Axioms of Adaptivity (AoA) in Lecture 2 (sufficient for optimal convergence rates)
|
|
- Ursula Tate
- 5 years ago
- Views:
Transcription
1 Axioms of Adaptivity (AoA) in Lecture 2 (sufficient for optimal convergence rates) Carsten Carstensen Humboldt-Universität zu Berlin 2018 International Graduate Summer School on Frontiers of Applied and Computational Mathematics Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
2 Contents L2 1 Reduction Property 2 Plain Convergence 3 Linear Convergence 4 Quasimonotonicity 5 Comparison Lemma 6 Repetition on Optimal Rates 7 Separate Marking 8 Alternative Adaptive LS FEM 4 Laplace Open-Access Reference: C-Feischl-Page-Praetorius: AoA. Comp Math Appl 67 (2014) Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
3 Reduction Property Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
4 With Dörfler Marking (A1)+(A2)=(A12) Abbreviate T := T l and T := T l+1 in (A1)-(A2) with η(k) := η l (K) for K T resp. η(t ) := η l+1 (T ) for T T and δ := δ(t, T ). Then (A1)-(A2) read η( T T ) η(t T ) Λ 1 δ η( T \ T ) ϱ 2 η(t \ T ) + Λ 2 δ Underlying sum convention η 2 (M) := M M η2 (M) Since marked T are refined, Dörfler marking leads to Θη 2 (T ) η 2 (T \ T ) Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
5 Weighted geometric-arithmetic mean inequality for a, b R reads (a + b) 2 (1 + λ) a 2 + (1 + 1/λ) b 2 for all λ > 0 (with equality if a, b > 0 for the minimizing choice of λ) Application to (A1) shows for any λ > 0 η 2 ( T T ) (1 + λ)η 2 (T T ) + (1 + 1/λ)Λ 2 1δ 2 Application to (A2) shows for any µ > 0 η 2 ( T \ T ) ϱ 2 2(1 + µ)η 2 (T \ T ) + (1 + 1/µ)Λ 2 2 δ 2 The sum gives η 2 ( T ) = η 2 ( T T ) + η 2 ( T \ T ) on LHS Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
6 Hence η 2 ( T ) (1 + λ)η 2 (T T ) + ϱ 2 2(1 + µ)η 2 (T \ T ) + ( (1 + 1/λ)Λ (1 + 1/µ)Λ 2 ) 2 2 δ }{{} Λ 12 Recall 0 < Θ 1 and 0 < ϱ 2 < 1 so there exist 0 < µ < ϱ and 0 < λ < Θ 1 (1 + µ)ϱ2 2 1 Θ Theorem (A12) (A1)-(A2) and Dörfler marking imply η 2 ( T ) ϱ 12 η 2 (T ) + Λ 12 δ 2 with ϱ 12 < 1 and Λ 12 < for any such choice of λ, µ Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
7 Proof of (A12) Recall η 2 ( T ) (1 + λ)η 2 (T T ) + ϱ 2 2(1 + µ)η 2 (T \ T ) + Λ 12 δ 2 Recall η 2 (T T ) = η 2 (T ) η 2 (T \ T ) and rewrite η 2 ( T ) Λ 12 δ 2 (1 + λ)η 2 (T T ) + ϱ 2 2(1 + µ)η 2 (T \ T ) ( ) = (1 + λ)η 2 (T ) + ϱ 2 2(1 + µ) (1 + λ) η 2 (T \ T ) Since ϱ 2 2 (1 + µ) < 1 < 1 + λ, the factor in brackets is 0 and Dörfler marking with Θη 2 (T ) η 2 (T \ T ) leads to Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
8 η 2 ( T ) Λ 12 δ 2 ( ) (1 + λ)η 2 (T ) + ϱ 2 2(1 + µ) (1 + λ) η 2 (T \ T ) ( ) (1 + λ)(1 Θ) + Θϱ 2 2(1 + µ) η 2 (T ) }{{} ϱ 12 The proof concludes with ϱ 12 < 1 iff λ < Θ 1 (1+µ)ϱ2 2 1 Θ calculation) (by a minor NB. λ, µ small reduce ϱ 12 but increase Λ 12 Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
9 Repeat (A12) Abbreviate T := T l and T := T l+1 in (A1)-(A2) with η(k) := η l (K) for K T resp. η(t ) := η l+1 (T ) for T T and δ := δ(t, T ) =: δ l,l+1. Recall there exist 0 < µ < ϱ and 0 < λ < Θ 1 (1 + µ)ϱ2 2 1 Θ Theorem (A12) (A1)-(A2) and Dörfler marking imply ηl+1 2 ϱ 12 ηl 2 + Λ 12δl,l+1 2 with ϱ 12 < 1 and Λ 12 < for any such choice of λ, µ Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
10 Plain Convergence Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
11 Convergence η k 0 as k Theorem (plain convergence) (A12), (A4), and Λ := (1 + Λ 12 Λ 4 )/(1 ϱ 12 ) < imply ηk 2 Λη2 l for all l N 0. k=l Proof. Recall (A12) as η 2 k+1 ϱ 12η 2 k + Λ 12δ 2 k,k+1. Then l+m k=l l+m+1 ηk 2 k=l η 2 k η2 l + ϱ 12 l+m k=l η 2 k + Λ 12 l+m k=l Recall (A4) k=l δ2 k,k+1 Λ 4ηl 2 for the last term and utilize ϱ 12 < 1 to conclude the proof δ 2 k,k+1 Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
12 Linear Convergence Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
13 R-Linear Convergence Uniformly on Each Level Theorem (A12),(A4),Λ, and q := 1 1/Λ < 1 imply ηl+m 2 qm Λ ηl 2 for all l, m N 0. Proof. Plain convergence gives ξl 2 := ηk 2 Λ η2 l < k=l and so Λ 1 ξl 2 η2 l = ξ2 l ξ2 l+1 This proves ξl+1 2 qξ2 l (for each l N 0 ) Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
14 Recall ξ 2 l+1 qξ2 l for all l N 0 Mathematical induction leads to ξ 2 l+m qm ξ 2 l for all m N 0 This and ξ 2 l := k=l η2 k Λ η2 l show η 2 l+m ξ2 l+m qm ξ 2 l qm Λη 2 l R-linear convergence uniformly on each level implies via a geometric series l 1 k=0 η 1/s k η 1/s l Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
