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Differential Model for 2D Turbulence

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Sergey Nazarenko, Warwick, UK. In collaboration with Victor Lvov, Weizmann ... 'gelation' and anomalous wake. Self-similar solution reaching infinite k in finite time ... – PowerPoint PPT presentation

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Title: Differential Model for 2D Turbulence


1
Differential Model for 2D Turbulence
  • Sergey Nazarenko, Warwick, UK
  • In collaboration with Victor Lvov, Weizmann
  • JETP Letters, 2006, Vol. 83, No. 12, pp. 541545.

2
Leith68 model of 3D turbulence
  • Kolmogorov solution

Thermodynamic energy equipartition
3
Warm cascade
  • Analytical solution with both cascade and
    thermodynamic components, Connaugton
    Nazarenko2004.
  • Describes the bottleneck phenomenon.

4
warm cascade (Connaughton, Nazarenko, 2004)
  • Cascade scaling at low k
  • Thermodynamic at large k

5
gelation and anomalous wake
  • Self-similar solution reaching infinite k in
    finite time
  • Spectrum in the wake is steeper than Kolmogorov

6
Setup of Kolmogorov
  • After reaching infinite k, the Kolmogorov
    spectrum sets up as a reflected from infinity
    wave
  • Typical for all finite capacity spectra
  • Previously seen in Weak MHD turbulence (Galtier,
    Nazarenko, Newell, Pouquet, 2000)

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12
Superfluid turbulence
  • Turbulent superfluid and normal components
    coupled via mutual friction, Lvov, Nazarenko,
    Volovik2005 Vinen 2005 Lvov, Nazarenko,
    Skrbek2006.

13
Systems with dual cascades
  • Gravity wave turbulence on water surface,
    Hasselmann Hasselmann85 Dyachenko, Newell,
    Pushkarev, Zakharov91

14
Differential model for 2D turbulence (DM2D)
  • Lvov and Nazarenko2006.

15
Invariants of DM2D
16
Energy and Enstrophy Fluxes
17
Cascade solutions
18
Predictions for Kolmogorov constants
Lvov, Pomyalov, Proccacia2002
  • Ihihara Kaneda2001 Danilov Gurarie2001
    DNS
  • CQ/CP1.9/60.32

19
Effect of friction
  • Change of scaling like in superfluids?
  • Change of scaling due to friction in passive
    scalar (Chertkov98) and 2D turbulence Boffetta
    et al2005)

20
Nastrom-Gage spectrum
  • Nastrom Gage84,
  • Friction?
  • Gkioulekas05

21
Not here
  • Now, the -3 exponent is in resonance with the
    inverse cascade exponent.
  • Hence a log rather than power-law correction.

22
Direct cascade with friction
23
Inverse cascade with friction
24
Summary of friction effects
  • There is no Nastrom-Gage shape
  • Friction arrests both cascades at finite scales.

25
Lilly89 model
  • Get rid of the thermodynamic solutions 2nd
    order equation

NG spectrum, Lilly89
26
Summary
  • Differential models put something in in order to
    get more useful stuff out.
  • Time evolution. Setup of cascades. Rate of total
    energy and enstrophy decay.
  • Mixed solutions with simultaneous cascades and
    thermal components.
  • Friction effects and other modifications.
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