Individual differences |
Methods | Statistics | Clinical | Educational | Industrial | Professional items | World psychology |
In acoustics the harmonic of a wave is a component frequency of the signal that is an integer multiple of the fundamental frequency. For example, if the frequency is f, the harmonics have frequency 2f, 3f, 4f, etc, as well as f itself. The harmonics have the property that they are all periodic at the signal frequency. Also, due to the properties of Fourier series, the sum of the signal and its harmonics is also periodic at that frequency.
Many oscillators, including the human voice, a bowed violin string, are more or less periodic, and thus can be decomposed into harmonics.
Most passive oscillators, such as a plucked guitar string or a struck drum head or struck bell, naturally oscillate at several frequencies known as overtones. When the oscillator is long and thin, such as a guitar string, a trumpet, or a chime, the overtones are still integer multiples of the fundamental frequency. Hence, these devices can mimic the sound of singing and are often incorporated into music. Overtones whose frequency is not an integer multiple of the fundamental are called inharmonic and are often perceived as unpleasant.
The untrained human ear typically does not perceive harmonics as separate notes. Instead, they are perceived as the timbre of the tone. In a musical context, overtones that are not exactly integer multiples of the fundamental are known as inharmonics. Inharmonics that are not close to harmonics are known as partials. Bells have more clearly perceptible partials than most instruments. Antique singing bowls are well known for their unique quality of producing multiple harmonic overtones or multiphonics.
The tight relation between overtones and harmonics in music often leads to their being used synonymously in a strictly musical context, but they are counted differently leading to some possible confusion. This chart demonstrates how they are counted:
|1f||440 Hz||fundamental frequency||first harmonic|
|2f||880 Hz||first overtone||second harmonic|
|3f||1320 Hz||second overtone||third harmonic|
|4f||1760 Hz||third overtone||fourth harmonic|
In many musical instruments, it is possible to play the upper harmonics without the fundamental note being present. In a simple case (e.g. recorder) this has the effect of making the note go up in pitch by an octave; but in more complex cases many other pitch variations are obtained. In some cases it also changes the timbre of the note. This is part of the normal method of obtaining higher notes in wind instruments, where it is called overblowing. The extended technique of playing multiphonics also produces harmonics. On string instruments it is possible to produce very pure sounding notes, called harmonics by string players, which have an eerie quality, as well as being high in pitch. Harmonics may be used to check at a unison the tuning of strings that are not tuned to the unison. For example, lightly fingering the node found half way down the highest string of a cello produces the same pitch as lightly fingering the node 1/3 of the way down the second highest string. For the human voice see Overtone singing, which uses harmonics.
Harmonics may be either used or considered as the basis of just intonation systems. Composer Arnold Dreyblatt is able to bring out different harmonics on the single string of his modified double bass by slightly altering his unique bowing technique halfway between hitting and bowing the strings. Composer Lawrence Ball uses harmonics to generate music electronically.
The fundamental frequency is the reciprocal of the period of the periodic phenomenon.
Harmonics on stringed instruments
The following table displays the stop points on a stringed instrument, such as the guitar, at which gentle touching of a string will force it into a harmonic mode when vibrated.
|harmonic||stop note||harmonic noteing||cents||reduced|
|3||just perfect fifth||P8 + P5||1902.0||702.0|
|4||just perfect fourth||2P8||2400.0||0.0|
|5||just major third||2P8 + just M3||2786.3||386.3|
|6||just minor third||2P8 + P5||3102.0||702.0|
|7||septimal minor third||2P8 + septimal m7||3368.8||968.8|
|8||septimal major second||3P8||3600.0||0.0|
|9||Pythagorean major second||3P8 + pyth M2||3803.9||203.9|
|10||just minor whole tone||3P8 + just M3||3986.3||386.3|
|11||greater unidecimal neutral second||3P8 + just M3 + GUN2||4151.3||551.3|
|12||lesser unidecimal neutral second||3P8 + P5||4302.0||702.0|
|13||tridecimal 2/3-tone||3P8 + P5 + T23T||4440.5||840.5|
|14||2/3-tone||3P8 + P5 + septimal m3||4568.8||968.8|
|15||septimal (or major) diatonic semitone||3P8 + P5 + just M3||4688.3||1088.3|
|16||just (or minor) diatonic semitone||4P8||4800.0||0.0|
Table of harmonics
- Problems playing the files? See media help.
|Violin natural harmonic stop points on the A string|
|Demonstration of harmonics using electronic sine tones - fundamental and 15 harmonics of 110 Hz, 0.5s each. Note that each harmonic is presented at the same signal level as the fundamental; the sample tones get louder as they go up in frequency|
|This page uses Creative Commons Licensed content from Wikipedia (view authors).|