Tabellenanhang - Alex-weingarten.de

88 ANHANG O. BEISPIELE LATEX
\end{array} \right.
\end{equation}
\begin{equation}
{n+1 \choose k} = {n \choose k} + {n \choose k-1}
\end{equation}
\begin{equation}
\mbox{
\fbox{\parbox{60mm}{\begin{displaymath}
\forall x \in {\rm R}: \qquad x^2 \geq 0
\end{displaymath}}}}
\end{equation}
\vspace{1mm}
\begin{equation}
\forall x,y,z \in {\rm M}: \qquad (xRy \wedge xRz)
\Rightarrow y = z
\end{equation}
\begin{equation}
A \cdot B = \overline{\bar A + \bar B}
\end{equation}
\begin{equation}
\rho \cdot \bar{v}_k \cdot \frac{\partial \bar{v}_j}
{\partial{x}_k} = - \frac{\partial \bar{p}}
{\partial x_j} + \frac{\partial}{\partial x_k}
\left( \mu \frac{\partial \bar{v}_j}{\partial x_k}
- \rho\:\overline{v’_k v’_j} \right)
\end{equation}
\begin{equation}
r’ = \frac{\overline{v’_1 v’_2}}{\sqrt{\bar{v’^2_1}}
\: \sqrt{\bar{v’^2_2}}}
\end{equation}
\begin{equation}
\tau_{tur} = \rho l^2 \; | \frac{\partial \bar{v_1}}
{\partial x_2} | \; \frac{\partial \bar{v_1}}{\partial x_2}
\end{equation}
\begin{eqnarray}
\label{formel}
\ddot R & = & \frac{1}{\Psi} ( V_r - \dot R)
+ R {\dot \Phi}^2 \nonumber\\
\ddot \Phi & = & \big\lbrack \frac{1}{\Psi}