\begin{table}%t3 \caption[]{\label{tab:24133_wd} Photometric solutions for V1130~Tau. } {\begin{tabular}{lrrrr} \hline \hline\noalign{\smallskip} & $y$ & $b$ & $v$ & $u$\\ \noalign{\smallskip} \hline \noalign{\smallskip} $i$ \, (\degr) & 73.97 & 73.84 & 73.73 & 74.20\vspace{-0.8mm}\\ & $\pm $2 & $\pm $4 & $\pm $4 & $\pm $6\\ $\Omega_{\rm p}$ & 4.5138 & 4.5079 & 4.4954 & 4.5642\vspace{-0.8mm}\\ & $\pm $39 & $\pm $40 & $\pm $41 & $\pm $64\\ $\Omega_{\rm s}$ & 4.0727 & 4.0753 & 4.0775 & 4.0805\vspace{-0.8mm}\\ & $\pm $25 & $\pm $29 & $\pm $30 & $\pm $45\\ $r_{\rm p}$ & 0.2956 & 0.2961 & 0.2973 & 0.2911\\ $r_{\rm s}$ & 0.3542 & 0.3539 & 0.3536 & 0.3532\\ $k$ & 1.198 & 1.195 & 1.189 & 1.213\\ $r_{\rm p} + r_{\rm s}$ & 0.6498 & 0.6500 & 0.6509 & 0.6443\\ $u_{\rm p} = u_{\rm s}$ & 0.52 & 0.61 & 0.67 & 0.63 \\ $T_{{\rm eff},\rm s}$ & 6638 & 6639 & 6643 & 6628\vspace{-0.8mm}\\ &$\pm $4 & $\pm $3 &$\pm $3 &$\pm $4\\ $L_{\rm s}/L_{\rm p}$ & 1.444 & 1.436 & 1.429 & 1.436 \\ $\sigma$ \, (mmag) & 4.5 & 4.3 & 4.3 & 6.5 \\ \hline \end{tabular} } \tablefoot {Limb darkening coefficients by van Hamme (\cite{vh93}), gravity darkening exponents of~0.33, and bolometric albedo coefficients of~0.5 were adopted, as appropriate for convective envelopes. $T_{{\rm eff},p}$ was assumed to be 6650~K, see Sect.~\ref{sec:absdim}. The errors quoted for the free parameters are the {\it formal} standard errors determined from the iterative least squares solution procedure.} \end{table}