Table 2
Radio jet properties for an isothermal conical flow with uniform ionization fraction.
| Assumed parameters | Radio observables | Jet energetics | ||||||||||||
| ϵ | q T | q x | F(α) | x 0 | T | ν m | ν | S45 × d2 | α | ψ | i | V jet | Ṁ jet | ṗ jet |
| (K) | (GHz) | (GHz) | (mJy × kpc2) | (°) | (°) | (km s-1) | (M⊙ yr-1) | (M⊙ yr-1 km s-1) | ||||||
|
|
||||||||||||||
| 1 | 0 | 0 | 1.5−1.1 | 1 | 104 | 50−100 | 44.7 | 1.15 × 4.62 | 0.6−0.9 | 22 |
60−90 | 600 | 0.2−0.8 × 10-5 | 1.2−4 × 10-3 |
| 1000 | 0.4−1.4 × 10-5 | 0.4−1.4 × 10-2 | ||||||||||||
| 1 | 0 | 0 | 1.24 | 1 | 10 4 | 50 | 44.7 | 1.15 × 4.6 2 | 0.75 | 22 | 60 | 1000 | 0.8 × 10 -5 | 8 × 10 -3 |
Notes. Columns 1 to 6 define the properties of the ionized gas following the formalism by Reynolds (1986). The parameters ϵ, qT, and qx are the indexes of the power-law dependence of the jet width, temperature, and ionization fraction with the jet radius (w ∝ rϵ, T ∝ rqT, x ∝ rqx), respectively. Columns 7 to 13 list the radio observables that enter into Eq. (1). The last two columns report the derived jet mass loss and momentum rates. The last row lists the fiducial jet parameters used in comparison with the large-scale secondary outflow.
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