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Table 2.

Simulation parameters and results.

Model Prot min(Ra) (1) ΔΩ/Ωeq(2) urms(3) Ro (4) Pcyc (5) (5) (5) (5)
[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.

(1)

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.

(2)

Differential rotation parameter, ΔΩ/Ωeq = (Ωeq − Ω45)/Ωeq, where Ωeq and Ω45 are the angular velocities at 0° and 45° latitude, respectively.

(3)

urms⟩ is the volume average of the turbulent velocity in the entire convection zone.

(4)

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).

(5)

Toroidal and radial magnetic field averaged over longitude and time. The subscripts NSL and TAC correspond to r = 0.95 R and r = 0.76 R, respectively.

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