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Software – centered approach to the simulation of thin porous media and their properties D A d Wi Dr. Andreas Wiegmann , Dr. Jürgen Becker, Dr. Liping Cheng, Dr. Erik Glatt and Dr. Stefan Rief. Fraunhofer-Institut Techno- und Wirtschaftsmathematik, Kaiserslautern 2011 Bordeaux, Wiegmann 3/30/11

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Page 1: Software – centered approach to the simulation of thin ... · ti d f th i time and money for their matil l i til terial analysis, material developments and product developments

Software – centered approach to the simulation of thin porous media and their propertiesp p p

D A d Wi Dr. Andreas Wiegmann, Dr. Jürgen Becker, Dr. Liping Cheng, Dr. Erik Glatt and Dr. Stefan Rief.

Fraunhofer-InstitutTechno- und Wirtschaftsmathematik, Kaiserslautern

© Fraunhofer ITWM1

2011 Bordeaux, Wiegmann 3/30/11

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Outline

GeoDict in general

Thin porous Media Thin porous Media

Material propertiesp p

GeoDict: Software for

Virtual Material Design

© Fraunhofer ITWM2

2011 Bordeaux, Wiegmann 3/30/11

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Computer Aided Material Engineering

T hPorous Media

or Composite CT Image Model

image

Lab Tomograph

filter &segment

Composite Material

g

generate

Voxel Mesh

measureManufacturenext sample

Try next parameter

set

P i

compute

P i

design

PropertiesProperties

© Fraunhofer ITWM3

2011 Bordeaux, Wiegmann 3/30/11

next sample

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Modules

- FiberGeo, SinterGeo, WeaveGeo, GridGeo, PackGeo, PaperGeo, PleatGeo,

- DpfGeo, LungGeo , UserGeo , GadGeo (structure generators)

- ProcessGeo (3d image processing)

- LayerGeo (layered media)

- ImportGeo (e.g. tomography, STL, .gad)

- ExportGeo (e.g. Fluent, Abaqus)

- FlowDict (single phase flow properties)

- PleatDict (porous media flow)

- ElastoDict (effective elastic properties)

- ConductoDict (effective conductivity)

- DiffuDict (effective diffusivity)

- FilterDict (pressure drop, efficiency, capacity)

S t Di t (t h fl ti )- SatuDict (two phase flow properties)

- PoroDict (pore size measures)

- AcoustoDict (acoustic absorption)

GadDict (Analysis and export of analytic descriptions)

© Fraunhofer ITWM4

2011 Bordeaux, Wiegmann 3/30/11

- GadDict (Analysis and export of analytic descriptions)

Page 5: Software – centered approach to the simulation of thin ... · ti d f th i time and money for their matil l i til terial analysis, material developments and product developments

Modules

- FiberGeo, SinterGeo, WeaveGeo, GridGeo, PackGeo, PaperGeo, PleatGeo,

- DpfGeo, LungGeo , UserGeo , GadGeo (structure generators)

- ProcessGeo (3d image processing)Every structure - LayerGeo (layered media)

- ImportGeo (e.g. tomography, STL, .gad)

- ExportGeo (e.g. Fluent, Abaqus)

Every structure • tomogram or

- FlowDict (single phase flow properties)

- PleatDict (porous media flow)

- ElastoDict (effective elastic properties)

g• generated

- ConductoDict (effective conductivity)

- DiffuDict (effective diffusivity)

- FilterDict (pressure drop, efficiency, capacity)

S t Di t (t h fl ti )

is compatible with every t i l ti !- SatuDict (two phase flow properties)

- PoroDict (pore size measures)

- AcoustoDict (acoustic absorption)

GadDict (Analysis and export of analytic descriptions)

property simulation!

© Fraunhofer ITWM5

2011 Bordeaux, Wiegmann 3/30/11

- GadDict (Analysis and export of analytic descriptions)

Page 6: Software – centered approach to the simulation of thin ... · ti d f th i time and money for their matil l i til terial analysis, material developments and product developments

Outline

GeoDict in general

Thin porous Media Thin porous Media

Material propertiesp p

GeoDict: Software for

Virtual Material Design

© Fraunhofer ITWM7

2011 Bordeaux, Wiegmann 3/30/11

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Scanning Electron Microscopy,photo & tomogram of thin porous mediaphoto & tomogram of thin porous media

Gas Diffusion Layer, Micro Porous Layer, Metal wire mesh and Cellulose mediaMetal wire mesh and Cellulose media

© Fraunhofer ITWM8

2011 Bordeaux, Wiegmann 3/30/11

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3d structure idea

Two sources: 1) t h i ( t ti ) 2) i t ll t d 1) tomography image (segmentation) 2) virtually generated

