Table 9
Upper part of the VMS model grid: mass loss rates extrapolated from the predictions by Kudritzki (2002) (ṀK02) versus our values (Ṁov).
| log L∗ | Teff | M∗ | Z∗ | ṀK02 | Ṁov | |
| (L⊙) | (K) | (M⊙) | (Z⊙) | (10-6 M⊙/yr) | (10-6 M⊙/yr) | |
|
|
||||||
| 8.0 | 65 000 | 3000 | 1 | 95 050 | 385 | |
| 45 000 | 3000 | 1 | 95 050 | 923 | ||
| 30 000 | 3000 | 1 | 95 050 | 1025 | ||
| 8.0 | 65 000 | 3000 | 0.05 | 95 050 | 132 | |
| 45 000 | 3000 | 0.05 | 95 050 | 285 | ||
| 30 000 | 3000 | 0.05 | 24 103 | 179 | ||
| 7.5 | 65 000 | 1000 | 1 | 76 740 | 98 | |
| 45 000 | 1000 | 1 | 14 130 | 190 | ||
| 30 000 | 1000 | 1 | 12 810 | 250 | ||
| 7.5 | 65 000 | 1000 | 0.05 | 17 650 | 35 | |
| 45 000 | 1000 | 0.05 | 3250 | 53 | ||
| 30 000 | 1000 | 0.05 | 2946 | 34 | ||
| 7.03 | 50 000 | 600 | 1 | 530 | 34 | |
| 7.03 | 50 000 | 600 | 0.05 | 120 | 6 | |
Notes. As in the work of Belkus et al. (2007), for those models for which this extrapolation predicts mass loss rates in excess of the upper limit given by Owocki et al. (2004), we have used the upper limit instead. Note that the true mass loss rates (Ṁov) are significantly lower than the extrapolated values.
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