The observation of a coronal transient directed at earth

1982 ◽  
Vol 263 ◽  
pp. L101 ◽  
Author(s):  
R. A. Howard ◽  
D. J. Michels ◽  
N. R., Jr. Sheeley ◽  
M. J. Koomen
Keyword(s):  
1980 ◽  
Vol 91 ◽  
pp. 317-321 ◽  
Author(s):  
G. W. Pneuman

The association of coronal transients with two-ribbon solar flares is well established. During the Skylab period, every two-ribbon flare when observed close enough to the limb was accompanied by a coronal transient. Flares do not occur with all transients, however many of these transients are associated with soft X-ray enhancements in the corona similar to but less energetic than the intense X-ray loops that occur with two-ribbon flares [cf. MacCombie and Rust (1979) for a review]. The eruption of a filament seems to be the ingredient common to all these events - more so than flares. For these reasons, we consider this class of phenomena, regardless of whether a flare occurs or not, to be exhibiting a common physical process. To produce chromospheric emission requires a substantial amount of energy. Hence, one should expect chromospheric flares to be associated with only the most energetic phenomena. Nevertheless, the most comprehensive observations covering a wide range of wavelengths (Hα, EUV, X-ray, radio, white light) are available for the large two-ribbon flares, and the study of these events sheds the most light on the mechanism which produces coronal transients.


Solar Physics ◽  
1975 ◽  
Vol 45 (2) ◽  
pp. 363-376 ◽  
Author(s):  
E. Hildner ◽  
J. T. Gosling ◽  
R. T. Hansen ◽  
J. D. Bohlin

Solar Physics ◽  
1983 ◽  
Vol 85 (2) ◽  
pp. 351-373 ◽  
Author(s):  
S. T. Wu ◽  
S. Wang ◽  
M. Dryer ◽  
A. I. Poland ◽  
D. G. Sime ◽  
...  

2000 ◽  
Vol 141 (3) ◽  
pp. 357-369 ◽  
Author(s):  
A. Klassen ◽  
H. Aurass ◽  
G. Mann ◽  
B. J. Thompson

1980 ◽  
Vol 91 ◽  
pp. 241-244
Author(s):  
E. J. Schmahl

A classic filament disruption/coronal transient event ocurred on 10 January 1974. After the prominence liftoff, “gradual” x-rays were recorded by Solrad 9. A white light coronal ejection, interpreted as a loop seen edge-on, followed. During the mass outflow, Hα loops formed at the original site of the prominence. The loops appeared also in EUV spectroheliograms, and rose rapidly before vanishing abruptly. During the disintegration of the loops the apices showed great enhancements and vertical spike structures. The overall behavior of this loop prominence system is compatible with reconnection models.


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