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1 Micromechanics using Spectral Method Interface Decohesion in - - PowerPoint PPT Presentation
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
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 Spectral Solver
- Basic scheme
- Some applications
- Demo: a very simple (1D) implementation using petsc4py
- Smeared damage mechanics
- Interface decohesion in Polycrystals.
- Future Work
Mo Motiv tivation ation
- strain localization
- damage initiation
- recrystallization nucleation
- β¦
- tool design
- crashworthiness
- component properties
- β¦
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 !
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)
CP CPFEM/ FEM/CPFFT CPFFT st strat rategy egy
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M
material point model
π π
solver for
- equilibrium
- compatibility
F P
deformation partitioning & homogenization crystallite elasto-plasticity
Fe
Lp S constitutive law
- elasticity
- plasticity
Th The sp spectral tral so solv lver
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- 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
Sp Spectral ctral me method hod
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div π = 0 Static equilibrium: Split strain: π» = π» + π» π»π+1 = π»π β π β ππ
FFT
Material law: π = π«π» Introduce reference medium: Stiffness π« π»π+1 = π»π β β±β1 π: ππ
with Ξππππ = ππππ πππ and πππ = ππππ π·ππππ
β1
Co Comp mparion arion FEM FEM vs vs FFT FFT
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- P. Eisenlohr., M. Diehl, R. A. Lebensohn, F. Roters: International Journal of Plasticity (2013), 37 - 53
Ex Experim rimental ental-Numerical Numerical
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Example: Basal slip in Magnesium
- F. Wang, S. Sandloebes, M. Diehl, L. Sharma, F. Roters, D. Raabe:Acta Materialia 80 (2014) 77-93
Me Mesosc
- scale
ale me mechan hanics ics
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- High Resolution Crystal plasticity enabled through robust
spectral solvers Shanthraj et al. [IJP, 2015]
Demo mo (1D elasticity + spectral method using petsc4py)
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Int nterface erface decoh
- hesion
esion (form
- rmab
ability ility li limi miter) er)
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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
Int nterface erface mo modeli ling ng of
- f pol
- lycrystals
crystals
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Interface elements Interface band
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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).
Field problem
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Dama mage ge re regulariz gularization ation so solv lved us usin ing g FFT FFT
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- Utilize Fourier transform
- Solved for its roots using
Jacobian free Newton method.
- Hetrogenous regularization lengthscale
Te Test st Si Simu mulatio lation
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Pol
- lycryst
ycrystal al Si Simulation mulation
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- 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)
Polyc ycryst rystal al Si Simu mula latio tion: n: Dama mage e ev evolutio tion
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Polyc ycryst rystal al Si Simu mula latio tion: n: St Stes ess s Unloadin ding
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Polyc ycryst rystal al Si Simu mula latio tion: n: Dama mage e vs Plastic sticity ity
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Fut Future ure wo work rk
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- Coupling with damage models in the bulk
- Monolithic schemes for Multiphysics
- Implementation using petsc4py
- Time integrators (Fortran support)
Acknowl knowledgme edgment nt
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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
Thank you. Questions?
Si Simu mulat lation ion (hexag
xagon
- nal
al polycry cryst stal al loaded ded hori rizo zont ntall ally )
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Si Simu mulat lation ion
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St Stra rain in lo localis lisation ation
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Br Britt ittle le Si Simu mulat lation ion
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Damage Strain (F11) Stress (P11)
Me Mesosc
- scale
ale me mechan hanics ics
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- Crystal plasticity.
- FFT based Spectral method
Shanthraj et al. [2015]
Ex Experim rimental ental-Numerical Numerical
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Example: Basal slip in Magnesium
Wang et al. [2014]
Ra Rate te in independe endent nt
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Ra Rate te in independe endent nt
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Local Damage
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- 1 for undamaged material
- 0 for fully damaged
- Monotonously decreases
(irreversibility)
Normal opening strains
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Tangential opening strains
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Stress Integration (the Local problem)
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Mesh Objectivity
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- Coarse mesh (10 fourier points in the
band)
- Fine = 2x coarse
Wo Work rk of
- f se
separation ration wi with h band nd thi hickness kness
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Vox
- xelize
elized fie ield ld of
- f the
he no norm rmals als
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- Generator points of
standard voronoi tessellation.
- First order cartesian
moments. [Libermann et al., 2015]
1 1 1 1 1 1 1 1 1 1 1 2 3 3 3 3 3 2 2 2 2 2 2 4 4 4 4