A wooden plank of length and uniform cross-section is hinged at one end to the bottom of a tank as shown in the figure below. The tank is filled with water up to a height of . The specific gravity of the plank is . Find the angle that the plank makes with the vertical in the equilibrium position such that .
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The forces acting on the plank are shown in the figure. The height of water level is x = 0.5 m. The length of the plank is 2 x = 1 m.
The weight of the plank acts through the centre C of the plank. We have AC = 0.5 m. The buoyant force B acts through the point B, which is the middle point of the dipped part AD of the plank.
So, AB = 2 A D = 2 cos θ x
Let the mass per unit length of the plank be p .
Plank's weight, W = m g = p ( 2 x ) g = 2 p x g
The mass of the part AD of the plank = cos θ x p
The mass of water displaced = specific gravity 1 cos θ x p = cos θ 2 x p
So the buoyant force, B = cos θ 2 x p g
Now, for equilibrium, the torque of m g about C should balance the torque of B about B.
So, m g (AC) sin θ = B (AB) sin θ
⟹ 2 p x g × x = cos θ 2 x p g × 2 cos θ x
⟹ cos 2 θ = 2 1
⟹ cos θ = 2 1 = 4 5 o