">wave</span> speed of the vertical mode m. At each frequency and vertical <span class="hlt">wave</span> number, energy is partitioned equally among the available inertial gravity modes so that the field tends toward horizontal isotropy at high frequency. The transition between Kelvin and mixed Rossby-gravity motion at low frequency and inertial-gravity motion at high frequency occurs at a period of roughly 1 week. At periods in the range 1-3 weeks, the model spectrum which fits the observations suggests that mixed Rossby-gravity motion dominates; at shorter periods gravity motion dominates. The model results are consistent with the low vertical coherence lengths observed (roughly 80 m</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMOS21E..01A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMOS21E..01A"><span>Modeling High-Resolution Coastal <span class="hlt">Ocean</span> Dynamics with COAMPS: System Overview, Applications and Future Directions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Allard, R. A.; Campbell, T. J.; Edwards, K. L.; Smith, T.; Martin, P.; Hebert, D. A.; Rogers, W.; Dykes, J. D.; Jacobs, G. A.; Spence, P. L.; Bartels, B.</p> <p>2014-12-01</p> <p>The Coupled <span class="hlt">Ocean</span> Atmosphere Mesoscale Prediction System (COAMPS®) is an atmosphere-<span class="hlt">ocean-wave</span> modeling system developed by the Naval Research Laboratory which can be configured to cycle regional forecasts/analysis models in single-model (atmosphere, <span class="hlt">ocean</span>, and <span class="hlt">wave</span>) or coupled-model (atmosphere-<span class="hlt">ocean</span>, <span class="hlt">ocean-wave</span>, and atmosphere-<span class="hlt">ocean-wave</span>) modes. The model coupling is performed using the Earth System Modeling Framework (ESMF). The <span class="hlt">ocean</span> component is the Navy Coastal <span class="hlt">Ocean</span> Model (NCOM), and the <span class="hlt">wave</span> components include Simulating <span class="hlt">WAves</span> Nearshore (SWAN) and <span class="hlt">Wave</span>Watch-III. NCOM has been modified to include wetting and drying, the effects of Stokes drift current, <span class="hlt">wave</span> radiation stresses due to horizontal gradients of the momentum flux of surface <span class="hlt">waves</span>, enhancement of bottom drag in shallow water, and enhanced vertical mixing due to Langmuir turbulence. An overview of the modeling system including <span class="hlt">ocean</span> data assimilation and specification of boundary conditions will be presented. Results from a high-resolution (10-250m) modeling study from the Surfzone Coastal Oil Pathways Experiment (SCOPE) near Ft. Walton Beach, Florida in December 2013 will be presented. ®COAMPS is a registered trademark of the Naval Research Laboratory</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1364035','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1364035"><span>Balancing <span class="hlt">Power</span> Absorption and Structural Loading for a Novel Fixed-Bottom <span class="hlt">Wave</span> Energy Converter with Nonideal <span class="hlt">Power</span> Take-Off in Regular <span class="hlt">Waves</span>: Preprint</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>Tom, Nathan M; Yu, Yi-Hsiang; Wright, Alan D</p> <p></p> <p>In this work, the net <span class="hlt">power</span> delivered to the grid from a nonideal <span class="hlt">power</span> take-off (PTO) is introduced followed by a review of the pseudo-spectral control theory. A <span class="hlt">power</span>-to-load ratio, used to evaluate the pseudo-spectral controller performance, is discussed, and the results obtained from optimizing a multiterm objective function are compared against results obtained from maximizing the net output <span class="hlt">power</span> to the grid. Simulation results are then presented for four different oscillating <span class="hlt">wave</span> energy converter geometries to highlight the potential of combing both geometry and PTO control to maximize <span class="hlt">power</span> while minimizing loads.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003JGRC..108.3049X','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003JGRC..108.3049X"><span>A numerical study of <span class="hlt">wave</span>-current interaction through surface and bottom stresses: Coastal <span class="hlt">ocean</span> response to Hurricane Fran of 1996</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Xie, L.; Pietrafesa, L. J.; Wu, K.</p> <p>2003-02-01</p> <p>A three-dimensional <span class="hlt">wave</span>-current coupled modeling system is used to examine the influence of <span class="hlt">waves</span> on coastal currents and sea level. This coupled modeling system consists of the <span class="hlt">wave</span> model-WAM (Cycle 4) and the Princeton <span class="hlt">Ocean</span> Model (POM). The results from this study show that it is important to incorporate surface <span class="hlt">wave</span> effects into coastal storm surge and circulation models. Specifically, we find that (1) storm surge models without coupled surface <span class="hlt">waves</span> 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 <span class="hlt">wave</span>-induced surface stress effect into storm surge models can significantly improve storm surge prediction, (3) incorporating <span class="hlt">wave</span>-induced bottom stress into the coupled <span class="hlt">wave</span>-current model further improves storm surge prediction, and (4) calibration of the <span class="hlt">wave</span> module according to minimum error in significant <span class="hlt">wave</span> height does not necessarily result in an optimum <span class="hlt">wave</span> module in a <span class="hlt">wave</span>-current coupled system for current and storm surge prediction.</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>Modelling <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 model of ice floe break-up under <span class="hlt">ocean</span> <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 model of <span class="hlt">ocean</span> <span class="hlt">wave</span> scattering by a finite array of compliant circular ice floes is coupled to a flexural failure model, 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 <span class="hlt">power</span> 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('https://www.ncbi.nlm.nih.gov/pubmed/23187338','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/23187338"><span>Phase-locking and coherent <span class="hlt">power</span> combining of broadband linearly chirped optical <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>Satyan, Naresh; Vasilyev, Arseny; Rakuljic, George; White, Jeffrey O; Yariv, Amnon</p> <p>2012-11-05</p> <p>We propose, analyze and demonstrate the optoelectronic phase-locking of optical <span class="hlt">waves</span> whose frequencies are chirped continuously and rapidly with time. The optical <span class="hlt">waves</span> are derived from a common optoelectronic swept-frequency laser based on a semiconductor laser in a negative feedback loop, with a precisely linear frequency chirp of 400 GHz in 2 ms. In contrast to monochromatic <span class="hlt">waves</span>, a differential delay between two linearly chirped optical <span class="hlt">waves</span> results in a mutual frequency difference, and an acoustooptic frequency shifter is therefore used to phase-lock the two <span class="hlt">waves</span>. We demonstrate and characterize homodyne and heterodyne optical phase-locked loops with rapidly chirped <span class="hlt">waves</span>, and show the ability to precisely control the phase of the chirped optical waveform using a digital electronic oscillator. A loop bandwidth of ~ 60 kHz, and a residual phase error variance of < 0.01 rad(2) between the chirped <span class="hlt">waves</span> is obtained. Further, we demonstrate the simultaneous phase-locking of two optical paths to a common master waveform, and the ability to electronically control the resultant two-element optical phased array. The results of this work enable coherent <span class="hlt">power</span> combining of high-<span class="hlt">power</span> fiber amplifiers-where a rapidly chirping seed laser reduces stimulated Brillouin scattering-and electronic beam steering of chirped optical <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017LatJP..54f..32B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017LatJP..54f..32B"><span>New Hydrokinetic Turbine for Free Surface Gravitational <span class="hlt">Wave</span> Transformation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Berins, J.</p> <p>2017-12-01</p> <p>The present article deals with an alternative form of energy - the conversion of marine/<span class="hlt">ocean</span> <span class="hlt">wave</span> energy using an axial self-regulating blade (SB) hydrokinetic turbine (ASRBHK turbine). The article analyses the operation of the ASRBHK turbine and draws the resulting conclusions about the mechanism, in which the <span class="hlt">power</span> transfer element is a self-regulating blade.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/26857371','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/26857371"><span>Development of a floating photobioreactor with internal partitions for efficient utilization of <span class="hlt">ocean</span> <span class="hlt">wave</span> into improved mass transfer and algal culture mixing.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kim, Z-Hun; Park, Hanwool; Hong, Seong-Joo; Lim, Sang-Min; Lee, Choul-Gyun</p> <p>2016-05-01</p> <p>Culturing microalgae in the <span class="hlt">ocean</span> has potentials that may reduce the production cost and provide an option for an economic biofuel production from microalgae. The <span class="hlt">ocean</span> holds great potentials for mass microalgal cultivation with its high specific heat, mixing energy from <span class="hlt">waves</span>, and large cultivable area. Suitable photobioreactors (PBRs) that are capable of integrating marine energy into the culture systems need to be developed for the successful <span class="hlt">ocean</span> cultivation. In this study, prototype floating PBRs were designed and constructed using transparent low-density polyethylene film for microalgal culture in the <span class="hlt">ocean</span>. To improve the mixing efficiency, various types of internal partitions were introduced within PBRs. Three different types of internal partitions were evaluated for their effects on the mixing efficiency in terms of mass transfer (k(L)a) and mixing time in the PBRs. The partition type with the best mixing efficiency was selected, and the number of partitions was varied from one to three for investigation of its effect on mixing efficiency. When the number of partitions is increased, mass transfer increased in proportion to the number of partitions. However, mixing time was not directly related to the number of partitions. When a green microalga, Tetraselmis sp. was cultivated using PBRs with the selected partition under semi-continuous mode in the <span class="hlt">ocean</span>, biomass and fatty acid productivities in the PBRs were increased by up to 50 % and 44% at high initial cell density, respectively, compared to non-partitioned ones. The results of internally partitioned PBRs demonstrated potentials for culturing microalgae by efficiently utilizing <span class="hlt">ocean</span> <span class="hlt">wave</span> energy into culture mixing in the <span class="hlt">ocean</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19830050148&hterms=Ocean+Stratification&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DOcean%2BStratification','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19830050148&hterms=Ocean+Stratification&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D10%26Ntt%3DOcean%2BStratification"><span>A baroclinic quasigeostrophic open <span class="hlt">ocean</span> model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Miller, R. N.; Robinson, A. R.; Haidvogel, D. B.</p> <p>1983-01-01</p> <p>A baroclinic quasigeostrophic open <span class="hlt">ocean</span> model is presented, calibrated by a series of test problems, and demonstrated to be feasible and efficient for application to realistic mid-<span class="hlt">oceanic</span> mesoscale eddy flow regimes. Two methods of treating the depth dependence of the flow, a finite difference method and a collocation method, are tested and intercompared. Sample Rossby <span class="hlt">wave</span> calculations with and without advection are performed with constant stratification and two levels of nonlinearity, one weaker than and one typical of real <span class="hlt">ocean</span> flows. Using exact analytical solutions for comparison, the accuracy and efficiency of the model is tabulated as a function of the computational parameters and stability limits set; typically, errors were controlled between 1 percent and 10 percent RMS after two <span class="hlt">wave</span> periods. Further Rossby <span class="hlt">wave</span> tests with realistic stratification and <span class="hlt">wave</span> parameters chosen to mimic real <span class="hlt">ocean</span> conditions were performed to determine computational parameters for use with real and simulated data. Finally, a prototype calculation with quasiturbulent simulated data was performed successfully, which demonstrates the practicality of the model for scientific use.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013OcMod..70..152B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013OcMod..70..152B"><span><span class="hlt">Wave</span>-current interaction: Effect on the <span class="hlt">wave</span> field in a semi-enclosed basin</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Benetazzo, A.; Carniel, S.; Sclavo, M.; Bergamasco, A.</p> <p>2013-10-01</p> <p>The effect on <span class="hlt">waves</span> of the <span class="hlt">Wave</span>-Current Interaction (WCI) process in the semi-enclosed Gulf of Venice (northern region of the Adriatic Sea) was investigated using the Coupled <span class="hlt">Ocean-Atmosphere-Wave</span>-Sediment Transport (COAWST) modeling system. COAWST relies on the <span class="hlt">ocean</span> model ROMS (Regional <span class="hlt">Ocean</span> Modeling System), the <span class="hlt">wave</span> model SWAN (Simulating <span class="hlt">WAves</span> Nearshore), and the CSTMS (Community Sediment Transport Modeling System) routines. The two-way data transfer between circulation and <span class="hlt">wave</span> 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 <span class="hlt">waves</span> were compared with observations at the CNR-ISMAR Acqua Alta oceanographic tower, located off the Venice littoral. <span class="hlt">Wave</span> 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 <span class="hlt">waves</span> generated by prevailing and dominant winds blowing on the Adriatic Sea: Bora and Sirocco. Due to the variable wind direction with respect to the <span class="hlt">ocean</span> current direction different effects on WCI were depicted, showing that within the northern Adriatic Sea the <span class="hlt">ocean-wave</span> interactions are strongly dependent on the wind forcing direction. Further</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1406245-high-power-rf-testing-cell-superconducting-traveling-wave-accelerating-structure','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1406245-high-power-rf-testing-cell-superconducting-traveling-wave-accelerating-structure"><span>High <span class="hlt">Power</span> RF Testing of A 3-Cell Superconducting Traveling <span class="hlt">Wave</span> Accelerating Structure</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>Kanareykin, Alex; Kostin, Romna; Avrakhov, Pavel</p> <p></p> <p>Euclid Techlabs has completed the Phase II SBIR project, entitled “High <span class="hlt">Power</span> RF Testing of a 3-Cell Superconducting Traveling <span class="hlt">Wave</span> Accelerating Structure” under Grant #DE-SC0006300. In this final technical report, we summarize the major achievements of Phase I of the project and review the details of Phase II of the project. The accelerating gradient in a superconducting structure is limited mainly by quenching, i.e., by the maximum surface RF magnetic field. Various techniques have been developed to increase the gradient. A traveling <span class="hlt">wave</span> accelerating SC structure with a feedback waveguide was suggested to allow an increased transit time factor andmore » ultimately, a maximum gradient that is 22%-24% higher than in the best of the time standing <span class="hlt">wave</span> SRF cavity solution. The proposed structure has an additional benefit in that it can be fabricated much longer than the standing <span class="hlt">wave</span> ones that are limited by the field flatness factor. Taken together, all of these factors will result in a significant overall length and, correspondingly cost reduction of the SRF based linear collider ILC or SRF technology based FELs. In Phase I of this project, a 3-cell L-band SC traveling <span class="hlt">wave</span> cavity was designed. Cavity shape, surface field ratios, inter-cell coupling coefficients, accelerating field flatness have been reviewed with the analysis of tuning issues. Moreover, the technological aspects of SC traveling <span class="hlt">wave</span> accelerating structure fabrication have been studied. As the next step in the project, the Phase II experimental program included engineering design, manufacturing, surface processing and high gradient testing. Euclid Techlabs, LLC contracted AES, Inc. to manufacture two niobium cavities. Euclid Techlabs cold tested traveling <span class="hlt">wave</span> regime in the cavity, and the results showed very good agreement with mathematical model specially developed for superconducting traveling <span class="hlt">wave</span> cavity performance analysis. Traveling <span class="hlt">wave</span> regime was adjusted by amplitude and phase</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.P51F..09V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.P51F..09V"><span>Tidal-Induced Internal <span class="hlt">Ocean</span> <span class="hlt">Waves</span> as an Explanation for Enceladus' Tiger Stripe Pattern and Hotspot Activity</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Vermeersen, B. L. A.; Maas, L. R.; van Oers, S.; Rabitti, A.; Jara-Orue, H.</p> <p>2014-12-01</p> <p>One of the most peculiar features on Saturn moon Enceladus is its so-called tiger stripe pattern at the geologically active South Polar Terrain (SPT), as first observed in detail by the Cassini spacecraft early 2005. It is generally assumed that the four almost parallel surface lines that constitute this pattern are faults in the icy surface overlying a confined salty water reservoir. Indeed, later Cassini observations have shown that salty water jets originate from the tiger stripes [e.g., Hansen et al., Science, 311, 1422-1425, 2006; Postberg et al., Nature, 474, 620-622, 2011]. More recently, Porco et al. [Astron. J., 148:45, Sep. 2014] and Nimmo et al. [Astron. J., 148:46, Sep. 2014] have reported strong evidence that the geysers are not caused by frictional heating at the surface, but that geysers must originate deeper in Enceladus' interior. Tidal flexing models, like those of Hurford et al., Nature, 447, 292-294, 2007, give a good match for the brightness variations Cassini observes, but they seem to fail to reproduce the exact timing of plume brightening. Although jet activity is thus strongly connected to tidal forcing, another mechanism must be involved as well. Last year, we formulated the original idea [Vermeersen et al., AGU Fall Meeting 2013, abstract #P53B-1848] that the tiger stripe pattern is formed and maintained by induced, tidally and rotationally driven, <span class="hlt">wave</span>-attractor motions in the <span class="hlt">ocean</span> underneath the icy surface of the tiger-stripe region. Such <span class="hlt">wave</span>-attractor motions are observed in water tank experiments in laboratories on Earth and in numerical experiments [Maas et al., Nature, 338, 557-561, 1997; Drijfhout and Maas, J. Phys. Oceanogr., 37, 2740-2763, 2007; Hazewinkel et al., Phys. Fluids, 22, 107102, 2010]. The latest observations by Porco et al. and Nimmo et al. seem to be in agreement with this tidal-induced <span class="hlt">wave</span> attractor phenomenon, both with respect to tiger stripe pattern and with respect to timing of hotspot activity. However, in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://pubs.er.usgs.gov/publication/70179088','USGSPUBS'); return false;" href="https://pubs.er.usgs.gov/publication/70179088"><span>A multimodal <span class="hlt">wave</span> spectrum-based approach for statistical downscaling of local <span class="hlt">wave</span> climate</span></a></p> <p><a target="_blank" href="http://pubs.er.usgs.gov/pubs/index.jsp?view=adv">USGS Publications Warehouse</a></p> <p>Hegermiller, Christie; Antolinez, Jose A A; Rueda, Ana C.; Camus, Paula; Perez, Jorge; Erikson, Li; Barnard, Patrick; Mendez, Fernando J.</p> <p>2017-01-01</p> <p>Characterization of <span class="hlt">wave</span> climate by bulk <span class="hlt">wave</span> parameters is insufficient for many coastal studies, including those focused on assessing coastal hazards and long-term <span class="hlt">wave</span> climate influences on coastal evolution. This issue is particularly relevant for studies using statistical downscaling of atmospheric fields to local <span class="hlt">wave</span> conditions, which are often multimodal in large <span class="hlt">ocean</span> basins (e.g. the Pacific). Swell may be generated in vastly different <span class="hlt">wave</span> generation regions, yielding complex <span class="hlt">wave</span> spectra that are inadequately represented by a single set of bulk <span class="hlt">wave</span> parameters. Furthermore, the relationship between atmospheric systems and local <span class="hlt">wave</span> conditions is complicated by variations in arrival time of <span class="hlt">wave</span> groups from different parts of the basin. Here, we address these two challenges by improving upon the spatiotemporal definition of the atmospheric predictor used in statistical downscaling of local <span class="hlt">wave</span> climate. The improved methodology separates the local <span class="hlt">wave</span> spectrum into “<span class="hlt">wave</span> families,” defined by spectral peaks and discrete generation regions, and relates atmospheric conditions in distant regions of the <span class="hlt">ocean</span> basin to local <span class="hlt">wave</span> conditions by incorporating travel times computed from effective energy flux across the <span class="hlt">ocean</span> basin. When applied to locations with multimodal <span class="hlt">wave</span> spectra, including Southern California and Trujillo, Peru, the new methodology improves the ability of the statistical model to project significant <span class="hlt">wave</span> height, peak period, and direction for each <span class="hlt">wave</span> family, retaining more information from the full <span class="hlt">wave</span> spectrum. This work is the base of statistical downscaling by weather types, which has recently been applied to coastal flooding and morphodynamic applications.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..1817873E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1817873E"><span><span class="hlt">Ocean</span> thermal gradient as a generator of electricity. OTEC <span class="hlt">power</span> plant</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Enrique, Luna-Gomez Victor; Angel, Alatorre-Mendieta Miguel</p> <p>2016-04-01</p> <p>The OTEC (<span class="hlt">Ocean</span> Thermal Energy Conversion) is a <span class="hlt">power</span> plant that uses the thermal gradient of the sea water between the surface and a depth of about 700 meters. It works by supplying the heat to a steam machine, for evaporation, with sea water from the surface and cold, to condense the steam, with deep sea water. The energy generated by the <span class="hlt">power</span> plant OTEC can be transferred to the electric <span class="hlt">power</span> grid, another use is to desalinate seawater. During the twentieth century in some countries experimental <span class="hlt">power</span> plants to produce electricity or obtaining drinking water they were installed. On the Mexico's coast itself this thermal gradient, as it is located in tropical seas it occurs, so it has possibilities of installing OTEC <span class="hlt">power</span> plant type. In this paper one type OTEC <span class="hlt">power</span> plant operation is represented in most of its components.