Table 2
Summary of the properties of the statistically-steady nonlinear dynamo calculations.
Run | ζ0 | Urms | Re | Rm | Pm |
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A1 | 0.111 | 0.304 | 89 | 500 | 5.62 | 0.031 | 0.076 |
A2 | 0.125 | 0.337 | 149 | 492 | 3.30 | 0.024 | 0.047 |
A3 | 0.136 | 0.385 | 339 | 517 | 1.53 | 0.020 | 0.025 |
A4 | 0.15 | 0.409 | 479 | 498 | 1.04 | 0.012 | 0.008 |
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B1 | 0.15 | 0.303 | 89 | 369 | 4.15 | 0.031 | 0.059 |
B2 | 0.15 | 0.336 | 148 | 409 | 2.76 | 0.029 | 0.048 |
B3 | 0.15 | 0.378 | 333 | 460 | 1.38 | 0.028 | 0.037 |
B4 | 0.15 | 0.390 | 458 | 475 | 1.04 | 0.027 | 0.030 |
Notes. The convective flows correspond to those given in Table 1. As before, Urms corresponds to the time-averaged rms velocity, and both Re and Rm have been derived from this. The quantity corresponds to the horizontally-averaged value of the modulus of Bz at the surface, Beq,0 is the equipartition field strength at z = 0, whilst KE and ME represent the total kinetic and magnetic energies respectively. All of these quantities have also been time-averaged.
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