Consider a pair of electric dipoles μ and μ′, oriented in the directions (θ,ϕ) and (θ′,ϕ′), respectively; the distance R between their centers is assumed to be fixed. The potential energy in this orientation is given by
−R3μμ′{2cosθcosθ′−sinθsinθ′cos(ϕ−ϕ′)}.
Now, consider the pair to be in thermal equilibrium, their orientations being governed by a canonical distribution. Show that the mean force between the dipoles, at high temperatures, is given by
−2kTμμ′R7R^,R^ being a unit vector in the direction of the line of centers.