The radial distribution function is a special case of the pair distribution function for an isotropic system.
A Fourier transform of the radial distribution function results in the structure factor, which is experimentally measure able.
Density Expansion of the radial distribution function
The radial distribution function of a compressed gas may be expanded in powers of the density (Ref. 2)

where
is the number of molecules per unit volume and
is the intermolecular pair potential. The
function
is normalized to the value 1 for large distances.
As is known,
,
, ... can be expressed by
cluster integrals in which the position of of two particles is kept fixed.
In classical mechanics, and on the assumption of additivity of intermolecular forces, one has


where
is the distance
, where
is the Mayer f-function

and



References
- John G. Kirkwood and Elizabeth Monroe Boggs "The Radial Distribution Function in Liquids", Journal of Chemical Physics 10 pp. 394-402 (1942)
- B. R. A. Nijboer and L. Van Hove "Radial Distribution Function of a Gas of Hard Spheres and the Superposition Approximation", Physical Review 85 pp. 777 - 783 (1952)
- J. L. Lebowitz and J. K. Percus "Asymptotic Behavior of the Radial Distribution Function", Journal of Mathematical Physics 4 pp. 248-254 (1963)