Fig. 6.

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Toroidal field Bϕ normalised to the initial amplitude of the poloidal field B0, as a function of (Pm/Lu)2Rec/E and at the particular location θ = π/6 and r = 0.65r0. The different symbols correspond to the different runs D1–D7 of Table 1 (no contraction term in induction equation) namely, Rec = 10−1, Lu = 104 (circle); Rec = 10−1, Lu = 5 × 104 (square); Rec = 1, Lu = 5 × 103 (hexagon); Rec = 1, Lu = 104 (up triangle); Rec = 1, Lu = 5 × 104 (pentagon); Rec = 5, Lu = 104 (down triangle) and Rec = 5, Lu = 5 × 104 (diamond). The other parameters are fixed to E = 10−4, Pr(N0/Ω0)2 = 104, and Pm = 102.
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