15 Quasimonotonicity Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
16 (QM) Estimator Quasimonotonicity Theorem (QM) (A1) (A3) and Λ mon := 1 + Λ Λ2 2 Λ 3 imply η( T ) Λ mon η(t ) for any refinement T of any T in T Proof. For any 0 < λ <, utilize (A1)-(A2) in the decomposition η 2 ( T ) = η 2 ( T T ) + η 2 ( T \T ) Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
17 η 2 ( T ) = η 2 ( T T ) + η 2 ( T \T ) ( (1 + λ) η 2 (T T ) + η 2 (T \ T ) ) }{{} η 2 (T ) + (1 + 1/λ)(Λ Λ 2 2)δ 2 (A3) reads δ 2 Λ 2 3 η2 (T ) and leads to η 2 ( T ) (1 + λ + (1 + 1/λ)(Λ Λ 2 2)Λ 2 3)η 2 (T ) }{{} Λ 2 mon Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
18 Comparison Lemma Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
19 Comparison Lemma Given 0 < κ < 1 and s > 0 with M := sup (N + 1) s min η(t ) < N N 0 T T(N) 0 < θ 0 < 1 l N 0 ˆT l T(T l ) s.t. (a) η( ˆT l ) κη(t l ) (b) κη l T l \ ˆT l s Λ mon M (c) θ 0 η 2 l η2 l (T l \ ˆT l ) Proof. (1) W.l.o.g. η l η(t l ) > 0. Then (QM) implies 0 < η 0 M Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
20 (2) Choose minimal N l N 0 s.t. (N l + 1) s κη l Λ mon M < N s l 1 (N l 1 because η l Λ 1 mon/m η 0 /M 1) (3) Set T l := T l T for T with T T(N l ) s.t. (N l + 1) s η(t ) M Quasimonotonicity and overlay control lead to (a), η( T l ) Λ mon M(N l + 1) s κη l and T l T l + N l Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
21 Proof of (b)-(c) in Comparison Lemma (4) Proof of (b). Count triangles to verify T l \ T l T l T l N l < κ 1/s η 1/s l Λ 1/s monm 1/s from from (2) (5) Any T l T(T l ) with (a) allows for (c). Given 0 < µ < κ 2 1, (A1) plus (a) and (A3) imply η 2 l (T l T l ) (1+µ)η 2 ( T l, T l T l ) +(1+1/µ)Λ 2 1δ 2 (T l, T l ) (1 + µ)κ 2 η 2 l + (1 + 1/µ)Λ2 1Λ 2 3η 2 l (T l\ T l ) This and η 2 l = η2 l (T l T l ) + η 2 l (T l\ T l ) lead to (1 (1 + µ)κ 2 ) η 2 l (1 + (1 + 1/µ)Λ2 1Λ 2 3) η 2 l (T l\ T l ) NB. Θ 0 is a quotient that depends onκ and µ. Fix those paramaters. Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
22 Repetition on Optimal Rates Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
23 Optimality Analysis at a Glance II R satisfies bulk criterion if θ A θ 0 thus M l R for optimal set M l of marked cells. AFEM utilizes almost minimal M l, whence M l M l R Set M := sup N N0 (1 + N) s min T T(N) η(t ) with (writing κ 1) R M 1/s η 1/s l Recall closure overhead control and combine with aforementioned estimates for l 1 l 1 T l T 0 M k M 1/s k=0 k=0 η 1/s k M 1/s η 1/s l Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
24 Separate Marking Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
25 Adaptive Algorithm: SAFEM Input: T 0, 0 < κ, θ A 1, ρ B < 1 l = 0, 1, 2, 3,... Compute η 2 l (K) and µ2 (K) for all K T l if µ 2 l := µ2 (T l ) κη 2 l T l+1 := Dörfler marking(θ A, T l, η 2 l ) else T l+1 := T l data approximation(ρ B µ 2 l, T 0, µ 2 l ) Output: Sequence (T l ), (η l ), (µ l ) abreviate σ 2 l := η2 l + µ2 l Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
26 Axioms (A1) (A4) Supposeρ 2 <1,Λ k < s.t. T T ˆT T (T ) R T s.t. T \ ˆT R R T \ ˆT η( ˆT, T ˆT ) η(t, T ˆT ) Λ 1 δ(t, ˆT ) (A1) η( ˆT, ˆT \ T ) ρ 2 η(t, T \ ˆT ) + Λ 2 δ(t, ˆT ) (A2) δ 2 (T, ˆT ) Λ 3 ( η 2 (T, R)+µ 2 (T ) ) + Λ 3 η 2 ( ˆT ) (A3) δ 2 (T k, T k+1 ) Λ 4 σl 2 for all l N 0 (A4) k=l Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
27 Axioms (B1) (B2) Tol > 0 T Tol = data approx(tol, T 0, µ 2 ) T satisfies µ 2 (T Tol ) Tol and T Tol T 0 Λ 5 Tol 1/(2s) (B1) T T, ˆT T(T ) µ 2 ( ˆT ) Λ 6 µ 2 (T ) (B2) (B1) (B2) follow for Approx from subadditivity µ 2 ( ˆT (M)) := µ 2 (T ) Λ 6 µ 2 (M) (SA) K M T ˆT (K) Typical example TSA by Binev and DeVore but also Dörfler marking over sufficient levels could do [C-Rabus 2016] Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
28 Theorem (C-Rabus 2016) SAFEM leads to optimal convergence rates in total estimators provided (A1)-(A4), (B1)-(B2), 0 < θ A < θ 0 := 1 κλ2 1 Λ Λ 2 1 Λ 3 and κ < 1 ρ A Λ 6 1 plus Quasimonotonicity (e.g. for (Λ Λ2 2 ) Λ 3 < 1) T T ˆT T (T ) σ( ˆT ) Λ 7 σ(t ). Applications to div-lsfem and to MFEM with convergence rates in H(div, Ω) L 2 (Ω) in [C-Rabus 2016] Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
29 Alternative Adaptive LS FEM 4 Laplace Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
