Waves and ripples in water, air, and æther : $b Being a course of Christmas lectures delivered at the Royal Institution of Great BritainFleming, J. A. (John Ambrose), Sir
Science
Waves and ripples in water, air, and æther : $b Being a course of Christmas lectures delivered at the Royal Institution of Great Britain
Fleming, J. A. (John Ambrose), Sir
Electric waves; Sound; Waves
CHAPTER IV.
SOUND AND MUSIC.
Our discussion of waves and ripples in the air would be very incomplete
if we left it without any further reference to the difference between
those motions in the air which constitute noise or sound, and those
to which we owe the pleasure-producing effects of musical tones. I
propose, therefore, to devote our time to-day to a brief exposition of
the properties and modes of production of those air-vibrations which
give rise to the class of sensations we call music. Sufficient has
already been said to make it clear to you that one essential difference
between sound or noise and music, as far as regards the events taking
place outside of our own organism, is that, in the first case, we
have a more or less irregular motion in the air, and, in the second,
a rhythmical movement, constituting a train of air waves. The greater
pleasure we experience from the latter is, no doubt, partly due to
their rhythmic character. We derive satisfaction from all regularly
repeated muscular movements, such as those involved in dancing,
skating, and rowing, and the agreeable sensation we enjoy in their
performance is partly due to their periodic or cyclical character.
In the same way, our ears are satisfied by the uniformly repeated and
sustained vibrations proceeding from an organ-pipe or tuning-fork in
action, but we are irritated and annoyed by the sensations set up when
irregular vibrations of the air due to the bray of a donkey or the
screech of a parrot fall upon them. Before, however, we can advance
further in an analysis of the nature of musical sounds, two things must
be clearly explained. The first of these is the meaning of the term
_natural period of vibration_, and the second is the nature of the
effect called _resonance_. You see before you three small brass balls
suspended by strings. One string is 1 foot long, the second 4 feet, and
the third 9 feet. These suspended balls are called _simple pendulums_.
Taking in my hands the balls attached to the 1-foot and the 4-foot
strings, I withdraw them a little way from their positions of rest and
let them go. They vibrate like pendulums, but, as you see, the 1-foot
pendulum makes two swings in the time that the 4-foot makes one swing.
Repeating the experiment with the 1-foot and the 9-foot pendulum, we
find that the short one now makes three swings in the time the long
one makes one swing. The inference immediately follows that these
pendulums, whose respective lengths are 1, 4, and 9 feet, make their
swings from side to side in times which are respectively in the ratio
of 1, 2, and 3.
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