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Fig. 17

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A typical simulation of step (ii) from the procedure described in Sect. 4.2. The initial Bφ has been wound up from the magnetic noise eventually reaching a configuration as in Fig. 16 with w = 100. At the time corresponding to t = 0 in the plot, the constraints on the velocity were removed and the system could evolve freely, cs = 100,N2 ≈ 104.

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