Table 1
Summary of the runs.
Run | Grid | ![]() |
Pr | PrSGS | PrM | Ta | Ra | Re | Pe | ReM | Co | Γρ | Δt | ![]() |
![]() |
|ΔΩr| | |ΔΩθ| |
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
A1 | 144 × 288 × 576 | 1.0 | 58 | 2.50 | 1.00 | 6.32 × 106 | 6.54 × 107 | 40 | 100 | 40 | 1.6 | 22 | 22 | –0.26 | –0.37 | 0.26 | 0.37 |
A2 | 144 × 288× 576 | 1.0 | 69 | 0.30 | 1.00 | 4.39 × 106 | 8.00 × 105 | 36 | 10 | 36 | 1.4 | 21 | 23 | –0.22 | –0.24 | 0.22 | 0.24 |
B | 144 × 288 × 576 | 1.5 | 58 | 2.50 | 1.00 | 1.42 × 107 | 6.54 × 107 | 40 | 100 | 40 | 2.4 | 22 | 32 | –0.11 | –0.17 | 0.22 | 0.24 |
C1 | 144 × 288 × 576 | 1.8 | 58 | 2.50 | 1.00 | 2.03 × 107 | 6.54 × 107 | 41 | 102 | 41 | 2.8 | 22 | 26 | –0.08 | –0.11 | 0.14 | 0.20 |
C2 | 144 × 288 × 576 | 1.8 | 58 | 1.00 | 1.00 | 2.03 × 107 | 1.29 × 107 | 43 | 43 | 43 | 2.6 | 22 | 45 | 0.78 | –0.35 | 0.13 | 0.17 |
C3 | 144 × 288 × 576 | 1.8 | 77 | 0.33 | 1.00 | 1.14 × 107 | 7.00 × 105 | 28 | 9 | 28 | 3.0 | 20 | 88 | 0.07 | 0.17 | 0.12 | 0.30 |
D | 128 × 256 × 512 | 2.1 | 67 | 3.00 | 1.00 | 2.03 × 107 | 4.55 × 107 | 32 | 98 | 32 | 3.5 | 26 | 29 | 0.003 | 0.007 | 0.008 | 0.01 |
E | 128 × 256 × 512 | 2.9 | 78 | 3.50 | 1.00 | 2.64 × 107 | 3.11 × 107 | 25 | 90 | 25 | 5.0 | 24 | 87 | 0.06 | 0.06 | 0.18 | 0.17 |
F1 | 128 × 256 × 512 | 4.3 | 66 | 3.00 | 1.00 | 8.10 × 107 | 3.31 × 107 | 28 | 86 | 28 | 7.9 | 23 | 33 | 0.01 | 0.04 | 0.06 | 0.15 |
F2 | 144 × 288 × 576 | 4.3 | 57 | 1.00 | 1.00 | 1.17 × 108 | 1.29 × 107 | 33 | 33 | 33 | 8.3 | 19 | 37 | 0.03 | 0.06 | 0.13 | 0.24 |
F3 | 144 × 288 × 576 | 4.3 | 58 | 0.25 | 1.00 | 1.17 × 108 | 9.00 × 105 | 27 | 6 | 27 | 9.8 | 18 | 49 | 0.02 | 0.07 | 0.10 | 0.28 |
Ga | 256 × 512 × 1024 | 4.9 | 43 | 1.20 | 1.00 | 3.47 × 108 | 4.55 × 107 | 50 | 61 | 50 | 9.3 | 21 | 37 | 0.03 | 0.04 | 0.03 | 0.10 |
GW | 180 × 256 × 128 | 4.8 | 67 | 2.00 | 1.00 | 1.25 × 108 | 4.00 × 107 | 34 | 68 | 34 | 8.3 | 31 | 22 | 0.05 | 0.07 | 0.21 | 0.29 |
H | 128 × 256 × 512 | 7.1 | 69 | 3.00 | 1.00 | 2.25 × 108 | 2.04 × 107 | 24 | 72 | 24 | 15.6 | 21 | 200 | 0.01 | 0.03 | 0.10 | 0.20 |
Ha | 256 × 512 × 1024 | 7.8 | 51 | 1.40 | 1.00 | 6.61 × 108 | 5.21 × 107 | 40 | 56 | 40 | 16.1 | 18 | 36 | 0.004 | 0.014 | 0.03 | 0.10 |
