{"id":822,"date":"2020-03-04T10:00:18","date_gmt":"2020-03-04T09:00:18","guid":{"rendered":"http:\/\/yvcharron.com\/?page_id=822"},"modified":"2020-12-20T11:57:52","modified_gmt":"2020-12-20T10:57:52","slug":"three-dimension-structures-type-2","status":"publish","type":"page","link":"https:\/\/yvcharron.com\/index.php\/three-dimension-structures-type-2\/","title":{"rendered":"Three Dimension Structures &#8211; Two oscillating waves &#8211; 3D_2"},"content":{"rendered":"\n<p style=\"text-align:center\" class=\"has-text-color has-small-font-size has-cyan-bluish-gray-color\">Keywords: structured surfaces three-dimension structures two-orthogonal waves flow drag reduction turbulent turbulence<\/p>\n\n\n\n<h2 class=\"wp-block-heading\" style=\"text-align:center\"><strong>Adding a normal wave to the transverse wave<\/strong><\/h2>\n\n\n\n<p class=\"has-text-color has-very-dark-gray-color\"><strong>Two dimension structured\nsurfaces<\/strong> have shown the capability to provide a flow drag\nreduction of the order of 10 %. This flow drag reduction is lower in the case\nof riblets with a triangle shape (5 to 6%) and larger in the case of riblets\nwith a knife blade shape (10 to 12%). These performances were calculated with a\nRANS code and found in line with experiments carried out in the past by\nnumerous workers. See web page on \u201c2D structured surfaces\u201d.<\/p>\n\n\n\n<p style=\"text-align:center\"><a href=\"http:\/\/yvcharron.com\/index.php\/two-dimension-structures\/\">http:\/\/yvcharron.com\/index.php\/two-dimension-structures\/<\/a><\/p>\n\n\n\n<p class=\"has-text-color has-very-dark-gray-color\"><strong>A three dimension structure surface &#8211; Type 1<\/strong> including two flow drag reduction mechanisms has been analysed. These mechanisms are: a 2D structured surface associated with a transverse oscillating flow (wave). The resulting flow drag reduction is of the order of 20% at the optimum condition. These performances were determined with a LES code. See web page on \u201c3D structured surfaces \u2013 Type 1\u201d.<\/p>\n\n\n\n<p style=\"text-align:center\">_<a href=\"http:\/\/yvcharron.com\/index.php\/three-dimension-structured-surfaces-type-1\/\">http:\/\/yvcharron.com\/index.php\/three-dimension-structured-surfaces-type-1\/<\/a><\/p>\n\n\n\n<p class=\"has-text-color has-very-dark-gray-color\"><strong>A new shape of 3D structured surface (Type 2)<\/strong> is proposed to provide a greater flow drag reduction. This type 2 <strong>includes two orthogonal oscillating waves<\/strong>, one parallel to the structured surface (as per type 1) and a new one normal to the structured surface and oriented in the flow direction. As very little calculation has been performed with this type of 3D structured surface, a phenomenological analysis is provided below to explain the mode of operation of the different types of riblets: 2D longitudinal riblets and 3D riblets, types 1 and 2.<\/p>\n\n\n\n<div class=\"wp-block-image\"><figure class=\"aligncenter\"><img loading=\"lazy\" decoding=\"async\" width=\"293\" height=\"190\" src=\"http:\/\/yvcharron.com\/wp-content\/uploads\/2020\/03\/image-13.png\" alt=\"Principle of operation of a three dimension structured surface including a conventional structured surface (riblets) and two orthogonal periodic waves: one transversal and one normal\" class=\"wp-image-827\"\/><\/figure><\/div>\n\n\n\n<div class=\"wp-block-file aligncenter\"><a href=\"http:\/\/yvcharron.com\/wp-content\/uploads\/2020\/03\/a_3_3_Surf-Struc-3DTypeTwoOrtWav_Ang_2007.pdf\">FOR MORE DETAILS : ______ a_3_3_Surf Struc 3DTypeTwoOrtWav_Ang_2007<\/a><a href=\"http:\/\/yvcharron.com\/wp-content\/uploads\/2020\/03\/a_3_3_Surf-Struc-3DTypeTwoOrtWav_Ang_2007.pdf\" class=\"wp-block-file__button\" download>T\u00e9l\u00e9charger<\/a><\/div>\n\n\n\n<h2 class=\"wp-block-heading\" style=\"text-align:center\"><strong>Potential of the integration of a third flow drag reduction mechanism<\/strong><\/h2>\n\n\n\n<p class=\"has-text-color has-very-dark-gray-color\">A <strong>LES Code<\/strong> could establish the mechanism of drag reduction provided by a plate oscillating transversely to the main flow direction. The maximum flow drag reduction was obtained for a <strong>dimensionless period of 100<\/strong>. In this specific case, the drag reduction tends to increase with the amplitude of the oscillation, disregarding the energy required to move the plate.