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1912760C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1912760C"><span>The Global Drifter Program Currents, Sea Surface Temperature, Atmospheric Pressure and <span class="hlt">Waves</span> in the World's <span class="hlt">Ocean</span>The Global Drifter Program Currents, Sea Surface Temperature, Atmospheric Pressure and <span class="hlt">Waves</span> in the World's <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Centurioni, Luca</p> <p>2017-04-01</p> <p>The Global Drifter Program is the principal component of the Global Surface Drifting Buoy Array, a branch of NOAA's Global <span class="hlt">Ocean</span> Observing System and a scientific project of the Data Buoy Cooperation Panel (DBCP). The DBCP is an international program coordinating the use of autonomous data buoys to observe atmospheric and oceanographic conditions over <span class="hlt">ocean</span> areas where few other measurements are taken. The Global Drifter Program maintains an array of over 1,250 Lagrangian drifters, reporting in near real-time and designed measure 15 m depth Lagrangian currents, sea surface temperature (SST) and sea level atmospheric pressure (SLP), among others, to fulfill the needs to observe the air-sea interface at temporal and spatial scales adequate to support short to medium-range weather forecasting, <span class="hlt">ocean</span> state estimates and climate science. This overview talk will discuss the main achievements of the program, the main impacts for satellite SST calibration and validation, for numerical weather prediction, and it will review the main scientific findings based on the use of Lagrangian currents. Finally, we will present new developments in Lagrangian drifter technology, which include special drifters designed to measure sea surface salinity, wind and directional <span class="hlt">wave</span> spectra. New opportunities for expanding the scope of the Global Drifter Program will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2012-02-06/pdf/2012-2547.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2012-02-06/pdf/2012-2547.pdf"><span>77 FR 5817 - <span class="hlt">Ocean</span> Renewable <span class="hlt">Power</span> Company, Tidal Energy Project, Cobscook Bay, ME</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2012-02-06</p> <p>... <span class="hlt">ocean</span> floor, used for generating electricity from tidal currents and is now providing the public the... impacts associated with installation of an underwater cable assembly to transfer electricity to a <span class="hlt">power</span>...</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_18");'>18</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li class="active"><span>20</span></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_20 --> <div id="page_21" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_19");'>19</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li class="active"><span>21</span></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="401"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSA33A2582R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSA33A2582R"><span>Universal <span class="hlt">Power</span> Law of the Gravity <span class="hlt">Wave</span> Manifestation in the AIM CIPS Polar Mesospheric Cloud Images</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rong, P. P.; Yue, J.; Russell, J. M., III; Siskind, D. E.; Randall, C. E.</p> <p>2017-12-01</p> <p>A large ensemble of gravity <span class="hlt">waves</span> (GWs) resides in the PMCs and we aim to extract the universal law that governs the <span class="hlt">wave</span> display throughout the GW population. More specifically, we examined how <span class="hlt">wave</span> display morphology and clarity level varies throughout the <span class="hlt">wave</span> population manifested through the PMC albedo data. Higher clarity refers to more distinct exhibition of the features which often correspond to larger variances and better organized nature. A gravity <span class="hlt">wave</span> tracking algorithm is designed and applied to the PMC albedo data taken by the AIM Cloud Imaging and Particle Size (CIPS) instrument to obtain the gravity <span class="hlt">wave</span> detections throughout the two northern summers in 2007 and 2010. The horizontal wavelengths in the range of 20-60km are the focus of the study because they are the most commonly observed and readily captured in the CIPS orbital strips. A 1-dimensional continuous wavelet transform (CWT) is applied to PMC albedo along all radial directions within an elliptical region that has a radius of 400 km and an axial ratio of 0.65. The center of the elliptical region moves around the CIPS orbital strips so that <span class="hlt">waves</span> at different locations and orientations can be captured. It shows that the CWT albedo <span class="hlt">power</span> statistically increases as the background gets brighter. We resample the <span class="hlt">wave</span> detections to conform to a normal distribution via removing the dependence of the albedo <span class="hlt">power</span> on the background cloud brightness because we tend to examine the <span class="hlt">wave</span> morphology beyond the cloud brightness impact. Sample cases are selected at the two tails and the peak of the normal distribution, and at three brightness levels, to represent the high, medium, and low albedo <span class="hlt">power</span> categories. For these cases the albedo CWT <span class="hlt">power</span> spectra follow exponential decay toward smaller scales. The high albedo <span class="hlt">power</span> has the most rapid decay (i.e., exponent=-3.2) and corresponds to the most distinct <span class="hlt">wave</span> display. Overall higher albedo <span class="hlt">power</span> and more rapid decay both contributed to the more</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19920037308&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=19920037308&hterms=fashion+models&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Dfashion%2Bmodels"><span>Fitting dynamic models to the Geosat sea level observations in the tropical Pacific <span class="hlt">Ocean</span>. I - A free <span class="hlt">wave</span> model</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fu, Lee-Lueng; Vazquez, Jorge; Perigaud, Claire</p> <p>1991-01-01</p> <p>Free, equatorially trapped sinusoidal <span class="hlt">wave</span> solutions to a linear model on an equatorial beta plane are used to fit the Geosat altimetric sea level observations in the tropical Pacific <span class="hlt">Ocean</span>. The Kalman filter technique is used to estimate the <span class="hlt">wave</span> amplitude and phase from the data. The estimation is performed at each time step by combining the model forecast with the observation in an optimal fashion utilizing the respective error covariances. The model error covariance is determined such that the performance of the model forecast is optimized. It is found that the dominant observed features can be described qualitatively by basin-scale Kelvin <span class="hlt">waves</span> and the first meridional-mode Rossby <span class="hlt">waves</span>. Quantitatively, however, only 23 percent of the signal variance can be accounted for by this simple model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1014394','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1014394"><span>Generation and Evolution of Internal <span class="hlt">Waves</span> in Luzon Strait</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-09-30</p> <p>1 DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Generation and Evolution of Internal <span class="hlt">Waves</span> in Luzon...inertial <span class="hlt">waves</span> , nonlinear internal <span class="hlt">waves</span> (NLIWs), and turbulence mixing––in the <span class="hlt">ocean</span> and thereby help develop improved parameterizations of mixing for...<span class="hlt">ocean</span> models. Mixing within the stratified <span class="hlt">ocean</span> is a particular focus as the complex interplay of internal <span class="hlt">waves</span> from a variety of sources and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/AD1007273','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/AD1007273"><span>Generation and Evolution of Internal <span class="hlt">Waves</span> in Luzon Strait</span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2016-03-01</p> <p>1 DISTRIBUTION STATEMENT A: Distribution approved for public release; distribution is unlimited. Generation and Evolution of Internal <span class="hlt">Waves</span> in...internal tides, inertial <span class="hlt">waves</span> , nonlinear internal <span class="hlt">waves</span> (NLIWs), and turbulence mixing––in the <span class="hlt">ocean</span> and thereby help develop improved parameterizations of...mixing for <span class="hlt">ocean</span> models. Mixing within the stratified <span class="hlt">ocean</span> is a particular focus as the complex interplay of internal <span class="hlt">waves</span> from a variety of</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.gpo.gov/fdsys/pkg/FR-2012-01-11/pdf/2012-272.pdf','FEDREG'); return false;" href="https://www.gpo.gov/fdsys/pkg/FR-2012-01-11/pdf/2012-272.pdf"><span>77 FR 1674 - <span class="hlt">Ocean</span> Renewable <span class="hlt">Power</span> Company Maine, LLC; Notice of Availability of Environmental Assessment for...</span></a></p> <p><a target="_blank" href="http://www.gpo.gov/fdsys/browse/collection.action?collectionCode=FR">Federal Register 2010, 2011, 2012, 2013, 2014</a></p> <p></p> <p>2012-01-11</p> <p>... DEPARTMENT OF ENERGY Federal Energy Regulatory Commission [Project No. 12711-005] <span class="hlt">Ocean</span> Renewable... Bay Tidal Energy Project In accordance with the National Environmental Policy Act of 1969 and the..., 52 FR 47897), the Office of Energy Projects has reviewed <span class="hlt">Ocean</span> Renewable <span class="hlt">Power</span> Company, LLC's...</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><span class="hlt">Ocean</span>-atmosphere dynamics during Hurricane Ida and Nor'Ida: An application of the coupled <span class="hlt">ocean</span>-;atmosphere–wave–sediment transport (COAWST) modeling 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 coupled ocean–atmosphere–wave–sediment transport (COAWST) modeling 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 modeled 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 (modeled with Weather Research and Forecasting, the WRF model), the <span class="hlt">ocean</span> (modeled with Regional <span class="hlt">Ocean</span> Modeling System (ROMS)), and the <span class="hlt">wave</span> propagation and generation model (modeled with Simulating <span class="hlt">Waves</span> Nearshore (SWAN)). Special attention was given to the role of the <span class="hlt">ocean</span> surface roughness. Three different <span class="hlt">ocean</span> roughness closure models 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 <span class="hlt">ocean</span> roughness in the atmospheric module improved the wind intensity estimation and therefore also the wind <span class="hlt">waves</span>, 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 <span class="hlt">wave</span>-induced <span class="hlt">ocean</span> 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/2017APS..DFDM19009V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017APS..DFDM19009V"><span>Internal <span class="hlt">wave</span> mode resonant triads in an arbitrarly stratified finite-depth <span class="hlt">ocean</span> with background rotation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Varma, Dheeraj; Mathur, Manikandan</p> <p>2017-11-01</p> <p>Internal tides generated by barotropic tides on bottom topography or the spatially compact near-inertial mixed layer currents excited by surface winds can be conveniently represented in the linear regime as a superposition of vertical modes at a given frequency in an arbitrarily stratified <span class="hlt">ocean</span> of finite depth. Considering modes (m , n) at a frequency ω in the primary <span class="hlt">wave</span> field, we derive the weakly nonlinear solution, which contains a secondary <span class="hlt">wave</span> at 2 ω that diverges when it forms a resonant triad with the primary <span class="hlt">waves</span>. In nonuniform stratifications, resonant triads are shown to occur when the horizontal component of the classical RTI criterion k->1 +k->2 +k->3 = 0 is satisfied along with a non-orthogonality criterion. In nonuniform stratifications with a pycnocline, infinitely more pairs of primary <span class="hlt">wave</span> modes (m , n) result in RTI when compared to a uniform stratification. Further, two nearby high modes at around the near-inertial frequency often form a resonant triad with a low mode at 2 ω , reminiscent of the features of PSI near the critical latitude. The theoretical framework is then adapted to investigate RTI in two different scenarios: low-mode internal tide scattering over topography, and internal <span class="hlt">wave</span> beams incident on a pycnocline. The authors thank the Ministry of Earth Sciences, Government of India for financial support under the Monsoon Mission Grant MM/2014/IND-002.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1416257-power-load-balancing-asymmetric-heave-wave-energy-converters-nonideal-power-take-off','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1416257-power-load-balancing-asymmetric-heave-wave-energy-converters-nonideal-power-take-off"><span><span class="hlt">Power</span>-to-load balancing for asymmetric heave <span class="hlt">wave</span> energy converters with nonideal <span class="hlt">power</span> take-off</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>Tom, Nathan M.; Madhi, Farshad; Yeung, Ronald W.</p> <p></p> <p>The aim of this study is to maximize the <span class="hlt">power</span>-to-load ratio for asymmetric heave <span class="hlt">wave</span> energy converters. Linear hydrodynamic theory was used to calculate bounds of the expected time-averaged <span class="hlt">power</span> (TAP) and corresponding surge-restraining force, pitch-restraining torque, and <span class="hlt">power</span> take-off (PTO) control force with the assumption of sinusoidal displacement. This paper formulates an optimal control problem to handle an objective function with competing terms in an attempt to maximize <span class="hlt">power</span> capture while minimizing structural and actuator loads in regular and irregular <span class="hlt">waves</span>. Penalty weights are placed on the surge-restraining force, pitch-restraining torque, and PTO actuation force, thereby allowing the controlmore » focus to concentrate on either <span class="hlt">power</span> absorption or load mitigation. The penalty weights are used to control peak structural and actuator loads that were found to curb the additional losses in <span class="hlt">power</span> absorption associated with a nonideal PTO. Thus, in achieving these goals, a per-unit gain in TAP would not lead to a greater per-unit demand in structural strength, hence yielding a favorable benefit-to-cost ratio. Demonstrative results for 'The Berkeley Wedge' in the form of output TAP, reactive TAP needed to drive WEC motion, and the amplitudes of the surge-restraining force, pitch-restraining torque, and PTO control force are shown.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/pages/biblio/1416257-power-load-balancing-asymmetric-heave-wave-energy-converters-nonideal-power-take-off','SCIGOV-DOEP'); return false;" href="https://www.osti.gov/pages/biblio/1416257-power-load-balancing-asymmetric-heave-wave-energy-converters-nonideal-power-take-off"><span><span class="hlt">Power</span>-to-load balancing for asymmetric heave <span class="hlt">wave</span> energy converters with nonideal <span class="hlt">power</span> take-off</span></a></p> <p><a target="_blank" href="http://www.osti.gov/pages">DOE PAGES</a></p> <p>Tom, Nathan M.; Madhi, Farshad; Yeung, Ronald W.</p> <p>2017-12-11</p> <p>The aim of this study is to maximize the <span class="hlt">power</span>-to-load ratio for asymmetric heave <span class="hlt">wave</span> energy converters. Linear hydrodynamic theory was used to calculate bounds of the expected time-averaged <span class="hlt">power</span> (TAP) and corresponding surge-restraining force, pitch-restraining torque, and <span class="hlt">power</span> take-off (PTO) control force with the assumption of sinusoidal displacement. This paper formulates an optimal control problem to handle an objective function with competing terms in an attempt to maximize <span class="hlt">power</span> capture while minimizing structural and actuator loads in regular and irregular <span class="hlt">waves</span>. Penalty weights are placed on the surge-restraining force, pitch-restraining torque, and PTO actuation force, thereby allowing the controlmore » focus to concentrate on either <span class="hlt">power</span> absorption or load mitigation. The penalty weights are used to control peak structural and actuator loads that were found to curb the additional losses in <span class="hlt">power</span> absorption associated with a nonideal PTO. Thus, in achieving these goals, a per-unit gain in TAP would not lead to a greater per-unit demand in structural strength, hence yielding a favorable benefit-to-cost ratio. Demonstrative results for 'The Berkeley Wedge' in the form of output TAP, reactive TAP needed to drive WEC motion, and the amplitudes of the surge-restraining force, pitch-restraining torque, and PTO control force are shown.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2003ASAJ..114.2418S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2003ASAJ..114.2418S"><span>Nonlinear and linear <span class="hlt">wave</span> equations for propagation in media with frequency <span class="hlt">power</span> law losses</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Szabo, Thomas L.</p> <p>2003-10-01</p> <p>The Burgers, KZK, and Westervelt <span class="hlt">wave</span> equations used for simulating <span class="hlt">wave</span> propagation in nonlinear media are based on absorption that has a quadratic dependence on frequency. Unfortunately, most lossy media, such as tissue, follow a more general frequency <span class="hlt">power</span> law. The authors first research involved measurements of loss and dispersion associated with a modification to Blackstock's solution to the linear thermoviscous <span class="hlt">wave</span> equation [J. Acoust. Soc. Am. 41, 1312 (1967)]. A second paper by Blackstock [J. Acoust. Soc. Am. 77, 2050 (1985)] showed the loss term in the Burgers equation for plane <span class="hlt">waves</span> could be modified for other known instances of loss. The authors' work eventually led to comprehensive time-domain convolutional operators that accounted for both dispersion and general frequency <span class="hlt">power</span> law absorption [Szabo, J. Acoust. Soc. Am. 96, 491 (1994)]. Versions of appropriate loss terms were developed to extend the standard three nonlinear <span class="hlt">wave</span> equations to these more general losses. Extensive experimental data has verified the predicted phase velocity dispersion for different <span class="hlt">power</span> exponents for the linear case. Other groups are now working on methods suitable for solving <span class="hlt">wave</span> equations numerically for these types of loss directly in the time domain for both linear and nonlinear media.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.2375I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.2375I"><span>Progress Report on the GROWTH (GNSS Reflectometry for <span class="hlt">Ocean</span> <span class="hlt">Waves</span>, Tides, and Height) Research Project</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ichikawa, Kaoru; Akiyama, Hiroaki; Ebinuma, Takuji; Isoguchi, Osamu; Kimura, Noriaki; Kitazawa, Yukihito; Konda, Masanori; Kouguchi, Nobuyuki; Tamura, Hitoshi; Tomita, Hiroyuki; Yoshikawa, Yutaka; Waseda, Takuji</p> <p>2016-04-01</p> <p>There has been considerable interest in GNSS Reflectometry (GNSS-R) as a new remote-sensing method. We have started a research program for GNSS-R applications on oceanographic observations under the contract with MEXT (Ministry of Education Culture, Sports, Science and Technology, JAPAN) and launched a Japanese research consortium, GROWTH. It is aiming to evaluate the capabilities of GNSS-R observations for oceanographic phenomena with different time scales, such as <span class="hlt">ocean</span> <span class="hlt">waves</span> (1/10 to tens of seconds), tides (one or half days), and sea surface dynamic height (a few days to years). In situ observations of <span class="hlt">ocean</span> <span class="hlt">wave</span> spectrum, wind speed vertical profile, and sea surface height will be quantitatively compared with equivalent estimates from simultaneous GNSS-R measurements. The GROWTH project will utilize different types of observation platforms; marine observation towers (about 20 m height), multi-copters (about 100 to 200 m height), and much higher-altitude CYGNSS data. Cross-platform data, together with in situ oceanographic observations, will be compared after adequate temporal averaging that accounts differences of the footprint sizes and temporal and spatial scales of oceanographic phenomena. This paper will provide overview of the GROWTH project, preliminary test results obtained by the multi-sensor platform at observation towers, and preparation status of a ground station that will be supplied to receive CYGNSS data at Japan.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/1335572-balancing-power-absorption-structural-loading-asymmetric-heave-wave-energy-converter-regular-waves','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/1335572-balancing-power-absorption-structural-loading-asymmetric-heave-wave-energy-converter-regular-waves"><span>Balancing <span class="hlt">Power</span> Absorption and Structural Loading for an Asymmetric Heave <span class="hlt">Wave</span>-Energy Converter in Regular <span class="hlt">Waves</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>Tom, Nathan M.; Madhi, Farshad; Yeung, Ronald W.</p> <p>2016-06-24</p> <p>The aim of this paper is to maximize the <span class="hlt">power</span>-to-load ratio of the Berkeley Wedge: a one-degree-of-freedom, asymmetrical, energy-capturing, floating breakwater of high performance that is relatively free of viscosity effects. Linear hydrodynamic theory was used to calculate bounds on the expected time-averaged <span class="hlt">power</span> (TAP) and corresponding surge restraining force, pitch restraining torque, and <span class="hlt">power</span> take-off (PTO) control force when assuming that the heave motion of the <span class="hlt">wave</span> energy converter remains sinusoidal. This particular device was documented to be an almost-perfect absorber if one-degree-of-freedom motion is maintained. The success of such or similar future <span class="hlt">wave</span> energy converter technologies would requiremore » the development of control strategies that can adapt device performance to maximize energy generation in operational conditions while mitigating hydrodynamic loads in extreme <span class="hlt">waves</span> to reduce the structural mass and overall cost. This paper formulates the optimal control problem to incorporate metrics that provide a measure of the surge restraining force, pitch restraining torque, and PTO control force. The optimizer must now handle an objective function with competing terms in an attempt to maximize <span class="hlt">power</span> capture while minimizing structural and actuator loads. A penalty weight is placed on the surge restraining force, pitch restraining torque, and PTO actuation force, thereby allowing the control focus to be placed either on <span class="hlt">power</span> absorption or load mitigation. Thus, in achieving these goals, a per-unit gain in TAP would not lead to a greater per-unit demand in structural strength, hence yielding a favorable benefit-to-cost ratio. Demonstrative results in the form of TAP, reactive TAP, and the amplitudes of the surge restraining force, pitch restraining torque, and PTO control force are shown for the Berkeley Wedge example.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5666229','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=5666229"><span>Modelling <span class="hlt">wave</span>-induced sea ice break-up in the marginal ice zone</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Squire, V. A.</p> <p>2017-01-01</p> <p>A model of ice floe break-up under <span class="hlt">ocean</span> <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 model of <span class="hlt">ocean</span> <span class="hlt">wave</span> scattering by a finite array of compliant circular ice floes is coupled to a flexural failure model, 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 <span class="hlt">power</span> 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. PMID:29118659</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/29118659','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/29118659"><span>Modelling <span class="hlt">wave</span>-induced sea ice break-up in the marginal ice zone.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Montiel, F; Squire, V A</p> <p>2017-10-01</p> <p>A model of ice floe break-up under <span class="hlt">ocean</span> <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 model of <span class="hlt">ocean</span> <span class="hlt">wave</span> scattering by a finite array of compliant circular ice floes is coupled to a flexural failure model, 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 <span class="hlt">power</span> 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/2013GeoJI.195.1862K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013GeoJI.195.1862K"><span>High-frequency Po/So guided <span class="hlt">waves</span> in the <span class="hlt">oceanic</span> lithosphere: I-long-distance propagation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kennett, B. L. N.; Furumura, T.