“…In particular, the specific Gibbs free energy might be the thermodynamic potential of choice, see [13] for further discussion. In fact, the Gibbs potential is the natural choice in the case of elastic bodies with constitutive relation in the form B = e ( T ) , where e is a tensor-valued function, see especially [14], [16] and [19], and also [20] for the case of thermoviscoelastic solids. For the sake of simplicity, however, we stick to the Helmholtz free energy, which allows us to utilise or recover some well known formulae for Green elastic (hyperelastic) solids, and document the relation of our work to the classical nonlinear elasticity theory.…”