Abstract
The equation of motion of a system of 864 particles interacting through a Lennard-Jones potential has been integrated for various values of the temperature and density, relative, generally, to a fluid state. The equilibrium properties have been calculated and are shown to agree very well with the corresponding properties of argon. It is concluded that, to a good approximation, the equilibrium state of argon can be described through a two-body potential.
- Received 30 January 1967
DOI:https://doi.org/10.1103/PhysRev.159.98
©1967 American Physical Society
