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DICTIONARY OF MUSIC - El Atril

DICTIONARY OF MUSIC - El Atril

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HARMONICS HARMONICS 299<br />

ments as separate volumes), and was one of<br />

the best musical periodicals ever published in<br />

England. w. H. H.<br />

HARMONICS, tones of higher pitch which<br />

accompany every perfect musical sound in a<br />

regular series. As they ascend they diminish<br />

in intensity, and ajiproximate in pitch. If<br />

the piano be opened and a bass note be struck<br />

smartly and kept down, on listening atten-<br />

tively a succession of faint sounds will be<br />

heard, apparently rising out of the principal<br />

sound and floating round it. These are the<br />

harmonics. They are really constituents of the<br />

main musical tone, and are produced by the<br />

concurrent vibration of the aliquot 2>arts of the<br />

string. Hence Helmholtz jiroposes to call them<br />

' partial tones ' {Partialtime). This term is no<br />

doubt more appropriate, inasmuch as above the<br />

tentli degree most of these notes form inter\'al3<br />

dissonant from tile jirime note and also from<br />

each other, and thus become perceptibly inharmonic.<br />

On the best musical instruments,<br />

however, these high inharmonic tones are not<br />

reached, the vibratory impulse being exhausted<br />

on the prime note and the lower harmonics,<br />

which are consonant both with the prime note<br />

and among themselves. At the same time the<br />

smaller the aliquot parts become in the ascending<br />

series, the less easily are they set in a state<br />

of separate vibration. Consequently these high<br />

dissonant harmonics are distinctly audible only<br />

on highly resonant metallic instruments, such<br />

as the cymbals, bell, and triangle, and for<br />

practical purposes the old term harmonic<br />

answers as well as the term ' partial.'<br />

A few instruments, such as the tuning-fork<br />

and the wide stopped organ -pipe, practically<br />

yield no harmonics. The human voice, the<br />

harmonium, and all orchestral instruments, are<br />

rich in them—the human voice probably the<br />

richest of all ; but nature has so admirably<br />

compounded them that it is very difficult to<br />

analyse them scientifically. Rameau distinguished<br />

harmonics in the human voice as early<br />

as the beginning of the 18th century.<br />

Harmonics naturally reinforce the fundamental<br />

sound, in which case their extent and<br />

distribution largely influence the intensity and<br />

the quality of the sound. They may, however,<br />

in many instances, be produced singly by<br />

mechanically checking the vibration of the<br />

fundamental note. In this relation they con-<br />

stitute an important practical department in<br />

most orchestral instruments.<br />

Law of Harmiynics.—A sonorous body not<br />

only vibrates as a whole but in each of its<br />

several fractions or aliquot parts, \, -J, \, i, i,<br />

-f, and so on at the same time ; and each of<br />

these parts gives a separate note, the \ yielding<br />

the octave, the i the fifth, the \ the double<br />

octave, the i the third above the double octave,<br />

and so on. The following scheme or diagram,<br />

taken from Momigny, shows the harmonics of<br />

the open string G on<br />

thirteen pflaces :—<br />

the violoncello up to<br />

IMimimilltmiMi^<br />

Here the bottom G is produced by the vibration<br />

of the whole string. The two G's next<br />

above are produced by the vibration of the two<br />

halves. The three D's next above by the vibration<br />

of the three thirds ; and so on. Thus the<br />

diagram represents the whole of the notes produced<br />

by the vibrations of tlie whole string and<br />

its various sections up to its one-fourteenth<br />

part.<br />

In this scheme the first F (counting upwards),<br />

the C a fifth above it, and the topmost notes E<br />

and F, are more or less faulty. In practically<br />

deducing the diatonic scale from this scheme,<br />

these inter\'als have to be corrected by the ear.<br />

By inspection of this scheme we discover the<br />

intervals of the diatonic scale in the following<br />

order :<br />

^*e<br />

From this scale may obviously be deduced the<br />

chords of the third, fifth, seventh, and ninth.<br />

By combining and transposing these notes into<br />

one octave we get the following scale :<br />

-m=r:"^^1 ^r-i~^ which is the scale of C major ascending from<br />

dominant to dominant. As the same thing<br />

happens in other keys, we have thus proved the<br />

law that the intervals of each scale are generated<br />

by its dominant. The dominant, not the tonic,<br />

is therefore the true root of the whole scale.<br />

FiXd'fical eff'Xt of Harmonics heard simul-<br />

taneously ivith the fundamental note.—The harmonics<br />

not only determine the diatonic intervals,<br />

but to some extent the intensity and, as has<br />

been lately proved by Helmholtz, the quality<br />

of musical tones. On applying the ear to the<br />

sound-hole of a violin during a long crescendo<br />

on one note, tlie reinforcement of the tone by<br />

the gradual addition of the higher and more<br />

piercing harmonics is distinctly perceptible.<br />

The principle and the ellect are precisely the<br />

same in a crescendo produced by the addition<br />

of the mixture stops on an organ. The loudest<br />

musical instruments, caeteris jmribus, are those<br />

in whicli the highest harmonics predominate,<br />

e.g. the cymbals, triangle, bell, and gong.<br />

The etlect of harmonics on the quality of<br />

musical sounds is easily tested by carefully comparing<br />

the tones of an old and a new violin.<br />

In the former the strong vibrations of the fundamental<br />

note and the lower harmonics leave but

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