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author | joshuab <> | 2010-07-12 22:40:45 +0000 |
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committer | bnewbold <bnewbold@adelie.robocracy.org> | 2010-07-12 22:40:45 +0000 |
commit | 93ee966ec05bc1ce36db9eb21ff073ed46c4f775 (patch) | |
tree | 643377f2603dc2d539b6da6a0a1fd5be7ed9a465 | |
parent | 3691af780fe86b90c4e52c4c6124a8b2dd58d8a3 (diff) | |
download | afterklein-wiki-93ee966ec05bc1ce36db9eb21ff073ed46c4f775.tar.gz afterklein-wiki-93ee966ec05bc1ce36db9eb21ff073ed46c4f775.zip |
typo fixed
-rw-r--r-- | ClassJune28.page | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/ClassJune28.page b/ClassJune28.page index 1934c8e..6359933 100644 --- a/ClassJune28.page +++ b/ClassJune28.page @@ -205,7 +205,7 @@ 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, -$$ a_m = \int_0^{2\pi} \, f \, \frac{1}{\sqrt{2\pi}} \, e^ {-inx} \, dx $$ +$$ a_m = \int_0^{2\pi} \, f \, \frac{1}{\sqrt{2\pi}} \, e^ {-imx} \, dx $$ This is the common definition for the terms of the Fourier series. |