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	<updated>2026-04-30T18:41:11Z</updated>
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	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=TIP4P_model_of_water&amp;diff=3219</id>
		<title>TIP4P model of water</title>
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		<updated>2007-07-04T14:17:15Z</updated>

		<summary type="html">&lt;p&gt;83.149.19.6: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;TIP4P&#039;&#039;&#039; is a rigid planar model of [[water]], having a similar geometry to the Bernal and  Fowler ([[BF]]) model.&lt;br /&gt;
==Parameters==&lt;br /&gt;
{| style=&amp;quot;width:75%; height:100px&amp;quot; border=&amp;quot;1&amp;quot;&lt;br /&gt;
|- &lt;br /&gt;
| r (OH) (&lt;/div&gt;</summary>
		<author><name>83.149.19.6</name></author>
	</entry>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Mean_spherical_approximation&amp;diff=3212</id>
		<title>Mean spherical approximation</title>
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		<updated>2007-07-04T10:59:47Z</updated>

		<summary type="html">&lt;p&gt;83.149.19.6: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;Lebowitz and Percus&#039;&#039;&#039; mean spherical approximation (MSA) (1966) (Ref. 1) [[Closure relations | closure relation]] is given by&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;c(r) = -\beta \omega(r), ~~~~ r&amp;gt;\sigma.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
In the &#039;&#039;&#039;Blum and Høye&#039;&#039;&#039; mean spherical approximation for mixtures  (Refs 2 and 3) the closure is given by&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;{\rm g}_{ij}(r) \equiv h_{ij}(r)  1=0 ~~~~~~~~ r &amp;lt; \sigma_{ij} = (\sigma_i   \sigma_j)/2&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;c_{ij}(r)= \sum_{n=1} \frac{K_{ij}^{(n)}}{r}e^{-z_nr} ~~~~~~ \sigma_{ij} &amp;lt; r&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;h_{ij}(r)&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;c_{ij}(r)&amp;lt;/math&amp;gt; are the total and the direct correlation functions for two spherical&lt;br /&gt;
molecules of &#039;&#039;i&#039;&#039; and &#039;&#039;j&#039;&#039; species, &amp;lt;math&amp;gt;\sigma_i&amp;lt;/math&amp;gt; is the diameter of &#039;&#039;&#039;i&#039;&#039; species of molecule.&lt;br /&gt;
Duh and Haymet (Eq. 9 Ref. 4) write the MSA approximation as&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;g(r) = \frac{c(r)   \beta \Phi_2(r)}{1-e^{\beta \Phi_1(r)}}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\Phi_1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\Phi_2&amp;lt;/math&amp;gt; comes from the &lt;br /&gt;
[[Weeks-Chandler-Anderson perturbation theory | Weeks-Chandler-Anderson division]] &lt;br /&gt;
of the [[Lennard-Jones model | Lennard-Jones]] potential.&lt;br /&gt;
By introducing the definition  (Eq. 10 Ref. 4) &lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;\left.s(r)\right. = h(r) -c(r) -\beta \Phi_2 (r)&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
one can arrive at  (Eq. 11 in Ref. 4)&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;B(r) \approx B^{\rm MSA}(s) = \ln (1 s)-s&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
The [[Percus Yevick]] approximation may be recovered from the above equation by setting &amp;lt;math&amp;gt;\Phi_2=0&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==Thermodynamic consistency==&lt;br /&gt;
&lt;br /&gt;
See Ref. 5.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
#[http://dx.doi.org/10.1103/PhysRev.144.251  J. L. Lebowitz and J. K. Percus &amp;quot;Mean Spherical Model for Lattice Gases with Extended Hard Cores and Continuum Fluids&amp;quot;, Physical Review &#039;&#039;&#039;144&#039;&#039;&#039; pp. 251 - 258 (1966)]&lt;br /&gt;
#[http://dx.doi.org/10.1007/BF01011750 L. Blum and J. S. Høye &amp;quot;Solution of the Ornstein-Zernike equation with Yukawa closure for a mixture&amp;quot;, Journal  of Statistical Physics, &#039;&#039;&#039;19&#039;&#039;&#039; pp. 317-324 (1978)]&lt;br /&gt;
#[http://dx.doi.org/10.1007/BF01013935   Lesser Blum &amp;quot;Solution of the Ornstein-Zernike equation for a mixture of hard ions and Yukawa closure&amp;quot; Journal  of Statistical Physics, &#039;&#039;&#039;22&#039;&#039;&#039; pp. 661-672 (1980)]&lt;br /&gt;
#[http://dx.doi.org/10.1063/1.470724      Der-Ming Duh and A. D. J. Haymet &amp;quot;Integral equation theory for uncharged liquids: The Lennard-Jones fluid and the bridge function&amp;quot;, Journal of Chemical Physics &#039;&#039;&#039;103&#039;&#039;&#039; pp. 2625-2633 (1995)]&lt;br /&gt;
#[http://dx.doi.org/10.1063/1.2712181 Andrés Santos &amp;quot;Thermodynamic consistency between the energy and virial routes in the mean spherical approximation for soft potentials&amp;quot; Journal of Chemical Physics &#039;&#039;&#039;126&#039;&#039;&#039; 116101 (2007)]&lt;br /&gt;
[[Category:Integral equations]]&lt;/div&gt;</summary>
		<author><name>83.149.19.6</name></author>
	</entry>
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