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The Story of Thin Accretion Disks

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The Story of Thin Accretion Disks. 2. An Outline. Why ... Sakura & Sunyaev's (1973) Turbulence Scale ~ H so. Then Far from the. BH Horizon. 6 November, 2002 ... – PowerPoint PPT presentation

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Title: The Story of Thin Accretion Disks


1
The Story ofThin Accretion Disks
  • Niayesh Afshordi
  • Princeton Observatory
  • 6 November, 2002

2
An Outline
  • Why Thin Disks?
  • Steady State Accretion
  • And About Viscosity
  • Coronae of Accretion Disks
  • Characteristic Time Scales
  • Instabilities
  • The Moral of the Story

3
Why Thin Disks?
L1 L2 L3 L4 L5
  • In order to
  • Minimize the Energy
  • Conserve the Total Angular Momentum
  • the orbits should become
  • circular and
  • lie on a disk.
  • Then, viscosity leads to a
  • diffusion equation for Surface Density
  • So, matter spreads in the disk and is sunk into
    the center.


L1 L2 L3 L4 L5
4
Steady State Accretion
  • Equations
  • Mass
  • Angular Momentum
  • Radial Momentum
  • Vertical Momentum
  • Energy
  • Sakura Sunyaevs
  • (1973) Turbulence Scale H so
  • Then Far from the
  • BH Horizon

5
Steady State Accretion
  • Spectrum
  • Big Blue Bump (not observed)
  • Emission Lines (not observed)

6
And About Viscosity
  • Molecular Viscosity is too small
  • Keplerian disks are Rayleigh stable, so no
    hydrodynamic turbulence
  • Magnetic disturbances grow due to
  • differential rotation, MHD Turbulence (Balbus
    Hawley 1991)
  • 0.1 gt gt 0.01 and in general varies with time
    and R in simulations.
  • But all simulations ignore cooling which is
    essential for having disks.

density and a volumetric rendering of the
magnetic pressure (Stone et al. 1996)
7
Coronae of Accretion Disks
  • Observational Evidence
  • Polarization (presumably caused by scattering)
  • Reprocessed Emission Lines in X-ray
  • Theoretical Picture
  • Parker Instability and evaporation of magnetic
    field lines/loops
  • Heating due to magnetic reconnection

Parker Instability, http//www.hao.ucar.edu/yfan
/fluxemg.html
8
Coronae of Accretion Disks
9
Characteristic Time Scales
  • Rotational
  • Thermal
  • Infall/Viscous
  • Magneto-rotational

Far From the BH Horizon
This is responsible for the formation of thin disk
10
Instabilities
  • Thermal
  • when heating/cooling equilibrium is not
    stable

Stable
Ionized
Unstable
Recombination
Neutral
Stable
Theoretical duty cycle of a dwarf nova
Light curve observation vs. theory
Lasota, J.-P. 2001, New Astr. Rev, 45, 449
11
Instabilities
  • Viscous
  • When the momentum transfer equations are not
    stable
  • Depends crucially on how changes with other
    physical parameters

Unstable
Stable
R/R_S
12
Instabilities
  • MHD
  • Parker, Magneto-rotational

Deviation of angular momentum from the Keplerian
one in magneto-rotational instability (Stone et
al. 1996)
13
Instabilities
  • Rayleigh (inside marginally stable orbit)
  • Papaloizou-Pringle (azimuthally asymmetric)
  • Jets
  • Is it some kind of instability?
  • ??

14
The Moral of the Story
  • Thin Accretion Disks are inevitable in the
    presence of Cooling and Gravity
  • Almost non of the predictions of the simple
    theory of steady state thin accretion is
    confirmed with observations
  • Most observations can be explained by adding
    extra components, e.g. corona, instabilities,
    MHD, outflows etc.

15
The Moral of the Story
Pringle, J. 1981, ARAA, 19, 137
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