Table 4
Model parameters for the cases of large inclination.
| i | 40° | 50° | 60° | 70° |
|---|---|---|---|---|
| q | 0.043 | 0.052 | 0.059 | 0.063 |
| βorb,M | 0.00480 | 0.00480 | 0.00480 | 0.00480 |
| βorb,m | 0.1106 | 0.0928 | 0.0821 | 0.0757 |
 |
0.0711 | 0.0711 | 0.0711 | 0.0711 |
| M8 + m8 | 63.4 | 38.3 | 27.0 | 21.5 |
| M8 | 60.8 | 36.4 | 25.5 | 20.2 |
| m8 | 2.6 | 1.9 | 1.5 | 1.3 |
| r(pc) | 0.0243 | 0.0205 | 0.0183 | 0.0169 |
| ϵ1 | 0.013 | 0.0090 | 0.0071 | 0.0061 |
Notes. q = m∕M, i is the inclination angle of the orbital plane with respect to the disk of the primary hole (or the angle between the orbital axis and the primary disk axis (jet), βorb, M = vorb, M /c – the primary hole orbital velocity, βorb,m = vorb,m /c – the secondary hole orbital velocity, M8 + m8 – the total mass of the binary in units of 108 M⊙, M8 and m8 – the masses of the primary and secondary holes, respectively. ϵ1 – the post Newtonian factor and r (pc) – the binary separation. Here the derived parameters are given for four cases: i = 40°, 50°, 60° and 70°.
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