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vpde_lecture20 [2020/03/19 15:50] trinh [Fourier series for even and odd- extensions] |
vpde_lecture20 [2020/03/20 19:19] trinh |
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====== MA20223 Lecture 20 ====== | ====== MA20223 Lecture 20 ====== | ||
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+ | < | ||
+ | <iframe width=" | ||
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==== Fourier convergence theorem ==== | ==== Fourier convergence theorem ==== | ||
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$$ | $$ | ||
is the odd extension. | is the odd extension. | ||
+ | |||
+ | Once you have drawn (or derived) the extension, then it becomes a simple matter to calculate the Fourier series. For example, since $f_e(x)$ is an even function then only cosines are present, and | ||
+ | $$ | ||
+ | f_e(x) \sim \frac{a_0}{2} + \sum_{n=1}^\infty a_n \cos(nx), | ||
+ | $$ | ||
+ | where | ||
+ | $$ | ||
+ | a_n = \frac{2}{\pi} \int_0^\pi x^2 \cos(nx) \, \mathrm{d}x. | ||
+ | $$ | ||
+ | Above, we have used the even property to double up the integral over the positive $x$ values. Similarly, the Fourier series for the odd extension is | ||
+ | $$ | ||
+ | f_o(x) \sim \sum_{n=1}^\infty b_n \sin(nx), | ||
+ | $$ | ||
+ | where | ||
+ | $$ | ||
+ | b_n = \frac{2}{\pi} \int_0^\pi x^2 \sin(nx) \, \mathrm{d}x. | ||
+ | $$ |