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	<updated>2026-04-30T20:58:35Z</updated>
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	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14468</id>
		<title>Combining rules</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14468"/>
		<updated>2015-01-15T21:19:29Z</updated>

		<summary type="html">&lt;p&gt;38.105.236.163: Updated Lorentz reference&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;combining rules&#039;&#039;&#039;  are geometric expressions designed to provide the interaction energy between two dissimilar non-bonded atoms (here labelled UNIQa5d53e6b5f34ffec-math-0000006C-QINU and UNIQa5d53e6b5f34ffec-math-0000006D-QINU). Most of the rules are designed to be used with a specific [[Idealised models| interaction potential]] in mind. (&#039;&#039;See also&#039;&#039; [[Mixing rules]]).&lt;br /&gt;
==Böhm-Ahlrichs==&lt;br /&gt;
UNIQa5d53e6b5f34ffec-ref-0000006E-QINU&lt;br /&gt;
==Diaz Peña-Pando-Renuncio==&lt;br /&gt;
UNIQa5d53e6b5f34ffec-ref-0000006F-QINU&lt;br /&gt;
UNIQa5d53e6b5f34ffec-ref-00000070-QINU&lt;br /&gt;
==Fender-Halsey==&lt;br /&gt;
The Fender-Halsey combining rule for the [[Lennard-Jones model]] is given by UNIQa5d53e6b5f34ffec-ref-00000071-QINU&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-00000072-QINU&lt;br /&gt;
==Gilbert-Smith==&lt;br /&gt;
The Gilbert-Smith rules for the [[Born-Huggins-Meyer potential]]UNIQa5d53e6b5f34ffec-ref-00000073-QINUUNIQa5d53e6b5f34ffec-ref-00000074-QINUUNIQa5d53e6b5f34ffec-ref-00000075-QINU.&lt;br /&gt;
==Good-Hope rule==&lt;br /&gt;
The Good-Hope rule for [[Mie potential |Mie]]–[[Lennard-Jones model |Lennard‐Jones]] or [[Buckingham potential]]s UNIQa5d53e6b5f34ffec-ref-00000076-QINU is given by (Eq. 2):&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-00000077-QINU&lt;br /&gt;
==Hudson and McCoubrey==&lt;br /&gt;
UNIQa5d53e6b5f34ffec-ref-00000078-QINU&lt;br /&gt;
==Hogervorst rules==&lt;br /&gt;
The Hogervorst rules for the [[Exp-6 potential]] UNIQa5d53e6b5f34ffec-ref-00000079-QINU:&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-0000007A-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-0000007B-QINU&lt;br /&gt;
&lt;br /&gt;
==Kong rules==&lt;br /&gt;
The Kong rules for the [[Lennard-Jones model]] are given by (Table I in &lt;br /&gt;
UNIQa5d53e6b5f34ffec-ref-0000007C-QINU):&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-0000007D-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-0000007E-QINU&lt;br /&gt;
==Kong-Chakrabarty  rules==&lt;br /&gt;
The Kong-Chakrabarty rules for the [[Exp-6 potential]] UNIQa5d53e6b5f34ffec-ref-0000007F-QINU are given by (Eqs. 2-4):&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-00000080-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-00000081-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-00000082-QINU&lt;br /&gt;
&lt;br /&gt;
==Lorentz-Berthelot rules==&lt;br /&gt;
The Lorentz rule is given by UNIQa5d53e6b5f34ffec-ref-00000083-QINU&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-00000084-QINU&lt;br /&gt;
&lt;br /&gt;
which is only really valid for the [[hard sphere model]].&lt;br /&gt;
&lt;br /&gt;
The Berthelot rule is given by UNIQa5d53e6b5f34ffec-ref-00000085-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-00000086-QINU&lt;br /&gt;
&lt;br /&gt;
These rules are simple and widely used, but are not without their failings UNIQa5d53e6b5f34ffec-ref-00000087-QINU&lt;br /&gt;
UNIQa5d53e6b5f34ffec-ref-00000088-QINU&lt;br /&gt;
UNIQa5d53e6b5f34ffec-ref-00000089-QINU&lt;br /&gt;
UNIQa5d53e6b5f34ffec-ref-0000008A-QINU.&lt;br /&gt;
&lt;br /&gt;
==Mason-Rice rules==  &lt;br /&gt;
