The \(\mathcal{A}\)-Stokes approximation for non-stationary problems (Q2814320)
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scientific article; zbMATH DE number 6595933
| Language | Label | Description | Also known as |
|---|---|---|---|
| English | The \(\mathcal{A}\)-Stokes approximation for non-stationary problems |
scientific article; zbMATH DE number 6595933 |
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21 June 2016
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A-caloric approximation
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A-Stokes approximation
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unsteady Stokes problem
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\(L^s\) approximations
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Lipschitz truncation
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0.9383633
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0.91111493
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0.9098326
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0.9094459
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0.9071971
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0.9059891
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0.90432763
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The \(\mathcal{A}\)-Stokes approximation for non-stationary problems (English)
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The paper is concerning the approximation theory for unsteady problems in fluid mechanics. The A-caloric approximation is used: in the heat equation, the operator \(\Delta u \) is replaced by \( \operatorname{div}( A \nabla u) \) where \(A\) is a tensor with good enough properties. The main point is to show that almost solutions to the A-caloric problem in a \(L^p\) type space can be approximated by functions in a \(L^s\) type space, with \(s<p\). The previous result [the author et al., J. Differ. Equations 253, No. 6, 1910--1942 (2012; Zbl 1245.35080)] is extended to the parabolic problems. An \(L^q\) theory for the non-stationary A-Stokes problem is given. Important tools are the parabolic maximal operators (with the inequality (2.4)), the Hardy-Littlewood maximal inequality and the Bogovskii operator (related with the differential equation \(\operatorname{div} u = f\)).
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