{"id":364,"date":"2020-11-02T21:58:56","date_gmt":"2020-11-02T21:58:56","guid":{"rendered":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/?page_id=364"},"modified":"2026-01-07T20:34:00","modified_gmt":"2026-01-07T20:34:00","slug":"movies","status":"publish","type":"page","link":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/movies\/","title":{"rendered":"Movies"},"content":{"rendered":"\n\n\n\n\n\n\n\n\n\n
\"Lagrangian<\/a><\/td>\nLagrangian particles in the wave bottom boundary layer during transition. 6 second wave period – side view.<\/a><\/td>\n<\/tr>\n
\"Vorticity<\/a><\/td>\nVorticity fields from calculations of flow over a sand ripple.<\/a><\/td>\n<\/tr>\n
\"Kinetic<\/a><\/td>\nKinetic energy dissipation rate for simulations of the wave bottom boundary layer over a smooth surface.\u00a0 5 second period, Um = 80 cm\/s, side view (x-z plane).<\/a><\/td>\n<\/tr>\n
\"Kinetic<\/a><\/td>\nKinetic energy dissipation rate for simulations of the wave bottom boundary layer over a smooth surface.\u00a0 Top view (x-z plane).<\/a><\/td>\n<\/tr>\n
\"Sheet<\/a><\/td>\nSheet flow simulation with a two-phase variable density model.\u00a0 A vertical plane of the reference concentration and velocity vectors from a 3D simulation are shown.<\/a><\/td>\n<\/tr>\n
\"3D<\/a><\/td>\nSheet flow simulation #2, a 3D visualization of reference concentration of sediment in a 3 second period turbulent boundary layer.\u00a0 The blue iso-surface is the 5 percent concentration contour.<\/a><\/td>\n<\/tr>\n
\"Sheet<\/a><\/td>\nSheet flow simulation of Horikawa’s experiment.\u00a0 Model results have similar mean flow properties to the lab measurements.<\/a><\/td>\n<\/tr>\n
\"Volume<\/a><\/td>\nVolume of Fluid simulation of waves in a tank.\u00a0 Both the water and air are modeled together.\u00a0 Velocity vectors and density contours are shown.<\/a><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n","protected":false},"excerpt":{"rendered":"

Lagrangian particles in the wave bottom boundary layer during transition. 6 second wave period – side view. Vorticity fields from calculations of flow over a sand ripple. Kinetic energy dissipation rate for simulations of the wave bottom boundary layer over a smooth surface.\u00a0 5 second period, Um = 80 cm\/s, side view (x-z plane). Kinetic […]<\/p>\n","protected":false},"author":418,"featured_media":270,"parent":0,"menu_order":2,"comment_status":"closed","ping_status":"closed","template":"page-templates\/page-sidebar-none.php","meta":{"_acf_changed":false,"inline_featured_image":false,"featured_post":"","footnotes":"","_links_to":"","_links_to_target":""},"class_list":["post-364","page","type-page","status-publish","has-post-thumbnail","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/wp-json\/wp\/v2\/pages\/364","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/wp-json\/wp\/v2\/users\/418"}],"replies":[{"embeddable":true,"href":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/wp-json\/wp\/v2\/comments?post=364"}],"version-history":[{"count":20,"href":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/wp-json\/wp\/v2\/pages\/364\/revisions"}],"predecessor-version":[{"id":740,"href":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/wp-json\/wp\/v2\/pages\/364\/revisions\/740"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/wp-json\/wp\/v2\/media\/270"}],"wp:attachment":[{"href":"https:\/\/faculty.eng.ufl.edu\/donald-slinn\/wp-json\/wp\/v2\/media?parent=364"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}