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GR/MHD SIMULATIONS OF ACCRETION ONTO BLACK HOLES (cont.) Jean-Pierre De Villiers John Hawley Shigenobu Hirose JHK
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TOPICS Magnetic Field Distribution and Structure Accretion Fluctuations Angular Momentum Flow and Stress Distribution Connection to Dissipation Possible Consequences for Observations
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Magnetic Field Intensity a/M=0 a/M=0.5 a/M=0.9a/M=0.998
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Field-line Shapes a/M = 0.9: disk bodya/M = 0.9: corona For more detail, see poster by S. Hirose
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Accretion History
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Accretion Rate Power Spectrum
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Angular Momentum Flow Magnetic torques cause outward angular momentum flow, permit mass inflow Steady-state inflow achieved when angular momentum losses to outward rings match gains from inner Net flow subtracts torques from that associated with rest-mass of matter, its enthalpy, and advected magnetic energy
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Angular Momentum Flux Key: = matter, = torque, = Angular momentum at these radii increases over time
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Novikov-Thorne Model Geometrically-thin, time-steady disks Conserve rest-mass, energy, angular momentum Guess the conserved angular momentum flux by assuming zero stress inside the marginally stable orbit. Compute stress, dissipation, energy release
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Exception! Magnetic Fields E.g., as pointed out in Page & Thorne (1974), Thorne (1974), K. (1999), Gammie (1999), Magnetic fields can stretch across the marginally stable region, exerting large stresses even when connected to matter of little inertia
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Fluid Frame Stress
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Angular Momentum Flux per Rest-Mass Large outward a.m. flux carried electromagnetically
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Two Views of Dissipation Global: difference between orbital energy released in accretion and work done by torques---related to integrated stress Local: resistivity, reconnection, etc.--- related to small-scale magnetic structure
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Locations of Dissipation (?) a/M=0 a/M=0.5 a/M=0.9a/M=0.998
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Dynamical Implications Limit to spin-up? Larger radiation efficiency? Altered surface density in inner disk, depends on black hole spin Strong fluctuations Are we seeing a Blandford-Znajek analog?
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Radiation Implications Greater dissipation overall, particularly in inner disk and plunging region---harder spectra, especially edge-on, more illumination of outer disk by returning radiation Coronal activity concentrated in inner region (?)--- test with Fe K alpha profiles Inner edge of thermal radiation not same as inner edge for reflection not equal to radius of ISCO Fluctuations drive “red noise” in lightcurves (?)
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