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arXiv 1503.06953astro-ph.SRastro-ph.EPastro-ph.HEphysics.flu-dyn
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天体物理圆盘中的垂直剪切不稳定性

On the vertical-shear instability in astrophysical discs

Adrian J. Barker, Henrik N. Latter

摘要:

我们探讨的线性稳定性的天体物理光盘表现出垂直剪切,这是出现时,有一个径向变化的温度或熵。这样的磁盘受到“垂直剪切不稳定性”,最近的非线性模拟显示,驱动器的MRI稳定区域的原行星盘的流体动力学活动。我们首先使用Nelson等人(2013)推导的准全局简化模型重新审视局部等温盘。这种分析,然后扩展到全球轴对称扰动的圆柱形域。我们还推导和研究了一个简化的模型,描述光盘与幂律径向熵分布(“局部多变光盘”),这是有点更现实的,因为他们拥有物理(而不是数值)表面。在所有情况下,增长最快的模式具有非常短的波长,并且局限于圆盘表面(如果存在),在那里垂直剪切最大。另一类适度增长的垂直全球体模式被激发,对应于不稳定的经典惯性波(“r-模式”)。我们讨论这两种类型的模式的属性,并强调那些增长最快的发生在最短的可用长度尺度(由数值网格或物理粘性长度确定)。这种不适定性使得对不稳定性的模拟难以解释。最后,我们对非线性饱和和由此产生的角动量输运进行了一些简短的推测。

英文摘要:

We explore the linear stability of astrophysical discs exhibiting vertical shear, which arises when there is a radial variation in the temperature or entropy. Such discs are subject to a "vertical-shear instability", which recent nonlinear simulations have shown to drive hydrodynamic activity in the MRI-stable regions of protoplanetary discs. We first revisit locally isothermal discs using the quasi-global reduced model derived by Nelson et al. (2013). This analysis is then extended to global axisymmetric perturbations in a cylindrical domain. We also derive and study a reduced model describing discs with power law radial entropy profiles ("locally polytropic discs"), which are somewhat more realistic in that they possess physical (as opposed to numerical) surfaces. In all cases the fastest growing modes have very short wavelengths and are localised at the disc surfaces (if present), where the vertical shear is maximal. An additional class of modestly growing vertically global body modes is excited, corresponding to destabilised classical inertial waves ("r-modes"). We discuss the properties of both types of modes, and stress that those that grow fastest occur on the shortest available length scales (determined either by the numerical grid or the physical viscous length). This ill-posedness makes simulations of the instability difficult to interpret. We end with some brief speculation on the nonlinear saturation and resulting angular momentum transport.

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