具有临界直径的非周期性等周平面均质化:动态单边边界条件的通用非局部奇异项

Pub Date : 2024-03-11 DOI:10.1134/S1064562424701734
J. I. Díaz, T. A. Shaposhnikova, A. V. Podolskiy
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引用次数: 0

摘要

摘要 我们研究了当一个基本单元的直径(\(\varepsilon \))变为 0 时,扩散方程在一个平面域中的解的渐近行为。在被移除集合的边界上(或粒子集合的外部,如化学工程中出现的情况),我们考虑了动态单边 Signorini 边界条件,其中包含一个大增长参数 ( ( ( \beta (\varepsilon )\ ))。当问题的参数达到 "临界值 "时,我们将推导出均质化模型并证明其合理性。在这种情况下,均质化问题是普遍的(即它不依赖于穿孔或粒子的形状),并包含一个 "奇异项",该 "奇异项 "由一个非线性、时间非局部、单调的算子 H 给出,该算子被定义为一个 ODE 算子的障碍问题的解。极限问题的解可以取负值,即使在原始问题中,对于任何 \(\varepsilon \),在穿孔或粒子的边界上解都是非负的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Aperiodical Isoperimetric Planar Homogenization with Critical Diameter: Universal Non-local Strange Term for a Dynamical Unilateral Boundary Condition

Aperiodical Isoperimetric Planar Homogenization with Critical Diameter: Universal Non-local Strange Term for a Dynamical Unilateral Boundary Condition

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Aperiodical Isoperimetric Planar Homogenization with Critical Diameter: Universal Non-local Strange Term for a Dynamical Unilateral Boundary Condition

We study the asymptotic behavior of the solution to the diffusion equation in a planar domain, perforated by tiny sets of different shapes with a constant perimeter and a uniformly bounded diameter, when the diameter of a basic cell, \(\varepsilon \), goes to 0. This makes the structure of the heterogeneous domain aperiodical. On the boundary of the removed sets (or the exterior to a set of particles, as it arises in chemical engineering), we consider the dynamic unilateral Signorini boundary condition containing a large-growth parameter \(\beta (\varepsilon )\). We derive and justify the homogenized model when the problem’s parameters take the “critical values”. In that case, the homogenized problem is universal (in the sense that it does not depend on the shape of the perforations or particles) and contains a “strange term” given by a non-linear, non-local in time, monotone operator H that is defined as the solution to an obstacle problem for an ODE operator. The solution of the limit problem can take negative values even if, for any \(\varepsilon \), in the original problem, the solution is non-negative on the boundary of the perforations or particles.

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