{"id":861,"date":"2025-10-17T03:56:03","date_gmt":"2025-10-17T03:56:03","guid":{"rendered":"https:\/\/ibphysicswithrao.com\/home\/?p=861"},"modified":"2025-10-17T03:59:22","modified_gmt":"2025-10-17T03:59:22","slug":"suvat-vs-energy-methods","status":"publish","type":"post","link":"https:\/\/ibphysicswithrao.com\/home\/suvat-vs-energy-methods\/","title":{"rendered":"The SUVAT Shortcut is a Dead End: Why You Need the Energy Highway!"},"content":{"rendered":"\n<h3 class=\"wp-block-heading\">When Your Favorite &#8220;Shortcut&#8221; Fails<\/h3>\n\n\n\n<p>In physics, you learn a powerful set of &#8220;shortcut&#8221; formulas: the SUVAT equations. They are your trusted tools for problems with <strong>constant acceleration<\/strong>\u2014like a ball in freefall or a car speeding up steadily.<sup><\/sup> They\u2019re clean, simple, and effective.<\/p>\n\n\n\n<p>But what happens when the situation gets more complex? What if the force, and therefore the acceleration, is constantly changing? This is where many students hit a frustrating dead end. Suddenly, the SUVAT shortcut leads nowhere. This is the story of why we sometimes need to ignore the messy, moment-by-moment details of a journey and instead take a bigger, <strong>more powerful route: the Energy Highway.<\/strong><\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">The Problem: When Forces Aren&#8217;t Friendly<\/h3>\n\n\n\n<p>The single biggest limitation of the SUVAT equations is that they <em><strong>demand <\/strong><\/em>constant acceleration. This means the net force on the object must also be constant. <strong><em>But in the real world, many forces are variable.<\/em><\/strong><\/p>\n\n\n\n<p>In our last post, we explored the unique rhythm of <strong>Simple Harmonic Motion (SHM)<\/strong> and saw why SUVAT equations fail for it. The reason? A variable restoring force from the spring (F=\u2212kx). SHM is a perfect, specific example of the challenge we&#8217;re tackling today. But it&#8217;s just one type of variable force. This post offers a powerful solution\u2014<strong><em>The Energy Highway<\/em><\/strong>\u2014that works for a whole general class of these problems. While our SHM analysis focused on describing the <em>path<\/em> and <em>phase<\/em> of the motion over time, the energy method allows us to solve for speeds and positions without needing to track every moment of the journey.<\/p>\n\n\n\n<p>Consider this classic problem that highlights the issue:<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p>A compressed spring is used to launch an object along a horizontal frictionless surface. When the spring is no longer compressed, what determines the speed of the object?<\/p>\n<\/blockquote>\n\n\n\n<p>As the spring expands, its force on the object gets weaker and weaker. Since F=ma, if the force is changing, the <strong>acceleration is also changing<\/strong>. You can&#8217;t just pick one value for &#8216;a&#8217; and plug it into a SUVAT equation. So, how do we solve it? We need a different way of thinking. Watch this video to solve one such problem related to spring forces<\/p>\n\n\n\n<figure class=\"wp-block-embed is-type-video is-provider-youtube wp-block-embed-youtube wp-embed-aspect-16-9 wp-has-aspect-ratio\"><div class=\"wp-block-embed__wrapper\">\n<iframe title=\"8. A compressed spring is used to launch an object along a horizontal frictionless surface. When\" width=\"640\" height=\"360\" src=\"https:\/\/www.youtube.com\/embed\/b6mVzdodYkQ?feature=oembed\" frameborder=\"0\" allow=\"accelerometer; autoplay; clipboard-write; encrypted-media; gyroscope; picture-in-picture; web-share\" referrerpolicy=\"strict-origin-when-cross-origin\" allowfullscreen><\/iframe>\n<\/div><\/figure>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">The Historical Journey: From Constant Force to a Deeper Truth<\/h3>\n\n\n\n<p>Our understanding of motion was built over centuries, piece by piece.