The Mason-Rice rules for the [[Exp-6 potential]] UNIQa5d53e6b5f34ffec-ref-0000008B-QINU.&lt;br /&gt;
==Srivastava and Srivastava rules==&lt;br /&gt;
The Srivastava and Srivastava rules for the [[Exp-6 potential]] UNIQa5d53e6b5f34ffec-ref-0000008C-QINU.&lt;br /&gt;
==Sikora rules==&lt;br /&gt;
The Sikora rules for the [[Lennard-Jones model]] UNIQa5d53e6b5f34ffec-ref-0000008D-QINU.&lt;br /&gt;
==Tang and Toennies==&lt;br /&gt;
UNIQa5d53e6b5f34ffec-ref-0000008E-QINU&lt;br /&gt;
==Waldman-Hagler rules==&lt;br /&gt;
The Waldman-Hagler rules UNIQa5d53e6b5f34ffec-ref-0000008F-QINU are given by:&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-00000090-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQa5d53e6b5f34ffec-math-00000091-QINU&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
UNIQa5d53e6b5f34ffec-references-00000092-QINU&lt;br /&gt;
&#039;&#039;&#039;Related reading&#039;&#039;&#039;&lt;br /&gt;
*[http://dx.doi.org/10.1021/ja00046a032 Thomas A. Halgren &amp;quot;The representation of van der Waals (vdW) interactions in molecular mechanics force fields: potential form, combination rules, and vdW parameters&amp;quot;, Journal of the American Chemical Society &#039;&#039;&#039;114&#039;&#039;&#039; pp. 7827-7843 (1992)]&lt;br /&gt;
[[category: mixtures]]&lt;/div&gt;</summary>
		<author><name>38.105.236.163</name></author>
	</entry>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14467</id>
		<title>Combining rules</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14467"/>
		<updated>2015-01-15T21:18:01Z</updated>

		<summary type="html">&lt;p&gt;38.105.236.163: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;combining rules&#039;&#039;&#039;  are geometric expressions designed to provide the interaction energy between two dissimilar non-bonded atoms (here labelled UNIQf4e7a62258c5cdf7-math-00000068-QINU and UNIQf4e7a62258c5cdf7-math-00000069-QINU). Most of the rules are designed to be used with a specific [[Idealised models| interaction potential]] in mind. (&#039;&#039;See also&#039;&#039; [[Mixing rules]]).&lt;br /&gt;
==Böhm-Ahlrichs==&lt;br /&gt;
UNIQf4e7a62258c5cdf7-ref-0000006A-QINU&lt;br /&gt;
==Diaz Peña-Pando-Renuncio==&lt;br /&gt;
UNIQf4e7a62258c5cdf7-ref-0000006B-QINU&lt;br /&gt;
UNIQf4e7a62258c5cdf7-ref-0000006C-QINU&lt;br /&gt;
==Fender-Halsey==&lt;br /&gt;
The Fender-Halsey combining rule for the [[Lennard-Jones model]] is given by UNIQf4e7a62258c5cdf7-ref-0000006D-QINU&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-0000006E-QINU&lt;br /&gt;
==Gilbert-Smith==&lt;br /&gt;
The Gilbert-Smith rules for the [[Born-Huggins-Meyer potential]]UNIQf4e7a62258c5cdf7-ref-0000006F-QINUUNIQf4e7a62258c5cdf7-ref-00000070-QINUUNIQf4e7a62258c5cdf7-ref-00000071-QINU.&lt;br /&gt;
==Good-Hope rule==&lt;br /&gt;
The Good-Hope rule for [[Mie potential |Mie]]–[[Lennard-Jones model |Lennard‐Jones]] or [[Buckingham potential]]s UNIQf4e7a62258c5cdf7-ref-00000072-QINU is given by (Eq. 2):&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-00000073-QINU&lt;br /&gt;
==Hudson and McCoubrey==&lt;br /&gt;
UNIQf4e7a62258c5cdf7-ref-00000074-QINU&lt;br /&gt;
==Hogervorst rules==&lt;br /&gt;
The Hogervorst rules for the [[Exp-6 potential]] UNIQf4e7a62258c5cdf7-ref-00000075-QINU:&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-00000076-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-00000077-QINU&lt;br /&gt;
&lt;br /&gt;
==Kong rules==&lt;br /&gt;
The Kong rules for the [[Lennard-Jones model]] are given by (Table I in &lt;br /&gt;
UNIQf4e7a62258c5cdf7-ref-00000078-QINU):&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-00000079-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-0000007A-QINU&lt;br /&gt;
