<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>http://www.sklogwiki.org/SklogWiki/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=103.221.246.79</id>
	<title>SklogWiki - User contributions [en]</title>
	<link rel="self" type="application/atom+xml" href="http://www.sklogwiki.org/SklogWiki/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=103.221.246.79"/>
	<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php/Special:Contributions/103.221.246.79"/>
	<updated>2026-05-01T16:29:51Z</updated>
	<subtitle>User contributions</subtitle>
	<generator>MediaWiki 1.41.0</generator>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Virial_equation_of_state&amp;diff=20451</id>
		<title>Virial equation of state</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Virial_equation_of_state&amp;diff=20451"/>
		<updated>2020-11-17T13:51:56Z</updated>

		<summary type="html">&lt;p&gt;103.221.246.79: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;virial equation of state&#039;&#039;&#039; is used to describe the behavior of diluted gases. &lt;br /&gt;
It is usually written as an expansion of the [[compressibility factor]], &amp;lt;math&amp;gt; Z &amp;lt;/math&amp;gt;, in terms of either the&lt;br /&gt;
density or the pressure. Such an expansion was first introduced in 1885 by Thiesen &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1002/andp.18852600308 M. Thiesen &amp;quot;Untersuchungen über die Zustandsgleichung&amp;quot;, Annalen der Physik &#039;&#039;&#039;24&#039;&#039;&#039; pp. 467-492 (1885)]&amp;lt;/ref&amp;gt; and extensively studied by Heike Kamerlingh Onnes &amp;lt;ref&amp;gt; H. Kammerlingh Onnes &amp;quot;Expression of the equation of state of gases and liquids by means of series&amp;quot;, Communications from the Physical Laboratory of the University of Leiden &#039;&#039;&#039;71&#039;&#039;&#039; pp. 3-25 (1901)&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://www.digitallibrary.nl/proceedings/search/detail.cfm?pubid=436&amp;amp;view=image&amp;amp;startrow=1 H. Kammerlingh Onnes &amp;quot;Expression of the equation of state of gases and liquids by means of series&amp;quot;, Proceedings of the Koninklijke Nederlandse Akademie van Wetenschappen &#039;&#039;&#039;4&#039;&#039;&#039; pp. 125-147 (1902)]&amp;lt;/ref&amp;gt;, and mathematically by Ursell &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1017/S0305004100011191 H. D. Ursell &amp;quot;The evaluation of Gibbs&#039; phase-integral for imperfect gases&amp;quot;, Mathematical Proceedings of the Cambridge Philosophical Society &#039;&#039;&#039;23&#039;&#039;&#039; pp. 685-697 (1927)]&amp;lt;/ref&amp;gt;. One has&lt;br /&gt;
 &lt;br /&gt;
:&amp;lt;math&amp;gt; \frac{p V}{N k_B T } = Z = 1 + \sum_{k=2}^{\infty} B_k(T) \rho^{k-1}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
where &lt;br /&gt;
&lt;br /&gt;
* &amp;lt;math&amp;gt; p &amp;lt;/math&amp;gt; is the [[pressure]]&lt;br /&gt;
*&amp;lt;math&amp;gt; V &amp;lt;/math&amp;gt;  is the volume&lt;br /&gt;
*&amp;lt;math&amp;gt; N &amp;lt;/math&amp;gt; is the number of molecules&lt;br /&gt;
*&amp;lt;math&amp;gt; T &amp;lt;/math&amp;gt; is the [[temperature]]&lt;br /&gt;
*&amp;lt;math&amp;gt;k_B&amp;lt;/math&amp;gt; is the [[Boltzmann constant]]&lt;br /&gt;
*&amp;lt;math&amp;gt; \rho \equiv \frac{N}{V} &amp;lt;/math&amp;gt; is the (number) density&lt;br /&gt;
*&amp;lt;math&amp;gt; B_k\left( T \right) &amp;lt;/math&amp;gt; is called the k-th virial coefficient&lt;br /&gt;
==Virial coefficients==&lt;br /&gt;
