Energy and momentum of rotating systems practice problems AP Physics 1, Unit 6
Rotational kinetic energy, rolling without slipping, angular momentum and its conservation. Try each question before you look: use the hint if you are stuck, then reveal the worked solution one step at a time.
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Key equations for energy and momentum of rotating systems
| K = ½Iω2 | rotational kinetic energy |
|---|---|
| L = Iω | angular momentum of a rigid object |
| L = mvr sinθ | angular momentum of a point mass |
| ΔL = τΔt | angular impulse |
| vcm = rω | rolling without slipping |
All questions use g = 9.8 m/s², as on the AP Physics 1 equation sheet. A calculator is allowed, as in the exam. The full sheet is in our AP Physics 1 equation sheet.
Warm-up questions
Quick checks on the core ideas. If these feel easy, go straight to the exam-style questions.
Hint
Use the rotational version of ½mv2.
Worked solution
- K = ½Iω2 = ½ × 0.20 × 102.
- K = 10 J.
Hint
Is there an external torque on the skater?
Worked solution
- With negligible external torque, angular momentum L = Iω is conserved.
- Pulling the arms in reduces I, so ω must increase to keep L constant.
- The answer is B.
Hint
L = Iω.
Worked solution
- L = 0.50 × 8.0 = 4.0 kg·m²/s.
Hint
Both lose the same potential energy per kilogram. Which one has to put more of it into spinning?
Worked solution
- Each object's energy at the bottom is shared between moving along and spinning.
- The hoop has all its mass at the rim, so a larger I (MR2) than the sphere (⅖MR2).
- The hoop puts more of its energy into rotation, leaving less for forward motion.
- The sphere is faster all the way down: B.
Exam-style questions
Questions at the level of the AP Physics 1 exam. The ones marked Challenge combine more than one idea.
Hint
Angular momentum is conserved. You can keep the rates in revolutions per second, since the units cancel.
Worked solution
- I1ω1 = I2ω2.
- 3.0 × 2.0 = 1.2 × ω2.
- ω2 = 5.0 rev/s.
Hint
Share the potential energy between translational and rotational kinetic energy, and use v = Rω.
Worked solution
- Energy: Mgh = ½Mv2 + ½Iω2.
- With I = ½MR2 and ω = v/R, the rotational term is ¼Mv2.
- So gh = ¾v2, giving v = √(4gh/3) = √(4 × 9.8 × 1.5 / 3) = √19.6.
- v = 4.43 m/s.
Hint
Add the translational and rotational kinetic energies.
Worked solution
- Translational: ½Mv2 = ½ × 3.0 × 4.0 = 6.0 J.
- Rotational: ½(MR2)(v/R)2 = ½Mv2 = 6.0 J.
- Total: 12 J. For a hoop, the two parts are always equal.
Hint
Angular momentum about the axle is conserved. Find the clay's angular momentum before it hits.
Worked solution
- Clay's angular momentum about the centre: L = mvr = 0.10 × 5.0 × 0.50 = 0.25 kg·m²/s.
- Afterwards the clay is part of the system: I = 0.40 + 0.10 × 0.502 = 0.425 kg·m².
- ω = L / I = 0.25 / 0.425 = 0.59 rad/s.
Hint
The work done by a torque is τΔθ.
Worked solution
- Work done: W = τΔθ = 5.0 × 10 = 50 J.
- This becomes rotational kinetic energy: 50 = ½ × 0.25 × ω2.
- ω2 = 400, so ω = 20 rad/s.
Hint
Write K in terms of L: K = L2 / 2I.
Worked solution
- With no external torque, L stays constant.
- The sand increases I, so ω falls.
- K = L2/2I: with L fixed and I larger, K decreases. The lost energy becomes internal energy as the sand sticks.
- The answer is B.
Free-response practice
One original question in the style of the exam's free-response section. Answer it in full, with working, before you open the scoring guide.
Qualitative/quantitative translation style · 6 points · about 20 minutes
Disc A spins at angular velocity ω0 on a frictionless axle. An identical disc B, not spinning, is dropped onto it on the same axle. Friction between the discs makes them spin together.
- (a) Derive an expression for the final angular velocity of the two discs, in terms of ω0.
- (b) Find the fraction of the original kinetic energy that remains after the discs spin together.
- (c) Explain why angular momentum is conserved in this process but kinetic energy is not.
Write your full answer on paper first, then open the scoring guide and tick each point you earned.
Scoring guide and model answer
Part (a)
No external torque about the axle, so angular momentum is conserved: Iω0 = (2I)ω, so ω = ω0/2.
Part (b)
Before: ½Iω02. After: ½(2I)(ω0/2)2 = ¼Iω02. So half the kinetic energy remains.
Part (c)
The friction torques between the discs are internal: they are equal and opposite, so the total angular momentum is unchanged. But the discs slide over each other while friction acts, and that converts kinetic energy into internal (thermal) energy.
Your mark: 0 of 6
Common mistakes in energy and momentum of rotating systems
- Leaving out rotational kinetic energy for an object that rolls.
- Assuming kinetic energy is conserved whenever angular momentum is.
- Using the wrong rotational inertia: check whether the object is a hoop, a disc or a sphere.
- Forgetting the r in L = mvr when a point mass joins a rotating object.
Keep going
Revise the ideas behind these questions:
Then try real exam questions: AP Physics 1 past papers, with official scoring guidelines. · All AP Physics 1 units