A two-dimensional Riemann solver with self-similar sub-structure - Alternative formulation based on least squares projection

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• 作者：Dinshaw S. Balsara^a ; ^{dbalsara@nd.edu" class="auth_mail" title="E-mail the corresponding author} ; Jeaniffer Vides^b ; ^{jeaniffer.vides@rs2n.eu" class="auth_mail" title="E-mail the corresponding author} ; Katharine Gurski^c ; ^{kgurski@howard.edu" class="auth_mail" title="E-mail the corresponding author} ; Boniface Nkonga^b ; ^{boniface.nkonga@unice.fr" class="auth_mail" title="E-mail the corresponding author} ; Michael Dumbser^d ; ^{michael.dumbser@ing.unitn.it" class="auth_mail" title="E-mail the corresponding author} ; Sudip Garain^a ; ^{sgarain@nd.edu" class="auth_mail" title="E-mail the corresponding author} ; Edouard Audit^e ; ^{edouard.audit@cea.fr" class="auth_mail" title="E-mail the corresponding author}
• 关键词：Hyperbolic systems ; Conservation laws ; Multidimensional Riemann solvers ; Higher order Godunov schemes
• 刊名：Journal of Computational Physics
• 出版年：2016
• 出版时间：1 January 2016
• 年：2016
• 卷：304
• 期：Complete
• 页码：138-161
• 全文大小：4820 K

文摘

Just as the quality of a one-dimensional approximate Riemann solver is improved by the inclusion of internal sub-structure, the quality of a multidimensional Riemann solver is also similarly improved. Such multidimensional Riemann problems arise when multiple states come together at the vertex of a mesh. The interaction of the resulting one-dimensional Riemann problems gives rise to a strongly-interacting state. We wish to endow this strongly-interacting state with physically-motivated sub-structure. The self-similar formulation of Balsara [16] proves especially useful for this purpose. While that work is based on a Galerkin projection, in this paper we present an analogous self-similar formulation that is based on a different interpretation. In the present formulation, we interpret the shock jumps at the boundary of the strongly-interacting state quite literally. The enforcement of the shock jump conditions is done with a least squares projection (Vides, Nkonga and Audit [67]). With that interpretation, we again show that the multidimensional Riemann solver can be endowed with sub-structure. However, we find that the most efficient implementation arises when we use a flux vector splitting and a least squares projection. An alternative formulation that is based on the full characteristic matrices is also presented. The multidimensional Riemann solvers that are demonstrated here use one-dimensional HLLC Riemann solvers as building blocks.

Several stringent test problems drawn from hydrodynamics and MHD are presented to show that the method works. Results from structured and unstructured meshes demonstrate the versatility of our method. The reader is also invited to watch a video introduction to multidimensional Riemann solvers on PDE-Course">http://www.nd.edu/~dbalsara/Numerical-PDE-Course.