All Figures

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{2245fig1.eps} \end{figure}$ Figure 1: Horizontally averaged correlations of $u_{\rm z}$ with respect to the snapshot at t = 100 for the run Co0. Each curve is separated by $\Delta t = 1$ in time units of $\sqrt {d/g}$ .
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=7.8cm,clip]{2245fig2.eps} \end{figure}$ Figure 2: Velocity autocorrelations for u_z as functions of r and rotation for the runs indicated in the legend.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=7.9cm,clip]{2245fig3.eps} \end{figure}$ Figure 3: Vertical positions of two test particles in the run Co0. The dotted vertical lines denote the times where the particle denoted by the solid line changes direction from downward motion to upward motion. The dash-dotted line shows a particle which is stuck in the lower overshoot layer for the whole duration of the calculation.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=7.8cm,clip]{2245fig4.eps} \end{figure}$ Figure 4: Distribution of turnover times from run the Co0 with the test particle method.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=16.8cm,clip]{2245fig5.eps} \end{figure}$ Figure 5: The correlation time $\tau _{\rm c}$ ( left) and the Strouhal number ${\rm St}$ ( right) functions of the Coriolis number. Powerlaws ${\tau _{\rm c} \propto {\rm Co}^{-0.28}}$ and ${\rm St} \propto {\rm Co}^{-0.32}$ are plotted. The stars, diamonds, triangles, and squares represents the calculations at latitudes $0 \hbox {$^\circ $ }$ (equator), $-30\hbox {$^\circ $ }$ , $-60\hbox {$^\circ $ }$ , and $-90 \hbox {$^\circ $ }$ (south pole), respectively.
Open with DEXTER

In the text

$\begin{figure} \par\includegraphics[width=8.8cm,clip]{2245fig1.eps} \end{figure}$	Figure 1: Horizontally averaged correlations of $u_{\rm z}$ with respect to the snapshot at t = 100 for the run Co0. Each curve is separated by $\Delta t = 1$ in time units of $\sqrt {d/g}$ .
Open with DEXTER

$\begin{figure} \par\includegraphics[width=7.8cm,clip]{2245fig2.eps} \end{figure}$	Figure 2: Velocity autocorrelations for u_z as functions of r and rotation for the runs indicated in the legend.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=7.9cm,clip]{2245fig3.eps} \end{figure}$	Figure 3: Vertical positions of two test particles in the run Co0. The dotted vertical lines denote the times where the particle denoted by the solid line changes direction from downward motion to upward motion. The dash-dotted line shows a particle which is stuck in the lower overshoot layer for the whole duration of the calculation.
Open with DEXTER

$\begin{figure} \par\includegraphics[width=7.8cm,clip]{2245fig4.eps} \end{figure}$	Figure 4: Distribution of turnover times from run the Co0 with the test particle method.
Open with DEXTER