Lennard-Jones model: Difference between revisions

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Lennard-Jones Potential:
The Lennard-Jones potential is given by


<math> V(r) = 4 \epsilon \left[ \left(\frac{\sigma}{r} \right)^{12}-  \left( \frac{\sigma}{r}\right)^6 \right] </math>
<math> V(r) = 4 \epsilon \left[ \left(\frac{\sigma}{r} \right)^{12}-  \left( \frac{\sigma}{r}\right)^6 \right] </math>
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==References==  
==References==  


#J. E. Lennard-Jones "Cohesion", Proc. Phys. Soc. Lond. volume 43 pages 461 (1931)
#J. E. Lennard-Jones "Cohesion", Proc. Phys. Soc. Lond. '''43''' pp. 461- (1931)

Revision as of 16:55, 23 February 2007

The Lennard-Jones potential is given by

V(r)=4ϵ[(σr)12−(σr)6]

where:

  • V(r) : Potential energy of interaction betweeen 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

References

  1. J. E. Lennard-Jones "Cohesion", Proc. Phys. Soc. Lond. 43 pp. 461- (1931)