<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>https://drorbn.net/index.php?action=history&amp;feed=atom&amp;title=Notes_for_AKT-140110%2F0%3A35%3A38</id>
	<title>Notes for AKT-140110/0:35:38 - Revision history</title>
	<link rel="self" type="application/atom+xml" href="https://drorbn.net/index.php?action=history&amp;feed=atom&amp;title=Notes_for_AKT-140110%2F0%3A35%3A38"/>
	<link rel="alternate" type="text/html" href="https://drorbn.net/index.php?title=Notes_for_AKT-140110/0:35:38&amp;action=history"/>
	<updated>2026-06-22T02:11:47Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
	<generator>MediaWiki 1.39.6</generator>
	<entry>
		<id>https://drorbn.net/index.php?title=Notes_for_AKT-140110/0:35:38&amp;diff=16542&amp;oldid=prev</id>
		<title>Leo algknt at 19:57, 25 May 2018</title>
		<link rel="alternate" type="text/html" href="https://drorbn.net/index.php?title=Notes_for_AKT-140110/0:35:38&amp;diff=16542&amp;oldid=prev"/>
		<updated>2018-05-25T19:57:25Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 15:57, 25 May 2018&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&#039;&#039;&#039;Lagrangian Mechanics&#039;&#039;&#039; is a tool used in studying motions in Classical Mechanics and it was introduced by Joseph-Louis Lagrange in 1788. An important concept in Lagragian Mechanics is that the equations of motion of Classical Mechanics can be based on a variational principle, namely, that along a path describing classical motion the &#039;&#039;&#039;action integral&#039;&#039;&#039; assumes a minimal value (Hamiltonian Principle of Least Action)&lt;/div&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&#039;&#039;&#039;Lagrangian Mechanics&#039;&#039;&#039; is a tool used in studying motions in Classical Mechanics and it was introduced by Joseph-Louis Lagrange in 1788. An important concept in Lagragian Mechanics is that the equations of motion of Classical Mechanics can be based on a variational principle, namely, that along a path describing classical motion the &#039;&#039;&#039;action integral&#039;&#039;&#039; assumes a minimal value (Hamiltonian Principle of Least Action)&lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The action integral is given by &amp;lt;math&amp;gt;S[x(t)] = \int^{t_1}_{t_0} dt \mathcal{L}(x(t),,t)&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;\mathcal{L}(x(t),&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;\.{&lt;/del&gt;x(t)&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;}&lt;/del&gt;,t) = \frac12 &lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;\.&lt;/del&gt;{x(t)}^2-U(x(t))/math&amp;gt; is called the Lagrangian.&lt;/div&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The action integral is given by &amp;lt;math&amp;gt;S[x(t)] = \int^{t_1}_{t_0} dt \mathcal{L}(x(t),&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;x^\prime(t)&lt;/ins&gt;,t)&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;\mathcal{L}(x(t),x&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;^\prime&lt;/ins&gt;(t),t) = \frac12 {x&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;^\prime&lt;/ins&gt;(t)}^2-U(x(t))&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&amp;lt;&lt;/ins&gt;/math&amp;gt; is called the Lagrangian.&lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;

&lt;!-- diff cache key drordb-drorbn_:diff:wikidiff2:1.12:old-16541:rev-16542:1.13.0 --&gt;
&lt;/table&gt;</summary>
		<author><name>Leo algknt</name></author>
	</entry>
	<entry>
		<id>https://drorbn.net/index.php?title=Notes_for_AKT-140110/0:35:38&amp;diff=16541&amp;oldid=prev</id>
		<title>Leo algknt at 19:52, 25 May 2018</title>
		<link rel="alternate" type="text/html" href="https://drorbn.net/index.php?title=Notes_for_AKT-140110/0:35:38&amp;diff=16541&amp;oldid=prev"/>
		<updated>2018-05-25T19:52:27Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 15:52, 25 May 2018&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;
