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Fig. 5

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(a) Azimuthal velocity field shown on both spherical surfaces and meridional cross-sections at ϕ=0 and 3 π/2 at time t=0.53 tη. The flow takes the form of a strong prograde equatorial surface jet, with retrograde motion near the poles and in the interior. (b) Spatial structure of the magnetic field, with br shown on the outer boundary, and ∣b∣ in the interior. The radial field at the surface is strongly dipolar, and the interior field shows very localised activity. The surface field is much weaker than in the interior.

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