NP6.3 | Transport and Mixing in Planetary Convection
Transport and Mixing in Planetary Convection
Co-organized by EMRP2/GD3
Convener: Thierry AlboussiereECSECS | Co-conveners: yanick Ricard, Stephane Labrosse

Planetary convection provides many challenges, regarding the equation of state (EoS), the coefficients of transport of momentum, heat and different species, and the governing equations. The non-linear transport of momentum causes turbulence (in the restricted sense) but the non-linear transport of heat and mass causes also a range of temporal and spatial scales, chaotic mixing, enhanced transport. Compressibility (cf. EoS), planetary rotation, dynamo action are all circumstances affecting planetary convection. In addition, the interaction between planetary envelopes, at the ICB or CMB for instance, have been shown to affect convection on one or both sides of the boundaries, with or without melting and crystallization. Mathematical, numerical and experimental studies are welcome within this broad subject.

Planetary convection provides many challenges, regarding the equation of state (EoS), the coefficients of transport of momentum, heat and different species, and the governing equations. The non-linear transport of momentum causes turbulence (in the restricted sense) but the non-linear transport of heat and mass causes also a range of temporal and spatial scales, chaotic mixing, enhanced transport. Compressibility (cf. EoS), planetary rotation, dynamo action are all circumstances affecting planetary convection. In addition, the interaction between planetary envelopes, at the ICB or CMB for instance, have been shown to affect convection on one or both sides of the boundaries, with or without melting and crystallization. Mathematical, numerical and experimental studies are welcome within this broad subject.