30 Alternative A Posteriori Error Control Estimator η and data approximation error µ in 2D η 2 (T, K) := (1 Π 0 )p LS 2 L 2 (K) + K 1/2 ( ) [p LS ] E τ E 2 L 2 (E) + [ u LS/ ν E ] E 2 L 2 (E\ Ω) E E(K) µ 2 (K) := f Π 0 f 2 L 2 (K) for K T [C-Park 2015] satisfy discrete reliability (A3) (for k = 0) (Proof with explicit Crouzeix-Raviart and Raviart-Thomas functions, discrete Helmholtz decomposition, mixed intermediate solutions still leaves extra term) Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
31 References and Further Reading C, M. Feischl, M. Page, D. Praetorius, Axioms of adaptivity, Comput. Math. Appl., 67 (2014), pp C, H. Rabus. Axioms of adaptivity with separate marking for data resolution. SIAM J. Numer. Anal. 55(6) (2018) P. Bringmann, C, G. Starke: An adaptive least-squares FEM for linear elasticity with optimal conv rates, SIAM J. Numer. Anal. 56 (2018) P. Bringmann, C: h-adaptive least-squares FEMs for 2D Stokes eqns of any order with optimal conv rates, Comput. Math. Appl. 74 (2017) P. Bringmann, C: An adaptive least-squares FEM for Stokes eqns with optimal conv rates, Numer. Math. 135 (2017) C, E. J. Park, P. Bringmann: Convergence of natural adaptive least squares FEMs, Numer. Math. 136 (2017) C, E.-J. Park: Convergence and optimality of adaptive least squares FEMs, SIAM J. Numer. Anal. 53 (2015) Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
32 Prepare yourself for tomorrow Conforming P 1 FEM for Poisson Model Problem (weak form, H0 1(Ω), energy scalar product a(, ) := Ω dx, energy norm) Inverse estimates (for polynomials) Trace inequality (for Sobolev functions) Discrete trace inequality (for polynomials) Shape regularity (for triangles, simplices) Poincaré and Friedrichs inequality (for Sobolev functions) Equivalence of norms in finite dimensional vector spaces Scaling argument (for derivatives of Sobolev functions) Triangle inequality (in normed linear spaces) Cauchy inequality (in Hilbert spaces like L 2 or w.r.t. a(, )) C, F. Hellwig: Constants in Discrete Poincaré and Friedrichs Inequalities and Discrete Quasi-interpolation, CMAM (arxiv: ), Carsten Carstensen (HU Berlin) Axioms of Adaptivity Lecture 2 Shanghai / 32
Axioms of Adaptivity
Axioms of Adaptivity Carsten Carstensen Humboldt-Universität zu Berlin Open-Access Reference: C-Feischl-Page-Praetorius: Axioms of Adaptivity. Computer & Mathematics with Applications 67 (2014) 1195 1253
More informationAxioms of Adaptivity (AoA) in Lecture 1 (sufficient for optimal convergence rates)
Axioms of Adaptivity (AoA) in Lecture 1 (sufficient for optimal convergence rates) Carsten Carstensen Humboldt-Universität zu Berlin 2018 International Graduate Summer School on Frontiers of Applied and
More informationAxioms of Adaptivity (AoA) in Lecture 3 (sufficient for optimal convergence rates)
Axioms of Adaptivity (AoA) in Lecture 3 (sufficient for optimal convergence rates) Carsten Carstensen Humboldt-Universität zu Berlin 2018 International Graduate Summer School on Frontiers of Applied and
More informationNumerische Mathematik
Numer. Math. (2017) 136:1097 1115 DOI 10.1007/s00211-017-0866-x Numerische Mathematik Convergence of natural adaptive least squares finite element methods Carsten Carstensen 1 Eun-Jae Park 2 Philipp Bringmann
More informationFive Recent Trends in Computational PDEs
Five Recent Trends in Computational PDEs Carsten Carstensen Center Computational Science Adlershof and Department of Mathematics, Humboldt-Universität zu Berlin C. Carstensen (CCSA & HU Berlin) 5 Trends
More informationLecture Note III: Least-Squares Method
Lecture Note III: Least-Squares Method Zhiqiang Cai October 4, 004 In this chapter, we shall present least-squares methods for second-order scalar partial differential equations, elastic equations of solids,
More informationAdaptive approximation of eigenproblems: multiple eigenvalues and clusters
Adaptive approximation of eigenproblems: multiple eigenvalues and clusters Francesca Gardini Dipartimento di Matematica F. Casorati, Università di Pavia http://www-dimat.unipv.it/gardini Banff, July 1-6,
More informationWorkshop on CENTRAL Trends in PDEs Vienna, November 12-13, 2015
Workshop on CENTRAL Trends in PDEs Vienna, November 12-13, 2015 Venue: Sky Lounge, 12th floor, Faculty of Mathematics, Oskar-Morgenstern-Platz 1, Vienna Thursday, November 12, 2015 14:00-14:30 Registration
More informationGoal. Robust A Posteriori Error Estimates for Stabilized Finite Element Discretizations of Non-Stationary Convection-Diffusion Problems.
