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Table 1.

Summary of the dimensionless parameters that characterize the simulations.

Run Ω/Ω cf Co Ta Re ReM Pe
C1 20 0 57.2 2.53(9) 22.1 22.1 55.3 0 9.16(−4) 3.42(−3) 4.26(−4) 5.02(−4)
C2 20 1.0(−4) 55.6 2.53(9) 22.8 22.8 57.0 8.75(−1) 9.27(−4) 3.60(−3) 4.62(−4) 5.30(−4)
C3 20 1.0(−4) 56.7 2.53(9) 22.3 22.3 55.8 8.75(−1) 8.40(−4) 3.66(−3) 6.23(−4) 6.28(−4)
D1 30 0 137.9 5.72(9) 13.8 13.8 34.6 0 −2.51(−4) 4.51(−4) 8.05(−5) 1.23(−4)
D2 30 1.0(−4) 137.8 5.72(9) 13.8 13.8 34.8 8.75(−1) −2.42(−4) 4.75(−4) 1.15(−4) 1.54(−4)
D3 30 1.0(−3) 130.1 5.72(9) 14.6 14.6 36.6 8.75 −6.34(−5) 8.70(−4) 1.52(−4) 2.39(−4)

Notes. Co is the Coriolis number, Ta is the Taylor number, Re and ReM are the fluid and magnetic Reynolds numbers, and Pe is the Péclet number. For each run, Pr = 60, PrM = 1, and PrSGS = 2.5. denote the radial and latitudinal differential rotation and are defined in Eqs. (21) and (22), respectively. ⟨...⟩t denotes averages over time, and the prime denotes fluctuating quantities.

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