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Table 1.
Stellar parameters of the model grid with derived values of the terminal velocity v∞ (in km s−1) and the mass-loss rate Ṁ (in M⊙ yr−1).
| Z = Z⊙ | Z = 0.5 Z⊙ |
Z = 0.2 Z⊙ |
||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| C1 = 1 |
C1 = 1 |
C1 = 10 |
C1 = 1 |
C1 = 10 |
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| Model | Teff | R* | v∞ | Ṁ | v∞ | Ṁ | v∞ | Ṁ | v∞ | Ṁ | v∞ | Ṁ |
| [kK] | [R⊙] | |||||||||||
| M = 25 M⊙, log(L/L⊙) = 5.28, Γ = 0.18 | ||||||||||||
| 275-25 | 27.5 | 19.3 | 1890 | 9.1 × 10−8 | 1920 | 7.7 × 10−8 | 2040 | 8.4 × 10−8 | 1880 | 5.9 × 10−8 | 2090 | 6.5 × 10−8 |
| 250-25 | 25.0 | 23.3 | 1640 | 7.5 × 10−8 | 1540 | 6.7 × 10−8 | 1730 | 7.4 × 10−8 | 1340 | 5.5 × 10−8 | 1750 | 5.5 × 10−8 |
| 225-25 | 22.5 | 28.8 | 1130 | 7.4 × 10−8 | 1060 | 6.3 × 10−8 | 1300 | 7.3 × 10−8 | 1240 | 4.6 × 10−8 | 1500 | 5.1 × 10−8 |
| 200-25 | 20.0 | 36.4 | 760 | 7.9 × 10−8 | 1520 | 4.0 × 10−8 | 960 | 1.3 × 10−7 | 1220 | 3.9 × 10−8 | 960 | 5.2 × 10−8 |
| 175-25 | 17.5 | 47.6 | 570 | 1.4 × 10−7 | 380 | 5.9 × 10−8 | 820 | 1.9 × 10−7 | 1020 | 2.5 × 10−8 | 720 | 7.5 × 10−8 |
| 150-25 | 15.0 | 64.8 | 510 | 3.1 × 10−7 | 470 | 1.5 × 10−7 | 510 | 2.6 × 10−7 | 1050 | 1.3 × 10−8 | 670 | 4.5 × 10−8 |
| 125-25 | 12.5 | 93.3 | 120 | 1.7 × 10−7 | 130 | 1.2 × 10−7 | 120 | 1.3 × 10−7 | 120 | 3.5 × 10−8 | 130 | 4.7 × 10−8 |
| 100-25 | 10.0 | 146 | 480 | 8.8 × 10−9 | 410 | 1.1 × 10−8 | 430 | 1.1 × 10−8 | 360 | 8.6 × 10−9 | 430 | 9.6 × 10−9 |
| M = 40 M⊙, log(L/L⊙) = 5.66, Γ = 0.27 | ||||||||||||
| 275-40 | 27.5 | 29.9 | 1300 | 3.4 × 10−7 | 1510 | 2.6 × 10−7 | 1370 | 3.1 × 10−7 | 1670 | 1.4 × 10−7 | 1960 | 2.0 × 10−7 |
| 250-40 | 25.0 | 36.1 | 1600 | 2.0 × 10−7 | 1320 | 1.9 × 10−7 | 1610 | 2.1 × 10−7 | 1170 | 1.5 × 10−7 | 1500 | 1.6 × 10−7 |
| 225-40 | 22.5 | 44.6 | 1160 | 2.0 × 10−7 | 880 | 2.0 × 10−7 | 820 | 2.7 × 10−7 | 860 | 1.6 × 10−7 | 1220 | 1.7 × 10−7 |
| 200-40 | 20.0 | 56.4 | 700 | 2.6 × 10−7 | 670 | 1.9 × 10−7 | 1100 | 4.6 × 10−7 | 930 | 1.1 × 10−7 | 890 | 1.9 × 10−7 |
| 175-40 | 17.5 | 73.7 | 630 | 6.3 × 10−7 | 580 | 3.2 × 10−7 | 520 | 8.6 × 10−7 | 530 | 1.0 × 10−7 | 780 | 2.8 × 10−7 |
| 150-40 | 15.0 | 100 | 110 | 1.5 × 10−6 | 90 | 7.3 × 10−7 | 110 | 1.2 × 10−6 | 60 | 1.5 × 10−7 | 80 | 5.0 × 10−7 |
| 125-40 | 12.5 | 145 | 80 | 6.6 × 10−7 | 100 | 4.3 × 10−7 | 100 | 4.7 × 10−7 | 70 | 1.7 × 10−7 | 110 | 1.9 × 10−7 |
| 100-40 | 10.0 | 226 | 410 | 2.9 × 10−8 | 410 | 3.3 × 10−8 | 440 | 3.4 × 10−8 | 400 | 2.7 × 10−8 | 410 | 2.7 × 10−8 |
| M = 60 M⊙, log(L/L⊙) = 5.88, Γ = 0.30 | ||||||||||||
| 275-60 | 27.5 | 38.5 | 1240 | 6.1 × 10−7 | 1680 | 4.1 × 10−7 | 1520 | 4.9 × 10−7 | 1910 | 3.0 × 10−7 | 1930 | 3.6 × 10−7 |
| 250-60 | 25.0 | 46.5 | 1850 | 3.2 × 10−7 | 1780 | 2.8 × 10−7 | 1720 | 3.4 × 10−7 | 1520 | 2.3 × 10−7 | 1860 | 2.5 × 10−7 |
| 225-60 | 22.5 | 57.5 | 1000 | 3.4 × 10−7 | 880 | 3.1 × 10−7 | 1310 | 4.6 × 10−7 | 940 | 2.6 × 10−7 | 1250 | 2.8 × 10−7 |
| 200-60 | 20.0 | 72.7 | 760 | 4.3 × 10−7 | 650 | 3.2 × 10−7 | 1230 | 8.8 × 10−7 | 1170 | 1.7 × 10−7 | 1080 | 2.7 × 10−7 |
| 175-60 | 17.5 | 95.0 | 820 | 1.2 × 10−6 | 650 | 5.2 × 10−7 | 800 | 1.4 × 10−6 | 1570 | 1.0 × 10−7 | 940 | 2.4 × 10−7 |
| 150-60 | 15.0 | 129 | 490 | 2.1 × 10−6 | 540 | 1.1 × 10−6 | 530 | 1.6 × 10−6 | 460 | 3.9 × 10−7 | 580 | 4.9 × 10−7 |
| 125-60 | 12.5 | 186 | 110 | 1.3 × 10−6 | 150 | 8.1 × 10−7 | 140 | 8.9 × 10−7 | 130 | 3.1 × 10−7 | 140 | 3.8 × 10−7 |
| 100-60 | 10.0 | 291 | 120 | 6.8 × 10−8 | 120 | 6.0 × 10−8 | 120 | 6.2 × 10−8 | 130 | 4.8 × 10−8 | 110 | 4.5 × 10−8 |
Notes. Γ is the Eddington parameter for electron Thomson scattering opacity.
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