<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong>Galileo Galilei (Early 1600s):<\/strong> He was the first to show that, ignoring air resistance, all objects in freefall have the same <strong>constant acceleration<\/strong>. This brilliant discovery laid the foundation for the kind of thinking that produced the SUVAT equations.<\/li>\n\n\n\n<li><strong>Isaac Newton (Late 1600s):<\/strong> Newton gave us the master equation, F=ma, and with his invention of calculus, he provided the tools to derive the SUVAT equations from his laws. For any constant force, these equations were a triumph.<\/li>\n<\/ul>\n\n\n\n<p>But even Newton knew the universe was more complicated. The force from a spring isn&#8217;t constant. The gravitational force between planets changes with distance. <strong><em>Trying to use SUVAT for these problems is like trying to use a ruler to measure the coastline<\/em><\/strong>\u2014it&#8217;s the wrong tool for a complex job. Physicists needed a new perspective.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">The Breakthrough: The Unseen Constant<\/h3>\n\n\n\n<p>Instead of getting bogged down by changing forces, scientists started asking a different question: <strong><em>In a system, is there anything that doesn&#8217;t change? The answer was energy.<\/em><\/strong> This wasn&#8217;t a single &#8220;Eureka!&#8221; moment, but a gradual dawning of a profound truth during the Industrial Revolution, a time filled with steam engines, heat, and machines.<\/p>\n\n\n\n<h2 class=\"wp-block-heading\"><strong>James[1<\/strong><sup data-fn=\"2f98f665-8b7c-4352-94d8-fb3e0bdcae0b\" class=\"fn\"><a href=\"#2f98f665-8b7c-4352-94d8-fb3e0bdcae0b\" id=\"2f98f665-8b7c-4352-94d8-fb3e0bdcae0b-link\">1<\/a><\/sup><strong>] Prescott Joule&#8217;s Paddlewheel Experiment (1840):<\/strong> <\/h2>\n\n\n\n<div class=\"wp-block-group alignfull is-content-justification-center\" style=\"margin-top:0;margin-bottom:0;padding-top:calc( 0.5 * var(--wp--style--root--padding-right, var(--wp--custom--gap--horizontal)));padding-right:var(--wp--style--root--padding-right, var(--wp--custom--gap--horizontal));padding-bottom:calc( 0.5 * var(--wp--style--root--padding-right, var(--wp--custom--gap--horizontal)));padding-left:var(--wp--style--root--padding-left, var(--wp--custom--gap--horizontal))\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-container-core-group-is-layout-b073b61b wp-block-group-is-layout-constrained\">\n<div style=\"height:calc( 0.25 * var(--wp--style--root--padding-right, var(--wp--custom--gap--horizontal)))\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<div class=\"wp-block-columns alignwide are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-6aa4370a wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-image size-large is-resized\"><a href=\"https:\/\/blog.scienceandindustrymuseum.org.uk\/james-joules-energy\/\"><img fetchpriority=\"high\" decoding=\"async\" width=\"1024\" height=\"683\" src=\"https:\/\/ibphysicswithrao.com\/home\/wp-content\/uploads\/2025\/10\/paddlewheel-1024x683.png\" alt=\"\" class=\"wp-image-862\" style=\"width:313px;height:auto\" srcset=\"https:\/\/ibphysicswithrao.com\/home\/wp-content\/uploads\/2025\/10\/paddlewheel-1024x683.png 1024w, https:\/\/ibphysicswithrao.com\/home\/wp-content\/uploads\/2025\/10\/paddlewheel-300x200.png 300w, https:\/\/ibphysicswithrao.com\/home\/wp-content\/uploads\/2025\/10\/paddlewheel-768x512.png 768w, https:\/\/ibphysicswithrao.com\/home\/wp-content\/uploads\/2025\/10\/paddlewheel-600x400.png 600w, https:\/\/ibphysicswithrao.com\/home\/wp-content\/uploads\/2025\/10\/paddlewheel.png 1536w\" sizes=\"(max-width: 1024px) 100vw, 1024px\" \/><\/a><figcaption class=\"wp-element-caption\"><strong><span style=\"text-decoration: underline;\">Source<\/span><\/strong>: Padlet Wheel Experiment<\/figcaption><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\">\n<p>Joule was a meticulous experimentalist (and a brewer!). He was obsessed with the idea that energy wasn&#8217;t &#8220;lost&#8221; but simply changed form. In his most famous experiment, he used a falling weight to turn a paddlewheel inside an insulated barrel of water. He proved that the mechanical work done by the falling weight was directly converted into a specific amount of heat, which he measured with a tiny temperature increase in the water. \ud83d\udca7 He established the &#8220;mechanical equivalent of heat,&#8221; providing concrete, experimental proof that mechanical energy could transform into thermal energy in a predictable way.