Stellar atmospheres : $b A contribution to the observational study of high temperature in the reversing layers of starsPayne-Gaposchkin, Cecilia
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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.)
The homogeneity of the spectra in a given class is striking, and the
fact that large numbers of stars display exactly similar spectra
has a significance—considered in another chapter[504]—to which
the classification problem cannot do more than call attention. The
similarity of the spectra becomes the more striking when it is
remembered that the range of conditions embraced within any one
class is very wide; the ratio in mean density may be as great as
10[505] between stars of the same class but of differing absolute
magnitude.[506]
[Pg 194]
The close spectral similarity between, giants and dwarfs, in spite of
the great differences in physical conditions, should not, however, be
misinterpreted. The observed facts are in exact accordance with what
might have been anticipated. In the first place, thermal ionization
is governed by the surface gravity, and only indirectly by the mean
density.[507]
TABLE XXX
Class
Characteristic Lines
O
H
He
Si+++
C++
N++
He+
H
He
Si+++
He+
O+
H
He
Si+++
O+*
H
He*
H
He
H
He
Si+
Ca+
H
He
Si+
Ca+
Mg+
H
He
Si+
Ca+
Mg+
H*
Si+*
Ca+
Mg+
H
Ca+
Mg+*
Ca
Fe
H
Ca+
Mg+
Ca
Fe
H
Ca+
Ca
Fe
Ti
H
Ca+
Ca
Fe
Ti
H
Ca+
Ca
Fe
Ti
G bd.
H
Ca+
Ca
Fe
Ti
G bd.
H
Ca+
Ca
Fe
Ti
G bd.
H
Ca+*
Ca
Fe*
Ti*
G bd.*
H
Ca+
Ca*
Fe
Ti
TiO₂
H
Ca+
Ca
Fe
Ti
TiO₂
H
Ca+
Ca
Fe
Ti
TiO₂
The division into “arc,” “spark,” and “superspark” is clearly shown
by the table. Maxima of the lines which are used as criteria of class
are marked with an asterisk.
[Pg 195]
It is shown in Chapter III that the range in surface gravity is
far smaller than the range in mean density. Secondly, the basis
of the classification has been shown to be the degree of thermal
ionization.[508] Granted that the value of the partial electron
pressure is low enough, in dwarfs as well as in giants, for thermal
ionization to predominate over ionization by collision, a mass of gas
will pass through the same succession of ionization-stages with
changing temperature, whatever the surface gravity. Any given stage of
ionization will, however, be reached at a lower temperature, the lower
the pressure, since, as pointed out in Chapter X,[509] lowered pressure
tends to increase the degree of ionization, and will help to produce a
given degree of ionization at a lower temperature.
Public-domain text, read in full here on John Shaqi.
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