2000
DOI: 10.1016/s0764-4442(00)00311-6
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Coupled and uncoupled limits for a N -dimensional multidomain Neumann problem

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Cited by 4 publications
(8 citation statements)
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“…A preliminary version of these results, concerning the model problem, but including oscillating coefficients, was published in [12] with sketch of proofs.…”
Section: Introductionmentioning
confidence: 99%
“…A preliminary version of these results, concerning the model problem, but including oscillating coefficients, was published in [12] with sketch of proofs.…”
Section: Introductionmentioning
confidence: 99%
“…Then, by making use of the method of oscillating test functions, introduced by L. Tartar in [17], by applying some results obtained by A. Gaudiello, B. Gustafsson, C. Lefter and J. Mossino in [6] and [7] and by adapting the techniques used by M. Vanninathan in [16], we derive the limit eigenvalue problem and the limit of the rescaled basis, as n → +∞, in the case h n ≃ r For the study of thin multi-structures we refer to [2], [3], [4], [11], [12], [13], [14] and the references quoted therein. For a thin multi-structure as considered in this paper, we refer to [5], [6], [7], [8], [9] and [10]. For the study of the spectrum of the Laplace operator in a thin tube with a Dirichlet condition on its boundary we refer to [1].…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…6.2-1 and Th. 6.2-2 in [15]) for every n ∈ N, there exists an increasing diverging sequence of positive numbers {λ n,k } k∈N and a H n -Hilbert orthonormal basis {u n,k } k∈N , such that {λ n,k } k∈N forms the set of all the eigenvalues of the following problem: 5) and, for every k ∈ N, u n,k ∈ V n is an eigenvector of (2.5) with eigenvalue λ n,k . Moreover,…”
Section: Introduction and Main Resultsmentioning
confidence: 99%
“…The proofs of these results make use of the main ideas of Γ-convergence method introduced by E. De Giorgi (see [10]) and they develop in several steps: a priori estimates, construction of the recovery sequence, density results and l.s.c arguments (see Subsection 2.2). The main difficulty with respect to [11], where the asymptotic behavior of the Laplacian is studied when h n r 2 n , arises from the fact that the set of the admissible vector valued functions of Problem (1.1) is not a convex set, due to the constraint |V ((x 1 ,x 2 ,x 3 ))| = 1. This difficulty is overcome by working with a projection from R 3 into S 2 = {(x 1 ,x 2 ,x 3 ) ∈ R 3 : |(x 1 ,x 2 ,x 3 )| =1}, introduced in [4] (see also [1]), and by using the Sard's Lemma.…”
Section: Introductionmentioning
confidence: 99%
“…This difficulty is overcome by working with a projection from R 3 into S 2 = {(x 1 ,x 2 ,x 3 ) ∈ R 3 : |(x 1 ,x 2 ,x 3 )| =1}, introduced in [4] (see also [1]), and by using the Sard's Lemma. Moreover, point out that the cases h n << r 2 n and h n >> r 2 n are not treated in [11]. Remark that it is not necessary that the two cylinders are scaled to the same one or that the first cylinder has height 1.…”
Section: Introductionmentioning
confidence: 99%