Mehr Folien und einige Typos.

7 files changed, 428 insertions, 53 deletions

diff --git a/vorlesungen/08_dgl/Makefile b/vorlesungen/08_dgl/Makefile
index 613a5d9..f646db6 100644
--- a/vorlesungen/08_dgl/Makefile
+++ b/vorlesungen/08_dgl/Makefile
@@ -5,15 +5,28 @@
 #
 all:	dgl-handout.pdf MathSem-08-dgl.pdf
 
+# SHELL = /bin/bash
+
 include ../slides/Makefile.inc
 
 SOURCES = common.tex slides.tex $(slides)
+IMAGES = vektorfelder-1.pdf
+
+
+MathSem-08-dgl.pdf:	MathSem-08-dgl.tex $(SOURCES) $(IMAGES)
+	pdflatex MathSem-08-dgl.tex > /dev/null
 
-MathSem-08-dgl.pdf:	MathSem-08-dgl.tex $(SOURCES)
-	pdflatex MathSem-08-dgl.tex
+dgl-handout.pdf:	dgl-handout.tex $(SOURCES) $(IMAGES)
+	pdflatex dgl-handout.tex > /dev/null
 
-dgl-handout.pdf:	dgl-handout.tex $(SOURCES)
-	pdflatex dgl-handout.tex
+vektorfelder-1.pdf: ../slides/10/vektorfelder.mp
+	cd ../slides/10/; \
+	TEX=latex mpost vektorfelder.mp; \
+	for f in vektorfelder.[0-9]*; \
+	do \
+	  mptopdf $${f} > /dev/null; \
+	done; \
+	rm -f vektorfelder.[0-9]* vektorfelder.log vektorfelder.mpx
 
 thumbnail:	thumbnail.jpg # fix1.jpg
 
diff --git a/vorlesungen/08_dgl/slides.tex b/vorlesungen/08_dgl/slides.tex
index db4e27c..48b01ff 100644
--- a/vorlesungen/08_dgl/slides.tex
+++ b/vorlesungen/08_dgl/slides.tex
@@ -17,8 +17,10 @@
 % 6. Strömungslinien = Pfade für Lie-Theorie, A lokal, exp(Ax) global
 % 7. Beispiele so(2), Jordan-Block, vielleicht [0 1; 1 0]
 
-%\folie{10/taylor.tex}
+\folie{10/taylor.tex}
+\folie{5/potenzreihenmethode.tex}
 \folie{10/n-zu-1.tex}
-%\folie{5/potenzreihenmethode.tex}
+\folie{10/matrix-vektor-dgl.tex}
+\folie{10/so2.tex}
 
-%\folie{10/eindimensional.tex}
\ No newline at end of file
+%\folie{10/eindimensional.tex}
diff --git a/vorlesungen/slides/10/matrix-vektor-dgl.tex b/vorlesungen/slides/10/matrix-vektor-dgl.tex
index d9bd97c..f7bd995 100644
--- a/vorlesungen/slides/10/matrix-vektor-dgl.tex
+++ b/vorlesungen/slides/10/matrix-vektor-dgl.tex
@@ -6,50 +6,6 @@
 %
 % !TeX spellcheck = de_CH
 \bgroup
-%\begin{frame}[t]
-%\setlength{\abovedisplayskip}{5pt}
-%\setlength{\belowdisplayskip}{5pt}
-%\frametitle{Matrix-Vektor-DGL}
-%\vspace{-20pt}
-%\begin{columns}[t,onlytextwidth]
-%\begin{column}{0.48\textwidth}
-%  \begin{block}{Bekannt}
-%    Vorgehen für DGL 1.~Ordnung mit Skalaren.
-%    Aufgabe: Sei $a, x, x_0 \in \mathbb R$, 
-%    \[
-%      \dot x = ax,
-%      \quad 
-%      x(0) = x_0
-%    \]
-%    Lösung: $x(t) = \exp(at) x_0$, wobei
-%    \begin{align*}
-%      \exp(at)
-%      &= 1 + at + \frac{a^2t^2}{2!} + \ldots\\
-%      &= e^{at}
-%    \end{align*}
-%  \end{block}
-%\end{column}
-%\begin{column}{0.48\textwidth}
-%  \begin{block}{Mit Matrizen}
-%    Wir können:
-%    \begin{itemize}
-%      \item Matrizen potenzieren: $A$, $A^2$, $A^3$
-%      \item Matrizen skalieren: $At$
-%      \item Matrizen addieren: $A_1 + A_2$
-%    \end{itemize}
-%    Also ist auch
-%    \[
-%    \exp(At) = 1 + At + \frac{A^2t^2}{2!} + \ldots
-%    \]
-%    wohldefiniert.
-%  \end{block}
-%\end{column}
-%\end{columns}
-%Folglich, sei $A \in M_n$ und $x \in \mathbb R^n$,
-%\[ \dot x = Ax, \quad x(0) = x_0, \]
-%dann ist
-%\[ x = \exp(At)x_0. \]
-%\end{frame}
 
