\begin{table}
%%\begin{center}
\par
%\begin{tabular}{c|c|c|cc|cc|cc|cc}\hline
%\multirow{2}{*}{$\eta$} & \multirow{2}{*}{$\alpha$} &
%\multirow{2}{*}{$L_{\rm lobe}$ (cm)} & \multicolumn{2}{|c|}{$<v>_{\rm
%	flow}$ (\kms)} & \multicolumn{2}{|c|}{$v_{\rm max}$ (\kms)} &
%\multicolumn{2}{|c|}{$\displaystyle\frac{m_{\rm observed}}{m_{\rm H_2}}$} &
%\multicolumn{2}{|c}{$\displaystyle\frac{|P_{\rm blue}| + |P_{\rm red}|}{
%P_{{\rm H_2}, z}}$} \\
% & & & (2 -- 40) & (7 -- 40)  & (2 -- 40) & (7 -- 40) & (2 -- 40) & 
% (7 -- 40) & (2 -- 40) & (7 -- 40) \\
%\hline
%\multirow{4}{*}{0.1} & $0^\circ$ & $2.82\times10^{17}$ & 2.68 & 8.82 &
%6 & 17 & 0.33 & $3.0\times10^{-3}$ & 0.39 & $1.2\times10^{-2}$ \\
%		& $30^\circ$ & $1.65\times10^{17}$ & 3.47 & 10.17 & 15 & 25 & 0.37 
%		& $3.4\times10^{-2}$ & 0.56 & 0.15 \\
%		& $60^\circ$ & $1.12\times10^{17}$ & 4.94 & 11.81 & 20 & 32 & 0.35 
%		& $7.7\times10^{-2}$ & 0.76 & 0.41 \\
%		& $90^\circ$ & $3.14\times10^{16}$ & 5.55 & 12.50 & 20 & 35 & 0.34 
%		& $8.8\times10^{-2}$ & 0.85 & 0.50 \\ \hline
%\multirow{4}{*}{1} & $0^\circ$ & $6.21\times10^{17}$ & 3.80 & 8.65 & 11
%& 17 & 0.66 & $5.4\times10^{-2}$ & 1.72 & 0.32 \\
%		& $30^\circ$ & $5.03\times10^{17}$ & 3.70 & 9.24 & 13 & 24 & 0.64 
%		& $5.1\times10^{-2}$ & 1.61 & 0.32 \\
%		& $60^\circ$ & $2.79\times10^{17}$ & 3.62 & 10.57 & 13 & 31 & 0.50 
%		& $5.5\times10^{-2}$ & 1.26 & 0.41 \\
%		& $90^\circ$ & $4.76\times10^{16}$ & 4.90 & 11.24 & 17 & 36 & 0.26 
%		& $5.6\times10^{-2}$ & 0.89 & 0.45  \\ 
%\end{tabular}
%%\end{center}
\par
%\caption{Masses and momenta of the outflows calculated from the $m_{\rm
%H_2}(v)$ relation using the velocity ranges 2 -- 40 \kms and 7 -- 40 \kms with 
%a bin width of 1 \kms.  Also shown are $<v>_{\rm lobe}$ and $v_{\rm max}$ 
%(see text).
%\label{vmin-truncation-table}}
%\end{table}