Evolution of transonicity in an accretion disc
| dc.contributor.author | Ray, Arnab K. | |
| dc.contributor.author | Bhattacharjee, Jayanta K. | |
| dc.date.accessioned | 2012-03-06T04:42:44Z | |
| dc.date.available | 2012-03-06T04:42:44Z | |
| dc.date.issued | 2007-01-10 | |
| dc.description.abstract | For inviscid, rotational accretion ows driven by a general pseudo Newtonian potential on to a Schwarzschild black hole, the only possible xed points are saddle points and centre-type points. For the speci c choice of the Newtonian potential, the ow has only two critical points, of which the outer one is a saddle point while the inner one is a centre-type point. A restrictive upper bound is imposed on the admissible range of values of the angular momentum of sub-Keplerian ows through a saddle point. These ows are very unstable to any deviation from a necessarily precise boundary condition. The di culties against the physical realisability of a solution passing through the saddle point have been addressed through a temporal evolution of the ow, which gives a non-perturbative mechanism for selecting a transonic solution passing through the saddle point. An equation of motion for a real-time perturbation about the stationary ows reveals a very close correspondence with the metric of an acoustic black hole, which is also an indication of the primacy of transonicity | en_US |
| dc.identifier.uri | http://hdl.handle.net/11007/605 | |
| dc.language.iso | en | en_US |
| dc.relation.ispartofseries | IUCAA Preprint;04/07 | |
| dc.subject | Transonicity | en_US |
| dc.subject | Accretion disc | en_US |
| dc.title | Evolution of transonicity in an accretion disc | en_US |
| dc.type | Article | en_US |