Aggregation equilibria of dilute fluids of spherical classical particl
es are considered using a formalism derived by Lockett and Wertheim. T
he present theory is a simple application of the Lockett-Wertheim theo
ry, and uses a set of ring, chain, and star Mayer graphs in the grand
canonical ensemble partition function. This analysis is applied to a f
luid of hard spheres with a thin exterior square well. Calculated here
are the equilibrium constants for n-mer association, the n-mer distri
bution, and the fluid pressure. The shape of the n-mer aggregates is i
nferred from their individual structure factors. (C) 1997 American Ins
titute of Physics.