2016
DOI: 10.1016/j.camwa.2016.08.032
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A posteriori error analysis of an augmented mixed method for the Navier–Stokes equations with nonlinear viscosity

Abstract: In this work we develop the a posteriori error analysis of an augmented mixed finite element method for the 2D and 3D versions of the Navier-Stokes equations when the viscosity depends nonlinearly on the module of the velocity gradient. Two different reliable and efficient residual-based a posteriori error estimators for this problem on arbitrary (convex or non-convex) polygonal and polyhedral regions are derived. Our analysis of reliability of the proposed estimators draws mainly upon the global inf-sup condi… Show more

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Cited by 20 publications
(27 citation statements)
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“…Finally, the derivation of the upper bound for boldR 2 false‖ 0 ( d i v ; Ω ) makes use of a stable Helmholtz decomposition for 0 ( d i v ; Ω ) which has been recently proved for n = 3 in , Lemma 4.3] (see also , Theorem 3.1]), the Raviart–Thomas interpolation operator (see ), the classical Clément interpolator (), and the local approximation properties of them. This estimate follows basically from suitable modifications of the proofs of , Theorem 3.7] and , Lemmas 3.8 and 3.9]. In this regard, we just comment that within the process of bounding boldR 2 false‖ 0 ( d i v ; Ω ) it also appears the local term h T 2 bold-italicu h bold-italict h bold-italicρ h false‖ 0 , T 2 , which being dominated by e ( bold-italicu h ) bold-italict h false‖ 0 , T 2 + bold-italicρ h bold-italicu h + e ( bold-italicu h ) false‖ 0 , T 2 , is then omitted from the final definition of Θ T 2 (cf.…”
Section: A Posteriori Error Analysismentioning
confidence: 86%
See 3 more Smart Citations
“…Finally, the derivation of the upper bound for boldR 2 false‖ 0 ( d i v ; Ω ) makes use of a stable Helmholtz decomposition for 0 ( d i v ; Ω ) which has been recently proved for n = 3 in , Lemma 4.3] (see also , Theorem 3.1]), the Raviart–Thomas interpolation operator (see ), the classical Clément interpolator (), and the local approximation properties of them. This estimate follows basically from suitable modifications of the proofs of , Theorem 3.7] and , Lemmas 3.8 and 3.9]. In this regard, we just comment that within the process of bounding boldR 2 false‖ 0 ( d i v ; Ω ) it also appears the local term h T 2 bold-italicu h bold-italict h bold-italicρ h false‖ 0 , T 2 , which being dominated by e ( bold-italicu h ) bold-italict h false‖ 0 , T 2 + bold-italicρ h bold-italicu h + e ( bold-italicu h ) false‖ 0 , T 2 , is then omitted from the final definition of Θ T 2 (cf.…”
Section: A Posteriori Error Analysismentioning
confidence: 86%
“…To prove the reliability of our a posteriori error estimator, we follow the strategy proposed originally in , and then used in , which is based on a linearization technique that involves the Gâteaux derivatives of the nonlinear terms of the formulation. More precisely, proceeding similarly as in , we begin with the result to be introduced next. However, we notice in advance that due to the new meaning of the unknown bold-italict and the presence of additional terms in the present augmented formulation, two of the resulting bounded functionals, whose norms need to be estimated later on, do not coincide with those in (see boldR 3 and boldR 4 below).Lemma Let bold-italict true→ H and bold-italict true→ h boldH h be the unique solutions of the continuous and discrete problems (3.5) and (4.1), respectively.…”
Section: A Posteriori Error Analysismentioning
confidence: 99%
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“…The remaining terms in 2 B,T and 2 D,T can be treated very much in the same way as done in [24,27,28], where the analysis is based on inverse inequalities found in [19], together with the localisation technique based on tetrahedron-bubble and facetbubble functions [34]. Such a theory requires further notation and preliminary results collected in what follows.…”
Section: Efficiencymentioning
confidence: 99%