From: Magnetic field stretching at the top of the shell of numerical dynamos
Model | Patch type | St/Ad | \({\mathcal {P}}/{\mathcal {T}}\) | \(H_u\) | \({\text{corr}}(|B_r|,\delta _h^-)\) | \({\text{corr}}(|B_r|,\delta _h^+)\) | \(\xi _{a}\) | \(\xi _{s}\) | \(\xi _{\text {e}}\) |
---|---|---|---|---|---|---|---|---|---|
1 | HN | 0.69 ± 0.23 | 0.34 ± 0.05 | 0.91 ± 0.11 | 0.44 ± 0.19 | −0.28 ± 0.08 | 0.44 ± 0.09 | 0.76 ± 0.09 | 0.92 ± 0.09 |
LN | 0.28 ± 0.00 | 0.60 ± 0.00 | 0.70 ± 0.00 | 0.38 ± 0.00 | −0.34 ± 0.00 | 0.11 ± 0.00 | 0.31 ± 0.00 | 0.62 ± 0.00 | |
LR | 0.48 ± 0.14 | 0.63 ± 0.11 | 0.79 ± 0.19 | 0.42 ± 0.17 | −0.18 ± 0.13 | 0.07 ± 0.04 | 0.20 ± 0.06 | 0.68 ± 0.13 | |
2 | HN | 0.55 ± 0.21 | 0.40 ± 0.07 | 0.83 ± 0.09 | 0.29 ± 0.19 | −0.19 ± 0.09 | 0.28 ± 0.09 | 0.59 ± 0.18 | 0.77 ± 0.20 |
LN | 0.33 ± 0.10 | 0.59 ± 0.12 | 0.71 ± 0.23 | 0.43 ± 0.24 | −0.17 ± 0.13 | 0.11 ± 0.06 | 0.38 ± 0.16 | 0.56 ± 0.22 | |
LR | 0.43 ± 0.16 | 0.79 ± 0.14 | 0.59 ± 0.22 | 0.28 ± 0.22 | −0.04 ± 0.19 | 0.11 ± 0.08 | 0.25 ± 0.13 | 0.62 ± 0.19 | |
3 | HN | 0.60 ± 0.19 | 0.33 ± 0.05 | 0.91 ± 0.03 | 0.30 ± 0.18 | −0.19 ± 0.11 | 0.24 ± 0.08 | 0.56 ± 0.16 | 0.87 ± 0.06 |
LN | – | – | – | – | – | – | – | – | |
LR | 0.65 ± 0.27 | 0.61 ± 0.06 | 0.82 ± 0.09 | 0.60 ± 0.14 | −0.20 ± 0.03 | 0.26 ± 0.08 | 0.52 ± 0.13 | 0.84 ± 0.09 | |
4 | HN | 1.27 ± 0.51 | 0.32 ± 0.07 | 0.87 ± 0.20 | 0.71 ± 0.10 | −0.39 ± 0.11 | 0.63 ± 0.13 | 0.61 ± 0.13 | 0.85 ± 0.09 |
LN | 1.10 ± 0.29 | 0.39 ± ± 0.02 | 0.91 ± 0.05 | 0.78 ± 0.03 | −0.48 ± 0.08 | 0.58 ± 0.14 | 0.35 ± 0.09 | 0.57 ± 0.11 | |
LR | 0.24 ± 0.01 | 0.69 ± 0.01 | 0.52 ± 0.06 | −0.23 ± 0.06 | 0.14 ± 0.01 | 0.06 ± 0.00 | 0.28 ± 0.02 | 0.24 ± 0.01 | |
5 | HN | 0.95 ± 0.30 | 0.32 ± 0.05 | 0.83 ± 0.14 | 0.54 ± 0.13 | −0.35 ± 0.06 | 0.57 ± 0.14 | 0.75 ± 0.08 | 0.93 ± 0.04 |
