“…Moreover, it is well known that G! : ) and Hij$ are related to thermal effects and consequently to the temperature derivatives of the C$:)s at constant pressure [8,3]. Thus, for ijkl = 1111, 1122, 1133, 3333, 2323 one obtains by evaluation at initial state where al and a3 are the linear thermal expansion coefficients and a, is the volume coefficient of thermal expansion, with a, = 2 a l + a3 for the considered symmetry.…”