A History of Science — Volume 5Williams, Henry Smith
History
A History of Science — Volume 5
Williams, Henry Smith
Science -- History
"Thus, in sufficiently supersaturated damp air a cloud is deposited on
these charged particles and they are thus rendered visible. This is the
first step towards counting them. The drops are, however, far too small
and too numerous to be counted directly. We can, however, get their
number indirectly as follows: suppose we have a number of these
particles in dust-free air in a closed vessel, the air being saturated
with water-vapor; suppose now that we produce a sudden expansion of the
air in the vessel; this will cool the air, it will be supersaturated
with vapor, and drops will be deposited round the charged particles. Now
if we know the amount of expansion produced we can calculate the cooling
of the gas, and, therefore, the amount of water deposited. Thus we know
the volume of water in the form of drops, so that if we know the volume
of one drop we can deduce the number of drops. To find the size of a
drop, we make use of the investigations made by Sir George Stokes on the
rate at which small spheres fall through the air. In consequence of
the viscosity of the air small bodies fall exceedingly slowly, and the
smaller they are the slower they fall." *
Professor Thompson gives us the formula by which Stokes made his
calculation. It is a relatively simple algebraic one, but need not be
repeated here. For us it suffices that with the aid of this formula,
by merely measuring the actual descent of the top of a vapor cloud,
Professor Thompson was able to find the volume of the drops and thence
the number of particles. The number of particles being known, the
charge of electricity carried by each could be determined, as already
suggested. Experiments were made with air, hydrogen, and carbonic acid,
and it was found that the particles had the same charge in all of these
gases. "A strong argument," says Professor Thompson, "in favor of
the atomic character of electricity." When we add that the charge in
question was found to be the same as the unit charge of an ion in a
liquid, it will be seen that the experiment has other points of interest
and suggestiveness.
Public-domain text, read in full here on John Shaqi.
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