<\/p>\n<\/div>\n<\/div>\n\n\n\n<div style=\"height:calc( 0.25 * var(--wp--style--root--padding-right, var(--wp--custom--gap--horizontal)))\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n<\/div><\/div>\n\n\n\n<h2 class=\"wp-block-heading\">Helmholtz [2<sup data-fn=\"30051995-21f8-4d4d-8d50-913e5949eb65\" class=\"fn\"><a href=\"#30051995-21f8-4d4d-8d50-913e5949eb65\" id=\"30051995-21f8-4d4d-8d50-913e5949eb65-link\">2<\/a><\/sup>] Grand Theory (1840, Germany )<\/h2>\n\n\n\n<div class=\"wp-block-group alignfull is-content-justification-center\" style=\"margin-top:0;margin-bottom:0;padding-top:calc( 0.5 * var(--wp--style--root--padding-right, var(--wp--custom--gap--horizontal)));padding-right:var(--wp--style--root--padding-right, var(--wp--custom--gap--horizontal));padding-bottom:calc( 0.5 * var(--wp--style--root--padding-right, var(--wp--custom--gap--horizontal)));padding-left:var(--wp--style--root--padding-left, var(--wp--custom--gap--horizontal))\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-container-core-group-is-layout-b073b61b wp-block-group-is-layout-constrained\">\n<div style=\"height:calc( 0.25 * var(--wp--style--root--padding-right, var(--wp--custom--gap--horizontal)))\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<div class=\"wp-block-columns alignwide are-vertically-aligned-center is-layout-flex wp-container-core-columns-is-layout-6aa4370a wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\">\n<p>While Joule was proving the concept in his lab, Helmholtz, a physician and physicist, was crafting the grand theory. He started from a simple, powerful idea: a perpetual motion machine is impossible. From this single philosophical premise, he argued that a universal quantity\u2014what we now call energy\u2014must be conserved in all interactions of nature. In 1847, he published his work, mathematically unifying mechanics, heat, electricity, magnetism, and chemistry under the single umbrella of the <strong>Law of Conservation of Energy<\/strong>.<\/p>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\"><div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full is-resized\"><img decoding=\"async\" width=\"620\" height=\"844\" src=\"https:\/\/ibphysicswithrao.com\/home\/wp-content\/uploads\/2025\/10\/image-8.png\" alt=\"\" class=\"wp-image-864\" style=\"width:275px;height:auto\" srcset=\"https:\/\/ibphysicswithrao.com\/home\/wp-content\/uploads\/2025\/10\/image-8.png 620w, https:\/\/ibphysicswithrao.com\/home\/wp-content\/uploads\/2025\/10\/image-8-220x300.png 220w, https:\/\/ibphysicswithrao.com\/home\/wp-content\/uploads\/2025\/10\/image-8-600x817.png 600w\" sizes=\"(max-width: 620px) 100vw, 620px\" \/><figcaption class=\"wp-element-caption\">Herman Von Helmholtz, 1894<\/figcaption><\/figure><\/div><\/div>\n<\/div>\n\n\n\n<div style=\"height:calc( 0.25 * var(--wp--style--root--padding-right, var(--wp--custom--gap--horizontal)))\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n<\/div><\/div>\n\n\n\n<p>Together, Joule\u2019s tangible proof and Helmholtz\u2019s unifying theory cemented one of the most fundamental principles of the universe. This was the revolutionary breakthrough that opened up the <strong>Energy Highway<\/strong>. Now, physicists could bypass the messy details of variable forces and simply track the flow of this conserved quantity.<\/p>\n\n\n\n<p>Let&#8217;s go back to our spring problem.<\/p>\n\n\n\n<blockquote class=\"wp-block-quote is-layout-flow wp-block-quote-is-layout-flow\">\n<p><strong>Video Example:<\/strong> A horizontal spring of spring constant k and negligible mass is compressed through a distance y. What is the final speed of the mass?