Table 2
Adopted model parameters together with predicted mass loss rates for two clumping stratifications and porosity descriptions.
| Teff | R | log L | M | 3∞ | log Cc | log Ṁ [M⊙ yr-1] | |||||
| (K) | [R⊙] | [L⊙] | [M⊙] | [km s-1] | Cc from vs | Cc from 0.4 3∞ | |||||
| D = 10 | D = 100 | D = 1000 | D = 10 | D = 100 | D = 1000 | ||||||
|
|
|||||||||||
| Dwarfs | |||||||||||
| 30 000 | 6.6 | 4.50 | 12.9 | 2176 | 0.0 | –7.67 | –7.67 | –7.67 | –7.67 | –7.67 | –7.67 |
| 0.5 | –7.97 | –7.71 | –7.67 | –7.84 | –7.67 | –7.65 | |||||
| 1.0 | –8.20 | –7.79 | –7.67 | –7.96 | –7.67 | –7.60 | |||||
| 1.5 | –8.54 | –7.86 | –7.55 | –8.06 | –7.64 | –7.45 | |||||
| 2.0 | –8.95 | –7.93 | –7.36 | –8.01 | –7.54 | –7.19 | |||||
| 40 000 | 10.7 | 5.42 | 34.6 | 2585 | 0.0 | –6.13 | –6.13 | –6.13 | –6.13 | –6.13 | –6.13 |
| 0.5 | –6.46 | –6.22 | –6.19 | –6.37 | –6.16 | –6.13 | |||||
| 1.0 | –6.71 | –6.27 | –6.16 | –6.52 | –6.19 | –6.10 | |||||
| 1.5 | –7.01 | –6.38 | –6.14 | –6.61 | –6.24 | –6.03 | |||||
| 2.0 | –7.34 | –6.52 | –6.17 | –6.64 | –6.22 | –5.94 | |||||
|
|
|||||||||||
| Supergiants | |||||||||||
| 30 000 | 22.4 | 5.56 | 28.8 | 1506 | 0.0 | –5.90 | –5.90 | –5.90 | –5.90 | –5.90 | –5.90 |
| 0.5 | –6.26 | –6.00 | –5.96 | –6.15 | –5.98 | –5.93 | |||||
| 1.0 | –6.41 | –5.97 | –5.87 | –6.28 | –5.91 | –5.81 | |||||
| 1.5 | –6.63 | –5.90 | –5.67 | –6.35 | –5.81 | –5.63 | |||||
| 2.0 | –6.88 | –5.91 | –5.42 | –6.27 | –5.72 | –5.38 | |||||
| 40 000 | 19.1 | 5.93 | 58.1 | 2212 | 0.0 | –5.22 | –5.22 | –5.22 | –5.22 | –5.22 | –5.22 |
| 0.5 | –5.57 | –5.36 | –5.30 | –5.51 | –5.28 | –5.26 | |||||
| 1.0 | –5.79 | –5.44 | –5.35 | –5.64 | –5.32 | –5.22 | |||||
| 1.5 | –6.08 | –5.57 | –5.39 | –5.77 | –5.36 | –5.18 | |||||
| 2.0 | –6.43 | –5.71 | –5.41 | –5.76 | –5.36 | –5.13 | |||||
|
|
|||||||||||
Notes. The scale of the clumps is given by Hρ/D. The clumping laws are: clumping starts at the sonic point (i.e. Cc from vs) and clumping starts at 0.4 3∞ (i.e. Cc up to vs). We again emphasize that the mass-loss rates given here have been calculated assuming that all of the change in wind energy benefits Ṁ. However, e.g. in the case in which clumping and porosity set in at 0.4 3∞ this is highly unlikely; most of the change contributes to 3∞.
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