

{"id":212,"date":"2017-11-28T16:00:25","date_gmt":"2017-11-28T15:00:25","guid":{"rendered":"https:\/\/project.inria.fr\/bendali\/?page_id=212"},"modified":"2017-11-28T16:01:15","modified_gmt":"2017-11-28T15:01:15","slug":"stephan","status":"publish","type":"page","link":"https:\/\/project.inria.fr\/bendali\/program\/stephan\/","title":{"rendered":"Ernst Stephan"},"content":{"rendered":"<p>Leibniz University Hannover, with H. Gimperlein, D. Stark (Heriot-Watt University, Edinburgh) and C.Oezdemir (LUH)<\/p>\n<h2>Adaptive and higher-order time domain boundary elements for the wave equation<\/h2>\n<p>We present $h$ and $p$-versions of the time domain boundary element method for boundary and screen problems for the wave equation in $\\mathbb{R}^3$. First, graded meshes are shown to recover optimal approximation rates for solution in the presence of edge and corner singularities on screens. Then an a posteriori error estimate is presented for general discretizations, and it gives rise to adaptive mesh refinement procedures. We also discuss preliminary results for $p$ and $hp$-versions of the time domain boundary element method. Numerical experiments illustrate the theory.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Leibniz University Hannover, with H. Gimperlein, D. Stark (Heriot-Watt University, Edinburgh) and C.Oezdemir (LUH) Adaptive and higher-order time domain boundary elements for the wave equation We present $h$ and $p$-versions of the time domain boundary element method for boundary and screen problems for the wave equation in $\\mathbb{R}^3$. First, graded\u2026<\/p>\n<p> <a class=\"continue-reading-link\" href=\"https:\/\/project.inria.fr\/bendali\/program\/stephan\/\"><span>Continue reading<\/span><i class=\"crycon-right-dir\"><\/i><\/a> <\/p>\n","protected":false},"author":248,"featured_media":0,"parent":68,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-212","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/pages\/212","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/users\/248"}],"replies":[{"embeddable":true,"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/comments?post=212"}],"version-history":[{"count":1,"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/pages\/212\/revisions"}],"predecessor-version":[{"id":213,"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/pages\/212\/revisions\/213"}],"up":[{"embeddable":true,"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/pages\/68"}],"wp:attachment":[{"href":"https:\/\/project.inria.fr\/bendali\/wp-json\/wp\/v2\/media?parent=212"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}