Robust A Posteriori Error Estimates for Stabilized Finite Element s of Non-Stationary Convection-Diffusion Problems L. Tobiska and R. Verfürth Universität Magdeburg Ruhr-Universität Bochum www.ruhr-uni-bochum.de/num
More informationTraces and Duality Lemma
Traces and Duality Lemma Recall the duality lemma with H / ( ) := γ 0 (H ()) defined as the trace space of H () endowed with minimal extension norm; i.e., for w H / ( ) L ( ), w H / ( ) = min{ ŵ H () ŵ
More informationENERGY NORM A POSTERIORI ERROR ESTIMATES FOR MIXED FINITE ELEMENT METHODS
ENERGY NORM A POSTERIORI ERROR ESTIMATES FOR MIXED FINITE ELEMENT METHODS CARLO LOVADINA AND ROLF STENBERG Abstract The paper deals with the a-posteriori error analysis of mixed finite element methods
More informationA posteriori error estimates for non conforming approximation of eigenvalue problems
A posteriori error estimates for non conforming approximation of eigenvalue problems E. Dari a, R. G. Durán b and C. Padra c, a Centro Atómico Bariloche, Comisión Nacional de Energía Atómica and CONICE,
More informationAn a posteriori error estimate and a Comparison Theorem for the nonconforming P 1 element
Calcolo manuscript No. (will be inserted by the editor) An a posteriori error estimate and a Comparison Theorem for the nonconforming P 1 element Dietrich Braess Faculty of Mathematics, Ruhr-University
More informationMULTIGRID PRECONDITIONING IN H(div) ON NON-CONVEX POLYGONS* Dedicated to Professor Jim Douglas, Jr. on the occasion of his seventieth birthday.
MULTIGRID PRECONDITIONING IN H(div) ON NON-CONVEX POLYGONS* DOUGLAS N ARNOLD, RICHARD S FALK, and RAGNAR WINTHER Dedicated to Professor Jim Douglas, Jr on the occasion of his seventieth birthday Abstract
More informationUnified A Posteriori Error Control for all Nonstandard Finite Elements 1
Unified A Posteriori Error Control for all Nonstandard Finite Elements 1 Martin Eigel C. Carstensen, C. Löbhard, R.H.W. Hoppe Humboldt-Universität zu Berlin 19.05.2010 1 we know of Guidelines for Applicants
More informationENERGY NORM A POSTERIORI ERROR ESTIMATES FOR MIXED FINITE ELEMENT METHODS
MATHEMATICS OF COMPUTATION Volume 75, Number 256, October 2006, Pages 1659 1674 S 0025-57180601872-2 Article electronically published on June 26, 2006 ENERGY NORM A POSTERIORI ERROR ESTIMATES FOR MIXED
More informationAdaptive Boundary Element Methods Part 1: Newest Vertex Bisection. Dirk Praetorius
CENTRAL School on Analysis and Numerics for PDEs November 09-12, 2015 Part 1: Newest Vertex Bisection Dirk Praetorius TU Wien Institute for Analysis and Scientific Computing Outline 1 Regular Triangulations
More informationAdaptive Boundary Element Methods Part 2: ABEM. Dirk Praetorius
CENTRAL School on Analysis and Numerics for PDEs November 09-12, 2015 Adaptive Boundary Element Methods Part 2: ABEM Dirk Praetorius TU Wien Institute for Analysis and Scientific Computing Outline 1 Boundary
More informationBasic Concepts of Adaptive Finite Element Methods for Elliptic Boundary Value Problems
Basic Concepts of Adaptive Finite lement Methods for lliptic Boundary Value Problems Ronald H.W. Hoppe 1,2 1 Department of Mathematics, University of Houston 2 Institute of Mathematics, University of Augsburg
More informationQUASI-OPTIMAL CONVERGENCE RATE OF AN ADAPTIVE DISCONTINUOUS GALERKIN METHOD
QUASI-OPIMAL CONVERGENCE RAE OF AN ADAPIVE DISCONINUOUS GALERKIN MEHOD ANDREA BONIO AND RICARDO H. NOCHEO Abstract. We analyze an adaptive discontinuous finite element method (ADFEM) for symmetric second
More informationarxiv: v1 [math.na] 19 Dec 2017
Arnold-Winther Mixed Finite Elements for Stokes Eigenvalue Problems Joscha Gedicke Arbaz Khan arxiv:72.0686v [math.na] 9 Dec 207 Abstract This paper is devoted to study the Arnold-Winther mixed finite
More informationAdaptive Finite Element Methods Lecture 1: A Posteriori Error Estimation
Adaptive Finite Element Methods Lecture 1: A Posteriori Error Estimation Department of Mathematics and Institute for Physical Science and Technology University of Maryland, USA www.math.umd.edu/ rhn 7th
More informationA Mixed Nonconforming Finite Element for Linear Elasticity
A Mixed Nonconforming Finite Element for Linear Elasticity Zhiqiang Cai, 1 Xiu Ye 2 1 Department of Mathematics, Purdue University, West Lafayette, Indiana 47907-1395 2 Department of Mathematics and Statistics,
More informationAMS subject classifications. Primary, 65N15, 65N30, 76D07; Secondary, 35B45, 35J50
A SIMPLE FINITE ELEMENT METHOD FOR THE STOKES EQUATIONS LIN MU AND XIU YE Abstract. The goal of this paper is to introduce a simple finite element method to solve the Stokes equations. This method is in
More informationDiscontinuous Petrov-Galerkin Methods
Discontinuous Petrov-Galerkin Methods Friederike Hellwig 1st CENTRAL School on Analysis and Numerics for Partial Differential Equations, November 12, 2015 Motivation discontinuous Petrov-Galerkin (dpg)
More informationEnergy norm a-posteriori error estimation for divergence-free discontinuous Galerkin approximations of the Navier-Stokes equations
INTRNATIONAL JOURNAL FOR NUMRICAL MTHODS IN FLUIDS Int. J. Numer. Meth. Fluids 19007; 1:1 [Version: 00/09/18 v1.01] nergy norm a-posteriori error estimation for divergence-free discontinuous Galerkin approximations
More informationRate optimal adaptive FEM with inexact solver for strongly monotone operators
ASC Report No. 19/2016 Rate optimal adaptive FEM with inexact solver for strongly monotone operators G. Gantner, A. Haberl, D. Praetorius, B. Stiftner Institute for Analysis and Scientific Computing Vienna
More informationNumerical Solutions to Partial Differential Equations
Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University Nonconformity and the Consistency Error First Strang Lemma Abstract Error Estimate
More informationb i (x) u + c(x)u = f in Ω,
SIAM J. NUMER. ANAL. Vol. 39, No. 6, pp. 1938 1953 c 2002 Society for Industrial and Applied Mathematics SUBOPTIMAL AND OPTIMAL CONVERGENCE IN MIXED FINITE ELEMENT METHODS ALAN DEMLOW Abstract. An elliptic
More informationMIXED FINITE ELEMENTS FOR PLATES. Ricardo G. Durán Universidad de Buenos Aires
MIXED FINITE ELEMENTS FOR PLATES Ricardo G. Durán Universidad de Buenos Aires - Necessity of 2D models. - Reissner-Mindlin Equations. - Finite Element Approximations. - Locking. - Mixed interpolation or
More informationOn an Approximation Result for Piecewise Polynomial Functions. O. Karakashian
BULLETIN OF THE GREE MATHEMATICAL SOCIETY Volume 57, 010 (1 7) On an Approximation Result for Piecewise Polynomial Functions O. arakashian Abstract We provide a new approach for proving approximation results
More informationConvergence and optimality of an adaptive FEM for controlling L 2 errors
Convergence and optimality of an adaptive FEM for controlling L 2 errors Alan Demlow (University of Kentucky) joint work with Rob Stevenson (University of Amsterdam) Partially supported by NSF DMS-0713770.
