1 Micromechanics using Spectral Method Interface Decohesion in - - PowerPoint PPT Presentation

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1 Micromechanics using Spectral Method Interface Decohesion in - - PowerPoint PPT Presentation

1 Micromechanics using Spectral Method Interface Decohesion in Polycrystals L. Sha harma, P. Shanthraj, M.Diehl, F. Roters, D. Raabe, R. Peerlings and M. Geers Ou Outline line Motivation DAMASK- material simulation kit The


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SLIDE 1

1

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SLIDE 2

Micromechanics using Spectral Method

Interface Decohesion in Polycrystals

  • L. Sha

harma, P. Shanthraj, M.Diehl, F. Roters, D. Raabe,

  • R. Peerlings and M. Geers
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SLIDE 3

Ou Outline line

  • Motivation
  • DAMASK- material simulation kit
  • The Spectral Solver
  • Basic scheme
  • Some applications
  • Demo: a very simple (1D) implementation using petsc4py
  • Smeared damage mechanics
  • Interface decohesion in Polycrystals.
  • Future Work
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SLIDE 4

Mo Motiv tivation ation

  • strain localization
  • damage initiation
  • recrystallization nucleation
  • …
  • tool design
  • crashworthiness
  • component properties
  • …
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SLIDE 5

Mo Motiv tivation ation

5

http://www.virtualexplorer.com.au/special/meansvolume/contribs/jessell/labs/02a.m

  • v

Crystal Plasticity is always a multi-scale problem !

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SLIDE 6

Mo Motiv tivation ation

6

simulation requirements

  • arbitrary mechanical

boundary value problems

  • continuum mechanics
  • accounting for crystal

plasticity Crystal Plasticity Finite Elemente Method (CPFEM) Or Crystal Plasticity Spectral Method (CPFFT)

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SLIDE 7

CP CPFEM/ FEM/CPFFT CPFFT st strat rategy egy

7

M

material point model

𝐆 𝐐

solver for

  • equilibrium
  • compatibility

F P

deformation partitioning & homogenization crystallite elasto-plasticity

Fe

Lp S constitutive law

  • elasticity
  • plasticity
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SLIDE 8

Th The sp spectral tral so solv lver

8

  • Use spectral method instead of FEM
  • Solution based on FFT
  • Much faster than FEM
  • Small strain framework
  • Elastic material law
  • Extended to viscoplastic materials
  • Large strain formulation
  • Coupled with DAMASK

A little history

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SLIDE 9

Sp Spectral ctral me method hod

9

div 𝝉 = 0 Static equilibrium: Split strain: 𝜻 = 𝜻 + 𝜻 πœ»π‘›+1 = πœ»π‘› βˆ’ 𝜟 βˆ— 𝝉𝑛

FFT

Material law: 𝝉 = π‘«πœ» Introduce reference medium: Stiffness 𝑫 πœ»π‘›+1 = πœ»π‘› βˆ’ β„±βˆ’1 𝜟: 𝝉𝑛

with Ξ“π‘—π‘˜π‘™π‘š = π‘™π‘˜π‘™π‘š 𝑂𝑗𝑙 and 𝑂𝑗𝑙 = π‘™π‘šπ‘™π‘˜ π·π‘—π‘˜π‘™π‘š

βˆ’1

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SLIDE 10

Co Comp mparion arion FEM FEM vs vs FFT FFT

10

  • P. Eisenlohr., M. Diehl, R. A. Lebensohn, F. Roters: International Journal of Plasticity (2013), 37 - 53
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SLIDE 11

Ex Experim rimental ental-Numerical Numerical

11

Example: Basal slip in Magnesium

  • F. Wang, S. Sandloebes, M. Diehl, L. Sharma, F. Roters, D. Raabe:Acta Materialia 80 (2014) 77-93
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SLIDE 12

Me Mesosc

  • scale

ale me mechan hanics ics

12

  • High Resolution Crystal plasticity enabled through robust

spectral solvers Shanthraj et al. [IJP, 2015]

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SLIDE 13

Demo mo (1D elasticity + spectral method using petsc4py)

13

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SLIDE 14

Int nterface erface decoh

  • hesion

esion (form

  • rmab

ability ility li limi miter) er)

14

Void Initiation Role e of th the e Int nter erfa face ces Sur urroun

  • undin

ding Microst

  • stru

ructur ture

?

