Download - MHG of large scale magnetic field in the advective accretion disks G.S. Bisnovatyi-Kogan IKI RAN
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MHG of large scale magnetic field in the advective accretion disks
G.S. Bisnovatyi-Kogan
IKI RAN
MG12, Paris, July 15, 2009
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Accretion disk around BH with large scale magnetic field (non-rotating disk)
Bisnovatyi-Kogan , Ruzmaikin, Ap. Space Sci. 28, 45 (1974); 42, 401 (1976)
Sketch of the magnetic field threading an
accretion disk. Shown increase of the field owing to flux freezing in the accreting disk matter
At presence of large-scale magnetic field the efficiency of accretion is alvays large (0.3-0.5) of the rest mass energy
flux
Turbulent electrical conductivity
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Magnetic diffusivity is of the order of kinematic viscosity in the turbulent disk, D>>1
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Bisnovatyi-Kogan, Lovelace, 2007, ApJL, 667: L167–L169, 2007 October 1
Large scale magnetic field is amplified during the disk accretion, due to currents in the radiative outer layers, with
very high electrical conductivity
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In this situation we may expect a nonuniform distribution of the angular velocity over the disk thickness: The main body of the turbulent disk is rotates with the velocity close to the Keplerian one, and outer optically thin layers rotate substantially slower by ~ 30%.
B(min) ~ 10^8/sqrt(M_solar) for Schwarzschild BH
Turbulence in the outer layers is produced by shear instability
Magnetic field may be ~10 times larger for rapid Kerr BH
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ADVECTION OF MAGNETIC FIELDS IN ACCRETION DISKS: NOT SO DIFFICULT AFTER ALL
D. M. Rothstein, and R. V. E. Lovelace
arXiv 0801.2158
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ADVECTION/DIFFUSION OF LARGE-SCALE B FIELD IN ACCRETION DISKS
R.V. E. Lovelace, D.M. Rothstein, & G.S. Bisnovatyi-Kogan
arXiv:0906.0345v1 [astro-ph] 1 Jun
Here, we calculate the vertical (z) profiles of the stationary accretion flows (with radial and azimuthal components), and the profiles of the large-scale, magnetic field taking into account the turbulent viscosity
and diffusivity due to the MRI and the fact that the turbulence vanishes at the surface of the disk.
Boundary condition on the disk surface:
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Accretion disk around a black hole in binary system
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rateaccretion
luminosity
2
M
LcM
Lη
electronsfor section -cross scatteringThomson
proton of mass
4
T
p
T
pE
σ
m
σ
cπGMmL
T
pEE cσ
πGMm
c
LM
42
Efficiency of the conversion of the energy into luminosity
Eddington luminosity
(critical luminosity)
Critical accretion rate
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pressure
stress viscous
P
t
Pt
r
r
locityangular ve
density
tcoefficien viscositykinematic
νdr
drt r
Algebraic relation
(Shakura 1972)
Angular velocity gradientdependent viscous stress
“alpha disk” model
,
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Angular momentum balance
Standard model (local, )
-accretion rate, r – radius, h- semithickness of the disk
l – specific angular momentum
- integration constant, specific angular momentum at the inner boundary
Mass conservation equationv– radial velocity
Gravitational potential, Paczynski� – Wiita, 1980
=
- heating rate,
- cooling rate
Energy balance
Vertical pressure balance
= = Radial equilibrium, thin disk
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Two families of solutions to the steady state disk structure equations, for given alpha,
1. Optically thick ( τ* >> 1 ) – unstable in the radiation
dominated region with vertical radiative transfer
Emission of AGN in the UV - soft X-ray range
( T ~ 105 K)
Emission of stellar BHs in the X-ray range
( T ~ 107 K)
2. Optically thin ( τ* << 1) - globally unstable
Hard X-ray and γ-ray emission of AGN and stellar BHs
( T ~ 109 K)
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X-ray spectral states in Cyg X-1. Classical soft (red) and hard (blue)
States, from Gierli´nski et al. (1999).
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Detailed description is in the paper B.-K., Blinnikov A&A (1977), 59, 111
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Sketch of picture of a disk accretion on to a black hole at sub-critical luminosity.
I – radiation dominated region, electron scattering.II – gas-dominated region, electron scattering.III- gas-dominated region, Krammers opacity.
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Optically thick limit ( τ* >> 1, τ0 >> 1 )F0 = 2 a Tc
4c / 3 τ0
Optically thin limit ( τ* << 1, τ0 >> τ* )
F0 = a Tcc τα
Radiative flux from the disk surface
τ0 – total optical depth to electron scattering
τα - total optical depth to absorption
τ* – effective optical depth, τ* = (τ0 τα) ½
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Solutions without advection(BH mass = 10 solar masses, α=0.5) r*=r/rg ,rg =GM/c2
50m
36m
30m
20m
10m
The dependence of the Thomson scattering depth on the radius
Eddington limitcorresponds to =16
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Solutions without advection(BH mass = 10 solar masses, α=0.5)
50m
36m
30m
20m
The dependence of the effective optical depth on the radius
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Taking advection into account
The vertically averaged energy conservation
Paczynski. Bisnovatyi-Kogan (1981)
Qadv=Q+ - Q-,
The equation of motion in radial direction
rΩΩdr
dP
ρdr
dvv K 221
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R
ccβT
ττ
τaTβ)P (
P
Pβ
DN
dr
d
vr
cα
r
lΩ
rc
ΩΩ
Ω
Ωr
D
N
c
v
c
cr
D
N
v
vr
s
*
cg
sin
sK
K
s
s
´
K
22
20
04
insK
2
2
22
22
2
2
3
2
3
41
3
41
31 ,
M , α ,l , c , v, β ,Ω , Ω ,r of functions - ,
where
11
Set of equations for “αP” viscosity prescription with advection
Artemova Yu. V.Bisnovatyi-Kogan G. S.Igumenshchev I. V.Novikov I. D.ApJ, 2006, 637:968–977
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Boundary conditions
r >> 100 rg → ” Standard disk ”
Parameters in singular point must satisfy conditions
N = 0
D = 0
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The behavior of the integral curves in presence of singular points
Outer singular point is a non-important artefact
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50m
36m
30m
20m
10m
Solutions with advection(BH mass = 10 solar masses, α=0.5)
The dependence of the Thomson scattering depth on the radius
Eddington limitcorresponds to =16
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Solutions with advection(BH mass = 10 solar masses, α=0.5)
50m
36m
30m
20m
The dependence of the effective optical depth on the radius
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The dependence of the effective optical depth on the radius
Solutions with advection(BH mass = 10 solar masses, α=0.5, accretion rate = 30.0)
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With optical depth transition
Without optical depth transition
The dependence of the temperature on the radius
Artemova, Bisnovatyi-Kogan, Igumenshchev , Novikov,
ApJ, 2006, 637, 968
Solutions with advection(BH mass = 10 solar masses, α=0.5, accretion rate = 48.0)
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With optical depth transition
Without optical depth transition
Solutions with advection(BH mass = 10 solar masses, α=0.5, accretion rate = 48.0)
The dependence of the effective optical depth on the radius
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3. Solutions for advective disks exist for all luminosities
4. At high luminosities the solution represents disk, which is optically thick outside, and optically thin inside.
5. The temperature in the optically thin region is about a billion K, and may be responsible for appearance of hard tails (as well as hot corona, or instabilities)
Conclusons
1. Jets from accretion disk are magnetically collimated bylarge scale poloidal magnetic field
2. This field is amplified during disk accretion due to high conductivity in outer radiative layers