Striped Blandford/Znajek jets from advection of small-scale magnetic field

被引:27
作者
Mahlmann, J. F. [1 ]
Levinson, A. [2 ]
Aloy, M. A. [1 ]
机构
[1] Univ Valencia, Dept Astron & Astrofis, E-46100 Burjassot, Spain
[2] Tel Aviv Univ, Raymond & Beverly Sackler Sch Phys & Astron, IL-69978 Tel Aviv, Israel
关键词
accretion; accretion discs; black hole physics; magnetic fields; methods: numerical; GENERAL-RELATIVISTIC MAGNETOHYDRODYNAMICS; BLACK-HOLE ELECTRODYNAMICS; ELECTROMAGNETIC EXTRACTION; EXPLOSIVE RECONNECTION; PARTICLE-ACCELERATION; ACCRETION DISCS; GRB JETS; SIMULATIONS; FLUX; MHD;
D O I
10.1093/mnras/staa943
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Black hole - accretion disc systems are the central engines of relativistic jets from stellar to galactic scales. We numerically quantify the unsteady outgoing Poynting flux through the horizon of a rapidly spinning black hole endowed with a rotating accretion disc. The disc supports small-scale, concentric, flux tubes with zero net magnetic flux. Our general relativistic force-free electrodynamics simulations follow the accretion on to the black hole over several hundred dynamical time-scales in 3D. For the case of counter-rotating accretion discs, the average process efficiency reaches up to <epsilon > approximate to 0.43, compared to a stationary energy extraction by the Blandford/Znajek process. The process efficiency depends on the cross-sectional area of the loops, i.e. on the product l x h, where l is the radial loop thickness and It its vertical scale height. We identify a strong correlation between efficient electromagnetic energy extraction and the quasi-stationary setting of ideal conditions for the operation of the Blandford/Znajek process (e.g. optimal field line angular velocity and fulfillment of the so-called Znajek condition). Remarkably, the energy extraction operates intermittently (alternating episodes of high and low efficiency) without imposing any large-scale magnetic field embedding the central object. Scaling our results to supermassive black holes, we estimate that the typical variability time-scale of the system is of the order of days to months. Such time-scales may account for the longest variability scales of TeV emission observed, e.g. in M87.
引用
收藏
页码:4203 / 4225
页数:23
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