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1 A multigrid method for the design of heterogeneous material in tribology Hugo Boffy – Kees Venner Tribodays 2013

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Page 1: A multigrid method for the design of heterogeneous .../file/Boffy_lulea.pdf · A multigrid method for the design of heterogeneous material in tribology . Hugo Boffy – Kees Venner

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A multigrid method for the design of heterogeneous material in tribology

Hugo Boffy – Kees Venner

Tribodays 2013

Page 2: A multigrid method for the design of heterogeneous .../file/Boffy_lulea.pdf · A multigrid method for the design of heterogeneous material in tribology . Hugo Boffy – Kees Venner

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Context

- Reduction of the industrial costs and green policy are daily problems

- Higher level of stresses - improvement of performances

and fatigue life - Focus on interfaces between elements

- Advanced numerical methods are required

- Analysis performed by engineers to provide innovative and

efficient solutions (materials) !

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Objectives

- Modelling of homogeneous and heterogeneous materials - Be able to deal with low and high property ratios

- Provide accurate solutions in local area/volume

- Fast solution to have low turn around time of computations

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Perform 3D simulations involving millions DoF

Be able to get accurate solutions at low numerical costs

Fiber reinforced composite

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Outline

- 3D numerical tool - Multigrid method - Advanced numerical tools for heterogeneous material design - Applications - Conclusion

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3D numerical tool

Lame's equations - 3 PDE - λ, μ: Lame's coefficients depend of material properties : (E, ν) = f(x,y,z) - ui: displacements along x, y and z (unknowns) - Both Neumann and Dirichlet boundary conditions can be imposed

(λuj, j),i + (μui, j),j + (μuj, i),j = 0 i,j=1,2,3

x y

z

ui(x,y,z)

σ(x,y)

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Page 6: A multigrid method for the design of heterogeneous .../file/Boffy_lulea.pdf · A multigrid method for the design of heterogeneous material in tribology . Hugo Boffy – Kees Venner

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How to solve the equations: finite difference method

Lame's equations can be written as a system of equations: Lh<u>i,j,k - The discrete operator Lh uses a second order scheme - Residual: rh

i,j,k = fhi,j,k – Lh <uh>i,j,k - Converged solution: rh

i,j,k = 0 for all point M[i,j,k] in the computation domain - Iterative solver: adjust solution point by point such that the residual is reduced or eliminated. - Sweep across all points: relaxation (Gauss-Seidel).

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Multilevel method

- Highest level should represent solution with the desired accuracy. - Lower levels are a means to accelerate the convergence speed. The solution

and the residuals are transferred between the different level of grids. - Components with a low frequency relative to a fine grid have a high frequency

relative to a coarse grid.

level i level i-1 level i+1

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Page 8: A multigrid method for the design of heterogeneous .../file/Boffy_lulea.pdf · A multigrid method for the design of heterogeneous material in tribology . Hugo Boffy – Kees Venner

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A common multilevel schedule

time

Final solution

= relax = interpolate = restrict

finest grid k*k*k

k/2*k/2*k/2

coarsest grid

Full Multigrid cycle

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Local refinement strategy

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[1] Bai, D., Brandt, A. Local Mesh Refinement Multilevel Techniques. SIAM J. Sci. Comput. Vol 8. 1987

- Be able to realize very precise local calculations:

- Advantages:

Reduction of memory cost Reduction of CPU time Increase of the number of levels Higher accuracy in the refined volume - Convergence speed of the algorithm not affected [1]

Global strategy: 3 levels

Local strategy: 2 refined levels

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Polycrystalline media [1]

- Heterogeneous structure: 4000 grains (Voronoi tessellation) Gaussian distribution of the properties Grain size and shape controlled by the algorithm - Numerical modeling : Top surface : Hertzian pressure (a0,P0) Bulk size [8a0,8a0,4a0] Meshing : 5 global levels - 3 local levels Polycrystalline behavior restrain on Ω8 Number of points : 11.106 CPU time : 15-20 minutes

Gaussian distribution of E

x

z

y

[1] Boffy, H., Baietto, M. C., Lubrecht, A. A. and Sainsot, P. Technique multigrilles et raffinement pour un modèle 3D efficace de milieux

hétérogènes sous sollicitations de contact. 2012.

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Polycrystalline media

Computation of the Von-Mises stresses

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Inclusions in an homogeneous media

- Presence of 2 inclusions in an homogeneous media (E, ν):

- Inclusion 1 size: R1=0.05 mechanical properties: E1=0.01E ,ν1=ν

- Inclusion 2

size: R2=0.1 mechanical properties: E1=5E ,ν1=ν

- Numerical modeling : Top surface : Hertzian pressure (a0,P0) Bulk size [8a0,8a0,4a0] Meshing : 5 global levels - 3 local levels Number of points : 11.106 CPU time : 15 minutes

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x

z

y

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Application: spherical hole in an homogeneous material

- Homogeneous material (E, ν) with a

spherical void (Ev/E=1/1000) - Bulk size: [0.1;0.1;0.1]

- Mesh: [257;257;257] - BC : Hertzian pressure top surface

Zero displacements bottom Free other boundaries

- CPU time < 10 min - Principal stress σ1 in the plan (x,y=0,z)

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Hard fibers in an infinite matrix

- Two coated copper fibers

inside an epoxy matrix. - Soft and hard interphases are

considered - Bulk size: [0.1;0.1;0.1] - Mesh: [513;513;513] - BC: vertical displacement w0

imposed on top and bottom surfaces

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Hard fibers in an infinite matrix

- Iso-values of the principal stress σ1 - Effect of the interlayer on the stress field highlighted: Location and intensity of the maxima (σ1max=1.13 | 0.68) Discontinuity of the stress field

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Fiber reinforced material

- Oriented cylinders in a matrix - Horizontal fiber planes -Bulk size: [0.1;0.1;0.1] -Mesh: [513;513;513] - Boundary conditions: Vertical displacement on the top surface: w0 Zero displacements on the bottom Free other boundaries

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Fiber reinforced material

- Aligned fibers (Ө1,2=0) - Effect of the density of the fibers : stress path (tensile stress)

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mikado

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Fiber reinforced material

- Oriented fibers (Ө2=π/2) – (Ө1,2=±π/5) - Effect of the density and orientation of the fibers : different stress path

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mikado

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Conclusion

- Development of a fast efficient solver to deal with 3D elastic problems involving strongly heterogeneous materials

- Ability to consider hundred millions DoF in order to take into account

small scale variations in great detail - Fast calculations on a PC allowing parametric studies at different scales

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Page 20: A multigrid method for the design of heterogeneous .../file/Boffy_lulea.pdf · A multigrid method for the design of heterogeneous material in tribology . Hugo Boffy – Kees Venner

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Prospects

- Consider other types of heterogeneous materials - Take into account the material anisotropy - Design new materials

- Create a path between macro/micro

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contact roughness coatings microstructure

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Acknowledgement

- Thanks to:

Dutch technology foundation (STW) Dutch fundamental research foundation (FOM)

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Thank you for your attention Questions ?

Hugo Boffy – Kees Venner

Tribodays 2013