Table 3
Summary of the runs.
| Run | a | b | n |
|
ztop | zτ = 1 | ρτ = 1 | τadjust | Teff | Kbot | |
|
|
|||||||||||
| A4 | 1 | −3.5 | 3.25 | 104 | 8 | 2.8 | 1.0 × 10-4 | 50 | 23 600 | 3.9 × 10-6 | |
| A5 | 1 | −3.5 | 3.25 | 105 | 8 | 5.2 | 1.7 × 10-5 | 90 | 13 900 | 4.6 × 10-7 | |
| A6 | 1 | −3.5 | 3.25 | 106 | 8 | 6.6 | 2.5 × 10-6 | 700 | 7800 | 4.6 × 10-8 | |
| A7 | 1 | −3.5 | 3.25 | 107 | 8 | 7.4 | 3.7 × 10-7 | 15 000 | 4400 | 4.4 × 10-9 | |
|
|
|||||||||||
| B4 | 1 | 0 | 1.5 | 104 | 5 | 1.4 | 2.2 × 10-4 | 40 | 26 600 | 4.53 × 10-6 | |
| B5 | 1 | 0 | 1.5 | 105 | 5 | 2.9 | 9.0 × 10-5 | 60 | 16 300 | 5.15 × 10-7 | |
| B6 | 1 | 0 | 1.5 | 106 | 5 | 3.8 | 3.7 × 10-5 | 400 | 9300 | 5.38 × 10-8 | |
| B7 | 1 | 0 | 1.5 | 107 | 5 | 4.3 | 1.6 × 10-5 | 5000 | 5200 | 5.08 × 10-9 | |
|
|
|||||||||||
| C4 | 1 | 1 | 1 | 104 | 4 | 1 | 2.6 × 10-4 | 7 | 27 600 | 5.1 × 10-6 | |
| C5 | 1 | 1 | 1 | 105 | 4 | 2.3 | 1.3 × 10-4 | 20 | 17 400 | 5.6 × 10-7 | |
| C6 | 1 | 1 | 1 | 106 | 4 | 3.1 | 7.0 × 10-5 | 200 | 10 100 | 6.0 × 10-8 | |
| C7 | 1 | 1 | 1 | 107 | 4 | 3.4 | 3.9 × 10-5 | 2100 | 5700 | 6.1 × 10-9 | |
|
|
|||||||||||
| D4 | 1 | 5 | −1 | 104 | 2 | 0.2 | 3.6 × 10-4 | 6 | 31 000 | 1.1 × 10-5 | |
| D5 | 1 | 5 | −1 | 105 | 2 | 0.8 | 2.8 × 10-4 | 7 | 23 100 | 1.3 × 10-6 | |
| D6 | 1 | 5 | −1 | 106 | 2 | 1 | 2.8 × 10-4 | 80 | 15 600 | 1.9 × 10-7 | |
| D7 | 1 | 5 | −1 | 107 | 2 | 1 | 3.2 × 10-4 | 700 | 10100 | 3.1 × 10-8 | |
|
|
|||||||||||
| E4 | −1 | 3 | 0/0 | 104 | 4 | 3.0 | 8.7 × 10-5 | 6 | 23 700 | 4.47 × 10-6 | |
| E5 | −1 | 3 | 0/0 | 105 | 4 | 3.6 | 5.6 × 10-5 | 45 | 14 900 | 4.47 × 10-7 | |
| E6 | −1 | 3 | 0/0 | 106 | 4 | 3.8 | 3.9 × 10-5 | 400 | 8800 | 4.47 × 10-8 | |
Notes. The size of the domain ztop and the height of the surface zτ = 1 are in Mm, the density at the surface ρτ = 1 is in g cm-3, the thermal adjustment time τadjust is in ks, the effective temperature Teff is in K, radiative heat conductivity at the bottom of the domain Kbot is in g cm-3 km3 s-3 Mm K-1 and the normalized opacity 
is in Mm-1 cm3 g-1 are shown for each run. The second to the sixth columns show quantities which are input parameters to the models whereas the quantities in last five columns are the results of the simulations, computed from the equilibrium state.
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