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\begin{figure}[h]
%  \centering 
 
\begin{minipage}{6cm}
 \includegraphics[width=1\textwidth]{Bilder/VG} 
\end{minipage}
\hfill
\begin{minipage}{0.5\textwidth}
\vspace{-130pt}
  \begin{align*} 
  p_{E} &= p_{t,E} - \Delta p_{t,E,E} = p_{ref} - \Delta p_{ref,t,E} - \Delta p_{t,E,E} \\ 
  p_{t,E} &= p_{ref} - \Delta p_{ref,t,E} \\ 
  p_{A} &= p_{t,A} - \Delta p_{t,A,A} = p_{ref} + \Delta p_{t,A,ref} - \Delta p_{t,A,A} \\ 
  p_{t,A} &= p_{ref} + \Delta p_{ref,t,E} 
  \end{align*} 
 \end{minipage} 
 \caption{Variante G} 

\end{figure}

\begin{figure}[h]
  \centering
  \subfigure{ 
    \includegraphics[width=6cm]{Bilder/VG}}
  \begin{align*}
  p_{E} &= p_{t,E} - \Delta p_{t,E,E} = p_{ref} - \Delta p_{ref,t,E} - \Delta p_{t,E,E} \\ 
  p_{t,E} &= p_{ref} - \Delta p_{ref,t,E} \\ 
  p_{A} &= p_{t,A} - \Delta p_{t,A,A} = p_{ref} + \Delta p_{t,A,ref} - \Delta p_{t,A,A} \\ 
  p_{t,A} &= p_{ref} + \Delta p_{ref,t,E}
  \end{align*}
  \caption{Variante G}
  \label{V7}
\end{figure}

\subsubsection{Variante G}
Anders als Variante A werden die Totaldrücke nicht absolut gemessen, sondern bilden die Differenz mit dem Umgebungsdruck. (Siehe Abbildung \ref{V7})

\begin{figure}[h]
  \centering
  \subfigure{ 
    \includegraphics[width=6cm]{Bilder/VG}}
  \subfigure{\begin{tabular}{c}
  $p_{E} = p_{t,E} - \Delta p_{t,E,E} = p_{ref} - \Delta p_{ref,t,E} - \Delta p_{t,E,E}$ \\ 
  $p_{t,E} = p_{ref} - \Delta p_{ref,t,E}$ \\ 
  $p_{A} = p_{t,A} - \Delta p_{t,A,A} = p_{ref} + \Delta p_{t,A,ref} - \Delta p_{t,A,A}$ \\ 
  $p_{t,A} = p_{ref} + \Delta p_{ref,t,E}$ \\ 
  \end{tabular}     
  }
  \caption{Variante G}
  \label{V7}
\end{figure}