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Crack Initiation in Brittle Materials
Authors:Antonin Chambolle  Alessandro Giacomini  Marcello Ponsiglione
Institution:(1) CMAP, Ecole Polytechnique, CNRS, 91128 Palaiseau, France;(2) Dipartimento di Matematica, Facoltà di Ingegneria, Università degli Studi di Brescia, Via Valotti 9, 25133 Brescia, Italy;(3) Max Planck Institute for Mathematics in the Sciences, Inselstrasse 22, 04103 Leipzig, Germany
Abstract:In this paper we study the crack initiation in a hyper-elastic body governed by a Griffith-type energy. We prove that, during a load process through a time-dependent boundary datum of the type tt g(x) and in the absence of strong singularities (e.g., this is the case of homogeneous isotropic materials) the crack initiation is brutal, that is, a big crack appears after a positive time t i > 0. Conversely, in the presence of a point x of strong singularity, a crack will depart from x at the initial time of loading and with zero velocity. We prove these facts for admissible cracks belonging to the large class of closed one-dimensional sets with a finite number of connected components. The main tool we employ to address the problem is a local minimality result for the functional $$\epsilon(\nu, \Gamma)\,:=\int_{\Omega} f(x,\nabla v)\,{\rm d}x+k{\mathcal{H}}^{1} (\Gamma),$$ where $$\Omega \subseteq {\mathbb{R}}^{2}$$ , k > 0 and f is a suitable Carathéodory function. We prove that if the uncracked configuration u of Ω relative to a boundary displacement ψ has at most uniformly weak singularities, then configurations (uΓ, Γ) with $${\mathcal{H}}^{1} (\Gamma)$$ small enough are such that $$\epsilon(u,\emptyset) < \epsilon(u_{\Gamma},\Gamma)$$ .
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