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 method applied by Saha to stellar atmospheres was borrowed
from physical chemistry. The Law of Mass Action, and the theory of
ionization in solutions which is based upon it, have in general been
very well satisfied in dilute solution.[387] The ionization considered
[Pg 111]
by chemical theory is the separation of a molecule in solution
into charged radicals. The essential point is the acquisition of a
charge at dissociation, and this is the only feature that the chemical
ionization has in common with the thermal ionization, where the
atom is separated into a positively charged ion and an electron
which constitutes the negative charge.
The step from the theory first formulated for solutions to the theory
of gaseous ionization is a long one, and its legitimacy has been
questioned.[388] It appears, however, that the step is justified.[389]
The stellar conditions are certainly simpler than those in a
solution, and if the requisite dilution obtains, the law may be
expected to hold with considerable closeness. Saha contemplated
pressures of the order of an atmosphere, and it may be shown that under
such conditions the volume concentration would be too great and the
theory would be invalid. At pressures of
, however, the
effect of concentration is just becoming inappreciable, and the theory
probably holds with fair exactness.
LABORATORY EVIDENCE BEARING ON THE THEORY
(a) Ultimate Lines[390]—The physical tests of the Saha theory
that have been made in the laboratory have all supported it strongly.
The fact that the ultimate lines of an atom are the lines normally
absorbed by the cold vapor has long been familiar. Indeed it is this
fact that is tacitly assumed in the identification of lines of zero
excitation potential in the laboratory with lines which are strongest
in the low-temperature furnace spectrum. De Gramont[391] designated the
ultimate lines “raies de grande sensibilité” for the detection of small
quantities of a substance, because they are the last to disappear from
the flame spectrum when the quantity of the substance is decreased.
[Pg 112]
(b) Temperature Class.—The effect, upon the absorption
spectrum of a substance, of raising the temperature has also long been
recognized as an increase in the strength of lines associated with the
higher excitation potentials. The use of A. S. King’s “temperature
class” in assigning series relations[392] involves a tacit admission
of the validity of the theory of thermal ionization in predicting
the relative numbers of atoms able to absorb light corresponding to
different levels of energy.[393]
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