12,131 research outputs found

    The Neumann problem in thin domains with very highly oscillatory boundaries

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    In this paper we analyze the behavior of solutions of the Neumann problem posed in a thin domain of the type Rϵ={(x1,x2)∈R2  ∣  x1∈(0,1), − ϵ b(x1)<x2<ϵ G(x1,x1/ϵα)}R^\epsilon = \{(x_1,x_2) \in \R^2 \; | \; x_1 \in (0,1), \, - \, \epsilon \, b(x_1) < x_2 < \epsilon \, G(x_1, x_1/\epsilon^\alpha) \} with α>1\alpha>1 and ϵ>0\epsilon > 0, defined by smooth functions b(x)b(x) and G(x,y)G(x,y), where the function GG is supposed to be l(x)l(x)-periodic in the second variable yy. The condition α>1\alpha > 1 implies that the upper boundary of this thin domain presents a very high oscillatory behavior. Indeed, we have that the order of its oscillations is larger than the order of the amplitude and height of RϵR^\epsilon given by the small parameter ϵ\epsilon. We also consider more general and complicated geometries for thin domains which are not given as the graph of certain smooth functions, but rather more comb-like domains.Comment: 20 pages, 4 figure

    Products of finite groups and nonmeasurable subgroups

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    It is proven that if GG is a finite group, then GωG^\omega has 2c2^{\mathfrak c} dense nonmeasurable subgroups. Also, other examples of compact groups with dense nonmeasurable subgroups are presented.Comment: 5 page

    Spectral analysis of the biharmonic operator subject to Neumann boundary conditions on dumbbell domains

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    We consider the biharmonic operator subject to homogeneous boundary conditions of Neumann type on a planar dumbbell domain which consists of two disjoint domains connected by a thin channel. We analyse the spectral behaviour of the operator, characterizing the limit of the eigenvalues and of the eigenprojections as the thickness of the channel goes to zero. In applications to linear elasticity, the fourth order operator under consideration is related to the deformation of a free elastic plate, a part of which shrinks to a segment. In contrast to what happens with the classical second order case, it turns out that the limiting equation is here distorted by a strange factor depending on a parameter which plays the role of the Poisson coefficient of the represented plate.Comment: To appear in "Integral Equations and Operator Theory
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