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Question
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
${{M{L^2}{\omega ^2}} \over 2}$
${{ML{\omega ^2}} \over 2}$
${{M{L^2}\omega } \over 2}$
$ML{\omega ^2}$

Solution

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