Lennard-Jones model: Difference between revisions
Jump to navigation
Jump to search
Carl McBride (talk | contribs) mNo edit summary |
Carl McBride (talk | contribs) mNo edit summary |
||
Line 1: | Line 1: | ||
The Lennard-Jones potential is given by | 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> | ||
where: | where: |
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)