Common nematic liquid crystals represent diamagnetic fluids. Molecular diamagnetism in non-ordered isotropic materials in general, as well as the mean diamagnetic polarizability in ordered materials, is temperature independent. However, due to thermal expansion of the material the volume susceptibility x is not constant but decreases with increasing temperature.' It is therefore sometimes convenient to introduce the temperature independent quantities x'~', the susceptibility per mole, or x (~) , the mass susceptibility, which are related to x by x (~) = M,X/p (m3 mol-'1 and X(m) = X I P (m3 kg -') where M,,, is the molar mass of the substance and p is the mass density.