$A$ tube of length $L$ is filled completely with an incompressible liquid of mass $M$ and closed at both the ends. The tube is then rotated in a horizontal plane about one of its ends with a uniform angular velocity $\omega$. The force exerted by the liquid at the other end is

  • A
    $\frac{ML\omega^2}{2}$
  • B
    $ML\omega^2$
  • C
    $\frac{M\omega L^2}{2}$
  • D
    $\frac{ML^2\omega^2}{2}$

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