Table 6.
Mass outflow rate, momentum injection rate and kinetic energy injection at a distance of 1 kpc from the nucleus.
| Cone geometry |
Shell geometry |
||||||||||||||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Ionised |
Molecular |
Ionised |
Molecular |
||||||||||||
| log(Ṁ) | log(ṗ) | log(Ė) | log(Ṁ) | log(ṗ) | log(Ė) | log(Ṁ) | log(ṗ) | log(Ė) | log(Ṁ) | log(ṗ) | log(Ė) | ||||
| vbr | −0.24 | 32.80 | 40.12 | 1.89 | 34.85 | 41.85 | −0.02 | 33.02 | 40.34 | 2.11 | 35.07 | 42.07 | |||
| vmax | 0.28 | 33.84 | 41.32 | 2.23 | 35.53 | 42.72 | 0.50 | 34.06 | 41.54 | 2.26 | 35.43 | 42.56 | |||
| v10 | 0.41 | 33.83 | 41.19 | 2.42 | 35.50 | 42.49 | 0.64 | 34.05 | 41.41 | 2.64 | 35.73 | 42.72 | |||
| W80 | 0.50 | 34.02 | 41.49 | 2.40 | 35.47 | 42.44 | 0.72 | 34.24 | 41.71 | 2.62 | 35.69 | 42.66 | |||
Notes. Units for mass outflow rates (Ṁ) are M⊙ yr−1, for the momentum injection rates (ṗ) are dyne, and for energy injection rates (Ė) are erg s−1. We do not provide the formal measurement errors here since they are significantly smaller than the spread implied by the different asummptions.
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