Table 2.
Simulation parameters and results.
Model | Prot | min(Ra) (1) | ΔΩ/Ωeq(2) | ⟨urms⟩ (3) | Ro (4) | Pcyc |
![]() |
![]() |
![]() |
![]() |
---|---|---|---|---|---|---|---|---|---|---|
[days] | [m s−1] | [years] | [T] | [T] | [T] | [T] | ||||
P29 | 29 | 4.5 × 106 | 0.087 | 87.06 | 2.13 | 6.42 | 0.0422 | 0.0012 | 0.4559 | 0.0113 |
P25 | 25 | 4.5 × 106 | 0.047 | 80.13 | 1.64 | 6.87 | 0.0403 | 0.0013 | 0.4372 | 0.0147 |
P21 | 21 | 4.5 × 106 | 0.023 | 79.35 | 1.38 | 8.59 | 0.0392 | 0.0016 | 0.4027 | 0.0174 |
Notes.
A minimum Rayleigh number for the simulations may be estimated as , where Θe is the ambient state potential temperature, α = 9.64 × 10−9 s−1, is the inverse of the Newtonian cooling time limiting the growing of perturbations of Θ, rcz = 0.2 R⋆ is the depth of the convection zone and ν = 108 m2 s−1 is the maximum value of the numerical viscosity estimated by Strugarek et al. (2016), for EULAG-MHD simulations with a similar resolution.
Differential rotation parameter, ΔΩ/Ωeq = (Ωeq − Ω45)/Ωeq, where Ωeq and Ω45 are the angular velocities at 0° and 45° latitude, respectively.
Rossby number is defined as Ro = Prot/τc and computed with τc = αHp/urms, where Hp is the pressure scale height, and it is measured at one pressure height scale above the bottom of the convective zone (Gilman 1980).
Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.
Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.
Initial download of the metrics may take a while.