Waves and ripples in water, air, and æther : $b Being a course of Christmas lectures delivered at the Royal Institution of Great BritainFleming, J. A. (John Ambrose), Sir
Science
Waves and ripples in water, air, and æther : $b Being a course of Christmas lectures delivered at the Royal Institution of Great Britain
Fleming, J. A. (John Ambrose), Sir
Electric waves; Sound; Waves
Electromotive force may be created in many ways, and time will
not permit us to refer to these in detail, but it must be taken
that electrical machines, batteries, and dynamos are all of them
appliances for creating electromotive force, or, as it is sometimes
called, electric pressure, just as various kinds of force-pumps
are contrivances for creating pressure in fluids. We find that
electromotive force acts differently on various substances when they
are subjected to its operation. In some substances electromotive
force produces a continuous electric current, and in these cases the
material is called a _conductor_. In other cases electromotive force
creates what is called _electric strain_, or electric displacement,
and these substances are generally called _non-conductors_. The
difference between conductors and non-conductors can be illustrated by
a mechanical analogy. Consider, for instance, a force-pump consisting
of a cylinder with a tightly fitted piston; suppose the bottom of the
pump-tube to be closed by a pipe having in it a tap. If we open the
tap and apply pressure to the piston, we can force out of the pipe a
current of air which continues to flow as long as the piston is being
pressed down. In this case the pressure on the piston corresponds to
an electromotive force, and the current of air flowing out corresponds
with the electric current in the electrical circuit.
Supposing, however, that we shut the tap and then attempt to force down
the piston, we find at once an elastic resistance to motion. The piston
can be pressed down a little way, compressing the air and thus creating
a strain; but if the pressure is removed the piston flies up again, on
account of the compressional elasticity of the air. In this operation
we have a mechanical illustration of the action of electromotive force
on a material such as glass or air, which is called a non-conductor, or
sometimes a dielectric. In these bodies electromotive force produces
an electric strain, just as the mechanical force produces in the air
enclosed in the cylinder a mechanical strain. When the tap at the
bottom of the cylinder is closed, we can, by applying pressure, force
down the piston a little way, but that movement cannot be continued,
because we are building up an opposing pressure due to the elasticity
of the air.
Public-domain text, read in full here on John Shaqi.
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