Guaranteed and robust discontinuous Galerkin a posteriori error - - PowerPoint PPT Presentation

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Guaranteed and robust discontinuous Galerkin a posteriori error - - PowerPoint PPT Presentation

Guaranteed and robust discontinuous Galerkin a posteriori error estimates for convectiondiffusionreaction problems . Stephansen 2 & Martin Vohralk 3 Alexandre Ern 1 , Annette F 1 CERMICS Universit Paris-Est (Ecole des Ponts) 2


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SLIDE 1

Guaranteed and robust discontinuous Galerkin a posteriori error estimates for convection–diffusion–reaction problems

Alexandre Ern1, Annette F . Stephansen2 & Martin Vohralík3

1CERMICS

Université Paris-Est (Ecole des Ponts)

2Centre for Integrated Petroleum Research

Bergen, Norway

3Laboratoire Jacques-Louis Lions

Université Pierre et Marie Curie (Paris 6)

Paris, January 22, 2009

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SLIDE 2

I Abstract framework A posteriori estimates C

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 3

I Abstract framework A posteriori estimates C

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 4

I Abstract framework A posteriori estimates C

What is an a posteriori error estimate

A posteriori error estimate Let u be a weak solution of a PDE. Let uh be its approximate numerical solution. A priori error estimate: u − uhΩ ≤ f(u)hq. Dependent on u, not computable. Useful in theory. A posteriori error estimate: u − uhΩ f(uh). Only uses uh, computable. Great in practice. Usual form f(uh)2 =

T∈Th ηT(uh)2, where ηT(uh) is an element

indicator. Can be used to determine mesh elements with large error. We can then refine these elements: mesh adaptivity.

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 5

I Abstract framework A posteriori estimates C

What is an a posteriori error estimate

A posteriori error estimate Let u be a weak solution of a PDE. Let uh be its approximate numerical solution. A priori error estimate: u − uhΩ ≤ f(u)hq. Dependent on u, not computable. Useful in theory. A posteriori error estimate: u − uhΩ f(uh). Only uses uh, computable. Great in practice. Usual form f(uh)2 =

T∈Th ηT(uh)2, where ηT(uh) is an element

indicator. Can be used to determine mesh elements with large error. We can then refine these elements: mesh adaptivity.

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 6

I Abstract framework A posteriori estimates C

Example of an a posteriori error estimator

2 4 6 8 10 12 14 16 18 x 10

−3

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

Estimated error distribution

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 7

I Abstract framework A posteriori estimates C

What an a posteriori error estimate should fulfill

Guaranteed upper bound (global error upper bound) u − uh2

Ω ≤ T∈Th ηT(uh)2

no undetermined constant: error control remark (reliability): u − uh2

Ω ≤ C T∈Th ηT(uh)2

Local efficiency (local error lower bound) ηT(uh)2 ≤ C2

eff,T

  • T ′ close to T u − uh2

T ′

necessary for optimal mesh refinement Asymptotic exactness

  • T∈Th ηT(uh)2/u − uh2

Ω → 1

  • verestimation factor goes to one with mesh size

Robustness Ceff,T does not depend on data, mesh, or solution Negligible evaluation cost estimators can be evaluated locally

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 8

I Abstract framework A posteriori estimates C

What an a posteriori error estimate should fulfill

Guaranteed upper bound (global error upper bound) u − uh2

Ω ≤ T∈Th ηT(uh)2

no undetermined constant: error control remark (reliability): u − uh2

Ω ≤ C T∈Th ηT(uh)2

Local efficiency (local error lower bound) ηT(uh)2 ≤ C2

eff,T

  • T ′ close to T u − uh2

T ′

necessary for optimal mesh refinement Asymptotic exactness

  • T∈Th ηT(uh)2/u − uh2

Ω → 1

  • verestimation factor goes to one with mesh size

Robustness Ceff,T does not depend on data, mesh, or solution Negligible evaluation cost estimators can be evaluated locally

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-9
SLIDE 9

I Abstract framework A posteriori estimates C

What an a posteriori error estimate should fulfill

Guaranteed upper bound (global error upper bound) u − uh2

Ω ≤ T∈Th ηT(uh)2

no undetermined constant: error control remark (reliability): u − uh2

Ω ≤ C T∈Th ηT(uh)2

Local efficiency (local error lower bound) ηT(uh)2 ≤ C2

eff,T

  • T ′ close to T u − uh2

T ′

necessary for optimal mesh refinement Asymptotic exactness

  • T∈Th ηT(uh)2/u − uh2

Ω → 1

  • verestimation factor goes to one with mesh size

Robustness Ceff,T does not depend on data, mesh, or solution Negligible evaluation cost estimators can be evaluated locally

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 10

I Abstract framework A posteriori estimates C

What an a posteriori error estimate should fulfill

Guaranteed upper bound (global error upper bound) u − uh2

Ω ≤ T∈Th ηT(uh)2

no undetermined constant: error control remark (reliability): u − uh2

Ω ≤ C T∈Th ηT(uh)2

Local efficiency (local error lower bound) ηT(uh)2 ≤ C2

eff,T

  • T ′ close to T u − uh2

T ′

necessary for optimal mesh refinement Asymptotic exactness

  • T∈Th ηT(uh)2/u − uh2

Ω → 1

  • verestimation factor goes to one with mesh size

Robustness Ceff,T does not depend on data, mesh, or solution Negligible evaluation cost estimators can be evaluated locally

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 11

I Abstract framework A posteriori estimates C

What an a posteriori error estimate should fulfill

Guaranteed upper bound (global error upper bound) u − uh2

Ω ≤ T∈Th ηT(uh)2

no undetermined constant: error control remark (reliability): u − uh2

Ω ≤ C T∈Th ηT(uh)2

Local efficiency (local error lower bound) ηT(uh)2 ≤ C2

eff,T

  • T ′ close to T u − uh2

T ′

necessary for optimal mesh refinement Asymptotic exactness

  • T∈Th ηT(uh)2/u − uh2

Ω → 1

  • verestimation factor goes to one with mesh size

Robustness Ceff,T does not depend on data, mesh, or solution Negligible evaluation cost estimators can be evaluated locally

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-12
SLIDE 12

I Abstract framework A posteriori estimates C

What an a posteriori error estimate should fulfill

Guaranteed upper bound (global error upper bound) u − uh2

Ω ≤ T∈Th ηT(uh)2

no undetermined constant: error control remark (reliability): u − uh2

Ω ≤ C T∈Th ηT(uh)2

Local efficiency (local error lower bound) ηT(uh)2 ≤ C2

eff,T

  • T ′ close to T u − uh2

T ′

necessary for optimal mesh refinement Asymptotic exactness

  • T∈Th ηT(uh)2/u − uh2

Ω → 1

  • verestimation factor goes to one with mesh size

Robustness Ceff,T does not depend on data, mesh, or solution Negligible evaluation cost estimators can be evaluated locally

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 13

I Abstract framework A posteriori estimates C

Previous results on a posteriori error estimation in DG

DG, pure diffusion case Karakashian and Pascal (2003), Becker, Hansbo, and Larson (2003), residual-based estimates Rivière and Wheeler (2003), L2-estimates Ainsworth (2007), reconstruction of side fluxes Kim (2007), Cochez-Dhondt and Nicaise (2008), Lazarov, Repin, and Tomar (numerical experiments, 2008), our works, reconstruction of equilibrated H(div, Ω)-conforming fluxes DG, convection–diffusion–reaction case Sun and Wheeler (2006), L2-estimates Schötzau and Zhu (2008, preprint), res.-based estimates

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 14

I Abstract framework A posteriori estimates C

Previous results on a posteriori error estimation in DG

DG, pure diffusion case Karakashian and Pascal (2003), Becker, Hansbo, and Larson (2003), residual-based estimates Rivière and Wheeler (2003), L2-estimates Ainsworth (2007), reconstruction of side fluxes Kim (2007), Cochez-Dhondt and Nicaise (2008), Lazarov, Repin, and Tomar (numerical experiments, 2008), our works, reconstruction of equilibrated H(div, Ω)-conforming fluxes DG, convection–diffusion–reaction case Sun and Wheeler (2006), L2-estimates Schötzau and Zhu (2008, preprint), res.-based estimates

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 15

I Abstract framework A posteriori estimates C

Previous results

Equilibrated fluxes estimates Prager and Synge (1947) Ladevèze and Leguillon (1983) Repin (1997) Destuynder and Métivet (1999) Luce and Wohlmuth (2004) Convection–diffusion problems Verfürth (1998, 2005), conforming finite elements Sangalli (2008), conforming finite elements

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 16

I Abstract framework A posteriori estimates C

Previous results

Equilibrated fluxes estimates Prager and Synge (1947) Ladevèze and Leguillon (1983) Repin (1997) Destuynder and Métivet (1999) Luce and Wohlmuth (2004) Convection–diffusion problems Verfürth (1998, 2005), conforming finite elements Sangalli (2008), conforming finite elements

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 17

I Abstract framework A posteriori estimates C

Motivations and key points

Motivations establish an optimal abstract framework for a posteriori error estimation in potential- and flux-nonconforming methods derive estimates for DG satisfying as many as possible of the five optimal properties Key points focus on inhomogeneous and anisotropic diffusion case of nonmatching meshes singular regimes of dominant convection or reaction

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 18

I Abstract framework A posteriori estimates C

Motivations and key points

Motivations establish an optimal abstract framework for a posteriori error estimation in potential- and flux-nonconforming methods derive estimates for DG satisfying as many as possible of the five optimal properties Key points focus on inhomogeneous and anisotropic diffusion case of nonmatching meshes singular regimes of dominant convection or reaction

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 19

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 20

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A model convection–diffusion–reaction problem

A model convection–diffusion–reaction problem −∇·(K∇u) + β·∇u + µu = f in Ω, u =

  • n ∂Ω

Bilinear form B(u, v) := (K∇u, ∇v) + (β·∇u, v) + (µu, v), u, v ∈ H1(Th) Weak solution Find u ∈ H1

0(Ω) such that B(u, v) = (f, v)

∀v ∈ H1

0(Ω).

