stress induced instabilities in material science and biology
DESCRIPTION
Stress induced instabilities in material science and biology. C. Misbah, CNRS and Univ. J. Fourier Grenoble I. Los Angeles October. 2005. Uniaxial stress. Biaxial stress. Questions. Melt, vapor. 1) Front growth or recession?. Solid. 2) Planar front stable?. Solid. 3) Ultimate stage?. - PowerPoint PPT PresentationTRANSCRIPT
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Oct. 18th 2005 IPAM Oct. 2005
Stress induced instabilities inmaterial science and biology
Los Angeles October. 2005
C. Misbah, CNRS and Univ. J. Fourier Grenoble I
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Uniaxial stress
Biaxial stress
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Solidxx xx
Solid
QuestionsMelt, vapor
1) Front growth or recession?
2) Planar front stable?
3) Ultimate stage?
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timeCoarsening or fixed ?
t ?
Stranski-Krastanov?
Size selection?Perpetual coarsening?
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ATG Intability (Asaro-Tiller,1972 -Grinfeld, 1986)
Quantum dots formation
pyramid-shaped quantum dots grown from indium, gallium, and arsenic. Each dot is about 20 nanometers wide and 8 nanometers in height.
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Swelling or shrinkage of gels
Clamped at bottom Gel swelling
T. Tanaka, H. Tanaka, Kawasaki, Sekimoto, Onuki
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Misbah C., Renard F., Gratier J.P., Kassner K., Geoph. Res. Lett., 31, L6618 (2004).J. Schmittbuhl, F. Renard, J. P. Gratier, and R. ToussaintPhys. Rev. Lett. 93, 238501 (2004)
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Misbah C., Renard F., Gratier J.P., Kassner K., Geoph. Res. Lett., 31, L6618 (2004).J. Schmittbuhl, F. Renard, J. P. Gratier, and R. ToussaintPhys. Rev. Lett. 93, 238501 (2004)
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Stylolithes formation
dissolution
Stress-inducedcorrugation
(ex:limestone, queensland,Australia)
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ATG instability comes to life!
Actin-assisted cell motility
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L. A. Cameron et al., PNAS, 96, 4908 (1999).
J. van der Gucht et al. PNAS, 102, 7847 (2005)
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Actin Polymerization at bead/layer interface
1 E
E2
P. Peyla, C. Misbah, preprint (2005)
1 E
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Physical picture of the instability
solidxxxx
zz
)sin(dSdSx
)cos(dSdS z
tdF
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Physical picture of the instability
solidxxxx
zz
)sin(dSdSx
)cos(dSdS z
tdF
][
])[sin()cos(
)sin()cos(
xxzz
xxzz
zzzxxxt
dS
dS
dSdSdF
Instability unavoidable
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Typical lengthscales of the pattern
h
Strain due to protuberance h
Ee 0
zzxx)0()0(
0
Strain energy gain hh
E
2
0
Surface energy loss hh
LL
20 )(
0L
L
hhhhE
G
][
2
20
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hgE
][
2
20
hhgE lsg )(
0g
0g
c mmg
c
12231120 101011010 gE cc
bar 10 c
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hgE
][
2
20
hhgE lsg )(
0g
0g
c mmg
c
222
0
)//()/(
aabaaE
E
GeSi /For 50/ab
%4/ aa
nm 20 GaAsInGaAs /For
%7/ aa
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Yang and Srolovitz (1993)Kassner and Misbah (1994)
Spencer Meiron (steady-states, 1994)
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][2
2
2
1nnttE
Surface tension effectStress effect
RRRE
20
Close to a crack
R
R1
Sound speed, finite interface width
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Simple ansatz
Cycloid (Chui,Gao, 1993)
Double cycloid (conformal mapping, Kassner, Misbah, 2001)
Multicycloids (Kohlert, Kassner, Misbah, 2003)
, derivation of groove velocities
(good agreement with numerics with few modes)
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Phase-field approach: singularity?
