171 research outputs found

    Mesoscale asymptotic approximations to solutions of mixed boundary value problems in perforated domains

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    We describe a method of asymptotic approximations to solutions of mixed boundary value problems for the Laplacian in a three-dimensional domain with many perforations of arbitrary shape, with the Neumann boundary conditions being prescribed on the surfaces of small voids. The only assumption made on the geometry is that the diameter of a void is assumed to be smaller compared to the distance to the nearest neighbour. The asymptotic approximation, obtained here, involves a linear combination of dipole fields constructed for individual voids, with the coefficients, which are determined by solving a linear algebraic system. We prove the solvability of this system and derive an estimate for its solution. The energy estimate is obtained for the remainder term of the asymptotic approximation.Comment: 20 pages, 8 figure

    Eigenvalue problem in a solid with many inclusions: asymptotic analysis

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    We construct the asymptotic approximation to the first eigenvalue and corresponding eigensolution of Laplace's operator inside a domain containing a cloud of small rigid inclusions. The separation of the small inclusions is characterised by a small parameter which is much larger compared with the nominal size of inclusions. Remainder estimates for the approximations to the first eigenvalue and associated eigenfield are presented. Numerical illustrations are given to demonstrate the efficiency of the asymptotic approach compared to conventional numerical techniques, such as the finite element method, for three-dimensional solids containing clusters of small inclusions.Comment: 55 pages, 5 figure

    Mesoscale models and approximate solutions for solids containing clouds of voids

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    For highly perforated domains the paper addresses a novel approach to study mixed boundary value problems for the equations of linear elasticity in the framework of mesoscale approximations. There are no assumptions of periodicity involved in the description of the geometry of the domain. The size of the perforations is small compared to the minimal separation between neighboring defects and here we discuss a class of problems in perforated domains, which are not covered by the homogenization approximations. The mesoscale approximations presented here are uniform. Explicit asymptotic formulas are supplied with the remainder estimates. Numerical illustrations, demonstrating the efficiency of the asymptotic approach developed here, are also given

    Asymptotic analysis of solutions to transmission problems in solids with many inclusions

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    We construct an asymptotic approximation to the solution of a transmission problem for a body containing a region occupied by many small inclusions. The cluster of inclusions is characterised by two small parameters that determine the nominal diameter of individual inclusions and their separation within the cluster. These small parameters can be comparable to each other. Remainder estimates of the asymptotic approximation are rigorously justified. Numerical illustrations demonstrate the efficiency of the asymptotic approach when compared with benchmark finite element algorithms.Comment: 30 pages, 5 figure

    Interaction of scales for a singularly perturbed degenerating nonlinear Robin problem

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    We study the asymptotic behaviour of solutions of a boundary value problem for the Laplace equation in a perforated domain in [Formula: see text], [Formula: see text], with a (nonlinear) Robin boundary condition on the boundary of the small hole. The problem we wish to consider degenerates in three respects: in the limit case, the Robin boundary condition may degenerate into a Neumann boundary condition, the Robin datum may tend to infinity, and the size ϵ of the small hole where we consider the Robin condition collapses to 0. We study how these three singularities interact and affect the asymptotic behaviour as ϵ tends to 0, and we represent the solution and its energy integral in terms of real analytic maps and known functions of the singular perturbation parameters. This article is part of the theme issue 'Non-smooth variational problems and applications'

    Interaction of scales for a singularly perturbed degenerating nonlinear Robin problem

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    We study the asymptotic behavior of the solutions of a boundary value problem for the Laplace equation in a perforated domain in Rn\mathbb{R}^n, n3n\geq 3, with a (nonlinear) Robin boundary condition on the boundary of the small hole. The problem we wish to consider degenerates under three aspects: in the limit case the Robin boundary condition may degenerate into a Neumann boundary condition, the Robin datum may tend to infinity, and the size ϵ\epsilon of the small hole where we consider the Robin condition collapses to 00. We study how these three singularities interact and affect the asymptotic behavior as ϵ\epsilon tends to 00, and we represent the solution and its energy integral in terms of real analytic maps and known functions of the singular perturbation parameters

    Meso-Scale Approximations of Fields Around Clusters of Defects

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    The Dirichlet problem in a planar domain with two moderately close holes

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    We investigate a Dirichlet problem for the Laplace equation in a domain of R2\mathbb{R}^2 with two small close holes. The domain is obtained by making in a bounded open set two perforations at distance ϵ1|\epsilon_1| one from the other and each one of size ϵ1ϵ2|\epsilon_1\epsilon_2|. In such a domain, we introduce a Dirichlet problem and we denote by uϵ1,ϵ2u_{\epsilon_1,\epsilon_2} its solution. We show that the dependence of uϵ1,ϵ2u_{\epsilon_1,\epsilon_2} upon (ϵ1,ϵ2)(\epsilon_1,\epsilon_2) can be described in terms of real analytic maps of the pair (ϵ1,ϵ2)(\epsilon_1,\epsilon_2) defined in an open neighborhood of (0,0)(0,0) and of logarithmic functions of ϵ1\epsilon_1 and ϵ2\epsilon_2. Then we study the asymptotic behaviour of of uϵ1,ϵ2u_{\epsilon_1,\epsilon_2} as ϵ1\epsilon_1 and ϵ2\epsilon_2 tend to zero. We show that the first two terms of an asymptotic approximation can be computed only if we introduce a suitable relation between ϵ1\epsilon_1 and ϵ2\epsilon_2
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