Editing Fundamental frequency

{{Short description|Lowest frequency of a periodic waveform, such as sound}}
{{Use American English|date=January 2019}}
[[File:Harmonic partials on strings.svg|thumb|250px|[[Vibration]] and [[standing wave]]s in a string, The fundamental and the first six [[overtone]]s]]

The '''fundamental frequency''', often referred to simply as the '''''fundamental''''' (abbreviated as '''{{var|f}}<sub>0</sub>''' or '''{{var|f}}<sub>1</sub>''' ), is defined as the lowest [[frequency]] of a [[Periodic signal|periodic]] [[waveform]].<ref>{{Cite web |last=Nishida |first=Silvia Mitiko |title=Som, intensidade, frequência |url=https://www2.ibb.unesp.br/nadi/Museu2_qualidade/Museu2_corpo_humano/Museu2_como_funciona/Museu_homem_nervoso/Museu2_homem_nervoso_audicao/Museu2_qualidade_homem_nervoso_audicao_som.htm |access-date=2024-09-05 |website=Instituto de Biociências da [[Unesp]]}}</ref> In music, the fundamental is the musical [[pitch (music)|pitch]] of a note that is perceived as the lowest [[Harmonic series (music)#Partial|partial]] present. In terms of a superposition of [[Sine wave|sinusoid]]s, the fundamental frequency is the lowest frequency sinusoidal in the sum of harmonically related frequencies, or the frequency of the difference between adjacent frequencies.  In some contexts, the fundamental is usually abbreviated as '''{{var|f}}<sub>0</sub>''', indicating the lowest frequency [[Zero-based numbering|counting from zero]].<ref>{{cite web |url=http://www.phon.ucl.ac.uk/home/johnm/sid/sidf.htm |title=sidfn |publisher=Phon.UCL.ac.uk |access-date=2012-11-27 |archive-url=https://web.archive.org/web/20130106050848/http://www.phon.ucl.ac.uk/home/johnm/sid/sidf.htm |archive-date=2013-01-06 |url-status=dead }}</ref><ref>{{cite web|url= http://www.acoustics.hut.fi/publications/files/theses/lemmetty_mst/chap3.html |last=Lemmetty |first=Sami |title=Phonetics and Theory of Speech Production |publisher=Acoustics.hut.fi |date=1999 |access-date=2012-11-27}}</ref><ref>{{cite web |url=http://fourier.eng.hmc.edu/e101/lectures/Fundamental_Frequency.pdf |archive-url=https://web.archive.org/web/20140514122624/http://fourier.eng.hmc.edu/e101/lectures/Fundamental_Frequency.pdf |archive-date=2014-05-14 |url-status=dead |title=Fundamental Frequency of Continuous Signals |date=2011 |publisher=Fourier.eng.hmc.edu |access-date=2012-11-27 }}</ref> In other contexts, it is more common to abbreviate it as '''{{var|f}}<sub>1</sub>''', the first [[harmonic]].<ref>{{cite web |url=https://nchsdduncanapphysics.wikispaces.com/file/view/Standing+Waves+in+a+Tube+II.pdf |title=Standing Wave in a Tube II – Finding the Fundamental Frequency |publisher=Nchsdduncanapphysics.wikispaces.com |access-date=2012-11-27 |archive-date=2014-03-13 |archive-url=https://web.archive.org/web/20140313133719/https://nchsdduncanapphysics.wikispaces.com/file/view/Standing+Waves+in+a+Tube+II.pdf |url-status=dead }}</ref><ref>{{cite web |url=http://physics.kennesaw.edu/P11_standwaves3.pdf |title=Physics: Standing Waves |publisher=Physics.Kennesaw.edu |access-date=2012-11-27 |archive-date=2019-12-15 |archive-url=https://web.archive.org/web/20191215062640/https://csm.kennesaw.edu/physics/ |url-status=dead }}</ref><ref>{{cite web |url= http://www.colorado.edu/physics/phys1240/phys1240_fa05/notes/lect24_Tu11_22_4up.pdf |title=Phys 1240: Sound and Music |last=Pollock |first=Steven |publisher=Colorado.edu |date=2005 |access-date=2012-11-27 |archive-url=https://web.archive.org/web/20140515180200/http://www.colorado.edu/physics/phys1240/phys1240_fa05/notes/lect24_Tu11_22_4up.pdf |archive-date=2014-05-15 |url-status=dead}}</ref><ref>{{cite web |url= http://hyperphysics.phy-astr.gsu.edu/hbase/waves/string.html |title=Standing Waves on a String |publisher=Hyperphysics.phy-astr.gsu.edu |access-date=2012-11-27}}</ref><ref>{{cite web |url=http://openlearn.open.ac.uk/mod/oucontent/view.php?id=397877&section=5.13.2 |title=Creating musical sounds |work=OpenLearn |publisher=Open University |access-date=2014-06-04 |archive-date=2020-04-09 |archive-url=https://web.archive.org/web/20200409044223/https://www.open.edu/openlearn/science-maths-technology/engineering-and-technology/technology/creating-musical-sounds/content-section-0 |url-status=dead }}</ref> (The second harmonic is then {{var|f}}<sub>2</sub> = 2⋅{{var|f}}<sub>1</sub>, etc.)

