The telephone, the microphone & the phonographDu Moncel, Th., comte
History
The telephone, the microphone & the phonograph
Du Moncel, Th., comte
Microphone; Phonograph; Telephone
In order to reconcile these experiments with his preconceived ideas,
Mr. Hughes thought that, since the differences of resistance proceeding
from the vibrations of the conductor were only produced when it
was broken, the molecular movements were arrested by the lateral
resistances which were equal and opposite, but that if one of these
resistances were destroyed, the molecular movement could be freely
developed. He considers that an imperfect contact is equivalent to
the suppression of one of these resistances, and as soon as this
movement can take place, the molecular expansions and contractions
which result from the vibrations must correspond to the increase
or diminution of resistance in the circuit. We need not pursue Mr.
Hughes’s theory further, since it would take too long to develope it,
and we must continue our examination of the different properties of the
microphone.[17]
Carbon, as we have said, is not the only substance which can be
employed to form the sensitive organ of this system of transmission.
Mr. Hughes has tried other substances, including those which are good
conductors, such as metals. Iron afforded rather good results, and the
effect produced by surfaces of platinum when it was greatly subdivided
was equal, if not superior, to that furnished by the mercurised carbon.
Yet since the difficulty of making instruments with this metal is
greater, he prefers the carbon, which resembles it in being incapable
of oxidation.
We have already said that the microphone may be used as a thermoscope,
in which case it must have the special arrangement represented in fig.
43. Under these conditions, heat, reacting on the conductivity of these
contacts, may cause such variations in the resistance of the circuit
that the current of three Daniell cells will be annulled by approaching
the hand to the tube. In order to estimate the relative intensity of
the different sources of heat, it will be enough to introduce into
the circuit of the two electrodes A and B, fig. 43, a battery P, of
one or two Daniell cells, and a moderately sensitive galvanometer G.
For this purpose one of 120 turns will suffice. When the deviation
decreases, it shows that the source of heat is superior to the
surrounding atmosphere; and conversely, that it is inferior when the
deviation increases. Mr. Hughes says that the effects resulting from
the intervention of sunshine and shadow are shown on the instrument by
considerable variations in the deviations of the galvanometer. Indeed
it is so sensitive to the slightest variations of temperature that it
is impossible to maintain it in repose.
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