</p> <p>2013-12-01</p> <p>In many parts of the <span class="hlt">ocean</span> high-frequency seismic energy is carried to very great distances from the source. The onsets of the P and S energy travel with speeds characteristic of the mantle lithosphere. The complex and elongated waveforms of such Po and So <span class="hlt">waves</span> and their efficient transport of high frequencies (>10 Hz) have proved difficult to explain in full. Much of the character can be captured with stratified models, provided a full allowance is made for reverberations in the <span class="hlt">ocean</span> and the basal sediments. The nature of the observations implies a strong scattering environment. By analysing the nature of the long-distance propagation we are able to identify the critical role played by shallow reverberations in the water and sediments, and the way that these link with propagation in a heterogeneous mantle. 2-D finite difference modelling to 10 Hz for ranges over 1000 km demonstrates the way in which heterogeneity shapes the wavefield, and the way in which the properties of the lithosphere and asthenosphere control the nature of the propagation processes. The nature of the Po and So phases are consistent with pervasive heterogeneity in the <span class="hlt">oceanic</span> lithosphere with a horizontal correlation length (˜10 km) much larger than the vertical correlation length (˜0.5 km).</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017ApPhL.110p3505T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017ApPhL.110p3505T"><span>Self-bending elastic <span class="hlt">waves</span> and obstacle circumventing in wireless <span class="hlt">power</span> transfer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tol, S.; Xia, Y.; Ruzzene, M.; Erturk, A.</p> <p>2017-04-01</p> <p>We demonstrate self-bending of elastic <span class="hlt">waves</span> along convex trajectories by means of geometric and phased arrays. Potential applications include ultrasonic imaging and manipulation, <span class="hlt">wave</span> focusing, and wireless <span class="hlt">power</span> transfer around obstacles. The basic concept is illustrated through a geometric array, which is designed to implement a phase delay profile among the array elements that leads to self-bending along a specified circular trajectory. Experimental validation is conducted for the lowest asymmetric Lamb <span class="hlt">wave</span> mode in a thin plate over a range of frequencies to investigate the bandwidth of the approach. Experiments also illustrate the functionality of the array as a transmitter to deliver elastic <span class="hlt">wave</span> energy to a receiver/harvester located behind a large obstacle for electrical <span class="hlt">power</span> extraction. It is shown that the trajectory is not distorted by the presence of the obstacle and circumventing is achieved. A linear phased array counterpart of the geometric array is then constructed to illustrate the concept by imposing proper time delays to the array elements, which allows the generation of different trajectories using the same line source. This capability is demonstrated by tailoring the path diameter in the phased array setting, which offers the flexibility and versatility to induce a variety of convex trajectories for self-bending elastic <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018ACP....18..883R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018ACP....18..883R"><span>Universal <span class="hlt">power</span> law of the gravity <span class="hlt">wave</span> manifestation in the AIM CIPS polar mesospheric cloud images</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rong, Pingping; Yue, Jia; Russell, James M., III; Siskind, David E.; Randall, Cora E.</p> <p>2018-01-01</p> <p>We aim to extract a universal law that governs the gravity <span class="hlt">wave</span> manifestation in polar mesospheric clouds (PMCs). Gravity <span class="hlt">wave</span> morphology and the clarity level of display vary throughout the <span class="hlt">wave</span> population manifested by the PMC albedo data. Higher clarity refers to more distinct exhibition of the features, which often correspond to larger variances and a better-organized nature. A gravity <span class="hlt">wave</span> tracking algorithm based on the continuous Morlet wavelet transform is applied to the PMC albedo data at 83 km altitude taken by the Aeronomy of Ice in the Mesosphere (AIM) Cloud Imaging and Particle Size (CIPS) instrument to obtain a large ensemble of the gravity <span class="hlt">wave</span> detections. The horizontal wavelengths in the range of ˜ 20-60 km are the focus of the study. It shows that the albedo (<span class="hlt">wave</span>) <span class="hlt">power</span> statistically increases as the background gets brighter. We resample the <span class="hlt">wave</span> detections to conform to a normal distribution to examine the <span class="hlt">wave</span> morphology and display clarity beyond the cloud brightness impact. Sample cases are selected at the two tails and the peak of the normal distribution to represent the full set of <span class="hlt">wave</span> detections. For these cases the albedo <span class="hlt">power</span> spectra follow exponential decay toward smaller scales. The high-albedo-<span class="hlt">power</span> category has the most rapid decay (i.e., exponent = -3.2) and corresponds to the most distinct <span class="hlt">wave</span> display. The <span class="hlt">wave</span> display becomes increasingly blurrier for the medium- and low-<span class="hlt">power</span> categories, which hold the monotonically decreasing spectral exponents of -2.9 and -2.5, respectively. The majority of <span class="hlt">waves</span> are straight <span class="hlt">waves</span> whose clarity levels can collapse between the different brightness levels, but in the brighter background the <span class="hlt">wave</span> signatures seem to exhibit mildly turbulent-like behavior.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFM.A41J3196F','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFM.A41J3196F"><span>Towards Removing the Southern <span class="hlt">Ocean</span> Short <span class="hlt">Wave</span> Bias in HadGEM3: Mixed-phase Cloud Improvements.</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Field, P.; Furtado, K.</p> <p>2014-12-01</p> <p>Many IPCC models suffer from significant Sea Surface Temperature (SST) biases in the Southern <span class="hlt">Ocean</span> that adversely affects the representation of the cryosphere and global circulation in these models. Evidence suggests that much of this error is linked to Short <span class="hlt">Wave</span> (SW) radiation, sensible and latent heat biases. Flaws in the representation of clouds and a deficit of supercooled liquid water in mixed-phase clouds are suspected as a likely source of the SW error. A physically based method that uses subgrid turbulence to control a new liquid production term has been developed. Comparisons between theory, based on a stochastic differential equation used to represent supersaturation fluctuations, and decametre resolution Large Eddy Simulations will be presented. An implementation of this approach in a GCM shows an increased prevalance of supercooled liquid water and a reduction in the magnitude of the Southern <span class="hlt">Ocean</span> SW bias. To conclude, we will summarize the complete package of changes that have been made to tackle the Southern <span class="hlt">Ocean</span> SST bias in a physically meaningful way.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JIEIB..98..213K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JIEIB..98..213K"><span>Electronic <span class="hlt">Power</span> Conditioner for Ku-band Travelling <span class="hlt">Wave</span> Tube</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kowstubha, Palle; Krishnaveni, K.; Ramesh Reddy, K.</p> <p>2017-04-01</p> <p>A highly sophisticated regulated <span class="hlt">power</span> supply is known as electronic <span class="hlt">power</span> conditioner (EPC) is required to energise travelling <span class="hlt">wave</span> tubes (TWTs), which are used as RF signal amplifiers in satellite payloads. The assembly consisting of TWT and EPC together is known as travelling <span class="hlt">wave</span> tube amplifier (TWTA). EPC is used to provide isolated and conditioned voltage rails with tight regulation to various electrodes of TWT and makes its RF performance independent of solar bus variations which are caused due to varying conditions of eclipse and sunlit. The payload mass and their <span class="hlt">power</span> consumption is mainly due to the existence of TWTAs that represent about 35 % of total mass and about 70-90 % (based on the type of satellite application) of overall dc <span class="hlt">power</span> consumption. This situation ensures a continuous improvement in the design of TWTAs and their associated EPCs to realize more efficient and light products. Critical technologies involved in EPCs are design and configuration, closed loop regulation, component and material selection, energy limiting of high voltage (HV) outputs and potting of HV card etc. This work addresses some of these critical technologies evolved in realizing and testing the state of art of EPC and it focuses on the design of HV supply with a HV and high <span class="hlt">power</span> capability, up to 6 kV and 170 WRF, respectively required for a space TWTA. Finally, an experimental prototype of EPC with a dc <span class="hlt">power</span> of 320 W provides different voltages required by Ku-band TWT in open loop configuration.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017PhRvC..95e4001V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017PhRvC..95e4001V"><span><span class="hlt">Power</span> counting in peripheral partial <span class="hlt">waves</span>: The singlet channels</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Valderrama, M. Pavón; Sánchez, M. Sánchez; Yang, C.-J.; Long, Bingwei; Carbonell, J.; van Kolck, U.</p> <p>2017-05-01</p> <p>We analyze the <span class="hlt">power</span> counting of the peripheral singlet partial <span class="hlt">waves</span> in nucleon-nucleon scattering. In agreement with conventional wisdom, we find that pion exchanges are perturbative in the peripheral singlets. We quantify from the effective field theory perspective the well-known suppression induced by the centrifugal barrier in the pion-exchange interactions. By exploring perturbation theory up to fourth order, we find that the one-pion-exchange potential in these channels is demoted from leading to subleading order by a given <span class="hlt">power</span> of the expansion parameter that grows with the orbital angular momentum. We discuss the implications of these demotions for few-body calculations: though higher partial <span class="hlt">waves</span> have been known for a long time to be irrelevant in these calculations (and are hence ignored), here we explain how to systematize the procedure in a way that is compatible with the effective field theory expansion.</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/2016EGUGA..1817327S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..1817327S"><span>Determining <span class="hlt">Ocean</span>-Bottom Seismometer Orientations from the RHUM-RUM experiment from P-<span class="hlt">wave</span> and Rayleigh <span class="hlt">wave</span> polarizations</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Scholz, John-Robert; Barruol, Guilhem; Fontaine, Fabrice R.; Sigloch, Karin</p> <p>2016-04-01</p> <p>To image the upper mantle structure beneath La Réunion hotspot, a large-scale seismic network has been deployed on land and at sea in the frame of the RHUM-RUM project (Réunion Hotspot and Upper Mantle - Réunions Unterer Mantel). This French-German passive seismic experiment was designed to investigate and image the deep structure beneath La Réunion, from crust to core, to precise the shape and depth origin of a mantle plume, if any, and to precise the horizontal and vertical mantle flow associated to a possible plume upwelling, to its interaction with the overlying plate and with the neighboring Indian ridges. For this purpose, 57 <span class="hlt">Ocean</span>-Bottom Seismometers (OBS) were installed around La Réunion and along the Central and Southwest Indian ridges. Broad-band instruments were deployed with the French R/V Marion Dufresne in late 2012 (cruise MD192), and recovered 13 months later by the German R/V Meteor (cruise M101). The pool of OBS was complemented by ~60 terrestrial stations, installed on different islands in the western Indian <span class="hlt">Ocean</span>, such as La Réunion, Madagascar, Mauritius, Seychelles, Mayotte and the Îles Éparses in the Mozambique channel. The OBS installation is a free-fall down to the seafloor, where they landed in an unknown orientation. Since seismologic investigations of crustal and upper mantle structure (e.g., receiver functions) and azimuthal anisotropy (e.g., SKS-splitting and Rayleigh <span class="hlt">waves</span>) rely on the knowledge of the correct OBS orientation with respect to the geographic reference frame, it is of importance to determine the orientations of the OBS while recording on the seafloor. In an isotropic, horizontally homogeneous and non-dipping layered globe, the misorientation of each station refers to the offset between theoretical and recorded back-azimuth angle of a passive seismic event. Using large earthquakes (MW > 5.0), it is possible to establish multiple successful measurements per station and thus to determine with good confidence the</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20000110131&hterms=statistics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dstatistics','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20000110131&hterms=statistics&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D90%26Ntt%3Dstatistics"><span>Sea Surface Slope Statistics for Intermediate and Shore Scale <span class="hlt">Ocean</span> <span class="hlt">Waves</span> Measured Using a Low-Altitude Aircraft</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vandemack, Douglas; Crawford, Tim; Dobosy, Ron; Elfouhaily, Tanos; Busalacchi, Antonio J. (Technical Monitor)</p> <p>1999-01-01</p> <p><span class="hlt">Ocean</span> surface remote sensing techniques often rely on scattering or emission linked to shorter- scale gravity-capillary <span class="hlt">ocean</span> wavelets. However, it is increasingly apparent that slightly longer wavelengths of O(10 to 500 cm) are vital components in the robust sea surface description needed to link varied global remote sensing data sets. This paper describes a sensor suite developed to examine sea surface slope variations in the field using an aircraft flying at very low altitude (below 30 m) and will also provide preliminary measurements detailing changes in slope characteristics versus sea state and friction velocity. Two-dimensional surface slope is measured using simultaneous range measurements from three compact short-range laser altimeters mounted in an equilateral triangle arrangement with spacing of about 1 m. In addition, all three lasers provide independent <span class="hlt">wave</span> elevation profiles after GPS-aided correction for aircraft altitude. Laser range precision is 1 cm rms while vertical motion correction is 15 cm rms. The measurements are made along-track at approximately 1 m intervals setting the spatial scale of the measurement to cover <span class="hlt">waves</span> of intermediate to long scale. Products available for this array then include surface elevation, two-dimensional slope distribution, and the cross- and along-track 1-D slope distributions. To complement the laser, a down-looking mm-<span class="hlt">wave</span> radar scatterometer is centered within the laser array to measure radar backscatter simultaneously with the laser slope. The radar's footprint is nominally 1 m in diameter. Near-vertical radar backscatter is inversely proportional to the small-scale surface slope variance and to the tilt of the underlying (laser-measured) surface facet. Together the laser and radar data provide information on <span class="hlt">wave</span> roughness from the longest scales down to about 1 cm. These measurements are complemented by aircraft turbulence probe data that provides robust surface flux information.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017Nanot..28r5403A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017Nanot..28r5403A"><span>Design guidelines of triboelectric nanogenerator for water <span class="hlt">wave</span> energy harvesters</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ahmed, Abdelsalam; Hassan, Islam; Jiang, Tao; Youssef, Khalid; Liu, Lian; Hedaya, Mohammad; Abu Yazid, Taher; Zu, Jean; Wang, Zhong Lin</p> <p>2017-05-01</p> <p><span class="hlt">Ocean</span> <span class="hlt">waves</span> are one of the cleanest and most abundant energy sources on earth, and <span class="hlt">wave</span> energy has the potential for future <span class="hlt">power</span> generation. Triboelectric nanogenerator (TENG) technology has recently been proposed as a promising technology to harvest <span class="hlt">wave</span> energy. In this paper, a theoretical study is performed on a duck-shaped TENG <span class="hlt">wave</span> harvester recently introduced in our work. To enhance the design of the duck-shaped TENG <span class="hlt">wave</span> harvester, the mechanical and electrical characteristics of the harvester’s overall structure, as well as its inner configuration, are analyzed, respectively, under different <span class="hlt">wave</span> conditions, to optimize parameters such as duck radius and mass. Furthermore, a comprehensive hybrid 3D model is introduced to quantify the performance of the TENG <span class="hlt">wave</span> harvester. Finally, the influence of different TENG parameters is validated by comparing the performance of several existing TENG <span class="hlt">wave</span> harvesters. This study can be applied as a guideline for enhancing the performance of TENG <span class="hlt">wave</span> energy harvesters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28397707','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28397707"><span>Design guidelines of triboelectric nanogenerator for water <span class="hlt">wave</span> energy harvesters.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ahmed, Abdelsalam; Hassan, Islam; Jiang, Tao; Youssef, Khalid; Liu, Lian; Hedaya, Mohammad; Yazid, Taher Abu; Zu, Jean; Wang, Zhong Lin</p> <p>2017-05-05</p> <p><span class="hlt">Ocean</span> <span class="hlt">waves</span> are one of the cleanest and most abundant energy sources on earth, and <span class="hlt">wave</span> energy has the potential for future <span class="hlt">power</span> generation. Triboelectric nanogenerator (TENG) technology has recently been proposed as a promising technology to harvest <span class="hlt">wave</span> energy. In this paper, a theoretical study is performed on a duck-shaped TENG <span class="hlt">wave</span> harvester recently introduced in our work. To enhance the design of the duck-shaped TENG <span class="hlt">wave</span> harvester, the mechanical and electrical characteristics of the harvester's overall structure, as well as its inner configuration, are analyzed, respectively, under different <span class="hlt">wave</span> conditions, to optimize parameters such as duck radius and mass. Furthermore, a comprehensive hybrid 3D model is introduced to quantify the performance of the TENG <span class="hlt">wave</span> harvester. Finally, the influence of different TENG parameters is validated by comparing the performance of several existing TENG <span class="hlt">wave</span> harvesters. This study can be applied as a guideline for enhancing the performance of TENG <span class="hlt">wave</span> energy harvesters.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoRL..45.2424C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoRL..45.2424C"><span>Abyssal Upwelling in Mid-<span class="hlt">Ocean</span> Ridge Fracture Zones</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Clément, Louis; Thurnherr, Andreas M.</p> <p>2018-03-01</p> <p>Turbulence in the abyssal <span class="hlt">ocean</span> plays a fundamental role in the climate system by sustaining the deepest branch of the overturning circulation. Over the western flank of the Mid-Atlantic Ridge in the South Atlantic, previously observed bottom-intensified and tidally modulated mixing of abyssal waters appears to imply a counterintuitive densification of deep and bottom waters. Here we show that inside fracture zones, however, turbulence is elevated away from the seafloor because of intensified downward propagating near-inertial <span class="hlt">wave</span> energy, which decays below a subinertial shear maximum. Ray-tracing simulations predict a decay of <span class="hlt">wave</span> energy subsequent to <span class="hlt">wave</span>-mean flow interactions. The hypothesized <span class="hlt">wave</span>-mean flow interactions drive a deep flow toward lighter densities of up to 0.6 Sv over the mid-<span class="hlt">ocean</span> ridge flank in the Brazil Basin, and the same process may also cause upwelling of abyssal waters in other <span class="hlt">ocean</span> basins with mid-<span class="hlt">ocean</span> ridges with fracture zones.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005NCimC..28...33C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005NCimC..28...33C"><span>Langmuir cells and mixing in the upper <span class="hlt">ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Carniel, S.; Sclavo, M.; Kantha, L. H.; Clayson, C. A.</p> <p>2005-01-01</p> <p>The presence of surface gravity <span class="hlt">waves</span> at the <span class="hlt">ocean</span> surface has two important effects on turbulence in the <span class="hlt">oceanic</span> mixed layer (ML): the <span class="hlt">wave</span> breaking and the Langmuir cells (LC). Both these effects act as additional sources of turbulent kinetic energy (TKE) in the <span class="hlt">oceanic</span> ML, and hence are important to mixing in the upper <span class="hlt">ocean</span>. The breaking of high <span class="hlt">wave</span>-number components of the wind <span class="hlt">wave</span> spectrum provides an intense but sporadic source of turbulence in the upper surface; turbulence thus injected diffuses downward, while decaying rapidly, modifying <span class="hlt">oceanic</span> near-surface properties which in turn could affect the air-sea transfer of heat and dissolved gases. LC provide another source of additional turbulence in the water column; they are counter-rotating cells inside the ML, with their axes roughly aligned in the direction of the wind (Langmuir I., Science871938119). These structures are usually made evident by the presence of debris and foam in the convergence area of the cells, and are generated by the interaction of the <span class="hlt">wave</span>-field-induced Stokes drift with the wind-induced shear stress. LC have long been thought to have a substantial influence on mixing in the upper <span class="hlt">ocean</span>, but the difficulty in their parameterization have made ML modelers consistently ignore them in the past. However, recent Large Eddy Simulations (LES) studies suggest that it is possible to include their effect on mixing by simply adding additional production terms in the turbulence equations, thus enabling even 1D models to incorporate LC-driven turbulence. Since LC also modify the Coriolis terms in the mean momentum equations by the addition of a term involving the Stokes drift, their effect on the velocity structure in the ML is also quite significant and could have a major impact on the drift of objects and spilled oil in the upper <span class="hlt">ocean</span>. In this paper we examine the effect of surface gravity <span class="hlt">waves</span> on mixing in the upper <span class="hlt">ocean</span>, focusing on Langmuir circulations, which is by far the dominant</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20000072434','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20000072434"><span>Arctic Climate and Atmospheric Planetary <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>Cavalieri, D. J.; Haekkinen, S.</p> <p>2000-01-01</p> <p>Analysis of a fifty-year record (1946-1995) of monthly-averaged sea level pressure data provides a link between the phases of planetary-scale sea level pressure <span class="hlt">waves</span> and Arctic <span class="hlt">Ocean</span> and ice variability. Results of this analysis show: (1) a breakdown of the dominant <span class="hlt">wave</span> I pattern in the late 1960's, (2) shifts in the mean phase of <span class="hlt">waves</span> 1 and 2 since this breakdown, (3) an eastward shift in the phases of both <span class="hlt">waves</span> 1 and 2 during the years of simulated cyclonic Arctic <span class="hlt">Ocean</span> circulation relative to their phases during the years of anticyclonic circulation, (4) a strong decadal variability of <span class="hlt">wave</span> phase associated with simulated Arctic <span class="hlt">Ocean</span> circulation changes. Finally, the Arctic atmospheric circulation patterns that emerge when <span class="hlt">waves</span> 1 and 2 are in their extreme eastern and western positions suggest an alternative approach to determine significant forcing patterns of sea ice and high-latitude variability.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012APS..DPPGO6012P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012APS..DPPGO6012P"><span>Fast <span class="hlt">wave</span> <span class="hlt">power</span> flow along SOL field lines in NSTX</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Perkins, R. J.; Bell, R. E.; Diallo, A.; Gerhardt, S.; Hosea, J. C.; Jaworski, M. A.; Leblanc, B. P.; Kramer, G. J.; Phillips, C. K.; Roquemore, L.; Taylor, G.; Wilson, J. R.; Ahn, J.