System of Particles and Rotational Motion — Exam Practice
Practice questions in CBSE, NEET, and JEE Main style covering torque, moment of inertia, and angular momentum.
1CBSE Board Exam Style
Curling the body pulls mass closer to the axis of rotation, reducing moment of inertia. Since angular momentum (L = Iω) is conserved in the air (no external torque), a smaller I means a larger ω — the diver spins faster.
For a particle of mass mi at distance ri from the axis, tangential force Fi = miai = mi(riα). Torque due to this particle: τi = riFi = miri²α.
Summing over all particles: τ = (Σmiri²)α = Iα, where I = Σmiri² is the moment of inertia.
(a) The moment of inertia about any axis equals the moment of inertia about a parallel axis through the centre of mass, plus Md² (d = distance between the axes): I = Icm + Md².
(b) Icm = ML²/12 = (2×1)/12 ≈ 0.1667 kg·m². The end axis is at distance d = L/2 = 0.5 m from the centre.
Iend = Icm + Md² = 0.1667 + 2×(0.5)² = 0.1667 + 0.5 = 0.667 kg·m² (equivalently ML²/3).
2NEET Style (Single-Correct MCQ)
Every point on a ring lies at exactly the same distance R from the central axis, so I = MR² directly — the largest moment of inertia (for given M, R) among common shapes.
τ = dL/dt. With zero net external torque, L stays exactly constant, even if I and ω individually change (as in the diver example).
Torque = force × perpendicular distance, giving N·m — numerically the same unit as work/energy (joule), though torque is a vector and treated distinctly.
KErot = ½Iω² — the direct rotational analogue of ½mv² for linear motion, with I replacing m and ω replacing v.
3JEE Main Style
I = ½MR² = ½×1×(0.5)² = 0.125 kg·m².
KE = ½Iω² = ½×0.125×(10)² = ½×0.125×100 = 6.25 J.
The solid sphere has a smaller moment of inertia (2/5 MR² vs. 2/3 MR² for the shell), so less of its gravitational PE goes into rotational KE and more into translational KE — giving it greater linear acceleration down the incline.
α = τ/I = 10/2 = 5 rad/s².

You must be logged in to post a comment.