More informationc 2007 Society for Industrial and Applied Mathematics
SIAM J. NUMR. ANAL. Vol. 45, No. 1, pp. 68 82 c 2007 Society for Industrial and Applied Mathematics FRAMWORK FOR TH A POSTRIORI RROR ANALYSIS OF NONCONFORMING FINIT LMNTS CARSTN CARSTNSN, JUN HU, AND ANTONIO
More informationarxiv: v2 [math.na] 23 Apr 2016
Improved ZZ A Posteriori Error Estimators for Diffusion Problems: Conforming Linear Elements arxiv:508.009v2 [math.na] 23 Apr 206 Zhiqiang Cai Cuiyu He Shun Zhang May 2, 208 Abstract. In [8], we introduced
More informationLECTURE 1: SOURCES OF ERRORS MATHEMATICAL TOOLS A PRIORI ERROR ESTIMATES. Sergey Korotov,
LECTURE 1: SOURCES OF ERRORS MATHEMATICAL TOOLS A PRIORI ERROR ESTIMATES Sergey Korotov, Institute of Mathematics Helsinki University of Technology, Finland Academy of Finland 1 Main Problem in Mathematical
More informationNumerical Solutions to Partial Differential Equations
Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University The Residual and Error of Finite Element Solutions Mixed BVP of Poisson Equation
More informationChapter 5 A priori error estimates for nonconforming finite element approximations 5.1 Strang s first lemma
Chapter 5 A priori error estimates for nonconforming finite element approximations 51 Strang s first lemma We consider the variational equation (51 a(u, v = l(v, v V H 1 (Ω, and assume that the conditions
More informationarxiv: v1 [math.na] 27 Jan 2016
Virtual Element Method for fourth order problems: L 2 estimates Claudia Chinosi a, L. Donatella Marini b arxiv:1601.07484v1 [math.na] 27 Jan 2016 a Dipartimento di Scienze e Innovazione Tecnologica, Università
More informationNUMERICAL EXPERIMENTS FOR THE ARNOLD WINTHER MIXED FINITE ELEMENTS FOR THE STOKES PROBLEM
NUMERICAL EXPERIMENTS FOR THE ARNOLD WINTHER MIXED FINITE ELEMENTS FOR THE STOKES PROBLEM CARSTEN CARSTENSEN, JOSCHA GEDICKE, AND EUN-JAE PARK Abstract. The stress-velocity formulation of the stationary
More informationAn optimal adaptive finite element method. Rob Stevenson Korteweg-de Vries Institute for Mathematics Faculty of Science University of Amsterdam
An optimal adaptive finite element method Rob Stevenson Korteweg-de Vries Institute for Mathematics Faculty of Science University of Amsterdam Contents model problem + (A)FEM newest vertex bisection convergence
More informationAxioms of adaptivity. ASC Report No. 38/2013. C. Carstensen, M. Feischl, M. Page, D. Praetorius
ASC Report No. 38/2013 Axioms of adaptivity C. Carstensen, M. Feischl, M. Page, D. Praetorius Institute for Analysis and Scientific Computing Vienna University of Technology TU Wien www.asc.tuwien.ac.at
More informationIntroduction to finite element exterior calculus
Introduction to finite element exterior calculus Ragnar Winther CMA, University of Oslo Norway Why finite element exterior calculus? Recall the de Rham complex on the form: R H 1 (Ω) grad H(curl, Ω) curl
More informationLECTURE # 0 BASIC NOTATIONS AND CONCEPTS IN THE THEORY OF PARTIAL DIFFERENTIAL EQUATIONS (PDES)
LECTURE # 0 BASIC NOTATIONS AND CONCEPTS IN THE THEORY OF PARTIAL DIFFERENTIAL EQUATIONS (PDES) RAYTCHO LAZAROV 1 Notations and Basic Functional Spaces Scalar function in R d, d 1 will be denoted by u,
More informationNumerische Mathematik
Numer. Math. (2013) :425 459 DOI 10.1007/s00211-012-0494-4 Numerische Mathematik Effective postprocessing for equilibration a posteriori error estimators C. Carstensen C. Merdon Received: 22 June 2011
More informationA Multigrid Method for Two Dimensional Maxwell Interface Problems
A Multigrid Method for Two Dimensional Maxwell Interface Problems Susanne C. Brenner Department of Mathematics and Center for Computation & Technology Louisiana State University USA JSA 2013 Outline A
More informationSpline Element Method for Partial Differential Equations
for Partial Differential Equations Department of Mathematical Sciences Northern Illinois University 2009 Multivariate Splines Summer School, Summer 2009 Outline 1 Why multivariate splines for PDEs? Motivation
More informationSZEGÖ ASYMPTOTICS OF EXTREMAL POLYNOMIALS ON THE SEGMENT [ 1, +1]: THE CASE OF A MEASURE WITH FINITE DISCRETE PART
