Difference between revisions of "Gay-Berne model"

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The '''Gay-Berne''' model is used extensively in simulations of [[liquid crystals | liquid crystalline]] systems. The Gay-Berne model
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The '''Gay-Berne model''' (Ref. 1) 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 anistropic form of the [[Lennard-Jones model | Lennard-Jones 12:6 potential]].
<math>U_{ij}^{\mathrm LJ/GB} =
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:<math>U_{ij}^{\mathrm LJ/GB} =
 
4 \epsilon_0^{\mathrm LJ/GB}
 
4 \epsilon_0^{\mathrm LJ/GB}
 
[\epsilon^{\mathrm LJ/GB}]^{\mu}
 
[\epsilon^{\mathrm LJ/GB}]^{\mu}
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\right],
 
\right],
 
</math>
 
</math>
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where, in the limit of one of the particles being spherical, gives:
 
where, in the limit of one of the particles being spherical, gives:
  

Revision as of 11:11, 26 September 2008