A cylindrical piece of cork of density of base area A and height h floats in a liquid of density ρ_r. The cork is depressed slightly and then released. Show that the cork oscillates up and down simple harmonically with a period T = 2π where ρ is the density of cork. (Ignore damping due to viscosity of the liquid).
Let the cylindrical cork have base area A, height h, and density ρ. It floats in a liquid of density ρᵣ.
Step 1: Equilibrium Position At equilibrium, let x₀ be the height of cork submerged in the liquid. By Archimedes' principle, the buoyant force equals the weight of the cork.
Weight of cork = mg = ρ × A × h × g Buoyant force = ρᵣ × A × x₀ × g
At equilibrium: ρ × A × h × g = ρᵣ × A × x₀ × g Therefore, x₀ = (ρ/ρᵣ) × h
Step 2: Displacement from Equilibrium When the cork is depressed by a small distance y from its equilibrium position, the submerged height becomes (x₀ + y).
The additional buoyant force acting upward = ρᵣ × A × y × g
Step 3: Equation of Motion This additional buoyant force acts as the restoring force. By Newton's second law:
F = ma -ρᵣ × A × y × g = m × (d²y/dt²)
The negative sign indicates the force is opposite to displacement y.
Step 4: Simple Harmonic Motion Form Rearranging: d²y/dt² = -(ρᵣ × A × g / m) × y
This is of the form d²y/dt² = -ω²y, which represents simple harmonic motion.
Thus, ω² = ρᵣ × A × g / m
Step 5: Time Period Since m = ρ × A × h, we get:
ω² = ρᵣ × A × g / (ρ × A × h) = ρᵣ × g / (ρ × h)
T = 2π/ω = 2π
T = 2π
Hence proved.
Explanation
This question tests the application of Archimedes' principle and SHM concepts. The key insight is that when a floating body is displaced from equilibrium, the change in buoyant force acts as a linear restoring force, which is the defining characteristic of SHM. The derivation follows the standard approach: find equilibrium, determine restoring force for small displacement, apply Newton's second law, and identify the angular frequency ω to get the time period.
Solution Steps
Step 1: Apply equilibrium condition using Archimedes' principle to find submerged height x₀ = (ρ/ρᵣ)h
Step 2: Determine additional buoyant force when displaced by y: F = -ρᵣ × A × y × g
Step 3: Apply Newton's second law: -ρᵣ × A × y × g = m(d²y/dt²)
Step 4: Identify SHM form: d²y/dt² = -ω²y where ω² = ρᵣAg/m
Step 5: Substitute m = ρAh and derive T = 2π