Statistical entropy and a qualitative gas-liquid phase diagram

For a classical monatomic fluid, gas and liquid phases are differentiatedon the basis of their statistical-mechanical entropy expressions. In the customary picture of a gas, each particle is first allowed to move independently over the entire volume; interactions are then introduced, and the configurational entropy becomes 1 minus the interaction corrections. In a liquid, the configurational entropy is assumed to be dominated by correlations, and is expressed as S/sup (2)/ plus higher-order correlation corrections, where the two-particle term S/sup (2)/ is of order -2. For liquid argon at 85 K on the saturation curve, S/sup (2)/ is evaluated from the measured radial distribution function, and the entropy is accurately given by liquid statistical theory, with the higher-order correlation corrections being approximately 13% of the magnitude of S/sup (2)/. A qualitative gas-liquid phase diagram is drawn for a classical monatomic fluid