The [[second virial coefficient]] represents the initial departure from [[Ideal gas |ideal-gas]] behaviour &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;B_{2}(T)= \frac{N_A}{2V} \int .... \int (1-e^{-\Phi/k_BT}) ~d\tau_1 d\tau_2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;N_A&amp;lt;/math&amp;gt; is [[Avogadro constant | Avogadros number]] and &amp;lt;math&amp;gt;d\tau_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;d\tau_2&amp;lt;/math&amp;gt; are volume elements of two different molecules&lt;br /&gt;
in configuration space. &lt;br /&gt;
&lt;br /&gt;
One can write the third virial coefficient as&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;B_{3}(T)= - \frac{1}{3V} \int \int \int f_{12} f_{13} f_{23}  dr_1 dr_2 dr_3&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &#039;&#039;f&#039;&#039; is the [[Mayer f-function]] (see also: [[Cluster integrals]]).&lt;br /&gt;
See also &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1080/002689796173453 M. S. Wertheim &amp;quot;Fluids of hard convex molecules III. The third virial coefficient&amp;quot;, Molecular Physics &#039;&#039;&#039;89&#039;&#039;&#039; pp. 1005-1017 (1996)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Convergence==&lt;br /&gt;
For a commentary on the convergence of the virial equation of state see &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.1704186     J. L. Lebowitz and O. Penrose &amp;quot;Convergence of Virial Expansions&amp;quot;, Journal of Mathematical Physics &#039;&#039;&#039;5&#039;&#039;&#039; pp. 841-847 (1964)]&amp;lt;/ref&amp;gt; and section 3 of &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1088/0953-8984/20/28/283102 A. J. Masters &amp;quot;Virial expansions&amp;quot;, Journal of Physics: Condensed Matter &#039;&#039;&#039;20&#039;&#039;&#039; 283102 (2008)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
==Quantum virial coefficients==&lt;br /&gt;
Using the [[path integral formulation]] one can also calculate the virial coefficients of quantum systems  &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.3573564 Giovanni Garberoglio and Allan H. Harvey &amp;quot;Path-integral calculation of the third virial coefficient of quantum gases at low temperatures&amp;quot;, Journal of Chemical Physics 134, 134106 (2011)]&amp;lt;/ref&amp;gt;.&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
&#039;&#039;&#039;Related reading&#039;&#039;&#039;&lt;br /&gt;
*[http://dx.doi.org/10.1088/0034-4885/7/1/312 James A Beattie and Walter H Stockmayer &amp;quot;Equations of state&amp;quot;, Reports on Progress in Physics &#039;&#039;&#039;7&#039;&#039;&#039; pp. 195-229 (1940)]&lt;br /&gt;
*Edward Allen Mason and Thomas Harley Spurling &amp;quot;The virial equation of state&amp;quot;, Pergamon Press (1969) ISBN 0080132928&lt;br /&gt;
*[http://dx.doi.org/10.1063/1.4929392  Nathaniel S. Barlow, Andrew J. Schultz, Steven J. Weinstein and David A. Kofke &amp;quot;Analytic continuation of the virial series through the critical point using parametric approximants&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;143&#039;&#039;&#039; 071103 (2015)]&lt;br /&gt;
*[https://doi.org/10.1063/1.5016165 Harold W. Hatch, Sally Jiao, Nathan A. Mahynski, Marco A. Blanco, and Vincent K. Shen &amp;quot;Communication: Predicting virial coefficients and alchemical transformations by extrapolating Mayer-sampling Monte Carlo simulations&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;147&#039;&#039;&#039; 231102 (2017)]&lt;br /&gt;
&lt;br /&gt;
[[category:equations of state]]&lt;/div&gt;</summary>
		<author><name>103.221.246.79</name></author>
	</entry>
</feed>