Table 5
[O I] mass-flux rates and comparison with Ṁacc.
| Obj. | Region | Box | θ | vt |  |
 |
 |
|---|---|---|---|---|---|---|---|
| (″) | (km s−1) | (10−7 M⊙ yr−1) | (10−7 M⊙ yr−1) | (10−7 M⊙ yr−1) | |||
| HH111 | HH111IRS | B1 | 20 | 270(a) | 26−53 |  |
− |
| jet (knots F-O) | B2 | 45 | 260(a) | 6−12 |  |
1.8−4 (b) | |
| SVS13 | SVS13 | B1 | 22 | 270(c) | 25−51 |  |
38−66 (d) |
| HH8-11 | B2 | 40 | 340(c) | 8.5−17.2 |  |
≲1−10 (e) | |
| HH7 | B3 | 21 | 400(c) | 18−37 |  |
48(f) | |
| HH26 | HH26A | B2 | 28 | 100(c) | 5−9 |  |
18−21 (g) |
| HH34 | counter jet, HH34IRS | B1 | 26 | 160(h) | 11−23 |  |
0.5−5 (i) |
| HH30 | HH30IRS | B1 | 20 | 190(j) | <0.1−0.2 |  |
0.002−0.02 (k) |
Notes. 
and
are calculated via Eq. (7) and Eq. (6), respectively. Green cell colours (light) indicate the regions where the HM89 model is likely to be applicable, and red cells (dark) mark the doubtful cases (see Sect. 5.2).
References. (a) Hartigan et al. (2001), (b) Hartigan et al. (1994); Lefloch et al. (2007), (c)Chrysostomou et al. (2000), (d) Molinari et al. (2000); Dionatos et al. (2020), (e)estimate based on Snell & Edwards (1981); Lizano et al. (1988); Molinari et al. (2000); Dionatos et al. (2020), (f) Molinari et al. (2000), (g) Benedettini et al. (2000) , (h) Eislöffel & Mundt (1992), (i)Hartigan et al. (1994); Heathcote & Reipurth (1992); Bacciotti & Eislöffel (1999); Garcia Lopez et al. (2008); Antoniucci et al. (2008); Nisini et al. (2016), (j)Mundt et al. (1990), (k)Mundt et al. (1990); Bacciotti & Eislöffel (1999).
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