Abstract
The theory of thermal ionization of gases was first given by M. N. Saha in a series of papers (1920
a
, 1920
b
, 1921) and widely applied by him and others to furnish a satisfactory physical theory of stellar spectra. The theory was further developed by Fowler (1923) to include the different excited states of the atom and of the ionized atom, all of which are simultaneously in thermodynamical equilibrium. At the time when the theory was first formulated the ionization potentials and the spectral characteristics of only a few elements were known, but now we possess almost a complete knowledge of the ionization potentials and the spectra of almost all the elements in their different stages of ionization. Hence a detailed comparison of the theory with experimental results can now be satisfactorily undertaken.
Reference14 articles.
1. Bacher R. F. and Goudsmit S. 1932 Atomic energy states 1st ed. New York and London: McGraw-Hill Book Co.
2. Proc. Roy;Dewar J.;Soc. A,1913
3. I. Dissociation-equilibria by the method of partitions
4. Hartmann H. and Schneider R. 1929
5. Kelley K. K. 1935 Bull. U.S. Bur. Mines no. 383.
Cited by
4 articles.
订阅此论文施引文献
订阅此论文施引文献,注册后可以免费订阅5篇论文的施引文献,订阅后可以查看论文全部施引文献
1. Molecular Systems at Low Densities;Statistical Mechanics, Kinetic Theory, and Stochastic Processes;1972
2. Oпpeдeлehиe cил ocцилляtopob b cпeкtpax atomob;Journal of Quantitative Spectroscopy and Radiative Transfer;1964-01
3. The thermionic constants of metals and semi-conductors I. Graphite;Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences;1952-06-24
4. Studies on the ionization produced by metallic salt in flames - III. Ionic equilibria in hydrogen/air flames containing alkali metal salts;Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences;1952-02-07