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Reading Time: 6 min
Last Updated: March 30, 2026
Main Ideas: 4
Reading Time: 6 min
Last Updated: March 30, 2026
Main Ideas: 4

Topic 6.3 Notes – Angular Momentum and Angular Impulse

Verified for 2027 AP® Physics 1 Exam
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This is the rotational version of linear momentum and impulse. You’ll connect torque, time, and changes in rotational motion, and you’ll practice reading this relationship from equations and graphs.

1. What Angular Momentum Is

Angular momentum (L) measures how much rotational motion something has about a specific axis or point.

  • Symbol: LL
  • Units: kg⋅m2/s \text{kg}\cdot\text{m}^2/\text{s}
  • In AP Physics 1, treat direction using 1D sign conventions (clockwise vs. counterclockwise as +/−). You won’t use full 3D vector math.

Two things increase angular momentum:

  • Larger rotational inertia (harder to spin)
  • Faster rotation

And one huge idea:

Angular momentum always depends on the axis or reference point you choose.

Change the axis → you usually change LL.

2. How to Calculate Angular Momentum

There are two common cases. You need to recognize which situation you’re in.

a. Rigid object rotating about a fixed axis

If something is spinning as a solid object (disk, rod, wheel):

L=Iω L = I\omega

  • II = moment of inertia about that axis
  • ω\omega = angular velocity

If II is constant, then changing LL means changing ω\omega.

Example idea:
If a wheel with larger II spins at the same ω\omega as a smaller one, the larger II wheel has more angular momentum.

On tests, they may give you II or expect you to know common formulas (like for a disk or hoop).

b. Object moving in a straight line (about a point)

An object does not need to spin to have angular momentum.

A particle moving past a point has angular momentum about that point:

L=rmvsin⁡θ L = r m v \sin\theta

  • rr = distance from reference point
  • mm = mass
  • vv = speed
  • θ\theta = angle between the radius line and velocity

Key physical meanings:

  • If motion is directly toward or away from the point, then θ=0∘\theta = 0^\circ → L=0L = 0
  • Maximum LL when motion is perpendicular to the radius
  • Increasing mm, vv, or rr increases LL

In the diagram below, the velocity is broken into components parallel and perpendicular to the radius. Only the perpendicular component contributes to angular momentum, which is why the formula can also be thought of as L=rmv⊥L = r m v_\perp.

Angular momentum of a particle about point O

AP loves asking about how LL changes if the reference point changes. Same motion, different point → different rr → different LL.

3. What Angular Impulse Is

Angular impulse tells you how much torque changes angular momentum over time.

Angular impulse=τΔt \text{Angular impulse} = \tau \Delta t

  • Units: N⋅m⋅s \text{N}\cdot\text{m}\cdot\text{s} , same as kg⋅m2/s \text{kg}\cdot\text{m}^2/\text{s}
  • Direction follows the same sign as torque

So:

  • Bigger torque → bigger change in LL
  • Longer time → bigger change in LL

This is the rotational version of linear impulse FΔtF\Delta t.

Angular impulse from graphs

If you’re given a torque vs. time graph, the area under the curve equals angular impulse.

For example, a constant positive torque applied over a time interval creates a rectangular area. That shaded area represents ΔL \Delta L .

Torque vs. time graph showing angular impulse as area

  • Rectangle → τΔt \tau \Delta t
  • Irregular shape → find total area (add and subtract if below axis)

Students often forget to subtract negative regions. If torque is negative, the area counts as negative impulse.

4. The Rotational Impulse-Momentum Theorem

This is the central equation of the topic:

τnetΔt=ΔL \tau_{\text{net}} \Delta t = \Delta L

Also written as:

ΔL=Lf−Li \Delta L = L_f - L_i

That means:

Net angular impulse equals change in angular momentum.

If τnet=0 \tau_{\text{net}} = 0 , then ΔL=0 \Delta L = 0 .
That’s conservation of angular momentum.

Link to Newton’s Second Law (rotation)

The rotational form of Newton’s second law is:

τnet=ΔLΔt \tau_{\text{net}} = \frac{\Delta L}{\Delta t}

If II is constant:

τnet=Iα \tau_{\text{net}} = I\alpha

So this whole topic connects directly to τ=Iα \tau = I\alpha . The impulse-momentum equation just comes from applying that over a time interval.

Reading angular momentum graphs

If you see an LL vs. time graph, think slope first. The slope of the graph tells you the net torque.

Angular momentum vs. time graph

  • Slope = net torque
  • Steeper slope → larger torque
  • Flat line → zero net torque (angular momentum constant)

This shows up often in conceptual multiple-choice questions.

Key Takeaways

For rigid rotation, use L=IωL = I\omega; for a particle about a point, use L=rmvsin⁡θL = rmv\sin\theta.
Angular momentum depends on the chosen axis or reference point.
Angular impulse equals τΔt \tau \Delta t and has the same sign as the torque.
Area under a torque–time graph equals ΔL \Delta L .
Slope of an angular momentum–time graph equals net torque.
If net external torque is zero, angular momentum stays constant.

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Notes

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