OBSERVATIONS OF FIVE IONIZATION STAGES OF IRON IN THE SOLAR CORONA
Observations of five ionization stages of iron in the solar corona using the climax coronagraph
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Observations of five ionization stages of iron in the solar corona using the climax coronagraph
Three frequency observation of 1967 Crab Nebula occultation by solar corona
Magnetic potential model of solar corona structure for March 1970 eclipse
Proposed model with with neutrons as energy source for solar corona, discussing validity based on capture gamma ray flux expectation
The oxygen-to-neon abundance ratio in the solar corona is determined to be 4.7 + or - 1.5 on the basis of a relatively model-independent analysis utilizing 25 separate measurements of the O VIII to Ne IX resonance line ratio. The stated uncertainty includes random and possible systematic experimental error in the data but does not include possible error in the calculated flux ratios which have been fitted to the observations. This abundance ratio is smaller than most published results based upon EUV or X-ray observations but is in good agreement with direct measurements of flare cosmic rays.
Use of a satellite photometric observatory (SPO) to measure the solar corona from Miahuatlan, Mexico during the Mar. 7, 1970, total eclipse of the sun. The SPO is equipped with a 24-in. Cassegrainian telescope, a four-channel photoelectric photometer, a Wollaston prism, and a rotating half-wave plate. Simultaneous measurements were made of the two orthogonal components of coronal light in the B and R bands of the UBVRI system. A 1-minute arc aperture was scanned from the lunar disk center out to five solar radii in a series of spirals of gradually increasing radius. For the first time, simultaneous multicolor intensity, degree, and angle of polarization profiles are computed from photoelectric measurements. Comparison of the variations of the measurements for each spiral scan yield a detailed picture of the intensity and polarization features in the K corona.
Solar corona temperature from intensity gradients measured during total eclipse of May 30, 1965
Intensity and polarization of forbidden bands of solar corona spectrum
Intensity ratios effect of forbidden Fe and Ca transitions in solar corona on Fe/Ca ratio, noting cascading configurations
Two-dimensional isophotes of outer solar corona derived from integrated vidicon pictures taken from lunar surface by Surveyors 6 and 7
Linearly polarized CW signal transmission through near solar corona, measuring Faraday rotation
Long term storage of relativistic energetic electrons and protons in solar corona from IMP 4 and Pioneer 8 observations related to delayed emission from flares
Two dimensional isophotes of extreme solar corona from integrated vidicon pictures taken from moon surface by Surveyors 6 and 7
The brightness temperature distribution of the quiet solar corona at a wavelength of 8.9 meters is measured by two types of radio telescope: (1) a 'T' type array with a resolution of 26'X38', and (2) a fan beam interferometer with an E-W resolution of 3'. It is found that the persistent bright regions do not have any angular structure on scales of 6' or less. The daily variations of the brightness temperature of different regions are studied and the possible interpretation discussed.
The possible role of waves in the heating of the solar corona has been investigated. A general dispersion relation has been derived for waves propagating in a homogeneous plasma subject to dissipation by viscosity and thermal conduction. The dissipation mechanisms have been incorporated self-consistently into the equations, and no assumptions about the strength of the damping have been made. Solutions of the sixth-order dispersion relation provide information on how the damping of both slow and fast mode waves depends upon the plasma density, temperature, field strength, and angle of propagation relative to the background magnetic field. We provide a detailed comparison to the standard approach, which is to solve for the wave quantities in the absence of dissipation and then to use these quantities in expressions for the heating due to viscosity and thermal conduction.
A linear model for gyroscopic waves in the base of the solar corona is proposed. The purpose was to point out possible observational manifestations of the phenomenon. According to the model, these waves move slowly around the sun along heliolatitude circles. The fact that the red line corona is fainter on the solar side facing the apex and north-south and east-west asymmetries of the red coronal emission line could be interpreted as a possible observational manifestation of the gyroscopic wave phenomenon in the coronal base.
The white-light coronagraph experiment has made frequent, periodic observations of the solar corona from 1.5 to 6.0 solar radii during the Skylab mission, and these observations will permit the determination of the three-dimensional extent of coronal forms. There are several time scales on which visual changes in coronal structures occur, ranging from approximately one-half rotation to less than hours. A number of events corresponding to the shortest time scale - coronal transients - cause major restructuring of the corona.
Relative line strengths of UV lines of Fe XIV CALCULATED for solar corona