Self-Similar Force-Free Wind From an Accretion Disk
arXiv:astro-ph/0610817 · doi:10.1111/j.1365-2966.2006.11272.x
Abstract
We consider a self-similar force-free wind flowing out of an infinitely thin disk located in the equatorial plane. On the disk plane, we assume that the magnetic stream function scales as , where is the cylindrical radius. We also assume that the azimuthal velocity in the disk is constant: , where is a constant. For each choice of the parameters and , we find an infinite number of solutions that are physically well-behaved and have fluid velocity throughout the domain of interest. Among these solutions, we show via physical arguments and time-dependent numerical simulations that the minimum-torque solution, i.e., the solution with the smallest amount of toroidal field, is the one picked by a real system. For , the Lorentz factor of the outflow increases along a field line as $γ\approx M(z/\Rfp)^{(2-ν)/2} \approx R/R_{\rm A}$, where $\Rfp$ is the radius of the foot-point of the field line on the disk and $R_{\rm A}=\Rfp/M$ is the cylindrical radius at which the field line crosses the Alfven surface or the light cylinder. For , the Lorentz factor follows the same scaling for $z/\Rfp < M^{-1/(1-ν)}$, but at larger distances it grows more slowly: $γ\approx (z/\Rfp)^{ν/2}$. For either regime of , the dependence of on shows that the rotation of the disk plays a strong role in jet acceleration. On the other hand, the poloidal shape of a field line is given by $z/\Rfp \approx (R/\Rfp)^{2/(2-ν)}$ and is independent of . Thus rotation has neither a collimating nor a decollimating effect on field lines, suggesting that relativistic astrophysical jets are not collimated by the rotational winding up of the magnetic field.
21 pages, 15 figures, accepted to MNRAS
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