A spherical solid ball of volume V is made of a material of density ρ1. It is falling through a liquid of density ρ2(ρ2<ρ1). Assume that the liquid applies a viscous force on the ball that is proportional to the square of its speed v, i.e., Fviscous=−kv2(k>0). The terminal speed of the ball is.
√Vg(ρ1−ρ2)k
The forces acting on the ball are gravity force, buoyancy force and viscous force. When ball acquires terminal speed, it is in dynamic equilibrium, let terminal speed of ball be vT. So
Vρ2g+kv2T=Vρ1g
vT=√V(ρ1−ρ2)gk