{"id":282,"date":"2020-04-14T22:58:46","date_gmt":"2020-04-14T22:58:46","guid":{"rendered":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/?page_id=282"},"modified":"2026-05-13T07:28:59","modified_gmt":"2026-05-13T07:28:59","slug":"torsionpendulum","status":"publish","type":"page","link":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/exhibits\/mechanics\/torsionpendulum\/","title":{"rendered":"Torsion Pendulum"},"content":{"rendered":"<h1 style=\"margin-top:var(--wp--preset--spacing--50);margin-bottom:var(--wp--preset--spacing--20)\" class=\"is-style-mini-bar wp-block-post-title\">Torsion Pendulum<\/h1>\n\n\n<div class=\"wp-block-group alignfull has-base-background-color has-background has-global-padding is-layout-constrained wp-block-group-is-layout-constrained\" style=\"margin-top:0;margin-bottom:0;padding-top:var(--wp--preset--spacing--40);padding-bottom:var(--wp--preset--spacing--60)\">\n<div class=\"wp-block-columns alignnone is-layout-flex wp-container-core-columns-is-layout-b4b75a54 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<div class=\"wp-block-group is-layout-constrained has-global-padding wp-block-group-is-layout-constrained\">\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-b4b75a54 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"400\" height=\"300\" src=\"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-content\/uploads\/sites\/10\/2020\/04\/TorstionPen-1i.jpg\" alt=\"\" class=\"wp-image-283\" srcset=\"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-content\/uploads\/sites\/10\/2020\/04\/TorstionPen-1i.jpg 400w, https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-content\/uploads\/sites\/10\/2020\/04\/TorstionPen-1i-300x225.jpg 300w\" sizes=\"auto, (max-width: 400px) 100vw, 400px\" \/><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"400\" height=\"300\" src=\"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-content\/uploads\/sites\/10\/2020\/04\/TorstionPenl-2i.jpg\" alt=\"\" class=\"wp-image-284\" srcset=\"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-content\/uploads\/sites\/10\/2020\/04\/TorstionPenl-2i.jpg 400w, https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-content\/uploads\/sites\/10\/2020\/04\/TorstionPenl-2i-300x225.jpg 300w\" sizes=\"auto, (max-width: 400px) 100vw, 400px\" \/><\/figure>\n<\/div>\n<\/div>\n\n\n\n<p class=\"wp-block-paragraph\">&nbsp;<\/p>\n\n\n\n<p class=\"wp-block-paragraph\">In torsion pendulums (like the one used in some clocks), the oscillation speed depends on the moment of inertia of the pendulum system and the spring constant of the wire, which is a measure of how torque is required to twist the wire through some angle. (See the <a href=\"..\/RotatingPlatform\"><em>Angular Momentum Turntable exhibit<\/em> <\/a>for more on the moment of inertia.)<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong><u>Experiment 1:<\/u><\/strong> <strong><u>WHAT TO DO:<\/u><\/strong><\/p>\n\n\n\n<ol class=\"wp-block-list is-style-more-space\">\n<li>Place the two <strong>large<\/strong> masses on the <strong>outer<\/strong> two pins of the torsion arm.<\/li>\n\n\n\n<li>Pull one side of the torsion arm towards you a <u>small<\/u> distance and then let it go.<\/li>\n\n\n\n<li>Count the time it takes the arm to make ten oscillations.<\/li>\n\n\n\n<li>Replace the large masses with the two small masses in the same spots.<\/li>\n\n\n\n<li>Pull one side of the torsion arm towards you the same small distance as before and let it go.<\/li>\n\n\n\n<li>Count the time it takes the arm to make ten oscillations.<\/li>\n<\/ol>\n\n\n\n<p class=\"wp-block-paragraph\"><strong><u>HOW DO THE OSCILLATION TIMES (PERIODS) COMPARE?<\/u><\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Answer: The period of the torsion arm with the larger masses is twice as long as the period of the arm with the smaller masses.