{"id":418,"date":"2016-03-22T19:34:40","date_gmt":"2016-03-22T16:34:40","guid":{"rendered":"https:\/\/cfd.spbstu.ru\/wp_agarbaruk\/?page_id=418"},"modified":"2018-09-17T12:50:14","modified_gmt":"2018-09-17T09:50:14","slug":"practice","status":"publish","type":"page","link":"https:\/\/cfd.spb.ru\/agarbaruk\/lecture\/srs_methods\/practice\/","title":{"rendered":"\u0420\u0430\u0441\u0447\u0435\u0442\u043d\u043e\u0435 \u0437\u0430\u0434\u0430\u043d\u0438\u0435"},"content":{"rendered":"<p>\u0426\u0435\u043b\u044c\u044e \u043d\u0430\u0441\u0442\u043e\u044f\u0449\u0435\u0433\u043e \u0440\u0430\u0441\u0447\u0435\u0442\u043d\u043e\u0433\u043e \u0437\u0430\u0434\u0430\u043d\u0438\u044f \u044f\u0432\u043b\u044f\u0435\u0442\u0441\u044f \u043e\u0431\u0443\u0447\u0435\u043d\u0438\u0435 \u043f\u0440\u0430\u043a\u0442\u0438\u0447\u0435\u0441\u043a\u043e\u043c\u0443 \u043f\u0440\u0438\u043c\u0435\u043d\u0435\u043d\u0438\u044e \u0441\u043e\u0432\u0440\u0435\u043c\u0435\u043d\u043d\u044b\u0445 \u0432\u0438\u0445\u0440\u0435\u0440\u0430\u0437\u0440\u0435\u0448\u0430\u044e\u0449\u0438\u0445 \u043f\u043e\u0434\u0445\u043e\u0434\u043e\u0432.<\/p>\n<p>\u041d\u0435\u043e\u0431\u0445\u043e\u0434\u0438\u043c\u043e \u043f\u0440\u043e\u0432\u0435\u0441\u0442\u0438 \u0440\u0430\u0441\u0447\u0435\u0442 \u0443\u0441\u0442\u0430\u043d\u043e\u0432\u0438\u0432\u0448\u0435\u0433\u043e\u0441\u044f \u0442\u0435\u0447\u0435\u043d\u0438\u044f \u0432 \u043f\u043b\u043e\u0441\u043a\u043e\u043c \u043a\u0430\u043d\u0430\u043b\u0435 \u0438\u043b\u0438 \u043e\u0431\u0442\u0435\u043a\u0430\u043d\u0438\u044f \u0446\u0438\u043b\u0438\u043d\u0434\u0440\u0430 \u0441 \u043d\u0430\u0433\u0440\u0435\u0442\u043e\u0439 \u0441\u0442\u0435\u043d\u043a\u043e\u0439, \u0438\u0441\u0441\u043b\u0435\u0434\u043e\u0432\u0430\u0442\u044c \u0432\u043b\u0438\u044f\u043d\u0438\u0435 \u0440\u0430\u0437\u043b\u0438\u0447\u043d\u044b\u0445 \u043f\u0430\u0440\u0430\u043c\u0435\u0442\u0440\u043e\u0432 (\u0432 \u0437\u0430\u0432\u0438\u0441\u0438\u043c\u043e\u0441\u0442\u0438 \u043e\u0442 \u0432\u0430\u0440\u0438\u0430\u043d\u0442\u0430) \u0438 \u043f\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u0438\u0442\u044c \u043e\u0442\u0447\u0435\u0442 \u043f\u043e \u043f\u0440\u043e\u0434\u0435\u043b\u0430\u043d\u043d\u043e\u0439 \u0440\u0430\u0431\u043e\u0442\u0435.<\/p>\n<p>\u0412\u0430\u0440\u0438\u0430\u043d\u0442\u044b \u0440\u0430\u0441\u0447\u0435\u0442\u043d\u044b\u0445 \u0437\u0430\u0434\u0430\u043d\u0438\u0439 \u043f\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043b\u0435\u043d\u044b <a href=\"\/agarbaruk\/lecture\/modern_methods\/practice\/formulation\/\">\u0437\u0434\u0435\u0441\u044c<\/a>.