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 number of molecules per unit volume and  is the intermolecular pair potential. The 
function
is the intermolecular pair potential. The 
function  is normalized to the value 1 for large distances.
As is known,
 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
, ... 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
 is the distance  , where
, where  is the Mayer f-function
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)