$A$ ball of mass $m$ and radius $r$ is gently released in a viscous liquid. The mass of the liquid displaced by it is $m'$ such that $m > m'$. The terminal velocity is proportional to

  • A
    $\frac{m - m'}{r}$
  • B
    $\frac{m + m'}{r}$
  • C
    $\frac{m + m'}{r^2}$
  • D
    $(m - m')r^2$

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