AP Physics C: Mechanics mock exam Free full practice test
A full-length practice test built from our exam-style questions on every unit of AP Physics C: Mechanics. Each answer is marked as you go, and every question has a worked solution to open afterwards.
Before you start
- Set a timer for about 140 minutes and work without notes. Use g = 9.8 m/s², as on the AP reference sheet. You can type answers like 4.9, 1/3 or 3.6e2.
- There are no hints in the mock. Answer every question before you open its worked solution: opening it first counts the question as missed.
- Write the free-response questions on paper, then mark them yourself with the scoring guide.
Section I: 35 exam-style questions
Hint
Displacement is the integral of velocity.
Worked solution
- Δx = ∫02 (4t3 − 3t2) dt = [t4 − t3]02.
- Δx = 16 − 8 = 8 m.
Hint
Only the vertical component matters for height.
Worked solution
- Vertical component: 20 sin 30° = 10 m/s.
- At the top vy = 0: h = vy2/(2g) = 100/19.6.
- h = 5.10 m.
Hint
Integrate twice, using both initial conditions.
Worked solution
- v = t2 + 1 (using v(0) = 1).
- x = t3/3 + t (using x(0) = 0).
- x(3) = 9 + 3 = 12 m.
Hint
At rest means v = 0.
Worked solution
- v = 3t2 − 12t + 9 = 3(t − 1)(t − 3).
- v = 0 at t = 1 s and t = 3 s: B.
Hint
Find the time to fall 45 m from the vertical motion; the horizontal velocity stays 12 m/s.
Worked solution
- Vertically: 45 = ½(9.8)t2, so t = 3.03 s.
- Horizontally: x = 12 × 3.03 = 36.4 m.
Hint
Treat the two masses as one system pulled by the difference in weights.
Worked solution
- Net force on the system: (6 − 4)g = 19.6 N; total mass 10 kg.
- a = 19.6/10 = 1.96 m/s².
Hint
Only the component of gravity along the incline accelerates it.
Worked solution
- a = g sin 30°.
- a = 9.8 × 0.5 = 4.9 m/s².
Hint
At terminal speed the acceleration is zero.
Worked solution
- At terminal speed: mg = bvT.
- vT = 0.20 × 9.8/0.50 = 3.92 m/s.
Hint
a(t) = F/m. Integrate to find v(t).
Worked solution
- a = 6t/2 = 3t, so v = 1.5t2.
- v(2) = 1.5 × 4 = 6 m/s.
Hint
Write m dv/dt = −bv, separate the variables and integrate.
Worked solution
- m dv/dt = −bv gives dv/v = −(b/m) dt, so v = v0e−bt/m.
- bt/m = 0.40 × 5.0/2.0 = 1.0.
- v = 10e−1 = 3.68 m/s.
Hint
Spring energy becomes kinetic energy.
Worked solution
- ½kx2 = ½mv2, so v = x√(k/m).
- v = 0.10 × √(200/0.050) = 0.10 × 63.2.
- v = 6.32 m/s.
Hint
F = −dU/dx.
Worked solution
- dU/dx = 8x − 4x3, which is 4 at x = 1.
- F = −dU/dx = −4 N, in the negative x direction.
Hint
At constant speed the driving force equals the resistance.
Worked solution
- Driving force = 600 N.
- P = Fv = 600 × 20 = 12000 W (12 kW).
Hint
F = −dU/dx. What does the force do if the particle moves slightly away?
Worked solution
- At a minimum, dU/dx = 0, so F = 0.
- Moving either way makes F point back towards the minimum, so the equilibrium is stable: B.
Hint
All the gravitational energy is removed by friction on the floor.
Worked solution
- mgh = μkmg d, and m and g cancel.
- d = h/μk = 2.0/0.25 = 8 m.
Hint
A perfectly inelastic collision: one final velocity.
Worked solution
- 2.0 × 3.0 = 3.0v.
- v = 2 m/s.
Hint
Integrate F(t) over the contact time.
Worked solution
- J = ∫00.20 2000(0.20t − t2) dt = 2000[0.10t2 − t3/3]00.20.
- = 2000(0.0040 − 0.002667).
- J = 2.67 N·s.
Hint
xcm = ∫ xλ dx / ∫ λ dx.
Worked solution
- Mass: ∫03 2x dx = 9 kg.
- ∫03 2x2 dx = 18 kg·m.
- xcm = 18/9 = 2 m.
Hint
ΣFext = Macm.
Worked solution
- With no external force, acm = 0.
- So the centre of mass moves with constant velocity (which may be zero): B.
Hint
Use conservation of momentum and of kinetic energy, or the elastic collision result v2 = 2m1u/(m1 + m2).
Worked solution
- Momentum: 6 = v1 + 2v2. Elastic, so relative speed reverses: v2 − v1 = 6.
- Adding: 3v2 = 12.
- v2 = 4 m/s (and the 1.0 kg ball rebounds at 2 m/s).
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.
Hint
Conserve angular momentum. Units of rev/s work on both sides.
