Hertzian Wave Wireless TelegraphyFleming, J. A. (John Ambrose), Sir
Science
Hertzian Wave Wireless Telegraphy
Fleming, J. A. (John Ambrose), Sir
Electric waves; Telegraph, Wireless
In the third case, when the electron vibrates, we have a state in
which self-closed lines of electric strain and magnetic flux are
thrown off and move away through the ether constituting electric
radiation, The manner in which this happens was first described by
Hertz in a Paper on "Electric Oscillations treated according to the
Method of Maxwell."[5] As this phenomenon lies at the very root of
Hertzian wave wireless telegraphy, we must spend a moment or two in
its careful examination.
Let us imagine two metal rods placed in line and constituting what is
called a linear oscillator. Let these rods have adjacent ends
separated by a very small air space, and let one rod be charged with
positive and the other with negative electricity. On the electronic
theory this is explained by stating that there is an accumulation of
electrons in one and of co-electrons in the other. These charges
create a distribution of electric strain throughout their
neighbourhood, which follows approximately the same law of
distribution as the lines of magnetic force of a bar magnet, and may
be roughly represented as in Fig. 1. Suppose then that the air gap is
destroyed, these charges move towards each other and disappear by
uniting, the lines of electric strain then collapse, and as they
shrink in give rise to circular lines of magnetic flux embracing the
rods. This external distribution of magnetism constitutes an electric
current in the rods produced by the movement of the two opposite
electric charges. At this stage it may be explained that the electrons
or atoms of electricity can in some cases make their way freely
between the atoms of ponderable matter. The former are incomparably
smaller than the latter, and in those cases in which this electronic
movement can take place easily, we call the material a good conductor.
[Illustration: FIG. 1.--LINES OF ELECTRIC STRAIN BETWEEN A POSITIVE
AND NEGATIVE ELECTRON AT REST.]
Suppose then the electric charges reappear in reversed positions and
go through an oscillatory motion. The result in the external space
would be the alternate production of lines of electric strain and
magnetic flux, the direction of these lines being reversed each half
cycle. Inside the rods we have a movement of electrons and
co-electrons to and fro, electric charges at the ends of the rods
alternating with electric currents in the rods, the charges being at a
maximum when the current is zero, and the current at a maximum when
the charges have for the moment disappeared. Outside the rods we have
a corresponding set of charges, lines of electric strain stretching
from end to end of the rod, alternating with rings of magnetic flux
embracing the rod. So far we have supposed the oscillation to be
relatively a slow one.
[Illustration: FIG. 2.--SUCCESSIVE STAGES IN THE DEFORMATION OF A LINE
OF STRAIN BETWEEN POSITIVE AND NEGATIVE ELECTRONS IN RAPID
OSCILLATION, SHOWING CLOSED LOOP OF ELECTRIC STRAIN THROWN OFF.]
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