==Kong-Chakrabarty  rules==&lt;br /&gt;
The Kong-Chakrabarty rules for the [[Exp-6 potential]] UNIQf4e7a62258c5cdf7-ref-0000007B-QINU are given by (Eqs. 2-4):&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-0000007C-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-0000007D-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-0000007E-QINU&lt;br /&gt;
&lt;br /&gt;
==Lorentz-Berthelot rules==&lt;br /&gt;
The Lorentz rule is given by UNIQf4e7a62258c5cdf7-ref-0000007F-QINU&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-00000080-QINU&lt;br /&gt;
&lt;br /&gt;
which is only really valid for the [[hard sphere model]].&lt;br /&gt;
&lt;br /&gt;
The Berthelot rule is given by UNIQf4e7a62258c5cdf7-ref-00000081-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-00000082-QINU&lt;br /&gt;
&lt;br /&gt;
These rules are simple and widely used, but are not without their failings UNIQf4e7a62258c5cdf7-ref-00000083-QINU&lt;br /&gt;
UNIQf4e7a62258c5cdf7-ref-00000084-QINU&lt;br /&gt;
UNIQf4e7a62258c5cdf7-ref-00000085-QINU.&lt;br /&gt;
&lt;br /&gt;
==Mason-Rice rules==  &lt;br /&gt;
The Mason-Rice rules for the [[Exp-6 potential]] UNIQf4e7a62258c5cdf7-ref-00000086-QINU.&lt;br /&gt;
==Srivastava and Srivastava rules==&lt;br /&gt;
The Srivastava and Srivastava rules for the [[Exp-6 potential]] UNIQf4e7a62258c5cdf7-ref-00000087-QINU.&lt;br /&gt;
==Sikora rules==&lt;br /&gt;
The Sikora rules for the [[Lennard-Jones model]] UNIQf4e7a62258c5cdf7-ref-00000088-QINU.&lt;br /&gt;
==Tang and Toennies==&lt;br /&gt;
UNIQf4e7a62258c5cdf7-ref-00000089-QINU&lt;br /&gt;
==Waldman-Hagler rules==&lt;br /&gt;
The Waldman-Hagler rules UNIQf4e7a62258c5cdf7-ref-0000008A-QINU are given by:&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-0000008B-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQf4e7a62258c5cdf7-math-0000008C-QINU&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
UNIQf4e7a62258c5cdf7-references-0000008D-QINU&lt;br /&gt;
&#039;&#039;&#039;Related reading&#039;&#039;&#039;&lt;br /&gt;
*[http://dx.doi.org/10.1021/ja00046a032 Thomas A. Halgren &amp;quot;The representation of van der Waals (vdW) interactions in molecular mechanics force fields: potential form, combination rules, and vdW parameters&amp;quot;, Journal of the American Chemical Society &#039;&#039;&#039;114&#039;&#039;&#039; pp. 7827-7843 (1992)]&lt;br /&gt;
[[category: mixtures]]&lt;/div&gt;</summary>
		<author><name>38.105.236.163</name></author>
	</entry>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14466</id>
		<title>Combining rules</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14466"/>
		<updated>2015-01-15T21:15:44Z</updated>

		<summary type="html">&lt;p&gt;38.105.236.163: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;combining rules&#039;&#039;&#039;  are geometric expressions designed to provide the interaction energy between two dissimilar non-bonded atoms (here labelled UNIQ1d8d2241b28493a9-math-0000006C-QINU and UNIQ1d8d2241b28493a9-math-0000006D-QINU). Most of the rules are designed to be used with a specific [[Idealised models| interaction potential]] in mind. (&#039;&#039;See also&#039;&#039; [[Mixing rules]]).&lt;br /&gt;
==Böhm-Ahlrichs==&lt;br /&gt;
UNIQ1d8d2241b28493a9-ref-0000006E-QINU&lt;br /&gt;
==Diaz Peña-Pando-Renuncio==&lt;br /&gt;
UNIQ1d8d2241b28493a9-ref-0000006F-QINU&lt;br /&gt;
UNIQ1d8d2241b28493a9-ref-00000070-QINU&lt;br /&gt;
==Fender-Halsey==&lt;br /&gt;
The Fender-Halsey combining rule for the [[Lennard-Jones model]] is given by UNIQ1d8d2241b28493a9-ref-00000071-QINU&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-00000072-QINU&lt;br /&gt;
==Gilbert-Smith==&lt;br /&gt;
