For PM = 1, Yadav et al. [10] explored various dynamo states by varying F0 in the interval of [1:40]. They observed pure fluid solution (Eb = 0) till F0 = 3.9 after which a constant steady-state magnetic field (Eb > 0) was observed. The critical magnetic Reynolds number Rc M is around 19.9. They also studied the time series of some of the low wavenumber Fourier modes. Fig. 5 exhibits the time series of real part of Bx(0,0,1) for fixed point (F0 = 3.9), a periodic state (F0 = 10), a quasiperiodic state (F0 = 36), and a chaotic state (F0 = 4.8) of the dynamo.
For PM = 1, Yadav et al. [10] explored various dynamo states by varying F0 in the interval of [1:40]. They observed pure fluid solution (Eb = 0) till F0 = 3.9 after which a constant steady-state magnetic field (Eb > 0) was observed. The critical magnetic Reynolds number Rc M is around 19.9. They also studied the time series of some of the low wavenumber Fourier modes. Fig. 5 exhibits the time series of real part of Bx(0,0,1) for fixed point (F0 = 3.9), a periodic state (F0 = 10), a quasiperiodic state (F0 = 36), and a chaotic state (F0 = 4.8) of the dynamo.
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