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
Parallel to this very complete establishment of the validity in the
X-ray field of the Einstein photo-electric equation, and of its inverse
the Bohr equation, has come the rapid working out in the domain of
optics of the very large field of ionizing and radiating potentials
which has also involved the utilization and verification of the same
reciprocal relation. This will be seen at once from the definition of
the ionizing potential of an atom as the electronic energy which must
be thrown into it by bombardment to just remove from it one of its
outer electrons. Through the return of such removed electrons there is
in general a whole spectral series emitted. Similarly the radiating
potential of an atom is defined as the bombarding energy which must be
supplied to it to just lift one of its outer electrons from its normal
orbit to the first virtual orbit outside that normal orbit. When this
electron drops back there is in general the emission of a single-line
spectrum. All this work took its origin in the fundamental experiments
of Franck and Hertz[176] on mercury vapor in 1914. From 1916-22 the
field was worked out in great detail, especially in America by Foote
and Mohler, Wood, McLennan. Davis and Goucher, and others.
Suffice it to say that whether the energy comes in the form of ether
waves which through absorption in an atom lift an electron out of
a normal orbit, so that the atom passes over to an excited or to
an ionized state, or whether the energy enters in the form of a
bombarding electron and reappears as a radiated frequency, the
[Pg 248]
reciprocal relation represented in the Einstein-Bohr equation
has been found fulfilled in the most complete
manner.
In view of all these methods and experiments the general validity of
the Einstein equation, first proved photo-electrically about ten years
ago, is now universally conceded.
VI. OBJECTIONS TO AN ETHER-STRING THEORY
In spite of the credentials which have just been presented for
Einstein’s equation, the essentially corpuscular theory out of which he
got it has not yet met with general acceptance even by physicists of
Bohr’s type. There seems to be no possibility, at present, of bringing
it into harmony with a whole group of well-established facts of physics.
The recent practically complete bridging of the gap between X-rays and
light,[177] as well as that between heat waves and wireless waves,[178]
with the perfectly continuous passage of the latter over into static
electrical fields, appears to demand that, if we attempt to interpret
high frequency electromagnetic waves—X-rays and light—in terms of
undulatory “darts of light,” we also interpret wireless waves in the
same way, and this in turn requires us to use a similar mechanism in
the interpretation of static electrical fields. This brings us back to
Thomson’s ether-string theory, which seems to be a necessary part of
Einstein’s conception, if it is to have any physical basis whatever.
[Pg 249]
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