Table 2
Parameters for the simulation setup.
| Type | z↓(*) (ztot) (Mm) | x0, y0 (Mm) | ∆x, y (km) | ∆z (km) | log10 g (cm s−2) | (Teff)hd(*) (K) | (Teff)SSD(*) (K) | 〈‖В‖〉τ=1(*) (G) | 〈∣Bz∣〉τ=1(*) (G) | 〈‖В‖〉τ=1(*) (G) |
|---|---|---|---|---|---|---|---|---|---|---|
| F3V | 11.11 (13.00) | 23 | 45 | 26 | 4.301 | 6817 ± 7 | 6807 ± 8 | 188 ± 15 | 93 ± 8 | 132 ± 10 |
| G2V | 4.09 (5.00) | 9 | 17.5 | 10 | 4.438 | 5834 ± 9 | 5840 ± 9 | 127 ± 12 | 66 ± 6 | 113 ± 10 |
| K0V | 2.05 (2.31) | 4.62 | 8.2 | 4.62 | 4.609 | 4668 ± 5 | 4671 ± 5 | 103 ± 6 | 50 ± 3 | 103 ± 6 |
| M0V | 0.90 (1.14) | 2.043 | 3.99 | 2.28 | 4.826 | 3825 ± 1 | 3827 ± 2 | 106 ± 6 | 54 ± 4 | 107 ± 6 |
Notes.(*) These quantities are determined after running the simulations. The change in Teff will not influence the total radiative output on long timescales (>105 yr) corresponding to the Kelvin-Helmholtz timescale. See Spruit (1982) for details.
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