Table 2
Reformulation of the grid of wind solutions from KK17 (their Table 1), using their stellar parameters, but performing our own self-consistent solutions for the line-force and wind parameters.
| Model | Teff (K) | log g | R* (R⊙) | k | α | δ | v∞ (km s−1) |  |
 |
 |
|---|---|---|---|---|---|---|---|---|---|---|
| Main sequence (V) | ||||||||||
| 325−V | 32.5 | 3.92 | 7.4 | 0.015 ± .001 | 0.672 ± .005 | 0.032 ± .001 | 3330±180 | −8.222 ± .097 | −0.855 | −0.368 |
| 350−V | 35.0 | 3.92 | 8.3 | 0.131 ± .006 | 0.607 ± .004 | 0.090 ± .002 | 2210±120 | −6.783 ± .096 | 0.137 | 0.636 |
| 375−V | 37.5 | 3.92 | 9.4 | 0.169 ± .010 | 0.524 ± .005 | 0.046 ± .002 | 1980±130 | −6.816 ± .101 | −0.293 | 0.143 |
| 400−V | 40.0 | 3.92 | 10.7 | 0.162 ± .009 | 0.495 ± .006 | 0.015 ± .003 | 2040±130 | −6.732 ± .095 | −0.595 | −0.130 |
| 425−V | 42.5 | 3.92 | 12.2 | 0.136 ± .007 | 0.519 ± .005 | 0.013 ± .002 | 2310±130 | −6.380 ± .090 | −0.584 | −0.034 |
| Giants (III) | ||||||||||
| 300−III | 30.0 | 3.49 | 13.1 | 0.048 ± .001 | 0.684 ± .002 | 0.102 ± .001 | 2070 ± 220 | −6.789 ± .111 | 0.007 | 0.419 |
| 325−III | 32.5 | 3.53 | 13.4 | 0.065 ± .002 | 0.680 ± .003 | 0.100 ± .001 | 2100±180 | −6.385 ± .068 | 0.047 | 0.536 |
| 350−III | 35.0 | 3.58 | 13.9 | 0.081 ± .003 | 0.661 ± .004 | 0.085 ± .002 | 2150±140 | −6.111 ± .066 | −0.014 | 0.509 |
| 375−III | 37.5 | 3.63 | 14.4 | 0.092 ± .004 | 0.637 ± .005 | 0.068 ± .002 | 2190±140 | −5.943 ± .070 | −0.120 | 0.433 |
| 400−III | 40.0 | 3.67 | 15.0 | 0.093 ± .004 | 0.615 ± .005 | 0.049 ± .002 | 2170±130 | −5.858 ± .069 | −0.238 | 0.152 |
| 425−III | 42.5 | 3.72 | 15.6 | 0.091 ± .003 | 0.595 ± .004 | 0.031 ± .002 | 2220±130 | −5.810 ± .060 | −0.463 | 0.014 |
| Supergiants (I) | ||||||||||
| 325−I | 32.5 | 3.30 | 21.4 | 0.054± .002 | 0.689 ± .003 | 0.092 ± .002 | 1910±220 | −5.887 ± .081 | 0.120 | 0.463 |
| 350−I | 35.0 | 3.41 | 20.5 | 0.065 ± .002 | 0.674 ± .004 | 0.077 ± .002 | 2100±200 | −5.732 ± .068 | 0.038 | 0.512 |
| 375−I | 37.5 | 3.52 | 19.8 | 0.077 ± .003 | 0.657 ± .004 | 0.065 ± .002 | 2280 ±160 | −5.606 ± .067 | −0.174 | 0.315 |
| 400−I | 40.0 | 3.63 | 19.1 | 0.084± .003 | 0.627 ± .004 | 0.046 ± .002 | 2430 ±140 | −5.629 ± .067 | −0.301 | 0.115 |
| 425−I | 42.5 | 3.75 | 18.5 | 0.096 ± .004 | 0.573 ± .005 | 0.023 ± .002 | 2470±130 | −5.779 ± .068 | −0.527 | −0.034 |
Notes. Differences in logarithm scale on mass-loss rate, compared with both formulae from Vink et al. (2001) and Krtička & Kubát (2017), are included in the last two columns (see also Fig. 5).
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