Georgian Mathematical Journal Volume 4 (27), Number 4, 673 68 SZEGÖ ASYMPOICS OF EXREMAL POLYNOMIALS ON HE SEGMEN [, +]: HE CASE OF A MEASURE WIH FINIE DISCREE PAR RABAH KHALDI Abstract. he strong asymptotics
More informationError estimates for the Raviart-Thomas interpolation under the maximum angle condition
Error estimates for the Raviart-Thomas interpolation under the maximum angle condition Ricardo G. Durán and Ariel L. Lombardi Abstract. The classical error analysis for the Raviart-Thomas interpolation
More informationA Posteriori Error Estimation Techniques for Finite Element Methods. Zhiqiang Cai Purdue University
A Posteriori Error Estimation Techniques for Finite Element Methods Zhiqiang Cai Purdue University Department of Mathematics, Purdue University Slide 1, March 16, 2017 Books Ainsworth & Oden, A posteriori
More informationMedius analysis and comparison results for first-order finite element methods in linear elasticity
IMA Journal of Numerical Analysis Advance Access published November 7, 2014 IMA Journal of Numerical Analysis (2014) Page 1 of 31 doi:10.1093/imanum/dru048 Medius analysis and comparison results for first-order
More informationBUBBLE STABILIZED DISCONTINUOUS GALERKIN METHOD FOR STOKES PROBLEM
BUBBLE STABILIZED DISCONTINUOUS GALERKIN METHOD FOR STOKES PROBLEM ERIK BURMAN AND BENJAMIN STAMM Abstract. We propose a low order discontinuous Galerkin method for incompressible flows. Stability of the
More informationOn the p-laplacian and p-fluids
LMU Munich, Germany Lars Diening On the p-laplacian and p-fluids Lars Diening On the p-laplacian and p-fluids 1/50 p-laplacian Part I p-laplace and basic properties Lars Diening On the p-laplacian and
More informationAN EQUILIBRATED A POSTERIORI ERROR ESTIMATOR FOR THE INTERIOR PENALTY DISCONTINUOUS GALERKIN METHOD
AN EQUILIBRATED A POSTERIORI ERROR ESTIMATOR FOR THE INTERIOR PENALTY DISCONTINUOUS GALERIN METHOD D. BRAESS, T. FRAUNHOLZ, AND R. H. W. HOPPE Abstract. Interior Penalty Discontinuous Galerkin (IPDG) methods
More informationA Least-Squares Finite Element Approximation for the Compressible Stokes Equations
A Least-Squares Finite Element Approximation for the Compressible Stokes Equations Zhiqiang Cai, 1 Xiu Ye 1 Department of Mathematics, Purdue University, 1395 Mathematical Science Building, West Lafayette,
More informationStability of an abstract wave equation with delay and a Kelvin Voigt damping
Stability of an abstract wave equation with delay and a Kelvin Voigt damping University of Monastir/UPSAY/LMV-UVSQ Joint work with Serge Nicaise and Cristina Pignotti Outline 1 Problem The idea Stability
More informationNumerische Mathematik
Numer. Math. 2015 130:395 423 DOI 10.1007/s00211-014-0672-7 Numerische Mathematik Weakly over-penalized discontinuous Galerkin schemes for Reissner Mindlin plates without the shear variable Paulo Rafael
More informationA posteriori error estimates applied to flow in a channel with corners
Mathematics and Computers in Simulation 61 (2003) 375 383 A posteriori error estimates applied to flow in a channel with corners Pavel Burda a,, Jaroslav Novotný b, Bedřich Sousedík a a Department of Mathematics,
More informationETNA Kent State University
Electronic Transactions on Numerical Analysis. Volume 37, pp. 166-172, 2010. Copyright 2010,. ISSN 1068-9613. ETNA A GRADIENT RECOVERY OPERATOR BASED ON AN OBLIQUE PROJECTION BISHNU P. LAMICHHANE Abstract.
More informationELLIPTIC RECONSTRUCTION AND A POSTERIORI ERROR ESTIMATES FOR PARABOLIC PROBLEMS
ELLIPTIC RECONSTRUCTION AND A POSTERIORI ERROR ESTIMATES FOR PARABOLIC PROBLEMS CHARALAMBOS MAKRIDAKIS AND RICARDO H. NOCHETTO Abstract. It is known that the energy technique for a posteriori error analysis
More informationInstitut für Mathematik
U n i v e r s i t ä t A u g s b u r g Institut für Mathematik Dietrich Braess, Carsten Carstensen, and Ronald H.W. Hoppe Convergence Analysis of a Conforming Adaptive Finite Element Method for an Obstacle
More informationFinite Element Methods for Maxwell Equations
CHAPTER 8 Finite Element Methods for Maxwell Equations The Maxwell equations comprise four first-order partial differential equations linking the fundamental electromagnetic quantities, the electric field
More informationFind (u,p;λ), with u 0 and λ R, such that u + p = λu in Ω, (2.1) div u = 0 in Ω, u = 0 on Γ.