-W.; Gray, T. K.; Green, D. L.; McLean, A.; Maingi, R.; Ryan, P. M.; Jaeger, E. F.; Sabbagh, S.</p> <p>2012-10-01</p> <p>On NSTX, a major loss of high-harmonic fast <span class="hlt">wave</span> (HHFW) <span class="hlt">power</span> can occur along open field lines passing in front of the antenna over the width of the scrape-off layer (SOL). Up to 60% of the RF <span class="hlt">power</span> can be lost and at least partially deposited in bright spirals on the divertor floor and ceiling [1,2]. The flow of HHFW <span class="hlt">power</span> from the antenna region to the divertor is mostly aligned along the SOL magnetic field [3], which explains the pattern of heat deposition as measured with infrared (IR) cameras. By tracing field lines from the divertor back to the midplane, the IR data can be used to estimate the profile of HHFW <span class="hlt">power</span> coupled to SOL field lines. We hypothesize that surface <span class="hlt">waves</span> are being excited in the SOL, and these results should benchmark advanced simulations of the RF <span class="hlt">power</span> deposition in the SOL (e.g., [4]). Minimizing this loss is critical optimal high-<span class="hlt">power</span> long-pulse ICRF heating on ITER while guarding against excessive divertor erosion.[4pt] [1] J.C. Hosea et al., AIP Conf Proceedings 1187 (2009) 105. [0pt] [2] G. Taylor et al., Phys. Plasmas 17 (2010) 056114. [0pt] [3] R.J. Perkins et al., to appear in Phys. Rev. Lett. [0pt] [4] D.L. Green et al., Phys. Rev. Lett. 107 (2011) 145001.</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><span class="hlt">Ocean</span> dynamics studies. [of current-<span class="hlt">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 current-<span class="hlt">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 currents; and (3) the interaction of capillary-gravity with the nonuniform currents. <span class="hlt">Wave</span> current interaction was measured and the feasibility of using such measurements for remote sensing of surface currents was considered. A laser probe was developed to measure the surface statistics, and the possibility of using current-<span class="hlt">wave</span> interaction as a means of current measurement was demonstrated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28049299','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28049299"><span>Four-body correlation embedded in antisymmetrized geminal <span class="hlt">power</span> <span class="hlt">wave</span> function.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Kawasaki, Airi; Sugino, Osamu</p> <p>2016-12-28</p> <p>We extend the Coleman's antisymmetrized geminal <span class="hlt">power</span> (AGP) to develop a <span class="hlt">wave</span> function theory that can incorporate up to four-body correlation in a region of strong correlation. To facilitate the variational determination of the <span class="hlt">wave</span> function, the total energy is rewritten in terms of the traces of geminals. This novel trace formula is applied to a simple model system consisting of one dimensional Hubbard ring with a site of strong correlation. Our scheme significantly improves the result obtained by the AGP-configuration interaction scheme of Uemura et al. and also achieves more efficient compression of the degrees of freedom of the <span class="hlt">wave</span> function. We regard the result as a step toward a first-principles <span class="hlt">wave</span> function theory for a strongly correlated point defect or adsorbate embedded in an AGP-based mean-field medium.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JAP...122m3103M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JAP...122m3103M"><span>Theory of energy and <span class="hlt">power</span> flow of plasmonic <span class="hlt">waves</span> on single-walled carbon nanotubes</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moradi, Afshin</p> <p>2017-10-01</p> <p>The energy theorem of electrodynamics is extended so as to apply to the plasmonic <span class="hlt">waves</span> on single-walled carbon nanotubes which propagate parallel to the axial direction of the system and are periodic <span class="hlt">waves</span> in the azimuthal direction. Electronic excitations on the nanotube surface are modeled by an infinitesimally thin layer of free-electron gas which is described by means of the linearized hydrodynamic theory. General expressions of energy and <span class="hlt">power</span> flow associated with surface <span class="hlt">waves</span> are obtained by solving Maxwell and hydrodynamic equations with appropriate boundary conditions. Numerical results for the transverse magnetic mode show that energy, <span class="hlt">power</span> flow, and energy transport velocity of the plasmonic <span class="hlt">waves</span> strongly depend on the nanotube radius in the long-wavelength region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018OptCo.410..830G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018OptCo.410..830G"><span>Aperture averaging and BER for Gaussian beam in underwater <span class="hlt">oceanic</span> turbulence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gökçe, Muhsin Caner; Baykal, Yahya</p> <p>2018-03-01</p> <p>In an underwater wireless optical communication (UWOC) link, <span class="hlt">power</span> fluctuations over finite-sized collecting lens are investigated for a horizontally propagating Gaussian beam <span class="hlt">wave</span>. The <span class="hlt">power</span> scintillation index, also known as the irradiance flux variance, for the received irradiance is evaluated in weak <span class="hlt">oceanic</span> turbulence by using the Rytov method. This lets us further quantify the associated performance indicators, namely, the aperture averaging factor and the average bit-error rate (<BER>). The effects on the UWOC link performance of the <span class="hlt">oceanic</span> turbulence parameters, i.e., the rate of dissipation of kinetic energy per unit mass of fluid, the rate of dissipation of mean-squared temperature, Kolmogorov microscale, the ratio of temperature to salinity contributions to the refractive index spectrum as well as system parameters, i.e., the receiver aperture diameter, Gaussian source size, laser wavelength and the link distance are investigated.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016OcMod.103..118M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016OcMod.103..118M"><span>On the modeling of <span class="hlt">wave</span>-enhanced turbulence nearshore</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Moghimi, Saeed; Thomson, Jim; Özkan-Haller, Tuba; Umlauf, Lars; Zippel, Seth</p> <p>2016-07-01</p> <p>A high resolution k-ω two-equation turbulence closure model, including surface <span class="hlt">wave</span> forcing was employed to fully resolve turbulence dissipation rate profiles close to the <span class="hlt">ocean</span> surface. Model results were compared with observations from Surface <span class="hlt">Wave</span> Instrument Floats with Tracking (SWIFTs) in the nearshore region at New River Inlet, North Carolina USA, in June 2012. A sensitivity analysis for different physical parameters and <span class="hlt">wave</span> and turbulence formulations was performed. The flux of turbulent kinetic energy (TKE) prescribed by <span class="hlt">wave</span> dissipation from a numerical <span class="hlt">wave</span> model was compared with the conventional prescription using the wind friction velocity. A surface roughness length of 0.6 times the significant <span class="hlt">wave</span> height was proposed, and the flux of TKE was applied at a distance below the mean sea surface that is half of this roughness length. The <span class="hlt">wave</span> enhanced layer had a total depth that is almost three times the significant <span class="hlt">wave</span> height. In this layer the non-dimensionalized Terray scaling with <span class="hlt">power</span> of - 1.8 (instead of - 2) was applicable.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMOS43A1400S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMOS43A1400S"><span>Validation of the Fully-Coupled Air-Sea-<span class="hlt">Wave</span> COAMPS System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Smith, T.; Campbell, T. J.; Chen, S.; Gabersek, S.; Tsu, J.; Allard, R. A.</p> <p>2017-12-01</p> <p>A fully-coupled, air-sea-<span class="hlt">wave</span> numerical model, COAMPS®, has been developed by the Naval Research Laboratory to further enhance understanding of <span class="hlt">oceanic</span>, atmospheric, and <span class="hlt">wave</span> interactions. The fully-coupled air-sea-<span class="hlt">wave</span> system consists of an atmospheric component with full physics parameterizations, an <span class="hlt">ocean</span> model, NCOM (Navy Coastal <span class="hlt">Ocean</span> Model), and two <span class="hlt">wave</span> components, SWAN (Simulating <span class="hlt">Waves</span> Nearshore) and <span class="hlt">Wave</span>Watch III. Air-sea interactions between the atmosphere and <span class="hlt">ocean</span> components are accomplished through bulk flux formulations of wind stress and sensible and latent heat fluxes. <span class="hlt">Wave</span> interactions with the <span class="hlt">ocean</span> include the Stokes' drift, surface radiation stresses, and enhancement of the bottom drag coefficient in shallow water due to the <span class="hlt">wave</span> orbital velocities at the bottom. In addition, NCOM surface currents are provided to SWAN and <span class="hlt">Wave</span>Watch III to simulate <span class="hlt">wave</span>-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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014AGUFMOS13A1311M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014AGUFMOS13A1311M"><span>Optimisation Of a Magnetostrictive <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>Mundon, T. R.; Nair, B.</p> <p>2014-12-01</p> <p>Oscilla <span class="hlt">Power</span>, Inc. (OPI) is developing a patented magnetostrictive <span class="hlt">wave</span> energy converter aimed at reducing the cost of grid-scale electricity from <span class="hlt">ocean</span> <span class="hlt">waves</span>. Designed to operate cost-effectively across a wide range of <span class="hlt">wave</span> conditions, this will be the first use of reverse magnetostriction for large-scale energy production. The device architecture is a straightforward two-body, point absorbing system that has been studied at length by various researchers. A large surface float is anchored to a submerged heave (reaction) plate by multiple taut tethers that are largely made up of discrete, robust <span class="hlt">power</span> takeoff modules that house the magnetostrictive generators. The unique generators developed by OPI utilize the phenomenon of reverse magnetostriction, which through the application of load to a specific low cost alloy, can generate significant magnetic flux changes, and thus create <span class="hlt">power</span> through electromagnetic induction. Unlike traditional generators, the mode of operation is low-displacement, high-force, high damping which in combination with the specific multi-tether configuration creates some unique effects and interesting optimization challenges. Using an empirical approach with a combination of numerical tools, such as ORCAFLEX, and physical models, we investigated the properties and sensitivities of this system arrangement, including various heave plate geometries, with the overall goal of identifying the mass and hydrodynamic parameters required for optimum performance. Furthermore, through a detailed physical model test program at the University of New Hampshire, we were able to study in more detail how the heave plate geometry affects the drag and added mass coefficients. In presenting this work we will discuss how alternate geometries could be used to optimize the hydrodynamic parameters of the heave plate, allowing maximum inertial forces in operational conditions, while simultaneously minimizing the forces generated in extreme <span class="hlt">waves</span>. This presentation</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA274651','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA274651"><span>Nonlinear <span class="hlt">Ocean</span> <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>1994-01-06</p> <p>for all of this work is the fact that the Kadomtsev - Petviashvili equation , a1(atu + ui)xU + a.3u) + ay2u = 0, (KP) describes approximately the evolution...the contents of these two papers. (a) Numerically induced chaos The cubic-nonlinear Schrtdinger equation in one dimension, iatA +,2V + 21i,1 =0, (NLS...arises in several physical contexts, including the evolution of nearly monochromatic, one-dimensional <span class="hlt">waves</span> in deep water. The equation is known to be</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMDI51A2659A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMDI51A2659A"><span>Comparison of <span class="hlt">Oceanic</span> and Continental Lithosphere, Asthenosphere, and the LAB Through Shear Velocity Inversion of Rayleigh <span class="hlt">Wave</span> Data from the ALBACORE Amphibious Array in Southern California</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Amodeo, K.; Rathnayaka, S.; Weeraratne, D. S.; Kohler, M. D.</p> <p>2016-12-01</p> <p>Continental and <span class="hlt">oceanic</span> lithosphere, which form in different tectonic environments, are studied in a single amphibious seismic array across the Southern California continental margin. This provides a unique opportunity to directly compare <span class="hlt">oceanic</span> and continental lithosphere, asthenosphere, and the LAB (Lithosphere-Asthenosphere Boundary) in a single data set. The complex history of the region, including spreading center subduction, block rotation, and Borderland extension, allows us to study limits in the rigidity and strength of the lithosphere. We study Rayleigh <span class="hlt">wave</span> phase velocities obtained from the ALBACORE (Asthenospheric and Lithospheric Broadband Architecture from the California Offshore Region Experiment) offshore seismic array project and invert for shear <span class="hlt">wave</span> velocity structure as a function of depth. We divide the study area into several regions: continent, inner Borderland, outer Borderland, and <span class="hlt">oceanic</span> seafloor categorized by age. A unique starting Vs model is used for each case including layer thicknesses, densities, and P and S velocities which predicts Rayleigh phase velocities and are compared to observed phase velocities in each region. We solve for shear <span class="hlt">wave</span> velocities with the best fit between observed and predicted phase velocity data in a least square sense. Preliminary results indicate that lithospheric velocities in the <span class="hlt">oceanic</span> mantle are higher than the continental region by at least 2%. The LAB is observed at 50 ± 20 km beneath 15-35 Ma <span class="hlt">oceanic</span> seafloor. Asthenospheric low velocities reach a minimum of 4.2 km/s in all regions, but have a steeper positive velocity gradient at the base of the <span class="hlt">oceanic</span> asthenosphere compared to the continent. Seismic tomography images in two and three dimensions will be presented from each study region.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2005AGUSMOS41A..04K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2005AGUSMOS41A..04K"><span>Simulation the Effect of Internal <span class="hlt">Wave</span> on the Acoustic Propagation</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Ko, D. S.</p> <p>2005-05-01</p> <p>An acoustic radiation transport model with the Monte Carlo solution has been developed and applied to study the effect of internal <span class="hlt">wave</span> induced random <span class="hlt">oceanic</span> fluctuations on the deep <span class="hlt">ocean</span> acoustic propagation. Refraction in the <span class="hlt">ocean</span> sound channel is performed by means of bi-cubic spline interpolation of discrete deterministic ray paths in the angle(energy)-range-depth coordinates. Scattering by random internal <span class="hlt">wave</span> fluctuations is accomplished by sampling a <span class="hlt">power</span> law scattering kernel applying the rejection method. Results from numerical experiments show that the mean positions of acoustic rays are significantly displaced tending toward the sound channel axis due to the asymmetry of the scattering kernel. The spreading of ray depths and angles about the means depends strongly on frequency. The envelope of the ray displacement spreading is found to be proportional to the square root of range which is different from "3/2 law" found in the non-channel case. Suppression of the spreading is due to the anisotropy of fluctuations and especially due to the presence of sound channel itself.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19930010971','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19930010971"><span>Radar <span class="hlt">Ocean</span> <span class="hlt">Wave</span> Spectrometer (ROWS) preprocessing program (PREROWS2.EXE). User's manual and program description</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Vaughn, Charles R.</p> <p>1993-01-01</p> <p>This Technical Memorandum is a user's manual with additional program documentation for the computer program PREROWS2.EXE. PREROWS2 works with data collected by an <span class="hlt">ocean</span> <span class="hlt">wave</span> spectrometer that uses radar (ROWS) as an active remote sensor. The original ROWS data acquisition subsystem was replaced with a PC in 1990. PREROWS2.EXE is a compiled QuickBasic 4.5 program that unpacks the recorded data, displays various variables, and provides for copying blocks of data from the original 8mm tape to a PC file.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JGRC..123.2172E','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JGRC..123.2172E"><span>Turbulence Scaling Comparisons in the <span class="hlt">Ocean</span> Surface Boundary Layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Esters, L.; Breivik, Ø.; Landwehr, S.; ten Doeschate, A.; Sutherland, G.; Christensen, K. H.; Bidlot, J.-R.; Ward, B.</p> <p>2018-03-01</p> <p>Direct observations of the dissipation rate of turbulent kinetic energy, ɛ, under open <span class="hlt">ocean</span> conditions are limited. Consequently, our understanding of what chiefly controls dissipation in the open <span class="hlt">ocean</span>, and its functional form with depth, is poorly constrained. In this study, we report direct open <span class="hlt">ocean</span> measurements of ɛ from the Air-Sea Interaction Profiler (ASIP) collected during five different cruises in the Atlantic <span class="hlt">Ocean</span>. We then combine these data with <span class="hlt">ocean</span>-atmosphere flux measurements and <span class="hlt">wave</span> information in order to evaluate existing turbulence scaling theories under a diverse set of open <span class="hlt">ocean</span> conditions. Our results do not support the presence of a "breaking" or a "transition layer," which has been previously suggested. Instead, ɛ decays as |z|-1.29 over the depth interval, which was previously defined as "transition layer," and as |z|-1.15 over the mixing layer. This depth dependency does not significantly vary between nonbreaking or breaking <span class="hlt">wave</span> conditions. A scaling relationship based on the friction velocity, the <span class="hlt">wave</span> age, and the significant <span class="hlt">wave</span> height describes the observations best for daytime conditions. For conditions during which convection is important, it is necessary to take buoyancy forcing into account.</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_20");'>20</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li class="active"><span>22</span></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_22 --> <div id="page_23" class="hiddenDiv"> <div class="row"> <div class="col-sm-12"> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li class="active"><span>23</span></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li><a href="#" onclick='return showDiv("page_25");'>25</a></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div> </div> <div class="row"> <div class="col-sm-12"> <ol class="result-class" start="441"> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012EGUGA..14.9562C','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012EGUGA..14.9562C"><span>Variability of ULF <span class="hlt">wave</span> <span class="hlt">power</span> at the magnetopause: a study at low latitude with Cluster data</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Cornilleau-Wehrlin, N.; Grison, B.; Belmont, G.; Rezeau, L.; Chanteur, G.; Robert, P.; Canu, P.</p> <p>2012-04-01</p> <p>Strong ULF <span class="hlt">wave</span> activity has been observed at magnetopause crossings since a long time. Those turbulent-like <span class="hlt">waves</span> are possible contributors to particle penetration from the Solar Wind to the Magnetosphere through the magnetopause. Statistical studies have been performed to understand under which conditions the ULF <span class="hlt">wave</span> <span class="hlt">power</span> is the most intense and thus the <span class="hlt">waves</span> can be the most efficient for particle transport from one region to the other. Clearly the solar wind pressure organizes the data, the stronger the pressure, the higher the ULF <span class="hlt">power</span> (Attié et al 2008). Double STAR-Cluster comparison has shown that ULF <span class="hlt">wave</span> <span class="hlt">power</span> is stronger at low latitude than at high latitude (Cornilleau-Wehrlin et al, 2008). The different studies performed have not, up to now, shown a stronger <span class="hlt">power</span> in the vicinity of local noon. Nevertheless under identical activity conditions, the variability of this <span class="hlt">power</span>, even at a given location in latitude and local time is very high. The present work intends at understanding this variability by means of the multi spacecraft mission Cluster. The data used are from spring 2008, while Cluster was crossing the magnetopause at low latitude, in particularly quite Solar Wind conditions. The first region of interest of this study is the sub-solar point vicinity where the long wavelength surface <span class="hlt">wave</span> effects are most unlikely.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016PhDT.......179A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016PhDT.......179A"><span>Studies of <span class="hlt">oceanic</span>, atmospheric, cryospheric, and fluvial processes through spectral analysis of seismic noise</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Anthony, Robert Ernest</p> <p></p> <p> opportunities and the optimization of deployment strategies for future seismological research in the Polar Regions, and in mountain glacier systems. Chapter 2 details the analysis of 23 years of microseism observations on the Antarctic Peninsula to investigate <span class="hlt">wave</span>-sea ice interactions and assess the influence of the Southern Annular Mode (SAM) on storm activity and <span class="hlt">wave</span> state in the Drake Passage. The lack of landmasses, climatological low pressure, and strong circumpolar westerly winds between latitudes of 50°S to 65°S produce exceptional Southern <span class="hlt">Ocean</span> storm-driven <span class="hlt">wave</span> conditions. This combination makes the Antarctic Peninsula one of Earth's most notable regions of high amplitude <span class="hlt">wave</span> activity and one of the planet's strongest sources of <span class="hlt">ocean</span>-swell driven microseism noise in both the primary (direct <span class="hlt">wave</span>-coastal region interactions) and secondary (direct <span class="hlt">ocean</span> floor forcing due to interacting <span class="hlt">wave</span> trains) period bands. Microseism observations are examined from 1993-2015 from long running seismographs located at Palmer Station (PMSA), on the west coast of the Antarctic Peninsula, and from the sub-Antarctic East Falkland Island (EFI). These records provide a spatially integrative measure of Southern <span class="hlt">Ocean</span> amplitudes and of the degree of coupling between <span class="hlt">ocean</span> <span class="hlt">waves</span> and the solid earth with and without the presence of sea ice (which can reduce <span class="hlt">wave</span> coupling with the continental shelf). A spatiotemporal correlation-based approach illuminates how the distribution of sea ice influences seasonal primary and secondary microseism <span class="hlt">power</span>. I characterize primary and secondary microseism <span class="hlt">power</span> due to variations in sea ice, and find that primary microseism energy is both more sensitive to sea ice and more capable of propagating across <span class="hlt">ocean</span> basins than secondary microseism energy. During positive phases of the SAM, sea ice is reduced in the Bellingshausen Sea and overall storm activity in the Drake Passage increases, resulting in strongly increased microseism <span class="hlt">power</span> levels. The field</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.15703042P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.15703042P"><span>Parametric Instabilities During High <span class="hlt">Power</span> Helicon <span class="hlt">Wave</span> Injection on DIII-D</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Porkolab, M.; Pinsker, R. I.