Issue |
A&A
Volume 583, November 2015
|
|
---|---|---|
Article Number | A90 | |
Number of page(s) | 18 | |
Section | Astrophysical processes | |
DOI | https://doi.org/10.1051/0004-6361/201525763 | |
Published online | 30 October 2015 |
Online material
Appendix A: Results from model UA1
In this section we show results from model UA1. These can be compared to those results for UB1 as found in the main text.
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Fig. A.1
Contour plot of velocity contours evaluated in Boyer-Lindquist coordinates for a uniform supersonic flow past a non-spinning black hole with flow parameters given by model UA1, evaluated at time t = 300M. The stagnation point is marked. |
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Fig. A.2
Contour plot of velocity for a supersonic flow with density perturbed by ϵρ = 0.2 past a black hole with spin a = 0.9 and flow parameters given by model UA1, evaluated at time t = 400M, with the axes in units of M. |
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Fig. A.3
Accretion regions for two supersonic models based on UA1. The solid line shows the accretion region for a = 0, ϵρ = 0, and the dashed line shows the accretion region for a = 0.9, ϵρ = 0.2. |
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Appendix B: Mass accretion and shock-angle dependence
In this section we show details of how the mass accretion rates and shock-angles depend on the size of the density perturbation.
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Fig. B.1
Mass accretion rate against density perturbation for different spins. The wind direction is parallel to the equatorial plane of the black hole in all cases. |
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Fig. B.2
Mass accretion rates against density perturbation. The labels refer to the angle between the equatorial plane and the wind direction. a) Spin a = 0.5; b) Spin a = 0.9. |
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Fig. B.3
Shock angles against density perturbation, varying the spin of the black hole. The wind direction is in the equatorial plane of the black hole in all cases. |
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Fig. B.4
Shock-cone angles against density perturbation. The angles are all taken in the plane containing the wind direction and the y-axis. The data points above and below the axis correspond to the shock-angles above and below the wind-direction axis. The labels correspond to the angle between the equatorial plane of the black hole and the wind direction. a) Spin a = 0.5; b) Spin a = 0.9. |
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© ESO, 2015
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