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
is oscillatory, and the electric strain in the non-conductor, or
dielectric, viz. the air around the plates, dies away by a series of
rapidly alternating electric strains in opposite directions.
Now, at this point I must recall to your recollection that, in speaking
about the production of air waves, I pointed out that one condition
essential to the production of an air wave was that there must be a
very sudden application or release of the air-pressure, such as is
caused by an explosion or escape of compressed air. We cannot produce
an air wave by moving any object such as a fan slowly to and fro
through the air. In order to produce an air wave we must strike the
air a very sudden blow, or, which comes to the same thing, we must
apply and remove a very sudden pressure to the air; and under these
circumstances we start into existence an air wave, which travels away
from the vibrating or rapidly moving body, and continues its journey
out into surrounding space.
I want to show you that, in the case of the Hertz oscillator, these
very sudden reversals of electric strain in the air or space round
about it, which take place at the moment when the oscillatory spark
passes between the knobs, creates in a similar manner what is called
an _electric wave_, which travels out into the space around. The point
you must appreciate is, that just as an air wave conveys away to
distant places a rapidly alternating compression made in the air by a
vibrating body at a particular place, so an electric wave conveys away
to distant places an alternating electric strain, which is originated
at some point in the medium by the oscillatory discharge of some
form of condenser. Before, however, we can demonstrate this fact, we
must have some means for detecting the influence of what we call an
electric wave. You will remember that, in the case of experiments with
air waves, I used a sensitive flame in order to make evident to you the
presence of waves in the air which you could not see, so here I must
use an appropriate detector for electric waves, the operation of which
will render evident to us the existence in the space round our electric
oscillator of the electric waves we cannot see.
Time will not permit me to discuss all the different forms of
electric-wave detector which have been invented. For our present
purposes we must limit ourselves to the description of one plan, which
depends on the remarkable fact that finely powdered dry metal or
metallic filings are non-conductors of the electric current until they
are subjected to an electromotive force exceeding a certain value, when
the metallic filings at once pass into a conductive condition.
Public-domain text, read in full here on John Shaqi.
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