Review on development of a scalable high-order nonhydrostatic multi-moment constrained finite volume dynamical core.
暂无分享,去创建一个
Chungang Chen | Feng Xiao | Xingliang Li | Xueshun Shen | Chungang Chen | F. Xiao | Xingliang Li | Xueshun Shen
[1] P. Roe. Approximate Riemann Solvers, Parameter Vectors, and Difference Schemes , 1997 .
[2] Brian J. Hoskins,et al. Stability of the Rossby-Haurwitz wave , 1973 .
[3] Feng Xiao,et al. CIP/multi-moment finite volume method for Euler equations: A semi-Lagrangian characteristic formulation , 2007, J. Comput. Phys..
[4] Akio Arakawa,et al. Integration of the Nondivergent Barotropic Vorticity Equation with AN Icosahedral-Hexagonal Grid for the SPHERE1 , 1968 .
[6] Xingliang Li,et al. A multi-moment transport model on cubed-sphere grid , 2011 .
[7] Colin J. Cotter,et al. Mixed finite elements for numerical weather prediction , 2011, J. Comput. Phys..
[8] William C. Skamarock,et al. A unified approach to energy conservation and potential vorticity dynamics for arbitrarily-structured C-grids , 2010, J. Comput. Phys..
[9] Mark A. Taylor,et al. The Spectral Element Atmosphere Model (SEAM): High-Resolution Parallel Computation and Localized Resolution of Regional Dynamics , 2004 .
[10] Yong Li,et al. Numerical simulations of Rossby–Haurwitz waves , 2000 .
[11] Feng Xiao,et al. A high‐order multi‐moment constrained finite‐volume global shallow‐water model on the Yin‐Yang grid , 2015 .
[12] Sang Hun Park,et al. Idealized global nonhydrostatic atmospheric test cases on a reduced‐radius sphere , 2015 .
[13] Colin J. Cotter,et al. A finite element exterior calculus framework for the rotating shallow-water equations , 2012, J. Comput. Phys..
[15] William C. Skamarock,et al. A time-split nonhydrostatic atmospheric model for weather research and forecasting applications , 2008, J. Comput. Phys..
[16] S. Osher,et al. Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .
[17] Chi-Wang Shu. Total-variation-diminishing time discretizations , 1988 .
[18] Mark A. Taylor,et al. CAM-SE: A scalable spectral element dynamical core for the Community Atmosphere Model , 2012, Int. J. High Perform. Comput. Appl..
[19] A. Kageyama,et al. ``Yin-Yang grid'': An overset grid in spherical geometry , 2004, physics/0403123.
[20] R. Sadourny. Conservative Finite-Difference Approximations of the Primitive Equations on Quasi-Uniform Spherical Grids , 1972 .
[21] Feng Xiao,et al. A Slope Constrained 4th Order Multi-Moment Finite Volume Method with WENO Limiter , 2015 .
[22] V. Guinot. Approximate Riemann Solvers , 2010 .
[23] Mark A. Taylor,et al. High-Resolution Mesh Convergence Properties and Parallel Efficiency of a Spectral Element Atmospheric Dynamical Core , 2005, Int. J. High Perform. Comput. Appl..
[25] S. Osher,et al. Uniformly high order accurate essentially non-oscillatory schemes, 111 , 1987 .
[26] Feng Xiao,et al. A global multimoment constrained finite-volume scheme for advection transport on the hexagonal geodesic grid , 2011 .
[27] Feng Xiao,et al. A global shallow water model using high order multi-moment constrained finite volume method and icosahedral grid , 2010, J. Comput. Phys..
[28] Jean Côté,et al. Experiments with different discretizations for the shallow‐water equations on a sphere , 2012 .
[29] B. V. Leer,et al. Towards the ultimate conservative difference scheme V. A second-order sequel to Godunov's method , 1979 .
[30] Colin J. Cotter,et al. Analysis of a mixed finite-element pair proposed for an atmospheric dynamical core , 2013 .
[31] Roni Avissar,et al. The Ocean-Land-Atmosphere Model (OLAM). Part II: Formulation and Tests of the Nonhydrostatic Dynamic Core , 2008 .
[32] Chi-Wang Shu,et al. Runge-Kutta Discontinuous Galerkin Method Using WENO Limiters , 2005, SIAM J. Sci. Comput..
[33] B. V. Leer,et al. Towards the Ultimate Conservative Difference Scheme , 1997 .
[34] Feng Xiao,et al. High order multi-moment constrained finite volume method. Part I: Basic formulation , 2009, J. Comput. Phys..
