Development of flare morphology in X-rays, and the flare scenario
β Scribed by C. Jager
- Publisher
- Springer
- Year
- 1983
- Tongue
- English
- Weight
- 580 KB
- Volume
- 86
- Category
- Article
- ISSN
- 0038-0938
No coin nor oath required. For personal study only.
β¦ Synopsis
We define the ~p~iUs phgL6s of a flare as its first phase, characterized by: X-ray bursts of short (seconds to tens of seconds) duration, a patchy X-ray morphology, and injection of energy. It lasts some five to ten minutes. The g~d~cg~ or ~s phase starts virtually at the same time as the impulsive one and is characterized by a gradually varying X-ray flux from a larger, diffuse, area situated higher than the sources of the impulsive X-ray bursts. The diffuse cloud is initially (during the first five minutes) hotter by a few million degrees than the sources of the impulsive phase bursts and is assumed to be caused by convective motions with upward velocities of a few hundred km s -I. It contains about the same number of energetic electrons as the impulsive burst patches contained initially. It cools gradually down by radiative and conductive losses, a process that may last for about an hour.
π SIMILAR VOLUMES
aboard the SMM satellite imaged extensive coronal structures after occurrences of two-ribbon flares. The archlike structures extended along the neutral line of the longitudinal magnetic field to altitudes of 1 x 105 to 2 β’ 105 km. The first arch observed by HXIS on 6-7 November appeared after the f
We present observations of another post-flare arch following an eruptive flare, detected in X-ray lines above the western solar limb on 2 May 1985.
Soft X-ray flare data in the wavelength range 2.6-10 A are used to examine the time variation of emission measure and electron temperature. The thermal plasma parameters were derived according to a two-temperature model proposed by Herring and Craig (1973). Estimates of electron density and source v