The electron, its isolation and measurement and the determination of some of its properties — John Stuart Mill — John Shaqi
The electron, its isolation and measurement and the determination of some of its properties
John Stuart Mill · en
Laue in Munich had suggested in 1912 the use of the regular spacing of
the molecules of a crystal for the analysis, according to the principle
of the grating, of ether waves of very short wave-length, such as
X-rays were supposed to be, and the Braggs[144] had not only perfected
an X-ray spectrometer which utilized this principle, but had determined
accurately the wave-lengths of the X-rays which are characteristic of
certain metals. The accuracy with which this can be done is limited
simply by the accuracy in the determination of , so that the
whole new field of exact X-ray spectrometry is made available through
our exact knowledge of . Moseley’s discovery,[145] made as a
result of an elaborate and difficult study of the wave-lengths of the
characteristic X-rays which were excited when cathode rays were made
to impinge in succession upon anticathodes embracing most of the known
elements, was that these characteristic wave-lengths of the different
elements, or, better, their characteristic frequencies, are related
in a very simple but a very significant way. These frequencies
were found to constitute the same sort of an arithmetical progression
as do the charges which we found to exist on our oil drops. It
was the square root of the frequencies rather than the frequencies
themselves which showed this beautifully simple relationship, but this
is an unimportant detail. The significant fact is that, arranged
in the order of increasing frequency of their characteristic X-ray
[Pg 198]
spectra, all the known elements which have been examined constitute a
simple arithmetical series each member of which is obtained from its
predecessor by adding always the same quantity.
The plate opposite this page shows photographs of the X-ray spectra
of a number of elements whose atomic numbers—that is, the numbers
assigned them in Moseley’s arrangement of the elements on the basis of
increasing X-ray frequency—are given on the left. These photographs
were taken by Siegbahn.[146] The distance from the “central image”—in
this case the black line on the left—to a given line of the line
spectrum on the right is approximately proportional to the wave-length
of the rays producing this line. The photographs show beautifully,
first, how the atoms of all the elements produce spectra of just the
same type, and, secondly, how the wave-lengths of corresponding lines
decrease, or the frequencies increase, with increasing atomic number.
The photograph on the left shows this progression for the highest
frequency rays which the atoms produce, the so-called series,
while the one on the right shows the same sort of a progression for
the rays of next lower frequency, namely, those of the so-called
series, which have uniformly from seven to eight times the wave-length
of the series. The plate opposite p. 200 shows some very
beautiful photographs taken by De Broglie in Paris[147] in October,
1916.