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong><u>Experiment 2:<\/u><\/strong> <strong><u>WHAT TO DO:<\/u><\/strong><\/p>\n\n\n\n<ol class=\"wp-block-list is-style-more-space\">\n<li>Put the <strong>small<\/strong> masses on the same <strong>outer<\/strong> two pins of the torsion arm.<\/li>\n\n\n\n<li>Pull one side of the torsion arm towards you a small distance and then let it go.<\/li>\n\n\n\n<li>Count the time it takes the arm to make ten oscillations.<\/li>\n\n\n\n<li>Remove the small masses.<\/li>\n\n\n\n<li>Place the two <strong>large<\/strong> masses on the <strong>INNER<\/strong> two pins of the torsion arm.<\/li>\n\n\n\n<li>Pull one side of the torsion arm towards you the same small distance as before and let it go.<\/li>\n\n\n\n<li>Count the time it takes the arm to make ten oscillations.<\/li>\n<\/ol>\n\n\n\n<p class=\"wp-block-paragraph\"><strong><u>HOW DO THE OSCILLATION TIMES (PERIODS) COMPARE?<\/u><\/strong><\/p>\n\n\n\n<p class=\"wp-block-paragraph\">Answer: The period of the torsion arm with the smaller masses is equal to the period of the torsion arm with the larger masses.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><strong><u>What is going on?<\/u><\/strong> The moment of inertia, <em>I<\/em>, depends on the mass on the pendulum and its distance from the center of rotation of the pendulum. A smaller the moment of inertia increases the oscillation frequency and decreases the period of the pendulum. In Exp.1, the pendulum has a <u>higher <em>I<\/em><\/u> with the larger masses than with the small, so the period is <u>longer<\/u> than with the small masses. In Exp. 2, the moment of inertia for the small masses at a big distance is equal to the moment of inertia for the big masses at a small distance, so the periods are the <u>same<\/u> in both cases.<\/p>\n\n\n<div style=\"font-size: 1.125rem\" class=\"is-style-blockquote wp-block-uw-blocks-uw-quote\">\n\t<blockquote><em>Original 1918 Museum Exhibit<\/em><\/blockquote>\n\t<div class=\"uw-quote-bottom-container\">\n\t\t\t<\/div>\n<\/div>\n\n\n\n<p class=\"wp-block-paragraph\"><i><b><a href=\"https:\/\/wiki.physics.wisc.edu\/facultywiki\/Demonstrations\">Physics Lecture Demonstration Database<\/a><\/b><\/i><\/p>\n\n\n\n<ul class=\"wp-block-list is-style-more-space\">\n<li><p id=\"Torsion_Pendulum.2C_3A10.30\"><a href=\"https:\/\/wiki.physics.wisc.edu\/facultywiki\/Torsion_Pendulum\">Torsion Pendulum, 3A10.30<\/a><\/p><br><\/li>\n<\/ul>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>&nbsp; In torsion pendulums (like the one used in some clocks), the oscillation speed depends on the moment of inertia of the pendulum system and the spring constant of the wire, which is a measure of how torque is required to twist the wire through some angle. (See the Angular Momentum Turntable exhibit for more &hellip;<\/p>\n","protected":false},"author":2,"featured_media":0,"parent":50,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_uw_migration_status":"complete","_uw_gutenberg_post_content_before_migration":"","_uw_seo_meta_title":"","_uw_seo_meta_description":"","_uw_seo_twitter_card_type":"","_uw_seo_meta_image":"","_uw_seo_meta_image_url":"","_uw_seo_meta_image_sizes":[],"_uw_seo_custom_meta_tags":[],"footnotes":""},"class_list":["post-282","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-json\/wp\/v2\/pages\/282","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-json\/wp\/v2\/users\/2"}],"replies":[{"embeddable":true,"href":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-json\/wp\/v2\/comments?post=282"}],"version-history":[{"count":8,"href":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-json\/wp\/v2\/pages\/282\/revisions"}],"predecessor-version":[{"id":1013,"href":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-json\/wp\/v2\/pages\/282\/revisions\/1013"}],"up":[{"embeddable":true,"href":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-json\/wp\/v2\/pages\/50"}],"wp:attachment":[{"href":"https:\/\/wp.physics.wisc.edu\/ingersollmuseum\/wp-json\/wp\/v2\/media?parent=282"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}