Quiescent prominence dynamics observed with the Hinode Solar Optical Telescope . II. Prominence Bubble Boundary Layer Characteristics and the Onset of a Coupled Kelvin-Helmholtz Rayleigh-Taylor Instability [SSA]

http://arxiv.org/abs/1707.05265


We analyze solar quiescent prominence bubble characteristics and instability dynamics using Hinode Solar Optical Telescope (SOT) data. We measure bubble expansion rate, prominence downflows, and the profile of the boundary layer brightness and thickness as a function of time. The largest bubble analyzed rises into the prominence with a speed of about 1.3 km/s until it is destabilized by a localized shear flow on the boundary. Boundary layer thickness grows gradually as prominence downflows deposit plasma onto the bubble with characteristic speeds of 20 to 35 km/s. Lateral downflows initiate from the thickened boundary with characteristic speeds of 25 to 50 km/s, draining the layer of plasma. Strong shear flow across one bubble boundary leads to a coupled Kelvin-Helmholtz Rayleigh-Taylor (KHRT) instability. We measure shear flow speeds above the bubble of 10 km/s and infer interior bubble flow speeds on the order of 100 km/s. Comparing the measured growth rate of the instability to analytic expressions, we infer a magnetic flux density across the bubble boundary of 0.001 T (10 gauss) at an angle of approximately 70 degrees to the prominence plane. The results are consistent with the hypothesis that prominence bubbles are caused by magnetic flux that emerges below a prominence, setting up the conditions for RT, or combined KHRT, instability flows that transport flux, helicity, and hot plasma upward into the overlying coronal magnetic flux rope.

Read this paper on arXiv…

T. Berger, A. Hillier and W. Liu
Tue, 18 Jul 17
65/66

Comments: 15 pages, 7 figures