From: Magnetic field stretching at the top of the shell of numerical dynamos
Model | St/Ad | \({\mathcal {P}}/{\mathcal {T}}\) | \(H_u\) | \({\text {corr}}(|B_r|,\delta _h^-)\) | \({\text {corr}}(|B_r|,\delta _h^+)\) | HN | LN | LR |
---|---|---|---|---|---|---|---|---|
1 | 0.56 ± 0.04 | 0.43 ± 0.03 | 0.84 ± 0.04 | 0.30 ± 0.05 | −0.11 ± 0.02 | 40 | 1 | 10 |
2 | 0.48 ± 0.06 | 0.47 ± 0.03 | 0.78 ± 0.03 | 0.27 ± 0.04 | −0.08 ± 0.03 | 48 | 5 | 19 |
3 | 0.62 ± 0.15 | 0.41 ± 0.01 | 0.84 ± 0.01 | 0.31 ± 0.05 | −0.08 ± 0.02 | 28 | 0 | 5 |
4 | 0.93 ± 0.15 | 0.40 ± 0.03 | 0.88 ± 0.03 | 0.37 ± 0.09 | −0.15 ± 0.04 | 29 | 4 | 3 |
5 | 0.76 ± 0.10 | 0.39 ± 0.02 | 0.87 ± 0.02 | 0.30 ± 0.05 | −0.14 ± 0.03 | 25 | 2 | 1 |
6 | 0.68 ± 0.10 | 0.41 ± 0.03 | 0.85 ± 0.02 | 0.37 ± 0.02 | −0.13 ± 0.02 | 31 | 3 | 6 |
7 | 0.95 ± 0.12 | 0.33 ± 0.01 | 0.87 ± 0.01 | 0.29 ± 0.04 | −0.15 ± 0.02 | 21 | 3 | 3 |
8 | 0.71 ± 0.08 | 0.34 ± 0.02 | 0.84 ± 0.03 | 0.28 ± 0.05 | −0.13 ± 0.01 | 29 | 0 | 2 |
9 | 0.65 ± 0.05 | 0.36 ± 0.01 | 0.80 ± 0.02 | 0.42 ± 0.03 | −0.13 ± 0.01 | 26 | 8 | 6 |