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		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Radial_distribution_function&amp;diff=3917</id>
		<title>Radial distribution function</title>
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		<updated>2007-09-07T03:43:43Z</updated>

		<summary type="html">&lt;p&gt;68.37.255.44: Small grammer edit&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;radial distribution function&#039;&#039;&#039; is a special case of the  [[pair distribution function]] for an isotropic system.&lt;br /&gt;
A [[Fourier analysis | Fourier transform]] of the radial distribution function results in the [[structure factor]], which is experimentally measurable. &lt;br /&gt;
==Density Expansion of the radial distribution function==&lt;br /&gt;
The  &#039;&#039;&#039;radial distribution function&#039;&#039;&#039; of a compressed gas may be expanded in powers of the density (Ref. 2)&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left. {\rm g}(r) \right. = e^{-\beta \Phi(r)} (1 + \rho {\rm g}_1 (r) + \rho^2 {\rm g}_2 (r) + ...)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\rho&amp;lt;/math&amp;gt; is the number of molecules per unit volume and &amp;lt;math&amp;gt;\Phi(r)&amp;lt;/math&amp;gt;&lt;br /&gt;
is the [[intermolecular pair potential]]. The &lt;br /&gt;
function &amp;lt;math&amp;gt;{\rm g}(r)&amp;lt;/math&amp;gt; is normalized to the value 1 for large distances.&lt;br /&gt;
As is known, &amp;lt;math&amp;gt;{\rm g}_1 (r)&amp;lt;/math&amp;gt;, &amp;lt;math&amp;gt;{\rm g}_2 (r)&amp;lt;/math&amp;gt;, ... can be expressed by &lt;br /&gt;
[[Cluster diagrams | cluster integrals]] in which the position of of two particles is kept fixed.&lt;br /&gt;
In classical mechanics, and on the assumption of additivity of intermolecular forces, one has&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;{\rm g}_1 (r_{12})= \int f (r_{13}) f(r_{23}) ~{\rm d}{\mathbf r}_3&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;{\rm g}_2 (r_{12})= \frac{1}{2}({\rm g}_1 (r_{12}))^2 + \varphi (r_{12})&lt;br /&gt;
+ 2\psi (r_{12}) + \frac{1}{2} \chi (r_{12})&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;r_{ik}&amp;lt;/math&amp;gt; is the distance &amp;lt;math&amp;gt;|{\mathbf r}_i -{\mathbf r}_k|&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;f(r)&amp;lt;/math&amp;gt;&lt;br /&gt;
is the [[Mayer f-function]]&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left. f(r) \right. = e^{-\beta \Phi(r)} -1&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\varphi (r_{12}) = \int  f (r_{13})  f (r_{24})  f (r_{34}) ~ {\rm d}{\mathbf r}_3 {\rm d}{\mathbf r}_4&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\psi (r_{12})  = \int  f (r_{13}) f (r_{23})  f (r_{24}) f (r_{34}) ~ {\rm d}{\mathbf r}_3 {\rm d}{\mathbf r}_4&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\chi (r_{12})  = \int  f (r_{13}) f (r_{23}) f (r_{14}) f (r_{24}) f (r_{34}) ~ {\rm d}{\mathbf r}_3 {\rm d}{\mathbf r}_4&amp;lt;/math&amp;gt;&lt;br /&gt;
==References==&lt;br /&gt;
#[http://dx.doi.org/10.1063/1.1723737     John G. Kirkwood and Elizabeth Monroe Boggs &amp;quot;The Radial Distribution Function in Liquids&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;10&#039;&#039;&#039; pp. 394-402 (1942)]&lt;br /&gt;
#[http://dx.doi.org/10.1103/PhysRev.85.777  B. R. A. Nijboer and L. Van Hove &amp;quot;Radial Distribution Function of a Gas of Hard Spheres and the Superposition Approximation&amp;quot;, Physical Review &#039;&#039;&#039;85&#039;&#039;&#039; pp. 777 - 783 (1952)]&lt;br /&gt;
#[http://dx.doi.org/10.1063/1.1703948 J. L. Lebowitz and J. K. Percus &amp;quot;Asymptotic Behavior of the Radial Distribution Function&amp;quot;, Journal of Mathematical Physics &#039;&#039;&#039;4&#039;&#039;&#039; pp. 248-254 (1963)]&lt;br /&gt;
[[category: statistical mechanics]]&lt;/div&gt;</summary>
		<author><name>68.37.255.44</name></author>
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