Stellar atmospheres : $b A contribution to the observational study of high temperature in the reversing layers of starsPayne-Gaposchkin, Cecilia
Science
Stellar atmospheres : $b A contribution to the observational study of high temperature in the reversing layers of stars
Payne-Gaposchkin, Cecilia
Astrophysics; Stars -- Spectra; Stars -- Temperature; Thesis (Ph. D.)
Fowler and Milne[477] pointed out that the “marginal appearance,” when
the line is at the limit of visibility, is a function of the abundance
of the corresponding atom. For this reason their own theory, which
dealt not with the marginal appearance but with the maximum of an
absorption line, was capable of a more satisfactory observational test
than Saha’s. It is possible, as shown below, to extend the Fowler-Milne
considerations and to use the observed marginal appearances as a
measure of relative abundance.
The conditions for marginal appearance must first be formulated.
When a strong absorption line is at maximum, the light received from
its center comes from the deepest layer that is possible for the
corresponding frequency. The actual depth depends, as was pointed out
in Chapter IX, upon the number of absorbing atoms per unit volume, and
upon the atomic absorption coefficient for the frequency in question.
The suggestions that were put forward in the chapter just quoted
indicate that different lines, at their maxima, arise from different
“effective levels,” the more abundant atoms appearing, other things
being equal, at higher levels.
As an absorption line is traced through the classes adjacent to the one
at which it attains maximum, it begins to diminish in intensity, owing
to the decrease in the number of suitable atoms. If the line is very
intense, the first effect of the fall in the number of suitable atoms
is a reduction in the width and wings. As the number of suitable atoms
per unit volume decreases further, a greater and greater thickness of
atmosphere is required to produce the same amount of absorption, and
accordingly the line originates deeper and deeper in the atmosphere
of the star. As the “effective level” falls, the temperature of the
[Pg 180]
layer that gives rise to the line increases, owing to the temperature
gradient in the stellar reversing layer. The observed fall in the
intensity of the line is caused both by the reduction in the number of
suitable atoms, and by the decreased contrast between the line and the
background. The former cause predominates for strong (saturated) lines,
and the latter for weak (unsaturated) lines.
Public-domain text, read in full here on John Shaqi.
Reviews
Reviews
No reviews yet
Be the first to share your thoughts on this work.
Elsewhere in the archive
Join the Discussion
Join the discussion
Sign in to leave a comment or review.
Sign InorCreate an account