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		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Hyper-netted_chain&amp;diff=11315</id>
		<title>Hyper-netted chain</title>
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		<updated>2011-04-01T21:54:15Z</updated>

		<summary type="html">&lt;p&gt;136.159.234.143: space added before can&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;hyper-netted chain&#039;&#039;&#039; (HNC) equation has a clear physical basis in the [[Kirkwood superposition approximation]] (Ref. 1). The hyper-netted chain approximation is obtained by omitting the [[Cluster diagrams | elementary clusters]], &amp;lt;math&amp;gt;E(r)&amp;lt;/math&amp;gt;, in the exact convolution equation for &amp;lt;math&amp;gt;g(r)&amp;lt;/math&amp;gt;. The  hyper-netted chain  approximation was developed almost simultaneously by various&lt;br /&gt;
groups, namely: van Leeuwen, Groeneveld and de Boer, 1959 (Ref. 2). Morita and Hiroike, 1960 (Ref.s 3-8),&lt;br /&gt;
Rushbrooke, 1960 (Ref. 9), Verlet, 1960 (Ref. 10), and Meeron, 1960 (Ref. 11). The hyper-netted chain omits the [[bridge function]], i.e. &amp;lt;math&amp;gt; B(r) =0 &amp;lt;/math&amp;gt;, thus&lt;br /&gt;
the  [[cavity correlation function]] becomes&lt;br /&gt;
:&amp;lt;math&amp;gt;\ln y (r) =  h(r)  -c(r) \equiv \gamma (r)&amp;lt;/math&amp;gt;&lt;br /&gt;
The  hyper-netted chain [[Closure relations | closure relation]] can be written as&lt;br /&gt;
:&amp;lt;math&amp;gt;f \left[ \gamma (r) \right] = e^{[-\beta \Phi (r) + \gamma (r)]} - \gamma (r) -1&amp;lt;/math&amp;gt;&lt;br /&gt;
or&lt;br /&gt;
:&amp;lt;math&amp;gt;c\left(r\right)= h(r) - \beta \Phi(r) - \ln {\rm g}(r)&amp;lt;/math&amp;gt;&lt;br /&gt;
or (Eq. 12 Ref. 1)&lt;br /&gt;
:&amp;lt;math&amp;gt; c\left( r \right)= g(r) - \omega(r) &amp;lt;/math&amp;gt;&lt;br /&gt;
where &amp;lt;math&amp;gt;\Phi(r)&amp;lt;/math&amp;gt; is the [[intermolecular pair potential]].&lt;br /&gt;
The hyper-netted chain  approximation is well suited for long-range potentials, and in particular, Coulombic systems. For details of the numerical solution of the hyper-netted chain equation  for ionic systems (see Ref. 12).&lt;br /&gt;
==References==&lt;br /&gt;
#[http://dx.doi.org/10.1080/00268978300102111 G. A. Martynov; G. N. Sarkisov &amp;quot;Exact equations and the theory of liquids. V&amp;quot; Molecular Physics &#039;&#039;&#039;49&#039;&#039;&#039; pp.1495-1504 (1983)]&lt;br /&gt;
#[http://dx.doi.org/10.1016/0031-8914(59)90004-7  J. M. J. van Leeuwen, J. Groeneveld and J. de Boer &amp;quot;New method for the calculation of the pair correlation function. I&amp;quot; Physica &#039;&#039;&#039;25&#039;&#039;&#039; pp. 792-808 (1959)]&lt;br /&gt;
#[http://dx.doi.org/10.1143/PTP.20.920  Tohru Morita &amp;quot;Theory of Classical Fluids: Hyper-Netted Chain Approximation, I: Formulation for a One-Component System&amp;quot;, Progress of Theoretical Physics &#039;&#039;&#039;20&#039;&#039;&#039; pp. 920 -938 (1958)]&lt;br /&gt;
#[http://dx.doi.org/10.1143/PTP.21.361 Tohru Morita &amp;quot;Theory of Classical Fluids: Hyper-Netted Chain Approximation. II: Formulation for Multi-Component Systems&amp;quot; Progress of Theoretical Physics &#039;&#039;&#039;21&#039;&#039;&#039; pp. 361-382 (1959)]&lt;br /&gt;
#[http://dx.doi.org/10.1143/PTP.23.829 Tohru Morita &amp;quot;Theory of Classical Fluids: Hyper-Netted Chain Approximation. III: A New Integral Equation for the Pair Distribution Function&amp;quot; Progress of Theoretical Physics &#039;&#039;&#039;23&#039;&#039;&#039; pp. 829-845 (1960)]&lt;br /&gt;
#[http://dx.doi.org/10.1143/PTP.23.1003 Tohru Morita and Kazuo Hiroike &amp;quot;A New Approach to the Theory of Classical Fluids. I&amp;quot; Progress of Theoretical Physics &#039;&#039;&#039;23&#039;&#039;&#039; pp. 1003-1027 (1960)]&lt;br /&gt;
#[http://dx.doi.org/10.1143/PTP.24.317 Kazuo Hiroike &amp;quot;A New Approach to the Theory of Classical Fluids. II: Multicomponent Systems&amp;quot; Progress of Theoretical Physics &#039;&#039;&#039;24&#039;&#039;&#039; pp. 317-330 (1960)]&lt;br /&gt;
#[http://dx.doi.org/10.1143/PTP.25.537 Tohru Morita and Kazuo Hiroike &amp;quot;A New Approach to the Theory of Classical Fluids. III: General Treatment of Classical Systems&amp;quot; Progress of Theoretical Physics &#039;&#039;&#039;25&#039;&#039;&#039; pp. 537-578 (1961)]&lt;br /&gt;
#[http://dx.doi.org/10.1016/0031-8914(60)90020-3  G. S. Rushbrooke &amp;quot;On the hyper-chain approximation in the theory of classical fluids&amp;quot; Physica &#039;&#039;&#039;26&#039;&#039;&#039; pp. 259-265 (1960)]&lt;br /&gt;
#L. Verlet &amp;quot;On the Theory of Classical Fluids.&amp;quot;, Il Nuovo Cimento &#039;&#039;&#039;18&#039;&#039;&#039; pp. 77- (1960)&lt;br /&gt;
#[http://dx.doi.org/10.1063/1.1703652 Emmanuel Meeron &amp;quot;Nodal Expansions. III. Exact Integral Equations for Particle Correlation Functions&amp;quot;, Journal of Mathematical Physics &#039;&#039;&#039;1&#039;&#039;&#039; pp.  192-201 (1960)]&lt;br /&gt;
#[http://dx.doi.org/10.1080/00268978800101271 M. Kinoshita; M. Harada &amp;quot;Numerical solution of the HNC equation for ionic systems&amp;quot;, Molecular Physics &#039;&#039;&#039;65&#039;&#039;&#039; pp. 599-618 (1988)]&lt;br /&gt;
&lt;br /&gt;
[[Category: Integral equations]]&lt;/div&gt;</summary>
		<author><name>136.159.234.143</name></author>
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