 \begin{frame}[t]
   \setlength{\abovedisplayskip}{5pt}
diff --git a/vorlesungen/slides/10/so2.tex b/vorlesungen/slides/10/so2.tex
new file mode 100644
index 0000000..e3f74ae
--- /dev/null
+++ b/vorlesungen/slides/10/so2.tex
@@ -0,0 +1,138 @@
+%
+% so2.tex -- Illustration of so(2) -> SO(2)
+%
+% (c) 2021 Prof Dr Andreas Müller, OST Ostschweizer Fachhochschule
+% Erstellt durch Roy Seitz
+%
+% !TeX spellcheck = de_CH
+\bgroup
+
+\newcommand{\gSL}[2]{\ensuremath{\text{SL}(#1, \mathbb{#2})}}
+\newcommand{\gSO}[1]{\ensuremath{\text{SO}(#1)}}
+\newcommand{\gGL}[2]{\ensuremath{\text{GL}(#1, \mathbb #2)}}
+
+\newcommand{\asl}[2]{\ensuremath{\mathfrak{sl}(#1, \mathbb{#2})}}
+\newcommand{\aso}[1]{\ensuremath{\mathfrak{so}(#1)}}
+\newcommand{\agl}[2]{\ensuremath{\mathfrak{gl}(#1, \mathbb #2)}}
+
+\begin{frame}[t]
+\setlength{\abovedisplayskip}{5pt}
+\setlength{\belowdisplayskip}{5pt}
+\frametitle{Von der Lie-Gruppe zur -Algebra}
+\vspace{-20pt}
+\begin{columns}[t,onlytextwidth]
+\begin{column}{0.48\textwidth}
+  \begin{block}{Lie-Gruppe}
+    Darstellung von \gSO2:
+    \begin{align*}
+      \mathbb R 
+      &\to 
+      \gSO2
+      \\
+      t
+      &\mapsto
+      \begin{pmatrix}
+        \cos t &         -\sin t \\ 
+        \sin t & \phantom-\cos t
+      \end{pmatrix}
+    \end{align*}
+  \end{block}
+  \begin{block}{Ableitung am neutralen Element}
+    \begin{align*}
+    \frac{d}{d t}
+    &
+    \left.
+    \begin{pmatrix}
+      \cos t &         -\sin t \\ 
+      \sin t & \phantom-\cos t
+    \end{pmatrix}
+    \right|_{ t = 0}
+    \\
+    =
+    & 
+    \begin{pmatrix} -\sin0 & -\cos0 \\ \phantom-\cos0 & -\sin0 \end{pmatrix}
+    = 
+    \begin{pmatrix} 0 & -1 \\ 1 &  \phantom-0 \end{pmatrix}
+    \end{align*}
+  \end{block}
+\end{column}
+\begin{column}{0.48\textwidth}
+  \begin{block}{Lie-Algebra}
+    Darstellung von \aso2:
+    \begin{align*}
+      \mathbb R 
+      &\to 
+      \aso2
+      \\
+      t
+      &\mapsto
+      \begin{pmatrix}
+        0 &         -t \\ 
+        t & \phantom-0
+      \end{pmatrix}
+    \end{align*}
+  \end{block}
+\end{column}
+\end{columns}
+\end{frame}
+
+
+\begin{frame}[t]
+\setlength{\abovedisplayskip}{5pt}
+\setlength{\belowdisplayskip}{5pt}
+\frametitle{Von der Lie-Algebra zur -Gruppe}
+\vspace{-20pt}
+\begin{columns}[t,onlytextwidth]
+\begin{column}{0.48\textwidth}
+  \begin{block}{Differentialgleichung}
+    Gegeben:
+    \[
+    A
+    =
+    \dot\gamma(0) = \begin{pmatrix} 0 & -1 \\ 1 & \phantom-0 \end{pmatrix}
+    \]
+    Gesucht:
+    \[ \dot \gamma (t) = \gamma(t) A \qquad \gamma \in \gSO2 \]
