diff options
author | LordMcFungus <mceagle117@gmail.com> | 2021-03-22 18:05:11 +0100 |
---|---|---|
committer | GitHub <noreply@github.com> | 2021-03-22 18:05:11 +0100 |
commit | 76d2d77ddb2bed6b7c6b8ec56648d85da4103ab7 (patch) | |
tree | 11b2d41955ee4bfa0ae5873307c143f6b4d55d26 /vorlesungen/slides/8/fourier.tex | |
parent | more chapter structure (diff) | |
parent | add title image (diff) | |
download | SeminarMatrizen-76d2d77ddb2bed6b7c6b8ec56648d85da4103ab7.tar.gz SeminarMatrizen-76d2d77ddb2bed6b7c6b8ec56648d85da4103ab7.zip |
Merge pull request #1 from AndreasFMueller/master
update
Diffstat (limited to 'vorlesungen/slides/8/fourier.tex')
-rw-r--r-- | vorlesungen/slides/8/fourier.tex | 83 |
1 files changed, 83 insertions, 0 deletions
diff --git a/vorlesungen/slides/8/fourier.tex b/vorlesungen/slides/8/fourier.tex new file mode 100644 index 0000000..86d8086 --- /dev/null +++ b/vorlesungen/slides/8/fourier.tex @@ -0,0 +1,83 @@ +% +% fourier.tex +% +% (c) 2021 Prof Dr Andreas Müller, OST Ostschweizer Fachhochschule +% +\begin{frame}[t] +\setlength{\abovedisplayskip}{5pt} +\setlength{\belowdisplayskip}{5pt} +\frametitle{Fourier-Transformation} +\vspace{-20pt} +\begin{columns}[t,onlytextwidth] +\begin{column}{0.48\textwidth} +\begin{block}{Algebra} +Die Laplace-Matrix eines Graphen ist symmetrisch +\uncover<2->{% + +$\Rightarrow$ +Es gibt eine Basis aus Eigenvektoren $g_i\in\mathbb{R}^n$ von $L(G)$: +\begin{align*} +L(G)g_i&=\lambda_i g_i +\end{align*}} +\end{block} +\uncover<12->{% +\vspace{-20pt} +\begin{block}{Fourier-Transformation} +Jedes $f\in\mathbb{R}^n$ kann durch die $g_i$ ausgedrückt werden +\begin{align*} +\uncover<13->{ +f&= a_1 g_1 + \dots + a_n g_n +} +\\ +\uncover<14->{ +&= \hat{f}_1 g_1 + \dots + \hat{f}_ng_n = \sum_{k=1}^n \hat{f}_kg_k +} +\end{align*} +\uncover<15->{% +Zerlegung nach Zeitkonstante $\lambda_i$ +} +\end{block}} +\end{column} +\begin{column}{0.48\textwidth} +\uncover<3->{% +\begin{block}{Anwendung} +Wärmeleitungsgleichung +\begin{align*} +\uncover<4->{ +\frac{d}{dt}f &= L(G) f +} +\intertext{\uncover<5->{{\usebeamercolor[fg]{title}Ansatz:}}} +\uncover<6->{ +f&=a_1g_1T_1(t)+\dots + a_ng_nT_n(t) +} +\\ +\uncover<7->{ +\frac{d}{dt}f +&= +a_1g_1\dot{T}_1(t) + \dots + a_1g_1 \dot{T}_n(t) +} +\\ +\uncover<8->{ +&= +a_1Lg_1 + \dots + a_nLg_n +} +\\ +\uncover<9->{ +&= +a_1\lambda_1 g_1 + \dots + a_n\lambda_n g_n +} +\\ +\uncover<10->{ +\dot{T}_i(t) &= \lambda_i T_i(t) +} +\uncover<11->{ +\quad +\Rightarrow +\quad +T_i(t) = e^{\lambda_it} \uncover<-9>{T_i(0)} +} +\end{align*} +\end{block}} +\end{column} +\end{columns} +\end{frame} |