Answers are grounded in this paper and cite their sources.
We investigate the corrections to the representation of the joint distribution of $q+l$ particles, nq+l, by the product nqnₗ for large separation between the sets of q and l particles. For a system in which there exists a "finite correlation length," we find explicitly the 1/N correction term to the simple product, where N is the number of particles in our system. When $q+l$ is equal to two, this expression reduces to that familiar from the Ornstein-Zernike relations for scattering of light from a fluid. In a uniform gas, our derivation also yields the explicit 1/N dependence of equilibrium distributions. Our result on the asymptotic form is then used to determine the low-order distribution functions for an equilibrium system of varying density, as well as for a nonequilibrium system represented by a local-equilibrium ensemble. These distribution functions are shown to be governed by the temperature and density in the vicinity of the molecules considered. We find as expected that the two-body distribution function coincides, to within quadratic terms in the gradients, with its equilibrium value for a uniform system at the temperature and density of the midpoint. For the higher-order distributions, correction terms linear in the gradients are found.
No takes yet. Share an insight, caveat, or question.
Lebowitz et al. (1961) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: