Multiscale Modeling Questions for the Mathematicians • For a given continuum law, what can we deduce about the defect laws? (If time permits): • Fits.

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Transcript Multiscale Modeling Questions for the Mathematicians • For a given continuum law, what can we deduce about the defect laws? (If time permits): • Fits.

Multiscale Modeling
Questions for the Mathematicians
• For a given continuum law, what can
we deduce about the defect laws?
(If time permits):
• Fits of emergent theories are often
sloppy – the parameters are not well
determined by the data. Can we explain
the characteristic common features of
these sloppy models?
Transitions between Scales
Multiscale Modeling
Microphysics:
Atoms, Grains,
Defects…
Match?
Numerics:
Finite Element/Diff,
Galerkin…
Continuum Laws
Defect Dynamics
Coupled system: continuum and defects. Defect properties,
evolution determined by gradients in continuum fields.
For a given continuum law, what can
we deduce about the defect laws?
Deducing Defect Laws
More specific formulation
In the space of all reasonable microscopic systems
(numerical implementations, regularizations) consistent
with a given continuum law, what defect laws can
emerge?
(1) Extracting defect laws (Activated 2D Dislocation Glide):
Complete Picture
Velocity explicitly calculated from local stress fields
Environmental Impact and Dependence, Functional Forms
(2) Guessing defect laws (2D Crack Growth):
Velocity assumed dependent on local stress fields
Symmetry and analyticity assumptions yield form of law
(3) Laws from the continuum? (Faceting in etched Silicon)
Shock evolution law?
Viscosity solution disagrees with experiment
Extracting Laws
Dislocation Glide: Nick Bailey
Thermally activated glide
Glide slides planes of atoms, v×b=0
Barrier ~ midway between equilibria
External stress s
Velocity ~ v0(s) exp(-EB(s)/kBT)
Dislocation
Edge of Missing Row
Burgers Vector b
How fast will the dislocations
move, given an external stress
tensor s? What is the barrier
EB(s) and prefactor v0(s)?
Environmental Impact, Dependence
Dislocation Glide, Nick Bailey
General solution to continuum theory expandable in multipoles
ui(r) =  r n M[n]i(q,f)
Environmental Impact:
• n=0, logs, arctan: Dislocation displacement field s  b
• n=-1: Volume change, elastic dipole due to dislocation
• n=-2, … Near-field corrections
Controls interaction between defects
Environmental Dependence:
• n=1: External stress s
• n=2, 3, … Boundary conditions, interfaces
Multipole expansions for arbitrary continua?
Finding Functional Forms
Dislocation Glide, Nick Bailey
Symmetries: Inverting Stress
EB(sxy) = EB(-sxy) – a2 sxy
sxx
Singularities: Saddle-Node Transition
EB(sxy) = c3/2 (sc –sxy)3/2+ c5/2 (sc –sxy)5/2…
Physical Model:
Sinusoidal Potential + Corrections
Fit to Physical Functional Form
EB(sxx, syy, sxy) = -(a2/2) sxy + (a2 sc/p)
(arcsin(sxy/sc) + Sn An (1-(sxy/sc)2)n+1/2)
Taylor Series for sc, A1, A2:
Nine Parameters Total Fits Entire Range
(Nine Measurements or DFT Calculations!)
EB
sxy
(Ballistic)
sc
sxy
sxx
Guessing Laws
Crack Growth Laws: Jennifer Hodgdon
Environmental Dependence
Solution of Elasticity with Cut:
Three terms with s  r-1/2
Stress Intensity Factors K I,K II, K III
• Mode I: Crack Opening
• Mode II: Shearing
• Mode III: Twisting
How fast will the crack grow,
given an external stress tensor
s? What direction will it grow?
Guessing Laws
Crack Growth Laws: Jennifer Hodgdon
Ingraffea: FEM
Given current shape, force
Finds stress intensities
KI, KII, KIII
Wants Direction q (or n)
and Velocity v of Growth
Symmetry Implies:
dX/dt = v(KI, KII2) n
dn/dt = -f(KI, KII2) KII b
dn/dt: b odd, needs odd KII
Doesn’t turn if KII=0
Cotterell and Rice: KII = KI Dq/2
Dq ~ exp[(-f KI /2v) x]
How big is the decay length
2v /f KI? Length set by microscopic
scale of material: grain size,
nonlinear zone size, atom size
Crack turns abruptly until KII=0
(Principle of Local Symmetry)
Is Analyticity Guaranteed?
Crack Growth Laws: Jennifer Hodgdon
Landau theory assumes power
series: analyticity. Analyticity
natural for finite systems, time
t<, temp. T>0
(Else critical points, bifurcations,
power laws)
Ductile fracture: large region
around crack tip: collective
behavior
Fatigue fracture: large region,
long times, history
Brittle fracture: OK!
Abraham, Duchaineau, and De La Rubia
Billion atoms of copper
Too small to see nonlinear zone!
Restrictions to exclude
ductile fracture would be
prudent, acceptable.
Laws from the Continuum?
Faceting in etched Silicon
Melissa Hines, Rik Wind, Markus Rauscher
Etching rate jumps
Etching rate
are associated with
has cusps at
a faceting
low-index
transition
surfaces
First-order: nucleation
CACTUS, FFTW
CCMR, Microsoft
Which shock evolution law?
Faceting in etched Silicon
Melissa Hines, Rik Wind, Markus Rauscher
Continuum law:  h / t = [vn = etch rate (q,f)]
Forms facets in finite time: how to evolve thereafter?
“Viscosity solution” flattens. Experimental facets persist!
Energy anisotropy can affect evolution at cusps (Watson)
Math: What shock evolution laws can emerge?
Experiment: What do we need to measure?
Numerics: How do we implement them?