<\/p>\n<\/blockquote>\n\n\n\n<p>The SUVAT &#8220;dead end&#8221; forces you to think about the changing acceleration. The Energy Highway lets you bypass that completely:<\/p>\n\n\n\n<p><strong>Energy at the Start = Energy at the End<\/strong><\/p>\n\n\n\n<p>Initially, all the energy is stored in the compressed spring as <strong>Elastic Potential Energy (Ep\u200b)<\/strong>. At the end, after the mass is launched, all that energy has been converted into the <strong>Kinetic Energy (Ek\u200b)<\/strong> of the moving mass.<\/p>\n\n\n\n<p>A similar problem has been worked in this example, watch this video until the end to understand the method of cracking such problems<\/p>\n\n\n\n<figure class=\"wp-block-embed is-type-video is-provider-youtube wp-block-embed-youtube wp-embed-aspect-16-9 wp-has-aspect-ratio\"><div class=\"wp-block-embed__wrapper\">\n<iframe title=\"A horizontal spring of spring constant k and negligible mass is compressed through a distance y f\" width=\"640\" height=\"360\" src=\"https:\/\/www.youtube.com\/embed\/JnOLt-VpoHo?feature=oembed\" frameborder=\"0\" allow=\"accelerometer; autoplay; clipboard-write; encrypted-media; gyroscope; picture-in-picture; web-share\" referrerpolicy=\"strict-origin-when-cross-origin\" allowfullscreen><\/iframe>\n<\/div><\/figure>\n\n\n\n<p>Look at that! A problem that was impossible with SUVAT becomes a simple algebraic equation. This powerful approach works for a huge range of problems you&#8217;ll see, from masses hanging on springs to blocks being launched, as shown in our video solutions.<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">A Final Thought: Your Role as the Knower<\/h3>\n\n\n\n<p>In TOK, we learn that a <strong>model<\/strong> is a simplified representation of reality, powerful within its specific <strong>scope<\/strong>, but limited outside of it. The SUVAT equations are a fantastic model for the AOK of Natural Sciences, but only for the limited scope of constant acceleration.<\/p>\n\n\n\n<p>Recognizing this limitation isn&#8217;t a failure. It&#8217;s a crucial step in your development as a <strong>knower<\/strong>. It prompts you to ask a powerful <strong>knowledge question<\/strong>: <em>How does the scientific community decide when a model is no longer adequate?<\/em><\/p>\n\n\n\n<p>The shift from a purely force-based analysis to an energy-based one is a classic example of a <strong>paradigm shift<\/strong> in physics. It teaches us that knowledge isn&#8217;t static; it&#8217;s a dynamic process of finding better, more comprehensive models. The &#8220;Energy Highway&#8221; isn&#8217;t just a calculation trick; it&#8217;s a more fundamental and universal way of describing the cosmos.<\/p>\n\n\n\n<p>So, when you face a problem, don&#8217;t just search for a formula. First, analyze the situation. Ask yourself: Is the &#8220;shortcut&#8221; appropriate here, or do I need a more powerful framework? By choosing the right tool, you&#8217;re not just solving for &#8216;x&#8217;\u2014you&#8217;re engaging in the real work of a scientist. \ud83e\udde0<\/p>\n\n\n\n<p>To solve more such problems on variable forces, visit my collection of problems on variable forces by clicking the link below: <strong><a href=\"https:\/\/www.youtube.com\/playlist?list=PLckoYLuTGRA6YC-8Z8iUFmeJps0seMWM3\">VARIABLE FORCES PLAYLIST ON YOUTUBE<\/a><\/strong><\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Sources:<\/h2>\n\n\n<ol class=\"wp-block-footnotes\"><li id=\"2f98f665-8b7c-4352-94d8-fb3e0bdcae0b\"><a href=\"https:\/\/blog.scienceandindustrymuseum.org.uk\/james-joules-energy\/\">https:\/\/blog.scienceandindustrymuseum.org.uk\/james-joules-energy\/<\/a> <a href=\"#2f98f665-8b7c-4352-94d8-fb3e0bdcae0b-link\" aria-label=\"Jump to footnote reference 1\">\u21a9\ufe0e<\/a><\/li><li id=\"30051995-21f8-4d4d-8d50-913e5949eb65\"><a href=\"https:\/\/www.britannica.com\/biography\/Hermann-von-Helmholtz\/Later-life\">https:\/\/www.britannica.com\/biography\/Hermann-von-Helmholtz\/Later-life<\/a> <a