Table 2.
Measured periodicities in the nonlinear simulations (see Sect. 4 for explanation of different measurements).
η | j0 | tc (measured) | P (FFT) | P (reversal) | lc | jc |
---|---|---|---|---|---|---|
0.00003 | 0.1 | 1.99 | 5.46–6.67 | 5.69 | 0.28 | 192.55 |
0.0001 | 0.1 | 2.01 | 5.46–6.67* | 5.60 | 0.28 | 87.38 |
0.0003 | 0.1 | 2.04 | 5.46–6.67 | 5.52 | 0.26 | 37.03 |
0.001 | 0.1 | 2.11 | 5.46–6.67 | 5.56 | 0.24 | 12.72 |
0.0001 | 0.01 | 3.27 | 7.27–8.89 | 7.61 | 0.08 | 12.84 |
0.0001 | 0.05 | 2.38 | 6.15–7.27 | 6.22 | 0.19 | 50.75 |
0.0001 | 0.1 | 2.01 | 5.33–6.15* | 5.60 | 0.28 | 87.38 |
0.0001 | 0.2 | 1.65 | 4.79–5.53 | 4.78 | 0.39 | 145.98 |
Notes. The two η = 10−4, j0 = 0.1 simulations are identical, but slightly different-sized spectral windows are reported above (indicated by the asterisk). This is because the Fourier transforms are performed on the time-series data up to to the lowest end time achieved in each set of simulations, to achieve the same frequency sampling within each group.
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