<\/p>\n<p>\u0412 \u043f\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043b\u0435\u043d\u043d\u044b\u0445 \u043d\u0438\u0436\u0435 \u0434\u043e\u043a\u0443\u043c\u0435\u043d\u0442\u0430\u0445 \u043c\u043e\u0436\u043d\u043e \u043d\u0430\u0439\u0442\u0438 \u043c\u0435\u0442\u043e\u0434\u0438\u0447\u0435\u0441\u043a\u0438\u0435 \u0443\u043a\u0430\u0437\u0430\u043d\u0438\u044f \u043f\u043e \u0432\u044b\u043f\u043e\u043b\u043d\u0435\u043d\u0438\u044e \u0440\u0430\u0441\u0447\u0435\u0442\u043d\u043e\u0433\u043e \u0437\u0430\u0434\u0430\u043d\u0438\u044f \u0438 \u0434\u0440\u0443\u0433\u0438\u0435 \u043f\u043e\u043b\u0435\u0437\u043d\u044b\u0435 \u0434\u043e\u043a\u0443\u043c\u0435\u043d\u0442\u044b.<\/p>\n<p><strong>\u042d\u0442\u0438 \u0434\u043e\u043a\u0443\u043c\u0435\u043d\u0442\u044b \u0438 \u0441\u0430\u0439\u0442\u044b \u043c\u043e\u0433\u0443\u0442 \u043f\u0440\u0438\u0433\u043e\u0434\u0438\u0442\u044c\u0441\u044f \u043f\u0440\u0438 \u0432\u044b\u043f\u043e\u043b\u043d\u0435\u043d\u0438\u0438\u0438 \u0440\u0430\u0441\u0447\u0435\u0442\u043d\u043e\u0433\u043e \u0437\u0430\u0434\u0430\u043d\u0438\u044f<\/strong><br \/>\n<img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-51\" src=\"\/agarbaruk\/imgs\/pdf.png\" alt=\"pdf\" width=\"16\" height=\"16\" \/><a href=\"\/agarbaruk\/doc\/1990_Niederschulte-Adrian-Hanratty_Experiments-in-Fluids-9.pdf\">1990_Niederschulte, Adrian, Hanratty_Experiments in Fluids 9<\/a><br \/>\nNiederschulte, M. A., Adrian, R. J., &amp; Hanratty, T. J. (1990). Measurements of turbulent flow in a channel at low Reynolds numbers. Experiments in Fluids, 9, 222\u2013230.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-51\" src=\"\/agarbaruk\/imgs\/pdf.png\" alt=\"pdf\" width=\"16\" height=\"16\" \/><a href=\"\/agarbaruk\/doc\/1999_Moser-Kim-Mansour_Direct-numerical-simulation-of-turbulent-channel-flow-up-to-Re-590.pdf\">1999_Moser, Kim, Mansour_Direct numerical simulation of turbulent channel flow up to Re= 590<\/a><br \/>\nMoser, R. D., Kim, J., &amp; Mansour, N. N. (1999). Direct numerical simulation of turbulent channel flow up to Re= 590. Phys. Fluids, 11(4), 943\u2013945.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-51\" src=\"\/agarbaruk\/imgs\/pdf.png\" alt=\"pdf\" width=\"16\" height=\"16\" \/><a href=\"\/agarbaruk\/doc\/2001_Abe-Kawamura-Matsuo_Direct-Numerical-Simulation-of-a-Fully-Developed-Turbulent-Channel-Flow-With-Respect-to-the-Reynolds-Number-D.pdf\">2001_Abe, Kawamura, Matsuo_Direct Numerical Simulation of a Fully Developed Turbulent Channel Flow With Respect to the Reynolds Number D<\/a><br \/>\nAbe, H., Kawamura, H., &amp; Matsuo, Y. (2001). Direct Numerical Simulation of a Fully Developed Turbulent Channel Flow With Respect to the Reynolds Number Dependence. Journal of Fluids Engineering, 123(2), 382.