Abstract
Separation of an arbitrary potential ϕ into a short-range, repulsive part ϕ0 and a weak correction ϕ1 affords the possibility of describing the ϕ-system properties as corrections to the assumed-known ϕ0 reference system. We derive here an expression for such a correction of the classical Helmholtz free energy that is the analog of a result familiar from the development of the hypernetted-chain integral equation. Other corrections are obtained therefrom, including a corrected pair-distribution function proposed earlier. All results are easily adapted for numerical calculation.