(c) When drop is stationary, then
$q_{1}E = 6\pi\ \eta r\ v_{0}$ or $q_{1} = 6\pi\ \eta r\ v_{0}/E$
When drop moves upwards, then
$3q = \frac{6\pi\ \eta r\left( v_{0} + v_{0} \right)}{E} = 2 \times \left( \frac{6\pi\ \eta rv_{0}}{E} \right) = 2q_{1}$
$\therefore\ \ q_{1} = \frac{3}{2}q$