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-51\" src=\"\/agarbaruk\/imgs\/pdf.png\" alt=\"pdf\" width=\"16\" height=\"16\" \/><a href=\"\/agarbaruk\/doc\/2005_Hoyas-Jime\u0301nez_Scaling-of-the-velocity-fluctuations-in-turbulent-channels-up-to-Resub.pdf\">2005_Hoyas, Jime\u0301nez_Scaling of the velocity fluctuations in turbulent channels up to Resub<\/a><br \/>\n\u041f\u0440\u044f\u043c\u043e\u0435 \u0447\u0438\u0441\u043b\u0435\u043d\u043d\u043e\u0435 \u043c\u043e\u0434\u0435\u043b\u0438\u0440\u043e\u0432\u0430\u043d\u0438\u044f \u0442\u0435\u0447\u0435\u043d\u0438\u044f \u0432 \u043a\u0430\u043d\u0430\u043b\u0435<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-51\" src=\"\/agarbaruk\/imgs\/pdf.png\" alt=\"pdf\" width=\"16\" height=\"16\" \/><a href=\"\/agarbaruk\/doc\/2006_Hoyas-Jime\u0301nez_Scaling-of-the-velocity-fluctuations-in-turbulent-channels-up-to-Resub-\u03c42003.pdf\">2006_Hoyas, Jime\u0301nez_Scaling of the velocity fluctuations in turbulent channels up to Resub \u03c4=2003<\/a><br \/>\n\u041f\u0440\u044f\u043c\u043e\u0435 \u0447\u0438\u0441\u043b\u0435\u043d\u043d\u043e\u0435 \u043c\u043e\u0434\u0435\u043b\u0438\u0440\u043e\u0432\u0430\u043d\u0438\u0435 \u0442\u0435\u0447\u0435\u043d\u0438\u044f \u0432 \u043a\u0430\u043d\u0430\u043b\u0435 (Physics of Fluids)<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-51\" src=\"\/agarbaruk\/imgs\/pdf.png\" alt=\"pdf\" width=\"16\" height=\"16\" \/><a href=\"\/agarbaruk\/doc\/2014_Bernardini,%20Pirozzoli,%20Orlandi_Velocity%20statistics%20in%20turbulent%20channel%20flow%20up%20to.pdf\">2014_Bernardini, Pirozzoli, Orlandi_Velocity statistics in turbulent channel flow up to<\/a><br \/>\nBernardini, M., Pirozzoli, S., &amp; Orlandi, P. (2014). Velocity statistics in turbulent channel flow up to. Journal of Fluid Mechanics, 742, 171\u2013191.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-51\" src=\"\/agarbaruk\/imgs\/pdf.png\" alt=\"pdf\" width=\"16\" height=\"16\" \/><a href=\"\/agarbaruk\/doc\/channel_dns_moser_ret395.txt\">channel_dns_moser_ret395<\/a><br \/>\n\u0414\u0430\u043d\u043d\u044b\u0435 \u043f\u0440\u044f\u043c\u043e\u0433\u043e \u0447\u0438\u0441\u043b\u0435\u043d\u043d\u043e\u0433\u043e \u043c\u043e\u0434\u0435\u043b\u0438\u0440\u043e\u0432\u0430\u043d\u0438\u044f \u043f\u0440\u0438 \u0447\u0438\u0441\u043b\u0435 \u0420\u0435\u0439\u043d\u043e\u043b\u044c\u0434\u0441\u0430 400<\/p>\n<p><a href=\"http:\/\/newton.dma.uniroma1.it\/channel\/\">Channel flow DNS up to Re_tau=4000<\/a><br \/>\nChannel flow DNS up to