A “Vertically Lagrangian” Finite-Volume Dynamical Core for Global Models
暂无分享,去创建一个
[1] V. Starr,et al. A QUASI-LAGRANGIAN SYSTEM OF HYDRODYNAMICAL EQUATIONS , 1945 .
[2] R. Sadourny. Conservative Finite-Difference Approximations of the Primitive Equations on Quasi-Uniform Spherical Grids , 1972 .
[3] William Bourke,et al. A multi-level spectral model. I. Formulation and hemispheric integrations , 1974 .
[4] A. Kasahara. Various Vertical Coordinate Systems Used for Numerical Weather Prediction , 1974 .
[5] B. Vanleer,et al. Towards the ultimate conservative difference scheme. IV. A new approach to numerical convection , 1977 .
[6] B. V. Leer,et al. Towards the ultimate conservative difference scheme. IV. A new approach to numerical convection , 1977 .
[7] A. Arakawa,et al. A Potential Enstrophy and Energy Conserving Scheme for the Shallow Water Equations , 1981 .
[8] P. Woodward,et al. The Piecewise Parabolic Method (PPM) for Gas Dynamical Simulations , 1984 .
[9] P. Woodward,et al. The numerical simulation of two-dimensional fluid flow with strong shocks , 1984 .
[10] J. Hack,et al. Description of the NCAR Community Climate Model (CCM1) , 1987 .
[11] Richard B. Rood,et al. Numerical advection algorithms and their role in atmospheric transport and chemistry models , 1987 .
[12] Akio Arakawa,et al. Numerical modeling of the atmosphere with an isentropic vertical coordinate , 1990 .
[13] A. Harten. ENO schemes with subcell resolution , 1989 .
[14] S. Osher,et al. Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .
[15] P. Woodward,et al. Application of the Piecewise Parabolic Method (PPM) to meteorological modeling , 1990 .
[16] Richard B. Rood,et al. Application of a Monotonic Upstream-biased Transport Scheme to Three-Dimensional Constituent Transport Calculations , 1991 .
[17] Is the Midlatitude Zonal Flow Absolutely Unstable , 1993 .
[18] M. Suárez,et al. A proposal for the intercomparison of the dynamical cores of atmospheric general circulation models , 1994 .
[19] David A. Randall,et al. Geostrophic Adjustment and the Finite-Difference Shallow-Water Equations , 1994 .
[20] Shian-Jiann Lin,et al. A Class of the van Leer-type Transport Schemes and Its Application to the Moisture Transport in a General Circulation Model , 1994 .
[21] P. Paolucci,et al. The “Cubed Sphere” , 1996 .
[22] Shian-Jiann Lin,et al. Transport-induced interannual variability of carbon monoxide determined using a chemistry and transport model , 1996 .
[23] Shian‐Jiann Lin,et al. Multidimensional Flux-Form Semi-Lagrangian Transport Schemes , 1996 .
[24] James J. Hack,et al. Description of the NCAR Community Climate Model (CCM3). Technical note , 1996 .
[25] J. Thuburn. Multidimensional Flux-Limited Advection Schemes , 1996 .
[26] H. T. Huynh. Schemes and constraints for advection , 1997 .
[27] Shian-Jiann Lin,et al. An explicit flux‐form semi‐lagrangian shallow‐water model on the sphere , 1997 .
[28] Shian-Jiann Lin,et al. A finite‐volume integration method for computing pressure gradient force in general vertical coordinates , 1997 .
[29] P. Roe. Approximate Riemann Solvers, Parameter Vectors, and Difference Schemes , 1997 .
[31] S.-J. Lin,et al. Development of the Joint NASA/NCAR General Circulation Model , 1999 .
[32] Todd D. Ringler,et al. Modeling the Atmospheric General Circulation Using a Spherical Geodesic Grid: A New Class of Dynamical Cores , 2000 .
[33] Shian-Jiann Lin,et al. The Global Modeling Initiative Assessment Model: Model Description, Integration and Testing of the Transport Shell , 2000 .
[34] R. LeVeque. Finite Volume Methods for Hyperbolic Problems: Characteristics and Riemann Problems for Linear Hyperbolic Equations , 2002 .