\begin{table}%t2
%\centering
\par
\caption{\label{modpop1tab}Some properties of the 3D~simulation based on model M.}
\begin{tabular}{p{2.cm}p{2.cm}p{1.cm}p{1.3cm}p{1.0cm}p{1.0cm}p{1.0cm}
p{1.5cm}p{1.5cm}p{1.5cm}} 
\hline \hline \noalign{\smallskip}
Run & Grid & $w$ & $\Delta r$ & $\Delta\theta$ & $\Delta\phi$ & $R_{\rm e}$ &   $v_{\rm c}$  & $\tau_{\rm cnv}$ & $t_{\max}$ \\
$\mbox{[name]}$ & $N_{\rm r} \times N _\theta \times N_\phi$ & [$\dgr$] & 
[10$^{6}$~cm] & [$\dgr$] & [$\dgr$]  & & [10$^{6}~\cms$] & [s] & [s] \\
\hline 
heflpopI.3d & $270\times30\times30$ & 30 & 3.7 & 1 & 1 & $10^2$ & 1.1 & 1000 & 100~000 \\
\hline
\end{tabular} 
\tablefoot{Number of grid zones, wedge size~$w$, grid resolution in $r$, $\theta$ and~$\phi$ direction, estimated Reynolds number $R_{\rm e}$ \citep{PorterWoodward1994}, approximate characteristic velocity $v_{\rm c}$ of the convective flow, typical convective turnover timescale $\tau_{\rm cnv}$,  and maximum evolutionary time $t_{\max}$.}
\end{table}