dc.contributor.author | Narayan, R. | |
dc.contributor.author | McKinney, J. C. | |
dc.contributor.author | Farmer, A. J. | |
dc.date.accessioned | 2019-09-22T14:23:54Z | |
dc.date.issued | 2007 | |
dc.identifier.citation | Narayan, R., J. C. McKinney, and A. J. Farmer. 2007. “Self-Similar Force-Free Wind from an Accretion Disc.” Monthly Notices of the Royal Astronomical Society 375 (2): 548–66. https://doi.org/10.1111/j.1365-2966.2006.11272.x. | |
dc.identifier.issn | 0035-8711 | |
dc.identifier.issn | 1365-2966 | |
dc.identifier.uri | http://nrs.harvard.edu/urn-3:HUL.InstRepos:41384883 | * |
dc.description.abstract | We consider a self-similar force-free wind flowing out of an infinitely thin disc located in the equatorial plane. On the disc plane, we assume that the magnetic stream function P scales as P proportional to R(nu), where R is the cylindrical radius. We also assume that the azimuthal velocity in the disc is constant: v(phi) = Mc, where M < 1 is a constant. For each choice of the parameters nu and M, we find an infinite number of solutions that are physically well-behaved and have fluid velocity <= c 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 nu >= 1, the Lorentz factor of the outflow increases along a field line as gamma approximate to M(z/R(fp))((2-nu)/2) approximate to R/R(A), where R(fp) is the radius of the foot-point of the field line on the disc and R(A) = R(fp)/M is the cylindrical radius at which the field line crosses the Alfven surface or the light cylinder. For nu < 1, the Lorentz factor follows the same scaling for z/R(fp) < M(-1/(1-nu)), but at larger distances it grows more slowly: gamma (z/R(fp))(nu/2). For either regime of nu, the dependence of gamma on M shows that the rotation of the disc plays a strong role in jet acceleration. On the other hand, the poloidal shape of a field line is given by z/R(fp) approximate to (R/R(fp))(2/(2-nu)) and is independent of M. 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. | |
dc.language.iso | en_US | |
dc.publisher | Oxford University Press | |
dash.license | LAA | |
dc.title | Self-similar force-free wind from an accretion disc | |
dc.type | Journal Article | |
dc.description.version | Version of Record | |
dc.relation.journal | Monthly Notices of the Royal Astronomical Society | |
dash.depositing.author | Narayan, Ramesh::dc7afe5d74d62c7b451015317ea2ccbe::600 | |
dc.date.available | 2019-09-22T14:23:54Z | |
dash.workflow.comments | 1Science Serial ID 66200 | |
dc.identifier.doi | 10.1111/j.1365-2966.2006.11272.x | |
dash.source.volume | 375;2 | |
dash.source.page | 548-566 | |