“…Satisfying the set of field and constitutive equations of (cf. [1,3,4,7,15,21,47 It is easy to see that if a solution of the problems (a 1 ) and (a 2 ) is to be unique, it is necessary that the following respective conditions known from the isothermal theory of plasticity should be satisfied [1,3,4,7,13,14,16,47] h > 0 and h + g p : MF σ > 0, (2.37)whereh is the isothermal strain-hardening function obtained in [1,2,7],∂σ , b is the function describing evolution of internal parametersK [1,2,46,47]. For the problems (a 1 ) and (a 2 ), conditions (2.37) are also sufficient.…”