{"id":6483,"date":"2024-12-20T11:56:48","date_gmt":"2024-12-20T10:56:48","guid":{"rendered":"https:\/\/www.mi.uni-koeln.de\/NumSim\/?p=6483"},"modified":"2026-01-30T11:16:09","modified_gmt":"2026-01-30T10:16:09","slug":"snapshot-hyperbolic-viscous-flow-three-dimensional-cubic-lid-driven-cavity","status":"publish","type":"post","link":"https:\/\/www.mi.uni-koeln.de\/NumSim\/2024\/12\/20\/snapshot-hyperbolic-viscous-flow-three-dimensional-cubic-lid-driven-cavity\/","title":{"rendered":"Snapshot: Hyperbolic viscous flow &#8211; Three-dimensional cubic Lid-Driven Cavity"},"content":{"rendered":"<div style=\"width: 584px;\" class=\"wp-video\"><!--[if lt IE 9]><script>document.createElement('video');<\/script><![endif]-->\n<video class=\"wp-video-shortcode\" id=\"video-6483-1\" width=\"584\" height=\"329\" preload=\"metadata\" controls=\"controls\"><source type=\"video\/mp4\" src=\"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-content\/uploads\/2024\/12\/re1000_xz_short_compressed-1.mp4?_=1\" \/><a href=\"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-content\/uploads\/2024\/12\/re1000_xz_short_compressed-1.mp4\">https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-content\/uploads\/2024\/12\/re1000_xz_short_compressed-1.mp4<\/a><\/video><\/div>\n<p>x-z central cross section of 3d Lid-Driven Cavity flow, solving the unified model of Godunov, Peshkov, and Romenski for hyperbolic viscous flow. The upper row shows the macroscopic flow state, while the bottom row shows the distortion field, tracking fluid flow deformations as if it were a solid. The numerical solver is a simple explicit second order Finite Volume method (MUSCL-Hancock) using an HLL-type Riemann solver based on Toro-Vazquez flux splitting. The Reynolds number is 1000 and the mesh resolution is 384^3.<\/p>\n<p>This research has been carried out by Simone Chiocchetti, funded by the European Union\u2019s Horizon Europe Research and Innovation Programme under the Marie Sk\u0142odowska-Curie Postdoctoral Fellowship MoMeNTUM (grant agreement No. 101109532).<\/p>\n<p><a href=\"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-content\/uploads\/2026\/01\/image.png\"><img decoding=\"async\" loading=\"lazy\" src=\"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-content\/uploads\/2026\/01\/image-300x63.png\" alt=\"\" width=\"300\" height=\"63\" class=\"aligncenter size-medium wp-image-6678\" srcset=\"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-content\/uploads\/2026\/01\/image-300x63.png 300w, https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-content\/uploads\/2026\/01\/image-1024x215.png 1024w, https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-content\/uploads\/2026\/01\/image-768x161.png 768w, https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-content\/uploads\/2026\/01\/image-500x105.png 500w, https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-content\/uploads\/2026\/01\/image.png 1100w\" sizes=\"(max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>x-z central cross section of 3d Lid-Driven Cavity flow, solving the unified model of Godunov, Peshkov, and Romenski for hyperbolic viscous flow. The upper row shows the macroscopic flow state, while the bottom row shows the distortion field, tracking fluid &hellip; <a href=\"https:\/\/www.mi.uni-koeln.de\/NumSim\/2024\/12\/20\/snapshot-hyperbolic-viscous-flow-three-dimensional-cubic-lid-driven-cavity\/\">Continue reading <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":14,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[49],"tags":[],"post_mailing_queue_ids":[],"_links":{"self":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/6483"}],"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\/14"}],"replies":[{"embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/comments?post=6483"}],"version-history":[{"count":5,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/6483\/revisions"}],"predecessor-version":[{"id":6686,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/posts\/6483\/revisions\/6686"}],"wp:attachment":[{"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/media?parent=6483"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/categories?post=6483"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.mi.uni-koeln.de\/NumSim\/wp-json\/wp\/v2\/tags?post=6483"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}