The elastic constants Kij of the Frank‐Oseen energy density for uniaxial nematic liquid crystals depend on the Maier‐Saupe order parameter S and hence on temperature. Longa et al. recently used an extended Landau‐Ginzburg‐de Gennes theory to expand the functions Kij(S) up to fourth order in S. Here, a similar procedure is applied for the elastic energy density of biaxial nematic liquid crystals. The three chiral and 15 achiral constants are expressed as fourth‐order polynomials in the order parameter S and the degree of biaxiality T. Via the temperature dependence of the quantities S and T also the temperature dependence of the elastic constants is fixed.
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Monselesan et al. (1989) studied this question.
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