(stochastic geometry)

all structure models:cubic voxels (voxel = volume celll)

© Fraunhofer ITWM9

2011 Bordeaux, Wiegmann 3/30/11

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3D Models: Gas Diffusion Layer (GDL)Gas Diffusion Layer (GDL)

Typically: nonwoven fibre structures plus binder Typically: nonwoven fibre structures plus binder

Input:• Porosity

Fib di t d t• Fibre diameter and type• Anisotropy• (Weight% binder)• (Fibre crimp)( p)

© Fraunhofer ITWM10

2011 Bordeaux, Wiegmann 3/30/11

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3D Models:Microporous Layer (MPL)Microporous Layer (MPL)

Typically: carbon agglomerates Typically: carbon agglomerates

Input:• Particle size

P ti l A l t• Particles per Agglomerate• Porosity

Becker, Wieser, Fell, Steiner, 2011, to appear

© Fraunhofer ITWM11

2011 Bordeaux, Wiegmann 3/30/11

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3D M d l3D Models:Catalyst Layer (CL)

Carbon agglomerates plus elektrolyte Carbon agglomerates plus elektrolyte

Elekt. d

Elekt. b t

Elekt. d surrounds

C. Partikelsbetween C. Partikels

surrounds C. Partikels but not in between

© Fraunhofer ITWM12

2011 Bordeaux, Wiegmann 3/30/11

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3D Models: Catalyst Layer (CL)

Model example:

Porosity 33.3 % Carbon/Pt 50.1 vol% Elektrolyte 16.6 vol%y

Size: (800 nm)³, voxel length 1 nm

© Fraunhofer ITWM13

2011 Bordeaux, Wiegmann 3/30/11

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GDL model(fuel cell)

Emz mpg

3D Visualization (generated) SEM (real) (courtesy of Jeff Gostick, Univ. of Waterloo)

V P Schulz P P Mukherjee J Becker A Wiegmann and C Y Wang Modeling of Two

Emz.mpg

© Fraunhofer ITWM14

2011 Bordeaux, Wiegmann 3/30/11

V.P. Schulz, P.P. Mukherjee, J. Becker, A. Wiegmann and C.Y. Wang, Modeling of Two-phase Behavior in the Gas Diffusion Medium of Polymer Electrolyte Fuel Cells via Full Morphology Approach, Journal of the ECS, Issue 4, Vol. 154, 2007, pp B419-B426.

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Pipeline model (Oil & Gas)

Photo: M. Knefel Gebrüder Kufferath, Düren, Modell: E. Glatt, Fraunhofer ITWM, with GeoDict

© Fraunhofer ITWM15

2011 Bordeaux, Wiegmann 3/30/11

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Nonwoven model

Homogeneous Tomogram InhomogeneousHomogeneous Tomogram Inhomogeneous

© Fraunhofer ITWM16

2011 Bordeaux, Wiegmann 3/30/11

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Outline

GeoDict in general

Thin porous Media Thin porous Media

Material propertiesp p

GeoDict: Software for

Virtual Material Design

© Fraunhofer ITWM17

2011 Bordeaux, Wiegmann 3/30/11

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Determination ofEffective PropertiesEffective Properties

1. Start with a 3D voxel structure given1. Start with a 3D voxel structure given

2. Find effective properties based on the geometrical structurea) Geometrical properties:

i di t ib ti h l f • pore size distribution, pore morphology, surface areab) Transport properties:

i. Solve PDE on the voxel gridii. Find effective property by upscaling / averagingp p y y p g g g

3d Image is the computational gridGrid from μCT by segmentationGrid for models by discretization (vCT)Grid for models by discretization (vCT)Memory: factor 30 over FluentRun-time: FFT-methods possibleSimple visualization: structure, solution

© Fraunhofer ITWM18

2011 Bordeaux, Wiegmann 3/30/11

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Geometric analysis

Connectivity

Pore size distribution

TortuosityTortuosity

Anisotropy

Specific surface area

Triple linesTriple lines

Etc. etc

© Fraunhofer ITWM19

2011 Bordeaux, Wiegmann 3/30/11

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Cross section of resin-embedded fleece in planeresin embedded fleece, in plane

In plane,1,1mm x 1,1mmmagnification: 10xmagnification: 10x

© Fraunhofer ITWM20

2011 Bordeaux, Wiegmann 3/30/11

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Cross section of resin-embedded fleece in planeresin embedded fleece, in plane

In plane,1,1mm x 1,1mmmagnification: 10xmagnification: 10x

© Fraunhofer ITWM21

2011 Bordeaux, Wiegmann 3/30/11

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Cross section of resin-embedded fleece in planeresin embedded fleece, in plane

