flare plasma
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2016 ◽  
Vol 16 (12) ◽  
Author(s):  
V Smirnova ◽  
Yu Tcap ◽  
A Shumov ◽  
A Morgachev ◽  
G Motorina ◽  
...  
Keyword(s):  
X Ray ◽  

2013 ◽  
Vol 561 ◽  
pp. A20 ◽  
Author(s):  
B. O’Dwyer ◽  
G. Del Zanna ◽  
H. E. Mason
Keyword(s):  

2013 ◽  
Vol 31 (12) ◽  
pp. 2193-2200 ◽  
Author(s):  
A. Kryshtal ◽  
S. Gerasimenko ◽  
A. Voitsekhovska ◽  
V. Fedun

Abstract. The necessary physical conditions for development of the ion-acoustic instability in the chromospheric part of a flaring loop current circuit are investigated. Two possible scenarios have been studied. First, we consider that pre-flare loop plasma with the large-scale sub-Dreicer electric field has a classical Coulomb conductivity and, second, when anomalous resistance appears due to saturation of Bernstein turbulence. The Fontenla-Avrett-Loeser (FAL) model of the solar atmosphere was used to describe the pre-flare plasma. We have shown that investigated instability can grow and develop either in the presence of the Coulomb conductivity or saturated Bernstein turbulence. We demonstrate that in the case of small-scale instability, the threshold value for the degree of nonisothermality is high and, therefore, cannot be reached by inclusion of the ordinary Joule heating. The ion-acoustic instability can develop at the pre-flare loop footpoints provided the electrons are more than 10 times hotter than the ions there.


Author(s):  
Z. Kordylewski ◽  
J. Sylwester ◽  
B. Sylwester ◽  
A. Kȩpa ◽  
M. Kowaliński ◽  
...  

2013 ◽  
Vol 770 (2) ◽  
pp. 116 ◽  
Author(s):  
Harry P. Warren ◽  
John T. Mariska ◽  
George A. Doschek
Keyword(s):  

2012 ◽  
Vol 8 (S294) ◽  
pp. 541-542
Author(s):  
Arun Kumar Awasthi ◽  
Rajmal Jain

AbstractWe investigate 10 M-class flares observed by the SOXS mission to study the influence of the solar flare plasma cooling on the Neupert effect. We study the temporal evolution of 1s cadence X-ray emission in 7-10 keV and 10-30 keV representing the SXR and HXR emission respectively. We model the cooling as a function of time by the ratio of time-derivative of SXR with the HXR flux. We report that the ratio is exponentially decaying in rise phase of the flare, which, however, saturates after the impulsive phase. We estimate the cooling time scale in the rise phase for the flares and found to be varying between 39 and 525 s.


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