{"id":5339,"date":"2021-05-04T18:27:36","date_gmt":"2021-05-04T16:27:36","guid":{"rendered":"https:\/\/www.mi.uni-koeln.de\/NumSim\/?p=5339"},"modified":"2021-05-04T18:27:36","modified_gmt":"2021-05-04T16:27:36","slug":"new-paper-published-stability-of-discontinuous-galerkin-spectral-element-schemes-for-wave-propagation-when-the-coefficient-matrices-have-jumps","status":"publish","type":"post","link":"https:\/\/www.mi.uni-koeln.de\/NumSim\/2021\/05\/04\/new-paper-published-stability-of-discontinuous-galerkin-spectral-element-schemes-for-wave-propagation-when-the-coefficient-matrices-have-jumps\/","title":{"rendered":"New paper published: Stability of Discontinuous Galerkin Spectral Element Schemes for Wave Propagation when the Coefficient Matrices have Jumps"},"content":{"rendered":"<p>Abstract:<\/p>\n<p>We use the behavior of the <span id=\"MathJax-Element-1-Frame\" class=\"MathJax\" tabindex=\"0\"><span id=\"MathJax-Span-1\" class=\"math\"><span id=\"MathJax-Span-2\" class=\"mrow\"><span id=\"MathJax-Span-3\" class=\"msubsup\"><span id=\"MathJax-Span-4\" class=\"mi\">L<\/span><span id=\"MathJax-Span-5\" class=\"texatom\"><span id=\"MathJax-Span-6\" class=\"mrow\"><span id=\"MathJax-Span-7\" class=\"mn\">2<\/span><\/span><\/span><\/span><\/span><\/span><\/span> norm of the solutions of linear hyperbolic equations with discontinuous coefficient matrices as a surrogate to infer stability of discontinuous Galerkin spectral element methods (DGSEM). Although the <span id=\"MathJax-Element-2-Frame\" class=\"MathJax\" tabindex=\"0\"><span id=\"MathJax-Span-8\" class=\"math\"><span id=\"MathJax-Span-9\" class=\"mrow\"><span id=\"MathJax-Span-10\" class=\"msubsup\"><span id=\"MathJax-Span-11\" class=\"mi\">L<\/span><span id=\"MathJax-Span-12\" class=\"texatom\"><span id=\"MathJax-Span-13\" class=\"mrow\"><span id=\"MathJax-Span-14\" class=\"mn\">2<\/span><\/span><\/span><\/span><\/span><\/span><\/span> norm is not bounded by the initial data for homogeneous and dissipative boundary conditions for such systems, the <span id=\"MathJax-Element-3-Frame\" class=\"MathJax\" tabindex=\"0\"><span id=\"MathJax-Span-15\" class=\"math\"><span id=\"MathJax-Span-16\" class=\"mrow\"><span id=\"MathJax-Span-17\" class=\"msubsup\"><span id=\"MathJax-Span-18\" class=\"mi\">L<\/span><span id=\"MathJax-Span-19\" class=\"texatom\"><span id=\"MathJax-Span-20\" class=\"mrow\"><span id=\"MathJax-Span-21\" class=\"mn\">2<\/span><\/span><\/span><\/span><\/span><\/span><\/span> norm is easier to work with than a norm that discounts growth due to the discontinuities. We show that the DGSEM with an upwind numerical flux that satisfies the Rankine-Hugoniot (or conservation) condition has the same energy bound as the partial differential equation does in the <span id=\"MathJax-Element-4-Frame\" class=\"MathJax\" tabindex=\"0\"><span id=\"MathJax-Span-22\" class=\"math\"><span id=\"MathJax-Span-23\" class=\"mrow\"><span id=\"MathJax-Span-24\" class=\"msubsup\"><span id=\"MathJax-Span-25\" class=\"mi\">L<\/span><span id=\"MathJax-Span-26\" class=\"texatom\"><span id=\"MathJax-Span-27\" class=\"mrow\"><span id=\"MathJax-Span-28\" class=\"mn\">2<\/span><\/span><\/span><\/span><\/span><\/span><\/span> norm, plus an added dissipation that depends on how much the approximate solution fails to satisfy the Rankine-Hugoniot jump.<\/p>\n<p>Accepted in Journal of Scientific Computing.<\/p>\n<p>arXiv link:\u00a0<a href=\"https:\/\/arxiv.org\/abs\/2011.11746\">https:\/\/arxiv.org\/abs\/2011.11746<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Abstract: We use the behavior of the L2 norm of the solutions of linear hyperbolic equations with discontinuous coefficient matrices as a surrogate to infer stability of discontinuous Galerkin spectral element methods (DGSEM). Although the L2 norm is not bounded &hellip; <a href=\"https:\/\/www.mi.uni-koeln.de\/NumSim\/2021\/05\/04\/new-paper-published-stability-of-discontinuous-galerkin-spectral-element-schemes-for-wave-propagation-when-the-coefficient-matrices-have-jumps\/\">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\/5339"}],"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=5339"}],"version-history":[{"count":3,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/5339\/revisions"}],"predecessor-version":[{"id":5342,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/5339\/revisions\/5342"}],"wp:attachment":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/media?parent=5339"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/categories?post=5339"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/tags?post=5339"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}