\begin{table}%[!h]%TE1
%%%%\centering
\par
\caption{The functions $S_{1}$, $S_{2}$, $S_{3}$ for special values of $\gamma$, expressed in terms of the  elementary functions $W_{n}(x)$.\label{tabE1}}
\begin{tabular*}{135mm}% 
{@{\extracolsep{\fill}}ll}\hline\hline
$\gamma$ &  Function\\ \hline\\[-3.6mm]
 0 &  $S_{1}(R)$ = $\frac{Mc_{1}^{6}}{\pi b_{0}^{3}c_{2}^{5}}[2W_{5}(R/c_{2})+10W_{6}(R/c_{2})-60W_{7}(R/c_{2})+100W_{8}(R/c_{2})$\\ 
& \ \ \ \ \ \ \ \ \ \ $-70W_{9}(R/c_{2})+18W_{10}(R/c_{2})]$\\\\
 & $S_{2}(R) = \frac{Mc_{1}^{6}R^{2}}{\pi b_{0}^{3}c_{2}^{7}}\left[2W_{7}(R/c_{2})+14W_{8}(R/c_{2})-34W_{9}(R/c_{2})+18W_{10}(R/c_{2})\right]$\\ \\
 & $S_{3}(R) = \frac{Mc_{1}^{6}R^{4}}{\pi b_{0}^{3}c_{2}^{9}}\left[2W_{9}(R/c_{2})+18W_{10}(R/c_{2})\right]$ \\ \\ \\
1 &  $S_{1}(R) = \frac{Mc_{1}^{6}}{\pi b_{0}^{3}c_{2}^{5}}[2W_{5}(R/c_{2})+10W_{6}(R/c_{2})-40W_{7}(R/c_{2})+42W_{8}(R/c_{2})$\\ 
 &  \ \ \ \ \ \ \ \ \ \ $-14W_{9}(R/c_{2})]$\\ \\
& $S_{2}(R) = \frac{Mc_{1}^{6}R^{2}}{\pi b_{0}^{3}c_{2}^{7}}\left[2W_{7}(R/c_{2})+14W_{8}(R/c_{2})-14W_{9}(R/c_{2})\right]$\\ \\
 & $S_{3}(R) = \frac{Mc_{1}^{6}R^{4}}{\pi b_{0}^{3}c_{2}^{9}}[\frac{2c_{2}^{2}}{R^{2}}-2W_{2}(R/c_{2})-4W_{3}(R/c_{2})-6W_{4}(R/c_{2})-8W_{5}(R/c_{2})$\\
& \ \ \ \ \ \ \ \ \ \ $-10W_{6}(R/c_{2})-12W_{7}(R/c_{2})-14W_{8}(R/c_{2})-14W_{9}(R/c_{2})]$ \\ \\ \\
2 & $S_{1}(R) = \frac{Mc_{1}^{6}}{2\pi b_{0}^{3}c_{2}^{5}}[4W_{5}(R/c_{2})+20W_{6}(R/c_{2})-45W_{7}(R/c_{2})+21W_{8}(R/c_{2})]$\\ \\
& $S_{2}(R) = \frac{Mc_{1}^{6}R^{2}}{2\pi b_{0}^{3}c_{2}^{7}}[\frac{7\pi c_{2}}{2R}-7W_{1}(R/c_{2})-7W_{2}(R/c_{2})-7W_{3}(R/c_{2})-7W_{4}(R/c_{2})$\\
& $-7W_{5}(R/c_{2})-7W_{6}(R/c_{2})-3W_{7}(R/c_{2})+21W_{8}(R/c_{2})]$\\ \\
& $S_{3}(R) =\frac{Mc_{1}^{6}R^{4}}{2\pi b_{0}^{3}c_{2}^{9}}[\frac{7}{4}\frac{\pi c_{2}^{3}}{R^{3}}-\frac{24c_{2}^{2}}{R^{2}}+24W_{2}(R/c_{2})+41W_{3}(R/c_{2})+51W_{4}(R/c_{2})$\\
& \ \ \ \ \ \ \ \ \ \ $+54W_{5}(R/c_{2})+50W_{6}(R/c_{2})+39W_{7}(R/c_{2})+21W_{8}(R/c_{2})]$  \\\hline
\end{tabular*}
\end{table}