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Fig. 21.

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Time evolution of the integral radial scales Λ (Eq. (52)) in three regions I (r ≤ Rdomain/10), II (Rdomain/10 < r ≤ Rdomain/2), and III (r > Rdomain/2) for simulation runs A (full lines), B (dashed lines), and C (dotted lines). The discontinuity of ΛIII for run A is a result of not changing sign on the same radial scales for all φ, that is Rθθ(r′,t) does not cross zero during a few orbital periods.

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