Please use this identifier to cite or link to this item: http://hdl.handle.net/2248/8339
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dc.contributor.authorVemareddy, P-
dc.contributor.authorSyed Ibrahim, M-
dc.date.accessioned2024-01-25T05:50:21Z-
dc.date.available2024-01-25T05:50:21Z-
dc.date.issued2024-01-
dc.identifier.citationMonthly Notices of the Royal Astronomical Society, Vol. 527, No. 2, pp. 1774–1783en_US
dc.identifier.issn0035-8711-
dc.identifier.urihttp://hdl.handle.net/2248/8339-
dc.descriptionOpen Accessen_US
dc.descriptionThis is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted reuse, distribution, and reproduction in any medium, provided the original work is properly cited.-
dc.description.abstractUsing the SDO/AIA, SOHO/LASCO, STEREO/SECCHI, and ground-based H α, radio observations, we studied a prominence eruption (PE) from the western limb that occurred on 2013 December 4. PE is associated with a moderate coronal mass ejection (CME) and GOES class C4.7 flare. Before a couple of days, the prominence pre-existed as an inverse-S shaped filament lying above fragmented opposite polarities between two active regions. Initially, the prominence appears as kinked or writhed as observed from different vantage points. From a careful study of magnetic field observations, we infer that the flux emergence at one leg of the prominence causes the loss of equilibrium which then initiates the slow upward motion of the prominence followed by onset of the eruption at a projected height of 35 Mm. The fast rise motion is also in synchronization with the flare impulsive phase but the average acceleration is quite small (150 ms−2) compared to strong flare cases. In the LASCO field of view (FOV), the CME continues to accelerate at 3 ms−2 attaining a speed of 450 km s−1 at 16 R. In the extended STEREO-A FOV upto 38 R, the CME decelerates 0.82 m s−2. The PE launched type III bursts delayed by 14 min with respect to the flare peak time (04:58 UT). Since the prominence is lying in the fragmented polarities, it is likely that the sheared arcade has little contribution to the poloidal flux of the rising magnetic flux rope and subsequently weak flare is recorded. This study of PE emphasizes the influence of the magnetic reconnection on the CME speed, launch of type II, III burst, and the CME propagation distance farther away from the Sun.en_US
dc.language.isoenen_US
dc.publisherOxford University Press on behalf of Royal Astronomical Societyen_US
dc.relation.urihttps://doi.org/10.1093/mnras/stad3323-
dc.rights© 2023 The Author(s)-
dc.subjectmagnetic fieldsen_US
dc.subjectsolar-terrestrial relationsen_US
dc.subjectCMEsen_US
dc.subjectflaresen_US
dc.subjectminencesen_US
dc.subjectradio burstsen_US
dc.titleEruption of prominence initiated by loss of equilibrium: multipoint observationsen_US
dc.typeArticleen_US
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