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Table 3.

Summary of runs with different values of imposed field and Coriolis number.

Run B0/Beq0 Co λτtd BR
A2 0.026 0 0.35 0.9 0.08 (0.11) 0.92 (0.9) 1.28 ± 28.13 −0.029 Yes
G1 0.065 0.002 0.38 0.4 0.32 (0.40) 0.49 (0.55) 1.21 ± 21.20 −0.046 Yes
G2 0.066 0.004 0.54 0.9 0.32 (0.46) 0.73 (0.73) 1.27 ± 27.12 −0.041 Yes
G3 0.066 0.006 0.52 1.6 0.38 (0.52) 1.59 (1.59) 0.67 ± 67.05 −0.039 Yes
G4 0.067 0.012 0.50 2.5 0.38 (0.50) 1.34 (1.34) 0.50 ± 50.06 −0.048 Yes
G5 0.066 0.015 0.46 1.3 0.32 (0.42) 0.98 (1.89) 0.34 ± 34.07 Weak
G6 0.068 0.018 0.43 1.4 0.28 (0.34) 0.98 (0.98) 0.33 ± 33.06 −0.036 No
H1 0.13 0.002 0.50 0.8 0.28 (0.38) 0.5 (0.3) 0.55 ± 55.09 −0.069 Yes
H2 0.14 0.006 0.49 0.5 0.32 (0.42) 0.5 (0.5) 0.22 ± 22.13 −0.070 Yes
H3 0.14 0.012 0.63 2.3 0.44 (0.64) 0.7 (2.1) 0.20 ± 20.03 −0.067 Yes
H4 0.14 0.018 0.54 3.0 0.32 (0.54) 3.5 (0.9) 0.09 ± 09.04 −0.068 Weak
I1 0.27 0.002 0.59 0.4 0.24 (0.34) 0.4 (0.4) 0.50 ± 50.52 −0.12 Yes
I2 0.28 0.006 0.61 0.4 0.44 (0.58) 0.4 (0.4) 0.56 ± 56.29 −0.12 Yes
I3 0.29 0.013 0.56 1.0 0.42 (0.64) 0.6 (0.5) 0.21 ± 21.08 −0.12 Weak
I4 0.30 0.019 0.59 1.0 0.42 (0.74) 0.7 (1.0) 0.15 ± 15.07 −0.12 Very Weak
J1 0.77 0.003 0.69 0.05 0.20 (0.28) 0.22 (0.22) 0.10 ± 10.29 −0.15 Very weak
J2 0.82 0.007 0.64 0.21 0.21 (0.26) 0.32 (0.32) 0.05 ± 05.10 −0.16 Very weak
J3 0.91 0.014 0.69 0.37 0.23 (0.30) 1.31 (1.31) 0.02 ± 02.12 −0.15 No
J4 0.91 0.021 0.73 0.73 0.31 (0.38) 1.36 (1.36) 0.03 ± 03.10 −0.16 No

Notes. The colatitude is set to θ = 0°, corresponding to the pole. All other quantities are defined in Tables 1 and 2.

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