\begin{table}%t3
\caption{\label{tab:outflow}Summary of the simulations results.}
%\centerline
 $$
\begin{tabular}{lr@{.}lr@{.}lr@{.}lr@{.}lccl}
\hline \hline\noalign{\smallskip}
Model   
& \multicolumn{2}{c}{$\log\bar{E}_B^{\rm end}$} 
& \multicolumn{2}{c}{$\log E_B^{\rm out}$}
& \multicolumn{2}{c}{$E_B^{\rm out}/\bar{E}_B^{\rm end}$}
& \multicolumn{2}{c}{$\langle B \rangle$}
 & $t_{\rm e}$
 & $T_\Omega$
& Description \\
        & \multicolumn{2}{c}{} 
& \multicolumn{2}{c}{}
& \multicolumn{2}{c}{}
& \multicolumn{2}{c}{[$\mu$G]}
          & [Myr]
            & [Myr]
              & \\
% units - end }}}
\hline
R.01Q1$^a$       & 1&37 & 0&07 &  0&05 &  0&068 & 1~219 & 628 & slow rotation \\
R.02Q1           & 3&55 & 2&02 &  0&03 &  0&835 &    440 & 314 & slow rotation \\
R.03Q1$^b$       & 4&03 & 2&89 &  0&07 &  1&206 &    375 & 209 & medium rotation \\
R.04Q1           & 4&17 & 3&29 &  0&13 &  1&285 &    346 & 157 & fast rotation \\
R.05Q1$^c$      & 3&95 & 3&43 &  0&30 &  1&120 &    509 & 125 & fast rotation \\
\hline
R.01Q0           &--1&73 &--0&42 & 20&48 &  0&001 &     -- & 628 & low shear\\
R.01Q.5          & 0&06 &--0&35 &  0&39 &  0&011 &     -- & 628 & medium shear \\
R.01Q1$^a$       & 1&37 & 0&07 &  0&05 &  0&068 & 1~219 & 628 & medium shear \\
R.01Q1.5         & 1&26 & 0&15 &  0&08 &  0&056 & 1~232 & 628 & high shear \\
R.05Q0           &--1&00 & 0&04 & 10&78 &  0&003 &     -- & 125 & low shear \\
R.05Q.5          & 4&03 & 3&38 &  0&22 &  1&168 &    363 & 125 & medium shear \\
R.05Q1$^c$       & 3&95 & 3&43 &  0&30 &  1&120 &    509 & 125 & medium shear \\
R.05Q1.5         & 3&81 & 3&07 &  0&18 &  0&934 &    375 & 125 & high shear \\
\hline
SF3R.03Q.5       & 3&14 & 2&23 &  0&12 &  0&190 &    506 & 209 & low SFR \\
SF3R.03Q1        & 3&28 & 2&28 &  0&10 &  0&243 &    444 & 209 & low SFR \\
SF10R.03Q.5$^d$  & 3&87 & 2&28 &  0&03 &  0&991 &    403 & 209 & medium SFR \\
SF10R.03Q1$^b$   & 4&03 & 2&89 &  0&07 &  1&206 &    375 & 209 & medium SFR \\
SF30R.03Q.5      & 2&79 & 2&77 &  0&96 &  0&190 &    629 & 209 & high SFR \\
SF30R.03Q1       & 3&30 & 3&05 &  0&57 &  0&243 &    547 & 209 & high SFR \\
\hline
M10/100          & 3&78 & 2&73 &  0&09 &  0&833 &    422 & 209 & \\
M20/200$^d$      & 3&87 & 2&28 &  0&03 &  0&243 &    403 & 209 & \\
M50/100          & 4&05 & 2&92 &  0&07 &  1&001 &    404 & 209 & \\
M100/200         & 4&11 & 2&67 &  0&04 &  1&352 &    393 & 209 & \\
M100/100         & 3&86 & 2&72 &  0&07 &  0&751 &    422 & 209 & constantly exploding SNe\\
FIRST            & 2&37 & 1&33 &  0&09 &  0&113 &    572 & 209 & SN activity during first 50 Myr \\
\hline
\end{tabular}
$$
\par
\tablefoot{The subsequent columns show: the model name, the mean value of total magnetic energy $\bar{E}_B^{\rm end}$ over past $50~\textrm{Myr}$, the total outflow of magnetic energy during whole simulation (see Eq.~(\ref{eq:outflow})), the ratio of these two quantities, the final mean value of the magnetic field in a disc midplane $\langle B\rangle$ ($|z|<$~$20$~pc), the e-folding time of magnetic flux
increase $t_{\rm e}$, galaxy revolution timescale $T_\Omega$, and a short description of a model.
Superscripts are explained in Table~\ref{tab:models}. Values of magnetic field energy are normalized to the initial value.}
\end{table}