Viscoelasticity

A 3-dimensional singular kernel problem in viscoelasticity: an existence result

Materials with memory, namely those materials whose mechanical and/or thermodynamical behavior depends on time not only via the present time, but also through its past history, are considered. Specifically, a three dimensional viscoelastic body is studied. Its mechanical behavior is described via an integro-differential equation, whose kernel represents the relaxation modulus, characteristic of the viscoelastic material under investigation.

The relaxation function in viscoelasticity : classical and non-classical thermodynamically admissible examples

The model of a viscoelastic body is considered focussing the attention on the the kernel of the integro- differential model equation. It represents the relaxation modulus which characterises the response of the material with memory to deformation. An overview on the classical viscoelasticity model is followed by different generalisations. Two different cases of relaxation functions, whose physical admissibility is guarantied by appropriate assumptions, are listed. The first one concerns a relaxation modulus at the initial time t = 0.

Carleman estimate and application to an inverse source problem for a viscoelasticity model in anisotropic case

We consider an anisotropic hyperbolic equation with memory term: ?t2u(x,t)=?i,j=1n?i(aij(x)?ju)+?0t?|?|?2b?(x,t,?)?x?u(x,?)d?+R(x,t)f(x) for $x \in \Omega$ and $t\in (0, T)$ , which is a simplified model equation for viscoelasticity. The main result is a both-sided Lipschitz stability estimate for an inverse source problem of determining a spatial varying factor $f(x)$ of the force term $R(x, t)\,f(x)$ .

© Università degli Studi di Roma "La Sapienza" - Piazzale Aldo Moro 5, 00185 Roma