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首页> 外文期刊>Astronomy reports >Formation of a radiative wind and accretion disk in microquasars. Generation of flare activity in the disk due to an increase in the supply of material to the Lagrange point L-1. The system LMC X-3
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Formation of a radiative wind and accretion disk in microquasars. Generation of flare activity in the disk due to an increase in the supply of material to the Lagrange point L-1. The system LMC X-3

机译:在微类星体中形成辐射风和吸积盘。由于拉格朗日点L-1的材料供应增加,在磁盘中产生了耀斑活动。系统LMC X-3

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Three-dimensional numerical hydrodynamical modeling of a radiative wind and accretion disk in a close binary system with a compact object is carried out, using the massive X-ray binary LMC X-3 as an example. This system contains a precessing disk, and may have relativistic jets. These computations show that an accretion disk with a radius of about 0.20 (in units of the component separation) forms from the radiative wind from the donor when the action of the wind on the central source is taken into account, when the accretion rate is equal to the observed value (about 3.0 x 10(-8) M-circle dot/year, which corresponds to the case when the donor overflows its Roche lobe by nearly 1%). It is assumed that the speed of the donor wind at infinity is about 2200 km/s. The disk that forms is geometrically thick and nearly cylindrical in shape, with a low-density tunnel at its center extending from the accretor through the disk along the rotational axis. We have also modeled a flare in the disk due to short-term variations in the supply of material through the Lagrange point L-1, whose brightnesses and durations are able to explain flares in cataclysmic variables and X-ray binaries. The accretion disk is not formed when the donor underfills its Roche lobe by 0.5%, which corresponds to an accretion rate onto the compact object of 2.0 x 10(-9) M-circle dot/year. In place of a disk, an accretion envelope with a radius of about 0.03 forms, within which gas moves along very steep spiral trajectories before falling onto the compact object. As in the accretion-disk case, a tunnel forms along the rotational axis of the accretion envelope; a shock forms behind the accretor, where flares occur in a compact region a small distance from the accretor at a rate of about six flares per orbital period, with amplitudes of about 10(m) or more. The flare durations are two to four minutes, and the energies of individual particles at the flare maximum are about 100-150 keV. These flares appear to be analogous to the flares observed in gamma-ray and X-ray burst sources. We accordingly propose a model in which these phenomena are associated with massive, close X-ray binary systems with component-mass ratios exceeding unity, in which the donor does not fill its Roche lobe. Although no accretion disk forms around the compact object, an accretion region develops near the accretor, where the gamma-ray and X-ray flares occur.
机译:以大型X射线二进制LMC X-3为例,对具有紧凑物体的密闭二元系统中的辐射风和吸积盘进行了三维水动力数值模拟。该系统包含一个进动盘,并且可能具有相对论射流。这些计算表明,当考虑到风在中央源上的作用时,当考虑到风对中心源的作用时,来自供体的辐射风会形成一个半径约为0.20(以成分分离单位为单位)的吸积盘。到观测值(约3.0 x 10(-8)M圆点/年,对应于捐赠者的罗氏瓣溢出近1%的情况)。假定无穷大的供风速度约为2200 km / s。所形成的圆盘在几何形状上是厚的,并且几乎是圆柱形的,在其中心处具有低密度通道,该低密度通道从增生器沿着旋转轴延伸穿过圆盘。由于通过拉格朗日点L-1进行的物料供应的短期变化,我们还对圆盘中的耀斑进行了建模,该点的亮度和持续时间能够解释催化变量和X射线双星中的耀斑。当供体未充分填充其罗氏瓣0.5%时,就不会形成吸积盘,这相当于致密物体上的吸积率为2.0 x 10(-9)M圆点/年。代替圆盘,形成半径大约为0.03的吸积膜,其中气体沿着非常陡峭的螺旋轨迹运动,然后掉落到紧凑的物体上。与吸积盘一样,沿吸积膜的旋转轴形成一个通道。激振器后面会形成冲击,在与激振器相距一小段距离的紧凑区域中,耀斑以每个轨道周期约六个耀斑的速度发生,振幅约为10(m)或更大。耀斑持续时间为两到四分钟,并且耀斑最大值处的单个粒子的能量约为100-150 keV。这些耀斑似乎类似于在伽马射线和X射线猝发源中观察到的耀斑。因此,我们提出了一个模型,其中这些现象与组分质量比超过1的大规模,紧密的X射线二元系统相关,其中供体未填充其罗氏瓣。尽管在致密物体周围未形成吸积盘,但在吸积体附近会形成吸积区域,在该区域会发生伽马射线和X射线耀斑。

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