[35] Christiane Jablonowski,et al. MCore: A non-hydrostatic atmospheric dynamical core utilizing high-order finite-volume methods , 2012, J. Comput. Phys..
[36] T. Clark. A small-scale dynamic model using a terrain-following coordinate transformation , 1977 .
[37] Francis X. Giraldo,et al. A Scalable Spectral Element Eulerian Atmospheric Model (SEE-AM) for NWP: Dynamical Core Tests , 2004 .
[38] Dörthe Handorf,et al. Unsteady analytical solutions of the spherical shallow water equations , 2005 .
[39] Hirofumi Tomita,et al. Shallow water model on a modified icosahedral geodesic grid by using spring dynamics , 2001 .
[40] David L. Williamson,et al. The Cartesian method for solving partial differential equations in spherical geometry , 1998 .
[41] Almut Gassmann,et al. Non-hydrostatic modelling with ICON , 2010 .
[42] Chungang Chen,et al. An Adaptive Multimoment Global Model on a Cubed Sphere , 2011 .
[43] D. Durran,et al. A Compressible Model for the Simulation of Moist Mountain Waves , 1983 .
[44] K. Droegemeier,et al. The Advanced Regional Prediction System (ARPS) – A multi-scale nonhydrostatic atmospheric simulation and prediction model. Part I: Model dynamics and verification , 2000 .
[45] C. J. Cotter,et al. Compatible finite element methods for numerical weather prediction , 2014 .
[46] P. Woodward,et al. The numerical simulation of two-dimensional fluid flow with strong shocks , 1984 .
[47] Christopher Edwards,et al. Multi-scale geophysical modeling using the spectral element method , 2002, Comput. Sci. Eng..
[48] A. Staniforth,et al. The Operational CMC–MRB Global Environmental Multiscale (GEM) Model. Part I: Design Considerations and Formulation , 1998 .
[49] F. Xiao,et al. A Multimoment Finite-Volume Shallow-Water Model On The Yin-Yang Overset Spherical Grid , 2008 .
[50] Shian-Jiann Lin,et al. Finite-volume transport on various cubed-sphere grids , 2007, J. Comput. Phys..
[51] Takashi Yabe,et al. A universal solver for hyperbolic equations by cubic-polynomial interpolation I. One-dimensional solver , 1991 .
[52] C. Rossby. Relation between variations in the intensity of the zonal circulation of the atmosphere and the displacements of the semi-permanent centers of action , 1939 .
[53] Chi-Wang Shu,et al. Efficient Implementation of Weighted ENO Schemes , 1995 .
[54] Tsuyoshi Murata,et al. {m , 1934, ACML.
[55] Matthew R. Norman,et al. A low communication and large time step explicit finite-volume solver for non-hydrostatic atmospheric dynamics , 2011, J. Comput. Phys..
[56] Feng Xiao,et al. A global shallow‐water model on an icosahedral–hexagonal grid by a multi‐moment constrained finite‐volume scheme , 2014 .
[57] Feng Xiao,et al. Development of a hybrid parallel MCV-based high-order global shallow-water model , 2017, The Journal of Supercomputing.
[58] Feng Xiao,et al. A Multimoment Constrained Finite-Volume Model for Nonhydrostatic Atmospheric Dynamics , 2013 .
[59] Eleuterio F. Toro,et al. ADER: Arbitrary High Order Godunov Approach , 2002, J. Sci. Comput..
[60] Richard C. J. Somerville,et al. On the use of a coordinate transformation for the solution of the Navier-Stokes equations , 1975 .
[61] Chungang Chen,et al. Fourth order transport model on Yin-Yang grid by multi-moment constrained finite volume scheme , 2012, ICCS.
[62] Nash'at Ahmad,et al. Euler solutions using flux‐based wave decomposition , 2007 .
[63] Feng Xiao,et al. A 4th-order and single-cell-based advection scheme on unstructured grids using multi-moments , 2005, Comput. Phys. Commun..
[64] Feng Xiao,et al. Unified formulation for compressible and incompressible flows by using multi-integrated moments I: one-dimensional inviscid compressible flow , 2004 .
[65] Henry M. Tufo,et al. High-order Galerkin methods for scalable global atmospheric models , 2007, Comput. Geosci..
[66] Christiane Jablonowski,et al. The pros and cons of diffusion, filters and fixers in Atmospheric General Circulation Models , 2011 .
[67] Chi-Wang Shu. Numerical experiments on the accuracy of ENO and modified ENO schemes , 1990 .
