The electron, its isolation and measurement and the determination of some of its properties
John Stuart Mill · en
Repeating the experiment and the computations with foils made from a
considerable number of other metals, they found that in every case
the number of free positive charges on the atoms of different
substances was approximately equal to half its atomic weight. This
means that the aluminum atom, for example, has a nucleus containing
about thirteen free positive charges and that the nucleus of the
atom of gold contains in the neighborhood of a hundred. This result
was in excellent agreement with the conclusion reached independently
by Barkla[143] from experiments of a wholly different kind, namely,
experiments on the scattering of X-rays. These indicated that the
number of scattering centers in an atom—that is, its number of free
negative electrons—was equal to about half the atomic weight. But this
number must, of course, equal the number of free positive electrons in
the nucleus.
V. MOSELEY’S REMARKABLE DISCOVERY
The foregoing result was only approximate. Indeed, there was internal
evidence in Geiger and Marsden’s work itself that a half was somewhat
too high. The answer was made very definite and very precise in 1913
through the extraordinary work of a brilliant young Englishman,
Moseley, who, at the age of twenty-seven, had accomplished as notable
a piece of research in physics as has appeared during the last fifty
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years. Such a mind was one of the early victims of the world-war. He
was shot and killed instantly in the trenches in Gallipoli in the
summer of 1915.