Table C.1.
Overview of the stable (or failed) dynamo solutions. All the simulations have the same aspect ratio χ = 0.25, Ekman number E = 10−5, Rossby number Ro = 0.75, thermal and magnetic Prandtl numbers Pr = 0.1 and Pm = 1, and the same resolution (nr, nθ, nϕ) = (256, 256, 512). Note that the run named Ro0.75s is the same as in Barrère et al. (2023). This table displays the input parameter of the runs.
| Name | Pm | N/Ωo | Neff/Ωo | Λi |
|---|---|---|---|---|
| Ro0.75s | 1 | 0.1 | 0.03 | 10 |
| Pm1Pr0.1NO0.25 | 1 | 0.25 | 0.08 | Λ(Ro0.75s) |
| Pm1Pr0.1NO0.5 | 1 | 0.5 | 0.16 | Λ(Ro0.75s) |
| Pm1Pr0.1NO1 | 1 | 1 | 0.32 | Λ(Pm1Pr0.1NO0.5) |
| Pm2Pr0.1NO2 | 2 | 2 | 0.45 | Λ(Pm1Pr0.1NO1) |
| Pm2Pr0.1NO4 | 2 | 4 | 0.89 | Λ(Pm2Pr0.1NO2) |
| Pm2Pr0.1NO8 | 2 | 8 | 1.79 | Λ(Pm2Pr0.1NO4) |
| Pm4Pr0.1NO4 | 4 | 4 | 0.63 | Λ(Pm2Pr0.1NO4) |
| Pm4Pr0.1NO6 | 4 | 6 | 0.95 | Λ(Pm4Pr0.1NO4) |
| Pm4Pr0.1NO8 | 4 | 8 | 1.26 | Λ(Pm2Pr0.1NO8) |
| Pm4Pr0.1NO10 | 4 | 10 | 1.58 | Λ(Pm2Pr0.1NO10) |
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