Rotational Motion: Diagram-Based Questions (1)

easy 2 min read

Question

A uniform solid disc of mass M=2M = 2 kg and radius R=0.5R = 0.5 m rotates about its central axis. A force F=10F = 10 N is applied tangentially to the rim. Find the angular acceleration of the disc.

Solution — Step by Step

For a solid disc rotating about its central axis perpendicular to its plane:

I=12MR2=12×2×(0.5)2=0.25 kg m2I = \frac{1}{2} M R^2 = \frac{1}{2} \times 2 \times (0.5)^2 = 0.25 \text{ kg m}^2

The force is tangential, so the lever arm is RR and the torque is:

τ=FR=10×0.5=5 N m\tau = F R = 10 \times 0.5 = 5 \text{ N m}

α=τI=50.25=20 rad/s2\alpha = \frac{\tau}{I} = \frac{5}{0.25} = 20 \text{ rad/s}^2

Final answer: α=20\alpha = 20 rad/s2^2.

Why This Works

The equation τ=Iα\tau = I \alpha is the rotational version of F=maF = ma. The moment of inertia plays the role of mass — it measures how hard it is to angularly accelerate the body. The torque is the rotational analogue of force.

For a tangential force, the torque is simply FRF R. If the force were applied at angle θ\theta to the radius vector, we’d use τ=FRsinθ\tau = F R \sin\theta.

Alternative Method

Use energy methods if the question asks for angular velocity after rotation through an angle ϕ\phi: work done by torque =τϕ= \tau \phi equals change in rotational KE 12Iω2\frac{1}{2} I \omega^2. For pure angular acceleration, the direct τ=Iα\tau = I \alpha approach is faster.

Memorise the standard moments of inertia: solid disc 12MR2\frac{1}{2}MR^2, ring MR2MR^2, solid sphere 25MR2\frac{2}{5}MR^2, hollow sphere 23MR2\frac{2}{3}MR^2, rod about centre 112ML2\frac{1}{12}ML^2. These come up in every PYQ.

Common Mistake

Students sometimes use I=MR2I = MR^2 (ring formula) for a disc. The factor of 12\frac{1}{2} matters — using the wrong formula doubles your answer. Always pause and ask: solid or hollow? Disc or ring? The shape determines the constant.

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