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2019 | OriginalPaper | Chapter

6. Stokes–Darcy Equations

Author : Ulrich Wilbrandt

Published in: Stokes–Darcy Equations

Publisher: Springer International Publishing

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Abstract

Let \(\varOmega \subset \mathbb {R}^d\) be a Lipschitz domain split into two disjoint nonempty subdomains Ω p and Ω f which are Lipschitz, too. The index p refers to the Darcy subdomain where a porous medium is modeled, while the index f refers to the free flow domain with a Stokes model.

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Footnotes
1
Sometimes also called Beavers–Joseph–Saffman–Jones condition.
 
2
With this ψ it is \(a_{\mathrm {p}}(\varphi ,\psi ) = a_{\mathrm {p}}^R(\varphi ,\psi )\).
 
3
With this v it is https://static-content.springer.com/image/chp%3A10.1007%2F978-3-030-02904-3_6/470501_1_En_6_IEq224_HTML.gif .
 
4
The signs and positions of η f and η p are chosen such that the resulting system matches that in [DQV07] and [CGHW11].
 
5
For this approach it is assumed that Λ f = Λ p, see Sect. 6.6.8.
 
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Metadata
Title
Stokes–Darcy Equations
Author
Ulrich Wilbrandt
Copyright Year
2019
DOI
https://doi.org/10.1007/978-3-030-02904-3_6

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