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The transition to Earth-like torsional oscillations in magnetoconvection simulations

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Figure

Fig. 1. Parameter plots of output parameters against magnetic Ekman number en-compassing all simulations
Fig. 4. Azimuthal velocity, ⟨uφ⟩′ as a function of distance, s, from the rotation axis and time, t, in magnetic diffusion units for the runs of Table 1
Fig. 6. Reynolds force, F R (left column) and Lorentz force, FLD (right column) as a function of distance, s, from the rotation axis and time, t, in magnetic diffusion units.White curves (which are the same curves as those used in Fig
Fig. 7. Parameter space plots of core travel time, τc E , in years against Ekman numberfor various values of the magnetic Prandtl number

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