Torque and Angular Acceleration — τ = Iα

easy CBSE JEE-MAIN JEE-ADVANCED NCERT Class 11 3 min read

Question

A wheel of moment of inertia I=2 kg⋅m2I = 2 \text{ kg·m}^2 starts from rest and reaches an angular velocity of ω=10 rad/s\omega = 10 \text{ rad/s} in t=5 st = 5 \text{ s}. Find the torque required, assuming constant angular acceleration.


Solution — Step by Step

We know ω0=0\omega_0 = 0 (starts from rest), ω=10 rad/s\omega = 10 \text{ rad/s}, and t=5 st = 5 \text{ s}.

Using the rotational analogue of v=u+atv = u + at:

α=ωω0t=1005=2 rad/s2\alpha = \frac{\omega - \omega_0}{t} = \frac{10 - 0}{5} = 2 \text{ rad/s}^2

This is Newton’s second law for rotation. Just as F=maF = ma connects force to linear acceleration, τ=Iα\tau = I\alpha connects torque to angular acceleration. The moment of inertia II plays the role of “rotational mass.”

τ=Iα=2×2=4 N⋅m\tau = I\alpha = 2 \times 2 = 4 \text{ N·m}

The required torque is 4 N·m, applied constantly over 5 seconds.


Why This Works

The equation τ=Iα\tau = I\alpha is the rotational form of Newton’s second law. Every linear quantity has a rotational twin: force \leftrightarrow torque, mass \leftrightarrow moment of inertia, linear acceleration \leftrightarrow angular acceleration.

The key insight is that moment of inertia II tells us how hard it is to change the spin state of a body. A wheel with I=2 kg⋅m2I = 2 \text{ kg·m}^2 is harder to spin up than one with I=0.5 kg⋅m2I = 0.5 \text{ kg·m}^2 — you’d need 4× the torque to achieve the same α\alpha.

This problem is a direct application — no integration needed because α\alpha is constant throughout. That makes it a favourite for NCERT exercises and CBSE board short-answer questions.


Alternative Method

We can use the work-energy theorem for rotation as a cross-check.

The angular displacement in 5 s (starting from rest, constant α=2 rad/s2\alpha = 2 \text{ rad/s}^2):

θ=12αt2=12×2×25=25 rad\theta = \frac{1}{2}\alpha t^2 = \frac{1}{2} \times 2 \times 25 = 25 \text{ rad}

Work done by torque = gain in rotational kinetic energy:

τθ=12Iω2\tau \cdot \theta = \frac{1}{2}I\omega^2 τ×25=12×2×100=100 J\tau \times 25 = \frac{1}{2} \times 2 \times 100 = 100 \text{ J} τ=10025=4 N⋅m\tau = \frac{100}{25} = 4 \text{ N·m} \checkmark

Both methods give the same answer — good habit to cross-verify in JEE Main.


Common Mistake

Students often plug in ω=10 rad/s\omega = 10 \text{ rad/s} directly as α\alpha. These are different quantities — ω\omega is angular velocity (rad/s) while α\alpha is angular acceleration (rad/s²). Always compute α=Δω/Δt\alpha = \Delta\omega / \Delta t first. Writing τ=Iω\tau = I\omega is dimensionally wrong and is one of the most common errors in this chapter.

For any “from rest to ω\omega in time tt” problem, the first step is always α=ω/t\alpha = \omega/t. Memorise this reflex — it saves 30 seconds in JEE Main where time is everything.

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