It was reasoned that in normal ferroelastic crystals, if their prototypic (or peraelastic) phase transitions are of the second kind, the dependence of the spontaneous strain on temperature T should be proportional to ( T c - T ) 1/2 right below the transition temperature T c and the T dependence of the elastic compliance should obey the so-called “Curie-Weiss law” above and below T c . However, it is also considered that possible are ferroelastic crystals in which, whereas their prototypic phase transitions are of the second kind, the T dependence of the spontaneous strain should be proportional to T c - T right below T c and the T dependence of the elastic compliance should disobey the Curie-Weiss law above and below T c . In this paper, two models of such ferroelastic crystals are presented and thermodynamically investigated. One of these models is not only ferroelastic but also feeroelectric; its spontaneous polarization and electric susceptibility should so peculiarly depend on T as its spontaneous strain and elastic compliance. These crystals are a kind of partially ferroelastic and partially antiferroelastic crystals and a kind of partially ferroelectric and partially antiferroelectric crystals; the ferroelasticity and ferroelectricity are “weaker” than the antiferroelasticity and antiferroelectricity respectively.
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Kêitsirô Aizu (1970) studied this question.
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