Abstract:The interest in the use of quasimodes, or almost frequencies and almost eigenfunctions, to describe asymptotics for low-frequency and high-frequency vibrations in certain singularly perturbed spectral problems, which depend on a small parameter e, has been recently highlighted in many papers. In this paper we deal with the low frequencies for a Steklov-type eigenvalue homogenization problem: we consider harmonic functions in a bounded domain of R 2 , and strongly alternating boundary conditions of the Dirichle… Show more
“…The verification of the equivalence is of great importance because there exist many examples (cf., e.g., [33]) when a substitution in a problem with corner singularities leads to incorrect solutions. It is also of great importance when dealing with evolution problems (cf., e.g., [19]). In addition, notice that infinitely many realizations of an elliptic problem as a self-adjoint operator with the discrete spectra occur in domains with corners (cf.…”
Section: The Eigenvalue Sequence: What Is Known and What Is Expectedmentioning
We construct two-term asymptotics λ ε k = ε m−2 (M + εµ k + O(ε 3/2)) of eigenvalues of a mixed boundary-value problem in Ω ⊂ R 2 with many heavy (m > 2) concentrated masses near a straight part Γ of the boundary ∂Ω. ε is a small positive parameter related to size and periodicity of the masses; k ∈ N. The main term M > 0 is common for all eigenvalues but the correction terms µ k , which are eigenvalues of a limit problem with the spectral Steklov boundary conditions on Γ, exhibit the effect of asymptotic splitting in the eigenvalue sequence enabling the detection of asymptotic forms of eigenfunctions. The justification scheme implies isolating and purifying singularities of eigenfunctions and leads to a new spectral problem in weighed spaces with a "strongly" singular weight.
“…The verification of the equivalence is of great importance because there exist many examples (cf., e.g., [33]) when a substitution in a problem with corner singularities leads to incorrect solutions. It is also of great importance when dealing with evolution problems (cf., e.g., [19]). In addition, notice that infinitely many realizations of an elliptic problem as a self-adjoint operator with the discrete spectra occur in domains with corners (cf.…”
Section: The Eigenvalue Sequence: What Is Known and What Is Expectedmentioning
We construct two-term asymptotics λ ε k = ε m−2 (M + εµ k + O(ε 3/2)) of eigenvalues of a mixed boundary-value problem in Ω ⊂ R 2 with many heavy (m > 2) concentrated masses near a straight part Γ of the boundary ∂Ω. ε is a small positive parameter related to size and periodicity of the masses; k ∈ N. The main term M > 0 is common for all eigenvalues but the correction terms µ k , which are eigenvalues of a limit problem with the spectral Steklov boundary conditions on Γ, exhibit the effect of asymptotic splitting in the eigenvalue sequence enabling the detection of asymptotic forms of eigenfunctions. The justification scheme implies isolating and purifying singularities of eigenfunctions and leads to a new spectral problem in weighed spaces with a "strongly" singular weight.
“…We mention some of the first works in which keywords such as critical sizes and critical relations between parameters have been introduced [7,29,30] and [35], also [8] for nonhomogeneous boundary conditions. Let us refer to [5,6] and references therein for rapidly alternating Dirichlet-Steklov boundary conditions and [11,18,28] for further references and possible applications in the framework of Geophysics and Winkler beds (foundations). See [9][10][11][12][13][14][15] and [32] for an extensive and updated bibliography on different boundary homogenization problems with Robin-type boundary conditions.…”
We consider a homogenization problem for the Laplace operator posed in a bounded domain of the upper half-space, a part of its boundary being in contact with the plane $$\{x_3=0\}$$
{
x
3
=
0
}
. On this part, the boundary conditions alternate from Neumann to nonlinear-Robin, being of Dirichlet type outside. The nonlinear-Robin boundary conditions are imposed on small regions periodically placed along the plane and contain a Robin parameter that can be very large. We provide all the possible homogenized problems, depending on the relations between the three parameters: period $$\varepsilon $$
ε
, size of the small regions $$r_\varepsilon $$
r
ε
and Robin parameter $$\beta (\varepsilon )$$
β
(
ε
)
. In particular, we address the convergence, as $$\varepsilon $$
ε
tends to zero, of the solutions for the critical size of the small regions $$r_\varepsilon =O(\varepsilon ^{ 2})$$
r
ε
=
O
(
ε
2
)
. For certain $$\beta (\varepsilon )$$
β
(
ε
)
, a nonlinear capacity term arises in the strange term which depends on the macroscopic variable and allows us to extend the usual capacity definition to semilinear boundary conditions.
“…We explicitly notice that the low frequencies are related only with longitudinal vibrations along each branch of the T-like shaped thin structure (see Theorem 2.1 and Figure 2 (a)), while our results capture also vibrations depending on both variables, which are referred to as transverse vibrations along each branch, and are produced by high frequencies (see Theorems 5.2-5.4, Remark 5.5 and Figure 2 (b)). In fact, we get results for eigenvalues and eigenfunctions of (1.1) which are of interest in terms of the associated evolution problems since, from (1.8), we can construct standing waves which approach time-dependent solutions for long times, and these times can be precisely computed in terms of bounds for discrepancies such as that in (1.5) (see [41] and [34] for an abstract framework as well as for applications to very different vibrating systems). It should be emphasized that it seems to be a common fact to many mechanical systems arising in thin structures that the low frequencies give rise to longitudinal vibrations while for other kinds of vibrations such as torsional or stretching vibrations one must look among those associated to the high frequencies: see, for instance, [8], [23], [24], [35] and references therein.…”
We consider a spectral problem for the Laplacian operator in a planar T-like shaped thin structure Ω ε , where ε denotes the transversal thickness of both branches. We assume the homogeneous Dirichlet boundary condition on the ends of the branches and the homogeneous Neumann boundary condition on the remaining part of the boundary of Ω ε . We study the asymptotic behavior, as ε tends to zero, of the high frequencies of such a problem. Unlike the asymptotic behavior of the low frequencies where the limit problem involves only longitudinal vibrations along each branch of the T-like shaped thin structure (i.e. 1D limit spectral problems), we obtain a two dimensional limit spectral problem which allows us to capture other kinds of vibrations. We also give a characterization of the asymptotic form of the eigenfunctions originating these vibrations.Résumé: On considère le problème spectral pour le Laplacien, dans une structure mince bidimensionnelle Ω ε en forme de T, où ε désigne l'épaisseur des deux branches du T. Les conditions aux limites sont du type Neumann homogène sur tout le bord sauf aux extrémités des branches où une condition de Dirichlet homogène est imposée. Onétudie le comportement asymptotique des hautes fréquences lorsque ε tend vers zéro. Contrairement au comportement asymptotique des basses fréquences, pour lesquelles le problème limite ne fait apparaître que des vibrations longitudinales le long de chaque branche de la structure (c'est-à-dire, des problèmes spectraux limites 1D ), on obtientà la limite un problème spectral bidimensionnel, qui nous permet de capter d'autres types de vibrations. On donneégalement une caractérisation de la forme asymptotique des fonctions propres qui sontà l'origine de ces vibrations.
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