Rotation & Angular Dynamics · Physics

If net external torque is zero, angular momentum stays constant.

Conservation of angular momentum is one of the most powerful shortcuts in mechanics. The key is choosing the system and the axis so that external torques are truly negligible.

This topic

Conservation of Angular Momentum

Learn when L is conserved, how to choose the right axis, and how to solve classic “changing I” situations.

Condition
When angular momentum is conserved
Angular momentum changes only when there is a net external torque about the axis you care about. If that torque is zero (or negligible), L is constant.
  • Core condition: Στext = 0 about the chosen axis
  • Pick the system: what’s “inside” vs “outside”
  • Pick the axis: conservation can depend on axis choice
  • Impulse-like torques: short-time events
Mechanism
Changing I changes ω
For rotation about a fixed axis, L = Iω. If L is conserved and I changes, ω must change inversely to keep the product constant.
  • Fixed-axis form: L = Iω (about that axis)
  • Decrease I → increase ω (spin faster)
  • Increase I → decrease ω (spin slower)
  • Why energy is not necessarily conserved
Examples
Classic conservation scenarios
Skaters pulling in arms, turntables with added masses, and rotating platforms all showcase conservation of angular momentum when external torques are negligible.
  • Spinning skater: arms in/out
  • Turntable + person stepping on/off (idealized)
  • Masses sliding radially on a rotating disk
  • Collisions where objects stick and rotate together (preview)
Pitfalls
Choosing system and axis correctly
Conservation is powerful but easy to misuse. The most common errors are ignoring external torques that are not actually negligible or switching axes mid-solution.
  • Friction torques: when can you ignore them?
  • Support forces can create torque about some axes
  • Axis must be the same “before and after”
  • State assumptions explicitly (short time, smooth bearings)
Practice
Practice & Exercises
Practice deciding whether L is conserved, applying Lbefore = Lafter, and interpreting changes in ω when I changes.
  • Decide if Στext ≈ 0 about an axis
  • Fixed-axis problems using L = Iω
  • Skater/turntable style before–after problems
  • Compare angular momentum vs energy outcomes
  • Exam-style angular momentum conservation sets