Encyclopedia of Computational Mechanics 2004
DOI: 10.1002/0470091355.ecm023
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Finite Element Methods for M axwell Equations

Abstract: The article reviews fundamentals of Finite Element discretizations of time‐harmonic Maxwell equations. The paper includes a short introduction to Maxwell equations, derivation of the standard and regularized variational formulations, discussion of three fundamental Nedelec's elements in context of exact sequences, projection‐based interpolation, and the commuting diagram property. The presentation is biased towards hp ‐discretizations and hp ‐adaptivity.

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Cited by 11 publications
(10 citation statements)
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“…More specifically, recall that in Section 2, the weak form (9) for the local error equation equipped with the natural boundary condition (12) results in the variational problem (15) which is well posed by Lemma 2 if and only if k is not an eigenvalue of the appropriate boundary value problem (18). In this section, we determine the eigenvalues belonging to cubic subdomains.…”
Section: Lemmamentioning
confidence: 98%
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“…More specifically, recall that in Section 2, the weak form (9) for the local error equation equipped with the natural boundary condition (12) results in the variational problem (15) which is well posed by Lemma 2 if and only if k is not an eigenvalue of the appropriate boundary value problem (18). In this section, we determine the eigenvalues belonging to cubic subdomains.…”
Section: Lemmamentioning
confidence: 98%
“…The quantity γ τ curlE will be called the natural boundary data from now on. In the literature, the homogeneous natural boundary condition is called the magnetic symmetry wall condition [15]. Introducing this approximation into (9) we arrive at the variational problem for the implicit error estimate: Find…”
Section: Formulation Of the Local Problemmentioning
confidence: 99%
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“…It supports geometrical refinements through the use of its own geometrical package to accurately model the problem geometry. Hexahedral H(curl) conforming finite elements satisfying the commutativity of the so-called de Rham diagram and hence, assuring convergence and stability of the numerical solution, are used, [8,7].…”
Section: Hp-fem and Automatic Hp-adaptivity In 3dmentioning
confidence: 99%
“…With the electric field vanishing in a perfect conductor, and the tangential component of E being continuous across material interfaces, the tangential component of E on a boundary adjacent to a perfect conductor must vanish [8] n ×Ê φ = 0. In our case this simply translates into the condition,…”
Section: Statement Of the Problemmentioning
confidence: 99%