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arXiv 1305.7232astro-ph.EPastro-ph.SR
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原行星盘中的风驱动吸积- II:径向依赖和全局图象

Wind-driven Accretion in Protoplanetary Disks --- II: Radial Dependence and Global Picture

Xue-Ning Bai

摘要:

非理想磁流体动力学效应在决定原行星盘(protoplanetary disk,PPD)角动量输运机制和效率以及湍流水平方面起着至关重要的作用,是理解PPD演化和行星形成的关键。在我们以前的工作中,在1 AU,磁旋转不稳定性(MRI)被完全抑制时,欧姆电阻率和双极扩散(AD)被考虑在内,导致在一个层流吸积驱动的磁离心风。在这项工作中,我们研究了径向依赖的层流风的解决方案,使用本地剪切盒模拟。得到了层流风角动量输运的标度关系,发现风驱动吸积率可以近似为M_dot~ 0.91 × 10 ^(-8)R_AU^(1.21)(B_z/10 mG)^(0.93)M_Sun/yr,其中B_z是穿过盘的大尺度垂直磁场的强度。该结果与磁盘表面密度无关。给出了层流风解存在的四个判据:1).欧姆电阻率占主导地位的中平面区域; 2)。AD在盘上层占主导地位;存在(不太弱)净垂直磁通量。4)。充分电离的气体超出磁盘表面。对于典型的PPD吸积率,在盘的内部区域从~0.3 AU到大约5-10 AU,所有这些标准都可能得到满足。超过这个半径,角动量传输很可能由于MRI和盘风的结合而进行,并最终由MRI(在存在强AD的情况下)在外盘中主导。我们的模拟结果提供了一个新的范例在PPD的吸积过程中的关键成分。

英文摘要:

Non-ideal magnetohydrodynamical effects play a crucial role in determining the mechanism and efficiency of angular momentum transport as well as the level of turbulence in protoplanetary disks (PPDs), which are key to understanding PPD evolution and planet formation. It was shown in our previous work that at 1 AU, the magnetorotational instability (MRI) is completely suppressed when both Ohmic resistivity and ambipolar diffusion (AD) are taken into account, resulting in a laminar flow with accretion driven by magnetocentrifugal wind. In this work, we study the radial dependence of the laminar wind solution using local shearing-box simulations. Scaling relation on the angular momentum transport for the laminar wind is obtained, and we find that the wind-driven accretion rate can be approximated as M_dot~0.91x10^(-8)R_AU^(1.21)(B_z/10mG)^(0.93)M_Sun/yr, where B_z is the strength of the large-scale vertical magnetic field threading the disk. The result is independent of disk surface density. Four criteria are outlined for the existence of the laminar wind solution: 1). Ohmic resistivity dominated midplane region; 2). AD dominated disk upper layer; 3). Presence of (not too weak) net vertical magnetic flux. 4). Sufficiently well ionized gas beyond disk surface. All these criteria are likely to be met in the inner region of the disk from ~0.3 AU to about 5-10 AU for typical PPD accretion rates. Beyond this radius, angular momentum transport is likely to proceed due to a combination of the MRI and disk wind, and eventually dominated by the MRI (in the presence of strong AD) in the outer disk. Our simulation results provide key ingredients for a new paradigm on the accretion processes in PPDs.

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