1990
DOI: 10.1016/0045-7825(90)90121-2
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A least-squares finite element method for the Helmholtz equation

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Cited by 42 publications
(29 citation statements)
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“…As we shall see below, for (2.12), optimal convergence in the H 1 (Ω)-norm requires an additional "grid decomposition property" on the finite element spaces (see [61] and [72]) or an additional "curl" constraint added to the first-order system (2.11) (see [43], [44], [48], [49], [95], and [106].) Other examples of first-order systems that are not H 1 -coercive are given by particular decompositions of the biharmonic equation and the Stokes problem.…”
Section: A Recipe For Practicalitymentioning
confidence: 99%
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“…As we shall see below, for (2.12), optimal convergence in the H 1 (Ω)-norm requires an additional "grid decomposition property" on the finite element spaces (see [61] and [72]) or an additional "curl" constraint added to the first-order system (2.11) (see [43], [44], [48], [49], [95], and [106].) Other examples of first-order systems that are not H 1 -coercive are given by particular decompositions of the biharmonic equation and the Stokes problem.…”
Section: A Recipe For Practicalitymentioning
confidence: 99%
“…In view of the equation v = grad φ, one can augment (2.11) by a compatibility condition known as the curl constraint (see, e.g., [55], [49], [48], and [95])…”
Section: Discretization Levelmentioning
confidence: 99%
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“…The idea of adding the curl constraint in developing a least-squares functional for Poisson's equation has been used by several researchers (see, e.g., [13,16,17,23,14,15,24,30]). For Poisson's equation, the key tool is the proof that (H(div) ∩ H(curl)) is algebraically and topologically imbedded in (H 1 ) n , which was developed by Girault and Raviart [20] for problems with strictly Dirichlet or Neumann boundary conditions.…”
mentioning
confidence: 99%
“…Finite element methods for acoustic wave propagation problems such as (1.1a)-(1.1c) have been widely studied in the literature (cf., e.g., [4,12,15,28,30] as well as the survey article [17], the monographs [27,29] and the references therein). In case of large wavenumbers k, the finite element discretization typically requires fine meshes for a proper resolution of the waves and thus results in large linear algebraic systems to be solved.…”
mentioning
confidence: 99%