{"id":632,"date":"2022-07-27T12:18:27","date_gmt":"2022-07-27T16:18:27","guid":{"rendered":"http:\/\/people.clas.ufl.edu\/ufhatch\/?p=632"},"modified":"2026-03-19T09:03:24","modified_gmt":"2026-03-19T13:03:24","slug":"newtonian-mechanics","status":"publish","type":"post","link":"https:\/\/people.clas.ufl.edu\/ufhatch\/2022\/07\/27\/newtonian-mechanics\/","title":{"rendered":"Newtonian Mechanics"},"content":{"rendered":"\r\n<section class=\"fullwidth-text-block\">\r\n\t<div class=\"container px-0 pt-5\">\r\n\t\t<div class=\"row align-items-start\">\r\n\t\t\t<div class=\"col-12\">\r\n\t\t\t\t\n<h1 class=\"wp-block-heading\">Newtonian Mechanics<\/h1>\n\n\n\n<ol class=\"wp-block-list\"><li><strong>Momentum = mv<\/strong>, where m = inertial mass of the body, v = velocity of the body<\/li>\n<li><strong>Newton&#8217;s Laws of Motion:<\/strong>\n<ol type=\"A\">\n<li>Every body persists in its state of rest or of uniform motion in a straight line, except or until that state is changed by some impressed force.<\/li>\n<li>The force acting on a body is numerically equal to the rate of change of momentum of the body, and the rate of change of momentum is in the direction of the applied force.\n<div class=\"tabbedinset\">\n<em>F = rate of change of (mv)<br>\nor,    F=ma when the mass, m, remains constant<br>\n<\/em>\n<\/div>\n<\/li>\n<li>To every action (some force exerted on body A by body B) there is an equal and opposite reaction (force exerted by body A on body B).<\/li>\n<\/ol>\n<\/li><li><strong>Uniform circular motion:<\/strong><br>\n<img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/people.clas.ufl.edu\/ufhatch\/files\/newtonMechanics.jpg\" alt=\"\" width=\"550\" height=\"183\" class=\"aligncenter size-full wp-image-633\" srcset=\"https:\/\/people.clas.ufl.edu\/ufhatch\/files\/newtonMechanics.jpg 550w, https:\/\/people.clas.ufl.edu\/ufhatch\/files\/newtonMechanics-300x100.jpg 300w, https:\/\/people.clas.ufl.edu\/ufhatch\/files\/newtonMechanics-414x138.jpg 414w\" sizes=\"auto, (max-width: 550px) 100vw, 550px\" \/><br>\n<br>\n<\/li>\n<li><strong>Newton&#8217;s Law of Universal Gravitation:<\/strong>\n<p>Newton eventually had the following information:<\/p>\n<ol type=\"A\">\n<li>Kepler&#8217;s laws of planetary motion:\n<ol>\n<li>Elliptical orbits, with the sun at one focus.<\/li>\n<li>Equal areas in equal times.<\/li>\n<li>For all planets,<\/li>\n<\/ol>\n<p>where p = planet&#8217;s period about the sun, R = average distance of planet from sun, k = a constant.\n<\/p><\/li>\n<li>The law of free fall\n<div class=\"tabbedinset\">\nwhere D = distance, T = time of fall, A = acceleration due to gravity.\n<\/div>\n<\/li>\n<li>Newton&#8217;s three laws of motion:\n<ol>\n<li>Law of Inertia.<\/li>\n<li>Law of relation between force, mass, and acceleration: F = ma.<\/li>\n<li>Law of action and reaction.<\/li>\n<\/ol>\n<\/li><li>Law of force necessary to keep a body moving uniformly in a circle:<\/li>\n<\/ol>\n<\/li><li>Newton assumed:\n<ol type=\"A\">\n<li>That the laws of motion hold everywhere in the universe;<\/li>\n<li>(initially) that the orbits of the planets were circular rather than elliptical.<\/li>\n<\/ol>\n<p>The result:<br>\nNewton&#8217;s Law of Universal Gravitation: Every body in the universe attracts every other body with a force directly proportional to the Foduct of their masses and inversely proportional to the square of the distance between them.<\/p><!--PARAGRAPH_SEPARATOR--><p>As a formula, this law is expressed as follows:<br>\nForce is equal to the Gravitational Constant times:  Mass one time Mass two, divided by the radius (distance) squared.<\/p><!--PARAGRAPH_SEPARATOR--><p>Where F = the force of attraction, m and M = the two masses, R = the distance between the two masses, and G = the universal constant of gravitation.<\/p><\/li><\/ol>\n\n\n\r\n\t\t\t<\/div>\r\n\t\t<\/div>\r\n\t<\/div>\r\n<\/section>\r\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":1262,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_acf_changed":false,"featured_post":"off","footnotes":"","_links_to":"","_links_to_target":""},"categories":[4,5],"tags":[],"class_list":["post-632","post","type-post","status-publish","format-standard","hentry","category-history-of-science","category-study-guide"],"acf":[],"_links":{"self":[{"href":"https:\/\/people.clas.ufl.edu\/ufhatch\/wp-json\/wp\/v2\/posts\/632","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/people.clas.ufl.edu\/ufhatch\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/people.clas.ufl.edu\/ufhatch\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/people.clas.ufl.edu\/ufhatch\/wp-json\/wp\/v2\/users\/1262"}],"replies":[{"embeddable":true,"href":"https:\/\/people.clas.ufl.edu\/ufhatch\/wp-json\/wp\/v2\/comments?post=632"}],"version-history":[{"count":6,"href":"https:\/\/people.clas.ufl.edu\/ufhatch\/wp-json\/wp\/v2\/posts\/632\/revisions"}],"predecessor-version":[{"id":1404,"href":"https:\/\/people.clas.ufl.edu\/ufhatch\/wp-json\/wp\/v2\/posts\/632\/revisions\/1404"}],"wp:attachment":[{"href":"https:\/\/people.clas.ufl.edu\/ufhatch\/wp-json\/wp\/v2\/media?parent=632"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/people.clas.ufl.edu\/ufhatch\/wp-json\/wp\/v2\/categories?post=632"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/people.clas.ufl.edu\/ufhatch\/wp-json\/wp\/v2\/tags?post=632"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}