Exp-6 potential: Difference between revisions
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* <math> \sigma </math> is the value of <math>r</math> at which <math> \Phi_{12}(r)=0</math> | * <math> \sigma </math> is 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) | ||
* <math>\alpha</math> is the "steepness" of the repulsive energy | * <math>\alpha</math> is the "steepness" of the repulsive 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>. | |||
==See also== | ==See also== | ||
*[[Buckingham potential]] | *[[Buckingham potential]] |
Revision as of 11:50, 8 February 2011
The exp-6 potential is given by (Eq. 1 in [1]):
where
- is the intermolecular pair potential between two particles or sites
- is the value of at which
- is the well depth (energy)
- is the "steepness" of the repulsive energy
Melting point
An approximate method to locate the melting point is given in [2].
See also
References
Related reading
- Marvin Ross and Berni Alder "Shock Compression of Argon. II. Nonadditive Repulsive Potential", Journal of Chemical Physics 46 pp. 4203-4210 (1967)
- Marvin Ross and F. H. Ree "Repulsive forces of simple molecules and mixtures at high density and temperature", Journal of Chemical Physics 73 pp. 6146-6152 (1980)