In plane,1,1mm x 1,1mmmagnification: 10xmagnification: 10x

© Fraunhofer ITWM22

2011 Bordeaux, Wiegmann 3/30/11

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Cross section of resin-embedded fleece through planeresin embedded fleece, through plane

Through plane,1,1mm x 1,1mmmagnification: 10xmagnification: 10x

© Fraunhofer ITWM23

2011 Bordeaux, Wiegmann 3/30/11

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Cross section of resin-embedded fleece through planeresin embedded fleece, through plane

Through plane,1,1mm x 1,1mmmagnification: 10xmagnification: 10x

© Fraunhofer ITWM24

2011 Bordeaux, Wiegmann 3/30/11

Page 24: Software – centered approach to the simulation of thin ... · ti d f th i time and money for their matil l i til terial analysis, material developments and product developments

Cross section of resin-embedded fleece through planeresin embedded fleece, through plane

Through plane,1,1mm x 1,1mmmagnification: 10xmagnification: 10x

© Fraunhofer ITWM25

2011 Bordeaux, Wiegmann 3/30/11

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Estimation of the anisotropy:

Can estimate the anisotropy from pythe number of connected white components in the images

Use 5 images each:IP: 35, 36, 48, 79, 61 -- 52TP 164 144 158 170 168 161TP: 164, 144, 158, 170, 168 -- 161

find ß ~4,1 for the original (uncompressed) fleece., g ( p )

© Fraunhofer ITWM26

2011 Bordeaux, Wiegmann 3/30/11

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Effective diffusivity

Macroscopic description (homogenized porous media model)

Fick's first law: c=1 Fick s first law:

D* : effective diffusivity [m²/s] unknown j : diffusion flux [mol/m²/s] i [ l/ ³]

c 1

c : concentration [mol/m³]

Microscopic description(pore structure model)(pore structure model)

Laplace equation:

Boundary conditions: no-flux on fibre f t ti d

c=0

surface, concentration drop

D* can be determined from the solution!

© Fraunhofer ITWM27

2011 Bordeaux, Wiegmann 3/30/11

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Validation:Toray TGP H 060 Gas Diffusion LayerToray TGP H 060 Gas Diffusion Layer

Data from PSI:• Tomography images of Toray TGP H 060 at different compression

levels• Diffusivity, permeability and conductivity were measured at

different compression levels experimentally

Now: compute diffusivity, permeability and conductivity numerically and compare results

Becker, Flückiger, Reum, Büchi, Marone, Stampanoni, 2009, J. Electrochem. Soc. 156

© Fraunhofer ITWM28

2011 Bordeaux, Wiegmann 3/30/11

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Diffusivity

Perfect in tp directionPerfect in tp-direction

Small differences in ip-direction

1. ip-measurememts performed on a stack of GDLsof GDLs

2. tomography image shows single layer between sample h ldholder

© Fraunhofer ITWM29

2011 Bordeaux, Wiegmann 3/30/11

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Permeability

Perfect in tp directionPerfect in tp-direction

Small differences in ip-direction

1. ip-measurememts performed on a stack of GDLsGDLs

2. tomography image shows single layer between sample holder

© Fraunhofer ITWM30

2011 Bordeaux, Wiegmann 3/30/11

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Electric Conductivity

Tp conductivity too high!Tp-conductivity too high!

Reason: model assumes a perfect contact between the fibres (and the binder)

© Fraunhofer ITWM31

2011 Bordeaux, Wiegmann 3/30/11

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Pipeline model

Pressure drop Pressure drop evolution

Sand particles filtration

Mesh abrasion by sand particlessand particles

Flow simulations and Visualizations: M. Knefel, Gebrüder Kufferath, Düren, using GeoDict and built-in ParPac Lattice-Boltzmann solver

© Fraunhofer ITWM32

2011 Bordeaux, Wiegmann 3/30/11

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Filtration: Cake formation

Filter Efficiency Filter Efficiency evolution

Pressure drop evolution

© Fraunhofer ITWM33

2011 Bordeaux, Wiegmann 3/30/11

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Bubble point

Pressure at which break through occurs

© Fraunhofer ITWM34

2011 Bordeaux, Wiegmann 3/30/11

Page 34: Software – centered approach to the simulation of thin ... · ti d f th i time and money for their matil l i til terial analysis, material developments and product developments

Outline

GeoDict in general

Thin porous Media Thin porous Media

Material propertiesp p

GeoDict: Software for

Virtual Material Design

© Fraunhofer ITWM35

2011 Bordeaux, Wiegmann 3/30/11

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Pre-processing:Import & Structure GenerationImport & Structure Generation

Import + segmentationImport + segmentationor structure generation both yield segmented 3d image

Input parameters are measurables like porosity, fiber orientation, fiber diameter distributiondistribution

Randomness reproducible via random seeds

© Fraunhofer ITWM36

2011 Bordeaux, Wiegmann 3/30/11

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Solve: Standardized Property ComputationProperty Computation

For any pde the solver For any pde, the solver options always have similar options and meaning

The results are available as detailed solution and solution and aggregated into effective properties like diffusivity, filter

ffi i tefficiency, etc.

