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K emission-line widths and the solar chromosphere
Authors:M. K. V. Bappu  K. R. Sivaraman
Affiliation:(1) Astrophysical Observatory, Kodaikanal, India
Abstract:Closely spaced microphotometer tracings parallel to the dispersion of one excellent frame of a K-line time sequence have been utilized for a study of the nature of the K2v, K2R intensities in the case of the solar chromosphere. The frequency of occurrence of the categories of intensity ratio 
$${rm I}_{{text{K}}_{{text{2}}V} } /{rm I}_{{text{K}}_{{text{2}}R} }$$
are as follows: 
$${rm I}_{{text{K}}_{{text{2}}V} }  > {rm I}_{{text{K}}_{{text{2}}R} }  = 45.3$$
per cent; 
$${rm I}_{{text{K}}_{{text{2}}V} }  = {rm I}_{{text{K}}_{{text{2}}R} }  = 4.7$$
per cent; 
$${rm I}_{{text{K}}_{{text{2}}V} }  < {rm I}_{{text{K}}_{{text{2}}R} }  = 25$$
per cent; 
$${rm I}_{{text{K}}_{{text{2}}R} }  = 0 = 22.3$$
per cent; 
$${rm I}_{{text{K}}_{{text{2}}V} }  = 0 = 0.7$$
per cent. Two types of absorbing components are postulated to explain the pattern of observed K2v, k2R intensity ratios. One component with minor Doppler displacements acting on the normal K232 profile, where K2V >K2R, produces the cases K2v Gt K2R, K2v = K2R, K2v 2R. The other component arises from lsquodark condensationsrsquo which are of size 3500 kms as seen in K2R. They have principally large down flowing velocities in the range 5–8 km/sec and are seen on K3 spectroheliograms with sizes of about 5000 kms, within the coarse network of emission. These lsquodark condensationsrsquo give rise to the situation K2R = 0.K2-line widths are measured for all tracings where K2v, K2R are measurable simultaneously. The distribution curve of these widths is extremely sharp. The K2 emission source is identified with the bright fine mottles visible on the surface. Evidence for this interpretation comes from the study of auto-correlation functions of K2 intensity variations and the spacing between the bright fine mottles from both spectrograms and spectroheliograms. The life time of the fine mottling is 200 sec.The supergranular boundaries which constitute the coarse network come in two intensity classes. A low intensity network has the fine mottles as its principal contributor to the K emission. When the network is bright, the enhancement is caused by increased K emission due to the accumulation of magnetic fields at the supergranule boundary. The K2 widths of the low intensity supergranular boundary agree with the value found for the bright mottles. Those for the brighter network are lower than this value, similar to the K2 widths as seen in the active regions.It is concluded that bright fine mottling is responsible for the relation, found by Wilson and Bappu, between K emission line widths and absolute magnitudes of the stars.The paper discusses the solar cycle equivalents that stellar chromospheres can demonstrate and indicates a possible line of approach for successful detection of cyclic activity in stellar chromospheres.
Keywords:
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