According to Benward and Saker's ''Music: In Theory and Practice'':<ref>Benward, Bruce and Saker, Marilyn (1997/2003). ''Music: In Theory and Practice'', Vol. I, 7th ed.; p. xiii. McGraw-Hill. {{ISBN|978-0-07-294262-0}}.</ref>
{{Blockquote|1=Since the fundamental is the lowest frequency and is also perceived as the loudest, the ear identifies it as the specific pitch of the musical tone &#91;[[harmonic spectrum]]&#93;.... The individual partials are not heard separately but are blended together by the ear into a single tone.}}

==Explanation==
All sinusoidal and many non-sinusoidal waveforms repeat exactly over time – they are periodic. The period of a waveform is the smallest positive value <math>T</math> for which the following is true:

{{block indent|1=<math> x(t) = x(t + T)\text{ for all }t \in \mathbb{R} </math>}}

Where <math>x(t)</math> is the value of the waveform <math>t</math>. This means that the waveform's values over any interval of length <math>T</math> is all that is required to describe the waveform completely (for example, by the associated [[Fourier series]]). Since any multiple of period <math>T</math> also satisfies this definition, the fundamental period is defined as the smallest period over which the function may be described completely. The fundamental frequency is defined as its reciprocal:

{{block indent|1=<math> f_0 = \frac{1}{T}</math>}}

When the units of time are seconds, the frequency is in <math>s^{-1}</math>, also known as [[Hertz]].

===Fundamental frequency of a pipe===

For a pipe of length <math>L</math> with one end closed and the other end open the wavelength of the fundamental harmonic is <math>4L</math>, as indicated by the first two animations. Hence,
{{block indent|1=<math>\lambda_0 = 4L</math>}}

Therefore, using the relation

{{block indent|1=<math> \lambda_0 = \frac{v}{f_0}</math>}}

where <math>v</math> is the speed of the wave, the fundamental frequency can be found in terms of the speed of the wave and the length of the pipe:

{{block indent|1=<math> f_0 = \frac{v}{4L}</math>}}

If the ends of the same pipe are now both closed or both opened, the wavelength of the fundamental harmonic becomes <math>2L</math> . By the same method as above, the fundamental frequency is found to be

{{block indent|1=<math> f_0 = \frac{v}{2L}</math>}}

==In music==
In music, the fundamental is the musical [[pitch (music)|pitch]] of a note that is perceived as the lowest [[Harmonic series (music)#Partial|partial]] present. The fundamental may be created by [[vibration]] over the full length of a string or air column, or a higher harmonic chosen by the player. The fundamental is one of the [[harmonic]]s. A harmonic is any member of the harmonic series, an ideal set of frequencies that are positive integer multiples of a common fundamental frequency. The reason a fundamental is also considered a harmonic is because it is 1 times itself.<ref>{{cite book |title = Music, Cognition, and Computerized Sound |author-link=John R. Pierce |last=Pierce |first=John R. |chapter=Consonance and Scales |editor-first=Perry R. |editor-last=Cook |publisher=[[MIT Press]] |date=2001 |isbn=978-0-262-53190-0 |chapter-url= https://books.google.com/books?id=L04W8ADtpQ4C&q=musical+tone+harmonic+partial+fundamental+integer&pg=PA169}}</ref>