Energy norm Decompose B into B = BS + BA, where BS(u, v) := (K∇u, ∇v) +

  • µ − 1

2∇·β

  • u, v
  • ,

BA(u, v) :=

  • β·∇u + 1

2(∇·β)u, v

  • .

BS is symmetric on H1(Th); put |||v|||2 := BS(v, v) BA is skew-symmetric on H1

0(Ω)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-21
SLIDE 21

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A model convection–diffusion–reaction problem

A model convection–diffusion–reaction problem −∇·(K∇u) + β·∇u + µu = f in Ω, u =

  • n ∂Ω

Bilinear form B(u, v) := (K∇u, ∇v) + (β·∇u, v) + (µu, v), u, v ∈ H1(Th) Weak solution Find u ∈ H1

0(Ω) such that B(u, v) = (f, v)

∀v ∈ H1

0(Ω).

Energy norm Decompose B into B = BS + BA, where BS(u, v) := (K∇u, ∇v) +

  • µ − 1

2∇·β

  • u, v
  • ,

BA(u, v) :=

  • β·∇u + 1

2(∇·β)u, v

  • .

BS is symmetric on H1(Th); put |||v|||2 := BS(v, v) BA is skew-symmetric on H1

0(Ω)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-22
SLIDE 22

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A model convection–diffusion–reaction problem

A model convection–diffusion–reaction problem −∇·(K∇u) + β·∇u + µu = f in Ω, u =

  • n ∂Ω

Bilinear form B(u, v) := (K∇u, ∇v) + (β·∇u, v) + (µu, v), u, v ∈ H1(Th) Weak solution Find u ∈ H1

0(Ω) such that B(u, v) = (f, v)

∀v ∈ H1

0(Ω).

Energy norm Decompose B into B = BS + BA, where BS(u, v) := (K∇u, ∇v) +

  • µ − 1

2∇·β

  • u, v
  • ,

BA(u, v) :=

  • β·∇u + 1

2(∇·β)u, v

  • .

BS is symmetric on H1(Th); put |||v|||2 := BS(v, v) BA is skew-symmetric on H1

0(Ω)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-23
SLIDE 23

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A model convection–diffusion–reaction problem

A model convection–diffusion–reaction problem −∇·(K∇u) + β·∇u + µu = f in Ω, u =

  • n ∂Ω

Bilinear form B(u, v) := (K∇u, ∇v) + (β·∇u, v) + (µu, v), u, v ∈ H1(Th) Weak solution Find u ∈ H1

0(Ω) such that B(u, v) = (f, v)

∀v ∈ H1

0(Ω).

Energy norm Decompose B into B = BS + BA, where BS(u, v) := (K∇u, ∇v) +

  • µ − 1

2∇·β

  • u, v
  • ,

BA(u, v) :=

  • β·∇u + 1

2(∇·β)u, v

  • .

BS is symmetric on H1(Th); put |||v|||2 := BS(v, v) BA is skew-symmetric on H1

0(Ω)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-24
SLIDE 24

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Properties of the weak solution

0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.0 1.8 1.6 1.4 1.2 1.0 0.8 0.6 0.4 0.2 0.0

  • 0.2

1.0 exact solution

Solution u is in H1

0(Ω)

0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.0 1.5 1.0 0.5 0.0

  • 0.5
  • 1.0
  • 1.5

1.0

  • exact flux

Flux −K∇u is in H(div, Ω)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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SLIDE 25

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-26
SLIDE 26

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Optimal abstract estimate in the energy norm

Theorem (Optimal abstract estimate, energy norm (Vohralík ’07, Ern & Stephansen ’08)) Let u be the weak sol. and let uh ∈ H1(Th) be arbitrary. Then |||u − uh||| ≤ inf

s∈H1

0(Ω)

  • |||uh − s|||

+ inf

t∈H(div,Ω)

sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f − ∇·t − β·∇s − µs, ϕ)

−(K∇uh + t, ∇ϕ) +

  • µ − 1

2∇·β

  • (s − uh), ϕ
  • ≤ 2|||u − uh|||.

Properties Guaranteed upper bound, quasi-exact, and robust. Holds uniformly for any mesh (anis.) and pol. degree. Not computable (infimum over an infinite-dim. space).

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-27
SLIDE 27

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Optimal abstract estimate in the energy norm

Theorem (Optimal abstract estimate, energy norm (Vohralík ’07, Ern & Stephansen ’08)) Let u be the weak sol. and let uh ∈ H1(Th) be arbitrary. Then |||u − uh||| ≤ inf

s∈H1

0(Ω)

  • |||uh − s|||

+ inf

t∈H(div,Ω)

sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f − ∇·t − β·∇s − µs, ϕ)

−(K∇uh + t, ∇ϕ) +

  • µ − 1

2∇·β

  • (s − uh), ϕ
  • ≤ 2|||u − uh|||.

Properties Guaranteed upper bound, quasi-exact, and robust. Holds uniformly for any mesh (anis.) and pol. degree. Not computable (infimum over an infinite-dim. space).

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-28
SLIDE 28

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Optimal abstract estimate in the energy norm

Theorem (Optimal abstract estimate, energy norm (Vohralík ’07, Ern & Stephansen ’08)) Let u be the weak sol. and let uh ∈ H1(Th) be arbitrary. Then |||u − uh||| ≤ inf

s∈H1

0(Ω)

  • |||uh − s|||

+ inf

t∈H(div,Ω)

sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f − ∇·t − β·∇s − µs, ϕ)

−(K∇uh + t, ∇ϕ) +

  • µ − 1

2∇·β

  • (s − uh), ϕ
  • ≤ 2|||u − uh|||.

Properties Guaranteed upper bound, quasi-exact, and robust. Holds uniformly for any mesh (anis.) and pol. degree. Not computable (infimum over an infinite-dim. space).

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-29
SLIDE 29

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Approximate solution and approximate flux

0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.0 1.8 1.6 1.4 1.2 1.0 0.8 0.6 0.4 0.2 0.0

  • 0.2

1.0 exact solution approximate solution

Approximate solution uh is not in H1

0(Ω)

0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.0 1.5 1.0 0.5 0.0

  • 0.5
  • 1.0
  • 1.5

1.0

  • exact flux
  • approximate flux

Approximate flux −K∇uh is not in H(div, Ω)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-30
SLIDE 30

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Approximate solution and approximate flux

0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.0 1.8 1.6 1.4 1.2 1.0 0.8 0.6 0.4 0.2 0.0

  • 0.2

1.0 postprocessed solution approximate solution exact solution

Construct a postprocessed

  • approx. solution sh in H1

0(Ω)

0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0.0 1.5 1.0 0.5 0.0

  • 0.5
  • 1.0
  • 1.5

1.0

  • postprocessed flux
  • approximate flux
  • exact flux

Construct a postprocessed flux th in H(div, Ω)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-31
SLIDE 31

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-32
SLIDE 32

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A first computable estimate in the energy norm

Theorem (A first computable estimate, energy norm) Let u be the weak solution and let uh ∈ H1(Th) be arbitrary. Take any th ∈ H(div, Ω) and any sh ∈ H1

0(Ω). Then

|||u − uh||| ≤|||uh − sh||| + min

  • C1/2

F,ΩhΩ

minT∈Th c1/2

K,T

, 1 minT∈Th c1/2 β,µ,T

  • × f − ∇·th − β·∇sh − µsh

+

  • K

1 2 ∇uh + K− 1 2 th

  • 2+
  • µ− 1

2∇·β

1

2 (uh − sh)

  • 2 1

2

. Properties Guaranteed upper bound (CF,Ω ≤ 1).

  • K

1 2 ∇uh+K− 1 2 th

  • results from −K∇uh ∈ H(div, Ω).

|||uh − sh||| results from uh ∈ H1

0(Ω).

Advantage: scheme-independent (promoted by Repin). Disadvantage: no info. from computation used, too rough.

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-33
SLIDE 33

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A first computable estimate in the energy norm

Theorem (A first computable estimate, energy norm) Let u be the weak solution and let uh ∈ H1(Th) be arbitrary. Take any th ∈ H(div, Ω) and any sh ∈ H1

0(Ω). Then

|||u − uh||| ≤|||uh − sh||| + min

  • C1/2

F,ΩhΩ

minT∈Th c1/2

K,T

, 1 minT∈Th c1/2 β,µ,T

  • × f − ∇·th − β·∇sh − µsh

+

  • K

1 2 ∇uh + K− 1 2 th

  • 2+
  • µ− 1

2∇·β

1

2 (uh − sh)

  • 2 1

2

. Properties Guaranteed upper bound (CF,Ω ≤ 1).

  • K

1 2 ∇uh+K− 1 2 th

  • results from −K∇uh ∈ H(div, Ω).

|||uh − sh||| results from uh ∈ H1

0(Ω).

Advantage: scheme-independent (promoted by Repin). Disadvantage: no info. from computation used, too rough.

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-34
SLIDE 34

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A first computable estimate in the energy norm

Theorem (A first computable estimate, energy norm) Let u be the weak solution and let uh ∈ H1(Th) be arbitrary. Take any th ∈ H(div, Ω) and any sh ∈ H1

0(Ω). Then

|||u − uh||| ≤|||uh − sh||| + min

  • C1/2

F,ΩhΩ

minT∈Th c1/2

K,T

, 1 minT∈Th c1/2 β,µ,T

  • × f − ∇·th − β·∇sh − µsh

+

  • K

1 2 ∇uh + K− 1 2 th

  • 2+
  • µ− 1

2∇·β

1

2 (uh − sh)

  • 2 1

2

. Properties Guaranteed upper bound (CF,Ω ≤ 1).

