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Abstrakty
The aim of this paper is to give a direct boundary integral equations method for the slow motion of some rigid bodies of an arbitrary shape, near a plane wall in a viscous incompressible fluid. By using an integral representation of the velocity field as a sum between single-layer potentials and double-layer potentials, the problem is reduced to the study of a Fredholm integral system of the second kind. By following the properties of the single-layer and double-layer operators, the existence and uniqueness result of the corresponding solution is given. The numerical results are obtained by a standard boundary element method.
Czasopismo
Rocznik
Tom
Strony
217--232
Opis fizyczny
Bibliogr. 11 poz., wykr.
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- University Babes-Bolyai, Faculty of Mathematics Cluj - Napoca, ROMANIA
Bibliografia
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Bibliografia
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bwmeta1.element.baztech-article-BPZ2-0013-0011