© Fraunhofer ITWM37

2011 Bordeaux, Wiegmann 3/30/11

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Postprocessing:Visualization Animation Dexcel & MATLABVisualization, Animation, Dexcel & MATLAB

Structures and result fields can be Structures and result fields can be visualized and animated in 2d and 3d, as slices, virtual REM or vCT

Analysis available in Excel or MATLAB All operations are scriptable /

reproducible Software runs in Linux and Windows All codes use common framework 3d All codes use common framework 3d

structure classes, settings classes, etc. etc.

All i ti / i li ti d All animations / visualizations done with GeoDict

© Fraunhofer ITWM38

2011 Bordeaux, Wiegmann 3/30/11

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Contributors: 2001 - 2011DiffuDict Knudsen Solver SinterGeoFilterDictGeoDict DiffuDict Knudsen Solver

Jürgen Becker

ElastoDictHeiko Andrä

Dimiter Stoyanov

SinterGeoJürgen BeckerNorman EttrichKilian Schmidt

PleatGeo

FilterDictStefan RiefArnulf Latz

Andreas WiegmannKilian Schmidt

Christian Wagner

GeoDictAndreas Wiegmann

Jürgen BeckerErik Glatt

Stefan RiefHeiko Andrä

Inga ShklyaerAndreas Wiegmann

Vita RutkaDonatas Elvikis

FlowDict EFV Solver

Erik GlattAndreas Wiegmann

Jürgen Becker

PackGeoErik Glatt

Rolf Westerteiger

ThermoDict EJ SolverAndreas Wiegmann

Liping Cheng

Sven LindenKilian Schmidt

Ashok Kumar VaikuntamRolf WesterteigerChristian WagnerMohammed Alam FlowDict EFV Solver

Andreas WiegmannLiping Cheng

FiberGeoJürgen Becker

Erik GlattAndreas Wiegmann

Joachim Seibt

GridGeoErik Glatt

FlowDict Lattice BoltzmannPeter KleinDirk Merten

Konrad SteinerDirk Kehrwald

Mohammed AlamJianping Shen

UsersGuideBarbara Planas

Stefan RiefAndreas Wiegmann

Katja SchladitzJoachim Ohser

Hans-Karl HummelPetra Baumann

Liping ChengAndreas WiegmannRolf Westerteiger

RenderGeoMatthias Groß

Irina GinzburgDoris Reinel-Bitzer

FlowDict EJ SolverLiping Cheng

Andreas Wiegmann

Andreas Wiegmann

PoroDictAndreas Wiegmann

Jürgen BeckerKilian Schmidt

WeaveGeoErik Glatt

Andreas WiegmannRolf Westerteiger

Matthias GroßSven Linden

Carsten LojewskiRolf Westerteiger

PaperGeo

Andreas WiegmannAivars ZemitisDonatas Elvikis

Vita RutkaQing Zhang

Kilian SchmidtRolf Westerteiger

PleatDictAndreas Wiegmann

Oleg Iliev

© Fraunhofer ITWM39

2011 Bordeaux, Wiegmann 3/30/11

Erik GlattSatuDictJürgen Becker

Andreas WiegmannVolker Schulz

Rolf Westerteiger

Stefan Rief

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Fi d Find out more:

www geodict comwww.geodict.comwww.itwm.fhg.deglive demo outsidelive demo outside

© Fraunhofer ITWM40

2011 Bordeaux, Wiegmann 3/30/11

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GeoDict Mission

To help our industrial partners reduce R&D cost in terms of ti d f th i t i l l i t i l time and money for their material analysis, material developments and product developments.

To save our academic partners time to focus on research To save our academic partners time to focus on research in their own discipline and not on the details of Mathematics or Computer Science.

To minimize the need for real experiments by providing software. GeoDict performs standardized computer simulations yielding results on tomograms and model simulations yielding results on tomograms and model structures that are directly comparable to experiments.

© Fraunhofer ITWM41

2011 Bordeaux, Wiegmann 3/30/11