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Table 1
Adopted parameters and initial conditions for the MHD models of accretion shocks.
| Model | |Blb | | β slaba | n str0 | u str0 | r str | Ṁ | Magnetic field | z dip | Note |
| abbreviation | [G] | [cm-3] | [km s-1] | cm | [ M⊙ yr-1 ] | configuration | [cm] | ||
|
|
|||||||||
| B50-D11-Unif | 50 | 5 | 1011 | 500 | 1010 | 5 × 10-11 | Uniform | − | reference case |
| B500-D11-Unif | 500 | 0.06 | 1011 | 500 | 1010 | 5 × 10-11 | Uniform | − | reference case |
| B50-D11-Dip1 | 50 | 10 | 1011 | 500 | 1010 | 5 × 10-11 | Dipole | − 3 × 1010 | – |
| B500-D10.7-Dip1 | 500 | 0.05 | 5 × 1010 | 500 | 1010 | 2.5 × 10-11 | Dipole | − 3 × 1010 | – |
| B500-D11-Dip1 | 500 | 0.2 | 1011 | 500 | 1010 | 5 × 10-11 | Dipole | − 3 × 1010 | – |
| B50-D11-Dip2 | 50 | 100 | 1011 | 500 | 1010 | 5 × 10-11 | Dipole | − 1010 | – |
| B500-D10.7-Dip2 | 500 | 10b | 5 × 1010 | 500 | 1010 | 2.5 × 10-11 | Dipole | − 1010 | – |
| B500-D11-Dip2 | 500 | 10b | 1011 | 500 | 1010 | 5 × 10-11 | Dipole | − 1010 | – |
Notes.
(b)
In runs B500-D10.7-Dip2 and B500-D11-Dip2, βslab is measured in the slab generated by the oblique shock (see Sect. 3.2).
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