A spherical solid ball of volume $V$ is made of a material of density $\rho_{1} .$ It is falling through a liquid of density $\rho_{2}\left(\rho_{2}<\rho_{1}\right) .$ Assume that the liquid applies a viscous force on the ball that is proportional to the square of its speed $v$, i.e., $F_{\text {viscous }}=-\mathrm{k} v^{2}(\mathrm{k}>0)$. The terminal speed of the ball is:
(a) $\sqrt{\frac{\operatorname{Vg}\left(\rho_{1}-\rho_{2}\right)}{\mathrm{k}}}$
(b) $\frac{V g \rho_{1}}{k}$
(c) $\sqrt{\frac{V g \rho_{1}}{k}}$
(d) $\frac{V g\left(\rho_{1}+\rho_{2}\right)}{k}$