A POSTERIORI ESTIMATES FOR THE STOKES EIGENVALUE PROBLEM CARLO LOVADINA, MIKKO LYLY, AND ROLF STENBERG Abstract. We consider the Stokes eigenvalue problem. For the eigenvalues we derive both upper and
More informationMIXED FINITE ELEMENT METHODS FOR PROBLEMS WITH ROBIN BOUNDARY CONDITIONS
MIXED FINITE ELEMENT METHODS FOR PROBLEMS WITH ROBIN BOUNDARY CONDITIONS JUHO KÖNNÖ, DOMINIK SCHÖTZAU, AND ROLF STENBERG Abstract. We derive new a-priori and a-posteriori error estimates for mixed nite
More informationThe Dirichlet s P rinciple. In this lecture we discuss an alternative formulation of the Dirichlet problem for the Laplace equation:
Oct. 1 The Dirichlet s P rinciple In this lecture we discuss an alternative formulation of the Dirichlet problem for the Laplace equation: 1. Dirichlet s Principle. u = in, u = g on. ( 1 ) If we multiply
More informationA NOTE ON THE LADYŽENSKAJA-BABUŠKA-BREZZI CONDITION
A NOTE ON THE LADYŽENSKAJA-BABUŠKA-BREZZI CONDITION JOHNNY GUZMÁN, ABNER J. SALGADO, AND FRANCISCO-JAVIER SAYAS Abstract. The analysis of finite-element-like Galerkin discretization techniques for the
More informationMath 328 Course Notes
Math 328 Course Notes Ian Robertson March 3, 2006 3 Properties of C[0, 1]: Sup-norm and Completeness In this chapter we are going to examine the vector space of all continuous functions defined on the
More informationAposteriorierrorestimatesinFEEC for the de Rham complex
AposteriorierrorestimatesinFEEC for the de Rham complex Alan Demlow Texas A&M University joint work with Anil Hirani University of Illinois Urbana-Champaign Partially supported by NSF DMS-1016094 and a
More informationA Posteriori Error Estimates for Weak Galerkin Finite Element Methods for Second Order Elliptic Problems
DOI 10.1007/s10915-013-9771-3 A Posteriori Error Estimates for Weak Galerkin Finite Element Methods for Second Order Elliptic Problems Long Chen Junping Wang Xiu Ye Received: 29 January 2013 / Revised:
More informationNumerical Solutions to Partial Differential Equations
Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University Sobolev Embedding Theorems Embedding Operators and the Sobolev Embedding Theorem
More informationA posteriori error estimates in FEEC for the de Rham complex
A posteriori error estimates in FEEC for the de Rham complex Alan Demlow Texas A&M University joint work with Anil Hirani University of Illinois Urbana-Champaign Partially supported by NSF DMS-1016094
More informationSolutions of Selected Problems
1 Solutions of Selected Problems October 16, 2015 Chapter I 1.9 Consider the potential equation in the disk := {(x, y) R 2 ; x 2 +y 2 < 1}, with the boundary condition u(x) = g(x) r for x on the derivative
More informationPARTITION OF UNITY FOR THE STOKES PROBLEM ON NONMATCHING GRIDS
PARTITION OF UNITY FOR THE STOES PROBLEM ON NONMATCHING GRIDS CONSTANTIN BACUTA AND JINCHAO XU Abstract. We consider the Stokes Problem on a plane polygonal domain Ω R 2. We propose a finite element method
More informationON SINGULAR PERTURBATION OF THE STOKES PROBLEM
NUMERICAL ANALYSIS AND MATHEMATICAL MODELLING BANACH CENTER PUBLICATIONS, VOLUME 9 INSTITUTE OF MATHEMATICS POLISH ACADEMY OF SCIENCES WARSZAWA 994 ON SINGULAR PERTURBATION OF THE STOKES PROBLEM G. M.
More informationRecovery-Based a Posteriori Error Estimators for Interface Problems: Mixed and Nonconforming Elements
Recovery-Based a Posteriori Error Estimators for Interface Problems: Mixed and Nonconforming Elements Zhiqiang Cai Shun Zhang Department of Mathematics Purdue University Finite Element Circus, Fall 2008,
More informationSupraconvergence of a Non-Uniform Discretisation for an Elliptic Third-Kind Boundary-Value Problem with Mixed Derivatives
Supraconvergence of a Non-Uniform Discretisation for an Elliptic Third-Kind Boundary-Value Problem with Mixed Derivatives Etienne Emmrich Technische Universität Berlin, Institut für Mathematik, Straße
More informationBesov regularity for operator equations on patchwise smooth manifolds
on patchwise smooth manifolds Markus Weimar Philipps-University Marburg Joint work with Stephan Dahlke (PU Marburg) Mecklenburger Workshop Approximationsmethoden und schnelle Algorithmen Hasenwinkel, March
More informationMultigrid Methods for Elliptic Obstacle Problems on 2D Bisection Grids
Multigrid Methods for Elliptic Obstacle Problems on 2D Bisection Grids Long Chen 1, Ricardo H. Nochetto 2, and Chen-Song Zhang 3 1 Department of Mathematics, University of California at Irvine. chenlong@math.uci.edu
More informationDISCRETE EXTENSION OPERATORS FOR MIXED FINITE ELEMENT SPACES ON LOCALLY REFINED MESHES
DISCRETE EXTENSION OPERATORS FOR MIXED FINITE ELEMENT SPACES ON LOCALLY REFINED MESHES MAR AINSWORTH, JOHNNY GUZMÁN, AND FRANCISCO JAVIER SAYAS Abstract. The existence of uniformly bounded discrete extension
More informationSymmetry-Free, p-robust Equilibrated Error Indication for the hp-version of the FEM in Nearly Incompressible Linear Elasticity
Computational Methods in Applied Mathematics Vol. 13 (2013), No. 3, pp. 291 304 c 2013 Institute of Mathematics, NAS of Belarus Doi: 10.1515/cmam-2013-0007 Symmetry-Free, p-robust Equilibrated Error Indication
More informationPREPRINT 2010:23. A nonconforming rotated Q 1 approximation on tetrahedra PETER HANSBO
PREPRINT 2010:23 A nonconforming rotated Q 1 approximation on tetrahedra PETER HANSBO Department of Mathematical Sciences Division of Mathematics CHALMERS UNIVERSITY OF TECHNOLOGY UNIVERSITY OF GOTHENBURG
More informationGuaranteed Velocity Error Control for the Pseudostress Approximation of the Stokes Equations
Guaranteed Velocity Error Control for the Pseudostress Approximation of the Stokes Equations P. Bringmann, 1 C. Carstensen, 1 C. Merdon 2 1 Department of Mathematics, Humboldt-Universität zu Berlin, Unter
More informationSECOND-ORDER FULLY DISCRETIZED PROJECTION METHOD FOR INCOMPRESSIBLE NAVIER-STOKES EQUATIONS
Tenth MSU Conference on Differential Equations and Computational Simulations. Electronic Journal of Differential Equations, Conference 3 (06), pp. 9 0. ISSN: 07-669. URL: http://ejde.math.txstate.edu or
More informationA u + b u + cu = f in Ω, (1.1)
A WEIGHTED H(div) LEAST-SQUARES METHOD FOR SECOND-ORDER ELLIPTIC PROBLEMS Z. CAI AND C. R. WESTPHAL Abstract. This paper presents analysis of a weighted-norm least squares finite element method for elliptic
More informationMath 497 R1 Winter 2018 Navier-Stokes Regularity
Math 497 R Winter 208 Navier-Stokes Regularity Lecture : Sobolev Spaces and Newtonian Potentials Xinwei Yu Jan. 0, 208 Based on..2 of []. Some ne properties of Sobolev spaces, and basics of Newtonian potentials.