[68] B. Haurwitz. THE MOTION OF ATMOSPHERIC DISTURBANCES ON THE SPHERICAL EARTH , 2019 .
[69] H. Tufo,et al. Computational aspects of a scalable high-order discontinuous Galerkin atmospheric dynamical core , 2009 .
[70] Nigel Wood,et al. Runge-Kutta IMEX schemes for the Horizontally Explicit/Vertically Implicit (HEVI) solution of wave equations , 2013, J. Comput. Phys..
[71] Feng Xiao,et al. A note on the general multi-moment constrained flux reconstruction formulation for high order schemes , 2012 .
[72] Yu Wang,et al. New generation of multi-scale NWP system (GRAPES): general scientific design , 2008 .
[73] Eleuterio F. Toro,et al. Towards Very High Order Godunov Schemes , 2001 .
[74] S. Osher,et al. Uniformly high order accuracy essentially non-oscillatory schemes III , 1987 .
[75] R. K. Scott,et al. An initial-value problem for testing numerical models of the global shallow-water equations , 2004 .
[76] William C. Skamarock,et al. Efficiency and Accuracy of the Klemp-Wilhelmson Time-Splitting Technique , 1994 .
[77] Feng Xiao,et al. Global shallow water models based on multi-moment constrained finite volume method and three quasi-uniform spherical grids , 2014, J. Comput. Phys..
[78] T. Yabe,et al. The constrained interpolation profile method for multiphase analysis , 2001 .
[79] Rupert Klein,et al. A moist pseudo-incompressible model , 2014 .
[80] Roni Avissar,et al. The Ocean-Land-Atmosphere Model (OLAM). Part I: Shallow-Water Tests , 2008 .
[81] Christiane Jablonowski,et al. An Intercomparison of 10 Atmospheric Model Dynamical Cores , 2008 .
[82] Stephen J. Thomas,et al. The NCAR Spectral Element Climate Dynamical Core: Semi-Implicit Eulerian Formulation , 2005, J. Sci. Comput..
[83] Feng Xiao,et al. A Non-oscillatory Multi-Moment Finite Volume Scheme with Boundary Gradient Switching , 2017, J. Sci. Comput..
[84] J. Hack,et al. Spectral transform solutions to the shallow water test set , 1995 .
[85] Masaki Satoh,et al. Nonhydrostatic icosahedral atmospheric model (NICAM) for global cloud resolving simulations , 2008, J. Comput. Phys..
[86] Janusz A. Pudykiewicz. On numerical solution of the shallow water equations with chemical reactions on icosahedral geodesic grid , 2011, J. Comput. Phys..
[87] Amik St-Cyr,et al. A Dynamic hp-Adaptive Discontinuous Galerkin Method for Shallow-Water Flows on the Sphere with Application to a Global Tsunami Simulation , 2012 .
[88] George H. Bryan,et al. A Benchmark Simulation for Moist Nonhydrostatic Numerical Models , 2002 .
[89] Mark A. Taylor,et al. A compatible and conservative spectral element method on unstructured grids , 2010, J. Comput. Phys..
[90] Chungang Chen,et al. An MCV Nonhydrostatic Atmospheric Model with Height-Based Terrain following Coordinate: Tests of Waves over Steep Mountains , 2016 .
[91] T. Yabe,et al. Completely conservative and oscillationless semi-Lagrangian schemes for advection transportation , 2001 .
[92] Francis X. Giraldo,et al. A study of spectral element and discontinuous Galerkin methods for the Navier-Stokes equations in nonhydrostatic mesoscale atmospheric modeling: Equation sets and test cases , 2008, J. Comput. Phys..
[93] Feng Xiao,et al. Unified formulation for compressible and incompressible flows by using multi-integrated moments II: Multi-dimensional version for compressible and incompressible flows , 2006, J. Comput. Phys..
[94] R. LeVeque. Approximate Riemann Solvers , 1992 .
[95] David L. Williamson,et al. Integration of the barotropic vorticity equation on a spherical geodesic grid , 1968 .
[96] Feng Xiao,et al. CIP/multi-moment finite volume method with arbitrary order of accuracy , 2007 .
[97] Z. Qingcun,et al. Nonlinear baroclinic haurwitz waves , 1986 .
[98] A. Harten. High Resolution Schemes for Hyperbolic Conservation Laws , 2017 .
[99] Feng Xiao,et al. Shallow water model on cubed-sphere by multi-moment finite volume method , 2008, J. Comput. Phys..
[100] F. Xiao,et al. Numerical simulations of free-interface fluids by a multi-integrated moment method , 2005 .