I | 128 × 256 × 512 | 9.6 | 71 | 2.08 | 1.04 | 4.63 × 108 | 3.93 × 107 | 26 | 55 | 27 | 20.4 | 28 | 52 | 0.01 | 0.03 | 0.11 | 0.23 |
IW | 128 × 256 × 128 | 9.6 | 71 | 2.08 | 1.04 | 4.63 × 108 | 3.83 × 107 | 27 | 56 | 28 | 19.9 | 28 | 20 | 0.01 | 0.02 | 0.11 | 0.20 |
J | 128 × 256 × 512 | 14.5 | 62 | 2.50 | 1.00 | 1.30 × 109 | 1.12 × 107 | 25 | 63 | 25 | 36.1 | 18 | 62 | –0.001 | 0.01 | 0.01 | 0.14 |
JW | 180 × 256 × 128 | 15.5 | 69 | 2.00 | 1.00 | 1.30 × 109 | 3.93 × 107 | 21 | 43 | 21 | 41.7 | 26 | 53 | 0.004 | 0.009 | 0.05 | 0.13 |
K1 | 128 × 256 × 512 | 21.4 | 74 | 3.00 | 1.00 | 2.03 × 109 | 1.00 × 107 | 16 | 50 | 16 | 67.5 | 13 | 18 | –0.001 | 0.007 | 0.03 | 0.15 |
K2 | 128 × 256 × 512 | 21.4 | 55 | 2.25 | 1.00 | 3.60 × 109 | 1.56 × 107 | 21 | 48 | 21 | 71.2 | 13 | 18 | –0.001 | 0.005 | 0.03 | 0.11 |
La | 256 × 512 × 1024 | 23.3 | 60 | 1.60 | 1.00 | 4.6 × 109 | 4.58 × 107 | 21 | 32 | 21 | 83.4 | 15 | 51 | 1 × 10−4 | 0.002 | 0.003 | 0.04 |
LW | 180 × 256 × 128 | 23.3 | 70 | 2.00 | 1.00 | 2.92 × 109 | 4.00 × 107 | 16 | 33 | 16 | 82.4 | 24 | 53 | − 1 × 10−4 | 0.003 | 0.002 | 0.07 |
M | 128 × 256 × 512 | 28.5 | 61 | 2.50 | 1.00 | 5.18 × 109 | 6.00 × 106 | 18 | 46 | 18 | 98.7 | 9 | 24 | –0.001 | 0.003 | 0.02 | 0.10 |
Ma | 256 × 512 × 1024 | 28.5 | 31 | 2.50 | 1.00 | 2.07 × 1010 | 1.48 × 105 | 33 | 82 | 33 | 109.9 | 15 | 33 | − 7 × 10−5 | 9 × 10−4 | 0.002 | 0.03 |
MW | 180 × 256 × 128 | 31.0 | 71 | 2.00 | 1.00 | 5.18 × 109 | 1.03 × 108 | 14 | 28 | 14 | 126.5 | 21 | 49 | − 1 × 10−4 | 0.002 | 0.003 | 0.07 |
Notes. The quantities in the Cols. (2) to (8) are input parameters of the runs whereas the quantities from Cols. (9) to (18) are outcomes of the simulations. Superscripts a denote high-resolution runs and superscripts W denote π∕2 wedges. The horizontal line denotes the transition from axisymmetric (antisolar) magnetic field (rotation profile) to a nonaxisymmetric (solar) field (rotation profile). The Δ t value indicates the time span of the saturated stage in years. The and
values indicate the relative radial and latitudinal differential rotation, see Eq. (16), whereas |ΔΩr | and |ΔΩθ | are the absolute radial and latitudinal differential rotation; see Eq. (17).
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