The Gilbert-Smith rules for the [[Born-Huggins-Meyer potential]]UNIQ1d8d2241b28493a9-ref-00000073-QINUUNIQ1d8d2241b28493a9-ref-00000074-QINUUNIQ1d8d2241b28493a9-ref-00000075-QINU.&lt;br /&gt;
==Good-Hope rule==&lt;br /&gt;
The Good-Hope rule for [[Mie potential |Mie]]–[[Lennard-Jones model |Lennard‐Jones]] or [[Buckingham potential]]s UNIQ1d8d2241b28493a9-ref-00000076-QINU is given by (Eq. 2):&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-00000077-QINU&lt;br /&gt;
==Hudson and McCoubrey==&lt;br /&gt;
UNIQ1d8d2241b28493a9-ref-00000078-QINU&lt;br /&gt;
==Hogervorst rules==&lt;br /&gt;
The Hogervorst rules for the [[Exp-6 potential]] UNIQ1d8d2241b28493a9-ref-00000079-QINU:&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-0000007A-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-0000007B-QINU&lt;br /&gt;
&lt;br /&gt;
==Kong rules==&lt;br /&gt;
The Kong rules for the [[Lennard-Jones model]] are given by (Table I in &lt;br /&gt;
UNIQ1d8d2241b28493a9-ref-0000007C-QINU):&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-0000007D-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-0000007E-QINU&lt;br /&gt;
==Kong-Chakrabarty  rules==&lt;br /&gt;
The Kong-Chakrabarty rules for the [[Exp-6 potential]] UNIQ1d8d2241b28493a9-ref-0000007F-QINU are given by (Eqs. 2-4):&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-00000080-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-00000081-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-00000082-QINU&lt;br /&gt;
&lt;br /&gt;
==Lorentz-Berthelot rules==&lt;br /&gt;
The Lorentz rule is given by UNIQ1d8d2241b28493a9-ref-00000083-QINU&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-00000084-QINU&lt;br /&gt;
&lt;br /&gt;
which is only really valid for the [[hard sphere model]].&lt;br /&gt;
&lt;br /&gt;
The Berthelot rule is given by UNIQ1d8d2241b28493a9-ref-00000085-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-00000086-QINU&lt;br /&gt;
&lt;br /&gt;
These rules are simple and widely used, but are not without their failings UNIQ1d8d2241b28493a9-ref-00000087-QINU&lt;br /&gt;
UNIQ1d8d2241b28493a9-ref-00000088-QINU&lt;br /&gt;
UNIQ1d8d2241b28493a9-ref-00000089-QINU&lt;br /&gt;
UNIQ1d8d2241b28493a9-ref-0000008A-QINU.&lt;br /&gt;
&lt;br /&gt;
==Mason-Rice rules==  &lt;br /&gt;
The Mason-Rice rules for the [[Exp-6 potential]] UNIQ1d8d2241b28493a9-ref-0000008B-QINU.&lt;br /&gt;
==Srivastava and Srivastava rules==&lt;br /&gt;
The Srivastava and Srivastava rules for the [[Exp-6 potential]] UNIQ1d8d2241b28493a9-ref-0000008C-QINU.&lt;br /&gt;
==Sikora rules==&lt;br /&gt;
The Sikora rules for the [[Lennard-Jones model]] UNIQ1d8d2241b28493a9-ref-0000008D-QINU.&lt;br /&gt;
==Tang and Toennies==&lt;br /&gt;
UNIQ1d8d2241b28493a9-ref-0000008E-QINU&lt;br /&gt;
==Waldman-Hagler rules==&lt;br /&gt;
The Waldman-Hagler rules UNIQ1d8d2241b28493a9-ref-0000008F-QINU are given by:&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-00000090-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ1d8d2241b28493a9-math-00000091-QINU&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
UNIQ1d8d2241b28493a9-references-00000092-QINU&lt;br /&gt;
&#039;&#039;&#039;Related reading&#039;&#039;&#039;&lt;br /&gt;
*[http://dx.doi.org/10.1021/ja00046a032 Thomas A. Halgren &amp;quot;The representation of van der Waals (vdW) interactions in molecular mechanics force fields: potential form, combination rules, and vdW parameters&amp;quot;, Journal of the American Chemical Society &#039;&#039;&#039;114&#039;&#039;&#039; pp. 7827-7843 (1992)]&lt;br /&gt;
[[category: mixtures]]&lt;/div&gt;</summary>
		<author><name>38.105.236.163</name></author>
	</entry>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14465</id>
