Torque and rotational dynamics practice problems AP Physics C: Mechanics, Unit 5
Torque, rotational inertia by integration and the parallel axis theorem, and Newton's second law for rotation. 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 torque and rotational dynamics
| τ = rF sin θ | torque |
|---|---|
| I = ∫ r2 dm | rotational inertia |
| I = Icm + Md2 | parallel axis theorem |
| Στ = Iα | Newton's second law for rotation |
| a = rα | rolling or string without slipping |
Use g = 9.8 m/s², as on the AP reference sheet. You can type answers like 4.9, 1/3 or 3.6e2. The full sheet is in our AP Physics C equation sheet.
Warm-up questions
Quick checks on the core ideas. If these feel easy, go straight to the exam-style questions.
Hint
τ = rF when the force is perpendicular.
Worked solution
- τ = 0.50 × 20 = 10 N·m.
Hint
I = mr2.
Worked solution
- I = 2.0 × 0.302 = 0.18 kg·m².
Hint
Rotational inertia grows with mass placed far from the axis.
Worked solution
- All of the hoop's mass is at radius R; much of the disk's is closer in.
- Ihoop = MR2 > Idisk = ½MR2: A.
Exam-style questions
Questions at the level of the AP Physics C: Mechanics exam. The ones marked Challenge combine more than one idea.
Hint
Integrate r2 dm with dm = (M/L) dr from 0 to L.
Worked solution
- I = ∫0L r2(M/L) dr = ML2/3.
- I = 3.0 × 4.0/3 = 4 kg·m².
Hint
I = ½MR2 for a disk.
Worked solution
- I = ½ × 4.0 × 0.502 = 0.50 kg·m².
- α = τ/I = 6.0/0.50 = 12 rad/s².
Hint
Parallel axis theorem, with d = R.
Worked solution
- I = ½MR2 + MR2 = 1.5MR2.
- I = 1.5 × 2.0 × 0.16 = 0.48 kg·m².
Hint
The one with less of its energy going into rotation moves faster.
Worked solution
- The sphere has I = (2/5)MR2, the hoop MR2.
- The sphere puts a smaller share of its energy into rotation, so it moves faster and arrives first: A.
Hint
Write F = ma for the block and τ = Iα for the pulley, with a = Rα.
Worked solution
- Block: mg − T = ma. Pulley: TR = (½MR2)(a/R), so T = ½Ma.
- mg = (m + ½M)a, so a = 9.8/(1.0 + 1.0).
- a = 4.9 m/s².
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.
Mathematical routines style · 7 points · about 20 minutes
A uniform rod of mass M and length L is pivoted at one end on a frictionless axle. It is held horizontal and then released from rest.
- (a) Use integration to show that the rod's rotational inertia about the pivot is ML2/3.
- (b) Find the angular acceleration just after release, for L = 1.2 m.
- (c) Show that the free end initially accelerates faster than g, and explain how that is possible.
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)
I = ∫0L r2(M/L) dr = (M/L)(L3/3) = ML2/3.
Part (b)
τ = MgL/2, so α = (MgL/2)/(ML2/3) = 3g/(2L) = 12.25 rad/s2.
Part (c)
a = αL = 3g/2 > g. The rod is rigid, so the pivot and the rest of the rod push the end down faster than free fall.
Your mark: 0 of 7
Common mistakes in torque and rotational dynamics
- Using the length of the rod as the lever arm for its weight: it acts at the centre of mass.
- Using I = ML2/12 (about the centre) for a rod pivoted at its end.
- Assuming the tension equals the hanging weight when the pulley has mass.
- Forgetting the sin θ in τ = rF sin θ.
Keep going
Revise the ideas behind these questions:
Then try real exam questions: AP Physics C: Mechanics past papers, with official scoring guidelines. · All AP Physics C: Mechanics units