LN | 0.43 ± 0.00 | 0.42 ± 0.00 | 0.91 ± 0.00 | 0.57 ± 0.00 | −0.22 ± 0.00 | 0.47 ± 0.00 | 0.72 ± 0.00 | 0.94 ± 0.00 | |
LR | 0.72 ± 0.00 | 0.86 ± 0.00 | 0.71 ± 0.00 | 0.49 ± 0.00 | −0.23 ± 0.00 | 0.09 ± 0.00 | 0.16 ± 0.00 | 0.67 ± 0.00 | |
6 | HN | 0.74 ± 0.15 | 0.34 ± 0.05 | 0.91 ± 0.04 | 0.40 ± 0.18 | −0.27 ± 0.10 | 0.39 ± 0.07 | 0.69 ± 0.11 | 0.87 ± 0.10 |
LN | 0.69 ± 0.15 | 0.60 ± 0.07 | 0.91 ± 0.01 | 0.54 ± 0.18 | −0.18 ± 0.00 | 0.12 ± 0.10 | 0.32 ± 0.26 | 0.82 ± 0.04 | |
LR | 0.68 ± 0.13 | 0.73 ± 0.31 | 0.85 ± 0.06 | 0.54 ± 0.18 | −0.19 ± 0.03 | 0.11 ± 0.06 | 0.17 ± 0.08 | 0.76 ± 0.09 | |
7 | HN | 1.18 ± 0.28 | 0.28 ± 0.08 | 0.80 ± 0.15 | 0.54 ± 0.13 | −0.30 ± 0.07 | 0.59 ± 0.09 | 0.62 ± 0.08 | 0.89 ± 0.06 |
LN | 0.81 ± 0.20 | 0.40 ± 0.01 | 0.91 ± 0.02 | 0.54 ± 0.16 | −0.25 ± 0.12 | 0.55 ± 0.06 | 0.51 ± 0.05 | 0.74 ± 0.04 | |
LR | 1.12 ± 0.12 | 0.58 ± 0.01 | 0.81 ± 0.04 | 0.48 ± 0.06 | −0.09 ± 0.02 | 0.08 ± 0.06 | 0.04 ± 0.04 | 0.67 ± 0.05 | |
8 | HN | 0.78 ± 0.20 | 0.27 ± 0.04 | 0.83 ± 0.12 | 0.45 ± 0.15 | −0.30 ± 0.06 | 0.50 ± 0.12 | 0.68 ± 0.08 | 0.89 ± 0.06 |
LN | – | – | – | – | – | – | – | – | |
LR | 0.93 ± 0.00 | 0.94 ± 0.00 | 0.60 ± 0.00 | 0.57 ± 0.00 | −0.18 ± 0.00 | 0.14 ± 0.00 | 0.20 ± 0.00 | 0.63 ± 0.00 | |
9 | HN | 0.68 ± 0.15 | 0.31 ± 0.06 | 0.81 ± 0.11 | 0.48 ± 0.18 | −0.24 ± 0.07 | 0.32 ± 0.06 | 0.63 ± 0.07 | 0.84 ± 0.04 |
LN | 0.61 ± 0.13 | 0.45 ± 0.07 | 0.82 ± 0.04 | 0.51 ± 0.05 | −0.23 ± 0.04 | 0.28 ± 0.05 | 0.54 ± 0.07 | 0.83 ± 0.02 | |
LR | 0.85 ± 0.09 | 0.67 ± 0.17 | 0.70 ± 0.06 | 0.55 ± 0.19 | −0.22 ± 0.07 | 0.20 ± 0.20 | 0.25 ± 0.25 | 0.88 ± 0.07 | |
\(\bar{x}\) | HN | 0.82 | 0.32 | 0.86 | 0.46 | −0.28 | 0.44 | 0.65 | 0.90 |
LN | 0.61 | 0.49 | 0.84 | 0.53 | −0.27 | 0.32 | 0.45 | 0.73 | |
LR | 0.68 | 0.72 | 0.71 | 0.42 | −0.13 | 0.13 | 0.23 | 0.66 |