To produce them it is desirable, if not necessary, to have the two
primary tones of considerable intensity. Helmholtz prefers the siren
to all other means of exciting them, and with this instrument they
are very readily obtained. It requires some attention at first, on
the part of the listener, to single out the resultant tone from the
general mass of sound; but, with a little practice, this is readily
accomplished; and though the unpracticed ear may fail, in the first
instance, thus to analyze the sound, the clang-tint is influenced in an
unmistakable manner by the admixture of resultant tones. I set Dove’s
siren in rotation, and open two series of holes at the same time; with
the utmost strain of attention, I am as yet unable to hear the least
symptom of a resultant tone. Urging the instrument to greater rapidity,
a dull, low droning mingles with the two primary sounds. Raising the
speed of rotation, the low, resultant tone rises rapidly in pitch, and
now, to those who stand close to the instrument, it is very audible.
The two series of holes here open number 8 and 12 respectively. The
resultant tone is in this case an octave below the deepest of the two
primaries. Opening two other series of orifices, numbering 12 and
16 respectively, the resultant tone is quite audible. Its rate of
vibration is one-third of the rate of the deepest of the two primaries.
In all cases, _the resultant tone is that which corresponds to a rate
of vibration equal to the difference of the rates of the two primaries_.
The resultant tone here spoken of is that actually heard in the
experiment. But with finer methods of experiment other resultant tones
are proved to exist. Those on which we have now fixed our attention
are, however, the most important. They are called _difference-tones_ by
Helmholtz, in consequence of the law just mentioned.
Public-domain text, read in full here on John Shaqi.
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