“…For , , T , q ,p , , , , p , and represented generically by f , we have (79) Here, g = grad , G s = grad C s (a third-order tensor), and d = grad . This type of constitutive relation represents materials devoid of memory (Truesdell and Noll, 1992), able to describe thermoelasticity and viscoelasticity of the Voigt type (Bowen, 1968). While this list of dependent variables seems daunting, it is justified by our effort to consider both solid and fluid constituents (hence the need for C s , and for the solid, and for the fluids), and the fact that the entropy inequality of Eq.…”