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Table 1.

Summary of magnetohydrodynamic simulations analyzed in this paper.

Run ηk1/cs νk1/cs PrM Lu Luν CM C L ( 1 / 4 ) $ C_{\mathrm{L}}^{(1/4)} $ Cξ C τξ τ ​​ϵK/ϵM​​ MaA N3
M0 4 × 10−7 4 × 10−6 10 5400 1600 36.0 ± 1.4 4.2 91 0.39 0.82 0.28 0.9 0.20 20483
M1 4 × 10−7 2 × 10−6 5 5830 2600 30.5 ± 0.8 3.5 87 0.35 0.72 0.23 0.9 0.24 20483
M2 1 × 10−6 2 × 10−6 2 2354 1660 26.2 ± 0.3 3.8 81 0.32 0.63 0.20 0.6 0.28 20483
M3 1 × 10−6 5 × 10−6 5 2186 980 25.6 ± 0.6 3.7 80 0.32 0.74 0.22 0.8 0.25 10243
M4 2.5 × 10−6 5 × 10−6 2 823 580 20.1 ± 0.5 3.7 73 0.27 0.61 0.17 0.6 0.31 10243
M5 5 × 10−6 5 × 10−6 1 386 386 14.5 ± 0.7 3.3 64 0.23 0.45 0.12 0.5 0.38 10243

Notes. The time unit of τξ and τ is [t]=(csk1)−1.

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