{"id":8793,"date":"2020-08-03T15:18:50","date_gmt":"2020-08-03T19:18:50","guid":{"rendered":"https:\/\/www.purdue.edu\/freeform\/me274\/?page_id=8793"},"modified":"2022-07-10T10:30:26","modified_gmt":"2022-07-10T14:30:26","slug":"two-story-building-response","status":"publish","type":"page","link":"https:\/\/www.purdue.edu\/freeform\/me274\/course-material\/animations\/two-story-building-response\/","title":{"rendered":"Two-story building response"},"content":{"rendered":"<p>Consider the two-story building below that is experiencing horizontal ground motion.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-7747 aligncenter\" style=\"border: 1px solid #000000\" src=\"https:\/\/www.purdue.edu\/freeform\/me274\/wp-content\/uploads\/sites\/15\/2020\/08\/Untitled.jpg\" alt=\"\" width=\"347\" height=\"240\" \/><\/p>\n<p>Suppose that we model the building as a single-degree-of-freedom oscillator with ground motion <em>y<\/em>(t). Let m be the mass of the second floor and k be the side-to-side stiffness of the exterior sidewalls. The side-to-side motion, x, can then be represented by the following for harmonically time-varying ground motion.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-7747 aligncenter\" style=\"border: 1px solid #000000\" src=\"https:\/\/www.purdue.edu\/freeform\/me274\/wp-content\/uploads\/sites\/15\/2020\/08\/Untitled-2-300x201.jpg\" alt=\"\" width=\"347\" height=\"240\" \/><\/p>\n<p>A plot of the steady-state amplitude of motion <em>A<\/em> is shown below as a function of the ground motion frequency Omega.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-7747 aligncenter\" style=\"border: 1px solid #000000\" src=\"https:\/\/www.purdue.edu\/freeform\/me274\/wp-content\/uploads\/sites\/15\/2020\/08\/Untitled-3-300x208.jpg\" alt=\"\" width=\"347\" height=\"240\" \/><\/p>\n<p>Let&#8217;s consider several frequencies of ground motion, as described below.<\/p>\n<p><strong><em>Low frequency ground motion<\/em><\/strong><br \/>\nThe plot above shows that the building response in-phase with the ground motion, with the amplitude of motion for the building being roughly equal to that of the ground. That is, the second floor motion effectively tracks the motion of the ground. This is seen in the animation below for <em>Omega<\/em> &lt;&lt; <em>omega<\/em>_n.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter\" style=\"border: 1px solid #000000\" src=\"https:\/\/www.purdue.edu\/freeform\/me274\/wp-content\/uploads\/sites\/15\/2020\/08\/sdof_building_subresonance.gif\" width=\"621\" height=\"313\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><strong><em>Ground motion frequency near resonance<br \/>\n<\/em><\/strong>With Omega near omega_n, the amplitude of steady-state response becomes large. This is as shown in the animation below.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter\" style=\"border: 1px solid #000000\" src=\"https:\/\/www.purdue.edu\/freeform\/me274\/wp-content\/uploads\/sites\/15\/2020\/08\/sdof_building_atresonance.gif\" width=\"621\" height=\"313\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><strong><em>High frequency ground motion<\/em><\/strong><br \/>\nThe plot above shows that the building response out-of-phase with the ground motion, with the amplitude of motion for the building being small as compared to that of the ground. That is, the second floor motion is nearly zero. This is seen in the animation below for <em>Omega<\/em>\u00a0&gt;&gt;\u00a0<em>omega<\/em>_n.<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"aligncenter\" style=\"border: 1px solid #000000\" src=\"https:\/\/www.purdue.edu\/freeform\/me274\/wp-content\/uploads\/sites\/15\/2020\/08\/sdof_building_supresonance.gif\" width=\"621\" height=\"313\" \/><\/p>\n<p>&nbsp;<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Consider the two-story building below that is experiencing horizontal ground motion. Suppose that we model the building as a single-degree-of-freedom oscillator with ground motion y(t). Let m be the mass of the second floor and k be the side-to-side stiffness of the exterior sidewalls. The side-to-side motion, x, can then be represented by the following &hellip; <a href=\"https:\/\/www.purdue.edu\/freeform\/me274\/course-material\/animations\/two-story-building-response\/\" class=\"more-link\">Continue reading <span class=\"screen-reader-text\">Two-story building response<\/span> <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":10,"featured_media":0,"parent":14,"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-8793","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/www.purdue.edu\/freeform\/me274\/wp-json\/wp\/v2\/pages\/8793","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.purdue.edu\/freeform\/me274\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.purdue.edu\/freeform\/me274\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.purdue.edu\/freeform\/me274\/wp-json\/wp\/v2\/users\/10"}],"replies":[{"embeddable":true,"href":"https:\/\/www.purdue.edu\/freeform\/me274\/wp-json\/wp\/v2\/comments?post=8793"}],"version-history":[{"count":5,"href":"https:\/\/www.purdue.edu\/freeform\/me274\/wp-json\/wp\/v2\/pages\/8793\/revisions"}],"predecessor-version":[{"id":8796,"href":"https:\/\/www.purdue.edu\/freeform\/me274\/wp-json\/wp\/v2\/pages\/8793\/revisions\/8796"}],"up":[{"embeddable":true,"href":"https:\/\/www.purdue.edu\/freeform\/me274\/wp-json\/wp\/v2\/pages\/14"}],"wp:attachment":[{"href":"https:\/\/www.purdue.edu\/freeform\/me274\/wp-json\/wp\/v2\/media?parent=8793"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}