首页> 外文期刊>The Astrophysical journal >SMOOTHED PARTICLE HYDRODYNAMIC SIMULATIONS OF GALACTIC GASEOUS DISK WITH BAR: DISTRIBUTION AND KINEMATIC STRUCTURE OF MOLECULAR CLOUDS TOWARD THE GALACTIC CENTER
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SMOOTHED PARTICLE HYDRODYNAMIC SIMULATIONS OF GALACTIC GASEOUS DISK WITH BAR: DISTRIBUTION AND KINEMATIC STRUCTURE OF MOLECULAR CLOUDS TOWARD THE GALACTIC CENTER

机译:带棒的银质气碟的光滑颗粒水力模拟:分子向银河中心的分布和运动结构

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摘要

We have performed smoothed particle hydrodynamic (SPH) simulations to study the response of molecular clouds in the Galactic disk to a rotating bar and their subsequent evolution in the Galactic center (GC) region. The Galactic potential in our models is contributed by three axisymmetric com- ponents (massive halo, exponential disk, compact bulge) and a nonaxisymmetric bar. These components are assumed to be invariant in time in the frame corotating with the bar. Some noticeable features such as an elliptical outer ring, spiral arms, a gas-depletion region, and a central concentration have been developed due to the influence of the bar. The rotating bar induces noncircular motions of the SPH particles, but hydrodynamic collisions tend to suppress the random components of the velocity. The velocity field of the SPH particles is consistent with the kinematics of molecular clouds observed in HCN (1-0) transition, these clouds are thought to be very dense clouds. However, the longitude-velocity (l-v) diagram of the clouds traced by CO is quite different from that of our SPH simulation, being more similar to that obtained from simulations using collisionless particles. The l-v diagram of a mixture of collisional and collisionless particles gives better reproduction of the kinematic structures of the GC clouds observed in the CO line. The fact that the kinematics of HCN clouds can be reproduced by the SPH particles suggests that the dense clouds in the GC are formed via cloud collisions induced by the rotating bar.
机译:我们已经执行了平滑粒子流体动力学(SPH)模拟,以研究银河系盘中分子云对旋转棒的响应以及它们在银河系中心(GC)区域的后续演化。我们模型中的银河系潜力是由三个轴对称组件(大量光晕,指数圆盘,紧实的凸起)和一个非轴对称杆所贡献的。假定这些分量在随杆一起旋转的框架中在时间上是不变的。由于棒的影响,已经开发出一些值得注意的特征,例如椭圆形的外环,螺旋臂,气体消耗区域和中心浓度。旋转杆引起SPH粒子的非圆周运动,但是流体动力碰撞往往会抑制速度的随机分量。 SPH粒子的速度场与在HCN(1-0)跃迁中观察到的分子云的运动学一致,这些云被认为是非常致密的云。但是,由CO跟踪的云的经度-速度(l-v)图与我们的SPH模拟的图有很大不同,与从使用无碰撞粒子的模拟中获得的图更相似。碰撞粒子与无碰撞粒子的混合物的lv图可以更好地再现在CO线中观察到的GC云的运动学结构。 HCN云的运动学可以通过SPH粒子重现的事实表明,GC中的密集云是通过旋转棒引起的云碰撞形成的。

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