		<title>Combining rules</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14465"/>
		<updated>2015-01-15T21:14:47Z</updated>

		<summary type="html">&lt;p&gt;38.105.236.163: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;combining rules&#039;&#039;&#039;  are geometric expressions designed to provide the interaction energy between two dissimilar non-bonded atoms (here labelled UNIQ0f04d0997b4299f9-math-0000006C-QINU and UNIQ0f04d0997b4299f9-math-0000006D-QINU). Most of the rules are designed to be used with a specific [[Idealised models| interaction potential]] in mind. (&#039;&#039;See also&#039;&#039; [[Mixing rules]]).&lt;br /&gt;
==Böhm-Ahlrichs==&lt;br /&gt;
UNIQ0f04d0997b4299f9-ref-0000006E-QINU&lt;br /&gt;
==Diaz Peña-Pando-Renuncio==&lt;br /&gt;
UNIQ0f04d0997b4299f9-ref-0000006F-QINU&lt;br /&gt;
UNIQ0f04d0997b4299f9-ref-00000070-QINU&lt;br /&gt;
==Fender-Halsey==&lt;br /&gt;
The Fender-Halsey combining rule for the [[Lennard-Jones model]] is given by UNIQ0f04d0997b4299f9-ref-00000071-QINU&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-00000072-QINU&lt;br /&gt;
==Gilbert-Smith==&lt;br /&gt;
The Gilbert-Smith rules for the [[Born-Huggins-Meyer potential]]UNIQ0f04d0997b4299f9-ref-00000073-QINUUNIQ0f04d0997b4299f9-ref-00000074-QINUUNIQ0f04d0997b4299f9-ref-00000075-QINU.&lt;br /&gt;
==Good-Hope rule==&lt;br /&gt;
The Good-Hope rule for [[Mie potential |Mie]]–[[Lennard-Jones model |Lennard‐Jones]] or [[Buckingham potential]]s UNIQ0f04d0997b4299f9-ref-00000076-QINU is given by (Eq. 2):&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-00000077-QINU&lt;br /&gt;
==Hudson and McCoubrey==&lt;br /&gt;
UNIQ0f04d0997b4299f9-ref-00000078-QINU&lt;br /&gt;
==Hogervorst rules==&lt;br /&gt;
The Hogervorst rules for the [[Exp-6 potential]] UNIQ0f04d0997b4299f9-ref-00000079-QINU:&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-0000007A-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-0000007B-QINU&lt;br /&gt;
&lt;br /&gt;
==Kong rules==&lt;br /&gt;
The Kong rules for the [[Lennard-Jones model]] are given by (Table I in &lt;br /&gt;
UNIQ0f04d0997b4299f9-ref-0000007C-QINU):&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-0000007D-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-0000007E-QINU&lt;br /&gt;
==Kong-Chakrabarty  rules==&lt;br /&gt;
The Kong-Chakrabarty rules for the [[Exp-6 potential]] UNIQ0f04d0997b4299f9-ref-0000007F-QINU are given by (Eqs. 2-4):&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-00000080-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-00000081-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-00000082-QINU&lt;br /&gt;
&lt;br /&gt;
==Lorentz-Berthelot rules==&lt;br /&gt;
The Lorentz rule is given by UNIQ0f04d0997b4299f9-ref-00000083-QINU&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-00000084-QINU&lt;br /&gt;
&lt;br /&gt;
which is only really valid for the [[hard sphere model]].&lt;br /&gt;
&lt;br /&gt;
The Berthelot rule is given by UNIQ0f04d0997b4299f9-ref-00000085-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-00000086-QINU&lt;br /&gt;
&lt;br /&gt;
These rules are simple and widely used, but are not without their failings UNIQ0f04d0997b4299f9-ref-00000087-QINU&lt;br /&gt;
UNIQ0f04d0997b4299f9-ref-00000088-QINU&lt;br /&gt;
UNIQ0f04d0997b4299f9-ref-00000089-QINU&lt;br /&gt;
UNIQ0f04d0997b4299f9-ref-0000008A-QINU.&lt;br /&gt;
&lt;br /&gt;
==Mason-Rice rules==  &lt;br /&gt;
The Mason-Rice rules for the [[Exp-6 potential]] UNIQ0f04d0997b4299f9-ref-0000008B-QINU.&lt;br /&gt;
==Srivastava and Srivastava rules==&lt;br /&gt;
The Srivastava and Srivastava rules for the [[Exp-6 potential]] UNIQ0f04d0997b4299f9-ref-0000008C-QINU.&lt;br /&gt;
