Impact of parameterized lee wave drag on the energy budget of an eddying global ocean model
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S. Jayne | J. Goff | A. Wallcraft | E. Metzger | B. Arbic | S. Garner | D. Trossman | E. J. Metzger | Stephen T. Garner | John A. Goff | E. Metzger
[1] A. Hogg,et al. The energetics of a collapsing meridional overturning circulation , 2013 .
[2] Baylor Fox-Kemper,et al. Can Large Eddy Simulation Techniques Improve Mesoscale Rich Ocean Models , 2013 .
[3] K. Polzin,et al. Internal waves and turbulence in the Antarctic Circumpolar Current , 2013 .
[4] Darran G. Furnival,et al. Global Observations of Ocean-Bottom Subinertial Current Dissipation , 2013 .
[5] Tomohiro Nakamura,et al. Processes of breaking of large‐amplitude unsteady lee waves leading to turbulence , 2013 .
[6] Alistair Adcroft,et al. Routes to energy dissipation for geostrophic flows in the Southern Ocean , 2012, Nature Geoscience.
[7] Carsten Eden,et al. An estimate of Lorenz energy cycle for the world ocean based on the 1/10º STORM/NCEP simulation , 2012 .
[8] C. Eriksen,et al. Dissipation of Turbulent Kinetic Energy Inferred from Seagliders: An Application to the Eastern Nordic Seas Overflows , 2012 .
[9] Andrew J. Watson,et al. Turbulence and diapycnal mixing in Drake Passage , 2012 .
[10] F. Qiao,et al. Comparison between vertical shear mixing and surface wave-induced mixing in the extratropical ocean , 2012 .
[11] A. Wallcraft,et al. An evaluation of the barotropic and internal tides in a high‐resolution global ocean circulation model , 2012 .
[12] C. Wunsch,et al. On the Wind Power Input to the Ocean General Circulation , 2012 .
[13] J. A. Saenz,et al. Mechanical power input from buoyancy and wind to the circulation in an ocean model , 2012 .
[14] E. Kunze,et al. Turbulent Mixing and Exchange with Interior Waters on Sloping Boundaries , 2012 .
[15] Xiaoming Zhai,et al. The Combined Effect of Tidally and Eddy-Driven Diapycnal Mixing on the Large-Scale Ocean Circulation , 2012 .
[16] C. Wright,et al. Bottom dissipation of subinertial currents at the Atlantic zonal boundaries , 2012 .
[17] LuAnne Thompson,et al. Application of Thin-Plate Splines in Two Dimensions to Oceanographic Tracer Data , 2011 .
[18] John A. Goff,et al. Global rate and spectral characteristics of internal gravity wave generation by geostrophic flow over topography , 2011 .
[19] J. Richman,et al. Energetics of a global ocean circulation model compared to observations , 2011 .
[20] W. Dewar,et al. Submesoscale generation by boundaries , 2011 .
[21] Raffaele Ferrari,et al. Global energy conversion rate from geostrophic flows into internal lee waves in the deep ocean , 2011 .
[22] H. Aiki,et al. Maintenance of the mean kinetic energy in the global ocean by the barotropic and baroclinic energy routes: the roles of JEBAR and Ekman dynamics , 2011 .
[23] Zhenya Song,et al. Improvement of MOM4 by including surface wave-induced vertical mixing , 2011 .
[24] John A. Goff,et al. Global prediction of abyssal hill root‐mean‐square heights from small‐scale altimetric gravity variability , 2010 .
[25] R. Tailleux. Entropy versus APE production: On the buoyancy power input in the oceans energy cycle , 2010 .
[26] F. Qiao,et al. Application of wave-induced vertical mixing to the K profile parameterization scheme , 2010 .
[27] J. R. Taylor,et al. Reduction of the usable wind‐work on the general circulation by forced symmetric instability , 2010 .
[28] D. Marshall,et al. Significant sink of ocean-eddy energy near western boundaries , 2010 .
[29] R. Ferrari,et al. Radiation and Dissipation of Internal Waves Generated by Geostrophic Motions Impinging on Small-Scale Topography: Theory , 2010 .
[30] Steven A. Orszag,et al. Large Eddy Simulation of Complex Engineering and Geophysical Flows , 2010 .
[31] E. Joseph Metzger,et al. Concurrent Simulation of the Eddying General Circulation and Tides in a Global Ocean Model , 2010 .
[32] J. Goff,et al. Global prediction of abyssal hill roughness statistics for use in ocean models from digital maps of paleo-spreading rate, paleo-ridge orientation, and sediment thickness , 2010 .
[33] W. Dewar,et al. Topographic inviscid dissipation of balanced flow , 2010 .
[34] R. Ferrari,et al. The distribution of eddy kinetic and potential energies in the global ocean , 2010 .
[35] R. Scott,et al. An update on the wind power input to the surface geostrophic flow of the World Ocean , 2009 .
[36] Ayon Sen,et al. Estimates of bottom flows and bottom boundary layer dissipation of the oceanic general circulation from global high-resolution models , 2009 .
[37] K. Polzin. An abyssal recipe , 2009 .
[38] G. Madec,et al. A conservative leapfrog time stepping method , 2009 .
[39] K. Polzin. Mesoscale Eddy–Internal Wave Coupling. Part I: Symmetry, Wave Capture, and Results from the Mid-Ocean Dynamics Experiment , 2008 .
[40] T. Hibiya,et al. Model-predicted distribution of wind-induced internal wave energy in the world's oceans , 2008 .
[41] D. Marshall,et al. A Conjecture on the Role of Bottom-Enhanced Diapycnal Mixing in the Parameterization of Geostrophic Eddies , 2008 .
[42] Marika M. Holland,et al. Ocean viscosity and climate , 2008 .
[43] Ayon Sen,et al. Global energy dissipation rate of deep‐ocean low‐frequency flows by quadratic bottom boundary layer drag: Computations from current‐meter data , 2008 .
[44] B. Arbic,et al. On quadratic bottom drag, geostrophic turbulence, and oceanic mesoscale eddies , 2008 .
[45] J. McWilliams,et al. Routes to Dissipation in the Ocean : The 2 D / 3 D Turbulence Conundrum , 2007 .
[46] L. S. Laurent,et al. Estimates of Power Consumed by Mixing in the Ocean Interior , 2006 .
[47] A. Thurnherr,et al. Global Abyssal Mixing Inferred from Lowered ADCP Shear and CTD Strain Profiles , 2006 .
[48] S. Wood. Generalized Additive Models: An Introduction with R , 2006 .
[49] R. Slater,et al. The Energetics of Ocean Heat Transport , 2005 .
[50] S. Garner. A Topographic Drag Closure Built on an Analytical Base Flux , 2005 .
[51] H. Hurlburt,et al. Convergence of Laplacian diffusion versus resolution of an ocean model , 2005 .
[52] R. Hallberg. A thermobaric instability of Lagrangian vertical coordinate ocean models , 2005 .
[53] R. Hallberg,et al. The accuracy of surface elevations in forward global barotropic and baroclinic tide models , 2004 .
[54] G. Flierl,et al. Baroclinically Unstable Geostrophic Turbulence in the Limits of Strong and Weak Bottom Ekman Friction: Application to Midocean Eddies , 2004 .
[55] Stephen M. Griffies,et al. Fundamentals of Ocean Climate Models , 2004 .
[56] Wei Wang,et al. Wind Energy Input to the Surface Waves , 2004 .
[57] Gary D. Egbert,et al. Numerical modeling of the global semidiurnal tide in the present day and in the last glacial maximum , 2004 .
[58] J. Pedlosky,et al. Wind-driven barotropic gyre I : circulation control by eddy vorticity fluxes to an enhanced removal region , 2004 .
[59] M. Visbeck,et al. Widespread Intense Turbulent Mixing in the Southern Ocean , 2004, Science.
[60] Carl Wunsch,et al. VERTICAL MIXING, ENERGY, AND THE GENERAL CIRCULATION OF THE OCEANS , 2004 .
[61] G. Halliwell,et al. Evaluation of vertical coordinate and vertical mixing algorithms in the HYbrid-Coordinate Ocean Model (HYCOM) , 2004 .
[62] Eric P. Chassignet,et al. North Atlantic Simulations with the Hybrid Coordinate Ocean Model (HYCOM): Impact of the Vertical Coordinate Choice, Reference Pressure, and Thermobaricity , 2003 .
[63] M. Alford,et al. Improved global maps and 54‐year history of wind‐work on ocean inertial motions , 2003 .
[64] L. St. Laurent,et al. Estimating tidally driven mixing in the deep ocean , 2002 .
[65] Toshiyuki Hibiya,et al. Global estimates of the wind‐induced energy flux to inertial motions in the surface mixed layer , 2002 .
[66] Melinda S. Peng,et al. Navy Operational Global Atmospheric Prediction System (NOGAPS): Forcing for Ocean Models , 2002 .
[67] Rainer Bleck,et al. An oceanic general circulation model framed in hybrid isopycnic-Cartesian coordinates , 2002 .
[68] J. Toole,et al. Buoyancy Forcing by Turbulence above Rough Topography in the Abyssal Brazil Basin , 2001 .
[69] L. St. Laurent,et al. Parameterizing tidal dissipation over rough topography , 2001 .
[70] D. Webb,et al. Oceanography: Vertical mixing in the ocean , 2001, Nature.
[71] Jean-Marc Molines,et al. Circulation characteristics in three eddy-permitting models of the North Atlantic , 2001 .
[72] J. Toole,et al. Evidence for enhanced mixing over rough topography in the abyssal ocean , 2000, Nature.
[73] C. E. Neuzil,et al. Osmotic generation of ‘anomalous’ fluid pressures in geological environments , 2000, Nature.
[74] H. Hasumi,et al. Developments in ocean climate modelling , 2000 .
[75] John K. Dukowicz,et al. Inclusion of Thermobaricity in Isopycnic-Coordinate Ocean Models , 1999 .
[76] W. Munk,et al. Abyssal recipes II: energetics of tidal and wind mixing , 1998 .
[77] Carl Wunsch,et al. The Work Done by the Wind on the Oceanic General Circulation , 1998 .
[78] J. M. Toole,et al. Spatial Variability of Turbulent Mixing in the Abyssal Ocean , 1997, Science.
[79] Ross J. Murray,et al. Explicit Generation of Orthogonal Grids for Ocean Models , 1996 .
[80] Eric A. D'Asaro,et al. Available potential energy and mixing in density-stratified fluids , 1995, Journal of Fluid Mechanics.
[81] W. Large,et al. Oceanic vertical mixing: a review and a model with a nonlocal boundary layer parameterization , 1994 .
[82] L. A. Anderson,et al. Estimates of the energy cycle of the oceans , 1994 .
[83] A. Treguier. Kinetic Energy Analysis of an Eddy Resolving, Primitive Equation Model of the North Atlantic , 1992 .
[84] Thomas H. Jordan,et al. Stochastic Modeling of Seafloor Morphology: Inversion of Sea Beam Data for Second-Order Statistics , 1988 .
[85] T. H. Bell,et al. Topographically generated internal waves in the open ocean , 1975 .
[86] G. Taylor. Tidal Friction in the Irish Sea , 1919 .