Table 1.
Simulations presented in this paper.
| Name | κ | α | μ | δ |
 |
Zshock |
 |
 |
ro, FM | Ṁjet |
 |
Pjet |
 |
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| K1 | 0.05 | 12/16 | 1.41 | 50 | 7.34 | 2150 | 0.64 | 0.94 | 301 | 179 | 0.102 | 492 | 0.82 |
| K2 | 0.1 | 12/16 | 1.00 | 100 | 6.51 | 1850 | 0.67 | 1.05 | 323 | 363 | 0.096 | 616 | 0.81 |
| K2l | 0.1 | 12/16 | 1.00 | 100 | 12.3 | 2490 | 0.65 | 1.02 | 289 | 357 | 0.094 | 620 | 0.81 |
| K3 | 0.2 | 12/16 | 0.71 | 200 | 10.1 | 1810 | 0.69 | 1.09 | 368 | 743 | 0.093 | 768 | 0.80 |
| K4 | 0.5 | 12/16 | 0.45 | 500 | 8.67 | 1150 | 0.90 | 1.26 | 655 | 2040 | 0.093 | 1024 | 0.81 |
| K5 | 1.0 | 12/16 | 0.32 | 1000 | 4.62 | 700 | 0.99 | 1.34 | 670 | 4095 | 0.116 | 1264 | 0.96 |
| A1 | 0.1 | 10/16 | 1.00 | 100 | 9.08 | 1900 | 0.96 | 1.23 | 234 | 195 | 0.206 | 551 | 1.21 |
| A2 | 0.1 | 11/16 | 1.00 | 100 | 8.34 | 1800 | 0.87 | 1.15 | 349 | 272 | 0.137 | 578 | 0.99 |
| A3 | 0.1 | 13/16 | 1.00 | 100 | 5.79 | 1920 | 0.59 | 0.95 | 566 | 690 | 0.047 | 668 | 0.66 |
| A4 | 0.1 | 14/16 | 1.00 | 100 | 6.26 | 2050 | 0.64 | 0.94 | 398 | 1321 | 0.023 | 740 | 0.53 |
| A5 | 0.1 | 15/16 | 1.00 | 100 | 1.62 | 2030 | 0.50 | 0.83 | 1046 | 3275 | 0.009 | 848 | 0.41 |
| SP | 0.1 | 12/16 | 1.00 | 100 | 3.93 | 1250 | 0.82 | 1.09 | 506 | 392 | 0.097 | 613 | 0.98 |
Notes. All the simulations presented have been performed in the grid described in Sect. 2.2 (e.g., NR = 1408 and Nθ = 266) except K2l, performed in a lower resolution grid (e.g., NR = 704 and Nθ = 144) The parameters κ and α are varied independently, allowing us to compute μ, δ, and MS. The columns 
, and Pspine/Pjet are outputs of the simulation measured at the final time tend (given in 105Td units). Simulations K1 to A5 were done with a nonrotating spine, namely Ωa = 0 and ea = 2. Simulation SP is done for Ωa = ΩKd and ea = 10 and is discussed in Sect. 4.3. See Sect. 2.5 for the definition of all these quantities.
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