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Accretion into Black Hole, and Formation of Magnetically Arrested Accretion Disks

机译:吸积到黑洞中,并形成磁阻吸积盘

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The exact time-dependent solution is obtained for a magnetic field growth during a spherically symmetric accretion into a black hole (BH) with a Schwarzschild metric. Magnetic field is increasing with time, changing from the initially uniform into a quasi-radial field. Equipartition between magnetic and kinetic energies in the falling gas is supposed to be established in the developed stages of the flow. Estimates of the synchrotron radiation intensity are presented for the stationary flow. The main part of the radiation is formed in the relativistic region r ≤ 7 r g , where r g is a BH gravitational radius. The two-dimensional stationary self-similar magnetohydrodynamic solution is obtained for the matter accretion into BH, in a presence of a large-scale magnetic field, under assumption, that the magnetic field far from the BH is homogeneous and its influence on the flow is negligible. At the symmetry plane perpendicular to the direction of the distant magnetic field, the dense quasi-stationary disk is formed around BH, which structure is determined by dissipation processes. Solutions of the disk structure have been obtained for a laminar disk with Coulomb resistivity and for a turbulent disk. Parameters of the shock forming due to matter infall onto the disk are obtained. The radiation spectrum of the disk and the shock are obtained for the 10 M ⊙ BH. The luminosity of such object is about the solar one, for a characteristic galactic gas density, with possibility of observation at distances less than 1 kpc. The spectra of a laminar and a turbulent disk structure around BH are very different. The laminar disk radiates mainly in the ultraviolet, the turbulent disk emits a large part of its flux in the infrared. It may occur that some of the galactic infrared star-like sources are a single BH in the turbulent accretion state. The radiative efficiency of the magnetized disk is very high, reaching ~ 0.5 M ˙ c 2 . This model of accretion was called recently as a magnetically arrested disk (MAD). Numerical simulations of MAD and its appearance during accretion into neutron stars, are considered and discussed.
机译:使用Schwarzschild度量,在球形对称积聚到黑洞(BH)期间获得磁场增长的确切时间相关解决方案。磁场随着时间而增加,从最初的均匀磁场变为准径向磁场。下降的气体中的磁能和动能之间的均分应该在流动的发展阶段中建立。给出了固定流同步辐射强度的估算值。辐射的主要部分在相对论区域r≤7 r g中形成,其中r g是BH引力半径。在存在大范围磁场的情况下,假设远离BH的磁场是均匀的,并且对流动的影响为,则可以得到二维平稳的自相似磁流体动力学解,用于将物质吸附到BH中。微不足道。在垂直于远磁场方向的对称平面上,密集的准平稳盘围绕BH形成,其结构由耗散过程决定。对于具有库仑电阻率的层状盘和湍流盘已经获得了盘结构的解决方案。获得了由于物质落到盘上而形成的冲击的参数。对于10 M⊙BH,获得了磁盘的辐射光谱和震动。对于特定的银河气体密度,这种物体的光度大约是太阳的光度,可以在小于1 kpc的距离处观察到。 BH附近的层流和湍流盘结构的光谱非常不同。层状盘主要在紫外线中辐射,湍流盘在红外中发射很大一部分通量。可能会出现一些银河红外星状源是湍流积聚状态下的单个BH。磁化盘的辐射效率很高,达到〜0.5 M˙c 2。这种吸积模型最近被称为磁阻磁盘(MAD)。考虑并讨论了MAD及其在积聚成中子星期间的出现的数值模拟。

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