![\"\"](\"https:\/\/commons.princeton.edu\/josephhenry\/wp-content\/uploads\/sites\/71\/2024\/07\/Screenshot-2024-07-12-125032.png\")
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Oscillating compass needle – July 8 2024 – COMSOL FILE Version 6.2<\/a><\/p>\n The model above features an oscillating bar below a fixed bar. The bar oscillates due to an applied body force of 0.1N\/m. This is slightly larger than the calculated k=0.067N\/m. The reason for this disparity is the bar swings at a large enough angle for the amplitude to influence the force calculation. With small angles, the restoring force is approximately linear, however, restoring force = F = mg sin(\u0398). Therefore at larger angles, the restoring force can no longer be approximated linearly and no longer follows sqrt(k\/m).<\/p>\n Oscillation frequency = \u03c9[rad\/sec] \u03c9=0.924 rad\/s Oscillating compass needle – July 8 2024 – COMSOL FILE Version 6.2 The model above features an oscillating bar below a fixed bar. The bar oscillates due to an applied body force of 0.1N\/m. This is slightly larger than the calculated k=0.067N\/m. The reason for this disparity is the bar swings at a large … Continue reading “Finding Force on Rotating Bar from Oscillation Frequency”<\/span><\/a><\/p>\n","protected":false},"author":6118,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"categories":[],"tags":[],"class_list":["post-4704","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/commons.princeton.edu\/josephhenry\/wp-json\/wp\/v2\/pages\/4704","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/commons.princeton.edu\/josephhenry\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/commons.princeton.edu\/josephhenry\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/commons.princeton.edu\/josephhenry\/wp-json\/wp\/v2\/users\/6118"}],"replies":[{"embeddable":true,"href":"https:\/\/commons.princeton.edu\/josephhenry\/wp-json\/wp\/v2\/comments?post=4704"}],"version-history":[{"count":4,"href":"https:\/\/commons.princeton.edu\/josephhenry\/wp-json\/wp\/v2\/pages\/4704\/revisions"}],"predecessor-version":[{"id":4718,"href":"https:\/\/commons.princeton.edu\/josephhenry\/wp-json\/wp\/v2\/pages\/4704\/revisions\/4718"}],"wp:attachment":[{"href":"https:\/\/commons.princeton.edu\/josephhenry\/wp-json\/wp\/v2\/media?parent=4704"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/commons.princeton.edu\/josephhenry\/wp-json\/wp\/v2\/categories?post=4704"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/commons.princeton.edu\/josephhenry\/wp-json\/wp\/v2\/tags?post=4704"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}
\n\u03c9 = sqrt(k\/m)<\/p>\n![\"\"](\"https:\/\/commons.princeton.edu\/josephhenry\/wp-content\/uploads\/sites\/71\/2024\/07\/Screenshot-2024-07-19-140516.png\")
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\nJ= 0.0785kg
\nk= \u03c92J
\nk= 0.067N\/m
\nSource:\u00a0http:\/\/hyperphysics.phy-astr.gsu.edu\/hbase\/shm2.html<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"