  • K

1 2 ∇uh+K− 1 2 th

  • results from −K∇uh ∈ H(div, Ω).

|||uh − sh||| results from uh ∈ H1

0(Ω).

Advantage: scheme-independent (promoted by Repin). Disadvantage: no info. from computation used, too rough.

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-35
SLIDE 35

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A first computable estimate in the energy norm

Theorem (A first computable estimate, energy norm) Let u be the weak solution and let uh ∈ H1(Th) be arbitrary. Take any th ∈ H(div, Ω) and any sh ∈ H1

0(Ω). Then

|||u − uh||| ≤|||uh − sh||| + min

  • C1/2

F,ΩhΩ

minT∈Th c1/2

K,T

, 1 minT∈Th c1/2 β,µ,T

  • × f − ∇·th − β·∇sh − µsh

+

  • K

1 2 ∇uh + K− 1 2 th

  • 2+
  • µ− 1

2∇·β

1

2 (uh − sh)

  • 2 1

2

. Properties Guaranteed upper bound (CF,Ω ≤ 1).

  • K

1 2 ∇uh+K− 1 2 th

  • results from −K∇uh ∈ H(div, Ω).

|||uh − sh||| results from uh ∈ H1

0(Ω).

Advantage: scheme-independent (promoted by Repin). Disadvantage: no info. from computation used, too rough.

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-36
SLIDE 36

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A first computable estimate in the energy norm

Theorem (A first computable estimate, energy norm) Let u be the weak solution and let uh ∈ H1(Th) be arbitrary. Take any th ∈ H(div, Ω) and any sh ∈ H1

0(Ω). Then

|||u − uh||| ≤|||uh − sh||| + min

  • C1/2

F,ΩhΩ

minT∈Th c1/2

K,T

, 1 minT∈Th c1/2 β,µ,T

  • × f − ∇·th − β·∇sh − µsh

+

  • K

1 2 ∇uh + K− 1 2 th

  • 2+
  • µ− 1

2∇·β

1

2 (uh − sh)

  • 2 1

2

. Properties Guaranteed upper bound (CF,Ω ≤ 1).

  • K

1 2 ∇uh+K− 1 2 th

  • results from −K∇uh ∈ H(div, Ω).

|||uh − sh||| results from uh ∈ H1

0(Ω).

Advantage: scheme-independent (promoted by Repin). Disadvantage: no info. from computation used, too rough.

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-37
SLIDE 37

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A first computable estimate in the energy norm

Theorem (A first computable estimate, energy norm) Let u be the weak solution and let uh ∈ H1(Th) be arbitrary. Take any th ∈ H(div, Ω) and any sh ∈ H1

0(Ω). Then

|||u − uh||| ≤|||uh − sh||| + min

  • C1/2

F,ΩhΩ

minT∈Th c1/2

K,T

, 1 minT∈Th c1/2 β,µ,T

  • × f − ∇·th − β·∇sh − µsh

+

  • K

1 2 ∇uh + K− 1 2 th

  • 2+
  • µ− 1

2∇·β

1

2 (uh − sh)

  • 2 1

2

. Properties Guaranteed upper bound (CF,Ω ≤ 1).

  • K

1 2 ∇uh+K− 1 2 th

  • results from −K∇uh ∈ H(div, Ω).

|||uh − sh||| results from uh ∈ H1

0(Ω).

Advantage: scheme-independent (promoted by Repin). Disadvantage: no info. from computation used, too rough.

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-38
SLIDE 38

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-39
SLIDE 39

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A dual norm augmented by the convective derivative

define BD(u, v) := −

  • F∈Fh

(β·nF[ [u] ], { {Π0v} })F. introduce the augmented norm |||v|||⊕ := |||v||| + sup

ϕ∈H1

0(Ω), |||ϕ|||=1

{BA(v, ϕ) + BD(v, ϕ)} when ∇·β∞,T is controlled by (µ − 1

2∇·β) on T for all T

and when v ∈ H1

0(Ω), recover the augmented norm

introduced by Verfürth ’05 BD contribution is new and specific to the nonconforming case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-40
SLIDE 40

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A dual norm augmented by the convective derivative

define BD(u, v) := −

  • F∈Fh

(β·nF[ [u] ], { {Π0v} })F. introduce the augmented norm |||v|||⊕ := |||v||| + sup

ϕ∈H1

0(Ω), |||ϕ|||=1

{BA(v, ϕ) + BD(v, ϕ)} when ∇·β∞,T is controlled by (µ − 1

2∇·β) on T for all T

and when v ∈ H1

0(Ω), recover the augmented norm

introduced by Verfürth ’05 BD contribution is new and specific to the nonconforming case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-41
SLIDE 41

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A dual norm augmented by the convective derivative

define BD(u, v) := −

  • F∈Fh

(β·nF[ [u] ], { {Π0v} })F. introduce the augmented norm |||v|||⊕ := |||v||| + sup

ϕ∈H1

0(Ω), |||ϕ|||=1

{BA(v, ϕ) + BD(v, ϕ)} when ∇·β∞,T is controlled by (µ − 1

2∇·β) on T for all T

and when v ∈ H1

0(Ω), recover the augmented norm

introduced by Verfürth ’05 BD contribution is new and specific to the nonconforming case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-42
SLIDE 42

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

A dual norm augmented by the convective derivative

define BD(u, v) := −

  • F∈Fh

(β·nF[ [u] ], { {Π0v} })F. introduce the augmented norm |||v|||⊕ := |||v||| + sup

ϕ∈H1

0(Ω), |||ϕ|||=1

{BA(v, ϕ) + BD(v, ϕ)} when ∇·β∞,T is controlled by (µ − 1

2∇·β) on T for all T

and when v ∈ H1

0(Ω), recover the augmented norm

introduced by Verfürth ’05 BD contribution is new and specific to the nonconforming case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-43
SLIDE 43

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Optimal abstract estimate in the augmented norm

Theorem (Optimal abstract estimate, augmented norm) Let u be the weak sol. and let uh ∈ H1(Th) be arbitrary. Then |||u − uh|||⊕ ≤ 2 inf

s∈H1

0(Ω)

  • |||uh − s||| +

inf

t∈H(div,Ω)

sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f − ∇·t − β·∇s − µs, ϕ)

− (K∇uh + t, ∇ϕ) +

  • µ − 1

2∇·β

  • (s − uh), ϕ
  • +

sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • inf

t∈H(div,Ω)

{(f − ∇·t − β·∇uh − µuh, ϕ)−(K∇uh + t, ∇ϕ)}−BD(uh, ϕ)

  • ≤5|||u − uh|||⊕.

Comments

  • nly the highlighted terms are new

their form is similar to the energy estimate necessary for robustness in the convection-dominated case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-44
SLIDE 44

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Optimal abstract estimate in the augmented norm

Theorem (Optimal abstract estimate, augmented norm) Let u be the weak sol. and let uh ∈ H1(Th) be arbitrary. Then |||u − uh|||⊕ ≤ 2 inf

s∈H1

0(Ω)

  • |||uh − s||| +

inf

t∈H(div,Ω)

sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f − ∇·t − β·∇s − µs, ϕ)

− (K∇uh + t, ∇ϕ) +

  • µ − 1

2∇·β

  • (s − uh), ϕ
  • +

sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • inf

t∈H(div,Ω)

{(f − ∇·t − β·∇uh − µuh, ϕ)−(K∇uh + t, ∇ϕ)}−BD(uh, ϕ)

  • ≤5|||u − uh|||⊕.

Comments

  • nly the highlighted terms are new

their form is similar to the energy estimate necessary for robustness in the convection-dominated case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-45
SLIDE 45

I Abstract framework A posteriori estimates C Energy norm A first computable estimate Augmented norm

Optimal abstract estimate in the augmented norm

Theorem (Optimal abstract estimate, augmented norm) Let u be the weak sol. and let uh ∈ H1(Th) be arbitrary. Then |||u − uh|||⊕ ≤ 2 inf

s∈H1

0(Ω)

  • |||uh − s||| +

inf

t∈H(div,Ω)

sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f − ∇·t − β·∇s − µs, ϕ)

− (K∇uh + t, ∇ϕ) +

  • µ − 1

2∇·β

  • (s − uh), ϕ
  • +

sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • inf

t∈H(div,Ω)

{(f − ∇·t − β·∇uh − µuh, ϕ)−(K∇uh + t, ∇ϕ)}−BD(uh, ϕ)

  • ≤5|||u − uh|||⊕.

