N-6 Lennard-Jones potential: Difference between revisions

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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 <ref>[http://dx.doi.org/10.1063/1.3253686 Alauddin Ahmed and Richard J. Sadus "Solid-liquid equilibria and triple points of n-6 Lennard-Jones fluids", Journal of Chemical Physics '''131''' 174504 (2009)]</ref>:
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 <ref>[http://dx.doi.org/10.1063/1.3253686 Alauddin Ahmed and Richard J. Sadus "Solid-liquid equilibria and triple points of n-6 Lennard-Jones fluids", Journal of Chemical Physics '''131''' 174504 (2009)]</ref>:



Revision as of 10:45, 14 May 2015

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, "1" and "2".
  • 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]. See also [3].

Shear viscosity

[4]

References

Related reading