Table 1.
Self-consistent line-force parameters (k, α, δ) calculated for the stellar parameters corresponding to the positions indicated by circles in Fig. 1, together with their resulting terminal velocities and mass-loss rates (Ṁsc).
| Input stellar parameters |
|||||||||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Name | Teff | log g | R* | M* | log L* | He/H | C/C⊙ | N/N⊙ | O/O⊙ | Ω | k | α | δ | v∞ | log Ṁsc |
 |
 |
| [kK] | [R⊙] | [M⊙] | [L⊙] | [km s−1] | [M⊙ yr−1] | ||||||||||||
| P120z10-01 | 52.0 | 4.12 | 15.8 | 120.0 | 6.22 | 0.085 | 1.0 | 1.0 | 1.0 | 0.0 | 0.125 | 0.566 | 0.026 | 3520 ± 110 | −5.455 ± .100 | ||
| 0.4 | 0.113 | 0.578 | 0.025 | 3320 ± 110 | −5.417 ± .100 | 1.090 | 1.092 | ||||||||||
| P120z10-02 | 50.5 | 4.03 | 17.2 | 115.9 | 6.23 | 0.087 | 0.73 | 3.12 | 0.87 | 0.0 | 0.105 | 0.584 | 0.024 | 3360 ± 110 | −5.407 ± .063 | ||
| 0.32 | 0.105 | 0.586 | 0.025 | 3230 ± 110 | −5.387 ± .063 | 1.057 | 1.056 | ||||||||||
| P120z10-03 | 52.0 | 4.01 | 16.9 | 106.5 | 6.27 | 0.155 | 0.08 | 11.66 | 0.09 | 0.0 | 0.106 | 0.584 | 0.028 | 3190 ± 100 | −5.312 ± .065 | ||
| 0.18 | 0.104 | 0.586 | 0.028 | 3150 ± 100 | −5.307 ± .067 | 1.013 | 1.013 | ||||||||||
| P120z10-04 | 54.0 | 4.00 | 16.3 | 96.1 | 6.31 | 0.308 | 0.05 | 12.35 | 0.02 | 0.0 | 0.101 | 0.573 | 0.025 | 2900 ± 110 | −5.314 ± .073 | ||
| 0.07 | 0.100 | 0.573 | 0.025 | 2890 ± 110 | −5.312 ± .065 | 1.004 | 1.002 | ||||||||||
| P070z10-01 | 49.0 | 4.18 | 11.3 | 70 | 5.82 | 0.085 | 1.0 | 1.0 | 1.0 | 0.0 | 0.159 | 0.537 | 0.027 | 3100 ± 100 | −5.999 ± .081 | ||
| 0.4 | 0.143 | 0.547 | 0.026 | 2 930 ± 100 | −5.969 ± .073 | 1.072 | 1.078 | ||||||||||
| P070z10-02 | 47.0 | 4.06 | 12.7 | 67.8 | 5.85 | 0.085 | 0.94 | 1.45 | 0.97 | 0.0 | 0.154 | 0.557 | 0.023 | 3030 ± 100 | −5.826 ± .070 | ||
| 0.34 | 0.144 | 0.565 | 0.022 | 2910 ± 100 | −5.803 ± .069 | 1.054 | 1.050 | ||||||||||
| P070z10-03 | 47.0 | 3.98 | 13.6 | 63.7 | 5.91 | 0.116 | 0.40 | 7.51 | 0.47 | 0.0 | 0.135 | 0.576 | 0.026 | 2960 ± 100 | −5.686 ± .079 | ||
| 0.22 | 0.131 | 0.580 | 0.025 | 2900 ± 100 | −5.672 ± .070 | 1.029 | 1.022 | ||||||||||
| P070z10-04 | 49.0 | 3.97 | 13.3 | 59.8 | 5.96 | 0.199 | 0.15 | 10.86 | 0.16 | 0.0 | 0.112 | 0.574 | 0.029 | 2700 ± 100 | −5.711 ± .068 | ||
| 0.13 | 0.111 | 0.575 | 0.029 | 2710 ± 100 | −5.708 ± .068 | 1.007 | 1.006 | ||||||||||
| P070z10-05 | 52.5 | 3.97 | 12.5 | 53.3 | 6.03 | 0.481 | 0.05 | 12.24 | 0.03 | 0.0 | 0.105 | 0.560 | 0.027 | 2440 ± 100 | −5.659 ± .073 | ||
| 0.05 | 0.104 | 0.561 | 0.027 | 2440 ± 100 | −5.658 ± .067 | 1.002 | 1.001 | ||||||||||
