论文标题
非放射和非气体天体外流。 xi。 ry tau的情节环境的模拟
Nonradial and nonpolytropic astrophysical outflows. XI. Simulations of the circumstellar environment of RY Tau
论文作者
论文摘要
语境。最近有观察证据表明,Ry Tau可能会呈现两个不同的流出阶段,一个静止的阶段和一个更活跃的流出阶段。我们尝试建模这种现象。目标。我们已经根据分析解决方案进行了新的2.5D磁磁动力学模拟Ry Tau的可能吸收流出环境,以减少松弛时间。方法。我们用作初始条件,用于对Ry Tau微型射流进行建模的分析自相似解决方案。在磁层的闭合场线区域中,我们通过增加密度和速度来逆转流动方向并提高积聚速率。我们还实施了加热速率,并根据流量的速度对其进行了调整。积聚磁盘被视为边界条件。结果。模拟表明,恒星射流和积聚的磁层仅在几个恒星旋转中达到了稳态,从而证实了自相似溶液的稳健性和稳定性。另外,观察到两种类型的行为类似于Ry Tau中观察到的行为。稳定的恒星流出和磁层流入通过低静电力区域分离,或者恒星射流和磁层吸积之间的相互作用会产生冠状动脉质量弹出,该冠状动脉质量弹出源自磁盘,并弹跳到恒星上。结论。与在Ry Tau中观察到的行为变化相吻合的质量损失率与质量积聚率的比率,在微型射流初始分析期间已测量的比率范围内。
Context. There are recent observational evidences that RY Tau may present two different outflow stages, a quiescent one and a more active one. We try to model that phenomenon. Aims. We have performed new 2.5D magneto-hydrodynamical simulations of the possible accretion-outflow environment of RY Tau based on analytical solutions to reduce the relaxation time. Methods. We used as initial conditions the analytical self-similar solution we used to model the RY Tau micro jet. In the closed field line region of the magnetosphere we have reversed the direction of the flow and increased the accretion rate by increasing the density and the velocity. We have also implemented the heating rate and adjusted it according to the velocity of the flow. The accretion disk is treated as a boundary condition. Results. The simulations show that the stellar jet and the accreting magnetosphere attain a steady state in only a few stellar rotations, confirming the robustness and stability of self-similar solutions. Additionally, two types of behavior were observed similar to the one observed in RY Tau. Either the steady stellar outflow and magnetospheric inflow are separated by a low static force free region or the interaction between the stellar jet and the magnetospheric accretion creates coronal episodic mass ejections originating from the disk and bouncing back onto the star. Conclusions. The ratio of mass loss rate to mass accretion rate that coincides with the change of behaviour observed in RY Tau, lays within the range of ratios that have been measured during the period of the micro jet initial analysis.