Hertzian Wave Wireless TelegraphyFleming, J. A. (John Ambrose), Sir
Science
Hertzian Wave Wireless Telegraphy
Fleming, J. A. (John Ambrose), Sir
Electric waves; Telegraph, Wireless
It is a little difficult without the employment of mathematical
analysis to explain precisely the manner in which earthing one side of
the loop or making the loop unsymmetrical as regards inductance has
the effect of creating overtones in it. The following rough
illustration may, however, be of some assistance. Imagine a long
spiral metallic spring supported horizontally by threads. Let this
represent a conductor, and let any movement to or fro of a part of the
spring represent a current in that conductor. Suppose we take hold of
the spring at one end, we can move it bodily to and fro as a whole. In
this case, every part of the spring is moving one way or the other in
the same manner at the same time. This corresponds with the case in
which the discharge of the condenser through the uniform loop
conductor is a flow of electricity, all in one direction one way or
the other. The current is in the same direction in all parts of the
loop at the same time, and, therefore, if the current is going up one
side of the loop it is at the same time coming down the other side.
Hence the two sides of the loop are always in exact opposition as
regards the effect of the current in them on the external space, and
the loop does not radiate. Returning again to the case of the spring.
Supposing that we add a weight to one end of the spring by attaching
to it a metal ball, and then move the other end to and fro with
certain periodic motion, it will be found quite easy to set up in the
spring a pulsatory motion resembling the movement of the air in an
open organ-pipe. Under these circumstances both ends of the spring
will be moving inwards or outwards at the same time, and the central
portions of the spring, although being pressed and expanded slightly,
are moving to and fro very little. This corresponds in the case of the
looped aerial with a current flowing up or down both sides at the same
time; in other words, when this mode of electrical oscillation is
established in the loop, its electrical condition is just that of two
simple Marconi aerials joined together at the top and vibrating in
their fundamental manner. Accordingly, if one side of the double loop
is earthed, we then have an arrangement which radiates waves.
Professor Slaby found that by giving one side of the loop less
inductance than the other, and at the same time earthing the side
having greater inductance at the bottom, he was able to make an
arrangement which radiated, not in virtue of the normal oscillations
of the condenser, but in virtue of the harmonic oscillations set up in
the conductor itself. The mathematical theory of this radiator has
been very fully developed by Dr. Georg Seibt.
Public-domain text, read in full here on John Shaqi.
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