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Table 3

Results for the runs presented in this paper.

Label 107 × τz ι ϕ σ ϕ n zf

R1-P4 3.94 ± 0.08 0.10 ± 0.2 2.0 ± 2 1.4 ± 0.2 1.5 ± 0.3 6% − 55% 0
R1-P4-C4 3.80 ± 0.10 1.10 ± 0.4 5.0 ± 2 0.7 ± 0.4 0.8 ± 0.3 3% − 81% 0
R1-P3 14.30 ± 0.8 8.00 ± 1 23.0 ± 2 2.8 ± 0.5 3.0 ± 0.6 − 13% − 51% 7
R1-P2 75.00 ± 0.8 27.40 ± 0.6 22.0 ± 2 22.0 ± 8 4.0 ± 2 97% 0% 5
R1-M3 6.50 ± 0.5 2.00 ± 1 4.0 ± 5 10.0 ± 2 3.1 ± 0.7 − 99% 6% 0

R10-P3 24.00 ± 2 8.00 ± 2 18.0 ± 4 40.0 ± 8 21.0 ± 4 96% 6% 9
R10-P2 131.00 ± 6 47.00 ± 6 88.0 ± 35 117.0 ± 44 24.0 ± 9 91% 5% 9
R10-M3 10.50 ± 0.8 8.90 ± 0.7 24.0 ± 3 14.0 ± 3 13.0 ± 3 − 7% 12% 0
R10-M3-C2 23.00 ± 2 17.00 ± 2 43.0 ± 11 18.0 ± 4 19.0 ± 4 12% 73% 0

3D-R1-P4 4.00 ± 0.05 0.74 ± 0.08 2.8 ± 0.4 1.2 ± 0.2 1.2 ± 0.2 4% − 45% 0
3D-R1-P3 18.90 ± 0.3 2.40 ± 0.3 18.7 ± 0.2 2.4 ± 0.8 2.4 ± 0.8 0% − 59% 2
3D-R1-M4 1.09 ± 0.04 0.32 ± 0.06 0.0 ± 0.1 1.3 ± 0.2 1.3 ± 0.2 − 7% 20% 0
3D-R10-P3 16.00 ± 1 8.10 ± 0.5 16.0 ± 5 12.0 ± 2 11.0 ± 2 0% − 24% 2

Notes. The table lists: label of the run; normalized horizontal and vertical stresses, and as defined by Eq. (8), volume-averaged from 3r0 to 8r0; accretion rate due to the vertical stress only τz, as defined in Eq. (9); wind mass loss rates in the southern and northern corona, and , defined by Eq. (10), normalized to the disk mass; symmetry coefficients ιϕ and σϕ, as defined by Eqs. (11)and (12); number of zonal flows identified at the end of the simulation nzf. Except for nzf, all quantities are time-averaged, and the uncertainties are standard deviations over time.

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