Pitch and frequency Pitch is an auditory sensation in which a listener assigns
musical tones to relative positions on a
musical scale based primarily on their perception of the
frequency of vibration (
audio frequency). Pitch is closely related to frequency, but the two are not equivalent. Frequency is an objective, scientific attribute which can be measured. Pitch is the subjective perception of a sound wave by the individual person, which cannot be directly measured. However, this does not necessarily mean that people will not agree on which notes are higher and lower. The
oscillations of sound waves can often be characterized in terms of
frequency.
Pitches are usually associated with, and thus quantified as,
frequencies (in cycles per second, or hertz), by comparing the sounds being assessed against sounds with
pure tones (ones with
periodic,
sinusoidal waveforms). Complex and aperiodic sound waves can often be assigned a
pitch by this method. According to the
American National Standards Institute, pitch is the auditory attribute of sound allowing those sounds to be ordered on a scale from low to high. Since pitch is such a close
proxy for frequency, it is almost entirely determined by how quickly the sound wave is making the air vibrate and has almost nothing to do with the intensity, or
amplitude, of the wave. That is, "high" pitch means very rapid oscillation, and "low" pitch corresponds to slower oscillation. Despite that, the
idiom relating vertical height to sound pitch is shared by most languages. In most cases, the pitch of complex sounds such as
speech and
musical notes corresponds very nearly to the repetition rate of periodic or nearly-periodic sounds, or to the
reciprocal of the time interval between repeating similar events in the sound waveform. Pitch depends to a lesser degree on the
sound pressure level (loudness, volume) of the tone, especially at frequencies below 1,000 Hz and above 2,000 Hz. The pitch of lower tones gets lower as sound pressure increases. For instance, a tone of 200 Hz that is very loud seems one semitone lower in pitch than if it is just barely audible. Above 2,000 Hz, the pitch gets higher as the sound gets louder. and W. Snow. Later investigations, e.g. by A. Cohen, have shown that in most cases the apparent pitch shifts were not significantly different from pitch‐matching errors. When averaged, the remaining shifts followed the directions of Stevens's curves but were small (2% or less by frequency, i.e. not more than a semitone). File:C3 131 Hz oscillogram.png|Lower pitches have lower frequency. C3, an octave below middle C. The frequency is half that of
middle C (131 Hz). (Scale: 1 square is equal to 1
millisecond) File:Middle C, or 262 hertz, on a virtual oscilloscope.png|
Oscillogram of middle C (262 Hz) (
pure tone) File:C5 523 Hz oscillogram.png|Higher pitches have higher frequency. Oscillogram of C5, an
octave above middle C. The frequency is twice that of middle C (523 Hz).
Theories of pitch perception Theories of pitch perception try to explain how the physical sound and specific physiology of the auditory system work together to yield the experience of pitch. In general, pitch perception theories can be divided into
place coding and
temporal coding. Place theory holds that the perception of pitch is determined by the place of maximum excitation on the
basilar membrane. A place code, taking advantage of the
tonotopy in the auditory system, must be in effect for the perception of high frequencies, since neurons have an upper limit on how fast they can
phase-lock their
action potentials. Temporal theories offer an alternative that appeals to the temporal structure of action potentials, mostly the
phase-lock of action potentials to frequencies in a stimulus. The precise way this temporal structure helps code for pitch at higher levels is still debated, but the processing seems to be based on an
autocorrelation of action potentials in the auditory nerve. However, it has long been noted that a neural mechanism that may accomplish a delay—a necessary operation of a true autocorrelation—has not been found. however, earlier work has shown that certain sounds with a prominent peak in their autocorrelation function do not elicit a corresponding pitch percept, and that certain sounds without a peak in their autocorrelation function nevertheless elicit a pitch. To be a more complete model, autocorrelation must therefore apply to signals that represent the output of the
cochlea, as via auditory-nerve interspike-interval histograms. The
jnd is typically tested by playing two tones in quick succession with the listener asked if there was a difference in their pitches. The
jnd becomes smaller if the two tones are played
simultaneously as the listener is then able to discern
beat frequencies. The total number of perceptible pitch steps in the human hearing range is about 1,400; the total number of notes in the equal-tempered scale, from 16 to 16,000 Hz, is 120.
Harmonics are an important class of overtones with frequencies that are integer multiples of the fundamental. Whether or not the higher frequencies are integer multiples, they are collectively called the
partials, referring to the different parts that make up the total spectrum. A sound or note of
indefinite pitch is one that a listener finds impossible or relatively difficult to identify as to pitch. Sounds with indefinite pitch do not have harmonic spectra or have altered harmonic spectra—a characteristic known as
inharmonicity. It is still possible for two sounds of indefinite pitch to clearly be higher or lower than one another. For instance, a
snare drum sounds higher pitched than a
bass drum though both have indefinite pitch, because its sound contains higher frequencies. In other words, it is possible and often easy to roughly discern the relative pitches of two sounds of indefinite pitch, but sounds of indefinite pitch do not neatly correspond to any specific pitch. ==Pitch standards and standard pitch==