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
The fact that there is such a space-filling æther is, therefore, only
to be deduced by reasoning from experiments and observations, but it is
not directly the object of our sense-perceptions in the same way that
water or air can be. Nevertheless, there is abundant proof that it is
not merely a convenient scientific fiction, but is as much an actuality
as ordinary gross, tangible, and ponderable substances. It is, so to
speak, matter of a higher order, and occupies a rank in the hierarchy
of created things which places it above the materials we can see and
touch.
The question we have next to discuss is—What are the fundamental
properties of this æther? and what are the terms in which we must
describe its qualities? In order to answer these questions, we must
direct attention to some electrical effects, since it has been shown
that most of the electrical phenomena, like those of optics, point
to the necessity for the assumption of a similar universal medium,
different from ordinary matter. Abundant proof has been gathered in,
that the electro-magnetic medium and the luminiferous æther are one and
the same.
We are met at the very outset of our electrical studies by the term
_electric current_. Most of us know that the operation of electric
telegraphs and telephones, electric lamps and electric railways, depend
upon this employment of an agency called an electric current.
The question then arises—What _is_ an electric current? and the
answer to this question is not easy to give in a few words. We can,
however, begin by explaining what an electric current can do, and how
its presence can be recognized. Before me on the table is a spiral of
copper wire, and in this wire, by special means, I can create what we
call an electric current. I shall ask you to notice that when this is
done two effects are immediately produced. In the first place, the wire
becomes _hot_, and, secondly, it becomes _magnetic_. The fact that it
is hot is evident, because it is now nearly red hot, and is visibly
incandescent in the dark. If we dip the wire in iron filings, you will
see that these cling to the wire and are taken up by it, just as when
an ordinary steel magnet is substituted for the wire. The copper wire,
when traversed by the current, also attracts a compass needle, and we
thus demonstrate in another way its magnetic quality.
Whenever, therefore, we find these two states of heat and magnetism
present together in and round a wire, we may take it as an indication
that it forms part of a circuit through which an electric current is
flowing. An electric current is a physical state or condition which can
only exist in or all along a closed path which is called an electric
circuit. This electric circuit may consist of a metallic wire, or, as
we generally call it, a conductor, or, as we shall see, it may also in
part consist of what is usually called a non-conductor.
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