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> | ||
| − | Fourier series can be generalized to [[Fourier transformation]]s for | + | 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.