Pro 🔒~20 min

Rotational Motion & Torque

Angular momentum, moment of inertia, and spinning objects

How it works

Torque is the rotational equivalent of force: τ = rF sinθ. The rotational equivalent of Newton's 2nd Law is τ = Iα. Angular momentum L = Iω is conserved when no external torque acts — this is why a spinning skater spins faster when they pull in their arms (reducing I increases ω to keep L constant). The moment of inertia I depends on how mass is distributed relative to the rotation axis.

Why do figure skaters spin faster when they pull their arms in?

No extra push, no extra energy input — yet they visibly accelerate. The answer lies in angular momentum conservation.

What you'll learn

  • Moment of Inertia. Moment of inertia is the rotational equivalent of mass — it measures how hard it is to change an object's rotation. Unlike mass, it depends on how the mass is distributed relative to the axis. Moving mass farther from the axis dramatically increases the moment of inertia.
  • Angular Momentum Conservation. When no external torque acts on a system, angular momentum L = Iw is conserved. If the moment of inertia decreases (arms pulled in), angular velocity must increase proportionally. This is why a skater pulling in their arms can triple their spin rate.
  • Torque: The Rotational Force. Torque is what causes angular acceleration, just as force causes linear acceleration. It depends on three factors: the magnitude of the force, the distance from the pivot (lever arm), and the angle of application. This is why longer wrenches make bolts easier to turn.
  • Rotational Kinetic Energy. A spinning object carries kinetic energy even if its center of mass is stationary. When a skater pulls in their arms, their rotational KE actually increases — the extra energy comes from the work done by their muscles pulling inward against centripetal acceleration.

Step-by-step

  1. Apply torque to spin the disk.
  2. Observe angular acceleration α = τ/I.
  3. Then switch to the skater mode: start spinning with arms out, then pull them in and watch ω increase.
  4. The angular momentum display confirms conservation.
  5. Adjust the arm radius and watch the dramatic effect on spin speed.

Key formulas

  • τ=rFsinθ=Iα\tau = rF\sin\theta = I\alphaTorque (rotational equivalent of F=ma)
  • L=IωL = I\omegaAngular momentum
  • Li=LfI1ω1=I2ω2L_i = L_f \Rightarrow I_1\omega_1 = I_2\omega_2Conservation of angular momentum
  • I=miri2I = \sum m_i r_i^2Moment of inertia (depends on mass distribution)
  • KErot=12Iω2KE_{rot} = \frac{1}{2}I\omega^2Rotational kinetic energy

Frequently asked questions

A disk (I = 2 kg·m²) has a net torque of 8 N·m applied. What is its angular acceleration?
The correct answer is: 4 rad/s². Α = τ/I.
A skater spins at 2 rad/s with I = 4 kg·m². They pull in arms to I = 1 kg·m². New ω?
The correct answer is: 8 rad/s. L = Iω is conserved: I₁ω₁ = I₂ω₂.
Why does a longer wrench make it easier to loosen a bolt?
The correct answer is: It increases the lever arm, producing more torque for the same force. Τ = rF — larger r means larger torque for same force.
A solid disk (I = ½MR²) and a hollow ring (I = MR²) of equal mass and radius start from rest on an incline. Which reaches the bottom first?
The correct answer is: The solid disk (lower I means more translational KE). Lower I → more of PE converts to translational KE. Use energy conservation.