Lightning Conductors: Their History, Nature, and Mode of ApplicationAnderson, Richard, F.C.S.
History
Lightning Conductors: Their History, Nature, and Mode of Application
Anderson, Richard, F.C.S.
Lightning conductors
The place filled in America by Lenz, and in Germany by Ohm, is
generally assigned in France to Professor Claude Pouillet, a savant who
devoted, perhaps, more time than any other in his own country to the
study of the phenomena of electricity. Born in 1791, Professor Pouillet
became, at a comparatively early age, the director of the celebrated
scientific institution of Paris known as the ‘Conservatoire des arts
et métiers,’ which led him to enter upon a course of experiments in
electricity, and most particularly, at the request of the government,
upon investigations as to the best material for lightning conductors.
The result of these was published in a lengthened treatise, in which
Professor Pouillet set down the electric conductivity of the principal
metals, taking copper at a hundred, as follows:—
Gold 103·05
Copper 100·00
Silver 81·26
Brass from 23·40 to 15·20
Platinum 22·50
Iron from 18·20 to 15·60
Cast Steel 14·75
Mercury 2·60
It will be seen that Professor Pouillet, differing from other
investigators, as they among themselves, regarding the relative
conductivity of the precious metals, gold, silver, and platinum, agreed
in the main with them as regards the relative proportions of copper
and iron. Most painstaking and minute in his experiments, he found
moreover that iron, as well as brass--the latter a mixed metal, and
as such variable in composition--was not always the same in respect
to conductivity, the changes being due to difference in temperature,
as well as greater or lesser metallic purity. As set down by him,
the variations in iron were between a maximum of 18·20 in regard to
100·00 of copper, and a minimum of 15·60, which gives a mean of 16·90.
Taking this mean, the comparative list of the positions held by copper
and iron in regard to electrical conductivity, according to the five
investigators, may be set forth in the following summary:—
Copper Iron
Davy 100·00 14·60
Becquerel 100·00 15·80
Lenz 100·00 17·74
Ohm 100·00 17·40
Pouillet 100·00 16·90
Taking the average of these five statements, it will be found that the
relative conductivity of copper to iron stands as 100 to 16½--that is,
a little over six to one. The approximate correctness of this figure,
being the result of all the investigations by the most eminent men who
studied the subject, can therefore admit of no reasonable doubt.
Public-domain text, read in full here on John Shaqi.
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