Difference between revisions of "Fourier series"

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:<math>b_n = \frac{2}{T} \int_{t_1}^{t_2} f(t) \sin(\omega_n t)\, dt </math>
 
:<math>b_n = \frac{2}{T} \int_{t_1}^{t_2} f(t) \sin(\omega_n t)\, dt </math>
  
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Fourier series can be generalized to [[Fourier transformation]]s for non-perodic, piecewise continuous, [[square integrable function]]s.
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Fourier series can be generalized to [[Fourier transformation]]s for other classes of functions, for instance [[square integrable function]]s.
  
 
[[category: mathematics]]
 
[[category: mathematics]]

Revision as of 14:53, August 22, 2008

Fourier series express a piecewise continuous, bounded, periodic function as a linear combination of orthogonal sine and cosine functions.

The Fourier series of a function f(t) is of the form:

where, n is an integer and

Fourier series can be generalized to Fourier transformations for other classes of functions, for instance square integrable functions.