variational methods in dislocation dynamics · • theory of linear elastic dislocations. •...
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![Page 1: Variational Methods in Dislocation Dynamics · • Theory of linear elastic dislocations. • Special case: Activity on single slip system, single slip plane →Phase-field model](https://reader030.vdocuments.us/reader030/viewer/2022040618/5f252d230133417b7e3030d2/html5/thumbnails/1.jpg)
Michael OrtizOberwolfach 09/03
Variational Methods in Dislocation Dynamics
M. OrtizM. OrtizCalifornia Institute of Technology
Acknowledgements: P. Ariza, A. Cuitiño, A. Garroni, M. Koslowski, Stefan Müller
Workshop on PDEs and MaterialsOberwolfach, Germany
September 8, 2003
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Michael OrtizOberwolfach 09/03
Outline
• Mechanistic basis of crystal plasticity.• Theory of linear elastic dislocations.• Special case: Activity on single slip system,
single slip plane → Phase-field model.• Numerical implementation, simulations.• Results of rigorous analysis (Γ-convergence).
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Michael OrtizOberwolfach 09/03
Metal plasticity - Lengthscales
Lattice defects, EoS
Dislocation dynamics
Subgrainstructures
time
µsns
Polycrystals
Engineeringcalculations
ms
mmnm µmlength
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Michael OrtizOberwolfach 09/03
Crystal plasticity – Macroscopic behavior
Uniaxialtension test
Copper tensile test(Franciosi and Zaoui ’82)
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Michael OrtizOberwolfach 09/03
Crystal plasticity – Relaxation
Irreversibleaccommodation of shear deformation
by crystallographic slip
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Michael OrtizOberwolfach 09/03
Crystal plasticity – Energy barriers
Irreversibleaccommodation of shear deformation
by crystallographic slip
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Michael OrtizOberwolfach 09/03
Crystal plasticity and dislocations
slip plane
dislocationcore
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Michael OrtizOberwolfach 09/03
Crystal plasticity and dislocations
Burgersvector
Burgerscircuit
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Michael OrtizOberwolfach 09/03
Example - Nanoindentation of [001] Au
• Nanoindentation of [001] Au, 2x2x1 micrometers
• Spherical indentor, R=7 and 70 nm
• Johnson EAM potential
• Total number of atoms ~ 0.25 10^12
• Initial number of nodes ~ 10,000
• Final number of nodes ~ 100,000
Detail of initial computational mesh(Knap and Ortiz, 2002)
(Movie)
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Michael OrtizOberwolfach 09/03
Example - Nanoindentation of [001] Au
70 nm indenter, depth = 0.75 nm
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Michael OrtizOberwolfach 09/03
Dislocation dynamics – Numerical tools• First-principles calculations: Dislocation cores,
dipoles, quadrupoles… ~ 103 atoms (T. Arias ’00)• Molecular dynamics: Empirical potentials… ~ 109
atoms (F. Abraham ’03)• Linear elasticity: Dislocation dynamics, L ~ 106b, ε ~ 1% (Bulatov et al. ’03)
Ta quadrupole(T. Arias ´00)
FCC ductile fracture(F.F. Abraham ´03)
FCC dislocation dynamics(M. Rhee et al.´02)
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Michael OrtizOberwolfach 09/03
Theory of linear-elastic dislocations
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Michael OrtizOberwolfach 09/03
Theory of linear-elastic dislocations
The slip systems of fcc crystals
(Schmidt and Boas nomenclature)
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Michael OrtizOberwolfach 09/03
Theory of linear-elastic dislocations
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Michael OrtizOberwolfach 09/03
Theory of linear-elastic dislocations
![Page 16: Variational Methods in Dislocation Dynamics · • Theory of linear elastic dislocations. • Special case: Activity on single slip system, single slip plane →Phase-field model](https://reader030.vdocuments.us/reader030/viewer/2022040618/5f252d230133417b7e3030d2/html5/thumbnails/16.jpg)
Michael OrtizOberwolfach 09/03
Theory of linear-elastic dislocations
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Michael OrtizOberwolfach 09/03
Theory of linear-elastic dislocations
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Michael OrtizOberwolfach 09/03
Single slip plane – Phase field model
0 1 2
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Michael OrtizOberwolfach 09/03
Single slip plane – Phase field model
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Michael OrtizOberwolfach 09/03
Single slip plane – Phase field model
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Michael OrtizOberwolfach 09/03
Single slip plane – Phase field model
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Michael OrtizOberwolfach 09/03
Single slip plane – Phase field model
1) Unconstrained slip 2) Phase field 3) Slip distribution
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Michael OrtizOberwolfach 09/03
Dislocation-obstacle interaction
Impenetrable obstacles
(Humphreys and Hirsch ’70)
Obstacles of finite strength
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Michael OrtizOberwolfach 09/03
Dislocation obstacle interaction
Reaction coordinate
Favorable Junction
Unfavorable Junction
Details of Intersection Process
ζ
τf f
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Michael OrtizOberwolfach 09/03
Dislocation-obstacle interaction
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Michael OrtizOberwolfach 09/03
Dislocation-obstacle interaction
Stress-strain curve
a b c
d e f
g h iDislocation density
(Movie)
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Michael OrtizOberwolfach 09/03
Dislocation-obstacle interaction
a
c d
b
e f3D view of slip field showingswitching of pinning cusps
Stress-strain curveshowing return-point
memory effect
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Michael OrtizOberwolfach 09/03
Line-tension anisotropy
b
-50 0 50-1
-0.5
0
0.5
1τ/τ0
γ/γo
ν = 0.0ν = 0.3ν = 0.5
-50 0 500
0.05
0.1
0.15
0.2
0.25
0.3
0.35
0.4
0.45ρ/ρ0
γ/γo
ν = 0.0ν = 0.3ν = 0.5
Stress-strain curve Dislocation density vs.strain
0.0=ν 3.0=ν 5.0=ν
Stress-strain curve Dislocation density
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Michael OrtizOberwolfach 09/03
Obstacle density, sample size
22 10)( −=cba 42 10)( −=cbb
62 10)( −=cbc 82 10)( −=cbd
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Michael OrtizOberwolfach 09/03
Concluding remarks
• Phase-field model provides a variational characterization of dislocation dynamics
• Phase-field model offers computational advantages (gridless implementation), and is amenable to rigorous analysis.
• Extensions:– Full 3D theory, multiple slip– Lattice statics theory– Anharmonic effects in dislocation cores
• Reference: http://www.solids.caltech.edu/~ortiz/publications.html
Koslowski M, Cuitino AM, Ortiz M A phase-field theory of dislocation dynamics, strain hardening and hysteresis in ductile single crystalsJ MECH PHYS SOLIDS 50 (12): 2597-2635 DEC 2002