N-6 Lennard-Jones potential: Difference between revisions

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m ("explained" the 12 subscript for Phi)
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* <math> \epsilon </math> is the well depth (energy)
* <math> \epsilon </math> is the well depth (energy)
==Melting point==
==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>.
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>. See also <ref>[http://dx.doi.org/10.1063/1.4707746 J. M. G. Sousa, A. L. Ferreira, and M. A. Barroso  "Determination of the solid-fluid coexistence of the n − 6 Lennard-Jones system from free energy calculations", Journal of Chemical Physics '''136''' 174502 (2012)]</ref>.
 
==References==
==References==
<references/>
<references/>

Revision as of 15:10, 3 May 2012

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]:

where

  • is the intermolecular pair potential between two particles, "1" and "2".
  • is the diameter (length), i.e. the value of at which
  • is the well depth (energy)

Melting point

An approximate method to locate the melting point is given in [2]. See also [3].

References

Related reading