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.
“…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 },…”
“…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 },…”
“…(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
Citation: DISCACCIATI, M. and OYARZUA, R., 2016. A conforming mixed finite element method for the Navier Stokes/Darcy coupled problem. Numerische Mathematik, 135(2), pp. 571 606. Abstract In this paper we develop the a priori analysis of a mixed finite element method for the coupling of fluid flow with porous media flow. Flows are governed by the Navier-Stokes and Darcy equations, respectively, and the corresponding transmission conditions are given by mass conservation, balance of normal forces, and the Beavers-Joseph-Saffman law. We consider the standard mixed formulation in the Navier-Stokes domain and the dual-mixed one in the Darcy region, which yields the introduction of the trace of the porous medium pressure as a suitable Lagrange multiplier. The finite element subspaces defining the discrete formulation employ Bernardi-Raugel and RaviartThomas elements for the velocities, piecewise constants for the pressures, and continuous piecewise linear elements for the Lagrange multiplier. We show stability, convergence, and a priori error estimates for the associated Galerkin scheme. Finally, several numerical results illustrating the good performance of the method and confirming the theoretical rates of convergence are reported.
“…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.…”
By the standard theory, the stable Q k+1,k − Q k,k+1 /Q dc k divergence-free element converges with the optimal order of approximation for the Stokes equations, but only order k for the velocity in H 1 -norm and the pressure in L 2 -norm. This is due to one polynomial degree less in y direction for the first component of velocity, which is a Q k+1,k polynomial of x and y. In this manuscript, we will show by supercloseness of the divergence free element that the order of convergence is truly k + 1, for both velocity and pressure. For special solutions (if the interpolation is also divergence-free), a two-order supercloseness is shown to exist. Numerical tests are provided confirming the accuracy of the theory.
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