+    \[ \Rightarrow \gamma(t) = \exp(At) \gamma(0) = \exp(At) \]
+  \end{block}
+\end{column}
+\begin{column}{0.48\textwidth}
+  \begin{block}{Lie-Algebra}
+    Potenzen von A:
+    \begin{align*}
+      A^2 &= -I &
+      A^3 &= -A &
+      A^4 &=  I &
+      \ldots
+    \end{align*}
+  \end{block}
+\end{column}
+\end{columns}
+Folglich:
+\begin{align*}
+  \exp(At)
+  &= I + At 
+  + A^2\frac{t^2}{2!} 
+  + A^3\frac{t^3}{3!}
+  + A^4\frac{t^4}{4!}
+  + A^5\frac{t^5}{5!}
+  + \ldots \\
+  &= \begin{pmatrix}
+    \vspace*{3pt}
+    1 - \frac{t^2}{2} + \frac{t^4}{4!} - \ldots
+    &
+    -t + \frac{t^3}{3!} - \frac{t^5}{5!} + \ldots
+    \\ 
+    t - \frac{t^3}{3!} + \frac{t^5}{5!} - \ldots
+    &
+    1 - \frac{t^2}{2!} + \frac{t^4}{4!} - \ldots
+  \end{pmatrix}
+  =
+  \begin{pmatrix}
+    \cos t &         -\sin t \\ 
+    \sin t & \phantom-\cos t
+  \end{pmatrix}
+\end{align*}
+
+\end{frame}
+\egroup
diff --git a/vorlesungen/slides/10/taylor.tex b/vorlesungen/slides/10/taylor.tex
index bbd1126..920470f 100644
--- a/vorlesungen/slides/10/taylor.tex
+++ b/vorlesungen/slides/10/taylor.tex
@@ -1,5 +1,5 @@
 %
-% eindiomensional.tex -- Lösung der eindimensionalen DGL
+% taylor.tex -- Repetition Taylot-Reihen
 %
 % (c) 2021 Prof Dr Andreas Müller, OST Ostschweizer Fachhochschule
 % Erstellt durch Roy Seitz
diff --git a/vorlesungen/slides/10/vektorfelder.mp b/vorlesungen/slides/10/vektorfelder.mp
new file mode 100644
index 0000000..f488327
--- /dev/null
+++ b/vorlesungen/slides/10/vektorfelder.mp
@@ -0,0 +1,266 @@
+%
+% Stroemungsfelder linearer Differentialgleichungen
+%
+% (c) 2015 Prof Dr Andreas Mueller, Hochschule Rapperswil
+% 2021-04-14, Roy Seitz, Copied for SeminarMatrizen
+%
+verbatimtex
+\documentclass{book}
+\usepackage{times}
+\usepackage{amsmath}
+\usepackage{amssymb}
+\usepackage{amsfonts}
+\usepackage{txfonts}
+\begin{document}
+etex;
+
+input TEX;
+
+TEXPRE("%&latex" & char(10) &
+"\documentclass{book}" &
+"\usepackage{times}" &
+"\usepackage{amsmath}" &
+"\usepackage{amssymb}" &
+"\usepackage{amsfonts}" &
+"\usepackage{txfonts}" &
+"\begin{document}");
+TEXPOST("\end{document}");
+
+%
+% Vektorfeld in der Ebene mit Lösungskurve
+% so(2)
+%
+beginfig(1)
+
+% Scaling parameter
+numeric unit;
+unit := 150;
+
+% Some points
+z1 = (-1.5,    0) * unit;
+z2 = ( 1.5,    0) * unit;
+z3 = (   0, -1.5) * unit;
+z4 = (   0,  1.5) * unit;
+
+pickup pencircle scaled 1pt;
+drawarrow (z1 shifted (-10,0))--(z2 shifted (10,0));
+drawarrow (z3 shifted (0,-10))--(z4 shifted (0,10));
+label.top(btex $x_1$ etex, z2 shifted (10,0));
+label.rt(btex $x_2$ etex, z4 shifted (0,10));
