{"id":1043,"date":"2019-10-14T17:39:10","date_gmt":"2019-10-14T17:39:10","guid":{"rendered":"http:\/\/fluidslab.chemeng.upatras.gr\/?p=1043"},"modified":"2019-10-14T17:43:11","modified_gmt":"2019-10-14T17:43:11","slug":"discretization-of-three-dimensional-free-surface-flows-and-moving-boundary-problems-via-elliptic-grid-methods-based-on-variational-principles","status":"publish","type":"post","link":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/2019\/10\/14\/discretization-of-three-dimensional-free-surface-flows-and-moving-boundary-problems-via-elliptic-grid-methods-based-on-variational-principles\/","title":{"rendered":"Discretization of three-dimensional free surface flows and moving boundary problems via elliptic grid methods based on variational principles"},"content":{"rendered":"\n<h3 class=\"wp-block-heading\">Authors<\/h3>\n\n\n\n<p>D.Fraggedakis, J.Papaioannou, Y.Dimakopoulos, J.Tsamopoulos<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">Abstract<\/h3>\n\n\n\n<p>A new boundary-fitted technique to describe free surface and moving  boundary problems is presented. We have extended the 2D elliptic grid  generator developed by Dimakopoulos and Tsamopoulos (2003) <a href=\"https:\/\/www.sciencedirect.com\/science\/article\/pii\/S002199911730339X#br0190\">[19]<\/a> and further advanced by Chatzidai et al. (2009) <a href=\"https:\/\/www.sciencedirect.com\/science\/article\/pii\/S002199911730339X#br0180\">[18]<\/a> to 3D geometries. The set of equations arises from the fulfillment of the <a href=\"https:\/\/www.sciencedirect.com\/topics\/physics-and-astronomy\/variational-principles\">variational principles<\/a> established by Brackbill and Saltzman (1982) <a href=\"https:\/\/www.sciencedirect.com\/science\/article\/pii\/S002199911730339X#br0210\">[21]<\/a>, and refined by Christodoulou and Scriven (1992) <a href=\"https:\/\/www.sciencedirect.com\/science\/article\/pii\/S002199911730339X#br0220\">[22]<\/a>. These account for both smoothness and orthogonality of the grid lines of tessellated <a href=\"https:\/\/www.sciencedirect.com\/topics\/computer-science\/physical-domain\">physical domains<\/a>.  The elliptic-grid equations are accompanied by new boundary constraints  and conditions which are based either on the equidistribution of the  nodes on boundary surfaces or on the existing 2D quasi-elliptic grid  methodologies. The capabilities of the proposed algorithm are first  demonstrated in tests with analytically described complex surfaces. The  sequence in which these tests are presented is chosen to help the reader  build up experience on the best choice of the elliptic grid parameters.  Subsequently, the mesh equations are coupled with the Navier\u2013Stokes  equations, in order to reveal the full potential of the proposed  methodology in free surface flows. More specifically, the problem of gas  assisted injection in ducts of circular and square cross-sections is  examined, where the fluid domain experiences extreme <a href=\"https:\/\/www.sciencedirect.com\/topics\/physics-and-astronomy\/deformation\">deformations<\/a>. Finally, the flow-mesh solver is used to calculate the equilibrium shapes of <a href=\"https:\/\/www.sciencedirect.com\/topics\/physics-and-astronomy\/statics\">static<\/a><a href=\"https:\/\/www.sciencedirect.com\/topics\/physics-and-astronomy\/menisci\">menisci<\/a> in capillary tubes.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">Keywords<\/h3>\n\n\n\n<p>Moving boundary problems, Mesh generation, Free-surface flows, Elliptic-grid generation, Moving contact line, Contact angle models<\/p>\n\n\n\n<p><a href=\"https:\/\/doi.org\/10.1016\/j.jcp.2017.04.060\">https:\/\/doi.org\/10.1016\/j.jcp.2017.04.060<\/a><\/p>\n ","protected":false},"excerpt":{"rendered":"<p>Authors D.Fraggedakis, J.Papaioannou, Y.Dimakopoulos, J.Tsamopoulos Abstract A new boundary-fitted technique to describe free surface and moving boundary problems is presented. We have extended the 2D elliptic grid generator developed by Dimakopoulos and Tsamopoulos (2003) [19] and further advanced by Chatzidai et al. (2009) [18] to 3D geometries. The set of equations arises from the fulfillment [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"footnotes":""},"categories":[191],"tags":[],"class_list":{"0":"post-1043","1":"post","2":"type-post","3":"status-publish","4":"format-standard","6":"category-191","7":"czr-hentry"},"_links":{"self":[{"href":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/wp-json\/wp\/v2\/posts\/1043","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/wp-json\/wp\/v2\/comments?post=1043"}],"version-history":[{"count":1,"href":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/wp-json\/wp\/v2\/posts\/1043\/revisions"}],"predecessor-version":[{"id":1044,"href":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/wp-json\/wp\/v2\/posts\/1043\/revisions\/1044"}],"wp:attachment":[{"href":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/wp-json\/wp\/v2\/media?parent=1043"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/wp-json\/wp\/v2\/categories?post=1043"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/fluidslab.chemeng.upatras.gr\/index.php\/wp-json\/wp\/v2\/tags?post=1043"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}