Open main menu
Home
Random
Recent changes
Special pages
Community portal
Preferences
About Wikipedia
Disclaimers
Incubator escapee wiki
Search
User menu
Talk
Dark mode
Contributions
Create account
Log in
Editing
Pure tone
(section)
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
== Relation to pitch and musical tones == Pure tones have been used by 19th century physicists like [[Georg Ohm]] and [[Hermann von Helmholtz]] to support theories asserting that the ear functions in a way equivalent to a [[Fourier analysis|Fourier frequency analysis]].<ref>{{cite book |last1=von Helmholtz |first1=Hermann L. F. |last2=Ellis |first2=Alexander J. |title=On the sensations of tone as a physiological basis for the theory of music |date=1875 |publisher=Longmans, Green, and Co. |location=London, UK |url=https://archive.org/stream/onsensationston00helmgoog#page/n2/mode/2up}}</ref><ref>{{cite journal |last1=Ohm |first1=Georg |title=Ueber die Definition des Tones, nebst daran geknupfter Theorie der Sirene und ahnlicher tonbildenden Vorrichtungen |journal=Poggendor's Annalen der Physik und Chemie |date=1843 |volume=59 |pages=513β565}}</ref> In [[Ohm's acoustic law]], later further elaborated by Helmholtz, [[musical tone]]s are perceived as a set of pure tones. The percept of [[Pitch (music)|pitch]] depends on the frequency of the most prominent tone, and the phases of the individual components is discarded. This theory has often been blamed for creating a confusion between pitch, frequency and pure tones.<ref>{{cite book | title = Foundations of Modern Auditory Theory | editor = Jerry V. Tobias | publisher = Academic Press | volume = 1 | author = W. Dixon Ward | chapter = Musical Perception |year = 1970 | page = 438}}</ref> Unlike [[musical tone]]s that are composed of the sum of a number of harmonically related sinusoidal components, pure tones only contain one such sinusoidal waveform. When presented in isolation, and when its frequency pertains to a certain range, pure tones give rise to a single pitch percept, which can be characterized by its frequency. In this situation, the instantaneous phase of the pure tone varies linearly with time. If a pure tone gives rise to a constant, steady-state percept, then it can be concluded that its phase does not influence this percept. However, when multiple pure tones are presented at once, like in musical tones, their relative phase plays a role in the resulting percept. In such a situation, the perceived pitch is not determined by the frequency of any individual component, but by the frequency relationship between these components (see [[missing fundamental]]).<gallery> File:Middle C, or 262 hertz, on a virtual oscilloscope.png|Pure tone [[Oscilloscope|oscillogram]] of middle C (262 Hz). (Scale: 1 square is equal to 1 [[millisecond]]) File:C3 131 Hz oscillogram.png|Pure tone for C3, an [[octave]] below middle C. The frequency is half that of [[C (musical note)|middle C]] (131 Hz). File:C5 523 Hz oscillogram.png|Pure tone oscillogram of C5, an [[octave]] above middle C. The frequency is twice that of middle C (523 Hz). </gallery>
Edit summary
(Briefly describe your changes)
By publishing changes, you agree to the
Terms of Use
, and you irrevocably agree to release your contribution under the
CC BY-SA 4.0 License
and the
GFDL
. You agree that a hyperlink or URL is sufficient attribution under the Creative Commons license.
Cancel
Editing help
(opens in new window)