diff --git a/v0.1/Graphiken/transformator.svg b/v0.1/Graphiken/transformator.svg
new file mode 100644
index 0000000000000000000000000000000000000000..3cae9d3ec520fa4c007b002126149aa29c73f90d
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diff --git a/v0.1/ac_circuit.tex b/v0.1/ac_circuit.tex
index 628bec8c28da7e1e1b9ed4bd67c945d2dc457fcb..92f27897af9138774e6f8e3caed3cef0d11c0462 100644
--- a/v0.1/ac_circuit.tex
+++ b/v0.1/ac_circuit.tex
@@ -163,7 +163,7 @@ fließen l\"asst. Wir erhalten die Differenzialgleichung f\"ur $I$:
 \ddot{I} = -\frac{1}{LC} I
 \end{equation}
 mit der Randbedingung $I(t=0)=0$ l\"asst sich diese Gleichung (harmonischer Oszillator) 
-mit dem Ansatz l\"osen $I(t)=I_0 \sin(\omega t)$. Um die Kreisfrequenz $\omega$ 
+mit dem Ansatz l\"osen $I(t)=I_0 \sin(\omega t+\alpha)$. Um die Kreisfrequenz $\omega$ 
 zu bestimmen, rechnen wir
  $$\ddot{I}=-\omega^2\,I_0\,\sin(\omega t)=-\omega^2\,I(t),$$ 
  damit ergibt sich aus dem Vergleich mit Gl.~\ref{eqn:current}
diff --git a/v0.1/figures/transformator.png b/v0.1/figures/transformator.png
new file mode 100644
index 0000000000000000000000000000000000000000..802111120be6f70e1bf4a17ddd66a47b6a9556b0
Binary files /dev/null and b/v0.1/figures/transformator.png differ
diff --git a/v0.1/induktion.tex b/v0.1/induktion.tex
index 4965977abcea126643a94365ff345e368ca3639e..bf405a900e6c6fe7c0084ccbd6a99eac2ff831df 100644
--- a/v0.1/induktion.tex
+++ b/v0.1/induktion.tex
@@ -117,7 +117,26 @@ elektromotischen Kraft (EMK) in einigen Lehrbüchern.
  weiter verstärkt. Das würde wiederum einen größeren Strom induzieren. 
 Eine sich in dieser Weise selbst-verstärkende Reaktion nennen wir auch Instabilität.
 
+
+
 \textbf{Demonstrationsexperiment: Lenz'sche Regel mit Ring-Kanone, Gauss-Kanone}
+
+\section{Generator}
+\label{section:generator}
+Ein zeitlich sich ändernder magnetischer Fluss erzeugt eine induzierte Spannung. Die technische wichtigste Nutzung ist der Generator, bei
+dem wir Bewegungsenergie in elektrische Energie umwandeln. Der einfachste Wechselstromgenerator besteht aus einer drehbaren Spule in einem
+äußeren Magnetfeld $B$ (z.B. ein Hufeisenmagnet). Wenn sich die Spule  mit $N$ Windungen und der Fläche $A$ im äußeren Magnetfeld dreht, 
+wird der magnetische Fluss durch
+die rotierende Fläche, die von der Spule aufgespannt wird, periodisch mit der Kreisfrequenz $\omega$ moduliert:
+\[ 
+ \varphi_m = NBA\cos\omega t.
+\]
+In der Spule wird dann die Spannung $U_\mathrm{ind}=-\dot\varphi_m$, also
+\[
+	U_\mathrm{ind} = -NBA\omega \sin(\omega t)
+\]
+induziert.
+
    
  \section{Wirbelströme}
   Bislang haben wir die induzierten Ströme in Kabeln betrachtet. Für den Fall, dass wir 
@@ -154,8 +173,7 @@ Anziehung dazu führen, dass eine Gesamtkraft der Bewegungsrichtung entgegenwirk
 Kraft ist proportional zur Geschwindigkeit und verhält sich also ganz ähnlich zu  Newton'scher
 Reibung.}
   \end{figure}
-\section{Anwendung: Transformator}
-tbd.
+  
  \section{Selbst- und Gegeninduktion}
  \subsection{Selbstinduktion: Induktivität $L$}
  Jede Flussänderung induziert eine Spannung, die nach der Lenz'schen Regel der Flussänderung
@@ -209,6 +227,42 @@ induziert eine Spannung $U_\mathrm{ind}$, die der Änderung entgegenwirkt, also
    \subsection{Gegeninduktion}
    TBD.
 
+
+ \subsection{Anwendung: Transformator}
+  Wir betrachten eine Spule (Primärwicklung) mit $N_1$ Windungen auf einem Eisenjoch (z.B. laminiertes Harteisen) - siehe 
+  Abbildung~\ref{fig:transformator}. Auf dem selben Eisenjoch 
+  ist eine Sekundärwicklung mit $N_2$ Windungen angebracht. Wenn wir jetzt die Primärwicklung mit einem Generator (siehe Abschnitt 
+  ~\ref{section:generator}) verbinden, erzeugen wir einen zeitlich variierenden magnetischen Fluss 
+  \[ U_1 = - N_1 \dot\varphi.\]
+  Der magnetische Fluss $\varphi$ wird im idealen, verlustfreien Transformator durch das Eisenjoch geleitet, so dass die Sekundärspule
+  den selben Fluss sieht, so dass dort die Spannung 
+  \[ U_2 = - N_2 \dot \varphi \]
+  induziert wird.
+  Für das Verhältnis der Spannungen im Falle eines unbelasteten Transformators ergibt sich
+  \[
+	   \frac{U_1}{U_2} = \frac{N_1}{N_2}.
+   \]
+   Andererseits kann die Leistung $P=U_1 I_1=U_2 I_2$ aufgrund der Energieerhaltung sich nicht ändern, so dass
+   \[ \frac{I_2}{I_1} = \frac{N_1}{N_2} \]
+   gelten muss. 
+   \begin{figure}
+	   \begin{center}
+	   \includegraphics[width=0.7\linewidth]{figures/transformator.png}
+	   \end{center}
+	   \caption{\label{fig:transformator} Schematische Darstellung eines Transformators.}
+
+   \end{figure}
+
+   Mit einem Transformator lässt sich die Spannung an der Sekundärwicklung durch ein geeignet gewähltes Verhältnis 
+   der Wicklungen entweder hochtransformieren ($N_2>N_1$) oder heruntertransformieren ($N_2<N_1$). Die Ströme in
+   der Sekundärspule werden beim Hochtransformieren um das selbe Verhältnis verkleinert. Beim Heruntertransformieren werden die Ströme 
+   vergrößert. 
+
+   Im Detail ist beim Transformator zu berücksichtigen, dass ein Teil des magnetischen Flusses nicht in der Sekundärspule ankommt. Ein weiterer
+   wichtiger Punkt ist die Phasenlage der beiden Wechselströme, die durch eine Belastung der Sekundärspule modifizert wird. Interessant
+   ist auch die Orientierung der Wicklungen zueinander (siehe auch hier die Abbildung~\ref{fig:transformator}). 
+
+  
   
  \section{Maxwell'scher Verschiebungsstrom: Amp\`ere-Maxwell-Gleichung}
  \label{section:maxwell-strom}