Conservative Transport Schemes for Spherical Geodesic Grids: High-Order Flux Operators for ODE-Based Time Integration

Higher-order finite-volume flux operators for transport algorithms used within Runge‐Kutta time integration schemes on irregular Voronoi (hexagonal) meshes are proposed and tested. These operators are generalizations of third- and fourth-order operators currently used in atmospheric models employing regular, orthogonal rectangular meshes. Two-dimensional least squares fit polynomials are used to evaluate the higher-order spatial derivatives needed to cancel the leading-order truncation error terms of the standard second-order centered formulation. Positive definite or monotonic behavior is achieved by applying an appropriate limiter during the final Runge‐Kutta stage within a given time step. The third- and fourth-order formulations are evaluated using standard transport tests on the sphere. The new schemes are more accurate and significantly more efficient than the standard second-order scheme and other schemes in the literature examined by the authors. The third-order formulation is equivalent to the fourth-order formulation plus an additional diffusion term that is proportional to the Courant number. An optimalvalueforthecoefficientscalingthisdiffusiontermischosenbasedonqualitativeevaluationofthetest results. Improvements using the higher-order scheme in place of the traditional second-order centered approach are illustrated within 3D unstable baroclinic wave simulations produced using two global nonhydrostatic models employing spherical Voronoi meshes.

[1]  P. Swarztrauber,et al.  A standard test set for numerical approximations to the shallow water equations in spherical geometry , 1992 .

[2]  Louis J. Wicker,et al.  Time-Splitting Methods for Elastic Models Using Forward Time Schemes , 2002 .

[3]  Peter H. Lauritzen,et al.  A class of deformational flow test cases for linear transport problems on the sphere , 2010, J. Comput. Phys..

[4]  William C. Skamarock,et al.  A unified approach to energy conservation and potential vorticity dynamics for arbitrarily-structured C-grids , 2010, J. Comput. Phys..

[5]  R. James Purser,et al.  Accuracy Considerations of Time-Splitting Methods for Models Using Two-Time-Level Schemes , 2007 .

[6]  J. Verwer,et al.  A positive finite-difference advection scheme , 1995 .

[7]  Almut Gassmann,et al.  Towards a consistent numerical compressible non‐hydrostatic model using generalized Hamiltonian tools , 2008 .

[8]  M. Giorgetta,et al.  Icosahedral Shallow Water Model (ICOSWM): results of shallow water test cases and sensitivity to model parameters , 2009 .

[9]  William H. Lipscomb,et al.  An Incremental Remapping Transport Scheme on a Spherical Geodesic Grid , 2005 .

[10]  William Skamarock,et al.  Conservative Transport Schemes for Spherical Geodesic Grids: High-Order Reconstructions for Forward-in-Time Schemes , 2010 .

[11]  S. Zalesak Fully multidimensional flux-corrected transport algorithms for fluids , 1979 .

[12]  William C. Skamarock,et al.  A time-split nonhydrostatic atmospheric model for weather research and forecasting applications , 2008, J. Comput. Phys..

[13]  Dale R. Durran,et al.  Selective monotonicity preservation in scalar advection , 2008, J. Comput. Phys..

[14]  Roni Avissar,et al.  The Ocean-Land-Atmosphere Model (OLAM). Part II: Formulation and Tests of the Nonhydrostatic Dynamic Core , 2008 .

[15]  Kao-San Yeh,et al.  The streamline subgrid integration method: I. Quasi-monotonic second-order transport schemes , 2007, J. Comput. Phys..

[16]  Todd D. Ringler,et al.  A multiresolution method for climate system modeling: application of spherical centroidal Voronoi tessellations , 2008 .

[17]  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..

[18]  Hailong Wang,et al.  Evaluation of Scalar Advection Schemes in the Advanced Research WRF Model Using Large-Eddy Simulations of Aerosol–Cloud Interactions , 2009 .

[19]  Aimé Fournier,et al.  Voronoi, Delaunay, and Block-Structured Mesh Refinement for Solution of the Shallow-Water Equations on the Sphere , 2009 .

[20]  Michael Buchhold,et al.  The Operational Global Icosahedral-Hexagonal Gridpoint Model GME: Description and High-Resolution Tests , 2002 .

[21]  W. Skamarock,et al.  Global non-hydrostatic modelling using Voronoi meshes: The MPAS model , 2011 .

[22]  Audra E. Kosh,et al.  Linear Algebra and its Applications , 1992 .

[23]  Hirofumi Tomita,et al.  Shallow water model on a modified icosahedral geodesic grid by using spring dynamics , 2001 .

[24]  H. Miura An Upwind-Biased Conservative Advection Scheme for Spherical Hexagonal–Pentagonal Grids , 2007 .

[25]  D. Williamson,et al.  A baroclinic instability test case for atmospheric model dynamical cores , 2006 .