Table 7
Maximum mass-loss rates, minimum clumping factors and alternative boundaries of the defined wind regions (adapted-regions approach, see Sect. 3) providing the best-fit models for some objects in the sample.
Source | Ṁmax | R* | β | υ∞ | Reg. 2 | Region 3 | Reg. 4 | Reg. 5 | Comments | |||
---|---|---|---|---|---|---|---|---|---|---|---|---|
(10−6 M⊙ yr−1) | (R⊙) | (km s−1) | ![]() ![]() |
rmid | ![]() |
rout | ![]() |
![]() |
![]() |
|||
HD 66811 (ζ Pup) | 4.2 | 18.6 | 0.7 | 2250 | 5.0 (1.12) | 2.0 | 3.1 | 12.0 | 1.0 | 1.2 | 1.0 | |
8.5 | 29.7 | 5.0 (1.12) | 2.0 | 3.1 | 12.0 | 1.0 | 1.2 | 1.0 | ||||
HD 152408 | 9.5 | 30.0 | 2.1 | 955 | 1.0 | 3.5 | 4.0 | 15.0 | 1.0 | 3.0 | 1.0 | |
HD 151804 | 6.4 | 36.0 | 2.0 | 1450 | 1.0 | 5.0 | 8.5 | 12.0 | 1.0 | 1.0 | 1.0 | |
HD 149404 | 8.27 | 37.0 | 1.3 | 2450 | 1.0 | 2.5 | 7.0 | 15.0 | 1.0 | (6.0) | 1.0 | Binary |
HD 30614 (α Cam) | 1.75 | 20.70 | 1.15 | 1550 | 6.0 (1.1) | 4.0 | 1.0 | 15.0 | 1.0 | (2.0) | 1.0 | |
HD 37128 (ϵ Ori) | 1.25 | 24.7 | 1.5 | 1910 | 5.0 | 2.0 | 8.0 | 6.0 | 1.0 | 1.0 | 1.0 | |
HD 38771 (κ Ori) | ≲0.7(a) | 23.0 | 1.5 | 1525 | 20.0 | 1.55 | 1.0 | 15.0 | 1.0 | (8.0) | 1.0 | |
HD 154090 | 1.2 | 39.0 | 1.5 | 915 | 4.0 (1.4) | 2.0 | 3.5 | 15.0 | 1.0 | (8.0) | 1.0 | |
HD 169454 | 10.4 | 98.2 | 2.1 | 850 | 1.0 | 4.0 | 4.5 | 15.0 | 1.0 | 2.5 | 1.0 | eBHG |
HD 152236 (ζ1 Sco) | 6.2 | 104.0 | 2.0 | 390 | 1.0 | 2.0 | 3.0 | 10.0 | 1.0 | 1.0 | 1.0 | eBHG |
HD 53138 (o2 CMa) | ≲1.8(c) | 65.0 | 2.0 | 865 | 3.0 | 1.3 | 1.0 | 15.0 | 1.0 | (18.0) | 1.0 (50.0) | |
Cyg OB2#12 | 3.0(d) | 240.0 | 3.0 | 400 | 1.0 | 2.5 | 12.0 | 8.0 | 10.0 | 12.0 | 5.0/15.0 | eBHG |
1.02(d) | 116.7 | 3.0 | 400 | 1.0 | 2.5 | 12.0 | 8.0 | 10.0 | 12.0 | 5.0/15.0 | ||
HD 24912 (ξ Per) | 1.4 | 23.4 | 0.9 | 2450 | 5.0 (1.1) | 4.0 | 1.0 | 15.0 | 1.0/3.0 | (5.0) | 1.0/3.0 |
Notes. Column descriptions and values in parentheses or separated by forward slashes as in Table 6.
indicates values different from the nominal, adopted rin = 1.05 R*, and rfar is always set to 50 R*. (a)Upper limit of Ṁmax, derived from upper radio-flux limits. (c)Upper limit of Ṁmax derived from well-defined FIR fluxes. No radio fluxes measurements available. (d)Well-defined Ṁmax, derived from FIR fluxes, since well-defined radio fluxes are not consistent with all the data.
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