The Kelvin–Helmholtz instability in weakly ionized plasmas – II. Multifluid effects in molecular clouds
Article first published online: 8 DEC 2011
© 2011 The Authors Monthly Notices of the Royal Astronomical Society © 2011 RAS
Monthly Notices of the Royal Astronomical Society
Volume 420, Issue 1, pages 817–828, February 2012
How to Cite
Jones, A. C. and Downes, T. P. (2012), The Kelvin–Helmholtz instability in weakly ionized plasmas – II. Multifluid effects in molecular clouds. Monthly Notices of the Royal Astronomical Society, 420: 817–828. doi: 10.1111/j.1365-2966.2011.20095.x
- Issue published online: 23 JAN 2012
- Article first published online: 8 DEC 2011
- Accepted 2011 October 28. Received 2011 October 18; in original form 2011 September 8
- ISM: clouds;
- ISM: kinematics and dynamics
We present a study of the Kelvin–Helmholtz instability in a weakly ionized, multifluid magnetohydrodynamic (MHD) plasma with parameters matching those of a typical molecular cloud. The instability is capable of transforming well-ordered flows into disordered flows. As a result, it may be able to convert the energy found in, for example, bowshocks from stellar jets into the turbulent energy found in molecular clouds. As these clouds are weakly ionized, the ideal MHD approximation does not apply at scales of around a tenth of a parsec or less. This paper extends the work of Jones & Downes on the evolution of the Kelvin–Helmholtz instability in the presence of multifluid MHD effects. These effects of ambipolar diffusion and the Hall effect are here studied together under physical parameters applicable to molecular clouds. We restrict our attention to the case of a single shear layer with a transonic, but super-Alfvénic, velocity jump and the computational domain is chosen to match the wavelength of the linearly fastest growing mode of the instability.
We find that while the introduction of multifluid effects does not affect the linear growth rates of the instability, the non-linear behaviour undergoes considerable change. The magnetic field is decoupled from the bulk flow as a result of the ambipolar diffusion, which leads to a significant difference in the evolution of the field. The Hall effect would be expected to lead to a noticeable re-orientation of the magnetic field lines perpendicular to the plane. However, the results reveal that the combination with ambipolar diffusion leads to a surprisingly effective suppression of this effect.