1985
DOI: 10.2307/2007793
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Analysis of Some Finite Elements for the Stokes Problem

Abstract: Abstract. We study some finite elements which are used in the approximation of the Stokes problem, so as to obtain error estimates of optimal order.Résumé. Nous étudions deux éléments finis utilisés pour l'approximation du problème de Stokes et obtenons des estimations d'erreur d'ordre optimal.

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Cited by 80 publications
(123 citation statements)
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“…We first solve the Stokes eigenvalue problem (2.12) by the lowest order Bernardi-Raugel mixed finite element ( [6], [9] and [14]) and solve the Stokes source problem (3.4) by the Q 2 − P 1 mixed finite element on the rectangular meshes ( [9] and [14]). Now, we introduce the lowest order Bernadi-Raugel mixed finite element V h = {v ∈ (H 1 0 (Ω)) 2 : v| e ∈ Q 12 × Q 21 , ∀ e ∈ T h },…”
Section: Numerical Resultsmentioning
confidence: 99%
“…We first solve the Stokes eigenvalue problem (2.12) by the lowest order Bernardi-Raugel mixed finite element ( [6], [9] and [14]) and solve the Stokes source problem (3.4) by the Q 2 − P 1 mixed finite element on the rectangular meshes ( [9] and [14]). Now, we introduce the lowest order Bernadi-Raugel mixed finite element V h = {v ∈ (H 1 0 (Ω)) 2 : v| e ∈ Q 12 × Q 21 , ∀ e ∈ T h },…”
Section: Numerical Resultsmentioning
confidence: 99%
“…(Ω S ) be the Bernardi-Raugel interpolation operator (see [9,30]), which is linear and bounded with respect to the H 1 (Ω S )-norm. We remark that, given v ∈ H 1 ΓS (Ω S ), there holds…”
Section: Preliminariesmentioning
confidence: 99%
“…[4,9,11,24,44]). Note that each one of them is named after the unknown to which it is applied later on.…”
Section: Convergence Of the Galerkin Schemementioning
confidence: 99%
“…Fig. 2, by the divergence Q k+1,k − Q k,k+1 element (2.3) and by the rotated Bernardi-Raugel element [5,10,21]:…”
Section: Numerical Testsmentioning
confidence: 99%
“…Ainsworth and Coggins established [1] the stability and the optimal order of convergence for the Taylor-Hood Q k+1 /Q k element, where the pressure space is continuous too. The Bernardi-Raugel element [5] optimizes the Q k+1 /Q dc k−1 element, when k = 1, by reducing the velocity space to Q 1,2 − Q 2,1 polynomials. Here the first component of velocity in the Bernardi-Raugel element is a polynomial of degree 1 in x direction, but of degree 2 in y direction.…”
mentioning
confidence: 99%