+
+% Draw circles
+for x = 0.2 step 0.2 until 1.4:
+  path p;
+  p = (x,0);
+  for a = 5 step 5 until 355:
+    p := p--(x*cosd(a), x*sind(a));
+  endfor;
+  p := p--cycle;
+  pickup pencircle scaled 1pt;
+  draw p scaled unit withcolor red;
+endfor;
+
+% Define DGL
+def dglField(expr x, y) =
+  %(-0.5 * (x + y), -0.5 * (y - x))
+  (-y, x)
+enddef;
+
+% Draw arrows for each grid point
+pickup pencircle scaled 0.5pt;
+for x = -1.5 step 0.1 until 1.55:
+  for y = -1.5 step 0.1 until 1.55:
+    drawarrow ((x, y) * unit)
+      --(((x,y) * unit) shifted (8 * dglField(x,y)))
+        withcolor blue;
+  endfor;
+endfor;
+
+endfig;
+
+
+
+%
+% Vektorfeld in der Ebene mit Lösungskurve
+% X \in sl(2, R)
+%
+beginfig(2)
+
+numeric unit;
+unit := 150;
+
+z0 = (   0,    0);
+z1 = (-1.5,    0) * unit;
+z2 = ( 1.5,    0) * unit;
+z3 = (   0, -1.5) * unit;
+z4 = (   0,  1.5) * unit;
+
+pickup pencircle scaled 1pt;
+drawarrow (z1 shifted (-10,0))--(z2 shifted (10,0));
+drawarrow (z3 shifted (0,-10))--(z4 shifted (0,10));
+label.top(btex $x_1$ etex, z2 shifted (10,0));
+label.rt(btex $x_2$ etex, z4 shifted (0,10));
+
+% Draw flow lines
+for y = -1.4 step 0.2 until 1.4:
+  path p;
+  p = (-1.5,y) -- (1.5, y);
+  pickup pencircle scaled 1pt;
+  draw p scaled unit withcolor red;
+endfor;
+
+def dglField(expr x, y) =
+  (y, 0)
+enddef;
+
+% Draw arrows for each grid point
+pickup pencircle scaled 0.5pt;
+for x = -1.5 step 0.1 until 1.55:
+  for y = -1.5 step 0.1 until 1.55:
+    drawarrow ((x, y) * unit)
+      --(((x,y) * unit) shifted (8 * dglField(x,y)))
+        withcolor blue;
+  endfor;
+endfor;
+
+endfig;
+
+
+
+
+%
+% Vektorfeld in der Ebene mit Lösungskurve
+% Y \in sl(2, R)
+%
+beginfig(3)
+
+numeric unit;
+unit := 150;
+
+z0 = (   0,    0);
+z1 = (-1.5,    0) * unit;
+z2 = ( 1.5,    0) * unit;
+z3 = (   0, -1.5) * unit;
+z4 = (   0,  1.5) * unit;
+
+pickup pencircle scaled 1pt;
+drawarrow (z1 shifted (-10,0))--(z2 shifted (10,0));
+drawarrow (z3 shifted (0,-10))--(z4 shifted (0,10));
+label.top(btex $x_1$ etex, z2 shifted (10,0));
+label.rt(btex $x_2$ etex, z4 shifted (0,10));
+
+% Draw flow lines
+for x = -1.4 step 0.2 until 1.4:
+  path p;
+  p = (x, -1.5) -- (x, 1.5);
+  pickup pencircle scaled 1pt;
+  draw p scaled unit withcolor red;
+endfor;
+
+def dglField(expr x, y) =
+  (0, x)
+enddef;
+
+% def dglFieldp(expr z) =
+%   dglField(xpart z, ypart z)
+% enddef;
+% 
+% def curve(expr z, l) =
+%   path p;
+%   p := z;
+%   for t = 0 step 1 until l:
+%     p := p--((point (length p) of p) shifted (0.01 * dglFieldp(point (length p) of p)));
