<?xml version="1.0"?>
<?xml-stylesheet type="text/css" href="http://editthis.info/skins/common/feed.css?207"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
		<id>http://editthis.info/VectorCalcUMB/?action=history&amp;feed=atom&amp;title=Hamiltonian_function</id>
		<title>Hamiltonian function - Revision history</title>
		<link rel="self" type="application/atom+xml" href="http://editthis.info/VectorCalcUMB/?action=history&amp;feed=atom&amp;title=Hamiltonian_function"/>
		<link rel="alternate" type="text/html" href="http://editthis.info/VectorCalcUMB/?title=Hamiltonian_function&amp;action=history"/>
		<updated>2026-10-13T22:27:06Z</updated>
		<subtitle>Revision history for this page on the wiki</subtitle>
		<generator>MediaWiki 1.15.1</generator>

	<entry>
		<id>http://editthis.info/VectorCalcUMB/?title=Hamiltonian_function&amp;diff=1410&amp;oldid=prev</id>
		<title>Aaronwelles at 21:30, 2 May 2006</title>
		<link rel="alternate" type="text/html" href="http://editthis.info/VectorCalcUMB/?title=Hamiltonian_function&amp;diff=1410&amp;oldid=prev"/>
				<updated>2006-05-02T21:30:38Z</updated>
		
		<summary type="html">&lt;p&gt;&lt;/p&gt;

		&lt;table style=&quot;background-color: white; color:black;&quot;&gt;
		&lt;col class='diff-marker' /&gt;
		&lt;col class='diff-content' /&gt;
		&lt;col class='diff-marker' /&gt;
		&lt;col class='diff-content' /&gt;
		&lt;tr valign='top'&gt;
		&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;←Older revision&lt;/td&gt;
		&lt;td colspan='2' style=&quot;background-color: white; color:black;&quot;&gt;Revision as of 21:30, 2 May 2006&lt;/td&gt;
		&lt;/tr&gt;
		&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 7:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 7:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;We call the total energy function the Hamiltonian Function, and denote it H. &amp;nbsp;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;We call the total energy function the Hamiltonian Function, and denote it H. &amp;nbsp;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background: #eee; color:black; font-size: smaller;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;-&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;The paragraph: &lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;For &lt;/ins&gt;a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;particle of mass m moving on a line&lt;/ins&gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Kinetic = p^2/2m&lt;/ins&gt;. &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;If the particle &lt;/ins&gt;is &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;moving under the influence of &lt;/ins&gt;a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;conservative force, &lt;/ins&gt;like &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;gravity, then there is a potential energy, U, which is a function &lt;/ins&gt;of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;position&lt;/ins&gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;-&lt;/td&gt;&lt;td style=&quot;background: #ffa; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;&amp;quot;But energy is more than just &lt;/del&gt;a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;conserved quantity: it determines &lt;/del&gt;..&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;&amp;quot; (pg.65) (1st page of Chpt 4) &lt;/del&gt;is a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;dramatic pargraph and I &lt;/del&gt;like &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;it. We should start out with something &lt;/del&gt;of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;this nature as an opening paragraph&lt;/del&gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;-aaron&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&amp;#160;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt;&amp;nbsp;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;background: #cfc; color:black; font-size: smaller;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;H:=p^2/2m+U(r)&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;!-- diff generator: internal 2026-10-13 22:27:06 --&gt;
&lt;/table&gt;</summary>
		<author><name>Aaronwelles</name></author>	</entry>

	<entry>
		<id>http://editthis.info/VectorCalcUMB/?title=Hamiltonian_function&amp;diff=1406&amp;oldid=prev</id>
		<title>Aaronwelles at 20:56, 2 May 2006</title>
		<link rel="alternate" type="text/html" href="http://editthis.info/VectorCalcUMB/?title=Hamiltonian_function&amp;diff=1406&amp;oldid=prev"/>
				<updated>2006-05-02T20:56:15Z</updated>
		
		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;The total energy function. (pg. 65-66)&lt;br /&gt;
&lt;br /&gt;
In a closed physical system the energy of the system is constant as the system moves through time.&lt;br /&gt;
&lt;br /&gt;
Example: Ball being thrown into air: Total energy = p^2/2m +mgr  (kinetic + potential)&lt;br /&gt;
&lt;br /&gt;
We call the total energy function the Hamiltonian Function, and denote it H. &lt;br /&gt;
&lt;br /&gt;
The paragraph: &lt;br /&gt;
&amp;quot;But energy is more than just a conserved quantity: it determines ..&amp;quot; (pg.65) (1st page of Chpt 4) is a dramatic pargraph and I like it. We should start out with something of this nature as an opening paragraph. -aaron&lt;/div&gt;</summary>
		<author><name>Aaronwelles</name></author>	</entry>

	</feed>