magnetic flux rope
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2021 ◽  
Vol 923 (1) ◽  
pp. L10
Author(s):  
Changxue Chen ◽  
Yang Su ◽  
Jianchao Xue ◽  
Weiqun Gan ◽  
Yu Huang

Abstract Prominence bubbles and plumes often form near the lower prominence–corona boundary. They are believed to play an important role in mass supply and evolution of solar prominences. However, how they form is still an open question. In this Letter we present a unique high-resolution Hα observation of a quiescent prominence by the New Vacuum Solar Telescope. Two noteworthy bubble–plume events are studied in detail. The two events are almost identical, except that an erupting mini filament appeared below the prominence–bubble interface in the second event, unlike the first one or any of the reported bubble observations. Analysis of the Hα and extreme-ultraviolet data indicates that the rising magnetic flux rope (MFR) in the mini filament is the cause of bubble expansion and that the interaction between the prominence and MFR results in plume formation. These observations provided clear evidence that emerging MFR may be a common trigger of bubbles and suggested a new mechanism of plumes in addition to Rayleigh–Taylor instability and reconnection.


2021 ◽  
Vol 9 ◽  
Author(s):  
Kyunghwan Dokgo ◽  
Kyoung-Joo Hwang ◽  
James L. Burch ◽  
Peter H. Yoon

Understanding the nature and characteristics of high-frequency waves inside a flux rope may be important as the wave-particle interaction is important for charged-particle energization and the ensuing dissipation process. We analyze waves generated by an electron beam in a crater-shaped magnetic flux rope observed by MMS spacecraft on the dawnside tailward magnetopause. In this MMS observation, a depression of magnetic field, or a crater, of ∼100 km is located at the center of the magnetic flux rope of ∼650 km. There exist parallel and perpendicular electrostatic wave modes inside the depression of the magnetic field at the center of the flux rope, and they are distinguished by their locations and frequencies. The parallel mode exists at the center of the magnetic depression and its power spectrum peaks below Fce (electron cyclotron frequency). In contrast, the perpendicular mode exists in the outer region associated with the magnetic depression, and its power spectrum peaks near Fce. The linear analysis of kinetic instability using a generalized dispersion solver shows that the parallel mode can be generated by the electron beam of 5,000 km/s. They can thermalize electrons ≲100 eV effectively. However, the generation mechanism of the perpendicular mode is not clear yet, which requires further study.


2021 ◽  
Author(s):  
Andris Vaivads ◽  
Yuri V. Khotyaintsev ◽  
Alessandro Retino ◽  
Elena A. Kronberg ◽  
Patrick W. Daly ◽  
...  

2021 ◽  
Vol 12 (1) ◽  
Author(s):  
Ze Zhong ◽  
Yang Guo ◽  
M. D. Ding

AbstractWhether a solar eruption is successful or failed depends on the competition between different components of the Lorentz force exerting on the flux rope that drives the eruption. The present models only consider the strapping force generated by the background magnetic field perpendicular to the flux rope and the tension force generated by the field along the flux rope. Using the observed magnetic field on the photosphere as a time-matching bottom boundary, we perform a data-driven magnetohydrodynamic simulation for the 30 January 2015 confined eruption and successfully reproduce the observed solar flare without a coronal mass ejection. Here we show a Lorentz force component, resulting from the radial magnetic field or the non-axisymmetry of the flux rope, which can essentially constrain the eruption. Our finding contributes to the solar eruption model and presents the necessity of considering the topological structure of a flux rope when studying its eruption behaviour.


2021 ◽  
Author(s):  
Charles Bowers ◽  
James A. Slavin ◽  
Gina A. DiBraccio ◽  
Gangkai Poh ◽  
Takuya Hara ◽  
...  

Author(s):  
S. Pal ◽  
E. Kilpua ◽  
S. Good ◽  
J. Pomoell ◽  
D. Price

2021 ◽  
Vol 48 (7) ◽  
Author(s):  
Z. Z. Chen ◽  
H. S. Fu ◽  
Z. Wang ◽  
Z. Z. Guo ◽  
Y. Xu ◽  
...  

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