Presentation is loading. Please wait.

Presentation is loading. Please wait.

Accretion onto Black Hole : Advection Dominated Flow

Similar presentations


Presentation on theme: "Accretion onto Black Hole : Advection Dominated Flow"— Presentation transcript:

1 Accretion onto Black Hole : Advection Dominated Flow
K. Hayashida Osaka University

2 Free Fall & Escape Velocity
E= (at Infinite) E=1/2v2-GM/r=0 (at r ) v=sqrt(2GM/r) v=Free Fall Velocity=Escape Velocity v=c … r=rg =2GM/c2 Schwartzshild radius 3km for 1Mo

3 Kepler Motion GM/r2 = v2/r = rW2 v=sqrt(GM/r) ; W =sqrt(GM/r3)
l (angular momentum) = vr = sqrt(GMr) E=1/2 v2 –GM/r = –GM/2r = –(GM)2/2l2 To accrete from r1 to r2, particle must lose DE=GM/2r2 – GM/2r1 … e.g. Radiation Must lose Dl=sqrt(GMr1) - sqrt(GMr2) …Angular Momentum Transfer

4 Viscosity Viscosity force h: dynamical viscotiy
Angular Momemtum Flow Viscosity r v(r) Viscosity force h: dynamical viscotiy h =rn (n: kinematic viscosity) ※Viscosity time scale >Hubble time unless turbulence or magnetic field exists. r-Dr v(r-Dr)

5 Effective Potential Stable Circular Orbit r>=3rg
Binding Energy at r=3rg =0.0572c2 … Mass conversion efficiency

6 Accretion Flow (Disk) Models
Start from Kepler Motion Optically Thick Standard Disk Optically Thin Disk Irradiation Effect, Relativistic Correction, Advection etc. Slim Disk (Optically Thick ADAF) Optically Thin ADAF Start from Free Fall Hydrodynamic Spherical Accretion Flow=Bondi Accretion … transonic flow

7 Standard Accretion Disk Model
Shakura and Sunyaev (1973) Optically Thick Geometrically Thin (r/H<<1) Rotation = Local Keplerian Steady, Axisymmetric Viscosity is proportional to Pressure

8 Standard Disk Model-2 Mass Conservation Angular Velocity
Angular Momentum Conservation Hydrostatic Balance One zone approx.

9 Standard Disk Model-3 Energy Balance Equation of State Opacity
Viscosity Prescription a-disk model

10 Standard Disk Thermal Equilibrium Curve
Corresponds to L~0.1LEdd Double Valued Solutions for fixed S

11 Standard Disk Heating and Cooling
Low Temperature High Temperature

12 Disk Blackbody Spectra
Total Disk (see Mitsuda et al., 1984)

13 Optically Thin Disk Problem of Optically Thick Disk
Fail to explain Hard X-ray, Gamma-ray Emission Optically Thin Disk (Shapiro-Lightman-Earley Disk) (1976) Radiation Temperature can reach Tvir

14 Optically Thin Disk-2 Energy Balance Disk

15 Stability (Secular, Thermal)

16 Advection Terms Energy Equation Energy Balance

17 Optically Thick (& High dM/dt) ADAF

18 Optically Thin (& Low Density) ADAF
Depending on S, Number of Solutions Changes.

19 Thermal Equilibrium ADAF (Optically Thin)

20 Thermal Equilibrium ADAF
ADAF (thick or thin)… H/r ~1 Conical Flow

21 ADAF (Opticallt Thick and Thin)

22 Optically Thin, Two Temperature ADAF

23 Optically Thin, Two Temperature ADAF (Model fit to SgrA)
dM/dt is known from observation. L is too low unless ADAF is considered.

24 Presence of Event Horizon : BH vs NS
Luminosity at Quiescence Lmin NS with Surface BH without Surface Narayan et al., Theory of Black Hole Accretion Discs, 1998, p.177

25 Slim Disk Model = Optically Thick ADAF
Mineshige et al., 2000 NLS1

26 Summary


Download ppt "Accretion onto Black Hole : Advection Dominated Flow"

Similar presentations


Ads by Google