Lennard-Jones model: Difference between revisions
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* Temperature; <math> T^* \equiv k_B T/\epsilon </math>, where <math> T </math> is the absolute temperature and <math> k_B </math> is the [[Boltzmann constant]] | * Temperature; <math> T^* \equiv k_B T/\epsilon </math>, where <math> T </math> is the absolute temperature and <math> k_B </math> is the [[Boltzmann constant]] | ||
==Argon== | |||
The Lennard-Jones parameters for argon are | |||
==References== | ==References== | ||
#[http://dx.doi.org/10.1088/0959-5309/43/5/301 J. E. Lennard-Jones, "Cohesion", Proceedings of the Physical Society, '''43''' pp. 461-482 (1931)] | #[http://dx.doi.org/10.1088/0959-5309/43/5/301 J. E. Lennard-Jones, "Cohesion", Proceedings of the Physical Society, '''43''' pp. 461-482 (1931)] | ||
[[Category:Models]] | [[Category:Models]] |
Revision as of 12:49, 22 March 2007
The Lennard-Jones potential is given by
where:
- : potential energy of interaction between two particles at a distance r;
- : diameter (length);
- : well depth (energy)
Reduced units:
- Density, , where (number of particles divided by the volume .)
- Temperature; , where is the absolute temperature and is the Boltzmann constant
Argon
The Lennard-Jones parameters for argon are