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Sawtooth-like Oscillations of Black Hole Accretion Disks Ryoji Matsumoto (Chiba Univ.) Mami Machida (NAOJ)
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Black Hole Candidates Sometimes Show Quasi Periodic Oscillations Power Density 0.11101000.01Hz GX 339-4 0.11101000.01Hz XTE J1550-564 McClintock and Remillard 2004 LFQPO HFQPO
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Let’s Show How QPOs are Excited by Global 3D MHD Simulations of Black Hole Accretion Flows Gravitational potential : φ= - GM/(r-r g ) Magnetic Field : purely azimuthal Pgas/Pmag =100 at r = r 0 Anomalous Resistivity = (1/Rm) max [(J /v c – 1, 0.0] 2 250*32*384mesh 250*64*384mesh r g =3.0 x 10 6 (M/10M sun ) cm t 0 =r g /c=10 -4 (M/10M sun ) sec Unit
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Basic Equations of Resistive MHD
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Numerical Results for Radiatively Inefficient Hot Disk Power Spectral Density of time variation of accretion rate
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QPOs Appear When a Hot Disk is Cooled Down SurfaceDensity AccretionRate Slim Optically thick Optically thin ADAF Advection Standard disk Radiation Abramowicz et al. 1995 QPO Hot disk Cold disk
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Time Evolution of Cooler Disk Density distributionAzimuthal magnetic field
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Magnetic Reconnection in Accretion Disks Dense blob accretes Current Sheet is Formed Magnetic Reconnection Takes Place Machida and Matsumoto 2003
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Accumulation and Release of Magnetic Energy Magnetic Energy Joule Heating Rate
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Sawtooth Oscillation in Nonlinear Systems Sawtooth oscillation takes place when instability and dissipation coexists (e.g., Tokamak fusion reactors) When dissipation is large Growth of instability Energy release Sawtooth oscillationApproach to a quasi-steady state When dissipation is small
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Growth and Disruption of m=1 Non-Axisymmetric Mode Isosurface of DensityEquatorial Density
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Sawtooth-like Oscillations Excite High Frequency QPOs SawtoothHFQPO 1Hz10Hz100Hz Radial Dependence of PSD PSD of Luminosity
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Another Example: Double Periodic Oscillation Density Distribution
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Time Evolution of Mass Accretion Rate and Joule Heating Rate Mass accretion rate Joule heating
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PSD of Mass Accretion Rate Frequency (Hz)
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Mass Outflow Rate also Shows QPOs (Machida’s poster) Log(Temperature)Density
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Summary Global 3D resistive MHD simulations of cool disks indicate that cool disks show sawtooth-like oscillations During the sawtooth oscillation, amplification of magnetic energy and subsequent release of the magnetic energy repeats The sawtooth oscillation appears when one-armed density distribution develops in the inner torus The frequency of the sawtooth oscillation is several times of the rotation period of the torus, and typically 5-10Hz in stellar mass black holes. This frequency agrees with that of low frequency QPOs in galactic black hole candidates The sawtooth-like oscillation excites high frequency QPOs
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Similar Behaviors have been Observed in Resistive 3D Local MHD Simulations Sano and Inutsuka 2001
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