<\/p>\n\n\n\n<p class=\"has-text-color has-very-dark-gray-color\">2D\nriblets of the knife blade type provide a maximum drag reduction of the order\nof 10 %. The same result was found with RANS and LES codes (see corresponding\nWeb site pages).<\/p>\n\n\n\n<p class=\"has-text-color has-very-dark-gray-color\"><strong>3D <\/strong>structured surfaces (Type 1) combining the above two flow drag reduction mechanisms (2D riblets and transposed transverse flow oscillation) provide a drag reduction of the order of 20 % according to the LES code validated with the oscillating plate and 2D riblets. The maximum drag reduction was achieved for a dimensionless period of 100 and a maximum angle of the transverse oscillation of the order of 10 degrees.<\/p>\n\n\n\n<p class=\"has-text-color has-very-dark-gray-color\"><strong>It is anticipated that further drag reduction could be obtained by adding a second oscillating wave oriented in the flow direction and orthogonal to the transverse wave<\/strong>. <strong>This second wave (normal wave) could be of a sine wave type with a frequency equal to twice the transverse wave frequency<\/strong>. This normal wave would provide a riblet height increase at the crests of the transverse wave and a riblet height decrease at the inflexion points of the transverse wave. This should provide several advantages:<\/p>\n\n\n\n<ul class=\"wp-block-list\"><li>A\nbetter control of the low speed streaks at the transverse wave crests<\/li><li>Less\nviscous losses at the inflexion points of the transverse wave<\/li><li>An\nadditional parietal oscillating effect provided by the normal wave.<\/li><\/ul>\n\n\n\n<p class=\"has-text-color has-very-dark-gray-color\">This\noptimum dimension values (h<sup>+<\/sup> and S<sup>+<\/sup>) obtained during the\n2D riblet calculations (flow simulation with RANS code) should be reviewed in\nrelation with 3D riblets whatever they are of type 1 (A single oscillating\nwave) or type 2 (Two oscillating waves).\n\nOnce a complete\noptimisation study has been carried out, it is expected to get a flow drag\nreduction significantly greater than 25 per cent.\n\n\n\n<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Keywords: structured surfaces three-dimension structures two-orthogonal waves flow drag reduction turbulent turbulence Adding a normal wave to the transverse wave Two dimension structured surfaces have shown the capability to provide a flow drag reduction of the order of 10 %. This flow drag reduction is lower in the case of riblets with a triangle shape&hellip; <br \/> <a class=\"read-more\" href=\"https:\/\/yvcharron.com\/index.php\/three-dimension-structures-type-2\/\">Read more<\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-822","page","type-page","status-publish","hentry"],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v24.9 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>Three Dimension Structures - Two oscillating waves - 3D_2 - CHARRON Yves<\/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:\/\/yvcharron.com\/index.php\/three-dimension-structures-type-2\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Three Dimension Structures - Two oscillating waves - 3D_2 - CHARRON Yves\" \/>\n<meta property=\"og:description\" content=\"Keywords: structured surfaces three-dimension structures two-orthogonal waves flow drag reduction turbulent turbulence Adding a normal wave to the transverse wave Two dimension structured surfaces have shown the capability to provide a flow drag reduction of the order of 10 %. 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