\begin{table}%t2
%\centering
\par
\caption{\label{tab:j_v_const}The same parameters as in Table~\ref{tab:ppa_coeffs} for rigid
  rotation and the  ``exotic'' $j_{\rm const}$ and $v_{\rm const}$ rotators.}
\small \begin{tabular}{r*{3}{c}}
\hline\hline\noalign{\smallskip}
Model              & Rigid  &  $j_{\rm const}$  & $v_{\rm const}$ \\
\hline 
$\Omega_{\rm c}$~[rad/s] & 0.37242  & 6.4076  & 10.120   \\
\hline
$r_{\rm equator} / r_{\rm pol} $ & 1.477 & 2.183 & 2.183 \\
%\hline
$adr$              &  --  &  0.5  & 0.2 \\
%\hline 
$M ~[M_{\sun}]$ & 1.4661    & 1.8025  & 1.7067   \\
%\hline
$M_{\rm high}~[M_{\sun}]$ &  1.302          & 1.534 & 1.493    \\
%\hline
$M_{\rm high}/M ~[\%]$ &  88.8          & 85.1 & 87.5 \\
%\hline
$M_{\rm med}~[M_{\sun}]$ &  0.126         & 0.191 & 0.157     \\
%\hline
$M_{\rm med}/M ~[\%] $ & 8.6        & 10.6 & 9.2 \\
%\hline
$r_{\rm pol} ~[10^{~8} {\rm cm}]$ &  2.1721         & 1.8087 & 1.8134 \\
%\hline
$ r_{\rm equator} ~[10^{~8} {\rm cm}]$ &  3.2092        & 3.9481 & 3.95858 \\
%\hline
$E_{\rm int}~[10^{~51}{\rm ~erg}]$  &  2.5878          & 3.0072 & 2.9678 \\
%\hline
$E_{\rm grav}~[10^{~51}{\rm ~erg}]$ & --3.2074           & --4.2779 & --4.0604 \\
%\hline
$E_{\rm rot}~$[10$^{~50}$~erg]     &  0.442            & 3.163 & 2.393 \\ 
%\hline
$E_{\rm bind}~$[10$^{~50}$~erg]    &  --5.754             & --9.544 & --8.533 \\ 
%\hline
$\beta~[\%]$                    &  1.3769             & 7.3941 & 5.8933 \\
%\hline
$ J~[10^{~50}~{\rm g \;cm}^2 / {\rm s}]$ & 0.37747    & 1.3785 & 1.0535 \\
\hline
\end{tabular}
\end{table}