  &lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&#039;&#039;&#039;Lagrangian Mechanics&#039;&#039;&#039; is a tool used in studying motions in Classical Mechanics and it was introduced by Joseph-Louis Lagrange in 1788. An important concept in Lagragian Mechanics is that the equations of motion of Classical Mechanics can be based on a variational principle, namely, that along a path describing classical motion the &#039;&#039;&#039;action integral&#039;&#039;&#039; assumes a minimal value (Hamiltonian Principle of Least Action)&lt;/div&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&#039;&#039;&#039;Lagrangian Mechanics&#039;&#039;&#039; is a tool used in studying motions in Classical Mechanics and it was introduced by Joseph-Louis Lagrange in 1788. An important concept in Lagragian Mechanics is that the equations of motion of Classical Mechanics can be based on a variational principle, namely, that along a path describing classical motion the &#039;&#039;&#039;action integral&#039;&#039;&#039; assumes a minimal value (Hamiltonian Principle of Least Action)&lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;br /&gt;&lt;/td&gt;
&lt;/tr&gt;
&lt;tr&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;−&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The action integral is given by &amp;lt;math&amp;gt;S[x(t)] = \int^{t_1}_{t_0} dt \mathcal{L}(x(t),&lt;del style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;\.{x(t)}&lt;/del&gt;,t)&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;\mathcal{L}(x(t),\.{x(t)},t) = \frac12 \.{x(t)}^2-U(x(t))/math&amp;gt; is called the Lagrangian.&lt;/div&gt;&lt;/td&gt;
  &lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;
  &lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;The action integral is given by &amp;lt;math&amp;gt;S[x(t)] = \int^{t_1}_{t_0} dt \mathcal{L}(x(t),,t)&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;\mathcal{L}(x(t),\.{x(t)},t) = \frac12 \.{x(t)}^2-U(x(t))/math&amp;gt; is called the Lagrangian.&lt;/div&gt;&lt;/td&gt;
&lt;/tr&gt;

&lt;!-- diff cache key drordb-drorbn_:diff:wikidiff2:1.12:old-16540:rev-16541:1.13.0 --&gt;
&lt;/table&gt;</summary>
		<author><name>Leo algknt</name></author>
	</entry>
	<entry>
		<id>https://drorbn.net/index.php?title=Notes_for_AKT-140110/0:35:38&amp;diff=16540&amp;oldid=prev</id>
		<title>Leo algknt: Created page with &quot;&#039;&#039;&#039;Lagrangian Mechanics&#039;&#039;&#039; is a tool used in studying motions in Classical Mechanics and it was introduced by Joseph-Louis Lagrange in 1788. An important concept in Lagragian ...&quot;</title>
		<link rel="alternate" type="text/html" href="https://drorbn.net/index.php?title=Notes_for_AKT-140110/0:35:38&amp;diff=16540&amp;oldid=prev"/>
		<updated>2018-05-25T19:48:40Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;&amp;#039;&amp;#039;&amp;#039;Lagrangian Mechanics&amp;#039;&amp;#039;&amp;#039; is a tool used in studying motions in Classical Mechanics and it was introduced by Joseph-Louis Lagrange in 1788. An important concept in Lagragian ...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;Lagrangian Mechanics&amp;#039;&amp;#039;&amp;#039; is a tool used in studying motions in Classical Mechanics and it was introduced by Joseph-Louis Lagrange in 1788. An important concept in Lagragian Mechanics is that the equations of motion of Classical Mechanics can be based on a variational principle, namely, that along a path describing classical motion the &amp;#039;&amp;#039;&amp;#039;action integral&amp;#039;&amp;#039;&amp;#039; assumes a minimal value (Hamiltonian Principle of Least Action)&lt;br /&gt;
&lt;br /&gt;
The action integral is given by &amp;lt;math&amp;gt;S[x(t)] = \int^{t_1}_{t_0} dt \mathcal{L}(x(t),\.{x(t)},t)&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;\mathcal{L}(x(t),\.{x(t)},t) = \frac12 \.{x(t)}^2-U(x(t))/math&amp;gt; is called the Lagrangian.&lt;/div&gt;</summary>
		<author><name>Leo algknt</name></author>
	</entry>
</feed>