(c) Terminal velocity of the ball through a viscous medium
$v = \frac{2}{9} \times \frac{g}{ɳ}(\rho - \sigma)r^{2}$
$v = \frac{2}{9} \times \frac{g}{ɳ}(\rho)r^{2}$
because viscous medium of negligible density $(\sigma = 0)$
$v = \frac{2}{9} \times \frac{g}{ɳ} \times \frac{m}{\frac{4}{3}{\pi r}^{3}} \times r^{2\ \ \ \ \ \ \ \ \ }\ \ \ \ \left( \therefore e = \frac{m}{\frac{4}{3}{\pi r}^{3}} \right)$
$or\ \ v = \frac{2}{9} \times \frac{g}{ɳ} \times \frac{m}{\frac{4}{3}{\pi r}^{3}}$
$\Longrightarrow \ \ \ \ v = \frac{1}{r}$
For the second ball
$v \propto \frac{1}{2r}$
Because radius of second ball is twice that of the first ball
$\frac{v}{v} = \frac{2r}{r}\ or\ v^{'} = \frac{v}{2}$