Philipp Reis: Inventor of the Telephone: A Biographical SketchThompson, Silvanus P. (Silvanus Phillips)
History
Philipp Reis: Inventor of the Telephone: A Biographical Sketch
Thompson, Silvanus P. (Silvanus Phillips)
Reis, Philipp, 1834-1874; Telephone -- History
It is known[21] that if an electric current be led through a spiral
which surrounds an iron rod in the manner described, at every
interruption of the same a tone is audible arising from the vibration
of the rod. If the closings and interruptions of the circuit follow
one another relatively slowly, then there is produced by the changes
of position of the molecules of the rod, evoked by the electricity, a
tone,--the so-called longitudinal tone of the rod,--which is dependent
upon the length and stoutness of the rod. But if the closings and
interruptions of the electric current in the spiral follow one another
more rapidly than the vibrations of the smallest particles of the
iron rod,[22] which vibrations are determined by its elasticity, then
these particles cannot complete their paths, receive new impacts,
their vibrations become smaller, but quicker, and follow one another
as frequently as the interruptions. The iron rod then no longer gives
its longitudinal tone, but a tone, which is higher according as the
interruptions are more frequent in the given time, or lower, as they
are less frequent. It is known that the height and depth of tones
depends only on the number of air-waves which follow one another in a
second. We have seen above that by this is determined the number of
interruptions of the electric current of our apparatus by means of the
membrane and the platinum strip. The iron wire must therefore give out
the tone in the same height or depth as that which struck the membrane.
Now since a very far leading of the electricity makes it suffer
scarcely any weakening in proper apparatus, it is intelligible that one
can make the tone which acts on the membrane at one place audible, by
means of the iron rod, at any desired distance.
That the tone is made audible at a distance by the electric
agitations, and not by direct conduction of the sound-waves through the
wires is proved in the most evident way of all, because one instantly
hears no more the tone through the spiral when a good short circuit is
made, as, for example, by laying upon the two wires which conduct the
electricity a strip of sheet metal right in front of the spiral.
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