Nonlinear Variational Inequalities with Bilateral Constraints Coinciding on a Set of Positive Measure

Pub Date : 2024-04-18 DOI:10.1134/S1064562424701813
A. A. Kovalevsky
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Abstract

We consider variational inequalities with invertible operators \({{\mathcal{A}}_{s}}{\text{:}}~\,W_{0}^{{1,p}}\left( {{\Omega }} \right) \to {{W}^{{ - 1,p'}}}\left( {{\Omega }} \right),\) \(s \in \mathbb{N},\) in divergence form and with constraint set \(V = \{ {v} \in W_{0}^{{1,p}}\left( {{\Omega }} \right){\text{: }}\varphi \leqslant {v} \leqslant \psi ~\) a.e. in \({{\Omega }}\} ,\) where \({{\Omega }}\) is a nonempty bounded open set in \({{\mathbb{R}}^{n}}\) \(\left( {n \geqslant 2} \right)\), p > 1, and \(\varphi ,\psi {{:\;\Omega }} \to \bar {\mathbb{R}}\) are measurable functions. Under the assumptions that the operators \({{\mathcal{A}}_{s}}\) G-converge to an invertible operator \(\mathcal{A}{\text{: }}W_{0}^{{1,p}}\left( {{\Omega }} \right) \to {{W}^{{ - 1,p'}}}\left( {{\Omega }} \right)\), \({\text{int}}\left\{ {\varphi = \psi } \right\} \ne \varnothing ,\) \({\text{meas}}\left( {\partial \left\{ {\varphi = \psi } \right\} \cap {{\Omega }}} \right)\) = 0, and there exist functions \(\bar {\varphi },\bar {\psi } \in W_{0}^{{1,p}}\left( {{\Omega }} \right)\) such that \(\varphi \leqslant \overline {\varphi ~} \leqslant \bar {\psi } \leqslant \psi \) a.e. in \({{\Omega }}\) and \({\text{meas}}\left( {\left\{ {\varphi \ne \psi } \right\}{{\backslash }}\left\{ {\bar {\varphi } \ne \bar {\psi }} \right\}} \right) = 0,\) we establish that the solutions us of the variational inequalities converge weakly in \(W_{0}^{{1,p}}\left( {{\Omega }} \right)\) to the solution u of a similar variational inequality with the operator \(\mathcal{A}\) and the constraint set V. The fundamental difference of the considered case from the previously studied one in which \({\text{meas}}\left\{ {\varphi = \psi } \right\} = 0\) is that, in general, the functionals \({{\mathcal{A}}_{s}}{{u}_{s}}\) do not converge to \(\mathcal{A}u\) even weakly in \({{W}^{{ - 1,p'}}}\left( {{\Omega }} \right)\) and the energy integrals \(\langle {{\mathcal{A}}_{s}}{{u}_{s}},{{u}_{s}}\rangle \) do not converge to \(\langle \mathcal{A}u,u\rangle \).

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非线性变分不等式与正量程集合上的双边约束重合
Abstract We consider variational inequalities with invertible operators \({{\mathcal{A}}_{s}}{text{:}}~\,W_{0}^{{1,p}}}left( {{Omega }} \right) \to {{W}^{ - 1,p'}}}left( {{Omega }} \right),\)\(s在mathbb{N},\)中的发散形式和约束集\(V = \{v} \ in W_{0}^{1,p}}left( {{\Omega }} \right){\text{:}}varphi \leqslant {v} \leqslant \psi ~\) a.e..in \({{\Omega }}} ,\) where \({{\Omega }}\) is a nonempty bounded open set in \({{\mathbb{R}}^{n}}\) \(\left( {n \geqslant 2} \right)\), p > 1, and \(\varphi ,\psi {text{:Omega } \to bar\{mathbb{R}}\) 都是可测函数。假设算子 \({{mathcal{A}}_{s}}\) G-converge 到一个可逆算子 \(\mathcal{A}}\{text{:W_{0}^{{1,p}}}left( {{\Omega }} \right) \to {{W}^{ -1,p'}}}left( {{\Omega }} \right)\), (({ \text{int}}}left\{ {\varphi = \psi } \right\} \ne \emptyset 、\)({\text{meas}}左({\partial \left\{ {\varphi = \psi } \right} \cap {\Omega }} \right))= 0,并且存在函数(\bar {\varphi },\bar {\psi })。\in W_{0}^{1,p}}left( {{\Omega }} \right)\) such that \(\varphi \leqslant \overline {\varphi ~})\(leqslant) (bar {\psi }\a.e. in \({{\Omega }}\) and \({\text{meas}}left( {\left\{ {{varphi \ne\psi } })\right}({{backslash}}) (left) ({\bar {\varphi }\ne\bar {\psi }\Rright}\right) = 0,()我们确定变分不等式的解 us 在 \(W_{0}^{1,p}}\left( {{\Omega }} \right)\)中弱收敛于具有算子 \(\mathcal{A}\)和约束集 V 的类似变分不等式的解 u。所考虑的情况与之前研究的情况({\text{meas}}\left\{ {\varphi = \psi } \right\} = 0\ )的根本区别在于,一般来说,函数 \({{\mathcal{A}}_{s}}{{u}_{s}}\) 不会收敛到 \({{W}^{ - 1、p'}}}left({{\Omega}}\right)\),能量积分 \(angle {{mathcal{A}}_{s}}{{u}_{s}},{{u}_{s}}\rangle \)也不会收敛到 \(\langle \mathcal{A}}u,u\rangle \)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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