</p> <p>2017-10-01</p> <p>High <span class="hlt">power</span> helicon (whistler) <span class="hlt">waves</span> at a frequency of 0.47 GHz are being considered for efficient off-axis current generation in high performance DIII-D plasmas and in K-Star [3]. The need for deploying helicon <span class="hlt">waves</span> for current profile control has been noted in previous publications since penetration to the core of reactor grade plasmas is easier than with lower hybrid slow <span class="hlt">waves</span> (LHCD) which suffer from accessibility limitations and strong electron Landau absorption in fusion grade high temperature plasmas. In this work we show that under typical experimental conditions in present day tokamaks with 1 MW of RF <span class="hlt">power</span> coupled per antenna, the associated perpendicular electric fields of the order of 40 kV/m can drive strong parametric decay instabilities near the lower hybrid layer. The EXB and polarization drift velocities which are the dominant driver of the PDI can be comparable to the speed of sound in the outer plasma layers, a key measure of driving PDI instabilities. Here we calculate growth rates and convective thresholds for PDIs, and we find that decay <span class="hlt">waves</span> into hot ion lower hybrid <span class="hlt">waves</span> and ion cyclotron quasi modes dominate in the vicinity of the lower hybrid layer, possibly leading to pump depletion. Such instabilities in future reactor grade high temperature plasmas are less likely.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA620038','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA620038"><span>Environmental Hydrocarbon Harvesting for Micro-Scale <span class="hlt">Power</span> Sources using Thermopower <span class="hlt">Waves</span></span></a></p> <p><a target="_blank" href="http://www.dtic.mil/">DTIC Science & Technology</a></p> <p></p> <p>2015-04-06</p> <p>expected by thermoelectricity . The peak specific <span class="hlt">power</span> was found to be as high as 7 kW kg-1. Additionally, an analytical expression governing the...unipolar voltage across the ends of the conduit. Conventional theories of thermoelectricity and Seebeck coefficient are unable to predict the electrical...behavior of thermopower <span class="hlt">wave</span> devices. We studied the differences in these two phenomena of conventional thermoelectricity and thermopower <span class="hlt">waves</span></p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19940033982&hterms=oceans+tide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Doceans%2Btide','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19940033982&hterms=oceans+tide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Doceans%2Btide"><span>Diurnal tides in the Arctic <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kowalik, Z.; Proshutinsky, A. Y.</p> <p>1993-01-01</p> <p>A 2D numerical model with a space grid of about 14 km is applied to calculate diurnal tidal constituents K(1) and O(1) in the Arctic <span class="hlt">Ocean</span>. Calculated corange and cotidal charts show that along the continental slope, local regions of increased sea level amplitude, highly variable phase and enhanced currents occur. It is shown that in these local regions, shelf <span class="hlt">waves</span> (topographic <span class="hlt">waves</span>) of tidal origin are generated. In the Arctic <span class="hlt">Ocean</span> and Northern Atlantic <span class="hlt">Ocean</span> more than 30 regions of enhanced currents are identified. To prove the near-resonant interaction of the diurnal tides with the local bottom topography, the natural periods of oscillations for all regions have been calculated. The flux of energy averaged over the tidal period depicts the gyres of semitrapped energy, suggesting that the shelf <span class="hlt">waves</span> are partially trapped over the irregularities of the bottom topography. It is shown that the occurrence of near-resonance phenomenon changes the energy flow in the tidal <span class="hlt">waves</span>. First, the flux of energy from the astronomical sources is amplified in the shelf <span class="hlt">wave</span> regions, and afterwards the tidal energy is strongly dissipated in the same regions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMSM11G..07B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMSM11G..07B"><span>Plasma Pancakes and Deep Cavities Generated by High <span class="hlt">Power</span> Radio <span class="hlt">Waves</span> from the Arecibo Observatory</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bernhardt, P. A.; Briczinski, S. J., Jr.; Zawdie, K.; Huba, J.; Siefring, C. L.; Sulzer, M. P.; Nossa, E.; Aponte, N.; Perillat, P.; Jackson-Booth, N.</p> <p>2017-12-01</p> <p>Breakdown of the neutral atmosphere at ionospheric altitudes can be achieved with high <span class="hlt">power</span> HF <span class="hlt">waves</span> that reflect on the bottomside of the ionosphere. For overdense heating (i.e., <span class="hlt">wave</span> frequency < maximum plasma frequency in the F-layer), the largest electric fields in the plasma are found just below the reflection altitude. There, electromagnetic <span class="hlt">waves</span> are converted into electron plasma (Langmir) <span class="hlt">waves</span> and ion acoustic <span class="hlt">waves</span>. These <span class="hlt">waves</span> are measured by scattering of the 430 MHz radar at Arecibo to from an enhanced plasma line. The photo-electron excitation of Langmuir <span class="hlt">waves</span> yields a weaker plasma-line profile that shows the complete electron profile with the radar. Once HF enhanced Langmuir <span class="hlt">waves</span> are formed, they can accelerate the photo-electron population to sufficient energies for neutral breakdown and enhanced ionization inside the HF Radio Beam. Plasma pancakes are produced because the breakdown process continues to build up plasma on bottom of the breakdown clouds and recombination occurs on the older breakdown plasma at the top of these clouds. Thus, the plasma pancake falls with altitude from the initial HF <span class="hlt">wave</span> reflection altitude near 250 km to about 160 km where ion-electron recombination prevents the plasma cloud from being sustained by the high <span class="hlt">power</span> HF. Experiments in March 2017 have produced plasma pancakes with about 100 Mega-Watts effective radiated <span class="hlt">power</span> 5.1 MHz with the Arecibo HF Facility. Observations using the 430 MHz radar show falling plasma pancakes that disappear at low altitudes and reform at the F-layer critical reflection altitude. Sometimes the periodic and regular falling motion of the plasma pancakes is influenced by Acoustic Gravity <span class="hlt">Waves</span> (AGW) propagating through the modified HF region. A rising AGW can cause the plasma pancake to reside at nearly constant altitude for 10 to 20 minutes. Dense cavities are also produced by high <span class="hlt">power</span> radio <span class="hlt">waves</span> interacting with the F-Layer. These structures are observed with the Arecibo 430 MHz</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/5901245','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/5901245"><span><span class="hlt">Ocean</span> Thermal Energy Conversion <span class="hlt">power</span> system development. Phase I. Final report</span></a></p> <p><a target="_blank" href="http://www.osti.gov/search">DOE Office of Scientific and Technical Information (OSTI.GOV)</a></p> <p>Not Available</p> <p>1978-12-04</p> <p>This report covers the conceptual and preliminary design of closed-cycle, ammonia, <span class="hlt">ocean</span> thermal energy conversion <span class="hlt">power</span> plants by Westinghouse Electric Corporation. Preliminary designs for evaporator and condenser test articles (0.13 MWe size) and a 10 MWe modular experiment <span class="hlt">power</span> system are described. Conceptual designs for 50 MWe <span class="hlt">power</span> systems, and 100 MWe <span class="hlt">power</span> plants are also descirbed. Design and cost algorithms were developed, and an optimized <span class="hlt">power</span> system design at the 50 MWe size was completed. This design was modeled very closely in the test articles and in the 10 MWe Modular Application. Major component and auxiliary system design, materials,more » biofouling, control response, availability, safety and cost aspects are developed with the greatest emphasis on the 10 MWe Modular Application <span class="hlt">Power</span> System. It is concluded that all <span class="hlt">power</span> plant subsystems are state-of-practice and require design verification only, rather than continued research. A complete test program, which verifies the mechanical reliability as well as thermal performance, is recommended and described.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2014EGUGA..1616134G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2014EGUGA..1616134G"><span>Offshore remote sensing of the <span class="hlt">ocean</span> by stereo vision systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Gallego, Guillermo; Shih, Ping-Chang; Benetazzo, Alvise; Yezzi, Anthony; Fedele, Francesco</p> <p>2014-05-01</p> <p>In recent years, remote sensing imaging systems for the measurement of <span class="hlt">oceanic</span> sea states have attracted renovated attention. Imaging technology is economical, non-invasive and enables a better understanding of the space-time dynamics of <span class="hlt">ocean</span> <span class="hlt">waves</span> over an area rather than at selected point locations of previous monitoring methods (buoys, <span class="hlt">wave</span> gauges, etc.). We present recent progress in space-time measurement of <span class="hlt">ocean</span> <span class="hlt">waves</span> using stereo vision systems on offshore platforms, which focus on sea states with wavelengths in the range of 0.01 m to 1 m. Both traditional disparity-based systems and modern elevation-based ones are presented in a variational optimization framework: the main idea is to pose the stereoscopic reconstruction problem of the surface of the <span class="hlt">ocean</span> in a variational setting and design an energy functional whose minimizer is the desired temporal sequence of <span class="hlt">wave</span> heights. The functional combines photometric observations as well as spatial and temporal smoothness priors. Disparity methods estimate the disparity between images as an intermediate step toward retrieving the depth of the <span class="hlt">waves</span> with respect to the cameras, whereas elevation methods estimate the <span class="hlt">ocean</span> surface displacements directly in 3-D space. Both techniques are used to measure <span class="hlt">ocean</span> <span class="hlt">waves</span> from real data collected at offshore platforms in the Black Sea (Crimean Peninsula, Ukraine) and the Northern Adriatic Sea (Venice coast, Italy). Then, the statistical and spectral properties of the resulting oberved <span class="hlt">waves</span> are analyzed. We show the advantages and disadvantages of the presented stereo vision systems and discuss furure lines of research to improve their performance in critical issues such as the robustness of the camera calibration in spite of undesired variations of the camera parameters or the processing time that it takes to retrieve <span class="hlt">ocean</span> <span class="hlt">wave</span> measurements from the stereo videos, which are very large datasets that need to be processed efficiently to be of practical usage</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFM.C51E..07S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFM.C51E..07S"><span>SPINDLE: A 2-Stage Nuclear-<span class="hlt">Powered</span> Cryobot for <span class="hlt">Ocean</span> World Exploration</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stone, W.; Hogan, B.; Siegel, V. L.; Howe, T.; Howe, S.; Harman, J.; Richmond, K.; Flesher, C.; Clark, E.; Lelievre, S.; Moor, J.; Rothhammer, B.</p> <p>2016-12-01</p> <p>SPINDLE (Sub-glacial Polar Ice Navigation, Descent, and Lake Exploration) is a 2-stage autonomous vehicle system consisting of a robotic ice-penetrating carrier vehicle (cryobot) and a marsupial, hovering autonomous underwater vehicle (HAUV). The cryobot will descend through an ice body into a sub-ice aqueous environment and deploy the HAUV to conduct long range reconnaissance, life search, and sample collection. The HAUV will return to, and auto-dock with, the cryobot at the conclusion of the mission for subsequent data uplink and sample return to the surface. The SPINDLE cryobot has been currently designed for a 1.5 kilometer penetration through a terrestrial ice sheet and the HAUV has been designed for persistent exploration and science presence in for deployments up to a kilometer radius from the cryobot. Importantly, the cryobot is bi-directional and vertically controllable both in an ice sheet as well as following breakthrough into a subglacial water cavity / <span class="hlt">ocean</span>. The vehicle has been designed for long-duration persistent science in subglacial cavities and to allow for subsequent return-to-surface at a much later date or subsequent season. Engineering designs for the current SPINDLE cryobot will be presented in addition to current designs for autonomous rendezvous, docking, and storing of the HAUV system into the cryobot for subsequent recovery of the entire system to the surface. Taken to completion in a three-phase program, SPINDLE will deliver an integrated and field-tested system that will be directly transferable into a Flagship-class mission to either the hypothesized shallow lakes of Europa, the sub-surface <span class="hlt">ocean</span> of Ganymede, or the geyser/plume sources on both Europa and Enceladus. We present the results of several parallel laboratory investigations into advanced <span class="hlt">power</span> transmission systems (laser, high voltage) as well as onboard systems that enable the SPINDLE vehicle to access any subglacial lake on earth while using non-nuclear surrogate, surface</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1435406','SCIGOV-STC'); return false;" href="https://www.osti.gov/servlets/purl/1435406"><span>Water <span class="hlt">Power</span> Technologies Office 2017 Marine Energy Accomplishments</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>Water Power Technologies Office</p> <p></p> <p>The U.S. Department of Energy's Water <span class="hlt">Power</span> Technologies Office's marine and hydrokinetic portfolio has numerous projects that support industry advancement in <span class="hlt">wave</span>, tidal, and <span class="hlt">ocean</span> and river current technologies. In order to strengthen state-of-the-art technologies in these fields and bring them closer to commercialization, the Water <span class="hlt">Power</span> Technologies Office funds industry, academia, and the national laboratories. A U.S. chapter on marine and hydrokinetic energy research and development was included in the <span class="hlt">Ocean</span> Energy Systems' Technology Programme—an intergovernmental collaboration between countries, which operates under a framework established by the International Energy Agency. This brochure is an overview of the U.S. accomplishmentsmore » and updates from that report.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1918465S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1918465S"><span>Mid-Twenty-First-Century Changes in Global <span class="hlt">Wave</span> Energy Flux: Single-Model, Single-Forcing and Single-Scenario Ensemble Projections</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Semedo, Alvaro; Lemos, Gil; Dobrynin, Mikhail; Behrens, Arno; Staneva, Joanna; Miranda, Pedro</p> <p>2017-04-01</p> <p>The knowledge of <span class="hlt">ocean</span> surface <span class="hlt">wave</span> energy fluxes (or <span class="hlt">wave</span> <span class="hlt">power</span>) is of outmost relevance since <span class="hlt">wave</span> <span class="hlt">power</span> has a direct impact in coastal erosion, but also in sediment transport and beach nourishment, and ship, as well as in coastal and offshore infrastructures design. Changes in the global <span class="hlt">wave</span> energy flux pattern can alter significantly the impact of <span class="hlt">waves</span> in continental shelf and coastal areas. Up until recently the impact of climate change in future global <span class="hlt">wave</span> climate had received very little attention. Some single model single scenario global <span class="hlt">wave</span> climate projections, based on CMIP3 scenarios, were pursuit under the auspices of the COWCLIP (coordinated <span class="hlt">ocean</span> <span class="hlt">wave</span> climate projections) project, and received some attention in the IPCC (Intergovernmental Panel for Climate Change) AR5 (fifth assessment report). In the present study the impact of a warmer climate in the near future global <span class="hlt">wave</span> energy flux climate is investigated through a 4-member "coherent" ensemble of <span class="hlt">wave</span> climate projections: single-model, single-forcing, and single-scenario. In this methodology model variability is reduced, leaving only room for the climate change signal. The four ensemble members were produced with the <span class="hlt">wave</span> model WAM, forced with wind speed and ice coverage from EC-Earth projections, following the representative concentration pathway with a high emissions scenario 8.5 (RCP8.5). The ensemble present climate reference period (the control run) has been set for 1976 to 2005. The projected changes in the global <span class="hlt">wave</span> energy flux climate are analyzed for the 2031-2060 period.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ClDy...45..989M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ClDy...45..989M"><span>The <span class="hlt">ocean</span>-atmosphere response to wind-induced thermocline changes in the tropical South Western Indian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Manola, Iris; Selten, F. M.; de Ruijter, W. P. M.; Hazeleger, W.</p> <p>2015-08-01</p> <p>In the Indian <span class="hlt">Ocean</span> basin the sea surface temperatures (SSTs) are most sensitive to changes in the <span class="hlt">oceanic</span> depth of the thermocline in the region of the Seychelles Dome. Observational studies have suggested that the strong SST variations in this region influence the atmospheric evolution around the basin, while its impact could extend far into the Pacific and the extra-tropics. Here we study the adjustments of the coupled atmosphere-<span class="hlt">ocean</span> system to a winter shallow doming event using dedicated ensemble simulations with the state-of-the-art EC-Earth climate model. The doming creates an equatorial Kelvin <span class="hlt">wave</span> and a pair of westward moving Rossby <span class="hlt">waves</span>, leading to higher SST 1-2 months later in the Western equatorial Indian <span class="hlt">Ocean</span>. Atmospheric convection is strengthened and the Walker circulation responds with reduced convection over Indonesia and cooling of the SST in that region. The Pacific warm pool convection shifts eastward and an <span class="hlt">oceanic</span> Kelvin <span class="hlt">wave</span> is triggered at thermocline depth. The <span class="hlt">wave</span> leads to an SST warming in the East Equatorial Pacific 5-6 months after the initiation of the Seychelles Dome event. The atmosphere responds to this warming with weak anomalous atmospheric convection. The changes in the upper tropospheric divergence in this sequence of events create large-scale Rossby <span class="hlt">waves</span> that propagate away from the tropics along the atmospheric waveguides. We suggest to repeat these types of experiments with other models to test the robustness of the results. We also suggest to create the doming event in June so that the East-Pacific warming occurs in November when the atmosphere is most sensitive to SST anomalies and El Niño could possibly be triggered by the doming event under suitable conditions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/21344675-wave-propagation-downstream-high-power-helicon-dipolelike-magnetic-field','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/21344675-wave-propagation-downstream-high-power-helicon-dipolelike-magnetic-field"><span><span class="hlt">Wave</span> propagation downstream of a high <span class="hlt">power</span> helicon in a dipolelike magnetic field</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>Prager, James; Winglee, Robert; Roberson, B. Race</p> <p>2010-01-15</p> <p>The <span class="hlt">wave</span> propagating downstream of a high <span class="hlt">power</span> helicon source in a diverging magnetic field was investigated experimentally. The magnetic field of the <span class="hlt">wave</span> has been measured both axially and radially. The three-dimensional structure of the propagating <span class="hlt">wave</span> is observed and its wavelength and phase velocity are determined. The measurements are compared to predictions from helicon theory and that of a freely propagating whistler <span class="hlt">wave</span>. The implications of this work on the helicon as a thruster are also discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=20090004437&hterms=advanced+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dadvanced%2Bwaves','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=20090004437&hterms=advanced+waves&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dadvanced%2Bwaves"><span>First On-Wafer <span class="hlt">Power</span> Characterization of MMIC Amplifiers at Sub-Millimeter <span class="hlt">Wave</span> Frequencies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Fung, A. K.; Gaier, T.; Samoska, L.; Deal, W. R.; Radisic, V.; Mei, X. B.; Yoshida, W.; Liu, P. S.; Uyeda, J.; Barsky, M.; <a style="text-decoration: none; " href="javascript:void(0); " onClick="displayelement('author_20090004437'); toggleEditAbsImage('author_20090004437_show'); toggleEditAbsImage('author_20090004437_hide'); "> <img style="display:inline; width:12px; height:12px; " src="images/arrow-up.gif" width="12" height="12" border="0" alt="hide" id="author_20090004437_show"> <img style="width:12px; height:12px; display:none; " src="images/arrow-down.gif" width="12" height="12" border="0" alt="hide" id="author_20090004437_hide"></p> <p>2008-01-01</p> <p>Recent developments in semiconductor technology have enabled advanced submillimeter <span class="hlt">wave</span> (300 GHz) transistors and circuits. These new high speed components have required new test methods to be developed for characterizing performance, and to provide data for device modeling to improve designs. Current efforts in progressing high frequency testing have resulted in on-wafer-parameter measurements up to approximately 340 GHz and swept frequency vector network analyzer waveguide measurements to 508 GHz. On-wafer noise figure measurements in the 270-340 GHz band have been demonstrated. In this letter we report on on-wafer <span class="hlt">power</span> measurements at 330 GHz of a three stage amplifier that resulted in a maximum measured output <span class="hlt">power</span> of 1.78mW and maximum gain of 7.1 dB. The method utilized demonstrates the extension of traditional <span class="hlt">power</span> measurement techniques to submillimeter <span class="hlt">wave</span> frequencies, and is suitable for automated testing without packaging for production screening of submillimeter <span class="hlt">wave</span> circuits.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.5172S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.5172S"><span>Regional <span class="hlt">Wave</span> Climates along Eastern Boundary Currents</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Semedo, Alvaro; Soares, Pedro</p> <p>2016-04-01</p> <p>Two types of wind-generated gravity <span class="hlt">waves</span> coexist at the <span class="hlt">ocean</span> surface: wind sea and swell. Wind sea <span class="hlt">waves</span> are <span class="hlt">waves</span> under growing process. These young growing <span class="hlt">waves</span> receive energy from the overlaying wind and are strongly coupled to the local wind field. <span class="hlt">Waves</span> that propagate away from their generation area and no longer receive energy input from the local wind are called swell. Swell <span class="hlt">waves</span> can travel long distances across entire <span class="hlt">ocean</span> basins. A qualitative study of the <span class="hlt">ocean</span> <span class="hlt">waves</span> from a locally vs. remotely generation perspective is important, since the air sea interaction processes is strongly modulated by <span class="hlt">waves</span> and vary accordingly to the prevalence of wind sea or swell <span class="hlt">waves</span> in the area. A detailed climatology of wind sea and swell <span class="hlt">waves</span> 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 <span class="hlt">waves</span>, whereas lower winter wind speeds in these areas, along with stronger winter extratropical storms far away, lead to a predominance of swell <span class="hlt">waves</span> 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 <span class="hlt">waves</span> downwind of capes and points. Hence the spatial patterns of the wind sea or swell regional <span class="hlt">wave</span> fields are shown to be different from the open <span class="hlt">ocean</span> along EBC, due to coastal geometry and fetch dimensions. Swell <span class="hlt">waves</span> will be shown to be considerably more prevalent and to carry more energy in winter along EBC, while in summer locally generated wind sea <span class="hlt">waves</span> are either more comparable to swell <span class="hlt">waves</span> or</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018GeoJI.tmp..199P','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018GeoJI.tmp..199P"><span>Traveltime delay relative to the maximum energy of the <span class="hlt">wave</span> train for dispersive tsunamis propagating across the Pacific <span class="hlt">Ocean</span>: the case of 2010 and 2015 Chilean Tsunamis</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Poupardin, A.; Heinrich, P.; Hébert, H.; Schindelé, F.; Jamelot, A.; Reymond, D.; Sugioka, H.