多种粉尘的流态不稳定性- 1 .线性生长的有利条件

Zhaohuan Zhu(朱照寰), Chao-Chin Yang(楊朝钦)
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引用次数: 23

摘要

最近的研究表明,作为驱动星子形成的主要机制之一,流的不稳定性可能不像以前认为的那样有效。在某些条件下,考虑多种粉尘时,不稳定性的线性增长率显著降低,且不稳定性增长的时间尺度可能长于圆盘的寿命。为了进一步探索这一发现,我们使用线性分析和气体流体和尘埃颗粒的直接数值模拟来更详细地相互验证和研究不稳定的不稳定模式。我们在粉尘粒径分布$[T_{s,min}, T_{s,max}]$和总固气质量比$\varepsilon$的范围内将先前研究的参数空间扩展一个数量级,并引入粒径分布斜率$q$的第三维度。我们发现收敛的快速增长区和非收敛的慢增长区在$ $ varepsilon$-$T_{s,max}$空间中有一个明显的边界,而该边界对$q$或$T_{s,min}$不明显敏感。此外,不稳定模态的生长不一定由最大的沙尘种主导,较小的沙尘种可以显著提高或降低沙尘种的生长速率。在任何情况下,我们发现收敛的快速增长区以$\varepsilon\gtrsim1$或$T_{s,max}\gtrsim1$为界,这可能代表了星子形成的有利条件。
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Streaming instability with multiple dust species – I. Favourable conditions for the linear growth
Recent study suggests that the streaming instability, one of the leading mechanisms for driving the formation of planetesimals, may not be as efficient as previously thought. Under some disc conditions, the linear growth rate of the instability decreases significantly when multiple dust species are considered, and the instability growth timescale can be longer than the disc lifetime. To further explore this finding, we use both linear analysis and direct numerical simulations with gas fluid and dust particles to mutually validate and study the unstable modes of the instability in more detail. We extend the previously studied parameter space by one order of magnitude in both the range of the dust-size distribution $[T_{s,min}, T_{s,max}]$ and the total solid-to-gas mass ratio $\varepsilon$ and introduce a third dimension with the slope $q$ of the size distribution. We find that the converged fast-growth regime and the non-converged slow-growth regime are distinctly separated by a sharp boundary in the $\varepsilon$-$T_{s,max}$ space, while this boundary is not appreciably sensitive to $q$ or $T_{s,min}$. Moreover, it is not necessary that the largest dust species dominate the growth of the unstable modes, and the smaller dust species can either increase or decrease the growth rate significantly. In any case, we find that the converged fast-growth regime is bounded by $\varepsilon\gtrsim1$ or $T_{s,max}\gtrsim1$, which may represent the favourable conditions for planetesimal formation.
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