\def\slideleftmargin{5.1cm}
\def\slidetopmargin{-0.6cm}
+\newcommand{\ham}{\mathcal{H}}
+\newcommand{\pot}{\mathcal{V}}
+
% topic
\begin{slide}
\begin{itemize}
\item Innere Energie:
\[
- E = <K> + <U> = < \sum_i \frac{|{\bf p}_i|^2}{2m_i} > + <U({\bf q})>
+ E = <K> + <U> = < \sum_i \frac{{\bf p}_i^2}{2m_i} > + <U({\bf q})>
+ \]
+ \item Temperatur/Druck
+ \begin{eqnarray}
+ <p_k \frac{\partial \ham}{\partial p_k}> &=& k_BT \nonumber \\
+ <q_k \frac{\partial \ham}{\partial q_k}> &=& k_BT \nonumber
+ \end{eqnarray}
+ \begin{center}
+ "Aquipartitionstheorem
+ \end{center}
+ Temperatur:
+ \[
+ \sum_i {\bf p}_i \frac{{\bf p}_i}{m_i} = 3Nk_BT \quad
+ \Rightarrow \quad T=\frac{1}{3Nk_B} \sum_i \frac{{\bf p}_i^2}{m_i}
\]
- \item Temperatur:
+ Druck:
\[
- E_{kin}=<K>=\frac{3}{2}Nk_BT
- \Rightarrow T=\frac{1}{3Nk_B} \sum_i \frac{|{\bf p}_i|^2}{m_i}
+ \sum_i {\bf q}_i \nabla_{{\bf q}_i} \pot = 3Nk_BT \quad
+ \stackrel{\textrm{kart. Koord.}}{\Rightarrow} \quad
+ - \sum_i {\bf r}_i \nabla_{{\bf r}_i} \pot = -3Nk_BT \quad
\]
- \item Druck
\item W"armekapazit"at
\item Struktur Werte
\item Diffusion
{\large\bf
EAM
}
+
\end{slide}
\begin{slide}