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Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre Drossart LESIA

Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

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Page 1: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Convection dans les coquilles sphériques et circulation des

planètes géantes

Convection in spherical shells and general circulation of

giant planets

Pierre DrossartLESIA

Page 2: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Collaboration

Proponents :• André Mangeney • Olivier Talagrand (LMD)• Pierre DrossartPhD Students : E. Brottier, A. Abouelainine, V. LesueurExternal collaborations : M. Rieutord, M. Faure,

J.I. Yano, …Time scale : 1986-1996

Page 3: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Situation of the question

• Giant planets:

- global radiative balance > solar heating

- General circulation = zonal

- Alternance of bands with +/- zonal velocities

- Small pole-equator temperature gradient

Page 4: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Giant planets meteorology:

-banded structure-Highly turbulent regime-Internal heating source

Page 5: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Internal heating

• Source : separation of He in the internal core or residual contraction (?)

=> internal convection presentQuestion: is the general circulation and the banded

appearance due to solar heating OR internal heating ?

Dimensionless parameter : E = ratio of emitted to solar heating

ratio of conductive time to radiative time

Page 6: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre
Page 7: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Numerical simulation (new approach in the context of the mid-80’s…)

• Full spherical (spherical shell) approach

• 3D simulation

• Approximation for convection : Boussinesq

(neglecting compressibility effects, except for thermal dilatation)

Page 8: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

General adimensional Equations

• ………………….

Fields : u = velocity, P = pressure, T = temperature, = vorticityCharacteristic numbers :

T = Taylor, Coriolis vs viscosityP = Prandtl , ratio of diffusivitiesF = Froude, centrifugal force vs gravity

Page 9: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre
Page 10: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre
Page 11: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Boundary conditions• Rigid or free conditions at the

inner and outer shells• Temperature conditions adapted

to the planetary conditions• Pressure condition : Kleiser-

Schumann method for ensuring exact conditions at the boundary

• Thermal conditions related to observed planetary conditions

Page 12: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre
Page 13: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre
Page 14: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Numerical approach

• Spectral methods• Semi-implicit scheme• Chebyshev spectral decomposition for the

fields (FFT related)• Exact boundary conditions – adapted to

planetary conditions• Computers : CONVEX (Observatoire),

Cray (CIRCE/IDRISS), …

Page 15: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

First results (1)

• Threshold for convective instability for various boundary conditions (free, fixed, etc.)

=> Exact comparison possible with Chandrasekhar calculations

Page 16: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Linear solution : convective instability for the mostunstable spherical harmonics

Page 17: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Non linear calculation

Page 18: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Radial velocity field for E=5 = 10-3

Page 19: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Azimutal velocity on the outer planet E=1.8 =5 x 10-3

Page 20: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Radial velocity for a « Neptune » case E=2.61 =10-4

Page 21: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

First results (2)

• Viscous regime

Page 22: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Towards a turbulent regime

Page 23: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

What have we learned from this program

• Geostrophic solution for deep circulation

Deep circulation can be maintained by solar heating at the boundary condition !

• Zonal circulation appear at the outer boundary• Extension of Hide’s theorem in the deep shell

regime• Inversion of the zonal circulation compared to

geostrophic solution

Page 24: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Extension of the science program

• Collaboration with J.I. Yano : other approaches

• Collaboration with A. Sanchez-Lavega (Bilbao) for specific topics in Giant Planets dynamics (hot spot dynamics)

Page 25: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Conclusions of this work• Robust and validated program, method re-used by

several other projects• Good introduction (for LESIA) in the field of

dynamics, • Initiation of a fruitful long term collaboration

between LESIA and LMD• Two PhD thesis• Few publication (low bibliometrics, but …)• The G.P. Circulation problem is still there !• and …

Page 26: Convection dans les coquilles sphériques et circulation des planètes géantes Convection in spherical shells and general circulation of giant planets Pierre

Most important :

…. a lot of fun