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A wooden plank of length 1m and uniform cross-section is hinged at one end to the bottom of a tank as shown in fig. The tank is filled with water upto a hight 0.5m. The specific gravity of the plank is 0.5. Find the angle `theta` that the plank makes with the vertical in the equilibrium position. (Exclude the case `theta=theta^@`)

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The correct Answer is:
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Let y be the length of the plank inside water.
`y=0.5/(costheta)`
let `A` be the cross sectiona area of the plank. Then buoyant force on it is `F_(b)=Vrho_(w)g=(Ay)rho_(w)g`

Since plank is in rotational equilibrium so `sumvectau_(0)=0`
or `mgxxl/2 sintheta-F_(b)xxy/2sintheta=0` or `mgl-F_(b)xxy=0`
or `(Alxx0.5)gl-(Ay)dvy=0` or `0.5^(2)=y^(2)`
or `0.5xx(1)^(2)=(0.5/(costheta))^(2)` or `cos^(2)theta=1/2`
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