Void Growth/Propagation Compu puta tati tion

  • nal to

tool to to model Inte terfa face ce decohesion ion

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SLIDE 15

Int nterface erface mo modeli ling ng of

  • f pol
  • lycrystals

crystals

15

Interface elements Interface band

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SLIDE 16

16

Ei Eige gen n St Stra rain in Dama mage ge (Pandolf

  • lfi,

i, Ortiz z et al.; ; Menzel el, , Ekh et al., 2002)

)

  • Accomodation by eigen strain.
  • (interface-) plane stretching effects.
  • In an anisotropic way (normal and tangential modes).
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SLIDE 17

Field problem

17

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SLIDE 18

Dama mage ge re regulariz gularization ation so solv lved us usin ing g FFT FFT

18

  • Utilize Fourier transform
  • Solved for its roots using

Jacobian free Newton method.

  • Hetrogenous regularization lengthscale
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SLIDE 19

Te Test st Si Simu mulatio lation

19

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SLIDE 20

Pol

  • lycryst

ycrystal al Si Simulation mulation

20

  • Res

esolut ution

  • n: 256x256x2
  • Int

nter erfa face ce Band nd th thickne ness: 4 voxels

  • Ran

andomly ly orien enta tati tion

  • n

FCC

  • Elas

asto to-pl plas astic tic-dam damage age (cryst ystal plasti ticit ity) y)

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SLIDE 21

Polyc ycryst rystal al Si Simu mula latio tion: n: Dama mage e ev evolutio tion

21

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SLIDE 22

Polyc ycryst rystal al Si Simu mula latio tion: n: St Stes ess s Unloadin ding

22

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SLIDE 23

Polyc ycryst rystal al Si Simu mula latio tion: n: Dama mage e vs Plastic sticity ity

23

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SLIDE 24

Fut Future ure wo work rk

24

  • Coupling with damage models in the bulk
  • Monolithic schemes for Multiphysics
  • Implementation using petsc4py
  • Time integrators (Fortran support)
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SLIDE 25

Acknowl knowledgme edgment nt

25

DΓΌsseldorf Advanced MAterial Simulation Kit, DAMASK

  • Available as freeware according to GPL 3
  • Integrates into MSC.Marc and Abaqus

(std. and expl.)

  • Standalone spectral solver
  • Web: https://DAMASK.mpie.de
  • Email: DAMASK@mpie.de
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SLIDE 26

Thank you. Questions?

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SLIDE 27

Si Simu mulat lation ion (hexag

xagon

  • nal

al polycry cryst stal al loaded ded hori rizo zont ntall ally )

27

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SLIDE 28

Si Simu mulat lation ion

28

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SLIDE 29

St Stra rain in lo localis lisation ation

29

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SLIDE 30

Br Britt ittle le Si Simu mulat lation ion

30

Damage Strain (F11) Stress (P11)

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SLIDE 31

Me Mesosc

  • scale

ale me mechan hanics ics

31

  • Crystal plasticity.
  • FFT based Spectral method

Shanthraj et al. [2015]

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SLIDE 32

Ex Experim rimental ental-Numerical Numerical

32

Example: Basal slip in Magnesium

Wang et al. [2014]

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SLIDE 33

Ra Rate te in independe endent nt

33

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SLIDE 34

Ra Rate te in independe endent nt

34

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SLIDE 35

Local Damage

35

  • 1 for undamaged material
  • 0 for fully damaged
  • Monotonously decreases

(irreversibility)

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SLIDE 36

Normal opening strains

36

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SLIDE 37

Tangential opening strains

37

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SLIDE 38

Stress Integration (the Local problem)

38

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SLIDE 39

Mesh Objectivity

39

  • Coarse mesh (10 fourier points in the

band)

  • Fine = 2x coarse
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SLIDE 40

Wo Work rk of

  • f se

separation ration wi with h band nd thi hickness kness

40

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SLIDE 41

Vox

  • xelize

elized fie ield ld of

  • f the

he no norm rmals als

41

  • Generator points of

standard voronoi tessellation.

  • First order cartesian

moments. [Libermann et al., 2015]

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