1993
DOI: 10.1137/0914020
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Analysis of Iterative Methods for the Steady and Unsteady Stokes Problem: Application to Spectral Element Discretizations

Abstract: Abstract. A new and detailed analysis of the basic Uzawa algorithm for decoupling of the pressure and the velocity in the steady and unsteady Stokes operator is presented. The paper focuses on the following new aspects: explicit construction of the Uzawa pressure-operator spectrum for a semiperiodic model problem; general relationship of the convergence rate of the Uzawa procedure to classical inf-sup discretization analysis; and application of the method to high-order variational discretization.

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Cited by 112 publications
(92 citation statements)
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“…(4.14), that a necessary condition for the stability of h/p methods, such as CG or DG, where both h and p refinement can be performed independently is dictated by: 17) where C h/p denotes a constant independent of the spatial discretisation. We also note that Maday et al [27] showed, in the context of the Uzawa algorithm when using high order C 0 schemes, that the inf-sup constant relates to the minimum eigenvalue of the pressure Schur complement of the discrete NS system, which is consistent with our analysis.…”
Section: Algebraic Systemsupporting
confidence: 91%
“…(4.14), that a necessary condition for the stability of h/p methods, such as CG or DG, where both h and p refinement can be performed independently is dictated by: 17) where C h/p denotes a constant independent of the spatial discretisation. We also note that Maday et al [27] showed, in the context of the Uzawa algorithm when using high order C 0 schemes, that the inf-sup constant relates to the minimum eigenvalue of the pressure Schur complement of the discrete NS system, which is consistent with our analysis.…”
Section: Algebraic Systemsupporting
confidence: 91%
“…First we orthogonalize the elements in X 0 N , followed by the elements in X e N . For the fully coupled system of Method 1, the corresponding Uzawa pressure operator can be constructed explicitly, and the smallest eigenvalue of this operator is directly connected to the inf-sup parameter β; see [14]. By computing numerically the minimum eigenvalue and the condition number of the Uzawa pressure operator, the numerical results indicate that these are constant for our problem and equal to 7.3×10 −2 and 14, respectively, independent of N (at least for the range of values we are dealing with).…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Further details regarding this kind of Schur-complement approximation can be found in [16] for generalized Stokes systems, in [29,14] for steady and unsteady Stokes systems, and in [30] for general partial differential equations. For unsteady Stokes problems the above approximation is known as the Cahouet-Chabard preconditioner [16].…”
Section: −1mentioning
confidence: 99%