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		<id>https://en.formulasearchengine.com/w/index.php?title=Jenny_Harrison&amp;diff=13451</id>
		<title>Jenny Harrison</title>
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		<updated>2014-01-12T14:45:25Z</updated>

		<summary type="html">&lt;p&gt;71.202.143.159: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;multiplicity function&#039;&#039;&#039; for a two state paramagnet, W(n,N), is the number of spin states such that n of the N spins point in the z-direction. This function is given by the [[Combinations|combinatoric function C(N,n)]]. That is:&lt;br /&gt;
&amp;lt;center&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;W (n,N) = {N \choose n} = {{N!} \over {n!(N - n)!}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;/center&amp;gt;&lt;br /&gt;
&lt;br /&gt;
It is primarily used in introductory [[statistical mechanics]] and  [[thermodynamics]] textbooks to explain the microscopic definition of entropy to students. If the spins are non-interacting, then the multiplicity function counts the number of states which have the same energy in an external magnetic field. By definition, the [[entropy]] S is then given by the [[natural logarithm]] of this number:&lt;br /&gt;
&lt;br /&gt;
&amp;lt;center&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;S = k\ln{W }\,&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;Schroeder, Daniel V.. An Introduction to Thermal Dynamics. San Francisco: Addison Wesley Longman 2002.&amp;lt;/ref&amp;gt;&lt;br /&gt;
Where k is the [[Boltzmann constant]]&lt;br /&gt;
&amp;lt;/center&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
[[Category:Thermodynamics]]&lt;/div&gt;</summary>
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