{"id":871,"date":"2017-06-17T20:49:04","date_gmt":"2017-06-17T11:49:04","guid":{"rendered":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/?p=871"},"modified":"2017-06-17T20:51:36","modified_gmt":"2017-06-17T11:51:36","slug":"871","status":"publish","type":"post","link":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/?p=871","title":{"rendered":"\u6d41\u4f53\u529b\u5b66\u30bb\u30df\u30ca\u30fc"},"content":{"rendered":"<p>\u7686\u69d8\u30016\/26\u65e5(\u6708)\u306e\u6d41\u4f53\u529b\u5b66\u30bb\u30df\u30ca\u30fc\u3092\u5fa1\u6848\u5185\u3044\u305f\u3057\u307e\u3059\u3002<br \/>\n\u5fa1\u6765\u8074\u6b53\u8fce\u3044\u305f\u3057\u307e\u3059\u3002<\/p>\n<p>\u65e5\u6642\uff1a2016\u5e74 6\u6708 26\u65e5\uff08\u6708\uff09 15:00 \u304b\u3089 16:30<\/p>\n<p>\u5834\u6240\uff1a \u4eac\u90fd\u5927\u5b66 \u6570\u7406\u89e3\u6790\u7814\u7a76\u6240 204\u53f7\u5ba4<\/p>\n<p>\u8b1b\u5e2b\uff1a Prof.  Tamer A. Zaki<br \/>\n\uff08Mechanical Engineering, Johns Hopkins University\uff09<\/p>\n<p>\u8b1b\u6f14\u984c\u76ee\uff1a<br \/>\nLARGE-SCALE STRUCTURES IN TRANSITIONAL AND TURBULENT BOUNDARY LAYERS<\/p>\n<p>\u8b1b\u6f14\u8981\u65e8\uff1a<br \/>\n In transitional and turbulent boundary layers, an interface separates<br \/>\nthe non-turbulent and turbulent regions of the flow. In the transition<br \/>\nzone, this interface surrounds localized patches of turbulence that<br \/>\nare formed sporadically and spread to consume the surrounding laminar<br \/>\nflow. In the turbulent regime, the interface marks the free-stream<br \/>\nedge of the boundary layer and separates the vortical near-wall motion<br \/>\nfrom the outer potential flow. Using direct numerical simulations, we<br \/>\nexamine characteristics of this turbulent\/non-turbulent (T\/NT)<br \/>\ninterface. In the case of transition we relate its formation, or the<br \/>\ninception of turbulence patches, to the streaky structures known as<br \/>\nKlebanoff distortions. In the fully turbulent boundary layer,<br \/>\nstatistical evidence is presented that the interface is locally<br \/>\nmodulated by the large-scale velocity perturbations in both the<br \/>\nstreamwise and spanwise directions. The modulation is different when<br \/>\nthe coherent structure is high- versus low-speed motion: high-speed<br \/>\nstructures lead to a wedgeshaped deformation of the T\/NT interface,<br \/>\nwhich causes an anti-correlation between the angles of the interface<br \/>\nand the internal shear layer. On the other hand, low-speed structures<br \/>\nare correlated with crests in the interface. Finally, the sudden<br \/>\nchanges in turbulence statistics across the interface are in line with<br \/>\nthe changes in the population of low-speed structures, which consist<br \/>\nof slower mean streamwise velocity and stronger turbulence than the<br \/>\nhigh-speed counterparts.<\/p>\n<p>+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;+&#8211;<\/p>\n<p>\u4e16\u8a71\u4eba\uff1a\u5c71\u7530 \u9053\u592b(\u4eac\u5927\u6570\u7406\u7814)\uff0c \u7af9\u5e83 \u771f\u4e00\uff08\u4eac\u5927\u6570\u7406\u7814\uff09\uff0c<br \/>\n\u3000\u3000\u3000\u3000\u85e4 \u5b9a\u7fa9(\u4eac\u5927)\uff0c\u677e\u672c \u525b(\u4eac\u5927\u7406)<br \/>\n\u30a2\u30c9\u30d0\u30a4\u30b6\u30fc\uff1a\u6c34\u5cf6 \u4e8c\u90ce(\u540c\u5fd7\u793e\u5927\u5de5)\uff0c \u4f59\u7530 \u6210\u7537\uff08\u4eac\u5927\u7406\uff09<br \/>\n\u9023\u7d61\u5148\uff1a\u5c71\u7530\u9053\u592b yamada_at_kurims.kyoto-u.ac.jp<br \/>\n=========================================================<\/p>\n","protected":false},"excerpt":{"rendered":"<p>\u7686\u69d8\u30016\/26\u65e5(\u6708)\u306e\u6d41\u4f53\u529b\u5b66\u30bb\u30df\u30ca\u30fc\u3092\u5fa1\u6848\u5185\u3044\u305f\u3057\u307e\u3059\u3002 \u5fa1\u6765\u8074\u6b53\u8fce\u3044\u305f\u3057\u307e\u3059\u3002 \u65e5\u6642\uff1a2016\u5e74 6\u6708 26\u65e5\uff08\u6708\uff09 15:00 \u304b\u3089 16:30 \u5834\u6240\uff1a \u4eac\u90fd\u5927\u5b66 \u6570\u7406\u89e3\u6790\u7814\u7a76\u6240 204\u53f7\u5ba4 \u8b1b\u5e2b\uff1a Prof.  [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[47],"tags":[],"class_list":["post-871","post","type-post","status-publish","format-standard","hentry","category-47"],"_links":{"self":[{"href":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/index.php?rest_route=\/wp\/v2\/posts\/871","targetHints":{"allow":["GET"]}}],"collection":[{"href":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=871"}],"version-history":[{"count":4,"href":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/index.php?rest_route=\/wp\/v2\/posts\/871\/revisions"}],"predecessor-version":[{"id":875,"href":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/index.php?rest_route=\/wp\/v2\/posts\/871\/revisions\/875"}],"wp:attachment":[{"href":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=871"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=871"},{"taxonomy":"post_tag","embeddable":true,"href":"http:\/\/kyoryu.scphys.kyoto-u.ac.jp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=871"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}