We study the equilibrium properties of inhomogeneous model colloid-polymer
mixtures. By integrating out the degrees of freedom of the ideal polymer co
ils, we derive a formal expression for the effective one-component Hamilton
ian of the (hard sphere) colloids that is valid for arbitrary external pote
ntials acting on both the colloids and the polymers. We show how one can re
cover information about the distribution of polymer in the mixture given kn
owledge of the colloid correlation functions calculated using the effective
one-component Hamiltonian. This result is then used to furnish the connect
ion between the free-volume and perturbation theory approaches to determini
ng the bulk phase equilibria. For the special case of a planar hard wall th
e effective Hamiltonian takes an explicit form, consisting of zero-, one-,
and two-body, but no higher-body, contributions provided the size ratio q=s
igma (p)/sigma (c)<0.1547, where <sigma>(c) and sigma (p) denote the diamet
ers of colloid and polymer respectively. We employ a simple density functio
nal theory to calculate colloid density profiles from this effective Hamilt
onian for q=0.1. The resulting profiles are found to agree well with those
from Monte Carlo simulations for the same Hamiltonian. Adding very small am
ounts of polymer gives rise to strong depletion effects at the hard wall wh
ich lead to pronounced enhancement of the colloid density profile (close to
the wall) over what is found for hard spheres at a hard wall.