(b) In case of refraction from a curved surface, we have
$\frac{\mu_{2}}{v} - \frac{\mu_{1}}{u} = \frac{\mu_{2} - \mu_{1}}{R} \Rightarrow \frac{1}{v} - \frac{2}{( - 15)} = \frac{(1 - 2)}{- 10} \Rightarrow v = - 30\ cm$
$i.e.,$ the curved surface will form virtual image $I$ at distance of $30\ cm$ from $P$. Since the image is virtual there will be no refraction at the plane surface $CD$ (as the rays are not actually passing through the boundary), the distance of final image $I$ from $P$ will remain $30\ cm$