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Suppression of magnetorotational instability in viscous resistive magnetized Taylor-Couette flow

机译:粘性电阻磁化泰勒 - 汤流动中磁化机构不稳定性的抑制

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摘要

Magnetorotational instability (MRI) is an instability that is responsible for accretion, the phenomenon observed in astrophysical disks, for example around black holes. MRI can be modeled using the equations of MHD. A typical linear analysis in the past made use of the small Prandtl number approximation, which results in dropping one term from these equations. Previously, one of the authors (Herron) showed that the small magnetic Prandtl number approximation suppresses MRI in axisymmetric viscous resistive magnetized Taylor-Couette flow when one has no-slip velocity boundary conditions, and insulating magnetic boundary conditions. We follow up here with a proof that MRI is still suppressed with perfectly conducting magnetic boundary conditions on the cylinders.
机译:磁化机构不稳定性(MRI)是负责accretion的不稳定性,在天体物理磁盘中观察到的现象,例如黑洞。 可以使用MHD的等式进行建模MRI。 过去的典型线性分析利用小普朗特数近似,导致从这些方程滴下一个术语。 以前,其中一个作者(Herron)表明,当具有无滑移速度边界条件和绝缘磁边缘条件时,小磁性PrandT1号近似抑制了轴对称粘性磁化泰勒 - 耦合的MRI。 我们在这里跟进了一个证据,即MRI仍然抑制了气缸上的磁边界条件。

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