6.2.2Energy and Momentum of Rotating Systems
Angular Impulse — AP PHYSICS 1 Revision Notes & Topical Questions
5 min read 9 parts Lesson 5 of 13 1 quiz
Lesson summary
6.2.2 Angular Impulse — AP PHYSICS 1 notes: Define angular impulse and use it to find the change in angular momentum produced by a torque acting over time.Angular impulse = the product of the average torque and the time interval over which it acts, τΔt.Unit — N·m·s = kg·m2/s, the…
- Linear analogue
- τΔt = ΔL = Lf − Li
- Rigid body about a fixed axis
- Generality
- Convention
- Torque along L
Section 1 of 9Definition
Angular impulse
Angular impulse the product of the average torque and the time interval over which it acts, τΔt.
Unit
- N·m·s = kg·m2/s, the unit of angular momentum.
Direction
- Direction same as the net torque; zero average torque gives no angular impulse.
Linear analogue
- FΔt changes momentum, so τΔt changes angular momentum.
Section 2 of 9Link to angular momentum
Link to angular momentum
τΔt
ΔL = Lf − Li
- from Στ = ΔL/Δt.
Rigid body about a fixed axis
- ΣτΔt = I(ωf − ωi) = IΔω.
Generality
- Generality also valid when I changes during the motion, unlike Στ = Iα used simply.
Section 3 of 9Sign and direction
Convention
- Convention counterclockwise positive, clockwise negative.
Torque along L
- Torque along L increases its magnitude.
Torque against L
- Torque against L decreases it, and acting long enough it reverses the rotation.
Section 4 of 9Applying angular impulse
1
Find the torque from each force, τ = rF sinθ.
2
Multiply by the time for which it acts.
3
Set the result equal to the change in angular momentum.
4
Divide by I to find the change in angular velocity.
Best for
- Best for short torques where time is known.
- (a bat hitting a ball, a hammer striking a rod)
Variable torque
- Variable torque use the average torque or the area under the torque–time graph.
Section 5 of 9Comparison with linear motion
| Linear | Angular |
|---|---|
| Force F | Torque τ |
| Momentum p | Angular momentum L |
| Mass m | Rotational inertia I |
| Impulse FΔt = Δp | Angular impulse τΔt = ΔL |
- Same impulse, different I
- same ΔL but different Δω because ω = L/I; a larger I gives less change in spin rate.
Section 6 of 9Impulse versus work
| Quantity | Involves | Changes |
|---|---|---|
| Angular impulse τΔt | Time | Angular momentum |
| Work τΔθ | Angle | Kinetic energy |
1Starting from rest with constant τ
- Starting from rest with constant τ impulse gives ω = τt/I;
- work gives ½Iω2 = τΔθ with Δθ = ½(τ/I)t2;
- both agree.
2Choose impulse
- Choose impulse for short interactions with known duration.
3Choose work
- Choose work when the angle or number of turns is known.
4Unit check
- N·m·s divided by kg·m2 leaves s−1.
Section 7 of 9More from the specification
More from the specification
Distance
- Total length of path travelled, a scalar.
Collision
- Short interaction with large internal forces.
Newton
- Unit of force, kg m s-2.
External torque
- Torque produced by a force from outside the system.
Rigid system
- System that holds its shape while rotating.
Section 8 of 9Key terms
| Term | Meaning |
|---|---|
| Angular impulse | Product of net torque and the time it acts, τΔt. |
| Torque | Rotational effect of a force, τ = rF sinθ. |
| Change in angular momentum | ΔL = Lf − Li, equal to the angular impulse. |
| Net torque | Sum of all external torques on the system. |
| N·m·s | Unit of angular impulse. |
Section 9 of 9Exam technique
1
Confusing angular impulse τΔt with linear impulse FΔt.
2
Forgetting to use the net torque when several torques act.
3
Using angular impulse where the angle is given but not the time.
4
Dropping the sign when a torque opposes the rotation.
5
Calculating Δω as impulse times I instead of impulse divided by I.
Marked practiceQuizzes for this lesson
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