STABLE AND UNSTABLE ACCRETION FLOWS WITH ANGULAR-MOMENTUM NEAR A POINT MASS

被引:48
作者
RYU, DS
BROWN, GL
OSTRIKER, JP
LOEB, A
机构
[1] CHUNGNAM NATL UNIV, DEPT ASTRON & SPACE SCI, TAEJON 305764, SOUTH KOREA
[2] PRINCETON UNIV, DEPT MECH & AEROSP ENGN, PRINCETON, NJ 08544 USA
[3] INST ADV STUDY, PRINCETON, NJ 08540 USA
[4] CTR ASTROPHYS, CAMBRIDGE, MA 02138 USA
关键词
ACCRETION; ACCRETION DISKS; BLACK HOLE PHYSICS; HYDRODYNAMICS METHODS; NUMERICAL; SHOCK WAVES;
D O I
10.1086/176308
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
The properties of axisymmetric accretion flows of cold adiabatic gas with zero total energy in the vicinity of a Newtonian point mass are characterized by a single dimensionless parameter, the thickness of incoming flow. In the limit of thin accretion hows with vanishing thickness, we show that the governing equations become self-similar involving no free parameters. We study numerically thin accretion flows with finite thickness as well as those with vanishing thickness. Mass elements of the incoming flow enter the computational regime as thin rings. In the case with finite thickness, after a transient period of initial adjustment, an almost steady state accretion shock with a small oscillation amplitude forms, confirming the previous work by Molteni, Lanzafame, & Chakrabarti. The gas in the region of vorticity between the funnel wall and the accretion shock follows closed streamlines, forming a torus. This torus, in turn, behaves as an effective barrier to the incoming flow and supports the accretion shock which reflects the incoming gas away from the equatorial plane. The postshock flow, which is further accelerated by the pressure gradient behind the shock, goes through a second shock which then reflects the flow away from the symmetry axis to form a conical outgoing wind. As the thickness of the inflowing layer decreases (or if the ratio of the half-thickness to the distance to the funnel wall along the equatorial plan is smaller than similar to 0.1), the how becomes unstable. In the case with vanishing thickness, the accretion shock formed to stop the incoming how behind the funnel wall oscillates quasi-periodically with an amplitude comparable to the thickness. The structure between the funnel wall and the accretion shock is destroyed as the shock moves inward toward the central mass and regenerated as it moves outward. We suggest a possible explanation for the instability. The phenomenon may be related to the quasi-periodic oscillations observations in accreting galactic sources.
引用
收藏
页码:364 / 378
页数:15
相关论文
共 28 条
[1]  
[Anonymous], 1957, ELEMENTS GASDYNAMICS
[2]  
ANZER U, 1987, ASTRON ASTROPHYS, V176, P235
[3]   On the mechanism of accretion by stars [J].
Bondi, H ;
Hoyle, F .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1944, 104 (01) :0273-0282
[4]   ON SPHERICALLY SYMMETRICAL ACCRETION [J].
BONDI, H .
MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, 1952, 112 (02) :195-204
[5]   STANDING RANKINE-HUGONIOT SHOCKS IN THE HYBRID MODEL FLOWS OF THE BLACK-HOLE ACCRETION AND WINDS [J].
CHAKRABARTI, SK .
ASTROPHYSICAL JOURNAL, 1989, 347 (01) :365-372
[6]   SMOOTHED PARTICLE HYDRODYNAMICS CONFRONTS THEORY - FORMATION OF STANDING SHOCKS IN ACCRETION DISKS AND WINDS AROUND BLACK-HOLES [J].
CHAKRABARTI, SK ;
MOLTENI, D .
ASTROPHYSICAL JOURNAL, 1993, 417 (02) :671-676
[7]   JET PRODUCTION IN SUPER-EDDINGTON ACCRETION DISKS [J].
EGGUM, GE ;
CORONITI, FV ;
KATZ, JI .
ASTROPHYSICAL JOURNAL, 1985, 298 (02) :L41-L45
[8]   RADIATION HYDRODYNAMIC CALCULATION OF SUPER-EDDINGTON ACCRETION DISKS [J].
EGGUM, GE ;
CORONITI, FV ;
KATZ, JI .
ASTROPHYSICAL JOURNAL, 1988, 330 (01) :142-167
[9]   RADIATION-HYDRODYNAMIC CALCULATION OF SUB-EDDINGTON ACCRETION DISKS [J].
EGGUM, GE ;
CORONITI, FV ;
KATZ, JI .
ASTROPHYSICAL JOURNAL, 1987, 323 (02) :634-646
[10]  
Goldreich P., 1965, MNRAS, V130, P125, DOI [10.1093/mnras/130.2.125, DOI 10.1093/MNRAS/130.2.125]