{"id":18446,"date":"2022-12-05T02:14:33","date_gmt":"2022-12-04T23:14:33","guid":{"rendered":"https:\/\/w3.bilkent.edu.tr\/en\/?p=18446"},"modified":"2022-12-06T20:46:01","modified_gmt":"2022-12-06T17:46:01","slug":"math-seminar-on-the-well-posedness-of-an-inviscid-fluid-structure-interaction-model-amjad-tuffaha-400pm-december-6-en","status":"publish","type":"post","link":"https:\/\/w3.bilkent.edu.tr\/en\/math-seminar-on-the-well-posedness-of-an-inviscid-fluid-structure-interaction-model-amjad-tuffaha-400pm-december-6-en\/","title":{"rendered":"MATH Seminar: \u201cOn the well-posedness of an inviscid fluid-structure interaction model\u201d, Amjad Tuffaha, 4:00PM December 6 (EN)"},"content":{"rendered":"<p>You are cordially invited to the Analysis Seminar organized by the Department of Mathematics.<\/p>\n<p>Speaker: Amjad Tuffaha (American University of Sharjah, United Arab Emirates)<\/p>\n<p>\u201cOn the well-posedness of an inviscid fluid-structure interaction model\u201d<\/p>\n<p>Abstract: We consider the Euler equations on a domain with free moving interface. The motion of the interface is governed by a 4th order linear Euler-Bernoulli beam equation. The fluid-structure interaction dynamics are realized through normal velocity matching of the fluid and the structure in addition to the aerodynamic forcing due to the fluid pressure.<br \/>\nWe derive a-priori estimates and construct local-in-time solutions to the system in the Sobolev space H^r, with r&gt;5\/2. We also establish uniqueness in the Sobolev space H^r with r&gt;3.<br \/>\nAn important consequence of the existence theorem is that the Taylor-Rayleigh instability does not occur. This is joint work with Igor Kukavica.<\/p>\n<p>Date: Tuesday, December 6, 2022<br \/>\nTime: 16:00-17:00 GMT+3.<br \/>\nPlace: SA141- Mathematics Seminar Room<\/p>\n","protected":false},"excerpt":{"rendered":"<p>You are cordially invited to the Analysis Seminar organized by the Department of Mathematics. Speaker: Amjad Tuffaha (American University of Sharjah, United Arab Emirates) \u201cOn the well-posedness of an inviscid fluid-structure interaction model\u201d Abstract: We consider the Euler equations on a domain with free moving interface. The motion of the [\u2026] <\/p>\n<div class=\"clear\"><\/div>\n<p><a class=\"more_link clearfix\" href=\"https:\/\/w3.bilkent.edu.tr\/en\/math-seminar-on-the-well-posedness-of-an-inviscid-fluid-structure-interaction-model-amjad-tuffaha-400pm-december-6-en\/\" rel=\"nofollow\">Read More<\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[12],"tags":[],"class_list":["post-18446","post","type-post","status-publish","format-standard","hentry","category-oldposts"],"_links":{"self":[{"href":"https:\/\/w3.bilkent.edu.tr\/en\/wp-json\/wp\/v2\/posts\/18446","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/w3.bilkent.edu.tr\/en\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/w3.bilkent.edu.tr\/en\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/w3.bilkent.edu.tr\/en\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/w3.bilkent.edu.tr\/en\/wp-json\/wp\/v2\/comments?post=18446"}],"version-history":[{"count":1,"href":"https:\/\/w3.bilkent.edu.tr\/en\/wp-json\/wp\/v2\/posts\/18446\/revisions"}],"predecessor-version":[{"id":18447,"href":"https:\/\/w3.bilkent.edu.tr\/en\/wp-json\/wp\/v2\/posts\/18446\/revisions\/18447"}],"wp:attachment":[{"href":"https:\/\/w3.bilkent.edu.tr\/en\/wp-json\/wp\/v2\/media?parent=18446"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/w3.bilkent.edu.tr\/en\/wp-json\/wp\/v2\/categories?post=18446"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/w3.bilkent.edu.tr\/en\/wp-json\/wp\/v2\/tags?post=18446"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}