The
Potential of Mean Force of a system with N particles is by construction the potential that gives the average force over all the configurations of all the n+1...N particles acting on a particle
j at any fixed configuration keeping fixed a set of particles 1...n ::-\nabla_jw^{(n)} \, = \, \frac {\int e^{-\beta V} (- \nabla_j V)d q_{n+1}\dots dq_N } {\int e^{-\beta V} d q_{n+1}\dots dq_N} ,~ j =1,2,\dots,n Above, -\nabla_jw^{(n)} is the averaged force, i.e. "mean force" on particle
j. And w^{(n)} is the so-called potential of mean force. For n=2 , w^{(2)}(r) is the average work needed to bring the two particles from infinite separation to a distance r . It is also related to the
radial distribution function of the system, g(r) , by: :: g(r) = e^{-\beta w^{(2)}(r)} == Application ==