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	<title>Characteristic state function - Revision history</title>
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	<updated>2026-05-09T17:56:55Z</updated>
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		<title>imported&gt;Fadesga: /* References */</title>
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		<updated>2022-07-19T17:32:31Z</updated>

		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;References&lt;/span&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{short description|Particular relationship between the partition function of an ensemble}}&lt;br /&gt;
{{Refimprove|date=July 2007}}&lt;br /&gt;
The &amp;#039;&amp;#039;&amp;#039;characteristic state function&amp;#039;&amp;#039;&amp;#039; or &amp;#039;&amp;#039;&amp;#039;Massieu&amp;#039;s potential&amp;#039;&amp;#039;&amp;#039;&amp;lt;ref&amp;gt;{{Cite journal|date=2017-11-01|title=François Massieu and the thermodynamic potentials|journal=Comptes Rendus Physique|language=en|volume=18|issue=9–10|pages=526–530|doi=10.1016/j.crhy.2017.09.011|issn=1631-0705|doi-access=free|last1=Balian|first1=Roger|bibcode=2017CRPhy..18..526B}} &amp;quot;Massieu&amp;#039;s potentials [...] are directly recovered as logarithms of partition functions.&amp;quot;&amp;lt;/ref&amp;gt; in [[statistical mechanics]] refers to a particular relationship between the [[partition function (statistical mechanics)|partition function]] of an [[Statistical ensemble (mathematical physics)|ensemble]].&lt;br /&gt;
&lt;br /&gt;
In particular, if the partition function &amp;#039;&amp;#039;P&amp;#039;&amp;#039; satisfies&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;P = \exp(- \beta Q) \Leftrightarrow Q=-\frac{1}{\beta} \ln(P)  &amp;lt;/math&amp;gt; or &amp;lt;math&amp;gt;P = \exp(+ \beta Q) \Leftrightarrow Q=\frac{1}{\beta} \ln(P) &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
in which &amp;#039;&amp;#039;Q&amp;#039;&amp;#039; is a thermodynamic quantity, then &amp;#039;&amp;#039;Q&amp;#039;&amp;#039; is known as the &amp;quot;characteristic state function&amp;quot; of the ensemble corresponding to &amp;quot;P&amp;quot;. Beta refers to the [[thermodynamic beta]].&lt;br /&gt;
&lt;br /&gt;
== Examples ==&lt;br /&gt;
*The [[microcanonical ensemble]] satisfies &amp;lt;math&amp;gt; \Omega(U,V,N) = e^{ \beta T S} \;\, &amp;lt;/math&amp;gt; hence, its characteristic state function is &amp;lt;math&amp;gt;TS&amp;lt;/math&amp;gt;.&lt;br /&gt;
*The [[canonical ensemble]] satisfies &amp;lt;math&amp;gt;Z(T,V,N) = e^{- \beta A} \,\;&amp;lt;/math&amp;gt; hence, its characteristic state function is the [[Helmholtz free energy]] &amp;lt;math&amp;gt;A&amp;lt;/math&amp;gt;.&lt;br /&gt;
*The [[grand canonical ensemble]] satisfies &amp;lt;math&amp;gt;\mathcal Z(T,V,\mu) = e^{-\beta \Phi} \,\; &amp;lt;/math&amp;gt;, so its characteristic state function is the [[Grand potential]] &amp;lt;math&amp;gt;\Phi&amp;lt;/math&amp;gt;.&lt;br /&gt;
*The [[isothermal-isobaric ensemble]] satisfies &amp;lt;math&amp;gt;\Delta(N,T,P) = e^{-\beta G} \;\, &amp;lt;/math&amp;gt; so its characteristic function is the [[Gibbs free energy]] &amp;lt;math&amp;gt;G&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
State functions are those which tell about the equilibrium state of a system&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&lt;br /&gt;
{{Statistical mechanics topics}}&lt;br /&gt;
[[Category:Statistical mechanics]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
{{thermodynamics-stub}}&lt;br /&gt;
{{statisticalmechanics-stub}}&lt;/div&gt;</summary>
		<author><name>imported&gt;Fadesga</name></author>
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