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Fourier sine and cosine series
Special cases of the Fourier series
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.
Notation
In this article, f denotes a real-valued function on \mathbb{R} which is periodic with period 2L.
Sine series
If f is an odd function with period 2L, then the Fourier Half Range sine series of f is defined to be f(x) = \sum_{n=1}^\infty b_n \sin \left(\frac{n\pi x}{L}\right) which is just a form of complete Fourier series with the only difference that a_0 and a_n are zero, and the series is defined for half of the interval.
In the formula we have b_n = \frac{2}{L} \int_0^L f(x) \sin \left(\frac{n\pi x}{L}\right) , dx, \quad n \in \mathbb{N} .
Cosine series
If f is an even function with a period 2L, then the Fourier cosine series is defined to be
f(x) = \frac{a_0}{2} + \sum_{n=1}^{\infty} a_n \cos \left(\frac{n \pi x}{L}\right)
where
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 .
Remarks
This notion can be generalized to functions which are not even or odd, but then the above formulas will look different.
Bibliography
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