The electron, its isolation and measurement and the determination of some of its propertiesMillikan, Robert Andrews
Philosophy
The electron, its isolation and measurement and the determination of some of its properties
Millikan, Robert Andrews
Electrons
We have shown in the preceding chapters how within the last two
decades there has been discovered beneath the nineteenth-century world
of molecules and atoms a wholly new world of electrons, the very
existence of which was undreamed of twenty years ago. We have seen
that these electrons, since they can be detached by X-rays from all
kinds of neutral atoms, must be constituents of all atoms. Whether or
not they are the sole constituents we have thus far made no attempt to
determine. We have concerned ourselves with studying the properties of
these electrons themselves and have found that they are of two kinds,
negative and positive, which are, however, exactly alike in strength
of charge but wholly different in inertia or mass, the negative being
commonly associated with a mass which is but ¹⁄₁₈₄₅ of that of the
lightest known atom, that of hydrogen, while the positive appears never
to be associated with a mass smaller than that of the hydrogen atom. We
have found how to isolate and measure accurately the electronic charge
and have found that this was the key which unlocked the door to many
another otherwise inaccessible physical magnitude. It is the purpose
of this chapter to consider certain other fields of exact knowledge
which have been opened up through the measurement of the electron, and
in particular to discuss what the physicist, as he has peered with his
newly discovered agencies, X-rays, radioactivity, ultra-violet light,
[Pg 183]
etc., into the insides of atoms, has been able to discover regarding
the numbers and sizes and relative positions and motions of these
electronic constituents, and to show how far he has gone in answering
the question as to whether the electrons are the sole building-stones
of the atoms.
1. THE SIZES OF ATOMS
One of the results of the measurement of the electronic charge was to
make it possible to find the quantity which is called the diameter
of an atom with a definiteness and precision theretofore altogether
unattained.
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