{"id":4705,"date":"2019-01-14T02:44:01","date_gmt":"2019-01-14T07:44:01","guid":{"rendered":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/?page_id=4705"},"modified":"2019-01-14T02:47:24","modified_gmt":"2019-01-14T07:47:24","slug":"three-dof-system-free-response","status":"publish","type":"page","link":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/chapter-ii-animations\/three-dof-system-free-response\/","title":{"rendered":"Three-DOF system"},"content":{"rendered":"<p><!--This file created 3\/26\/04 6:42 PM by Claris Home Page version 2.0-->Here we will look at the three natural modes of vibration for a three-DOF problem. Shown below is the response of the system for three different sets of initial conditions, each corresponding to one of the modes. Note that in all cases the response of the particles is synchronous (masses moving either in phase or completely out of phase with each other) and that the response is harmonic (of a single frequency).<\/p>\n<p><center>\u00a0<\/center><\/p>\n<table style=\"width: 605px;\" border=\"1\" width=\"500\" cellpadding=\"6\">\n<tbody>\n<tr>\n<td style=\"width: 318.125px;\"><center><img decoding=\"async\" src=\"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-content\/uploads\/sites\/18\/2019\/01\/mode_01.gif\" \/><\/center><\/td>\n<td style=\"width: 250.890625px;\"><center><b><i><span style=\"color: #af0000; font-family: Arial;\">FIRST MODE<\/span><\/i><\/b><\/center><span style=\"color: #af0000; font-family: Arial;\">Note that all masses are moving in phase with respect to each other. This is typical of the first natural mode of multi-DOF systems.<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 318.125px;\"><center><img decoding=\"async\" src=\"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-content\/uploads\/sites\/18\/2019\/01\/mode_02.gif\" \/><\/center><\/td>\n<td style=\"width: 250.890625px;\"><center><b><i><span style=\"color: #af0000; font-family: Arial;\">SECOND MODE<\/span><\/i><\/b><\/center><span style=\"color: #af0000; font-family: Arial;\">Here the blue and green particles are moving in phase with each other and the red particle is moving out of phase with the other two.<\/span><\/td>\n<\/tr>\n<tr>\n<td style=\"width: 318.125px;\"><center><img decoding=\"async\" src=\"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-content\/uploads\/sites\/18\/2019\/01\/mode_03.gif\" \/><\/center><\/td>\n<td style=\"width: 250.890625px;\"><center><b><i><span style=\"color: #af0000; font-family: Arial;\">THIRD MODE<\/span><\/i><\/b><\/center><span style=\"color: #af0000; font-family: Arial;\">Here the red and blue particles are moving in phase with each other and the green particle is moving out of phase with the other two.<\/span><\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n<p>&nbsp;<\/p>\n<hr \/>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Here we will look at the three natural modes of vibration for a three-DOF problem. Shown below is the response of the system for three different sets of initial conditions, each corresponding to one of the modes. Note that in all cases the response of the particles is synchronous (masses moving either in phase or &hellip; <a href=\"https:\/\/www.purdue.edu\/freeform\/ervibrations\/chapter-ii-animations\/three-dof-system-free-response\/\" class=\"more-link\">Continue reading <span class=\"screen-reader-text\">Three-DOF system<\/span> <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":10,"featured_media":0,"parent":4682,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"footnotes":""},"class_list":["post-4705","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-json\/wp\/v2\/pages\/4705","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-json\/wp\/v2\/users\/10"}],"replies":[{"embeddable":true,"href":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-json\/wp\/v2\/comments?post=4705"}],"version-history":[{"count":3,"href":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-json\/wp\/v2\/pages\/4705\/revisions"}],"predecessor-version":[{"id":4712,"href":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-json\/wp\/v2\/pages\/4705\/revisions\/4712"}],"up":[{"embeddable":true,"href":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-json\/wp\/v2\/pages\/4682"}],"wp:attachment":[{"href":"https:\/\/www.purdue.edu\/freeform\/ervibrations\/wp-json\/wp\/v2\/media?parent=4705"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}