It's just a plank, bro.

A wooden plank of length 1 1 m m 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 0.5 0.5 m m . The specific gravity of the plank is 0.5 0.5 . Find the angle θ \theta that the plank makes with the vertical in the equilibrium position such that θ 0 o , 9 0 o \theta \neq 0^{o}, 90^{o} .

1 5 o 15^{o} 6 0 o 60^{o} 4 5 o 45^{o} 3 0 o 30^{o}

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1 solution

The forces acting on the plank are shown in the figure. The height of water level is x x = 0.5 m. The length of the plank is 2 x 2x = 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 B acts through the point B, which is the middle point of the dipped part AD of the plank.

So, AB = A D 2 \frac{AD}{2} = x 2 cos θ \frac{x}{2\cos\theta}

Let the mass per unit length of the plank be p p .

Plank's weight, W W = m g mg = p ( 2 x ) g p(2x)g = 2 p x g 2pxg

The mass of the part AD of the plank = x p cos θ \frac{xp}{\cos\theta}

The mass of water displaced = 1 specific gravity \frac{1}{\text{specific gravity}} x p cos θ \frac{xp}{\cos\theta} = 2 x p cos θ \frac{2xp}{\cos\theta}

So the buoyant force, B B = 2 x p g cos θ \frac{2xpg}{\cos\theta}

Now, for equilibrium, the torque of m g mg about C should balance the torque of B B about B.

So, m g mg (AC) sin θ \sin\theta = B B (AB) sin θ \sin\theta

\implies 2 p x g × x 2pxg \times x = 2 x p g cos θ × x 2 cos θ \frac{2xpg}{\cos\theta} \times \frac{x}{2\cos\theta}

\implies cos 2 θ \cos^{2}\theta = 1 2 \frac{1}{2}

\implies cos θ \cos\theta = 1 2 \frac{1}{\sqrt2} = 4 5 o \boxed{45^{o}}

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