|
|
Proto-planetary accretion discs |
Accretion discs in black hole (BH) or neutron star (NS) binaries |
Accretion discs around white dwarfs (WD) in cataclysmic binaries |
Accretion discs in quasars and other AGNs |
Accretion discs in gamma ray burst (GRB) sources |
|
Image
|
|
|
|
| |
Basic physics |
The central part of a dense molecular cloud collapses to a proto-star sourrended by a proto-planetary accretion disc. Self gravity and sedimentation trigger the formation of planets. Bipolar outflows ("slow" jets) often emerge from proto-planetary discs.
|
|
X-ray binaries (XRB) consist a mass loosing main-sequence "secondary" star and accreting BH or NS. Among XRBs, the soft X-ray transients (with BH or NS) show quasi-periodic outbursts. Most of the BH XRBs exhibit "fast" jets, and for this reason are called microquasars. |
|
U Gem is the prototype of a dwarf novae system, i.e. a close stellar binary, with "primary" being a WD with accretion disc. Disc's brightness in the visible light increases 100-fold every ~120 days and returns to the original level after a ~week, due to (mainly) a limit-cycle instability. |
|
AGNs are supermassive BH at centers of galaxies. Accretion produces radiative power that often outshines the host galaxy. A large torus of gas and dust partially obscures the accretion disc. "Fast" (almost speed of light) jets emerge from many AGNs. |
|
GRBs are the most energetic explosions in the universe. Models of GRBs invoke a black hole (M~3Msun) accreting matter at highly super-Eddington rates. Huge power of gamma-rays is possibly due to an extraction of the BH rotational energy (the Blandford- Znajek mechanism). |
|
The high angular momentum of matter in an accretion disc is gradually transported outwards by stresses (turbulent, magnetic, etc.). This allows matter to gradually spiral inwards, towards the gravity center. Matter's gravitational energy is degraded to heat. A fraction of the heat converts into radiation, which partially escapes and cools down the accretion disc. For more details see the sub-section 2. Basic physics of accretion discs |
|
|
Angular momentum transport
| ???
| ???
| ???
| ???
| ??? |
|
Cooling
| ???
| ???
| ???
| ???
| ??? |
|
Central accreting object
| 1 Msun star
| 3-10 Msun BH, or ~1 Msun NS
| ~1 Msun WD
| 106-109Msun BH
| 3-10 Msun BH |
|
Disc's size
Rin-Rout
| ???-??? cm 10-2-200 AU
| 106-1011 cm ???
| 109-1010 cm ???
| 1013-1018 cm x[M/107Msun]
0.3 pc ???
| ??? 3-30 RS |
|
Disc's temperature
Tmax-Tout
| 103-101 K
| 107-103 K
| 105-103 K
| 105-102 K
| 1010-109 K |
|
Time behavior, oscillations
| ???
| ???
| ???
| ???
| ??? |
|
Theoretical models
| Numerical simulations
| Thin discs, slim discs, adafs
| Thin discs
| Thick discs, slim discs
| Thick discs, numerical |
|
References
| Larson (2003) Alexander (2008)
| McClintock, Remillard (2003) Narayan, McClintock (2008)
| Lasota (2001) Warner (2003)
| on-line compilation Krolik (1998)
| Piran (2005) Meszaros (2006) |
|
The table is based on a lecture by Kristen Menou (2008, Nordita, Stockholm, Sweden) |
</table>
</table>