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
In the previous chapters your attention has been directed to the
subject of waves on water and waves in air, and we shall now proceed
to discuss some of the more difficult matters connected with the
production of waves in the æther. We shall find that this portion of
our subject makes more demands upon our powers of comprehension, since
much that we have to consider is not directly the object of sense
perception, and the inferences which we have to make from observed
facts are less simple and easy to follow. Nevertheless, I trust that
if you have been able to grasp clearly the nature of a surface-wave on
water and of a compressional wave in air, you will not readily allow
yourselves to be discouraged from encountering a new class of ideas,
but will be able to advance still further, and gain a more or less
clear conception of the nature of an electric wave in the æther.
In the first place, we must consider the medium in which these waves
are created. We can see with our eyes a water-surface, and we are
able to understand without much difficulty that the surface can be
thrown into humps and hollows, or become wrinkled, and also that these
elevations and depressions can change their position, thus creating a
surface wave which moves forward. The movement of the water wave is,
therefore, only the result of a local elevation of the surface which
travels along or takes place progressively at different places on the
surface. Then, again, in the case of an air wave, although we cannot
see the air, we are able, with some little assistance from experiments,
to present to ourselves a clear mental picture of a progressive
movement through the air of a region of compression, that is to say, a
certain slice, layer, or zone of the air is more compressed than the
neighbouring portions, and this region of compression changes its place
progressively. It has been carefully explained that the production of
a wave of any kind implies, therefore, two things—first, a medium or
material in which the wave exists; and, secondly, some kind of periodic
change or movement which is experienced by the various portions of this
medium at different places successively.
If, therefore, we are given any medium, say water or air, and asked
to explain the production of a wave in it, we have first to consider
what kind of changes can take place in it, or on it, which can appear
progressively at different parts. In the case of the water-surface,
some parts may be heaped up higher than the rest, and the heaping up
may occur at successive places in such fashion that when it disappears
at one place it reappears at a contiguous or neighbouring place. In the
case of air, some portion may be compressed more than the rest, and
the place of compression may move forward, so that as the compression
is released in one place it makes its appearance in an adjacent one.
In the first case, we have a wave of elevation on water; in the second
case, a wave of compression in the air.
Public-domain text, read in full here on John Shaqi.
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