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		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Wertheim%27s_first_order_thermodynamic_perturbation_theory_(TPT1)&amp;diff=19315</id>
		<title>Wertheim&#039;s first order thermodynamic perturbation theory (TPT1)</title>
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		<updated>2016-07-20T22:15:26Z</updated>

		<summary type="html">&lt;p&gt;Galileo: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Wertheim&#039;s first order thermodynamic perturbation theory (TPT1) &amp;lt;ref&amp;gt;[http://dx.doi.org/10.1007/BF01017362 	M. S. Wertheim &amp;quot;Fluids with highly directional attractive forces. I. Statistical thermodynamics&amp;quot; Journal of Statistical Physics &#039;&#039;&#039;35&#039;&#039;&#039; pp. 19-34 (1984)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1007/BF01017363 M. S. Wertheim &amp;quot;Fluids with highly directional attractive forces. II. Thermodynamic perturbation theory and integral equations&amp;quot; Journal of Statistical Physics &#039;&#039;&#039;35&#039;&#039;&#039; pp. 35-47 (1984)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1007/BF01127721 M. S. Wertheim &amp;quot;Fluids with highly directional attractive forces. III. Multiple attraction sites&amp;quot; Journal of Statistical Physics &#039;&#039;&#039;42&#039;&#039;&#039; pp. 459-476 (1986)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1007/BF01127722 M. S. Wertheim &amp;quot;Fluids with highly directional attractive forces. IV. Equilibrium polymerization&amp;quot; Journal of Statistical Physics &#039;&#039;&#039;42&#039;&#039;&#039; pp. 477-492 (1986)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
&amp;lt;ref&amp;gt;[http://dx.doi.org/10.1063/1.453326  M. S. Wertheim &amp;quot;Thermodynamic perturbation theory of polymerization&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;87&#039;&#039;&#039; pp. 7323-7331 (1987)]&amp;lt;/ref&amp;gt;&lt;br /&gt;
can be expressed as:&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;Z_{\rm TPT1} = \frac{p}{\rho k_BT}= mZ_{\rm monomer}- (m-1)\left( 1 + \rho_{\rm monomer}\frac{\partial \ln {\rm g}(\sigma)}{\partial \rho_{\rm monomer}}\right)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;Z_{\rm monomer}&amp;lt;/math&amp;gt; is the [[equations of state | equation of state]] of the monomer system and &#039;&#039;m&#039;&#039; is the number of monomers in the chains.&lt;br /&gt;
&lt;br /&gt;
For example, in the study of the [[Flexible hard sphere chains | flexible hard sphere chain]] model one can use the &lt;br /&gt;
[[Carnahan-Starling equation of state]] for &amp;lt;math&amp;gt;Z_{\rm monomer}&amp;lt;/math&amp;gt;, leading to&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
Z_{\rm FHSC} = m \frac{ 1 + \eta + \eta^2 - \eta^3 }{(1-\eta)^3 } - (m-1) \frac{1+\eta-( \eta^2/2)}{(1-\eta)(1-\eta/2)}= 1+ m \frac{ 4\eta -2 \eta^2 }{(1-\eta)^3 } - (m-1) \frac{5\eta-2 \eta^2}{(1-\eta)(2-\eta)}&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
==See also==&lt;br /&gt;
*[[SAFT]]&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;references/&amp;gt;&lt;br /&gt;
;Related reading&lt;br /&gt;
*[http://dx.doi.org/10.1063/1.4947023  Bennett D. Marshall &amp;quot;Dual chain perturbation theory: A new equation of state for polyatomic molecules&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;144&#039;&#039;&#039; 164104 (2016)]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[category:perturbation theory]]&lt;/div&gt;</summary>
		<author><name>Galileo</name></author>
	</entry>
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