Difference between revisions of "Kihara potential"

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m (References: Added a forthcoming publication)
m (References: Added volume and page numbers)
 
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*[http://dx.doi.org/10.1063/1.473473 L. G. MacDowell, B. Garzón, S. Calero, and S. Lago "Dynamical properties and transport coefficients of Kihara linear fluids", Journal of Chemical Physics '''106''' pp. 4753- (1997)]
 
*[http://dx.doi.org/10.1063/1.473473 L. G. MacDowell, B. Garzón, S. Calero, and S. Lago "Dynamical properties and transport coefficients of Kihara linear fluids", Journal of Chemical Physics '''106''' pp. 4753- (1997)]
 
*[http://dx.doi.org/10.1103/PhysRevE.68.011704 Alejandro Cuetos, Bruno Martínez-Haya,  Santiago Lago and Luis F. Rull "Liquid crystal behavior of the Kihara fluid", Physical Review E '''68''' 011704 (2003)]
 
*[http://dx.doi.org/10.1103/PhysRevE.68.011704 Alejandro Cuetos, Bruno Martínez-Haya,  Santiago Lago and Luis F. Rull "Liquid crystal behavior of the Kihara fluid", Physical Review E '''68''' 011704 (2003)]
*[http://dx.doi.org/10.1080/00268976.2014.996191 Alejandro Cuetos and Bruno Martínez-Haya "Liquid crystal phase diagram of soft repulsive rods and its mapping on the hard repulsive reference fluid", Molecular Physics (''Latest articles'') (2015)]
+
*[http://dx.doi.org/10.1080/00268976.2014.996191 Alejandro Cuetos and Bruno Martínez-Haya "Liquid crystal phase diagram of soft repulsive rods and its mapping on the hard repulsive reference fluid", Molecular Physics '''113''' pp. 1137-1144 (2015)]
  
  
 
[[category: models]]
 
[[category: models]]

Latest revision as of 13:11, 22 May 2015

The Kihara potential, developed by Taro Kihara [1] in 1951, is a non-spherical generalisation of the Lennard-Jones model. It is given by


\Phi_{12}(\rho)=\Phi_0 \left[\frac{m}{n-m}\left(\frac{\rho_{0}}{\rho}\right)^n-\frac{n}{n-m}\left(\frac{\rho_{0}}{\rho}\right)^m\right], ~~~ n>m>3.


where \Phi_{12} is the intermolecular pair potential, and \rho is the shortest distance between molecule cores.

Oblate core[edit]

[2].

References[edit]

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