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author | siveshs <siveshs@gmail.com> | 2010-07-03 05:30:53 +0000 |
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committer | bnewbold <bnewbold@adelie.robocracy.org> | 2010-07-03 05:30:53 +0000 |
commit | 860a88ac4a6b4cd50f32f00ea77e6b98c5535dfb (patch) | |
tree | df7537738e537ab679cb17464d7d6f1ea4eee24f | |
parent | 8c7d2e6af68b04e0e33842c2aa052c20dcfb0506 (diff) | |
download | afterklein-wiki-860a88ac4a6b4cd50f32f00ea77e6b98c5535dfb.tar.gz afterklein-wiki-860a88ac4a6b4cd50f32f00ea77e6b98c5535dfb.zip |
editing
-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 8010928..06e2d9b 100644 --- a/Fourier Series.page +++ b/Fourier Series.page @@ -13,7 +13,7 @@ We first begin with a few basic identities on the size of sets. Then, we will sh ## Proof that no. of available functions is greater than number of functions required to define the periodic function Consider any arbitrary periodic function in the interval $[-\pi,\pi]$. This can be represented as a series of values at various points in the interval. For example, -$ f(0) = ... , f(0.1) = ..., f(0.2) = ... $ and so on. At each point, we can assign any real number (i.e. $\in \mathbb R$). So, the number of possible periodic functions in an interval is of the order of $\mathbb R^{\mathbb R}$. +$\qquad f(0) = ... , f(0.1) = ..., f(0.2) = ... $ and so on. At each point, we can assign any real number (i.e. $\in \mathbb R$). So, the number of possible periodic functions in an interval is of the order of $\mathbb R^{\mathbb R}$. --> don't quite remember how this goes. #<b>Why Fourier decomposition is plausible?</b> |