\begin{table}%t1
%\centering
\par
\caption{Setup values for the simulations of the flame
  evolution.\label{values_tab}}
$$
\begin{array}{llllllll}
\hline\hline
\noalign{\smallskip}
{\rm Label} & \mbox{$\rho_{\rm u} [~{\rm g} ~{\rm cm}^{-3}]$} & \mbox{$\rho_{\rm b} [~{\rm g}
~{\rm cm}^{-3}]$} & \mbox{$\mu$} & \mbox{${\it At}$} & \mbox{$s_{\rm l} [~{\rm cm} ~{\rm s}^{-1}]$} (TW) &
\mbox{$e_{i,\rm u} [~{\rm erg} ~{\rm g}^{-1}]$}
& \mbox{$e_{i,\rm b} [~{\rm erg} ~{\rm g}^{-1}]$}\\
\noalign{\smallskip}
\hline
\noalign{\smallskip}
\mbox{$1 \times 10^7$} & \mbox{$9.969 \times 10^6$} & \mbox{$2.691 \times 10^6 $} & 3.70 &
0.575 & \mbox{$2.39 \times 10^5$} & \mbox{$1.619 \times 10^{17}$} & \mbox{$8.59 \times
10^{17}$}\\
\mbox{$1.25 \times 10^7$} & \mbox{$ 1.232 \times 10^7$} & \mbox{$3.830 \times 10^6 $} & 3.22 &
0.526 & \mbox{$2.86 \times 10^5$} & \mbox{$2.005 \times 10^{17}$} & \mbox{$8.99 \times
10^{17}$}\\
\mbox{$2.5 \times 10^7$} & \mbox{$ 2.484 \times 10^7$} & \mbox{$8.69 \times 10^6 $} & 2.86 &
0.482 & \mbox{$5.01 \times 10^5$} & \mbox{$2.56 \times 10^{17}$} & \mbox{$9.50 \times
10^{17}$}\\
\mbox{$5 \times 10^7$} & \mbox{$ 4.988 \times 10^7$} & \mbox{$2.071 \times 10^7 $} & 2.41 &
0.413 & \mbox{$8.74 \times 10^5$} & \mbox{$3.584 \times 10^{17}$} & \mbox{$1.051 \times
10^{18}$}\\
\mbox{$7.5 \times 10^7$} & \mbox{$ 7.50 \times 10^7$} & \mbox{$3.345 \times 10^7 $} & 2.24 &
0.383 & \mbox{$1.21 \times 10^6$} & \mbox{$4.29 \times 10^{17}$} & \mbox{$1.13 \times
10^{18}$}\\
\mbox{$1 \times 10^8$} & \mbox{$ 1.00 \times 10^8$} & \mbox{$4.789 \times 10^7 $} & 2.09 &
0.352 & \mbox{$1.53 \times 10^6$} & \mbox{$4.89 \times 10^{17}$} & \mbox{$1.182 \times
10^{18}$}\\
\mbox{$1 \times 10^9$} & \mbox{$ 1.00 \times 10^9$} & \mbox{$6.80 \times 10^8 $} & 1.47 &
0.190 & \mbox{$9.75 \times 10^6$} & \mbox{$1.27 \times 10^{18}$} & \mbox{$1.96 \times
10^{18}$}\\
\noalign{\smallskip}
\hline
\end{array}
$$
\end{table}