A thin circular ring of mass M and radius R is rotating about its axis with a constant angular velocity \(\omega\). Two objects each of mass m are attached gently to the ring on either side. The ring now rotates with an angular velocity:
Show Hint
When adding mass to a rotating body without external torque, use angular momentum conservation: \(I_i \omega_i = I_f \omega_f\).
Step 1: Conservation of angular momentum. No external torque acts, so L_i = L_f. Step 2: Initial angular momentum. L_i = I_ring ω = M R² ω. Step 3: Final moment of inertia. After attaching two masses at the rim, I_f = M R² + 2 m R² = (M + 2m) R². Step 4: Equating and solving. M R² ω = (M + 2m) R² ω_f → ω_f = [M/(M + 2m)] ω. Step 5: Conclusion. The new angular velocity is M/(M+2m) times ω.