Pure tone

A pure tone's pressure waveform versus time looks like this; its frequency determines the x axis scale; its amplitude determines the y axis scale; and its phase determines the x origin.

In psychoacoustics, a pure tone is a sound with a sinusoidal waveform; that is, a sine wave of constant frequency, phase-shift, and amplitude.[1] By extension, in signal processing a single-frequency tone or pure tone is a purely sinusoidal signal (e.g., a voltage). A pure tone has the property – unique among real-valued wave shapes – that its wave shape is unchanged by linear time-invariant systems; that is, only the phase and amplitude change between such a system's pure-tone input and its output.

Sine and cosine waves can be used as basic building blocks of more complex waves. As additional sine waves having different frequencies are combined, the waveform transforms from a sinusoidal shape into a more complex shape. When considered as part of a whole spectrum, a pure tone may also be called a spectral component.

In clinical audiology, pure tones are used for pure-tone audiometry to characterize hearing thresholds at different frequencies. Sound localization is often more difficult with pure tones than with other sounds.[2][3]

  1. ^ ANSI S1.1-1994 Acoustical Terminology
  2. ^ Stanley Smith Stevens and Edwin B. Newman (1936). "The localization of actual sources of sound". The American Journal of Psychology. 48 (2): 297–306. doi:10.2307/1415748. JSTOR 1415748.
  3. ^ Hartmann, W. M. (1983). "Localization of sound in rooms". The Journal of the Acoustical Society of America. 74 (5): 1380–1391. Bibcode:1983ASAJ...74.1380H. doi:10.1121/1.390163. PMID 6643850.

Developed by StudentB