(b) If spherical body of radius a is dropped in a viscous fluid, it is first accelerated and then its acceleration becomes zero and it attains a constant velocity called terminal velocity.
$Terminal\ velocity,\ \ v = \frac{2}{9}\ \frac{a^{2}(\rho - \sigma)g}{ɳ}$
where $\rho$ is the density of the body,$\sigma$ is the density of fluid and ɳ is coefficient of viscosity.