A tube of length $L$ is filled completely with 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 on the tube at other end is
A tube of length $L$ is filled completely with 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 on the tube at other end is
- A
$\frac{{ML{\omega ^2}}}{2}$
- B
${ML{\omega ^2}}$
- C
$\frac{{M{\omega ^2}L^2}}{2}$
- D
$\frac{{M{\omega }L^2}}{2}$
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