Accretion onto Black Hole : Advection Dominated Flow K. Hayashida Osaka University
Free Fall & Escape Velocity E=0 (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
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
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)
Effective Potential Stable Circular Orbit r>=3rg Binding Energy at r=3rg =0.0572c2 … Mass conversion efficiency
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
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
Standard Disk Model-2 Mass Conservation Angular Velocity Angular Momentum Conservation Hydrostatic Balance One zone approx.
Standard Disk Model-3 Energy Balance Equation of State Opacity Viscosity Prescription a-disk model
Standard Disk Thermal Equilibrium Curve Corresponds to L~0.1LEdd Double Valued Solutions for fixed S
Standard Disk Heating and Cooling Low Temperature High Temperature
Disk Blackbody Spectra Total Disk (see Mitsuda et al., 1984)
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
Optically Thin Disk-2 Energy Balance Disk
Stability (Secular, Thermal)
Advection Terms Energy Equation Energy Balance
Optically Thick (& High dM/dt) ADAF
Optically Thin (& Low Density) ADAF Depending on S, Number of Solutions Changes.
Thermal Equilibrium ADAF (Optically Thin)
Thermal Equilibrium ADAF ADAF (thick or thin)… H/r ~1 Conical Flow
ADAF (Opticallt Thick and Thin)
Optically Thin, Two Temperature ADAF
Optically Thin, Two Temperature ADAF (Model fit to SgrA) dM/dt is known from observation. L is too low unless ADAF is considered.
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
Slim Disk Model = Optically Thick ADAF Mineshige et al., 2000 NLS1
Summary