Comments

  • nly the highlighted terms are new

their form is similar to the energy estimate necessary for robustness in the convection-dominated case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-46
SLIDE 46

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-47
SLIDE 47

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Discontinuous Galerkin method

Discontinuous Galerkin method Find uh ∈ Pk(Th) such that for all vh ∈ Pk(Th) (K∇uh, ∇vh) + ((µ − ∇·β)uh, vh) − (uh, β·∇vh) −

  • F∈Fh

{(nF·{ {K∇uh} }ω, [ [vh] ])F + θ(nF·{ {K∇vh} }ω, [ [uh] ])F} +

  • F∈Fh
  • ((αFγK,Fh−1

F

+ γβ,F)[ [uh] ], [ [vh] ])F + (β·nF{ {uh} }, [ [vh] ])F

  • = (f, vh).

jump operator [ [v] ] = v− − v+ average operator { {v} } = 1

2(v− + v+)

diffusivity-weighted av. operator { {v} }ω = (ω−v− + ω+v+) diff.-dep. penalties γK,F (Ern, Stephansen, and Zunino 08) θ: different scheme types (SIPG/NIPG/IIPG/OBB) γβ,F: upwind-weighting stabilization uh ∈ H1

0(Ω), −K∇uh ∈ H(div, Ω)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-48
SLIDE 48

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Discontinuous Galerkin method

Discontinuous Galerkin method Find uh ∈ Pk(Th) such that for all vh ∈ Pk(Th) (K∇uh, ∇vh) + ((µ − ∇·β)uh, vh) − (uh, β·∇vh) −

  • F∈Fh

{(nF·{ {K∇uh} }ω, [ [vh] ])F + θ(nF·{ {K∇vh} }ω, [ [uh] ])F} +

  • F∈Fh
  • ((αFγK,Fh−1

F

+ γβ,F)[ [uh] ], [ [vh] ])F + (β·nF{ {uh} }, [ [vh] ])F

  • = (f, vh).

jump operator [ [v] ] = v− − v+ average operator { {v} } = 1

2(v− + v+)

diffusivity-weighted av. operator { {v} }ω = (ω−v− + ω+v+) diff.-dep. penalties γK,F (Ern, Stephansen, and Zunino 08) θ: different scheme types (SIPG/NIPG/IIPG/OBB) γβ,F: upwind-weighting stabilization uh ∈ H1

0(Ω), −K∇uh ∈ H(div, Ω)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-49
SLIDE 49

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Discontinuous Galerkin method

Discontinuous Galerkin method Find uh ∈ Pk(Th) such that for all vh ∈ Pk(Th) (K∇uh, ∇vh) + ((µ − ∇·β)uh, vh) − (uh, β·∇vh) −

  • F∈Fh

{(nF·{ {K∇uh} }ω, [ [vh] ])F + θ(nF·{ {K∇vh} }ω, [ [uh] ])F} +

  • F∈Fh
  • ((αFγK,Fh−1

F

+ γβ,F)[ [uh] ], [ [vh] ])F + (β·nF{ {uh} }, [ [vh] ])F

  • = (f, vh).

jump operator [ [v] ] = v− − v+ average operator { {v} } = 1

2(v− + v+)

diffusivity-weighted av. operator { {v} }ω = (ω−v− + ω+v+) diff.-dep. penalties γK,F (Ern, Stephansen, and Zunino 08) θ: different scheme types (SIPG/NIPG/IIPG/OBB) γβ,F: upwind-weighting stabilization uh ∈ H1

0(Ω), −K∇uh ∈ H(div, Ω)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-50
SLIDE 50

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-51
SLIDE 51

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Potential- and flux-conforming reconstructions

Choice of sh: the Oswald interpolate of uh IOs : Pk(Th) → Pk(Th) ∩ H1

0(Ω)

prescribed at Lagrange nodes by arithmetic averages IOs(vh)(V) = 1 #(TV)

  • T∈TV

vh|T(V)

  • ne can also use diffusivity-weighted averages

(Ainsworth ’05) Choice of th: a new H(div, Ω) flux reconstruction Ern, Nicaise & Vohralík ’07 (matching meshes) the present work (nonmatching meshes)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-52
SLIDE 52

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Potential- and flux-conforming reconstructions

Choice of sh: the Oswald interpolate of uh IOs : Pk(Th) → Pk(Th) ∩ H1

0(Ω)

prescribed at Lagrange nodes by arithmetic averages IOs(vh)(V) = 1 #(TV)

  • T∈TV

vh|T(V)

  • ne can also use diffusivity-weighted averages

(Ainsworth ’05) Choice of th: a new H(div, Ω) flux reconstruction Ern, Nicaise & Vohralík ’07 (matching meshes) the present work (nonmatching meshes)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-53
SLIDE 53

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Diffusive flux reconstruction

RTNl(Th): Raviart–Thomas–Nédélec spaces of degree l

Intro du tion La mtho de GD Estimat i
  • ns
d'erreur a p
  • sterio
ri Pure diusion ADR: semi-robust estimat e s ADR: robust estima t e s Numeri al results Lo ally
  • mputable
estimate I I I Ravia rtThomas FE spa es
  • f
degree l : RT l h l = l = 1 Constru tion
  • f
t h RT l h ( l p
  • r
p 1) dof 's fo r no rmal
  • mp
  • nent
  • n
ea h fa e: q h l F , t h n F q h F n t F K h u h F u h q h F dof 's in ea h element: r h d l 1 T , t h r h T K u h r h T F T T F n t F Kr h u h F Alexan d re Ern Estimat i
  • ns
d'erreur a p
  • sterio
ri p
  • ur
les mtho des GD

Construction of th ∈ RTNl(Th), l = k or l = k − 1 normal components on each side: ∀qh ∈ Pl(F), (th·nF, qh)F =

  • −nF·{

{K∇uh} }ω + αFγK,Fh−1

F [

[uh] ], qh

  • F
  • n each element (only for l ≥ 1): ∀rh ∈ Pd

l−1(T),

(th, rh)T = −(K∇uh, rh)T + θ

  • F∈FT

ωT,F(nF·Krh, [ [uh] ])F

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-54
SLIDE 54

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Diffusive flux reconstruction

RTNl(Th): Raviart–Thomas–Nédélec spaces of degree l

Intro du tion La mtho de GD Estimat i
  • ns
d'erreur a p
  • sterio
ri Pure diusion ADR: semi-robust estimat e s ADR: robust estima t e s Numeri al results Lo ally
  • mputable
estimate I I I Ravia rtThomas FE spa es
  • f
degree l : RT l h l = l = 1 Constru tion
  • f
t h RT l h ( l p
  • r
p 1) dof 's fo r no rmal
  • mp
  • nent
  • n
ea h fa e: q h l F , t h n F q h F n t F K h u h F u h q h F dof 's in ea h element: r h d l 1 T , t h r h T K u h r h T F T T F n t F Kr h u h F Alexan d re Ern Estimat i
  • ns
d'erreur a p
  • sterio
ri p
  • ur
les mtho des GD

Construction of th ∈ RTNl(Th), l = k or l = k − 1 normal components on each side: ∀qh ∈ Pl(F), (th·nF, qh)F =

  • −nF·{

{K∇uh} }ω + αFγK,Fh−1

F [

[uh] ], qh

  • F
  • n each element (only for l ≥ 1): ∀rh ∈ Pd

l−1(T),

(th, rh)T = −(K∇uh, rh)T + θ

  • F∈FT

ωT,F(nF·Krh, [ [uh] ])F

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-55
SLIDE 55

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Diffusive flux reconstruction property

Crucial diffusive flux reconstruction property note that all the terms of the DG scheme are used in the construction of th denote by Πl the L2-orthogonal projection onto Pk(Th) the above construction yields ∇·th = Πl(f) Proof: (∇·th, ξh)T = −(th, ∇ξh)T + th·n, ξh∂T = Bh(uh, ξh) = (f, ξh)T diffusive flux as in the Raviart–Thomas–Nédélec mixed finite element method of order l, by local postprocessing

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-56
SLIDE 56

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Diffusive flux reconstruction property

Crucial diffusive flux reconstruction property note that all the terms of the DG scheme are used in the construction of th denote by Πl the L2-orthogonal projection onto Pk(Th) the above construction yields ∇·th = Πl(f) Proof: (∇·th, ξh)T = −(th, ∇ξh)T + th·n, ξh∂T = Bh(uh, ξh) = (f, ξh)T diffusive flux as in the Raviart–Thomas–Nédélec mixed finite element method of order l, by local postprocessing

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-57
SLIDE 57

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Diffusive flux reconstruction property

Crucial diffusive flux reconstruction property note that all the terms of the DG scheme are used in the construction of th denote by Πl the L2-orthogonal projection onto Pk(Th) the above construction yields ∇·th = Πl(f) Proof: (∇·th, ξh)T = −(th, ∇ξh)T + th·n, ξh∂T = Bh(uh, ξh) = (f, ξh)T diffusive flux as in the Raviart–Thomas–Nédélec mixed finite element method of order l, by local postprocessing

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-58
SLIDE 58

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Diffusive flux reconstruction property

Crucial diffusive flux reconstruction property note that all the terms of the DG scheme are used in the construction of th denote by Πl the L2-orthogonal projection onto Pk(Th) the above construction yields ∇·th = Πl(f) Proof: (∇·th, ξh)T = −(th, ∇ξh)T + th·n, ξh∂T = Bh(uh, ξh) = (f, ξh)T diffusive flux as in the Raviart–Thomas–Nédélec mixed finite element method of order l, by local postprocessing

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-59
SLIDE 59

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Diffusive flux reconstruction property

Crucial diffusive flux reconstruction property note that all the terms of the DG scheme are used in the construction of th denote by Πl the L2-orthogonal projection onto Pk(Th) the above construction yields ∇·th = Πl(f) Proof: (∇·th, ξh)T = −(th, ∇ξh)T + th·n, ξh∂T = Bh(uh, ξh) = (f, ξh)T diffusive flux as in the Raviart–Thomas–Nédélec mixed finite element method of order l, by local postprocessing

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-60
SLIDE 60

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) = f

Towards an a posteriori error estimate recall that the energy norm framework gives |||u−uh||| ≤ |||uh−sh|||+ sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f−∇·th, ϕ)−(K∇uh+th, ∇ϕ)
  • note that, by the Cauchy–Schwarz inequality:

(K∇uh + th, ∇ϕ)T ≤ K

1 2 ∇uh + K− 1 2 thT|||ϕ|||T

local conservativity of th: (f − ∇·th, ϕ)T = (f − ∇·th, ϕ − Π0(ϕ))T Poincaré inequality (CP = 1/π2), energy norm definition: ϕ − Π0(ϕ)T ≤ C

