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
After a very short time, therefore, the electrical conditions which
existed at the moment before the air broke down are exactly reproduced,
only the direction of the strain is reversed. In other words, the rod
which was positively electrified is now negatively, and _vice versâ_.
Then this state of strain again begins to disappear, producing in
the rod an electric current, again in the reverse direction; and so
the energy, which was originally communicated to the space round the
rods in the form of an electric strain, continually changes its form,
existing at one moment as energy of the electric current passing across
the spark gap, and the next moment as energy of electric strain. We
may ask why this state of things does not continue indefinitely, and
the answer to that question is twofold. First because the rods possess
a property called electrical resistance, and this acts towards the
electric current just as friction acts towards the motion of material
substances; in other words, it fritters away the energy into heat. So
at each reversal of the electric current in the rod a certain quantity
of the original store of energy has disappeared, due to the resistance.
There is, however, a further and more important source of dissipation
of energy, and this is due to the fact that an electrical oscillation
of this kind taking place in a finite straight circuit, or, as it
is called, an open electric circuit, creates in the space around an
electric wave. The rapid reversal of the electric strain in the air
results in the production of an electric wave, just as in the case of
an explosion made in air, the rapid compression of the air results in
the production of an air wave. It is not easy for those who come to the
subject for the first time to fully grasp the notion of what is implied
by the term “an electric wave.”
In the first lecture, you will perhaps remember, I pointed out that
the production of a wave in a medium of any kind can take place if
the medium possesses two properties. In the first place, it must
elastically resist some change or distortion, and, in the second place,
when that distortion is made it must tend to disappear if the medium
is left to itself, and in so doing the displacement of the medium must
overshoot the mark and be reproduced in the opposite direction, owing
to some inertia-like quality or power of persistence in the medium.
Public-domain text, read in full here on John Shaqi.
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