More informationAn a posteriori error estimator for the weak Galerkin least-squares finite-element method
An a posteriori error estimator for the weak Galerkin least-squares finite-element method James H. Adler a, Xiaozhe Hu a, Lin Mu b, Xiu Ye c a Department of Mathematics, Tufts University, Medford, MA 02155
More informationR T (u H )v + (2.1) J S (u H )v v V, T (2.2) (2.3) H S J S (u H ) 2 L 2 (S). S T
2 R.H. NOCHETTO 2. Lecture 2. Adaptivity I: Design and Convergence of AFEM tarting with a conforming mesh T H, the adaptive procedure AFEM consists of loops of the form OLVE ETIMATE MARK REFINE to produce
More informationExistence and uniqueness of the weak solution for a contact problem
Available online at www.tjnsa.com J. Nonlinear Sci. Appl. 9 (216), 186 199 Research Article Existence and uniqueness of the weak solution for a contact problem Amar Megrous a, Ammar Derbazi b, Mohamed
More informationOn Friedrichs inequality, Helmholtz decomposition, vector potentials, and the div-curl lemma. Ben Schweizer 1
On Friedrichs inequality, Helmholtz decomposition, vector potentials, and the div-curl lemma Ben Schweizer 1 January 16, 2017 Abstract: We study connections between four different types of results that
More informationA NONCONFORMING PENALTY METHOD FOR A TWO DIMENSIONAL CURL-CURL PROBLEM
A NONCONFORMING PENALTY METHOD FOR A TWO DIMENSIONAL CURL-CURL PROBLEM SUSANNE C. BRENNER, FENGYAN LI, AND LI-YENG SUNG Abstract. A nonconforming penalty method for a two-dimensional curl-curl problem
More informationIMPLEMENTATION OF FUNCTIONAL-TYPE A POSTERIORI ERROR ESTIMATES FOR LINEAR PROBLEMS IN SOLID MECHANICS. Maksim Frolov
IMPLEMENTATION OF FUNCTIONAL-TYPE A POSTERIORI ERROR ESTIMATES FOR LINEAR PROBLEMS IN SOLID MECHANICS Maksim Frolov Peter the Great St.Petersburg Polytechnic University AANMPDE11, FINLAND 06 10 August
More informationA Locking-Free MHM Method for Elasticity
Trabalho apresentado no CNMAC, Gramado - RS, 2016. Proceeding Series of the Brazilian Society of Computational and Applied Mathematics A Locking-Free MHM Method for Elasticity Weslley S. Pereira 1 Frédéric
More informationMAT 771 FUNCTIONAL ANALYSIS HOMEWORK 3. (1) Let V be the vector space of all bounded or unbounded sequences of complex numbers.
MAT 771 FUNCTIONAL ANALYSIS HOMEWORK 3 (1) Let V be the vector space of all bounded or unbounded sequences of complex numbers. (a) Define d : V V + {0} by d(x, y) = 1 ξ j η j 2 j 1 + ξ j η j. Show that
More informationA Posteriori Existence in Adaptive Computations
Report no. 06/11 A Posteriori Existence in Adaptive Computations Christoph Ortner This short note demonstrates that it is not necessary to assume the existence of exact solutions in an a posteriori error
More informationMIXED FINITE ELEMENT APPROXIMATION OF THE VECTOR LAPLACIAN WITH DIRICHLET BOUNDARY CONDITIONS
MIXED FINITE ELEMENT APPROXIMATION OF THE VECTOR LAPLACIAN WITH DIRICHLET BOUNDARY CONDITIONS DOUGLAS N. ARNOLD, RICHARD S. FALK, AND JAY GOPALAKRISHNAN Abstract. We consider the finite element solution
More informationA UNIFYING THEORY OF A POSTERIORI FINITE ELEMENT ERROR CONTROL
A UNIFYING THEORY OF A POSTERIORI FINITE ELEMENT ERROR CONTROL C. CARSTENSEN Abstract. Residual-based a posteriori error estimates are derived within a unified setting for lowest-order conforming, nonconforming,
More informationWeierstraß-Institut. für Angewandte Analysis und Stochastik. Leibniz-Institut im Forschungsverbund Berlin e. V. Preprint ISSN
Weierstraß-Institut für Angewandte Analysis und Stochastik Leibniz-Institut im Forschungsverbund Berlin e. V. Preprint ISSN 2198-5855 On the divergence constraint in mixed finite element methods for incompressible
More informationMath 209B Homework 2
Math 29B Homework 2 Edward Burkard Note: All vector spaces are over the field F = R or C 4.6. Two Compactness Theorems. 4. Point Set Topology Exercise 6 The product of countably many sequentally compact
More informationChapter 6 A posteriori error estimates for finite element approximations 6.1 Introduction
Chapter 6 A posteriori error estimates for finite element approximations 6.1 Introduction The a posteriori error estimation of finite element approximations of elliptic boundary value problems has reached
More informationSTOKES PROBLEM WITH SEVERAL TYPES OF BOUNDARY CONDITIONS IN AN EXTERIOR DOMAIN
Electronic Journal of Differential Equations, Vol. 2013 2013, No. 196, pp. 1 28. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu ftp ejde.math.txstate.edu STOKES PROBLEM
More informationA Domain Decomposition Method for Quasilinear Elliptic PDEs Using Mortar Finite Elements
W I S S E N T E C H N I K L E I D E N S C H A F T A Domain Decomposition Method for Quasilinear Elliptic PDEs Using Mortar Finite Elements Matthias Gsell and Olaf Steinbach Institute of Computational Mathematics
More information