Hertzian Wave Wireless TelegraphyFleming, J. A. (John Ambrose), Sir
Science
Hertzian Wave Wireless Telegraphy
Fleming, J. A. (John Ambrose), Sir
Electric waves; Telegraph, Wireless
This distinction is a perfectly fair one. Any telegraph or telephone
wire can be tapped, if it is desired, but unless there is some fault
on the line, no station will receive a message against its desires.
Moreover, it may be noted that there are penalties attached to tapping
a telegraph wire, and at present there are none connected with the
misappropriation of an ether wave.
We shall, therefore, consider in the first place the methods so far
proposed for preventing any given receiver from being affected by
Hertzian waves sent out from other stations, except that of those from
which it is desired to receive them. The first method is that which
has been called the method of _electrical syntony_, and consists in
adjusting the electrical capacity and inductance of the various open
and closed circuits of the receiving and transmitting stations to be
put in communication so that they have the same electrical
time-period.[60]
In the Cantor Lectures before the Society of Arts in 1900, on
electrical oscillations and electric waves, the author has discussed
at length the conditions under which powerful electrical oscillations
can be set up in a circuit. It was there shown that every electric
circuit having capacity and inductance has a particular or natural
time-period of electrical oscillation depending on the product of
these qualities, and that, to accumulate powerful electrical
oscillations in it, the electromotive impulses on it must be delivered
at this rate. Illustrations were drawn from mechanics, such as the
examples furnished by vibrating pendulums and springs, and from
acoustics, as illustrated by the phenomena of resonance, to show that
small or feeble blows or impulses delivered at the proper time
intervals have a cumulative effect in setting up vibrations in a body
capable of oscillation. It is a familiar fact that if we time our
blows, we can achieve that which no single blow, however powerful, can
accomplish in throwing into vibration a body such as a pendulum, which
is capable of oscillation under the action of a restoring force.
Precisely the same is true of an electric circuit. We have already
seen that the receiving aerial has an alternating electromotive force
set up in it by the impact of the successive electric waves sent out
from the transmitter. It must, however, be remembered that the
transmitter sends out a series of trains of waves, not by any means a
continuous train, but one cut up into groups of probably ten to fifty
waves, each separated by intervals of silence, long, compared with the
duration of a single train of waves.
[Illustration: FIG. 22.--SEIBT'S APPARATUS FOR EXHIBITING ELECTRIC
RESONANCE. I, induction coil; S, spark gap; CC, condensers; L,
variable inductance; E, earth plate; WW, wire spirals; VV, vacuum
tubes.]
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