{"id":5413,"date":"2021-08-03T10:39:32","date_gmt":"2021-08-03T08:39:32","guid":{"rendered":"https:\/\/www.mi.uni-koeln.de\/NumSim\/?p=5413"},"modified":"2021-08-03T10:39:32","modified_gmt":"2021-08-03T08:39:32","slug":"new-paper-published-an-entropy-stable-nodal-discontinuous-galerkin-method-for-the-resistive-mhd-equations-part-ii-subcell-finite-volume-shock-capturing","status":"publish","type":"post","link":"https:\/\/www.mi.uni-koeln.de\/NumSim\/2021\/08\/03\/new-paper-published-an-entropy-stable-nodal-discontinuous-galerkin-method-for-the-resistive-mhd-equations-part-ii-subcell-finite-volume-shock-capturing\/","title":{"rendered":"New paper published: An entropy stable nodal discontinuous Galerkin method for the resistive MHD equations. Part II: Subcell finite volume shock capturing"},"content":{"rendered":"<p id=\"sp0300\">The second paper of this series presents two robust entropy stable shock-capturing methods for discontinuous Galerkin spectral element (DGSEM) discretizations of the compressible magneto-hydrodynamics (MHD) equations. Specifically, we use the resistive GLM-MHD equations, which include a divergence cleaning mechanism that is based on a generalized Lagrange multiplier (GLM). For the continuous entropy analysis to hold, and due to the divergence-free constraint on the magnetic field, the GLM-MHD system requires the use of non-conservative terms, which need special treatment.<\/p>\n<p id=\"sp0310\">Hennemann et al. (2020) <a class=\"workspace-trigger\" href=\"https:\/\/www.sciencedirect.com\/science\/article\/pii\/S0021999121004757?via%3Dihub#br0250\" name=\"bbr0250\">[25]<\/a> recently presented an entropy stable shock-capturing strategy for DGSEM discretizations of the <a class=\"topic-link\" title=\"Learn more about Euler equations from ScienceDirect's AI-generated Topic Pages\" href=\"https:\/\/www.sciencedirect.com\/topics\/computer-science\/euler-equation\">Euler equations<\/a> that blends the DGSEM scheme with a subcell first-order finite volume (FV) method. Our first contribution is the extension of the method of Hennemann et al. to systems with non-conservative terms, such as the GLM-MHD equations. In our approach, the advective and non-conservative terms of the equations are discretized with a hybrid FV\/DGSEM scheme, whereas the visco-resistive terms are discretized only with the high-order DGSEM method. We prove that the extended method is semi-discretely entropy stable on three-dimensional unstructured curvilinear meshes. Our second contribution is the derivation and analysis of a second entropy stable shock-capturing method that provides enhanced resolution by using a subcell reconstruction procedure that is carefully built to ensure entropy stability.<\/p>\n<p>We provide a numerical verification of the properties of the hybrid FV\/DGSEM schemes on curvilinear meshes and show their robustness and accuracy with common benchmark cases, such as the Orszag-Tang <a class=\"topic-link\" title=\"Learn more about vortex from ScienceDirect's AI-generated Topic Pages\" href=\"https:\/\/www.sciencedirect.com\/topics\/physics-and-astronomy\/vortices\">vortex<\/a> and the GEM (Geospace Environmental Modeling) reconnection challenge. Finally, we simulate a space physics application: the interaction of <a class=\"topic-link\" title=\"Learn more about Jupiter's from ScienceDirect's AI-generated Topic Pages\" href=\"https:\/\/www.sciencedirect.com\/topics\/physics-and-astronomy\/jupiter\">Jupiter&#8217;s<\/a> magnetic field with the plasma <a class=\"topic-link\" title=\"Learn more about torus from ScienceDirect's AI-generated Topic Pages\" href=\"https:\/\/www.sciencedirect.com\/topics\/physics-and-astronomy\/toruses\">torus<\/a> generated by the moon Io.<\/p>\n<p>Published in Journal of Computational Physics (<a href=\"https:\/\/www.sciencedirect.com\/science\/article\/pii\/S0021999121004757?via%3Dihub\">ScienceDirect<\/a>)<\/p>\n","protected":false},"excerpt":{"rendered":"<p>The second paper of this series presents two robust entropy stable shock-capturing methods for discontinuous Galerkin spectral element (DGSEM) discretizations of the compressible magneto-hydrodynamics (MHD) equations. Specifically, we use the resistive GLM-MHD equations, which include a divergence cleaning mechanism that &hellip; <a href=\"https:\/\/www.mi.uni-koeln.de\/NumSim\/2021\/08\/03\/new-paper-published-an-entropy-stable-nodal-discontinuous-galerkin-method-for-the-resistive-mhd-equations-part-ii-subcell-finite-volume-shock-capturing\/\">Continue reading <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":12,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[46],"tags":[],"post_mailing_queue_ids":[],"_links":{"self":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/5413"}],"collection":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/users\/12"}],"replies":[{"embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/comments?post=5413"}],"version-history":[{"count":2,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/5413\/revisions"}],"predecessor-version":[{"id":5415,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/5413\/revisions\/5415"}],"wp:attachment":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/media?parent=5413"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/categories?post=5413"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/tags?post=5413"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}