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| author | siveshs <siveshs@gmail.com> | 2010-07-03 04:27:27 +0000 |
|---|---|---|
| committer | bnewbold <bnewbold@adelie.robocracy.org> | 2010-07-03 04:27:27 +0000 |
| commit | 008401b708e4b836fb17c5bc9378368e94413f83 (patch) | |
| tree | 5ea490825d3cc5861b249e463befcda527ce5c00 /Fourier Series.page | |
| parent | af054ef30a72de36df80bf21e974696ce17116a1 (diff) | |
| download | afterklein-wiki-008401b708e4b836fb17c5bc9378368e94413f83.tar.gz afterklein-wiki-008401b708e4b836fb17c5bc9378368e94413f83.zip | |
section 3 editing
Diffstat (limited to 'Fourier Series.page')
| -rw-r--r-- | Fourier Series.page | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/Fourier Series.page b/Fourier Series.page index d53530c..2c9ddd9 100644 --- a/Fourier Series.page +++ b/Fourier Series.page @@ -125,7 +125,7 @@ $$ & = & \frac{1}{2\pi} \, \int_0^{2\pi} \, e^{i(n-m)x} \, dx \\ \end{array} $$ -The exponential can be expanded using $e^{inx} = \cos nx + i \sin nx$. Then, integrating, we get the following: +The exponential can be expanded using $e^{ikx} = \cos kx + i \sin kx$. Then, integrating, we get the following: $$ \begin{array}{ccl} n = m \Rightarrow (f_n,f_m) & = & 1\\ |