Hertzian Wave Wireless TelegraphyFleming, J. A. (John Ambrose), Sir
Science
Hertzian Wave Wireless Telegraphy
Fleming, J. A. (John Ambrose), Sir
Electric waves; Telegraph, Wireless
for Hertzian wave telegraphy are exactly those which should be taken
in making a good earth for a lightning conductor.
Whilst on the subject of aerials, a word may be said on the
localisation of wireless telegraph stations on the Marconi system. For
reasons which were explained previously, the transmission of signals
is effected more easily over water than over dry land, and it is
hindered if the soil in the neighbourhood of the sending station is a
poor conductor. Hence, all active Hertzian wave telegraph stations,
like all active volcanoes, are generally found near the sea. In those
cases in which a multiple aerial has to be put up consisting of many
wires, one mast may be insufficient to support the structure, and
several masts arranged in the form of a square or a circle have to be
employed. The illustrated papers have reproduced numerous pictures of
the Marconi power stations at Poldhu in Cornwall, Glace Bay in Nova
Scotia, and Cape Cod in the United States. In these stations, after
preliminary failures to obtain the necessary structural strength with
ordinary masts, tall lattice girder wooden towers have been built,
about 215 feet in height, well stayed against wind pressure, and which
so far have proved themselves capable of withstanding any storm of
wind which has come against them.
An important question in connection with the sending power of an
aerial is that of the relation of its height to the distance covered.
Some time ago Mr. Marconi enunciated a law, as the result of his
experiments, connecting these two quantities, which may be called
Marconi's Law. He stated that the height of the aerial to cover a
given distance, other things remaining the same, varies as the square
root of the distance. Let D be the distance and let L be the length of
the aerial, then if both the transmitting and receiving aerial are the
same height, we may say that D varies as L^{2}. This relation may be
theoretically deduced as follows:--Any given receiving apparatus for
Hertzian wave telegraphy requires a certain minimum energy to be
imparted to it to make it yield a signal. If the resistance and the
capacity of the receiver is taken as constant, this minimum working
energy is proportional to the square of the electromotive force set up
in the receiving aerial by the impact on it of the electric waves.
This electromotive force varies as the length of the receiving aerial
and as the magnetic force due to the wave cutting across it, and the
magnetic force varies as the current in the transmitting aerial, and
therefore, for any given voltage varies as the capacity, and therefore
as the length of the transmitting aerial. If, therefore, the
transmitting and receiving aerial have the same length, the minimum
energy varies as the square of the electromotive force in the
receiving aerial, and therefore as the fourth power of the length of
either aerial, since the electromotive force varies as the product of
the lengths of the aerials.
Public-domain text, read in full here on John Shaqi.
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