暂无分享,去创建一个
Emil M. Constantinescu | Robert L. Jacob | Hong Zhang | Shinhoo Kang | R. Jacob | E. Constantinescu | Hong Zhang | Shinhoo Kang
[1] David A. Kopriva,et al. A Conservative Isothermal Wall Boundary Condition for the Compressible Navier–Stokes Equations , 2007, J. Sci. Comput..
[2] Alexandros Syrakos,et al. A critical analysis of some popular methods for the discretisation of the gradient operator in finite volume methods , 2016 .
[3] Carol S. Woodward,et al. Evaluation of Implicit‐Explicit Additive Runge‐Kutta Integrators for the HOMME‐NH Dynamical Core , 2019, Journal of Advances in Modeling Earth Systems.
[4] P. Müller. The Equations of Oceanic Motions , 2006 .
[5] Stuart D. Smith. Coefficients for sea surface wind stress, heat flux, and wind profiles as a function of wind speed and temperature , 1988 .
[6] Pavel B. Bochev,et al. Interface Flux Recovery coupling method for the ocean–atmosphere system , 2020 .
[7] E. F. Bradley,et al. Bulk parameterization of air‐sea fluxes for Tropical Ocean‐Global Atmosphere Coupled‐Ocean Atmosphere Response Experiment , 1996 .
[8] Emil M. Constantinescu,et al. Acceleration of the IMplicit–EXplicit nonhydrostatic unified model of the atmosphere on manycore processors , 2017, Int. J. High Perform. Comput. Appl..
[9] John Thuburn,et al. Some conservation issues for the dynamical cores of NWP and climate models , 2008, J. Comput. Phys..
[10] Jan S. Hesthaven,et al. Application of implicit-explicit high order Runge-Kutta methods to discontinuous-Galerkin schemes , 2007, J. Comput. Phys..
[11] Michael Bader,et al. A High-Order , 2019 .
[12] Steven H. Frankel,et al. Entropy Stable Spectral Collocation Schemes for the Navier-Stokes Equations: Discontinuous Interfaces , 2014, SIAM J. Sci. Comput..
[13] Francis X. Giraldo,et al. High‐order semi‐implicit time‐integrators for a triangular discontinuous Galerkin oceanic shallow water model , 2009 .
[14] Pavel B. Bochev,et al. Explicit synchronous partitioned algorithms for interface problems based on Lagrange multipliers , 2019, Comput. Math. Appl..
[15] Hiroaki Nishikawa,et al. Two Ways to Extend Diffusion Schemes to Navier-Stokes Schemes: Gradient Formula or Upwind Flux , 2011 .
[16] Lorenzo Pareschi,et al. A Unified IMEX Runge-Kutta Approach for Hyperbolic Systems with Multiscale Relaxation , 2017, SIAM J. Numer. Anal..
[17] Florian Lemarié,et al. On the numerical stability of surface–atmosphere coupling in weather and climate models , 2016 .
[18] P. Roe. CHARACTERISTIC-BASED SCHEMES FOR THE EULER EQUATIONS , 1986 .
[19] Emil M. Constantinescu,et al. Extrapolated Implicit-Explicit Time Stepping , 2009, SIAM J. Sci. Comput..
[20] Steven J. Ruuth,et al. Implicit-explicit Runge-Kutta methods for time-dependent partial differential equations , 1997 .
[21] Danna Zhou,et al. d. , 1840, Microbial pathogenesis.
[22] Per-Olof Persson,et al. A high-order discontinuous Galerkin method for fluid-structure interaction with efficient implicit-explicit time stepping , 2014, J. Comput. Phys..
[23] M. Carpenter,et al. Additive Runge-Kutta Schemes for Convection-Diffusion-Reaction Equations , 2003 .
[24] Lorenzo Pareschi,et al. Implicit-explicit runge-kutta schemes and applications to hyperbolic systems with relaxation , 2010, 1009.2757.
[25] G. G. Stokes. "J." , 1890, The New Yale Book of Quotations.
[26] Eric Blayo,et al. Analysis of Ocean-atmosphere Coupling Algorithms: Consistency and Stability , 2017, ICCS.
[27] Nigel Wood,et al. Runge-Kutta IMEX schemes for the Horizontally Explicit/Vertically Implicit (HEVI) solution of wave equations , 2013, J. Comput. Phys..
