The atom and the Bohr theory of its structure : $b an elementary presentationHolst, Helge
Science
The atom and the Bohr theory of its structure : $b an elementary presentation
Holst, Helge
Atomic theory
The work of Kirchhoff and Bunsen put at the disposal of science
became a new tool of incalculable scope. First and foremost, spectrum
examinations were taken into the service of chemistry as _spectrum
analysis_. It has thus become possible to analyse quantities of
matter so small that the general methods of chemistry would be quite
powerless to detect them. It is also possible by spectrum analysis
to detect minute traces of an element; several elements were in this
way first discovered by the spectroscope. Moreover, chemical analysis
has been extended to the study of the sun and stars. The spectral
lines have given us answers to many problems of physics—problems which
formerly seemed insoluble. Last but not least spectrum analysis has
given us a key to the deepest secrets of the atom, a key which Niels
Bohr has taught us how to use.
In the discussion of the spectrum we have hitherto restricted ourselves
to the visible spectrum limited on the one side by red and on the other
by violet. But these boundaries are in reality fortuitous, determined
by the human eye. The spectrum can be studied by other methods than
those of direct observation. The more indirect methods include the
effect of the rays on photographic plates and their heating effect on
fine conducting wires for electricity, held in various parts of the
spectrum. It has thus been discovered that beyond the visible violet
end of the spectrum there is an _ultra-violet_ region with strong
photographic activity and an _infra-red_ region producing marked
heat effects. There are both dark and light spectral lines in these
new parts of the spectrum. The fact that glass is not transparent to
ultra-violet or infra-red rays has been an obstacle in the experiments,
but the difficulty can be overcome by using other substances, such as
quartz or rock salt, for the prisms and lenses, or by substituting
concave gratings. By special means it has been possible to detect rays
with wave-lengths as great as 300 μ and as small as about 0·02 μ,
corresponding to frequencies between 10¹², and 15 × 10¹⁵ vibrations per
second, while the wave-lengths of the luminous rays lie between 0·8 and
0·4 μ. The term “light wave” is often used to refer to the ultra-violet
and infra-red rays which can be shown in the spectra produced by prisms
or gratings.
[Illustration: FIG. 11.—Photographic effect of X-rays, which
are passed through the atom grating in a magnesia crystal.]
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