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| author | siveshs <siveshs@gmail.com> | 2010-07-03 04:54:25 +0000 |
|---|---|---|
| committer | bnewbold <bnewbold@adelie.robocracy.org> | 2010-07-03 04:54:25 +0000 |
| commit | d547404c5ae2e7de36ed13b80b997b98aaf8a515 (patch) | |
| tree | fc01b600ac136bbeb5c8e9a69fb7dc8b032e1e9f /Fourier Series.page | |
| parent | a6d372bdff0c016d8afdae72f911804fedbc0fd0 (diff) | |
| download | afterklein-wiki-d547404c5ae2e7de36ed13b80b997b98aaf8a515.tar.gz afterklein-wiki-d547404c5ae2e7de36ed13b80b997b98aaf8a515.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 d87cc22..0909384 100644 --- a/Fourier Series.page +++ b/Fourier Series.page @@ -173,7 +173,7 @@ Due to orthonormality of basis vectors, the inner product in the right-hand side Thus, $$ (f, f_m) = a_m $$ Using the definition of the inner product, -$$ a_m = \int_0^{2\pi} \, f \, \frac{1}{sqrt{2\pi}} \, e^ {-inx} \, dx $$ +$$ a_m = \int_0^{2\pi} \, f \, \frac{1}{\sqrt{2\pi}} \, e^ {-inx} \, dx $$ This is the common definition for the terms of the Fourier series. |