Worked solution
- I1ω1 = I2ω2: 4.0 × 2.0 = 1.6ω2.
- ω2 = 5 rev/s.
Hint
Share the energy between translation and rotation, with I = ½MR2 and v = Rω.
Worked solution
- Mgh = ½Mv2 + ½(½MR2)(v/R)2 = ¾Mv2.
- v = √(4gh/3) = √(4 × 9.8 × 1.5/3) = √19.6.
- v = 4.43 m/s.
Hint
The centre of mass falls L/2. Use I = ML2/3 about the pivot.
Worked solution
- Mg(L/2) = ½(ML2/3)ω2, so ω = √(3g/L).
- ω = √(3 × 9.8/1.2) = √24.5.
- ω = 4.95 rad/s.
Hint
τ = dL/dt. Is there a torque about P?
Worked solution
- No net force acts, so there is no torque about P.
- So L = mvr⊥ is constant, with r⊥ the fixed perpendicular distance from P to the line: C.
Hint
Conserve angular momentum about the centre; the clay adds m(L/2)2 to I.
Worked solution
- Before: L = mv(L/2) = 0.20 × 5.0 × 0.50 = 0.50 kg·m²/s.
- After: I = ML2/12 + m(L/2)2 = 0.10 + 0.05 = 0.15 kg·m².
- ω = 0.50/0.15 = 3.33 rad/s.
Hint
Differentiate, or use vmax = Aω.
Worked solution
- v = −0.50 sin(10t), so vmax = Aω = 0.050 × 10.
- vmax = 0.5 m/s.
Hint
amax = Aω2.
Worked solution
- amax = 0.050 × 102 = 5 m/s².
Hint
At maximum displacement all the energy is in the spring.
Worked solution
- E = ½kA2 = ½ × 200 × 0.010.
- E = 1 J.
Hint
Look at T = 2π√(m/k). Does A appear?
Worked solution
- The period depends only on m and k.
- So it stays the same: C. The maximum speed doubles instead.
Hint
Physical pendulum: T = 2π√(I/(mgd)), with I = mL2/3 and d = L/2.
Worked solution
- T = 2π√((mL2/3)/(mgL/2)) = 2π√(2L/(3g)).
- T = 2π√(2.0/29.4) = 2π × 0.261.
- T = 1.64 s.
Section II: 4 free-response questions
Free-response question 1: Kinematics
Mathematical routines style · 6 points · about 15 minutes
A particle moves along the x-axis with position x(t) = t3 − 6t2 + 9t, in metres, for 0 ≤ t ≤ 4 s.
- (a) Find expressions for the velocity v(t) and acceleration a(t).
- (b) Find the times when the particle is at rest, and its position at each.
- (c) Find the total distance travelled from t = 0 to t = 4 s.
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)
v = 3t2 − 12t + 9; a = 6t − 12.
Part (b)
v = 3(t − 1)(t − 3) = 0 at t = 1 s (x = 4 m) and t = 3 s (x = 0).
Part (c)
x(0) = 0, x(1) = 4, x(3) = 0, x(4) = 4. Distance = 4 + 4 + 4 = 12 m.
Your mark: 0 of 6
Free-response question 2: Work, energy and power
Mathematical routines style · 6 points · about 20 minutes
A 0.50 kg block is attached to a nonlinear spring that exerts a force F(x) = −kx − βx3, with k = 50 N/m and β = 200 N/m3. The block moves on a frictionless horizontal surface.
- (a) Derive an expression for the potential energy U(x), taking U(0) = 0.
- (b) The block is released from rest at x = 0.20 m. Find its speed at x = 0.
- (c) Is x = 0 a position of stable equilibrium? Justify your answer.
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)
U = −∫0x F dx = ½kx2 + ¼βx4.
Part (b)
U(0.20) = 25(0.04) + 50(0.0016) = 1.08 J. ½(0.50)v2 = 1.08, so v = 2.08 m/s.
Part (c)
Yes: U has a minimum at x = 0, and for any small displacement F points back towards x = 0.
Your mark: 0 of 6
Free-response question 3: Torque and rotational dynamics
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
Free-response question 4: Oscillations
Mathematical routines style · 6 points · about 15 minutes
A block of mass m on a frictionless horizontal surface is attached to a spring of spring constant k. It is pulled a distance A from equilibrium and released from rest at t = 0.
- (a) Write the differential equation for the block's position x(t).
- (b) Show that x(t) = A cos(ωt) is a solution, and find ω.
- (c) For m = 0.20 kg, k = 80 N/m and A = 0.050 m, find the maximum speed.
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)
m d2x/dt2 = −kx.
Part (b)
d2x/dt2 = −Aω2 cos(ωt) = −ω2x. Matching gives ω = √(k/m). x(0) = A, as required.
Part (c)
ω = √(80/0.20) = 20 rad/s. vmax = Aω = 1.0 m/s.
Your mark: 0 of 6
After the mock
Note every question you missed and its unit, then go back to that unit's practice page: all AP Physics C: Mechanics units. Then try the real thing with official AP Physics C: Mechanics past papers.