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Phase field models
1 2 1 2
Phase field
Sharp interface Diffuse interface
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Reference state
uu ijijkkij 2
Reference state 1 : stress=0 when strain=0
Ref. state 2: uij
)0(
uuu ijijij
)0(
'
)'')0()0( (2)( uuuu ijijijkkkkij
Zero strain is no stress free
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)2) ( ( uuuu eq
ijijij
eq
kkkk
eq
ijij
If equilibrium: ij
eq
ij p0
ij
eq
ij
pu 32
0
If ref. state: strain is zero when when stress is
ijsp
0 ij
eq
ij
ppu s
320 0
BC:
0u For z=0 0uxx
00p
0uzz
Because 0 zz There is no stress a all!
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)2) ( ( uuuu eq
ijijij
eq
kkkk
eq
ijij
If equilibrium: ij
eq
ij p0
ij
eq
ij
pu 32
0
If ref. state: strain is zero when when stress is
ijsp
0 ij
eq
ij
ppu s
320 0
BC: 0' u xx
2
0p
u szz
0 zz
22
0p
sxx Plays the role of a unixial stressp
s0
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uuuuu iijjiiijijpf
2
sppp 00 Viewed as the work ofexternal force
]21),([ )(
22 ijufrdF
Solid
Gas (liq., vac.)
Diffuse
1
0
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ff hhf01
)](1[)(
]21),([ )(
22 ijufrdF
0)0( ,1)1( , )23(2
hhh
f1
f0solid gas
F
t 0
iuF
uuuuu iijjiiijijpf
2
)1(22
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Sharp interface limit, asymptotics
0
Is a Singular perturbation ]
21),([ )(
22 ijufrdF
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......),,(),,(),,( 10 tsrtsrtsr
......),,(),,(),,( 10 tststs
Outer solution (regular)
Inner solution (singular)
rMatching inner-outer solutions
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Outer solutions: constant + Lamé
Inner solutions:
(1) Zeroth order: )1(2' 000
)]tanh(1[210 (at all orders)
And BC 0 , ntnnp
(2) First order: )()L(01
G
][2
2
2
1nnttE
kV n
r
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Main Results
1) Increase of the amplitude without bound
2) Phase-field supresses finite time singularity
3) Perpetual coarsening
4) A finite interface width « Yield stress »
0y
5) Final groove velocity 1V
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1D dynamics
Stress accumulation in the grooves, fracture?
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CoarseningMass flux
jvdt
dR
2/1)/1( RRj
.2 Constdt
dRR 3/1tR
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CoarseningMass flux
jvdtdR
Rj /1
.2 Constdt
dRR 3/1tR
If non conserved:
1/Rvdt
dR
2/1tR
Exceptions in 1d with no noise!
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Contact coalescence
tRCtedt
dRR
dt
dRS
dt
dV , , , 2
3
Volume variation ~ surface
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Coarsening dominated by elasticity
2/1tR conserved
tR nonconserved
In progress
Agreement with the experiment of Koehn et al.,Geochimica and Cosmochimica Acta, 2004
(cycloids show driving force independent of R)
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Heteroepitaxy
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Oswald ripening?
Narrow size observed InGaAs/GaAs, InAs/inP, InAS/InGaAs, …...
Stressed filmPartial relaxation
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substrate
Monoatomic films
Marchenko-Parshin (1980) and Marchenko 1992Alerhand et al. 1989.
eCCae 21/
)sin(
coverage 21/CC =step energy/elastic energy
Elastic monopoles
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(Tersoff, Villain, Müller, Kern….)
Coasening should be inevitable!
Gain in elastic energy and in surface energy
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Open questions
1) In the pure thermodynamical limit, does coarseningpersist? 2) Is it thermodynamical or kinetical? In the first casewhich ingredients would supress coarsening? Coarsening is subtle (Politi, Misbah, Phys. Rev. Lett. 2004)
3) In Dynamical simulations: coarsening stops or slowed down?4) Some systems QD form under compression but not under tension!5) Cell motility: bead-gel friction decisive?