{"id":1066,"date":"2021-06-24T19:08:05","date_gmt":"2021-06-24T19:08:05","guid":{"rendered":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/?p=1066"},"modified":"2021-12-30T18:53:43","modified_gmt":"2021-12-30T18:53:43","slug":"section-4-4-v2","status":"publish","type":"post","link":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/2021\/06\/24\/section-4-4-v2\/","title":{"rendered":"Chapter 4: Measuring motion"},"content":{"rendered":"\n<h2 class=\"wp-block-heading\">4.4 Acceleration<\/h2>\n\n\n\n<p>If you closed your eyes and were transported to another location, you would not know what your new position is; we do not have a sense of position. If you closed your eyes and were moved at a constant speed, you also would not know. We do not have a sense of velocity, either. However, if your speed changed, or if your direction of motion changed, you would know\u2014we have a sense that detects <em>changes<\/em> in motion. This sense is how we stay balanced and is detected by organs in the inner ear. Large or sudden changes in motion may also be felt in your gut.<\/p>\n\n\n\n<p>Just like velocity is the rate of change of displacement, <em>acceleration<\/em> is the rate of change of velocity:<\/p>\n\n\n<p>\\[<br \/>\n  \\text{acceleration} = \\frac{\\text{change in velocity}}{\\text{change in time}}<br \/>\n\\]<\/p>\n\n\n\n<p>Or, in symbols (for motion along the \\(x\\) axis):<\/p>\n\n\n<p>\\[<br \/>\n  a_x = \\frac{\\Delta v_x}{\\Delta t} \\tag{4.4}<br \/>\n\\]<\/p>\n\n\n\n<p>The SI unit for acceleration is meters per second per second (m\/s\/s), more commonly expressed as meters per second squared (m\/s<sup>2<\/sup>). Since velocity is a vector, acceleration must also be a vector. For two-dimensional motion, we use the rate of change of each component of the velocity:<\/p>\n\n\n<p>\\[<br \/>\n\\vec{a} = \\underbrace{\\left(\\frac{\\Delta v_x}{\\Delta t}\\right)}_{a_x}\\hat{x} + \\underbrace{\\left(\\frac{\\Delta v_y}{\\Delta t}\\right)}_{a_y}\\hat{y} \\tag{4.5}<br \/>\n\\]<\/p>\n\n\n\n<p>However, the direction of acceleration alone does not tell you anything about which direction you are traveling; it only tells you how the velocity is <em>changing<\/em>. If your acceleration is in the same direction as your velocity (whether that is positive or negative) you are &#8220;speeding up;&#8221; the magnitude of your velocity is increasing. Conversely, if your acceleration is in the opposite direction as your velocity, you are &#8220;slowing down.&#8221; (In physics we generally do not use the term &#8220;deceleration.&#8221;) This is summarized for one-dimensional motion in the table below.<\/p>\n\n\n\n<figure class=\"wp-block-table aligncenter is-style-stripes\"><table><thead><tr><th>Direction of \\(\\vec{v}\\)<\/th><th>Direction of \\(\\vec{a}\\)<\/th><th>Speed (\\(v\\)) is&#8230;<\/th><\/tr><\/thead><tbody><tr><td>+<\/td><td>+<\/td><td>Increasing<\/td><\/tr><tr><td>+<\/td><td>&#8211;<\/td><td>Decreasing<\/td><\/tr><tr><td>&#8211;<\/td><td>+<\/td><td>Decreasing<\/td><\/tr><tr><td>&#8211;<\/td><td>&#8211;<\/td><td>Increasing<\/td><\/tr><\/tbody><\/table><figcaption>Table summarizing the relationship between direction of velocity, direction of acceleration, and speed.<\/figcaption><\/figure>\n\n\n\n<h4 class=\"wp-block-heading\">practice 4.8<\/h4>\n\n\n\n<!-- iframe plugin v.6.0 wordpress.org\/plugins\/iframe\/ -->\n<iframe loading=\"lazy\" src=\"https:\/\/my.compclassnotes.com\/canonical\/PHYS110\/PHYS110_book_ch4v2_prac_v2\" width=\"100%\" height=\"600\" marginwidth=\"0\" marginheight=\"0\" scrolling=\"yes\" class=\"iframe-class\" frameborder=\"0\"><\/iframe>\n\n\n\n\n<h4 class=\"wp-block-heading\">Practice 4.9<\/h4>\n\n\n\n<!