the extended finite element method for boundary layers€¦ · the extended finite element method...
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![Page 1: The Extended Finite Element Method for Boundary Layers€¦ · The Extended Finite Element Method for Boundary Layers Alaskar Alizada, Thomas-Peter Fries Research group: “Numerical](https://reader030.vdocuments.mx/reader030/viewer/2022041105/5f073b6c7e708231d41bf784/html5/thumbnails/1.jpg)
The Extended Finite Element Methodfor Boundary Layers
Alaskar Alizada, Thomas-Peter Fries
Research group: “Numerical methods for discontinuities“
WCCM8, Venice, 30 June - 4 July, 2008
Chair for Computational Analysisof Technical Systems
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Alaskar Alizada The XFEM for Boundary Layers Slide: 2
Overview
Motivation
XFEM for Boundary Layers in 1D
XFEM for Boundary Layers in 2D
Conclusions & Outlook
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Alaskar Alizada The XFEM for Boundary Layers Slide: 3
Motivation
Boundary Layers:
occur in advection-diffusion problems such as flows.
are characterised by high gradients normal to the wall.
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Alaskar Alizada The XFEM for Boundary Layers Slide: 4
Motivation
Numerical methods for Boundary Layers:
FEM- refined mesh near the wall many new elements new DoF
Find appropriate enrichment functions for BL
XFEM- adjust the approximation space,
but does not manipulate the mesh
![Page 5: The Extended Finite Element Method for Boundary Layers€¦ · The Extended Finite Element Method for Boundary Layers Alaskar Alizada, Thomas-Peter Fries Research group: “Numerical](https://reader030.vdocuments.mx/reader030/viewer/2022041105/5f073b6c7e708231d41bf784/html5/thumbnails/5.jpg)
Alaskar Alizada The XFEM for Boundary Layers Slide: 5
XFEM for BL in 1D
Model problem: Advection-diffusion problem
advection diffusion
The exact solution has the form:
10
1
c=0
c modera
te
c large
Boundary Layer
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Alaskar Alizada The XFEM for Boundary Layers Slide: 6
XFEM for BL in 1D
The standard XFEM approximation:
Enrichment functions are sought such that for all ratios:- high accuracy is obtained- no oscillations occur- the approximation space remains sufficiently linearly
independent
enrichment 1 enrichment 2
Enrichment functions should be defined locally near thewall and independent of and coefficients
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Alaskar Alizada The XFEM for Boundary Layers Slide: 7
XFEM for BL in 1D
This family of enrichment functions is found useful:
where scales the gradient and
at the wallwithin layers from the wall
else
The pair ( , ) defines each
wall
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Alaskar Alizada The XFEM for Boundary Layers Slide: 8
XFEM for BL in 1D
Using only one enrichment function is not sufficient tocover the whole range of ratios without oscillations
The „optimal“ set of enrichment functions under thechoosen criteria is:
50
15
12
10
1
1
23
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Alaskar Alizada The XFEM for Boundary Layers Slide: 9
c=1
c=20
c=40
XFEM for BL in 1DL2 Norm for XFEM and FEM approximations
10 640 elements
1.e-6
1.e-1L2Norm
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Alaskar Alizada The XFEM for Boundary Layers Slide: 10
XFEM for BL in 1D Max. oscillations of XFEM and FEM approximations
FEM, 10 elements
FEM, 40 elements
FEM, 160 elements
No oscillations for XFEM occur
1 500c coefficient
0
-2.5
osci
llatio
ns
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Alaskar Alizada The XFEM for Boundary Layers Slide: 11
XFEM for BL in 1D
Summary
High accuracy is obtained
No oscillations occur
The approximation space is linearly independent
The enrichment functions are locally defined and areindependent of the problem coefficients
For the proposed set of 4 enrichment functions:
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Alaskar Alizada The XFEM for Boundary Layers Slide: 12
XFEM for BL in 2D
Model problem: Advection-diffusion problem
advection diffusion
The exact solution has the form:
![Page 13: The Extended Finite Element Method for Boundary Layers€¦ · The Extended Finite Element Method for Boundary Layers Alaskar Alizada, Thomas-Peter Fries Research group: “Numerical](https://reader030.vdocuments.mx/reader030/viewer/2022041105/5f073b6c7e708231d41bf784/html5/thumbnails/13.jpg)
Alaskar Alizada The XFEM for Boundary Layers Slide: 13
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Alaskar Alizada The XFEM for Boundary Layers Slide: 14
XFEM for BL in 2D
A similar set of enrichment functions is taken as for 1D:
where scales the gradient and :
- is constructed by FE-shape functions
- is characteristic for the wall-distance
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Alaskar Alizada The XFEM for Boundary Layers Slide: 15
XFEM for BL in 2D
The 1D set of enrichment functions ist straightforward extended to 2D with the same pairs ( , ):
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Alaskar Alizada The XFEM for Boundary Layers Slide: 16
c=5
c=20
c=100
XFEM for BL in 2DL2 Norm for XFEM and FEM approximations ( )
10 300 elements
1.e-5
1.e+1L2Norm
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Alaskar Alizada The XFEM for Boundary Layers Slide: 17
XFEM for BL in 2DMax.oscillations of XFEM and FEM approximations
FEM, 10 elements
FEM, 20 elements
FEM, 30 elements
No oscillations for XFEM occur
5 100c coefficient
0
-0.8
osci
llatio
ns
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Alaskar Alizada The XFEM for Boundary Layers Slide: 18
Conclusions
A set of enrichment functions for XFEM is proposed that:
captures arbitrary high gradients normal to the wall
captures moderate changes of the solution tangential to the wall
captures the properties of boundary layers without increasingthe DoF´s significantly
Using proposed enrichment functions in the XFEM,no mesh refinement for boundary layers is required.
This idea is going to be extended to fluid problems,starting with driven cavity at high Reynolds-numbers.
Outlook
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Alaskar Alizada The XFEM for Boundary Layers Slide: 19
THANK YOUFOR YOUR
ATTENTION !