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Table 3.

Similar to Table 1, but for the 2D hydromagnetic simulations analyzed in Sect. 6. Here kp/k1 = 200.

Run ηk1/cs νk1/cs PrM Lu CM C L ( 1 / 4 ) $ C_{\mathrm{L}}^{(1/4)} $ Cξ Cℰ τξ τℰ ϵK/ϵM MaA N2
2m1 5 × 10−9 5 × 10−7 100 75 000 36.7 ± 4.6 2.2 221 0.164 0.34 1.26 13 0.41 16 3842
2m2 2 × 10−9 2 × 10−7 100 182 000 39.5 ± 1.0 1.9 241 0.164 0.41 1.25 21 0.43 16 3842
2m3 1 × 10−9 1 × 10−7 100 358 000 42.7 ± 1.7 1.7 254 0.168 0.46 1.30 33 0.44 16 3842
2m4 1 × 10−9 2 × 10−8 20 356 000 43.8 ± 2.5 1.8 248 0.175 0.50 1.50 11 0.44 81922
2m5 2 × 10−9 2 × 10−8 10 178 000 43.9 ± 3.0 2.1 247 0.177 0.49 1.53 6.0 0.44 81922
2m6 2 × 10−9 2 × 10−8 10 178 000 45.3 ± 1.8 2.2 254 0.178 0.47 1.45 6.0 0.44 16 3842
2M1 4 × 10−9 2 × 10−8 5 90 800 42.5 ± 2.1 2.4 241 0.175 0.47 1.34 3.5 0.45 81922
2M2 2 × 10−8 1 × 10−7 5 19 000 36.8 ± 2.6 3.1 217 0.169 0.37 1.40 2.9 0.45 81922
2M3 1 × 10−7 5 × 10−7 5 3900 30.2 ± 2.0 3.8 191 0.157 0.34 1.36 1.5 0.42 40962
2M4 1 × 10−7 5 × 10−7 5 770 18.9 ± 0.6 3.6 347 0.054 1.30 3.66 0.8 0.42 40962
2M5 1 × 10−9 1 × 10−9 1 365 000 44.1 ± 1.8 1.8 252 0.175 0.52 1.49 0.7 0.44 81922
2M6 5 × 10−9 5 × 10−9 1 72 300 39.9 ± 1.9 2.4 232 0.171 0.43 1.43 0.8 0.46 81922
2M7 2 × 10−8 2 × 10−8 1 18 700 36.8 ± 1.7 3.1 233 0.157 0.44 1.23 0.8 0.46 81922
2M8 1 × 10−7 1 × 10−7 1 3830 31.0 ± 0.7 3.9 213 0.146 0.35 1.07 0.7 0.45 81922
2M9 5 × 10−7 5 × 10−7 1 742 18.7 ± 0.8 3.6 156 0.119 0.22 0.83 0.5 0.51 40962
2M10 5 × 10−7 5 × 10−7 1 125 10.0 ± 0.4 3.0 284 0.035 0.83 1.66 0.5 0.63 40962

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