Transcript pattern

Non-equilibrium systems
External flux
d ~ characteristic size
electro
convection
10-4
self-organization
(Dt
1/2~
ocean
…… currents
104
characteristic size
Desert vegetation patterns
Chemical Turing patterns (Swinney)
Experimental cell
Striped & hexagonal patterns
Labyrinthine pattern
Animal coats & Turing patterns
Simulated by
RD equations
Zebra & leopard
Spiral patterns in m range
(CO oxidation on Pt, Imbihl & Ertl, 1995)
Polycrystalline surface
110 surface
STM image of Pt(110) – (1x2)
showing the corrugated-iron
structure; the inset shows a line
scan across that structure
K. Swamy, E. Bertel and I. Vilfan
Surface Science, 425 L369 (1999)
Dewetting pattern
J.Klein et al,
PRL 86 4863 (2001)
I.Leizerson & S.G.Lipson
Patterns of crystal growth
 The crystal growth sequence on
an (001) cleavage plane in a
BaSO4 solution
Pina et al, Nature 395, 483 (1998)
Colloidal assembly
J.E.G. Wijnhoven and W.L. Vos, Science
281, 802 (1998)
G. Subramania et al,
Phys. Rev. B 63 235111 (2001)
Nanoscale deposition pattern
 STM image of a periodic array of
Fe islands nucleated on the
dislocation network of a Cu
bilayer on Pt(111)
Nanocluster arrays on interfaces

STM images of In nanoclusters on
Si(111)
J.-L.Li et al, PRL 88 066101 (2002)
Molecular self-assembly on interfaces
 Rows of pentacene on Cu(110)
produced by a substrate-mediated
repulsion
 S.Lucas et al, PRL 88 028301 (2002)
Rayleigh–Bénard convection
Devil’s Causeway
Rayleigh–Bénard convection
rolls,squares, hexagons, etc.
Spiral defect chaos
Patterns of vibrating sand (Swinney)
Development of Turing pattern
Activator excited locally
Long-range inhibitor excited
Activator suppressed at
neighboring locations
Periodic pattern
starts to develop
activators & inhibitors
convection
buoyancy
heat transfer
optical cavity
refractive index
light intensity
solid film
elastic stress
surface tension
neuron
membrane potential
ionic conductance
epidemics
infectious agent
immunity
Taylor column
centrifugal force
viscosity
Crystals & patterns
Equilibrium systems
Non-equilibrium systems
Short-range repulsion
Long-range attraction
Short-range activator
Long-range inhibitor
Crystal
Turing pattern
Evolution to equilibrium
Frozen defects
Non-potential effects:
Dynamic regimes are possible
Hexagonal & striped Turing patterns
0-hex
stripe
p-hex
Double triplet: quasicrystal
Two-wavelength Turing patterns
A two-layer system
with different
diffusivities
L. Yang, M. Dolnik,
A.M.Zhabotinsky, and
I.R.Epstein, PRL 88 208303
(2002)
Two-wavelength superposition patterns
A two-layer system with
strongly different diffusivities
L. Yang, M. Dolnik, A.M.Zhabotinsky,
and I.R.Epstein, PRL 88 208303 (2002)
Resonant superlattice patterns
G. Dewel et al, 2001
Superlattice patterns: convection in vibrated layer
W. Pesch et al, PRL 85 4281 (2000)
Rayleigh–Bénard convection: complex patterns
Experiments of V.Steinberg
Rolls, up- and down- hexagons
Nucleation of hexagons in a defect core
Two-frequency forced parametric waves
H.Arbell and J.Fineberg, PRE 65 036224 (2002)
Dynamics of spots in the plane
C.P.Schenk,M.Or-Guil,M.Bode,and H.-G.Purwins, Phys.Rev.Lett.78,3781 (1997)
Spirals and labyrinth patterns in BZ reaction
Action of incoherent light:
 A spiral wave forms in the upper half
of the same reactor, which is in the
dark
 A labyrinthine standing-wave pattern
forms in the lower half of the
reactor, which is illuminated with light
pulsed at twice the natural frequency
of the reaction
Chemical waves in the BZ reaction. Top: target patterns in a thin film of reagent (1.5 mm). Bottom: spiral waves in reagent similar to above
except less acidic. Both sequences from left to right are at 60 s intervals. Reprinted with permission from: Winfree, A. T. Prog. Theor. Chem.
1978, 4, 1.
Spiral wave patterns in CGLE
Frustrated pattern
P. G. Kevrekidis, A. R. Bishop, and K. Ø. Rasmussen
Phys. Rev. E 65, 016122 (2002)
Turbulent pattern
Spiral wave and its break-up
M. Baer, M. OrGuil,
PRL 82 1160 (1999)
Instability of a reaction front
Boundary dynamics: cn= cn(v) + f(k)
Labirynthine pattern develops from a
single stripe when the inhibitor is fast
(Meron et al)
Spiral turbulence develops from a
single stripe when the inhibitor is slow
3D instabilities in surface growth
Snowflakes
Multiple-exposure
photograph of a
dendrite advancing
downwards
Huang and Glicksman
Acta Metall.29 717 (1981)
Dendritic patterns in
electrodeposition
Bacterial colony