Fourier series: Difference between revisions

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==The Fourier Series==
==The Fourier Series==
A Fourier series is an expansion of a periodic function f(x) in terms of an infinite sum of sines and cosines. Fourier series make use of the orthogonality relationships of the sine and cosine functions.
A Fourier series is an expansion of a periodic function <math>f</math> in terms of an infinite sum of sines and cosines. Fourier series make use of the orthogonality relationships of the sine and cosine functions.


[[Orthogonal Functions]])
[[Orthogonal Functions]]


Principle author of this page:  [[User:Goeari|Aric Goe]]
Principle author of this page:  [[User:Goeari|Aric Goe]]

Revision as of 21:51, 27 October 2004

Diriclet Conditions

The conditions for a periodic function f with period 2L to have a convergent Fourier series.

Theorem:

Let f be a piecewise regular real-valued function defined on some interval [-L,L], such that f has only a finite number of discontinuities and extrema in [-L,L]. Then the Fourier series of this function converges to f when f is continuous and to the arithmetic mean of the left-handed and right-handed limit of f at a point where it is discontinuous.

The Fourier Series

A Fourier series is an expansion of a periodic function f in terms of an infinite sum of sines and cosines. Fourier series make use of the orthogonality relationships of the sine and cosine functions.

Orthogonal Functions

Principle author of this page: Aric Goe