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 13:49, 22 March 2007

The Lennard-Jones potential is given by

V(r)=4ϵ[(σr)12−(σr)6]

where:

  • V(r) : potential energy of interaction between two particles at a distance r;
  • σ : diameter (length);
  • ϵ : well depth (energy)

Reduced units:

  • Density, ρ*≡ρσ3, where ρ=N/V (number of particles N divided by the volume V.)
  • Temperature; T*≡kBT/ϵ, where T is the absolute temperature and kB is the Boltzmann constant

Argon

The Lennard-Jones parameters for argon are

References

  1. J. E. Lennard-Jones, "Cohesion", Proceedings of the Physical Society, 43 pp. 461-482 (1931)