stochastic geometry of turbulence gregory falkovich weizmann institute november 2014 d. bernard, g....

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Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A. Celani, S. Musacchio, K. Turitsyn, M. Vucelja

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Page 1: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Stochastic geometry of turbulence

Gregory FalkovichWeizmann Institute

November 2014

D. Bernard, G. Boffetta, A. Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Page 2: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Fractals, multi-fractals and God knows what

depends neither on q nor on r - fractal

depends on q – multi-fractal

depends on r - God knows what

Page 3: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Turbulence is a state of a physical system with many degrees of freedom

deviated far from equilibrium. It is irregular both in time and in space.

Energy cascade and Kolmogorov scaling

Transported scalar (Lagrangian invariant)

Page 4: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Full level set is fractal with D = 2 - ζ

Random Gaussian Surfaces

What about a single isoline?

Page 5: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

3d is a mess

Page 6: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Schramm-Loewner Evolution - SLE

2d is a paradise

Page 7: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 8: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

What it has to do with turbulence?

Page 9: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

C=ξ(t)

Page 10: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 11: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Euler equation in 2d describes transport of vorticity

Page 12: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Family of transport-type equations

m=2 Navier-Stokes m=1 Surface quasi-geostrophic model,m=-2 Charney-Hasegawa-Mima model

Electrostatic analogy: Coulomb law in d=4-m dimensions

Page 13: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

This system describes geodesics on an infinitely-dimensional Riemannian manifold of the area-preserving diffeomorfisms. On a torus,

Page 14: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

(*)

Add force and dissipation to provide for turbulence

lhs of (*) conserves

Page 15: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

pumping

kQ

Kraichnan’s double cascade picture

P

Page 16: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Inverse Q-cascade

ζ

m

Page 17: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Small-scale forcing – inverse cascades

Page 18: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 19: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

perimeter P

Boundary Frontier Cut points

Boundary Frontier Cut points

Bernard, Boffetta, Celani &GF, Nature Physics 2006, PRL2007

Page 20: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 21: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 22: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 23: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 24: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Scalar exponents ζ of the scalar field (circles) and stream function (triangles), and universality class κ for different m

ζ κ

Page 25: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 26: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Inverse cascade versus Direct cascade

Page 27: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

M Vucelja , G Falkovich & K S Turitsyn Fractal iso-contours of passive scalar in two-dimensional smooth random flows. J Stat Phys 147 : 424–435 (2012)

Page 28: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Smooth velocity, locally anisotropic contours

Page 29: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 30: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 31: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 32: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 33: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 34: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 35: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 36: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja

Within experimental accuracy, isolines of advected quantities are conformal invariant (SLE) in turbulent inverse cascades. Why?

Vorticity isolines in the direct cascade are multi-fractal.

Isolines of passive scalar in the Batchelor regime continue to change on a time scale vastly exceeding the saturation time of the bulk scalar field.Why?

Conclusion

Page 37: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 38: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 39: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja
Page 40: Stochastic geometry of turbulence Gregory Falkovich Weizmann Institute November 2014 D. Bernard, G. Boffetta, A.Celani, S. Musacchio, K. Turitsyn, M. Vucelja