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Stress induced instabilities in material science and biology

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Presentation on theme: "Stress induced instabilities in material science and biology"— Presentation transcript:

1 Stress induced instabilities in material science and biology
C. Misbah, CNRS and Univ. J. Fourier Grenoble I Los Angeles October. 2005 Oct. 18th 2005 IPAM Oct. 2005

2 Uniaxial stress Biaxial stress Oct. 18th 2005 IPAM Oct. 2005

3 Questions 1) Front growth or recession? Solid 2) Planar front stable?
Melt, vapor 1) Front growth or recession? Solid 2) Planar front stable? Solid 3) Ultimate stage? Oct. 18th 2005 IPAM Oct. 2005

4 time Coarsening or fixed ? Stranski-Krastanov? Size selection?
Perpetual coarsening? Oct. 18th 2005 IPAM Oct. 2005

5 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. Oct. 18th 2005 IPAM Oct. 2005

6 Swelling or shrinkage of gels
Clamped at bottom Gel swelling T. Tanaka, H. Tanaka, Kawasaki, Sekimoto, Onuki Oct. 18th 2005 IPAM Oct. 2005

7 Misbah C., Renard F., Gratier J.P., Kassner K.,
Geoph. Res. Lett., 31, L6618 (2004). J. Schmittbuhl, F. Renard, J. P. Gratier, and R. Toussaint Phys. Rev. Lett. 93, (2004) Oct. 18th 2005 IPAM Oct. 2005

8 Misbah C., Renard F., Gratier J.P., Kassner K.,
Geoph. Res. Lett., 31, L6618 (2004). J. Schmittbuhl, F. Renard, J. P. Gratier, and R. Toussaint Phys. Rev. Lett. 93, (2004) Oct. 18th 2005 IPAM Oct. 2005

9 Stylolithes formation
(ex:limestone, queensland, Australia) dissolution Stress- induced corrugation Oct. 18th 2005 IPAM Oct. 2005

10 ATG instability comes to life!
Actin-assisted cell motility Oct. 18th 2005 IPAM Oct. 2005

11 J. van der Gucht et al. PNAS, 102, 7847 (2005)
L. A. Cameron et al., PNAS, 96, 4908 (1999). J. van der Gucht et al. PNAS, 102, 7847 (2005) Oct. 18th 2005 IPAM Oct. 2005

12 at bead/layer interface
Actin Polymerization at bead/layer interface P. Peyla, C. Misbah, preprint (2005) Oct. 18th 2005 IPAM Oct. 2005

13 Physical picture of the instability
solid Oct. 18th 2005 IPAM Oct. 2005

14 Physical picture of the instability
solid Instability unavoidable Oct. 18th 2005 IPAM Oct. 2005

15 Typical lengthscales of the pattern
Strain due to protuberance Strain energy gain Surface energy loss Oct. 18th 2005 IPAM Oct. 2005

16 Oct. 18th 2005 IPAM Oct. 2005

17 For For Oct. 18th 2005 IPAM Oct. 2005

18 Spencer Meiron (steady-states, 1994)
Yang and Srolovitz (1993) Kassner and Misbah (1994) Spencer Meiron (steady-states, 1994) Oct. 18th 2005 IPAM Oct. 2005

19 Sound speed, finite interface width
Surface tension effect Stress effect Close to a crack Sound speed, finite interface width Oct. 18th 2005 IPAM Oct. 2005

20 Simple ansatz Cycloid (Chui,Gao, 1993)
Double cycloid (conformal mapping, Kassner, Misbah, 2001) , derivation of groove velocities Multicycloids (Kohlert, Kassner, Misbah, 2003) (good agreement with numerics with few modes) Oct. 18th 2005 IPAM Oct. 2005

21 Phase-field approach: singularity?
Oct. 18th 2005 IPAM Oct. 2005

22 Phase field models Sharp interface Diffuse interface Oct. 18th 2005
IPAM Oct. 2005

23 Reference state 1 : stress=0 when strain=0
Ref. state 2: Zero strain is no stress free Oct. 18th 2005 IPAM Oct. 2005

24 If ref. state: strain is zero when when stress is
If equilibrium: If ref. state: strain is zero when when stress is BC: For z=0 There is no stress a all! Because Oct. 18th 2005 IPAM Oct. 2005

25 If ref. state: strain is zero when when stress is
If equilibrium: If ref. state: strain is zero when when stress is BC: Plays the role of a unixial stress Oct. 18th 2005 IPAM Oct. 2005

26 Gas (liq., vac.) Diffuse Solid Viewed as the work of external force
Oct. 18th 2005 IPAM Oct. 2005

27 gas solid Oct. 18th 2005 IPAM Oct. 2005

28 Sharp interface limit, asymptotics
Is a Singular perturbation Oct. 18th 2005 IPAM Oct. 2005

29 Outer solution (regular)
Inner solution (singular) Matching inner-outer solutions Oct. 18th 2005 IPAM Oct. 2005

30 Outer solutions: + Lamé Inner solutions: (1) Zeroth order:
(at all orders) And BC (2) First order: Oct. 18th 2005 IPAM Oct. 2005

31 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 » 5) Final groove velocity Oct. 18th 2005 IPAM Oct. 2005

32 Stress accumulation in the grooves, fracture?
1D dynamics Stress accumulation in the grooves, fracture? Oct. 18th 2005 IPAM Oct. 2005

33 Coarsening Mass flux Oct. 18th 2005 IPAM Oct. 2005

34 Exceptions in 1d with no noise!
Coarsening Mass flux If non conserved: Exceptions in 1d with no noise! Oct. 18th 2005 IPAM Oct. 2005

35 Volume variation ~ surface
Contact coalescence Volume variation ~ surface Oct. 18th 2005 IPAM Oct. 2005

36 Coarsening dominated by elasticity
conserved nonconserved In progress (cycloids show driving force independent of R) Agreement with the experiment of Koehn et al.,Geochimica and Cosmochimica Acta, 2004 Oct. 18th 2005 IPAM Oct. 2005

37 Heteroepitaxy Oct. 18th 2005 IPAM Oct. 2005

38 Partial relaxation Stressed film Oswald ripening?
Narrow size observed InGaAs/GaAs, InAs/inP, InAS/InGaAs, …... Oct. 18th 2005 IPAM Oct. 2005

39 =step energy/elastic energy
Monoatomic films substrate Elastic monopoles coverage =step energy/elastic energy Marchenko-Parshin (1980) and Marchenko 1992 Alerhand et al Oct. 18th 2005 IPAM Oct. 2005

40 (Tersoff, Villain, Müller, Kern….)
Coasening should be inevitable! Gain in elastic energy and in surface energy Oct. 18th 2005 IPAM Oct. 2005

41 1) In the pure thermodynamical limit, does coarsening persist?
Open questions 1) In the pure thermodynamical limit, does coarsening persist? 2) Is it thermodynamical or kinetical? In the first case which 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? Oct. 18th 2005 IPAM Oct. 2005


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