“…The material constitutive model is then obtained from the balance of conservative and dissipative forces as ∂ (F ,P ,z) W (F , P , z) + ∂ ( Ḟ , Ṗ , ż) R(P , z, Ṗ , ż) 0, see Subsection 1.5. This balance embodies the variational structure of the model, which in turn yields thermodynamical consistency, see Subsection 1.4, and allows for a comprehensive mathematical treatment [44]. The potentials R z and R p are positively 1-homogeneous in the rate variables, so that the constitutive model is of rate-independent type [50], as it is often assumed in damage and plasticity.…”