Table 1
Parameters used in the simulation models.
| Case | θ | γ j | ν | σ | L j | Domain | Grid |
|
|
|||||||
| A | 0 | 5 | 1 × 10-4 | 10-3 | 1.6 × 1046 | 2 × 4 × 2 | 384 × 768 × 384 |
| B | 0 | 2.5 | 4 × 10-4 | 10-3 | 1.6 × 1046 | 2 × 4 × 2 | 384 × 768 × 384 |
| C | 0 | 1.25 | 2.66 × 10-3 | 10-3 | 1.6 × 1046 | 4 × 4 × 4 | 768 × 768 × 768 |
| D | 0 | 5 | 1 × 10-5 | 10-2 | 1.6 × 1045 | 4 × 8 × 4 | 768 × 1024 × 768 |
| E | 0 | 5 | 1 × 10-6 | 10-2 | 1.6 × 1044 | 4 × 8 × 4 | 768 × 1024 × 768 |
| F | 30° | 5 | 1 × 10-6 | 10-2 | 1.6 × 1044 | 4 × 8 × 4 | 768 × 1024 × 768 |
Notes. In the first column we have the case identifier, in the second column the angle between the jet axis and the major axis of the triaxial density distribution, in the third column the jet Lorentz factor, in the fourth column the density ratio, in the fifth column the magnetization parameter σ, in the sixth column the jet power, in the seventh column the size of the computational domain in units of rc and in the eighth column the grid size. Lj is measured in erg s-1 and is computed for rc = 4 kpc and ρ0 = 1 cm-3, the dependence of Lj on rc and ρ0 is given by Eq. (9).
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