Table 1.
Input parameters and output diagnostics of the numerical simulation runs (see main text for definitions).
| Name | δ0 | Lu0 | Pr ⋅ 102 | t1 ωA0 | ![]() |
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|---|---|---|---|---|---|---|---|
| TU0(1) | 0 | 917 | – | 26.6 | 0 | 677 | 1.09 |
| TU1 | 0 | 611 | – | 50.6 | 0 | 406 | 1.09 |
| TU2 | 0 | 367 | – | 31.5 | 0 | 242 | 1.06 |
| TU3 | 0 | 244 | – | 51.4 | 0 | 122 | 0.90 |
| TU4 | 0 | 122 | – | 61.6 | 0 | 30 | 0.28 |
| TU5 | 0 | 61 | – | 40.9 | 0 | 10 | Stable |
| TU6 | 0 | 31 | – | 26.1 | 0 | 3 | Stable |
| TS1(1) | 8 | 917 | 1 | 24.3 | 3.5 | 681 | 0.94 |
| TS2(1) | 63 | 917 | 1 | 24.2 | 27 | 682 | 0.77 |
| TS3(1) | 126 | 917 | 1 | 26.0 | 54 | 680 | 0.60 |
| TS4(1) | 209 | 917 | 1 | 25.2 | 90 | 681 | 0.43 |
| TS5(1) | 300 | 917 | 1 | 26.9 | 130 | 678 | 0.28 |
| TS6(1, 2) | 419 | 917 | 1 | 24.5 | 180 | 682 | 0.16 |
| TS7(1) | 628 | 917 | 1 | 27.7 | 272 | 678 | 0.07 |
| TS8(1) | 900 | 917 | 1 | 27.3 | 321 | 678 | 0.04 |
| TS9(2) | 419 | 458 | 2 | 11.6 | 180 | 342 | Stable |
| TS10(2) | 419 | 1833 | 0.5 | 46.0 | 180 | 1367 | 0.47 |
| TS11(2) | 419 | 3667 | 0.25 | 91.2 | 180 | 2735 | 0.68 |
| TS12(2) | 419 | 7333 | 0.125 | 173.2 | 180 | 5481 | 0.85 |
| TS13 | 628 | 458 | 2 | 13.8 | 272 | 339 | Stable |
| TS14 | 739 | 306 | 3 | 9.3 | 321 | 226 | Stable |
| TS15 | 739 | 397 | 2.31 | 12.1 | 321 | 293 | Stable |
| TS16 | 739 | 611 | 1.5 | 18.3 | 321 | 452 | Stable |
| TS17 | 63 | 57 | 16 | 1.7 | 27 | 42 | Stable |
| TS18 | 63 | 458 | 2 | 12.7 | 27 | 340 | 0.55 |
Notes. Superscripts (1) and (2) in the run names indicate a run pertaining to the simulation subsets 1 and 2, respectively (see Fig. 9). The time at which the nonaxisymmetric perturbations are introduced is t1. The final column reports the growth rate of the m = 1 mode, with “Stable” indicating decaying perturbations. All runs have a magnetic Prandtl number of Pm = 1. For all stratified runs, the ratio of the thermal diffusion rate to the mean Alfvén frequency at the perturbation time is
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