\begin{table}%t1
\caption{\label{tab:runs}Summary of the runs with varying $\Pm$.  }
      \small%\centering
\par
         \begin{tabular}{cccrccccccccc}
           \hline\hline
           \noalign{\smallskip}
Run & Grid  & $\Ma$   & $\Pm$ & $\Rm$ & $\tilde\lambda$ & $\epsilon_{\rm f}$ & $k_{\rm f}^{(\omega)}$/$\kef$ & $\tilde\brms$ & $\tilde{\mean{B}}_x$ & $\tilde{\mean{B}}_y$ & $\tilde{\mean{B}}$ & $bc$ \\ 
 \noalign{\smallskip}\hline \noalign{\smallskip} 
VF1 & 128$^3$  & 0.049 & 0.05 & 0.78& $-$0.027 & $-$0.070 & 1.63 &   $-$           &   $-$                &     $-$              &   $-$     &  $VF$ \\  
VF2 & 128$^3$  & 0.034 & 0.10 & 1.1 &  0.013 & $-$0.073 & 1.58 & 1.04        & 0.14               &    0.99            & 1.00    &  $VF$ \\  
VF3 & 128$^3$  & 0.041 & 0.17 & 2.2 &  0.030 & $-$0.067 & 1.58 & 2.04        & 0.19               &    1.98            & 1.99    &  $VF$ \\ % vf128a6
{\bf VF4} & 128$^3$  & 0.046 & 0.25 & {\bf 3.7} & 0.036 & $-$0.066 & 1.60 & 2.28        & 0.22               &    2.18            & 2.18    &  $VF$ \\ % vf128a3
VF5 & 128$^3$  & 0.046 & 0.50 & 7.4 & 0.042 & $-$0.066 & 1.60 & 2.02        & 0.19               &    1.85            & 1.85    &  $VF$ \\ % vf128a2
VF6 & 128$^3$  & 0.044 & 1.00 & 14  & 0.046 & $-$0.068 & 1.63 &  1.94        & 0.22               &    1.65            & 1.66    &  $VF$ \\ % vf128a1
{\bf VF7}& 128$^3$  & 0.042 & 2.50 & {\bf 34} & 0.038 & $-$0.068 & 1.60 & 2.06        & 0.22               &    1.62            & 1.63    &  $VF$ \\ % vf128a
VF8 & 256$^3$  & 0.040 & 5.00 & 63  &  0.032 & $-$0.069 & 1.63 & 2.13        & 0.20               &    1.57            & 1.58    &  $VF$ \\ % vf256a
VF9 & 256$^3$  & 0.039 & 10.00 & 122 &  0.047 & $-$0.062 & 1.64 & 2.09        & 0.20               &    1.31            & 1.32    &  $VF$ \\ % vf256a1
{\bf VF10}& 512$^3$  & 0.035 & 20.00 & {\bf 222}& 0.071 & $-$0.067 & 1.68 & 2.14        & 0.21               &    1.09            & 1.11    &  $VF$ \\ % vf512a
       \noalign{\smallskip}
PC1 & 128$^3$  & 0.045 & 0.25 & 3.6 &  $-$0.019 & $-$0.065 & 1.61 &  $-$         &  $-$                 &     $-$              &  $-$      &  $PC$ \\ % pc128a3
{\bf PC2}& 128$^3$  & 0.034 & 0.50 & {\bf 5.4}& 0.011 & $-$0.072 & 1.57 & 1.08        & 0.14               &    0.92            & 0.93    &  $PC$ \\ % pc128a2
PC3 & 128$^3$  & 0.035 & 0.67 & 7.5 & 0.016 & $-$0.072 & 1.58 & 1.67        & 0.20               &    1.49            & 1.50    &  $PC$ \\ % pc128a4
PC4 & 128$^3$  & 0.040 & 1.00 & 13  & 0.021 & $-$0.076 & 1.58 & 2.44        & 0.26               &    2.23            & 2.23    &  $PC$ \\ % pc128a1
{\bf PC5}& 128$^3$  & 0.040 & 2.50 & {\bf 32} & 0.028 & $-$0.072 & 1.58 & 3.22        & 0.31               &    2.90            & 2.90    &  $PC$ \\ % pc128a
PC6 & 256$^3$  & 0.038 & 5.00 & 61  & 0.027 & $-$0.062 & 1.62 & 3.05        & 0.33               &    2.55            & 2.56    &  $PC$ \\ % pc256a
PC7 & 256$^3$  & 0.035 & 10.00& 112 & 0.049 & $-$0.065 & 1.63 & 2.29        & 0.22               &    1.53            & 1.55    &  $PC$ \\ % pc256a1
{\bf PC8}& 384$^3$  & 0.037 & 14.29& {\bf 168}& 0.057 & $-$0.056 & 1.65 & 1.83        & 0.17               &    0.95            & 0.96    &  $PC$ \\ % pc384a
PC9 & 512$^3$  & 0.038 & 20.00 & 239 & 0.064  &$-$0.054 & 1.64 &     1.62   &           0.16     &          0.74    &  0.76   &  $PC$ \\ % pc512a
           \hline
         \end{tabular}
\tablefoot{$\tilde\lambda$, $\epsilon_{\rm f}$, and $\kef^{(\omega)}$ are given 
for the kinematic stage whereas all the other numbers are given for 
the saturated state of the dynamo. The last column specifies the 
vertical boundary condition for the magnetic field. In all runs, 
$\Co\approx0.8$, $\Sh\approx-0.4$, $\Rey\approx12$, and 
$\Pra\approx0.7$. The adiabatic sound speed squared varies in the 
range $\cst/(gd)=0.33{-}1.38$ in the domain. Six of the runs are 
discussed in particular detail, so we have marked them here in 
boldface and have also highlighted the corresponding values of $\Rm$.
}
\end{table}