Using the generalized Kirkwood-Buff formula for a surface tension we study the interfacial properties of liquid crystals. Surface tension, δ, is calculated for the dilute hard rod system in the sharp interface approximation as a function of a tilt angle, θt, measured from the normal to the flat interface. This function has a minimum at θ t corresponding to the preferred orientation of liquid
... [Show full abstract] crystal molecule at the nematic-isotropic interface and in our case θ t = 60°. We also argue that hard-core repulsion favours perpendicular alignment at the nematic free surface i.e θt=0°.