-- iframe plugin v.6.0 wordpress.org\/plugins\/iframe\/ -->\n<iframe loading=\"lazy\" src=\"https:\/\/my.compclassnotes.com\/canonical\/PHYS110\/PHYS110_book_chapter4_prac_q2\" width=\"100%\" height=\"600\" marginwidth=\"0\" marginheight=\"0\" scrolling=\"yes\" class=\"iframe-class\" frameborder=\"0\"><\/iframe>\n\n\n\n\n<h4 class=\"wp-block-heading\">Practice 4.10<\/h4>\n\n\n\n<!-- iframe plugin v.6.0 wordpress.org\/plugins\/iframe\/ -->\n<iframe loading=\"lazy\" src=\"https:\/\/my.compclassnotes.com\/canonical\/PHYS110\/PHYS110_book_chapter4_prac_q3\" width=\"100%\" height=\"600\" marginwidth=\"0\" marginheight=\"0\" scrolling=\"yes\" class=\"iframe-class\" frameborder=\"0\"><\/iframe>\n\n\n\n\n<h3 class=\"wp-block-heading\">4.4.1 Determining acceleration from a velocity vs time graph<\/h3>\n\n\n\n<p>Just as we could produce a velocity vs. time plot from position vs. time data, we can take our knowledge of how an object&#8217;s velocity is changing with time, and produce an acceleration vs. time graph. In the case of constant velocity (such as in the figures of the <a rel=\"noreferrer noopener\" href=\"https:\/\/books.compclassnotes.com\/rothphys110-2e\/2021\/06\/24\/section-4-3-v2\/\" target=\"_blank\">previous section<\/a>), that graph would simply be a straight line at \\(a = 0\\).<\/p>\n\n\n\n<p>You&#8217;ll notice that the mathematics involved here are exactly the same as what we used to create velocity graphs from position graphs! So, the <a rel=\"noreferrer noopener\" href=\"https:\/\/books.compclassnotes.com\/rothphys110-2e\/2021\/06\/24\/section-4-3-v2\/\" target=\"_blank\">section 4.3<\/a> example and practice problems will build the exact same skills as you need for this material. This is one of the beauties of mathematics; the same math can describe different physical situations.<\/p>\n\n\n\n","protected":false},"excerpt":{"rendered":"<p>4.4 Acceleration If you closed your eyes and were transported to another location, you would not know what your new position is; we do not have a sense of position. If you closed your eyes and were moved at a <span class=\"readmore\"><a href=\"https:\/\/books.compclassnotes.com\/rothphys110-2e\/2021\/06\/24\/section-4-4-v2\/\">Continue Reading<\/a><\/span><\/p>\n","protected":false},"author":3,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[1],"tags":[],"class_list":["post-1066","post","type-post","status-publish","format-standard","hentry","category-uncategorized"],"_links":{"self":[{"href":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/wp-json\/wp\/v2\/posts\/1066","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/wp-json\/wp\/v2\/comments?post=1066"}],"version-history":[{"count":9,"href":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/wp-json\/wp\/v2\/posts\/1066\/revisions"}],"predecessor-version":[{"id":1621,"href":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/wp-json\/wp\/v2\/posts\/1066\/revisions\/1621"}],"wp:attachment":[{"href":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/wp-json\/wp\/v2\/media?parent=1066"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/wp-json\/wp\/v2\/categories?post=1066"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/books.compclassnotes.com\/rothphys110-2e\/wp-json\/wp\/v2\/tags?post=1066"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}