1 2

P hT∇ϕT ≤ C1/2 P

hT c1/2

K,T

|||ϕ|||T notation: cK,T (CK,T) is the min (max) eigenvalue of K on T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-61
SLIDE 61

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) = f

Towards an a posteriori error estimate recall that the energy norm framework gives |||u−uh||| ≤ |||uh−sh|||+ sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f−∇·th, ϕ)−(K∇uh+th, ∇ϕ)
  • note that, by the Cauchy–Schwarz inequality:

(K∇uh + th, ∇ϕ)T ≤ K

1 2 ∇uh + K− 1 2 thT|||ϕ|||T

local conservativity of th: (f − ∇·th, ϕ)T = (f − ∇·th, ϕ − Π0(ϕ))T Poincaré inequality (CP = 1/π2), energy norm definition: ϕ − Π0(ϕ)T ≤ C

1 2

P hT∇ϕT ≤ C1/2 P

hT c1/2

K,T

|||ϕ|||T notation: cK,T (CK,T) is the min (max) eigenvalue of K on T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-62
SLIDE 62

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) = f

Towards an a posteriori error estimate recall that the energy norm framework gives |||u−uh||| ≤ |||uh−sh|||+ sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f−∇·th, ϕ)−(K∇uh+th, ∇ϕ)
  • note that, by the Cauchy–Schwarz inequality:

(K∇uh + th, ∇ϕ)T ≤ K

1 2 ∇uh + K− 1 2 thT|||ϕ|||T

local conservativity of th: (f − ∇·th, ϕ)T = (f − ∇·th, ϕ − Π0(ϕ))T Poincaré inequality (CP = 1/π2), energy norm definition: ϕ − Π0(ϕ)T ≤ C

1 2

P hT∇ϕT ≤ C1/2 P

hT c1/2

K,T

|||ϕ|||T notation: cK,T (CK,T) is the min (max) eigenvalue of K on T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-63
SLIDE 63

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) = f

Towards an a posteriori error estimate recall that the energy norm framework gives |||u−uh||| ≤ |||uh−sh|||+ sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f−∇·th, ϕ)−(K∇uh+th, ∇ϕ)
  • note that, by the Cauchy–Schwarz inequality:

(K∇uh + th, ∇ϕ)T ≤ K

1 2 ∇uh + K− 1 2 thT|||ϕ|||T

local conservativity of th: (f − ∇·th, ϕ)T = (f − ∇·th, ϕ − Π0(ϕ))T Poincaré inequality (CP = 1/π2), energy norm definition: ϕ − Π0(ϕ)T ≤ C

1 2

P hT∇ϕT ≤ C1/2 P

hT c1/2

K,T

|||ϕ|||T notation: cK,T (CK,T) is the min (max) eigenvalue of K on T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-64
SLIDE 64

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) = f

Towards an a posteriori error estimate recall that the energy norm framework gives |||u−uh||| ≤ |||uh−sh|||+ sup

ϕ∈H1

0(Ω), |||ϕ|||=1

  • (f−∇·th, ϕ)−(K∇uh+th, ∇ϕ)
  • note that, by the Cauchy–Schwarz inequality:

(K∇uh + th, ∇ϕ)T ≤ K

1 2 ∇uh + K− 1 2 thT|||ϕ|||T

local conservativity of th: (f − ∇·th, ϕ)T = (f − ∇·th, ϕ − Π0(ϕ))T Poincaré inequality (CP = 1/π2), energy norm definition: ϕ − Π0(ϕ)T ≤ C

1 2

P hT∇ϕT ≤ C1/2 P

hT c1/2

K,T

|||ϕ|||T notation: cK,T (CK,T) is the min (max) eigenvalue of K on T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-65
SLIDE 65

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) = f

Theorem (A posteriori error estimate, pure diffusion case) There holds |||u − uh|||2 ≤

  • T∈Th
  • η2

NC,T + (ηR,T + ηDF,T)2

. nonconformity estimator

ηNC,T := |||uh − IOs(uh)|||T

diffusive flux estimator

ηDF,T := K

1 2 ∇uh + K− 1 2 thT

residual estimator

ηR,T := C1/2

P

hT c1/2

K,T

f − Πl(f)T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-66
SLIDE 66

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) = f

Theorem (A posteriori error estimate, pure diffusion case) There holds |||u − uh|||2 ≤

  • T∈Th
  • η2

NC,T + (ηR,T + ηDF,T)2

. nonconformity estimator

ηNC,T := |||uh − IOs(uh)|||T

diffusive flux estimator

ηDF,T := K

1 2 ∇uh + K− 1 2 thT

residual estimator

ηR,T := C1/2

P

hT c1/2

K,T

f − Πl(f)T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-67
SLIDE 67

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) = f

Theorem (A posteriori error estimate, pure diffusion case) There holds |||u − uh|||2 ≤

  • T∈Th
  • η2

NC,T + (ηR,T + ηDF,T)2

. nonconformity estimator

ηNC,T := |||uh − IOs(uh)|||T

diffusive flux estimator

ηDF,T := K

1 2 ∇uh + K− 1 2 thT

residual estimator

ηR,T := C1/2

P

hT c1/2

K,T

f − Πl(f)T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-68
SLIDE 68

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) = f

Theorem (A posteriori error estimate, pure diffusion case) There holds |||u − uh|||2 ≤

  • T∈Th
  • η2

NC,T + (ηR,T + ηDF,T)2

. nonconformity estimator

ηNC,T := |||uh − IOs(uh)|||T

diffusive flux estimator

ηDF,T := K

1 2 ∇uh + K− 1 2 thT

residual estimator

ηR,T := C1/2

P

hT c1/2

K,T

f − Πl(f)T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-69
SLIDE 69

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Convective flux reconstruction

Diffusive flux reconstruction th ∈ RTNl(Th), l = k or l = k − 1 as in the pure diffusion case Convective flux reconstr. qh ∈ RTNl(Th), l = k or l = k − 1 normal components on each side: ∀qh ∈ Pl(F), (qh·nF, qh)F = (β·nF{ {uh} } + γβ,F[ [uh] ], qh)F

  • n each element (only for l ≥ 1): ∀rh ∈ Pd

l−1(T),

(qh, rh)T = (uh, β·rh)T Crucial property (∇·th+∇·qh+(µ−∇·β)uh, ξh)T = (f, ξh)T ∀T ∈ Th, ∀ξh ∈ Pl(T)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-70
SLIDE 70

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Convective flux reconstruction

Diffusive flux reconstruction th ∈ RTNl(Th), l = k or l = k − 1 as in the pure diffusion case Convective flux reconstr. qh ∈ RTNl(Th), l = k or l = k − 1 normal components on each side: ∀qh ∈ Pl(F), (qh·nF, qh)F = (β·nF{ {uh} } + γβ,F[ [uh] ], qh)F

  • n each element (only for l ≥ 1): ∀rh ∈ Pd

l−1(T),

(qh, rh)T = (uh, β·rh)T Crucial property (∇·th+∇·qh+(µ−∇·β)uh, ξh)T = (f, ξh)T ∀T ∈ Th, ∀ξh ∈ Pl(T)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-71
SLIDE 71

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Convective flux reconstruction

Diffusive flux reconstruction th ∈ RTNl(Th), l = k or l = k − 1 as in the pure diffusion case Convective flux reconstr. qh ∈ RTNl(Th), l = k or l = k − 1 normal components on each side: ∀qh ∈ Pl(F), (qh·nF, qh)F = (β·nF{ {uh} } + γβ,F[ [uh] ], qh)F

  • n each element (only for l ≥ 1): ∀rh ∈ Pd

l−1(T),

(qh, rh)T = (uh, β·rh)T Crucial property (∇·th+∇·qh+(µ−∇·β)uh, ξh)T = (f, ξh)T ∀T ∈ Th, ∀ξh ∈ Pl(T)

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-72
SLIDE 72

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-73
SLIDE 73

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) + β·∇u + µu = f

Theorem (A posteriori error estimate, energy norm) There holds |||u − uh||| ≤ η, η :=

  • T∈Th

η2

NC,T

1/2 +

  • T∈Th

(ηR,T + ηDF,T + ηC,1,T + ηC,2,T + ηU,T)2 1

2

, where ηNC,T = |||uh − IOs(uh)|||T (nonconformity), ηDF,T = min

  • η(1)

DF,T, η(2) DF,T

  • (diffusive flux),

ηR,T = mTf − ∇·th − ∇·qh − (µ − ∇·β)uh0,T (residual), ηC,1,T = mT(Id − Π0)(∇·(qh − βsh))0,T (convection), ηC,2,T = c−1/2

β,µ,T

  • 1

2(∇·β)(uh − sh)

  • 0,T (convection),

ηU,T =

F∈FT mFΠ0,F((qh − βsh)·nF)F (upwinding).

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-74
SLIDE 74

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A post. estimate for −∇·(K∇u) + β·∇u + µu = f

Theorem (A posteriori error estimate, energy norm) There holds |||u − uh||| ≤ η, η :=

  • T∈Th

η2

NC,T

1/2 +

  • T∈Th

(ηR,T + ηDF,T + ηC,1,T + ηC,2,T + ηU,T)2 1

2

, where ηNC,T = |||uh − IOs(uh)|||T (nonconformity), ηDF,T = min

  • η(1)

DF,T, η(2) DF,T

  • (diffusive flux),

ηR,T = mTf − ∇·th − ∇·qh − (µ − ∇·β)uh0,T (residual), ηC,1,T = mT(Id − Π0)(∇·(qh − βsh))0,T (convection), ηC,2,T = c−1/2

β,µ,T

  • 1

2(∇·β)(uh − sh)

  • 0,T (convection),

ηU,T =

F∈FT mFΠ0,F((qh − βsh)·nF)F (upwinding).

