Propagation of velocity waves are investigated in the solar chromosphere, with a special view to high frequencies (periods --->60 s). Four line profiles have been observed during 27 mn with the Sacramento Peak vacuum telescope (Ha, 3933, 8498 and 8542 Can). Three Fourier analysis are performed accor
Mass motion in the solar chromosphere
โ Scribed by R. A. Jones; W. A. Rense
- Publisher
- Springer
- Year
- 1970
- Tongue
- English
- Weight
- 235 KB
- Volume
- 15
- Category
- Article
- ISSN
- 0038-0938
No coin nor oath required. For personal study only.
โฆ Synopsis
A high resolution profile of the solar OI 1304.9 A line has been measured from rocket spectrograms. The profile is nearly flat-topped, showing only a slight solar reversal after instrument effects and absorption due to atomic oxygen in the earth's atmosphere have been allowed for. A theoretical analysis of this line, under the assumption of non-LTE conditions and a homogeneous, spherically symmetric chromosphere, predicts a rather deep solar reversal. The theoretical profile may be made consistent with the observed profile if mass motion is present in the chromospheric region where the line is formed. A Gaussian distribution of up and down velocities with a root mean square velocity of about 7 km/sec gives best agreement between the predicted and observed profile. This result is consistent with the conclusion made from a study of high resolution profiles of solar lines in the visible spectrum that mass vertical velocities increase with height above the photosphere.
๐ SIMILAR VOLUMES
Extreme ultraviolet spectroheliograms in Mg x (625 ~) and the Lyman continuum (897/~) obtained from OSO-6 are used to determine the differential rotation rate in the solar chromosphere and corona. The equatorial rotation rate agrees with spectroscopic measurements of the photospheric plasma velocity
In order to precise previous results about wave propagation in the quiet chromosphere (N. Mein and P. Mein, 1976), we study the behaviour of Doppler shifts and intensity fluctuations in 3 lines of Ca II. We use the same observation as in our previous work, that is to say a sequence of spectra lasti