We discuss a liquid-state theory for the equilibrium structure of inho
mogeneous polymeric liquids. The theory consists of an equation for th
e;density profile of a liquid in an external potential, which has been
derived previously by density functional methods. In general, this eq
uation must be solved by sim;lation techniques. However, if the chains
are modeled as random walks-which is a reasonable approximation for f
lexible polymers,at mel densities-we show that the theory reduces to a
set of coupled integral equations which can be solved;numerically. We
present results for a single component liquid near a hard wall. Last,
we show that, in the Gaussian thread limit, the theory reduces to a f
orm that is very similar to Edwards-Helfand-Tagami ''self-consistent f
ield'' theory. However, there are important differences between the tw
o theories for multicomponent liquids (a blend for example) if the typ
es of polymers are structurally dissimilar. (C) 1995 American Institut
e of Physics.