Lateral Mixing in the Eddying Regime and a New Broad‐Ranging Formulation
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Beth A. Wingate | Mark R. Petersen | Mathew E. Maltrud | Elizabeth C. Hunke | M. Maltrud | E. Hunke | M. Hecht | M. Petersen | B. Wingate | Matthew W. Hecht
[1] P. Gent,et al. Isopycnal mixing in ocean circulation models , 1990 .
[2] Eric P. Chassignet,et al. Impact of wind forcing, bottom topography, and inertia on midlatitude jet separation in a quasigeostrophic model , 1997 .
[3] M. Maltrud,et al. Numerical simulation of the North Atlantic Ocean at 1/10 degrees , 2000 .
[4] Darryl D. Holm,et al. Implementation of the LANS-α turbulence model in a primitive equation ocean model , 2008, J. Comput. Phys..
[5] Darryl D. Holm. Averaged Lagrangians and the mean effects of fluctuations in ideal fluid dynamics , 2001 .
[6] M. Maltrud,et al. An eddy resolving global 1/10° ocean simulation , 2005 .
[7] Beth A. Wingate,et al. Efficient form of the LANS-α turbulence model in a primitive-equation ocean model , 2008, J. Comput. Phys..
[8] É. Deleersnijder,et al. Overshootings and spurious oscillations caused by biharmonic mixing , 2007 .
[9] A. Adcroft,et al. Representation of Topography by Shaved Cells in a Height Coordinate Ocean Model , 1997 .
[10] A. Nurser,et al. Spurious diapycnal mixing of the deep waters in an eddy-permitting global ocean model , 2002 .
[11] Richard J. Greatbatch,et al. A Diagnosis of Thickness Fluxes in an Eddy-Resolving Model , 2007 .
[12] P. Gent,et al. Anisotropic GM Parameterization for Ocean Models , 2004 .
[13] Darryl D. Holm,et al. Navier-Stokes-alpha model: LES equations with nonlinear dispersion , 2001, nlin/0103036.
[14] W. R. Holland,et al. Application of a Third-Order Upwind Scheme in the NCAR Ocean Model* , 1998 .
[15] T. Rossby. The North Atlantic Current and surrounding waters: At the crossroads , 1996 .
[16] Philip J. Rasch,et al. Upwind‐weighted advection schemes for ocean tracer transport: An evaluation in a passive tracer context , 1995 .
[17] Darryl D. Holm,et al. Baroclinic Instabilities of the Two-Layer Quasigeostrophic Alpha Model , 2005 .
[18] Darryl D. Holm,et al. The Navier–Stokes-alpha model of fluid turbulence , 2001, nlin/0103037.
[19] Y. Mintz,et al. Numerical simulation of the Gulf Stream and Mid-Ocean eddies , 1977 .
[20] Stephen M. Griffies,et al. Fundamentals of Ocean Climate Models , 2004 .
[21] Patrick J. Hogan,et al. Impact of 1/8° to 1/64° resolution on Gulf Stream model–data comparisons in basin-scale subtropical Atlantic Ocean models , 2000 .
[22] Darryl D. Holm,et al. Implementation of the LANS-alpha turbulence model in a primitive equation ocean model , 2007 .
[23] Jerrold E. Marsden,et al. EULER-POINCARE MODELS OF IDEAL FLUIDS WITH NONLINEAR DISPERSION , 1998 .
[24] Darryl D. Holm. Fluctuation effects on 3D Lagrangian mean and Eulerian mean fluid motion , 1999, chao-dyn/9903034.
[25] Darryl D. Holm,et al. Modeling Mesoscale Turbulence in the Barotropic Double-Gyre Circulation , 2003 .
[26] Rainer Bleck,et al. An oceanic general circulation model framed in hybrid isopycnic-Cartesian coordinates , 2002 .
[27] M. Maltrud,et al. On the grid dependence of lateral mixing parameterizations for global ocean simulations , 2008 .
[28] Robert Hallberg,et al. The Role of Eddies in Determining the Structure and Response of the Wind-Driven Southern Hemisphere Overturning: Results from the Modeling Eddies in the Southern Ocean (MESO) Project , 2006 .
[29] D. G. Andrews,et al. An exact theory of nonlinear waves on a Lagrangian-mean flow , 1978, Journal of Fluid Mechanics.
[30] David P. Marshall,et al. Do We Require Adiabatic Dissipation Schemes in Eddy-Resolving Ocean Models? , 1998 .
[31] Darryl D. Holm,et al. Direct numerical simulations of the Navier–Stokes alpha model , 1999, Physica D: Nonlinear Phenomena.
[32] James C. McWilliams,et al. Anisotropic horizontal viscosity for ocean models , 2003 .
[33] Beth A. Wingate. The Maximum Allowable Time Step for the Shallow Water α Model and Its Relation to Time-Implicit Differencing , 2004 .
[34] F. Bryan,et al. Climate impacts of systematic errors in the simulation of the path of the North Atlantic Current , 2006 .
[35] Stephen M. Griffies,et al. Biharmonic Friction with a Smagorinsky-Like Viscosity for Use in Large-Scale Eddy-Permitting Ocean Models , 2000 .
[36] Walter Munk,et al. ON THE WIND-DRIVEN OCEAN CIRCULATION , 1950 .
[37] Stephen M. Griffies,et al. Spurious Diapycnal Mixing Associated with Advection in a z-Coordinate Ocean Model , 2000 .
[38] Frank O. Bryan,et al. Resolution convergence and sensitivity studies with North Atlantic circulation models. Part I: The western boundary current system , 2007 .
[39] Richard Smith,et al. Toward a Physical Understanding of the North Atlantic: A Review of Model Studies in an Eddying Regime , 2013 .
[40] Darryl D. Holm,et al. Camassa-Holm Equations as a Closure Model for Turbulent Channel and Pipe Flow , 1998, chao-dyn/9804026.
[41] Darryl D. Holm,et al. Regularization modeling for large-eddy simulation , 2002, nlin/0206026.
[42] Willem Hundsdorfer,et al. Method of lines and direct discretization: a comparison for linear advection , 1994 .
[43] Darryl D. Holm,et al. The Camassa-Holm equations and turbulence , 1999 .