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Table 1.

Summary of the simulations.

Run β [°] urms [m/s] (Brms, Brmsstar) [kG] (Brmspol, Brmstor) [kG] Co Pe Re ReM Pcyc [years]

MHDr2 51 (60, 21) (19, 22) 10.1 7 35 24 1.88 ± 0.09
DipA 50 (60, 33) (23, 19) 8.7 8 40 28 1.66 ± 0.07
DipAt 30° 50 (58, 31) (22, 19) 8.7 8 40 28 1.79 ± 0.03
DipAt2 60° 51 (59, 28) (20, 21) 8.7 8 40 28 1.81 ± 0.05
DipAh 90° 53 (58, 23) (18, 21) 8.3 8 42 29 1.88 ± 0.03

DipB* 28 (172, 53) (102, 54) 15.6 4 22 15 no cycles
DipBt* 30° 28 (172, 53) (96, 65) 15.8 4 22 15 no cycles
DipBt2* 60° 31 (141, 44) (77, 45) 14.2 5 24 17 no cycles
DipBt3* 80° 35 (116, 37) (54, 32) 12.4 5 28 19 no cycles
DipBt4* 85° 36 (105, 34) (44, 27) 11.9 6 29 20 no cycles
DipBh* 90° 52 (53, 26) (16, 16) 8.4 8 42 29 1.71 ± 0.26

DipB 29 (157, 47) (90, 52) 15.2 4 23 16 no cycles
DipBt 30° 30 (147, 46) (83, 49) 14.5 5 24 17 no cycles
DipBt2 60° 33 (129, 40) (64, 35) 13.3 5 26 18 no cycles
DipBh 90° 53 (55, 26) (18, 20) 8.5 8 41 29 1.66 ± 0.04

Notes. From left to right: obliquity angle of the added dipole field, the rms velocity urms, the volume-averaged rms magnetic field Brms, the poloidal and toroidal components of Brms, the Coriolis number, the SGS Péclet number, the fluid and magnetic Reynolds numbers, and the magnetic cycle period. Quantities are averaged over the convective core r < 0.2R unless “*” is indicated, in which case the average is over r < R.

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