The electron, its isolation and measurement and the determination of some of its properties
John Stuart Mill · en
Now what does Dr. Ehrenhaft say to these very obvious suggestions as
to the cause of his troubles? Merely that he has avoided all oxygen,
and hence that an oxide film is impossible. Yet he makes his metal
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particle by striking an electric arc between metal electrodes.
This, as everyone knows, brings out all sorts of occluded gases.
Besides, chemical activity in the electric arc is tremendously intense,
so that there is opportunity for the formation of all sorts of higher
nitrides, the existence of which in the gases coming from electric arcs
has many times actually been proved. Dr. Ehrenhaft says further that he
photographs big mercury droplets and finds them spherical and free from
oxides. But the fact that some drops are pure mercury is no reason for
assuming that all of them are, and it is only the data on those which
are not which he publishes. Further, because big drops which he can see
and measure are of mercury is no justification at all for assuming that
sub-microscopic particles are necessarily also spheres of pure mercury.
In a word, Dr. Ehrenhaft’s tests as to sphericity and purity are all
absolutely worthless as applied to the particles in question, which
according to him have radii of the order .—a figure a
hundred times below the limit of sharp resolution.
IV. THE BEARING OF THE VIENNA WORK ON THE QUESTION
OF THE EXISTENCE OF A SUB-ELECTRON
But let us suppose that these observers do actually work with
particles of pure mercury and gold, as they think they do, and that
the observational and evaporational errors do not account for the low
values of . Then what conclusion could legitimately be drawn
from their data? Merely this and nothing more, that (1) Einstein’s
Brownian-movement equation is not universally applicable, and (2) that
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the law of motion of their very minute charged particles through
air is not yet fully known.[128] So long as they find exact multiple
relationships, as Dr. Ehrenhaft now does, between the charges carried
by a given particle when its charge is changed by the capture of ions
or the direct loss of electrons, the charges on these ions must be the
same as the ionic charges which I have accurately and consistently
measured and found equal to ;
for they, in their experiments, capture exactly the same sort of
ions, produced in exactly the same way as those which I captured and
measured in my experiments. That these same ions have one sort of a
charge when captured by a big drop and another sort when captured by a
little drop is obviously absurd. If they are not the same ions which
are caught, then in order to reconcile the results with the existence
of the exact multiple relationship found by Dr. Ehrenhaft as well as
ourselves, it would be necessary to assume that there exist in the air
an infinite number of different kinds of ionic charges corresponding
to the infinite number of possible radii of drops, and that when a