Abstract
It is shown that the repulsive (not merely the positive) portion of the Lennard-Jones potential quantitatively dominates the equilibrium structure of the Lennard-Jones liquid. A simple and accurate approximation for the radial distribution function at high densities is presented.
- Received 15 June 1970
DOI:https://doi.org/10.1103/PhysRevLett.25.149
©1970 American Physical Society