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-75
SLIDE 75

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Individual estimators

Diffusive flux estimator ηDF,T ηDF,T = min

  • η(1)

DF,T, η(2) DF,T

  • η(1)

DF,T = K

1 2 ∇uh + K− 1 2 th0,T

η(2)

DF,T = mT(Id − Π0)(∇·(K∇uh + th))0,T +

  • m1/2

T

  • F∈FT C1/2

t,T,F(K∇uh + th)·nFF

cutoff fcts of local Péclet and Damköhler numbers in η(2)

DF,T:

mT := min{C1/2

P

hTc−1/2

K,T , c−1/2 β,µ,T},

  • mT := min{(CP + C1/2

P

)hTc−1

K,T, h−1 T c−1 β,µ,T + c−1/2 β,µ,Tc−1/2 K,T /2}

η(1)

DF,T alone cannot be shown semi-robust (Verfürth ’08)

the idea of defining of ηDF,T using a min has recently been proposed in Cheddadi, Fuˇ cík, Prieto, Vohralík ’08 in context

  • f conforming FEM and reaction–diffusion problems
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-76
SLIDE 76

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Individual estimators

Diffusive flux estimator ηDF,T ηDF,T = min

  • η(1)

DF,T, η(2) DF,T

  • η(1)

DF,T = K

1 2 ∇uh + K− 1 2 th0,T

η(2)

DF,T = mT(Id − Π0)(∇·(K∇uh + th))0,T +

  • m1/2

T

  • F∈FT C1/2

t,T,F(K∇uh + th)·nFF

cutoff fcts of local Péclet and Damköhler numbers in η(2)

DF,T:

mT := min{C1/2

P

hTc−1/2

K,T , c−1/2 β,µ,T},

  • mT := min{(CP + C1/2

P

)hTc−1

K,T, h−1 T c−1 β,µ,T + c−1/2 β,µ,Tc−1/2 K,T /2}

η(1)

DF,T alone cannot be shown semi-robust (Verfürth ’08)

the idea of defining of ηDF,T using a min has recently been proposed in Cheddadi, Fuˇ cík, Prieto, Vohralík ’08 in context

  • f conforming FEM and reaction–diffusion problems
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-77
SLIDE 77

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Individual estimators

Diffusive flux estimator ηDF,T ηDF,T = min

  • η(1)

DF,T, η(2) DF,T

  • η(1)

DF,T = K

1 2 ∇uh + K− 1 2 th0,T

η(2)

DF,T = mT(Id − Π0)(∇·(K∇uh + th))0,T +

  • m1/2

T

  • F∈FT C1/2

t,T,F(K∇uh + th)·nFF

cutoff fcts of local Péclet and Damköhler numbers in η(2)

DF,T:

mT := min{C1/2

P

hTc−1/2

K,T , c−1/2 β,µ,T},

  • mT := min{(CP + C1/2

P

)hTc−1

K,T, h−1 T c−1 β,µ,T + c−1/2 β,µ,Tc−1/2 K,T /2}

η(1)

DF,T alone cannot be shown semi-robust (Verfürth ’08)

the idea of defining of ηDF,T using a min has recently been proposed in Cheddadi, Fuˇ cík, Prieto, Vohralík ’08 in context

  • f conforming FEM and reaction–diffusion problems
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-78
SLIDE 78

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Individual estimators

Diffusive flux estimator ηDF,T ηDF,T = min

  • η(1)

DF,T, η(2) DF,T

  • η(1)

DF,T = K

1 2 ∇uh + K− 1 2 th0,T

η(2)

DF,T = mT(Id − Π0)(∇·(K∇uh + th))0,T +

  • m1/2

T

  • F∈FT C1/2

t,T,F(K∇uh + th)·nFF

cutoff fcts of local Péclet and Damköhler numbers in η(2)

DF,T:

mT := min{C1/2

P

hTc−1/2

K,T , c−1/2 β,µ,T},

  • mT := min{(CP + C1/2

P

)hTc−1

K,T, h−1 T c−1 β,µ,T + c−1/2 β,µ,Tc−1/2 K,T /2}

η(1)

DF,T alone cannot be shown semi-robust (Verfürth ’08)

the idea of defining of ηDF,T using a min has recently been proposed in Cheddadi, Fuˇ cík, Prieto, Vohralík ’08 in context

  • f conforming FEM and reaction–diffusion problems
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-79
SLIDE 79

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Individual estimators

Diffusive flux estimator ηDF,T ηDF,T = min

  • η(1)

DF,T, η(2) DF,T

  • η(1)

DF,T = K

1 2 ∇uh + K− 1 2 th0,T

η(2)

DF,T = mT(Id − Π0)(∇·(K∇uh + th))0,T +

  • m1/2

T

  • F∈FT C1/2

t,T,F(K∇uh + th)·nFF

cutoff fcts of local Péclet and Damköhler numbers in η(2)

DF,T:

mT := min{C1/2

P

hTc−1/2

K,T , c−1/2 β,µ,T},

  • mT := min{(CP + C1/2

P

)hTc−1

K,T, h−1 T c−1 β,µ,T + c−1/2 β,µ,Tc−1/2 K,T /2}

η(1)

DF,T alone cannot be shown semi-robust (Verfürth ’08)

the idea of defining of ηDF,T using a min has recently been proposed in Cheddadi, Fuˇ cík, Prieto, Vohralík ’08 in context

  • f conforming FEM and reaction–diffusion problems
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-80
SLIDE 80

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Individual estimators

Diffusive flux estimator ηDF,T ηDF,T = min

  • η(1)

DF,T, η(2) DF,T

  • η(1)

DF,T = K

1 2 ∇uh + K− 1 2 th0,T

η(2)

DF,T = mT(Id − Π0)(∇·(K∇uh + th))0,T +

  • m1/2

T

  • F∈FT C1/2

t,T,F(K∇uh + th)·nFF

cutoff fcts of local Péclet and Damköhler numbers in η(2)

DF,T:

mT := min{C1/2

P

hTc−1/2

K,T , c−1/2 β,µ,T},

  • mT := min{(CP + C1/2

P

)hTc−1

K,T, h−1 T c−1 β,µ,T + c−1/2 β,µ,Tc−1/2 K,T /2}

η(1)

DF,T alone cannot be shown semi-robust (Verfürth ’08)

the idea of defining of ηDF,T using a min has recently been proposed in Cheddadi, Fuˇ cík, Prieto, Vohralík ’08 in context

  • f conforming FEM and reaction–diffusion problems
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-81
SLIDE 81

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Individual estimators

Upwinding estimator ηU,T ηU,T =

F∈FT mFΠ0,F((qh − βsh)·nF)F

cutoff function of local Péclet and Damköhler numbers: m2

F = min

  • max

T∈TF

  • CF,T,F

|F|h2

T

|T|cK,T

  • , max

T∈TF

  • |F|

|T|cβ,µ,T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-82
SLIDE 82

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Individual estimators

Upwinding estimator ηU,T ηU,T =

F∈FT mFΠ0,F((qh − βsh)·nF)F

cutoff function of local Péclet and Damköhler numbers: m2

F = min

  • max

T∈TF

  • CF,T,F

|F|h2

T

|T|cK,T

  • , max

T∈TF

  • |F|

|T|cβ,µ,T

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-83
SLIDE 83

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Properties of the estimate

Principal properties guaranteed upper bound no constants in principal estimators, known constants in the other ones cutoff functions of local Péclet (hTβ∞,Tc−1

K,T) and

Damköhler (h2

Tcβ,µ,Tc−1 K,T) numbers (here cβ,µ,T is the

(essential) minimum of (µ − 1

2∇·β))

explicit dependence on the mesh and data valid for arbitrary polynomial degree and data nonmatching meshes residual estimator ηR,T is a higher-order term (data

  • scillation)
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-84
SLIDE 84

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.
  • Loc. efficiency for −∇·(K∇u) + β·∇u + µu = f

Theorem (Local efficiency, energy norm) There holds ηNC,T +ηDF,T +ηR,T +ηC,1,T +ηC,2,T +ηU,T ≤ Ceff,T|||u −uh|||∗,

ET .

Properties the estimates are locally efficient

  • nly semi-robustness: overestimation is a function of local

Péclet and Damköhler numbers

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-85
SLIDE 85

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.
  • Loc. efficiency for −∇·(K∇u) + β·∇u + µu = f

Theorem (Local efficiency, energy norm) There holds ηNC,T +ηDF,T +ηR,T +ηC,1,T +ηC,2,T +ηU,T ≤ Ceff,T|||u −uh|||∗,

ET .

Properties the estimates are locally efficient

  • nly semi-robustness: overestimation is a function of local

Péclet and Damköhler numbers

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-86
SLIDE 86

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.
  • Loc. efficiency for −∇·(K∇u) + β·∇u + µu = f

Theorem (Local efficiency, energy norm) There holds ηNC,T +ηDF,T +ηR,T +ηC,1,T +ηC,2,T +ηU,T ≤ Ceff,T|||u −uh|||∗,

ET .

