Difference between revisions of "Gay-Berne model"

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The '''Gay-Berne model''' <ref>[http://dx.doi.org/10.1063/1.441483  J. G. Gay and B. J. Berne "Modification of the overlap potential to mimic a linear site–site potential", Journal of Chemical Physics '''74''' pp. 3316-3319  (1981)]</ref> is used extensively in simulations of [[liquid crystals | liquid crystalline]] systems. The Gay-Berne model
 
The '''Gay-Berne model''' <ref>[http://dx.doi.org/10.1063/1.441483  J. G. Gay and B. J. Berne "Modification of the overlap potential to mimic a linear site–site potential", Journal of Chemical Physics '''74''' pp. 3316-3319  (1981)]</ref> is used extensively in simulations of [[liquid crystals | liquid crystalline]] systems. The Gay-Berne model
is an anistropic form of the [[Lennard-Jones model | Lennard-Jones 12:6 potential]].
+
is an anisotropic form of the [[Lennard-Jones model | Lennard-Jones 12:6 potential]].
 
:<math>U_{ij}^{\mathrm LJ/GB} =
 
:<math>U_{ij}^{\mathrm LJ/GB} =
 
4 \epsilon_0^{\mathrm LJ/GB}
 
4 \epsilon_0^{\mathrm LJ/GB}

Revision as of 17:03, 22 November 2011