+%   endfor;
+%   draw p scaled unit withcolor red;
+% enddef;
+%
+% numeric outerlength;
+% outerlength = 200;
+% curve(( 0.1, 0), outerlength);
+% curve(( 0.2, 0), outerlength);
+%
+% numeric innerlength;
+% innerlength = 500;
+% 
+% for a = 0 step 30 until 330:
+%   curve(0.05 * (cosd(a), sind(a)), innerlength);
+% endfor;
+
+% Draw arrows for each grid point
+pickup pencircle scaled 0.5pt;
+for x = -1.5 step 0.1 until 1.55:
+  for y = -1.5 step 0.1 until 1.55:
+    drawarrow ((x, y) * unit)
+      --(((x,y) * unit) shifted (8 * dglField(x,y)))
+        withcolor blue;
+  endfor;
+endfor;
+
+endfig;
+
+
+%
+% Vektorfeld in der Ebene mit Lösungskurve
+% H \in sl(2, R)
+%
+beginfig(4)
+
+numeric unit;
+unit := 150;
+
+z0 = (   0,    0);
+z1 = (-1.5,    0) * unit;
+z2 = ( 1.5,    0) * unit;
+z3 = (   0, -1.5) * unit;
+z4 = (   0,  1.5) * unit;
+
+pickup pencircle scaled 1pt;
+drawarrow (z1 shifted (-25,0))--(z2 shifted (25,0));
+drawarrow (z3 shifted (0,-10))--(z4 shifted (0,10));
+label.top(btex $x_1$ etex, z2 shifted (25,0));
+label.rt(btex $x_2$ etex, z4 shifted (0,10));
+
+def dglField(expr x, y) =
+  (x, -y)
+enddef;
+
+def dglFieldp(expr z) =
+  dglField(xpart z, ypart z)
+enddef;
+
+def curve(expr z, l) =
+  path p;
+  p := z;
+  for t = 0 step 1 until l:
+    p := p--((point (length p) of p) shifted (0.01 * dglFieldp(point (length p) of p)));
+  endfor;
+  draw p scaled unit withcolor red;
+enddef;
+
+for i = -1 step 2 until 1:
+  for k = -1 step 2 until 1:
+    curve((1.3 * i,  1.5 * k), 18);
+    curve((1.1 * i,  1.5 * k), 35);
+    curve((0.9 * i,  1.5 * k), 55);
+    curve((0.7 * i,  1.5 * k), 80);
+    curve((0.5 * i,  1.5 * k), 114);
+    curve((0.3 * i,  1.5 * k), 165);
+    curve((0.1 * i,  1.5 * k), 275);
+  endfor;
+endfor;
+
+% Draw arrows for each grid point
+pickup pencircle scaled 0.5pt;
+for x = -1.5 step 0.1 until 1.55:
+  for y = -1.5 step 0.1 until 1.55:
+    drawarrow ((x, y) * unit)
+      --(((x,y) * unit) shifted (8 * dglField(x,y)))
+        withcolor blue;
+  endfor;
+endfor;
+
+endfig;
+
+
+
+end;
diff --git a/vorlesungen/slides/5/potenzreihenmethode.tex b/vorlesungen/slides/5/potenzreihenmethode.tex
index 0c3503d..12d3fa5 100644
--- a/vorlesungen/slides/5/potenzreihenmethode.tex
+++ b/vorlesungen/slides/5/potenzreihenmethode.tex
@@ -79,7 +79,7 @@ a_k=\frac1{k!}a^kC}
 \\
 \uncover<4->{
 \Rightarrow y(x) &= C}\uncover<8->{+Cax}\uncover<9->{ + C\frac12(ax)^2}
-\uncover<10->{ + C \frac16(ac)^3}
+\uncover<10->{ + C \frac16(ax)^3}
 \uncover<11->{ + \dots+C\frac{1}{k!}(ax)^k+\dots}
 \ifthenelse{\boolean{presentation}}{
 \only<12>{