论文标题
具有有限光学深度的积聚盘中辐射传递方程的分析解
Analytical Solutions of Radiative Transfer Equations in Accretion Discs with Finite Optical Depth
论文作者
论文摘要
本文的主要目的是获得与具有有限光学深度的积聚盘垂直结构相关的辐射传递方程的分析解决方案。在非灰色大气中,我们采用光学深度依赖的爱丁顿因子来定义平均强度和辐射应力张量之间的关系。在两种情况下实现了分析溶液:(i)辐射平衡,(ii)具有均匀内部加热的盘,两种情况都假定为局部热力学平衡(LTE)。这些解决方案使我们能够研究散射和光盘光学深度的可能作用,对新出现的强度和其他辐射量。我们的结果表明,在第一种情况下,恒定爱丁顿因子的平均强度的表面值比可变因子大三倍。此外,散射在圆盘的垂直辐射结构中没有作用,并具有第一种情况的假设。另一方面,对于第二种情况,随着光子破坏概率降低(这等同于增加散射),我们会遇到所有辐射量的减少。此外,对于两种总光学深度的情况都小于统一的情况,向极性方向的外部强度远小于圆盘的边缘,这与肢体变形相反。最后,我们将结果应用于基于两个动态模型的积聚系统的频谱。因此,我们可以看到总的光学深度如何随频率而变化,并导致新兴光谱的显着变化。
The main purpose of this paper is to obtain analytical solutions for radiative transfer equations related to the vertical structure of accretion discs with finite optical depth. In the non-gray atmosphere, we employ the optical-depth dependent Eddington factor to define the relationship between the mean intensity and radiation stress tensor. Analytical solutions are achieved for two cases: (i) radiative equilibrium, and (ii) a disc with uniform internal heating and both cases are assumed to be in local thermodynamical equilibrium (LTE), too. These solutions enable us to study the probable role of scattering and disc optical depth on the emergent intensity and other radiative quantities. Our results show that for the first case, the surface value of mean intensity with constant Eddington factor is three times larger than that with a variable factor. Moreover, scattering has no role in the vertical radiative structure of discs with the assumptions of the first case. On the other hand, for the second case, we encounter reductions in all radiative quantities as the photon destruction probability decreases (which is equivalent to increasing scattering). Furthermore, for both cases with total optical depth less than unity, the outward intensity towards the polar direction becomes less than that from the edges of disc which is contrary to limb-darkening. In the end, we apply our results to find the spectrum from accretion systems, based on two dynamical models. Consequently, we can see how the total optical depth varies with frequency and causes remarkable changes in the emergent spectra.