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Fig. 19

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Surface-averaged Br scaled by the volume-averaged Bφ in dependence on the strength of the initial toroidal field (represented by w which is determined by the time of winding up the field in step (i), Sect. 4.2). The values of Br and Bφ were calculated for the flow soon after saturation, at t = 0.1   [2π0]  (corresponding to the rightmost side of Fig. 17).

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