\begin{table}%T5
\caption{\label{tab:resultpg}Model quantities temporally averaged at the outer boundary for Planck mean models. The numbers printed in subscript in the $T_{{\rm tot}}$ column indicates the upper limit in the time-interval used in the calculation of the average quantities of the corresponding model (cf\@.~Sect.~\ref{sec:resultpg_old}). The values shown in bold face for the PC~models indicate that the value differ from the corresponding value given by {HJLA98} (by $\ge$$10\%$). For the PC~models an~"H'' in the last column indicates that the same model parameters were used in a model in {HJLA98}. See the caption of Table~\ref{tab:resultcg} for further details.}
%\centering
\par
\begin{tabular}{lr@{\ \ }rcr@{\ \ }rcr@{\ \ }rcr@{\ \ }rcr@{\ \ }rrrrl}\hline\hline
   Model & \multicolumn{2}{c}{\mmdot} &&
           \multicolumn{2}{c}{\muinf} &&
           \multicolumn{2}{c}{\mfcond} &&
           \multicolumn{2}{c}{\mdrhog} &&
           \multicolumn{2}{c}{\mtaud} &
           \multicolumn{1}{c}{\mvdri} &
           \multicolumn{1}{c}{$T_{{\rm tot}}$} &
           Type \\
           \multicolumn{3}{r}{\mmdotv} &&
           \multicolumn{2}{c}{$[\kns]$} &&
           \multicolumn{2}{c}{$[\%]$} &&
           \multicolumn{2}{c}{$[10^{-4}]$} &&
           \multicolumn{2}{c}{$[10^{-2}]$} &
           \multicolumn{1}{c}{$[\kns]$} &
           \multicolumn{1}{c}{$[P]$}\\
         &&\multicolumn{1}{c}{(\sistd)} &&
         & \multicolumn{1}{c}{(\sistd)} &&
         & \multicolumn{1}{c}{(\sistd)} &&
         & \multicolumn{1}{c}{(\sistd)} &&
         & \multicolumn{1}{c}{(\sistd)}\\\hline
\multicolumn{4}{l}{\textsc{Position coupled models}} &
\multicolumn{7}{l}{(illustrated with the symbol "$\Box$'')}\\\hline\\[-1.8ex]
P07FU6C14 & ${\bf 0.60}$& $(0.069)$ && $1.7$         & $(0.10)$ && ${\bf 55}$ & $(0.44)$  && ${\bf 12}$ & $(0.10)$ && $55$ & $(9.9)$ &       & $350$       & i & H$_{\boxplus}$\\
P07FU4C18 & $0.21$         & $(0.015)$ && $6.4$         & $(0.10)$ && $13$          & $(0.099)$ && $5.6$         & $(0.04)$ && $6.5$& $(0.3)$ &       & $330$       & i & H$_{\boxplus}$ \\[0.5ex]
P10FU4C14 & $0.71$         & $(0.12)$  && $2.2$         & $(0.18)$ && ${\bf 23}$ & $(0.22)$  && $5.2$         & $(0.05)$ && $23$ & $(1.8)$ &       & $480$       & i & H$_{\boxplus}$\\
P10FU2C18 & $0.18$         & $(0.019)$ && $8.6$         & $(0.14)$ && $4.6$         & $(0.18)$  && $2.1$         & $(0.08)$ && $1.6$& $(0.1)$ &       & $_{140}430$ & i & H$_{\boxplus}$\\
P10FU4C18 & ${\bf 1.1}$ & $(0.49)$  && $14$          & $(0.77)$ && ${\bf 16}$ & $(2.6)$   && $7.2$         & $(1.2)$  && $7.3$& $(2.4)$ &       & $_{150}410$ & i & H\\
P10FU6C16 & $2.7$          & $(1.4)$   && $13$          & $(1.1)$  && $27$          & $(4.0)$   && $9.2$         & $(1.3)$  && $22$ & $(11)$  &       & $_{180}390$ & i \\
P10FU6C18 & ${\bf 2.0}$ & $(0.61)$  && $16$          & $(0.48)$ && $21$          & $(1.8)$   && $9.3$         & $(0.83)$ && $15$ & $(4.9)$ &       & $_{120}390$ & i & H\\[0.5ex]
P13FU6C14 & ${\bf 4.7}$ & $(2.3)$   && ${\bf 10}$ & $(0.76)$ && $26$          & $(2.7)$   && $6.0$         & $(0.61)$ && $34$ & $(16)$  &       & $_{110}520$ & i & H\\
P13FU4C16 & $2.3$          & $(0.39)$  && $12$          & $(0.30)$ && $15$          & $(1.1)$   && $5.2$         & $(0.39)$ && $8.6$& $(1.7)$ &       & $_{140}440$ & i \\
P13FU6C16 & $3.9$          & $(0.51)$  && $14$          & $(0.23)$ && $21$          & $(9.6)$   && $7.3$         & $(0.33)$ && $19$ & $(2.0)$ &       & $_{80}390$  & i \\
\multicolumn{4}{l}{\textsc{Drift models}} &
\multicolumn{7}{l}{(illustrated with the symbol "\boxfd'')}\\\hline
P07FU6C14 & \multicolumn{2}{c}{---}   &&               &          &&               &           &&               &          &&       &        &       &             & --- \\
P07FU4C18 & \multicolumn{2}{c}{---}   &&               &          &&               &           &&               &          &&       &        &       &             & --- \\
P10FU4C14 & \multicolumn{2}{c}{---}   &&               &          &&               &           &&               &          &&       &        &       &             & --- \\
P10FU2C18 & \multicolumn{2}{c}{---}   &&               &          &&               &           &&               &          &&       &        &       &             & t \\
P10FU4C18 & $0.82$         & $(0.12)$ && $11$          & $(0.24)$ && $12$          & $(5.3)$   && $5.4$         & $(2.9)$  && $3.3$ & $(0.5)$& $4.5$ &       $93$  & i & \dpa \\
P10FU6C16 & $1.1$          & $(1.0)$  && $8.5$         & $(1.1)$  && $19$          & $(18)$    && $7.9$         & $(13)$   && $8.7$ & $(5.6)$& $7.2$ &       $110$ & i & \dpa \\
P10FU6C18 & $2.2$          & $(2.8)$  && $22$          & $(2.3)$  && $27$          & $(34)$    && $39$          & $(210)$  && $25$  & $(10)$ & $16$  &        $65$ & 2\~q &      \\
P13FU6C14 & $1.9$          & $(2.0)$  && $7.5$         & $(1.5)$  && $24$          & $(24)$    && $8.4$         & $(30)$   && $17$  & $(16)$ & $10$  &       $130$ & i & \dpa \\
P13FU4C16 & $2.5$          & $(0.69)$ && $13$          & $(0.43)$ && $23$          & $(24)$    && $11$          & $(18)$   && $8.7$ & $(1.5)$& $4.9$ &       $130$ & 2\~q &      \\
P13FU6C16 & $4.1$          & $(4.0)$  && $14$          & $(1.1)$  && $19$          & $(21)$    && $11$          & $(39)$   && $16$  & $(4.1)$& $4.0$ &       $130$ & i\\[1.0ex]\hline
\end{tabular}
\end{table}