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A uniform horizontal circular platform of mass 200kg is rotating at 5 rpm about vertical axis passing through its centre. A boy of mass 80kg is standing at its edge. if boy moves to centre of platform, find out final angular speed

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To solve the problem, we will use the principle of conservation of angular momentum. The angular momentum of a system remains constant if no external torque acts on it. ### Step-by-Step Solution: 1. **Identify Initial Conditions:** - Mass of the platform (M) = 200 kg - Mass of the boy (m) = 80 kg - Initial angular speed (ω_initial) = 5 rpm 2. **Convert Angular Speed to Radians per Second:** - Since 1 rpm = \( \frac{2\pi}{60} \) rad/s, we convert 5 rpm to rad/s: \[ \omega_{\text{initial}} = 5 \times \frac{2\pi}{60} = \frac{5\pi}{30} = \frac{\pi}{6} \text{ rad/s} \] 3. **Calculate Initial Moment of Inertia:** - The moment of inertia of the platform (I_platform) is given by: \[ I_{\text{platform}} = \frac{1}{2} M R^2 \] - The boy is initially at the edge, so his moment of inertia (I_boy_initial) is: \[ I_{\text{boy initial}} = m R^2 \] - Total initial moment of inertia (I_initial): \[ I_{\text{initial}} = I_{\text{platform}} + I_{\text{boy initial}} = \frac{1}{2} M R^2 + m R^2 = \left(\frac{1}{2} \times 200 + 80\right) R^2 = (100 + 80) R^2 = 180 R^2 \] 4. **Calculate Initial Angular Momentum:** - Angular momentum (L_initial) is given by: \[ L_{\text{initial}} = I_{\text{initial}} \cdot \omega_{\text{initial}} = 180 R^2 \cdot \frac{\pi}{6} = 30\pi R^2 \] 5. **Calculate Final Moment of Inertia:** - When the boy moves to the center, his moment of inertia becomes zero (I_boy_final = 0). Therefore, the final moment of inertia (I_final) is: \[ I_{\text{final}} = I_{\text{platform}} + I_{\text{boy final}} = \frac{1}{2} M R^2 + 0 = \frac{1}{2} \times 200 R^2 = 100 R^2 \] 6. **Apply Conservation of Angular Momentum:** - According to the conservation of angular momentum: \[ L_{\text{initial}} = L_{\text{final}} \] - Thus, \[ 30\pi R^2 = 100 R^2 \cdot \omega_{\text{final}} \] 7. **Solve for Final Angular Speed (ω_final):** - Dividing both sides by \( R^2 \) (assuming \( R \neq 0 \)): \[ 30\pi = 100 \omega_{\text{final}} \] - Therefore, \[ \omega_{\text{final}} = \frac{30\pi}{100} = \frac{3\pi}{10} \text{ rad/s} \] ### Final Answer: The final angular speed of the platform after the boy moves to the center is \( \frac{3\pi}{10} \) rad/s.
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