Properties the estimates are locally efficient

  • nly semi-robustness: overestimation is a function of local

Péclet and Damköhler numbers

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-87
SLIDE 87

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-88
SLIDE 88

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A dual norm augmented by the convective derivative

define BD(u, v) := −

  • F∈Fh

(β·nF[ [u] ], { {Π0v} })F. introduce the augmented norm |||v|||⊕ := |||v||| + sup

ϕ∈H1

0(Ω), |||ϕ|||=1

{BA(v, ϕ) + BD(v, ϕ)} when ∇·β∞,T is controlled by (µ − 1

2∇·β) on T for all T

and when v ∈ H1

0(Ω), recover the augmented norm

introduced by Verfürth ’05 BD contribution is new and specific to the nonconforming case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-89
SLIDE 89

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A dual norm augmented by the convective derivative

define BD(u, v) := −

  • F∈Fh

(β·nF[ [u] ], { {Π0v} })F. introduce the augmented norm |||v|||⊕ := |||v||| + sup

ϕ∈H1

0(Ω), |||ϕ|||=1

{BA(v, ϕ) + BD(v, ϕ)} when ∇·β∞,T is controlled by (µ − 1

2∇·β) on T for all T

and when v ∈ H1

0(Ω), recover the augmented norm

introduced by Verfürth ’05 BD contribution is new and specific to the nonconforming case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-90
SLIDE 90

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A dual norm augmented by the convective derivative

define BD(u, v) := −

  • F∈Fh

(β·nF[ [u] ], { {Π0v} })F. introduce the augmented norm |||v|||⊕ := |||v||| + sup

ϕ∈H1

0(Ω), |||ϕ|||=1

{BA(v, ϕ) + BD(v, ϕ)} when ∇·β∞,T is controlled by (µ − 1

2∇·β) on T for all T

and when v ∈ H1

0(Ω), recover the augmented norm

introduced by Verfürth ’05 BD contribution is new and specific to the nonconforming case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-91
SLIDE 91

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

A dual norm augmented by the convective derivative

define BD(u, v) := −

  • F∈Fh

(β·nF[ [u] ], { {Π0v} })F. introduce the augmented norm |||v|||⊕ := |||v||| + sup

ϕ∈H1

0(Ω), |||ϕ|||=1

{BA(v, ϕ) + BD(v, ϕ)} when ∇·β∞,T is controlled by (µ − 1

2∇·β) on T for all T

and when v ∈ H1

0(Ω), recover the augmented norm

introduced by Verfürth ’05 BD contribution is new and specific to the nonconforming case

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-92
SLIDE 92

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Augmented norm a posteriori error estimate

Estimator

  • η := 2η +

T∈Th

(ηR,T + ηDF,T + ηC,1,T + ηU,T)2 1/2 η, ηR,T, and ηDF,T defined previously for the energy norm

  • ηC,1,T and

ηU,T – slight modifications of ηC,1,T and ηU,T Global jump seminorm define |||v|||2

#,Fh =

  • T∈Th
  • F∈FT

1 #(TF)

  • cK,T

cK,TT αFγK,Fh−1

F [

[v] ]2

F

+ cβ,µ,ThF[ [v] ]2

F + m2 TT β2 ∞,TT h−1 F [

[v] ]2

0,FF ∩FT

  • ,

the first two terms are natural for DG methods the third term at least contains the cutoff factor mTT

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-93
SLIDE 93

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Augmented norm a posteriori error estimate

Estimator

  • η := 2η +

T∈Th

(ηR,T + ηDF,T + ηC,1,T + ηU,T)2 1/2 η, ηR,T, and ηDF,T defined previously for the energy norm

  • ηC,1,T and

ηU,T – slight modifications of ηC,1,T and ηU,T Global jump seminorm define |||v|||2

#,Fh =

  • T∈Th
  • F∈FT

1 #(TF)

  • cK,T

cK,TT αFγK,Fh−1

F [

[v] ]2

F

+ cβ,µ,ThF[ [v] ]2

F + m2 TT β2 ∞,TT h−1 F [

[v] ]2

0,FF ∩FT

  • ,

the first two terms are natural for DG methods the third term at least contains the cutoff factor mTT

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-94
SLIDE 94

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Augmented norm estimate and its efficiency

Theorem (Fully robust a posteriori estimate) There holds |||u − uh|||⊕ + |||u − uh|||#,Fh ≤ η + |||uh|||#,Fh ≤ ˜ C(|||u − uh|||⊕ + |||u − uh|||#,Fh). fully robust with respect to convection- or reaction dominance sharper than Schötzau & Zhu ’08 because of the cutoff factor in the jump seminorm

  • nly global efficiency

the norm ||| · |||⊕ is a dual norm and is difficult to evaluate

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-95
SLIDE 95

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Augmented norm estimate and its efficiency

Theorem (Fully robust a posteriori estimate) There holds |||u − uh|||⊕ + |||u − uh|||#,Fh ≤ η + |||uh|||#,Fh ≤ ˜ C(|||u − uh|||⊕ + |||u − uh|||#,Fh). fully robust with respect to convection- or reaction dominance sharper than Schötzau & Zhu ’08 because of the cutoff factor in the jump seminorm

  • nly global efficiency

the norm ||| · |||⊕ is a dual norm and is difficult to evaluate

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-96
SLIDE 96

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Augmented norm estimate and its efficiency

Theorem (Fully robust a posteriori estimate) There holds |||u − uh|||⊕ + |||u − uh|||#,Fh ≤ η + |||uh|||#,Fh ≤ ˜ C(|||u − uh|||⊕ + |||u − uh|||#,Fh). fully robust with respect to convection- or reaction dominance sharper than Schötzau & Zhu ’08 because of the cutoff factor in the jump seminorm

  • nly global efficiency

the norm ||| · |||⊕ is a dual norm and is difficult to evaluate

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-97
SLIDE 97

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Augmented norm estimate and its efficiency

Theorem (Fully robust a posteriori estimate) There holds |||u − uh|||⊕ + |||u − uh|||#,Fh ≤ η + |||uh|||#,Fh ≤ ˜ C(|||u − uh|||⊕ + |||u − uh|||#,Fh). fully robust with respect to convection- or reaction dominance sharper than Schötzau & Zhu ’08 because of the cutoff factor in the jump seminorm

  • nly global efficiency

the norm ||| · |||⊕ is a dual norm and is difficult to evaluate

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-98
SLIDE 98

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Augmented norm estimate and its efficiency

Theorem (Fully robust a posteriori estimate) There holds |||u − uh|||⊕ + |||u − uh|||#,Fh ≤ η + |||uh|||#,Fh ≤ ˜ C(|||u − uh|||⊕ + |||u − uh|||#,Fh). fully robust with respect to convection- or reaction dominance sharper than Schötzau & Zhu ’08 because of the cutoff factor in the jump seminorm

  • nly global efficiency

the norm ||| · |||⊕ is a dual norm and is difficult to evaluate

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-99
SLIDE 99

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-100
SLIDE 100

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Nonmatching grids

Oswald interpolate on nonmatching grids consider a matching simplicial submesh Th of Th consider uh ∈ Pk(Th) as function in Pk( Th) take IOs(uh) on Th Reconstruction of th by direct prescription directly prescribe th ∈ RTNl( Th) by the values of uh this gives (∇·th, ξh)T = (f, ξh)T for all T ∈ Th and all ξh ∈ Pl(T) Reconstruction of th by solving local linear systems consider the simplicial submesh RT of each T solve a local minimization problem (local linear system) on each T get in particular ∇·th = Πlf

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-101
SLIDE 101

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Nonmatching grids

Oswald interpolate on nonmatching grids consider a matching simplicial submesh Th of Th consider uh ∈ Pk(Th) as function in Pk( Th) take IOs(uh) on Th Reconstruction of th by direct prescription directly prescribe th ∈ RTNl( Th) by the values of uh this gives (∇·th, ξh)T = (f, ξh)T for all T ∈ Th and all ξh ∈ Pl(T) Reconstruction of th by solving local linear systems consider the simplicial submesh RT of each T solve a local minimization problem (local linear system) on each T get in particular ∇·th = Πlf

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-102
SLIDE 102

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Nonmatching grids

Oswald interpolate on nonmatching grids consider a matching simplicial submesh Th of Th consider uh ∈ Pk(Th) as function in Pk( Th) take IOs(uh) on Th Reconstruction of th by direct prescription directly prescribe th ∈ RTNl( Th) by the values of uh this gives (∇·th, ξh)T = (f, ξh)T for all T ∈ Th and all ξh ∈ Pl(T) Reconstruction of th by solving local linear systems consider the simplicial submesh RT of each T solve a local minimization problem (local linear system) on each T get in particular ∇·th = Πlf

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-103
SLIDE 103

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-104
SLIDE 104

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Convection-dominated problem, FVs, energy estimates

consider the convection–diffusion–reaction equation −ε△u + ∇·(u(0, 1)) + u = f in Ω = (0, 1) × (0, 1) analytical solution: layer of width a u(x, y) = 0.5

  • 1 − tanh

0.5 − x a

  • consider

ε = 1, a = 0.5 ε = 10−2, a = 0.05 ε = 10−4, a = 0.02

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-105
SLIDE 105

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Analytical solutions

0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.2 0.4 0.6 0.8 1 0.2 0.4 0.6 0.8 1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 x y p

Case ε = 1, a = 0.5

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0.2 0.4 0.6 0.8 1 0.2 0.4 0.6 0.8 1 0.2 0.4 0.6 0.8 1 x y p

Case ε = 10−4, a = 0.02

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-106
SLIDE 106

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Error distribution on a uniformly refined mesh, ε = 1, a = 0.5

1 1.5 2 2.5 3 3.5 4 4.5 x 10

−3

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

Estimated error distribution

0.5 1 1.5 2 2.5 3 x 10

−3

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

Exact error distribution

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-107
SLIDE 107

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Estimated and actual errors and the effectivity index, ε = 1, a = 0.5

10

1

10

2

10

3

10

4

10

5

10

−5

10

−4

10

−3

10

−2

10

−1

10 Number of triangles Energy error error uniform

  • est. uniform
  • est. res. uniform
  • est. nonc. uniform
  • est. upw. uniform
  • est. react. uniform
  • est. conv. uniform

