Scientific American Supplement, No. 595, May 28, 1887Various
Science
Scientific American Supplement, No. 595, May 28, 1887
Various
Science -- Periodicals
According to the wave theory, a condensation and rarefaction are
necessary to constitute a sound wave. Surely, if a condensation is not
produced, there can be no sound wave! We have then no need to consider
anything but the condensation or compression of the supposed air
molecules, which will shorten the discussion. The property of mobility of
the air and fluidity of water are well known. In the case of water, which
is almost incompressible, this property is well marked, and
unquestionably would be very nearly the same if water were wholly
incompressible. In the case of the air, it is conceded by Tyndall,
Thomson, Daniell, Helmholtz, and others that any compression or
condensation of the air must be well marked or defined to secure the
transmission of a sound pulse. The reason for this is on account of this
very property of mobility. Tyndall says: "The prong of the fork in its
swift advancement condenses the air." Thomson says: "If I move my hand
vehemently through the air, I produce a condensation." Helmholtz says:
"The pendulum swings from right to left with a uniform motion. Near to
either end of its path it moves slowly, and in the middle fast. Among
sonorous bodies which move in the same way, only very much faster, we may
mention tuning forks." Tyndall says again: "When a common pendulum
oscillates, it tends to form a condensation in front and a rarefaction
behind. But it is only a tendency; the motion is so slow, and the air so
elastic, that it moves away in front before it is sensibly condensed, and
fills the space behind before it can become sensibly dilated. Hence waves
or pulses are not generated by the pendulum." And finally, Daniell says:
"A vibrating body, _before it can act_ as a sounding body, must produce
alternate compressions and rarefactions in the air, and these must be
well marked. If, however, the vibrating body be so small that at each
oscillation the surrounding air has time to _flow round_ it, there is at
every oscillation a local rearrangement--a local flow and reflow of the
air; but the air at a distance is almost wholly unaffected by this."
Public-domain text, read in full here on John Shaqi.
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