N-6 Lennard-Jones potential: Difference between revisions

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m (Added mention of the Mie potential.)
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* <math> \sigma </math> is the  diameter (length), ''i.e.'' the value of <math>r</math> at which <math> \Phi_{12}(r)=0</math>
* <math> \sigma </math> is the  diameter (length), ''i.e.'' the value of <math>r</math> at which <math> \Phi_{12}(r)=0</math>
* <math> \epsilon </math> is the well depth (energy)
* <math> \epsilon </math> is the well depth (energy)
 
==Melting point==
An approximate method to locate the melting point is given in <ref>[http://dx.doi.org/10.1063/1.3552948  Sergey A. Khrapak, Manis Chaudhuri, and Gregor E. Morfill "Freezing of Lennard-Jones-type fluids", Journal of Chemical Physics '''134''' 054120 (2011)]</ref>.
==References==
==References==
<references/>
<references/>
[[category: models]]
[[category: models]]

Revision as of 12:48, 8 February 2011

The n-6 Lennard-Jones potential is a variant the more well known Lennard-Jones model (or from a different point of view, a particular case of the Mie potential).. The potential is given by [1]:

Φ12(r)=ϵ(nn−6)(n6)6n−6[(σr)n−(σr)6]

where

  • r:=|r1−r2|
  • Φ12(r) is the intermolecular pair potential between two particles or sites
  • σ is the diameter (length), i.e. the value of r at which Φ12(r)=0
  • ϵ is the well depth (energy)

Melting point

An approximate method to locate the melting point is given in [2].

References