Viscoelasticity with time-dependent memory kernels. Part II: asymptotic behavior of solutions

preprint2016arXivOpen access

Abstract

We continue the analysis on the model equation arising in the theory of viscoelasticity ∂ttu(t)−[1+kt(0)]Δu(t)−∫0∞kt′(s)Δu(t−s)ds+f(u(t))=g \partial_{tt} u(t)-\big[1+k_t(0)\big]Δu(t) -\int_0^\infty k'_t(s)Δu(t-s) d s + f(u(t)) = g in the presence of a (convex, nonnegative and summable) memory kernel kt(⋅)k_t(\cdot) explicitly depending on time. Such a model is apt to describe, for instance, the dynamics of aging viscoelastic materials. The earlier paper [4] was concerned with the correct mathematical setting of the problem, and provided a well-posedness result within the novel theory of dynamical systems acting on time-dependent spaces, recently established by Di Plinio {\it et al.}\ [14] In this second work, we focus on the asymptotic properties of the solutions, proving the existence and the regularity of the time-dependent global attractor for the dynamical process generated by the equation. In addition, when ktk_t approaches a multiple mδ0mδ_0 of the Dirac mass at zero as t→∞t\to\infty, we show that the asymptotic dynamics of our problem is close to the one of its formal limit ∂ttu(t)−Δu(t)−mΔ∂tu(t)+f(u(t))=g\partial_{tt} u(t)-Δu(t) -mΔ\partial_t u(t)+ f(u(t)) = g describing viscoelastic solids of Kelvin-Voigt type.

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