Hertzian Wave Wireless TelegraphyFleming, J. A. (John Ambrose), Sir
Science
Hertzian Wave Wireless Telegraphy
Fleming, J. A. (John Ambrose), Sir
Electric waves; Telegraph, Wireless
We may next proceed to apply these principles to the explanation of
the action of the simplest form of Hertzian wave telegraphic radiator,
viz., the Marconi aerial wire. In its original form this consists of a
long vertical insulated wire, A, the lower end of which is attached to
one of the spark balls S of an induction coil, I, the other spark ball
being connected to earth E, and the two spark balls being placed a few
millimetres apart (see Fig. 3). When the coil is set in action
oscillatory or Hertzian sparks pass between the balls, electric
oscillations are set up in the wire and electric waves are radiated
from it. Deferring for the moment a more detailed examination of the
operations of the coil and at the spark gap, we may here say that the
action which takes place in the aerial wire is as follows: The wire is
first charged to a high potential, let us suppose, with negative
electricity. We may imagine this process to consist in forcing
additional electrons into it, the induction coil acting as an electron
pump. Up to a certain pressure the spark gap is a perfect insulator,
but at a critical pressure, which for spark gap lengths of four or
five millimetres and balls about one centimetre in diameter
approximates to three thousand volts per millmetre, the insulation of
the air gives way, and the charge in the wire rushes into the earth.
In consequence, however, of the inertia of the medium or of the
electrons, the charge, so to speak, overshoots the mark, and the wire
is then left with a charge of opposite sign. This again in turn
rebounds, and so the wire is discharged by a series of electrical
oscillations, consisting of alternations of static charge and electric
discharge. We may fasten our attention either on the events taking
place in the vertical wire or in the medium outside, but the two sets
of phenomena are inseparably connected and go on together. When the
aerial wire is statically charged, we may describe it by saying that
there is an accumulation of electrons or co-electrons in it. Outside
the wire there is, however, a distribution of electric strain the
strain lines proceeding from the wire to the earth (see Fig. 4).
[Illustration: FIG. 4.--LINES OF ELECTRIC STRAIN (DOTTED LINES)
EXTENDING BETWEEN A MARCONI AERIAL, A, AND THE EARTH _ee_ BEFORE
DISCHARGE.]
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