SUMMARYIn this paper, we analyze a contact problem with irreversible adhesion between a viscoelastic body and a rigid support. On the basis of Frémond's theory, we detail the derivation of the model and of the resulting partial differential equation system. Hence, we prove the existence of global in time solutions (to a suitable variational formulation) of the related Cauchy problem by means of an approximation procedure, combined with monotonicity and compactness tools, and with a prolongation argument. In fact the approximate problem (for which we prove a local well-posedness result) models a contact phenomenon in which the occurrence of repulsive dynamics is allowed for. We also show local uniqueness of the solutions, and a continuous dependence result under some additional assumptions.

This paper deals with a phase transitions model describing the evolution of damage in thermoviscoelastic materials. The resulting system is highly non-linear, mainly due to the presence of quadratic dissipative terms and non-smooth constraints on the variables. Existence and uniqueness of a solution are proved, as well as regularity results, on a suitable finite time interval.

In this paper, we consider a contact problem with adhesion between a viscoelastic body and a rigid support, taking thermal effects into account. The PDE system we deal with is derived within the modelling approach proposed by M. Frémond and, in particular, includes the entropy balance equations, describing the evolution of the temperatures of the body and of the adhesive material. Our main result consists in showing the existence of global in time solutions (to a suitable variational formulation) of the related initial and boundary value problem.

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In this paper two models of damaged\ud materials are presented. The first one describes a\ud structure composed by two adherents and an adhesive\ud which is micro-cracked and subject to two different\ud regimes, one in traction and one in compression. The\ud second model is a model of interface derived from the\ud first one through an asymptotic analysis, and it can be\ud interpreted as a model for contact with adhesion and\ud unilateral constraint. Simple numerical examples are\ud presented