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The Magnetorotational Instability
16 October 2004Large Scale Computation in Astrophysics
John F. HawleyUniversity of Virginia
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Collaborators:
Jean-Pierre De Villiers (UVa; U. Calgary)
Steven A. Balbus (UVa)
Julian H. Krolik, Shigenobu Hirose (JHU)
Charles F. Gammie (Illinois)
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Outline
• About the MRI
• Simulations – local disk MRI studies
• Simulations – global Kerr black hole accretion and jet formation
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The Accretion Context
Artist’s conception of a black holebinary with accretion disk
Volumetric rendering of density in3D accretion disk simulation
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The Magnetorotational InstabilityThe MRI is important in accretion disks
because they are locally hydrodynamically stable by the Rayleigh criterion, dL/dR > 0, but are MHD unstable when d2/dR < 0
The MHD instability is:• Local• Linear• Independent of field strength and
orientation
The measure of the importance of a magnetic field isnot determined solely by the value of
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Magnetorotational Instability
• Stability requirement is
• One can always find a small enough wavenumber k so there will be an instability unless
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MRI maximum growth
• Maximum unstable growth rate:
• Maximum rate occurs for wavenumbers
• For Keplerian profiles maximum growth rate and wavelengths:
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Disks and Stars
• Disks – supported by rotation
• Stars – supported by pressure
• Disks – Entropy gradients generally perpendicular to angular velocity gradients
• Stars – BV frequency larger than rotational frequency
• Disks – solid body rotation not possible
• Stars – solid body rotation possible
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Hoiland Criteria
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Regions of Instability: Generalized Hoiland criteria, Keplerian profile
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Numerical Simulations of the MRI: Local and Global
• Local “Shearing boxes”
• Cylindrical disks (semi-global)
• Axisymmetric global
• Full 3D global simulations – Newtonian, pseudo-Newtonian
• Global simulations in Kerr metric
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MRI in a shearing box
• MRI produces turbulence• Maxwell stress
proportional to Pmag
• Maxwell stress dominates over Reynolds
• Field value 10-100• Toroidal field dominates
Angular Velocity perturbationsIn a shearing box
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Stress as a function of rotation profile
Hawley, Balbus, Winters 1999
Solid body Rayleigh unstableKeplerian
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Summary: Turbulence in Disks – Local Simulations
• Turbulence and transport are the inevitable consequence of differential rotation and magnetism
• Hydrodynamic (i.e. non MHD) disk turbulence is not sustained: it has no way to tap locally the free energy of differential rotation
• The MRI is an effective dynamo• The flow is turbulent not viscous. Turbulence is
a property of the flow; viscosity is a property of the fluid. A high Reynolds number turbulent flow does not resemble a low Reynolds number viscous flow
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The Global Picture
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General Relativistic Magnetohydrodynamics Codes
• Wilson (1975)
• Koide et al. (2000)
• Gammie, McKinney & Toth (2003)
• Komissarov (2004)
• De Villiers & Hawley (2003)
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GRMHD implementation
• Fixed Kerr Metric in spherical Boyer Lindquist coordinates
• Graded radial mesh - inner boundary just outside horizon; zones concentrated at equator
• Induction equation of form • F + F + F = 0• Baryon Conservation, stress-energy conservation,
entropy conservation (internal energy); no cooling• First order, time-explicit, operator split finite
differencing • Similar to ZEUS code
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References:
De Villiers & Hawley 2003, ApJ, 589, 458
De Villiers, Hawley & Krolik 2003, ApJ, 599, 1238
Hirose, Krolik, De Villiers, & Hawley 2004, ApJ, 606, 1083
De Villiers, Hawley, Krolik, & Hirose, astroph-0407092
Krolik, Hawley, & Hirose, astroph-0409231
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Initial Torus (density)
r = 25 M
Outer boundary 120M
Initial poloidal field loops
Ensemble of black hole spins: a/M = 0, 0.5, 0.9, 0.998
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Global Disk Simulation
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Accretion flow structures
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Field in main disk
• Field is tangled; toroidal component dominates
• Field is sub-equipartion;
• Field is correlated to provide stress
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Properties of Accretion Disk
• Accretion disk angular momentum distribution near Keplerian
• Disk is MHD turbulent due to the MRI• Maxwell stress drives accretion. Average
stress values 0.1 to 0.01 thermal pressure. Toroidal fields dominate, stress ~ ½ magnetic pressure
• Large scale fluctuations and low-m spiral features
• Low-spin models have come into approximate steady state
• Relative accretion rate drops as a function of increasing black hole spin
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What about Jets? A combination of Rotation, Accretion, Magnetic Field• Young stellar objects – accreting young
star• X-ray binaries – accreting NS or BH• Symbiotic stars – accreting WD• Supersoft X-ray sources – accreting WD• Pulsars – rotating NS• AGN – accreting supermassive BH• Gamma ray burst systems
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Funnel Properties
• Funnel is evacuated• Poloidal radial field created
by ejection of field from plunging inflow into funnel
• Field in pressure equilibrium with corona
• Toroidal field can be generated by black hole spin – outgoing Poynting flux
• Unbound mass outflow at funnel wall
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Origin of funnel field
• Magnetic field is ejected into the centrifugally-evacuated funnel
• Spin of the black hole creates outgoing EM energy
Radial magnetic field energy density
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Poynting Flux for Different Black Hole Spins
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Jet Luminosity
a/M jet jet / ms Poynting
0.0 0.002 0.03 0.06
0.5 0.013 0.16 0.34
0.9 0.029 0.18 0.47
0.998 0.18 0.56 0.87
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Funnel and jets: a summary
• Outflow throughout funnel, but only at funnel wall is there significant mass flux
• Outgoing velocity ~0.4 - 0.6 c in mass flux• Poynting flux dominates in funnel• Jet luminosity increases with hole spin• Fraction of jet luminosity in Poynting flux
increases with spin• Both pressure and Lorentz forces
important for acceleration
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Conclusions
• Magnetic field fundamentally alters stability properties of rotating fluid – Hoiland criteria replaced
• MRI effective in generating turbulence, amplifying field (dynamo), transporting angular momentum
• Centrifugal effects create evacuated funnel• Magnetic fields can launch jets and other
outflows• Rotation of black hole can power jets and affect
disk