A Weak Galerkin Finite Element Method for the Maxwell Equations
This paper introduces a numerical scheme for the time-harmonic Maxwell equations by using weak Galerkin (WG) finite element methods. The WG finite element method is based on two operators: discrete weak curl and discrete weak gradient, with appropriately defined stabilizations that enforce a weak co...
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| Published in | Journal of scientific computing Vol. 65; no. 1; pp. 363 - 386 |
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| Main Authors | , , , |
| Format | Journal Article |
| Language | English |
| Published |
New York
Springer US
01.10.2015
Springer Nature B.V |
| Subjects | |
| Online Access | Get full text |
| ISSN | 0885-7474 1573-7691 |
| DOI | 10.1007/s10915-014-9964-4 |
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| Summary: | This paper introduces a numerical scheme for the time-harmonic Maxwell equations by using weak Galerkin (WG) finite element methods. The WG finite element method is based on two operators: discrete weak curl and discrete weak gradient, with appropriately defined stabilizations that enforce a weak continuity of the approximating functions. This WG method is highly flexible by allowing the use of discontinuous approximating functions on arbitrary shape of polyhedra and, at the same time, is parameter free. Optimal-order of convergence is established for the WG approximations in various discrete norms which are either
H
1
-like or
L
2
and
L
2
-like. An effective implementation of the WG method is developed through variable reduction by following a Schur-complement approach, yielding a system of linear equations involving unknowns associated with element boundaries only. Numerical results are presented to confirm the theory of convergence. |
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| Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 14 |
| ISSN: | 0885-7474 1573-7691 |
| DOI: | 10.1007/s10915-014-9964-4 |