[28] Francis X. Giraldo,et al. A Conservative Discontinuous Galerkin Semi-Implicit Formulation for the Navier-Stokes Equations in Nonhydrostatic Mesoscale Modeling , 2009, SIAM J. Sci. Comput..
[29] J. Bao,et al. Numerical Simulations of Air-Sea Interaction under High Wind Conditions Using a Coupled Model: A Study of Hurricane Development , 2000 .
[30] Ralf Wolke,et al. Multirate Runge-Kutta schemes for advection equations , 2009 .
[31] S. Valcke,et al. The OASIS3 coupler: a European climate modelling community software , 2012 .
[32] William R. Young,et al. Dynamic Enthalpy, Conservative Temperature, and the Seawater Boussinesq Approximation , 2010 .
[33] William J. Layton,et al. Decoupled Time Stepping Methods for Fluid-Fluid Interaction , 2012, SIAM J. Numer. Anal..
[34] Pierre Gentine,et al. Coupling between the terrestrial carbon and water cycles—a review , 2019, Environmental Research Letters.
[35] Mariana Vertenstein,et al. A new flexible coupler for earth system modeling developed for CCSM4 and CESM1 , 2012, Int. J. High Perform. Comput. Appl..
[36] Dimitri Komatitsch,et al. Some illustrative examples of the use of a spectral-element method in ocean acoustics. , 2012, The Journal of the Acoustical Society of America.
[37] G. Taylor,et al. Mechanism of the production of small eddies from large ones , 1937 .
[38] A. Quarteroni,et al. On the coupling of 3D and 1D Navier-Stokes equations for flow problems in compliant vessels , 2001 .
[39] W. Liu,et al. Bulk Parameterization of Air-Sea Exchanges of Heat and Water Vapor Including the Molecular Constraints at the Interface , 1979 .
[40] W. Washington,et al. An Introduction to Three-Dimensional Climate Modeling , 1986 .
[41] Adrian Sandu. A Class of Multirate Infinitesimal GARK Methods , 2019, SIAM J. Numer. Anal..
[42] Adrian Sandu,et al. Extrapolated Multirate Methods for Differential Equations with Multiple Time Scales , 2013, J. Sci. Comput..
[43] E. Toro. Riemann Solvers and Numerical Methods for Fluid Dynamics , 1997 .
[44] Jean-François Remacle,et al. Multirate time stepping for accelerating explicit discontinuous Galerkin computations with application to geophysical flows , 2013 .
[45] C. Bruneau,et al. The 2D lid-driven cavity problem revisited , 2006 .
[46] Robert Jacob,et al. Stability Analysis of Interface Conditions for Ocean–Atmosphere Coupling , 2019, Journal of Scientific Computing.
[47] Jonas Koko,et al. Operator-splitting and Lagrange multiplier domain decomposition methods for numerical simulation of two coupled Navier-Stokes fluids , 2006 .
[48] C. Deng. CO2 , 2020, ioChem-BD Computational Chemistry Datasets.
[49] Emil M. Constantinescu,et al. Multirate Timestepping Methods for Hyperbolic Conservation Laws , 2007, J. Sci. Comput..
[50] Edgar L. Andreas,et al. Formulation of the Sea Surface Friction Velocity in Terms of the Mean Wind and Bulk Stability , 2015 .
[51] V. Springel. E pur si muove: Galilean-invariant cosmological hydrodynamical simulations on a moving mesh , 2009, 0901.4107.
[52] Emil M. Constantinescu,et al. Semi-Implicit Time Integration of Atmospheric Flows with Characteristic-Based Flux Partitioning , 2015, SIAM J. Sci. Comput..
[53] Jay Walter Larson,et al. M × N Communication and Parallel Interpolation in Community Climate System Model Version 3 Using the Model Coupling Toolkit , 2005, Int. J. High Perform. Comput. Appl..
[54] Carol S. Woodward,et al. Implicit–explicit (IMEX) Runge–Kutta methods for non-hydrostatic atmospheric models , 2017 .
[55] Francis X. Giraldo,et al. IMEX HDG-DG: a coupled implicit hybridized discontinuous Galerkin (HDG) and explicit discontinuous Galerkin (DG) approach for shallow water systems , 2017, J. Comput. Phys..
[56] Emil M. Constantinescu,et al. Implicit-Explicit Formulations of a Three-Dimensional Nonhydrostatic Unified Model of the Atmosphere (NUMA) , 2013, SIAM J. Sci. Comput..