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	<id>http://205.166.159.208/wiki/index.php?action=history&amp;feed=atom&amp;title=Discrete_Energy_levels_and_Boltzmann_Distribution</id>
	<title>Discrete Energy levels and Boltzmann Distribution - Revision history</title>
	<link rel="self" type="application/atom+xml" href="http://205.166.159.208/wiki/index.php?action=history&amp;feed=atom&amp;title=Discrete_Energy_levels_and_Boltzmann_Distribution"/>
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	<updated>2026-06-26T05:20:34Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
	<generator>MediaWiki 1.35.5</generator>
	<entry>
		<id>http://205.166.159.208/wiki/index.php?title=Discrete_Energy_levels_and_Boltzmann_Distribution&amp;diff=12550&amp;oldid=prev</id>
		<title>Bes at 19:49, 6 February 2020</title>
		<link rel="alternate" type="text/html" href="http://205.166.159.208/wiki/index.php?title=Discrete_Energy_levels_and_Boltzmann_Distribution&amp;diff=12550&amp;oldid=prev"/>
		<updated>2020-02-06T19:49:11Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&quot; data-mw=&quot;interface&quot;&gt;
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				&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 19:49, 6 February 2020&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l3&quot; &gt;Line 3:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 3:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Like a baseball, an electron also has a continuum of PE and KE when it is not confined. When there exist boundaries, like those within an atomic structure, the energy of the electron becomes restricted and we describe such a system as having '''discrete energy states'''. This existence of discrete energy states is a unique property of quantum mechanics.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Like a baseball, an electron also has a continuum of PE and KE when it is not confined. When there exist boundaries, like those within an atomic structure, the energy of the electron becomes restricted and we describe such a system as having '''discrete energy states'''. This existence of discrete energy states is a unique property of quantum mechanics.&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-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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;For a moment think about a hypothetical situation involving CSB. CSB has 3 discrete levels. If we measured the potential energy of any given individual in the CSB it would be one of three values, PE1, PE2, PE3, where PE1 represents the potential energy while on floor 1, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;as &lt;/del&gt;so on. Although there are people transitioning from floor 1 to 2 and 2 to 3 during a passing period, very seldom, if ever, do we find an individual doing there school work on the stairs (or between the energy levels). CSB can be thought of as having 3 discrete energy levels. Humans are complex beings, they will find themselves on any of the floors without any particular reason. Electrons are inherently lazy and will exist in the lowest energy state, but due to temperature, electrons have some inherent energy and so depending on how different the energy levels are you might find a few electrons on the 2nd or even 3rd floor.  &lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;For a moment think about a hypothetical situation involving CSB. CSB has 3 discrete levels. If we measured the potential energy of any given individual in the CSB it would be one of three values, PE1, PE2, PE3, where PE1 represents the potential energy while on floor 1, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;and &lt;/ins&gt;so on. Although there are people transitioning from floor 1 to 2 and 2 to 3 during a passing period, very seldom, if ever, do we find an individual doing there school work on the stairs (or between the energy levels). CSB can be thought of as having 3 discrete energy levels. Humans are complex beings, they will find themselves on any of the floors without any particular reason. Electrons are inherently lazy and will exist in the lowest energy state, but due to temperature, electrons have some inherent energy and so depending on how different the energy levels are you might find a few electrons on the 2nd or even 3rd floor.  &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-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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Ludwig Boltzmann was the individual that showed mathematically how the population of two states is dependent on the difference in the energy between the two states. The Boltzmann distribution is shown in eq. 2.2.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Ludwig Boltzmann was the individual that showed mathematically how the population of two states is dependent on the difference in the energy between the two states. The Boltzmann distribution is shown in eq. 2.2.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Bes</name></author>
	</entry>
	<entry>
		<id>http://205.166.159.208/wiki/index.php?title=Discrete_Energy_levels_and_Boltzmann_Distribution&amp;diff=9944&amp;oldid=prev</id>
		<title>Bes at 19:31, 24 January 2019</title>
		<link rel="alternate" type="text/html" href="http://205.166.159.208/wiki/index.php?title=Discrete_Energy_levels_and_Boltzmann_Distribution&amp;diff=9944&amp;oldid=prev"/>
		<updated>2019-01-24T19:31:06Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left diff-editfont-monospace&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
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				&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 19:31, 24 January 2019&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l3&quot; &gt;Line 3:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 3:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;Like a baseball, an electron also has a continuum of PE and KE when it is not confined. When there exist boundaries, like those within an atomic structure, the energy of the electron becomes restricted and we describe such a system as having '''discrete energy states'''. This existence of discrete energy states is a unique property of quantum mechanics.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;Like a baseball, an electron also has a continuum of PE and KE when it is not confined. When there exist boundaries, like those within an atomic structure, the energy of the electron becomes restricted and we describe such a system as having '''discrete energy states'''. This existence of discrete energy states is a unique property of quantum mechanics.