The fundamental is the frequency at which the entire wave vibrates. Overtones are other sinusoidal components present at frequencies above the fundamental. All of the frequency components that make up the total waveform, including the fundamental and the overtones, are called partials. Together they form the harmonic series. Overtones which are perfect integer multiples of the fundamental are called harmonics. When an overtone is near to being harmonic, but not exact, it is sometimes called a harmonic partial, although they are often referred to simply as harmonics. Sometimes overtones are created that are not anywhere near a harmonic, and are just called partials or inharmonic overtones.

The fundamental frequency is considered the ''first harmonic'' and the ''first partial''.  The numbering of the partials and harmonics is then usually the same; the second partial is the second harmonic, etc.  But if there are inharmonic partials, the numbering no longer coincides. Overtones are numbered as they appear {{em|above}} the fundamental. So strictly speaking, the ''first'' overtone is the ''second'' partial (and usually the ''second'' harmonic). As this can result in confusion, only harmonics are usually referred to by their numbers, and overtones and partials are described by their relationships to those harmonics.

== Mechanical systems ==
Consider a spring, fixed at one end and having a mass attached to the other; this would be a single degree of freedom (SDoF) oscillator. Once set into motion, it will oscillate at its natural frequency. For a single degree of freedom oscillator, a system in which the motion can be described by a single coordinate, the natural frequency depends on two system properties: mass and stiffness; (providing the system is undamped). The natural frequency, or fundamental frequency, {{var|ω}}<sub>0</sub>, can be found using the following equation:

{{block indent|1=<math> \omega_\mathrm{0} = \sqrt{\frac{k}{m}} \, </math>}}

where:
* {{var|k}} = [[stiffness]] of the spring
* {{var|m}} = mass
* {{var|ω}}<sub>0</sub> = natural frequency in radians per second.

To determine the natural frequency in Hz, the omega value is divided by 2{{var|[[Pi|π]]}}. 
Or:

{{block indent|1=<math>f_\mathrm{0} = \frac{1}{2\pi} \sqrt{\frac{k}{m}} \,</math>}}

where:
* {{var|f}}<sub>0</sub> = natural frequency (SI unit: hertz)
* {{var|k}} = stiffness of the spring (SI unit: newtons/metre or N/m)
* {{var|m}} = mass (SI unit: kg).

While doing a [[modal analysis]], the frequency of the 1st mode is the fundamental frequency.

This is also expressed as:

{{block indent|1=<math>f_\mathrm{0} = \frac{1}{2l} \sqrt{\frac{T}{\mu}} \,</math>}}

where:
* {{var|f}}<sub>0</sub> = natural frequency (SI unit: hertz)
* {{var|l}} = length of the string (SI unit: metre)
* {{var|μ}} = mass per unit length of the string (SI unit: kg/m)
* {{var|T}} = tension on the string (SI unit: newton)<ref>{{Cite web|url=https://www.wirestrungharp.com/material/strings/about_string_calculator/|title=About the String Calculator|website=www.wirestrungharp.com}}</ref>

==See also==
*[[Greatest common divisor]]
*[[Hertz]]
*[[Missing fundamental]]
*[[Natural frequency]]
*[[Oscillation]]
*[[Harmonic series (music)#Terminology]]
*[[Pitch detection algorithm]]
*[[Scale of harmonics]]

==References==
{{Reflist}}

{{Acoustics}}
{{Strings (music)}}
{{Timbre}}
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[[Category:Musical tuning]]
[[Category:Acoustics]]
[[Category:Fourier analysis]]
[[Category:Spectrum (physical sciences)]]