</p> <p>2018-05-01</p> <p>This paper evaluates the importance of frequency dispersion in the propagation of recent trans-Pacific tsunamis. Frequency dispersion induces a time delay for the most energetic <span class="hlt">waves</span>, which increases for long propagation distances and short source dimensions. To calculate this time delay, propagation of tsunamis is simulated and analyzed from spectrograms of time-series at specific gauges in the Pacific <span class="hlt">Ocean</span>. One- and two-dimensional simulations are performed by solving either shallow water or Boussinesq equations and by considering realistic seismic sources. One-dimensional sensitivity tests are first performed in a constant-depth channel to study the influence of the source width. Two-dimensional tests are then performed in a simulated Pacific <span class="hlt">Ocean</span> with a 4000-m constant depth and by considering tectonic sources of 2010 and 2015 Chilean earthquakes. For these sources, both the azimuth and the distance play a major role in the frequency dispersion of tsunamis. Finally, simulations are performed considering the real bathymetry of the Pacific <span class="hlt">Ocean</span>. Multiple reflections, refractions as well as shoaling of <span class="hlt">waves</span> result in much more complex time series for which the effects of the frequency dispersion are hardly discernible. The main point of this study is to evaluate frequency dispersion in terms of traveltime delays by calculating spectrograms for a time window of 6 hours after the arrival of the first <span class="hlt">wave</span>. Results of the spectral analysis show that the <span class="hlt">wave</span> packets recorded by pressure and tide sensors in the Pacific <span class="hlt">Ocean</span> seem to be better reproduced by the Boussinesq model than the shallow water model and approximately follow the theoretical dispersion relationship linking <span class="hlt">wave</span> arrival times and frequencies. Additionally, a traveltime delay is determined above which effects of frequency dispersion are considered to be significant in terms of maximum surface elevations.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2013AGUFM.S51E..02S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2013AGUFM.S51E..02S"><span>Seismic noise frequency dependent P and S <span class="hlt">wave</span> sources</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Stutzmann, E.; Schimmel, M.; Gualtieri, L.; Farra, V.; Ardhuin, F.</p> <p>2013-12-01</p> <p>Seismic noise in the period band 3-10 sec is generated in the <span class="hlt">oceans</span> by the interaction of <span class="hlt">ocean</span> <span class="hlt">waves</span>. Noise signal is dominated by Rayleigh <span class="hlt">waves</span> but body <span class="hlt">waves</span> can be extracted using a beamforming approach. We select the TAPAS array deployed in South Spain between June 2008 and September 2009 and we use the vertical and horizontal components to extract noise P and S <span class="hlt">waves</span>, respectively. Data are filtered in narrow frequency bands and we select beam azimuths and slownesses that correspond to the largest continuous sources per day. Our procedure automatically discard earthquakes which are localized during short time durations. Using this approach, we detect many more noise P-<span class="hlt">waves</span> than S-<span class="hlt">waves</span>. Source locations are determined by back-projecting the detected slowness/azimuth. P and S <span class="hlt">waves</span> are generated in nearby areas and both source locations are frequency dependent. Long period sources are dominantly in the South Atlantic and Indian <span class="hlt">Ocean</span> whereas shorter period sources are rather in the North Atlantic <span class="hlt">Ocean</span>. We further show that the detected S-<span class="hlt">waves</span> are dominantly Sv-<span class="hlt">waves</span>. We model the observed body <span class="hlt">waves</span> using an <span class="hlt">ocean</span> <span class="hlt">wave</span> model that takes into account all possible <span class="hlt">wave</span> interactions including coastal reflection. We use the <span class="hlt">wave</span> model to separate direct and multiply reflected phases for P and S <span class="hlt">waves</span> respectively. We show that in the South Atlantic the complex source pattern can be explained by the existence of both coastal and pelagic sources whereas in the North Atlantic most body <span class="hlt">wave</span> sources are pelagic. For each detected source, we determine the equivalent source magnitude which is compared to the model.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOS.A33A..06D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOS.A33A..06D"><span>-> Air entrainment and bubble statistics in three-dimensional breaking <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>Deike, L.; Popinet, S.; Melville, W. K.</p> <p>2016-02-01</p> <p><span class="hlt">Wave</span> breaking in the <span class="hlt">ocean</span> is of fundamental importance for quantifying <span class="hlt">wave</span> dissipation and air-sea interaction, including gas and momentum exchange, and for improving air-sea flux parametrizations for weather and climate models. Here we investigate air entrainment and bubble statistics in three-dimensional breaking <span class="hlt">waves</span> through direct numerical simulations of the two-phase air-water flow using the Open Source solver Gerris. As in previous 2D simulations, the dissipation due to breaking is found to be in good agreement with previous experimental observations and inertial-scaling arguments. For radii larger than the Hinze scale, the bubble size distribution is found to follow a <span class="hlt">power</span> law of the radius, r-10/3 and to scale linearly with the time dependent turbulent dissipation rate during the active breaking stage. The time-averaged bubble size distribution is found to follow the same <span class="hlt">power</span> law of the radius and to scale linearly with the <span class="hlt">wave</span> dissipation rate per unit length of breaking crest. We propose a phenomenological turbulent bubble break-up model that describes the numerical results and existing experimental results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2600502','PMC'); return false;" href="https://www.pubmedcentral.nih.gov/articlerender.fcgi?tool=pmcentrez&artid=2600502"><span>Low-<span class="hlt">Power</span> Testing of Losses in Millimeter-<span class="hlt">Wave</span> Transmission Lines for High-<span class="hlt">Power</span> Applications</span></a></p> <p><a target="_blank" href="http://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pmc">PubMed Central</a></p> <p>Han, S. T.; Comfoltey, E. N.; Shapiro, M. A.; Sirigiri, J. R.; Tax, D. S.; Temkin, R. J.; Woskov, P. P.; Rasmussen, D. A.</p> <p>2008-01-01</p> <p>We report the measurement of small losses in transmission line (TL) components intended for high-<span class="hlt">power</span> millimeter-<span class="hlt">wave</span> applications. Measurements were made using two different low-<span class="hlt">power</span> techniques: a coherent technique using a vector network analyzer (VNA) and an incoherent technique using a radiometer. The measured loss in a 140 GHz 12.7 mm diameter TL system, consisting of 1.7 m of circular corrugated waveguide and three miter bends, is dominated by the miter bend loss. The measured loss was 0.3±0.1 dB per miter bend using a VNA; and 0.22±0.1 dB per miter bend using a radiometer. Good agreement between the two measurement techniques implies that both are useful for measuring small losses. To verify the methodology, the VNA technique was employed to measure the extremely small transmission loss in a 170 GHz ITER prototype TL system consisting of three lengths of 1 m, 63.5 mm diameter, circular corrugated waveguide and two miter bends. The measured loss of 0.05±0.02 dB per miter bend may be compared with the theoretical loss of 0.027 dB per miter bend. These results suggest that low-<span class="hlt">power</span> testing of TL losses, utilizing a small, simple TL system and a VNA, is a reliable method for evaluating performance of low-loss millimeter-<span class="hlt">wave</span> TL components intended for use in high-<span class="hlt">power</span> applications. PMID:19081774</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EGUGA..1916800R','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EGUGA..1916800R"><span>Impact of <span class="hlt">wave</span> mixing on the sea ice cover</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Rynders, Stefanie; Aksenov, Yevgeny; Madec, Gurvan; Nurser, George; Feltham, Daniel</p> <p>2017-04-01</p> <p>As information on surface <span class="hlt">waves</span> in ice-covered regions becomes available in ice-<span class="hlt">ocean</span> models, there is an opportunity to model <span class="hlt">wave</span>-related processes more accurate. Breaking <span class="hlt">waves</span> cause mixing of the upper water column and present mixing schemes in <span class="hlt">ocean</span> models take this into account through surface roughness. A commonly used approach is to calculate surface roughness from significant <span class="hlt">wave</span> height, parameterised from wind speed. We present results from simulations using modelled significant <span class="hlt">wave</span> height instead, which accounts for the presence of sea ice and the effect of swell. The simulations use the NEMO <span class="hlt">ocean</span> model coupled to the CICE sea ice model, with <span class="hlt">wave</span> information from the ECWAM model of the European Centre for Medium-Range Weather Forecasts (ECMWF). The new <span class="hlt">waves</span>-in-ice module allows <span class="hlt">waves</span> to propagate in sea ice and attenuates <span class="hlt">waves</span> according to multiple scattering and non-elastic losses. It is found that in the simulations with <span class="hlt">wave</span> mixing the mixed layer depth (MLD) under ice cover is reduced, since the parameterisation from wind speed overestimates <span class="hlt">wave</span> height in the ice-covered regions. The MLD change, in turn, affects sea ice concentration and ice thickness. In the Arctic, reduced MLD in winter translates into increased ice thicknesses overall, with higher increases in the Western Arctic and decreases along the Siberian coast. In summer, shallowing of the mixed layer results in more heat accumulating in the surface <span class="hlt">ocean</span>, increasing ice melting. In the Southern <span class="hlt">Ocean</span> the meridional gradient in ice thickness and concentration is increased. We argue that coupling <span class="hlt">waves</span> with sea ice - <span class="hlt">ocean</span> models can reduce negative biases in sea ice cover, affecting the distribution of nutrients and, thus, biological productivity and ecosystems. This coupling will become more important in the future, when <span class="hlt">wave</span> heights in a large part of the Arctic are expected to increase due to sea ice retreat and a larger <span class="hlt">wave</span> fetch. Therefore, <span class="hlt">wave</span> mixing constitutes a possible</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=STS007-05-245&hterms=turbidity+coast&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dturbidity%2Bcoast','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=STS007-05-245&hterms=turbidity+coast&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D20%26Ntt%3Dturbidity%2Bcoast"><span>Internal <span class="hlt">Waves</span>, South China Sea</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p></p> <p>1983-01-01</p> <p>Subsurface <span class="hlt">ocean</span> currents, frequently referred to as internal <span class="hlt">waves</span>, are frequently seen from space under the right lighting conditions when depth penetration can be achieved. These internal <span class="hlt">waves</span> observed in the South China Sea off the SE coast of the island of Hainan (18.5N, 110.5E) visibly demonstrate turbidity in the <span class="hlt">ocean</span>'s depths at the confluence of conflicting currents.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JGRC..122.2012M','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JGRC..122.2012M"><span>Variability of upper-<span class="hlt">ocean</span> characteristics and tropical cyclones in the South West Indian <span class="hlt">Ocean</span></span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Mawren, D.; Reason, C. J. C.</p> <p>2017-03-01</p> <p>Track and intensity are key aspects of tropical cyclone behavior. Intensity may be impacted by the upper-<span class="hlt">ocean</span> heat content relevant for TC intensification (known as Tdy) and barrier layer thickness (BLT). Here the variability of Tdy and BLT in the South West Indian <span class="hlt">Ocean</span> and their relationships with tropical cyclones are investigated. It is shown that rapid cyclone intensification is influenced by large Tdy values, thick barrier layers and the presence of anticyclonic eddies. For TC generation in the South West Indian <span class="hlt">Ocean</span>, the parameter Tdy was found to be important. Large BLT values overlay with large Tdy values during summer. Both fields are modulated by the westward propagation of Rossby <span class="hlt">waves</span>, which are often associated with ENSO. For example, the 1997-1998 El Niño shows a strong signal in Tdy, SST, and BLT over the South West Indian <span class="hlt">Ocean</span>. After this event, an increasing trend in Tdy occurred over most of the basin which may be associated with changes in atmospheric circulation. Increasing SST, <span class="hlt">Power</span> Dissipation Index and frequency of Category 5 tropical cyclones also occurred from 1980 to 2010. To further examine the links between tropical cyclones, Tdy, and BLT, the <span class="hlt">ocean</span> response to Category 5 Tropical Cyclone Bansi that developed near Madagascar during January 2015 was analyzed. Its unusual track was found to be linked with the strengthening of the monsoonal north westerlies while its rapid intensification from Category 2 to Category 4 was linked to a high-Tdy region, associated with a warm core eddy and large BLT.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1826b0024A','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1826b0024A"><span>Design of a quasi-flat linear permanent magnet generator for pico-scale <span class="hlt">wave</span> energy converter in south coast of Yogyakarta, Indonesia</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Azhari, Budi; Prawinnetou, Wassy; Hutama, Dewangga Adhyaksa</p> <p>2017-03-01</p> <p>Indonesia has several potential <span class="hlt">ocean</span> energies to utilize. One of them is tidal <span class="hlt">wave</span> energy, which the potential is about 49 GW. To convert the tidal <span class="hlt">wave</span> energy to electricity, linear permanent magnet generator (LPMG) is considered as the best appliance. In this paper, a pico-scale tidal <span class="hlt">wave</span> <span class="hlt">power</span> converter was designed using quasi-flat LPMG. The generator was meant to be applied in southern coast of Yogyakarta, Indonesia and was expected to generate 1 kW output. First, a quasi-flat LPMG was designed based on the expected output <span class="hlt">power</span> and the <span class="hlt">wave</span> characteristic at the placement site. The design was then simulated using finite element software of FEMM. Finally, the output values were calculated and the output characteristics were analyzed. The results showed that the designed <span class="hlt">power</span> plant was able to produce output <span class="hlt">power</span> of 725.78 Wp for each phase, with electrical efficiency of 64.5%. The output characteristics of the LPMG: output <span class="hlt">power</span> would increase as the average <span class="hlt">wave</span> height or <span class="hlt">wave</span> period increases. Besides, the efficiency would increase if the external load resistance increases. Meanwhile the output <span class="hlt">power</span> of the generator would be maximum at load resistance equals 11 Ω.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19830005505','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19830005505"><span>Further SEASAT SAR coastal <span class="hlt">ocean</span> <span class="hlt">wave</span> analysis</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Kasischke, E. S.; Shuchman, R. A.; Meadows, G. A.; Jackson, P. L.; Tseng, Y.</p> <p>1981-01-01</p> <p>Analysis techniques used to exploit SEASAT synthetic aperture radar (SAR) data of gravity <span class="hlt">waves</span> are discussed and the SEASAT SAR's ability to monitor large scale variations in gravity <span class="hlt">wave</span> fields in both deep and shallow water is evaluated. The SAR analysis techniques investigated included motion compensation adjustments and the semicausal model for spectral analysis of SAR <span class="hlt">wave</span> data. It was determined that spectra generated from fast Fourier transform analysis (FFT) of SAR <span class="hlt">wave</span> data were not significantly altered when either range telerotation adjustments or azimuth focus shifts were used during processing of the SAR signal histories, indicating that SEASAT imagery of gravity <span class="hlt">waves</span> is not significantly improved or degraded by motion compensation adjustments. Evaluation of the semicausal (SC) model using SEASAT SAR data from Rev. 974 indicates that the SC spectral estimates were not significantly better than the FFT results.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19820013596&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dfunction%2Bwave','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19820013596&hterms=function+wave&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D40%26Ntt%3Dfunction%2Bwave"><span>Optimal spatial filtering and transfer function for SAR <span class="hlt">ocean</span> <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>Beal, R. C.; Tilley, D. G.</p> <p>1981-01-01</p> <p>The impulse response of the SAR system is not a delta function and the spectra represent the product of the underlying image spectrum with the transform of the impulse response which must be removed. A digitally computed spectrum of SEASAT imagery of the Atlantic <span class="hlt">Ocean</span> east of Cape Hatteras was smoothed with a 5 x 5 convolution filter and the trend was sampled in a direction normal to the predominant <span class="hlt">wave</span> direction. This yielded a transform of a noise-like process. The smoothed value of this trend is the transform of the impulse response. This trend is fit with either a second- or fourth-order polynomial which is then used to correct the entire spectrum. A 16 x 16 smoothing of the spectrum shows the presence of two distinct swells. Correction of the effects of speckle is effected by the subtraction of a bias from the spectrum.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/biblio/22047044-grating-formation-high-power-radio-wave-near-equator-ionosphere','SCIGOV-STC'); return false;" href="https://www.osti.gov/biblio/22047044-grating-formation-high-power-radio-wave-near-equator-ionosphere"><span>Grating formation by a high <span class="hlt">power</span> radio <span class="hlt">wave</span> in near-equator ionosphere</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>Singh, Rohtash; Sharma, A. K.; Tripathi, V. K.</p> <p>2011-11-15</p> <p>The formation of a volume grating in the near-equator regions of ionosphere due to a high <span class="hlt">power</span> radio <span class="hlt">wave</span> is investigated. The radio <span class="hlt">wave</span>, launched from a ground based transmitter, forms a standing <span class="hlt">wave</span> pattern below the critical layer, heating the electrons in a space periodic manner. The thermal conduction along the magnetic lines of force inhibits the rise in electron temperature, limiting the efficacy of heating to within a latitude of few degrees around the equator. The space periodic electron partial pressure leads to ambipolar diffusion creating a space periodic density ripple with <span class="hlt">wave</span> vector along the vertical. Suchmore » a volume grating is effective to cause strong reflection of radio <span class="hlt">waves</span> at a frequency one order of magnitude higher than the maximum plasma frequency in the ionosphere. Linearly mode converted plasma <span class="hlt">wave</span> could scatter even higher frequency radio <span class="hlt">waves</span>.« less</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUFMNG23A1823S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUFMNG23A1823S"><span>A Coupled Model of Langmuir Circulations and Ramp-like Structures in the Upper <span class="hlt">Ocean</span> Turbulent Boundary Layer</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Soloviev, A.; Dean, C.; Lukas, R.; Donelan, M. A.; Terray, E. A.</p> <p>2016-12-01</p> <p>Surface-<span class="hlt">wave</span> breaking is a <span class="hlt">powerful</span> mechanism producing significant energy flux to small scale turbulence. Most of the turbulent energy produced by breaking <span class="hlt">waves</span> dissipates within one significant <span class="hlt">wave</span> height, while the turbulent diffusion layer extends to approximately ten significant <span class="hlt">wave</span> heights. Notably, the near-surface shear may practically vanish within the <span class="hlt">wave</span>-stirred layer due to small-scale turbulent mixing. The surface <span class="hlt">ocean</span> temperature-salinity structure, circulation, and mass exchanges (including greenhouse gases and pollutants) substantially depend on turbulent mixing and non-local transport in the near-surface layer of the <span class="hlt">ocean</span>. Spatially coherent organized motions have been recognized as an important part of non-local transport. Langmuir circulation (LC) and ramp-like structures are believed to vertically transfer an appreciable portion of the momentum, heat, gases, pollutants (e.g., oil), and other substances in the upper layer of the <span class="hlt">ocean</span>. Free surface significantly complicates the analysis of turbulent exchanges at the air-sea interface and the coherent structures are not yet completely understood. In particular, there is growing observational evidence that in the case of developing seas when the wind direction may not coincide with the direction of the energy containing <span class="hlt">waves</span>, the Langmuir lines are oriented in the wind rather than the <span class="hlt">wave</span> direction. In addition, the vortex force due to Stokes drift in traditional models is altered in the breaking-<span class="hlt">wave</span>-stirred layer. Another complication is that the ramp-like structures in the upper <span class="hlt">ocean</span> turbulent boundary layer have axes perpendicular to the axes of LC. The ramp-like structures are not considered in the traditional model. We have developed a new model, which treats the LC and ramp-like structures in the near-surface layer of the <span class="hlt">ocean</span> as a coupled system. Using computational fluid dynamics tools (LES), we have been able to reproduce both LC and ramp-like structures coexisting in space</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016P%26SS..130...30H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016P%26SS..130...30H"><span>A passive low frequency instrument for radio <span class="hlt">wave</span> sounding the subsurface <span class="hlt">oceans</span> of the Jovian icy moons: An instrument concept</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Hartogh, P.; Ilyushin, Ya. A.</p> <p>2016-10-01</p> <p>Exploration of subsurface <span class="hlt">oceans</span> on Jovian icy moons is a key issue of the icy moons' geology. Electromagnetic <span class="hlt">wave</span> propagation is the only way to probe their icy mantles from the orbit. In the present paper, a principal concept of a passive interferometric instrument for deep sounding of the icy moons' crust is proposed. Its working principle is measuring and correlating Jupiter's radio <span class="hlt">wave</span> emissions with reflections from the deep sub-surface of the icy moons. A number of the functional aspects of the proposed experiment are studied, in particular, impact of the <span class="hlt">wave</span> scattering on the surface terrain on the instrument performance and digital sampling of the noisy signal. Results of the test of the laboratory prototype of the instrument are also presented in the paper.