Abstract
The helical magnetorotational instability of the magnetized Taylor-Couette flow is studied numerically in a finite cylinder. A distant upstream insulating boundary is shown to stabilize the convective instability entirely while reducing the growth rate of the absolute instability. The reduction is less severe with greater height. After we model the boundary conditions properly, the wave patterns observed in the experiment turn out to be a noise-sustained convective instability. After the source of the noise resulting from unstable Ekman and Stewartson layers is switched off, a slowly decaying inertial oscillation is observed in the simulation. We reach the conclusion that the experiments completed to date have not yet reached the regime of absolute instability.
Original language | English (US) |
---|---|
Pages (from-to) | 998-1003 |
Number of pages | 6 |
Journal | Astrophysical Journal |
Volume | 692 |
Issue number | 2 |
DOIs | |
State | Published - Feb 20 2009 |
Keywords
- Accretion, accretion disks
- Instabilities
- MHD
- Methods: numerical
ASJC Scopus subject areas
- Astronomy and Astrophysics
- Space and Planetary Science