href=\"#30051995-21f8-4d4d-8d50-913e5949eb65-link\" aria-label=\"Jump to footnote reference 2\">\u21a9\ufe0e<\/a><\/li><\/ol>\n\n\n<p><\/p>\n","protected":false},"excerpt":{"rendered":"<p>When Your Favorite &#8220;Shortcut&#8221; Fails In physics, you learn a powerful set of &#8220;shortcut&#8221; formulas: the SUVAT equations. They are your trusted tools for problems with constant acceleration\u2014like a ball in freefall or a car speeding up steadily. They\u2019re clean, simple, and effective. But what happens when the situation gets more complex? What if the force, and therefore the acceleration, is constantly changing? This is where many students hit a frustrating dead end. Suddenly, the SUVAT shortcut leads nowhere. This is the story of why we sometimes need to ignore the messy, moment-by-moment details of a journey and instead take a bigger, more powerful route: the Energy Highway. The Problem: When Forces Aren&#8217;t Friendly The single biggest limitation of the SUVAT equations is that they demand constant acceleration. This means the net force on the object must also be constant. But in the real world, many forces are variable. In our last post, we explored the unique rhythm of Simple Harmonic Motion (SHM) and saw why SUVAT equations fail for it. The reason? A variable restoring force from the spring (F=\u2212kx). SHM is a perfect, specific example of the challenge we&#8217;re tackling today. But it&#8217;s just one type of variable force. This post offers a powerful solution\u2014The Energy Highway\u2014that works for a whole general class of these problems. While our SHM analysis focused on describing the path and phase of the motion over time, the energy method allows us to solve for speeds and positions without needing to track every moment of the journey. Consider this classic problem that highlights the issue: A compressed spring is used to launch an object along a horizontal frictionless surface. When the spring is no longer compressed, what determines the speed of the object? As the spring expands, its force on the object gets weaker and weaker. Since F=ma, if the force is changing, the acceleration is also changing. You can&#8217;t just pick one value for &#8216;a&#8217; and plug it into a SUVAT equation. So, how do we solve it? We need a different way of thinking. Watch this video to solve one such problem related to spring forces The Historical Journey: From Constant Force to a Deeper Truth Our understanding of motion was built over centuries, piece by piece. But even Newton knew the universe was more complicated. The force from a spring isn&#8217;t constant. The gravitational force between planets changes with distance. Trying to use SUVAT for these problems is like trying to use a ruler to measure the coastline\u2014it&#8217;s the wrong tool for a complex job. Physicists needed a new perspective. The Breakthrough: The Unseen Constant Instead of getting bogged down by changing forces, scientists started asking a different question: In a system, is there anything that doesn&#8217;t change? The answer was energy. This wasn&#8217;t a single &#8220;Eureka!&#8221; moment, but a gradual dawning of a profound truth during the Industrial Revolution, a time filled with steam engines, heat, and machines. James[1] Prescott Joule&#8217;s Paddlewheel Experiment (1840): Joule was a meticulous experimentalist (and a brewer!). He was obsessed with the idea that energy wasn&#8217;t &#8220;lost&#8221; but simply changed form. In his most famous experiment, he used a falling weight to turn a paddlewheel inside an insulated barrel of water. He proved that the mechanical work done by the falling weight was directly converted into a specific amount of heat, which he measured with a tiny temperature increase in the water. \ud83d\udca7 He established the &#8220;mechanical equivalent of heat,&#8221; providing concrete, experimental proof that mechanical energy could transform into thermal energy in a predictable way. Helmholtz [2] Grand Theory (1840, Germany ) While Joule was proving the concept