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Fig. 14

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Space–time evolution of the horizontally averaged azimuthal magnetic field, By, as a function of time in run 1-OA-5-e. The run starts with odd symmetry for the azimuthal field. At t ≃ 1000 Ω-1 a current layer forms and is ejected at t = 1410 Ω-1, leaving an azimuthal field with even symmetry.

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