\begin{table}%TB.2
%\centering
\par
\caption{Main parameters of the relaxation runs. 
         These runs had uniform $\nu=0.1$ and $\sigma$ (as given in the
	 table). $t_{\rm relax}$ is the duration of the runs.
	 $t_{\rm r2}=1$ for the runs with $\rho_0=B_0^2$, and
	 $t_{\rm r2}=5$ for the runs with $\rho_0=|\vec{B}_0|$
	 (except the one at $\Phi_{\rm g}=2.50~\pi$, in which also an
	 artificial reduction of $\rho$ was applied).} 
%note:  $t_{\rm r2}=1$ for the run with $\rho_0=|\vec{B}_0|$ and 2.50 $\pi$.
%Density was reduced by a factor of 10 in this run.
\begin{tabular}{ccllcr}
\hline \hline 
$y_0$ & $\rho_0$      & $v_0$ & $(1-\sigma)$ & $\Phi_{\rm g}$ 
                                                          & $ t_{\rm relax}$\\
                                                                    %& name
\hline
  1.0 & $B_0^2$       & 0.001 & 0.0004       & 2.06 $\pi$ & 120  \\ %& rsv12gr
      &               &       & 0.0004       & 2.30 $\pi$ & 120  \\ %& rsv12hr
      &               &       & 0.001        & 2.53 $\pi$ & 280  \\ %& rsv12ir
      &               &       & 0.002        & 2.75 $\pi$ & 753  \\ %& rsv12jrn
      &               &       & 0.005        & 2.95 $\pi$ & 1095 \\ %& rsv12krn
\hline
  1.0 & $|\vec{B}_0|$ & 0.01  & 0.0001       & 0.39 $\pi$ & 120  \\ %& rsv8ar
      &               &       & 0.0001       & 0.86 $\pi$ & 200  \\ %& rsv8br
      &               &       & 0.0001       & 1.33 $\pi$ & 200  \\ %& rsv8cr
      &               &       & 0.0001       & 2.28 $\pi$ & 600  \\ %& rsv8dr
      &               &       & 0.0005       & 2.50 $\pi$ &      \\ %& rsv8d0r
      &               &       & 0.0001       & 2.65 $\pi$ & 1120 \\ %& rsv8d1r
      &               &       & 0.0001       & 2.91 $\pi$ & 1358 \\ 
\hline  
\end{tabular}
\label{Tab2}
\end{table}