Lennard-Jones model: Difference between revisions
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Lennard-Jones | 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. | #J. E. Lennard-Jones "Cohesion", Proc. Phys. Soc. Lond. '''43''' pp. 461- (1931) |
Revision as of 15:55, 23 February 2007
The Lennard-Jones potential is given by
where:
- : Potential energy of interaction betweeen 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
References
- J. E. Lennard-Jones "Cohesion", Proc. Phys. Soc. Lond. 43 pp. 461- (1931)