On the Connexion of the Physical SciencesSomerville, Mary
Science
On the Connexion of the Physical Sciences
Somerville, Mary
Physical sciences; Science
heard at a distance through the air, the effect is as a landscape seen
in miniature beauty through a concave lens, compared with the same scene
viewed by ordinary vision through a murky atmosphere.”
Every one is aware of the reinforcement of sound by the resonance of
cavities. When singing or speaking near the aperture of a wide-mouthed
vessel, the intensity of some one note in unison with the air in the
cavity is often augmented to a great degree. Any vessel will resound if
a body vibrating the natural note of the cavity be placed opposite to
its orifice, and be large enough to cover it, or at least to set a large
portion of the adjacent air in motion. For the sound will be alternately
reflected by the bottom of the cavity and the undulating body at its
mouth. The first impulse of the undulating substance will be reflected
by the bottom of the cavity, and then by the undulating body, in time to
combine with the second new impulse. This reinforced sound will also be
twice reflected in time to conspire with the third new impulse; and, as
the same process will be repeated on every new impulse, each will
combine with all its echoes to reinforce the sound prodigiously.
Professor Wheatstone, to whose ingenuity we are indebted for so much new
and valuable information on the theory of sound, has given some very
striking instances of resonance. If one of the branches of a vibrating
tuning-fork be brought near the embouchure of a flute, the lateral
apertures of which are stopped so as to render it capable of producing
the same sound as the fork, the feeble and scarcely audible sound of the
fork will be augmented by the rich resonance of the column of air within
the flute, and the tone will be full and clear. The sound will be found
greatly to decrease by closing or opening another aperture; for the
alteration in the length of the column of air renders it no longer fit
perfectly to reciprocate the sound of the fork. This experiment may be
made on a concert flute with a C tuning-fork. But Professor Wheatstone
observes, that in this case it is generally necessary to finger the
flute for B, because, when blown into with the mouth, the under-lip
partly covers the embouchure, which renders the sound about a semitone
flatter than it would be were the embouchure entirely uncovered. He has
also shown, by the following experiment, that any one among several
simultaneous sounds may be rendered separately audible. If two bottles
be selected, and tuned by filling them with such a quantity of water as
will render them unisonant with two tuning-forks which differ in pitch,
on bringing both of the vibrating tuning-forks to the mouth of each
bottle alternately, in each case that sound only will be heard which is
reciprocated by the unisonant bottle.
Public-domain text, read in full here on John Shaqi.
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