in his lab, Helmholtz, a physician and physicist, was crafting the grand theory. He started from a simple, powerful idea: a perpetual motion machine is impossible. From this single philosophical premise, he argued that a universal quantity\u2014what we now call energy\u2014must be conserved in all interactions of nature. In 1847, he published his work, mathematically unifying mechanics, heat, electricity, magnetism, and chemistry under the single umbrella of the Law of Conservation of Energy. Together, Joule\u2019s tangible proof and Helmholtz\u2019s unifying theory cemented one of the most fundamental principles of the universe. This was the revolutionary breakthrough that opened up the Energy Highway. Now, physicists could bypass the messy details of variable forces and simply track the flow of this conserved quantity. Let&#8217;s go back to our spring problem. Video Example: A horizontal spring of spring constant k and negligible mass is compressed through a distance y. What is the final speed of the mass? The SUVAT &#8220;dead end&#8221; forces you to think about the changing acceleration. The Energy Highway lets you bypass that completely: Energy at the Start = Energy at the End Initially, all the energy is stored in the compressed spring as Elastic Potential Energy (Ep\u200b). At the end, after the mass is launched, all that energy has been converted into the Kinetic Energy (Ek\u200b) of the moving mass. A similar problem has been worked in this example, watch this video until the end to understand the method of cracking such problems Look at that! A problem that was impossible with SUVAT becomes a simple algebraic equation. This powerful approach works for a huge range of problems you&#8217;ll see, from masses hanging on springs to blocks being launched, as shown in our video solutions. A Final Thought: Your Role as the Knower In TOK, we learn that a model is a simplified representation of reality, powerful within its specific scope, but limited outside of it. The SUVAT equations are a fantastic model for the AOK of Natural Sciences, but only for the limited scope of constant acceleration. Recognizing this limitation isn&#8217;t a failure. It&#8217;s a crucial step in your development as a knower. It prompts you to ask a powerful knowledge question: How does the scientific community decide when a model is no longer adequate? The shift from a purely force-based analysis to an energy-based one is a classic example of a&#8230;<\/p>\n","protected":false},"author":1,"featured_media":866,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":"[{\"content\":\"<a href=\\\"https:\/\/blog.scienceandindustrymuseum.org.uk\/james-joules-energy\/\\\">https:\/\/blog.scienceandindustrymuseum.org.uk\/james-joules-energy\/<\/a>\",\"id\":\"2f98f665-8b7c-4352-94d8-fb3e0bdcae0b\"},{\"content\":\"<a href=\\\"https:\/\/www.britannica.com\/biography\/Hermann-von-Helmholtz\/Later-life\\\">https:\/\/www.britannica.com\/biography\/Hermann-von-Helmholtz\/Later-life<\/a>\",\"id\":\"30051995-21f8-4d4d-8d50-913e5949eb65\"}]"},"categories":[1],"tags":[44,26,45,43],"class_list":["post-861","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-blog","tag-energy-methods","tag-ibdp-physics","tag-springs","tag-suvat-equations"],"_links":{"self":[{"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/posts\/861","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/comments?post=861"}],"version-history":[{"count":1,"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/posts\/861\/revisions"}],"predecessor-version":[{"id":865,"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/posts\/861\/revisions\/865"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/media\/866"}],"wp:attachment":[{"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/media?parent=861"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/categories?post=861"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/ibphysicswithrao.com\/home\/wp-json\/wp\/v2\/tags?post=861"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}