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 have no space to refer to the whole of the steps of discovery which
led up to the invention of all the various forms of the modern
electric kumascope or wave detector. Suffice it to say that the
researches of Hertz in 1887 threw a flood of light upon many
previously obscure phenomena, and enabled us to see that an electric
spark, and especially an oscillatory spark, creates a disturbance in
the ether, which has a resemblance in Nature to the expanding ripples
produced by a stone hurled into water. Scientific investigation then
returned with fresh interest to previously incomprehensible effects,
and a new meaning was read into many old observations. Again and again
it had been noticed that loose metallic contacts, loose aggregations
of metallic filings or fragments, had a mysterious way of altering
their conductivity under the action of electric sparks, lightning
discharges and high electromotive forces.
As far back as 1852, Mr. Varley had noticed that masses of powdered
metals had a very small conductivity, which increased in a remarkable
way during thunderstorms;[25] and in 1866, C. and S. A. Varley
patented a device for protecting telegraphic instruments from
lightning, which consisted of a small box of powdered carbon in which
were buried two nearly touching metal points, and they stated that
"powdered conducting matter offers a great resistance to a current of
moderate tension, but offers but little resistance to currents of high
tension."[26]
We then pass over a long interval and find that the next published
account of similar observations was due to Professor T.
Calzecchi-Onesti, who described in an Italian journal, _Il Nuovo
Cimento_ (see Vol. XVI., p. 58, and Vol. XVII., p. 38), in 1884 and
1885 his observations on the decrease in resistance of metal powders
when the spark from an induction coil was sent through them.[27] These
observations did not attract much attention until Professor E. Branly,
of Paris, in 1890 and 1891, repeated them on an extended scale and
with great variations, making the important observation that an
electric spark _at a distance_ had a similar effect in increasing the
conductivity of metallic powders.[28] Branly, however, noticed that in
some cases of conductors in powder, such as the peroxide of lead or
antimony, the effect of the spark was to cause a decrease of
conductivity.
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