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1418667','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1418667"><span><span class="hlt">Wave</span> Energy Prize - 1/50th Testing - Oscilla <span class="hlt">Power</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Wesley Scharmen</p> <p>2016-01-08</p> <p>This submission of data includes all the 1/50th scale testing data completed on the <span class="hlt">Wave</span> Energy Prize for the Oscilla <span class="hlt">Power</span> team, and includes: 1/50th test data (raw & processed) 1/50th test data video and pictures 1/50th Test plans and testing documents SSTF_Submission (summarized results)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.osti.gov/servlets/purl/1418340','SCIGOV-DOEDE'); return false;" href="https://www.osti.gov/servlets/purl/1418340"><span><span class="hlt">Wave</span> Energy Prize - 1/50th Testing - Principle <span class="hlt">Power</span></span></a></p> <p><a target="_blank" href="http://www.osti.gov/dataexplorer">DOE Data Explorer</a></p> <p>Wesley Scharmen</p> <p>2016-01-08</p> <p>This submission of data includes all the 1/50th scale testing data completed on the <span class="hlt">Wave</span> Energy Prize for the Principle <span class="hlt">Power</span> team, and includes: 1/50th test data (raw & processed) 1/50th test data video and pictures 1/50th Test plans and testing documents SSTF_Submission (summarized results)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/20140017306','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/20140017306"><span>A Novel Multimode Waveguide Coupler for Accurate <span class="hlt">Power</span> Measurement of Traveling <span class="hlt">Wave</span> Tube Harmonic Frequencies</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Wintucky, Edwin G.; Simons, Rainee N.</p> <p>2014-01-01</p> <p>This paper presents the design, fabrication and test results for a novel waveguide multimode directional coupler (MDC). The coupler fabricated from two dissimilar waveguides is capable of isolating the <span class="hlt">power</span> at the second harmonic frequency from the fundamental <span class="hlt">power</span> at the output port of a traveling-<span class="hlt">wave</span> tube (TWT). In addition to accurate <span class="hlt">power</span> measurements at harmonic frequencies, a potential application of the MDC is in the design of a beacon source for atmospheric propagation studies at millimeter-<span class="hlt">wave</span> frequencies.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMGC22B..02Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMGC22B..02Z"><span>A Machine LearningFramework to Forecast <span class="hlt">Wave</span> Conditions</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Y.; James, S. C.; O'Donncha, F.</p> <p>2017-12-01</p> <p>Recently, significant effort has been undertaken to quantify and extract <span class="hlt">wave</span> energy because it is renewable, environmental friendly, abundant, and often close to population centers. However, a major challenge is the ability to accurately and quickly predict energy production, especially across a 48-hour cycle. Accurate forecasting of <span class="hlt">wave</span> conditions is a challenging undertaking that typically involves solving the spectral action-balance equation on a discretized grid with high spatial resolution. The nature of the computations typically demands high-performance computing infrastructure. Using a case-study site at Monterey Bay, California, a machine learning framework was trained to replicate numerically simulated <span class="hlt">wave</span> conditions at a fraction of the typical computational cost. Specifically, the physics-based Simulating <span class="hlt">WAves</span> Nearshore (SWAN) model, driven by measured <span class="hlt">wave</span> conditions, nowcast <span class="hlt">ocean</span> currents, and wind data, was used to generate training data for machine learning algorithms. The model was run between April 1st, 2013 and May 31st, 2017 generating forecasts at three-hour intervals yielding 11,078 distinct model outputs. SWAN-generated fields of 3,104 <span class="hlt">wave</span> heights and a characteristic period could be replicated through simple matrix multiplications using the mapping matrices from machine learning algorithms. In fact, <span class="hlt">wave</span>-height RMSEs from the machine learning algorithms (9 cm) were less than those for the SWAN model-verification exercise where those simulations were compared to buoy <span class="hlt">wave</span> data within the model domain (>40 cm). The validated machine learning approach, which acts as an accurate surrogate for the SWAN model, can now be used to perform real-time forecasts of <span class="hlt">wave</span> conditions for the next 48 hours using available forecasted boundary <span class="hlt">wave</span> conditions, <span class="hlt">ocean</span> currents, and winds. This solution has obvious applications to <span class="hlt">wave</span>-energy generation as accurate <span class="hlt">wave</span> conditions can be forecasted with over a three-order-of-magnitude reduction in</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017EPJWC.14904014T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017EPJWC.14904014T"><span>The gyrotron - a natural source of high-<span class="hlt">power</span> orbital angular momentum millimeter-<span class="hlt">wave</span> beams</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Thumm, M.; Sawant, A.; Choe, M. S.; Choi, E. M.</p> <p>2017-08-01</p> <p>Orbital angular momentum (OAM) of electromagnetic-<span class="hlt">wave</span> beams provides further diversity to multiplexing in wireless communication. The present report shows that higher-order mode gyrotrons are natural sources of high-<span class="hlt">power</span> OAM millimeter (mm) <span class="hlt">wave</span> beams. The well-defined OAM of their rotating cavity modes operating at near cutoff frequency has been derived by photonic and electromagnetic <span class="hlt">wave</span> approaches.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2009JGRC..114.1018Z','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2009JGRC..114.1018Z"><span>On wind-<span class="hlt">wave</span>-current interactions during the Shoaling <span class="hlt">Waves</span> Experiment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Zhang, Fei W.; Drennan, William M.; Haus, Brian K.; Graber, Hans C.</p> <p>2009-01-01</p> <p>This paper presents a case study of wind-<span class="hlt">wave</span>-current interaction during the Shoaling <span class="hlt">Waves</span> Experiment (SHOWEX). Surface current fields off Duck, North Carolina, were measured by a high-frequency <span class="hlt">Ocean</span> Surface Current Radar (OSCR). Wind, wind stress, and directional <span class="hlt">wave</span> 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 <span class="hlt">waves</span> 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 <span class="hlt">ocean</span> surface.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19870066014&hterms=Wave+filter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DWave%2Bfilter','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19870066014&hterms=Wave+filter&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D60%26Ntt%3DWave%2Bfilter"><span>Approximating SIR-B response characteristics and estimating <span class="hlt">wave</span> height and wavelength for <span class="hlt">ocean</span> imagery</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Tilley, David G.</p> <p>1987-01-01</p> <p>NASA Space Shuttle Challenger SIR-B <span class="hlt">ocean</span> scenes are used to derive directional <span class="hlt">wave</span> spectra for which speckle noise is modeled as a function of Rayleigh random phase coherence downrange and Poisson random amplitude errors inherent in the Doppler measurement of along-track position. A Fourier filter that preserves SIR-B image phase relations is used to correct the stationary and dynamic response characteristics of the remote sensor and scene correlator, as well as to subtract an estimate of the speckle noise component. A two-dimensional map of sea surface elevation is obtained after the filtered image is corrected for both random and deterministic motions.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://eric.ed.gov/?q=Thermal+AND+power+AND+plant&pg=2&id=EJ320354','ERIC'); return false;" href="https://eric.ed.gov/?q=Thermal+AND+power+AND+plant&pg=2&id=EJ320354"><span>Unlocking Electric <span class="hlt">Power</span> in the <span class="hlt">Oceans</span>.</span></a></p> <p><a target="_blank" href="http://www.eric.ed.gov/ERICWebPortal/search/extended.jsp?_pageLabel=advanced">ERIC Educational Resources Information Center</a></p> <p>Hurwood, David L.</p> <p>1985-01-01</p> <p>Cruising or stationary <span class="hlt">ocean</span> thermal plants could convert the vast heat energy of the <span class="hlt">ocean</span> into electricity for islands and underdeveloped countries. This approach to energy conservation is described with suggestions for design and outputs of plants. A model project operating in Hawaii is noted. (DH)</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2018JPhD...51k5306W','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018JPhD...51k5306W"><span><span class="hlt">Wave</span> propagation and <span class="hlt">power</span> flow in an acoustic metamaterial plate with lateral local resonance attachment</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Wang, Ting; Sheng, Meiping; Ding, Xiaodong; Yan, Xiaowei</p> <p>2018-03-01</p> <p>This paper presents analysis on <span class="hlt">wave</span> propagation and <span class="hlt">power</span> flow in an acoustic metamaterial plate with lateral local resonance. The metamaterial is designed to have lateral local resonance systems attached to a homogeneous plate. Relevant theoretical analysis, numerical modelling and application prospect are presented. Results show that the metamaterial has two complete band gaps for flexural <span class="hlt">wave</span> absorption and vibration attenuation. Damping can smooth and lower the metamaterial’s frequency responses in high frequency ranges at the expense of the band gap effect, and as an important factor to calculate the <span class="hlt">power</span> flow is thoroughly investigated. Moreover, the effective mass density becomes negative and unbounded at specific frequencies. Simultaneously, <span class="hlt">power</span> flow within band gaps are dramatically blocked from the <span class="hlt">power</span> flow contour and <span class="hlt">power</span> flow maps. Results from finite element modelling and <span class="hlt">power</span> flow analysis reveal the working mechanism of the flexural <span class="hlt">wave</span> attenuation and <span class="hlt">power</span> flow blocked within the band gaps, where part of the flexural vibration is absorbed by the vertical resonator and the rest is transformed through four-link-mechanisms to the lateral resonators that oscillate and generate inertial forces indirectly to counterbalance the shear forces induced by the vibrational plate. The <span class="hlt">power</span> flow is stored in the vertical and lateral local resonance, as well as in the connected plate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012AGUFMOS31F1780V','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012AGUFMOS31F1780V"><span>A Self-<span class="hlt">Powered</span> Fast-Sampling Profiling Float in support of a Mesoscale <span class="hlt">Ocean</span> Observing System in the Western North Pacific</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Valdez, T.; Chao, Y.; Davis, R. E.; Jones, J.</p> <p>2012-12-01</p> <p>This talk will describe a new self-<span class="hlt">powered</span> profiling float that can perform fast sampling over the upper <span class="hlt">ocean</span> for long durations in support of a mesoscale <span class="hlt">ocean</span> observing system in the Western North Pacific. The current state-of-the-art profiling floats can provide several hundreds profiles for the upper <span class="hlt">ocean</span> every ten days. To quantify the role of the upper <span class="hlt">ocean</span> in modulating the development of Typhoons requires at least an order of magnitude reduction for the sampling interval. With today's profiling float and battery technology, a fast sampling of one day or even a few hours will reduce the typical lifetime of profiling floats from years to months. Interactions between the <span class="hlt">ocean</span> and typhoons often involves mesoscale eddies and fronts, which require a dense array of floats to reveal the 3-dimensional structure. To measure the mesoscale <span class="hlt">ocean</span> over a large area like the Western North Pacific therefore requires a new technology that enables fast sampling and long duration at the same time. Harvesting the <span class="hlt">ocean</span> renewable energy associated with the vertical temperature differentials has the potential to <span class="hlt">power</span> profiling floats with fast sampling over long durations. Results from the development and deployment of a prototype self-<span class="hlt">powered</span> profiling float (known as SOLO-TREC) will be presented. With eight hours sampling in the upper 500 meters, the upper <span class="hlt">ocean</span> temperature and salinity reveal pronounced high frequency variations. Plans to use the SOLO-TREC technology in support of a dense array of fast sampling profiling floats in the Western North Pacific will be discussed.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://images.nasa.gov/#/details-PIA15799.html','SCIGOVIMAGE-NASA'); return false;" href="https://images.nasa.gov/#/details-PIA15799.html"><span>NASA Aquarius Maps <span class="hlt">Ocean</span> Salinity Structure</span></a></p> <p><a target="_blank" href="https://images.nasa.gov/">NASA Image and Video Library</a></p> <p></p> <p>2012-06-12</p> <p>NASA Aquarius instrument on the Aquarius/SAC-D observatory gives an unprecedented look at a key factor involved in the formation of an <span class="hlt">oceanic</span> <span class="hlt">wave</span> feature in the tropical Pacific and Atlantic <span class="hlt">Oceans</span> that influences global climate patterns.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AIPC.1892n0001I','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AIPC.1892n0001I"><span><span class="hlt">Power</span> converter for raindrop energy harvesting application: Half-<span class="hlt">wave</span> rectifier</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Izrin, Izhab Muhammad; Dahari, Zuraini</p> <p>2017-10-01</p> <p>Harvesting raindrop energy by capturing vibration from impact of raindrop have been explored extensively. Basically, raindrop energy is generated by converting the kinetic energy of raindrop into electrical energy by using polyvinylidene fluoride (PVDF) piezoelectric. In this paper, a <span class="hlt">power</span> converter using half-<span class="hlt">wave</span> rectifier for raindrop harvesting energy application is designed and proposed to convert damping alternating current (AC) generated by PVDF into direct current (DC). This research presents parameter analysis of raindrop simulation used in the experiment and resistive load effect on half-<span class="hlt">wave</span> rectifier converter. The experiment is conducted by using artificial raindrop from the height of 1.3 m to simulate the effect of different resistive load on the output of half-<span class="hlt">wave</span> rectifier converter. The results of the 0.68 MΩ resistive load showed the best performance of the half-<span class="hlt">wave</span> rectifier converter used in raindrop harvesting energy system, which generated 3.18 Vaverage. The peak instantaneous output generated from this experiment is 15.36 µW.</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/2018E%26ES..140a2031H','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2018E%26ES..140a2031H"><span>Parameter Governing of <span class="hlt">Wave</span> Resonance in Water Chamber and Its Application</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Husain, F.; Alie, M. Z. M.; Rahman, T.</p> <p>2018-04-01</p> <p>It has become known that the oscillating water column (OWC) device is very popular as one of <span class="hlt">wave</span> energy extraction facilities installed in coastal and <span class="hlt">ocean</span> structures. However, it has not been clarified sufficiently how to obtain an effective cross section design of the structure until now. This paper describes theoretical procedure to yield effective cross section of water chamber type of sea wall, which is similar to the OWC type structure in relation to <span class="hlt">wave</span> period or <span class="hlt">wave</span> length. The water chamber type sea wall has a water chamber partitioned by a curtain wall installed in front of part of the structure. This type of sea wall also can be applied to extract <span class="hlt">wave</span> <span class="hlt">power</span> same as of OWC function. When the <span class="hlt">wave</span> conditions on site are known, the dimensions especially the breadth of water chamber type sea wall can be determined.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016EGUGA..18.8196D','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016EGUGA..18.8196D"><span>Integration of WERA <span class="hlt">Ocean</span> Radar into Tsunami Early Warning Systems</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Dzvonkovskaya, Anna; Helzel, Thomas; Kniephoff, Matthias; Petersen, Leif; Weber, Bernd</p> <p>2016-04-01</p> <p>High-frequency (HF) <span class="hlt">ocean</span> radars give a unique capability to deliver simultaneous wide area measurements of <span class="hlt">ocean</span> surface current fields and sea state parameters far beyond the horizon. The WERA® <span class="hlt">ocean</span> radar system is a shore-based remote sensing system to monitor <span class="hlt">ocean</span> surface in near real-time and at all-weather conditions up to 300 km offshore. Tsunami induced surface currents cause increasing orbital velocities comparing to normal oceanographic situation and affect the measured radar spectra. The theoretical approach about tsunami influence on radar spectra showed that a tsunami <span class="hlt">wave</span> train generates a specific unusual pattern in the HF radar spectra. While the tsunami <span class="hlt">wave</span> is approaching the beach, the surface current pattern changes slightly in deep water and significantly in the shelf area as it was shown in theoretical considerations and later proved during the 2011 Japan tsunami. These observed tsunami signatures showed that the velocity of tsunami currents depended on a tsunami <span class="hlt">wave</span> height and bathymetry. The HF <span class="hlt">ocean</span> radar doesn't measure the approaching <span class="hlt">wave</span> height of a tsunami; however, it can resolve the surface current velocity signature, which is generated when tsunami reaches the shelf edge. This strong change of the surface current can be detected by a phased-array WERA system in real-time; thus the WERA <span class="hlt">ocean</span> radar is a valuable tool to support Tsunami Early Warning Systems (TEWS). Based on real tsunami measurements, requirements for the integration of <span class="hlt">ocean</span> radar systems into TEWS are already defined. The requirements include a high range resolution, a narrow beam directivity of phased-array antennas and an accelerated data update mode to provide a possibility of offshore tsunami detection in real-time. The developed software package allows reconstructing an <span class="hlt">ocean</span> surface current map of the area observed by HF radar based on the radar <span class="hlt">power</span> spectrum processing. This fact gives an opportunity to issue an automated tsunami identification message</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.neracoos.org','SCIGOVWS'); return false;" href="http://www.neracoos.org"><span>NERACOOS | weather | <span class="hlt">ocean</span> | marine forecast | <span class="hlt">waves</span> | buoy | marine</span></a></p> <p><a target="_blank" href="http://www.science.gov/aboutsearch.html">Science.gov Websites</a></p> <p></p> <p></p> <p>to address today's highly complex <span class="hlt">ocean</span> and <em>coastal</em> challenges through integrated graduate education Avery Point campus faculty, staff and students carry out cutting-edge research in <em>coastal</em> oceanography <span class="hlt">Ocean</span> Data Products team Regional <em>Coastal</em> Observing Systems: Alaska * Pacific Northwest * Central and</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017JPhCS.941a2106K','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017JPhCS.941a2106K"><span>Cloud-based design of high average <span class="hlt">power</span> traveling <span class="hlt">wave</span> linacs</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Kutsaev, S. V.; Eidelman, Y.; Bruhwiler, D. L.; Moeller, P.; Nagler, R.; Barbe Welzel, J.</p> <p>2017-12-01</p> <p>The design of industrial high average <span class="hlt">power</span> traveling <span class="hlt">wave</span> linacs must accurately consider some specific effects. For example, acceleration of high current beam reduces <span class="hlt">power</span> flow in the accelerating waveguide. Space charge may influence the stability of longitudinal or transverse beam dynamics. Accurate treatment of beam loading is central to the design of high-<span class="hlt">power</span> TW accelerators, and it is especially difficult to model in the meter-scale region where the electrons are nonrelativistic. Currently, there are two types of available codes: tracking codes (e.g. PARMELA or ASTRA) that cannot solve self-consistent problems, and particle-in-cell codes (e.g. Magic 3D or CST Particle Studio) that can model the physics correctly but are very time-consuming and resource-demanding. Hellweg is a special tool for quick and accurate electron dynamics simulation in traveling <span class="hlt">wave</span> accelerating structures. The underlying theory of this software is based on the differential equations of motion. The effects considered in this code include beam loading, space charge forces, and external magnetic fields. We present the current capabilities of the code, provide benchmarking results, and discuss future plans. We also describe the browser-based GUI for executing Hellweg in the cloud.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012Ge%26Ae..52..403S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012Ge%26Ae..52..403S"><span>Spatial structure of the magnetic field induced by an infrasonic <span class="hlt">wave</span> in the <span class="hlt">oceanic</span> waveguide</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Semkin, S. V.; Smagin, V. P.</p> <p>2012-05-01</p> <p>The magnetic field generated by an acoustic <span class="hlt">wave</span> propagating in the <span class="hlt">oceanic</span> waveguide has been considered. The effect of the self-induction factor on the spatial structure of this field has been studied. It has been indicated that there exists a frequency range where it is necessary to take into consideration self-induction. It has been indicated that the induced field is most substantial at frequencies when only the first normal mode exists. The dependences of the induced field on the depth, frequency, and geomagnetic field direction have been obtained and analyzed for this frequency range.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/19659350','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/19659350"><span>Ultralow-<span class="hlt">power</span> four-<span class="hlt">wave</span> mixing with Rb in a hollow-core photonic band-gap fiber.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Londero, Pablo; Venkataraman, Vivek; Bhagwat, Amar R; Slepkov, Aaron D; Gaeta, Alexander L</p> <p>2009-07-24</p> <p>We demonstrate extremely efficient four-<span class="hlt">wave</span> mixing with gains greater than 100 at microwatt pump <span class="hlt">powers</span> and signal-to-idler conversion of 50% in Rb vapor confined to a hollow-core photonic band-gap fiber. We present a theoretical model that demonstrates such efficiency is consistent with the dimensions of the fiber and the optical depths attained. This is, to our knowledge, the largest four-<span class="hlt">wave</span> mixing gain observed at such low total pump <span class="hlt">powers</span> and the first demonstrated example of four-<span class="hlt">wave</span> mixing in an alkali-metal vapor system with a large (approximately 30 MHz) ground state decoherence rate.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2015ConPh..56..359N','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2015ConPh..56..359N"><span><span class="hlt">Wave</span> turbulence</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Nazarenko, Sergey</p> <p>2015-07-01</p> <p><span class="hlt">Wave</span> turbulence is the statistical mechanics of random <span class="hlt">waves</span> with a broadband spectrum interacting via non-linearity. To understand its difference from non-random well-tuned coherent <span class="hlt">waves</span>, one could compare the sound of thunder to a piece of classical music. <span class="hlt">Wave</span> turbulence is surprisingly common and important in a great variety of physical settings, starting with the most familiar <span class="hlt">ocean</span> <span class="hlt">waves</span> to <span class="hlt">waves</span> at quantum scales or to much longer <span class="hlt">waves</span> in astrophysics. We will provide a basic overview of the <span class="hlt">wave</span> turbulence ideas, approaches and main results emphasising the physics of the phenomena and using qualitative descriptions avoiding, whenever possible, involved mathematical derivations. In particular, dimensional analysis will be used for obtaining the key scaling solutions in <span class="hlt">wave</span> turbulence - Kolmogorov-Zakharov (KZ) spectra.