论文标题
旋转裂变后小行星系统的动力学
Dynamics of asteroid systems post rotational fission
论文作者
论文摘要
据信,在近地物中发现的小行星二进制物是由旋转裂变形成的。在本文中,我们旨在研究裂变后的小行星系统的动态演变。初始条件被建模为触点二进制,类似于Boldrin等人。 (2016)。两种身体都是建模为椭圆形的,并且次要的二件$ y $轴的初始旋转角度。此外,我们考虑六种不同的情况,三个,其中次要的密度有所不同,三个不同的情况变化了。模拟考虑了次级的45个不同的初始倾斜角,每个角度都有37个不同的质量比。我们在触点二进制达到旋转裂变极限的那一刻开始动力学模拟,我们的模型确保了两个物体表面之间的最接近距离始终保持在1 cm。两种物体之间的力,扭矩和重力电位是使用新开发的表面积分方案进行建模的,从而为两个椭圆形提供了精确的结果。我们发现,超过80%的模拟以两种影响的影响结束,并且当次级密度较低或延长时,身体之间的碰撞更为常见。与Pravec等人的小行星对数据进行比较。 (2019年)我们发现,次要的密度和形状的变化可以解释观察到的对旋转期间看到的一些扩散。此外,次级也可能达到表面破坏的自旋极限,从而产生三元/多重系统。我们发现,次级裂变通常发生在接触二进制分离后的前五个小时内,并且当次级密度较小或伸长时更为常见。
Asteroid binaries found amongst the Near-Earth objects are believed to have formed from rotational fission. In this paper, we aim to study the dynamical evolution of asteroid systems the moment after fission. The initial condition is modelled as a contact binary, similar to that of Boldrin et al. (2016). Both bodies are modelled as ellipsoids, and the secondary is given an initial rotation angle about its body-fixed $y$-axis. Moreover, we consider six different cases, three where the density of the secondary varies, and three where we vary its shape. The simulations consider 45 different initial tilt angles of the secondary, each with 37 different mass ratios. We start the dynamical simulations at the moment the contact binary reaches a spin fission limit, and our model ensures that the closest distance between the surfaces of the two bodies is always kept at 1 cm. The forces, torques and gravitational potential between the two bodies are modelled using a newly developed surface integration scheme, giving exact results for two ellipsoids. We find that more than 80% of the simulations end with the two bodies impacting, and collisions between the bodies are more common when the density of the secondary is lower, or when it becomes more elongated. When comparing with data on asteroid pairs from Pravec et al. (2019) we find that variations in density and shape of the secondary can account for some of the spread seen in the rotation period for observed pairs. Furthermore, the secondary may also reach a spin limit for surface disruption, creating a ternary/multiple system. We find that secondary fission typically occurs within the first five hours after the contact binary separates, and is more common when the secondary is less dense or more elongated.