The different estimators

10

1

10

2

10

3

10

4

10

5

1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2 Number of triangles Efficiency efficiency uniform

Effectivity index

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-108
SLIDE 108

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Error distribution on a uniformly refined mesh, ε = 10−2, a = 0.05

2 4 6 8 10 12 14 16 18 x 10

−3

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

Estimated error distribution

0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 2.2 x 10

−3

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1

Exact error distribution

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-109
SLIDE 109

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Approximate solution and the corresponding adaptively refined mesh, ε = 10−4, a = 0.02

0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 0.2 0.4 0.6 0.8 1 0.2 0.4 0.6 0.8 1 0.2 0.4 0.6 0.8 1 x y p

Approximate solution

0.2 0.4 0.6 0.8 1 0.2 0.4 0.6 0.8 1 x y

Adaptively refined mesh

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-110
SLIDE 110

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Convection-dominated problem, DG, energy and augmented estimates, ǫ = 10−2

energy norm augmented norm N err. est. eff. err. est. eff. |||uh|||#,Fh 128 7.74e-3 1.10e-1 14 1.40e-1 3.28e-1 2.3 3.40e-2 512 4.03e-3 4.35e-2 11 3.97e-2 1.29e-1 3.3 1.16e-2 2048 1.88e-3 1.43e-2 7.6 9.77e-3 4.14e-2 4.2 2.72e-3 8192 9.30e-4 3.58e-3 3.8 2.98e-3 1.02e-2 3.4 8.25e-4

  • rder

1.0 2.0

  • 1.7

2.0

  • 1.7

Errors (|||u − uh||| and |||u − uh|||⊕′ + |||u − uh|||#,Fh), estimates (η and ˜ η + |||uh|||#,Fh), and effectivity indices for the energy and augmented norms; ǫ = 10−2

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-111
SLIDE 111

I Abstract framework A posteriori estimates C

  • Flux. rec.
  • En. norm
  • Aug. norm
  • Nonm. grids
  • Num. exp.

Convection-dominated problem, DG, energy and augmented estimates, ǫ = 10−4

energy norm augmented norm N err. est. eff. err. est. eff. |||uh|||#,Fh 128 1.70e-3 1.34e-1 79 3.67e-1 4.05e-1 1.10 4.02e-2 512 5.65e-4 7.01e-2 124 1.44e-1 2.11e-1 1.47 2.11e-2 2048 2.14e-4 3.09e-2 144 5.35e-2 9.36e-2 1.75 9.99e-3 8192 1.00e-4 1.25e-2 125 2.14e-2 3.89e-2 1.82 4.96e-3

  • rder

1.1 1.3

  • 1.3

1.3

  • 1.0

Errors (|||u − uh||| and |||u − uh|||⊕′ + |||u − uh|||#,Fh), estimates (η and ˜ η + |||uh|||#,Fh), and effectivity indices for the energy and augmented norms; ǫ = 10−4

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-112
SLIDE 112

I Abstract framework A posteriori estimates C

Outline

1

Introduction and motivation

2

Abstract framework Optimal energy norm abstract framework A first computable estimate Optimal augmented norm abstract framework

3

A posteriori error estimates Flux reconstructions Energy norm error estimates Augmented norm error estimates Nonmatching grids Numerical experiments

4

Concluding remarks and future work

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-113
SLIDE 113

I Abstract framework A posteriori estimates C

Comments on the estimates and their efficiency

General comments u ∈ H1(Ω), no additional regularity no saturation assumption no Helmholtz decomposition no shape-regularity and polynomial data needed for the upper bounds (only for the efficiency proofs) the only important tools: Cauchy–Schwarz and optimal Poincaré–Friedrichs and trace inequalities based on local conservativity (no global Galerkin

  • rthogonality used)
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-114
SLIDE 114

I Abstract framework A posteriori estimates C

Comments on the estimates and their efficiency

General comments u ∈ H1(Ω), no additional regularity no saturation assumption no Helmholtz decomposition no shape-regularity and polynomial data needed for the upper bounds (only for the efficiency proofs) the only important tools: Cauchy–Schwarz and optimal Poincaré–Friedrichs and trace inequalities based on local conservativity (no global Galerkin

  • rthogonality used)
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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I Abstract framework A posteriori estimates C

Comments on the estimates and their efficiency

General comments u ∈ H1(Ω), no additional regularity no saturation assumption no Helmholtz decomposition no shape-regularity and polynomial data needed for the upper bounds (only for the efficiency proofs) the only important tools: Cauchy–Schwarz and optimal Poincaré–Friedrichs and trace inequalities based on local conservativity (no global Galerkin

  • rthogonality used)
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-116
SLIDE 116

I Abstract framework A posteriori estimates C

Comments on the estimates and their efficiency

General comments u ∈ H1(Ω), no additional regularity no saturation assumption no Helmholtz decomposition no shape-regularity and polynomial data needed for the upper bounds (only for the efficiency proofs) the only important tools: Cauchy–Schwarz and optimal Poincaré–Friedrichs and trace inequalities based on local conservativity (no global Galerkin

  • rthogonality used)
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-117
SLIDE 117

I Abstract framework A posteriori estimates C

Comments on the estimates and their efficiency

General comments u ∈ H1(Ω), no additional regularity no saturation assumption no Helmholtz decomposition no shape-regularity and polynomial data needed for the upper bounds (only for the efficiency proofs) the only important tools: Cauchy–Schwarz and optimal Poincaré–Friedrichs and trace inequalities based on local conservativity (no global Galerkin

  • rthogonality used)
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-118
SLIDE 118

I Abstract framework A posteriori estimates C

Comments on the estimates and their efficiency

General comments u ∈ H1(Ω), no additional regularity no saturation assumption no Helmholtz decomposition no shape-regularity and polynomial data needed for the upper bounds (only for the efficiency proofs) the only important tools: Cauchy–Schwarz and optimal Poincaré–Friedrichs and trace inequalities based on local conservativity (no global Galerkin

  • rthogonality used)
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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I Abstract framework A posteriori estimates C

Essentials of the estimates

Essentials of the estimates nonconformity estimate: compare the approximate solution uh to a H1(Ω)-conforming potential sh diffusive flux estimate: compare the flux of the approximate solution −K∇uh to a H(div, Ω)-conforming flux th evaluate the residue for th use the local conservativity to get the local cutoff functions use the augmented norm

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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I Abstract framework A posteriori estimates C

Essentials of the estimates

Essentials of the estimates nonconformity estimate: compare the approximate solution uh to a H1(Ω)-conforming potential sh diffusive flux estimate: compare the flux of the approximate solution −K∇uh to a H(div, Ω)-conforming flux th evaluate the residue for th use the local conservativity to get the local cutoff functions use the augmented norm

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-121
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I Abstract framework A posteriori estimates C

Essentials of the estimates

Essentials of the estimates nonconformity estimate: compare the approximate solution uh to a H1(Ω)-conforming potential sh diffusive flux estimate: compare the flux of the approximate solution −K∇uh to a H(div, Ω)-conforming flux th evaluate the residue for th use the local conservativity to get the local cutoff functions use the augmented norm

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-122
SLIDE 122

I Abstract framework A posteriori estimates C

Essentials of the estimates

Essentials of the estimates nonconformity estimate: compare the approximate solution uh to a H1(Ω)-conforming potential sh diffusive flux estimate: compare the flux of the approximate solution −K∇uh to a H(div, Ω)-conforming flux th evaluate the residue for th use the local conservativity to get the local cutoff functions use the augmented norm

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

slide-123
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I Abstract framework A posteriori estimates C

Essentials of the estimates

Essentials of the estimates nonconformity estimate: compare the approximate solution uh to a H1(Ω)-conforming potential sh diffusive flux estimate: compare the flux of the approximate solution −K∇uh to a H(div, Ω)-conforming flux th evaluate the residue for th use the local conservativity to get the local cutoff functions use the augmented norm

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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Conclusions

Conclusions guaranteed, locally efficient, and robust a posteriori error estimates directly and locally computable almost asymptotically exact

  • ptimal framework (exact and robust)

works for all major numerical schemes (FDs, FVs, FEs, NCFEs, MFEs) based on local conservativity

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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Open questions and future work

Open questions are the energy/augmented norms optimal? can a robust estimate without the jump seminorm be

  • btained?

can a robust estimate in the energy norm be obtained? Future work nonlinear (degenerate) cases multi-scale, multi-numerics, multi-physics, mortars estimates of quantities of interest

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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I Abstract framework A posteriori estimates C

Open questions and future work

Open questions are the energy/augmented norms optimal? can a robust estimate without the jump seminorm be

  • btained?

can a robust estimate in the energy norm be obtained? Future work nonlinear (degenerate) cases multi-scale, multi-numerics, multi-physics, mortars estimates of quantities of interest

  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems

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I Abstract framework A posteriori estimates C

Bibliography

Bibliography

ERN A., STEPHANSEN, A. F., VOHRALÍK M., Guaranteed and robust discontinuous Galerkin a posteriori error estimates for convection–diffusion–reaction problems, submitted to M3AS, http://hal.archives-ouvertes.fr/hal-00193540/. ERN A., STEPHANSEN, A. F., A posteriori energy-norm error estimates for advection-diffusion equations approximated by weighted interior penalty methods, J. Comp. Math. 26 (2008), 488–510. VOHRALÍK M., A posteriori error estimates for lowest-order mixed finite element discretizations of convection–diffusion–reaction equations, SIAM J. Numer. Anal. 45 (2007), 1570–1599. VOHRALÍK M., Residual flux-based a posteriori error estimates for finite volume and related locally conservative methods,

  • Numer. Math. 111 (2008), 121–158.
  • A. Ern, A. F. Stephansen & M. Vohralík

Guaranteed and robust estimates for DG and CRD problems