{"id":31,"date":"2016-01-11T13:15:33","date_gmt":"2016-01-11T13:15:33","guid":{"rendered":"http:\/\/192.168.142.227\/memocs\/?p=31"},"modified":"2018-12-17T10:09:14","modified_gmt":"2018-12-17T10:09:14","slug":"corsi-di-dottorato","status":"publish","type":"post","link":"http:\/\/memocscenter.univaq.it\/memocs\/en\/attivita\/corsi-di-dottorato\/","title":{"rendered":"PHD Courses"},"content":{"rendered":"<div style=\"width: 80%; text-align: center; margin-left: auto; margin-right: auto; margin-bottom: 20px;\">\n<span style=\"font-family: georgia, palatino, serif; font-size: 18pt;\">Analytical Continuum Mechanics and Applications<\/span><\/p>\n<p><span style=\"font-family: georgia, palatino, serif; font-size: 16pt;\">(Prof. F. dell\u2019Isola)<\/span><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Space of Configurations and the problem of determining the Equation of Motion<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/sGClklKhu8A\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Action Functional and Lagrange Equations for systems<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/C6TlzcnNtRA\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Lagrangian action for the system constituted by two interacting particles<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/YvqXi4OJ2wY\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Piola\u2019s unitary description of the kinematics of rigid and deformable mechanical systems<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/up2WoqFKnpw\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">An invitation to Levi-Civita Ricci Tensor Algebra and Calculus.<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/ZybejdhYCn8\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">A Gramscian digression In Search of the Educational Principle.<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/BZ5jZwt9IR8\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Independence of energy from the observer<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/_nL9lXPZZL4\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Derivation of Eulerian description form general Lagrangian formulation.<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/25_h3HN5_o4\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Cauchy Tetrahedron argument, Part I.<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/Hra2iuFXmPc\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Cauchy Tetrahedron argument, Part II.<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/DYtPJw67ENc\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Introduction to second gradient continua<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/DX8pfWW_feg\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Capillary Fluids<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/yWnBqBY6cbQ\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Invariants<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/48OQ9JNe2o4\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Representation of isotropic scalar functions<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/LE7NrGb3p8o\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Isotropic constitutive relations, Part I<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/2w447FM_TKU\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Isotropic constitutive relations, Part II<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/K51Kro9yeXA\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>\n<div class=\"phd\">\n<p class=\"phd-title\">Linearization procedure in continuum mechanics<\/p>\n<p><iframe loading=\"lazy\" class=\"phd-video\" src=\"\/\/www.youtube.com\/embed\/nNFTV2Ln9lk\" width=\"300\" height=\"150\" allowfullscreen=\"allowfullscreen\"><\/iframe><\/p>\n<\/div>","protected":false},"excerpt":{"rendered":"<p>Analytical Continuum Mechanics and Applications (Prof. F. dell\u2019Isola) Space of Configurations and the problem of determining the Equation of Motion Action Functional and Lagrange Equations for systems Lagrangian action for the system constituted by two interacting particles Piola\u2019s unitary description of the kinematics of rigid and deformable mechanical systems An &hellip;<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":[],"categories":[6],"tags":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v20.5 - https:\/\/yoast.com\/wordpress\/plugins\/seo\/ -->\n<title>PHD Courses - M&amp;MoCS<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"http:\/\/memocscenter.univaq.it\/memocs\/en\/attivita\/corsi-di-dottorato\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"PHD Courses - M&amp;MoCS\" \/>\n<meta property=\"og:description\" content=\"Analytical Continuum Mechanics and Applications (Prof. F. dell\u2019Isola) Space of Configurations and the problem of determining the Equation of Motion Action Functional and Lagrange Equations for systems Lagrangian action for the system constituted by two interacting particles Piola\u2019s unitary description of the kinematics of rigid and deformable mechanical systems An &hellip;\" \/>\n<meta property=\"og:url\" content=\"http:\/\/memocscenter.univaq.it\/memocs\/en\/attivita\/corsi-di-dottorato\/\" \/>\n<meta property=\"og:site_name\" content=\"M&amp;MoCS\" \/>\n<meta property=\"article:published_time\" content=\"2016-01-11T13:15:33+00:00\" \/>\n<meta property=\"article:modified_time\" content=\"2018-12-17T10:09:14+00:00\" \/>\n<meta name=\"author\" content=\"admin\" \/>\n<meta name=\"twitter:card\" content=\"summary_large_image\" \/>\n<meta name=\"twitter:label1\" content=\"Written by\" \/>\n\t<meta name=\"twitter:data1\" content=\"admin\" \/>\n\t<meta name=\"twitter:label2\" content=\"Est. reading time\" \/>\n\t<meta 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