\begin{table}%T5 \caption{\label{Ha}Comparison between IC~4662 H$\alpha$ fluxes from the literature. Inferred intensities, luminosities and Lyman continuum fluxes, follow from an adopted distance of 2.44~Mpc, and include 3~cm radio continuum derived ionizing flux from \citet{Johnson2003}. } %\centerline { \begin{tabular}{l@{\hspace{1.5mm}}c@{\hspace{1.5mm}}c@{\hspace{1.5mm}}c@{\hspace{1.5mm}}c@{\hspace{1.5mm}}c@{\hspace{1.5mm}}c@{\hspace{1.5mm}}c@{\hspace{1.5mm}}r} \hline\hline & $\theta^{\ast}$ & $F$(H$\alpha$+[N~{\sc ii}]) & $F$[N~{\sc ii}]/$F$(H$\alpha$) & $E(B-V)$ & $I$(H$\alpha$) & $\log L$(H$\alpha$) & $Q_0$ \\ & (arcmin) & (erg s$^{-1}$ cm$^{-2}$) & & (mag) & (erg s$^{-1}$ cm$^{-2}$) & (erg s$^{-1}$) & (10$^{49}$ s$^{-1}$) \\ \hline\\[-3.2mm] \citet{Kennicutt1983} & 2\phantom{.0} & $7.9\times10^{-12}$ & 0.05 & 0.00 & $7.6\times10^{-12}$ & 39.73 & \phantom{0}400 \\ \citet{Lonsdale1987} & 2\phantom{.0} & $7.9\times10^{-12}$ & 0.05 & 0.43 & $2.1\times10^{-11}$ & 40.17 & 1100 \\ %\citet{Hidalgo2001} & $5.1\times10^{-12}$ & -- & 0.03 %& 5.0\times10^{-12}$ & 0.14 & 39.52 & 244 \\ \citet{Helmboldt2004} & 2:\phantom{0} & $1.4\times10^{-11}$ & 0.05 & 0.29: & $2.6\times 10^{-11}$ & 40.28 & 1410 \\ \citet{Hunter2004} & 2.2 & $1.4\times10^{-11}$ & 0.00 & 0.16 & $2.1\times 10^{-11}$ & 40.17 & 1110 \\ \citet{Kennicutt2008} & 2\phantom{.0} & $1.1\times10^{-11}$ & 0.08 & 0.07 & $1.2\times10^{-11}$ & 39.92 & \phantom{0}615 \\ This study & 0.2 & $5.1\times10^{-12}$ & 0.03 & 0.16 & $7.2\times10^{-12}$ & 39.71 & \phantom{0}380 \\ \citet{Johnson2003} & 1:\phantom{0} & & & & & & \phantom{0}530 \\ \hline \end{tabular}} \medskip \par {$^\ast$ Approximate aperture radii.} \end{table}