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016ChPhB..25f4101T','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016ChPhB..25f4101T"><span>Electromagnetic backscattering from one-dimensional drifting fractal sea surface I: <span class="hlt">Wave</span>-current coupled model</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Tao, Xie; Shang-Zhuo, Zhao; William, Perrie; He, Fang; Wen-Jin, Yu; Yi-Jun, He</p> <p>2016-06-01</p> <p>To study the electromagnetic backscattering from a one-dimensional drifting fractal sea surface, a fractal sea surface <span class="hlt">wave</span>-current model is derived, based on the mechanism of <span class="hlt">wave</span>-current interactions. The numerical results show the effect of the <span class="hlt">ocean</span> current on the <span class="hlt">wave</span>. <span class="hlt">Wave</span> amplitude decreases, wavelength and kurtosis of <span class="hlt">wave</span> height increase, spectrum intensity decreases and shifts towards lower frequencies when the current occurs parallel to the direction of the <span class="hlt">ocean</span> <span class="hlt">wave</span>. By comparison, <span class="hlt">wave</span> amplitude increases, wavelength and kurtosis of <span class="hlt">wave</span> height decrease, spectrum intensity increases and shifts towards higher frequencies if the current is in the opposite direction to the direction of <span class="hlt">ocean</span> <span class="hlt">wave</span>. The <span class="hlt">wave</span>-current interaction effect of the <span class="hlt">ocean</span> current is much stronger than that of the nonlinear <span class="hlt">wave-wave</span> interaction. The kurtosis of the nonlinear fractal <span class="hlt">ocean</span> surface is larger than that of linear fractal <span class="hlt">ocean</span> surface. The effect of the current on skewness of the probability distribution function is negligible. Therefore, the <span class="hlt">ocean</span> <span class="hlt">wave</span> 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.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24084855','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24084855"><span>Detection of cerebral ischemia using the <span class="hlt">power</span> spectrum of the pulse <span class="hlt">wave</span> measured by near-infrared spectroscopy.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Ebihara, Akira; Tanaka, Yuichi; Konno, Takehiko; Kawasaki, Shingo; Fujiwara, Michiyuki; Watanabe, Eiju</p> <p>2013-10-01</p> <p>The diagnosis and medical treatment of cerebral ischemia are becoming more important due to the increase in the prevalence of cerebrovascular disease. However, conventional methods of evaluating cerebral perfusion have several drawbacks: they are invasive, require physical restraint, and the equipment is not portable, which makes repeated measurements at the bedside difficult. An alternative method is developed using near-infrared spectroscopy (NIRS). NIRS signals are measured at 44 positions (22 on each side) on the fronto-temporal areas in 20 patients with cerebral ischemia. In order to extract the pulse-<span class="hlt">wave</span> component, the raw total hemoglobin data recorded from each position are band-pass filtered (0.8 to 2.0 Hz) and subjected to a fast Fourier transform to obtain the <span class="hlt">power</span> spectrum of the pulse <span class="hlt">wave</span>. The ischemic region is determined by single-photon emission computed tomography. The pulse-<span class="hlt">wave</span> <span class="hlt">power</span> in the ischemic region is compared with that in the symmetrical region on the contralateral side. In 17 cases (85%), the pulse-<span class="hlt">wave</span> <span class="hlt">power</span> on the ischemic side is significantly lower than that on the contralateral side, which indicates that the transmission of the pulse <span class="hlt">wave</span> is attenuated in the region with reduced blood flow. Pulse-<span class="hlt">wave</span> <span class="hlt">power</span> might be useful as a noninvasive marker of cerebral ischemia.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2012SPIE.8340E..0CJ','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2012SPIE.8340E..0CJ"><span>Standing <span class="hlt">wave</span> tube electro active polymer <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>Jean, Philippe; Wattez, Ambroise; Ardoise, Guillaume; Melis, C.; Van Kessel, R.; Fourmon, A.; Barrabino, E.; Heemskerk, J.; Queau, J. P.</p> <p>2012-04-01</p> <p>Over the past 4 years SBM has developed a revolutionary <span class="hlt">Wave</span> Energy Converter (WEC): the S3. Floating under the <span class="hlt">ocean</span> surface, the S3 amplifies pressure <span class="hlt">waves</span> similarly to a Ruben's tube. Only made of elastomers, the system is entirely flexible, environmentally friendly and silent. Thanks to a multimodal resonant behavior, the S3 is capable of efficiently harvesting <span class="hlt">wave</span> energy from a wide range of <span class="hlt">wave</span> periods, naturally smoothing the irregularities of <span class="hlt">ocean</span> <span class="hlt">wave</span> amplitudes and periods. In the S3 system, Electro Active Polymer (EAP) generators are distributed along an elastomeric tube over several <span class="hlt">wave</span> lengths, they convert <span class="hlt">wave</span> induced deformations directly into electricity. The output is high voltage multiphase Direct Current with low ripple. Unlike other conventional WECs, the S3 requires no maintenance of moving parts. The conception and operating principle will eventually lead to a reduction of both CAPEX and OPEX. By integrating EAP generators into a small scale S3, SBM achieved a world first: direct conversion of <span class="hlt">wave</span> energy in electricity with a moored flexible submerged EAP WEC in a <span class="hlt">wave</span> tank test. Through an extensive testing program on large scale EAP generators, SBM identified challenges in scaling up to a utility grid device. French Government supports the consortium consisting of SBM, IFREMER and ECN in their efforts to deploy a full scale prototype at the SEMREV test center in France at the horizon 2014-2015. SBM will be seeking strategic as well as financial partners to unleash the true potentials of the S3 Standing <span class="hlt">Wave</span> Tube Electro Active Polymer WEC.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://ntrs.nasa.gov/search.jsp?R=19910068669&hterms=oceans+tide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Doceans%2Btide','NASA-TRS'); return false;" href="https://ntrs.nasa.gov/search.jsp?R=19910068669&hterms=oceans+tide&qs=Ntx%3Dmode%2Bmatchall%26Ntk%3DAll%26N%3D0%26No%3D30%26Ntt%3Doceans%2Btide"><span>Energetics of global <span class="hlt">ocean</span> tides from Geosat altimetry</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Cartwright, David E.; Ray, Richard D.</p> <p>1991-01-01</p> <p>The present paper focuses on resonance and energetics of the daily tides, especially in the southern <span class="hlt">ocean</span>, the distribution of gravitational <span class="hlt">power</span> input of daily and half-daily tides, and comparison with other estimates of global dissipation rates. The present global tidal maps, derived from Geosat altimetry, compare favorably with ground truth data at about the same rms level as the models of Schwiderski (1983), and are slightly better in lunar than in solar tides. Diurnal admittances clearly show Kelvin <span class="hlt">wave</span> structure in the southern <span class="hlt">ocean</span> and confirm the resonant mode of Platzman (1984) at 28.5 + or - 0.1 hr with an apparent Q of about 4. Driving energy is found to enter dominantly in the North Pacific for the daily tides and is strongly peaked in the tropical <span class="hlt">oceans</span> for the half-daily tides. Global rates of working on all major tide constituents except S2 agree well with independent results from analyses of gravity through satellite tracking. Comparison at S2 is improved by allowing for the air tide in gravitational results but suggests deficiencies in all solar tide models.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2017AGUFMEP23A1918B','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2017AGUFMEP23A1918B"><span>The Occurrence of Ridge-and-Runnel Beach Morphology Associated with Deep-Water <span class="hlt">Wave</span> Steepness on New York's <span class="hlt">Ocean</span> Coast</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Bokuniewicz, H.; Fallon, K.</p> <p>2017-12-01</p> <p>The occurrences of ridge-and-runnels were documented along the <span class="hlt">ocean</span> shoreline of New York. These ephemeral beach morphologies represent the post-storm recovery period as sand eroded from the subaerial beach makes its way back on shore. Daily images from a camera in East Hampton, NY (40.964;-72.185) were examined to look for the occurrence and duration of ridge-and-runnel events between October 2010 to November 2012 and again from February 2014 to July 2016. Seventy-five ridge-and-runnel events were seen lasting between one to seven days, and representing about 16% of the time. Deep-water <span class="hlt">wave</span> steepness has long been used as a parameter to determine beach erosion and accretion, because steep <span class="hlt">waves</span> remove sand from the subaerial beach and deposit it as an offshore bar which remains until <span class="hlt">waves</span> of low steepness return it. The time series of <span class="hlt">wave</span> steepness (NOAA Buoy 44017) was found to be dominated by rapid increases to values of about 0.06 followed by gradual decays to about 0.012. <span class="hlt">Wave</span> steepness is positively correlated to wind speed representing the passage of mesoscale weather systems. These cycles occurred about every five days; when ridge-and runnels occurred, they appeared, on average, 2.7 days after the peak in <span class="hlt">wave</span> steepness.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008JGRC..113.5008G','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008JGRC..113.5008G"><span>Formation of undular bores and solitary <span class="hlt">waves</span> in the Strait of Malacca caused by the 26 December 2004 Indian <span class="hlt">Ocean</span> tsunami</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Grue, J.; Pelinovsky, E. N.; Fructus, D.; Talipova, T.; Kharif, C.</p> <p>2008-05-01</p> <p>Deformation of the Indian <span class="hlt">Ocean</span> tsunami moving into the shallow Strait of Malacca and formation of undular bores and solitary <span class="hlt">waves</span> in the strait are simulated in a model study using the fully nonlinear dispersive method (FNDM) and the Korteweg-deVries (KdV) equation. Two different versions of the incoming <span class="hlt">wave</span> are studied where the waveshape is the same but the amplitude is varied: full amplitude and half amplitude. While moving across three shallow bottom ridges, the back face of the leading depression <span class="hlt">wave</span> steepens until the <span class="hlt">wave</span> slope reaches a level of 0.0036-0.0038, when short <span class="hlt">waves</span> form, resembling an undular bore for both full and half amplitude. The group of short <span class="hlt">waves</span> has very small amplitude in the beginning, behaving like a linear dispersive <span class="hlt">wave</span> train, the front moving with the shallow water speed and the tail moving with the linear group velocity. Energy transfer from long to short modes is similar for the two input <span class="hlt">waves</span>, indicating the fundamental role of the bottom topography to the formation of short <span class="hlt">waves</span>. The dominant period becomes about 20 s in both cases. The train of short <span class="hlt">waves</span>, emerging earlier for the larger input <span class="hlt">wave</span> than for the smaller one, eventually develops into a sequence of rank-ordered solitary <span class="hlt">waves</span> moving faster than the leading depression <span class="hlt">wave</span> and resembles a fission of the mother <span class="hlt">wave</span>. The KdV equation has limited capacity in resolving dispersion compared to FNDM.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/24869503','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/24869503"><span>Resting-state slow <span class="hlt">wave</span> <span class="hlt">power</span>, healthy aging and cognitive performance.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Vlahou, Eleni L; Thurm, Franka; Kolassa, Iris-Tatjana; Schlee, Winfried</p> <p>2014-05-29</p> <p>Cognitive functions and spontaneous neural activity show significant changes over the life-span, but the interrelations between age, cognition and resting-state brain oscillations are not well understood. Here, we assessed performance on the Trail Making Test and resting-state magnetoencephalographic (MEG) recordings from 53 healthy adults (18-89 years old) to investigate associations between age-dependent changes in spontaneous oscillatory activity and cognitive performance. Results show that healthy aging is accompanied by a marked and linear decrease of resting-state activity in the slow frequency range (0.5-6.5 Hz). The effects of slow <span class="hlt">wave</span> <span class="hlt">power</span> on cognitive performance were expressed as interactions with age: For older (>54 years), but not younger participants, enhanced delta and theta <span class="hlt">power</span> in temporal and central regions was positively associated with perceptual speed and executive functioning. Consistent with previous work, these findings substantiate further the important role of slow <span class="hlt">wave</span> oscillations in neurocognitive function during healthy aging.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://hdl.handle.net/2060/19780005774','NASA-TRS'); return false;" href="http://hdl.handle.net/2060/19780005774"><span>Minimal-resource computer program for automatic generation of <span class="hlt">ocean</span> <span class="hlt">wave</span> ray or crest diagrams in shoaling waters</span></a></p> <p><a target="_blank" href="http://ntrs.nasa.gov/search.jsp">NASA Technical Reports Server (NTRS)</a></p> <p>Poole, L. R.; Lecroy, S. R.; Morris, W. D.</p> <p>1977-01-01</p> <p>A computer program for studying linear <span class="hlt">ocean</span> <span class="hlt">wave</span> refraction is described. The program features random-access modular bathymetry data storage. Three bottom topography approximation techniques are available in the program which provide varying degrees of bathymetry data smoothing. Refraction diagrams are generated automatically and can be displayed graphically in three forms: Ray patterns with specified uniform deepwater ray density, ray patterns with controlled nearshore ray density, or crest patterns constructed by using a cubic polynomial to approximate crest segments between adjacent rays.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2008AGUFMOS41B1220Y','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2008AGUFMOS41B1220Y"><span>Preliminary Study on Coupling <span class="hlt">Wave</span>-Tide-Storm Surges Prediction System</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>You, S.; Park, S.; Seo, J.; Kim, K.</p> <p>2008-12-01</p> <p>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 <span class="hlt">wave</span> and storm surges are among the most serious threats. To predict more accurate <span class="hlt">wave</span> and storm surge, the development of coupling <span class="hlt">wave</span>-tide-storm surges prediction system is essential. For the time being, <span class="hlt">wave</span> 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 <span class="hlt">waves</span> and recommended further investigations into the effects of <span class="hlt">wave</span>-tide-storm surges interactions and coupling module on <span class="hlt">wave</span> heights. However, tidal height and current give a great effect on the <span class="hlt">wave</span> prediction in the Yellow sea where is very high tide and related research is not enough. At present, KMA has operated the <span class="hlt">wave</span> (RWAM : Regional <span class="hlt">Wave</span> Model) and storm surges/tide prediction system (RTSM : Regional Tide/Storm Surges Model) for <span class="hlt">ocean</span> forecasting. The RWAM is WAVEWATCH III which is a third generation <span class="hlt">wave</span> model developed by Tolman (1989). The RTSM is based on POM (Princeton <span class="hlt">Ocean</span> Model, Blumberg and Mellor, 1987). The RWAM and RTSM cover the northwestern Pacific <span class="hlt">Ocean</span> 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 <span class="hlt">wave</span>-tide-storm surges are incorporated within the frame of KMA <span class="hlt">Ocean</span> prediction system, has been considered as a step forward in respect of <span class="hlt">ocean</span> forecasting. In addition, advanced <span class="hlt">wave</span> prediction model will be applicable to the effect of <span class="hlt">ocean</span> 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</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 <span class="hlt">ocean</span> 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 current 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 model, 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> coupling for a continuously stratified fluid using a fully non-linear 2D numerical model (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: Coupling 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 <span class="hlt">ocean</span>, Cambridge University Press, 336pp.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://adsabs.harvard.edu/abs/2016AGUOSPO21A..04S','NASAADS'); return false;" href="http://adsabs.harvard.edu/abs/2016AGUOSPO21A..04S"><span>Spontaneous <span class="hlt">Wave</span> Generation from Submesoscale Fronts and Filaments</span></a></p> <p><a target="_blank" href="http://adsabs.harvard.edu/abstract_service.html">NASA Astrophysics Data System (ADS)</a></p> <p>Shakespeare, C. J.; Hogg, A.</p> <p>2016-02-01</p> <p>Submesoscale features such as eddies, fronts, jets and filaments can be significant sources of spontaneous <span class="hlt">wave</span> generation at the <span class="hlt">ocean</span> surface. Unlike near-inertial <span class="hlt">waves</span> forced by winds, these spontaneous <span class="hlt">waves</span> are typically of higher frequency and can propagate through the thermocline, whereupon they break and drive mixing in the <span class="hlt">ocean</span> interior. Here we investigate the spontaneous generation, propagation and subsequent breaking of these <span class="hlt">waves</span> using a combination of theory and submesoscale resolving numerical models. The mechanism of generation is nearly identical to that of lee <span class="hlt">waves</span> where flow is deflected over a rigid obstacle on the sea floor. Here, very sharp fronts and filaments of order 100m width moving in the submesoscale surface flow generate "surface lee <span class="hlt">waves</span>" by presenting an obstacle to the surrounding stratified fluid. Using our numerical model we quantify the net downward <span class="hlt">wave</span> energy flux from the surface, and where it is dissipated in the water column. Our results suggest an alternative to the classical paradigm where the energy associated with mixing in the <span class="hlt">ocean</span> interior is sourced from bottom-generated lee <span class="hlt">waves</span>.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('https://www.ncbi.nlm.nih.gov/pubmed/28430520','PUBMED'); return false;" href="https://www.ncbi.nlm.nih.gov/pubmed/28430520"><span>Wind Generated Rogue <span class="hlt">Waves</span> in an Annular <span class="hlt">Wave</span> Flume.</span></a></p> <p><a target="_blank" href="https://www.ncbi.nlm.nih.gov/entrez/query.fcgi?DB=pubmed">PubMed</a></p> <p>Toffoli, A; Proment, D; Salman, H; Monbaliu, J; Frascoli, F; Dafilis, M; Stramignoni, E; Forza, R; Manfrin, M; Onorato, M</p> <p>2017-04-07</p> <p>We investigate experimentally the statistical properties of a wind-generated <span class="hlt">wave</span> field and the spontaneous formation of rogue <span class="hlt">waves</span> in an annular flume. Unlike many experiments on rogue <span class="hlt">waves</span> where <span class="hlt">waves</span> are mechanically generated, here the <span class="hlt">wave</span> field is forced naturally by wind as it is in the <span class="hlt">ocean</span>. What is unique about the present experiment is that the annular geometry of the tank makes <span class="hlt">waves</span> propagating circularly in an unlimited-fetch condition. Within this peculiar framework, we discuss the temporal evolution of the statistical properties of the surface elevation. We show that rogue <span class="hlt">waves</span> and heavy-tail statistics may develop naturally during the growth of the <span class="hlt">waves</span> just before the <span class="hlt">wave</span> height reaches a stationary condition. Our results shed new light on the formation of rogue <span class="hlt">waves</span> in a natural environment.</p> </li> <li> <p><a target="_blank" onclick="trackOutboundLink('http://www.dtic.mil/docs/citations/ADA601190','DTIC-ST'); return false;" href="http://www.dtic.mil/docs/citations/ADA601190"><span>An Arctic Ice/<span class="hlt">Ocean</span> Coupled Model 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>2013-09-30</p> <p>motion in the presence of currents and <span class="hlt">waves</span>. In the <span class="hlt">wave</span> attenuation experiments, between 35 and 80 ‘ice floes’ (0.99 m diameter wooden disks) were...moored with springs to the tank floor and plane <span class="hlt">waves</span> were sent down, with an array of <span class="hlt">wave</span> probes to measure the reflected and transmitted <span class="hlt">waves...waves</span> propagating in the MIZ as opposed to the acoustic <span class="hlt">wave</span> solution shown. This outcome offers significant new capabilities for tracking fully</p> </li> </ol> <div class="pull-right"> <ul class="pagination"> <li><a href="#" onclick='return showDiv("page_1");'>«</a></li> <li><a href="#" onclick='return showDiv("page_21");'>21</a></li> <li><a href="#" onclick='return showDiv("page_22");'>22</a></li> <li><a href="#" onclick='return showDiv("page_23");'>23</a></li> <li><a href="#" onclick='return showDiv("page_24");'>24</a></li> <li class="active"><span>25</span></li> <li><a href="#" onclick='return showDiv("page_25");'>»</a></li> </ul> </div> </div><!-- col-sm-12 --> </div><!-- row --> </div><!-- page_25 --> <div class="footer-extlink text-muted" style="margin-bottom:1rem; text-align:center;">Some links on this page may take you to non-federal websites. Their policies may differ from this site.</div> </div><!-- container --> <footer><a id="backToTop" href="#top"> </a><nav><a id="backToTop" href="#top"> </a><ul class="links"><a id="backToTop" href="#top"> </a><li><a id="backToTop" href="#top"></a><a href="/sitemap.html">Site Map</a></li> <li><a href="/members/index.html">Members Only</a></li> <li><a href="/website-policies.html">Website Policies</a></li> <li><a href="https://doe.responsibledisclosure.com/hc/en-us" target="_blank">Vulnerability Disclosure Program</a></li> <li><a href="/contact.html">Contact Us</a></li> </ul> <div class="small">Science.gov is maintained by the U.S. Department of Energy's <a href="https://www.osti.gov/" target="_blank">Office of Scientific and Technical Information</a>, in partnership with <a href="https://www.cendi.gov/" target="_blank">CENDI</a>.</div> </nav> </footer> <script type="text/javascript"><!-- // var lastDiv = ""; function showDiv(divName) { // hide last div if (lastDiv) { document.getElementById(lastDiv).className = "hiddenDiv"; } //if value of the box is not nothing and an object with that name exists, then change the class if (divName && document.getElementById(divName)) { document.getElementById(divName).className = "visibleDiv"; lastDiv = divName; } } //--> </script> <script> /** * Function that tracks a click on an outbound link in Google Analytics. * This function takes a valid URL string as an argument, and uses that URL string * as the event label. */ var trackOutboundLink = function(url,collectionCode) { try { h = window.open(url); setTimeout(function() { ga('send', 'event', 'topic-page-click-through', collectionCode, url); }, 1000); } catch(err){} }; </script> <!-- Google Analytics --> <script> (function(i,s,o,g,r,a,m){i['GoogleAnalyticsObject']=r;i[r]=i[r]||function(){ (i[r].q=i[r].q||[]).push(arguments)},i[r].l=1*new Date();a=s.createElement(o), m=s.getElementsByTagName(o)[0];a.async=1;a.src=g;m.parentNode.insertBefore(a,m) })(window,document,'script','//www.google-analytics.com/analytics.js','ga'); ga('create', 'UA-1122789-34', 'auto'); ga('send', 'pageview'); </script> <!-- End Google Analytics --> <script> showDiv('page_1') </script> </body> </html>