\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}