&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-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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;For a moment think about a hypothetical situation involving CSB. CSB has 3 discrete levels. If we measured the potential energy of any given individual in the CSB it would be one of three values, PE1, PE2, PE3, where PE1 represents the potential energy while on floor 1, as so on. Although there are people transitioning from floor 1 to 2 and 2 to 3 during a passing period, very seldom, if ever, do we find an individual doing there school work on the stairs (or between the energy levels). CSB &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;has &lt;/del&gt;3 discrete energy levels. Humans are complex &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;being&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;if there were no classes &lt;/del&gt;on the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;3rd floor there would be no &lt;/del&gt;reason &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;for anyone to go to the 3rd floor&lt;/del&gt;. Electrons are inherently lazy and will exist in the lowest energy state &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;unless&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;For a moment think about a hypothetical situation involving CSB. CSB has 3 discrete levels. If we measured the potential energy of any given individual in the CSB it would be one of three values, PE1, PE2, PE3, where PE1 represents the potential energy while on floor 1, as so on. Although there are people transitioning from floor 1 to 2 and 2 to 3 during a passing period, very seldom, if ever, do we find an individual doing there school work on the stairs (or between the energy levels). CSB &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;can be thought of as having &lt;/ins&gt;3 discrete energy levels. Humans are complex &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;beings&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;they will find themselves &lt;/ins&gt;on &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;any of &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;floors without any particular &lt;/ins&gt;reason. Electrons are inherently lazy and will exist in the lowest energy state&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;, but due to temperature, electrons have some inherent energy and so depending on how different the energy levels are you might find a few electrons on the 2nd or even 3rd floor. &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-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;/td&gt;&lt;td class='diff-marker'&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;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&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;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt; If humans behaved as electrons do, they might all exist &lt;/del&gt;on the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;first floor, ie. &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;lowest &lt;/del&gt;energy &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;state, since there &lt;/del&gt;is &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;no apparent reason for them to be on &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;second floor&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&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;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Ludwig Boltzmann was the individual that showed mathematically how the population of two states is dependent &lt;/ins&gt;on the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;difference in &lt;/ins&gt;the energy &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;between the two states. The Boltzmann distribution &lt;/ins&gt;is &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;shown in eq. 2.2.&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&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; &lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&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;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;'''Activity'''&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&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;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;:Reproduce &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;graph (left side) in Example problem 2.1 using Mathematica&lt;/ins&gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Bes</name></author>
	</entry>
	<entry>
		<id>http://205.166.159.208/wiki/index.php?title=Discrete_Energy_levels_and_Boltzmann_Distribution&amp;diff=9943&amp;oldid=prev</id>
		<title>Bes: Created page with &quot;Many classical physics problems calculate the energy of an object. The potential energy of an object, like a baseball, is proportional to the height of the ball relative to a...&quot;</title>
		<link rel="alternate" type="text/html" href="http://205.166.159.208/wiki/index.php?title=Discrete_Energy_levels_and_Boltzmann_Distribution&amp;diff=9943&amp;oldid=prev"/>
		<updated>2019-01-24T18:49:13Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;quot;Many classical physics problems calculate the energy of an object. The potential energy of an object, like a baseball, is proportional to the height of the ball relative to a...&amp;quot;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;Many classical physics problems calculate the energy of an object. The potential energy of an object, like a baseball, is proportional to the height of the ball relative to a surface, like the ground. Since the ball can exist at any height, the potential energy (PE) can have any value between PE-max and 0 (on the ground). Likewise the kinetic energy (KE) of a baseball is proportional to the speed or velocity of the ball and can have a value between KE-max and 0 (at rest). The PE and the KE represent a '''continuum of energy states'''.&lt;br /&gt;
&lt;br /&gt;
Like a baseball, an electron also has a continuum of PE and KE when it is not confined. When there exist boundaries, like those within an atomic structure, the energy of the electron becomes restricted and we describe such a system as having '''discrete energy states'''. This existence of discrete energy states is a unique property of quantum mechanics.&lt;br /&gt;
&lt;br /&gt;
For a moment think about a hypothetical situation involving CSB. CSB has 3 discrete levels. If we measured the potential energy of any given individual in the CSB it would be one of three values, PE1, PE2, PE3, where PE1 represents the potential energy while on floor 1, as so on. Although there are people transitioning from floor 1 to 2 and 2 to 3 during a passing period, very seldom, if ever, do we find an individual doing there school work on the stairs (or between the energy levels). CSB has 3 discrete energy levels. Humans are complex being, if there were no classes on the 3rd floor there would be no reason for anyone to go to the 3rd floor. Electrons are inherently lazy and will exist in the lowest energy state unless&lt;br /&gt;
&lt;br /&gt;
 If humans behaved as electrons do, they might all exist on the first floor, ie. the lowest energy state, since there is no apparent reason for them to be on the second floor.&lt;/div&gt;</summary>
		<author><name>Bes</name></author>
	</entry>
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