Table 1.
Summary of the initial physical parameters characterizing the different models.
| Model | Tj (106 K) | nj (104 cm−3) | χb | υb (km s−1) | Rb | ROT | Ṁj (10−8 M⊙yr−1) |
|---|---|---|---|---|---|---|---|
| Light jet | |||||||
| LJ1 | 3 | 1 | 3 | 300–700c | 1 | no | 1.3−5.4 |
| LJ2 | 3 | 1 | 1.5 | 300–700c | 1 | no | 1.3−2.7 |
| LJ3 | 3 | 1 | 3 | 500 | 1 | no | 1.3−3.9 |
| LJ4 | 3 | 1 | 3 | 500 | 1/3 | no | 1.3−1.6 |
| LJ5_refa b | 3 | 1 | 3 | 500 | 1 | yes | 1.4−4.0 |
| LJ6 | 3 | 1 | 1.5 | 500 | 1 | no | 1.3−2.0 |
| LJ7 | 3 | 1 | 1.5 | 500 | 1/3 | no | 1.3−1.4 |
| LJ8 | 3 | 1 | 10 | 500 | 1 | no | 1.3−12.8 |
| LJ9 | 3 | 2 | 1.5 | 500 | 1 | no | 2.6−3.9 |
| LJ10 | 2 | 3 | 1.5 | 500 | 1 | no | 3.9−5.8 |
| Heavy jet | |||||||
| HJ1 | 1 | 1 | 3 | 300–700c | 1 | no | 1.3−5.3 |
| HJ2b | 1 | 1 | 1.5 | 300–700c | 1 | yes | 1.3−2.7 |
| HJ3_refab | 1 | 1 | 1.5 | 300–700c | 1/3 | yes | 1.3−1.5 |
| HJ4 | 1 | 1 | 3 | 500 | 1 | no | 1.3−3.8 |
| HJ5 | 1 | 1 | 3 | 500 | 1/3 | no | 1.3−1.6 |
| HJ6b | 1 | 1 | 3 | 500 | 1 | yes | 1.3−3.9 |
| HJ7 | 1 | 1 | 1.5 | 500 | 1 | no | 1.3−1.9 |
| HJ8 | 1 | 1 | 1.5 | 500 | 1/3 | no | 1.3−1.4 |
| HJ9 | 1.5 | 1 | 1.5 | 500 | 1 | no | 1.3−1.9 |
| HJ10 | 2 | 1 | 1.5 | 500 | 1 | no | 1.3−1.9 |
| HJ11 | 1.5 | 1 | 3 | 500 | 1 | no | 1.3−3.8 |
| HJ12 | 2 | 1 | 3 | 500 | 1 | no | 1.3−3.8 |
Notes. Columns are: jet temperature at the lower boundary, Tj; jet density at the lower boundary (continuous component), nj; initial blob-to-jet particle number density ratio (pulsed component), χb = nb/nj; blob velocity at the lower boundary (pulsed component), υb; initial blob-to-jet radius ratio (pulsed component), Rb = rb/rj; a parameter, ROT, that indicates if there is rotation in the jet (“yes”) or not (“no”); and the mass loss rate calculated at the lower boundary, Ṁj. The initial temperature, density, and pressure of the ambient are Ta = 10 K, na = 5000 cm−3, and pa ≈ 1.4 × 10−11 dyne cm−2, respectively, in the LJ models; and Ta = 100 K, na = 100 cm−3, and pa ≈ 2.8 × 10−12 dyne cm−2 in the HJ models. The rest of the parameters are constant and equal for all the models: ambient magnetic field, Bz = 4 mG; jet velocity at the lower boundary, υj = 500 km s−1. The top panel shows the models for the light jet, a jet less dense than the ambient medium. The bottom panel displays the models for the heavy jet, a jet denser than the ambient medium.
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