dorsal/arxiv
View SchemaTransonic instabilities in accretion disks
| Authors | Hans Goedbloed, Rony Keppens |
|---|---|
| Categories | |
| ArXiv ID | physics/0411180 |
| URL | https://arxiv.org/abs/physics/0411180 |
Abstract
In two previous publications$^{1,2}$, we have demonstrated that stationary rotation of magnetized plasma about a compact central object permits an enormous number of different MHD instabilities, with the well-known magneto-rotational instability as just one of them. We here concentrate on the new instabilities found that are driven by transonic transitions of the poloidal flow. A particularly promising class of instabilities, from the point of view of MHD turbulence in accretion disks, is the class of {\em trans-slow Alfven continuum modes}, that occur when the poloidal flow exceeds a critical value of the slow magnetosonic speed. When this happens, virtually every magnetic/flow surface of the disk becomes unstable with respect to highly localized modes of the continuous spectrum. The mode structures rotate, in turn, about the rotating disk. These structure lock and become explosively unstable when the mass of the central object is increased beyond a certain critical value. Their growth rates then become huge, of the order of the Alfven transit time. These instabilities appear to have all requisite properties to facilitate accretion flows across magnetic surfaces and jet formation.[1] R. Keppens, F. Casse, J.P. Goedbloed, "Waves and instabilities in accretion disks: Magnetohydrodynamic spectroscopic analysis", Astrophys. J. {\bf 569}, L121--L126 (2002).[2] J.P. Goedbloed, A.J.C. Belien, B. van der Holst, R. Keppens, "Unstable continuous spectra of transonic axisymmetric plasmas", Phys. Plasmas {\bf 11}, 28--54 (2004).
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"abstract": "In two previous publications$^{1,2}$, we have demonstrated that stationary\nrotation of magnetized plasma about a compact central object permits an\nenormous number of different MHD instabilities, with the well-known\nmagneto-rotational instability as just one of them. We here concentrate on the\nnew instabilities found that are driven by transonic transitions of the\npoloidal flow. A particularly promising class of instabilities, from the point\nof view of MHD turbulence in accretion disks, is the class of {\\em trans-slow\nAlfven continuum modes}, that occur when the poloidal flow exceeds a critical\nvalue of the slow magnetosonic speed. When this happens, virtually every\nmagnetic/flow surface of the disk becomes unstable with respect to highly\nlocalized modes of the continuous spectrum. The mode structures rotate, in\nturn, about the rotating disk. These structure lock and become explosively\nunstable when the mass of the central object is increased beyond a certain\ncritical value. Their growth rates then become huge, of the order of the Alfven\ntransit time. These instabilities appear to have all requisite properties to\nfacilitate accretion flows across magnetic surfaces and jet formation.[1] R.\nKeppens, F. Casse, J.P. Goedbloed, \"Waves and instabilities in accretion disks:\nMagnetohydrodynamic spectroscopic analysis\", Astrophys. J. {\\bf 569},\nL121--L126 (2002).[2] J.P. Goedbloed, A.J.C. Belien, B. van der Holst, R.\nKeppens, \"Unstable continuous spectra of transonic axisymmetric plasmas\", Phys.\nPlasmas {\\bf 11}, 28--54 (2004).",
"arxiv_id": "physics/0411180",
"authors": [
"Hans Goedbloed",
"Rony Keppens"
],
"categories": [
"physics.plasm-ph",
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],
"title": "Transonic instabilities in accretion disks",
"url": "https://arxiv.org/abs/physics/0411180"
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