Scribner, Bourdon F.
Chief, National Bureau of Standards, Washington, D. C.,
Pages: 10 Published: Jan 1948
The light source in spectrographic analysis serves a two-fold function, first, as a means of vaporizing and dissociating the sample and, second, of exciting the atoms to radiate their characteristic spectra. Both factors are important to the development of the intensities of spectral lines; consequently a discussion of excitation in spectrographic analysis will necessarily involve the consideration of sample forms and physical states as well as the processes occurring in excitation itself. When it is considered that the material to be analyzed may be in the form of a gas, a liquid, or a solid, that it may be a conductor or nonconductor of electricity, and that the concentrations of atoms are to be measured over wide ranges, it is apparent that a variety of factors are involved in the general problem of excitation. Various light sources employing electrical discharges or gas flames have been devised to meet the needs of spectrographic analysis. However, it has become evident that the future development of spectrographic analysis will depend largely on improvements in present excitation sources or even in the application of radically different means of excitation. The sources in practical use are well described in standard texts on the subject or in the general literature. A recent review by Convey (1) provides a detailed treatment of the usual light sources and their applications in analysis. The following discussion outlines briefly certain of the problems that are involved in excitation and indicates lines of investigation that are being followed toward their solution. Quantitative spectrographic analysis is based on the observation that the intensities of spectral lines of elements excited in a light source vary in proportion to the concentrations of the elements present. For light sources in which excitation is mainly thermal, the intensity of a spectral line radiated by the excited atoms in the column of hot gas may be described (2) by the expression:
Paper ID: STP47898S