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JEE Advanced 1984 · Mechanical Properties of Fluids

A wooden plank of length 1 m1\,\text{m} 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 height 0.5 m0.5\,\text{m}. The specific gravity of the plank is 0.50.5. Find the angle θ\theta that the plank makes with the vertical in the equilibrium position. (Exclude the case θ=0∘\theta = 0^\circ)

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Written solution

Step 1: Identify the given parameters.

Let the parameters of the system be:

  • Length of the plank: L=1 mL = 1\,\text{m}
  • Height of the water: h=0.5 mh = 0.5\,\text{m}
  • Specific gravity of the plank: s=0.5s = 0.5
  • Uniform cross-sectional area of the plank: AA
  • Density of water: ρw\rho_w
  • Density of the plank: ρp=sρw\rho_p = s\rho_w
  • Immersed length of the plank: xx

Step 2: Express the forces acting on the plank.

The weight WW of the plank acts downwards at its center of gravity (at a distance of L2\frac{L}{2} from the hinge).

W=ρpALg=sρwALgW = \rho_p A L g = s \rho_w A L g

The buoyant force FBF_B acts upwards at the center of gravity of the submerged portion (at a distance of x2\frac{x}{2} from the hinge).

FB=ρwAxgF_B = \rho_w A x g

Step 3: Set up the torque balance about the hinge.

For rotational equilibrium, the torque due to the weight must balance the torque due to the buoyant force.

τW=τB\tau_W = \tau_B W(L2sin⁡θ)=FB(x2sin⁡θ)W \left(\frac{L}{2} \sin\theta\right) = F_B \left(\frac{x}{2} \sin\theta\right)

Since θ≠0∘\theta \neq 0^\circ, we can divide both sides by sin⁡θ\sin\theta.

WL=FBxW L = F_B x

Step 4: Solve for the immersed length xx.

Substitute the expressions for WW and FBF_B into the torque balance equation.

(sρwALg)L=(ρwAxg)x(s \rho_w A L g) L = (\rho_w A x g) x sL2=x2s L^2 = x^2 x=Lsx = L\sqrt{s}

Substitute the given values L=1 mL = 1\,\text{m} and s=0.5s = 0.5.

x=1⋅0.5≈0.707 mx = 1 \cdot \sqrt{0.5} \approx 0.707\,\text{m}

Step 5: Determine the angle θ\theta using geometry.

The vertical projection of the immersed length xx must equal the water height hh.

xcos⁡θ=hx \cos\theta = h cos⁡θ=hx\cos\theta = \frac{h}{x}

Substitute h=0.5 mh = 0.5\,\text{m} and x=0.5 mx = \sqrt{0.5}\,\text{m}.

cos⁡θ=0.50.5=0.5=12\cos\theta = \frac{0.5}{\sqrt{0.5}} = \sqrt{0.5} = \frac{1}{\sqrt{2}} θ=45∘\theta = 45^\circ

Answer: θ=45∘\theta = 45^\circ

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