summaryrefslogtreecommitdiffstats
path: root/Fourier Series.page
diff options
context:
space:
mode:
authorsiveshs <siveshs@gmail.com>2010-07-02 03:24:56 +0000
committerbnewbold <bnewbold@adelie.robocracy.org>2010-07-02 03:24:56 +0000
commit99524349daae12733b5d48fb220c1d5b551219c6 (patch)
tree77740b933fe821963aeed35ef7fd0f30150317b0 /Fourier Series.page
parentbd74caeb943c803ea175aed89e059e2fd6743781 (diff)
downloadafterklein-wiki-99524349daae12733b5d48fb220c1d5b551219c6.tar.gz
afterklein-wiki-99524349daae12733b5d48fb220c1d5b551219c6.zip
still testing
Diffstat (limited to 'Fourier Series.page')
-rw-r--r--Fourier Series.page8
1 files changed, 4 insertions, 4 deletions
diff --git a/Fourier Series.page b/Fourier Series.page
index c90f37e..ad3c6d8 100644
--- a/Fourier Series.page
+++ b/Fourier Series.page
@@ -7,10 +7,10 @@ To show that Fourier series is plausible, let us consider some arbitrary trignom
$1. \cos(2x) = 1 - 2 \sin^2(x)$
$$\begin{array}{ccl}
-e^{iy} = 1+iy+\frac{(iy)^{2}}{2!}+\frac{(iy)^{3}}{3!}+\frac{(iy)^{4}}{4!}+\frac{(iy)^{5}}{5!}+\cdots\\
- = 1+iy-\frac{y^{2}}{2!}-i\frac{y^{3}}{3!}+\frac{y^{4}}{4!}+i\frac{y^{5}}{5!}+\cdots\\
- = (1-\frac{y^{2}}{2!}+\frac{y^{4}}{4!}+\cdots)+i(y-\frac{y^{3}}{3!}+\frac{y^{5}}{5!}-\cdots)\\
- = \cos y+i\sin y\end{array}$$
+e^{iy} & = 1+iy+\frac{(iy)^{2}}{2!}+\frac{(iy)^{3}}{3!}+\frac{(iy)^{4}}{4!}+\frac{(iy)^{5}}{5!}+\cdots\\
+ & = 1+iy-\frac{y^{2}}{2!}-i\frac{y^{3}}{3!}+\frac{y^{4}}{4!}+i\frac{y^{5}}{5!}+\cdots\\
+ & = (1-\frac{y^{2}}{2!}+\frac{y^{4}}{4!}+\cdots)+i(y-\frac{y^{3}}{3!}+\frac{y^{5}}{5!}-\cdots)\\
+ & = \cos y+i\sin y\end{array}$$
##What is the Fourier series actually?</b>