On Proton and Electron Acceleration by Shock Waves during Large Solar Flares

1978 ◽  
Vol 3 (3) ◽  
pp. 236-238
Author(s):  
V. M. Gubchenko ◽  
V. V. Zaitsev

Lin and Hudson (1976) have recently analysed non-thermal processes in proton flares, using observations of a series of major events in August 1972. They concluded that the 10–100 keV electrons accelerated during the flash phase account for the bulk of the total energy of a large proton flare (about 1032 – 1033 ergs); that most protons are accelerated later than the 10 — 100 keV electrons; and that most energetic protons escape to the interplanetary medium. Their conclusions with regard to proton acceleration are supported firstly by the delay of the maximum of γ-ray emission by 3-5 minutes after the maximum of X-ray emission, and secondly by the satisfactory agreement between the 7-ray spectrum and the thin-target model of emission. The energetic protons contain a very small fraction of the total flare energy (of the order of 10-5).

1975 ◽  
Vol 68 ◽  
pp. 425-426
Author(s):  
H. S. Hudson ◽  
T. W. Jones ◽  
R. P. Lin

SummaryIn many small solar flares the ∼10–100 keV electrons accelerated during the flash phase contain the bulk of the total flare energy output. In large flares, such as those in the period 1972, August 2–7, the flash phase electrons are present in substantially greater numbers. These electrons can explosively heat the chromosphere-lower corona and eject flare material. The ejected matter can produce a shock wave which will then accelerate nucleons and electrons to relativistic energies. We analyze energetic particle, radio, X-ray, gamma ray and interplanetary shock observations of the 1972 August flares to obtain quantitative estimates of the energy contained in each facet of these large flares. In general these observations are consistent with the above hypothesis. In particular: (1)From the X-ray emission (van Beek et al., 1973) the energy contained in >25 keV electrons is calculated to be 2 × 1032 erg for the 1972, August 4 event. Since the lower energy cutoff to the electron spectrum is known to be below 25 keV and possibly below 10 keV, the electrons contain enough energy to produce the following interplanetary shock wave, which has by far the bulk of the energy dissipated in the flare. Similar numbers are obtained for the large August 7 flare event.(2)From the γ-ray emission (Chupp et al., 1973) the energy in protons dumped at the same level of the atmosphere, assuming a thick target situation, is at least a factor of three smaller than the electrons. Moreover the γ-ray emission indicates that the bulk of the protons are accelerated at least several minutes after the electrons. Thus it is more likely that the electrons are responsible for the flare optical (Hα and white light) emissions which occur in the chromosphere.(3)Approximately 5% of the electrons and 99% of the protons escape into the interplanetary medium to be observed by spacecraft. This situation is consistent with the hypothesis of shock acceleration of the protons high in the solar corona.(4)The four most intense X-ray bursts observed during the period July 31–August 11 are the only bursts followed by an interplanetary shock wave and a new injection of energetic protons into the interplanetary medium.


Solar Physics ◽  
1989 ◽  
Vol 119 (1) ◽  
pp. 125-142 ◽  
Author(s):  
Neru Nazir ◽  
Ranjna Bakaya ◽  
R. R. Rausaria ◽  
P. K. Koul ◽  
P. N. Khosa
Keyword(s):  

1994 ◽  
Vol 144 ◽  
pp. 267-270 ◽  
Author(s):  
Z. K. Smith ◽  
M. Dryer ◽  
M. Armstrong

AbstractSolar flares are a source of impulsive energy releases on the Sun that can inject energy into the interplanetary medium. Some of these energy injections drive interplanetary shocks that can, in turn cause disturbances in Earth’s environment. In an attempt to quantify these energy releases using readily available observational data, we explore the possibility of using, as a proxy, the solar flare signatures observed in soft X-ray data. Our motivation has been prompted by the real-time operational requirements of NOAA and U. S. Air Force to provide estimates of arrival times and strengths of shocks that impact Earth’s magnetosphere. The luxury of extensive,ex post factostudies of flare total energy outputs is not possible in an operational context. This study is restricted to flares associated with shocks seen in the corona as metric type II radio bursts. Using GOES data, the energy released in the 1-8Å X-ray wavelength band is computed and then compared to the estimates made from a numerical model based on two-dimensional, time-dependent MHD modeling of flare-initiated interplanetary shocks. We find that the proxy energy estimates computed from the GOES data provideno advantageover the estimates made using the MHD-based numerical model.


1975 ◽  
Vol 68 ◽  
pp. 385-409 ◽  
Author(s):  
R. P. Lin

Because ∼5–100 keV electrons are frequently accelerated and emitted by the Sun in small flares, it is possible to define a detailed characteristic physical picture of these events. This review summarizes both the direct spacecraft observations of non-relativistic solar electrons, and observations of the X-ray and radio emission generated by these particles at the Sun and in the interplanetary medium. These observations bear on the basic astrophysical process of particle acceleration in tenuous plasmas. We find that in many small solar flares the ∼5–100 keV electrons accelerated during flash phase constitute the bulk of the total flare energy. Thus the basic flare mechanism in these flares essentially converts the available flare energy into fast electrons. These electrons may produce the other flare electromagnetic emissions through their interactions with the solar atmosphere. In large proton flares these electrons may provide the energy to eject material from the Sun and to create a shock wave which could then accelerate nuclei and electrons to much higher energies.


2003 ◽  
Vol 32 (12) ◽  
pp. 2483-2488
Author(s):  
C GOFF ◽  
S MATTHEWS ◽  
L HARRA
Keyword(s):  

Sign in / Sign up

Export Citation Format

Share Document