2020
DOI: 10.1016/j.cam.2019.112367
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Goal-oriented a posteriori error estimation for conforming and nonconforming approximations with inexact solvers

Abstract: We derive a unified framework for goal-oriented a posteriori estimation covering in particular higher-order conforming, nonconforming, and discontinuous Galerkin finite element methods, as well as the finite volume method. The considered problem is a model linear second-order elliptic equation with inhomogeneous Dirichlet and Neumann boundary conditions and the quantity of interest is given by an arbitrary functional composed of a volumetric weighted mean value (source) term and a surface weighted mean (Dirich… Show more

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Cited by 27 publications
(20 citation statements)
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“…Finally, Appendix C presents the application of our mass-conservative total flux reconstruction in H(div, Ω) to a challenging two-phase porous media flow problem with a finite volume fully implict/iterative coupling discretization. Applications to other problems, namely when deriving guaranteed upper bounds on the total error in presence of inexact solvers, have already been considered in [34,35] to steady and unsteady variational inequalities, in [26] to eigenvalue problems, in [60] to goal-oriented error estimates, and in [87,2] to degenerate multiphase (multicompositional) flows.…”
Section: Introductionmentioning
confidence: 99%
“…Finally, Appendix C presents the application of our mass-conservative total flux reconstruction in H(div, Ω) to a challenging two-phase porous media flow problem with a finite volume fully implict/iterative coupling discretization. Applications to other problems, namely when deriving guaranteed upper bounds on the total error in presence of inexact solvers, have already been considered in [34,35] to steady and unsteady variational inequalities, in [26] to eigenvalue problems, in [60] to goal-oriented error estimates, and in [87,2] to degenerate multiphase (multicompositional) flows.…”
Section: Introductionmentioning
confidence: 99%
“…In fact, it was observed in Reference 38 that g m is in most cases a better approximation of the true value g ex . A bounding of g ex is, therefore: ggexg+, where g:=gm12eCRΩ(u_H,σ__^H)eCRΩ(ũ_H˜,σ˜__^H˜), and g+:=gm+12eCRΩ(u_H,σ__^H)eCRΩ(ũ_H˜,σ˜__^H˜). …”
Section: Settingsmentioning
confidence: 96%
“…Recent developments dedicated a great deal of effort to account for inexactness of the algebraic approximations and introduce stopping criteria based on the interplay between discretization and algebraic computation in adaptive FEM. Among others, we mention the seminal contributions [10,26,4,5,34,30,33,32,21,31,29,20].…”
Section: Prolongate Smooth Solvementioning
confidence: 99%