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arXiv 1607.01017astro-ph.GAastro-ph.SR
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原行星盘的正面吸积

Face-on accretion onto a protoplanetary disc

T. P. G. Wijnen, O. R. Pols, F. I. Pelupessy, S. Portegies Zwart

摘要:

球状星团(GC)是已知的拥有多个恒星星族。为了解释这些观测结果,巴斯蒂安等人提出了一种设想,即第二个星族是由富集物质吸积到初始GC星族中的低质量恒星上形成的。这个想法是,低质量的前主序星在穿过GC核心时,将同代大质量恒星排出的气体扫到它们的原行星盘中。我们进行模拟与2个不同的平滑粒子流体动力学代码,以调查如果一个低质量的恒星包围的原行星盘可以吸积的富集材料的量在这种情况下所需的。我们专注于气体加载速率到光盘和恒星以及光盘的寿命。我们发现,气体加载速率是一个因素2小于几何速率,因为有效的截面的磁盘是小于其表面积。无论分辨率如何,两种代码的加载速率均一致。圆盘在高分辨率运行中获得质量,但在10^4年的时间尺度上损失角动量。在我们的模拟中,两种效应决定了(特定)角动量的损失:1)连续的冲压压力剥离和2)没有方位角动量的物质吸积。我们的研究和以前的工作表明,前者,占主导地位的过程主要是由数值而不是物理效应,而后者不是。后一个过程使圆盘变得更加紧凑,从而增加了较小半径处的表面密度分布。当流体第一次撞击阀瓣时,阀瓣尺寸首先由柱塞压力决定。进一步的演化是由盘的比角动量的减小所控制的。我们的结论是,光盘的大小和寿命可能不足以吸积巴斯蒂安等人所需的质量。的情景。

英文摘要:

Globular clusters (GCs) are known to harbor multiple stellar populations. To explain these observations Bastian et al. suggested a scenario in which a second population is formed by the accretion of enriched material onto the low-mass stars in the initial GC population. The idea is that the low-mass, pre-main sequence stars sweep up gas expelled by the massive stars of the same generation into their protoplanetary disc as they move through the GC core. We perform simulations with 2 different smoothed particle hydrodynamics codes to investigate if a low-mass star surrounded by a protoplanetary disc can accrete the amount of enriched material required in this scenario. We focus on the gas loading rate onto the disc and star as well as on the lifetime of the disc. We find that the gas loading rate is a factor of 2 smaller than the geometric rate, because the effective cross section of the disc is smaller than its surface area. The loading rate is consistent for both codes, irrespective of resolution. The disc gains mass in the high resolution runs, but loses angular momentum on a time scale of 10^4 yrs. Two effects determine the loss of (specific) angular momentum in our simulations: 1) continuous ram pressure stripping and 2) accretion of material with no azimuthal angular momentum. Our study and previous work suggest that the former, dominant process is mainly caused by numerical rather than physical effects, while the latter is not. The latter process causes the disc to become more compact, increasing the surface density profile at smaller radii. The disc size is determined in the first place by the ram pressure when the flow first hits the disc. Further evolution is governed by the decrease in the specific angular momentum of the disc. We conclude that the size and lifetime of the disc are probably not sufficient to accrete the amount of mass required in Bastian et al.'s scenario.

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