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{{Short description|Special cases of the Fourier series}}
In mathematics, particularly the field of [[calculus]] and [[Fourier analysis]], the '''Fourier sine and cosine series''' are two [[mathematical series]] named after [[Joseph Fourier]].
{{distinguish-redirect|Sine and cosine series|Sine and cosine#Series definitions}}

In [[mathematics]], particularly the field of [[calculus]] and [[Fourier analysis]], the '''Fourier sine and cosine series''' are two [[mathematical series]] named after [[Joseph Fourier]].


==Notation==
==Notation==
In this article, ''f'' denotes a real valued function on <math>\mathbb{R}</math> which is periodic with period 2''L''.
In this article, {{math|''f''}} denotes a [[real number|real]]-valued [[function (mathematics)|function]] on <math>\mathbb{R}</math> which is [[periodic function|periodic]] with period 2''L''.


==Sine series==
==Sine series==
If f(x) is an [[odd function]], then the Fourier sine series of f is defined to be
If {{math|''f''}} is an [[odd function]] with period <math>2L</math>, then the Fourier Half Range sine series of ''f'' is defined to be
<math display="block">f(x) = \sum_{n=1}^\infty b_n \sin \left(\frac{n\pi x}{L}\right) </math>
which is just a form of complete [[Fourier series]] with the only difference that <math>a_0</math> and <math>a_n</math> are zero, and the series is defined for half of the [[interval (mathematics)|interval]].


In the formula we have
:<math> f(x) = \sum_{n=1}^\infty b_n \sin \frac{n\pi x}{L}</math>
<math display="block">b_n = \frac{2}{L} \int_0^L f(x) \sin \left(\frac{n\pi x}{L}\right) \, dx, \quad n \in \mathbb{N} .</math>
which ia juat a form of completw fourier series with the only difference that <math> a_0 </math> and <math> a_nn </math> is zero, and the series is defined for half of the interval.

In the formula we have ....
:<math>b_n=\frac{2}{L}\int_0^L f(x) \sin \frac{n\pi x}{L} \, dx, n\in \mathbb{N}</math>.


==Cosine series==
==Cosine series==
If f(x) is an [[even function]], then the Fourier cosine series is defined to be
If {{math|''f''}} is an [[even function]] with a period <math>2L</math>, then the Fourier cosine series is defined to be
<math display="block">f(x) = \frac{a_0}{2} + \sum_{n=1}^{\infty} a_n \cos \left(\frac{n \pi x}{L}\right) </math>

:<math> f(x)=\frac{c_0}{2} + \sum_{n=1}^\infty c_n \cos \frac{n\pi x}{L}</math>
where
where
:<math>c_n=\frac{2}{L}\int_0^L f(x) \cos \frac{n\pi x}{L} \, dx, n\in \mathbb{N}_0</math>.
<math display="block">a_n = \frac{2}{L} \int_0^L f(x) \cos \left(\frac{n\pi x}{L}\right) \, dx, \quad n \in \mathbb{N}_0 .</math>


==Remarks==
==Remarks==
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*[[Fourier series]]
*[[Fourier series]]
*[[Fourier analysis]]
*[[Fourier analysis]]
*[[Least-squares spectral analysis]]


==Bibliography==
==Bibliography==

Latest revision as of 13:17, 2 November 2024

In mathematics, particularly the field of calculus and Fourier analysis, the Fourier sine and cosine series are two mathematical series named after Joseph Fourier.

Notation

[edit]

In this article, f denotes a real-valued function on which is periodic with period 2L.

Sine series

[edit]

If f is an odd function with period , then the Fourier Half Range sine series of f is defined to be which is just a form of complete Fourier series with the only difference that and are zero, and the series is defined for half of the interval.

In the formula we have

Cosine series

[edit]

If f is an even function with a period , then the Fourier cosine series is defined to be where

Remarks

[edit]

This notion can be generalized to functions which are not even or odd, but then the above formulas will look different.

See also

[edit]

Bibliography

[edit]
  • Byerly, William Elwood (1893). "Chapter 2: Development in Trigonometric Series". An Elementary Treatise on Fourier's Series: And Spherical, Cylindrical, and Ellipsoidal Harmonics, with Applications to Problems in Mathematical Physics (2 ed.). Ginn. p. 30.
  • Carslaw, Horatio Scott (1921). "Chapter 7: Fourier's Series". Introduction to the Theory of Fourier's Series and Integrals, Volume 1 (2 ed.). Macmillan and Company. p. 196.