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.)
+1.50
5.3
1.8
8.89
2.8
1.2
8,600
+2.20
1.9
1.9
2.31
7,000
+2.5
1.6
1.8
5.48
}680
+2.9
1.2
1.4
3.37
6,080
+3.5
1.3
1.0
5.98
+4.2
4.28
}7600
5,460
+4.5
-1.5
4.78
4,820
+4.8
+0.6
8.98
4,240
+6.20
+1.05
19.65
}160 (giant)
6.85
3,600
+7.20
+0.50
4.80
}22 (giant)
3,380
+ 10.20
+0.40
2.10
Excitation and ionization conditions differ so widely for different
atoms that it would be expected that two factors, one of which
encourages ionization, while the other discourages recombination, would
not in every case balance exactly, even when their mean effect was
constant, as it is for any one Draper class.
The Henry Draper Catalogue, as we have emphasized, was made on the
basis of the general resemblance of the spectra, an arrangement which
corresponds to the greatest physical homogeneity that can be obtained.
As regards features of their spectra, it is therefore to be expected
that the members of any one class will correspond closely, and care
[Pg 198]
must be exercised in eliminating redundancies from discussions of the
homogeneity of the individual classes.
There are, however, other types of discussion, independent of
spectroscopic data, and such investigations have shown that the Draper
classes have indeed a significance far beyond the mere formation
of homogeneous groups of spectra. In illustration of the profound
statistical significance of the classification, the table on page 197
of the present chapter contains a brief synopsis of some of the
most salient features that have been correlated with spectral class.
Successive columns contain the class, the effective temperature,[513]
the mean absolute magnitude,[514] the galactic concentration,[515] the
percentage of the class in the Draper catalogue,[516] and the computed
number per million cubic parsecs.[517]
FOOTNOTES:
[497]
H. A., 91-99.
[498]
Rep. I. A. U., Rome, 1922.
[499]
H. A., 28, 131, 1901.
[500]
Observatory, 38, 381, 1915.
[501]
Mt. W. Contr. 199, 1918.
[502]
Harper and Young, J. R. A. S. Can., 18, 9, 1924.
[503]
Observatory, 38, 381, 1915.
[504]
Chapter XIII, p. 178.
[505]
Observatory, 38, 381, 1915.
[506]
Chapter III, p. 36.
[507]
Chapter III, p. 35.
[508]
See above, p. 193.
[509]
P. 141.
[510]
M. N. R. A. S., 83, 403, 1923.
[511]
Chapter II, p. 31.
[512]
Adams and Joy; Mt. W. Contr. 142, 1917.
[513]
A. N., 219, 361, 1923.
[514]
Lundmark, Pub. A. S. P., 34, 147, 1922.
[515]
Shapley, H. B. 796, 1924.
[516]
Shapley and Cannon, Proc. Am. Ac. Sci., 59, 217, 1924.
[517]
Shapley and Cannon, ibid., 59, 230,1924.
[Pg 199]
CHAPTER XV
ON THE FUTURE OF THE PROBLEM
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