The Evaluation of Energy Storage Mechanisms in the Gradual Phase of Solar Flares

Author(s):  
H. A. Garcia
1987 ◽  
Vol 317 ◽  
pp. 956 ◽  
Author(s):  
B. Schmieder ◽  
T. G. Forbes ◽  
J. M. Malherbe ◽  
M. E. Machado

1986 ◽  
Vol 6 (6) ◽  
pp. 257-266
Author(s):  
Keith T. Strong
Keyword(s):  

Solar Physics ◽  
1989 ◽  
Vol 121 (1-2) ◽  
pp. 399-417 ◽  
Author(s):  
Zdeněk Švestka
Keyword(s):  

2001 ◽  
Vol 552 (2) ◽  
pp. 821-832 ◽  
Author(s):  
Nariaki V. Nitta ◽  
Jun Sato ◽  
Hugh S. Hudson

1980 ◽  
Vol 91 ◽  
pp. 231-234 ◽  
Author(s):  
K. Tanaka ◽  
Z. Smith ◽  
M. Dryer

The flare energy is generally considered to be stored in stressed (twisted or sheared) magnetic fields. Origin of the stress may be either intrinsic or due to horizontal shear motion (Tanaka and Nakagawa 1973) or due to propagation of twist from below (Piddington 1974). Characteristic magnetic configurations in the great activities (inverted, twisted δ-configuration; Zirin and Tanaka 1973) suggest an inherent shape of fluxtube for these regions: a twisted magnetic knot. Further, evolutionary characteristics such as rapid growths of spots and growth of twist in parallel with apparent shear motion of spot, together with the fact that the shear motion is associated with upward velocity (Tanaka and LaBonte 1979), suggest a continuous emergence of such a twisted knot from below throughout the activity (Tanaka 1979). In this model (Fig. 1) the flare energy may be supplied directly into the corona as the twisted portion of the fluxtube emerges out. The amount of energy supplied between t0 and t may be equated to the energy contained in the twist (ɸ) between z1 and z2,


1985 ◽  
Vol 107 ◽  
pp. 293-298
Author(s):  
P. A. Sturrock ◽  
P. Kaufmann ◽  
D. F. Smith

In early research on solar flares, attention was focused on the impulsíve or flash phase, and it was assumed implicitly that virtually all the energy of a flare is released during that short phase. In recent years, however, it has been realized that the long-lived soft X-ray emission which follows the impulsive phase may require a separate energy-release process, which has been termed the “gradual phase” (Kane 1974). The fact that the impulsive phase is often preceded by soft X-ray emission has also led to the suggestion that there may be a third phase of energy release, which might be termed the “onset phase” (Sturrock 1980). It has long been realized that filament eruptions frequently precede flares, and it has been suggested (Kiepenheuer 1964) that the two should be regarded as parts of the same process. For these and other reasons, it is appropriate to question how many phases of energy release are involved in flares and what are their characteristics.


Sign in / Sign up

Export Citation Format

Share Document