{"id":6647,"date":"2019-08-30T15:56:33","date_gmt":"2019-08-30T15:56:33","guid":{"rendered":"http:\/\/www.ukctrf.com\/?page_id=6647"},"modified":"2019-08-30T17:25:48","modified_gmt":"2019-08-30T17:25:48","slug":"simulations-for-bench-marking-using-senga","status":"publish","type":"page","link":"https:\/\/www.ukctrf.com\/index.php\/hamish\/simulations-for-bench-marking-using-senga\/","title":{"rendered":"Simulations for bench marking using SENGA+"},"content":{"rendered":"\n\t<h2>Planar flame simulations<\/h2>\n<p><img loading=\"lazy\" src=\"http:\/\/www.ukctrf.com\/wp-content\/uploads\/2019\/08\/Planar_flame_table-1024x293.png\" alt=\"\" width=\"930\" height=\"266\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" src=\"http:\/\/www.ukctrf.com\/wp-content\/uploads\/2019\/08\/Planar_flame_2-D_contours_progress_variable.png\" alt=\"\" width=\"2198\" height=\"1191\" \/><\/p>\n<h4>Progress variable contours on the x-y mid-plane<\/h4>\n<h2>Flame-wall interaction of oblique flame in a fully turbulent channel flow<\/h2>\n<p>Oblique flame-wall interaction simulations at <img loading=\"lazy\" src=\"http:\/\/www.ukctrf.com\/wp-content\/uploads\/2019\/08\/re_tau_110-300x58.png\" alt=\"\" width=\"78\" height=\"15\" \/> fully developed channel flow conditions have been performed under isothermal and adiabatic wall boundary conditions.<\/p>\n<p><img loading=\"lazy\" src=\"http:\/\/www.ukctrf.com\/wp-content\/uploads\/2019\/08\/V-flame_iso_3D195_3D_crop.png\" alt=\"\" width=\"4114\" height=\"1349\" \/><\/p>\n<h4>Isothermal wall boundary conditions<\/h4>\n<p>&nbsp;<\/p>\n<p><img loading=\"lazy\" src=\"http:\/\/www.ukctrf.com\/wp-content\/uploads\/2019\/08\/3D0188_AD_crop.png\" alt=\"\" width=\"4108\" height=\"1344\" \/><\/p>\n<h4>Adiabatic wall boundary conditions<\/h4>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<h2>Access to the data sets<\/h2>\n<p>The data sets for the planar flames and flame-wall interaction are available upon request. Please contact:<\/p>\n<p>Dr Umair Ahmed (email: umair.ahmed@newcastle.ac.uk)<\/p>\n<p>Professor Nilanjan Chakraborty (email: nilanjan.chakraborty@newcastle.ac.uk)<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Planar flame simulations &nbsp; Progress variable contours on the x-y mid-plane Flame-wall interaction of oblique flame in a fully turbulent channel flow Oblique flame-wall interaction simulations at fully developed channel flow conditions have been performed under isothermal and adiabatic wall boundary conditions. Isothermal wall boundary conditions &nbsp; Adiabatic wall boundary [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":5948,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v17.2.1 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>Simulations for bench marking using SENGA+ - UKCTRF<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/www.ukctrf.com\/index.php\/hamish\/simulations-for-bench-marking-using-senga\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Simulations for bench marking using SENGA+ - UKCTRF\" \/>\n<meta property=\"og:description\" content=\"Planar flame simulations &nbsp; Progress variable contours on the x-y mid-plane Flame-wall interaction of oblique flame in a fully turbulent channel flow Oblique flame-wall interaction simulations at fully developed channel flow conditions have been performed under isothermal and adiabatic wall boundary conditions. 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