Thermo-visco-elasticity for Norton-Hoff-type models with homogeneous thermal expansion

TL;DR

This paper develops a thermo-visco-elastic model incorporating homogeneous thermal expansion, linearizes it to preserve energy, and proves the existence of solutions including displacement derivatives, advancing understanding of thermal-mechanical coupling.

Contribution

It introduces a linearized model with thermal expansion that maintains energy conservation and includes a novel second coupling in the heat equation, with proven solution existence.

Findings

Existence of solutions for the coupled system.

Proof of displacement's time derivative existence.

Energy conservation in the linearized model.

Abstract

In this work we study a quasi-static evolution of thermo-visco-elastic model with homogeneous thermal expansion. We assume that material is subject to two kinds of mechanical deformations: elastic and inelastic. Inelastic deformation is related to a hardening rule of Norton-Hoff type. Appearance of inelastic deformation causes transformation of mechanical energy into thermal one, hence we also take into the consideration changes of material's temperature. The novelty of this paper is to take into account the thermal expansion of material. We are proposing linearisation of the model for homogeneous thermal expansion, which preserves symmetry of system and therefore total energy is conserved. Linearisation of material's thermal expansion is performed in definition of Cauchy stress tensor and in heat equation. In previous studies, it was done in different way. Considering of such linearisation leads to system where the coupling between temperature and displacement occurs in two places, i.e. in the constitutive function for the evolution of visco-elastic strain and in the additional term in the heat equation, in comparison to models without thermal expansion. The second coupling was not considered previously. For such system of equations we prove the existence of solutions. Moreover, we obtain existence of displacement's time derivative, which has not been done previously.