Difference between revisions of "Kihara potential"

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{{Stub-general}}
 
{{Stub-general}}
The '''Kihara potential''' was developed by Taro Kihara
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The '''Kihara potential''', developed by Taro Kihara
 
<ref>[http://dx.doi.org/10.1143/JPSJ.6.289 Taro Kihara "The Second Virial Coefficient of Non-Spherical Molecules", Journal of the Physical Society of Japan '''6''' pp. 289-296 (1951)]</ref>
 
<ref>[http://dx.doi.org/10.1143/JPSJ.6.289 Taro Kihara "The Second Virial Coefficient of Non-Spherical Molecules", Journal of the Physical Society of Japan '''6''' pp. 289-296 (1951)]</ref>
in 1951 and was inspired by the [[Lennard-Jones model]]. It is given by  
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in 1951, is a non-spherical generalisation of the [[Lennard-Jones model]]. It is given by  
  
  
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where <math>\Phi_{12}</math> is the [[intermolecular pair potential]], and <math>\rho</math> is the intermolecular distance.
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where <math>\Phi_{12}</math> is the [[intermolecular pair potential]], and <math>\rho</math> is the [[Source code for the minimum distance between two rods | shortest distance between molecule cores]].
 
==References==
 
==References==
 
<references/>
 
<references/>

Revision as of 12:55, 19 November 2009