scholarly journals Slow-Drift Solar Radio Bursts: Harmonic Frequency Ratios, Frequency Drift Rates, and Solar Longitude Variation.

1960 ◽  
Vol 65 ◽  
pp. 503
Author(s):  
Marion B. Wood
1961 ◽  
Vol 14 (2) ◽  
pp. 234 ◽  
Author(s):  
Marion B Wood

Frequency ratios of second harmonic to fundamental bands are determined for 19 slow drift bursts. The ratios measured at the high frequency edges of the bands yield a mean value of 2� 00, whereas the mean value of the low frequency edge ratios is significantly lower than 2.


Nature ◽  
1959 ◽  
Vol 184 (4697) ◽  
pp. 1471-1472
Author(s):  
M. B. WOOD ◽  
C. S. WARWICK

1963 ◽  
Vol 68 (5) ◽  
pp. 1347-1354 ◽  
Author(s):  
A. Maxwell ◽  
M. P. Hughes ◽  
A. R. Thompson

1966 ◽  
Vol 19 (5) ◽  
pp. 635 ◽  

This paper reports statistical investigations of "chains" of type I bursts recorded with the Dapto radio spectrograph. Various characteristics of chains have been investigated, including their distribution with mid frequency, rate of frequency drift, posi


1965 ◽  
Vol 18 (2) ◽  
pp. 167 ◽  
Author(s):  
The Late AA Weiss

Velocities of the sources of type II bursts are derived from rates of frequency drift using standard density models, both statistically for 21 bursts, and individually for 5 bursts extending over wide frequency ranges. The derived velocities exceed the speed of sound in the magnetic-field.free corona: on the average the velocity decreases with increasing height to a minimum of ,....., 750 kmjs at a little below I Ro' and j,hereafter slowly increases with height. The nature of the type II source is discussed in relation to these velocities, and also in relation to detailed measurements of harmonic ratios and band splitting for the five individual bursts. It is suggested that the type II source is either a strong parallel shock (direction of propagation of shock parallel to magnetic field) or a perpendicular shock. Magnetic field strengths of 2-20 G at 0�5 R 0 above the photosphere, decreasing to 1-10 G at 2 Ro, are derived. Finally, it is shown that theories by which fundamental emission arises in front of the shock, whilst harmonic emission originates in the interior of the shock, are untenable.


1994 ◽  
Vol 144 ◽  
pp. 283-284
Author(s):  
G. Maris ◽  
E. Tifrea

The type II solar radio bursts produced by a shock wave passing through the solar corona are one of the most frequently studied solar activity phenomena. The scientific interest in this type of phenomenon is due to the fact that the presence of this radio event in a solar flare is an almost certain indicator of a future geophysical effect. The origin of the shock waves which produce these bursts is not at all simple; besides the shocks which are generated as a result of a strong energy release during the impulsive phase of a flare, there are also the shocks generated by a coronal mass ejection or the shocks which appear in the interplanetary space due to the supplementary acceleration of the solar particles.


GPS Solutions ◽  
2021 ◽  
Vol 25 (2) ◽  
Author(s):  
Yu. V. Yasyukevich ◽  
A. S. Yasyukevich ◽  
E. I. Astafyeva

Solar Physics ◽  
2021 ◽  
Vol 296 (2) ◽  
Author(s):  
Maoshui Lv ◽  
Yao Chen ◽  
V. Vasanth ◽  
Mohd Shazwan Radzi ◽  
Zamri Zainal Abidin ◽  
...  

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