| P040z10-01 | 43.5 | 4.22 | 8.1 | 40.0 | 5.33 | 0.085 | 1.0 | 1.0 | 1.0 | 0.0 | 0.247 | 0.468 | 0.019 | 2410 ± 110 | −6.874 ± .110 | ||
| 0.4 | 0.214 | 0.479 | 0.018 | 2280 ± 150 | −6.849 ± .146 | 1.059 | 1.069 | ||||||||||
| P040z10-02 | 42.0 | 3.99 | 10.4 | 38.6 | 5.43 | 0.086 | 0.91 | 1.75 | 0.95 | 0.0 | 0.175 | 0.488 | 0.013 | 2180 ± 100 | −6.742 ± .103 | ||
| 0.34 | 0.160 | 0.498 | 0.014 | 2090 ± 100 | −6.709 ± .093 | 1.076 | 1.049 | ||||||||||
| P040z10-03 | 39.5 | 3.72 | 13.6 | 35.5 | 5.60 | 0.157 | 0.41 | 7.51 | 0.46 | 0.0 | 0.108 | 0.560 | 0.028 | 2050 ± 110 | −6.268 ± .075 | ||
| 0.16 | 0.106 | 0.562 | 0.029 | 2030 ± 110 | −6.263 ± .073 | 1.010 | 1.008 | ||||||||||
| P040z10-04 | 36.0 | 3.44 | 18.1 | 33.0 | 5.69 | 0.264 | 0.26 | 9.54 | 0.28 | 0.0 | 0.072 | 0.648 | 0.068 | 1990 ± 160 | −5.855 ± .050 | ||
| 0.04 | 0.072 | 0.649 | 0.069 | 1990 ± 160 | −5.850 ± .050 | 1.010 | 1.001 | ||||||||||
| P040z10-05 | 32.0 | 3.19 | 23.9 | 32.1 | 5.73 | 0.289 | 0.24 | 9.79 | 0.26 | 0.0 | 0.050 | 0.700 | 0.105 | 1770 ± 440 | −5.761 ± .149 | ||
| 0.02 | 0.050 | 0.700 | 0.105 | 1770 ± 440 | −5.761 ± .149 | 1.000 | 1.000 | ||||||||||
| P025z10-01 | 38.0 | 4.25 | 6.2 | 25.0 | 4.85 | 0.085 | 1.0 | 1.0 | 1.0 | 0.0 | 0.306 | 0.462 | 0.033 | 2120 ± 100 | −7.510 ± .070 | ||
| 0.4 | 0.287 | 0.462 | 0.032 | 1940 ± 100 | −7.503 ± .088 | 1.016 | 1.064 | ||||||||||
| P025z10-02 | 36.0 | 4.03 | 8.0 | 24.7 | 4.98 | 0.085 | 0.95 | 1.28 | 0.98 | 0.0 | 0.185 | 0.515 | 0.048 | 2070 ± 110 | −7.237 ± .073 | ||
| 0.39 | 0.171 | 0.532 | 0.056 | 1970 ± 100 | −7.123 ± .075 | 1.300 | 1.054 | ||||||||||
| P025z10-03 | 34.0 | 3.81 | 10.1 | 24.4 | 5.09 | 0.088 | 0.80 | 2.44 | 0.92 | 0.0 | 0.097 | 0.644 | 0.098 | 2370 ± 110 | −6.615 ± .064 | ||
| 0.38 | 0.090 | 0.653 | 0.099 | 2250 ± 110 | −6.591 ± .059 | 1.059 | 1.061 | ||||||||||
| P025z10-04 | 32.0 | 3.62 | 12.6 | 24.1 | 5.17 | 0.095 | 0.68 | 3.49 | 0.84 | 0.0 | 0.060 | 0.689 | 0.109 | 2390 ± 120 | −6.558 ± .047 | ||
| 0.37 | 0.058 | 0.691 | 0.108 | 2240 ± 120 | −6.550 ± .038 | 1.018 | 1.056 | ||||||||||
| P025z10-05 | 30.0 | 3.44 | 15.3 | 23.9 | 5.23 | 0.105 | 0.61 | 4.28 | 0.78 | 0.0 | 0.038 | 0.697 | 0.099 | 2230 ± 230 | −6.740 ± .044 | ||
| 0.35 | 0.036 | 0.705 | 0.099 | 2170 ± 230 | −6.710 ± .053 | 1.050 | 1.051 | ||||||||||
Notes. Ratios showing the enhancement of the mass-loss rate due to rotation, adopting either our self-consistent procedure or MM00, are also shown in the last columns.
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