A spherical solid ball of volume $V$ is made of a material of density $\rho_1$ . It is falling through a liquid of density $\rho_2 (\rho_2 < \rho_1 )$. Assume that the liquid applies a viscous force on the ball that is proportional to the square of its speed $v$, i.e., $F_{viscous}= -kv^2 (k >0 )$,The terminal speed of the ball is 

  • [AIEEE 2008]
  • [AIIMS 2013]
  • A

    $\frac{{Vg\left( {{\rho _1} - {\rho _2}} \right)}}{k}$

  • B

    $\sqrt {\;\frac{{Vg\left( {{\rho _1} - {\rho _2}} \right)}}{k}} $

  • C

    $\;\frac{{Vg{\rho _1}}}{k}$

  • D

    $\;\sqrt {\frac{{Vg{\rho _1}}}{k}} $

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