A circular disc of weight 500 N and radius 1 m is started from rest by a constant horizontal force of 25 N applied tangentially to the disc. The kinetic energy of the disc after \(t = 2\,s\) is:
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For rotational motion problems, always use \( \tau = I\alpha \) and \( KE = \frac{1}{2}I\omega^2 \).
Step 1: Mass from weight. W = 500 N → m = 500/10 = 50 kg. Step 2: Moment of inertia. For a solid disc, I = ½ M R² = ½×50×1² = 25 kg m². Step 3: Torque and angular acceleration. τ = F R = 25×1 = 25 N m; α = τ/I = 25/25 = 1 rad s⁻². Step 4: Angular velocity after 2 s. ω = α t = 1×2 = 2 rad s⁻¹. Step 5: Rotational kinetic energy. KE = ½ I ω² = ½×25×4 = 50 J.