Abstract

Context. Coronal rain are cool dense blobs that form in solar coronal loops and are a manifestation of catastrophic cooling linked to thermal instability. Once formed, rain falls towards the solar surface at sub-ballistic speeds, which is not well-understood. Pressure forces seem to be the prime candidate to explain this. In many observations rain is accompanied by transverse oscillations and the interaction between the two needs to be explored. Aims. Therefore, an alternative kinematic model for coronal rain kinematics in transversely oscillating loops is developed to understand the physical nature of the observed sub-ballistic falling motion of rain. It explicitly explores the role of the ponderomotive force arising from the transverse oscillation on the rain motion as well as the capacity of rain to excite wave motion. Methods. An analytical model is presented that describes a rain blob guided by the coronal magnetic field supporting a onedimensional shear Alfven wave as a point mass on an oscillating string. The model includes gravity and the ponderomotive force from the oscillation acting on the mass, as well as the inertia of the mass acting on the oscillation. Results. The kinematics of rain in the limit of negligible rain mass are explored and falling and trapped regimes are found, depending on wave amplitude. In the trapped regime for the fundamental mode, the rain blob bounces back and forth around the loop top at a long period inversely proportional to the oscillation amplitude. The model is compared with several observational rain studies, including one in-depth comparison with an observation that shows rain with up-and down bobbing motion. The role of rain inertia in exciting transverse oscillations is explored in inclined loops. Conclusions. It is found that the model requires displacement amplitudes of the transverse oscillation that are typically an order of magnitude larger than observed to explain the measured sub-ballistic motion of the rain. Therefore, it is concluded that the ponderomotive force is not the primary reason for understanding sub-ballistic motion, but it plays a role in cases of large loop oscillations. The appearance of rain causes the excitation of small-amplitude transverse oscillations that may explain observed events and provide a seismological tool to measure rain mass.

Highlights

  • Coronal rain are cool dense blobs that form in warm active region loops and fall along the guiding magnetic field to the solar surface (Kawaguchi 1970; Leroy 1972; Athay et al 1980; Schrijver 2001; De Groof et al 2004; de Groof et al 2005; Vashalomidze et al 2015)

  • We have studied the kinematics of coronal rain in the presence of a transversely oscillating loop using an analytical model of a rain blob guided by the coronal magnetic field as the mechanical analogue of a moving point mass on an oscillating string with gravity

  • If the oscillation is damped, this motion is temporary and as soon as the amplitude goes below the critical amplitude, the rain eventually falls towards the surface

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Summary

Introduction

Coronal rain are cool dense blobs that form in warm active region loops and fall along the guiding magnetic field to the solar surface (Kawaguchi 1970; Leroy 1972; Athay et al 1980; Schrijver 2001; De Groof et al 2004; de Groof et al 2005; Vashalomidze et al 2015) They are traditionally observed in chromospheric lines, such as H-α or Ca II H, as well as in transition region lines. Antolin & Verwichte (2011) presented an observational study with Hinode/SOT in In Ca II H in which multiple coronal rain blobs are seen to oscillate transversely in phase.

Mechanical model
Coronal rain kinematics in presence of transverse oscillation
R 44 R
Modelling of observations of coronal rain oscillations
Excitation of transverse loop oscillations by coronal rain
16 April 2012 A11 Short-period K16 Long-period K16
Findings
Discussion
Full Text
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