1998
DOI: 10.1002/(sici)1099-1476(199806)21:9<823::aid-mma976>3.0.co;2-b
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Vector potentials in three-dimensional non-smooth domains

Abstract: This paper presents several results concerning the vector potential which can be associated with a divergence‐free function in a bounded three‐dimensional domain. Different types of boundary conditions are given, for which the existence, uniqueness and regularity of the potential are studied. This is applied firstly to the finite element discretization of these potentials and secondly to a new formulation of incompressible viscous flow problems.

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Cited by 783 publications
(1,005 citation statements)
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References 20 publications
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“…and applying the incompressibility constraint, we obtain 5) which implies that the pressure can be eliminated from (2.1). Moreover, we also introduce the velocity gradient as an auxiliary variable t := ∇u in Ω. Consequently, we end up with the following system, expressed in terms of the unknowns t, σ, and u:…”
Section: The Boundary Value Problemmentioning
confidence: 99%
“…and applying the incompressibility constraint, we obtain 5) which implies that the pressure can be eliminated from (2.1). Moreover, we also introduce the velocity gradient as an auxiliary variable t := ∇u in Ω. Consequently, we end up with the following system, expressed in terms of the unknowns t, σ, and u:…”
Section: The Boundary Value Problemmentioning
confidence: 99%
“…Since Ω is simply-connected, we recall from [2,Cor. 3.16] that this quantity is a norm, which is equivalent to the graph norm of H(div, Ω) ∩ H(curl, Ω), i.e., that there exists a constant c only depending on Ω such that…”
Section: Analysis Of the Modelmentioning
confidence: 99%
“…Let W be in X(Ω c ) and set W 1 = (1 − χ)W . Then, W 1 is in H 0 (curl; Ω 2 ) ∩ H(div; Ω 2 ) and therefore is in H s (Ω 2 ) (see [1]). …”
Section: Appendixmentioning
confidence: 99%