Scientific American Supplement, No. 455, September 20, 1884Various
Science
Scientific American Supplement, No. 455, September 20, 1884
Various
Science -- Periodicals
With earth currents we have here very little to do. The rotation of the
earth is in itself sufficient to generate small currents, and the fact
that they vary in strength at regular periods of the day and of the year
enforces the suggestion that the sun exerts considerable electrical
influence on the earth. Letting it be granted, however, that the earth is
variously charged, how comes it that the air is also charged, and with
electricity of greater tension than that of the earth itself? It was
pointed out by Sir W. Grove that if the extremities of a piece of platinum
wire be placed in a candle flame, one at the bottom and the other near the
top, an electric current will flow through the wire, indicating the
presence of electricity. If an electrified body be heated, the electricity
escapes more rapidly as the temperature rises. If a vessel of water be
electrified, and the water then converted into steam, the electric charge
will be rapidly dissipated. If a vessel containing water be electrified,
and the water allowed to escape drop by drop, electricity will escape with
each drop, and the vessel will soon be discharged.
We regard it as an established fact that the earth has always a greater or
less charge; whence it is safe to assume that in the process of
evaporation which is going on all over the surface of the globe, more
particularly in equatorial regions, every particle of water, as it rises
into the air, carries with it its portion, however minute that portion may
be, of the earth's electric charge. This small charge distributes itself
over the surface of the aqueous particle, and the vapor rises higher and
higher until it reaches that point above which the air is too rare to
support it. It then flows away laterally, and as it approaches colder
regions gets denser, sinking lower and nearer to the earth's surface. The
aqueous particles becoming reduced in size, the extent of their surfaces
is proportionately reduced. It follows that as the particles and their
surfaces are reduced, the charge is confined to a smaller surface, and
attains, therefore, a greater "surface density," or in simpler language, a
greater amount of electricity per unit of surface.
Electricity, as above set forth, is in what is known as the "static"
condition (to distinguish it from electricity which is being transferred
in the form of a current), when it has the property of "repelling itself"
to the utmost limits of any conductor upon which it may be confined. This
will account for the charge finding its way to the surface of the water
particles, and will furthermore account for the greater density of the
charge as the particle gets smaller and has the extent of its surface
rapidly diminished. It may be mentioned that the surface of a sphere
varies as the cube of its radius.
Public-domain text, read in full here on John Shaqi.
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