==Sikora rules==&lt;br /&gt;
The Sikora rules for the [[Lennard-Jones model]] UNIQ0f04d0997b4299f9-ref-0000008D-QINU.&lt;br /&gt;
==Tang and Toennies==&lt;br /&gt;
UNIQ0f04d0997b4299f9-ref-0000008E-QINU&lt;br /&gt;
==Waldman-Hagler rules==&lt;br /&gt;
The Waldman-Hagler rules UNIQ0f04d0997b4299f9-ref-0000008F-QINU are given by:&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-00000090-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ0f04d0997b4299f9-math-00000091-QINU&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
UNIQ0f04d0997b4299f9-references-00000092-QINU&lt;br /&gt;
&#039;&#039;&#039;Related reading&#039;&#039;&#039;&lt;br /&gt;
*[http://dx.doi.org/10.1021/ja00046a032 Thomas A. Halgren &amp;quot;The representation of van der Waals (vdW) interactions in molecular mechanics force fields: potential form, combination rules, and vdW parameters&amp;quot;, Journal of the American Chemical Society &#039;&#039;&#039;114&#039;&#039;&#039; pp. 7827-7843 (1992)]&lt;br /&gt;
[[category: mixtures]]&lt;/div&gt;</summary>
		<author><name>38.105.236.163</name></author>
	</entry>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14464</id>
		<title>Combining rules</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14464"/>
		<updated>2015-01-15T20:38:33Z</updated>

		<summary type="html">&lt;p&gt;38.105.236.163: Undo revision 14463 by 38.105.236.163 (talk)&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;combining rules&#039;&#039;&#039;  are geometric expressions designed to provide the interaction energy between two dissimilar non-bonded atoms (here labelled UNIQ0460e71333a2b13d-math-0000006C-QINU and UNIQ0460e71333a2b13d-math-0000006D-QINU). Most of the rules are designed to be used with a specific [[Idealised models| interaction potential]] in mind. (&#039;&#039;See also&#039;&#039; [[Mixing rules]]).&lt;br /&gt;
==Böhm-Ahlrichs==&lt;br /&gt;
UNIQ0460e71333a2b13d-ref-0000006E-QINU&lt;br /&gt;
==Diaz Peña-Pando-Renuncio==&lt;br /&gt;
UNIQ0460e71333a2b13d-ref-0000006F-QINU&lt;br /&gt;
UNIQ0460e71333a2b13d-ref-00000070-QINU&lt;br /&gt;
==Fender-Halsey==&lt;br /&gt;
The Fender-Halsey combining rule for the [[Lennard-Jones model]] is given by UNIQ0460e71333a2b13d-ref-00000071-QINU&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-00000072-QINU&lt;br /&gt;
==Gilbert-Smith==&lt;br /&gt;
The Gilbert-Smith rules for the [[Born-Huggins-Meyer potential]]UNIQ0460e71333a2b13d-ref-00000073-QINUUNIQ0460e71333a2b13d-ref-00000074-QINUUNIQ0460e71333a2b13d-ref-00000075-QINU.&lt;br /&gt;
==Good-Hope rule==&lt;br /&gt;
The Good-Hope rule for [[Mie potential |Mie]]–[[Lennard-Jones model |Lennard‐Jones]] or [[Buckingham potential]]s UNIQ0460e71333a2b13d-ref-00000076-QINU is given by (Eq. 2):&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-00000077-QINU&lt;br /&gt;
==Hudson and McCoubrey==&lt;br /&gt;
UNIQ0460e71333a2b13d-ref-00000078-QINU&lt;br /&gt;
==Hogervorst rules==&lt;br /&gt;
The Hogervorst rules for the [[Exp-6 potential]] UNIQ0460e71333a2b13d-ref-00000079-QINU:&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-0000007A-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-0000007B-QINU&lt;br /&gt;
&lt;br /&gt;
==Kong rules==&lt;br /&gt;
The Kong rules for the [[Lennard-Jones model]] are given by (Table I in &lt;br /&gt;
UNIQ0460e71333a2b13d-ref-0000007C-QINU):&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-0000007D-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-0000007E-QINU&lt;br /&gt;
==Kong-Chakrabarty  rules==&lt;br /&gt;
