Abstract
A Padé approximant is used as an interpolation formula to obtain the density dependence of radial distribution functions. The equation is of the form gexp(u / kT) = (1 + a1ρ + a2ρ2) / (1 + b1ρ + b2ρ2), where g is the radial distribution function, u is the pair potential energy, k is Boltzmann's constant, T is the absolute temperature, and ρ is the number density. Padé constants are determined for the Gaussian and hard‐sphere models of a fluid.