Re_tau=4000<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-51\" src=\"\/agarbaruk\/imgs\/pdf.png\" alt=\"pdf\" width=\"16\" height=\"16\" \/><a href=\"\/agarbaruk\/doc\/ComputationalCases.pdf\">ComputationalCases<\/a><br \/>\n\u0412\u0430\u0440\u0438\u0430\u043d\u0442\u044b \u0440\u0430\u0441\u0447\u0435\u0442\u043d\u044b\u0445 \u0437\u0430\u0434\u0430\u043d\u0438\u0439<\/p>\n<p><a href=\"http:\/\/turbulence.ices.utexas.edu\/\">DNS channel data<\/a><br \/>\n\u0414\u0430\u043d\u043d\u044b\u0435 DNS \u043f\u043e \u0442\u0435\u0447\u0435\u043d\u0438\u044e \u0432 \u043a\u0430\u043d\u0430\u043b\u0435<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-51\" src=\"\/agarbaruk\/imgs\/pdf.png\" alt=\"pdf\" width=\"16\" height=\"16\" \/><a href=\"\/agarbaruk\/modern_methods\/Term11_project_channel.pdf\">Guide_channel_LES<\/a><br \/>\n\u041c\u0435\u0442\u043e\u0434\u0438\u0447\u0435\u0441\u043a\u0438\u0435 \u0443\u043a\u0430\u0437\u0430\u043d\u0438\u044f \u043f\u043e \u0432\u044b\u043f\u043e\u043b\u043d\u0435\u043d\u0438\u044e \u0440\u0430\u0441\u0447\u0435\u0442\u043d\u043e\u0433\u043e \u0437\u0430\u0434\u0430\u043d\u0438\u044f \u043f\u043e \u043a\u0443\u0440\u0441\u0443<\/p>\n<p><a href=\"http:\/\/www.thtlab.t.u-tokyo.ac.jp\/\">Tokyo University<\/a><br \/>\nTurbulence and Heat Transfer (Nobuhide Kasagi Lab.), Department of Mechanical Engineering. \u041d\u0430 \u0441\u0430\u0439\u0442\u0435 \u0434\u043e\u0441\u0442\u0443\u043f\u043d\u044b \u0434\u0430\u043d\u043d\u044b\u0435 DNS \u0438 \u044d\u043a\u0441\u043f\u0435\u0440\u0438\u043c\u0435\u043d\u0442\u0430<\/p>\n","protected":false},"excerpt":{"rendered":"<p>\u0426\u0435\u043b\u044c\u044e \u043d\u0430\u0441\u0442\u043e\u044f\u0449\u0435\u0433\u043e \u0440\u0430\u0441\u0447\u0435\u0442\u043d\u043e\u0433\u043e \u0437\u0430\u0434\u0430\u043d\u0438\u044f \u044f\u0432\u043b\u044f\u0435\u0442\u0441\u044f \u043e\u0431\u0443\u0447\u0435\u043d\u0438\u0435 \u043f\u0440\u0430\u043a\u0442\u0438\u0447\u0435\u0441\u043a\u043e\u043c\u0443 \u043f\u0440\u0438\u043c\u0435\u043d\u0435\u043d\u0438\u044e \u0441\u043e\u0432\u0440\u0435\u043c\u0435\u043d\u043d\u044b\u0445 \u0432\u0438\u0445\u0440\u0435\u0440\u0430\u0437\u0440\u0435\u0448\u0430\u044e\u0449\u0438\u0445 \u043f\u043e\u0434\u0445\u043e\u0434\u043e\u0432. \u041d\u0435\u043e\u0431\u0445\u043e\u0434\u0438\u043c\u043e \u043f\u0440\u043e\u0432\u0435\u0441\u0442\u0438 \u0440\u0430\u0441\u0447\u0435\u0442 \u0443\u0441\u0442\u0430\u043d\u043e\u0432\u0438\u0432\u0448\u0435\u0433\u043e\u0441\u044f \u0442\u0435\u0447\u0435\u043d\u0438\u044f \u0432 \u043f\u043b\u043e\u0441\u043a\u043e\u043c \u043a\u0430\u043d\u0430\u043b\u0435 \u0438\u043b\u0438 \u043e\u0431\u0442\u0435\u043a\u0430\u043d\u0438\u044f \u0446\u0438\u043b\u0438\u043d\u0434\u0440\u0430 \u0441 \u043d\u0430\u0433\u0440\u0435\u0442\u043e\u0439 \u0441\u0442\u0435\u043d\u043a\u043e\u0439, \u0438\u0441\u0441\u043b\u0435\u0434\u043e\u0432\u0430\u0442\u044c \u0432\u043b\u0438\u044f\u043d\u0438\u0435 \u0440\u0430\u0437\u043b\u0438\u0447\u043d\u044b\u0445 \u043f\u0430\u0440\u0430\u043c\u0435\u0442\u0440\u043e\u0432 (\u0432 \u0437\u0430\u0432\u0438\u0441\u0438\u043c\u043e\u0441\u0442\u0438 \u043e\u0442 \u0432\u0430\u0440\u0438\u0430\u043d\u0442\u0430) \u0438 \u043f\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u0438\u0442\u044c \u043e\u0442\u0447\u0435\u0442 \u043f\u043e \u043f\u0440\u043e\u0434\u0435\u043b\u0430\u043d\u043d\u043e\u0439 \u0440\u0430\u0431\u043e\u0442\u0435. \u0412\u0430\u0440\u0438\u0430\u043d\u0442\u044b \u0440\u0430\u0441\u0447\u0435\u0442\u043d\u044b\u0445 \u0437\u0430\u0434\u0430\u043d\u0438\u0439 \u043f\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043b\u0435\u043d\u044b \u0437\u0434\u0435\u0441\u044c. \u0412 \u043f\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043b\u0435\u043d\u043d\u044b\u0445 \u043d\u0438\u0436\u0435 \u0434\u043e\u043a\u0443\u043c\u0435\u043d\u0442\u0430\u0445 \u043c\u043e\u0436\u043d\u043e \u043d\u0430\u0439\u0442\u0438 \u043c\u0435\u0442\u043e\u0434\u0438\u0447\u0435\u0441\u043a\u0438\u0435 \u0443\u043a\u0430\u0437\u0430\u043d\u0438\u044f \u043f\u043e \u0432\u044b\u043f\u043e\u043b\u043d\u0435\u043d\u0438\u044e \u0440\u0430\u0441\u0447\u0435\u0442\u043d\u043e\u0433\u043e &hellip; <a href=\"https:\/\/cfd.spb.ru\/agarbaruk\/lecture\/srs_methods\/practice\/\" class=\"more-link\">Continue reading <span class=\"screen-reader-text\">\u0420\u0430\u0441\u0447\u0435\u0442\u043d\u043e\u0435 \u0437\u0430\u0434\u0430\u043d\u0438\u0435<\/span> <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":2,"featured_media":0,"parent":59,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-418","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/cfd.spb.ru\/agarbaruk\/wp-json\/wp\/v2\/pages\/418","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/cfd.spb.ru\/agarbaruk\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/cfd.spb.ru\/agarbaruk\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/cfd.spb.ru\/agarbaruk\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/cfd.spb.ru\/agarbaruk\/wp-json\/wp\/v2\/comments?post=418"}],"version-history":[{"count":0,"href":"https:\/\/cfd.spb.ru\/agarbaruk\/wp-json\/wp\/v2\/pages\/418\/revisions"}],"up":[{"embeddable":true,"href":"https:\/\/cfd.spb.ru\/agarbaruk\/wp-json\/wp\/v2\/pages\/59"}],"wp:attachment":[{"href":"https:\/\/cfd.spb.ru\/agarbaruk\/wp-json\/wp\/v2\/media?parent=418"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}