The Kong-Chakrabarty rules for the [[Exp-6 potential]] UNIQ0460e71333a2b13d-ref-0000007F-QINU are given by (Eqs. 2-4):&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-00000080-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-00000081-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-00000082-QINU&lt;br /&gt;
&lt;br /&gt;
==Lorentz-Berthelot rules==&lt;br /&gt;
The Lorentz rule is given by UNIQ0460e71333a2b13d-ref-00000083-QINU&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-00000084-QINU&lt;br /&gt;
&lt;br /&gt;
which is only really valid for the [[hard sphere model]].&lt;br /&gt;
&lt;br /&gt;
The Berthelot rule is given by UNIQ0460e71333a2b13d-ref-00000085-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-00000086-QINU&lt;br /&gt;
&lt;br /&gt;
These rules are simple and widely used, but are not without their failings UNIQ0460e71333a2b13d-ref-00000087-QINU&lt;br /&gt;
UNIQ0460e71333a2b13d-ref-00000088-QINU&lt;br /&gt;
UNIQ0460e71333a2b13d-ref-00000089-QINU&lt;br /&gt;
UNIQ0460e71333a2b13d-ref-0000008A-QINU.&lt;br /&gt;
&lt;br /&gt;
==Mason-Rice rules==  &lt;br /&gt;
The Mason-Rice rules for the [[Exp-6 potential]] UNIQ0460e71333a2b13d-ref-0000008B-QINU.&lt;br /&gt;
==Srivastava and Srivastava rules==&lt;br /&gt;
The Srivastava and Srivastava rules for the [[Exp-6 potential]] UNIQ0460e71333a2b13d-ref-0000008C-QINU.&lt;br /&gt;
==Sikora rules==&lt;br /&gt;
The Sikora rules for the [[Lennard-Jones model]] UNIQ0460e71333a2b13d-ref-0000008D-QINU.&lt;br /&gt;
==Tang and Toennies==&lt;br /&gt;
UNIQ0460e71333a2b13d-ref-0000008E-QINU&lt;br /&gt;
==Waldman-Hagler rules==&lt;br /&gt;
The Waldman-Hagler rules UNIQ0460e71333a2b13d-ref-0000008F-QINU are given by:&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-00000090-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ0460e71333a2b13d-math-00000091-QINU&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
UNIQ0460e71333a2b13d-references-00000092-QINU&lt;br /&gt;
&#039;&#039;&#039;Related reading&#039;&#039;&#039;&lt;br /&gt;
*[http://dx.doi.org/10.1021/ja00046a032 Thomas A. Halgren &amp;quot;The representation of van der Waals (vdW) interactions in molecular mechanics force fields: potential form, combination rules, and vdW parameters&amp;quot;, Journal of the American Chemical Society &#039;&#039;&#039;114&#039;&#039;&#039; pp. 7827-7843 (1992)]&lt;br /&gt;
[[category: mixtures]]&lt;/div&gt;</summary>
		<author><name>38.105.236.163</name></author>
	</entry>
	<entry>
		<id>http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14463</id>
		<title>Combining rules</title>
		<link rel="alternate" type="text/html" href="http://www.sklogwiki.org/SklogWiki/index.php?title=Combining_rules&amp;diff=14463"/>
		<updated>2015-01-15T20:28:11Z</updated>

		<summary type="html">&lt;p&gt;38.105.236.163: /* Lorentz-Berthelot rules */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;The &#039;&#039;&#039;combining rules&#039;&#039;&#039;  are geometric expressions designed to provide the interaction energy between two dissimilar non-bonded atoms (here labelled UNIQ879f6b467d81d4c5-math-0000008B-QINU and UNIQ879f6b467d81d4c5-math-0000008C-QINU). Most of the rules are designed to be used with a specific [[Idealised models| interaction potential]] in mind. (&#039;&#039;See also&#039;&#039; [[Mixing rules]]).&lt;br /&gt;
==Böhm-Ahlrichs==&lt;br /&gt;
UNIQ879f6b467d81d4c5-ref-0000008D-QINU&lt;br /&gt;
==Diaz Peña-Pando-Renuncio==&lt;br /&gt;
UNIQ879f6b467d81d4c5-ref-0000008E-QINU&lt;br /&gt;
UNIQ879f6b467d81d4c5-ref-0000008F-QINU&lt;br /&gt;
==Fender-Halsey==&lt;br /&gt;
The Fender-Halsey combining rule for the [[Lennard-Jones model]] is given by UNIQ879f6b467d81d4c5-ref-00000090-QINU&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-00000091-QINU&lt;br /&gt;
==Gilbert-Smith==&lt;br /&gt;
