“…The modern approaches for the constitutive modeling of both polycrystalline and single-crystal ferroelectroelastic materials can be classified into macroscopic phenomenological models [ 26 , 27 , 28 , 29 , 30 ], micromechanical models [ 31 , 32 , 33 , 34 , 35 , 36 , 37 , 38 , 39 , 40 , 41 , 42 ], and phase–field methods [ 43 , 44 , 45 , 46 , 47 , 48 , 49 , 50 ]. Among the phenomenological models, one can single out models based on the theory of phase transitions [ 51 ], models based on analogies with plasticity [ 26 , 27 , 28 , 30 ], models based on the statistical theory of Kolmogorov–Avrami–Ishibashi [ 52 , 53 ], hybrid models [ 54 ], models with internal variables [ 29 ] and semi-macroscopic models accounting for a hysteresis curve [ 55 ]. Micromechanical models are based on analytical (Reuss [ 31 , 32 ], Voigt [ 56 ] or self-consistent [ 31 ] methods) or numerical [ 35 , 38 ] homogenization.…”