The Gilbert-Smith rules for the [[Born-Huggins-Meyer potential]]UNIQ879f6b467d81d4c5-ref-00000092-QINUUNIQ879f6b467d81d4c5-ref-00000093-QINUUNIQ879f6b467d81d4c5-ref-00000094-QINU.&lt;br /&gt;
==Good-Hope rule==&lt;br /&gt;
The Good-Hope rule for [[Mie potential |Mie]]–[[Lennard-Jones model |Lennard‐Jones]] or [[Buckingham potential]]s UNIQ879f6b467d81d4c5-ref-00000095-QINU is given by (Eq. 2):&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-00000096-QINU&lt;br /&gt;
==Hudson and McCoubrey==&lt;br /&gt;
UNIQ879f6b467d81d4c5-ref-00000097-QINU&lt;br /&gt;
==Hogervorst rules==&lt;br /&gt;
The Hogervorst rules for the [[Exp-6 potential]] UNIQ879f6b467d81d4c5-ref-00000098-QINU:&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-00000099-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-0000009A-QINU&lt;br /&gt;
&lt;br /&gt;
==Kong rules==&lt;br /&gt;
The Kong rules for the [[Lennard-Jones model]] are given by (Table I in &lt;br /&gt;
UNIQ879f6b467d81d4c5-ref-0000009B-QINU):&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-0000009C-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-0000009D-QINU&lt;br /&gt;
==Kong-Chakrabarty  rules==&lt;br /&gt;
The Kong-Chakrabarty rules for the [[Exp-6 potential]] UNIQ879f6b467d81d4c5-ref-0000009E-QINU are given by (Eqs. 2-4):&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-0000009F-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-000000A0-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-000000A1-QINU&lt;br /&gt;
&lt;br /&gt;
==Lorentz-Berthelot rules==&lt;br /&gt;
The Lorentz rule is given by UNIQ879f6b467d81d4c5-ref-000000A2-QINU&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-000000A3-QINU&lt;br /&gt;
&lt;br /&gt;
which is only really valid for the [[hard sphere model]].&lt;br /&gt;
&lt;br /&gt;
The Berthelot rule is given by UNIQ879f6b467d81d4c5-ref-000000A4-QINU&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-000000A5-QINU&lt;br /&gt;
&lt;br /&gt;
These rules are simple and widely used, but are not without their failings UNIQ879f6b467d81d4c5-ref-000000A6-QINU&lt;br /&gt;
UNIQ879f6b467d81d4c5-ref-000000A7-QINU&lt;br /&gt;
UNIQ879f6b467d81d4c5-ref-000000A8-QINU&lt;br /&gt;
UNIQ879f6b467d81d4c5-ref-000000A9-QINU.&lt;br /&gt;
&lt;br /&gt;
==Mason-Rice rules==  &lt;br /&gt;
The Mason-Rice rules for the [[Exp-6 potential]] UNIQ879f6b467d81d4c5-ref-000000AA-QINU.&lt;br /&gt;
==Srivastava and Srivastava rules==&lt;br /&gt;
The Srivastava and Srivastava rules for the [[Exp-6 potential]] UNIQ879f6b467d81d4c5-ref-000000AB-QINU.&lt;br /&gt;
==Sikora rules==&lt;br /&gt;
The Sikora rules for the [[Lennard-Jones model]] UNIQ879f6b467d81d4c5-ref-000000AC-QINU.&lt;br /&gt;
==Tang and Toennies==&lt;br /&gt;
UNIQ879f6b467d81d4c5-ref-000000AD-QINU&lt;br /&gt;
==Waldman-Hagler rules==&lt;br /&gt;
The Waldman-Hagler rules UNIQ879f6b467d81d4c5-ref-000000AE-QINU are given by:&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-000000AF-QINU&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
:UNIQ879f6b467d81d4c5-math-000000B0-QINU&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
UNIQ879f6b467d81d4c5-references-000000B1-QINU&lt;br /&gt;
&#039;&#039;&#039;Related reading&#039;&#039;&#039;&lt;br /&gt;
*[http://dx.doi.org/10.1021/ja00046a032 Thomas A. Halgren &amp;quot;The representation of van der Waals (vdW) interactions in molecular mechanics force fields: potential form, combination rules, and vdW parameters&amp;quot;, Journal of the American Chemical Society &#039;&#039;&#039;114&#039;&#039;&#039; pp. 7827-7843 (1992)]&lt;br /&gt;
[[category: mixtures]]&lt;/div&gt;</summary>
		<author><name>38.105.236.163</name></author>
	</entry>
</feed>